Section 1.1
Chapter 1
Prerequisites for Calculus
Section 1.1 Exercises
1. Dx 5 21 2 1 5 22
Dy 5 21 2 2 5 23
■ Section 1.1 Lines (pp. 1–9)
2. Dx 5 21 2 (23) 5 2
Dy 5 22 2 2 5 24
Quick Review 1.1
3. Dx 5 28 2 (23) 5 25
Dy 5 1 2 1 5 0
1. y 5 22 1 4(3 2 3) 5 22 1 4(0) 5 22 1 0 5 22
2. 3
3
2x
x
4. Dx 5 0 2 0 5 0
Dy 5 22 2 4 5 26
5 3 2 2(x 1 1)
5 3 2 2x 2 2
5 22
5 21
223
524
5. (a, c)
y
5
21
1
3. m 5 }} 5 }} 5 21
B
2 2 (23)
3 2 (21)
5
4
4. m 5 }} 5 }}
5
x
A
142
1
5. (a) 3(2) 2 4 }} 0 5
621 55
Yes
(b) 3(3) 2 4(21) 0 5
13 Þ 5
1 2 (22)
221
3
1
(b) m 5 }} 5 }} 5 3
No
6. (a, c)
6. (a) 7 0 22(21) 1 5
7 5 2 1 5 Yes
y
5
(b) 1 5 22(22) 1 5
1 Þ 9 No
7. d 5 Ï(x
ww
wwxw
2
)2w1
ww(w
y2w
2wyw
)2w
2
1
1
5
x
A
5 Ï(0
ww
2w
1w
)2w
1w(1ww
2w0w
)2
B
5 Ï2w
8. d = Ï(x
ww
wwxw
2
)2w1
ww(w
y2w
2wyw
)2w
2
1
1
5
5
5
5
!(1§§2§2)§§1§12§§§2§1§2
1
}}
3
2
2
22 2 (21)
1 2 (22)
7. (a, c)
1
3
y
5
!(2
§1§)§§1§12§}§3}§2
4 2
2
21
3
(b) m 5 }} 5 }} 5 2}}
B
!§§§§
16
9
A
1 1 }}
5
! §§
25
}}
9
x
5
3
5 }}
9. 4x 2 3y 5 7
323
21 2 2
0
23
(b) m 5 }} 5 }} 5 0
23y 5 24x 1 7
4
3
7
3
y 5 }}x 2 }}
8. (a, c)
y
5
10. 22x 1 5y 5 23
A
5y 5 2x 2 3
2
5
3
5
y 5 }}x 2 }}
5
B
x
1
2
Section 1.1
8. continued
26. The line contains (0, 0) and (5, 2).
23 2 2
25
(b) m 5 }} 5 }} (undefined)
121
0
This line has no slope.
9. (a) x 5 2
(b) y 5 3
220
520
2
y 5 }}x
5
2
5
m 5 }} 5 }}
27. 3x 1 4y 5 12
10. (a) x 5 21
4y 5 23x 1 12
4
3
(b) y 5 }}
3
4
y 5 2}}x 1 3
11. (a) x 5 0
(b) y 5 2Ï2w
3
4
(a) Slope: 2}}
12. (a) x 5 2p
(b) y-intercept: 3
(b) y 5 0
(c)
13. y 5 1(x 2 1) 1 1
14. y 5 21[x 2 (21)] 1 1
y 5 21(x 1 1) 1 1
15. y 5 2(x 2 0) 1 3
[210, 10] by [210, 10]
16. y 5 22[x 2 (24)] 1 0
y 5 22(x 1 4) 1 0
28. x 1 y 5 2
y 5 2x 1 2
320
3
220
2
3
y 5 }}(x 2 0) 1 0
2
3
y 5 }}x
2
17. m 5 }} 5 }}
(a) Slope: 21
(b) y-intercept: 2
(c)
2y 5 3x
3x 2 2y 5 0
121
221
[210, 10] by [210, 10]
0
1
18. m 5 }} 5 }} 5 0
y 5 0(x 2 1) 1 1
y51
22 2 0
22 2 (22)
x
y
3
4
y
x
}} 5 2}} 1 1
4
3
4
y 5 2}}x 1 4
3
29. }} 1 }} 5 1
22
0
19. m 5 }} 5 }} (undefined)
4
3
(a) Slope: 2}}
Vertical line: x 5 22
23
22 2 1
4
2 2 (22)
3
y 5 2}}[x 2 (22)] 1 1
4
3
4
20. m 5 }} 5 }} 5 2}}
(b) y-intercept: 4
(c)
4y 5 23(x 1 2) 1 4
4y 5 23x 2 2
[210, 10] by [210, 10]
30. y 5 2x 1 4
3x 1 4y 5 22
(a) Slope: 2
21. y 5 3x 2 2
22. y 5 21x 1 2 or y 5 2x 1 2
(b) y-intercept: 4
(c)
1
2
23. y 5 2}}x 2 3
1
3
24. y 5 }}x 2 1
[210, 10] by [210, 10]
25. The line contains (0, 0) and (10, 25).
25 2 0
10 2 0
5
y 5 }}x
2
25
10
5
2
m 5 }} 5 }} 5 }}
Section 1.1
31. (a) The desired line has slope 21 and passes through
(0, 0):
y 5 21(x 2 0) 1 0 or y 5 2x.
21
(b) The desired line has slope }} 5 1 and passes through
21
(0, 0):
y 5 1(x 2 0) 1 0 or y 5 x.
39. (a) y 5 0.680x 1 9.013
(b) The slope is 0.68. It represents the approximate average
weight gain in pounds per month.
(c)
32. (a) The given equation is equivalent to y 5 22x 1 4.
The desired line has slope 22 and passes through
(22, 2):
y 5 22(x 1 2) 1 2 or y 5 22x 2 2.
21
22
1
2
(b) The desired line has slope }} 5 }} and passes through
[15, 45] by [15, 45]
(d) When x 5 30, y < 0.680(30) 1 9.013 5 29.413.
She weighs about 29 pounds.
40. (a) y 5 1,060.4233x 2 2,077,548.669
(22, 2):
1
2
3
(b) The slope is 1,060.4233. It represents the approximate
rate of increase in earnings in dollars per year.
1
2
y 5 }}(x 1 2) 1 2 or y 5 }}x 1 3.
33. (a) The given line is vertical, so we seek a vertical line
through (22, 4): x 5 22.
(c)
(b) We seek a horizontal line through (22, 4): y 5 4.
34. (a) The given line is horizontal, so we seek a horizontal
1
1
2
2
1
2
line through 21, }} : y 5 }}.
1
2
1
(b) We seek a vertical line through 21, }} : x 5 21.
2
922
7
35. m 5 }} 5 }}
321
2
7
7
3
f(x) 5 }}(x 2 1) 1 2 5 }}x 2 }}
2
2
2
7
3
Check: f(5) 5 }}(5) 2 }} 5 16, as expected.
2
2
7
3
7
3
Since f(x) 5 }}x 2 }}, we have m 5 }} and b 5 2}}.
2
2
2
2
24 2 (21)
23
3
422
2
2
3
3
f(x) 5 2}}(x 2 2) 1 (21) 5 2}}x 1 2
2
2
3
Check: f(6) 5 2}}(6) 1 2 5 27, as expected.
2
3
3
Since f(x) 5 2}}x 1 2, we have m 5 2}} and b 5 2.
2
2
36. m 5 }} 5 }} 5 2}}
37.
2
3
y23
4 2 (22)
2}} 5 }}
2
3
2}}(6) 5 y 2 3
24 5 y 2 3
(d) When x 5 2000,
y < 1,060.4233(2000) 2 2,077,548.669 < 43,298.
In 2000, the construction workers’ average annual compensation will be about $43,298.
41. y 5 1 ? (x 2 3) 1 4
y5x2314
y5x11
This is the same as the equation obtained in Example 5.
x
c
y
When x 5 0, we have }} 5 1, so y 5 d.
d
x
(b) When y 5 0, we have }} 5 2, so x 5 2c.
c
y
When x 5 0, we have }} 5 2, so y 5 2d.
d
42. (a) When y 5 0, we have }} 5 1, so x 5 c.
The x-intercept is 2c and the y-intercept is 2d.
2
k
3
k
43. (a) The given equations are equivalent to y 5 2}}x 1 }}
and y 5 2x 1 1, respectively, so the slopes are
2
k
2
k
2}} and 21. The lines are parallel when 2}} 5 21,
so k 5 2.
2
21
(b) The lines are perpendicular when 2}} 5 }}, so
k
21
k 5 22.
21 5 y
38.
[1975, 1995] by [20,000, 35,000]
2 2 (22)
x 2 (28)
2 5 }}
2(x 1 8) 5 4
x18 52
x 5 26
68 2 69.5
0.4 2 0
21.5
0.4
44. (a) m < }} 5 }} 5 23.75 degrees/inch
10 2 68
4 2 0.4
258
3.6
5 2 10
4.7 2 4
25
0.7
(b) m < }} 5 }} < 216.1 degrees/inch
(c) m < }} 5 }} 5 27.1 degrees/inch
(d) Best insulator: Fiberglass insulation
Poorest insulator: Gypsum wallboard
The best insulator will have the largest temperature
change per inch, because that will allow larger
temperature differences on opposite sides of thinner
layers.
4
Section 1.1
Dp
Dd
10.94 2 1
100 2 0
9.94
100
45. Slope: k 5 }} 5 }} 5 }}
y
5 0.0994 atmospheres per meter
6
(–1, 4)
At 50 meters, the pressure is
p 5 0.0994(50) 1 1 5 5.97 atmospheres.
(2, 3)
46. (a) d(t) 5 45t
(–1, 1)
(b)
x
6
(2, 0)
y
[0, 6] by [250, 300]
6
(c) The slope is 45, which is the speed in miles per hour.
(d) Suppose the car has been traveling 45 mph for several
hours when it is first observed at point P at time t 5 0.
(2, 3)
(e) The car starts at time t 5 0 at a point 30 miles past P.
(–1, 1)
47. (a) y 5 5632x 2 11,080,280
6
(2, 0)
(–1, –2)
(b) The rate at which the median price is increasing in
dollars per year
(c) y 5 2732x 2 5,362,360
50.
(d) The median price is increasing at a rate of about $5632
per year in the Northeast, and about $2732 per year in
the Midwest. It is increasing more rapidly in the
Northeast.
y
(c, d)
W
(a, b)
48. (a) Suppose x8F is the same as x8C.
X
Z
9
5
x 5 }}x 1 32
(g, h)
11 2 }5}2x 5 32
9
4
5
x
x
(e, f)
Y
2}}x 5 32
Suppose that the vertices of the given quadrilateral are
x 5 240
(a, b), (c, d), (e, f ), and (g, h). Then the midpoints of the
Yes, 2408F is the same as 2408C.
consecutive sides are W }}, }} , X }}, }} ,
a1c b1d
c1e d1f
2
2
2
2
e1g f1h
g1a h1b
Y }}, }} , and Z }}, }} . When these four
2
2
2
2
1
(b)
2
1
1
2
2 1
2
points are connected, the slopes of the sides of the resulting
figure are:
[290, 90] by [260, 60]
It is related because all three lines pass through the
point (240, 240) where the Fahrenheit and Celsius
temperatures are the same.
49. The coordinates of the three missing vertices are (5, 2),
(21, 4) and (21, 22), as shown below.
y
6
(2, 3)
(5, 2)
(–1, 1)
(2, 0)
6
x
d1f
b1d
}} 2 }}
2
2
f2b
WX: }}
5 }}
c1e
a1c
e
2a
}} 2 }}
2
2
f1h
d1f
}} 2 }}
2
2
h2d
XY: }}
5 }}
e1g
c1e
g2c
}} 2 }}
2
2
f1h
h1b
}} 2 }}
2
2
f2b
ZY: }}
5 }}
e1g
g1a
e
2a
}} 2 }}
2
2
h1b
b1d
}} 2 }}
2
2
h2d
WZ: }}
5 }}
g1a
a1c
g2c
}} 2 }}
2
2
Opposite sides have the same slope and are parallel.
Section 1.1
420
320
4
3
51. The radius through (3, 4) has slope }} 5 }}.
21
4/3
3
4
3
4
The tangent line is tangent to this radius, so its slope is }} 5 2}}. We seek the line of slope 2}} that passes through (3, 4).
3
4
3
9
y 5 2}}x 1 }} 1 4
4
4
3
25
y 5 2}}x 1 }}
4
4
y 5 2}}(x 2 3) 1 4
52. (a) The equation for line L can be written as
A
B
C
B
21
2A/B
A
B
B
A
y 5 2}}x 1 }}, so its slope is 2}}. The perpendicular line has slope }} 5 }} and passes through (a, b), so its equation is
B
A
y 5 }}(x 2 a) 1 b.
B
A
(b) Substituting }}(x 2 a) 1 b for y in the equation for line L gives:
3A
4
B
Ax 1 B }}(x 2 a) 1 b 5 C
A2x 1 B2(x 2 a) 1 ABb 5 AC
(A2 1 B2)x 5 B2a 1 AC 2 ABb
B2a 1 AC 2 ABb
A 1B
x 5}
2 }
2
Substituting the expression for x in the equation for line L gives:
B2a 1 AC 2 ABb
A 1B
2A(B2a 1 AC 2 ABb)
C(A2 1 B2)
By 5 }}}
1}
}
2
2
A 1B
A2 1 B 2
1
2
1 By 5 C
A}
2 }
2
2AB2a 2 A2C 1 A2Bb 1 A2C 1 B2C
A 1B
By 5 }}}}
2
2
A2Bb 1 B2C 2 AB2a
A 1B
By 5 }}}
2
2
A2b 1 BC 2 ABa
A 1B
y 5 }}
2
2
1
B2a 1 AC 2 ABb A2b 1 BC 2 ABa
A 1B
A 1B
2
, }}
.
The coordinates of Q are }}
2
2
2
2
(c)
Distance 5 Ï(x
ww
2w
aw
)2w
1w(yw2
wwbw
)2
5
!1§}
§§A§§1}
§B §§§§§2§a2§§1§1}
§§§A§§1}
§B §§§§§2§b2§
5
}}}} 2 1 1 }}}} 2
!1§§§
§§§§§
§
A 1B
A 1B
5
!§1 §§§§§§§§§§2 §1§1§§§§§§§§§§§2
5
!§1}
§§A§§1}
§B§§§§2 §1§1}
§§§A§§1}
§B§§§§2
5
1
!§§§§§§
5
}}}
!§§
(A 1 B )
5
!}
§§§A§§1}
§B§§§
2
B2a 1 AC 2 ABb
2
2
B2a 1 AC 2 ABb 2 a(A2 1 B2) 2
2
A(C 2 Bb 2 Aa) 2
2
BC 2 ABa 2 B2b 2
}
}
A2 1 B2
B(C 2 Aa 2 Bb) 2
2
A2(C 2 Aa 2 Bb)2
}}
(A2 1 B2)2
2 2
(C 2 Aa 2 Bb)2
2
)C 2 Aa 2 Bb)
5 }}
B 2w
ÏA
w2w1
ww
)Aa 1 Bb 2 C)
5 }}
A 2w1
B 2w
Ïw
ww
2
B2(C 2 Aa 2 Bb)2
}}
(A2 1 B2)2
(A2 1 B2)(C 2 Aa 2 Bb)2
2
A2b 1 BC 2 ABa 2 b(A2 1 B2) 2
2
2
2
2
2
AC 2 ABb 2 A2a 2
}
}
A2 1 B 2
2
A2b 1 BC 2 ABa
2
2
5
6
Section 1.2
■ Section 1.2 Functions and Graphs
(pp. 9–19)
Exploration 1
Composing Functions
1. y3 5 g + f, y4 5 f + g
2. Domain of y3: [22, 2] Range of y3: [0, 2]
y1:
[24.7, 4.7] by [22, 4.2]
y2:
[24.7, 4.7] by [22, 4.2]
5. x2 , 16
Solutions to x2 5 16: x 5 24, x 5 4
Test x 5 26 (26)2 5 36 . 16
x2 , 16 is false when x , 24
Test x 5 0: 02 5 0 , 16
x2 , 16 is true when 24 , x , 4
Test x 5 6: 62 5 36 . 16
x2 , 16 is false when x . 4.
Solution set: (24, 4)
6. 9 2 x2 $ 0
Solutions to 9 2 x2 5 0: x 5 23, x 5 3
Test x 5 24: 9 2 (24)2 5 9 2 16 5 27 , 0
9 2 x2 $ 0 is false when x , 23.
Test x 5 0: 9 2 02 5 9 . 0
9 2 x2 $ 0 is true when 23 , x , 3.
Test x 5 4: 9 2 42 5 9 2 16 5 27 , 0
9 2 x2 $ 0 is false when x . 3.
Solution set: [23, 3]
7. Translate the graph of f 2 units left and 3 units downward.
8. Translate the graph of f 5 units right and 2 units upward.
y3:
9. (a)
[24.7, 4.7] by [22, 4.2]
3. Domain of y4: [0, `); Range of y4: (2`, 4]
y4:
(b)
f(x)
x2 2 5
x2 2 9
(x 1 3)(x 2 3)
x
54
54
50
50
5 23 or x 5 3
f(x) 5 26
x2 2 5 5 26
x2 5 21
No real solution
10. (a) f(x) 5 25
1
}} 5 25
x
1
x 5 2}}
5
[22, 6] by [22, 6]
4. y3 5 y2 ( y1(x)) 5 Ïw
y1(x
w)w 5 Ï4ww
2wx 2w
2
y4 5 y1( y2(x)) 5 4 2 (y2(x)) 5 4 2 (Ïxw)2 5 4 2 x, x $ 0
Quick Review 1.2
1. 3x 2 1 # 5x 1 3
22x # 4
x $ 22
Solution: [22, `)
2. x(x 2 2) . 0
Solutions to x(x 2 2) 5 0: x 5 0, x 5 2
Test x 5 21: 21(21 2 2) 5 3 . 0
x(x 2 2) . 0 is true when x , 0.
Test x 5 1: 1(1 2 2) 5 21 , 0
x(x 2 2) . 0 is false when 0 , x , 2.
Test x 5 3: 3(3 2 2) 5 3 . 0
x(x 2 2) . 0 is true when x . 2.
Solution set: (2`, 0) < (2, `)
3. )x 2 3) # 4
24 # x 2 3 # 4
21 # x # 7
Solution set: [21, 7]
4. )x 2 2) $ 5
x 2 2 # 25 or x 2 2 $ 5
x # 23 or x $ 7
Solution set: (2`, 23] < [7, `)
(b) f(x) = 0
1
}} 5 0
x
No solution
11. (a)
(b)
12. (a)
(b)
f(x) = 4
Ïxww
1w7 5 4
x 1 7 5 16
x 59
Check: Ï9ww
1w7 5 Ï1w6w 5 4; it checks.
f(x) 5 1
Ïxww
1w7 5 1
x17 51
x 5 26
Check: Ï2
w6ww
1w7 5 1; it checks.
f(x)
Ïxww
2w1
x21
x
3
3
5 22
5 22
5 28
5 27
f(x) 5 3
Ïxw2
ww1 5 3
x 2 1 5 27
x 5 28
Section 1.2
8. (a) Since we require 2x $ 0, the domain is (2`, 0].
Section 1.2 Exercises
d 2
122
7
pd
4
2
1. Since A 5 pr2 5 p }} , the formula is A 5 }}, where A
(b) (2`, 0]
(c)
represents area and d represents diameter.
2. Let h represent height and let s represent side length.
s 2
122
h2 1 }}
5 s2
[210, 3] by [24, 2]
(d) None
1
4
h2 5 s2 2 }}s2
3
4
9. (a) Since we require 3 2 x $ 0, the domain is (2`, 3].
h2 5 }}s2
(b) [0, `)
Ï3w
h 5 6}}s
(c)
2
Since side length and height must be positive, the formula
Ïw3
is h 5 }}s.
2
[24.7, 4.7] by [26, 6]
(d) None
s
s
h
s
2
s
2
10. (a) Since we require x 2 2 Þ 0, the domain is
(2`, 2) < (2, `).
1
x22
(b) Since }} can assume any value except 0, the range is
(2`, 0) < (0, `).
s
3. S 5 6e2, where S represents surface area and e represents
edge length.
(c)
4
4. V 5 }}pr3, where V represents volume and r represents
3
radius.
5. (a) (2`, `) or all real numbers
[24.7, 4.7] by [26, 6]
(b) (2`, 4]
(d) None
(c)
11. (a) (2`, `) or all real numbers
(b) (2`, `) or all real numbers
(c)
[25, 5] by [210, 10]
(d) Symmetric about y-axis (even)
6. (a) (2`, `) or all real numbers
(b) [29, `)
[26, 6] by [23, 3]
(d) None
(c)
12. (a) (2`, `) or all real numbers
(b) The maximum function value is attained at the point
(0, 1), so the range is (2`, 1].
[25, 5] by [210, 10]
(c)
(d) Symmetric about the y-axis (even)
7. (a) Since we require x 2 1 $ 0, the domain is [1, `).
(b) [2, `)
[26, 6] by [23, 3]
(c)
(d) Symmetric about the y-axis (even)
[23, 10] by [23, 10]
(d) None
8
Section 1.2
13. (a) Since we require 2x $ 0, the domain is (2`, 0].
x3, so its domain is
18. (a) This function is equivalent to y 5 Ïw
[0, `).
(b) [0, `)
(b) [0, `)
(c)
(c)
[210, 3] by [21, 2]
[22, 5] by [22, 8]
(d) None
14. (a) Since we require x Þ 0, the domain is
(2`, 0) < (0, `).
1
x
(d) None
19. Even, since the function is an even power of x.
1
x
(b) Note that }} can assume any value except 0, so 1 1 }}
20. Neither, since the function is a sum of even and odd powers
of x.
21. Neither, since the function is a sum of even and odd powers
of x (x1 1 2x0).
can assume any value except 1.
The range is (2`, 1) < (1, `).
22. Even, since the function is a sum of even powers of x
(x2 2 3x0).
(c)
23. Even, since the function involves only even powers of x.
24. Odd, since the function is a sum of odd powers of x.
25. Odd, since the function is a quotient of an odd function (x3)
and an even function (x2 2 1).
[24, 4] by [24, 4]
(d) None
15. (a) Since we require 4 2 x2 $ 0, the domain is [22, 2].
(b) Since 4 2 x2 will be between 0 and 4, inclusive (for x
in the domain), its square root is between 0 and
2, inclusive. The range is [0, 2].
(c)
26. Neither, since, (for example), y(22) 5 41/3 and y(2) 5 0.
27. Neither, since, (for example), y(21) is defined and y(1) is
undefined.
28. Even, since the function involves only even powers of x.
29. (a)
[29.4, 9.4] by [26.2, 6.2]
[24.7, 4.7] by [23.1, 3.1]
Note that f(x) 5 2)x 2 3) 1 2, so its graph is the graph
of the absolute value function reflected across the
x-axis and then shifted 3 units right and 2 units upward.
(d) Symmetric about the y-axis (even)
3
x2, so its domain is
16. (a) This function is equivalent to y 5 Ïw
all real numbers.
(b) [0, `)
(b) (2`, `)
(c) (2`, 2]
(c)
30. (a) The graph of f(x) is the graph of the absolute value
function stretched vertically by a factor of 2 and then
shifted 4 units to the left and 3 units downward.
[22, 2] by [21, 2]
(d) Symmetric about the y-axis (even)
17. (a) Since we require x2 Þ 0, the domain is
(2`, 0) < (0, `)
1
x
(b) Since }}2 . 0 for all x, the range is (1, `).
[210, 5] by [25, 10]
(b) (2`, `) or all real numbers
(c) [23, `)
31. (a)
(c)
[24, 4] by [21, 5]
(d) Symmetric about the y-axis (even)
[24.7, 4.7] by [21, 6]
(b) (2`, `) or all real numbers
(c) [2, `)
Section 1.2
44. Line through (21, 0) and (0, 23):
32. (a)
23
1
23 2 0
0 2 (21)
m 5 }} 5 }} 5 23, so y 5 23x 2 3
Line through (0, 3) and (2, 21):
21 2 3
220
24
2
m 5 }} 5 }} 5 22, so y 5 22x 1 3
[24, 4] by [22, 3]
(b) (2`, `) or all real numbers
f(x) 5
(c) [0, `)
33. (a)
h
23x 2 3,
22x 1 3,
21 , x # 0
0,x#2
45. Line through (21, 1) and (0, 0): y 5 2x
Line through (0, 1) and (1, 1): y 5 1
Line through (1, 1) and (3, 0):
[23.7, 5.7] by [24, 9]
021
21
1
321
2
2
1
1
3
so y 5 2}}(x 2 1) 1 1 5 2}}x 1 }}
2
2
2
m 5 }} 5 }} 5 2}},
(b) (2`, `) or all real numbers
(c) (2`, `) or all real numbers
h
34. (a)
2x,
21 # x , 0
0,x#1
f(x) 5 1,
1
3
2}}x 1 }},
2
2
[22.35, 2.35] by [21, 3]
1
2
46. Line through (22, 21) and (0, 0): y 5 }}x
(b) (2`, `) or all real numbers
Line through (0, 2) and (1, 0): y 5 22x 1 2
(c) [0, `)
35. Because if the vertical line test holds, then for each
x-coordinate, there is at most one y-coordinate giving a
point on the curve. This y-coordinate would correspond to
the value assigned to the x-coordinate. Since there is only
one y-coordinate, the assignment would be unique.
36. If the curve is not y 5 0, there must be a point (x, y) on the
curve where y Þ 0. That would mean that (x, y) and (x, 2y)
are two different points on the curve and it is not the graph
of a function, since it fails the vertical line test.
37. No
Line through (1, 21) and (3, 21): y 5 21
h
1
}}x,
2
40. No
12 2
T
47. Line through }}, 0 and (T, 1):
120
T 2 (T/2)
x,
2x 1 2,
h
0#x#1
1,x#2
48. f (x) 5
1
3
5
3
so y 5 2}}(x 2 2) 1 1 5 2}}x 1 }}
h
1
3
5
3
2}}x 1 }},
1
T
2
2
2
T
h
A,
2A,
A,
T
2
0 # x # }}
T
}} , x # T
2
T
2
0 # x , }}
T
}} # x , T
2
3T
T # x , }}
2
3T
}} # x # 2T
2
(b) g( f (x))5 (x 1 5)2 2 3
5 (x 2 1 10x 1 25) 2 3
5 x 2 1 10x 1 22
021
522
21
3
1
3
Line through (2, 1) and (5, 0): m 5 }} 5 }} 5 2}},
2x 1 2,
2
T
49. (a) f (g(x)) 5 (x 2 2 3) 1 5 5 x 2 1 2
43. Line through (0, 2) and (2, 0): y 5 2x 1 2
1
3
T
2A,
0#x,1
1#x,2
2#x,3
3#x#4
2,
0,
42. f(x) 5
2,
0,
2
T
m 5 }} 5 }}, so y 5 }} x 2 }} 1 0 5 }}x 2 1
41. Line through (0, 0) and (1, 1): y 5 x
Line through (1, 1) and (2, 0): y 5 2x 1 2
h
0,x#1
1,x#3
21,
0,
f (x) 5 2
}}x 2 1,
39. Yes
f(x) 5
22 # x # 0
f(x) 5 22x 1 2,
h
38. Yes
f (x) 5
1,x,3
0,x#2
2,x#5
(c) f (g(0)) 5 02 1 2 5 2
(d) g( f (0)) 5 02 1 10 ? 0 1 22 5 22
(e) g(g(22)) 5 [(22)2 2 3]2 2 3 5 12 2 3 5 22
(f) f ( f(x)) 5 (x 1 5) 1 5 5 x 1 10
9
10
Section 1.2
g + f:
50. (a) f (g(x)) 5 (x 2 1) 1 1 5 x
(b) g( f (x)) 5 (x 1 1) 2 1 5 x
(c) f (g(x)) 5 0
(d) g( f (0)) 5 0
(e) g(g(22)) 5 (22 2 1) 2 1 5 23 2 1 5 24
(f) f ( f (x)) 5 (x 1 1) 1 1 5 x 1 2
[24.7, 4.7] by [22, 4]
51. (a) Enter y1 5 f(x) 5 x 2 7, y2 5 g(x) 5 Ïxw,
y3 5 ( f + g)(x) 5 y1(y2(x)),
and y4 5 (g + f )(x) 5 y2(y1(x))
f + g:
g + f:
Domain: (2`, 21] < [1, `)
Range: [0, `)
ww2)2 2 3
(b) ( f + g)(x) 5 (Ïxw1
5 (x 1 2) 2 3, x $ 22
5 x 2 1, x $ 22
(g + f )(x) 5 Ïw
(x2ww
2w3w
)w
1w
2 5 Ïw
x2w
2w1
2x 2 1
x13
3x 1 1
22x
54. (a) Enter y1(x) 5 f(x) 5 }}, y2 5 }},
[210, 70] by [210, 3]
Domain: [0, `)
Range: [27, `)
(b) ( f + g)(x) 5 Ïxw 2 7
[23, 20] by [24, 4]
Domain: [7, `)
Range: [0, `)
y3 5 ( f + g)(x) 5 y1(y2(x)),
and y4 5 (g + f )(x) 5 y2(y1(x)).
Use a “decimal window” such as the one shown.
f + g:
(g + f )(x) 5 Ïxw2
ww7
52. (a) Enter y1 5 f(x) 5 1 2 x 2, y2 5 g(x) 5 Ïxw,
y3 5 ( f + g)(x) 5 y1(y2(x)),
and y4 5 (g + f )(x) 5 y2(y1(x))
f + g:
[29.4, 9.4] by [26.2, 6.2]
Domain: (2`, 2) < (2, `)
Range: (2`, 2) < (2, `)
g + f:
[26, 6] by [24, 4]
Domain: [0, `)
Range: (2`, 1]
g + f:
[29.4, 9.4] by [26.2, 6.2]
Domain: (2`, 23) < (23, `)
Range: (2`, 23) < (23, `)
[22.35, 2.35] by [21, 2.1]
Domain: [21, 1]
Range: [0, 1]
(b) ( f + g)(x) 5 1 2 (Ïxw)2 5 1 2 x, x $ 0
(g + f )(x) 5 Ïw1w
2wx2w
53. (a) Enter y1 5 f(x) 5 x 2 2 3, y2 5 g(x) 5 Ïxw1
ww2,
y3 5 ( f + g)(x) 5 y1(y2(x)),
and y4 5 (g + f)(x) 5 y2(y1(x)).
f + g:
1
3x 1 1
2
2 }} 2 1
22x
(b) ( f + g)(x) 5 }}
3x 1 1
}} 1 3
22x
2(3x 1 1) 2 (2 2 x)
(3x 1 1) 1 3(2 2 x)
5 }}}, x Þ 2
7x
7
5 }}, x Þ 2
5 x, x Þ 2
1
2x 2 1
2
3 }} 1 1
x13
(g + f )(x) 5 }}
2x 2 1
2 2 }}
x13
3(2x 2 1) 1 (x 1 3)
5 }}}, x Þ 23
2(x 1 3) 2 (2x 2 1)
7x
7
[210, 10] by [210, 10]
5 }}, x Þ 23
Domain: [22, `)
Range: [23, `)
5 x, x Þ 23
Section 1.2
55.
11
58.
[25, 5] by [22, 5]
[22.35, 2.35] by [21.55, 1.55]
We require x 2 2 4 $ 0 (so that the square root is defined)
We require x 2 2 1 Þ 0, so the domain is
and x 2 2 4 Þ 0 (to avoid division by zero), so the domain
(2`, 21) < (21, 1) < (1, `). For values of x in the
is (2`, 22) < (2, `). For values of x in the domain, x2 2 4
domain, x 2 2 1 can attain any value in [21, 0) < (0, `), so
}2 can attain any positive
1and hence Ïwx2w2w4 and }
2w4
Ïw
xw
Ïw
x 2w
2w1 can also attain any value in [21, 0) < (0, `).
1
2
value, so the range is (0, `). (Note that grapher failure may
3
1
cause the range to appear as a finite interval on a
Therefore, }
3 } can attain any value in
Ïxw2
ww1
(2`, 21] < (0, `). The range is (2`, 21] < (0, `).
grapher.
(Note that grapher failure can cause the intervals in the
56.
range to appear as finite intervals on a grapher.)
59. (a)
y
1.5
[25, 5] by [22, 5]
We require 9 2 x 2 $ 0 (so that the fourth root is defined)
–2
0
2
x
and 9 2 x 2 Þ 0 (to avoid division by zero), so the domain
–1.5
is (23, 3). For values of x in the domain, 9 2 x 2 can attain
4
any value in (0, 9]. Therefore, Ï9ww
2wx 2w can attain any
(b)
y
2
value in (0, Ïw3], and }
} can attain any value in
4
2wx 2w
Ïw9w
3
2
3
1.5
2
2
2
}}, ` . The range is }}, ` or approximately [1.15, `).
Ïw3
Ï3w
–2
(Note that grapher failure may cause the range to appear as
0
a finite interval on a grapher.)
2
x
–1.5
57.
60. (a)
y
2
[24.7, 4.7] by [23.1, 3.1]
We require 9 2 x 2 Þ 0, so the domain is
–2
–1
1
(2`, 23) < (23, 3) < (3, `). For values of x in the
–1
domain, 9 2 x 2 can attain any value in
–2
3
(2`, 0) < (0, 9], so Ï9ww
2wx 2w can attain any value in
3
2
(2`, 0) < (0, Ï9w]. Therefore, }
} can attain any
3
2wx 2w
Ï9ww
2
value in (2`, 0) < }3 }, ` . The range is
Ïw9
2
(2`, 0) < }3 }, ` or approximately (2`, 0) < [0.96, `).
Ïw9
(Note that grapher failure can cause the intervals in the
3
3
2
2
range to appear as finite intervals on a grapher.)
2
x
12
Section 1.2
60. continued
(b)
(d) Since ( f + g)(x) 5 f (Ïxw) 5 )x), f(x) 5 x 2.
The completed table is shown. Note that the absolute
value sign in part (d) is optional.
y
2
1
–2
–1
1
2
g(x)
f (x)
( f + g)(x)
x2
Ïxw2
ww5
Ïw
x 2w
2w5
1
}}
x21
1 1 }}
x, x Þ 21
1
}}
x
1
}}
x
x, x Þ 0
Ïxw
x2
)x), x $ 0
x
1
x
–2
61. (a)
y
1.3
–2
–1
1
2
x
64. (a) Note that the data in the table begins at x 5 20. (We do
not include the initial investment in the data.) The
power regression equation is y 5 27.1094x 2.651044.
(b)
–1.3
(b)
y
[0, 30] by [220,000, 180,000]
1.3
–2
–1
1
2
x
(d) The linear regression equation is
y 5 12,577.97x 2 177,275.52. When
x 5 30, y < 200,064. According to the linear regression
equation, the investment will grow to approximately
$200,064.
–1.3
62. (a)
(c) When x 5 30, y < 223,374. According to the power
regression equation, the investment will grow to
approximately $223,374.
y
65. (a) Because the circumference of the original circle was
8p and a piece of length x was removed.
1.3
8p 2 x
2p
x
2p
(b) r 5 }} 5 4 2 }}
–2
0
2
x
(c) h 5 Ï1w6ww
2wr2w
(b)
!1§6§§2§14§§2§}2§p}§2
4x
x
5 16 2 116 2 }} 1 }}2
!§§§§§§§§p§§§4§p§
4x
x
5 }} 2 }}
!§p§§§4§p§
16px
x
5 }} 2 }}
!§4§p§§§§4§p§
x 2
5
–1.3
2
y
2
1.3
2
2
2
–2
0
2
x
2
2
Ï1w6wp
wxw2
wwx 2w
5 }}
2p
–1.3
63. (a) Since ( f + g)(x) 5 Ïgw(x
w)w2
ww5 5 Ïw
x2w
2w
5, g(x) 5 x 2.
1
g(x)
1
1
}} 5 x 2 1, so g(x) 5 }}.
g(x)
x21
1
1
(c) Since ( f + g)(x) 5 f }} 5 x, f (x) 5 }}.
x
x
(b) Since ( f + g)(x) 5 1 1 }} 5 x, we know that
12
1
3
1 8p 2 x 2 Ïw
1w
6w
pxww
2wx 2w
5 }}p }} ? }}
3
2p
2p
(8p 2 x)2Ï1
w6wp
wxw2
wwx 2w
5 }}}
2
24p
(d) V 5 }}pr 2h
1
2
Section 1.3
66. (a) Note that 2 mi 5 10,560 ft, so there are Ï8w0w0w2w1
wwx2w
feet of river cable at $180 per foot and (10,560 2 x)
feet of land cable at $100 per foot. The cost is
C(x) 5 180Ïw8w0w02ww
1wx2w 1 100(10,560 2 x)
(b)
C(0) 5 $1,200,000
C(500) < $1,175,812
C(1000) < $1,186,512
C(1500) 5 $1,212,000
C(2000) < $1,243,732
C(2500) < $1,278,479
C(3000) < $1,314,870
Values beyond this are all larger. It would appear that
the least expensive location is less than 2000 ft from
point P.
13
5.
[25, 5] by [22, 5]
6. 22x , 32x , 52x for x , 0; 22x . 32x . 52x for x . 0;
22x 5 32x 5 52x for x 5 0.
Quick Review 1.3
1. Using a calculator, 52/3 < 2.924.
2. Using a calculator, 3Ï2w < 4.729.
3. Using a calculator, 321.5 < 0.192.
4. x 3 5 17
3
x 5 Ï1w7w
x < 2.5713
67. (a)
[23, 3] by [21, 3]
(b) Domain of y1: [0, `)
Domain of y2: (2`, 1]
Domain of y3: [0, 1]
(c) The functions y1 2 y2, y2 2 y1, and y1 ? y2 all have
domain [0, 1], the same as the domain of y1 1 y2 found
in part (b).
y
Domain of }}1 : [0, 1)
y2
y
Domain of }}2 : (0, 1]
y1
5. x5 5 24
5
x 5 Ï2w4w
x < 1.8882
6. x10 5 1.4567
10
x 5 6Ï1w.4
w5w6w7w
x < 61.0383
7. 500(1.0475)5 < $630.58
8. 1000(1.063)3 < $1201.16
(x23y2)2
(x y )
5 x26212y429
(d) The domain of a sum, difference, or product of two
functions is the intersection of their domains.
The domain of a quotient of two functions is the
intersection of their domains with any zeros of the
denominator removed.
68. (a) Yes. Since
( f ? g)(2x) 5 f (2x) ? g(2x) 5 f (x) ? g(x) 5 ( f ? g)(x),
the function ( f ? g)(x) will also be even.
(b) The product will be even, since
( f ? g)(2x) 5 f (2x) ? g(2x)
5 (2f (x)) ? (2g(x))
5 f (x) ? g(x)
5 ( f ? g)(x).
■ Section 1.3 Exponential Functions
5 x218y25
1
x y
5}
18}
5
1
a3b22 2 a4c22 21 a6b24
b3
5 }}
}}
}
?
3
8
4}
c
b
c
a c22
b3c2
a6
5 }4}8 ? }}
a4
bc
10. }}
4
21
2
5 a 624b2413c2812
a2
bc
5 a 2b21c26 5 }}6
Section 1.3 Exercises
1. The graph of y 5 2x is increasing from left to right and has
the negative x-axis as an asymptote. (a)
1 x
132
2. The graph of y 5 32x or, equivalently, y 5 }} , is
(pp. 20–26)
Exploration 1
x26y4
x y
9. }
4}
12}
3 3 5}
9
Exponential Functions
1.
decreasing from left to right and has the positive x-axis as
an asymptote. (d)
3. The graph of y 5 232x is the reflection about the x-axis of
the graph in Exercise 2. (e)
[25, 5] by [22, 5]
2. x . 0
3. x , 0
4. x 5 0
4. The graph of y 5 20.52x or, equivalently, y 5 22x, is the
reflection about the x-axis of the graph in Exercise 1. (c)
5. The graph of y 5 22x 2 2 is decreasing from left to right
and has the line y 5 22 as an asymptote. (b)
6. The graph of y 5 1.5x 2 2 is increasing from left to right
and has the line y 5 22 as an asymptote. (f)
14
Section 1.3
7.
16.
[24, 4] by [28, 6]
Domain: (2`, `)
Range: (2`, 3)
x-intercept: < 1.585
y-intercept: 2
[26, 6] by [22, 6]
x < 1.3863
17.
8.
[26, 6] by [23, 5]
x < 20.6309
[24, 4] by [22, 10]
18.
Domain: (2`, `)
Range: (3, `)
x-intercept: None
y-intercept: 4
[26, 6] by [23, 5]
9.
x < 21.5850
19.
x
Dy
y
1 21
2
[24, 4] by [24, 8]
Domain: (2`, `)
Range: (22, `)
x-intercept: < 0.405
y-intercept: 1
2
1
3
3
4
5
2
2
10.
20.
x
Dy
y
1
1
23
[24, 4] by [28, 4]
Domain: (2`, `)
Range: (2`, 21)
x-intercept: None
y-intercept: 22
11. 9 5 (3 ) 5 3
2x
2 2x
2
23
3
1 2x
182
25
23
4x
4
12. 163x 5 (24)3x 5 212x
13. }}
22
5 (223)2x 5 226x
1 x
27
1 2
21.
x
1
28
Dy
y
1
14. }} 5 (323)x 5 323x
15.
3
2
4
5
3
9
7
4
[26, 6] by [22, 6]
x < 2.3219
16
Section 1.3
22.
x
1
ratio
y
8.155
31. Let A be the amount of the initial investment, and let t be
the number of years. We wish to solve
2.718
2
22.167
3
60.257
4
1
2.718
t < 19.108. It will take about 19.108 years.
24. (a) The population is given by P(t) 5 6250(1.0275)t, where
t is the number of years after 1890.
Population in 1915: P(25) < 12,315
Population in 1940: P(50) < 24,265
(b) Solving P(t) 5 50,000 graphically, we find that
t < 76.651. The population reached 50,000 about
77 years after 1890, in 1967.
1 t/14
122
25. (a) A(t) 5 6.6 }}
(b) Solving A(t) 5 1 graphically, we find that t < 38.1145.
There will be 1 gram remaining after about 38.1145
days.
26. Let t be the number of years. Solving 2300(1.06)t 5 4150
graphically, we find that t < 10.129. It will take about
10.129 years. (If the interest is not credited to the account
until the end of each year, it will take 11 years.)
27. Let A be the amount of the initial investment, and let t be
the number of years. We wish to solve A(1.0625)t 5 2A,
which is equivalent to 1.0625t 5 2. Solving graphically, we
find that t < 11.433. It will take about 11.433 years. (If the
interest is credited at the end of each year, it will take 12
years.)
28. Let A be the amount of the initial investment, and let t be
the number of years. We wish to solve
1
2
2.718
23. Let t be the number of years. Solving
500,000(1.0375)t 5 1,000,000 graphically, we find that
t < 18.828. The population will reach 1 million in about
19 years.
0.0625 12t
5 2A, which is equivalent to
12
12t
0.0625
1 1 }}
5 2. Solving graphically, we find that
12
1
0.0575 365t
5 3A, which is equivalent to
365
0.0575 365t
1 1 }}
5 3. Solving graphically, we find that
365
1
A 1 1 }}
163.794
A 1 1 }}
15
2
32. Let A be the amount of the initial investment, and let t be
the number of years. We wish to solve Ae 0.0575t 5 3A,
which is equivalent to e 0.0575t 5 3. Solving graphically, we
find that t < 19.106. It will take about 19.106 years.
33. After t hours, the population is P(t) 5 2 t/0.5 or, equivalently,
P(t) 5 22t. After 24 hours, the population is
P(24) 5 2 48 < 2.815 3 1014 bacteria.
34. (a) Each year, the number of cases is 100% 2 20% 5 80%
of the previous year’s number of cases. After t years,
the number of cases will be C(t) 5 10,000(0.8)t.
Solving C(t) 5 1000 graphically, we find that
t < 10.319. It will take about 10.319 years.
(b) Solving C(t) 5 1 graphically, we find that t < 41.275.
It will take about 41.275 years.
35. Since Dx 5 1, the corresponding value of Dy is equal to the
slope of the line. If the changes in x are constant for a linear function, then the corresponding changes in y are constant as well.
36. (a) When t 5 0, B 5 100e0 5 100. There were 100
bacteria present initially.
(b) When t 5 6, B 5 100e 0.693(6) < 6394.351.
After 6 hours, there are about 6394 bacteria.
(c) Solving 100e 0.693t 5 200 graphically, we find that
t < 1.000. The population will be 200 after about
1 hour. Since the population doubles (from 100 to 200)
in about 1 hour, the doubling time is about 1 hour.
37. (a) Let x 5 0 represent 1900, x 5 1 represent 1901, and so
on. The regression equation is P(x) 5 6.033(1.030)x.
2
2
t < 11.119. It will take about 11.119 years. (If the interest
is credited at the end of each month, it will take 11 years 2
months.)
29. Let A be the amount of the initial investment, and let t be
the number of years. We wish to solve Ae 0.0625t 5 2A,
which is equivalent to e 0.0625t 5 2. Solving graphically, we
find that t < 11.090. It will take about 11.090 years.
30. Let A be the amount of the initial investment, and let t be
the number of years. We wish to solve A(1.0575) t 5 3A,
which is equivalent to 1.0575t 5 3. Solving graphically, we
find that t < 19.650. It will take about 19.650 years. (If the
interest is credited at the end of each year, it will take 20
years.)
[0, 100] by [210, 90]
(b) The regression equation gives an estimate of
P(0) < 6.03 million, which is not very close to the
actual population.
(c) Since the equation is of the form P(x) 5 P(0) ? 1.030x,
the annual rate of growth is about 3%.
38. (a) The regression equation is P(x) 5 4.831(1.019)x.
[0, 100] by [25, 30]
(b) P(90) < 26.3 million
(c) Since the equation is of the form P(x) 5 P(0) ? 1.019x,
the annual rate of growth is approximately 1.9%.
16
Section 1.4
■ Section 1.4 Parametric Equations
(pp. 26–31)
39. 5422(1.018)19 < 7609.7 million
40. (a)
Exploration 1
Parametrizing Circles
1. Each is a circle with radius )a). As )a) increases, the radius
of the circle increases.
[25, 5] by [22, 10]
In this window, it appears they cross twice, although a
third crossing off-screen appears likely.
(b)
x
change in Y1
change in Y2
[24.7, 4.7] by [23.1, 3.1]
1
3
2
5
4
7
8
p
2
2. 0 # t # }}:
2
3
4
[24.7, 4.7] by [23.1, 3.1]
0 # t # p:
It happens by the time x 5 4.
(c) Solving graphically, x < 20.7667, x 5 2, x 5 4.
(d) The solution set is approximately
(20.7667, 2) < (4, `).
41. Since f (1) 5 4.5 we have ka 5 4.5, and since f (21) 5 0.5
we have ka21 5 0.5.
Dividing, we have
[24.7, 4.7] by [23.1, 3.1]
3p
0 # t # }}:
2
4.5
ka
}21
} 5 }}
0.5
ka
a2 5 9
[24.7, 4.7] by [23.1, 3.1]
2p # t # 4p:
a 5 63
Since f (x) 5 k ? a x is an exponential function, we require
a . 0, so a 5 3. Then ka 5 4.5 gives 3k 5 4.5, so k 5 1.5.
The values are a 5 3 and k 5 1.5.
42. Since f (1) 5 1.5 we have ka 5 1.5, and since f (21) 5 6
we have ka21 5 6. Dividing, we have
[24.7, 4.7] by [23.1, 3.1]
0 # t # 4p:
1.5
ka
}21
} 5 }}
6
ka
a2 5 0.25
a 5 60.5
Since f (x) 5 k ? a x is an exponential function, we require
a . 0, so a 5 0.5. Then ka 5 1.5 gives 0.5k 5 1.5, so
k 5 3. The values are a 5 0.5 and k 5 3.
[24.7, 4.7] by [23.1, 3.1]
Let d be the length of the parametric interval. If d , 2p,
d
2p
you get }} of a complete circle. If d 5 2p, you get the
complete circle. If d . 2p, you get the complete circle but
portions of the circle will be traced out more than once. For
example, if d 5 4p the entire circle is traced twice.
Section 1.4
Exploration 2
3.
Parametrizing Ellipses
1. a 5 2, b 5 3:
p
3p
}} # t # }}
2
2
[212, 12] by [28, 8]
initial point: (0, 3)
terminal point: (0, 23)
a 5 2, b 5 4:
[212, 12] by [28, 8]
p # t # 2p
initial point: (23, 0)
terminal point: (3, 0)
a 5 2, b 5 5:
[212, 12] by [28, 8]
a 5 2, b 5 6:
3p
}} # t # 3p
2
initial point: (0, 23)
terminal point: (23, 0)
p # t # 5p
initial point: (23, 0)
terminal point: (23, 0)
4. For 0 # t # 2p the complete circle is traced once clockwise beginning and ending at (2, 0).
For p # t # 3p the complete circle is traced once clockwise beginning and ending at (22, 0).
p
2
3p
2
[212, 12] by [28, 8]
2. a 5 3, b 5 4:
[29, 9] by [26, 6]
a 5 5, b 5 4:
[29, 9] by [26, 6]
a 5 6, b 5 4:
For }} # t # }} the half circle below is traced clockwise
starting at (0, 22) and ending at (0, 2).
[29, 9] by [26, 6]
a 5 7, b 5 4:
[29, 9] by [26, 6]
3. If )a) . )b), then the major axis is on the x-axis and the
minor on the y-axis. If )a) , )b), then the major axis is on
the y-axis and the minor on the x-axis.
17
18
Section 1.4
p
2
Exploration 3
4. 0 # t # }}:
Graphing the Witch of Agnesi
1. We used the parameter interval [0, p] because our graphing
calculator ignored the fact that the curve is not defined
when t 5 0 or p. The curve is traced from right to left
across the screen. x ranges from 2` to `.
[26, 6] by [24, 4]
0 # t # p:
p
2
p
2
2. 2}} # t # }}:
[25, 5] by [22, 4]
[26, 6] by [24, 4]
p
2
0 , t # }}:
3p
2
0 # t # }}:
[25, 5] by [22, 4]
[26, 6] by [24, 4]
p
}} # t , p:
2
0 # t # 4p:
[26, 6] by [24, 4]
Let d be the length of the parametric interval. If d , 2p,
d
2p
you get }} of a complete ellipse. If d 5 2p, you get the
complete ellipse. If d . 2p, you get the complete ellipse
but portions of the ellipse will be traced out more than
once. For example, if d 5 4p the entire ellipse is traced
twice.
5. 0 # t # 2p:
[25, 5] by [22, 4]
p
2
p
2
For 2}} # t # }}, the entire graph described in part 1 is
drawn. The left branch is drawn from right to left across the
screen starting at the point (0, 2). Then the right branch is
drawn from right to left across the screen stopping at the
p
2
p
2
point (0, 2). If you leave out 2}} and }}, then the point
(0, 2) is not drawn.
[26, 6] by [24, 4]
initial point: (5, 0)
terminal point: (5, 0)
p
2
For 0 , t # }}, the right branch is drawn from right to left
across the screen stopping at the point (0, 2). If you leave
p
2
out }}, then the point (0, 2) is not drawn.
p # t # 3p:
p
2
For }} # t , p, the left branch is drawn from right to left
across the screen starting at the point (0, 2). If you leave
[26, 6] by [24, 4]
p
3p
}} # t # }}:
2
2
initial point: (25, 0)
terminal point: (25, 0)
[26, 6] by [24, 4]
initial point: (0, 22)
terminal point: (0, 2)
Each curve is traced clockwise from the initial point to the
terminal point.
p
2
out }}, then the point (0, 2) is not drawn.
3. If you replace x 5 2 cot t by x 5 22 cot t, the same graph
is drawn except it is traced from left to right across the
screen. If you replace x 5 2 cot t by x 5 2 cot (p 2 t), the
same graph is drawn except it is traced from left to right
across the screen.
Quick Review 1.4
328
25
421
3
5
y 5 2}}(x 2 1) 1 8
3
5
29
y 5 2}}x 1 }}
3
3
5
3
1. m 5 }} 5 }} 5 2}}
19
Section 1.4
2. y 5 24
Section 1.4 Exercises
1. Graph (c). Window: [24, 4] by [23, 3], 0 # t # 2p
3. x 5 2
2. Graph (a). Window: [22, 2] by [22, 2], 0 # t # 2p
2
x
9
4. When y 5 0, we have }} 5 1, so the x-intercepts are 23
3. Graph (d). Window: [210, 10] by [210, 10], 0 # t # 2p
y2
16
and 3. When x 5 0, we have }} 5 1, so the y-intercepts are
4. Graph (b). Window: [215, 15] by [215, 15], 0 # t # 2p
24 and 4.
5. (a) The resulting graph appears to be the right half of a
hyperbola in the first and fourth quadrants. The
parameter a determines the x-intercept. The parameter
b determines the shape of the hyperbola. If b is smaller,
the graph has less steep slopes and appears “sharper.” If
b is larger, the slopes are steeper and the graph appears
more “blunt.” The graphs for a 5 2 and b 5 1, 2, and 3
are shown.
x2
16
5. When y 5 0, we have }} 5 1, so the x-intercepts are 24
y2
9
and 4. When x 5 0, we have 2}} 5 1, which has no real
solution, so there are no y-intercepts.
6. When y 5 0, we have 0 5 x 1 1, so the x-intercept is 21.
1
When x 5 0, we have 2y2 5 1, so the y-intercepts are 2}}
Ïw2
1
and }}.
Ïw2
7. (a) 2(1)2(1) + 12 0 3
3 5 3 Yes
(b) 2(21)2(21) 1 (21)2 0 3
22 1 1 0 3
21 Þ 3
(c)
(b)
No
[210, 10] by [210, 10]
1 2
122
2 }} (22) 1 (22)2 0 3
This appears to be the left half of the same hyberbola.
21 1 4 0 3
353
(c)
Yes
8. (a) 9(1)2 2 18(1) 1 4(3)2 5 27
9 2 18 1 36 0 27
27 5 27 Yes
[210, 10] by [210, 10]
(b) 9(1) 2 18(1) 1 4(23) 0 27
9 2 18 1 36 0 27
27 5 27 Yes
2
(c)
[210, 10] by [210, 10]
2
9(21)2 2 18(21) 1 4(3)2 0 27
9 1 18 1 36 0 27
63 Þ 27
No
9. (a) 2x 1 3t 5 25
3t 5 22x 2 5
22x 2 5
3
t 5 }}
(b) 3y 2 2t 5 21
22t 5 23y 2 1
2t 5 3y 1 1
3y 1 1
t 5 }}
2
10. (a) The equation is true for a $ 0.
(b) The equation is equivalent to “Ïaw2w 5 a or
Ïwa2w 5 2a.” Since Ïaw2w 5 a is true for a $ 0 and
Ïwa2w 5 2a is true for a # 0, at least one of the two
equations is true for all real values of a. Therefore, the
given equation Ïwa2w 5 6a is true for all real values
of a.
(c) The equation is true for all real values of a.
One must be careful because both sec t and tan t are
discontinuous at these points. This might cause the
grapher to include extraneous lines (the asymptotes of
the hyperbola) in its graph. The extraneous lines can be
avoided by using the grapher’s dot mode instead of
connected mode.
(d) Note that sec2 t 2 tan2 t 5 1 by a standard
x
a
y
b
trigonometric identity. Substituting }} for sec t and }} for
x 2
y 2
1 a 2 2 1}b}2
tan t gives }}
5 1.
(e) This changes the orientation of the hyperbola. In this
case, b determines the y-intercept of the hyperbola, and
a determines the shape. The parameter interval
p p
12}2}, }2}2 gives the upper half of the hyperbola. The
p 3p
parameter interval 1}}, }}2 gives the lower half. The
2 2
same values of t cause discontinuities and may add
y
b
extraneous lines to the graph. Substituting }} for sec t
x
a
and }} for tan t in the identity sec2 t 2 tan2 t 5 1 gives
y 2
x 2
1}b}2 2 1}a}2
5 1.
20
Section 1.4
6. (a)
10. (a)
[26, 6] by [24, 4]
[24.7, 4.7] by [23.1, 3.1]
The graph is a circle of radius 2 centered at (h, 0). As h
changes, the graph shifts horizontally.
Initial and terminal point: (4, 0)
x 2
y 2
1 4 2 1 1}2}2
(b) }}
(b)
5 cos2 t 1 sin2 t 5 1
The parametrized curve traces all of the ellipse defined
x 2
y 2
1 4 2 1 1}2}2
by }}
5 1.
11. (a)
[26, 6] by [24, 4]
The graph is a circle of radius 2 centered at (0, k). At k
changes, the graph shifts vertically.
(c) Since the circle is to be centered at (2, 23), we use
h 5 2 and k 5 23. Since a radius of 5 is desired, we
need to change the coefficients of cos t and sin t to 5.
x 5 5 cos t 1 2, y 5 5 sin t 2 3, 0 # t # 2p
[24.7, 4.7] by [23.1, 3.1]
Initial point: (0, 2)
Terminal point: (0, 22)
(d) x 5 5 cos t 2 3, y 5 2 sin t 1 4, 0 # t # 2p
x 2
y 2
1 4 2 1 1}2}2
7. (a)
(b) }}
5 sin2 t 1 cos2 t 5 1
The parametrized curve traces the right half of the
x 2
y 2
1 4 2 1 1}2}2
ellipse defined by }}
5 1 (or all of the curve
defined by x 5 2Ï4ww
2wy2w).
[23, 3] by [22, 2]
Initial point: (1, 0)
Terminal point: (21, 0)
12. (a)
(b) x 2 1 y 2 5 cos2 t 1 sin 2 t 5 1
The parametrized curve traces the upper half of the
circle defined by x 2 1 y 2 5 1 (or all of the semicircle
defined by y 5 Ïw1w
2wx 2w).
[29, 9] by [26, 6]
8. (a)
Initial and terminal point: (0, 5)
x 2
y 2
1 4 2 1 1}5}2
(b) }}
5 sin2 t 1 cos2 t 5 1
The parametrized curve traces all of the ellipse defined
x 2
by }}
Initial and terminal point: (0, 1)
(b) x 2 1 y 2 5 sin2 (2pt) 1 cos2 (2pt) 5 1
The parametrized curve traces all of the circle defined
by x 2 1 y 2 5 1.
y 2
1 4 2 1 1}5}2
[23, 3] by [22, 2]
5 1.
13. (a)
9. (a)
[23, 3] by [21, 3]
No initial or terminal point.
(b) y 5 9t 2 5 (3t)2 5 x 2
The parametrized curve traces all of the parabola
defined by y 5 x 2.
[23, 3] by [22, 2]
Initial point: (21, 0)
Terminal point: (0, 1)
14. (a)
(b) x 1 y 5 cos (p 2 t) 1 sin (p 2 t) 5 1
The parametrized curve traces the upper half of the
circle defined by x 2 1 y 2 5 1 (or all of the semicircle
defined by y 5 Ïw1w
2wx2w).
2
2
2
2
[23, 3] by [21, 3]
Initial point: (0, 0)
Terminal point: None
Section 1.4
(b) y 5 t 5 (2Ïtw)2 5 x 2
The parametrized curve traces the left half of the
parabola defined by y 5 x 2 (or all of the curve defined
by x 5 2Ïwy).
21
19. (a)
15. (a)
[29, 9] by [26, 6]
No initial or terminal point.
(b) y 5 4t 2 7 5 2(2t 2 5) 1 3 5 2x 1 3
The parametrized curve traces all of the line defined by
y 5 2x 1 3.
[21, 5] by [21, 3]
Initial point: (0, 0)
Terminal point: None
20. (a)
(b) y 5 Ïtw 5 Ïxw
The parametrized curve traces all of the curve defined
by y 5 Ïwx (or the upper half of the parabola defined
by x 5 y 2).
[26, 6] by [24, 4]
16. (a)
No initial or terminal point.
(b) y 5 1 1 t 5 2 2 (1 2 t) 5 2 2 x 5 2x 1 2
The parametrized curve traces all of the line defined by
y 5 2x 1 2.
21. (a)
[23, 9] by [24, 4]
No initial or terminal point.
(b) x 5 sec2 t 2 1 5 tan2 t 5 y 2
The parametrized curve traces all of the parabola
defined by x 5 y 2.
[23, 3] by [22, 2]
17. (a)
Initial point: (0, 1)
Terminal point: (1, 0)
(b) y 5 1 2 t 5 1 2 x 5 2x 1 1
The Cartesian equation is y 5 2x 1 1. The portion
traced by the parametrized curve is the segment from
(0, 1) to (1, 0).
[23, 3] by [22, 2]
No initial or terminal point. Note that it may be
necessary to use a t-interval such as [21.57, 1.57] or
use dot mode in order to avoid “asymptotes” showing
on the calculator screen.
22. (a)
(b) x 2 2 y 2 5 sec2 t 2 tan2 t 5 1
The parametrized curve traces the left branch of the
hyperbola defined by x 2 2 y 2 5 1 (or all of the curve
defined by x 5 2Ïw
y2w
1w
1).
[22, 4] by [21, 3]
Initial point: (3, 0)
Terminal point: (0, 2)
2
3
18. (a)
2
3
(b) y 5 2t 5 (2t 2 2) 1 2 5 2}}(3 2 3t) 1 2 5 2}}x 1 2
2
3
The Cartesian equation is y 5 2}}x 1 2. The portion
traced by the curve is the segment from (3, 0) to (0, 2).
[26, 6] by [25, 1]
23. (a)
No initial or terminal point. Note that it may be
necessary to use a t-interval such as [21.57, 1.57] or
use dot mode in order to avoid “asymptotes” showing
on the calculator screen.
y 2
122
(b) }}
2 x 2 5 sec2 t 2 tan2 t 5 1
The parametrized curve traces the lower branch of the
y 2
122
hyperbola defined by }}
2 x 2 5 1 (or all of the curve
defined by y 5 22Ïw
x2w
1w
1).
[26, 6] by [22, 6]
Initial point: (4, 0)
Terminal point: None
(b) y 5 Ïtw 5 4 2 (4 2 Ïtw) 5 4 2 x 5 2x 1 4
The parametrized curve traces the portion of the line
defined by y 5 2x 1 4 to the left of (4, 0), that is, for
x # 4.
22
Section 1.4
30. The vertex of the parabola is at (21, 21), so the left half of
the parabola is given by y 5 x 2 1 2x for x # 21.
Substituting t for x, we obtain one possible parametrization:
x 5 t, y 5 t 2 1 2t, t # 21.
24. (a)
[21, 5] by [21, 3]
Initial point: (0, 2)
Terminal point: (4, 0)
2wt2w 5 Ï4ww
2wx
(b) y 5 Ï4ww
The parametrized curve traces the right portion of the
curve defined by y 5 Ïw4w
2wx, that is, for x $ 0.
25. (a)
31. For simplicity, we assume that x and y are linear functions
of t and that the point (x, y) starts at (2, 3) for t 5 0 and
passes through (21, 21) at t 5 1. Then x 5 f(t), where
f(0) 5 2 and f(1) 5 21.
Dx
Dt
21 2 2
120
Since slope 5 }} 5 }} 5 23,
x 5 f(t) 5 23t 1 2 5 2 2 3t. Also, y 5 g(t), where
g(0) 5 3 and g(1) 5 21.
Dy
Dt
21 2 3
120
Since slope 5 }} 5 }} 5 24,
y 5 g(t) 5 24t 1 3 5 3 2 4t.
[23, 3] by [22, 2]
No initial or terminal point, since the t-interval has no
beginning or end. The curve is traced and retraced in
both directions.
(b) y 5 cos 2t
5 cos2 t 2 sin2 t
5 1 2 2 sin2 t
5 1 2 2x 2
5 22x 2 1 1
The parametrized curve traces the portion of the
parabola defined by y 5 22x 2 1 1 corresponding to
21 # x # 1.
One possible parametrization is:
x 5 2 2 3t, y 5 3 2 4t, t $ 0.
32. For simplicity, we assume that x and y are linear functions
of t and that the point (x, y) starts at (21, 2) for t 5 0 and
passes through (0, 0) at t 5 1. Then x 5 f(t), where
f(0) 5 21 and f (1) 5 0.
Dx
Dt
0 2 (21)
120
Since slope 5 }} 5 }} 5 1,
x 5 f (t) 5 1t 1 (21) 5 21 1 t.
Also, y 5 g(t), where g(0) 5 2 and g(1) 5 0.
26. (a)
Dy
Dt
022
120
Since slope 5 }} 5 }} 5 22,
y 5 g(t) 5 22t 1 2 5 2 2 2t.
[24, 5] by [24, 2]
Initial point: None
Terminal point: (23, 0)
(b) x 5 t 2 2 3 5 y 2 2 3
The parametrized curve traces the lower half of the
parabola defined by x 5 y 2 2 3 (or all of the curve
defined by y 5 2Ïw
xw
1w
3).
27. Using (21, 23) we create the parametric equations
x 5 21 1 at and y 5 23 1 bt, representing a line which
goes through (21, 23) at t 5 0. We determine a and b so
that the line goes through (4, 1) when t 5 1.
Since 4 5 21 1 a, a 5 5.
Since 1 5 23 1 b, b 5 4.
Therefore, one possible parametrization is x 5 21 1 5t,
y 5 23 1 4t, 0 # t # 1.
28. Using (21, 3) we create the parametric equations
x 5 21 1 at and y 5 3 1 bt, representing a line which
goes through (21, 3) at t 5 0. We determine a and b so that
the line goes through (3, 22) at t 5 1.
Since 3 5 21 1 a, a 5 4.
Since 22 5 3 1 b, b 5 25.
Therefore, one possible parametrization is x 5 21 1 4t,
y 5 3 2 5t, 0 # t # 1.
29. The lower half of the parabola is given by x 5 y 2 1 1
for y # 0. Substituting t for y, we obtain one possible
parametrization: x 5 t 2 1 1, y 5 t, t # 0.
One possible parametrization is:
x 5 21 1 t, y 5 2 2 2t, t $ 0.
33. The graph is in Quadrant I when 0 , y , 2, which
corresponds to 1 , t , 3. To confirm, note that x(1) 5 2
and x(3) 5 0.
34. The graph is in Quadrant II when 2 , y # 4, which
corresponds to 3 , t # 5. To confirm, note that x(3) 5 0
and x(5) 5 22.
35. The graph is in Quadrant III when 26 # y , 24, which
corresponds to 25 # t , 23. To confirm, note that
x(25) 5 22 and x(23) 5 0.
36. The graph is in Quadrant IV when 24 , y , 0, which
corresponds to 23 , t , 1. To confirm, note that
x(23) 5 0 and x(1) 5 2.
37. The graph of y 5 x 2 1 2x 1 2 lies in Quadrant I for all
x . 0. Substituting t for x, we obtain one possible
parametrization:
x 5 t, y 5 t 2 1 2t 1 2, t . 0.
ww3 lies in Quadrant I for all x $ 0.
38. The graph of y 5 Ïxw1
Substituting t for x, we obtain one possible parametrization:
x 5 t, y 5 Ïw
tw
1w3, t . 0.
Section 1.5
39. Possible answers:
(a) x 5 a cos t, y 5 2a sin t, 0 # t # 2p
(b) x 5 a cos t, y 5 a sin t, 0 # t # 2p
(c) x 5 a cos t, y 5 2a sin t, 0 # t # 4p
(d) x 5 a cos t, y 5 a sin t, 0 # t # 4p
40. Possible answers:
(a) x 5 2a cos t, y 5 b sin t, 0 # t # 2p
23
■ Section 1.5 Functions and Logarithms
(pp. 32–40)
Exploration 1
Testing for Inverses Graphically
1. It appears that ( f + g)(x) 5 (g + f )(x) 5 x, suggesting that f
and g may be inverses of each other.
(a) f and g:
(b) x 5 2a cos t, y 5 2b sin t, 0 # t # 2p
(c) x 5 2a cos t, y 5 b sin t, 0 # t # 4p
(d) x 5 2a cos t, y 5 2b sin t, 0 # t # 4p
41. Note that m/OAQ 5 t, since alternate interior angles
[24.7, 4.7] by [23.1, 3.1]
(b) f + g:
formed by a transversal of parallel lines are congruent.
OQ
AQ
2
x
2
tan t
Therefore, tan t 5 }} 5 }}, so x 5 }} 5 2 cot t.
[24.7, 4.7] by [23.1, 3.1]
Now, by equation (iii), we know that
(c) g + f :
2
(AQ)
AO
AQ
5 }} (AQ)
AO
AB 5 }}
1 2
5 (cos t)(x)
[24.7, 4.7] by [23.1, 3.1]
5 (cos t)(2 cot t)
2. It appears that f + g 5 g + f 5 g, suggesting that f may be the
identity function.
2 cos2 t
sin t
5 }}.
(a) f and g:
Then equation (ii) gives
2 cos2 t
sin t
y 5 2 2 AB sin t 5 2 2 }} ? sin t 5 2 2 2 cos2 t
5 2 sin2 t.
[24.7, 4.7] by [23.1, 3.1]
The parametric equations are:
x 5 2 cot t, y 5 2 sin2 t, 0 , t , p
(b) f + g:
Note: Equation (iii) may not be immediately obvious, but it
may be justified as follows. Sketch segment QB. Then
/OBQ is a right angle, so nABQ , nAQO, which gives
[24.7, 4.7] by [23.1, 3.1]
(c) g + f :
AQ
AB
}} 5 }}.
AO
AQ
42. (a) If x2 5 x1 then the line is a vertical line and the first
parametric equation gives x 5 x1, while the second will
give all real values for y since it cannot be the case that
y2 5 y1 as well.
Otherwise, solving the first equation for t gives
t 5 (x 2 x1)/(x2 2 x1).
Substituting that into the second equation gives
y 5 y1 1 [(y2 2 y1)/(x2 2 x1)](x 2 x1)
which is the point-slope form of the equation for the
line through (x1, y1) and (x2, y2).
Note that the first equation will cause x to take on all
real values, because (x2 2 x1) is not zero. Therefore, all
of the points on the line will be traced out.
[24.7, 4.7] by [23.1, 3.1]
3. It appears that ( f + g)(x) 5 (g + f )(x) 5 x, suggesting that f
and g may be inverses of each other.
(a) f and g:
[24.7, 4.7] by [23.1, 3.1]
(b) f + g:
(b) Use the equations for x and y given in part (a), with
0 # t # 1.
[24.7, 4.7] by [23.1, 3.1]
24
Section 1.5
5. Substituting t for x, one possible answer is:
3. continued
(c) g + f :
1
t21
x 5 t, y 5 }}, t $ 2.
6. Substituting t for x, one possible answer is:
x 5 t, y 5 t, t , 23.
7.
[24.7, 4.7] by [23.1, 3.1]
4. It appears that ( f + g)(x) 5 (g + f )(x) 5 x, suggesting that f
and g may be inverse of each other. (Notice that the domain
of f + g is (0, `) and the domain of g + f is (2`, `).)
(a) f and g:
[210, 10] by [210, 10]
(4, 5)
8.
[24.7, 4.7] by [23.1, 3.1]
(b) f + g:
[210, 10] by [210, 10]
1}3}, 232 < (2.67, 23)
8
9. (a)
[24.7, 4.7] by [23.1, 3.1]
(c) g + f :
[210, 10] by [210, 10]
(1.58, 3)
[24.7, 4.7] by [23.1, 3.1]
Exploration 2
Supporting the Product Rule
1. They appear to be vertical translations of each other.
(b) No points of intersection, since 2x . 0 for all
values of x.
10. (a)
[210, 10] by [210, 10]
[21, 8] by [22, 4]
2. This graph suggests that each difference (y3 5 y1 2 y2) is a
constant.
(21.39, 4)
(b) No points of intersection, since e2x . 0 for all values
of x.
Section 1.5 Exercises
1. No, since (for example) the horizontal line y 5 2 intersects
the graph twice.
[21, 8] by [22, 4]
3. y3 5 y1 2 y2 5 ln (ax) 2 ln x 5 ln a 1 ln x 2 ln x 5 ln a
Thus, the difference y3 5 y1 2 y2 is the constant ln a.
1. ( f + g)(1) 5 f(g(1)) 5 f (2) 5 1
2. (g + f )(27) 5 g( f(27)) 5 g(22) 5 5
3
ww1
ww1)w2
ww1
3. ( f + g)(x) 5 f(g(x)) 5 f (x 1 1) 5 Ï(x
3
5 Ïw
x 2 5 x 2/3
3
4. (g + f )(x) 5 g( f(x)) 5 g(Ïxw2
ww1)
3
ww1)2 1 1
5 (Ïxw2
5 (x 2 1)2/3 1 1
3. Yes, since each horizontal line intersects the graph at most
once.
4. No, since (for example) the horizontal line y 5 0.5
intersects the graph twice.
Quick Review 1.5
2
2. Yes, since each horizontal line intersects the graph only
once.
2
5. Yes, since each horizontal line intersects the graph only
once.
6. No, since (for example) the horizontal line y 5 2 intersects
the graph at more than one point.
Section 1.5
13. y 5 2x 1 3
7.
y 2 3 5 2x
y23
}} 5 x
2
Interchange x and y.
[210, 10] by [210, 10]
Yes, the function is one-to-one since each horizontal line
intersects the graph at most once, so it has an inverse
function.
x23
}} 5 y
2
x23
f 21(x) 5 }}.
2
Verify.
x23
1 2 2
x23
5 21}}2 1 3
2
( f + f 21)(x) 5 f }}
8.
5 (x 2 3) 1 3
5x
[210, 10] by [210, 10]
No, the function is not one-to-one since (for example) the
horizontal line y 5 0 intersects the graph twice, so it does
not have an inverse function.
( f 21 + f )(x) 5 f 21(2x 1 3)
(2x 1 3) 2 3
2
2x
5 }}
2
5 }}
5x
9.
14. y 5 5 2 4x
4x 5 5 2 y
52y
4
x 5 }}
[210, 10] by [210, 10]
No, the function is not one-to-one since (for example) the
horizontal line y 5 5 intersects the graph more than once,
so it does not have an inverse function.
10.
Interchange x and y.
52x
4 52x
(x) 5 }}
4
y 5 }}
f
21
Verify.
1
52x
4
2
1
52x
4
2
( f + f 21)(x) 5 f }} 5 5 2 4 }}
5 5 2 (5 2 x)
5x
(f
21
+ f )(x) 5 f 21(5 2 4x)
5 2 (5 2 4x)
4x 4
5 }}
4
[25, 5] by [220, 20]
5 }}
Yes, the function is one-to-one since each horizontal line
intersects the graph only once, so it has an inverse function.
5x
11.
15. y 5 x 2 1
3
y 1 1 5 x3
(y 1 1)1/3 5 x
[210, 10] by [210, 10]
No, the function is not one-to-one since each horizontal line
intersects the graph twice, so it does not have an inverse
function.
Interchange x and y.
(x 1 1)1/3 5 y
3
ww1
f 21(x) 5 (x 1 1)1/3 or Ïxw1
Verify.
3
ww1)
( f + f 21)(x) 5 f (Ïxw1
12.
3
ww1)3 2 1 5 (x 1 1) 2 1 5 x
5 (Ïxw1
( f 21 + f)(x) 5 f 21(x3 2 1)
3
3
w3w2
ww1)w1
ww1 5 Ïw
x3 5 x
5 Ï(x
[29, 9] by [22, 10]
Yes, the function is one-to-one since each horizontal line
intersects the graph at most once, so it has an inverse
function.
25
26
Section 1.5
For x # 2 (the domain of f),
16. y 5 x 2 1 1, x $ 0
( f 21 + f )(x) 5 f 21(2(x 2 2)2)
y215x ,x$0
2
ww
2w2w
)2
5 2 2 Ï(x
Ïyw2
ww1 5 x
5 2 2 )x 2 2) 5 2 1 (x 2 2) 5 x
Interchange x and y.
Ïxw2
ww1 5 y
ww1 or (x 2 1)1/2
f 21(x) 5 Ïxw2
Verify. For x $ 1 (the domain of f 21),
(f + f
20. y 5 (x 1 2x 1 1), x $ 21
2
21
)(x) 5 f (Ïxw2
ww1)
ww1)2 1 1
5 (Ïxw2
5 (x 2 1) 1 1 5 x
y 5 (x 1 1)2, x $ 21
Ïyw 5 x 1 1
Ïyw 2 1 5 x
Interchange x and y.
Ïxw 2 1 5 y
For x . 0, (the domain of f),
f 21(x) 5 Ïxw 2 1 or x 1/2 2 1
( f 21 + f)(x) 5 f 21(x 2 1 1)
Verify.
w w1
ww1)w2
ww1
5 Ï(x
2
5 Ïw
x 2 5 )x) 5 x
For x $ 0 (the domain of f 21),
( f + f 21)(x) 5 f (Ïxw 2 1)
5 [(Ïxw 2 1)2 1 2(Ïxw 2 1) 1 1]
17. y 5 x 2, x # 0
5 (Ïxw)2 2 2Ïxw 1 1 1 2Ïxw 2 2 1 1
x 5 2Ïyw
5 (Ïxw)2 5 x
Interchange x and y.
For x $ 21 (the domain of f),
y 5 2Ïxw
f
21
(x) 5 2Ïxw or 2x
1/2
(f 21 + f )(x) 5 f 21(x 2 1 2x 1 1)
x2w
1w2xw1
ww1 2 1
5 Ïw
Verify.
ww
1w1w
)2 2 1
5 Ï(x
For x $ 0 (the domain of f 21),
5 )x 1 1) 2 1
( f + f 21)(x) 5 f(2Ïxw) 5 (2Ïxw)2 5 x
For x # 0, (the domain of f ),
x 2 5 2)x) 5 x
( f 21 + f)(x) 5 f 21(x 2) 5 2Ïw
18. y 5 x 2/3, x $ 0
y 3/2 5 (x 2/3)3/2, x $ 0
y 3/2 5 x
f
1
x
1
x 2 5 }}, x . 0
y
1
1
x 5 }} 5 }}
y
Ïwy
21. y 5 }}2 , x . 0
!§
Interchange x and y.
Interchange x and y.
x
5 (x 1 1) 2 1 5 x
3/2
5y
21
(x) 5 x 3/2
Verify.
For x $ 0 (the domain of f 21),
( f + f 21)(x) 5 f (x 3/2) 5 (x 3/2)2/3 5 x
for x $ 0, (the domain of f ),
( f 21 + f )(x) 5 f 21(x2/3) 5 (x 2/3)3/2 5 )x) 5 x
19. y 5 2(x 2 2)2, x # 2
(x 2 2) 5 2y, x # 2
2
wyw
x 2 2 5 2Ï2
x 5 2 2 Ï2
wyw
Interchange x and y.
wxw
y 5 2 2 Ï2
f 21(x) 5 2 2 Ï2
wxw or 2 2 (2x)1/2
Verify.
For x # 0 (the domain of f 21)
wxw)
( f + f 21)(x) 5 f (2 2 Ï2
wxw) 2 2]2
5 2[(2 2 Ï2
5 2(2Ï2
wxw)2 5 2)x) 5 x
1
y 5 }}
Ïwx
1
1
f 21(x) 5 } } or }1}
x /2
Ïwx
Verify.
For x . 0 (the domain of f 21),
1 2
1
1
( f + f 21)(x) 5 f }} 5 }} 5 x
(1/Ïwx)2
Ïwx
For x . 0 (the domain of f),
1 2
1
1
x2 5 )x) 5 x
(f 21 + f)(x) 5 f 21 }}2 5 }} 5 Ïw
x
/x 2w
Ï1ww
1
22. y 5 }}3
x
1
y
3 1
1
x 5 }} 5 }3 }
y
Ïwy
x 3 5 }}
!§
Interchange x and y.
1
y 5 }3 }
Ïwx
1
1
f 21(x) 5 }3 } or }1}
x /3
Ïwx
Verify.
1 2
1 2
1
1
( f + f 21)(x) 5 f }3 } 5 }3} 5 x
(1/Ïxw)3
Ïwx
1
1
( f 21 + f)(x) 5 f 21 }}3 5 }
5x
3 }
x
Ï1w/x
w3w
Section 1.5
2x 1 1
x13
x13
x22
24. y 5 }}
23. y 5 }}
xy 2 2y 5 x 1 3
xy 1 3y 5 2x 1 1
xy 2 x 5 2y 1 3
xy 2 2x 5 1 2 3y
x(y 2 1) 5 2y 1 3
(y 2 2)x 5 1 2 3y
2y 1 3
y21
x 5 }}
1 2 3y
x 5 }}
y22
Interchange x and y.
2x 1 3
x21
y 5 }}
Interchange x and y.
1 2 3x
x22
y 5 }}
2x 1 3
x21
f 21(x) 5 }}
1 2 3x
x22
f 21(x) 5 }}
Verify.
Verify.
2x 1 3
1x21 2
( f + f 21)(x) 5 f }}
1 2 3x
1x22 2
( f + f 21)(x) 5 f }}
1
1 2 3x
5
2
2 }} 1 1
x22
5 }}
1 2 3x
}} 1 3
x22
2(1 2 3x) 1 (x 2 2)
(1 2 3x) 1 3(x 2 2)
5 }}}
25x
25
1x 2 22
( f 21 + f)(x) 5 f 21 }}
x13
1x 2 22
2 }} 1 3
2x 1 1
( f 21 + f)(x) 5 f 21 }}
1
2x 1 1
2
1 2 3 }}
x13
5 }}
2x 1 1
}} 2 2
x13
(x 1 3) 2 3(2x 1 1)
(2x 1 1) 2 2(x 1 3)
5 }}}
25x
25
5 }} 5 x
(2x 1 3) 1 3(x 2 1)
(2x 1 3) 2 2(x 2 1)
5x
5 }} 5 x
5
5 }}}
x13
5 }} 5 x
1 x13 2
2x 1 3
}} 1 3
x21
}}
2x 1 3
}} 2 2
x21
5 }}
x13
}} 2 1
x22
2(x 1 3) 1 3(x 2 2)
(x 1 3) 2 (x 2 2)
5x
5 }} 5 x
5
5 }}}
25. Graph of f: x1 5 t, y1 5 et
Graph of f 21: x2 5 e t, y2 5 t
Graph of y 5 x: x3 5 t, y3 5 t
[26, 6] by [24, 4]
26. Graph of f: x1 5 t, y1 5 3t
Graph of f 21: x2 5 3t, y2 5 t
Graph of y 5 x: x3 5 t, y3 5 t
[26, 6] by [24, 4]
27
28
Section 1.5
27. Graph of f: x1 5 t, y1 5 22t
Graph of f
21
33.
2t
: x2 5 2 , y2 5 t
Graph of y 5 x: x3 5 t, y3 5 t
[210, 5] by [27, 3]
Domain: (`, 3)
Range: (2`, `)
34.
[24.5, 4.5] by [23, 3]
28. Graph of f: x1 5 t, y1 5 32t
Graph of f 21: x2 5 32t, y2 5 t
Graph of y 5 x: x3 5 t, y3 5 t
[25, 10] by [25, 5]
Domain: (22, `)
Range: (2`, `)
35.
[24.5, 4.5] by [23, 3]
29. Graph of f: x1 5 t, y1 5 ln t
Graph of f 21: x2 5 ln t, y2 5 t
[23, 6] by [22, 4]
Graph of y 5 x: x3 5 t, y3 5 t
Domain: (21, `)
Range: (2`, `)
36.
[24.5, 4.5] by [23, 3]
30. Graph of f: x1 5 t, y1 5 log t
Graph of f 21: x2 5 log t, y2 5 t
Graph of y 5 x: x3 5 t, y3 5 t
[22, 10] by [22, 4]
Domain: (4, `)
Range: (2`, `)
37. (1.045)t 5 2
ln(1.045)t 5 ln 2
t ln 1.045 5 ln 2
ln 2
ln 1.045
t 5 }} < 15.75
[24.5, 4.5] by [23, 3]
Graphical support:
21
31. Graph of f: x1 5 t, y1 5 sin
t
Graph of f 21: x2 5 sin21 t, y2 5 t
Graph of y 5 x: x3 5 t, y3 5 t
[22, 18] by [21, 3]
38. e 0.05t 5 3
ln e 0.05t 5 ln 3
[23, 3] by [22, 2]
32. Graph of f: x1 5 t, y1 5 tan21 t
Graph of f
21
21
: x2 5 tan
t, y2 5 t
0.05t 5 ln 3
ln 3
0.05
t 5 }} 5 20 ln 3 < 21.97
Graphical support:
Graph of y 5 x: x3 5 t, y3 5 t
[25, 35] by [21, 4]
[26, 6] by [24, 4]
Section 1.5
39. e x 1 e 2x 5 3
100
112
43. y 5 }}
2x
e x 2 3 1 e 2x 5 0
e x(e x 2 3 1 e 2x) 5 e x(0)
(e x)2 2 3e x 1 1 5 0
3 6 Ï(2
w3ww
)2w
2w4(1
w)(
w1w)w
e 5 }}}
2(1)
3 6 Ïw
5
e x 5 }}
2
3 6 Ïw
5
x 5 ln }} < 20.96 or 0.96
2
x
1
100
y
1 1 22x 5 }}
100
y
22x 5 }} 2 1
1y 2
100
2x 5 log21}} 2 12
y
100
x 5 2log21}} 2 12
y
100 2 y
5 2log21}}2
y
y
5 log21}}2
100 2 y
100
log2(22x) 5 log2 }} 2 1
2
Graphical support:
Interchange x and y.
1 100 2 x 2
x
21
f (x) 5 log21}}2
100 2 x
x
y 5 log2 }}
[24, 4] by [24, 8]
40. 2x 1 22x 5 5
Verify.
1
x
100 2 x
( f + f 21)(x) 5 f log2 }}
2x 2 5 1 22x 5 0
2
2x(2x 2 5 1 22x) 5 2x(0)
(2x)2 2 5(2x) 1 1 5 0
5 6 Ï(2
w5w)w2w
2w
4(1
w)(
w1w)w
2x 5 }}}
100
5 }}
x}
1 1 22log21}
100 2 x 2
2(1)
w1w
5 6 Ï2
2x 5 }}
2
w1w
5 6 Ï2
x 5 log2 }} < 22.26 or 2.26
2
1
2
100
5 }}
100 2 x
1 1 2log21}x}2
Graphical support:
100
5 }}
100 2 x
11}
}
x
100x
100
100x
x 1 (100 2 x)
5 }} 5 }} 5 x
[24, 4] by [24, 8]
41. ln y 5 2t 1 4
e ln y 5 e 2t 1 4
y 5 e 2t 1 4
42. ln(y 2 1) 2 ln 2 5 x 1 ln x
ln(y 2 1) 5 x 1 ln x 1 ln 2
e ln(y21) 5 e x 1 ln x 1 ln 2
y 2 1 5 e x(x)(2)
y 5 2xe x 1 1
11 1 2 2
100
( f 21 + f )(x) 5 f 21 }}
2x
1
100
}}
1 1 22x
5 log2 }}
100
100 2 }
}
2x
112
1 100(1 1 2
2
100
5 log2 }}}
2x
12 2
1
) 2 100
2
5 log2 }2x
} 5 log2(2 x) 5 x
29
30
Section 1.5
2w( w
f (x)
ww
)2
45. (a) f ( f(x)) 5 Ï1ww
50
1 1 1.1
44. y 5 }}
2x
5 Ï1ww
2w(1ww
2wx 2w)
50
1 1 1.1 5 }}
y
50
2x
1.1 5 }} 2 1
y
2x
5 Ïw
x2 5 )x) 5 x, since x $ 0
1
2
50
log1.1(1.1 ) 5 log1.1 }} 2 1
y
50
2x 5 log1.1 }} 2 1
y
50
50 2 y
y
x 5 2log1.1 }} 2 1 5 2log1.1 }} 5 log1.1 }}
y
y
50 2 y
2x
1
1
2
2
1
2
Interchange x and y:
1
x
50 2 x
y 5 log1.1 }}
f
21
1
1
2
1
x
1
1/x
(b) f( f(x)) 5 f 1}}2 5 }} 5 x for all x Þ 0
1 t/12
2
46. (a) Amount 5 81}}2
1 t/12
51
2
1 t/12
1
5 }}
}}
2
8
1 t/12
1 3
5 }}
}}
2
2
t
}} 5 3
12
(b) 81}}2
12
2
x
50 2 x
12
2
(x) 5 log1.1 }}
Verify.
1
12
t 5 36
1 50 2 x 22
x
( f + f 21)(x) 5 f log1.1 }}
There will be 1 gram remaining after 36 hours.
47. 500(1.0475)t 5 1000
50
5 }}}
x}
1 1 1.12log1.11}
50 2 x 2
1.0475t 5 2
ln(1.0475t) 5 ln 2
50
5 }}
50 2 x
1 1 1.1log1.11}x}2
t ln 1.0475 5 ln 2
ln 2
ln 1.0475
t 5 }} < 14.936
It will take about 14.936 years. (If the interest is paid at the
end of each year, it will take 15 years.)
50
5 }}
50 2 x
11}
}
x
48. 375,000(1.0225)t 5 1,000,000
50x
x 1 (50 2 x)
50x
50
5 }} 5 }} 5 x
8
3
1.0225t 5 }}
8
3
8
t ln 1.0225 5 ln }}
3
ln(8/3)
t 5 }} < 44.081
ln 1.0225
ln(1.0225t) 5 ln1}}2
12
50
1 1 1.1
( f 21 + f )(x) 5 f 211}}
2x 2
It will take about 44.081 years.
5
1
50
}}
1 1 1.12x
log1.1 }}
50 2 }50}
1 1 1.12x
2
50
50(1 1 1.1 ) 2 50
5 log1.11}}}
2x
2
49. (a) y 5 22539.852 1 636.896 ln x
(b) When x 5 75, y < 209.94. About 209.94 million metric
tons were produced.
(c) 22539.852 1 636.896 ln x 5 400
636.896 ln x 5 2939.852
2939.852
636.896
ln x 5 }}
1
1.1
x
5 log1.11}}
2x 2 5 log1.1(1.1 ) 5 x
2939.852
}
636.8
96 < 101.08
x 5 e}
According to the regression equation, Saudi Arabian oil
production will reach 400 million metric tons when
x < 101.08, in about 2001.
Section 1.6
50. (a) y 5 2590.969 1 152.817 ln x
(b) When x 5 85, y < 87.94.
About 87.94 million metric tons were produced.
(c) 2590.969 1 152.817 ln x 5 120
ax1 1 b
ax2 1 b
}
}5}
}
cx1 1 d
cx2 1 d
710.969
152.817
ln x 5 }}
x5
(b) The expression a logb(x 2 c) 1 d is defined when
x 2 c . 0, so the domain is (c, `).
Since a logb(x 2 c) 1 d attains every real value for
some value of x, the range is (2`, `).
56. (a) Suppose f (x1) 5 f (x2). Then:
152.817 ln x 5 710.969
710.}
969
152.817
e}
31
< 104.84
According to the regression equation, oil production
will reach 120 million metric tons when x < 104.84, in
about 2005.
51. (a) Suppose that f (x1) 5 f (x2). Then mx1 1 b 5 mx2 1 b
so mx1 5 mx2. Since m Þ 0, this gives x1 5 x2.
(b) y 5 mx 1 b
(ax1 1 b)(cx2 1 d) 5 (ax2 1 b)(cx1 1 d)
acx1x2 1 adx1 1 bcx2 1 bd
5 acx1x2 1 adx2 1 bcx1 1 bd
adx1 1 bcx2 5 adx2 1 bcx1
(ad 2 bc)x1 5 (ad 2 bc)x2
Since ad 2 bc Þ 0, this means that x1 5 x2.
ax 1 b
cx 1 d
(b) y 5 }}
y 2 b 5 mx
y2b
}} 5 x
m
cxy 1 dy 5 ax 1 b
Interchange x and y.
(cy 2 a)x 5 2dy 1 b
x2b
}} 5 y
m
x 5 }}
2dy 1 b
cy 2 a
x2b
m
f 21(x) 5 }}
Interchange x and y:
The slopes are reciprocals.
y 5 }}
(c) If the original functions both have slope m, each of the
1
m
inverse functions will have slope }}. The graphs of the
inverses will be parallel lines with nonzero slope.
1
(d) If the original functions have slopes m and 2}},
m
respectively, then the inverse functions will have slopes
1
1
}} and 2m, respectively. Since each of }} and 2m is
m
m
the negative reciprocal of the other, the graphs of the
inverses will be perpendicular lines with nonzero
slopes.
52. (a) y2 is a vertical shift (upward) of y1, although it’s
difficult to see that near the vertical asymptote at x 5 0.
One might use “trace” or “table” to verify this.
(b) Each graph of y3 is a horizontal line.
(c) The graphs of y4 and y 5 a are the same.
(d) e y22y1 5 a, ln(e y22y1) 5 ln a,
y2 2 y1 5 ln a, y1 5 y2 2 ln a 5 ln x 2 ln a
53. If the graph of f (x) passes the horizontal line test, so will
the graph of g(x) 5 2f(x) since it’s the same graph
reflected about the x-axis.
Alternate answer: If g(x1) 5 g(x2) then
2f (x1) 5 2f (x2), f (x1) 5 f (x2), and x1 5 x2
since f is one-to-one.
1
f(x1)
1
f(x2)
54. Suppose that g(x1) 5 g(x2). Then }} 5 }},
f (x1) 5 f (x2), and x1 and x2 since f is one-to-one.
55. (a) The expression a(b c2x) 1 d is defined for all values of
x, so the domain is (2`, `). Since b c2x attains all
positive values, the range is (d, `) if a . 0 and the
range is (2`, d) if a , 0.
2dx 1 b
cx 2 a
2dx 1 b
f 21(x) 5 }}
cx 2 a
ax 1 b
cx 1 d
a
c
(c) As x → 6`, f (x) 5 }} → }}, so the horizontal
a
c
asymptote is y 5 }} (c Þ 0). Since f(x) is undefined at
d
c
d
c
x 5 2}}, the vertical asymptote is x 5 2}}.
2dx 1 b
d
cx 2 a
c
d
tal asymptote is y 5 2}} (c Þ 0). Since f 21(x) is
c
a
a
undefined at x 5 }}, the vertical asymptote is x 5 }}.
c
c
(d) As x → 6`, f 21(x) 5 }} → 2}}, so the horizon-
The horizontal asymptote of f becomes the vertical
asymptote of f 21 and vice versa due to the reflection of
the graph about the line y 5 x.
■ Section 1.6 Trigonometric Functions
(pp. 41–51)
Exploration 1
Functions
Unwrapping Trigonometric
1. (x1, y1) is the circle of radius 1 centered at the origin (unit
circle). (x2, y2) is one period of the graph of the sine
function.
32
Section 1.6
2. The y-values are the same in the interval 0 # t # 2p.
3.
3. The y-values are the same in the interval 0 # t # 4p.
4. The x1-values and the y2-values are the same in each
interval.
5. y2 5 tan t:
[23, 3] by [22, 2]
Using trace, cos t and sin t are being computed for 0, 15,
30, … , 360 degrees.
Quick Review 1.6
y2 5 csc t:
p
3
1808
p
1. }} ? }} 5 608
2. 22.5 ? }} 5 12}}28 < 2143.248
y2 5 sec t:
1808
p
450
p
p
1808
2p
9
3. 2408 ? }} 5 2}}
p
1808
p
4
4. 458 ? }} 5 }}
5.
y2 5 cot t:
[0, 2p] by [21.5, 1.5]
For each value of t, the value of y2 5 tan t is equal to the
y
x < 0.6435, x < 2.4981
6.
ratio }}1 .
x1
For each value of t, the value of y2 5 csc t is equal to the
1
y1
ratio }}.
[0, 2p] by [21.5, 1.5]
x < 1.9823, x < 4.3009
For each value of t, the value of y2 5 sec t is equal to the
7.
1
ratio }}.
x1
For each value of t, the value of y2 5 cot t is equal to the
x
p 3p
ratio }}1 .
y1
Exploration 2
Finding Sines and Cosines
1. The decimal viewing window [24.7, 4.7] by [23.1, 3.1] is
square on the TI-82/83 and many other calculators. There
are many other possibilities.
[24.7, 4.7] by [23.1, 3.1]
2. Using the Ask table setting for the independent variable on
the TI-83 we obtain
32}2}, }2}4 by [22, 2]
p
5p
x < 0.7854 1or }}2, x < 3.9270 1or }}2
4
4
8. f(2x) 5 2(2x)2 2 3 5 2x 2 2 3 5 f (x)
The graph is symmetric about the y-axis because if a point
(a, b) is on the graph, then so is the point (2a, b).
9. f(2x) 5 (2x)3 2 3(2x)
5 2x 3 1 3x
5 2(x 3 2 3x) 5 2f (x)
The graph is symmetric about the origin because if a point
(a, b) is on the graph, then so is the point (2a, 2b).
10. x $ 0
Section 1.6 Exercises
5p
8
5p
4
1. Arc length 5 1}}2(2) 5 }}
10
}}
72
2. Radius 5 1758 }p} 5 }} < 3.274
7p
1808
1 2
Section 1.6
2p
p
16. (a) Period 5 }} 5 2
1
2
7
14
3. Angle 5 }} 5 }} radian or about 28.658
(b) Amplitude 5 1
p
4
3p/2
6
4. Angle 5 }} 5 }} radian or 458
(c) [24, 4] by [22, 2]
5. (a) The period of y 5 sec x is 2p, so the window should
have length 4p.
One possible answer: [0, 4p] by [23, 3]
2p
3
17. (a) Period 5 }}
(c) The period of y 5 cot x is p, so the window should
have length 2p.
One possible answer: [0, 2p] by [23, 3]
6. (a) The period of y 5 sin x is 2p, so the window should
have length 4p.
One possible answer: [0, 4p] by [22, 2]
p
6
p p
2 2
p
p
p
sin }} 5 0.5, sin21(0.5) 5 }} radian or }}
6
6
6
7. Since }} is in the range 32}}, }}4 of y 5 sin21 x and
?
1808
}} 5 308.
p
kp
3
equivalent to x Þ }} for integers k.
(c) Since )csc (3x 1 p)) $ 1, the range excludes numbers
between 23 2 2 5 25 and 3 2 2 5 1. The range is
(2`, 25] < [1, `).
(d)
2p 2p
32}3}, }3}4 by [28, 8]
2p
4
2
p
2
18. (a) Period 5 }} 5 }}
(b) Domain: (2`, `)
(c) Since )sin (4x 1 p)) # 1, the range extends from
22 1 3 5 1 to 2 1 3 5 5. The range is [1, 5].
(d)
p
p p
8. Since 2}} is the range 2}}, }} of y 5 sin21 x and
4
2 2
Ïw2
Ï2w
p
p
21
sin 2}} 5 2}}, sin 2}} 5 2}} radian or
2
2
4
4
p 1808
2}} ? }} 5 2458.
4
p
3
(k 2 1)p
3
3x 1 p Þ kp, or x Þ }}. This requirement is
(b) The period of y 5 cos x is 2p, so the window should
have length 4p.
One possible answer: [0, 4p] by [22, 2]
(c) The period of y 5 tan x is p, so the window should
have length 2p.
One possible answer: [0, 2p] by [23, 3]
1
sin (3x 1 p)
(b) Domain: Since csc (3x 1 p) 5 }}, we require
(b) The period of y 5 csc x is 2p, so the window should
have length 4p.
One possible answer: [0, 4p] by [23, 3]
1
33
4
1
2
9. Using a calculator, tan21(25) < 21.3734 radians or
278.69018.
10. Using a calculator, cos21(0.7) < 0.7954 radian or 45.57308.
p p
32}2}, }2}4 by [28, 8]
p
3
19. (a) Period 5 }}
(k 2 2)p
6
2p
2
Therefore, x Þ }} for odd integers k. This
11. (a) Period 5 }} 5 p
(b) Amplitude 5 1.5
(c) [22p, 2p] by [22, 2]
2p
3
12. (a) Period 5 }}
(b) Amplitude 5 2
kp
2
(b) Domain: We require 3x 1 p Þ }} for odd integers k.
kp
6
requirement is equivalent to x Þ }} for odd integers k.
(c) Since the tangent function attains all real values, the
range is (2`, `).
(d)
2p 2p
(c) 2}}, }} by [24, 4]
3 3
2p
13. (a) Period 5 }} 5 p
2
3
4
(b) Amplitude 5 3
p p
32}2}, }2}4 by [28, 8]
(c) [22p, 2p] by [24, 4]
2p
14. (a) Period 5 }} 5 4p
1/2
(b) Amplitude 5 5
(c) [24p, 4p] by [210, 10]
2p
2
20. (a) Period 5 }} 5 p
(b) Domain: (2`, `)
)
(d)
2p
p/3
15. (a) Period 5 }} 5 6
(b) Amplitude 5 4
(c) [23, 3] by [25, 5]
p
3
)
(c) Range: Since sin 12x 1 }}2 # 1, the range is [22, 2].
[2p, p] by [23, 3]
34
Section 1.6
21. Note that Ï8w2w1
ww15w2w 5 17.
p
2
8
17
p
2
11p
6
Since sin u 5 }} and 2}} # u # }},
cos u 5 Ï1ww
2wsin
w2wuw 5
x 5 }}. Since y 5 sin x has period 2p, the solutions are
!§§§§§
8 2
17
15
17
sin u
cos u
15
17
8
17
1
cos u
15
8
1
sin u
17
15
17
8
p
sin u
25/13
5
12/13
12
2
cos u
12
5
have sin u 5 2}} and cos u 5 }}. In summary:
13
13
12
5
5
sin u 5 2}}, cos u 5 }}, tan u 5 2}},
13
13
12
1
1
12
13
cot u 5 }} 5 2}}, sec u 5 }} 5 }},
5
12
tan u
cos u
1
13
csc u 5 }} 5 2}}
5
sin u
p
2
Since tan u 5 2}} 5 }} 5 }} and 2}} # u # }}, we
3
5
cot u 5 5
r
}}
x
sec u 5 5
y
x
5
2}},
3
r
}}
y
csc u 5 5
2
y
x
2
22
r
x
2Ïw2
22
1
4
3
5
}}
4
1
22
2
w
2Ï2
2
sec u 5 }} 5 }} 5 2Ï2w, csc u 5 }} 5 }} 5 Ï2w
25. The angle tan21(2.5) < 1.190 is the solution to this
p
2
7
11
Ï7w2w
w
6Ï2
11
!1§§2§1§§2
7 2
}}
11
5 }} 5 }} < 0.771.
p
2
9
13
tan u 5 }} 5 }} 5 21, cot u 5 }} 5 }} 5 21,
r
y
7
11
sin 1cos211}}22 5 sin u 5 Ï1ww
2wcoww
s2w
u5
11
sin u 5 }} 5 }} 5 }} cos u 5 }} 5 }} 5 2}},
r
r
2Ï2w
2Ï2w
Ï2w
Ï2w
x
y
p
4
3p
integer. This is equivalent to x 5 }} 1 kp, where k is any
4
all solutions are of the form x 5 2}} 1 kp, where k is any
p
2
32. Let u 5 sin21 1}}2. Then 2}} # u # }} and sin u 5 }}, so
22
x
p
4
x 5 tan21(21) 5 2}}. Since the period of y 5 tan x is p,
7
11
24. Note that r 5 Ï(2
w2ww
)2w
1w22w 5 2Ï2w. Then:
y
p
2
31. Let u 5 cos211}}2. Then 0 # u # p and cos u 5 }}, so
sin u 5 }} 5 }}, cos u 5 }} 5 2}}, tan u 5 }} 5 2}},
3
2}},
4
p
2
integer.
23. Note that r 5 Ï(2
w3ww
)2w
1w42w 5 5. Then:
x
r
1
21
30. The equation is equivalent to tan x 5 }} 5 21, so the
solution in the interval 2}} , x , }} is
22. Note that Ï5w2w1
ww12w2w 5 13.
4
5
11p
6
is any integer.
8
15
cot u 5 }} 5 }}, sec u 5 }} 5 }}, csc u 5 }} 5 }}
y
r
x
}}
y
7p
6
all of the form x 5 }} 1 2kp or x 5 }} 1 2kp, where k
1 2 1}}2 5 }}.
Therefore: sin u 5 }}, cos u 5 }}, tan u 5 }} 5 }},
1
tan u
7p
6
29. The solutions in the interval 0 # x , 2p are x 5 }} and
cos u 5 Ï1ww
2wsin
w2wuw 5
!1§§2§1§2§ 5
9 2
}}
13
sin u
9
13
Ïw8w8
}}.
13
9/13
Therefore,
9
tan 1sin211}}22 5 tan u 5 }} 5 }} 5 }} < 0.959.
13
cos u
Ï8w8w/13 Ï8w8w
33. (a) Using a graphing calculator with the sinusoidal
regression feature, the equation is
y 5 1.543 sin (2468.635x 2 0.494) 1 0.438.
9
p
2
equation in the interval 2}} , x , }}. Another solution in
0 # x , 2p is tan21(2.5) 1 p < 4.332. The solutions are
x < 1.190 and x < 4.332.
[0, 0.01] by [22.5, 2.5]
26. The angle cos21(20.7) < 2.346 is the solution to this
equation in the interval 0 # x # p. Since the cosine
function is even, the value 2cos21(20.7) < 22.346 is also
a solution, so any value of the form 6cos21(20.7) 1 2kp
is a solution, where k is an integer. In 2p # x , 4p the
solutions are x 5 cos21(20.7) 1 2p < 8.629 and
x 5 2cos21(20.7) 1 4p < 10.220.
1
2
27. This equation is equivalent to sin x 5 }}, so the solutions in
p
6
5p
6
the interval 0 # x , 2p are x 5 }} and x 5 }}.
1
3
28. This equation is equivalent to cos x 5 2}}, so the solution
in the interval 0 # x # p is y 5 cos21 12}}2 < 1.911.
1
3
Since the cosine function is even, the solutions in the
interval 2p # x , p are x < 21.911 and x < 1.911.
(b) The frequency is 2468.635 radians per second, which is
2468.635
2p
equivalent to }} < 392.9 cycles per second (Hz).
The note is a “G.”
2p
12
p
6
34. (a) b 5 }} 5 }}
80 2 30
2
(b) It’s half of the difference, so a 5 }} 5 25.
80 1 30
2
(c) k 5 }} 5 55
(d) The function should have its minimum at t 5 2 (when
the temperature is 308F) and its maximum at t 5 8
(when the temperature is 808F). The value of h is
218
}}
2
p
6
5 5. Equation: y 5 25 sin 3}}(x 2 5)4 1 55
Section 1.6
35
(b) Amplitude < 1.414 (that is, Ï2w)
(e)
Period 5 2p
p
4
Horizontal shift < 20.785 1that is, 2}}2
7p
4
or 5.498 1that is, }}2
[21, 13] by [210, 100]
35. (a) Amplitude 5 37
Vertical shift: 0
2p
(b) Period 5 }} 5 365
(2p/365)
(c)
(c) Horizontal shift 5 101
1 2
1
36. (a) Highest: 25 1 37 5 628F
Lowest: 25 2 37 5 2128F
(b) Average 5
p
4
p
4
1
5 (sin x)1}}2 1 (cos x) }}
Ïw2
Ï2w
1
5 }}(sin x 1 cos x)
Ïw2
p
Therefore, sin x 1 cos x 5 Ïw2 sin 1x 1 }}2.
(d) Vertical shift 5 25
62 1 (212)
}}
2
p
4
sin 1x 1 }}2 5 (sin x)1cos }}2 1 (cos x)1sin }}2
4
p
43. (a) Ïw2 sin ax 1 }}
4
1
5 258F
This average is the same as the vertical shift because
2
(b) See part (a).
(c) It works.
the average of the highest and lowest values of
cos (2x)
sin (2x)
cos (x)
2sin (x)
37. (a) cot (2x) 5 }} 5 }} 5 2cot (x)
(b) Assume that f is even and g is odd.
Then
f(2x)
}}
g(2x)
f(x)
f(x)
f
5 }} 5 2}} so }} is odd. The situation
g(x)
g
2g(x)
g
f
is similar for }}.
p
4
1
1
5 (sin ax) }} 1 (cos ax) }}
Ïw2
Ïw2
1
5 }}(sin ax 1 cos ax)
Ïw2
p
4
1 2
p
4
1
2
So, sin (ax) 1 cos (ax) 5 Ï2w sin ax 1 }} .
44. (a) One possible answer:
y 5 Ïaw2w1
wwb 2w sin 1x 1 tan211}b}22
(b) See part (a).
(c) It works.
(d) sin 1x 1 tan211}}22
b
a
(b) Assume that f is odd.
1
2f (x)
1 2
a
1
1
38. (a) csc (2x) 5 }} 5 }} 5 2csc (x)
sin (2x)
2sin (x)
1
f(2x)
p
4
(d) sin 1ax 1 }}2 5 (sin ax)1cos }}2 1 (cos ax)1sin }}2
y 5 sin x is 0.
1
f(x)
1
f
Then }} 5 }} 5 2}} so }} is odd.
39. Assume that f is even and g is odd.
Then f (2x)g(2x) 5 ( f(x))(2g(x)) 5 2f (x)g(x) so ( fg) is
odd.
40. If (a, b) is the point on the unit circle corresponding to the
angle u, then (2a, 2b) is the point on the unit circle
corresponding to the angle (u 1 p) since it is exactly half
way around the circle. This means that both tan (u) and
b
tan (u 1 p) have the same value, }}.
a
41. (a) Using a graphing calculator with the sinusoidal
regression feature, the equation is
y 5 3.0014 sin (0.9996x 1 2.0012) 1 2.9999.
(b) y 5 3 sin ( x 1 2) 1 3
42. (a)
5 sin (x) cos 1tan211}}22 1 cos (x) sin 1tan211}}22
b
a
a
b
a
b
5 sin (x) 1}}2 1 cos (x) 1}}2
b 2w
Ïaw2w1
ww
Ïaw2w1
wwb2w
1
5 }} ? (a sin x 1 b cos x)
b 2w
Ïaw2w1
ww
and multiplying through by the square root gives the
desired result. Note that the substitutions
a
cos 1tan21 }}2 5 }} and
a
b 2w
Ïaw2w1
ww
b
b
sin 1tan21 }}2 5 }} depend on the requirement
a
Ïaw2w1
wwb2w
that a is positive. If a is negative, the formula does not
b
work.
45. Since sin x has period 2p, sin3 (x 1 2p) 5 sin3 (x). This
function has period 2p. A graph shows that no smaller
number works for the period.
[22p, 2p] by [22, 2]
The graph is a sine/cosine type graph, but it is shifted
and has an amplitude greater than 1.
[22p, 2p] by [21.5, 1.5]
36
Chapter 1 Review
46. Since tan x has period p, )tan (x 1 p)) 5 )tan x). This
function has period p. A graph shows that no smaller
number works for the period.
4
3
9. Since 4x 1 3y 5 12 is equivalent to y 5 2}}x 1 4, the
slope of the given line (and hence the slope of the desired
4
3
line) is 2}}.
4
3
4
2}}x
3
y 5 2}}(x 2 4) 2 12
y5
[22p, 2p] by [21, 5]
2p
p
47. The period is }} 5 }}. One possible graph:
60
30
20
3
2 }}
3
5
1
5
10. Since 3x 2 5y 5 1 is equivalent to y 5 }}x 2 }}, the slope of
3
5
the given line is }} and the slope of the perpendicular line is
5
3
2}}.
5
3
5
2}}x
3
y 5 2}}(x 1 2) 2 3
p p
2}}, }} by [22, 2]
60 60
2p
1
48. The period is }} 5 }}. One possible graph:
30
60p
3
4
y5
19
3
2 }}
1
2
1
3
3
2
11. Since }}x 1 }}y 5 1 is equivalent to y 5 2}}x 1 3, the slope
3
2
of the given line is 2}} and the slope of the perpendicular
2
3
line is }}.
2
3
2
}}x
3
y 5 }}(x 1 1) 1 2
y5
32}60}, }6}0 4 by [22, 2]
1
1
12. The line passes through (0, 25) and (3, 0)
■ Chapter 1 Review Exercises
(pp. 52–53)
1. y 5 3(x 2 1) 1 (26)
y 5 3x 2 9
1
2
1
2}}x
2
y5
224
2 2 (22)
3
2
f (x) 5
1
2
1
2
1
2}}x
2
13
1
2
Check: f(4) 5 2}}(4) 1 3 5 1, as expected.
28
4
4. m 5 }} 5 }} 5 22
14. The line passes through (4, 22) and (23, 0).
y 5 22(x 1 3) 1 6
y5
5. y 5 2
523
2
22 2 3
25
2
2}}(x 2 3) 1 3
5
2
21
2}} 1 }}
5
5
0 2 (22)
2
23 2 4
27
2
2}}(x 2 4) 2 2
7
2
6
2}}x 2 }}
7
7
2
7
m 5 }} 5 }} 5 2}}
y 5 22x
y5
2
5
6. m 5 }} 5 }} 5 2}}
y5
22
4
f (x) 5 2}}(x 1 2) 1 4
3. x 5 0
y5
5
3
13. m 5 }} 5 }} 5 2}}
1 }}
22 2 6
1 2 (23)
0 2 (25)
320
5
}}x 2 5
3
m 5 }} 5 }}
2. y 5 2}}(x 1 1) 1 2
y5
8
3
1 }}
15.
7. y 5 23x 1 3
8. Since 2x 2 y 5 22 is equivalent to y 5 2x 1 2, the slope
of the given line (and hence the slope of the desired line)
is 2.
y 5 2(x 2 3) 1 1
y 5 2x 2 5
[23, 3] by [22, 2]
Symmetric about the origin.
16.
[23, 3] by [22, 2]
Symmetric about the y-axis.
Chapter 1 Review
37
29. (a) Since the square root requires 16 2 x 2 $ 0, the domain
is [24, 4].
17.
(b) For values of x in the domain, 0 # 16 2 x 2 # 16, so
0 # Ï1w6ww
2wx 2w # 4. The range is [0, 4].
(c)
[26, 6] by [24, 4]
Neither
18.
[29.4, 9.4] by [26.2, 6.2]
30. (a) The function is defined for all values of x, so the
domain is (2`, `).
[21.5, 1.5] by [20.5, 1.5]
(b) Since 322x attains all positive values, the range is
(1, `).
Symmetric about the y-axis.
19. y(2x) 5 (2x)2 1 1 5 x 2 1 1 5 y(x)
Even
(c)
20. y(2x) 5 (2x)5 2 (2x)3 2 (2x) 5 2x 5 1 x 3 1 x 5 2y(x)
Odd
21. y(2x) 5 1 2 cos(2x) 5 1 2 cos x 5 y(x)
Even
31. (a) The function is defined for all values of x, so the
domain is (2`, `).
22. y(2x) 5 sec (2x) tan (2x)
sin (2x)
cos (2x)
[26, 6] by [24, 20]
(b) Since 2e 2x attains all positive values, the range is
(23, `).
2sin x
cos x
5}
2
2 } 5 }}
5 2sec x tan x 5 2y(x)
(c)
Odd
(2x)4 1 1
x4 1 1
x4 1 1
23. y(2x) 5 }
}5}
} 5 2}
} 5 2y(x)
(2x)3 2 2(2x)
2x 3 1 2x
x 3 2 2x
Odd
24. y(2x) 5 1 2 sin (2x) 5 1 1 sin x
Neither even nor odd
25. y(2x) 5 2x 1 cos (2x) 5 2x 1 cos x
Neither even nor odd
[24, 4] by [25, 15]
32. (a) The function is equivalent to y 5 tan 2x, so we require
4
27. (a) The function is defined for all values of x, so the
domain is (2`, `).
(b) Since )x) attains all nonnegative values, the range is
[22, `).
kp
2
kp
}} for
4
2x Þ }} for odd integers k. The domain is given by
wx)
ww2
ww1 5 Ïw
xw
2w1
26. y(2x) 5 Ï(2
Even
4
xÞ
odd integers k.
(b) Since the tangent function attains all values, the range
is (2`, `).
(c)
(c)
p p
32}2}, }2}4 by [28, 8]
[210, 10] by [210, 10]
28. (a) Since the square root requires 1 2 x $ 0, the domain is
(2`, 1].
33. (a) The function is defined for all values of x, so the
domain is (2`, `).
2wx attains all nonnegative values, the range
(b) Since Ï1ww
is [22, `).
(b) The sine function attains values from 21 to 1, so
22 # 2 sin (3x 1 p) # 2, and hence
23 # 2 sin (3x 1 p) 2 1 # 1. The range is [23, 1].
(c)
(c)
[29.4, 9.4] by [23, 3]
[2p, p] by [25, 5]
38
Chapter 1 Review
34. (a) The function is defined for all values of x, so the
domain is (2`, `).
5
x 2, which attains
(b) The function is equivalent to y 5 Ïw
all nonnegative values. The range is [0, `).
(c)
39. First piece: Line through (0, 1) and (1, 0)
021
120
21
1
m 5 }} 5 }} 5 21
y 5 2x 1 1 or 1 2 x
Second piece:
Line through (1, 1) and (2, 0)
021
221
21
1
m 5 }} 5 }} 5 21
[28, 8] by [23, 3]
35. (a) The logarithm requires x 2 3 . 0, so the domain is
(3, `).
(b) The logarithm attains all real values, so the range is
(2`, `).
(c)
y 5 2(x 2 1) 1 1
y 5 2x 1 2 or 2 2 x
f(x) 5
h
1 2 x,
2 2 x,
0#x,1
1#x#2
40. First piece: Line through (0, 0) and (2, 5)
520
220
5
}}x
2
5
2
m 5 }} 5 } }
y5
[23, 10] by [24, 4]
36. (a) The function is defined for all values of x, so the
domain is (2`, `).
(b) The cube root attains all real values, so the range is
(2`, `).
(c)
Second piece: Line through (2, 5) and (4, 0)
025
25
5
422
2
2
5
y 5 2}}(x 2 2) 1 5
2
5
5x
y 5 2}}x 1 10 or 10 2 }}
2
2
5x
0#x
}},
f(x) 5 2
5x
10 2 }},
2#x
2
m 5 }} 5 }} 5 2}}
5
,2
#4
(Note: x 5 2 can be included on either piece.)
[210, 10] by [24, 4]
37. (a) The function is defined for 24 # x # 4, so the domain
is [24, 4].
w)w, 24 # x # 4,
(b) The function is equivalent to y 5 Ï)x
which attains values from 0 to 2 for x in the domain.
The range is [0, 2].
(c)
1
41. (a) ( f + g)(21) 5 f (g(21)) 5 f 1}}2 5 f (1) 5 }} 5 1
1
1w2
Ï2
w1ww
1
1
[26, 6] by [23, 3]
(b) See the graph in part (c). The range is [21, 1].
(c)
!}§5}
2
(c) ( f + f )(x) 5 f ( f(x)) 5 f 1}}2 5 }} 5 x, x Þ 0
1
1/x
1
x
1
38. (a) The function is defined for 22 # x # 2, so the domain
is [22, 2].
1
1
(b) (g + f )(2) 5 g( f (2)) 5 g1}}2 5 }} 5 }} or
2
Ï1w/w2w
+w2
Ïw2.5
w
(d) (g + g)(x) 5 g(g(x)) 5 g1}}2 5
Ïxw1
ww2
4
Ïxw1
ww2
}}
5
Ï1ww
1w2w
Ïxw1
ww2
42. (a)
1
}}
Ïw
1/Ï
wxww1
ww
w
w2w
1w
2
( f + g)(21) 5 f (g(21))
3
5 f (Ï2
w1ww
1w1)
5 f (0) 5 2 2 0 5 2
3
(b) (g + f )(2) 5 g( f (2)) 5 g(2 2 2) 5 g(0) 5 Ï0ww
1w1 5 1
(c) ( f + f )(x) 5 f ( f (x)) 5 f (2 2 x) 5 2 2 (2 2 x) 5 x
[23, 3] by [22, 2]
3
(d) (g + g)(x) 5 g(g(x)) 5 g(Ïxw1
ww1) 5
3 3
Ï
Ïxw
w
w1
www1w
w
1w
1
Chapter 1 Review
43. (a) ( f + g)(x) 5 f (g(x))
x
4
39
y
4
(b) Substituting cos t 5 }} and sin t 5 }} in the identity
ww2)
5 f (Ïxw1
ww2)
5 2 2 (Ïxw1
cos2 t 1 sin2 t 5 1 gives the Cartesian equation
2
x 2
1}4}2
5 2x, x $ 22
y 2
4
1 1}}2 5 1, or x 2 1 y 2 5 16. The left half of the
circle is traced by the parametrized curve.
(g + f )(x) 5 g( f(x))
5 g(2 2 x 2)
47. (a)
ww
2wxw)w
1w2 5 Ï4ww
2wxw
5 Ï(2
2
2
(b) Domain of f + g: [22, `)
Domain of g + f: [22, 2]
(c) Range of f + g: (2`, 2]
Range of g + f: [0, 2]
[28, 8] by [210, 20]
Initial point: (4, 15)
Terminal point: (22, 3)
The line segment is traced from right to left starting at
(4, 15) and ending at (22, 3).
44. (a) ( f + g)(x) 5 f (g(x))
5 f (Ï1ww
2wx)
(b) Substituting t 5 2 2 x into y 5 11 2 2t gives the
Cartesian equation y 5 11 2 2(2 2 x), or y 5 2x 1 7.
The part of the line from (4, 15) to (22, 3) is traced by
the parametrized curve.
5 ÏÏ
w1ww
2wx
4
5 Ï1ww
2wx
(g + f )(x) 5 g( f(x)) 5 g(Ïxw) 5 Ï1ww
2w
Ïxw
48. (a)
(b) Domain of f + g: (2`, 1]
Domain of g + f: [0, 1]
(c) Range of f + g: [0, `)
Range of g + f: [0, 1]
[28, 8] by [24, 6]
Initial point: None
Terminal point: (3, 0)
The curve is traced from left to right ending at the
point (3, 0).
45. (a)
[26, 6] by [24, 4]
Initial point: (5, 0)
Terminal point: (5, 0)
The ellipse is traced exactly once in a counterclockwise
direction starting and ending at the point (5, 0).
x
5
y
2
(b) Substituting cos t 5 }} and sin t 5 }} in the identity
cos2 t 1 sin2 t 5 1 gives the Cartesian equation
1}5}2
x
2
2
1 1}}2 5 1.
y
2
The entire ellipse is traced by the curve.
(b) Substituting t 5 x 2 1 into y 5 Ï4ww
2w
2tw gives the
Cartesian equation y 5 Ï4ww
2w
2(x
ww
2w
1)w, or
y 5 Ïw6w
2w2wx. The entire curve is traced by the
parametrized curve.
49. (a) For simplicity, we assume that x and y are linear
functions of t, and that the point (x, y) starts at (22, 5)
for t 5 0 and ends at (4, 3) for t 5 1. Then x 5 f (t),
where f(0) 5 22 and f(1) 5 4. Since
Dx
Dt
4 2 (22)
120
slope 5 }} 5 }} 5 6,
x 5 f (t) 5 6t 2 2 5 22 1 6t.
Also, y 5 g(t), where g(0) 5 5 and g(1) 5 3. Since
Dy
Dt
325
120
slope 5 }} 5 }} 5 22,
46. (a)
y 5 g(t) 5 22t 1 5 5 5 2 2t.
One possible parametrization is:
x 5 22 1 6t, y 5 5 2 2t, 0 # t # 1
[29, 9] by [26, 6]
Initial point: (0, 4)
3p
Terminal point: None (since the endpoint }} is not
2
included in the t-interval)
The semicircle is traced in a counterclockwise direction
starting at (0, 4) and extending to, but not including,
(0, 24).
40
Chapter 1 Review
y 5 Ïxw 2 2
f 21(x) 5 Ïxw 2 2
Verify.
For x $ 0 (the domain of f 21)
( f + f 21)(x) 5 f ( f 21(x))
5 f (Ïwx 2 2)
5 [(Ïwx 2 2) 1 2]2
5 (Ïwx)2 5 x
For x $ 22 (the domain of f),
( f 21 + f )(x) 5 f 21( f(x))
5 f 21((x 1 2)2)
5 Ïw
(xw
1w2w
)2 2 2
5 )x 1 2) 2 2
5 (x 1 2) 2 2 5 x
50. For simplicity, we assume that x and y are linear functions
of t and that the point (x, y) passes through (23, 22) for
t 5 0 and (4, 21) for t 5 1. Then x 5 f (t), where
f (0) 5 23 and f (1) 5 4. Since
Dx
Dt
4 2 (23)
120
slope = }} 5 }} 5 7,
x 5 f (t) 5 7t 2 3 5 23 1 7t.
Also, y 5 g(t), where g(0) 5 22 and g(1) 5 21.
Since
Dy
Dt
21 2 (22)
120
slope 5 }} 5 }} 5 1
y 5 g(t) 5 t 2 2 5 22 1 t.
One possible parametrization is:
x 5 23 1 7t, y 5 22 1 t, 2` , t , `.
51. For simplicity, we assume that x and y are linear functions
of t and that the point (x, y) starts at (2, 5) for t 5 0 and
passes through (21, 0) for t 5 1. Then x 5 f(t), where
f (0) 5 2 and f (1) 5 21. Since
Dx
Dt
21 2 2
120
Dy
Dt
025
120
(b)
slope 5 }} 5 }} 5 23, x 5 f (t) 5 23t 1 2 5 2 2 3t.
Also, y 5 g(t), where g(0) 5 5 and g(1) 5 0. Since
slope 5 }} 5 }} 5 25, y 5 g(t) 5 25t 1 5 5 5 2 5t.
One possible parametrization is:
x 5 2 2 3t, y 5 5 2 5t, t $ 0.
52. One possible parametrization is:
x 5 t, y 5 t(t 2 4), t # 2.
56. Using a calculator, tan21(22.3) < 21.1607 radians or
266.50148.
3
7
57. Since cos u 5 }} and 0 # u # p,
53. (a) y 5 2 2 3x
sin u 5 Ï1ww
2wcoww
s2wu 5
3x 5 2 2 y
22y
3
x 5 }}
!1§§2§1§§2 5 !§§ 5
3 2
}}
7
40
}}
49
Ï4w0w
}}.
7
Therefore,
Interchange x and y.
22x
3
[26, 12] by [24, 8]
55. Using a calculator, sin21(0.6) < 0.6435 radians or
36.86998.
Ï4w0w
Ï4w0w
sin u
3
cos u
3
1
1
7
cot u 5 }} 5 }}, sec u 5 }} 5 }},
3
tan u
cos u
Ï4ww0
7
1
csc u 5 }} 5 }}
sin u
Ïw4w0
3
7
sin u 5 }}, cos u 5 }}, tan u 5 }} 5 }},
y 5 }}
7
22x
3
f 21(x) 5 }}
Verify.
( f + f 21)(x) 5 f ( f 21(x))
22x
3
5 f 1}}2
22x
3
5 2 2 31}}2
5 2 2 (2 2 x) 5 x
( f 21 + f )(x) 5 f 21( f(x))
5 f 21(2 2 3x)
2 2 (2 2 3x)
3
3x
}} 5 x
3
5 }}
5
58. (a) Note that sin21(20.2) < 20.2014. In [0, 2p), the
solutions are x 5 p 2 sin21(20.2) < 3.3430 and
x 5 sin21(20.2) 1 2p < 6.0818.
(b) Since the period of sin x is 2p, the solutions are
x < 3.3430 1 2kp and x < 6.0818 1 2kp, k any
integer.
59. e20.2x 5 4
ln e20.2x 5 ln 4
20.2x 5 ln 4
ln 4
x 5 }} 5 25 ln 4
20.2
60. (a) The given graph is reflected about the y-axis.
y
3
(0, 2)
(b)
(–1, 0)
x
(3, 0)
–3
[26, 6] by [24, 4]
54. (a) y 5 (x 1 2)2, x $ 22
Ïwy 5 x 1 2
x 5 Ïwy 2 2
Interchange x and y.
y = f(–x)
–3
Chapter 1 Review
(b) The given graph is reflected about the x-axis.
y
62. (a) V 5 100,000 2 10,000x, 0 # x # 10
(b)
3
(1, 0)
(–3, 0)
–3
3
x
41
V 5 55,000
100,000 2 10,000x 5 55,000
210,000x 5 245,000
x 5 4.5
The value is $55,000 after 4.5 years.
63. (a) f (0) 5 90 units
(b) f (2) 5 90 2 52 ln 3 < 32.8722 units
(c)
y = –f(x)
(0, –2)
–3
(c) The given graph is shifted left 1 unit, stretched
vertically by a factor of 2, reflected about the x-axis,
and then shifted upward 1 unit.
[0, 4] by [220, 100]
y
y = –2f(x + 1) + 1
(–4, 1)
64. 1500(1.08)t 5 5000
3
5000
1500
10
3
1.08t5 }} 5 }}
(0, 1)
–4
2
10
3
10
}}
3
ln (1.08)t 5 ln }}
x
t ln 1.08 5 ln
ln (10/3)
ln 1.08
t 5 }}
(–1, –3)
(d) The given graph is shifted right 2 units, stretched
vertically by a factor of 3, and then shifted downward
2 units.
4
t < 15.6439
It will take about 15.6439 years. (If the bank only pays
interest at the end of the year, it will take 16 years.)
65. (a) N(t) 5 4 ? 2t
(b) 4 days: 4 ? 24 5 64 guppies
1 week: 4 ? 27 5 512 guppies
y y = 3f(x – 2) – 2
(2, 4)
(c)
x
–2
4
(–1, –2)
(3, –2)
61. (a)
y
(3, 2)
–3
3
ln 500
ln 2
t5 }} < 8.9658
There will be 2000 guppies after 8.9658 days, or after
nearly 9 days.
(d) Because it suggests the number of guppies will
continue to double indefinitely and become arbitrarily
large, which is impossible due to the finite size of the
tank and the oxygen supply in the water.
3
(–3, 2)
N(t) 5 2000
4 ? 2t 5 2000
2t 5 500
ln 2t 5 ln 500
t ln 2 5 ln 500
x
66. (a) y 5 20.627x 1 338.622
(–1, –1) (1, –1)
–3
(b)
y
[0, 30] by [2100, 1000]
3
(3, 2)
(–1, 1)
–3
3
(1, –1)
(–3, –2)
–3
x
(b) When x 5 30, y < 957.445. According to the
regression equation, about 957 degrees will be earned.
(c) The slope is 20.627. It represents the approximate
annual increase in the number of doctorates earned by
Hispanic Americans per year.
67. (a) y 5 14.60175 ? 1.00232x
(b) Solving y 5 25 graphically, we obtain x < 232.
According to the regression equation, the population
will reach 25 million in the year 2132.
(c) 0.232%
42
Section 2.1
4. (a) lim 2 p(s) 5 3
Chapter 2
Limits and Continuity
s→22
(b) lim 1 p(s) 5 3
s→−2
■ Section 2.1 Rates of Change and Limits
(pp. 55–65)
(c) lim p(s) 5 3
s→22
(d) p(22) 5 3
Quick Review 2.1
1. f (2) 5 2(2 ) 2 5(2) 1 4 5 0
3
2
4(2)2 2 5
2 14
11
12
5. (a) lim2 F(x) 5 4
2. f (2) 5 }
3 } 5 }}
x→0
3. f (2) 5 sin 1p ? }}2 5 sin p 5 0
4. f (2) 5
1
}
}
22 2 1
5
2
2
(b) lim1 F(x) 5 –3
1
}}
3
(c) lim F(x) does not exist, because the left- and
x→0
x→0
5. )x) , 4
24 , x , 4
right-hand limits are not equal.
6. )x) , c 2
2c 2 , x , c 2
(d) F(0) 5 4
6. (a) lim2 G(x) 5 1
7. )x 2 2) , 3
23 , x 2 2 , 3
21 , x , 5
x→2
(b) lim1 G(x) 5 1
8. )x 2 c) , d 2
2d 2 , x 2 c , d 2
2d 2 1 c , x , d 2 1 c
9.
x2 2 3x 2 18
}}
x13
2x 2 x
}
}
2x2 1 x 2 1
2
10.
5
5
(x 1 3)(x 2 6)
}}
x13
x(2x 2 1)
}}
(2x 2 1)(x 1 1)
x→2
(c) lim G(x) 5 1
x→2
5 x 2 6, x Þ 23
5
x
}},
x11
1
x Þ }}
2
Section 2.1 Exercises
(d) G(2) 5 3
1 2
2
7. lim 3x 2(2x 2 1) 5 312}}2 3212}}2 2 14 5 31}}2(22)
x→21/2
1
2
1
4
3
2
5 2}}
Graphical support:
1. (a) lim2 f (x) 5 3
x→3
(b) lim1 f (x) 5 –2
x→3
(c) lim f (x) does not exist, because the left- and
[23, 3] by [22, 2]
x→3
right-hand limits are not equal.
8. lim (x 1 3)1998 5 (24 1 3)1998 5 (21)1998 5 1
x→24
(d) f (3) = 1
Graphical support:
2. (a) lim 2 g(t) 5 5
t→24
(b) lim 1 g(t) 5 2
t→24
(c) lim g(t) does not exist, because the left- and
[24.001, 23.999] by [0, 5]
t→24
right-hand limits are not equal.
9. lim (x 3 1 3x 2 2 2x 2 17) 5 (1)3 1 3(1)2 2 2(1) 2 17
x→1
5 1 1 3 2 2 2 17 5 215
(d) g(24) 5 2
3. (a) lim2 f (h) 5 24
Graphical support:
h→0
(b) lim1 f (h) 5 24
h→0
(c) lim f (h) 5 –4
h→0
(d) f (0) 5 24
[23, 3] by [225, 25]
Section 2.1
y2 1 5y 1 6
y12
y→2
22 1 5(2) 1 6
212
20
4
10. lim }} 5 }} 5 }} 5 5
x→p/2
Graphical support:
[23, 3] by [25, 10]
[2p, p] by [23, 1]
(23) 1 4(23) 1 3
(23) 2 3
y 1 4y 1 3
y 23
2
0
6
11. lim }
5 }} 5 0
2
2 } 5 }}}
y→23
p
2
16. lim ln (sin x) 5 ln 1sin }}2 5 ln 1 5 0
Graphical support:
2
43
Graphical support:
17. You cannot use substitution because the expression Ïxw2
ww2
is not defined at x 5 22. Since the expression is not
defined at points near x 5 22, the limit does not exist.
1
x
18. You cannot use substitution because the expression }}2 is
1
x
not defined at x 5 0. Since }}2 becomes arbitrarily large as x
approaches 0 from either side, there is no (finite) limit. (As
[25, 5] by [25, 5]
12. lim int x 5 int
x→1/2
1
}}
2
1
we shall see in Section 2.2, we may write lim }}2 5 `.)
x→0 x
50
Note that substitution cannot always be used to find limits
of the int function. Its use here can be justified by the
Sandwich Theorem, using g(x) 5 h(x) 5 0 on the interval
(0, 1).
Graphical support:
)x)
x
19. You cannot use substitution because the expression }} is not
)x)
)x)
x
defined at x 5 0. Since lim }} 5 21 and lim1 }} 5 1, the
x→02 x
x→0
left- and right-hand limits are not equal and so the limit
does not exist.
20. You cannot use substitution because the expression
(4 1 x)2 2 16
}} is not defined at x 5 0. Since
x
(4 1 x)2 2 16
}}
x
[24.7, 4.7] by [23.1, 3.1]
13. lim (x 2 6)2/3 5 (22 2 6)2/3 5 Ï(2
w8ww
)2 5 Ï6w4w 5 4
3
3
8x 1 x2
x
5 }} 5 8 1 x for all x Þ 0, the limit exists
and is equal to lim (8 1 x) 5 8 1 0 5 8.
x→22
x→0
Graphical support:
21.
[24.7, 4.7] by [23.1, 3.1]
[210, 10] by [210, 10]
x21
14. lim Ïxw1
ww3 5 Ï2ww
1w3 5 Ï5w
1
2
lim }} 5 }}
x→2
2
x→1 x 2 1
Graphical support:
Algebraic confirmation:
x21
x21
1
1
111
1
2
lim }} 5 lim }} 5 lim }} 5 }} 5 }}
2
x→1 x 2 1
x→1 (x 1 1)(x 2 1)
x→1 x 1 1
22.
[24.7, 4.7] by [23.1, 3.1]
15. lim (e xcos x) 5 e 0 cos 0 5 1 ? 1 5 1
x→0
Graphical support:
[24.7, 4.7] by [23.1, 3.1]
t2 2 3t 1 2
t 24
t→2
1
4
lim }
2 } 5 }}
Algebraic confirmation:
(t 2 1)(t 2 2)
t 2 3t 1 2
t21
221
1
}}
lim }
2 } 5 lim (t 1 2)(t 2 2) 5 lim }} 5 }} 5 }}
2
[24.7, 4.7] by [23.1, 3.1]
t→2
t 24
t→2
t→2 t 1 2
212
4
44
Section 2.1
27.
23.
[24.7, 4.7] by [23.1, 3.1]
5x3 1 8x2
lim }
2
4 }
x→0 3x 2 16x
5
[24.7, 4.7] by [23.1, 3.1]
1
2 }}
2
sin x
lim }} 5 21
2
x→0 2x 2 x
Algebraic confirmation:
5x3 1 8x2
3
x→0 x 2 16x
Algebraic confirmation:
x2(5x 1 8)
x
x→0 (3x 2 16)
5x 1 8
5 lim }
2 }
x→0 3x 2 16
5(0) 1 8
5 }2 }
3(0) 2 16
8
1
5 }} 5 2}}
216
2
lim }
2 5 lim }
4 }
2
2}
sin x
x
lim }} 5 lim 1}} ? }}2
sin x
2
x→0 2x 2 x
1 x→0
x→0
sin x
x
1
2x 2 1
lim }}2 5 (1)1}}2 5 21
21 x→0
2x 2 1
2(0) 2 1
1
5 lim }}
1
28.
24.
[24.7, 4.7] by [23.1, 3.1]
1
}}
21x
2
1
}}
2
x→0
Algebraic confirmation:
1
4
lim } 5 2}}
x→0
x
1
2
2 }}
x 1 sin x
x
lim }} 5 lim 11 1 }}2
Algebraic confirmation:
1
}}
21x
x 1 sin x
x
lim }} 5 2
[24.7, 4.7] by [23.1, 3.1]
x→0
5 1 lim 12 1 1 lim }}2
2 2 (2 1 x)
x→0 x(2 1 x)(2)
2x
5 lim }}
x→0 x(2 1 x)(2)
21
5 lim }}
x→0 2(2 1 x)
21
1
5 }} 5 2}}
2(2 1 0)
4
lim } 5 lim }}
x→0
x
sin x
x
x→0
x→0
x→0
sin x
x
511152
29.
25.
[24.7, 4.7] by [23.1, 3.1]
sin2 x
x→0 x
lim }} 5 0
[24.7, 4.7] by [25, 20]
Algebraic confirmation:
(2 1 x)3 2 8
lim }}
x
x→0
sin2 x
x→0 x
5 12
lim }} 5 lim 1sin x ? }}2
5 1lim sin x2 ? 1lim }}2
Algebraic confirmation:
(2 1 x) 2 8
x
3
12x 1 6x 1 x
x
2
x→0
3
lim }} 5 lim }}
x→0
x→0
sin x
x
x→0
x→0
sin x
x
5 (sin 0)(1) 5 0
5 lim (12 1 6x 1 x )
2
x→0
30.
5 12 1 6(0) 1 (0)2 5 12
26.
[22, 2] by [210, 10]
3 sin 4x
lim }} 5 4
x→0 sin 3x
[24.7, 4.7] by [23.1, 3.1]
Algebraic confirmation:
sin 2x
lim }}
x
x→0
x→0 sin 3x
52
lim }} 5 4 lim 1}} ? }}2
3 sin 4x
Algebraic confirmation:
sin 2x
lim }}
x
x→0
5
sin 2x
2 lim }}
x→0 2x
5 2(1) 5 2
3x
sin 4x
sin 3x
4x
sin 3x
lim }}
x→0 3x
x→0
5 41lim }}2 4 1
x→0
sin 4x
4x
5 4(1) 4 (1) 5 4
2
Section 2.1
x
)x)
31. (a) True
x
42. Since }} 5 21 for x , 0, lim2 }} 5 21.
(b) True
x→0 )x)
43. (a) lim (g(x) 1 3) 5 1 lim g(x)2 1 1 lim 32 5 3 1 3 5 6
(c) False, since lim2 f (x) 5 0.
x→4
x→0
x→4
x→4
(d) True, since both are equal to 0.
(b) lim x f (x) 5 1 lim x21 lim f (x)2 5 4 ? 0 5 0
(e) True, since (d) is true.
(c) lim g (x) 5 1 lim g(x)2 5 32 5 9
x→4
x→4
2
x→4
(f) True
(g) False, since lim f (x) 5 0.
(d)
x→0
(h) False, lim2 f (x) 5 1, but lim f (x) is undefined.
x→1
x→1
g(x)
lim }}
x→4 f(x) 2 1
x→4
lim g(x)
x →4
3
}}}
5 lim f(x) 2 lim 1 5 }} 5 23
1
2 1
2 021
x→4
x→4
44. (a) lim (f (x) 1 g(x))5 1 lim f(x)2 1 1 lim g(x)2
x→b
x→b
x→b
5 7 1 (23) 5 4
(i) False, lim1 f (x) 5 0, but lim f (x) is undefined.
x→1
x→4
2
x→1
(b) lim ( f (x) ? g(x))5 1 lim f (x)21 lim g(x)2
(j) False, since lim2 f (x) 5 0.
x→b
x→b
x→2
x→b
5 (7)(23) 5 221
32. (a) True
(b) False, since lim f (x) 5 1.
(c) lim 4g(x) 5 4lim g(x) 5 4(23) 5 212
(c) False, since lim f (x) 5 1.
lim f (x)
7
7
f(x)
x→b
(d) lim }} 5 }
5 }} 5 2}}
lim g(x)
3
23
x→b g(x)
x→b
x→2
x→2
(d) True
x→b
x→b
(e) True
(f) True, since lim2 f (x) Þ lim1 f (x).
x→1
45. (a)
x→1
(g) True, since both are equal to 0.
(h) True
(i) True, since lim f (x) 5 1 for all c in (1, 3).
[23, 6] by [21, 5]
x→c
x 1x22
x21
2
(x 2 1)(x 1 2)
x21
33. y1 5 }} 5 }} 5 x 1 2, x Þ 1
(b) lim1 f (x) 5 2; lim2 f (x) 5 1
x→2
x→2
(c) No, because the two one-sided limits are different.
(c)
46. (a)
x2 2 x 2 2
x21
(x 1 1)(x 2 2)
x21
34. y1 5 }} 5 }}
(b)
x 2 2 2x 1 1
x21
(x 2 1)2
x21
[23, 6] by [21, 5]
35. y1 5 }} 5 }} 5 x 2 1, x Þ 1
(b) lim1 f (x) 5 1; lim2 f (x) 5 1
(d)
x→2
x2 1 x 2 2
x11
x→2
(c) Yes. The limit is 1.
(x 2 1)(x 1 2)
x11
36. y1 5 }} 5 }}
47. (a)
(a)
37. Since int x 5 0 for x in (0, 1), lim1 int x 5 0.
x→0
[25, 5] by [24, 8]
38. Since int x 5 21 for x in (21, 0), lim2 int x 5 21.
(b) lim1 f (x) 5 4; lim2 f (x) does not exist.
39. Since int x 5 0 for x in (0, 1), lim int x 5 0.
(c) No, because the left-hand limit does not exist.
x→0
x→0.01
x→1
x→1
48. (a)
40. Since int x 5 1 for x in (1, 2), lim2 int x 5 1.
x→2
x
)x)
x
41. Since }} 5 1 for x . 0, lim1 }} 5 1.
x→0 )x)
[24.7, 4.7] by [23.1, 3.1]
45
46
Section 2.1
48. continued
54.
(b) lim 1 f (x) 5 0; lim 2 f (x) 5 0
x→21
x→21
(c) Yes. The limit is 0.
49. (a)
[24.7, 4.7] by [25, 5]
lim (x 2 sin x) 5 0
x→0
Confirm using the Sandwich Theorem, with g(x) = 2x 2 and
h(x) 5 x 2.
)x 2 sin x) 5 )x 2) ? )sin x) # )x 2) ? 1 5 x 2.
2x 2 # x 2 sin x # x 2
[22p, 2p] by [22, 2]
(b) (22p, 0) < (0, 2p)
(c) c 5 2p
Because lim (2x 2) 5 lim x 2 5 0, the Sandwich Theorem
(d) c 5 22p
x→0
x→0
gives lim (x 2 sin x) 5 0
50. (a)
x→0
55.
[2p, p] by [23, 3]
p
2
p
2
[20.5, 0.5] by [20.25, 0.25]
(b) 12p, }}2 < 1}}, p2
(c) c 5 p
1
x
lim 1x 2 sin }}2 2 5 0
(d) c 5 2p
x→0
51. (a)
Confirm using the Sandwich Theorem, with g(x) 5 2x 2
and h(x) 5 x 2.
1
1
x 2 sin }}2 5 )x 2) ? sin }}2 # )x 2) ? 1 5 x 2.
)
x
)
)
x
)
1
2x # x sin }}2 # x 2
x
2
2
Because lim (2x 2) 5 lim x 2 5 0, the Sandwich Theorem
[22, 4] by [21, 3]
x→0
(b) (0, 1) < (1, 2)
(c) c 5 2
1
1
x
2
x→0
give lim x 2 sin }}2 5 0.
(d) c 5 0
x→0
56.
52. (a)
[20.5, 0.5] by [20.25, 0.25]
[24.7, 4.7] by [23.1, 3.1]
(b) (2`, 21) < (21, 1) < (1, `)
(c) None
(d) None
1
x
lim 1x 2 cos }}2 2 5 0
x→0
Confirm using the Sandwich Theorem, with g(x) 5 2x 2
and h(x) 5 x 2.
1
1
x2 cos }}2 5 )x2) ? cos }}2 # )x2) ? 1 5 x2.
53.
)
x
[24.7, 4.7] by [23.1, 3.1]
Confirm using the Sandwich Theorem, with g(x) 5 2)x)
and h(x) 5 )x).
)x sin x) 5 )x) ? )sin x) # )x) ? 1 5 )x)
2)x) # x sin x # )x)
Because lim (2)x)) 5 lim )x) 5 0, the Sandwich Theorem
x→0
gives lim (x sin x) 5 0.
x→0
)
x
)
2
Because lim (2x 2) 5 lim x 2 5 0, the Sandwich Theorem
x→0
lim (x sin x) 5 0
x→0
x→0
)
1
2x # x cos }}2 # x 2
x
2
1
x
x →0
give lim 1x 2 cos }}2 2 5 0.
x→0
57. (a) In three seconds, the ball falls 4.9(3)2 5 44.1 m, so its
44.1
3
average speed is }} 5 14.7 m/sec.
47
Section 2.1
(b) The average speed over the interval from time t 5 3 to
time 3 1 h is
4.9(3 1 h)2 2 4.9(3)2
Dy
4.9(6h 1 h2)
}} 5 }}} 5 }}
(3 1 h) 2 3
Dt
h
63. (a) Because the right-hand limit at zero depends only on
the values of the function for positive x-values near
zero.
1
2
1
2
sin u
2
(b) Area of nOAP 5 }}(base)(height) 5 }}(1)(sin u) 5 }}
5 29.4 1 4.9h
Since lim (29.4 1 4.9h) 5 29.4, the instantaneous
h→0
speed is 29.4 m/sec.
(angle)(radius)2
u(1)2
u
2
2
2
1
1
tan u
Area of nOAT 5 }}(base)(height) 5 }}(1)(tan u) 5 }}
2
2
2
Area of sector OAP 5 }} 5 }} 5 }}
(c) This is how the areas of the three regions compare.
58. (a)
y 5 gt
(d) Multiply by 2 and divide by sin u.
2
(e) Take reciprocals, remembering that all of the values
involved are positive.
20 5 g(42)
20
16
5
4
g 5 }} 5 }} or 1.25
(f) The limits for cos u and 1 are both equal to 1. Since
20
4
(b) Average speed 5 }} 5 5 m/sec
(c) If the rock had not been stopped, its average speed over
the interval from time t 5 4 to time t 5 4 1 h is
sin u
}} is between them, it must also have a limit of 1.
u
sin (2u)
2sin u
sin (u)
(g) }} 5 }} 5 }}
2u
2u
u
(h) If the function is symmetric about the y-axis, and the
right-hand limit at zero is 1, then the left-hand limit at
zero must also be 1.
1.25(4 1 h)2 2 1.25(4)2
Dy
1.25(8h 1 h2)
}} 5 }}} 5 }}
(4 1 h) 2 4
Dt
h
5 10 1 1.25h
Since lim (10 1 1.25h) 5 10, the instantaneous speed
h→0
(i) The two one-sided limits both exist and are equal to 1.
64. (a) The limit can be found by substitution.
is 10 m/sec.
lim f (x) 5 f (2) 5 Ï3w(2
w)w2
ww2 5 Ï4w 5 2
59. (a)
x→2
20.1
x
20.01
20.001
20.0001
f (x) 20.054402 20.005064 20.000827 20.000031
(b) The graphs of y1 5 f (x), y2 5 1.8, and y3 5 2.2 are
shown.
(b)
0.1
x
0.01
0.001
0.0001
f (x) 20.054402 20.005064 20.000827 20.000031
[1.5, 2.5] by [1.5, 2.3]
The limit appears to be 0.
60. (a)
(b)
x
20.1
f (x)
0.5440
x
0.1
20.01
20.001
20.0001
0.5064 20.8269
0.01
0.3056
0.001
0.0001
f (x) 20.5440 20.5064 0.8269 20.3056
The intersections of y1 with y2 and y3 are at
x < 1.7467 and x 5 2.28, respectively, so we may
choose any value of a in [1.7467, 2) (approximately)
and any value of b in (2, 2.28].
One possible answer: a 5 1.75, b 5 2.28.
(c) The graphs of y1 5 f (x), y2 5 1.99, and y3 5 2.01 are
shown.
There is no clear indication of a limit.
61. (a)
x
20.1
20.01 20.001 20.0001
f (x) 2.0567 2.2763 2.2999
(b)
x
0.1
0.01
0.001
2.3023
0.0001
[1.97, 2.03] by [1.98, 2.02]
f (x) 2.5893 2.3293 2.3052 2.3029
The limit appears to be approximately 2.3.
62. (a)
x
20.1
20.01
20.001
20.0001
f (x) 0.074398 20.009943 0.000585 0.000021
(b)
x
0.1
f (x) 20.074398
0.01
0.009943
The limit appears to be 0.
0.001
0.0001
20.000585 20.000021
The intersections of y1 with y2 and y3 are at x 5 1.9867
and x < 2.0134, respectively, so we may choose any
value of a in [1.9867, 2) and any value of b in
(2, 2.0134] (approximately).
One possible answer: a 5 1.99, b 5 2.01
48
Section 2.2
p
6
p
6
■ Section 2.2 Limits Involving Infinity
1
2
65. (a) f 1}}2 5 sin }} 5 }}
(b) The graphs of y1 5 f (x), y2 5 0.3, and y3 5 0.7 are
shown.
(pp. 65–73)
Exploration 1
Exploring Theorem 5
1. Neither lim f (x) or lim g(x) exist. In this case, we can
x→`
x→`
describe the behavior of f and g as x → ` by writing
lim f (x) 5 ` and lim g(x) 5 `. We cannot apply the
[0, 1] by [0, 1]
x→`
The intersections of y1 with y2 and y3 are at x < 0.3047
and x < 0.7754, respectively, so we may choose any
Example 5,
p
6
value of a in 30.3047, }}2 and any value of b in
1
p
}}, 0.7754 , where the interval endpoints are
6
4
approximate.
One possible answer: a 5 0.305, b 5 0.775
x→`
quotient rule because both limits must exist. However, from
5x 1 sin x
x
1
sin x
x
2
lim }} 5 lim 5 1 }} 5 5 1 0 5 5,
x→`
x→`
so the limit of the quotient exists.
2. Both f and g oscillate between 0 and 1 as x → `, taking on
each value infinitely often. We cannot apply the sum rule
because neither limit exists. However,
(c) The graphs of y1 5 f (x), y2 5 0.49, and y3 5 0.51 are
shown.
lim (sin2 x 1 cos2 x) 5 lim (1) 5 1,
x→`
x→`
so the limit of the sum exists.
3. The limt of f and g as x → ` do not exist, so we cannot
apply the difference rule to f 2 g. We can say that
lim f (x) 5 lim g(x) 5 `. We can write the difference as
[0.49, 0.55] by [0.48, 0.52]
x→`
The intersections of y1 with y2 and y3 are at x < 0.5121
and x < 0.5352, respectively, so we may choose any
3
p
6
2
value of a in 0.5121, }} , and any value of b in
1
p
}}, 0.5352 , where the interval endpoints are
6
4
approximate.
One possible answer: a 5 0.513, b 5 0.535
x→`
We can use graphs or tables to convince ourselves that this
limit is equal to ln 2.
4. The fact that the limits of f and g as x → ` do not exist
does not necessarily mean that the limits of f 1 g, f 2 g or
f
}} do not exist, just that Theorem 5 cannot be applied.
g
Quick Review 2.2
2
66. Line segment OP has endpoints (0, 0) and (a, a ), so its
0 1 a 0 1 a2
a a2
midpoint is }}, }} = }}, }} and its slope is
2
2
2 2
a2 2 0
}} 5 a. The perpendicular bisector is the line through
a20
a a2
1
}}, }} with slope 2}}, so its equation is
2 2
a
1
a
a2
y 5 2}} x 2 }} 1 }}, which is equivalent to
a
2
2
1 1 a2
1 1 a2
1
y 5 2}}x 1 }}. Thus the y-intercept is b 5 }}. As
a
2
2
1
1
2 1
2
2
1
2
1. y 5 2x 2 3
y 1 3 5 2x
y13
}} 5 x
2
Interchange x and y.
x13
}} 5 y
2
x13
2
f 21(x) 5 }}
the point P approaches the origin along the parabola, the
value of a approaches zero. Therefore,
1 1 a2
2
a→0
1 1 02
2
1
2
lim b 5 lim }} 5 }} 5 }}.
P→0
2x
x11
f (x) 2 g(x) 5 ln (2x) 2 ln (x 1 1) 5 ln }}.
[212, 12] by [28, 8]
Section 2.2
7. (a) f (2x) 5 cos (2x) 5 cos x
2. y 5 e x
ln y 5 x
Interchange x and y.
ln x 5 y
f 21(x) 5 ln x
1x2
1x2
1
1
(b) f }} 5 cos }}
8. (a) f (2x) 5 e2(2x) 5 e x
1x2
1
(b) f }} 5 e21/x
ln (2x)
x
ln (2x)
2x
9. (a) f (2x) 5 }} 5 2 }}
1x2
1
ln 1/x
1/x
(b) f }} 5 }} 5 x ln x21 5 2x ln x
[26, 6] by [24, 4]
1 2x 2
1
5 1x 1 }}2 sin x
x
3. y 5 tan x
p
2
p
2
tan y 5 x, 2}} , y , }}
1x2
1
p
2
tan x 5 y, 2}} , x , }}
p
2
p
2
1
1
x
1
1/x
1.
[25, 5] by [21.5, 1.5]
[26, 6] by [24, 4]
4. y 5 cot21x
cot y 5 x, 0 , x , p
Interchange x and y.
cot x 5 y, 0 , y , p
f 21(x) 5 cot x, 0 , x , p
(a) lim f (x) 5 1
x→`
(b) lim
x→ 2`
f (x) 5 1
(c) y 5 1
[26, 6] by [24, 4]
2.
2
}}
3
3x 3 1 4x 2 5q2ww
x 3w
2wx
3w2ww
1 wxw
2w1
8
3
10
3
5
3
7
3
2x3 1 0x2 1 }}x 2 }}
[210, 10] by [21, 1]
23x2 2 }}x 1 }}
2
3
q(x) 5 }}
5
3
7
3
r(x) 5 23x 2 2 }}x 1 }}
6.
2x2 1 2x 1 1
x 2 x 1 1qw2w
x 5w
1w0w
x 4ww
2 w
x 3w
1w0w
x 2ww
1 xw2
ww1
5
4
3
2x 2 2x 1 0x 1 2x2
2x4 2 x3 2 2x2 1 x 2 1
2x4 2 2x3 1 0x2 1 2x
x3 2 2x2 2 x 2 1
x3 2 x2 1 0x 1 1
2 x2 2 x 2 2
3
2
q(x) 5 2x 2 1 2x 1 1
r(x) 5 2x 2 2 x 2 2
2
Section 2.2 Exercises
f 21(x) 5 tan x, 2}} , x , }}
5.
1
x
2
1x2 1x
1
1
2
1x2
1
(b) f }} 5 }} 1 }} sin }} 5 }} 1 x sin }}
Interchange x and y.
p
2
1
1
10. (a) f (2x) 5 2x 1 }} sin (2x) 5 2 x 1 }} (2sin x)
21
(a) lim f (x) 5 0
x→`
(b) lim
x→ 2`
(c) y 5 0
f (x) 5 0
49
50
Section 2.2
3.
6.
[25, 5] by [210, 10]
[220, 20] by [24, 4]
(a) lim f (x) 5 2
(a) lim f (x) 5 0
x→`
x→`
(b) lim f (x) 5 22
x→2`
(b) lim f (x) 5 2`
(c) y 5 2, y 5 22
x→2`
(c) y 5 0
7.
4.
[25, 5] by [22, 2]
[210, 10] by [2100, 300]
(a) lim f (x) 5 1
x→`
(a) lim f (x) 5 `
(b) lim f (x) 5 21
x→`
(b) lim f (x) 5 `
x→2`
x→2`
(c) y 5 1, y 5 21
8.
(c) No horizontal asymptotes.
5.
[25, 5] by [22, 2]
[220, 20] by [24, 4]
(a) lim f (x) 5 1
x→`
(b) lim f (x) 5 1
(a) lim f (x) 5 3
x→`
(b) lim f (x) 5 23
x→2`
(c) y 5 3, y 5 23
x→2`
(c) y 5 1
Section 2.2
9.
13.
[22, 6] by [21, 5]
[24, 4] by [23, 3]
1
lim }} 5 `
10.
int x
x
lim }} 5 0
x→21 x22
x→01
14.
[22, 6] by [23, 3]
[24, 4] by [23, 3]
x
lim }} 5 2`
11.
int x
x
lim }} 5 `
x→22 x22
x→02
15.
[27, 1] by [23, 3]
[23, 3] by [23, 3]
1
lim }} 5 2`
lim csc x 5 `
x→232 x13
12.
x→01
16.
[27, 1] by [23, 3]
x
lim }} 5 2`
x→231 x13
[2p, p] by [23, 3]
lim
x→(p/2)1
sec x 5 2`
51
52
Section 2.2
17.
22.
[24, 4] by [23, 3]
[22p, 2p] by [23, 3]
p
2
(a) x 5 22, x 5 2
(a) x 5 }} 1 np, n any integer
(b) Left-hand limit at 22 is `.
Right-hand limit at 22 is 2`.
Left-hand limit at 2 is 2`.
Right-hand limit at 2 is `.
(b) If n is even:
Left-hand limit is `.
Right-hand limit is 2`.
If n is odd:
Left-hand limit is 2`.
Right-hand limit is `.
18.
2(x 1 1) 2 x
x
x2
x2
x11
x11 51x
51x
x12
x2
x 3 1 2x 2
5 }} }}2 5 }
}
3
x11 51x
x 1 x 2 1 5x 1 5
1
21
2 1
21
2
23. y 5 2 2 }} }}2 5 }} }}2
1
[27, 5] by [25, 3]
(a) x 5 22
(b) Left-hand limit at 22 is 2`.
Right-hand limit at 22 is `.
19.
21
2
x3
x
An end behavior model for y is }}3 5 1.
lim y 5 lim 1 5 1
x→`
x→`
lim y 5 lim 1 5 1
x→2`
x→2`
5x2 2 1
x
5x3 1 10x2 2 x 2 2
5 }}}
x3
1x
21
2
2 1
2 1 x 5x2 2 1
x
x
21
2
5 }} }}
24. y 5 }} 1 1 }}
2
2
[26, 6] by [212, 6]
(a) x 5 21
(b) Left-hand limit at 21 is 2`.
Right-hand limit at 21 is `.
5x3
x
An end behavior model for y is }}
3 5 5.
lim y 5 lim 5 5 5
20.
x→`
x→`
lim y 5 lim 5 5 5
x→2`
x→2`
25. Use the method of Example 10 in the text.
[22, 4] by [22, 2]
1
2
1x2
1
cos }}
(a) x 5 2}}, x 5 3
cos x
cos (0)
110
1
1
cos (0)
110
1
1
lim }
5 lim1 }} 5 }} 5 }} 5 1
1
1
2
(b) Left-hand limit at 2}} is `.
1
2
Right-hand limit at 2}} is 2`.
Left-hand limit at 3 is `.
Right-hand limit at 3 is 2`.
x→` 1 1 }}
x
x→0 1 1 x
1x2
1
cos }}
cos x
lim }
5 lim2 }} 5 }} 5 }} 5 1
1
x→2` 1 1 }}
x
x→0 1 1 x
2x 1 sin x
x
sin x
x
26. Note that y 5 }} 5 2 1 }}.
sin x
x
So, lim y 5 lim 2 1 lim }} 5 2 1 0 5 2.
21.
x→`
x→`
x→`
Similarly, lim y 5 2.
x→2`
[22p, 2p] by [23, 3]
(a) x 5 kp, k any integer
(b) at each vertical asymptote:
Left-hand limit is 2`.
Right-hand limit is `.
Section 2.2
sin x
2x 1 x
sin x
}} 5 0
x
1
}} 5 0
2x 1 1
sin x
x
41. (a, b) The function y 5 x is both a right end behavior
1
2x 1 1
27. Use y 5 }
2 } 5 }} ? }}
lim
x→6`
lim
x→6`
model and a left end behavior model because
lim
x→6`
So, lim y 5 0 and lim y 5 0.
x→`
1 sin x
x x
model and a left end behavior model because
28. y 5 2 }} 1 }} }}
x2 1 sin x
sin x
2
2
lim 11 1 }}2 5 1.
1}x}2 5x→6
x
x→6`
`
lim
So, lim y 5 0 and lim y 5 0.
x→`
ln )x)
42. (a, b) The function y 5 x 2 is both a right end behavior
x→2`
sin x
x
x 1 ln )x)
1}x}2 5lim
11 1 }x}2 5 1 1 0 5 1.
x→6`
x→2`
43.
2x3
x
29. An end behavior model is }} 5 2x 2. (a)
x5
2x
30. An end behavior model is }}2 5 0.5x 3. (c)
[24, 4] by [21, 3]
2x4
2x
31. An end behavior model is }} 5 22x 3. (d)
1
x
2x
32. An end behavior model is }}2 5 2x 2. (b)
33. (a) 3x
lim f (x) 5 lim1
x→`
2
x→0
lim2 f (x) 5 lim2
x→`
(b) None
34. (a) 24x
1x2 x
1
f 1}}2 5 `
x
1
f 1}}2 5 0
x
1
The graph of y 5 f }} 5 }}e 1/x is shown.
4
x→0
44.
3
(b) None
x
2x
1
2x
35. (a) }}2 5 }}
[24, 4] by [21, 3]
(b) y 5 0
1x2 x
1
lim f (x) 5 lim f 1}}2 5 0
x
x→`
x→0
1
lim f (x) 5 lim f 1}}2 5 `
x
x→2`
x→0
3x2
x
1
1
The graph of y 5 f }} 5 }}2 e 21/x is shown.
36. (a) }}
2 53
(b) y 5 3
1
4x3
37. (a) }} 5 4x 2
x
2
45.
(b) None
2x4
x
2
38. (a) }}
2 5 2x
(b) None
[23, 3] by [22, 2]
39. (a) The function y 5 e x is a right end behavior model
ex 2 2x
e
x→`
1
x→`
2x
e
2
because lim }}
5 lim 1 2 }}x 5 1 2 0 5 1.
x
(b) The function y 5 22x is a left end behavior model
ex 2 2x
x→2` 22x
ex
12}2}x 1 12 5 0 1 1 5 1.
x→2`
because lim }} 5 lim
1x2
)x)
1
lim f (x) 5 lim f 1}}2 5 0
x
x→`
x→0
1
lim f (x) 5 lim f 1}}2 5 0
x
x→2`
x→0
1
1
The graph of y 5 f }} 5 x ln }} is shown.
1
2
46.
40. (a) The function y 5 x is a right end behavior model
2
x2 1 e2x
x
e2x
x
1
2
because lim }}
5 lim 1 1 }}
2
2 5 1 1 0 5 1.
x→`
x→`
(b) The function y 5 e 2x is a left end behavior model
2x
x 1e
e
2
because lim }2x
} 5 lim
x→2`
2 x
1}} 1 12
x
2x
x→2` e
5 lim (x e 1 1) 5 0 1 1 5 1.
x→2`
2
[25, 5] by [21.5, 1.5]
1x2 x
1
lim f (x) 5 lim f 1}}2 5 1
x
x→`
x→0
1
lim f (x) 5 lim f 1}}2 5 1
x
x→2`
x→0
1
sin x
The graph of y 5 f }} 5 }} is shown.
1
2
53
54
Section 2.2
53. (a) Using 1980 as x 5 0:
y 5 22.2316x 3 1 54.7134x 2 2 351.0933x 1 733.2224
12
x→2` x
1
47. (a) lim f (x) 5 lim }} 5 0
x→2`
(b) lim f (x) 5 lim (21) 5 21
x→`
x→`
1
x
(c) lim2 f (x) 5 lim2 }} 5 2`
x→0
x→0
(d) lim1 f (x) 5 lim1(21) 5 21
x→0
x→0
x22
x→2` x 2 1
x
x→2` x
48. (a) lim f (x) 5 lim }} 5 lim }} 5 1
x→2`
[0, 20] by [0, 800]
(b) Again using 1980 as x 5 0:
y 5 1.458561x 4 2 60.5740x 3 1 905.8877x 2
2 5706.0943x 1 12967.6288
1
(b) lim f (x) 5 lim }}2 5 0
x→` x
x→`
x22
022
021
(c) lim2 f (x) 5 lim2 }} 5 }} 5 2
x→0 x 2 1
x→0
1
(d) lim1 f (x) 5 lim1 }}2 5 `
[0, 20] by [0, 800]
x→0 x
x→0
(c) Cubic: approximately 22256 dollars
Quartic: approximately 9979 dollars
49. One possible answer:
y
(d) Cubic: End behavior model is 22.2316x3.
This model predicts that the grants will
become negative by 1996.
5
y = f(x)
x
10
Quartic: End behavior model is 1.458561x4.
This model predicts that the size of the grants
will grow very rapidly after 1995.
Neither of these seems reasonable. There is no reason
to expect the grants to disappear (become negative)
based on the data. Similarly, the data give no indication
that a period of rapid growth is about to occur.
50. One possible answer:
54. (a) Note that fg 5 f (x)g(x) 5 1.
f → 2` as x → 02, f → ` as x → 01, g → 0, fg → 1
y
(b) Note that fg 5 f (x)g(x) 5 28.
f → ` as x → 02, f → 2` as x → 01, g → 0, fg → 28
5
y = f(x)
7
x
(c) Note that fg 5 f (x)g(x) 5 3(x 2 2)2.
f → 2` as x → 22, f → ` as x → 21, g → 0, fg → 0
5
(x 2 3)
(d) Note that fg 5 f (x)g(x) 5 }}2 .
f → `, g → 0, fg → `
(e) Nothing – you need more information to decide.
f1(x)g2(x)
f1(x)/g1(x)
f1(x)/f2(x)
51. Note that }
}5}
}5}
}.
g1(x)f2(x)
f2(x)/g2(x)
g1(x)/g2(x)
f
f
As x becomes large, }1} and }}2 both approach 1. Therefore,
g1
g2
f /f2
must also approach 1.
using the above equation, }1 }
g1/g2
52. Yes. The limit of ( f 1 g) will be the same as the limit of g.
This is because adding numbers that are very close to a
given real number L will not have a significant effect on the
value of ( f 1 g) since the values of g are becoming
arbitrarily large.
55. (a) This follow from x 2 1 , int x # x, which is true for
all x. Dividing by x gives the result.
x21
x
(b, c) Since lim }} 5 lim 1 5 1, the Sandwich
x→6`
x→6`
int x
x→` x
x→2`
int x
x
e2x
x
1
x
Theorem gives lim }} 5 lim }} 5 1.
56. For x . 0, 0 , e2x , 1, so 0 , }} , }}.
1
x
Since both 0 and }} approach zero as x → `, the Sandwich
e2x
x
Theorem states that }} must also approach zero.
57. This is because as x approaches infinity, sin x continues to
oscillate between 1 and 21 and doesn’t approach any given
real number.
ln x2
x→` ln x
ln x2
ln x
2 ln x
x
58. lim }} 5 2, because }} 5 }} 5 2.
Section 2.3
ln x
x→` log x
ln x
log x
55
(b) lim1 f (x) 5 lim1(4 2 x) 5 4 2 2 5 2
ln x
(ln x)/(ln 10)
59. lim }} 5 ln (10), since }} 5 }}
x→2
5 ln 10.
x→2
(c) lim f (x) does not exist, because the left- and
x→2
right-hand limits are not equal.
ln (x11)
ln x
x→`
60. lim }} 5 1
(d) f (2) 5 4 2 2 5 2
31
1
Since ln (x 1 1) 5 ln x 1 1 }}
x
1
1
24
1
2
1
5 ln x 1 ln 1 1 }} ,
x
2
1
1
2
ln x 1 ln 1 1 }}
ln 1 1 }}
x
x
ln (x 1 1)
}} 5 }} 5 1 1 }}
ln x
ln x
ln x
But as x → `, 1 1 1/x approaches 1, so ln(1 1 1/x)
approaches ln (1) 5 0. Also, as x → `, ln x approaches
infinity. This means the second term above approaches 0
and the limit is 1.
2
2
1
1
2
1
2x 2 1
2
1 11
(g + f )(x) 5 g( f (x)) 5 g }} 5 }
2x 2 1
x15
}}
x15
2x 2 1
3x 1 4
x15
5 }} 1 }} 5 }}, x Þ 25
2x 2 1
2x 2 1
2x 2 1
5. Note that sin x 2 5 (g + f )(x) 5 g( f (x)) 5 g(x 2).
Therefore: g(x) 5 sin x, x $ 0
( f + g)(x) 5 f (g(x)) = f (sin x) 5 (sin x)2 or sin2 x, x $ 0
■ Section 2.3 Continuity
(pp. 73–81)
Exploration 1
1
1
2 }} 1 1 2 1
x
1
4. ( f + g)(x) 5 f (g(x)) 5 f }} 1 1 5 }}
1
x
}} 1 1 1 5
x
2(1 1 x) 2 x
x12
5 }} 5 }}, x Þ 0
(1 1 x) 1 5x
6x 1 1
Removing a Discontinuity
1
x
6. Note that }} 5 (g + f )(x) 5 g( f (x)) 5 Ïf(
wx)
ww
2w1.
1. x 2 2 9 5 (x 2 3)(x 1 3). The domain of f is (2`, 23) <
(23, 3) < (3, `) or all x Þ 63.
Therefore, Ïf(
wx)
ww
2w1 5 }} for x . 0. Squaring both sides
2. It appears that the limit of f as x → 3 exists and is a little
more than 3.
gives f (x) 2 1 5 }}2 . Therefore, f (x) 5 }}2 1 1, x . 0.
1
x
1
x
1
x
1
1
( f + g)(x) 5 f (g(x)) 5 }} 1 15 }} 1 1
x21
(Ïxw2
ww1) 2
11x21
x
5 }} 5 }}, x . 1
x21
x21
7. 2x 2 1 9x 2 5 5 0
(2x 2 1)(x 1 5) 5 0
[23, 6] by [22, 8]
1
2
10
3
Solutions: x 5 }}, x 5 25
3. f (3) should be defined as }}.
4. x 3 2 7x 2 6 5 (x 2 3)(x 1 1)(x 1 2), x 2 2 9
(x 1 1)(x 1 2)
x13
(x 1 1)(x 1 2)
20
10
Thus, lim }} 5 }} 5 }}.
x13
6
3
x→3
10
5. lim g(x) 5 }} 5 g(3), so g is continuous at x 5 3.
3
x→3
8.
5 (x 2 3)(x 1 3), so f (x) 5 }} for x Þ 3.
Quick Review 2.3
3x 2 2x 1 1
x 14
2
3(21) 2 2(21) 1 1
(21) 1 4
2
6
3
1. lim }
5 }} 5 2
3
3 } 5 }}}
x→–1
2. (a) lim 2 f (x) 5 lim 2 int (x) 5 22
x→21
x→21
(b) lim 1 f (x) 5 lim 1 f (x) 5 21
x→21
x→21
(c) lim f (x) does not exist, because the left- and
x→21
right-hand limits are not equal.
(d) f(21) 5 int (21) 5 21
3. (a) lim2 f (x) 5 lim2(x 2 2 4x 1 5) 5 22 2 4(2) 1 5 5 1
x→2
x→2
[25, 5] by [210, 10]
Solution: x < 0.453
9. For x # 3, f (x) 5 4 when 5 2 x 5 4, which gives x 5 1.
(Note that this value is, in fact, # 3.)
For x . 3, f (x) 5 4 when 2x 2 1 6x 2 8 5 4, which gives
x 2 2 6x 1 12 5 0. The discriminant of this equation is
b 2 2 4ac 5 (26)2 2 4(1)(12) 5 212. Since the
discriminant is negative, the quadratic equation has no
solution.
The only solution to the original equation is x 5 1.
56
Section 2.3
10.
)x)
x
7. The function y 5 }} is equivalent to
y5
h
21,
1,
x,0
x . 0.
It has a jump discontinuity at x 5 0.
[22.7, 6.7] by [26, 6]
A graph of f (x) is shown. The range of f (x) is
(2`, 1) < [2, `). The values of c for which f (x) 5 c has
no solution are the values that are excluded from the range.
Therefore, c can be any value in [1, 2).
cos x
sin x
8. The function y 5 cot x is equivalent to y 5 }}, a quotient
of continuous functions, so it is continuous. Its only points
of discontinuity occur where it is undefined. It has infinite
discontinuities at x 5 kp for all integers k.
Section 2.3 Exercises
1
(x 1 2)
1. The function y 5 }}2 is continuous because it is a
9. The function y 5 e 1/x is a composition ( f + g)(x) of the
1
x
quotient of polynomials, which are continuous. Its only
continuous functions f (x) 5 e x and g(x) 5 }}, so it is
point of discontinuity occurs where it is undefined. There is
continuous. Its only point of discontinuity occurs at x 5 0,
an infinite discontinuity at x 5 22.
where it is undefined. Since lim1 e 1/x 5 `, this may be
x→0
x11
2. The function y 5 }
} is continuous because it is a
x 2 2 4x 1 3
quotient of polynomials, which are continuous. Its only
points of discontinuity occur where it is undefined, that is,
where the denominator x 2 2 4x 1 3 5 (x 2 1)(x 2 3) is
zero. There are infinite discontinuities at x 5 1 and at
x 5 3.
considered an infinite discontinuity.
10. The function y 5 ln (x 1 1) is a composition ( f + g)(x) of
the continuous functions f (x) 5 ln x and g(x) 5 x 1 1, so it
is continuous. Its points of discontinuity are the points not
in the domain, i.e., x , 21.
11. (a) Yes, f (21) 5 0.
(b) Yes, lim 1 5 0.
x→21
(c) Yes
1
x 11
3. The function y 5 }
2 } is continuous because it is a
quotient of polynomials, which are continuous.
(d) Yes, since 21 is a left endpoint of the domain of f and
f (x) 5 f (21), f is continuous at x 5 21.
lim
x→211
Furthermore, the domain is all real numbers because the
denominator, x 1 1, is never zero. Since the function is
12. (a) Yes, f (1) 5 1.
2
continuous and has domain (2`, `), there are no points of
discontinuity.
(b) Yes, lim f (x) 5 2.
x→1
(c) No
(d) No
4. The function y 5 )x 2 1) is a composition ( f + g)(x) of the
continuous functions f (x) 5 )x) and g(x) 5 x 2 1, so it is
continuous. Since the function is continuous and has
domain (2`, `), there are no points of discontinuity.
5. The function y 5 Ï2wxw1
ww3 is a composition ( f + g)(x) of
13. (a) No
(b) No, since x 5 2 is not in the domain.
14. Everywhere in [21, 3) except for x 5 0, 1, 2.
15. Since lim f (x) 5 0, we should assign f (2) 5 0.
x→2
the continuous functions f (x) 5 Ïxw and g(x) 5 2x 1 3, so
16. Since lim f (x) 5 2, we should reassign f (1) 5 2.
it is continuous. Its points of discontinuity are the points
17. No, because the right-hand and left-hand limits are not the
same at zero.
x→1
3
2
not in the domain, i.e., all x , 2}}.
3
6. The function y 5 Ï2wxw2
ww1 is a composition (f + g)(x) of
3
the continuous functions f (x) 5 Ïxw and g(x) 5 2x 2 1, so
it is continuous. Since the function is continuous and has
domain (2`, `), there are no points of discontinuity.
18. Yes. Assign the value 0 to f (3). Since 3 is a right endpoint
of the extended function and lim2 f (x) 5 0, the extended
x→3
function is continuous at x 5 3.
Section 2.3
19.
sin x
x
27. Since lim }} 5 1, the extended function is
h
x→0
sin x
}},
y5 x
1,
[23, 6] by [21, 5]
xÞ0
x 5 0.
sin 4x
x
sin 4x
4x
28. Since lim }} 5 4 lim }} 5 4(1) 5 4, the extended
(a) x 5 2
x→0
(b) Not removable, the one-sided limits are different.
function is
h
sin 4x
}},
x
y5
20.
x→0
4,
xÞ0
x 5 0.
29. For x Þ 4 (and x . 0),
(Ïxw 1 2)(Ïxw 2 2)
x24
f (x) 5 }} 5 }}} 5 Ïxw 1 2.
Ïxw 2 2
Ïxw 2 2
[23, 6] by [21, 5]
(a) x 5 2
(b) Removable, assign the value 1 to f (2).
The extended function is y 5 Ïxw 1 2.
21.
30. For x Þ 2 (and x Þ 22),
x3 2 4x 2 2 11x 1 30
x 24
(x 2 2)(x 2 5)(x 1 3)
5 }}}
(x 2 2)(x 1 2)
(x 2 5)(x 1 3)
5 }}
x12
x 2 2 2x 2 15
5 }}.
x12
f (x) 5 }}}
2
[25, 5] by [24, 8]
(a) x 5 1
(b) Not removable, it’s an infinite discontinuity.
22.
x 2 2 2x 2 15
x12
The extended function is y 5 }}.
31. One possible answer:
Assume y 5 x, constant functions, and the square root
function are continuous.
[24.7, 4.7] by [23.1, 3.1]
(a) x 5 21
(b) Removable, assign the value 0 to f (21).
23. (a) All points not in the domain along with x 5 0, 1
(b) x 5 0 is a removable discontinuity, assign f (0) 5 0.
x 5 1 is not removable, the one-sided limits are
different.
24. (a) All points not in the domain along with x 5 1, 2
(b) x 5 1 is not removable, the one-sided limits are
different.
x 5 2 is a removable discontinuity, assign f (2) 5 1.
x2 2 9
x13
(x 1 3)(x 2 3)
x13
25. For x Þ 23, f (x) 5 }} 5 }} 5 x 2 3.
The extended function is y 5 x 2 3.
x3 2 1
x 21
(x 2 1)(x 2 1 x 1 1)
5 }}}
(x 1 1)(x 2 1)
x2 1 x 1 1
5 }}.
x11
x2 1 x 1 1
The extended function is y 5 }}.
x11
26. For x Þ 1, f (x) 5 }
2 }
By the sum theorem, y 5 x 1 2 is continuous.
By the composite theorem, y 5 Ïxw1
ww2 is continuous.
1
By the quotient theorem, y 5 }} is continuous.
Ïxw1
ww2
Domain: (22, `)
32. One possible answer:
Assume y 5 x, constant functions, and the cube root
function are continuous.
By the difference theorem, y 5 4 2 x is continuous.
3
By the composite theorem, y 5 Ï4ww
2wx is continuous.
By the product theorem, y 5 x 2 5 x ? x is continuous.
3
By the sum theorem, y 5 x 2 1 Ïw4w
2wx is continuous.
Domain: (2`, `)
33. Possible answer:
Assume y 5 x and y 5 )x) are continuous.
By the product theorem, y 5 x 2 5 x ? x is continuous.
By the constant multiple theorem, y 5 4x is continuous.
By the difference theorem, y 5 x 2 2 4x is continuous.
By the composite theorem, y 5 )x 2 2 4x) is continuous.
Domain: (2`, `)
57
58
Section 2.3
34. One possible answer:
Assume y 5 x and y 5 1 are continuous.
39.
Use the product, difference, and quotient theorems. One
also needs to verify that the limit of this function as
x approaches 1 is 2.
Alternately, observe that the function is equivalent to
y 5 x 1 1 (for all x), which is continuous by the sum
theorem.
Domain: (2`, `)
[23, 3] by [22, 2]
Solving x 5 x 4 2 1, we obtain the solutions
x < 20.724 and x < 1.221.
40.
35. One possible answer:
y
5
y = f(x)
5
x
[26, 6] by [24, 4]
Solving x 5 x 3 1 2, we obtain the solution x < 21.521.
41. We require that lim1 2ax 5 lim2 (x 2 2 1):
x→3
x→3
2a(3) 5 32 2 1
6a 5 8
36. One possible answer:
y
4
3
a 5 }}
5
42. Consider f (x) 5 x 2 e 2x. f is continuous, f (0) 5 21, and
y = f(x)
5
x
1
e
f (1) 5 1 2 }} . 0.5. By the Intermediate Value Theorem,
for some c in (0, 1), f (c) 5 0 and e2c 5 c.
43. (a) Sarah’s salary is $36,500 5 $36,500(1.035)0 for the
first year (0 # t , 1), $36,500(1.035) for the second
year (1 # t , 2), $36,500(1.035)2 for the third year
(2 # t , 3), and so on. This corresponds to
y 5 36,500(1.035)int t.
37. One possible answer:
y
5
(b)
y = f(x)
5
x
[0, 4.98] by [35,000, 45,000]
The function is continuous at all points in the domain
[0, 5) except at t 5 1, 2, 3, 4.
38. One possible answer:
44. (a) We require:
y
5
y = f(x)
f(x) 5
5
x
{
0
1.10,
2.20,
3.30,
4.40,
5.50,
6.60,
7.25,
x50
0,x#1
1,x#2
2,x#3
3,x#4
4,x#5
5,x#6
6 , x # 24.
This may be written more compactly as
21.10 int(2x), 0 # x # 6
f (x) 5
7.25,
6 , x # 24
5
Section 2.4
59
49. For any real number a, the limit of this function as x
approaches a cannot exist. This is because as x approaches
a, the values of the function will continually oscillate
between 0 and 1.
(b)
Section 2.4 Rates of Change and
Tangent Lines (pp. 82–90)
■
[0, 24] by [0, 9]
This is continuous for all values of x in the domain
[0, 24] except for x 5 0, 1, 2, 3, 4, 5, 6.
1
x
45. (a) The function is defined when 1 1 }} . 0, that is, on
(2`, 21) < (0, `). (It can be argued that the domain
Quick Review 2.4
1. Dx 5 3 2 (25) 5 8
Dy 5 5 2 2 5 3
should also include certain values in the interval
2. Dx 5 a 2 1
Dy 5 b 2 3
(21, 0), namely, those rational numbers that have odd
3. m 5 }} 5 }} 5 2}}
denominators when expressed in lowest terms.)
21 2 3
5 2 (22)
24
7
3 2 (21)
3 2 (23)
4
6
4
7
2
3
4. m 5 }} 5 }} 5 }}
(b)
3
2
3
y 5 }}x 1 6
2
5. y 5 }}[x 2 (22)] 1 3
[25, 5] by [23, 10]
21 2 6
27
421
3
7
y 5 2}}(x 2 1) 1 6
3
7
25
y 5 2}}x 1 }}
3
3
(c) If we attempt to evaluate f (x) at these values, we obtain
1
1
1 21
5 021 5 }} (undefined) and
0
21
2
f (21) 5 1 1 }}
1 0
f (0) 5 1 1 }} (undefined). Since f is undefined at
0
1
2
7
3
6. m 5 }} 5 }} 5 2}}
3
4
3
19
y 5 2}}x 1 }}
4
4
7. y 5 2}}(x 2 1) 1 4
these values due to division by zero, both values are
points of discontinuity.
(d) The discontinuity at x 5 0 is removable because the
right-hand limit is 0. The discontinuity at x 5 21 is not
removable because it is an infinite discontinuity.
4
3
1
23/4
8. m 5 2}} 5 }}
4
3
4
8
y 5 }}x 1 }}
3
3
y 5 }}(x 2 1) 1 4
(e)
2
3
5
3
9. Since 2x 1 3y 5 5 is equivalent to y 5 2}}x 1 }}, we use
2
3
2
y 5 2}}[x 2 (21)] 1 3
3
2
7
y 5 2}}x 1}}
3
3
m 5 2}}.
[0, 20] by [0, 3]
10.
The limit is about 2.718, or e.
46. This is because lim f (a 1 h) 5 lim f (x).
h→0
x→a
47. Suppose not. Then f would be negative somewhere in the
interval and positive somewhere else in the interval. So, by
the Intermediate Value Theorem, it would have to be zero
somewhere in the interval, which contradicts the
hypothesis.
48. Since the absolute value function is continuous, this follows
from the theorem about continuity of composite functions.
b23
5
}} 5 }}
422
3
10
b 2 3 5 }}
3
19
b 5 }}
3
Section 2.4 Exercises
Df
Dx
f(3) 2 f (2)
322
Df
Dx
f(1) 2 f (21)
1 2 (21)
Df
Dx
f (2) 2 f (0)
220
28 2 9
1
1. (a) }} 5 }} 5 }} 5 19
220
2
(b) }} 5 }} 5 }} 5 1
321
2
2. (a) }} 5 }} 5 }} 5 1
w1w
f (12) 2 f (10)
7 2 Ï4
Df
(b) }} 5 }} 5 }} < 0.298
Dx
12 2 10
2
60
Section 2.4
1 2 e22
2
Df
Dx
f(0) 2 f (22)
0 2 (22)
Df
Dx
f(3) 2 f (1)
321
e3 2 e
2
Df
Dx
f(4) 2 f (1)
421
ln 4 2 0
3
Df
Dx
f(103) 2 f (100)
103 2 100
3. (a) }} 5 }} 5 }} < 0.432
9. (a)
4 2 4h 1 h2 2 4
h
h→0
5 lim }}
(b) }} 5 }} 5 }} < 8.684
24h 1 h2
h
h→0
ln 4
3
5 lim }}
4. (a) }} 5 }} 5 }} 5 }} < 0.462
ln 103 2 ln 100
3
1
3
103
100
5 lim (24 1 h)
(b) }} 5 }} 5 }} 5 }} ln }}
1
5 }} ln 1.03 < 0.0099
3
f (3p/4) 2 f (p/4)
21 2 1
Df
4
5. (a) }} 5 }} 5 }} 5 2}} < 21.273
(3p/4) 2 (p/4)
p/2
Dx
p
f (p/2) 2 f (p/6)
0 2 Ï3w
3Ï3w
Df
(b) }} 5 }} 5 }} 5 2 }} < 21.654
(p/2) 2 (p/6)
Dx
Df
Dx
f (p) 2 f (0)
p20
p/3
123
p
p
2
p
6. (a) }} 5 }} 5 }} 5 2}} < 20.637
h→0
= 24
(b) The tangent line has slope 24 and passes through
(22, y(22)) 5 (22, 4).
y 5 24[x 2 (22)] 1 4
y 5 24x 2 4
1
24
through (22, y(22)) 5 (22, 4).
1
4
1
9
y 5 }}x 1 }}
4
2
y 5 }}[x 2 (22)] 1 4
7. We use Q1 5 (10, 225), Q2 5 (14, 375), Q3 5 (16.5, 475),
Q4 5 (18, 550), and P 5 (20, 650).
650 2 225
20 2 10
650 2 375
Slope of PQ2: }} < 46
20 2 14
650 2 475
slope of PQ3: }} 5 50
20 2 16.5
650 2 550
Slope of PQ4: }} 5 50
20 2 18
(a) Slope of PQ1: }} < 43
Slope
PQ1
43
PQ2
46
PQ3
50
PQ4
50
(d)
[28, 7] by [21, 9]
y(1 1 h) 2 y(1)
h
[(1 1 h)2 2 4(1 1 h)] 2 [12 2 4(1)]
5 lim }}}}
h
h→0
10. (a) lim }}
h→0
1 1 2h 1 h2 2 4 2 4h 1 3
h
h→0
h2 2 2h
5 lim }}
h
h→0
5 lim }}}
5 lim (h 2 2)
The appropriate units are meters per second.
h→0
5 22
(b) Approximately 50 m/sec
8. We use Q1 5 (5, 20), Q2 5 (7, 38), Q3 5 (8.5, 56),
Q4 5 (9.5, 72), and P 5 (10, 80).
80 2 20
10 2 5
80 2 38
Slope of PQ2: }} 5 14
10 2 7
80 2 56
Slope of PQ3: }} 5 16
10 2 8.5
80 2 72
Slope of PQ4: }} 5 16
10 2 9.5
(a) Slope of PQ1: }} 5 12
Secant
Slope
PQ1
12
PQ2
14
PQ3
16
PQ4
16
The appropriate units are meters per second.
(b) Approximately 16 m/sec
1
4
(c) The normal line has slope 2}} 5 }} and passes
f (p) 2 f (2p)
121
Df
(b) }} 5 }} 5 }} 5 0
p 2 (2p)
2p
Dx
Secant
(22 1 h)2 2 (22)2
h
h→0
y(22 1 h) 2 y(22)
h
h→0
lim }}} 5 lim }}}
(b) The tangent line has slope 22 and passes through
(1, y(1)) 5 (1, 23).
y 5 22(x 2 1) 2 3
y 5 22x 2 1
1
22
1
2
(c) The normal line has slope 2}} 5 }} and passes
through (1, y(1)) 5 (1, 23).
1
2
1
7
y 5 }}x 2 }}
2
2
y 5 }}(x 2 1) 2 3
(d)
[26, 6] by [26, 2]
Section 2.4
1
11. (a)
1
}} 2 }}
(2 1 h) 2 1
221
y(2 1 h) 2 y(2)
lim }} 5 lim }}}
h
h
h→0
h→0
1
}} 2 1
h11
13. (a) Near x 5 2, f (x) 5 )x) 5 x.
1
1
h11
2
h→0
f(23 1 h) 2 f(23)
h
h→0
(3 2 h) 2 3
h
5 lim 21 5 21
5 lim }}
h→0
(2 1 h) 2 2
h
lim }}} 5lim }}
h→0
5 lim 2}}
h→0
(b) Near x 5 23, f(x) 5 )x) 5 2x.
h
1 2 (h 1 1)
h→0 h(h 1 1)
f(2 1 h) 2 f(2)
h
lim }} 5 lim }} 5 lim 1 5 1
h→0
5 lim }}
h→0
61
h→0
14. Near x 5 1, f (x) 5 )x 2 2) 5 2(x 2 2) 5 2 2 x.
[2 2 (1 1 h)] 2 (2 2 1)
f(1 1 h) 2 f(1)
h
h
h→0
12h21
5 lim }} 5 lim 21 5 21
h
h→0
h→0
lim }} 5 lim }}}
h→0
5 21
(b) The tangent line has slope 21 and passes through
(2, y(2)) 5 (2, 1).
y 5 2(x 2 2) 1 1
y 5 2x 1 3
15. First, note that f (0) 5 2.
f(0 1 h) 2 f(0)
h
h→0
(2 2 2h 2 h 2) 2 2
h
h→0
22h 2 h 2
5 lim2 }}
h
h→0
lim2 }} 5 lim2 }}
1
21
(c) The normal line has slope 2}} 5 1 and passes
through (2, y(2)) 5 (2, 1).
5 lim2 (22 2 h)
y 5 1(x 2 2) 1 1
5 22
h→0
y5x21
f(0 1 h) 2 f(0)
h
(2h 1 2) 2 2
h
lim }} 5 lim1 }}
h→01
(d)
h→0
5 lim1 2
h→0
52
No, the slope from the left is 22 and the slope from the
right is 2. The two-sided limit of the difference quotient
does not exist.
[24.7, 4.7] by [23.1, 3.1]
12. (a)
y(0 1 h) 2 y(0)
h
h→0
(h2 2 3h 2 1) 2 (21)
h
h→0
lim }} 5 lim }}}
h2 2 3h
h
h→0
5 lim }}
5 lim (h 2 3)
h→0
5 23
16. First, note that f(0) 5 0.
f (0 1 h) 2 f (0)
2h 2 0
h
h
h→0
f(0 1 h) 2 f(0)
(h2 2 h) 2 0
lim }} 5 lim1 }}
h
h
h→01
h→0
lim }} 5 lim2 }} 5 21
h→02
5 lim1 (h 2 1) 5 21
h→0
(b) The tangent line has slope 23 and passes through
1
2
17. First, note that f (2) 5 }}
(0, y(0)) 5 (0, 21).
y 5 23(x 2 0) 2 1
y 5 23x 2 1
1
23
1
3
(c) The normal line has slope 2}} 5 }} and passes
through (0, y(0)) 5 (0, 21).
1
3
1
y 5 }}x 2 1
3
y 5 }}(x 2 0) 2 1
(d)
[26, 6] by [25, 3]
Yes. The slope is 21.
1
1
}} 2 }}
21h
2
f(2 1 h) 2 f(2)
lim2 }} 5 lim2 }}
h
h
h→0
h→0
2 2 (2 1 h)
5 lim2 }}
2h(2 1 h)
h→0
2h
5 lim2 }}
h→0 2h(2 1 h)
1
5 lim2 2}}
2(2 1 h)
h→0
1
= 2}}
4
62
Section 2.4
17. continued
f(2 1 h) 2 f(2)
h
(b) The slope of the tangent steadily decreases as a
increases.
4 2 (2 1 h)
1
}} 2 }}
4
2
lim }} 5 lim1 }}
h→01
1
4
Yes. The slope is 2}}.
h
[4 2 (2 1 h)] 2 2
5 lim1 }}
4h
h→0
2h
5 lim1 }}
h→0 4h
1
52}}
4
23. Let f (t) 5 100 2 4.9t 2.
h→0
f(2 1 h) 2 f(2)
h
[100 2 4.9(2 1 h) 2] 2 [100 2 4.9(2) 2]
5 lim }}}}
h
h→0
100 2 19.6 2 19.6h 2 4.9h 2 2 100 1 19.6
5 lim }}}}}
h
h→0
lim }}
h→0
3p
4
5 lim (219.6 2 4.9h)
18. No. The function is discontinuous at x 5 }}
because lim
x→(3p/4)2
f(x) 5 lim
x→(3p/4)2
h→0
Ïw2
3p
4
sin x 5 sin }} 5 }}
The object is falling at a speed of 19.6 m/sec.
Ïw2
3p
3p
but f }} 5 cos }} 5 2}}.
142
19. (a)
4
2
f(a 1 h) 2 f(a)
h
h→0
[(a 1 h) 2 1 2] 2 (a 2 1 2)
h
a 2 1 2ah 1 h 2 1 2 2 a 2 2 2
}}}}
h
2ah 1 h 2
}}
h
lim }} 5 lim }}}
h→0
5 lim
h→0
5 lim
h→0
f(a 1 h) 2 f(a)
h
5 2a
5 60
h→0
}} 2 }}
a
a1h
lim }} 5 lim }}
h
2a 2 2(a 1 h)
5 lim }}
ah(a 1 h)
h→0
22
5 lim }}
h→0 a(a 1 h)
2
5 2} }2
a
h→0
(b) The slope of the tangent is always negative. The
tangents are very steep near x 5 0 and nearly
horizontal as a moves away from the origin.
1
(a 2 1) 2 (a 1 h 2 1)
5 lim }}}
h→0 h(a 2 1)(a 1 h 2 1)
1
(a 2 1)(a 1 h 2 1)
5 lim 2}}}
h→0
1
(a 2 1)
5 2}}2
(b) The slope of the tangent is always negative. The
tangents are very steep near x 5 1 and nearly
horizontal as a moves away from the origin.
[9 2 (a 1 h)2] 2 (9 2 a 2)
h
h→0
9 2 a 2 2 2ah 2 h 2 2 9 1 a 2
5 lim }}}}
h
h→0
22ah 2 h 2
5 lim }}
h
h→0
22. (a) lim }} 5 lim }}}
5 lim (22a 2 h)
h→0
5 22a
The rocket’s speed is 60 ft/sec.
25. Let f(r) 5 pr 2, the area of a circle of radius r.
f(3 1 h) 2 f(3)
h
p(3 1 h)2 2 p(3)2
h
9p 1 6ph 1 ph 2 2 9p
5 lim }}}
h
h→0
lim }} 5 lim }}
h→0
h→0
5 lim (6p 1 ph)
h→0
5 6p
The area is changing at a rate of 6p in2/in., that is,
6p square inches of area per inch of radius.
1
}} 2 }}
a1h21
a21
f(a 1 h) 2 f(a)
21. (a) lim }} 5 lim }}
h
h
h→0
h→0
f(a 1 h) 2 f(a)
h
h→0
f(10 1 h) 2 f(10)
3(10 1 h) 2 2 300
h
h
h→0
h→0
300 1 60h 1 3h 2 2 300
5 lim }}}
h
h→0
lim }} 5 lim }}
5 lim (60 1 3h)
(b) The slope of the tangent steadily increases as a
increases.
2
2
h→0
24. Let f (t) 5 3t 2.
5 lim (2a 1 h)
h→0
20. (a)
5 219.6
2
4
3
4
4
}}p(2 1 h)3 2 }}p(2)3
3
3
f(2 1 h) 2 f(2)
lim }} 5 lim }}}
h
h
h→0
h→0
4
(2 1 h)3 2 23
5 }}p lim }}
3 h→0
h
8 1 12h 1 6h 2 + h 32 8
4
5 }}p lim }}}
h
3 h→0
4
5 }}p lim (12 1 6h 1 h 2)
3 h→0
4
5 }}p ? 12
3
26. Let f (r) 5 }}pr 3.
5 16p
The volume is changing at a rate of 16p in3/in., that is, 16p
cubic inches of volume per inch of radius.
Section 2.4
s(1 1 h) 2 s(1)
h
h→0
1.86(1 1 h)2 2 1.86(1)2
h
h→0
1.86 1 3.72h 1 1.86h2 2 1.86
5 lim }}}}
h
h→0
27. lim }} 5 lim }}}
5 lim (3.72 1 1.86h)
h→0
5 3.72
The speed of the rock is 3.72 m/sec.
s(2 1 h) 2 s(2)
h
h→0
11.44(2 1 h)2 2 11.44(2)2
h
h→0
45.76 1 45.76h 1 11.44h 2 2 45.76
5 lim }}}}
h
h→0
28. lim }} 5 lim }}}
5 lim (45.76 1 11.44h)
h→0
5 45.76
The speed of the rock is 45.76 m/sec.
29. First, find the slope of the tangent at x 5 a.
f(a 1 h) 2 f(a)
h
[(a 1 h)2 1 4(a 1 h) 2 1] 2 (a 2 1 4a 2 1)
5 lim }}}}}
h
h→0
a 2 1 2ah 1 h 2 1 4a 1 4h 2 1 2 a 2 2 4a 1 1
5 lim }}}}}
h
h→0
2ah 1 h 2 1 4h
5 lim }}
h
h→0
lim }}
h→0
5 lim (2a 1 h 1 4)
h→0
5 2a 1 4
The tangent at x 5 a is horizontal when 2a 1 4 5 0, or
a 5 22. The tangent line is horizontal at
(22, f (22)) 5 (22, 25).
30. First, find the slope of the tangent at x 5 a.
f (a 1 h) 2 f (a)
h
h→0
[3 2 4(a 1 h) 2 (a 1 h)2] 2 (3 2 4a 2 a 2)
5 lim }}}}}
h
h→0
3 2 4a 2 4h 2 a 2 2 2ah 2 h 2 2 3 1 4a 1 a 2
5 lim }}}}}
h
h→0
lim }}
24h 22ah 2 h2
h
h→0
5 lim }}
5 lim (24 2 2a 2 h)
31. (a) From Exercise 21, the slope of the curve at x 5 a, is
1
(a 2 1)
1
2}}2 5 21, which gives (a 2 1)2 5 1, so a 5 0
(a 2 1)
1
or a 5 2. Note that y(0) 5 }} 5 21 and
021
1
y(2) 5 }} 5 1, so we need to find the equations of
221
2}}2 . The tangent has slope 21 when
lines of slope 21 passing through (0, 21) and (2, 1),
respectively.
At x 5 0: y 5 21(x 2 0) 2 1
y 5 2x 2 1
At x 5 2: y 5 21(x 2 2) 1 1
y 5 2x 1 3
(b) The normal has slope 1 when the tangent has slope
21
}} 5 21, so we again need to find lines through
1
(0, 21) and (2, 1), this time using slope 1.
At x 5 0: y 5 1(x 2 0) 2 1
y5x21
At x 5 2: y 5 1(x 2 2) 1 1
y5x21
There is only one such line. It is normal to the curve at
two points and its equation is y 5 x 2 1.
32. Consider a line that passes through (1, 12) and a point
(a, 9 2 a 2) on the curve. Using the result of Exercise 22,
this line will be tangent to the curve at a if its slope is 22a.
(9 2 a2) 2 12
}} 5 22a
a21
9 2 a 2 2 12
2a 2 2 3
a 2 2 2a 2 3
(a 1 1)(a 2 3)
a
5 22a(a 2 1)
5 22a 2 1 2a
50
50
5 21 or a 5 3
At a 5 21 (or x 5 21), the slope is 22(21) 5 2.
y 5 2(x 2 1) 1 12
y 5 2x 1 10
At a 5 3 (or x 5 3), the slope is 22(3) 5 26.
y 5 26(x 2 1) 1 12
y 5 26x 1 18
2.1 2 1.5
1995 2 1993
33. (a) }} 5 0.3
The rate of change was 0.3 billion dollars per year.
h→0
5 24 2 2a
The tangent at x 5 a is horizontal when 2 4 2 2a 5 0, or
a 5 22. The tangent line is horizontal at
(22, f (22)) 5 (22, 7).
63
3.1 2 2.1
1997 2 1995
(b) }} 5 0.5
The rate of change was 0.5 billion dollars per year.
(c) y 5 0.0571x 2 2 0.1514x 1 1.3943
[0, 10] by [0, 4]
64
Section 2.4
33. continued
y(5) 2 y(3)
523
y(7) 2 y(5)
}} < 0.53
725
(d) }} < 0.31
According to the regression equation, the rates were 0.31 billion dollars per year
and 0.53 billion dollars per year.
(e)
y(7 1 h) 2 y(7)
h
h→0
[0.0571(7 1 h)2 2 0.1514(7 1 h) 1 1.3943] 2 [0.0571(7)2 2 0.1514(7) 1 13943]
h
h→0
0.0571(14h 1 h 2) 2 0.1514h
5 lim }}}
h
h→0
lim }} 5 lim }}}}}}}}}
5 lim [0.0571(14) 2 0.1514 1 0.0571h]
h→0
< 0.65
The funding was growing at a rate of about 0.65 billion dollars per year.
34. (a)
[7, 18] by [0, 900]
(b) Q from year
Slope
4402225
}} < 23.9
17 2 8
440 2 289
}} < 18.9
17 2 9
440 2 270
}} < 24.3
17 2 10
440 2 493
}} < 28.8
17 2 11
440 2 684
}} 5 248.8
17 2 12
440 2 763
}} < 280.8
17 2 13
440 2 651
}} < 270.3
17 2 14
440 2 600
}} 5 280.0
17 2 15
440 2 296
}} 5 144.0
17 2 16
1988
1989
1990
1991
1992
1993
1994
1995
1996
(c) As Q gets closer to 1997, the slopes do not seem to be approaching a limit value.
The years 1995–97 seem to be very unusual and unpredictable.
f (1 1 h) 2 f (1)
h
e11h 2 e
h
35. (a) }} 5 }}
(b)
[24, 4] by [21, 5]
Limit < 2.718
(c) They’re about the same.
(d) Yes, it has a tangent whose slope is about e.
Section 2.4
f(1 1 h) 2 f(1)
h
211h 2 2
h
f (0 1 h) 2 f (0)
36. (a) }} 5 }}
65
f(h)
40. Let f (x) 5 x2/3. The graph of y 5 }} 5 }}
h
h
is shown.
(b)
[24, 4] by [21, 5]
[24, 4] by [23, 3]
The left- and right-hand limits are 2` and `, respectively.
Since they are not the same, the curve does not have a
vertical tangent at x 5 0. No.
41. This function has a tangent with slope zero at the origin. It
is sandwiched between two functions, y 5 x 2 and y 5 2x 2,
both of which have slope zero at the origin.
Limit < 1.386
(c) They’re about the same.
Looking at the difference quotient,
(d) Yes, it has a tangent whose slope is about ln 4.
f (0 1 h) 2 f (0)
h
f(h)
h
37. Let f (x) 5 x 2/5. The graph of y 5 }} 5 }}
is shown.
f(0 1 h) 2 f(0)
h
2h # }} # h,
so the Sandwich Theorem tells us the limit is 0.
42. This function does not have a tangent line at the origin. As
the function oscillates between y 5 x and y 5 2x infinitely
often near the origin, there are an infinite number of
difference quotients (secant line slopes) with a value of 1
and with a value of 21. Thus the limit of the difference
quotient doesn’t exist.
[24, 4] by [23, 3]
The left- and right-hand limits are 2` and `, respectively.
Since they are not the same, the curve does not have a
vertical tangent at x 5 0. No.
f (0 1 h) 2 f (0)
f(h)
38. Let f (x) 5 x 3/5. The graph of y 5 }} 5 }}
h
h
is shown.
f(0 1 h) 2 f(0)
h
1
h
The difference quotient is }} 5 sin }} which
oscillates between 1 and 21 infinitely often near zero.
43. Let f (x) 5 sin x. The difference quotient is
sin (1 1 h) 2 sin (1)
f(1 1 h) 2 f(1)
.
}} 5 }}}
h
h
A graph and table for the difference quotient are shown.
[24, 4] by [23, 3]
Yes, the curve has a vertical tangent at x 5 0 because
f (0 1 h) 2 f (0)
h
[24, 4] by [21.5, 1.5]
lim }} 5 `.
h→0
f (0 1 h) 2 f (0)
f(h)
39. Let f(x) 5 x1/3. The graph of y 5 }} 5 }}
h
h
is shown.
Since the limit as h→0 is about 0.540, the slope of
y 5 sin x at x 5 1 is about 0.540.
[24, 4] by [23, 3]
Yes, the curve has a vertical tangent at x 5 0 because
f (0 1 h) 2 f (0)
h
lim }} 5 `.
h→0
66
Chapter 2 Review
13. Since lim (2e 2x) 5 lim e 2x 5 0, and
■ Chapter 2 Review Exercises
x→`
gives lim e 2x cos x 5 0.
1. lim (x 3 2 2x 2 1 1) 5 (22)3 2 2(22)2 1 1 5215
x→`
x→22
(22)2 1 1
3(22) 2 2(22) 1 5
x2 1 1
x→−2 3x 2 2x 1 5
14. Since the expression x is an end behavior model for both
5
21
2. lim }
5 }}
} 5 }}}
2
2
3. No limit, because the expression Ï1ww
2w2xw is undefined for
values of x near 4.
4
2wx w is undefined for
4. No limit, because the expression Ï9ww
values of x near 5.
2
1
1
}} 2 }}
21x
2
1
2x 1 3
2x
x→6` 5x 1 7
x→6` 5x
2
15. Limit exists.
16. Limit exists.
17. Limit exists.
20. Limit exists.
21. Yes
22. No
2
5
6. lim }
2 } 5 lim } }
2 5 }}
23. No
x4 1 x3
12x 1 128
x4
12x
1
12
7. An end behavior model for }
3 } is }}
3 5 }}x.
24. Yes
25. (a) lim2 g(x) 5 1
x→3
Therefore:
(b) g(3) 5 1.5
x4 1 x3
1
x→` 12x 1 128
x→` 12
x 4 1 x3
1
lim }
3 } 5 lim }}x 5 2`
x→2` 12x 1 128 x→2` 12
lim }
3 } 5 lim }}x 5 `
sin 2x
4x
1
sin 2x
2 x→0 2x
(c) No, since lim2 g(x) Þ g(3).
x→3
1
2
(d) g is discontinuous at x 5 3 (and at points not in the
domain).
1
2
8. lim }} 5 }} lim }} 5 }}(1) 5 }}
(e) Yes, the discontinuity at x 5 3 can be removed by
assigning the value 1 to g(3).
9. Multiply the numerator and denominator by sin x.
x csc x 1 1
x 1 sin x
sin x
lim }} 5 lim }} 5 lim 1 1 }}
x csc x
x
x
x→0
x→0
x→0
sin x
5 lim 1 1 lim }} 5 1 1 1 5 2
x→0
x→0 x
1
1
x
x→` x
19. Limit exists.
2
2
x 1 sin x
x→` x 1 cos x
x 1 sin x and x 1 cos x, lim } 5 lim }} 5 1.
18. Limit does not exist.
2 2 (2 1 x)
2x
x
x→0
x→0 2x(2 1 x)
x→0 2x(2 1 x)
1
1
1
5 lim 2}} 5 2}} 5 2}}
4
2(2 1 x)
2(2 1 0)
x→0
5. lim }} 5 lim }} 5 lim }}
x→0
x→`
2e 2x # e2x cos x # e2x for all x, the Sandwich Theorem
(pp. 91–93)
2 1
2
26. (a) lim2 k(x) 5 1.5
x→1
(b) lim1 k(x) 5 0
2
x→1
(c) k(1) 5 0
10. lim e x sin x 5 e 0 sin 0 5 1 ? 0 5 0
(d) No, since lim2 k(x) Þ k(1)
x→0
x→1
(e) k is discontinuous at x 5 1 (and at points not in the
domain).
1 22
7
int (2x 2 1) 5 int 321}}2 1 2h – 14 5 int (6 1 2h) 5 6,
2
7
2
1
11. Let x 5 }} 1 h, where h is in 0, }} . Then
(f) No, the discontinuity at x 5 1 is not removable because
the one-sided limits are different.
27.
because 6 1 2h is in (6, 7).
Therefore, lim 1 int (2x – 1) 5 lim 16 5 6.
x→7/2
x→7/2
7
2
1
1
2
2
12. Let x 5 }} 1 h, where h is in 2}}, 0 . Then
3 122
7
4
int (2x 2 1) 5 int 2 }} 1 2h 2 1 5 int (6 1 2h) 5 5,
because 6 1 2h is in (5, 6).
x13
(b) Left-hand limit 5 lim 2 }} 5 2`
x→–2 x 1 2
x13
Right-hand limit: lim 1 }} 5 `
Therefore, lim 2 int (2x 2 1) 5 lim 2 5 5 5
x→7/2
[24, 4] by [23, 3]
(a) Vertical asymptote: x 5 22
x→7/2
x→–2 x 1 2
Chapter 2 Review
2x
x
28.
67
2
x
33. (a) End behavior model: }}2 , or }}
(b) Horizontal asymptote: y 5 0 (the x-axis)
2x2
x
34. (a) End behavior model: }}
2 , or 2
[24, 4] by [23, 3]
(a) Vertical asymptotes: x 5 0, x 5 22
(b) Horizontal asymptote: y 5 2
x3
x
35. (a) End behavior model: }}, or x 2
(b) At x 5 0:
x21
x→0 x (x 1 2)
x21
Right-hand limit 5 lim1 }
2 } 5 2`
x→0 x (x 1 2)
Left-hand limit 5 lim2 }
2 } 5 2`
At x 5 22:
x21
x→–2 x (x 1 2)
x21
Right-hand limit 5 lim 1 }
2 } 5 2`
x→–2 x (x 1 2)
Left-hand limit 5 lim 2 }
2 }5`
(b) Since the end behavior model is quadratic, there are no
horizontal asymptotes.
x4
x
36. (a) End behavior model: }}3 , or x
(b) Since the end behavior model represents a
nonhorizontal line, there are no horizontal asymptotes.
x 1 ex
e
x→`
1e
2
x
37. (a) Since lim }}
5 lim }}x 1 1 5 1, a right end
x
x→`
x
behavior model is e .
29. (a) At x 521:
Left-hand limit 5 lim 2 f (x) 5 lim 2 (1) 5 1
x→21
x→21
x→2`
Right-hand limit 5 lim 1 f (x) 5 lim 1 (2x) 5 1
x→21
x 1 ex
x
11 1 }x}2 5 1, a left end
ex
(b) Since lim }} 5 lim
x→2`
behavior model is x.
x→21
At x 5 0:
Left-hand limit 5 lim2 f (x) 5 lim2 (2x) 5 0
x→0
x→6`
x→0
12}ln})x) 2 5 lim 1}ln})x) 2 5 0 and
1
38. (a, b) Note that lim
sin x
ln)x)
1
ln)x)
1
x→6`
1
ln)x)
Right-hand limit 5 lim1 f (x) 5 lim1 (2x) 5 0
2}} , }} , }} for all x Þ 0.
At x 5 1:
Therefore, the Sandwich Theorem gives
x→0
x→0
Left-hand limit 5 lim2 f (x) 5 lim2 (2x) 5 21
x→1
x→1
Right-hand limit 5 lim1 f (x) 5 lim1 (1) 5 1
x→1
sin x
lim }} 5 0. Hence
x→6` ln)x)
(b) At x 5 21: Yes, the limit is 1.
At x 5 0: Yes, the limit is 0.
At x 5 1: No, the limit doesn’t exist because the two
one-sided limits are different.
(c) At x 5 21: Continuous because f (21) 5 the limit.
At x 5 0: Discontinuous because f (0) Þ the limit.
At x 5 1: Discontinuous because the limit does not
exist.
ln)x) 1 sin x
sin x
1 1 }} 5 1 1 0 5 1,
ln)x)
ln)x)
x→6`
lim }} = lim
x→1
x→6`
1
2
so ln)x) is both a right end behavior model and a left
end behavior model.
x2 1 2x – 15
x–3
x→3
(x – 3)(x 1 5)
x–3
39. lim f(x) 5 lim }} 5 lim }}
x→3
x→3
5 lim (x 1 5) 5 3 1 5 5 8.
x→3
30. (a) Left-hand limit 5 lim2 f (x) 5 lim2 )x 3 2 4x)
x→1
x→1
5 )(1)3 2 4(1)) 5 )23) 5 3
sin x
2x
1
sin x
2 x→0 x
1
2
1
2
40. lim f(x) 5 lim }} 5 }} lim }} 5 }}(1) 5 }}
Right-hand limit 5 lim1 f (x) 5 lim1 (x 2 2 2x 2 2)
x→1
Assign the value k 5 8.
x→1
5 (1)2 2 2(1) 2 2 5 23
x→0
x→0
41. One possible answer:
(b) No, because the two one-sided limits are different.
(c) Every place except for x 5 1
(d) At x 5 1
31. Since f(x) is a quotient of polynomials, it is continuous and
its points of discontinuity are the points where it is
undefined, namely x 5 22 and x 5 2.
32. There are no points of discontinuity, since g(x) is
continuous and defined for all real numbers.
1
2
Assign the value k 5 }}.
y
10
y = f(x)
10
x
68
Chapter 2 Review
48. At x 5 a, the slope of the curve is
42. One possible answer:
y
[(a 1 h)2 2 3(a 1 h)] 2 (a 2 2 3a)
h
h→0
f (a 1 h) 2 f (a)
h
h→0
lim }} 5 lim }}}}
5
a 2 1 2ah 1 h 2 2 3a – 3h 2 a 2 1 3a
h
h→0
2ah 2 3h 1 h 2
5 lim }}
h
h→0
5 lim }}}}
5
x
y = f(x)
5 lim (2a 2 3 1 h)
h→0
5 2a 2 3
f (p/2) – f (0)
p/2 – 0
221
p/2
3
2
The tangent is horizontal when 2a 2 3 5 0, at a 5 }}
2
p
43. }} 5 }} 5 }}
1
1
}}p(a 1 h)2H 2 }}pa 2H
3
3
V(a 1 h) 2 V(a)
h
h→0
a 2 1 2ah 1 h 2 2 a 2
1
5 }}pH lim }}}
h
3
h→0
1
5 }}pH lim (2a 1 h)
3
h→0
1
5 }}pH(2a)
3
2
5 }}paH
3
44. lim }} 5 lim }}}
h→0
h
6(a 1 h)2 2 6a2
S(a 1 h) 2 S(a)
h
h
h→0
h→0
2
2
2
6a 1 12ah 1 6h 2 6a
5 lim }}}
h
h→0
45. lim }} 5 lim }}
5 lim (12a 1 6h)
1or x 5 }2}2. Since f 1}2}2 5 2}4}, the point where this occurs
3
9
is }}, 2}} .
12 42
3
3
9
200
1 1 7e
200
8
49. (a) p(0) 5 }}
20.1(0) 5 }} 5 25
Perhaps this is the number of bears placed in the
reserve when it was established.
200
1
200
(b) lim p(t) 5 lim }}
20.1t 5 }} 5 200
t→` 1 1 7e
t→`
(c) Perhaps this is the maximum number of bears which
the reserve can support due to limitations of food,
space, or other resources. Or, perhaps the number is
capped at 200 and excess bears are moved to other
locations.
3.20 2 1.35 int (2x 1 1), 0 , x # 20
50. (a) f (x) 5
0,
x50
h
h→0
(Note that we cannot use the formula
f (x) 5 3.20 1 1.35 int x, because it gives incorrect
results when x is an integer.)
5 12a
y(a 1 h) 2 y(a)
h
[(a 1 h)2 2 (a 1 h) 2 2] 2 (a 2 2 a 2 2)
5 lim }}}}}
h
h→0
a 2 1 2ah 1 h 2 2 a 2 h 2 2 2 a 2 1 a 1 2
5 lim }}}}}
h
h→0
2ah 1 h 2 2 h
5 lim }}
h
h→0
46. lim }}
(b)
h→0
5 lim (2a 1 h 2 1)
h→0
5 2a 2 1
[(1 1 h)2 2 3(1 1 h)] 2 (22)
f (1 1 h) 2 f (1)
h
h
h→0
h→0
1 1 2h 1 h 2 2 3 2 3h 1 2
5 lim }}}
h
h→0
47. (a) lim }} 5 lim }}}}
5 lim (21 1 h)
h→0
5 21
(b) The tangent at P has slope 21 and passes through
(1, 22).
y 5 21(x 2 1) 2 2
y 5 2x 2 1
(c) The normal at P has slope 1 and passes through
(1, 22).
y 5 1(x 2 1) 2 2
y5x23
[0, 20] by [25, 32]
f is discontinuous at integer values of x: 0, 1, 2, ..., 19.
51. (a) Cubic: y 5 21.644x 3 1 42.981x 2 2 254.369x
1 300.232
Quartic: y 5 2.009x 4 2 102.081x 3 1 1884.997x 2
2 14918.180x 1 43004.464
(b) Cubic: 21.644x 3, predicts spending will go to 0
Quartic: 2.009x 4, predicts spending will go to `
52. Let A 5 lim f (x) and B 5 lim g(x). Then A 1 B 5 2 and
x→c
x→c
3
2
A 2 B 5 1. Adding, we have 2A 5 3, so A 5 }}, whence
3
1
3
}} 1 B 5 2, which gives B 5 }}. Therefore, lim f (x) 5 }}
2
2
2
x→c
1
and lim g(x) 5 }}.
2
x→c
53. (a)
[3, 12] by [22, 24]
Section 3.1
(b) Year of Q
69
Slope of PQ
20.1 2 2.7
}} 5 3.48
2000 2 1995
20.1 2 4.8
}} 5 3.825
2000 2 1996
20.1 2 7.8
}} 5 4.1
2000 2 1997
20.1 2 11.2
}} 5 4.45
2000 2 1998
20.1 2 15.2
}} 5 4.9
2000 2 1999
1995
1996
1997
1998
1999
(c) Approximately 5 billion dollars per year.
(d) y 5 0.3214x 2 2 1.3471x 1 1.3857
[0.3214(10 1 h) 2 2 1.3471(10 1 h) 1 1.3857] 2 [0.3214(10)2 2 1.3471(10) 1 1.3857]
y(10 1 h) 2 y(10)
lim }} 5 lim }}}}}}}}}
h
h→0
h
h→0
0.3214(20h 1 h 2) 2 1.3471h
h
h→0
5 lim }}}
5 0.3214(20) 2 1.3471
< 5.081
The predicted rate of change in 2000 is about
5.081 billion dollars per year.
Chapter 3
Derivatives
■ Section 3.1 Derivative of a Function (pp. 95–104)
Exploration 1
Reading the Graphs
1. The graph in Figure 3.3b represents the rate of change of the depth of the water in the puddle with respect to time. Since y is
dy
dx
measured in inches and x is measured in days, the derivative }} would be measured in inches per day. Those are the units that
should be used along the y-axis in Figure 3.3b.
2. The water in the ditch is 1 inch deep at the start of the first day and rising rapidly. It continues to rise, at a gradually decreasing
rate, until the end of the second day, when it achieves a maximum depth of 5 inches. During days 3, 4, 5, and 6, the water level
goes down, until it reaches a depth of 1 inch at the end of day 6. During the seventh day it rises again, almost to a depth of
2 inches.
3. The weather appears to have been wettest at the beginning of day 1 (when the water level was rising fastest) and driest at the end
of day 4 (when the water level was declining the fastest).
4. The highest point on the graph of the derivative shows where the water is rising the fastest, while the lowest point (most
negative) on the graph of the derivative shows where the water is declining the fastest.
5. The y-coordinate of point C gives the maximum depth of the water level in the ditch over the 7-day period, while the
x-coordinate of C gives the time during the 7-day period that the maximum depth occurred. The derivative of the function
changes sign from positive to negative at C 9, indicating that this is when the water level stops rising and begins falling.
6. Water continues to run down sides of hills and through underground streams long after the rain has stopped falling. Depending
on how much high ground is located near the ditch, water from the first day’s rain could still be flowing into the ditch several
days later. Engineers responsible for flood control of major rivers must take this into consideration when they predict when
floodwaters will “crest,” and at what levels.
70
Section 3.1
Quick Review 3.1
h→0
(2 1 h}
)2 2 4 5 lim }
(4 1 4h 1}
h 2) 2 4
1. lim }
4
h
h→0
f (3 1 h) 2 f (3)
h
2. f 9(3) 5 lim }}
1
1
}} 2 }}
3
31h
h→0
5 lim }}
5 lim 4 1 h
h
h→0
h→0
541054
3 2 (3 1 h)
5 lim }}
h→0 3h(3 1 h)
x 1}
35}
2 1}
3 5 }5}
2. lim+ }
2
2
2
21
1
9
5 lim }} 5 2}}
x→2
)y)
)y)
y
y→0 y
h→0 3(3 1 h)
3. Since }} 5 21 for y , 0, lim2}} 5 21.
2(Ïxw 1 2)(Ïxw 2 2)
2x 2 8
x→3
1
1
}} 2 }}
x
3
5 lim }
h→4
x→3 x 2 3
5. The vertex of the parabola is at (0, 1). The slope of the line
32x
5 lim }}
x→3 (x 2 3)(x)(3)
through (0, 1) and another point (h, h 1 1) on the parabola
2
(h 2 1 1) 2 1
h20
is }} 5 h. Since lim h 5 0, the slope of the line
x→3
x→1
lim f (x) 5 lim2 (x 1 2) 5 1 1 2 5 3
x→12
h→0
h→0
h→0
3h
5 lim }} 5 lim 3 5 3
h→0 h
dy
dx
h→0
y(x 1 h) 2 y(x)
h
7(x 1 h) 2 7x
}}
h
7h
}} 5 lim 7 5 7
h
h→0
5. }} 5 lim }}
h→0
h→0
5 lim
8. lim1 f (1 1 h) 5 lim1 f (x) 5 0
[3(x 1 h) 2 12] 2 (3x 2 12)
5 lim }}}
h
5 lim
x→1
f (x 1 h) 2 f (x)
h
4. f 9(x) 5 lim }}
6. Use the graph of f in the window [26, 6] by [24, 4] to find
that (0, 2) is the coordinate of the high point and (2, 22) is
the coordinate of the low point. Therefore, f is increasing
on (2`, 0] and [2, `).
7. lim1 f (x) 5 lim1 (x 2 1)2 5 (1 2 1)2 5 0
1
9
1
3x
5 lim 2}} 5 2}}
h→0
tangent to the parabola at its vertex is 0.
x→1
f (x) 2 f (3)
x23
3. f 9(3) 5 lim }}
4. lim }} 5 lim }}}
Ïxw 2 2
x→4 Ïx
w 2 2 x→4
5 lim 2(Ïwx 1 2) 5 2(Ï4w 1 2) 5 8
h→0
x→1
9. No, the two one-sided limits are different (see Exercise 7).
10. No, f is discontinuous at x 5 1 because lim f (x) does not
x→1
exist.
Section 3.1 Exercises
1. (a) The tangent line has slope 5 and passes through (2, 3).
y 5 5(x 2 2) 1 3
y 5 5x 2 7
1
5
(b) The normal line has slope 2}} and passes through
(2, 3).
1
5
1
17
y 5 2}}x 1 }}
5
5
y 5 2}}(x 2 2) 1 3
6. Let f (x) 5 x 2.
f (x 1 h) 2 f (x)
d
}}(x 2) 5 f 9(x) 5 lim }}
h
dx
h→0
(x 1 h)2 2 x 2
5 lim }}
h
h→0
x 2 1 2xh 1 h 2 2 x 2
5 lim }}}
h
h→0
5 lim (2x 1 h) 5 2x
h→0
7. The graph of y 5 f1(x) is decreasing for x , 0 and
increasing for x . 0, so its derivative is negative for x , 0
and positive for x . 0. (b)
8. The graph of y 5 f2(x) is always increasing, so its derivative
is always $ 0. (a)
9. The graph of y 5 f3(x) oscillates between increasing and
decreasing, so its derivative oscillates between positive and
negative. (d)
10. The graph of y 5 f4(x) is decreasing, then increasing , then
decreasing, and then increasing, so its derivative is
negative, then positive, then negative, and then positive. (c)
Section 3.1
dy
dx
y(x 1 h) 2 y(x)
h
[2(x 1 h)2 2 13(x 1 h) 1 5] 2 (2x 2 2 13x 1 5)
}}}}}
h
2x 2 1 4xh 1 2h 2 2 13x 2 13h 1 5 2 2x 2 1 13x 2 5
}}}}}}
h
4xh 1 2h 2 2 13h
}}
h
11. }} 5 lim }}
h→0
5 lim
h→0
5 lim
h→0
5 lim
h→0
5 lim (4x 1 2h 2 13) 5 4x 2 13
h→0
dy
dx
At x 5 3, }} 5 4(3) 2 13 5 21, so the tangent line has
slope 21 and passes through (3, y(3)) 5 (3, 216).
y 5 21(x 2 3) 2 16
y 5 2x 2 13
12. Let f (x) 5 x 3.
f (1 1 h) 2 f (1)
h
(1 1 h)3 2 13
}}
h
1 1 3h 1 3h 2 1 h 3 2 1
}}}
h
f 9(1) 5 lim }}
h→0
5 lim
h→0
5 lim
h→0
15. (a) The amount of daylight is increasing at the fastest rate
when the slope of the graph is largest. This occurs
about one-fourth of the way through the year, sometime
around April 1. The rate at this time is approximately
1
4 hours
}} or }} hour per day.
6
24 days
(b) Yes, the rate of change is zero when the tangent to the
graph is horizontal. This occurs near the beginning of
the year and halfway through the year, around
January 1 and July 1.
(c) Positive: January 1 through July 1
Negative: July 1 through December 31
16. The slope of the given graph is zero at x < 22 and at
x < 1, so the derivative graph includes (22, 0) and (1, 0).
The slopes at x 5 23 and at x 5 2 are about 5 and the
slope at x 5 20.5 is about 22.5, so the derivative graph
includes (23, 5), (2, 5), and (20.5, 22.5). Connecting the
points smoothly, we obtain the graph shown.
y
5
5 lim (3 1 3h 1 h2) 5 3
h→0
5
(a) The tangent line has slope 3 and passes through (1, 1).
Its equation is y 5 3(x 2 1) 1 1, or y 5 3x 2 2.
1
3
1
(1, 1). Its equation is y 5 2}}(x 2 1) 1 1, or
3
1
4
y 5 2}}x 1 }}.
3
3
71
x
(b) The normal line has slope 2}} and passes through
13. Since the graph of y 5 x ln x 2 x is decreasing for
0 , x , 1 and increasing for x . 1, its derivative is
negative for 0 , x , 1 and positive for x . 1. The only
one of the given functions with this property is y 5 ln x.
Note also that y 5 ln x is undefined for x , 0, which
further agrees with the given graph. (ii)
14. Each of the functions y 5 sin x, y 5 x, y 5 Ïxw has the
property that y(0) 5 0 but the graph has nonzero slope (or
undefined slope) at x 5 0, so none of these functions can be
its own derivative. The function y 5 x 2 is not its own
derivative because y(1) 5 1 but
(1 1 h)2 2 12
h
h→0
2h 1 h 2
h
h→0
y9(1) 5 lim }} 5 lim }}
5 lim (2 1 h) 5 2.
h→0
This leaves only e x, which can plausibly be its own
derivative because both the function value and the slope
increase from very small positive values to very large
values as we move from left to right along the graph. (iv)
17. (a) Using Figure 3.10a, the number of rabbits is largest
after 40 days and smallest from about 130 to 200 days.
Using Figure 3.10b, the derivative is 0 at these times.
(b) Using Figure 3.10b, the derivative is largest after
20 days and smallest after about 63 days. Using
Figure 3.10a, there were 1700 and about 1300 rabbits,
respectively, at these times.
1
220
2
0 2(24)
22 2 2
The slope from x 5 0 to x 5 1 is }} 5 24.
120
22 2(22)
The slope from x 5 1 to x 5 4 is }} 5 0.
421
22(22)
The slope from x 5 4 to x 5 6 is }} 5 2.
624
18. (a) The slope from x 5 24 to x 5 0 is }} 5 }}.
Note that the derivative is undefined at x 5 0, x 5 1,
and x 5 4. (The function is differentiable at x 5 24
and at x 5 6 because these are endpoints of the domain
and the one-sided derivatives exist.) The graph of the
derivative is shown.
y
5
4
3
2
–5–4–3–2 –1
–2
–3
–4
–5
1 2 3 4 5 6 7
x
72
Section 3.1
18. continued
(b)
(b) x 5 0, 1, 4
19.
Midpoint of
Interval (x)
0.5
1.5
2.5
3.5
4.5
5.5
6.5
7.5
8.5
9.5
Dy
1 Dx 2
Slope }}
3.3 2 0
}} 5 3.3
120
13.3 2 3.3
}} 5 10.0
221
29.9 2 13.3
}} 5 16.6
322
53.2 2 29.9
}} 5 23.3
423
83.2 2 53.2
}} 5 30.0
524
119.8 2 83.2
}} 5 36.6
625
163.0 2 119.8
}} 5 43.2
726
212.9 2 163.0
}} 5 49.9
827
269.5 2 212.9
}} 5 56.6
928
332.7 2 269.5
}} 5 63.2
10 2 9
A graph of the derivative data is shown.
Midpoint of
Interval (x)
Slope }}
0.00 1 0.56
}} 5 0.28
2
1512 2 1577
}} < 2116.07
0.56 2 0.00
0.56 1 0.92
}} 5 0.74
2
1448 2 1512
}} < 2177.78
0.92 2 0.56
0.92 1 1.19
}} 5 1.055
2
1384 2 1448
}} < 2237.04
1.19 2 0.92
1.19 1 1.30
}} 5 1.245
2
1319 2 1384
}} < 2590.91
1.30 2 1.19
1.30 1 1.39
}} 5 1.345
2
1255 2 1319
}} < 2711.11
1.39 2 1.30
1.39 1 1.57
}} 5 1.48
2
1191 2 1255
}} < 2355.56
1.57 2 1.39
1.57 1 1.74
}} 5 1.655
2
1126 2 1191
}} < 2382.35
1.74 2 1.57
1.74 1 1.98
}} 5 1.86
2
1062 2 1126
}} < 2266.67
1.98 2 1.74
1.98 1 2.18
}} 5 2.08
2
998 2 1062
}} 5 2320.00
2.18 2 1.98
2.18 1 2.41
}} 5 2.295
2
933 2 998
}} < 2282.61
2.41 2 2.18
2.41 1 2.64
}} 5 2.525
2
869 2 933
}} < 2278.26
2.64 2 2.41
2.64 1 3.24
}} 5 2.94
2
805 2 869
}} < 2106.67
3.24 2 2.64
Dy
1 Dx 2
A graph of the derivative data is shown.
[0, 10] by[210, 80]
(a) The derivative represents the speed of the skier.
(b) Since the distances are given in feet and the times are
given in seconds, the units are feet per second.
(c) The graph appears to be approximately linear and
[0, 3.24] by [2800, 100]
(c) Since the elevation y is given in feet and the distance x
down river is given in miles, the units of the gradiant
are feet per mile.
passes through (0, 0) and (9.5, 63.2), so the slope is
63.2 2 0
}} < 6.65. The equation of the derivative is
9.5 2 0
approximately D 5 6.65t.
(d) Since the elevation y is given in feet and the distance x
dy
dx
downriver is given in miles, the units of the distance }}
20. (a)
are feet per mile.
(e) Look for the steepest part of the curve. This is where
the elevation is dropping most rapidly, and therefore the
most likely location for significant “rapids.”
[20.5, 4] by [700, 1700]
(f) Look for the lowest point on the graph. This is where
the elevation is dropping most rapidly, and therefore the
most likely location for significant “rapids.”
21.
[2p, p] by [21.5, 1.5]
The cosine function could be the derivative of the sine
function. The values of the cosine are positive where the
sine is increasing, zero where the sine has horizontal
tangents, and negative where sine is decreasing.
Section 3.1
22. We show that the right-hand derivative at 1 does not exist.
f (1 1 h) 2 f (1)
3(1 1 h) 2 (1)3
h
h
h→0
2 1 3h
2
5 lim1 }} 5 lim1 }} 1 3 5 `
h
h
h→0
h→0
(e) Yes, the one-sided limits exist and are the same, so
lim f 9(x) 5 2.
lim }} 5 lim1 }}
h→01
1
x→1
2
f (1 1 h) 2 f (1)
(1 1 h)2 2 12
h
h
h→0
h→0
2h 1 h2
5 lim2 }} 5 lim2 (2 1 h) 5 2
h
h→0
h→0
(f) lim2 }} 5 lim2 }}
Ïwh 2 Ïw0
Ïwh
f (0 1 h) 2 f (0)
23. lim1 }} 5 lim1 }} 5 lim1 }}
h
1
5 lim1 }} 5 `
h→0 Ïw
h
h→0
h
h→0
h→0
73
h
f (1 1 h) 2 f (1)
2(1 1 h) 2 12
h
h
h→0
h→0
1 1 2h
1
5 lim2 }} 5 lim2 }} 1 2 5 2`
h
h
h→0
h→0
(g) lim1 }} 5 lim2 }}
1
Thus, the right-hand derivative at 0 does not exist.
24. Two parabolas are parallel if they have the same derivative
at every value of x. This means that their tangent lines are
parallel at each value of x.
Two such parabolas are given by y 5 x 2 and y 5 x 2 1 4.
They are graphed below.
2
The right-hand derivative does not exist.
(h) It does not exist because the right-hand derivative does
not exist.
27. The y-intercept of the derivative is b 2 a.
28. Since the function must be continuous at x 5 1, we have
lim1 (3x 1 k) 5 f (1) 5 1, so 3 1 k 5 1, or k 5 22.
x→1
This gives f (x) 5
f (1 1 h) 2 f (1)
h
h→0
slope 22 that passes through (0, 21): y 5 22x 2 1. Then
y(21) 5 22(21) 2 1 5 1, so for x , 21, the graph of
y 5 f (x) must lie on a line of slope 1 that passes through
(21, 1): y 5 1(x 1 1) 1 1 or y 5 x 1 2.
x , 21
x $ 21
(1 1 h)3 2 (1)3
h
h→0
3h 1 3h 2 1 h 3
5 lim }}
h
h→0
lim2 }} 5 lim2 }}
25. For x . 21, the graph of y 5 f (x) must lie on a line of
5
x#1
x . 1.
Now we confirm that f (x) is differentiable at x 5 1.
[24, 4] by [25, 20]
The parabolas are “everywhere equidistant,” as long as the
distance between them is always measured along a vertical
line.
x 1 2,
Thus f (x) 5
22x 2 1,
x 3,
53x 2 2,
5 lim (3 1 3h 1 h 2) 5 3
h→0
[3(1 1 h) 2 2] 2 (1)3]
f (1 1 h) 2 f (1)
h
h
h→0
h→0
(1 1 3h) 2 1
5 lim1 }} 5 lim1 3 5 3
h
h→0
h→0
lim1 }} 5 lim1 }}}
Since the right-hand derivative equals the left-hand
derivative at x 5 1, the derivative exists (and is equal to 3)
when k 5 22.
364
365
363
365
29. (a) 1 ? }} ? }} < 0.992
y
P
365 3
Alternate method: }
}
3 < 0.992
5
365
(b) Using the answer to part (a), the probability is about
1 2 0.992 5 0.008.
5
x
(c) Let P represent the answer to part (b), P < 0.008. Then
the probability that three people all have different
birthdays is 1 2 P. Adding a fourth person, the
f (x 1 h) 2 f (x)
h
(x 1 h)2 2 x 2
2xh 1 h 2
5 lim }} 5 lim }}
h
h
h→0
h→0
26. (a) f 9(x) 5 lim }}
h→0
5 lim (2x 1 h) 5 2x
h→0
f (x 1 h) 2 f (x)
h
2(x 1 h) 2 2x
5 lim }} 5 lim 2 5 2
h
h→0
h→0
(b) f 9(x) 5 lim }}
h→0
(c) lim2 f 9(x) 5 lim2 2x 5 2(1) 5 2
x→1
x→1
(d) lim1 f 9(x) 5 lim1 2 5 2
x→1
x→1
probability that all have different birthdays is
1 365 2
362
1 2(1 2 P)1}}2 < 0.016.
365
362
(1 2 P) }} , so the probability of a shared birthday is
(d) No. Clearly February 29 is a much less likely birth
date. Furthermore, census data do not support the
assumption that the other 365 birth dates are equally
likely. However, this simplifying assumption may still
give us some insight into this problem even if the
calculated probabilities aren’t completely accurate.
74
Section 3.2
■ Section 3.2 Differentiability (pp. 105–112)
Quick Review 3.2
1. Yes
Exploration 1 Zooming in to “See”
Differentiability
1. Zooming in on the graph of f at the point (0, 1) always
produces a graph exactly like the one shown below,
provided that a square window is used. The corner shows
no sign of straightening out.
2. No (The f (h) term in the numerator is incorrect.)
3. Yes
4. Yes
5. No (The denominator for this expression should be 2h).
6. All reals
7. [0, `)
8. [3, `)
9. The equation is equivalent to y 5 3.2x 1 (3.2p 1 5), so the
slope is 3.2.
f (3 1 0.001) 2 f (3 2 0.001)
0.002
5(3 1 0.001) 2 5(3 2 0.001)
0.002
5(0.002)
5 }} 5 5
0.002
10. }}} 5 }}}
[20.25, 0.25] by [0.836, 1.164]
2. Zooming in on the graph of g at the point (0, 1) begins to
reveal a smooth turning point. This graph shows the result
of three zooms, each by a factor of 4 horizontally and
vertically, starting with the window
[24, 4] by [21.624, 3.624].
Section 3.2 Exercises
1. Left-hand derivative:
f (0 1 h) 2 f (0)
h
h→0
h2 2 0
h
h→0
lim2 }} 5 lim2 }} 5 lim2 h 5 0
h→0
Right-hand derivative:
f (0 1 h) 2 f (0)
h
h20
h
lim }} 5 lim1 }} 5 lim1 1 5 1
h→01
[20.0625, 0.0625] by [0.959, 1.041]
3. On our grapher, the graph became horizontal after 8 zooms.
Results can vary on different machines.
4. As we zoom in on the graphs of f and g together, the
differentiable function gradually straightens out to resemble
its tangent line, while the nondifferentiable function
stubbornly retains its same shape.
h→0
h→0
Since 0 Þ 1, the function is not differentiable at the
point P.
2. Left-hand derivative:
f (1 1 h) 2 f (1)
h
222
h
lim }} 5 lim2 }} 5 lim2 0 5 0
h→02
h→0
h→0
Right-hand derivative:
f (1 1 h) 2 f (1)
h
2(1 1 h) 2 2
h
lim }} 5 lim1 }} 5 lim1 2 5 2
h→01
h→0
h→0
Since 0 Þ 2, the function is not differentiable at the
point P.
[20.03125, 0.03125] by [0.9795, 1.0205]
3. Left-hand derivative:
Exploration 2 Looking at the Symmetric
Difference Quotient Analytically
f (10 1 h) 2 f (10)
h
(10.01)2 2 102
0.01
Ïw1w
f (1 1 h) 2 f (1)
1w
h21
lim2 }} 5 lim2 }}
h
h→0
1. }} 5 }} 5 20.01
h→0
5 lim2
f 9(10) 5 2 ? 10 5 20
h→0
5 lim2
The difference quotient is 0.01 away from f 9(10).
h→0
1
The symmetric difference quotient exactly equals f 9(10).
Right-hand derivative:
f (10 1 h) 2 f (10)
h
h→01
(10.01)3 2 103
0.01
f (1 1 h) 2 f (1)
h
[2(1 1 h) 2 1] 2 1
h
lim }} 5 lim1 }}
f 9(10) 5 3 ? 102 5 300
h→0
2h
h
5 lim1 }}
h→0
The difference quotient is 0.3001 away from f 9(10).
f (10 1 h) 2 f (10 2 h)
(10.01)3 2 (9.99)3
}}} 5 }} 5 300.0001.
2h
0.02
1
5 lim2 }} 5 }}
2
h→0 Ï1
h11
ww
1w
f (10 1 h) 2 f (10 2 h)
(10.01)2 2 (9.99)2
2. }}} 5 }} 5 20
2h
0.02
3. }} 5 }} 5 300.3001.
h
ww
1wh 2 1)(Ï1
ww
1wh 1 1)
(Ï1
}}}
h(Ïw
1w
1wh 1 1)
(1 1 h) 2 1
}}
h(Ïw
1w
1wh 1 1)
5 lim1 2 5 2
h→0
1
2
The symmetric difference quotient is 0.0001 away from
Since }} Þ 2, the function is not differentiable at the
f 9(10).
point P.
Section 3.2
4. Left-hand derivative:
f (1 1 h) 2 f (1)
h
(1 1 h) 2 1
h
15. Note that y 5 3x 2 2)x) 2 1 5
lim }} 5 lim2 }} 5 lim2 1 5 1
h→02
h→0
1
}} 2 1
11h
lim }} 5 lim1 }}
h→01
3
1
17. Find the zeros of the denominator.
x2 2 4x 2 5 5 0
(x 1 1)(x 2 5) 5 0
x 5 21 or x 5 5
The function is a rational function, so it is differentiable for
all x in its domain: all reals except x 5 21, 5.
6. (a) All points in [22, 3]
(b) None
(c) None
7. (a) All points in [23, 3] except x 5 0
18. The function is differentiable except possibly where
3x 2 6 5 0, that is, at x 5 2. We check for differentiability
at x 5 2, using k instead of the usual h, in order to avoid
confusion with the function h(x).
(b) None
(c) x 5 0
8. (a) All points in [22, 3] except x 5 21, 0, 2
(b) x 5 21
3
[Ï3
w(2
ww
1wk)w2
ww6 1 5] 2 5
h(2 1 k) 2 h(2)
lim }} 5 lim }}}
(c) x 5 0, x 5 2
The function has a vertical tangent at x 5 2. It is
differentiable for all reals except x 5 2.
10. (a) All points in [23, 3] except x 5 22, 2
(b) x 5 22, x 5 2
11. Since lim tan21 x 5 tan21 0 5 0 Þ y(0), the problem is a
x→0
discontinuity.
4/5
h
h
h→0
h4/5
}} 5 lim
h
h→01
1
h
1
}1/5
}5`
h
12. lim2 }} 5 lim2 }} 5 lim2 }1/5
} 5 2`
g(0 1 h) 2 g(0)
h
h→0
5
h→0
222
}} 5 lim 0 5 0
h
h→02
(2h 1 2) 2 2
}} 5 lim 2 5 2
h
h→01
3
Ïwh
y(0 1 h) 2 y(0)
(32Ïwh) 2 3
14. lim }} 5 lim }} 5 lim 2}}
h
2
The problem is a vertical tangent.
h→0
h 2 1 2h
h
h→0
5 lim2 (h 1 2) 5 2
The problem is a corner.
h
h→0
1
5 lim 2}2/3
} 5 2`
h
h→0
(h 1 1)2 2 1
h
h→0
lim2 }} 5 lim2 }} 5 lim2 }}
13. Note that y 5 x 1 Ïw
x 2 1 2 5 x 1 )x) 1 2
2,
x#0
5
2x 1 2,
x . 0.
3
20. Since the cosine function is even,
so Q(x) 5 3 cos ()x)) 5 3 cos x. The function is
differentiable for all reals.
21. The function is piecewise-defined in terms of polynomials,
so it is differentiable everywhere except possibly at x 5 0
and at x 5 3. Check x 5 0:
The problem is a cusp.
h→0
19. Note that the sine function is odd, so
2sin x 2 1, x , 0
P(x) 5 sin ()x)) 2 1 5
sin x 2 1,
x $ 0.
The graph of P(x) has a corner at x 5 0. The function is
differentiable for all reals except x 5 0.
5
(c) None
y(0 1 h) 2 y(0)
}} 5 lim
h
h→02
y(0 1 h) 2 y(0)
}} 5 lim
h
h→01
k
k→0
3
1
5 lim }} 5 Ï3w lim }2}
/3 5 `
k→0 k
k→0 k
(c) None
y(0 1 h) 2 y(0)
h
h→0
y(0 1 h) 2 y(0)
lim }} 5 lim1
h
h→01
h→0
3
Ïw3kw
(b) x 5 0
h→0
k
k→0
9. (a) All points in [21, 2] except x 5 0
1
2
The problem is a cusp.
(c) None
lim
h
h
h
h→0
h→0
1
5 lim2 2}2/3
} 5 2`
h
h→0
3
3
Ï)h
w)w 2 0
Ïhw
y(0 1 h) 2 y(0)
lim1 }} 5 lim1 }} 5 lim1 }}
h
h
h
h→0
h→0
h→0
1
5 lim1 }2/3
}5`
h→0 h
h→0
(b) None
h→01
3
Ï)h
ww) 2 0
y(0 1 h) 2y(0)
2Ïhw
16. lim2 }} 5 lim2 }} 5 lim2 }}
5. (a) All points in [23, 2]
lim
y(0 1 h) 2y(0)
(5h 2 1) 2 (21)
h
h
h→0
h→0
y(0 1 h) 2 y(0)
(h 2 1) 2 (21)
lim1 }} 5 lim1 }} 5 lim1 1 5 1
h
h
h→0
h→0
h→0
lim }} 5 lim2 }} 5 lim2 5 5 5
The problem is a corner.
h
1 2 (1 1 h)
5 lim1 }}
h(1 1 h)
h→0
2h
5 lim1 }}
h→0 h(1 1 h)
1
5 lim1 2}} 5 21
11h
h→0
h→0
Since 1 Þ 21, the function is not differentiable at the
point P.
h→02
x#0
x.0
h→02
Right-hand derivative:
f (1 1 h) 2 f (1)
h
h→0
5x5x221,1,
75
h
g(0 1 h) 2 g(0)
h
(2h 1 1) 21
h
lim }} 5 lim1 }} 5 lim1 2 5 2
h→01
h→0
The function is differentiable at x 5 0.
h→0
76
Section 3.2
21. continued
27.
Check x 5 3:
Since g(3) 5 (4 2 3)2 5 1 and
lim g(x) 5 lim2 (2x 1 1) 5 2(3) 1 1 5 7, the function is
x→32
[22p, 2p] by [24, 4]
x→3
dy
}} 5 tan x
dx
not continuous (and hence not differentiable) at x 5 3.
The function is differentiable for all reals except x 5 3.
22. Note that C(x) 5 x)x) 5
2x ,
5x 2 ,
2
Note: Due to the way NDER is defined, the graph of
x,0
, so it is
x$0
y 5 NDER (x) actually has two asymptotes for each
asymptote of y 5 tan x. The asymptotes of y 5 NDER (x)
differentiable for all x except possibly at x 5 0.
p
2
occur at x 5 }} 1 kp 6 0.001, where k is an integer. A
Check x 5 0:
C(0 1 h) 2 C(0)
h
h→0
h)h) 2 0
h
h→0
good window for viewing this behavior is [1.566, 1.576] by
lim }} 5 lim }} 5 lim )h) 5 0
[21000, 1000].
h→0
The function is differentiable for all reals.
28.
23. (a) x 5 0 is not in their domains, or, they are both
discontinuous at x 5 0.
1 2
1 2
1
1
x
x
1
1
For }}2 : NDER }}2 , 0 5 0
x
x
(b) For }}: NDER }}, 0 5 1,000,000
(c) It returns an incorrect response because even though
these functions are not defined at x 5 0, they are
defined at x 5 60.001. The responses differ from each
1
x
other because }}2 is even (which automatically makes
1
2
1
1
NDER }}2 , 0 5 0) and }} is odd.
x
x
24.
[22p, 2p] by [220, 20]
The graph of NDER (x) does not look like the graph of any
basic function.
29. (a)
lim f (x) 5 f (1)
x→12
lim (3 2 x) 5 a(1)2 1 b(1)
x→12
2 5a1b
The relationship is a 1 b 5 2.
(b) Since the function needs to be continuous, we may
assume that a 1 b 5 2 and f (1) 5 2.
f (1 1 h) 2 f (1)
h
3 2 (1 1 h) 2 2
h
lim }} 5 lim2 }}
h→02
[25, 5] by [210, 10]
dy
}} 5 x 3
dx
25.
h→0
5 lim2 (21) 5 21
h→0
f (1 1 h) 2 f (1)
h
h→0
h→0
5 lim2
h→0
5 lim2
h→0
[22p, 2p] by [21.5, 1.5]
dy
}} 5 sin x
dx
26.
a(1 1 h)2 1 b(1 1 h) 2 2
h
a 1 2ah 1 ah 2 1 b 1 bh 2 2
}}}}
h
2ah 1 ah 2 1 bh 1 (a 1 b 2 2)
}}}}
h
lim1 }} 5 lim2 }}}
5 lim2 (2a 1 ah 1 b)
h→0
5 2a 1 b
Therefore, 2a 1 b 5 21. Substituting 2 2 a for b gives
2a 1 (2 2 a) 5 21, so a 5 23.
Then b 5 2 2 a 5 2 2 (23) 5 5. The values are
a 5 23 and b 5 5.
[26, 6] by [24, 4]
dy
}} 5 abs (x) or )x)
dx
30. The function f (x) does not have the intermediate value
property. Choose some a in (21, 0) and b in (0, 1). Then
f (a) 5 0 and f (b) 5 1, but f does not take on any value
between 0 and 1. Therefore, by the Intermediate Value
Theorem for Derivatives, f cannot be the derivative of any
function on [21, 1].
Section 3.3
1
x
31. (a) Note that 2x # sin }} # x, for all x,
1
1
x
2
so lim x sin }} 5 0 by the Sandwich Theorem.
x→0
Therefore, f is continuous at x 5 0.
1
h sin }} 2 0
h
f (0 1 h) 2 f (0)
1
(b) }} 5 }} 5 sin }}
h
h
h
1
h
(c) The limit does not exist because sin }} oscillates
between 21 and 1 an infinite number of times
arbitrarily close to h 5 0 (that is, for h in any open
interval containing 0).
9. These are all constant functions, so the graph of each
function is a horizontal line and the derivative of each
function is 0.
x1h
x
p
p
}} 2 }}
p
p
f (x 1 h) 2 f (x)
10. (a) f 9(x) 5 lim }} 5 lim }}
h
h
h→0
h→0
x1h2x
1
1
5 lim }} 5 lim }} 5 }}
ph
p
h→0
h→0 p
}} 2 }}
f (x 1 h) 2 f (x)
x
x1h
(b) f 9(x) 5 lim }} 5 lim }}
h
h
h→0
h→0
px 2 p(x 1 h)
2ph
5 lim }} 5 lim }}
hx(x 1 h)
h→0
h→0 hx(x 1 h)
p
p
5 lim 2}} 5 2}}2 5 2px 22
x(x 1 h)
x
h→0
Section 3.3 Exercises
(d) No, because the limit in part (c) does not exist.
12
1
h 2 sin }} 2 0
h
g(0 1 h) 2 g(0)
1
(e) }} 5 }} 5 h sin }}
h
h
h
As noted in part (a), the limit of this as x approaches
zero is 0, so g9(0) 5 0.
■ Section 3.3 Rules for Differentiation
(pp. 112–121)
dy
d
d
dx
dx
dx
d 2y
d
}}2 5 }}(22x) 5 22
dx
dx
1. }} 5 }}(2x 2) 1 }}(3) 5 22x 1 0 5 22x
1 2
dy
d 1
d
dx
dx 3
dx
d 2y
d
d
}}2 5 }}(x 2) 2 }}(1) 5 2x 2 0 5 2x
dx
dx
dx
2. }} 5 }} }}x 3 2 }}(x) 5 x 2 2 1
dy
d
d
dx
dx
dx
d 2y
d
}}2 5 }}(2) 5 0
dx
dx
3. }} 5 }}(2x) 1 }}(1) 5 2 1 0 5 2
Quick Review 3.3
1. (x 2 2 2)(x 21 1 1) 5 x 2x 21 1 x 2 ? 1 2 2x 21 2 2 ? 1
5 x 1 x 2 2 2x 21 2 2
1x
21
x2 1 1
x2
1
x
5 }} 5 }} 1 }} 5 x 1 x 21
x
x
x
11
2
2. }
2 }
2
x
5
x
3. 3x 2 2 }} 1 }}2 5 3x 2 2 2x 21 1 5x 22
3x 4 2 2x 3 1 4
2x
3x 4
2x
2x 3
2x
4
2x
3
2
4. }}
5 }}2 2 }}2 1 }}2 5 }}x 2 2 x 1 2x 22
2
5. (x 21 1 2)(x 22 1 1) 5 x 21x 22 1 x 21 ? 1 1 2x 22 1 2 ? 1
5 x 23 1 x 21 1 2x 22 1 2
x 21 1 x 22
6. }23
} 5 x 3(x 21 1 x 22) 5 x 2 1 x
x
7.
dy
d
d
d
dx
dx
dx
dx
d 2y
d
d
}}2 5 }}(2x) 1 }}(1) 5 2 1 0 5 2
dx
dx
dx
4. }} 5 }}(x 2) 1 }}(x) 1 }}(1) 5 2x 1 1 1 0 5 2x 1 1
dy
dx
1 2
1 2
d 1
dx 3
d 1
dx 2
d
dx
5. }} 5 }} }}x 3 1 }} }}x 2 1 }}(x)
5 x2 1 x 1 1
d 2y
d
d
d
}}2 5 }}(x 2) 1 }}(x) 1 }}(1) 5 2x 1 1 1 0 5 2x 1 1
dx
dx
dx
dx
dy
dx
d
dx
d
dx
d
dx
d
dx
6. }} 5 }}(1) 2 }}(x) 1 }}(x 2) 2 }}(x 3)
5 0 2 1 1 2x 2 3x 2 5 21 1 2x 2 3x 2
d 2y
d
d
d
}}2 5 }}(21) 1 }}(2x) 2 }}(3x 2)
dx
dx
dx
dx
5 0 1 2 2 6x 5 2 2 6x
dy
dx
d
dx
d
dx
d
dx
d
dx
7. }} 5 }}(x 4) 2 }}(7x 3) 1 }}(2x 2) 1 }}(15)
5 4x 3 2 21x 2 1 4x 1 0 5 4x 3 2 21x 2 1 4x
[0, 5] by [26, 6]
d 2y
d
d
d
}}2 5 }}(4x 3) 2 }}(21x 2) 1 }}(4x) 5 12x 2 2 42x 1 4
dx
dx
dx
dx
At x < 1.173, 500x 6 < 1305.
At x < 2.394, 500x 6 < 94,212
After rounding, we have:
At x < 1, 500x 6 < 1305.
At x < 2, 500x 6 < 94,212.
dy
d
d
dx
dx
dx
d 2y
d
d
}}2 5 }}(15x 2) 2 }}(15x 4) 5 30x 2 60x 3
dx
dx
dx
8. }} 5 }}(5x 3) 2 }}(3x 5) 5 15x 2 2 15x 4
8. (a) f (10) 5 7
dy
dx
(c) f (x 1 h) 5 7
f (x) 2 f (a)
x2a
d
dx
d
dx
5 28x23 2 8 1 0 5 28x 23 2 8
727
(d) lim }} 5 lim }} 5 lim 0 5 0
x→a
d
dx
9. }} 5 }}(4x 22) 2 }}(8x) 1 }}(1)
(b) f (0) 5 7
x→a x 2 a
x→a
d 2y
d
d
}}2 5 }}(28x 23) 2 }}(8) 5 24x 24 2 0 5 24x 24
dx
dx
dx
77
78
Section 3.3
dy
dx
1
d 1
dx 4
d
1 }}(3)
dx
2
1
2
d 1
dx 3
1
2
d 1
dx 2
d
dx
10. }} 5 }} }}x 24 2 }} }}x 23 1 }} }}x 22 2 }}(x 21)
5 2x 25 1 x 24 2 x 23 1 x 22 1 0
1
1
(Ïxw 1 1)}} 2 (Ïxw 2 1)}}
2Ïwx
2Ïxw
}}}}
dy
d Ïxw 2 1
18. }} 5 }} } 5
(Ïxw 1 1)2
dx
dx Ïxw 1 1
1
2
2
1
(Ïxw 1 1) 2 (Ïxw 2 1)
5 }}}
5 }}2 5 }}2
2Ïxw(Ïxw 1 1)
Ïxw(Ïxw 1 1)
2Ïxw(Ïxw 1 1)2
5 2x 25 1 x 24 2 x 23 1 x 22
d 2y
d
d
d
d
}}2 5 }}(2x 25) 1 }}(x 24) 2 }}(x 23) 1 }}(x 22)
dx
dx
dx
dx
dx
5 5x 26 2 4x 25 1 3x 24 2 2x 23
dy
dx
dy
dx
d (x 1 1)(x 1 2)
dx (x 2 1)(x 2 2)
1
d x 2 1 3x 1 2
dx x 2 3x 1 2
2
1
19. }} 5 }} }} 5 }} }}
2
d
dx
11. (a) }} 5 }}[(x 1 1)(x 2 1 1)]
d
dx
2
(x 2 2 3x 1 2)(2x 1 3) 2 (x 2 1 3x 1 2)(2x 2 3)
(x 2 3x 1 2)
5 }}}}}
2
2
d
dx
5 (x 1 1)}}(x 2 1 1) 1 (x 2 1 1) }}(x 1 1)
(2x 3 2 3x 2 2 5x 1 6) 2 (2x 3 1 3x 2 2 5x 2 6)
(x 2 3x 1 2)
5 (x 1 1)(2x) 1 (x 2 1 1)(1)
5 }}}}}
2
2
5 2x 2 1 2x 1 x 2 1 1
5 }}
2
2
12 2 6x 2
(x 2 3x 1 2)
5 3x 2 1 2x 1 1
20. (a) Let f (x) 5 x.
dy
d
(b) }} 5 }}[(x 1 1)(x 2 1 1)]
dx
dx
d
5 }}(x 3 1 x 2 1 x 1 1)
dx
f (x 1 h) 2 f (x)
(x 1 h) 2 x
d
}} (x) 5 f 9(x) 5 lim }} 5 lim }}
h
h
dx
h→0
h→0
h
5 lim }} 5 lim (1) 5 1
h→0 h
h→0
5 3x 2 1 2x 1 1
(b) Note that u 5 u(x) is a function of x.
d x 13
x
dx
1
dy
dx
2
2
12. (a) }} 5 }} }}
d
dx
2u(x 1 h) 2 [2u(x)]
d
}} (2u) 5 lim }}}
h
dx
h→0
d
dx
x}}(x 2 1 3) 2 (x 2 1 3)}}(x)
h→0
x
h→0
x 23
x
1
2
d
dx
d
dx
d
d
dx
This is equivalent to the answer in part (a).
(3x 2 2)(2) 2 (2x 1 5)(3)
dy
d 2x 1 5
13. }} 5 }} }} 5 }}}
5 2}19}2
(3x 2 2)2
dx
dx 3x 2 2
(3x 2 2)
dy
d x 2 1 5x 2 1
d
14. }} 5 }} }}
5 }} (1 1 5x 21 2 x 22)
x2
dx
dx
dx
5
2
5 0 2 5x 22 1 2x 23 5 2}}2 1 }}3
x
x
1
2
d x3 2 1
dx
x
d
3
23
24
5 }}(1 2 x ) 5 0 1 3x 5 }}4
dx
x
1
d (x 2 1)(x 2 1 x 1 1)
x
dx
2
1
d 12x
dx 1 1 x
x 2 2 2x 2 1
5 }}
(1 1 x 2)2
2
d
x2
dx 1 2 x
2
f (x) ? 0 2 1 ? }} f (x)
dx
d
1
f 9(x)
22. }} }} 5 }}}
5 2}}2
[ f (x)]2
dx f (x)
[ f (x)]
1 2
d
dx
23. (a) At x 5 0, }} (uv) 5 u(0)v9(0) 1 v(0)u9(0)
5 (5)(2) 1 (21)(23) 5 13
v(0)u9(0) 2 u(0)v9(0)
d u
[v(0)]
dx v
(21)(23) 2 (5)(2)
5 }}
5 27
(21)2
12
(b) At x 5 0, }} }} 5 }}}
2
12
d v
dx u
u(0)v9(0) 2 v(0)u9(0)
[u(0)]
(c) At x 5 0, }} }} 5 }}}
2
2
15. }} 5 }} }}}
5 }} }}
3
3
(5)(2) 2 (21)(23)
(5)
(1 1 x 2)(21) 2 (1 2 x)(2x)
(1 1 x )
d
dx
(d) At x 5 0, }}(7v 2 2u) 5 7v9(0) 2 2u9(0)
5 7(2) 2 2(23) 5 20
(1 2 x 3)(2x) 2 x 2(23x 2)
(1 2 x )
7
25
5 }}
5 }}
2
16. }} 5 }} }}2 5 }}}
2 2
1
d
dx
d
dx
d x2 1 3
x
dx
3
5 1 2 }}2
x
dy
dx
du
dx
5 c ? }} f (x) 1 0 5 c ? }} f (x)
(b) }} 5 }} }} 5 }}(x 1 3x 21) 5 1 2 3x 22
1
u(x 1 h) 2 u(x)
h
d
dx
5 }}
2
dy
dx
2
21. }}(c ? f (x)) 5 c ? }} f (x) 1 f (x) ? }} (c)
2
dy
dx
u(x 1 h) 2 u(x)
h
5 2lim }} 5 2}}
x(2x) 2 (x 2 1 3)
5 }}
x2
dy
dx
1
5 lim 2}}
5 }}}
2
x 4 1 2x
(1 2 x )
17. }} 5 }} }}3 5 }}}
5}
3 2
3 2
Section 3.3
d
dx
24. (a) At x 5 2, }} (uv) 5 u(2)v9(2) 1 v(2)u9(2)
5 (3)(2) 1 (1)(24) 5 2
v(2)u9(2) 2 u(2)v9(2)
d u
[v(2)]
dx v
(1)(24) 2 (3)(2)
5 }}
5 210
(1)2
12
(b) At x 5 2, }} }} 5 }}}
2
u(2)v9(2) 2 v(2)u9(2)
d v
[u(2)]
dx u
(3)(2) 2 (1)(24)
10
5 }}
5 }}
(3)2
9
79
29. y9(x) 5 6x 2 2 6x 2 12
5 6(x 2 2 x 2 2)
5 6(x 1 1)(x 2 2)
The tangent is parallel to the x-axis when y9 5 0, at x 5 21
and at x 5 2. Since y(21) 5 27 and y(2) 5 0, the two
points where this occurs are (21, 27) and (2, 0).
Graphical support:
12
(c) At x 5 2, }} }} 5 }}}
2
d
(d) Use the result from part (a) for }} (uv).
dx
d
At x 5 2, }} (3u 2 2v 1 2uv)
dx
d
5 3u9(2) 2 2v9(2) 1 2}} (uv)
dx
5 3(24) 2 2(2) 1 2(2)
[23, 3] by [210, 30]
30. y9(x) 5 3x 2
y9(22) 5 12
The tangent line has slope 12 and passes through (22, 28),
so its equation is y 5 12(x 1 2) 2 8, or y 5 12x 1 16. The
4
3
x-intercept is 2}} and the y-intercept is 16.
5 212
Graphical support:
25. y9(x) 5 2x 1 5
y9(3) 5 2(3) 1 5 5 11
The slope is 11. (iii)
3
2
26. The given equation is equivalent to y 5 }}x 1 6, so the
3
2
slope is }}. (iii)
27. y9(x) 5 3x 2 3
y9(2) 5 3(2)2 2 3 5 9
2
The tangent line has slope 9, so the perpendicular line has
1
9
slope 2}} and passes through (2, 3).
1
9
1
29
y 5 2}}x 1 }}
9
9
y 5 2}}(x 2 2) 1 3
[23, 3] by [220, 20]
(x 2 1 1)(4) 2 4x(2x)
(x 1 1)
24x 2 1 4
(x 1 1)
31. y9(x) 5 }}}
5}
2
2
2 }
2
At the origin: y9(0) 5 4
The tangent is y 5 4x.
At (1, 2): y9(1) 5 0
The tangent is y 5 2.
Graphical support:
Graphical support:
[24.7, 4.7] by [23.1, 3.1]
[24.7, 4.7] by [22.1, 4.1]
28. y9(x) 5 3x 2 1 1
The slope is 4 when 3x 2 1 1 5 4, at x 5 61. The tangent
at x 5 21 has slope 4 and passes through (21, 22), so its
equation is y 5 4(x 1 1) 2 2, or y 5 4x 1 2. The tangent at
x 5 1 has slope 4 and passes through (1, 2), so its equation
is y 5 4(x 2 1) 1 2, or y 5 4x 2 2. The smallest slope
occurs when 3x 2 1 1 is minimized, so the smallest slope is
1 and occurs at x 5 0.
(4 1 x 2)(0) 2 8(2x)
16x
(4 1 x )
(4 1 x )
1
y9(2) 5 2}}
2
1
The tangent has slope 2}} and passes through (2, 1). Its
2
1
1
equation is y 5 2}}(x 2 2) 1 1, or y 5 2}}x 1 2.
2
2
32. y9(x) 5 }}}
5 2}}
2 2
2 2
Graphical support:
Graphical support:
[23, 5] by [22, 4]
[24.7, 4.7] by [23.1, 3.1]
80
Section 3.4
dP
dV
an 2
d nRT
V
dV V2nb
d
d
(V 2 nb)}}(nRT) 2 (nRT)}}(V 2 nb)
dV
dV
d
5 }}}}
2 }} (an 2V 22)
(V 2 nb)2
dV
1
33. }} 5 }} }} 2 }}
2
2
0 2 nR T
(V 2 nb)
5 }}2 1 2an 2V 23
nRT
(V 2 nb)
2an
V
rule given in the text.
(d) Because dx is ‘infinitely small,” and this could be
thought of as dividing by zero.
1v2
u
ds
d
dt
dt
d 2s
d
5 }}(9.8t) 5 9.8
}}
dt 2
dt
34. }} 5 }}(4.9t 2) 5 9.8t
3 1
1
dv
dx
u 1 du
u
v 1 dv
v
(u 1 du)(v) 2 (u)(v 1 dv)
5 }}}
(v 1 dv)(v)
uv 1 vdu 2 uv 2 udv
5 }}}
v 2 1 vdv
vdu 2 udv
5 }}
v2
(e) d }} 5 }} 2 }}
2
5 2}}2 1 }}
3
dR
dM
du
dx
d
dx
(c) }}(uv) 5 v}} 1 u}}. This is equivalent to the product
24
2
C
M
d
2
3
dM
1 3
d C 2
5 }} }}M 2 }}M
3
dM 2
35. }} 5 }} M 2 }} 2 }}
■ Section 3.4 Velocity and Other Rates
of Change (pp. 122–133)
Exploration 1
5 CM 2 M 2
36. If the radius of a circle is changed by a very small amount
Dr, the change in the area can be thought of as a very thin
strip with length given by the circumference, 2pr, and
width Dr. Therefore, the change in the area can be thought
of as (2pr)(Dr), which means that the change in the area
divided by the change in the radius is just 2pr.
37. If the radius of a sphere is changed by a very small amount
Dr, the change in the volume can be thought of as a very
thin layer with an area given by the surface area, 4pr 2, and
a thickness given by Dr. Therefore, the change in the
volume can be thought of as (4pr 2)(Dr), which means that
the change in the volume divided by the change in the
radius is just 4pr 2.
38. Let t(x) be the number of trees and y(x) be the yield per tree
x years from now. Then t(0) 5 156, y(0) 5 12, t9(0) 5 13,
and y9(0) 5 1.5. The rate of increase of production is
d
}}(ty) 5 t(0)y9(0) 1 y(0)t9(0) 5 (156)(1.5) 1 (12)(13)
dx
5 390 bushels of annual production per year.
39. Let m(x) be the number of members and c(x) be the
Growth Rings on a Tree
1. Figure 3.22 is a better model, as it shows rings of equal
area as opposed to rings of equal width. It is not likely that
a tree could sustain increased growth year after year,
although climate conditions do produce some years of
greater growth than others.
2. Rings of equal area suggest that the tree adds
approximately the same amount of wood to its girth each
year. With access to approximately the same raw materials
from which to make the wood each year, this is how most
trees actually grow.
3. Since change in area is constant, so also is
change in area
}}. If we denote this latter constant by k, we
2p
k
have }} 5 r, which means that r varies
change in radius
inversely as the change in the radius. In other words, the
change in radius must get smaller when r gets bigger, and
vice-versa.
Exploration 2
Modeling Horizontal Motion
1. The particle reverses direction at about t 5 0.61 and
t 5 2.06.
pavillion cost x years from now. Then m(0) 5 65,
c(0) 5 250, m9(0) 5 6, and c9(0) 5 10. The rate of change
1 2
d c
dx m
m(0)c9(0) 2 c(0)m9(0)
of each member’s share is }} }} 5 }}}
[m(0)]2
(65)(10) 2 (250)(6)
5 }}}
< 20.201 dollars per year. Each
(65)2
member’s share of the cost is decreasing by approximately
20 cents per year.
40. (a) It is insignificant in the limiting case and can be treated
as zero (and removed from the expression).
(b) It was “rejected” because it is incomparably smaller
than the other terms: v du and u dv.
2. When the trace cursor is moving to the right the particle is
moving to the right, and when the cursor is moving to the
left the particle is moving to the left. Again we find the
particle reverses direction at about t 5 0.61 and t 5 2.06.
Section 3.4
3. When the trace cursor is moving upward the particle is
moving to the right, and when the cursor is moving
downward the particle is moving to the left. Again we find
the same values of t for when the particle reverses
direction.
81
Quick Review 3.4
1. The coefficient of x 2 is negative, so the parabola opens
downward.
Graphical support:
[21, 9] by [2300, 200]
4. We can represent the velocity by graphing the parametric
equations
x4(t) 5 x19(t) 5 12t 2 2 32t 1 15, y4(t) 5 2 (part 1),
x5(t) 5 x19(t) 5 12t 2 2 32t 1 15, y5(t) 5 t (part 2),
x6 (t) 5 t, y6(t) 5 x19(t) 5 12t 2 2 32t 1 15 (part 3)
[28, 20] by [23, 5]
(x4, y4)
2. The y-intercept is f (0) 5 2256.
See the solution to Exercise 1 for graphical support.
3. The x-intercepts occur when f(x) 5 0.
216x 2 1 160x 2 256 5 0
216(x 2 2 10x 1 16) 5 0
216(x 2 2)(x 2 8) 5 0
x 5 2 or x 5 8
The x-intercepts are 2 and 8. See the solution to Exercise 1
for graphical support.
4. Since f (x) 5 216(x 2 2 10x 1 16)
5 216(x 2 2 10x 1 25 2 9) 5 216(x 2 5)2 1 144,
the range is (2`, 144].
See the solution to Exercise 1 for graphical support.
5. Since f(x) 5 216(x 2 2 10x 1 16)
5 216(x 2 2 10x 1 25 2 9)5 216(x 2 5)2 1 144,
the vertex is at (5, 144). See the solution to Exercise 1 for
graphical support.
[28, 20] by [23, 5]
6.
(x5, y5)
f (x) 5 80
216x 2 1 160x 2 256 5 80
216x 2 1 160x 2 336 5 0
216(x 2 2 10x 1 21) 5 0
216(x 2 3)(x 2 7) 5 0
x 5 3 or x 5 7
f (x) 5 80 at x 5 3 and at x 5 7.
See the solution to Exercise 1 for graphical support.
[22, 5] by [210, 20]
(x6, y6)
7.
For (x4, y4) and (x5, y5), the particle is moving to the right
when the x-coordinate of the graph (velocity) is positive,
moving to the left when the x-coordinate of the graph
(velocity) is negative, and is stopped when the x-coordinate
of the graph (velocity) is 0. For (x6, y6), the particle is
moving to the right when the y-coordinate of the graph
(velocity) is positive, moving to the left when the
y-coordinate of the graph (velocity) is negative, and is
stopped when the y-coordinate of the graph (velocity) is 0.
dy
}} 5 100
dx
232x 1 160 5 100
60 5 32x
15
8
dy
15
}} 5 100 at x 5 }}
8
dx
x 5 }}
Graphical support: the graph of NDER f (x) is shown.
Exploration 3 Seeing Motion on a Graphing
Calculator
1. Let tMin 5 0 and tMax 5 10.
2. Since the rock achieves a maximum height of 400 feet, set
yMax to be slightly greater than 400, for example
yMax 5 420.
4. The grapher proceeds with constant increments of t (time),
so pixels appear on the screen at regular time intervals.
When the rock is moving more slowly, the pixels appear
closer together. When the rock is moving faster, the pixels
appear farther apart. We observe faster motion when the
pixels are farther apart.
[21, 9] by [2200, 200]
8.
dy
}} . 0
dx
232x 1 160 . 0
232x . 2160
x ,5
dy
}} . 0 when x , 5.
dx
See the solution to Exercise 7 for graphical support.
82
Section 3.4
9. Note that f 9(x) 5 232x 1 160.
(e)
f (3 1 h) 2 f (3)
h
lim }} 5 f 9(3) 5 232(3) 1 160 5 64
h→0
For graphical support, use the graph shown in the solution
to Exercise 7 and observe that NDER (f (x), 3) < 64.
10. f 9(x) 5 232x 1 160
f 0(x) 5 232
At x 5 7 (and, in fact, at any other of x),
s(t) 5 0
24t 2 0.8t 2 5 0
0.8t(30 2 t) 5 0
t 5 0 or t 5 30
The rock was aloft from t 5 0 to t 5 30, so it was aloft
for 30 seconds.
4. On Mars:
ds
dt
d
dt
Velocity 5 }} 5 }}(1.86t 2) 5 3.72t
d 2y
}}2 5 232.
dx
Solving 3.72t 5 16.6, the downward velocity reaches
Graphical support: the graph of NDER(NDER f (x)) is
shown.
16.6 m/sec after about 4.462 sec.
On Jupiter:
ds
dt
d
dt
Velocity 5 }} 5 }}(11.44t 2) 5 22.88t
Solving 22.88t 5 16.6, the downward velocity reaches
16.6 m/sec after about 0.726 sec.
[21, 9] by [240, 10]
Section 3.4 Exercises
dV
ds
1. Since V 5 s 3, the instantaneous rate of change is }} 5 3s 2.
2. (a) Displacement = s(5) 2 s(0) 5 12 2 2 5 10 m
10 m
5 sec
(b) Average velocity 5 }} 5 2 m/sec
(c) Velocity 5 s9(t) 5 2t 2 3
At t 5 4, velocity 5 s9(4) 5 2(4) 2 3 5 5 m/sec
(d) Acceleration 5 s0(t) 5 2 m/sec 2
(e) The particle changes direction when
3
2
s9(t) 5 2t 2 3 5 0, so t 5 }} sec.
(f) Since the acceleration is always positive, the position s
is at a minimum when the particle changes direction, at
122
3
2
3
1
4
t 5 }} sec. Its position at this time is s }} 5 2}} m.
ds
dt
d
dt
dv
d
Acceleration: a(t) 5 }} 5 }}(24 2 1.6t) 5 21.6 m/sec2
dt
dt
3. (a) Velocity: v(t) 5 }} 5 }}(24t 2 0.8t 2) 5 24 2 1.6t m/sec
(b) The rock reaches its highest point when
v(t) 5 24 2 1.6t 5 0, at t 5 15. It took 15 seconds.
(c) The maximum height was s(15) 5 180 meters.
1
2
s(t) 5 }}(180)
(d)
24t 2 0.8t 2 5 90
0 5 0.8t 2 2 24t 1 90
24 6Ï(2
w2w4w)w2w
2w
4(0
w.8
w)(
w9w0w)w
t 5 }}}
2(0.8)
< 4.393, 25.607
It took about 4.393 seconds to reach half its maximum
height.
5. The rock reaches its maximum height when the velocity
s9(t) 5 24 2 9.8t 5 0, at t < 2.449. Its maximum height is
about s(2.449) < 29.388 meters.
6. Moon:
s(t) 5 0
832t 2 2.6t 2 5 0
2.6t(320 2 t) 5 0
t 5 0 or t 5 320
It takes 320 seconds to return.
Earth:
s(t) 5 0
832t 2 16t 2 5 0
16t(52 2 t) 5 0
t 5 0 or t 5 52
It takes 52 seconds to return.
7. The following is one way to simulate the problem situation.
For the moon:
x1(t) 5 3(t , 160) 1 3.1(t $ 160)
y1(t) 5 832t 2 2.6t 2
t-values: 0 to 320
window: [0, 6] by [210,000, 70,000]
For the earth:
x1(t) 5 3(t , 26) 1 3.1(t $ 26)
y1(t) 5 832t 2 16t 2
t-values: 0 to 52
window: [0, 6] by [21000, 11,000]
8. The growth rate is given by
b9(t) 5 104 2 2 ? 103t 5 10,000 2 2000t.
At t 5 0: b9(0) 5 10,000 bacteria/hour
At t 5 5: b9(5) 5 0 bacteria/hour
At t 5 10: b9(10) 5 210,000 bacteria/hour
Section 3.4
9. Q(t) 5 200(30 2 t)2 5 200(900 2 60t 1 t 2)
5 180,000 2 12,000t 1 200t 2
Q9(t) 5 212,000 1 400t
The rate of change of the amount of water in the tank after
10 minutes is Q9(10) 5 28000 gallons per minute.
Note that Q9(10) , 0, so the rate at which the water is
running out is positive. The water is running out at the rate
of 8000 gallons per minute.
13. a(t) 5 v9(t) 5 6t 2 2 18t 1 12
Find when acceleration is zero.
6t 2 2 18t 1 12 5 0
6(t 2 2 3t 1 2) 5 0
6(t 2 1)(t 2 2) 5 0
t 5 1 or t 5 2
At t 5 1, the speed is )v(1)) 5 )0) 5 0 m/sec.
At t 5 2, the speed is )v(2)) 5 )21) 5 1 m/sec.
d
dx
d
h9(x) 5 }}(x 3 2 2) 5 3x 2
dx
d
t9(x) 5 }}(x 3 1 3) 5 3x 2
dx
14. (a) g9(x) 5 }}(x 3) 5 3x 2
The average rate for the first 10 minutes is
Q(10) 2 Q(0)
80,000 2 180,000
}} 5 }} 5 210,000 gallons per
10 2 0
10
minute.
The water is flowing out at an average rate of 10,000
83
(b) The graphs of NDER g(x), NDER h(x), and NDER t(x)
are all the same, as shown.
gallons per minute over the first 10 min.
c(100)
100
11,000
100
10. (a) Average cost 5 }} 5 }} 5 $110 per machine
(b) c9(x) 5 100 2 0.2x
Marginal cost 5 c9(100) 5 $80 per machine
[24, 4] by [210, 20]
(c) Actual cost of 101st machine is
c(101) 2 c(100) 5 $79.90, which is very close to the
marginal cost calculated in part (b).
11. (a)
(c) f (x) must be of the form f (x) = x 3 1 c, where c is a
constant.
(d) Yes. f (x) 5 x 3
(e) Yes. f (x) 5 x 3 1 3
15. (a)
[0, 50] by [2500, 2200]
The values of x which make sense are the whole
numbers, x $ 0.
d
dx
3
1
1
x11
24
(b) Marginal revenue 5 r9(x) 5 }} 2000 1 2 }}
d
dx
1
[0, 200] by [22, 12]
(b) The values of x which make sense are the whole
numbers, x $ 0.
(c)
2
2000
x11
(x 1 1)(0) 2 (2000)(1)
2000
5 0 2 }}}
5 }}2
(x 1 1)2
(x 1 1)
5 }} 2000 2 }}
2000
2000
(c) r9(5) 5 }}2 5 }} < 55.56
36
(5 1 1)
The increase in revenue is approximately $55.56.
(d) The limit is 0. This means that as x gets large, one
reaches a point where very little extra revenue can be
expected from selling more desks.
12. v(t) 5 s9(t) 5 3t 2 2 12t 1 9
a(t) 5 v9(t) 5 6t 2 12
Find when velocity is zero.
3t 2 2 12t 1 9 5 0
3(t 2 2 4t 1 3) 5 0
3(t 2 1)(t 2 3) 5 0
t 5 1 or t 5 3
At t 5 1, the acceleration is a(1) 5 26 m/sec2
At t 5 3, the acceleration is a(3) 5 6 m/sec2
[0, 200] by [20.1, 0.2]
P is most sensitive to changes in x when )P9(x)) is
largest. It is relatively sensitive to changes in x between
approximately x 5 60 and x 5 160.
(d) The marginal profit, P9(x), is greatest at x < 106.44.
Since x must be an integer,
P(106) < 4.924 thousand dollars or $4924.
(e) P9(50) < 0.013, or $13 per package sold
P9(100) < 0.165, or $165 per package sold
P9(125) < 0.118, or $118 per package sold
P9(150) < 0.031, or $31 per package sold
P9(175) < 0.006, or $6 per package sold
P9(300) < 1026, or $0.001 per package sold
(f) The limit is 10. The maximum possible profit is
$10,000 monthly.
(g) Yes. In order to sell more and more packages, the
company might need to lower the price to a point
where they won’t make any additional profit.
84
Section 3.4
16. (a) 190 ft/sec
(b) 2 seconds
(c) After 8 seconds, and its velocity was 0 ft/sec then
(d) After about 11 seconds, and it was falling 90 ft/sec then
(e) About 3 seconds (from the rocket’s highest point)
(f) The acceleration was greatest just before the engine
stopped. The acceleration was constant from t 5 2 to
t 5 11, while the rocket was in free fall.
17. Note that “downward velocity” is positive when McCarthy
is falling downward. His downward velocity increases
steadily until the parachute opens, and then decreases to a
constant downward velocity. One possible sketch:
(b) The particle speeds up when its speed is increasing,
which occurs during the approximate intervals
1.153 # t # 2.167 and t $ 3.180. It slows down during
the approximate intervals 0 # t # 1.153 and
2.167 # t # 3.180. One way to determine the
endpoints of these intervals is to use a grapher to find
the minimums and maximums for the speed,
)NDER x(t)), using function mode in the window
[0, 5] by [0, 10].
(c) The particle changes direction at t < 1.153 sec and at
t < 3.180 sec.
(d) The particle is at rest “instantaneously” at
t < 1.153 sec and at t < 3.180 sec.
Downward velocity
(e) The velocity starts out positive but decreasing, it
becomes negative, then starts to increase, and becomes
positive again and continues to increase.
The speed is decreasing, reaches 0 at t < 1.15 sec, then
increases until t < 2.17 sec, decreases until
t < 3.18 sec when it is 0 again, and then increases after
that.
Time
18. (a) We estimate the slopes at several points as follows,
then connect the points to create a smooth curve.
t (days)
0
10
20
30
40
(f) The particle is at (5, 2) when
2t 3 2 13t 2 1 22t 2 5 5 5 at t < 0.745 sec,
t < 1.626 sec, and at t < 4.129 sec.
21. (a) s(ft)
50
50
Slope (flies/day) 0.5 3.0 13.0 14.0 3.5 0.5
p′ (slope)
20
t(sec)
5
(b) s9(1) 5 18, s9(2.5) 5 0, s9(3.5) 5 212
50
t
22. (a)
s(ft)
30
Horizontal axis: Days
Vertical axis: Flies per day
(b) Fastest: Around the 25th day
Slowest: Day 50 or day 0
5
t(sec)
19. The particle is at (5, 2) when 4t 3 2 16t 2 1 15t 5 5, which
occurs at t < 2.83.
20. The motion can be simulated in parametric mode using
x1(t) 5 2t 3 2 13t 2 1 22t 2 5 and y1(t) 5 2 in [26, 8] by
[23, 5].
(a) It begins at the point (25, 2) moving in the positive
direction. After a little more than one second, it has
moved a bit past (6, 2) and it turns back in the negative
direction for approximately 2 seconds. At the end of
that time, it is near (22, 2) and it turns back again in
the positive direction. After that, it continues moving in
the positive direction indefinitely, speeding up as it
goes.
(b) s9(1) 5 26, s9(2.5) 5 12, s9(3.5) 5 24
23. (a) The body reverses direction when v changes sign, at
t 5 2 and at t 5 7.
(b) The body is moving at a constant speed, )v) 5 3 m/sec,
between t 5 3 and t 5 6.
Section 3.4
(c) The speed graph is obtained by reflecting the negative
portion of the velocity graph, 2 , t , 7, about the
x-axis.
85
Velocity graph:
v(t) (cm/sec)
4
Speed(m/sec)
2
3
2
1
1
2
4
6
8
10
t(sec)
2
3
4
2
3
4
5
6
t(sec)
–2
–1
–4
–2
Speed graph:
–3
320
120
23 2 3
3: a 5 }} 5 23 m/sec 2
321
23 2 (23)
6: a 5 }} 5 0 m/sec 2
623
3 2(23)
8: a 5 }} 5 3 m/sec 2
826
023
10: a 5 }} 5 21.5 m/sec 2
10 2 8
(d) For 0 # t , 1: a 5 }} 5 3 m/sec 2
For 1 , t ,
For 3 , t ,
For 6 , t ,
For 8 , t #
Acceleration (m/sec2)
3
2
1
(1, 3)
(6, 3) (8, 3)
(3, 0)
2
(6, 0)
4
6
8
(8, –1.5)
–1
–2
–3
(3, –3)
10
t(sec)
(10, –1.5)
(1, –3)
24. (a) The particle is moving left when the graph of s has
negative slope, for 2 , t , 3 and for 5 , t # 6.
The particle is moving right when the graph of s has
positive slope, for 0 # t , 1.
The particle is standing still when the graph of s is
horizontal, for 1 , t , 2 and for 3 , t , 5.
220
120
(b) For 0 # t , 1: v 5 }} 5 2 cm/sec
Speed 5 )v) 5 2 cm/sec
222
221
For 1 , t , 2: v 5 }} 5 0 cm/sec
Speed 5 )v) 5 0 cm/sec
22 2 2
322
For 2 , t , 3: v 5 }} 5 24 cm/sec
Speed 5 )v) 5 4 cm/sec
222(22)
523
For 3 , t , 5: v 5 }} 5 0 cm/sec
Speed 5 )v) 5 0 cm/sec
24 2(22)
625
For 5 , t # 6: v 5 }} 5 22 cm/sec
Speed 5 )v) 5 2 cm/sec
|v(t)| (cm/sec)
4
2
1
5
6
t(sec)
–2
–4
25. (a) The particle moves forward when v . 0, for
0 # t , 1 and for 5 , t , 7.
The particle moves backward when v , 0, for
1 , t , 5.
The particle speeds up when v is negative and
decreasing, for 1 , t , 2, and when v is positive and
increasing, for 5 , t , 6.
The particle slows down when v is positive and
decreasing, for 0 # t , 1 and for 6 , t , 7, and when
v is negative and increasing, for 3 , t , 5.
dv
dt
(b) Note that the acceleration a 5 }} is undefined at
t 5 2, t 5 3, and t 5 6.
The acceleration is positive when v is increasing, for
3 , t , 6.
The acceleration is negative when v is decreasing, for
0 # t , 2 and for 6 , t , 7.
The acceleration is zero when v is constant, for
2 , t , 3 and for 7 , t # 9.
(c) The particle moves at its greatest speed when )v) is
maximized, at t 5 0 and for 2 , t , 3.
(d) The particle stands still for more than an instant when v
stays at zero, for 7 , t # 9.
86
Section 3.4
26. (a) To graph the velocity, we estimate the slopes at several
points as follows, then connect the points to create a
smooth curve.
t (hours)
0
2.5
5
7.5
10 12.5
v (km/hour)
0
56
75
56
0
(b) v 5 s9(t) 5 980t
a 5 s0(t) 5 980
172
4
The velocity was s9 }} 5 560 cm/sec.
15
294 2225
172
4
The acceleration was s0 }} 5 980 cm/sec 2.
v(km/hr)
4
7
(c) Since there were about 16 flashes during }} of a second,
100
5
15
the light was flashing at a rate of about 28 flashes per
t(hours)
second.
–100
–200
–300
To graph the acceleration, we estimate the slope of the
velocity graph at several points as follows, and then
connect the points to create a smooth curve.
t (hours)
2
v (km/hour )
0
2.5
5
7.5
10
12.5
30
15
0
215 230 245 260
a(km/hr2)
50
15
28. Graph C is position, graph A is velocity, and graph B is
acceleration.
A is the derivative of C because it is positive, negative, and
zero where C is increasing, decreasing, and has horizontal
tangents, respectively. The relationship between B and A is
similar.
29. Graph C is position, graph B is velocity, and graph A is
acceleration.
B is the derivative of C because it is negative and zero
where C is decreasing and has horizontal tangents,
respectively.
A is the derivative of B because it is positive, negative, and
zero where B is increasing, decreasing, and has horizontal
tangents, respectively.
25
10
15
t(hours)
dy
dt
d
t 2
dt
12
d
t
t2
5 }} 6 1 2 }} 1 }}
dt
6
144
d
1
5 }} 6 2 t 1 }}t 2
dt
24
t
t
5 0 2 1 1 }} 5 }} 2 1
12
12
31
31
1
24
30. (a) }} 5 }} 6 1 2 }}
–25
–50
ds
dt
(b) }} 5 30t 2 3t 2
2
24
dy
dt
(b) The fluid level is falling fastest when }} is the most
dy
dt
negative, at t 5 0, when }} 5 21. The fluid level is
dy
dt
falling slowest at t 5 12, when }} 5 0.
[0, 15] by [2300, 100]
(c)
d 2s
}}2 5 30 2 6t
dt
[0, 12] by [22, 6]
dy
dt
y is decreasing and }} is negative over the entire
[0, 15] by [2100, 50]
interval. y decreases more rapidly early in the interval,
The graphs are very similar.
4
7
27. (a) Solving 160 5 490t 2 gives t 5 6}}.
4
7
It took }} of a second. The average velocity was
160 cm
} sec = 280 cm/sec.
4
12
}}
7
dy
dt
dy
dt
and the magnitude of }} is larger then. }} is 0 at
t 5 12, where the graph of y seems to have a horizontal
tangent.
Section 3.5
dV
dr
1
d 4
dr 3
87
37. (a) Assume that f is even. Then,
2
31. (a) }} 5 }} }}pr 3 5 4pr 2
f(2x 1 h) 2 f(2x)
h
f(x 2 h) 2 f(x)
5 lim }}, and substituting k 5 2h,
h
h→0
f(x 1 k) 2 f(x)
5 lim }}
2k
k→0
f(x 1 k) 2 f(x)
5 2lim }} 5 2f 9(x)
k
k→0
f 9(2x) 5 lim }}
dV
dr
When r 5 2, }} 5 4p(2)2 5 16p cubic feet of
h→0
volume per foot of radius.
(b) The increase in the volume is
4
4
}}p(2.2)3 2 }}p(2)3 < 11.092 cubic feet.
3
3
So, f 9 is an odd function.
32. For t . 0, the speed of the aircraft in meters per second
20
9
3600 sec
1h
1 km
1000 m
after t seconds is }}t. Multiplying by }} ? }},
(b) Assume that f is odd. Then,
f(2x 1 h) 2 f(2x)
h
2f(x 2 h) 1 f(x)
5 lim }},
h
h→0
f 9(2x) 5 lim }}
we find that this is equivalent to 8t kilometers per hour.
h→0
Solving 8t 5 200 gives t 5 25 seconds. The aircraft takes
25 seconds to become airborne, and the distance it travels
and substituting k 5 2h,
during this time is D(25) < 694.444 meters.
2f(x 1 k) 1 f(x)
2k
f(x 1 k) 2 f(x)
5 lim }} 5 f 9(x)
k
k→0
5 lim }}
k→0
33. Let v0 be the exit velocity of a particle of lava. Then
ds
dt
s(t) 5 v0t 2 16t 2 feet, so the velocity is }} 5 v0 2 32t.
v
ds
Solving }} 5 0 gives t 5 }}0 . Then the maximum height, in
dt
32
v 2
v
v
v 2
feet, is s }}0 5 v0 }}0 2 16 }}0 5 }0}. Solving
64
32
32
32
v0 2
}} 5 1900 gives v0 < 6348.712. The exit velocity was
64
3600 sec
1 mi
about 348.712 ft/sec. Multiplying by }} ? }}, we
1h
5280 ft
1 2
1 2
1 2
find that this is equivalent to about 237.758 mi/h.
34. By estimating the slope of the velocity graph at that point.
35. Since profit 5 revenue 2 cost, the Sum and Difference
d
dx
d
dx
d
dx
Rule gives }}(profit) 5 }}(revenue) 2 }}(cost), where x is
the number of units produced. This means that marginal
profit 5 marginal revenue 2 marginal cost.
36. (a) It takes 135 seconds.
DF
Dt
520
73 2 0
5
73
(b) Average speed 5 }} 5 }} 5 }}
< 0.068 furlongs/sec.
So, f 9 is an even function.
d
dx
d
dx
d
d
dx
dx
dh
dg
df
5 f g ? }} 1 h ? }} 1 gh ? }}
dx
dx
dx
dg
dh
df
5 }} gh 1 f }} h 1 fg }}
dx
dx
dx
38. }}(fgh) 5 }}[f(gh)] 5 f ? }}(gh) 1 gh ? }}( f)
1
1 2
1 2
Exploration 1
Making a Conjecture with NDER
1. When the graph of sin x is increasing, the graph of
NDER (sin x) is positive (above the x-axis).
2. When the graph of sin x is decreasing, the graph of
NDER (sin x) is negative (below the x-axis).
3. When the graph of sin x stops increasing and starts
decreasing, the graph of NDER (sin x) crosses the x-axis
from above to below.
4. The slope of the graph of sin x matches the value of
NDER (sin x) at these points.
5. We conjecture that NDER (sin x) 5 cos x. The graphs
coincide, supporting our conjecture.
speed is approximately
(d) The horse is running the fastest during the last furlong
(between 9th and 10th furlong markers). This furlong
takes only 11 seconds to run, which is the least amount
of time for a furlong.
(e) The horse accelerates the fastest during the first furlong
(between markers 0 and 1).
1 2
■ Section 3.5 Derivatives of Trigonometric
Functions (pp. 134–141)
(c) Using a symmetric difference quotient, the horse’s
DF
422
2
1
}} 5 }} 5 }} 5 }} < 0.077 furlongs/sec.
Dt
59 2 33
26
13
2
[22p, 2p] by [24, 4]
88
Section 3.5
6. When the graph of cos x is increasing, the graph of
NDER (cos x) is positive (above the x-axis).
When the graph of cos x is decreasing, the graph of
NDER (cos x) is negative (below the x-axis).
When the graph of cos x stops increasing and starts
decreasing, the graph of NDER (cos x) crosses the x-axis
from above to below.
The slope of the graph of cos x matches the value of
NDER (cos x) at these points.
We conjecture that NDER (cos x) 5 2sin x. The graphs
coincide, supporting our conjecture.
d
dx
3
d
dx
d
dx
d
dx
5. }}(4 2 x 2 sin x)5 }}(4) 2 x 2}}(sin x) 1 (sin x)}}(x 2)
5 0 2[x cos x 1 (sin x)(2x)]
2
4
5 2x 2 cos x 2 2x sin x
d
dx
3 dx
d
dx
d
d
dx
4
6. }}(3x 1 x tan x) 5 }}(3x) 1 x}}(tan x) 1 (tan x)}}(x)
5 3 1 x sec x 1 tan x
2
1 2
d
4
dx cos x
d
dx
7. }} }} 5 }}(4 sec x) 5 4 sec x tan x
d
[22p, 2p] by [24, 4]
d
Quick Review 3.5
1. 135° ? }} 5 }} < 2.356
(1 1 cot x)(2csc 2 x) 2 (cot x)(2csc 2 x)
(1 1 cot x)
5 }}}}}
2
1p2
180°
306
2. 1.7 ? }} 5 }} ° < 97.403°
p
csc2 x
(1 1 cot x)
d
2
(1 1 sin x)(2sin x) 2 (cos x)(cos x)
(1 1 sin x)
2sin x 2 sin 2 x 2 cos 2 x
(1 1 sin x)
5 }}}
2
Range: All reals
6. cos a 5 6Ï1ww
2wsin
w2waw 5 6Ï1ww
2(2
w1ww
)2 5 6Ï0w 5 0
2(1 1 sin x)
(1 1 sin x)
5 }}
2
3p
4
7. If tan a 5 21, then a 5 }} 1 kp for some integer k, so
1
sin a 5 6}}.
Ïw2
1 2 cos 2 h
(1 2 cos h)(1 1 cos h)
1 2 cos h
8. }} 5 }}} 5 }}
h(1 1 cos h)
h(1 1 cos h)
h
sin2 h
5 }}
h(1 1 cos h)
9. y9(x) 5 6x 2 14x
y9(3) 5 12
The tangent line has slope 12 and passes through (3, 1), so
its equation is y 5 12(x 2 3) 1 1, or y 5 12x 2 35.
2
10. a(t) 5 v9(t) 5 6t 2 2 14t
a(3) 5 12
Section 3.5 Exercises
d
dx
1. }}(1 1 x 2 cos x) 5 0 1 1 2(2sin x) 5 1 1 sin x
d
dx
2. }}(2 sin x 2 tan x) 5 2 cos x 2 sec 2 x
2
1
x
3. }} }} 1 5 sin x 5 2}}2 1 5 cos x
d
dx
d
dx
d
5 }}}}
2
kp
5. Domain: x Þ }} for odd integers k
2
1
1
(sin x 1 cos x)
(1 1 sin x)}}(cos x) 2 (cos x)}}(1 1 sin x)
d
cos x
dx
dx
10. }} }} 5 }}}}}
dx 1 1 sin x
(1 1 sin x)2
4. Domain: All reals
Range: [21, 1]
d 1
dx x
csc2 x sin2 x
(1 1 cot x) sin x
5 2}}2 5 2}}
2
2 5 2}}
2
Ï3w
p
3. sin }} 5 }}
3
d
(1 1 cot x)}}(cot x) 2 (cot x)}}(1 1 cot x)
d
cot x
dx
dx
9. }} }} 5 }}}}}
(1 1 cot x)2
dx 1 1 cot x
3p
4
p
180°
d
(1 1 cos x)}}(x) 2 x }}(1 1 cos x)
d
x
dx
dx
8. }} }} 5 }}}}
(1 1 cos x)2
dx 1 1 cos x
1 1 cos x 1 x sin x
5 }}
(1 1 cos x)2
d
dx
4. }}(x sec x) 5 x}}(sec x) 1 sec x}}(x)
5 x sec x tan x 1 sec x
1
1 1 sin x
5 2}}
d
dx
11. y9(x) 5 }}(sin x 1 3) 5 cos x
y9(p) 5 cos p 5 21
The tangent line has slope 21 and passes through
(p, sin p 1 3) 5 (p, 3).
Its equation is y 5 21(x 2 p) 1 3, or y 5 2x 1 p 1 3.
Section 3.5
d
d
d
x}}(tan x) 2 tan x}}(x)
d tan x
dx
dx
12. y9(x) 5 }} }} 5 }}}
x2
dx x
x sec2 x 2 tan x
x
p
2)2 2 1
}} ? (Ïw
4
p
8p 2 16
}}
y9 }} 5
5 }}
p 2
4
p2
}}
142
and passes through
1
1 2
2
d cos x
dx sin x
d
dx
16. (a) }} cot x 5 }} }}
p2
p2
The normal line has slope 2}} 5 }}
8p 2 16
16 2 8p
p
tan }}
p
4
}}, }
p
4
}}
4
d
1 4 p2
p 4
(sin x)(2sin x) 2 (cos x)(cos x)
sin x
5 }}}}
2
2
p
p2
4
Its equation is y 5 }} x 2 }} 1 }}, or
4
16 2 8p
p
p2
16 2 8p
p3
64 2 32p
d
(sin x)}}(cos x) 2 (cos x)}}(sin x)
dx
dx
5 }}}}
(sin x)2
5 }}, }} .
1
d
(cos x)}}(1) 2 (1)}}(cos x)
d
d 1
dx
dx
(b) }} sec x 5 }} }} 5 }}}
(cos x)2
dx
dx cos x
(cos x)(0) 2 (1)(2sin x)
5 }}}
cos 2 x
sin x
5 }}
5 sec x tan x
cos2 x
5 }}
2
12
89
2(sin2 x 1 cos2 x)
sin x
5 }}
2
4
p
y 5 }}x 2 }} 1 }}.
1
sin x
2
5 2}}
2 5 2csc x
Using decimals, this equation is approximately
d
dx
d 1
dx sin x
(b) }} csc x 5 }} }}
y 5 21.081x 1 2.122.
d
d
dx
d
dx
d
dx
13. y9(x) 5 }}(x 2 sin x) 5 x 2}}(sin x) 1 (sin x)}}(x 2)
(sin x)(0) 2 (1)(cos x)
sin x
5 x 2 cos x 1 2x sin x
5 }}}
2
y9(3) 5 9 cos 3 1 6 sin 3
The tangent line has slope 9 cos 3 1 6 sin 3 and passes
through (3, 9 sin 3). Its equation is
y 5 (9 cos 3 1 6 sin 3)(x 2 3) 1 9 sin 3, or
y 5 (9 cos 3 1 6 sin 3)x 2 27 cos 3 2 9 sin 3. Using
decimals, this equation is approximately
y 5 28.063x 1 25.460.
cos (x 1 h) 2 cos x
h
14. lim }}}
h→0
(cos x cos h 2 sin x sin h) 2 cos x
h
cos x(cos h 2 1) 2 sin x sin h
h
1
cos h 2 1
h
so the slope of the tangent line is 0.
d
dx
sin h
h
12
p
2
1 h→0
cos h 2 1
h
2
1 h→0
sin h
h
2
5 (cos x) lim }} 2 (sin x) lim }}
5 (cos x)(0) 2 (sin x)(1) 5 2sin x
d
d
(cos x)}}(sin x) 2 (sin x)}}(cos x)
d
d sin x
dx
dx
15. (a) }} tan x 5 }} }} 5 }}}}
(cos x)2
dx
dx cos x
(cos x)(cos x) 2 (sin x)(2sin x)
5 }}}}
cos 2 x
cos2 x 1 sin2 x
cos x
d
dx
the tangent line is 0. }} cos x 5 2sin x which is 0 at x 5 0,
19. y9(x) 5 }}(Ï2w cos x) 5 2Ï2w sin x
5 lim (cos x)}} 2 (sin x)}}
h→0
d
dx
17. }} sec x 5 sec x tan x which is 0 at x 5 0, so the slope of
d
1
dx
cos x
d
1
, which is never 0.
}} cot x 5 2csc 2 x 5 2}}
dx
sin2 x
5 lim }}}}
h→0
cos x
sin x
5 2}}
2 5 2csc x cot x
18. }} tan x 5 sec 2 x 5 }}
2 , which is never 0.
5 lim }}}}
h→0
d
(sin x)}}(1) 2 (1)}}(sin x)
dx
dx
5 }}}
(sin x)2
1
cos x
2
5 }}
5 }}
2
2 5 sec x
1 2
p
1
y9 }} 5 2Ï2w sin }} 5 2Ï2w }} 5 21
4
4
Ï2w
The tangent line has slope 21 and passes through
1}4}, Ï2w cos }4}2 5 1}4}, 12, so its equation is
p
p
y 5 21 x 2 }} 1 1, or y 5 2x 1 }} 1 1.
1 42
4
p
p
p
14 2
p
The normal line has slope 1 and passes through }}, 1 , so
1
p
4
2
p
4
its equation is y 5 1 x 2 }} 1 1, or y 5 x 1 1 2 }}.
90
Section 3.5
d
dx
y9(x) 5 0
(b)
20. y9(x) 5 }}tan x 5 sec 2 x
2Ï2w csc x cot x 2 csc 2 x 5 0
d
dx
y9(x) 5 }}(2x) 5 2
Ïw2 cos x
1
2}}
2 }}
50
2
2
sin x
sin x
1
2}}
(Ï2w cos x 1 1) 5 0
sin2 x
sec 2 x 5 2
sec x 5 6Ï2w
1
1
cos x 5 6}}
Ïw2
1
p p
2 2
2
p
4
On 2}}, }} , the solutions are x 5 6}}. The points on the
1
1 2
3p
4
p
curve are 2}}, 21 and }}, 1 .
d
21. y9(x) 5 }}(4 1 cot x 2 2 csc x)
dx
14 2
3p
5 0 2 csc x 1 2 csc x cot x
The coordinates of Q are }}, 2 .
5 2csc 2 x 1 2 csc x cot x
p
p
2
The equation of the horizontal line is y 5 2.
p
2
p
2
(a) y9 }} 5 2csc 2 }} 1 2 csc }} cot }}
5 212 1 2(1)(0) 5 21
The tangent line has slope 21 and passes through
12 2
1
p
p
2
2
P }}, 2 . Its equation is y 5 21 x 2 }} 1 2, or
p
2
y 5 2x 1 }} 1 2.
Speed: )2Ï2w) 5 Ï2w m/sec
p
4
2 cos x
sin x
2 }}
50
2 1 }}
2
1
(2 cos x 2 1) 5 0
}}
sin2 x
1
cos x 5 }}
2
p
x 5 }} at point Q
3
p
p
p
y }} 5 4 1 cot }} 2 2 csc }}
3
3
3
1
2
5 4 1 }} 2 2 }}
Ïw3
Ïw3
3
5 4 2 }} 5 4 2 Ï3w
Ïw3
p
The coordinates of Q are }}, 4 2 Ï3w .
3
12
p
4
(b) Velocity: 22 cos }} 5 2Ï2w m/sec
p
4
Jerk: 2 cos }} 5 Ï2w m/sec 3
2csc 2 x 1 2 csc x cot x 5 0
1
sin x
23. (a) Velocity: s9(t) 5 22 cos t m/sec
Speed: )s9(t)) 5 )2 cos t) m/sec
Acceleration: s0(t) 5 2 sin t m/sec 2
Jerk: s-(t)5 2 cos t m/sec 3
Acceleration: 2 sin }} 5 Ï2w m/sec 2
y9(x) 5 0
(b)
5 1 1 Ï2w(Ï2w) 1 (21)
52
2
122
4
3p
4
3p
4
y }} 5 1 1 Ï2w csc }} 1 cot }}
2 14 2
p
4
cos x 5 2}}
Ïw2
3p
x 5 }} at point Q
1 2
1
2
The equation of the horizontal line is y 5 4 2 Ï3w.
d
dx
(c) The body starts at 2, goes to 0 and then oscillates
between 0 and 4.
Speed:
Greatest when cos t 5 61 (or t 5 kp), at the center of
the interval of motion.
kp
2
Zero when cos t 5 0 (or t 5 }}, k odd), at the
endpoints of the interval of motion.
Acceleration:
Greatest (in magnitude) when sin t 5 61
kp
2
(or t 5 }}, k odd)
Zero when sin t 5 0 (or t 5 kp)
22. y9(x) 5 }}(1 1 Ï2w csc x 1 cot x)
5 0 1 Ï2w(2csc x cot x) 1 (2csc 2 x)
Jerk:
5 2Ï2w csc x cot x 2 csc 2 x
Greatest (in magnitude) when cos t 5 61 (or t 5 kp)
12
p
4
p
4
p
4
1
5 22 2 2 5 24
The tangent line has slope 24 and passes through
p
1
p
4
2
P }}, 4 . Its equation is y 5 24 x 2 }} 1 4, or
y 5 24x 1 p 1 4.
2
24. (a) Velocity: s9(t) 5 cos t 2 sin t m/sec
Speed: )s9(t)) 5 )cos t 2 sin t) m/sec
Acceleration: s0(t) 5 2sin t 2 cos t m/sec2
Jerk: s-(t) 5 2cos t 1 sin t m/sec3
5 2Ï2w(Ï2w)(1) 2 (Ï2w)2
14 2
kp
2
Zero when cos t 5 0 or t 5 }}, k odd
p
4
(a) y9 }} 5 2Ï2w csc }} cot }} 2 csc 2 }}
91
Section 3.5
p
4
p
4
d
dx
(b) Velocity: cos }} 2 sin }} 5 0 m/sec
cos (x 1 h) 2 cos x
h
(d) }} cos x 5 lim }}}
Speed: )0) 5 0 m/sec
h→0
cos x cos h 2 sin x sin h 2 cos x
h
(cos x)(cos h 2 1) 2 sin x sin h
5 lim }}}}
h
h→0
5 lim }}}}
h→0
p
p
4
4
p
p
Jerk: 2cos }} 1 sin }} 5 0 m/sec3
4
4
Acceleration: 2sin }} 2 cos }} 5 2Ï2
w m/sec2
(c) The body starts at 1, goes to Ï2w and then oscillates
between 6Ï2w.
Speed:
1 →0
21 →0
cos h 2 1
h
2 1 →0
21 →0
sin h
h
h
h
h
h
p
1 180 2
5 (cos x)(0) 2 (sin x) }}
p
180
5 2}} sin x
3p
Greatest when t 5 }} 1 kp
4
p
Zero when t 5 }} 1 kp
4
d2
dx
d p
dx 180
p
180
1
p
180
2
(e) }}2 sin x 5 }} }} cos x 5 }} 2}} sin x
p2
5 2}}2 sin x
180
d3
d
p2
p2 p
sin
x 5 }} 2}}2 sin x 5 2}}2 }} cos x
}}3
dx
dx
180
180 180
p3
5 2}}3 cos x
180
d2
d
p
p p
}}2 cos x 5 }} 2}} sin x 5 2}} }} cos x
dx
dx 180
180 180
p2
5 2}}2 cos x
180
d3
d
p2
p2
p
cos
x 5 }} 2}}2 cos x 5 2}}2 2}} sin x
}}3
dx
dx
180
180
180
p3
5 }}3 sin x
180
Acceleration:
p
4
Greatest (in magnitude) when t 5 }} 1 kp
3p
Zero when t 5 }} 1 kp
4
Jerk:
3p
4
Greatest (in magnitude) when t 5 }} 1 kp
p
4
Zero when t 5 }} 1 kp
1
2
1
2
1
25. (a)
1
1
2
2
2
1
2
d
dx
d
y0 5 }}(2csc x cot x)
dx
d
d
5 2(csc x)}}(cot x) 2 (cot x)}}(csc x)
dx
dx
26. y9 5 }} csc x 5 2csc x cot x
[2360, 360] by [20.01, 0.02]
p
180
The limit is }} because this is the conversion factor
for changing from degrees to radians.
5 2(csc x)(2csc2 x) 2 (cot x)(2csc x cot x)
(b)
5 csc3 x 1 csc x cot2 x
d
du
d
d
5 u}}(tan u) 1 (tan u)}}(u)
du
du
27. y9 5 }}(u tan u)
[2360, 360] by [20.02, 0.02]
5 u sec2 u 1 tan u
This limit is still 0.
sin (x 1 h) 2 sin x
d
(c) }} sin x 5 lim }}
dx
h
h→0
sin x cos h 1 cos x sin h 2 sin x
5 lim }}}}
h
h→0
sin x(cos h 2 1) 1 cos x sin h
5 lim }}}}
h
h→0
cos h 2 1
5 lim sin x lim }} 1 lim cos x
h
h→0
h→0
h→0
p
5 (sin x)(0) 1 (cos x) }}
180
p
5 }} cos x
180
1
21
2 1
1 2
d
du
d
d
d
5 u}}[(sec u)(sec u)] 1 (sec2 u)}}(u) 1 }}(tan u)
du
du
du
d
d
5 u (sec u)}}(sec u) 1 (sec u)}}(sec u) 1 sec2 u 1
du
du
y0 5 }}(u sec2 u 1 tan u)
3
}}2
21 lim
→0 h
sin h
h
2
5 lim cos x lim }} 2 lim sin x lim }}
sec2 u
5 2u sec2 u tan u 1 2 sec2 u
5 (2u tan u 1 2)(sec2 u)
or, writing in terms of sines and cosines,
2 1 2u tan u
cos u
2 cos u 1 2u sin u
5 }}
cos3 u
5 }}
2
4
92
Section 3.6
28. Continuous:
d
dx
d
dx
d
5 2}}(sin x cos x)
dx
d
d
5 2 (sin x)}}(cos x) 1 (cos x)}}(sin x)
dx
dx
33. }} sin 2x 5 }}(2 sin x cos x)
Note that g(0) 5 lim1 g(x) 5 lim1 cos x 5 cos (0) 5 1, and
x→0
x→0
lim2 g(x) 5 lim2 (x 1 b) 5 b. We require lim2 g(x) 5 g(0),
x→0
x→0
3
x→0
so b 5 1. The function is continuous if b 5 1.
Differentiable:
For b 5 1, the left-hand derivative is 1 and the right-hand
derivative is 2sin (0) 5 0, so the function
is not differentiable. For other values of b, the function is
discontinuous at x 5 0 and there is no
left-hand derivative. So, there is no value of b that will
make the function differentiable at x 5 0.
5 2[(sin x)(2sin x) 1 (cos x)(cos x)]
5 2(cos2 x 2 sin2 x)
5 2 cos 2x
d
dx
d
dx
34. }} cos 2x 5 }}[(cos x)(cos x) 2 (sin x)(sin x)]
3
d
}} cos x 5 2sin x
dx
d2
}}2 cos x 5 2cos x
dx
d3
}}3 cos x 5 sin x
dx
d4
}}4 cos x 5 cos x
dx
d
}}5
dx
d6
}}6
dx
d7
}}7
dx
d8
}}8
dx
5 22 sin 2x
cos x 5 cos x
(cos h 2 1)
h
h→0
cos2 h 2 1
h→0 h(cos h 1 1)
2sin2 h
5 lim }}
h→0 h(cos h 1 1)
1 h→0 h 21 h→0 cos h 1 1 2
0
5 2(1)1}}2 5 0
2
sin h
d
dx
d
y0 5 }}(A cos x 2 B sin x) 5 2A sin x 2 B cos x
dx
36. y9 5 }}(A sin x 1 B cos x) 5 A cos x 2 B sin x
dn
}}n sin x 5 cos x when n 5 4k 1 1 for any whole number
dx
k.
d 725
dx
Since 725 5 4(181) 1 1, }7}
25 sin x 5 cos x.
31. The line is tangent to the graph of y 5 sin x at (0, 0). Since
y9(0) 5 cos (0) 5 1,
the line has slope 1 and its equation is y 5 x.
32. (a) Using y 5 x, sin (0.12) < 0.12.
(b) sin (0.12) < 0.1197122; The approximation is within
0.0003 of the actual value.
y0 2 y 5 sin x
Solve:
(2A sin x 2 B cos x) 2 (A sin x 1 B cos x) 5 sin x
sin x 5 sin x
Continuing the pattern, we see that
sin h
5 2 lim }} lim }}
30. Observe the pattern:
sin x 5 2cos x
h→0
5 lim }}
d 999
dx
sin x 5 2sin x
(cos h 2 1)(cos h 1 1)
h(cos h 1 1)
35. lim }} 5 lim }}}
Since 999 5 4(249) 1 3, }9}
99 cos x 5 sin x.
sin x 5 cos x
4
5 22(2 sin x cos x)
cos x 5 sin x
k.
d5
}}5
dx
d6
}}6
dx
d7
}}7
dx
d8
} }8
dx
3
5 24 sin x cos x
cos x 5 2cos x
dn
}}n cos x 5 sin x when n 5 4k 1 3 for any whole number
dx
d
}} sin x 5 cos x
dx
d2
}}2 sin x 5 2sin x
dx
d3
}}3 sin x 5 2cos x
dx
d4
}}4 sin x 5 sin x
dx
d
dx
d
d
(sin x)}}(sin x) 1 (sin x)}}(sin x)
dx
dx
5 2(cos x)(2sin x) 2 2(sin x)(cos x)
cos x 5 2sin x
Continuing the pattern, we see that
4
d
dx
5 (cos x)}}(cos x) 1 (cos x)}}(cos x) 2
29. Observe the pattern:
5
4
22A sin x 2 2B cos x 5 sin x
p
1
At x 5 }}, this gives 22A 5 1, so A 5 2}}.
2
2
At x 5 0, we have 22B 5 0, so B 5 0.
1
2
Thus, A 5 2}} and B 5 0.
■ Section 3.6 Chain Rule (pp. 141–149)
Quick Review 3.6
1. f (g(x) 5 f (x 2 1 1) 5 sin (x 2 1 1)
2. f (g(h(x))) 5 f (g(7x) 5 f ((7x)2 1 1)
5 sin [(7x)2 1 1] 5 sin (49x 2 1 1)
3. (g + h)(x) 5 g(h(x)) 5 g(7x) 5 (7x)2 1 1 5 49x 2 1 1
4. (h + g)(x) 5 h(g(x)) 5 h(x 2 1 1) 5 7(x 2 1 1) 5 7x 2 1 7
1 h(x) 2 1
g(x)
x2 1 1
7x
2
x2 1 1
7x
5. f }} 5 f }} 5 sin }}
Section 3.6
6. Ïco
wswxw1
ww2 5 g(cos x) 5 g( f (x))
s2wxw
1w2 5 g(3 cos2 x) 5 g(h(cos x)) 5 g(h( f (x)))
7. Ï3wwcoww
dy
dx
1w3w
x 2 5 cos Ï3ww
x 2w
1w2 5 f (Ï3ww
x 2w
1w2)
10. cos Ï2ww
5 f (g(3x 2)) 5 f (g(h(x)))
1
dy
dx
d
dx
5 2(csc x 1 cot x)22}}(csc x 1 cot x)
1
(csc x 1 cot x)
d
dx
(csc x)(cot x 1 csc x)
(csc x 1 cot x)
d
dx
dy
dx
d
dx
5 25 sin26 x cos x 1 3 cos2 x sin x
d
dx
3. }} 5 }} cos (Ï3wx) 5 [2sin (Ï3wx)]}}(Ï3wx)
dy
dx
d
dx
d
dx
d
dx
5 (x 3)(4)(2x 2 5)3}}(2x 2 5) 1 (2x 2 5)4(3x 2)
5 [sec2 (2x 2 x 3)](2 2 3x 2) 5 (2 2 3x 2) sec2 (2x 2 x 3)
d
dx
3
1 24 3
1 24
2
x
1 24
5 (x 3)(4)(2x 2 5)3(2) 1 3x 2(2x 2 5)4
5 8x 3(2x 2 5)3 1 3x 2(2x 2 5)4
2
x
d
dx
2
10
2
5 25 csc2 }} (22x 22) 5 }}2 csc2 }}
x
x
x
3
5 25 csc2 }} }}(2x21)
dy
dx
5 x 2(2x 2 5)3[8x 1 3(2x 2 5)]
12
5 x 2(2x 2 5)3(14x 2 15)
2
d
sin x
sin x
d
sin x
5 2 }} }} }}
dx 1 1 cos x
1 1 cos x dx 1 1 cos x
1
2
6. }} 5 }} }}
1
2 1
d
2
d
1
21
(1 1 cos x)(cos x) 2 (sin x)(2sin x)
sin x
5 21}}21}}}} 2
(1 1 cos x)
1 1 cos x
cos x 1 cos x 1 sin x
sin x
5 21}}21}}}2
(1 1 cos x)
1 1 cos x
sin x
1 1 cos x
5 21}}21}}2
1 1 cos x (1 1 cos x)
sin x
1
5 21}}21}}2
1 1 cos x 1 1 cos x
sin x
5 2 }}
1 1 cos x
(1 1 cos x)}} sin x 2 sin x}}(1 1 cos x)
dx
dx
}}}}}
(1 1 cos x)2
dy
dx
2
d
dx
d
dx
d
dx
5 (sin3 x)(sec2 4x)}}(4x) 1 (tan 4x)(3 sin2 x)}} (sin x)
5 (sin3 x)(sec2 4x)(4) 1 (tan 4x)(3 sin2 x)(cos x)
2
2
2 sin x
5 }}2
(1 1 cos x)
5 4 sin3 x sec2 4x 1 3 sin2 x cos x tan 4x
d
dx
d
dx
5 2sin (sin x) cos x
d
dx
d
dx
1
d
5 4 ? }} }}(sec x 1 tan x)
2Ïse
wcwxw1
wwtan
wwx dx
5 }}(sec x tan x 1 sec2 x)
Ïse
wcwxw1
wwtan
wwx
sec x 1 tan x
5 2 sec x}}
Ïse
wcwxw1
wwtan
wwx
wcwxw1
wwtan
wwx
5 2 sec xÏse
d
dx
8. }} 5 }} sec (tan x) 5 sec (tan x) tan (tan x)}}(tan x)
5 sec (tan x) tan (tan x) sec2 x
dy
dx
wcwxw1
wwtan
wwx)
14. }} 5 }}(4Ïse
2
7. }} 5 }} cos (sin x) 5 [2sin (sin x)]}} (sin x)
dy
dx
d
dx
5 (sin3 x)}}(tan 4x) 1 (tan 4x)}}(sin3 x)
2
dy
dx
d
dx
13. }} 5 }}(sin3 x tan 4x)
2
2
d
dx
5 (x 3)}}(2x 2 5)4 1 (2x 2 5)4}}(x 3)
4. }} 5 }} tan (2x 2 x 3) 5 [sec2 (2x 2 x 3)]}}(2x 2 x 3)
dy
dx
d
dx
12. }} 5 }}[x 3 (2x 2 5)4]
5 [2sin (Ï3wx)](Ï3w) 5 2Ï3w sin (Ï3wx)
5. }} 5 }} 5 cot }}
d
dx
5 (25 sin26 x)}}(sin x) 2 (3 cos2 x)}}(cos x)
5 [cos (7 2 5x)](25) 5 25 cos (7 2 5x)
d
dx
d
dx
11. }} 5 }}(sin25 x 2 cos3 x)
d
dx
2. }} 5 }} sin (7 2 5x) 5 [cos (7 2 5x)]}}(7 2 5x)
d
dx
csc x
csc x 1 cot x
5 }}}
5 }}
2
5 [cos (3x 1 1)](3) 5 3 cos (3x 1 1)
dy
dx
d
dx
52}}2 (2cot x csc x 2 csc2 x)
d
dx
dy
dx
2
10. }} 5 }}(csc x 1 cot x)21
1. }} 5 }} sin (3x 1 1) 5 [cos (3x 11)]}}(3x 1 1)
dy
dx
1
5 22(x 1 Ïxw)23 1 1 }}
2Ïxw
Section 3.6 Exercises
dy
dx
d
dx
9. }} 5 }}(x 1 Ïxw)22 5 22(x 1 Ïxw)23}}(x 1 Ïxw)
wswxw1
ww2)2
8. 3 cos x 1 6 5 3(cos x 1 2) 5 3(Ïco
5 h(Ïco
wswxw1
ww2) 5 h(g(cos x)) 5 h(g( f (x)))
9. cos 27x 4 5 f (27x 4) 5 f (3(3x 2)2) 5 f (h(3x 2)) 5 f (h(h(x)))
d
dx
93
94
Section 3.6
dy
d
1
3
15. }} 5 }} }}
dx
dx Ï2wxw1
ww1
dy
dx
2
d
d
dx
5 3(1 1 cos2 7x)2}}(1 1 cos2 7x)
d
ww1)}}(3) 2 3}}(Ï2wxw1
ww1)
(Ï2wxw1
dx
dx
5 }}}}
(Ïw
2w
xw
1w1)2
1
d
dx
5 3(1 1 cos2 7x)2(2 cos 7x)}}(cos 7x)
d
dx
5 3(1 1 cos2 7x)2(2 cos 7x)(2sin 7x)}}(7x)
2
ww1)(0) 2 3 }1} }d}(2x 1 1)
(Ï2wxw1
2Ïw2xww
1w
1 dx
5 3(1 1 cos2 7x)2(2 cos 7x)(2sin 7x)(7)
5 }}}}}
2x 1 1
1
d
dx
19. }} 5 }}(1 1 cos2 7x)3
5 242(1 1 cos2 7x)2 cos 7x sin 7x
2
1
23 }} (2)
2Ïw2xww
1w1
5 }}
dy
d
1
3
5 2}}
(2x 1 1)Ï2wxw1
ww1
5 }}(sec2 5x)}}(5x)
dx
2Ïtwan
ww5xw
5 23(2x 1 1)23/2
5 }}(sec2 5x)(5)
2Ïtwan
ww5xw
1
d
1
5 sec2 5x
dy
d
d
wnww5xw) 5 }} }} tan 5x
20. }} 5 }}(Ïta
dx
dx
2Ïtwan
ww5xw dx
2x 1 1
5
5 }} or }}(tan 5x)21/2 sec2 5x
2
tan
2Ïw
ww5xw
x
16. }} 5 }} }}
dx
dx Ï1ww
1wx 2w
ds
dt
p
12 2
p
d p
5 32sin 1}} 2 3t24}}1}} 2 3t2
2
dt 2
p
5 32sin 1}} 2 3t24(23)
2
p
5 3 sin 1}} 2 3t2
2
d
dt
21. }} 5 }} cos }} 2 3t
d
d
(Ïw1w
1wx 2w)}}(x) 2 x}}(Ïw
1w
1wx 2w)
dx
dx
}}}}
5
(Ïw
1w
1wx 2w)2
1
2
1
d
(Ï1ww
1wx 2w)(1) 2 x }} }}(1 1 x 2)
1wx 2w dx
2Ï1
ww
5 }}}}}
1 1 x2
1 2Ï1ww1wxw 2
1
Ï1ww
1wx 2w 2 x }} (2x)
2
ds
dt
11x
(1 1 x ) 2 x
2
d
dt
22. }} 5 }}[t cos (p 2 4t)]
5 }}}
2
d
dt
d
dt
5 (t)}}[cos (p 2 4t)] 1 cos (p 2 4t)}}(t)
2
5 }}
(1 1 x 2)(Ï1ww
1wx 2w)
5 t[2sin (p 2 4t)]}}(p 2 4t) 1 cos (p 2 4t)(1)
5 (1 1 x2)23/2
5 t[2sin (p 2 4t)](24) 1 cos (p 2 4t)
d
dt
5 4t sin (p 2 4t) 1 cos (p 2 4t)
17. The last step here uses the identity 2 sin a cos a 5 sin 2a.
dy
d
}} 5 }} sin2 (3x 2 2)
dx
dx
d
5 2 sin (3x 2 2)}} sin (3x 2 2)
dx
d
5 2 sin (3x 2 2) cos (3x 2 2)}}(3x 2 2)
dx
ds
dt
3 12 2
1 4 24
3p d 3p
7p d 7p
5 cos 1}}t2}}1}}t2 2 sin 1}}t2}}1}}t2
2 dt 2
4 dt 4
3p
3p
7p
7p
5 }} cos 1}}t2 2 }} sin 1}}t2
2
2
4
4
d
dx
d
dx
18. }} 5 }}(1 1 cos 2x)2 5 2(1 1 cos 2x)}}(1 1 cos 2x)
d
dx
5 2(1 1 cos 2x)(2sin 2x)}}(2x)
5 2(1 1 cos 2x)(2sin 2x)(2)
5 24(1 1 cos 2x)(sin 2x)
3p
d
dt
7p
24. }} 5 }} sin }}t 1 cos }}t
5 3 sin (6x 2 4)
dy
dx
2
d 4
4
dt 3p
5p
4
d
4
d
5 }}(cos 3t)}}(3t) 1 }}(2sin 5t)}}(5t)
3p
dt
5p
dt
4
4
5 }}(cos 3t)(3) 1 }}(2sin 5t)(5)
3p
5p
4
4
5 }} cos 3t 2 }} sin 5t
p
p
5 2 sin (3x 2 2) cos (3x 2 2)(3)
5 6 sin (3x 2 2) cos (3x 2 2)
1
ds
dt
23. }} 5 }} }} sin 3t 1 }} cos 5t
dr
du
d
du
d
du
25. }} 5 }} tan (2 2 u) 5 sec2 (2 2 u)}}(2 2 u)
5 sec2 (2 2 u)(21) 5 2sec2 (2 2 u)
dr
du
d
du
26. }} 5 }}(sec 2u tan 2u)
d
du
d
du
5 (sec 2u)}}(tan 2u) 1 (tan 2u)}}(sec 2u)
d
du
d
du
5 (sec 2u)(sec2 2u)}}(2u) 1 (tan 2u)(sec 2u tan 2u)}}(2u)
5 2 sec3 2u 1 2 sec 2u tan2 2u
Section 3.6
dr
1
d
d
27. }} 5 }}Ïuwwsin
wwu 5 }} }}(u sin u)
du
du
2Ïu
wwsin
wwu du
3
1
d
d
5 }} u}}(sin u) 1 (sin u)}}(u)
du
2Ïu
wwsin
wwu du
4
1
5 }}(u cos u 1 sin u)
2Ïw
uwsw
inwu
u cos u 1 sin u
5 }}
2 Ïw
uwsw
inw
u
dr
du
d
du
d
du
5 (2u)}}(Ïse
wcwuw) 1 (Ïse
wcwuw)}}(2u)
1
2
1
5 (2u)1}}2(sec u tan u) 1 2Ïse
wcwuw
2Ïw
secwu
w
1
d
wcwuw
5 (2u) }} }}(sec u) 1 2Ïse
2Ïswecwu
w du
5 u(Ïse
wcwuw)(tan u) 1 2Ïse
wcwuw
5 Ïse
wcwuw(u tan u 1 2)
12
12
pu
10
pu
p
5 2}} csc2 }}
10
10
5
d
g9(x) 5 }}(5Ïxw) 5 }}
dx
2Ïwx
d
du
1
pu d pu
2
1 10 2 du 1 10 2
35. f 9(u) 5 }} cot }} 5 2csc2 }} }} }}
3
1 2
1 241 2
12
d
du
36. f 9(u) 5 }}[u 1 (cos u)22]
5 2 sec x tan x
2
d
du
5 1 2 2(cos u)23}} cos u
d
dx
d
d
y0 5 }}(2csc2 x) 5 (22 csc x)}}(csc x)
dx
dx
30. y9 5 }} cot x 5 2csc2 x
5 (22 csc x)(2csc x cot x)
5 2 csc2 x cot x
d
dx
d
dx
31. y9 5 }} cot (3x 2 1) 5 2csc2 (3x 2 1)}}(3x 2 1)
5 23 csc2 (3x 2 1)
d
dx
y0 5 }}[23 csc2(3x 2 1)]
2 sin u
cos u
5 1 1 }}
3
d
dx
1
1
1
( f + g)9 }} 5 f 9(g(}}))g9 }}
4
4
4
p
1
5 f 9 }} g9 }}
4
4
g9(x) 5 }}(px) 5 p
12
12
1 2 12
5
1
2
}}
Ï2w
2
1 1 }3 (p)
1}Ï}2w 2
1
5 5p
d
5 23[2 csc (3x 2 1)]}} csc (3x 2 1)
dx
5 23[2 csc (3x 2 1)] ?
d
dx
[2csc (3x 2 1) cot (3x 2 1)]}}(3x 2 1)
5 23[2 csc (3x 2 1)][2csc (3x 2 1) cot (3x 2 1)](3)
5 18 csc2 (3x 2 1) cot (3x 2 1)
1 3 24 5 9 sec2 1}3}2}d}x 1}3}2
x
5 3 sec2 1}}2
3
d
x
x d
x
y0 5 }}33 sec2 1}}24 5 332 sec 1}}24}} sec 1}}2
dx
3
3 dx
3
x
x
x d x
5 63sec 1}}243sec 1}}2 tan 1}}24}} 1}}2
3
3
3 dx 3
x
x
5 2 sec2 1}}2 tan 1}}2
3
3
x
d
1
du
u
d
d
g9(x) 5 }}(1 2 x)21 5 2(1 2 x)22}}(1 2 x)
dx
dx
1
5 2(1 2 x)22(21) 5 }}2
(1 2 x)
1
( f + g)9(21) 5 f 9(g(21))g9(21) 5 f 9 }} g9(21)
2
1
5 (4) }} 51
4
p 5
p
}}
2
2
10
5
p
p
5 2}}(1) }} 5 2}}
2
4
10
5 (2 sec x)(sec x tan x)
3
5
2
5 2}} csc2 }}
d
dx
d
d
y0 5 }} sec2 x 5 (2 sec x)}}(sec x)
dx
dx
d
dx
1
( f + g)9(1) 5 f 9(g(1))g9(1) 5 f 9(5)g9(1)
29. y9 5 }} tan x 5 sec2 x
32. y9 5 }} 9 tan }}
122
( f + g)9(1) 5 f 9(g(1))g9(1) 5 f 9(1)g9(1) 5 (5) }} 5 }}
34. f 9(u) 5 }}(1 2 u 21) 5 u 22 5 }}2
wcwuw)
28. }} 5 }}(2uÏse
d
du
d
du
1
d
g9(x) 5 }}(Ïxw) 5 }}
dx
2Ïwx
33. f 9(u) 5 }}(u 5 1 1) 5 5u 4
x d x
d
d
(u 2 11)}}(2u) 2 (2u)}}(u 2 11)
2u
d
du
du
5
37. f 9(u) 5 }} }
}}}}
}
(u 2 1 1)2
du u 2 1 1
(u 2 1 1)(2) 2 (2u)(2u)
22u 2 1 2
(u 1 1)
(u 1 1)
d
2
g9(x) 5 }}(10x 1 x 1 1) 5 20x 1 1
dx
5 }}}
5}
2
2
2 }
2
( f + g)9(0) 5 f 9(g(0))g9(0) 5 f 9(1)g9(0) 5 (0)(1) 5 0
95
96
Section 3.6
u21 d u21
d u21 2
5 2 }} }} }}
u 1 1 du u 1 1
du u 1 1
1
2
1
38. f 9(u) 5 }} }}
2 1
d
2
d
(u 1 1)}}(u 2 1) 2 (u 2 1)}}(u 1 1)
du
du
u21
5 2 }} }}}}
(u 1 1)2
u11
u 2 1 (u 1 1) 2 (u 2 1)
4(u 2 1)
5 2 }} }}
5 }}3
(u 1 1)2
u11
(u 1 1)
1
1
2
2
d
dx
dx
dt
d
dt
41. }} 5 }}(2 cos t) 5 22 sin t
dy
d
}} 5 }}(2 sin t) 5 2 cos t
dt
dt
dy
}} 5
dx
dy
}}
dt
}
dx
}}
dt
2 cos t
22 sin t
5 }} 5 2cot t
p
4
1
p
4
2
g9(x) 5 }}(x 22 2 1) 5 22x 23
The line passes through 2 cos }}, 2 sin }} 5 (Ï2w, Ï2w)
( f + g)9(21) 5 f 9(g(21))g9(21)
and has slope 2cot }} 5 21. Its equation is
5 f 9(0)g9(21)
5 (24)(2) 5 28
dy
dx
dy du
du dx
d
d
5 }}(cos u)}}(6x 1 2)
du
dx
39. (a) }} 5 }} }}
5 (2sin u)(6)
y 5 2(x 2 Ï2w) 1 Ï2w, or y 5 2x 1 2Ï2w.
dx
dt
d
dt
5 26 sin (6x 1 2)
dy du
du dx
d
d
5 }}(cos 2u)}}(3x 1 1)
du
dx
(b) }} 5 }} }}
5 (2sin 2u)(2) ? (3)
5 26 sin 2u
d
dt
42. }} 5 }}(sin 2pt) 5 (cos 2pt)}}(2pt) 5 2p cos 2pt
dy
d
d
}} 5 }}(cos 2pt) 5 (2sin 2pt)}}(2pt) 5 22p sin 2pt
dt
dt
dt
dy
}} 5
dx
5 26 sin u
dy
dx
p
4
dy
}}
dt
}
dx
}}
dt
22p sin 2pt
2p cos 2pt
5 }} 5 2tan 2pt
Ïw3 1
2p
2p
The line passes through sin }}, cos }} 5 2}}, }}
1
1
dx
dt
2
2
2
2
d
dt
d
dt
43. }} 5 }}(sec 2 t 2 1) 5 (2 sec t)}}(sec t)
5 (2 sec t)(sec t tan t)
5 26 sin (6x 1 2)
dy
dy
40. (a) }} 5 }}
dx
du
d
5 }}
du
2 1
26
26
2p
and has slope 2tan }} 5 Ï3w. Its equation is
26
Ïw3
1
y 5 Ï3ww x 1 }} 1 }}, or y 5 Ï3wx 1 2.
2
2
5 2 sec 2 t tan t
du
}}
dx
d
sin (u 1 1)}}(x 2)
dx
5 cos (u 1 1)(1) ? 2x
dy
d
}} 5 }} tan t 5 sec 2 t
dt
dt
dy
}} 5
dx
5 2x cos (u 1 1)
5 2x cos (x 2 1 1)
dy
}}
dt
}
dx
}}
dt
5 (cos u)(2x)
5 2x cos u
1
2
The line passes through
1sec 12}4}2 2 1, tan 12}4}22 5 (1, 21) and has
1
p
1
slope }} cot 12}}2 5 2}}. Its equation is
2
4
2
p
2
dy
dy du
(b) }} 5 }} }}
dx
du dx
d
d
5 }}(sin u)}}(x 2 1 1)
du
dx
sec2 t
2 sec t tan t
5 }2 } 5 }} cot t.
p
1
2
1
2
1
2
y 5 2}}(x 2 1) 2 1, or y 5 2}}x 2 }}.
dx
d
dt
dt
dy
d
}} 5 }} tan t 5 sec 2 t
dt
dt
44. }} 5 }} sec t 5 sec t tan t
5 2x cos (x 1 1)
2
dy
}} 5
dx
dy
}}
dt
}
dx
}}
dt
sec 2 t
sec t tan t
sec t
tan t
1
sin t
5 }} 5 }} 5 }} 5 csc t
1
2 1
2
p
2
1
has slope csc }} 5 2. Its equation is y 5 21x 2 }}2 1 }},
6
Ï3w
Ï3w
p
p
2
1
The line passes through sec }}, tan }} 5 }}, }} and
6
6
Ï3w Ï3w
or y 5 2x 2 Ï3w.
Section 3.6
dx
dt
dx
d
dt
dt
dy
d
}} 5 }} sin t 5 cos t
dt
dt
d
dt
49. (a) }} 5 }}(t 2 1 t) 5 2t 1 1
45. }} 5 }}t 5 1
dy
1
d
}} 5 }}Ïtw 5 }}
dt
dt
2Ïwt
dy
}} 5
dx
dy
}}
dt
}
dx
}}
dt
dy
}} 5
dx
1/(2Ïwt)
1
5 } } 5 }}
1
2Ïwt
1 !§2 1 2
1 2
1
1
1 1
The line passes through }}, }} 5 }}, }} and has slope
4
4
4 2
1
}
1
1
1 5 1. Its equation is y 5 1 x 2 }} 1 }}, or
4
2
2 }}
!§4
dy
}}
dt
}
dx
}}
dt
1 2
d dy
dt dx
d cos t
dt 2t 1 1
d
d
(2t 1 1)}}(cos t) 2 (cos t)}}(2t 1 1)
dt
dt
5 }}}}
(2t 1 1)2
(2t 1 1)(2sin t) 2 (cos t)(2)
(2t 1 1)
5 }}}
2
1
4
(2t 1 1)(sin t) 1 2 cos t
(2t 1 1)
5 2}}}
2
dx
d
dt
dt
dy
d
}} 5 }}(t 4) 5 4t 3
dt
dt
46. }} 5 }}(2t 2 1 3) 5 4t
dy
}} 5
dx
dy
dx
(c) Let u 5 }}.
4t 3
4t
5 }} 5 t 2
du
dt
dx
dt
1 2
1 2
(2t 1 1)(sin t) 1 2 cos t
(2t 1 1)
(d) The expression in part (c).
sin t
1 2 cos t
5 }}
50. Since the radius passes through (0, 0) and (2 cos t, 2 sin t),
it has slope given by tan t. But the slope of the tangent is
The line passes through
dy
}} 5
dx
Ïw3 1
1}3} 2 sin }3}, 1 2 cos }3}2 5 1}3} 2 }2}, }2}2 and has slope
p
p
p
p
p
sin }}
3
1 2
132
3
2
2
reciprocal of tan t. This means that the radius and the
kp
2
either the radius is horizontal and the tangent is vertical or
2
the radius is vertical and the tangent is horizontal, so the
p
y 5 Ï3wx 1 2 2 }}.
Ï3w
result still holds.)
dx
d
dt
dt
dy
d
}} 5 }}(1 1 sin t) 5 cos t
dt
dt
48. }} 5 }} cos t 5 2sin t
ds
dt
du
dt
d
du
1 dt 2
du
5 (2sin u) }}
3p
2
cos t
2sin t
1
ds du
du dt
51. }} 5 }} }} 5 }}(cos u) }}
du
dt
ds
dt
1
3p
2
2
When u 5 }} and }} 5 5, }} 5 2sin }} (5) 5 5.
5 }} 5 2cot t
p
2
p
2
2
The line passes through cos }}, 1 1 sin }} 5 (0, 2) and
12
22 cos t
2 sin t
5 }} 5 2cot t, which is the negative
down when t 5 }}, where k is an integer. At these values,
Ïw3
p
1
y 5 Ï3w x 2 }} 1 }} 1 }}, or
1
dy
}}
dt
}
dx
}}
dt
tangent are perpendicular. (The preceding argument breaks
}} 5 Ï3
w. Its equation is
p
1 2 cos }}
dy
}} 5
dx
du
dt
5 2}}}
3
dx
d
dt
dt
dy
d
}} 5 }}(1 2 cos t) 5 sin t
dt
dt
dy
}}
dt
}
dx
}}
dt
du
dx
dx
d dy
d dy
}} }} 5 }} }} 4 }}
dt
dx dx
dt dx
(2t 1 1)(sin t) 1 2 cos t
5 2}}}
4 (2t 1 1)
(2t 1 1)2
47. }} 5 }}(t 2 sin t) 5 1 2 cos t
dy
}} 5
dx
du dx
dx dt
Then }} 5 }} }}, so }} 5 }} 4 }}. Therefore,
The line passes through (2(21)2 1 3, (21)4) 5 (5, 1) and
has slope (21)2 = 1. Its equation is y 5 1(x 2 5) 1 1, or
y 5 x 2 4.
dy
}}
dt
}
dx
}}
dt
cos t
2t 1 1
5 }}
(b) }} }} 5 }} }}
y 5 x 1 }}.
dy
}}
dt
}
dx
}}
dt
97
p
has slope 2cot }} 5 0. Its equation is y 5 2.
2
dy
dt
dy dx
dx dt
dx
dt
d
dx
52. }} 5 }} }} 5 }}(x 2 1 7x 2 5)}}
1 dt 2
dx
5 (2x 1 7) }}
dy
dt
1 dy
3 dt
132
1
When x 5 1 and }} 5 }}, }} 5 [2(1) 1 7] }} 5 3.
98
Section 3.6
dy
dx
d
dx
1
x
2
2 12
1
2
dy
dx
1
2
x d x
2 dx 2
d
dx
(e) }} f(g(x)) 5 f 9(g(x))g9(x)
x
2
53. }} 5 }} sin }} 5 cos }} }} }} 5 }} cos }}
1
2
x
2
3
1 1
2 2
4
Since the range of the function f(x) 5 }} cos }} is 2}}, }} ,
the largest possible value of }} is }}.
dy
dx
d
dx
d
dx
54. }} 5 }}(sin mx) 5 (cos mx)}}(mx) 5 m cos mx
px
4
1
1 2
px
}}
4
142
p
1
f 9(x)
(f) }} Ïf(
wx)
w 5 } }} f(x) 5 }}
dx
2 Ïfw(x)
w dx
f (x)
2Ïw
w
d
1
}}
f 9(2)
3
} 5 } 5 }1} 5 }1}.
2Ïw
f (w
2w)
2Ï8
w
6(2Ï2
w) 12Ï2w
2 1 2
px d px
4 dx 4
55. }} 5 }} 2 tan }} 5 2 sec 2 }} }} }}
p
5 }} sec 2
2
p
y9(1) 5 }}
2
1
At x 5 2, the derivative is
through (0, 0), so its equation is y 5 mx.
d
dx
132
f 9(g(2))g9(2) 5 f 9(2)g9(2) 5 }} (23) 5 21.
d
The desired line has slope y9(0) 5 m cos 0 5 m and passes
dy
dx
At x 5 2, the derivative is
d 1
dx g (x)
d
dx
2g 9(x)
[g(x)]
d
dx
(g) }} }2 } 5 }}[g(x)]22 5 22[g(x)]23}}g(x) 5 2}}3
p
2
sec 2 }} 5 }}(Ï2w)2 5 p.
At x 5 3, the derivative is
The tangent line has slope p and passes through
2g 9(3)
[g(3)]
2(5)
(24)
10
264
5
32
2}}3 5 2}}3 5 2}} 5 }}.
11, 2 tan }4}2 5 (1, 2). Its equation is y 5 p(x 2 1) 1 2, or
p
y 5 px 2 p 1 2.
1
p
The normal line has slope 2}} and passes through (1, 2). Its
1
1
1
equation is y 5 2}}(x 2 1) 1 2, or y 5 2}}x 1 }} 1 2.
p
p
p
1
}} d
d
2
2
(h) }}Ïw
f 2(x
w)w1
wwg 2w(x)
w 5 2Ïw
2
f 2(x
w)w1
wwg w
(x)
w }d}x [ f (x) 1 g (x)]
dx
1
}}
d
d
5 2Ïw
f 2(x
w)w1
wwg 2w(x)
w [2f(x)}d}x f(x) 1 2g(x)}d}x g(x)]
f(x) f 9(x) 1 g(x)g9(x)
5 }}}
2
2
Graphical support:
Ïw
f (x
w)w1
wwg w(x)
w
At x 5 2, the derivative is
12
1
(8) }} 1 (2)(23)
3
f (2) f 9(2) 1 g(2)g9(2)
}}} 5 }}
2
2
Ïw
f w
(2w
)w
1w
g w(w
2w)
Ï8w2w1
ww22w
[24.7, 4.7] by [23.1, 3.1]
10
d
dx
56. (a) }}[2 f (x)] 5 2 f 9(x)
132
1
2
3
At x 5 2, the derivative is 2 f 9(2) 5 2 }} 5 }}.
d
(b) }}[ f (x) 1 g(x)] 5 f 9(x) 1 g9(x)
dx
At x 5 3, the derivative is f 9(3) 1 g9(3) 5 2p 1 5.
d
dx
(c) }}[ f (x) ? g(x)] 5 f(x)g9(x) 1 g(x) f 9(x)
At x 5 3, the derivative is
10
2}}
}}
3
3
5
}
5
5 2 } 5 2} }
Ïw6w8
2Ï1
w7w
3Ï1
w7w
d
dx
57. (a) }}[5 f (x) 2 g(x)] 5 5 f 9(x) 2 g9(x)
At x 5 1, the derivative is
1 32 1 32
1
d
dx
d
5 15 2 8p.
d
dx
dx
5 3 f (x)g 2(x)g9(x) 1 g 3(x) f 9(x)
At x 5 0, the derivative is 3 f(0)g 2(0)g9(0) 1 g 3(0) f 9(0)
132
1
5 3(1)(1)2 }} 1 (1)3(5) 5 6.
g(x) f 9(x) 2 f(x)g9(x)
[g(x)]
(d) }} }} 5 }}}
2
At x 5 2, the derivative is
12
1
(2) }} 2 (8)(23)
3
g(2) f 9(2) 2 f(2)g9(2)
5
}}}
}}
[g(2)]2
(2)2
74
}}
37
3
5}
5 }}.
4
6
d
dx
(b) }} f(x)g 3(x) 5 f(x)}}g 3(x) 1 g 3(x)}}f(x)
5 f (x)[3g 2(x)]}}g(x) 1 g 3(x) f 9(x)
f(3)g9(3) 1 g(3) f 9(3) 5 (3)(5) 1 (24)(2p)
d f(x)
dx g(x)
8
5 f 9(1) 2 g9(1) 5 5 2}} 2 2}} 5 1.
Section 3.6
d
99
d
dx
d
58. For y 5 sin 2x, y9 5 (cos 2x)}}(2x) 5 2 cos 2x and the
[g(x) 1 1]}}f(x) 2 f(x)}}[g(x) 1 1]
dx
dx
d
f (x)
(c) }} }} 5 }}}}
[g(x) 1 1]2
dx g(x) 1 1
slope at the origin is 2.
[g(x) 1 1] f 9(x) 2 f(x)g9(x)
[g(x) 1 1]
x
2
1
2 12
1
2
x d x
2 dx 2
x
2
For y 5 2sin }}, y9 5 2cos }} }} }} 5 2}} cos }} and the
5 }}}
2
1
2
slope at the origin is 2}}. Since the slopes of the two
At x 5 1, the derivative is
1 2
1 2
1
8
(24 1 1) 2}} 2 (3) 2}}
3
3
[g(1) 1 1] f 9(1) 2 f(1)g9(1)
5
}}}
}}}
[g(1) 1 1]2
(24 1 1)2
1
2
tangent lines are 2 and 2}}, the lines are perpendicular and
the curves are orthogonal.
A graph of the two curves along with the tangents y 5 2x
9
9
5 }} 5 1.
1
2
and y 5 2}}x is shown.
d
(d) }} f(g(x)) 5 f 9(g(x))g9(x)
dx
At x 5 0, the derivative is
1 3 21 3 2
1
1
1
9
f 9(g(0))g9(0) 5 f 9(1)g9(0) 5 2}} }} 5 2}}.
d
dx
(e) }} g( f(x)) 5 g9( f(x)) f 9(x)
[24.7, 4.7] by [23.1, 3.1]
At x 5 0, the derivative is
1 2
8
40
g9( f(0)) f 9(0) 5 g9(1) f 9(0) 5 2}} (5) 5 2}}
3
3
d
dx
d
dx
(f) }} [g(x) 1 f(x)]22 5 22[g(x) 1 f(x)]23 }}[g(x) 1 f(x)]
2[g9(x) 1 f 9(x)]
[g(x) 1 f(x)]
5 2}}
3
At x 5 1, the derivative is
2[g9(1) 1 f 9(1)]
[g(1) 1 f(1)]
1
8
3
1
3
2
2 2}} 2 }}
26
21
}}
2}}
3 5 2 (24 1 3)3 5 2}} 5 26.
d
dx
d
dx
(g) }} [ f(x 1 g(x))] 5 f 9(x 1 g(x))}}[x 1 g(x)]
dy dy
dx du
du
dx
59. Because the symbols }}, }}, and }} are not fractions. The
individual symbols dy, dx, and du do not have numerical
values.
60. Velocity: s9(t) 5 22pbA sin (2pbt)
acceleration: s0(t) 5 24p 2b 2A cos (2pbt)
jerk: s-(t) 5 8p 3b 3A sin (2pbt)
The velocity, amplitude, and jerk are proportional to b, b 2,
and b 3, respectively. If the frequency b is doubled, then the
amplitude of the velocity is doubled, the amplitude of the
acceleration is quadrupled, and the amplitude of the jerk is
multiplied by 8.
3 365
4
2p
d
dt
2p
3 365
4 ? }d}x 3}36}5 (x 2 101)4 1 0
5 f 9(x 1 g(x))(1 1 g9(x))
5 37 cos }}(x 2 101)
At x 5 0, the derivative is
5 37 cos }}(x 2 101)
1
1
3
12
1 21 2
5 f 9(1)
1
5 2}}
3
2
4
}}
3
4
4
}} 5 2}}.
3
9
d
2p
3 365
4 ? }36}5
74p
2p
5 }} cos 3}}(x 2 101)4
365
365
2p
f 9(0 1 g(0))(1 1 g9(0)) 5 f 9(0 1 1) 1 1 }}
d
dt
61. (a) y9(t) 5 }} 37 sin }}(x 2 101) 1 }}(25)
2p
Since cos u is greatest when u 5 0, 62p, and so on,
2p
365
y9(t) is greatest when }}(x 2 101) 5 0, or
x 5 101. The temperature is increasing the fastest on
day 101 (April 11).
(b) The rate of increase is
74p
365
y9(101) 5 }} < 0.637 degrees per day.
100
Section 3.6
1
d
d
62. Velocity: s9(t) 5 }}Ï1ww
1w4tw 5 }} }}(1 1 4t)
dt
1w4tw dt
2Ï1
ww
4
dT
du
2
5 }} 5 }}
1w4tw
1w4tw
2Ï1
ww
Ï1ww
2
5
d
(Ï1
ww
1w4tw)}}(2) 2 2 }}Ï1
ww
1w
4tw
dt
dt
5 }}}}
(Ïw
1w
1w4wt)2
2
1
d
22 }} }}(1 1 4t)
1w
2Ï1
ww
4tw dt
5 }}}
1 1 4t
24
}}
1w
4tw
Ïw1w
f 9(g(1))g9(1) 5 0, so either g9(1) 5 0 or f 9(g(1)) 5 0. This
4
(1 1 4t)
1 2
means that either the graph of y 5 g(x) has a horizontal
4
125
3
dv
ds
4
d
ds
63. Acceleration 5 }} 5 }} }} 5 }} (v) 5 }}(kÏsw) (kÏsw)
1 2
k
k2
5 }} (kÏsw) 5 }}, a constant.
2
2Ïws
!§
1
L
kT
}} (kL) 5 kp }} 5 }}
g
g
2
y 5 f(g(x)) has a horizontal tangent at x 5 1, then
4
[1 1 4(6)]
dv ds
ds dt
L
}}
g
d
dx
2
At t 5 6, the acceleration is 2}}
3/2 5 2}} m/sec
dv
dt
p
}
2
d L
}} }} (kL)
dL g
68. Yes. Note that }} f(g(x)) 5 f 9(g(x))g9(x). If the graph of
5 } 5 2}}
3/2
1 1 4t
1
}
L
2 }}
67. No, this does not contradict the Chain Rule. The Chain
Rule states that if two functions are differentiable at the
appropriate points, then their composite must also be
differentiable. It does not say: If a composite is
differentiable, then the functions which make up the
composite must all be differentiable.
2
Acceleration: s0(t)5 }} }}
dt Ï1
1w4tw
ww
1
1 !§ 21
1 !§ 21 2
g
2
d
L
d
5 2p
At t 5 6, the velocity is }} 5 }} m/sec
4(6
Ï1ww
1w
w)w 5
d
1 dL !§g 2
dT dL
dL du
66. }} 5 }} }} 5 }} 2p }} (kL)
tangent at x 5 1, or the graph of y 5 f(u) has a horizontal
tangent at u 5 g(1).
69. For h 5 1:
64. Note that this Exercise concerns itself with the slowing
down caused by the earth’s atmosphere, not the acceleration
[22, 3.5] by [23, 3]
caused by gravity.
For h 5 0.5:
k
Given: v 5 }}
Ïws
dv
dt
dv ds
ds dt
1 ds 2
1 ds 2
dv
dv
Acceleration 5 }} 5 }} }} 5 }} (v) 5 (v) }}
1 2
k
d
k
5 }} }} }}
Ïws ds Ïws
[22, 3.5] by [23, 3]
Ïsw}d}(k) 2 k }d}Ïsw
1 21}}
2
(Ïsw)
k
5 }}
Ïws
2
1 2
k
5 }}
Ïws
1 2
2k
}}
(2Ïws)
}
s
k2
5 2}}, s $ 0
2s 2
Thus, the acceleration is inversely proportional to s 2.
dv
dt
For h 5 0.2:
ds
ds
df (x)
dt
df (x) dx
dx dt
65. Acceleration 5 }} 5 }} 5 }} }} 5 f 9(x) f(x)
[22, 3.5] by [23, 3]
As h → 0, the second curve (the difference quotient)
approaches the first (y 5 2 cos 2x). This is because
2 cos 2x is the derivative of sin 2x, and the second curve is
the difference quotient used to define the derivative of
sin 2x. As h → 0, the difference quotient expression should
be approaching the derivative.
Section 3.7
70. For h 5 1:
dG
dx
d
dx
d
dx
101
d
dx
72. }} 5 }} Ïuwvw 5 }} Ïx(
wxw1
wwc)w 5 }} Ïw
x 2w
1wcxw
1
2x 1 c
d
x 1 (x 1 c)
5 }} }} (x 2 1 cx) 5 }} 5 }}
1wcxw dx
1wcxw
x(w
xw
1wcw)
2Ïw
x2w
2Ïxw2w
2Ïw
u1v
A
5 }} 5 }}
G
2Ïwuwv
[22, 3] by [25, 5]
For h 5 0.7:
■ Section 3.7 Implicit Differentiation
(pp. 149–157)
Exploration 1
An Unexpected Derivative
1. 2x 2 2y 2 2xy9 1 2yy9 5 0. Solving for y9, we find that
dy
}} 5 1 (provided y Þ x).
dx
[22, 3] by [25, 5]
For h 5 0.3:
2. With a constant derivative of 1, the graph would seem to be
a line with slope 1.
3. Letting x 5 0 in the original equation, we find that
y 5 62. This would seem to indicate that this equation
defines two lines implicitly, both with slope 1. The two
lines are y 5 x 1 2 and y 5 x 2 2.
[22, 3] by [25, 5]
As h → 0, the second curve (the difference quotient)
approaches the first (y 5 22x sin (x 2)). This is because
22x sin (x 2) is the derivative of cos (x 2), and the second
curve is the difference quotient used to define the derivative
of cos (x 2). As h → 0, the difference quotient expression
should be approaching the derivative.
4. Factoring the original equation, we have
[(x 2 y) 2 2][(x 2 y) 1 2] 5 0
[ x 2 y 2 2 5 0 or x 2 y 1 2 5 0
[ y 5 x 2 2 or y 5 x 1 2.
The graph is shown below.
71. (a) Let f(x) 5 )x).
Then
1
21 2
du
du
d
d
d
u
}})u) 5 }} f(u) 5 f 9(u) }} 5 }} )u) }} 5 }} u9.
dx
dx
dx
dx
du
)u)
The derivative of the absolute value function is 11 for
positive values, 21 for negative values, and undefined
at 0. So f 9(u) 5
h
21,
1,
u,0
u . 0.
u
)u)
3 dx
d
} 5 }}
4?}
)x 2 9)
)x 2 9)
x2 2 9
dy
dx
5. At each point (x, y) on either line, }} 5 1. The condition
y Þ x is true because both lines are parallel to the line
y 5 x. The derivative is surprising because it does not
depend on x or y, but there are no inconsistencies.
Quick Review 3.7
But this is exactly how the expression }} evaluates.
(b) f 9(x) 5 }} (x 2 2 9)
[24.7, 4.7] by [23.1, 3.1]
(2x)(x 2 2 9)
2
2
1. x 2 y 2
x
6Ïwx
y1
50
5 y2
5y
5 Ïxw, y25 2Ïxw
d
dx
g9(x) 5 }}()x) sin x)
d
dx
d
dx
5 )x) }}(sin x) 1 (sin x) }} )x)
x sin x
)x)
5 )x) cos x 1 }}
[26, 6] by [24, 4]
Note: The expression for g9(x) above is undefined at
x 5 0, but actually
g(0 1 h) 2 g(0)
h
)h) sin h
h
g9(0) 5 lim }} 5 lim }} 5 0.
h→0
h→0
Therefore, we may express the derivative as
g9(x) 5
h
)x) cos x 1 }},
xÞ0
0,
x 5 0.
x sin x
)x)
102
Section 3.7
7. y9 sin x 2 x cos x 5 xy9 1 y
2. 4x2 1 9y 2 5 36
y9 sin x 2 xy9 5 y 1 x cos x
9y 2 5 36 2 4x 2
36 2 4x
4
9
9
2
y 5 6}}Ï9ww
2wx2w
3
2
2
y1 5 }}Ï9ww
2wx2w, y2 5 2}}Ï9ww
2wx2w
3
3
2
(sin x 2 x)y9 5 y 1 x cos x
y 2 5 }} 5 }}(9 2 x 2)
y 1 x cos x
y9 5 }}
sin x 2 x
8. x(y 2 2 y9) 5 y9(x 2 2 y)
xy 2 5 y9(x 2 2 y 1 x)
xy2
y9 5 }
}
2
x 2y1x
3
9. Ïxw(x 2 Ïxw) 5 x 1/2(x 2 x 1/3)
5 x 1/2x 2 x 1/2x 1/3
5 x 3/2 2 x 5/6
[24.7, 4.7] by [23.1, 3.1]
x 2 2 4y 2 5 0
3.
3
(x 1 2y)(x 2 2y) 5 0
x
2
y 5 6 }}
x
2
x
2
y1 5 }}, y2 5 2}}
x + Ïw
x2
x 1 x 2/3
10. }} 5 }3/}
x 2
Ïxw3
x
x 2/3
5 }3}
/2
/2 1 }3}
x
x
5x
21/2
1 x 25/6
Section 3.7 Exercises
dy
d
dx
9
4
9
4
1. }} 5 }}x 9/4 5 }}x (9/4)21 5 }}x 5/4
dx
dy
[26, 6] by [24, 4]
4. x 1 y
y2
y
y1
2
2
59
5 9 2 x2
5 6Ïw9w
2wx2w
5 Ïw9w
2wx2w, y2 5 2Ï9ww
2wy2w
3
5
d
dx
3
5
2. }} 5 }}x 23/5 5 2}}x (23/5) 2 1 5 2}}x 28/5
dx
dy
d 3
dx
d
dx
1
3
1
3
d 4
dx
d
dx
1
4
1
4
3. }} 5 }}Ïxw 5 }}x 1/3 5 }}x (1/3) 2 1 5 }}x 22/3
dx
dy
4. }} 5 }}Ïxw 5 }}x 1/4 5 }}x (1/4) 2 1 5 }}x 23/4
dx
dy
1
d
2
dx
1
5 2}}(2x 1 5)23/2(2) 5 2(2x 1 5)23/2
2
d
dx
5. }} 5 }}(2x 1 5)21/2 5 2}}(2x 1 5)(21/2) 2 1}}(2x 1 5)
dx
[24.7, 4.7] by [23.1, 3.1]
5. x 1 y
y2
y
y1
2
2
5 2x 1 3
5 2x 1 3 2 x 2
5 6Ïw2w
xw
1w
3w
2wx2w
5 Ïw2w
xw
1w
3w
2wx2w, y2 5 2Ï2wxw1
ww3w
2wx2w
dy
d
dx
2
d
5 }}(1 2 6x)(2/3)21}}(1 2 6x)
3
dx
2
5 }}(1 2 6x)21/3(26)
3
6. }} 5 }}(1 2 6x)2/3
dx
5 24(1 2 6x)21/3
dy
d
dx
d
d
5 x}}Ïw
x 2w
1w
1 1 Ïw
x 2w
1w1 }}(x)
dx
dx
d
5 x}}(x 2 1 1)1/2 1 (x 2 1 1)1/2
dx
1
5 x ? }}(x 2 1 1)21/2(2x) 1 (x 2 1 1)1/2
2
7. }} 5 }}(xÏw
x 2w
1w
1)
dx
[24.7, 4.7] by [23.1, 3.1]
6. x 2y9 2 2xy 5 4x 2 y
x 2y9 5 4x 2 y 1 2xy
4x 2 y 1 2xy
y9 5 }}
2
x
5 x 2(x 2 1 1)21/2 1 (x 2 1 1)1/2
2x 2 1 1
Note: This answer is equivalent to }}.
x 2w
1w
1
Ïw
Section 3.7
d
d
(x 2 1 1)1/2}}x 2 x}}(x 2 1 1)1/2
dy
x
d
dx
dx
8. }} 5 }} }} 5 }}}}
x2 1 1
dx
dx Ïw
1w1
x 2w
x2y
x 2 5 }}
12.
x1y
d 2
d x2y
}}(x ) 5 }} }}
dx
dx x 1 y
1
1
(x 2 1 1)1/2 2 x ? }}(x 2 1 1)21/2(2x)
dy
2
1
(x 1 y)
x2 1 1 2 x2
(x 1 1)(x 1 1)
5 }}
2
2
1/2
3x 2 x}d}x 1 y 2 y}d}x 4 2 3x 1 x}d}x 2 y 2 y}d}x 4
dy
dy
dy
23/2
x 2y 1 xy 2 5 6
9.
d
d
}}(x 2y) 1 }}(xy 2)
dx
dx
dy
dy
x 2}} 1 y(2x) 1 x(2y)}} 1 y 2(1)
dx
dx
dy
2 dy
x }} 1 2xy}}
dx
dx
dy
(2xy 1 x 2)}}
dx
dy
}}
dx
d
d
}}(x 3) 1 }}(y 3)
dx
dx
dy
3x 2 1 3y 2}}
dx
dy
2 dy
3y }} 2 18x}}
dx
dx
dy
(3y 2 2 18x)}}
dx
dy
}}
dx
dy
}}
dx
11.
d
dx
5 }}(6)
50
5 2(2xy 1 y 2)
2y 2 2x}}
dx
2x 5 }}
(x 1 y)2
dy
x(x 1 y)2 5 y 2 x}}
dx
dy
x}} 5 y 2 x(x 1 y)2
dx
dy
y
y 2 x(x 1 y)2
}} 5 }} 5 }} 2 (x 1 y)2
dx
x
x
Alternate solution:
x2y
x 2 5 }}
5 2(2xy 1 y 2)
x1y
2xy 1 y 2
5 2}}2
2xy 1 x
x 2(x 1 y) 5 x 2 y
x 3 1 x 2y 5 x 2 y
x 3 1 y 3 5 18xy
10.
y2
d
}}y 2
dx
dy
2y}}
dx
dy
2y}}
dx
dy
}}
dx
dy
dy
2x 5 }}}}}
(x 1 y)2
1
(x 1 1)
5}
2 }
3/2
5 (x 1 1)
2
dx
dx
2x 5 }}}}
2
x 11
2
dy
(x 1 y) 1 2 }} 2 (x 2 y) 1 1 }}
2
5 }}}}
2
d
dx
5 }}(18xy)
dy
5 18x }} 1 18y (1)
dx
d
d
d
d
}}(x 3) 1 }}(x 2y) 5 }}(x) 2 }}(y)
dx
dx
dx
dx
dy
dx
dx
dy
(x 1 1)}} 5 1 2 3x 2 2 2xy
dx
dy
1 2 3x 2 2 2xy
}} 5 }
}
dx
x2 1 1
2
5 18y 2 3x 2
5 18y 2 3x 2
18y 2 3x 2
5}
2 }
3y 2 18x
6y 2 x 2
5}
}
y 2 2 6x
x21
5 }}
x11
d x21
5 }} }}
dx x 1 1
(x 1 1)(1) 2 (x 2 1)(1)
5 }}}
(x 1 1)2
2
5 }}2
(x 1 1)
1
5 }}2
y(x 1 1)
dy
3x 2 1 x 2}} 1 y(2x) 5 1 2 }}
dy
d
dx
1
d
5 }}(1 2 x 1/2)21/2}}(1 2 x 1/2)
2
dx
1
1
5 }}(1 2 x 1/2)21/2 2}}x 21/2
2
2
1
5 2}}(1 2 x 1/2)21/2x 21/2
4
13. }} 5 }} (1 2 x 1/2)1/2
dx
1
dy
dx
2
d
dx
14. }} 5 }}3(2x21/2 1 1)21/3
d
dx
5 2(2x21/2 1 1)24/3 }}(2x21/2 1 1)
5 2(2x21/2 1 1)24/3(2x23/2)
5 x23/2(2x21/2 1 1)24/3
dy
dx
d
dx
9
d
5 }}(csc x)1/2}}(csc x)
2
dx
9
5 }}(csc x)1/2(2csc x cot x)
2
9
5 2}}(csc x)3/2 cot x
2
15. }} 5 }}3(csc x)3/2
103
104
Section 3.7
dy
dx
(c) Differentiating both sides of the given equation
d
dx
5
d
5 }}[sin (x 1 5)]1/4}} sin (x 1 5)
4
dx
5
5 }}[sin (x 1 5)]1/4 cos (x 1 5)
4
16. }} 5 }}[sin (x 1 5)]5/4
17.
1
3
that f -(x) 5 2}}x 24/3.
3
2
(d) If f 9(x) 5 }}x 2/3 1 6, then f 0(x) 5 x 21/3, which matches
x 5 tan y
the given equation.
d
d
}}(x) 5 }}(tan y)
dx
dx
dy
1 5 sec2 y }}
dx
dy
1
5
5 cos2 y
}}
}}
dx
sec2 y
18.
1
3
f 0(x) 5 x 21/3 gives f -(x) 5 2}}x 24/3, so it must be true
Conclusion: (b), (c), and (d) could be true.
4
22. (a) If g9(t) 5 4Ïtw 2 4, then
x 5 sin y
t
given equation.
d
d
}}(x) 5 }}(sin y)
dx
dx
dy
1 5 cos y }}
dx
dy
1
}} 5 }} 5 sec y
dx
cos y
(b) Differentiating both sides of the given equation
1
3
4
23/4
g0(t) 5 }3}
gives g-(t) 5 2}}t 27/4, which is not
/4 5 t
t
4
consistent with g-(t) 5 2}4}.
Ïtw
x 1 tan xy 5 0
19.
16
5
1
g0(t) 5 t 23/4 5 }3}
, which matches the given
t /4
(c) If g(t) 5 t 2 7 1 }}t 5/4, then g9(t) 5 1 1 4t 1/4 and
d
d
}}(x) 1 }}(tan xy) 5 0
dx
dx
d
1 1 sec2 (xy)}}(xy) 5 0
dx
dy
1 1 (sec2 xy)[x}} 1 (y)(1)] 5 0
dx
equation.
1
4
contradicts the given equation.
Conclusion: (a) and (c) could be true.
23.
x 1 sin y 5 xy
d
d
d
}}(x) 1 }}(sin y) 5 }}(xy)
dx
dx
dx
dy
dy
1 1 (cos y)}} 5 x}} 1 (y)(1)
dx
dx
dy
dx
21 1 y
dy
12y
}} 5 }} 5 }}
dx
cos y 2 x
x 2 cos y
(cos y 2 x)}} 5 21 1 y
1
16
(d) If g9(t) 5 }}t 1/4, then g0(t) 5 }}t 23/4, which
dy
dx
21 2 y sec2 xy
dy
}} 5 }}
x sec2 xy
dx
dy
1
y
}} 5 2}} cos2 xy 2 }}
dx
x
x
(sec2 xy)(x)}} 5 21 2 (sec2 xy)(y)
20.
1
d
dx
g0(t) 5 }}(4t 1/4 2 4) 5 t 23/4 5 }3}
/4 , which matches the
x2 1 y2 5 1
d
d
d
}}(x 2) 1 }}(y 2) 5 }}(1)
dx
dx
dx
2x 1 2yy9 5 0
2yy9 5 22x
x
y
y9 5 2}}
d
dx
1 y2
x
y0 5 }} 2}}
(y)(1) 2 (x)(y9)
y
5 2}}
2
3
2
21. (a) If f (x) 5 }}x 2/3 2 3, then
1
3
f 9(x) 5 x21/3 and f 0(x) 5 2}}x24/3
which contradicts the given equation f 0(x) 5 x21/3.
9
10
(b) If f (x) 5 }}x 5/3 2 7, then
3
2
f 9(x) 5 }}x 2/3 and f 0(x) 5 x 21/3,
which matches the given equation.
1 y2
x
y 2 x 2}}
5 2}}
2
y
x2 1 y2
5 2}}
y3
Since our original equation was x 2 1 y 2 5 1, we may
1
y
substitute 1 for x 2 1 y 2, giving y0 5 2}}3 .
Section 3.7
x2/3 1 y2/3 5 1
24.
d
d
d
d
}}(x 2) 1 }}(xy) 2 }}(y 2) 5 }}(1)
dx
dx
dx
dx
dy
dy
2x 1 x}} 1 (y)(1) 2 2y}} 5 0
dx
dx
dy
(x 2 2y)}} 5 22x 2 y
dx
dy
22x 2 y
2x 1 y
}} 5 }} 5 }}
dx
x 2 2y
2y 2 x
2(2) 1 3
7
Slope at (2, 3): }} 5 }}
2(3) 2 2
4
d
d
d
}}(x2/3) 1 }}(y2/3) 5 }}(1)
dx
dx
dx
2
2
}}x21/3 1 }}y21/3y9 5 0
3
3
x 2 1 /3
y
y 1/3
1x2
y
d
y0 5 }}321}}2 4
x
dx
y9 5 2}2}
1/3 5 2 }}
1/3
7
4
12
1 y
5 2}}1}}2
3 x
12
4
7
}}
x2
y 1/3
12
28.
2/3 1/3
1 x y 1y
3 x y
x 2/3 1 y 2/3
5}
1/3
4/3}
y
Since our original equation was x 2/3 1 y 2/3 5 1, we may
substitute 1 for x
1y
3
4
25
4
4
3
4
3
x 2y 2 5 9
29.
d
d
}}(x 2y 2) 5 }}(9)
dx
dx
2yy9 5 2x 1 2
dy
dx
(x 2)(2y)}} 1 (y 2)(2x) 5 0
2x 1 2
x11
2y
y
d x11
y0 5 }} }}
dx y
(y)(1) 2 (x 1 1)y9
5 }}
y2
y9 5 }} 5 }}
1
x11
dy
dx
dy
2xy 2
y
5 2}}
}} 5 2}}
dx
2x 2y
x
3
Slope at (21, 3): 2}} 5 3
21
2x 2y}} 5 22xy 2
2
y 2 (x 1 1) }}
y
5 }}
y2
y 2 2 (x 1 1)2
5 }}
y3
(a) Tangent: y 5 3(x 1 1) 1 3 or y 5 3x 1 6
1
3
Since our original equation was y 5 x 1 2x, we may
write y 2 2 (x 1 1)2 5 (x 2 1 2x) 2 (x 2 1 2x 1 1) 5 21,
1
which gives y0 5 2}}3 .
y
26. y 1 2y 5 2x 1 1
2
d
d
}}(y 2 1 2y) 5 }}(2x 1 1)
dx
dx
(2y 1 2)y9 5 2
1
y11
d 1
y0 5 }} }}
dx y 1 1
y9 5 }}
1
3
2
30.
y 2 2 2x 2 4y 2 1 5 0
d
d
d
d
}}(y 2) 2 }}(2x) 2 }}(4y) 2 }}(1)
dx
dx
dx
dx
dy
dy
2y}} 2 2 2 4}} 2 0
dx
dx
dy
(2y 2 4)}}
dx
dy
}}
dx
1
Slope at (22, 1): }} 5 21
122
d
dx
5 }}(0)
50
52
1
y22
5 }}
(a) Tangent: y 5 2(x 1 2) 1 1 or y 5 2x 2 1
(b) Normal: y 5 1(x 1 2) 1 1 or y 5 x 1 3
22
y9
1
1y 1 12
5 2(y 1 1)22 }}
5 2}}3
8
3
(b) Normal: y 5 2}}(x 1 1) 1 3 or y 5 2}}x 1 }}
2
1
(y 1 1)
3
4
x 2 1 y 2 5 25
(b) Normal: y 5 2}}(x 2 3) 1 (24) or y 5 2}}x
d
d
d
}}(y 2) 5 }}(x 2) 1 }}(2x)
dy
dy
dy
5 2(y 1 1)
29
7
(a) Tangent: y 5 }}(x 2 3) 1 (24) or y 5 }}x 2 }}
1
, giving y0 5 }
}.
3x4/3y1/3
2/3
y 2 5 x 2 1 2x
25.
4
7
d
d
d
}}(x 2) 1 }}(y 2) 5 }}(25)
dx
dx
dx
dy
2x 1 2y}} 5 0
dx
dy
x
}} 5 2}}
dx
y
3
3
Slope at (3, 24): 2}} 5 }}
4
24
5 }} }
4/3}
2/3
3x
1
2
(b) Normal: y 5 2}}(x 2 2) 1 3 or y 5 2}}x 1 }}
22/3 xy9 2 (y)(1)
2(x) }}
2y
x
1
5 2}} }}
4/3 2/3
x y
3
7
4
(a) Tangent: y 5 }}(x 2 2) 1 3 or y 5 }}x 2 }}
1 y 22/3 d y
}} }}
3 x
dx x
5 2}} }}
2/3
x 2 1 xy 2 y 2 5 1
27.
105
106
Section 3.7
6x 2 1 3xy 1 2y 2 1 17y 2 6 5 0
31.
34. x sin 2y 5 y cos 2x
d
d
d
d
d
d
}}(6x 2) 1 }}(3xy) 1 }}(2y 2) 1 }}(17y) 2 }}(6) 5 }}(0)
dx
dx
dx
dx
dx
dx
dy
dy
dy
12x 1 3x}} 1 (3y)(1) 1 4y}} 1 17}} 2 0 5 0
dx
dx
dx
dy
dy
dy
3x}} 1 4y}} 1 17}} 5 212x 2 3y
dx
dx
dx
dy
(3x 1 4y 1 17)}} 5 212x 2 3y
dx
dy
212x 2 3y
}} 5 }}
dx
3x 1 4y 1 17
212(21) 2 3(0)
3(21) 1 4(0) 1 17
12
14
6
7
6
7
6
7
6
7
d
d
}}(x sin 2y) 5 }}(y cos 2x)
dx
dx
dy
dx
(x)(cos 2y)(2)}} 1 (sin 2y)(1) 5
1 dx 2
dy
(y)(2sin 2x)(2) 1 (cos 2x) }}
dy
dx
Slope at (21, 0): }} 5 }} 5 }}
p
7
6
1
d
dx
5 }}(5)
1
2
50
5 yÏ3w 2 2x
d
dx
2(p/2)
2(1) 1 p cos(p/2)
dy
dx
1
2
5 2 cos (px 2 y) p 2 }}
5 2p cos (px 2 y)
2p cos (px 2 y)
1 1 2 cos (px 2 y)
5 }}
2p(21)
1 1 2(21)
1
2p
p
2
2
p
x
2p
1
2p
36. x 2 cos2 y 2 sin y 5 0
p
2
p
2
p
2
d
dx
(b) Normal: y 5 2}}(x 2 1) 1 0 or y 5 2}} 1 }}
(a) Tangent: y 5 2}}(x 2 1) 1 }} or y 5 2}}x 1 p
2
p
5p
8
(a) Tangent: y 5 2p(x 2 1) 1 0 or y 5 2px 2 2p
Slope at 1, }} : 2}} 5 2}}
p
2
1
2
5 }} 2 sin (px 2 y)
2p cos p
1 1 2 cos p
dy
dx
dy
(2x 1 p cos y)}} 5 22y
dx
dy
2y
}} 5 2}}
dx
2x 1 p cos y
2
p
2
Slope at (1, 0): }} 5 }} 5 2p
2x}} 1 2y(1) 1 p cos y }} 5 0
p
2
2
y 5 2 sin (px 2 y)
dy
}}
dx
dy
}}
dx
dy
[1 1 2 cos (px 2 y)]}}
dx
dy
}}
dx
2}}(xy) 1 p}}(sin y) 5 }}(2p)
1
p
4
1
35.
w 2 2x
yÏ3
5 }}
2xÏw
3 1 4y
2xy 1 p sin y 5 2p
dy
dx
p
2
2
(b) Normal: y 5 2}} x 2 }} 1 }} or y 5 2}}x 1 }}
(b) Normal: x 5 Ï3w
d
dx
p
4
1
(a) Tangent: y 5 2 x 2 }} 1}} or y 5 2x
(a) Tangent: y 5 2
d
dx
122
1}2}2(21) 2 0
w 2 2Ï3w
2Ï3
Slope at (Ïw3, 2): }} 5 0
2Ïw
3Ïw3 1 4(2)
33.
142
(p)(1) 1 0
x 2 2 Ï3wxy 1 2y 2 5 5
d
w}d}(xy) 1 2}d}(y 2)
}}(x 2) 2 Ï3
dx
dx
dx
dy
dy
2x 2 Ï3w(x)}} 2 Ï3w(y)(1) 1 4y}}
dx
dx
dy
(2xÏ3w 1 4y)}}
dx
dy
}}
dx
2
5 2}}
52
p
7
6
(b) Normal: y 5 2}}(x 1 1) 1 0 or y 5 2}}x 2 }}
32.
p
1 2 1 2
2 }} sin }} 1 sin (p)
2
2
p p
Slope at }}, }} : 2}}}
4 2
2 }p} cos (p) 2 cos }p}
(a) Tangent: y 5 }}(x 1 1) 1 0 or y 5 }}x 1 }}
7
6
dy
dx
dy
2y sin 2x 1 sin 2y
}} 5 2 }}
2x cos 2y 2 cos 2x
dx
(2x cos 2y)}} 2 (cos 2x)}} 5 22y sin 2x 2 sin 2y
2
p
p
2
(b) Normal: y 5 }}(x 2 1) 1 }} or y 5 }}x 2 }} 1 }}
d
d
d
}}(x 2 cos2 y) 2 }}(sin y) 5 }}(0)
dx
dx
dx
dy
dy
(x 2)(2 cos y)(2sin y) }} 1 (cos2 y)(2x) 2 (cos y)}} 5 0
dx
dx
dy
2
2
2(2x cos y sin y 1 cos y)}} 5 22x cos y
dx
2x cos2 y
dy
2x cos y
5 }}
}} 5 }}}
cos y 1 2x 2 cos y sin y
dx
1 1 2x2 sin y
1 2
2(0) cos p
1 1 2(0) sin p
Slope at (0, p): }}
50
2
(a) Tangent: y 5 p
(b) Normal: x 5 0
107
Section 3.7
y4 5 y2 2 x 2
37. (a)
d
}}(y4)
dx
dy
4y3}}
dx
dy
3
(4y 2 2y)}}
dx
dy
}}
dx
Ïw3 Ïw3
At }}, }} :
4
2
1
39. (a) (21)3(1)2 5 cos (p) is true since both sides equal 21.
d
dx
d
dx
5 }}(y2) 2 }}x 2
dy
dx
d
d
}}(x 3y 2) 5 }} cos (py)
dx
dx
5 2y}} 2 2x
dy
dx
5 22x
dy
dx
(x 3)(2y)}} 1 (y 2)(3x 2) 5 (2sin py)(p)}}
22x
4y 2 2y
dy
dx
dy
3x 2y 2
}} 5 2}
}
dx
2x 3y 1 p sin py
x
y 2 2y
(2x 3y 1 p sin py)}} 5 23x 2y 2
5}
3 } 5 }}
3
2
3(21)2(1)
2(21) (1) 1 p sin p
3
The slope of the tangent line is }}.
2
Ïw3
}}
4
Ïw3
Ïw3
}} 2 2 }}
2
2
Ïw3
4
}}
}}
4
Ï3w
}} }
Ï3w 3Ïw3
4
}} 2 }} }}
2
4
Ï3w
1 2
5
?
2
3
2
40. (a) When x 5 2, we have y 3 2 2y 5 21, or
1
5 }} 5 21
223
y 3 2 2y 1 1 5 0. Clearly, y 5 1 is one solution, and
we may factor y 3 2 2y + 1 as (y 2 1)(y 2 1 y 2 1). The
Ï3w 1
At }}, }} :
4
23
22
Slope at (21, 1): 2}}}
5 }} 5 }}
3
Slope 5 }}3
1
x 3y 2 5 cos(py)
(b)
2
solutions of y 2 1 y 2 1 = 0 are
Ï3w
}}
4
Slope 5 }}3 5
1
1
}} 2 2 }}
2
2
12
Ïw3
}}
4
}
1
1
}} 2 }}
2
4
21 6 Ï(1
w)w2w
2w4(1
w)(
w2
w1w)w
21 6 Ï5w
y 5 }}} 5 }}. Hence,
Ï3w
4
2(1)
2
21 2 Ï5w
there are three possible y-values: 1, }}, and
2
21 1 Ïw
5
}}.
2
? }4} 5 }1} 5 Ï3w
(b)
(b)
d
d
d
}}(y3) 2 }}(xy) 5 }}(21)
dx
dx
dx
[21.8, 1.8] by [21.2, 1.2]
Parameter interval: 21 # t # 1
3y 2y9 2 xy9 2 (y)(1) 5 0
y2(2 2 x) 5 x 3
38. (a)
d
}}[y2(2 2 x)]
dx
dy
(y2)(21) 1 (2 2 x)(2y)}}
dx
dy
2y(2 2 x)}}
dx
dy
}}
dx
3(1)2 1 (1)2
2(1)(2 2 1)
y 3 2 xy 5 21
(3y 2 2 x)y9 5 y
d
5 }}(x 3)
dx
y
3y 2 x
y
d
y0 5 }} }
}
dx 3y 2 2 x
2
(3y 2 x)(y9) 2 (y)(6y y9 2 1)
5 }}}}
(3y 2 2 x)2
y 2 xy9 2 3y 2 y9
5 }}
(3y 2 2 x)2
y9 5 }
2}
5 3x 2
5 3x 2 1 y2
3x 2 1 y2
2y(2 2 x)
5 }}
4
2
Slope at (1, 1): }} 5 }} 5 2
Tangent: y 5 2(x 2 1) 1 1 or y 5 2x 2 1
1
2
1
2
3
2
Normal: y 5 2}}(x 2 1) 1 1 or y 5 2}}x 1 }}
x3
!§2§2§§x
(b) One way is to graph the equations y 5 6 }}.
Since we are working with numerical information,
there is no need to write a general expression for y0 in
terms of x and y.
To evaluate f 9(2), evaluate the expression for y9 using
x 5 2 and y 5 1:
1
3(1) 2 2
1
1
f 9(2) 5 }2} 5 }} 5 1
To evaluate f 0(2), evaluate the expression for y0 using
x 5 2, y 5 1, and y9 5 1:
(1) 2 2(1) 2 3(1)2(1)
[3(1) 2 2]
24
1
f z0(2) 5 }}}
5 }} 5 24
2
2
108
Section 3.7
41. Find the two points:
The curve crosses the x-axis when y 5 0, so the equation
becomes x 2 1 0x 1 0 5 7, or x 2 5 7. The solutions are
x 5 6Ïw7, so the points are (6Ïw7, 0).
Show tangents are parallel:
2
d
d
d
}}(x 2) 1 }}(xy) 1 }}(y 2)
dx
dx
dx
dy
dy
2x 1 x}} 1 (y)(1) 1 2y}}
dx
dx
dy
(x 1 2y)}}
dx
dy
}}
dx
57
57
57
57
7
5 6 }}
!§
3
7
7
7
}} and 2 }}, 2 }} .
3
3
3
1 !§ !§2
7
The points are 22 }},
3
x 1 xy 1 y 5 7
2
x 2 1 xy 1 y 2
(22y) 1 (22y)(y) 1 y 2
4y 2 2 2y 2 1 y 2
3y 2
y
2
d
5 }}(7)
dx
1 !§ !§2
Note that these are the same points that would be
obtained by interchanging x and y in the solution to
part (a).
50
5 2(2x 1 y)
43. First curve:
2x 1 y
5 2 }}
x 1 2y
2x 2 1 3y 2 5 5
2Ï7w 1 0
Slope at (Ï7w, 0): 2}} 5 22
Ïw7 1 2(0)
2(2Ï7w) 1 0
Slope at (2Ïw7, 0): 2}} 5 22
2 Ï7
w 1 2(0)
The tangents at these points are parallel because they have
the same slope. The common slope is 22.
d
d
d
}}(2x 2) 1 }}(3y 2) 5 }}(5)
dx
dx
dx
dy
4x 1 6y}} 5 0
dx
dy
4x
2x
}} 5 2}} 5 2}}
dx
6y
3y
Second curve:
y2 5 x3
x 2 1 xy 1 y 2 5 7
42.
d
d
}}y 2 5 }}x 3
dx
dx
dy
2y}} 5 3x 2
dx
dy
3x 2
}} 5 }}
dx
2y
d
d
d
d
}}(x 2) 1 }}(xy) 1 }}(y 2) 5 }}(7)
dx
dx
dx
dx
dy
dx
dy
dx
2x 1 x}} 1 (y)(1) 1 2y}} 5 0
2
3
3
2
At (1, 1), the slopes are 2}} and }} respectively. At (1, 21),
dy
(x 1 2y)}} 5 2(2x 1 y)
dx
2
3
3
2
the slopes are }} and 2}} respectively. In both cases, the
dy
2x 1 y
}} 5 2}}
dx
x 1 2y
tangents are perpendicular. To graph the curves and normal
lines, we may use the following parametric equations for
(a) The tangent is parallel to the x-axis when
dy
2x 1 y
}} 5 2}} 5 0, or y 5 22x.
dx
x 1 2y
Substituting 22x for y in the original equation, we have
x 2 1 xy 1 y 2 5 7
2
x 1 (x)(22x) 1 (22x)2 5 7
x 2 2 2x 2 1 4x 2 5 7
3x 2 5 7
7
x 5 6 }}
!§3
7
7
1 !§ !§2 1!}§3}, 22!}§3}2.
2p # t # p:
First curve: x 5
!}§2}3cos t, y 5 !}§3} sin t
5
Second curve: x 5 Ïw
t 2, y 5 t
Tangents at (1, 1):
x 5 1 1 3t, y 5 1 2 2t
x 5 1 1 2t, y 5 1 1 3t
Tangents at (1, 21):
x 5 1 1 3t, y 5 21 1 2t
x 5 1 1 2t, y 5 21 2 3t
7
7
The points are 2 }}, 2 }} and
3
3
(b) Since x and y are interchangeable in the original
dx
dy
equation, }} can be obtained by interchanging x and y
dy
dx
dx
dy
2y 1 x
x 1 2y
in the expression for }}. That is, }} 5 2}}. The
dx
dy
tangent is parallel to the y-axis when }} 5 0, or
x 5 22y. Substituting 22y for x in the original
equation, we have:
5
[22.4, 2.4] by [21.6, 1.6]
Section 3.7
3
2
d
dt
(b) The tangent is horizontal when
44. v(t) 5 s9(t) 5 }}(4 1 6t)3/2 5 }}(4 1 6t)1/2(6)
dy
3y 2 x 2
x2
}} 5 }
2 } 5 0, or y 5 }}.
dx
y 2 3x
3
x2
Substituting }} for y in the original equation, we have:
3
5 9(4 1 6t)1/2
d
dt
a(t) 5 v9(t) 5 }}[9(4 1 6t)1/2]
9
2
5 }}(4 1 6t)21/2(6) 5 27(4 1 6t)21/2
x 3 1 y 3 2 9xy 5 0
At t 5 2, the velocity is v(2) 5 36 m/sec and the
x2 3
132
x6
27
x 3 1 }} 2 3x 3 5 0
d
dt
45. Acceleration 5 }} 5 }}[8(s 2 t)1/2 1 1]
x3
}}(x 3 2 54) 5 0
27
21/2 ds
5 4(s 2 t)
x2
132
x 3 1 }} 2 9x }} 5 0
27
acceleration is a(2) 5 }} m/sec2.
4
dv
dt
109
1}d}t 2 12
3
3
x 5 0 or x 5 Ï5w4w 5 3Ï2w
5 4(s 2 t)21/2(v 2 1)
5 4(s 2 t)21/2[(8(s 2 t)1/2 1 1) 2 1]
At x 5 0, we have y 5 }} 5 0, which gives the
5 32(s 2 t)21/2(s 2 t)1/2
point (0, 0), which is the origin. At x 5 3Ï2w, we have
5 32 ft/sec2
y 5 }}(3Ï2w)2 5 }}(9Ï4w) 5 3Ï4w, so the point other
02
3
1
3
3
1
3
3
3
3
3
3
than the origin is (3Ï2w, 3Ï4w) or approximately
y 4 2 4y 2 5 x 4 2 9x 2
46.
(3.780, 4.762).
d
d
d
d
}}(y 4) 2 }}(4y 2) 5 }}(x 4) 2 }}(9x 2)
dx
dx
dx
dx
dy
dy
4y 3}} 2 8y}} 5 4x 3 2 18x
dx
dx
(c) The equation x 3 1 y 3 2 9xy is not affected by
interchanging x and y, so its graph is symmetric about
the line y 5 x and we may find the desired point by
dy
4x 3 2 18x
2x 3 2 9x
}} 5 }
}
3 }5}
dx
4y 2 8y
2y 3 2 4y
interchanging the x-value and the y-value in the answer
3
approximately (4.762, 3.780).
2(23)3 2 9(23)
27
Slope at (23, 2): }
} 5 2 }}
2(2)3 2 4(2)
8
2(23)3 2 9(23)
2(22) 2 4(22)
27
8
Slope at (23, 22): }
3 } 5 }}
2(3) 2 9(3)
2(22) 2 4(22)
3
27
8
Slope at (3, 22): }
3 } 5 2}}
47. (a)
3
to part (b). The desired point is (3Ï4w, 3Ï2w) or
2(3)3 2 9(3)
27
Slope at (3, 2): }
} 5 }}
2(2)3 2 4(2)
8
x 3 1 y 3 2 9xy 5 0
d
d
d
d
}}(x 3) 1 }}(y 3) 2 9}}(xy) 5 }}(0)
dx
dx
dx
dx
dy
dy
3x 2 1 3y 2}} 2 9x}} 2 9(y)(1) 5 0
dx
dx
dy
(3y 2 2 9x)}} 5 9y 2 3x 2
dx
dy
9y 2 3x 2
3y 2 x 2
}} 5 }
}5}
}
dx
3y 2 2 9x
y 2 2 3x
2
3(2) 2 (4)
210
5
Slope at (4, 2): }
} 5 }} 5 }}
(2)2 2 3(4)
28
4
3(4) 2 (2)2
4
8
Slope at (2, 4): }
} 5 }} 5 }}
(4)2 2 3(2)
5
10
x2 1 2xy 2 3y2 5 0
48.
d
d
d
d
}}(x2) 1 2}}(xy) 2 }}(3y2) 5 }}(0)
dx
dx
dx
dx
dy
dy
2x 1 2x}} 1 2(y)(1) 2 6y}} 5 0
dx
dx
dy
(2x 2 6y)}} 5 22x 2 2y
dx
dy
22x 2 2y
x1y
}} 5 }} 5 }}
dx
2x 2 6y
3y 2 x
111
3(1) 2 1
2
2
At (1, 1) the curve has slope }} 5 }} 5 1, so the
normal line is y 5 21(x 2 1) + 1 or y 5 2x 1 2.
Substituting 2x 1 2 for y in the original equation, we have:
x 2 1 2xy 2 3y 2 5 0
x 1 2x(2x 1 2) 2 3(2x 1 2)2 5 0
x 2 2 2x 2 1 4x 2 3(x 2 2 4x 1 4) 5 0
24x 2 1 16x 2 12 5 0
24(x 2 1)(x 2 3) 5 0
x 5 1 or x 5 3
Since the given point (1, 1) had x 5 1, we choose x 5 3
and so y 5 2(3) 1 2 5 21. The desired point is (3, 21).
2
110
Section 3.7
xy 1 2x 2 y 5 0
49.
d
d
d
}}(xy) 1 }}(2x) 2 }}(y)
dx
dx
dx
dy
dy
x}} 1 (y)(1) 1 2 2 }}
dx
dx
dy
(x 2 1)}}
dx
dy
}}
dx
x2
y2
}}2 1 }}2 5 1
a
b
51. (a)
50
b 2x 2 1 a 2y 2 5 a 2b 2
50
d
d
d
}}(b 2x 2) 1 }}(a 2y 2) 5 }}(a 2b 2)
dx
dx
dx
dy
2b 2x 1 2a 2y}} 5 0
dx
5 22 2 y
22 2 y
x21
21y
12x
5 }} 5 }}
dy
2b 2x
b 2x
}} 5 2}}
2 5 2}2}
dx
2a y
a y
Since the slope of the line 2x 1 y 5 0 is 22, we wish to
b 2x
find points where the normal has slope 22, that is, where
The slope at (x1, y1) is 2}2}1 .
a y1
1
2
the tangent has slope }}. Thus, we have
a y1
21y
1
}} 5 }}
12x
2
a y1y 2 a
2
2(2 1 y) 5 1 2 x
5 2b x1x 1 b x12
2
2
ellipse. Therefore, a 2y1y 1 b 2x1x 5 a 2b 2, and
Substituting 22y 2 3 in the original equation, we have:
xy 1 2x 2 y 5 0
(22y 2 3)y 1 2(22y 2 3) 2 y 5 0
22y 2 2 8y 2 6 5 0
22(y 1 1)(y 1 3) 5 0
y 5 21 or y 5 23
At y 5 21, x 5 22y 2 3 5 2 2 3 5 21.
At y 5 23: x 5 22y 2 3 5 6 2 3 5 3.
The desired points are (21, 21) and (3, 23).
Finally, we find the desired normals to the curve, which are
the lines of slope 22 passing through each of these points.
At (21, 21), the normal line is y 5 22(x 1 1) 2 1 or
y 5 22x 2 3. At (3, 23), the normal line is
y 5 22(x 2 3) 2 3 or y 5 22x 1 3.
xx
yy
a
b
1
dividing by a 2b 2 gives }1}
2 1 }}
2 5 1.
x2
y2
}}2 2 }}2 5 1
a
b
(b)
b 2x 2 2 a 2y 2 5 a 2b 2
d
d
d
}}(b 2x 2) 2 }}(a 2y 2) 5 }}(a 2b 2)
dx
dx
dx
dy
2b 2x 2 2a 2y}} 5 0
dx
dy
22b 2x
b 2x
5 }2}
}} 5 }}
dx
22a 2y
a y
b 2x
The slope at (x1, y1) is }2}1 .
a y1
x 5 y2
b 2x
The tangent line is y 2 y1 5 }2}1 (x 2 x1).
a y1
d
d
}}(x) 5 }}(y 2)
dx
dx
dy
1 5 2y}}
dx
dy
1
}} 5 }}
dx
2y
This gives:
a 2y1y 2 a2y12 5 b2x1x 2 b2x12
b2x12 2 a 2y12 5 b 2x1x 2 a 2y1y
The normal line at (x, y) has slope 22y. Thus, the normal
line at (b 2, b) is y 5 22b(x 2 b2) 1 b, or
y 5 22bx 1 2b 1 b. This line intersects the x-axis at
3
2b3 1 b
1
x 5 }} 5 b 2 1 }}, which is the value of a and must be
2
2b
1
greater than }} if b Þ 0.
2
The two normals at (b 2, 6b) will be perpendicular when
they have slopes 61, which gives 22y 5 61 or
1
1
2
2
2
1
1
1
3
b 2 1 }} 5 }} 1 }} 5 }}. Thus, the two nonhorizontal
2
2
2
4
3
normals are perpendicular when a 5 }}.
4
2
y 5 6}} or b 5 6}} . The corresponding value of a is
12
y12
But a 2y12 1 b 2x12 5 a 2b 2 since (x1, y1) is on the
x 5 22y 2 3
1
2
a 2y1y 1 b 2x1x 5 a 2y12 1 b 2x12.
4 1 2y 5 1 2 x
50.
b 2x
The tangent line is y 2 y1 5 2}2}1 (x 2 x1). This gives:
But b 2x12 2 a 2y12 5 a 2b 2 since (x1, y1) is on the
hyperbola. Therefore, b 2x1x 2 a 2y1y 5 a 2b 2, and
xx
yy
a
b
1
dividing by a 2b 2 gives }1}
2 2 }}
2 5 1.
52. (a) Solve for y:
x2
y2
}}2 2 }}2 5 1
a
b
y2
x2
2}}2 5 2}}2 1 1
b
a
b2
y 2 5 }}2 (x 2 2 a 2)
a
b
y 5 6}}Ïw
x 2w
2w
a 2w
a
Section 3.8
b
2
2w
a 2w
}}Ïxww
f (x)
a
(b) lim }} 5 lim }}
b
x→` g(x)
}})x)
a
x→`
Ïxw2w
2w
a 2w
5 lim }}
x→`
Ïxw2
5 lim
x→`
!1§§2§}x}§ 5 1
a2
2
2}b}Ïw
x 2w
2w
a 2w
f (x)
a
(c) lim }} 5 lim }}
b
x→` g(x)
x→`
2}})x)
a
Ïxw2w
2w
a 2w
5 lim }}
2
x→`
Ïxw
5 lim
x→`
!1§§2§}x}§ 5 1
a2
2
■ Section 3.8 Derivatives of Inverse
Trigonometric Functions (pp. 157–163)
Exploration 1 Finding a Derivative on an
Inverse Graph Geometrically
1. The graph is shown at the right. It appears to be a one-toone function
6. The reflection of line L is the tangent line to the graph of
dy
dx
y 5 x 5 1 2x 2 1 at the point (1, 2). The slope is }} at
x 5 1, which is 7.
7. The slope of L is the reciprocal of the slope of its reflection
1since }D}x gets reflected to become }D}y 2. It is }7}.
Dy
Dx
1
7
8. }}
Quick Review 3.8
1. Domain: [21, 1]
3
p p
2 2
4
Range: 2}}, }}
p
At 1: }}
2
2. Domain: [21, 1]
Range: [0, p]
At 1: 0
3. Domain: all reals
1
p p
2 2
2
Range: 2}}, }}
p
At 1: }}
4
[24.7, 4.7] by [23.1, 3.1]
2. f 9(x) 5 5x 1 2. The fact that this function is always
positive enables us to conclude that f is everywhere
increasing, and hence one-to-one.
4
4. Domain: (2`, 21] < [1, `)
3 22 12 4
p
p
Range: 0, }} < }}, p
At 1: 0
21
3. The graph of f is shown to the right, along with the
graph of f. The graph of f 21 is obtained from the graph of f
by reflecting it in the line y 5 x.
5. Domain: all reals
Range: all reals
At 1: 1
6. f(x) 5 y 5 3x 2 8
y 1 8 5 3x
[24.7, 4.7] by [23.1, 3.1]
4. The line L is tangent to the graph of f 21 at the point (2, 1).
y18
3
x 5 }}
Interchange x and y:
x18
3
x18
f 21(x) 5 }}
3
y 5 }}
3
7. f(x) 5 y 5 Ïxw1
ww5
[24.7, 4.7] by [23.1, 3.1]
5. The reflection of line L is tangent to the graph of f at the
point (1, 2).
y3 5 x 1 5
x 5 y3 2 5
Interchange x and y:
y 5 x3 2 5
f 21(x) 5 x 3 2 5
[24.7, 4.7] by [23.1, 3.1]
111
1
112
Section 3.8
8
x
8
x 5 }}
y
dy
ds
d
ds
5. }} 5 }} sec 21 (2s 1 1)
8. f(x) 5 y 5 }}
1
d
d
)2s 1 1) Ï(2
wsw1
ww1w
)w
2w1 s
5 }}} }} (2s 1 1)
2
Interchange x and y:
1
8
x
8
f 2 1(x) 5 }}
x
y 5 }}
1
5 }}} (2) 5 }}
)2s 1 1) Ï4
ww
s w
1w4sw
)2s 1 1) Ïw
s 2w
1ws
2
dy
ds
d
ds
dy
dx
d
dx
1
1
d
)5s) Ï(5
ws)
w2w2
ww1 ds
6. }} 5 }} sec 21 5s 5 }} }} (5s) 5 }}
3x 2 2
x
9. f(x) 5 y 5 }}
)s) Ï2
w5ww
s 2w
2w1
7. }} 5 }} csc 21 (x 2 1 1)
xy 5 3x 2 2
(y 2 3)x 5 22
1
d
5 2}}} }} (x 2 1 1)
)x2 1 1)Ï(x
w2w1
ww1)w2w
2w1 dx
22
2
x 5 }} 5 }}
y23
32y
2x
2
5 2}}} 5 2}}
(x 1 1)Ïw
x w
1w2w
x
2
Interchange x and y:
2
32x
2
f 2 1(x) 5 }}
32x
y 5 }}
4
(x 1 1)Ïw
x 2w
1w
2
2
2
Note that the condition x . 0 is required in the last step.
1
12
dy
d
x
d x
8. }} 5 }} csc 21 }} 5 2}}
}} }}
x
x 2
dx
dx
2
x
10. f(x) 5 y 5 arctan }}
3
p
p
x
tan y 5 }}, 2}} , y , }}
2
2
3
p
p
x 5 3 tan y, 2}} , y , }}
2
2
)}2})
2
!§1}§2}§2 §2§1 dx 1 2 2
5 2}}
)x) Ïw
x 2w
2w4
Interchange x and y:
p
2
p
2
dy
dt
f
21
1t2
p
p
(x) 5 3 tan x, 2}} , x , }}
2
2
1
1
1
1 t2
12
d 1
dt t
1
1
) ) !§1 §§2 §§
1 2
}} 2 1
t
1
}}
t
dy
1
d
d
1. }} 5 }} cos 21 (x 2) 5 2}} }}(x 2)
2 2 dx
dx
dx
Ï1ww
2(x
ww)w
Ï1ww
2wt 2w
Note that the condition t . 0 is required in the last step.
2x
5 2}} (2x) 5 2}}
2wxw
Ï1ww
2wx 4w
Ï1ww
4
12
dy
dt
1
!§§1§§x 2§
12
1 x2
1
1
5 2}} 2}}2 5 }}
!§§§1§§2
1
1 2 }}
x
2
)x) Ïw
x 2w
2w1
1
dy
d
d
Ï2w
3. }} 5 }} sin 21 Ï2w t 5 }} }} (Ï2w t) 5 }}
dt
dt
2 dt
Ï1ww
2w
2w
t2
Ï1ww
2w
(Ï2
wwtw
)
1
d
dt
d
2 dt
Ï1ww
2(1
ww
2wt)w
4. }} 5 }} sin 21 (1 2 t) 5 }} }} (1 2 t)
1
5 2}}
Ï2wtw2
wwt 2w
1t 2
d
dt
1
3
d
1t 2
3
10. }} 5 }} sin 21 }}2 5 }} }} }}2
1
dy
1
d
d 1
2. }} 5 }} cos 21 }} 5 2}} }} }}
dx
x
dx
1 2 dx x
1 2 }}
dy
dt
)}t}) !§1}§t}§2 §2§1
2
5 }} 2}}2 5 2}
Section 3.8 Exercises
1
1
1
d
dt
9. }} 5 }} sec 21 }} 5 }} }} }}
y 5 3 tan x, 2}} , x , }}
3 2 dt
1 2 }}2
t
!§§1§§2§
1 t2
6
1
6
5 } 2}}3 5 2}}
!1§§2§}t9}§
tÏw
t 4w
2w9
4
dy
d
1
d
11. }} 5 }} cot 21 Ïtw 5 2}}
}} Ïtw
dt
dt
1 1 (Ïtw)2 dt
1
5 2}}
2Ïtw (t 1 1)
dy
1
d
d
12. }} 5 }} cot 21 Ïtw2
ww15 2}} }} Ïtw2
ww1
dt
dt
t2
1 1 (Ïw
ww1)2 dt
1
1
2(
1
)
1
5 2 }} } 5 2}}
1 1 t 2 1 2Ïtw2
2tÏtw2
ww1
ww1
Section 3.8
dy
ds
d
ds
dy
dx
d
ds
13. }} 5 }} (sÏ1ww
2ws2w) 1 }}(cos 21s)
1 2Ï1ww2wsw 2
1
d
dx
5 2[sin 21(2x)]22 }} sin 21 (2x)
1
Ï1ww
2ws2w
2
1
5 2[sin 21 (2x)]22 }}2 (2)
s2
1
5 2} 1 Ï1ww
2ws2w 2 }
2
Ïw1w
2wsw
Ï1ww
2ws2w
Ï1ww
2w4w
x
2
5 2}}}
[sin 21 (2x)]2Ï1
ww
2w4xw2
2s 2 1 (1 2 s 2) 2 1
5 }}}
Ïw1w
2ws2w
14 2
142
p
The tangent line is given by y 5 2 x 2 }} 1 1, or
1 42
Ï1ww
2ws2w
p
2
1
1
2Ïw
s 2w
2w1
)s) Ïw
s 2w
2w
1
dy
dx
s)s) 2 1
5 }}
)s)Ïw
s 2w
2w1
(b) Since the graph of y 5 f(x) includes the point (1, 3) and
1
5 }} }} (Ïw
x 2w
2w1) 2 }}
)x)Ïw
x w
2w
1
2
the slope of the graph is 12 at this point, the graph of
1
1
1
5 }} }} (2x) 2 }}
2
2
x 2 2Ïw
)x)
Ï
x
w
w
2w
1
x w
2w1
y 5 f 21(x) will include (3, 1) and the slope will be
1
1
5 }} 2 }}
xÏw
x 2w
2w1
)x)Ïw
x 2w
2w1
assumed that f 21(x) is defined and differentiable at
50
x 5 3. This is true by Theorem 3, because
1
1
}}. Thus, f 21(3) 5 1 and (f 21)9(3) 5 }}. (We have
12
12
f 9(x) 5 5x 4 1 6x 2 1 1, which is never zero.)
Note that the condition x . 1 is required in the last step.
d
dx
1
1
x
2
21. (a) Note that f 9(x) 5 2sin x 1 3, which is always between
2 and 4. Thus f is differentiable at every point on the
interval(2`, `) and f 9(x) is never zero on this interval,
so f has a differentiable inverse by Theorem 3.
d
dx
16. }} 5 }} cot 21 }} 2 }}(tan 21 x)
12
d 1
dx x
(b) f (0) 5 cos 0 1 3(0) 5 1;
f 9(0) 5 2sin 0 1 3 5 3
1
11x
1
5 2}
}} }} 2 }}2
1 2
1
1 1 }}2
x
(
)1
(c) Since the graph of y 5 f (x) includes the point (0, 1)
2
1
1
1
5 2}
2}}2 2 }}2
1
x
1
1
x
1 1 }}2
x
1
x 11
and the slope of the graph is 3 at this point, the graph
of y 5 f 21(x) will include (1, 0) and the slope will be
1
11x
5}
2 } 2 }}
2
1
1
}}. Thus, f 21(1) 5 0 and (f 21)9(1) 5 }}.
3
3
5 0, x Þ 0
22.
The condition x Þ 0 is required because the original
function was undefined when x Þ 0.
dy
dx
p
20. (a) Note that f 9(x) 5 5x 4 1 6x 2 1 1. Thus f (1) 5 3 and
f 9(1) 5 12.
d
Ïw
x w
2w1) 1 }}(csc 21 x)
dx
2
1
d
x 2w
1 1 (Ïw
2w
1)2 dx
1 42
1
1
2
1+1
1
p
The tangent line is given by y 5 }}(x 2 1) 1 }}, or
2
4
1
1
p
y 5 }}x 2 }} 1 }}.
2
2
4
1
11x
(b) Since }} 5 }}2 , the slope at 1, }} is }}2 5 }}.
5 }} (2s) 2 }}
dy
dx
p
y 5 2x 2 }} 1 1.
d
ds
14. }} 5 }} Ïw
s 2w
2w
1 2 }} sec 21 s
dy
d
15. }} 5 }}(tan 21
dx
dx
p
dy
dx
19. (a) Since }} 5 sec 2 x, the slope at }}, 1 is sec 2 }} 5 2.
2s 2
5 2}
d
ds
d
dx
18. }} 5 }}[sin 21(2x)]21
5 (s) }} (22s) 1 (Ï1ww
2ws2w)(1) 2 }
dy
ds
d
dx
d
dx
17. }} 5 }} (x sin 21 x) 1 }}(Ï1ww
2wx 2w)
1 Ï1ww2wxw 2
[22p, 2p] by [24, 4]
5 (x) }} 1 (sin 21 x)(1) 1 }} (22x)
(a) All reals
5 sin 21 x
(b) 2}}, }}
1
2
113
1
2wx 2w
2Ï1
ww
3
p p
2 2
4
114
Section 3.8
p
2
22. continued
(b) y 5 }}
p
2
(c) At the points x 5 k}}, where k is an odd integer.
(d)
1
d
dx
(c) None, since }} sec 21 x 5 }} Þ 0.
)x)Ïw
x 2w
2w1
30. (a) y 5 0
y
(b) y 5 0
2
1
d
dx
(c) None, since }} csc21 x 5 2}} Þ 0.
–2π
x
2π
31. (a) None, since sin 21 x is
undefined for x . 1.
)x)Ïw
x 2w
2w
1
(b) None, since sin 21 x is undefined for x , 21.
1
d
dx
(c) None, since }} sin 21 x 5 }} Þ 0.
–2
2wx 2w
Ï1ww
32. (a) None, since cos 21 x is undefined for x . 1.
d
dx
(e) f 9(x) 5 }} sin 21 (sin x)
(b) None, since cos 21 x is undefined for x , 21.
1
d
5 }} }} sin x
Ïw1w
2wsw
in2wwx dx
cos x
5 }}
2wsw
in2wwx
Ïw1w
1
d
dx
(c) None, since }} cos 21 x 5 2}} Þ 0.
33. (a)
1
which is 61 depending on whether
2wx2w
Ï1ww
β
α
x
cos x is positive or negative.
a 5 cos 21 x, b 5 sin 21 x
dx
1
23. (a) v(t) 5 }} 5 }}2 which is always positive.
dt
11t
dv
2t
(b) a(t) 5 }} 5 2}}
which is always negative.
dt
(1 1 t 2)2
p
(c) }}
2
1
(b)
a 5 tan 21 x, b 5 cot 21 x
d
5 0 2 }} sin 21 (x)
dx
1
5 2}2
Ïw1w
2wx w
1
d p
dx 2
d
5 0 2 }} tan 21 (x)
dx
1
5 2}}2
11x
x
1
24. }} cos 21 (x) 5 }} }} 2 sin 21 x
d
dx
β
α
2
d p
dx 2
d
dx
p
2
So cos 21 x 1 sin 21 x 5 a 1 b 5 }}.
p
2
So tan 21 x 1 cot 21 x 5 a 1 b 5 }}.
(c)
x
β
α
2
25. }} cot 21 x 5 }} }} 2 tan 21 (x)
1
a 5 sec 21 x, b 5 csc 21 x
p
2
So sec 21 x 1 csc 21 x 5 a 1 b 5 }}.
34.
1
2
d
d p
26. }} csc 21 (x) 5 }} }} 2 sec 21 (x)
dx
dx 2
d
dx
1
2}}
5
)x)Ïw
x 2w
2w1
5 0 2 }} sec 21 (x)
A
B
C
p
27. (a) y 5 }}
2
p
(b) y 5 2}}
2
d
dx
1
11x
(c) None, since }} tan 21 x 5 }}2 Þ 0.
28. (a) y 5 0
(b) y 5 p
d
dx
1
11x
(c) None, since }} cot 21 x 5 2}}2 Þ 0.
p
2
29. (a) y 5 }}
The “straight angle” with the arrows in it is the sum of the
three angles A, B, and C.
A is equal to tan 21 3 since the opposite side is 3 times as
long as the adjacent side.
B is equal to tan 21 2 since the side opposite it is 2 units
and the adjacent side is one unit.
C is equal to tan 21 1 since both the opposite and adjacent
sides are one unit long.
But the sum of these three angles is the “straight angle,”
which has measure p radians.
Section 3.9
35.
s
log x 15
15 log x
log4 x
12 log4 x
Fold 1
Fold 2
g
(x 3)(12x 2)
3x
5 ln }} 5 ln (4x 4)
b
a
Fold 3
s
2
3x 5 19
8.
ln 3x 5 ln 19
x ln 3 5 ln 19
If s is the length of a side of the square, then
ln 19
ln 3
x 5 }} < 2.68
s
s
s
tan b 5 }s 5 2, so b 5 tan 21 2.
tan a 5 }} 5 1, so a 5 tan 21 1 and
9.
}}
2
5t ln 5 5 18
18
ln 5
18
ln 5t 5 ln }}
ln 5
5 t 5 }}
From Exercise 34, we have
g 5 p 2 a 2 b 5 p 2 tan 21 1 2 tan 21 2 5 tan 21 3.
t ln 5 5 ln 18 2 ln (ln 5)
■ Section 3.9 Derivatives of Exponential
and Logarithmic Functions (pp. 163–171)
Leaving Milk on the Counter
ln 18 2 ln (ln 5)
ln 5
t 5 }} < 1.50
3x11 5 2x
10.
1. The temperature of the refrigerator is 428F, the temperature
of the milk at time t 5 0.
2. The temperature of the room is 728F, the limit to which y
tends as t increases.
3. The milk is warming up the fastest at t 5 0. The second
derivative y0 5 230(ln(0.98))2(0.98)t is negative, so y9 (the
rate at which the milk is warming) is maximized at the
lowest value of t.
4. We set y 5 55 and solve;
72 2 30(0.98)t 5 55
ln 3x11 5 ln 2x
(x 1 1) ln 3 5 x ln 2
x(ln 3 2 ln 2) 5 2ln 3
ln 3
ln 2 2 ln 3
x 5 }} < 22.71
Section 3.9 Exercises
dy
dx
d
dx
dy
dx
d
dx
d
dx
dy
dx
d
dx
d
dx
dy
dx
d
dx
d
dx
dy
dx
d
dx
d 2x
dx 3
dy
dx
d
dx
d
dx
dy
dx
d
dx
dy
dx
d
dx
1. }} 5 }}(2e x) 5 2e x
17
30
(0.98)t 5 }}
2. }} 5 }}(e 2x) 5 e 2x }}(2x) 5 2e 2x
1 2
17
t ln (0.98) 5 ln }}
30
3. }} 5 }}e 2x 5 e 2x }}(2x) 5 2e 2x
1 2
t 5 } < 28.114
17
ln }}
30
4. }} 5 }}e 25x 5 e 25x }}(25x) 5 25e 25x
ln (0.98)
The milk reaches a temperature of 558F after about
28 minutes.
1 2
17
ln }}
30
dy
5. }} 5 230 ln (0.98) ? (0.98)t. At t 5 },
ln (0.98)
dt
dy
}} < 0.343 degrees/minute.
dt
ln 8
ln 5
1. log5 8 5 }}
2
3
1 42
1
4
x
6. }} 5 }}e 2x/4 5 e 2x/4 }} 2}} 5 2}}e 2x/4
d
dx
d
dx
8. }} 5 }}(x 2e x) 2 }}(xe x)
x
2. 7x 5 e ln 7 5 e x ln 7
3. ln (e
1 2
5. }} 5 }}e 2x/3 5 e 2x/3 }} }} 5 }}e 2x/3
7. }} 5 }}(xe 2) 2 }}(e x) 5 e 2 2 e x
Quick Review 3.9
tan x
5
4
7. 3 ln x 2 ln 3x 1 ln (12x 2) 5 ln x 3 2 ln 3x 1 ln (12x 2)
s
Exploration 1
15
12
4
6. }4}
12 5 }} 5 }} 5 }}, x . 0
5 (x 2)(e x) 1 (e x)(2x) 2 [(x)(e x) 1 (e x)(1)]
) 5 tan x
x 24
x12
2
(x 1 2)(x 2 2)
x12
4. ln (x 2 2 4) 2 ln (x 1 2) 5 ln }} 5 ln }}
5 ln (x 2 2)
5. log2 (8x25) 5 log2 (23)x25 5 log2 23x215 5 3x 2 15
5 x 2e x 1 xe x 2 e x
eÏxw
9. }} 5 }} e Ïxw 5 e Ïxw }}(Ïxw) 5 }}
dx
dx
dx
2Ïxw
dy
d
dy
dx
d
dx
d
d
dx
10. }} 5 }} e (x ) 5 e (x ) }}(x 2) 5 2xe (x )
2
2
2
115
116
Section 3.9
dy
dx
d
dx
25. }} 5 }} ln (x 1 2) 5 }} }}(x 1 2) 5 }}, x . 22
dy
dx
dy
dx
d
dx
26. }} 5 }} ln (2x 1 2) 5 }} }}(2x 1 2) 5 }}
dy
dx
d
dx
dy
dx
d
dx
dy
dx
d
dx
dy
dx
d
dx
11. }} 5 }}(x p) 5 px p21
12. }} 5 }}(x 11Ï2w) 5 (1 1 Ï2w)x 11Ï2w21 5 (1 1 Ï2w)x Ï2w
13. }} 5 }} x 2 Ï2w 5 2Ï2wx 2 Ï2w21
dy
dx
d
dx
d
dx
dy
dx
dy
dx
ln y 5 ln x ln x
dy
dx
1
d
dx
d ln x 2
dx ln 4
1
2
1
}} 5 }} 5 }}
x
x ln 4
x ln 2
d
dx
31 ln 4 2
2
?
4
d
dx
1
d
(3x 1 1) ln 2 dx
1
3
3
(3x 1 1) ln 2
5 }}, x . 2}}
5 }}(ln x)2
1x2
dy
dx
1
1 d
2 dx
d
dx
34. }} 5 }} log10 (x 1 1)1/2 5 }} }} log10 (x 1 1)
5 (2 ln x) }}
1
1
d
2 (x 1 1) ln 10 dx
2y ln x
x
2x ln x ln x
5 }}
x
1
2(x 1 1) ln 10
5 }} }} }}(x 1 1) 5 }}, x . 21
dy
dx
1x2
1
d
dx
d
dx
1
x ln 2
35. }} 5 }} log2 }} 5 }}(2log2 x) 5 2}}, x . 0
20. Use logarithmic differentiation.
dy
dx
d
1
1
d
dx log2 x
(log2 x) dx
1
1
1
ln 2
5 2}}2 }} 5 2}}2 or 2}}2
(log2 x) x ln 2
x(ln 2)(log2 x)
x(ln x)
36. }} 5 }} }} 5 2}}2 }}(log2 x)
y 5 x 1/ln x
ln y 5 ln x 1/ln x
dy
dx
d
dx
d
dx
37. }} 5 }}(ln 2 ? log2 x) 5 (ln 2)}}(log2 x)
1
ln x
ln y 5 }} ln x
1 x ln 2 2
1
1
x
5 (ln 2) }} 5 }}, x . 0
ln y 5 1
y 5e
1 d
x dx
2
x
1
x
d
dx
d
dx
1
ln 10
5 }}
2 ln x
x
dy
dx
1
x
d
dx
d
dx
40. }} 5 }} ln 10x 5 }}(x ln 10) 5 ln 10
1
x
23. }} 5 }} ln (x 21) 5 }}(2ln x) 5 2}}, x . 0
d
dx
dy
dx
ln e
ln 10
39. }} 5 }}(log10 e x) 5 }}(x log10 e) 5 log10 e 5 }}
22. }} 5 }}(ln x)2 5 2 ln x }}(ln x) 5 }}
d
dx
d
dx
1
d
(1 1 x ln 3) ln 3 dx
ln 3
1
1
5 }} 5 }}, x . 2}}
(1 1 x ln 3) ln 3
1 1 x ln 3
ln 3
21. }} 5 }} ln (x 2) 5 }}2 }}(x 2) 5 }}2 (2x) 5 }}
d
dx
dy
dx
38. }} 5 }} log3 (1 1 x ln 3) 5 }} }}(1 1 x ln 3)
dy
d
}} 5}}(e) 5 0, x . 0
dx
dx
10
x
1x2
33. }} 5 }} log2 (3x 1 1) 5 }} }}(3x 1 1)
ln y 5 ln x ln x
d
dx
1
x ln x
1
y 5x ln x
dy
dx
1
x
}} ln x
dy
d
d ln x 1/2
d 2
32. }} 5 }}(log5 Ïxw) 5 }} }} 5 }} }
dx
dx
dx ln 5
dx ln 5
1
1
d
1
1
5 }} }}(ln x) 5 }} ? }} 5 }}, x . 0
2 ln 5 dx
2 ln 5 x
2x ln 5
19. Use logarithmic differentiation.
d
dx
1
ln x
d
dx
2
5 }}
ln 4
5 23cot x (ln 3)(csc 2x)
dy
dx
2x
x 11
31. }} 5 }}(log4 x 2) 5 }} }} 5 }} }} (ln x)
5 3cot x (ln 3)(2csc 2 x)
d
dx
1 d
ln x dx
5 1 1 ln x 2 1 5 ln x
dy
d
d
}} 5 }} 3cot x 5 3cot x (ln 3)}}(cot x)
dx
dx
dx
dy
dx
1
d
x 1 1 dx
30. }} 5 }}(x ln x 2 x) 5 (x) }} 1 (ln x)(1) 2 1
5 23csc x (ln 3)(csc x cot x)
d
dx
2
2x 1 2
1
d
2 2 cos x dx
d
dx
d
dx
5 3csc x (ln 3)(2csc x cot x)
dy
dx
1
d
2x 1 2 dx
29. }} ln (ln x) 5 }} }} ln x 5 }} ? }} 5 }}
17. }} 5 }} 3csc x 5 3csc x (ln 3)}}(csc x)
5 }}
1
x12
2
28. }} 5 }} ln (x 2 1 1) 5 }
2 } }}(x 1 1) 5 }
2 }
d
dx
d
dx
d
dx
1
5 }}, x . 21
x11
d
dx
sin x
5 }}
2 2 cos x
16. }} 5 }} 92x 5 92x (ln 9)}}(2x) 5 292x ln 9
d
}}(ln y)
dx
1 dy
}} }}
y dx
dy
}}
dx
dy
}}
dx
dy
dx
dy
dx
15. }} 5 }} 8x 5 8x ln 8
18.
1
d
x 1 2 dx
27. }} 5 }} ln (2 2 cos x) 5 }} }}(2 2 cos x)
14. }} 5 }} x 12e 5 (1 2 e)x 12e21 5 (1 2 e)x 2e
dy
dx
d
dx
1
x
24. }} 5 }} ln }} 5 }}(ln 10 2 ln x) 5 0 2 }} 5 2}}, x . 0
Section 3.9
41. The line passes through (a, e a) for some value of a and has
slope m 5 e a. Since the line also passes through the origin,
y 5
45.
e
a
(x 2 3)4(x 2 1 1) 1/5
2
3
3
(x 2 3) (x 1 1) 1/5
4
2
2
(2x 1 5)
(x 2 3) (x 1 1)
(2x 1 5)
4
1
5
2
ln y 5 }} ln }}
3
y 5 ex.
1
5
ln y 5 }}[4 ln (x 2 3) 1 ln (x 2 1 1) 2 3 ln (2x 1 5)]
4 d
d
}}(ln y) 5 }} }} ln (x 2 3) 1
5 dx
dx
42. For y 5 xe x, we have y9 5 (x)(e x) 1 (e x)(1) 5 (x 1 1)e x, so
the normal line through the point (a, ae a)
1 d
3 d
}} }} ln (x 2 1 1) 2 }} }} ln (2x 1 5)
5 dx
5 dx
1
(a 1 1)e
has slope m 5 2}}a and its equation is
1 dy
4 1
1
1
3
1
}} }} 5 }} }} 1 }} }
} (2x) 2 }} }} (2)
y dx
5 x23
5 x2 1 1
5 2x 1 5
1
(a 1 1)e
y 5 2}}a (x 2 a) 1 ae a. The desired normal line
1
1
0 5 2}}a (0 2 a) 1 ae a
(a 1 1)e
a
0 5 }}a 1 ae a
(a 1 1)e
1
0 5 a }}a 1 e a
(a 1 1)e
1
a 5 0 or }}a 1 e a 5 0
(a 1 1)e
1
The equation }}a 1 e a 5 0 has no solution, so we
(a 1 1)e
1
2
2
dy
2x
4
6
}} 5 y }} 1 }
} 2 }}
dx
5(x 2 3)
5(x 2 1 1)
5(2x 1 5)
includes the point (0, 0), so we have:
1
(x 2 3) (x 1 1) 1/5
4
2
dy
}} 5 }}
dx
(2x 1 5)3
2
?
} 1 }} 2 }}
1}
5(x 2 3)
5(x 1 1)
5(2x 1 5) 2
2x
4
6
2
xÏw
x2w
1w1
(x 1 1)
x(x 2 1 1)1/2
(x 1 1)
y 5 }}
2/3 5 }}
2/3
46.
x(x 2 1 1)1/2
(x 1 1)
ln y 5 ln }}
2/3
1
2
2
3
ln y 5 ln x 1 }} ln (x 2 1 1) 2 }} ln (x 1 1)
need to use a 5 0. The equation of the normal line is
1 d
2 d
d
d
}} ln y 5 }} ln x 1 }} }} ln (x 2 1 1) 2 }} }} ln (x 1 1)
2 dx
3 dx
dx
dx
1
(0 1 1)e
y 5 2}}0 (x 2 0) 1 0e 0, or y 5 2x.
1 dy
1
1
1
2 1
}} }} 5 }} 1 }} }
} (2x) 2 }} }} (1)
y dx
x
2 x2 1 1
3 x11
y 5 (sin x)x
1
2
ln y 5 ln (sin x)x
dy
1
x
2
}} 5 y }} 1 }
} 2 }}
dx
x
x2 1 1
3(x 1 1)
ln y 5 x ln (sin x)
xÏw
xw
1w1 1
dy
x
2
}} 5 }}
}} 1 }
} 2 }}
(x 1 1)2/3 x
dx
x2 1 1
3(x 1 1)
d
}} ln y
dx
1 dy
}} }}
y dx
dy
}}
dx
dy
}}
dx
44.
4
5
1
e a 5 }}, so a 5 1. Hence, the slope is e and the equation is
43.
2
!}
§(x§2§(23§x)§1(x§}
§5§)1§1)§ 5 1}}
(2x 1 5)
ln y 5 ln }}
3
ea 2 0
a20
the slope is also given by m 5 }} and we have
a
117
d
5 }}[x ln (sin x)]
dx
1
5 (x) }} (cos x) 1 ln (sin x)(1)
sin x
1 2
5 y[x cot x 1 ln (sin x)]
5 (sin x)x[x cot x 1 ln (sin x)]
)
1 t/140
122
22t/140
d
dt
d
dx
1x2
1
2
2
4
This means that the rate of decay is the positive rate of
tan x
x
tan x tan x
5x
}} 1 (ln x)(sec 2 x)
x
3
t
140
dA
(221/70)(ln 2)
}} 5 2}} < 20.098 grams/day.
dt
7
5 (tan x) }} 1 (ln x)(sec 2 x)
5 y }} 1 (ln x)(sec 2 x)
1
5 20 (22t/140)(ln 2)}} 2}}
At t 5 2 days, we have
5 }}[(tan x)(ln x)]
3
d
dt
d
5 20 }}
dt
47. }} 5 20 }} }}
1
tan x
ln y 5 (tan x)(ln x)
d
}} ln y
dx
1 dy
}} }}
y dx
dy
}}
dx
dy
}}
dx
dA
dt
2
1
5 20(22t/140)(ln 2) 2}}
140
(22t/140)(ln 2)
5 2}}
7
y 5 x tan x
ln y 5 ln (x
1
2
4
approximately 0.098 grams/day.
d
dx
1 d
kx dx
d
dx
d
dx
k
kx
1
x
48. (a) }} ln (kx) 5 }} }} kx 5 }} 5 }}
(b) }} ln (kx) 5 }} (ln k 1 ln x)
d
dx
1
x
5 0 1 }} ln x 5 }}
118
Chapter 3 Review
■ Chapter 3 Review Exercises
49. (a) Since f 9(x) 5 2x ln 2, f 9(0) 5 20 ln 2 5 ln 2.
f(h) 2 f(0)
h
h→0
2h 2 20
h
h→0
2h 2 1
h
h→0
(b) f 9(0) 5 lim }} 5 lim }} 5 lim }}
(c) Since quantities in parts (a) and (b) are equal,
(pp. 172–175)
d
dx
dy
dx
d
dx
dy
dx
d
dx
(d) By following the same procedure as above using
50. Recall that a point (a, b) is on the graph of y 5 e x if and
only if the point (b, a) is on the graph of y 5 ln x.
Since there are points (x, e x) on the graph of y 5 e x with
arbitrarily large x-coordinates, there will be points (x, ln x)
on the graph of y 5 ln x with arbitrarily large y-coordinates.
(b) The graph of y3 is always a horizontal line.
y3
We conclude that the graph of y3 is a horizontal line at
y 5 ln a.
y
(c) }} a x 5 a x if and only if y3 5 }}2 5 1.
y1
d x
So if y3 5 ln a, then }} a will equal a x if and only if
dx
ln a 5 1, or a 5 e.
d
dx
(d) y2 5 }} a x 5 a x ln a. This will equal y1 5 a x if and
only if ln a 5 1, or a 5 e.
1
2
1
2
1
x
d
dx
d
dx
5 22 sin 2 x 1 2 cos 2 x
Alternate solution:
dy
d
d
}} 5 }}(2 sin x cos x) 5 }} sin 2x 5 (cos 2x)(2)
dx
dx
dx
5 2 cos 2x
dy
dx
d 2x 1 1
dx 2x 2 1
ds
dt
d
dt
ds
dt
d
dt
5
ln a 0.693147 1.098612 1.386294 1.609438
d
dx
1
4
(2x 2 1)(2) 2 (2x 1 1)(2)
(2x 2 1)
4
(2x 2 1)
4. }} 5 }} }} 5 }}}
5 2}}2
2
0.693147 1.098613 1.386295 1.609439
d
dx
1
4
d
dx
51. (a) The graph y4 is a horizontal line at y 5 a.
4
2
5 2(sin x)}}(cos x) 1 2(cos x)}}(sin x)
7h 2 1
h
h→0
3
1
4
3. }} 5 }}(2 sin x cos x)
g(x) 5 7x, we may see that lim }} 5 ln 7.
2
1
8
2. }} 5 }}(3 2 7x 3 1 3x 7) 5 221x 2 1 21x 6
2h 2 1
lim }} 5 ln 2.
h
h→0
a
1
dy
dx
1. }} 5 }} x 5 2 }}x 2 1 }}x 5 5x 4 2 }}x 1 }}
52. }} 2}}x 2 1 k 5 2x and }}(ln x 1 c) 5 }}.
5. }} 5 }} cos (1 2 2t) 5 2sin (1 2 2t)(22) 5 2 sin (1 2 2t)
1t2
2
1}t}2
1 t 2 dt 1 t 2
2
1 t 21 t 2
2 d 2
2
2
6. }} 5 }} cot }} 5 2csc 2 }} }} }} 5 2csc 2 }} 2}}2
2
t
5 }}2 csc 2
dy
d
1
1
2
d
7. }} 5 }} Ïxw 1 1 1 }} 5 }}(x 1/2 1 1 1 x 21/2)
dx
dx
dx
Ïwx
1
1
1
1
5 }}x 21/2 2 }}x 23/2 5 }} 2 }3/2
}
2
2
2x
2Ïwx
dy
d
dr
du
d
du
1
2
1
8. }} 5 }}(xÏ2wxw1
ww1) 5 (x) }} (2) 1 (Ï2wxw1
w 1)(1)
dx
dx
2Ï2
wxw1
ww1
x 1 (2x 1 1)
3x 1 1
5 }} 5 }}
Ï2wxw1
ww1
Ï2wxw1
ww1
9. }} 5 }} sec (1 1 3u) 5 sec (1 1 3u) tan (1 1 3u)(3)
5 3 sec (1 1 3u) tan (1 1 3u)
Therefore, at any given value of x, these two curves will
have perpendicular tangent lines.
dr
du
d
du
10. }} 5 }} tan 2 (3 2 u 2)
d
du
5 2 tan (3 2 u 2)}} tan (3 2 u 2)
53. (a) Since the line passes through the origin and has slope
1
x
}}, its equation is y 5 }}.
e
e
5 2 tan (3 2 u 2) sec 2 (3 2 u 2)(22u)
524u tan (3 2 u 2) sec 2 (3 2 u 2)
(b) The graph of y 5 ln x lies below the graph of the line
x
e
x
e
y 5 }} for all positive x Þ e. Therefore, ln x , }} for all
positive x Þ e.
dy
dx
d
dx
11. }} 5 }}(x 2 csc 5x)
5 (x 2)(2csc 5x cot 5x)(5) 1 (csc 5x)(2x)
(c) Multiplying by e, e ln x , x or ln x , x.
e
(d) Exponentiating
both sides of ln x e , x, we have
e
e ln x , e x, or x e , e x for all positive x Þ e.
(e) Let x 5 p to see that p e , e p. Therefore, e p is bigger.
5 25x 2 csc 5x cot 5x 1 2x csc 5x
dy
d
dy
dx
d
dx
dy
dx
d
dx
1
d
1
1
1
12. }} 5 }} ln Ïxw 5 }} }} Ïxw 5 }} ? }} 5 }}, x . 0
dx
dx
Ïwx dx
Ïwx 2Ïwx 2x
1
d
1 1 e dx
ex
11e
13. }} 5 }} ln (1 1 e x) 5 }}x }}(1 1 e x) 5 }}x
14. }} 5 }}(xe 2x) 5 (x)(e 2x)(21) 1 (e 2x)(1) 5 2xe 2x 1 e 2x
Chapter 3 Review
dy
dx
d
dx
d
dx
d
dx
Alternate solution, using logarithmic differentiation:
15. }} 5 }}(e 11ln x) 5 }}(e 1e ln x) 5 }}(ex) 5 e
(2x)2x
y 5 }}
x 2w
1w1
Ïw
dy
cos x
d
1 d
16. }} 5 }} ln (sin x) 5 }} }}(sin x) 5 }} 5 cot x, for
dx
sin x
dx
sin x dx
ln y 5 ln (2x) 1 ln (2x) 2 ln Ïw
x 2w
1w1
values of x in the intervals (kp, (k 1 1)p), where k is even.
1
2
ln y 5 ln 2 1 ln x 1 x ln 2 2 }} ln (x 2 1 1)
dr
d
1
d
17. }} 5 }} ln (cos 21 x) 5 }21
} }} cos 21 x
dx
dx
cos x dx
1
1
1
5 }21
} 2}} 5 2}}
cos x
2wx 2w
Ï1ww
cos 21xÏ1ww
2wx 2w
1
dr
du
d
du
ds
dt
d
dt
2
2u
u ln 2
1
d
u ln 2 du
2
u ln 2
2
18. }} 5 }} log2 (u 2) 5 }
2 } }}(u ) 5 }
2 } 5 }}
1
d
(t 2 7) ln 5 dt
1
(t 2 7) ln 5
19. }} 5 }} log5 (t 2 7) 5 }} }}(t 2 7) 5 }},
t.7
ds
dt
d
}} ln y
dx
1 dy
}} }}
y dx
dy
}}
dx
dy
}}
dx
dy
dx
d
dt
1
2
d
dx
5 }}[ln 2 1 ln x 1 x ln 2 2 }} ln (x 2 1 1)]
1
x
1
1
2 x 11
1
x
5 y }} 1 ln 2 2 }
}
x
x2 1 1
(2x)2x 1
x
5 }} }} 1 ln 2 2 }
}
x2 1 1
x 2w
1w1 x
Ïw
5 0 1 }} 1 ln 2 2 }} }
2 } (2x)
1
d
dx
23. }} 5 }} e tan
d
dt
119
21
2
1
x
5 e tan
21
2
21
etan x
}} tan 21x 5 }}2
dx
11x
x d
20. }} 5 }}(82t ) 5 82t(ln 8)}}(2t) 5 282t ln 8
dy
du
d
du
24. }} 5 }} sin 21 Ï1ww
2w
u 2w
21. Use logarithmic differentiation.
5
y 5x ln x
1
u
dy
dt
2w
)u) Ï1
ww
u 2w
1
2
d
dt
25. }} 5 }}(t sec 21 t 2 }} ln t)
d
5 }}(ln x)2
dx
d
5 2 ln x }} ln x
dx
2y ln x
5 }}
x
2x ln x ln x
5 }}
x
1 )t) Ïwt w2w1 2
1
1
2t
5 (t) }} 1 (sec 21 t)(1) 2 }}
2
t
1
2t
5 }} 1 sec 21 t 2 }}
)t) Ïw
t 2w
2w1
dy
dt
d
dt
26. }} 5 }}[(1 1 t 2) cot 21 2t]
1
1
1 1 (2t)
2
5 (1 1 t 2) 2}}2 (2) 1 (cot 21 2t)(2t)
dy
d (2x)2x
22. }} 5 }} }}
dx
dx Ïw
x 2w
1w1
d
d
Ïw
x 2w
1w1 }d}x [(2x)2x] 2 (2x)(2x)}}
dx
2 1 2t
1 1 4t
Ïw
x 2w
1w
1
dy
dz
1
2Ïw
x w
1w
1
5 }}}}}}
2
2wz 2w
Ï1ww
2
1
2wz 2w
2Ï1
ww
z
z
2wz 2w
Ï1ww
2wz 2w
Ï1ww
5 2}} 1 cos 21 z 1 }}
x 11
5 cos 21 z
(x 2 1 1)(2x)(2x ln 2 1 2) 2 2x 2(2x)
(x 1 1)
5 }}}}
2
3/2
dy
dx
d
dx
28. }} 5 }}(2Ïxw2
ww1 csc 21 Ïxw)
?
5 }}}}
2
3/2
(2 2x)[(x 2 1 1)(x ln 2 1 1) 2 x 2]
(x 1 1)
?
5 }}}}}
2
3/2
(2 2 )(x ln 2 1 x 1 x ln 2 1 1 2 x )
(x 1 1)
(2 2x)(x 3 ln 2 1 x ln 2 1 1)
(x 1 1)
1
5 (z) 2}} 1 (cos 21 z)(1) 2 }}(22z)
1
Ïw
x 2w
1w1[(2x)(2x)(ln 2) 1 (2x)(2)] 2 (2x)(2x)}}(2x)
2
?
5 }}}
2
3/2
d
dz
27. }} 5 }}(z cos 21 z 2 Ï1ww
2wz 2w)
x 11
2
2
5 2}}2 1 2t cot 21 2t
5 }}}}}
2
3
1
2w
Ïwu 2w 2Ï1ww
u 2w
ln y 5 (ln x)(ln x)
x
Ï1ww
2w
u 2w
5 }} }}(22u) 5 2}}
ln y 5 ln (x ln x)
d
}} ln y
dx
1 dy
}} }}
y dx
dy
}}
dx
dy
}}
dx
1
}} d
}}
Ïw1w
2w
(Ïw
1w
2w
u 2w
w)2w du
2
1
21 2
1
1
5 (2Ïxw2
ww1) 2}} }}
)Ïxw)Ïw
(Ïw
xw)2w2
ww1 2Ïwx
1
1
1 (2 csc 21 Ïxw) }}
2Ïxw2
ww1
2
Ïxw2
ww1
csc21 Ïxw
5 2 }} 1 }}
Ïxw2
ww1
(Ïxw)2Ïxw2
ww1
21 Ïw
1
csc
x
5 2}} 1 }}
x
Ïxw2
ww1
120
Chapter 3 Review
dy
dx
32. Since y 5 sin x 2 x cos x is defined for all real x and
d
dx
29. }} 5 }} csc 21 (sec x)
dy
}} 5 cos x 2 (x)(2sin x) 2 (cos x)(1) 5 x sin x, the
dx
1
}}} d
5 2
}}(sec x)
)sec x) Ïw
sew
c 2wxw
2w1 dx
1
2
function is differentiable for all real x.
1
5 2}} sec x tan x
)sec x) Ïta
wwn 2wwx
33. Since y 5
sec x tan x
5 2}}
)sec x tan x)
1 sin x
}} } }
cos x cos x
2}}
1 sin x
}} } }
cos x cos x
5
)
)
x 2 2 2x 2 1
5 }}}
, which is defined only for x , 1,
2Ï1
ww
2wx (1 1 x 2)3/2
3p
2
the function is differentiable for all x , 1.
Alternate method:
p
2
3p
2
On the domain 0 # x # 2p, x Þ }}, x Þ }}, we may
rewrite the function as follows:
y 5 csc 21 (sec x)
p
2
p
5 }} 2 cos 21 (cos x)
2
p
p
0 # x # p, x Þ }}
}} 2 x,
2
5 2
p
3p
}} 2(p 2 x), p , x # 2p, x Þ }}
2
2
5 }} 2 sec 21 (sec x)
x15
2x 2 7
(2x 2 7)(1) 2 (x 1 5)(2)
7
dy
17
5 2}}2 , the
x Þ }} and }} 5 }}}
2
dx
(2x 2 7)
(2x 2 7)2
34. Since y 5 (2x 2 7)21(x 1 5) 5 }} is defined for all
7
function is differentiable for all x Þ }}.
2
5
5
35. Use implicit differentiation.
xy 1 2x 1 3y 5 1
d
d
d
}}(xy) 1 }}(2x) 1 }}(3y)
dx
dx
dx
dy
dy
x }} 1 (y)(1) 1 2 1 3 }}
dx
dx
dy
(x 1 3)}}
dx
dy
}}
dx
p
p
0 # x # p, x Þ }}
}} 2 x,
2
2
p
3p
2}} 1 x, p , x # 2p, x Þ }}
2
2
p
21, 0 # x , p, x Þ }}
2
p
1, p , x # 2p, x Þ }}
2
5
d 1 1 sin u 2
du 1 2 cos u
1
2
1 1 sin u (1 2 cos u)(cos u) 2 (1 1 sin u)(sin u)
5 21}}21}}}}2
(1 2 cos u)
1 2 c os u
1 1 sin u cos u 2 cos u 2 sin u 2 sin u
5 21}}21}}}}2
(1 2 cos u)
1 2 c os u
1 1 sin u cos u 2 sin u 2 1
5 21}}21}}2
(1 2 cos u)
1 2 c os u
30. }} 5 }} }}
5 2(y 1 2)
y12
x13
5 2}}
d
d
d
}}(5x 4/5) 1 }}(10y 6/5) 5 }}(15)
dx
dx
dx
dy
4x 21/5 1 12y 1/5 }} 5 0
dx
dy
4x 2 1/5
1
5 2}}
}} 5 2}}
dx
12y 1/5
3(xy)1/5
37. Use implicit differentiation.
Ïxy
w 51
2
d
}}
dx
2
2
31. Since y 5 ln x 2 is defined for all x Þ 0 and
dy
2x
2
1 d
}} 5 }}2 }}(x 2) 5 }}2 5 }}, the function is differentiable for
dx
x
x
x dx
all x Þ 0.
50
5x 4/5 1 10y 6/5 5 15
2
2
d
dx
5 }}(1)
36. Use implicit differentiation.
Note that the derivative exists at 0 and 2p only because
these are the endpoints of the given domain; the two-sided
derivative of y 5 csc 21(sec x) does not exist at these
points.
dr
du
2
!§1§1§x§
sin x
)sin x)
5 2}}
p
2
dy
Therefore, }} 5
dx
12x
1
} (1 1x 2)(21) 2 (1 2 x)(2x)
dy
}} 5
1 2 x }}}
(1 1 x 2)2
dx
2 }}2
5 2sign (sin x), x Þ }}, p, }}
5
!}
§1§1}
§x§ is defined for all x , 1 and
Ïxy
w 5 }d}(1)
dx
1
dy
}}[x }} 1 (y)(1)] 5 0
xy dx
2Ïw
dy
x }} 1 y 5 0
dx
dy
y
}} 5 2}}
dx
x
Alternate method:
1
x
Since Ïxy
w 5 1, we have xy 5 1 and y 5 }}.
dy
dx
1
x
Therefore, }} 5 2}}2 .
121
Chapter 3 Review
38. Use implicit differentiation.
y 3 1 y 5 2 cos x
41.
x
x11
d
d
x
}} y 2 5 }} }}
dx
dx x 1 1
dy
(x 1 1)(1) 2 (x)(1)
2y }} 5 }}
dx
(x 1 1)2
dy
1
}} 5 }}2
dx
2y(x 1 1)
y 2 5 }}
39.
d
d
d
}}(y 3) 1 }}(y) 5 }}(2 cos x)
dx
dx
dx
3y 2y9 1 y9 5 22 sin x
(3y 2 1 1)y9 5 22 sin x
x3 1 y3 5 1
2 sin x
3y 1 1
y9 5 2}
2}
d
d
d
}}(x 3) 1 }}(y 3) 5 }}(1)
dx
dx
dx
d
dx
3x 2 1 3y 2y9 5 0
1
2 sin x
3y 1 1
2
y0 5 }} 2}
2}
x2
y9 5 2}}2
y
x2
d
y0 5 }} 2}}2
y
dx
(3y 2 1 1)(2 cos x) 2 (2 sin x)(6yy9)
(3y 1 1)
5 2}}}}
2
2
1 2
1
(3y 1 1)
1 2
2
(3y 2 1 1)2 cos x 1 12y sin 2 x
(3y 1 1)
5 22}}}}
2
3
5 2 }}}
y4
x 1/3 1 y 1/3 5 4
42.
2xy 3 1 2x 4
y
2x(x 3 1 y 3)
5 2 }}
y5
2x
5 2}}5
y
5 2}}
5
d
d
d
}}(x 1/3) 1 }}(y 1/3) 5 }}(4)
dx
dx
dx
1
1
}}x 22/3 1 }}y 22/3y9 5 0
3
3
x 2 2/3
y 2/3
y9 5 2}
}5 2 }}
y 2 2/3
x
12
since x 3 1 y 3 5 1
y 2/3
3 1x2 4
2 y
xy9 2 (y)(1)
5 2}}1}}2
1}x}2
3 x
d
dx
y0 5 }} 2 }}
40.
2
x
y 2 5 1 2 }}
21/3
2
12
d
d
d 2
}}(y 2) 5 }}(1) 2 }} }}
dx
dx
dx x
2
2yy9 5 }}2
x
2
1
y9 5 }
} 5 }2}
x 2(2y)
x y
d 1
y0 5 }} }2}
dx x y
1
d
5 2}2}2 }}(x 2y)
(x y) dx
1
5 2}2}2 [(x 2)(y9) 1 (y)(2x)]
(x y)
1
1
5 2}2}2 (x 2) }2} 1 2xy
(x y)
x y
1 1
5 2}4}2 }} 1 2xy
x y y
1 1 2xy 2
5 2}4}
x y3
2 y 21/3
12
5 2}} }}
3 x
4
1
y 2/3
3 1x2 4 2 y
(x) 2 }}
}}
x2
2
3
2
5 2}}x 1/3y 21/3(2x 25/3y 2/3 2 x 22y)
1 2
3 1 2
1
2
2
5 2}}}}}
2
2
x2
(y )(2x) 2 (x )(2y) 2}}2
y
2
2 sin x
3y 1 1
(3y 2 1 1)(2 cos x) 2 (12y sin x) 2}
2}
(y 2)(2x) 2 (x 2)(2y)(y9)
5 2}}}
y4
2
3
2
3
5 }}x 24/3y 1/3 1 }}x 25/3y 2/3
43. y9 5 2x 3 2 3x 2 1,
y0 5 6x 2 2 3,
y- 5 12x,
y (4) 5 12, and the rest are all zero.
4
44. y9 5 }x},
24
3
y0 5 }x},
6
2
y- 5 }x},
2
y (4) 5 x,
y (5) 5 1, and the rest are all zero.
122
Chapter 3 Review
1
x21
45. }d}y 5 }d} Ïw
x 2w
2w2xw 5 }} (2x 2 2) 5 }}
dx
2w2xw
2Ïw
x 2w
dx
2w2xw
Ïxw2w
At x 5 3, we have y 5 Ï3w2w2
ww2(3
w)w 5 Ï3w
321
dy
5
4
4
5
2
2
2
(a) Tangent: y 5 }}(x 2 3) 1 Ï3w or y 5 }}x 2 Ï3w
Ïw3
Ïw3
22 sin t
2 cos t
dx
}}
dt
3p
4
3p
4
3p
4
dy
dx
y 5 2 cos }} 5 2Ï2w, and }} 5 2tan }} 5 1.
d
dx
46. }} 5 }}(4 1 cot x 2 2 csc x)
The equation of the tangent line is
y 5 1(x 2 Ï2w) 1 (2Ï2w), or y 5 x 2 2Ï2w.
5 2csc 2 x 1 2 csc x cot x
p
At x 5 }}, we have
2
p
p
y 5 4 1 cot }} 2 2 csc }} 5 4 1 0 2 2 5 2 and
2
2
dy
p
p
p
}} 5 2csc 2 }} 1 2 csc }} cot }} 5 21 1 2(1)(0) 5 21.
dx
2
2
2
2
p
p
(a) Tangent: y 5 21 x 2 }} 1 2 or y 5 2x 1 }} 1 2
2
2
p
2
dy
}}
dy
dx
At t 5 }}, we have x 5 2 sin }} 5 Ï2w,
2
Ï3w
5Ï3w
or y 5 2}}x 1 }}
2
2
1
11
5
dt
49. }} 5 }
5 }} 5 2tan t
3p
4
Ïw3
(b) Normal: y 5 2}}(x 2 3) 1 Ï3w
1
4
5
(b) Normal: y 5 }}(x 2 4) 1 1 or y 5 }}x 2 }}
and }} 5 }} 5 }}.
dx
Ï3w2w2
ww2(3
w)w Ï3w
dy
dx
5
4
(a) Tangent: y 5 2}}(x 2 4) 1 1 or y 5 2}}x 1 6
2
p
2
dy
}}
dy
dx
4
3
4 cos t
23 sin t
dt
5 }} 5 2}} cot t
50. }} 5 }
dx
}}
dt
3p
3p
3Ïw2
At t 5 }}, we have x 5 3 cos }} 5 2}},
4
4
3p
4
2
dy
dx
3p
4
4
3
4
3
y 5 4 sin }} 5 2Ï2w, and }} 5 2}} cot }} 5 }}.
(b) Normal: y 5 1 x 2 }} 1 2 or y 5 x 2 }} 1 2
The equation of the tangent line is
47. Use implicit differentiation.
4
3Ï2w
4
y 5 }} x 1 }} 1 2Ï2w, or y 5 }}x 1 4Ï2w.
x 2 1 2y 2 5 9
3
d
d
d
}}(x 2) 1 }}(2y 2) 5 }}(9)
dx
dx
dx
dy
2x 1 4y }} 5 0
dx
dy
2x
x
}} 5 2}} 5 2}}
dx
4y
2y
1
1
Slope at (1, 2): 2}} 5 2}}
4
2(2)
dy
51. }} 5
dx
1
2
dy
}}
dt
}
dx
}}
dt
2
3
5 sec 2 t
3 sec t tan t
5 sec t
3 tan t
5
3 sin t
5 }} 5 }} 5 }}
p
6
p
6
At t 5 }}, we have x 5 3 sec }} 5 2Ï3w,
1
4
1
4
p
5Ï3w
dy
10
5
y 5 5 tan }} 5 }}, and }} 5 } 5 }}.
6
9
4
(a) Tangent: y 5 2}}(x 2 1) 1 2 or y 5 2}}x 1 }}
dx
3
3 sin }p}
162
3
The equation of the tangent line is
(b) Normal: y 5 4(x 2 1) 1 2 or y 5 4x 2 2
10
5Ï3w
10
y 5 }}(x 2 2Ï3w) 1 }}, or y 5 }}x 2 5Ï3w.
3
48. Use implicit differentiation.
w56
x 1 Ïxy
d
d
w) 5 }d}(6)
}}(x) 1 }}(Ïxy
dx
dx
dx
1
3 1 2
4
dy
1 1 }} (x) }} 1 (y)(1) 5 0
dx
xy
2Ïw
x dy
y
}} }} 5 21 2 }}
xy dx
xy
2Ïw
2Ïw
dy
2Ïw
y
xy
}} 5 }} 21 2 }}
dx
x
xy
2Ïw
1
!§x
y
2
y
x
5 22 }} 2 }}
!§4
1
1
4
2
2
1
4
5
4
Slope at (4, 1): 22 }} 2 }} 5 2}} 2 }} 5 2}}
3
3
Chapter 3 Review
dy
52. }} 5
dx
dy
}}
dt
}
dx
}}
dt
123
(c) Nowhere in its domain
1 1 cos t
5 }}
2sin t
59.
y
2
y = f 9(x)
Ïw2
p
p
At t 5 2}}, we have x 5 cos 2}} 5 }},
4
4
2
1 2
–3
3
Ï2w
p
p
p
y 5 2}} 1 sin 2}} 5 2}} 2 }}, and
1 42
4
4
p
1 2
1 2
–2
2
1 1 cos 2}}
Ï2w
4
1 1 }}
}}
2
dy
}
5 Ï2w 1 1.
}} 5 2sin 2}p} 5
Ï2w
dx
4
}}
x
60.
y
2
y = f 9(x)
The equation of the tangent line is
Ïw
Ïw
y 5 (Ï2
w 1 1) x 2 }}2 2 }p} 2 }}2 , or
1
2
2
4
2
p
y 5 (1 1 Ï2w)x 2 Ï2w 2 1 2 }}.
4
This is approximately y 5 2.414x 2 3.200.
x
61. (a) iii
(b) i
(c) ii
53. (a)
62. The graph passes through (0, 5) and has slope 22 for
x , 2 and slope 20.5 for x . 2.
y
7
3
5
3
4
[21, 3] by 21, }}
(b) Yes, because both of the one-sided limits as x → 1 are
equal to f(1) 5 1.
y = f(x)
(c) No, because the left-hand derivative at x 5 1 is 11 and
the right-hand derivative at x 5 1 is 21.
54. (a) The function is continuous for all values of m, because
the right-hand limit as x → 0 is equal to f (0) 5 0 for
any value of m.
(b) The left-hand derivative at x 5 0 is 2 cos (2 ? 0) 5 2,
and the right-hand derivative at x 5 0 is m, so in order
for the function to be differentiable at x 5 0, m must
be 2.
55. (a) For all x Þ 0
7
x
63. The graph passes through (21, 2) and has slope 22 for
x , 1, slope 1 for 1 , x , 4, and slope 21 for 4 , x , 6.
y
7
(b) At x 5 0
(c) Nowhere
56. (a) For all x
y = f(x)
(b) Nowhere
(c) Nowhere
7
x
57. Note that lim2 f(x) 5 lim2 (2x 2 3) 5 23 and
x→0
x→0
lim1 f(x) 5 lim1 (x 2 3) 5 23. Since these values agree
x→0
x→0
with f(0), the function is continuous at x 5 0. On the other
hand,
f 9(x) 5
x 5 0.
64. i.
9
28
3
4
If f (x) 5 }}x 7/3 1 9, then f 9(x) 5 }}x 4/3 and
f 0(x) 5 x 1/3, which matches the given equation.
5
2, 21 # x , 0
1, 0 , x # 4
, so the derivative is undefined at
(a) [21, 0) < (0, 4]
3
4
contradicts the given equation f 0(x) 5 x 1/3.
(b) At x 5 0
(c) Nowhere in its domain
58. Note that the function is undefined at x 5 0.
(a) [22, 0) < (0, 2]
9
28
ii. If f 9(x) 5 }}x 7/3 2 2, then f 0(x) 5 }}x 4/3, which
(b) Nowhere
3
4
iii. If f 9(x) 5 }}x 4/3 1 6, then f 0(x) 5 x 1/3, which matches
the given equation.
124
Chapter 3 Review
64. continued
d
dx
(d) }} f(1 2 5 tan x) 5 f 9(1 2 5 tan x)(25 sec 2 x)
3
4
iv. If f (x) 5 }}x 4/3 2 4, then f 9(x) 5 x 1/3 and
At x 5 0, the derivative is
1
f 0(x) 5 }}x 22/3, which contradicts the given equation
3
f 0(x) 5 x 1/3.
152
1
f 9(1 2 5 tan 0)(25 sec 2 0) 5 f 9(1)(25) 5 }} (25)
5 21.
Answer is D: i and iii only could be true. Note,
d
f(x)
dx 2 1 cos x
(2 1 cos x)( f 9(x)) 2 ( f (x))(2sin x)
(2 1 cos x)
(e) }} }} 5 }}}}
2
however that i and iii could not simultaneously be true.
At x 5 0, the derivative is
(2 1 cos 0)(f 9(0)) 2 (f(0))(2sin 0)
3f 9(0)
2
5 }}
5 2}}.
}}}}
(2 1 cos 0)2
32
3
65. (a)
122
px
px p
5 10 sin }} (2f(x)f 9(x)) 1 10f (x) cos }} }}
1 22
1 2 21 2 2
px
d
dx
(f) }}[10 sin }} f 2(x)]
2
[21, 5] by [210, 80]
(b) t interval
px
2
At x 5 1, the derivative is
38 2 10
}} 5 56
0.5 2 0
58 2 38
}} 5 40
1 2 0.5
70 2 58
}} 5 24
1.5 2 1
74 2 70
}} 5 8
2 2 1.5
70 2 74
}} 5 28
2.5 2 2
58 2 70
}} 5 224
3 2 2.5
38 2 58
}} 5 240
3.5 2 3
10 2 38
}} 5 256
4 2 3.5
[0, 0.5]
[0.5, 1]
[1, 1.5]
[1.5, 2]
[2, 2.5]
[2.5, 3]
[3, 3.5]
[3.5, 4]
5 212.
d
dx
67. (a) }}[3f (x) 2 g(x)] 5 3f 9(x) 2 g9(x)
At x 5 21, the derivative is
3f 9(21) 2 g9(21) 5 3(2) 2 1 5 5.
d
dx
(b) }}[f 2(x)g 3(x)]
5 f 2(x) ? 3g 2(x)g9(x) 1 g 3(x) ? 2f(x)f 9(x)
5 f (x)g 2(x)[3f(x)g9(x) 1 2g(x)f 9(x)]
At x 5 0, the derivative is
f(0)g 2(0)[3f(0)g9(0) 1 2g(0)f 9(0)]
5 (21)(23)2[3(21)(4) 1 2(23)(22)]
5 29[212 1 12] 5 0.
1
g9(f(21))f 9(21) 5 g9(0)f 9(21) 5 (4)(2) 5 8.
Ï1w f 9(1) 1 }1} f (1) 5 1 }1} 1 }1} (23) 5 2}1}3 .
1
d
dx
(c) }} g(f(x)) 5 g9(f(x))f 9(x)
At x 5 21, the derivative is
66. (a) }}[Ïxw f (x)] 5 Ïxw f 9(x) 1 }} f(x)
dx
2Ïwx
At x 5 1, the derivative is
d
152
1
(d) Average velocity is a good approximation to velocity.
152 122
p
2
5 20(23) }} (1) 1 5p(23)2(0)
[21, 5] by [280, 80]
2Ïw1
p
2
20 f(1) f 9(1) sin }} 1 5p f 2(1) cos }}
(c)
d
px
2
5 20 f(x)f 9(x) sin }} 1 5p f 2(x) cos }}
avg. vel.
10
f 9(x)
wx)
w 5 }} f 9(x) 5 }}
(b) }} Ïf(
dx
f(x)
f (x)
2Ïw
w
2Ïw
w
f 9(0)
2
1
At x 5 0, the derivative is }} 5 2}} 5 2}}.
3
f (w0w)
2Ïw
2Ï9w
f 9(Ïxw)
d
d
(c) }} f(Ïxw) 5 f 9(Ïxw)}} Ïxw 5 }}
dx
dx
2Ïxw
1
}}
w) f 9(1)
f 9(Ï1
1
5
At x 5 1, the derivative is }} 5 }} 5 }
5 }}.
2
2
10
2Ï1
w
d
dx
(d) }} f(g(x)) 5 f 9(g(x))g9(x)
At x 5 21, the derivative is
f 9(g(21))g9(21) 5 f 9(21)g9(21) 5 (2)(1) 5 2.
d
f (x)
dx g(x) 1 2
(g(x) 1 2)f 9(x) 2 f(x) g9(x)
(g(x) 1 2)
(e) }} }} 5 }}}
2
At x 5 0, the derivative is
(g(0) 1 2)f 9(0) 2 f(0)g9(0)
(23 1 2)(22) 2 (21)(4)
5 }}}
}}}
(g(0) 1 2)2
(23 1 2)2
5 6.
Chapter 3 Review
d
dx
d
dx
(f) }} g(x 1 f(x)) 5 g9(x 1 f(x))}}(x 1 f(x))
dw
ds
p
4
t 5 }}. The velocity is given by
At x 5 0, the derivative is g9(0 1 f(0))[1 1 f 9(0)]
v(t) 5 210 sin t 1 }} , so the velocity at
5 g9(0 2 1)[1 1(22)] 5 (1)(21) 5 21
p
t 5 }} is 210 sin
4
p
speed at t 5 }} is
4
d
dr
d
ds
3
1
p
6
24
68. }} 5 }} }} 5 }}[sin (Ïrw 2 2)]}} 8 sin s 1 }}
3
43
1
1
p
24
1
2
p
At s 5 0, we have r 5 8 sin 0 1 }} 5 4 and so
6
dw
1
w 2 2)}} 8 cos 0 1 }p}
}} 5 cos (Ï4
ds
6
2Ï4w
cos 0
p
1 8Ïw3
5 }} 8 cos }} 5 }} }} 5 Ï3w
4
6
4
2
3
43 1
2 1 21 2
21
24
2
ds
d
dt
dt
d 2s
d
}}2 5 }}(64 2 32t) 5 232
dt
dt
ds
dt
ds
dt
ds
dt
d
dt
(d) Since }} 5 }}(64t 2 2.6t 2) 5 64 2 5.2t, the
1 5.2 2
64
The maximum height is s }} < 393.8 ft.
1 2
4
7
72. (a) Solving 160 5 490t 2, it takes }} sec.
2u 4(u 2 1 7)22/3
2u(u 2 1 7)22/3
dr
5 }}
}} 5 }}
3(22u 23 1 u 22)
3(u 2 2)
dt
160 5 280 cm/sec.
The average velocity is }
4
}}
7
At t 5 0, we may solve u 2t 1 u 5 1 to obtain u 5 1,
2(8)22/3
23
64
5.2
maximum height is reached at t 5 }} < 12.3 sec.
1
dr
}}(u 2 1 7)22/3(2u) 5 }} (22u 23 1 u 22)
3
dt
ds
dt
(b) Since v(t) 5 }} 5 980t, the velocity is
172
4
acceleration is 980 cm/sec 2.
70. (a) One possible answer:
2
x(t) 5 10 cos t 1 }} , y(t) 5 1
p
4
(b) s(0) 5 10 cos }} 5 5Ï2w
dv
dt
(980) }} = 560 cm/sec. Since a(t) 5 }} 5 980, the
1
6
and so }} 5 }} 5 }} 5 2}}.
dV
dx
d
dx
31
x
3
2 4
d
dx
31
1
3
24
73. }} 5 }} p 10 2 }} x 2 5 }} p 10x 2 2 }}x 3
5 p(20x 2 x 2)
1
x 2
40
2
3
20
1
1600
74. (a) r(x) 5 3 2 }} x 5 9x 2 }}x 2 1 }}x 3
(c) Farthest left:
p
4
2
When cos t 1 }} 5 21, we have s(t) 5 210.
(b) The marginal revenue is
3
10
3
1600
r9(x) 5 9 2 }}x 1 }}x 2
Farthest right:
1
p
4
71. (a) }} 5 }}(64t 2 16t 2) 5 64 2 32t
dr d
d
}}(u 2 1 7)1/3 5 }} }}(u 22 2 u 21)
dt du
du
1
1
(c) When t 5 0, }} 5 64, so the velocity is 64 ft/sec.
dr dt
dr
}} 5 }} }}
dt du
du
p
4
)210) 5 10. The acceleration is given
occurs at t 5 2 sec.
12u
u
1
2
p
}} 5 210, and the
2
(b) The maximum height is reached when }} 5 0, which
22
t 5 }}
2 u 21, and we may write:
2 5u
2(1)4(12 1 7)22/3
3(1 2 2)
p
4
p
p
t 5 }} is 210 cos }} 5 0.
4
2
69. Solving u 2t 1 u 5 1 for t, we have
dr
dt
1
by a(t) 5 210 cos t 1 }} , so the acceleration at
5 cos (Ïrw 2 2)}} 8 cos s 1 }}
6
2Ïrw
1
p
2
(d) Since cos }} 5 0, the particle first reaches the origin at
5 g9(x 1 f(x))(1 1 f 9(x))
dw dr
dr ds
125
p
4
2
When cos t 1 }} 5 1, we have s(t) 5 10.
3
1600
3
5 }}(x 2 40)(x 2 120),
1600
5 }}(x 2 2 160x 1 4800)
which is zero when x 5 40 or x 5 120. Since the bus
holds only 60 people, we require 0 # x # 60. The
marginal revenue is 0 when there are 40 people, and the
40 2
corresponding fare is p(40) 5 3 2 }} 5 $4.00.
1
40
2
126
Chapter 3 Review
74. continued
(c) One possible answer:
If the current ridership is less than 40, then the
proposed plan may be good. If the current ridership is
greater than or equal to 40, then the plan is not a good
idea. Look at the graph of y 5 r(x).
200
11e
78. (a) P(0) 5 }}5 < 1 student
200
200
1
(b) lim P(t) 5 lim }}
52t 5 }} 5 200 students
t→` 1 1 e
t→`
d
dt
(c) P9(t) 5 }} 200(1 1 e 52t)21
5 2200(1 1 e 52t)22(e 52t)(21)
200e 52t
(1 1 e )
5 }}
5 2t 2
[0, 60] by [250, 200]
(1 1 e52t)2(200e52t)(21) 2 (200e52t)(2)(1 1 e52t)(e52t)(21)
75. (a) Since x 5 tan u, we have
dx
du
}} 5 (sec 2 u)}} 5 20.6 sec 2 u. At point A, we have
dt
dt
dx
u 5 0 and }} 5 20.6 sec 2 0 5 20.6 km/sec.
dt
rad
sec
1 revolution
2p rad
60 sec
1 min
P0(t) 5}}}}}}}
(1 1 e52t)4
(1 1 e 52t)(2200e 52t) 1 400(e 52t)2
(1 1 e )
5 }}}}
52t 3
(200e 52t)(e 52t 2 1)
(1 1 e )
5 }}}
52t 3
18
p
(b) 0.6 }} ? }} ? }} = }} revolutions per
Since P0 5 0 when t 5 5, the critical point of y 5 P9(t)
minute or approximately 5.73 revolutions per minute.
occurs at t 5 5. To confirm that this corresponds to the
76. Let f(x) 5 sin (x 2 sin x). Then
maximum value of P9(t), note that P0(t) . 0 for t , 5
d
dx
f 9(x) 5 cos (x 2 sin x)}}(x 2 sin x)
and P0(t) , 0 for t . 5. The maximum rate occurs at
5 cos (x 2 sin x)(1 2 cos x). This derivative is zero when
cos (x 2 sin x) 5 0 (which we need not solve) or when
t 5 5, and this rate is
cos x 5 1,which occurs at x 5 2kp for integers k. For each
P9(5) 5 }}
0 2 5 }}
2 5 50 students per day.
of these values, f(x) 5 f(2kp) 5 sin (2kp 2 sin 2kp)
Note: This problem can also be solved graphically.
5 sin (2kp 2 0) 5 0. Thus, f(x) 5 f 9(x) 5 0 for x 5 2kp,
200e 0
(1 1 e )
200
2
79.
which means that the graph has a horizontal tangent at each
of these values of x.
1
1
1
!§1
1
!§§1
!§§2 1 !§§2 1 2
!§§2 1 !§§2 1 2
!§§2 1 !§2
!§§§
2
!§§2 1 !§§2
!§§
! §§
d 1
T
1
T d 1
1
T
}} 5 }} }} }} }} 5 2}}
}}
dr 2rl pd
2l pd dr r
2r 2l pd
d 1
T
1
T d 1
1
T
y9(l) 5 }} }} }} 5 }} }} }} }} 5 2}}2 }}
dl 2rl pd
2r pd dl l
2rl
pd
d 1
T
1
T d
y9(d) 5 }} }} }} 5 }} }} }}(d 21/2)
dd 2rl pd
2rl p dd
1
T
1
T
1
5 }} }} 2}}d 23/2 5 2}} }}3
2
2rl p
4rl pd
d 1
T
1
1 d
y9(T) 5 }} }} }} 5 }} }} }}(ÏT
w)
dT 2rl pd
2rl pd dT
1
1
1
1
5 }} }} }} 5 }}
2rl pd 2Ïw
T
4rlÏp
wdwT
w
77. y9(r) 5 }} }}
2
Since y9(r) , 0, y9(l) , 0, and y9(d) , 0, increasing r, l, or
d would decrease the frequency. Since y9(T) . 0,
increasing T would increase the frequency.
[2p, p] by [24, 4]
p
4
p p
(b) 2}}, }}
2 2
(a) x Þ k}}, where k is an odd integer
1
2
p
4
(c) Where it’s not defined, at x 5 k}}, k an odd integer
p
2
(d) It has period }} and continues to repeat the pattern seen
in this window.
Section 4.1
Quick Review 4.1
80. Use implicit differentiation.
1
21
d
1. f 9(x) 5 }} ? }}(4 2 x) 5 }}
2wx dx
2wx
2Ï4
ww
2Ïw4w
x2 2 y2 5 1
d
d
d
}}(x 2) 2 }}(y 2) 5 }}(1)
dx
dx
dx
3
4
2. f 9(x) 5 }}x21/4
2x 2 2yy9 5 0
d
dx
d
dx
3. f 9(x) 5 }}2(9 2 x 2)21/2 5 2(9 2 x 2)23/2 ? }}(9 2 x 2)
2x
x
y9 5 }} 5 }}
2y
y
d x
y0 5 }} }}
dx y
(y)(1) 2 (x)(y9)
5 }}
y2
2x
(9 2 x )
5 2(9 2 x 2)23/2(22x) 5 }}
2 3/2
1
3
1
22x
5 2}}(x 2 2 1)24/3(2x) 5 }
}
3
3(x 2 2 1)4/3
d
dx
d
dx
4. f 9(x) 5 }}(x 2 2 1)21/3 5 2}}(x 2 2 1)24/3 ? }}(x 2 2 1)
1y2
x
y 2 x }}
1
x 11
2x
x 11
d
dx
2
5. g9(x) 5 }
2 } ? }}(x 1 1) 5 }
2 }
5}
2
y
y2 2 x2
y
sin (ln x)
x
d
dx
6. g9(x) 5 2sin (ln x) ? }} ln x 5 2}}
5 }}
3
1
y
5 2}}3
d
dx
7. h9(x) 5 e 2x ? }}2x 5 2e 2x
(since the given equation is x 2 2 y 2 5 1)
d 2y
127
1
1
1
At (2, Ï3w), }}2 5 2}}3 5 2}} 5 2}}.
dx
y
(Ï3w)3
3Ï3w
Chapter 4
Applications of Derivatives
d
dx
d
dx
8. h9(x) 5 }}e ln x 5 }}x 5 1
9. As x → 32, Ï9ww
2wx 2w → 01. Therefore, lim2 f (x) 5 `.
x→3
10. As x → 231, Ï9ww
2wx 2w → 01. Therefore, lim 1 f (x) 5 `.
x→23
■ Section 4.1 Extreme Values of Functions
(pp. 177– 185)
Exploration 1
d
dx
11. (a) }}(x 3 2 2x) 5 3x 2 2 2
f 9(1) 5 3(1)2 2 2 5 1
Finding Extreme Values
1. From the graph we can see that there are three critical
points: x 5 21, 0, 1.
Critical point values: f (21) 5 0.5, f (0) 5 0, f (1) 5 0.5
Endpoint values: f (22) 5 0.4, f (2) 5 0.4
Thus f has absolute maximum value of 0.5 at x 5 21 and
x 5 1, absolute minimum value of 0 at x 5 0, and local
minimum value of 0.4 at x 5 22 and x 5 2.
d
dx
(b) }}(x 1 2) 5 1
f 9(3) 5 1
(c) Left-hand derivative:
[(2 1 h)3 2 2(2 1 h)] 2 4
f (2 1 h) 2 f (2)
h
h
h→0
h→0
h 3 1 6h 2 1 10h
5 lim2 }}
h
h→0
lim2 }} 5 lim2 }}}
5 lim2 (h 2 1 6h 1 10)
h→0
5 10
[22, 2] by [21, 1]
2. The graph of f 9 has zeros at x 5 21 and x 5 1 where the
graph of f has local extreme values. The graph of f 9 is not
defined at x 5 0, another extreme value of the graph of f.
Right-hand derivative:
f (2 1 h) 2 f (2)
h
[(2 1 h) 1 2] 2 4
h
lim }} 5 lim1 }}
h→01
h→0
h
h
5 lim1 }}
h→0
5 lim1 1
h→0
[22, 2] by [21, 1]
)x)
d
3. Using the chain rule and }} )x) 5 }}, we find
x
dx
)x)
df
1 2 x2
}} 5 }} ? }
}.
x (x 2 1 1)2
dx
( )
51
Since the left- and right-hand derivatives are not equal,
f 9(2) is undefined.
128
Section 4.1
12. (a) The domain is x Þ 2. (See the solution for 11.(c)).
3x 2 2 2, x , 2
(b) f 9(x) 5
x.2
1,
h
14. The first derivative k9(x) 5 22xe2x has a zero at x 5 0.
2
Since the domain has no endpoints, any extreme value must
occur at x 5 0. Since k(0) 5 e20 5 1 and lim k(x) 5 0,
2
Section 4.1 Exercises
x→6`
1. Maximum at x 5 b, minimum at x 5 c2;
The Extreme Value Theorem applies because f is
continuous on [a, b], so both the maximum and minimum
exist.
the maximum value is 1 at x 5 0.
p
5p
x 5 }}, x 5 }}.
4
4
2. Maximum at x 5 c, minimum at x 5 b;
The Extreme Value Theorem applies because f is
continuous on [a, b], so both the maximum and minimum
exist.
Critical point values: x 5 }}
3. Maximum at x 5 c, no minimum;
The Extreme Value Theorem does not apply, because the
function is not defined on a closed interval.
Endpoint values:
4. No maximum, no minimum;
The Extreme Value Theorem does not apply, because the
function is not continuous or defined on a closed interval.
5. Maximum at x 5 c, minimum at x 5 a;
The Extreme Value Theorem does not apply, because the
function is not continuous.
6. Maximum at x 5 a, minimum at x 5 c;
The Extreme Value Theorem does not apply since the
function is not continuous.
7. Local minimum at (21, 0), local maximum at (1, 0)
p
4
1
2
15. The first derivative f 9(x) 5 cos x 1 }} , has zeros at
p
4
5p
x 5 }}
4
f (x) 5 1
x50
f (x) 5 }}
Ï2w
f (x) 5 0
f (x) 5 21
1
7p
4
p
Maximum value is 1 at x 5 }};
4
5p
minimum value is 21 at x 5 }};
4
1
local minimum at 0, }} ;
Ïw2
7p
local maximum at }}, 0
4
x 5 }}
1
1
2
2
16. The first derivative g9(x) 5 sec x tan x has zeros at x 5 0
p
2
8. Minima at (22, 0) and (2, 0), maximum at (0, 2)
and x 5 p and is undefined at x 5 }}. Since g(x) 5 sec x is
9. Maximum at (0, 5) Note that there is no minimum since the
endpoint (2, 0) is excluded from the graph.
also undefined at x 5 }}, the critical points occur only at
10. Local maximum at (23, 0), local minimum at (2, 0),
maximum at (1, 2), minimum at (0, 21)
1
1
11. The first derivative f 9(x) 5 2}}2 1 }} has a zero at x 5 1.
x
x
Critical point value: f (1) 5 1 1 ln 1 5 1
Endpoint values: f (0.5) 5 2 1 ln 0.5 < 1.307
1
f (4) 5 }} 1 ln 4 < 1.636
4
1
Maximum value is }} 1 ln 4 at x 5 4;
4
1
2
12. The first derivative g9(x) 5 2e
only consider the endpoints.
g(21) 5 e 2(21) 5 e
has no zeros, so we need
1
e
g(1) 5 e21 5 }}
Maximum value is e at x 5 21;
1
e
minimum value is }} at x 5 1.
1
13. The first derivative h9(x) 5 }} has no zeros, so we need
x11
only consider the endpoints.
h(0) 5 ln 1 5 0
h(3) 5 ln 4
Maximum value is ln 4 at x 5 3;
minimum value is 0 at x 5 0.
Critical point values:
x50
x5p
g(x) 5 1
g(x) 5 21
Since the range of g(x) is (2`, 21] < [1, `), these values
must be a local minimum and local maximum, respectively.
Local minimum at (0, 1); local maximum at (p, 21)
2
5
17. The first derivative f 9(x) 5 }}x23/5 is never zero but is
Critical point value: x 5 0
f (x) 5 0
Endpoint value:
x 5 23 f (x) 5 (23)2/5
5 32/5 < 1.552
local maximum at }}, 2 2 ln 2
2x
x 5 0 and x 5 p.
undefined at x 5 0.
minimum value is 1 at x 5 1;
12
p
2
Since f (x) . 0 for x Þ 0, the critical point at x 5 0 is a
local minimum, and since f (x) # (23)2/5 for 23 # x , 1,
the endpoint value at x 5 23 is a global maximum.
Maximum value is 32/5 at x 5 23;
minimum value is 0 at x 5 0.
3
5
18. The first derivative f 9(x) 5 }}x22/5 is never zero but is
undefined at x 5 0.
Critical point value: x 5 0
Endpoint value:
x53
f (x) 5 0
f (x) 5 33/5 < 1.933
Since f (x) , 0 for x , 0 and f (x) . 0 for x . 0, the
critical point is not a local minimum or maximum. The
maximum value is 33/5 at x 5 3.
Section 4.1
19.
129
24.
[22, 6] by [22, 4]
[24.7, 4.7] by [23.1, 3.1]
Minimum value is 1 at x 5 2.
To confirm that there are no “hidden” extrema, note that
22x
(x 2 1)
20.
y9 5 2(x 2 2 1)22(2x) 5 }
2 }
2 which is zero only at
x 5 0 and is undefined only where y is undefined. There is
a local maximum at (0, 21).
25.
[26, 6] by [22, 7]
To find the exact values, note that y9 5 3x 2 2 2, which is
!§3
2
4Ï6w
12!}§3}, 4 1 }9}2 < (20.816, 5.089); local minimum at
2
4Ïw6
1!}§3}, 4 2 }9}2 < (0.816, 2.911)
2
zero when x 5 6 }}. Local maximum at
[21.5, 1.5] by [20.5, 3]
The minimum value is 1 at x 5 0.
26.
21.
[24.7, 4.7] by [23.1, 3.1]
The actual graph of the function has asymptotes at
x 5 61, so there are no extrema near these values. (This is
an example of grapher failure.) There is a local
minimum at (0, 1).
[26, 6] by [25, 20]
To find the exact values, note that
y9 5 3x 2 1 2x 2 8 5 (3x 2 4)(x 1 2), which is zero when
4
3
27.
x 5 22 or x 5 }}. Local maximum at (22, 17);
13
4
41
27
2
local minimum at }}, 2}}
22.
[24.7, 4.7] by [23.1, 3.1]
Maximum value is 2 at x 5 1;
minimum value is 0 at x 5 21 and at x 5 3.
28.
[26, 6] by [24, 4]
Note that y9 5 3x 2 2 6x 1 3 5 3(x 2 1)2, which is zero at
x 5 1. The graph shows that the function assumes lower
values to the left and higher values to the right of this point,
so the function has no local or global extreme values.
[24, 4] by [280, 30]
115
2
Minimum value is 2}} at x 5 23;
23.
local maximum at (0, 10);
1
13
2
2
local minimum at 1, }}
[24, 4] by [22, 4]
29.
Minimum value is 0 at x 5 21 and at x 5 1.
[25, 5] by [20.7, 0.7]
1
2
Maximum value is }} at x 5 1;
1
2
minimum value is 2}} at x 5 21.
130
Section 4.1
30.
36. Note that f (x) 5
hx2x219x,9x,
Therefore, f 9(x) 5
[25, 5] by [20.8, 0.6]
3
3
x # 23 or 0 # x , 3
23 , x , 0 or x $ 3.
h3x23x219, 9,
x , 23 or 0 , x , 3
23 , x , 0 or x . 3.
2
2
(a) No, since the left- and right-hand derivatives at x 5 0
are 29 and 9, respectively.
1
2
Maximum value is }} at x 5 0;
(b) No, since the left- and right-hand derivatives at x 5 3
are 218 and 18, respectively.
1
2
minimum value is 2}} at x 5 22.
31.
(c) No, since the left- and right-hand derivatives at x 5 23
are 218 and 18, respectively.
(d) The critical points occur when f 9(x) 5 0
(at x 5 6Ï3w) and when f 9(x) is undefined (at x 5 0 or
x 5 63). The minimum value is 0 at x 5 23, at x 5 0,
[26, 6] by [0, 12]
Maximum value is 11 at x 5 5;
minimum value is 5 on the interval [23, 2];
local maximum at (25, 9)
32.
and at x 5 3; local maxima occur at (2Ï3w, 6Ï3w) and
(Ï3w, 6Ï3w).
37.
[24, 4] by [23, 3]
[23, 8] by [25, 5]
2
33.
crit. pt.
4
5
x 5 2 }}
x50
[26, 6] by [26, 6]
Maximum value is 5 on the interval [3, `);
minimum value is 25 on the interval (2`, 22].
5x 1 4
y9 5 x2/3(1) 1 }}x21/3(x 1 2) 5 }3}
3
3Ïxw
Maximum value is 4 on the interval [5, 7];
minimum value is 24 on the interval [22, 1].
derivative extremum
0
value
12
25
local max }}101/3 < 1.034
undefined local min
0
38.
34.
[24, 4] by [23, 3]
8x 2 2 8
2
y9 5 x2/3(2x) 1 }}x21/3(x 2 2 4) 5 }3}
3
3Ïwx
[26, 6] by [0, 9]
Minimum value is 4 on the interval [21, 3]
2
35. (a) No, since f 9(x) 5 }}(x 2 2)21/3, which is undefined at
3
x 5 2.
(b) The derivative is defined and nonzero for all x Þ 2.
Also, f (2) 5 0 and f (x) . 0 for all x Þ 2.
(c) No, f (x) need not not have a global maximum because
its domain is all real numbers. Any restriction of f to a
closed interval of the form [a, b] would have both a
maximum value and a minimum value on the interval.
(d) The answers are the same as (a) and (b) with 2 replaced
by a.
crit. pt. derivative extremum value
x 5 21
x50
x51
0
minimum
undefined local max
0
minimum
23
0
23
131
Section 4.1
39.
42.
[22.35, 2.35] by [23.5, 3.5]
[24, 4] by [21, 6]
y9 5
1
y9 5 x ? }}(22x) 1 (1)Ï4ww
2wx 2w
2wx 2w
2Ï4
ww
2x 2 1 (4 2 x2)
4 2 2x 2
x,0
x.0
crit. pt. derivative
5 }} 5 }}
2wx 2w
2wx w2
Ï4ww
Ï4ww
crit. pt.
derivative extremum value
x 5 22
undefined local max
0
minimum
22
x 5 Ï2w
0
maximum
2
undefined local min
0
extremum value
x50
undefined
local min
3
x51
0
local max
4
43.
0
x 5 2Ï2w
x52
h21,
2 2 2x,
[24, 6] by [22, 6]
y9 5
40.
22x 2 2,
h22x
1 6,
x,1
x.1
crit. pt. derivative extremum value
x 5 21
x51
[24.7, 4.7] by [21, 5]
2x 1 4x(3 2 x)
0
5
1
x53
1
y 5 x 2 ? }}(21) 1 2xÏ3ww
2wx
2wx
2Ï3
ww
2
maximum
undefined local min
0
maximum
5
44.
25x 1 12x
2
5 }} 5 }}
2w
x
2Ï3
2wx
2Ï3
ww
ww
crit. pt.
derivative extremum
value
x50
0
minimum
0
12
5
0
local max
144
}}151/2 < 4.462
125
x 5 }}
x53
undefined minimum
0
[24, 6] by [25, 5]
We begin by determining whether f 9(x) is defined at x 5 1,
where
f (x) 5
41.
h
1
4
1
2
15
4
2}}x 2 2 }}x 1 }},
x#1
x 3 2 6x 2 1 8x,
x.1
Left-hand derivative:
[24.7, 4.7] by [0, 6.2]
y9 5
h22,
1,
x,1
x.1
crit. pt. derivative
x51
undefined
1
1
15
2}}(1 1 h)2 2 }}(1 1 h) 1 }} 2 3
4
2
4
f (1 1 h) 2 f (1)
lim2 }} 5 lim2 }}}}
h
h
h→0
h→0
2h 2 2 h
5 lim2 }}
4h
h→0
1
5 lim2 }}(2h 2 4h)
h→0 4
5 21
extremum value
minimum
2
Right-hand derivative:
f (1 1 h) 2 f (1)
h
(1 1 h)3 2 6(1 1 h)2 1 8(1 1 h) 2 3
5 lim1 }}}}
h
h→0
h 3 2 3h 2 2 h
5 lim1 }}
h
h→0
lim }}
h→01
5 lim1 (h 2 2 3h 2 1)
h→0
5 21
Thus f 9(x) 5
h
1
2
1
2
2}}x 2 }},
x#1
3x 2 2 12x 1 8,
x.1
132
Section 4.2
44. continued
1
2
1
2
Note that 2}}x 2 }} 5 0 when x 5 21, and
12 6 Ï1
w2w2w2
ww4(3
w)(
w8w)w
3x 2 2 12x 1 8 5 0 when x 5 }}}
2(3)
12 6 Ï4w8w
2Ï3w
5 }} 5 2 6 }}.
6
[23, 3] by [25, 5]
3
2Ïw3
But 2 2 }} < 0.845 , 1, so the only critical points
3
2Ïw3
occur at x 5 21 and x 5 2 1 }} < 3.155.
3
crit. pt.
derivative extremum
value
x 5 21
0
local max
x < 3.155
0
local max < 23.079
4
The function f (x) 5 x 3 1 x has no critical points.
(b) The function can have either two local extreme values
or no extreme values. (If there is only one critical point,
the cubic function has no extreme values.)
52. (a) By the definition of local maximum value, there is an
open interval containing c where f (x) # f (c),
so f (x) 2 f (c) # 0.
(b) Because x → c 1,we have (x 2 c) . 0, and the sign of
the quotient must be negative (or zero). This means the
limit is nonpositive.
45. Graph (c), since this is the only graph that has positive
slope at c.
(c) Because x → c 2, we have (x 2 c) , 0, and the sign of
the quotient must be positive (or zero). This means the
limit is nonnegative.
46. Graph (b), since this is the only graph that represents a
differentiable function at a and b and has negative slope
at c.
(d) Assuming that f 9(c) exists, the one-sided limits in (b)
and (c) above must exist and be equal. Since one is
nonpositive and one is nonnegative, the only possible
common value is 0.
(e) There will be an open interval containing c where
f (x) 2 f (c) $ 0. The difference quotient for the
left-hand derivative will have to be negative (or zero),
and the difference quotient for the right-hand derivative
will have to be positive (or zero). Taking the limit, the
left-hand derivative will be nonpositive, and the
right-hand derivative will be nonnegative. Therefore,
the only possible value for f 9(c) is 0.
47. Graph (d), since this is the only graph representing a
function that is differentiable at b but not at a.
48. Graph (a), since this is the only graph that represents a
function that is not differentiable at a or b.
49. (a) V(x) 5 160x 2 52x 2 1 4x 3
V9(x) 5 160 2 104x 1 12x 2 5 4(x 2 2)(3x 2 20)
The only critical point in the interval (0, 5) is at x 5 2.
The maximum value of V(x) is 144 at x 5 2.
(b) The largest possible volume of the box is 144 cubic
units, and it occurs when x 5 2.
50. (a) P9(x) 5 2 2 200x 22
The only critical point in the interval (0, `) is at
x 5 10. The minimum value of P(x) is 40 at x 5 10.
53. (a)
(b) The smallest possible perimeter of the rectangle is
40 units and it occurs at x 5 10, which makes the
rectangle a 10 by 10 square.
[20.1, 0.6] by [21.5, 1.5]
51. (a) f 9(x) 5 3ax 1 2bx 1 c is a quadratic, so it can have
0, 1, or 2 zeros, which would be the critical points of f.
Examples:
2
f (0) 5 0 is not a local extreme value because in any
open interval containing x 5 0, there are infinitely
many points where f (x) 5 1 and where f (x) 521.
(b) One possible answer, on the interval [0, 1]:
f (x) 5
h
1
12x
(1 2 x) cos }},
0,
0#x,1
x51
This function has no local extreme value at
x 5 1. Note that it is continuous on [0, 1].
[23, 3] by [25, 5]
The function f (x) 5 x 2 3x has two critical points at
x 5 21 and x 5 1.
3
■ Section 4.2 Mean Value Theorem
(pp. 186–194)
Quick Review 4.2
[23, 3] by [25, 5]
The function f (x) 5 x 3 2 1 has one critical point at
x 5 0.
1.
2x 2 2 6 , 0
2x 2 , 6
x2 , 3
2Ïw3 , x , Ï3w
Interval: (2Ï3w, Ï3w)
Section 4.2
2.
3x 2 2 6 . 0
3x 2 . 6
x2 . 2
x , 2Ï2w or x . Ï2w
Intervals: (2`, 2Ï2w) < (Ï2w, `)
2
x
3. (a) h9(x) 5 2}}2
Since h9(x) is never zero and is undefined only where
h(x) is undefined, there are no critical points. Also, the
domain (2`, 0) < (0, `) has no endpoints. Therefore,
h(x) has no local extrema.
8 2 2x 2 $ 0
8 $ 2x 2
4 $ x2
22 # x # 2
The domain is [22, 2].
3. Domain:
(b) Since h9(x) is never positive, h(x) is not increasing on
any interval.
(c) Since h9(x) , 0 on (2`, 0) < (0, `), h(x) is decreasing
on (2`, 0) and on (0, `).
4. f is continuous for all x in the domain, or, in the interval
[22, 2].
5. f is differentiable for all x in the interior of its domain, or,
in the interval (22, 2).
6. We require x 2 2 1 Þ 0, so the domain is x Þ 61.
7. f is continuous for all x in the domain, or, for all x Þ 61.
8. f is differentiable for all x in the domain, or, for all x Þ 61.
(b) Since f 9(x) is always positive, f (x) is increasing on
(2`, `).
(c) Since f 9(x) is never negative, f (x) is not decreasing on
any interval.
1. (a) f 9(x) 5 5 2 2x
6. (a) f 9(x) 5 20.5e 20.5x
1 22
2
5
f 9(x) , 0 on 1}}, `2, we know that f (x) has a local
2
5
5
25
maximum at x 5 }}. Since f 1}}2 5 }}, the local
2
2
4
5 25
maximum occurs at the point 1}}, }}2. (This is also a
2 4
5
5
Since f 9(x) . 0 on 2`, }} , f 9(x) 5 0 at x 5 }}, and
global maximum.)
1
5
2
2
12 2
32 2
5
5
(c) Since f 9(x) , 0 on }}, ` , f (x) is decreasing on }}, ` .
2. (a) g9(x) 5 2x 2 1
1
1 2
1
2
2
1
2
Since g9(x) , 0 on 2`, }} , g9(x) 5 0 at x 5 }}, and
1
g9(x) . 0 on }}, ` , we know that g(x) has a local
2
1
minimum at x 5 }}.
2
1
49
Since g }} 5 2}}, the local minimum occurs at the
2
4
1
49
point }}, 2}} . (This is also a global minimum.)
2
4
1
2
12 2
32 2
1
1
(b) Since g9(x) . 0 on }}, ` , g(x) is increasing on }}, ` .
1
1
2
2
(c) Since g9(x) , 0 on 2`, }} , g(x) is decreasing on
12`, }2}4.
1
Since f 9(x) is never zero or undefined, and the domain
of f (x) has no endpoints, f (x) has no extrema.
(b) Since f 9(x) is never positive, f (x) is not increasing on
any interval.
(c) Since f 9(x) is always negative, f (x) is decreasing on
(2`, `).
1
(b) Since f 9(x) . 0 on 2`, }} , f (x) is increasing on
12
(b) Since k9(x) . 0 on (2`, 0), k(x) is increasing on
(2`, 0).
Since f 9(x) is never zero or undefined, and the domain
of f (x) has no endpoints, f (x) has no extrema.
Section 4.2 Exercises
4
Since k9(x) is never zero and is undefined only where
k(x) is undefined, there are no critical points. Also, the
domain (2`, 0) < (0, `) has no endpoints. Therefore,
k(x) has no local extrema.
5. (a) f 9(x) 5 2e 2x
10. 21 5 (1)2 1 2(1) 1 C
21 5 3 1 C
C 5 24
1
2
x
4. (a) k9(x) 5 2}}3
(c) Since k9(x) , 0 on (0, `), k(x) is decreasing on (0, `).
9. 7 5 22(22) 1 C
7 541C
C 53
5
2`, }} .
2
133
7. (a) y9 5 2}}
2Ïxw1
ww2
In the domain [22, `), y9 is never zero and is
undefined only at the endpoint x 5 22. The function y
has a local maximum at (22, 4). (This is also a global
maximum.)
(b) Since y9 is never positive, y is not increasing on any
interval.
(c) Since y9 is negative on (22, `), y is decreasing on
[22, `).
8. (a) y9 5 4x 3 2 20x 5 4x(x 1 Ï5w)(x 2 Ï5w)
The function has critical points at x 5 2Ï5w, x 5 0,
and x 5 Ï5w. Since y9 , 0 on (2`, 2Ï5
w) and
(0, Ï5w) and y9 . 0 on (2Ï5w, 0) and (Ï5w, `), the
points at x 5 6Ïw5 are local minima and the point at
x 5 0 is a local maximum. Thus, the function has a
local maximum at (0, 9) and local minima at
(2Ïw5, 216) and (Ïw5, 216). (These are also global
minima.)
(b) Since y9 . 0 on (2Ï5w, 0) and (Ï5w, `), y is increasing
on [2Ï5w, 0] and [Ï5w, `).
w), y is
(c) Since y9 , 0 on (2`, 2Ï5w) and (0, Ï5
decreasing on (2`, 2Ï5w] and [0, Ï5w].
134
Section 4.2
(b) Since h9(x) . 0 on (2`, 22) and (2, `), h(x) is
increasing on (2`, 22] and [2, `).
9.
(c) Since h9(x) , 0 on (22, 2), h(x) is decreasing on
[22, 2].
12.
[24.7, 4.7] by [23.1, 3.1]
1
(a) f 9(x) 5 x ? }}(21) 1 Ï4ww
2wx
2wx
2Ï4
ww
23x 1 8
5 }}
2wx
2Ïw4w
8
The local extrema occur at the critical point x 5 }} and
[24.7, 4.7] by [23.1, 3.1]
(x 2 2 4)(1) 2 x(2x)
(x 2 4)
at the endpoint x 5 4. There is a local (and absolute)
1
Since k9(x) is never zero and is undefined only where
k(x) is undefined, there are no critical points. Since
there are no critical points and the domain includes no
endpoints, k(x) has no local extrema.
2
8 16
maximum at }}, }} or approximately (2.67, 3.08),
3 3Ïw
3
and a local minimum at (4, 0).
1
8
3
(b) Since k9(x) is never positive, k(x) is not increasing on
any interval.
2
(b) Since f 9(x) . 0 on 2`, }} , f (x) is increasing on
1
4
8
2`, }} .
3
(c) Since k9(x) is negative wherever it is defined, k(x) is
decreasing on each interval of its domain: on
(2`, 22), (22, 2), and (2, `).
13 2
8
(c) Since f 9(x) , 0 on }}, 4 , f (x) is decreasing on
3 4
8
}}, 4 .
3
x2 1 4
(x 2 4)
(a) k9(x) 5 }}}
5 2}
2
2
2 }
2
3
13.
10.
[24, 4] by [26, 6]
(a) f 9(x) 5 3x 2 2 2 1 2 sin x
Note that 3x 2 2 2 . 2 for )x) $ 1.2 and )2 sin x) # 2 for
all x, so f 9(x) . 0 for )x) $ 1.2. Therefore, all critical
points occur in the interval (21.2, 1.2), as suggested by
the graph. Using grapher techniques, there is a local
maximum at approximately (21.126, 20.036), and a
local minimum at approximately (0.559, 22.639).
[25, 5] by [215, 15]
4x 1 8
3x
1
3
(a) g9(x) 5 x 1/3(1) 1 }}x 22/3(x 1 8) 5 }}
2/3
The local extrema can occur at the critical points
x 5 22 and x 5 0, but the graph shows that no extrema
(b) f (x) is increasing on the intervals (2`, 21.126] and
[0.559, `), where the interval endpoints are
approximate.
occurs at x 5 0. There is a local (and absolute)
3
minimum at (22, 26Ï2w) or approximately
(22, 27.56).
(b) Since g9(x) . 0 on the intervals (22, 0) and (0, `), and
g(x) is continuous at x 5 0, g(x) is increasing on
[22, `).
(c) f (x) is decreasing on the interval [21.126, 0.559],
where the interval endpoints are approximate.
14.
(c) Since g9(x) , 0 on the interval (2`, 22), g(x) is
decreasing on (2`, 22].
11.
[26, 6] by [212, 12]
(a) g9(x) 5 2 2 sin x
Since 1 # g9(x) # 3 for all x, there are no critical
points. Since there are no critical points and the domain
has no endpoints, there are no local extrema.
[25, 5] by [20.4, 0.4]
(x 2 1 4)(21) 2 (2x)(2x)
(x 1 4)
(x 1 2)(x 2 2)
5}
}
(x 2 1 4)2
(b) Since g9(x) . 0 for all x, g(x) is increasing on (2`, `).
x2 2 4
(x 1 4)
(a) h9(x) 5 }}}
5}
2
2
2 }
2
(c) Since g9(x) is never negative, g(x) is not decreasing on
any interval.
The local extrema occur at the critical points, x 5 62.
1
1
4
2
There is a local (and absolute) maximum at 22, }}
1
2
1
and a local (and absolute) minimum at 2, 2}} .
4
Section 4.2
15. (a) f is continuous on [0, 1] and differentiable on (0, 1).
(b)
20. (a) The secant line passes through (1, f (1)) 5 (1, 0) and
f (1) 2 f (0)
120
2 2 (21)
2c 1 2 5 }}
1
(3, f (3)) 5 (3, Ï2w), so its slope is
f 9(c) 5 }}
Ïw2 2 0 Ïw2
1
}} 5 }} 5 }}.
321
2
Ï2w
1
The equation is y 5 }}(x 2 1) 1 0
Ïw2
1
1
or y 5 }}x 2 }}, or y < 0.707x 2 0.707.
Ïw2
Ïw2
2c 5 1
1
2
c 5 }}
16. (a) f is continuous on [0, 1] and differentiable on (0, 1).
(b)
f (1) 2 f (0)
120
120
5 }}
1
3
5 }}
2
3 23
5 }}
2
8
5 }}
27
f 9(c) 5 }}
2
}}c 21/3
3
c 21/3
c
c
135
1
(b) We need to find c such that f 9(c) 5 }}.
Ïw2
1
1
}} 5 }}
2Ïw
c2
ww1
Ï2w
2Ïcw2
ww1 5 Ï2w
1
2
3
c 5 }}
2
c 2 1 5 }}
12
1 2 2 !}§2} 5 }Ï}2w
3
f (c) 5 f }} 5
17. (a) f is continuous on [21, 1] and differentiable on
(21, 1).
1
1
1
(b)
The tangent line has slope }} and passes through
Ïw2
3 1
1
3
1
}}, }} . Its equation is y 5 }} x 2 }} 1 }} or
2 Ïw2
2
Ï2w
Ï2w
1
1
y 5 }}x 2 }}, or y < 0.707x 2 0.354.
2Ïw2
Ïw2
f (1) 2 f (21)
f 9(c) 5 }}
1 2 (21)
1
p
p
}} 2 2}}
2
2
1 2
1
}} 5 }}
2
2wc 2w
Ïw1w
2
Ï1ww
2wc 2w 5 }}
p
4
1 2 c 5 }}2
p
2
2
1
1
3
21. (a) Since f 9(x) 5 }}x 22/3, f is not differentiable at x 5 0.
(b)
4
c 5 1 2 }}2
p
2
!§§§p§
4
c 5 6 1 2 }}2 < 60.771
[21, 1] by [21, 1]
18. (a) f is continuous on [2, 4] and differentiable on (2, 4).
(b)
f (4) 2 f (2)
422
ln 3 2 ln 1
5 }}
2
2
5 }}
ln 3
2
5 1 1 }} < 2.820
ln 3
f 9(c) 5 }}
1
}}
c21
c21
c
19. (a) The secant line passes through (0.5, f (0.5)) 5 (0.5, 2.5)
and (2, f(2)) 5 (2, 2.5), so its equation is y 5 2.5.
(b) The slope of the secant line is 0, so we need to find c
such that f 9(c) 5 0.
1 2 c 22
c 22
c
f (c)
50
51
51
5 f (1) 5 2
The tangent line has slope 0 and passes through (1, 2),
so its equation is y 5 2.
2
(c)
f (1) 2 f (21)
1 2 (21)
1 22/3
1 2 (21)
5 }}
}}c
3
2
1 22/3
51
}}c
3
f 9(c) 5 }}
c22/3 5 3
c 5 6323/2 < 0.192
136
Section 4.2
22. (a) Since f 9(x) 5
h
21,
1,
0#x,1
3$x.1
(b)
,
f is not differentiable at x 5 1. (If f were differentiable
at x 5 1, it would violate the Intermediate Value
Theorem for Derivatives.)
[2p, p] by [21, 2]
(c) Note that f 9(x) 5
(b)
h
2sin x, 2p # x , 0
.
cos x,
0,x#p
f (p) 2 f (2p)
p 2 (2p)
1 2 (21)
2p
1
p
We require f 9(c) 5 }} 5 }} 5 }}.
1
p
For 2p , c , 0, this occurs when 2sin c 5 }}, so
[0, 3] by [21, 3]
1p2
1
c 5 2sin21 }} < 20.324 or
f (3) 2 f (0)
221
1
(c) We require f 9(c) 5 }} 5 }} 5 }}, but
320
3
3
f 9(x) 5 61 for all x where f 9(x) is defined. Therefore,
h1,21,
1
1
p
possible values of c are approximately
21 # x , 0
,
1$x.0
f is not differentiable at x 5 0. (If f were differentiable
at x 5 1, it would violate the Intermediate Value
Theorem for Derivatives.)
22.818, 20.324, and 1.247.
x2
2
25. f (x) 5 }} 1 C
26. f (x) 5 2x 1 C
27. f (x) 5 x 3 2 x 2 1 x 1 C
(b)
28. f (x) 5 2cos x 1 C
29. f (x) 5 e x 1 C
30. f (x) 5 ln (x 2 1) 1 C
31.
[21, 1] by [21, 2]
f (1) 2 f (21)
1 2 (21)
1
}} 1 C 5 1
2
1
C 5 }}
2
1
1
f (x) 5 }} 1 }}, x . 0
x
2
f 9(x) 5 61 for all x where f 9(x) is defined. Therefore,
there is no such value of c.
24. (a) We test for differentiability at x 5 0, using the limits
32.
f (x) 5 x 1/4 1 C
f (1) 5 22
11/4 1 C 5 22
1 1 C 5 22
C 5 23
f (x) 5 x 1/4 2 3
33.
f (x)
f (21)
ln (21 1 2) 1 C
01C
C
f (x)
34.
f (x)
f (0)
01C
C
f (x)
given in Section 3.5.
Left-hand derivative:
f (0 1 h) 2 f (0)
h
cos h 2 1
h
lim }} 5 lim2 }} 5 0
h→0
Right-hand derivative:
f(0 1 h) 2 f(0)
h
(1 1 sin h) 2 1
h
sin h
5 lim1 }}
h
h→0
lim }} 5 lim1 }}
h→01
h→0
51
Since the left- and right-hand derivatives are not equal,
f is not differentiable at x 5 0.
1
x
f (x) 5 }} 1 C, x . 0
f (2) 5 1
020
2
(c) We require f 9(c) 5 }} 5 }} 5 0, but
h→02
1p2
1
occurs when cos c 5 }}, so c 5 cos21 }} < 1.247. The
there is no such value of c.
23. (a) Since f 9(x) 5
1p2
c 5 2p 1 sin21 }} < 22.818. For 0 , c , p, this
5 ln (x 1 2) 1 C
53
53
53
53
5 ln (x 1 2) 1 3
5 x 2 1 x 2 sin x 1 C
53
53
53
5 x 2 1 x 2 sin x 1 3
Section 4.2
35. Possible answers:
(a)
(b)
[22, 4] by [22, 4]
[21, 4] by [0, 3.5]
(c)
36. Possible answers:
(b)
[21, 5] by [22, 4]
(c)
[21, 5] by [21, 8]
(d)
[21, 5] by [21, 8]
42. The runner’s average speed for the marathon was
approximately 11.909 mph. Therefore, by the Mean Value
Theorem, the runner must have been going that speed at
least once during the marathon. Since the initial speed and
final speed are both 0 mph and the runner’s speed is
continuous, by the Intermediate Value Theorem, the
runner’s speed must have been 11 mph at least twice.
43. (a) Since v9(t) 5 1.6, v(t) 5 1.6t 1 C. But v(0) 5 0, so
C 5 0 and v(t) 5 1.6t. Therefore,
v(30) 5 1.6(30) 5 48. The rock will be going
48 m/sec.
(b) Let s(t) represent position.
Since s9(t) 5 v(t) 5 1.6t, s(t) 5 0.8t 2 1 D. But
s(0) 5 0, so D 5 0 and s(t) 5 0.8t 2. Therefore,
s(30) 5 0.8(30)2 5 720. The rock travels 720 meters in
the 30 seconds it takes to hit bottom, so the bottom of
the crevasse is 720 meters below the point of release.
[21, 4] by [0, 3.5]
(a)
137
[21, 5] by [21, 8]
(c) The velocity is now given by v(t) 5 1.6t 1 C, where
v(0) 5 4. (Note that the sign of the initial velocity is
the same as the sign used for the acceleration, since
both act in a downward direction.) Therefore,
v(t) 5 1.6t 1 4, and s(t) 5 0.8t 2 1 4t 1 D, where
s(0) 5 0 and so D 5 0. Using s(t) 5 0.8t 2 1 4t and the
known crevasse depth of 720 meters, we solve
s(t) 5 720 to obtain the positive solution t < 27.604,
and so v(t) 5 v(27.604) 5 1.6(27.604) 1 4 < 48.166.
The rock will hit bottom after about 27.604 seconds,
and it will be going about 48.166 m/sec.
37. One possible answer:
44. (a) We assume the diving board is located at s 5 0 and the
water at s 5 10, so that downward velocities are
positive. The acceleration due to gravity is 9.8 m/sec2,
[23, 3] by [215, 15]
38. One possible answer:
so v9(t) 5 9.8 and v(t) 5 9.8t 1 C. Since v(0) 5 0, we
have v(t) 5 9.8t. Then the position is given by s(t)
where s9(t) 5 v(t) 5 9.8t, so s(t) 5 4.9t 2 1 D. Since
s(0) 5 0, we have s(t) 5 4.9t 2. Solving s(t) 5 10 gives
[23, 3] by [270, 70]
39. Because the trucker’s average speed was 79.5 mph, and by
the Mean Value Theorem, the trucker must have been going
that speed at least once during the trip.
40. Let f (t) denote the temperature indicated after t seconds.
We assume that f 9(t) is defined and continuous for
0 # t # 20. The average rate of change is 10.68F/sec.
Therefore, by the Mean Value Theorem, f 9(c) 5 10.68F/sec
for some value of c in [0, 20]. Since the temperature was
constant before t 5 0, we also know that f 9(0) 5 08F/min.
But f 9 is continuous, so by the Intermediate Value Theorem,
the rate of change f 9(t) must have been 10.18F/sec at some
moment during the interval.
41. Because its average speed was approximately 7.667 knots,
and by the Mean Value Theorem, it must have been going
that speed at least once during the trip.
10
4.9
100
49
10
7
t 2 5 }} 5 }}, so the positive solution is t 5 }}. The
172
172
10
10
velocity at this time is v }} 5 9.8 }} 5 14 m/sec.
(b) Again v(t) 5 9.8t 1 C, but this time v(0) 5 22 and so
v(t) 5 9.8t 2 2. Then s9(t) 5 9.8t 2 2, so
s(t) 5 4.9t 2 2 2t 1 D. Since s(0) 5 0, we have
s(t) 5 4.9t 2 2 2t. Solving s(t) 5 10 gives the positive
2 1 10Ïw
2
solution t 5 }} < 1.647 sec.
9.8
The velocity at this time is
w
w
2 1 10Ï2
2 1 10Ï2
v }} 5 9.8 }} 2 2 5 10Ï2w m/sec or
1
9.8
2
1
about 14.142 m/sec.
9.8
2
138
Section 4.3
45. Because the function is not continuous on [0, 1]. The
function does not satisfy the hypotheses of the Mean Value
Theorem, and so it need not satisfy the conclusion of the
Mean Value Theorem.
46. Because the Mean Value Theorem applies to the function
y 5 sin x on any interval, and y 5 cos x is the derivative of
sin x. So, between any two zeros of sin x, its derivative,
cos x, must be zero at least once.
47. f (x) must be zero at least once between a and b by the
Intermediate Value Theorem. Now suppose that f (x) is zero
twice between a and b. Then by the Mean Value Theorem,
f 9(x) would have to be zero at least once between the two
zeros of f (x), but this can’t be true since we are given that
f 9(x) Þ 0 on this interval. Therefore, f (x) is zero once and
only once between a and b.
48. Let f (x) 5 x 4 1 3x 1 1. Then f (x) is continuous and
differentiable everywhere. f 9(x) 5 4x 3 1 3, which is never
zero between x 5 22 and x 5 21. Since f (22) 5 11 and
f (21) 5 21, exercise 47 applies, and f (x) has exactly one
zero between x 5 22 and x 5 21.
49. Let f (x) 5 x 1 ln (x 1 1). Then f (x) is continuous and
1
x11
differentiable everywhere on [0, 3]. f 9(x) 5 1 1 }},
which is never zero on [0, 3]. Now f (0) 5 0, so x 5 0 is
one solution of the equation. If there were a second
solution, f (x) would be zero twice in [0, 3], and by the
Mean Value Theorem, f 9(x) would have to be zero
somewhere between the two zeros of f (x). But this can’t
happen, since f 9(x) is never zero on [0, 3]. Therefore,
f (x) 5 0 has exactly one solution in the interval [0, 3].
50. Consider the function k(x) 5 f (x) 2 g(x). k(x) is continuous
and differentiable on [a, b], and since
k(a) 5 f (a) 2 g(a) 5 0 and k(b) 5 f (b) 2 g(b) 5 0, by the
Mean Value Theorem, there must be a point c in (a, b)
where k9(c) 5 0. But since k9(c) 5 f 9(c) 2 g9(c), this
means that f 9(c) 5 g9(c), and c is a point where the graphs
of f and g have parallel or identical tangent lines.
52. (a) Toward: 0 , t , 2 and 5 , t , 8;
away: 2 , t , 5
(b) A local extremum in this problem is a time/place where
Priya changes the direction of her motion.
(c) Regression equation:
y 5 20.0820x 3 1 0.9163x 2 2 2.5126x 1 3.3779
[20.5, 8.5] by [20.5, 5]
(d) Using the unrounded values from the regression
equation, we obtain
f 9(t) 5 20.2459t 2 1 1.8324t 2 2.5126. According to
the regression equation, Priya is moving toward the
motion detector when f 9(t) , 0 (0 , t , 1.81 and
5.64 , t , 8), and away from the detector when
f 9(t) . 0 (1.81 , t , 5.64).
1
1
}} 2 }}
f(b) 2 f(a)
b2a
1
ab
b
a
53. }} 5 }
5 2}}
b2a
1
c
1
c
1
ab
f 9(c) 5 2}}2 , so 2}}2 5 2}} and c 2 5 ab.
Thus, c 5 Ïawbw.
f (b) 2 f (a)
b2a
b2 2 a2
b2a
54. }} 5 }} 5 b 1 a
a1b
2
f 9(c) 5 2c, so 2c 5 b 1 a and c 5 }}.
55. By the Mean Value Theorem,
sin b 2 sin a 5 (cos c)(b 2 a) for some c between a and b.
Taking the absolute value of both sides and using
)cos c) # 1 gives the result.
56. Apply the Mean Value Theorem to f on [a, b].
f(b) 2 f(a)
b2a
Since f (b) , f (a), }} is negative, and hence f 9(x)
must be negative at some point between a and b.
[21, 1] by [22, 2]
51. (a) Increasing: [22, 21.3] and [1.3, 2];
decreasing: [21.3, 1.3];
local max: x < 21.3
local min: x < 1.3
(b) Regression equation: y 5 3x 2 2 5
57. Let f (x) be a monotonic function defined on an interval D.
For any two values in D, we may let x1 be the smaller value
and let x2 be the larger value, so x1 , x2. Then either
f (x1) , f (x2) (if f is increasing), or f (x1) . f (x2) (if f is
decreasing), which means f (x1) Þ f (x2). Therefore, f is
one-to-one.
■ Section 4.3 Connecting f9 and f 0 with the
Graph of f (pp. 194–206)
Finding f from f 9
1. Any function f (x) 5 x 4 2 4x 3 1 C where C is a real
number. For example, let C 5 0, 1, 2. Their graphs are all
vertical shifts of each other.
Exploration 1
[22.5, 2.5] by [28, 10]
(c) Since f 9(x) 5 3x 2 2 5, we have f (x) 5 x 3 2 5x 1 C.
But f (0) 5 0, so C 5 0. Then f (x) 5 x 3 2 5x.
2. Their behavior is the same as the behavior of the function f
of Example 8.
Section 4.3
Finding f from f 9 and f 0
Exploration 2
Section 4.3 Exercises
1. f has an absolute maximum at x 5 0 and an absolute
minimum of 1 at x 5 4. We are not given enough
information to determine f (0).
1. (a) Zero: x 5 61;
positive: (2`, 21) and (1, `);
negative: (21, 1)
2. f has a point of inflection at x 5 2.
(b) Zero: x 5 0;
positive: (0, `);
negative: (2`, 0)
3.
2. (a) Zero: x < 0, 61.25;
positive: (21.25, 0) and (1.25, `);
negative: (2`, 21.25) and (0, 1.25)
(b) Zero: x < 60.7;
positive: (2`, 20.7) and (0.7, `);
negative: (20.7, 0.7)
[23, 5] by [25, 20]
Quick Review 4.3
1.
x2 2 9 , 0
(x 1 3)(x 2 3) , 0
Intervals
Sign of
(x 1 3)(x 2 3)
3. (a) (2`, 22] and [0, 2]
(b) [22, 0] and [2, `)
x , 23 23 , x , 3 3 , x
1
2
(c) Local maxima: x 5 22 and x 5 2;
local minimum: x 5 0
1
4. (a) [22, 2]
(b) (2`, 22] and [2, `)
Solution set: (23, 3)
2.
(c) Local maximum: x 5 2;
local minimum: x 5 22
x 3 2 4x . 0
x(x 1 2)(x 2 2) . 0
Intervals
x , 22 22 , x , 0
0,x,2
2,x
2
1
Sign of
x(x 1 2)(x 2 2)
2
1
Solution set: (22, 0) < (2, `)
3. f: all reals
f 9: all reals, since f 9(x) 5 xe x 1 e x
5. (a) [0, 1], [3, 4], and [5.5, 6]
(b) [1, 3] and [4, 5.5]
(c) Local maxima: x 5 1, x 5 4
(if f is continuous at x 5 4), and x 5 6;
local minima: x 5 0, x 5 3, and x 5 5.5
6. If f is continuous on the interval [0, 3]:
(a) [0, 3]
4. f: all reals
(b) Nowhere
3
f 9: x Þ 0, since f 9(x) 5 }}x 22/5
5
(c) Local maximum: x 5 3;
local minimum: x 5 0
5. f: x Þ 2
(x 2 2)(1) 2 (x)(1)
(x 2 2)
22
(x 2 2)
5 }}2
f 9: x Þ 2, since f 9(x) 5 }}
2
6. f: all reals
2
5
f 9: x Þ 0, since f 9(x) 5 }}x 23/5
7. Left end behavior model: 0
Right end behavior model: 2x 2e x
Horizontal asymptote: y 5 0
7. y9 5 2x 2 1
1
2
1
2
Intervals
x , }}
x . }}
Sign of y9
2
1
Behavior of y Decreasing Increasing
y0 5 2 (always positive: concave up)
Graphical support:
2 2x
8. Left end behavior model: x e
Right end behavior model: 0
Horizontal asymptote: y 5 0
9. Left end behavior model: 0
Right end behavior model: 200
Horizontal asymptotes: y 5 0, y 5 200
10. Left end behavior model: 0
Right end behavior model: 375
Horizontal asymptotes: y 5 0, y 5 375
[24, 4] by [23, 3]
32 2
1
(a) }}, `
1
1
2
4
(b) 2`, }}
(c) (2`, `)
(d) Nowhere
12
1
5
4
2
(e) Local (and absolute) minimum at }}, 2}}
(f) None
139
140
Section 4.3
8. y9 5 26x 2 1 12x 5 26x(x 2 2)
1
1
x
2
10. y9 5 xe 1/x(2x 22) 1 e 1/x 5 e 1/x 1 2 }}
Intervals
x,0
0,x,2
2,x
Sign of y9
2
1
2
Behavior of y Decreasing Increasing Decreasing
Intervals
x,0
0,x,1
1,x
Sign of y9
1
2
1
Behavior of y Increasing Decreasing Increasing
y0 5 212x 1 12 5 212(x 2 1)
Intervals
x,1
x.1
Sign of y0
1
2
Behavior of y
1
Concave up Concave down
Intervals
x,0
x.0
Sign of y0
2
1
Graphical support:
[24, 4] by [26, 6]
[28, 8] by [26, 6]
(a) [0, 2]
(b) (2`, 0] and [2, `)
(c) (2`, 1)
(a) (2`, 0) and [1, `)
(b) (0, 1]
(c) (0, `)
(d) (2`, 0)
(e) Local minimum: (1, e)
(d) (1, `)
(f) None
(e) Local maximum: (2, 5);
local minimum: (0, 23)
9. y9 5 8x 3 2 8x 5 8x(x 2 1)(x 1 1)
Intervals
x , 21
Sign of y9
2
Intervals
21 , x , 0 0 , x , 1
1
Behavior of y Decreasing
1,x
2
Increasing
1
Decreasing Increasing
y0 5 24x 2 2 8 5 8(Ï3wx 2 1)(Ï3wx 1 1)
1
1
x , 2}}
Ïw3
1
2} } , x , }}
Ï3w
Ïw3
1
}} , x
Ïw3
1
2
1
Concave up
Concave down
Concave up
Sign of y0
8 2 2x2
1
2wx 2w)(1) 5 }}
11. y9 5 x}}(22x) 1 (Ï8ww
2wx 2w
2wx 2w
2Ï8
ww
Ïw8w
(f) At (1, 1)
Behavior of y
e 1/x
x
2
Behavior of y Concave down Concave up
Graphical support:
Intervals
1
x
y0 5 e 1/x(x 22) 1 1 2 }} e 1/x(2x 22) 5 }}
3
Graphical support:
2Ï8w , x , 22 22 , x , 2 2 , x , Ï8w
2
1
2
Decreasing
Increasing
Decreasing
Sign of y9
Behavior of y
1
(Ï8
ww
2wx2w)(24x) 2 (8 2 2x2)}}(22x)
2wx 2w
2Ï8ww
y0 5 }}}}}
2 2
(Ïw
8w
2wxw)
2x 3 2 24x
(8 2 x )
2x(x 2 2 12)
(8 2 x )
5 }}
2 3/2 5 }}
2 3/2
Intervals
2Ï8w , x , 0
0 , x , Ï8w
Sign of y0
1
2
Concave up
Concave down
Behavior of y
Graphical support:
[24, 4] by [23, 3]
(a) [21, 0] and [1, `)
[23.02, 3.02] by [26.5, 6.5]
(b) (2`, 21] and [0, 1]
1
1
2
1
2
1
1
(c) 2`, 2}} and }}, `
Ïw3
Ï3w
1
1
2
(d) 2}}, }}
Ï3w Ï3w
(e) Local maximum: (0, 1);
local (and absolute) minima: (21, 21) and (1, 21)
(f)
16}Ï}3w , 2}9}2
1
1
(a) [22, 2]
(b) [2Ï8w, 22] and [2, Ï8w]
(c) (2Ï8w, 0)
(d) (0, Ï8w)
(e) Local maxima: (2Ï8w, 0) and (2, 4);
local minima: (22, 24) and (Ï8w, 0)
Note that the local extrema at x 5 62 are also absolute
extrema.
(f) (0, 0)
Section 4.3
12. y9 5
22x,
h2x,
141
x,0
x.0
Intervals
x,0
x.0
Sign of y9
1
1
Behavior of y Increasing Increasing
y0 5
h22,
2,
x,0
x.0
Intervals
x,0
x.0
Sign of y0
2
1
Behavior of y Concave down Concave up
Graphical support:
[24, 4] by [23, 6]
(a) (2`, 0) and [0, `)
(b) None
(c) (0, `)
(d) (2`, 0)
(e) Local minimum: (0, 1)
(f) Note that (0, 1) is not an inflection point because the graph has no tangent line at this point. There are no inflection points.
13. y9 5 12x 2 1 42x 1 36 5 6(x 1 2)(2x 1 3)
3
2
22 , x , 2}}
x , 22
Intervals
1
2
1
Increasing
Decreasing
Increasing
Sign of y9
Behavior of y
3
2
2}} , x
y0 5 24x 1 42 5 6(4x 1 7)
7
4
7
4
Intervals
x , 2}}
2}} , x
Sign of y0
2
1
Behavior of y Concave down Concave up
Graphical support:
[24, 4] by [280, 20]
3
3
2
2
(a) (2`, 22] and 2}}, `
3
3
24
7
(c) 12}}, `2
4
7
(d) 12`, 2}}2
4
(b) 22, 2}}
1
3
2
161
4
(e) Local maximum: (22, 240); local minimum: 2}}, 2}}
(f)
1
2
7
321
2}}, 2}}
4
8
2
142
Section 4.3
14. y9 5 24x 3 1 12x 2 2 4
Using grapher techniques, the zeros of y9 are x < 20.53, x < 0.65, and x < 2.88.
x , 20.53 20.53 , x , 0.65 0.65 , x , 2.88
Intervals
1
2
1
2
Increasing
Decreasing
Increasing
Decreasing
Sign of y9
Behavior of y
2.88 , x
y0 5 212x 1 24x 5 212x(x 2 2)
2
Intervals
x,0
0,x,2
2,x
Sign of y0
2
1
2
Behavior of y Concave down Concave up Concave down
Graphical support:
[22, 4] by [220, 20]
(2`, 20.53] and [0.65, 2.88]
[20.53, 0.65] and [2.88, `)
(0, 2)
(2`, 0) and (2, `)
Local maxima: (20.53, 2.45) and (2.88, 16.23);local minimum: (0.65, 20.68)
Note that the local maximum at x < 2.88 is also an absolute maximum.
(f) (0,1) and (2, 9)
(a)
(b)
(c)
(d)
(e)
2
5
15. y9 5 }}x 24/5
Intervals
Sign of y9
Behavior of y
x,0
0,x
1
1
Increasing Increasing
8
25
y0 5 2}}x 29/5
Intervals
x,0
0,x
Sign of y0
1
2
Behavior of y Concave up Concave down
Graphical support:
[26, 6] by [21.5, 7.5]
(a) (2`, `)
(b) None
(c) (2`, 0)
(d) (0, `)
(e) None
(f) (0, 3)
1
3
16. y9 5 2}}x 22/3
Intervals
x,0
0,x
Sign of y9
2
2
Behavior of y Decreasing Decreasing
Section 4.3
143
2
9
y0 5 }}x 25/3
Intervals
x,0
0,x
Sign of y0
2
1
Behavior of y Concave down Concave up
Graphical support:
[28, 8] by [0, 10]
(a) None
(b) (2`, `)
(c) (0, `)
(d) (2`, 0)
(e) None
(f) (0, 5)
17. This problem can be solved using either graphical or analytic methods. For a graphical solution, use NDER to obtain the graphs
shown.
y
y9
y0
[210, 20] by [0, 5]
[210, 20] by [0, 0.3]
[210, 20] by [20.02, 0.02]
An analytic solution follows.
(e x 1 3e 0.8x)(5e x) 2 5e x(e x 1 2.4e 0.8x)
(e 1 3e )
y9 5 }}}}
x
0.8x 2
5e 2x 1 15e 1.8x 2 5e 2x 2 12e 1.8x
(e 1 3e )
5 }}}}
x
0.8x 2
3e 1.8x
(e 1 3e )
5}
}
x
0.8x 2
Since y9 . 0 for all x, y is increasing for all x.
(e x 1 3e 0.8x)2(5.4e 1.8x) 2 (3e 1.8x)(2)(e x 1 3e 0.8x)(e x 1 2.4e 0.8x)
(e 1 3e )
y0 5 }}}}}}}
x
0.8x 4
(e x 1 3e 0.8x)(5.4e 1.8x) 2 (6e 1.8x)(e x 1 2.4e 0.8x)
(e 1 3e )
5 }}}}}
x
0.8x 3
(20.6e x 1 1.8e 0.8x)e 1.8x
(e 1 3e )
5 }}}
x
0.8x 3
0.6(3 2 e 0.2x)e 2.6x
(e 1 3e )
5 }}
x
0.8x 3
Solve y0 5 0: 3 2 e 0.2x 5 0
0.2x 5 ln 3
x 5 5 ln 3
Intervals
x , 5 ln 3
5 ln 3 , x
Sign of y0
1
2
Behavior of y Concave up Concave down
144
Section 4.3
17. continued
(a) (2`, `)
(b) None
(c) (2`, 5 ln 3) < (2`, 5.49)
(d) (5 ln 3, `) < (5.49, `)
(e) None
(f)
15 ln 3, }52}2 < (5.49, 2.50)
18. This problem can be solved using either graphical or analytic methods. For a graphical solution, use NDER to obtain the graphs
shown.
y
y9
y0
[26, 10] by [0, 4]
[26, 10] by [0, 0.6]
[26, 10] by [20.15, 0.15]
An analytic solution follows.
8e 2x
1 5e
8
2 1 5e
y 5}
}
2x
21.5x 5 }}
20.5x
2e
(2 1 5e 20.5x)(0) 2 (8)(22.5e 20.5x)
(2 1 5e
)
y9 5 }}}}
20.5x 2
20e 20.5x
(2 1 5e
)
5 }}
20.5x 2
Since y9 . 0 for all x, y is increasing for all x.
(2 1 5e 20.5x)2(210e 20.5x) 2 (20e 20.5x)(2)(2 1 5e 20.5x)(22.5e 20.5x)
(2 1 5e
)
y0 5 }}}}}}}
20.5x 4
(2 1 5e 20.5x)(10e 20.5x) 2 (40e 20.5x)(22.5e 20.5x)
(2 1 5e
)
5 }}}}}}
20.5x 3
10e 20.5x(5e 20.5x 2 2)
(2 1 5e
)
5 }}}
20.5x 3
5e 20.5x 2 2 5 0
Solve y0 5 0:
2
5
e 20.5x 5 }}
2
5
20.5x 5 ln }}
2
5
5
2
x 5 22 ln }} 5 2 ln }}
5
2
5
2
Intervals
x , 2 ln }}
2 ln }} , x
Sign of y0
1
2
Concave up
Concave down
Behavior of y
(a) (2`, `)
(b) None
1
5
2
2
(c) 2`, 2 ln }} < (2`, 1.83)
1
5
2
2
(d) 2 ln }}, ` < (1.83, `)
(e) None
(f)
12 ln }2}, 22 < (1.83, 2)
5
Section 4.3
19. y9 5
h
2,
22x,
x,1
x.1
Intervals
x,1
1,x
Sign of y9
1
2
Increasing
Decreasing
Behavior of y
y0 5
h
0,
22,
x,1
x.1
x,1
Intervals
0
2
Linear
Concave down
Sign of y0
Behavior of y
1,x
Graphical support:
[22, 3] by [–5, 3]
(a) (2`, 1)
(b) [1, `)
(c) None
(d) (1, `)
(e) None
(f) None
20. y9 5 e x
y0 5 e x
Since y9 and y0 are both positive on the entire domain, y is increasing and concave up on the entire domain.
Graphical support:
[0, 2p] by [0, 20]
(a) [0, 2p]
(b) None
(c) (0, 2p)
(d) None
(e) Local (and absolute) maximum: (2p, e2p); local (and absolute) minimum: (0, 1)
(f) None
21. y9 5 xe 1/x (22x 23) 1 (e 1/x )(1)
2
2
1
x2 2 2
x
2
5 e 1/x (1 2 2x 22) 5 e 1/x }}
2
2
Intervals
Sign of y9
Behavior of y
2
x , 2Ï2w 2Ï2w , x , 0 0 , x , Ï2w
Ï2w , x
1
2
2
1
Increasing
Decreasing
Decreasing
Increasing
145
146
Section 4.3
21. continued
y0 5 (e 1/x )(4x 23) 1 (1 2 2x 22)(e 1/x )(22x 23)
2
2
5 (e 1/x )(2x 23 1 4x 25)
2
1
2
x2 1 2
x
2
5 2e 1/x }}
5
Intervals
x,0
0,x
Sign of y0
2
1
Behavior of y Concave down Concave up
Graphical support:
[212, 12] by [29, 9]
(a) (2`, 2Ï2w] and [Ï2w, `)
(b) [2Ï2w, 0) and (0, Ï2w]
(c) (0, `)
(d) (2`, 0)
(e) Local maximum: (2Ï2w, 2Ï2wew) < (21.41, 22.33); local minimum: (Ï2w, Ï2wew) < (1.41, 2.33)
(f) None
22. This problem can be solved using either graphical or analytic methods. For a graphical solution, use NDER to obtain the graphs
shown.
y
y9
y0
[24.7, 4.7] by [23, 11]
[24.7, 4.7] by [210, 10]
[24.7, 4.7] by [210, 10]
An analytic solution follows.
1
2wx 2w(2x)
y9 5 x 2}}(22x) 1 Ï9ww
2wx 2w
2Ï9ww
23x 3 1 18x
23x(x 2 2 6)
5 }} 5 }}
2wx 2w
Ï9ww
2wx 2w
Ïw9w
23 , x , 2Ï6w 2Ï6w , x , 0 0 , x , Ï6w Ï6w , x , 3
Intervals
1
2
1
2
Increasing
Decreasing
Increasing
Decreasing
Sign of y9
Behavior of y
1
(Ï9ww
2wx 2w)(29x 2 1 18) 2 (23x 3 1 18x)}}(22x)
2wx 2w
2Ï9
ww
y0 5 }}}}}}
(Ïw
9w
2wx 2w)2
(9 2 x 2)(29x 2 1 18) 1 (23x 3 1 18x)(x)
5 }}}}}
2 3/2
(9 2 x )
6x 2 81x 1 162
4
2
5 }}
2 3/2
(9 2 x )
Section 4.3
Find the zeros of y0:
3(2x 4 2 27x 2 1 54)
50
}}}
(9 2 x 2)3/2
2x 4 2 27x 2 1 54 5 0
w3w
27 6 Ï2
w7w2w2
ww4(2
w)(
w5w4w)w
27 6 3Ï3
x 2 5 }}} 5 }}
2(2)
4
!§§§§§§§
x56
w3w
27 2 3Ï3
}} < 61.56
4
!§§§§4 §§§
w3w
27 1 3Ï3
Note that we do not use x 5 6 }} < 63.33, because these values are outside of the domain.
Intervals
23 , x , 21.56 21.56 , x , 1.56
2
1
2
Concave down
Concave up
Concave down
Sign of y0
Behavior of y
1.56 , x , 3
(a) [23, 2Ï6w] and [0, Ï6w] or, <[23, 22.45]
and [0, 2.45]
(b) [2Ï6w, 0] and [Ï6w, 3] or, <[22.45, 0] and [2.45, 3]
(c) Approximately (21.56, 1.56)
(d) Approximately (23, 21.56) and (1.56, 3)
(e) Local maxima: (6Ï6w, 6Ï3w) < (62.45, 10.39);
local minima: (0, 0) and (63, 0)
(f) <(61.56, 6.25)
1
11x
23. y9 5 }}2
Since y9 . 0 for all x, y is always increasing.
22x
(1 1 x )
d
dx
y0 5 }}(1 1 x 2)21 5 2(1 1 x 2)22(2x) 5 }}
2 2
Intervals
x,0
0,x
Sign of y0
1
2
Behavior of y Concave up Concave down
Graphical support:
[24, 4] by [22, 2]
(a) (2`, `)
(b) None
(c) (2`, 0)
(d) (0, `)
(e) None
(f) (0, 0)
147
148
Section 4.3
(a) [1, `)
24. y 5 x 3/4(5 2 x) 5 5x 3/4 2 x 7/4
15
7
15 2 7x
y9 5 }}x 21/4 2 }}x 3/4 5 }}
4
4
4x 1/4
Intervals
(c) (2`, 22) and (0, `)
15
0 , x , }}
7
15
}} , x
7
1
2
Increasing
Decreasing
Sign of y9
Behavior of y
(b) (2`, 1]
15
16
23(7x 1 5)
5 }}
16x 5/4
(d) (22, 0)
(e) Local minimum: (1, 23)
3
(f) (22, 6Ï2w) < (22, 7.56) and (0, 0)
26. y 5 x 1/4(x 1 3) 5 x 5/4 1 3x 1/4
5
4
21
16
5x 1 3
4x
3
4
y9 5 }}x 1/4 1 }}x 23/4 5 }}
3/4
y0 5 2}}x 25/4 2 }}x 21/4
Since y9 . 0 for all x . 0, y is always increasing on its
domain x $ 0.
Since y0 , 0 for all x . 0, the graph of y is concave down
for x . 0.
5
16
9
5
0 , x , }}
Intervals
Behavior of y
(a)
3
9
}} , x
5
2
1
Concave down
Concave up
Sign of y0
[0, 8] by [26, 6]
5x 2 9
16x
9
16
y0 5 }}x 23/4 2 }}x 27/4 5 }}
7/4
Graphical support:
Graphical support:
4
15
0, }}
7
37 2
15
(b) }}, `
(c) None
[0, 6] by [0, 12]
(d) (0, `)
(a) [0, `)
(e) Local (and absolute) maximum:
(b) None
15 3/4
1}7}, 1}7}2
15
15 2
? }7}2 < 1}7}, 5.062;
20
9
15
(c) }}, `
local minimum: (0, 0)
1 52
9
(d) 0, }}
(f) None
(e) Local (and absolute) minimum: (0, 0)
25. y 5 x 1/3(x 2 4) 5 x 4/3 2 4x 1/3
(f)
4
4
4x 2 4
y9 5 }}x 1/3 2 }}x 22/3 5 }}
3
3
3x 2/3
1}5}, }5} ? !}§5}2 < 1}5}, 5.562
9 24
4
9
9
Intervals
x,0
0,x,1
1,x
27. We use a combination of analytic and grapher techniques to
Sign of y9
2
2
1
solve this problem. Depending on the viewing window
Behavior of y Decreasing Decreasing Increasing
4
9
behavior near x 5 2 because, for example,
4x 1 8
9x
8
9
chosen, graphs obtained using NDER may exhibit strange
y0 5 }}x 22/3 1 }}x 25/3 5 }}
5/3
NDER (y, 2) < 1,000,000 while y9 is actually undefined at
Intervals
x , 22
22 , x , 0
0,x
Sign of y0
1
2
1
x 3 2 2x 2 1 x 2 1
x22
x 5 2. The graph of y 5 }} is shown below.
Behavior of y Concave up Concave down Concave up
Graphical support:
[24,7, 4.7] by [25, 15]
[24, 8] by [26, 8]
Section 4.3
(x 2 2)(3x 2 2 4x 1 1) 2 (x 3 2 2x 2 1 x 2 1)(1)
(x 2 2)
y95 }}}}}
2
2x 3 2 8x 2 1 8x 2 1
(x 2 2)
5 }}}
2
The graph of y9 is shown below.
[24,7, 4.7] by [210, 10]
The zeros of y9 are x < 0.15, x < 1.40, and x < 2.45.
Intervals
x , 0.15
Sign of y9
2
0.15 , x , 1.40 1.40 , x , 2 2 , x , 2.45
Behavior of y Decreasing
2.45 , x
1
2
2
1
Increasing
Decreasing
Decreasing
Increasing
(x 2 2)2(6x 2 2 16x 1 8) 2 (2x 3 2 8x 2 1 8x 2 1)(2)(x 2 2)
(x 2 2)
y0 5 }}}}}}}
4
(x 2 2)(6x 2 2 16x 1 8) 2 2(2x 3 2 8x 2 1 8x 2 1)
(x 2 2)
5 }}}}}}
3
2x 3 2 12x 2 1 24x 2 14
(x 2 2)
5 }}}
3
2(x 2 1)(x 2 2 5x 1 7)
(x 2 2)
5 }}}
3
The graph of y0 is shown below.
[24,7, 4.7] by [210, 10]
Note that the discriminant of x 2 2 5x 1 7 is (25)2 2 4(1)(7) 5 23, so the only solution of y0 5 0 is x 5 1.
Intervals
x,1
1,x,2
2,x
Sign of y0
1
2
1
Behavior of y Concave up Concave down Concave up
(a) Approximately [0.15, 1.40] and [2.45, `)
(b) Approximately (2`, 0.15], [1.40, 2), and (2, 2.45]
(c) (2`, 1) and (2, `)
(d) (1, 2)
(e) Local maximum: <(1.40, 1.29);local minima: <(0.15, 0.48) and (2.45, 9.22)
(f) (1, 1)
149
150
Section 4.3
(x 2 1 1)(1) 2 x(2x)
(x 1 1)
2x 2 1 1
(x 1 1)
28. y9 5 }}}
5}
2
2
2 }
2
Intervals
x , 21
21 , x , 1
1,x
Sign of y9
2
1
2
Increasing
Decreasing
Behavior of y Decreasing
(x 2 1 1)2(22x) 2 (2x 2 1 1)(2)(x 2 1 1)(2x)
(x 1 1)
y0 5 }}}}}
2
4
(x 2 1 1)(22x) 2 4x(2x 2 1 1)
(x 1 1)
5 }}}}
2
3
2x(x 2 2 3)
(x 1 1)
2x 3 2 6x
(x 1 1)
5}
2 }
3 5}
2 }
3
Intervals
x , 2Ï3w
Sign of y0
2
2Ï3w , x , 0
0 , x , Ï3w
Ï3w , x
2
1
1
Behavior of y Concave down
Concave up
Concave down Concave up
Graphical support:
[24.7, 4.7] by [20.7, 0.7]
(a) [21, 1]
(b) (2`, 21] and [1, `)
(c) (2Ï3w, 0) and (Ï3w, `)
(d) (2`, 2Ï3w) and (0, Ï3w)
1 22
1
(e) Local maximum: 1, }} ;
1
22
Ï3w
Ïw3
(0, 0), 1Ï3w, }}2, and 12Ï3w, 2}}2
4
4
1
local minimum: 21, 2}}
(f)
29. y9 5 (x 2 1)2(x 2 2)
Intervals
x,1
1,x,2
2,x
Sign of y9
2
2
1
Behavior of y Decreasing Decreasing Increasing
y0 5 (x 2 1)2(1) 1 (x 2 2)(2)(x 2 1)
5 (x 2 1)[(x 2 1) 1 2(x 2 2)]
5 (x 2 1)(3x 2 5)
Intervals
x,1
1 , x , }}
5
3
5
}} , x
3
Sign of y0
1
2
1
Behavior of y Concave up Concave down Concave up
(a) There are no local maxima.
(b) There is a local (and absolute) minimum at x 5 2.
5
3
(c) There are points of inflection at x 5 1 and at x 5 }}.
Section 4.3
30. y9 5 (x 2 1)2(x 2 2)(x 2 4)
Intervals
x,1
1,x,2
2,x,4
4,x
Sign of y9
1
1
2
1
Increasing
Increasing
Behavior of y
Decreasing Increasing
d
dx
y0 5 }}[(x 2 1)2(x 2 2 6x 1 8)]
5 (x 2 1)2(2x 2 6) 1 (x 2 2 6x 1 8)(2)(x 2 1)
5 (x 2 1)[(x 2 1)(2x 2 6) 1 2(x 2 2 6x 1 8)]
5 (x 2 1)(4x 2 2 20x 1 22)
5 2(x 2 1)(2x 2 2 10x 111)
Note that the zeros of y0 are x 5 1 and
w2w 5 6 Ï3w
10 6 Ï1
w0w2w2
ww4(2
w)(
w1w1w)w
10 6 Ï1
x 5 }}} 5 }} 5 }} < 1.63 or 3.37.
4
4
2
The zeros of y0 can also be found graphically, as shown.
[23, 7] by [28, 4]
Intervals
x,1
Sign of y0
2
1 , x , 1.63 1.63 , x , 3.37
Behavior of y Concave down
1
2
1
Concave up
Concave down
Concave up
(a) Local maximum at x 5 2
(b) Local minimum at x 5 4
(c) Points of inflection at x 5 1, at x < 1.63, and at x < 3.37.
31.
y
y = f′(x)
y = f(x)
P
x
y = f′′(x)
32.
y
P y = f(x)
0
y = f ′(x)
x
y = f ′′(x)
3.37 , x
151
152
Section 4.3
33. (a) Absolute maximum at (1, 2);
absolute minimum at (3, 22)
(b) None
(b) a(t) 5 v9(t) 5 22
(c) It begins at position 6 and moves in the negative
direction thereafter.
(c) One possible answer:
39. (a) v(t) 5 s9(t) 5 3t 2 2 3
y
2
(b) a(t) 5 v9(t) 5 6t
y = f(x)
1
1
2
3
x
(c) It begins at position 3 moving in a negative direction. It
moves to position 1 when t 5 1, and then changes
direction, moving in a positive direction thereafter.
40. (a) v(t) 5 s9(t) 5 6t 2 6t 2
(b) a(t) 5 v9(t) 5 6 2 12t
–1
–2
34. (a) Absolute maximum at (0, 2);
absolute minimum at (2, 21) and (22, 21)
(b) At (1, 0) and (21, 0)
(c) It begins at position 0. It starts moving in the positive
direction until it reaches position 1 when t 5 1, and
then it changes direction. It moves in the negative
direction thereafter.
41. (a) The velocity is zero when the tangent line is horizontal,
at approximately t 5 2.2, t 5 6, and t 5 9.8.
(c) One possible answer:
(b) The acceleration is zero at the inflection points,
approximately t 5 4, t 5 8, and t 5 11.
y
2
42. (a) The velocity is zero when the tangent line is horizontal,
at approximately t 5 20.2, t 5 4, and t 5 12.
y = f(x)
–3
3
x
–1
–2
(d) Since f is even, we know f (3) 5 f (23). By the
continuity of f, since f (x) , 0 when 2 , x , 3, we
know that f (3) # 0, and since f (2) 5 21 and f 9(x) . 0
when 2 , x , 3, we know that f (3) . 21. In
summary, we know that f (3) 5 f (23), 21 , f (3) # 0,
and 21 , f (23) # 0.
35.
38. (a) v(t) 5 s9(t) 5 22 2 2t
(b) The acceleration is zero at the inflection points,
approximately t 5 1.5, t 5 5.2, t 5 8, t 5 11,
and t 5 13.
43. No. f must have a horizontal tangent at that point, but f
could be increasing (or decreasing), and there would be no
local extremum. For example, if f (x) 5 x 3,
f 9(0) 5 0 but there is no local extremum at x 5 0.
44. No. f 0(x) could still be positive (or negative) on both sides
of x 5 c, in which case the concavity of the function would
not change at x 5 c. For example, if f (x) 5 x 4, then
f 0(0) 5 0, but f has no inflection point at x 5 0.
45. One possible answer:
y
y
4
5
3
y = f(x)
2
1
–5
1
2
3
4
5
6
–5
y
46. One possible answer:
5
4
3
2
1
–1
–2
–3
x
x
–1
36.
5
y
5
2
3
x
37. (a) v(t) 5 s9(t) 5 2t 2 4
(b) a(t) 5 v9(t) 5 2
(c) It begins at position 3 moving in a negative direction. It
moves to position 21 when t 5 2, and then changes
direction, moving in a positive direction thereafter.
–5
5
–5
x
Section 4.4
153
(1 1 ae 2bx)(0) 2 (c)(2abe 2bx)
(1 1 ae )
47. One possible answer:
51. (a) f 9(x) 5 }}}}
2bx 2
y
abce 2bx
(1 1 ae )
(–2, 8) 10
5 }}
2bx 2
(0, 4)
abce bx
(e 1 a)
5 }}
bx
2,
–5
(2, 0)
5
x
so the sign of f 9(x) is the same as the sign of abc.
–10
(e bx 1 a)2(ab 2ce bx) 2 (abce bx)2(e bx 1 a)(be bx)
(e 1 a)
(b) f 0(x) 5 }}}}}
bx
4
48. One possible answer:
(e bx 1 a)(ab 2ce bx) 2 (abce bx)(2be bx)
(e 1 a)
5 }}}}
bx
3
y
8
(6, 7)
ab 2ce bx(e bx 2 a)
(e 1 a)
5 2}}
bx
3
6
(4, 4)
4
2
–2
ln a
b
Since a . 0, this changes sign when x 5 }} due to
(2, 1)
2
4
6
8
the e bx 2 a factor in the numerator, and f (x) has a point
x
of inflection at that location.
–2
52. (a) f 9(x) 5 4ax 3 1 3bx 2 1 2cx 1 d
f 0(x) 5 12ax 2 1 6bx 1 2c
Since f 0(x) is quadratic, it must have 0, 1, or 2 zeros. If
f 0(x) has 0 or 1 zeros, it will not change sign and the
concavity of f (x) will not change, so there is no point
of inflection. If f 0(x) has 2 zeros, it will change sign
twice, and f (x) will have 2 points of inflection.
49. (a) Regression equation:
2161.4541
1 1 28.1336e
y 5 }}}
20.8627x
[0, 8] by [2400, 2300]
(b) At approximately x 5 3.868 (late in 1996), when the
sales are about 1081 million dollars/year
(b) If f has no points of inflection, then f 0(x) has 0 or 1
zeros, so the discriminant of f 0(x) is # 0. This gives
(6b)2 2 4(12a)(2c) # 0, or 3b 2 # 8ac.
If f has 2 points of inflection, then f 0(x) has 2 zeros and
the inequality is reversed, so 3b 2 . 8ac. In summary, f
has 2 points of inflection if and only if 3b 2 . 8ac.
(c) 2161.45 million dollars/year
■ Section 4.4 Modeling and Optimization
b
7
3a
4
which is the x-value where the point of inflection
50. (a) In exercise 13, a 5 4 and b 5 21, so 2}} 5 2}},
(pp. 206–220)
3
2
occurs. The local extrema are at x 5 22 and x 5 2}},
7
4
which are symmetric about x 5 2}}.
b
(b) In exercise 8, a 5 22 and b 5 6, so 2}} 5 1, which
3a
is the x-value where the point of inflection occurs. The
local extrema are at x 5 0 and x 5 2, which are
symmetric about x 5 1.
(c) f 9(x) 5 3ax 2 1 2bx 1 c and
f 0(x) 5 6ax 1 2b.
The point of inflection will occur where
b
3a
If there are local extrema, they will occur at the zeros
of f 9(x). Since f 9(x) is quadratic, its graph is a parabola
and any zeros will be symmetric about the vertex which
will also be where f 0(x) 5 0.
Exploration 1
Constructing Cones
1. The circumference of the base of the cone is the
circumference of the circle of radius 4 minus x, or 8p 2 x.
8p 2 x
2p
Thus, r 5 }}. Use the Pythagorean Theorem to find h,
and the formula for the volume of a cone to find V.
2. The expression under the radical must be nonnegative, that
1
8p 2 x 2
$ 0.
2p
2
is, 16 2 }}
Solving this inequality for x gives: 0 # x # 16p.
f 0(x) 5 0, which is at x 5 2}}.
[0, 16p] by [210, 40]
154
Section 4.4
3. The circumference of the original circle of radius 4 is 8p.
Thus, 0 # x # 8p.
[0, 8p] by [210, 40]
4. The maximum occurs at about x 5 4.61. The maximum
volume is about V 5 25.80.
2p
3
p dh
dh
dr
3 dx
dx
dx
dV
dV
substitute these values in }}, set }} 5 0, and solve for x to
dx
dx
w)p
8(3 2 Ï6
obtain x 5 }} < 4.61.
3
128pÏw
3
Then V 5 }} < 25.80.
27
dV
dx
dr
dx
5. Start with }} 5 }}rh}} 1 }}r 2}}. Compute }} and }},
9. x 2 1 y 2 5 4 and y 5 Ï3wx
x 2 1 (Ï3wx)2 5 4
x 2 1 3x 2 5 4
4x 2 5 4
x 5 61
Since y 5 Ïw3x, the solutions are:
x 5 1 and y 5 Ïw3, or, x 5 21 and y 5 2Ï3w.
In ordered pair notation, the solutions are (1, Ï3w) and
(21, 2Ïw3).
x2
4
y2
9
10. }} 1 }} 5 1 and y 5 x 1 3
x2
(x 1 3)2
}} 1 }} 5 1
4
9
9x 2 1 4(x 1 3)2 5 36
9x 2 1 4x 2 1 24x 1 36 5 36
13x 2 1 24x 5 0
Quick Review 4.4
1. y9 5 3x 2 2 12x 1 12 5 3(x 2 2)2
Since y9 $ 0 for all x (and y9 . 0 for x Þ 2), y is
increasing on (2`, `) and there are no local extrema.
2. y9 5 6x 2 1 6x 2 12 5 6(x 1 2)(x 2 1)
y0 5 12x 1 6
The critical points occur at x 5 22 or x 5 1, since y9 5 0
at these points. Since y0(22) 5 218 , 0, the graph has a
local maximum at x 5 22. Since y0(1) 5 18 . 0, the graph
has a local minimum at x 5 1. In summary, there is a local
maximum at (22, 17) and a local minimum at (1, 210).
1
3
1
3
x(13x 1 24) 5 0
24
13
x 5 0 or x 5 2}}
Since y 5 x 1 3, the solutions are:
24
13
15
13
x 5 0 and y 5 3, or, x 5 2}} and y 5 }}.
In ordered pair notation, the solutions are
1
24 15
13 13
2
(0, 3) and 2}}, }} .
Section 4.4 Exercises
200p
3
3. V 5 }}pr 2h 5 }}p(5)2(8) 5 }} cm3
1. Represent the numbers by x and 20 2 x, where 0 # x # 20.
4. V 5 pr 2h 5 1000
SA 5 2prh 1 2pr 2 5 600
1000
pr
Solving the volume equation for h gives h 5 }}
2 .
Substituting into the surface area equation gives
2000
}} 1 2pr 2 5 600. Solving graphically, we have
r
(a) The sum of the squares is given by
f (x) 5 x 2 1 (20 2 x)2 5 2x 2 2 40x 1 400. Then
f 9(x) 5 4x 2 40. The critical point and endpoints occur
at x 5 0, x 5 10, and x 5 20. Then f (0) 5 400,
f (10) 5 200, and f (20) 5 400. The sum of the squares
is as large as possible for the numbers 0 and 20, and is
as small as possible for the numbers 10 and 10.
Graphical support:
r < 211.14, r < 4.01, or r < 7.13. Discarding the negative
1000
pr
value and using h 5 }}
2 to find the corresponding values
of h, the two possibilities for the dimensions of the cylinder
are:
r < 4.01 cm and h < 19.82 cm, or,
r < 7.13 cm and h < 6.26 cm.
5. Since y 5 sin x is an odd function, sin (2a) 5 2sin a.
6. Since y 5 cos x is an even function, cos (2a) 5 cos a.
7.
sin (p 2 a) 5 sin p cos a 2 cos p sin a
5 0 cos a 2 (21) sin a
5 sin a
8. cos (p 2 a) 5 cos p cos a 1 sin p sin a
5 (21) cos a 1 0 sin a
5 2cos a
[0, 20] by [0, 450]
(b) The sum of one number plus the square root of the
other is given by g(x) 5 x 1 Ï2w0ww
2wx. Then
1
g9(x) 5 1 2 }}. The critical point occurs when
2Ï2
2wx
w0ww
1
79
2Ïw2w0w
2wx 5 1, so 20 2 x 5 }} and x 5 }}. Testing the
4
4
endpoints and critical point, we find
142
79
81
4
g(0) 5 Ï2w0w < 4.47, g }} 5 }} 5 20.25, and
g(20) 5 20.
Section 4.4
The sum is as large as possible when the numbers are
1
79
1
79
}} and }} summing }} +
4
4
4
155
Graphical support:
!}§4}2, and is as small as
1
possible when the numbers are 0 and 20
(summing 0 + Ï2w0w).
[0, 20] by [0, 40]
Graphical support:
4. Let x represent the length of the rectangle in meters
(0 , x , 4). Then the width is 4 2 x and the area is
A(x) 5 x(4 2 x) 5 4x 2 x 2. Since A9(x) 5 4 2 2x, the
critical point occurs at x 5 2. Since A9(x) . 0 for
0 , x , 2 and A9(x) , 0 for 2 , x , 4, this critical point
corresponds to the maximum area. The rectangle with the
largest area measures 2 m by 4 2 2 5 2m, so it is a square.
[0, 20] by [210, 25]
2. Let x and y represent the legs of the triangle, and note that
Graphical support:
0 , x , 5. Then x 2 1 y 2 5 25, so y 5 Ï2w5
ww
2wx 2w (since
1
2
1
2
y . 0). The area is A 5 }}xy 5 }}xÏ2w5ww
2wx 2w, so
dA
1
1
1
w5ww
2wx 2w
}} 5 }}x}}(22x) 1 }}Ï2
dx
2 2Ï2
2
2wx 2w
w5ww
[0, 4] by [21.5, 5]
5. (a) The equation of line AB is y 5 2x 1 1, so the
y-coordinate of P is 2x 1 1.
25 2 2x 2
5 }}.
2Ï2
ww5w
2wx 2w
(b) A(x) 5 2x(1 2 x)
The critical point occurs when 25 2 2x 2 5 0, which means
5
x 5 }}, (since x . 0). This value corresponds to the
Ï2w
dA
5
largest possible area, since }} . 0 for 0 , x , }} and
dx
Ï2w
dA
5
5
}} , 0 for }} , x , 5. When x 5 }}, we have
dx
Ï2w
Ïw2
5 2
5
y 5 25 2 }} 5 }} and
Ïw2
Ïw2
1
1 5 2
25
A 5 }}xy 5 }} }} 5 }}. Thus, the largest possible area is
2
2 Ï2
4
w
!§§§§1§§§2
1 2
d
dx
1
1
occurs at x 5 }}. Since A9(x) . 0 for 0 , x , }} and
2
2
1
A9(x) , 0 for }} , x , 1, this critical point corresponds
2
(c) Since A9(x) 5 }}(2x 2 2x 2) 5 2 2 4x, the critical point
to the maximum area. The largest possible area is
122
1
1
2
A }} 5 }} square unit, and the dimensions of the
1
2
rectangle are }} unit by 1 unit.
Graphical support:
25
5
5
}} cm2, and the dimensions (legs) are }} cm by }} cm.
4
Ï2w
Ï2w
Graphical support:
[0, 1] by [20.5, 1]
[0, 5] by [22, 7]
3. Let x represent the length of the rectangle in inches (x . 0).
16
x
Then the width is }} and the perimeter is
1
16
x
2
32
x
2(x2 2 16)
Since P9(x) 5 2 2 32x 22 5 }}
the critical point
x2
P(x) 5 2 x 1 }} 5 2x 1 }}.
6. If the upper right vertex of the rectangle is located at
(x, 12 2 x 2) for 0 , x , Ï1w2w, then the rectangle’s
dimensions are 2x by 12 2 x 2 and the area is
A(x) 5 2x(12 2 x 2) 5 24x 2 2x 3. Then
A9(x) 5 24 2 6x 2 5 6(4 2 x 2), so the critical point
(for 0 , x , Ïw1w2) occurs at x 5 2. Since A9(x) . 0 for
0 , x , 2 and A9(x) , 0 for 2 , x , Ïw1w2, this critical
point corresponds to the maximum area. The largest
possible area is A(2) 5 32, and the dimensions are 4 by 8.
Graphical support:
occurs at x 5 4. Since P9(x) , 0 for 0 , x , 4 and
P9(x) . 0 for x . 0, this critical point corresponds to the
minimum perimeter. The smallest possible perimeter is
P(4) 5 16 in., and the rectangle’s dimensions are
4 in. by 4 in.
[0, Ï1w2w] by [210, 40]
156
Section 4.4
7. Let x be the side length of the cut-out square (0 , x , 4).
Then the base measures 8 2 2x in. by 15 2 2x in.,
and the volume is
V(x) 5 x(8 2 2x)(15 2 2x) 5 4x 3 2 46x 2 1 120x. Then
V9(x) 5 12x 2 2 92x 1 120 5 4(3x 2 5)(x 2 6). Then the
5
3
5
5
V9(x) . 0 for 0 , x , }} and V9(x) , 0 for }} , x , 4, the
3
3
critical point (in 0 , x , 4) occurs at x 5 }}. Since
9. Let x be the length in meters of each side that adjoins the
river. Then the side parallel to the river measures
800 2 2x meters and the area is
A(x) 5 x(800 2 2x) 5 800x 2 2x 2 for 0 , x , 400.
Therefore, A9(x) 5 800 2 4x and the critical point occurs at
x 5 200. Since A9(x) . 0 for 0 , x , 200 and A9(x) , 0
for 200 , x , 400, the critical point corresponds to the
maximum area. The largest possible area is
A(200) 5 80,000 m2 and the dimensions are 200 m
(perpendicular to the river) by 400 m (parallel to the river).
Graphical support:
critical point corresponds to the maximum volume.
132
5
2450
27
5
14
35
dimensions are }} in. by }} in. by }} in.
3
3
3
The maximum volume is V }} 5 }} < 90.74 in3, and the
[0, 400] by [225,000, 90,000]
Graphical support:
10. If the subdividing fence measures x meters, then the
216
x
pea patch measures x m by }} m and the amount of fence
216
x
needed is f (x) 5 3x 1 2}} 5 3x 1 432x 21. Then
f 9(x) 5 3 2 432x 22 and the critical point (for x . 0)
[0, 4] by [225, 100]
8. Note that the values a and b must satisfy a 2 1 b 2 5 202
and so b 5 Ï4w0w0ww
2w
a 2w. Then the area is given by
1
2
1
2
A 5 }}ab 5 }}aÏ4w0w0ww
2w
a 2w for 0 , a , 20, and
1
2
dA
1
1
1
w0w0ww
2w
a 2w
}} 5 }}a }} (22a) 1 }}Ï4
da
2 2Ï4w0ww0w
2
2w
a 2w
2a 2 1 (400 2 a 2)
200 2 a 2
5 }} 5 }}. The critical point occurs
2Ï4w0w0ww
2w
a 2w
2w
a 2w
Ïw40ww0w
occurs at x 5 12. Since f 9(x) , 0 for 0 , x , 12 and
f 9(x) . 0 for x . 12, the critical point corresponds to the
minimum total length of fence. The pea patch will measure
12 m by 18 m (with a 12-m divider), and the total amount
of fence needed is f (12) 5 72 m.
Graphical support:
dA
da
when a 2 5 200. Since }} . 0 for 0 , a , Ï2w0w0w and
dA
}} , 0 for
da
Ï2w0w0w , a , 20, this critical point corresponds
to the maximum area. Furthermore, if a 5 Ï2w0w0w then
2w
a 2w 5 Ï2w0w0w, so the maximum area occurs
b 5 Ï4w0w0ww
when a 5 b.
[0, 40] by [0, 250]
11. (a) Let x be the length in feet of each side of the square
500
x
base. Then the height is }}
2 ft and the surface area
(not including the open top) is
Graphical support:
1x 2
500
2
21
S(x) 5 x 2 1 4x }}
2 5 x 1 2000x . Therefore,
2(x 3 2 1000)
x
S9(x) 5 2x 2 2000x 22 5 }}
and the critical
2
point occurs at x 5 10. Since S9(x) , 0 for 0 , x , 10
[0, 20] by [230, 110]
and S9(x) . 0 for x . 10, the critical point corresponds
to the minimum amount of steel used. The dimensions
should be 10 ft by 10 ft by 5 ft, where the height is 5 ft.
(b) Assume that the weight is minimized when the total
area of the bottom and the four sides is minimized.
Section 4.4
15. We assume that a and b are held constant. Then
1125
x
12. (a) Note that x 2y 5 1125, so y 5 }}
2 . Then
1
2
1
2
p
(for 0 , u , p) occurs at u 5 }}. Since A9(u) . 0 for
2
p
p
0 , u , }} and A9(u) , 0 for }} , u , p, the critical point
2
2
A(u) 5 }}ab sin u and A9(u) 5 }}ab cos u. The critical point
c 5 5(x 2 1 4xy) 1 10xy
5 5x 2 1 30xy
1
1125
x
2
5 5x 2 1 30x }}
2
corresponds to the maximum area. The angle that
21
5 5x 1 33,750x
2
157
p
2
maximizes the triangle’s area is u 5 }} (or 908).
dc
10(x 3 2 3375)
}} 5 10x 2 33,750x 22 5 }}
dx
x2
dc
dx
The critical point occurs at x 5 15. Since }} , 0 for
16. Let the can have radius r cm and height h cm. Then
dc
0 , x , 15 and }} . 0 for x . 15, the critical point
dx
pr 2h 5 1000, so h 5 }}
2 . The area of material used is
corresponds to the minimum cost. The values of x and
A 5 pr 2 1 2prh 5 pr 2 1 }}, so
y are x 5 15 ft and y 5 5 ft.
(b) The material for the tank costs 5 dollars/sq ft and the
excavation charge is 10 dollars for each square foot of
the cross-sectional area of one wall of the hole.
13. Let x be the height in inches of the printed area. Then the
50
x
50
dimensions are x 1 8 in. by }} 1 4 in. The amount of
x
width of the printed area is }} in. and the overall
paper used is
1
50
x
2
1000
pr
2000
r
dA
2pr 3 2 2000
. The critical point
}} 5 2pr 2 2000r 22 5 }}
dr
r2
3 1000
dA
occurs at r 5 }} 5 10p21/3 cm. Since }} , 0 for
p
dr
dA
0 , r , 10p21/3 and }} . 0 for r . 10p21/3, the critical
dr
!§§§§
point corresponds to the least amount of material used and
hence the lightest possible can. The dimensions are
r 5 10p21/3 < 6.83 cm and h 5 10p21/3 < 6.83 cm. In
Example 2, because of the top of the can, the “best” design
is less big around and taller.
400
x
A(x) 5 (x 1 8) }} 1 4 5 4x 1 82 1 }} in2. Then
A9(x) 5 4 2 400x
22
4(x 2 2 100)
x
5 }}
and the critical point
2
(for x . 0) occurs at x 5 10. Since A9(x) , 0 for
0 , x , 10 and A9(x) . 0 for x . 10, the critical point
corresponds to the minimum amount of paper. Using
50
x
x 1 8 and }} 1 4 for x 5 10, the overall dimensions are
18 in. high by 9 in. wide.
14. (a) s(t) 5 216t 1 96t 1 112
v(t) 5 s9(t) 5 232t 1 96
At t 5 0, the velocity is v(0) 5 96 ft/sec.
2
(b) The maximum height occurs when v(t) 5 0, when
t 5 3. The maximum height is s(3) 5 256 ft and it
occurs at t 5 3 sec.
(c) Note that
s(t) 5 216t 2 1 96t 1 112 5 216(t 1 1)(t 2 7),
so s 5 0 at t 5 21 or t 5 7. Choosing the positive
value of t, the velocity when s 5 0 is
v(7) 5 2128 ft/sec.
1000
pr
17. Note that pr 2h 5 1000, so h 5 }}
2 . Then
2000
r
dA
16(r 3 2 125)
. The critical point
}} 5 16r 2 2000r22 5 }}
dr
r2
3
dA
occurs at r 5 Ï1w2w5w 5 5 cm. Since }} , 0 for 0 , r , 5
dr
dA
and }} . 0 for r . 5, the critical point corresponds to the
dr
A 5 8r 2 1 2prh 5 8r 2 1 }}, so
least amount of aluminum used or wasted and hence the
most economical can. The dimensions are r 5 5 cm and
40
p
8
p
h 5 }}, so the ratio of h to r is }} to 1.
158
Section 4.4
15 2 2x
2
(d) V9(x) 5 24x 2 2 336x 1 864 5 24(x 2 2 14x 1 36)
The critical point is at
18. (a) The base measures 10 2 2x in. by }} in., so the
volume formula is
w2w
14 6 Ï(2
w1w4w)w2w
2w4(1
w)(
w3w6w)w
14 6 Ï5
x 5 }}} 5 }} 5 7 6 Ï1w3w,
x(10 2 2x)(15 2 2x)
2
2(1)
V(x) 5 }}} 5 2x 3 2 25x 2 1 75x.
2
that is, x < 3.39 or x < 10.61. We discard the larger
value because it is not in the domain. Since
V0(x) 5 24(2x 2 14), which is negative when x < 3.39,
the critical point corresponds to the maximum volume.
The maximum value occurs at x 5 7 2 Ïw1w3 < 3.39,
which confirms the results in (c).
(b) We require x . 0, 2x , 10, and 2x , 15. Combining
these requirements, the domain is the interval (0, 5).
(e) 8x 3 2 168x 2 1 864x 5 1120
8(x 3 2 21x 2 1 108x 2 140) 5 0
8(x 2 2)(x 2 5)(x 2 14) 5 0
Since 14 is not in the domain, the possible values of x
are x 5 2 in. or x 5 5 in.
[0, 5] by [220, 80]
(c)
(f) The dimensions of the resulting box are 2x in.,
(24 2 2x) in., and (18 2 2x) in. Each of these
measurements must be positive, so that gives the
domain of (0, 9).
[0, 5] by [220, 80]
20.
6 mi
The maximum volume is approximately 66.02 in3 when
x < 1.96 in.
x
2 mi
(d) V9(x) 5 6x 2 2 50x 1 75
6–x
Village
4 + x2 miles
Ïwwww
Jane
The critical point occurs when V9(x) 5 0, at
w0w
50 6 Ï(2
w5w0w)w2w
2w4(6
w)(
w7w5w)w
50 6 Ïw70
x 5 }}} 5 }}
Let x be the distance from the point on the shoreline nearest
2(6)
12
25 6 5Ïw7
5 }}, that is, x < 1.96 or x < 6.37. We discard
6
Jane’s boat to the point where she lands her boat. Then she
the larger value because it is not in the domain. Since
5 mph. The total amount of time to reach the village is
V0(x) 5 12x 2 50, which is negative when x < 1.96,
Ïw4w
62x
1wx w2
f (x) 5 }} 1 }} hours (0 # x # 6). Then
the critical point corresponds to the maximum volume.
The maximum volume occurs when
25 2 5Ï7w
x 5 }} < 1.96, which confirms the result in (c).
6
needs to row Ï4ww
1wx 2w mi at 2 mph and walk 6 2 x mi at
5
2
1
1
1
x
1
f 9(x) 5 }} }}(2x) 2 }} 5 }} 2 }}. Solving
2
2
2 2Ïw
5
5
1wx w
1wx w
4w
2Ï4
ww
f 9(x) 5 0, we have:
x
1
} } 5 }}
5
1wx 2w
2Ïw
4w
5x 5 2Ï4ww
1wx 2w
19. (a) The “sides” of the suitcase will measure 24 2 2x in. by
18 2 2x in. and will be 2x in. apart, so the volume
formula is
V(x) 5 2x(24 2 2x)(18 2 2x) 5 8x 3 2 168x 2 1 864x.
25x 2 5 4(4 1 x 2)
21x 2 5 16
(b) We require x . 0, 2x , 18, and 2x , 24. Combining
these requirements, the domain is the interval (0, 9).
4
x 5 6}}
Ï2w1w
We discard the negative value of x because it is not in the
domain. Checking the endpoints and critical point, we have
[0, 9] by [2400, 1600]
(c)
[0, 9] by [2400, 1600]
The maximum volume is approximately 1309.95 in3
when x < 3.39 in.
1
4
2
f (0) 5 2.2, f }} < 2.12, and f(6) < 3.16. Jane should
Ïw21w
4
land her boat }} < 0.87 miles down the shoreline from
Ïw21w
the point nearest her boat.
Section 4.4
21. If the upper right vertex of the rectangle is located at
(x, 4 cos 0.5x) for 0 , x , p, then the rectangle has width
2x and height 4 cos 0.5x, so the area is A(x) 5 8x cos 0.5x.
Then A9(x) 5 8x(20.5 sin 0.5x) 1 8(cos 0.5x)(1)
5 24x sin 0.5x 1 8 cos 0.5x.
Solving A9(x) graphically for 0 , x , p, we find that
x < 1.72. Evaluating 2x and 4 cos 0.5x for x < 1.72, the
dimensions of the rectangle are approximately
3.44 (width) by 2.61 (height), and the maximum area is
approximately 8.98.
159
(c)
[0, 1.1] by [20.2, 0.6]
(d) Quadratic:
A < 20.91a 2 1 0.54a 1 0.34
22. Let the radius of the cylinder be r cm, 0 , r , 10. Then
the height is 2Ï1w0w0ww
2wr 2w and the volume is
V(r) 5 2pr 2Ï1w0w0ww
2wr 2w cm3. Then
1
[20.5, 1.5] by [20.2, 0.6]
Cubic:
A < 1.74 a 3 2 3.78a 2 1 1.86a 1 0.19
2
1
2wr 2w)(2r)
V9(r) 5 2pr 2 }} (22r) 1 (2pÏ1w0w0ww
2Ï1
w0w0ww
2wr 2w
22pr 3 1 4pr(100 2 r 2)
5 }}}
Ïw1w0w0w
2wr 2w
2pr(200 2 3r 2)
5 }}
Ïw1w0w0w
2wr 2w
The critical point for 0 , r , 10 occurs at
[20.5, 1.5] by [20.2, 0.6]
Quartic:
A < 21.92a 4 1 5.96a 3 2 6.87a 2 1 2.71a 1 0.12
!}§3§}§ 5 10!}§3}. Since V9(r) . 0 for
2
2
0 , r , 10!}§} and V9(r) , 0 for 10!}§} < r < 10, the
3
3
r5
200
2
critical point corresponds to the maximum volume. The
!§
2
3
dimensions are r 5 10 }} < 8.16 cm and
[20.5, 1.5] by [20.2, 0.6]
(e) Quadratic:
’
20
h 5 }} < 11.55 cm, and the volume is
Ïw3
4000p
}} < 2418.40 cm3.
3Ï3w
23. (a) f 9(x) 5 x(2e 2x) 1 e 2x(1) 5 e 2x(1 2 x)
The critical point occurs at x 5 1. Since f 9(x) . 0 for
0 # x , 1 and f 9(x) , 0 for x . 1, the critical point
corresponds to the maximum value of f. The absolute
maximum of f occurs at x 5 1.
(b) To find the values of b, use grapher techniques to solve
xe 2x 5 0.1e 20.1, xe 2x 5 0.2e 20.2, and so on. To find
the values of A, calculate (b 2 a)ae 2a, using the
unrounded values of b . (Use the list features of the
grapher in order to keep track of the unrounded values
for part (d).)
a
b
A
0.1 3.71 0.33
0.2 2.86 0.44
0.3 2.36 0.46
[20.5, 1.5] by [20.2, 0.6]
According to the quadratic regression equation, the
maximum area occurs at a < 0.30 and is approximately
0.42.
Cubic:
[20.5, 1.5] by [20.2, 0.6]
According to the cubic regression equation, the
maximum area occurs at a < 0.31 and is approximately
0.45.
Quartic:
0.4 2.02 0.43
0.5 1.76 0.38
0.6 1.55 0.31
0.7 1.38 0.23
0.8 1.23 0.15
0.9 1.11 0.08
1.0 1.00 0.00
[20.5, 1.5] by [20.2, 0.6]
According to the quartic regression equation the
maximum area occurs at a < 0.30 and is approximately
0.46.
160
Section 4.4
24. (a) f 9(x) is a quadratic polynomial, and as such it can have
0, 1, or 2 zeros. If it has 0 or 1 zeros, then its sign
never changes, so f (x) has no local extrema.
If f 9(x) has 2 zeros, then its sign changes twice, and
f (x) has 2 local extrema at those points.
26. Since 2x 1 2y 5 36, we know that y 5 18 2 x. In part (a),
x
2p
the radius is }} and the height is 18 2 x, and so the
volume is given by
and so f 0(x) 5 2 1 32x 23, so f 0(2) 5 6, which is
positive as expected. So, use a 5 16.
(b) We require f 0(1) 5 0. Since f 0(x) 5 2 1 2ax 23, we
have f 0(1) 5 2 1 2a, so our requirement is that
2 1 2a 5 0. Therefore, a 5 21. To verify that x 5 1 is
in fact an inflection point, note that we now have
f 0(x) 5 2 2 2x 23, which is negative for 0 , x , 1 and
positive for x . 1. Therefore, the graph of f is concave
down in the interval (0, 1) and concave up in the
interval (1, `), So, use a 5 21.
2x 3 2 a
x
a 1/3
f 9(x) occurs at x 5 }} , where the sign changes from
2
29. f 9(x) 5 2x 2 ax 22 5 }}
, so the only sign change in
2
12
negative to positive. This means there is a local
1
4p
pr 2h 5 p }} (18 2 x) 5 }}x 2(18 2 x). In part (b), the
radius is x and the height is 18 2 x, and so the volume is
given by pr h 5 px (18 2 x). Thus, each problem requires
2
a
4
requirement is that 4 2 }} 5 0. Therefore, a 5 16. To
minimum, note that we now have f 9(x) 5 2x 2 16x 22
25. Let x be the length in inches of each edge of the square
end, and let y be the length of the box. Then we require
4x 1 y # 108. Since our goal is to maximize volume, we
assume 4x 1 y 5 108 and so y 5 108 2 4x. The volume is
V(x) 5 x 2(108 2 4x) 5 108x 2 2 4x 3, where 0 , x , 27.
Then V9 5 216x 2 12x 2 5 212x(x 2 18), so the critical
point occurs at x 5 18 in. Since V9(x) . 0 for 0 , x , 18
and V9(x) , 0 for 18 , x , 27, the critical point
corresponds to the maximum volume. The dimensions of
the box with the largest possible volume are
18 in. by 18 in. by 36 in.
1 2
a
4
f 9(x) 5 2x 2 ax 22, we have f 9(2) 5 4 2 }} and so our
verify that the critical point corresponds to a local
(b) Possible answers:
No local extrema: y 5 x 3;
2 local extrema: y 5 x 3 2 3x
x 2
2p
28. (a) We require f (x) to have a critical point at x 5 2. Since
2
us to find the value of x that maximizes f (x) 5 x 2(18 2 x)
in the interval 0 , x , 18, so the two problems have the
same answer.
To solve either problem, note that f (x) 5 18x 2 2 x 3 and so
f 9(x) 5 36x 2 3x 2 5 23x(x 2 12). The critical point
occurs at x 5 12. Since f 9(x) . 0 for 0 , x , 12 and
f 9(x) , 0 for 12 , x , 18, the critical point corresponds to
the maximum value of f (x). To maximize the volume in
either part (a) or (b), let x 5 12 cm and y 5 6 cm.
27. Note that h 2 1 r 2 5 3 and so r 5 Ï3ww
2w
h 2w. Then the
p
p
p
3
3
3
dV
2
2
for 0 , h , Ï3w, and so }} 5 p 2 ph 5 p(1 2 h ). The
dh
dV
critical point (for h . 0) occurs at h 5 1. Since }} . 0 for
dh
dV
0 , h , 1 and }} , 0 for 1 , h , Ï3w, the critical point
dh
volume is given by V 5 }}r 2h 5 }}(3 2 h 2)h 5 ph 2 }}h 3
corresponds to the maximum volume. The cone of greatest
2p
3
volume has radius Ï2w m, height 1 m, and volume }} m3.
minimum at that point, and there are no local maxima.
30. (a) Note that f 9(x) 5 3x 2 1 2ax 1 b. We require
f 9(21) 5 0 and f 9(3) 5 0, which give 3 2 2a 1 b 5 0
and 27 1 6a 1 b 5 0. Subtracting the first equation
from the second, we have 24 1 8a 5 0 and so a 5 23.
Substituting into the first equation, we have 9 1 b 5 0,
so b 5 29. Therefore, our equation for
f (x) is f (x) 5 x 3 2 3x 2 2 9x. To verify that we have a
local maximum at x 5 21 and a local minimum at
x 5 3, note that
f 9(x) 5 3x2 2 6x 2 9 5 3(x 1 1)(x 2 3), which is
positive for x , 21, negative for 21 , x , 3, and
positive for x . 3. So, use a 5 23 and b 5 29.
(b) Note that f 9(x) 5 3x 2 1 2ax 1 b and f 0(x) 5 6x 1 2a.
We require f 9(4) 5 0 and f 0(1) 5 0, which give
48 1 8a 1 b 5 0 and 6 1 2a 5 0. By the second
equation, a 5 23, and so the first equation becomes
48 2 24 1 b 5 0. Thus b 5 224. To verify that we
have a local minimum at x 5 4, and an inflection
point at x 5 1, note that we now have f 0(x) 5 6x 2 6.
Since f 0 changes sign at x 5 1 and is positive at x 5 4,
the desired conditions are satisfied. So, use a 5 23 and
b 5 224.
161
Section 4.4
31. Refer to the illustration in the problem statement. Since
33. (a) Note that w 2 1 d 2 5 122, so d 5 Ï1w4w4ww
2w
w 2w. Then we
x 2 1 y 2 5 9, we have x 5 Ï9ww
2wy 2w. Then the volume of
may write S 5 kwd 3 5 kw(144 2 w 2)3/2, so
the cone is given by
dS
}} 5 kw
dw
1
1
3
3
1
5 }}p(9 2 y 2)(y 1 3)
3
p
5 }}(2y 3 2 3y 2 1 9y 1 27),
3
V 5 }}pr 2h 5 }}px 2(y 1 3)
5 (kÏ1w4w4ww
2w
w 2w)(23w 2 1 144 2 w 2)
5 (24kÏ1w4w4ww
2w
w 2w)(w 2 2 36)
The critical point (for 0 , w , 12) occurs at w 5 6.
for 23 , y , 3.
dS
dw
dS
dw
Since }} . 0 for 0 , w , 6 and }} , 0 for
dV
p
}} 5 }}(23y 2 2 6y 1 9) 5 2p(y 2 1 2y 2 3)
dy
3
Thus
3
? }2}(144 2 w2)1/2(22w) 1 k(144 2 w2)3/2(1)
6 , w , 12, the critical point corresponds to the
5 2p(y 1 3)(y 2 1), so the critical point in
dV
the interval (23, 3) is y 5 1. Since }} . 0 for 23 , y , 1
dy
dV
and }} , 0 for 1 , y , 3, the critical point does
dy
32p
correspond to the maximum value, which is V(1) 5 }}
3
maximum stiffness. The dimensions are 6 in. wide by
6Ï3w in. deep.
(b)
cubic units.
32. (a) Note that w 2 1 d 2 5 122, so d 5 Ï1w4w4ww
2w
w 2w. Then we
[0, 12] by [22000, 8000]
The graph of S 5 w(144 2 w2)3/2 is shown. The
maximum stiffness shown in the graph occurs at w 5 6,
which agrees with the answer to part (a).
may write S 5 kwd 2 5 kw(144 2 w 2) 5 144kw 2 kw 3
for 0 , w , 12,
dS
dw
so }} 5 144k 2 3kw 2 5 23k(w 2 2 48). The critical
(c)
point (for 0 , w , 12) occurs at w 5 Ï4w8w 5 4Ï3w.
dS
dw
dS
dw
Since }} . 0 for 0 , w , 4Ï3w and }} , 0 for
4Ï3w , w , 12, the critical point corresponds to the
maximum strength. The dimensions are 4Ï3w in. wide
by 4Ï6w in. deep.
(b)
[0, 12] by [22000, 8000]
The graph of S 5 d 3Ï1w4w4ww
2w
d 2w is shown. The
maximum stiffness shown in the graph occurs at
d 5 6Ïw3 < 10.4 agrees with the answer to part (a),
and its value is the same as the maximum value found
in part (b), as expected.
Changing the value of k changes the maximum
stiffness, but not the dimensions of the stiffest beam.
The graphs for different values of k look the same
except that the vertical scale is different.
[0, 12] by [2100, 800]
The graph of S 5 144w 2 w 3 is shown. The maximum
strength shown in the graph occurs at w 5 4Ï3w < 6.9,
which agrees with the answer to part (a).
34. (a) v(t) 5 s9(t) 5 210p sin pt
The speed at time t is 10p)sin pt). The maximum speed
1
2
(c)
3
2
5
2
is 10p cm/sec and it occurs at t 5 }}, t 5 }}, t 5 }}, and
7
2
t 5 }} sec. The position at these times is s 5 0 cm (rest
position), and the acceleration
[0, 12] by [2100, 800]
The graph of S 5 d Ï1w4w4ww
2w
dw is shown. The
maximum strength shown in the graph occurs at
d 5 4Ïw6 < 9.8, which agrees with the answer to part
(a), and its value is the same as the maximum value
found in part (b), as expected.
2
2
Changing the value of k changes the maximum
strength, but not the dimensions of the strongest beam.
The graphs for different values of k look the same
except that the vertical scale is different.
a(t) 5 v9(t) 5 210p 2 cos pt is 0 cm/sec2 at these
times.
(b) Since a(t) 5 210p2 cos pt, the greatest magnitude of
the acceleration occurs at t 5 0, t 5 1, t 5 2, t 5 3, and
t 5 4. At these times, the position of the cart is either
s 5 210 cm or s 5 10 cm, and the speed of the cart is
0 cm/sec.
162
Section 4.4
di
dt
35. Since }} 5 22 sin t 1 2 cos t, the largest magnitude of the
x 2 is positive, it has an absolute minimum at the point
current occurs when 22 sin t 1 2 cos t 5 0, or
sin t 5 cos t. Squaring both sides gives sin2 t 5 cos2 t, and
1
2
we know that sin2 t 1 cos2 t 5 1, so sin2 t 5 cos2 t 5 }}.
p 3p 5p
4 4 4
Thus the possible values of t are }}, }}, }}, and so on.
Eliminating extraneous solutions, the solutions of
p
4
sin t 5 cos t are t 5 }} 1 kp for integers k, and at these
times )i) 5 )2 cos t 1 2 sin t) 5 2Ï2w. The peak current is
2Ï2w amps.
36. The square of the distance is
1
12 42
1 3
where f 9(x) 5 2x 2 1 5 0, and that point is }}, }} .
39. (a) Because f (x) is periodic with period 2p.
(b) No. Since f (x) is continuous on [0, 2p], its absolute
minimum occurs at a critical point or endpoint.
Find the critical points in [0, 2p]:
f 9(x) 5 24 sin x 2 2 sin 2x 5 0
24 sin x 2 4 sin x cos x 5 0
24(sin x)(1 1 cos x) 5 0
sin x 5 0 or cos x 5 21
x 5 0, p, 2p
The critical points (and endpoints) are (0, 8), (p, 0),
and (2p, 8). Thus, f (x) has an absolute minimum at
(p, 0) and it is never negative.
40. (a)
3 2
9
1 (Ïxw 1 0)2 5 x 2 2 2x 1 }},
2
4
D(x) 5 x 2 }}
38. No. Since f (x) is a quadratic function and the coefficient of
2
so D9(x) 5 2x 2 2 and the critical point occurs at x 5 1.
Since D9(x) , 0 for x , 1 and D9(x) . 0 for x . 1, the
critical point corresponds to the minimum distance. The
Ïw
minimum distance is ÏD
w(1
w)w 5 }}5 .
2 sin t 5 sin 2t
2 sin t 5 2 sin t cos t
2(sin t)(1 2 cos t) 5 0
sin t 5 0 or cos t 5 1
t 5 kp, where k is an integer
The masses pass each other whenever t is an integer
multiple of p seconds.
(b) The vertical distance between the objects is the
absolute value of f (x) 5 sin 2t 2 2 sin t.
Find the critical points in [0, 2p]:
2
37. Calculus method:
f 9(x) 5 2 cos 2t 2 2 cos t 5 0
The square of the distance from the point (1, Ï3w) to
2(2 cos2 t 2 1) 2 2 cos t 5 0
(x, Ï1w6ww
2wx 2w) is given by
2(2 cos2 t 2 cos t 2 1) 5 0
D(x) 5 (x 2 1)2 1 (Ï1w6ww
2wx 2w 2 Ï3w)2
2(2 cos t 1 1)(cos t 2 1) 5 0
5 x 2 2 2x 1 1 1 16 2 x 2 2 2Ï4w8ww
2w3w
x2 1 3
1
5 22x 1 20 2 2Ï4w8ww
2w3w
x 2. Then
2
cos t 5 2}} or cos t 5 1
2
2p 4p
6x
D9(x) 5 22 2 }}(26x) 5 22 1 }}.
2w3xw2
2w3xw2
2Ï4
w8ww
Ï4w8ww
Solving D9(x) 5 0, we have:
6x 5 2Ï4w8ww
2w
3w
x2
2
2
36x 5 4(48 2 3x )
9x 2 5 48 2 3x 2
12x 2 5 48
x 5 62
We discard x 5 22 as an extraneous solution, leaving
x 5 2. Since D9(x) , 0 for 24 , x , 2 and D9(x) . 0 for
2 , x , 4, the critical point corresponds to the minimum
distance. The minimum distance is Ïw
Dw
(2w) 5 2.
t 5 }}, }}, 0, 2p
3
The critical points (and endpoints) are (0, 0),
3Ï3w
2p
2p
3
The distance is greatest when t 5 }} sec and when
4p
3Ïw3
t 5 }} sec. The distance at those times is }} meters.
3
the semicircle is the distance along the radius containing
the point (1, Ï3w). That distance is 4 2 2 5 2.
p
3
p
p
sin t 5 sin t cos }} 1 cos t sin }}
3
3
Ïw3
1
sin t 5 }} sin t 1 }} cos t
2
2
Ïw3
1
}} sin t 5 }} cos t
2
2
2
sin t 5 sin (t 1 }})
41. (a)
The semicircle is centered at the origin and has radius 4.
Ï1w2w1
ww(Ï
w3ww
)2 5 2. The shortest distance from the point to
4p 3Ï3w
1}3}, 2}2}2, 1}3}, }2}2, and (2p, 0)
Geometry method:
The distance from the origin to (1, Ï3w) is
3
tan t 5 Ï3w
p
3
Solving for t, the particles meet at t 5 }} sec and at
4p
3
t 5 }} sec.
163
Section 4.4
(b) The distance between the particles is the absolute value
42. The trapezoid has height (cos u) ft and the trapezoid bases
Ï3w
p
1
of f (t) 5 sin t 1 }} 2 sin t 5 }} cos t 2 }} sin t. Find
3
2
2
measure 1 ft and (1 1 2 sin u) ft, so the volume is given by
the critical points in [0, 2p]:
V(u) 5 }}(cos u)(1 1 1 1 2 sin u)(20)
1
2
1
2
Ïw3
1
f 9(t) 5 2}} sin t 2 }} cos t 5 0
5 20(cos u)(1 1 sin u).
2
Ïw3
1
2}} sin t 5 }} cos t
2
2
1
tan t 5 2}}
Ïw3
5p
11p
The solutions are t 5 }} and t 5 }}, so the critical
6
6
5p
11p
points are at }}, 21 and }}, 1 , and the interval
6
6
Ïw3
Ïw3
endpoints are at 0, }} , and 2p, }} . The particles
2
2
5p
11p
are farthest apart at t 5 }} sec and at t 5 }} sec, and
6
6
2
1
2
1
1
2
V9(u) 5 20(cos u)(cos u) 1 20(1 1 sin u)(2sin u)5 0
20 cos2 u 2 20 sin u 2 20 sin2 u 5 0
20(1 2 sin2 u) 2 20 sin u 2 20 sin2 u 5 0
2
1
220(2 sin2 u 1 sin u 2 1) 5 0
2
the maximum distance between the particles is 1 m.
(c) We need to maximize f 9(t), so we solve f 0(t) 5 0.
220(2 sin u 2 1)(sin u 1 1) 5 0
1
2
sin u 5 }} or sin u 5 21
p
16
p
6
volume is maximized when u 5 }}.
p
4p
solutions are t 5 }} sec and t 5 }} sec.
3
3
43. (a)
D
C
8.5
R
S
y
For the function y 5 f 9(t), the critical points occur at
p
4p
}}, 21 and }}, 1 , and the interval endpoints are at
3
3
1
1
0, 2}} and 2p, 2}} .
2
2
p
4p
Thus, ) f 9(t)) is maximized at t 5 }} and t 5 }}. But
3
3
2
2
1
1
2
2
these are the instants when the particles pass each
other, so the graph of y 5 )f (t)) has corners at these
d
dt
points and }}) f (t)) is undefined at these instants. We
cannot say that the distance is changing the fastest at
p
3
any particular instant, but we can say that near t 5 }} or
4p
3
t 5 }} the distance is changing faster than at any other
time in the interval.
2
The critical point is at }}, 15Ï3w . Since V9(u) . 0 for
corresponds to the maximum possible trough volume. The
2
Ï3w
1
}} sin t 5 }} cos t
2
2
This is the same equation we solved in part (a), so the
1
1
p
6
u 5 }}
p
p
p
0 # u , }} and V9(u) , 0 for }} , u , }}, the critical point
6
6
2
Ïw3
1
f 0(t) 5 2}} cos t 1 }} sin t 5 0
2
p
2
Find the critical points for 0 # u , }}:
Q
y
L
x
x
A
P
B
Sketch segment RS as shown, and let y be the length of
segment QR. Note that PB 5 8.5 2 x, and so
QB 5 Ïw
x 2w
2w(w8w
.5w
2wxw
)2 5 Ïw8w
.5w
(2w
xw
2w8w
.5w).
Also note that triangles QRS and PQB are similar.
QR
PQ
}} 5 }}
RS
QB
x
y
}} 5 }}
8.5
Ï8w.5
w(2
wxw2
ww8.5
w)w
y2
x2
}}2 5 }}
8.5
8.5(2x 2 8.5)
8.5x 2
2x 2 8.5
y 2 5 }}
L2 5 x2 1 y2
8.5x 2
2x 2 8.5
L 2 5 x 2 1 }}
x 2(2x 2 8.5) 1 8.5x 2
2x 2 8.5
L 2 5 }}}
2x 3
2x 2 8.5
L 2 5 }}
164
Section 4.4
43. continued
46.
Normal
3
2x
2x 2 8.5
(b) Note that x . 4.25, and let f (x) 5 L 2 5 }}. Since
B
A
y # 11, the approximate domain of f is 5.20 # x # 8.5.
Then
(2x 2 8.5)(6x ) 2 (2x )(2)
(2x 2 8.5)
2
3
x (8x 2 51)
(2x 2 8.5)
2
x
P
51
8
x 5 }} 5 6.375 in., and this corresponds to a minimum
value of f (x) because f 9(x) , 0 for 5.20 , x , 6.375
and f 9(x) . 0 for x . 6.375. Therefore, the value of x
that minimizes L 2 is x 5 6.375 in.
(c) The minimum value of L is
!§§§§§§§§§§ < 11.04 in.
2(6.375)3
}}
2(6.375) 2 8.5
12
C
M
3
2
C
2
1
3
44. Since R 5 M 2 }} 2 }} 5 }}M 2 2 }}M 3, we have
dR
}} 5 CM 2 M 2. Let f (M) 5 CM 2 M 2. Then
dM
Q
c
Let P be the foot of the perpendicular from A to the mirror,
and Q be the foot of the perpendicular from B to the mirror.
Suppose the light strikes the mirror at point R on the way
from A to B. Let:
a 5 distance from A to P
b 5 distance from B to Q
c 5 distance from P to Q
x 5 distance from P to R
To minimize the time is to minimize the total distance the
light travels going from A to B. The total distance is
D(x) 5 Ïw
x 2w
1w
a 2w 1 Ïw
(cw
2wxw
)2w
1w
b 2w
Then
1
f 9(M) 5 C 2 2M, and the critical point for f occurs at
C
2
M 5 }}.This value corresponds to a maximum because
C
2
C
dR
of M that maximizes }} is M 5 }}.
2
dM
c–x
R
f 9(x) 5 }}}
5 }}
2
2
For x . 5.20, the critical point occurs at
b
u1 u2
a
C
2
f 9(M) . 0 for M , }} and f 9(M) , 0 for M . }}. The value
1
D9(x) 5 }}(2x) 1 }}[22(c 2 x)]
1w
2Ïxw2w
a 2w
2Ï(c
ww
2wx)w2w
1w
b 2w
x
c2x
5 }} 2 }}
1w
1w
Ïxw2w
a 2w
Ï(c
ww
2wx)w2w
b 2w
Solving D9(x) 5 0 gives the equation
x
c2x
}} 5 }}
1w
1w
Ïw
x 2w
a 2w
Ï(c
ww
2wxw
)2 w
b 2w
45. The profit is given by
which we will refer to as Equation 1. Squaring both sides,
P(x) 5 (n)(x 2 c) 5 a 1 b(100 2 x)(x 2 c)
we have:
5 2bx 1 (100 1 c)bx 1 (a 2 100bc).
2
x2
(c 2 x)2
}
} 5 }}
x2 1 a2
(c 2 x)2 1 b 2
x 2[(c 2 x)2 1 b 2] 5 (c 2 x)2(x 2 1 a 2)
Then P9(x) 5 22bx 1 (100 1 c)b
x 2(c 2 x)2 1 x 2b 2 5 (c 2 x)2x 2 1 (c 2 x)2a 2
5 b(100 1 c 2 2x).
100 1 c
2
c
2
The critical point occurs at x 5 }} 5 50 1 }}, and this
value corresponds to the maximum profit because
c
c
2
2
c
A selling price of 50 1 }} will bring the maximum profit.
2
P9(x) . 0 for x , 50 1 }} and P9(x) , 0 for x . 50 1 }}.
x 2b 2 5 (c 2 x)2a 2
x 2b 2 5 [c 2 2 2xc 1 x 2]a 2
0 5 (a 2 2 b 2)x 2 2 2a 2cx 1 a 2c 2
0 5 [(a 1 b)x 2 ac][(a 2 b)x 2 ac]
ac
a1b
ac
a2b
x 5 }} or x 5 }}
ac
a2b
Note that the value x 5 }} is an extraneous solution
because x and c 2 x have opposite signs for this value.
ac
a1b
The only critical point occurs at x 5 }}.
Section 4.4
To verify that this critical point represents the minimum
distance, note that
(
)
x
(Ïw
x 2w
1w
a 2w)(1) 2 (x) }}
1w
Ïxw2w
a 2w
D0(x) 5 }}}}
2
2
2
x 1a
1
2(c 2 x)
2
(Ï(c
ww
2wxw
)2 w
1w
b 2w)(21) 2 (c 2 x) }}
2wxw
)2w
1w
b 2w
Ï(c
ww
}}}}}}
2
2
(c 2 x) 1 b
(x 2 1 a 2) 2 x2
(x 1 a )
2[(c 2 x)2 1 b 2] 1 (c 2 x)2
[(c 2 x) 1 b ]
5 }}
2
2 3/2 2 }}}
2
2 3/2
r(x) 5 [200 2 2(x 2 50)]x 5 22x 2 1 300x
c(x) 5 6000 1 32x
p(x) 5 r(x) 2 c(x)
5 22x 2 1 268x 2 6000, 50 # x # 80
49. Revenue:
Cost:
Profit:
Since p9(x) 5 24x 1 268 5 24(x 2 67), the critical point
occurs at x 5 67. This value represents the maximum
because p0(x) 5 24, which is negative for all x in the
domain. The maximum profit occurs if 67 people go on the
tour.
5}
}
2
2 3/2 ,
2
2 3/2 1 }}
km
q
h
2
when }}
2 5 }}, or q 5
! §§
which is positive for q . 0.
which is always positive.
(b) The new formula for average weekly cost is
(k 1 bq)m
hq
q
2
km
hq
5 }} 1 bm 1 cm 1 }}
q
2
B(q) 5 }} 1 cm 1 }}
We now know that D(x) is minimized when Equation 1 is
PR
AR
h
2
2km
}}. This corresponds to the
h
50. (a) Since A9(q) 5 2kmq 22 1 }}, the critical point occurs
minimum value of A(q) because A0(q) 5 2kmq 23,
b2
[(c 2 x) 1 b ]
a2
(x 1 a )
165
QR
BR
true, or, equivalently, }} 5 }}. This means that the two
5 A(q) 1 bm
right triangles APR and BQR are similar, which in turn
implies that the two angles must be equal.
Since B(q) differs from A(q) by a constant, the
dv
dx
minimum value of B(q) will occur at the same q-value
47. }} 5 ka 2 2kx
ka
2k
a
2
The critical point occurs at x 5 }} 5 }}, which represents a
quantity is again
maximum value
d 2v
dx
because }}2 5 22k, which is negative for all x. The
maximum value of v is
a 2
122 122
a
kax 2 kx 2 5 ka }} 2 k }}
ka 2
4
5 }}.
48. (a) v 5 cr0r 2 2 cr 3
dv
}} 5 2cr0r 2 3cr 2 5 cr(2r0 2 3r)
dr
2r
The critical point occurs at r 5 }}0 . (Note that r 5 0 is
3
not in the domain of v.) The critical point represents a
d 2v
dr
as the minimum value of A(q). The most economical
}.
!}§§
h
2km
51. The profit is given by
p(x) 5 r(x) 2 c(x)
5 6x 2 (x 3 2 6x 2 1 15x)
5 2x 3 1 6x 2 2 9x, for x $ 0.
Then p9(x) 5 23x 2 1 12x 2 9 5 23(x 2 1)(x 2 3), so the
critical points occur at x 5 1 and x 5 3. Since p9(x) , 0 for
0 # x , 1, p9(x) . 0 for 1 , x , 3, and p9(x) , 0 for
x . 3, the relative maxima occur at the endpoint x 5 0 and
at the critical point x 5 3. Since p(0) 5 p(3) 5 0, this
means that for x $ 0, the function p(x) has its absolute
maximum value at the points (0, 0) and (3, 0). This result
can also be obtained graphically, as shown.
maximum because }}2 5 2cr0 2 6cr 5 2c(r0 2 3r),
r
which is negative in the domain }}0 # r # r0.
2
(b) We graph v 5 (0.5 2 r)r 2, and observe that the
132
2
1
3
maximum indeed occurs at v 5 }} 0.5 5 }}.
[0, 5] by [28, 2]
52. The average cost is given by
c(x)
x
a(x) 5 }} 5 x 2 2 20x 1 20,000. Therefore,
a9(x) 5 2x 2 20 and the critical value is x 5 10, which
represents the minimum because a0(x) 5 2, which is
positive for all x. The average cost is minimized at a
[0, 0.5] by [20.01, 0.03]
production level of 10 items.
166
Section 4.4
aÏw6
aÏ3w
(c) Since r 5 }} and h 5 }}, the relationship is
53. (a) According to the graph, y9(0) 5 0.
3
(b) According to the graph, y9(2L) 5 0.
3
r
w.
}} 5 Ï2
h
(c) y(0) 5 0, so d 5 0.
Now y9(x) 5 3ax 2 1 2bx 1 c, so y9(0) implies that
55. (a) Let x0 represent the fixed value of x at point P, so that
c 5 0. Therefore, y(x) 5 ax 3 1 bx 2 and
P has coordinates (x0, a),
y9(x) 5 3ax 2 1 2bx. Then y(2L) 5 2aL 3 1 bL 2 5 H
and let m 5 f 9(x0) be the slope of line RT. Then the
and y9(2L) 5 3aL 2 2 2bL 5 0, so we have two linear
equation of line RT is
equations in the two unknowns a and b. The second
y 5 m(x 2 x0) 1 a. The y-intercept of this line is
3aL
2
m(0 2 x0) 1 a 5 a 2 mx0,
equation gives b 5 }}. Substituting into the first
3
3
3aL
aL
2
2
H
H
a 5 2}}3 . Therefore, b 5 3}}2 and the equation for y is
L
L
H
H
x 3
x 2
y(x) 5 2}}3 x 3 1 3}}2 x 2, or y(x) 5 H 2 }} 1 3 }} .
L
L
L
L
equation, we have 2aL 3 1 }} 5 H, or }} 5 H, so
312
1 24
2pa 2 x
2p
2pa 2 x 2
2
a 2 }} .
2p
54. (a) The base radius of the cone is r 5 }} and so the
height is h 5 Ïaw2w2
wwr 2w 5
Therefore,
!§§§§1§§§§§§2
1
2pa 2 x 2
p
3
p d
3 dr
wwr 2w)
f 9(r) 5 }} }}(r 2Ïaw2w2
4
1
3
4
5 }} }}
3
Ïwa 2w2
wwr 2w
p 2a 2r 2 3r 3
3
1
2
21
2
2
2
f(x) 2
f 9(x)
3
4
have A(x) 5 2f 9(x) x 2 }} .
(b) The domain is the open interval (0, 10).
!§§§1§0§0
x2
To graph, let y1 5 f (x) 5 5 1 5 1 2 }},
4
5 }} }}
3 Ïa
w2w2
wwr 2w
pr(2a 2 2 3r 2)
5 }}
2
3Ïaww
2
wwr 2w
2a 2
The critical point occurs when r 2 5 }}, which gives
3
y2 5 f 9(x) 5 NDER(y1), and
1
y 2
2
y3 5 A(x) 5 2y2 x 2 }}1 .
y2
The graph of the area function y3 5 A(x) is shown
2
aÏ6w
r 5 a }} 5 }}. Then
3
3
!§
wwr 2w 5
h 5 Ïaw2w2
5 2(Area of triangle ORT)
Substituting x for x0, f 9(x) for m, and f (x) for a, we
wwr 2w)(2r)
= }} r 2 ? }} ? (22r) 1 (Ïaw2w2
3
2Ïa
w2w2
wwr 2w
p 2r 3 1 2r(a 2 2 r 2)
(Area of triangle RST)
1
1
1
volume 5 f(r) 5 }}r 2Ïaw2w2
wwr 2w, where 0 , r , a.
3
m
Let O designate the origin. Then
1
2
1 mx 2 a
5 2 ? }} }0 } (a 2 mx0)
2
m
mx0 2 a mx0 2 a
5 2m }} }}
m
m
mx0 2 a 2
5 2m }}
m
a 2
5 2m x0 2 }}
m
(b) To simplify the calculations, we shall consider the
volume as a function of r:
p
mx 2 a
m(x 2 x0) 1 a 5 0, or x 5 }0 }.
5 2 ? }}(x-intercept of line RT)(y-intercept of line RT)
2 !a§2§2§§1}
§§§2p}
§§§2 .
p 2pa 2 x 2
3
2p
p
3
V(x) 5 }}r 2h 5 }} }}
and the x-intercept is the solution of
below.
aÏw3
!a§§2§§}§3}§ 5 !}§3}§ 5 }3}. Using
2
2a
2
a
2
aÏw6
aÏ3w
r 5 }} and h 5 }},
3
3
we may now find the values of r and h for the given
values of a.
4Ï6w
4Ïw3
When a 5 4: r 5 }}, h 5 }};
3
3
3
3
5Ïw6
5Ïw3
when a 5 5: r 5 }}, h 5 }};
when a 5 6: r 5 2Ï6w, h 5 2Ï3w;
8Ïw6
8Ïw3
when a 5 8: r 5 }}, h 5 }}
3
3
[0, 10] by [2100, 1000]
The vertical asymptotes at x 5 0 and x 5 10
correspond to
horizontal or vertical tangent lines, which do not form
triangles.
Section 4.4
167
(c) Using our expression for the y-intercept of the tangent line, the height of the triangle is
a 2 mx 5 f (x) 2 f 9(x) ? x
1
2x
1
x2
2wx 2w 2 }}x
5 5 1 }}Ï1w0w0ww
2
2wx 2w
2Ï1
w0w0ww
5 5 1 }}Ï1w0w0ww
2wx 2w 1 }}
2
2Ï1
w0w0ww
2wx 2w
We may use graphing methods or the analytic method in part (d) to find that the minimum value of A(x) occurs at x < 8.66.
Substituting this value into the expression above, the height of the triangle is 15. This is 3 times the y-coordinate of the
center of the ellipse.
(d) Part (a) remains unchanged. The domain is (0, C). To graph, note that
!§§§C§
x2
B
C
w2w2
wwx 2w and
f (x) 5 B 1 B 1 2 }}2 5 B 1 }}ÏC
2Bx
1
B
f 9(x) 5 }} }}(22x) 5 }}.
C 2ÏC
2wx 2w
w2w2
wwx 2w
CÏC
w2ww
Therefore, we have
3
3
4
w2w2
wwx 2w 2
B 1 }B}ÏC
Bx
f (x) 2
C
5 }} x 2 }}
2Bx
f 9(x)
CÏC
w2w2
wwx 2w
}}
CÏC
w2w2
wwx 2w
A(x) 5 2f 9(x) x 2 }}
4
3
(BC 1 BÏC
w2w2
wwx2w)ÏC
w2w2
wwx 2w
Bx
5 }} x 2 }}}}
2
2
2Bx
CÏC
ww2
wwx w
4
2
1
5 }}[Bx 2 1 (BC 1 BÏC
w2w2
wwx 2w)(ÏC
w2w2
wwx 2w)]2
BCxÏC
w2w2
wwx 2w
1
5 }}[Bx 2 1 BCÏC
w2w2
wwx 2w 1 B(C 2 2 x 2)]2
BCxÏC
w2w2
wwx 2w
1
5 }}[BC(C 1 ÏC
w2w2
wwx 2w)]2
BCxÏC
w2w2
wwx 2w
w2w2
wwx 2w)2
BC(C 1 ÏC
5 }}}
2
xÏC
ww
wwx w2
2
A9(x) 5 BC ?
1
2x
2
2x
1
2
(xÏC
w2w2
wwx 2w)(2)(C 1 ÏC
w2w2
wwx 2w) }} 2 (C 1 ÏC
w2w2
wwx 2w)2 x}} 1 ÏC
w2w2
wwx 2w(1)
2wx 2w
2wx 2w
ÏC
w2ww
ÏC
w2ww
}}}}}}}}}}
x 2(C 2 2 x 2)
(
)4
w2w2
wwx 2w)
BC(C 1 ÏC
2x 2
5 }}}
22x 2 2 (C 1 ÏC
w2w2
wwx 2w) }
w2w2
wwx 2w
} 1 ÏC
2 2
2
x (C 2 x )
2wx 2w
ÏC
w2ww
3
[
]
w2w2
wwx 2w)
BC(C 1 ÏC
Cx2
5 }}}
22x 2 1 }} 2 CÏC
w2w2
wwx 2w 1 x 2 2 (C 2 2 x 2)
2 2
2
x (C 2 x )
ÏC
w2w2
wwx2w
(
)
BC(C 1 ÏC
w2w2
wwx 2w)
Cx 2
5 }}}
w2w2
wwx 2w 2 C 2
}} 2 CÏC
2 2
2
x (C 2 x )
ÏC
w2w2
wwx 2w
BC(C 1 ÏC
w2w2
wwx 2w)
5 }}}
[Cx 2 2 C(C 2 2 x 2) 2 C 2ÏC
w2w2
wwx 2w]
2 2
2 3/2
x (C 2 x )
BC 2(C 1 ÏC
w2w2
wwx 2w) 2
5 }}}
(2x 2 C 2 2 CÏC
w2w2
wwx 2w)
2 2
2 3/2
x (C 2 x )
168
Section 4.5
55. continued
To find the critical points for 0 , x , C, we solve:
2x 2 2 C 2 5 CÏC
w2w2
wwx 2w
4x 4 2 4C 2x 2 1 C 4 5 C 4 2 C 2x 2
4x 4 2 3C 2x 2 5 0
x 2(4x 2 2 3C 2) 5 0
CÏ3w
3C 2
The minimum value of A(x) for 0 , x , C occurs at the critical point x 5 }}, or x 2 5 }}. The
4
2
corresponding triangle height is
a 2 mx 5 f (x) 2 f 9(x) ? x
Bx2
B
5 B 1 }}ÏC
w2w2
wwx 2w 1 }}
C
CÏC
w2w2
wwx 2w
1 2
2
B
C
3C
B }
}
4
2
3C
}}
2
C 2 }} 1
3C 2
4
C C 2 2 }}
!§§§§§§ !§§§§§§
5 B 1 }}
4
3BC 2
}}
B C
4
5 B 1 }} }} 1 }
C2
C 2
1 2
B
2
}}
2
3B
2
5 B 1 }} 1 }}
5 3B
This shows that the triangle has minimum area when its height is 3B.
■ Section 4.5 Linearization and Newton’s Method (pp. 220–232)
Exploration 1
Approximating with Tangent Lines
1. f 9(x) 5 2x, f 9(1) 5 2, so an equation of the tangent line is y 2 1 5 2(x 2 1) or y 5 2x 2 1.
3. Since (y1 2 y2)(1) 5 y1(1) 2 y2(1) 5 1 2 1 5 0, this view shifts the action from the point (1, 1) to the point (1, 0). Also
(y1 2 y2)9(1) 5 y19(1) 2 y29(1) 5 2 2 2 5 0. Thus the tangent line to y1 2 y2 at x 5 1 is horizontal (the x-axis). The measure of
how well y2 fits y1 at (1, 1) is the same as the measure of how well the x-axis fits y1 2 y2 at (1, 0).
4. These tables show that the values of y1 2 y2 near x 5 1 are close to 0 so that y2 is a good approximation to y1 near
x 5 1. Here are two tables with D Table 5 0.0001.
Section 4.5
Exploration 2
Grapher
Using Newton’s Method on the
1–3. Here are the first 11 computations.
169
7. (a) x 1 1 5 0
x 5 21
(b) 2ex 1 e 1 1 5 0
2ex 5 2(e 1 1)
e11
x 5 2}} < 20.684
2e
8. f 9(x) 5 3x 2 4
f 9(1) 5 3(1)2 2 4 5 21
Since f (1) 5 22 and f 9(1) 5 21, the graph of g(x) passes
through (1, 22) and has slope 21. Its equation is
g(x) 5 21(x 2 1) 1 (22), or g(x) 5 2x 2 1.
2
x
4. Answers will vary. Here is what happens for x1 5 22.
Quick Review 4.5
dy
dx
d
dx
dy
dx
(x 1 1)(1 2 sin x) 2 (x 1 cos x)(1)
(x 1 1)
1. }} 5 cos (x 2 1 1) ? }}(x 2 1 1) 5 2x cos (x 2 1 1)
f (x)
g(x)
0.7
21.457
21.7
0.8
21.688
21.8
0.9
21.871
21.9
1.0
22
22
1.1
22.069
22.1
1.2
22.072
22.2
1.3
22.003
22.3
9. f 9(x) 5 cos x
f 9(1.5) 5 cos 1.5
Since f (1.5) 5 sin 1.5 and f 9(1.5) 5 cos 1.5, the tangent
line passes through (1.5, sin 1.5) and has slope cos 1.5. Its
equation is y 5 (cos 1.5)(x 2 1.5) 1 sin 1.5, or
approximately y 5 0.071x 1 0.891
2. }} 5 }}}}
2
x 2 x sin x 1 1 2 sin x 2 x 2 cos x
(x 1 1)
5 }}}}
2
1 2 cos x 2 (x 1 1) sin x
(x 1 1)
5 }}}
2
3.
[0, p] by [20.2, 1.3]
1
1
10. For x . 3, f 9(x) 5 }}, and so f 9(4) 5 }}. Since
2
2Ïxw2
ww3
1
f (4) 5 1 and f 9(4) 5 }}, the tangent line passes through
2
1
1
(4, 1) and has slope }}. Its equation is y 5 }}(x 2 4) 1 1, or
2
2
1
y 5 }}x 2 1.
2
[22, 6] by [23, 3]
x < 20.567
4.
[21, 7] by [22, 2]
[24, 4] by [210, 10]
x < 20.322
5. f 9(x) 5 (x)(2e 2x) 1 (e 2x)(1) 5 e 2x 2 xe 2x
f 9(0) 5 1
The lines passes through (0, 1) and has slope 1. Its equation
is y 5 x 1 1.
6. f 9(x) 5 (x)(2e 2x) 1 (2e 2x)(1) 5 e 2x 2 xe 2x
f 9(21) 5 e 1 2 (2e 1) 5 2e
The lines passes through (21, 2e 1 1) and has slope 2e.
Its equation is y 5 2e(x 1 1) 1 (2e 1 1), or
y 5 2ex 1 e 1 1.
Section 4.5 Exercises
1. (a) f 9(x) 5 3x 2 2 2
We have f (2) 5 7 and f 9(2) 5 10.
L(x) 5 f (2) 1 f 9(2)(x 2 2)
5 7 1 10(x 2 2)
5 10x 2 13
(b) Since f (2.1) 5 8.061 and L(2.1) 5 8, the
approximation differs from the true value in absolute
value by less than 1021.
170
Section 4.5
x
1
2. (a) f 9(x) 5 }}(2x) 5 }}
1w
2Ïxw2w
1w9
Ïxw2w
9
4
We have f (24) 5 5 and f 9(24) 5 2}}.
5
L(x) 5 f (24) 1 f 9(24)(x 2 (24))
4
5
5 5 2 }}(x 1 4)
4
9
5 2}}x 1 }}
5
5
(b) Since f (23.9) < 4.9204 and L(23.9) 5 4.92, the
approximation differs from the true value by less than
1023.
3. (a) f 9(x) 5 1 2 x 22
We have f (1) 5 2 and f 9(1) 5 0.
L(x) 5 f (1) 1 f 9(1)(x 2 1)
5 2 1 0(x 2 1)
52
(b) Since f (1.1) < 2.009 and L(1.1) 5 2, the
approximation differs from the true value by less than
1022.
1
x11
4. (a) f 9(x) 5 }}
We have f (0) 5 0 and f 9(0) 5 1.
L(x) 5 f (0) 1 f 9(0)(x 2 0)
5 0 1 1x
5x
(b) Since f (0.1) < 0.0953 and L(0.1) 5 0.1 the
approximation differs from the true value by less than
1022.
5. (a) f 9(x) 5 sec2 x
We have f (p) 5 0 and f 9(p) 5 1.
L(x) 5 f (p) 1 f 9(p)(x 2 p)
5 0 1 1(x 2 p)
5x2p
(b) Since f (p 1 0.1) < 0.10033 and L(p 1 0.1) 5 0.1, the
approximation differs from the true value in absolute
value by less than 1023.
1
6. (a) f 9(x) 5 2}}
2wx 2w
Ïw1w
p
We have f (0) 5 }} and f 9(0) 5 21.
2
L(x) 5 f (0) 1 f 9(0)(x 2 0)
p
2
5 }} 1 (21)(x 2 0)
p
2
5 2x 1 }}
(b) Since f (0.1) < 1.47063 and L(0.1) < 1.47080, the
approximation differs from the true value in absolute
value by less than 1023.
7. f 9(x) 5 k(1 1 x)
We have f (0) 5 1 and f 9(0) 5 k.
L(x) 5 f (0) 1 f 9(0)(x 2 0)
5 1 1 k(x 2 0)
5 1 1 kx
k21
8. (a) f (x) 5 (1 2 x)6 5 [1 1 (2x)]6 < 1 1 6(2x) 5 1 2 6x
2
12x
(b) f (x) 5 }} 5 2[1 1 (2x)]21 < 2[1 1 (21)(2x)]
5 2 1 2x
1 22
1
x
2
(c) f (x) 5 (1 1 x) 21/2 < 1 1 2}} x 5 1 2 }}
x 2 1/2
1 22
1 x
x
< Ï2w11 1 }} }}2 5 Ï2w11 1 }}2
2 2
4
(d) f (x) 5 Ï2ww
1wx 2w 5 Ï2w 1 1 }}
2
2
3x 1/3
1 42
1
3
x
x
< 41/311 1 }} }}2 5 41/311 1 }}2
3 4
4
(e) f (x) 5 (4 1 3x)1/3 5 41/3 1 1 }}
2/3
1 2/3
1
5 1 1 2}}
21x
21x
2
1
2
< 1 1 }} 2}} 5 1 2 }}
3
21x
6 1 3x
1
2
2
(f) f (x) 5 1 2 }}
1
3
1
24
1
9. f 9(x) 5 }} 1 cos x
2Ïxw1
ww1
3
We have f (0) 5 1 and f 9(0) 5 }}
2
L(x) 5 f (0) 1 f 9(0)(x 2 0)
3
2
5 1 1 }}x
The linearization is the sum of the two individual
1
2
linearizations, which are x for sin x and 1 1 }}x
for Ïxw1
ww1.
10. (a) (1.002)100 5 (1 1 0.002)100 < 1 1 (100)(0.002)
5 1.2;
)1.002100 2 1.2) < 0.021 , 1021
3
1
3
(b) Ï1w.0
w0w9w 5 (1 1 0.009)1/3 < 1 1 }}(0.009) 5 1.003;
3
)Ï1w.0
w0w9w 2 1.003) < 9 3 1026 , 1025
11. Center 5 21
f 9(x) 5 4x 1 4
We have f (21) 5 25 and f 9(21) 5 0
L(x) 5 f (21) 1 f 9(21)(x 2 (21)) 5 25 1 0(x 1 1) 5 25
12. Center 5 8
1
3
f 9(x) 5 }}x22/3
1
12
We have f (8) 5 2 and f 9(8) 5 }}.
1
12
x
12
4
3
L(x) 5 f (8) 1 f 9(8)(x 2 8) 5 2 1 }}(x 2 8) 5 }} 1 }}
Section 4.5
13. Center 5 1
171
17. Let f (x) 5 x 2 2 2x 1 1 2 sin x.
(x 1 1)(1) 2 (x)(1)
1
(x 1 1)
(x 1 1)
1
1
We have f (1) 5 }} and f 9(1) 5 }}
2
4
1
1
1
1
L(x) 5 f (1) 1 f 9(1)(x 2 1) 5 }} 1 }}(x 2 1) 5 }}x 1 }}
2
4
4
4
n
n
n
n
xn11 5 xn 2 }}
5 xn 2 }}}
Alternate solution:
solutions
f 9(x) 5 }}
5 }}2
2
3
Using center 5 }}, we have f
2
3
3
3
L(x) 5 f }} 1 f 9 }} x 2 }}
2
2
2
12
1 21
2
12
Then f 9(x) 5 2x 2 2 2 cos x and
x
f (x )
2
2 2x 1 1 2 sin x
2xn 2 2 2 cos xn
f 9(xn)
The graph of y 5 f (x) shows that f (x) 5 0 has two
12
1 2
3
3
3
4
}} 5 }} and f 9 }} 5 }}.
2
5
2
25
3
3
4
4
9
5 }} 1 }} x 2 }} 5 }}x 1}}
5
2
25
25
25
p
2
14. Center 5 }}
[24, 4] by [23, 3]
f 9(x) 5 2sin x
p
p
We have f }} 5 0 and f 9 }} 5 21.
2
2
p
p
p
p
p
L(x) 5 f }} 1 f 9 }} x 2 }} 5 0 2 1 x 2 }} 5 2x 1 }}
2
2
2
2
2
1 2
1 2
1 2 1 21 2
1
2
15. Let f (x) 5 x 3 1 x 2 1. Then f 9(x) 5 3x 2 1 1 and
f (x )
x
3
1x 21
n
n
n
xn11 5 xn 2 }}
5 xn 2 }
2 }.
3xn 1 1
f 9(xn)
Note that f is cubic and f 9 is always positive, so there is
exactly one solution. We choose x1 5 0.
x1 5 0
x2 5 1
x3 5 0.75
x4 < 0.6860465
x5 < 0.6823396
x6 < 0.6823278
x7 < 0.6823278
Solution: x < 0.682328
16. Let f (x) 5 x 4 1 x 2 3. Then f 9(x) 5 4x 3 1 1 and
f (x )
x
4
1x 23
n
n
n
xn11 5 xn 2 }}
5 xn 2 }
3}
f 9(xn)
4xn 1 1
The graph of y 5 f (x) shows that f (x) 5 0 has two
x1
x2
x3
x4
x5
5 0.3
< 0.3825699
< 0.3862295
< 0.3862369
< 0.3862369
x1 5 2
x2 < 1.9624598
x3 < 1.9615695
x4 < 1.9615690
x5 < 1.9615690
Solutions: x < 0.386237, 1.961569
18. Let f (x) 5 x 4 2 2. Then f 9(x) 5 4x 3 and
f (x )
x
4
22
n
n
xn11 5 xn 2 }}
5 xn 2 }
}
3 .
f 9(xn)
4xn
Note that f (x) 5 0 clearly has two solutions, namely
4
x 5 6Ï2w. We use Newton’s method to find the decimal
equivalents.
x1 5 1.5
x2 < 1.2731481
x3 < 1.1971498
x4 < 1.1892858
x5 < 1.1892071
x6 < 1.1892071
Solutions: x < 61.189207
dy
dx
19. (a) Since }} 5 3x 2 2 3, dy 5 (3x 2 2 3) dx.
(b) At the given values,
dy 5 (3 ? 22 2 3)(0.05) 5 9(0.05) 5 0.45.
solutions.
(1 1 x 2)(2) 2 (2x)(2x)
dy
(1 1 x )
dx
2 2 2x2
dy 5 }}
dx.
(1 1 x2)2
2 2 2x 2
(1 1 x )
5 }}
20. (a) Since }} 5 }}}
2 2
2 2,
[23, 3] by [24, 4]
x1
x2
x3
x4
x5
5 21.5
5 21.455
< 21.4526332
< 21.4526269
< 21.4526269
x1 5 1.2
x2 < 1.6541962
x3 < 1.1640373
x4 < 1.1640351
x5 < 1.1640351
Solutions: x < 21.452627, 1.164035
(b) At the given values,
2 2 2(22)2
[1 1 (22) ]
228
5
dy 5 }}
2 2 (0.1) 5 }}
2 (0.1)
5 20.024.
dy
dx
1x2
1
21. (a) Since }} 5 (x 2) }} 1 (ln x)(2x) 5 2x ln x 1 x,
dy 5 (2x ln x 1 x) dx.
(b) At the given values,
dy 5 [2(1) ln (1) 1 1](0.01) 5 1(0.01) 5 0.01
172
Section 4.5
1
dy
1
2
22. (a) Since }} 5 (x) }} (22x) 1(Ï1ww
2wx 2w)(1)
dx
2wx 2w
2Ï1
ww
2x 2
2x 2 1 (1 2 x 2)
1 2 2x 2
5 }} 1 Ï1ww
2wx 2w 5 }} 5 }},
2wx 2w
2wx 2w
2wx w2
Ï1ww
Ïw1w
Ï1ww
1 2 2x
2
20
11
2
11
29. (a) Df 5 f (0.55) 2 f (0.5) 5 }} 2 2 5 2}}
(b) Since f 9(x) 5 2x 22, f 9(0.5) 5 24.
1
5
Therefore, df 5 24 dx 5 24(0.05) 5 20.2 5 2}}
dy 5 }} dx.
2wx w2
Ï1ww
1 2 2(0)2
(b) At the given values, dy 5 }}(20.2) 5 20.2.
2w(w0w
)2
Ïw1w
dy
23. (a) Since }} 5 e sin x cos x, dy 5 (cos x)e sin x dx.
dx
)
2
11
1
5
)
1
55
(c) )Df 2 df ) 5 2}} 1 }} 5 }}
30. (a) Df 5 f (1.01) 2 f (1) 5 1.04060401 2 1 5 0.04060401
(b) Since f 9(x) 5 4x 3, f 9(1) 5 4.
Therefore, df 5 4 dx 5 4(0.01) 5 0.04.
(c) )Df 2 df ) 5 )0.04060401 2 0.04) 5 0.00060401
(b) At the given values,
dy 5 (cos p)(e sin p)(20.1) 5 (21)(1)(20.1) 5 0.1.
dV
dr
31. Note that }} 5 4pr 2, dV 5 4pr 2 dr. When r changes from
a to a 1 dr, the change in volume is approximately
1 2 1
1 2 1 2
1 2 1 2
21 2
dy
1
x
x
24. (a) Since }} 5 23 csc 1 2 }} cot 1 2 }} 2}}
dx
3
3
3
x
x
5 csc 1 2 }} cot 1 2 }} ,
3
3
x
x
dy 5 csc 1 2 }} cot 1 2 }} dx.
3
3
1
3
2 1
1
3
2
dy 5 csc 1 2 }} cot 1 2 }} (0.1)
2
2
5 0.1 csc }} cot }} < 0.205525
3
3
25. (a)
dS
dr
32. Note that }} 5 8pr, so dS 5 8pr dr. When r changes from
a to a 1 dr, the change in surface area is approximately
8pa dr.
(b) At the given values,
1
4pa 2 dr.
y 1 xy 2 x 5 0
y(1 1 x) 5 x
x
x11
dy
(x 1 1)(1) 2 (x)(1)
1
Since }} 5 }}
5 }}2 ,
dx
(x 1 1)2
(x 1 1)
dx
dy 5 }}2 .
(x 1 1)
y 5 }}
(b) At the given values,
0.01
(0 1 1)
dV
dx
33. Note that }} 5 3x 2, so dV 5 3x 2 dx. When x changes from
a to a 1 dx, the change in volume is approximately 3a 2 dx.
dS
dx
34. Note that }} 5 12x, so dS 5 12x dx. When x changes from
a to a 1 dx, the change in surface area is approximately
12a dx.
dV
dr
35. Note that }} 5 2prh, so dV 5 2prh dr. When r changes
from a to a 1 dr, the change in volume is approximately
2pah dr.
dy 5 }}2 5 0.01.
dy
dx
26. (a) Since }} 5 sec (x 2 2 1) tan (x 2 2 1) ? (2x),
dy 5 2x sec (x 2 2 1) tan (x 2 21 ) dx.
(b) At the given values,
dy 5 2(1.5) sec (1.52 2 1) tan (1.52 2 1) ? (0.05)
5 0.15 sec 1.25 tan 1.25 < 1.431663.
27. (a) Df 5 f (0.1) 2 f (0) 5 0.21 2 0 5 0.21
(b) Since f 9(x) 5 2x 1 2, f 9(0) 5 2.
Therefore, df 5 2 dx 5 2(0.1) 5 0.2.
(c) )Df 2 df ) 5)0.21 2 0.2) 5 0.01
28. (a) Df 5 f (1.1) 2 f (1) 5 0.231 2 0 5 0.231
(b) Since f 9(x) 5 3x 2 2 1, f 9(1) 5 2.
Therefore, df 5 2dx 5 2(0.1) 5 0.2.
(c) )Df 2 df ) 5 )0.231 2 0.2) 5 0.031
dS
dh
36. Note that }} 5 2pr, so dS 5 2pr dh. When h changes from
a to a 1 dh, the change in lateral surface area is
approximately 2pr dh.
37. (a) Note that f 9(0) 5 cos 0 5 1.
L(x) 5 f (0) 1 f 9(0)(x 2 0) 5 1 1 1x 5 x 1 1
(b) f (0.1) < L(0.1) 5 1.1
(c) The actual value is less than 1.1. This is because the
derivative is decreasing over the interval [0, 0.1], which
means that the graph of f (x) is concave down and lies
below its linearization in this interval.
Section 4.5
dA
dr
38. (a) Note that A 5 pr 2 and }} 5 2pr, so dA 5 2pr dr.
When r changes from a to a 1 dr, the change in area is
approximately 2pa dr. Substituting 2 for a and 0.02 for
dr, the change in area is approximately
2p(2)(0.02) 5 0.08p < 0.2513
173
43. Let u 5 angle of elevation and h 5 height of building. Then
dh
du
h 5 30 tan u, so }} 5 30 sec2 u and dh 5 30 sec2 u du. We
want )dh) , 0.04h, which gives:
)30 sec2 u du) , 0.04 (30 tan u)
0.04 sin u
1
)du) , }}
}}
cos u
cos2 u
)du) , 0.04 sin u cos u
dA
0.08p
(b) }} 5 }} 5 0.02 5 2%
A
4p
39. Let A 5 cross section area, C 5 circumference, and
C
p
dD
1
1
dC
p
p
D 2
C 2
C2
dA
C
Also, A 5 p }} 5 p }} 5 }}, so }} 5 }} and
2
2p
4p
dC
2p
C
dA 5 }} dC. When C increases from 10p in. to
2p
D 5 diameter. Then D 5 }}, so }} 5 }} and dD 5 }} dC.
1 2
1 2
10p 1 2 in. the diameter increases by
1
p
2
p
dD 5 }}(2) 5 }} < 0.6366 in. and the area increases by
10p
approximately dA 5 }}(2) 5 10 in2.
2p
40. Let x 5 edge length and V 5 volume. Then V 5 x 3, and so
dV 5 3x2 dx. With x 5 10 cm and dx 5 0.01x 5 0.1 cm, we
have V 5 103 5 1000 cm3 and dV 5 3(10)2(0.1) 5 30 cm3,
so the percentage error in the volume measurement is
dV
V
5p
12
5p
5p
)du) , 0.04 sin }} cos }} 5 0.01 radian. The angle should
12
12
For u 5 758 5 }} radians, we have
30
1000
approximately }} 5 }} 5 0.03 5 3%.
be measured with an error of less than 0.01 radian (or
approximately 0.57 degrees), which is a percentage error of
approximately 0.76%.
dV
dh
44. Note that }} 5 3ph 2, so dV 5 3ph 2 dh. We want
)dV) # 0.01V, which gives )3ph 2 dh) # 0.01(ph 3), or
0.01h
3
)dh) # }}. The height should be measured with an error
1
3
of no more than }}%.
45. (a) Note that V 5 pr 2h 5 10pr 2 5 2.5pD2, where D is the
dV
dD
interior diameter of the tank. Then }} 5 5pD, so
dV 5 5pD dD. We want )dV) # 0.01V, which gives
)5pD dD) # 0.01(2.5pD 2), or )dD) # 0.005D. The
interior diameter should be measured with an error of
41. Let x 5 side length and A 5 area. Then A 5 x2 and
dA
}} 5 2x, so dA 5 2x dx. We want )dA) # 0.02A, which
dx
gives )2x dx) # 0.02x 2, or )dx) # 0.01x. The side length
no more than 0.5%.
(b) Now we let D represent the exterior diameter of the
tank, and we assume that the paint coverage rate
should be measured with an error of no more than 1%.
(number of square feet covered per gallon of paint) is
42. The volume of a cylinder is V 5 pr h. When h is held
2
dV
dr
known precisely. Then, to determine the amount of
fixed, we have }} 5 2prh, and so dV 5 2prh dr.
paint within 5%, we need to calculate the lateral
For h 5 30 in., r 5 6 in., and dr 5 0.5 in., the thickness of
surface area S with an error of no more than 5%. Note
the shell is approximately
that S 5 2prh 5 10pD, so }} 5 10p and
dV 5 2prh dr 5 2p(6)(30)(0.5) 5 180p < 565.5 in3.
dS 5 10p dD. We want )dS) # 0.05S, which gives
dS
dD
)10p dD) # 0.05(10pD), or dD # 0.05D. The exterior
diameter should be measured with an error of no more
than 5%.
174
Section 4.5
dV
dr
46. Since V 5 pr 2h, we have }} 5 2prh, and dV 5 2prh dr.
52. (a)
i. Q(a) 5 f (a) implies that b0 5 f (a).
ii. Since Q9(x) 5 b1 1 2b2(x 2 a), Q9(a) 5 f 9(a)
implies that b1 5 f 9(a).
We want )dV) # 0.001V, which gives
)2prh dr) # 0.001 pr 2h, or )dr) # 0.0005r. The variation of
iii. Since Q0(x) 5 2b2, Q0(a) 5 f 0(a) implies that
1
the radius should not exceed }} of the ideal radius, that
2000
f 0(a)
2
b2 5 }}
is, 0.05% of the ideal radius.
f 0(a)
2
In summary, b0 5 f (a), b1 5 f 9(a), and b2 5 }}.
dW
dg
47. We have }} 5 2bg 22, so dW 5 2bg 22 dg.
dW
22
2b(5.2)
2b(32)
dg
dg
2
32
5.2
oon
Then }m}
5 }}
5 }}2 < 37.87. The ratio is
22
dWearth
(b) f (x) 5 (1 2 x)21
f 9(x) 5 21(1 2 x)22(21) 5 (1 2 x)22
f 0(x) 5 22(1 2 x)23(21) 5 2(1 2 x)23
about 37.87 to 1.
Since f (0) 5 1, f 9(0) 5 1, and f 0(0) 5 2, the
2
2
coefficients are b0 5 1, b1 5 1, and b2 5 }} 5 1. The
dT
dg
48. (a) Note that T 5 2pL 1/2g 21/2, so }} 5 2pL 1/2g23/2 and
quadratic approximation is Q(x) 5 1 1 x 1 x 2.
dT 5 2pL 1/2g 23/2 dg.
(b) Note that dT and dg have opposite signs. Thus, if g
increases, T decreases and the clock speeds up.
(c)
2pL1/2g 23/2 dg 5 dT
2p(100)1/2(980)23/2 dg 5 0.001
dg < 20.9765
Since dg < 20.9765, g < 980 2 0.9765 5 979.0235.
f (x1)
0
49. If f 9(x) Þ 0, we have x2 5 x1 2 }}
5 x1 2 }} 5 x1.
f 9(x1)
f 9(x1)
Therefore x2 5 x1, and all later approximations are also
equal to x1.
(c)
[22.35, 2.35] by [21.25, 3.25]
As one zooms in, the two graphs quickly become
indistinguishable. They appear to be identical.
(d) g(x) 5 x 21
g 9(x) 5 2x 22
g 0(x) 5 2x 23
Since g(1) 5 1, g9(1) 5 21, and g 0(1) 5 2, the
1/2
1
2h
h
50. If x1 5 h, then f 9(x1) 5 }}
1/2 and x2 5 h 2 }
1
}}
2h 1/2
5 h 2 2h 5 2h. If x1 5 2h, then
1
h 1/2
f 9(x1) 5 2}} and x2 5 2h 2 } 5 2h 1 2h 5 h
1
2Ïwh
2}}
1/2
2
2
coefficients are bo 5 1, b1 5 21, and b2 5 }} 5 1. The
quadratic approximation is
Q(x) 5 1 2 (x 2 1) 1 (x 2 1)2.
2h
[21.35, 3.35] by [21.25, 3.25]
As one zooms in, the two graphs quickly become
indistinguishable. They appear to be identical.
[23, 3] by [20.5, 2]
1
3
f (x )
n
51. Note that f 9(x) 5 }}x 22/3 and so xn11 5 xn 2 }}
x
f 9(xn)
1/3
n
5 xn 2 }
5 xn 2 3xn 5 22xn. For x1 5 1, we have
22/3
xn
}
}
3
x2 5 22, x3 5 4, x4 5 28, and x5 5 16; )xn) 5 2n21.
[210, 10] by [23, 3]
Section 4.6
(e)
175
55. g(a) 5 c, so if E(a) 5 0, then g(a) 5 f (a) and c 5 f (a).
h(x) 5 (1 1 x)1/2
1
h9(x) 5 }}(1 1 x)21/2
2
1
h0(x) 5 2}}(1 1 x)23/2
4
1
1
Since h(0) 5 1, h9(1) 5 }}, and h0(1) 5 2}}, the
2
4
Then E(x) 5 f (x) 2 g(x) 5 f (x) 2 f (a) 2 m(x 2 a).
1
2}}
1
1
4
5 2}}.
coefficients are b0 5 1, b1 5 }}, and b2 5 }
2
2
8
x
2
f (x) 2 f (a)
E(x)
x2a
x2a
f (x) 2 f (a)
E(x)
lim }} 5 f 9(a), so lim }} 5 f 9(a) 2 m.
x2a
x→a
x→a x 2 a
E(x)
Therefore, if the limit of }} is zero, then m 5 f 9(a) and
x2a
Thus, }} 5 }} 2 m.
x2
8
g(x) 5 L(x).
The quadratic approximation is Q(x) 5 1 1 }} 2 }}.
■ Section 4.6 Related Rates (pp. 232–241)
Exploration 1
Sliding Ladder
1. Here the x-axis represents the ground and the y-axis
represents the wall. The curve (x1, y1) gives the position of
[21.35, 3.35] by [21.25, 3.25]
As one zooms in, the two graphs quickly become
indistinguishable. They appear to be identical.
(f) The linearization of any differentiable function u(x) at
x 5 a is L(x) 5 u(a) 1 u9(a)(x 2 a) 5 b0 1 b1(x 2 a),
where b0 and b1 are the coefficients of the constant and
linear terms of the quadratic approximation. Thus, the
linearization for f (x) at x 5 0 is 1 1 x; the linearization
the bottom of the ladder (distance from the wall) at any
13
3
time t in 0 # t # }}. The curve (x2, y2) gives the position
13
3
of the top of the ladder at any time in 0 # t # }}.
13
3
2. 0 # t # }}
3. This is a snapshot at t < 3.1. The top of the ladder is
moving down the y-axis and the bottom of the ladder is
moving to the right on the x-axis. Both axes are hidden
from view.
for g(x) at x 5 1 is 1 2 (x 2 1) or 2 2 x; and the
x
2
linearization for h(x) at x 5 0 is 1 1 }}.
53. Just multiply the corresponding derivative formulas by dx.
d
(a) Since }}(c) 5 0, d(c) 5 0.
dx
dy
du
dx
d
dx
(b) Since }}(cu) 5 c}}, d(cu) 5 c du.
du
dv
d
(c) Since }}(u + v) 5 }} 1 }}, d(u 1 v) 5 du 1 dv
dx
dx
dx
d
(d) Since }}(u
dx
dv
du
? v) 5 u}d}x 1 v}d}x , d(u
du
? v) 5 u dv 1 v du.
12
12
du
dx
(f) Since }}u n 5 nu n21}}, d(u n) 5 nu n21 du.
54.
tan x
x→0 x
sin x/cos x
x
x→0
1 sin x
5 lim }} }}
x→0 cos x x
sin x
1
5 lim }} lim }}
x→0 cos x x→0 x
1
y9(1.5) < 21.107 ft/sec2, y9(2) < 21.561 ft/sec2.
Since lim 2y9(t) 5 2`, the speed of the top of the ladder
t→(13/3)
is infinite as it hits the ground.
21
5 (1)(1) 5 1.
2
Quick Review 4.6
1. D 5 Ï(7
ww
2w0w
)2w
1w(0ww
2w5w
)2 5 Ï4w9ww
1w25w 5 Ï7w4w
2
2
2
2. D 5 Ï(b
ww
2w0)ww
1w(0ww
2wa)w 5 Ïaww1
wwb 2w
3. Use implicit differentiation.
lim }} 5 lim }}
1
9t
4. }} 5 y9(t) 5 2}}
dt
Ï1w3w2w2
ww9tw2
y9(0.5) < 20.348 ft/sec2, y9(1) < 20.712 ft/sec2,
dv
v}} 2 u}}
dx
dx
u
v du 2 u dv
d u
, d }} 5 }}
.
(e) Since }} }} 5}}
v2
v
v2
dx v
d
dx
[21, 15] by [21, 15]
2
d
d
}}(2xy 1 y 2) 5 }}(x 1 y)
dx
dx
dy
dy
dy
2x}} 1 2y(1) 1 2y}} 5 (1) 1 }}
dx
dx
dx
dy
(2x 1 2y 2 1)}} 5 1 2 2y
dx
dy
1 2 2y
}} 5 }}
dx
2x 1 2y 2 1
176
Section 4.6
4. Use implicit differentiation.
d
d
}}(x sin y) 5 }}(1 2 xy)
dx
dx
dy
dy
(x)(cos y)}} 1 (sin y)(1) 5 2x}} 2 y(1)
dx
dx
dy
(x 1 x cos y)}} 5 2y 2 sin y
dx
dy
2y 2 sin y
}} 5 }}
dx
x 1 x cos y
dy
y 1 sin y
}} 5 2}}
dx
x 1 x cos y
5. Use implicit differentiation.
dV
dt
dV
dt
dV dr
dr dt
dV
dt
dh
dt
dr
dt
(b) Since }} 5 }} }}, we have }} 5 2prh}}.
dV
d
d
dt
dt
dt
dV
dh
dr
}} 5 p r 2}} 1 h(2r)}}
dt
dt
dt
dV
dh
dr
}} 5 pr 2}} 1 2prh}}
dt
dt
dt
(c) }} 5 }}pr 2h 5 p}}(r 2h)
1
2
dP
d
dt
dt
dP
dR
d
}} 5 R}}I 2 1 I 2}}
dt
dt
dt
dP
dI
dR
}} 5 R 2I}} 1 I 2}}
dt
dt
dt
dP
dI
2 dR
5
2RI
1
I
}}
}}
}}
dt
dt
dt
1 2
dP
dt
(b) If P is constant, we have }} 5 0, which means
6. Use implicit differentiation.
1
dV dh
dh dt
4. (a) }} 5 }}(RI 2)
d
d
}}x 2 5 }} tan y
dx
dx
dy
2x 5 sec2 y}}
dx
dy
2x
}} 5 }}
dx
sec2 y
dy
}} 5 2x cos2 y
dx
d
}} ln (x 1 y)
dx
dy
1
}} 1 1 }}
dx
x1y
dy
1 1 }}
dx
dy
}}
dx
dV
dt
3. (a) Since }} 5 }} }}, we have }} 5 pr 2}}.
dI
dt
dR
dt
dR
dt
2R dI
I dt
2P dI
I dt
2RI}} 1 I 2}} 5 0, or }} 5 2}} }} 5 2}}
3 }}.
d
dx
5 }}(2x)
252
ds
dt
d
dt
5. }} 5 }}Ïw
x 2w
1wy 2w1
wwz 2w
5 2(x 1 y)
5 2x 1 2y 2 1
7. Using A(22, 1) we create the parametric equations
x 5 22 1 at and y 5 1 1 bt, which determine a line
passing through A at t 5 0. We determine a and b so that
the line passes through B(4, 23) at t 5 1. Since
4 5 22 1 a, we have a 5 6, and since 23 5 1 1 b, we
have b 5 24. Thus, one parametrization for the line
segment is x 5 22 1 6t, y 5 1 2 4t, 0 # t # 1. (Other
answers are possible.)
8. Using A(0, 24), we create the parametric equations
x 5 0 1 at and y 5 24 1 bt, which determine a line
passing through A at t 5 0. We now determine a and b so
that the line passes through B(5, 0) at t 5 1. Since
5 5 0 1 a, we have a 5 5, and since 0 5 24 1 b, we have
b 5 4. Thus, one parametrization for the line segment is
x 5 5t, y 5 24 1 4t, 0 # t # 1. (Other answers are
possible.)
ds
1
d
}} 5 }} }}(x 2 1 y 2 1 z 2)
2
2
2
dt
2Ïw
x w
1wy w1
wwz w dt
1
2
ds
1
dx
dy
dz
}} 5 }} 2x}} 1 2y}} 1 2z}}
2
2
2
dt
d
t
d
t
dt
2Ïw
x w
1wy w1
wwz w
dx
dy
dz
x}} 1 y}} 1 z}}
dt
dt
dt
ds
}}
5
}}
dt
Ïxw2w
1wy 2w1
wwz 2w
dA
dt
dA
}} 5
dt
dA
}} 5
dt
1
1
1
2
d 1
dt 2
1 da
db
}} }} ? b ? sin u 1 a ? }} ? sin u 1 ab
2 dt
dt
1
da
db
du
b
sin
u
1
a
sin
u
}}
}}
}} 1 ab cos u}}
2
dt
dt
dt
6. }} 5 }} }}ab sin u
? }d}t sin u2
d
2
7. (a) Since V is increasing at the rate of 1 volt/sec,
p
3p
9. One possible answer: }} # t # }}
2
2
dV
}} 5 1 volt/sec.
dt
3p
2
10. One possible answer: }} # t # 2p
1
3
(b) Since I is decreasing at the rate of }} amp/sec,
dI
1
}} 5 2}} amp/sec.
dt
3
Section 4.6 Exercises
dA
dt
dA dr
dr dt
dA
dt
dS
dt
dS dr
dr dt
dS
dt
dr
dt
1. Since }} 5 }} }}, we have }} 5 2pr}}.
dr
dt
2. Since }} 5 }} }}, we have }} 5 8pr}}.
(c) Differentiating both sides of V 5 IR, we have
dV
dR
dI
}} 5 I}} 1 R}}.
dt
dt
dt
Section 4.6
(d) Note that V 5 IR gives 12 5 2R, so R 5 6 ohms. Now
substitute the known values into the equation in (c).
dR
dt
1 32
1
15 2}} 1 6 2}}
dR
dt
3 5 2 }}
177
(b) P 5 2l 1 2w
dP
dl
dw
}} 5 2}} 1 2}}
dt
dt
dt
dP
}} 5 2(22) 1 2(2) 5 0 cm/sec
dt
The rate of change of the perimeter is 0 cm/sec.
dR
3
}} 5 }} ohms/sec
dt
2
3
2
R is changing at the rate of }} ohms/sec. Since this
value is positive, R is increasing.
8. Step 1:
r 5 radius of plate
A 5 area of plate
l 2w
1w
w 2w
(c) D 5 Ïw
dl
dw
l}} 1 w}}
dt
dt
dD
1
dl
dw
}} 5 }} 2l}} 1 2w}} 5 }}
2
2
2
dt
d
t
d
t
1w
2Ïw
l w
ww
Ïw
l w
1w
w 2w
dD
(12)(22) 1 (5)(2)
14
}} 5 }} 5 2}} cm/sec
dt
13
Ïw12w2w1
ww52w
1
2
The rate of change of the length of the diameter is
Step 2:
dr
dt
At the instant in question, }} 5 0.01 cm/sec, r 5 50 cm.
Step 3:
dA
dt
We want to find }}.
14
13
2}} cm/sec.
(d) The area is increasing, because its derivative is positive.
The perimeter is not changing, because its derivative is
zero. The diagonal length is decreasing, because its
derivative is negative.
10. Step 1:
x, y, z 5 edge lengths of the box
V 5 volume of the box
S 5 surface area of the box
s 5 diagonal length of the box
Step 4:
A 5 pr 2
Step 5:
dA
dr
}} 5 2pr}}
dt
dt
Step 2:
Step 6:
dA
}} 5 2p(50)(0.01) 5 p cm2/sec
dt
At the instant in question, the area is increasing at the rate
of p cm2/sec.
At the instant in question,
dx
dy
dz
}} 5 1 m/sec, }} 5 22 m/sec, }} 5 1 m/sec, x 5 4 m,
dt
dt
dt
y = 3 m, and z 5 2 m.
Step 3:
9. Step 1:
l 5 length of rectangle
w 5 width of rectangle
A 5 area of rectangle
P 5 perimeter of rectangle
D 5 length of a diagonal of the rectangle
dV dS
dt dt
ds
dt
We want to find }}, }}, and }}.
Steps 4, 5, and 6:
(a) V 5 xyz
dV
dz
dy
dx
}} 5 xy}} 1 xz}} 1 yz}}
dt
dt
dt
dt
dV
}} 5 (4)(3)(1) 1 (4)(2)(22) 1 (3)(2)(1) 5 2 m3/sec
dt
Step 2:
At the instant in question,
dl
dw
}} 5 22 cm/sec, }} 5 2 cm/sec, l 5 12 cm,
dt
dt
and w 5 5 cm.
The rate of change of the volume is 2 m3/sec.
(b) S 5 2(xy 1 xz1 yz)
Step 3:
dA dP
dt dt
dD
dt
We want to find }}, }}, and }}.
Steps 4, 5, and 6:
(a) A 5 lw
dA
dw
dl
}} 5 l}} 1 w}}
dt
dt
dt
dA
}} 5 (12)(2) 1 (5)(22) 5 14 cm2/sec
dt
The rate of change of the area is 14 cm2/sec.
1
2
dS
dy
dx
dz
dx
dz
dy
}} 5 2 x}} 1 y}} 1 x}} 1 z}} 1 y}} 1 z}}
dt
dt
dt
dt
dt
dt
dt
dS
}} 5 2[(4)(22) 1 (3)(1) 1 (4)(1) 1
dt
(2)(1) 1 (3)(1) 1 (2)(22)] 5 0 m2/sec
The rate of change of the surface area is 0 m2/sec.
178
Section 4.6
10. continued
x 2w
1wy 2w1
wwz 2w
(c) s 5 Ïw
1
ds
dx
dy
dz
2x}} 1 2y}} 1 2z}}
}} 5 }}
2
dt
dt
dt
dy
2Ïw
x w
1wy 2ww
1wz 2w
1
2
dx
dy
dz
x}} 1 y}} 1 z}}
dt
dt
dt
13. Step 1:
x 5 distance from wall to base of ladder
y 5 height of top of ladder
A 5 area of triangle formed by the ladder, wall, and ground
u 5 angle between the ladder and the ground
Step 2:
dx
dt
At the instant in question, x 5 12 ft and }} 5 5 ft/sec.
5 }}
Ïxw2w
1wy 2w1
wwz 2w
Step 3:
(4)(1) 1 (3)(22) 1 (2)(1)
ds
0
5 }} 5 0 m/sec
}} 5 }}}
dt
Ïw42w1
ww32w1
ww22w
Ïw29w
The rate of change of the diagonal length is 0 m/sec.
11. Step 1:
s 5 (diagonal) distance from antenna to airplane
x 5 horizontal distance from antenna to airplane
Step 2:
At the instant in question,
dy dA
dt dt
du
dt
We want to find 2}}, }}, and }}.
Step 4, 5, and 6:
(a) x 2 1 y 2 5 169
dx
dt
dy
dt
2x}} 1 2y}} 5 0
To evaluate, note that, at the instant in question,
y 5 Ï1w6w9ww
2wx 2w 5 Ï1w6w9ww
2w
12w2w 5 5.
dy
dt
dy
dy
}} 5 212 ft/sec or 2}} 5 12 ft/sec
dt
dt
Then 2(12)(5) 1 2(5)}} 5 0
ds
dt
s 5 10 mi and }} 5 300 mph.
1
Step 3:
dx
dt
2
We want to find }}.
The top of the ladder is sliding down the wall at the
Step 4:
s 2w
2w49w
x 2 1 49 5 s 2 or x 5 Ïw
rate of 12 ft/sec. (Note that the downward rate of
Step 5:
motion is positive.)
1
2
dx
1
ds
s
ds
}} 5 }} 2s}} 5 }} }}
dt
dt
2w
2w
2Ïw
s 2w
49w
Ïw
s 2w
49
w dt
1
2
(b) A 5 }}xy
Step 6:
dx
10
3000
}} 5 }}(300) 5 }} mph < 420.08 mph
2
dt
Ï1w0ww2
ww49w
Ï5w1w
The speed of the airplane is about 420.08 mph.
12. Step 1:
h 5 height (or depth) of the water in the trough
V 5 volume of water in the trough
1
2
dA
1 dy
dx
}} 5 }} x}} 1 y}}
dt
2 dt
dt
Using the results from step 2 and from part (a), we
dA
dt
1
2
119
2
have }} 5 }}[(12)(212) 1 (5)(5)] 5 2}} ft/sec.
The area of the triangle is changing at the rate of
259.5 ft2/sec.
Step 2:
dV
dt
At the instant in question, }} 5 2.5 ft3/min and h 5 2 ft.
dy
dx
x}} 2 y}}
du
dt
dt
sec u}} 5 }}
x2
dt
p
5
Since tan u 5 }}, we have for 0 # u , }}
2
12
1
}
12
1
6
9
cos u 5 }} and so sec2 u 5 12 2 5 }}.
13
144
}}
2
Step 3:
dh
dt
1
We want to find }}.
Step 4:
4
3
The width of the top surface of the water is }}h, so we have
1
2
y
x
(c) tan u 5 }}
13 2
4
V 5 }}(h) }}h (15), or V 5 10h 2
2
1 13 2
Combining this result with the results from step 2 and
169 du
144 dt
(12)(212) 2 (5)(5)
12
Step 5:
, so
from part (a), we have }} }} 5 }}
2
dV
dh
}} 5 20h}}
dt
dt
du
}} 5 21 radian/sec. The angle is changing at the rate
dt
Step 6:
of 21 radian/sec.
dh
dt
2.5 5 20(2)}}
dh
1
}} 5 0.0625 5 }} ft/min
dt
16
1
16
The water level is increasing at the rate of }} ft/min.
Section 4.6
14. Step 1:
179
Step 5:
Kite
s
Inge
dV
dr
}} 5 12pr}}
dt
dt
Step 6:
300 ft
dV
1
19p
}} 5 12p(1.900) }} 5 }} 5 0.0076p
dt
3000
2500
1
x
2
< 0.0239 in /min
3
s 5 length of kite string
x 5 horizontal distance from Inge to kite
The volume is increasing at the rate of approximately
Step 2:
0.0239 in3/min.
dx
dt
At the instant in question, }} 5 25 ft/sec and s 5 500 ft
16. Step 1:
Step 3:
h
ds
dt
We want to find }}.
Step 4:
r
x 1 300 5 s
2
2
2
r 5 base radius of cone
h 5 height of cone
V 5 volume of cone
Step 5:
dx
dt
ds
dt
dx
dt
ds
dt
2x}} 5 2s}} or x}} 5 s}}
Step 2:
Step 6:
At the instant in question, since x 2 1 3002 5 s 2, we have
x 5 Ïw
s 2w
2w30w0w2w 5 Ï5w0w0w2w2
ww30w0w2w 5 400.
ds
dt
dV
dt
At the instant in question, h 5 4 m and }} 5 10 m3/min.
Step 3:
ds
dt
dh
dt
dr
dt
Thus (400)(25) 5 (500)}}, so }} 5 20 ft/sec. Inge must let
We want to find }} and }}.
the string out at the rate of 20 ft/sec.
Step 4:
3
8
15. Step 1:
Since the height is }} of the base diameter, we have
3
8
4
3
h 5 }}(2r) or r 5 }}h.
1
3
1
3
2
16ph 3
27
13 2
4
We also have V 5 }}pr 2h 5 }}p }}h h 5 }}. We will
6 in.
16ph 3
27
4
3
use the equations V 5 }} and r 5 }}h.
Steps 5 and 6:
r
The cylinder shown represents the shape of the hole.
r 5 radius of cylinder
V 5 volume of cylinder
Step 2:
dr
dt
0.001 in.
3 min
1
3000
At the instant in question, }} 5 }} 5 }} in./min
and (since the diameter is 3.800 in.), r 5 1.900 in.
Step 3:
dV
We want to find }}.
dt
Step 4:
V 5 pr 2(6) 5 6pr 2
16ph 2 dh
9
dt
16p(4)2 dh
10 5 }} }}
9
dt
dh
1125
45
}} 5 }} m/min 5 }} cm/min
dt
32p
128p
dV
dt
(a) }} 5 }} }}
The height is changing at the rate of
1125
}} < 11.19 cm/min.
32p
(b) Using the results from Step 4 and part (a), we have
1
2
dr
4 dh
4 1125
375
}} 5 }} }} 5 }} }} 5 }} cm/min.
dt
3 dt
3 32p
8p
The radius is changing at the rate of
375
}} < 14.92 cm/min.
8p
180
Section 4.6
17. Step 1:
Step 6:
45 m
r
dy
dt
26 5 [26p(8) 2 p(82)]}}
dy
dt
26 5 144p}}
6m
dy
1
}} 5 2}} < 20.01326 m/min
dt
24p
25
or 2}} < 21.326 cm/min
6p
h
r 5 radius of top surface of water
h 5 depth of water in reservoir
V 5 volume of water in reservoir
(b) Since r 2 1 (13 2 y)2 5 132,
r 5 Ï1w6w9ww
2w(1w3ww
2wyw
)2 5 Ï2w6wyw2
wwy 2w.
Step 2:
dV
dt
At the instant in question, }} 5 250 m3/min and h 5 5 m.
Step 3:
dh
dt
dr
dt
(c) Step 1:
y 5 depth of water
r 5 radius of water surface
V 5 volume of water in bowl
We want to find 2}} and }}.
Step 2:
Step 4:
At the instant in question, }} 5 26 m3/min, y 5 8 m,
dV
dt
dy
dt
1
24p
h
6
r
45
1
1
Then V 5 }}pr 2h 5 }}p(7.5h)2h 5 18.75ph3
3
3
and therefore (from part (a)) }} 5 2}} m/min.
Step 5 and 6:
We want to find the value of }}.
Note that }} 5 }} by similar cones, so r 5 7.5h.
Step 3:
dr
dt
dV
dt
dh
dt
(a) Since V 5 18.75ph 3, }} 5 56.25ph 2}}.
Step 4:
dh
dt
dh
8
32
}} 5 2}} m/min 5 2}} cm/min.
dt
225p
9p
32
The water level is falling by }} < 1.13 cm/min.
9p
dh
(Since }} , 0, the rate at which the water level is
dt
From part (b), r 5 Ï2w6wyw2
wwy 2w.
falling is positive.)
dr
13 2 8
1
5
1
}} 5 }} }} 5 }} 2}}
dt
12
24p
Ï2w6w(8
w)w2
ww82w 224p
5
5 2}} < 20.00553 m/min
288p
125
or 2}} < 20.553 cm/min
72p
Thus 250 5 56.25p(52)}}, and so
dr
dt
Step 5:
dr
1
dy
13 2 y dy
}} 5 }}(26 2 2y)}} 5 }} }}
dt
dt
y2
2Ï2
w6ww
wwy 2w
Ï2w6ww
y2
wwy 2w dt
Step 6:
1
dh
dt
80
3p
(b) Since r 5 7.5h, }} 5 7.5}} 5 2}} cm/min. The rate
of change of the radius of the water’s surface is
80
3p
2}} < 28.49 cm/min.
2
1
2
19. Step 1:
r 5 radius of spherical droplet
S 5 surface area of spherical droplet
V 5 volume of spherical droplet
18. (a) Step 1:
y 5 depth of water in bowl
V 5 volume of water in bowl
Step 2:
No numerical information is given.
Step 2:
dV
dt
At the instant in question, }} 5 26 m3/min and
Step 3:
y 5 8 m.
We want to show that }} is constant.
Step 3:
Step 4:
dy
We want to find the value of }}.
dt
S 5 4pr 2, V 5 }}pr 3, }} 5 kS for some constant k
Step 4:
Steps 5 and 6:
p
3
dr
dt
4
3
p
3
V 5 }}y 2(39 2 y) or V 5 13py 2 2 }}y 3
Step 5:
dV
dy
}} 5 (26py 2 py 2)}}
dt
dt
dV
dt
4
dV
dr
3
dt
dt
dV
dr
Substituting kS for }} and S for 4pr 2, we have kS 5 S}},
dt
dt
dr
or }} 5 k.
dt
Differentiating V 5 }}pr 3, we have }} 5 4pr 2}}.
Section 4.6
20. Step 1:
r 5 radius of spherical balloon
S 5 surface area of spherical balloon
V 5 volume of spherical balloon
6
(b) u 5 cos21 }}
l
Step 2:
dV
At the instant in question, }} 5 100p ft3/min and r 5 5 ft.
dt
Step 3:
1
du
6 dl
}} 5 2 }}2 2}2} }}
dt
l dt
6
1 2 }}
1 2
!§§§1§l 2§
du
1
6
3
}} 5 2}}12}}2(22) 5 2}} radian/sec
dt
1
0
2
0
Ï1ww
2w0.6
ww
2
2
dr
dt
dS
dt
We want to find the values of }} and }}.
Steps 4, 5, and 6:
3
20
The rate of change of angle u is 2}} radian/sec.
22. Step 1:
x 5 distance from origin to bicycle
y 5 height of balloon (distance from origin to balloon)
s 5 distance from balloon to bicycle
4
3
(a) V 5 }}pr 3
dV
dr
}} 5 4pr 2}}
dt
dt
dr
dt
100p 5 4p(5)2}}
Step 2:
dr
}} 5 1 ft/min
dt
dy
dt
dx
dt
We know that }} is a constant 1 ft/sec and }} is a constant
The radius is increasing at the rate of 1 ft/min.
(b) S 5 4pr2
17 ft/sec. Three seconds before the instant in question, the
values of x and y are x 5 0 ft and y 5 65 ft. Therefore, at
the instant in question x 5 51 ft and y 5 68 ft.
Step 3:
dS
dr
}} 5 8pr}}
dt
dt
dS
}} 5 8p(5)(1)
dt
dS
}} 5 40p ft2/min
dt
ds
dt
We want to find the value of }} at the instant in question.
Step 4:
The surface area is increasing at the rate of
s 5 Ïw
x 2w
1wy 2w
40p ft2/min.
Step 5:
21. Step 1:
l 5 length of rope
x 5 horizontal distance from boat to dock
u 5 angle between the rope and a vertical line
Step 2:
dl
At the instant in question, }} 5 22 ft/sec and l 5 10 ft.
dt
Step 3:
dx
1
2
Step 6:
(51)(17) 1 (68)(1)
ds
5 11 ft/sec
}} 5 }}
dt
Ï5w1w2ww
1w68
w2w
The distance between the balloon and the bicycle is
increasing at the rate of 11 ft/sec.
dc
dt
d
dt
23. (a) }} 5 }}(x 3 2 6x 2 1 15x)
dx
dt
5 (3x 2 2 12x 1 15)}}
Step 4, 5, and 6:
5 [3(2)2 2 12(2) 1 15](0.1)
dx
dt
du
dt
(a) x 5 Ïw
l 2w
2w36w
dx
l
dl
}} 5 }} }}
dt
2w36
Ïw
l 2w
w dt
dx
10
}} 5 }}(22) 5 22.5 ft/sec
dt
Ï1w0w2w2
ww36w
The boat is approaching the dock at the rate of
dy
x}} 1 y}}
dt
dt
ds
1
dx
dy
}}
5
2x
1
2y
5
}} }} }}
}}
2
dt
dt
dt
Ïw
x w
1wy 2w
1wy 2w
2Ïw
x 2w
We want to find the values of 2}} and }}.
2.5 ft/sec.
181
5 0.3
dr
dx
d
}} 5 }}(9x) 5 9}} 5 9(0.1) 5 0.9
dt
dt
dt
dp
dr
dc
}} 5 }} 2 }} 5 0.9 2 0.3 5 0.6
dt
dt
dt
dc
dt
1
2
2
45
x
45 dx
2
5 3x 2 12x 2 }}2 }}
x dt
d
dt
(b) }} 5 }} x 3 2 6x 2 1 }}
1
45
5 33(1.5)2 2 12(1.5) 2 }}4(0.05)
1.5
2
5 21.5625
dr
dx
d
}} 5 }}(70x) 5 70}} 5 70(0.05) 5 3.5
dt
dt
dt
dp
dr
dc
}} 5 }} 2 }} 5 3.5 2 (21.5625) 5 5.0625
dt
dt
dt
182
Section 4.6
24. (a) Note that the level of the coffee in the cone is not
needed until part (b).
Step 1:
V1 5 volume of coffee in pot
y 5 depth of coffee in pot
Step 2:
25. Step 1:
Q 5 rate of CO2 exhalation (mL/min)
D 5 difference between CO2 concentration in blood
pumped to the lungs and CO2 concentration in blood
returning from the lungs (mL/L)
y 5 cardiac output
Step 2:
dV
}}1 5 10 in3/min
dt
At the instant in question, Q 5 233 mL/min, D 5 41 mL/L,
Step 3:
dy
We want to find the value of }}.
dt
Step 4:
dD
dQ
}} 5 22 (mL/L)/min, and }} 5 0 mL/min2.
dt
dt
Step 3:
dy
dt
We want to find the value of }}.
V1 5 9py
Step 4:
Step 5:
Q
D
y 5 }}
dV
dy
}}1 5 9p}}
dt
dt
Step 5:
Step 6:
dQ
dD
D}} 2 Q}}
dt
dt
dy
}} 5 }}
D2
dt
dy
dt
10 5 9p}}
dy
10
}} 5 }} < 0.354 in./min
dt
9p
The level in the pot is increasing at the rate of
Step 6:
approximately 0.354 in./min.
(41)(0) 2 (233)(22)
dy
466
5 }} < 0.277 L/min2
}} 5 }}}
(41)2
dt
1681
(b) Step 1:
V2 5 volume of coffee in filter
r 5 radius of surface of coffee in filter
h 5 depth of coffee in filter
The cardiac output is increasing at the rate of
approximately 0.277 L/min2.
26. Step 1:
y
Step 2:
dV
At the instant in question, }}2 5 210 in3/min and
dt
(x, y)
h 5 5 in.
Step 3:
u
dh
dt
We want to find 2}}.
x
Step 4:
r
h
3
6
h
2
Note that }} 5 }}, so r 5 }}.
1
ph 3
Then V2 5 }}pr 2h 5 }}.
3
12
Step 5:
x 5 x-coordinate of particle’s location
y 5 y-coordinate of particle’s location
u 5 angle of inclination of line joining the particle to the
origin.
dV
ph 2 dh
}}2 5 }} }}
dt
4 dt
Step 2:
Step 6:
At the instant in question,
p(5)2 dh
210 5 }} }}
4 dt
dh
8
}} 5 2}} in./min
dt
5p
dh
Note that }} , 0, so the rate at which the level is
dt
dx
}} 5 10 m/sec and x 5 3 m.
dt
Step 3:
falling is positive. The level in the cone is falling at the
Step 4:
8
rate of }} < 0.509 in./min.
5p
Since y 5 x 2, we have tan u 5 }} 5 }} 5 x and so, for
du
dt
We want to find }}.
y
x
x . 0, u 5 tan21 x.
x2
x
Section 4.6
Step 5:
183
28. Step 1:
x 5 x-coordinate of particle
y 5 y-coordinate of particle
D 5 distance from origin to particle
du
dx
1
}} 5 }}2 }}
dt
1 1 x dt
Step 6:
du
1
}} 5 }}2 (10) 5 1 radian/sec
dt
113
Step 2:
The angle of inclination is increasing at the rate of
At the instant in question, x 5 5 m, y 5 12 m,
1 radian/sec.
dx
dy
}} 5 21 m/sec, and }} 5 25 m/sec.
dt
dt
Step 3:
27. Step 1:
dD
dt
We want to find }}.
y
Step 4:
D 5 Ïw
x 2w
1wy 2w
(x, y)
Step 5:
dx
dy
x}} 1 y}}
dt
dt
dD
1
dx
dy
}} 5 }} 2x}} 1 2y}} 5 }}
2
dt
dt
dt
Ïw
x w
1wy 2w
1wy 2w
2Ïw
x 2w
θ
1
x
2
Step 6:
x 5 x-coordinate of particle’s location
y 5 y-coordinate of particle’s location
u 5 angle of inclination of line joining the particle to the
origin
(5)(21) 1 (12)(25)
dD
5 25 m/sec
}} 5 }}}
dt
Ï5w2w1
ww12w2w
The particle’s distance from the origin is changing at the
rate of 25 m/sec.
29. Step 1:
Step 2:
dx
dt
At the instant in question, }} 5 28 m/sec and x 5 24 m.
Street
light
Step 3:
du
dt
16 ft
We want to find }}.
Step 4:
6 ft
Ïwxw
Since y 5 Ï2
wwx, we have tan u 5 }y} 5 }2
} 5 2(2x)21/2,
x
x
and so, for x , 0,
u 5 p 1 tan
21
21/2
[2 (2x)
21
] 5 p 2 tan
21/2
(2x)
.
Shadow
x
s
x 5 distance from streetlight base to man
s 5 length of shadow
Step 2:
Step 5:
dx
dt
At the instant in question, }} 5 25 ft/sec and x 5 10 ft.
1
du
1
dx
2}}(2x)23/2(21) }}
}} 5 2 }}
1 1 [(2x)21/2]2
dt
2
dt
1
1
1
1 2 }} 2(2x)
2
dx
dt
5 2}
}}
3/2 }}
1
1x2
1
dx
5 }} }}
2Ïw
2wx(x 2 1) dt
Step 3:
ds
dt
We want to find }}.
Step 4:
s1x
16
s
6
By similar triangles, }} 5 }}. This is equivalent to
3
5
16s 5 6s 1 6x, or s 5 }}x.
Step 6:
Step 5:
du
2
1
}} 5 }}(28) 5 }} radian/sec
dt
5
2Ï4
w(24 2 1)
ds
3 dx
}} 5 }} }}
dt
5 dt
The angle of inclination is increasing at the rate of
Step 6:
2
}} radian/sec.
5
ds
3
}} 5 }}(25) 5 23ft/sec
dt
5
The shadow length is changing at the rate of 23 ft/sec.
184
Section 4.6
30. Step 1:
s 5 distance ball has fallen
x 5 distance from bottom of pole to shadow
122
At the instant in question, s 5 16 }}
12
ds
1
}} 5 32 }} 5 16 ft/sec.
dt
2
At the instant in question,
dV
1
}} 5 28 mL/min 5 28 cm3/min and r 5 }}(20) = 10 cm.
dt
2
Step 2:
1 2
Step 2:
5 4 ft and
Step 3:
dS
dt
We want to find 2}}.
Step 3:
Step 4:
dx
dt
We want to find }}.
4
3
We have V 5 }}pr 3 and S 5 4pr 2. These equations can be
Step 4:
x 2 30
x
By similar triangles, }} 5 }}. This is equivalent to
50 2 s
50
50x 2 1500 5 50x 2 sx, or sx 5 1500. We will use
3V 1/3
1 4p 2
combined by noting that r 5 }}
3V 2/3
1 4p 2
, so S 5 4p }}
Step 5:
x 5 1500s21.
dS
2 3V 21/3 3 dV
3V 21/3 dV
}} 5 4p }} }}
}} }} 5 2 } }
}}
dt
3 4p
dt
4p dt
4p
Step 5:
Step 6:
dx
ds
}} 5 21500s 22}}
dt
dt
Note that V 5 }}p(10)3 5 }}.
Step 6:
dS
3
}} 5 2 }} ?
dt
4p
dS
Since }} , 0, the rate of decrease is positive. The surface
dt
1 21 2 1 2
4
4000p
3
3
4000p 21/3
216
2
(28) 5 }
}}
3 } 5 21.6 cm /min
3
Ï1ww0w00w
1
dx
}} 5 21500(4)22(16) 5 21500 ft/sec
dt
The shadow is moving at a velocity of 21500 ft/sec.
31. Step 1:
x 5 position of car (x 5 0 when car is right in front of
you)
u 5 camera angle. (We assume u is negative until the car
passes in front of you, and then positive.)
1 2
2
area is decreasing at the rate of 1.6 cm2/min.
33. Step 1:
p 5 x-coordinate of plane’s position
x 5 x-coordinate of car’s position
s 5 distance from plane to car (line-of-sight)
Step 2:
Step 2:
dx
dt
At the first instant in question, x 5 0 ft and }} 5 264 ft/sec.
At the instant in question,
dp
dt
ds
dt
A half second later, x 5 }}(264) 5 132 ft and
p 5 0, }} 5 120 mph, s 5 5 mi, and }} 5 2160 mph.
dx
}} 5 264 ft/sec.
dt
Step 3:
Step 3:
We want to find 2}}.
1
2
dx
dt
du
dt
We want to find }} at each of the two instants.
Step 4:
Step 4:
(x 2 p)2 1 32 5 s 2
1 132 2
x
u 5 tan21 }}
Step 5:
Step 5:
2(x 2 p) }} 2 }} 5 2s}}
dx
1
du
}} 5 }}
x 2
dt
1 1 }}
1 132 2
1 dt
1 dx
} }}
?}
132 dt
2
ds
dt
Step 6:
Note that, at the instant in question,
Step 6:
1
du
1
When x 5 0: }} 5 }}2 }} (264) 5 2 radians/sec
dt
132
0
1 1 }}
1 132 2
du
dt
dp
dt
1 2
1
1 132 2
1
When x 5 132: }} 5 }}2 }} (264) 5 1 radian/sec
1 2
132
1 1 }}
132
32. Step 1:
r 5 radius of balls plus ice
S 5 surface area of ball plus ice
V 5 volume of ball plus ice
x 5 Ï5w2w2
ww32w 5 4 mi.
1 dt
2
dx
81}} 2 1202 5 21600
dt
dx
2(4 2 0) }} 2 120 5 2(5)(2160)
dx
}} 2 120 5 2200
dt
dx
}} 5 280 mph
dt
The car’s speed is 80 mph.
Section 4.6
185
Step 6:
34. Step 1:
s 5 shadow length
u 5 sun’s angle of elevation
du
(20)(22) 2 (10)(1)
}} 5 }
} 5 20.1 radian/sec
dt
102 1 202
< 25.73 degrees/sec
Step 2:
To the nearest degree, the angle is changing at the rate
At the instant in question,
du
dt
s 5 60 ft and }} 5 0.278/min 5 0.0015p radian/min.
of 26 degrees per second.
36. Step 1:
Step 3:
A
ds
dt
We want to find 2}}.
Step 4:
c
a
80
tan u 5 }} or s 5 80 cot u
s
120°
Step 5:
O
ds
du
}} 5 280 csc2 u}}
dt
dt
b
B
a 5 distance from O to A
b 5 distance from O to B
c 5 distance from A to B
Step 6:
80
60
Note that, at the moment in question, since tan u 5 }} and
p
4
5
0 , u , }}, we have sin u 5 }} and so csc u 5 }}.
2
5
4
ds
5 2
}} 5 280 }} (0.0015p)
dt
4
12 in
ft
5 20.1875p }} ? }}
1 ft
min
12
5 22.25p in./min
Step 2:
At the instant in question, a 5 5 nautical miles,
da
dt
db
dt
b 5 3 nautical miles, }} 5 14 knots, and }} 5 21 knots.
Step 3:
dc
dt
We want to find }}.
< 27.1 in./min
ds
Since }} , 0, the rate at which the shadow length is
dt
Step 4:
Law of Cosines:
c 2 5 a 2 1 b 2 2 2ab cos 1208
c 2 5 a 2 1 b 2 1 ab
decreasing is positive. The shadow length is decreasing at
Step 5:
the rate of approximately 7.1 in./min.
dc
dt
da
dt
db
dt
db
dt
da
dt
2c}} 5 2a}} 1 2b}} 1 a}} 1 b}}
35. Step 1:
a 5 distance from origin to A
b 5 distance from origin to B
u 5 angle shown in problem statement
Step 6:
Note that, at the instant in question,
c 5 Ïaw2w1
wwb 2w1
wwabw 5 Ï(5
ww
)2w
1w(3ww
)2w
1w(5w)(
w3w)w 5 Ï4w9w 5 7
Step 2:
da
dt
db
dt
At the instant in question, }} 5 22 m/sec, }} 5 1 m/sec,
dc
dt
dc
14}} 5 413
dt
dc
}} 5 29.5 knots
dt
2(7)}} 5 2(5)(14) 1 2(3)(21) 1 (5)(21) 1 (3)(14)
a 5 10 m, and b 5 20 m.
Step 3:
du
dt
The ships are moving apart at a rate of 29.5 knots.
We want to find }}.
Step 4:
dy
dt
12
Step 5:
da
db
da
db
b}} 2 a}}
b}} 2 a}}
dt
dt
dt
dt
1
du
5
}}
}} 5 }2 }}
b2
a2 1 b2
dt
a
1 1 }}
1b2
dy dx
dx dt
dx
Since }} 5 3 cm/sec, we have
dt
dy
60x
cm/sec.
}} 5 2}}
dt
(1 1 x2)2
dx
dt
dx
20x
(1 1 x ) dt
37. }} 5 }} }} 5 210(1 1 x 2)22(2x)}} 5 2}}
2 2 }}
a
a
tan u 5 }} or u 5 tan21 }}
b
b
dy
dt
60(22)
[1 1 (22) ]
dy
dt
60(0)
(1 1 0 )
dy
dt
60(20)
(1 1 20 )
120
5
24
5
(a) }} 5 2}}
2 2 5 }}
2 5 }} cm/sec
(b) }} 5 2}}
2 2 5 0 cm/sec
(c) }} 5 2}}
2 2 < 20.00746 cm/sec
186
Chapter 4 Review
dy
dt
dy dx
dx
dx dt
dt
dx
dy
Since }} 5 22 cm/sec, we have }} 5 8 2 6x 2 cm/sec.
dt
dt
38. }} 5 }} }} 5 (3x 2 2 4)}}
dy
dv
du
d
}} 5 }}(uv) 5 u}} 1 v}}
dt
dt
dt
dt
41. (a)
5 u(0.05v) 1 v(0.04u)
5 0.09uv
5 0.09y
dy
dt
(a) }} 5 8 2 6(23)2 5 246 cm/sec
dy
dt
Since }} 5 0.09y, the rate of growth of total production
dy
dt
(b) }} 5 8 2 6(1)2 5 2 cm/sec
dy
dt
(c) }} 5 8 2 6(4)2 5 288 cm/sec
is 9% per year.
5 u(0.03v) 1 v(20.02u)
5 0.01uv
5 0.01y
The total production is increasing at the rate of 1% per
year.
39. (a) The point being plotted would correspond to a point on
the edge of the wheel as the wheel turns.
(b) One possible answer is u 5 16pt, where t is in seconds.
(An arbitrary constant may be added to this expression,
and we have assumed counterclockwise motion.)
(c) In general, assuming counterclockwise motion:
dx
du
}} 5 22 sin u}} 5 22(sin u)(16p) 5 232p sin u
dt
dt
dy
du
}} 5 2 cos u}} 5 2(cos u)(16p) 5 32p cos u
dt
dt
p
At u 5 }}:
4
dx
p
w) < 271.086 ft/sec
}} 5 232p sin }} 5 216p(Ï2
dt
4
dy
p
w) < 71.086 ft/sec
}} 5 32p cos }} 5 16p(Ï2
dt
4
p
At u 5 }}:
2
dx
p
}} 5 232p sin }} 5 232p < 2100.531 ft/sec
dt
2
dy
p
}} 5 32p cos }} 5 0 ft/sec
dt
2
dy
dv
du
d
}} 5 }}(uv) 5 u}} 1 v}}
dt
dt
dt
dt
(b)
■ Chapter 4 Review (pp. 242–245)
1. y 5 xÏ2ww
2wx
1
2
1
y9 5 x }} (21) 1 (Ï2ww
2wx)(1)
2wx
2Ï2
ww
2x 1 2(2 2 x)
5 }}
2Ïw2w
2wx
4 2 3x
5 }}
2Ï2
ww
2wx
4
The first derivative has a zero at }}.
3
Critical point value:
x 5 }}
4Ï6w
y 5 }} < 1.09
Endpoint values:
x 5 22
y 5 24
x52
y50
4
3
At u 5 p:
dx
}} 5 232p sin p 5 0 ft/sec
dt
dy
}} 5 32p cos p 5 232p < 2100.531 ft/sec
dt
40. (a) One possible answer:
x 5 30 cos u, y 5 40 1 30 sin u
(b) Since the ferris wheel makes one revolution every
10 sec, we may let u 5 0.2pt and we may write
x 5 30 cos 0.2pt, y 5 40 1 30 sin 0.2pt.
(This assumes that the ferris wheel revolves
counterclockwise.)
In general:
4Ïw6
9
minimum value is 24 at x 5 22.
2. Since y is a cubic function with a positive leading
coefficient, we have lim y 5 2` and lim y 5 `. There are
x→2`
3. y9 5 (x 2)(e 1/x )(22x23) 1 (e 1/x )(2x)
2
2
1
2
1
x
2
2e 1/x (x 2 1)(x 1 1)
5 }}}
x
2
5 2e 1/x 2}} 1 x
x , 21
Sign of y9
2
At t 5 5:
Behavior of y Decreasing
dx
}} 5 26p sin 1.6p < 17.927 ft/sec
dt
dy
}} 5 6p cos 1.6p < 5.825 ft/sec
dt
x→`
no global extrema.
Intervals
At t 5 8:
4
3
The global maximum value is }} at x 5 }}, and the global
dx
}} 5 230(sin 0.2pt)(0.2p) 5 26p sin 0.2pt
dt
dy
}} 5 30(cos 0.2pt)(0.2p) 5 6p cos 0.2pt
dt
dx
}} 5 26p sin p 5 0 ft/sec
dt
dy
}} 5 6p cos p 5 6p(21) < 218.850 ft/sec
dt
9
d
dx
21 , x , 0 0 , x , 1
1
Increasing
2
x.1
1
Decreasing Increasing
y0 5 }}[2e 1/x (2x21 1 x)]
2
5 (2e 1/x )(x22 1 1) 1 (2x21 1 x)(2e 1/x )(22x23)
2
5 (2e 1/x )(x 22 1 1 1 2x 24 2 2x 22)
2
2
2e 1/x (x 4 2 x 2 1 2)
x
2
2e 1/x [(x 2 2 0.5)2 1 1.75]
5 }}}
x4
5 }}
4
2
Chapter 4 Review
The second derivative is always positive (where defined), so
the function is concave up for all x Þ 0.
Graphical support:
187
5. y9 5 1 2 2x 2 4x 3
Using grapher techniques, the zero of y9 is x < 0.385.
Intervals
x , 0.385 0.385 , x
1
Sign of y9
2
Behavior of y Increasing Decreasing
(a) [21, 0) and [1, `)
y0 5 22 2 12x 2 5 22(1 1 6x 2)
The second derivative is always negative so the function is
concave down for all x.
(b) (2`, 21] and (0, 1]
Graphical support:
[24, 4] by [21, 5]
(c) (2`, 0) and (0, `)
(d) None
(e) Local (and absolute) minima at (1, e) and (21, e)
(f) None
[24, 4] by [24, 2]
4. Note that the domain of the function is [22, 2].
1
(a) Approximately (2`, 0.385]
(b) Approximately [0.385, `)
2
1
2wx 2w)(1)
y9 5 x }} (22x) 1 (Ï4ww
2wx 2w
2Ïw
4w
2x 2 1 (4 2 x 2)
5 }}
2wx 2w
Ïw4w
2
4 2 2x
5 }}
2wx 2w
Ïw4w
Intervals
(d) (2`, `)
(e) Local (and absolute) maximum at < (0.385, 1.215)
(f) None
22 , x , 2Ï2w 2Ï2w , x , Ï2w Ï2w , x , 2
2
1
2
Decreasing
Increasing
Decreasing
Sign of y9
Behavior of y
(c) None
1
1
2
(Ï4
ww
2wx 2w)(24x) 2 (4 2 2x 2) }} (22x)
2wx 2w
2Ï4
ww
y0 5 }}}}}
2
42x
2x(x 2 2 6)
5 }}
(4 2 x 2)3/2
Note that the values x 5 6Ï6w are not zeros of y0 because
they fall outside of the domain.
Intervals
22 , x , 0
0,x,2
Sign of y0
1
2
Behavior of y Concave up Concave down
6. y9 5 e x21 2 1
Intervals
x,1
1,x
Sign of y9
2
1
Behavior of y Decreasing Increasing
y0 5 e x21
The second derivative is always positive, so the function is
concave up for all x.
Graphical support:
[24, 4] by [22, 4]
(a) [1, `)
Graphical support:
(b) (2`, 1]
(c) (2`, `)
(d) None
(e) Local (and absolute) minimum at (1, 0)
(f) None
[22.35, 2.35] by [23.5, 3.5]
(a) [2Ï2w, Ï2w]
(b) [22, 2Ï2w] and [Ï2w, 2]
(c) (22, 0)
(d) (0, 2)
(e) Local maxima: (22, 0), (Ï2w, 2)
Local minima: (2, 0), (2Ï2w, 22)
Note that the extrema at x 5 6Ïw2 are also absolute
extrema.
(f) (0, 0)
188
Chapter 4 Review
Graphical support:
7. Note that the domain is (21, 1).
y 5 (1 2 x 2)21/4
1
4
x
2(1 2 x )
y9 5 2}}(1 2 x 2)25/4(22x) 5 }}
2 5/4
[24.7, 4.7] by [23.1, 3.1]
21 , x , 0 0 , x , 1
Intervals
2
1
Decreasing
Increasing
Sign of y9
Behavior of y
(a) (2`, 2221/3] < (2`, 20.794]
(b) [2221/3, 1) < [20.794, 1) and (1, `)
(c) (2`, 221/3) < (2`, 21.260) and (1, `)
142
(d) (221/3, 1) < (21.260, 1)
5
2(1 2 x 2)5/4(1) 2 (x)(2) }} (1 2 x 2)1/4(22x)
y0 5 }}}}}
2 5/2
4(1 2 x )
(e) Local maximum at
(1 2 x 2)1/4[2 2 2x 2 1 5x 2]
5 }}}
4(1 2 x 2)5/2
12221/3, }3} ? 221/32 < (20.794, 0.529)
2
3x 2 1 2
4(1 2 x )
5 }}
2 9/4
(f)
The second derivative is always positive, so the function is
concave up on its domain (21, 1).
Graphical support:
1221/3, }3} ? 21/32 < (21.260, 0.420)
1
9. Note that the domain is [21, 1].
1
y9 5 2}}
2wx 2w
Ï1ww
Since y9 is negative on (21, 1) and y is continuous, y is
decreasing on its domain [21, 1].
d
dx
1
x
5 }}(1 2 x 2)23/2(22x) 5 2}}
2
(1 2 x 2)3/2
y0 5 }}[2(1 2 x 2)21/2]
[21.3, 1.3] by [21, 3]
(a) [0, 1)
(b) (21, 0]
(c) (21, 1)
21 , x , 0
Intervals
(d) None
Behavior of y
(f) None
(x 3 2 1)(1) 2 (x)(3x 2)
(x 2 1)
2x 3 1 1
(x 2 1)
x ,2221/3 2221/3 , x , 1
1
Sign of y9
Behavior of y Increasing
1,x
2
2
Decreasing
Decreasing
p 5p
[21.175, 1.175] by 2}}, }}
3
(x 3 2 1)2(6x 2) 2 (2x 3 1 1)(2)(x 3 2 1)(3x 2)
(x 2 1)
3
(d) (0, 1)
6x 2(x 3 1 2)
5}
}
(x 3 2 1)3
(e) Local (and absolute) maximum at (21, p);
local (and absolute) minimum at (1, 0)
(f)
Sign of y0
4
(c) (21, 0)
2
5 2}}}}
3
3
Intervals
4
(b) [21, 1]
(x 2 1)(6x ) 2 (2x 1 1)(6x )
(x 2 1)
2
4
(a) None
y0 5 2}}}}}
3
4
3
2
Concave down
Graphical support:
8. y9 5 }}}
5 2}
3
2
3 }
2
Intervals
1
Concave up
Sign of y0
(e) Local minimum at (0, 1)
0,x,1
x , 221/3 221/3 , x , 0
1
2
0,x,1
1,x
2
1
Behavior of y Concave up Concave down Concave down Concave up
p
10, }2}2
Chapter 4 Review
10. This problem can be solved graphically by using NDER to obtain the graphs shown below.
y
y9
y0
[24, 4] by [21, 0.3]
[24, 4] by [20.4, 0.6]
[24, 4] by [20.7, 0.8]
An alternative approach using a combination of algebraic and graphical techniques follows.
Note that the denominator of y is always positive because it is equivalent to (x 1 1)2 1 2.
(x 2 1 2x 1 3)(1) 2 (x)(2x 1 2)
(x 1 2x 1 3)
2x 2 1 3
5 }}
(x 2 1 2x 1 3)2
y9 5 }}}}
2
2
Intervals
x , 2Ï3w 2Ï3w , x , Ï3w
2
Sign of y9
Behavior of y Decreasing
Ï3w , x
1
2
Increasing
Decreasing
(x 2 1 2x 1 3)2(22x) 2 (2x 2 1 3)(2)(x 2 1 2x 1 3)(2x 1 2)
(x 1 2x 1 3)
y0 5 }}}}}}}
2
4
(x 2 1 2x 1 3)(22x) 2 2(2x 1 2)(2x 2 1 3)
5 }}}}}
2
3
(x 1 2x 1 3)
2x 3 2 18x 2 12
5}
}
(x 2 1 2x 1 3)3
Using graphing techniques, the zeros of 2x 3 2 18x 2 12 (and hence of y0) are at
x < 22.584, x < 20.706, and x < 3.290.
Intervals
(2`, 22.584) (22.584, 20.706) (20.706, 3.290)
Sign of y0
1
2
1
Concave up
Concave down
Concave up
2
Behavior of y Concave down
(a) [2Ï3w, Ï3w]
(b) (2`, 2Ï3w] and [Ï3w, `)
(c) Approximately (22.584, 20.706) and (3.290, `)
(d) Approximately (2`, 22.584) and (20.706, 3.290)
Ïw3 2 1
(e) Local maximum at Ï3w, }}
1
2
4
< (1.732, 0.183);
w21
2Ï3
local minimum at 2Ï3w, }}
1
4
(3.290, `)
2
< (21.732, 20.683)
(f) <(22.584, 20.573), (20.706, 20.338), and
(3.290, 0.161)
189
190
Chapter 4 Review
d
1
dx
x
d
1
1
For x , 0: y9 5 }} ln (2x) 5 }}(21) 5 }}
dx
2x
x
1
Thus y9 5 }} for all x in the domain.
x
11. For x . 0, y9 5 }} ln x 5 }}
Intervals
(22, 0)
(0, 2)
Sign of y9
2
1
Behavior of y Decreasing
Increasing
y0 5 2x22
The second derivative is always negative, so the function is concave down on
each open interval of its domain.
Graphical support:
[22.35, 2.35] by [23, 1.5]
(a) (0, 2]
(b) [22, 0)
(c) None
(d) (22, 0) and (0, 2)
(e) Local (and absolute) maxima at (22, ln 2) and (2, ln 2)
(f) None
12. y9 5 3 cos 3x 2 4 sin 4x
Using graphing techniques, the zeros of y9 in the domain
p
2
3p
x < 2.148, and x < 2.965, x < 3.834, x 5 }}, x < 5.591
2
0 # x # 2p are x < 0.176, x < 0.994, x 5 }} < 1.57,
Intervals
Sign of y9
Behavior of y
Intervals
Sign of y9
Behavior of y
p p
2 2
0 , x , 0.176 0.176 , x , 0.994 0.994 , x , }} }} , x , 2.148 2.148 , x , 2.965
1
2
1
2
1
Increasing
Decreasing
Increasing
Decreasing
Increasing
2.965 , x , 3.834
3p
2
3.834 , x , }}
3p
}} , x , 5.591 5.591 , x , 2p
2
2
1
2
1
Decreasing
Increasing
Decreasing
Increasing
Chapter 4 Review
y0 5 29 sin 3x 2 16 cos 4x
Using graphing techniques, the zeros of y0 in the domain
0 # x # 2p are x < 0.542, x < 1.266, x < 1.876,
x < 2.600, x < 3.425, x < 4.281, x < 5.144 and x < 6.000.
Intervals
0 , x , 0.542 0.542 , x , 1.266 1.266 , x , 1.876 1.876 , x , 2.600 2.600 , x , 3.425
Behavior of y Concave down
Intervals
1
2
1
2
Concave up
Concave down
Concave up
Concave down
2
Sign of y0
3.425 , x , 4.281 4.281 , x , 5.144 5.144 , x , 6.000 6.000 , x , 2p
1
2
1
2
Concave up
Concave down
Concave up
Concave down
Sign of y0
Behavior of y
Graphical support:
p 9p
32}4}, }4}4 by [22.5, 2.5]
p
2
3
4
3
3p
2
4
3
(a) Approximately [0, 0.176], 0.994, }} , [2.148, 2.965], 3.834, }} , and 5.591, 2p
p
32
3p
4
32
(b) Approximately [0.176, 0.994], }}, 2.148 , [2.965, 3.834], and }}, 5.591
4
4
(c) Approximately (0.542, 1.266), (1.876, 2.600), (3.425, 4.281), and (5.144, 6.000)
(d) Approximately (0, 0.542), (1.266, 1.876), (2.600, 3.425), (4.281, 5.144), and (6.000, 2p)
p
12 2
(e) Local maxima at <(0.176, 1.266), }}, 0
3p
12 2
and (2.965, 1.266), }}, 2 , and (2p,1);
local minima at <(0, 1), (0.994, 20.513),
(2.148, 20.513), (3.834, 21.806),
and (5.591, 21.806)
3p
2
Note that the local extrema at x < 3.834, x 5 }},
and x < 5.591 are also absolute extrema.
(f) <(0.542, 0.437), (1.266, 20.267), (1.876, 20.267), (2.600, 0.437), (3.425, 20.329), (4.281, 0.120),
(5.144, 0.120), and (6.000, 20.329)
191
192
Chapter 4 Review
13. y9 5
,
h2e
4 2 3x ,
2x
2
x,0
x.0
Intervals
x,0
0 , x , }}
Ïw3
2
}} , x
Ïw3
Sign of y9
2
1
2
Increasing
Decreasing
2
Behavior of y Decreasing
y0 5
h
e 2x,
26x,
x,0
x.0
Intervals
x,0
0,x
Sign of y0
1
2
Behavior of y Concave up Concave down
Graphical support:
[24, 4] by [22, 4]
1
2
(a) 0, }}
Ïw3
4
3
2
(b) (2`, 0] and }}, `
Ï3w
(c) (2`, 0)
2
(d) (0, `)
1
2
16
2
(e) Local maximum at }}, }} < (1.155, 3.079)
Ïw3 3Ï3w
(f) None. Note that there is no point of inflection at x 5 0 because the derivative is undefined and no tangent line exists
at this point.
14. y9 5 25x 4 1 7x 2 1 10x 1 4
Using graphing techniques, the zeros of y9 are x < 20.578 and x < 1.692.
Intervals
x , 20.578 20.578 , x , 1.692 1.692 , x
2
1
2
Decreasing
Increasing
Decreasing
Sign of y9
Behavior of y
y0 5 220x 3 1 14x 1 10
Using graphing techniques, the zero of y0 is x < 1.079.
Intervals
x , 1.079
1.079 , x
Sign of y0
1
2
Behavior of y Concave up Concave down
Graphical support:
[24, 4] by [210, 25]
Chapter 4 Review
(a) Approximately [20.578, 1.692]
(b) Approximately (2`, 20.578] and [1.692, `)
(c) Approximately (2`, 1.079)
(d) Approximately (1.079, `)
(e) Local maximum at < (1.692, 20.517);local minimum at < (20.578, 0.972)
(f) <(1.079, 13.601)
15. y 5 2x 4/5 2 x 9/5
8
8 2 9x
9
y9 5 }}x 21/5 2 }}x 4/5 5 }5}
5
5
5Ïwx
Intervals
x,0
0 , x , }}
8
9
8
}} , x
9
Sign of y9
2
1
2
Increasing
Decreasing
Behavior of y Decreasing
4(2 1 9x)
25x
36
25
8
25
y0 5 2}}x 26/5 2 }}x 21/5 5 2}}
6/5
2
9
2
9
Intervals
x , 2}}
2}} , x , 0
0,x
Sign of y0
1
2
2
Behavior of y Concave up Concave down Concave down
Graphical support:
[24, 4] by [23, 3]
3 94
8
(a) 0, }}
39 2
8
(b) (2`, 0] and }}, `
1
2
9
(c) 2`, 2}}
1
2
9
2
2
(d) 2}}, 0 and (0, `)
8 4/5
19
1 9 2 2 < (0.889, 1.011);
8 10
9
(e) Local maximum at }}, }} ? }}
local minimum at (0, 0)
(f)
2 4/5
12}9}, }9} ? 12}9}2 2 < 12}9}, 0.6672
2 20
2
193
194
Chapter 4 Review
16. We use a combination of analytic and grapher techniques to solve this problem. Depending on the viewing windows chosen,
graphs obtained using NDER may exhibit strange behavior near x 5 2 because, for example, NDER (y, 2) < 5,000,000 while y9
5 2 4x 1 4x 2 2 x 3
x22
is actually undefined at x 5 2. The graph of y 5 }} is shown below.
[25.875, 5.875] by [250, 30]
(x 2 2)(24 1 8x 2 3x 2) 2 (5 2 4x 1 4x 2 2 x 3)(1)
(x 2 2)
22x 3 1 10x2 2 16x 1 3
5 }}}
(x 2 2)2
y9 5 }}}}}}
2
The graph of y9 is shown below.
[25.875, 5.875] by [250, 30]
The zero of y9 is x < 0.215.
Intervals
Sign of y9
x , 0.215 0.215 , x , 2
1
Behavior of y Increasing
2,x
2
2
Decreasing
Decreasing
(x 2 2)2(26x 2 1 20x 2 16) 2 (22x 3 1 10x 2 2 16x 1 3)(2)(x 2 2)
(x 2 2)
y0 5 }}}}}}}
4
(x 2 2)(26x 2 1 20x 2 16) 2 2(22x 3 1 10x 2 2 16x 1 3)
(x 2 2)
5 }}}}}}
3
22(x 3 2 6x 2 1 12x 2 13)
(x 2 2)
5 }}}
3
The graph of y0 is shown below.
[25.875, 5.875] by [220, 20]
The zero of x 3 2 6x 2 1 12x 2 13
(and hence of y0) is x < 3.710.
Intervals
x,2
Sign of y0
2
Behavior of y Concave down
2 , x , 3.710
1
2
Concave up
Concave down
(a) Approximately (2`, 0.215]
(b) Approximately [0.215, 2) and (2, `)
(c) Approximately (2, 3.710)
(d) (2`, 2) and approximately (3.710, `)
(e) Local maximum at < (0.215, 22.417)
(f) <(3.710, 23.420)
3.710 , x
Chapter 4 Review
17. y9 5 6(x 1 1)(x 2 2)2
3
4
Intervals
x , 21
21 , x , 2
2,x
Sign of y9
2
1
1
Increasing
Increasing
Behavior of y Decreasing
1
3
1
2
1
3
1
2
f (x) 5 }}x 4/3 1 }}x 3 1 }}x 2 1 x 1 C
24.
f (1) 5 0
3
1
1
}} 1 }} 1 }} 1 1 1 C 5 0
4
3
2
31
12
C 5 2}}
y0 5 6(x 1 1)(2)(x 2 2) 1 6(x 2 2) (1)
5 6(x 2 2)[(2x 1 2) 1 (x 2 2)]
5 18x(x 2 2)
2
3
4
Intervals
x,0
0,x,2
2,x
Sign of y0
1
2
1
Behavior of y Concave up Concave down Concave up
(a) There are no local maxima.
(b) There is a local (and absolute) minimum at x 5 21.
(c) There are points of inflection at x 5 0 and at x 5 2.
18. y9 5 6(x 1 1)(x 2 2)
Intervals
x , 21
Sign of y9
1
21 , x , 2
Behavior of y Increasing
2,x
2
1
Decreasing
Increasing
Sign of y0
25. v(t)
s(t)
s(0)
C
s(t)
5 s9(t) 5 9.8t 1 5
5 4.9t 2 1 5t 1 C
5 10
5 10
5 4.9t 2 1 5t 1 10
26. a(t) 5 v9(t) 5 32
v(t) 5 32t 1 C1
v(0) 5 20
C1 5 20
v(t)
s(t)
s(0)
C2
s(t)
5 s9(t) 5 32t 1 20
5 16t 2 1 20t 1 C2
55
55
5 16t 2 1 20t 1 5
27. f (x) 5 tan x
d
dx
y0 5 }}6(x 2 2 x 2 2) 5 6(2x 2 1)
Intervals
1
x , }}
2
1
}} , x
2
2
1
Behavior of y Concave down Concave up
(a) There is a local maximum at x 5 21.
(b) There is a local minimum at x 5 2.
f 9(x) 5 sec2 x
p
p
p
1 4 2 1 4 23 1 4 24
p
p
p
5 tan 12}}2 1 sec2 12}}21x 1 }}2
4
4
4
p
5 21 1 21x 1 }}2
4
L(x) 5 f 2}} 1 f 9 2}} x 2 2}}
p
2
5 2x 1 }} 2 1
1
2
(c) There is a point of inflection at x 5 }}.
1
2
1
d
19. Since }} 2}}x 24 2 e 2x 5 x 25 1 e 2x,
4
dx
1
f (x) 5 2}}x 24 2 e 2x 1 C.
4
d
dx
20. Since }} sec x 5 sec x tan x, f (x) 5 sec x 1 C.
d
dx
1
2
1
3
2
x
21. Since }} 2 ln x 1 }}x 3 1 x 5 }} 1 x 2 1 1,
1
3
f (x) 5 2 ln x 1 }}x 3 1 x 1 C.
1
d 2
2
3
23.
f (x)
f (p)
1101C
C
f (x)
5 2cos x 1 sin x 1 C
53
53
52
5 2cos x 1 sin x 1 2
28. f (x) 5 sec x
f 9(x) 5 sec x tan x
p
p
p
1 4 2 1 4 21 4 2
p
p
p
p
5 sec 1}}2 1 sec 1}}2 tan 1}}21x 2 }}2
4
4
4
4
p
5 Ï2w 1 Ï2w(1)1x 2 }}2
4
L(x) 5 f }} 1 f 9 }} x 2 }}
pÏ2w
5 Ï2wx 2 }} 1 Ï2w
4
1
22. Since }} }}x 3/2 1 2x 1/2 5 Ïxw 1 }},
dx 3
Ïwx
2
f (x) 5 }}x 3/2 1 2x 1/2 1 C.
31
12
f (x) 5 }}x 4/3 1 }}x 3 1 }}x 2 1 x 2 }}
1
1 1 tan x
29. f (x) 5 }}
f 9(x)5 2(1 1 tan x)22(sec2 x)
1
cos x(1 1 tan x)
1
5 2}}2
(cos x 1 sin x)
5 2}
}2
2
L(x) 5 f (0) 1 f 9(0)(x 2 0)
5 1 2 1(x 2 0)
5 2x 1 1
195
196
Chapter 4 Review
30. f (x) 5 e x 1 sin x
f 9(x) 5 e x 1 cos x
L(x) 5 f (0) 1 f 9(0)(x 2 0)
5 1 1 2(x 2 0)
5 2x 1 1
1x2
1
(b) f 9(x) 5 (x) }} 1 (ln x)(1) 5 1 1 ln x
Using a 5 0.5 and b 5 3, we solve as follows.
f (3) 2 f (0.5)
3 2 0.5
f 9(c) 5 }}
1
2
31. The global minimum value of }} occurs at x 5 2.
32. (a) The values of y9 and y0 are both negative where the
graph is decreasing and concave down, at T.
(b) The value of y9 is negative and the value of y0 is positive where the graph is decreasing and concave up, at
P.
33. (a) The function is increasing on the interval (0, 2].
(b) The function is decreasing on the interval [23, 0).
(c) The local extreme values occur only at the endpoints of
the domain. A local maximum value of 1 occurs at
x 5 23, and a local maximum value of 3 occurs at
x 5 2.
34. The 24th day
35.
3 ln 3 2 0.5 ln 0.5
2.5
1 1 ln c 5 }}
1
33
2
ln }}
0.50.5
ln c 5 }} 2 1
2.5
ln c 5 0.4 ln(27Ï2w) 2 1
c 5 e 21(27Ï2w)0.4
5
c 5 e 21Ï1w4w5w8w < 1.579
(c) The slope of the line is
y
f (b) 2 f (a)
b2a
m 5 }} 5 0.4 ln (27Ï2w) 5 0.2 ln 1458, and
2
the line passes through (3, 3 ln 3). Its equation is
–3
3
x
y 5 0.2(ln 1458)(x 2 3) 1 3 ln 3, or approximately
y 5 1.457x 2 1.075.
y = f(x)
–3
36. (a) We know that f is decreasing on [0, 1] and increasing
on [1, 3], the absolute minimum value occurs at x 5 1
and the absolute maximum value occurs at an endpoint.
Since f (0) 5 0, f (1) 5 22, and f (3) 5 3, the absolute
minimum value is 22 at x 5 1 and the absolute maximum value is 3 at x 5 3.
(b) The concavity of the graph does not change. There are
no points of inflection.
(c)
y
(d) The slope of the line is m 5 0.2 ln 1458, and the line
passes through
5
5
(c, f (c)) 5 (e21Ïw1w4w5w8, e21Ïw1w4w5w8(21 1 0.2 ln 1458))
< (1.579, 0.722).
Its equation is
y 5 0.2(ln 1458)(x 2 c) 1 f (c),
5
y 5 0.2 ln 1458(x 2 e 21Ïw1w4w5w8)
5
1 e 21Ïw1w4w5w8(21 1 0.2 ln 1458),
5
y 5 0.2(ln 1458)x 2 e 21Ïw1w4w5w8,
or approximately y 5 1.457x 2 1.579.
38. (a) v(t) 5 s9(t) 5 4 2 6t 2 3t 2
3
(b) a(t) 5 v9(t) 5 26 2 6t
–1
1
3
4
x
–3
37. (a) f (x) is continuous on [0.5, 3] and differentiable on
(0.5, 3).
(c) The particle starts at position 3 moving in the positive
direction, but decelerating. At approximately t 5 0.528,
it reaches position 4.128 and changes direction, beginning to move in the negative direction. After that, it
continues to accelerate while moving in the negative
direction.
39. (a) L(x) 5 f (0) 1 f 9(0)(x 2 0)
5 21 1 0(x 2 0) 5 21
(b) f (0.1) < L(0.1) 5 21
(c) Greater than the approximation in (b), since f 9(x) is
actually positive over the interval (0, 0.1) and the
estimate is based on the derivative being 0.
dy
dx
40. (a) Since }} 5 (x 2)(2e2x) 1 (e2x)(2x) 5 (2x 2 x 2)e2x,
dy 5 (2x 2 x 2)e2x dx.
(b) dy 5 [2(1) 2 (1)2](e21)(0.01)
5 0.01e21
< 0.00368
Chapter 4 Review
2701.73
1 1 17.28e
41. (a) Regression equation y 5 }}
20.36x
[0, 20] by [2300, 2800]
(b) Note that
d
dx
y9 5 }}2701.73(1 1 17.28e 20.36x)21
5 22701.73(1 1 17.28e20.36x)22(17.28)(20.36e 20.36x)
197
43. Let t represent time in seconds, where the rocket lifts off at
t 5 0. Since a(t) 5 v9(t) 5 20 m/sec2 and v(0) 5 0 m/sec,
we have v(t) 5 20t, and so v(60) 5 1200 m/sec. The speed
after 1 minute (60 seconds) will be 1200 m/sec.
44. Let t represent time in seconds, where the rock is blasted
upward at t 5 0. Since a(t) 5 v9(t) 5 23.72 m/sec2 and
v(0) 5 93 m/sec, we have v(t) 5 23.72t 1 93. Since
s9(t) 5 23.72t 1 93 and s(0) 5 0, we have
s(t) 5 21.86t 2 1 93t. Solving v(t) 5 0, we find that the
rock attains its maximum height at t 5 25 sec and its height
at that time is s(25) 5 1162.5 m.
45. Note that s 5 100 2 2r and the sector area is given by
1 2pr 2
s
16,806.9e 20.36x
(1 1 17.28e
)
1
2
1
2
A 5 pr 2 }} 5 }}rs 5 }}r(100 2 2r) 5 50r 2 r 2. To find
< }}}
20.36x 2
the domain of A(r) 5 50r 2 r 2, note that r . 0 and
The graph of y9 is shown below.
50
p11
0 , s , 2pr, which gives 12.1 < }} , r , 50. Since
A9(r) 5 50 2 2r, the critical point occurs at r 5 25. This
value is in the domain and corresponds to the maximum
area because A0(r) 5 22, which is negative for all r.
[0, 20] by [275, 275]
Using graphing techniques, y9 has its maximum at
x < 7.92. This corresponds to the year 1998 and
represents the inflection point of the logistic curve. The
logistic regression equation predicts that the rate of
increase in debit card transactions will begin to
decrease in 1998, and since y(7.92) < 1351, there are
approximately 1351 million transactions that year.
The greatest area is attained when r 5 25 ft and s 5 50 ft.
46.
y
27
(x, 27 – x2)
(c) As x increases, the value of y will increase toward
2701.73. The logistic regression equation predicts a
ceiling of approximately 2702 million transactions per
year.
–4
4
x
42. f (x) 5 2 cos x 2 Ï1ww
1wx
1
f 9(x) 5 22 sin x 2 }}
1wx
2Ï1
ww
f (xn)
xn11 5 xn 2 }}
f 9(xn)
2 cos xn 2 Ï1
ww
1wxwn
5 xn 2 }}}
1
22 sin xn 2 }}
1wxnw
2Ï1
ww
The graph of y 5 f (x) shows that f (x) 5 0 has one solution,
near x 5 1.
For 0 , x , Ï2w7w, the triangle with vertices at (0, 0) and
(6x, 27 2 x 2) has an area given by
1
2
A(x) 5 }}(2x)(27 2 x 2) 5 27x 2 x 3. Since
A9 5 27 2 3x 2 5 3(3 2 x)(3 1 x) and A0 5 26x, the
critical point in the interval (0, Ï2w7w) occurs at x 5 3 and
corresponds to the maximum area because A0(x) is negative
in this interval. The largest possible area is
A(3) 5 54 square units.
[22, 10] by [26, 2]
x1 5 1
x2 < 0.8361848
x3 < 0.8283814
x4 < 0.8283608
x5 < 0.8283608
Solution: x < 0.828361
198
Chapter 4 Review
47. If the dimensions are x ft by x ft by h ft, then the total
r
6
12 2 h
12
50. Note that, from similar cones, }} 5 }}, so h 5 12 22r.
amount of steel used is x 2 1 4xh ft2. Therefore,
The volume of the smaller cone is given by
108 2 x 2
x 1 4xh 5 108 and so h 5 }}. The volume is given
4x
108x 2 x 3
2
by V(x) 5 x h 5 }} 5 27x 2 0.25x 3. Then
4
2
1
3
2p
3
1
3
V 5 }}pr 2h 5 }}pr 2(12 2 2r) 5 4pr 2 2 }}r 3 for
dV
dr
0 , r , 6. Then }} 5 8pr 2 2pr 2 5 2pr(4 2 r), so the
V9(x) 5 27 2 0.75x 5 0.75(6 1 x)(6 2 x) and
2
critical point occurs at r 5 4. This critical point
V0(x) 5 21.5x. The critical point occurs at x 5 6, and it
dV
dr
corresponds to the maximum volume because }} . 0 for
corresponds to the maximum volume because V0(x) , 0 for
dV
dr
0 , r , 4 and }} , 0 for 4 , r , 6. The smaller cone has
108 2 62
x . 0. The corresponding height is }} 5 3 ft. The
4(6)
the largest possible value when r 5 4 ft and h 5 4 ft.
base measures 6 ft by 6 ft, and the height is 3 ft.
51.
48. If the dimensions are x ft by x ft by h ft, then we have
Lid
32
x
x 2h 5 32 and so h 5 }}2 . Neglecting the quarter-inch
thickness of the steel, the area of the steel used is
x
10 in.
Base
128
A(x) 5 x 2 1 4xh 5 x 2 1 }}. We can minimize the weight
x
x
of the vat by minimizing this quantity. Now
2
x
A9(x) 5 2x 2 128x 22 5 }}2 (x 3 2 43) and
A0(x) 5 2 1 256x23. The critical point occurs at x 5 4 and
x
x
15 in.
(a) V(x) 5 x(15 2 2x)(5 2 x)
(b, c) Domain: 0 , x , 5
corresponds to the minimum possible area because
A0(x) . 0 for x . 0. The corresponding height is
32
5 2 ft. The base should measure 4 ft by 4 ft, and the
}}
42
[0, 5] by [220, 70]
height should be 2 ft.
h 2
122
49. We have r 2 1 }}
h
4
5 3, so r 2 5 3 2 }}. We wish to
minimize the cylinder’s volume
h2
ph 3
4
4
dV
3ph 2
3p
Since }} 5 3p 2 }} 5 }}(2 1 h)(2 2h) and
dh
4
4
d 2V
3ph
5
2
,
the
critical
point
occurs at h 5 2 and it
}}
}
}
dh 2
2
d 2V
corresponds to the maximum value because }}2 , 0 for
dh
22
h . 0. The corresponding value of r is 3 2 }} 5 Ï2w.
4
1
The maximum volume is approximately 66.019 in3 and
it occurs when x < 1.962 in.
2
2
V 5 pr 2h 5 p 3 2 }} h 5 3ph 2 }} for 0 , h , 2Ï3w.
!§§§§
The largest possible cylinder has height 2 and radius Ï2w.
(d) Note that V(x) 5 2x 3 2 25x 2 1 75x,
so V9(x) 5 6x 2 2 50x 1 75.
Solving V9(x) 5 0, we have
x
w0w
50 6 Ï(2
w5
w0
ww
)2w
2w(6
4w)(
w7
w5
w)w
50 6 Ï7w0
5 }}} 5 }}
2(6)
12
w 25 6 5Ï7w
50 6 10Ï7
5 }} 5 }}.
12
6
These solutions are approximately x < 1.962 and
x < 6.371, so the critical point in the appropriate
domain occurs at
25 2 5Ïw
7
x 5 }}.
6
Chapter 4 Review
52.
199
54. The length of the track is given by 2x 1 2pr, so we have
y
10
2x 1 2pr 5 400 and therefore x 5 200 2 pr. Then the area
of the rectangle is
(x, 8 cos 0.3x)
A(r) 5 2rx
5 2r(200 2 pr)
–2π
π
–π
2π
200
p
x
5 400r 2 2pr 2, for 0 , r , }}.
Therefore, A9(r) 5 400 2 4pr and A0(r) 5 24p, so the
5p
3
For 0 , x , }}, the area of the rectangle is given by
A(x) 5 (2x)(8 cos 0.3x) 5 16x cos 0.3x.
100
p
critical point occurs at r 5 }} m
and this point corresponds to the maximum rectangle area
Then A9(x) 5 16x(20.3 sin 0.3x) 1 16(cos 0.3x)(1)
5 16(cos 0.3x 2 0.3x sin 0.3x)
because A0(r) , 0 for all r.
The corresponding value of x is
Solving A9(x) 5 0 graphically, we find that the critical
point occurs at x < 2.868 and the corresponding area is
approximately 29.925 square units.
1p2
100
x 5 200 2 p }} 5 100 m.
The rectangle will have the largest possible area when
100
p
x 5 100 m and r 5 }} m.
53. The cost (in thousands of dollars) is given by
55. Assume the profit is k dollars per hundred grade B tires and
C(x) 5 40x 1 30(20 2 y) 5 40x 1 600 2 30Ïw
x w
2w14w4w.
2
30
30x
Then C9(x) 5 40 2 }}(2x) 5 40 2 }}.
2
2
2w1w
2w
1w
2Ïw
x w
4w
4
Ïw
x w
4w
4
2k dollars per hundred grade A tires.
Then the profit is given by
Solving C9(x) 5 0, we have:
30x
}} 5 40
2w
14
Ïw
x 2w
w4w
3x 5 4Ïw
x 2w
2w14w4w
9x 2 5 16x 2 2 2304
2304 5 7x 2
Choose the positive solution:
48
x 5 1}} < 18.142 mi
Ïw7
36
y 5 Ïw
x 2w
2w1w22w 5 }} < 13.607 mi
Ïw7
40 2 10x
52x
P(x) 5 2kx 1 k ? }}
(20 2 5x) 1 x(5 2 x)
52x
5 2k ? }}}
20 2 x 2
52x
5 2k ? }}
(5 2 x)(22x) 2 (20 2 x 2)(21)
(5 2 x)
P9(x) 5 2k ? }}}}
2
x 2 2 10x 1 20
(5 2 x)
5 2k ? }}
2
The solutions of P9(x) 5 0 are
10 6 Ï(2
w1w0w)w2w
2w4(1
w)(
w2w0w)w
x 5 }}} 5 5 6 Ï5w, so the solution in
2(1)
the appropriate domain is x 5 5 2 Ï5w < 2.76.
Check the profit for the critical point and endpoints:
Critical point:
x < 2.76
P(x) < 11.06k
Endpoints:
x50
P(x) 5 8k
x54
P(x) 5 8k
The highest profit is obtained when x < 2.76 and y < 5.53,
which corresponds to
276 grade A tires and 553 grade B tires.
200
Chapter 4 Review
56. (a) The distance between the particles is ) f (t)) where
p
1 42
p
f 9(t) 5 2sin t 1 sin 1t 1 }}2
4
f (t) 5 2cos t 1 cos t 1 }} . Then
Solving f 9(t) 5 0 graphically, we obtain t < 1.178, t < 4.230, and so on.
[0, 2p] by [22, 2]
Alternatively, f 9(t) 5 0 may be solved analytically as follows.
p
p
p
p
31t 1 }8}2 2 }8}4 2 sin 31t 1 }8}2 1 }8}4
p
p
p
p
p
p
p
p
5 3sin 1t 1 }}2 cos }} 2 cos 1t 1 }}2 sin }}4 2 3sin 1t 1 }}2 cos }} 1 cos 1t 1 }}2 sin }}4
8
8
8
8
8
8
8
8
p
p
5 22 sin }} cos 1t 1 }}2,
8
8
f 9(t) 5 sin
so the critical points occur when
1
p
8
2
3p
8
cos t 1 }} 5 0, or t 5 }} 1 kp. At each of these values,
3p
8
f (t) 5 62 cos }} < 60.765 units, so the maximum distance between
the particles is 0.765 units.
1
p
4
2
(b) Solving cos t 5 cos t 1 }} graphically, we obtain t < 2.749, t < 5.890, and so on.
[0, 2p] by [22, 2]
Alternatively, this problem may be solved analytically as follows.
p
1 42
p
p
p
p
cos 31t 1 }}2 2 }}4 5 cos 31t 1 }}2 1 }}4
8
8
8
8
p
p
p
p
p
p
p
p
cos 1t 1 }}2 cos }} 1 sin 1t 1 }}2 sin }} 5 cos 1t 1 }}2 cos }} 2 sin 1t 1 }}2 cos }}
8
8
8
8
8
8
8
8
p
p
2 sin 1t 1 }}2 sin }} 5 0
8
8
p
sin 1t 1 }}2 5 0
8
cos t 5 cos t 1 }}
7p
8
t 5 }} 1 kp
7p
8
The particles collide when t 5 }} < 2.749 (plus multiples of p if they keep going.)
Chapter 4 Review
57. The dimensions will be x in. by 10 2 2x in. by 16 2 2x in.,
so V(x) 5 x(10 2 2x)(16 2 2x) 5 4x 3 2 52x 2 1 160x
for 0 , x , 5.
Then V9(x) 5 12x 2 2 104x 1 160 5 4(x 2 2)(3x 2 20), so
the critical point in the correct domain is x 5 2.
This critical point corresponds to the maximum possible
volume because V9(x) . 0 for 0 , x , 2
and V9(x) , 0 for 2 , x , 5. The box of largest volume
has a height of 2 in. and a base measuring
6 in. by 12 in., and its volume is 144 in3.
201
59. Step 1:
x 5 x-coordinate of particle
y 5 y-coordinate of particle
D 5 distance from origin to particle
Step 2:
At the instant in question, x 5 5 m, y 5 12 m,
dx
dy
}} 5 21 m/sec, and }} 5 25 m/sec.
dt
dt
Step 3:
Graphical support:
dD
dt
We want to find }}.
Step 4:
D 5 Ïw
x 2w
1wy 2w
[0, 5] by [240, 160]
Step 5:
58. Step 1:
r 5 radius of circle
A 5 area of circle
dx
dy
x}} 1 y}}
dt
dt
dD
1
dx
dy
}}
}} 5 }} 2x}} 1 2y}} 5
2
dt
dt
dt
Ïw
x w
1wy 2w
1wy 2w
2Ïw
x 2w
1
2
Step 6:
Step 2:
dr
dt
2
p
At the instant in question, }} 5 2}} m/sec and r 5 10 m.
Step 3:
dA
dt
(5)(21) 1 (12)(25)
dD
5 25 m/sec
}} 5 }}}
dt
Ï5w2w1
ww12w2w
dD
Since }} is negative, the particle is approaching the origin
dt
at the positive rate of 5 m/sec.
We want to find }}.
60. Step 1:
x 5 edge of length of cube
V 5 volume of cube
Step 4:
A 5 pr 2
Step 5:
Step 2:
dA
dr
}} 5 2pr}}
dt
dt
At the instant in question,
Step 6:
dV
}} 5 1200 cm3/min and x 5 20 cm.
dt
1 2
dA
2
}} 5 2p(10) 2}} 5 240
dt
p
Step 3:
The area is changing at the rate of 240 m /sec.
2
dx
dt
We want to find }}.
Step 4:
V 5 x3
Step 5:
dV
dx
}} 5 3x 2}}
dt
dt
Step 6:
dx
dt
1200 5 3(20)2}}
dx
}} 5 1 cm/min
dt
The edge length is increasing at the rate of 1 cm/min.
202
Chapter 4 Review
63. Step 1:
r 5 radius of outer layer of cable on the spool
u 5 clockwise angle turned by spool
s 5 length of cable that has been unwound
61. Step 1:
x 5 x-coordinate of point
y 5 y-coordinate of point
D 5 distance from origin to point
Step 2:
Step 2:
dD
dt
At the instant in question, x 5 3 and }} 5 11 units per sec.
ds
dt
At the instant in question, }} 5 6 ft/sec and r 5 1.2 ft
Step 3:
Step 3:
du
dt
We want to find }}.
dx
We want to find }}.
dt
Step 4:
Step 4:
s 5 ru
Since D 2 5 x 2 1 y 2 and y 5 x 3/2, we have
Step 5:
D 5 Ïw
x 2w
1wx 3w for x $ 0.
ds
dt
du
dt
Since r is essentially constant, }} 5 r}}.
Step 6:
Step 5:
du
dt
6 5 1.2}}
dD
1
dx
}} 5 }}(2x 1 3x 2)}}
dt
dt
1wx 3w
2Ïw
x 2w
2
3x 1 2 dx
2x 1 3x dx
5 }} }} 5 }} }}
1wx dt
1wx dt
2xÏ1ww
2Ï1
ww
du
}} 5 5 radians/sec
dt
The spool is turning at the rate of 5 radians per second.
Step 6:
3(3) 1 2 dx
11 5 }} }}
2Ï4w dt
dx
}} 5 4 units per sec
dt
h
r
10
4
5r
2
2h
5
62. (a) Since }} 5 }}, we may write h 5 }} or r 5 }}.
(b) Step 1:
h 5 depth of water in tank
r 5 radius of surface of water
V 5 volume of water in tank
64. a(t) 5 v9(t) 5 2g 5 232 ft/sec2
Since v(0) 5 32 ft/sec, v(t) 5 s9(t) 5 232t 1 32.
Since s(0) 5 217 ft, s(t) 5 216t 2 1 32t 2 17.
The shovelful of dirt reaches its maximum height when
v(t) 5 0, at t 5 1 sec. Since s(1) 5 21, the shovelful of dirt
is still below ground level at this time. There was not
enough speed to get the dirt out of the hole. Duck!
1
3
2
3
2
3
When the radius changes from a to a 1 dr, the volume
2
3
change is approximately dV 5 }}pah dr.
Step 2:
At the instant in question,
dV
dr
65. We have V 5 }}pr 2h, so }} 5 }}prh and dV 5 }}prh dr.
66. (a) Let x 5 edge of length of cube and S 5 surface area of
dS
dx
dV
}} 5 25 ft3/min and h 5 6 ft.
dt
cube. Then S 5 6x 2, which means }} 5 12x and
Step 3:
dS 5 12x dx. We want )dS) # 0.02S, which gives
We want to find 2}}.
)12x dx) # 0.02(6x 2) or )dx) # 0.01x. The edge should
Step 4:
be measured with an error of no more than 1%.
dh
dt
1
3
4
75
V 5 }}pr 2h 5 }}ph 3
Step 5:
dV
dh
4
}} 5 }}ph 2}}
dt
dt
25
Step 6:
dh
4
dt
25
dh
125
}} 5 2}} < 20.276 ft/min
dt
144p
dh
Since }} is negative, the water level is dropping at the
dt
25 5 }}p(6)2}}
positive rate of <0.276 ft/min.
(b) Let V 5 volume of cube. Then V 5 x 3, which means
dV
}} 5 3x 2 and dV 5 3x 2 dx. We have )dx) # 0.01x,
dx
which means )3x 2 dx) # 3x 2(0.01x) 5 0.03V,
so )dV) # 0.03V. The volume calculation will be
accurate to within approximately 3% of the correct
volume.
Chapter 4 Review
203
67. Let C 5 circumference, r 5 radius, S 5 surface area, and V 5 volume.
dC
dr
(a) Since C 5 2pr, we have }} 5 2p and so dC 5 2p dr.
) dCC ) ) 22ppdrr ) ) drr )
0.4 cm
10 cm
Therefore, }} 5 }} 5 }} , }} 5 0.04 The calculated radius will be within approximately 4% of the correct
radius.
dS
dr
dS
8pr dr
dS 5 8pr dr. Therefore, }} 5 }}
S
4pr 2
2 dr
5 }} # 2(0.04) 5 0.08. The calculated surface area will be within approximately 8% of the correct surface area.
r
(b) Since S 5 4pr 2, we have }} 5 8pr and so
) ) )
) )
4
3
)
dV
dr
dV
3 dr
4pr 2 dr
2
dV 5 4pr dr. Therefore }} 5 } 5 }} # 3(0.04) 5 0.12.
4
V
r
}}pr 3
(c) Since V 5 }}pr 3, we have }} 5 4pr 2 and so
) )
)
)
3
) )
The calculated volume will be within approximately 12% of the correct volume.
a
6
a 1 20
h
68. By similar triangles, we have }} 5 }}, which gives ah 5 6a 1 120, or h 5 6 1 120a 21. The height of the lamp post is
dh
da
1
12
approximately 6 1 120(15)21 5 14 ft. The estimated error in measuring a was )da) # 1 in. 5 }} ft. Since }} 5 2120a 22, we
1 12 2
1
2
45
2
45
8
15
have )dh) 5 )2120a 22 da) # 120(15)22 }} 5 }} ft, so the estimated possible error is 6}} ft or 6}} in.
dy
dx
69. }} 5 2 sin x cos x 2 3. Since sin x and cos x are both between 1 and 21, the value of 2 sin x cos x is never greater than 2.
dy
dx
Therefore, }} # 2 2 3 5 21 for all values of x.
dy
dx
Since }} is always negative, the function decreases on every interval.
204
Section 5.1
Chapter 5
The Definite Integral
■ Section 5.1 Estimating with Finite Sums
(pp. 247–257)
Exploration 1
Which RAM is the Biggest?
y
y
y
5
5
5
4
4
4
3
3
3
2
2
2
1
1
1
1
2
x
3
1
2
x
3
1
2
x
3
1. LRAM . MRAM . RRAM
y
y
y
5
5
5
4
4
4
3
3
3
2
2
2
1
2
x
3
1
2
3
x
1
2
3
x
2. MRAM . RRAM . LRAM
3. RRAM . MRAM . LRAM, because the heights of the rectangles increase as you move toward the right under an increasing
function.
4. LRAM . MRAM . RRAM, because the heights of the rectangles decrease as you move toward the right under a decreasing
function.
Quick Review 5.1
1. 80 mph ? 5 hr 5 400 mi
2. 48 mph ? 3 hr 5 144 mi
3. 10 ft/sec2 ? 10 sec 5 100 ft/sec
3600 sec
1 mi
1h
5280 ft
3600 sec 24 hr
4. 300,000 km/sec ? }} ? }}
1 hr
1 day
12
100 ft/sec ? }} ? }} < 68.18 mph
< 9.46 3 10
km
365 days
} ? 1 yr
?}
1 yr
5. (6 mph)(3 h) 1 (5 mph)(2 h) 5 18 mi 1 10 mi 5 28 mi
60 min
1h
6. 20 gal/min ? 1 h ? }} 5 1200 gal
7. (218C/h)(12 h) 1 (1.58C)(6 h) 5 238C
3600 sec
1h
24 h
1 day
8. 300 ft3/sec ? }} ? }} ? 1 day 5 25,920,000 ft3
9. 350 people/mi2 ? 50 mi2 5 17,500 people
3600 sec
1h
10. 70 times/sec ? }} ? 1 h ? 0.7 5 176,400 times
Section 5.1
Section 5.1 Exercises
1. (a)
y
2
R
2
(b)
x
y
2
2
x
1
2
Dx 5 }}
1
1 2 1
1
1
3
3 2 1
5
1
5
1 2 2 3 1 2 2 1 2 2 41}2}2 1 [2(1) 2 (1)2]1}2}2 1 321}2}2 2 1}2}2 41}2}2 5 }4} 5 1.25
LRAM: [2(0) 2 (0)2] }} 1 2 }} 2 }}
2. (a)
y
2
2
x
1 2 1
1
1
3 2 1
3
3 1 2 2 1 2 2 41}2}2 1 [2(1) 2 (1)2]1}2}2 1 321}2}2 2 1}2}2 41}2}2 1 [2(2) 2 (2)2]1}2}2 5 }4} 5 1.25
RRAM: 2 }} 2 }}
(b)
y
2
2
x
1 2 1
1
3
3 2 1
5
5 2 1
7
7 2 1
11
3 1 4 2 1 4 2 41}2}2 1 321}4}2 2 1}4}2 41}2}2 1 321}4}2 2 1}4}2 41}2}2 1 321}4}2 2 1}4}2 41}2}2 5 }8} 5 1.375
MRAM: 2 }} 2 }}
3.
n
LRAMn
MRAMn
RRAMn
10
1.32
1.34
1.32
50
1.3328
1.3336
1.3328
100 1.3332
1.3334
1.3332
500 1.333328 1.333336 1.333328
4
3
4. The area is 1.3
w3w3w 5 }}.
205
206
5.
Section 5.1
LRAMn
MRAMn
RRAMn
10
12.645
13.4775
14.445
RRAM: 10 ? (44 1 15 1 35 1 … 1 35) 5 3840 ft
50
13.3218
13.4991
13.6818
Average 5 }} 5 3665 ft
100 13.41045
13.499775 13.59045
500 13.482018 13.499991 13.518018
Estimate the area to be 13.5.
6.
n
LRAMn MRAMn RRAMn
10
1.16823 1.09714
1.03490
50
1.11206 1.09855
1.08540
100 1.10531 1.09860
1.09198
500 1.09995 1.09861
1.09728
1000 1.09928 1.09861
1.09795
13. (a) LRAM: 0.001(0 1 40 1 62 1 … 1 137) 5 0.898 mi
RRAM: 0.001(40 1 62 1 82 1 … 1 142) 5 1.04 mi
Average 5 0.969 mi
(b) The halfway point is 0.4845 mi. The average of LRAM
and RRAM is 0.4460 at 0.006 h and 0.5665 at 0.007 h.
Estimate that it took 0.006 h 5 21.6 sec. The car was
going 116 mph.
14. Use f (x) 5 Ï2w5ww
2wx 2w and approximate the volume using
2 2
pr 2h 5 p(Ï2w5ww
2wnw
) Dx, so for the MRAM program, use
i
2
p(25 2 x ) on the interval [25, 5].
n
MRAM
526.21677
LRAMn MRAMn RRAMn
20
524.25327
10
0.98001 0.88220
0.78367
40
523.76240
50
0.90171 0.88209
0.86244
80
523.63968
100 0.89190 0.88208
0.87226
160 523.60900
500 0.88404 0.88208
0.88012
1000 0.88306 0.88208
0.88110
n
Estimate the area to be 0.8821.
8.
3490 ft 1 3840 ft
2
10
Estimate the area to be 1.0986.
7.
12. LRAM: 10 ? (0 1 44 1 15 1 … 1 30 ) 5 3490 ft
n
4
3
500p
3
15. V 5 }}p(5)3 5 }} < 523.59878
n
error
% error
10 2.61799
0.5
n
LRAMn MRAMn RRAMn
20 0.65450
0.125
10
1.98352 2.00825
1.98352
40 0.16362 0.0312
50
1.99934 2.00033
1.99934
80 0.04091 0.0078
100 1.99984 2.00008
1.99984
500 1.99999 2.00000
1.99999
Estimate the area to be 2.
9. LRAM:
Area
< f (2) ? 2 1 f (4) ? 2 1 f (6) ? 2 1 … 1 f (22) ? 2
5 2 ? (0 1 0.6 1 1.4 1 … 1 0.5)
5 44.8 (mg/L) ? sec
RRAM:
Area
< f (4) ? 2 1 f (6) ? 2 1 f (8) ? 2 1 … 1 f (24) ? 2
5 2(0.6 1 1.4 1 2.7 1 … 1 0)
5 44.8 (mg/L) ? sec
Patient’s cardiac output:
5 mg
}}
44.8 (mg/L) ? sec
60 sec
} < 6.7 L/min
?}
1 min
Note that estimates for the area may vary.
10. (a) LRAM: 1 ? (0 1 12 1 22 1 10 1 5 1 13 1 11 1 6
1 2 1 6) 5 87 in. 5 7.25 ft
(b) RRAM: 1 ? (12 1 22 1 10 1 5 1 13 1 11 1 6 1 2
1 6 1 0) 5 87 in. 5 7.25 ft
11. 5 min 5 300 sec
(a) LRAM: 300 ? (1 1 1.2 1 1.7 1 … 1 1.2) 5 5220 m
(b) RRAM: 300 ? (1.2 1 1.7 1 2.0 1 … 1 0) 5 4920 m
160 0.01023 0.0020
16. (a) Use LRAM with p(16 2 x 2).
S8 < 146.08406
S8 is an overestimate because each rectangle is above
the curve.
)V 2 S )
8
(b) }}
< 0.09 5 9%
V
17. (a) Use RRAM with p(16 2 x 2).
S8 < 120.95132
S8 is an underestimate because each rectangle is below
the curve.
)V 2 S )
8
(b) }}
< 0.10 5 10%
V
18. (a) Use LRAM with p(64 2 x 2) on the
interval [4, 8], n 5 8.
S < 372.27873 m3
)V 2 S8)
V
(b) }} < 0.11 5 11%
19. (a) (5)(6.0 1 8.2 1 9.1 1 … 1 12.7)(30) < 15,465 ft3
(b) (5)(8.2 1 9.1 1 9.9 1 … 1 13.0)(30) < 16,515 ft3
20. Use LRAM with px on the interval [0, 5], n 5 5.
1(0 1 p 1 2p 1 3p 1 4p) 5 10p < 31.41593
Section 5.1
21. Use MRAM with px on the interval [0, 5], n 5 5.
1
3
5
7
9
25
1 }}p 1 }}p 1 }}p 1 }}p 1 }}p 5 }}p < 39.26991
2
2
2
2
2
2
1
2
22. (a) LRAM5:
32.00 1 19.41 1 11.77 1 7.14 1 4.33 5 74.65 ft/sec
(b) RRAM5:
19.41 1 11.77 1 7.14 1 4.33 1 2.63 5 45.28 ft/sec
(c) The upper estimates for speed are 32.00 ft/sec for the
first sec, 32.00 1 19.41 5 51.41 ft/sec for the second
sec, and 32.00 1 19.41 1 11.77 5 63.18 ft/sec for the
third sec. Therefore, an upper estimate for the distance
fallen is 32.00 1 51.41 1 63.18 5 146.59 ft.
23. (a) 400 ft/sec 2 (5 sec)(32 ft/sec2) 5 240 ft/sec
(b) Use RRAM with 400 2 32x on [0, 5], n 5 5.
368 1 336 1 304 1 272 1 240 5 1520 ft
24. (a) Upper 5 70 1 97 1 136 1 190 1 265 5 758 gal
Lower 5 50 1 70 1 97 1 136 1 190 5 543 gal
(b) Upper 5 70 1 97 1 136 1 190 1 265 1 369 1 516
1 720 5 2363 gal
Lower 5 50 1 70 1 97 1 136 1 190 1 265 1 369
1 516 5 1693 gal
(c) 25,000 2 2363 5 22,637 gal
22,637
}} < 31.44 h (worst case)
720
25,000 2 1693 5 23,307 gal
23,307
}} < 32.37 h (best case)
720
25. (a) Since the release rate of pollutants is increasing, an
upper estimate is given by using the data for the end of
each month (right rectangles), assuming that new
scrubbers were installed before the beginning of
January. Upper estimate:
30(0.20 1 0.25 1 0.27 1 0.34 1 0.45 1 0.52)
< 60.9 tons of pollutants
A lower estimate is given by using the data for the end
of the previous month (left rectangles). We have no
data for the beginning of January, but we know that
pollutants were released at the new-scrubber rate of
0.05 ton/day, so we may use this value.
Lower estimate:
30(0.05 1 0.20 1 0.25 1 0.27 1 0.34 1 0.45)
< 46.8 tons of pollutants
(b) Using left rectangles, the amount of pollutants released
by the end of October is
30(0.05 1 0.20 1 0.25 1 0.27 1 0.34 1 0.45
1 0.52 1 0.63 1 0.70 1 0.81) < 126.6 tons.
Therefore, a total of 125 tons will have been released
into the atmosphere by the end of October.
26. The area of the region is the total number of units sold, in
millions, over the 10-year period. The area units are
(millions of units per year)(years) 5 (millions of units).
27. (a) The diagonal of the square has length 2, so the side
length is Ï2w. Area 5 (Ï2w)2 5 2
207
(b) Think of the octagon as a collection of 16 right
triangles with a hypotenuse of length 1 and an acute
2p
p
16
8
p
p
sin }} cos }}
8
8
p
}}
4
angle measuring }} 5 }}.
1
1 2 21
Area 5 16 }}
5 4 sin
21
2
5 2Ï2w < 2.828
(c) Think of the 16-gon as a collection of 32 right triangles
with a hypotenuse of length 1 and an acute angle
2p
p
32
16
1
p
p
Area 5 32 }} sin }} cos }}
2
16
16
p
5 8 sin }} < 3.061
8
measuring }} 5 }}.
1 21
21
2
(d) Each area is less than the area of the circle, p. As n
increases, the area approaches p.
28. The statement is false. We disprove it by presenting a
counterexample, the function f (x) 5 x 2 over the interval
0 # x # 1, with n 5 1. MRAM1 5 1f (0.5) 5 0.25
LRAM1 1 RRAM1
1f (0) 1 1f (1)
5 }}
}}}
2
2
011
5 }} 5 0.5 Þ MRAM1
2
29. RRAMn f 5 (Dx)[ f (x1) 1 f (x2) 1 … 1 f (xn21) 1 f (xn)]
5 (Dx)[ f (x0) 1 f (x1) 1 f (x2) 1 … 1 f (xn21)]
1 (Dx)[ f (xn) 2 f (x0)]
5 LRAMn f 1 (Dx)[ f (xn) 2 f (x0)]
But f (a) 5 f (b) by symmetry, so f (xn) 2 f (x0) 5 0.
Therefore, RRAMn f 5 LRAMn f.
30. (a) Each of the isosceles triangles is made up of two right
triangles having hypotenuse 1 and an acute angle
2p
2n
1
is AT 5 2 }} sin
2
p
n
p
p
1
2p
}} cos }} 5 }} sin }}.
n
n
2
n
measuring }} 5 }}. The area of each isosceles triangle
1 21
21
2
(b) The area of the polygon is
2p
n
n
2p
lim AP 5 lim }} sin }} 5 p
n
n→`
n→` 2
n
2
AP 5 nAT 5 }} sin }}, so
(c) Multiply each area by r 2:
1
2p
2
n
n 2
2p
AP 5 }}r sin }}
2
n
AT 5 }}r 2 sin }}
lim AP 5 pr 2
n→`
208
Section 5.2
■ Section 5.2 Definite Integrals
(pp. 258–268)
Exploration 1
7. 0. (The equal areas above and below the x-axis sum to
zero.)
Finding Integrals by Signed Areas
1. 22. (This is the same area as
E sin x dx, but below the
p
0
x-axis.)
[22p, 2p] by [23, 3]
8. 4. (Each rectangle in a typical Riemann sum is twice as
E sin x dx.)
p
wide as in
0
[22p, 2p] by [23, 3]
2. 0. (The equal areas above and below the x-axis sum to
zero.)
[22p, 2p] by [23, 3]
9. 0. (The equal areas above and below the x-axis sum to
zero.)
[22p, 2p] by [23, 3]
E sin x dx.)
p
3. 1. (This is half the area of
0
[22p, 2p] by [23, 3]
10. 0. (The equal areas above and below the x-axis sum to zero,
since sin x is an odd function.)
[22p, 2p] by [23, 3]
4. 2p 1 2. (The same area as
of area p 3 2.)
E sin x dx sits above a rectangle
p
0
[22p, 2p] by [23, 3]
Exploration 2
More Discontinuous Integrands
1. The function has a removable discontinuity at x 5 2.
[22p, 2p] by [23, 3]
5. 4. (Each rectangle in a typical Riemann sum is twice as tall
E sin x dx.)
p
as in
[24.7, 4.7] by [21.1, 5.1]
0
2. The thin strip above x 5 2 has zero area, so the area under
E (x 1 2) dx, which is 10.5.
3
the curve is the same as
0
[22p, 2p] by [23, 3]
6. 2. (This is the same region as in
2 units to the right.)
E sin x dx, translated
p
0
[24.7, 4.7] by [21.1, 5.1]
[22p, 2p] by [23, 3]
Section 5.2
3. The graph has jump discontinuities at all integer values, but
2
2wcw
Dxk 5 E Ï4ww
2wx 2w dx where P is any par∑ Ï4ww
k
0
))P))→0
n
1
5. lim
k51
the Riemann sums tend to the area of the shaded region
tition of [0, 1].
shown. The area is the sum of the areas of 5 rectangles (one
∑ (sin3 ck)Dxk 5 E2p sin3 x dx where P is any
))P))→0
p
n
of them with height 0):
E int(x) dx 5 0 1 1 1 2 1 3 1 4 5 10.
5
6. lim
k51
0
partition of [2p, p].
7.
E
8.
E (220) dx 5 (220)(7 2 3) 5 280
1
22
5 dx 5 5[1 2 (22)] 5 15
7
[22.7, 6.7] by [21.1, 5.1]
3
Quick Review 5.2
1.
∑ n 2 5 (1)2 1 (2)2 1 (3)2 1 (4)2 1 (5)2 5 55
9.
0
10.
E
11.
E
12.
E
n51
21
4
2.
E (2160) dt 5 (2160)(3 2 0) 5 2480
3
5
∑ (3k 2 2) 5 [3(0) 2 2] 1 [3(1) 2 2] 1 [3(2) 2 2]
24
p
p
3p
}} du 5 }}[21 2 (24)] 5 }}
2
2
2
k50
1 [3(3) 2 2] 1 [3(4) 2 2] 5 20
3.4
4
3.
∑ 100( j 1 1)2 5 100[(1)2 1 (2)2 1 (3)2 1 (4)2 1 (5)2]
j50
5 5500
22.1
0.5 ds 5 0.5[3.4 2 (22.1)] 5 2.75
Ï1
w8
w
Ï2
w
Ï2w dr 5 Ï2w(Ï1w8w 2 Ï2w) 5 4
99
4.
∑k
x
2
13. Graph the region under y 5 }} 1 3 for 22 # x # 4.
k51
25
5.
∑ 2k
y
5
k50
500
6.
∑ 3k 2
k51
50
50
50
x51
x51
x51
7. 2∑ x 2 1 3∑ x 5 ∑ (2x 2 1 3x)
8.
8
20
20
k50
k59
k50
5
x
∑ xk 1 ∑ xk 5 ∑ xk
n
9.
∑ (21)k 5 0 if n is odd.
E 1}2x} 1 32 dx 5 }12}(6)(2 1 5) 5 21
4
k50
22
n
10.
∑ (21)k 5 1 if n is even.
1
2
Section 5.2 Exercises
∑ ck Dxk 5 E0 x
n
1. lim
2
2
))P))→0 k51
2
y
dx where P is any partition of [0, 2].
∑ (ck2 2 3ck)Dxk 5 E27(x 2 2 3x) dx where P is any
))P))→0
n
5
2. lim
k51
3. lim
∑
))P))→0 k51
1
}}Dxk 5
ck
of [2, 3].
3
1
E
1
}} dx where P is any partition of [1, 4].
1 x
5
k
x
x=1 x=3
2
2
3
4. lim
k51
4
4
1
1
}Dxk 5 E }} dx where P is any partition
∑}
12c
2 12x
))P))→0
n
5
2
partition of [27, 5].
n
3
2
14. Graph the region under y 5 22x 1 4 for }} # x # }}.
k50
209
E
3/2
1/2
1
2
(22x 1 4) dx 5 }}(1)(3 1 1) 5 2
210
Section 5.2
15. Graph the region under y 5 Ï9ww
2wx 2w for 23 # x # 3.
18. Graph the region under y 5 1 2 )x) for 21 # x # 1.
y
y
2
5
5
x
2
This region is half of a circle of radius 3.
E
3
23
1
21
1
9p
Ï9ww
2wx 2w dx 5 }}p(3)2 5 }}
2
E
2
x
(1 2 )x)) dx 5 }1}(2)(1) 5 1
2
19. Graph the region under y 5 2 2 )x) for 21 # x # 1.
16. Graph the region under y 5 Ï1w6ww
2wx w for 24 # x # 0.
2
y
2
y
5
2
5
x
E
1
The region is one quarter of a circle of radius 4.
E
0
24
x
1
Ï1w6ww
2wx 2w dx 5 }}p(4)2 5 4p
4
21
(2 2 )x)) dx 5 }1}(1)(1 1 2) 1 }1}(1)(1 1 2) 5 3
2
2
20. Graph the region under y 5 1 1 Ï1ww
2wx 2w for 21 # x # 1.
y
17. Graph the region under y 5 )x) for 22 # x # 1.
2
y
2
2
2
x
E
1
21
E
1
22
1
2
1
2
x
5
2
)x) dx 5 }}(2)(2) 1 }}(1)(1) 5 }}
p
2
1
2
(1 1 Ï1ww
2wx 2w) dx 5 (2)(1) 1 }}p(1)2 5 2 1 }}
21. Graph the region under y 5 u for p # u # 2p
y
2p
p
p
E
2p
p
1
2
2p
u
3p2
2
u du 5 }}(2p 2 p)(2p 1 p) 5 }}
Section 5.2
22. Graph the region under y 5 r for Ï2w # r # 5Ï2w.
y
10
211
33. Observe from the graph below that the region under the
graph of f (x) 5 1 2 x 3 for 0 # x # 1 cuts out a region R
from the square identical to the region under the graph of
g(x) 5 x 3 for 0 # x # 1.
y
1
y = f(x)
r
√2
E
5√2
5Ï2
w
Ï2
w
10
1
2
r dr 5 }}(5Ï2w 2 Ï2w)(Ï2w 1 5Ï2w) 5 24
1
E
1
1
23. x dx 5 }}(b)(b) 5 }}b 2
2
2
0
2
0
E 2s ds 5 }12}(b 2 a)(2b 1 2a) 5 b
b
a
2
2 a2
E 3t dt 5 }12}(b 2 a)(3b 1 3a) 5 }32}(b
b
26.
2
a
E
2a
27.
a
E
1
1
2
1
2
x 3 dx 5 2(area below x-axis) 1 (area above x-axis) 5 0
3
E (x
0
3
1
4
13
4
1 3) dx 5 }} 1 3 5 }}
31. Observe that the region under the graph of f (x) 5 (x 2 2)3
for 2 # x # 3 is just the region under the graph of
g(x) 5 x 3 for 0 # x # 1 translated two units to the right.
E (x 2 2) dx 5 E x
3
1
3
2
0
3
1
4
dx 5 }}
32. Observe that the graph of f (x) 5 )x)3 is symmetric with
respect to the y-axis and the right half is the graph of
g(x) 5 x 3.
E
1
21
2
3a 2
2
1
2
30. The graph of f (x) 5 x 1 3 is three units higher than the
graph of g(x) 5 x 3. The extra area is (3)(1) 5 3.
1
3
4
y
x dx 5 }}(Ï3wa 2 a)(Ï3wa 1 a) 5 }}(3a 2 2 a 2) 5 a 2
a
21
1
4
dx 5 1 2 }} 5 }}
34. Observe from the graph of f (x) 5 ()x) 2 1)3 for
21 # x # 2 that there are two regions below the x-axis and
one region above the axis, each of whose area is equal to
the area of the region under the graph of g(x) 5 x 3 for
0 # x # 1.
2 a 2)
29. Observe that the graph of f (x) 5 x 3 is symmetric with
respect to the origin. Hence the area above and below the
x-axis is equal for 21 # x # 1.
E
3
0
x
x dx 5 }}(2a 2 a)(2a 1 a) 5 }}
Ï3
wa
28.
1
3
0
E 4x dx 5 }12}(b)(4b) 5 2b
b
25.
1
E (1 2 x ) dx 5 1 2 E x
b
24.
R
E
1
1
2
)x)3 dx 5 2 x 3 dx 5 }}
0
y = f(x)
E
2
21
2
x
()x) 2 1)3 dx 5 212}1}2 1 1}1}2 5 2}1}
4
4
4
x 3
122
35. Observe that the graph of f (x) 5 }}
for 0 # x # 2 is just
a horizontal stretch of the graph of g(x) 5 x 3 for 0 # x # 1
x 3
122
by a factor of 2. Thus the area under f (x) 5 }}
for
0 # x # 2 is twice the area under the graph of g(x) 5 x 3
for 0 # x # 1.
E 1}2x}2
2
0
3
E
1
1
2
dx 5 2 x 3 dx 5 }}
0
36. Observe that the graph of f (x) 5 x 3 is symmetric with
respect to the origin. Hence the area above and below the
x-axis is equal for 28 # x # 8.
E
8
28
x 3 dx 5 2(area below x-axis) 1 (area above x-axis) 5 0
212
Section 5.2
37. Observe from the graph below that the region between the
graph of f (x) 5 x 3 2 1 and the x-axis for 0 # x # 1 cuts
out a region R from the square identical to the region under
the graph of g(x) 5 x 3 for 0 # x # 1.
44. (a) The function has discontinuities at
x 5 25, 24, 23, 22, 21, 0, 1, 2, 3, 4, 5.
(b)
y
x
1
[26, 5] by [218, 4]
E
5
26
y = f(x)
1 (212) 1 (210) 1 (28) 1 (26) 1 (24) 1 (22)
R
1 0 1 2 5 288
–1
E (x
1
2 int(x 2 3) dx 5 (218) 1 (216) 1 (214)
1
4
3
4
2 1) dx 5 21 1 }} 5 2}}
3
0
45. (a) The function has a discontinuity at x 5 21.
(b)
38. Observe from the graph below that the region between the
3
graph of f (x) 5 Ïxw and the x-axis for 0 # x # 1 cuts out a
[23, 4] by [24, 3]
region R from the square identical to the region under the
E
4
graph of g(x) 5 x 3 for 0 # x # 1.
23
x2 2 1
1
1
7
}} dx 5 2}}(4)(4) 1 }}(3)(3) 5 2}}
x11
2
2
2
46. (a) The function has a discontinuity at x 5 3.
y
(b)
1
R
y = f(x)
[25, 6] by [29, 2]
E
6
9 2 x2
1
1
77
}} dx 5 }}(2)(2) 2 }}(9)(9) 5 2}}
2
2
2
25 x 2 3
x
1
47. (a) As x approaches 0 from the right, f (x) goes to `.
E
1
Ïxw dx 5 1 2 }1} 5 }3}
4
4
0
x
39. NINT }
,
x,
0,
5
< 0.9905
}
x2 1 4
p
40. 3 1 2 ? NINT tan x, x, 0, }} < 4.3863
3
1
2
1
(b) Using right endpoints we have
E }x1} dx 5 lim ∑
n
1
2
0
2
n→` k51
n
5 lim
41. NINT(4 2 x 2, x, 22, 2) < 10.6667
11 2 2
1
}2
k
}}
n
1}n}2
1
∑ }n}
2
n→` k51 k
42. NINT(x 2e2x, x, 21, 3) < 1.8719
5 lim n 1 1 }}2 1 … 1 }}2 .
43. (a) The function has a discontinuity at x 5 0.
1
2
1
n→`
1
n
2
1
1
Note that n 1 1 }}2 1 … 1 }}2 . n and n → `, so
2
n
1
1
n 1 1 }}2 1 … 1 }}2 → `.
2
n
1
(b)
2
1
[22, 3] by [22, 2]
2
1
n
k
n
48. (a) Dx 5 }}, xk 5 }}
E
1 2
3
1n2
RRAM 5 }}
x
}} dx 5 22 1 3 5 1
22 )x)
n
2 2
n 2
? }n} 1 1}n}2 ? }n} 1 … 1 1}n}2 ? }n}
1
1
1
2
5∑
1
k
11}n}2 ? }n}2
k51
n
(b)
n
2
n
∑ 11}k}2 ? }1n}2 5 ∑ 1}nk}3 2 5 }n1}3 ∑ k 2
k51 n
k51
k51
n
2
n(n 1 1)(2n 1 1)
6
n(n 1 1)(2n 1 1)
6n
(c) }}3 ∑ k 2 5 }}3 ? }} 5 }}
3
1
n
k51
1
n
Section 5.3
`
2
n(n 1 1)(2n 1 1)
lim }}
∑ 11}k}2 ? }1n}2 5 n→`
6n3
n→` k51 n
(d) lim
2n 3 1 3n 2 1 n
6n
n→`
2
1
5 }} 5 }}
6
3
5 lim }}
3
Ex
1
(e) Since
Exploration 2
Integral
213
Finding the Derivative of an
Pictures will vary according to the value of x chosen.
(Indeed, this is the point of the exploration.) We show a
typical solution here.
y
2
dx equals the limit of any Riemann sum
0
over the interval [0, 1] as n approaches `, part (d)
Ex
1
proves that
2
0
1
3
dx 5 }}.
x
0 a
b
x
■ Section 5.3 Definite Integrals and
Antiderivatives (pp. 268–276)
Exploration 1 How Long is the Average Chord
of a Circle?
1. The chord is twice as long as the leg of the right triangle in
the first quadrant, which has length Ïw
r2w
2wx2w by the
Pythagorean Theorem.
1. We have chosen an arbitrary x between a and b.
2. We have shaded the region using vertical line segments.
E f (t) dt using the
x
3. The shaded region can be written as
a
definition of the definite integral in Section 5.2. We use t as
y
a dummy variable because x cannot vary between a and
r2 − x2
r
itself.
4. The area of the shaded region is our value of F(x).
x
x
y
1
r 2 (2r)
2. Average value 5 }}
2
2r
3. Average value 5 }}
E
r
E
r
2r
2Ïw
r2w
2wx2w dx.
Ïw
r2w
2wx2w dx
1
r
pr2
2
5 }} ? }}
b
x
∆F
2r
5 }} ? (area of semicircle of radius r)
1
r
x
0 a
5. We have drawn one more vertical shading segment to
represent DF.
6. We have moved x a distance of Dx so that it rests above the
new shading segment.
pr
2
5 }}
y
4. Although we only computed the average length of chords
∆x
perpendicular to a particular diameter, the same
computation applies to any diameter. The average length of
pr
2
a chord of a circle of radius r is }}.
5. The function y 5 2Ïw
rw
2wxw is continuous on [2r, r], so
2
x
0 a
b
x
∆F
2
the Mean Value Theorem applies and there is a c in [a, b]
pr
2
so that y(c) is the average value }}.
7. Now the (signed) height of the newly-added vertical
segment is f (x).
8. The (signed) area of the segment is DF 5 Dx ? f (x),
DF
so F9(x) 5 lim }} 5 f (x)
Dx→0 Dx
214
Section 5.3
Quick Review 5.3
E [2 f (x) 2 3h(x)] dx 5 E 2f (x) dx 2 E 3h(x) dx
5 2E f (x) dx 2 3E h(x) dx
9
(c)
9
7
dy
dx
1. }} 5 sin x
9
7
7
9
7
E f (x) dx 5 2E f (x) dx 5 1
1
dy
dx
sec x tan x
sec x
(d)
dy
dx
c os x
sin x
(e)
dy
dx
sec x tan x 1 sec2 x
sec x 1 tan x
3. }} 5 }} 5 tan x
9
9
1
E f (x) dx 5 E f (x) dx 1 E f (x) dx
5 E f (x) dx 2 E f (x) dx
7
4. }} 5 }} 5 cot x
1
5. }} 5 }}} 5 sec x
1
1x2
7
1
9
9
9
1
7
E [h(x) 2 f (x)] dx 5 E h(x) dx 2 E f (x) dx
5 2E h(x) dx 1 E f (x) dx
7
(f)
(n 1 1)x n
n11
7
9
7. }} 5 }} 5 x n
dy
1
8. }} 5 2}
}
dx
(2x 1 1)2
9
5 21 2 5 5 26
6. }} 5 x }} 1 ln x 2 1 5 ln x
dy
dx
7
5 2(5) 2 3(4) 5 22
dy
2. }} 5 cos x
dx
dy
dx
9
7
9
9
9
7
2x ln 2
(ln 2)2 5 2}
}
(2x 1 1)2
?
9
7
5 24 1 5 5 1
x
E f (u) du 5 5
2
dy
dx
3. (a)
9. }} 5 xe x 1 e x
1
E Ï3wf (z) dz 5 Ï3wE f (z) dz 5 5Ï3w
2
dy
dx
1
x 11
(b)
10. }} 5 }
2 }
2
1
1
E f (t) dt 5 2E f (t) dt 5 25
1
(c)
Section 5.3 Exercises
2
E g(x) dx 5 0
2
1. (a)
(d)
5
5
E 3 f (x) dx 5 3E
2
1
1
(d)
f (x) dx 5 3(24) 5 212
(b)
E
g(u) du 5 Ï2w
(c)
E
[2g(x)] dx 5 2
(d)
E
0
5
1
2
1
E [ f (x) 2 g(x)] dx 5 E f (x) dx 2 E g(x) dx
5
1
5
1
23
(f)
E
E f (z) dz 5 E
4
5. (a)
3
1
E [4f (x) 2 g(x)] dx 5 E 4f (x) dx 2 E g(x) dx
5 4E f (x) dx 2 E g(x) dx
1
3
1
5
1
1
(b)
7
4
7
551459
9
0
23
g(r) dr 5 1
E
4
f (z) dz 1
E
3
f (z) dz
E
0
4
f (z) dz 1
0
f (z) dz
0
3
0
4
0
1
9
g(x) dx 5 2Ï2w
23
3
0
5 27 1 3 5 24
9
E [ f (x) 1 h(x)] dx 5 E f (x) dx 1 E h(x) dx
9
0
0
4
1
E 22f (x) dx 5 22E f (x) dx 5 22(21) 5 2
9
E
E f (t) dt 5 E f (t) dt 1 E f (t) dt
5 2E f (t) dt 1 E f (t) dt
3
(b)
5 4(6) 2 8 5 16
2. (a)
g(t) dt 5 2Ï2w
5 23 1 7 5 4
5
5
0
52
5
1
23
g(r)
1
}} dr 5 }}
23 Ï2
w
Ïw2
5 6 2 8 5 22
5
E
0
0
1
5
23
0
5
5 4 1 6 5 10
(e)
g(t) dt 5 2
0
1
2
1
E
4. (a)
E f (x) dx 5 E f (x) dx 1 E f (x) dx
5 2E f (x) dx 1 E f (x) dx
2
2
23
1
2
5
E [2f (x)] dx 5 2E f (x) dx 5 25
1
E g(x) dx 5 2E g(x) dx 5 28
1
(c)
1
2
2
(b)
2
E h(r) dr 5 E
3
6. (a)
1
21
1
52
7
E
h(r) dr 1
E
1
21
1
(b) 2 h(u) du5 2
3
5
E
3
21
3
h(r) dr
21
3
h(r) dr 1
E
3
E
E
h(u) du 2
h(u) du 2
21
h(r) dr 5 6
21
E
E
1
1
h(u) du
21
21
h(u) du 5 6
Section 5.3
7. An antiderivative of 7 is F(x) 5 7x.
E
1
3
17. Divide the shaded area as follows.
y
7 dx 5 F(1) 2 F(3) 5 7 2 21 5 214
3
5
8. An antiderivative of 5x is F(x) 5 }}x 2
2
2
R2
E 5x dx 5 F(2) 2 F(0) 5 10 2 0 5 10
R1
y = x2 – 1
0
x2
1
6
5
25
x
9
}} dx 5 F(5) 2 F(3) 5 }} 2 }} 5 1
16
16
3 8
x
8
9. An antiderivative of }} is F(x) 5 }}.
E
E (2t 2 3) dt 5 F(2) 2 F(0) 5 22 2 0 5 22
2
0
1
11. An antiderivative of t 2 Ïw2 is F(t) 5 }}t 2 2 tÏ2w.
2
Ï2
w
E
1
3
Note that an antiderivative of x 2 2 1 is F(x) 5 }}x3 2 x.
Area of R1 5 3(1) 5 3
Area of R2 5 (3)(1) 2
z
2
z2
4
12. An antiderivative of 1 1 }} is F(z) 5 z 1 }}.
E 11 1 }2z}2 dz 5 F(1) 2 F(2) 5 }54} 2 3 5 2}74}
1
E (x
2
2
2
E
Area of R3 5 2 (x 2 2 1) dx
0
5 2[F(1) 2 F(0)]
2
31 3 2
1 2
1
14. An antiderivative of }} is F(x) 5 sin21 x.
2wx 2w
Ï1ww
1/2
dx
1
1
p
p
p
}} 5 F }} 2 F 2}} 5 }} 2 2}} 5 }}
2
2
2
6
6
3
21/2 Ï1
2wx w
ww
E
12
1 2
Ee
2
0
x
5
3
y
3
y = 3 – 3x 2
R1
2
0
5 3 ln 4 2 0
5 3 ln 4 < 4.159
x
R2
3
x11
16. An antiderivative of }} is F(x) 5 3 ln )x 1 1).
3
16
3
18. Divide the shaded area as follows.
dx 5 F(2) 2 F(0) 5 e2 2 1 < 6.389
3 dx
E}
} 5 F(3) 2 F(0)
x11
2
3
Total shaded area 5 3 1 }} 1 }} 5 }}
1 2
15. An antiderivative of e x is F(x) 5 e x.
2
3
4
5 2 2}} 2 0 5 }}
1
11x
p
p
p
1
}}2 dx 5 F(1) 2 F(21) 5 }} 2 2}} 5 }}
4
4
2
1x
5
3
31 3 2 1 3 24
1
13. An antiderivative of }}2 is F(x) 5 tan21 x.
1
2 1) dx
5 3 2 }} 2 2}} 5 }}
2
21 1
2
1
5 3 2 [F(2) 2 F(1)]
(t 2 Ï2w) dt 5 F(Ï2w) 2 F(0) 5 21 2 0 5 21
0
x
2
R3
10. An antiderivative of 2t 2 3 is F(t) 5 t 2 2 3t.
E
215
R3
–9
Note that an antiderivative of 3 2 3x 2 is F(x) 5 3x 2 x 3.
Area of R1 5
E (3 2 3x ) dx 5 F(1) 2 F(0) 5 2
1
2
0
Area of R2 5 (9)(1) 5 9
Area of R3 5 (9)(1) 1
E (3 2 3x ) dx
2
2
1
5 9 1 [F(2) 2 F(1)]
5 9 1 (22 2 2) 5 5
Total shaded area 5 2 1 9 1 5 5 16
216
Section 5.3
19. Divide the shaded area as follows.
(b) Area 5
y
2.25
E (x
2
2
0
2 6x 1 8) dx 2
E (x
3
2
2
2 6x 1 8) dx
5 [F(2) 2 F(0)] 2 [F(3) 2 F(2)]
y = 3x – x 2
20
13
20
3
2 1
22
3
2
5 }} 2 0 2 6 2 }} 5 }}
R1
x
R2 4
22.
–4
3
1
2
3
3
9
9
2
Area of R1 5 (3x 2 x ) dx 5 F(3) 2 F(0) 5 }} 2 0 5 }}
2
2
0
4
[0, 2] by [25, 3]
Note that an antiderivative of 3x 2 x 2 is F(x) 5 }}x 2 2 }}x 3.
E
An antiderivative of 2x 2 1 5x 2 4 is
E
1
3
3
5 2[F(4) 2 F(3)]
E (2x
2
(a)
8
9
11
5 2 }} 2 }} 5 }}
3
2
6
9
11
19
Total shaded area 5 }} 1 }} 5 }}
2
6
3
1
5
2
F(x) 5 2}}x 3 1 }}x 2 2 4x.
Area of R2 5 2 (3x 2 x 2) dx
2
2
0
2
3
2
3
1 5x 2 4) dx 5 F(2) 2 F(0) 5 2}} 2 0 5 2}}
E
1
(b) Area 5 2 (2x 2 1 5x 2 4) dx 1
0
E (2x
2
2
1
1 5x 2 4) dx
5 2[F(1) 2 F(0)] 1 [F(2) 2 F(1)]
20. Divide the shaded area as follows.
1
11
6
2
3
2 3
1
11
6
24
5 2 2}} 2 0 1 2}} 2 2}} 5 3
y
23.
3
y=
x2
– 2x
R2
3
R1
[0, 3] by [23, 2]
x
1
3
An antiderivative of 2x 2 x 2 is F(x) 5 x 2 2 }}x 3.
1
3
E
(a)
2
(b) Area 5
0
5 2[F(2) 2 F(0)]
4
3
2
2
0
Area of R1 5 2 (x 2 2 2x) dx
1
3
E (2x 2 x ) dx 5 F(3) 2 F(0) 5 0 2 0 5 0
3
Note that an antiderivative of x 2 2 2x is F(x) 5 }}x3 2 x 2.
Area of R2 5
E (x
2
2
3
2
0
2
2
5 [F(2) 2 F(0)] 2 [F(3) 2 F(2)]
4
3
5 2 2}} 2 0 5 }}
2
E (2x 2 x ) dx 2 E (2x 2 x ) dx
4
13
2 1
4
3
2
8
3
5 }} 2 0 2 0 2 }} 5 }}
2 2x) dx
5 F(3) 2 F(2)
24.
4
4
5 0 2 2}} 5 }}
3
3
4
4
8
Total shaded area 5 }} 1 }} 5 }}
3
3
3
1 2
[0, 5] by [25, 5]
21.
1
3
An antiderivative of x 2 2 4x is F(x) 5 }}x3 2 2x 2.
E (x
5
(a)
0
[0, 3] by [21, 8]
1
3
An antiderivative of x 2 2 6x 1 8 is F(x) 5 }}x 3 2 3x 2 1 8x.
E (x
3
(a)
0
2
2 6x 1 8) dx 5 F(3) 2 F(0) 5 6 2 0 5 6
2
25
3
25
3
2 4x) dx 5 F(5) 2 F(0) 5 2}} 2 0 5 2}}
Section 5.3
E
4
(b) Area 5 2 (x 2 2 4x) dx 1
0
E (x
5
2
4
30. The region between the graph and the x-axis is a rectangle
2 4x) dx
with a half circle of radius 1 cut out. The area of the region
5 2[F(4) 2 F(0)] 1 [F(5) 2 F(4)]
1
32
3
2 3
25
3
32
3
1
24
1
2
E
1
2p
1
2
42p
4
E
2p
0
1
2p
f (t) dt 5 }} ? 0 5 0
32. Since tan u is an odd function, there are equal areas above
and below the x-axis.
1
p/2
av( f ) 5 }}
E
p/4
2
p
f (u) du 5 }} ? 0 5 0
2p/4
1
2
1
1
1
}} # }}4 dx # 1
2
0 11x
33. min f 5 }} and max f 5 1
3
x
x
2
6
3
1
x2
1
1 9
3
av 5 }} 2}} dx 5 }}[F(3) 2 F(0)] 5 }} 2}} 5 2}}
3 0
2
3
3 2
2
c2
3
Find x 5 c in [0, 3] such that 2}} 5 2}}.
2
2
26. An antiderivative of 2}} is F(x) 5 2}}.
1 2
c2 5 3
E
16
17
34. f (0.5) 5 }}
1}2}21}1}7 2 # E0
0.5
1 16
1
1
}}4 dx # }} (1)
2
11x
0.5
1
8
1
}} #
}}4 dx # }}
2
17
0 11x
1
1 1
1 16
1
}} }} #
}}4 dx # }} }}
2 2
2 17
0.5 1 1 x
1
1
1
8
}} #
}}4 dx # }}
4
17
0.5 1 1 x
1
1
1
8
1
8
}} 1 }} # }}4 dx # }} 1 }}
4
2
17
17
0 11x
1
49
33
1
}} # }}4 dx # }}
68
34
0 11x
E
c 5 6Ï3w
E
1 21 2
Since Ï3w is in [0, 3], x 5 Ï3w.
E
27. An antiderivative of 23x 2 2 1 is F(x) 5 2x 3 2 x.
E
1 42p
2
2
f (t) dt 5 }} }} 5 }}.
21
av( f ) 5 }}
Find x 5 c in [0, Ï3w] such that c2 2 1 5 0
c2 5 1
c 5 61
Since 1 is in [0, Ïw3], x 5 1.
1
1
1
31. There are equal areas above and below the x-axis.
4
E1 2
E
av( f ) 5 }}
1
25. An antiderivative of x 2 2 1 is F(x) 5 }}x 3 2 x.
3
Ï3
w
1
2
(x 2 1) dx
av 5 }}
Ïw3 0
1
5 }} F(Ï3w) 2 F(0)
Ïw3
1
5 }}(0 2 0) 5 0
Ïw3
2
42p
2
1
2
is 2(1) 2 }}p(1)2 5 }}.
5 2 2}} 2 0 1 2}} 2 2}} 5 13
3
1
av 5 }} (23x 2 2 1) dx 5 F(1) 2 F(0) 5 22
Find x 5 c in [0, 1] such that 23c2 2 1 5 22
23c2 5 21
12
1 21 2
E
E
0
35. max sin (x 2 ) 5 sin (1) on [0, 1]
E sin (x ) dx # sin (1) , 1
1
3
1
c2 5 }}
2
0
1
c 5 6}}
Ïw3
36. max Ïxw1
ww8 5 3 and min Ïxw1
ww8 5 2Ï2w on [0, 1]
1
1
Since }} is in [0, 1]. x 5 }}.
Ïw3
Ïw3
2Ï2w #
1
28. An antiderivative of (x 2 1)2 is F(x) 5 }}(x 2 1)3.
3
3
1
1
1 8
1
av 5 }} (x 2 1)2 dx 5 }}[F(3) 2 F(0)] 5 }} }} 1 }} 5 1
3 0
3
3 3
3
E
1
2
Find x 5 c in [0, 3] such that (c 2 1)2 5 1.
c 2 1 5 61
c 5 2 or c 5 0.
Since both are in [0, 3], x 5 0 or x 5 2.
29. The region between the graph and the x-axis is a triangle of
height 3 and base 6, so the area of the region
1
2
is }}(3)(6) 5 9.
1
6
E
av( f ) 5 }}
2
9
6
3
2
f (x) dx 5 }} 5 }}
24
217
E Ïxw1ww8 dx # 3
1
0
37. (b 2 a) min f (x) $ 0 on [a, b]
0 # (b 2 a) min f (x) #
E f (x) dx
b
a
38. (b 2 a) max f (x) # 0 on [a, b]
E f (x) dx # (b 2 a) max f (x) # 0
b
a
218
Section 5.4
E
b
39. Yes,
a
av( f ) dx 5
E
46. An antiderivative of F9(x) is F(x) and an antiderivative of
b
f (x) dx.
a
G9(x) is G(x).
This is because av( f ) is a constant, so
E
b
3
av( f ) dx 5 av( f ) ? x
a
E F9(x) dx 5 F(b) 2 F(a)
E G9(x) dx 5 G(b) 2 G(a)
Since F9(x) 5 G9(x), E F9(x) dx 5 E G9(x) dx, so
b
b
4
a
b
a
5 av( f ) ? b 2 av( f ) ? a
a
b
5 (b 2 a)av( f )
3
1
b2a
5 (b 2 a) }}
5
E
b
a
E
a
b
a
b
f (x) dx
4
a
F(b) 2 F(a) 5 G(b) 2 G(a).
f (x) dx
■ Section 5.4 Fundamental Theorem of
Calculus (pp. 277–288)
40. (a) 300 mi
150 mi
30 mph
150 mi
50 mph
(b) }} 1 }} 5 8 h
Exploration 1
300 mi
(c) }} 5 37.5 mph
8h
2. The function y 5 tan x has vertical asymptotes at all odd
(d) The average speed is the total distance divided by the
d 1d
1
total time. Algebraically, }
}2 . The driver computed
t1 1 t2
d
1 d
}} }}1 1 }}2 . The two expressions are not equal.
2 t1
t2
1
2
1000 m3
10 m /min
1000 m3
Time for second release 5 }3} 5 50 min
20 m /min
total released
2000 m3
1
Average rate 5 }} 5 }} 5 13}} m3/min
total time
150 min
3
41. Time for first release 5 }3} 5 100 min
E sin x dx # E x dx 5 3}12}x 410 5 }12}
1
42.
1
0
p
2
multiples of }}. There are six of these between 210 and 10.
3. In attempting to find F(210) 5
E
210
3
tan (t) dt 1 5, the
calculator must find a limit of Riemann sums for the
integral, using values of tan t for t between 210 and 3. The
large positive and negative values of tan t found near the
asymptotes cause the sums to fluctuate erratically so that no
limit is approached. (We will see in Section 8.3 that the
“areas” near the asymptotes are infinite, although NINT is
not designed to determine this.)
4. y 5 tan x
2
0
E sec x dx $ E 11 1 }x2}2 dx 5 3x 1 }x6}410 5 }76}
1
43.
Graphing NINT f
1
0
2
3
0
[1.6, 4.7] by [22, 2]
1
2
44. (a) Area 5 }}bh
5. The domain of this continuous function is the open interval
h
2b
(b) }}x 2 1 C
p 3p
E y(x) dx 5 3}2h}b x 4b0 5 }h2bb} 5 }12}bh
b
(c)
1}2}, }2}2.
2
2
6. The domain of F is the same as the domain of the
0
1
k
E
k
1 1
k k11
3
45. av(x k) 5 }} x k dx 5 }} }}x k11
0
x11
k
k k11
}
40 5 }
k(k 1 1)
x
x(x 1 1)
Graph y1 5 }} and y2 5 x on a graphing calculator
and find the point of intersection for x . 1.
p 3p
2
12
2
continuous function in step 4, namely }}, }} .
7. We need to choose a closed window narrower than
p 3p
1}2}, }2}2 to avoid the asymptotes.
[1.6, 4.7] by [0, 16]
[1, 3] by [0, 3]
8. The graph of F looks like the graph in step 7. It would be
Thus, k < 2.39838
p
12 4
3
3p
2
2
decreasing on }}, p and increasing on p, }} , with
p
3p
vertical asymptotes at x 5 }} and x 5 }}.
2
2
Section 5.4
Exploration 2
The Effect of Changing a in
E f (t) dt
dy
dx
1
dx/dy
219
1
3x
10. }} 5 }} 5 }}
x
a
Section 5.4 Exercises
1.
E 12 2 }1x}2 dx 5 32x 2 ln )x)4
3
3
1.
1/2
1/2
1
2
1
2
5 (6 2 ln 3) 2 1 2 ln }}
[24.7, 4.7] by [23.1, 3.1]
2.
1
2
5 5 2 ln 3 1 ln }}
5 5 2 ln 3 2 ln 2
5 5 2 ln 6 < 3.208
[24.7, 4.7] by [23.1, 3.1]
3. Since NINT(x 2, x, 0, 0) 5 0, the x-intercept is 0.
4. Since NINT(x , x, 5, 5) 5 0, the x-intercept is 5.
d
dx
E
21
2.
2
1
ln 3
2
E
x
a
It will always be the same as the graph of y 5 f (x).
26
3 ln 3
x
a
a
Quick Review 5.4
dy
dx
a
f (t) dt.
4.
2
E
3
E
2
}}2 dx 5 2
22 x
E
32
41
22
1
12
3
x22 dx 5 2 2x21
E sin x dx 5 32cos x4
0
p
4
p
0
5 p < 3.142
dy
dx
E
p/3
9.
3
0
p/3
40
2 sec2 u du 5 2 tan u
5 2(Ï3w 2 0)
(2sin x)(x) 2 (cos x)(1)
dy
x sin x 1 cos x
7. }} 5 }}}
5 2}}
x2
x2
dx
5 2Ï3w < 3.464
E
5p/6
10.
p/6
3
5p/6
4p/6
csc2 u du 5 2cot u
5 Ï3w 2 (2Ï3w)
5 2Ï3w < 3.464
9. Implicitly differentiate:
dy
dy
x}} 1 (1)y 1 1 5 2y}}
dx
dx
dy
}}(x 2 2y) 5 2(y 1 1)
dx
dy
y11
y11
}} 5 2}} 5 }}
dx
x 2 2y
2y 2 x
1
2
5 (p 1 0) 2 (0 1 0)
5. }} 5 2x ln 2
dy
dx
dt
dt
dy
dy/dt
cos t
}} 5 }} 5 }} 5 2cot t
dx
dx/dt
2sin t
3
5 2 1 2 }} 5 1
5 1 2 (21) 5 2
0
8. }} 5 cos t, }} 5 2sin t
21
4
0
E (1 1 cos x) dx 5 3x 1 sin x4
dy
3
7
4. }} 5 }} 2 }} 5 0
dx
3x
7x
dy
1
1
6. }} 5 }}x21/2 5 }}
dx
2
2Ïwx
2
5
2
2
22
p
8.
2
3
5 25 }} 2 1 5 }}
21
p
7.
1
40 1 3
2
5
3
21
dy
2. }} 5 2(sin x)(cos x) 5 2 sin x cos x
dx
5
2
3 5 40
x26/5 dx 5 25x21/5
1
1
2
3
dx 5 }}x 5/2 5 }}(25Ï5w 2 0) 5 10Ï5w < 22.361
32
5.
1
3
1 Ïxw) dx 5 }}x 3 1 }}x 3/2 5 }} 1 }} 2 (0 1 0) 5 1
3/2
0
6.
5 2 sec2 x tan x 2 2 tan x sec2 x 5 0
Ex
5
1
2
0
1. }} 5 cos(x 2) ? 2x 5 2x cos (x 2)
dy
3. }} 5 2(sec x)(sec x tan x) 2 2(tan x)(sec2 x)
dx
E (x
1
3.
such a way that a is always the x-intercept. If we change
E
2
5 2}} < 27.889
E f (t) dt vertically in
from a1 to a2, the distance of the vertical shift is
1
1
1 ln 3 21 3
5 }} } } 2 9
5. Changing a has no effect on the graph of y 5 }} f (t) dt.
6. Changing a shifts the graph of y 5
21
31 2 42
3x dx 5 }} 3x
11.
E
csc x cot x dx 5 2csc x
12.
E
4 sec x tan x dx 5 4 sec x
3p/4
p/4
p/3
0
3
3p/4
4p/4
3
p/3
40
5 (2Ï2w) 2 (2Ï2w) 5 0
5 4(2 2 1) 5 4
220
Section 5.4
E
1
13.
21
3
1
3
(r 1 1)2 dr 5 }}(r 1 1)3
14.
4
0
4
8
3
21/2
0
8
3
5 } } 2 0 5 }}
21
1 2 Ïuw
E}
} du 5 E (u
Ïuw
4
1
17. Graph y 5 x 3 2 3x 2 1 2x.
2 1) du
3
5 2u1/2 2 u
4
40
[0, 2] by [21, 1]
5 (4 2 4) 2 (0 2 0) 5 0
15. Graph y 5 2 2 x.
Over [0, 1]:
E (x
1
1
34
1
40
1
41
1
4
1
4
2 3x 2 1 2x) dx 5 }}x 4 2 x 3 1 x 2 5 }} 2 0 5 }}
3
0
Over [1, 2]:
E (x
2
1
1
4
1
4
) 14 ) ) 14 )
1
2
Total area 5 }} 1 2}} 5 }}
[0, 3] by [22, 3]
E
2
1
Over [0, 2]: (2 2 x) dx 5 2x 2 }}x 2
2
0
3
2
40 5 2
18. Graph y 5 x 3 2 4x.
E (2 2 x) dx 5 32x 2 }12}x 4 5 }32} 2 2 5 2}12}
3
Over [2, 3]:
2
34
2 3x 2 1 2x) dx 5 }}x 4 2 x 3 1 x 2 5 0 2 }} 5 2}}
3
2
2
3
2
1
5
Total area 5 )2) 1 2}} 5 }}
2
2
) )
[22, 2] by [24, 4]
16. Graph y 5 3x 2 3.
2
Over [22, 0]:
E
0
22
1
0
34
4
1
40
(x 3 2 4x) dx 5 }}x 4 2 2x 2
5 0 2 (24) 5 4
22
Over [0, 2]:
E (x
2
[22, 2] by [24, 10]
34
0
Over [22, 21]:
E
21
22
Total area 5 )4) 1 )4) 5 8
3
4
(3x 2 2 3) dx 5 x 3 2 3x
21
5 2 2 (22) 5 4
22
Over [21, 1]:
E
1
21
Over [1, 2]:
x2 2 1
x11
3
E (3x
1
x2 2 1
x11
19. (a) No, f (x) 5 }} is discontinuous at x 5 21.
(b) }} 5 x 2 1, x Þ 21
4
(3x 2 2 3) dx 5 x 3 2 3x
2
2
2 4x) dx 5 }}x 4 2 2x2 5 24 2 0 5 24
3
2
1
5 22 2 2 5 24
21
3
2
41
2 3) dx 5 x 3 2 3x 5 2 2 (22) 5 4
Total area 5 )4) 1 )24) 1 )4) 5 12
The area between the graph of f and the x-axis over
1
2
9
2
[22, 1) where f is negative is }}(3)(3) 5 }}. The area
between the graph of f and the x-axis over (1, 3] where
1
2
f is positive is }}(2)(2) 5 2.
E
3
x2 2 1
9
5
}} dx 5 2}} 1 2 5 2}}
2
2
22 x 1 1
9 2 x2
3x 2 9
20. (a) No, f (x) 5 }} is discontinuous at x 5 3.
31x
3
9 2 x2
3x 2 9
(b) }} 5 2}}, x Þ 3
Note that f is negative for x in [0, 5]. f (0) 5 21 and
8
3
f (5) 5 2}}. The area between the graph of f and the
1
2
5
55
9 2 x2
}} dx 5 2}}
6
0 3x 2 9
1
8
3
2
55
6
x-axis over [0, 5] is }}(5 2 0) 1 1 }} 5 }}
E
Section 5.4
p
2
3p
2
21. (a) No, f (x) 5 tan x is discontinuous at x 5 }} and x 5 }}.
26. First find the area under the graph of y 5 Ïxw.
Ex
1
p
(b) The integral does not have a value. If 0 , b , }}, then
2
E tan x dx 5 32ln )cos x)4
b
0
b
5 2ln )cos b) since the
0
p
Fundamental Theorem applies for [0, b]. As b → }}2,
2
cos b → 01 so 2ln )cos b) → ` or
E tan x dx → `.
b
1/2
0
1
2
2
3
3 3 40
dx 5 }}x 3/2 5 }}
Next find the area under the graph of y 5 x 2.
Ex
2
2
1
1
2
8
3
3 3 41
1
3
7
3
dx 5 }}x 3 5 }} 2 }} 5 }}
2
3
27. First find the area under the graph of y 5 1 1 cos x.
E (1 1 cos x) dx 5 3x 1 sin x4
p
[0, 2p], so it doesn’t exist over [0, 2p].
(b) The integral does not have a value. If 0 , b , 1, then
x11
1
E}
} dx 5 E }} dx 5 3ln )x 2 1)4
x 21
x21
b
0
b
Area of the shaded region 5 2p 2 p 5 p.
28. First, find the area of the region between y 5 sin x and the
5 ln )b 2 1),
0
x11
1
since }
} 5 }} and the Fundamental Theorem
x2 2 1
x21
2
applies for [0, b]. As b → 1 , ln )b 2 1) → 2` or
x11
E}
} dx → 2`. Hence the integral does not exist
x 21
b
0
5p
0
The area of the rectangle is 2p.
x11
x 21
0
p
0
22. (a) No, f (x) 5 }
2 } is discontinuous at x 5 1.
2
7
3
Area of the shaded region 5 }} 1 }} 5 3
0
Hence the integral does not exist over a subinterval of
b
p 5p
6
36
4
x-axis for }}, }} .
E
5p/6
p/6
3
sin x dx 5 2cos x
5p/6
4p/6
Ïw3
Ïw3
5 }} 2 2}} 5 Ï3w
1
p 2p
6 3
1
2
sin x
x
(b) NINT }}, x, 21, 2 < 2.55. The integral exists since
sin x
x
the area is finite because }} is bounded.
1 2 cos x
24. (a) No, f (x) 5 }}
is discontinuous at x 5 0.
x2
1 2 cos x
(b) NINT }}
, x, 22, 3 < 2.08. The integral exists
x2
1 2 cos x
since the area is finite because }}
is bounded.
x2
1
p
3
Area of the shaded region 5 Ï3w 2 }}
1 3 1 2 sin x
2
2x 2 1
30. NINT1}}, x, 20.8, 0.82 < 1.427
x 21
2
4
1
2
wswxw, x, 21, 1) < 0.914
31. }}NINT(Ïco
2w
2w
x 2 $ 0 between x 5 22 and x 5 2
32. Ï8ww
NINT(Ï8ww
2w2w
x 2, x, 22, 2) < 8.886
2
33. Plot y1 5 NINT(e 2t , t, 0, x), y2 5 0.6 in a [0, 1] by [0,1]
window, then use the intersect function to find
x < 0.699.
34. When y 5 0, x 5 1.
y3 5 1 2 x3
3
25. First, find the area under the graph of y 5 x 2.
1
3
1
3 40
1
3
dx 5 }}x 3 5 }}
Next find the area under the graph of y 5 2 2 x.
E (2 2 x) dx 5 32x 2 }12}x 4
2
1
p
3
4
sin x
x
0
21 2
2
29. NINT }}, x, 0, 10 < 3.802
23. (a) No, f (x) 5 }} is discontinuous at x 5 0.
2
2
1
[0, 2].
1
1
2
The area of the rectangle is sin }} }} 5 }}
2
over a subinterval of [0, 2], so it does not exist over
Ex
221
2
2
3
2
1
2
5 2 2 }} 5 }}
1
1
3
1
2
5
6
Area of the shaded region 5 }} 1 }} 5 }}
y 5 Ï1ww
2wx 3w
3
NINT(Ï1ww
2wx 3w, x, 0, 1) < 0.883
222
Section 5.4
E f (t) dt 1 K 5 E f (t) dt
K 5 2E f (t) dt 1 E f (t) dt
5 E f (t) dt 1 E f (t) dt
5 E f (t) dt
K 5 E (t 2 3t 1 1) dt
x
35.
43. Choose (d).
x
a
b
x
dy
d
}} 5 }}
dx
dx
x
a
a
x
x
21
2
3
1
3
3
3
2
8
4 33
E
dy
d
}} 5 }}
dx
dx
36. To find an antiderivative of sin2 x, recall from trigonometry
1
2
1
2
that cos 2x 5 1 2 2 sin2 x, so sin2 x 5 }} 2 }}cos 2x.
E sin
0
2
21
t dt
2
E 3}12} 2 }12}cos (2x)4 dx
2
1
1
4
32
1
0
4
sin 2 cos 2
2
sin 2 cos 2 2 2
2
2
1
x
d
x
4
1
1
1
d
1E
0
cos (2t) dt 2
E
x
2
5 cos (2x ) ? 3x 2 cos (2x ) ? 2x
3
2
1E
1E
d
dx
d
5 }}
dx
cos x
sin x
cos x
0
a
a
1E1 f (t) dt2 5 }d}x (x 2 2 2x 1 1) 5 2x 2 2
2
sin x
0
10
E }111}
dt 5 }}
t 2
11x
x
0
0
E }111}
dt 5 2
t
0
0
x
2
2
5 2px sin px 1 cos px
f (4)5 24p sin 4p 1 cos 4p 5 1
E
E
2
E
sin x
2
t 2 dt
0
2
5 2sin x cos2 x 2 sin2 x cos x
p
k
51. One arch of sin kx is from x 5 0 to x 5 }}.
t 2 dt
t 2 dt 2
d
1
1E
Area 5
5 cos x ? (2sin x) 2 sin x ? cos x
2
E f (t) dt 5 0
2
5 3x 2 cos (2x 3) 2 2x cos (2x 2)
42. }} 5 }}
dt 2 3 5 0 2 3 5 23
5 x(2p sin px) 1 1 ? cos px
cos (2t) dt
0
2
d
f (t) dt
dx 0
d
5 }}(x cos px)
dx
d
dx
3
2
dt 2 3 5 e2x
x
50. f (x) 5 }}
40. }} 5 cos (2x) }}(2x) 5 2 cos (2x)
x
2t2
1
f9(0) 5 10
39. }} 5 sin (Ïxw)2 }} (Ïxw) 5 (sin x) ? }}x21/2 5 }}
dx
2
dx
2Ïxw
dy
d
41. }} 5 }}
dx
dx
1
2
L(x) 5 2 1 10x
1
dy
dx
Ee
f (0) 5 2 1
1E }t} dt2 5 }d}x 12E }t} dt2 5 2}x}
3
x
d
dx
dy
37. }} 5 Ï1ww
1wx 2w
dx
dy
1E1 e2t
49. f9(x) 5 }} 2 1
5 0 2 1 2 }} 5 }} < 21.189
1
46. Choose (a).
d
dx
0
2
1
0
48. f (x) 5 }}
2
1
2
x
47. x 5 a since
4
5 }}x 2 }}sin x cos x
1E0 sec t dt 1 42 5 sec x
0
y(1) 5
0
32
sec t dt 1 4 5 0 1 4 5 4
E sec t dt 1 4 5 0 1 4 5 4
y(0) 5
dy
d
}} 5 }}
dx
dx
5 }}x 2 }}sin (2x)
21
45. Choose (b).
3
2
4
5 2}} 2 }} 1 (21) 2 }} 2 6 1 2 5 2}}
dy
dx
x
42
d
dx
dt 2 3 5 0 2 3 5 23
1E21sec t dt 1 42 5 sec x
y(21) 5
21
1
3
5 }}t 3 2 }}t 2 1 t
3
2
dy
dx
2
2t 2
p
dy
d
}} 5 }}
dx
dx
2
38. }} 5 }}
2
dt 2 3 5 e2x
44. Choose (c).
b
5
p
2
b
a
K5
x
Ee
y(p) 5
b
1Ep e2t
52. (a)
23
p/k
0
3
1
k
40
sin kx dx 5 2}} cos kx
3
p/k
1
k
1
1 k2
1
2
1
3
22
3
125
5 }}
6
1
27
2
2
2
423
(6 2 x 2 x 2) dx 5 6x 2 }}x 2 2 }}x 3
5 }} 2 2}}
2
k
5 }} 2 2}} 5 }}
Section 5.4
2(21)
2(21)
1
2
1
55. (a) s9(3) 5 f (3) 5 0 units/sec
(b) The vertex is at x 5 }} 5 2}}. Recall that the
b
2a
vertex of a parabola y 5 ax 2 1 bx 1 c is at x 5 2}}.
1
25
4
1 22
25
4
2
y 2}} 5 }}, so the height is }}.
(c) The base is 2 2 (23) 5 5.
2
2
25
125
}}(base)(height) 5 }}(5) }} 5 }}
3
3
4
6
1 2
53. (a) H(0) 5
E f (t) dt 5 0
0
0
d
dx
1E0 f (t) dt2 5 f (x)
x
(b) H9(x) 5 }}
H 9(x) . 0 when f (x) . 0.
H is increasing on [0, 6].
(c) H is concave up on the open interval where
H 0(x) 5 f9(x) . 0.
f9(x) . 0 when 9 , x # 12.
H is concave up on (9, 12).
E
(b) s0(3) 5 f9(3) . 0 so acceleration is positive.
(c) s(3) 5
E f (x) dx 5 }12}(26)(3) 5 29 units
(d) s(6) 5
E f (x) dx 5 }12}(26)(3) 1 }12}(6)(3) 5 0, so the
0
3
0
6
0
particle passes through the origin at t 5 6 sec.
(e) s0(t) 5 f9(t) 5 0 at t 5 7 sec
(f) The particle is moving away from the origin in the
negative direction on (0, 3) since s(0) 5 0 and
s9(t) , 0 on (0, 3). The particle is moving toward the
origin on (3, 6) since s9(t) . 0 on (3, 6) and s(6) 5 0.
The particle moves away from the origin in the positive
direction for t . 6 since s9(t) . 0.
(g) The particle is on the positive side since
s(9) 5
E
9
f (x) dx . 0 (the area below the x-axis is
0
smaller than the area above the x-axis).
12
(d) H(12) 5
f (t) dt . 0 because there is more area
above the x-axis than below the x-axis.
(e) H 9(x) 5 f (x) 5 0 at x 5 6 and x 5 12. Since
H 9(x) 5 f (x) . 0 on [0, 6), the values of H are
increasing to the left of x 5 6, and since
H 9(x) 5 f (x) , 0 on (6, 12], the values of H are
decreasing to the right of x 5 6. H achieves its
maximum value at x 5 6.
(f) H(x) . 0 on (0, 12]. Since H(0) 5 0, H achieves its
minimum value at x 5 0.
54. (a) s9(t) 5 f (t). The velocity at t 5 5 is f (5) 5 2 units/sec.
E
0
56. (a) f (t) is an even function so
E
2x
sin (t)
}} dt 5
t
2x
sin (t)
E}
} dt.
t
(b) Si(0) 5
E }sint}t dt 5 0
0
0
(c) Si9(x) 5 f (t) 5 0 when t 5 pk, k a nonzero integer.
(d)
3
0
(d) s has its largest value at t 5 6 sec since
s9(6) 5 f (6) 5 0 and s0(6) 5 f9(6) , 0.
(e) The acceleration is zero when s0(t) 5 f9(t) 5 0. This
occurs when t 5 4 sec and t 5 7 sec.
(f) Since s(0) 5 0 and s9(t) 5 f (t) . 0 on (0, 6), the
particle moves away from the origin in the positive
direction on (0, 6). The particle then moves in the
negative direction, towards the origin, on (6, 9) since
s9(t) 5 f (t) , 0 on (6, 9) and the area below the x-axis
is smaller than the area above the x-axis.
(g) The particle is on the positive side since
s(9) 5
E f (x) dx . 0 (the area below the x-axis is
9
0
smaller than the area above the x-axis).
0
E
E
(b) s0(t) 5 f9(t) , 0 at t 5 5 since the graph is decreasing,
so acceleration at t 5 5 is negative.
E f (x) dx 5 }12}(3)(3) 5 4.5 units
x
sin (t)
}} dt
t
0
0
sin (t)
5 2 }} dt
t
2x
x
sin (t)
5 2 }} dt 5 2Si(x)
t
0
Si(2x)5
H(12) is positive.
(c) s(3) 5
223
[220, 20] by [23, 3]
E 1}dd}cx 2 dx
1
5 E }} dx 5 3Ïxw4
2Ïwx
57. (a) c(100) 2 c(1)5
100
1
100
100
1
1
5 10 2 1 5 9 or $9
E 1}dd}cx 2 dx
1
5 E }} dx5 3Ïxw4
2Ïwx
(b) c(400) 2 c(100) 5
400
100
400
400
100
100
5 20 2 10 5 10 or $10
224
Section 5.5
2
E 12 2 }
} dx 5 32x 1 2(x 1 1) 4
(x 1 1) 2
3
58.
21
2
0
3
1
2
9
2
4
5 6 1 }} 2 2 5 }}
1
solutions, using the functions Si(x) and f (t) as defined in
E 1450 2 }x2}2 dx 5 }31}0 3450x 2 }x6}4
30
3 30
2
0
0
5 300 drums
(b) True, because h and h9 are both differentiable by part
(a).
(c) True, because h9(1) 5 f (1) 5 0.
(d) True, because h9(1) 5 f (1) 5 0 and h0(1) 5 f9(1) , 0.
E
x
f (t) dt 5 2 f (t) dt because the area
0
of the area between the curve and the x-axis from 2x to 0,
but it is on the opposite side of the x-axis.
0
E
f (t) dt 5 2
3 E
x
4 E f (t) dt
f (t) dt 5 2 2 f (t) dt 5
2x
E f (t) dt is even.
x
Thus
0
0
x
0
0
E
0
62. Since f (t) is even,
f (t) dt 5
2x
This means that
Si((2k 1 2)p) 2 Si(2kp) 5
)f (x)) dx .
E
E
(2k12)p
(2k11)p
)f (x)) dx.
(2k12)p
2kp
f (x) dx . 0, so each
sin x
x
2
continuous for x . 0, this means Si(x) . 1.42 (and hence
between the curve and the x-axis from 0 to x is the opposite
2x
2kp
1
(g) True, because h9(x) 5 f (x), and f is a decreasing
function that includes the point (1, 0).
E
E
(2k11)p
the previous one, so
Since f (2p) < NINT }}, x, 0, 2p < 1.42 and Si(x) is
(f) False, because h 0(1) 5 f9(1) Þ 0
2x
Furthermore, each arch of y 5 f (x) is smaller in height than
successive minimum value is greater than the previous one.
(e) False, because h 0(1) 5 f9(1) , 0.
0
decreasing on each interval [(2k 1 1)p, (2k 1 2)p], where
local minima at x 5 2kp, where k is a positive integer.
60. (a) True, because h9(x) 5 f (x) and therefore h0(x) 5 f9(x).
E
increasing on each interval [2kp, (2k 1 1)p] and
k is a nonnegative integer. Thus, for x . 0, Si(x) has its
(b) (300 drums)($0.02 per drum) 5 $6
61. Since f (t) is odd,
sin x
x
d
dx
Exercise 56. Since }}Si(x) 5 f (x) 5 }}, Si(x) is
The company should expect $4500.
1
30 2 0
2
x < 1.0648397. We now argue that there are no other
0
5 4.5 thousand
59. (a) }}
sin t
t
64. Solving NINT }}, t, 0, x 5 1 graphically, the solution is
3
E f (t) dt because the area
x
0
Si(x) Þ 1) for x $ 2p. Now, Si(x) 5 1 has exactly one
solution in the interval [0, p] because Si(x) is increasing on
this interval and x < 1.065 is a solution. Furthermore,
Si(x) 5 1 has no solution on the interval [p, 2p] because
Si(x) is decreasing on this interval and Si(2p) < 1.42 . 1.
Thus, Si(x) 5 1 has exactly one solution in the interval
[0, `). Also, there is no solution in the interval (2`, 0]
because Si(x) is odd by Exercise 56 (or 62), which means
that Si(x) # 0 for x # 0 (since Si(x) $ 0 for x $ 0).
between the curve and the x-axis from 0 to x is the same as
the area between the curve and the x-axis from 2x to 0.
E
2x
0
E
f (t) dt 5 2
E
f (t) dt 5 2 f (t) dt
2x
Exploration 1
0
0
E f (t) dt is odd, but
x
63. If f is an even continuous function, then
E
0
x
d
}} f (t) dt 5 f (x). Therefore, f is the derivative of the odd
dx 0
x
continuous function
■ Section 5.5 Trapezoidal Rule (pp. 289–297)
x
E f (t) dt is odd.
x
Thus
0
E f (t) dt.
0
Similarly, if f is an odd continuous function, then f is the
E f (t) dt.
x
derivative of the even continuous function
0
Area Under a Parabolic Arc
1. Let y 5 f (x) 5 Ax 2 1 Bx 1 C
Then y0 5 f (2h) 5 Ah 2 2 Bh 1 C,
y1 5 f (0) 5 A(0)2 1 B(0) 1 C 5 C, and
y2 5 f (h) 5 Ah 2 1 Bh 1 C.
2. y0 1 4y1 1 y2 5 Ah 2 2 Bh 1 C 1 4C 1 Ah 2 1 Bh 1 C
5 2Ah 2 1 6C.
3. Ap 5
E
h
(Ax 2 1 Bx 1 C) dx
2h
3
x
x2
h
3
2
2h
h3
h2
h3
h2
5 A}} 1 B}} 1 Ch 2 2A}} 1 B}} 2 Ch
3
2
3
2
h3
5 2A}} 1 2Ch
3
h
5 }}(2Ah 2 1 6C)
3
3
5 A}} 1 B}} 1 Cx
4
1
2
Section 5.5
4. Substitute the expression in step 2 for the parenthetically
enclosed expression in step 3:
Section 5.5 Exercises
220
4
h
3
h
5 }}(y0 1 4y1 1 y2).
3
Ap 5 }}(2Ah 2 1 6C)
x
0
f (x)
0
1
}}
2
1
}}
2
Quick Review 5.5
1. y9 5 2sin x
y0 5 2cos x
y0 , 0 on [21, 1], so the curve is concave down on
[21, 1].
2. y9 5 4x 2 12
y0 5 12x 2
y0 . 0 on [8, 17], so the curve is concave up on [8, 17].
3
3. y9 5 12x 2 6x
y0 5 24x 2 6
y0 , 0 on [28, 0], so the curve is concave down on
[28, 0].
2
1
2
1
4
0
220
4
0
f (x)
0
1
4
1
}}
2
1
}}
4
Ex
2
(c)
2
0
4
9
142
142
2
2
1
8
3
3 3 40
dx 5 }}x 3 5 }}
220
4
1
2
3. (a) f (x) 5 x 3, h 5 }} 5 }}
x
0
f (x)
0
1
}}
2
1
}}
8
1
4
3
}}
2
27
}}
8
1
1
1
1
2
8
27
182
182
2
T 5 }} 0 1 2 }} 1 2(1) 1 2 }} 1 8 5 4.25
(b) f9(x) 5 3x , f 0(x) 5 6x . 0 on [0, 2]
The approximation is an overestimate.
2
Ex
2
(c)
3
0
2
1
3 4 40
dx 5 }}x 4 5 4
221
4
1
x
1
4
4. (a) f (x) 5 }}, h 5 }} 5 }}
9. y9 5 2100x 9
y0 5 2900x 8
y0 , 0 on [10, 1010], so the curve is concave down on
[10, 1010].
10. y9 5 cos x 1 sin x
y0 5 2sin x 1 cos x
y0 , 0 on [1, 2], so the curve is concave down.
1
2
(b) f9(x) 5 2x, f 0(x) 5 2 . 0 on [0, 2]
The approximation is an overestimate.
[100, 200].
8. y9 5 2csc x cot x
y 0 5 (2csc x)(2csc2 x) 1 (csc x cot x)(cot x)
5 csc3 x 1 csc x cot2 x
y0 . 0 on [0, p], so the curve is concave up on [0, p].
3
}}
2
9
}}
4
1
1
1
y0 , 0 on [100, 200], so the curve is concave down on
y0 . 0 on [3, 6], so the curve is concave up on [3, 6].
1
2
T 5 }} 0 1 2 }} 1 2(1) 1 2 }} 1 4 5 2.75
1
y0 5 2}}2
x
2
x
2
2
x
1
x
y0 5 }}3
2
2. (a) f (x) 5 x , h 5 }} 5 }}
6. y9 5 }}
1
x
122
E x dx 5 3}12}x 4 5 2
2
[48p, 50p].
7. y9 5 2}}2
2
3
122
0
x
2
5. y9 5 2e
y0 5 4e 2x
y0 . 0 on [25, 5], so the curve is concave up on [25, 5].
1
1
2
(c)
y0 5 2}} sin }}
2x
1
2
(b) f9(x) 5 1, f 0(x) 5 0
The approximation is exact.
x
2
y0 # 0 on [48p, 50p], so the curve is concave down on
3
}}
2
3
}}
2
1
T 5 }} 0 1 2 }} 1 2(1) 1 2 }} 1 2 5 2
4. y9 5 }}cos }}
1
4
1
2
1. (a) f (x) 5 x, h 5 }} 5 }}
x
1
f (x)
1
1
8
1
5
}}
4
4
}}
5
4
152
3
}}
2
2
}}
3
2
132
7
}}
4
4
}}
7
2
1
}}
2
4
172
1
2
2
T 5 }} 1 1 2 }} 1 2 }} 1 2 }} 1 }} < 0.697
1
2
(b) f9(x) 5 2}}2 , f 0(x) 5 }}3 . 0 on [1, 2]
x
x
The approximation is an overestimate.
E }1x} dx 5 3ln)x)4
2
(c)
1
2
1
5 ln 2 < 0.693
225
226
Section 5.5
420
4
3 2 (21)
4
5. (a) f (x) 5 Ïxw, h 5 }} 5 1
x
0
1
f (x)
0
1
2
10. (a) f (x) 5 x 3 2 2x, h 5 }} 5 1
3
Ï2w Ï3w
4
x
21
0
1
2
3
2
f (x)
1
0
21
4
21
1
3
S 5 }}(1 1 4(0) 1 2(21) 1 4(4) 1 21) 5 12
1
2
T 5 }}(0 1 2(1) 1 2(Ï2w) 1 2(Ï3w) 1 2) < 5.146
1
2
1
4
(b) f9(x) 5 }}x21/2, f 0(x) 5 2}}x23/2 , 0 on [0, 4]
E
(b)
3
1
34
(x 3 2 2x) dx 5 }}x 4 2 x 2
21
The approximation is an underestimate.
(c)
3/2
0
1
p20
4
0
f (x)
0
Ïw2
}}
2
p
4
1
3p
}}
4
p
1
Ïw2
}}
2
0
(d) Simpson’s Rule for cubic polynomials will always give
exact values since f (4) 5 0 for all cubic polynomials.
11. The average of the 13 discrete temperatures gives equal
weight to the low values at the end.
122
122
2
1
12. (a) }}(126 1 2 ? 65 1 2 ? 66 1 … 1 2 ? 58 1 110) 5 841
2
1
12
av( f) < }} ? 841 < 70.08
(b) f9(x) 5 cos x, f 0(x) 5 2sin x , 0 on [0, p]
The approximation is an underestimate.
E sin x dx 5 32cos x4
p
(c)
0
2
(c) For f (x) 5 x 3 2 2x, Mf (4) 5 0 since f (4) 5 0.
p
}}
2
Ïw2
Ï2w
p
T 5 }} 0 1 2 }} 1 2(1) 1 2 }} 1 0 < 1.896
8
2 1
p
5 12
)Es) 5 0
6. (a) f (x) 5 sin x, h 5 }} 5 }}
x
21
4
0
p
}}
4
3
81
1
5 }} 2 9 2 }} 2 1
4
4
E Ïxw dx 5 3}23}x 4 5 }13}6 < 5.333
4
4
52
0
7. }}(6.0 1 2(8.2) 1 2(9.1) 1 … 1 2(12.7) 1 13.0)(30)
5
2
5 15,990 ft3
8. (a) }}(0 1 2(520) 1 2(800) 1 2(1000) 1 … 1 2(860)
200
2
1 0)(20) 5 26,360,000 ft3
(b) You plan to start with 26,360 fish. You intend to have
(0.75)(26,360) 5 19,770 fish to be caught. Since
(b) We are approximating the area under the temperature
graph. By doubling the endpoints, the error in the first
and last trapezoids increases.
13. S50 < 3.13791, S100 < 3.14029
14. S50 < 1.08943, S100 < 1.08943
15. S50 5 1.37066, S100 5 1.37066 using a 5 0.0001 as lower
limit
S50 5 1.37076, S100 5 1.37076 using a 5 0.000000001 as
lower limit
16. S50 < 0.82812, S100 < 0.82812
17. (a) T10 < 1.983523538
T100 < 1.999835504
T1000 < 1.999998355
(b)
19,770
}} 5 988.5, the town can sell at most 988 licenses.
20
1
3600
9. Sum the trapezoids and multiply by }} to change seconds
n
)ET) 5 2 2 Tn
10
0.016476462 5 1.6476462 3 1022
100
1.64496 3 1024
1000
1.645 3 1026
to hours
1
}}(2.2(0 1 30) 1 (3.2 2 2.2)(30 1 40)
2
1 (4.5 2 3.2)(40 1 50) 1 (5.9 2 4.5)(50 1 60)
1 (7.8 2 5.9)(60 1 70) 1 (10.2 2 7.8)(70 1 80)
1 (12.7 2 10.2)(80 1 90) 1 (16.0 2 12.7)(90 1 100)
(c) )ET
10n
1 (26.2 2 20.6)(110 1 120)
1
1 3600 2
1 (37.1 2 26.2)(120 1 130)) }} < 0.9785 miles
n
p2
n
p p2
p3
)ET ) # }} }}2 5 }}2
n
12 n
12n
p3
ET # }}2 5 1022)ET )
10n
n
12(10n)
(d) b 2 a 5 p, h 2 5 }}2 , M 5 1
)
1 (20.6 2 16.0)(100 1 110)
) < 1022)ET )
)
1 2
Chapter 5 Review
18. (a) S10 < 2.000109517
S100 < 2.000000011
S1000 < 2.000000000
(b)
22. Note that the tank cross-section is represented by the
shaded area, not the entire wing cross-section. Using
Simpson’s Rule, estimate the cross-section area to be
n
)ES) 5 2 2 Sn
10
1.09517 3 1024
100
1.1 3 1028
1000
0
(c) )ES
1
}}[y0 1 4y1 1 2y2 1 4y3 1 2y4 1 4y5 1 y6]
3
1
5 }}[1.5 1 4(1.6) 1 2(1.8) 1 4(1.9) 1 2(2.0)
3
1 4(2.1) 1 2.1] 5 11.2 ft2
1
1
1 42 lb/ft 21 11.2 ft 2
Length < (5000 lb) }}3 }}2 < 10.63 ft
) < 1024)ESn)
h
2
23. Tn 5 }}[y0 1 2y1 1 2y2 1 … 1 2yn21 1 yn]
10n
p
n
4
(d) b 2 a 5 p, h 4 5 }}4 , M 5 1
p p
p
4
h[ y 1 y 1 … 1 y
] 1 h[y 1 y 1 … 1 y ]
0
1
n21
1
2
n
5 }}}}}}
2
5
}
)ESn) # }180}1}n}4 2 5 }
180n 4
LRAMn 1 RRAMn
5 }}}
2
p5
} 5 1024)ES )
)ES10n) # }
n
180(10n)4
19. (a) f9(x) 5 2x cos (x 2)
f 0(x) 5 2x ? 22x sin (x 2) 1 2 cos (x 2)
5 24x 2 sin (x 2) 1 2 cos (x 2)
h
3
24. S2n 5 }}(y0 1 4y1 1 2y2 1 4y3 1 … 1 2y2n22
1 4y2n21 1 y2n )
1
3
5 }}[h(y0 1 2y1 1 2y2 1 … 1 2y2n21 1 y2n)
(b)
1 (2h)(y1 1 y3 1 y5 1 … 1 y2n21)]
2T2n 1 MRAMn
b2a
5 }}
, where h 5 }}.
3
2n
[21, 1] by [23, 3]
(c) The graph shows that 23 # f 0(x) # 2 so ) f 0(x)) # 3
for 21 # x # 1.
1 2 (21)
12
h2
2
(d) )ET ) # }}(h 2)(3) 5 }}
h2
2
■ Chapter 5 Review (pp. 298–301)
1.
y
4
0.12
2
(e) For 0 , h # 0.1, )ET) # }} # }} 5 0.005 , 0.01
1 2 (21)
h
2
0.1
(f) n $ }} $ }} 5 20
20. (a) f -(x) 5 24x2 ? 2x cos (x 2) 2 8x sin (x 2) 2 4x sin (x 2)
5 28x3 cos (x 2) 2 12x sin (x 2)
f (4)(x)5 28x3 ? 22x sin (x 2) 2 24x2 cos (x 2)
2 12x ? 2x cos (x 2) 2 12 sin (x 2)
5 (16x 4 2 12)sin (x 2) 2 48x 2 cos (x 2)
(b)
2
2.
1
2
1
2
x
y
4
[21, 1] by [230, 10]
(c) The graph shows that 230 # f (4)(x) # 10
so )f (4)(x)) # 30 for 21 # x # 1.
1 2 (21)
180
h4
3
2
(d) )Es) # }}(h 4)(30) 5 }}
4
h
3
4
0.4
3
(e) For 0 , h # 0.4, )ES) # }} # }} < 0.00853 , 0.01
1 2 (21)
h
2
0.4
(f) n $ }} $ }} 5 5
24 in.
6
21. h 5 }} 5 4 in.
Estimate the area to be
4
}}[0 1 4(18.75) 1 2(24) 1 4(26) 1 2(24) 1 4(18.75) 1
3
0] < 466.67 in2
1
2
1
15
8
x
21
8
2
15
4
LRAM4: }} 0 1 }} 1 3 1 }} 5 }} 5 3.75
227
228
Chapter 5 Review
3.
E f (x) dx 5 2E f (x) dx 5 23
2
y
9. (a)
5
5
4
2
The statement is true.
E
5
(b)
2
22
E
5E
5
1
2
1 63
2 64
165
64
1
x
195
64
105
64
5
E g(x) dx
f (x) dx 1 E f (x) dx 1 E
5
f (x) dx 1
22
2
22
5
22
2
5
g(x) dx
22
54131259
2
MRAM4: }} }} 1 }} 1 }} 1 }} 5 4.125
4.
[f (x) 1 g(x)] dx
y
The statement is true.
(c) If f (x) # g(x) on [22, 5], then
4
E
5
f (x) dx #
22
E
5
22
g(x) dx,
but this is not true since
E
E
5
22
5
2
22
1
2
1 15
2 8
21
8
1
E
2
E f (x) 5 4 1 3 5 7 and
f (x) 1
22
5
2
g(x) dx 5 2. The statement is false.
10. (a) Volume of one cylinder: pr 2h 5 p sin2 (mi ) Dx
x
n
2
15
4
∑ p sin2(mi ) Dx
n→`
Total volume: V 5 lim
RRAM4: }} }} 1 3 1 }} 1 0 5 }} 5 3.75
5.
f (x) dx 5
i51
(b) Use p sin2 x on [0, p].
y
NINT(p sin2 x, x, 0, p) < 4.9348
4
11. (a) Approximations may vary. Using Simpson’s Rule, the
area under the curve is approximately
2
1
}}[0 1 4(0.5) 1 2(1) 1 4(2) 1 2(3.5) 1 4(4.5) 1
3
2(4.75) 1 4(4.5) 1 2(3.5) 1 4(2) 1 0] 5 26.5
2
The body traveled about 26.5 m.
1
2
1 15
2 4
1
15
4
2
T4 5 }}(LRAM4 1 RRAM4) 5 }} }} 1 }} 5 3.75
E (4x 2 x ) dx 5 32x
2
6.
3
0
7.
2
1
4
n
LRAMn MRAMn RRAMn
10
1.78204 1.60321 1.46204
20
1.69262 1.60785 1.53262
30
1.66419 1.60873 1.55752
50
1.64195 1.60918 1.57795
1.62557 1.60937 1.59357
E }1x} dx 5 3ln )x)4 5 ln 5 2 ln 1 5 ln 5 < 1.60944
1
5
1
30
40
100
5
s
2 }}x 4 5 8 2 4 5 4
1000 1.61104 1.60944 1.60784
8.
(b)
2
Position (m)
1
x
10
t
Time (sec)
The curve is always increasing because the velocity is
always positive, and the graph is steepest when the
velocity is highest, at t 5 6.
Chapter 5 Review
E x dx
(b) E x sin x dx
(c) E x(3x 2 2) dx
1
(d) E }} dx
11x
px
(e) E p19 2 sin }}2 dx
10
10
12. (a)
E }1x} dx 5 3ln )x)4 5 1 2 0 5 1
36
25. E }} dx 5 E 36(2x 1 1)
(2x 1 1)
24.
0
1
10
1
1
0
10
e
e
3
1
3
0
0
3
5 29(2x 1 1)
2
0
2
10
E 1x 1 }x1}2 dx 5 E (x 1 x
2
26.
2
2
2
1
1
6
0
3
2
1
2
40 3
E
28.
E
29.
2
E}
} dy 5 32 ln )y 1 1)4 5 2 ln 3 2 0 5 2 ln 3
y11
3
2p/3
1
5 [8 2 0] 2 [6 2 8] 5 10
21
3
p/2
0
cos x dx 2
3
p/2
40
5 sin x
E
2
15.
E
16.
E 4x dx 5 32x 4
22
5
2
E
p/4
17.
cos x dx
3
4p/2
2 sin x
E
1
18.
21
[21.35, 3.35] by [20.5, 2.6]
The region under the curve is a quarter of a circle of radius
2.
E Ï4ww2wxw dx 5 }14}p(2)
2
5
5 50 2 8 5 42
3
40
2
2
1
421
5 6 2 (210) 5 16
E (8s 2 12s 1 5) ds 5 32s 2 4s 1 5s4
4
4
20. E }} dx 5 32}}4 5 22 2 (24) 5 2
x
x
3
2
4
3
0
E
3
y24/3 dy 5 23y21/3
E }tÏdt}wt 5 E t
4
22.
4
1
E
1
p/3
23.
0
532053
0
1
27
1
1
2
1
21.
[24, 8] by [0, 8]
The region under the curve consists of two triangles.
2
2
23/2
5p
Ï2w
Ïw2
5 }} 2 0 5 }}
3
1
2
31. Graph y 5 )x) dx on [24, 8].
p/4
(3x 2 2 4x 1 7) dx 5 x 3 2 2x 2 1 7x
19.
2
0
2
cos x dx 5 sin x
0
30. Graph y 5 Ï4ww
2wx w on [0, 2].
p
2
2
0
2
p
3 422 5 10 2 (210) 5 20
5 dx 5 5x
0
p/2
5 (1 2 0) 2 (0 2 1) 5 2
2
1
421 5 1 2 1 5 0
2x sin (1 2 x 2) dx 5 cos (1 2 x 2)
2
p
14. The graph is above the x-axis for 0 # x , }} and below the
2
p
x-axis for }} , x # p
2
E
0
42p/3 5 1 2 2 5 21
sec x tan x dx 5 sec x
6
44
5 4x 2 }}x 2 2 4x 2 }}x 2
1
1 22
27.
4
4
2
41
5 }} 2 2}} 5 2
0
E (4 2 x) dx 2 E (4 2 x) dx
4
Total area 5
) dx
32
x-axis for 4 , x # 6
1
2
22
5 }}x 2 2 x21
13. The graph is above the x-axis for 0 # x , 4 and below the
3
dx
1
40
22
1
0
Total area 5
23
5 21 2 (29) 5 8
10
0
229
27
41
1
2
1
2
)x) dx 5 }}(4)(4) 1 }}(8)(8) 5 40
32. Graph y 5 Ï6w4ww
2wx 2w on [28, 8].
4
3
3
8
24
5 21 2 (23) 5 2
41
dt 5 22t21/2 5 21 2 (22) 5 1
p/3
40
sec2 u du 5 tan u
E
5 Ï3w 2 0 5 Ï3w
[29.4, 9.4] by [23.2, 9.2]
The region under the curve y 5 Ï6w4ww
2wx 2w is half a circle
of radius 8.
E
8
28
2Ï6w4ww
2wx 2w dx 5 2
E
8
1
Ï6w4ww
2wx 2w dx 5 23}}p(8)24 5 64p
28
2
230
Chapter 5 Review
33. (a) Note that each interval is 1 day 5 24 hours
Upper estimate:
24(0.020 1 0.021 1 0.023 1 0.025 1 0.028
1 0.031 1 0.035) 5 4.392 L
Lower estimate:
24(0.019 1 0.020 1 0.021 1 0.023 1 0.025
1 0.028 1 0.031) 5 4.008 L
42.
1E0
43. c(x) 5
x
425 1 50
The total cost for printing 2500 newsletters is $230.
E
E
5E
0
24
0
4
Rich’s average daily inventory is 4800 cases.
E f (x) dx
(x 2 2) dx 1 E x dx
f (x) dx 1
c(t) 5 0.04I(t) 5 24 1 24t
4
0
4
24
1
14
3
4
0
2
1
1 }}x 3
3
24
64
4
16
3
0
37. Let f (x) 5 Ï1ww
1wsin
w2wxw
min f 5 1 since min sin2 x 5 0
2
E Ï1ww1wsinwwxw dx # Ï2w
2
1 2
4 3
3
4
1 16
4 3
40
1
2
4
3
38. (a) av(y) 5 }} Ïxw dx 5 }} }}x 3/2 5 }} }} 2 0 5 }}
0
1
4
1 4
5 }}x 2 x 2 1 3x
4
3
5 192
0
x
40
2 2t 1 3) dt 5 }}t 4 2 t 2 1 3t
or x < 1.63052.
0
4
3
14
4
Using a graphing calculator, x < 23.09131
0
E
3
x 4 2 4x 2 1 12x 2 16 5 0
E Ï1ww1wsinwwxw dx # (max f)(1 2 0)
1
420
0
1
14
(24 1 24t) dt 5 }} 24t 1 12t 2
1
}}x 4 2 x 2 1 3x 5 4
4
1
}}x 4 2 x 2 1 3x 2 4 5 0
4
max f 5 Ï2w since max sin2 x 5 1
(min f)(1 2 0) #
E (t
x
45.
5 [0 2 16] 1 }} 2 0 5 }}
1
14
Rich’s average daily holding cost is $192.
We could also say (0.04)4800 5 192.
4
3 40
33
E
av(c) 5 }}
0
1
5 }}x 2 2 2x
2
14
1
(600 1 600t) dt
14 0
14
1
5 }}[600t 1 300t 2 5 4800
14
0
44. av(I) 5 }}
35. One possible answer:
The dx is important because it corresponds to the actual
physical quantity Dx in a Riemann sum. Without the Dx,
our integral approximations would be way off.
0,1#
x
c(2500) 5 4Ï2w5w0w0w 1 30 5 230
5 95.1 ft
1
2
5 4Ïxw 1 30
3
2
24
0
5 4Ïxw 2 20 1 50
(b) }}[5.30 1 2(5.25) 1 2(5.04) 1 … 1 2(1.11) 1 0]
f (x) dx 5
x
25
3
34. (a) Upper estimate:
3(5.30 1 5.25 1 5.04 1 … 1 1.11) 5 103.05 ft
Lower estimate:
3(5.25 1 5.04 1 4.71 1 … 1 0) 5 87.15 ft
4
1
E}
} dt
t 11 2
E }Ï2}tw dt 1 50
5 4t1/2
1 0.035] 5 4.2 L
E
1
}
} dt 2
t2 1 1
1
1
5 }2} ? 2 2 }
}
(2x) 1 1
x2 1 1
2
1
5}
}2}
}
4x 2 1 1
x2 1 1
24
(b) }}[0.019 1 2(0.020) 1 2(0.021) 1 … 1 2(0.031)
2
36.
2x
dy
d
}} 5 }}
dx
dx
46. (a) True, because g9(x) 5 f (x).
(b) True, because g is differentiable.
(c) True, because g9(1) 5 f (1) 5 0.
1
a20
E
a
1 2
a 3
3
a
40
(d) False, because g0(1) 5 f9(1) . 0.
2
3
(b) av(y) 5 }} aÏxw dx 5 }} }}ax 3/2 5 }}a3/2
0
(e) True, because g9(1) 5 f (1) 5 0 and g0(1) 5 f9(1) . 0.
(f) False, because g0(1) 5 f9(1) Þ 0.
dy
dx
39. }} 5 Ï2ww
1wcoww
s3wx
dy
dx
(g) True, because g9(x) 5 f (x), and f is an increasing
function which includes the point (1, 0).
d
dx
40. }} 5 Ï2ww
1wcoww
s3w(7ww
x 2)w ? }}(7x 2) 5 14xÏ2ww
1wcoww
s3w(7ww
x 2)w
dy
dx
d
dx
1
E 3 16 t 2
x
4
0
6
31x
41. }} 5 }} 2 }}4 dt 5 2}}4
1
E Ï1ww1wxw dx 5 F(1) 2 F(0)
1
47.
48. y(x) 5
E }sint}t dt 1 3
x
5
Chapter 5 Review
b2a
2n
1
x
1
y0 5 2 2 }}2
x
49. y9 5 2x 1 }}
(b) Let h 5 }}.
S2n 5 }}[y0 1 4y1 1 2y2 1 4y3 1 2y4 1 … 1 2y2n22
h
3
1 4y2n21 1 y2n]
Thus, it satisfies condition i.
y(1) 5 1 1
E }1t} dt 1 1 5 1 1 0 1 1 5 2
1
1
1
1
y9(1) 5 2 1 }} 5 2 1 1 5 3
5 }}[h(y0 1 4y1 1 y2) 1 h(y2 1 4y3 1 y4) 1 …
1
3
1 h(y2n22 1 4y2n21 1 y2n )]
Thus, it satisfies condition ii.
Since each expression of the form
h(y2i22 1 4y2i21 1 y2i ) is equal to twice the area of
50. Graph (b).
y5
231
E 2t dt 1 4 5 3t 4
x
2
1
x
1 4 5 (x 2 2 1) 1 4 5 x 2 1 3
1
1
12
51. (a) Each interval is 5 min 5 }} h.
1
}}[2.5 1 2(2.4) 1 2(2.3) 1 … 1 2(2.4) 1 2.3]
24
29
5 }} < 2.42 gal
12
12
(b) (60 mi/h) }} h/gal < 24.83 mi/gal
29
1
2
1
52. (a) Using the freefall equation s 5 }}gt 2 from Section 3.4,
2
1
the distance A falls in 4 seconds is }}(32)(42) 5 256 ft.
2
When her parachute opens, her altitude is
6400 2 256 5 6144 ft.
(b) The distance B falls in 13 seconds is
1
}}(32)(132) 5 2704 ft. When her parachute opens, her
2
altitude is 7000 2 2704 5 4296 ft.
(c) Let t represent the number of seconds after A jumps.
For t $ 4 sec, A’s position is given by
SA(t) 5 6144 2 16(t 2 4) 5 6208 2 16t, so A lands at
6208
16
t 5 }} 5 388 sec. For t $ 45 1 13 5 58 sec, B’s
the ith of n rectangles plus the area of the ith of n
2 ? MRAM 1 T
n
n
trapezoids, S2n 5 }}
.
54. (a) g(1) 5
(b) g(3) 5
3
E f (t) dt 5 0
1
1
E f (t) dt 5 2}12}(2)(1) 5 21
3
1
(c) g(21) 5
E
21
1
E
f (t) dt 5 2
1
21
1
4
f (t) dt 5 2}}p(2)2 5 2p
(d) g9(x) 5 f (x); Since f (x) . 0 for 23 , x , 1 and
f (x) , 0 for 1 , x , 3, g(x) has a relative maximum at
x 5 1.
(e) g9(21) 5 f (21) 5 2
The equation of the tangent line is
y 2 (2p) 5 2(x 1 1) or y 5 2x 1 2 2 p
(f) g 0(x) 5 f9(x), f9(x) 5 0 at x 5 21 and f9(x) is not
defined at x 5 2. The inflection points are at x 5 21
and x 5 2. Note that g0(x) 5 f 9(x) is undefined at
x 5 1 as well, but since g0(x) 5 f 9(x) is negative on
both sides of x 5 1, x 5 1 is not an inflection point.
(g) Note that the absolute maximum is g(1) 5 0 and the
absolute minimum is
g(23) 5
E
23
1
E
f (t) dt 5 2
1
23
1
2
f (t) dt 5 2}}p(2)2 5 22p.
The range of g is [22p, 0].
55. (a) NINT(e2x
2/2
, x, 210, 10) < 2.506628275
2x 2/2
position is given by
NINT(e
SB(t) 5 4296 2 16(t 2 58) 5 5224 2 16t,
5224
16
so B lands at t 5 }} 5 326.5 sec. B lands first.
1
2
53. (a) Area of the trapezoid 5 }}(2h)(y1 1 y3) 5 h(y1 1 y3)
Area of the rectangle 5 (2h)y2 5 2hy2
h(y1 1 y3) 1 2(2hy2) 5 h(y1 1 4y2 1 y3)
, x, 220, 20) < 2.506628275
(b) The area is Ï2wp
w.
56. First estimate the surface area of the swamp.
20
}}[146 1 2(122) 1 2(76) 1 2(54) 1 2(40) 1 2(30)
2
1 13] 5 8030 ft2
1 yd3
27 ft
(5 ft)(8030 ft2) ? }}3 < 1500 yd3
232
Section 6.1
5. Again h 5 k 5 1. The y-coordinate of the midpoint of each
57. (a) V 2 5 (V max)2 sin2 (120pt)
7
2
line segment is }}. The x-coordinates of the midpoint of
Using NINT:
19
2
slopes of the line segments are
!§§§§
The 10 graphs are graphs of the functions.
5 (Vmax
Vrms 5
1 3 5
2 2 2
each line segment are }}, }}, }}, ..., }}. From left to right the
E (V ) sin (120pt) dt
(V )
1
) E sin (120pt) dt 5 (V ) }} 5 }}
2
2
1
av(V ) 5 }}
1
2
2
1
0
1
2
2
max
2
2
2
max
max
0
(Vmax)2
V x
}
} 5 }ma
}
2
Ï2w
2
2
2
2
,}
,}
, ..., }
}
1
3
5
19
}} 1 1 }} 1 1 }} 1 1
}} 1 1
2
2
(b) Vmax 5 240Ï2w < 339.41 volts
2
1 2
1 21
1 21
1x 2 }2}2 1 }2}, 0 # x # 1,
2
y1 5 }
1
}} 1 1
2
Chapter 6
Differential Equations and
Mathematical Modeling
3
y2 5 }
3
}} 1 1
2
■ Section 6.1 Antiderivatives and
Slope Fields (pp. 303–315)
Exploration 1
2
2
y3 5 }
5
}} 1 1
2
1
7
3
2
2
7
2
5
2
2
7
2
x 2 }} 1 }}, 1 # x # 2,
x 2 }} 1 }}, 2 # x # 3,
A
Constructing a Slope Field
1. As i and j vary from 1 to 10, 100 ordered pairs are produced. Each ordered pair represents a distinct point in the
viewing window.
1 21
2
y10 5 }
19
}} 1 1
2
19
2
2
7
2
x 2 }} 1 }}, 9 # x # 10.
2. The distance between the points with j fixed and i 5 r and
i 5 r 1 1 is the distance between their x-coordinates.
3Xmin 1 12(r 1 1) 2 12}2}4 2 3Xmin 1 (2r 2 1)}2}4
h
h
h
2
5 (Xmin 2 Xmin) 1 (2r 1 2 2 1 2 2r 1 1)}} 5 h
3. The distance between the points with i fixed and j 5 r and
j 5 r 1 1 is the distance between their y-coordinates.
3
k
2
4 3
k
2
Ymin 1 (2(r 1 1) 2 1)}} 2 Ymin 1 (2r 2 1)}}
4
k
5 (Ymin 2 Ymin) 1 (2r 1 2 2 1 2 2r 1 1)}} 5 k
2
[0, 10] by [0, 10]
6. For each line segment in part (5), make a column of parallel line segments as in part (4).
7. WL
Quick Review 6.1
1. 100(1.06) 5 $106.00
1
0.06 4
< $106.14
4
1
0.06 12
< $106.17
12
1
0.06 365
< $106.18
365
2. 100 1 1 }}
4. Here h 5 k 5 1. Each line segment in the third column has
slope }}, because the x-coordinate of the midpoint of each
3. 100 1 1 }}
1 3 5
19
line segment is 2.5. The y-coordinates are }}, }}, }}, …, }}.
2 2 2
2
4. 100 1 1 }}
4
7
The 10 graphs are graphs of the functions
dy
dx
d
dx
dy
dx
d
dx
dy
dx
d
dx
dy
dx
d
dx
2
2
2
y 5 }} (x 2 2.5) 1 }}, 2 # x # 3, for n 5 1, 3, 5, …, 19.
5. }} 5 }} sin 3x 5 (cos 3x)(3) 5 3 cos 3x
The length of the line segment can be increased or
6. }} 5 }} tan }}x 5 sec 2 }}x }} 5 }} sec 2 }}x
172
4
n
2
decreased by adjusting the restriction 2 # x # 3.
5
2
1
5
2
21 2 2
5
5
2
7. }} 5 }} Ce 2x 5 (Ce 2x)(2) 5 2Ce 2x
1
x12
8. }} 5 }} ln (x 1 2) 5 }}
[0, 10] by [0, 10]
5
2
Section 6.1
E x 11 3
9.
6. }} dx 5 ln )x 1 3) 1 C
Check:
d
1
}}[ln )x 1 3) 1 C] 5 }}
dx
x13
[0.01, 5] by [23, 3]
By setting the left endpoint at x 5 0.01 instead of x 5 0,
we avoid an error that occurs when our calculator attempts
1x
2
1
E
E
x22
2
x2
2
8. (2x 23 1 x 2 1) dx 5 }} 1 }} 2 x 1 C
to calculate NINT }}, x, 1, 0 . The graph appears to be the
9.
same as the graph of y 5 ln x.
x6
6
7. (x 5 2 6x 1 3) dx 5 }} 2 3x 2 1 3x 1 C
E1e
t/2
5
t
E
2
2 }}2 dt 5 (e t/2 2 5t 2 2) dt
5 2e t/2 1 5t 2 1 1 C
10.
5
t
5 2e t/2 1 }} 1 C
E 43
E 43
3
10. }} Ïtw dt 5 }} t 1/3 dt 5 t 4/3 1 C
[25, 20.01] by [23, 3]
11.
E1x
1
x
2
we avoid an error that occurs when our calculator attempts
1x
2
1
the same as the graph of y 5 ln (2x).
Section 6.1 Exercises
1.
E
x3
(x 2 2x 1 1) dx 5 }} 2 x 2 1 x 1 C
3
2
12.
E1Ïxw 1 }Ï1}wx 2 dx 5 E(x
3
d x3
}} }} 2 x 2 1 x 1 C 5 x 2 2 2x 1 1
dx 3
1
2
E
2. (23x 24) dx 5 x 23 1 C
Check:
d
}}(x 23 1 C) 5 23x 24
dx
E
E
x3
8
(x 2 2 4Ïwx) dx 5 (x 2 2 4x 1/2) dx 5 }} 2 }}x 3/2 1 C
3
3
Check:
1
2
8
d x3
}} }} 2 }}x 3/2 1 C 5 x 2 2 4x 1/2 5 x 2 2 Ïxw
3
dx 3
E
3
4
3
2
E 13
13. }}x 22/3 dx 5 x 1/3 1 C
E
cos 3x
3
p
E p2 1 p2 2
12 2
16. E2 sec t tan t dt 5 2 sec t 1 C
1
2
17. E }} 1 }} dx 5 2 ln )x 2 1) 1 ln )x) 1 C
1x 2 1 x 2
1
18. E }} 1 sin 5x 2 e
1x 2 2
2 dx
15. }} cos }} x dx 5 sin }} x 1 C
22x
cos 5x
5
E
20. Ecsc
19. 5 sec 2 5r dr 5 tan 5r 1 C
2
Ecos
d
}}(8x 2 csc x 1 C) 5 8 1 csc x cot x
dx
1
4
5. e 4x dx 5 }}e 4x 1 C
Check:
2
d 1
}} }}e 4x 1 C 5 e 4x
dx 4
e 2 2x
2
5 ln )x 2 2) 2 }} 1 }} 1 C
21.
Check:
1
1 x 21/3) dx
5 }}x 4/3 1 }}x 2/3 1 C
4. (8 1 csc x cot x) dx 5 8x 2 csc x 1 C
E
1/3
3
14. (3 sin x 2 sin 3x) dx 5 23 cos x 2 }} 1 C
Check:
3.
x4
x22
4
2
x4
1
5 }} 1 }}2 1 C
4
2x
5 }} 1 }} 1 C
By setting the right endpoint at x 5 20.01 instead of x 5 0,
to calculate NINT }}, x, 21, 0 . The graph appears to be
E
2 }}3 dx 5 (x 3 2 x23) dx
3
cot 7t
7
7t dt 5 2}} 1 C
2
E 1 1 c2os 2x
1
cos 2x
5 E1}} 1 }}2 dx
2
2
x dx 5 }} dx
x
2
sin 2x
4
5 }} 1 }} 1 C
E
E 1 2 c2os 2x
1
cos 2x
sin 2x
x
5 E }} 2 }} dx 5 }} 2 }} 1 C
12 2 2 2 4
23. Etan u du 5 E(sec u 2 1) du 5 tan u 2 u 1 C
22. sin 2 x dx 5 }} dx
2
2
233
234
Section 6.1
E
E
24. cot 2 t dt 5 (csc 2 t 2 1) dt 5 2cot t 2 t 1 C
29.
E}dd}yx dx 5 Esec
25. (a) Graph (b)
(b) The slope is always positive, so (a) and (c) can be ruled
out.
2
x dx
y 5 tan x 1 C
142
p
Initial condition: y }} 5 21
26. (a) Graph (b)
p
4
21 5 tan }} 1 C
(b) The solution should have positive slope when x is
27.
dy
}} 5 sec 2 x
dx
negative, zero slope when x is zero and negative slope
21 5 1 1 C
dy
when x is positive since slope 5 }} 5 2x. Graphs (a)
dx
22 5 C
and (c) don’t show this slope pattern.
Solution: y 5 tan x 2 2
dy
}} 5 2x 2 1
dx
E}dd}yx dx 5 E(2x 2 1) dx
y 5 x2 2 x 1 C
Initial condition: y(2) 5 0
0 5 22 2 2 1 C
0521C
22 5 C
Solution: y 5 x 2 2 x 2 2
32}2}, }2}4 by [28, 8]
p p
30.
dy
}} 5 x 22/3
dx
E}dd}yx dx 5 Ex
22/3
dx
y 5 3x 1/3 1 C
Initial condition: y(21) 5 25
25 5 3(21)1/3 1 C
25 5 23 1 C
22 5 C
y 5 3x 1/3 2 2
[24, 4] by [23, 3]
28.
dy
1
}} 5 }}2 1 x
dx
x
E}dd}yx dx 5 E(x
22
1 x) dx
x2
2
y 5 2x 21 1 }} 1 C
x2
2
[24, 4] by [28, 4]
1
x
y 5 }} 2 }} 1 C
Initial condition: y(2) 5 1
22
1
2
2
3
1 5 }} 1 C
2
1
2}} 5 C
2
x2
1
1
Solution: y 5 }} 2 }} 2 }}
2
x
2
1 5 }} 2 }} 1 C
[26, 6] by [24, 4]
31.
dy
}} 5 9x 2 2 4x 1 5
dx
E}dd}yx dx 5 E(9x
2
2 4x 1 5) dx
y 5 3x 3 2 2x 2 1 5x 1 C
Initial condition: y(21) 5 0
0 5 3(21)3 2 2(21)2 1 5(21) 1 C
0 5 210 1 C
10 5 C
Solution: y 5 3x 3 2 2x 2 1 5x 1 10
Section 6.1
32.
dy
}} 5 cos x 1 sin x
dx
35.
E}dd}yx dx 5 E(cos x 1 sin x) dx
E
y 5 sin x 2 cos x 1 C
Initial condition: y(p) 5 1
1 5 sin p 2 cos p 1 C
1511C
05C
Solution: y 5 sin x 2 cos x
33.
2t
0 5 2cos 0 1 C1
0 5 21 1 C1
1 5 C1
dy
du
First derivative: }} 5 2cos u 1 1
dt
E}dd}uy du 5 E(2cos u 1 1) du
y 5 22e 2t 1 C
Initial condition: y(ln 2) 5 0
y 5 2sin u 1 u 1 C2
0 5 22e 2ln 2 1 C
Initial condition: y(0) 5 23
2
0 5 2}} 1 C
2
23 5 2sin 0 1 0 1 C2
15C
23 5 C2
Solution: y 5 22e 2t 1 1
34.
E
Initial condition: y9(0) 5 0
dy
}} 5 2e 2t
dt
E}dd}yt dt 5 E2e
d 2y
}}2 5 sin u
du
d 2y
}}2 du 5 sin u du
du
dy
}} 5 2cos u 1 C1
du
dy
1
}} 5 }}
dx
x
E}dd}yx dx 5 E}1x} dx
y 5 ln )x) 1 C
Initial condition: y(e 3) 5 0
0 5 ln (e 3) 1 C
0 531C
23 5 C
Solution: y 5 ln )x) 2 3
Solution: y 5 2sin u 1 u 2 3
36.
d 2y
}}2 dx 5 2 2 6x
dx
d 2y
}}2 dx 5 (2 2 6x) dx
dx
dy
}} 5 2x 2 3x 2 1 C1
dx
E
E
Initial condition: y9(0) 5 4
4 5 2(0) 2 3(0)2 1 C1
4 5 C1
dy
dx
First derivative: }} 5 2x 2 3x 2 1 4
E}dd}yx dx 5 E(2x 2 3x
2
1 4) dx
y 5 x 2 2 x 3 1 4x 1 C2
Initial condition: y(0) 5 1
1 5 02 2 03 1 4(0) 1 C2
1 5 C2
Solution: y 5 x 2 2 x 3 1 4x 1 1
or y 5 2x 3 1 x 2 1 4x 1 1
235
236
Section 6.1
d 3y
1
dt
t
d 3y
dt5 t 2 3 dt
}}
dt 3
d 2y
1
5 2}}t 2 2 1 C1
}}
dt 2
2
37. }}3 5 }}3
E
38.
E
23 5 21 1 C1
22 5 C1
d 3y
du
Third derivative: }}3 5 2cos u 1 sin u 2 2
d 2y
dt
1
2
5
2
Second derivative: }}2 5 2}}t 2 2 1 }}
E1
2 dt
d 2y
1
5
dt5 2}}t 2 2 1 }}
}}
dt 2
2
2
dy
1 21
5
1 }}t 1 C2
}} 5 }}t
dt
2
2
E}ddu}y du 5 E(2cos u 1 sin u 2 2) du
3
3
d 2y
}}2 5 2sin u 2 cos u 2 2u 1 C2
du
Initial condition: y0(0) 5 21
21 5 2sin 0 2 cos 0 2 2(0) 1 C2
Initial condition: y9(1) 5 3
21 5 21 1 C2
5
2
3 5 }}(1)21 1 }}(1) 1 C2
0 5 C2
3 5 3 1 C2
d 2y
du
Second derivative: }}2 5 2sin u 2 cos u 2 2u
0 5 C2
E}ddu}y du 5 E(2sin u 2 cos u 2 2u) du
2
2
dy
dt
1
2
5
2
First derivative: }} 5 }}t 2 1 1 }}t
E}dd}yt dt 5 E1}12}t
1
2
E
23 5 2cos 0 1 sin 0 1 C1
1
2
1
2 5 2}} 1 C1
2
5
}} 5 C1
2
2 5 2}}(1)22 1 C1
1
2
E
Initial condition: y (3)(0) 5 23
Initial condition: y0(1) 5 2
E
d 4y
}}4 5 sin u 1 cos u
du
d 4y
}}4 du 5 (sin u 1 cos u) du
du
d 3y
}}3 5 2cos u 1 sin u 1 C1
du
21
5
2
2
1 }}t dt
5
4
y 5 }}ln )t) 1 }}t 2 1 C3
Initial condition: y(1) 5 1
1
5
2
4
5
1 5 } } 1 C3
4
1
2}} 5 C3
4
1
5
1
Solution: y 5 }} ln )t) 1 }}t 2 2 }}
2
4
4
1 5 }} ln 1 1 }}(1)2 1 C3
dy
}} 5 cos u 2 sin u 2 u 2 1 C3
du
Initial condition: y9(0) 5 21
21 5 cos 0 2 sin 0 2 02 1 C3
21 5 1 1 C3
22 5 C3
dy
du
First derivative: }} 5 cos u 2 sin u 2 u 2 2 2
E}dd}uy du 5 E(cos u 2 sin u 2 u
2
2 2) du
u
3
3
y 5 sin u 1 cos u 2 }} 2 2u 1 C4
Initial condition: y(0) 5 23
03
3
23 5 sin 0 1 cos 0 2 }} 2 2(0) 1 C4
23 5 1 1 C4
24 5 C4
u3
3
Solution: y 5 sin u 1 cos u 2 }} 2 2u 2 4
ds
dt
ds
}} dt 5 (9.8t 1 5) dt
dt
39. }} 5 v 5 9.8t 1 5
E
E
s 5 4.9t 1 5t 1 C
2
Initial condition: s(0) 5 10
10 5 4.9(0)2 1 5(0) 1 C
10 5 C
Solution: s 5 4.9t 2 1 5t 1 10
Section 6.1
ds
dt
ds
}} dt 5 sin pt dt
dt
1
s 5 2}} cos pt 1 C
p
40. }} 5 v 5 sin pt
E
E
dv
dt
dv
}} dt 5 cos t dt
dt
42. }} 5 a 5 cos t
E
E
v 5 sin t 1 C1
Initial condition: s(1) 5 0
Initial condition: v(0) 5 21
1
0 5 2}} cos p 1 C
p
1
0 5 }} 1 C
p
1
2}} 5 C
p
1
1
Solution: s 5 2}} cos pt 2 }}
p
p
1
or s 5 2}}(1 1 cos pt)
p
21 5 sin 0 1 C1
dv
dt
dv
}} dt 5
dt
21 5 C1
ds
dt
Velocity: }} 5 v 5 sin t 2 1
E}dd}st dt 5 E(sin t 2 1) dt
s 5 2cos t 2 t 1 C2
Initial condition: s(0) 5 1
41. }} 5 a 5 32
E
1 5 2cos 0 2 0 1 C2
E 32 dt
1 5 21 1 C2
v 5 32t 1 C1
2 5 C2
Initial condition: v(0) 5 20
20 5 32(0) 1 C1
20 5 C1
Solution: s 5 2cos t 2 t 1 2
43.
ds
dt
Velocity: }} 5 v 5 32t 1 20
E}dd}st dt 5 E(32t 1 20) dt
s 5 16t 2 1 20t 1 C2
[22, 2] by [23, 3]
44.
Initial condition: s(0) 5 0
0 5 16(0)2 + 20(0) 1 C2
050
Solution: s 5 16t 2 1 20t
[22, 3] by [23, 3]
d
dx
1
11x
45. }}(tan 21 x 1 C) 5 }}2
1
d
dx
46. }}(sin 21 x 1 C) 5 }}
2wx 2w
Ï1ww
d
dx
1
47. }}(sec 21 x 1 C) 5 }}
)x)Ïw
x 2w
2w1
1
d
dx
48. }}(2cos 21 x 1 C) 5 }}
2wx 2w
Ï1ww
dy
1
dx
x
dy
}} dx 5 (x 2 x 22) dx
dx
x2
x2
1
y 5 }} 1 x 21 1 C 5 }} 1 }} 1 C
2
2
x
49. (a) }} 5 x 2 }}2
E
E
Initial condition: y(1) 5 2
12
1
2
1
3
2 5 }} 1 C
2
1
}} 5 C
2
2 5 }} 1 }} 1 C
x2
2
1
x
1
2
Solution: y 5 }} 1 }} 1 }}, x . 0
237
238
Section 6.1
49. continued
52. (a)
x2
1
(b) Again, y 5 }} 1 }} 1 C.
2
x
Initial condition: y(21) 5 1
(21)2
1
2
(21)
1
1 5 2}} 1 C
2
3
}} 5 C
2
x2
1
3
Solution: y 5 }} 1 }} 1 }}, x , 0
2
x
2
1 5 }} 1 }} 1 C
1
x2
d 1
2
dx x
1
5 2}}2 1 x
x
1
5 x 2 }}2 .
x
dy
x2
d 1
For x . 0, }} 5 }} }} 1 }} 1 C2
dx
2
dx x
1
5 2}}2 1 x
x
1
5 x 2 }}2 .
x
dy
And for x 5 0, }} is undefined.
dx
dy
dx
(c) For x , 0, }} 5 }} }} 1 }} 1 C1
1
E[2f (x)] dx 5 2Ef (x) dx 5 2x e
(d)
E[2g(x)] dx 5 2Eg(x) dx 5 2x sin x 1 C
(e)
E[ f (x) 1 g(x)] dx 5 Ef (x) dx 1 Eg(x) dx
2 x
1C
5 x 2e x 1 x sin x 1 C
(f)
E[ f (x) 2 g(x)] dx 5 Ef (x) dx 2 Eg(x) dx
5 x 2e x 2 x sin x 1 C
2
(g)
E[x 1 f (x)] dx 5 Ex dx 1 Ef (x) dx 5 }x2} 1 x e
(h)
E[g(x) 2 4] dx 5 Eg(x) dx 2 E4 dx 5 x sin x 2 4x 1 C
2
E}ddt}s dt 5 E2k dt
2
53. (a)
2
ds
}} 5 2kt 1 C1
dt
ds
dt
1
2
Initial condition: }} 5 88 when t 5 0
88 5 (2k)(0) 1 C1
y(22) 5 2
88 5 C1
1
22
(22)2
1
2 5 }} 1 }} 1 C1
2
2
2
(22)
5
3
21 5 }} 1 C2
2 5 } } 1 C1
2
2
7
1
2}} 5 C2
}} 5 C1
2
2
1
7
Thus, C1 5 }} and C2 5 2}}.
2
2
21 5 }} 1 }} 1 C2
ds
dt
Velocity: }} 5 2kt 1 88
E}dd}st dt 5 E(2kt 1 88) dt
k
2
s 5 2}}t 2 1 88t 1 C2
Initial condition: s 5 0 when t 5 0
E
dr
}} dx 5 (3x 2 2 6x 1 12) dx
dx
k
2
0 5 2}}(0)2 1 88(0) 1 C2
r 5 x 3 2 3x 2 1 12x 1 C
0 5 C2
Initial condition: r(0) 5 0
Solution: s 5 2}} 1 88t
kt 2
2
0 5 03 2 3(0)2 1 12(0) 1 C
(b)
05C
88
k
t 5 }}
E
51. }} dx 5 (3x 2 2 12x 1 15) dx
c 5 x 3 2 6x 2 1 15x 1 C
Initial condition c(0) 5 400
400 5 03 2 6(0)2 1 15(0) 1 C
400 5 C
Solution: c(x) 5 x 3 2 6x 2 1 15x 1 400
ds
}} 5 0
dt
2kt 1 88 5 0
Solution: r(x) 5 x 3 2 3x 2 1 12x
E ddcx
1C
(c)
2
3
2
E
2 x
Eg(x) dx 5 E}dd}x (x sin x) dx 5 x sin x 1 C
value from part (a). Thus, C1 5 }} and C2 5 }}.
50.
2 x
(b)
(d) Let C1 be the value from part (b), and let C2 be the
(e) y(2) 5 21
Ef (x) dx 5 E}dd}x (x e ) dx 5 x e
(c)
1k2
88
k 88
2}} }} 1 88 }} 5 242
1k2
21 k 2
88
s }} 5 242
2
3872
}} 5 242
k
k 5 16 ft/sec 2
2 x
1C
Section 6.1
d 2s
dt
54. We first solve }}2 5 2k with the initial conditions
d 2s
dt
56. Solving }}2 5 a, s(0) 5 s0, and v(0) 5 v0:
E}ddt}s dt 5 Ea dt
2
s9(0) 5 44 and s(0) 5 0.
2
E
d 2s
dt 5 2k
}}
dt 2
ds
}} 5 2kt 1 C1
dt
ds
}} 5 at 1 C1
dt
Initial condition: s9(0) 5 44
v0 5 (a)(0) 1 C1
44 5 (2k)(0) 1 C1
v0 5 C1
44 5 C1
Velocity: }} 5 at 1 v0
Initial condition: s9(0) 5 v0
ds
dt
E}dd}st dt 5 E(at 1 v ) dt
ds
dt
Velocity: }} 5 2kt 1 44
0
E}dd}st dt 5 E(2kt 1 44) dt
a
s 5 }}t 2 1 v0t 1 C2
2
k
2
s 5 2}}t 2 1 44t 1 C2
Initial condition: s(0) 5 s0
Initial condition: s(0) 5 0
s0 5 }}(0)2 1 (v0 )(0) 1 C2
a
2
k
2
0 5 2}}(0)2 1 44(0) 1 C2
s0 5 C2
0 5 C2
Position: s 5 }}t 2 1 v0t 1 s0
a
2
k
2
Position: s 5 2}}t 2 1 44t
ds
dt
44
k
Now, }} 5 2kt 1 44 5 0 when t 5 }}, so it takes
44
}} seconds to stop, and we require:
k
1 2
1 2
44
s }} 5 45
k
It requires a constant deceleration of approximately
21.5 ft/sec 2.
1 2 2
3 5
d 4p
5 }} }}h 3
dt 75
4p dh
5 }}h 2}}
25 dt
dh
5 h 3/2 }}
dt
3/2 dh
5 h }} dt
dt
2
5 }}h 5/2 1 C
5
1 2
1 2
4p
75
E
E
Initial condition: h 5 10 when t 5 0.
25
24p
2
5
2}}(0) 5 }}(10)5/2 1 C
E
55. }}2 dt 5 25.2 dt
2
5
C 5 2}}(10)5/2
ds
}} 5 25.2t 1 C1
dt
ds
dt
Initial condition: }} 5 0 when t 5 0
0 5 25.2(0) 1 C1
0 5 C1
2
2
25
5
5
24p
125t
5/2
2}} 5 h 2 10 5/2
48p
125t
h5/2 5 2}} 1 105/2
48p
2/5
125t
h 5 2}} 1 105/2
48p
2/5
125t
The height is given by h 5 2}} 1 105/2
and the
48p
2}}t 5 }}h 5/2 2 }}(10)5/2
1
ds
dt
Velocity: }} 5 25.2t
E
25
24p
25
2 }} dt
24p
25
2}}t
24p
2}}
968
k 5 }} < 21.5
45
2
dV
}}
dt
1
6
968
}} 5 45
k
E ddt s
1
3
V 5 }}pr 2h 5 }}p }}h h 5 }}h 3
2}}Ïhw
44
k 44 2
2}} }} 1 44 }} 5 45
k
2 k
1 2
57. We use the method of Example 7.
E
ds
}} dt 5 25.2 dt
dt
s 5 22.6t 2 1 C2
Initial condition: s 5 4 when t 5 0
1
2
volume is given by
4p
75
4p
75
1
125t
48p
V 5 }}h 3 5 }} 2}} 1 105/2
4 5 22.6(0)2 1 C2
4 5 C2
Position: s(t) 5 22.6t 2 1 4
4
2.6
Solving s(t) 5 0, we have t 2 5 }}, so the positive
solution is t < 1.240 sec. They took about 1.240 sec to fall.
2
6/5
2
.
239
240
Section 6.1
58. (a) y 5 500e 0.0475t
63. Use differential equation graphing mode.
For reference, the equations of the solution curves are as
follows.
(1, 1): y 5 e (x 21)/2
(21, 2): y 5 2e (x 21)/2
(0, 22): y 5 22e x /2
(22, 21): y 5 2e (x 24)/2
(b) 1000 5 500e 0.0475t
25e
2
0.0475t
2
2
ln 2 5 0.0475t
2
ln 2
0.0475
t 5 }} < 14.6
It will take approximately 14.6 years.
59. (a) y 5 1200e 0.0625t
[26, 6] by [24, 4]
(b) 3600 5 1200e 0.0625t
The concavity of each solution curve indicates the sign of
y0.
3 5 e 0.0625t
ln 3 5 0.0625t
ln 3
0.0625
t 5 }} < 17.6
It will take approximately 17.6 years.
60. (a)
Ex
2
cos x dx 5
Et
0
(b) We require
Et
x
0
2
cos t dt 1 C
cos t dt 1 C 5 1, so C 5 1.
2
0
Et
x
The required antiderivative is
cos t dt 1 1.
2
0
61. (a)
Exe
x
dx 5
E te dt 1 C
x
t
E te dt 1 C 5 1, so C 5 1.
The required antiderivative is E te dt 1 1.
0
t
0
x
t
0
E}ddx}y dx 5 E6x dx
2
62. (a)
[24, 4] by [23, 3]
The concavity of each solution curve indicates the sign of
y0.
0
(b) We require
64. Use differential equation graphing mode.
For reference, the equations of the solution curves are as
follows.
(0, 1): y 5 e x
(0, 2): y 5 2e x
(0, 21): y 5 2e x
2
65. Use differential equation graphing mode.
For reference, the equations of the solution curves are as
follows.
(0, 1): y 5 23e 2x 1 4
(0, 4): y 5 4
(0, 5): y 5 e 2x 1 4
dy
}} 5 3x 2 1 C1
dx
Initial condition (horizontal tangent): y9(0) 5 0
0 5 3(0)2 1 C1
[23, 3] by [24, 10]
0 5 C1
dy
dx
First derivative: }} 5 3x 2
E}dd}yx dx 5 E3x
2
dx
y 5 x 3 1 C2
Initial condition (contains (0, 1)): y(0) 5 1
1 5 (0)3 1 C2
1 5 C2
Solution: y 5 x 3 1 1
(b) Only one function satisfies the differential equation on
(2`, `) and the initial conditions.
The concavity of each solution curve indicates the sign of
y0.
Section 6.2
66. Use differential equation graphing mode.
241
2
3
3. y1 5 y2 1 }}. By Corollary 3 to the Mean Value Theorem of
For reference, the equations of the solution curves are as
Section 4.2, y1 and y2 must differ by a constant. We find
follows.
that constant by evaluating the two functions at x 5 0.
1
(0, 1): y 5 2}}
x21
2
(0, 2): y 5 2}}
2x 2 1
1
(0, 21): y 5 2}}
x11
(0, 0): y 5 0
[23, 3] by [22, 8]
4.
[22.35, 2.35] by [21.55, 1.55]
[210, 10] by [230, 30]
The concavity of each solution curve indicates the sign of
y0.
1
x
d
dx
67. (a) }}(ln x 1 C) 5 }} for x . 0
d
dx
5. The derivative with respect to x of each function graphed in
part (4) is equal to Ï1ww
1wx 2w.
Exploration 2 Two Routes to the Integral
1 2
1 d
2x dx
1
2x
1
x
(b) }}[ln (2x) 1 C] 5 }} }} (2x) 5 }} (21) 5 }}
for x , 0
E
1
1.
21
E
E
3x 2Ïw
x 3w
1w1 dx 5
E Ïuw du 5 }23}u 4
2
3/2
0
E
2
3
4Ï2w
5 }}
3
0
2
3
4Ïw2
5 }}.
3
2. 3x 2Ïw
x 3w
1w1 dx 5 Ïuw du 5 }}u3/2 5 }}(x 3 1 1)3/2 so
1
(c) For x . 0, ln )x) 1 C 5 ln x 1 C, which is a solution
to the differential equation, as we showed in part (a).
For x , 0, ln )x) 1 C 5 ln (2x) 1 C, which is a
21
0
part (b). Thus, }} ln )x) 5 }} for all x except 0.
4
1
5
dy
dx
1
x
■ Section 6.2 Integration by Substitution
1
5
40
5
1
1
5
32
5
1/2
1
2
3
2
2
3
3
2
16
5 }}(8) 5 }}
3
3
dy
dx
3. }} 5 3x
dy
dx
4. }} 5 3x
dy
dx
5. }} 5 4(x 3 2 2x 2 1 3)3(3x 2 2 4x)
(pp. 315–323)
Exploration 1 Supporting Indefinite Integrals
Graphically
EÏ1ww1wxw ? 2x dx 5 EÏuw du
2
2
5 }}u3/2 1 C
3
2
5 }}(1 1 x 2)3/2 1 C
3
dy
dy
dx
dx
2. Their derivatives are equal: }}1 5 }}2 5 Ï1
ww
1wx 2w ? 2x.
dy
dx
6. }} 5 2 sin (4x 2 5) cos (4x 2 5) ? 4
5 8 sin (4x 2 5) cos (4x 2 5)
dy
dx
1
cos x
dy
dx
1
sin x
7. }} 5 }} ? 2sin x 5 2tan x
8. }} 5 }} ? cos x 5 cot x
5
41
dx 5 }}(x 2 1)3/2
5 }}(4)3/2 2 }}(0)3/2
part (a). For x . 0, we have y 5 ln x 1 C1, which is a
part (b). Thus, }} 5 }} for all x except 0.
2
E Ïxw2ww1 dx 5 E (x 2 1)
solution to the differential equation, as we showed in
solution to the differential equation, as we showed
1
421
dx 5 }}x 5 5 }}(2)5 2 }}(0)5 5 }}
5
2.
(d) For x , 0, we have y 5 ln (2x) 1 C2, which is a
Ex
2
1.
1
x
d
dx
2
3
3x 2Ïw
x 3w
1w1 dx 5 }}(x 3 1 1)3/2
Quick Review 6.2
solution to the differential equation, as we showed in
1.
2
242
Section 6.2
dy
dx
4. u 5 7x 2 2
1
sec x 1 tan x
sec x tan x 1 sec2 x
5 }}}
sec x 1 tan x
sec x(tan x 1 sec x)
5 }}}
sec x 1 tan x
9. }} 5 }} ? (sec x tan x 1 sec2 x)
du 5 7 dx
1
}} du 5 dx
7
E28(7x 2 2)
5 sec x
dy
dx
1
7
d
Check: }}[(7x 2 2)4 1 C] 5 4(7x 2 2)3(7) 5 28(7x 2 2)3
dx
1
csc x 1 cot x
csc x cot x 1 csc2 x
5 2}}}
csc x 1 cot x
csc x(cot x 1 csc x)
5 2}}}
csc x 1 cot x
10. }} 5 }}(2csc x cot x 2 csc2 x)
x
3
5. u 5 }}
1
3
du 5 }} dx
3 du 5 dx
3u
dx
E}
} 5 E}}
x 19
9u 1 9
du
3
5 } } E }}
9 u 11
1
du
5 }}E}}
3 u 11
5 2csc x
2
Section 6.2 Exercises
2
2
1. u 5 3x
2
du 5 3 dx
1
}}du 5 dx
3
1
3
1
5 2}} cos 3x 1 C
3
1
1
d
Check: }} 2}} cos 3x 1 C 5 2}}(2sin 3x)(3) 5 sin 3x
3
dx 3
5 2}} cos u 1 C
1
1
5 }} tan21 u 1 C
3
1
x
5 }} tan21 }} 1 C
3
3
1
1
d 1
x
Check: }} }} tan21 }} 1 C 5 }} }2
3 11 x
dx 3
3
}}
12
Esin 3x dx 5 }13}Esin u du
2
1
2
132
1
1
}
? }3} 5 }
9 1 x2
6. u 5 12 r 3
du 5 23r 2 dr
1
3
9r2 dr
1
}} 5 9 2}}
3
3
2wr w
Ï1ww
2}} du 5 r 2 dr
2. u 5 2x 2
E
du 5 4x dx
1 2E}Ï}wu
E
Ex cos (2x ) dx 5 }14}Ecos u du
5 23(2)u1/2 1 C
2
1
4
1
5 }} sin (2x 2) 1 C
4
1
d 1
Check: }} }}sin (2x 2) 1 C 5 }}cos (2x 2)(4x) 5 x cos (2x2)
4
dx 4
5 26Ï1ww
2wr 3w 1 C
5 }} sin u 1 C
1
du
5 23 u21/2 du
1
4
x dx 5 }} du
2
3. u 5 2x
d
1
1
9r
2
5 }}
2wr3w
Ï1ww
t
2
1
2
Esec 2x tan 2x dx 5 }12}Esec u tan u du
1
2
1
5 }} sec 2x 1 C
2
1
d 1
Check: }} }}sec 2x 1 C 5 }}sec 2x tan 2x
2
dx 2
E1
5 }} sec u 1 C
1
t
2
t
2 du 5 sin }} dt
2
t 2
t
1 2 cos }} sin }} dt5 2 u2 du
2
2
2
5 }}u3 1 C
3
2
t 3
5 }} 1 2 cos }} 1 C
3
2
d 2
t 3
Check: }} }} 1 2 cos }} 1 C
dx 3
2
t 2
t 1
5 2 1 2 cos }} sin }} }}
2
2 2
t 2
t
5 1 2 cos }} sin }}
2
2
du 5 }}sin }} dt
1
}} du 5 dx
2
2
? 2 5 sec 2x tan
2
2wr 3w 1 C) 5 26 }} (23r 2)
Check: }}(26Ï1ww
dx
2wr 3w
2Ï1
ww
7. u 5 1 2 cos }}
du 5 2 dx
2x
E
dx 5 }} 28u3 du 5 u4 1 C 5 (7x 2 2)4 1 C
3
E
2
1
31
1
1
21
2
2 4
21 2
2
Section 6.2
14. Let u 5 tan x
8. u 5 y 4 1 4y 2 1 1
du 5 (4y 3 1 8y) dy
du 5 sec2 x dx
du 5 4(y 3 1 2y) dy
E8(y
4
E
p/4
1
}} du 5 (y 3 1 2y) dy
4
tan2 x sec2 x dx 5
2p/4
1 4 2E
E
1
3
3
4
5 }}u3
2
5 }}u3 1 C
3
2
5 }}(y 4 1 4y 2 1 1)3 1 C
3
1
21
1
1
5 }}(1) 2 }}(21)3
3
3
4
d 2
dx 3
u2 du
21
1
1 4y 2 1 1)2(y 3 1 2y) dy 5 8 }} u2 du
1
Check: }} }}(y 4 1 4y 2 1 1)3 1 C
1
3
1
3
2
3
5 }} 1 }} 5 }}
5 2(y 4 1 4y 2 1 1)2(4y 3 1 8y)
15. Let u 5 3z 1 4
5 8(y 4 1 4y 2 1 1)2(y 3 1 2y)
du 5 3 dz
9. Let u 5 1 2 x
1
}} du 5 dz
3
du 5 2dx
E
Ecos (3z 1 4) dz 5 }13}Ecos u du
E
du
dx
}}2 5 2 }}2
u
(1 2 x)
1
3
1
5 }}sin (3z 1 4) 1 C
3
5 }}sin u 1 C
5 u21 1 C
1
12x
5 }} 1 C
16. Let u 5 cot x
10. Let u 5 x 1 2
du 5 2csc2 x dx
du 5 dx
Esec
2
EÏcowtwxw csc
2
E
(x 1 2) dx 5 sec u du
2
E
x dx 5 2 u1/2 du
2
3
2
5 2}}(cot x)3/2 1 C
3
5 2}}u3/2 1 C
5 tan u 1 C
5 tan (x 1 2) 1 C
17. Let u 5 ln x
11. Let u 5 tan x
du 5 sec x dx
EÏtawnwwx sec
2
E}lnx}x dx 5 Eu
6
E
x dx 5 u
1/2
du
2
3
2
5 }}(tan x)3/2 1 C
3
du 5 du
Esec 1u 1 }p2}2 tan 1u 1 }p2}2 du 5 Esec u tan u du
5 sec u 1 C
p
2
2
5 sec u 1 }} 1 C
13. Let u 5 ln x
1
x
6
dx
}} 5
e x ln x
E
E
ln 6
1
du
}} 5 ln )u)
u
ln 6
41
5 ln (ln 6)
du
x
2
1
x
du 5 }}sec2}} dx
2
2
x
x
tan7 }} sec2 }} dx 5 2 u7 du
2
2
1
5 2 ? }}u8 1 C
8
1
x
5 }} tan8 }} 1 C
4
2
18. Let u 5 tan }}
p
12. Let u 5 u 1 }}
2
1
6
1
5 }}u7 1 C
7
1
5 }}(ln7 x) 1 C
7
5 }}u3/2 1 C
du 5 }} dx
1
x
du 5 }} dx
2
E
E
243
244
Section 6.2
19. Let u 5 s4/3 2 8
4
du 5 }}s1/3 ds
3
3
}}du 5 s1/3 ds
4
Es
p/4
E
3p/4
cot x dx 5
p/4
E
3
4
3
5 }} sin u 1 C
4
3
5 }} sin(s4/3 2 8) 1 C
4
du 5 cos x dx
E
3p/4
p/4
E
cos x
}} dx 5
sin x
E sindx3x E
20. }2} 5 csc2 3x dx
x53p/4
1
}} du
x 5 p/4 u
5 ln )u)
5 ln )sin x)
du 5 3 dx
1
}} du 5 dx
3
2
x 5 3p/4
4
x 5 p/4
Let u 5 3x
Ecsc
cos x
}} dx
sin x
Let u 5 sin x
cos (s4/3 2 8) ds 5 }} cos u du
1/3
E
3p/4
23.
1
3
1
3
1
5 2}} cot (3x) 1 C
3
)2)
du 5 dx
1
dx
E}
} 5 E }} du
u
x12
9
0
2
5 ln u
du 5 2sin (2t 1 1)(2) dt
1
2
1
sin (2t 1 1)
}
} dt 5 2}} u22 du
2
cos2 (2t 1 1)
1
5 }}u21 1 C
2
1
5 }} 1 C
2 cos (2t 1 1)
1
5 }}sec (2t 1 1) 1 C
2
E
25. Let u 5 x 2 1 1
du 5 2x dx
1
2
x dx 5 }} du
E
E
3
x dx
1
}
2 } 5 }}
2
21 x 1 1
22. Let u 5 2 1 sin t
1
2
du 5 cos t dt
10
2
1
}} du
u
22
du
5 26u21 1 C
6
2 1 sin t
5 2}} 1 C
1
2
10
42
5 }}ln )u)
6 cos t
E}
} dt 5 6Eu
(2 1 sin t)
2
9
42
5 ln 9 2 ln 2 < 1.504
2}}du 5 sin (2t 1 1) dt
E
)2)
24. Let u 5 x 1 2
7
21. Let u 5 cos (2t 1 1)
4p/4
Ïw2
Ï2w
5 ln }} 2 ln }} 5 0
E
3x dx 5 }} csc2 u du
5 2}} cot u 1 C
3p/4
1
2
5 }}(ln 10 2 ln 2) 5 }}ln 5 < 0.805
Section 6.2
E
5
40 dx
26. }
2 }5
0 x 1 25
E
E }}
dx
25
x
2
1}5}2
0
E
25
1 25 2
1 }}
5
2
2
1
40
dx
5 }} }
2
0
x
}}
5
12
x 1 cot x
E 1 csc
csc x 1 cot x 2
csc x 1 csc x cot x
5 E}}} dx
csc x 1 cot x
30. csc x dx 5 csc x }} dx
40
}}
25
5
Let u 5 csc x 1 cot x
11
du 5 2csc x cot x 2 csc2 x dx
x
5
Let u 5 }}
Ecsc x dx 5 2E}1u} du
1
5
du 5 }} dx
5 2ln )u) 1 C
5 du 5 dx
8
1
40 dx
E}
} 5 }}(5)E }} du
5
x 1 25
u 11
5
0
1
2
0
5 2ln )csc x 1 cot x) 1 C
2
5 8 arctan u
1
40
5 8(arctan 1)
31. Let u 5 y 1 1
du 5 dy
E Ïyw1ww1 dy 5 E u
3
p
4
1 2
5 8 }} 5 2p
4
0
Let u 5 cos 3x
du 5 23 sin 3x dx
2}} du 5 sin 3x dx
E
E}1u} du
du 5 22r dr
ln )u) 1 C
ln )cos 3x) 1 C
1
3
1
2
2}} du 5 r dr
E rÏ1ww2wrw dr 5 2}12}E u
1
0
2
0
1/2
du
1
0
1 2
2 3
1
1
1
1
5 2}}(0) 1 }}(1) 5 }}
3
3
3
4
5 2}} ? }}u3/2
28. Let u 5 5x 1 8
du 5 5 dx
1
}} du 5 dx
5
dx
1
}} 5 }} u21/2 du
5
xw
Ïw5w
1w8
1
5 }} ? 2u1/2 1 C
5
2
5 }}Ï5wxw1
ww8 1 C
5
E
4
32. Let u 5 1 2 r 2
(An equivalent expression is }} ln )sec 3x) 1 C.)
E
du
4
2
3
1
2 3/2
2
5 }}(4) 2 }}(1)3/2
3
3
2
2
14
5 }}(8) 2 }} 5 }}
3
3
3
5 }}u3/2
E codtx3x E csoins 33xx
27. }} 5 }} dx
1
3
1
dx
}} 5 2 } }
3
cot 3x
1
5 2 }}
3
1
5 2 }}
3
1/2
1
E
33. Let u 5 tan x
du 5 sec2 x dx
E
0
tan x sec2 x dx 5
2p/4
u du
21
1
2
x 1 tan x
E 1 sec
sec x 1 tan x 2
sec x 1 sec x tan x
5 E}}} dx
sec x 1 tan x
0
421
1
2
1
2
5 }}(0) 2 }}(21)2
2
1
2
5 2}}
Let u 5 sec x 1 tan x
Esec x dx 5 E}1u} du 5 ln )u) 1 C 5 ln )sec x 1 tan x) 1 C
0
5 }}u2
29. sec x dx 5 sec x ? }} dx
du 5 sec x tan x 1 sec2 x dx
E
34. Let u 5 4 1 r 2
du 5 2r dr
1
}} du 5 r dr
21
5
5r
}}
2 2 dr 5 }}
2
21 (4 1 r )
E
Eu
5
5
22
du 5 0
245
246
Section 6.2
35. Let u 5 1 1 u3/2
dy
dx
dy
}} 5 (x 1 2)dx
y15
39. }} 5 (y 1 5)(x 1 2)
3
2
du 5 }}u1/2 du
Integrate both sides.
2
}} du 5 u1/2 du
3
dy
E}
} 5 E(x 1 2) dx
y15
2
10Ïuw
E}
} du 5 }}(10)E u
3
(1 1 u )
1
2
3/2 2
0
22
du
On the left,
1
20
3
2
let u 5 y 1 5
41
5 2}}u21
20 1
3 2
1
5 2 }} }} 2 1
20
3
2
1
2
E
10
3
1 2
5 2 }} 2 }} 5 }}
36. Let u 5 4 1 3 sin x
)y 1 5) 5 e (1/2)x
du 5 3 cos x dx
1
}} du 5 cos x dx
3
p
cos x
1
}} dx 5 }}
3
2p Ïw
1w
3wsw
4w
inwx
E
4
21/2
4
du 5 0
(y 1 5) is positive or negative. Then
du 5 (5t 4 1 2) dt
5
0
4
1 2) dt 5
1/2
5 }}u3/2
3
212x
y 5 Ce (1/2)x
2
3
5 }}Ï2w7w 5 2Ï3w
25
212x
2 5.
dy
dx
40. }} 5 xÏyw cos2 Ïyw
dy
}} 5 x dx
Ïwy cos2 Ïyw
38. Let u 5 cos 2u
Integrate both sides.
dy
E}
} 5 Ex dx
Ïyw cos Ïyw
du 5 22 sin 2u du
2
1
2
2}} du 5 sin 2u du
p/6
0
y 5 C9e (1/2)x
equation), we may write the solution as
40
2
5 }}(3)3/2
3
E
212x
value C9 5 0 gives a solution to the original differential
du
0
2
3
y 1 5 5 C9e (1/2)x
Since C9 represents an arbitrary constant (note that even the
Eu
3
212x
We now let C9 5 eC or C9 5 2e C, depending on whether
37. Let u 5 t 5 1 2t
E Ïwt w1w2tw (5t
212x1C
)y 1 5) 5 e Ce(1/2)x
Eu
1
du 5 dy
1
1
}} du 5 }}x 2 1 2x 1 C
u
2
1
ln )u) 5 }}x 2 1 2x 1 C
2
1
ln )y 1 5) 5 }}x 2 1 2x 1 C
2
cos
23
E
On the left, let u 5 Ïyw
1/2
1
2u sin 2u du 5 2}}
u23 du
2 1
1
1
5 2}} ? 2}} u22
2
2
1 1 22
5 }} }}
21
4 2
1
3
5 }}(3) 5 }}
4
4
1
2
du 5 }}y21/2 dy
1/2
1 2 41
11 2
2
2 du 5 y21/2 dy
E codsu u 12
1
2Esec u du 5 }}x
2
2 }}
5 }}x 2 1 C
2
2
1C
2
1
2
2 tan u 5 }}x 2 1 C
1
2
2 tan Ïyw 5 }}x 2 1 C
1
4
tan Ïyw 5 }}x 2 1 C
C
2
(Note: technically, C is now C9 5 }}. But C’s are generic.)
2
Ïyw 5 tan211}x} 1 C2
4
3
1
x2
4
2
24
y 5 tan21 }} 1 C
247
Section 6.2
dy
dx
dy
}} 5 (cos x)(e y esin x)
dx
dy
}}y 5 cos x esin x dx
e
41. }} 5 (cos x)e y1sin x
Integrate both sides.
E}de}y 5 Ecos x e
sin x
dx
y
dy
4Ïyw ln x
44. }} 5 }}
dx
dy
}} 5 4
Ïyw
x
ln x
}} dx
x
Integrate both sides.
E}Ïdy}yw 5 4E}lnx}x dx
On the right, let u 5 ln x
1
x
On the right, let u 5 sin x
du 5 }} dx
du 5 cos x dx
2y1/2 5 4 u du
2e2y 5 e u du
2y1/2 5 4 }}u2 1 C
2e2y 5 e u 1 C
2y1/2 5 2(ln x)2 1 C
2e2y 5 e sin x 1 C
y1/2 5 (ln x)2 1 C
E
1
12 2
e2y 5 2e sin x 1 C
y 5 [(ln x)2 1 C]2
(Note: technically C is now C9 5 2C.)
2y 5 ln (C 2 e
sin x
y 5 2ln (C 2 e
sin x
45. (a) Let u 5 x 1 1
x
x
e 5e 1C
x
y 5 ln (e x 1 C)
dy
43. }} 5 22xy 2
dx
dy
2}}2 5 2x dx
y
dy
2 }}2 5 2x dx
y
E
E
y 21 5 x 2 1 C
1
y5}
2 }
x 1C
1
11C
y(1) 5 }} 5 0.25
11C54
C53
1
x 13
y5}
2 }
C50
y 5 (ln x)4
Note: Absolute value signs are not needed because the
original problem involved ln x, so we know that x . 0.
E}ed}y 5 Ee dx
Ee dy 5 Ee dx
y
(1 1 C)2 5 1
)
Integrate both sides.
y
y(e) 5 [(ln e)2 1 C]2 5 1
)
dy
42. }} 5 e x 2 y
dx
dy
}} 5 e xe 2y
dx
dy
}2}y 5 e x dx
e
2y
E
du 5 dx
EÏxw1ww1 dx 5 Eu
1/2
du
2
3
2
5 }}(x 1 1)3/2 1 C
3
d 2
Alternatively, }} }}(x 1 1)3/2 1 C 5 Ïxw1
ww1.
dx 3
5 }}u3/2 1 C
1
2
(b) By Part 1 of the Fundamental Theorem of Calculus,
dy
dy
ww1 and }}2 5 Ïxw1
ww1, so both are
}}1 5 Ïxw1
dx
dx
antiderivatives of Ïxw1
ww1.
(c) Using NINT to find the values of y1 and y2, we have:
x
0
1
2
y1
0
1.219
2.797
24.667 23.448 21.869
y2
y1 2 y2
4.667
4.667
4.667
2
3
C 5 4}}
(d) C 5 y1 2 y2
E Ïxw1ww1 dx 2 E Ïxw1ww1 dx
ww1 dx 1 E Ïxw1
ww1 dx
5 E Ïxw1
ww1 dx
5 E Ïxw1
5
x
x
0
x
3
3
0
3
x
0
3
4
4.667 6.787
0
2.120
4.667 4.667
248
Section 6.2
47. Let u 5 x 4 1 9, du 5 4x 3 dx.
d
dx
46. (a) }}[F(x) 1 C] should equal f (x).
x dx
E}
}5E
x w
1w9
Ïw
1
(b) The slope field should help you visualize the solution
curve y 5 F(x).
(c) The graphs of y1 5 F(x) and y2 5
(a)
3
4
0
E f (t) dt should
x
0
differ only by a vertical shift C.
10
1
1
}}u21/2 du 5 }}u1/2
2
9 4
1
1
5 }}Ï1w0w 2 }}Ï9w
2
2
1
3
5 }}Ï1w0w 2 }} < 0.081
2
2
x
1
E}
} dx 5 E}}u
4
x 19
3
(b)
(d) A table of values for y1 2 y2 should show that
y1 2 y2 5 C for any value of x in the appropriate
domain.
21/2
4
1
2
1
2
x 4w
1w9 1 C
5 }}Ïw
x
1
E}
x w
1w94
} dx 5 }}Ïw
2
x 19
1
(f) First, we need to find F(x). Let u 5 x 2 1 1, du 5 2x dx.
21/2
2
0
3
4
1
4
0
1
1
5 }}Ï1w0w 2 }}Ï9w
2
2
du
1
2
3
2
5 }}Ï1w0w 2 }} < 0.081
5 u1/2
48. Let u 5 1 2 cos 3x, du 5 3 sin 3x dx.
5 Ïw
x 2w
1w1 1 C
E
p/3
x 2w
1w1.
Therefore, we may let F(x) 5 Ïw
a)
du
5 }}u1/2 1 C
(e) The graph of f should be the same as the graph of
NDER of F(x).
x
1
E}
} dx 5 E}}u
2
1w1
Ïw
x w
10
49
(a)
p/6
(1 2 cos 3x) sin 3x dx 5
E }13}u du 5 }16}u 4
2
2
1
2
1
1
1
1
5 }}(2)2 2 }}(1)2 5 }}
6
6
2
d
1
x 2w
1w
1 1 C) 5 }}(2x)
}}(Ïw
dx
2Ïw
x 2w
1w1
x
5 }} 5 f (x)
1w1
Ïw
x 2w
(b)
E(1 2 cos 3x) sin 3x dx 5 E}13}u du
b)
1
6
5 }}u2 1 C
1
6
5 }}(1 2 cos 3x)2 1 C
E
p/3
[24, 4] by [23, 3]
p/6
1
6
(1 2 cos 3x) sin 3x dx 5 }}(1 2 cos 3x)2
c)
1
6
1
6
1
2
5 }}(2)2 2 }}(1)2 5 }}
49. We show that f 9(x) 5 tan x and f (3) 5 5, where
) ccooss 3x )
cos 3
d
f 9(x) 5 }}1ln )}}) 1 52
cos x
dx
f (x) 5 ln }} 1 5.
[24, 4] by [23, 3]
d)
p/3
4p/6
x
0
1
2
3
y1
1.000
1.414
2.236
3.162 4.123
y2
0.000
0.414
1.236
2.162 3.123
y1 2 y2
1
1
1
1
4
1
d
dx
5 }}(ln )cos 3) 2 ln )cos x) 1 5)
d
dx
1
5 2}}(2sin x) 5 tan x
cos x
cos 3
f (3) 5 ln }} 1 5 5 (ln 1) 1 5 5 5
cos 3
5 2}} ln )cos x)
)
e)
[24, 4] by [23, 3]
)
Section 6.3
(c) u 5 2x, du 5 2 dx
u 5 cot 2u, du 5 22 csc2 2u du
50. (a)
Ecsc
2
E2 sin x cos x dx 5 Esin 2x dx
1
5 E}} sin u du
2
E
1
2
1 u2
5 2}} }} 1 C
2
2
u2
5 2}} 1 C
4
1
5 2}} cot2 2u 1 C
4
2u cot 2u du 5 2}} u du
?
1
2
1
5 2}} cos 2x 1 C
2
5 2}} cos u 1 C
d
dx
d
}}(2cos2 x 1 C) 5 (22 cos x)(2sin x) 5 2 sin x cos x
dx
1
1
d
}} 2}} cos 2x 1 C 5 }} sin 2x (2)
2
dx 2
(d) }}(sin2 x 1 C) 5 2 sin x cos x
1
4
F1(u) 5 2}} cot2 2u
(b) u 5 csc 2u, du 5 22 csc 2u cot 2u du
Ecsc
2
1
E
1
2
1 u2
5 2}} }} 1 C
2
2
u2
5 2 }} 1 C
4
1
5 2}} csc2 2u 1 C
4
2u cot 2u du 5 2}} u du
2 1
5 2 sin x cos x
■ Section 6.3 Integration by Parts
1
F2(u) 5 2}} csc2 2u
4
(pp. 323–329)
1
1 2
2
1
F29(u) 5 12}} csc 2u2(22 csc 2u cot 2u)
2
(c) F19(u) 5 2}} cot 2u (22 csc2 2u) 5 csc2 2u cot 2u
Exploration 1
Integrals
Evaluating and Checking
dx
x
1. u 5 ln x ⇒ du 5 }} and dv 5 dx ⇒ v 5 x. Thus,
Eln x dx 5 Eu dv
5 csc 2u cot 2u
2
E
5 uv 2 v du
(d) F1(u) 5 F2(u) 1 b
1
4
E
5 x ln x 2 dx
2}} cot2 2u 5 2}} csc2 2u 1 b
1
4
1 1 2 cos2 2u
1 sin2 2u
1
5 }} }}
5 }} }2} 5 }}
sin2 2u
4
4 sin 2u
4
5 x ln x 2 x 1 C
b 5 }}(csc2 2u 2 cot2 2u)
1
2
5 sin 2x
?
1
4
249
2
1
2
51. (a) u 5 sin x, du 5 cos x dx
E2 sin x cos x dx 5 E2u du 5 u
2
1 C 5 sin x 1 C
2
1
d
dx
1x2
2. }}(x ln x 2 x) 5 ln x 1 x }} 2 1 5 ln x
dy
dx
3. The slope field of }} 5 ln x shows the direction of the
curve as it is graphed from left to right across the window.
(b) u 5 cos x, du 5 2sin x dx
E2 sin x cos x dx 5 E(22u) du
5 2u2 1 C
5 2cos2 x 1 C
[0, 6] by [22, 5]
250
Section 6.3
4. The graph of y2 5 x ln x 2 x appears to be a vertical shift
of the graph of y1 5
E ln t dt (down 1 unit). Thus, y
x
1
2
appears to be an antiderivative of ln x which
dy
dx
9. }} 5 x 1 sin x
dy 5 (x 1 sin x)dx
Integrate both sides.
supports x ln x 2 x 1 C as the set of all antiderivatives of
Edy 5 E(x 1 sin x) dx
ln x.
y 5 }}x 2 2 cos x 1 C
1
2
y(0) 5 21 1 C 5 2
C53
1
y 5 }}x 2 2 cos x 1 3
2
d 1
dx 2
1
1
5 }}e x(cos x 1 sin x) 1 (sin x 2 cos x)}}e x
2
2
1
1
1
1
5 }}e x cos x 1 }}e x sin x 1 }}e x sin x 2 }}e x cos x
2
2
2
2
1
2
10. }} }}e x(sin x 2 cos x)
[0, 6] by [22, 5]
5 e x sin x
Quick Review 6.3
dy
dx
1. }} 5 (x 3)(cos 2x)(2) 1 (sin 2x)(3x 2)
5 2x 3 cos 2x 1 3x 2 sin 2x
dy
dx
3
1 3x 1 1 2
2. }} 5 (e 2x) }} 1 ln (3x 1 1)(2e 2x)
3e 2x
3x 1 1
5 }} 1 2e 2x ln (3x 1 1)
dy
1
3. }} 5 }}2
dx
1 1 (2x)
2
5 }}2
1 1 4x
dy
?2
Section 6.3 Exercises
1. Let u 5 x
du 5 dx
5 2x cos x 1 sin x 1 C
d
Check: }}(2x cos x 1 sin x 1 C)
dx
5 (2x)(2sin x) 1 (cos x)(21) 1 cos x
5 x sin x
1
2. Let u5 x 2
y 5 tan21 3x
tan y 5 3x
Ex
1
3
x 5 }}tan y
6.
7.
E sin px dx 5 2}p1} cos px4
0
dy 5 e 2x dx
Integrate both sides.
Edy 5 Ee
1
2
2x
dx
y 5 }}e 2x 1 C
E
cos x dx 5 x 2 sin x 2 2 x sin x dx
5 2x cos x 1 (x 2 2 2)sin x 1 C
1
0
1
1
p
p
1
1
2
5 2}}(21) 1 }} 5 }}
p
p
p
dy
dx
2
v 5 sin x
5 x 2 sin x 2 2[2x cos x 1 sin x] 1 C
5 2}} cos p 1 }} cos 0
8. }} 5 e 2x
du5 2x dx
dv 5 cos x dx
Using the result from Exercise 1,
y 5 cos21 (x 1 1)
cos y 5 x 1 1
x 5 cos y 2 1
1
v 5 2cos x
Ex sin x dx 5 2x cos x 1 Ecos x dx
4. }} 5 }}
dx
2w(xw1
Ï1ww
ww3)w2
5.
dv 5 sin x dx
d
dx
Check: }}[2x cos x 1 (x 2 2 2)sin x 1 C]
5 (2x)(2sin x) 1 (2 cos x)(1) 1 (x 2 2 2)(cos x)
1 (sin x)(2x)
5 x 2 cos x
Section 6.3
3. Let u 5 ln y
dv 5 y dy
1
y
du 5 }} dy
2
E 12 1y
1
ln y 2 }}Ey dy
2
1
2
Esin
21
ln y 2 }}y 2 ? }} dy
3
v 5u
21
u du 5 u sin
Let w 5 1 2 u 2
1
2
1
1
5 }}y 2 ln y 2 }}y 2 1 C
2
4
1 2
d 1 2
Check: }} }}y ln y 2 }}y 1 C
4
dy 2
1 2 1
1
5 }}y }} 1 (ln y)(y) 2 }}y
2
y
2
5 }}y 2
dv 5 du
1
du 5 }}
2wu2w
Ïw1w
v 5 }}y 2
Ey ln y dy 5 }12}y
6. Let u 5 sin21 u
E
1
u 2 u}} du
2w
Ï1ww
u 2w
dw 5 22u du
E
1
1
4
5 u sin21 u 1 Ï1ww
2wu2w 1 C
5 y ln y
u 5 tan21 y
dv 5 dy
1
11y
du 5 }}2 dy
Etan
21
v5y
E 1 1y y
y dy 5 y tan21 y 2 }}2 dy
[21, 1] by [20.5, 2]
7. Let u 5 t 2
Let w 5 1 1 y 2
dw 5 2y dy
E 1 1y y
E
1 1
2 w
1
5 y tan21 y 2 }} ln )w) 1 C
2
1
5 y tan21 y 2 }} ln (1 1 y 2) 1 C
2
1
d
Check: }} y tan21 y 2 }} ln (1 1 y 2) 1 C
2
dy
1
y
1
21
5 }}2 1 tan y 2 }} }}2 (2y) 5 tan21 y
2 11y
11y
y tan21 y 2 }}2 dy 5 y tan21 y 2 }} }} dw
3
5. Let u 5 x
du 5 dx
Ex sec
2
1
2
dv 5 sec2 x dx
v 5 tan x
4
Et
dv 5 sin t dt
du 5 2t dt
2
v 5 2cos t
E
sin t dt 5 2t 2 cos t 1 2 (cos t)(t) dt
Let u 5 t
dv 5 cos t dt
du 5 dt
v 5 sin t
E
2t 2 cos t 1 2 t cos t dt
E
5 2t 2 cos t 1 2t sin t 2 2 sin t dt
5 2t cos t 1 2t sin t 1 2 cos t 1 C
2
5 (2 2 t 2) cos t 1 2t sin t 1 C
E
sin x
5 x tan x 2 E}} dx
cos x
x dx 5 x tan x 2 tan x dx
5 x tan x 1 ln )cos x) 1 C
[23, 3] by [0, 8]
8. Let u 5 t
du 5 dt
Et csc
2
[21.5, 1.5] by [21, 4]
E1
u sin21 u 2 u}} du 5 u sin21 u 1 }} }} dw
2wu2w
2 Ïw
Ï1ww
w
5 u sin21 u 1 w1/2 1 C
1 21 2
4. Let
251
dv 5 csc2 t dt
v 5 2cot t
E
cos t
5 2t cot t 1 E}} dt
sin t
t dt 5 2t cot t 1 cot t dt
5 2t cot t 1 ln usin tu 1 C
[0, 3] by [24, 4]
252
Section 6.3
9. Let u 5 ln x
1
x
1
4
du 5 }} dx
Ex
3
12. Use tabular integration with f (x) 5 x 3 and g(x) 5 e22x.
dv 5 x 3 dx
v 5 }}x 4
f(x) and its
derivatives
E 12
E
1
1
1
4
4
x
1
1
5 }}x 4 ln x 2 }} x 3 dx
4
4
1
1
5 }}x 4 ln x 2 }}x 4 1 C
4
16
ln x dx 5 }}x 4 ln x 2 }} x 4 }} dx
x3
(+)
e–2x
3x2
(–)
2}} e–2x
6x
(+)
6
(–)
2x
10. Use tabular integration with f (x) 5 x and g(x) 5 e .
4
f(x) and its
derivatives
Ex e
3 22x
e–x
(+)
4x 3
(–)
–e–x
12x 2
(+)
e–x
24x
(–)
–e–x
(+)
e–x
24
Ex e
4 2x
1
5 2x e
Ee
3 2x
2 4x e
2 2x
2 12x e
11. Let u 5 x 2 5x
2 24xe
2x
Let
x
du 5 (2x 2 5) dx
v 5 ex
du 5 e y dy
y
v 5 2cos y
E
sin y dy 5 2e y cos y 1 cos y e y dy
2
x
E
u 5 2x 2 5
dv 5 e dx
du 5 2 dx
v5e
E
du 5 e dy
x
y
y
y
y
y
E
5 (x 2 2 5x)e x 2 (2x 2 5)e x 1 2e x 1 C
dy
y
dv 5 cos y dy
2y
du 5 2e
dy
2y
E
v 5 sin y
cos y dy 5 e2ysin y 1 sin y e2y dy
Let u 5 e2y
5 (x 2 2 5x)e x 2 (2x 2 5)e x 1 2e x dx
y
y
14. Let u 5 e2y
Ee
x
v 5 sin y
Ee sin y dy 5 2e cos y 1 e sin y 2 Esin ye
2Ee sin y dy 5 2e cos y 1 e sin y
Ee sin y dy 5 }12}e (sin y 2 cos y) 1 C
x
(x 2 2 5x)e x 2 e x(2x 2 5) dx
5 (x 2 2 7x 1 7)ex 1 C
1C
dv 5 cos y dy
y
y
2 5x)e dx 5 (x 2 5x)e 2 e (2x 2 5) dx
x
2x
2 24e
dv 5 e dx
2
E(x
dv 5 sin y dy
Let u 5 e y
5 2(x 4 1 4x 3 1 12x 2 1 24x 1 24)e 2x 1 C
2
2
13. Let u 5 e y
dx
4 2x
dx
1
3
3
3
5 2}}x 3e22x 2 }}x 2e22x 2 }}xe22x 2 }}e22x 1 C
2
4
4
8
x3
3x 2
3x
3
5 2 }} 1 }} 1 }} 1 }} e22x 1 C
2
4
4
8
–e–x
0
1
2
1 –2x
}} e
4
1
2}} e–2x
8
1
}} e–2x
16
0
g(x) and its
integrals
x4
g(x) and its
integrals
Ee
2Ee
Ee
dv 5 sin y dy
du 5 2e2y dy
2y
2y
cos y dy 5 e
2y
2y
v 5 2cos y
E
sin y 2 e2ycos y 2 e2y cos y dy
cos y dy 5 e2y sin y 2 e2y cos y
1
2
cos y dy 5 }}e2y(sin y 2 cos y) 1 C
Section 6.3
15. Use tabular integration with f (x) 5 x 2 and g(x) 5 sin 2x.
f(x) and its
derivatives
g(x) and its
integrals
x2
(+)
2x
(–)
2
(+)
sin 2x
1
2
1
2 }} sin 2x
4
1
}} cos 2x
8
2 }} cos 2x
0
Ex
1
2
1
2
1
4
sin 2x dx 5 2}}x 2 cos 2x 1 }}x sin 2x 1 }} cos 2x 1 C
2
1
1 2 2x 2
4
x
2
2
5 }} cos 2x 1 }} sin 2x 1 C
E
p/2
31
1 2 2x 2
4
x
2
2
x 2 sin 2x dx 5 }} cos 2x 1 }} sin 2x
0
5
1
p 2
1 2
p/2
40
2
1 2 2 }}
2
1
}} (21) 1 0 2 }}(1) 2 0
4
4
p2
8
1
2
5 }} 2 }} < 0.734
p
2
1
2
Check: NINT x 2 sin 2x, x, 0, }} < 0.734
16. Use tabular integration with f (x) 5 x 3 and g(x) 5 cos 2x.
f(x) and its
derivatives
g(x) and its
integrals
x3
(+)
3x2
(–)
6x
(+)
6
(–)
cos 2x
1
}} sin 2x
2
1
2 }} cos 2x
4
1
2}} sin 2x
8
1
}} cos 2x
16
0
Ex
1
2
3
4
3
4
3
8
cos 2x dx 5 }}x 3 sin 2x 1 }}x 2 cos 2x 2 }}x sin 2x 2 }}cos 2x
3
x3
12
3x
4
3x 2
2
14
3
8
2
5 }} 2 }} sin 2x 1 }} 2 }} cos 2x 1 C
E
p/2
0
x 3cos 2x dx 5
x3
3x 2
p/2
31}2} 2 }4}2sin 2x 1 1}4} 2 }8}2cos 2x40
3x
3p2
1 16
3
8
2
3
1 82
3
5 0 1 }} 2 }} (21) 2 0 2 2}} (1)
3
4
3p2
16
5 }} 2 }} < 21.101
1
p
2
2
Check: NINT x 3cos 2x, x, 0, }} < 21.101
253
254
Section 6.3
17. Let u 5 e 2x
dv 5 cos 3x dx
1
3
du 5 2e 2x dx
Ee
2x
v 5 }} sin 3x
1
2 E1}3} sin 3x2(2e2x dx)
13
1
cos 3x dx 5 (e 2x) }} sin 3x 2
1
3
2
3
E
5 }}e2x sin 3x 2 }} e2x sin 3x dx
u 5 e2x
Let
dv 5 sin 3x dx
1
3
1
2
1
1
e 2x cos 3x dx 5 }}e 2x sin 3x 2 }} (e 2x) 2}} cos 3x 2 2}} cos 3x (2e 2x dx)
3
3
3
3
1 2x
4 2x
5 }}e (3 sin 3x 1 2cos 3x) 2 }} e cos 3x dx
9
9
13 2x
1 2x
}} e cos 3x dx 5 }}e (3 sin 3x 1 2 cos 3x)
9
9
1 2x
2x
e cos 3x dx 5 }}e (3 sin 3x 1 2 cos 3x)
13
3
1
3
e 2x cos 3x dx 5 }}e 2x(3 sin 3x 1 2 cos 3x)
13
22
22
du 5 2e 2x dx
v 5 2}} cos 3x
E
E
E
3
1
2 E1
E
E
3
2
4
4
1
13
1
5 }}[e6(2 cos 9 1 3 sin 9) 2 e24(2 cos 6 2 3 sin 6)]
13
5 }}[e 6(3 sin 9 1 2 cos 9) 2 e 24(3 sin (26) 1 2 cos (26)]
< 218.186
Check: NINT(e 2x cos 3x, x, 22, 3) < 218.186
u 5 e22x
18. Let
dv 5 sin 2x dx
22x
du 5 22e
Ee
22x
1
2
v 5 2}} cos 2x
dx
1
1
2
1
2 E12}2}cos 2x2(22e22x dx)
sin 2x dx 5 (e22x) 2}}cos 2x 2
1
2
E
5 2}}e22xcos 2x 2 e22xcos 2x dx
Let
Ee
22x
u 5 e22x
dv 5 cos 2x dx
du 5 22e22x
v 5 }}sin 2x
1
2
3
1
2
12
1
1
2 E1}2}sin 2x2(22e22x dx)4
sin 2x dx 5 2}}e22xcos 2x 2 (e22x) }}sin 2x 2
E
1
2
5 2}}e22x(cos 2x 1 sin 2x) 2 e22xsin 2x dx
E
Ee
Ee
1
2
2 e22x sin 2x dx 5 2}}e22x(cos 2x 1 sin 2x) 1 C
22x
2
23
e22x
4
sin 2x dx 5 2}}(cos 2x 1 sin 2x) 1 C
22x
3
e22x
4
sin 2x dx5 2}}(cos 2x 1 sin 2x)
423
2
e24
4
e6
4
e24
4
e6
4
5 2}}(cos 4 1 sin 4) 1 }}[cos (26) 1 sin (26)]
5 2}}(cos 4 1 sin 4) 1 }}(cos 6 2 sin 6)
< 125.028
Check: NINT(e22xsin 2x, x, 23, 2) < 125.028
Section 6.3
E
23. Let
19. y 5 x 2e4x dx
Let u 5 x 2
dv 5 e4xdx
1
4
du 5 2x dx
v 5 }}e4x
1
1 2 E1}4}e 2(2x dx)
1
1
5 }}x e 2 }}Exe dx
4
2
1
4
y 5 (x 2) }}e4x 2
dv 5 sin x dx
du 5 dx
v 5 2cos x
Ex sin x dx 5 2x cos x 1 Ecos x dx
5 2x cos x 1 sin x 1 C
4x
2 4x
E )x sin x) dx 5 E x sin x dx
p
(a)
4x
Let u 5 x
p
0
0
3
5 2p(21) 1 0 1 0(1) 2 0
1
4
v 5 }}e4x
5p
3 1 2 E1 2 4
1
1
1
1
}}e4x dx
4
2
4
4
1 2 4x
1 4x
1 4x
y 5 }}x e 2 }}xe 1 }}e 1 C
4
8
32
x2
x
1
y 5 }} 2 }} 1 }} e4x 1 C
4
8
32
y 5 }}x 2e4x 2 }} (x) }}e4x 2
1
p
40
5 2x cos x 1 sin x
dv 5 e4x dx
du 5 dx
E
E
2p
(b)
p
2p
)x sin x) dx 5 2
3
5 x cos x 2 sin x
2
p
x sin x dx
4p
2p
5 2p(1) 2 0 2 p(21) 1 0
E
20. y 5 x 2 ln x dx
5 3p
Let u 5 ln x
dv 5 x dx
2
1 2 E1 21
0
1
2
E(x
p
0
)x sin x) dx
dv 5 e2x dx
v 5 2e2x
du 5 (2x 1 1) dx
2
1 x 1 1)e2x dx
E
5 2(x 2 1 x 1 1)e2x 1 (2x 1 1)e2x dx
v 5 }}u2
dv 5 e2x dx
Let u 5 2x 1 1
in the expression for du.
1
1
1
} du2
1 2 2 E1}2}u221}
uÏu
ww2
ww1
E 2)u) du
2p
Let u 5 x 2 1 x 1 1
Note that we are told u . 1, so no absolute value is needed
1
p
E
dv 5 u du
y 5 (sec21 u) }}u2 2
E )x sin x) dx 1 E
24. We begin by evaluating (x 2 1 x 1 1)e2x dx.
E
1
)x sin x) dx 5
5 p 1 3p 5 4p
21. y 5 u sec21 u du
du 5 }} du
uÏu
w2w2
ww1
2p
2
E
Let u 5 sec21 u
E
(c)
1
1
du 5 }} dx
v 5 }}x 3
x
3
1 3
1 3 1
y 5 (ln x) }}x 2 }}x }} dx
3
3
x
1 3
1 2
y 5 }}x ln x 2 }} x dx
3
3
1
1
y 5 }}x 3 ln x 2 }}x 3 1 C
3
9
u2
u5x
2
y 5 }}sec21 u 2 }} }}
2
4 Ïuw2w2
ww1
2
Let w 5 u 2 1, dw 5 2u du
E(x
v 5 2e2x
du 5 2 dx
2
1 x 1 1)e2x dx
E
5 2(x 2 1 x 1 1)e2x 2 (2x 1 1)e2x 1 2e2x dx
5 2(x 2 1 x 1 1)e 2x 2 (2x 1 1)e 2x 2 2e2x 1 C
5 2(x 2 1 3x 1 4)e2x 1 C
E
u2
1
2
4
u2
1
21
y 5 }} sec u 2 }}w1/2 1 C
2
2
u2 21
1
y 5 }}sec u 2 }}Ïuw2w2
ww1 1 C
2
2
y 5 }}sec21 u 2 }} w21/2 dw
E
22. y 5 u sec u tan u du
Let
u5u
du 5 du
E
dv 5 sec u tan u du
v 5 sec u
y 5 u sec u 2 sec u du
y 5 u sec u 2 ln )sec u 1 tan u) 1 C
Note: In the last step, we used the result of Exercise 29 in
Section 6.2.
[23, 3] by [23, 3]
The graph shows that the two curves intersect at x 5 k,
where k < 1.050. The area we seek is
E (x
k
0
2
1 x 1 1)e2x 2
3
Ex
k
2
dx
0
5 2(x 2 1 3x 1 4)e2x
40 2 3}3}x340
k
1
< (22.888 1 4) 2 (0.386 2 0)
< 0.726
k
255
256
Section 6.3
E
(c) Using the result from part (b):
25. First, we evaluate e2t cos t dt.
u 5 e2t
Let
2t
Ee
du 5 2e
2t
dt
E
2t
cos t dt 5 e sin t 1 sin t e
Let u 5 e2t
Ex
v 5 sin t
2t
du 5 3x 2 dx
3
dt
5 x e 2 3(x 2 2 2x 1 2)e x 1 C
3 x
5 (x 3 2 3x 2 1 6x 2 6)e x 1 C
2t
2t
2t
3
2t
d
dx
or [x 2 nx
n
cos t dt
2t
n21
dn
dx
1 n(n 2 1)x
… 1 (21)
2t
2t
d2
dx
4
(d) x n 2 }}x n 1 }}2 x n 2 … 1 (21)n}}n x n ex 1 C
v 5 2cos t
Ee cos t dt 5 e sin t 2 e cos t 2 Ee
2Ee cos t dt 5 e (sin t 2 cos t) 1 C
Ee cos t dt 5 }12}e (sin t 2 cos t) 1 C
2t
E
v 5 ex
e x dx 5 x 3 e x 2 3x 2 e x dx
dv 5 sin t dt
du 5 2e2t dt
dv 5 e x dx
Let u 5 x 3
dv 5 cos t dt
n21
n22
2
(n 2 1)!x 1 (21)n(n!)]e x 1 C
(e) Use mathematical induction or argue based on tabular
Now we find the average value of y 5 2e2tcos t for
integration.
0 # t # 2p.
Alternately, show that the derivative of the answer to
E
1
p
2e2tcos t dt
31
d
}} x n 2 nx n21 1 n(n 2 1)x n22 2
dx
0
E
5 }}
part (d) is x ne x:
2p
1
Average value 5 }}
2p
e2tcos t dt
0
5 [x 2 nx
n
4
1
2p
5 }}e2t(sin t 2 cos t)
2p
0
x
2
(n!)x 1 (21)nn!]e x 1
n21
… 1 (21)n21(n!)x 1 (21)nn!]
5 [xn 2 nx n21 1 n(n 2 1)x n22 2
… 1 (21)n21(n!)x 1 (21)nn!]e x
dv 5 e x dx
E
1 [nx n21 2 n(n 2 1)x n22
v 5 ex
1 n(n 2 1)(n 2 2)x n23 2
dx 5 xe x 2 e x dx
… 1 (21)n21n!]e x
5 xe x 2 e x 1 C
5 x ne x
5 (x 2 1)e x 1 C
dx
(b) Using the result from part (a):
Let
Ex
2
u 5 x2
dv 5 e x dx
du 5 2x dx
v 5 ex
E
e x dx 5 x 2 e x 2 2x e x dx
5 x 2e x 2 2(x 2 1)e x 1 C
5 (x 2 2 2x 1 2)e x 1 C
4
d
dx
1 2 e22p
5 }} < 0.159
2p
Exe
1 n(n 2 1)x
n22
ex}}[x n 2 nx n21 1 n(n 2 1)x n22 2
1
2p
du 5 dx
n21
… 1 (21)
5 }}[e22p(21) 2 e0(21)]
26. (a) Let u 5 x
2
… 1 (21)n21(n!)x 1 (21)nn! e x 1 C
2p
27. Let w 5 Ïxw. Then dw 5 }}, so dx 5 2Ïxw dw 5 2w dw.
2Ïxw
sin Ïwx dx 5 (sin w)(2w dw) 5 2 w sin w dw
E
E
Let u 5 w
E
dv 5 sin w dw
du 5 dw
v 5 2cos w
Ew sin w dw 5 2w cos w 1 Ecos w dw
5 2w cos w 1 sin w 1 C
Esin Ïxw dx 5 2Ew sin w dw
5 22w cos w 1 2 sin w 1 C
5 22Ïxw cos Ïxw 1 2 sin Ïxw 1 C
Section 6.3
28. Let w 5 Ï3wxw1
ww9. Then dw 5 }1}(3) dx, so
2Ïw
3xww
1w9
2
dx 5 }}Ï3wxw1
ww9 dw 5 }2}w dw.
3
3
w9w dx 5 (ew) }2}w dw 5 }2} w ew dw
eÏ3wx1
3
3
E
E 1
2 E
dv 5 cos x dx
31. Let u 5 x n
Ex
du 5 nx
dx
5 xn
Let u 5 w dv 5 e dw
Ew e
w
dw
u 5 xn
32. Let
v 5 ew
E
5 w ew 2 ew dw
Ex
5 w e w 2 ew
w
3x19
dw
Ex e
E
dx 5 (x ) e
E
1
x dx 5 }} w 3 e w dw.
2
Use tabular integration with f (x) 5 w 3 and g(w) 5 e w.
f(w) and its
derivatives
g(w) and its
integrals
w3
(+)
ew
3w2
(–)
ew
6w
(+)
ew
6
(–)
ew
E
Ew
3
Ex e
1
1
1 a 2 E1}a}eax2(nxn21 dx)
x ne ax
a
E(ln x)
dv 5 dx
n(ln x)
x
n21
du 5 }} dx v 5 x
n
E 3 n(ln xx) 4
2 nE(ln x)
dx
n21
dx 5 (ln x)n(x) 2 x }} dx
5 x(ln x)n
n21
35. (a) Let y 5 f 21(x). Then x 5 f (y), so dx 5 f9(y) dy.
E
E
E
Hence, f 21(x) dx 5 (y)[f9(y) dy] 5 y f9(y) dy
1
r
30. Let y 5 ln r. Then dy 5 }} dr, and so dr 5 r dy 5 e y dy.
Using the result of Exercise 13, we have:
dy
1
5 }}e y(sin y 2 cos y) 1 C
2
1
5 }}eln r[sin (ln r) 2 cos (ln r)] 1 C
2
r
5 }}[sin (ln r) 2 cos (ln r)] 1 C
2
dv 5 f9( y)dy
du 5 dy
v 5 f (y)
21
21
E
1
2
1
5 }}(w 3 2 3w 2 1 6w 2 6)e w 1 C
2
2
(x 6 2 3x 4 1 6x 2 2 6)ex
5 }}} 1 C
2
u5y
Ey f9(y) dy 5 y f ( y) 2 Ef (y) dy
5 f (x)(x) 2 Ef (y) dy
Hence, Ef (x) dx 5 Ey f9( y) dy
5 x f (x) 2 Ef ( y) dy.
dx 5 }} w 3 e w dw
y
E
u 5 (ln x)n
34. Let
(b) Let
Esin (ln r) dr 5 E(sin y)e
n
a
5 }} 2 }} x n21e ax dx, a Þ 0
e w dw 5 w 3 e w 2 3w 2e w 1 6w e w 2 6e w 1 C
7 x2
1
a
v 5 }}e ax
dx 5 (x n) }}e ax 2
n ax
5 (w 3 2 3w 2 1 6w 2 6)e w 1 C
Ex e
E
dv 5 e ax dx
du 5 nx n21 dx
ew
0
v 5 2cos x
dx
33. Let u 5 x n
29. Let w 5 x 2. Then dw 5 2x dx.
2 3 x2
n21
5 2x ncos x 1 n x n21cos x dx
2
5 }}(w 2 1)ew
3
2
w9w 1 C
5 }}(Ï3wxw1
ww9 2 1)eÏ3wx1
3
7 x2
sin x dx
sin x dx 5 (x n)(2cos x) 2 (2cos x)(nx n21 dx)
5 (w 2 1)ew
EeÏwww dx 5 }23}Ew e
n21
dv 5 sin x dx
du 5 nx
n
E
sin x 2 nEx
cos x dx 5 x n sin x 2 (sin x)(nx n21dx)
n
w
du 5 dw
v 5 sin x
n21
21
36. Let u 5 f 21(x)
Ef
1
dv 5 dx
2
d
du 5 }} f 21(x) dx
dx
21
(x) dx 5 x f
21
v5x
E 1 ddx
2
(x) 2 x }} f 21(x) dx
37. (a) Using y 5 f 21(x) 5 sin21 x and f (y) 5 sin y,
p
2
p
2
2}} # y # }}, we have:
Esin
21
E
x dx 5 x sin21 x 2 sin y dy
5 x sin21 x 1 cos y 1 C
5 x sin21 x 1 cos (sin21 x) 1 C
257
258
Section 6.4
40. (a) Using y 5 f 21(x) 5 log2 x and f (y) 5 2 y, we have
37. continued
(b)
Esin
21
E 1 ddx
2
1
x 2 Ex}} dx
2wx w
Ï1ww
Elog
x dx 5 x sin21 x 2 x }} sin21 x dx
5 x sin21
2y
ln 2
1
5 x log2 x 2 }} 2log2 x
ln 2
5 x log2 x 2 }} 1 C
1
2
E
5 x sin21 x 1 }} u21/2 du
5 x sin
E
x dx 5 x log2 x 2 2 y dy
2
u 5 1 2 x 2, du 5 22x dx
21
2
x1u
1/2
(b)
1C
Elog
2
5 x log2
5 x sin21 x 1 Ï1ww
2wx 2w 1 C
5 x log2
(c) cos (sin21 x) 5 Ï1ww
2wx 2w
1 ln 2 2
1
5 x log2 x 2 }} x 1 C
38. (a) Using y 5 f 21(x) 5 tan21 x and f (y) 5 tan y,
p
2
(c) 2log2 x 5 x
p
2
2}} , y , }}, we have:
Etan
21
E 1 ddx 2
1
x 2 Ex1}}2 dx
x ln 2
dx
x 2 E}}
ln 2
x dx 5 x log2 x 2 x }} log2 x dx
E
x dx 5 x tan21 x 2 tan y dy
■ Section 6.4 Exponential Growth and
Decay (pp. 330–341)
5 x tan21 x 2 ln )sec y) 1 C
(Section 6.2, Example 7)
Exploration 1
5 x tan21 x 1 ln )cos y) 1 C
5 x tan21 x 1 ln )cos (tan21 x)) dx 1 C
(b)
Etan
21
Slowing Down More Slowly
1. As m increases the velocity of the object represented by the
graph slows down more slowly. That is, the y-coordinates
of the graphs decrease to 0 more slowly as m increases.
E 1 ddx
2
1
x 2 Ex1}}2 dx
11x
x dx 5 x tan21 x 2 x }} tan21 x dx
5 x tan21
2
u 5 1 1 x , du 5 2x dx
2
E
1
2
1
5 x tan21 x 2 }}ln )u) 1 C
2
1
5 x tan21 x 2 }}ln (1 1 x 2) 1 C
2
5 x tan21 x 2 }} u21 du
)
)
1
f ( y) 5 cos x, 0 # x # p, we have:
Since s(0) 5
0
0
traveled by the object at time t.
x 2 sin y 1 C
5 x cos21 x 2 sin (cos21 x) 1 C
(b)
Ecos
21
E1
E1
u 5 1 2 x 2, du 5 22x dx
1
2
E
5 x cos21 x 2 }} u21/2 du
5 x cos21 x 2 u1/2 1 C
5 x cos
[0, 70] by [0, 1500]
2
2
d
x dx 5 x cos x 2 x }} cos21 x dx
dx
1
5 x cos21 x 2 x 2}} dx
2wx 2w
Ïw1w
21
21
x 2 Ï1ww
2wx w 1 C
2
(c) sin (cos21 x) 5 Ï1ww
2wx 2w
0
E v(u) du 5 0, the integral gives the distance
E
5 x cos
t
distance traveled by the object over the time interval [0, t].
x dx 5 x cos21 x 2 cos y dy
21
E v(u) du gives the
3. The total distance traveled is about 200 units for m 5 1,
about 400 units for m 5 2, about 800 units for m 5 4, and
about 1200 units for m 5 6.
39. (a) Using y 5 f 21(x) 5 cos21 x and
21
2. As we saw in Section 5.1, s(t) 5
1
(c) ln )cos (tan21 x)) 5 ln }} 5 2}}ln (1 1 x 2)
2
1wx 2w
Ï1ww
Ecos
[0, 20] by [0, 120]
Quick Review 6.4
1. a 5 eb
2. c 5 ln d
3. ln (x 1 3) 5 2
x 1 3 5 e2
x 5 e2 2 3
4. 100e2x 5 600
e2x 5 6
2x 5 ln 6
1
x 5 }} ln 6
2
Section 6.4
5.
0.85x 5 2.5
5. Doubling time:
A(t) 5 A0ert
ln 0.85x 5 ln 2.5
2000 5 1000e0.086t
x ln 0.85 5 ln 2.5
2 5 e0.086t
ln 2.5
x 5 }} < 25.638
ln 0.85
6.
2
k11
53
ln 2
k11
5 ln 3
ln 2 5 0.086t
ln 2
0.086
t 5 }} < 8.06 yr
k
Amount in 30 years:
A 5 1000e(0.086)(30) < $13,197.10
k
(k 1 1)ln 2 5 k ln 3
6. Annual rate:
A(t) 5 A0e rt
4000 5 2000e(r)(15)
2 5 e15r
ln 2 5 15r
ln 2
r 5 }} < 0.0462 5 4.62%
15
Amount in 30 years:
A(t) 5 A0e rt
A 5 2000e[(ln 2)/15](30)
5 2000e2 ln 2
5 2000 ? 22
5 $8000
ln 2 5 k(ln 3 2 ln 2)
ln 2
ln 3 2 ln 2
k 5 }} < 1.710
7.
1.1t 5 10
ln 1.1t 5 ln 10
t ln 1.1 5 ln 10
ln 10
ln 1.1
1
log 1.1
t 5 }} 5 }} < 24.159
1
4
8. e22t 5 }}
142
7. Initial deposit:
1
22t 5 ln }}
1
2
12
1
4
A(t) 5 A0e rt
1
2
t 5 2}} ln }} 5 }} ln 4 5 ln 2
2898.44 5 A0e(0.0525)(30)
9. ln (y 1 1) 5 2x 1 3
y 1 1 5 e2x13
y 5 21 1 e2x13
2898.44
e
A0 5 }
}
1.57
5 < $600.00
Doubling time:
A(t) 5 A0e rt
10. ln )y 1 2) 5 3t 2 1
)y 1 2) 5 e3t21
y 1 2 5 6e3t21
y 5 22 6 e3t21
1200 5 600e0.0525t
2 5 e0.0525t
ln 2 5 0.0525t
Section 6.4 Exercises
ln 2
0.0525
1. y(t)5 y0e kt
y(t) 5 100e1.5t
t 5 }} < 13.2 years
2. y(t) 5 y0e kt
y(t) 5 200e205t
8. Annual rate:
3. y(t) 5 y0e kt
y(t) 5 50e kt
y(5) 5 100 5 50e 5k
2 5 e 5k
ln 2 5 5k
k 5 0.2 ln 2
Solution: y(t) 5 50e(0.2 ln 2)t or y(t) 5 50 ? 20.2t
4. y(t) 5 y0e kt
A(t) 5 A0e rt
10,405.37 5 1200e(r)(30)
104.0537
}} 5 e30r
12
104.0537
ln }} 5 30r
12
104.0537
1
r 5 }}ln }} < 0.072 5 7.2%
12
30
Doubling time:
y(t) 5 60e kt
y(10)5 30 5 60e
A(t) 5 A0e rt
10k
2400 5 1200e0.072t
1
}} 5 e10k
2
1
ln }} 5 10k
2
2 5 e0.072t
ln 2 5 0.072t
1
2
k 5 0.1 ln }} 5 20.1 ln 2
2(0.1 ln 2)t
Solution: y(t) 5 60e
or y(t) 5 60 ? 2
2t/10
ln 2
0.072
t 5 }} < 9.63 years
259
260
Section 6.4
9. (a) Annually:
2 5 1.0475 t
ln 2 5 t ln 1.0475
ln 2
t 5 }} < 14.94 years
11. (a) Since there are 48 half-hour doubling times in 24
hours, there will be 248 < 2.8 3 1014 bacteria.
(b) The bacteria reproduce fast enough that even if many
are destroyed there are still enough left to make the
person sick.
ln 1.0475
12. Using y 5 y0e kt, we have
(b) Monthly:
10,000 5 y0e3k and 40,000 5 y0e5k.
0.0475 12t
12
0.0475
ln 2 5 12t ln 1 1}}
12
ln 2
t 5 }}
0.0475 < 14.62 years
12 ln 1 1}}
1
2
2 5 1 1 }}
1
2
1
12
y0e
e2k 5 4, or k 5 ln 2. Solving 10,000 5 y0e3ln 2, we have
2
y0 5 1250. There were 1250 bacteria initially.
We could solve this more quickly by noticing that the
(c) Quarterly:
population increased by a factor of 4, i.e. doubled twice, in
0.0475 4t
4
1
y e5k
40,000
10,000
Hence }} 5 }0 }
3k , which gives
2
2 5 1 1 }}
2 hrs, so the doubling time is 1 hr. Thus in 3 hrs the
ln 2 5 4t ln 1.011875
population would have doubled 3 times, so the initial
ln 2
t 5 }} < 14.68 years
4 ln 1.011875
(d) Continuously:
10,0000
5 1250.
population was }}
3
2
13.
0.9 5 e20.18t
ln 0.9 5 20.18t
ln 0.9
t 5 2}} < 0.585 days
0.18
2 5 e0.0475t
ln 2
k
ln 2
0.005
14. (a) Half-life 5 }} 5 }} < 138.6 days
ln 2 5 0.0475t
ln 2
0.0475
t 5 }} < 14.59 years
(b)
0.05 5 e20.005t
ln 0.05 5 20.005t
10. (a) Annually:
ln 0.05
0.005
t 5 2}} < 599.15 days
2 5 1.0825t
The sample will be useful for about 599 days.
ln 2 5 t ln 1.0825
ln 2
ln 1.0825
t 5 }} < 8.74 years
15. Since y0 5 y (0) 5 2, we have:
y 5 2e kt
(b) Monthly:
5 5 2e(k)(2)
0.0825 12t
1
2
2 5 1 1 }}
12
ln 5 5 ln 2 1 2k
1
2
0.0825
ln 2 5 12t ln 1 1 }}
12
ln 2
t 5 }}
0.0825 < 8.43 years
12 ln 1 1 }}
1
12
2
Function: y 5 2e(0.5 ln 2.5)t or y < 2e0.4581t
16. Since y0 5 y (0) 5 1.1, we have:
(c) Quarterly:
1
ln 5 2 ln 2
2
k 5 }} 5 0.5 ln 2.5
0.0825 4t
4
2
2 5 1 1 }}
ln 2 5 4t ln 1.020625
ln 2
4 ln 1.020625
t 5 }} < 8.49 years
(d) Continuously:
2 5 e0.0825t
ln 2 5 0.0825t
ln 2
0.0825
t 5 }} < 8.40 years
y 5 1.1e kt
3 5 1.1e(k)(23)
ln 3 5 ln 1.1 2 3k
1
k 5 }}(ln 1.1 2 ln 3)
3
Function: y 5 1.1e(ln 1.1 2 ln 3)t/3 or y < 1.1e20.3344t
Section 6.4
3
261
20. First, we find the value of k.
17. At time t 5 }}, the amount remaining is
k
y0e2kt 5 y0e2k(3/k) 5 y0e23 < 0.0499y0. This is less than
Taking “right now” as t 5 0, 608 above room temperature
5% of the original amount, which means that over 95% has
means T0 2 Ts 5 60. Thus, we have
decayed already.
T 2 Ts 5 (T0 2 Ts)e2kt
70 5 60e(2k)(220)
18. T 2 Ts 5 (T0 2 Ts) e2kt
7
}} 5 e20k
6
7
1
k 5 }}ln }}
20 6
35 2 65 5 (T0 2 65)e2(k)(10)
50 2 65 5 (T0 2 65)e2(k)(20)
Dividing the first equation by the second, we have:
2 5 e10k
(a) T 2 Ts 5 (T0 2 Ts)e2kt 5 60e(2(1/20)ln (7/6))(15) < 53.45
It will be about 53.458C above room temperature.
1
10
k 5 }} ln 2
Substituting back into the first equation, we have:
230 5 (T0 2 65)e2[(ln 2)/10](10)
(b) T 2 Ts 5 (T0 2 Ts)e2kt 5 60e(2(1/20)ln (7/6))(120) < 23.79
It will be about 23.798 above room temperature.
12
1
230 5 (T0 2 65) }}
2
260 5 T0 2 65
(c) T 2 Ts 5 (T0 2 Ts)e2kt
5 5 T0
10 5 60e(2(1/20)ln (7/6))t
The beam’s initial temperature is 58F.
1
1
6
2
7
1
6
20
20 ln (1/6)
t 5 2}} < 232.47 min
ln (7/6)
ln }} 5 2}} ln }} t
19. (a) First, we find the value of k.
T 2 Ts 5 (T0 2 Ts)e2kt
It will take about 232.47 min or 3.9 hr.
60 2 20 5 (90 2 20)e2(k)(10)
4
}} 5 e210k
7
4
1
k 5 2}} ln }}
7
10
ln 2
5700
21. Use k 5 }} (see Example 3).
e2kt 5 0.445
When the soup cools to 358, we have:
35 2 20 5 (90 2 20)e[(1/10) ln
15 5 70e [(1/10) ln
3
14
4
7
1
1 10
2kt 5 ln 0.445
ln 0.445
k
(4/7)]t
5700 ln 0.445
ln2
t 5 2}} 5 2}} < 6658 years
(4/7)]t
Crater Lake is about 6658 years old.
2
ln 2
5700
ln }} 5 }} ln }} t
22. Use k 5 }} (see Example 3).
3
1 2
172
(a) e2kt 5 0.17
10 ln }}
14
t 5 }}
< 27.53 min
4
ln }}
2kt 5 ln 0.17
It takes a total of about 27.53 minutes, which is an
additional 17.53 minutes after the first 10 minutes.
ln 0.17
k
5700 ln 0.17
ln 2
t 5 2}} 5 2}} < 14,571 years
The animal died about 14,571 years before A.D. 2000,
(b) Using the same value of k as in part (a), we have:
T 2 Ts 5 (T0 2 Ts)e2kt
35 2 (215)5 [90 2 (215)]e[(1/10) ln
50 5 105e
[(1/10) ln (4/7)]t
10
4
1
ln }} 5 }} ln }} t
21
7
10
1
2
10
1 2
10 ln }}
21
t 5 }}
< 13.26
4
ln }}
172
It takes about 13.26 minutes
(4/7)]t
in 12,571 B.C.
(b) e2kt 5 0.18
2kt 5 ln 0.18
ln 0.18
k
5700 ln 0.18
ln 2
t 5 2}} 5 2}} < 14,101 years
The animal died about 14,101 years before A.D. 2000,
in 12,101 B.C.
262
Section 6.4
22. continued
26.
(c) e2kt 5 0.16
2kt 5 ln 0.16
ln 0.16
k
5700 ln 0.16
ln 2
t 5 2}} 5 2}} < 15,070 years
The animal died about 15,070 years before A.D. 2000,
0.2 5 e20.1t
ln 0.2 5 20.1t
t 5 210 ln 0.2 < 16.09 yr
It will take about 16.09 years.
dp
dn
dp
}} 5 k dh
p
dp
}} 5 k dh
p
27. (a) }} 5 kp
in 13,070 B.C.
E
23. Note that the total mass is 66 1 7 5 73 kg.
v 5 v0e2(k/m)t
v 5 9e23.9t/73
E
ln )p) 5 kh 1 C
eln )p) 5 e kh1C
2190
13
(a) s(t) 5 9e23.9t/73dt 5 2}}e23.9t/73 1 C
)p) 5 eCe kh
2190
13
Since s(0) 5 0 we have C 5 }} and
lim s(t) 5 lim }}(1 2 e23.9t/73) 5 }} < 168.5
p 5 Ae kh
The cyclist will coast about 168.5 meters.
Initial condition: p 5 p0 when h 5 0
2190
t→` 13
t→`
(b)
1 5 9e
2190
13
p0 5 Ae0
23.9t/73
A 5 p0
3.9t
}} 5 ln 9
73
73 ln 9
t 5 }} < 41.13 sec
3.9
Solution: p 5 p0e kh
Using the giving altitude-pressure data, we have
It will take about 41.13 seconds.
p0 5 1013 millibars, so:
24. v 5 v0e2(k/m)t
p 5 1013e kh
v 5 9e2(59,000/51,000,000)t
90 5 1013e(k)(20)
v 5 9e259t/51,000
90
}} 5 e20k
1013
1
90
k 5 }} ln }} < 20.121 km21
20
1013
E
459,000
59
459,000
Since s(0) 5 0, we have C 5 }} and
59
459,000
259t/51,000
lim s(t) 5 lim }}(1 2 e
)
59
t→`
t→`
459,000
5 }} < 7780 m
59
(a) s(t) 5 9e259t/51,000 dt 5 2}}e59t/51,000 1 C
The ship will coast about 7780 m, or 7.78 km.
1 5 9e
(b)
259t/51,000
59t
}} 5 ln 9
51,000
51,000 ln 9
t 5 }} < 1899.3 sec
59
It will take about 31.65 minutes.
25.
E
y 5 y0e2kt
800 5 1000e2(k)(10)
0.8 5 e
ln 0.8
10
1013e((1/20) ln (90/1013))(50) < 2.383 millibars.
(c)
900 5 1013e kh
900
}} 5 e kh
1013
1
20 ln (900/1013)
900
h 5 }} ln }} 5 }} < 0.977 km
k
ln (90/1013)
1013
The pressure is 900 millibars at an altitude of about
0.977 km.
28. By the Law of Exponential Change, y 5 100e20.6t. At
t 5 1 hour, the amount remaining will be
100e20.6(1) < 54.88 grams.
(b) 0.1 5 e2(1/40)t
k 5 2}}
At t 5 10 1 14 5 24 h:
y 5 1000e2(2ln 0.8/10)24
5 1000e
(b) At 50 km, the pressure is
29. (a) By the Law of Exponential Change, the solution is
V 5 V0e2(1/40)t.
210k
2.4 ln 0.8
Thus, we have p < 1013e20.121h
< 585.4 kg
About 585.4 kg will remain.
t
40
ln 0.1 5 2}}
t 5 240 ln 0.1 < 92.1 sec
It will take about 92.1 seconds.
Section 6.4
30. (a) A(t) 5 A0e t
It grows by a factor of e each year.
34. (a) T 2 Ts 5 79.47(0.932)t
(b) T 5 10 1 79.47(0.932)t
(b) 3 5 e
ln 3 5 t
It will take ln 3 < 1.1 yr.
t
(c) In one year your account grows from A0 to A0e, so you
can earn A0e 2 A0, or (e 2 1) times your initial
amount. This represents an increase of about 172%.
E
vm
31. (a) s(t) 5 v0e2(k/m)t dt 5 2}0}e2(k/m)t 1 C
k
Initial condition: s(0) 5 0
[0, 35] by [0, 90]
(c) Solving T 5 12 and using the exact values from the
regression equation, we obtain t < 52.5 sec.
(d) Substituting t 5 0 into the equation we found in part
(b), the temperature was approximately 89.478C.
vm
0 5 2}0} 1 C
k
vm
}0} 5 C
k
vm
vm
s(t) 5 2}0}e2(k/m)t 1 }0}
k
k
vm
5 }0} 1 2 e2(k/m)t
k
1
dT
}} 5 2k dt
T 2 Ts
1
2
dT
E}
} 5 2k dt
T2T
s
vm
(b) lim s(t) 5 lim }0} 1 2 e2(k/m)t 5 }0}
t→`
32. (a)
dT
}} 5 2k(T 2 Ts)
dt
35. (a)
2
vm
t→`
k
ln )T 2 Ts) 5 2kt 1 C
k
)T 2 Ts) 5 e2kt1C
90 5 e(r)(100)
ln 90 5 100r
T 2 Ts 5 6eCe2kt
ln 90
100
r 5 }} < 0.045 or 4.5%
(b)
T 2 Ts 5 Ae2kt
131 5 e(r)(100)
Initial condition: T 5 T0 when t 5 0
ln 131 5 100r
T0 2 Ts 5 Ae2(k)(0)
ln 131
100
r 5 }} < 0.049 or 4.9%
vm
33.
}0} 5 coasting distance
k
(0.80)(49.90)
}} 5 1.32
k
998
k 5 }}
33
vm
20
k
998
We know that }0} 5 1.32 and }} 5 }} 5 }}.
33
k
m
33(49.9)
Using Equation 3, we have:
T0 2 Ts 5 A
Solution: T 2 Ts 5 (T0 2 Ts)e2kt
(b) lim T 5 lim [Ts 1 (T0 2 Ts)e2kt] 5 Ts
t→`
36. (a) 2y0 5 y0e rt
2 5 e rt
vm
k
ln 2 5 rt
5 1.32(1 2 e220t/33)
ln 2
r
t 5 }}
< 1.32(1 2 e20.606t)
A graph of the model is shown superimposed on a graph of
the data.
t→`
Horizontal asymptote: T 5 Ts
s(t) 5 }0}(1 2 e2(k/m)t)
(b)
[0, 0.1] by [0, 100]
[0, 4.7] by [0, 1.4]
263
0.69
r
(c) ln 2 < 0.69, so the doubling time is }} which is
almost the same as the rules.
70
5
72
5
(d) }} 5 14 years or }} = 14.4 years
264
Section 6.4
r 5 0.5
36. continued
(e) 3y05y0e rt
ln 35 rt
ln 3
r
t 5}}
108
100r
108
i
Since ln 3 < 1.099, a suitable rule is }} or }}.
(We choose 108 instead of 110 because 108 has more
factors.)
1.6289
1.6467
1.6485
1.6487
1.6487
e 0.5 < 1.6487
Graphical support:
0.5 x
x
1
2
y1 5 1 1 }} , y2 5 e0.5
1
1 x
1 1 }}
x
x
10
100
1000
10,000
100,000
2
2.5937
2.7048
2.7169
2.7181
2.7183
[0, 10] by [0, 3]
(c) As we compound more times, the increment of time
between compounding approaches 0. Continuous
compounding is based on an instantaneous rate of
change which is a limit of average rates as the
increment in time approaches 0.
e < 2.7183
Graphical support:
1 x
x
1
2
y1 5 1 1 }} , y2 5 e
38. (a) To simplify calculations somewhat, we may write:
[0, 50] by [0, 4]
(b) r 5 2
11 1 }2x}2
x
10
100
1000
10,000
100,000
6.1917
7.2446
7.3743
7.3876
7.3889
e 2 < 7.389
Graphical support:
2 x
y1 5 1 1 }} , y2 5 e 2
x
2
[0, 500] by [0, 10]
x
mg e at 2 e2at eat
}} }
} }}
k eat 1 e2at eat
2at
mg e 2 1
}} }
}
k e2at 1 1
mg (e2at 1 1) 2 2
}} }}
e2at 1 1
k
!§§
5 !§§
5 !§§
mg
2
5 !}
}
§k}§11 2 }
e 1 12
v(t) 5
1
x
10
100
1000
10,000
100,000
3 5 ert
37. (a)
11 1 }0x.5}2
x
2at
The left side of the differential equation is:
!}§k}§(2)(e2at 1 1)22 (2ae2at)
mg
5 4ma !}
§k}§ (e2at 1 1)22 (e2at)
gk mg 2at
5 4m !}§}§ !}
} (e 1 1)22(e 2at)
m §k§
dv
dt
m }} 5 m
mg
4mge 2at
(e 1 1)
5}
2at }
2
Section 6.5
The right side of the differential equation is:
1 k 21
mg
2
2
11
2
mg 2 kv 2 5 mg 2 k }} 1 2 }
2at }
3
e
1
2
2
11
24
5 mg 1 2 1 2 }
2at }
e
1
4
11
4
1 1)
2
5 mg 1 2 1 1 }
2at } 2 }
2at }
2
e
(e
4(e 1 1) 2 4
(e 1 1)
2at
5 mg }
2at }
2
4 mg e2at
(e 11)
5}
2at }
2
Since the left and right sides are equal, the differential equation is satisfied.
And v(0) 5
mg e0 2 e0
} 5 0, so the initial condition is also satisfied.
!}§k}§ }
e 1e
0
0
mg eat 2 e2at
e2at
1 }} }} ? }e }2
t→`
t→` !§k§ e 1 e
mg 1 2 e
5 lim 1!}
}2
§k}§ }
11e
t→`
mg 1 2 0
mg
5 !}
} 5 }}
§k}§1}
1 1 0 2 !§k§
mg
The limiting velocity is!}
§k}§.
(b) lim v(t) 5 lim
at
2at
2a t
22at
22at
(c)
!}§k}§ 5 !}
§0§.0}
§0§5 < 179 ft/sec
mg
160
The limiting velocity is about 179 ft/sec,
or about 122 mi/hr.
■ Section 6.5 Population Growth
(pp. 342–349)
Quick Review 6.5
1. All real numbers
50
110
2. lim f (x) 5 }} 5 50
x→`
lim f (x) 5 0
x→2`
3. y 5 0, y 5 50
4. In both f 9 and f 0, the denominator will be a power of
1 1 5e 20.1x, which is never 0. Thus, the domains of both are all real numbers.
5.
[230, 70] by [210, 60]
f (x) has no zeros.
265
266
Section 6.5
6. Use NDER f (x), or calculate the derivative as follows.
d
50
dx 1 1 5e
(1 1 5e20.1x)(0) 2 (50)(5e20.1x)(20.1)
5 }}}}
(1 1 5e20.1x)2
20.1x
25e
5 }}
(1 1 5e20.1x)2
f9(x) 5 }} }}
20.1x
[230, 70] by [20.5, 2]
(a) (2`, `)
(b) None
7. Use NDER(NDER f (x)), or calculate the second derivatives as follows.
d
25e20.1x
dx (1 1 5e
)
(1 1 5e20.1x)2(25e20.1x)(20.1) 2 (25e20.1x)(2)(1 1 5e20.1x)(5e20.1x)(20.1)
5 }}}}}}}}
(1 1 5e20.1x)4
20.1x
20.1x
22.5e
[(1 1 5e
) 2 2(5e20.1x]
5 }}}}
20.1x 3
(1 1 5e
)
12.5e20.2x 2 2.5e20.1x
5 }}}
(1 1 5e20.1x)3
f 0(x) 5 }} }}
20.1x 2
[230, 70] by [20.08, 0.08]
Locate the inflection point using graphical methods, or analytically as follows.
f 0(x) 5 0
20.2x
12.5e
2 2.5e20.1x
50
}}}
(1 1 5e20.1x)3
2.5e20.1x(5e20.1x 2 1) 5 0
1
5
e20.1x 5 }}
20.1x 5 2ln 5
x 5 10 ln 5 < 16.094
(a) Since f 0(x) . 0 for x , 10 ln 5, the graph of f is concave up on the interval (2`, 10 ln 5), or approximately (2`, 16.094).
(b) Since f 0(x) , 0 for x . 10 ln 5, the graph of f is concave down on the interval (10 ln 5, `), or approximately (16.094, `).
8. Using the result of the previous exercise, the inflection point occurs at x 5 10 ln 5.
50
1 1 5e
Since f (10 ln 5) 5 }}
2ln 5 5 25,
the point of inflection is (10 ln 5, 25), or approximately (16.094, 25).
x 2 12
x 2 4x
A
x
B
x24
9. }
2 } 5 }} 1 }}
x 2 12 5 A(x 2 4) 1 Bx
x 2 12 5 (A 1 B)x 2 4A
Since A 1 B 5 1 and 24A 5 212, we have A 5 3 and
B 5 22.
Section 6.5
2x 1 16
x 1x26
A
x13
B
x22
10. }
} 5 }} 1 }}
2
dP
k
dt
m
dP
0.02
}} 5 }}P(150 2 P)
dt
150
dP
1
}} 5 }}P(150 2 P)
dt
7500
4. (a) }} 5 }}P(M 2 P)
2x 1 16 5 A(x 2 2) 1 B(x 1 3)
When x 5 23, the equation becomes 10 5 25A, and when
x 5 2, the equation becomes 20 5 5B. Thus, A 5 22 and
B 5 4.
267
M
1 1 Ae
150
P 5 }}
1 1 Ae20.02t
(b) P 5 }}
2kt
Section 6.5 Exercises
Initial condition: P(0) 5 15
dP
1. (a) }} 5 0.025P
dt
150
1 1 Ae
150
1 1 A 5 }} 5 10
15
15 5 }}0
(b) Using the Law of Exponential Change from Section
6.4, the formula is P 5 75,000e 0.025t
A59
(c)
150
1 1 9e
Formula: P 5 }}
20.02t
(c)
[0, 100] by [0, 1,000,000]
dP
dt
2. (a) }} 5 0.019P
[0, 200] by [0, 200]
(b) Using the Law of Exponential Change from Section
6.4, the formula is P 5 110,000e0.019t.
(c)
5. The growth rate is 20.3 or 230%.
6. The growth rate is 0.075 or 7.5%.
dP
dt
7. }} 5 0.04P 2 0.0004P2
5 0.0004P(100 2 P)
0.04
100
k
5 }}P(M 2 P)
M
5 }}P(100 2 P)
[0, 100] by [0, 1,000,000]
dP
k
dt
M
dP
0.05
}} 5 }}P(200 2 P)
dt
200
dP
}} 5 0.00025P(200 2 P)
dt
3. (a) }} 5 }}P(M 2 P)
M
1 1 Ae
200
P 5 }}
1 1 Ae20.05t
(b) P 5 }}
2kt
Initial condition: P(0) 5 10
200
1 1 Ae
200
1 1 A 5 }} 5 20
10
10 5 }}0
A 5 19
200
1 1 19e
Formula: P 5 }}
20.05t
Thus, k 5 0.04 and the carrying capacity is M 5 100.
50
P
1
}}
P
dP
P
dt
250
dP
1
P
}} 5 }} 2 2 }}
dt
50
250
1
P
5 }} 1 2 }}
25
500
P
5 0.04 1 2 }}
500
P
5 k 1 2 }}
M
8. }} }} 5 2 2 }}
1
1
1
1
2
2
2
2
Thus, k 5 0.04 and the carrying capacity is M 5 500.
9. Choose the slope field that shows slopes that increase as y
increases. (d)
10. Choose the slope field that matches a logistic differential
equation with M 5 100. (b)
11. Choose the only slope field whose slopes vary with x as
well as with y. (c)
(c)
12. Choose the slope field that matches a logistic differential
equation with M 5 150. (a)
[0, 100] by [0, 250]
268
Section 6.5
1000
11e
1000
5 }4.}
1 1 e 8e20.7t
M
5 }}
1 1 Ae2kt
dP
dt
13. (a) P(t) 5 }4}
.820.7t
17. (a) }} 5 0.0015P(150 2 P)
0.225
150
k
5 }}P(M 2 P)
M
5 }}P(150 2 P)
This is a logistic growth model with k 5 0.7 and
M 5 1000.
Thus, k 5 0.225 and M 5 150.
M
1 1 Ae
150
5 }}
1 1 Ae20.225t
P 5 }}
2kt
1000
<8
(b) P(0) 5 }}
1 1 e4.8
Initially there are 8 rabbits.
Initial condition: P(0) 5 6
150
1 1 Ae
6 5 }}0
200
11e
200
5 }}
1 1 e 5.3e2t
M
5 }}
1 1 Ae2kt
14. (a) P(t) 5 }}
5.32t
1 1 A 5 25
A 5 24
150
1 1 24e
Formula: P 5 }}
20.225t
This is a logistic growth model with k 5 1 and
M 5 200.
(b)
200
11e
(b) P(0) 5 }}
5.3 < 1
Initially 1 student has the measles.
?
?
15. (a) Note that }} 5 }} ? }}
dP
dT
1 person
14 sec
365 24 3600 sec
1 yr
< 2,252,571 people per year.
The relative growth rate is
dP
}}
dT
2,252,571
} < }} < 0.00875 or 0.875%
P
257,313,431
(b) The population after 8 years will be approximately
P0e rt 5 257,313,431e 8r
< 275,980,017, where r is the unrounded rate
from part (a).
150
1 1 24e
3
1 1 24e20.225t 5 }}
2
1
20.225t
24e
5 }}
2
1
e20.225t 5 }}
48
100 5 }}
20.225t
20.225t 5 2ln 48
ln 48
0.225
150
125 5 }}
1 1 24e20.225t
6
1 1 24e20.225t 5 }}
5
1
24e20.225t 5 }}
5
1
e20.225t 5 }}
120
t 5 }} < 17.21 weeks
20.225t 5 2ln 120
ln 120
0.225
t 5 }} < 21.28
16. (a) Let t be the number of years.
1000 5 10,000(0.8)t
0.1 5 0.8 t
ln 0.15 t ln 0.8
ln 0.1
ln 0.8
t 5 }} < 10.32
It will take about 10.32 years.
(b) Let f (t) 5 10,000(0.8)t. So that f (t) will round to less
than 1, we actually require f (t) , 0.5.
0.5 5 10,000(0.8)t
0.00005 5 0.8t
ln 0.00005 5 t ln 0.8
ln 0.00005
ln 0.8
t 5 }} < 44.38
It will take about 44.4 years.
It will take about 17.21 weeks to reach 100 guppies,
and about 21.28 weeks to reach 125 guppies.
Section 6.5
Now find the time to grow from 10,000 bees to 25,000
bees.
dP
dt
18. (a) }} 5 0.0004P(250 2 P)
0.1
250
k
5 }}P(M 2 P)
M
5 }}P(250 2 P)
dP
1
}} 5 }}P
dt
12
P(t) 5 10,000e t/12
Thus, k 5 0.1 and M 5 250.
25,000 5 10,000e t/12
M
1 1 Ae
250
5 }}
1 1 Ae 20.1t
2.5 5 e t/12
P 5 }}
2kt
t
12
ln 2.5 5 }}
Initial condition: P(0) 5 28, where t 5 0 represents the
year 1970.
250
1 1 Ae
28 5 }}0
250
111
A 5 }} 2 1 5 }} < 7.9286
28
14
250
Formula: P(t) 5 }}
, or approximately
1 1 111e20.1t/14
250
P(t) 5 }}
1 1 7.9286e20.1t
(b) The population P(t) will round to 250 when
249.5 5 }}
20.1t
111e20.1t
14
(249.5)(111e20.1t)
}} 5 0.5
14
14
e20.1t 5 }}
55,389
14
20.1t 5 ln }}
55,389
1
/14
2
249.5 1 1 }} 5 250
t 5 10(ln 55,389 2 ln 14) < 82.8
It will take about 83 years.
19. (a) y 5 y0e20.01(t/1000) 5 y0e20.00001t
20.00001t
0.9 5 e
ln 0.9 5 20.00001t
t 5 2100,000 ln 0.9 < 10,536
It will take about 10,536 years.
(c) y 5 y0e2(0.00001)(20,000) < 0.819y0
The tooth size will be about 81.9% of our present tooth
size.
20. First find the time to grow from 5000 bees to 10,000 bees.
dP
1
}} 5 }}P
dt
4
P(t) 5 5000e0.25t
10,000 5 5000e0.25t
2 5 e0.25t
ln 2 5 0.25t
4 ln 2 5 t
The total time required is 4 ln 2 1 12 ln 2.5 < 13.8 years.
dx
}} 5 1000 1 0.10x
dt
dx
E}
} 5 Edt
1000 1 0.1x
10 ln )1000 1 0.1x) 5 t 1 C
ln )1000 1 0.1x) 5 0.1(t 1 C)
1000 1 0.1x 5 6e0.1(t1C)
0.1x 5 21000 6 e0.1C e0.1t
x 5 210,000 6 10e0.1C e0.1t
P(t) $ 249.5.
250
1 1 111e
12 ln 2.5 5 t
21. (a)
28(1 1 A) 5 250
(b)
269
x 5 210,000 1 Ae0.1t
Initial condition: x(0) 5 1000
1000 5 210,000 1 Ae0
11,000 5 A
Solution: x 5 11,000e0.1t 2 10,000
(b) 100,000 5 11,000e0.1t 2 10,000
10 5 e0.1t
ln 10 5 0.1t
t 5 10 ln 10 < 23 yr
It will take about 23 years.
22. (a) Using the Law of Exponential Change in Section 6.4,
the solution is p(x) 5 p0e2x/100, where p0 5 p(0).
Initial condition: p(100) 5 20.09
20.09 5 p0e21
20.09e 5 p0
Solution: p(x) 5 (20.09e)e2x/100
or p(x) 5 20.09e120.01x
(b) p(10) 5 20.09e0.9 < $49.41
p(90) 5 20.09e0.1 < $22.20
(c) r(x)5 xp(x) 5 20.09x e120.01x
r9(x) 5 20.09[(x)(e120.01x)(20.01) 1 (e120.01x)(1)]
5 20.09e120.01x(1 2 0.01x)
The derivative is zero at x 5 100, positive for x , 100,
and negative for x . 100, so r(x) has its maximum
value at x 5 100.
270
Section 6.5
23. (a) Note that the given years correspond to x 5 0, x 5 20,
16.90
1 1 5.132e
26. (a) y 5 }}
20.0666x
x 5 50, x 5 70, and x 5 80.
(b) Carrying capacity 5 lim y 5 16.90 representing
18.70
1 1 1.075e
y 5 }}
20.0422x
x→`
16.9 million people.
dy
dx
27. }} 5 (cos x)e sin x
Edy 5 E(cos x)e
Edy 5 Ee du
sin x
dx
u
[0, 100] by [0, 20]
y 5 eu 1 C
(b) Carrying capacity 5 lim y 5 18.70, representing
18.7 million people. x→`
y 5 e sin x 1 C
(c) Using NDER twice and solving graphically, we find
that y 0 5 0 when x < 1.7, corresponding to the year
1912. The population at this time was about
y(1.7) < 9.35 million.
Initial value: y(0) 5 0
0 5 esin 0 1 C
21 5 C
Solution: y 5 e sin x 2 1
24.76
1 1 7.195e
24. (a) y 5 }}
20.0513x
28.
dy
}} 5 22(y 2 3)
dx
dy
}}5 22 dx
y23
E
E
ln )y 2 3)5 22x 1 C
[0, 50] by [0, 15]
y 2 35 6e22x1C
(b) Carrying capacity 5 lim y 5 24.76, representing
y 5 3 1 Ae22x
x→`
Initial condition: y(0) 5 5
24.76 million people.
5 5 3 1 Ae0
(c) Using NDER twice and solving graphically, we find
that y 0 5 0 when x < 38.44, corresponding to the year
1988. The population at this time was about
y(38.44) < 12.38 million.
25.
dP
}}
dt
M dP
}}
P(M 2 P)
(M 2 P) 1 P
}} dP
P(M 2 P)
1
1
}} 1 }} dP
P
M2P
1
2
k
M
2 5A
Solution: y 5 3 1 2e22x
5 }}P(M 2 P)
29.
5 k dt
5 k dt
dy
x
}} 5 }}
dx
y
Ey dy 5 Ex dx
y2
x2
}} 5 }} 1 C
2
2
5 k dt
Initial condition:
ln )P) 2 ln )M 2 P) 5 kt 1 C
) M P2 P )
M2P
ln )}}) 5 2kt 2 C
P
ln }} 5 kt 1 C
M2P
}} 5 6e2Ce2kt
P
M2P
}} 5 Ae2kt
P
M 2 P 5 APe2kt
M 5 P(1 1 Ae2kt)
M
P 5 }}
2kt
1 1 Ae
y(0) 5 2
22
02
}} 5 } } 1 C
2
2
2 5C
y2
2
x2
2
This gives }} 5 }} 1 2, or y 2 5 x 2 1 4.
But this equation represents two functions, y 5 6Ïw
x 2w
1w4.
The solution of the initial value problem is the function that
x 2w
1w4.
satisfies the initial condition, namely y 5 Ïw
Section 6.5
30.
dy
}} 5 yÏxw
dx
dy
}} 5 x1/2 dx
y
2
ln )y) 5 }}x3/2 1 C
3
E
(c)
E
1200Ae0 1 100
1 1 Ae
300 5 }}
0
300(1 1 A) 5 1200A 1 100
300 2 100 5 1200A 2 300A
200 5 900A
3/21C
)y) 5 e(2/3)x
3/2
2
9
1200(2/9)e11kt/12 1 100
P(t) 5 }}}
1 1 (2/9)e11kt/12
1200(2)e11kt/12 1 100(9)
P(t) 5 }}}
9 1 2e11k/12
300(8e11kt/12 1 3)
P(t) 5 }}
9 1 2e11kt/12
y 5 6eCe(2/3)x
y 5 Ae(2/3)x
271
A 5 }}
3/2
Initial condition: y(0) 5 1
1 5 Ae0
15A
Solution: y 5 e(2/3)x
(d)
3/2
dP
dt
31. (a) Note that k . 0 and M . 0, so the sign of }} is the
same as the sign of (M 2 P)(P 2 m). For m , P , M,
[0, 75] by [0, 1500]
both M 2 P and P 2 m are positive, so the product is
Note that the slope field is given by
positive. For P , m or P . M, the expressions M 2 P
dP
0.1
}} 5 }}(1200 2 P)(P 2 100).
dt
1200
and P 2 m have opposite signs, so the product is
negative.
dP
dP
M
}} }} 5 k
(M 2 P)(P 2 m) dt
k
(b) }} 5 }}(M 2 P)(P 2 m)
dt
M
dP
M
M 2m
}} }} }} 5 k
M 2 m (M 2 P)(P 2 m) dt
(P 2 m) 1 (M 2 P) dP
M2m
}}} }} 5 }}k
(M 2 P)(P 2 m) dt
M
dP
k
}} 5 }}(1200 2 P)(P 2 100)
dt
1200
1200
dP
}}} }} 5 k
(1200 2 P)(P 2 100) dt
(P 2 100) 1 (1200 2 P) dP
11
}}} }} 5 }}k
(1200 2 P)(P 2 100) dt
12
} 1 }}2 }} 5 }}k
1}
12
1200 2 P
P 2 100 dt
1
dP
1
11
11
1
1
E1}
} 1 }}2 dP 5 }} k dt
12
1200 2 P
P 2 100
11
12
2ln )1200 2 P) 1 ln )P 2 100) 5 }}kt 1 C
P 2 100
)
11
ln }} 5 }}kt 1 C
12
1200 2 P
P 2 100
}} 5 6eCe11kt/12
1200 2 P
P 2 100
}} 5 Ae11kt/12
1200 2 P
P 2 100 5 1200Ae11kt/12 2 APe11kt/12
P(1 1 Ae11kt/12) 5 1200Ae11kt/12 1 100
1200Ae11kt/12 1 100
1 1 Ae
P 5 }}}
11kt/12
M2m
} 1 }}2 }} 5 }}k
1}
M
M2P
P 2 m dt
M2m
1
1
E1}
} 1 }}2 dP 5 E}}k dt
M
M2P
P2m
1
1100
dP
11
}}} }} 5 }}k
(1200 2 P)(P 2 100) dt
12
)
dP
k
}} 5 }}(M 2 P)(P 2 m)
dt
M
(e)
dP
1
M2m
M
M2m
P2m
ln }} 5 }}kt 1 C
M
M2P
P2m
}} 5 6e Ce (M2m)kt/M
M2P
P2m
}} 5 Ae (M2m)kt/M
M2P
2ln )M 2 P) 1 ln )P 2 m)5 }}kt 1 C
)
)
P 2 m 5 (M 2 P)Ae (M2m)kt/M
P(1 1 Ae (M2m)kt/M) 5 AMe (M2m)kt/M 1 m
AMe (M2m)kt/M 1 m
1 1 Ae
P 5 }}
(M2m)kt/M
AM e 0 1 m
1 1 Ae
AM 1 m
11A
P(0) 5 }}
0 5 }}
P(0)(1 1 A) 5 AM 1 m
A(P(0) 2 M) 5 m 2 P(0)
m 2 P(0)
P(0) 2 M
P(0) 2 m
M 2 P(0)
A 5 }} 5 }}
Therefore, the solution to the differential equation is
AMe (M2m)kt/M 1 m
1 1 Ae
P(0) 2 m
M 2 P(0)
P 5 }}
(M2m)kt/M where A 5 }}.
272
Section 6.6
32. (a)
E
■ Section 6.6 Numerical Methods
dp
}} 5 k(t)p
dt
dp
}} 5 k(t) dt
p
(pp. 350–356)
E
ln ) p) 5 E k(u) du 1 C
Quick Review 6.6
t
1. f9(x) 5 3x 2 2 3
f9(2) 5 3(2)2 2 3 5 9
E k(u) du
0
t
p 5 6eCe 0
2. L(x) 5 f (2) 1 f9(2)(x 2 2)
5 2 1 9(x 2 2)
5 9x 2 16
E k(u) du
t
p 5 Ae 0
Initial condition: p(0) 5 p0.
E k(u) du
3. f9(x) 5 sec2 x
0
p0 5 Ae 0
p0 5 Ae
p
p0 5 A
p
142
t
0
E
9
0
k(u) du 5
p
1 4 21
p
5 1 1 21x 2 }}2
4
p
4
4. L(x) 5 f }} 1 f9 }} x 2 }}
E k(u) du
Solution: p(t) 5 p e
(b)
p
4
142
f9 }} 5 sec2 }} 5 (Ï2w)2 5 2
0
0
2
p
2
5 2x 1 1 2 }}
0.04
E}
} du
11u
9
0
4
5 0.04 ln (1 1 u)
5. f9(x) 5 0.2x 2 5x22
f9(4) 5 0.2(4) 2 5(4)22 5 0.4875
9
0
6. L(x) 5 f (4) 1 f9(4)(x 2 4)
5 2.85 1 0.4875(x 2 4)
5 0.4875x 1 0.9
5 0.04(ln 10 2 ln 1)
5 0.04 ln 10
E k(u) du
9
7. L(4.1) 5 0.4875(4.1) 1 0.9 5 2.89875
p(9) 5 p0e 0
5
4.1
f (4.1) 5 0.1(4.1)2 1 }} < 2.900512
5 100e0.04 ln 10 < 109.65
After 9 years during which the inflation rate is
(a) )L(4.1) 2f (4.1)) < 0.001762
0.04
}} per year, the price of an item which originally
11t
(b) }} < 0.00061 5 0.061%
)L(4.1) 2 f (4.1))
f (4.1)
cost $100 will be increased to $109.65.
E 0.04 du 5 100e0.04(9) < 143.33
p(9) 5 p e
9
(c)
0
0
The price will be $143.33.
E
9
(d)
0
k(u) du 5
E (0.04 1 0.004u) du
p(9) 5 p0
33. (a)
EP
)L(4.2) 2 f (4.2))
f (4.2)
(b) }} < 0.00236 5 0.236%
0
3
4
9
5 0.522
E k(u) du 5 100e0.522 < 168.54
e
9
0
0
E
5
4.5
f (4.5) 5 0.1(4.5)2 1 }} < 3.136111
)L(4.5) 2 f (4.5))
f (4.5)
(b) }} < 0.01351 5 1.351%
dP 5 k dt
2P21 5 kt 1 C
10. L(3.5) 5 0.4875(3.5) 1 0.9 5 2.60625
1
kt 1 C
P 5 2 }}
5
3.5
f (3.5) 5 0.1(3.5)2 1 }} < 2.653571
Initial condition: P(0) 5 P0
1
C
1
C 5 2}}
P0
9. L(4.5) 5 0.4875(4.5) 1 0.9 5 3.09375
(a) )L(4.5) 2 f (4.5)) < 0.042361
dP
}} 5 kP2
dt
22
5
4.2
f (4.2) 5 0.1(4.2)2 1 }} < 2.954476
(a) )L(4.2) 2 f (4.2)) < 0.006976
9
5 0.04u 1 0.002u2
8. L(4.2) 5 0.4875(4.2) 1 0.9 5 2.9475
(a) )L(3.5) 2 f (3.5)) < 0.047321
P0 5 2}}
)L(3.5) 2 f (3.5))
f (3.5)
(b) }} < 0.01783 5 1.783%
1
kt 2 (1/P0)
P
0
Solution: P 5 2}} 5 }}
1 2 kP0t
1
kP0
(b) There is a vertical asymptote at t 5 }}
Section 6.6
y 5 6e C e x 2 1
Section 6.6 Exercises
y 5 Ae x 2 1
1. Check the differential equation:
d
dx
y9 5 }}(x 2 1 1 2e2x) 5 1 1 2e2x(21) 5 1 2 2e2x
2x
x 2 y 5 x 2 (x 2 1 1 2e ) 5 1 2 2e
Initial condition: y(0) 5 1
1 5 Ae0 2 1
25A
Solution: y 5 2 e x 2 1
2x
Therefore, y9 5 x 2 y.
6.
Check the initial condition:
y(0) 5 0 2 1 1 2e2(0) 5 21 1 2 5 1
2. Check the differential equation:
dy
}} 5 x(1 2 y)
dx
dy
}} 5 x dx
12y
1
2ln )1 2 y) 5 }}x 2 1 C
2
E
E
)1 2 y) 5 e2(x /2)2C
2
d
y9 5 }}(x 2 1 2 e2x) 5 1 2 e2x(21) 5 1 1 e2x
dx
2x
x 2 y 5 x 2 (x 2 1 2 e ) 5 1 1 e
1 2 y 5 6e2(x /2)2C
2
2x
y 5 6e2Ce2x /2 1 1
2
Therefore, y9 5 x 2 y.
y 5 Ae2x /2 1 1
2
Check the initial condition:
Initial condition: y(22) 5 0
2
0 5 Ae2(22) /2 1 1
22
0 5 Ae 1 1
2e2 5 A
2
2
Solution: y 5 2e2 e2x /2 1 1 or y 5 2e2(x /2)12 1 1
y(0) 5 0 2 1 2 e2(0) 5 21 2 1 5 22
3. Check the differential equation:
2 e2x 2 2 cos x 1 sin x
d e2x 2 2 sin x 2 cos x
5
5
dx
e2x 2 2 sin x 2 cos x
2y 1 sin x5 2 }}} 1 sin x
5
2e2x 2 4 sin x 2 2 cos x 1 5 sin x
5 }}}}
5
2 e2x 2 2 cos x 1 sin x
5 }}}
5
1
2
y9 5 }} }}} 5 }}}
1
dy
}} 5 2y(x 1 1)
dx
dy
}} 5 2(x 1 1) dx
y
dy
}} 5 (2x 1 2) dx
y
7.
2
E
E
ln )y) 5 x 2 1 2x 1 C
)y) 5 e x 12x1C
2
Therefore, y9 5 2y 1 sin x
y 5 6eC e x 12x
Check the initial condition:
y 5 A e x 12x
e2(0) 2 2 sin 0 2 cos 0
5
2
2
121
5
Initial condition: y(22) 5 2
2
2 5 Ae(22) 12(22)
25A
2
Solution: y 5 2e x 12x
y(0) 5 }}} 5 }} 5 0
4. Check the differential equation:
d
dx
y9 5 }}(e x 2 e2x 2 1) 5 e x 2 2e2x
y 2 e2x 1 1 5 (e x 2 e2x 2 1) 2 e2x 1 1 5 ex 2 2e2x
Therefore, y9 5 y 2 e 1 1.
2x
8.
Ey
22
y(0) 5 e 2 e
2(0)
2 1 5 21
5. Note that we are finding an exact solution to the initial
value problem discussed in Examples 1–4.
dy
}} 5 1 1 y
dx
dy
}} 5 dx
11y
E
E
ln)1 1 y) 5 x 1 C
)1 1 y) 5 e x1C
1 1 y 5 6e x1C
E
dy 5 (1 1 2x) dx
2y21 5 x 1 x 2 1 C
Check the initial condition:
0
dy
}} 5 y 2(1 1 2x)
dx
1
x 1x1C
y 5 2}
}
2
Initial condition: y(21) 5 21
1
(21) 1 (21) 1 C
1
21 5 2}}
C
21 5 2}
}
2
C51
1
x 1x11
Solution: y 5 2}
}
2
273
274
Section 6.6
9. To find the approximate values, set y1 5 2y 1 sin x and use
EULERT with initial values x 5 0 and y 5 0 and step size
0.1 for 10 points. The exact values are given by
1
5
y 5 }}(e2x 2 2 sin x 2 cos x).
x
y (Euler) y (exact)
Error
11. To find the approximate values, set y1 5 2y(x 1 1) and use
IMPEULT with initial values x 5 22 and y 5 2 and
step size 0.1 for 20 points. The exact values are given by
2
y 5 2e x 12x.
x
y
1 improved
Euler 2
y (exact)
Error
0
0
0
0
0.1
0
0.0053
0.0053
22
2
2
0
0.2
0.0100
0.0229
0.0129
21.9
1.6560
1.6539
0.0021
1.3983
1.3954
0.0030
0.3
0.0318
0.0551
0.0233
21.8
0.4
0.0678
0.1051
0.0374
21.7
1.2042
1.2010
0.0032
1.0578
1.0546
0.0032
0.5
0.1203
0.1764
0.0561
21.6
0.6
0.1923
0.2731
0.0808
21.5
0.9478
0.9447
0.0031
0.8663
0.8634
0.0029
0.7
0.2872
0.4004
0.1132
21.4
0.8
0.4090
0.5643
0.1553
21.3
0.8077
0.8050
0.0027
0.7683
0.7658
0.0025
0.9
0.5626
0.7723
0.2097
21.2
1.0
0.7534
1.0332
0.2797
21.1
0.7456
0.7432
0.0024
21.0
0.7381
0.7358
0.0023
20.9
0.7455
0.7432
0.0023
20.8
0.7682
0.7658
0.0024
20.7
0.8075
0.8050
0.0024
Error
20.6
0.8659
0.8634
0.0025
0
20.5
0.9473
0.9447
0.0026
21.8000 21.8048 0.0048
20.4
1.0572
1.0546
0.0026
0.2
21.6100 21.6187 0.0087
20.3
1.2036
1.2010
0.0026
0.3
21.4290 21.4408 0.0118
20.2
1.3976
1.3954
0.0022
0.4
21.2561 21.2703 0.0142
20.1
1.6553
1.6539
0.0014
0.5
21.0905 21.1065 0.0160
0
1.9996
2
0.0004
0.6
20.9314 20.9488 0.0174
0.7
20.7783 20.7966 0.0183
0.8
20.6305 20.6493 0.0189
0.9
20.4874 20.5066 0.0191
1.0
20.3487 20.3679 0.0192
10. To find the approximate values, set y1 5 x 2 y and use
EULERT with initial values x 5 0 and y 5 22 and step
size 0.1 for 10 points. The exact values are given
by y 5 x 2 1 2 e2x.
x
0
0.1
y (Euler) y (exact)
22
22
Section 6.6
12. To find the approximate values, set y1 5 x(1 2 y) and use IMPEULT with initial values x 5 22 and y 5 0 and
2
step size 0.1 for 20 points. The exact values are given by y 5 2e2(x /2)12 1 1.
1 improved
Euler 2
y (exact)
Error
22
0
0
0
21.9
20.2140
20.2153 0.0013
21.8
20.4593
20.4623 0.0029
21.7
20.7371
20.7419 0.0049
21.6
21.0473
21.0544 0.0071
21.5
21.3892
21.3989 0.0097
21.4
21.7607
21.7732 0.0125
21.3
22.1585
22.1740 0.0155
21.2
22.5780
22.5966 0.0186
21.1
23.0131
23.0350 0.0219
21.0
23.4565
23.4817 0.0252
20.9
23.9000
23.9283 0.0284
20.8
24.3341
24.3656 0.0315
20.7
24.7491
24.7834 0.0344
20.6
25.1348
25.1719 0.0370
20.5
25.4815
25.5208 0.0394
20.4
25.7796
25.8210 0.0413
20.3
26.0210
26.0639 0.0430
20.2
26.1986
26.2427 0.0441
20.1
26.3073
26.3522 0.0449
0
26.3438
26.3891 0.0452
x
y
275
276
Section 6.6
13. To find the approximate values, set y1 5 x 2 y and use EULERT and IMPEULT with initial values x 5 0 and
y 5 1 and step size 0.1 for 20 points. The exact values are given by y 5 x 2 1 1 2e2x.
x
y (Euler)
y
1 improved
Euler 2
y (exact) Error (Euler)
Error
1
improved
Euler
0
1
1
1
0
0
0.1
0.9000
0.9100
0.9097
0.0097
0.0003
0.2
0.8200
0.8381
0.8375
0.0175
0.0006
0.3
0.7580
0.7824
0.7816
0.0236
0.0008
0.4
0.7122
0.7416
0.7406
0.0284
0.0010
0.5
0.6810
0.7142
0.7131
0.0321
0.0011
0.6
0.6629
0.6988
0.6976
0.0347
0.0012
0.7
0.6566
0.6944
0.6932
0.0366
0.0012
0.8
0.6609
0.7000
0.6987
0.0377
0.0013
0.9
0.6748
0.7145
0.7131
0.0383
0.0013
1.0
0.6974
0.7371
0.7358
0.0384
0.0013
1.1
0.7276
0.7671
0.7657
0.0381
0.0013
1.2
0.7649
0.8037
0.8024
0.0375
0.0013
1.3
0.8084
0.8463
0.8451
0.0367
0.0013
1.4
0.8575
0.8944
0.8932
0.0357
0.0012
1.5
0.9118
0.9475
0.9463
0.0345
0.0012
1.6
0.9706
1.0050
1.0038
0.0332
0.0012
1.7
1.0335
1.0665
1.0654
0.0318
0.0011
1.8
1.1002
1.1317
1.1306
0.0304
0.0011
1.9
1.1702
1.2002
1.1991
0.0290
0.0010
2.0
1.2432
1.2716
1.2707
0.0275
0.0010
2
Section 6.6
277
14. To find the approximate values, set y1 5 y 2 e2x 1 1 and use EULERT and IMPEULT with initial values x 5 0 and
y 5 21 and step size 0.1 for 20 points. The exact values are given by y 5 e x 2 e2x 2 1.
y (Euler)
x
y
1
improved
Euler
2
y (exact)
Error (Euler) Error
1
improved
Euler
0
21
21
21
0
0
0.1
21.1000
21.1161
21.1162
0.0162
0.0002
0.2
21.2321
21.2700
21.2704
0.0383
0.0004
0.3
21.4045
21.4715
21.4723
0.0677
0.0007
0.4
21.6272
21.7325
21.7337
0.1065
0.0012
0.5
21.9125
22.0678
22.0696
0.1571
0.0018
0.6
22.2756
22.4954
22.4980
0.2224
0.0026
0.7
22.7351
23.0378
23.0414
0.3063
0.0037
0.8
23.3142
23.7224
23.7275
0.4133
0.0050
0.9
24.0409
24.5832
24.5900
0.5492
0.0068
1.0
24.9499
25.6616
25.6708
0.7209
0.0092
1.1
26.0838
27.0087
27.0208
0.9370
0.0121
1.2
27.4947
28.6872
28.7031
1.2084
0.0159
1.3
29.2465
210.7738
210.7944
1.5480
0.0206
1.4
211.4175
213.3628
213.3894
1.9719
0.0267
1.5
214.1037
216.5696
216.6038
2.5001
0.0342
1.6
217.4227
220.5358
220.5795
3.1568
0.0437
1.7
221.5182
225.4345
225.4902
3.9720
0.0556
1.8
226.5664
231.4781
231.5486
4.9822
0.0705
1.9
232.7829
238.9262
239.0153
6.2324
0.0891
2.0
240.4313
248.0970
248.2091
7.7778
0.1121
dy
}} 5 2y 2(x 2 1)
dx
dy
}}2 5 2(x 2 1)dx
y
15. (a)
Ey
2
22
E
dy 5 (2x 2 2) dx
2y21 5 x 2 2 2x 1 C
1
2
Initial value: y (2) 5 2}}
2 5 22 2 2(2) 1 C
25C
1
x 2 2x 1 2
Solution: 2y21 5 x 2 2 2x 1 2 or y 5 2}
}
2
1
3 2 2(3) 1 2
1
5
y(3) 5 2}
} 5 2}} 5 20.2
2
1
2
(b) To find the approximation, set y1 5 2y 2(x 2 1) and use EULERT with initial values x 5 2 and y 5 2}} and step size 0.2 for
5 points. This gives y(3) < 20.1851; error < 0.0149.
(c) Use step size 0.1 for 10 points. This gives
y(3) < 20.1929; error < 0.0071.
(d) Use step size 0.05 for 20 points. This gives
y(3) < 20.1965; error < 0.0035.
278
16. (a)
Section 6.6
19. Set y1 5 2y 1 sin x and use EULERG with initial values
x 5 0 and y 5 0 and step size 0.1. The exact solution is
1
y 5 }}(e2x 2 2 sin x 2 cos x).
dy
}} 5 y 2 1
dx
dy
}} 5 dx
y21
E
E
5
ln )y 2 1) 5 x 1 C
)y 2 1) 5 e x1C
y 2 1 5 6eCe x
y 5 Ae x 1 1
[20.1, 1.1] by [20.13, 0.88]
20. Set y1 5 x 2 y and use EULERG with initial values
x 5 0 and y 5 22 and step size 0.1. The exact solution is
y 5 x 2 1 2 e2x.
Initial condition: y(0) 5 3
3 5 Ae0 1 1
25A
Solution: y 5 2e x 1 1
y(1) 5 2e 1 1 < 6.4366
(b) To find the approximation, set y1 5 y 2 1 and use
EULERT with initial values x 5 0 and y 5 3 and step
size 0.2 for 5 points. This gives y (1) < 5.9766;
error < 0.4599.
[20.1, 1.1] by [22.3, 0.3]
21. Set y1 5 2y(x 1 1) and use IMPEULG with initial values
x 5 22 and y 5 2 and step size 0.1. The exact solution is
2
y 5 2e x 12x.
(c) Use step size 0.1 for 10 points.
This gives y(1) < 6.1875; error < 0.2491.
(d) Use step size 0.05 for 20 points. This gives
y(1) < 6.3066; error < 0.1300.
1
x 2 2x 1 2
17. The exact solution is y 5 2}
}, so y(3) 5 20.2.
2
(a) To find the approximation, set y1 5 2y 2(x 2 1) and use
1
2
IMPEULT with initial values x 5 2 and y 5 2}} and
[22.2, 0.2] by [20.2, 2.2]
22. Set y1 5 x(1 2 y) and use IMPEULG with initial values
x 5 22 and y 5 0 and step size 0.1. The exact solution is
2
y 5 2e2(x /2)12 1 1.
step size 0.2 for 5 points. This gives y (3) < 20.2024;
error < 0.0024.
(b) Use step size 0.1 for 10 points. This gives
y(3) < 20.2005; error < 0.0005.
(c) Use step size 0.05 for 20 points. This gives
y(3) 5 20.2001; error < 0.0001.
(d) As the step size decreases, the accuracy of the method
increases and so the error decreases.
18. The exact solution is y 5 2e x 1 1, so
y(1) 5 2e 1 1 < 6.4366.
[22.2, 0.2] by [27.3, 1.1]
23. To find the approximate values, set y1 5 x 1 y and use
EULERT with initial values x 5 0 and y 5 1 and step size
20.1 for 10 points. The exact values are given by
y 5 2e x 2 x 2 1.
x
y (Euler) y (exact)
Error
0
1
1.0
0
20.1
0.9000
0.9097
0.0097
20.2
0.8200
0.8375
0.0175
20.3
0.7580
0.7816
0.0236
(b) Use step size 0.1 for 10 points. This gives
y(1) < 6.4282; error < 0.0084
20.4
0.7122
0.7406
0.0284
(c) Use step size 0.05 for 20 points. This gives
y1 < 6.4344; error < 0.0022.
20.5
0.6810
0.7131
0.0321
20.6
0.6629
0.6976
0.0347
20.7
0.6566
0.6932
0.0366
20.8
0.6609
0.6987
0.0377
20.9
0.6748
0.7131
0.0383
21.0
0.6974
0.7358
0.0384
(a) To find the approximation, set y1 5 y 2 1 and use
IMPEULT with initial values x 5 0 and y 5 3 and step
size 0.2 for 5 points. This gives y (1) < 6.4054;
error < 0.0311.
(d) As the step size decreases, the accuracy of the method
increases and so the error decreases.
Section 6.6
24. To find the approximate values, set y1 5 x 1 y and use
IMPEULT with initial values x 5 0 and y 5 1 and step size
20.1 for 10 points. The exact values are given by
y 5 2e x 2 x 2 1.
x
y
1
improved
Euler
2
y (exact)
(b)
[0, 10] by [0, 3]
Error
0
1
1.0
0
20.1
0.9100
0.9097
0.0003
20.2
0.8381
0.8375
0.0006
20.3
0.7824
0.7816
0.0008
20.4
0.7416
0.7406
0.0010
20.5
0.7142
0.7131
0.0011
20.6
0.6988
0.6976
0.0012
20.7
0.6944
0.6932
0.0012
20.8
0.7000
0.6987
0.0013
20.9
0.7145
0.7131
0.0013
21.0
0.7371
0.7358
0.0013
25. Set y1 5 y 1 e 2 2 and EULERG, with initial values
x 5 0 and y 5 2 and step sizes 0.1 and 0.05.
x
(a)
279
28. Set y 5 sin (2x 2 y) and use IMPEULG with initial values
x 5 0 and y 5 1 and step sizes 0.1 and 0.05.
(a)
[0, 10] by [0, 5]
(b)
[0, 10] by [0, 5]
29. To find the approximate values, let y1 5 y and use
EULERT with initial values x 5 0 and y 5 1 and step size
0.05 for 20 points. This gives y(1) < 2.6533.
Since the exact solution to the initial value problem is
y 5 e x, the exact value of y (1) is e.
[0, 4.7] by [0, 100]
30. To find the approximate values, let y1 5 3y and use
IMPEULT with initial values x 5 0 and y 5 1 and step size
0.05 for 20 points. This gives y(1) < 19.8845.
Since the exact solution to the initial value problem is
y 5 e3x, the exact value of y(1) is e3.
(b)
[0, 4.7] by [0, 100]
26. Set y1 5 cos (2x 2 y) and use EULERG with initial values
x 5 0 and y 5 2 and step sizes 0.1 and 0.05.
(a)
[0, 10] by [0, 6]
(b)
[0, 10] by [0, 6]
1
2
1
27. Set y1 5 y }} 2 ln )y) and use IMPEULG with initial values
2
1
x 5 0 and y 5 }} and step size 0.1 and 0.05.
3
(a)
[0, 10] by [0, 3]
31. To find the approximate values, let y1 5 1 1 y and use
RUNKUTT with initial values x 5 0 and y 5 1 and step
size 0.1 for 10 points. The exact values are given by
y 5 2e x 2 1.
x
y (Runge-Kutta)
y (exact)
Error
0
1
1
0
0.1
1.2103
1.2103
0.0000002
0.2
1.4428
1.4428
0.0000004
0.3
1.6997
1.6997
0.0000006
0.4
1.9836
1.9836
0.0000009
0.5
2.2974
2.2974
0.0000013
0.6
2.6442
2.6442
0.0000017
0.7
3.0275
3.0275
0.0000022
0.8
3.4511
3.4511
0.0000027
0.9
3.9192
3.9192
0.0000034
1.0
4.4366
4.4366
0.0000042
280
Chapter 6 Review
32. (a) Set y1 5 x 2 y and use RUNKUTT with initial values
x 5 0 and y 5 1 and step size 0.1.
5. Let u 5 sin x
du 5 cos x dx
E
p/2
0
5 sin 3/2 x cos x dx 5
E 5u
1
3/2
du
0
2
5
5 5 ? }}u 5/2
4
5 2(1 2 0)
[0, 10] by [23, 10]
52
(b) Use RUNKUTT with initial values x 5 0 and y 5 22
and step size 0.1.
E
4
6.
x 2 1 3x
}} dx 5
x
1/2
E
4
1/2
(x 1 3) dx (x Þ 0)
4
12
24
1
5 1}}(16) 1
2
1 1
3
3(4)2 2 1}}1}}2 1 }}2
2 4
2
1
12
5 20 2 1}} 1 }}2
8
8
1
5 }}x 2 1 3x
1/2
[0, 10] by [23, 10]
■ Chapter 6 Review Exercises
(pp. 358 – 361)
E
p/3
1.
0
4
sec 2 u du 5 tan u
E 1x 1 }x1}2dx 5 3}12}x
2
2.
2
2
1
p/3
0
147
8
5 }}
2 x 21
2
4
1
12
1
13
8
5 20 2 }}
p
3
5 tan }} 2 tan 0 5 Ï3w
1
2
2 12 2
1
5 }}(4) 2 }} 2 }} 2 1
7. Let u 5 tan x
du 5 sec 2 x dx
E
0
3
2
Ee
5e
4
p/4
e tan x sec 2 x dx 5
1
2
5 }} 1 }}
5e21
8. Let u 5 ln r
1
}} du 5 dx
2
1
r
du 5 }} dr
36
1
E}
} dx 5 18E }} du
(2x 1 1)
u
1
3
3
1
3
1 2 4
1 2
1 2
1
5 18 2}} u 22
2
1
5 29 }} 2 1
9
8
5 29 2}}
9
1
1
1
1/2
du
0
2
3
5 }}u 3/2
1
4
0
2
5 }}(1 2 0)
3
2
3
5 }}
9. Let u 5 2 2 sin x
4. Let u 5 1 2 x 2
du 5 2cos x dx
du 5 22x dx
1
Ïw
lnwr
E}
} dr 5 E u
r
e
3
58
21
du
1
0
du 5 2 dx
E
u
5 e1 2 e0
3. Let u 5 2x 1 1
2du 5 2x dx
0
u
4
5 }} 5 2
2
0
1
2du 5 cos x dx
E
0
2x sin (1 2 x 2) dx 5 2 sin u du 5 0
0
1
cos x
E}
} dx 5 2E}} du
u
2 2 sin x
5 2ln )u) 1 C
5 2ln )2 2 sin x) 1 C
1
0
Chapter 6 Review
15. Let u 5 ln x
10. Let u 5 3x 1 4
1
x
du 5 }} dx
du 5 3 dx
1
x
E}x dln}
5 E}} du
u
x
1
}} du 5 dx
3
E
5 ln )u) 1 C
E
dx
1
}
3
5 }} u 21/3 du
Ïw3w
xw
1w4
3
1 3
5 }} ? }}u 2/3 1 C
3 2
1
5 }}(3x 1 4)2/3 1 C
2
11. Let u 5 t 2 1 5
5 ln )ln x) 1 C
E dt E dt
5 Et
16. }} 5 }3/}2
t
tÏwt
2 3/2
2
5 2}} 1 C
Ïtw
1
}} du 5 t dt
2
t dt
1 1
1
E}
} 5 }}E}} du 5 }} ln )u) 1 C
2 u
2
t 15
2
1
2
1
5 }} ln (t 2 1 5) 1 C
2
5 }} ln )t 2 1 5) 1 C
17. Use tabular integration with f (x) 5 x 3 and g(x) 5 cos x.
f(x) and its
derivatives
1
u
12. Let u 5 }}
1
du 5 2}}2 du
u
E}u1} sec }1u} tan }1u} du 5 2Esec u tan u du
g(x) and its
integrals
x3
(+)
cos x
3x2
(–)
sin x
6x
(+)
–cos x
6
(–)
–sin x
2
0
5 2sec u 1 C
1
u
5 2sec }} 1 C
3
cos x dx
18. Let u 5 ln x
1
y
du 5 }} dy
tan (ln y)
E}
} dy 5 Etan u du
y
sin u
5 E}} du
cos u
Let w 5 cos u
dw 5 2sin u du
E w1
5 2 }} dw
5 ln )w) 1 C
5 2ln )cos u) 1 C
5 2ln )cos (ln y)) 1 C
x
x
Ex
cos x
5 x 3 sin x 1 3x 2 cos x 2 6x sin x 2 6 cos x 1 C
13. Let u 5 ln y
Ee
dt
5 22t 2 1/2 1 C
du 5 2t dt
14. Let u 5 e
du 5 e x dx
281
E
sec (e x) dx 5 sec u du
5 ln )sec u 1 tan u) 1 C
5 ln )sec (e x) 1 tan (e x)) 1 C
1
x
du 5 }} dx
Ex
4
dv 5 x 4 dx
1
5
v 5 }}x 5
E 12
E
1
1
1
5
5
x
1 5
1 4
5 }}x ln x 2 }} x dx
5
5
1
1
5 }}x 5 ln x 2 }}x 5 1 C
5
25
ln x dx 5 }}x 5 ln x 2 }}x 5 }} dx
282
Chapter 6 Review
19. Let u 5 e 3x
Ee
dv 5 sin x dx
du 5 3e 3x dx
dy
1 2
}} 5 x 1 }}
dx
x
1 2
dy 5 x 1 }} dx
x
1 2
dy 5 x 1 }} dx
x
1
2
y 5 x 1 2 1 }}2 dx
x
1
y 5 }}x 3 1 2x 2 x 21 1 C
3
1
y (1) 5 }} 1 2 2 1 1 C 5 1
3
22.
v 5 2cos x
E
sin x dx 5 2e 3x cos x 1 3 cos x e 3x dx
3x
E
Integrate by parts again.
Let u 5 3e 3x
dv 5 cos x dx
du 5 9e 3x dx
Ee
10Ee
Ee
v 5 sin x
E
3x
sin x dx 5 2e 3x cos x 1 3e 3x sin x 2 9e 3x sin x dx
3x
sin x dx 5 2e
3x
cos x 1 3e
3x
1
3
C 5 2}}
1
3
1
3
2
3
E
dx 5 2}}x 2e 23x 1 }} e 23xx dx
[22, 2] by [210, 10]
dv 5 e 23x dx
dy
dt
1
3
3
E
1
2
1
1
3
3
3
3
1 2 23x
2 23x
2
5 2}}x e
2 }}xe
1 }} e 23x dx
3
9
9
1 2 23x
2 23x
2
5 2}}x e
2 }}xe
2 }}e 23x 1 C
3
9
27
x2
2x
2
5 2}} 2 }} 2 }} e 23x 1 C
3
9
27
52}}x 2e 23x 1 }} 2}}xe 23x 1 }} e 23x dx
1
dy
x2
21. }} 5 1 1 x 1 }}
dx
2
x2
dy 5 1 1 x 1 }} dx
2
x2
dy 5 1 1 x 1 }} dx
2
1 2
1 3
y 5 x 1 }}x 1 }}x 1 C
2
6
2
E1
2
y(0) 5 C 5 1
x3
6
E
2
x2
2
y 5 }} 1 }} 1 x 1 1
Graphical support:
1
t14
1
dy 5 }} dt
t14
1
dy 5 }} dt
t14
23. }} 5 }}
v 5 2}}e 23x
du 5 dx
E
Graphical support:
v 5 2}}e 23x
Let u 5 x
1
1
x
dv 5 e 23x dx
du 5 2x dx
2 23x
x3
3
4
E
E
y 5 ln )t 1 4) 1 C
y(23) 5 ln (1) 1 C 5 2
C52
y 5 ln (t 1 4) 1 2
Graphical Support:
[24.5, 5] by [22, 5]
dy
du
24. }} 5 csc 2u cot 2u
dy 5 csc 2u cot 2u du
Edy 5 Ecsc 2u cot 2u du
1
2
y 5 2}} csc 2u 1 C
142
p
1
2
y }} 5 2}} 1 C 5 1
3
2
C 5 }}
[24, 4] by [23, 3]
1
3
y 5 }} 1 2x 2 }} 2 }}
2
20. Let u 5 x 2
Ex e
2
4
}} 1 C 5 1
3
sin x 1 C
1
3x
sin x dx 5 }}[2e 3x cos x 1 3e 3x sin x] 1 C
10
3 sin x
cos x
5 }} 2 }} e 3x 1 C
10
10
1
1 2
1 2
E1 2
E1
1
2
3
2
y 5 2}} csc 2u 1 }}
[0, 1.57] by [25, 3]
Chapter 6 Review
d(y 9)
1
}} 5 2x 2 }}2
dx
x
1
d(y9) 5 2x 2 }}2 dx
x
1
d(y9) 5 2x 2 }}2 dx
x
25.
E
1
E1
2
26.
Ed(r0) 5 E2cos t dt
2
r0 5 2sin t 1 C
r0(0) 5 C 5 21
y9(1) 5 2 1 C 5 1
r0 5 2sin t 2 1
C 5 21
Ed(r9) 5 E(2sin t 2 1) dt
y9 5 x 2 1 x 21 2 1
2
r9 5 cos t 2 t 1 C
1 x 21 2 1) dx
r9(0) 5 1 1 C 5 21
1
y 5 }}x 3 1 ln x 2 x 1 C
3
1
y (1) 5 }} 1 0 2 1 1 C 5 0
3
C 5 22
r9 5 cos t 2 t 2 2
Edr 5 E(cos t 2 t 2 2) dt
2
3
2}} 1 C 5 0
t2
2
r 5 sin t 2 }} 2 2t 1 C
2
3
x3
2
y 5 }} 1 ln x 2 x 1 }}
3
3
C 5 }}
r(0) 5 C 5 21
t2
2
r 5 sin t 2 }} 2 2t 2 1
Graphical support:
x3
3
d(r 0)
}} 5 2cos t
dt
d(r0) 5 2cos t dt
y9 5 x 2 1 x 21 1 C
Edy 5 E(x
283
Graphical support:
2
3
Let f (x) 5 }} 1 ln x 2 x 1 }}.
We first show the graph of y 5 r0 5 2sin t 2 1 along
We first show the graph of y 5 f 9(x) 5 x 2 1 x 21 2 1,
1
x
with the slope field for y9 5 r- 5 2cos t.
x . 0, along with the slope field for y9 5 f 0(x) 5 2x 2 }}2 .
[26, 4] by [23, 3]
[20.5, 4.21] by [29, 21]
Next, we show the graph of y 5 r9 5 cos t 2 t 2 2 along
We now show the graph of y 5 f (x) along with the slope field
for y9 5 f 9(x) 5 x 1 x
2
21
with the slope field for y9 5 r0 5 2sin t 2 1.
2 1.
[26, 4] by [23, 3]
[20.5, 4.21] by [29, 21]
t2
2
Finally we show the graph of y 5 r 5 sin t 2 }} 2 2t 2 1
along with the slope field for y9 5 r9 5 cos t 2 t 2 2.
[26, 4] by [28, 2]
284
Chapter 6 Review
E
dy
dx
dy
}} 5 dx
y12
dy
}} 5 dx
y12
27. }} 5 y 1 2
E
E
E
30. [x 1 f (x)] dx 5 x dx 1 f (x) dx
2
x
2
x2
5 }} 1 1 2 Ïxw 1 C
2
5 }} 1 (1 2 Ïxw) 1 C
E
ln )y 1 2) 5 x 1 C
Since 1 1 C is an arbitrary constant, we may write the
y 1 2 5 Ce x
indefinite integral as }} 2 Ïxw 1 C.
x2
2
E
y 5 Ce x 2 2
E
E
31. [2f (x) 2 g(x)] dx 5 2 f (x) dx 2 g(x) dx
y(0) 5 C 2 2 5 2
5 2(1 2 Ïxw) 2 (x 1 2) 1 C
C54
5 22Ïxw 2 x 1 C
E
y 5 4e x 2 2
E
E
32. [g(x) 2 4] dx 5 g(x) dx 2 4 dx
Graphical support:
5 (x 1 2) 2 4x 1 C
5 2 2 3x 1 C
Since 2 1 C is an arbitrary constant, we may write the
indefinite integral as 23x 1 C.
[25, 5] by [25, 20]
dy
}} 5 (2x 1 1)(y 1 1)
dx
dy
}} 5 (2x 1 1) dx
y11
dy
}} 5 (2x 1 1) dx
y11
28.
E
E
ln )y 1 1) 5 x 2 1 x 1 C
y 1 1 5 Ce
x21x
sin x
x
33. We seek the graph of a function whose derivative is }}.
sin x
x
Graph (b) is increasing on [2p, p], where }} is positive,
and oscillates slightly outside of this interval. This is the
correct choice, and this can be verified by graphing
1
2
sin x
x
NINT }}, x, 0, x .
34. We seek the graph of a function whose derivative is e 2x .
Since e 2x . 0 for all x, the desired graph is increasing for
all x. Thus, the only possibility is graph (d), and we may
verify that this is correct by graphing NINT(e 2x , x, 0, x).
2
2
y 5 Ce x 1x 2 1
2
2
y (21) 5 C 2 1 5 1
35. (iv) The given graph looks like the graph of y 5 x 2, which
C52
y 5 2e x 1x 2 1
2
Graphical support:
dy
dx
satisfies }} 5 2x and y(1) 5 1.
36. Yes, y 5 x is a solution.
dv
dt
37. (a) }} 5 2 1 6t
Edv 5 E(2 1 6t) dt
v 5 2t 1 3t 2 1 C
Initial condition: v 5 4 when t 5 0
[23, 3] by [210, 40]
E
E
4501C
29. 2f (x) dx 5 2 f (x) dx
45C
5 2(1 2 Ïxw) 1 C
v 5 2t 1 3t 2 1 4
5 21 1 Ïxw 1 C
Since 21 1 C is an arbitrary constant, we may write the
indefinite integral as Ïxw 1 C.
E v(t) dt 5 E (2t 1 3t 1 4) dt
5 t 1 t 1 4t
3
4
1
(b)
0
1
2
0
2
3
5620
56
The particle moves 6 m.
1
0
Chapter 6 Review
285
40. Set y1 5 (2 2 y)(2x 1 3) and use IMPEULT with intial
values x 5 23 and y 5 1 and step size 0.1 for 20 points.
38.
[210, 10] by [210, 10]
39. Set y1 5 y 1 cos x and use EULERT with initial values
x 5 0 and y 5 0 and step size 0.1 for 20 points.
x
x
y
23
1
22.9
0.6680
22.8
0.2599
22.7
20.2294
y
22.6
20.8011
0
0
22.5
21.4509
0.1
0.1000
22.4
22.1687
0.2
0.2095
22.3
22.9374
0.3
0.3285
22.2
23.7333
0.4
0.4568
22.1
24.5268
0.5
0.5946
22.0
25.2840
0.6
0.7418
21.9
25.9686
0.7
0.8986
21.8
26.5456
0.8
1.0649
21.7
26.9831
0.9
1.2411
21.6
27.2562
1.0
1.4273
21.5
27.3488
1.1
1.6241
21.4
27.2553
1.2
1.8319
21.3
26.9813
1.3
2.0513
21.2
26.5430
1.4
2.2832
21.1
25.9655
1.5
2.5285
21.0
25.2805
1.6
2.7884
1.7
3.0643
1.8
3.3579
1.9
3.6709
2.0
4.0057
x 2 2y
x11
41. To estimate y(3), set y1 5 }} and use IMPEULT with
initial values x 5 0 and y 5 1 and step size 0.05 for 60
points. This gives y (3) < 0.9063.
x 2 2 2y 1 1
x
42. To estimate y(4), set y1 5 }} and use EULERT
with initial values x 5 1 and y 5 1 and step size 0.05 for
60 points. This gives y(4) < 4.4974.
43. Set y1 5 e2(x1y12) and use EULERG with initial values
x 5 0 and y 5 22 and step sizes 0.1 and 20.1.
(a)
[20.2, 4.5] by [22.5, 0.5]
286
Chapter 6 Review
43. continued
(b) Note that we choose a small interval of x-values
because the y-values decrease very rapidly and our
calculator cannot handle the calculations for x # 21.
(This occurs because the analytic solution is
y 5 22 1 ln (2 2 e2x ), which has an asymptote at
x 5 2ln 2 < 20.69. Obviously, the Euler
approximations are misleading for x # 20.7.)
47. T 2 Ts 5 (T0 2 Ts)e2kt
We have the system:
5
39 2 Ts 5 (46 2 Ts )e210k
33 2 Ts 5 (46 2 Ts )e220k
392 T
33 2 T
46 2 Ts
46 2 Ts
Thus, }}s 5 e 210k and }}s 5 e 220k.
Since (e 210k )2 5 e 220k, this means:
( )
33 2 T
392 T 2
}}s 5 }}s
46 2 Ts
46 2 Ts
(39 2 Ts)2 5 (33 2 Ts)(46 2 Ts)
[21, 0.2] by [210, 2]
1521 2 78Ts 1 Ts2 5 1518 2 79Ts 1 Ts2
x2 1 y
e 1x
Ts 5 23
44. Set y1 5 2}
y } and use IMPEULG with initial
values x 5 0 and y 5 0 and step sizes 0.1 and 20.1.
(a)
The refrigerator temperature was 238C.
48. Use the method of Example 3 in Section 6.4.
e 2kt 5 0.995
2kt 5 ln 0.995
1
k
(b)
5700
ln 2
t 5 2}} ln 0.995 5 2}} ln 0.995 < 41.2
[20.2, 4.5] by [25, 1]
The painting is about 41.2 years old.
49. Use the method of Example 3 in Section 6.4.
[24.5, 0.2] by [21, 5]
ln 2
k
ln 2
2.645 5 }}
k
ln 2
k 5 }} < 0.262059
2.645
45. (a) Half-life 5 }}
1
(b) Mean life 5 }} < 3.81593 years
k
46. T 2 Ts 5 (T0 2 Ts)e2kt
2kt
T 2 40 5 (220 2 40)e
Use the fact that T 5 180 and t 5 15 to find k.
180 2 40 5 (220 2 40)e2(k)(15)
180
9
e 5 }} 5 }}
140
7
9
1
k 5 }} ln }}
7
15
15k
T 2 40 5 (220 2 40)e2((1/15) ln (9/7))t
70 2 40 5 (220 2 40)e2((1/15) ln (9/7))t
180
30
e((1/15) ln (9/7))t 5 }} 5 6
1}15} ln }7}2t 5 ln 6
1
9
15 ln 6
ln (9/7)
t 5 }} < 107 min
It took a total of about 107 minutes to cool from 2208F to
708F. Therefore, the time to cool from 1808F to 708F was
about 92 minutes.
Since 90% of the carbon-14 has decayed, 10% remains.
e 2kt 5 0.1
2kt 5 ln 0.1
1
k
5700
ln 2
t 5 2}} ln 0.1 5 2}} ln 0.1 < 18,935
The charcoal sample is about 18,935 years old.
50. Use t 5 1988 2 1924 5 64 years.
250 e rt 5 7500
e rt 5 30
rt 5 ln 30
ln 30
t
ln 30
64
r 5 }} 5 }} < 0.053
The rate of appreciation is about 0.053, or 5.3%.
Chapter 6 Review
51. Using the Law of Exponential Change in Section 6.4 with
150
11e
(c) }}
4.32t 5 125
appropriate changes of variables, the solution to the
differential equation is L(x) 5 L0e 2kx, where L0 5 L(0) is
the surface intensity. We know 0.5 5 e 218k, so
ln 0.5
218
6
}} 5 1 1 e 4.32t
5
1
}} 5 e 4.32t
5
2ln 5 5 4.3 2 t
k 5 }} and our equation becomes
t 5 4.3 1 ln 5 < 5.9 days
1 x/18
. We now find the depth
2
12
L(x) 5 L0e (ln 0.5)(x/18) 5 L0 }}
It took about 6 days.
where the intensity is one-tenth of the surface value.
54. Use the Fundamental Theorem of Calculus.
1 x/18
122
0.1 5 }}
d
dx
12
1
x
2
18
18 ln 0.1
x 5 }} < 59.8 ft
ln 0.5
ln 0.1 5 }} ln }}
x
0
2
d
dx
sin t 2 dt 1 }}(x 3 1 x 1 2)
5 (sin x 2) 1 (3x 2 1 1)
d
dx
y0 5 }}(sin x 2 1 3x 2 1 1)
You can work without artificial light to a depth of about
5 (cos x 2)(2x) 1 6x
59.8 feet.
52. (a)
1E
y9 5 }}
5 2x cos (x 2) 1 6x
dy
kA
}} 5 }}(c 2 y)
dt
V
kA
dy
}} 5 }} dt
V
c2y
kA
2ln )c 2 y) 5 }}t 1 C
V
kA
ln )c 2 y) 5 2}}t 2 C
V
E
Thus, the differential equation is satisfied.
E
Verify the initial conditions:
y9(0) 5 (sin 02) 1 3(0)2 1 1 5 1
y(0) 5
)c 2 y) 5 e 2(kA/V)t2C
E
0
0
sin(t 2) dt 1 03 1 0 1 2 5 2
1
2
dP
800 2 P
}} 5 0.002P1}}2
dt
800
dP
P
}} 5 0.002P 1 2 }}
dt
800
55.
c 2 y 5 6e 2(kA/V)t2C
y 5 c 6 e 2(kA/V)t2C
800
}} dP 5 0.002 dt
P(800 2 P)
y 5 c 1 De 2(kA/V)t
(800 2 P) 1 P
}} dP 5 0.002 dt
P(800 2 P)
Initial condition y 5 y0 when t 5 0
1
E1}P1} 1 }
} dP 5 0.002 dt
800 2 P 2
y0 5 c 1 D
y0 2 c 5 D
ln )P) 2 ln )800 2 P) 5 0.002t 1 C
2(kA/V)t
Solution: y 5 c 1 (y0 2 c)e
(b) lim y(t) 5 lim [c 1 (y0 2 c)e
t→`
t→`
150
11e
) 800P2 P )
800 2 P
ln )}}) 5 20.002t 2 C
P
800 2 P
)}P}) 5 e
ln }} 5 0.002t 1 C
2(kA/V)t
]5c
150
11e e
53. (a) P(t) 5 }}
4.32t 5 }}
4.3 2t
M
1 1 Ae
20.002t2C
4.3
This is P 5 }}
2kt where M 5 150, A 5 e , and
k 5 1. Therefore, it is a solution of the logistic
800 2 P
}} 5 6e 2Ce 20.002t
P
differential equation.
800
}} 2 1 5 Ae 20.002t
P
dP
dP
k
1
}} 5 }}P(M 2 P), or }} 5 }}P(150 2 P). The
dt
dt
M
150
carrying capacity is 150.
150
11e
(b) P(0) 5 }}
4.3 < 2
Initially there were 2 infected students.
800
1 1 Ae
P 5 }}
20.002t
Initial condition: P(0) 5 50
800
1 1 Ae
50 5 }}0
1 1 A 5 16
A 5 15
800
1 1 15e
Solution: P 5 }}
20.002t
287
288
Section 7.1
56. Method 1–Compare graph of y1 5 x 2 ln x with
1
x 3 ln x
3
x3
9
60. (a) T 5 79.961(0.9273)t
2
y2 5 NDER }} 2 }} . The graphs should be the same.
Method 2–Compare graph of y1 5 NINT(x 2 ln x) with
x 3 ln x
3
x3
9
y2 5 }} 2 }}. The graphs should be the same or differ
[21, 33] by [25, 90]
only by a vertical translation.
(b) Solving T(t) 5 40 graphically, we obtain t < 9.2 sec.
The temperature will reach 408 after about 9.2 seconds.
57. (a) 20,000 5 10,000(1.063)t
(c) When the probe was removed, the temperature was
about T(0) < 79.968C.
2 5 1.063t
ln 2 5 t ln 1.063
ln 2
ln 1.063
t 5 }} < 11.345
61.
vm
}0} 5 coasting distance
k
(0.86)(30.84)
}} 5 0.97
k
k < 27.343
It will take about 11.3 years.
vm
(b) 20,000 5 10,000e
s(t) 5 }0}(1 2 e 2(k/m)t )
0.063t
k
s(t) 5 0.97(1 2 e 2(27.343/30.84)t )
2 5 e 0.063t
s(t) 5 0.97(1 2 e 20.8866t )
ln 2 5 0.063t
ln 2
0.063
t 5 }} < 11.002
It will take about 11.0 years.
d
dx
d
g9(x) 5 }}
dx
58. (a) f 9(x) 5 }}
A graph of the model is shown superimposed on a graph of
the data.
E u(t) dt 5 u(x)
E u(t) dt 5 u(x)
x
0
x
3
[0, 3] by [0,1]
(b) C 5 f (x) 2 g(x)
E
5E
5E
5
x
0
x
0
3
E
u(t) dt 1 E
u(t) dt 2
x
u(t) dt
3
3
Chapter 7
Applications of Definite Integrals
u(t) dt
x
u(t) dt
0
56.0716
1 1 5.894e
59. (a) y 5 }}
20.0205x
■ Section 7.1 Integral as Net Change
(pp. 363–374)
Exploration 1
1. s(t) 5
E1t
03
3
2
Revisiting Example 2
8
(t 1 1)
t3
3
2
8
t11
2 }}2 dt 5 }} 1 }} 1 C
8
011
s(0) 5 }} 1 }} 1 C 5 9 ⇒ C 5 1
[220, 200] by [210, 60]
(b) The carrying capacity is about 56.0716 million people.
(c) Use NDER twice to solve y0 5 0. The solution is
x < 86.52, representing (approximately) the year 1887.
The population at this time was approximately
P(86.52) < 28.0 million people.
t3
3
8
t11
Thus, s(t) 5 }} 1 }} 1 1.
13
3
8
111
16
3
2. s(1) 5 }} 1 }} 1 1 5 }}. This is the same as the
answer we found in Example 2a.
53
3
8
511
3. s(5) 5 }} 1 }} 1 1 5 44. This is the same answer we
found in Example 2b.
289
Section 7.1
Quick Review 7.1
p
2
p
2
1. On the interval, sin 2x 5 0 when x 5 2}}, 0, or }}. Test one
3p
4
point on each subinterval: for x 5 2}}, sin 2x 5 1;
–
+
–p
–3
–
f (x)
2
–
f (x)
+
x
–5 0
30
x2 2 2
x 24
w and is undefined when
8. }
2 } 5 0 when x 5 6Ï2
x 5 62. Test one point on each subinterval: for x 5 2}},
2. x 2 2 3x 1 2 5 (x 2 1)(x 2 2) 5 0 when x 5 1 or 2. Test
one point on each subinterval: for x 5 0, x 2 2 3x 1 2 5 2;
3
2
1
2
x
x 11
5
2
x
p 2
2
0
1
2
x
x 11
for x 5 21, }
2 } 5 2}}; for x 5 1, }
2 } 5 }}. The
function changes sign at 0. The graph is
p
p
for x 5 2}}, sin 2x 5 21; for x 5 }}, sin 2x 5 1; and for
4
4
3p
p
x 5 }}, sin 2x 5 21. The function changes sign at 2}}, 0,
4
2
p
and }}. The graph is
2
+
x
x 11
7. }
2 } 5 0 when x 5 0. Test one point on each subinterval:
1
4
for x 5 }}, x 2 2 3x 1 2 5 2}}; and for x 5 3,
x2 2 2
17
x2 2 2
}
} 5 }}; for x 5 21.9, }
} < 24.13; for x 5 0,
x2 2 4
9
x2 2 4
2
2
x 22
1
x 22
5
}
} 5 }}; for x 5 1.9, }
} < 24.13; and for x 5 }},
x2 2 4
2
x 2 24
2
x2 2 2
17
w, Ï2w
}
} 5 }}. The function changes sign at 22, 2Ï2
x2 2 4
9
and 2. The graph is
x 2 2 3x 1 2 5 2. The function changes sign at 1 and 2.
+
The graph is
–
+
–
√2 2
–3 –2 –√2
+
–
–2
1
x
2
1
cos (1 1 )cos x))
2wsin
w2wxw) 5 }} is undefined when
9. sec (1 1 Ï1ww
4
x
–4
x < 0.9633 1 kp or 2.1783 1 kp for any integer k. Test for
x 5 0: sec (1 1 Ï1ww
2wsin
w2w0w) < 22.4030.
Test for x 5 61: sec (1 1 Ï1ww
2wsin
w2w1w) < 32.7984. The
f (x)
+
2
sign alternates over successive subintervals. The function
1
2
4. 2x 3 2 3x 2 1 1 5 (x 2 1)2(2x 1 1) 5 0 when x 5 2}} or 1.
Test one point on each subinterval: for x 5 21,
2x 3 2 3x 2 1 1 5 24; for x 5 0, 2x 3 2 3x 2 1 1 5 1; and
3
2
x 5 }}, 2x 3 2 3x 2 1 1 5 1. The function changes sign at
1
2
2}}. The graph is
changes sign at 0.9633 1 kp or 2.1783 1 kp, where k is an
integer. The graph is
–
+
f (x)
+
f (x)
x
–2.1783 –0.9633 0.9633 2.1783
1
3p
1
2p
1
p 3p
4 4
5p
4
function changes sign at }}, }}, and }}. The graph is
3p
4
–
1
x 5 0.15, sin }} < 0.37; and for x 5 0.2,
x cos 2x 5 p; and for x 5 4, x cos 2x < 20.58. The
+
1x2
1
2
1x2
1
–
1x2
point on each subinterval: for x 5 0.1, sin }} < 20.54; for
x
p 3p
5p
5. On the interval, x cos 2x 5 0 when x 5 0, }}, }}, or }}.
4 4
4
p
Test one point on each subinterval: for x 5 }},
8
pÏw2
p
p
x cos 2x 5 }}; for x 5 }}, x cos 2x 5 2}}; for x 5 p,
16
2
2
p
4
–
1
2
0
+
1x2
+
+
–
10. On the interval, sin }} 5 0 when x 5 }} or }}. Test one
–1
–2
x
3
f (x)
+
3. x 2 2 2x 1 3 5 0 has no real solutions, since
b 2 2 4ac 5 (22)2 2 4(1)(3) 5 28 , 0. The function is
always positive. The graph is
–
f (x)
+
f (x)
x
5p 4
4
6. xe 2x 5 0 when x 5 0. On the rest of the interval, xe 2x is
always positive.
1
3p
1
2p
sin }} < 20.96. The graph changes sign at }}, and }}.
The graph is
–
+
0.1 1
3p
–
1
2p
f (x)
x
0.2
290
Section 7.1
Section 7.1 Exercises
4. (a) Right when
1. (a) Right when v(t) . 0, which is when cos t . 0, i.e.,
p
2
3p
2
p
3p
i.e., when }} , t , }}. Stopped when cos t 5 0,
2
2
p
3p
i.e., when t 5 }} or }}.
2
2
when 0 # t , }} or }} , t # 2p. Left when cos t , 0,
2p
0
5
2p
3 4
5 cos t dt 5 5 sin t
(c) Distance 5
E
p/2
0
i.e., when 0 # t , 1. Left when 6(t 2 1)(t 2 2) , 0,
i.e., when 1 , t , 2. Stopped when
6(t 2 1)(t 2 2) 5 0, i.e., when x 5 1, or 2.
(b) Displacement 5
(b) Displacement 5
E
v(t) 5 6t 2 2 18t 1 12 5 6(t 2 1)(t 2 2) . 0,
5 5[sin 2p 2 sin 0] 5 0
3
2p
(c) Distance 5
)5 cos t) dt
0
5 cos t dt 1
E
3p/2
25 cos t dt 1
p/2
E
2p
5 cos t dt
3p/2
2
0
4
2
2 18t 1 12) dt
2
5 2t 3 2 9t 2 1 12t 5 [(16 2 36 1 24) 2 0] 5 4
0
E
E (6t
5
E (6t
1
E )6t
2
0
2 18t 1 12) dt
2
0
2 18t 1 12) dt 1
2
0
E (26t
2
2
1
1 18t 2 12) dt
551156
5 5 1 10 1 5 5 20
5. (a) Right when v(t) . 0, which is when sin t Þ 0 and
2. (a) Right when v(t) . 0, which is when sin 3t . 0,
p
3
p
2
3p
2
i.e., when 0 , t , }}. Left when sin 3t , 0, i.e., when
cos t . 0, i.e., when 0 , t , }} or }} , t , 2p. Left
p
p
}} , t # }}. Stopped when sin 3t 5 0, i.e., when t 5 0
3
2
p
or }}.
3
when sin t Þ 0 and cos t , 0, i.e., when }} , t , p or
(b) Displacement 5
E
p/2
0
3p
5 22 cos }} 2 cos 0 5 2
2
3
(c) Distance 5
5
E
p/3
0
E
p/2
0
3
4
1
6 sin 3t dt 5 6 2}} cos 3t
3
4
p/2
0
3p
2
p , t , }}. Stopped when sin t 5 0 or cos t 5 0,
E
p/2
p/3
26 sin 3t dt 5 4 1 2 5 6
3. (a) Right when v(t) 5 49 2 9.8t . 0, i.e., when 0 # t , 5.
(b) Displacement 5
(b) Displacement 5
3
4
5 49t 2 4.9t 2
(c) Distance 5
5
E
10
E
10
0
10
(49 2 9.8t) dt
5 49[(10 2 10) 2 0] 5 0
0
)49 2 9.8t) dt
E (49 2 9.8t) dt 1 E
5
0
0
10
5
5 122.5 1 122.5 5 245
(249 1 9.8t) dt
3p
2
E
2p
0
33
4
1
5 sin2 t cos t dt 5 5 }} sin3 t
5 5[0 2 0] 5 0
(c) Distance 5
5
E
p/2
0
5
3
E
2p
0
E
0
3p/2
p/2
E
5 sin2 t cos t dt
10
3
5
3
2p
2p
)5 sin2 t cos t) dt
5 sin2 t cos t dt 1
1
Left when 49 2 9.8t , 0, i.e., when 5 , t # 10.
Stopped when 49 2 9.8t 5 0, i.e., when t 5 5.
p
2
i.e., when t 5 0, }}, p, }}, or 2p.
)6 sin 3t) dt
6 sin 3t dt 1
p
2
25 sin2 t cos t dt
3p/2
20
3
5 }} 1 }} 1 }} 5 }}
6. (a) Right when v(t) . 0, which is when 4 2 t . 0, i.e.,
when 0 # t , 4. Left: never, since Ï4ww
2wt cannot be
negative. Stopped when 4 2 t 5 0, i.e., when t 5 4.
(b) Displacement 5
E Ï4ww2wt dt 5 32}23}(4 2 t) 4
4
0
2
16
5 2}}[0 2 8] 5 }}
3
3
(c) Distance 5
E Ï4ww2wt dt 5 }13}6
4
0
3/2
4
0
Section 7.1
7. (a) Right when v(t) . 0, which is when cos t . 0,
p
2
3p
2
i.e., when 0 # t , }} or }} , t # 2p. Left when
p
2
3p
2
p
3p
cos t 5 0, i.e., when t 5 }} or }}.
2
2
cos t , 0, i.e., when }} , t , }}. Stopped when
(b) Displacement 5
E
2p
e
sin t
0
3 4
cos t dt 5 e
sin t
5 [e 2 e ] 5 0
0
0
(c) Distance 5
E
3p/2
p/2
E
)esin t cos t) dt 5
2e sin t cos t dt 1
1
C2 5 s(0) 5 0. Solve s(t) 5 0:
0
1
e
E
2p
E
p/2
0
esin t cos t dt 1
e sin t cos t dt
3p/2
2 1
1
e
2
2
e
1
t
E}
} dt 5 3}} ln (1 1 t )4
2
11t
3
2
3
0
ln 10
t
E}
} dt 5 }} < 1.15
2
11t
1
2
5.625
2
5.625 2
5.625
5 216 }} 1 90 }} 5 126.5625, and
2
2
1
2
1
2
2
0
E
3/2
1 C, and since v(0) 5 0,
v(t) 5 t 1 2t 3/2. Then v(9) 5 9 1 2(27) 5 63 mph.
(b) First convert units:
12. Displacement 5
E v(t) dt 5 24 1 5 2 24 5 223 cm
13. Total distance 5
E )v(t)) dt 5 4 1 5 1 24 5 33 cm
c
0
c
0
E v(t) dt 5 15 2 4 5 11.
At t 5 b, s 5 s(0) 1 E v(t) dt 5 15 2 4 1 5 5 16.
At t 5 c, s 5 s(0) 1 E v(t) dt 5 15 2 4 1 5 2 24 5 28.
14. At t 5 a, s 5 s(0) 1
t
t 3/2
3600
1800
9
t
t 3/2
Distance 5
}} 1 }} dt
1800
0 3600
2
5/2
t
t
9
27
9
5 }} 1 }} 5 }} 1 }} 2 0 5 0.06525 mi
7200
4500 0
800
500
t 1 2t 3/2 mph 5 }} 1 }} mi/sec. Then
2
4 31
2
4
5 344.52 ft.
a
0
b
0
c
0
dv
dt
15. At t 5 a, where }} is at a maximum (the graph is steepest
upward).
10. (a) Displacement 5
3
E (t 2 2) sin t dt
4
0
dv
dt
16. At t 5 c, where }} is at a maximum (the graph is steepest
4
4
5 sin t 2 t cos t 1 2 cos t
upward).
0
5 [(sin 4 2 4 cos 4 1 2 cos 4) 2 2] < 21.44952 m
(b) Because the velocity is negative for 0 , t , 2, positive
for 2 , t , p, and negative for p , t # 4,
Distance 5
Displacement 5 0.
Distance 5 2(Max. Height) 5 253.125 ft.
3
9. (a) v(t) 5 a(t) dt 5 t 1 2t
3
(c) Since starting height 5 ending height,
(d) Max. Height 5 s }}
2
0
45
8
when t 5 0 or t 5 }} 5 5.625 sec.
The projectile hits the ground at 5.625 sec.
1
ln 10
5 }}[ln (10) 2 ln (1)] 5 }} < 1.15
2
2
E1
Then v(3) 5 232(3) 1 90 5 26 ft/sec.
E
8. (a) Right when v(t) . 0, which is when 0 , t # 3. Left:
never, since v(t) is never negative. Stopped when t 5 0.
(c) Distance 5
C1 5 v(0) 5 90.
(b) s(t) 5 v(t) dt 5 216t2 1 90t 1 C2, where
2p
5 (e 2 1) 1 e 2 }} 1 1 2 }} 5 2e 2 }} < 4.7
(b) Displacement 5
E
11. (a) v(t) 5 a(t) dt 5 232 dt 5 232t 1 C1, where
216t 2 1 90t 5 2t(28t 1 45) 5 0
2p
0
E
291
E 2(t 2 2) sin t dt 1 E (t 2 2) sin t dt
1 E 2(t 2 2) sin t dt
p
2
0
4
2
p
5 [(2 2 sin 2) 1 (p 2 sin 2 2 2)
1 (p 1 2 cos 4 2 sin 4 2 2)]
5 2p 1 2 cos 4 2 2 sin 2 2 sin 4 2 2 < 1.91411 m.
12
1
2
17. Distance 5 Area under curve 5 4 }} ? 1 ? 2 5 4
(a) Final position 5 Initial position 1 Distance
5 2 1 4 5 6; ends at x 5 6.
(b) 4 meters
18. (a) Positive and negative velocities cancel: the sum of
signed areas is zero. Starts and ends at x 5 2.
(b) Distance 5 Sum of positive areas 5 4(1 ? 1) 5 4
meters
292
Section 7.1
19. (a) Final position 5 2 1
E v(t) dt
25. (Answers may vary.)
Plot the speeds vs. time. Connect the points and find the
area under the line graph. The definite integral also gives
the area under the curve.
7
0
1
1
2
2
1
1
1 }}(2)(2) 2 }}(2)(1)
2
2
5 2 2 }}(1)(2) 1 }}(1)(2) 1 1(2)
26. (a) Sum of numbers in Sales column 5 797.5 thousand
(b) Enter the table in a graphing calculator and use
QuadReg: B(x) 5 1.6x 2 1 2.3x 1 5.0.
5 5;
ends at x 5 5.
E )v(t)) dt 5 }12}(1)(2) 1 }12}(1)(2) 1 1(2) 1 }12}(2)(2)
1.6
1
2
1 }}(2)(1)
10
v(t) dt
0
1
5 }}(2
2
E
)v(t)) dt
1
1
1
? 3) 1 }2}(1)(3) 1 3(3) 1 }2}(1)(3) 1 }2}(3)(3)
3
27.08 ? e t/25 dt 5 27.08 25e t/25
0
4
< 332.965 billion barrels
E3
24
10
5 27.08[25e 0.4 2 25]
0
24
28.8
pt
pt
3.9 2 2.4 sin }} dt 5 3.9t 1 }} cos }}
22.
p
12
12
0
28.8
28.8
5 93.6 1 }} 2 }} 5 93.6 kilowatt-hours
p
p
31
2
1 24
4
3
1 24
0
E 10,000(2 2 r)(2pr) dr 5 20,000pE (2r 2 r ) dr
2
2
0
2
0
4
2
31
8
3
2
5 20,000p r 2 2 }}r 3 5 20,000p 4 2 }} 2 0
0
24. (a) Width 5 Dr, Length 5 2pr: Area 5 2prDr
(b) Volume per second
E 8(10 2 r )(2pr) dr 5 16pE (10r 2 r ) dr
3
2
0
3
0
3
4
3
n21
b2a
2 f (xi) 1 f (xn)
}} f (x0) 1
2n
i51
18 2 8
5 }}[120 1 2(110) 1 2(115) 1 2(115) 1 2(119)
2(10)
∑
3
4
1 2(120) 1 2(120) 1 2(115) 12(112) 1 2(110)
1 121]
4
(b) W 5
E F(x) dx 5 E 2x dx 5 3x 4
9
0
9
2
0
9
0
5 81 N ? cm
30. F(x) 5 kx; 10,000 5 k(1), so k 5 10,000.
(a) W 5
E kx dx 5 3}12}kx 4
d
0
2
d
1
2
1
2
5 }}kd 2 5 }}(10,000)(0.5)2
0
1
2
(b) For total distance: W 5 }}(10,000)(1)2 5 5000
W 5 5000 2 1250 5 3750 inch-pounds
in3
sec
in.
sec
8(10 2 r 2)}} ? (2pr)Dr in2 5 flow in }}
31
2
1
81
5 16p 5r 2 }}r 4 5 16p 45 2 }} 2 0
4 0
4
in3
in3
5 396p }} < 1244.07 }}
sec
sec
2
< 798.97 thousand
For second half of distance:
5 Inches per second 3 Cross section area
3
20.5
28. Treat 6 P.M. as 18 o’clock:
5 1250 inch-pounds
80,000
3
5 }}p < 83,776
(c)
10.5
(a) F(9) 5 2(9) 5 18N
(c) Population 5 Population density 3 Area
1
3
4
2.3
2
29. F(x) 5 kx; 6 5 k(3), so k 5 2 and F(x) 5 2x.
(b) Width 5 Dr, Length 5 2pr: Area 5 2prDr
3
1.6
3
5 1156.5
23. (a) Solve 10,000(2 2 r) 5 0: r 5 2 miles.
(d)
(1.6x 2 1 2.3x 1 5.0) dx
(b) The answer in (a) corresponds to the area of midpoint
rectangles. The curve now gives a better approximation
since part of each rectangle is above the curve and part
is below.
10
10
20.5
3
5 19.5 meters
21.
E
5 }}x 3 1 }}x 2 1 5.0x
ends at x 5 22.5.
0
0
10.5
27. (a)
5 22.5;
E
11
(d) The answer in (a) corresponds to the area of left hand
rectangles. These rectangles lie under the curve B(x).
The answer in (c) corresponds to the area under the
curve. This area is greater than the area of rectangles.
1
1
1
5 2 1 }}(2)(3) 2 }}(1)(3) 2 (3)(3) 2 }}(1)(3)
2
2
2
1
1 }}(3)(3)
2
(b) Distance 5
4
2.3
2
< 904.02 thousand
5 7 meters
E
33
5 }}x 3 1 }}x 2 1 5.0x
0
20. (a) Final position 5 2 1
(1.6x 2 1 2.3x 1 5.0) dx
0
7
(b)
E
11
(c)
4
(12 2 0)
2(12)
31. }}[0.04 1 2(0.04) 1 2(0.05) 1 2(0.06) 1 2(0.05)
1 2(0.04) 1 2(0.04) 1 2(0.05) 1 2(0.04)
1 2(0.06) 1 2(0.06) 1 2(0.05) 1 0.05] 5 0.585
0.585
12
The overall rate, then, is }} 5 0.04875.
Section 7.2
(12 2 0)
2(12)
32. }}[3.6 1 2(4.0) 1 2(3.1) 1 2(2.8) 1 2(2.8) 1 2(3.2)
1 2(3.3) 1 2(3.1) 1 2(3.2) 1 2(3.4) 1 2(3.4)
1 2(3.9) 1 4.0] 5 40 thousandths or 0.040
293
■ Section 7.2 Areas in the Plane
(pp. 374–382)
Exploration 1
A Family of Butterflies
1. For k 5 1:
E [(2 2 sin x) 2 sin x] dx 5 E
p
∑mkxk
M
33. (a) xw 5 }}y 5 }. Taking dm 5 ddA as mk and letting
M
∑mk
0
(2 2 2 sin x) dx
5 2p 2 4
4
p
0
For k 5 2:
E
p/2
∑mky
M
(b) yw 5 }}y 5 }. Taking dm 5 ddA as mk and letting
M
∑mk
34. By symmetry, wx 5 0. For yw, use horizontal strips:
0
5 2x 1 2 cos x
Ex dm
dA → 0, k → ` yields }.
Edm
Ey dm
dA → 0, k →` yields }.
Edm
p
0
5
E
[(4 2 2 sin 2x) 2 (2 sin 2x)] dx
p/2
0
(4 2 4 sin 2x) dx
4
5 4x 1 2 cos 2x
p/2
5 2p 2 4
0
2. It appears that the areas for k $ 3 will continue to be
2p 2 4.
E
5E
3. Ak 5
Ey dm Ey d dA Ey dA
Edm Ed dA EdA
E y(2Ïyw) dy
}}
5
E 2Ïyw dy
yw 5 } 5 } 5 }
p/k
0
p/k
0
[(2k 2 k sin kx) 2 k sin kx] dx
(2k 2 2k sin kx) dx
If we make the substitution u 5 kx, then du 5 k dx and the
4
u-limits become 0 to p. Thus,
0
4
E (2k 2 2k sin kx) dx
5 E (2 2 2 sin kx)k dx
5 E (2 2 2 sin u) du.
Ak 5
0
3
4
3
4
2
4
2 }}y 5/2
5
0
5 }}
0
4. 2p 2 4
12
5
5 }}
35. By symmetry, y 5 0. For x, use vertical strips:
Ex dm Exd dA Ex dA
x 5}5}5}
Edm Ed dA EdA
E x(2x) dx
5 }}
E 2x dx
2
5. Because the amplitudes of the sine curves are k, the kth
butterfly stands 2k units tall. The vertical edges alone have
lengths (2k) that increase without bound, so the perimeters
are tending to infinity.
Quick Review 7.2
0
3}}x34
5 3 0
3 40
2x
0
E
p/4
3.
2
}
2
x2
3
1
3 4
1
2
1
2
0
3
4
E (4x 2 x ) dx 5 32x
3
0
5.
E
23
5 2[21 2 1] 5 2
0
sec2 x dx 5 tan x
2p/4
3
p
dx5 }}e2x 5 }}(e2 2 1) < 3.195
2
4.
4
sin x dx5 2cos x
Ee
1
2.
2
0
E
p
1.
0
4
5 }}
3
0
p/k
0
p
2
4
2 }}y 3/2
3
0
2
p/k
2
p/4
5 1 2 (21) 5 2
2p/4
1
4
4
2
2 }}x 4 5 (8 2 4) 2 0 5 4
0
9p
Ï9ww
2wx 2w dx 5 }} (This is half the area of a circle of
radius 3.)
2
294
Section 7.2
6. Solve x 2 2 4x 5 x 1 6.
x 2 2 5x 2 65 0
(x 2 6)(x 1 1) 5 0
x 5 6 or x 5 21
y 5 6 1 6 5 12 or y 5 21 1 6 5 5
(6, 12) and (21, 5)
E (y
1
3.
2
0
1
4
1
4
1
1
12
0
E [(12y 2 12y ) 2 (2y 2 2y)] dy
5 E (212y 1 10y 1 2y) dy
1
4.
33
2 y 3) dy 5 }}y 3 2 }}y 4 5 }}
2
3
2
0
1
7. Solve e 5 x 1 1. From the graphs, it appears that e is
x
x
always greater than or equal to x 1 1, so that if they are
ever equal, this is when e x 2 (x 1 1) is at a minimum.
d
}}[e x 2 (x 1 1)] 5 e x 2 1 is zero when e x 5 1, i.e., when
dx
x 5 0. Test: e0 5 0 1 1 5 1. So the solution is (0, 1).
3
2
0
3
10
3
5 23y 4 1 }}y 3 1 y 2
1
4
0
10
3
4
3
5 23 1 }} 1 1 5 }}
5. Use the region’s symmetry:
E
E
2
8. Inspection of the graphs shows two intersection points:
(0, 0), and (p, 0). Check: 02 2 p ? 0 5 sin 0 5 0 and
p 2 2 p 2 5 sin p 5 0.
2
2 [2x 2 2 (x 4 2 2x 2)] dx 5 2 (2x 4 1 4x 2) dx
0
0
3
1
5
4
3
5 2 2}}x 5 1 }}x 3
2x
x 11
3
9. Solve }
2 }5x .
31
2
4
0
2
4
32
32
128
5 2 2}} 1 }} 2 0 5 }}
5
3
15
(0, 0) is a solution. Now divide by x.
2
}
} 5 x2
x2 1 1
6. Use the region’s symmetry:
E
1
33
1
2
5
4
1
2
4
1
13
1
2
5
2
0
x4 1 x2 2 2 5 0
0
7. Integrate with respect to y:
21 6 Ïw1w
1w8
x 5 }} 5 22 or 1
2
2
E
1
Throw out the negative solution.
0
x 5 61
33
4
(2Ïyw 2 y) dy 5 }}y 3/2 2 }}y2
13
4
1
2
2
1
0
5
6
5 }} 2 }} 2 0 5 }}
y 5 x 3 5 61
(0, 0), (21, 21) and (1, 1)
8. Integrate with respect to y:
E
1
10. Use the intersect function on a graphing calculator:
0
[(2 2 y) 2 Ïyw] dy
3
1
2
2
3
1
4 1
1
2
2
3
2
5
6
5 2y 2 }}y 2 2 }}y 3/2 5 2 2 }} 2 }} 2 0 5 }}
0
9. Integrate in two parts:
E [(2x 2 x 2 5x) 2 (2x 1 3x)] dx 1
E [(2x 1 3x) 2 (2x 2 x 2 5x)] dx
5 E (2x 2 8x) dx 1E (22x 1 8x) dx
0
[22, 2] by [22, 2]
0
Section 7.2 Exercises
1.
E
0
3
4
1
1
(1 2 cos x) dx 5 }}x 2 }} sin 2x
2
4
2
p
p
5 }}
2
0
E 1}12} sec
p/3
0
2
2
2
2
0
3
32
1
2
2
3
22
5 }}x 4 2 4x 2
3
0
422 1 32}2}x4 1 4x240
0
1
2
5 [0 2 (8 2 16)] 1 [(28 1 16) 2 0] 5 16
2. Use symmetry:
2
3
22
2
(20.9286, 20.8008), (0, 0), and (0.9286, 0.8008)
p
22
15
2 (x 2 1 2x 4) dx 5 2 }}x 3 1 }}x 5 5 2 }} 1 }} 5 }}
2 5 x4 1 x2
2
t 1 4 sin2 t dt 5
E
p/3
0
(sec2 t 1 8 sin2 t) dt
3
4
5 tan t 1 4t 2 2 sin 2t
p/3
0
4p
5 Ï3w 1 }} 2 Ï3w 2 0
3
1
4p
3
5 }}
2
295
Section 7.2
13. Solve 7 2 2x 2 5 x 2 1 4: x 2 5 1, so the curves intersect at
10. Integrate in three parts:
E
21
22
x 5 61.
[(2x 1 2) 2 (4 2 x )] dx 1
2
E
1
21
E
2
21
[(7 2 2x 2) 2 (x 2 1 4)] dx 5
[(4 2 x 2) 2 (2x 1 2)] dx 1
2
5
E
(x 2 x 2 2) dx 1
22
2
E (x
3
2
2
3
5
21
1
3
4
1
2
(2x 1 x 1 2) dx 1
2
3
4
1 3
1 2
1 2}}x 1 }}x 1 2x
22
2
3
2
2
4
1
21
2
1
21
[23, 3] by [21, 5]
4
The curves intersect at x 5 61 and x 5 62. Use the
2
region’s symmetry:
8
E
8
1
E
1
2
2 [(x 4 2 4x 2 1 4) 2 x 2] dx 1 2 [x 2 2 (x 4 2 4x 2 1 4)] dx
0
312}3} 1 2 1 42 2 1}3} 1 }2} 2 224 1
1
E
E
1
2 1
9 2 }9} 2 6 2 }8} 2 2 2 4
2
3
1
2
5 2 (x 4 2 5x 2 1 4) dx 1 2 (2x 4 1 5x 2 2 4) dx
0
24
1
3
4
3
4 31
1
5
5 2 }}x 5 2 }}x 3 1 4x
5
3
1
3
1
5
5
3
1 2 2}}x 5 1 }}x 3 2 4x
0
2
4
1
2 1
24 5 8
1
5
32
40
1
5
5 2 }} 2 }} 1 4 1 2 2}} 1 }} 2 8 2 2}} 1 }} 2 4
5
3
5
3
5
3
1
6
5 }49} 5 8}}
6
1
3
3 3 1 3 24 5 4
3
1
31
(1 2 x 2) dx
21
5 3 }} 2 2}}
312}3} 2 }2} 1 22 2 12}3} 2 2 1 424 1
1
1
14.
21
1 3
1 2
}}x 2 }}x 2 2x
3
2
E
(23x 2 1 3) dx
3
2 x 2 2) dx
5 }}x 3 2 }}x 2 2 2x
3
E
2
21
5 3 x 2 }}x 3
2
21
1
53
E [(2x 1 2) 2 (4 2 x )] dx
3
E
15.
11. Solve x 2 2 2 5 2: x 2 5 4, so the curves intersect at
x 5 62.
E
2
22
[2 2 (x 2 2 2)] dx 5
3
1
3
5 4x 2 }}x 3
E
2
22
(4 2 x 2) dx
3
422 5 18 2 }3}2 2 128 1 }3}2 5 }3} 5 10}3}
8
2
32}2}a, }2}a4 by [2a2, a2]
8
32
2
12. Solve 2x 2 x 2 5 23: x 2 2 2x 2 3 5 (x 2 3)(x 1 1) 5 0,
The curves intersect at x 5 0 and x 5 6a. Use the region’s
symmetry:
E
a
so the curves intersect at x 5 21 and x 5 3.
E
3
3
4
1
5 (9 2 9 1 9) 2 11 1 }} 2 32
3
1
3
(2x 2 x 1 3) dx 5 x 2 }}x 3 1 3x
3
21
21
2
2
32
3
2
3
5 }} 5 10}}
3
3 3
4
1 3
5 230 2 12}}a 24
3
1
2 xÏaw2w2
wwx 2w dx 5 2 2}}(a 2 2 x 2)3/2
0
2
3
5 }}a 3
a
0
296
Section 7.2
18. Solve y 2 5 y 1 2: y2 2 y 2 2 5 (y 2 2)(y 1 1) 5 0, so the
16.
curves intersect at y 5 21 and y 5 2.
E
2
[22, 12] by [0, 3.5]
21
0
3
2
3
5 } 1 }}(2x)3/2
5
4
3
3
21
1
}}x 2 1 6x
2
2
}}x 3/2 2 }
5
3
4
2
9
2
1
2
5 } } 5 4} }
y
4
y2
4
2
3
1 } 2 }}x3/2
5
21
y2
4
y
4
y
4
Now solve }} 2 1 5 }} 1 4: }} 2 }} 2 5 5 0,
4
1
}}x 2 1 6x
2
2 1
y2
4
9
0
1
2
19. Solve for x: x 5 }} 2 1 and x 5 }} 1 4.
0
1
}}x 2 1 6x
2
4
8
1
1
5 2 1 4 2 }} 2 }} 2 2 1 }}
3
2
3
4
21
1
3
1
The curves intersect at three points:
x 5 21, x 5 4 and x 5 9.
Because of the absolute value sign, break the integral up at
x 5 0 also:
x16
x16
E 1}
wxw2 dx 1 E 1}
} 2 Ï2
} 2 Ïxw2 dx 1
5
5
x16
E 1Ïxw 2 }
} dx
5 2
32
(y 1 2 2 y 2) dy 5 }}y 2 1 2y 2 }}y 3
4
y 2 2 y 2 20 5 (y 2 5)(y 1 4) 5 0.
4
1
The curves intersect at y 5 24 and y 5 5.
0
E 31}4y} 1 42 2 1}y4} 2 124 dy
y
y
5 E 12}} 1 }} 1 52 dy
4
4
5
9
2
24
5
4
2
24
3
1
24 1 31
11
2
5 0 2 2}} 1 }}
10
3
31
189
10
2 1
1
6
5
3
2
4
32
16
}} 2 }} 2 0 1
5
3
16
3
32
5
24
18 2 }} 2 }} 2 }}
13
30
16
15
3
y3
12
1
125
12
y2
8
5 2}} 1 }} 1 5y
5
4
24
2 13
25
8
2
16
243
8
3
8
5 2}} 1 }} 1 25 2 }} 1 2 2 20 5 }} 5 30}}
2
3
5 }} 1 }} 1 }} 5 }} 5 1}}
20. Solve for x: x 5 y 2 and x 5 3 2 2y 2. Now solve
17.
y 2 5 3 2 2y 2: y 2 5 1, so the curves intersect at y 5 61.
Use the region’s symmetry:
E (3 2 2y
1
[25, 5] by [21, 14]
2
The curves intersect at x 5 0 and x 5 64. Because of the
absolute value sign, break the integral up
at x 5 62 also (where )x 2 2 4) turns the corner). Use the
graph’s symmetry:
E 31}x2} 1 42 2 (4 2 x )4 dx 1 2E 31}x2} 1 42 2 (x
3x
x
5 2E }} dx 1 2E 12}} 1 82 dx
2
2
2
2
4
2
2
0
2
2
2
4
2
0
2
2
0
E (3 2 3y ) dy
5 6E (1 2 y ) dy
1
2 y 2) dy 5 2
2
0
1
2
0
3
4
1
3
5 6 y 2 }}y 3
4
2 4) dx
31
1
3
1
0
2
4
5 6 1 2 }} 2 0 5 4
2
2
x3 2
x3
5 2 }} 1 2 2}} 1 8x
2 0
6
3 4
3
31
4
21. Solve for x: x 5 2y 2 and x 5 2 2 3y 2.
4
2
2 1
32
4
5 2[4] 1 2 2}} 1 32 2 2}} 1 16
3
3
24
64
3
1
3
5 }} 5 21}}
Now solve 2y 2 5 2 2 3y 2: y 2 5 1, so the curves intersect
at y 5 61. Use the region’s symmetry:
E (2 2 3y 1 y ) dy 5 2E (2 2 2y ) dy
1
1
8
5 4E (1 2 y ) dy 5 43y 2 }}y 4 5 4311 2 }}2 2 04 5 }}
3
3
3
1
2
2
2
0
1
2
0
1
0
2
3
1
0
Section 7.2
22. Solve for y: y 5 4 2 4x 2 and y 5 x 4 2 1.
297
27.
Now solve 4 2 4x 2 5 x 4 2 1:
x 4 1 4x 2 2 5 5 (x 2 2 1)(x 2 1 5) 5 0.
[21.5, 1.5] by [21.5, 1.5]
The curves intersect at x = 61.
The curves intersect at x 5 0 and x 5 61. Use the area’s
Use the region’s symmetry:
symmetry:
E [(4 2 4x ) 2 (x 2 1)] dx
5 2E (2x 2 4x 1 5) dx
1
2
2
4
1
4
E 3sin 1}p2}x 2 2 x4 dx 5 232}p2} cos 1}p2}x 2 2 }12}x 4
1
0
2
2
0
2
0
3
3
1
5
4
3
31
1
5
0
5 }} < 0.273
4
2
4
3
5 2 2}} 2 }} 1 5 2 0
104
15
42p
p
4
28. Use the region’s symmetry, and simplify before integrating:
E
p/4
14
15
2
5 }} 5 6}}
0
E
52E
E1
0
2
E
p/4
E1
2
2
3y 2
3 2 }} dy
0
4
2
y3
5 2 3y 2 }}
4 0
3
34
dx 5 2 x
p/4
p
2
5 }}
0
29. Use the region’s symmetry:
Use the region’s symmetry:
2
[sec2 x 2 (sec2 x 2 1)] dx
0
p/4
0
so the curves intersect at y 5 62.
y2
3 2 y 2 1 }} dy 5 2
4
(sec2 x 2 tan2 x) dx
p/4
52
y2
23. Solve for x: x 5 3 2 y and x 5 2}}.
4
y2 2
2
Now solve 3 2 y 5 2}}: y 5 4,
4
2
2
4
2
0
E
p
0
p
2
E
0
3
(8 cos x 2 sec x) dx 5 2 8 sin x 2tan x
p/4
0
2
24 5 4
E
p/2
30.
0
3
2
3
3 sin y Ïco
wswyw dy 5 3 2}}(cos y)3/2
3
p/2
4
0
1 24 5 2
2
5 3 0 2 2}}
3
p/3
4
4
5 4 2 p < 0.858
0
1
1
2 1 }} 2 22 1 }}
2
2
2
p
4
31
25. Use the region’s symmetry:
p/3
4
5 4 1 2 }} 2 0
4
2 1
tan2 y dy
3
3
31
p/4
0
5 4 tan y 2 y
1
(2 sin x 2 sin 2x) dx 5 22 cos x 1 }} cos 2x
2
5
E
(tan2 y 1 tan2 y) dy5 4
5 2(6 2 2) 2 0 5 8
24.
1 24
1
1
2
5 2 2}} 2 2}}
2
p
0
5 2 2}}x 5 2 }}x 3 1 5x
1
31. Solve for x: x 5 y 3 and x 5 y.
0
5 2[(4Ï3w 2 Ï3w) 2 0] 5 6Ï3w
26.
[21.5, 1.5] by [21.5, 1.5]
The curves intersect at x 5 0 and x 5 61. Use the area’s
[21.1, 1.1] by [20.1, 1.1]
1
The curves intersect at x 5 0 and x 5 61, but they do not
cross at x 5 0.
E 31 2 x
1
2
0
3
1
3
2
px
1 2 24 dx
2 cos }}
px
1
2
p
1 2 24
2
4
5 2 x 2 }}x 3 2 }} sin }}
31
E
0
1
4
2
4
5 2 1 2 }} 2 }} 2 0 5 }} 2 }} < 0.0601
3
3
p
p
32
1
1
4
1
4
1
2
symmetry: 2 ( y 2 y 3) dy 5 2 }}y 2 2 }}y 4 5 }}
0
0
298
Section 7.2
(b) The two areas in Quadrant I, where x 5 Ïyw, are equal:
32.
E Ïyw dy 5 E Ïyw dy
c
4
0
c
3}3}y3/240 5 3}3}y3/24
2
[20.5, 2.5] by [20.5, 1.5]
1
x
0
1
2
1
2
0
1
c 3/2 5 4
2
3
1
2
4
1
2
5 }} 1 2}} 2 (21) 5 1
c 5 42/3 5 24/3
p
4
33. The curves intersect when sin x 5 cos x, i.e., at x 5 }}.
E
p/4
3
(c) Divide the upper right section into a (4 2 c)-by-Ïcw
p/4
4
(cos x 2 sin x) dx 5 sin x 1 cos x
0
c
2c 3/2 5 8
E x dx 1 E }x1} dx 5 3}12}x 4 1 32}1x}4
2
4
2
2
2
}}c 3/2 5 }}43/2 2 }}c 3/2
3
3
3
y 5 x and y 5 }}2 intersect at x 5 1. Integrate in two parts:
1
2
c
rectangle and a leftover portion:
0
5 Ï2w 2 1 < 0.414
E
E
Ïcw
34.
0
2
(c 2 x 2) dx5 (4 2 c)Ïcw 1
Ïcw
3cx 2 }3}x34
1
3
c
[23, 3] by [22, 4]
2
2
0
1 1) dx 5 2
c
31
8
3
2 1
1
3
24
1 8 2 }} 2 4Ïcw 2 }}c3/2
2
16
1
}}c3/2 5 4Ïcw 2 c3/2 1 }} 2 4Ïcw 1 }}c3/2
3
3
3
Use the region’s symmetry:
E (3 2 x
2
4Ïw
1
2 }}c3/2 5 4Ïcw 2 c3/2
3
(a) The curves intersect at x 5 62.
2
1
3
5 4Ïcw 2 c3/2 1 4x 2 }}x 3
0
3/2
(4 2 x 2) dx
Ïcw
E (4 2 x ) dx
2
4
16
}}c3/2 5 }}
3
3
2
0
3
4
1
3
5 2 4x 2 }}x 3
31
2
c3/2 5 4
0
2
4
c 5 42/3 5 24/3
8
32
5 2 8 2 }} 2 0 5 }}
3
3
(b) Solve y 5 3 2 x 2 for x: x 5 6Ï3ww
2wy. The
36.
y-intercepts are 21 and 3.
E
3
21
2Ï3ww
2wy dy
3
4
2
3
5 2 2}}(3 2 y)3/2
3
1
24
16
5 2 0 2 2}}
3
35. (a)
3
21
32
5 }}
3
[21, 5] by [21, 3]
The key intersection points are at x 5 0, x 5 1 and x 5 4.
y
5
y=4
(–2, 4)
y = x2
Integrate in two parts:
E 11 1 Ïxw 2 }4x}2 dx 1 E 1}Ï2}wx 2 }4x}2 dx
(2, 4)
1
y=c
4
0
(–√c, c)
(√c, c)
3
3
x
If y 5 x 2 5 c, then x 5 6Ïcw. So the points are
(2Ïcw, c) and (Ïcw, c).
1
2
x2
5 x 1 }}x 3/2 2 }}
3
8
1
1
x2
4
4 1 34Ïxw 2 }8}4
0
2 3
1
1
24 5 }3}
2
1
1
5 1 1 }} 2 }} 1 (8 2 2) 2 4 2 }}
3
8
8
11
299
Section 7.2
43. First graph y 5 cos x and y 5 x 2.
37. First find the two areas.
1
2
For the triangle, }}(2a)(a 2) 5 a 3
E
a
3
1
3
a
4
4
3
For the parabola, 2 (a 2 2 x 2) dx 5 2 a 2x 2 }}x 3 5 }}a 3
0
3
0
3
4
a
The ratio, then, is } 5 }}, which remains
4
}}a 3
3
[21.5, 1.5] by [20.5, 1.5]
constant as a
The curves intersect at x < 60.8241. Use NINT to find
E
0.8241
approaches zero.
(cos x 2 x 2) dx < 1.0948. Multiplying both
2
0
E [2f (x) 2 f (x)] dx 5 E f (x) dx, which we already know
b
38.
b
a
a
equals 4.
functions by k will not change the x-value of any
intersection point, so the area condition to be met is
E
252
0.8241
(k cos x 2 kx 2) dx
E
0
39. Neither; both integrals come out as zero because the
21-to-0 and 0-to-1 portions of the integrals cancel each
other.
⇒25k?2
40. Sometimes true, namely when dA 5 [f (x) 2 g(x)] dx is
always nonnegative. This happens when f (x) $ g(x) over
the entire interval.
⇒ k < 1.8269.
0.8241
(cos x 2 x 2) dx
0
⇒ 2 < k(1.0948)
44. (a) Solve for y:
41.
x2
y2
}}2 1 }}2 5 1
a
b
x2
a
1
y 2 5 b 2 1 2 }}2
!§§§§
y 5 6b
[21.5, 1.5] by [21.5, 1.5]
The curves intersect at x 5 0 and x 5 61. Use the area’s
symmetry:
2x
E 1}
} 2 x 2 dx 5 23ln 1x
x 11
1
2
0
3
2
2
2
1
4
1 1 2 }}x 4
1
5 2 ln 2 2 }}
2
1
5 ln 4 2 }} < 0.886
2
2
x2
1 2 }}2
a
E 3b!1§§2§}ax}§ 2 12b!1§§2§}ax}§24 dx or
x
x
2E b 1 2 }} dx or 4E b 1 2 }} dx
!§§§a§
!§§§a§
(b)
1
4
0
a
2
2a
a
2
2
2
a
2
2
2a
2
2
0
(c) Answers may vary.
E b!1§§2§}ax}§ dx 5 2b3}2x}!1§§2§}ax}§ 1 }a2} sin }ax}4
(d, e) 2
42.
a
2
2
2a
2
2
3
a
21
2a
a
a
5 2b }} sin21 (1) 2 }} sin21 (21)
2
2
4
5 pab
[21.5, 1.5] by [21.5, 1.5]
The curves intersect at x 5 0 and x < 60.9286. Use NINT
E
45. By hypothesis, f (x) 2 g(x) is the same for each region,
0.9286
to find 2
0
(sin x 2 x 3) dx < 0.4303.
where f (x) and g(x) represent the upper and lower edges.
But then Area 5
each.
E [f (x) 2 g(x)] dx will be the same for
b
a
300
Section 7.3
Quick Review 7.3
1
2
46. The curves are shown for m 5 }}:
1. x 2
x2
x
2. s 5 }}, so Area 5 s 2 5 }}.
2
Ï2w
px 2
2
1
2
3. }}pr 2 or }}
[21.5, 1.5] by [21, 1]
1
2
x
x 11
In general, the intersection points are where }
2 } 5 mx,
!§§§
which is where x 5 0 or else x 5 6
E
Ï(1
w/m
w)2
w1
w
1
1m
4
x
2
x
2
4
x2
1
7. b 5 h 5 }}, so Area 5 }}bh 5 }}.
2
4
Ï2w
8.
5 ln }} 2 1 1 1 2
1
2
2
1
2
2
1
Ï3w
Ï3w
1
5. b 5 x and h 5 }}x, so Area 5 }}bh 5 }}x 2.
6. b 5 h 5 x, so Area 5 }}bh 5 }}.
x
}
} 2 mx dx
0
x2 1 1
Ï(1
w/m
w)2
w1w
1
1
5 2 }} ln (x 2 1 1) 2 }}mx 2
2
2
0
3
px 2
8
or }}
2
1
}} 2 1. Then,
m
because of symmetry, the area is
2
d 2
122
4. }}p }}
2x
2x
2
1
m }} 2 1 5 m 2 ln (m) 2 1.
m
■ Section 7.3 Volumes
x
(pp. 383–394)
Exploration 1
Volume by Cylindrical Shells
1. Its height is f (xk) 5 3xk 2 xk2.
2. Unrolling the cylinder, the circumference becomes one
dimension of a rectangle, and the height becomes the other.
The thickness Dx is the third dimension of a slab with
dimensions 2p(xk 1 1) by 3xk 2 xk2 by Dx. The volume is
obtained by multiplying the dimensions together.
E 2p(x 1 1)(3x 2 x ) dx.
3
3. The limit is the definite integral
2
0
45p
2
4. }}
Exploration 2
1.
Surface Area
E 2py!§§§1§§2§
b
dy 2
1 1 }} dx
dx
a
The limit will exist if f and f 9 are continuous on the interval
[a, b].
b 5 x and h 5
Ï1ww5
!(2§x)§§2§§1}§2}x§2§ 5 }2}x, so
1
2
2
Ï1w5w
1
Area 5 }}bh 5 }}x 2.
2
4
9. This is a 3-4-5 right triangle. b 5 4x, h 5 3x, and
1
2
Area 5 }}bh 5 6x 2.
10. The hexagon contains six equilateral triangles with sides of
Ï3w
3Ï3w
length x, so from Exercise 5, Area 5 6 }}x 2 5 }}x 2.
14 2
2
Section 7.3 Exercises
1. In each case, the width of the cross section is
w 5 2Ï1ww
2wx 2w.
w
2
w 2
122
(a) A 5 pr 2, where r 5 }}, so A(x) 5 p }}
5 p(1 2 x 2).
(b) A 5 s 2, where s 5 w, so A(x) 5 w 2 5 4(1 2 x 2).
dy
dx
2. y 5 sin x, so }} 5 cos x and
E 2py!1§§1§1}§dd}y§x 2§ dx
1wcoww
s wx dx < 14.424.
5 E 2p sin x Ï1ww
b
2
a
p
2
0
dy
1
3. y 5 Ïxw, so }} 5 }} and
dx
2Ïxw
E 2pÏxw!1§§1§1}§2§Ï1}§xw 2§ dx < 36.177.
4
0
2
w
w 2
1 2
(c) A 5 s 2, where s 5 }}, so A(x) 5 }}
Ï2w
Ïw2
5 2(1 2 x 2).
Ïw3
(d) A 5 }}w 2 (see Quick Review Exercise 5), so
4
Ïw3
A(x) 5 }}(2Ï1ww
2wx 2w)2 5 Ï3w(1 2 x 2).
4
Section 7.3
2. In each case, the width of the cross section is w 5 2Ïxw.
w 2
122
w
2
(a) A 5 pr 2, where r 5 }}, so A(x) 5 p }}
5 px.
w 2
1 2
w
(c) A 5 s 2, where s 5 }}, so A(x) 5 }}
Ï2w
Ïw2
8. A cross section has width w 5 sec x 2 tan x.
w 2
122
(a) A(x) 5 pr 2 5 p }}
(b) A 5 s 2, where s 5 w, so A(x) 5 w 2 5 4x.
V5
5 2x.
Ïw3
(d) A 5 }}w 2 (see Quick Review Exercise 5), so
Ïw3
A(x) 5 }}(2Ïxw)2 5 Ï3wx.
3. A cross section has width w 5 2Ïxw and area
0
4. A cross section has width w 5 (2 2 x 2) 2 x 2 5 2 2 2x 2
w 2
and area A(x) 5 pr 5 p }} 5 p(1 2 x 2)2. The volume is
2
2
E
1
21
p(1 2 x ) dx 5 p
2 2
E
1
1 2
21
3
V5
4
21
1
3
1
3
4
w 2
A(x) 5 s 5 }} 5 2(1 2 x 2). The volume is
Ïw2
1
1
1
2(1 2 x 2) dx 5 2 (1 2 x 2) dx 5 2 x 2 }}x 3
3
21
21
1 2
E
E
E }54p}y
2
1
16
3
5 }}.
21
31
E
p/3
3
p
6
2p/3
p/3
2p/3
p
6
2 1
24
(sec x 2 tan x)2 dx, which by same method as
2p/3
122
4
4
2
3
1
8
5 }}.
3
21
Ïw3
(a) A(x) 5 }}w 2 5 Ï3w sin x, and
5p
4 2
5 }}y 4. The volume is
p
4
3 4
dy 5 }} y 5
5 8p.
0
10. A cross section has width w 5 2Ï1ww
2wy 2w and area
1
1
}}s 2 5 }}w 2 5 2(1 2 y 2). The volume is
21
2
1
1
8
2(1 2 y 2) dy 5 2 y 2 }}y 3
5 }}.
3 21
3
21
E
7. A cross section has width w 5 2Ïsi
wnwwx.
3
4
11. (a) The volume is the same as if the square had moved
without twisting: V 5 Ah 5 s 2h.
(b) Still s 2h: the lateral distribution of the square cross
sections doesn’t affect the volume. That’s Cavalieri’s
Volume Theorem.
12. Since the diameter of the circular base of the solid extends
4
12
2
from y 5 }} 5 6 to y 5 12, for a diameter of 6 and a radius
E Ï3w sin x dx
5 Ï3wE sin x dx
V5
p
2
4
1
2
w 2
6. A cross section has width w 5 2Ï1ww
2wx 2w and area
2
3
pr 2 5 p }}
(1 2 x 2) dx 5 4 x 2 }}x 3
21
p
2
p/3
9. A cross section has width w 5 Ï5wy 2 and area
21
A(x) 5 s 2 5 w 2 5 4(1 2 x 2). The volume is
E
4
in part (a) equals 4Ï3w 2 }}p.
0
4(1 2 x 2) dx 5 4
3
(sec2 x 2 2 sec x tan x 1 tan2 x) dx
(b) A(x) 5 s 2 5 w 2 5 (sec x 2 tan x)2, and
1
5. A cross section has width w 5 2Ï1ww
2wx 2w and area
1
p
4
p/3
2p/3
p2
6
2
1
2
5 p }}x 5 2 }}x 3 1 x
5
3
16
5 }}p.
15
E
E
5 pÏ3w 2 }}.
(x 2 2x 1 1) dx
4
p
4
5 }} Ï3w 2 2 2 }} 2 2Ï3w 2 2 1 }}
4
0
p
}}(sec x 2 tan x)2 dx
2p/3 4
5 }} tan x 2 sec x 2 }}x
2
1 2 5 2x. The volume is
E 2x dx 5 3x24 5 16.
4
p/3
p
4
5 }}(sec x 2 tan x)2, and
5 }} tan x 2 2 sec x 1 tan x 2 x
4
w
A(x) 5 s 5 }}
Ïw2
E
5 }}
4
2
301
p
of 3, the solid has the same cross sections as the right
0
p
0
3
5 Ï3w 2cos x
circular cone. The volumes are equal by Cavalieri’s
p
4
Theorem.
0
5 2Ï3w.
13. The solid is a right circular cone of radius 1 and height 2.
1
3
V5
E 4 sin x dx 5 4E sin x dx 5 432cos x4
p
0
p
0
1
3
1
3
2
3
V 5 }}Bh 5 }}(pr 2)h 5 }}(p12)2 5 }}p
(b) A(x) 5 s 2 5 w 2 5 4 sin x, and
p
0
5 8.
14. The solid is a right circular cone of radius 3 and height 2.
1
3
1
3
1
3
V 5 }}Bh 5 }}(pr 2)h 5 }}(p32)2 5 6p
302
Section 7.3
p
14 2
15. A cross section has radius r 5 tan }}y and area
p
19.
14 2
p
E p tan2 1}4}y2 dy 5 p3}p4} tan 1}p4}y2 2 y4
4
5 p1}} 2 12
p
A(y) 5 pr 2 5 p tan2 }}y . The volume is
1
1
0
[26, 6] by [24, 4]
0
The solid is a sphere of radius r 5 3. The volume is
5 4 2 p.
4
}}pr 3 5 36p.
3
16. A cross section has radius r 5 sin x cos x and area
20.
A(x) 5 pr 2 5 p sin2 x cos2 x. The shaded region extends
from x 5 0 to where sin x cos x drops back to 0, i.e., where
[20.5, 1.5] by [20.5, 0.5]
p
2
x 5 }}. Now, since cos 2x 5 2 cos2 x 2 1, we know
1 1 cos 2x
cos x 5 }} and since cos 2x 5 1 2 2 sin2 x, we
2
p/2
1 2 cos 2x
2
know sin x 5 }}.
p sin2 x cos2 x dx
0
2
p/2
1 2 cos 2x 1 1 cos 2x
5p
}} ? }} dx
0
2
2
p/2
p/2
p
p
2
5 }}
(1 2 cos 2x) dx 5 }}
sin2 2x dx
0
0
4
4
p/2
p/2
p
1 2 cos 4x
p
5 }}
(1 2 cos 4x) dx
}} dx 5 }}
4 0
2
8 0
p/2
p
1
p p
p2
5 }} x 2 }} sin 4x
5 }} }} 2 0 2 0 5 }}.
8
4
8 2
16
0
The parabola crosses the line y 5 0 when
2
x 2 x 2 5 x(1 2 x) 5 0, i.e., when x 5 0 or x 5 1. A cross
E
E
E
E
E
3
4
section has radius r 5 x 2 x 2 and area
A(x) 5 pr 2 5 p(x 2 x 2)2 5 p(x 2 2 2x 3 1 x 4).
The volume is
E
31
2
E p(x
1
0
2
33
1
1
2
1
5
4
1
p
30
2 2x 3 1 x 4) dx 5 p }}x 3 2 }}x 4 1 }}x 5 5 }}.
0
21.
4
17.
[21, 2] by [21, 2]
Use cylindrical shells: A shell has radius y and height y.
The volume is
E 2p(y)( y) dy 5 2p3}13}y 4
1
[22, 4] by [21, 5]
3
0
A cross section has radius r 5 x 2 and area
1
0
2
3
5 }}p.
22.
A(x) 5 pr 2 5 px4. The volume is
E px
2
4
0
2
35 4
1
32p
5
dx 5 p }}x 5 5 }}.
0
[21, 3] by [21, 3]
18.
Use washer cross sections: A washer has inner radius r 5 x,
outer radius R 5 2x, and area A(x) 5 p(R 2 2 r 2) 5 3px 2.
E 3px
1
The volume is
[24, 6] by [21, 9]
0
A cross section has radius r 5 x and area
3
A(x) 5 pr 2 5 px 6. The volume is
E px
2
0
6
2
37 4
1
128p
7
dx 5 p }}x 7 5 }}.
0
2
33 4
1
1
dx 5 3p }}x 3 5 p.
0
Section 7.3
23.
303
26.
[22, 3] by [21, 6]
[21, 5] by [23, 1]
The curves intersect when x 2 1 1 5 x 1 3, which is when
x 2 2 x 2 2 5 (x 2 2)(x 1 1) 5 0, i.e., when
x 5 21 or x 5 2. Use washer cross sections: a washer has
inner radius r 5 x 2 1 1, outer radius R 5 x 1 3, and area
A(x) 5 p(R 2 2 r 2)
5 p[(x 1 3)2 2 (x2 1 1)2]
5 p(2x 4 2 x 2 1 6x 1 8). The volume is
E
2
21
The curves intersect where 2Ïxw 5 22, which is where
x 5 4. Use washer cross sections: a washer has inner radius
r 5 Ïwx, outer radius R 5 2, and area
A(x) 5 p(R 2 2 r 2) 5 p(4 2 x).
E p(4 2 x) dx 5 p34x 2 }12}x 4
4
The volume is
2
0
4
5 8p
0
27.
p(2x 4 2 x 2 1 6x 1 8) dx
3
1
5
2
1
3
5 p 2}}x5 2 }}x 3 1 3x 2 1 8x
31
4
21
2 1
32
8
1
1
5 p 2}} 2 }} 1 12 1 16 2 }} 1 }} 1 3 2 8
5
3
5
3
24 5 }5}.
[20.5, 1.5] by [20.5, 2]
117p
The curves intersect at x < 0.7854. A cross section has
24.
radius r 5 Ï2w 2 sec x tan x and area
A(x) 5 pr 2 5 p(Ï2w 2 sec x tan x)2. Use NINT to find
E
0.7854
[22, 3] by [21, 5]
The curves intersect when 4 2 x 2 5 2 2 x, which is when
x2 2 x 2 2 5 (x 2 2)(x 1 1) = 0, i.e., when x 5 21 or
x 5 2. Use washer cross sections: a washer has inner radius
r 5 2 2 x, outer radius R 5 4 2 x 2, and area
A(x) 5 p(R 2 2 r 2)
5 p[(4 2 x 2)2 2 (2 2 x)2]
5 p(12 1 4x 2 9x 2 1 x 4).
28.
[21, 3] by [21, 3]
p
2
The curve and horizontal line intersect at x 5 }}. A cross
The volume is
E
2
21
section has radius 2 2 2 sin x and area
p(12 1 4x 2 9x 2 1 x 4) dx
3
1
5
5 p 12x 1 2x 2 2 3x 3 1 }}x 5
31
p(Ï2w 2 sec x tan x)2 dx < 2.301.
0
A(x) 5 pr 2 5 4p(1 2 sin x)2 5 4p(1 2 2 sin x 1 sin2 x).
2
4
The volume is
21
E
p/2
2 1
32
1
5 p 24 1 8 2 24 1 }} 2 212 1 2 1 3 2 }}
5
5
24
108p
5 }}.
5
0
4p(1 2 2 sin x 1 sin2 x) dx
p/2
32
4
4
3p
5 4p1}} 2 22 5 p(3p 2 8)
4
3
1
5 4p }}x 1 2 cos x 2 }}sin 2x
25.
0
29.
3
p p
2}}, }} by [20.5, 2]
3
3
4
Use washer cross sections: a washer has inner radius
r 5 sec x, outer radius R 5 Ï2w, and area
A(x) 5 p(R 2 2 r 2) 5 p(2 2 sec2 x).
The volume is
E
p/4
A cross section has radius r 5 Ï5wy 2 and area
3
p(2 2 sec2 x) dx 5 p 2x 2 tan x
2p/4
[21, 3] by [21.5, 1.5]
31
p/4
4
A(y) 5 pr 2 5 5py 4.
2p/4
p
2
2 1
p
2
5 p }} 2 1 2 2}} 1 1
5 p 2 2 2p.
E
1
24
The volume is
21
1
3 4
5py 4 dy 5 p y 5
21
5 2p.
304
Section 7.3
30.
35.
[21, 4] by [21, 3]
[21, 5] by [21, 3]
The curved and horizontal line intersect at (4, 2).
A cross section has radius r 5 y 3/2 and area
(a) Use washer cross sections: a washer has inner radius
A(y) 5 pr 2 5 py 3. The volume is
E py
2
0
3
2
r 5 Ïxw, outer radius R 5 2, and area
0
A(x) 5 p(R 2 2 r 2) 5 p(4 2 x). The volume is
34 4
1
dy 5 p }}y 4 5 4p.
31.
E p(4 2 x) dx 5 p34x 2 }12}x 4
4
2
0
4
5 8p
0
(b) A cross section has radius r 5 y 2 and area
A(y) 5 pr 2 5 py 4.
[21.2, 3.5] by [21, 2.1]
E py
2
Use washer cross sections. A washer has inner radius r 5 1,
The volume is
0
outer radius R 5 y 1 1, and area
E p(y
1
2
0
3
1
4
1
3
1
2
32p
5
5 }}.
0
A(x) 5 pr 25 p(2 2 Ïxw)2 5 p(4 2 4Ïxw 1 x).
4
3
1 2y) dy 5 p }}y 3 1 y 2 5 }}p.
0
35 4
dy 5 p }}y 5
(c) A cross section has radius r 5 2 2 Ïxw and area
A(y) 5 p(R 2 2 r 2) 5 p[(y 1 1)2 2 1] 5 p(y 2 1 2y). The
volume is
4
The volume is
32.
E p(4 2 4Ïxw 1 x) dx 5 p34x 2 }83}x
4
3/2
0
1
2
4
4
8p
3
1 }}x 2 5 }}.
0
(d) Use washer cross sections: a washer has inner radius
[21.7, 3] by [21, 2.1]
r 5 4 2 y 2, outer radius R 5 4, and area
Use cylindrical shells: a shell has radius x and height x. The
E
1
3 4
1
volume is 2p(x)(x) dx 5 2p }}x 3
3
0
A(y) 5 p(R 2 2 r 2) 5 p[16 2 (4 2 y 2)2]
1
2
5 }}p.
3
0
5 p(8y 2 2 y4).
33.
The volume is
E p(8y
2
0
2
33
8
2
224p
15
4
1
5
2 y 4) dy 5 p }}y 3 2 }}y 5 5 }}
0
36.
[22, 4] by [21, 5]
Use cylindrical shells: A shell has radius x and height x 2.
E 2p(x)(x ) dx 5 2p3}14}x 4 5 8p.
2
The volume is
2
4
0
2
0
34.
[21, 3] by [21, 3]
The slanted and vertical lines intersect at (1, 2)
(a) The solid is a right circular cone of radius 1 and
height 2. The volume is
[20.5, 1.5] by [20.5, 1.5]
The curves intersect at x 5 0 and x 5 1. Use cylindrical
shells: a shell has radius x and height Ïxw 2 x. The volume
E 2p(x)(Ïxw 2 x) dx 5 2p3}25}x
1
is
0
5/2
1
3
1
4
2p
15
2 }}x 3 5 }}.
0
1
1
1
2
}}Bh 5 }}(pr 2)h 5 }}(p12)2 5 }}p.
3
3
3
3
(b) Use cylindrical shells: a shell has radius 2 2 x and
height 2x. The volume is
E 2p(2 2 x)(2x) dx 5 4pE (2x 2 x ) dx
1
0
1
2
0
3
1
3
4
1
8p
3
5 4p x 2 2 }}x 3 5 }}.
0
305
Section 7.3
40.
37.
[22, 2] by [21, 2]
[22, 2] by [21, 3]
The curves intersect at (61, 1).
x 2 5 2 2 x at x 5 1. A shell has radius x and height
(a) A cross section has radius r 5 1 2 x 2 and area
2 2 x 2 x 2. The volume is
E 2p(x)(2 2 x 2 x ) dx 5 2p3x
A(x) 5 pr 2 5 p(1 2 x 2)2 5 p(1 2 2x 2 1 x 4).
1
1
21
2
0
The volume is
E
2
3
2
3
4
1
5
p(1 2 2x 2 1 x 4) dx 5 p x 2 }}x 3 1 }}x 5
1
16p
15
1
3
1
4
1
5p
6
4
2 }}x 3 2 }}x 4 5 }}.
0
41.
5 }}.
21
(b) Use cylindrical shells: a shell has radius 2 2 y and
height 2Ïyw. The volume is
[21, 5] by [21, 3]
E 2p(2 2 y)(2Ïyw) dy 5 4pE (2Ïyw 2 y
1
1
0
3/2
0
3
4
2
5 4p }}y 3/2 2 }}y 5/2
3
5
A shell has radius x and height Ïxw. The volume is
) dy
E 2p(x)(Ïxw) dx 5 2p3}25}x 4 5 }1258p}.
1
56p
5 }}.
15
0
4
4
(c) Use cylindrical shells: a shell has radius y 1 1 and
5/2
0
4
0
42.
height 2Ïyw. The volume is
E 2p(y 1 1)(2Ïyw) dy 5 4pE ( y
1
1
0
3/2
0
1 Ïyw) dy
3
2
2
5 4p }}y 5/2 1 }}y 3/2
5
3
1
x
b
64p
5 }}.
15
0
4
2
38. (a) A cross section has radius r 5 h 1 2 }} and area
1
x 2
b
2
2
x
E ph211 2 }b}2 dx 5 ph232}b3}11 2 }bx}234
A(x) 5 pr 2 5 ph 2 1 2 }} . The volume is
b
0
[22, 2] by [22, 2]
1
b
p
5 }}bh 2.
3
0
The functions intersect where 2x 2 1 5 Ïxw, i.e., at x 5 1.
A shell has radius x and height
Ïxw 2 (2x 2 1) 5 Ïxw 2 2x 1 1. The volume is
E 2p(x)(Ïxw 2 2x 1 1) dx 5 2pE (x
1
1
0
1
2
E 2p(x)h11 2 }bx}2 dx5 2phE 1x 2 }xb}2 dx
1
p
x
5 2ph3}}x 2 2 }}4 5 }}b 2h.
2
3
3b
x
b
b
b
0
2
0
3 b
35
2
2 2x 2 1 x) dx
2
3
7p
15
5 }}.
E 2p(y)12(y
1
0
2
E
1
2 y 3) dy 5 24p ( y 3 2 y 4) dy
0
34
1
1
5
E 2p(1 2 y)12(y 2 y ) dy
5 24pE ( y 2 2y 1 y ) dy
1
0
2
0
2
1
4
3
3
2
0
35
1
1
2
1
3
1
4
4p
5
5 24p }}y 5 2 }}y 4 1 }}y 3 5 }}.
x
3
2
0
1
4
6p
5
5 24p }}y 4 2 }}y 5 5 }}.
(b) A shell has radius 12 y. The volume is
1 22 2
3
The volume is E 2p(x)1}}x2 dx 5 p3x 34 5 8p.
2
0
(a) A shell has radius y. The volume is
39.
A shell has radius x and height x 2 2}} 5 }}x.
1
4
43. A shell has height 12(y 2 2 y 3).
0
[22, 3] by [22, 3]
1
2
5 2p }}x 5/2 2 }}x 3 1 }}x 2
(b) Use cylindrical shells: a shell has radius x and height
h 1 2 }} . The volume is
3/2
0
0
0
306
Section 7.3
43. continued
45.
8
5
(c) A shell has radius }} 2 y. The volume is
E 2p1}85} 2 y212( y 2 y ) dy
13
8
5 24pE 1 y 2 }}y 1 }}y 2 dy
5
5
1
2
3
0
1
4
3
[21, 3] by [21.4, 9.1]
2
The functions intersect at (2, 8).
0
35
1
13
20
8
15
1
4
5 24p }}y 5 2 }}y 4 1 }}y 3 5 2p.
(a) Use washer cross sections: a washer has inner radius
0
r 5 x 3, outer radius R 5 4x, and area
2
5
(d) A shell has radius y 1 }}. The volume is
E 1
1
A(x) 5 p(R2 2 r 2) 5 p(16x 2 2 x 6). The volume is
2
2
2p y 1 }} 12( y 2 2 y 3) dy
5
0
1
2
3
5 24p 2y 4 1}}y 3 1 }}y 2 dx
5
5
0
1
1 5
3 4
2
5 24p 2}}y 1}}y 1 }}y 3 5 2p.
5
20
15 0
E1
E p(16x
2
2
4
3
0
33
16
y
4
E 2p(8 2 y)1y 2 }4y}2 dy
y
5 2pE 18y 2 2y 2 y 1 }}2 dy
4
8
1/3
0
8
1/3
2
4/3
0
3
(a) A shell has radius y. The volume is
E 2p(y)1 y
2
0
4
y
4
2
34
1
1
24
512p
21
0
height y 1/3 2 }}. The volume is
1
2
2
4
1
7
2 x 6) dx 5 p }}x 3 2 }}x 7 5 }}.
(b) Use cylindrical shells: a shell has a radius 8 2 y and
y2
y4
44. A shell has height }} 2 }} 2
2
4
y2
y4
}} 5 y 2 2 }}.
2
4
2
2
2
4
8p
3
2 }} dy 5 2p }}y 4 2 }}y 6 5 }}.
0
3
7
8
832p
21
4
1
12
5 2p 6y 4/3 2 y 2 2 }}y 7/3 1 }}y 3 5 }}.
0
46.
(b) A shell has radius 2 2 y. The volume is
E 2p(2 2 y)1 y 2 }y4}2 dy
y
y
5 2pE 1 }} 2 }} 2 y 1 2y 2 dy
4
2
2
4
2
0
2
5
4
3
[20.5, 1.5] by [20.5, 1.5]
2
The functions intersect at (0, 0) and (1, 1).
0
3
1
2
1
1
5 2p }}y 6 2 }}y 5 2 }}y 4 1 }}y 3
4
3
24
10
2
8p
5 }}.
5
0
4
(c) A shell has radius 52 y. The volume is
E
2
y4
2p(5 2 y) y 2 2 }} dy
4
0
2 5
y
5y 4
5 2p }} 2 }} 2 y 3 1 5y 2 dy
4
0 4
2
1 5
1
5
1 6
5 2p }}y 2 }}y 2 }}y 4 1 }}y 3 5 8p.
4
4
3 0
24
E1
1
2
2
3
4
(a) Use cylindrical shells: a shell has radius x and height
2x 2 x 2 2 x 5 x 2 x 2. The volume is
E 2p(x)(x 2 x ) dx 5 2p3}13}x
1
2
3
0
5
8
4
2
0
2
5
4
3
2
0
3
1
24
1
32
1
4
5
24
4
2
5 2p 2}}y 6 2 }}y 5 1 }}y 4 1 }}y 3 5 4p.
0
0
p
6
5 }}.
height 2x 2 x 2 2 x 5 x 2 x 2. The volume is
E 2p(1 2 x)(x 2 x ) dx 5 2pE (x
1
1
2
0
34
1
3
2 2x 2 1 x) dx
2
3
1
2
5 2p }}x 4 2 }}x 3 1 }}x 2
p
6
5 }}.
E 2p1 y 1 }58}21 y 2 }y4}2 dy
y
5y
5y
5 2pE 12}} 2 }} 1 y 1 }}2 dy
4
32
8
2
1
4
(b) Use cylindrical shells: a shell has radius 1 2 x and
0
(d) A shell has radius y 1 }}. The volume is
1
4
2 }}x 4
1
4
0
Section 7.3
47.
307
(a) Solve
p2
d
}} p 2c 2 2 4pc 1 }} 5 0
2
dc
3
4
2p 2c 2 4p 5 0
[20.5, 2.5] by [20.5, 2.5]
pc 2 2 5 0
14 2 14 2
1
1
The intersection points are }}, 1 , }}, 2 , and (1, 1).
2
p
c 5 }}
1
1
(a) A washer has inner radius r 5 }}, outer radius R 5 }}2 ,
4
y
1
1
and area p(R 2 2 r 2) 5 p }}4 2 }} . The volume is
y
16
2
2
11p
1
1
1
1
p }}4 2 }} dy 5 p 2}}3 2 }}y 5 }}.
48
y
16
3y
16 1
1
1
E 1
2
2
3
1
1
1
2
1
a 2V
5 2p 2 . 0.
}}
dc 2
4
(b) A shell has radius x and height }} 2 1. The volume is
Ïwx
E
This value of c gives a minimum for V because
3
2
1
2p(x) }} 2 1 dx 5 2p }}x 3/2 2 }}x 2
3
2
1/4
Ïwx
1
4
2 2
1p 2
Then the volume is p 2 }}
p2
2
p2
2
2
p
anywhere else besides c 5 }}, the maximum must occur
11p
48
p2
2
at c 5 0 or c 5 1. The volume for c 5 0 is }} < 4.935,
x(sin x)
x
p(3p 2 8)
2
48. (a) For 0 , x # p, x f (x) 5 }} 5 sin x.
and for c 5 1 it is }} < 2.238. c 5 0
For x 5 0, x f (x) 5 0 ? 1 5 sin 0 5 sin x. So
x f (x) 5 sin x for 0 # x # p.
2
(b) Since the derivative with respect to c is not zero
5 }}.
1/4
1p 2
2 4p }} 1 }} 5 }} 2 4
maximizes the volume.
(c)
(b) Use cylindrical shells: a shell has radius x and height y.
E 2pxy dx, which from part (a) is
p
The volume is
E 2p sin x dx 5 2p32cos x4
0
p
0
p
5 4p.
[0, 2] by [0, 6]
0
x
49. (a) A cross section has radius r 5 }}Ï3w6ww
2wx 2w and area
12
p
A(x) 5 pr 2 5 }}(36x 2 2 x 4). The volume is
144
6
6
1
36p
p
p
}}(36x 2 2 x 4) dx 5 }} 12x 3 2 }}x 5 5 }} cm3.
5 0
5
144
0 144
E
1
3
36p
5
4
The volume gets large without limit. This makes sense,
since the curve is sweeping out space in an
ever-increasing radius.
d 2
122
C
p
51. (a) Using d 5 }}, and A 5 p }}
C2
4p
5 }} yields the
following areas (in square inches, rounded to the
nearest tenth): 2.3, 1.6, 1.5, 2.1, 3.2, 4.8, 7.0, 9.3, 10.7,
2
(b) }} cm3 (8.5 g/cm3) < 192.3 g
10.7, 9.3, 6.4, 3.2.
50. A cross section has radius r 5 )c 2 sin x) and area
(b) If C(y) is the circumference as a function of y, then the
A(x) 5 pr 2 5 p(c 2 sin x)2 5 p(c 2 2 2c sin x 1 sin2 x).
area of a cross section is
The volume is
E p(c
p
2
0
3
31
C(y)/p 2
C 2( y)
5 }},
2
4p
6
1
and the volume is }} C 2(y) dy.
4p 0
1
2
A(y) 5 p }}
2 2c sin x 1 sin2 x) dx
4
1
1
5 p c x 1 2c cos x 1 }}x 2 }}sin 2x
2
4
1
2
5 p c p 2 2c 1 }}p 2 2c
2
p2
2 2
5 p c 2 4pc 1 }}.
2
2
2
4
p
0
1
4p
E
E
E
6
6
1
4p 0
1 620
< }} }} [5.42 1 2(4.52 1 4.42
4p 24
(c) }} A( y) dy 5 }} C 2(y) dy
0
1
2
1 5.1 1 6.3 1 7.8 1 9.42 1 10.82 1 11.62
2
2
2
1 11.62 1 10.82 1 9.02) 1 6.32] < 34.7 in.3
308
Section 7.3
52. (a) A cross section has radius r 5 Ï2wyw and area
pr 2 5 2py. The volume is
E 2py dy 5 p3y 4 5 25p.
5
2
0
0
E
dV
(b) V(h) 5 A(h) dh, so }} 5 A(h).
dh
dV
dV dh
dh
[ }} 5 }} ? }} 5 A(h) ? }},
dt
dh dt
dt
dh
dV
1
so }} 5 }} ? }}
dt
A(h) dt
For h 5 4, the area is 2p(4) 5 8p,
dh
1
so }} 5 }}
dt
8p
53. (a)
units3
3
3 }} = }}
sec
8p
?
?
55. Solve ax 2 x 2 5 0: This is true at x 5 0 and x 5 a. For
5
revolution about the x-axis, a cross section has radius
r 5 ax 2 x 2 and area
A(x) 5 pr 2 5 p(ax 2 x 2)2 5 p(a 2x 2 2 2ax 3 1 x 4).
The volume is
E p(a x
a
2 2
0
33
1
1
2
1
5
4
2 2ax 3 1 x 4) dx 5 p }}a 2x 3 2 }}ax 4 1 }}x 5
units3
}}.
sec
a
0
1
5 }}pa 5.
30
y
For revolution about the y-axis, a cylindrical shell has
2
r
radius x and height ax 2 x 2. The volume is
x
E 2p(x)(ax 2 x ) dx 5 2p3}13}ax
a
2
3
0
4
a
1
6
0
Setting the two volumes equal,
–2
The remaining solid is that swept out by the shaded
region in revolution. Use cylindrical shells: a shell has
r 2w
2wx 2w. The volume is
radius x and height 2Ïw
E.
1
4
2 }}x 4 5 }}pa 4.
1
1
1
1
}}pa 5 5 }}pa 4 yields }}a 5 }}, so a 5 5.
30
6
30
6
56. The slant height Ds of a tiny horizontal slice can be
written as Ds 5 ÏD
ww
x 2w
1w
Dw
y 2 5 Ï1ww
1w( gw9(
wy)
ww
)2Dy. So the
.r
Ïw
r 2w
2w
22w
3
2p(x)(2Ïw
r 2w
2wx 2w) dx
n
1w(gw9(
wy)
ww
)2 Dy. The limit of that is the
Σ 2pg( yk)Ï1ww
k51
r
2
3
5 2p 2}}(r 2 2 x 2)3/2
4
3
surface area is approximated by the Riemann sum
4Ïwww
integral.
r2 2 4
32p
3
5 2}}p(28) 5 }}.
dx
(b) The answer is independent of r.
1
57. g9( y) 5 }} 5 }}, and
dy
2Ïyw
E 2pÏyw!1§§1§1}§2§Ï1}§yw 2§ dy 5 E pÏ4wyw1ww1 dy
2
2
2
0
54. Partition the appropriate interval in the axis of revolution
0
p
36
and measure the radius r(x) of the shadow region at these
E pr (x) dx.
b
a
2
0
13p
5 }} < 13.614
3
points. Then use an approximation such as the trapezoidal
rule to estimate the integral
4
5 }}(4y 1 1)3/2
2
dx
dy
58. g9( y) 5 }} 5 y 2, and
E 2p1}y3}2Ï1ww1w( wy w) dy 5 }23}p3}16}(1 1 y ) 4
1
3
2 2
4 3/2
0
p
9
1
0
5 }}(2Ï2w 2 1) < 0.638.
dx
dy
1
2
59. g9( y) 5 }} 5 }} y21/2 , and
E 2p3y 2 1}13}2 4!1§§1§3}§12}y§§§4§ dy
1
1
5 2pE 3y 2 1}}2 4 1 1 }} dy.
!§§§4§y
3
3
3/2
1/2
21/2
2
1
3
1/2
3/2
1
Using NINT, this evaluates to <16.110
309
Section 7.3
66. Use washer cross sections: a washer has inner radius
dx
1
60. g9( y) 5 }} 5 }}, and
dy
Ï2ww
y2
ww1
E
1
r 5 b 2 Ïaw2w2
wwy 2w, outer radius R 5 b 1 Ïaw2w2
wwy 2w, and
area p(R2 2 r 2)
!§§§1§§§§§2 dy
2
1
2pÏ2wyw2
ww1 1 1 }}
5/8
Ï2wyw2
ww1
5 2p
E
1
5 p[(b 1 Ïaw2w2
wwy 2w)2 2 (b 2 Ïaw2w2
wwy 2w)2]
Ï2wyw dy
5 4pbÏaw2w2
wwy 2w. The volume is
5/8
3
2
3
5 2Ï2wp }}y3/2
E
a
1
4
2a
5/8
E
pa 2
122
!§2
5 2p 2a2b
dy
dx
61. f 9(x) 5 }} 5 2x, and
E 2px Ï1ww1w(2wx)ww dx 5 E 2px Ï1ww1w4wx dx evaluates,
2
2
2
0
2
2
67. (a) Put the bottom of the bowl at (0, 2a). The area of a
2
wwy 2w)2 5 p(a2 2 y 2).
horizontal cross section is p(Ïaw2w2
0
The volume for height h is
using NINT, to < 53.226.
E
h2a
2a
dy
dx
62. f 9(x) 5 }} 5 3 2 2x, and
E 2p(3x 2 x )Ï1ww1w(3ww2w2x)ww dx evaluates, using NINT,
3
2
3
h2a
4
2a
ph2(3a 2 h)
3
5 }}.
p(52 2 12) 5 24p. The rate of rise is
dh
1 dV
1
1
}} 5 }} }} 5 }}(0.2) 5 }} m/sec.
dt
A dt
24p
120p
to < 44.877.
12x
dy
68. (a) A cross section has radius r 5 Ïaw2w2
wwx 2w and area
63. f 9(x) 5 }} 5 }}, and
dx
Ï2wxw2
wwx 2w
E
1.5
!§§§1§§§§§§2§
12x
2pÏ2wxw2
wwx 2w 1 1 }}
0.5
Ï2wxw2
wwx 2w
2
dx 5 2p
E
1 dx
0.5
volume is
1.5
34
0.5
5 2p < 6.283
dy
A(x) 5 pr 2 5 p(Ïaw2w2
wwx 2w)2 5 p(a2 2 x 2). The
1.5
5 2p x
E
a
2a
p(a2 2 x 2) dx
1
1
E 2pÏxw1ww1!1§§1§1}
§2§Ï§wx}
§1w§w1 §2 dx
5
a
3
1
3
4
31
1
3
2 1
5 p a2x 2 }}x 3
2a
1
3
5 p a3 2 }}a3 2 2a3 1 }}a3
64. f 9(x) 5 }} 5 }}, and
dx
2Ïxw1
ww1
2
24
4
3
5 }}pa3.
1
E !x§1§§}54}§ dx
5
1
5
5 3/2
331
2
4
25 3/2
31 4 2
5 }} }}
2 4
1
2
1
9 3/2
49p
1 4 2 4 5 }3} < 51.313
2 }}
area: pR2 2 ph2 5 A2
Since A1 5 A2, the two volumes are equal by Cavalieri’s
5 volume of cylinder 2 volume of cone
2
3
1
2
E pr 11 2 }2h}y 1 }hy}2 dy5 pr 3 y 2 }yh} 1 }3yh}4
h
2 2
Right circular cylinder with cone removed cross sectional
theorem. Thus, volume of hemisphere
2
volume is
ww2
wwhw) 5 A1.
65. Hemisphere cross sectional area: p(ÏR
5 pR3 2 }}pR3 5 }}pR3.
2y
y 2
y2
5 pr 2 1 2 }} 1 }}2 . The
h
h
h
A(y) 5 px 2 5 pr 2 1 2 }}
2
1
3
y
h
(b) A cross section has radius x 5 r 1 2 }} and area
1
5 2p }} x 1 }}
4p
3
1
3
p(a2 2 y 2) dy 5 p a2y 2 }}y 3
(b) For h 5 4, y 5 21 and the area of a cross section is
2
0
5 2p
Ïaw2w2
wwy 2w dy
2a
5 4pb }}
4Ïw2
5 5
5 }}p 1 2 }} }} < 2.997.
3
16 2
1
a
4pbÏaw2w2
wwy 2w dy5 4pb
0
2
2
2
2
2
3
h
2
0
1
5 }}pr 2h.
3
310
Section 7.4
■ Section 7.4 Lengths of Curves
3. (a) x9 5 cos y, so Length 5
(pp. 395–401)
(b)
E Ï1ww1wcowws wy dy.
p
2
0
Quick Review 7.4
1. Ï1ww
1w2xw1
wwx 2w 5 Ï(1
ww
1wxw
)2, which, since x $ 21, equals
1 1 x or x 1 1.
2.
!1§§2§x§1§}4}§ 5 !§11§2§}2}§2§, which, since x # 2, equals
x 2
x2
22x
2
x
2
1 2 }} or }}.
p
3. Ï1ww
1w(ta
wnwwxw
)2 5 Ï(s
wec
wwxw
)2, which, since 0 # x , }},
2
equals sec x.
4.
§§§x}
§§ which,
!1§§1§1}§4}§2§}x}§2§ 5 !}§2}§1§}1§}6 x§§1§}x}§ 5 }4}!}
x
1 2
1
1 2
1
1
(x 2 1 4)2
2
[21, 2] by [21, 4]
(c) Length < 3.820
4. (a) x9 5 2y(1 2 y 2)21/2, so
Length 5
y
E !1§§1§}
} dy.
1§
2§y §
1/2
2
2
21/2
(b)
2
x2 1 4
4x
since x . 0, equals }}.
p
2
p
2
1wcowsw2wxw 5 Ï2wwcoww
s2wx, which, since 2}} # x # }},
5. Ï1ww
equals Ï2w cos x.
[21, 2] by [21, 1]
(c) Length < 1.047
6. f (x) has a corner at x 5 4.
5. (a) y 2 1 2y 5 2x 1 1, so
10
d
y 2 1 2y 1 1 5 (y 1 1)2 5 2x 1 2, and
7. }}(5x 2/3) 5 }3} is undefined at x 5 0. f (x) has a cusp
dx
3Ïwx
there.
d 5
dx
1
y 5 Ï2wxw1
ww2 2 1. Then y9 5 }}, and
Ï2wxw1
ww2
7
1
Length 5
1 1 }} dx.
E !§§§2x§§1§2
1
5(x13)
8. }}(Ïx1
w3w) 5 }}
4/5 is undefined for x 5 23.
21
(b)
f (x) has a vertical tangent there.
9. Ïw
x 2w
2w4xw1
ww4 5 )x 2 2) has a corner at x 5 2.
d
dx
1
2
3
cos x
3(sin x)
10. }} 1 1 Ïsi
wnwwx 5 }}
2/3 is undefined for x 5 kp,
where k is any integer. f (x) has vertical tangents at these
values of x.
[21, 7] by [22, 4]
(c) Length < 9.294
6. (a) y9 5 cos x 1 x sin x 2 cos x 5 x sin x, so
Section 7.4 Exercises
Length 5
1. (a) y9 5 2x, so
Length 5
E
2
21
Ï1ww
1w(2wx)
w2w dx 5
E
2
21
E Ï1ww1wxwsiwnwwxw dx.
p
2
2
0
(b)
Ï1ww
1w4w
x 2 dx.
(b)
[0, p] by [21, 4]
(c) Length < 4.698
7. (a) y9 5 tan x, so Length 5
[21, 2] by [21, 5]
(c) Length < 6.126
2. (a) y9 5 sec x, so Length 5
2
(b)
E
0
E
p
(c) Length < 2.057
p/6
0
(b) y 5 tan x dx 5 ln ()sec x))
Ï1ww
1wsec
wwxw dx.
4
2p/3
p
32}3}, 04 by [23, 1]
E
30, }6}4 by [20.1, 0.2]
(c) Length < 0.549
Ï1ww
1wtan
w2wxw dx.
Section 7.4
8. (a) x9 5 Ïse
ww
c2wyw
2w1, so Length 5
E
p/4
sec y dy.
2p/3
5
3
2x 2
x
23
(b)
ww
c2wyw
2w1 5 )tan y),
(b) x9 5 Ïse
so x 5
e 2e
E !1§§1§1}
§§§2}
§§§2§ dx.
(e x 2 e2x)
2
10. y9 5 }}, so Length 5
p
3
2}} # y # 0
ln (cos y)
0 , y # }p}
2ln (cos y)
4
[23, 3] by [22, 12]
(c) Length < 20.036
1
2
x 2w
1w
2, so the length is
11. y9 5 }}(x 2 1 2)1/2(2x) 5 xÏw
E Ï1ww1w(w
xÏw
x w
1w2w
) dx 5 E Ïw
x w
1w2w
x w
1w1 dx
1
5 E (x 1 1) dx 5 3}}x 1 x4 5 12.
3
3
0
p p
[22.4, 2.4] by 2}}, }}
3
2
2
4
(c) Length < 2.198
9. (a) y9 5 sec x tan x, so
Length 5
E
p/3
Ï1ww
1wsec
w2wxwta
wnw2wxw dx.
2p/3
2
p p
(c) Length < 3.139
4
2
0
3
2
3
3
0
0
3
2
12. y9 5 }}Ïxw, so the length is
E !1§§1§1}§32}ϧxw§2§ dx 5 E !1§§1§}9§4}x dx
4
4
2
0
0
9x 3/2
4
Ï
w
w
80 10 2 8
5 }}.
27
3 27 1
1
4y
13. x9 5 y 2 2 }}2 , so the length is
5
E !1§y§1§§}41§y}2§ dy 5 3}13}y
3
2
2
0
E !1§§1§1y§§2§}41§y}§2 dy
3
2
2
2
1
1
4y
3
4
53
6
2 }} 5 }}.
3
2
1
4
2 4
8
5 }} 1 1 }}
(b)
32}3}, }3}4 by [21, 3]
3
2
1
1
4y
14. x9 5 y 3 2 }}3 , so the length is
E !1§§1§1y§§2§}41§y}§2 dy 5 E !§1y§1§§}41§y}§2 dy
2
2
2
3
3
1
2
3
3
1
34
1
4
1
8y
5 }}y 4 2 }}2
2
1
123
5 }}.
32
y2
2
1
2y
15. x9 5 }} 2 }}2 , so the length is
E !1§§1§1}§y2}§2§§}21§y}2§ dy 5 E !1§}y§2}§1§}21§y}§2§ dy
2
2
2
2
2
1
2
2
2
1
3
1
6
1
2y
2
4
17
12
5 }}y 3 2 }} 5 }}.
4
(4x 1 4)
1
1
4(x 1 1)
16. y9 5 x 2 1 2x 1 1 2 }}2 5 (x 1 1)2 2 }}2
so the length is
1
E !1§§1§1(x§§1§1)§§2§}
§§1}
§1§) §2 dx
4(x
1
5 E 1(x 1 1) 1 }}2 dx
!§§§§§§§4(x§§1§1§) §
2
2
2
2
0
2
2
2
2
0
33
1
1
4(x 1 1)
4
5 }}(x 1 1)3 2 }}
2
0
53
6
5 }}.
311
312
Section 7.4
17. x9 5 Ïse
ww
c4wyw
2w1, so the length is
E
p/4
Ï1ww
1w(se
ww
c4wyw
2w1)w dy 5
2p/4
E
p/4
24. The area is 300 times the length of the arch.
sec2 y dy
2p/4
3
4
5 tan y
p/4
21
22
Ï1ww
1w(3ww
x 4w
2w
1)w dx 5
E
2p/4
the cost (rounded to the nearest dollar): $38,422.
Ï3wx 2 dx
33 4
1
5 Ï3w }}x 3
21
7Ï3w
5 }}.
22
3
dy 2
dy
1
1
corresponds to }} here, so take }} as }}. Then
dx
dx
4x
2Ïwx
1 2
19. (a) }}
20.2x
y19 5 }}. NINT fails to evaluate
2w
0.2
Ï1w0ww0w
wxw2
E
So y 5 Ïxw.
the limits, so use the track’s symmetry, and “back away”
dx 2
dx
1
1
corresponds to }}4 here, so take }} as }}2 .
dy
dy
y
y
1
Then x 5 2}} 1 C and, since (0, 1) lies on the curve,
y
1
C 5 1. So y 5 }}.
12x
1 2
20. (a) }}
(b) Only one. We know the derivative of the function and
the value of the function at one value of x.
21. y9 5 Ïco
wsw2wxw, so the length is
p/4
Ï1ww
1wcowsw2wxw dx 5
0
25. For track 1: y1 5 0 at x 5 610Ï5w < 622.3607, and
y 5 Ïxw 1 C, and, since (1, 1) lies on the curve, C 5 0.
(b) Only one. We know the derivative of the function and
the value of the function at one value of x.
E
225
to < 73.185. Multiply that by 300, then by $1.75 to obtain
21
22
px
25
5 2.
x 4w
2w1, so the length is
18. y9 5 Ï3ww
E
p
1 2 2 1 50 2
E !1§§1§1}§p2}§22§sin§2§1}§p5}§0x 2§ dx, which evaluates, using NINT,
y9 5 2 }} sin }} , so the length is
E
p/4
0
Ï1ww
1w(w
y19)
w2w dx because of the undefined slope at
210Ï5
w
from the upper limit a little, and find
E
22.36
2
0
Ï1ww
1w(w
y19)
w2w dx < 52.548. Then, pretending the last
little stretch at each end is a straight line, add
2Ï1w0w0ww
2w
0.2
w(2
w2w.3
w6ww
)2 < 0.156 to get the total length of
track 1 as < 52.704. Using a similar strategy, find the
length of the right half of track 2 to be < 32.274. Now
enter Y1 5 52.704 and
Ï2wwcoww
s wx dx
3
10Ï5
w
2
4
5 Ï2w sin x
p/4
5 1.
0
1!1§§1§1}
§Ï§1w5w§0w§w2}
§w§0w.§2wt §2§, t, x, 02 and
2
20.2t
Y2 5 32.274 + NINT
2
graph in a [230, 0] by [0, 60] window to see the effect of
the x-coordinate of the lane-2 starting position on the length
22. y9 5 2(1 2 x 2/3)1/2x21/3, so the length is
E
1
8
intersection at x < 219.909, which leads to starting point
Ï1ww
1w(1ww
2wx 2/
w3w)w
x22/
w3w dx
Ï2
w/4
58
E
1
Ï2
w/4
E
58
coordinates (219.909, 8.410).
22/3
Ïw
x ww dx
1
3
2
3
26. f9(x) 5 }}x22/3 1 }}x21/3, but NINT fails on
1
21/3
x
Ï2
w/4
E Ï1ww1w(wf 9(xw))ww dx because of the undefined slope at
dx
2
5 8 }}x 2/3
2
0
1
3 2 4Ïw
3
of lane 2. (Be patient!) Solve graphically to find the
x 5 0. So, instead solve for x in terms of y using the
2/4
32
3
quadratic formula. (x1/3)2 1 x1/3 2 y 5 0, and
1 24 5 6.
3 1
2 2
5 8 }} 2 }} }}
3p
20
23. Find the length of the curve y 5 sin }}x for 0 # x # 20.
3p
20
3p
20
3p
3p 2
1 1 }} cos }}x dx, which evaluates, using NINT,
20
20
y9 5 }} cos }}x, so the length is
E !§§§1§§§§§§§§2§
20
0
to < 21.07 inches.
21 6 Ïw1w
1w
4wy
x1/3 5 }}. Using the positive values,
2
1
1w4yw 2 1)3. Then,
x 5 }}(Ï1ww
8
3
2
1w4yw 2 1)2 }} , and
x9 5 }}(Ï1ww
8
1w4yw
Ï1ww
E
2
0
1/3
2/3
12
1
2
Ï1ww
1w(x9
ww
)2 dy < 3.6142.
Section 7.5
(4x 2 1 1) 2 (8x 2 2 8x)
(4x 1 1)
31. Because the limit of the sum ΣDxk as the norm of the
4x 2 2 8x 2 1
(4x 1 1)
27. f 9(x) 5 }}}
5 2}}
2
2
2 , so the
partition goes to zero will always be the length (b 2 a) of
4x 2 8x 2 1
E !1§§1§§
dx which evaluates,
1}}
(4x 1 1) 2§
1
length is
2
2
2
21/2
313
2
the interval (a, b).
using NINT, to <2.1089.
32. No; the curve can be indefinitely long. Consider, for
28. There is a corner at x 5 0:
1x2
1
3
1
example, the curve }}sin }} + 0.5 for 0 , x , 1.
33. (a) The fin is the hypotenuse of a right triangle with leg
)
df
Dx 5 f 9(xk21)Dxk.
dx x5xk21 k
lengths Dxk and }}
[22, 2] by [21, 5]
n
ww
xkw
)2w
1w( w
f 9(x
ww
w)D
ww
xkw
)2
Σ Ï(D
k21
n→` k51
Break the function into two smooth segments:
y5
h
x 3 2 5x
x 3 1 5x
y9 5
h
3x 2 5
3x 2 1 5
5
E
1w( w
f 9(x
ww
w)w
)2
Σ DxkÏ1ww
k21
n→` k51
5 lim
5
22 # x , 0
.
0,x#1
E
1
0
n
22 # x # 0
and
0,x#1
2
The length is
(b) lim
Ï1ww
1w(3ww
x 2w
2w5w
)2 dx 1
22
b
2
a
34. Yes. Any curve of the form y 5 6x 1 c, where c is a
constant, has constant slope 61, so that
Ï1ww
1w(y9
ww
)2 dy
22
E Ï1ww1w( wf 9(xw))ww dx
E Ï1ww1w(y9ww) dx 5 E Ï2w dx 5 aÏ2w.
E Ï1ww1w(3wwx w1w5w) dx,
1
2
a
2
a
2
0
0
0
which evaluates, using NINT for each part, to < 13.132.
■ Section 7.5 Applications from Science
and Statistics
29. y 5 (1 2 Ïxw)2, 0 # x # 1
(pp. 401–411)
Quick Review 7.5
Ee
1
1. (a)
[20.5, 2.5] by [20.5, 1.5]
y9 5 }}, but NINT may fail using y9 over the entire
Ïxw
interval because y9 is undefined at x 5 0. So, split the curve
E
!§§§1§§§§§2
Ï xw 2 1
1 1 }}
1/4
Ïxw
which evaluates, using NINT, to < 1.623.
1
Ee
1
2. (a)
dx,
0
1
3 4
0
0
(b) < 1.718
3. (a)
E
p/4
3
4
sin x dx 5 2cos x
(b) < 0.707
E (x
3
30.
1
e
dx 5 e x 5 e 2 1
x
p/2
2
1
(b) < 0.632
into two equal segments by solving Ïxw 1 Ïyw 5 1 with
y 5 x: x 5 }}. The total length is 2
4
dx 5 2e2x 5 1 2 }}
0
Ïxw 2 1
1
4
3
2x
4. (a)
33
p/2
Ï2w
5 }}
2
p/4
4
1
3
1 2) dx 5 }}x 3 1 2x 5 15
2
0
0
(b) 15
x
1
E}
} dx 5 3}} ln (x
3
x 11
2
5. (a)
1
[0, 16] by [0, 2]
2
3
1
5 }}[ln
3
1
5 }}ln
3
1
4
y9 5 }}x23/4, but NINT may fail using y9 over the entire
x 5 y 4, 0 # y # 2: x9 5 4y 3 and the length is
(b) < 0.501
E 2p(x 1 2) sin x dx
7
E Ï1ww1w(4wwy w) dy, which evaluates,
6.
using NINT, to < 16.647.
7.
2
0
3 2
0
E (1 2 x )(2px) dx
7
0
2
1 1)
9
2
4
9 2 ln 2]
1}2}2
interval, because y9 is undefined at x 5 0. So, use
3
1
314
Section 7.5
E p cos
7
8.
2
1 16 2
1
1
s 5 }}, F 5 24001}}2 5 300 lb.
8
8
x dx
1
10. (a) F 5 ks, so 150 5 k }} and k 5 2400 lb/in. Then for
0
E p1}2y}2 (10 2 y) dy
7
9.
2
0
E }Ï4}3w sin
7
10.
2
E
1/8
x dx
(b)
0
0
3
4
2400x dx 5 1200x 2
1/8
5 18.75 in.-lb
0
Section 7.5 Exercises
E xe
5
1.
3
2x/3
dx 5 23e 2x/3(3 1 x)
0
E
3
5
4
11. When the end of the rope is x m from its starting point, the
24
e
5 2}5}
/3 1 9 < 4.4670 J
0
1 2
3
1 2
1 24
F(x) 5 (0.624)(50 2 x) N. The total work is
0
E
4Ï2w 2
3
5 }} }} 1 }}
1p
p
50
22
0
< 3.8473 J
E
3
3
4
1
3. xÏ9ww
2wx 2w dx 5 2}}(9 2 x 2)3/2
3
0
E
10
4.
0
(50 2 x) m of rope still to go weigh
3
px
px
px
4 4
2. x sin }} dx 5 }} }} sin }} 2 x cos }}
4
4
4
p p
0
3
12. (a) Work 5
59J
0
3
3
4
(esin x cos x 1 2) dx 5 esin x 1 2x
E
(p , V )
2 2
(p , V )
1 1
Work 5
0
Then
W5
E
0
3
(490 2 24.5x) dx 5 490x 2 12.25x 2
20
1
2
1
pA dx 5
E
(p , V )
2 2
E
(p , V )
2 2 109,350
}1}
V .4
(p , V )
1 1
4
dV
4
V 5 32
V 5 243
5 4900 J.
horizontal rectangle has area 2Ï9ww
2wy 2w Dy, where y is
distance from the top, and pressure 62.4y. The total
2
F(x) 5 490 }} 5 490 1 2 }} 5 490 2 19.6x N.
2
force is approximately ∑ (62.4yk)(2Ï9ww
2wyw
) Dy
k
Then
2
5 ∑ 124.8ykÏ9ww
2wyw
Dy.
k
W5
n
20
0
3
(490 2 19.6x) dx 5 490x 2 9.8x 2
20
4
5 5880 J.
k51
(b)
W5
E
2
1
18
0
3
4
5 1944 ft-lb
2
0
force is approximately
n
1600
200
9. (a) F 5 ks, so 21,714 5 k(8 2 5) and k 5 7238 lb/in.
5 904.75 < 905 in.-lb, and W 5
3
5 3619x 2
1
4
1/2
3
7238x dx 5 3619x 2
E
1/2
4
0
1
7238x dx
1/2
5 2714.25 < 2714 in.-lb.
!§§§§2
Σ (62.4yk)16
k51
(c) F 5 200s, so s 5 }} 5 8 in.
0
y2
2
0
E
!§§§6§4
distance from the top, and pressure 62.4y. The total
E 200x dx 5 3100x 4 5 400 in.-lb.
(b) F(x) 5 7238x. W 5
y2
8
horizontal rectangle has area 6 1 2 }} Dy, where y is
0
1/2
0
x2
3
8. (a) F 5 ks, so 800 5 k(14 2 10) and k 5 200 lb/in.
(b) F(x) 5 200x, and
3
14. (a) From the equation }}2 1 }}2 5 1, it follows that a thin
18
2
2 3/2
0
2
(144 2 4x) dx 5 144x 2 2x 2
2
5 1123.2 lb
18 2 x/2
x
F(x) 5 144 }} 5 144 1 2 }} 5 144 2 4x lb.
18
36
1
E 124.8yÏ9ww2wyw dy 5 3241.6(9 2 y ) 4
3
0
7. When the bag is x ft off the ground, the sand weighs
Then
k51
n
E
p dV
(p , V )
1 1
13. (a) From the equation x 2 1 y 2 5 32, it follows that a thin
0
x
25
(p , V )
1 1
5 780 J.
0
5 237,968.75 in.-lb
6. When the bucket is x m off the ground, the water weighs
20 2 4x/5
20
(p , V )
2 2
3
2
20
E
5 109,350 22.5V 20.4
20 2 x
x
F(x) 5 490 }} 5 490 1 2 }} 5 490 2 24.5x N.
20
20
1
F(x) dx 5
50
109,350
V
5. When the bucket is x m off the ground, the water weighs
2
4
and
(b) p1V11.4 5 (50)(243)1.4 5 109,350, so p 5 }1}
.4
10
5 esin 10 1 19 < 19.5804 J
1
1
2
(0.624)(50 2 x) dx 5 0.624 50x 2 }}x 2
2
n
64
k51
!§§§§
y
64
2 3/2 8
2
0
5 7987.2 lb
2
1 2 }k} Dy.
E 374.4y!1§§2§}6y}§4 dy 5 327987.211 2 }6y}4 2 4
8
(b)
y
1 2 }k} Dy 5 Σ 374.4yk
0
Section 7.5
3
8
15. (a) From the equation x 5 }}y, it follows that a thin
3
4
horizontal rectangle has area }}yDy, where y is the
distance from the top of the triangle, the pressure is
62.4(y 2 3). The total force is approximately
n
∑
k51
∑
1 2
E 46.8(y
8
(b)
n
3
62.4(yk 2 3) }}yk Dy 5
46.8(yk2 2 3yk) Dy.
4
k51
3
2
2
3
2 3y) dy 5 15.6y 3 2 70.2y 2
4
E
30
0
30
32 4
1
100p(51.2)y dy 5 5120p }}y 2
< 7,238,229 ft-lb
0
19. Work to pump through the valve is p(2)2(62.4)(y 1 15)Dy
for a thin disk and
0
2
1 15y
6
4
0
< 84,687.3 ft-lb
x2
2
16. (a) From the equation y 5 }}, it follows that a thin
horizontal rectangle has area 2Ï2wywDy, where y is
distance from the bottom, and pressure 62.4(4 2 y).
The total force is approximately
for the whole tank. Work to pump over the rim is
p(2)2(62.4)(6 1 15)Dy for a thin disk and
E 4p(62.4)(21) dy 5 4p(62.4)(21)(6) < 98,801.8 ft-lb for
6
0
n
yk)Dy
Σ 62.4(4 2 yk)(2Ï2ww
k51
where y is height up from the bottom. The total work is
6
3
5 3494.4 2 (2210.6) 2 3705 lb
18. The work needed to raise a thin disk is p(10)2(51.2)yDy,
E 4p(62.4)(y 1 15) dy 5 249.6p3}12}y
8
315
the whole tank. Through a hose attached to a valve in the
n
5 Σ 124.8Ï2w(4Ïw
yk 2 yk3/2)Dy.
bottom is faster, because it takes more time for a pump with
k51
E 124.8Ï2w(4Ïyw 2 y
4
(b)
3/2
a given power output to do more work.
) dy
0
33
8
2
5
4
5 124.8Ï2w }}y3/2 2 }}y5/2
4
20. The work is the same as if the straw were initially an inch
0
long and just touched the surface, and lengthened as the
5 1064.96Ï2w < 1506.1 lb
17. (a) Work to raise a thin slice 5 62.4(10 3 12)(Dy)y.
E
20
Total work 5
3
62.4(120)y dy 5 62.4 60y 2
0
5 1,497,600 ft-lb
20
4
0
(b) (1,497,600 ft-lb) 4 (250 ft-lb/sec) 5 5990.4 sec
< 100 min
(c) Work to empty half the tank 5
3
5 62.4 60y 2
10
4
E
10
liquid level dropped. For a thin disk, the volume is
y 1 17.5 2
1 14 2
y 1 17.5 2 4
p1 }}2 1}}2(8 2 y)Dy. The total work is
14
9
y 1 17.5 2 4
E p1 }14}2 1}9}2(8 2 y) dy, which using NINT evaluates
p }} Dy and the work to raise it is
7
0
to < 91.3244 in.-oz.
62.4(120)y dy
0
5 374,400 ft-lb, and
21. The work is that already calculated (to pump the oil to the
0
374,400 4 250 5 1497.6 sec < 25 min
rim) plus the work needed to raise the entire amount 3 ft
higher. The latter comes to
(d) The weight per ft3 of water is a simple multiplicative
factor in the answers. So divide by 62.4 and multiply
1}3}pr h2(57)(3) 5 57p(4) (8) 5 22,921.06 ft-lb, and the
1
2
2
total is 22,921.06 1 30,561.41 < 53,482.5 ft-lb.
by the appropriate weight-density
22. The weight density is a simple multiplicative factor: Divide
For 62.26:
1 62.4 2
62.26
5990.41}}2 5 5976.96 sec < 100 min.
62.4
62.26
1,497,600 }} 5 1,494,240 ft-lb and
For 62.5:
1 62.4 2
62.5
5990.41}}2 5 6000 sec 5 100 min.
62.4
62.5
1,497,600 }} 5 1,500,000 ft-lb and
by 57 and multiply by 64.5.
1 57 2
64.5
30,561.41 }} < 34,582.65 ft-lb.
316
Section 7.5
(d) 0 if we assume a continuous distribution. Between
23. The work to raise a thin disk is
pr 2(56)h 5 p(Ï1w0w2w2
wwy 2w)2(56)(10 1 2 2 y)Dy
59.5 in. and 60.5 in., the proportion is
E
60.5
5 56p(12 2 y)(100 2 y 2)Dy. The total work is
E
59.5
10
0
56p(12 2 y)(100 2 y 2) dy, which evaluates using NINT
to <967,611 ft-lb. This will come to
f (x) dx < 0.071 (7.1%)
28. Use f (x) 5 }}e2(x2498) /(2 ? 100 )
100Ï2wp
w
1
E
500
(967,611)($0.005) < $4838, so yes, there’s enough money
(a)
400
to hire the firm.
2
2
f (x) dx < 0.34 (34%)
(b) Take 1000 as a conveniently high upper limit:
E
1000
1
24. Pipe radius 5 }} ft;
6
700
E p1}16}2 (62.4)y dy 5 112,320p ft-lb.
Work to fill tank 5 E p(10) (62.4)y dy
Work to fill pipe 5
360
0.217(300) < 6.5 people
2
0
385
2
360
5 58,110,000p ft-lb.
f (x) dx < 0.217, which means about
29. Integration is a good approximation to the area (which
represents the probability), since the area is a kind of
Riemann sum.
30. The proportion of lightbulbs that last between 100 and 800
hours.
Total work 5 58,222,320p ft-lb, which will take
58,222,320p 4 1650 < 110,855 sec < 31 hr.
25. (a) The pressure at depth y is 62.4y, and the area of a thin
E
35,780,000
31.
6,370,000
35,780,000
3 4
1000MG
1
dr 5 1000 MG 2}}
}}
r2
r
, which for
6,370,000
M 5 5.975 3 1024, G 5 6.6726 3 10211 evaluates to
< 5.1446 3 1010 J.
11
horizontal strip is 2Dy. The depth of water is }} ft, so
6
32. (a) The distance goes from 2 m to 1 m. The work by an
the total force on an end is
E
11/6
0
(62.4y)(2 dy) < 209.73 lb.
external force equals the work done by repulsion in
moving the electrons from a 1-m distance to a 2-m
(b) On the sides, which are twice as long as the ends, the
initial total force is doubled to <419.47 lb. When the
11
3
tank is upended, the depth is doubled to }} ft, and the
E
11/3
force on a side becomes
(62.4y)(2 dy) < 838.93 lb,
0
which means that the fluid force doubles.
5
16
31
48
26. 3.75 in. 5 }} ft, and 7.75 in. 5 }} ft.
E
Force on a side 5 p dA 5
E
31/48
1 16 2
5
(64.5y) }} dy < 4.2 lb.
0
27. (a) 0.5 (50%), since half of a normal distribution lies
below the mean.
E
65
(b) Use NINT to find
f (x) dx, where
63
2
2
1
f (x) 5 }}e 2(x263.4) /(2 ? 3.2 ). The result is
3.2Ïw2w
p
<0.24 (24%).
(c) 6 ft 5 72 in. Pick 82 in. as a conveniently high upper
E
82
limit and with NINT, find
72
<0.0036 (0.36%).
f (x) dx. The result is
distance:
23 3 10
E}
} dr
r
1
5 23 3 10
32}r}4
Work 5
229
2
1
2
2
229
1
5 1.15 3 10228 J
(b) Again, find the work done by the fixed electrons in
pushing the third one away. The total work is the sum
of the work by each fixed electron. The changes in
distance are 4 m to 6 m and 2 m to 4 m, respectively.
Work 5
23 3 10
23 3 10
E}
} dr 1 E }} dr
r
r
229
6
4
229
4
2
6
2
2
4
13 4 3 r 4 2
1
r
5 23 3 10229 2}}
4
< 7.6667 3 10229 J.
1
1 2}}
2
Chapter 7 Review
1 dt 2
■ Chapter 7 Review Exercises
1 dx 2
dv
dv
33. F 5 m }} 5 mv }} , so
(pp. 413–415)
E F(x) dx
dv
5 E mv1}}2 dx
dx
5 E mv dv
W5
317
x
2
E v(t) dt 5 E (t 2 0.2t ) dt
1
5 }}t 2 0.05t
33
4 < 10.417 ft
2. E c(t) dt 5 E (4 1 0.001t ) dt
5 4t 1 0.0002t
3
4 < 31.361 gal
3. E B(x) dx 5 E (21 2 e
) dx
< 21x 2 33.333e
3
4 < 1464
5
x
1
x
2
5
2
1.
0
3
0
3
x
1
v
2
5
4
0
7
v
1
7
0
1
1
5 }}mv22 2 }}mv12
2
2
4
0
7
5
0
1
2
34. Work 5 Change in kinetic energy 5 }}mv2.
2 oz
1/8 lb
1
m 5 }}2 5 }}2 5 }} slug, so
32 ft/sec
32 ft/sec
256
1 1
Work 5 }} }} (160)2 5 50 ft-lb.
2 256
1 2
0.3125 lb
32 ft/sec
5280 ft
1 hr
90 mph 5 90 }} }} 5 132 ft/sec, so
1 mi
3600 sec
1
Work 5 change in kinetic energy 5 }}(0.009765625)(132)2
2
35. 0.3125 lb 5 }}2 5 0.009765625 slug, and
1
21
100
0
0.03x
0
0.03x
100
0
E r(x) dx 5 E (11 2 4x) dx 5 311x 2 2x 4 5 14 g
2
4.
2
0
2
E
24
5.
2
0
0
E
24
2
0
1 12 22 dt
12
pt
5 30032t 2 }} sin 1}}24 5 14,400
p
12
E(t) dt 5
< 85.1 ft-lb.
0
1
pt
300 2 2 cos }}
24
0
1 16 oz 2
1 lb
36. 1.6 oz 5 1.6 oz }} /(32 ft/sec2) 5 0.003125 slug, so
1
2
100
6.
Work 5 }}(0.003125)(280)2 5 122.5 ft-lb.
1 16 oz 2
1 lb
1
256
5280 ft
1 hr
124 mph 5 124 mph }} }} 5 181.867 ft/sec,
1 mi
3600 sec
1 1
so Work 5 }} }} (181.867)2 < 64.6 ft-lb.
2 256
37. 2 oz 5 2 oz }} /(32 ft/sec2) 5 }} slug, and
1 2
1
21
[21, 3] by [21, 2]
2
The curves intersect at x 5 1. The area is
E x dx 1 E }x1} dx 5 3}12}x 4 1 32}1x}4
1
1
2
1 lb
38. 14.5 oz 5 14.5 oz }} /(32 ft/sec2) < 0.02832 slug, so
16 oz
1
Work 5 }}(0.02832)(88)2 < 109.7 ft-lb.
2
1
2
1 lb
39. 6.5 oz 5 6.5 oz }} /(32 ft/sec2) < 0.01270 slug, so
16 oz
1
Work 5 }}(0.01270)(132)2 < 110.6 ft-lb.
2
1
8
1
256
1
1
1 2
5 }}ks 2 5 }}(18) }} 5 0.5625 ft-lb, and final height is
2
2
4
0.5625
given by mgh 5 0.5625 ft-lb, so h 5 }} 5 4.5 ft.
(1/256)(32)
0
1
2
1
2
0
1
2
1
2
1
1
5 }} 1 2}} 1 1 5 1.
2
2
7.
40. 2 oz 5 }} lb 5 }} slug. Compression energy of spring
12
2
[24, 4] by [24, 4]
The curves intersect at x 5 22 and x 5 1. The area is
E
1
22
[3 2 x 2 2 (x 1 1)] dx 5
E
1
(2x 2 2 x 1 2) dx
22
3
1
3
1
1
3
1
2
5 2}}x 3 2 }}x 2 1 2x
1
2
1
4
22
2 13
8
5 2}} 2 }} 1 2 2 }} 2 2 2 4
9
2
5 }}.
2
318
Chapter 7 Review
8. Ïxw 1 Ïyw 5 1 implies y 5 (1 2 Ïxw)2 5 1 2 2Ïxw 1 x.
12.
p 3p
32}2}, }2}4 by [23, 3]
[20.5, 2] by [20.5, 1]
E (1 2 2Ïxw 1 x) dx 5 3x 2 }43}x
1
The area is
1
2
4
1 }}x 2
3/2
0
1
6
E (2 sin x 2 sin 2x) dx 5 322 cos x 1 }12} cos 2x4
p
p
0
5 }}.
9. x 5 2y 2 implies y 5
The area is
1
0
5 4.
0
13.
!§
x
}}.
2
[25, 5] by [25, 5]
The curves intersect at x < 62.1281. The area is
[21, 19] by [21, 4]
E
2.1281
The curves intersect at x 5 18. The area is
E 13 2 !}§2x}2 dx 5 33x 2 }3}1}2}2 4
2
or E 2y dy 5 3}}y 4 5 18.
3
18
4 x 3/2
18
0
3
2
3
0
(4 2 x 2 2 cos x) dx,
22.1281
which using NINT evaluates to < 8.9023.
5 18,
14.
0
3
0
1
4
10. 4x 5 y 2 2 4 implies x 5 }}y 2 2 1, and 4x 5 y 1 16 implies
[24, 4] by [24, 4]
1
4
x 5 }}y 1 4.
The curves intersect at x < 60.8256. The area is
E
0.8256
(3 2 )x) 2 sec2 x) dx,
20.8256
which using NINT evaluates to < 2.1043.
[26, 6] by [26, 6]
15. Solve 1 1 cos x 5 2 2 cos x for the x-values at the two
The curves intersect at (3, 24) and (5.25, 5). The area is
p
3
E 31}14}y 1 42 2 1}14}y 2 124 dy
1
1
5 E 2}}y 1 }}y 1 5 dy
1 4 4 2
5
2
symmetry of the area:
24
5
E
7p/3
2
2
2p
3
425
24
1 2
38
3
[(1 1 cos x) 2 (2 2 cos x)] dx
E (2 cos x 2 1) dx
7p/3
5 2 2 sin x 2 x
3
42p
24
1
1
5 2}}y 3 1 }}y 2 1 5y
8
12
52
5
4
24
7p/3
2p
2
3
5 2Ï3w 2 }}p < 1.370.
243
8
5 }} 2 2}} 5 }} 5 30.375.
E
5p/3
11.
16.
p/3
[(2 2 cos x) 2 (1 1 cos x)] dx
E (1 2 2 cos x) dx
5p/3
5 x 2 2 sin x
3
4p/3
5
E
p/4
The area is
0
5p/3
p/3
4
3
5 2Ï3w 1 }}p < 7.653
[20.1, 1] by [20.1, 1]
32
1
4
(x 2 sin x) dx5 }}x 2 1 cos x
p/4
0
Ïw2
p2
5 }} 1 }} 2 1
32
2
< 0.0155.
5p
3
7p
3
ends of the region: x 5 2p 6 }}, i.e., }} or }}. Use the
Chapter 7 Review
x
x 11
17. Solve x 3 2 x 5 }
2 } to find the intersection points at
(c) Use cylindrical shells. A shell has radius 4 2 x and
height 2Ïxw 2 x. The total volume is
x 5 0 and x 5 621/4. Then use the area’s symmetry:
E 2p(4 2 x)(2Ïxw 2 x) dx
5 2pE (8Ïxw 2 4x 2 2x
16
4
5 2p }}x 2 2x 2 }}x
33
5
4
0
the area is
x
E 3}
} 2 (x 2 x) dx
4
x 11
1
1
1
5 23}} ln (x 1 1) 2 }}x 1 }}x 4
2
4
2
2
1/4
2
4
2
21/4
0
4
2
0
4
3
2
0
2
2
x2 2 3
312x 2 }} dx,
10
2
3
4
4
0
which using NINT evaluates to < 5.7312.
22. (a) Use disks. The volume is
E
p
19. Use the x- and y-axis symmetries of the area:
E x sin x dx 5 43sin x 2 x cos x4
p
4
64p
5
5 }}.
E 2p(4 2 y)1y 2 }y4}2 dy
y
5 2pE 4y 2 2y 1 }} dy
1
42
2
32p
1
5 2p 2y 2 }}y 1 }}y 5 }}.
3 3 16 4 3
The area is
1
4
y2
4
determine that the curves intersect at x < 61.8933.
21.8933
4
1
3
1 }}x 3
5/2
height y 2 }}. The total volume is
18. Use the intersect function on a graphing calculator to
E
2
(d) Use cylindrical shells. A shell has radius 4 2 y and
0
5 ln (Ï2w 1 1) 1 Ï2w 2 1 < 1.2956.
1.8933
1 x 2) dx
3/2
3/2
2
0
4
0
3
2
319
p
0
5 4p.
2
0
E
(b) p
0
20. A cross section has radius r 5 3x and area
k
0
E
(Ï2wyw)2 dy 5 p
4
2
0
4
2
2y dy 5 py 2 5 4p.
0
k
2y dy 5 py 2 5 pk 2
0
4
2 dV
dk
dt
dk
1 dV
1
1
When k 5 1, }} 5 }} }} 5 }} (2) 5 }},
dt
2pk dt
2p
p
1
so the depth is increasing at the rate of }} unit per
p
(c) Since V 5 pk , }} 5 2pk}}.
dt
A(x) 5 pr 5 9px .
2
V5
E
1
21
8
3 4
9px 8 dx 5 p x 9
1
5 2p.
21
21.
1 2
second.
23. The football is a solid of revolution about the x-axis. A
[25, 5] by [25, 5]
cross section has radius
The graphs intersect at (0, 0) and (4, 4).
!1§2§§11§2§}1§2}1§2 and area
4x 2
1 121 2
4x
4x
2E 12p 1 2 }} dx 5 24pE
1 121 2
11 2 }12}1 2 dx
1
2
5 24p x 2 }} }} x
3 1 11 2 1 3 2 4
11
11
5 24p3}} 2 }}4
2
6
4x 2
pr 2 5 12p 1 2 }} . The volume is, given the symmetry,
(a) Use cylindrical shells. A shell has radius y and height
2
y
4
y 2 }}. The total volume is
0
2
11/2
2
2
0
2
E 2p(y)1 y 2 }y4}2 dy 5 2pE 1 y 2 }y4}2 dy
1
1
5 2p }}y 2 }}y
3 3 16 4
4
11/2
0
4
3
2
0
3
4
4
11/2
0
5 88p < 276 in3.
0
32p
5 }}.
3
3
24. The width of a cross section is 2 sin x, and the area is
(b) Use cylindrical shells. A shell has radius x and height
E
2Ïxw 2 x. The total volume is
E 2p(x)(2Ïxw 2 x) dx 5 2pE (2x
4
0
4
0
35
4
3/2
2 x 2) dx
1
3
5 2p }}x 5/2 2 }}x 3
128p
15
5 }}.
1
1
}}pr 2 5 }}p sin2 x. The volume is
2p
2
1
p 1
1
}}p sin2 x dx 5 }} }}x 2 }}sin 2x
2 2
4
0 2
4
4
0
3
p
4
0
p2
4
5 }}.
320
Chapter 7 Review
29.
25.
[21, 2] by [21, 2]
[21, 3] by [23, 3]
Use washer cross sections. A washer has inner radius r 5 1,
y9 5 3x 2 2 6x equals zero when x 5 0 or 2. The maximum
outer radius R 5 e x/2, and area p(R2 2 r 2) 5 p(e x 2 1).
is at x 5 0, the minimum at x = 2. The distance between
The volume is
them along the curve is
E Ï1ww1w(3wwx w2w6x)ww dx, which
2
E
ln 3
3
4
p(e x 2 1) dx 5 p e x 2 x
0
4.5920
}} 5 2.296 sec.
2
5 p(3 2 ln 3 2 1)
5 p(2 2 ln 3).
26. Use cylindrical shells. Taking the hole to be vertical, a shell
has radius x and height 2Ï2w2w2
wwx 2w. The volume of the
E
Ï3
w
0
2p(x)(2Ï2w2w2
wwx 2w) dx 5 2p
E
2xÏ4ww
2wx 2w dx
0
3
2
3
4
Ï3w
0
27. The curve crosses the x-axis at x 5 63. y9 5 22x, so the
E
3
Ï1ww
1w(2
w2wx)
w2w dx 5
23
E
3
31. F9(x) 5 Ïw
x 4w
2w
1, so
E Ï1ww1w(Fw9(wx)ww) dx 5 E Ïwx dx
5 E x dx
1
5 }}x 5 39.
33 4
2
2
5
2
5
4
2
2
4
3
28p
5 }} < 29.3215 ft3.
3
5 2}}p(1 2 8)
30. If (b) were true, then the curve y 5 k sin x would have to
get vanishingly short as k approached zero. Since in fact the
curve’s length approaches 2p instead, (b) is false and (a) is
true.
5
Ï3
w
5 2p 2}}(4 2 x2)3/2
length is
2
using NINT evaluates to < 4.5920. The time taken is about
0
piece cut out is
2
0
ln 3
3
5
2
32. (a) (100 N)(40 m) = 4000 J
(b) When the end has traveled a distance y, the weight of
the remaining portion is (40 2 y)(0.8) 5 32 2 0.8y.
Ï1ww
1w4w
x 2 dx, which
23
The total work to lift the rope is
using NINT evaluates to < 19.4942.
E
40
28.
0
3
(32 2 0.8y) dy 5 32y 2 0.4y 2
40
4
5 640 J.
0
(c) 4000 1 640 5 4640 J
[22, 2] by [22, 2]
The curves intersect at x 5 0 and x 5 61. Use the graphs’
33. The weight of the water at elevation x (starting from x 5 0)
1 4750 2 95 1
2 2
128
1
128
1
is E }}14750 2 }}x2 dx 5 }}34750x 2 }}x 4
95
2
95
4
4750 2 x/2
128
1
is (800)(8) }} 5 }} 4750 2 }}x . The total work
4750
x- and y-axis symmetry:
2
0
0
d
}}(x 3 2 x) 5 3x 2 2 1, and the total perimeter is
dx
E
4750
5 22,800,000 ft-lb.
1
4 Ï1ww
1w(3ww
x 2w
2w
1w
)2 dx, which using NINT evaluates to
0
< 5.2454.
F
800
80
s
3
0.3
800
800 2
}}x dx 5 }}x
3
6
34. F 5 ks, so k 5 }} 5 }} 5 }} N/m. Then
Work 5
E
0.3
0
3
4
0.3
4
1.3
5 12 J.
0
To stretch the additional meter,
Work 5
E
1.3
0.3
3
800
800
}}x dx 5 }}x 2
3
6
< 213.3 J.
0.3
35. The work is positive going uphill, since the force pushes in
the direction of travel. The work is negative going downhill.
321
Chapter 7 Review
36. The radius of a horizontal cross section is Ï8w2w2
wwy 2w, where
y is distance below the rim. The area is p(64 2 y 2), the
1
42. Use f (x) 5 }}e2x /2.
Ï2wp
w
1
(a)
weight is 0.04p(64 2 y 2) Dy, and the work to lift it over
E
(c) E
2
the rim is 0.04p(64 2 y )( y) Dy. The total work is
(b)
E 0.04py(64 2 y ) dy 5 0.04pE (64y 2 y ) dy
1
5 0.04p 32y 2 }}y
3
4 4
8
2
2
3
2
2
4
21
f (x) dx evaluates, using NINT, to
< 0.6827 (68.27%).
2
8
E
2
22
3
8
23
f (x) dx < 0.9545 (95.45%)
f (x) dx < 0.9973 (99.73%)
43. Because f (x) $ 0 and
2
5 36p < 113.097 in.-lb.
E
`
2`
f (x) dx 5 1
44.
37. The width of a thin horizontal strip is 2(2y) 5 4y, and the
force against it is 80(2 2 y)4y Dy. The total force is
E 320y(2 2 y) dy 5 320E (2y
2
2
0
0
3
2
1 2y) dy
4
1
3
5 320 2}}y 3 1 y 2
3
2
x
2
A shell has radius x and height 2x 2 }} 5 }}x. The total
E 2p(x)1}32}x2 dx 5 p3x 4
2
1
volume is
3
0
0
1280
3
5 }} < 426.67 lb.
23
48
[21, 3] by [21, 3]
1
5 p.
0
45.
5
6
7
24
38. 5.75 in. 5 }} ft, 3.5 in. 5 }} ft, and 10 in. 5 }} ft.
For the base,
1 48
23
7
24
5
6
[23, 3] by [23, 3]
2
Force 5 57 }} 3 }} 3 }} < 6.6385 lb.
Force 5
E 1 2
5/6
0
E
2
5/6
3 4
399 1
7
57 }} y dy 5 }} }}y 2
24 2
24
< 5.7726 lb.
0
E 571}243}8 2y dy 5 }1341}81 3}12}y 4
5/6
2
0
1/2
5/6
1
E
2
1/2
2
3 4
2p dx 5 2px
5 3p.
1/2
< 9.4835 lb.
0
39. A square’s height is y 5 (Ï6w 2 Ïxw)2, and its area is
y 2 5 (Ï6w 2 Ïxw)4. The volume is
1x2
2p(x) }} dx 5
46.
For the sides,
Force 5
1
x
A shell has radius x and height }}. The total volume is
For the front and back,
E (Ï6w 2 Ïxw)
6
4
p 3p
32}2}, }2}4 by [22, 2]
dx,
0
A shell has radius x and height sin x. The total volume is
which using NINT evaluates to exactly 14.4.
40. Choose 50 cm as a conveniently large upper limit.
E
2
2
1
}} e2(x217.2) /(2?3.4 ) dx, evaluates,
20 3.4Ïw
2p
w
50
E 2p(x)(sin x) dx 5 2p3sin x 2 x cos x4
p
0
p
5 2p 2.
0
47.
using NINT to < 0.2051 (20.5%).
41. Answers will vary. Find m, then use the fact that 68% of the
[21, 4] by [24, 1]
class is within s of m to find s, and then choose a
The curves intersect at x 5 1 and x 5 3. A shell has radius
conveniently large number b and calculate
x and height x 2 3 2 (x 2 2 3x) 5 2x 2 1 4x 2 3. The total
E
b
10
2
2
1
}}e2(x2m) /(2s ) dx.
sÏ2wp
w
volume is
E 2p(x)(2x
3
1
2
E
3
1 4x 2 3) dx 5 2p (2x 3 1 4x 2 2 3x) dx
1
3
1
4
4
3
3
2
4
5 2p 2}}x 4 1 }}x 3 2 }}x 2
16p
5 }}.
3
3
1
322
Section 8.1
48. Use the intersect function on a graphing calculator to
x cos x 2 sin x
x
. The graphs of y and y clearly show
3. y5 5 }}
2
3
5
determine that the curves intersect at x 5 61.8933. A shell
x2 2 3
10
2
has radius x and height 312x 2 }}. The volume, which
1.8933
1
2
x2 2 3
10
x→0 y2
y
lim }}1 9.
1 2
x→0 y2
is calculated using the right half of the area, is
E
y
that l’Hôpital’s Rule does not say that lim }}1 is equal to
2
2p(x) 312x 2 }} dx, which using NINT
0
evaluates to < 9.7717.
5
4
5
4
49. (a) y 5 2}}(x 1 2)(x 2 2) 5 5 2 }}x 2
[23, 3] by [22, 2]
Quick Review 8.1
(b) Revolve about the line x 5 4, using cylindrical shells.
1.
5
4
A shell has radius 4 2 x and height 5 2 }}x 2. The total
volume is
E
2
22
1
5
4
2
2p(4 2 x) 5 2 }}x 2 dx
E1
3
2
2
1
5 10p
}}x 3 2 x 2 2 x 1 4 dx
22 4
2
1
1
1
5 10p }}x 4 2 }}x 3 2 }}x 2 1 4x
3
2
16
22
320
5 }}p < 335.1032 in3.
3
dL
dx
4
2.
2
x
1 1 ( f 9(x))2 5 }}2 1 }} f 9(x) 1 ( f 9(x))2, and
1
1
1
1
f 9(x) 5 }}x 2 }}. Then f (x) 5 }}x 2 2 }} ln x 1 C, and the
2
4
2
2x
3
requirement to pass through (1, 1) means that C 5 }}. The
4
1
1
3
x 2 2 2 ln x 1 3
function is f (x) 5 }}x 2 2 }} ln x 1 }} 5 }}.
4
2
4
4
51. y9 5 sec x, so the area is
E
p/4
0
2p(tan x)Ï1ww
1w(se
ww
c wxw
) dx,
2
1.1052
10,000
1.1052
1,000,000
1.1052
0.1 x
approaches 1.1052.
x
2
x
x1/(ln x)
0.1
2.7183
0.01
2.7183
0.001
2.7183
0.0001
2.7183
1 x
11 2 }x}2
x
Chapter 8
L’Hôpital’s Rule, Improper Integrals,
and Partial Fractions
■ Section 8.1 L’Hôpital’s Rule (pp. 417–425)
Exploration 1 Exploring L’Hôpital’s Rule
Graphically
cos x
1
1. lim }} 5 lim }} 5 1
y9
2. The two graphs suggest that lim }}1 5 lim }1}.
x→0 y2
1.1051
3.
which using NINT evaluates to < 5.02.
y
100
1000
As x→01, x1/(ln x) approaches 2.7183.
E 1 2!§§§1§§§2§
x→0
1.1046
2
1
1
52. x 5 }} and x9 5 2}}2 , so the area is
y
y
2
1
1 2
2p }} 1 1 2}}2 dy,
y
y
1
sin x
x
1.1000
0.00001 2.7183
which using NINT evaluates to < 3.84.
x→0
1
10
1
1
x
2
11 1 }x}2
As x→`, 1 1 }}
50. Since }} 5 }} 1 f 9(x) must equal Ï1ww
1w( w
f 9(x
w))
w2w,
1
x
0.1 x
x
x→0 y29
21
0.5
20.1
0.78679
20.01
0.95490
20.001
0.99312
20.0001
0.99908
20.00001
0.99988
20.000001 0.99999
1 x
approaches 1.
x
1
As x→02, 1 2 }}
4.
2
1 x
x
11 1 }x}2
21.1
13.981
21.01
105.77
21.001
1007.9
21.0001
10010
1
1 x
goes to `.
x
As x→212, 1 1 }}
2
Section 8.1
5.
323
3.
[0, 2] by [0, 3]
[0, 3] by [0, 3]
From the graph, the limit appears to be 1. The limit leads to
the indeterminate form `0.
t21
As t→1, }} approaches 2.
Ïwt 2 1
6.
1
1
2
ln 1 1 }}
x
1 x
1
ln 1 1 }} 5 x ln 1 1 }} 5 }}
1
x
x
1
2
1
1
1
x
2
1 2
2
1
1
}} 2}}2
1 1 1/x
x
ln 1 1 }}
[0, 500] by [0, 3]
}}
x
5 lim1}}
lim1}}
1
1
Ï4wxw2w
1w1
As x→`, }} approaches 2.
}}
x
x→0
x11
2}}2
x→0
x
1
7.
5 lim1 }
x→0
1
x
1 1 }}
x
5 lim1 }} 5 0
x→0 x 1 1
[25, 5] by [21, 4]
Therefore,
sin 3x
As x→0, }} approaches 3.
x
1
1 x
x
2
lim 1 1 }} 5 lim1 f (x) 5 lim1 e ln f (x) 5 e0 5 1.
x→01
8.
x→0
x→0
4.
[0, p] by [21, 2]
[0, 1000] by [0, 1]
p
tan u
As u → }}, }} approaches 1.
2 2 1 tan u
From the graph, the limit appears to be about 0.714.
5x 2 2 3x
x→` 7x 1 1
10x 2 3
14x
10
5
7
lim }
2 } 5 lim }} 5 lim }} 5 }} < 0.71429
1
h
9. y 5 }} sin h
x→`
x3 2 1
2x23
4x
x→1
10. y 5 (1 1 h)1/h
x→` 14
3x 2
21
12x
x→1
3
11
5. lim }
3 } 5 lim }2} 5 }}
Section 8.1 Exercises
1.
[0, 2] by [0, 1]
[0, 2] by [0, 1]
1
4
From the graph, the limit appears to be }}.
x22
x→2 x 2 4
1
x→2 2x
1
4
lim }
2 } 5 lim }} 5 }}
The graph supports the answer.
1 2 cos x
x
sin x
2x
x→0
x→0
x→0
2.
[22, 2] by [22, 6]
From the graph, the limit appears to be 5.
sin 5x
x
5 cos 5x
1
lim }} 5 lim }} 5 5
x→0
x→0
cos x
2
1
2
6. lim }}
5 lim }} 5 lim }} 5 }}
2
[25, 5] by [21, 1]
The graph supports the answer.
324
Section 8.1
7. The limit leads to the indeterminate form 1`.
1
sin t
ln(e x 1 x)
x
Let ln f (x) 5 ln(e x 1 x)1/x 5 }}.
ex 1 1
}
}
ex 1 x
ln(e x 1 x)
x
x→0
2
1
lim1 }} 5 lim1 } 5 lim1 }
x } 5 }} 5 2
1
x→0
x→0
61022
f (t) 60.1884 60.0167 60.0017
lim (e x 1 x)1/x 5 lim1 f (x) 5 lim1 e ln f (x) 5 e 2
x→01
61021
6100
t
ex 1 1
x→0 e 1 x
t 2 sin t
t sin t
1
t
12. Let f (t) 5 }} 2 }} 5 }}.
61023
60.00017
Estimate the limit to be 0.
x→0
1
1
t
1
2
t 2 sin t
t sin t
1 2 cos t
5 lim }}
t→0 t cos t 1 sin t
sin t
5 lim }}} 5 0
t→0 2t sin t 1 cos t 1 cos t
lim }} 2 }} 5 lim }}
t→0 sin t
[0, 5] by [0, 10]
t→0
13. Let f (x) 5 (1 1 x)1/x.
The graph supports the answer.
x
2x 1 3x
4x 1 3
4
x→` 3x 1 1
x→` 6x
2
8. lim }
} 5 lim }
3
2 } 5 lim }} 5 0
x→` x 1 x 1 1
10
102
103
104
105
f (x) 1.2710 1.0472 1.0069 1.0009 1.0001
Estimate the limit to be 1.
ln (1 1 x)
1
x
}}
11x
ln (1 1 x)
0
lim }} 5 lim } 5 }} 5 0
1
x
1
x→`
x→`
ln f (x) 5 }}
[25, 25] by [21, 2]
lim (1 1 x)1/x 5 lim f (x) 5 lim e ln f (x) 5 e 0 5 1
The graph supports the answer.
x→`
9. (a)
2
10
x
3
10
4
10
5
10
10
x→`
x→`
x 2 2x
3x 1 5x
2
14. Let f (x) 5 }
2 }.
f (x) 1.1513 0.2303 0.0345 0.00461 0.00058
10
x
102
103
104
105
Estimate the limit to be 0.
ln x 5
x→` x
5 ln x
x
x→`
5/x
x→` 1
f (x) 20.5429 20.6525 20.6652 20.6665 20.6667
0
1
(b) lim }} 5 lim }} 5 lim }} 5 }} 5 0
10. (a)
x
100
1021
1022
1023
1024
f (x) 0.1585 0.1666 0.1667 0.1667 0.1667
2
3
1 2 4x
4
2
x 2 2x 2
lim }
2 } 5 lim }} 5 lim 2}} 5 2}}.
6
3
x→` 3x 1 5x
x→` 6x 1 5
x→`
Estimate the limit to be 2}}.
sin u 2
u
u→0
1
6
x 2 sin x
1 2 cos x
(b) lim1 }}
5 lim1 }}
x3
3x 2
x→0
x→0
sin x
5 lim1 }}
6x
x→0
cos x
5 lim1 }}
6
x→0
1
5 }}
6
Estimate the limit to be }}.
2u cos u2
1
u→0
15. lim }} 5lim }} 5 (2)(0) cos (0)2 5 0
1 2 sin u
u→p/2 1 1 cos 2u
u
610
610
610
22
sin p/2
24 cos p
1
5 }}
4
5 }}
610
23
610
24
f (u) 20.1865 0.7589 0.7501 0.7500 0.7500
3
4
sin 3u
3 cos 3u
3
lim }} 5 lim }} 5 }}
4
u→0 sin 4u
u→0 4 cos 4u
Estimate the limit to be }}.
sin u
u→p/2 24 cos 2u
sin 3u
sin 4u
21
u→p/2 22 sin 2u
5 lim }}
11. Let f (u) 5 }}.
0
2cos u
16. lim }} 5 lim }}
cos t 2 1
2sin t
t→0 e 2 t 2 1
t→0 e 2 1
2cos t
e
17. lim }
5 21
} 5 lim }
t
t } 5 lim }}
t
t→0
Section 8.1
t21
1
18. lim }} 5 lim }}
t→1 ln t 2 sin pt
t→1 }1} 2 p cos pt
t
1
1 2 p(21)
5 }}
p
}} 2 y sin y
p
2
}} 2 y tan y 5 lim }}
cos y
y→p/2 2
y→p/2
22. lim
1
1
2
p
5 lim
1
p+1
5 }}
19.
y→p/2
p
p
p
(21)(1)
2(1)
5 }} 5 1
5 lim ln 2
ln x
23. lim1 x ln x 5 lim1 }
x→`
x→0
x→0
5 ln 2
1
}}
x→` }1}
2x 2
x
x→0
5 lim1 }}
(x 1 3) ln 3
(x 1 3) ln 3
x ln 2
5 lim }}
x ln 3 1 3 ln 3
x ln 2
1
}}
x
1
}}
x
}
5 lim1 1
x→0 2}}
x2
x ln 2
2
20. lim }}
5 lim }}
5 lim1 2x 5 0
x→0
5 lim }}
x→`
p
p
2
x ln 2
x→` x 1 1
x→`
2sin y
2sin }}
5 lim }}
x→` log3 (x 1 3)
1}2} 2 y2 cos y 1 (21) sin y
}}}
1}2} 2 }2}2 cos }2} 1 (21) sin }2}
5 }}}}
1
}}
x11
ln (x 1 1)
lim }} 5 lim }
x→` log2 x
x→` }1}
x ln 2
log x
2
ln 3
5 lim }}
x→` ln 2
1
tan }}
x
1
24. lim x tan }} 5 lim }
x x→` 1
x→`
}}
x
1
x
1
x
2}}2 sec2 }}
ln 3
ln 2
5 }}
5 lim }}
1
x→`
2y 1 2
}
}
y 2 1 2y
ln (y 2 1 2y)
21. lim1 }} 5 lim1 }
1
ln y
y→0
y→0
}}
y
2}}2
x
1
x
5 lim sec2 }}
x→`
y(2y 1 2)
y 1 2y
5 lim1 }
2 }
y→0
5 sec2 0 5 1
2y 2 1 2y
5 lim1 }
2
y→0 y 1 2y
4y 1 2
25. lim1 (csc x 2 cot x 1 cos x)
5 lim1 }}
y→0 2y 1 2
4(0) 1 2
2(0) 1 2
x→0
2
2
5 }} 5 }} 5 1
1 sin x
1
cos x
sin x
2
5 lim1 }} 2 }} 1 cos x
x→0
1 2 cos x 1 cos x sin x
sin x
5 lim1 }}}
x→0
sin x 1 cos x cos x 2 sin x sin x
cos x
5 lim1 }}}} 5 1
x→0
325
326
Section 8.1
1x 1 12
2x
26. lim (ln 2x 2 ln (x 1 1)) 5 lim ln }}
x→`
x→`
2x
x11
Let f (x) 5 }}.
2x
x→` x 1 1
33. The limit leads to the indeterminate form `0.
Let f (x) 5 (ln x)1/x.
ln (ln x)
x
ln (ln x)1/x 5 }}
2
x→` 1
lim }} 5 lim }} 5 2
1/x
}}
Therefore,
lim (ln 2x 2 ln (x 1 1)) 5 lim ln f (x) 5 ln 2
x→`
ln x
ln (ln x)
1
lim }} 5 lim } 5 lim }} 5 0
x
x→`
x→` 1
x→` x ln x
x→`
x
sin x
27. lim1 (ln x 2 ln sin x) 5 lim1 ln }}
x→0
x→0
x
sin x
x
1
Let f (x) 5 (1 1 2x)1/(2 ln x).
lim }} 5 lim1 }} 5 1
x→0 cos x
Therefore,
lim (ln x 2 ln sin x) 5 lim1 ln f (x) 5 ln 1 5 0
x→01
x→0
1
1
1 2Ïxw
28. lim1 }} 2 }} 5 lim1 }} 5 `
x
x
x→0
x→0
Ïwx
1
2
29. The limit leads to the indeterminate form 1`.
Let f (x) 5 (e 1 x) .
x
1/x
ln (e 1 x)
x
1/x
ln (1 1 2x)
2 ln x
ln (1 1 2x)1/(2 ln x) 5 }}
2
}}
ln (1 1 2x)
1
1
x
1 1 2x
lim }} 5 lim }
5 lim }} 5 lim }} 5 }}
2
2
l
n
x
2
x→`
x→`
x→` 1 1 2x
x→` 2
}}
x
lim (1 1 2x)1/(2 ln x) 5 lim eln f (x) 5 e1/2 5 Ïew
x→`
x→`
35. The limit leads to the indeterminate form 00.
Let f (x) 5 (x 2 2 2x 1 1)x21
ln (e x 1 x)
5 }}
x
ln (e x 1 x)
x
x→0
x→`
34. The limit leads to the indeterminate form `0.
Let f (x) 5 }}.
x→01 sin x
lim (ln x)1/x 5 lim eln f (x) 5 e0 5 1
x→`
ln (x 2 2 2x 1 1)x21 5 (x 2 1) ln (x 2 2 2x 1 1)
ex 1 1
}
}
ex 1 x
lim }} 5 lim } 5 2
x→0
ln (x 2 2x 1 1)
5 }}
2
1
1
}}
x21
lim (e x 1 x)1/x 5 lim e ln f (x) 5 e 2
x→0
x→0
30. The limit leads to the indeterminate form `0.
1 x
1x 2
Let f (x) 5 }}2 .
2x 2 2
}}
x 2 2 2x 1 1
ln (x 2 2 2x 1 1) 5 lim }}
lim }}
1
x→1
x→1 2}1}
}}
2
(x 2 1)
x21
1 2
2(x 2 1)
}}
(x 2 1)2
}}
5 lim
x→1 2}1}
(x 2 1)2
1
ln }}2
1 x
1
x
ln }}2 5 x ln }}2 5 }
1
x
x
1 2
1 2
1 2
1
ln }}2
x
lim }
5 lim
x→0
1
}}
x
}}
x
5 lim 22(x 2 1) 5 0
22/x 3
}}
1/x 2
}2 5 lim 2x 5 0
x→0 21/x
x→0
1 x
1 2
x→0 x
lim }}2 5 lim e ln f (x) 5 e 0 5 1
x→0
3x 2 5
3
31. lim }
2 } 5 lim }} 5 0
x→6` 2x 2 x 1 2 x→6` 4x 2 1
sin 7x
7 cos 7x
7
11
x→1
lim (x 2 2x 1 1)
2
x21
x→1
5 lim eln f (x) 5 e0 5 1
36. The limit leads to the indeterminate form 00.
Let f (x) 5 (cos x)cos x.
ln (cos x)
sec x
ln (cos x)cos x 5 (cos x) ln (cos x) 5 }}
32. lim }} 5 lim }}
5 }}
2
x→0 tan 11x
x→0 11 sec 11x
x→1
2sin x
}}
ln (cos x)
sec x
x→p/2
x→p/2 sec x tan x
cos x
lim 2 }} 5 lim 2 }}
2tan x
5 lim 2 }}
x→p/2 sec x tan x
5 lim 2 2cos x 5 0
x→p/2
lim (cos x)cos x 5 lim 2 e ln f (x) 5 e0 5 1
x→p/22
x→p/2
Section 8.1
37. The limit leads to the indeterminate form 1`.
Let f (x) 5 (1 1 x) .
1/x
E
2x
42.
x
3 4
dt
}} 5 ln )t)
t
ln (1 1 x)
x
1
}}
lim (1 1 x)1/x 5 lim1 eln f (x) 5 e1 5 e
x→0
38. The limit leads to the indeterminate form 1`.
Let f (x) 5 x
1/(x21)
E
2x
x→` x
ln (1 1 x)
11x
lim }} 5 lim1 }
}51
1
x
x→01
x→0
) 2xx )
5 ln )2x) 2 ln )x) 5 ln }}
x
lim
ln (1 1 x)1/x 5 }}
x→01
2x
327
) )
dt
2x
}} 5 lim ln }} 5 lim ln 2 5 ln 2
t
x
x→`
x→`
43. (a) L’Hôpital’s Rule does not help because applying
L’Hôpital’s Rule to this quotient essentially “inverts”
the problem by interchanging the numerator and
denominator (see below). It is still essentially the same
problem and one is no closer to a solution. Applying
L’Hôpital’s Rule a second time returns to the original
problem.
(9/2)(9x 1 1)21/2
Ï9ww
ww1
ww1
9Ïw
x1
x1
lim }} 5 lim }}
21/2 5 lim }}
x→` Ïx
x→` (1/2)(x 1 1)
x→` Ï9
x1
w1
ww1
ww
ww1
.
(b)
ln x
x21
1/x
ln x
lim }} 5 lim }} 5 1
x→1 x 2 1
x→1 1
ln x1/(x21) 5 }}
lim x1/(x21) 5 lim e ln f (x) 5 e1 5 e
x→1
x→1
[0, 100] by [0, 4]
The limit appears to be 3.
0
39. The limit leads to the indeterminate form 0 .
!9§§1§}x}§ Ï9w
Ï9ww
ww1
x1
}
(c) lim }} 5 lim
1 5 }} 5 3
x→` Ïw
x→`
x1
ww1
!1§§1§}x}§ Ï1w
1
Let f (x) 5 (sin x)x.
ln (sin x)
ln (sin x)x 5 x ln (sin x) 5 }
1
}}
x
44. (a) L’Hôpital’s Rule does not help because applying
L’Hôpital’s Rule to this quotient essentially “inverts”
the problem by interchanging the numerator and
denominator (see below). It is still essentially the same
problem and one is no closer to a solution. Applying
L’Hôpital’s Rule a second time returns to the original
problem.
cos x
}}
sin x
ln
(sin
x)
lim1 } 5 lim1 }
1
x→0
x→0 2}1}
}}
x
x2
2x 2 cos x
sin x
x→0
5 lim1 }}
sec x
x 2 sin x 2 2x cos x
5 lim1 }} 5 0
cos x
x→0
lim1 (sin x)x 5 lim1 e ln f (x) 5 e0 5 1
x→0
sec x tan x
sec x
tan x
lim }} 5 lim }}
5 lim }}
2
x→p/2 tan x
x→p/2
x→p/2 sec x
(b)
x→0
40. The limit leads to the indeterminate form 00.
Let f (x) 5 (sin x)tan x
ln (sin x)
tan x
[0, p] by [21, 5]
ln (sin x)
5 tan x ln (sin x) 5 }}
cot x
cos x
}}
sin x
ln (sin x)
lim1 }} 5 lim1 }
2 5 lim1 (2sin x cos x) 5 0
cot x
x→0
x→0 2csc x
x→0
lim (sin x)tan x 5 lim1 e ln f (x) 5 e0 5 1
x→01
1
}}
sec x
1
cos x
(c) lim }} 5 lim }
5 lim }} 5 1
x→p/2 tan x
sin x
x→p/2 }
}
x→p/2 sin x
cos x
45. Possible answers:
x→0
41. The limit leads to the indeterminate form 12`.
Let f (x) 5 x1/(12x).
ln x
12x
ln x
lim }} 5 lim1
x→11 1 2 x
x→1
1
}}
x
}
21
f (x)
7(x 2 3)
x23
7
lim }} 5 lim }} 5 lim }} 5 7
x→3
x→3 1
(b) f (x) 5 (x 2 3)2; g(x) 5 x 2 3
f (x)
(x 2 3)2
x23
2(x 2 3)
1
lim }} 5 lim }} 5 lim }} 5 0
5 21
x→3 g(x)
1
e
lim1 x1/(12x) 5 lim1 e ln f (x) 5 e21 5 }}
x→1
(a) f (x) 5 7(x 2 3); g(x) 5 x 2 3
x→3 g(x)
ln x1/(12x) 5 }}
x→1
The limit appears to be 1.
x→3
x→3
(c) f (x) 5 x 2 3; g(x) 5 (x 2 3)3
f (x)
x23
x→3 g(x)
x→3 (x 2 3)
1
lim }} 5 lim }}3 5 lim }}2 5 `
x→3 3(x 2 3)
328
Section 8.1
46. Answers may vary.
(a) f (x) 5 3x 1 1; g(x) 5 x
3x 1 1
x
f (x)
3
lim }} 5 lim }} 5 lim }} 5 3
x→` g(x)
x→`
x→` 1
(b) Part (a) shows that as the number of compoundings per
year increases toward infinity, the limit of interest compounded k times per year is interest compounded continuously.
(b) f (x) 5 x 1 1; g(x) 5 x 2
f9(x)
lim }} 5 1
x→0 g 9(x)
x11
f (x)
1
lim }} 5 lim }}
2 5 lim }} 5 0
x→` g(x)
x→` x
x→` 2x
f (x)
2x
x
lim }} 5 lim }} 5 lim }} 5 `
x→` x 1 1
x→` g(x)
2
1
f (x)
lim }} 5 }} 5 2
x→0 g (x)
(c) f (x) 5 x 2; g(x) 5 x 1 1
2
1
1
f9(x)
g 9(x)
50. (a) For x Þ 0, }} 5 }} 5 1.
x→` 1
(b) This does not contradict L’Hôpital’s Rule since
lim f (x) 5 2 and lim g (x) 5 1.
x→0
51. (a) A(t) 5
Ee
t
x→0
2x
0
3
4
47. Find c such that lim f (x) 5 c.
x→0
9x 2 3 sin 3x
5x
9 2 9 cos 3x
}}
15x2
27 sin 3x
}}
30x
81 cos 3x
81
27
}} 5 }} 5 }}
30
30
10
lim f (x) 5 lim }}
3
x→0
x→0
5 lim
x→0
5 lim
x→0
5 lim
x→0
1
t
dx 5 2e2x 5 2e2t 1 1
lim A(t) 5 lim (2e2t 1
t→`
2
1
e
0
t→`
1) 5 lim 2}}t 1 1 5 1
t→`
E (e
5 pE e
t
(b) V(t) 5 p
2x 2
) dx
0
t
22x
dx
0
27
Thus, c 5 }}. This works since lim f (x) 5 c 5 f (0), so f is
10
x→0
3
1
2
1
1
2
5 p 2}}e22x
continuous.
40
t
1
2
2
5 p 2}}e22t 1 }}
48. f (x) is defined at x Þ 0. lim f (x) leads to the indeterminate
p
2
x→0
5 }}(2e22t 1 1)
form 00.
p
p
}}(1)
}}(2e22t 1 1)
2
V(t)
p
2
lim }} 5 lim }}
5 } 5 }}
2t
2e 1 1
1
2
t→` A (t)
t→`
ln )x)
ln )x)x 5 x ln )x) 5 }
1
}}
x
1
}}
ln )x)
x
5 lim 2x 5 0
lim }
1 5 lim }
x→0 }}
x→0 2}1}
x→0
2
x
p
}}(2e22t 1 1)
V(t)
2
(c) lim1 }} 5 lim1 }}
2e2t 1 1
t→0 A (t)
t→0
x
lim )x) 5 lim e
x
x→0
x ln )x)
x→0
p
}}(2e22t)
2
5 e0 5 1
5 lim1 }
2t
Thus, f has a removable discontinuity at x 5 0. Extend the
definition of f by letting f (0) 5 1.
p
}}(2)
2
5}5p
49. (a) The limit leads to the indeterminate form 1`.
1
r kt
k
2
1
r
k
2
ln f (k) 5 kt ln 1 1 }} 5
1
2
r
t ln 1 1 }}
k
}}
1
}}
k
r
r 21
t 2}}2 1 1 }}
k
k
lim }} 5 lim }}
1
2}1}2
k→`
k→`
}}
k
k
1
r
k
2
1 21
t ln 1 1 }}
2
5 lim } 5 }} 5 rt
k→` 1 1 }r}
1
f (x)
0.1
0.04542
0.01
0.00495
0.001
0.00050
0.0001
0.00005
The limit appears to be 0.
sin x
0
1
(b) lim }} 5 }} 5 0
L’Hôpital’s Rule is not applied here because the limit is
k
r kt
r kt
5 A0 lim 1 1 }}
k
k
k→`
2
1
lim A0 1 1 }}
k→`
x
x→0 1 1 2x
rt
1
rt
1
52. (a)
Let f (k) 5 1 1 }} .
e
t→0
5 A0 lim e ln f (k)
k→`
5 A0 e rt
2
0
0
`
`
not of the form }} or }}, since the denominator has
limit 1.
Section 8.2
53. (a) f (x) 5 e x ln (1 1 1/x)
(b) f9(x) 5 2sin x, g 9(x) 5 cos x
p
122
1
1 1 }} . 0 when x , 21 or x . 0
x
p
2sin c
21
}} 5 }}
cos c
1
tan c 5 1
(b) The form is 021, so lim 2 f (x) 5 `
p
4
1
56. (a) ln f (x)g(x) 5 g(x) ln f (x)
2
ln 1 1 }}
1
x
(c) lim x ln 1 1 }} 5 lim }}
1
x
x→−`
x→−`
}}
2
1x→c
2
g(x)
lim f (x) g(x) 5 lim e ln f (x)
x→c
x→c
1x→c
x→c
lim f (x)
g(x)
x→c
lim f (x) 5 lim e x ln (111/x) 5 e
54. (a) Because the difference in the numerator is so small
compared to the values being subtracted, any calculator
or computer with limited precision will give the
incorrect result that 1 2 cos x 6 is 0 for even moderately
small values of x. For example, at x 5 0.1,
cos x 6 < 0.9999999999995 (13 places), so on a
10-place calculator, cos x 6 5 1 and 1 2 cos x 6 5 0.
(b) Same reason as in part (a) applies.
5 lim
x→0
5 lim
x→0
g(x)
5 lim eln f (x)
x→c
5 e` 5 `
(pp. 425–433)
Exploration 1
x→`
ax
x→` x
Comparing Rates of Growth as
(ln a)(a x)
2x
x→`
(ln a)2 a x
2
x→`
1. lim }}2 5 lim }} 5 lim }} 5 `, so a x grows
faster than x 2 as x→`.
3x
2
x→`
6x 5 sin x 6
12x
sin x 6
}}
2x 6
6x 5 cos x 6
}}
12x 5
cos x 6
1
}} 5 }}
2
2
2. lim }}x 5 lim 1.5x 5 `
(c) lim }1}
5 lim }}
2
11
x→0
2
■ Section 8.2 Relative Rates of Growth
x→−`
x→0
21x→c
5 (2`)(2`) 5 `
x
5 lim
5 e2` 5 0
(b) lim (g(x) ln f (x)) 5 lim g(x) lim ln f (x)
1
5 lim } 5 1
x→−` 1 1 }1}
1 2 cos x 6
x
x→0
2
5 `(2`) 5 2`
1 21
1
2}}2 1 1 }}
x
x
5 lim }}
x→−`
2}1}2
x
x→−`
21x→c
lim (g(x) ln f (x)) 5 lim g(x) lim ln f (x)
x→c
x
1 21
p
1 22
c 5 tan21 1 5 }} on 0, }}
x→21
1
122
f }} 2 f (0) 5 21, g }} 2 g(0) 5 1
Domain: (2`, 21) < (0, `)
1
329
a
x→` b
x
x→`
a x
12
x→` b
a
b
3. lim }}x 5 lim }} 5 ` because }} . 1.
Quick Review 8.2
1
}}
(d) The graph and/or table on a grapher show the value of
the function to be 0 for x-values moderately close to 0,
but the limit is 1/2. The calculator is giving unreliable
information because there is significant round-off error
in computing values of this function on a limited
precision device.
55. (a) f9(x) 5 3x 2, g 9(x) 5 2x 2 1
x
ln x
1. lim }}
x 50
x 5 lim }
x→` e
x→` e
ex
x→` x
ex
x→` 3x
ex
x→` 6x
ex
x→` 6
2. lim }}3 5 lim }}2 5 lim }} 5 lim }} 5 `
x2
x→2` e
3. lim }2}x 5 `
x2
x→` e
2x
2
4. lim }2}x 5 lim }}
2x 5 lim }}
2x 5 0
f (1) 2 f (21) 5 2, g(1) 2 g(21) 5 22
3c 2
2
} } 5 }}
2c 2 1
22
x→` 2e
x→` 4e
2x 3
x
5. 23x 4
6. }} 5 2x 2
1
1 1 }}
x
x 1 ln x
f (x)
7. lim }} 5 lim }} 5 lim } 5 1
1
x
x→` g(x)
x→`
x→`
3c 2 5 22c 1 1
3c 2 1 2c 2 1 5 0
Ï4wxw2w
f (x)
1w5xw
8. lim }} 5 lim }} 5 lim
(3c 2 1)(c 1 1) 5 0
x→` g(x)
1
3
c 5 }} or c 5 21
1
3
The value of c that satisfies the property is c 5 }}.
x→`
2x
x→`
!1§§1§}4§}x 5 1
5
330
Section 8.2
ex 1 x2
x2
e
e
2xe x 2 x 2e x
2x 2 x 2
f 9(x) 5 }2x
} 5 }}
ex
e
2x 2 x 2
50
}}
ex
12
9. (a) f (x) 5 }}
5 1 1 }}x
x
1
x }} 1 ln x 2 1
x
x ln x 2 x
6. lim }}
5 lim }}
x
ex
e
x→`
x→`
ln x
5 lim }}
x
x→` e
1/x
5 lim }}
x 50
x→` e
x(2 2 x) 5 0
x ln x 2 x grows slower than e x as x→`.
x 5 0 or x 5 2
f 9(x) , 0 for x , 0 or x . 2
The graph decreases, increases, and then decreases.
4
f (0) 5 1; f (2) 5 1 1 }}2 < 1.541
e
f has a local maximum at < (2, 1.541) and has a local
xe x
x→` e
8. lim }}
x 5 lim x 5 `
x→`
x1000
x→` e
(b) f is increasing on [0, 2]
1
9. lim }}
x 5 0 Repeated application of L’Hôpital’s Rule
(c) f is decreasing on (2`, 0] and [2, `).
2
1000!
1000
gets lim }}
grows slower than e x as x→`.
x 5 0. x
x→` e
x 1 sin x
sin x
x
x
sin x
Observe that }} , 1 since )sin x) , )x) for x Þ 0.
x
sin x
lim f (x) 5 1 1 lim }} 5 1 1 1 5 2
x→0
x→0 x
10. f (x) 5 }} 5 1 1 }}, x Þ 0
)
(e x 1 e2x)/2
1
1
1
e
2
2e
x→`
x→` 2
e x 1 e2x
x
}} grows at the same rate as e as x→`.
2
1
2
10. lim }}
5 lim }} 1 }}
x
2x 5 }}
Thus the values of f get close to 2 as x gets close to 0, so f
doesn’t have an absolute maximum value. f is not defined at
x 2 1 4x
x
x→`
1
4
x
2
11. lim }}
5 lim 1 1 }} 5 1
2
x→`
x 2 1 4x grows at the same rate as x 2 as x→`.
0.
Section 8.2 Exercises
x 3 2 3x 1 1 grows slower than e x as x→`.
11x
x
lim }}
5 lim
2
x→`
lim }} 1 1 5 1
!}
§§x}
§§ 5 x→
x §§§
` !§
11x
x→`
2
2
4
1
4
4
x
x 2 grows slower than e x as x→`, so Ï1ww
1wx 4w grows slower
than e x as x→`.
4 x
12
x→` e
4
e
4x grows faster than e x as x→`.
(5/2)x
5 x
5
2e
x→` e
x→` 2e
5 x
}} grows slower than e x as x→`.
2
1 2
1x
15
x→`
3
x
2
15x 1 3 grows slower than x 2 as x→`.
Ïxw4w
1w5xw
14. lim }}
5 lim
2
5 lim 1 1 }} 5 1
}}
x §§§ x→` !§§§x §
x→` !§§§
x
x 4 1 5x
5
4
3
2
ln x
1/x
1
x→` 2x
x→` 2x
2
15. lim }}
2 5 lim }} 5 lim }}
2 50
x→` x
2x
x→` x
(ln 2)2 x
2x
x→`
(ln 2)2 2 x
2
x→`
16. lim }}2 5 lim }} 5 lim }} 5 `.
log x 2
2 log x
2(ln x)/(ln 2)
ln x
2
ln 2
2
17. lim }2} 5 lim }}
5 lim }} 5 }}
x→`
ln x
x→`
ln x
x→`
log2 x 2 grows at the same rate as ln x as x→`.
log Ïwx
(ln x)/(ln 10)
log x
1
18. lim }} 5 lim }} 5 lim }} 5 }}
5. lim }}
x 5 lim e 5 e
x11
15x 1 3
x
2 x grows faster than x 2 as x→`.
4. lim }}
x 5 lim }} 5 0 since }} , 1.
e x 11
x→` e
x→`
ln x grows slower than x as x→`.
3. lim }}x 5 lim }} 5 ` since }} . 1.
12
2
Ïw
x w
1w5xw grows at the same rate as x as x→`.
2
x→` e
lim }}x 5 lim }}x 5 lim }}x 5 0
4x
x→` e
3
x
x 1 3 grows faster than x 2 as x→`.
4
2x
x→` e
1
3
x→`
Next compare x with e .
x2
x→` e
x→`
13. lim }}
5 lim }} 1 }}2 5 0
2
2. First observe that Ï1ww
1wx w grows at the same rate as x .
4
Ïwww4w
x3 1 3
x
x→`
12. lim }}
5 lim x 1 }}2 5 `
2
x 3 2 3x 1 1
3x 2 2 3
6x
6
1. lim }}
5 lim }}
5 lim }}x 5 lim }}x 5 0
x
e
ex
x→`
x→`
x→` e
x→` e
e
ecos x grows slower than e x as x→`.
xe xgrows faster than e x as x→`.
minimum at (0, 1).
)
ecos x
x→` e
cos x
7. lim }}
# e for all x.
x 5 0 since e
x→`
x→`
x
grows at the same rate as e as x→`.
ln x
x→` 2 ln x
x→`
2 ln x
log Ïxw grows at the same rate as ln x as x→`.
2 ln 10
Section 8.2
1/Ïxw
1
19. lim }} 5 lim }} 5 0
x→` ln x
x→` Ïx
w ln x
1
}} grows slower than ln x as x→`.
Ïwx
e2x
x→` ln x
25. Compare f1 to f2.
f2(x)
Ï1w0wxw1
ww1
1
lim }
w0w
} 5 lim }} 5 lim 10 1 }} 5 Ï1
x
x→` f1(x)
x→`
x→`
Ïxw
Thus f1 and f2 grow at the same rate.
!§§§§§
1
20. lim }} 5 lim }
x }50
Compare f1 to f3.
x→` e ln x
e2x grows slower than ln x as x→`.
f3(x)
Ïxw1
ww1
1
lim }
} 5 lim }} 5 lim 1 1 }} 5 1
x
x→`
x→`
Ïxw
Thus f1 and f3 grow at the same rate.
!§§§§
x→` f1(x)
x 2 2 ln x
ln x
1
2
x
1
1
21. lim }} 5 lim }} 2 2 5 lim }} 2 2
x→`
x→` ln x
331
x→` 1/x
2
5 lim (x 2 2) 5 `
By transitivity, f2 and f3 grow at the same rate, so all three
x 2 2 ln x grows faster than ln x as x→`.
functions grow at the same rate as x→`.
x→`
5 ln x
22. lim }} 5 5
26. Compare f1 to f2.
x→` ln x
f2(x)
Ïxw4w
1wx
lim }
5 lim
} 5 lim }}
2
5 ln x grows at the same rate as ln x as x→`.
x→` f1(x)
e
e x
12
x→` x
f3(x)
Ïxw4w
2wx 3w
lim }
5 lim
} 5 lim }}
2
e grows slower than x x.
x→` f1(x)
Compare e x to (ln x)x.
e
x
!1§§1§}x}§ 5 1
1
3
Compare f1 to f3.
lim }} 5 lim }} 5 0
x
x→` x
x
x→`
Thus f1 and f2 grow at the same rate.
23. Compare e x to x x.
x
x
x→`
1 2
e
x
x→`
x→`
!1§§2§}x}§ 5 1
1
Thus f1 and f3 grow at the same rate.
x
lim }} 5 lim }} 5 0
By transitivity, f2 and f3 grow at the same rate, so all three
e grows slower than (ln x)x.
functions grow at the same rate as x→`.
x
x→` (ln x)
x
x→` ln x
x
x/2
Compare e to e .
ex
x→` e
x/2
lim }x}
5`
/2 5 lim e
x→`
x
27. Compare f1 to f2.
x/2
e grows faster than e .
f2(x)
Ï9wxw1
ww2xw
lim }
} 5 lim }}
x
x→` f1(x)
Compare x x to (ln x)x.
x
x
1 2
x
x
x
Ï9wxw1
ww2xw
1
5 lim }}
x→`
Ï9wxw
lim }} 5 lim }} 5 ` since lim }} 5 lim }} 5 `.
x
x→` (ln x)
x
x→` ln x
x→` ln x
x grows faster than (ln x)x.
x→` 1/x
5 lim
x→`
Thus, in order from slowest-growing to fastest-growing, we
24. Compare 2x to x 2.
(ln 2)2 x
2x
x→`
(ln 2)2 2 x
2
x→`
lim }}2 5 lim }} 5 lim }} 5 `
2 x grows faster than x 2.
2
1 2
2
2
ln 2
2 grows faster than (ln 2)x.
2
2 x
1e2
2
e
2 grows slower than e x.
Compare x 2 to (ln 2)x.
x2
(ln
2)
x→`
lim }}x 5 ` since lim x 2 5 ` and lim (ln 2)x 5 0.
2
x→`
x→`
x
5 lim
!1§§2§1§2§ 5 1
4 x
}}
9
Thus f1 and f3 grow at the same rate.
By transitivity, f2 and f3 grow at the same rate, so all three
functions grow at the same rate as x→`.
lim }} 5 lim }} 5 0 since }} , 1.
x→`
3
5 lim }}
Ï9wxw
x→`
x→`
Compare 2 x to e x.
x
x→` e
x
x→`
9 24
x
x→` ln 2
x
f3(x)
Ï9wxw2
ww
4 xw
lim }
} 5 lim }}
x
Ïwxwwwxw
lim }} 5 lim }} 5 ` since }} . 1.
x
x→` (ln 2)
x
2 x
Compare f1 to f3.
x→` f1(x)
Compare 2 x to (ln 2)x.
x
!1§§1§1}§9}§2 5 1
Thus f1 and f2 grow at the same rate.
get e x/2, e x, (ln x)x, x x.
2x
x→` x
3
x→`
x grows faster than (ln 2) .
Thus, in order from slowest-growing to fastest-growing, we
get (ln 2)x, x 2, 2 x, e x.
332
Section 8.2
28. Compare f1 to f2.
f (x)
x→`
2
lim }
} 5 lim }}
3
x→` f1(x)
x
x→`
ex 1 x
e
x→`
x 4 1 2x 2 2 1
x 1x
x→`
3
2
ex 1 1
e
x→`
1
1 1 }}x
e
5 lim }
5 1 # 1.
1
x→`
1
1 1 }}2 2 }}4
x
x
5 lim }}
51
x→`
3
x→` 2
(e) True, since lim }}
5 lim }}
x
x
5 lim }
4 }
3
2
2 1 cos x
2
(d) True, since lim }} # lim }} 5 }}.
x 4 1 2x 2 2 1
}}
x11
1
x
1 1 }}
x ln x
x
ln x
x
1/x
(f) True, since lim }}
2 5 lim }} 5 lim }} 5 0.
x→`
Thus f1 and f2 grow at the same rate.
(g) True,
Compare f1 and f3.
2x 5 2 1
x→`
x→` 1
1
}}
x
l
nx
ln (ln x)
since lim }} 5 lim }
l
n
x
1
x→`
x→`
}}
x
}
}
f3(x)
x2 1 1
lim }
} 5 lim }
x3
x→` f1(x)
x→`
1
5 lim }} 5 0 # 1.
x→` ln x
2x 5 2 1
ln x
1/x
(h) False, since lim }2} 5 lim }
2x
5 lim }
5 }
3
x→` ln (x 1 1)
x→` x 1 x
1
2 2 }}5
x
5 lim }
52
1
x→`
1 1 }}2
x→` }}
2
x 11
x2 1 1
1
5 lim }}
2 5 }} Þ 0.
2
x→` 2x
x
Thus f1 and f3 grow at the same rate.
By transitivity, f2 and f3 grow at the same rate, so all three
functions grow at the same rate.
f (x)
g(x)
x→` g(x)
x→` f (x)
31. From the graph, lim }} 5 `, so lim }} 5 0.
Thus g 5 o(f ), so ii is true.
f (x)
32. From the graph, lim }} 5 0. Thus f 5 o(g), so i is true.
x→` g(x)
x
29. (a) False, since lim }} 5 1 Þ 0.
x→` x
f (x)
33. From the graph, lim }} # 1 and not equal to zero. Thus, f
x→` g(x)
x
(b) False, since lim }} 5 1 Þ 0.
x→` x 1 5
and g grow at the same rate, so iii is true.
x
(c) True, since lim }} 5 1 # 1.
f (x)
34. From the graph, lim }} # 3 and not equal to zero. Thus, f
x→` x 1 5
x→` g(x)
1
2
x
(d) True, since lim }} 5 }} # 1.
x→` 2x
ex
and g grow at the same rate, so iii is true.
1
35. (a) The nth derivative of x n is n!, a constant. We can apply
(e) True, since lim }2}x 5 lim }}x 5 0.
x→` e
x→` e
1
1 1 }}
x 1 ln x
x
(f) True, since lim }} 5 lim }
5 1 # 1.
1
x
x→`
x→`
1/x
x→` 1/x
ln x
x→` ln 2x
(g) False, since lim }} 5 lim }} 5 1 Þ 0.
Ïw
x 2w
1w5
(h) True, since lim }} 5 lim
x→`
30. (a) True,
x
1
}}
x13
since lim }
1
x→`
}}
x
x→`
(b) True,
!§§§§
x
x→` x 1 3
(c) False,
1
1
}} 2 }}2
x
x
since lim }
1
x→`
}}
x
Thus e x grows faster than x n as x→` for any positive
5 lim } 5 1 # 1.
1
1
x
1 2 }}
5 lim } 5 1 Þ 0.
1
(b) The nth derivative of a x, a . 1, is (ln a)n a x. We can
ax
x→` x
apply L’Hôpital’s Rule n times to find lim }}n .
ax
x→` x
1
x
x→`
ex
x→` n!
(ln a)n ax
n!
x→`
lim }}n 5 … 5 lim }} 5 `
1 1 }}
x→`
ex
x→` x
lim }}n 5 … 5 lim }} 5 `
integer n.
5
1 1 }}2 5 1 # 1.
x
5 lim }} 5 1 # 1.
1
1
}} 1 }}2
x
x
since lim }
1
x→`
}}
x
ex
x
x→`
L’Hôpital’s Rule n times to find lim }}n .
Thus a x grows faster than x n as x→` for any positive
integer n.
Section 8.2
39. Compare n log2 n to n3/2 as n→`.
36. (a) Apply L’Hôpital’s Rule n times to find
n log n
ex
1
n→`
1 a1 x 1 a0
ex
1
n
(ln n)
}}
(ln 2)
ex
x→` ann!
1 a1 x 1 a0
n
n→`
5 lim }} 5 `
lim }}}}
n
n21
…
x→` anx 1 an21x
log n
2
2
lim }3}
5 lim }1}
/2
/2
.
lim }}}}
n
n21
…
x→` anx 1 an21x
5 lim }
1/2
n→` n
1
}}
n ln 2
5 lim }
n→` }1}
2n1/2
Thus e x grows faster than
anx n 1 an21x n21 1 … 1 a1x 1 a0 as x→`.
(b) Apply L’Hôpital’s Rule n times to find
1 a1 x 1 a0
n log n
ax
5…
lim }}}}
n
n21
1 … 1 a1 x 1 a0
x→` anx 1 an21x
(ln a)na x
5 lim }} 5 `
ann!
x→`
Thus ax grows faster than
anx n 1 an21x n21 1 … 1 a1x 1 a0 as x→`.
1
}}
ln x
n
x
37. (a) lim }1/}n 5 lim }
5 lim }1}
/n 5 0
x→` x
x→` 1 (1/n)21
x→` x
}}x
n
Thus ln x grows slower than x1/n as x→` for any
Thus n log2 n grows slower than n(log2 n)2 as n→`.
The algorithm of order of n log2 n is likely the most
efficient because of the three functions, it grows the most
slowly as n→`.
40. (a) It might take 1,000,000 searches if it is the last item in
the search.
(b) log2 1,000,000 < 19.9; it might take 20 binary
searches.
41. Since f and g grow at the same rate, there exists a nonzero
f (x)
number L such that lim }} 5 L. Then for sufficiently
x→` g(x)
g(x)
f (x)
1
x→` ax
a
a . 0.
L
42. (a) The limit will be the ratio of the leading coefficients of
the polynomials since the polynomials must have the
same degree.
(b) By the same reason as in (a), the limit will be the ratio
of the leading coefficients of the polynomial.
ln x
38. lim }}}}
n
n21
1 … 1 a1 x 1 a0
x→` anx 1 an21x
x5
x→` x
43. (a) lim }}2 5 lim x 3 5 `
1
}}
x
5 lim }}}}}
n21
n22
…
1 (n 2 1)an21x
1
some integer N.
Thus ln x grows slower than x as x→` for any number
x→` nanx
n→` log2 n
Similarly, for sufficiently large x, }} , }} 1 1 # N for
(b) lim }}
a21 5 lim }}
a 5 lim }
a 50
x→` ax
n→` n(log2 n)
f (x)
g(x)
1
}}
x
ln x
1
2
lim }}
2 5 lim }} 5 0
large x, }} , L 1 1 # M for some integer M.
positive integer n.
x→` x
Thus n log2 n grows slower than n3/2 as n→`.
Compare n log2 n to n(log2 n)2
.
lim }}}}
n
n21
…
x→` anx 1 an21x
2
(ln 2)
5 lim }
1/2 } 5 0
n→` n
ax
1
333
1
1 a1
x→`
x 5 grows faster than x 2.
5x 3
x→` 2x
5
5
2
(b) lim }}3 5 lim }} 5 }}
1
5 lim }}}}
50
n
n21
1 … 1 a1 x
x→` nanx 1 (n 2 1)an21x
Thus ln x grows slower than any nonconstant
x→` 2
3
5x 3 and 2x have the same rate of growth.
xm
(c) m . n since lim }}n 5 lim x m2n 5 `.
x→` x
x→`
xm
polynomial as x→`.
(d) m 5 n since lim }}n 5 lim x m2n is nonzero and finite.
x→` x
x→`
g(x)
(e) Degree of g . degree of f (m . n) since lim }} 5 `.
x→` f (x)
g(x)
(f) Degree of g 5 degree of f (m 5 n) since lim }} is
x→` f (x)
nonzero and finite.
334
Section 8.3
3. If p . 1, then
f (x)
x→a g(x)
44. (a) f 5 o(g) as x→a if lim }} 5 0
E
1
Suppose f and g are both positive in some open interval
0
dx
}}p 5 lim
x
c→01
1
close to a.
b2a
180
(b) From Section 5.5, we know that )ES) # }} h 4M
E
1
on
0
dx
}}p 5 lim
x
c→01
where M is a bound for the absolute value of f 0 on
)ET)
M
M
[a, b]. Thus }}
# (b 2 a)}} # int (b 2 a)}} 1 1 as
h2
12
12
4
h→0, so )ET) 5 O(h ). Thus as h→0, ET→0.
2
) f(x))
2f (x)
x→` 2g(x)
f (x)
x→` g(x)
45. (a) lim }} 5 lim }} 5 lim }} 5 `
x→` ) g(x))
2f (x)
x→` 2g(x)
E
3
1.
0
2.
E
3.
3
dx
}} 5 ln )x 1 3)
x13
1
21
f (x)
x→2` g(x)
Thus f (2x) grows faster than g(2x) by definition.
3
■ Section 8.3 Improper Integrals
(pp. 433–444)
E
1
Exploration 1
Investigating
0
dx
}}
xp
1
x
1. Because }}p has an infinite discontinuity at x 5 0.
0
1
2
1
2
5 }} ln 2 2 }} ln 2 5 0
2
122
2
1
x
2
2
1
2
x
2
dx
1
}}4 5 x24 dx 5 2}}x23 1 C
x
3
E
E
5 }} tan21 }} 1 C
6. x 2 1 . 0 for x . 1
The domain is (1, `).
)cos x)
# }}2
)}x}
2 ) 5 }}
)x 2)
x
1
8. x 2 2 1 # x 2 so Ïw
x 2w
2w1 # Ïw
x 2 5 x for x . 1
definition.
dx
}} 5 lim
x
c→01
21
dx
dx
1
E}
} 5 }}E }
x
4
x 14
}} 1 1
cos x
Thus f (2x) grows at the same rate as g(x) by
1
1
4
7. 21 # cos x # 1, so )cos x ) # 1.
f (2x)
f (x)
(b) lim }} 5 lim }} 5 L
x→` g(2x) x→2` g(x)
E
0
5. 9 2 x 2 . 0 for 23 , x , 3
The domain is (23, 3).
46. (a) lim }} 5 lim }} 5 `
2.
4 5 ln 6 2 ln 3 5 ln 2
x dx
1
}
} 5 }} ln )x 2 1 1)
2
x2 1 1
1
4
4.
f (2x)
3
5 }} 2 tan21 }} 1 C
Thus ) f ) grows at the same rate as )g) as x→` by
x→` g(2x)
2
Quick Review 8.3
f (x)
x→` g(x)
definition.
dx
}}p
x
1
(b) lim }} 5 lim }} 5 lim }} 5 L
x→` ) g(x))
c
4
Thus ) f) grows faster than )g) as x→` by definition.
) f(x))
1
x2p11 1
c→0 2p 1 1 c
1 2 c2p11
1
5 lim1 }} 5 }}
2p 1 1
12p
c→0
as h→0, so )ES) 5 O(h 4). Thus as h→0, ES→0.
b2a
12
E
5 lim1 }}
4
(c) From Section 5.6, we know that )ET) # }} h 2M
2
4. If 0 , p , 1, then
)ES)
M
M
[a, b]. Thus, }}
# (b 2 a)}} # int (b 2 a)}} 1 1
h4
180
180
3
dx
}}p
x
4
f (x)
g(x)
3
c
5 lim1 }}
positive integer M for which }} # M for x sufficiently
where M is a bound for the absolute value of f
1
x2p11 1
2
p11 c
c→0
1 2 c2p11
5 lim1 }} 5 ` because (2p 1 1) , 0.
2p 1 1
c→0
containing a. Then f 5 O(g) as x→a if there is a
(4)
E
E
1
c
3 4
dx
1
}} 5 lim ln x 5 lim (2ln c) 5 `
x
c c→01
c→01
1
1
}} $ }}
x
2w1
x 2w
Ïw
f (x)
x→` g(x)
4e x 2 5
x→` 3e 1 7
4e x
x→` 3e
4
4
3
9. lim }} 5 lim }
x } 5 lim }}
x 5 lim }} 5 }}
x→` 3
Thus f and g grow at the same rate as x→`.
Ï2wxw2
ww1
f (x)
10. lim }} 5 lim }}
x→` g(x)
x→` Ïx
w1
ww3
2x 2 1
5 lim
!}
§x§1§}
§3§
5 lim
!§
x→`
1
x→`
2 2 }}
x
w
} 5 Ï2
3
1 1 }}
x
Section 8.3
Section 8.3 Exercises
1. (a) The integral is improper because of an infinite limit of
integration.
E
4. (a) The integral is improper because of two infinite limits
of integration.
b
dx
}
} 5 lim
x 2 1 1 b→`
0
2
0
b
21
b→`
E
E
`
(b)
dx
E}
}
x 11
5 lim 3tan x4
`
(b)
2`
0
2`
E
`
5 lim
0
b→2`
E
32(x
2
0
4
1 1)21
b
5 lim [21 1 (b 2 1 1)21] 5 21
b→`
p
2
E
5 }}
`
0
The integral converges.
b→2`
2x dx
E}
}
(x 1 1)
5 lim 3(2x 1 1) 4
2x dx
}
} 5 lim
(x 2 1 1)2
b→`
b
2
0
2
21
2
b→`
p
(c) }}
2
b
0
5 lim [2(b2 1 1)21 1 1] 5 1
E
`
2. (a) The integral is improper because the integrand has an
infinite discontinuity at x 5 0.
E
1
0
E
1
dx
}} 5 lim
Ïxw b→01
b
dx
}}
Ïwx
3 4
b→0
2`
b→`
2x dx
}
} 5 21 1 1 5 0
(x 2 1 1)2
The integral converges.
5 lim1 2Ïxw
(c) 0
5. (a) The integral is improper because the integrand has an
infinite discontinuity at 0.
1
b
E
ln 2
5 lim1 (2 2 2Ïbw) 5 2
(b)
b→0
0
E x
5 lim 2e
3 4
x22 e1/x dx 5 lim1
b→0
ln 2
22 1/x
b
1/x
The integral converges.
b→01
e
dx
ln 2
b
5 lim1 [2e1/ln 2 1 e1/b] 5 `
(c) 2
b→0
3. (a) The integral involves improper integrals because the
integrand has an infinite discontinuity at x 5 0.
E
E
1
(b)
E
0
2x dx
2x dx
2x dx
}
}5
}
}
2 }
2 1
2 }
2
(x2 1 1)2
2` (x 1 1)
0 (x 1 1)
0
2x dx
2x dx
}
} 5 lim
}}
(x 2 1 1)2 b→2` b (x 2 1 1)2
5 lim (tan21 b 2 0)
(b)
335
28
0
28
dx
5
}1}
x /3
E
0
28
dx
1
}1}
x /3
dx
5 lim
}1}
x /3 b→02
E
b
28
E
1
0
The integral diverges.
(c) No value
dx
}1}
x /3
dx
}1}
x /3
6. (a) The integral is improper because the integrand has an
infinite discontinuity at x 5 0.
b
32 4
3
5 lim 1}}b 2 62 5 26
2
dx
E }x } 5 lim E }xd}x
3
5 lim2 }}x 2/3
b→0
E
p/2
(b)
0
E cot u du
cos u du
5 lim E }}
sin u
5 lim 3ln )sin u)4
cot u du 5 lim1
b→0
28
b→02
0
b→0
1
1/3
b→01 b
3
The integral diverges.
b
(c) No value
2/3
b→0
3
2
E
1
28
3
9
dx
5 26 1 }} 5 2}}
}1}
2
2
x /3
The integral converges.
9
2
(c) 2}}
E
`
1
5 }}
b
b→0
1
32 4
3
3
5 lim 1}} 2 }}b 2
2
2
b→0
p/2
1
5 lim1 (0 2 ln )sin b)) 5 `
1/3
5 lim1 }}x 2/3
b
p/2
b→01 b
2/3
1
p/2
7.
1
x
E }x d}
5 lim 321000 x
dx
}
} 5 lim
x1.001
b→`
b→`
b
1
1.001
20.001
b
4
1
5 lim (21000b20.001 1 1000) 5 1000
b→`
336
Section 8.3
E
E
1
8.
21
0
21
dx
5
}2}
x /3
E
0
dx
1
}2}
x /3
21
dx
5 lim
}2}
x /3 b→02
E
b
21
E
1
0
E
22
dx
}2}
x /3
13.
2`
2 dx
}
} 5 lim
x 2 2 1 b→2`
dx
}2}
x /3
E
b
b→0
dx
5 lim1
}2}
x /3
b→0
E
1
b
21
b→2`
b→2`
5 lim
1
3 4
b→0
b→2`
b
b→0
E
1
21
9.
E
0
E
`
dx
531356
}2}
x /3
14.
2
3[t 2 (t 2 1)] dt
E }}
t(t 2 1)
3
3
5 lim E 1}} 2 }}2 dt
t
t21
5 lim 33 ln )t 2 1) 2 3 ln )t)4
t21
5 lim 33 ln )}})4
t
b21
1
5 lim 13 ln )}}) 2 3 ln }}2
b
2
dr
E}
}
2wr
Ï4ww
5 lim 322Ï4ww
2wr4
0
`
b
0
b→`
5 lim2 (22Ï4ww
2wb 1 4) 5 4
1
0
E }r d}r
5 lim 31000r
4
dr
}
} 5 lim
r0.999 b→01
0.999
1
0.001
b→0
b→`
1
b
1
5 3 ln 1 1 3 ln 2 5 3 ln 2
b→0
11.
E
0
dx
}} 5 lim
2wx 2w b→12
Ïw1w
E
0
3
15.
0
dx
}}
2wx 2w
Ïw1w
4
5 lim2 sin21 x
b→1
E
1
b
u11
}} 5 lim
u 2ww
1w2u
Ïw
w b→01
b→0
E
2`
2 dx
}
} 5 lim
x 2 1 4 b→2`
5 lim
b→2`
5 lim
b→2`
p
4
E
b
(1/2) dx
}2}
(x/2) 1 1
2
3
4
p
b
1}4} 2 tan }2}2
x
2
tan21 }}
b
21
p
2
3p
4
5 }} 1 }} 5 }}
1 (2u 1 2) du
}}}}
2 Ïu
w2w1
ww2wu
3
1
4
b
b→0
E
s
1
E 1}
} 1 }} ds
2ws w
2ws w 2
Ï4ww
Ï4ww
s
1
lim E 1}} 1 }}2 ds
2ws w
2Ï1
2w(s/
)
Ï4ww
ww
w2ww
s
5 lim 32Ï4ww
2ws w 1 sin }}4
2
b
5 lim 12Ï4ww
2w
b w 1 sin }} 1 22
2
2
12.
b
5 lim1 (Ï3w 2 Ïbww1
ww2bw) 5 Ï3w
p
2
2
1
2
0
5 lim2 (sin21 b 2 0) 5 }}
2
E
5 lim1 Ïuw2w1
ww2uw
b
b→1
2
b→`
b
5 lim1 (1000 2 1000b0.001) 5 1000
1
2
b
b→4
E
2
b→` 2
b
2
`
3 dt
}
} 5 lim
t 2 2 t b→`
b
dr
}} 5 lim
2wr b→42
Ïw4w
b→4
10.
b
5 ln 3 2 ln 1 5 ln 3
5 lim1 (3 2 3b1/3) 5 3
4
b
22
5 lim
dx
}2}
x /3
5 lim1 3x1/3
22
5 lim
5 lim2 (3b1/3 1 3) 5 3
1
b
b→2` b
3 4
b→0
22
22
5 lim
b
5 lim2 3x1/3
[(x 1 1) 2 (x 2 1)] dx
E }}}
(x 1 1)(x 2 1)
1
1
E 1}
} 2 }} dx
x21
x 1 12
3ln )x 2 1) 2 ln )x 1 1)4
x21
}
3ln )}
x 1 1 )4
b21
}
1ln 3 2 ln )}
b 1 1 )2
16.
0
s11
}} ds 5 lim
b→22
2ws 2w
Ïw4w
b
2
0
b
b→22 0
2
2
2
21
b→22
b
0
2
b→22
p
2
5 sin21 1 1 2 5 }} 1 2
21
2
Section 8.3
17. First integrate
dx
E}
} by letting
(1 1 x)Ïxw
E
`
20.
21
(u 1 3) 2 (u 1 2)
E }}
du
(u 1 3)(u 1 2)
1
1
5 lim E 1}} 2 }}2 du
u12
u13
5 lim 3ln )u 1 2) 2 ln )u 1 3)4
u12
b
5 lim 3ln )}})4
u 1 3 21
b12
1
5 lim 1ln )}}) 2 ln }}2 5 ln 2
b13
2
du
}
} 5 lim
u 2 1 5u 1 6 b→`
21
b
1
u 5 Ïxw, so du 5 }} dx.
2Ïwx
dx
2 du
}} 5 }}2
11u
(1 1 x)Ïwx
E
b
b→` 21
E
b
b→`
5 2 tan21 u 1 C
21
b→`
5 2 tan21 Ïxw 1 C
b→`
Now evaluate the improper integral. Note that the integrand
is infinite at x 5 0.
dx
dx
dx
E}
} 5 E }} 1 E }}
(1 1 x)Ïxw
(1 1 x)Ïxw
(1 1 x)Ïxw
dx
dx
5 lim E }} 1 lim E }}
(1 1 x)Ïxw
(1 1 x)Ïxw
`
0
3
21
21
5 lim1 (2 tan
b→0
21
lim (2 tan
1
p
2
16 tan x
E }}
dx 5 E16u du 5 8u
11x
21
c→` 1
5 lim1 2 tan
c→`
dx
11x
c
b→01 b
1
4b
3
21
Ïxw 1 lim 2 tan
c→`
21
Ïcw 2 2 tan
p
2
2 1
4
18.
E
E
1
2
1
dx
}} 5
2w
xÏw
x 2w
1
E
2
1
E
`
1)
16 tan21 x
dx 5 lim
}}
1 1 x2
b→`
0
E
b
E
`
2
3
4
5 lim1 (sec
b→1
2
E
4
22.
2 2 sec21 b)
21
E
0
21
p
3
dx
}} 5
Ï)x
w)w
E
2
dx
}} 5 lim
b→`
2w
xÏw
x 2w
1
E
b
2
3
5 lim sec
b→`
4
E
4
2)
0
dx
}}
Ïxw
`
1
E
2
19.
1
E
2
b
21
2
4
5 lim1 (sec
b→1
E
4
21
b→0
b→0
ds
}}
2w1
sÏw
s 2w
3
0
dx
}}
Ïwx
dx
}}
Ï2
wwx
3
4
b
21
E
4
b
dx
}}
Ïwx
3 4
1
4
b
2
5 lim1 4 2 2Ïbw 5 4
5 lim1 sec21 s
b→1
5 lim1
b→0
p
p
p
dx
}} 5 }} 1 }} 5 }}
3
6
2
2w
xÏw
x 2w
1
ds
}} 5 lim
2w1 b→11
sÏw
s 2w
21
5 lim1 2Ïxw
p
p
p
5 }} 2 }} 5 }}
2
3
6
E
b
4
b→0
x
b 2 sec
b→`
E
E
5 lim2 (22Ï2
wbw 1 2) 5 2
b
21
5 lim (sec
21
dx
}} 1
Ï2
wwx
b→0
2
21
0
2
5 lim2 22Ï2
wxw
dx
}}
2w1
xÏw
x 2w
21
E
dx
}} 5 lim
Ï2
wxw b→02
5 sec21 2 2 sec21 1 5 }}
`
2
b→`
2
b
b
0
21
dx
}}
2w1
xÏw
x 2w
dx
}}
2w1
x Ïw
x 2w
21
0
16 tan21 x
dx
}}
1 1 x2
b→`
5 lim1 sec21 x
b→1
b
3
4
5 lim 38(tan b) 2 04
p
5 81}}2 5 2p
2
2
2
E
5 lim 8 (tan21 x)2
dx
}} 1
2w1
xÏw
x 2w
dx
}} 5 lim
b→11
2w1
xÏw
x 2w
1C
5 8(tan21 x)2 1 C
1
5 }} 2 0 1 p 2 }} 5 p
`
2
2
c
Ïbw) 1
1 2 2 tan
21
Ïxw
x
du 5 }}2 .
1
1
b→0
21
`
1
0
E 161tan1 x
21. Integrate }}
dx by letting u 5 tan21 x, so
2
b
2 2 sec21 b)
p
3
5 sec21 2 2 sec21 1 5 }}
dx
}} 5 2 1 4 5 6
Ï)x
w)w
337
338
Section 8.3
E
25.
dv 5 eu du
u5u
u
0
0
2`
u
2 eu 1 C
b→2`
E
e2x dx 5 lim
u
4
2 eu
E
2`
b
c→`
c→`
1
5 lim 2}}c 5 0 and lim e b 5 lim e2c 5 0.
e
c→`
b→2`
c→`
u 5 2 sin u
dv 5 e2u du
du 5 2 cos u du
v 5 2e2u
dv 5 e
du 5 22 sin u du
v 5 2e2u
2
b→0
b→0
5 lim1
du
1Note that lim
b→01
2e
E
p/2
sin u du
27.
E
0
2 2e2u sin u du 5 22e2u sin u 2 2e2u cos u 1 C1
0
E 2e
5 lim 2e
3
b→` 0
2u
b→`
2b
5 lim (2e
b→`
4
1
4
2
1
b
1
4
2
ln b 1 }}b 2
b2
2
b→0
4
sin u 2 e2u cos u
2b
sin b 2 e
b
0
cos b 1 1) 5 1
b→0
1/b
22/b
2
tan u du 5 lim
E
5 lim
3
b
sin u
}} du
b→p/2 0 cos u
b→p/2
2ln )cos u)
b
4
0
5 lim [2ln )cos b) 1 0] 5 `
The integral diverges.
sin u du
ln b
1/b
b 2 ln b 5 lim1 }}2 5 lim1 }}3
b→p/2
sin u du 5 2e2u sin u 2 e2u cos u 1 C
sin u du 5 lim
32
1
1
12}4} 2 }2}b
5 lim1 2}} 5 0.
5 22e2u sin u 2 2e2u cos u 2 2e2u sin u du
E
1
4
ln x 2 }}x 2 1 C
1
4
E
2u
2
5 2}}
cos u du 5 22e2u cos u 2 2e2u sin u du
b
0
b
1
b→0
2u
4
b
1
1
5 lim1 }}x 2 ln x 2 }}x 2
Thus,
`
b→`
Ex ln x dx 5 }12}x ln x 2 E}12}x dx 5 }12}x
E x ln x 5 lim E x ln x dx
E
u 5 2 cos u
2u
3
e2x dx 5 lim 2e2x
(1 2 eb) 5 1
1
2
b→0
E
E2e
b→−`
b
v 5 }}x 2
1
E
2u
3 4 5 lim
dv 5 x dx
1
x
Integrate 2e2u cos u du by parts.
E2e
b
du 5 }} dx
sin u du 5 22e2u sin u 1 2e2u cos u du
2u
b→−`
0
ex
e2)x) dx 5 1 1 1 5 2
0
E2e
e x dx 5 lim
E
u 5 ln x
2
E
2u
0
e2x dx
0
E
24. Integrate 2e2u sin u du by parts.
2u
E
`
26. Integrate x ln x dx by parts.
c
e
Note that lim be b 5 lim 2ce2c 5 lim 2}}c
E2e
2`
E
b→`
`
0
b→2`
b→2`
e x dx 1
5 lim (2e2b 1 1) 5 1
5 lim (21 2 be b 1 e b ) 5 21
1
0
b→−` b
u
3ue
E
b→` 0
0
b→2` b
5 lim
e x dx 5 lim
`
u
u
E
2`
2`
Eue du 5 ue 2 Ee du 5 ue
E ue du 5 lim E ue du
u
e2)x) dx 5
0
v 5 eu
du 5 du
E
`
23. Integrate ueu du by parts.
Section 8.3
sin u
1
1
28. On [0, p], 0 # }} # }}, so
pw
2wu
2w
Ïw
Ïp
ww
u
E
E
p
0
p
0
E
p
sin u
}} du #
pw
2w
u
Ïw
0
1
}} du 5 lim
b→p2
2wu
Ïw
pw
E
b
E }Ïdx}wx 5 lim E
`
4
3
b→p
b
3 4 5 lim [2Ïbw 2 4] 5 `
dx
}} 5 lim 2Ïxw
Ïwx b→`
b→` 4
4
b→`
b
4
5 lim2 22Ïp
ww
2wu
b
Since this integral diverges, the given integral diverges.
1
}} du
2wu
Ïw
pw
0
1
32. 0 # }} # }} on [4, `)
Ïwx
Ïxw 2 1
1
}} du
2w
Ïw
pw
u
339
1
x 11
1
x
33. 0 # }
3 } # }}
3 on [1, `)
0
E
`
5 lim2 (22Ïp
ww
2wb 1 2Ïp
w)
b→p
1
E
b
dx
}}3 5 lim
x
b→`
1
dx
}}3
x
b
3 2 4
1
1
1
5 lim 32}}b 1 }}4 5 }}
2
2
2
5 22Ï0w 1 2Ïp
w
1
5 lim 2}}x22
b→`
5 2Ïp
w
1
22
b→`
Since this integral converges, the given integral converges.
E
E
`
29.
2
2`
`
0
E
2xe2x dx 5
`
2xe2x dx 1
2
0
E
b
2xe2x dx 5 lim
2
b→` 0
3
2
E
2`
2xe
2x 2
2
E
E
2
34.
0
1
b
4
0
E
1 1] 5 1
2x 2
2xe
dx
32e 4
0
E
4
b
1/2[(1 2 x) 1 (1 1 x)]
E }}}
dx
(1 2 x)(1 1 x)
1
1
5 lim E 3}} 1 }}4 dx
2(1 1 x)
2(1 2 x)
1
1
5 lim 3}} ln )1 1 x) 2 }} ln )1 2 x)4
2
2
1
11x
5 lim 3}} ln )}})4
2
12x
1
11b
5 lim 3}} ln )}}) 2 04 5 `
2
12b
b
dx
}}2 5 lim
12x
b→12
0
2
0
0
0
Since this integral diverges, the given integral diverges.
e2Ïxw
}} dx
Ïwx
3
4
5 lim1 22e2Ïxw
b→0
dx
}}2
12x
b→12
The integral converges.
e2Ïxw
}} dx 5 lim
b→01
Ïwx
1
b→12
b
b→2`
4
2
b
2
E
0
E
dx
}}2 1
12x
b→12
5 lim [21 1 e2b ] 5 21
30.
1
b→1
0
2x 2
b→2`
E
b
b→2` b
5 lim
dx
}}2 5
12x
b
0
dx 5 lim
2xe2x dx
0
5 lim [2e
b→`
2`
2
2b 2
0
0
2xe2x dx
5 lim 2e2x
b→`
E
Since this integral converges, the given integral converges.
4
E
E
2
35.
0
1
b
5 lim1 [22e22 1 2e2Ïbw]
b→0
5 22e22 1 2
0
dx
}} 5
12x
E
1
0
dx
}} 1
12x
dx
}} 5 lim
1 2 x b→12
E
b
0
3
E
2
1
dx
}}
12x
dx
}}
12x
4
5 lim2 2ln )1 2 x)
b→1
b
0
5 lim2 (2ln )1 2 b) 1 0) 5 `
b→1
The integral converges.
1
1
31. 0 # }} # }} on (0, p] since sin t $ 0 on [0, p].
Ïtw 1 sin t
Ïtw
E
p
0
dt
}} 5 lim
Ïtw b→01
E
p
b
dt
}}
Ïwt
3 4
5 lim1 2Ïtw
b→0
p
b
5 lim1 [2Ïp
w 2 2Ïbw]
b→0
w
5 2Ïp
Since this integral converges, the given integral converges.
Since this integral diverges, the given integral diverges.
340
Section 8.3
E
E ln x dx by symmetry of ln )x) about the
y-axis. Integrate Eln x dx by parts.
1
36.
ln )x) dx 5 2
21
0
E
E
`
1
40.
0
`
1
u 5 ln x
E
1
x
b→`
1
5 lim (2Ïbw 2 2) 5 `
b→`
Eln x dx 5 x ln x 2 Edx 5 x ln x 2 x 1 C
2E ln x dx 5 2 lim E ln x dx
5 2 lim x ln x 2 x
3
4
Since this integral diverges, the given integral diverges.
1
b→01 b
0
b
3 4
5 lim 2Ïxw
v5x
1
`
E
dv 5 dx
du 5 }} dx
E
1
dx
dx
dx
}} 5
}} 1
}}
0 Ïw
1 Ïw
x
x
Ïxw
b
dx
dx
}} 5 lim
}}
Ïxw b→` 1 Ïxw
E
`
1
b→01
1
2 1 cos x
x
x
b
dx
dx
}} 5 lim
}} 5 lim ln x
x
x
p
b→`
b→`
41. 0 # }} # }} on [p, `)
p
b
5 2 lim1 [21 2 b ln b 1 b] 5 22
E
3 4
b
5 lim (ln b 2 ln p) 5 `
p
b→`
Since this integral diverges, the given integral diverges.
b→0
1
ln b
1/b
1/b
Note that lim1 b ln b 5 lim1 }} 5 lim1 }}2
b→0
5 lim1 2b 5 0.
b→0
b→0
2
b→0 21/b
E
`
p
The integral converges.
1
1
11e
e
1
}}u du 5 lim
e
b→`
1 1 sin x
x
2 dx
5 lim
}}
x2
b→`
`
1
E
b
b→`
Since this integral converges, the given integral converges.
4
1
1
e
Since this integral converges, the given integral converges.
1
38. 0 # }} # }} on [2, `)
x
2w1
Ïxw2w
2
dx
}} 5 lim
x
b→`
E
b
2
1
e 1e
1
1
ex
}
}5}
} 5 }}
e x 1 e2x
e2x(e2x 1 1)
1 1 (e x)2
e x dx
Integrate }}
by letting u 5 e x so du 5 e x dx.
1 1 (e x)2
dx
e x dx
5 }}
}
x }
2x
e 1e
1 1 (e x)2
du
5 }}2
11u
43. First rewrite }
x }
2x .
5 }}
`
p
b→`
b
b→`
E
b
21
5 lim [2e2b 1 e21]
1
2x22 dx
p
b→`
e2u du
3
b
3 4
2
2
5 lim 122b 1 }}2 5 }}
p
p
1
5 lim 2e2u
E
5 lim 22x21
37. 0 # }}u # }}u on [1, `)
E
2
x
42. 0 # }}
# }}2 on [p, `)
2
3 4
dx
}} 5 lim ln x
x
b→`
b
2
5 lim (ln b 2 ln 2) 5 `
E
E
b→`
E
E
5 tan21 u 1 C
Since this integral diverges, the given integral diverges.
5 tan21 e x 1 C
Ïxw1
ww1
1
and g(x) 5 }3}
39. Let f (x) 5 }}
2
/2 . Both are continuous on
x
x
[1, `).
E
1
`
2`
0
2`
Ïxw1
ww1
f (x)
lim }} 5 lim }} 5 lim
x→` g(x)
x→`
x→`
Ïxw
`
E
E
1
dx 5 lim
}3}
x /2
b→`
E
b
x
23/2
1
21/2
1 2) 5 2
Since this integral converges, the given integral converges.
`
E
b→2`
3tan
21
21
5 lim [tan
b→2`
b
4
E
0
5 lim
dx
3
5 lim (22b
b→`
1
1
5 lim 22x21/2
b→`
!1§§1§}x}§ 5 1
E
dx
dx
dx
}
}5
}
}
x }
2x 1
x }
2x
e x 1 e2x
2` e 1 e
0 e 1e
0
dx
dx
}
} 5 lim
}}
e x 1 e2x b→2` b e x 1 e2x
p
4
4
ex
0
b
1 2 tan21 e b]
p
4
dx
}
}
e x 1 e2x
5 }} 2 0 5 }}
E
`
0
dx
}
} 5 lim
e x 1 e2x
b→`
E
b
0
3
4
5 lim tan21 e x
b→`
21
5 lim [tan
b→`
p
2
p
4
b
0
e 2 tan21 1]
b
p
4
5 }} 2 }} 5 }}
Thus, the given integral converges.
Section 8.3
E
`
44.
2`
E
`
0
E
1
0
dx
}} 5 2
1w1
x 4w
Ïw
dx
}} 5
1w1
x 4w
Ïw
E
`
0
E
1
dx
}} by symmetry about the y-axis
1w1
x 4w
Ïw
dx
}} 1
1w1
x 4w
Ïw
0
E
`
1
dx
}}
1w1
x 4w
Ïw
1
dx
}} exists because }} exists on [0, 1].
1w1
1w1
x 4w
x 4w
Ïw
Ïw
1
1
0 # }} # }}2 on [1, `).
x
1w1
x 4w
Ïw
E
`
1
1
}}2 dx 5 lim
x
b→`
E
b
b→`
3
y)
E 1 d1u u
5 }}
dy
5 lim
}}}
(1 1 y 2)(1 1 tan21 y) b→`
b→`
E
b
0
3
4
1
b
0
b) 2 0)
2
2`
E
2`
e dy
}
}1
y2 1 1
E
0
b→`
ln b
b
4
1
b
1/b
48. For x $ 0, y $ 0 on [1, `).
E }lnx}x dx 5 lim E }lnx}x dx
ln x
dx
Integrate E}} dx by letting u 5 ln x so du 5 }}.
x
x
ln x
1
1
E}x} dx 5 Eu du 5 }2}u 1 C 5 }2}(ln x) 1 C
1
1
Area 5 lim }}(ln x) 5 lim }}(ln b) 5 `
32 4
2
Area 5
`
b
b→` 1
1
e dy
}
}
y2 1 1
ey
2
y→` y
2
b→`
1
Area 5
E
`
1
dx
}}
x
(b) Refer to Exploration 2 of Section 7.3.
1
x
y9 5 2}}2
The surface area of the solid is given by the following
integral.
`
2
2
4
4
1
`
4
3
1
Ïw
1
x 4w
1w
1
Since 0 # }} # }}
on [1, `), the direct
x
x3
ey
y→` 2
lim }
2 } 5 lim }
2 } 5 lim }} 5 lim }} 5 `
Thus the given integral diverges.
2
b
1
2y
e dy
}
} diverges since
y2 1 1
ey
11
y
y→`
3
5 lim 2}} 2 }} 1 1 5 1
1
`
2y
e2y
y
11
y→2`
b
x 11
E 2p1}1x}2 !1§§1§12§}§x1}§2§ dx 5 2p E }1x} !}
§§x§}§ dx
Ïw
x w
1w
1
5 2p E }} dx
x
The integral converges.
e dy
}
}5
y2 1 1
4
49. (a) The integral in Example 1 gives the area of region R.
p
5 ln 1 1 }}
2
2`
0
1
x
b→`
b→`
dy
}}}
(1 1 y 2)(1 1 tan21 y)
b→`
E
E
ln x
x
2
5 lim (ln )1 1 tan
`
3
2
21
2y
2
ln b
5 lim ln )1 1 tan21 y)
46.
1
x
v 5 2}}
b→`
5 ln )1 1 tan21 y) 1 C
0
dv 5 }}2
1Note that lim }b} 5 lim }1} 5 0.2
5 ln )1 1 u) 1 C
2y
dx
x
u 5 ln x
b→`
4
E (1 1 y )(1dy1 tan
`
2
Area 5 lim 2}} 2 }}
45. Integrate }}}
by letting u 5 tan21 y so
2
21
0
ln x
dx
}}
x2
b→` 1
2
Since this integral converges, the given integral converges.
E
1
1
3
`
b
2
E}lnx}x 5 2}lnx}x 1 E}dx}x 5 2}lnx}x 2 }1x} 1 C
1
5 lim 2}} 1 1 5 1
b
b→`
E
`
b
4
dy
du 5 }}2
11y
dy
}}}
(1 1 y 2)(1 1 tan21 y)
E }lnx}x dx 5 lim E
ln x
Integrate E}} dx by parts.
x
Area 5
1
x
x22 dx
5 lim 2x21
47. For x $ 0, y $ 0 on [1, `).
du 5 }} dx
1
341
comparison test shows that the integral for the surface
area diverges. The surface area is `.
(c) Volume 5
E p1}1x}2
`
1
2
dx 5 p
E
`
1
1
}}2 dx
x
5 p lim
E
b
1
}} dx
2
b→` 1 x
b
3 x4
1
5 p lim 12}} 1 12 5 p
b
1
5 p lim 2}}
b→`
1
b→`
(d) Gabriel’s horn has finite volume so it could only hold a
finite amount of paint, but it has infinite surface area so
it would require an infinite amount of paint to cover
itself.
342
Section 8.3
1
50. (a) f (x) 5 }} e2x
Ïw2p
w
51. (a) For x $ 6, x 2 $ 6x, so e2x # e26x
2
2/2
E
`
6
e2x dx #
2
E
`
e26x dx
6
5 lim
E
b
e26x dx
b→` 6
1
b→`
f is increasing on (2`, 0]. f is decreasing on [0, `).
f has a
1
2
2
2
26b
E
1
6
1
make
E
f (x) dx and
b
E
E
E
E
`
b
`
b
f (x) dx ,
E
`
(c)
b
1
E
`
(d)
0
2x/2
2
2
E
#E
3
E
dx 1 E
e2x dx 1
2
0
e2x
2
`
e2x dx
2
3
`
e23x dx
3
since x 2 $ 3x for x . 3.
E
`
3
c
e23x dx
b
3
4
1
1
5 lim 12}}e
1 }}e 2
3
3
1
3
3
23b
E
29
b→`
`
1
3
5 }}e29 < 0.000041 , 0.000042
f (x) dx
b
is as small as we want. Likewise, for large enough b,
f (x) dx is as small as we want.
b→` 3
b→`
5 2e
2b
b
5 lim 2}} e23x
b
As b→`, 2e2b/2→0, so for large enough b,
E
e23x dx 5 lim
c→`
2b/2
2`
2
2
e2x dx 5
5 lim [22e2c/2 1 2e2b/2]
E
e2x dx
6
2
0
2x/2
c→` b
c→`
`
e2x dx 1 4 3 10217
3
E e dx
5 lim 22e
3
4
c
1
6
E
f (x) dx as small as we want
e2x/2 dx
e2x/2 dx 5 lim
2
e2x dx < NINT(e2x , x, 1, 6) < 0.1394027926
for x , 21) Thus,
`
e2x dx 1
(This agrees with Figure 8.16.)
0 , f (x) , e2x/2 for x . 1. (Likewise,
0 , f (x) , e
6
bounded by 4 3 10217.
f (x) dx as close to 1 as
by choosing b large enough. This is because
x/2
2
Thus, from part (a) we have shown that the error is
2b
2`
E
#E
e2x dx 5
1
we want by choosing b . 1 large enough. Also, we can
`
E
`
(b)
b
2b
236
5 }}e236 , 4 3 10217
(c) Part (b) suggests that as b increases, the integral
approaches 1. We can make
6
b→`
2
1
local maximum at (0, f (0)) 5 0, }}
Ïw2w
p
1
2x 2/2
, x, 21, 1 < 0.683
}} e
Ïw2w
p
2
1
}} e2x /2, x, 22, 2 < 0.954
Ïw2w
p
2
1
}} e2x /2, x, 23, 3 < 0.997
Ï2ww
p
1
NINT1
NINT 1
(b) NINT
b
3 6 4
1
1
5 lim 12}} e
1 }} e 2
6
6
5 lim 2}}e26x
[23, 3] by [0, 0.5]
52. (a) Since f is even, f (2x) 5 f (x). Let u 5 2x, du 5 2dx.
E
`
2`
E f (x) dx 1 E f (x) dx
5 E f (2u)(21) du 1 E f (x) dx
5 E f (u) du 1 E f (x) dx
5 2E f (x) dx
f (x) dx 5
`
0
2`
0
0
`
`
`
0
`
0
0
`
0
(b) Since f is odd, f (2x) 5 2f (x). Let u 5 2x, du 5 2dx
E
`
2`
E
5E
f (x) dx 5
0
2`
0
`
52
f (x) dx 1
E
0
f (x) dx
`
f (2u)(21) du 1
E
`
0
f (u) du 1
E
`
0
E
`
f (x) dx
0
f (x) dx 5 0
343
Section 8.3
E
`
53. (a)
0
2x dx
E}
}
x 11
5 lim 3ln (x 1 1)4
2x dx
}
} 5 lim
x 2 1 1 b→`
55. Suppose 0 # f (x) # g(x) for all x $ a.
b
0
2
2
b→`
From the properties of integrals, for any b . a,
b
E
b
0
5 lim ln (b 2 1 1) 5 `
a
b→`
Thus the integral diverges.
E
E
`
0
2x dx
2x dx
}
}
2 } and
2 } must converge in order
0 x 11
2` x 1 1
`
2x dx
for
}
2 } to converge.
2` x 1 1
(b) Both
E
(c) lim
E
b
b→` 2b
3
2x dx
}
} 5 lim ln (x 2 1 1)
x 2 1 1 b→`
4
b
5 lim [ln (b 1 1) 2 ln (b 1 1)]
2
b→`
E
b
2x
x 11
b
g(x) dx.
a
If the infinite integral of g converges, then taking the limit
in the above inequality as b→` shows that the infinite integral of f is bounded above by the infinite integral of g.
Therefore, the infinite integral of f must be finite and it converges. If the infinite integral of f diverges, it must grow to
infinity. So taking the limit in the above inequality as b→`
shows that the infinite integral of g must also diverge to
infinity.
E
`
e2x dx
0
5 lim 0 5 0.
Note that }
2 } is an odd function so
E
56. (a) For n 5 0:
2b
2
b→`
f (x) #
2b
E e dx
5 lim 2e
3 4
5 lim
b
2x
b→` 0
2x
b→`
2x dx
}
} = 0.
x2 1 1
(d) Because the determination of convergence is not made
using the method in part (c). In order for the integral to
converge, there must be finite areas in both directions
(toward ` and toward 2`). In this case, there are
infinite areas in both directions, but when one
computes the integral over an interval [2b, b], there is
cancellation which gives 0 as the result.
b
0
5 lim [2e2b 1 1] 5 1
For n 5 1:
u5x
du 5 dx
E
`
0
b→`
dv 5 e2x dx
v 5 2e2x
xe2x dx 5 lim
E
b
b→` 0
13 4 1 E e dx2
b
5 lim 12}}2 1 lim E e dx
e
1
5 lim 12}}2 1 1 5 1
e
2xe2x
= lim
b→`
54. By symmetry, find the perimeter of one side, say for
xe2x dx
b
b
2x
0
0
b
0 # x # 1, y $ 0.
y 2/3 5 1 2 x 2/3
For n 5 2:
u 5 x2
du 5 2x dx
y 5 (1 2 x 2/3)3/2
1
2
dy
3
2
}} 5 }}(1 2 x 2/3)1/2 2}}x21/3 5 2x21/3(1 2 x 2/3)1/2
dx
2
3
dy 2
1}d}x 2
5 x22/3(1 2 x 2/3) 5 (x22/3 2 1)
x ww 5 x
!1§§1§1}§d}§x 2§ 5 Ïw
E x dx 5 lim E x dx
dy 2
1
0
22/3
1
21/3
21/3
21/3
b→01 b
1
3 4
3
3
3
5 lim 3}} 2 }}b 4 5 }}
2
2
2
3
Thus, the perimeter is 41}}2 5 6.
2
5 lim1
b→0
3
}}x 2/3
2
b
2/3
b→01
E
`
0
b→`
b
b→`
b
2x
b→` 0
dv 5 e2x dx
v 5 2e2x
x 2 e2x dx 5 lim
E
b
b→` 0
x 2 e2x dx
132x e 4 1 E 2x e
b
5 lim 12}}2 1 2 lim E xe
e
2b
5 lim 12}}2 1 2(1)
e
2
5 lim 12}}2 1 2 5 2
e
2 2x
5 lim
b→`
b
0
2
b→`
b
b→`
b
b→`
b
b
2x
dx
0
b
b→` 0
2x
dx
2
344
Section 8.4
56. continued
E
(b) Evaluate x e
u 5 xn
du 5 nx n21
Ex
n 2x
e
dx using integration by parts
dv 5 e2x dx
v 5 2e2x
dx 5 2x e
E
`
1 nx
n21 2x
e
`
b
nx
n21 2x
e
dx
0
0
`
n
1 2
b
n21 2x
e
dx
0
2
(c) Since f (n 1 1) 5 nf (n),
f (n 1 1) 5 n(n 2 1) … f (1) 5 n!; thus
0
x ne2x dx converges for all integers n $ 0.
1
sin x
x
2
57. (a) On a grapher, plot NINT }}, x, 0, x or create a table
of values. For large values of x, f (x) appears to
approach approximately 1.57.
(b) Yes, the integral appears to converge.
E
1
58. (a)
2`
dx
}}2 5 lim
1 1 x b→2`
5 lim
b→2`
E
1
b
dx
}}2
11x
3
tan21 x
5 lim (tan
b→2`
p
4
1
4
b
21
p
2
1 2 tan21 b)
3p
4
5 }} 1 }} 5 }}
E
`
1
dx
}}2 5 lim
11x
b→`
E
b
1
dx
}}2
11x
3
5 lim tan21 x
b→`
5 lim [tan
b→`
p
2
p
4
4
b 2 tan21 1]
p
4
5 }} 2 }} 5 }}
E
`
2`
b
1
21
3p
p
dx
}}2 5 }} 1 }} 5 p
4
4
11x
0
`
0
E
`
f (x) dx 1
f (x) dx
c
0
c
2`
0
0
`
2`
1Note: apply L’Hôpital’s Rule n times to show that
bn
e
2`
0
0
`
0
c
0
0
c
5 nf (n)
lim 2}}b 5 0.
c
E f (x) dx 1 E f (x) dx 1 E f (x) dx 1 E f (x) dx
5 E f (x) dx 1 E f (x) dx, because
E f (x) dx 1 E f (x) dx 5 E f (x) dx 2 E f (x) dx 5 0.
5
3
4 1E
b
5 lim 12}}2 1 nE x
e
b→`
0
c
c
x ne2x dx
b→`
`
c
E
dx
0
5 lim 2x e
E
2`
`
2`
n 2x
b→`
E f (x) dx 1 E f (x) dx
f (x) dx 5 E f (x) dx 1 E f (x) dx
f (x) dx 5
Thus,
E
n 2x
f (n 1 1) 5
E
E
c
(b)
n 2x
0
c
c
0
c
0
■ Section 8.4 Partial Fractions and Integral
Tables (pp. 444–453)
Quick Review 8.4
1. Solving the first equation for B yields B 5 23A 2 5.
Substitute into the second equation.
22A 1 3(23A 2 5) 5 7
22A 2 9A 2 15 5 7
211A 5 22
A 5 22
Substituting A 5 22 into B 5 23A 2 5 gives B 5 1. The
solution is A 5 22, B 5 1.
2. Solve by Gaussian elimination. Multiply first equation by
23 and add to second equation. Multiply first equation by
21 and add to third equation.
A 1 2B 2 C 5 0
27B 1 5C 5 1
2B 1 2C 5 4
Multiply third equation by 27 and add to second equation.
A 1 2B 2 C 5 0
29C 5 227
2B 1 2C 5 4
Solve the second equation for C to get C 5 3. Solve for B
by substituting C 5 3 into the third equation.
2B 1 2(3) 5 4
2B 5 22
B5 2
Solve for A by substituting B 5 2 and C 5 3 into the first
equation.
A 1 2(2) 2 3 5 0
A 1 15 0
A 5 21
The solution is A 5 21, B 5 2, C 5 3.
2x 1 1
x 3w
2w5w
x 2w
2w
1w0w
xw
2w
7
3. x 2 2 3x 2 4qw2w
3
2
2x
2
6x
2
8x
}}}}}}
x 2 2 2x 2 7
x 2 2 3x 2 4
}}}}}
x23
x23
x 2 3x 2 4
2x 1 1 1 }
}
2
Section 8.4
2. x 2 2 2x 1 15 (x 2 1)2
2
4. x 2 1 4x 1 5q2ww
x 2w
1w11wxw1
ww06w
2
2x
1 8x 1 10
}}}}}}
3x 2 04
2x 1 2
A
B
}
} 5 }} 1 }}2
x 2 2 2x 1 1 x 2 1
(x 2 1)
2x 1 25 A(x 2 1) 1 B
3x 2 4
x 1 4x 1 5
21}
}
2
5 Ax 1 (2A 1 B)
5. x 2 3x 1 x 2 3 5 x (x 2 3) 1 (x 2 3)
3
2
2
5 (x 2 3)(x 1 1)
2
6. y 2 5y 1 4 5 ( y 2 4)(y 2 1)
5 ( y 2 2)(y 1 2)(y 2 1)(y 1 1)
4
2
345
2
2
3(x 1 3)
2
3
2(x 2 2)
7. }} 2 }} 5 }} 2 }}
(x 2 2)(x 1 3)
x13
x22
(x 2 2)(x 1 3)
2x 2 4 2 3x 2 9
5 }}
(x 2 2)(x 1 3)
2x 2 13
5 }}
(x 2 2)(x 1 3)
x 1 13
5 2}
}
x2 1 x 2 6
x21
2
x 2 4x 1 5
x15
(x 2 1)(x 1 5)
2(x 2 2 4x 1 5)
5 }}}
2 }}}
(x 1 5)(x 2 2 4x 1 5)
(x 1 5)(x 2 2 4x 1 5)
x 2 1 4x 2 5 2 2x 2 1 8x 2 10
5 }}}}
(x 1 5)(x 2 2 4x 1 5)
2x2 1 12x 2 15
5 }}}
(x 1 5)(x 2 2 4x 1 5)
8. }
} 2 }}
2
(3t 1 4)(t 2 1 2)
(t 2 1)(t 2 1 1)
3t 1 4
t21
9. }
2 }}
}2}
} 5 }}
(t 2 1 2)(t 2 1 1)
(t 2 1 2)(t 2 1 1)
t2 1 1
t2 1 2
3
2
t 2 t 1 t 2 1 2 3t 3 2 4t 2 2 6t 2 8
5 }}}}
(t 2 1 2)(t 2 1 1)
22t 3 2 5t 2 2 5t 2 9
5 }}}
(t 2 1 2)(t 2 1 1)
2t 3 1 5t 2 1 5t 1 9
5 2}}
(t 2 1 2)(t 2 1 1)
2
3
1
x21
(x 2 1)
(x 2 1)
2(x 2 1)2
3(x 2 1)
1
5 }}
2 }}3 1 }}3
(x 2 1)3
(x 2 1)
(x 2 1)
2x 2 2 4x 1 2 2 3x 1 3 1 1
5 }}}
(x 2 1)3
2
2x 2 7x 1 6
5 }}
(x 2 1)3
10. }} 2 }}2 1 }}3
Section 8.4 Exercises
1. x 2 2 3x 1 25 (x 2 2)(x 2 1)
5x 2 7
A
B
}
} 5 }} 1 }}
x 2 2 3x 1 2 x 2 2
x21
5x 2 75 A(x 2 1) 1 B(x 2 2)
5 (A 1 B)x 2 (A 1 2B)
Equating coefficients of like terms gives
A 1 B 5 5 and A 1 2B 5 7.
Solving the system simultaneously yields A 5 3, B 5 2.
5x 2 7
3
2
}
} 5 }} 1 }}
x 2 2 3x 1 2
x22
x21
Equating coefficients of like terms gives
A 5 2 and 2A 1 B 5 2.
Solving the system simultaneously yields A 5 2, B 5 4.
2x 1 2
2
4
}
} 5 }} 1 }}2
x 2 2 2x 1 1
x21
(x 2 1)
t11
t (t 2 1)
A
t21
B
t
C
t
3. }
2 } 5 }} 1 }} 1 }}
2
t 1 1 5 At 2 1 Bt(t 2 1) 1 C(t 2 1)
5 (A 1 B)t 2 1 (2B 1 C)t 2 C
Equating coefficients of like terms gives
A 1 B 5 0, 2B 1 C 5 1, and 2C 5 1.
Solving the system simultaneously yields
A 5 2, B 5 22, C 5 21.
t11
2
2
1
}
} 5 }} 2 }} 2 }}2
t
t 2(t 2 1)
t21
t
4. s 3 2 s 2 2 6s 5 s(s 2 2 s 2 6) 5 s(s 2 3)(s 1 2)
A
4
B
C
}
} 5 }} 1 }} 1 }}
s
s 3 2 s2 2 6s
s23
s12
4 5 A(s 2 3)(s 1 2) 1 B(s)(s 1 2) 1 C(s)(s 2 3)
5 A(s 2 2 s 2 6) 1 B(s 2 1 2s) 1 C(s 2 2 3s)
5 (A 1 B 1 C)s 2 1 (2A 1 2B 2 3C)s 2 6A
Equating coefficients of like terms gives
A 1 B 1 C 5 0, 2A 1 2B 2 3C 5 0, 26A 5 4
Solving the system simultaneously yields
2
3
4
15
2
5
A 5 2}}, B 5 }}, C 5 }}.
4
2
4
2
}
} 5 2}} 1 }} 1 }}
s 3 2 s2 2 6s
3s
15(s 2 3)
5(s 1 2)
346
Section 8.4
1
5. x 2 2 5x 1 6qw
x 2w
1w0xw1
ww8
2
x}}}}
2 5x 1 6
5x 1 2
8. x 2 1 2x 5 x(x 1 2)
A
1
B
}
} 5 }} 1 }}
x
x 2 1 2x
x12
1 5 A(x 1 2) 1 Bx
5x 1 2
x 18
}
}5 1 1 }
}
x 2 2 5x 1 6
x 2 2 5x 1 6
2
5 (A 1 B)x 1 2A
x 2 2 5x 1 6 5 (x 2 3)(x 2 2)
Equating coefficients of like terms gives
5x 1 2
A
B
}
} 5 }} 1 }}
x 2 2 5x 1 6
x23
x22
A 1 B 5 0 and 2A 5 1
dx
1/2
21/2
E}
} 5 E}} dx 1 E}} dx
x
x 1 2x
x12
5 (A 1 B)x 1 (22A 2 3B)
1
1
2
2
1
x
5 }} ln }} 1 C
2
x12
5 }} ln )x) 2 }} ln )x 1 2) 1 C
)
A 1 B 5 5 and 22A 2 3B 5 2
A 5 17, B 5 212.
1
2
2
Equating coefficients of like terms gives
Solving the system simultaneously yields
1
2
Solving the system simultaneously yields A 5 }}, B 5 2}}.
5x 1 2 5 A(x 2 2) 1 B(x 2 3)
)
9. y 2 2 2y 2 35 (y 2 3)(y 1 1)
y
A
B
}
} 5 }} 1 }}
y 2 2 2y 2 3 y 2 3
y11
x2 1 8
17
12
}
} 5 1 1 }} 2 }}
2
x 2 5x 1 6
x23
x22
y5 A( y 1 1) 1 B( y 2 3)
y
6. y 2 1 4qw
y 3w
1w0w
y 2w
1w0yw1
ww1
y 3 1 0y 2 1 4y 1 0
}}}}}}}
24y 1 1
5 (A 1 B)y 1 (A 2 3B)
Equating coefficients of like terms gives
A 1 B 5 1 and A 2 3B 5 0.
y3 1 1
2 4y 1 1
}
}5y1}
}
y2 1 4
y2 1 4
3
4
1
4
Solving the system simultaneously yields A 5 }}, B 5 }}.
y dy
3/4
1/4
E}
} 5 E}} dy 1 E}} dy
y 2 2y 2 3
y23
y11
The rational function cannot be decomposed any further.
2
3
4
1
A
B
}}2 5 }} 1 }}
12x
12x
11x
y 2 1 y 5 y(y 1 1)
10.
1 5 A(1 1 x) 1 B(1 2 x)
A
y14
B
}
} 5 }} 1 }}
y
y2 1 y
y11
5 (A 2 B)x 1 (A 1 B)
y 1 4 5 A(y 1 1) 1 By
Equating coefficients of like terms gives
A 2 B 5 0 and A 1 B 5 1.
Solving the system simultaneously yields
1
1
A 5 }}, B 5 }}.
2
2
dx
1/2
1/2
}}2 5 }} dx 1 }} dx
12x
12x
11x
1
1
5 2}} ln )1 2 x) 1 }} ln )1 1 x) 1 C
2
2
1
11x
5 }} ln }} 1 C
2
12x
E
E
E
)
)
1
4
5 }} ln )y 2 3) 1 }} ln )y 1 1) 1 C
7. 1 2 x 5 (1 2 x)(1 1 x)
2
5 (A 1 B)y 1 A
Equating coefficients of like terms gives
A 1 B 5 1 and A 5 4.
Solving the system simultaneously yields A 5 4, B 5 23.
4
y14
23
E}
} dy 5 E}} dy 1 E}} dy
y
y 1y
y11
2
5 4 ln )y) 2 3 ln )y 1 1) 1 C
Section 8.4
11. t 3 1 t 2 2 2t 5 t(t 2 1 t 2 2) 5 t(t 1 2)(t 2 1)
A
1
B
C
}
} 5 }} 1 }} 1 }}
t
t 3 1 t 2 2 2t
t12
t21
1 5 A(t 1 2)(t 2 1) 1 B(t)(t 2 1) 1 C(t)(t 1 2)
5 A(t 2 1 t 2 2) 1 B(t 2 2 t) 1 C(t 2 1 2t)
5 (A 1 B 1 C)t 2 1 (A 2 B 1 2C)t 2 2A
5
x 2w
1w5xw1
ww5
15. x 2 1 x 1 1q5ww
2
5x
1 5x 1 5
}}}}}
25x 2 5
5x 1 5
5x 2
}
}552}
}
2
x 1x11
x2 1 x 1 1
5x dx
x11
E}
} 5 E5 dx 2 5E}} dx
x 1x11
x 1x11
x11
5 5x 2 5E}} dx
x 1x11
2
2
Equating coefficients of like terms gives
A 1 B 1 C 5 0, A 2 B 1 2C 5 0, and 22A 5 1.
Solving the system simultaneously yields
1
1
1
2
6
3
21/2
dt
1/6
1/3
}
} 5 }} dt 1 }} dt 1 }} dt
t
t 3 1 t 2 2 2t
t12
t21
1
1
1
5 2}} ln )t) 1 }} ln )t 1 2) 1 }} ln )t 2 1) 1 C
2
6
3
A 5 2}}, B 5 }}, C 5 }}.
E
E
E
E
12. 2t 3 2 8t 5 2t(t 2 2 4) 5 2t(t 2 2)(t 1 2)
2
2
To evaluate the second integral, complete the square in the
denominator.
1
4
5 2A(t 2 2 4) 1 2B(t 2 1 2t) 1 2C(t 2 2 2t)
5 (2A 1 2B 1 2C)t 2 1 (4B 2 4C)t 2 8A
2
2
2
2
1
1
2A 1 2B 1 2C 5 0, 4B 2 4C 5 1, 28A 5 3
Solving the system simultaneously yields
3
5
1
8
16
16
23/8
t13
5/16
1/16
}
} dt5 }} dt 1 }} dt 1 }} dt
t
2t 3 2 8t
t22
t12
3
5
1
5 2}} ln )t) 1 }} ln )t 2 2) 1 }} ln )t 1 2) 1 C
8
16
16
E
1
1
2x 1 1
2
The second integral was evaluated by using Formula 16
from the Brief Table of Integrals.
5x dx
E}
}
x 1x11
2
2
5
1
5
2x 1 1
5 A(x 2 1 2x 1 1) 1 B(x 2 2 1) 1 C(x 2 1)
E
5 (A 1 B)x 2 1 (2A 1 C)x 1 A 2 B 2 C
Equating coefficients of like terms gives
A 1 B 5 1, 2A 1 C 5 0, and A 2 B 2 C 5 0.
Solving the system simultaneously yields
1
4
3
4
1
2
A 5 }}, B 5 }}, C 5 2}}.
x dx
E}}}
(x 2 1)(x 1 2x 1 1)
1/4
3/4
21/2
5 E}} dx 1 E}} dx 1 E}} dx
x21
x11
(x 1 1)
2
s 4 1 2s
2s 1 1
2s
1
}
} 5 s2 2 1 1 }
} 5 s2 2 1 1 }
}1}
}
s2 1 1
s2 1 1
s2 1 1
s2 1 1
4
s 1 2s
ds
2s ds
}
} ds 5 (s 2 2 1) ds 1 }
}1 }
}
s2 1 1
s2 1 1
s2 1 1
1
5 }}s 3 2 s 1 ln (s 2 1 1) 1 tan21 s 1 C
3
E
2
5 5x 2 }} ln (x 2 1 x 1 1) 2 }} tan21 }} 1 C
2
Ï3w
Ï3w
x 2 5 A(x 1 1)2 1 B(x 2 1)(x 1 1) 1 C(x 2 1)
s2 2 1
2
4
3
2
14. s 1 1qw
s w
+w0w
sw
+w0w
sw
1w2sw+
ww0
4
s}}}}}}}}}
+ s3 1 s 2+ s + 0
2s 2 1 2s + 0
2s 2 + s 2 1
}}}}}
2s 1 1
E
2
x2
A
B
C
5 }} 1 }} 1 }}2
}}}
2
(x 2 1)(x 1 2x 1 1)
x21
x11
(x 1 1)
s3
24s
}
}5s1}
}
s2 1 4
s2 1 4
s3
4s
}
} ds 5 s ds 2 }
} ds
s2 1 4
s2 1 4
1 2
5 }}s 2 2 ln (s 2 1 4) 1 C
2
E
x 1 1/2
16. (x 2 1)(x 2 1 2x 1 1) 5 (x 2 1)(x 1 1)2
s
13. s 2 1 4qw
s 3w
s 3w
1w4ws
3
s}}}
1 4s
24s
E
1
2
5 }} ln (x 2 1 x 1 1) 1 }} }} tan21 }}
2
2 Ïw3
Ïw3/2
1
E
1 2
2
5 }} ln (x 2 1 x 1 1) 1 }} tan21 }}
2
Ï3w
Ï3w
Equating coefficients of like terms gives
E
2
x11
E}
} dx
x 1x11
x11
5 E}} dx
(x 1 1/2) 1 3/4
x 1 1/2
1/2
5 E}} dx 1 E}} dx
(x 1 1/2) 1 3/4
(x 1 1/2) 1 3/4
dx
1
1
3
1
5 }} ln31x 1 }}2 1 }}4 1 }}E}}}
2
2
4
2 (x 1 1/2) 1 (Ï3
w/2)
2
t 1 3 5 2A(t 2 2)(t 1 2) 1 2B(t)(t 1 2) 1 2C(t)(t 2 2)
E
1 2
3
1 }}
2
4
1
3
4
x 2 1 x 1 1 5 x 2 1 x 1 }} 1 }} 5 x 1 }}
2
A
t13
B
C
}
} 5 }} 1 }} 1 }}
t
2t 3 2 8t
t22
t12
A 5 2}}, B 5 }}, C 5 }}.
E
347
E
2
2
1
4
3
4
1
2(x 1 1)
5 }} ln )x 2 1) 1 }} ln )x 1 1) 1 }} 1 C
348
Section 8.4
17. (x 2 2 1)2 5 (x 1 1)2(x 2 1)2
21. x 3 2 1 5 (x 2 1)(x 2 1 x 1 1)
1
A
B
C
D
}
} 5 }} 1 }}2 1 }} 1 }}2
(x 2 2 1)2
x11
(x 1 1)
x21
(x 2 1)
x 2 2 2x 2 2
Bx 1 C
A
}
} 5 }} 1 }
}
x3 2 1
x21
x2 1 x 1 1
1 5 A(x 1 1)(x 2 1)2 1 B(x 2 1)2 1 C(x 1 1)2(x 2 1)
x2 2 2x 2 2 5 A(x 2 1 x 1 1) 1 (Bx 1 C)(x 2 1)
1 D(x 1 1)2
5 (A 1 B)x 2 1 (A 2 B 1 C)x 1 (A 2 C)
5 A(x 3 2 x 2 2 x 1 1) 1 B(x 2 2 2x 1 1)
Equating coefficients of like terms gives
1 C(x 3 1 x 2 2 x 2 1) 1 D(x 2 1 2x 1 1)
5 (A 1 C)x 1 (2A 1 B 1 C 1 D)x
3
2
A 1 B 5 1, A 2 B 1 C 5 22, and A 2 C 5 22.
Solving the system simultaneously yields
1 (2A 2 2B 2 C 1 2D)x 1 (A 1 B 2 C 1 D)
A 5 21, B 5 2, C 5 1.
x 2 2x 2 2
2x 1 1
21
E}
} dx 5 E}} dx 1 E}} dx
x 21
x21
x 1x11
2
Equating coefficients of like terms gives
3
2
A 1 C 5 0, 2A 1 B 1 C 1 D 5 0,
5 2ln )x 2 1) 1 ln (x 1 x 1 1) 1 C
2
2A 2 2B 2 C 1 2D 5 0, and A 1 B 2 C 1 D 5 1
Solving the system simultaneously yields
1
1
1
1
4
4
4
4
dx
}
}
(x 2 2 1)2
1/4
1/4
21/4
1/4
5 }} dx 1 }}2 dx 1 }} dx 1 }}2 dx
x11
(x 1 1)
x21
(x 2 1)
1
1
1
1
5 }} ln )x 1 1) 2 }} 2 }} ln )x 2 1) 2 }} 1 C
4
4
4(x 1 1)
4(x 2 1)
A 5 }}, B 5 }}, C 5 2}}, D 5 }}.
E
E
E
E
E
22. x 3 1 1 5 (x 1 1)(x 2 2 x 1 1)
x 2 2 4x 1 4
Bx 1 C
A
}
} 5 }} 1 }
}
x3 1 1
x11
x2 2 x 1 1
x 2 2 4x 1 4 5 A(x 2 2 x 1 1) 1 (Bx 1 C)(x 1 1)
5 (A 1 B)x 2 1 (2A 1 B 1 C)x 1 (A 1 C)
Equating coefficients of like terms gives
A 1 B 5 1, 2A 1 B 1 C 5 24, and A 1 C 5 4.
Solving the system simultaneously yields
18. x 2 1 5x 2 6 5 (x 1 6)(x 2 1)
A 5 3, B 5 22, C 5 1.
x14
A
B
}
} 5 }} 1 }}
x 2 1 5x 2 6
x16
x21
x 2 4x 1 4
3
22x 1 1
E}
} dx 5 E}} dx 1 E}} dx
x 11
x11
x 2x11
2
3
x 1 4 5 A(x 2 1) 1 B(x 1 6)
2
5 3 ln )x 1 1) 2 ln (x 2 2 x 1 1) 1 C
5 (A 1 B)x 1 (2A 1 6B)
3x 2 2 2x 1 12
(x 1 4)
A 1 B 5 1 and 2A 1 6B 5 4.
3x 2 2 2x 1 12 5 (Ax 1 B)(x 2 1 4) 1 (Cx 1 D)
5 Ax 3 1 Bx 2 1 (4A 1 C)x 1 4B 1 D
Solving the system simultaneously yields
2
5
7
7
x14
2/7
5/7
dx 5 }} dx 1 }} dx
}
}
x 2 1 5x 2 6
x16
x21
2
5
5 }} ln )x 1 6) 1 }} ln )x 2 1) 1 C
7
7
A 5 }}, B 5 }}.
E
E
E
2
2 dr
2 dr
E}
} 5 E}} 5 2 tan
r 2 2r 1 2
(r 2 1) 1 1
2
2
21
(r 2 1) 1 C
20. Complete the square in the denominator.
r 2 2 4r 1 5 5 r 2 2 4r 1 4 1 1 5 (r 2 2)2 1 1
3 dr
3 dr
E}
} 5 E}} 5 3 tan
r 2 4r 1 5
(r 2 2) 1 1
2
2
21
A 5 0, B 5 3, 4A 1 C 5 22, and 4B 1 D 5 12
Solving the system simultaneously yields
3x 2 2x 1 12
3
22x
E}}
dx 5 E}} dx 1 E}} dx
(x 1 4)
x 14
(x 1 4)
2
r 2 2r 1 2 5 r 2 2r 1 1 1 1 5 (r 2 1) 1 1
2
Equating coefficients of like terms gives
A 5 0, B 5 3, C 5 22, D 5 0.
19. Complete the square in the denominator.
2
Cx 1 D
(x 1 4)
Ax 1 B
x 14
23. }
5}
2 }
2
2 }1}
2 }
2
Equating coefficients of like terms gives
(r 2 2) 1 C
2
2
2
2
2
3
1
x
5 }} tan21 }} 1 }
}1C
2
2
x2 1 4
The first integral was evaluated by using Formula 16 from
the Brief Table of Integrals.
Section 8.4
x 3 1 2x 2 1 2
(x 1 1)
Cx 1 D
(x 1 1)
Ax 1 B
(x 1 1)
24. }
5}
2 }
2
2 }1}
2 }
2
27.
x 3 1 2x 2 1 2 5 (Ax 1 B)(x 2 1 1) 1 (Cx 1 D)
349
1
}
} dy 5 e x dx
y2 2 y
1
}} dy 5 e x dx 5 e x 1 C
y(y 2 1)
A
1
B
}} 5 }} 1 }}
y
y(y 2 1)
y21
E
5 Ax 3 1 Bx 2 1 (A 1 C)x 1 (B 1 D)
E
1 5 A(y 2 1) 1 B(y)
Equating coefficients of like terms gives
A 5 1, B 5 2, A 1 C 5 0, B 1 D 5 2
5 (A 1 B)y 2 A
Solving the system simultaneously yields
Equating coefficients of like terms gives
A 5 1, B 5 2, C 5 21, D 5 0.
A 1 B 5 0 and 2A 5 1
x 1 2x 1 2
E}
} dx
(x 1 1)
2x
x12
5 E}} dx 1 E}} dx
x 11
(x 1 1)
2
x
x
5 E}} dx 1 E}} dx2 E}} dx
x 11
x 11
(x 1 1)
Solving the system simultaneously yields A 5 21, B 5 1.
3
2
2
2
2
2
2
2
2
2
1
2
2
1
2(x 1 1)
5 }} ln (x 2 1 1) 1 2 tan21 x 1 }
2}1C
1
25. u 1 1qu
ww
+w
1
u}}
11
21
1
1
0
1
0
0
2
u2
}
2 } du 5
u 11
1
(y 1 1)
1
}}2 dy 5 sin u du
(y 1 1)
1
2}} 5 2cos u 1 C
y11
p
Substitute x 5 }}, y 5 0.
2
E
E
The solution to the initial value problem is
1
y11
2}} 5 2cos u 2 1
u2
1
}
}512}
}
u2 1 1
u2 1 1
0
2ln 2 1 0 5 1 1 C or C 5 21 2 ln 2
21 5 0 1 C or C 5 21
1
ww1
26. u 1 1quww+
2
u}}
11
21
2
Substitute x 5 0, y 5 2.
28. }}2 dy 5 sin u du
5 1 2 ln 2
E
2ln )y) 1 ln )y 2 1) 5 e x 1 C
2ln )y) 1 ln )y 2 1) 5 e x 2 1 2 ln 2.
1
E E}
} du
u11
5 u 2 ln )u 1 1)
34 3
4
2
5 2ln )y) 1 ln )y 2 1) 1 C2
The solution to the initial value problem is
u
1
}} 5 1 2 }}
u11
u11
1
1
u
du 2
}} du 5
0 u11
0
E
1
1
1
E}
} dy 5 E2}} dy 1 E}} dy
y
y(y 2 1)
y21
E
2
0
du 2
2
E
2
0
1
}
} du
u2 1 1
2
3 4 2 3tan u4
5 u
1
cos u 1 1
1
y 5 }} 2 1
cos u 1 1
y 1 1 5 }}
21
0
5 2 2 tan21 2
0
dx
x 2 3x 1 2
29. dy 5 }
}
2
x 2 2 3x 1 2 5 (x 2 2)(x 2 1)
1
A
B
}
} 5 }} 1 }}
x 2 2 3x 1 2
x22
x21
1 5 A(x 2 1) 1 B(x 2 2)
1 5 (A 1 B)x 2 A 2 2B
Equating coefficients of like terms gives
A 1 B 5 0, 2A 2 2B 5 1
Solving the system simultaneously yields A 5 1, B 5 21.
dx
dx
dx
Edy 5 E}
} 5 E}} 2 E}}
x 2 3x 1 2
x22
x21
2
y 5 ln )x 2 2) 2 ln )x 2 1) 1 C
Substitute x 5 3, y 5 0.
0 5 0 2 ln 2 1 C or C 5 ln 2
The solution to the initial value problem is
y 5 ln )x 2 2) 2 ln )x 2 1) 1 ln 2
350
30.
Section 8.4
ds
dt
}} 5 }
}
2s 1 2
t 2 1 2t
1 ds
1
ds
}} 5 }} }} 5 }} ln )s 1 1) 1 C1
2 s11
2
2s 1 2
E
32. (a) Complete the square in the denominator.
E
x 2 2 2x 1 2 5 (x 2 2 2x 1 1) 1 1
t 2 1 2t 5 t(t 1 2)
5 (x 2 1)2 1 1
A
1
B
}
} 5 }} 1 }}
t
t 2 1 2t
t12
5 1 1 (x 2 1)2
1 5 A(t 1 2) 1 Bt
Let u 5 x 2 1 so du 5 dx and then use Formula 17
1 5 (A 1 B)t 1 2A
with x 5 u and a 5 1.
dx
du
E}
} 5 E}}
(x 2 2x 1 2)
(1 1 u )
Equating coefficients of like terms gives
2
2
A 1 B 5 0 and 2A 5 1
1
2
1
2
Solving the system simultaneously yields A 5 }}, B 5 2}}.
1/2
dt
1/2
E}
} 5 E}} dt 2 E}} dt
t
t 1 2t
t12
2
1
1
5 }} ln )t) 2 }} ln )t 1 2) 1 C2
2
2
1
1
1
}} ln )s 1 1) 5 }} ln )t) 2 }} ln )t 1 2) 1 C3
2
2
2
3
x
d
dx 2a (a 1 x )
ln 2 5 0 2 ln 3 1 C or C 5 ln 2 1 ln 3 5 ln 6
The solution to the initial value problem is
1
2a
1 (a 2 1 x 2) 2 x(2x)]
1
1/a
5 }}2 }}
1 }}3 }}2
(a 2 1 x 2)2
2a
2a 1 1 (x/a)
3
4
1
3
a2 2 x2
a2
1
5}
} 1 }}4 }
}
2a 2(a 2 1 x 2)2
2a a 2 1 x 2
2
3
4
3
4
9
33. Volume 5 E p1}}2 dx 5 9p E
3x 2 x
2a 2
1
1
5 }}2 }
} 5}
}
2a (a 2 1 x 2)2
(a 2 1 x 2)2
2.5
2
0.5
) t 16t 2 )
6t
)s 1 1) 5 )}}).
t12
ln )s 1 1) 5 ln }}
4
1
a2 2 x2
1
5 }}2 }
}1}
}
2a (a 2 1 x 2)2
a2 1 x2
2.5
ln )s 1 1) 5 ln )t) 2 ln )t 1 2) 1 ln 6
4
x
a
21
(b) }} }
}} 1 C
2 2}
2 1 }}
3 tan
ln )s 1 1) 5 ln )t) 2 ln )t 1 2) 1 C
Substitute t 5 1, s 5 1.
2 2
1
u
5 }}
1 }} tan21 u 1 C
2
2(1 1 u 2)
x21
1
5}
1 }} tan21 (x 2 1) 1 C
}
2
2(x 2 2 2x 1 2)
0.5
dx
}}2
3x 2 x
3x 2 x 2 5 x(3 2 x)
A
1
B
}}2 5 }} 1 }}
x
3x 2 x
32x
1 5 A(3 2 x) 1 Bx
31. (a) Complete the square in the denominator.
5 (2A 1 B)x 1 3A
5 1 4x 2 x 25 5 2 (x 2 2 4x)
5 9 2 (x 2 2 4x 1 4)
Equating coefficients of like terms gives
5 9 2 (x 2 2)2
2A 1 B 5 0 and 3A 5 1
1
3
1
3
Let u 5 x 2 2 so du 5 dx, and then use Formula 18
Solving the system simultaneously yields A 5 }}, B 5 }}.
with x 5 u and a 5 3.
9p
2.5
dx
du
E}
} 5 E}}
5 1 4x 2 x
92u
2
0.5
2
)
)
)
)
1
u13
6
u23
1
x11
5 }} ln }} 1 C
6
x25
5 }} ln }} 1 C
1
d 1
dx 2a
) xx 12 aa )
2
1 d
5 }} }} ln )x 1 a) 2 ln )x 2 a)
2a dx
2
1
1
1
5 }} }} 2 }}
2a x 1 a
x2a
4
1
x2a
x1a
5 }} }} 2 }}
2a (x 1 a)(x 2 a)
(x 1 a)(x 2 a)
1
1
5 2}
}5}
}
x2 2 a2
a2 2 x2
2.5
2.5
0.5
0.5
2.5
2.5
0.5
0.5
5 3p ln 25 5 6p ln 5
2
1
dx
dx
}
1E }x} 1 E }
3 2 x2
5 3p13ln )x)4 1 32ln )3 2 x)4 2
dx
}}2 5 3p
3x 2 x
5 3p(ln 2.5 2 ln 0.5 2 ln 0.5 1 ln 2.5)
(b) }} }} ln }} 1 C
1
3
E
Section 8.4
34. Volume 5
E
1
0
p
2
3 (x 1 1)(2 2 x) 4
E
25 2 t 2 5 25 2 25 sin 2 u 5 25 cos 2 u
1
EÏ2w5ww2wtw dt 5 E5 )cos u) (5 cos u) du
5 25Ecos u du
1 1 cos 2u
5 25E}} du
2
2
x 5 A(2 2 x) 1 B(x 1 1)
2
5 (2A 1 B)x 1 (2A 1 B)
Equating coefficients of like terms gives
1
3
1
0
1
0
12
1
1
Use Figure 8.18(b) from the text with a 5 5 and x 5 t to
0
0
2wt 2w 5 5)cos u).
get Ï2w5ww
4p
4p ln 2
5 }}(2ln 2 1 2 ln 2) 5 }}
3
3
p
2
p
2
35. y 5 3 tan u, dy 5 3 sec2 u du, 2}} , u , }}
9 1 y 2 5 9 1 9 tan2 u 5 9 sec2 u
dy
3 sec u
E}
} 5 E}} du
1wy w
)3 sec u)
Ï9ww
5 Esec u du
2
7
2
4x 2 2 49 5 49 sec 2 u 2 49 5 49 tan 2 u
2
5
5 ln )sec u 1 tan u) 1 C1
Ï9ww
1wy 2w
y
5 ln }} 1 }} 1 C1
3
3
)
E }12} sec u du
1
2
5 }} ln )sec u 1 tan u) 1 C1
5 ln )Ï9ww
1wy 2w 1 y) 2 ln 3 1 C1
)
)
)
)
Ï4wxw2w
w
1
2x
2w49
5 }} ln }} 1 }} 1 C1
2
5 ln )Ï9ww
1wy 2w 1 y) 1 C
1
2
E
7
7
)
Ïwwwww
)
1
2
5 }} ln 2x 1 Ï4ww
x 2w
2w49w 2 }} ln 7 1 C1
Use Formula 88 for sec u du with x 5 u and a 5 1. Use
1
2
Figure 8.18(a) from the text with a 5 3 to get
Ï9ww
1wy 2w 5 3 )sec u).
p
2
7
2
37. x 5 }} sec u, dx 5 }} sec u tan u du, 0 # u , }}
7/2 sec u tan u du
dx
E}
} 5 E}}
)7 tan u)
2w
Ï4ww
x w
49
w
2
)
25
2
2
2 5
5
5
ww
25
tÏw
25
2wt 2w
21 t
5 }} sin }} 1 }} 1 C
2
5
2
1
0
25
2
w5ww
25
25 t Ï2
t
2wt2w
5 }} sin21 }} 1 }} }} }} 1 C
x dx
}}
(x 1 1)(2 2 x)
2dx
2 dx
} 1 E }}
1E }
x11
2 2 x2
4p
5 }}132ln )x 1 1)4 1 322 ln )2 2 x)4 2
3
4p
3
5 }}
25 sin 2u
4
5 }}u 1 }} sin u cos u 1 C
2
3
Solving the system simultaneously yields A 5 2}}, B 5 }}.
E
25u
2
5 }} 1 }} 1 C
2A 1 B 5 1 and 2A 1 B 5 0
4p
p
2
36. t 5 5 sin u, dt 5 5 cos u du, 2}} # u # }}
2
2px }} dx
x dx
}}
0 (x 1 1)(2 2 x)
x
A
B
}} 5 }} 1 }}
(x 1 1)(2 2 x)
x11
22x
5 4p
351
5 }} ln 2x 1
4x 2 2 49 1 C
7
2
Use Figure 8.18(c) from the text with a 5 }} to get
!x§§2§}§4} 5 }2} tan u.
2
49
7
352
Section 8.4
p
2
p
2
p
2
38. x 5 tan u, dx 5 sec 2 u du, 2}} , u , }}
40. x 5 sec u, dx 5 sec u tan u du, 0 # u , }}
x 2 2 1 5 sec 2 u 2 1 5 tan 2 u
x 2 1 1 5 tan 2 u 1 1 5 sec 2 u
2 dx
2 sec u tan u du
E}
} 5 E}}
sec u )tan u)
2w1
x Ïxww
2 du
5 E}}
sec u
5 E2 cos u du
5 E11 1 cos 2u2 du
dx
sec u du
E}
} 5 E }}
ta
n u )sec u)
x Ïxww
1w
1
sec u du
5 E }}
tan u
cos u
5 E }} du
sin u
5 E (sin u) cos u du
2
2
3
2
2
2
2
2
2
22
5 2(sin u)
21
3
2
1
2
5 u 1 }} sin 2u 1 C
1C
5 u 1 sin u cos u 1 C
5 2csc u 1 C
Ïxw2w
2w1 1
5 sec21 x 1 }} }} 1 C
Ï1ww
1wx 2w
5 2}} 1 C
x
x
21
5 sec
Use Figure 8.18(a) from the text with a 5 1 to get
Ïw
x 2w
2w1
1x2
x 1 }}
1C
2
x
Ïw1w
1wx 2w
csc u 5 }}.
p
2
41. z 5 4 sin u, dz 5 4 cos u du, 0 , u , }}
x
p
2
p
2
39. x 5 sin u, dx 5 cos u du, 2}} , u , }}
16 2 z 2 5 16 2 16 sin 2 u 5 16 cos 2 u
Ï1w6ww
2wz w
E}
} dz
z
)4 cos u) (4 cos u) du
5 E}}
4 sin u
4 cos u
5 E }} du
sin u
4 2 4 sin u
5 E }} du
sin u
5 E (4 csc u 2 4 sin u) du
1 2 x 2 5 1 2 sin 2 u 5 cos 2 u
2
sin u cos u du
x dx
E}
} 5 E }}
)cos u)
Ï1ww
2wx w
5 E sin u du
5E (1 2 cos u) sin u du
3
3
2
3
2
2
2
1
3
5 2cos u 1 }} cos 3 u 1 C
1
1
3
2
5 cos u 21 1 }} cos 2 u 1 C
3
4
1
2wx w 21 1 }} (1 2 x 2) 1 C
5 Ï1ww
3
2
x 2Ïw
1w
2Ïw
1w
2wx2w
2wx 2w
5 2}} 2 }} 1 C
3
3
Use Figure 18.8(b) from the text with a 5 1
2wx 2w 5 cos u.
to get Ï1ww
5 24 ln )csc u 1 cot u) 1 4 cos u 1 C
)z
) 1 4 2
z
ww
4 1 Ï1w6
2wz w
2wz w 1 C
5 24 ln )}}) 1 Ï1w6ww
z
Ï1w6ww
Ï1w6ww
4
2wz 2w
2wz 2w
5 24 ln }} 1 }} 1 4 }} 1 C
2
2
Use Formula 89 with a 5 1 and x 5 u. Use Figure 8.18(b)
from the text with a 5 4 to get
Ï1w6ww
Ï1w6ww
4
2wz 2w
2wz 2w
csc u 5 }}, cot u 5 }} and cos u 5 }}.
)z)
)z)
4
p
2
p
2
42. w 5 2 sin u, dw 5 2 cos u du, 2}} , u , }}
4 2 w 2 5 4 2 4 sin 2 u 5 4 cos 2 u
8 dw
8(2 cos u) du
E}
} 5 E }}
4 sin u )2 cos u)
2w
w Ïw4w
ww
5 E 2 csc u du
2
2
2
2
5 22 cot u 1 C
22Ïw4w
2w
w w2
5 }} 1 C
w
Use Figure 8.18(b) from the text with a 5 2 and x 5 w to
Ïw4w
w w2
2w
get cot u 5 }}.
w
Section 8.4
45. For x $ 0, y $ 0 on [0, 3]
dx
43. dy 5 }}
2w9
Ïxw2w
p
x 5 3 sec u, dx 5 3 sec u tan u du, 0 , u , }}
2
x 2 9 5 9 sec u 2 9 5 9 tan u
2
2
Area 5
E
3
0
Ïw9w
2wx 2w
}} dx
3
9 2 x 2 5 9 2 9 sin 2 u 5 9 cos 2 u
E
3
0
3 )cos u)
E }
} 3 cos u du
3
5 E 3 cos u du
1 1 cos 2u
5 3E }} du
2
u
sin 2u
5 3 }} 1 }}
32 4 4
Ïw9w
2wx 2w
}} dx 5
3
)
46. Volume 5
2
The solution to the initial value problem is
2
2
0
dx 5 4p
E
1
0
dx
}}
(1 1 x 2)2
p
4
x 5 tan u, dx 5 sec 2 u du, 0 # u # }} (since 0 , x , 1)
E
1
0
p
2
p
2
E
5E
5E
dx
5
}}
(1 1 x 2)2
x 5 tan u, dx 5 sec 2 u du, 2}} , u , }}
x 2 1 1 5 tan 2 u 1 1 5 sec 2 u
dx
E}
}
(x 1 1)
sec u du
5 E }}
)sec u)
5 E cos u du
2
1
p
4
When x 5 0, u 5 0 and when x 5 1, u 5 }}.
44. (x 2 1 1)2 }} 5 Ïw
x 2w
1w1
y 5
2
E p1}
}
11x 2
0
1 1 x 2 5 1 1 tan 2 u 5 sec 2 u
)
Ïw
x 2w
9
x
2w
y 5 ln }} 1 }} .
dy
dx
dx
dy 5 }
}
(x 2 1 1)3/2
p/2
3p
4
5
4
ln 3 5 ln }} 1 }} 1 C or C 5 0
3
3
3
2
p/2
5 }} < 2.356
Substitute x 5 5, y 5 ln 3.
)3
0
p/2
0
Ïw
x 2w
x
2w9
5 ln }} 1 }} 1 C
1
p/2
0
5 ln )sec u 1 tan u) 1 C
3
p
2
When x 5 0, u 5 0 and when x 5 3, u 5 }}.
2
)3
p
2
x 5 3 sin u, dx 5 3 cos u du, 0 # u # }}
2
dx
E}
}
2w9
Ïw
x w
3 sec u tan u du
5 E }}
)3 tan u)
5 E sec u du
y5
353
3/2
2
3
5 sin u 1 C
x
5 }} 1 C
1w1
Ïxw2w
Substitute x 5 0, y 5 1.
15C
p/4
0
p/4
0
p/4
sec 2 u
du
}}
sec 4 u
cos 2 u du
1 1 cos 2u
}} du
2
p/4
1
sin 2u
5 }}u 1 }}
2
4
0
p
1
5 }} 1 }}
8
4
p
1
p
Volume 5 4p }} 1 }} 5 p }} 1 1 < 8.076
8
4
2
0
3
1
4
2 1
2
dx
1
x(1000 2 x)
250
A
1
B
}} 5 }} 1 }}
x
x(1000 2 x)
1000 2 x
47. (a) }} 5 }} dt
1 5 A(1000 2 x) 1 Bx
5 (2A 1 B)x 1 1000A
The solution to the initial value problem is
x
y 5 }} 1 1.
1w1
Ïxw2w
Equating the coefficients and solving for A and B gives
1
1
1000
1000
(1/1000) dx
(1/1000) dx
dx
}} 5 }} 1 }}
x
1000 2 x
x(1000 2 x)
1
1
5 }} ln x 2 }} ln (1000 2 x) 1 C1
1000
1000
1
x
5 }} ln }} 1 C1
1000
1000 2 x
1
x
t
}} ln }} 5 }} 1 C2
1000
1000 2 x
250
x
ln }} 5 4t 1 C
1000 2 x
x
}} 5 e 4t1C 5 Ae 4t
1000 2 x
A 5 }}, B 5 }}
E
E
E
354
Section 8.4
x
2
47. continued
When t 5 0, x 5 2.
sin x
1 1 cos x
(b) From part (a), z 5 }}
2
1
}} 5 A or A 5 }}
998
499
z(1 1 cos x) 5 sin x
x
1
}} 5 }}e4t
1000 2 x
499
1000
x
x 5 }}e4t 2 }}e 4t
499
499
1000e 4t
e 4t
x 1 1 } } 5 }}
499
499
1000e 4t
x 5 }}
499 1 e 4t
1000
or x 5 }}
1 1 499e 24t
1
z 2(1 1 cos x)2 5 sin 2 x
z 2(1 1 cos x)2 5 1 2 cos 2 x
2
z 2(1 1 cos x)2 2 (1 2 cos x)(1 1 cos x) 5 0
(1 1 cos x)(z 2 1 z 2cos x 2 1 1 cos x) 5 0
1 1 cos x 5 0
1
499
e24t 5 }}
1 2 z2
11z
cos x 5 }}2
1 2 z2
11z
(c) From part (b), cos x 5 }}2
1
499
t 5 2}} ln }} < 1.553
sin 2 x 5 1 2 cos 2 x
Half the population will have heard the rumor in about
1.553 days.
(1 2 z 2)2
(1 1 z )
5 1 2 }}
2 2
dx
1
(c) }} 5 }} x(1000 2 x)
dt
250
dx
}} will be greatest when y 5 x(1000 2 x) is greatest.
dt
(1 1 z 2)2 2 (1 2 z 2)2
(1 1 z )
5 }}}
2 2
This occurs when x 5 500 which occurs when
1 1 2z 2 1 z 4 2 1 1 2z 2 2 z 4
(1 1 z )
5 }}}}
2 2
t < 1.553 as shown in part (b).
4z 2
(1 1 z )
5 }}
2 2
dy
2x
48. }} 5 2}}2
dx
12x
5
2z
11z
sin x 5 6}}2
!§§§1§§§§2§
22x 2
dx
12x
1 1 }}2
2z
11z
Only sin x 5 }}2 makes sense in this case.
!§
x412x211
}}
(1 2 x 2)2
) x1 21x1 )
2
5 }}2 dx
x
2
(d) z 5 tan }}
x2 1 1
x 21
12 22
1
x
dz 5 }}11 1 tan }}2 dx
2
2
1
2
1
5 2}
2 } dx for 0 # x # }}
Arc length 5
x 11
E 12}
} dx
x 2 12
1/2
0
2
2
2
1
2
dz 5 }}(1 1 z 2) dx
2 dz
11z
dx 5 }}2
x2 1 1
2
x 21
x 21
2
A
B
}
} 5 }} 1 }}
x2 2 1
x21
x11
2}
2 } 5 21 2 }
2 }
where A 5 1 and B 5 21
x 11
1
1
E 12}
} dx 5 E
} 1 }} dx
121 2 }
x 2 12
x21
x 1 12
5 2x 2 ln )x 2 1) 1 ln )x 1 1)
3
4
0
2
2
x
dz 5 }} sec 2 }} dx
1
x 2 2 1 qw
x 2w
1w1
2
x}}
21
2
1/2
(z 2 1 1) cos x 5 1 2 z 2
cos x 5 21 does not make sense in this case.
1 1 499e24t 5 2
1
4
or
cos x 5 21
1000
(b) 500 5 }}
1 1 499e24t
ds 5
sin x
1 1 cos x
49. (a) From the figure, tan }} 5 }}.
1/2
0
1/2
1
2
1
2
3
2
5 2}} 2 ln }} 1 ln }}
1
2
5 ln 3 2 }}
0
Chapter 8 Review
50.
E
■ Chapter 8 Review Exercises
2 dz
}}2
11z
E
dx
}} 5 }}
2z
1 1 sin x
1 1 }}2
(pp. 454–455)
11z
2
1 2 }}
1 1 2t
t 2 ln (1 1 2t)
1. lim }}
5
lim
5 ` for t→02 and
}}
2t
t2
t→0
t→0
5
2 dz
E}
}
z 1 2z 1 1
5
2 dz
2
E}
} 5 2}} 1 C
(z 1 1)
z11
2
2` for t→01
The limit does not exist.
2
2
5 2}}
1C
x
tan }} 1 1
51.
dx
E}
}5E
1 2 cos x
5
E
E
x→0
4. The limit leads to the indeterminate form 1`.
f (x) 5 x1/(12x)
ln x
12x
ln x
1/x
lim }} 5 lim }} 5 21
x→1 1 2 x
x→1 21
ln f (x) 5 }}
1
tan }}
2
E
3
5
x cos x 1 sin x
sin x
2x sin x 1 cos x 1 cos x
5 lim }}} 5 2
cos x
x→0
x sin x
x→0 1 2 cos x
dz
}}2
z
1
z
52.
3 sec2 3t
t→0 5 sec 5t
3. lim }} 5 lim }}
2
2 dz
}}2
11z
}}2
12z
1 2 }}2
11z
5 2}} 1 C 5 2}
1C
x
du
}} 5
1 2 sin u
tan 3t
t→0 tan 5t
2. lim }} 5 lim }}
5 }}
2
2 dz
}}2
11z
}}
2z
1 2 }}2
11z
5
2 dz
E}
}
z 2 2z 1 1
5
2 dz
E}
}
(z 2 1)
1
e
lim x1/(12x) 5 lim eln f (x) 5 e21 5 }}
x→1
x→1
5. The limit leads to the indeterminate form `0.
f (x) 5 x1/x
2
ln x
x
ln f (x) 5 }}
2
ln x
x
1/x
lim }} 5 lim }} 5 0
x→`
x→` 1
ln f (x)
lim x1/x 5 lim e
2
z21
5 2}} 1 C
x→`
x→`
5 e0 5 1
2
5 2}}
1C
u
tan }} 2 1
6. The limit leads to the indeterminate form 1`.
2
2
5 }}
1C
u
1 2 tan }}
2 dz
}}2
11z
53.
dt
E}
} 5 E }}}
12z
2z
1 1 sin t 1 cos t
1 1 }} 1 }}
2
11z
5
2
3 x
x
1
2
f (x) 5 1 1 }}
2
11z
dz
E}
}
z11
5 ln )z 1 1) 1 C
t
5 ln )tan }} 1 1) 1 C
2
2
1
3
2
ln 1 1 }}
x
3
ln f (x) 5 x ln 1 1 }} 5 }}
1
x
}}
1
1
2
3
ln 1 1 }}
x
lim }}
1
x→`
}}
x
3 x
x
1
x→`
2
2
x
23/x 2
}}
1 1 3/x
5 lim }
x→` 2}1}
x2
3x
5 lim }} 5 3
x→` x 1 3
lim 1 1 }} 5 lim eln f (x) 5 e3
x→`
cos r
7. lim }} 5 0 since )cos r) # 1 and ln r→` as r→`.
r→` ln r
8. lim
u→p/2
1
p
2
2
p
2
u 2 }}
1
u 2 }} sec u 5 lim } 5 lim }} 5 21
u→p/2 cos u
u→p/2 2sin u
355
356
Chapter 8 Review
1
2
3
ln x 2 x 1 1
1
1
9. lim }} 2 }} 5 lim }}
(x 2 1) ln x
x→1 x 2 1
ln x
x→1
4
f (x)
x→` g(x)
1
}} 2 1
x
5 lim }}
x
2
1
x→1 }}
1 ln x
x
f (x)
x→` g(x)
12x
21
1
2
x→1 1 1 x/x 1 ln x
x→` g(x)
x→` tan
p
21
x→`
10. The limit leads to the indeterminate form ` .
0
x
x 5 }} and lim x 5 `
2
x→`
f grows faster than g.
f (x)
x→` g(x)
csc21 x
1/x
x→`
20. lim }} 5 lim }}
1 x
f (x) 5 1 1 }}
x
2
1
2}}
xÏxw2w
2w
1
1
ln (1 1 1/x)
ln f (x) 5 x ln 1 1 }} 5 }}
x
1/x
1
2
21/x 2
}}
1 1 1/x
ln (1 1 1/x)
1/x
5 lim }}
1
x→0
21/x
x→0
2}}
x→`
x
x11
x2
x
lim }} 5 lim1 }
2 5 lim1 }} 5 0
1
x
f (x)
19. lim }} 5 lim }2}
1 5 ` since
lim tan
lim
ex
x→` 100
x/100
x→` xe
f grows faster than g.
5 lim }} 5 2}}
x→01
x→` 1 2 1/x
18. lim }} 5 lim }2
}
x 5 lim }} 5 `
x→1
x→01
1
x→` x 1 1/x
f grows at the same rate as g.
5 lim }}
x 2 1 1 x ln x
1
x
17. lim }} 5 lim }} 5 lim }}2 5 1
5 lim }}
x→` Ïx
2w1
w2w
x2
}
}
x §§
2§
1
x→` !§
1
5 lim !}
}
§§ 5 1
1/x
1§
2§
x→` §
5 lim
1 x
1 1 }} 5 lim1 eln f (x) 5 e0 5 1
x
x→0
2
2
2
11. The limit leads to the indeterminate form 00.
f grows at the same rate as g.
f (u) 5 (tan u)u
f (x)
x→` g(x)
ln (tan u)
1/u
sec2 u
}}
tan u
ln (tan u)
lim }} 5 lim1 }
1/u
x→01
x→0 2}1}
u2
5 lim x ln x 2 log2x
x→`
5 lim xln x 2 (ln x)/ln 2
x→`
5 lim x (ln x)(1 2 1/ln 2)
u
sin u cos u
2
5 lim1 2}}
x→0
xln x
x→` x
21. lim }} 5 lim }
lo}
g 2x
ln f (u) 5 u ln (tan u) 5 }}
x→`
1 (ln x)(1/ln 2 2 1)
12
x→` x
5 lim }}
22u
x→0 2sin u 1 cos u
5 lim1 }
50
2 }
2
50
1
ln 2
Note that 1 2 }} , 0 since ln 2 , 1.
f grows slower than g.
u
lim (tan u) 5 lim1 e
x→01
ln f (u)
x→0
1u2
1
5e 51
0
sin t
t
cos t
2t
12. lim u 2 sin }} 5 lim1}}
2 5 lim1 }} 5 `
u→`
t→0
x 3 2 3x 2 1 1
x→` 2x 1 x 2 3
t→0
3x 2 2 6x
x→` 4x 1 1
6x 2 6
4
13. lim }}
5 lim }} 5 lim }} 5 `
2
6x 2 1
x→` 4x 2 3x
3x 2 2 x 1 1
x→` x 2 x 1 2
x→`
6
x→` 12x 2 6x
14. lim }
5 lim }
}
4
3
3 }
2 5 lim }
2} 5 0
f (x)
x
x→` g(x)
x→` 5x
f (x)
x→` g(x)
32x
x→` 2
2x
x→` 3
2 x
12
x→` 3
2
3
22. lim }} 5 lim }2}x 5 lim }}x 5 lim }} 5 0 since }} , 1.
1
5
15. lim }} 5 lim }} 5 }}
f grows at the same rate as g.
log2 x
(ln x)/(ln 2)
ln 3
f (x)
16. lim }} 5 lim }}
5 lim }} 5 }}
ln 2
g
(
x
)
x→`
x→` log3 x
x→` (ln x)/(ln 3)
f grows at the same rate as g.
f grows slower than g.
ln 2x
f (x)
ln x 1 ln 2
2 ln x
1/x
1
2
23. lim }} 5 lim }}2 5 lim }} 5 lim }} 5 }}
x→` g(x)
x→` ln x
x→`
f grows at the same rate as g.
f (x)
x→` g(x)
10x 3 1 2x 2
e
30x2 1 4x
}}
ex
60x 1 4
}}
ex
60
}}x 5 0
e
24. lim }} 5 lim }}
x
x→`
5 lim
x→`
5 lim
x→`
5 lim
x→`
f grows slower than g.
x→` 2/x
Chapter 8 Review
tan21 (1/x)
1/x
x→`
f (x)
x→` g(x)
25. lim }} 5 lim }}
1
}}4
x
x→` x 1 1
x→` }1} 1 }1}
2
4
x
5 lim }}
22
x
True
2x
x→`
1
34. lim } 5 lim }
2 }50 # 1
1
}}2 (2x22)
1 1 (1/x)
1
}}4
1
x
5 lim }
35. lim }
2 }50
1
5 lim }}2 5 1
x→` 1 1 (1/x)
x→` x 1 1
x→` }1} 1 }1}
2
4
x
x
True
f grows at the same rate as g.
1
}}
ln x
x
50
36. lim }} 5 lim }
x→` x 1 1
x→` 1
sin21 (1/x)
(1/x )
x→`
f (x)
x→` g(x)
26. lim }} 5 lim }}
2
True
1
}}(2x 22)
Ïw1w
2w(1
w/x
w2w)
5 lim }}
23
22x
x→`
x
5 lim }} 5 `
x→` 2Ï1
ww
2w(1
w/x
ww
)2
f grows faster than g.
2sin x 2 1
x→0 e 2 1
(ln 2)(cos x)2sin x
e
x→0
27. (a) lim f (x) 5 lim }
5 ln 2
x
x } 5 lim }}
x→0
x→0
True
sec21 x
1
x→`
p
2
p
2
38. lim }} 5 }} # }}
True
)3 cos u)
Ï9ww
2wx 2w
ln x
x→0 1/x
1/x
5 lim1 }}2
x→0 21/x
5 lim1 }}
5
5 lim1 (2x) 5 0
E du
5u1C
x→0
(b) Define f (0) 5 0.
x
5 sin21 }} 1 C
3
1
2
x2
x 4 5 lim 1 1 1 5 1 # 1
29. lim }
}}2
1
x
x→`
x→`
}}2
x
51#1
3 cos u du
x
E }d}
5 E }}
28. (a) lim1 f (x) 5 lim1 x ln x
1
1
}} 1 }}
1
}}
x
}
1
}}
x
p
p
39. x 5 3 sin u, dx 5 3 cos u du, 2}} # u # }}
2
2
(b) Define f (0) 5 ln 2.
x→0
ln 2x
37. lim }} 5 lim
x→` ln x
x→`
E
3
0
dx
}} 5 lim2
Ï9ww
2wx 2w b→3
E
b
0
dx
}}
2wx 2w
Ïw9w
True
30.
1
1
}}2 1 }}4
x
x
lim }
1
x→`
}}4
x
b→3
5 lim (x 2 1 1) 5 `
x→`
b→3
x
1
31. lim }} 5 lim } 5 1 Þ 0
x→` 1 1 }1}
x
False
32.
1
}}
x
l
nx
ln (ln x)
lim }} 5 lim }
1
l
n
x
x→`
x→` }}
x
True
tan21 x
1
x→`
p
2
p
2
33. lim }} 5 }} # }}
True
4
1
b
3
2
b
0
p
2
5 lim2 sin21 }} 5 }}
False
x→` x 1 ln x
3
x
3
5 lim2 sin21 }}
1
5 lim }} 5 0
x→` ln x
357
358
Chapter 8 Review
40. u 5 ln x
dv 5 dx
1
x
3
v5x
du 5 }} dx
1
b→0
3
b→0
4
where A 5 21, B 5 1.
b
E
`
b→0
3
2 dx
}} 5 lim
x(x 2 2) b→`
ln b
}}
1/b
1/b
}}2
21/b
5 21 2 lim1
b→0
5 21 2 lim1
b→0
21
0
21
E
0
21
E
dy
}2}
y /3
22/3
dy
1
dy
1
}2}
y /3
dy
5 lim
}2}
y /3 b→02
E
b
21
0
y
3
4
5 lim2 3y1/3
b→0
E
1
0
E
1
dy
5 lim1
}2}
y /3
b→0
b→`
4
E
21
E
E
0
42.
22
21
22
1
b
21
21
22
E
`
1
0
21
E
b
22
E
0
21
du
5 lim
}}
(u 1 1)3/5 b→211
E
E
0
22
b
2
1
0
b
b→`
1
4
3
4
22
4
b
4
v 5 2e2x
du 5 2x dx
2 2x
0
dv 5 e2x dx
45. u 5 x 2
Ex e
5
5
5
}} 2 }}(b 1 1)2/5 5 }}
2
2
2
5
5
du
5 2}} 1 }} 5 0
}}
2
2
(u 1 1)3/5
3
4
5 ln }} 1 ln 3 1 1 5 ln }} 1 1
b
du
}}
(u 1 1)3/5
32
1
b→`
4
5
b→21
3x 2 1
}
} dx
x 2(4x 2 1)
1
4
1
E 12}
} 1 }} 1 }} dx
x
4x 2 1
x 2
1
5 lim 32ln )4x 2 1) 1 ln )x) 2 }}4
x
1
b
5 lim 1ln }} 2 }} 1 ln 3 1 12
b
4b 2 1
du
}}
(u 1 1)3/5
5
5
5
}}(b 1 1)2/5 2 }} 5 2}}
2
2
2
5 lim 1 }}(u 1 1)2/5
5 lim 1
1
3x 2 1
}
} dx 5 lim
4x 3 2 x 2
b→`
du
}}
(u 1 1)3/5
32
3
b→21
b
b
5 lim 2
b→21
E
3x 2 1
}
} dx 5 lim
4x 3 2 x 2
b→`
where A 5 24, B 5 1, C 5 1
5
b→21
2
5 (A 1 4B)x 2 1 (2B 1 4C)x 2 C
b
du
1
}}
(u 1 1)3/5
du
5 lim
}}
(u 1 1)3/5 b→212
3
1
dy
531356
}2}
y /3
E
4
3x 2 1 5 Ax 2 1 Bx(4x 2 1) 1 C(4x 2 1)
b→0
du
5
}}
(u 1 1)3/5
3
3x 2 1
B
A
C
}
} 5 }} 1 }} 1 }}2
x
x 2(4x 2 1)
4x 2 1
x
5 lim 2 }}(u 1 1)2/5
E
E
`
44.
5 lim1 [3 2 3b1/3] 5 3
1
x22
x
3
b
b
1
y22/3 dy
3
b→0
4
b12
1
5 lim ln }} 2 ln }} 5 ln 3
b
3
b→`
b
5 lim1 3y1/3
3
5 lim ln }}
5 lim2 [3b1/3 1 3] 5 3
b→0
b
3
b→`
b→0
dy
5
}2}
y /3
1
E 12}1x} 1 }
} dx
x 2 22
5 lim 2ln )x) 1 ln )x 1 2)
5 21 2 lim1 (2b) 5 21
1
2 dx
}}
x(x 2 2)
3
1
5 lim1 (21 2 b ln b 1 b)
E
E
b
b
5 lim1 x ln x 2 x
41.
E
2 5 A(x 2 2) 1 Bx 5 (A 1 B)x 2 2A
1
1
2 dx
}
} 5 lim
x 2 2 2x b→`
A
2
B
}} 5 }} 1 }}
x
x(x 2 2)
x22
Eln x dx 5 x ln x 2 E dx 5 x ln x 2 x 1 C
E ln x dx 5 lim E ln x dx
0
E
`
43.
E
dx 5 2x 2e2x 1 2x e2x dx
u 5 2x
dv 5 e2x dx
du 5 2 dx
v 5 2e2x
Ex e
2 2x
dx
E
5 2x 2e2x 2 2x e2x 1 2e2x dx
5 2x 2e2x 2 2x e2x 2 2 e2x 1 C
E
`
0
E x e dx
5 lim 2x e 2 2x e 2 2 e
3
4
b
2b
2
5 lim 32}} 2 }} 2 }} 1 24 5 2
e
e
e
x 2e2x dx 5 lim
b
2 2x
b→` 0
2 2x
b→`
b→`
2x
b
0
2
b
2x
b
b
Chapter 8 Review
46. u 5 x
dv 5 e 3x dx
du 5 dx
Ex e
E
3x
1
3
has infinite discontinuities at t 5 0 and t 5 1.
1
1
3
3
1
1
5 }}x e3x 2 }} e3x 1 C
3
9
dx 5 }}x e3x 2 }} e3x dx
0
2`
Note that the integral must be broken up since the integrand
v 5 }}e 3x
E
xe
3x
E
0
dx 5 lim
xe
b→2` b
3x
E
0
21
b→2`
4t 3 1 t 2 1
t (t 2 1)(t 1 1)
b→0
dx
3
2}} 2 }}b e 3b 1 }} e 3b 5 2}}
1
3
B
t
C
t21
b
21
4t 3 1 t 2 1
}
} dt
2
t (t 2 1)(t 2 1 1)
3 t t 11
4
1
(b 2 1)
5 lim 32}} 1 ln }} 1 tan
b
b 11
p
b 2 1 2 ln 2 1 }}4 5 `
4
(t 2 1)2
1
4
1
9
E
21
t
5 lim2 2}} 1 ln }
2 } 1 tan
0
3
A
t
4t 3 1 t 2 1
}
} dt
t 2(t 2 1)(t 2 1 1)
5 lim2
1
1
5 lim }}x e 3x 2 }} e 3x
9
b→2` 3
5 lim
b→0
2
b
4
1
9
1
9
Dt 1 E
t 11
E
`
1 Ct (t 1 1) 1 (Dt 1 E)t (t 2 1)
2
5 (A 1 C 1 D)t 4 1 (2A 1 B 2 D 1 E)t 3
48.
2`
4 dx
}
}5
x 2 1 16
E
0
2`
0
2
2`
2
b→2` b
21 x
b
b→2`
`
b
2
b→` 0
2
x
4
5 lim tan21 }}
b→`
A 5 0, B 5 1, C 5 2, D 5 22, E 5 1.
3
E
`
2
2`
2
1
2
(t 2 1)2
t 11
1
t
21
t1C
5 2}} 1 ln }
2 } 1 tan
E
4t 1 t 2 1
4t 1 t 2 1
}} dt 1 E }} dt
t (t 2 1)(t 1 1)
t (t 2 1)(t 1 1)
4t 1 t 2 1
4t 1 t 2 1
}} dt 1 E }} dt
t (t 2 1)(t 1 1)
t (t 2 1)(t 1 1)
4t 3 1 t 2 1
}
} dt 1
2
t (t 2 1)(t 2 1 1)
1/2
1
21
2
2
1/2
2
E
E
b
3 4
b→`
1
5 lim ln b
2
b→`
3
2
!§§§§
5 lim ln u
3
2
`
3
2
4t 3 1 t 2 1
}
} dt
2
t (t 2 1)(t 2 1 1)
1
3
2
2
0
1
u
2 ww
Ïuww
11
1
f (u)
lim }} 5 lim }} 5 lim 1 1 }}2 5 1
u
u
u→` g(u)
u→`
u→`
`
`
1
g(u) du 5
Since
}} du
1
1 u
b
1
5 lim
}} du
1
u
b→`
g(u) 5 }}. Both are positive continuous functions on [1, `).
E
4t 3 1 t 2 1
}
} dt
2
t (t 2 1)(t 2 1 1)
0
4 dx
p
p
}
} 5 }} 1 }} 5 p
2
2
x 2 1 16
49. Use the limit comparison test with f(u) 5 }} and
Ïuw2w1
ww1
1
5 2}} 1 2 ln )t 2 1) 2 ln )t 2 1 1) 1 tan21 t 1 C
t
2`
b→`
2
2
E
1E
1E
0
21
4t 1 t 2 1
E}
} dt
t (t 2 1)(t 1 1)
dt
22t 1 1
2 dt
5 E}} 1 E}} 1 E}} dt
t
t 11
t21
dt
1 dt
2 dt
2t dt
5 E}} 1 E}} 2 E }} 1 E}}
t
t21
t 11
t 11
5
b
3
4
b
p
5 lim 1tan }}2 5 }}
4
2
Solving the system simultaneously yields
21
0
3tan }4}4
b
p
5 lim 12tan }}2 5 }}
4
2
4 dx
4 dx
E}
} 5 lim E }}
x 1 16
x 1 16
0
2`
4 dx
}
}
x 2 1 16
21
A 2 B 1 C 2 E 5 0, 2A 1 B 5 1 and 2B 5 21.
E
0
21
2
b→2`
A 1 C 1 D 5 0, 2A 1 B 2 D 1 E 5 4,
`
`
4 dx
x
E}
} 5 tan }} 1 C using Formula 16 with a 5 4
x 1 16
4
4 dx
4 dx
E }
} 5 lim E }}
x 1 16
x 1 16
5 lim
Equating coefficients of like terms gives
E
4 dx
}
}1
x 2 1 16
0
1 (A 2 B 1 C 2 E)t 2 1 (2A 1 B)t 2 B
2
21
Since this limit diverges, the given integral diverges.
4t 3 1 t 2 1 5 At(t 2 1)(t 2 1 1) 1 B(t 2 1)(t 2 1 1)
2 2
b
21
2
b→02
47. }
5 }} 1 }}2 1 }} 1 }
}
2
2
2 }
2
359
5 `,
2
E
`
we know that
1
E
`
g(u) du diverges and so
1
f (u) du
diverges. This means that the given integral diverges.
360
Chapter 8 Review
E
50. Evaluate e2x cos x dx using integration by parts.
u 5 cos x
dv 5 e2x dx
du 5 2sin x dx
v 5 2e2x
Ee
2x
cos x dx 5 2e
E
2x
Evaluate sin x e
cos x 2 sin x e
dv 5 e2x dx
du 5 cos x dx
v 5 2e2x
Esin x e
2x
Ee
2x
E
2x
dx
dx using integration by parts.
u 5 sin x
2x
dx 5 2e
E
sin x 1 e
2x
cos x dx 5 e
sin x 2 e
2x
2x
x
2x
`
2`
0
2`
x
2u
e2x sin x 2 e2x cos x b
3
40
2
e sin b 2 e cos b
1
5 lim 3}}} 1 }}4
2
2
2b
2x
x
0
2x
2x
x
b→2` b
3tan e 4b
p
p
5 lim 1}} 2 tan e 2 5 }}
4
4
dx
5 lim E }}
e 1e
21
x 0
21
E
`
dx
}
}
e x 1 e2x
b
b
2x
x
b→` 0
3
5 lim 1tan
40
b
5 lim tan21 e x
b→`
b→`
p
2
2x
2b
2`
b→2`
cos x 1 C1
5 lim }}}
b→`
`
2x
x
b→2`
p
4
21
p
4
2
e b 2 }}
p
4
5 }} 2 }} 5 }}
b→` 0
0
2x
ex 1 C
0
2x
b
21
0
x
e sin x 2 e cos x
Ee cos x dx 5 }}}
1C
2
E e cos u du 5 lim E e cos x dx
2x
21
2
`
0
2 e
x
du
dx
E}
} 5 E}} 5 tan u 1 C 5 tan
e 1e
u 11
dx
dx
dx
E }
} 5 E }} 1 E }}
e 1e
e 1e
e 1e
dx
dx
E }
} 5 lim E }}
e 1e
e 1e
cos x dx
E
2x
E (ee) d1x 1
dx
(e 1 1)
5 lim
cos x dx 5 2e2x cos x 1 e2x sin x 2 e 2x cos x dx
2x
Ee
Let u 5 e x, du 5 e x dx
E
2x
E e 1dxe
53. }
5 }
x }
2x 5 }
2x 2}
x
x 2}
Since these two integrals converge, the given integral
converges.
b→`
54. The integral has an infinite discontinuity at x 5 0.
1
2
5 }}
Note that we cannot use a comparison test since
e2x cos x , 0 for some values on [0, `).
1
ln z
51. 0 # }} # }} on [e, `)
z
z
`
b
dz
dz
b
}} 5 lim
}} 5 lim ln )z) 5 lim (ln b 2 1) 5 `
z
e b→`
e
b→` e z
b→`
`
1
Since this integral diverges,
}} dz diverges, so the given
e z
E
E
3 4
E
integral diverges.
E
`
2`
dx
}
}5
x 2(1 1 e x )
E
21
`
1
1
4x
E
dx
}
}1
x 2(1 1 e x )
1
E
0
dx
}
}1
x 2(1 1 e x )
0
dx
}
}
2
(1 1 e x )
21 x
`
E
1
dx
}
}
x 2(1 1 e x )
1
x (1 1 e )
x
0 # }}2 # }
}
2
x on (0, 1] since 1 1 e # 4 on (0, 1].
E
E }4dx}x 5 lim 32}41}x 41b 5 lim 32}14} 1 }41}b 4 5 `
dx
Since this integral diverges, E }} diverges, so the
x (1 1 e )
1
0
dx
}}2 5 lim
4x
b→01
1
b
2
b→01
b→01
1
0
2
x
given integral diverges.
e2t
52. 0 # }} # e2t on [1, `)
Ïwt
E
`
1
2t
e
dt 5 lim
E
b
b→` 1
e
2t
dt
3 41
1
1
5 lim 12e 1 }}2 5 }}
e
e
5 lim 2e2t
b
b→`
55. x 2 2 7x 1 12 5 (x 2 4)(x 2 3)
2x 1 1
A
B
}
} 5 }} 1 }}
x 2 2 7x 1 12
x24
x23
2x 1 1 5 A(x 2 3) 1 B(x 2 4)
5 (A 1 B)x 2 3A 2 4B
2b
b→`
Since this integral converges, the given integral converges.
Equating coefficients of like terms gives
A 1 B 5 2 and 23A 2 4B 5 1.
Solving the system simultaneously yields A 5 9, B 5 27.
27 dx
2x 1 1
9 dx
E}
} dx 5 E}} 1 E}}
x23
x 2 7x 1 12
x24
2
5 9 ln )x 2 4) 2 7 ln )x 2 3) 1 C
Chapter 8 Review
8
x (x 1 2)
A
x12
B
x
C
x
D
x
56. }
3 } 5 }} 1 }} 1 }}
2 1 }}
3
8 5 Ax 3 1 Bx 2(x 1 2) 1 Cx(x 1 2) 1 D(x 1 2)
5 (A 1 B)x 3 1 (2B 1 C)x 2 1 (2C 1 D)x 1 2D
Equating coefficients of like terms gives
A 1 B 5 0, 2B 1 C 5 0, 2C 1 D 5 0, and 2D 5 8
1
x 3w
1w0w
x2w
1wxw
1w1
59. x 3 2 xqw
3
x}}}}}}}
1 0x2 2 x + 0
x11
x11
x3 1 1
x11
x11
}
}511}
}511}
} 5 1 1 }}
x(x 2 1)(x 1 1)
x3 2 x
x3 2 x
x(x 2 2 1)
A
x11
B
C
}} 5 }} 1 }} 1 }}
x
x(x 2 1)(x 1 1)
x21
x11
x 1 1 5 A(x 2 1)(x 1 1) 1 Bx(x 1 1) 1 Cx(x 2 1)
Solving the system simultaneously yields
5 (A 1 B 1 C)x 2 1 (B 2 C)x 2 A
A 5 21, B 5 1, C 5 22, D 5 4
dx
22 dx
4 dx
8 dx
2dx
E}
} 5 E}} 1 E}} 1 E}} 1 E}}
x
x
x
x (x 1 2)
x12
3
2
2
x
361
3
2
x
5 2ln )x 1 2) 1 ln )x) 1 }} 2 }}2 1 C
Equating coefficients of like terms gives
A 1 B 1 C 5 0, B 2 C 5 1, and 2A 5 1.
Solving the system simultaneously yields
57. t 3 1 t 5 t(t 2 1 1)
A 5 21, B 5 1, C 5 0
3t 2 1 4t 1 4
A
Bt 1 C
}
} 5 }} 1 }
}
t
t2 1 1
t3 1 t
x 11
dx
dx
E}
} dx 5 Edx 2 E}} 1 E}}
x 2x
x
x21
3
3
3t 2 1 4t 1 4 5 A(t 2 1 1) 1 (Bt 1 C)t
5 x 2 ln )x) 1 ln )x 2 1) 1 C
5 (A 1 B)t 2 1 Ct 1 A
x
60. x 2 1 4x 1 3qw
x 3w
1w4w
x 2w
1w
0xw
3
x}}}}}
1 4x 2 1 3x
23x
Equating coefficients of like terms gives
A 1 B 5 3, C 5 4 and A 5 4.
Solving the system simultaneously yields
A 5 4, B 5 21, C 5 4
3t 1 4t 1 4
4 dt
2t 1 4
E}
} dt 5 E}} 1 E}} dt
t
t 11
t 1t
4 dt
t dt
4 dt
5 E}} 2 E}} 1 E}}
t
t 11
t 11
2
3
2
2
2
1
2
5 4 ln )t) 2 }} ln (t 2 1 1) 1 4 tan21 t 1 C
At 1 B
Ct 1 D
1
}
}5}
}1}
}
t2 1 1
t2 1 3
(t 2 1 1)(t 2 1 3)
Equating coefficients of like terms gives
A 1 C 5 0, B 1 D 5 0, 3A 1 C 5 0, and 3B 1 D 5 1
Solving the system simultaneously yields
1
2
A 5 0, B 5 }}, C 5 0, D 5 2}}
1/2
1/2
dt
E}
} 5 E}} dt 2 E}} dt
(t 1 3)(t 1 1)
t 11
t 13
2
Equating coefficients of like terms gives
3
2
x 1 4x
3/2
9/2
E}
} dx 5 Ex dx 1 E}} dx 2 E}} dx
x 1 4x 1 3
x11
x13
3
5 (A 1 C)t 3 1 (B 1 D)t 2 1 (3A 1 C)t 1 3B 1 D
2
23x 5 (A 1 B)x 1 3A 1 B
9
2
Solving the system simultaneously yields A 5 }}, B 5 2}}.
1 5 (At 1 B)(t 2 1 3) 1 (Ct 1 D)(t 2 1 1)
2
23x 5 A(x 1 3) 1 B(x 1 1)
A 1 B 5 23, 3A 1 B 5 0
58. t 4 1 4t 2 1 3 5 (t 2 1 3)(t 2 1 1)
1
2
x 3 1 4x 2
23x
23x
}
}5x1}
} 5 x 1 }}
2
x 1 4x 1 3
x 2 1 4x 1 3
(x 1 1)(x 1 3)
23x
A
B
}} 5 }} 1 }}
(x 1 1)(x 1 3)
x11
x13
2
1
1
t
5 }} tan21 t 2 }} tan21 }} 1 C
2
2Ïw3
Ïw3
Evaluate the integrals using Formula 16, with x 5 t, a 5 1
in the first integral and a 5 Ï3w in the second.
2
2
x2
2
3
2
9
2
5 }} 1 }} ln )x 1 1) 2 }} ln )x 1 3) 1 C
362
Chapter 8 Review
1
3
dy
y(500 2 y)
A
1
B
}} 5 }} 1 }}
y
y(500 2 y)
500 2 y
61. }} 5 0.002 dx
p
2
1 1 9y 2 5 1 1 tan2 u 5 sec2 u
3 dy
sec u du
E}
} 5 E}}
1w
9w
)sec u)
Ï1ww
y
5 Esec u du
2
1 5 A(500 2 y) 1 By
2
5 (B 2 A)y 1 500A
1
500
p
2
1
3
63. y 5 }} tan u, dy 5 }} sec2 u du, 2}} , u , }}
1
500
where A 5 }}, B 5 }}.
5 ln )sec u 1 tan u) 1 C
1/500
dy
1/500
E}
} 5 E}} dy 1 E}} dy
y
y(500 2 y)
500 2 y
5 ln )Ï1ww
1w9w
y 2 1 3y) 1 C
1
500
1
500
5 }} ln )y) 2 }} ln )500 2 y) 1 C1
)
)
1
y
5 }} ln }} 1 C1
500
500 2 y
)
)
1
y
}} ln }} 1 C1 5 0.002x 1 C2
500
500 2 y
)
)
y
ln }} 5 x 1 C
500 2 y
1
3
p
2
1
3
p
2
64. t 5 }} sin u, dt 5 }} cos u du, 2}} # u # }}
1 2 9t 2 5 1 2 sin2 u 5 cos2 u
2
2
Substitute x 5 0, y 5 20.
u
sin 2u
6
12
u
sin u cos u
5 }} 1 }} 1 C
6
6
sin21 3t
3tÏw
1w
9w
t2
2w
5 }} 1 }} 1 C
6
6
1
1
5 }} sin21 3t 1 }}tÏ1ww
2w9w
t2 1 C
6
2
1
Use Figure 8.18(b) with a 5 }} and x 5 t.
3
5 }} 1 }} 1 C
20
1
}} 5 ke0 or k 5 }}
480
24
y
1
}} 5 }} e x
500 2 y
24
24y 5 500e x 2 yex
(e x 1 24)y 5 500e x
500 e x
e 1 24
y5}
x }
3
5
p
2
3
5
65. x 5 }} sec u, dx 5 }} sec u tan u, 0 # u , }}
500
y 5 }}
1 1 24 e2x
25x 2 2 9 5 9 sec2 u 2 9 5 9 tan2 u
dy
dx
62. }
} 5 }}
y2 1 1
x11
dy
dx
}
} 5 }}
y2 1 1
x11
E
3 sec u tan u du
5 dx
E}
} 5 E }}
3 )tan u)
2w9
Ï2w5ww
x w
5 Esec u du
2
tan21 y 1 C1 5 ln )x 1 1) 1 C2
tan21 y 5 ln )x 1 1) 1 C
5 ln )sec u 1 tan u) 1 C1
p
Substitute x 5 0, y 5 }}
4
p
tan21 }} 5 C
4
)3
)
Ï2w5wxw2w
5x
2w9
5 ln }} 1 }} 1 C1
p
4
p
y 5 tan ln )x 1 1) 1 tan21 }}
4
tan21 y 5 ln )x 1 1) 1 tan21 }}
1
1
3
Use Figure 8.18(a) from the text with a 5 }}.
EÏ1ww2w9wt dt 5 E)cos u)1}13} cos u2 du
1
5 E}} cos u du
3
1 1 cos 2u
5 E}} du
6
y
}} 5 ke x
500 2 y
E
Integrate by using Formula 88 with a 5 1 and x 5 u.
2
3
5 ln (5x 1 Ï2w5ww
x 2w
2w
9) 1 C
Integrate by using Formula 88 with a 5 1 and x 5 u.
3
5
Use Figure 8.18(c) with a 5 }}.
Chapter 8 Review
p
2
68. For x $ 0, y $ 0 on [0, `).
p
2
E xe
Evaluate Exe
66. x 5 sin u, dx 5 cos u du, 2}} # u # }}
`
Area 5
2x
4 sin u cos u
4x dx
E}
} 5 E}} du
(1 2 x )
)cos u)
4(1 2 cos u)
5 E}} du
cos u
5 E(4 sec u 2 4) du
2
2
2 3/2
3
2
b
xe2x dx
dx by using integration by parts.
u5x
dv 5 e2x dx
du 5 dx
v 5 2e2x
Exe
2
E
b→` 0
0
2x
1 2 x 2 5 cos2 u
dx 5 lim
2x
E
dx 5 2xe2x 1 e2x dx 5 2xe2x 2 e2x 1 C
2
3
4
Area 5 lim 2xe2x 2 e2x
b→`
5 4 tan u 2 4u 1 C
5 lim [2be
2b
b→`
4x
5 }} 2 4 sin21 x 1 C
2wx 2w
Ïw1w
2b
2e
b
0
1 1]
b
5 2lim }}b 1 1
b→` e
Use Figure 8.18(b) with a 5 1.
1
5 2lim }}b 1 1 5 1
b→` e
67. For x $ 0, y $ 0 on (0, 1].
Volume 5
E
1
p(2ln x)2 dx
E
0
5p
1
(ln x) dx
0
E (ln x)
b→0
2
E
1
(ln x)2 dx
b
dx by using integration by parts.
u 5 (ln x)2
dv 5 dx
2 ln x
du 5 }} dx
x
v5x
E (ln x)
2
E
E
Evaluate 2 ln x dx by using integration by parts.
u 5 2 ln x
dv 5 dx
2
du 5 }} dx
x
v5x
E2 ln x dx 5 2x ln x 2 E2 dx 5 2x ln x 2 2x 1 C
E(ln x) dx 5 x (ln x) 2 2x ln x 1 2x 1 C
2
2
3
4
Area 5 p lim1 x(ln x)2 2 2x ln x 1 2x
b→0
1
b
5 p lim1 [2 2 b(ln b) 1 2b ln b 2 2b]
2
b→0
p(ln b)2
p ln b
1/b
1/b
b→0
b→0
2p(ln b)(1/b)
p/b
5 2p 2 lim1 }}
1 2 lim1 }}2
21/b2
b→0
b→0 21/b
5 2p 2 lim1 }} 1 2 lim1 }}
2p(ln b)
21/b
5 2p 2 lim1 }} 1 2 lim1 (2pb)
b→0
E
Substitute x 5 0, t 5 0
dx 5 x (ln x) 2 2 ln x dx
2
dx
}}2 5 k dt
(a 2 x)
dx
}}2 5 k dt 5 kt 1 C1
(a 2 x)
1
}} 1 C2 5 kt 1 C1
a2x
1
}} 5 kt 1 C
a2x
E
2
5 p lim1
Evaluate
dx
dt
69. (a) }} 5 k(a 2 x)2
b→0
2p/b
5 2p 2 lim1 }}
2 1 2p 2 lim1 2pb 5 2p
b→0 1/b
b→0
1
}} 5 C
a
1
1
}} 5 kt 1 }}
a
a2x
1
}} 5 a 2 x
kt 1 1/a
1
x 5 a 2 }}
kt 1 1/a
363
364
Section 9.1
69. continued
dx
(b) }} 5 k dt
(a 2 x)(b 2 x)
dx
}} 5 k dt 5 kt 1 C1
(a 2 x)(b 2 x)
1
A
B
}} 5 }} 1 }}
(a 2 x)(b 2 x)
a2x
b2x
E
E
1 5 A(b 2 x) 1 B(a 2 x)
Equating coefficients of like terms gives
2A 2 B 5 0 and bA 1 aB 5 1
Solving the system simultaneously yields
1
a2b
A 5 2}}, B 5 }}
21/(a 2 b)
1/(a 2 b)
dx
E}
} 5 E}} dx 1 E}} dx
a2x
b2x
(a 2 x)(b 2 x)
ln )a 2 x)
a2b
ln )b 2 x)
a2b
5 }} 2 }} 1 C2
1
a2b
) ab 22 xx )
5 }} ln }} 1 C2
)
)
)
a2x
1
}} ln }} 1 C2 5 kt 1 C1
b2x
a2b
a2x
ln }} 5 (a 2 b)kt 1 C
b2x
a2x
}} 5 De(a2b)kt
b2x
)
■ Section 9.1 Power Series (pp. 457–468)
Exploration 1
Power Series for Other Functions
1. 1 2 x 1 x 2 2 x 3 1 … 1 (2x)n 1 ….
2. x 2 x 2 1 x 3 2 x 4 1 … 1 (21)nx n11 1 ….
5 (2A 2 B)x 1 bA 1 aB
1
a2b
Chapter 9
Infinite Series
3. 1 1 2x 1 4x 2 1 8x 3 1 … 1 (2x)n 1 ….
4. 1 2 (x 2 1) 1 (x 2 1)2 2 (x 2 1)3 1 …
1 (21)n(x 2 1)n 1 ….
5. }} 2 }}(x 2 1) 1 }}(x 2 1)2 2 }}(x 2 1)3 1 …
1
3
1
3
1 n
1 32
1
3
1 2}} (x 2 1)n 1 ….
This geometric series converges for 21 , x 2 1 , 1,
which is equivalent to 0 , x , 2. The interval of convergence is (0, 2).
A Power Series for tan21 x
Exploration 2
1. 1 2 x 2 1 x 4 2 x 6 1 … 1 (21)nx 2n 1 ….
1
E}
} dt
11t
5 E (1 2 t 1 t
2. tan21 x 5
x
2
0
x
2
0
4
2 t 6 1 … 1 (21)nt 2n 1 …) dt
t3
t5
t7
t 2n11
3
5
7
2n 1 1
x3
x5
x7
x2n11
5 x 2 }} 1 }} 2 }} 1 … 1 (21)n}} ….
3
5
7
2n 1 1
3
5 t 2 }} 1 }} 2 }} 1 … 1 (21)n}} 1 …
Substitute t 5 0, x 5 0.
a
}} 5 D
b
a2x
a
}} 5 }}e(a2b)kt
b2x
b
1
3
4
x
0
3. The graphs of the first four partial sums appear to be converging on the interval (21, 1).
ab 2 bx 5 abe (a2b)kt 2 axe (a2b)kt
x(ae (a2b)kt 2 b) 5 ab(e (a2b)kt 2 1)
ab(e (a2b)kt 2 1)
ae
2b
x 5 }}
(a2b)kt
[25, 5] by [23, 3]
4. When x 5 1, the series becomes
e bkt
Multiply the rational expression by }b}
.
e kt
akt
bkt
ab(e 2 e )
x 5 }}
ae akt 2 be bkt
(21)n
2n 1 1
1 2 }} 1 }} 2 }} 1 … 1 }} 1 ….
1
3
1
5
1
7
This series does appear to converge. The terms are getting
smaller, and because they alternate in sign they cause the
partial sums to oscillate above and below a limit. The two
calculator statements shown below will cause the successive partial sums to appear on the calculator each time the
ENTER button is pushed. The partial sums will appear to
be approaching a limit of p/4 (which is
tan21(1)), although very slowly.
Section 9.1
Exploration 3
A Series with a Curious Property
x2
2!
x3
3!
xn
n!
1. f 9(x) 5 1 1 x 1 }} 1 }} 1 … 1 }} 1 ….
2. f (0) 5 1 1 0 1 0 1 … 5 1.
3. Since this function is its own derivative and takes on the
value 1 at x 5 0, we suspect that it must be e x.
dy
dx
4. If y 5 f (x), then }} 5 y and y 5 1 when x 5 0.
365
(21)1
1
(21)2
1
u2 5 }} 5 }}
2
2
(21)3
1
u3 5 }} 5 2}}
3
3
(21)4
1
u4 5 }} 5 }}
4
4
(21)30
1
u30 5 }} 5 }}
30
30
2. u1 5 }} 5 21
6
2
18
6
54
18
3. (a) Since }} 5 }} 5 }} 5 3, the common ratio is 3.
5. The differential equation is separable.
dy
}} 5 dx
y
dy
}} 5 dx
y
E
E
ln )y) 5 x 1 C
y 5 Ke
k
1 5 Ke0 ⇒ K 5 1
[ y 5 e x.
6. The first three partial sums are shown in the graph below. It
is risky to draw any conclusions about the interval of
convergence from just three partial sums, but so far the
convergence to the graph of y 5 e x only looks good on
(21, 1). Your answer might differ.
(b) 2(39) 5 39,366
(c) an 5 2(3n21)
24
8
21
2
2
24
1
2
1
2
4. (a) Since }} 5 }} 5 }} 5 2}}, the common ratio is 2}}.
1 9
1 22
(b) 8 2}}
1
64
5 2}}
1 n21
1 22
(c) an 5 8 2}}
5 8(20.5)n21
1
12n
n
2
5. (a) We graph the points n, }}
for n 5 1, 2, 3, … .
2
(Note that there is a point at (1, 0) that does not show
in the graph.)
[0, 25] by [20.5, 0.5]
[25, 5] by [23, 3]
7. The next three partial sums show that the convergence
extends outside the interval (21, 1) in both directions, so
(21, 1) was apparently an underestimate. Your answer in
#6 might have been better, but unless you guessed “all real
numbers,” you still underestimated! (See Example 3 in
Section 9.3.)
12n
n
(b) lim an 5 lim }}
2 50
n→`
n→`
1 1
1 n
for n 5 1, 2, 3, … .
n
22
6. (a) We graph the points n, 1 1 }}
[0, 23.5] by [21, 4]
[25, 5] by [23, 3]
Quick Review 9.1
4
4
3
112
4
4
u2 5 }} 5 }} 5 1
4
212
4
4
u3 5 }} 5 }}
5
312
4
2
4
u4 5 }} 5 }} 5 }}
6
3
412
1
4
4
u30 5 }} 5 }} 5 }}
8
30 1 2
32
1
1 n
5e
n
(b) lim an 5 lim 1 1 }}
n→`
n→`
2
7. (a) We graph the points (n, (21)n) for n 5 1, 2, 3, … .
1. u1 5 }} 5 }}
[0, 23.5] by [22, 2]
(b) lim an does not exist because the values of an
n→`
oscillate between 21 and 1.
366
Section 9.1
1
1 2 2n
1 1 2n
2
8. (a) We graph the points n, }} for n 5 1, 2, 3, … .
1
3
1
9
2. (a) Note that a0 5 1, a1 5 }}, a2 5 }}, and so on. Thus
1 n
132
an 5 } } .
1
2
1
3
(b) Note that a1 5 1, a2 5 2}}, a3 5 }}, and so on. Thus
(21)n21
n
an 5 }}.
[0, 23.5] by [22, 2]
1 2 2n
n→` 1 1 2n
(c) Note that a0 5 5, a1 5 0.5, a2 5 0.05, and so on. Thus
2
2
(b) lim an 5 lim }} 5 2}} 5 21
n→`
1
1
n
5
10
an 5 5(0.1)n 5 }}n .
2
9. (a) We graph the points n, 2 2 }} for n 5 1, 2, 3, … .
`
1 n21
1 22
3. Different, since the terms of ∑ 2}}
n51
alternate
between positive and negative, while the terms of
`
∑ 21}12}2
n21
are all negative.
n51
4. The same, since both series can be represented as
[0, 23.5] by [21, 3]
1
1
n
1 2 }} 1 }} 2 }} 1 … .
1
2
2
(b) lim an 5 lim 2 2 }} 5 2
n→`
n→`
1
ln (n 1 1)
n
2
10. (a) We graph the points n, }} for n 5 1, 2, 3, … .
1
4
1
8
5. The same, since both series can be represented as
1 2 }} 1 }} 2 }} 1 … .
1
2
1
4
1
8
`
1 n21
1 22
6. Different, since ∑ 2}}
n51
`
∑
n51
[0, 23.5] by [21, 1]
2 n
132
7. Converges; ∑ }}
ln (n 1 1)
(b) lim an 5 lim }} 5 lim } 5 0
1
n
n→`
n→`
n→`
n50
1
8
1 53
5}
2
1 2 }}
3
5
}}
4
5 2 n
5
15
5 3 }} 5 }}
}} }} 5 }
2
4 3
4
4
1 2 }}
`
1. (a) Let un represent the value of * in the n th term, starting
1
u1
1
u2
1 1
4 u3
1
9
with n 5 1. Then }} 5 1, 2}} 5 2}}, }} 5 }},
1
16
1
4
8. Diverges, because the terms do not approach zero.
Section 9.1 Exercises
1
u4
1
2
(21)n
1
1
1
}n2
} 5 21 1 }} 2 }} 1 }} 2 … .
2 1
2
4
8
`
1
}}
(n 1 1)
5 1 2 }} 1 }} 2 }} 1 … but
and 2}} 5 2}}, so
1 21 2
9. Converges; ∑
n50
12
3
10. Diverges, because the common ratio is $ 1 and the terms
do not approach zero.
u1 5 1, u2 5 4, u3 5 9, and u4 5 16. We may write
11. Diverges, because the terms alternate between 1 and 21
and do not approach zero.
un 5 n2, or * 5 n2.
12. Converges; ∑ 3(20.1)n 5 }} 5 }}
`
3
1 2 (20.1)
n50
(b) Let un represent the value of * in the nth term, starting
1
u0
1
u1
1 1
4 u2
1
9
with n 5 0. Then }} 5 1, 2}} 5 2}}, }} 5 }}, and
1
1
2}} 5 2}}, so u0 5 1, u1 5 4, u2 5 9, and
u3
16
u3 5 16. We may write un 5 (n 1 1)2, or * 5 (n 1 1)2.
21
21
21
1
2
3
21
…
(21)6 }}
1
, which is the same as the desired
42
1 2
1 2
4
5
(21)3 }}
2 1 (21) }}
2 1 (21) }}
2 1
series. Thus let * 5 3.
14
2
p
13. Converges; ∑ sin n }} 1 np
n50
1
1
2
3
2 1 1}Ï}2w 2 1 12}Ï}2w 2
1
5 1 1 2}}
Ïw2
1
1
1…
1
}}
Ïw2
1 5 }}
1 2 2}}
Ï2w 1 1
Ï2w
Ï2w(Ï2w 2 1)
}}}
w
2 2 Ï2
5 (Ï2w 1 1)(Ï2w 2 1) 5 }} 5 2 2 Ï2w
221
`
(c) If * 5 3, the series is
1 2
1 2
`
30
11
1
2
5 ∑ 2}}
n50
Ïw2
1
n
5
1
2
14. Diverges, because the terms do not approach zero.
Section 9.1
`
e n
1p2
15. Converges; since }} < 0.865 , 1, ∑ }}
e
p
n51
p
p2e
5 }}
`
`
5n
6
n50
`
n50
`
5}
e
1p2
n50
p
4
1
1 2 tan x
p
p
1
function f (x) 5 }}, 2}} 1 kp , x , }} 1 kp.
4
4
1 2 tan x
162
1
2
1 1
)2x) , 1 and the interval of convergence is 2}}, }} . Since
2 2
1
the sum of the series is }}, the series represents the
1 2 2x
1
1
1
function f (x) 5 }}, 2}} , x , }}.
2
2
1 2 2x
`
`
n50
n50
p
4
sum of the series is }}, the series represents the
n
n50
n50
2}} 1 kp , x , }} 1 kp, where k is any integer. Since the
17. Since ∑ 2 x 5 ∑ (2x) , the series converges when
n n
n50
)tan x) , 1. Thus, the series converges for
1 2 }}
1 5 n
5}
5 51
6 6
1 2 }}
12
`
22. Since ∑ tan n x 5 ∑ (tan x)n, the series converges when
1
1
}}
6
16. Converges; ∑ }n1
}1 5 ∑ }} }}
`
18. Since ∑ (21)n(x 1 1)n 5 ∑ [2(x 1 1)]n, the series
23. (a) Since the terms are all positive and do not approach
zero, the partial sums tend toward infinity.
(b) The partial sums are alternately 1 and 0.
(c) The partial sums alternate between positive and
negative while their magnitude increases toward
infinity.
`
e np
p
`
n50
n50
ep
p
common ratio r 5 }}e < 1.03, which is greater than one.
convergence is (22, 0). Since the sum of the series is
1
1
}} 5 }}, the series represents the function
1 2 [2(x 1 1)]
x12
1
f (x) 5 }}, 22 , x , 0.
x12
19. Since ∑
n50
`
25.
∑ x n 5 20
n50
1
}} 5 20, )x) , 1
12x
1 5 20 2 20x
`
1 n
32x n
2}} (x 2 3)n 5
}} , the series
2
2
n50
1 2
∑1
)
32x
2
2
20x 5 19
19
20
x 5 }}
)
converges when }} , 1 and the interval of convergence
1
2
x21
is (1, 5). Since the sum of the series is }} 5 }}.
(3 2 x)
1 2 }}
2
2
x21
the series represents the function f (x) 5 }}, 1 , x , 5.
`
1
x21 n
2
2
20. For ∑ 3 }} , the series converges when
n50
26. One possible answer:
For any real number a Þ 0,
use }} 1 }} 1 }} 1 }} 1 }} 1 … . To get 0,
a
2
a
a
a
a
4
8
16
32
1
1
1
1
1
use 1 2 }} 2 }} 2 }} 2 }} 2 }} … .
2
4
8
16
32
27. Assuming the series begins at n 5 1:
`
(a)
)}2}) , 1 and the interval of convergence is (21, 3).
x21
3
ep n
1p 2
24. Since ∑ }}
ne 5 ∑ }}
e , this is a geometric series with
converges when )2(x 1 1)) , 1 and the interval of
`
2
} 5 5, )r) , 1
∑ 2r n21 5 }
12r
n51
2 5 5 2 5r
5r 5 3
6
32x
Since the sum of the series is }} 5 }}, the series
(x 2 1)
1 2 }}
2
6
32x
`
`
n50
n51
n
n50
)sin x) , 1. Thus, the series converges for all values of x
p
2
p
2
except odd integer multiples of }}, that is, x Þ (2k 1 1)}}
1
1 2 sin x
for integers k. Since the sum of the series is }}, the
1
1 2 sin x
series represents the function f (x) 5 }},
p
2
x Þ (2k 1 1)}}.
3 n21
152
Series: ∑ 2 }}
21. Since ∑ sin x 5 ∑ (sin x) , the series converges when
n
3
5
r 5 }}
represents the function f (x) 5 }}, 21 , x , 3.
`
367
13
}}
`
∑
2
13
(b)
}}r n21 5 } 5 5, )r) , 1
12r
n51 2
13
}} 5 5 25r
2
3
5r 5 2}}
2
3
r 5 2}}
10
`
13
3 n21
Series:
}} 2}}
10
n51 2
^
1 2
368
Section 9.1
21
100
1
100
28. Let a 5 }} and r 5 }}, giving
0.2w1w 5 0.21 1 0.21(0.01) 1 0.21(0.01)2
1 0.21(0.01) 1 …
3
`
5 ∑ 0.21(0.01)n
n50
0.21
1 2 0.01
0.21
5 }}
0.99
7
5 }}
33
5 }}
234
1000
33. 1.4
w1w4w 5 1 1 0.414 1 0.414(0.001) 1 0.414(0.001)2
`
5 1 1 ∑ 0.414(0.001)n
n50
0.414
1 2 0.001
46
5 1 1 }}
111
157
5 }}
111
5 1 1 }}
34. 1.241
w2w3w 5 1.24 1 0.00123 1 0.00123(0.001)
1 0.00123(0.001)2 1 …
1
1000
29. Let a 5 }} and r 5 }}, giving
0.2w3w4w 5 0.234 1 0.234(0.001) 1 0.234(0.001)2
1 0.234(0.001)3 1 …
`
5 ∑ 0.234(0.001)n
n50
0.234
1 2 0.001
0.234
5 }}
0.999
26
5 }}
111
`
5 1.24 1 ∑ }}
0.00123
1
2 0.001
n51
0.00123
5 1.24 1 }}
0.999
124
41
5 }} 1 }}
100
33,300
41,333
5 }}
33,300
5 }}
30. 0.7
w 5 0.7 1 0.7(0.1) 1 0.7(0.1)2 1 0.7(0.1)3 1 …
`
5 ∑ 0.7(0.1)n
n50
0.7
1 2 0.1
0.7
5 }}
0.9
7
5 }}
9
5 }}
35. 3.1
w4w2w8w5w7w 5 3 1 0.142857(1 1 0.000001
1 0.0000012 1 …)
5
n50
1
0.142857
0.999999
1
5 3 1 }}
7
22
5 }}
7
5 3 1 }}
36. Total distance 5 4 1 2[4(0.6) 1 4(0.6)2 1 4(0.6)3 1 …]
`
5 4 1 2 ∑ 2.4(0.6)n
n50
∑
32. 0.06
w 5 0.06 1 0.06(0.1) 1 0.06(0.1)2 1 0.06(0.1)3 1 …
`
5 ∑ 0.06(.1)n
n50
0.06
5 }}
1 2 0.1
0.06
5 }}
0.9
1
5 }}
15
1 1 2 0.000001 2
5 3 1 (0.142857) }}
31. 0.d
w 5 }}[1 1 0.1 1 0.12 1 0.13 1 …]
d
10
`
d
5 }}
(0.1)n
10 n50
d
1
5 }} }}
10 1 2 0.1
d 1
5 }} }}
10 0.9
d
5 }}
9
`
3 1 0.142857 ∑ 0.000001n
2.4
1 2 0.6
5 4 1 2 ? }}
5412?6
5 16m
37. Total time 5
1 }
!}§4§.9} 1 23!}
§§4§.}
4.9
9§§ !§
4(0.6)
4
4(0.6)2
1 …4
!}
§§4§.}
9§
4(0.6)
4
5 !}
[1 1 Ï0w.6
w 1 (Ï0w.6
w)
§4§.9} 1 2!}
§§4.§}
9§§
1
5
4(0.6)3
? }}
!}§4§.9} 1 2!}
§§4§.}
9§§ 1 2 Ï0
w.6
w
4
< 7.113 sec
4(0.6)
1
2
1 …]
369
Section 9.1
38. The area of each square is half of the area of the preceding
`
1 n
122
square, so the total of all the areas is ∑ 4 }}
n50
4
2
5}
1 58m .
1 2 }}
Series: 3 1 3x 3 1 3x 6 1 … 1 3x 3n 1 …
`
Interval: The series converges when )x 3) , 1, so the interval
1 2
2
39. Total area 5 ∑ 2 n ? }} ? p }}n
5∑
1 2
1
2
of convergence is (21, 1).
1 n
p
}} ? }}
2
2
12
p 1 n
5 ∑ }} 1}}2
4 2
n51
`
1
1 1 (x 2 4)
and the common ratio is r 5 2(x 2 4).
p
}}
4
Series: 1 2 (x 2 4) 1 (x 2 4)2 2 … 1 (21)n(x 2 4)n 1 …
5}
1
122
1 2 }}
Interval: The series converges when )x 2 4) , 1, so the
interval of convergence is (3, 5).
40. (a) S 2 rS 5 (a 1ar 1 ar 2 1 ar 3 1 ... 1 ar n22 1 ar n21)
2(ar 1 ar 2 1 ar 3 1 ar 4 1 ... 1 ar n21 1 ar n)
5 a 2 ar n
1
4
Interval: The series converges when )x 2 1) , 1, so the
a 2 ar n
12r
interval of convergence is (0, 2).
41. Using the notation Sn 5 a 1 ar 1 ar 2 1 ar 3 1 ... 1 ar n21,
`
a
12r
Series: 1 1 (x 2 1) 1 (x 2 1)2 1 … 1 (x 2 1)n 1 …
n51
5 lim Sn 5 lim }} 5 }}.
If )r) . 1 or r 5 21, then r n has no finite limit as n → `,
`
a 2 ar n
12r
1
12 (x 2 1)
The first term is a 5 1 and the common ratio is r 5 x 2 1.
If )r) , 1, then lim r n 5 0 and so ∑ ar n21
a
12r
1
22x
47. Rewriting }} as }} and comparing with }},
a 2 ar n
12r
the formula from Exercise 40 is Sn 5 }}.
a 2 ar n
n→` 1 2 r
a
12r
1
1
1
1
}} 2 }}(x 2 1) 1 }}(x 2 1)2 2 … 1 }}(21)n(x 2 1)n 1 …
4
4
4
4
n
S 5 }}
n→`
2
Series:
S 2 rS 5 a 2 ar n
S (1 2 r) 5 a 2 ar
1
1
1
4 1 1 (x 2 1)
46. Comparing }} }} with }}, the first term is
a 5 }} and the common ratio is r 5 2(x 2 1) 5 1 2 x.
(b) Just factor and divide by 1 2 r:
n→`
a
12r
45. Comparing }} with }}, the first term is a 5 1
n50
p
5 }}
2
a
12r
the common ratio is r 5 x 3.
122
n51
`
3
12x
44. Comparing }}3 with }}, the first term is a 5 3 and
so the expression }} has no finite limit and ∑ ar n21
n51
diverges.
Interval: The series converges when )x 2 1) , 1, so the
interval of convergence is (0, 2).
Alternate solution:
1
If r 5 1, then the nth partial sum is na, which goes to 6`.
1
1 1 3x
a
12r
42. Comparing }} with }}, the leading term is a 5 1 and
the common ratio is r 5 23x.
Series: 1 2 3x 1 9x 2 … 1 (23x) 1 …
2
n
Interval: The series converges when )23x) , 1, so the
1
1 1
3 3
2
interval of convergence is 2}}, }} .
x
a
43. Comparing }} with }}, the first term is a 5 x and
1 2 2x
12r
the common ratio is r 5 2x.
Series: x 1 2x 2 1 4x 3 1 … 1 2n21x n 1 …
Interval: The series converges when )2x) , 1, so the interval
1
1 1
2 2
2
of convergence is 2}}, }} .
2 1 1 2 }} 2
122
1
1
a
and comparing with }},
Rewriting }} as }} }
x
22x
1
x
the first is a 5 }} and the common ratio is r 5 }}.
2
2
12r
Series: }} 1 }}x 1 }}x 2 1 … 1 }n11
}x n 1 …
1
2
1
4
1
8
1
2
)2)
x
Interval: The series converges when }} , 1, so the interval
of convergence is (22, 2).
`
48. 1 1 e b 1 e 2b 1 e 3b 1 … 5 ∑ (e b)n
n50
1
12e
5 }}b 5 9
1 5 9 2 9e b
9e b 5 8
8
9
e b 5 }}
192
8
b 5 ln }} 5 ln 8 2 ln 9
370
Section 9.1
`
1 n
122
49. (a) When t 5 1, S 5 ∑ }}
n50
51. Since }} 5 1 2 (x 2 1) 1 (x 2 1)2 2 (x 2 1)3 1 … 1
1
x
1
5}
1 5 2.
122
1 2 }}
) )
t
(b) S converges when }} , 1, or )t) , )1 1 t).
11t
(21)n(x 2 1)n 1 … , we may write ln x 5
(x 2 1)2
(x 2 1)3
2
3
(21)n(x 2 1)n
1 }}
n
2t , 2(1 1 t), which is always false.
For t $ 0, the inequality is equivalent to t , 1 1 t,
1
2
n50
t
n
Using the result from Example 4, we have:
2(1 2 x)23 5 0 1 2 1 6x 1 12x 2 1 ... 1 n (n21)x n22 1 …
11t
(1 1 t) 2 t
1
5 }}
5 }} 5 1 1 t, so
t
1 2 }}
11t
S . 10 when t . 9.
Thus, f (x) 5 2 1 6x 1 12x 2 1 … 1 n(n 2 1)x n22 1 … .
Replacing n by n 1 2, this may be written as
f (x) 5 2 1 6x 1 12x 2 1 (n 1 2)(n 1 1)x n 1 … .
4
11t
a
12r
50. (a) Comparing f (t) 5 }}2 with }}, the first term
is a 5 4 and the common ratio is r 5 2t 2.
First four terms: 4 2 4t 1 4t 2 4t
2
n
dx 5 (1 2 x)22 1 C.
1 nx n21 1 …)
(c) For t . 2}}, we have
11 1 t2
Ef (x) dx 5 E2(1 2 x)
d
d
}} (1 2 x)22 5 }} (1 1 2x 1 3x 2 1 4x 3 1 …
dx
dx
1
2
Thus, S converges for all t . 2}}.
`
4
6
2n
General term: (21) (4t )
(b) Note that G (0) 5 0, so the constant term of the power
series for G (x) will be 0. Integrate the terms for f (x) to
obtain the terms for G (x).
4
3
4
5
4
7
First four terms: 4x 2 }}x 3 1 }}x 5 2 }}x 7
1 2n 1 1 2
4
General term: (21)n }} x 2n11
Interval: The series converges when )x) , 1, so the interval
of convergence is (21, 1).
53. (a) No, because if you differentiate it again, you would
have the original series for f, but by Theorem 1, that
would have to converge for 22 , x , 2, which
contradicts the assumption that the original series
converges only for 21 , x , 1.
(b) No, because if you integrate it again, you would have
the original series for f, but by Theorem 2, that would
have to converge for 22 , x , 2, which contradicts
the assumption that the original series converges only
for 21 , x , 1.
e
2
54. Let L 5 lim an. Then by definition of convergence, for }}
n→`
(c) The series in part (a) converges when )2t 2) , 1, so the
there corresponds an N such that for all m and n,
e
2
e
2
n, m . N ⇒ )am 2 L) , }} and )an 2 L) , }}.
interval of convergence is (21, 1).
Now,
(d) The two numbers are x 5 61, which result in the
convergent series
1 2n 1 1 2
G (1) 5 4 2 }} 1 }} 2 }} 1 … 1 (21)n }} 1 …
4
3
4
5
4
7
4
and
G (21)
1 2n 1 1 2
5 24 1 }} 2 }} 1 }} 2 … 1 (21)n21 }} 1 … ,
4
3
respectively.
4
5
4
7
1
}} dt
t
(1 2 x)22 5 1 1 2x 1 3x 2 1 4x 3 1 … 1 nx n21 1 …
which is always true.
S 5 ∑ }}
1
52. To determine our starting point, we note that
23
1
2
2t , 1 1 t, which is true when t . 2}}.
(x 2 1)4
4
x
5 x 2 1 2 }} 1 }} 2 }} 1 …
For t , 21, this inequality is equivalent to
For 21 # t , 0, the inequality is equivalent to
E
4
)am 2 an) 5 )am 2 L 1 L 2 an)
e
2
e
2
# )am 2 L) 1 )an 2 L) , }} 1 }} = e
whenever m . N and n . N.
Section 9.2
55. Given an e . 0, by definition of convergence there
corresponds an N such that for all n , N, )L1 2 an) , e and
)L2 2 an) , e. (There is one such number for each series,
and we may let N be the larger of the two numbers.) Now
)L2 2 L1) 5 )L2 2 an 1 an 2 L1)
# )L2 2 an) 1 )an 2 L1)
,e1e
5 2e.
)L2 2 L1) , 2e says that the difference between two fixed
values is smaller than any positive number 2e. The only
nonnegative number smaller than every positive number
is 0, so )L2 2 L1) 5 0 or L1 5 L2.
Exploration 2
56. Consider the two subsequences ak(n) and ai(n), where
Exploration 3
lim ak(n) 5 L1, lim ai(n) 5 L2, and L1 Þ L2. Given an e . 0
n→`
n→`
there corresponds an N1 such that for k(n) . N1,
)ak(n) 2 L1) , e, and an N2 such that for i(n) . N2,
A Power Series for the Cosine
1. cos (0) 5 1
cos9 (0) 5 2sin (0) 5 0
cos0 (0) 5 2cos (0) 5 21
cos(3) (0) 5 sin (0) 5 0
etc.
The pattern 1, 0, 21, 0 will repeat forever. Therefore,
x2
2
x2
2
x4
4!
Approximating sin 13
4. 20 terms.
Quick Review 9.2
1
x21
Since the limit of a sequence is unique (by Exercise 55),
f 9(x) 5 2(x 2 1)22
an does not converge and hence diverges.
f 0(x) 5 2(x 2 1)23
3n 1 1
57. (a) lim }} 5 3
n→` n 1 1
x 2n
(2n)!
1. 0.4201670368…
2. f (x) 5 }}
n→`
x6
6!
2. A clever shortcut is simply to differentiate the previouslydiscovered series for sin x term-by-term!
implies that lim an 5 L1 and lim an 5 L2 where L1 Þ L2.
n→`
x6
6!
1 2 }} 1 }} 2 }} 1 … 1 (21)n}} 1 … .
)an 2 L1) , e and )an 2 L2) , e for infinitely many n. This
Let N 5 max {N1, N2}. Then for n . N, we have that
x4
4!
P6(x) 5 1 2 }} 1 }} 2 }}, and the Taylor series is
1. f (x) 5 e2x
f 9(x) 5 2e2x
f 0(x) 5 4e2x
f -(x) 5 8e2x
f (n)(x) 5 2ne2x
)ai(n) 2 L2) , e. Assume an converges.
f -(x) 5 26(x 2 1)24
(b) The line y 5 3 is a horizontal asymptote of the graph of
3x 1 1
x11
the function f (x) 5 }}, which means lim f (x) 5 3.
x→`
Because f (n) 5 an for all positive integers n,
it follows that lim an must also be 3.
n→`
■ Section 9.2 Taylor Series (pp. 469–479)
Exploration 1 Designing a Polynomial to
Specifications
1. Since P(0) 5 1, we know that the constant coefficient is 1.
Since P9(0) 5 2, we know that the coefficient of x is 2.
f (n)(x) 5 (21)nn!(x 2 1)2(n11)
3. f (x) 5 3x
f 9(x) 5 3x ln 3
f 0(x) 5 3x(ln 3)2
f -(x) 5 3x(ln 3)3
f (n)(x) 5 3x(ln 3)n
4. f (x) 5 ln x
f 9(x) 5 x 21
f 0(x) 5 2x 22
f -(x) 5 2x 23
f (4)(x) 5 26x 24
f (n)(x) 5 (21)n21(n 2 1)!x 2n for n $ 1
5. f (x) 5 x n
f 9(x) 5 nx n21
3
Since P0(0) 5 3, we know that the coefficient of x is }}.
2
f 0(x) 5 n(n 2 1)x n22
(The 2 in the denominator is needed to cancel the factor of
f -(x) 5 n(n 2 1)(n 2 2)x n23
2 that results from differentiating x 2.) Similarly, we find the
f (k)(x) 5 }}x n2k
2
4
5
coefficients of x 3 and x 4 to be }} and }}.
6
24
3
4
5
Thus, P(x) 5 1 1 2x 1 }}x 2 1 }}x 3 1 }}x 4.
2
6
24
371
n!
(n 2 k)!
n!
f (n)(x) 5 }}x 0 5 n!
0!
nx n21
n!
dy
dx
d xn
dx n!
dy
dx
d 2n(x 2 a)n
n!
dx
x n21
(n 2 1)!
6. }} 5 }} }} 5 }} 5 }}
2nn(x 2 a)n21
n!
2n(x 2 a)n21
( n 2 1) !
7. }} 5 }} }} 5 }} 5 }}
372
Section 9.2
x 2n11
(2n 1 1)!
3
dy
dx
d
dx
dy
dx
d (x 1 a)
dx (2n)!
2n
dy
dx
d (1 2 x)
n!
dx
n
(2n 1 1)x 2n
(2n 1 1)!
4
(21)nx 2n
(2n)!
8. }} 5 }} (21)n}} 5 (21)n}} 5 }}
2n(x 1 a)
(2n)!
2n21
(x 1 a)
(2n 2 1)!
2n
9. }} 5 }} }} 5 }} 5 }}
n21
n(1 2 x) (21)
n!
x2
2!
3
x4
4!
x 2n
(2n)!
5 (cos 2) 1 2 }} 1 }} 2 … 1 (21)n}} 1 …
3
3
5
x
x
5!
(2n 1 1)!
(cos 2)x 2
(sin 2)x 3
(cos 2)x 4
5 (cos 2) 2 (sin 2)x 2 }} 1 }} 1 }}
2!
3!
4!
(sin 2)x 5
2 }} 2 …
5!
(1 2 x)
(n 2 1)!
Section 9.2 Exercises
1. Substitute 2x for x in the Maclaurin series for sin x shown
x
3!
We need to write an expression for the coefficient of x k.
(21)n(cos 2)
(2n)!
(2x)3
(2x)5
(2x)2n11
3!
5!
(2n 1 1)!
n
2n11
4x 3
4x 5
(2
1
)
(
2x
)
5 2x 2 }} 1 }} 2 … 1 }} 1 …
3
15
(2n 1 1)!
sin 2x 5 2x 2 }} 1 }} 2 … 1 (21)n }} 1 …
This series converges for all real x.
2. Substitute 2x for x in the Maclaurin series for ln (1 1 x)
Thus the coefficient is
(21)int[(k11)/2](cos 2)
(21)k/2(cos 2)
}}, which is the same as }}}.
k!
k!
(21)n11(sin 2)
If k is odd, the coefficient is }} where
(2n 1 1)!
2n 1 1 5 k. Thus the coefficient is
(21)int[(k11)/2](cos 2)
(21)(k11)/2(sin 2)
}}, which is the same as }}}.
k!
(2n 1 1)!
(21)ABx n
n11
Hence the general term is }}, where A 5 int }} ,
n!
2
shown at the end of Section 9.2.
(2x)2
(2x)3
2
3
(2x)n
1 (21)n21}} 1 …
n
x2
x3
xn
5 2x 2 }} 2 }} 2 … 2 }} 2 …
2
3
n
ln (1 2 x) 5 (2x) 2 }} 1 }} 2 …
1
B 5 cos 2 if n is odd.
Another way to handle the general term is to observe that
of convergence is [21, 1).
21
3. Substitute x for x in the Maclaurin series for tan
p
2
1
2
2sin 2 5 cos 2 1 }} , 2cos 2 5 cos (2 1 p),
x
3 n!
1
shown at the end of Section 9.2.
(x 2)3
(x 2)5
(x 2)2n11
3
5
2n 1 1
6
10
n 4n12
x
x
(2
1
)
x
5 x 2 2 }} 1 }} 2 … 1 }} 1 …
3
5
2n 1 1
tan21 x 2 5 x 2 2 }} 1 }} 2 … 1 (21)n}} 1 …
1
np
2
24
and so on, so the general term is }} cos 2 1 }} x n.
The series converges for all real x.
This series converges when )x 2) # 1, so the interval of
x4
x 2n
4!
(2n)!
x4
(21)nx 2n11
x6
2
…
…
5 x 2 }} 1 }} 2
1 }} 1
2
(2n)!
24
convergence is [21, 1].
The series converges for all real x.
This series converges for all real x.
2
and B 5 sin 2 if n is even and
This series converges when 21 # 2x , 1, so the interval
x2
xn
2!
n!
7x 3
7x n11
5 7x 1 7x 2 1 }} 1 … 1 }}
2!
n!
4
If k is even, the coefficient is }} where 2n 5 k.
at the end of Section 9.2.
4. 7xe x 5 7x(1 1 x 1 }} 1 … 1 }} 1 …)
4
2n11
2 (sin 2) x 2 }} 1 }} 2 … 1(21)n}} 1 …
n 21
10. }} 5 }} }} 5 }} 5 2}}
2
5. cos (x 1 2) 5 (cos 2)(cos x) 2 (sin 2)(sin x)
x2
2!
1
6. x 2 cos x 5 x 2 1 2 }} 1 }} 2 … 1 (21)n}} 1 …
2
7. Factor out x and substitute x 3 for x in the Maclaurin series
1
12x
for }} shown at the end of Section 9.2.
1
2
x
1
}}3 5 x }}3
12x
12x
5 x[1 1 x 1 (x 3)2 1 … 1 (x 3)n 1 …]
3
5 x 1 x 4 1 x 7 1 … 1 x 3n11 1 …
The series converges for )x 3) , 1, so the interval of
convergence is (21, 1).
Section 9.2
8. Substitute 22x for x in the Maclaurin series for e x shown at
the end of Section 9.2.
(22x)2
(22x)n
2!
n!
(21)n2nx n
5 1 2 2x 1 2x 2 2 … 1 }} 1 …
n!
e 22x 5 1 1 (22x) 1 }} 1 … 1 }} 1 …
)
)x52
)x52 5 }14}, so }f 02(}!2) 5 }18}
3
f -(2)
1
f -(2) 5 26x24)
5 2}}, so }} 5 2}}
x52
8
3!
16
1
2
1
x22
P1(x) 5 }} 2 }}
2
4
1
x22
(x 2 2)2
P2(x) 5 }} 2 }} 1 }}
2
4
8
1
x22
(x 2 2)2
(x 2 2)3
P3(x) 5 }} 2 }} 1 }} 2 }}
2
4
8
16
P0(x) 5 }}
p
)x5p/4 5 }Ï2}w2
142
Ïw2
p
f 91}}2 5 cos x)
5 }}
x5p/4
4
2
p
f 01}}2
4
Ïw2
Ïw2
p
f 01}}2 5 2sin x)
5 2}}, so } 5 2}}
x5p/4
2!
4
2
4
10. f }} 5 sin x
p
1 2
f - }}
4
Ïw2
Ïw2
p
f - }} 5 2cos x
5 2}}, so } 5 2}}
x5p/4
3!
4
2
12
)
Ïw2
P0(x) 5 }}
2
Ï2w
Ïw2
p
P1(x) 5 }} 1 }} x 2 }}
1 2 21 4 2
Ï2w
Ïw2
Ï2w
p
p 2
P2(x) 5 }} 1 1}}21x 2 }}2 2 1}}21x 2 }}2
4
4
2
2
4
Ïw2
Ïw2
Ïw2
p
p 2
P3(x) 5 }} 1 1}}21x 2 }}2 2 1}}21x 2 }}2
4
4
2
2
4
Ï2w
p 3
2 1}}21x 2 }}2
4
12
2
p
)x5p/4 5 }Ï2}2w
142
Ïw2
p
f 91}}2 5 2sin x)
5 2}}
x5p/4
4
2
p
f 01}}2
4
Ïw2
Ï2w
p
f 01}}2 5 2cos x)
5 2}}, so } 5 2}}
x5p/4
2!
4
2
4
11. f }} 5 cos x
p
1 2
f - }}
4
Ïw2
Ïw2
p
f - }} 5 sin x
5 }}, so } 5 }}
x5p/4
3!
4
2
12
)
1 2
)x54 5 }4}
1
f 0(4)
5 2}}
)x54 5 2}3}2 , so }2}
!
64
1
4
1
f 0(4) 5 2}}x23/2
f -(4)
1
5 }}
)x54 5 }256}, so }3}
!
512
3
1
P0(x) 5 2
1
4
5 2}}
f 0(2) 5 2x23
1 2
1
2
f 9(4) 5 }}x21/2
3
8
1
1
5 }}
x x52
2
f 9(2) 5 2x22
)x54 5 2
f -(4) 5 }}x25/2
The series converges for all real x.
9. f (2) 5 }}
12. f(4) 5 x1/2
x24
4
x24
(x 2 4)2
P2(x) 52 1 }} 2 }}
4
64
x24
(x 2 4)2
(x 2 4)3
P3(x) 5 2 1 }} 2 }} 1 }}
4
64
512
P1(x) 5 2 1 }}
13. (a) Since f is a cubic polynomial, it is its own Taylor
polynomial of order 3.
P3(x) 5 x 3 2 2x 1 4 or 4 2 2x 1 x 3
(b) f (1) 5 x 3 2 2x 1 4
f 9(1) 5 3x 2 2 2
)x51 5 3
)x51 5 1
)x51 5 6, so }f 02(}!1) 5 3
f 0(1) 5 6x
f -(1) 5 6
f -(1)
}51
)x51 5 6, so }
3!
P3(x) 5 3 1 (x 2 1) 1 3(x 2 1)2 1 (x 2 1)3
14. (a) Since f is a cubic polynomial, it is its own Taylor
polynomial of order 3.
P3(x) 5 2x 3 1 x 2 1 3x 2 8 or 28 1 3x 1 x 2 1 2x 3
(b) f (1) 5 2x 3 1 x 2 1 3x 2 8
f 9(1) 5 6x 2 1 2x 1 3
f 0(1) 5 12x 1 2
)x51 5 22
)x51 5 11
f 0(1)
}57
)x51 5 14, so }
2!
f 9(1)
}52
)x51 5 12, so }
3!
f -(1) 5 12
P3(x) 5 22 1 11(x 2 1) 1 7(x 2 1)2 1 2(x 2 1)3
15. (a) Since f (0) 5 f 9(0) 5 f 0(0) 5 f -(0) 5 0, the Taylor
polynomial of order 3 is P3(0) 5 0.
)x51 5 1
(b) f (1) 5 x 4
f 9(1) 5 4x 3
)x51 5 4
f 0(1) 5 12x 2
f 0(1)
}56
)x51 5 12, so }
2!
Ïw2
P0(x) 5 }}
f -(1) 5 24x
Ïw2
Ïw2
p
P1(x) 5 }} 2 }} x 2 }}
P3(x) 5 1 1 4(x 2 1) 1 6(x 2 1)2 1 4(x 2 1)3
2
1 2 21 4 2
Ïw2
Ïw2
Ïw2
p
p 2
P2(x) 5 }} 2 1}}21x 2 }}2 2 1}}21x 2 }}2
4
4
2
2
4
Ï2w
Ïw2
Ï2w
p
p 2
P3(x) 5 }} 2 1}}21x 2 }}2 2 1}}21x 2 }}2
4
4
2
2
4
Ï2w
p 3
1 1}}21x 2 }}2
4
12
2
373
f -(1)
}54
)x51 5 24, so }
3!
28
2!
6
3!
16. (a) P3(x) 5 4 1 5x 1 }}x 2 1 }}x 3
5 4 1 5x 2 4x 2 1 x 3
f (0.2) < P3(0.2) 5 4.848
374
Section 9.2
16. continued
(x)(e x) 2 (e x 2 1)(1)
d ex 2 1
x
x
dx
xe x 2 e x 1 1
5 }}
x2
e2e11
g9(1) 5 }} 5 1
1
(c) g9(x) 5 }} }} 5 }}}
2
(b) Since the Taylor series of f 9(x) can be obtained by
differentiating the terms of the Taylor series of f (x), the
second order Taylor polynomial of f 9(x) is given by
From the series,
5 2 8x 1 3x 2. Evaluating at x 5 0.2,
1
3
2!
2
3!
17. (a) P3(x)5 4 1 (21)(x 2 1) 1 }}(x 2 1)2 1 }}(x 2 1)3
3
2
x2
x3
d
x
xn
3!
4!
dx
2!
(n 1 1)!
2x
3x 2
1
nx n21
5 }} 1 }} 1 }} 1 … 1 }} 1 …
3!
4!
2!
(n 1 1)!
`
nxn21
5
}}
n51 (n 1 1)!
`
n
Therefore, g9(1) 5
}}, which means
(n
1
1)!
n51
`
n
}} 5 1.
n51 (n 1 1)!
g9(x) 5 }} 1 1 }} 1 }} 1 }} 1 … 1 }} 1 …
f 9(0.2) < 3.52
1
3
5 4 2 (x 2 1) 1 }}(x 2 1)2 1 }}(x 2 1)3
f (1.2) < P3(1.2) < 3.863
2
∑
∑
∑
(b) Since the Taylor series of f 9(x) can be obtained by
differentiating the terms of the Taylor series of f (x), the
second order Taylor polynomial of f9(x) is given by
21 1 3(x 2 1) 1 (x 2 1)2. Evaluating at x 5 1.2,
f9(1.2) < 20.36
20. (a) Factor out 2 and substitute t 2 for x in the Maclaurin
1
12x
2
f (t) 5 }}2
12t
1
5 2 }}2
12t
series for }} at the end of Section 9.2.
1
2
5 2[1 1 t 1 (t 2)2 1 (t 2)3 1 … 1 (t 2)n 1 …]
2
1
x
1
18. (a) Since f 9(0)x 5 }}, f 9(0) 5 }} 5 }}.
2
2!
2!
f (10)(0)
10!
x 10
1
Since }}x 10 5 }}, f (10)(0) 5 }} 5 }}.
11!
10 !
11!
11
5 2 1 2t 2 1 2t 4 1 2t 6 1 … 1 2t 2n 1 …
(b) Since G(0) 5 0, the constant term is zero and we may
(b) Multiply each term of f (x) by x.
find G(x) by integrating the terms of the series for f (x).
x2
x3
x4
xn11
g(x) 5 x 1 }} 1 }} 1 }} 1 … 1 }} 1 …
2!
3!
4!
(n 1 1)!
(c) g(x) 5 e x 2 1
21. (a) f (0) 5 (1 1 x)1/2
x
2
19. (a) Substitute }} for x in the Maclaurin series for e x shown
at the end of Section 9.2
x 2
e
x/2
x n
1}}2
1}}2
2
2
x
5 1 1 }} 1 } 1 … 1 } 1 …
2
n!
2
x2
xn
x
5 1 1 }} 1 } } 1 … 1 }
}
8
2
2n ? n!
2x 2n11
2n 1 1
)x50 5 1
)x50 5 }2}
1
1
f 0(0)
1
f 0(0) 5 2}}(1 1 x)23/2)
5 2}}, so }} 5 2}}
4
4
2!
8
x50
3
3
f -(0)
1
25/2
f -(0) 5 }}(1 1 x)
5 }}
)x50 5 }8}, so }3}
8
!
16
1
2
1
x2
8
x3
16
(b) Since g(x) 5 f (x 2), the first four terms are
2
3
n
2
5 }} 1 1 x 1 }} 1 }} 1 ... 1 }} 1 … 2 1
1
x
x
x
x
2!
3!
n!
1
x2
x3
xn
…
5 }} x 1 }} 1 }} 1
1 }} 1 …
x
2!
3!
n!
x2
x n 21
x
…
5 1 1 }} 1 }} 1
1 }} 1 …
3!
2!
n!
2
This can also be written as
x2
3!
2x 7
7
f 9(0) 5 }}(1 1 x)21/2
x
2
ex 2 1
x
xn
(n 1 1)!
1 1 }} 1 }} 1 … 1 }} 1 ….
x
2!
2x 5
5
P4(x) 5 1 1 }} 2 }} 1 }}
(b) g(x) 5 }}
31
1
2x 3
3
G(x) 5 2x 1 }} 1 }} 1 }} 1 … 1 }} 1 …
4
x2
2
x4
8
x6
16
1 1 }} 2 }} 1 }}.
(c) Since h(0) 5 5, the constant term is 5. The next three
terms are obtained by integrating the first three terms of
the answer to part (b). The first four terms of the series
x3
6
x5
40
for h(x) are 5 1 x 1 }} 2 }}.
Section 9.2
22. (a) a0 5 1
4x
d
dx x 1 1
29. (a) Since f 9(x) 5 }} }
2 }
3
1
3
3
9
a2 5 }}a1 5 }} ? 3 5 }}
2
2
2
3
9
a3 5 }}a2 5 a2 5 }}
3
2
a1 5 }}a0 5 3 ? 1 5 3
(x 2 1 1)(4) 2 (4x)(2x)
(x 1 1)
5 }}}
2
2
4 2 4x 2
(x 1 1)
5}
2
2,
Since each term is obtained by multiplying the previous
we have f (0) 5 0, f 9(0) 5 4, f (Ï3w) 5 Ï3w and
n
3
n
3
n!
term by }}, an 5 }}.
`
375
∑ anx n 5 1 1 3x 1 }92}x 2 1 }92}x 3 1 … 1 }3n}! x n 1 …
n
n50
`
(b) Since the series can be written as ∑ }}, it represents
n50
(3x)n
n!
1
2
f 9(Ï3w) 5 2}}, so the linearizations are L1(x) 5 4x and
1
2
1
2
3
2
L2(x) 5 Ï3w 2 }}(x 2 Ï3w) 5 2}}x 1 }}Ï3w,
respectively.
the function f (x) 5 e .
3x
(c) f 9(1) 5 3e 3x
)x51 5 3e3
23. First, note that cos 18 < 0.6603.
`
Using cos x 5 ∑ (21)n}}, enter the following two-step
n50
x 2n
(2n)!
commands on your home screen and continue to hit
[22, 4] by [23, 3]
(b) f 0(a) must be 0 because of the inflection point, so the
second degree term in the Taylor series of f at x 5 a is
zero.
ENTER.
30. The series represents tan21 x. When x 5 1, it converges to
p
4
tan21 1 5 }}. When x 5 21, it converges to
p
4
tan21(21) 5 2}}.
The sum corresponding to N 5 25 is about 0.6582 (not
withing 0.001 of exact value), and the sum corresponding
to N 5 26 is about 0.6606, which is within 0.001 of the
exact value. Since we began with N 5 0, it takes a total of
27 terms (or, up to and including the 52nd degree term).
24. One possible answer: Because the end behavior of a
polynomial must be unbounded and sin x is not unbounded.
Another: Because sin x has an infinite number of local
extrema, but a polynomial can only have a finite number.
25. (1) sin x is odd and cos x is even
(2) sin 0 5 0 and cos 0 5 1
1
x
31. (a) f (x) 5 }}(sin x)
3
5
2n11
1
x
x
x
5 }}(x 2 }} 1 }} 2 … 1 (21)n}} 1 …)
(2n 1 1)!
x2
x4
x 2n
5 1 2 }} 1 }} 2 … 1 (21)n}} 1 …
3!
5!
(2n 1 1)!
x
3!
5!
(b) Because f is undefined at x 5 0.
(c) k 5 1
1
12x
32. Note that the Maclaurin series for }} is
1 1 x 1 x 2 1 … 1 x n 1 …. If we differentiate this series
26. Replace x by 3x in series for sin x. Therefore, we have
and multiply by x, we obtain the desired Maclaurin series
x 1 2x 2 1 3x 3 1 … 1 nx n 1 …. Therefore, the desired
(3x)5
35 81
}} so }} = }}.
5!
5! 40
function is
3
d
dx
1
4
27. Since }}3 ln x 5 2x 23, which is }} at x 5 2, the coefficient
1
}}
4
1
24
is } 5 }}.
3!
28. The linearization of f at a is the first order Taylor
polynomial generated by f at x 5 a.
d
1
dx 1 2 x
1
(1 2 x)
x
(x 2 1)
f (x) 5 x}} }} 5 x}}2 5 }}2 .
33. (a) f (x) 5 (1 1 x)m
f 9(x) 5 m(1 1 x)m21
f0(x) 5 m(m 2 1)(1 1 x)m22
f -(x) 5 m(m 2 1)(m 2 2)(1 1 x)m23
(b) Differentiating f (x) k times gives
f (k)(x) 5 m(m 2 1)(m 2 2) … (m 2 k 1 1)(1 1 x)m2k.
Substituting 0 for x, we have
f (k)(0) 5 m(m 2 1)(m 2 2) … (m 2 k 1 1).
376
Section 9.3
33. continued
3. Since f (x) is increasing and positive on [23, 0],
M 5 f (0) 5 1.
(c) The coefficient is
m(m 2 1)(m 2 2) … (m 2 k 1 1)
f (k)(0)
}} 5 }}}}
k!
k!
1
2
4. Since the minimum value of f (x) is f (21) 5 2}} and the
(d) f (0) 5 1, f 9(0) 5 m, and we’re done by part (c).
1
2
34. Because f (x) 5 (1 1 x) is a polynomial of degree m.
Alternately, observe that f (k)(0) 5 0 for k $ m 1 1.
■ Section 9.3 Taylor’s Theorem (pp. 480–487)
Exploration 1
7. No, since the function f (x) 5 ) x 2 2 4) has a corner at x 5 2.
f (n11)(c)
By Taylor’s Theorem, Rn(x) 5 }}(x 2 0)n, where
(n 1 1)!
f
8. Yes, since the derivatives of all orders for sin x and cos x
are defined for all values of x.
(c) is the (n 1 1)st derivative of cos x evaluated at
9. Yes, since the function f (x) 5 e2x has derivatives of the
form f (n)(x) 5 2e2x for odd values of n and f (n)(x) 5 e2x
for even values of n, and both of these expressions are
defined for all values of x.
some c between x and 0. As with sin x, we can say that
f (n11)(c) lies between 21 and 1 inclusive. Therefore, no
matter what x is, we have
)
) )
3
2
10. No, since f (x) 5 x 3/2, we have f9(x) 5 }}x1/2 and
)
f (n11)(c)
1
)x)n
)Rn(x)) 5 }}(x 2 0)n # }}x n 5 }}.
(n 1 1)!
(n 1 1)!
(n 1 1)!
3
4
f 0(x) 5 }}x21/2, so f 0(0) is undefined.
The factorial growth in the denominator, as noted in
Section 9.3 Exercises
Example 3, eventually outstrips the power growth in the
)x)n
(n 1 1)!
numerator, and we have }} → 0 for all x. This means
that Rn(x) → 0 for all x, which completes the proof.
Exploration 2
Euler’s Formula
(ix)2
(ix)3
(ix)n
2!
3!
n!
x2
x3
x4
x5
xn
5 1 1 ix 2 }} 2 i}} 1 }} 1 i}} 2 … 1 (i)n }} 1 …
2!
3!
4!
5!
n!
1. e ix 5 1 1 ix 1 }} 1 }} 1 … 1 }} 1 …
4
3
e
1
f (0.2) < P4(0.2) 5 0.6704
)
px
51
2 x50
p
px
f9(0) 5 2}} sin }} x50 5 0
2
2
p2
px
p2
f 0(0)
p2
f 0(0) 5 2}} cos }} x50 5 2}}, so }} 5 2}}
4
2
4
2!
8
p3
px
f -(0)
f -(0) 5 }} sin }} x50 5 0, so }} 5 0
8
2
3!
4
4
p
px
p
f (4)(0)
p4
f (4)(0) 5 }} cos }} x50 5 }}, so }} 5 }}
16
2
16
4!
384
p2
p4
P4(x) 5 1 2 }}x 2 1 }}x 4
8
384
2. f (0) 5 cos }}
2
5 cos x 1 i sin x.
(We are assuming here that we can rearrange the terms of a
convergent series without affecting the sum. It happens to
be true in this case, but we will see in Section 9.5 that it is
not always true.)
3. eip 5 cos p 1 i sin p 5 21 1 0 5 21
Thus, e ip 1 1 5 0
Quick Review 9.3
1. Since ) f (x)) 5 )2 cos (3x)) # 2 on [22p, 2p] and f (0) 5 2,
M 5 2.
2. Since f (x) is increasing and positive on [1, 2],
M 5 f (2) 5 7.
2
3
P4(x) 5 1 2 2x 1 2x 2 2 }}x 3 1 }}x4
we get:
x2
x3
x4
x5
xn
5 1 1 ix 2 }} 2 i}} 1 }} 1 i}} 2 … 1 (i)n }} 1 …
2!
3!
4!
5!
n!
2n
x2
x4
x6
n x
…
…
5 1 2 }} 1 }} 2 }} 1 1 (21) }} 1
2!
4!
6!
(2n)!
x3
x5
x7
x 2n11
…
1 i x 2 }} 1 }} 2 }} 1 1 (21)n}} 1 …
3!
5!
7!
(2n 1 1)!
)x50 5 1
5 22
f 9(0) 5 22e22x)
x50
f 0(0)
5 4, so }} 5 2
f 0(0) 5 4e22x)
x50
2!
f -(0)
4
5 28, so }} 5 2}}
f -(0) 5 28e22x)
x50
3
3!
f
(
0)
2
f (4)(0) 5 16e22x)
5 16, so }} 5 }}
x50
3
4!
1. f (0) 5 e22x
(4)
2. If we isolate the terms in the series that have i as a factor,
ix
5. On [23, 1], the minimum value of f (x) is f (23) 5 27 and
the maximum value of f (x) is f (0) 5 2. On (1, 3], f is
increasing and positive, so the maximum value of f is
f (3) 5 5. Thus ) f (x)) # 7 on [23, 3] and M 5 7.
6. Yes, since each expression for an nth derivative given by
the Quotient Rule will be a rational function whose
denominator is a power of x 1 1.
Your Turn
1. We need to consider what happens to Rn(x) as n → `.
(n11)
1
2
maximum value of f (x) is f (1) 5 }}, M 5 }}.
m
)
)
)
)
f (0.2) < P4(0.2) < 0.9511
377
Section 9.3
)
)
f9(0) 5 25 cos x)x50 5 25
f 0(0)
f 0(0) 5 5 sin x)x50 5 0, so }} 5 0
2!
f -(0)
5
f -(0) 5 5 cos x)x50 5 5, so }} 5 }}
3!
6
f (0)
f (4)(0) 5 25 sin x)x50 5 0, so }} 5 0
4!
1
2
1
2
1
(2x)2
2!
8. cos2 x 5 }} 1 }} cos (2x)
3. f(0) 5 5 sin (2x) x50 5 25 sin x x50 5 0
(2x)4
4!
(2x)2n
(2n)!
5 }} 1 }} 1 2 }} 1 }} 2 … 1 (21)n}} 1 …
1
2
1
2
2
4
2n 2n
2
5 1 2 }} 1 }} 2 … 1 (21)n }} 1 …
4x
2 ? 2!
16x
2 ? 4!
x4
3
2 x
2 ? (2n)!
22n21x 2n
(2n)!
5 1 2 x 2 1 }} 2 … 1 (21)n }} 1 …
(4)
1
2
1
2
9. sin2 x 5 }} 2 }} cos (2x)
5
6
P4(x) 5 25x 1}}x 3
(2x)2
2!
1
1
2
149
150
f (0.2) < P4(0.2) 5 2}} < 20.9933
1
2
(2x)6
6!
(2x)2n
(2n)!
1 (21)n }} 1 …
2
4x
2 ? 2!
(x 2)2
(x 2)3
(x 2)n
2
3
n
4
6
2n
x
x
x
5 x 2 2 }} 1 }} 2 … 1 (21)n21 }} 1 …
2
3
n
x4
2
Therefore, P4(x) 5 x 2 }} and f (0.2) < P(0.2) 5 0.0392.
2
)
64x
2 ? 6!
22n x2n
2 ? (2n)!
x4
3
2x 6
45
22n21 x 2n
(2n)!
Note: By replacing n with n 1 1, the general term can be
22n11 x 2n12
(2n 1 2)!
written as (21)n }}.
1 1 2 2x 2
x2
1 2 2x
1
10. }} 5 x 2 }}
5. f (0) 5 (1 2 x)22 x50 5 1
)
f 0(0)
f 0(0) 5 6(1 2 x)24)x50 5 6, so }} 5 3
2!
f -(0)
f -(0) 5 24(1 2 x)25)x50 5 24, so }} 5 4
3!
f (0)
(4)
26
f (0) 5 120(1 2 x) )x50 5 120, so }} 5 5
4!
5 x 2[1 1 2x 1 (2x)2 1 … 1 (2x)n 1 …]
f9(0) 5 2(1 2 x)23 x50 5 2
(4)
5 x 2 1 2x 3 1 4x 4 1 … 1 2nx n12 1 …
x3
6
11. Let f (x) 5 sin x. Then P4(x) 5 P3(x) 5 x 2 }}, so we use
the Remainder Estimation Theorem with n 5 4. Since
)f (5)(x)) 5 )cos x) # 1 for all x, we may use M 5 r 5 1,
P4(x) 5 1 1 2x 1 3x 2 1 4x 3 1 5x 4
)x)5
5!
giving )R4(x)) # }}, so we may assure that
f (0.2) < P4(0.2) 5 1.56
)x)5
5!
)R4(x)) # 5 3 1024 by requiring }} # 5 3 1024, or
xn
n!
6. xe x 5 x 1 1 x 1 }} 1 … 1 }} 1 …
5
2
)x) # Ï0w.0
w6w < 0.5697. Thus, the absolute error is no
greater than 5 3 1024 when
x3
x n11
5 x 1 x 2 1 }} 1 … 1 }} 1 …
2!
n!
20.56 , x , 0.56 (approximately).
x3
7. sin x 2 x 1}}
3!
x3
x5
x 2n11
x3
5 x 2 }} 1 }} 2 … 1 (21)n}} 1 … 2 x 1 }}
3!
5!
(2n 1 1)!
3!
2n11
x5
x7
x9
x
n
5 }} 2 }} 1 }} 2 … 1 (21) }} 1 …
5!
7!
9!
(2n 1 1)!
2
Note: By replacing n with n 1 2, the general term can be
x 2n15
written as (21)n}}
(2n15)!
16x
2 ? 4!
5 x 2 2 }} 1 }} 2 … 1 (21)n21 }} 1 …
ln (1 1 x 2) 5 x 2 2 }} 1 }} 2 … 1 (21)n21}} 1 …
1
2
6
1 (21)n21 }} 1 …
ln (1 1 x) at the end of Section 9.2, we have
x2
2!
4
5 }} 2 }} 1 }} 2 …
4. Substituting x 2 for x in the Maclaurin series given for
1
(2x)4
4!
5 }} 2 }} 1 2 }} 1}} 2 }} 1 …
Alternate method: Using graphing techniques,
)sin x 2 1x 2 }x6}2) # 5 3 10
3
24
when 20.57 , x , 0.57.
x2
2
12. Let f (x) 5 cos x. Then P3(x) 5 P2(x) 5 1 2 }}, so we may
use the Remainder Estimation Theorem with n 5 3. Since
)f (4)(x)) 5 )cos x) # 1 for all x, we may use M 5 r 5 1,
)x)4
4!
giving )R3(x)) # }}. For )x) , 0.5, the absolute error is less
(0.5)4
4!
than }} < 0.0026 (approximately).
378
Section 9.3
Alternate method:
12. continued
Using graphing techniques, we find that when )x) , 0.01,
Alternate method: Using graphing techniques, we find that
x
)
1 2 2)
0.01
# )Ï1ww
2w0.0
w1w 2 11 2 }
}
2 2)
1wx 2 1 1 }}
)error) 5 Ï1ww
when )x) , 0.5,
x
)
1 2 2)
0.5
, )cos 0.5 2 11 2 }}2)
2
2
)error) 5 cos x 2 1 2 }}
< 1.26 3 1025.
2
x2
2
15. Note that 1 1 x 1 }} is the second order Taylor polynomial
< 0.002583.
x2
2
The quantity 1 2 }} tends to be too small, as shown by the
x2
graphs of y 5 cos x and y 5 1 2 }}.
2
for f (x) 5 e x at x 5 0, so we may use the Remainder
Estimation Theorem with n 5 2. Since ) f -(x)) 5 e x, which
is less than e0.1 when )x) , 0.1 and r 5 1, giving
e0.1)x)3
3!
e0.1(0.1)3
error is about }} < 1.842 3 1024.
3!
)R2(x)) # }}. Thus, for )x) , 0.1, the maximum possible
xn
n!
x2
2!
Thus the terms with n even will cancel for
the Remainder Estimation Theorem with n 5 2. Since
1
2
sinh x 5 }}(e x 2 e2x), and the terms with n odd will cancel
)f -(x)) 5 )2cos x) # 1 for all x, we may use M 5 r 5 1,
1
2
x3
x5
x 2n11
sinh x 5 x 1 }} 1 }} 1 … 1 }} 1 …
3!
5!
(2n 1 1)!
x2
x4
x 2n
cosh x 5 1 1 }} 1 }} 1 … 1 }} 1 …
2!
4!
(2n)!
for cosh x 5 }}(e x 1 e2x).
giving )R2(x)) # }}. Thus, for )x) , 1023, the maximum
(1023)3
3!
possible error is about }} < 1.67 3 10210.
Alternate method:
Using graphing techniques, we find that when )x) , 1023,
23
)error) 5 )sin x 2 x) # )sin 10
23
2 10 ) < 1.67 3 10
210
The inequality x , sin x is true for x , 0, as we may see
xn
n!
e2x 5 1 2 x 1 }} 2 … 1 (21)n}} 1 …
13. Let f (x) 5 sin x. Then P2(x) 5 P1(x) 5 x, so we may use
)x)3
3!
x2
2!
16. Note that e x 5 1 1 x 1 }} 1 … 1 }} 1 … and
[2p, p] by [21.5, 1.5]
.
17. All of the derivatives of cosh x are either cosh x or sinh x.
For any real x, cosh x and sinh x are both bounded by e)x).
So for any real x, let M 5 e)x) and r 5 1 in the Remainder
e)x))x)n11
(n 1 1)!
Estimation Theorem. This gives )Rn(x)) # }}
by graphing y 5 sin x 2 x.
e)x))x)n11
n→` (n 1 1)!
But for any fixed value of x, lim }} 5 0. It follows
that the series converges to cosh x for all real values of x.
18. For n 5 0, Taylor’s Theorem with Remainder says that if f
has derivatives of all orders in an open interval I containing
[21023, 1023] by [22 3 10210, 2 3 10210]
x
2
14. Let f (x) 5 Ï1ww
1wx. Then P1(x) 5 1 1 }}, so we may use
the Remainder Estimation Theorem with n 5 1. Since
)
1
4
)
) f 0(x)) 5 2}} (1 1 x)23/2 , which is less than 0.2538 for
)x) , 0.01, we may use M 5 0.2538 and r 5 1, giving
0.2538)x)2
)R1(x)) # }}. Thus, for )x) , 0.01 the maximum
2!
possible absolute error is about
0.2538(0.01)2
}} < 1.27 3 1025.
2!
a, then for each x in I,
f (x) 5 f (a) 1 R(x), where R(x) 5 f 9(c)(x 2 a), so
f (x) 5 f (a) 1 f 9(c)(x 2 a) for some c between a and x.
Letting b 5 x this equation is f (b) 5 f (a) 1 f9(c)(b 2 a),
f (b) 2 f (a)
b2a
which is equivalent to f9(c) 5 }} for some c
between a and b. Thus, for the class of functions that have
derivatives of all orders in an open interval containing a
and b, the Mean Value Theorem can be considered a special
case of Taylor’s Theorem.
Section 9.3
)
19. f (0) 5 ln (cos x)
1
cos x
x50
)
22. f (0) 5 sec x x50 5 1
5 ln 1 5 0
)
)
)
)
f9(0) 5 sec x tan x x50 5 0
f 9(0) 5 }} (2sin x) x50 5 2tan x x50 5 0
)
f 0(0) 5 (sec x)(sec2 x) 1 (tan x)(sec x tan x) x50 5 1,
f 0(0)
1
f 0(0) 5 2sec x x50 5 21 so }} 5 2}}
2
2!
2
379
f 0(0)
2!
1
2
so }} 5 }}
(a) L(x) 5 0
(a) L(x) 5 1
1
(b) P2(x) 5 2}}x 2
2
(c) The graphs of the linear and quadratic approximations
fit the graph of the function near x 5 0.
x2
2
(b) P2(x) 5 1 1 }}
(c) The graphs of the linear and quadratic approximations
fit the graph of the function near x 5 0.
[23, 3] by [23, 1]
20. f (0) 5 e
sin x
f9(0) 5 e
[23, 3] by [21, 3]
)x50 5 e 5 1
cos x)x50 5 1
0
)
23. f (0) 5 tan x x50 5 0
sin x
3
4)
f 0(0) 5 (esin x)(2sin x) 1 (cos x)(esin x cos x)
f 0(0)
1
so }} 5 }}
2!
2
x50
5 1,
)
f9(0) 5 sec2 x x50 5 1
)
f 0(0)
2!
f 0(0) 5 (2 sec x)(sec x tan x) x50 5 0, so }} 5 0
(a) L(x) 5 x
(a) L(x) 5 1 1 x
(b) P2(x) 5 x
x2
2
(b) P2(x) 5 1 1 x 1 }}
(c) The graphs of the linear and quadratic approximations
fit the graph of the function near x 5 0.
(c) The graphs of the linear and quadratic approximations
fit the graph of the function near x 5 0.
[23, 3] by [22, 2]
[23, 3] by [21, 3]
2 21/2
21. f (0) 5 (1 2 x )
)
24. f (0) 5 (1 1 x)k x50 5 1
)x50 5 1
)
)
1
f9(0) 5 2}}(1 2 x 2)23/2(22x) x50 5 x(1 2 x 2)23/2 x50 5 0
2
3
f 0(0) 5 (x) 2}}(1 2 x2)25/2(22x) 1 (1 2 x 2)23/2
5 1,
2
x50
f 0(0)
1
so }} 5 }}
2!
2
3
4
)
(a) L(x) 5 1
x2
2
)
f9(0) 5 k(1 1 x)k21 x50 5 k
)
f 0(0) 5 k(k 2 1)(1 1 x)k22 x50 5 k(k 2 1),
f 0(0)
2!
k(k 2 1)
2
so }} 5 }}
k(k 2 1)
2
P2(x) 5 1 1 kx 1 }}x 2
For k 5 3, we have f (x) 5 (1 1 x)3 and f -(x) 5 6. We may
use the Remainder Estimation Theorem with n 5 2, M 5 6,
6)x)3
3!
(b) P2(x) 5 1 1 }}
and r 5 1, giving R2(x) # }} 5 )x)3. (In this particular
(c) The graphs of the linear and quadratic approximations
fit the graph of the function near x 5 0.
case it is actually true that R2(x) 5 x 3, since f (x) is a cubic
1
100
polynomial.) Thus the absolute error is less than }}
whenever )x)3 , 0.01. In the interval [0, 1], this occurs
3
w1w < 0.215.
when 0 # x , Ï0w.0
Alternate method:
[23, 3] by [21, 3]
Note that P2(x) 5 1 1 3x 1 3x 2. Using graphing
techniques,
1
100
)(1 1 x)3 2 (1 1 3x 1 3x 2)) , }} when )x) , 0.215.
380
Section 9.3
x2
2
x3
6
25. Let f (x) 5 e x. Then P3(x) 5 1 1 x 1 }} 1 }}, so we may
use the Remainder Estimation Theorem with n 5 3. Since
27. (a) No
(b) Yes, since
2
dy
}} 5 e2x
dx
)f (4)(x)) 5 e x, which is no more than e0.1 when )x) # 0.1, we
may use M 5 e
0.1
x4
2!
x 2n
n!
The constant term of y is y (0) 5 2, and we may obtain
e0.1(0.1)4
}} < 4.605 3 1026.
24
the remaining terms of y by integrating the above
Alternate method:
series.
Using graphing techniques, when )x) # 0.1,
x
x
) 1
2
6 2)
0.01
0.001
# )e 2 11 1 0.1 1 }} 1 }}2)
2
6
2
x3
3
3
26. Since the Maclaurin series is
1
}} 5 1 1 x 1 x 2 1 … 1 x n 1 …,
12x
x 2n11
(2n 1 1)n!
By substituting n 2 1 for n, the general term may also
x 2n21
(2n 2 1)(n 2 1)!
be written as (21)n21}}.
0.1
< 4.251 3 1026.
x5
10
y 5 2 1 x 2 }} 1 }} 2 … 1 (21)n}} 1 …
)error) 5 ex 2 1 1 x 1 }} 1 }}
(c) The power series equals the function y for all real
2
values of x. This is because the series for e2x
converges for all real values of x, so Theorem 2 of
Section 9.1 implies that the new series also converges
for all x.
28. (a) Substitute 2x for x in the Maclaurin series for
ln (1 1 x) given at the end of Section 9.2.
P3(x) 5 1 1 x 1 x 2 1 x 3.
Since ) f
(2x 2)n
n!
5 1 2 x 2 1 }} 2 … 1 (21)n }} 1 ….
for )x) # 0.1, the maximum possible absolute error is about
x2
2
24(0.9)25 when )x) # 0.1, we may use M 5 24(0.9)25 and
24(0.9)25)x)4
4!
11x
12x
1
x3
xn
3
n
n
x2
x3
x
1 x 1 }} 1 }} 1 … 1 }}
2
3
n
2x 3
2x 5
2x 2n11
…
5 2x 1 }} 1 }} 1
1 }} 1 …
3
5
2n 1 1
)x)4
0.9
x2
2
5 x 2 }} 1 }} 2 … 1 (21)n21 }} 1 …
)x) # 0.1, an upper bound for the magnitude of the
0.14
0.9
approximation error is }}5 < 1.694 3 1024. Rounding up
1
29. (a)
Alternate method:
Using graphing techniques, when )x) # 0.1,
)
)
1
# )}} 2 1.111) < 1.11 3 10
1 2 0.1
p p
32}2}, }2}4 by [22, 2]
1
)error) 5 }} 2 (1 1 x 1 x 2 1 x 3)
12x
The series approximates tan x.
24
.
xn
n
(b) ln }} 5 ln (1 1 x) 2 ln (1 2 x)
r 5 1, giving )R3(x)) # }} 5 }}5 . Thus, for
to be safe, an upper bound is 1.70 3 1024.
x3
3
ln (1 2 x) 5 2x 2 }} 2 }} 2 … 2 }} 2 …
25
(x)) 5 24(1 2 x) , which is no more than
(4)
(2x 2)2
2!
5 1 1 (2x 2) 1 }} 1 … 1 }} 1 …
e0.1)x)4
and r 5 1, giving )R3(x)) # }}. Thus,
4!
(b)
p p
32}2}, }2}4 by [21, 4]
The series approximates sec x.
2
2
381
Section 9.4
1
2
1
1
(2x)2
(2x)4
(2x)6
5 }} 2 }} 1 2 }} 1 }} 2 }} 1 …
2
2
2!
4!
6!
2n
n (2x)
1 (21) }} 1 …
(2n)!
256x 8
4x 2
16x 4
64x 6
5 }} 2 }} 1 }} 2 }}
2 ? 8!
2 ? 2!
2 ? 4!
2 ? 6!
1024x10
1 }} 2 …
2 ? 10!
x4
2x 6
x8
2x10
2
5 x 2 }} 1 }} 2 }} 1 }} 2 …
3
45
315
14,175
30. (a) sin2 x5 }}(1 2 cos 2x)
1
(b)
E
E
cos bx dx 1 i e ax sin bx dx
a 2 bi
a 1b
a 2 bi ax
5}
}e (cos bx 1 i sin bx)
a2 1 b2
eax
5 }
} (a cos bx 1 b sin bx 2 bi cos bx
a2 1 b2
(a1bi)x
5}
2 }
2e
1
2
1a
ax
e
1b
1 ai sin bx)
2
5 }
2 }
2 [(a cos bx 1 b sin bx)
4x 3
4x 5
8x7
(b) derivative 5 2x 2 }} 1 }} 2 }} 1 …
3
15
315
(2x)3
(2x)5
(2x)7
(c) part (b) 5 2x 2 }} 1 }} 2 }} 1 … 5 sin 2x
3!
5!
7!
1 i(a sin bx 2 b cos bx)]
Separating the real and imaginary parts gives
Ee
Ee
31. (a) It works. For example, let n 5 2. Then P 5 3.14 and
P 1 sin P < 3.141592653, which is accurate to more
than 6 decimal places.
estimate. Then
ax
5 e(a1bi)x dx
2
(b) Let P 5 p 1 x where x is the error in the original
Ee
e ax
a 1b
e ax
ax
sin bx dx 5 }
}(a sin bx 2 b cos bx)
a2 1 b2
ax
cos bx dx 5 }
2 }
2 (a cos bx 1 b sin bx) and
■ Section 9.4 Radius of Convergence
(pp. 487–496)
P 1 sin P 5 (p 1 x) 1 sin (p 1 x) 5 p 1 x 2 sin x
)x)3
6
But by the Remainder Theorem, )x 2 sin x) , }}.
Therefore, the difference between the new estimate
)x)3
6
P 1 sin P and p is less than }}.
(cos u 1 i sin u) 1 (cos (2u) 1 i sin (2u))
eiu 1 e2iu
32. (a) }} 5 }}}}}
2
2
cos u 1 i sin u 1 cos u 2 i sin u
5 }}}}
2
2 cos u
5 }} 5 cos u
2
(cos u 1 i sin u) 2 (cos (2u) 1 i sin (2u))
eiu 2 e2iu
(b) }} 5 }}}}}
2i
2i
(cos u 1 i sin u) 2 (cos u 2 i sin u)
5 }}}}
2i
2i sin u
5 }} 5 sin u
2i
d
33. }}[eax(cos bx 1 i sin bx)]
dx
5 (eax)(2b sin bx 1 bi cos bx) 1 (aeax)(cos bx 1 i sin bx)
5 (eax)[(bi2 sin bx 1 bi cos bx) 1 a(cos bx 1 i sin bx)]
5 (eax)[bi(cos bx 1 i sin bx) 1 a(cos bx 1 i sin bx)]
5 (a 1 bi)(eax)(cos bx 1 i sin bx)
5 (a 1 bi)e
(a1bi)x
34. (a) The derivative of the right-hand side is
a 2 bi
}
}(a 1 bi)e(a1bi)x
a2 1 b2
a 2 2 (bi)2 (a1bi)x
5}
}e
a2 1 b2
a 2 1 b 2 (a1bi)x
5}
5 e(a1bi)x,
}e
a2 1 b2
which confirms the antiderivative formula.
Exploration 1
Test
Finishing the Proof of the Ratio
1
}}
1. For ∑
n11
1
n
5 lim }} 5 1.
}}: L 5 lim }
n
n→` }1}
n→` n 1 1
n
1
}}2
(n 1 1)
For ∑}}2 : L 5 lim }
5 lim }}2 5 1.
1
1
n
n→`
n2
n→` (n 1 1)
}}2
n
2. (a)
E
1
k
}} dx 5 lim ln x 5 lim ln k 5 `.
x
1
k→`
k→`
(b)
E
1
1
k
}}2 dx 5 lim 2x 21 5 lim 2}} 1 1 5 1.
k
x
1
k→`
k→`
`
1
`
1
1 )2
)2
1
1
3. Figure 9.14a shows that ∑}} is greater than
1
n
2
E
`
1
the integral diverges, so must the series.
Figure 9.14b shows that ∑}}2 is less than 1 1
1
n
1
}} dx. Since
x
E
`
1
1
}}2 dx.
x
Since the integral converges, so must the series.
4. These two examples prove that L 5 1 can be true for either
a divergent series or a convergent series. The Ratio Test
itself is therefore inconclusive when L 5 1.
Exploration 2
)x)
n11
Revisiting a Maclaurin Series
n
)x)
n
1. L 5 lim }} ? }}n 5 lim }} )x) 5 )x). The series
n→` n 1 1
n→` n 1 1
converges absolutely when )x) , 1, so the radius of
convergence is 1.
2. When x 5 21, the series becomes
1
1
1
21 2 }} 2 }} 2 … 2 }} 2 ….
2
3
n
Each term in this series is the negative of the corresponding
term in the divergent series of Figure 9.14a. Just as ∑}}
diverges to 1`, this series diverges to 2`.
1
n
382
Section 9.4
3. Geometrically, we chart the progress of the partial sums as
in the figure below:
Section 9.4 Exercises
n
1. Diverges by the nth-Term Test, since lim }} 5 1 Þ 0.
1
n→` n 1 1
–2
1
+3
2n
n
n→` 1 1
2. Diverges by the nth-Term Test, since lim }} 5 `. (The
1
–4
1
+5
Ratio Test can also be used.)
1
L
1
1–2
3. Converges by the Ratio Test, since
etc.
1
1
1
1– 2 + 3 – 4
(n 1 1)2 2 1
2
n→`
a
2n
n 21
1
2
lim }n1
}1 5 lim }n1
}
?}
2 } 5 }} , 1.
1
1
1
1– 2 + 3
an
n→`
4. The series converges at the right-hand endpoint. As shown
in the picture above, the partial sums are closing in on
some limit L as they oscillate left and right by constantly
decreasing amounts.
1
8
4. Converges, because it is a geometric series with r 5 }},
so )r) , 1.
5. Converges by the Ratio Test, since
5. We know that the series does not converge absolutely at the
right-hand endpoint, because ∑
1
}} diverges (Exploration 1
n
of this section).
n→` an
n→` (3
∑1 2
Quick Review 9.4
n)x)
n→` n 1 1
2n11
3n 1 1
2
3
1 1)
2
2n
2 n
Alternately, note that }
} , }} for all n.
3
3n 1 1
`
`
n
2
2n
Since
converges by the Direct
}} converges,
}
}
n
n51 3
n51 3 1 1
a
lim }n1
5 }} , 1.
}1 5 lim }
n11} ? }}
n
∑
12
Comparison Test.
n
n→` n 1 1
1. lim }} 5 )x) lim }}5 )x)
n 2)x 2 3)
n→` n(n 1 1)
6. Diverges by the nth-Term Test, since
n2
n→` n 1 n
2. lim }} 5 )x 2 3) lim }
2 } 5 )x 2 3)
1n2
1
lim n sin }} 5 1 Þ 0
n→`
)x)n
3. lim }} 5 0
n→` n!
7. Converges by the Ratio Test, since
(Note: This limit is similar to the limit which is discussed
at the end of Example 3 in Section 9.3.)
(n 1 1)2e2n21
n e
n→`
a
lim }n1
5 e21 , 1.
}1 5 lim }
2}
2n
an
n→`
8. Converges by the Ratio Test, since
n 4 1 4n 3 1 6n 2 1 4n 1 1
(n 1 1)4x 2
4. lim }}
5 x 2 lim }}}
4
16n 4
(2n
)
n→`
n→`
2
1
x
5 x 2 }} 5 }}
16
16
1 2
)2x 1 1)n112n
)2x 1 1)
)2x 1 1)
5. lim }}
5 lim }} 5 }}
n11
)2x 1 1)n n→`
2
2
n→` 2
(n 1 1)10
n→` 10
a
n→` an
(n 1 4)!
a
an
n→` 3!(n 1 1)!3
n14
7. Since 5n . n5 for n $ 6, an 5 5n, bn 5 n 5 and N 5 6.
5 }} , 1.
1
2
1
1
9. Since 10 , n! and hence }}n . }} for n $ 25,
10
n!
1
1
an 5 }}n , bn 5 }}, and N 5 25.
10
n!
1
1
n
2
10. Since n 2 , n 3 and hence }}2 . n23 for
1
n $ 2, an 5 }}2 , bn 5 n23, and N 5 2.
n
3!n! 3n
(n 1 3)!
lim }n1
}1 5 lim }}
n11 ? }}
n→`
5 lim }}
n
1
10
9. Converges by the Ratio Test, since
6. Since n 2 . 5n for n $ 6, an 5 n 2, bn 5 5n, and N 5 6.
8. Since Ïnw . ln n for n $ 1, an 5 Ïnw, bn 5 ln n, and
N 5 1.
10 n
n
lim }n1
}1 5 lim }n1
}
} 5 }} , 1.
1 ? }10
n→` 3(n 1 1)
1
3
10. Diverges by the nth-Term Test, since
1 n
5 e Þ 0.
n
1
2
lim 1 1 }}
n→`
2
3
11. Converges, because it is a geometric series with r 5 2}},
so )r) , 1.
12. Diverges by the Ratio Test, since
a
(n 1 1)!e2n21
n!e
n→`
lim }n1
5 lim (n 1 1)e21 5 `.
}1 5 lim }}
2n
n→`
an
n→`
(The nth-Term Test can also be used.)
Section 9.4
13. Diverges by the Ratio Test, since
a 1
3n 1 1
lim }n1
} 5 lim }}
3 n11
n→` an
n→` (n 1 1) 2
3
3n
5 lim }}
3
n→` (n 1 1) (2)
3
5 }} . 1.
2
?
n32 n
}}
3n
a 1
(n 1 1)ln (n 1 1)
2n
lim }n1
} 5 lim }}
}}
?
n11
2
n ln n
n→` an
n→`
1 n 1 1 ln (n 1 1)
5 lim }} ? }} ? }}
n
ln n
n→` 2
1
5 }} , 1.
2
15. Converges by the Ratio Test, since
(2n 1 1)!
(n 1 1)!
n!
(2n 1 3)!
n11
}}
(2n 1 3)(2n 1 2)
1
}} 5 0 , 1.
2(2n 1 3)
lim }n1
}1 5 lim }} ? }}
an
n→`
5 lim
n→`
5 lim
n→`
16. Converges by the Ratio Test, since
a 1
(n 1 1)!
nn
lim }n1
} 5 lim }}
n11 ? }}
n!
n→` an
n→` (n 1 1)
(n 1 1)n n
5 lim }}n
n→` (n 1 1)(n 1 1)
n n
5 lim }}
n→` n 1 1
1
5 lim }}n
n→` (1 1 1/n)
1
5 }} , 1
e
1
n→`
an
)3x 2 2)n11
n11
n→`
n
)3x 2 2)
)
2
3
)
1
3
The series converges for )3x 2 2) , 1, or x 2 }} , }}, and
)
14. Converges by the Ratio Test, since
n→`
a
22. lim }n1
}1 5 lim }} ? }}n 5 )3x 2 2)
2
3
)
1
3
1
3
diverges for x 2 }} . }}, so the radius of convergence is }}.
(The nth 5 Term Test can also be used.)
a
) )
383
2
23. This is a geometric series which converges only for
) ) , 1, or )x 2 2) , 10, so the radius of convergence is
x22
}}
10
10.
) )
a
(n 1 1))x)n11
n13
n→`
24. lim }n1
}1 5 lim }}
n→`
an
n12
} 5 lim )x) 5 )x)
?}
n )x)n
n→
`
The series converges for )x) , 1 and diverges for )x) . 1, so
the radius of convergence is 1.
) )
)x)
a 1
nÏwn 3n
25. lim }n1
} 5 lim }}}
n11 ? }}
)x)n
ww
1w1 3
n→` an
n→` (n 1 1)Ïn
n11
)x)
)x)
3
5 lim }} 5 }}
n→` 3
The series converges for )x) , 3 and diverges for )x) . 3, so
the radius of convergence is 3.
) aa )
)x)2n13
n→` (n 1 1)!
x2
n→` n 1 1
n!
26. lim }n1
}1 5 lim }} ? }2n}
11 5 lim }} 5 0
n→`
n
)x)
The series converges for all values of x, so the radius of
convergence is `.
) aa )
(n 1 1))x 1 3)n11
5
n→`
)x 1 3)
)x 1 3)
5 lim }} 5 }}
5
5
n→`
27. lim }n1
}1 5 lim }}
n11
n→`
n
5n
}
?}
n)x 1 3)n
The series converges for )x 1 3) , 5 and diverges for
17. One possible answer:
`
∑
1
}} diverges (see Exploration 1 in this section) even
n51 n
1
though lim }} 5 0.
n→` n
)x 1 3) . 5, so the radius of convergence is 5.
) aa )
n→`
n
18. One possible answer:
Let an 5 22n and bn 5 32n
Then ∑an and ∑bn are convergent geometric series, but
n
∑}b}n 5 ∑1}32}2
a
(n 1 1))x)n11
[(n 1 1) 1 1]
n→` 4
)x)
)x)
5 lim }} 5 }}
4
n→` 4
28. lim }n1
}1 5 lim }}
n11
2
4n(n2 1 1)
}
?}
n)x)n
The series converges for )x) , 4 and diverges for )x) . 4, so
the radius of convergence is 4.
is a divergent geometric series.
n
19. This is a geometric series which converges only for )x) , 1,
so the radius of convergence is 1.
20. This is a geometric series which converges only for
)x 1 5) , 1, so the radius of convergence is 1.
) )
a 1
Ïnww
1w1)x)n11
3n
)x)
)x)
29. lim }n1
} 5 lim }n1
}
}} 5 lim }} 5 }}
?
1
n
3
3
3
n→` an
n→`
n→
`
Ïnw )x)
The series converges for )x) , 3 and diverges for )x) . 3, so
the radius of convergence is 3.
21. This is a geometric series which converges only for
)
1
4
)
1
4
)2(4x 1 1)) , 1, or x 1 }} , }}, so the radius of
1
4
convergence is }}.
384
Section 9.4
) aa )
35. This is a geometric series with first term a 5 1 and
(n 1 1)!)x 2 4)n11
n!)x 2 4)
n→`
30. lim }n1
}1 5 lim }}
n
n→`
n
5 lim (n 1 1))x 2 4)
(x 2 1)
} , 1, so the interval of convergence is
)}
4 )
2
n→`
5 ` (x Þ 4)
21 , x , 3.
The series converges only for x 5 4, so the radius of
1
a
Sum 5 }} 5 }}
(x 2 1)2
12r
convergence is 0.
) aa )
(x 2 1)2
4
common ratio r 5 }}. It converges only when
1 2 }}
4
4
5 }}2
4 2 (x 2 1)
)(22)n11)(n 1 2))x 2 1)n11
)22 )(n 1 1))x 2 1)
n→`
31. lim }n1
}1 5 lim }}}
n
n
n→`
n
4
2x 1 2x 1 3
5}
}
2
5 lim 2)x 2 1)
n→`
4
x 2 2x 2 3
5 2}
}
2
5 2)x 2 1)
1
2
The series converges for )x 2 1) , }} and diverges for
1
1
)x 2 1) . }}, so the radius of convergence is }}.
2
2
) aa )
)4x 2 5)2n13
n→` (n 1 1)
n3/2
)4x 2 5)
32. lim }n1
}1 5 lim }}
3/2 ? }}
2n11
n→`
n
5 lim (4x 2 5)2
36. This is a geometric series with first term a 5 1 and
(x 1 1)
} , 1, so the interval of convergence is
)}
9 )
2
24 , x , 2.
a
12r
Sum 5 }}
n→`
5 (4x 2 5)2
1
5 }}2
(x 1 1)
9
The series converges for (4x 2 5) , 1, which is equivalent
2
)
(x 1 1)2
9
common ratio r 5 }}. It converges only when
)
1 2 }}
9
9 2 (x 1 1)
to )4x 2 5) , 1, or x 2 }} , }} and diverges for
5 }}2
)x 2 }54}) . }14}. The radius of convergence is }14}.
5}
} 5 2}
}
2
2
5
4
1
4
) )
a 1
Ïnw
)x 1 p)n11
33. lim }n1
} 5 lim }} ? }}n
a
)x 1 p)
n→`
n→` Ïw
nw
1w1
n
5 lim )x 1 p)
n→`
5 )x 1 p)
9
2x 2 2x 1 8
37. This is a geometric series with first term a 5 1 and
Ïwx
common ratio r 5 }} 2 1. It converges only when
2
)}2} 2 1) , 1, so the interval of convergence is
Ïwx
0 , x , 16.
The series converges for )x 1 p) , 1 and diverges for
)x 1 p) . 1, so the radius of convergence is 1.
) )
a 1
w)2n13
)x 2 Ï2
2n
34. lim }n1
} 5 lim }n1
}
}}
?
1
a
2
n→`
n→`
)x 2 Ï2
w)2n11
n
1
n→` 2
1
5 }}(x 2 Ï2w)2
2
1
The series converges for }}(x 2 Ï2w)2 , 1, which is
2
5 lim }}(x 2 Ï2w)2
9
x 1 2x 2 8
a
12r
Sum 5 }} 5
1
}}
2
5 }}
Ïxw
1 2 }} 2 1
4
2
Ïxw
2
1
2
38. This is a geometric series with first term a 5 1 and
common ratio r 5 ln x. It converges only when )ln x) , 1,
1
e
so the interval of convergence is }} , x , e.
a
12r
1
1 2 ln x
Sum 5 }} 5 }}
39. This is a geometric series with first term a 5 1 and
) x 32 1 )
x2 2 1
3
2
equivalent to )x 2 Ï2w) , Ï2w, and diverges for
common ratio }}. It converges only when }} , 1,
)x 2 Ï2w) . Ï2w. The radius of convergence is Ï2w.
so the interval of convergence is 22 , x , 2.
a
12r
1
3
3 2 (x 2 1)
3
42x
Sum 5 }} 5 }}
5 }}
5 }}2
2
2
x 21
3
1 2 }}
Section 9.4
40. This is a geometric series with first term a 5 1 and
) sin2 x )
sin x
2
46.
common ratio }}. Since }} , 1 for all x, the interval
`
`
n51
n51
6
3
3
} 5 ∑ }} 2 }}
∑}
1 2n 2 1 2n 1 1 2
(2n 2 1)(2n 1 1)
3
s1 5 3 2 }}
3
of convergence is 2` , x , `.
1 52
5
3
3
3
3
5 (3 2 1) 1 11 2 }}2 1 1}} 2 }}2 5 3 2 }}
5
5
7
7
3
3
s2 5 (3 2 1) 1 1 2 }} 5 3 2 }}
a
2
1
Sum 5 }} 5 } 5 }}
sin x
12r
2 2 sin x
1 2 }}
s3
2
41. Almost, but the Ratio Test won’t determine whether there is
convergence or divergence at the endpoints of the interval.
sn 5 3 2 }}
42. (a) For k # N, it’s obvious that
S 5 lim sn 5 3
3
2n 1 1
n→`
`
a1 1 … 1 ak # a1 1 … 1 aN 1 ∑ cn.
n5N11
For all k . N,
47.
`
# a1 1 … 1 aN 1 ∑ cn
n5N11
(b) Since all of the an are nonnegative, the partial sums of
the series form a nondecreasing sequence of real
numbers. Part (a) shows that the sequence is bounded
above, so it must converge to a limit.
`
d1 1 … 1 dk # d1 1 … 1 dN 1 ∑ an.
n5N11
For all k . N,
d1 1 … 1 dk 5 d1 1 … 1 dN 1 dN11 1 … 1 dk
# d1 1 … 1 dN 1 aN11 1 … 1 ak
`
# d1 1 … 1 dN 1 ∑ an
n5N11
(b) If ∑an converged, that would imply that ∑dn was also
`
n51
n51
1
1
# a1 1 … 1 aN 1 cN11 1 … 1 ck
43. (a) For k # N, it’s obvious that
`
40n
5
5
} 5 ∑ }}2 2 }}2
∑}
3 (2n 2 1) (2n 1 1) 4
(2n21)2(2n11)2
5
s1 5 5 2 }}
9
5
5
5
5
s2 5 5 2 }} 1 }} 2 }} 5 5 2 }}
9
9
25
25
5
5
5
5
5
5
s3 5 5 2 }} 1 }} 2 }} 1 }} 2 }} 5 5 2 }}
9
9
25
25
49
49
5
sn 5 5 2 }}2
(2n 1 1)
a1 1 … 1 ak 5 a1 1 … 1 aN 1 aN11 1 … 1 ak
2 1
2 1
2
2 1
2
S 5 lim sn 5 5
n→`
48.
`
`
n51
n51
2n 1 1
1
1
} 5 ∑ }}2 2 }}2
∑}
1 n (n 1 1) 2
n 2(n 1 1)2
1
s1 5 1 2 }}
4
1
1
1
1
s2 5 1 2 }} 1 }} 2 }} 5 1 2 }}
4
4
9
9
1
1
1
1
1
1
s3 5 1 2 }} 1 }} 2 }} 1 }} 2 }} 5 1 2 }}
4
4
9
9
16
16
1
sn 5 1 2 }}2
(n 1 1)
1
1
2 1
2 1
2
2 1
2
S 5 lim sn 5 1
n→`
convergent.
1
49. s1 5 1 2 }}
Ïw2
44. Answers will vary.
45.
`
`
n51
n51
1
2 1
2
1
1
1
1
1
1
5 11 2 }}2 1 1}} 2 }}2 1 1}} 2 }}2 5 1 2 }}
Ï2w
Ïw2 Ï3w
Ï3w Ïw4
Ïw4
1
1
1
1
4
1
1
} 5 ∑ }} 2 }}
∑}
1 4n 2 3 4n 1 1 2
(4n 2 3)(4n 1 1)
s2 5 1 2 }} 1 }} 2 }} 5 1 2 }}
Ïw2
Ïw2 Ï3w
Ï3w
1
s1 5 1 2 }}
5
1
1
1
1
s2 5 1 2 }} 1 }} 2 }} 5 1 2 }}
5
5
9
9
1
1
1
1
1
1
s3 5 1 2 }} 1 }} 2 }} 1 }} 2 }} 5 1 2 }}
5
5
9
9
13
13
1
sn 5 1 2 }}
4n 1 1
s3
1
1
2 1
2 1
S 5 lim sn 5 1
n→`
385
2
2 1
2
1
sn 5 1 2 }}
1w1
Ïnww
S 5 lim sn 5 1
n→`
1
1
ln 3
ln 2
1
1
s2 5 }} 2 }} 1
ln 3
ln 2
1
1
s3 5 }} 2 }} 1
ln 3
ln 2
1
1
5 }} 2 }}
ln 5
ln 2
1
1
sn 5 }} 2 }}
ln(n 1 2)
ln 2
1
S 5 lim sn 5 2}}
ln 2
n→`
50. s1 5 }} 2 }}
1
1
2 1}ln}4 2 }ln}3 2 5 }ln}4 2 }ln}2
1
1
1
1
2 1}ln}4 2 }ln}3 2 1 1}ln}5 2 }ln}4 2
1
1
1
1
386
Section 9.5
p
4
51. s1 5 tan21 1 2 tan21 2 5 }} 2 tan21 2
s2 5 (tan21 1 2 tan21 2) 1 (tan21 2 2 tan21 3)
p
4
5 }} 2 tan21 3
s3 5 (tan21 1 2 tan21 2) 1 (tan21 2 2 tan21 3)
1 (tan21 3 2 tan21 4)
p
4
p
sn 5 }} 2 tan21 (n 1 1)
4
p
p
p
p
S 5 lim sn 5 }} 2 lim tan21 n 5 }} 2 }} 5 2}}
4 n→`
4
2
4
n→`
5 }} 2 tan21 4
`
52. }} 5 ∑ x n
1
12x
■ Section 9.5 Testing Convergence at
Endpoints (pp. 496–508)
Exploration 1
The p-Series Test
1. We first note that the Integral Test applies to any series of
the form ∑ }}p where p is positive. This is because the
1
n
function f (x) 5 x2p is continuous and positive for all x . 0,
and f9(x) 5 2p ? x p21 is negative for all x . 0.
If p . 1:
E
`
1
n50
E
1
x2p11
}}p dx 5 lim }}
1 x
k→` 2p11
1
1
= lim }} ? }p21
} 21
k
k→` 12p
k
1
}}p dx 5 lim
x
k→`
1
Differentiate:
`
∑
1
22
1
1
nx n21
}}2 5
(1 2 x)
n50
1
5 0 1 }} (since p21 . 0)
p21
Multiply by x:
5 }} , `.
∑
1
1
p21
`
x
nx n
}}2 5
(1 2 x)
n50
k
42
The series converges by the Intergral Test.
Differentiate:
(1 2 x)2(1) 2 (x)(2)(12 x)(21)
d
x
}} }}2 5 }}}}
(1 2 x)4
dx (1 2 x)
(1 2 x) 1 2x
5 }}
(1 2 x )3
x11
5 }}3
(1 2 x)
`
x11
n2x n21
}}3 5
(1 2 x)
n50
2. If 0 , p , 1:
E
`
1
1
}}p dx 5 lim
x
k→`
12
1 n
5 ∑ n 2 }}
1
1
}}
22
122
}
3
`
n50
`
6 5 ∑ }}n
2
n
n50 2
The sum is 6.
1
}}p dx
x
x2p11
k
1
1
1
5 lim }}
k→` 12p
`
1 3
}} }}
2 2
1
1
42
k→` 2p11
Multiply by x:
∑
k
5 lim }}
∑
x(x 1 1)
n 2x n
}}3 5
(1 2 x)
n50
1
Let x 5 }}:
2
E
? (k 12p21)2
5 ` (since 1 2 p . 0).
The series diverges by the Integral Test.
If p # 0, the series diverges by the nth Term Test. This
completes the proof for p , 1.
3. If p 5 1:
E }x1} dx 5 lim E
`
1
k
p
1
}} dx
k→` 1 x
k
1 42
k→`
5 lim ln x
1
5 lim ln k 5 `.
k→`
The series diverges by the Integral Test.
Exploration 2 The Maclaurin Series of a
Strange Function
1. Since f (n)(0) 5 0 for all n, the Maclaurin Series for f has all
`
zero coefficients! The series is simply ∑ 0 ? x n 5 0.
n50
2. The series converges (to 0) for all values of x.
3. Since f (x) 5 0 only at x 5 0, the only place that this series
actually converges to its f-value is at x 5 0.
387
Section 9.5
Quick Review 9.5
10. Converges by the Limit Comparison Test, since
E
`
1
}}p dx with p . 1
1 x
1
2. Diverges, limit comparison test with integral of }}
x
1. Converges, since it is of the form
1
3. Diverges, comparison test with integral of }}
x
5n 3 2 3n
}
}
n 2(n 1 2)(n 2 1 5)
lim }}
1
n→`
}}2
n
`
5 1, and ∑ }}2
n51
1
n
converges as a p-series with p 5 2.
11. Diverges by the nth-Term Test, since
2
4. Converges, comparison test with integral of }}2
x
3n21 1 1
3
n→`
1
3
lim }}
5 }} Þ 0.
n
1
5. Diverges, limit comparison test with integral of }}
Ïwx
6. Yes, for N 5 0
7. Yes, for N 5 2Ï2w
8. No, neither positive nor decreasing for x . Ï3w
9. No, oscillates
1
ln n
12. Converges by the Alternating Series Test. If un 5 }}, then
{un } is a decreasing sequence of positive terms with
lim un 5 0.
n→`
10 n
13. Diverges by the nth-Term Test, since lim }10
} 5 `.
10. No, not positive for x $ 1
n→` n
Ïwn 1 1
14. Converges by the Alternating Series Test. If un 5 }},
Section 9.5 Exercises
E
`
1. Diverges by the Integral Test, since
1
`
`
5
}} dx diverges.
x11
2. Diverges because ∑ }} 5 3∑ }1/2
}, which diverges by
n51 Ïn
n51 n
w
the p-series Test.
3
1
ln n
1
3. Diverges by the Direct Comparison Test, since }} . }} for
n
n
`
1
n $ 2 and
}} diverges.
n52 n
∑
1
E}
} dx diverges.
2x 2 1
`
4. Diverges by the Integral Test, since
1
n11
then {un} is a decreasing sequence of positive terms with
lim un 5 0. (To show that un is decreasing, let
n→`
Ïxw 1 1
f (x) 5 }} and observe that
x11
1
(x 1 1) }} 2 (Ïxw 1 1)(1)
1 2 x 2 2Ïxw
2Ïwx
,
f9(x) 5 }}}}
5 }}
2(x 1 1)2Ïxw
(x 1 1)2
1 2
which is negative, at least for x $ 1.)
ln n
ln n
1
2
1
2
which means each term is 6}}.
5. Diverges, since it is a geometric series with
1
ln 2
ln n
2 ln n
15. Diverges by the nth-Term Test since }}2 5 }} 5 }},
16. Diverges by the Limit Comparison Test.
r 5 }} < 1.44.
1
n
1
n
1
n
Let an 5 }} 2 }}2 and bn 5 }}.
6. Converges, since it is a geometric series with
Then an . 0 and bn . 0 for n $ 2 and
1
ln 3
r 5 }} < 0.91.
1
1
7. Diverges by the nth-Term Test, since lim n sin }} 5 1.
}} 2 }}2
a
n
n
n21
1
5 lim }} 5 lim 1 2 }} 5 1.
lim }}n 5 lim }
1
n
n
n→` bn
n→`
n→`
n→`
}}
8. Converges by the Direct Comparison Test, since
Since ∑ bn diverges, ∑ an also diverges.
n→`
1
n
`
∑
en
, e2n for n $ 0, and
e2n converges as a
}}
1 1 e 2n
n50
geometric series with r 5 e21 < 0.37.
1
n
`
`
n51
n51
2
17. Converges absolutely, because, absolutely, it is a geometric
series with
r 5 0.1.
18. Converges conditionally:
9. Converges by the Direct Comparison Test, since
Ïnw
`
∑
1
1
}
} , }3/2
} for n $ 1, and
}3/2
} converges as a p-series
n2 1 1
n
n
n50
3
with p 5 }}.
2
11n
n
1
n
1
n
If un 5 }}
2 5 }} 1 }}
2 , then {un} is a decreasing sequence
`
11n
n
of positive terms with lim un 5 0, so ∑ (21)n11}}
2
n→`
n51
converges by the Alternating Series Test.
`
11n
n
`
11n
1
1
$
for
n
$
1
and
}}
}
}
}} diverges.
n2
n
n51 n
But ∑ }}
2 diverges by the Direct Comparison Test, since
n51
∑
388
Section 9.5
`
2 n
132
19. Converges absolutely, since ∑ n2 }}
n51
converges by the
Ratio Test:
) )
12
2
1 3 n
}}2 }} 5 }} , 1.
3
n 2
12
?
(c) None
28. This is a geometric series which converges only for
)x 1 5) , 1, or 26 , x , 24.
20. Converges conditionally.
1
n ln n
(a) (26, 24)
If un 5 }}, then {un} is a decreasing sequence of
`
(b) (26, 24)
positive terms with lim un 5 0, so ∑ (21)n11}}
n→`
1
n ln n
n52
(c) None
converges by the Alternating Series Test.
29. This is a geometric series which converges only for
1
2
)4x 1 1) , 1, or 2}} , x , 0.
But ∑ }} diverges by the integral test, since
n52
1
n ln n
E }x l1n}x dx 5 lim 3ln )ln x)4 5 `.
`
(a) (21, 1)
(b) (21, 1)
a 1
2 n11
lim }n1
} 5 (n 1 1)2 }}
a
3
n→`
n
`
27. This is a geometric series which converges only for )x) , 1.
b
b→`
2
n!
21. Diverges by the nth-Term Test, since lim }}n 5 ` and so the
n→` 2
terms do not approach 0.
`
) )
n51
sin n
n
comparison to ∑ }}2 , which converges as a p-series with
n51
1
n
1
2
2
1
1
2
2
(b) 2}}, 0
(c) None
22. Converges absolutely, since ∑ }}
2 converges by direct
`
1
(a) 2}}, 0
2
)a )
a
n→`
n
)3x 2 2)
n
The series converges absolutely when )3x 2 2) , 1, or
`
p 5 2.
∑
1
1
(21)n
}} , x , 1. Check x 5 }}:
}} converges
3
3 n51 n
`
`
1n
1
conditionally. Check x 5 1:
}} 5
}} diverges.
n51 n
n51 n
∑
23. Converges conditionally:
1
If un 5 }}, then {un} is a decreasing sequence of
1 1 Ïwn
`
(21)n
positive terms with lim un 5 0, so
}} converges
n→`
n51 1 1 Ïw
n
(a) }}, 1
by the Alternating Series Test.
(b) }}, 1
∑
`
`
But ∑ }} diverges by direct comparison to ∑ }1/2
},
n51 1 1 Ïn
n51 n
w
1
which diverges as a p-series with p 5 }}.
1
1
2
`
24. Converges absolutely, since ∑
n51
)
)
n51
`
cos np
n
n51
(21)n+1
n
1
3
(c) At x 5 }}
x22
} , 1, or 28 , x , 12.
)}
10 )
(b) (28, 12)
(c) None
)a )
a
(n 1 1))x) n11
n13
n→`
n12
n)x)
32. lim }n1
}1 5 lim }} ? }}
n 5 )x)
n→`
26. Converges conditionally:
n
The series converges absolutely when )x) , 1, or
1
If un 5 }}, then {un } is a decreasing sequence
1w1
Ïwn 1 Ïwnw
`
(21)n
of positive terms with lim un 5 0, so
}}
n→`
n51 Ïw
n 1 Ïwnw
1w1
∑
converges by the Alternating Series Test.
`
n
21 , x , 1. For )x) $ 1, the series diverges by the
nth-Term Test.
(a) (21, 1)
But ∑ un diverges by the Limit Comparison Test:
1/2
1
If vn 5 }1/2
}, then lim }}n 5 lim }} 5 }}.
n
n→` vn
n→` Ïn
1w1 ` 2
w 1 Ïnww
`
1
Since ∑ vn diverges as a p-series with p 5 }}, ∑ un also
n51
1
∑
(See Examples 2 and 4.)
u
13 2
(a) (28, 12)
`
1
1
31. This is a geometric series which converges only for
`
25. Converges conditionally, since ∑ }} 5 2∑ }}.
n51
∑
33 2
cos np
1
}} 5
}3/2
}, which
n51 n
nÏnw
converges as a p-series.
diverges.
)3x 2 2)n11
n11
n→`
30. lim }n1
}1 5 lim }} ? }}n 5 )3x 2 2)
2
n51
(b) (21, 1)
(c) None
Section 9.5
a 1
nÏwn 3n
)x)
)x)n11
33. lim }n1
5 }}
} 5 lim }}} ? }}
n
3
)x
)
n11
n→` an
n→` (n 1 1)Ïn
ww
1w1 ? 3
The series converges absolutely for )x) , 3. Furthermore,
) )
`
Σ
)
n
)a )
(n 1 1)!)x 2 4)n11
n!)x 2 4)
n→`
a
38. lim }n1
}1 5 lim }}
n
n→`
n
5 lim (n 1 1))x 2 4)
n→`
`
)
Σ
x
1
when )x) 5 3,
}} 5
}3/2
}, which also converges
n
n
n51 nÏw
n51
n3
3
as a p-series with p 5 }}.
2
(a) [23, 3]
389
5`,0, xx Þ5 44
5
(a) Only at x 5 4
(b) At x 5 4
(c) None
(b) [23, 3]
)a )
a
)22) n11(n 1 2))x 2 1) n11
)22) (n 1 1))x 2 1)
n→`
5 )2(x 2 1))
39. lim }n1
}1 5 lim }}}
n
n
(c) None
) )
a 1
)x)2n13
34. lim }n1
} 5 lim }}
n→` an
n→` (n 1 1)!
?
n!
x2
}2n}
11 5 lim }} 5 0
)x)
n→` n 1 1
n→`
n
The series converges absolutely for )2(x 2 1)) , 1, or
The series converges absolutely for all real numbers.
1
3
}} , x , }}. For )2(x 2 1)) $ 1, the series diverges by the
2
2
(a) All real numbers
nth-Term Test.
(b) All real numbers
12 22
1 3
(a) }}, }}
(c) None
)a )
)x 1 3)
5n
5
n)x
1 3)
n→`
n
)x 1 3)
The series converges absolutely for }} , 1,
5
)x 1 3)
or 28 , x , 2. For }} $ 1, the series diverges by
5
a
(n 1 1))x 1 3)n11
5
n→`
35. lim }n1
}1 5 lim }n1
}
? }}n 5 }}
1
the nth-Term Test.
a
(n 1 1))x)n11
[(n 1 1) 1 1]
36. lim }n1
}1 5 lim }}
n11
2
n→` 4
4n(n2 1 1)
)x)
} 5 }}
?}
n)x)n
4
)x)
4
The series converges absolutely for }} , 1, or 24 , x , 4.
Check x 5 24:
`
)a )
a
)4x 2 5) 2n13
n→` (n 1 1)
n 3/2
)4x 2 5)
2
40. lim }n1
}1 5 lim }}
3/2 ? }}
2n11 5 (4x 2 5)
n→`
n
`
`
(21)2n11
1
n
n51
n51 n
3
3
converges as a p-series with p 5 }}. Check x 5 }}:
2
2
`
12n11
3
}3}
/2 converges as a p-series with p 5 }}.
2
n51 n
3
2
(c) None
n
(c) None
1 , x , }}. Check x 5 1: ∑ }3}
5 2∑ }3/2
}
/2
(b) (28, 2)
n→`
1 3
The series converges absolutely for (4x 2 5)2 , 1, or
(a) (28, 2)
)a )
12 22
(b) }}, }}
∑
3 24
3
(a) 1, }}
3 24
3
(b) 1, }}
(21) n
} converges by the Alternating Series Test.
∑}
n2 1 1
n
n50
Check x 5 4:
`
∑
n
}
2 } diverges by the Limit Comparison Test
n50 n 1 1
`
1
with
}}.
n51 n
∑
(c) None
a 1
Ïnw
)x 1 p) n11
41. lim }n1
} 5 lim }} ? }}n 5 )x 1 p)
)x 1 p)
n→` an
n→` Ïw
nw
1w
1
The series converges absolutely for )x 1 p) , 1, or
) )
2p 2 1 , x , 2p 1 1.
(a) [24, 4)
Check x 5 2p 2 1:
(b) (24, 4)
(21)
} converges by Alternating Series Test.
∑}
`
(c) At x 5 24
n→`
n
n→`
3
3n
)x)
? }}n 5 }3}
Ïnw )x)
The series converges absolutely for )x) , 3, or 23 , x , 3.
For )x) $ 3, the series diverges by the nth-Term Test.
(a) (23, 3)
(b) (23, 3)
(c) None
Ïnw
Check x 5 2p 1 1:
n51
a 1
Ïnww
1w1 )x)n11
37. lim }n1
} 5 lim }}
n11
)a )
n
`
∑ }1} diverges as a p-series with p 5 }12}.
Ïwn
(a) [2p 2 1, 2p 1 1)
n51
(b) (2p 2 1, 2p 1 1)
(c) At x 5 2p 2 1
390
Section 9.5
42. This is a geometric series which converges only for
46. (a) Diverges by the Limit Comparison Test.
1
e
1
1
)ln x) , 1, or }} , x , e.
Let ak 5 }} and bk 5 }1}
. Then ak . 0 and
k /2
Ï2wkw1
ww7
ak
k1/2
1
bk . 0 for k $ 1 and lim }} 5 lim }} 5 }}.
b
k→` k
k→` Ï2
wkw1
ww7 Ï2w
`
1
Since ∑ bk diverges as a p-series with p 5 }},
1e 2
1
(a) }}, e
1 2
∑
k51
2
k51
`
1
e
(b) }}, e
ak also diverges.
(c) None
43. n 5 13 3 109 ? 365 ? 24 ? 3600 5 4.09968 3 1017
ln (n 1 1) , sum , 1 1 ln n
ln (4.09968 3 1017 1 1) , sum , 1 1 ln (4.09968 3
1017)
40.5548... , sum , 41.5548...
40.554 , sum , 41.555
(b) Diverges by the nth-Term Test, since
k→`
E
f (x) dx , a1 1 … 1 an , a1 1
1
E f (x) dx.
)
If the integral diverges, it must go to infinity, and the first
inequality forces the partial sums of the series to go to
infinity as well, so the series is divergent. If the integral
converges, then the second inequality puts an upper bound
on the partial sums of the series, and since they are a
nondecreasing sequence, they must converge to a finite sum
for the series. (See the explanation preceding Exercise 42 in
Section 9.4.)
)
p-series with p 5 2.
(d) Diverges by the integral test, since
E }x 1ln8}x dx 5 lim 318 ln )ln x)4
`
b→`
3
`
b
5`
3
47. One possible answer: ∑ }}
n53
1
n ln n
This series diverges by the integral test, since
E }x l1n}x dx 5 lim 3ln )ln x)4 5 `. Its partial sums are
`
b
b→`
3
45.
`
∑
cos k
1
1
}} , }}2 for k $ 1 and
}}2 converges as a
k
k51 k
k 2 1 Ïwk
n
1
2
(c) Converges absolutely by the Comparison Test, since
44. Comparing areas in the figures, we have for all n $ 1,
n11
1 k
5 e Þ 0.
k
1
lim 1 1 }}
3
roughly ln (ln n), so they are much smaller than the partial
y
sums for the harmonic series, which are about ln n.
y = f (x)
48. (a) ak 5 (21)k11
a N aN + 1
an – 1
0
N N+1 N+2
an
n
n+1
x
E
1/k
6(kx)2 dx
0
1/k
3 4
2
1}k}2
5 (21)k11 2k 2x 3
0
y
5 (21)
(b) The series converges by the Alternating Series Test.
y = f (x)
a N a N + 1 aN + 2
(c) The first few partial sums are:
an
0
N–1
N N+1 N+2
n–1
x
n
Comparing areas in the figures, we have for all n $ N,
E
n11
N
k11
f (x) dx , aN 1 … 1 an , aN 1
E f (x) dx.
n
N
If the integral diverges, it must go to infinity, and the first
inequality forces the partial sums of the series to go to
infinity as well, so the series is divergent. If the integral
converges, then the second inequality puts an upper bound
on the partial sums of the series, and since they are a
nondecreasing sequence, they must converge to a finite sum
for the series. (See the explanation preceding Exercise 42 in
Section 9.4.)
5
3
7
47
37
6
30
30
319
533
1879
S7 5 }}, S8 5 }}, S9 5 }}. For an alternating
210
420
1260
S1 5 2, S2 5 1, S3 5 }}, S4 5 }}, S5 5 }}, S6 5 }},
series, the sum is between any two adjacent partial
3
2
sums, so 1 , S8 # sum # S9 , }}.
49. (a) Diverges by the Limit Comparison Test. Let
n
3n 1 1
1
n
an 5 }
2 } and bn 5 }}. Then an . 0 and bn . 0 for
a
n2
11
3n
n→`
1
3
n $ 1, and lim }}n 5 lim }
2 } 5 }}. Since
`
n→` bn
`
∑ bn diverges, ∑ an diverges.
n51
n51
391
Section 9.5
`
`
`
n51
n
3n 1 1
3
n
n51
xn
n
53. ln (1 1 x) 5 Σ (21)n11 }}, so at x 5 1, the series is
(b) S 5 ∑ }
2 } ? }} 5 ∑ }
2 }.
3
3n 1 1
`
This series converges by the Direct Comparison Test,
Σ
n51
`
∑
3
1
1
since }
} , }}2 and
}}2 is convergent as a
3n2 1 1
n
n51 n
n51
(21)n11
}}. This series converges by the Alternating Series
n
Test.
p-series with p 5 2.
`
x 2n11
2n 1 1
54. arctan x 5 ∑ (21)n}}
n50
At x 5 21, the sequence is
50. (a) From the list of Maclaurin series in Section 9.2,
x2
x3
xn
2
3
n
ln (1 1 x) 5 x 2 }} 1 }} 2 … 1 (21)n11 }} 1 ….
`
`
(21) (21)
(21)
} 5 2∑ }}, which converges by the
∑}
2n 1 1
2n 1 1
n
2n11
n50
n
n50
Alternating Series Test. At x 5 1, the sequence is
(b) 21 , x # 1
`
(21)
}, which converges by the Alternating Series Test.
∑}
2n 1 1
3
1
(c) To estimate ln }}, we would let x 5 }}
2
2
n
n50
The truncation error is less than the magnitude of the
55. (a) It fails to satisfy un $ un11 for all n $ N.
`
(b) The sum is
sixth nonzero term, or
`
} 2 }}
1 ∑ }3}2 2 1 ∑ }2}25 }
1 2 1/3
1 2 1/2
1
6
1/3
1/2
n
n51
1
1
} 5 }} , 0.002605
)2}x6}) 5 }
2 ?6
384
1
n
n51
1
2
5 }} 2 1
6
1
2
5 2}}.
Thus, a bound for the (absolute) truncation error is
56. Answers will vary.
0.002605.
`
`
(21)n11x 2n
1
(21)n11(x 2)n
1
(d)
}} 5 }}
}} 5 }}ln (1 1 x 2)
2
2
2
n
n
n51
n51
∑
∑
) )
a
2k11)x)k11
51. lim }k1}1 5 lim }}
a
l
k→`
k→` n (k 1 3)
k
ln (k 1 2)
} 5 2)x)
?}
2 k)x) k
1
The series converges absolutely for )x) , }},
2
1
1
or 2}} , x , }}.
2
2
1
Check x 5 2}}:
2
`
(21)k
}} converges by the Alternating Series Test.
k50 ln (k 1 2)
1
Check x 5 }}:
2
`
1
}} diverges by the Direct Comparison Test, since
k50 ln (k 1 2)
`
1
1
1
}} . }} for k $ 2 and
}} diverges. The original
k
ln (k 1 2)
k52 k
1
1
series converges for 2}} # x , }}.
2
2
∑
∑
∑
52. (a) The series converges by the Direct Comparison Test,
n
(Ïnw)2
n2
}}§ 5 lim }} 5 }}
2
2
2
n→` !§
n→`
n
n
57. (a) lim Ïawwn 5 lim
n→`
1
n
The series converges.
} 5 }}
!§1}
§2n§2}§1 §2 5 lim }
2
2n 2 1
n
n→`
n→`
n
n
n
(b) lim Ïawwn 5 lim
n
1
n→`
The series converges.
(c)
n
lim
n→`, n odd
n→`, n odd
5
lim
n→`, n even
!}§2}§
lim
n→`, n odd
n
Ïawwn 5
n
n
Ïawwn 5 lim
lim
n
Ïwn 1
}} 5 }}
2
2
n→`, n even
n
n
!}§2}§ 5 }2}
n
1
1
n
1
2
Thus, lim Ïawwn 5 }}, so the series converges.
n→`
n
n )x 2 1) n
n→`
)x 2 1)
5 }}
}}
4§§
4
n→` !§§
wwn) 5 lim
58. (a) lim Ï)a
n
)x 2 1)
4
since }
p } , }}
p for n $ 3, and ∑ }}
p converges as a
The series converges absolutely if }} , 1, or
p-series when p . 1.
23 , x , 5.
1
n ln n
`
1
n
n53
1
n
`
`
(b) For p 5 1, the series is ∑ }}, which diverges by the
E
`
Integral Test, since
2
n52
1
n ln n
3
4
1
}} dx 5 lim ln (ln x)
x ln x
b→`
b
5 `.
2
1
1
(c) For 0 # p , 1, we have }
} . }}, so
n p ln n
n ln n
`
1
}
p } diverges by the Direct Comparison Test with
n52 n ln n
1
}} from part (b).
n ln n
∑
Check x 5 23: ∑ (21)n diverges.
n50
`
Check x 5 5: ∑ 1n diverges.
n50
The interval of convergence is (23, 5).
392
Chapter 9 Review
58. continued
)a )
)x 1 4)
n3 n
3
)x
1
4)
n→`
n
)x 1 4)
The series converges absolutely for }} , 1,
3
)x 1 4)n11
n→` (n 1 1)3
a
5 lim
!§
?
Ïw ?
n )x 2 2) n
)x 2 2)
)x 2 2)
}
n } 5 }}
3
n 3
)x 2 2)
The series converges absolutely if }} , 1, or
3
n
(b) lim Ï)a
wwn) 5 lim
n→`
}
n 3n
n→`
n→`
2. lim }n1
}1 5 lim }}
n11 ? }}
n 5 }}
or 27 , x , 21.
`
Check x 5 27: ∑ }} converges
21 , x , 5.
`
n51
`
Check x 5 21: ∑
Check x 5 21: ∑ }} converges.
n51
`
(21)n
n
n51
∑
1
Check x 5 5:
}} diverges.
n51 n
(a) 3
The interval of convergence is [21, 5).
(c) (27, 21)
n
(b) [27, 21)
(d) At x 5 27
n
(c) lim Ï)a
wwn) 5 lim Ï2wnw)x)
wnw 5 2)x)
n→`
n→`
3. This is a geometric series, so it converges absolutely when
The series converges absolutely if
)r) , 1 and diverges for all other values of x. Since
1
1
2 `
2
1
Check x 5 2}}:
(21)n diverges.
2 n51
2)x) , 1, or 2}} , x , }}.
2
3
r 5 }}(x 2 1), the series converges absolutely when
∑
)}23}(x 2 1)) , 1, or 2}12} , x , }52}.
`
Check x 5 }}: ∑ 1 diverges.
1
2
1
1 1
2 2
2
The interval of convergence is 2}}, }} .
n
wwn) 5 lim Ï)ln
wwxw
) 5 )ln x)
(d) lim Ï)a
n→`
3
2
(a) }}
n51
n
1
1 5
2 2
2
1
1 5
2 2
2
(b) 2}}, }}
n
(c) 2}}, }}
n→`
The series converges absolutely if )ln x) , 1, or
1
}} , x , e.
e
(d) None
)a )
a
`
`
1 n
5
(21)n diverges.
e
n50
1 2
Check: x 5 }}: ∑ ln }}
1
e
n50
`
∑
n50
)x 2 1)2n
(2n 2 1)!
)x 2 1)
n→` (2n 1 1)!
)x 2 1)2
5 lim }} 5 0
n→` (2n 1 1)(2n)
4. lim }n1
}1 5 lim }} ? }}
2n22
n→`
n
`
Check x 5 e: ∑ (ln e)n 5 ∑ 1n diverges.
n50
(21)n
n
1
}} diverges.
n
The series converges absolutely for all x.
(a) `
1e 2
1
The interval of convergence is }}, e .
(b) All real numbers
(c) All real numbers
■ Chapter 9 Review Exercises
(pp. 509–511)
)a )
a
n
)a )
a
)2x)
n11
n!
)2x)
)x)
1. lim }n1
}1 5 lim }} ? }}n 5 lim }} 5 0
n→`
(d) None
n→` (n 1 1)!
n→` n 1 1
The series converges absolutely for all x.
(a) `
)3x 2 1)n11
n→` (n 1 1)
n2
)3x 2 1)
5. lim }n1
}1 5 lim }}
2 ? }}
n 5 )3x 2 1)
n→`
n
The series converges absolutely for
2
3
)3x 2 1) , 1, or 0 , x , }}. Furthermore, when
1
n
(b) All real numbers
)3x 2 1) 5 1, we have )an) 5 }}2 and
(c) All real numbers
∑ }n1}2 converges as a p-series with p 5 2, so ∑ an also
(d) None
`
n51
`
n51
converges absolutely at the interval endpoints.
1
3
(a) }}
3 34
2
(b) 0, }}
3 34
2
(c) 0, }}
(d) None
Chapter 9 Review
)a )
) )
(n 1 2))x)3n13
n→` (n 1 1))x)
a
3
6. lim }n1
}1 5 lim }}
3n 5 )x)
n→`
n
393
The series converges absolutely for )x) , 1, or
3
a 1
Ïnw
)x)n11
9. lim }n1
} 5 lim }} ? }}
n 5 )x)
n→` an
n→` Ïw
nw
1w1 )x)
The series converges absolutely for )x) , 1, or 21 , x , 1.
21 , x , 1. When )x) $ 1, the series diverges by the nth
Check x 5 21:
Term Test.
(21)
} converges by the Alternating Series Test.
∑}
n
`
n
n51
(a) 1
Check x 5 1:
(b) (21, 1)
∑ }1} diverges as a p-series with p 5 }12}.
`
Ïnw
(a) 1
(c) (21, 1)
n51
(d) None
(b) [21, 1)
) )
a 1
(n 1 2))2x 1 1)n11
7. lim }n1
} 5 lim }}
(2n 1 3)2n11
n→` an
n→`
)2x 1 1)
5 }}
2
?
(2n 1 1)2n
}}n
(n 1 1))2x 1 1)
(d) At x 5 21
)a )
e n11)x)n11
n→` (n 1 1)
a
)2x 1 1)
The series converges absolutely for }} , 1, or
2
3
1
)2x 1 1)
2}} , x , }}. When }} $ 1, the series diverges by the
2
2
2
nth-Term Test.
ne
e )x)
10. lim }n1
}1 5 lim }}
e ? }
n}
n 5 e)x)
n→`
n
The series converges absolutely for e)x) , 1,
1
e
1
e
or 2}} , x , }}.
`
1
`
Furthermore, when e)x) 5 1, we have )an) 5 }}e and ∑ }}e
(a) 1
1
n
n51
1
n
converges as a p-series with p 5 e, so ∑ an also converges
2
3 1
(b) 2}}, }}
2 2
(c)
(c) (21, 1)
n51
absolutely at the interval endpoints.
12}2}, }2}2
3 1
1
e
(a) }}
(d) None
)a )
)x)n11
nn
nn
)x)
n→`
n→` (n 1 1)
n→` (n 1 1)(n 1 1)
n
1
)x)
1
5 )x) lim }}
1 n 5 }} lim }} 5 0
e n→` n 1 1
n→` (n 1 1) 1 1 }}
a
8. lim }n1
}1 5 lim }}
n11 ? }}
n 5 )x) lim }}
n
1
n
2
3
1 1
e e
4
3
1 1
e e
4
(b) 2}}, }}
(c) 2}}, }}
(d) None
The series converges absolutely for all x.
)a )
) nx ) 1 12 2
n
n
observe that for n $ 2x, we have }}n # }} , so the terms
(n 1 2))x)2n11
3
n→`
3n
(n 1 1))x)
n→`
n
x2
The series converges absolutely when }} , 1,
3
a
Another way to see that the series must converge is to
x2
3
11. lim }n1
}1 5 lim }n1
}
? }}
1
2n21 5 }}
are (eventually) bounded by the terms of a convergent
or 2Ï3w , x , Ï3w.
geometric series.
When )x) $ Ï3w, the series diverges by the nth Term Test.
A third way to solve this exercise is to use the nth Root
(a) Ï3w
Test (see Exercises 57–58 in Section 9.5).
(b) (2Ï3w, Ï3w)
(a) `
(b) All real numbers
(c) All real numbers
(d) None
(c) (2Ï3w, Ï3w)
(d) None
394
Chapter 9 Review
)a )
a
)x 2 1)2n13
n→` 2n 1 3
2n 1 1
)x 2 1)
2
12. lim }n1
}1 5 lim }} ? }}
2n11 5 )x 2 1)
n→`
n
x2 2 1
2
16. This is a geometric series with r 5 }}, so it converges
) x 22 1 )
2
The series converges absolutely when )x 2 1)2 , 1,
absolutely when }} , 1, or 2Ï3w , x , Ï3w. It
or 0 , x , 2.
diverges for all other values of x.
`
`
(21)
2n 1 1
Check x 5 0: ∑ }} 5 2∑ }} converges
n
2n21
(21) (21)
2n 1 1
n50
n50
n
conditionally by the Alternating Series Test.
`
(21)n
2n 1 1
Check x 5 2: ∑ }} converges conditionally by the
n50
Alternating Series Test.
(a) Ï3w
(b) (2Ï3w, Ï3w)
(c) (2Ï3w, Ï3w)
(d) None
17. f (x) 5 }} 5 1 2 x 1 x 2 2 … 1 (21)nx n 1 …,
1
11x
(a) 1
1
evaluated at x 5 }}. Sum 5 }
1 5 }}.
1
4
(b) [0, 2]
(c) (0, 2)
x2
2
a
(n 1 1)!)x)2n12
2
n→`
2n
n!)x)
13. lim }n1
}1 5 lim }n1
}
? }}
1
2n
n→`
n
(n 1 1)x 2
2
n→`
5 lim }} 5
h
x3
3!
2
3
2
132
5
x5
5!
x 2n11
(2n 1 1)!
evaluated at x 5 p. Sum 5 sin p 5 0.
x2
2!
x4
4!
x 2n
(2n)!
20. f (x) 5 cos x 5 1 2 }} 1 }} 2 … 1 (21)n}} 1 …,
p
3
(b) x 5 0 only
a
x2
2!
)10x)n11
ln
(n 1 1)
n→`
ln n
)10x)
14. lim }n1
}1 5 lim }} ? }}n 5 )10x)
n
1
2
xn
n!
21. f (x) 5 e x 5 1 1 x 1 }} 1 … 1 }} 1 …, evaluated at
(d) None
)a )
p
3
evaluated at x 5 }}. Sum 5 cos }} 5 }}.
(c) x 5 0
The series converges absolutely for )10x) , 1,
1
10
1
10
or 2}} , x , }}.
`
∑
(21)n
1
Check n 5 2}}:
}} converges by the Alternating
10 n52 ln n
x 5 ln 2. Sum 5 e ln 2 5 2.
x 2n11
2n 1 1
1
1
p
evaluated at x 5 }}. Sum 5 tan21 }} 5 }}. (Note that
6
Ïw3
Ïw3
x3
3
x5
5
22. f (x) 5 tan21 x 5 x 2 }} 1 }} 2 … 1 (21)n}} 1 …,
1 2
when n is replaced by n 2 1, the general term of tan21 x
x 2n21
2n 2 1
becomes (21)n21}}, which matches the general term
Series Test.
`
Check n 5 }}: ∑ }} diverges by the Direct Comparison
1
1
10 n52 ln n
`
1
1
1
Test, since }} . }} for n $ 2 and
}} diverges.
n
ln n
n52 n
∑
given in the exercise.)
1
12x
23. Replace x by 6x in the Maclaurin series for }} given at
the end of Section 9.2.
1
10
(a) }}
3
1
}} 5 1 1 (6x) 1 (6x)2 1 … 1 (6x)n 1 …
1 2 6x
2
1 1
(b) 2}}, }}
10 10
1 1
10 10
5 1 1 6x 1 36x 2 1 … 1 (6x)n 1 …
2
(c) 2}}, }}
1
11x
24. Replace x by x 3 in the Maclaurin series for }} given at
1
10
(d) At x 5 2}}
)a )
a
(n 1 2)!)x)n11
n→` (n 1 1)!)x)
the end of Section 9.2.
15. lim }n1
}1 5 lim }}
n 5 lim (n 1 2))x) 5 ` (x Þ 0)
n→`
1
2
3
19. f (x) 5 sin x 5 x 2 }} 1 }} 2 … 1 (21)n}} 1 …,
0, x 5 0
`, x Þ 0
(a) 0
1
xn
n
evaluated at x 5 }}. Sum 5 ln 1 1 }} 5 ln }} .
The series converges only at x 5 0.
n→`
x3
3
18. f (x) 5 ln (1 1 x) 5 x 2 }} 1 }} 2 … 1 (21)n21}},
(d) At x 5 0 and x 5 2
)a )
4
5
142
1 1 }}
n
n→`
The series converges only at x 5 0.
(a) 0
(b) x 5 0 only
(c) x 5 0
(d) None
1
}}3 5 1 2 (x 3) 1 (x 3) 2 2 … 1 (2x 3)n 1 …
11x
5 1 2 x 3 1 x 6 2 … 1 (21)nx 3n 1 …
25. The Maclaurin series for a polynomial is the polynomial
itself: 1 2 2x 2 1 x 9.
395
Chapter 9 Review
4x
12x
33. Use the Maclaurin series for e x given at the end of
11 2 x2
1
26. }} 5 4x }}
5 4x(1 1 x 1 x 2 1 … 1 x n 1 …)
Section 9.2.
(2x 2)2
2!
3
(2x 2)n
n!
xe2x 5 x 1 1 (2x 2) 1 }} 1 … 1 }} 1 …
2
5 4x 1 4x 2 1 4x 3 1 … 1 4x n 1 1 1 …
x5
x 2n11
5 x 2 x 1 }} 2 … 1 (21)n}} 1 …
2!
n!
4
3
27. Replace x by px in the Maclaurin series for sin x given at
34. Replace x by 3x in the Maclaurin series for tan21 x given at
the end of Section 9.2.
(px)3
3!
(px)2n11
(2n 1 1)!
(px)5
5!
sin px 5 px 2 }} 1 }} 2 … 1 (21)n}} 1 …
2x
3
(
2x 3
2x 5
1}}2
2x 2n+1
1}}2
1}}2
2x
2x
3
3
3
1}
2 … 1 (21)n}
2sin }} 5 2 }} 2 }
3!
5!
(2n 1 1)!
3
3
(3x)3
3
)
given at the end of Section 9.2.
(22x)2
(22x)3
2
3
(22x)n
1 (21)n21}} 1 …
n
8x 3
(2x)n
2
5 22x 2 2x 2 }} 2 … 2 }} 2 ….
3
n
ln (1 2 2x) 5 22x 2 }} 1 }} 2 …
2x 2n11
1 2
x3
x5
x7
3!
5!
7!
2n11
x
1 (21)n}} 1 …
(2n 1 1)!
x3
x5 x7
x 2n11
5 2}} 1 }} 2}} 1 … 1 (21)n}} 1 …
3!
5! 7!
(2n 1 1)!
1
29. 2x 1 sin x 5 2x 1 x 2 }} 1 }} 2 }} 1 …
2
e x 1 e 2x
2
1
2
x2
2!
1
xn
n!
2
2
1
x
xn
2
2!
n!
2n
x2
x4
x
5 1 1 }} 1 }} 1 … 1 }} 1 …
2!
4!
(2n)!
1
1 }} 1 2 x 1 }} 1 … 1(21)n}} 1 …
2
31. Replace x by Ï5wxw in the Maclaurin series for cos x given at
the end of Section 9.2.
(Ïw5wx)2
(Ï5wxw)4
cos Ï5wxw 5 1 2 }} 1 }} 2 …
2!
4!
5wx)2n
n (Ïw
1 (21) }} 1 …
(2n)!
5x
(5x)2
(5x)n
5 1 2 }} 1 }} 2 … 1 (21)n}} 1 …
2!
4!
(2n)!
px
2
32. Replace x by }} in the Maclaurin series for e x given at the
end of Section 9.2.
(3x)2n11
2n 1 1
35. Replace x by 22x in the Maclaurin series for ln (1 1 x)
(21)n11 }}
2x
4x 3
4x 5
3
5 2}} 1 }} 2 }} 1 … 1 }}
(2n 1 1)!
3
81
3645
30. }} 5 }} 1 1 x 1 }} 1 … 1 }} 1 …
(3x)5
5
tan21 3x 5 3x 2 }} 1 }} 2 … 1 (21)n}} 1 …
28. Replace x by }} in the Maclaurin series for sin x given at
the end of Section 9.2
the end of Section 9.2.
36. Use the Maclaurin series for ln (1 1 x) given at the end of
Section 9.2.
x ln (1 2 x) 5 x ln [1 1 (2x)]
3
(2x)2
(2x)3
2
3
x3
x4
x n11
2
…
5 2x 2 }} 2 }} 2
2 }} 2 …
2
3
n
(2x)n
n
5 x 2x 2 }} 1 }} 2 … 1 (21)n21}} 1 …
4
)
37. f (2) 5 (3 2 x)21 x52 5 1
)x52 5 1
f 0(2)
f 0(2) 5 2(3 2 x)23)x52 5 2, so }} 5 1
2!
f -(2)
f -(2) 5 6(3 2 x)24)x52 5 6, so }} 5 1
3!
f (2)
(n)
2n21
f (2) 5 n!(3 2 x)
)x52 5 n!, so }
}51
n!
f9(2) 5 (3 2 x)
22
(n)
1
}} 5 1 1 (x 2 2) 1 (x 2 2)2 1 (x 2 2)3 1 …
32x
1 (x 2 2)n 1 …
)
38. f (21) 5 (x 3 2 2x 2 1 5) x521 5 2
)
f9(21) 5 (3x 2 2 4x) x521 5 7
)
f 0(21)
2!
f 0(21) 5 (6x 2 4) x521 5 210, so }} 5 25
)
f -(21)
3!
f -(21) 5 6 x521 5 6, so }} 5 1
px 2
1}}2
px n
1}}2
px
2
2
1…1}
1…
e px/2 5 1 1 }} 1 }
2!
n!
2
px
p 2x 2
1 px n
5 1 1 }} 1 }} 1 … 1 }} }} 1 …
2
8
n! 2
1 2
f (n)(21) 5 0 for n $ 4.
x 3 2 2x 2 1 5 5 2 1 7(x 1 1) 2 5(x 1 1)2 1 (x 1 1)3
This is a finite series and the general term for n $ 4 is 0.
396
Chapter 9 Review
1
x
)
45. Converges conditionally:
1
3
39. f (3) 5 }} x53 5 }}
)
1
ln (n 1 1)
If un 5 }}, then {un} is a decreasing sequence of
1
9
f9(3) 5 2x22 x53 5 2}}
)
f 0(3)
2
1
f 0(3) 5 2x x53 5 }}, so }} 5 }}
2!
27
27
f -(3)
2
1
f -(3) 5 26x24 x53 5 2}}, so }} 5 2}}
3!
27
81
f (n)(3)
(21)n
}} 5 }n}
3 +1
n!
1
1
1
1
1
}} 5 }} 2 }}(x 2 3) 1 }}(x 2 3)2 2 }}(x 2 3)3 1 …
x
3
9
27
81
(x 2 3)n
1 (21)n}n+}
3 1
23
)
)
)
2
b→`
)a )
)23)n11
n→` (n 1 1)!
a
n→`
n!
)23)
3
n
n→` n 1 1
48. Converges absolutely by the Direct Comparison Test, since
1
1
sin x 5 2(x 2 p) 1 }}(x 2 p)3 2 }}(x 2 p)5
3!
5!
1
1 }}(x 2 p)7 2 …
7!
1
1 (21)n11}}(x 2 p)2n11 1 …
(2n 1 1)!
41. Diverges, because it is 25 times the harmonic series:
n51
Comparison Test.
lim }n1
}1 5 lim }} ? }}n 5 lim }} 5 0.
5
n51
∑
47. Converges absolutely the the Ratio Test, because
0, if k is even
f (p) 5 21, if k 5 2n 1 1, n even
1, if k 5 2n 1 1, n odd
`
∑
2
f 0(p)
2!
f -(p)
1
f -(p) 5 2cos x x5p 5 1, so }} 5 }}
3!
6
`
1
1
n
ln
(n
1
1)
`
`
1
1
}} diverges, so
}} diverges by the Direct
n51 n
n51 ln (n 1 1)
conditional because }} . }} for n $ 1 and
`
f 0(p) 5 2sin x x5p 5 0, so }} 5 0
(k)
n→`
by the Alternating Series Test. The convergence is
1
1 b
1
E}
} dx 5 lim 2}} 5 }}.
3 ln x 42 ln 2
x(ln x)
f9(p) 5 cos x x5p 5 21
)
(21)n
ln
n51 (n 1 1)
46. Converges absolutely by the Integral Test, because
40. f (p) 5 sin x x5p 5 0
)
`
positive terms with lim un 5 0, so ∑ }} converges
∑ }2n}5 5 25∑ }1n} 5 2`
`
2n3n
1 n
1 n
for n $ 12 and
}}
}} is a convergent
n # }}
n
2
n51 2
12
∑1
2
geometric series. Alternately, we may use the Ratio Test or
the nth-Root Test (see Exercise 57 and 58 in Section 9.5).
49. Diverges by the nth-Term Test, since
(21)n(n2 1 1)
n→` 2n 1 n 2 1
lim }
} does not exist.
2
50. Converges absolutely by the Direct Comparison Test, since
42. Converges conditionally.
`
1
If un 5 }}, then {un} is a decreasing sequence of positive
Ïwn
`
(21)n
terms with lim un 5 0, so ∑ }} converges by the
n→`
n51 Ïn
w
Alternating Series Test. The convergence is conditional
`
1
2
because ∑ }} is a divergent p-series p 5 }} .
2
n51 Ïn
w
1
1
43. Converges absolutely by the Direct Comparison Test, since
`
∑
1
1
1
}} , }3/2
} and
}3/2
} converges as a p-series
n
n
n51
Ïwnw
(nw
1w1)(
wnww
1w
2)w
3
with p 5 }}.
2
51. Converges absolutely by the Limit Comparison Test.
1
1
Let an 5 }} and bn 5 }}2 .
n
nÏn
w2w2
ww1
`
0 # }}
3 , }}
2 for n $ 1 and ∑ }}
2 converges as a p-series
Then lim }}n 5 lim }} 5 1 and ∑ }}2 converges as a
n→` bn
n→` nÏn
n52 n
w2w2
ww1
with p 5 2.
p-series ( p 5 2). Therefore ∑ an converges.
ln n
n
1
n
1
n
n51
n2
a
`
n52
44. Converges absolutely by the Ratio Test, since
) )
a 1
n12
lim }n1
} 5 lim }}
n→` an
n→` (n 1 1)!
?
n!
n12
}} 5 lim }}2 5 0.
n 1 1 n→` (n 1 1)
52. Diverges by the nth-Term Test, since
n
1n 1 12
n
lim }}
n→`
1
1 2n
1
5 }} Þ 0.
n
e
2
5 lim 1 1 }}
n→`
1
Chapter 9 Review
(c) The fourth order Taylor polynomial for g(x) at x 5 4 is
53. This is a telescoping series.
`
`
1
1
1
} 5 ∑ }} 2 }}
∑}
1 2(2n 2 3) 2(2n 2 1) 2
(2n 2 3)(2n 2 1)
n53
n53
1
1
1
1
s1 5 }} 2 }} 5 }} 2 }}
6
2(2 ? 3 2 3)
2(2 ? 3 2 1)
10
1
1
1
1
1
1
s2 5 }} 2 }} 1 }} 2 }} 5 }} 2 }}
6
6
10
10
14
14
1
1
1
1
1
1
1
1
s3 5 }} 2 }} 1 }} 2 }} 1 }} 2 }} 5 }} 2 }}
6
6
10
10
14
14
18
18
1
1
sn 5 }} 2 }}
6
2(2n 2 1)
1
S 5 lim sn 5 }}
6
n→`
1
1
2 1
2 1
397
2
2 1
2
E [7 2 3(t 2 4) 1 5(t 2 4) 2 2(t 2 4) ] dx
3
5
1
x
5 7t 2 }}(t 2 4) 1 }}(t 2 4) 2 }}(t 2 4)
3 2
44
3
2
x
2
3
4
2
3
3
2
5
3
4
1
2
5 7(x 2 4) 2 }}(x 2 4)2 1 }}(x 2 4)3 2 }}(x 2 4)4
(d) No. One would need the entire Taylor series for f (x),
and it would have to converge to f (x) at x 5 3.
57. (a) Use the Maclaurin series for sin x given at the end of
Section 9.2.
54. This is a telescoping series.
`
`
n52
n52
122
x
5 sin }}
2
22
2
} 5 ∑ 2}} 1 }}
∑}
1 n n 1 12
n(n 1 1)
x
2
2
2
2
3
3
2
2
2
2
s2 5 21 1 }} 1 2}} 1 }} 5 21 1 }}
3
3
4
4
2
2
2
2
2
2
s3 5 21 1}} 1 2}} 1 }} 1 2}} 1 }} 5 21 1 }}
3
4
4
5
5
3
2
sn 5 21 1 }}
n12
s1 5 2}} 1 }} 5 21 1 }}
1
1
2 1
2 1
(x/2)3
(x/2)5
(x/2)2n11
3!
5!
(2n 1 1)!
5x
5x 3
x5
5
x 2n+1 …
5 }} 2 }} 1 }} 2 … 1 (21)n}} }}
1
2
48
768
(2n 1 1)! 2
32
5 5 }} 2 }} 1 }} 2 … 1 (21)n}} 1 …
2
2 1
2
(b) The series converges for all real numbers, according to
the Ratio Test:
)a )
a
n
n→`
f 0(3)
2!
55. (a) P3(x) 5 f (3) 1 f9(3)(x 2 3) 1 }}(x 2 3)2
f -(3)
1 }}(x 2 3)3
3!
5 1 1 4(x 2 3) 1 3(x 2 3)2 1 2(x 2 3)3
f (3.2) < P3(3.2) 5 1.936
(b) Since the Taylor series for f9 can be obtained by term-
))
))
5
x 2n13 (2n 1 1)! 2 2n+1
? }5} }x}
(2n
1
3)!
2
n→`
2
)x/2)
5 lim }} 5 0
n→` (2n 1 3)(2n 1 2)
lim }n1
}1 5 lim }} }}
n→`
S 5 lim sn 5 21
12
5
2
(c) Note that the absolute value of f (n)(x) is bounded by }}n
for all x and all n 5 1, 2, 3, ….
We may use the Remainder Estimation Theorem with
1
2
M 5 5 and r 5 }}.
So if 22 , x , 2, the truncation error using
by-term differentiation of the Taylor Series for f, the
Pn is bounded by
second order Taylor polynomial for f9 at x 5 3 is
5
}n11
}
2
4 1 6(x 2 3) 1 6(x 2 3)2. Evaluated at x 5 2.7,
To make this less than 0.1 requires n $ 4. So, two
f9(2.7) < 2.74.
terms (up through degree 4) are needed.
(c) It underestimates the values, since f 0(3) 5 6, which
means the graph of f is concave up near x 5 3.
56. (a) Since the constant term is f (4), f (4) 5 7. Since
f -(4)
3!
2n11
5
} 5 }}.
?}
(n 1 1)!
(n 1 1)!
1
12x
58. (a) Substitute 2x for x in the Maclaurin series for }}
given at the end of Section 9.2.
1
}} 5 1 1 2x 1 (2x)2 1 (2x)3 1 … 1 (2x)n 1 …
1 2 2x
5 1 1 2x 1 4x 2 1 8x 3 1 … 1 (2x)n 1 …
22 5 }}, f -(4) 5 212.
(b) Note that
P49(x) 5 23 1 10(x 2 4) 2 6(x 2 4)2 1 24(x 2 4)3.
The second degree polynomial for f9 at x 5 4 is given
by the first three terms of this expression, namely
23 1 10(x 2 4) 2 6(x 2 4)2. Evaluating at x 5 4.3,
f9(4.3) < 20.54.
4
1
1 1
2 2
2
1
12t
(b) 2}}, }} . The series for }} is known to converge for
2 1 , t , 1, so by substituting t 5 2x, we find the
resulting series converges for 21 , 2x , 1.
398
Chapter 9 Review
58. continued
(b) Integrate term by term.
1 42
1
2
3
(c) f 2}} 5 }}, so one percent is approximately 0.0067. It
takes 7 terms (up through degree 6). This can be found
1
4
by trial and error. Also, for x 5 2}}, the series is the
`
1 n
1 22
alternating series ∑ 2}} . If you use the Alternating
n50
Series Estimation Theorem, it shows that 8 terms (up
) 12 )
8
through degree 7) are sufficient since 2}} , 0.0067.
It is also a geometric series, and you could use the
remainder formula for a geometric series to determine
the number of terms needed. (See Example 2 in
ln )x 2 2) 5
E }t 21}2 dt
x
3
3
1
1
1
5 t 2 }}(t 2 3)2 1 }}(t 2 3)3 2 }}(t 2 3)4 1 …
2
3
4
x
n+1
(t
2
3)
1 (21)n}} 1 …
n11
3
(x 2 3)2
(x 2 3)3
(x 2 3)4
5 (x 2 3) 2 }} 1 }} 2 }} 1 …
2
3
4
n11
n (x 2 3)
1 (21) }} 1 …
n11
4
(c) Evaluate at x 5 3.5. This is the alternating series
1
1
1
1
}} 2 }
}1}
} 2 … 1 (21)n}
}1…
2
22 ? 2
23 ? 3
2n11(n 1 1)
By the Alternating Series Estimation Theorem, since
Section 9.3.)
)a )
a
1
24
the size of the third term is }} , 0.05, the first two
)x)n11(n 1 1)n11
n!
}
?}
(n 1 1)!
)x)nnn
n11
)x)(n 1 1)
5 lim }}
n
n→` (n 1 1)n
n11 n
5 )x)lim }} 5 )x)e
n
n→`
n→`
n
3
n→`
1
61. (a) Substitute 22x 2 for x in the Maclaurin series for e x
2
given at the end of Section 9.2.
1
e
The series converges for )x)e , 1, or )x) , }}, so the
2
1
e
1 32
1
1 1
1 2
3 1
3
1
2
1
5 2}} 1 }} 2 }}
3
9
6
5
5 2}} < 20.278
18
1 2
1 3
? }2}! 1 12}3}2 ? }3}!
22
33
(b) Use the Ratio Test:
)1 2
} < 0.132.
? }4}! ) 5 }
243
44
32
)
n!
2x
n
n→` (n 1 1)!
2x 2
n
n→` 1 1
5 lim }} 5 0
The series converges for all real numbers, so the
(c) This is an alternating series. The difference will be
)
f9(3) 5 2(x 2 2)22 x53 5 21
f 0(3)
2!
bounded by the magnitude of the fifth term, which is
f 0(3) 5 2(x 2 2)23 x53 = 2, so }} 5 1
)
n→`
interval of convergence is (2`, `).
60. (a) f (3) 5 (x 2 2)21 x53 5 1
)
2n11x 2n12
a
is no more than the magnitude of the next term, which
1 4
3
)a )
lim }n1
}1 5 lim }} ? }
n}
2n
(c) By the Alternating Series Estimation Theorem the error
is 2}}
(22x 2)2
(22x 2)3
2!
3!
(22x 2)n
1 … 1 }} 1 …
n!
4x 6
5 1 2 2x 2 1 2x 4 2 }} 1 …
3
2nx 2n
1 (21)n}} 1 …
n!
e22x 5 1 1 (22x 2) 1 }} 1 }}
radius of convergence is }}.
(b) f 2}} < 2}} ? }} 1 2}}
122
terms will suffice. The estimate for ln }} is 0.375.
59. (a) lim }n1
}1 5 lim }}
f -(3)
3!
f -(3) 5 26(x 2 2)24 x53 5 26, so }} 5 21
f (n)(3)
n!
f (n)(3) 5 (21)nn!, so }} 5 (21)n
f (x) 5 1 2 (x 2 3) 1 (x 2 3)2 2 (x 2 3)3 1 …
1 (21)n(x 2 3)n 1 …
(2x 2)4
2x 8
}} 5 }}. Since 20.6 # x # 0.6, this term is less
4!
3
2(0.6)8
than }} which is less than 0.02.
3
11 1 x2
1
62. (a) f (x) 5 x 2 }}
5 x 2(1 2 x 1 x 2 1 … 1 (2x)n 1 …)
5 x 2 2 x 3 1 x 4 1 … 1 (21)nx n+2 1 …
`
(b) No. At x 5 1, the series is ∑ (21)n and the partial
n50
sums form the sequence 1, 0, 1, 0, 1, 0, …, which has
no limit.
Chapter 9 Review
63. (a) Substituting x 2 for x in the Maclaurin series for sin x
du 5 2x dx
given at the end of Section 9.2,
6
10
4n12
sin x 2 5 x 2 2 }} 1 }} 2 … 1 (21)n}}.
x
3!
x
5!
x
(2n 1 1)!
Integrating term-by-term and observing that the
constant term is 0,
E sin t
x
0
2
x3
3
x7
7(3!)
(e) Let u 5 x 2
Ex e
2 x
v 5 ex
E
Let u 5 2x
dv 5 e x dx
du 5 2 dx
v 5 ex
E
3
x 2e x 2 2xe x dx 5 x 2e x 2 2xe x 2 2e x dx
5 x e 2 2xe 1 2e x 1 C
2 x
4n13
1 (21)n}} 1 …
x
(4n 1 3)(2n 1 1)!
1
E sin x dx 5 }13} 2 }7(13!)} 1 }
}2…
11(5!)
1
(b)
dv 5 e x dx
dx 5 x 2e x 2 2x e x dx
E
x1 1
11(5!)
dt 5 }} 2 }} 1 }} 2 …
Exe
1
0
1
1 (21)n}} 1 ….
(4n 1 3)(2n 1 1)!
1
1
Since the third term is }} 5 }} , 0.001, it
11(5!)
1320
suffices to use the first two nonzero terms (through
degree 7).
2 x
0
399
x
4
5 (x 2 2 2x 1 2)e x 1 C
40 5 e 2 2 < 0.71828
dx 5 (x 2 2 2x 1 2)e x
1
65. (a) Because [$1000(1.08)2n](1.08)n 5 $1000 will be
available after n years.
(b) Assume that the first payment goes to the charity at the
end of the first year.
1000(1.08)21 1 1000(1.08)22 1 1000(1.08)23 1 …
(c) This is a geometric series with sum equal to
(c) NINT(sin x 2, x, 0, 1) < 0.31026830
1
3
1
7(3!)
1
11(5!)
1
15(7!)
1000
1000/1.08
}} 5 }} 5 12,500. This means that $12,500
0.08
1 2 (1/1.08)
258,019
831,600
(d) }} 2 }} 1}} 2 }} 5 }} < 0.31026816
This is within 1.5 3 1027 of the answer in (c).
should be invested today in order to completely fund
the perpetuity forever.
66. We again assume that the first payment occurs at the end of
64. (a) Let f (x) 5 x 2e x dx.
Exe
1
0
2 x
dx 5
the year.
E f (x) dx
1
Present value 5 1000(1.06)21 1 1000(1.06)22
0
3
1
e
5 }}30 1 2}} 1 e4
4
4
4
h
2
1 1000(1.06)23 1 …
< }} f (0) 1 2f (0.5) 1 f (1)
0.5
e0.5
8
1000/1.06
1 2 (1/1.06)
The present value is $16,666.67.
e
4
5 }} 1 }}
< 0.88566
1
x2
2!
xn
n!
(b) x 2e x 5 x 2 1 1 x 1 }} 1 … 1 }} 1 …
2
x4
x n 12
5 x 1 x 1 }} 1 … 1 }} 1 …
2!
n!
x4
2
3
P4(x) 5 x 1 x 1 }}
2
1
x3
x4
41
x5 1
P4(x) 5 }} 1 }} 1 }} 5 }} < 0.68333
3
4
60
10 0
0
2
E
3
3
1000
1.06 2 1
5 }} 5 }} < 16,666.67
4
(c) Since f is concave up, the trapezoids used to estimate
the area lie above the curve, and the estimate is too
large.
(d) Since all the derivatives are positive (and x . 0), the
remainder, Rn(x), must be positive. This means that
Pn(x) is smaller than f (x).
400
Section 10.1
`
67. (a)
Sequence of
Tosses
Payoff
($)
Probability
12
1 3
1}2}2
1 4
1}2}2
122
1 2
11}}2
2
1 3
21}}2
2
1 4
31}}2
2
:
:
0
1
}}
2
HT
1
1 2
}}
2
HHT
2
HHHT
3
:
:
T
Term of
Series
70. (a) Note that ∑ x n11 is a geometric series with first term
n51
a 5 x and common ratio r 5 x, which explains the
2
1
0 }}
`
identity ∑ x n11 5 }} (for )x) , 1).
x2
12x
n51
Differentiate.
`
(1 2 x)(2x) 2 (x )(21)
2x 2 x
5 }}2
∑ (n 1 1)x n 5 }}}
(1 2 x)2
(1 2 x)
2
2
n51
Differentiate again.
`
∑ n(n 1 1)x n21
n51
(1 2 x)2(2 2 2x) 2 (2x 2 x 2)(2)(1 2 x)(21)
(1 2 x)
(1 2 x)(2 2 2x) 1 2(2x 2 x 2)
5 }}}}
(1 2 x)3
2
5 }}3
(1 2 x)
Expected payoff
1 2
122 122
1
5 0 }} 1 1 }}
1 3
122
1 2 }}
1 4
122
1 3 }}
5 }}}}}
4
1…
(b) }}2 5 1 1 2x 1 3x 2 1 … 1 nx n21 1 …
1
(1 2 x)
x2
(1 2 x)
(c) }}2 5 x 2(1 1 2x 1 3x 2 1 … 1 nx n21 1 …)
Multiply by x.
`
2x
}
∑ n(n 1 1)x n 5 }
(1 2 x)3
5 x 2 1 2x 3 1 3x4 1 … 1 nx n11 1 …
n51
1
(d)
If x 5 }}, the formula in part (c) matches the
2
nonzero2 terms of the series in part (a). Since
(1/2)
}}2 5 1, the expected payoff is $1.
1
x
Replace x by }}.
`
[1 2 (1/2)]
2
}}
x
n(n 1 1)
2x
}5}
∑}
1 3 5 }}3 , )x) . 1
xn
(x 2 1)
1 2 }}
68. (a) The area of an equilateral triangle whose sides have
1
n51
Ïw3s
1
s2Ïw3
length s is }}(s) }} 5 }}. The sequence of areas
2
2
4
1 2
2
x
2
2x 2
(x 2 1)
(b) Solve x 5 }}3 to get x < 2.769 for x . 1.
removed from the original triangle is
Chapter 10
Vectors
w
b2Ï3w
b 2 Ï3
b 2 Ïw3
}} 1 3 }} }} 1 9 }} }} 1 …
2
4
4
4
4
12
12
b Ïw3
1 3 1}}2 }} 1 … or
2
4
2
n
n
■ Section 10.1 Parametric Functions
w 32b2Ï3w … 3nb2Ï3w …
b2Ï3w
3b2Ï3
1 }}
1
1 }n1
}} 1 }}
}1 .
2
43
4
4
4 1
(pp. 513–520)
b2Ï3w
(b) This is a geometric series with initial term a 5 }}
3
4
2Ïw
4
b 3/4
1 2 (3/4)
and common ratio r 5 }}, so the sum is }} 5
Exploration 1 Investigating Cycloids
1.
b2Ï3w, which is the same as the area of the original
triangle.
[0, 20] by [21, 8]
(c) No, not every point is removed. For example, the
vertices of the original triangle are not removed. But
the remaining points are “isolated” enough that there
are no regions and hence no area remaining.
69. }} 5 1 1 x 1 x 2 1 x 3 1 …
1
12x
Differentiate both sides.
1
}}2 5 1 1 2x 1 3x 2 1 4x 3 1 5x 4 1 …
(1 2 x)
1
Substitute x 5 }} to get the desired result.
2
2. x 5 2nap for any integer n.
3. a . 0 and 1 2 cos t $ 0 so y $ 0.
4. An arch is produced by one complete turn of the wheel.
Thus, they are congruent.
5. The maximum value of y is 2a and occurs when
x 5 (2n 1 1)ap for any integer n.
6. The function represented by the cycloid is periodic with
period 2ap, and each arch represents one period of the
graph. In each arch, the graph is concave down, has an
absolute maximum of 2a at the midpoint, and an absolute
minimum of 0 at the two endpoints.
Section 10.1
dy
dy/dt
2Ï3w sin t
2. (a) }} 5 y9 5 }} 5 }} 5 Ï3w
Quick Review 10.1
1. (cos (0), sin (0)) 5 (1, 0)
dx
3p
3. x 2 1 y 2 5 1 (since cos2 t 1 sin2 t 5 1)
4. The portion in the first three quadrants, moving counterclockwise as t increases.
dy
dx
dy/dt
dx/dt
3 cos t
22 sin t
w/2) 3
3p
3(2Ï2
which at t 5 }} equals }} 5 }}.
4
22(Ï2
w/2) 2
7. }} 5 }} 5 }},
!§§§t§
3
5 2 3 1 }}
3Ïtw1
ww1
3/(2t 2Ï3
ww
1w3/t
w)
d 2y
dy9/dt
(b) }}2 5 }} 5 }} 5 2}}
dx
dx/dt
21/(2Ïtw1
ww1)
t 2Ï3ww
1w
3/t
w
Ï3w
5 2}3/}
2
3
3p
3Ïw2
8. y 5 }}x 1 C. For t 5 }}, x 5 2Ï2w and y 5 }}, so
2
4
3Ï2w
3
w) 1 C and C 5 3Ï2w.
}} 5 }}(2Ï2
2
2
3
Thus, y 5 }}x 1 3Ï2w.
2
2
2
3p
3Ï2w
9. y 5 2}}x 1 C. For t 5 }}, x 5 2Ï2w and y 5 }}, so
3
4
2
3Ï2w
2
5Ïw2
w) 1 C and C 5 }}.
}} 5 2}}(2Ï2
3
2
6
2
5Ï2w
Thus, y 5 2}}x 1 }}.
3
6
t
dy
dx
3
3 1
9
4
8
27
3/2 3
2 4
dy
dx
dy9/dt
dx/dt
[(2t 2 3)(6t) 2 (3t 2)(2)]/(2t 2 3)2
5 }}}}
2t 2 3
12t 2 2 18t 2 6t 2
5 }}
(2t 2 3)3
6t 2 2 18t
5 }}3
(2t 2 3)
d 2y
dx
313/2 2 8
27
d 2y
dx
1
2
1
dy9/dt
dx/dt
2}} sec2 t
1
8
2
(b) }}2 5 }} 5 }}
5 2}} sec3 t
4 cos t
dy/dt
dx/dt
2t 2 1
2t 1 1
dy9/dt
dx/dt
[(2t 1 1)(2) 2 (2t 2 1)(2)]/(2t 1 1)2
5 }}}}
2t 1 1
4
5 }}3
(2t 1 1)
(b) }}2 5 }}
1. (a) }} 5 y9 5 }} 5 }} 5 2}} tan t
d 2y
dx
3t 2
2t 2 3
(b) }}2 5 }}
dy
dx
22 sin t
4 cos t
dy/dt
dx/dt
dy/dt
dx/dt
5. (a) }} 5 y9 5 }} 5 }}
Section 10.1 Exercises
dy
dx
21
21/t
6. (a) }} 5 y9 5 }} 5 }}
5 }}.
0
dy9/dt
dx/dt
d 2y
dx
0
5 }} 1 1 }}x
1/t
21/t
(b) }}2 5 }} 5 }}2 5 t 2
2
0
3
dy/dt
dx/dt
4. (a) }} 5 y9 5 }} 5 }}2 5 2t
10. y9 5 }}Ïxw, so
E !1§§1§1}§32}ϧxw§2§ dx
9
5 E 1 1 }}x dx
!§§§4§
dy/dt
dx/dt
3/(2Ï3
wtw)
5 }}
21/(2Ïtw1
ww1)
3Ïtw1
ww1
5 2}
Ï3wtw
6. The graph is a circle with radius 2 centered at (2, 3).
Modify the x 5 cos t, y 5 sin t parameterization
correspondingly:
x 5 2 cos t 1 2, y 5 2 sin t 1 3, 0 # t # 2p.
Length 5
0
2sin t
3. (a) }} 5 y9 5 }}
5. x 5 t, y 5 t 2 1 1, 21 # t # 3
3
2
dy9/dt
dx/dt
(b) }}2 5 }} 5 }} 5 0
2. cos }} , sin }}
dy
dx
2sin t
dx/dt
d 2y
dx
1 1 2 2 1 2 22 5 (0, 21)
3p
401
dy
dx
dy/dt
dx/dt
cos t
2sin t
7. }} 5 }} 5 }} 5 2cot t
p
2
(a) 2cot 5 0 when t 5 }} 1 kp (k any integer). Then
1
12
p
2
12
p
22
(x, y) 5 2 1 cos }} 1 kp , 21 1 sin }} 1 kp
5 (2, 21 6 1). The points are (2, 0) and (2, 22).
(b) 2cot is undefined when t 5 kp (k any integer). Then
(x, y) 5 (2 1 cos (kp), 21 1 sin (kp)) 5 (2 6 1, 21).
The points are (1, 21) and (3, 21).
402
dy
dx
Section 10.1
sec2 t
sec t tan t
dy/dt
dx/dt
13. x9 5 t 2, y9 5 t, so
8. }} 5 }} 5 }} 5 csc t
E Ï(tww)w1wwt w dt
t w
1w
1 dt
5 E tÏw
(b) csc t is undefined when t 5 kp (k any integer). Then
(x, y) 5 (sec (kp), tan (kp)) 5 (61, 0).
The points are (1, 0) and (21, 0).
dy
dx
2
2
33
1
5 }}(t 2 1 1)3/2
3t 2 4
21
9. }} 5 }} 5 }} 5 4 2 3t 2
1
4
0
1
5 }}(23/2 2 1)
3
!§
4
w21
2Ï2
5 }} < 0.609
2
(a) 4 2 3t 2 5 0 when t 5 6 }} 5 6}}.
3
Ïw3
3
3
1
1 2 1 22
2
8
8
5 12 7 }}, 6}} 7 }}2,
Ï3w
3Ï3w
Ï3w
2
2 2
0
1
0
2
dy/dt
dx/dt
1
Length 5
(a) Nowhere, since csc t never equals zero.
2
Then (x, y)5 2 7 }}, 6 }}
Ïw3
Ïw3
2
7 4 }}
Ï3w
14. x9 5 8t cos t, y9 5 8t sin t, so
E Ï(8wtwcowswt)ww1ww(8wtwsiwnwwtw) dt
5 E 8t dt
5 4t
3 4 5p
p/2
Length 5
which evaluates to < (0.845, 23.079) and
< (3.155, 3.079).
0
(b) Nowhere, since 4 2 3t 2 is never undefined.
2
2
0
p/2
2
p/2
2
0
dy
dx
dy/dt
dx/dt
sec t tan t 1 sec2 t
sec t 1 tan t
3 cos t
23 sin t
10. }} 5 }} 5 }} 5 2cot t
15. x9 5 }} 2 cos t 5 sec t 2 cos t,
y9 5 2sin t, so
p
2
(a) 2cot t 5 0 when t 5 }} 1 kp (k any integer).
Then (x, y)
1
1
2
p
2
E Ï(swecwwtw2wcowswt)ww1ww(2wsiwnwwtw) dt
5 E Ïse
ww
cw
t2
ww1 dt
5 E tan t dt
5 ln )sec t)
3
4 5 ln 2
1
p
2
22
5 22 1 3 cos }} 1 kp , 1 1 3 sin }} 1 kp
(b) 2cot t is undefined when t 5 kp (k any integer). Then
(x, y)5 (22 1 3 cos (kp), 1 1 3 sin (kp))
5 (22 6 3, 1). The points are (1, 1) and (25, 1).
E Ï(2
wsi
wnwwtw
)w
1w(1ww
1wcowswt)
ww dt
5 E Ï2w(1
ww
1wcowswt)
w dt
t
5E
!4§§co§s§§1}§2}2§ dt
t
5 E 2 cos }} dt
122
t
5 2 2 sin }}
3 1 2 24 5 4
2
2
0
p
0
p
2
0
p
0
p
0
E Ïw
(Ï2wtw1
ww3w
)w
1w(1ww
1wtw
) dt
1
21
5 E (t 1 2) dt 5 }}t 1 2t 5 }}
32 4 2
Length 5
0
3
0
2
2
2
2
0
p/3
0
16. x9 5 et 2 2t, y9 5 1 2 e2t, so
E
2
Length 5
Ï(e
wtw
2w2t)
w2w1
ww(1ww
2we2
wtw)2w dt ,
21
17. x9 5 2sin t, y9 5 cos t, so
Area 5
E
2p
2p(2 1 sin t)Ï(2
wsi
wnwwtw
)2w
1wcoww
s2wt dt
E (2 1 sin t) dt
5 2p 2t 2 cos t
3
4 5 8p
0
2p
5 2p
0
2p
2
0
1
18. x9 5 Ïtw, y9 5 }}, so
Ïtw
E 2p1}23}t 2!(§Ïtw§)§1§§1}§Ï1}§tw 2§ dt
4p
t w
1w1 dt
5 }}E tÏw
3
Area 5
12. x9 5 Ï2wtw1
ww3, y9 5 1 1 t, so
3
2
which using NINT evaluates to < 4.497.
11. x9 5 2sin t, y9 5 1 1 cos t, so
p
2
0
p/3
0
p/3
5 (22, 1 6 3). The points are (22, 4) and (22, 22).
length 5
p/3
Length 5
2
3/2
2
2
0
2
2
0
3
4p 1
3 3
2
4
3
5 }} }}(t 2 1 1)3/2
0
4p(5Ïw5 2 1)
5 }} < 14.214
9
0
19. x9 5 1, y9 5 2t, so
Area 5
E 2p(t 1 1)Ï1ww1w(2wt)ww dt,
3
2
0
which using NINT evaluates to < 178.561.
Section 10.1
20. x9 5 sec t 2 cos t (see Ex. 15), y9 5 2sin t, so
E
5E
Length 5
p/3
0
p/3
2p(cos t)Ï(s
wec
wwtw
2wcowswt)
w2w1
ww(2
wsi
wnwwtw
)2 dx
dx
dx
becomes }} 5 1.
2p cos t Ïta
wnw2wtw dt
p/3
5 2p
dx
dt
25. In the first integral, replace t with x. Then }}
E sin t dt
5 2p 2cos t
3 4 5 p.
0
0
26. Parameterize the curve as x 5 g(y), y 5 y, c # y # d. The
p/3
parameter is y itself, so replace t with y in the general
dy
dt
(b) x9 5 2, y9 5 1, so
ww1, so
27. x9 5 t, y9 5 Ï2wtw1
E 2p(t 1 1)Ï2ww1ww1w dt
5 2pÏ5wE (t 1 1) dt
1
5 2pÏ5w }}t 1 t
32 4
Area 5
2
0
E Ïwt w1w(Ïw2wtw1ww1w) dt
5 E (t 1 1) dt
2
1
2
4
Total length 5
1
0
dy
dy
formula. Then }} becomes }} 5 1.
0
21. (a) x(t) 5 2t, y(t) 5 t 1 1, 0 # t # 1
1
403
2
2
0
4
0
32
1
0
5 }}t 2 1 t
5 3pÏ5w
32
0
4
1
Now solve }}t 2 1 t
(c) Slant height 5 Ï2w2w1
ww12w 5 Ï5w, so
Area 5 p(1 1 2)Ï5w 5 3pÏ5w
4
4 5 12.
m
12
2
5 }} for m:
0
1
}}m 2 1 m 5 6, or m2 1 2m 2 12 5 0, and
2
22 6 Ïw
4w
1w48
w
m 5 }} 5 21 6 Ï1w3w. Take the positive
2
r
h
22. (a) Because these values for x(t) and y(t) satisfy y 5 }}x,
which is the equation of the line through the origin and
solution. The midpoint is at t 5 Ï1w3w 2 1, which gives
(h, r), and this range of t-values gives the correct initial
(Ïw
1w
3 2 1)2 1
(x, y) 5 }}, }}(2Ï1w3w 2 1)3/2 < (3.394, 5.160).
and terminal points.
1
2
2
3
28.
(b) x9 5 h, y9 5 r, so
E 2p(rt)Ïhww1wwrw dt
5 prÏhww1
wwr w3t 4
1
Area 5
2
2
0
2
2
2
[24, 4] by [0, 10]
1
Use the right half of the curve, 0 # t # p.
0
5 pr Ïw
r 2w
1wh2w.
x9 5 3 cos t, y9 5 6 cos 2t, so
Area 5
(c) Slant height 5 Ïw
r 2w
1wh2w, so Area 5 prÏw
r 2w
1wh2w
E
5E
p/2
0
p/2
0
(Ï2
w2wwsin
ww2t)
w2w1
ww(2wwcowsw2wt)
w2w dt
E
5E
Length 5
[0, 9] by [23, 3]
p dt 5 p.
symmetry.
2p
0
29.
Use the top half of the curve, and make use of the shape’s
24. x9 5 23 sin t, y9 5 4 cos t, so
E
2
Ï(p
wwcowswp
wt)
w2w1
ww(2
wp
wwsin
ww
pt)
w2w dt
21/2
1/2
21/2
Length 5
2
0
2 dt 5 p.
(b) x9 5 p cos pt, y9 5 2p sin pt, so
1/2
p
which using NINT evaluates to < 159.485.
23. (a) x9 5 22 sin 2t, y9 5 2 cos 2t, so
Length 5
E 2p(3 sin t)Ï(3wwcowswt)ww1ww(6wwcowsw2wt)ww dt,
Ï(2
w3wwsin
wwtw
)2w
1w(4wwcowswt)
w2w dt
which using NINT evaluates to < 22.103.
x9 5 3 cos t, y9 5 6 cos 2t, so
E
Area 5 2
p/2
0
2p(3 sin 2t)Ï(3
wwcowswt)
w2w1
ww(6wwcowsw2wt)
w2w dt
which using NINT, evaluates to < 144.513.
404
Section 10.1
(b) x9 5 t cos t, y9 5 t sin t, so
30. y 5 0 for t 5 0 and t 5 2p. x9 5 a 2 a cos t, y9 5 a sin t,
Length 5
so
E 2p[a(1 2 cos t)]Ï(aww2wawcowswt)ww1ww(awwsinwwtw) dt
2w2wcowswtw dt
5 2pa E (1 2 cos t)Ï2ww
t
t
5 2pa E 12 sin 1}}22 4 sin 1}}2 dt
2 !§§§§§§
2§
t
5 8pa E sin }} dt
122
t
t
5 8pa E 11 2 cos 1}}22 sin 1}}2 dt
2
2
2p
Area 5
2
0
2p
2
2
0
2p
2
2
3
2
0
3
12
t
2
2p
t
2
64pa
3
v sin u
0
y 5 0 for t 5 0 or t 5 }
}. The maximum height is attained
16
v sin u
0
in mid-flight at t 5 }
}. To find the path length, evaluate
32
Ï(v
ww
wswuww
co
)w
1w(w
v0wsin
wwuw
2w
32wt)
w2w dt using NINT. To
0
2
find the
maximum height, calculate
dx
dt
31. }} 5 a(1 2 cos t)
(Note: integrate with respect to x from 0 to 2ap; integrate
E
5E
y dx
5a
2
2p
2
3
Length 5
2p
4
1
4
t
2
5 a2 t 2 2 sin t 1 }} 1 }}sin 2t
E
E
(75 sin 208)/8
Ï(1
w5w0wwcowsw2w0w8)
w2w1
ww(1w5w0wwsin
ww20w8w2
ww32wt)
w2w
0
dt which, using NINT, evaluates to < 461.749 ft
5 3pa2
y9 5 0,
p[a(1 2 cos t)] a(1 2 cos t) dt
2
E (1 2 3 cos t 1 3 cos t 2 cos
3
3
5 pa t 2 3 sin t 1 }}t 1 }}sin 2t
3
2
4
1
21sin t 2 }} sin t2
4
3
5 pa3
2
32
(b) The maximum height of the projectile occurs when
2p
0
v sin u 2
0
dx
32. }} 5 a(1 2 cos t), so
dt
Volume 5
1
x9 5 150 cos 208, y9 5 150 sin 208 2 32t
(1 2 2 cos t 1 cos t) dt
0
2
75
8
a(1 2 cos t)a(1 2 cos t) dt
E
32
t 5 0 or t 5 }} sin 208 < 3.206
2ap
0
v sin u
y 5 t(150 sin 208 2 16t) 5 0
2ap
0
1
0
0
ymax 5 (v0 sin u) }
} 2 16 }
} .
35. (a) The projectile hits the ground when y 5 0.
with respect to t from 0 to 2p.)
Area 5
t dt
0
For exercises 35–38, x9 5 v0 cos u and y9 5 v0 sin u 2 32t, and
0
5 }}
2p
(a) x 5 a(cos t 1 t sin t), y 5 a(sin t 2 t cos t)
v sin u/16
0
0
2
0
E
(b) Length 5 2ap 2
E
1 24
2
3
5 8pa 2 22 cos }} 1 }} cos3 }}
Ï(t
wwcowswt)
w2w1
ww(twsi
wnwwtw
)2 dt 5
34. All distances are a times as big as before.
2
0
2p
2p
5 2p 2
2
0
2p
2
E
2p
2
3
t) dt
0
3
3
1 16
75
16
2
75
so t 5 }} sin 208, y }} sin 208 < 41.125 ft
2p
0
5 5p 2a3
36. (a) < 641.236 ft
5625
64
(b) }} < 87.891 ft
37. (a) < 840.421 ft
16,875
64
(b) }} < 263.672 ft
33. (a) Q
wP
w has length t, so P can be obtained by starting at Q
and moving t sin t units right and t cos t units
downward.
(If either quantity is negative, the corresponding
direction is reversed.) Since Q 5 (cos t, sin t), the
coordinates of P are
x 5 cos t 1 t sin t and y 5 sin t 2 t cos t.
38. (a) It is not necessary to use NINT.
Length 5
E
75/8
0
3
(150 2 32t) dt 5 150t 2 16t 2
5625
5 }} 5 703.125 ft
8
75/8
4
0
5625
16
(b) }} 5 351.5625
y
E 2py!§1}d§d}x§t 2§1§§1}§dd}y§t 2§ dt, replace t with x
b
Q
39. In the integral
t sin t
t
t
t
t cos t
P(x, y)
(1, 0)
x
2
a
and y with f (x).
dx
dt
dx
dx
Then }} becomes }} 5 1.
2
Section 10.2
dy
dx
40. }} 5 e x, so Area 5
E 2pe Ï1ww1w(eww)w dx which using
3
x
x 2
0
NINT evaluates to < 1273.371.
dy
dx
1
x
41. }} 5 2}}2 , so Area 5
E 2p1}1x}2!1§§1§12§}§x}§2§ dx, which,
4
1
1 2
2
using NINT, evaluates to < 9.417.
405
5. (a) 2u 5 k2(3), 2(22)l 5 k6, 24l
3v 5 k3(22), 3(5)l 5 k26, 15l
2u 2 3v 5 k6 2 (26), 24 2 15l 5 k12, 219l
(b) Ï1w2w2w1
ww(2
w1w9ww
)2 5 Ï5w0w5w
6. (a) 22u 5 k22(3), 22(22)l 5 k26, 4l
5v 5 k5(22), 5(5)l 5 k210, 25l
22u 1 5v 5 k26 1 (210), 4 1 25l 5 k216, 29l
(b) Ï(2
w1w6ww
)2w
1w29w2w 5 Ï1w0w9w7w
dy
dx
42. }} 5 (ln 2)2 x 2 (ln 2)22x 5 (ln 2)(2 x 2 22x), so
Area 5
E
2
22
2p(2 x 1 22x)Ï1ww
1w(ln
ww2w
)2(2
wxw2
ww22
wxw)2w dx which
322
521
l k l
l k l
3
5
9
5
6
5
k
1 2
l k l
3
4
9
8
6
1 14
}}u 1 }}v 5 }} 1 2}} , 2}} 1 4 5 }}, }}
5
5
5
5
5
5 5
■ Section 10.2 Vectors in the Plane
Quick Review 10.2
1. Ï(5
ww
2w1w
)2w
1w(3ww
2w2w
)2 5 Ï1w7w
3
5
4
4
4
8
}}v 5 }}(22), }}(5) 5 2}}, 4
5
5
5
5
using NINT evaluates to < 116.687.
(pp. 520–529)
k
k
3
5
7. (a) }}u 5 }}(3), }}(22) 5 }}, 2}}
(b)
14 2
Ïw1w9w7
5
13
5
13
!§1}§5}§2 §1§1}§5}§§2 5 }5}
1 2
5
13
k
l k
15 10
13 13
1
4
k
l k
l
12
12
12
24 60
}}v 5 }}(22), }}(5) 5 2}}, }}
13
13
13
13 13
2. }} 5 }}
320
320
120
52a
521
22b
5. Slope of w
AB
w = Slope of C
ww
D, so }} 5 }} 5 and b 5 6.
321
628
6. (a) u 5 1208
2p
3
(b) u 5 }}
7. (a) u 5 2308
p
6
(b) u 5 2}}
8. (a) u 5 2458
p
4
(b) u 5 2}}
9. c2 5 32 1 52 2 2(3)(5) cos (308) 5 34 2 15Ï3w, so
w4ww
2w15wÏ
w3w < 2.832
c 5 Ï3
10. 242 5 272 1 192 2 2(27)(19) cos u, so
242 2 272 2 192
257
22(27)(19)
513
21 257
u 5 cos }} < 1.046 radians or 59.9358.
513
cos u 5 }} 5 }} and
Section 10.2 Exercises
1. (a) k3(3), 3(22)l = k9, 26l
ww(2
w6ww
)2 5 Ï1w1w7w 5 3Ï1w3w
(b) Ï9w2w1
2. (a) k22(22), 22(5)l 5 k4, 210l
ww(2
w1w0ww
) 2 5 Ï1w1w6w 5 2Ï2w9w
(b) Ï4w2w1
3. (a) k3 1 (22), 22 1 5l 5 k1, 3l
ww32w 5 Ï1w0w
(b) Ï1w2w1
4. (a) k3 2 (22), 22 2 5l 5 k5, 27l
ww(2
w7ww
)2 5 Ï7w4w
(b) Ï5w2w1
k
12
13
5
13
32b
523
1 13 2 13
15
13
24
10
60
13
l k
70
13
2}}u 1 }}v 5 2}} 1 2}} , }} 1 }} 5 23, }}
3. Solve }} 5 24: b 5 11.
4. Slope of w
AB
w = Slope of C
wD
w, so }} 5 }} and a 5 4.
l
8. (a) 2}}u 5 2}}(3), 2}}(22) 5 2}}, }}
(b)
Ï6w4w2w1w
!(2
§3§)§§1§1}§1}§3 §2 5 }1}
3
70 2
2
9. k2 2 1, 21 2 3l 5 k1, 24l
k
2 1 (24)
2
l
21 1 3
2
10. }} 2 0, }} 20 5 k21, 1l
11. k0 2 2, 0 2 3l 5 k22, 23l
12. E
AB 5 k2 2 1, 0 2 (21)l 5 k1, 1l
C
E
D 5 k22 2 (21), 2 2 3l 5 k21, 21l
A
E
B 1C
E
D 5 k1 1 (21), 1 1 (21)l 5 k0, 0l
k
k
l k
l
2l k
2p
2p
1 Ïw3
13. cos }}, sin }} 5 2}}, }}
3
1
3
3p
4
2 1
2
3p
4
14. cos 2}} , sin 2}}
2
1
1
l
5 2}}, 2}}
Ï2w Ï2w
15. This is the unit vector which makes an angle of
120 1 90 5 2108 with the positive x-axis;
k
k
l
l
Ïw3 1
kcos 2108, sin 2108l 5 2}}, 2}}
2
2
1
1
16. kcos 1358, sin 1358L 5 2}}, }}
Ï2w Ïw2
l
406
Section 10.2
17. The vector v is horizontal and 1 in. long. The vectors u and
11
w are }} in. long. w is vertical and u makes a 458 angle
16
with the horizontal. All vectors must be drawn to scale.
(a)
(d)
w
v
v
u
u+v
u
u+v+w=0
(b)
u+v+w
k l
k
1
5
3 4
5 5
ww42w 5 5; }} k3, 4l 5 }}, }}
19. Ï3w2w1
w
1
5
4
5
3
5
l
20. Ï4w2w1
ww(2
w3ww
)2 5 5; }}k4, 23l 5 }}, 2}}
v
u
k
1
17
15 8
17 17
l
21. Ï(2
w1w5ww
)2w
1w82w 5 17; }}k215, 8l 5 2}}, }}
(c)
–v
22. Ï(2
w5ww
)2w
1w(2
w2ww
)2 5 Ï2w9w;
k
u
l
1
5
2
}}k25, 22l 5 2}}, 2}}
Ï2w9w
Ï2w9w Ï2w9w
u–v
(d)
1
1
1
23. x9 5 }}, y9 5 1 1 }}; for t 5 1, x9 5 }}, y9 5 2, and
2
2Ïwt
Ïtw
Ï1w7w
2
2
Ïw
(xw
9)ww
1w(w
y9w
) 5 }}.
u
–w
2
u–w
18. The angles between the vectors is 1208 and vector u is
horizontal. They are all 1 in. long. Draw to scale.
(a)
u
k l k
k l k
l
2 1
1
4
Tangent: 6}} }}, 2 5 6 }}, }} ,
Ï1ww7 2
Ïw17w Ïw17w
2
1
4
1
Normal: 6}} 2, 2}} 5 6 }}, 2}} .
2
Ï1ww7
Ïw17w
Ï1w7w
l
1
2
1
t21
24. x9 5 }}, y9 5 1; for t 5 3, x9 5 }}, y9 5 1, and
–v
u–v
Ïw
5
Ï(x
w9)
w2w1
ww(y9
ww
)2 5 }}.
2
2
(b)
k l k l
k l k
l
1
1
2
Tangent: 6}} }}, 1 5 6 }}, }} ,
Ïw5 2
Ïw5 Ï5w
u
2
1
2
1
Normal 5 6}} 1, 2}} 5 6 }}, 2}} .
2
Ïw5
Ïw5 Ï5w
–v
p
3
25. x9 5 24 sin t, y9 5 5 cos t; for t 5 }}, x9 5 22Ï3w,
u–v+w
Ï7w3w
5
y9 5 }}, and Ï(x
w9)
w2w1
ww(y9
ww
)2 5 }}.
2
2
w
2
k
5
l k
12
5
l
Tangent 5 6}} 22Ï3w, }} 5 6 2}}, }}
2
Ï7w3w
Ï2w1w9w Ï7w3w
(c)
< 6k20.811, 0.585l,
2u
2
–v
2u – v
k
5
l k
5
12
Normal 5 6}} }}, 2Ï3w 5 6 }}, }}
Ï7w3w 2
Ï7w3w Ï2w1w9w
< 6k0.585, 0.811l.
l
Section 10.2
p
3
26. x9 5 23 sin t, y9 5 3 cos t; for t 5 2}}, x9 5 }},
4
Ï2w
3
y9 5 }}, and Ï(x
w9)
w2w1
ww(y9
ww
)2 5 3.
Ï2w
k
k
l k
l k
l
32. Since u and v are nonzero, we know that )u) ≠ 0 and )v) ≠ 0.
Therefore, the dot product u ? v 5 )u) )v) cos u is 0 if and
only if cos u 5 0, which occurs if and only if u and v are
p
orthogonal u 5 }} .
1
33.
1 3
3
1
1
Tangent: 6}} }}, }} 5 6 }}, }} ,
3 Ïw2 Ï2
w
Ïw2 Ïw2
407
2
2
(r1, r2)
l
1 3
3
1
1
Normal: 6}} }}, 2}} 5 6 }}, 2}} .
3 Ïw2
Ïw2
Ï2w
Ï2w
v
(u1, u2)
u
27. A
E
B 5 k3, 1l, BC
E 5 k21, 23l, and A
E
C 5 k2, 22l.
u+v
u
(v1, v2)
v
B
E
A 5 k23, 21l, CB
E 5 k1, 3l, and CA
E 5 k22, 2l.
)A
E
B ) 5 ) BA)
E 5 Ï1w0w, ) BC)
E 5 )CB)
E 5 Ï1w0w, and
) AC)
E 5 )CA)
E 5 2Ï2w.
r1 2 v1 5 u1 so r1 5 u1 1 v1
r2 2 v2 5 u2 so r2 5 u2 1 v2
AE
B ? AE
C
1 ) AEB ))AEC ) 2
Angle at A 5 cos21 }}
1
3(2) 1 1(22)
}}
5 cos21 (Ï1w0w)(2Ï2w)
34. (a) To find u 2 v, place both vectors with their initial
points at the origin. The vector drawn from the terminal
point of v to the terminal point of u is u 2 v. Or, add u
and 2v according to the parallelogram law.
2
(b)
1 2
1
5 cos21 }} < 63.4358,
Ï5w
?
Angle at B 5 cos21 }
BC
E E
BA
1 )BC
E ))E
BA ) 2
5
1
(u1, u2)
(21)(23) 1 (23)(21)
cos21 }}}
(Ï1
w0w)(Ï1w0w)
2
u
152
3
5 cos21 }} < 53.1308, and
CB
E ? CA
E
Angle at C 5 cos21 }
) CB))
E CA)
E
1
1
1(22) 1 3(2)
(–v1, –v2)
2
1 2
1
28. A
E
C 5 k2, 4L and B
E
D 5 k4, 22L.
E 5 2(4) 1 4(22) 5 0, so the angle measures 908.
AC
E ? BD
29. (a) u ? (v 1 w) 5 u1(v1 1 w1) 1 u2(v2 1 w2)
5 (u1v1 1 u1w1) 1 (u2v2 1 u2w2)
5 (u1v1 1 u2v2) 1 (u1w1 1 u2w2)
5u?v1u?w
(b) (u 1 v) ? w 5 (u1 1 v1)w1 1 (u2 1 v2)w2
5 (u1w1 1 v1w1) 1 (u2w2 1 v2w2)
5 (u1w1 1 u2w2) 1 (v1w1 1 v2w2)
5u?w1v?w
2
2 2
w
1wuw
) 5 )u)2
30. u ? u 5 u12 1 u22 5 (Ïuww
1
2
31. (u 1 v) ? (u 2 v)
5 (u1 1 v1)(u1 2 v1) 1 (u2 1 v2)(u2 2 v2)
5 (u12 1 u22) 2 (v12 1 v22)
5 )u)2 2 )v)2
(r1, r2)
u
–v
5 cos21 }} < 63.4358.
Ïw5
5 u12 2 v12 1 u22 2 v22
u–v
v
2
5 cos21 }}
(Ï1
w0w)(2Ï2w)
–v
u–v
r1 2 (2v1) 5 u1 → r1 5 u1 2 v1
r2 2 (2v2) 5 u2 → r2 5 u2 2 v2
35. (a) Let P 5 (a, b) and Q 5 (c, d). Then
1}2}2 OEP 1 1}2}2OEQ 5 1}2}2ka, bl 1 1}2}2kc, dl
1
1
k
1
(a 1 c) (b 1 d)
2
2
l
5 }}, }} 5 O
E
M
132
2
132
132
132
1
(b) O
E
M 5 }} O
E
P 1 }} O
E
Q
1
2
(c) O
E
M 5 }} O
E
P 1 }} O
E
Q
1
408
Section 10.2
40. The indicated diagonal is (u 1 v). The cosine of the angle
35. continued
(d) M is a fraction of the way from P to Q. Let d be this
fraction. Then
OM
E 5 d OQ
E 1 (1 2 d)OP.
E
Proof: PM
E 5 dPQ
E and MQ
E 5 (1 2 d)PQ,
E
1
1
so PQ
E 5 }}PM
E and PQ
E 5 }} MQ.
E
12d
d
1
d
1
12d
Therefore, }} PM5
E }} MQ.
E
But P
E
M 5 OM
E 2 OP
E and MQ
E 5 OQ
E 2O
E
M, so
1
1
1
1
E 2 }}OP
E 5 }} OQ
E 2 }} OM.
E
}}OM
d
d
12d
12d
Therefore,
1
1
1
1
E 1 }} OM
E 5 }} O
E
P 1 }} OQ.
E
}}OM
d
d
12d
12d
1
1
1
⇒O
E
M }} 5 }} E
OP 1 }} OQ
E
d
d(1 2 d)
12d
1
2
⇒O
E
M 5 (1 2 d) O
E
P 1 dOQ.
E
36. CA
E 5 2u 2 v and CB
E 5 u 2 v. Since
)v) 5 )u), these vectors are orthogonal, as
(2u 2 v) ? (u 2 v) 5 )v)2 2 )u)2 5 0.
37. Two adjacent sides of the rhombus can be given by two
vectors of the same length, u and v.
Then the diagonals of the rhombus are (u 1 v) and (u 2 v).
These two vectors are orthogonal since )u) 5 )v) so
(u 1 v) (u 2 v) 5 )u)2 2 )v)2 5 0.
?
38. Two adjacent sides of a rectangle can be given by two vectors u and v. The diagonals are then
(u 1 v) and (u 2 v). These two vectors will be orthogonal
if and only if u and v are the same length, since
(u 1 v) (u 2 v) 5 )u)2 2 )v)2.
?
39. Let two adjacent sides of the parallelogram be given by two
vectors u and v. The diagonals are then (u 1 v) and
(u 2 v). So the lengths of the diagonals satisfy
)u 1 v)2 5 (u 1 v) (u 1 v)
5 )u)2 1 2u v 1 )v)2
2
and )u 2 v) 5 (u 2 v) (u 2 v)
5 )u)2 2 2u v 1 )v)2.
The two lengths will be the same if and only if
u v 5 0, which means that u and v are perpendicular and
the parallelogram is a rectangle.
?
?
?
?
?
between the diagonal and u is
(u 1 v) ? u
)u)2 1 v ? u
}} 5 }}.
)u 1 v) )u)
)u 1 v) )u)
But the cosine of the angle between the diagonal and v is
(u 1 v) ? v
u ? v 1 )v)2
}} 5 }}.
)u 1 v) )v)
)u 1 v) )v)
If u and v are the same length then these two quantities are
equal, and the diagonal makes the same angle with both
sides.
41. The slopes are the same.
42. v 5 0 since any other vector has positive magnitude.
43. 258 west of north is 90 1 25 5 1158 north of east.
800kcos 1158, sin 1158l < k2338.095, 725.046l
44. 108 east of south is 270 1 10 5 2808 “north” of east.
600kcos 2808, sin 2808l < k104.189, 2590.885l
45. Initial velocity is 708 north of east:
325kcos 708, sin 708l < k111.157, 305.400l.
Wind velocity is 1308 north of east:
40kcos 1308, sin 1308l < k225.712, 30.642l.
Add the two vectors to get < k85.445, 336.042l.
The speed is the magnitude, < 346.735 mph.
1 85.445 2
336.042
The direction is tan21 }} < 75.7348 north of east, or
< 14.2668 east of north.
2.5 lb
cos 188
46. )w)cos (338 2 158) 5 2.5 lb, so )w) 5 }}.
2.5 lb
cos 188
Then w < }}kcos 338, sin 338l < k2.205, 1.432l.
47. Juana’s pull 5 23kcos 188, sin 188l < k21.874, 7.107l;
Diego’s pull 5 18kcos (2158), sin (2158)l
< k17.387, 24.659l. Add to get the combined pull of the
children: < k39.261, 2.449l. The puppy pulls with an
opposite force of the same magnitude:
Ïw3w9w
.2w6w12ww
1w2w
.4w4w92w < 39.337 lb.
48. (a) 7kcos 458, sin 458l has its terminal point at
<(4.950, 4.950).
(b) 7kcos 458, sin 458l 1 8kcos 2108, sin 2108l has its
terminal point at <(21.978, 0.950).
49. A
E
B 5 k23 20, 4 2 0l 5 k23, 4l 5 k1 2 4, 5 2 1l 5 C
E
D
50. AB
E 5 k22 2 (24), 22 2 3l
5 k2, 25l
5 k3 2 1, 24 2 1l 5 C
E
D
Section 10.3
51. u 5 ku1, u2l, v 5 kv1, v2l, w 5 kw1, w2l
(i) u 1 v 5 ku1 1 v1, u2 1 v2l
5 kv1 1 u1, v2 1 u2l 5 v 1 u
(ii) (u 1 v) 1 w
5 ku1 1 v1, u2 1 v2l 1 kw1, w2l
5 k(u1 1 v1) 1 w1, (u2 1 v2) 1 w2l
5 ku1 1 (v1 1 w1), u2 1 (v2 1 w2)l
5 u 1 (v 1 w)
(iii) u 1 0 5 ku1, u2l 1 k0, 0l 5 ku1 1 0, u2 1 0l
5 ku1, u2l 5 u
(iv) u 1 (2u) 5 ku1, u2l 1 k2u1, 2u2l
5 ku1 2 u1, u2 2 u2l 5 k0, 0l 5 0
(v) 0u 5 0ku1, u2l 5 k0u1, 0u2l 5 k0, 0l 5 0
(vi) 1u 5 1ku1, u2l 5 k1u1, 1u2l 5 ku1, u2l 5 u
(vii) a(bu) 5 a(b ku1, u2l) 5 akbu1, bu2l
5 kabu1, abu2l 5 abku1, u2l 5 (ab)u
(viii) a(u 1 v) 5 aku1 1 v1, u2 1 v2l
5 kau1 1 av1, au2 1 av2l
5 kau1, au2l 1 kav1, av2l
5 aku1, u2l 1 akv1, v2l
5 au 1 av
(ix) (a 1 b)u 5 (a 1 b)ku1, u2l
5 k(a 1 b)u1, (a 1 b)u2l
5 kau1 1 bu1, au2 1 bu2l
5 kau1, au2l 1 kbu1, bu2l 5 au 1 bu
52. Write the two vectors as ak1, 1l and bk1, 21l. Then their
dy
dx
dy/dt
dx/dt
5 cos t
24 sin t
dy
dx
dy/dt
dx/dt
5 cos t
24 sin t
p
2
3. }} 5 }} 5 }}, which for t 5 }} equals zero.
4. }} 5 }} 5 }}, which for t 5 p is undefined:
the tangent line is vertical.
dy
dy/dt
p
5Ï3w
5 cos t
5. }} 5 }} 5 }}, which for t 5 }} equals 2}}.
6
24 sin t
p
5
6
2
5
5Ïw3
tangent line is y 2 }} 5 2}}(x 2 2Ï3w), or
2
4
5Ï3w
y 5 2}} x 1 10.
4
dx
dx/dt
4
Also, at t 5 }}, x 5 2Ï3w and y 5 }}. The equation for the
1
2
dy
dy/dt
p
5Ï3w
5 cos t
6. }} 5 }} 5 }}, which for t 5 }} equals 2}}.
6
24 sin t
p
5
6
2
5
4
normal line is y 2 }} 5 }}(x 2 2Ï3w), or
2
5Ï3w
4Ïw3
9
y 5 }} x 1 }}.
15
10
dx
dx/dt
4
Also, at t 5 }}, x 5 2Ï3w and y 5 }}. The equation for the
1 2
x22
x22
1
4
1
7. lim }
2 } 5 lim }} 5 lim }} 5 }}
x→2 x 2 4
x→2 (x 1 2)(x 2 2)
8. y9 5 3 2 2x, and Length 5
x→2 x 1 2
E Ï1ww1w(3ww2w2x)ww dx, which
2
2
0
using NINT evaluates to < 3.400.
sum is ka 1 b, a 2 bl, so solve a 1 b 5 3, a 2 b 5 4 to get
7
2
k l k
1
2
7 7
2 2
1 1
2 2
l
a 5 }}, b 5 2}}. So k3, 4l 5 }}, }} 1 2}}, }} .
1
53. (a) Slope 5 2}} 5 21, so y 2 y1 5 m(x 2 x1) becomes
1
y 2 1 5 2(x 1 2) or y 5 2x 2 1.
(b) Slope 5 1, so y 2 y1 5 m(x 2 x1) becomes
y 2 1 5 x 1 2 or y 5 x 1 3.
3
4
54. The slopes of the lines are }} and 1, which means that
vectors k4, 3l and k1, 1l are parallel to the respective lines.
21
u 5 cos
w
4?113?1
7Ï2
}} 5 cos21 }} < 8.1308.
10
5Ï2w
1
2
1 2
■ Section 10.3 Vector-valued Functions
(pp. 529–539)
x
1. f9(x) 5 2}}, so for x 5 1, f (x) 5 Ï3w and
2wx 2w
Ï4ww
1
1
f9(x) 5 2}}. Then y 2 Ïw3 5 2}}(x 2 1) or
Ï3w
Ï3w
1
4
y 5 2}} x 1 }}.
Ï3w
Ïw3
1
9. x9 5 t cos t 1 sin t, and y9 5 2t sin t 1 cos t, and
E Ï(twwcowswtw1wwsinwwtw) w1w(2wtwsiwnwwtw1wcowswt)ww dt
5 E Ïw
t w
1w
1 dt,
Length 5
2
0
2
2
2
0
which using NINT evaluates to < 2.958.
10. y 5 xe x 2 e x 1 C (use integration by parts), so
2 5 0 2 e0 1 C and C 5 3:
y 5 xe x 2 e x 1 3
Section 10.3 Exercises
1. [5 2 (21)]i 1 (1 2 4)j 5 6i 2 3j
2. (0 2 3)i 1 [0 2 (24)]j 5 23i 1 4j
3. A
E
B 5 [0 2 (23)]i 1 (2 2 0)j 5 3i 1 2j and
C
E
D 5 (0 2 4)i 1 (23 2 0)j 5 24i 2 3j.
(a) [3 1 (24)]i 1 [2 1 (23)]j 5 2i 2 j
(b) [3 2 (24)]i 1 [2 2 (23)]j 5 7i 1 5j
Quick Review 10.3
2
x
2. f9(x) 5 2}}, so for x 5 1, f (x) 5 Ï3w and
2wx 2w
Ï4ww
1
f9(x) 5 2}}. Then y 2 Ïw3 5 Ï3w(x 2 1) or y 5 Ï3wx.
Ï3w
409
4. (a) (5 1 3)i 1 [(22) 1 4]j 5 8i 1 2j
(b) (5 2 3)i 1 [(22) 2 4]j 5 2i 2 6j
(c) 3(5)i 1 3(22)j 5 15i 2 6j
(d) [2(5)i 1 2(22)j] 2 [3(3)i 1 3(4)j] 5 i 2 16j
2
410
Section 10.3
5. (a)
8. (a)
[26, 6] by [24, 4]
[26, 6] by [23, 5]
d
dt
d
dt
(b) v(t) 5 }}(2 cos t)i 1 }}(3 sin t)j
d
dt
5 (22 sin t)i 1 (3 cos t)j
1t 1 12
d
2
d
2
a(t) 5 }}1}}2i 1 }}(2t)j 5 12}}2i 1 2j
dt t 1 1
dt
(t 1 1)
2
5 }} i 1 (2t)j
d
d
a(t) 5 }}(22 sin t)i 1 }}(3 cos t)j
dt
dt
5 (22 cos t)i 2(3 sin t)j
12
d
dt
(b) v(t) 5 }}(2 ln (t 1 1))i 1 }}(t 2)j
2
(c) v(1) 5 k1, 2l; speed 5 Ï1w2w1
ww22w 5 Ï5w,
p
2
(c) v }} 5 k22, 0l; speed 5 Ï(2
w2ww
)2w
1w
02w 5 2,
k
(d) Velocity 5 Ï5wk ,
l
Ïw Ïw
1
1
2
l
direction 5 }}k1, 2l 5 }}, }}
Ïw5
Ïw5 Ï5w
1
2
direction 5 }}k22, 0l 5 k21, 0l
1
2
}} }}
5
5
(d) Velocity 5 2k21, 0l
6. (a)
9. v(t) 5 (cos t)i 1 (2t 1 sin t)j, r(0) 5 2j and v(0) 5 i.
So the slope is zero (the velocity vector is horizontal).
(a) The horizontal line through (0, 21): y 5 21.
[24.5, 4.5] by [23, 3]
d
dt
(b) The vertical line through (0, 21): x 5 0.
d
dt
(b) v(t) 5 }}(cos 2t)i 1 }}(2 sin t)j
10. v(t) 5 (22 sin t)i 1 (3 cos t)j,
5 (22 sin 2t)i 1 (2 cos t)j
d
dt
12
1
2
p
3
2
3
3/Ïw
v1}}2 5 (2Ï2w)i 1 1}}2 j. So the slope is }} 5 2}}.
4
2
Ï2w
2Ï2
w
p
d
dt
3
r }} 5 (Ï2w 2 3)i 1 }} 1 1 j and
4
Ï2w
a(t) 5 }}(22 sin 2t)i 1 }}(2 cos t)j
5 (24 cos t)i 2 (2 sin t)j
(c) v(0) 5 k0, 2l; speed 5 Ï0w2w1
ww22w 5 2,
1
2
3
3
(a) y 2 }} 1 1 5 2}}[x 2 (Ï2w 2 3)] or
2
Ïw2
w27
3
6Ï2
y 5 2}}x 1 }}
1
direction 5 }}k0, 2l 5 k0, 1l
2
(d) Velocity 5 2k0, 1l
2
7. (a)
1
2
2
3
2
(b) y 2 }} 1 1 5 }}[x 2 (Ï2w 2 3)] or
3
Ïw2
w 1 18
2
5Ï2
y 5 }}x 1 }}
3
[26, 6] by [24, 4]
d
d
dt
dt
d
d
a(t) 5 }}(sec t tan t)i 1 }}(sec2 t)j
dt
dt
k l k
Ïw
kÏw , Ïw l
3 2 4
1
2
direction 5 }} }}, }} 5 }}, }}
3
3
2Ïw5
Ïw5 Ïw5
2 5 1
2
(d) Velocity 5 }} }} }}
3
5
5
1
2
2
3/2
1
2Ï5w
!§1}§3}§2 §1§1}§3}§2 5 }3},
2 2
2
1
4 2
l
2
1
5 23i 1 (4Ï2w 2 2)j
5 (sec t tan2 t 1 sec3 t)i 1 (2 sec2 t tan t)j
p
2 4
1 6 2 k3 3l
1E (6 2 6t) dt2i 1 1E 3Ïtw dt2 j
5 36t 2 3t 4 i 1 32t 4 j
2
11.
(b) v(t) 5 }}(sec t)i 1 }}(tan t)i 5 (sec t tan t)i 1 (sec2 t)j
(c) v }} 5 }}, }} ; speed 5
6
12.
1E
2 1E (1 1 cos t) dt2j
5 32cos t4
i 1 3t 1 sin t4
j
p
5 1Ï2w 1 }}2j
2
p/4
sin t dt i 1
2p/4
p/4
2p/4
p/4
p/4
2p/4
2p/4
Section 10.3
13.
1Esec t tan t dt2i 1 1Etan t dt2j
22. v(t) 5 (25 sin t)i 1 (5 cos t)j, and
5 (sec t 1 C1)i 1 (ln )sec t) 1 C2)j
5 (sec t)i 1 (ln )sec t))j 1 C
14.
a(t) 5 (25 cos t)i 1 (25 sin t)j.
Solve v ? a 5 0: (25 sin t cos t) 1 (225sin t cos t) 5 0,
which is true for all values of t.
1
1
1E}t} dt2i 1 1E}5 2}t dt2j
23. v(t)5 (22 sin t)i 1 (cos t)j, and
5 (ln )t) 1 C1)i 1 (2ln )5 2 t) 1 C2)j
a(t)5 (22 cos t)i 1 (2sin t)j. So
5 (ln )t))i 2 (ln )5 2 t))j 1 C
v }} 5 (2Ï2w)i 1 }} j, and
4
Ï2w
14 2 122
t
t
r(t) 5 1}} 1 2t 1 12i 1 1}} 1 12 j.
4
2
t
t
dr
dt
17. }} 5 (232t)j 1 C1 and r(t) 5 (216t 2)j 1 C1t 1 C2.
)
dr
5 C1 5 8i 1 8j. So
dt t50
r(0) 5 C2 5 100i, and }}
r(t) 5 (216t2)j 1 (8i 1 8j)t 1 100i
5 (8t 1 100)i 1 (216t 1 8t)j.
2
v?a
1 )v))a) 2
152
3
u 5 cos21 }} 5 cos21 }} < 53.1308.
24. v(t) 5 3i 1 (2t)j, and a(t) 5 2j. So v(0) 5 3i, and
a(0) 5 2j. These are perpendicular, i.e., the angle between
them measures 908.
25. (a) Both components are continuous at t 5 3, so the limit
1 3 1 3(3) 2
32 2 9
is 3i 1 }
2 } j 5 3i.
2
r(t) 5 2}} i 1 2}} j 1 C1t 1 C2
r(0) 5 C2 5 10i 1 10j, and
)
1 2 1 2
1
2 1
26. (a) Use L’Hôpital’s Rule for the i-component:
1
2
sin 2t
t
t→0
2 cos 2t
5 lim }} i 1 lim(ln (t 1 1))j
1
t→0
t→0
lim }} i 1 lim(ln (t 1 1))j
dr
5 C1 5 0, so
}}
dt t50
t2
t2
r(t) 5 2}} i 1 2}} j 1 (10i 1 10j)
2
2
t2
t2
5 2}} 1 10 i 1 2}} 1 10 j
2
2
2
19. v(t) 5 (1 2 cos t)i 1 (sin t)j and a(t) 5 (sin t)i 1 (cos t)j.
Solve v ? a 5 0: (sin t 2 sin t cos t) 1 (sin t cos t) 5 0
implies sin t 5 0, which is true for t 5 0, p, or 2p.
20. v(t) 5 (cos t)i 1 j, and a(t) 5 (2sin t)i.
Solve v ? a 5 0: 2sin t cos t 5 0, which is true for
kp
t 5 }}, k any nonnegative integer.
2
21. v(t) 5 (23 sin t)i 1 (4 cos t)j, and
a(t) 5 (23 cos t)i 1 (24 sin t)j.
Solve v ? a 5 0: (9 sin t cos t) 2 (16 sin t cos t) 5 0, is
true when sin t 5 0 or cos t 5 0, i.e., for
kp
2
3
2
v ? a 5 }}, and
(c) Discontinuous when t 2 1 3t 5 0, i.e., t 5 0 or 23
1 22 1 22
t
5
(b) Continuous so long as t 2 1 3t Þ 0, i.e., t Þ 0, 23
dr
dt
18. }} 5 2t i 2 t j 1 C1, and
t
!}§2},
Then )v) 5 )a) 5
2
2
2
1
2
16. r(t) 5 }} 1 2t 2 i 1 }} j 1 C, and r(0) 5 C 5 i 1 j, so
4
12
1 2
p
1
a1}}2 5 (2Ï2w)i 1 12}}2 j.
4
Ïw2
p
15. r(t) 5 (t 1 1)3/2 i 2 e2t j 1 C, and
r(0) 5 i 2 j 1 C 5 0, so C 5 2(i 2 j) 5 2i 1 j
r(t) 5 ((t 1 1)3/2 2 1)i 2 (e2t 2 1)j
4
411
t 5 }}, k any nonnegative integer.
t→0
1
2
5 2i 1 0j 5 2i.
(b) Continuous so long as t Þ 0 and t 1 1 . 0, i.e.,
(21, 0) < (0, `).
(c) Discontinuous when t 5 0 or t 1 1 # 0, i.e.,
(2` 21] < {0}.
27. v(t) 5 (sin t)i 1 (1 2 cos t)j, i.e.,
dx
dy
}} 5 sin t, and }} 5 1 2 cos t
dt
dt
E
5E
5E
Distance 5
2p/3
Ï(s
win
wwtw
)2w
1w(1ww
2wcowswt)
w2w dt
0
2p/3
Ï2ww
2w2wcowswtw dt
0
2p/3
122
t
5 324 cos 1}}24
2
0
t
2 sin }} dt
2p/3
0
52
412
Section 10.3
14
31. a(t) 5 3i 2 j, so v(t) 5 (3t)i 2 tj 1 C1 and
2
1
28. (a) r(0) 5 }}e0 2 0 i 1 (e0)j
12 2 12 2
3
14 2
1
1
Initial 5 1}}, 12, terminal 5 1}}e
4
4
and since v(0) must point directly from (1, 2) toward (4, 1)
1
r(2) 5 }}e8 2 2 i 1 (e4)j
8
with magnitude 2,
2
2 2, e4
dx
dt
dy
}} 5 2e2t.
dt
0
2
0
2
2
4t
2
5
5
w0w
Ïw10w
3 2
3Ï1
1
So r(t) 5 }}t 1 }}t 1 1 i 1 2}}t 2 2 }}t 1 2 j.
2
2
5
5
2t 2
1
dx
dt
3
1
4
4
e8 1 7
4
0
4t
4t
2
dy
dx
0
2
4t
4t
3 32
1
1
1
2
16
16
16
8
e 2 12e 2 69
5 p }} < 1,737,746.456
16
1
40
5 2p }}e8t 1 }}e4t 2 }}(4t 2 1)e4t 2 }}t 2
2
2
p
2
3p
2
at t 5 }} and }}; sin 2t 5 0 at t 5 0, }}, p, }}, and 2p.
p 3p
2 2
So v(t) 5 0 at t 5 }}, }}.
(c) x 5 sin t, y 5 cos 2t. Relate the two using the identity
cos 2u 5 1 2 2 sin2 u: y 5 1 2 2x 2, where as t ranges
over all possible values, 21 # x # 1. When t increases
from 0 to 2p, the particle starts at (0, 1), goes to
(1, 21), then goes to (21, 21), and then goes to (0, 1),
tracing the curve twice.
dy
dy/dt
3t 2 2 12
t2 2 4
30. (a) }} 5 }} 5 }
}5}
}
dx
dx/dt
6t 2 2 6t
2t 2 2 2t
(b) Horizontal tangents: t 2 4 5 0 for t 5 62.
Vertical tangents: 2t 2 2 2t 5 0 for t 5 0, 1.
Plugging the t-values into x 5 2t 3 2 3t 2 and
y 5 t 3 2 12t produces the x- and y-coordinates of the
critical points.
t 5 22: horizontal tangent at (228, 16)
t 5 0: vertical tangent at (0, 0)
t 5 1: vertical tangent at (21, 211)
t 5 2: horizontal tangent at (4, 216)
2
3
64
(b) 2}}(40)(40 2 160) 5 225 m
d
dt
(b) v(t) 5 0 when both cos t 5 0 and sin 2t 5 0. cos t 5 0
3p
2
33. (a) The j-component is zero at t 5 0 and t 5 160:
160 seconds.
3
4
15
2
3
3
64
32
15
equals }} m per second.
4
(c) }} 2}}t(t 2 160) 5 2}}t 1 }}, which for t 5 40
29. (a) v(t) 5 (cos t)i 2 (2 sin 2t)j
p
2
6t
1 2 2/t
which for t 5 2 equals 224.
4t
0
1
dy/dt
dx/dt
(1 2 2/t 2)6 2 (4/t 3)6t
d 2y
dy9
dy9/dt
,
}}2 5 }} 5 }} 5 }}}
(1 2 2/t 2)3
dx
dx
dx/dt
4t
8t
2
2
(c) When y 5 12, t 5 2.
2t 2
0
2
1
(b) }} 5 y9 5 }} 5 }}2 , which for t 5 1 equals 26.
E 2p1}14}e 2 t2Ï(ewww2w1w) w1w(2wwe w)w dt
1
5 2pE 1}}e 2 t2(e 1 1) dt
4
1
1
5 2pE 1}}e 1 }}e 2 te 2 t2 dt
4
4
2
2
t
2
point Ï2w 1 }}, 3(Ï2w)2 5 (2Ï2w, 6).
Ï2w
2
5 }} < 746.989
(c)
2 1
32. (a) }} 5 1 2 }}2 5 0 when t 5 Ï2w. That corresponds to
4t
0
5 }}e4t 1 t
2
6
2
5 }}i 2 }}j
Ïw1w0
Ïw1w0
w0w
Ïw10w
3Ï1
5 }}i 2 }}j
E Ï(ewww2w1w) w1w(2wwe w)w dt
www
1w1w
) dt
5 E Ï(e
5 E (e 1 1) dt
Length 5
4t
1
(4 2 1)i 1 (1 2 2)j
v(0) 5 C1 5 2 }}}
Ï(4
ww
2w1)w2w
1w(1
ww
2w
2)w2
(b) v(t) 5 (e4t 2 1)i 1 (2e2t)j; }} 5 e4t 2 1, and
2
1
r(t) 5 }}t 2 i 2 }}t 2 j 1 C1t 1 C2. r(0) 5 C2 5 i 1 2j,
1
4
5 }}i 1 j,
3
32
15
2
(d) v(t) 5 2}}t 1 }} equals 0 at t 5 80 seconds (and is
negative after that time).
3t
2
34. (a) Solve t 2 3 5 }} 2 4: t 5 2. Then check that
3t
2
(t 2 3)2 5 }} 2 2 for t 5 2: it does.
(b) First particle: v1(t) 5 i 1 2(t 2 3)j, so v1(2) 5 i 2 2j
k
1
1
l
2
l
and the direction unit vector v1 is }}, 2}} .
Ïw5 Ïw5
3
3
Second particle: v2(t) 5 }}i 1 }}j, which is constant, and
2
k
2
1
the direction unit vector is }}, }} .
Ïw2 Ï2w
Section 10.3
35. (a) Referring to the figure, look at the circular arc from the
point where t 5 0 to the point “m”. On one hand, this
arc has length given by r0u, but it also has length given
by vt. Setting those two quantities equal gives the
result.
1
2 1
2
v
v
vt
vt
a(t) 5 12}} cos }}2i 1 12}} sin }}2j
r
r
r
r
v
vt
vt
5 2}}31cos }}2i 1 1sin }}2j4
r
r
r
40. (a) Suppose u 5 ku1(t), u2(t)l.
d
d
}}(cu) 5 }}kcu1(t), cu2(t)l
dt
dt
k
k
0
0
0
d
dt
v 2
(c) From part (b) above, a(t) 5 2 }} r(t).
0
du
dt
dt
l k
du
du
dt
dt
l
du
dt
d
dt
5 k fu19 1 f 9u1, fu29 1 f 9u2l
0
1r 2
du
l
(b) }}( fu) 5 }}k fu1, fu2l
0
2
0
d
dt
5 c}}1 , c}}2 5 c }}1 , }}2 5 c}}
2
0
d
dt
5 }}(cu1(t)), }}(cu2(t))
vt
vt
(b) v(t) 5 2v sin }} i 1 v cos }} j, and
r0
r0
2
413
5 k fu19, fu29l 1 k f 9u1, f 9u2l
v 2
So, by Newton’s second law, F 5 2m }} r.
r0
1 2
Substituting for F in the law of gravitation gives the
5 fu9 1 f 9u
41. u 5 ku1, u2l, v 5 kv1, v2l
result.
d
dt
d
dt
d
d
5 }}(u1 1 v1), }}(u2 1 v2)
dt
dt
(a) }}(u 1 v) 5 }}(ku1 1 v1, u2 1 v2l)
vT
r0
k
(d) Set }} 5 2p and solve for vT.
2pr
5 ku19 1 v19, u29 1 v29l
GM
r0
(e) Substitute }}0 for v in v 2 5 }} and solve for T 2:
1
T
2pr0 2
GM
}} 5 }}
T
r0
2
du
dt
d
dt
d
dt
d
d
5 }}(u1 2 v1), }}(u2 2 v2)
dt
dt
k
1
GM
}}2 5 }2}3
T
4p r0
T
dv
dt
5 ku19, u29l 1 kv19, v29l 5 }} 1 }}
(b) }}(u 2 v) 5 }}(ku1 2 v1, u2 2 v2l)
4p r02
GM
5 }}
}}
T2
r0
2
2
l
l
5 ku19 2 v19, u29 2 v29l
4p 2
5 }}r03
GM
36. Solve both equations for t: t 5 e 2 1 and t 5 Ïyw1
ww1.
Now eliminate the t and solve for y:
e x 2 1 5 Ïw
yw
1w1, y 5 (e x 2 1)2 2 1, or y 5 e 2x 2 2e x,
where t $ 0 so x $ 0.
5 ku19, u29l 2 kv19, v29l
x
37. (a) Apply Corollary 3 to each component separately. If the
components all differ by scalar constants, the
difference vector is a constant vector.
(b) Follows immediately from (a) since any two
anti-derivatives of r(t) must have identical derivatives,
namely r(t).
d
d
38. }})v)2 5 }}(v ? v) 5 v9 ? v + v ? v9 5 2v ? v9 5 0.
dt
dt
Therefore, )v) is constant.
k
l
dC dC
dC
39. Let C 5 kC1, C2 l. }} 5 }}1 , }}2 5 k0, 0l.
dt
dt dt
du
dt
dv
dt
5 }} 2 }}
dr
dt
df
dt
dg
dt
42. }} 5 }}i 1 }}j
1}d}t 21}d}s 2 5 1}d}t i 1 }d}t j21}d}s 2
df dt
dg dt
5 1}} ? }}2i 1 1}} ? }}2j
dt ds
dt ds
dr
dt
df
df
ds
dg
dt
dg
ds
5 }}i 1 }}j
dr
ds
5 }}
43. f (t) and g(t) differentiable at c ⇒ f (t) and g(t) continuous at
c ⇒ r(t) 5 f (t)i 1 g(t)j is continuous at c.
414
Section 10.4
44. (a) Let r(t) 5 kx(t), y(t)l.
■ Section 10.4 Modeling Projectile Motion
E kr(t) dt 5 E kkx(t), ky(t)l dt 5 kE kx(t) dt, E ky(t) dtl
5 kkE x(t) dt, kE y(t) dtl
5 kkE x(t) dt, E y(t) dtl 5 kE kx(t), y(t)l dt
5 kE r(t) dt
b
b
b
a
a
b
a
b
a
b
a
b
a
b
a
b
b
a
a
a
(pp. 539–552)
Exploration 1 Hitting a Home Run
1. The graphs of the parametric equations
x 5 (152 cos 208 2 8.8)t, y 5 3 1 (152 sin 208)t 2 16t 2
and the fence are shown in the window [0, 450] by
[220, 60]. The fence was obtained using the line command
“Line(“. You can zoom in as shown in the second figure to
see that the ball does just clear the fence.
(b) Let r1(t) 5 kx1(t), y1(t)l and r2(t) 5 kx2(t), y2(t)l.
E (r (t) 6 r (t)) dt 5 E (kx (t), y (t)l 6 kx (t), y (t)l) dt
5 E kx (t) 6 x (t), y (t) 6 y (t)l dt
5 kE (x (t) 6 x (t)) dt, E (y (t) 6 y (t)) dtl
5 kE x (t) dt 6E x (t) dt, E y (t) dt 6E y (t) dtl
5 kE x (t) dt, E y (t) dtl 6 kE x (t) dt, E y (t) dtl
5 E r (t) dt 6 E r (t) dt
b
b
1
a
2
1
a
1
2
2
b
1
a
2
1
2
b
b
1
a
b
a
b
a
b
a
2
a
b
1
2
a
b
1
1
2
b
b
1
a
b
1
a
b
2
a
2
a
a
2
b
1
2
a
You can also use algebraic methods to show that t < 2.984
when x 5 400, and that y < 15.647 for this value of t.
2. angle (degrees)
range (ft)
25
flight time (sec) <4.061
(c) Let C 5 kC1, C2l, r(t) 5 kx(t), y(t)l.
E C ? r(t) dt 5 E (C x(t) 1 C y(t)) dt
5 C E x(t) dt 1 C E y(t) dt
5 kC , C l ? kE x(t) dt, E y(t) dtl
5 C ? E r(t) dt
b
b
a
1
a
b
2
a
a
a
4. angle (degrees)
range (ft)
25
E r(q) dq 5 }dd}t E [ f (q)i 1 g(q)j] dq
d
5 }}31E f (q) dq2 i 1 1E g(q) dq2 j4
dt
d
d
5 1}} E f (q) dq2i 1 1}}E g(q) dq2j
dt
dt
t
t
a
a
t
t
a
a
30
45
<559.444 <630.424 <724.988
flight time (sec) <4.061
45. (a) Let r(t) 5 f (t)i 1 g(t)j. Then
t
3. Using the same window of part (1) we can see that the ball
clears the fence.
b
b
a
<6.745
2 a
1
t
<4.789
b
1 a
a
45
2
b
d
}}
dt
30
<523.707 <588.279 <665.629
<4.789
<6.745
Exploration 2 Hitting a Baseball
152
0.05
1. x 5 }}(1 2 e 20.05t ) cos 208
152
0.05
32
1 }}2 (1 2 0.05t 2 e20.05t )
0.05
y 5 3 1 }}(1 2 e 20.05t ) sin 208
5 f (t)i 1 g(t)j 5 r(t).
(b) Let S(t) 5
E r(q) dq. Then part (a) shows that S(t) is an
t
a
antiderivative of r(t). Let R(t) be any antiderivative of
r(t). Then according to 37(b), S(t) 5 R(t) 1 C.
Letting t 5 a, we have 0 5 S(a) 5 R(a) 1 C.
Therefore, C 5 2R(a) and S(t) 5 R(t) 2 R(a).
The result follows by letting t 5 b.
[0, 450] by [–20, 60]
2. The ball reaches a maximum height of about 43.07 ft when
t is about 1.56 sec.
3. The range is about 425.47 ft and the flight time is about
3.23 sec.
Section 10.4
Quick Review 10.4
415
Section 10.4 Exercises
1. k50 cos 258, 50 sin 258l < k45.315, 21.131l
1. Solve vxt 5 (840 cos 60°)t 5 21,000 for t: t 5 50 seconds.
2. k80 cos 1208, 80 sin 1208l 5 k240, 40Ï3wl
v
3. To find the x-intercepts, solve 2x 2 1 11x 2 40 5 0 using
211 6 Ï1
w1w2w2
ww4(2
w)(
w2
w4w0w)w
2(2)
the quadratic formula: x 5 }}}
2
v
2
0
0
2. Use R 5 }
sin 2a; solve 24,500 5 }
sin 90°
g
9.8
for v0: v0 5 490 m/sec.
2v sin a
2(500)sin 45°
9.8
0
3. (a) t 5 }
} 5 }} < 72.154 seconds;
g
12 2
5
2
5
5 }} or 28. The x-intercepts are }}, 0 and (28, 0). For the
y-intercept, find f (0) 5 2(0)2 1 11(0) 2 40 5 240. The
y-intercept is (0, 240).
11
4
4. At the vertex, f 9(x) 5 4x 1 11 5 0 and x 5 2}}. Then the
1
11
4
11
441
5 2}}, 2}} .
4
8
11 2
1 42
vertex is 2}}, 2 2}}
1
2
1 42
11
1 11 2}} 2 40
2
6. At the vertex, g9(x) 5 20 2 2x 5 0 and x 5 10. Then the
vertex is (10, 20(10) 2 102) 5 (10, 100).
12
p
2
12
p
2
7. y 5 2cos x 1 C. y }} 5 2cos }} 1 C 5 C 5 2, so
1
8. y9 5 t 1 C1 and y 5 }}t 3 1 C1t 1 C2
3
2
y9(21) 5 (21)2 1 C1 5 1 1 C1 5 4, so C1 5 3.
1
10
y(21) 5 }}(21)3 1 3(21) 1 C2 5 2}} 1 C2 5 5, so
3
3
25
C2 5 }}
3
t3
25
y 5 }} 1 3t 1 }}
3
3
9.
E
5002
9.8
5 25.510 km downrange
1 2v
g
cos a
2
x 2 1 (tan a) x
(b) y 5 2 }
2
2 }
0
1 2(500) cos 45° 2
9.8
50002 + (tan 45°)5000 5 4020 m
52 }
2 }
2
E
(500 sin 45°)2
2(9.8)
0
(c) ymax 5 }
} 5 }} < 6377.551 m
2g
4. With the origin at the launch point
(so the ground is t 5 2 when y 5 232), use
1
2
y 5 (v0 sin a) t 2 }}gt 2.
1
2
232 5 (32 sin 30°)t 2 }}(32)t 2
22 5 t 2 t 2
t 5 2 seconds
Then x 5 (v0 cos a) t 5 (32 cos 30°)2 5 32Ï3w < 55.426
feet away (horizontally).
1
2
5. Use y 5 (v0 sin a)t 2 }}gt 2 1 6.5.
16t 2 2 22Ï2wt 2 6.5 5 0
w 1 Ï3w4w6w
11Ï2
t 5 }} < 2.135 seconds (by the quadratic
16
formula). Substitute that into x 5 (v0 cos a) t
dy
}} 5 dt
16 2 y
2ln )16 2 y) 5 t 1 C
5 (44 sin 45°)t to obtain x < 66.4206. 66.421 feet from the
stopboard.
16 2 y 5 ke 2t
y(0) 5 16 2 k 5 20 so k 5 24
y 5 16 1 4e
2
(v sin a)2
5. To find the x-intercepts, solve 20x 2 x 2 5 0: x 5 0 or 20.
The x-intercepts are (0, 0) and (20, 0). For the y-intercept,
find y (0): it is already known to be 0. So the y-intercept is
(0, 0).
y 5 2cos x 1 2.
v
0
R5}
g sin 2a 5 }} sin 90° < 25,510 m
2t
6. With the origin at the launch point, use
1
2
y 5 (v0 sin a)t 2 }}gt 2. 26.5 5 (44 sin 408)t 2 16t 2
E 4 2dy2y E
(44 sin 408) 1 Ï(4
w4wwsin
ww40w8)
w2w1
ww41w6w
t 5 }}}} < 1.974 sec
1
1
2}} ln )4 2 2y) 5 }}x 2 1 C
2
2
At t < 1.974, x 5 (44 cos 408)t < 66.5193 ft
10. }} 5 x dx
4 2 2y 5 ke 2x
k
2
y 5 2 2 }}e 2x
k
2
2
2
y(0) 5 2 2 }} 5 1 so k 5 2
y 5 2 2 e 2x
2
32
Thus the shot would have gone <0.0987 feet <1.18 inches
farther.
416
Section 10.4
v
2
v
2
0
7. (a) Use R 5 }
sin 2a; solve 10 5 }0} sin 90° for v0:
g
9.8
v0 5 7Ï2w < 9.899 m/sec.
(7Ïw2)2
(b) Solve 6 5 }} sin 2a for a: sin 2a 5 0.6, so
9.8
2a 5 sin 21 0.6 < 36.8708 and a < 18.4358 or
2a 5 180° 2 sin 21 0.6 < 143.130 and a < 71.5658.
40 3 1022 m
5 3 10 m/sec
1
1
positive) is }}gt 2 < }}(9.8)(8 3 1028)2 5 3.136 3 10214
2
2
8. t 5 }}
5 8 3 1028 sec. Then y (taking down as
6
2
(9.8)(16,000)
400
sin 21 0.98
sin 21 0.98
a 5 }} < 39.2618 or a 5 90 2 }}
2
2
< 50.7398.
16. (a) Substitute 2v0 for v0 in the formula for range.
(b) To increase the range (and height) by a factor of 2,
increase v0 by a factor of Ï2w < 1.41. That is an
increase of < 41%.
17. With the origin at the launch point,
1 2v
32
cos 40°
2
5
6
y52 }
x 2 1 (tan 40°)x. Setting x 5 73}} and
2
2 }
0
meters or 3.136 3 10212 cm.
v
v
0
15. Use R 5 }
sin 2a: sin 2a 5 }}
5 0.98;
}
2
g
y 5 26.5 and solving for v0 yields v0 < 46.597 ft/sec.
2
0
9. R 5 }
sin 2a
g
1
2
18. y(t) 5 v0(sin a)t 2 }}gt 2, and we know the maximum height
v02
(v sin a)2
v sin a
(248.8 yd)(3 ft/yd) 5 }}2 sin 18°
0
0
is }
} and it occurs when t 5 }
}. Substituting
v0 < 278.016 ft/sec or < 189.556 mph.
0
t5}
} into the equation for y(t) gives a height of
32 ft/sec
w 2
80Ï1w0
}}
v02
3
10. R 5 }
sin 2a ⇒ 200 5 }} sin 2a ⇒ sin 2a 5 0.9.
}
g
32
1
2
Taking the smaller of the two possible angles,
1
2
a 5 }} sin 21 0.9 < 32.0798. Then
1
80Ïw1w0 2
}} sin 2 32.079
3
g
2g
3(v0 sin a)2
}}, which is three-fourths of the maximum height.
8g
d
dt
19. Integrating, }}r(t) 5 c1i 1 (2gt 1 c2)j. The initial
condition on the velocity gives c1 5 v0 cos a
and c2 5 v0 sin a. Integrating again,
2
r(t) 5 ((v0 cos a)t 1 c3)i 1 }}gt 2 1 (v0 sin a)t 1 c4 j.
2(32)
The initial condition on the position gives
ymax < }}} < 31.339, which is well below
12
1
2
c3 5 x0 and c4 5 y0.
the ceiling height.
11. No. For a 5 30°, v0 5 90 ft/sec, and x 5 135 ft,
1
2g
v sin a
2
32
y52 }
} x 2 1 (tan a)x evaluates to < 29.942
2v02 cos 2 a
20. With the origin at the launch point, ymax 5 68 ft. Then
Ï2wyw
wgw
Ï2w(6
w8w)(
w3w2w)w
max
v0 5 }}
< v0 5 }} < 79.107 ft/sec.
sin a
sin 56.505°
feet above the ground, which is not quite high enough.
21. The horizontal distance is 30 yd 2 6 ft 5 84 ft. Then
1
2
32
12. Use y 5 2 }
} x 2 1 (tan 45°)x
2(116)2 cos 2 45°
2
5 2}}x 2 1 x. Set y 5 45, then solve for x using the
841
quadratic formula and taking the larger of the two values:
!§§§
481
1 1 }}
841 < 369.255 ft, which is < 0.255 ft < 3.059
x 5 }}
4
}}
841
2
x 2 1 (tan 20°)x. Set x 5 315 and
y52 }
2
2 }
0
w
16Ïw17
84
v0 5 }} (from Exercise 20). So t 5 }}
sin a
v0 cos a
68
21 }}
4
5
84 tan a
119
5 } 5 } = }} < 1.924 seconds. Then
16Ï1
ww7
4Ïw
1w
7
15Ïw17
w
1 2
1
2
13. (a) With the origin at the launch point, use
32
cos 20°
68
y 5 (v0 sin a) t 2 }}gt 2
inches beyond the pin.
1 2v
1 45 2
84 5 (v0 cos a) t, where a 5 tan 21 }} < 56.5° and
y 5 37 2 3 5 34, then solve to find
1260
v0 5 }}} < 149.307 ft/sec.
cos 20°Ï3
w1w5wwtan
ww20w°w2
ww34w
(b) Solve v0(cos 20°)t < 149.307(cos 20°)t 5 315 to find
t < 2.245 seconds.
14. In the formula for range, sin 2a 5 sin 2(90 2 a).
1
119
2
1
1
119
2
2
5 (16Ï1w7w ) }} 2 }}(32) }} < 67.698 ft.
2
15Ïw17
w
15Ïw17
w
The height above the ground is 6 ft more than that,
< 73.698, and the height above the rim is about
73.698 2 70 5 3.698 feet.
22. The projectile rises straight up and then falls straight down,
returning to the firing point.
Section 10.4
23. Angle is a < 62° (measurements may vary slightly). For
(v sin a)
2v sin a
g
2
(b)
417
v0
1
8
0
0 } 5 1 sec, y
flight time t 5 }
5}
} 5 }}gt 2
max
2g
1
8
5 }}(32)(1)2 5 4 ft (independent of the measured angle).
gt
gt
2 sin a
2 tan a
32(1)
< }} < 8.507 ft/sec (changes with the angle).
2 tan (62°)
v0 5 }}, so speed of engine 5 v0 cos a 5 }}
u
(Rcosb, Rsinb)
b
1
2
24. The height of A is given by yA 5 (v sin a)t 2 }}gt 2 and the
1
2
R
height of B is given by yB 5 R tan a 2 }}gt 2. The second
1
1
2
2
terms in yA and yB 2}}gt 2 are equal for any value of t. But
R
v cos a
2v
2
A moves R units horizontally to B’s line of fall in }}
0
R 5 }}
cos u sin (u 2 b) is maximum when
2
time units, and the first terms in yA and yB are also equal at
tan u 5 cot (u 2 b),
1 v cos a 2
R
g cos b
that time: (v sin a) }} 5 R tan a. Therefore, A and B
so u 2 b 5 908 2 u.
will always be at the same height when A reaches B’s line
The initial velocity vector bisects the angle between the
hill and the vertical for max range.
of fall.
26. (a) r(t) 5 (x(t))i 1 (y(t))j, where
x(t) 5 (145 cos 238 2 14)t and
y(t) 5 2.5 1 (145 sin 238)t 2 16t 2.
25. (a)
(v sin a)2
(145 sin 23°)2
64
0
(b) ymax 5 }
} 1 2.5 5 }} 1 2.5
2g
v sin a
0
< 52.655 feet , which is reached at t 5 }
}
g
v0
145 sin 23°
32
5 }} < 1.771 seconds.
u
(c) For the time, solve
b
R
(Rcosb, –Rsinb)
y 5 2.5 1 (145 sin 23°)t 2 16t 2 5 0 for t, using the
quadratic formula:
w4w5wwsin
ww23w°)
w2w1
ww16w0w
145 sin 23° 1 Ï(1
t 5 }}}} < 3.585 sec.
x 5 (v0 cos u)t
32
Then the range at t < 3.585 is about
1
y 5 (v0 sin u)t 2 }}gt 2
2
x 5 R cos b ⇒ R cos b 5 (v0 cos u)t
R cos b
v0 cos u
x 5 (145 cos 23° 2 14)(3.585) < 428.262 feet.
⇒ t 5 }}. Then y 5 2R sin b
(v sin u) R cos b
(d) For the time, solve y 5 2.5 1 (145 sin 23°)t 2 16t 2
g R cos b
2 v0 cos u
2
2
0
⇒ 2R sin b 5 }
} 2 }} }
2 }
2
5 20 for t, using the quadratic formula:
2v02
⇒ R 5 }}
cos u sin (u 1 b).
g cos2 b
t 5 }}}}} < 0.342 and
v0 cos u
145 sin 23° 6 Ï(1
w4w5wwsin
ww23w°)
w2w2
ww11w2w0w
32
Let f (u) 5 cos u sin (u 1 b).
3.199 seconds. At those times the ball is about
f 9(u) 5 cos u cos (u 1 b) 2 sin u sin (u 1 b)
x(0.342) 5 (145 cos 23° 2 14)(0.342) < 40.847 feet
f 9(u) 5 0 ⇒ tan u tan (u 1 b) 5 1
and x(3.199) 5 (145 cos 23° 2 14)(3.199) < 382.208
⇒ tan u 5 cot (u 1 b)
feet from home plate.
⇒ u 1 b 5 908 2 u. Note that f 0(u) , 0, so R is
maximum when a 5 u 1 b 5 908 2 u. Thus the initial
velocity bisects angle AOR.
(e) Yes. According to part (d), the ball is still 20 feet above
the ground when it is 382 feet from home plate.
418
Section 10.4
27. (a) (Assuming that “x” is zero at the point of impact.)
r(t) 5 (x(t))i 1 (y(t))j, where
x(t) 5 (35 cos 278)t and
y(t) 5 4 1 (35 sin 278)t 2 16t 2.
(v sin a)2
(35 sin 27°)2
2g
64
v0 sin a 35 sin 27°
which is reached at t 5 }
} = }}
g
32
0
(b) ymax 5 }
} 1 4 5 }} 1 4 < 7.945 feet,
< 0.497 seconds.
(d) Graph Y2 5 30 and use the intersect function to find
that y 5 30 for t < 0.689 and 2.305 seconds, at which
times the ball is about x(0.689) < 94.513 feet and
x(2.305) < 287.628 feet from home plate.
(e) Yes, the batter has hit a home run since a graph in
parametric mode shows that the ball is more than
14 feet above the ground when it passes over the fence.
29. (a) r(t) 5 (x(t))i 1 (y(t))j, where
1 0.08 2
152
y(t) 5 3 1 1}}2(1 2 e 20.08t)(sin 208)
0.08
32
1 1}}2(1 2 0.08t 2 e 20.08t)
0.08
1
(c) For the time, solve y 5 4 1 (35 sin 27°)t 2 16t 2 5 0
for t, using the quadratic formula:
35 sin 27° 1 Ï(2
w3w5wwsin
ww27w°)
w2w1
ww25w6w
t 5 }}}}
32
< 1.201 seconds.
Then the range is about x (1.201) 5 (35 cos 27°)(1.201)
< 37.406 feet.
x(t) 5 }} (1 2 e 20.08t)(152 cos 208 2 17.6) and
2
(b) Solve graphically: enter y (t) for Y1 (where X stands in
for t), then use the maximum function to find that at
t < 1.527 seconds the ball reaches a maximum height
of about 41.893 feet.
(c) Use the zero function to find that y 5 0 when the ball
(d) For the time, solve y 5 4 1 (35 sin 27°)t 2 16t 2 5 7
for t, using the quadratic formula:
35 sin 27° 6 Ï(2
w3w5wwsin
ww27w°)
w2w2
ww19w2w
t 5 }}}} < 0.254 and
32
0.740 seconds. At those times the ball is about
has traveled for < 3.181 seconds. The range is about
x(3.181)
1 0.08 2
1
5 }} (1 2 e 20.08(3.181))(152 cos 20° 2 17.6)
< 351.734 feet
x(0.254) 5 (35 cos 27°)(0.254) < 7.906 feet and
x(0.740) 5 (35 cos 27°)(0.740) < 23.064 feet from the
(d) Graph Y2 5 35 and use the interesect function to find
impact point, or about 37.460 2 7.906 < 29.554 feet
that y 5 35 for t < 0.877 and 2.190 seconds, at which
and 37.460 2 23.064 < 14.396 feet from the landing
times the ball is about < x(0.877) < 106.028 feet and
spot.
x(2.190) < 251.530 feet from home plate.
(e) Yes. It changes things because the ball won’t clear the
net (ymax < 7.945 ft).
(e) No; the range is less than 380 feet. To find the wind
needed for a home run, first use the method of part (d)
28. (a) r(t) 5 (x(t))i 1 (y(t))j, where
1 2
1 2
1 2
152
x(t) 5 }} (1 2 e 20.12t)(cos 208) and
0.12
152
y(t) 5 3 1 }} (1 2 e 20.12t)(sin 208)
0.12
32
1 }}2 (1 2 0.12t 2 e 20.12t)
0.12
(b) Solve graphically: enter y (t) for Y1 (where X stands in
for t), then use the maximum function to find that at
t < 1.484 seconds the ball reaches a maximum height
of about 40.435 feet.
(c) Use the zero function to find that y 5 0 when the ball
has traveled for < 3.126 seconds. The range is about
1 0.12 2
152
x(3.126) 5 }} (1 2 e 20.12(3.126))(cos 20°)
< 372.323 feet.
to find that y 5 20 at t < 0.376 and 2.716 seconds.
Then define
1 0.08 2
1
x(w) 5 }} (1 2 e 20.08(2.716))(152 cos 20° 1 w),
and solve x(w) 5 380 to find w < 12.846 ft/sec. This is
the speed of a wind gust needed in the direction of the
hit for the ball to clear the fence for a home run.
Section 10.5 419
30. (a) To save time, enter one expression for x(t) in the main
window, then use the ENTRY function to repeat it six
times in the parametric Y 5 menu. Do the same for
y(t), then make appropriate modifications.
dr
g
g
dt
k
k
d 2r
2kt
2kt
cos a)i 1 (2kv0e
sin a 2 ge 2kt)j
}} 5 (2kv0e
dt
dr
5 2gj 2 k}}
dt
32. }} 5 (v0e 2kt cos a)i 1 (v0e 2kt sin a 1 }}e 2kt 2 }})j
The initial conditions are also satisfied, since
v
r(0) 5 }}0 (1 2 e0)(cos a)i 1
k
v0
3}k}(1 2 e0)(sin a) 1 }k}(1 2 0 2 e0)4j
[0, 500] by [0, 50]
2
Now replace T with X in all the y(t) expressions in the
parametric Y 5 menu, then change to function mode
and enter Y1T for Y1, Y2T for Y2, and so on. Use the
functions in the CALC menu to fill in the tables for
parts (b) and (c).
(b)
drag coeff
time at max ht
t < 3.289
t < 3.273
t < 3.153
t < 3.088
t < 3.028
t < 2.974
462.152
452.478
386.274
352.983
324.410
299.661
2kt
k
t2
1 2 kt 2 e2kt
lim }}
5
2
}
}.
k2
2
k→0
As k → 0, the air resistance approaches 0.
12
2
R
31. The points in question are (x, y) 5 }}, ymax . So,
(v sin a)
2
0
x 5 }}, and y 5 }
}. Then
2g
v2 2
x 2 1 4 y 2 }0}
4g
1
2
v02 sin a cos a 2
(v0 sin a)2
v2 2
5 }
} 14 }
} 2 }0}
g
2g
4g
1
v
2
4
1
2
3
1
sin a
2
1 2
4
3
1
sin4 a
4
sin2 a
4
4
3
2
24
2
2
5 }0}
2 sin a cos a 1 4 }} 2 }}
g
v
4
1
16
24
2
2
5 }0}
2 sin a cos a 1 4 }} 2 }} 1 }}
g
v
1
4
2
2
2
2
2
5 }0}
2 sin a cos a 1 (sin a)(1 2 cos a) 2 sin a 1 }}
g
1
g
k
g
k
2
v4 1
v04
5 }0}
,
2 }} 5 }}
g 4
4g2
12
so the point (x, y) lies on the ellipse.
■ Section 10.5 Polar Coordinates and
Polar Graphs (pp. 552–559)
Exploration 1
Investigating Polar Graphs
1. The graph is drawn in the decimal window [24.7, 4.7] by
p
2
p
2
[23.1, 3.1] with 2}} ≤ u ≤ }}.
p
2
4. If (r, u) is a solution of r 2 5 4 cos u, then so is (r, 2u)
because cos (2u) 5 cos u. Thus, the graph is symmetric
about the x-axis.
If (r, u) is a solution of r 2 5 4 cos u, then so is (2r, 2u)
because (2r)2 5 r 2 and cos (2u) 5 cos u. Thus, the graph
is symmetric about the y-axis.
The graph is symmetric about the origin because it is
symmetric about both the x- and y-axes. You can also give a
direct proof by showing that (2r, u) lies on the graph if
(r, u) does.
1−e
lim }
} 5 t, and
g
)
5 (v0 cos a)i 1 (v0 sin a)j
3. p
k→0
sin a cos a
dr
dt
and }} t50 5 (v0e0 cos a)i 1 v0e0 sin a 1 }}e0 2 }} j
2. r1 and r2 are 0 for u 5 }}.
(d) This follows from the following two limits
(as k → 0):
v02
5 0i 1 0j 5 0,
max ht
k 5 0.01
t < 1.612
44.777
k 5 0.02
t < 1.599
44.336
k 5 0.10
t < 1.505
41.149
k 5 0.15
t < 1.454
39.419
k 5 0.20
t < 1.407
37.854
k 5 0.25
t < 1.363
36.431
(c) After flight times using the zero function, plug the
x-intercepts into T and read the ranges out as X1T, X2T,
etc.
drag coeff
flight time
range
k 5 0.01
k 5 0.02
k 5 0.10
k 5 0.15
k 5 0.20
k 5 0.25
g
4
420
Section 10.5
Exploration 2
Graphing Rose Curves
4. (a) No; y is a function of x and is not the zero function.
All graphs are drawn in the window [24.7, 4.7] by [23.1, 3.1].
(b) No;
y(2x) 5 (2x)3 2 (2x) 5 2x 3 1 x 5 2(x 3 2 x) Þ y(x)
1. The graphs are rose curves with 4 petals when n 5 62,
8 petals when n 5 64, and 12 petals when n 5 66.
(c) Yes; y(2x) 5 2y(x) (see part (b))
5. (a) No; y is a function of x and is not the zero function.
(b) No; y(2x) 5 (2x)2 2 (2x) 5 x 2 1 x Þ y(x)
(c) No; y(2x) Þ 2y(x) (see part (b))
6. (a) No; y is a function of x and is not the zero function.
n 5 62
(b) Yes; y(2x) 5 cos (2x) 5 cos x 5 y(x)
(c) No; y(2x) Þ 2y(x) (see part (b))
7. (a) Yes; Substitute 2y for y in the equation to get the
original equation.
(b) Yes; Substitute 2x for x in the equation to get the
original equation.
n 5 64
n 5 66
(c) Yes; since the curve is symmetric with respect to both
the x-axis and y-axis, it is symmetric with respect to the
origin. (Also, substitute 2x for x and 2y for y in the
equation to get the original equation.)
8. Solve for y: y 5 (x 2 2)1/2 or 2(x 2 2)1/2.
Enter the first expression for Y1, the second for Y2.
1
4 2 x 2 1/2
4 2 x 2 1/2
or 2 }} .
3
3
2
1
9. Solve for y: y 5 }}
2. 2p
3. The graph is a rose curve with 2)n) petals.
4. The graphs are rose curves with 3 petals when n 5 63,
5 petals when n 5 65, and 7 petals when n 5 67.
2
Enter the first expression for Y1, the second for Y2.
10. (x 2 2 4x) 1 ( y 2 1 6y 1 9) 5 0
(x 2 2 4x 1 4) 1 (y 2 1 6y 1 9) 5 4
(x 2 2)2 1 (x 1 3)2 5 22.
Center 5 (2, 23), Radius 5 2.
Section 10.5 Exercises
For Exercises 1 and 2, two pairs of polar coordinates label
the same point if the r-coordinates are the same and the
u-coordinates differ by an even multiple of p, or if the
r-coordinates are opposites and the u-coordinates differ by
an odd multiple of p.
n 5 63
n 5 65
1. (a) and (e) are the same.
(b) and (g) are the same.
(c) and (h) are the same.
(d) and (f) are the same.
2. (a) and (f) are the same.
(b) and (h) are the same.
(c) and (g) are the same.
(d) and (e) are the same.
n 5 67
3.
5. p
6. The graph is a rose cuve with )n) petals.
Quick Review 10.5
21 2 4
3 2 (22)
1. Slope 5 }} 5 21,
so y 2 4 5 21[x 2 (22)] or y 5 2x 1 2.
2. (x 2 0)2 1 (y 2 0)2 5 32, or x 2 1 y 2 5 9.
3. [x 2 (22)]2 1 ( y 2 4)2 5 22, or (x 1 2)2 1 ( y 2 4)2 5 4.
[23, 3] by [22, 2]
1
p
4
p
4
2
(a) Ï2w cos }}, Ï2w sin }} = (1, 1)
(b) (1 cos 0, 1 sin 0) 5 (1, 0)
(c)
10 cos }2}, 0 sin }2}2 = (0, 0)
p
1
p
p
4
p
4
2
(d) 2Ï2w cos }}, 2Ï2w sin }} 5 (21, 21)
421
Section 10.5
6.
4.
[29, 9] by [26, 6]
[29, 9] by [26, 6]
5p
5p
3Ï3w
3
(a) 23 cos }}, 23 sin }} 5 }}, 2}}
1
1
6
1
6
1 3 22
4
2 1
2
2
1
2
21
(a) r 5 Ï(2
wÏ
w3ww
)2w
1w(2
w1ww
)2 5 2, tan u 5 }} 5 }}
2Ï3w
Ï3w
1 3 222 5 (3, 4)
4
1
1
7p
6
2
(b) 5 cos tan21 }} , 5 sin tan21 }}
with u in quadrant III. The coordinates are 2, }} .
(c) (21 cos 7p, 21 sin 7p) 5 (1, 0)
122, }6}2 also works, since r has the opposite sign and u
1
2p
3
2p
3
p
2
(d) 2Ï3w cos }}, 2Ï3w sin }} 5 (2Ï3w, 3)
differs by p.
5.
4
3
ww42w 5 5, tan u 5 }} with u in quadrant I.
(b) r 5 Ï3w2w1
1
4
3
21
4
3
The coordinates are 5, tan21 }} . 25, p 1 tan21 }}
2
also works, since r has the opposite sign and u differs
[26, 6] by [24, 4]
1
21
by p.
(a) r 5 Ï(2
w1ww
)2w
1w12w 5 Ï2w, tan u 5 }} 5 21 with u in
1
3p
4
2
0
2
(c) r 5 Ï0ww
1w(2
w2ww
)2 5 2, tan u 5 2}} is undefined with u
quadrant II. The coordinates are Ï2w, }} .
1Ï2w, 2}4}2 also works, since r is the same and u
5p
1
1
2
2
0
2
(d) r 5 Ï2w2w1
ww02w 5 2, tan u 5 }} 5 0 with u on the
2
u in quadrant IV. The coordinates are 2, 2}} .
1
positive x-axis. The coordinates are (2, 0). (2, 2p) also
2p
22, }} also works, since r has the opposite sign and
3
works, since r is the same and u differs by 2p.
u differs by p.
7.
(c) r 5 Ï0w2w1
ww32w 5 3, tan u 5 }3} is undefined with u on
0
p
5p
the positive y-axis. The coordinates are 3, }} . 3, }}
2
2
1 21
also works, since r is the same and u differs by 2p.
2
by 2p.
Ïw3
(b) r 5 Ï1w2w1
ww(2
wÏ
w3ww
)2 5 2, tan u 5 2}} 5 2Ï3w with
p
3
3p
2
p
2, 2}} also works, since r is the same and u differs
2
differs by 2p.
1
1
on the negative y-axis. The coordinates are 2, }} .
2
0
21
(d) r 5 Ï(2
w1ww
)2w
1w02w 5 1, tan u 5 }} 5 0 with u on the
[26, 6] by [24, 4]
8.
negative x-axis. The coordinates are (1, p). (21, 0) also
works, since r has the opposite sign and u differs by p.
[26, 6] by [24, 4]
9.
[23, 3] by [22, 2]
10.
[23, 3] by [22, 2]
422
Section 10.5
25. x 2 1 y 2 5 r 2 and y 5 r sin u, so the equation is
x 2 1 y 2 5 4y ⇒ x 2 1 (y 2 2)2 5 4, a circle
(center 5 (0, 2), radius 5 2).
11.
5
sin u 2 2 cos u
26. r 5 }}
[29, 9] by [26, 6]
12.
r sin u 2 2r cos u 5 5
x 5 r cos u and y 5 r sin u, so the equation is y 2 2x 5 5,
a line (slope 5 2, y-intercept 5 5).
27. r 2 sin 2u 5 2
[26, 6] by [24, 4]
13.
2r 2 sin u cos u 5 2
(r sin u)(r cos u) 5 1
x 5 r cos u and y 5 r sin u, so the equation is xy 5 1
1or, y 5 }x}2, a hyperbola.
1
[23, 3] by [22, 2]
14.
28. r 5 cot u csc u
r sin u 5 cot u
x
y
y 5 r sin u and }} 5 cot u, so the equation is y 2 5 x, a
[23, 3] by [22, 2]
15.
parabola.
29. r 5 csc u ercosu
r sin u 5 ercosu
x 5 r cos u and y 5 r sin u, so the equation is y 5 e x, the
exponential curve.
[23, 3] by [22, 2]
16.
[23, 3] by [22, 2]
17.
30. cos2 u 5 sin2 u
(r cos u)2 5 (r sin u)2
x 5 r cos u and y 5 r sin u, so the equation is x 2 5 y 2 or
y 5 6x, the union of two lines.
31. r sin u 5 ln r 1 ln cos u
r sin u 5 ln (r cos u)
y 5 ln x, the logarithmic curve.
32. r 2 1 2r 2 cos u sin u 5 1
r 2 1 2(r cos u)(r sin u) 5 1
x 2 1 y 2 1 2xy 5 1
(x 1 y)2 5 1
x 1 y 5 61, the union of two lines.
[21.8, 1.8] by [21.2, 1.2]
18.
[23, 3] by [22, 2]
19. y 5 r sin u, so the equation is y 5 0, which is the x-axis.
20. x 5 r cos u, so the equation is x 5 0, which is the y-axis.
21. r 5 4 csc u
r sin u 5 4
y 5 r sin u, so the equation is y 5 4, a horizontal line.
22. r 5 23 sec u
r cos u 5 23
x 5 r cos u, so the equation is x 5 23, a vertical line.
23. x 5 r cos u and y 5 r sin u, so the equation is x 1 y 5 1, a
line (slope 5 21, y-intercept 5 1).
24. x 2 1 y 2 5 r 2, so the equation is x 2 1 y 2 5 1, a circle
(center 5 (0, 0), radius 5 1).
33. r 2 5 24r cos u
x 2 1 y 2 5 24x
(x 1 2)2 1 y 2 5 4, a circle (center 5 (22, 0), radius 5 2).
34. r 5 8 sin u
r 2 5 8r sin u
x 2 1 y 2 5 8y
x2 1 ( y 2 4)2 5 16, a circle (center 5 (0, 4), radius 5 4).
35. r 5 2 cos u 1 2 sin u
r 2 5 2r cos u 1 2r sin u
x 2 1 y 2 5 2x 1 2y
(x 2 1)2 1 (y 2 1)2 5 2,
a circle (center 5 (1, 1), radius 5 Ï2w).
Section 10.5
1
2
42. x 2 2 y 2 5 1
r 2 cos2 u 2 r 2 sin2 u 5 1
r 2(cos2 u 2 sin2 u) 5 1
p
6
p
p
r sin u cos }} 1 cos u sin }} 5 2
6
6
Ï3w
1
}}r sin u 1 }}r cos u 5 2
2
2
Ï3w
1
}}y 1 }}x 5 2
2
2
36. r sin u 1 }} 5 2
1
2
1
1
4
2
x 1 Ï3wy 5 4, a line slope 5 2}}, y-intercept 5 }} .
Ï3w
Ï3w
37. x 5 7
r cos u 5 7. The graph is a vertical line.
[24.7, 4.7] by [23.1, 3.1]
x2
y2
9
4
r 2 cos2 u
r 2 sin2 u
}} 1 }} 5 1
9
4
43. }} 1 }} 5 1
r 2(4 cos2 u 1 9 sin2 u) 5 36
[29.4, 9.4] by [26.2, 6.2]
38. y 5 1
r sin u 5 1
The graph is a horiztonal line.
[24.7, 4.7] by [23.1, 3.1]
44. xy 5 2
(r cos u)(r sin u) 5 2
r 2 cos u sin u 5 2
r 2 2 cos u sin u 5 4
r 2 sin 2u 5 4
[24.7, 4.7] by [23.1, 3.1]
p
4
39. x 5 y ⇒ r cos u 5 r sin u ⇒ tan u 5 1 ⇒ u 5 }}
p
4
More generally, u 5 }} 1 2kp for any integer k.
The graph is a slanted line.
[24.7, 4.7] by [23.1, 3.1]
45. y 2 5 4x
r 2 sin2 u 5 4r cos u
r sin2 u 5 4 cos u
[24.7, 4.7] by [23.1, 3.1]
40. x 2 y 5 3
r cos u 2 r sin u 5 3
[24.7, 4.7] by [23.1, 3.1]
46. x 2 1 xy 1 y 2 5 1
(r cos u)2 1 (r cos u)(r sin u) 1 (r sin u)2 5 1
r 2(1 1 cos u sin u) 5 1
[29.4, 9.4] by [26.2, 6.2]
41. x 2 1 y 2 5 4
r 2 5 4 or r 5 2 (or r 5 22)
[23, 3] by [22, 2]
[24.7, 4.7] by [23.1, 3.1]
423
424
Section 10.5
47. x 2 1 ( y 2 2)2 5 4
r 2 cos2 u 1 (r sin u 2 2)2 5 4
r 2 cos2 u 1 r 2 sin2 u 2 4r sin u 1 4 5 4
r 2 2 4r sin u 5 0
r 5 4 sin u.
The graph is a circle centered at (0, 2) with radius 2.
52. (a)
[23, 3] by [22, 2]
(b) Length of interval 5 2p
53. (a)
[24.7, 4.7] by [21.1, 5.1]
[23.75, 3.75] by [22, 3]
48. (x 2 3)2 1 (y 1 1)2 5 4
(b) Length of interval 5 2p
(r cos u 2 3)2 1 (r sin u 1 1)2 5 4
54. (a)
r 2 cos2 u 2 6r cos u 1 9 1 r 2 sin2 u 1 2r sin u 1 1 5 4
r 2 2 6r cos u 1 2r sin u 1 6 5 0
6 cos u 2 2 sin u 6 Ï(6
wwcowswuww
2w
2wsin
wwu)w2w
2w24
w
r 5 }}}}}
2
r 5 3 cos u 2 sin u 6 Ï(3
wwcowswuww
2wsin
wwuw
)2w
2w
6
[21.5, 1.5] by [21, 1]
(b) Length of interval 5 4p
55. (a)
[215, 15] by [210, 10]
(b) Required interval 5 (2`, `)
[26, 6] by [24, 4]
In Exercises 49–58, find the minimum u-interval by trying
different intervals on a graphing calculator.
56. (a)
49. (a)
[23, 3] by [22, 2]
(b) Length of interval 5 2p
57. (a)
[23, 3] by [22, 2]
(b) Length of interval 5 2p
50. (a)
[23, 3] by [22, 2]
(b) Length of interval 5 p
58. (a)
[26, 6] by [24, 4]
(b) Length of interval 5 2p
51. (a)
[23, 3] by [21, 3]
(b) Length of interval 5 2p
[21.5, 1.5] by [21, 1]
p
2
(b) Length of interval 5 }}
59. If (r, u) is a solution, so is (2r, u). Therefore, the curve is
symmetric about the origin. And if (r, u) is a solution, so is
(r, 2u). Therefore, the curve is symmetric about the x-axis.
And since any curve with x-axis and origin symmetry also
has y-axis symmetry, the curve is symmetric about the
y-axis.
60. If (r, u) is a solution, so is (2r, u). Therefore, the curve is
symmetric about the origin. The curve does not have x-axis
or y-axis symmetry.
Section 10.5
61. If (r, u) is a solution, so is (r, p 2 u). Therefore, the curve
is symmetric about the y-axis. The curve does not have
x-axis or origin symmetry.
62. If (r, u) is a solution, so is (2r, u). Therefore, the curve is
symmetric about the origin. And if (r, u) is a solution, so is
(r, 2u). Therefore, the curve is symmetric about the x-axis.
And since any curve with x-axis and origin symmetry also
has y-axis symmetry, the curve is symmetric about the
y-axis.
63. (a) Because r 5 a sec u is equivalent to r cos u 5 a, which
is equivalent to the Cartesian equation x 5 a.
425
66. (a)
[29, 9] by [26, 6]
The graph of r2 is the graph of r1 rotated by angle a
counterclockwise about the origin.
(b)
(b) r 5 a csc u is equivalent to y 5 a.
64. (a) The graph is the same for n 5 2 and n 5 22, and in
general, it’s the same for n 5 2k and
n 5 22k. The graphs for n 5 2, 4, and 6 are roses with
4, 8, and 12 “petals” respectively.
The graphs for n 5 62 and n 5 66 are shown below.
n 5 62
[29, 9] by [26, 6]
The graph of r2 is the graph of r1 rotated by angle 2a
clockwise about the origin.
(c) The graph of r2 is the graph of r1 rotated
counterclockwise about the origin by the
angle a.
67. d 5 Ï(x
ww
wwxw
2
)2w1
ww( w
y1w
2wyw
)2w
2
1
2
5 [(r2 cos u2 2 r1 cos u1)2 1 (r2 sin u2 2 r1 sin u1)2]1/2
[23, 3] by [22, 2]
n 5 66
5 [r22 cos2 u2 2 2r2 r1 cos u2 cos u1 1 r12 cos2 u1
1 r22 sin2 u2 2 2r2r1 sin u2 sin u1 1 r12 sin2 u1]1/2
2
5 Ïw
r12w1
wwrw
w
2w2w
r1w
r2wcowsw(u
ww
wwuw
2
)
2
1
2
[23, 3] by [22, 2]
68. (a)
(b) 2p
(c) The graph is a rose with 2)n) “petals”.
(d) The graphs are roses with 3, 5, and 7 “petals”
respectively. The “center petal” points upward if
n 5 23, 15, or 27.
The graphs for n 5 3 and n 5 23 are shown below.
[29, 9] by [26, 6]
The graphs are ellipses.
(b) Graphs for 0 , k , 1 are ellipses. As k → 01, the
graph approaches the circle of radius 2 centered at the
origin.
69. (a)
[23, 3] by [22, 2]
[25, 25] by [210, 10]
The graphs are hyperbolas.
[23, 3] by [22, 2]
(e) p
(f) The graph is a rose with )n) “petals”.
65. (a) We have x 5 r cos u and y 5 r sin u. By taking t 5 u,
we have r 5 f (t), so x 5 f (t) cos t and y 5 f (t) sin t.
(b) x 5 3 cos t, y 5 3 sin t
(c) x 5 (1 2 cos t) cos t, y 5 (1 2 cos t) sin t
(d) x 5 (3 sin 2t) cos t, y 5 (3 sin 2t) sin t
(b) Graphs for k . 1 are hyperbolas. As k → 11, the right
branch of the hyperbola goes to infinity and
“disappears”. The left branch approaches the parabola
y 2 5 4 2 4x.
426
Section 10.6
Section 10.6 Exercises
70. (a)
f 9(u ) sin u 1 f (u ) cos u
f 9(u ) cos u 2 f (u ) sin u
dy
dx
1. }} 5 }}}
cos u sin u 1 (21 1 sin u)cos u
cos u cos u 2 (21 1 sin u)sin u
5 }}}}
[29, 9] by [26, 6]
The graphs are parabolas.
(b) As k → 01, the limit of the graph is the negative x-axis.
2 sin u cos u 2 cos u
5 }}}
2
2
cos u 2 sin u 1 sin u
■ Section 10.6 Calculus of Polar Curves
(pp. 559–568)
)
)
dy
1
dy
1
5 2}} 5 21, }}
5 }} 5 1
}}
dx u50
1
dx u5p
1
f9(u) sin u 1 f (u) cos u
dy
dx
dy
dy/dt
5
5 cos t
dx
dx/dt
3
23 sin t
5
2. 2}} cot 2 < 0.763
3
p
3p
3. Solve cot t 5 0: t 5 }} or }};
2
2
1. }} 5 }} 5 }} 5 2}}cot t
)
1
2
)
dy
1
5 2}}, which is undefined.
dx u5p
0
and }}
1
3p
3p
and 3 cos }}, 5 sin }} 5 (0, 25)
2
2
p
2
p
2
2
f9(u) sin u 1 f (u) cos u
dy
dx
3. }} 5 }}}
f9(u) cos u 2 f (u) sin u
23 cos u sin u 1 (2 2 3 sin u) cos u
5 }}}}
23 cos u cos u 2 (2 2 3 sin u) sin u
5
3
4. 2}} cot t is undefined when t 5 0, p, or 2p;
2 cos u 2 6 sin u cos u
22 sin u 2 3(cos u 2 sin u)
the corrresponding points are
5 }}}}
2
2
(3 cos 0, 5 sin 0) 5 (3 cos 2p, 5 sin 2p) 5 (3, 0) and
(3 cos p, 5 sin p) 5 (23, 0).
dx 2
dy 2
}} 1 } } dt
dt
dt
0
p
2
)
)
)
dy
dy
22
2
5 }}
5 }} 5 2}},
}}
dx (2, 0)
dx u50
3
3
)
dy
dy
0
5 }}
5 }} 5 0,
}}
dx (21, p/2)
dx u5p/2
21
E !§1 §§2§§§1§§2§
wwtw1
ww25wwcoww
s wt dt,
5 E Ï9wwsin
5. Length 5
)
dy
1
dy
0
5 }}, which is undefined; }}
5 6}} 5 0;
}}
dx u50
0
dx u56p/2
1
the corresponding points are 3 cos }}, 5 sin }} 5 (0, 5)
p
22 sin 2u sin u 1 cos 2u cos u
}}}} .
2. }} 5 }}}
f9(u) cos u 2 f (u) sin u 5 22 sin 2u cos u 2 cos 2u sin u
Quick Review 10.6
)
)
dy
dy
2
5 }}
5 }}, and
}}
dx (2, p)
dx u5p
3
2
0
which using NINT evaluates to < 12.763.
)
)
dy
dy
0
5 }}
5 }} 5 0.
}}
dx (5, 3p/2)
dx u53p/2
25
For questions 6–8, the graph is:
f9(u) sin u 1 f (u) cos u
f9(u) cos u 2 f (u) sin u
dy
dx
4. }} 5 }}}
3 sin2 u 1 3 cos u(1 2 cos u)
3 sin u cos u 2 3 sin u(1 2 cos u)
5 }}}}
3 cos u 2 3(cos2 u 2 sin2 u)
6 sin u cos u 2 3 sin u
5 }}}
[22, 4] by [22, 2]
6. The upper half of the outer loop
)
7. The inner loop
dy
5
}}
dx (1.5, p/3)
8. The lower half of the outer loop
9. y 5 0 for x 5 0 or 6.
Area 5
E (6x 2 x ) dx 5 33x
6
0
2
2
1
3
40 5 36
2 }}x 3
6
10. Use a graphing calculator’s intersect function to find that
the curves cross at x < 0.270 and x < 2.248, then use
NINT to find
Area 5
E
2.248
0.270
[2 sin x 2 (x 2 2 2x 1 1)] dx < 2.403.
)
1 2
1
1
}} 2 2}}
2
2
}} ,
Ïw3 Ï3w
} } 2 }}
2
2
dy
5
}}
dx (4.5, 2p/3)
which is undefined;
1 2
1
1
2
2
}}
Ï3w Ï3w
2}} 2 }}
2
2
2}} 2 2}}
5 0;
)
dy
21 2 1
5 }}, which is undefined; and
}}
dx (6, p)
020
)
dy
0 2 (21)
5 }} 5 1.
}}
dx (3, 3p/2)
0 2 (21)
Section 10.6
427
7.
5.
[23.8, 3.8] by [22.5, 2.5]
[21.5, 1.5] by [21, 1]
The graph passes through the pole when r 5 3 cos u 5 0,
p
2
1
only consider u 5 }}. At this point, there appears to be a
1
p
2
vertical tangent line with equation u 5 }} (or x 5 0).
Confirm analytically:
x 5 (3 cos u) cos u 5 3 cos2 u
y 5 (3 cos u) sin u
dy
}} 5 (23 sin u)sin u 1 (3 cos u)cos u 5 3(cos2 u 2 sin2 u)
du
dx
and }} 5 6 cos u(2sin u).
du
p
dx
5 0, and
At 0, }} , }}
2
du u5p/2
p dx
dy
5 3(02 2 12) 5 23. So at 0, }} , }} 5 0
}}
2 du
du u5p/2
dy
dy
and }} Þ 0, so }} is undefined and the tangent line is
dx
du
1 2 )
)
3 1 24
3 1 24
3 1 24
3 1 24
8.
[23, 3] by [22, 2]
1
kp
2
2
The polar solutions are 0, }} for k 5 0, 1, 2, 3, 4, and for
6.
kp
a given k, the line u 5 }} appears to be tangent to the
2
kp
curve at 0, }} . This can be confirmed analytically by
2
dy
noting that the slope of the curve, }}, equals the slope of
dx
kp
the line, tan }}. So the tangent lines are u 5 0 [y 5 0] and
2
p
3p
u 5 }} [x 5 0]. u 5 p, u 5 }} and u 5 2p are duplicate
2
2
1
[23, 3] by [22, 2]
A trace of the graph suggests three tangent lines, one with
p
p
positive slope for u 5 }}, a vertical one for u 5 }}, and one
6
2
5p
with negative slope for u 5 }}.
6
Confirm analytically:
dy
}} 5 26 sin 3u sin u 1 2 cos 3u cos u and
du
dx
}} 5 26 sin 3u cos u 2 2 cos 3u sin u.
du
10, }6}2, 10, }2}2, and 10, }6}2 are all solutions.
p
p
5p
dy
dy/du
}} 5 }}, and so
dx
dx/du
26(1)(1/2) 1 2(0)(Ï3
w/2)
dy
1
5 }}} 5 }};
}}
26(1)(Ïw
3/2) 2 2(0)(1/2)
dx u5p/6
Ï3w
26(21)(1) 1 2(0)(0)
dy
5 }}} , which is undefined; and
}}
26(21)(0) 2 2(0)(1)
dx u5p/2
u55p/6
2
1 2
vertical.
)
)
dy
}})
dx
2
kp
a given k, the line u 5 }} appears to be tangent to the
5
kp
curve at 0, }} . This can be confirmed analytically by
5
dy
noting that the slope of the curve, }}, equals the slope of
dx
kp
the line, tan }}. So the tangent lines are u 5 0 [y 5 0],
5
p
p
2p
2p
u 5 }} y 5 tan }} x , u 5 }} y 5 tan }} x ,
5
5
5
5
3p
3p
4p
4p
u 5 }} y 5 tan }} x , and u 5 }} y 5 tan }} x .
5
5
5
5
u-interval 0 # p # 1 produces the entire graph, we need
p
2
kp
5
The polar solutions are 0, }} for k 5 0, 1, 2, 3, 4, and for
3p
2
which occurs when u 5 }} and when u 5 }}. Since the
26(1)(1/2) 1 2(0)(2Ï3
w/2)
1
5 }}} 5 2}}. The tangent
26(1)(2Ï3
w/2) 2 2(0)(1/2)
Ïw3
p
3
1
4
p
lines have equations u 5 }} y 5 }}x , u 5 }} [x 5 0],
6
2
Ïw3
5p
3
1
4
and u 5 }} y 5 2}}x .
6
Ï3w
2
solutions.
2
1
428
Section 10.6
dy
du
dy
du
9. }} 5 cos u sin u 1 (21 1 sin u)cos u
10. }} 5 2sin2 u 1 (1 1 cos u)cos u
5 cos2 u 1 cos u 2 sin2 u
5 cos u(2 sin u 2 1)
5 2 cos2 u 1 cos u 2 1
5 sin 2u 2 cos u
dx
}} 5 2sin u cos u 2 (1 1 cos u)sin u
du
dx
}} 5 cos2 u 2 (21 1 sin u)sin u
du
5 2sin u(1 1 2 cos u)
5 cos u 1 sin u 2 sin u
2
2
5 2sin 2u 2 sin u
21 6 Ïw
9
1
dy
}} 5 0 when cos u 5 }} 5 21 or }}, i.e., when
4
2
du
p
5p dx
u 5 p, }} or }}. }} 5 0 when u 5 0, p, 2p
3
3 du
2p 4p
(then sin u 5 0) or when u 5 }}, }}
3 3
5 22 sin2 u 1 sin u 1 1
p 3p
dy
}} 5 0 when u 5 }}, }} (cos u 5 0) or when
2 2
du
p 5p
dx
u 5 }}, }} (2 sin u 2 1 5 0). }} 5 0 when
6 6
du
21 6 Ï9w
1
7p 11p
sin u 5 }} 5 2}} or 1, i.e., when u 5 }}, }}, or
24
2
6
6
p
3p
}}. So there is a horizontal tangent line for u 5 }}, r 5 22
2
2
3the line y 5 22 sin }2} 5 24, for u 5 }6}, r 5 2}2}
1
p
1
5p
1
3the line y 5 2}2}sin }6} 5 2}4}4 and for u 5 }6}, r 5 2}2}
1
5p
1
3again, the line y 5 2}2} sin }6} 5 2}4}4.
3p
p
7p
6
1
3
2
There is a vertical tangent line for u 5 }}, r 5 2}}
3Ï3w
3the line x 5 2}2} cos }6} 5 }4}4 and for
11p
3
3
11p
3Ïw3
u 5 }}, r 5 2}} 3the line x 5 2}} cos }} 5 2}}4.
6
2
2
6
4
7p
3
p dy
2 du
dx
du
For u 5 }}, }} 5 }} 5 0, but
1 2
1 2
(then 1 1 2 cos u 5 0). So there is a horizontal tangent line
p
3
3
p
3Ï3w
for u 5 }}, r 5 }} the line y 5 }} sin }} 5 }} and for
3
2
3
2
3
4
4
5p
3
3
5p
3Ïw3
u 5 }}, r 5 }} the line y 5 }} sin }} 5 2}} . There is a
3
3
2
2
3
4
vertical tangent line for u 5 0, r 5 2
4
[the line x 5 2 cos 0 5 2], for u 5 2p, r 5 2 [again, the
2p
3
1
2
line x 5 2 cos 2p 5 2], for u 5 }}, r 5 }}
2p
1
4p
1
3
4
3
2
1
2p
1
again, the line x 5 }} cos }} 5 2}} .
2
3
4
dy
dx
For u 5 p, }} 5 }} 5 0, but
du
du
d dy
}} }} 5 24 cos u sin u 2 sin u 5 0 for u 5 p, and
du du
d dx
}} }} 5 22 cos 2u 2 cos u 5 21 for u 5 p,
du du
dy
so by L’Hôpital’s rule }} 5 0 and the tangent line is horidx
1
2
[the line x 5 }} cos }} 5 2}}] and for u 5 }}, r 5 }}
3
4
1 2
1 2
p
d dy
}} }} 5 2 cos 2u 1 sin u 5 21 for u 5 }} and
2
du du
p
d dx
}} }} 5 24 sin u cos u 1 cos u 5 0 for u 5 }}, so by
2
du du
zontal at u 5 p, r 5 0 [the line y 5 0].
dy
L’Hôpital’s rule }} is undefined and the tangent line is
dx
This information can be summarized as follows.
p
vertical at u 5 }}, r 5 0 [the line x 5 0].
2
Horizontal at: }}, }}
3 p
This information can be summarized as follows.
1 p
1 2 6 2 3y 5 2}4}4,
1 5p
1
12}2}, }6}2 3y 5 2}4}4,
3p
122, }2}2 3y 5 24
p
10, }2}2 [x 5 0],
3 7p
3Ï3w
12}2}, }6}2 3x 5 }4}4,
3 11p
3Ïw3
12}2}, }6}2 3x 5 2}4}4
Horizontal at: 2}}, }}
Vertical at:
3Ïw3
1 2 3 2 3y 5 }4}4,
(0, p) [y 5 0],
3 5p
1
3Ï3w
1}2}, }3}2 3y 5 2}4}4
Vertical at:
(2, 0) [x 5 2],
1 2p
1}2}, }3}2 3x 5 2}4}4,
1 4p
1
1}2}, }3}2 3x 5 2}4}4,
(2, 2p) [x 5 2]
1
Section 10.6
11. y 5 2 sin2 u
dy
du
12. }} 5 4 sin2 u 1 (3 2 4 cos u)cos u
dy
}} 5 4 sin u cos u
du
5 4(sin2 u 2 cos2 u) 1 3 cos u
5 2 sin 2u
5 28 cos2 u 1 3 cos u 1 4
x 5 2 sin u cos u
dx
}} 5 4 sin u cos u 2 (3 2 4 cos u)sin u
du
5 sin 2u
5 sin u(8 cos u 2 3)
dy
}} 5 2 cos 2u
du
p
dy
dx
}} 5 0 when u 5 0, }}, p, and }} 5 0 when
2
du
du
p 3p
u 5 }}, }}. They are never both zero.
4 4
p
For u 5 0, }}, p the curve has horizontal asymptotes
2
p
p
at (0, 0) [y 5 0 sin 0 5 0], 2, }} y 5 2 sin }} 5 2 , and
2
2
p 3p
(0, p) [ y 5 0 sin p 5 0]. For u 5 }}, }} the curve has
4 4
p
p
vertical asymptotes at Ï2w, }} [x 5 Ï2w cos }} 5 1] and
4
4
Ï2w, }3p} x 5 Ï2w cos }3p} 5 21 .
4
4
1 23
1
1
23
2
4
4
5 4 sin 2u 2 3 sin u
23 6 Ïw1w
3w
7
dy
}} 5 0 when cos u 5 }}, i.e., when
216
du
u < 0.405, 2.146, 4.137, or 5.878 (values solved for with a
dx
du
graphing calculator). }} 5 0 when u 5 0, p or 2p
182
3
(then sin u 5 0) or when u 5 cos21 }} < 1.186 or
182
3
2p 2 cos21 }} < 5.097 (then 8 cos u 2 3 5 0). So there
is a horizontal tangent line for u < 0.405, r < 20.676
[the line y < 20.676 sin 0.405 < 20.267], for u < 2.146,
This information can be summarized as follows.
r < 5.176 [the line y < 5.176 sin 2.146 < 4.343], for
Horizontal at: (0, 0) [y 5 0],
u < 4.137, r < 5.176
p
12, }2}2
[y 5 2],
(0, p) [y 5 0]
Vertical at:
429
p
1Ï2w, }4}2 [x 5 1],
3p
1Ï2w, }4}2 [x 5 21]
[the line y < 5.176 sin 4.137 < 24.343], and for
u < 5.878, r < 20.676
[the line y < 20.676 sin 5.878 < 0.267]. There is a vertical
tangent for u 5 0, r 5 21 [the line x 5 21 cos 0 5 21],
for u 5 p, r 5 7 [the line x 5 7 cos p 5 27], for u 5 2p,
r 5 21 [again, the line x 5 21 cos 2p 5 21], for
182
3
3
2
3
9
16
4
u 5 cos21 }} , r 5 }} the line x 5 }} , and for
u 5 2p 2 cos
21
12
3
This information can be summarized as follows.
Horizontal at: (20.676, 0.405) [y < 20.267],
(5.176, 2.146) [y < 4.343],
(5.176, 4.137) [y < 24.343],
(20.676, 5.878) [y < 0.267]
Vertical at:
4
3
3
9
}} , r 5 }} again, the line x 5 }} .
8
2
16
(21, 0) [x 5 21],
(1.5, 1.186)
3x 5 }1}6 4,
9
(7, p) [x 5 27],
(1.5, 5.097)
3x 5 }1}6 4,
9
(21, 2p) [x 5 21]
430
Section 10.6
13. The curve is complete for 0 # u # 2p (as can be verified
19.
by graphing). The area is
E
2p
0
1
}}(4 1 2 cos u)2 du
2
E (4 1 4 cos u 1 cos u) du
1
1
5 2 4u 1 4 sin u 1 }}u 1 }} sin 2u
3
4
2
4
52
2p
[22.5, 5.2] by [22, 3.1]
2
0
2p
The circles intersect at (x, y) coordinates (0, 0) and
5 18p
0
(1, 1). The area shared is twice the area inside the
p
4
14. The curve is complete for 0 # u # 2p (as can be verified
circle r 5 2 sin u between u 5 0 and u 5 }}.
by graphing). The area is
E
1
}}a2(1 1 cos u)2 du
0 2
2p
1
5 }}a2 (1 1 2 cos u 1 cos2 u) du
2 0
1
1
1
5 }}a2 u 1 2 sin u 1 }}u 1 }} sin 2u
2
2
4
E
3
5
2p
4
3
2
5 }}pa2
0
p
4
2}} # u # }}. The total area is
E
p/4
E cos 2u du
1
5 2a }} sin 2u
32 4
1
2
waw2wco
wsw2wuw )2 du 5 2a2
}}(Ï2
2p/4 2
p/4
p/4
2p/4
1
}}(2 sin u)2 du
2
0
E
p/4
0
4 sin2 u du
32
1
4
1
2
1
5 4 }}u 2 }} sin 2u
15. Use r 5 Ï2waw2wco
wsw2wuw. One lobe is complete for
p
4
E
Shared area 5 2
2p
4
p/4
0
p
1
p
5 4 }} 2 }} 5 }} 2 1.
8
4
2
20.
p/4
2
2p/4
5 2a2
(Integrating from 0 to 2p will not work, because r is not
defined over the entire interval.)
p
4
p
4
p/4
1
1
1
}} cos2 2u du 5 }}u 1 }} sin 4u
4
16
2p/4 2
[23, 3] by [22, 2]
p
E
54E
16. One leaf covers 2}} # u # }}. Its area is
E
3
p/4
4
2p/4
p/6
is 2
p
5 }}.
8
E
5 2cos 2u
3
4
p/2
1
}}(2 sin u)2 du 1 2
2
p/6
sin2 u du 1
32
1
1
4
Ï3w
2p
5 }} 2 }}
3
2
5 4 }}u 2 }} sin 2u
5 2.
0
0
0
17. Use r 5 Ï4wwsin
ww2wu. One loop is complete for 0 # u # }p}.
2
p/2
p/2
1
Its area is
wwsin
ww2uw)2 du5
2 sin 2u du
}}(Ï4
2
0
0
E
1 62
1
5p
6
2
The circles intersect at 1, }} and 1, }} . The shared area
4
E
E
p/2
p/6
1
}}(1)2 du
2
p/2
p/6
p/6
0
du
34
1 u
p/2
Ïw3
p
p
5 }} 2 }} 1 }}
13
p/6
2
2
3
21.
18. Use r 5 Ï2wwsin
ww3wu. One leaf is complete for 0 # u # }p}.
3
The total area is
E
p/3
6
0
E sin 3u du
5 2 2cos 3u
3
4 5 4.
1
wwsin
ww3uw)2 du 5 6
}}(Ï2
2
p/3
0
p/3
0
[24.7, 4.7] by [23.1, 3.1]
The shared area is half the circle plus two lobelike regions:
1
}}p(2)2 1 2
2
E
p/2
0
p/2
1
}}[2(1 2 cos u)]2 du
2
E (4 2 8 cos u 1 4 cos u) du
1
1
5 2p 1 4 u 2 2 sin u 1 }}u 1 }} sin 2u
3
4
2
4
5 2p 1
0
5 5p 2 8
2
p/2
0
Section 10.6
22.
431
25.
[24.7, 4.7] by [23.1, 3.1]
[26, 6] by [24, 4]
The area in question is half the circle minus two lobelike
regions:
Use the symmetries of the graphs: the shared area is
E
p/2
1
}}[2(1 2 cos u)]2 du
2
p/2
4
1
}}p(2)2 2 2
2
E (1 2 2 cos u 1 cos u) du
1
1
5 8 u 2 2 sin u 1 }}u 1 }} sin 2u
3
4
2
4
0
58
2
0
p/2
E
p/2
0
p/2
1
}}[2(1 2 sin u)]2 du
2
E (4 2 8 sin u 1 4 sin u) du
1
1
5 2p 2 4 u 1 2 cos u 1 }}u 2 }} sin 2u
3
4
2
4
5 2p 2
5 6p 2 16
0
23. For a 5 1:
2
0
p/2
582p
0
26.
[23, 3] by [22, 2]
[23, 3] by [22, 2]
(a) To find the integration limits, solve
The curves intersect at the origin and when
2 cos u 1 1 5 0
3a cos u 5 a(1 1 cos u)
u 5 6 }} .
2 cos u 5 1
Because of the curve’s symmetry, the area inside the
outer loop is
2p
3
p
3
u 5 6}}.
2p/3
Use the symmetries of the curves: the area in question is
E
p/3
0
E (9 cos u 2 1 2 2 cos u 2 cos u) du
5 a E (8 cos u 2 2 cos u 2 1) du
5 a 4u 1 2 sin 2u 2 2 sin u 2 u
3
4 5a p
p/3
5 a2
0
p/3
2
2
2
2
0
p/3
2
0
5
1
}}[(3a cos u)2 2 a 2(1 1 cos u)2] du
2
2
E
2
2
0
E
1
}}(2 cos u 1 1)2 du
2
2p/3
(4 cos2 u 1 4 cos u 1 1) du
0
3
5 2u 1 sin 2u 1 4 sin u 1 u
3Ïw3
5 }} 1 2p
2
E
p
2
3
The curves intersect when
6 cos 2u 5 3
5p
6
u 5 6}} or 6}}.
Use the symmetries of the curves. The area in question is
p/6
0
4
p
2p/3
3Ï3w
5 p 2 }}.
2
Subtract this from the answer in (a) to get 3Ï3w 1 p.
[23, 3] by [22, 2]
E
0
1
}}(2 cos u 1 1)2 du
2p/3 2
5 2u 1 sin 2u 1 4 sin u 1 u
4
2p/3
(b) Again, use the curve’s symmetry. The inner loop’s area
is
24.
p
6
4
3
1
}}(6 cos 2u 2 3) du 5 6 sin 2u 2 u
2
4
p/6
0
5 3Ï3w 2 p.
432
Section 10.6
30. The integral given is incorrect because r 5 cos u sweeps
27.
out the circle twice as u goes from 0 to 2p. Or, you can’t
use equation (2) from the text on the interval [0, 2p]
because r 5 cos u is negative for
[29, 9] by [26, 6]
p
3p
5p
}} , u , }}. The correct area is }}, which can be found
2
2
4
3p
p
by computing the areas of the cardioid }} and the circle }}
2
4
To find the integration limits, solve
3 csc u 5 6
separately and subtracting.
p 5p
6 6
5p/6
1
}}(62 2 32 csc2 u) du
p/6 2
5p/6
1
5 }} 36u 1 9 cot u
2
p/6
u 5 }}, }}. The area in question is
E
3
dr
du
31. }} 5 2u, so
4
E
5E
Length 5
Ï5
w
Ï(u
w2w)2w1
ww(2wuww
)2 du
0
5 12p 2 9Ï3w
28.
Ï5
w
uÏuw2w1
ww4 du
0
33
4
1
5 }}(u2 1 4)3/2
Ï5w
0
1
19
5 }}(27 2 8) 5 }}
3
3
[23, 3] by [-2, 2]
dr
E !§1}§Ïe}§2w §2 §1§1}§Ïe}§2w §2 du
5 E e du
9
4
Length 5
6 cos 2u 5 }} sec2 u
48 cos4 u 2 24 cos2 u 2 9 5 0
E 1
3
2
1
9
2
}} 6 cos 2u 2 }} sec2 u du
2
4 p/6
0
9
3Ïw3
5 3 sin 2u 2 }} tan u
5 }}.
4
4
0
4
dr
du
p/2
p/2
0
p/4
3
2
p
4
2p
sin2 u
cos u
y 5 tan u sin u ⇒ y 5 }}
x 5 21,
lim 2 x 5 1,
u→p/2
lim
u→2p/21
y5`
lim 2 y 5 `
u→p/2
2
2
0
p
0
p
3 1 2 24
u
5 8 sin }}
58
0
122 122
u
u
u
Length 5 E a sin 1}}2 1 a sin 1}}2 cos 1}}2 du
!§§§§§§§2 §§§§§§§§§2 §§§§§2 §
u
5 aE
!si§n§§1}§2}2§ du
u
dr
du
u
34. }} 5 a sin }} cos }} , so
p
(b) Yes. x 5 tan u cos u ⇒ x 5 sin u
2
0
2p
0
2p
2
p/4
5 ep 2 1
0
0
2p
p/4
Total area is twice that, or }} 2 }}.
lim
p
E Ï(1ww1wcowswuww) w1w(2wsiwnwwuw) du
1w2wcowswuw du,
5 E Ï2ww
u
5E
!2§§1§4§co§s§§1}§2}2§2§§2 du
u
5 E 2)cos 1}}2) du
2
u
5 4E cos 1}}2 du
2
Length 5
E }12}1}12} csc u2 du
1
1
5 }}3tan u 2 u4 1 }}32cot u4
2
4
1
p
1
3
p
5 }}11 2 }}2 1 }}(0 1 1) 5 }} 2 }}.
2
4
4
4
8
1
}} tan2 u du 1
2
u→2p/21
2
33. }} 5 2sin u, so
29. (a) Find the area of the right half in two parts, then double
the result: Right half area
0
u
2
u
3 4
p/6
p/4
u
5 eu
By the symmetry of the curves, the area in question is
E
p
0
p
0
3
cos u 5 }}
4
p
u 5 6}}.
6
2
5
eu
32. }} 5 }}, so
du
Ï2w
To find the intersection points, solve
2
4
2
0
p
2
0
3
p
1 2 24
u
5 2a 2cos }}
0
5 2a
2
2
433
Section 10.6
6 sin u
(1 1 cos u)
dr
du
41.
35. }} 5 }}2 , so
6
6 sin u
E !}
} du, which using
§(1§1§c}
§o§s §u)§1§§}
os§u§
(§
1§
1§c§
)
p/2
Length 5
2
2
2
2
0
4
NINT evaluates to < 6.887.
[21.5, 1.5] by [21, 1]
3 u
122
(Note: the integrand can simplify to 3 sec }} .)
dr
du
2r }} 5 22 sin 2u
2sin 2u
dr
}} 5 }}.
du
s w2wu
Ïcwow
dr
2 sin u
36. }} 5 2}}2 , so
du
(1 2 cos u)
Use the curve’s symmetry and note that r is defined for
E !§§§§§§§§§§§§§§§
p
Length 5
22
22 sin2 u
}}2 1 }}4 du, which using
(1 2 cos u)
(1 2 cos u)
p/2
u
(Note: the integrand can simplify to csc3 }} ).
2
12
u
4
2p sin u du
3
u
6
0
p/4
0
p/4
2p Ïco
wsw2wuw sin u
5 4p 2cos u
37. }} 5 2cos2 }} sin }} , so
p/4
p/4
0
132 132
u
u
u
Length 5 E
!co§s§§1}§3}2§1§§co§s§§1}§3}2§si§n§§§1}§3}2§ du
u
5E
!co§s§§1}§3}2§ du
1
3
2u p/4
p13
5 }}.
5 3}}u 1 }} sin 1}}24
2
4
3 0
8
dr
du
E
5 2E
52
NINT evalutes to < 2.296.
p
4
0 # u # }}: Surface area
p/4
4
} du
!co§s§2§u§§1§}
c§o§
s§
2u§
sin2 2u
5 (4 2 2Ï2w)p < 3.681
0
42. For a 5 1:
2
4
0
[23, 3] by [22, 2]
dr
}} 5 22a sin u, so surface area
du
p/2
cos 2u
dr
38. }} 5 }}, so
du
1wsiw
nw
Ï1ww
2u
w
52
Length 5
0
pÏ2
w
dx 2
p/4
5 ( f 9(u) cos u)2 1 ( f (u) sin u)2 1 ( f 9(u) sin u)2
!§§§§§§§§1§§§§§§§§2
sin 2u
2
(Ïco
wsw2wuw)2 1 2}} du
0
Ïcwosww2uw
p/4
5 2p
cos u Ïco
ww
s2w
2uww
1wsw
in2ww2wu du
E
5 2p E cos u du
5 2p sin u
3 4 5 pÏ2w < 4.443.
0
p/4
E
5E
5
0
p/2
0
2pÏ2we
u/2
sin u
u
2pe sin u Ï5w du
3
1
2
5 2Ï5wp }}e u(sin u 2 cos u)
5 Ï5wp(e
p/2
p/2
4
0
1 1) < 40.818
1
2p 2 0
E
a(1 2 cos u) du 5 }} u 2 sin u
1
2p 2 0
E
a du 5 }} u
2p
44. (a) }}
!(§Ï2w§e§§)§§1§1§§§2 (e§§§)§ du
u/2 2
1 ( f 9(u))2(cos2 u 1 sin2 u)
dr 2
Ïw2
dr
40. }} 5 }} e u/2, so surface area
p/2
5 ( f (u))2(cos2 u 1 sin2 u)
1 du 2
p/4
122
1 ( f (u) cos u)2
5 ( f (u))2 1 ( f 9(u))2 5 r 2 1 }}
0
du
dy 2
1 ( f 9(u) sin u 1 f (u) cos u)2
sin 2u
2p Ïco
wsw2wuw cos u
0
5 4a2p2
5 ( f 9(u) cos u 2 f (u) sin u)2
39. }} 5 }}(2sin 2u)(2) 5 2}} , so
du
2Ïcw
osw2
wuw
Ïcwosw2wuw
Surface area
E
p/2
1 du 2 1 1}d}u 2
43. }}
0
5
2
0
0
pÏ2
w
1
p/2
2
2
0
dr
0
5 16a2p
cos2 2u
}} 1 1 1 sin 2u du
1 1 sin 2u
2
2p(2a cos u) cos uÏ4waw2wco
ww
s2w
uw
1w4aw2wsi
wnw2wuw du
E cos u du
1
1
5 16a p }}u 1 }}sin 2u
32 4 4
E !§§§§§§§§§§§§§§
cos 2u 1 (1 1 sin 2u)
5E
}}} du
!§§
1 1 sin 2u
5E
Ï2w du 5 2p.
pÏ2
w
E
Ï2w
}}
2
2
u/2 2
(b) }}
0
a
2p
2p
0
1
p/2 2 (2p/2)
a
2p
E
(c) }}
p/2
34
2p
3
5a
0
5a
0
a
p
p/2
3 4
a cos u du 5 }} sin u
2p/2
2p
4
2p/2
2a
p
5 }}
45. If g(u) 5 2f (u), then
Ïw
(gw
(uw
)2w
1w
gw
9(wuw
)2w) 5 2Ïw
( f (u
ww
)2w
1wf 9(
wuww
)2)w, so the length of
g is 2 times the length of f.
434
Chapter 10 Review
46. If g(u) 5 2f (u), then
w(u
ww
)2w
1w
g 9(
wuww
)2)w
2p g(u) sin u Ï(g
2
5 4[2p f (u) sin u Ïw
(fw
(uw
)w
1wf w
9(uww
)2)w],
so the area generated by g is 4 times that of f.
2
3
2
2
evaluates to < 741.420 cm < 7.414 m.
b 2 1/2
2 1/2
1 2p 2 2 5 r 11 1 1}2p}r 2 2 < r
b
since 1}}2 is a very small quantity squared.
2pr
b
2
80p
4
5 236p < 741.416 cm
1. (a) 3k23, 4l 2 4k2, 25l 5 k29 2 8, 12 1 20l
5 k217, 32l
ww32w2w 5 Ï1w3w1w3w
(b) Ï1w7w2w1
2. (a) k23 1 2, 4 2 5l 5 k21, 21l
ww12w 5 Ï2w
(b) Ï1w2w1
3. (a) k22(23), 22(4)l 5 k6, 28l
k
made n complete turns, then the angle is 2pn. So from
the integral, La 5 pbn 1 2pr0n. Solving for n gives
2
1 21!§§§§ 2
bL
}2} 1 1 2 1 .
r0 p
[assuming counterclockwise].
k
Ïw3 1
6. }}, }}
2
2
1
l
1
2
k
1
3 4
2k l
8
2
l
7. 2 }} k4, 21l 5 }}, 2}}
Ï4w2w1
ww12w
Ï1w7w Ï1w7w
1
8. 25 }} }}, }} 5 k23, 24l
1w(4
Ï(3
w/5
w)w2w
w/5
ww
)2 5 5
(c) Since L is proportional to time, the formula in part (a)
shows that n will grow roughly as the square root of
time.
5 sin t
9. (a) }} 5 }} 5 }}
2
2
3
E
49. }}
0
E
2
5 }}a3
3
2
3
4
4
1
4
1 }} cos3 u sin u
E
2p
0
3
2p
4
2
2
4
dy9/dt
cos t
dx/dt
(1/2)sec t
p
1
which for t 5 }} equals }}.
3
4
2
d y
dx
dy9
dx
3
(b) }}2 5 }} 5 }} 5 }}
2 5 2 cos t,
3
3/t 2
2
22/t
5
1
dy
For t 5 2: x 5 }}, y 5 2}}, and }} 5 23.
4
2
dx
1
5
So the tangent line is y 1 }} 5 23 x 2 }} or
2
4
13
y 5 23x 1 }}.
4
dy
dx
(1 1 2 cos u 1 cos2 u) du
1
5 a }}u 1 2 sin u 1 }} sin 2u
2
4
1
dy/dt
dx/dt
10. (a) }} 5 }} 5 }}3 5 2}}t
a2(1 1 cos u)2 du
2 3
2
Ï3w
0
2p
2p
0
dx
2
Ïw3
1
y 5 }}x 1 }}.
2
3
E
Ï3w
Ï3w
p
dy
For t 5 }}; x 5 }}, y 5 1, and }} 5 }}. So the
tangent line is y 2 1 5 }} x 2 }} or
(cos u 1 3 cos u 1 3 cos u 1 cos u) du
5
5 }}pa3, and
2
(1/2)sec t tan t
(1/2)sec t
Ï3w
2
15
15
5 }}a3 3 sin u 1 }} sin u cos u 1 }} u 1 cos2 u sin u
3
8
8
5 a2
dy/dt
dx/dt
2
2p
0
dy
dx
3
a3(1 1 cos u)3 cos u du
2
2
(b) The take up reel slows down as time progresses.
2p
l
Ï3w 1
p
5. }} radians below the negative x-axis: 2}}, 2}}
6
0
48. (a) Use the approximation, La, from 47(e). If the reel has
r
n 5 }}0
b
(pp. 569–572)
ww25w2w 5 Ï7w2w5w 5 5Ï2w9w
(b) Ï1w0w2w1
0
0.03u
2p
■ Chapter 10 Review Exercises
4. (a) k5(2), 5(25)l 5 k10, 225l
0.06u
E 11.75 1 }
} du
2p 2
3
4a
ww82w 5 10
(b) Ï6w2w1
(e) L < 741.420 cm (from part (c)),
2 80p
4
3
5 }}a3, and
0
4a
0
(d) r 2 1 }}
p
10, }3p}2.
0.06u
0.06
E !§11.7§5§§1§}
§2p}§§2 §1§1}§2§p}§§2 du
80p
4
du 5 pa2. So
4
}}a3
length of the curve.
5 1.75u 1 }}
2
3
2
3
sin u du 5 }}a3 2cos u
3
5 }}. By symmetry, wx 5 0, so the centroid is
wy 5 }
pa2
3p
dr
b
(b) Since }} 5 }}, this is just Equation 4 for the
du
2p
La 5
0
p
3
0
0.06u
2p
1
p
Ea
47. (a) Let r 5 1.75 1 }}.
(c) Using NINT,
Ea
50. }}
1
5 3pa .
2
0
5
}}pa3
2
d 2y
dx
dy9
dx
dy9/dt
dx/dt
23/2
22/t
3t 3
4
2
(b) }}2 5 }} 5 }} 5 }}3 5 }}, which for t 5 2
5a
So wx 5 }2 5 }}.
3pa
6
1
5a
6
2
By symmetry, yw 5 0, so the centroid is }}, 0 .
equals 6.
Chapter 10 Review
dy
dt
1
2
11. }} 5 }} tan t sec t equals zero for t 5 kp, where k is any
dx
dt
435
17. (a)
1
2
integer. }} 5 }} sec2 t never equals zero.
12
1
1
1
1}2} tan p, }2} sec p2 5 10, 2}2}2.
1
2 1 22
1
2
1
(a) Horizontal tangents at }} tan 0, }} sec 0 5 0, }} and
[21.5, 1.5] by [21, 1]
(b) 2p
18. (a)
dx
dt
(b) There are no vertical tangents, since }} never equals
zero.
kp
2
dy
dt
12. }} 5 2 cos t equals zero for u 5 }}, where k is any odd
dx
dt
integer. }} 5 2 sin t equals zero for t 5 kp, where k is any
[23, 3] by [22, 2]
(b) p
19. (a)
integer.
1
p
2
p
2
2
(a) Horizontal tangents at 22 cos }}, 2 sin }} 5 (0, 2)
1
3p
2
3p
2
2
and 22 cos }}, 2 sin }} 5 (0, 22).
(b) Vertical tangents at (22 cos 0, 2 sin 0) 5 (22, 0) and
(22 cos p, 2 sin p) 5 (2, 0).
[21.5, 1.5] by [21, 1]
p
2
(b) }}
20. (a)
kp
2
dy
dt
13. }} 5 22 sin t cos t 5 2sin 2t equals zero for t 5 }},
dx
dt
where k is any integer. }} 5 sin t equals zero for t 5 kp,
[21.5, 1.5] by [21, 1]
where k is any integer. Where they are both zero, use
(b) p
L’Hôpital’s rule:
2sin 2t
t→kp sin t
dy/dt
t→kp dx/dt
22 cos 2t
cos t
t→kp
lim }} 5 lim }} 5 lim }} 5 62.
1
2
p
p
(a) Horizontal tangent at 2cos }}, cos2 }} 5 (0, 0).
2
2
(b) There are no vertical tangents.
kp
2
dy
dt
14. }} 5 9 cos t equals zero for t 5 }}, where k is any odd
dx
integer. }} 5 24 sin t equals zero for t 5 kp, where k is
dt
any integer.
1
p
2
p
2
2
(a) Horizontal tangents at 4 cos }}, 9 sin }} 5 (0, 9) and
14 cos }2}, 9 sin }2}2 5 (0, 29).
3p
3p
(b) Vertical tangents at (4 cos 0, 9 sin 0) 5 (4, 0) and
(4 cos p, 9 sin p) 5 (24, 0).
f9(u) sin u 1 f (u) cos u
f9(u) cos u 2 f (u) sin u
dy
dx
21. }} 5 }}}
22 sin 2u sin u 1 cos 2u cos u
22 sin 2u cos u 2 cos 2u sin u
5 }}}}
10, }4}2, 10, }4}2, 10, }4}2 and 10, }4}2 are polar solutions.
p
3p
5p
)
)
7p
)
w
w
dy
22/Ï2
dy
2/Ï2
5 }} 5 1, }}
5 }} 5 21,
}}
u
53p/4
dx u5p/4
d
x
22/Ï2
w
22/Ï2
w
)
dy
2/Ïw
2
dy
22Ïw
2
5 }} 5 1, }}
5 }} 5 21.
}}
u
57p/4
dx u55p/4
d
x
2/Ï2
2Ï2
w
w
The Cartesian equations are y 5 6x.
f9(u) sin u 1 f (u) cos u
f9(u) cos u 2 f (u) sin u
dy
dx
22. }} 5 }}}
22 sin 2u sin u 1 (1 1 cos 2u)cos u
22 sin 2u cos u 2 (1 1 cos 2u) sin u
5 }}}}
24 sin2 u cos u 1 cos u 1 2 cos3 u 2 cos u
24 cos u sin u 2 sin u 2 2 cos u sin u 1 sin u
15.
5 }}}}}
2
2
24 sin2 u 1 2 cos2 u
26 cos u sin u
5 }}}
[27.5, 7.5] by [25, 5]
16.
4 sin2 u 2 2 cos2 u
3 sin 2u
5 }}.
10, }2}2 and 10, }2}2 are polar solutions.
p
)
3p
)
dy
dy
4
5 }}
5 }} is undefined, so the tangent lines
}}
dx u5p/2
dx u53p/2
0
[27.5, 7.5] by [25, 5]
are vertical with equation x 5 0.
436
Chapter 10 Review
31
1 22
4
1 22
4
u
d
sin u
2
du
1
u
u
5 }} sin }} sin u 1 cos u 2 cos }} cos u
2
2
2
u
dx
d
}} 5 }} 1 2 cos }} cos u
2
du du
1
u
u
5 }} sin }} cos u 2 sin u 1 cos }} sin u
2
2
2
dy
Solve }} 5 0 for u with a graphing calculator: the solutions
du
dy
du
23. }} 5 }} 1 2 cos }}
31
12
12
25.
12
12
[21.5, 1.5] by [21, 1]
1
1
1
2
2
the middle four solutions to y 5 r sin u reveals
The tips have Cartesian coordinates }}, }} ,
Ïw2 Ï2w
1
1
1
1
1
1
2}}, }} , 2}}, 2}} , and }}, 2}} . From the
Ïw2 Ïw2
Ï2w Ïw2
Ï2w Ï2w
curve’s symmetries, it is evident that the tangent lines at
horizontal tangent lines at y < 60.443 and y < 61.739.
those points have slopes of 21, 1, 21, and 1, respectively.
1
are 0, <2.243, <4.892, <7.675, <10.323, and 4p. Using
dx
du
Solve }} 5 0 for u with a graphing calculator: the solutions
1
1
1
2
1
y 2 }} 5 2 x 2 }} or
Ïw2
Ï2w
y 5 2x 1 Ïw2,
Using the middle five solutions to find x 5 r cos u reveals
vertical tangent lines at x 5 2, x < 0.067, and x < 21.104.
1
1
y 2 }} 5 x 1 }} or
Ïw2
Ï2w
y 5 x 1 Ïw2,
dx
dt
Where }} and }} both equal zero (u 5 0, 4p), close
inspection of the plot shows that the tangent lines are
1
1
1
2
y 1}} 5 2 x 1 }} or
Ï2w
Ïw2
y 5 2x 2 Ï2w, and
horizontal, with equation y 5 0. (This can be confirmed
using L’Hôpital’s rule.)
1
dy
d
du
du
dx
d
}} 5 }}[2(1 2 sin u)cos u]
du du
2
So the equations of the tangent lines are
are 0, <1.070, <3.531, 2p, <9.035, <11.497, and 4p.
dy
dt
21
1
y 1 }} 5 x 2 }} or
Ïw2
Ï2w
y 5 x 2 Ïw2
24. }} 5 }}[2(1 2 sin u)sin u] 5 24 sin u cos u 1 2 cos u
26.
5 22 cos2 u 2 2 sin u 1 2 sin2 u
5 4 sin2 u 2 2 sin u 2 2
dy
du
Solve }} 5 0 for u:
p p 5p
6 2 6
3p
2
[23, 3] by [22, 2]
the solutions are }}, }}, }}, and }}.
Using the first, third, and fourth solutions to find
1
2
y 5 r sin u reveals horizontal tangent lines at y 5 }} and
y 5 24.
dx
du
Solve }} 5 0 for u (by first using the quadratic formula to
p 7p
2 6
11p
6
find sin u): the solutions are }}, }}, and }}. Using the last
two solutions to find x 5 r cos u reveals vertical tangent
3Ïw3
dy
dx
lines at x 5 6}} < 62.598. Where }} and }} both equal
1
p
2
2
2
dt
dt
zero u 5 }} , inspection of the plot shows that the tangent
line is vertical, with equation x 5 0. (This can be confirmed
using L’Hôpital’s rule.)
As the plot shows, the curve crosses the x-axis at
(x, y)-coordinates (21, 0) and (1, 0), with slope 21 and 1,
respectively. (This can be confirmed analytically.) So the
equations of the tangent lines are
y 2 0 5 2(x 1 1)
y 5 2x 2 1 and
y205x21
y 5 x 2 1.
27. r cos u 5 r sin u
x 5 y, a line
28. r 5 3 cos u
r 2 5 3r cos u
x 2 1 y 2 5 3x
9
4
9
4
x 2 2 3x 1 }} 1 y 2 5 }}
3 2
3 2
1x 2 }2}2 1 y 5 1}2}2
3
3
a circle 1center 5 1}}, 02, radius 5 }}2
2
2
2
437
Chapter 10 Review
29. r 5 4 tan u sec u
dr
du
37. }} 5 2sin u, so
r sin u
r cos u
r cos u 5 4 }}
y
x 5 4}} or x 2 5 4y, a parabola
x
1
2
E Ï(2
w1ww
1wcowswuww
)w
1w(2
wsi
wnwwuw
) du
2w2wcowswuw du
5 E Ï2ww
u
u
5E
!4§§sin§§}§2} du 5 324 cos }2}4 5 8.
p
3
p
p
r cos u cos }} 2 r sin u sin }} 5 2Ï3w
3
3
Ïw3
1
w
}} r cos u 2 }} r sin u 5 2Ï3
2
2
Ïw3
1
w
}}x 2 }}y 5 2Ï3
2
2
x
x 2 Ï3wy 5 4Ï3w or y 5 }} 2 4, a line
Ï3w
12
31. x 1 y 1 5y 5 0
r 2 1 5r sin u 5 0
r 5 25 sin u
2
2
2p
2
0
0
dr
38. }} 5 2 cos u 2 2 sin u, so Length
du p/2
E
5E
5E
5
0
p/2
0
p/2
0
Ï(2
wwsin
wwuw
1w2wcowswuww
)2w
1w(2wwcowswuww
2w2wsin
wwuw
)2 du
Ï8wwsin
w2wuww
1w8wcoww
s2wu du
2Ï2w du 5 pÏ2w.
2
132 132
u
u
u
Length 5 E
!§18§sin§§§1}§3}22§§1§§18§§sin§§§1}§3}2§co§s§§1}§3}22§§ du
u
u
u
5 E 8 sin 1}}2 sin 1}}2 1 cos 1}}2 du
§§§§§§§§3 §
3 !§§§§3
u
5 E 8 sin 1}}2 du
3
u
dr
du
p/4
(r cos u) 1 4(r sin u) 5 16
34. (x 1 2)2 1 (y 2 5)2 5 16
(r cos u 1 2)2 1 (r sin u 2 5)2 5 16
1 dy
8 dt
E !§12e§§2§}18}§2§1§§(e§)§ dt
1
1
5E
!4§e§§2§}2}§e§§1§}6§4}§1§e§ dt
5E
!§12e§§1§}18}§2§ dt
t
5 3e 1 }}4
8
2
t 2
0
4t
0
ln 2
2t
2t
2
2t
0
ln 2
2t
0
ln 2
5 4 1 }} 2 1
8
ln 2
8
2
2
32
1
p/4
1 3 24
2u
3
4
5p23
0
2sin 2u
dr
40. }} 5 }}, so Length
du
1wco
s2
Ï1ww
ww
wuw
E !(§Ï1w§w
§1w§cow§sw§2w§uw§)§§1§1}
§Ï§1w2w§1sin§w}
§cow2swu§§2wuw§2 du
(1 1 cos 2u)
sin 2u
5 E !}
1}
du
}
§§1§1§c§}
o§s§2§u§§§
2§
1§1§§
co§s§
u
1 1 2 cos 2u 1 cos 2u 1 sin 2u
5E
}}}} du
!§§§
1 1 cos 2u
5 E Ï2w du 5 pÏ2w
5
35. }} = 2e2t 2 }}, }} 5 e t, so
2t
2
5 8 }}u 2 }} sin }}
16
cos u 1 4 sin u
r 2 cos2 u 1 4r 2 sin2 u 5 16, or r 2 5 }
}
2
2
ln 2
2
2
0
2
ln 2
2
0
p/4
2
2
3
0
p/4
33. x 2 1 4y 2 5 16
Length 5
u
39. }} 5 8 sin2 }} cos }} , so
32. x 2 1 y 2 2 2y 5 0
r 2 2 2r sin u 5 0
r 5 2 sin u
dx
dt
2
0
2p
0
2p
30. r cos u 1 }} 5 2Ï3w
12
2p
Length 5
p/2
2
2
2p/2
p/2
2
2
2p/2
p/2
2
2
2p/2
p/2
2p/2
dx
dt
dy
dt
41. }} 5 22 sin t, }} 5 2t, so
E
5E
Length 5
ln 2 1 24
8
5 3 1 }} 5 }} < 3.087.
p/2
0
p/2
0
Ï(2
w2wwsin
wwtw
)2w
1w(2wt)
w2w dt
2Ïw
t 2w
1wsin
w2wtw dt,
which using NINT evaluates to < 3.183.
dx
dy
36. }} 5 2t, }} 5 t 2 2 1, so
dt
dt
E
5E
5E
Length 5
Ï3
w
2Ï3
w
Ï3
w
2Ï3
w
Ï3
w
2Ï3
w
5
Ï(2
wt)
w2w1
ww(w
t 2w
2w
1w
)2 dt
Ï4ww
t 2w
1wt 4w2
ww2w
t 2w
1w1 dt
Ï(t
ww1
ww1w
) dt
2
2
Ï3w
31 2 4
3
t
}} 1 t
3
2Ï3
w
dx
dt
dy
dt
42. }} 5 3 cos t, }} 5 3Ïtw, so
Length 5
3
2
3
2
0
2
0
which using NINT evaluates to < 12.363.
43. Area 5
E
2p
1
}}(2 2 cos u)2 du
2
2p
E
3
0
1
(4 2 4 cos u 1 cos2 u) du
2 0
1
1
1
5 }} 4u 2 4 sin u 1 }}u 1 }} sin 2u
2
2
4
5 }}
5 4Ï3w.
E Ï(3wwcowswt)ww1ww(3wÏwwtw)w dt 5 E 3Ïtw1wwcowws wt dt,
4
2p
0
9p
2
5 }}
438
Chapter 10 Review
44. Area 5
E
p/3
3
0
p/3
4
1
1 1
1
}} sin2 3u du 5 }} }}u 2 }} sin (6u)
2
2 2
12
p
12
50.
5 }}
0
45.
[21.5, 1.5] by [21, 1]
cos 2u
dr
p
r 5 6Ïsi
wnww2uw and }} 5 6}}, where 0 # u # }}, so
2
du
Ïswinww2wu
[23, 3] by [22, 2]
p
4
The curves cross where cos 2u 5 0, such as u 5 }}. Using
Area 5 2
E
5 2E (cos 2u 1 2 cos 2u) du
1
1
5 2 }} sin 4u 1 }}u 1 sin 2u
38
4
2
p/4
1
Length 5 4
}}[(1 1 cos 2u)2 2 1] du
2
0
p/4
E
p/2
0
!si§n§§2u§§1§}
§si§n}
§2u§ du
cos2 2u
cos u du
3
p/2
4
5 4p
0
d
dt
51. (a) v(t) 5 }}[(4 cos t)i 1 (Ï2w sin t)j]
p/4
5 (24 sin t)i 1 (Ï2w cos t)j
0
p
4
0
2p Ïsi
wnww2uw cos u
5 4p sin u
2
5 }} 1 2
p/2
5 4p
the curves’ symmetry,
0
E
d
dt
a(t) 5 }}[(24 sin t)i 1 (Ï2w cos t)j]
46.
5 (24 cos t)i 1 (2Ï2w sin t)j
) 1 2) !1§24§§sin§§§2§1§§1ϧ2w§§co§s§§2§
p 2
}}
4
p
4
(b) v }} 5
[24.5, 4.5] by [22, 4]
5 Ï8ww
1w1 5 3
Since the two curves are covered over different u-intervals,
E }12}[2(1 1 sin u)] du 2 pr
5 2E (1 1 2 sin u 1 sin u) du 2 p
1
1
5 2 u 2 2 cos u 1 }}u 2 }} sin 2u
3
4 2 p 5 5p
2
4
2p
0
2
2
2p
2
0
2p
0
dx
dt
E
5 (Ï3w sec t tan t)i 1 (Ï3w sec2 t)j
2p(2t)Ïw
t 2w
1w
22w dt
3
4
4p
5 }}(t 2 1 4)3/2
3
dx
dt
1
2t
Ï5w
0
dy
dt
d
dt
a(t) 5 }}[(Ï3w sec t tan t)i 1 (Ï3w sec2 t)j]
76p
5 }}
3
5 Ï3w(sec t tan2 t 1 sec3 t)i 1 (2Ï3w sec2 t tan t)j
48. }} 5 2t 2 }}2 , }} 5 4, so
E
1
1
v a
)v))a)
821
5 cos21 }}
(3)(3)
21 7
5 cos }} < 38.948.
9
52. (a) v(t) 5 }}[(Ï3w sec t)i 1 (Ï3w tan t)j]
Ï5
w
0
?
u 5 cos21 }
d
dt
dy
dt
47. }} 5 t, }} 5 2, so
Area 5
p
4
(c) At t 5 }}, v 5 22Ï2wi 1 j, a 5 22Ï2wi 2 j, and
find the two areas separately. Then
Area 5
p 2
}}
4
1
Area 5
2p t 1 }}
2t
w
1/Ï2
2
2!1§§§§§§2 §§§
1 2
2t 2 }}2 1 42 dt,
2t
which using NINT evaluates to < 10.110.
(b) )v(0)) 5 Ï3wwsec
w2w0wwtan
w2w0ww
1w3wsec
w4w0w 5 Ï0ww
1w
3 5 Ï3w
(c) At t 5 0, v 5 Ï3wj, a 5 Ï3wi
010
? 5}
u 5 cos21 }
} 5 cos21 0 5 908
)v))a)
(Ï3w)(Ïw3)
v a
dr
2sin 2u
49. }} 5 }}, so
du
s w2wu
Ïcwow
E
5E
Area 5
p/4
2p Ïco
wsw2wuw sin u
0
p/4
} du
!co§s§2§u§§1§}
c§o§
s§
2u§
sin2 2u
2p sin u du
0
3
4
5 2p 2cos u
p/4
0
5 p(2 2 Ï2w) < 1.840
t
(1 1 t )
1
(1 1 t )
2
2
t
1
1
2}}
1 }}
5 }}2 ,
(1 1 t 2)3/2
(1 1 t 2)3/2
11t
53. v(t) 5 2}}
2 3/2 i 1 }}
2 3/2 j
)}dd}rt ) 5 )v(t)) 5 !§
1 §§§§§§2§§§1§§§§§§2§
which is at a maximum of 1 when t 5 0.
Chapter 10 Review
dr
dt
dx
a(t) 5 }} 5 (e t cos t 2 e t sin t 2 e t sin t 2 e t cos t)i
dt
54. v(t) 5 }} = (e t cos t 2 e t sin t)i 1 (e t sin t 1 e t cos t )j
1 (e sin t 1 e cos t 1 e cos t 2 e sin t)j
t
t
t
t
k l k
,2
v(3) 5 k2
l, and
Ïw
Ïw
r(t) ? a(t) 5 (e t cos t)(22e t sin t) 1 (e t sin t)(2e t cos t) 5 0
for all t. The angle between r and a is always 908.
1
)
)
0
2
0
0
2 1E }t ln}t dt2 j
5 3ln t4 i 1 3ln (ln t)4 j 5 3i 1 (ln 2)j
dr
57. r(t) 5 E}} dt 5 (cos t)i 1 (sin t)j 1 C
dt
56.
1E
p
x
4
3
x2
y2
}} 1 }} 5 1.
9
25
1
2
e
e
2 ln t
}} dt i 1
t
2
e
2
e
2
1
e
e
e
2
e
r(0) 5 i 1 C 5 j, so C 5 2i 1 j, and
dx
dt
1
2
r(t) 5 (tan21 t 1 1)i 1 Ïw
t 2w
1w1j
E
5 1 or
E !§1}1§2}§2 §1§(5§§2§t)§ dt, which using NINT
10
2
2
0
E
10
0
dx
dt
t(10 2 t) 2
}} dt
2
py 2 }} dt
E1
E
3
10
2
(c) Area 5
E
10
0
4
t(10 2 t)
2
!§1}§2}§2 §1§(5§§2§t)§ dt, which
2p}}
1 2
2
using NINT evaluates to < 1040.728.
dy
dx
e t sin t 1 e t cos t
e cos t 2 e sin t
dy/dt
dx/dt
cos t 1 sin t
cos t 2 sin t
63. (a) }} 5 }} 5 }}
5 }}
t
t
r(t) 5 i 1 t 2j
E ddt r
dr
r(t) 5 E}} dt 5 2t i 2 t j 1 C t 1 C
dt
2
60. }} 5 }}2 dt 5 (22t)i 1 (22t)j 1 C1,
2
2
1
)
2
dr
5 22i 2 2j 1 C1 5 4i, so C1 5 6i 1 2j and
}}
dt t51
r(t) 5 (2t 2 1 6t)i 1 (2t 2 1 2t)j 1 C2
r(1) 5 5i 1 j 1 C2 5 3i 1 3j, so C2 5 22i 1 2j, and
r(t) 5 (2t 1 6t 2 2)i 1 (2t 1 2t 1 2)j
2
y 2
p
2 0
10
p
5 }} (100t 2 2 20t 3 1 t 4) dt
8 0
p 100 3
1 10
1250p
5 }} }}t 2 5t 4 1 }}t 5
5 }}
8 3
5 0
3
r(0) 5 j 1 C 5 i 1 j, so C 5 i and
dr
dt
x 2
1 3 2 1 1}5}2
evaluates to < 25.874.
E ddrt
)
2
dy
dt
Length 5
58. r(t) 5 }} dt 5 (tan21 t)i 1 Ïw
t 2w
1w1j 1 C
E
p
4
y
5
5 }}
dr
d 2r
dr
59. }} 5 }}2 dt 5 2tj 1 C1, r(t) 5 }} dt 5 t 2j 1 C1t 1 C2
dt
dt
dt
dr
5 C1 5 0, so r(t) 5 t 2j 1 C2. And r(0) 5 C2 5 i, so
}}
dt t50
3p2
62. (a) }} 5 }} and }} 5 5 2 t so
(b) Volume 5
r(t) 5 (cos t 2 1)i 1 (sin t 1 1)j
? 32 5 }}
2
(c) }} 5 cos }}t and }} 5 sin }}t, so }}
0
1
l
1
16Ï2w
25p
p
5p
5 }} sin 1}} ? 32 5 2}}
16
4
16Ï2w
d 2x
3p2
p
5 2}} cos }}
dt t53
16
4
(b) x-component: }}2
d y
dt t53
1
p
4
!§§§§§§§§
y-component: }}2
1E (3 1 6t) dt2i 1 1E 6p cos pt dt2 j
5 33t 1 3t 4 i 1 36 sin pt4 j 5 6i
5p
4
3p
5p
}} }}
4 2
4 2
9p 2
25p 2
pÏw
3w
4
pÏ1ww7
}} 1 }} 5 }} 5 }} < 3.238
32
32
4
4Ï2
w
2
55.
p
4
61. (a) v(t) 5 }}, }} 5 2}} sin }}t, }} cos }}t ,
)v(3)) 5
5 (22e t sin t)i 1 (2e t cos t)j
3p
4
dx dy
dt dt
2
439
)
dy
21
5 }} 5 1
}}
dx t5p
21
dy
dx
dt
dt
dy 2
2t
2
}} 5 e (sin t 1 2 sin t cos t 1 cos2 t)
dt
(b) }} 5 e t(sin t 1 cos t), }} 5 e t(cos t 2 sin t)
1 2
5 e 2t(1 1 2 sin t cos t)
dx 2
1}d}t 2
5 e 2t(cos2 t 2 2 cos t sin t 1 sin2 t)
5 e 2(1 2 2 cos t sin t)
)v(t)) 5 e tÏ2w
)v(3)) 5 e3Ï2w
E )v(t)) dt
5 E e Ï2w
3
5 Ï2w3e 4
0
(c) Distance 5
3
0
3
t
0
t
5 (e3 2 1)Ï2w
440
Chapter 10 Review
k
dx dy
dt dt
l k
l
6
5
k l
96
5
64. (a) v(t) 5 }}, }} 5 2t, }}t 2 , v(4) 5 8, }} , and
!§§§§1§§§2
6
(b) Distance 5 E (2t) 1 1}}t 2 dt
!§§§§§§5 §§
2
1w9w
t dt
5 E }}tÏ2w5ww
5
4144
2
4
5 }}(25 1 9t )
3 135
40 5 }13}5
)v(4)) 5
69. (a)
96 2
104
5 }}
5
5
82 1 }}
4
2
2
0
4
2
[22, 10] by [22, 6]
k
a(t) 5 k
2 3/2
dy
dx
dy/dt
dx/dt
6t 2/5
2t
3
5
3
5
(c) t 5 Ïxw1
ww2, so }} 5 }} 5 }} 5 }}t 5 }}Ïxw1
ww2
65. x degrees east of north is (90 2 x) degrees north of east.
Add the vectors:
K540 cos 108, 540 sin 108L 1 K55 cos (2108), 55 sin (2108)L
5 k595 cos 108, 485 sin 108l
< K585.961, 84.219L.
Speed < Ï5w8w5w.9
w6w1w2w1
ww84w.2
w1w9w2w < 591.982 mph.
1
585.961
84.219
l k
l k
dx dy
dt dt
d 2x d 2y
, }} 5 p2 sin pt, p2 cos pt
}}
dt 2 dt 2
l
(b) v(t) 5 }}, }} 5 p 2 p cos pt, p sin pt
2
0
2
Direction < tan21 }} < 81.8218 east of north
l
v(0) 5 k0, 0l
a(0) 5 k0, p 2l
v(1) 5 k2p, 0l
a(1) 5 k0, 2p 2l
v(2) 5 k0, 0l
a(2) 5 k0, p 2l
v(3) 5 k2p, 0l
a(3) 5 k0, 2p 2l
(c) Topmost point: 2p ft/sec
center of wheel: p ft/sec
Reasons: Since the wheel rolls half a circumference, or
p feet every second, the center of the wheel will move
p feet every second. Since the rim of the wheel is
turning at a rate of p ft/sec about the center, the
velocity of the topmost point relative to the center
is p ft/sec, giving it a total velocity of 2p ft/sec.
70. v0 5
, where a 5 458, g 5 32, and
!}
§si§n§}
2§
a
Rg
R 5 range
for 4325 yds 5 12,975 ft: v0 < 644.360 ft/sec
66. Add the vectors:
k120 cos 208, 120 sin 208l 1 k300 cos (258), 300 sin (258)l
< k411.622, 14.896l.
1 411.622 2
14.896
Direction < tan21 }} < 2.0738
Length < Ï4w1w1w.6
w2w2w2w1
ww14w.8
w9w6w2w < 411.891 lbs
67. Taking the launch point as the origin,
y 5 (44 sin 458)t 2 16t 2 equals 26.5 when t < 2.135 sec
(as can be determined graphically or using the quadratic
formula). Then x < (44 cos 458)(2.135) < 66.421
horizontal feet from where it left the thrower’s hand.
Assuming it doesn’t bounce or roll, it will still be there 3
seconds after it was thrown.
(80 sin 458)2
68. ymax 5 }} 1 7 5 57 feet
2(32)
for 4752 yds 5 14,256 ft: v0 < 675.420 ft/sec
71. (a) v0 5
5 Ï(1
w0w9w.5
w)(
w3w2w)w < 59.195 ft/sec
!}
§si§n§}
2§
a
Rg
(b) The cork lands at y 5 24, x 5 177.75.
1 2v
2
g
c
os a
0
gx 2
a 5 458: v0 5 2}} < 74.584 ft/sec
y2x
Solve y 5 2 }
x 2 1 (tan a)x for v0, with
2
2 }
!§§§§§
5
12
72. (a) The javelin lands at y 5 26.5, x 5 262}}.
1 2v
g
cos a
2
Solve y 5 2 }
x 2 1 (tan a)x for v0, with
2
2 }
0
a 5 408:
v0 5
}}} < 91.008 ft/sec
!2§§§
(2 cos 408)( y 2 x tan 408)
gx 2
2
(v sin a)2
0
(b) ymax 5 }
} 1 6.5
2g
(91.008 sin 408)2
64
< }} 1 6.5 < 59.970 ft
73. We have x 5 (v0t) cos a and
gt 2
2
y 1 }} 5 (v0t) sin a. Squaring and adding gives
1
gt 2 2
5 (v0t)2(cos2 a 1 sin2 a) 5 v02t 2.
2
x 2 1 y 1 }}
2
Cumulative Review
74. (a) r(t) 5 (155 cos 188 2 11.7)ti
1 (4 1 155 sin 188t 2 16t 2)j
x(t) 5 (155 cos 188 2 11.7)t
y(t) 5 4 1 155 sin 188t 2 16t 2
Cumulative Review Exercises
(pp. 573–576)
(155 sin 188)2
(b) ymax 5 }} 1 4 < 39.847 feet, reached at
2(32)
155 sin 188
tmax 5 }} < 1.497 sec
32
(c) y(t) 5 0 when t < 3.075 sec (found using the quadratic
formula), and then
x < (155 cos 188 2 11.7)(3.075) < 417.307 ft.
(d) Solve y(t) 5 25 using the quadratic formula:
At those times, x 5 (155 cos 188 2 11.7)t equals
< 72.406 and < 333.867 feet from home plate.
(e) Yes, the batter has hit a home run. When the ball is 380
feet from home plate (at t < 2.800 seconds), it is
approximately 12.673 feet off the ground and therefore
clears the fence by at least two feet.
4
75. (a) r(t) 5 (155 cos 188 2 11.7)}}(1 2 e20.09t) i
1
155 sin 188
0.09
2
sin 3x
4x
3 cos 3x
3
4
4
1
1
2}}2
}} 2 1
x11
(x 1 1)
3. By l’Hôpital’s Rule, lim }} 5 lim }} 5 21.
x
1
x→0
x→0
2. By l’Hôpital’s Rule, lim }} 5 lim }} 5 }}.
x→0
x→0
x 1 ex
x→` x 2 e
ex
2
x→` e
< 0.534 and 2.460 seconds.
3
2(1)2 2 1 2 1
5 0.
}}
12 1 1 2 12
1 1 ex
x→` 1 2 e
5 lim }}x 5 21.
232
1
0.09
1. Since the function has no discontinuity at x 5 1, the limit is
4. By l’Hôpital’s Rule, lim }}x 5 lim }}x
w5w5w2wsi
wnw2w1w8w8w2
ww4(1
w6w)(
w2w1w)w
2155 sin 188 6 Ï1
t 5 }}}}}
3
t(1 2 cos t)
t 2 sin t
t sin t 1 (1 2 cos t)
t cos t 1 2 sin t
5 lim }}} 5 lim }}
1 2 cos t
sin t
t→0
t→0
2t sin t 1 3 cos t
5 lim }} 5 3
cos t
t→0
5. By l’Hôpital’s Rule, lim }}
t→0
ex
}}
ln (e x 2 1)
(e x 2 1)
6. By l’Hôpital’s Rule, lim1 }} 5 lim1 }
1
ln x
x→0
x→0
}}
xe x
x→0 e 2 1
4
1
x(t) 5 (155 cos 188 2 11.7)}}(1 2 e 20.09t)
0.09
155 sin 188
y(t) 5 4 1 }} (1 2 e 20.09t)
0.09
32
1 }}2 (1 2 0.09t 2 e 20.09t)
0.09
2
(b) Plot y(t) and use the maximum function to find
y < 36.921 feet at t < 1.404 seconds.
(c) Plot y(t) and find that y (t) 5 0 at t < 2.959, then plug
this into the expression for x(t) to find
x(2.959) < 352.520 ft.
(d) Plot y(t) and find that y (t) 5 30 at t < 0.753 and
2.068 seconds. At those times, x < 98.799 and
256.138 feet (from home plate).
(e) No, the batter has not hit a home run. If the drag
coefficient k is less than <0.011, the hit will be a home
run.
(This result can be found by trying different k-values
until the parametrically plotted curve has y $ 10 for
x 5 380.)
76. (a) BD
E 5 AD
E 2 AB
E
1
2
1
2
ln (e x 1 x)
x
7. Use f (x) 5 (e x 1 x)1/x. Then ln f (x) 5 }}, and
1 }}2 (1 2 0.09t 2 e 20.09t) j
1
x
xe x 1 e x
e
x→0
5 lim1 }
51
x } 5 lim1 }}
x
1 4 1 }} (1 2 e 20.09t)
32
0.09
441
1
2
(b) A
E
P5A
E
B 1 }} B
E
D = }} A
E
B1 }} A
E
D
1
2
(c) AC
E5 A
E
B 1 AD,
E so by part (b), AP
E 5 }} A
E
C.
77. The widths between the successive turns are constant and
are given by 2pa.
ln (e x 1 x)
x
x→0
(e x 1 1)/(e x 1 x)
1
x→0
lim }} 5 lim }} 5 2.
So lim (e x 1 x)1/x 5 lim e ln f(x) 5 e 2.
x→0
1
x→0
3x 1 1
x
1
sin x
2
(3x 1 1) sin x 2 x
x sin x
8. lim }} 2 }} 5 lim }}
x→0
x→0
(3x 1 1) cos x 1 3 sin x 2 1
x cos x 1 sin x
5 lim }}}
x→0
2(3x 1 1) sin x 1 6 cos x
2x sin x 1 2 cos x
5 lim }}} 5 3
x→0
442
Cumulative Review
x2
11x
9. (a) 2(1) 2 12 5 1
19. y9 5 2x tan 21 x 1 }}2
(b) 2 2 1 5 1
20. y9 5 23x 24e x 1 e xx 23 5 (x 23 2 3x 24)e x
(c) 1 [from (a) and (b)]
(d) Yes, since lim f (x) 5 f (1) 5 1
x→1
2 (1 1 cos x)(2csc x cot x) 1 csc x sin x
1 1 1 cos x 2 1}}}}
2
(1 1 cos x)
csc x
(e) No.
Left-hand derivative:
21. y9 5 3 }}
2
2
f (1 1 h) 2 f (1)
h
3 csc x
(1 1 cos x)
5 }}4 (1 2 csc x cot x 2 cos x csc x cot x)
2(1 1 h) 2 (1 1 h)2 2 1
h
h→0
2 1 2h 2 1 2 2h 2 h 2 2 1
5 lim2 }}}
h
h→0
lim2 }} 5 lim2 }}}
h→0
3 csc2 x
(1 1 cos x)
5 }}4 (1 2 cot x csc x 2 cot 2 x)
3 csc2 x
(1 1 cos x)
h2
h
5 lim2 2}}
5 }}4 (1 2 csc 2 x 1 csc 2 x 2 cot x csc x 2 cot 2 x)
5 lim2 2h 5 0
5 }}4 (csc 2 x 2 cot x csc x 2 2 cot 2 x)
h→0
3 csc2 x
(1 1 cos x)
h→0
3
f (1 1 h) 2 f (1)
h
2 2 (1 1 h) 2 1
h
lim }} 5 lim1 }}
h→01
1 2 cos x 2 2 cos2 x
1 (sin x)(1 1 cos x) 21 sin x 2
(1 1 cos x)(1 2 2 cos x)
3
5 1}}}21}}}2
(sin x)(1 1 cos x)
sin x
5 }}}
2
4 }}}
2
Right-hand derivative:
h→0
2
2h
5 lim1 }} 5 21
h→0 h
Since the left- and right-hand derivatives are not equal,
f is not differentiable at x 5 1.
3(1 2 2 cos x)
(sin x)(1 1 cos x)
1
2
d p
dx 2
1
2
d p
dx 2
22. y9 5 }} }} 2 sin 21 x 2 }} }} 2 tan 21 x
1
1
5 2}} 1 }}2
2
1
1
x
2wxw
Ïw1w
11. Horizontal: since as x → 6`, 2x 2 2 x → 1` while
1
Vertical: solve 2x 2 2 x 5 0 to find x 5 0, x 5 }}.
2
1
23 1 }}, x , 2
(2 2 x)
12. One possible function is y 5
8
3 2 }},
x$2
x
2
5 }}}
4
3
10. Solve 4 2 x 2 # 0: all x # 22 and x $ 2.
21 # cos x # 1, the end behavior at both ends is y 5 0.
4
d
dx
d
dx
23. }}[cos (xy) 1 y 2 2 ln x] 5 }}(0)
h
1
x
2sin (xy)(xy9 1 y) 1 2yy9 2 }} 5 0
1
}} 1 y sin (xy)
x
1 1 xy sin (xy)
2xy 2 x sin (xy)
y9 5 }} 5 }}
2
2x sin (xy) 1 2y
1 2
1
1
d
)x) 5 )x)
24. y9 5 }})x)21/2 }})x) 5 }} }
}}
dy
dx
Ï9w 2 Ï4w 1
f (5) 2 f (0)
13. }} 5 }} 5 }}
5
5
(x 2 2)(1) 2 (x 1 1)(1)
(x 2 2)
26.
3
(x 2 2)
14. y9 5 }}}
5 2}}2
2
3
4
1
15. y9 5 2sin (Ï1ww
2w3wx) }}(1 2 3x)21/2 (23)
2
3 sin Ï1ww
2w3xw
5 }}
2Ï1ww
2w3xw
sin x
cos x
(sin x)(1 1 cos 2 x)
cos x
5 }}
2
1
2
18. y9 5 (e x
2x
2cos t
2sin t
x21
12y
ln y 5 x ln (cos x)
1
)(2x 2 1) 5 (2x 2 1)e x
2x
1
2
1
5 (cos x)
x21
2
[cos x ln (cos x) 2 x sin x]
27. By the Fundamental theorem of Calculus,
y9 5 Ï1ww
1wx 3w.
4
28. y 5 2cos t
2
2
1 dy
1
}} }} 5 x }} (2sin x) 1 ln cos x
y dx
cos x
dy
x sin x
}} 5 y ? ln (cos x) 2 }}
dx
cos x
x sin x
x
5 (cos x) ln (cos x) 2 }}
cos x
3
2x
x 11
17. y9 5 }
2 } (2x) 5 }
2 }
2
dy/dt
dx/dt
2xÏ)x
w)w
ln y 5 ln[(cos x)x]
16. y9 5 sin x sec 2 x 1 tan x cos x 5 }}
2 1 sin x
1
x 11
dx
25. }} 5 }} 5 }} 5 cot t 5 }}
[210, 10] by [24, 4]
520
2Ï)x
w)w x
2
x2
5 2cos (x 2) 1 cos (2x);
2x
y9 5 2x sin (x 2) 2 2 sin (2x)
Cumulative Review
d
dx
p
3Ïw3
35. At t 5 }}: x 5 1, y 5 }}, and
d
dx
29. }}(y 2 1 2y) 5 }}(sec x)
3
2
Ï3w
dy
dy/dt
3 cos (p/3)
}} 5 }} 5 }} 5 2}}.
dx
dx/dt
22 sin (p/3)
2
2yy9 1 2y9 5 sec x tan x,
sec x tan x
2y 1 2
(2y 1 2)(sec 3 x 1 sec x tan 2 x) 2 2y9 sec x tan x
y0 5 }}}}}
(2y 1 2)2
2
3
(2y 1 2) (sec x 1 sec x tan 2 x) 2 2 sec 2 x tan 2 x
5 }}}}}}
(2y 1 2)3
y9 5 }},
)
(1 1 v)u9 2 uv9
(1 2 3)(21) 2 (2)(3)
5 }}}
5 21
x50
(1 1 v)
(1 2 3)2
30. }}
2
443
dx
31. (a) v 5 }} 5 3t 2 2 12t 1 9
dt
dv
a 5 }} 5 6t 2 12
dt
Ï3w
3Ï3w
(a) y 2 }} 5 2}}(x 2 1) or
2
2
Ïw3
y 5 2}}x 1 2Ï3w < 20.866x 1 3.464
2
3Ï3w
2
(b) y 2 }} 5 }}(x 2 1) or
2
Ï3w
2
5
y 5 }}x 1 }} < 1.155x 1 1.443
Ïw3
2Ïw3
(b) Solve v 5 0 for t: 3(t 2 1)(t 2 3) 5 0; t 5 1 or
t 5 3.
142
142
p
p
p
r9 5 sec 1}}2 tan 1}}2i 1 sec 1}}2 j 5 Ï2wi 1 2j, so that
4
4
4
(c) Right: v . 0 for 0 # t , 1, 3 , t # 5
left: v , 0 for 1 , t , 3
dy
2
w.
}} 5 }} 5 Ï2
dx
Ï2w
p
4
(d) a 5 0 at t 5 2, and at that instant
v 5 3(2)2 2 12(2) 1 9 5 23 m/sec
32. For x 5 1, y 5 21 and
dy
}} 5 6(1)2 2 12(1) 1 4 5 22
dx
(a) y 1 1 5 22(x 2 1) or y 5 22x 1 1
1
2
p
p
36. At t 5 }}: r 5 sec }} i 1 tan }} j 5 Ï2wi 1 j and
1
2
3
2
(b) y 1 1 5 }}(x 2 1) or y 5 }}x 2 }}
p
p
p
p
3
3
3
6
dy
p
p
p
pÏ3w
1
3 2 pÏw
3
}} 5 2}} sin }} 1 cos }} 5 2}} 1 }} 5 }}.
dx
3
3
3
2
6
6
33. For x 5 }}, y 5 }} cos }} 5 }} and
2
(a) y 2 1 5 Ï2w(x 2 Ï2w) or y 5 Ï2wx 2 1 < 1.414x 2 1
1
(b) y 2 1 5 2}}(x 2 Ï2w) or
Ïw2
1
y 5 2}}x 1 2 < 20.707x 1 2
Ïw2
37. With f (x) 5
h
2x 1 C1, x , 3
, choose C1, C2 so that
2x 1 C2, x . 3
23 1 C1 5 2(3) 1 C2 5 1.
f (x) 5
h
2x 1 4, x # 3
.
2x 2 5, x . 3
w
p
3 2 pÏ3
p
(a) y 2 }} 5 }} x 2 }} or
1
6
6
21
3
2
w
3 2 pÏ3
p
p
y 5 }} x 2 }} 1 }} < 20.407x 1 0.950
1
6
21
p
1
6
1
6
21
3
2
21
6
p
2
(b) y 2 }} 5 }} x 2 }} or
6
3
pÏ3
w23
p
2
p
y 5 }} x 2 }} 1 }} < 2.458x 2 2.050
3
6
pÏ3
w23
x
}}
2
1
1
9x
34. }}(2x) 1 }}(2yy9) 5 0; y9 5 2}
5 2}}.
2y
4
9
4y
}}
9
Ïw3
3Ïw3
At x 5 1, y 5 }}, the slope is y9 5 2}}.
2
2
Ïw3
3Ï3w
(a) y 2 }} 5 2}}(x 2 1) or
2
2
Ïw3
y 5 2}}x 1 2Ï3w < 20.866x 1 3.464
2
3Ï3w
2
(b) y 2 }} 5 }}(x 2 1)
2
Ïw3
2
5
or y 5 }}x 1 }} < 1.155x 1 1.443
Ïw3
2Ïw3
[23, 6] by [21, 5]
38. (a) x Þ 0, 2
(b) x 5 0
(c) x 5 2
(d) Absolute maximum of 2 at x 5 0:
absolute minimum of 0 at x 5 22, 2, 3
39. According to the Mean Value Theorem the driver’s speed at
111
1.5
some time was }} 5 74 mph.
444
Cumulative Review
40. (a) Increasing in [20.7, 2] (where f 9 $ 0), decreasing in
[22, 20.7] (where f 9 # 0), and has a local minimum
at x < 20.7.
(e) Local (and absolute) maximum of approximately
3.079 at
2Ïw6
2Ïw6
x 5 2}} and x 5 }};
(b) y < 22x 2 1 3x 1 3
3
3
local (and absolute) minimum of 0 at x 5 0 and
at x 5 62
(f) <(61.042, 1.853)
[23, 3] by [215, 10]
2
3
3
2
(c) f (x) 5 2}}x 3 1 }}x 2 1 3x 1 C; choose C so that
2
3
3
2
f (0) 5 1: f (x) 5 2}}x 3 1 }}x 2 1 3x 1 1.
41. f (x) 5 x 2 2 3x 2 cos x 1 C; choose C so that f (0) 5 22:
f (x) 5 x 2 2 3x 2 cos x 2 1.
43. (a) f has an absolute maximum at x 5 1 and an absolute
minimum at x 5 3.
(b) f has a point of inflection at x 5 2.
h
1
2
(c) The function f (x) 5
7
2}}Ïxw2
ww2 1 }3},
2
2
42.
2}}(x 2 1)2 1 3, 21 # x # 2
2,x#3
is one example of a function with the given properties.
[22.35, 2.35] by [20.5, 3.5]
f (x) is defined on [22, 2].
8x 2 3x 3
x3
2wx w 2 }} 5 }2 ; solve
f 9(x) 5 2xÏ4ww
Ï4ww
2wx w
2wx 2w
Ïw4w
Ï
2 6w
f 9(x) 5 0 for x to find x 5 0, x 5 6}}.
3
[23.7, 5.7] by [23, 5]
2
The graph of y 5 f 9(x) is shown.
!§§§§
A(x) 5 4x 1 2
!§§§§ 5 xÏ1w6ww2wx .
x2
16
44. y = 2 1 2 }}, and the area of the rectangle for x . 0 is
x2
}}
16
2
x2
2(8 2 x 2)
2wx 2w 2 }} 5 }}, and so
A9(x) 5 Ï1w6ww
2wx 2w
Ï1w6ww
2wx 2w
Ïw16ww
A9(x) 5 0 when x = 62Ï2w and y 5 Ï2w. The maximum
possible area is A(2Ï2w) 5 8, with dimensions
4Ï2w by Ï2w.
[22.35, 2.35] by [210, 10]
2Ï6w
3
3
43
2Ïw6
3
(a) 22, 2}} , 0, }}
3
2Ï6w
3
43
2Ïw6
3
(b) 2}}, 0 , }}, 2
4
4
Use NDER to plot f 0(x) and find that f 0(x) 5 0 for
x < 61.042.
[22.35, 2.35] by [215, 5]
(c) Approximately (21.042, 1.042)
(d) Approximately (22, 21.042), (1.042, 2)
142
142 142
p
equation is y 2 Ï2w 5 Ï2w x 2 }} or
1 42
p
y 5 Ï2w x 2 }} 1 Ï2w < 1.414x 1 0.303
1 42
p
142
p
p
p
45. f }} 5 Ï2w and f 9 }} 5 sec }} tan }} 5 Ï2w. The
46. V 5 s 3
dV 5 3s 2 ds
Since )ds) 5 0.01s, the error of the volume calculation is
approximately )dV) 5 3s 2(0.01s) 5 0.03s 3 5 0.03V, or 3%.
Cumulative Review
47. Let s be the rope length remaining and x be the horizontal
distance from the dock.
dx
s
ds
(a) x 5 Ïw
s w
2w5w, }} 5 21.5, and }} 5 }} }},
dt
dt
2w25
Ïw
s 2w
w dt
which means that for s 5 8 ft,
du
s
2 1Ïxw
}} dx 5
Ïwx
E 1}Ï2}wx 1 12dx 5 34Ïxw 1 x4 5 12 2 5
4
4
1
1
1
x
55. Let u 5 ln x, so du 5 }} dx.
dx
8
speed 5 2}} 5 2}}(21.5) < 1.9 ft/sec
dt
2w25
Ï6w4ww
w
12
1
57
2 ds
2
E
4
54.
445
5
E x(ldnxx) E
dx
Therefore, E }} 5
x(ln x)
1
u
1
ln x
Then }}2 5 u 22 du 5 2}} 1 C 5 2}} 1 C.
ds
2e
(b) u 5 sec 21 }} , so }} 5 }} }}, which for
dt
5
2w25
)s)Ïsw2w
w dt
5
s 5 8 ft becomes }}(21.5) 5 20.15 rad/sec.
2w25
8Ï6
w4ww
w
2
e
} 1 }} 5 }} < 0.409
32}ln}x 4 5 32}
14
1 1 ln 2
1 1 ln 2
1
2e
1
1
ln 2
e
48. (a) Let h be the level of the coffee in the pot, and let V be
56.
the volume of the coffee in the pot.
dh
dt
V
16p
dV/dt
16p
E3(3 2 2t)i 1 1}1t}2j4 dt 5
3(3t 2 t )i 1 (ln t)j4
3
2
9
16p
h 5 }}, so }} 5 }} 5 }} < 0.179 in./min.
5 (ln 3)j 2 2i 5 22i 1 (ln 3)j
1
(b) Now let h be the level of the coffee in the cone, and let
57. Let u 5 e x 1 1, so du 5 e x dx.
Use the identity cot2 u 5 csc2 u 2 1.
V be the volume of the coffee in the cone.
h 2
12
1 21 2 1 2
1 21 2
dV
p
dh
dh
p
}} h 5 }}h 3, so }} 5 }}h 2 }} and }}
2
dt
4
dt
dt
12
dV
4
36
}} 5 }} (29) 5 2}}
dt
25p
25p
1
V 5 }}p
3
4
5 }}2
ph
Ee
x
E
5 E(csc
cot2 (e x 1 1) dx 5 cot2 u du
2
5 2cot u 2 u 1 C
5 2cot (e x 1 1) 2 (e x 1 1) 1 C
< 20.458 in./min.
dh
dt
Since }} is negative, the level in the cone is falling at
E
E
E
1
3
4
1
50.
)x) dx 5
2x dx 1 x dx 5 2}}x 2
2
22
22
0
1
5 2 1 }} 5 2.5
2
0
22
E
22
32
3 4
0
1 2 24
2
22
Alternately, observe that the region under the curve and
above the x-axis is a semicircle of radius 2, so the area is
1
}}p(2)2 5 2p.
2
E 1x
2
E
sec2 x dx 5 tan x
3
52.
p/4
53.
2
3
4
1
1
x
3
26
5 ln 3 1 }} < 9.765
3
1
0
1 }} dx 5 }}x 3 1 ln x
p/4
3 4
0
3
1
51
2
1
2
2
122
1
2
s
5 }} tan21 u 1 C 5 }} tan21 }} 1 C
59. Let u 5 cos (x 2 3) , so du 5 2sin (x 2 3) dx.
x
x
Ï4ww
2wx 2w dx 5 }}Ï4ww
2wx 2w 1 2 sin 21 }}
5 p 2 (2p) 5 2p.
ds
1
1
du
ds
ds
E}
} 5 E}} 5 }} E}} 5 }} E}}
2 2[(s/2) 1 1]
2 u 11
s 14
4(s/2) 1 4
2
1
1 }}x 2
2
1
51. Using Number 29 in the Table of Integrals, with a 5 2,
2
ds
2
s
2
58. Let u 5 }}, so du 5 }}.
49. (a) (1)(0 1 1.8 1 6.4 1 … 1 16.2) 5 165 in.
(b) (1)(1.8 1 6.4 1 12.6 1 … 1 0) 5 165 in.
0
Since 21 1 C is an arbitrary constant, we may redefine C
and write the solution as 2cot (e x 1 1) 2 e x 1 C.
the rate of about 0.458 in./min.
1
u 2 1) du
1
3
5 9 1 ln 3 2 }}
sin (x 2 3)
E}
} dx 5 E(2u
cos (x 2 3)
3
1
2 cos (x 2 3)
5}
2 }1C
23
1
2
) du 5 }}u 22 1 C
2
446
Cumulative Review
60. Use integration by parts.
65. Use integration by parts.
u 5 e 2x
dv 5 cos 2x dx
du 5 2e 2x dx
v 5 }} sin 2x
1
2
E
E
Now let
du 5 2x dx
v 5 2cos x
2
E
sin x dx 5 2x 2 cos x 1 2x cos x dx
Now let
1
2
1
v 5 2}} cos 2x
4
u 5 e 2x
dv 5 }} sin 2x dx
du 5 2e 2x dx
dv 5 2 cos x dx
du 5 dx
v 5 2 sin x
2
E
sin x dx 5 2x 2 cos x 1 2x sin x 2 2 sin x dx
52x cos x 1 2x sin x 1 2 cos x 1 C
2
cos 2x dx
1
2
u5x
Ex
Then
Ee
dv 5 sin x dx
Ex
1
1
e 2x cos 2x dx 5 }}e 2x sin 2x 1 }}e 2x sin 2x dx
2
2
2x
u 5 x2
1
4
1
4
E
5 }}e 2x sin 2x 2 }}e 2x cos 2x 2 }} e 2x cos 2x dx
5 (2 2 x 2) cos x 1 2x sin x 1 C
so
The graph of the slope field of the differential equation
E
e2x
e 2x cos 2x dx 5 }}(2 sin 2x 2 cos 2x) 1 C
5
x12
x 2 5x 2 6
x12
(x 1 1)(x 2 6)
A
x11
dy
}} 5 x 2 sin x and the antiderivative y 5 (2 2 x 2) cos x 1
dx
2x sin x is shown below.
B
x26
61. }
} 5 }} 5 }} 1 }}
2
x 1 2 5 A (x 2 6) 1 B(x 1 1) 5 (A 1 B) x 1 (B 2 6A)
1
7
8
7
Solving A 1 B 5 1, B 2 6A 5 2 yields A 5 2}}, B 5 }} so
x12
8
1
}
} 5 }} 2 }}. Then
x 2 2 5x 2 6
7(x 2 6)
7(x 1 1)
x12
8
1
}
} dx 5 }} 2 }} dx
x 2 2 5x 2 6
7(x 2 6)
7(x 1 1)
8
1
1
(x 2 6)8
5 }} ln )x 2 6) 2 }} ln )x 1 1) 1 C 5 }} ln }} 1 C
7
7
7
)x 1 1)
E
E1
2
62. Area < }}[3 1 2(8.3) 1 2(9.9) 1 … 1 2(8.3) 1 3] 5 359;
5
2
Volume < 25 3 359 5 8975 ft 3
[25, 5] by [210, 10]
66. Use integration by parts.
u5x
dv 5 e x dx
du 5 dx
Ex e
x
v 5 ex
E
dx 5 xe x 2 e x dx 5 xe x 2 e x 1 C5 e x(x 2 1) 1 C
Confirm by differentiation:
1
2
7
1
7
1
C 5 }} and y 5 2}} 2 }}e 22t 1 }}.
2
2
2
t11
1
2
63. y 5 2(t 1 1)21 2 }}e 22t 1 C; y (0) 5 21 2 }} 1 C 5 2, so
12
1
p
64. y9 5 2}} cos 2u 2 sin u 1 C1, and y9 }} 5 0 ⇒
2
2
1
1
y9 5 2}} cos 2u 2 sin u 1 }}.
2
2
1
1
p
y 5 2}} sin 2u 1 cos u 1 }} u 1 C2, and y }} 5 0
4
2
2
1
1
p
⇒ y 5 2}} sin 2u 1 cos u 1 }}u 2 }}
4
2
4
12
d
}}[e x(x 2 1) 1 C] 5 e x 1 (x 2 1)e x 5 xe x
dx
67. (a) y 5 Ce kt, with 6,000 5 Ce k(2) and 10,000 5 Ce k(5).
10,000
6,000
5
3
Then }} 5 e k(522), so }} 5 e 3k and therefore
12
5
ln }3}
k 5 } < 0.170.
3
6,000
Furthermore, C 5 }2}
< 4268. The approximate number
e k
of bacteria is given by y 5 4268e 0.170t.
(b) About 4268
Cumulative Review
68. Let t be the time in minutes where t 5 0 represents right
now, and let T(t) be the number of degrees above room
temperature. Then we may write T(t) 5 T0e 2kt where
T(0) 5 50 and T(215) 5 65, giving T0 5 50 and
1
15
13
10
k 5 }} ln }} < 0.0175.
(a) 50e 2k(120) < 6.13°C above room temperature.
ln 0.1
2k
72. The region has four congruent portions, so
Area 5 4
1
2
dy
y
dx
500
500 dy
}} 5 0.08 dx
y(500 2 y)
(500 2 y) 1 y
}} dy 5 0.08 dx
y(500 2 y)
1
1
}} 1 }} dy 5 0.08 dx
y
500 2 y
69. }} 5 0.08y 1 2 }}
1
E
p/2
4
1
2
0
2x 2 5 8 ⇒ x 5 62. Then
Area 5
E
2
22
3
[(5 2 x 2) 2 (x 2 2 3)] dx 5
4
2
3
5 8x 2 }}x 3
p/2
54
0
2
64
3
E
2
(8 2 2x 2) dx
22
5 }}
22
74. Solve y 2 3 5 y 1 2 to find the integration limits:
2
w1w
1 6 Ï2
y 2 2 y 2 5 5 0 ⇒ y 5 }}. Then
Area 5
E
2
(1 1 Ï2
w1
w)/2
w1
w)/2
(1 2 Ï2
1
2
75. Area 5 }}
E
[(y 1 2) 2 (y 2 2 3) dy < 16.039.
2p
1
2
r 2 du 5 }}
0
E
2p
0
9(1 1 cos u)2 du
E (1 1 2 cos u 1 cos u) du
9
1 1 cos 2u
5 }} E 11 1 2 cos u 1 }}2 du
2
2
9
3
1
5 }} E 1}} 1 cos u 1 }} cos 2u2 du
2
2
2
2p
9
2
5 }}
2
3
sin 2x dx 5 4 2}} cos 2x
73. Solve 5 2 x 2 5 x 2 2 3 to find the integration limits:
(b) Solving 5 5 50e 2kt gives t 5 }} < 131.6 minutes,
or about 2 hours and 12 minutes from now.
447
2
0
2p
0
Integrate both sides.
2p
ln )y) 2 ln )500 2 y)5 0.08x 1 C1
3
9 3
2 2
y ? (1 1 C2e
) 5 500C2e
0.08x
500
1 1 Ce
y 5 }}
20.08x
E
C1 (x 2/2)13x
y24 5e e
y 5 Ce(x
2
/2)13x
14
14
4
2p
0
9
27p
5 }} (3p 2 0) 5 }} < 42.412
2
2
E p1}x2}2 dx 5 }p4}3}17}x 4
1
76. Volume 5
dy
70.
}} 5 (y 2 4)(x 1 3)
dx
dy
}} 5 (x 1 3) dx
y24
dy
}} 5 (x 1 3) dx
y24
x2
ln )y 2 4) 5 }} 1 3x 1 C1
2
E
1
4
5 }} }}u 1 2 sin u 2 }} sin 2u
y
}} 5 C2e 0.08x
500 2 y
0.08x
0
3 2
7
21
1
p
14
5 }} < 0.224
21
77. Solve 4x 2 x 2 5 0 to find the limit of integration:
x 5 0 or x 5 4. By the cylindrical shell method,
E 2px(4x 2 x ) dx 5 2p E
4
1
128p
5 2p }}x 2 }}x 5 }}
33 4 4 3
4
Volume 5
2
4
0
0
3
4
(4x 2 2 x 3) dx
4
0
< 134.041.
78. The average value is the integral divided by the interval
length. Using NINT,
71. Use EULERT.
x
y
0
0.1
0.2
0.3
0.4
0.5
0.6
0.7
0.8
0.9
1.0
0
0.1
0.2095
0.3285
0.4568
0.5946
0.7418
0.8986
1.0649
1.2411
1.4273
1
p
average value 5 }}
E Ïsiwnwwx dx < 0.763
p
0
79. y9 5 sec 2 x, so we may use NINT to obtain
Length 5
E
p/4
Ï1ww
1w(se
ww
c 2wxw
)2 dx < 2.556.
2p/4
dx
dt
dy
dt
80. }} 5 cos t and }} 5 1 2 sin t, so we may use NINT to
obtain
E
5E
Length 5
p/2
Ïco
ww
s 2wtw
1w(1ww
2wsin
wwtw
)2 dt
2p/2
p/2
Ï2ww
2w2wsin
wwt dt 5 4.
2p/2
448
Cumulative Review
81. Using NINT,
Length 5
E !u§§1§§1}§d}§u §2 du 5 E Ï1ww1wuw du < 6.110.
p
p
dr 2
2
0
88. (a) The work required to raise a thin disk at height y from
2
the bottom is
0
y 2
5
dx
dt
E pe
2
E
Total work 5
!§§§1§§§§2
2x/2
5 15p
Ï4ww
1we 2
wxw dx < 8.423.
0
E
5E
Area 5
0
p/2
0
E
10
0
E
10
0
15py 2(12 2 y) dy
3
4
1
4
(2y 3 1 12y 2) dy 5 15p 2}}y 4 1 4y 3
5 22,500p < 70,686 ft-lb.
dy
dt
83. }} 5 cos t and }} 5 1 2 sin t, so
p/2
3 1 2 2 dy4(12 2 y).
(weight)(distance) 5 60p }}
dy
1
82. }} 5 2}}e 2x/2, so we may use NINT to obtain
dx
2
2
2e 2 x/2 2
Area 5 2pe 2x/2 1 1 }} dx
2
0
10
0
22,500p
275
(b) }} < 257 sec 5 4 min, 17 sec
2p sin t Ïco
ww
s 2wtw
1w(1ww
2wsin
wwtw
)2 dt
2p sin t Ï2ww
2w2wsin
wwt dt < 3.470.
89. The sideways force exerted by a thin disk at depth y is its
edge area times the pressure, or
dr
84. }} 5 1, so we may use NINT to obtain
du
p
Area 5
E
(2p dy)(849y) 5 1698py dy.
2pu sin uÏuw2w+
ww1 du < 32.683.
Total force 5
p/2
2
⇒H5
0
1
5/2
4
p 1
4 2
3
4
7
1
5
1
4
E
f (x) 5 ln x grows slower than g (x) 5 Ïxw.
1
t 24
91. Use the limit comparison test with f (t) 5 }
2 } and
1
t
g(t) 5 }}2 . Since f and g are both continuous on [3, `),
p (2 tan x) dx
0
E
5 8p E
2
p/4
5 8p
0
p/4
0
f (t)
t→` g(t)
tan2 x dx
E
`
3
4
1
x
1
ln x
lim