Several Variable Calculus

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Math 221
Examination 2
Spring 2013
Several Variable Calculus
Instructions These problems should be viewed as essay questions. Before making a calculation, you should explain in words what your strategy is.
Please write your solutions on your own paper. Each of the 10 problems counts
for 10 points.
1
πœ‹βˆ•2
1. Evaluate the iterated integral
∫0
∫0
π‘₯ cos(π‘₯𝑦) d𝑦 dπ‘₯.
Solution. Observe that π‘₯ cos(π‘₯𝑦) is the 𝑦-partial derivative of sin(π‘₯𝑦). Then
1
πœ‹βˆ•2
∫0
∫0
πœ‹βˆ•2
π‘₯ cos(π‘₯𝑦) d𝑦 dπ‘₯ =
∫0
|𝑦=1
sin(π‘₯𝑦) | dπ‘₯
|𝑦=0
πœ‹βˆ•2
=
∫0
(sin(π‘₯) − 0) dπ‘₯
|πœ‹βˆ•2
= − cos(π‘₯) |
|0
= − cos(πœ‹βˆ•2) + cos(0)
= 1.
2. Describe the solid whose volume is given by the spherical-coordinate triple
integral
πœ‹
πœ‹
∫0 ∫0 ∫1
2
𝜌2 sin(πœ™) d𝜌 dπœ™ dπœƒ.
(You do not need to evaluate the integral.)
Solution. Notice that 𝜌2 sin(πœ™) d𝜌 dπœ™ dπœƒ is d𝑉 , the volume element, expressed in spherical coordinates. Since 𝜌 goes from 1 to 2, the solid is contained in the shell between a sphere of radius 1 and a sphere of radius 2. The
angle πœ™ goes from 0 to πœ‹, its maximum range, so this angle does not restrict
the solid. The angle πœƒ goes from 0 to πœ‹, half its maximum range, so the solid
lies in the half-space where 𝑦 > 0. Thus the solid is a hemisphere of radius 2
with a concentric hemisphere of radius 1 removed.
The problem does not ask for the value of the integral. But that value works
out to 14πœ‹βˆ•3.
March 28, 2013
Page 1 of 6
Dr. Boas
Math 221
Examination 2
Spring 2013
Several Variable Calculus
𝑦
π‘₯𝑒𝑦 d𝐴, where 𝐷 is the region in the first
∬𝐷
quadrant bounded by the line 𝑦 = 0, the line π‘₯ = 1, and the parabola 𝑦 = π‘₯2 .
3. Evaluate the double integral
π‘₯
Solution. The convenient method is to integrate with respect to 𝑦 first:
π‘₯2
1
𝑦
∬𝐷
π‘₯𝑒 d𝐴 =
π‘₯𝑒𝑦 d𝑦 dπ‘₯
∫0 ∫0
1
|𝑦=π‘₯
=
π‘₯𝑒 |
dπ‘₯
|𝑦=0
∫0
1 (
)
2
π‘₯ 𝑒π‘₯ − 1 dπ‘₯
=
∫0
1
)
𝑒=π‘₯2
1( 𝑒
𝑒 − 1 d𝑒
=
∫0 2
]1
1[ 𝑒
=
𝑒 −𝑒 0
2
]
1[
=
(𝑒 − 1) − (1 − 0)
2
𝑒−2
=
.
2
2
𝑦
4. Find the volume of the solid bounded by the cylinder π‘₯2 + 𝑦2 = 1 and the
planes 𝑧 = 0 and π‘₯ + 𝑧 = 2.
Solution. One method is to use cylindrical coordinates. The variable 𝑧 goes
from 0 to 2 − π‘₯, or 2 − π‘Ÿ cos(πœƒ). Since the equation π‘₯2 + 𝑦2 = 1 describes a
circle of radius 1, the angle πœƒ is unrestricted, and π‘Ÿ goes from 0 to 1. Here
is the iterated integral:
2πœ‹
∫0
March 28, 2013
1
∫0 ∫0
2−π‘Ÿ cos(πœƒ)
2πœ‹
π‘Ÿ d𝑧 dπ‘Ÿ dπœƒ =
1
(2 − π‘Ÿ cos(πœƒ))π‘Ÿ dπ‘Ÿ dπœƒ
∫0
]1
2πœ‹ [
1 3
2
=
π‘Ÿ − π‘Ÿ cos(πœƒ) dπœƒ
∫0
3
0
]
2πœ‹ [
1
=
1 − cos(πœƒ) dπœƒ
∫0
3
= 2πœ‹.
∫0
Page 2 of 6
Dr. Boas
Math 221
Examination 2
Spring 2013
Several Variable Calculus
2
𝑦2
𝑦
𝑓 (π‘₯, 𝑦, 𝑧) d𝑧 dπ‘₯ d𝑦 as an iterated integral
5. Rewrite the integral
∫0 ∫0 ∫0
in the order dπ‘₯ d𝑦 d𝑧.
Solution. The solid lies in the first octant (since all three variables start at 0).
The solid lies under the parabolic cylinder 𝑧 = 𝑦2 (with axis along the π‘₯axis) and between the plane π‘₯ = 𝑦 and the 𝑦𝑧 plane. Also the solid stops at
the plane 𝑦 = 2.
√
Consequently, the variable π‘₯ goes from 0 to 𝑦; then 𝑦 goes from 𝑧 to 2, and
𝑧 goes from 0 to 4 (since the equation 𝑧 = 𝑦2 says that 𝑧 = 4 when 𝑦 = 2).
Here is the iterated integral:
4
2
∫0 ∫√𝑧 ∫0
𝑦
𝑓 (π‘₯, 𝑦, 𝑧) dπ‘₯ d𝑦 d𝑧.
6. Set up an integral for the surface area of the part of the paraboloid 𝑧 = π‘₯2 +𝑦2
that lies between the plane 𝑧 = 1 and the plane 𝑧 = 4.
(You do not need to evaluate the integral.)
Solution. The surface area element is
√
( )2 ( )2 √
πœ•π‘§
πœ•π‘§
+
= 1 + (2π‘₯)2 + (2𝑦)2
1+
πœ•π‘₯
πœ•π‘¦
√
= 1 + 4(π‘₯2 + 𝑦2 ).
Since 𝑧 goes from 1 to 4, the surface lies over the region in the π‘₯𝑦-plane
between the circle 1 = π‘₯2 +𝑦2 and the circle 4 = π‘₯2 +𝑦2 (which has radius 2).
Because of the circular symmetry, it is convenient to write the integral in
polar coordinates:
2πœ‹
2√
1 + 4π‘Ÿ2 π‘Ÿ dπ‘Ÿ dπœƒ.
∫0 ∫1
The problem
does not ask)for the value of the integral. But the value works
( √
√
πœ‹
out to
17 17 − 5 5 .
6
March 28, 2013
Page 3 of 6
Dr. Boas
Math 221
Examination 2
Spring 2013
Several Variable Calculus
𝑦
π‘₯
−1
7. Let 𝐷 be the square with vertices (1, 0), (0, 1), (−1, 0), and (0, −1). Rewrite
the double integral ∬𝐷 (π‘₯ + 𝑦)5 d𝐴 as an integral with respect to d𝑒 d𝑣, where
𝑒 = π‘₯ + 𝑦 and 𝑣 = π‘₯ − 𝑦.
(You do not need to evaluate the integral.)
−1
Solution. Compute the Jacobian:
| πœ•π‘’
|
πœ•(𝑒, 𝑣) || πœ•π‘₯
=
πœ•(π‘₯, 𝑦) || πœ•π‘£
| πœ•π‘₯
|
πœ•π‘’ ||
|
1||
πœ•π‘¦ || = ||1
πœ•π‘£ || |1 −1|| = −2.
|
|
πœ•π‘¦ ||
The area-magnification factor for the change of variables is the absolute
value of the Jacobian, so d𝑒 d𝑣 = 2 dπ‘₯ d𝑦, or dπ‘₯ d𝑦 = 21 d𝑒 d𝑣.
The side of the square in the first quadrant of the π‘₯𝑦-plane is part of the line
π‘₯ + 𝑦 = 1, which turns into the equation 𝑒 = 1. Similarly, the parallel side
in the third quadrant turns into the equation 𝑒 = −1. The side in the fourth
quadrant is part of the line π‘₯ − 𝑦 = 1, which corresponds to 𝑣 = 1, and the
parallel side in the second quadrant corresponds to 𝑣 = −1.
Consequently, the new integral in the 𝑒𝑣-plane is
1
1
∫−1 ∫−1
1 5
𝑒 d𝑒 d𝑣.
2
The problem does not ask for the value of the integral. But the value is 0 by
symmetry!
8. Find the work done by the force field 𝐹⃗ (π‘₯, 𝑦) = 𝑦2 πš€Μ‚ + 2π‘₯𝑦 πš₯Μ‚ on a particle that
moves in a straight line from the point (1, 2) to the point (5, 1).
Solution. One method is to observe that 𝐹⃗ (π‘₯, 𝑦) = ∇(π‘₯𝑦2 ). Therefore the
work integral ∫ 𝐹⃗ ⋅ dβƒ—π‘Ÿ equals
|(5,1)
π‘₯𝑦2 | = 5 − 4 = 1.
|(1,2)
Another method is to parametrize the line via
π‘₯ = 1 + 4𝑑
𝑦=2−𝑑
March 28, 2013
Page 4 of 6
0 ≤ 𝑑 ≤ 1.
Dr. Boas
Math 221
Examination 2
Spring 2013
Several Variable Calculus
Then dπ‘₯ = 4 d𝑑 and d𝑦 = − d𝑑, so
∫
𝐹⃗ ⋅ dβƒ—π‘Ÿ =
=
𝑦2 dπ‘₯ + 2π‘₯𝑦 d𝑦
∫
1
[
1
( 2
)
12𝑑 − 30𝑑 + 12 d𝑑
∫0
=
]
(2 − 𝑑)2 (4) + 2(1 + 4𝑑)(2 − 𝑑)(−1) d𝑑
∫0
= 4 − 15 + 12
= 1.
𝑦 d𝑠 when the parametric equations of 𝐢 are
∫𝐢
π‘₯ = 𝑑2 and 𝑦 = 2𝑑, where 0 ≤ 𝑑 ≤ 1.
9. Evaluate the line integral
Solution. The arc length element d𝑠 equals
√
( )2 ( )2
√
√
( )2
d𝑦
dπ‘₯
+
d𝑑 =
2𝑑 + 22 d𝑑 = 2 𝑑2 + 1 d𝑑.
d𝑑
d𝑑
Therefore
1
∫𝐢
𝑦 d𝑠 =
∫0
√
)3βˆ•2 |1 4 [ 3βˆ•2
]
4(2
4𝑑 𝑑2 + 1 d𝑑 =
𝑑 +1
2 −1 .
|=
|0 3
3
10. What does it mean to say that a vector field 𝐹⃗ is a conservative vector field?
Solution. A conservative vector field is the same thing as a gradient vector
field: there exists a function 𝑓 such that 𝐹⃗ = ∇𝑓 .
March 28, 2013
Page 5 of 6
Dr. Boas
Math 221
Examination 2
Spring 2013
Several Variable Calculus
Optional bonus problem for extra credit
Find the volume of an egg whose eggshell has the equation
π‘₯ 2 𝑦2 𝑧 2
+
+
= 1.
8
5
3
Solution. The problem asks for ∭𝐷 d𝑉 , where 𝐷 is the region inside the surface.
√
√
√
One method√
is to change variables via π‘₯ = 𝑒 8 and 𝑦 = 𝑣 5 and 𝑧 = 𝑀 3. Then
dπ‘₯ d𝑦 d𝑧 = 120 d𝑒 d𝑣 d𝑀, and the equation of the surface in the new coordinates
becomes 𝑒2 + 𝑣2 + 𝑀2 = 1, a sphere of radius 1. Since the volume of a ball of
radius π‘Ÿ equals 43 πœ‹π‘Ÿ3 , the volume of a ball of radius 1 equals 43 πœ‹. Accordingly,
∭𝐷
( )
√
d𝑉 = 120 34 πœ‹ ,
or
√
8πœ‹ 30
.
3
(If you forgot the formula for the volume of a ball of radius 1, then you could
compute it in spherical coordinates as
2πœ‹
∫0
1
πœ‹
∫0 ∫0
𝜌2 sin(πœ™) d𝜌 dπœ™ dπœƒ,
which works out to 4πœ‹βˆ•3.)
March 28, 2013
Page 6 of 6
Dr. Boas
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