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Math-2 Final Revision (1)

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Mathematics – 02
Final Revision
By: Mahmoud Osama & Mido
Revised By : Akram Gamal
Karem Moamen
Edited By : Mahmoud Osama & Nourhan Osama
Thanks to : Omar Atya
Table of Contents
Limits & Continuity ............................................................................................................. 002
Improper & Proper Fractions ......................................................................................... 010
Partial Derivatives ............................................................................................................... 033
Fourier Series ......................................................................................................................... 060
Maximum & Minimum Values ........................................................................................ 076
Taylor’s Theorem ................................................................................................................. 082
Improper Integrals .............................................................................................................. 094
Ellipse ........................................................................................................................................ 115
Parabola ..................................................................................................................................... 123
Series .......................................................................................................................................... 130
Page | 1
Choose The Correct Answer :
1] Is this limits π’π’Šπ’Ž(𝒙,π’š)→(𝟎,𝟎)
π’™πŸ −π’šπŸ
π’™πŸ +π’šπŸ
exists or not ?
A- It exists
C- 𝟏
B- No , it doesn’t exist
D- ( −𝟏 )
Solution:
By Substitution: π‘™π‘–π‘š(π‘₯,𝑦)→(0,0)
π‘₯ 2 −𝑦 2
π‘₯ 2 +𝑦 2
= π‘™π‘–π‘š(π‘₯,𝑦)→(0,0)
0
0
= 𝑒𝑛𝑑𝑒𝑓𝑖𝑛𝑒𝑑
There is no Simplification
By Using Paths method
1] On X-axis , at 𝑦 = 0 , π‘™π‘–π‘šπ‘₯→0
2] On Y-axis , at π‘₯ = 0 , π‘™π‘–π‘šπ‘¦→0
π‘₯ 2 −0
π‘₯ 2 +0
0−𝑦 2
0+𝑦 2
= π‘™π‘–π‘šπ‘₯→0
= π‘™π‘–π‘šπ‘¦→0
π‘₯2
π‘₯2
= π‘™π‘–π‘šπ‘₯→0 1 = 1 = 𝐿1
−𝑦 2
𝑦2
= π‘™π‘–π‘šπ‘¦→0 − 1 = −1 = 𝐿2
Since 𝐿1 ≠ 𝐿2 , Then It doesn’t exist
Choice B
2] Is this limits π’π’Šπ’Ž(𝒙,π’š)→(𝟎,𝟎)
A- It exists at
−𝟐
πŸ‘
B- No , it doesn’t exist
π’™πŸ −𝟐
πŸ‘+π’š
exists or not ?
C- 𝟏
D- ( −𝟏 )
Solution:
By Substitution: π‘™π‘–π‘š(π‘₯,𝑦)→(0,0)
Page | 2
π‘₯ 2 −2
3+𝑦
= π‘™π‘–π‘š(π‘₯,𝑦)→(0,0)
−2
3
=
−2
3
Then It exist at
−2
3
Choice A
3] Is this limits π’π’Šπ’Ž(𝒙,π’š)→(𝟎,𝟎)
A- It exists at
π’™πŸ +πŸ‘π’šπŸ
π’™πŸ +π’šπŸ
exists or not ?
C- 𝟏
B- No , it doesn’t exist
D- πŸ‘
Solution:
By Substitution: π‘™π‘–π‘š(π‘₯,𝑦)→(0,0)
π‘₯ 2 +3𝑦 2
0
= = 𝑒𝑛𝑑𝑒𝑓𝑖𝑛𝑒𝑑
π‘₯ 2 +𝑦 2
0
There is no Simplification
By Using Paths method
1] On X-axis , at 𝑦 = 0 , π‘™π‘–π‘šπ‘₯→0
2] On Y-axis , at π‘₯ = 0 , π‘™π‘–π‘šπ‘¦→0
π‘₯ 2 +3𝑦 2
π‘₯ 2 +𝑦 2
π‘₯ 2 +3𝑦 2
π‘₯ 2 +𝑦 2
= π‘™π‘–π‘šπ‘₯→0
= π‘™π‘–π‘šπ‘¦→0
π‘₯ 2 +0
π‘₯ 2 +0
= π‘™π‘–π‘šπ‘₯→0 1 = 1 = 𝐿1
0+3𝑦 2
0+𝑦 2
= π‘™π‘–π‘šπ‘¦→0 3 = 3 = 𝐿2
Since 𝐿1 ≠ 𝐿2 , Then It doesn’t exist
Choice B
4] Is this limits π’π’Šπ’Ž(𝒙,π’š)→(𝟏,𝟎)
π’š
𝒙+π’š−𝟏
A- It exists
C- 𝟏
B- No , it doesn’t exist
D- 𝟎
exists or not ?
Solution:
By Substitution: π‘™π‘–π‘š(π‘₯,𝑦)→(1,0)
Page | 3
𝑦
π‘₯+𝑦−1
= π‘™π‘–π‘š(π‘₯,𝑦)→(1,0)
0
1+0−1
0
= = 𝑒𝑛𝑑𝑒𝑓𝑖𝑛𝑒𝑑
0
There is no Simplification
By Using Paths method
1] On X-axis , at 𝑦 = 0 , π‘™π‘–π‘šπ‘₯→1
2] On Y-axis , at π‘₯ = 1 , π‘™π‘–π‘šπ‘¦→0
0
π‘₯+0−1
𝑦
1+𝑦−1
= π‘™π‘–π‘šπ‘₯→1 0 = 0 = 𝐿1
= π‘™π‘–π‘šπ‘¦→0 1 = 1 = 𝐿2
Since 𝐿1 ≠ 𝐿2 , Then It doesn’t exist
Choice B
5] Is this limits π’π’Šπ’Ž(𝒙,π’š)→(𝟎,𝟎)
π’™π’š
π‘₯2 +𝑦2
exists or not ?
𝟏
A- It exists
C- 𝟐
B- No , it doesn’t exist
D- 𝟎
Solution:
By Substitution: π‘™π‘–π‘š(π‘₯,𝑦)→(0,0)
π‘₯𝑦
π‘₯ 2 +𝑦 2
0
= = 𝑒𝑛𝑑𝑒𝑓𝑖𝑛𝑒𝑑
0
There is no Simplification
By Using Paths method
π‘₯∗0
1] On X-axis , at 𝑦 = 0 , π‘™π‘–π‘šπ‘₯→0
π‘₯ 2 +02
2] On Y-axis , at π‘₯ = 0 , π‘™π‘–π‘šπ‘¦→0
02 +𝑦 2
3] at π‘₯ = 𝑦 , π‘™π‘–π‘šπ‘¦→0
𝑦∗𝑦
𝑦 2 +𝑦 2
0∗𝑦
= π‘™π‘–π‘šπ‘¦→0
= 0 = 𝐿1
= 0 = 𝐿2
𝑦2
2𝑦 2
= π‘™π‘–π‘šπ‘¦→0
Since 𝐿1 = 𝐿2 ≠ 𝐿3 , Then It doesn’t exist
Choice B
Page | 4
1
2
1
= = 𝐿3
2
6] Is this limits π’π’Šπ’Ž(𝒙,π’š)→(𝟎,𝟎)
π’™π’šπŸ
π‘₯2 +𝑦4
exists or not ?
𝟏
A- It exists
C- 𝟐
B- No , it doesn’t exist
D- 𝟎
Solution:
π‘₯𝑦 2
By Substitution: π‘™π‘–π‘š(π‘₯,𝑦)→(0,0)
π‘₯ 2 +𝑦 4
0
= = 𝑒𝑛𝑑𝑒𝑓𝑖𝑛𝑒𝑑
0
There is no Simplification
By Using Paths method
1] On X-axis , at 𝑦 = 0 , π‘™π‘–π‘šπ‘₯→0
2] On Y-axis , at π‘₯ = 0 , π‘™π‘–π‘šπ‘¦→0
3] at π‘₯ = 𝑦 , π‘™π‘–π‘šπ‘¦→0
2
4] at π‘₯ = 𝑦 ,
𝑦∗𝑦 2
𝑦 2 +𝑦 4
= π‘™π‘–π‘šπ‘¦→0
π‘₯∗02
π‘₯ 2 +04
0∗𝑦 2
02 +𝑦 4
𝑦3
𝑦 2 +𝑦 4
𝑦 2 ∗𝑦 2
π‘™π‘–π‘šπ‘¦→0 (𝑦2 )2 4
+𝑦
= 0 = 𝐿1
= 0 = 𝐿2
= π‘™π‘–π‘šπ‘¦→0
= π‘™π‘–π‘šπ‘¦→0
𝑦 2 (𝑦)
𝑦 2 (1+𝑦2 )
𝑦4
2𝑦 4
= π‘™π‘–π‘šπ‘¦→0
= π‘™π‘–π‘šπ‘¦→0
𝑦
1+𝑦 2
1
2
= π‘™π‘–π‘šπ‘¦→0 0 = 0 = 𝐿3
1
= = 𝐿4
2
Since 𝐿1 = 𝐿2 = 𝐿3 ≠ 𝐿4 , Then It doesn’t exist
Choice B
7] Is this limits π’π’Šπ’Ž(𝒙,π’š)→(𝟏,𝟐) (πŸ“π’™πŸ‘ − π’™πŸ π’šπŸ ) exists or not ?
A- It exists at 𝟏
C- It exists at −𝟏
B- No , it doesn’t exist
D- 𝟏
Solution:
By Substitution:
π‘™π‘–π‘š(π‘₯,𝑦)→(1,2) (5π‘₯ 3 − π‘₯ 2 𝑦 2 ) = 5 ∗ 13 − 12 ∗ 22 = 1
Page | 5
Then it exists at 1
Choice A
8] Is this limits π’π’Šπ’Ž(𝒙,π’š)→(𝟎,𝟎)
𝑦 2 sin2 π‘₯
π‘₯ 4 +𝑦 4
A- It exists
C- 𝟎
B- No , it doesn’t exist
D- 𝟏
exists or not ?
Solution:
By Substitution: π‘™π‘–π‘š(π‘₯,𝑦)→(0,0)
𝑦 2 sin2 π‘₯
π‘₯ 4 +𝑦4
0
= = 𝑒𝑛𝑑𝑒𝑓𝑖𝑛𝑒𝑑
0
There is no Simplification
By Using Paths method
1] On X-axis , at 𝑦 = 0 , π‘™π‘–π‘šπ‘₯→0
2] On Y-axis , at π‘₯ = 0 , π‘™π‘–π‘šπ‘¦→0
3] at π‘₯ = 𝑦 , π‘™π‘–π‘šπ‘¦→0
𝑦 2 sin2 𝑦
𝑦 4 +𝑦 4
= π‘™π‘–π‘šπ‘¦→0
02 sin2 π‘₯
π‘₯ 4 +04
𝑦 2 sin2 0
04 +𝑦 4
sin2 𝑦
2𝑦 2
= 0 = 𝐿1
= 0 = 𝐿2
= π‘™π‘–π‘šπ‘¦→0
1
2
∗ π‘™π‘–π‘šπ‘¦→0
sin2 𝑦
𝑦2
1
1
2
2
= ∗ 1 = = 𝐿3
Since 𝐿1 = 𝐿2 ≠ 𝐿3 , Then It doesn’t exist
Choice B
9] Is this limits π’π’Šπ’Ž(𝒙,π’š)→(𝟏,−𝟏) 𝒆−π’™π’š 𝐜𝐨𝐬(𝒙 + π’š) exists or not ?
A- It exists at 𝒆
C- It exists at 𝟎
B- No , it doesn’t exist
D- 𝟏
Solution:
By Substitution: π‘™π‘–π‘š(π‘₯,𝑦)→(1,−1) 𝑒 −(1∗−1) π‘π‘œπ‘ (1 + (−1)) = 𝑒
Then it exists at 𝑒
Choice A
Page | 6
πŸ’−π’™π’š
10] Is this limits π’π’Šπ’Ž(𝒙,π’š)→(𝟐,𝟏) π’™πŸ +πŸ‘π’šπŸ exists or not ?
𝟐
A- It exists at πŸ•
C- It exists at 𝟎
B- No , it doesn’t exist
D- 𝟏
Solution:
By Substitution: π‘™π‘–π‘š(π‘₯,𝑦)→(2,1)
Then it exists at
4−2∗1
22 +3∗12
=
2
7
2
7
Choice A
𝒙−π’‚π’š
11] π’π’Šπ’Ž(𝒙,π’š)→(𝟎,𝟎) 𝒙+π’‚π’š along the path π’š = 𝟎
𝒂
A- 𝟎
C- 𝒃
B- 𝟏
D- None of them
Solution:
By Substitution: π‘™π‘–π‘šπ‘₯→0
π‘₯−π‘Ž∗0
π‘₯+π‘Ž∗0
=
π‘₯
π‘₯
=1
Choice B
π’™πŸ +π’šπŸ
12] π’π’Šπ’Ž [π’π’Šπ’Ž π’™πŸ −π’šπŸ] =
π’š→𝟎
𝒙→𝟎
A- 𝟎
C- 𝟏
B- −𝟏
D- None of them
Page | 7
Solution:
π‘™π‘–π‘š
π‘₯ 2 +𝑦 2
π‘₯→0 π‘₯ 2 −𝑦 2
π‘™π‘–π‘š [π‘™π‘–π‘š
=
02 +𝑦 2
02 −𝑦 2
π‘₯ 2 +𝑦2
𝑦→0 π‘₯→0 π‘₯ 2 −𝑦2
=
𝑦2
−𝑦 2
= −1
] = π‘™π‘–π‘š[−1] = −1
𝑦→0
Choice B
13] Determine the set of points at which the function is Continuous
𝒇(𝒙, π’š) =
π’™π’š
𝟏+𝒆𝒙−π’š
A- It is continuous on 𝐑
C- It is continuous on 𝐑 − {𝟎}
B- It is continuous on 𝐑 − {−𝟏}
D- It isn’t continuous on 𝐑
Solution:
We first find the Domain , then the function is continuous at its Domain
Domain of the numerator ; the Domain of (π‘₯𝑦) is R
Domain of the Denominator ; the Domain of (1 + 𝑒 π‘₯−𝑦 ) is R
1 + 𝑒 π‘₯−𝑦 ≠ 0 , 𝑒 π‘₯−𝑦 ≠ −1
So the function is continuous on R
Choice A
14] Determine the set of points at which the function is Continuous
𝒇(𝒙, π’š) =
𝟏+π’™πŸ +π’šπŸ
𝟏−π’™πŸ −π’šπŸ
Solution:
βž” 1 − π‘₯ 2 − 𝑦2 ≠ 0 , π‘₯ 2 + 𝑦2 ≠ 1 , 𝑦2 ≠ 1 − π‘₯ 2
𝑦 ≠ √1 − π‘₯ 2
Page | 8
Then: function is continuous at: ∀(π‘₯, 𝑦) ∈ 𝑅 | 𝑦 ≠ √1 − π‘₯ 2
Domain = { 𝑦 ∈ 𝑅: 𝑦 ≠ √1 − π‘₯ 2 }
15] Determine the set of points at which the function is Continuous
𝒇(𝒙, π’š) = 𝒍𝒏(π’™πŸ + π’šπŸ − πŸ’)
Solution:
βž” π‘₯ 2 + 𝑦 2 − 4 > 0 , π‘₯ 2 + 𝑦 2 > 4 , π‘₯ 2 > 4 − 𝑦 2 , π‘₯ > √4 − 𝑦 2
Domain = { π‘₯ ∈ 𝑅: π‘₯ > √4 − 𝑦 2 }
Page | 9
πŸ•π’™−πŸπŸ“
16] The partial Fraction decomposition of π’™πŸ −πŸ•π’™+𝟏𝟐 is
πŸ’
πŸ‘
πŸ’
πŸ‘
A- 𝒙−πŸ‘ + 𝒙−πŸ’
πŸ’
πŸ‘
πŸ’
πŸ‘
C- 𝒙−πŸ‘ − 𝒙−πŸ’
B- 𝒙+πŸ‘ − 𝒙+πŸ’
D- 𝒙+πŸ‘ + 𝒙−πŸ’
Solution:
7π‘₯−25
7π‘₯−25
π‘₯ 2 −7π‘₯+12
= (π‘₯−3)(π‘₯−4) =
7π‘₯−25
(π‘₯−3)(π‘₯−4)
=
A
π‘₯−3
+
B
(Proper Fraction)
π‘₯−4
𝐴(π‘₯−4)+𝐡(π‘₯−3)
(π‘₯−3)(π‘₯−4)
Then: 7π‘₯ − 25 = 𝐴(π‘₯ − 4) + 𝐡(π‘₯ − 3)
At x = 3 βž” 21 − 25 = A(3 − 4) + 0 , −4 = −A , then: 𝐀 = πŸ’
At x = 4 βž” 28 − 25 = 0 + B(4 − 3) , 3 = B , then: 𝐁 = πŸ‘
Then:
7π‘₯−25
π‘₯ 2 −7π‘₯+12
=
4
π‘₯−3
+
3
π‘₯−4
17] The partial Fraction decomposition of
𝟐
𝟏
𝟏
𝟐
𝟏
𝟏
A- 𝒙−𝟏 − (𝒙−𝟏)𝟐 − 𝒙−𝟐
π’™πŸ −πŸ‘π’™+𝟏
is
(𝒙−𝟏)𝟐 (𝒙−𝟐)
𝟐
𝟏
πŸ‘
𝟐
𝟏
𝟏
C- 𝒙−𝟏 + (𝒙−𝟏)𝟐 − 𝒙−𝟐
B- 𝒙−𝟏 − (𝒙−𝟏)𝟐 + 𝒙−𝟐
D- 𝒙−𝟏 + (𝒙−𝟏)𝟐 − 𝒙−𝟐
Solution:
π‘₯ 2 −3π‘₯+1
(π‘₯−1)2 (π‘₯−2)
=
A
π‘₯−1
B
+ (π‘₯−1)2 +
C
π‘₯−2
(Proper Fraction)
By multiplying in two sides by : (π‘₯ − 1)2 (π‘₯ − 2)
βž” π‘₯ 2 − 3π‘₯ + 1 = A(π‘₯ − 1)(π‘₯ − 2) + B(π‘₯ − 2) + C(π‘₯ − 1)2
At x = 1 βž” 1 − 3 + 1 = 0 + B(1 − 2) + 0 , −1 = −B , then: 𝐁 = 𝟏
Page | 10
At x = 2 βž” 4 − 6 + 1 = 0 + 0 + C(2 − 1)2 , −1 = C , then: 𝐂 = −𝟏
At x = 0 βž” 1 = A(0 − 1)(0 − 2) + B(0 − 2) + C(0 − 1)2 ,
1 = A(−1)(−2) + 1(−2) + (−1)(−1)2 = 2A − 3 = 1 , then: 𝐀 = 𝟐
π‘₯ 2 −3π‘₯+1
2
Then: (π‘₯−1)2 (π‘₯−2) =
π‘₯−1
1
+ (π‘₯−1)2 −
1
π‘₯−2
Choice D
𝟏
18] The partial Fraction decomposition of π’™πŸ’ (𝒙+𝟐)is
𝟏
𝟏
𝟏
𝟏
𝟏
C- πŸπŸ”π’™ + πŸ–π’™πŸ − πŸ’π’™πŸ‘ + πŸπ’™πŸ’ + πŸπŸ”(𝒙+𝟐)
𝟏
𝟏
𝟏
𝟏
𝟏
𝟏
D- − πŸπŸ”π’™ + πŸπŸ”π’™πŸ + πŸ’π’™πŸ‘ + πŸπ’™πŸ’ + πŸ–(𝒙+𝟐)
A- − πŸπŸ”π’™ − πŸ–π’™πŸ − πŸ’π’™πŸ‘ + πŸπ’™πŸ’ − πŸπŸ”(𝒙+𝟐)
𝟏
𝟏
𝟏
B- − πŸπŸ”π’™ + πŸ–π’™πŸ − πŸ’π’™πŸ‘ + πŸπ’™πŸ’ + πŸπŸ”(𝒙+𝟐)
𝟏
𝟏
𝟏
𝟏
𝟏
Solution:
1
π‘₯ 4 (π‘₯+2)
=
A
π‘₯
+
B
C
D
E
π‘₯
π‘₯
π‘₯
π‘₯+2
2 +
3 +
4 +
(Proper Fraction)
By multiplying in two sides by : π‘₯ 4 (π‘₯ + 2)
βž” 1 = Aπ‘₯ 3 (π‘₯ + 2) + Bπ‘₯ 2 (π‘₯ + 2) + Cπ‘₯ (π‘₯ + 2) + D(π‘₯ + 2) + Eπ‘₯ 4
1 = Aπ‘₯ 4 + 2Aπ‘₯ 3 + Bπ‘₯ 3 + 2Bπ‘₯ 2 + Cπ‘₯ 2 + 2Cπ‘₯ + Dπ‘₯ + 2D + Eπ‘₯ 4
At x = 0 βž” 1 = 2D , then: 𝐃 =
𝟏
𝟐
At x = −𝟐 βž” 1 = E(−2)4 , then: 𝐄 =
𝟏
πŸπŸ”
Equating Coefficient (π’™πŸ’ ) βž” 0 = A + E ; A = −E , then: 𝐀 =
Equating Coefficient (π’™πŸ‘ ) βž” 0 = 2A + B ; then: 𝐁 =
𝟏
Equating Coefficient (π’™πŸ ) βž” 0 = 2B + C ; then: 𝐂 =
−𝟏
Page | 11
πŸ–
πŸ’
−𝟏
πŸπŸ”
𝟏
Then:
1
π‘₯ 4 (π‘₯+2)
=−
1
16π‘₯
1
+
8π‘₯ 2
−
1
4π‘₯ 3
+
1
2π‘₯ 4
+
1
16(π‘₯+2)
Choice B
πŸ—π’™−πŸ•
19] The partial Fraction decomposition of (𝒙+πŸ‘)(π’™πŸ +𝟏) is
πŸπŸ•
πŸπŸ•π’™−πŸ”
A- − πŸ“(𝒙+πŸ‘) + πŸ“(π’™πŸ +𝟏)
πŸπŸ•
C-
πŸπŸ•π’™−πŸ”
B- (𝒙+πŸ‘) + πŸ“(π’™πŸ −𝟏)
D-
πŸπŸ•
πŸπŸ•π’™−πŸ”
πŸπŸ•
πŸπŸ•π’™−πŸ”
− πŸ“(π’™πŸ +𝟏)
πŸ“(𝒙+πŸ‘)
+ (π’™πŸ +𝟏)
πŸ“(𝒙+πŸ‘)
Solution:
9π‘₯−7
(π‘₯+3)(π‘₯ 2 +1)
=
A
π‘₯+3
+
Bπ‘₯+C
(Proper Fraction)
π‘₯ 2 +1
By multiplying in two sides by : (π‘₯ + 3)(π‘₯ 2 + 1)
βž” 9π‘₯ − 7 = A(π‘₯ 2 + 1) + (Bπ‘₯ + C)(π‘₯ + 3)
9π‘₯ − 7 = Aπ‘₯ 2 + A + Bπ‘₯ 2 + 3Bπ‘₯ + Cπ‘₯ + 3C
At 𝒙 = −πŸ‘ βž” −27 − 7 = A((−3)2 + 1) , then: 𝐀 = −
Equating Coefficient (π’™πŸ ) βž” 0 = A + B , then: 𝐁 =
πŸπŸ•
πŸπŸ•
πŸ“
Equating Coefficient (π’™πŸ ) βž” 9 = 3B + C , then: 𝐂 = −
Then:
9π‘₯−7
(π‘₯+3)(π‘₯ 2 +1)
=−
9π‘₯−7
(π‘₯+3)(π‘₯ 2 +1)
Choice A
Page | 12
17
5(π‘₯+3)
=−
+
17
5(π‘₯+3)
17
6
π‘₯−5
5
π‘₯ 2 +1
+
πŸ“
πŸ”
πŸ“
multiply by πŸ“ in numerator & denominator
17π‘₯−6
5(π‘₯ 2 +1)
20] The partial Fraction decomposition of
𝟏
𝒙+𝟏
𝒙+𝟏
𝟏
𝒙+𝟏
𝒙+𝟏
A- πŸ’(𝟏−𝒙) + 𝟐(𝟏+π’™πŸ ) − πŸ’(𝟏+π’™πŸ )𝟐
C-
B- πŸ’(𝟏−𝒙) − 𝟐(𝟏+π’™πŸ ) − πŸ’(𝟏+π’™πŸ)𝟐
D-
π’™πŸ
is
(𝟏−𝒙)(𝟏+π’™πŸ )𝟐
𝟏
𝒙+𝟏
𝒙+𝟏
𝟏
𝒙+𝟏
𝒙+𝟏
+ πŸ’(𝟏+π’™πŸ ) − 𝟐(𝟏+π’™πŸ )𝟐
πŸ’(𝟏−𝒙)
+ 𝟐(𝟏+π’™πŸ ) − πŸ’(𝟏+π’™πŸ )𝟐
𝟐(𝟏−𝒙)
Solution:
π‘₯2
(1−π‘₯)(1+π‘₯ 2 )2
A
Bπ‘₯+C
Dπ‘₯+E
= (1−π‘₯) + (1+π‘₯ 2 ) + (1+π‘₯ 2 )2
(Proper Fraction)
By multiplying in two sides by : (1 − π‘₯ )(1 + π‘₯ 2 )2
π‘₯ 2 = A(1 + π‘₯ 2 )2 + (Bπ‘₯ + C)(1 − π‘₯ )(1 + π‘₯ 2 ) + (Dπ‘₯ + E)(1 − π‘₯ )
π‘₯ 2 = A + Aπ‘₯ 4 + 2Aπ‘₯ 2 + Bπ‘₯ − Bπ‘₯ 2 + C − Cπ‘₯ + Bπ‘₯ 3 − Bπ‘₯ 4 + Cπ‘₯ 2
−Cπ‘₯ 3 + Dπ‘₯ + E − Dπ‘₯ 2 − Eπ‘₯
At 𝒙 = 1 βž” 1 = A(1 + 12 )2 , then: 𝐀 =
𝟏
πŸ’
Equating Coefficient (π’™πŸ’ ) βž” 0 = A − B , then: 𝐁 =
𝟏
Equating Coefficient (π’™πŸ‘ ) βž” 0 = B − C , then: 𝐂 =
𝟏
πŸ’
πŸ’
Equating Coefficient (π’™πŸ ) βž” 1 = 2A − B + C − D , then: 𝐃 = −
Equating Coefficient (π’™πŸ ) βž” 0 = B − C + D − E , then: 𝐄 = −
Then:
π‘₯2
(1−π‘₯)(1+π‘₯ 2 )2
=
Choice C
Page | 13
1
4(1−π‘₯)
+
=
1
4(1−π‘₯)
π‘₯+1
4(1+π‘₯ 2 )
−
+
1
1
π‘₯+4
4
(1+π‘₯ 2 )
π‘₯+1
2(1+π‘₯ 2 )2
1
1
−2π‘₯−2
+ (1+π‘₯ 2 )2
𝟏
𝟐
𝟏
𝟐
πŸπ’™−𝟏
21] The partial Fraction decomposition of (𝒙+𝟐)(𝒙−πŸ‘)is
𝟏
𝟏
𝟏
𝟏
A- 𝒙+𝟐 + 𝒙+πŸ‘
C-
B- 𝒙−𝟐 − 𝒙−πŸ‘
D-
𝟏
𝟏
𝟏
𝟏
− 𝒙−πŸ‘
𝒙+𝟐
+ 𝒙−πŸ‘
𝒙+𝟐
Solution:
2π‘₯−1
(π‘₯+2)(π‘₯−3)
=
A
π‘₯+2
+
B
π‘₯−3
(Proper Fraction)
By multiplying in two sides by : (π‘₯ + 2)(π‘₯ − 3)
βž” 2π‘₯ − 1 = A(π‘₯ − 3) + B(π‘₯ + 2)
At 𝒙 = πŸ‘ , 2 ∗ 3 − 1 = 0 + B(5) , 5 = 5B , then: 𝐁 = 𝟏
At 𝒙 = −𝟐 , 2 ∗ −2 − 1 = A(−2 − 3) + 0 , −5 = A(−5) , then: 𝐀 = 𝟏
2π‘₯−1
Then: (π‘₯+2)(π‘₯−3) =
1
π‘₯+2
+
1
π‘₯−3
Choice D
πŸπ’™+πŸ“
22] The partial Fraction decomposition of (𝒙−𝟐)(𝒙+𝟏) is
πŸ‘
𝟏
πŸ‘
𝟏
A- 𝒙−𝟐 − 𝒙+𝟏
C-
B- 𝒙+πŸ‘ − 𝒙+𝟏
D-
πŸ‘
𝟏
πŸ‘
𝟐
− 𝒙+𝟏
𝒙+𝟐
− 𝒙+𝟏
𝒙−𝟐
Solution:
2π‘₯+5
(π‘₯−2)(π‘₯+1)
=
A
π‘₯−2
+
B
π‘₯+1
(Proper Fraction)
By multiplying in two sides by : (π‘₯ − 2)(π‘₯ + 1)
βž” 2π‘₯ + 5 = A(π‘₯ + 1) + B(π‘₯ − 2)
At 𝒙 = −𝟏 , 2 ∗ −1 + 5 = 0 + B(−1 − 2) , 3 = −3B , then: 𝐁 = −𝟏
Page | 14
At 𝒙 = 𝟐 , 2 ∗ 2 + 5 = A(2 + 1) + 0 , 9 = 3A , then: 𝐀 = πŸ‘
2π‘₯+5
Then: (π‘₯−2)(π‘₯+1) =
3
π‘₯−2
−
1
π‘₯+1
Choice A
πŸ‘
23] The partial Fraction decomposition of (𝒙−𝟏)(πŸπ’™−𝟏) is
πŸ‘
πŸ”
πŸ‘
πŸ”
A- 𝒙−𝟏 + πŸπ’™−𝟏
C-
B- 𝒙−𝟏 − πŸπ’™−𝟏
D-
πŸ‘
πŸ”
πŸ–
πŸ”
− πŸπ’™+𝟏
𝒙−𝟏
− πŸπ’™−𝟏
𝒙−𝟏
Solution:
3
(π‘₯−1)(2π‘₯−1)
=
A
π‘₯−1
+
B
2π‘₯−1
(Proper Fraction)
By multiplying in two sides by : (π‘₯ − 1)(2π‘₯ − 1)
βž” 3 = A(2π‘₯ − 1) + B(π‘₯ − 1)
At 𝒙 = 𝟏 , 3 = A(2 ∗ 1 − 1) + 0 , 3 = A , then: 𝐀 = πŸ‘
𝟏
1
1
𝟐
2
2
At 𝒙 = , 3 = B ( − 1) , 3 = − B , then: 𝐁 = −πŸ”
3
Then: (π‘₯−1)(2π‘₯−1) =
3
π‘₯−1
−
6
2π‘₯−1
Choice B
𝟏
24] The partial Fraction decomposition of (𝒙+πŸ’)(𝒙−𝟐) is
𝟏
𝟏
𝟏
𝟏
A- − πŸ”(𝒙+πŸ’) + πŸ”(𝒙+𝟐)
B- − πŸ”(𝒙+πŸ’) + πŸ•(𝒙−𝟐)
Page | 15
𝟏
𝟏
C- − πŸ”(𝒙+πŸ’) + πŸ”(𝒙−𝟐)
D-
𝟏
𝟏
+ πŸ”(𝒙−𝟐)
πŸ”(𝒙+πŸ’)
Solution:
1
(π‘₯+4)(π‘₯−2)
=
A
π‘₯+4
+
B
(Proper Fraction)
π‘₯−2
By multiplying in two sides by : (π‘₯ + 4)(π‘₯ − 2)
βž” 1 = A(π‘₯ − 2) + B(π‘₯ + 4)
At 𝒙 = 𝟐 , 1 = 0 + B ∗ 6 , then: 𝐁 =
𝟏
πŸ”
At 𝒙 = −πŸ’ , 1 = A ∗ −6 + 0 , then: 𝐀 = −
1
Then: (π‘₯+4)(π‘₯−2) = −
1
6(π‘₯+4)
+
𝟏
πŸ”
1
6(π‘₯−2)
Choice C
25] To resolve a combined fraction into its parts is called
A- rational fraction
C- partial fraction
B- combined fraction
D- None of them
Solution:
Choice C
26] The partial Fraction decomposition of
𝟐
𝟏
πŸ‘
𝟐
𝟏
πŸ‘
A- (𝒙+𝟐) − (𝒙+𝟐)𝟐 + (𝒙+𝟏)
C-
B- (𝒙+𝟐) + (𝒙+𝟐)𝟐 + (𝒙+𝟏)
D-
πŸ“π’™πŸ +πŸπŸ•π’™+πŸπŸ“
(𝒙+𝟐)𝟐 (𝒙+𝟏)
𝟐
𝟏
πŸ‘
πŸ’
𝟏
πŸ‘
− (𝒙+𝟐)𝟐 − (𝒙+𝟏)
(𝒙+𝟐)
− (𝒙+𝟐)𝟐 + (𝒙+𝟏)
(𝒙+𝟐)
Solution:
5π‘₯ 2 +17π‘₯+15
(π‘₯+2)2 (π‘₯+1)
Page | 16
A
B
C
= (π‘₯+2) + (π‘₯+2)2 + (π‘₯+1)
is
(Proper Fraction)
By multiplying in two sides by : (π‘₯ + 2)2 (π‘₯ + 1)
βž” 5π‘₯ 2 + 17π‘₯ + 15 = A(π‘₯ + 2)(π‘₯ + 1) + B(π‘₯ + 1) + C(π‘₯ + 2)2
= A(π‘₯ 2 + 3π‘₯ + 2) + Bπ‘₯ + B + C(π‘₯ 2 + 4π‘₯ + 4)
At 𝒙 = −𝟐 , 5 ∗ (−2)2 + 17 ∗ −2 + 15 = B(−2 + 1) βž” 1 = B(−1) , then: 𝐁 = −𝟏
At 𝒙 = −𝟏 , 5 ∗ (−1)2 + 17 ∗ −1 + 15 = C(−1 + 2)2 βž” 3 = C , then: 𝐂 = πŸ‘
Equating Coefficient (π’™πŸ )
βž” 5 = A + C , 5 = A + 3 , then: 𝐀 = 𝟐
5π‘₯ 2 +17π‘₯+15
(π‘₯+2)2 (π‘₯+1)
Then:
2
1
3
= (π‘₯+2) − (π‘₯+2)2 + (π‘₯+1)
Choice A
27] The partial Fraction decomposition of
𝒙
(𝒙−πŸ‘)πŸ‘ (πŸπ’™+𝟏)
is
𝟐
𝟏
πŸ‘
πŸ’
A- − πŸ‘πŸ’πŸ‘(𝒙−πŸ‘)
+
+
+
πŸ’πŸ—(𝒙−πŸ‘)𝟐
πŸ•(𝒙−πŸ‘)πŸ‘
πŸ‘πŸ’πŸ‘(πŸπ’™+𝟏)
𝟐
𝟏
πŸ‘
πŸ’
B- − πŸ‘πŸ’πŸ‘(𝒙−πŸ‘)
−
+
+
πŸ’πŸ—(𝒙−πŸ‘)𝟐
πŸ•(𝒙−πŸ‘)πŸ‘
πŸ‘πŸ’πŸ‘(πŸπ’™+𝟏)
C-
𝟐
πŸ‘πŸ’πŸ‘(𝒙−πŸ‘)
+
𝟏
πŸ’πŸ—(𝒙−πŸ‘)𝟐
+
πŸ‘
πŸ•(𝒙−πŸ‘)πŸ‘
+
πŸ’
πŸ‘πŸ’πŸ‘(πŸπ’™+𝟏)
𝟐
𝟏
πŸ‘
πŸ’
D- − πŸ‘πŸ’πŸ‘(𝒙−πŸ‘)
+
+
+
𝟐
πŸ‘
πŸ’πŸ—(𝒙−πŸ‘)
πŸ•(𝒙+πŸ‘)
πŸ‘πŸ’πŸ‘(πŸπ’™+𝟏)
Solution:
π‘₯
(π‘₯−3)3 (2π‘₯+1)
A
B
C
D
= (π‘₯−3) + (π‘₯−3)2 + (π‘₯−3)3 + (2π‘₯+1)
(Proper Fraction)
By multiplying in two sides by : (x − 3)3 (2x + 1)
βž” π‘₯ = A(π‘₯ − 3)2 (2π‘₯ + 1) + B(π‘₯ − 3)(2π‘₯ + 1) + C(2π‘₯ + 1) + D(π‘₯ − 3)3
= A(2π‘₯ 3 − 11π‘₯ 2 + 12π‘₯ + 9) + B(2π‘₯ 2 − 5π‘₯ − 3) + C(2π‘₯ + 1)
+D(π‘₯ 3 − 9π‘₯ 2 + 27π‘₯ − 27)
Page | 17
At 𝒙 = πŸ‘ , 3 = C(2 ∗ 3 + 1) , 3 = C ∗ 7 , then: 𝐂 =
𝟏
1
1
𝟐
2
2
3
1
343
2
8
At 𝒙 = − , − = D (− − 3) , − = D (−
πŸ‘
πŸ•
πŸ’
) , then: 𝐃 = πŸ‘πŸ’πŸ‘
Equating Coefficient (π’™πŸ‘ )
βž” 0 = 2A + D , 0 = 2A +
4
343
, then: 𝐀 = −
𝟐
πŸ‘πŸ’πŸ‘
Equating Coefficient (π’™πŸ )
βž” 0 = −11A + 2B − 9D , 0 = −11 ∗ −
π‘₯
Then: (π‘₯−3)3 (2π‘₯+1) = −
2
343(π‘₯−3)
+
2
343
1
49(π‘₯−3)2
+ 2B − 9 ∗
+
3
7(π‘₯−3)3
+
4
343
, then: 𝐁 =
𝟏
πŸ’πŸ—
4
343(2π‘₯+1)
Choice A
28] The partial Fraction decomposition of
𝟏
𝟏
𝟏
𝟏
A- 𝟐(𝒙−𝟏) + (𝒙−𝟏)𝟐
C𝟏
B- 𝟐(𝒙−𝟏) + (𝒙+𝟏)𝟐 + 𝟐(𝒙+𝟏)
π’™πŸ +𝟏
(𝒙−𝟏)𝟐 (𝒙+𝟏)
𝟏
𝟏
𝟏
𝟏
𝟏
𝟏
− (𝒙−𝟏)𝟐 + 𝟐(𝒙+𝟏)
𝟐(𝒙−𝟏)
D- 𝟐(𝒙−𝟏) + (𝒙−𝟏)𝟐 + 𝟐(𝒙+𝟏)
Solution:
π‘₯ 2 +1
(π‘₯−1)2 (π‘₯+1)
A
B
C
= (π‘₯−1) + (π‘₯−1)2 + (π‘₯+1)
(Proper Fraction)
By multiplying in two sides by : (π‘₯ − 1)2 (π‘₯ + 1)
βž” π‘₯ 2 + 1 = A(π‘₯ − 1)(π‘₯ + 1) + B(π‘₯ + 1) + C(π‘₯ − 1)2
= A(π‘₯ 2 − 1) + B(π‘₯ + 1) + C(π‘₯ 2 − 2π‘₯ + 1)
At 𝒙 = 𝟏 , 2 = B(π‘₯ + 1) , then: 𝐁 = 𝟏
At 𝒙 = −𝟏 , 2 = C(π‘₯ − 1)2 , 2 = 4C , then: 𝐂 =
Page | 18
is
𝟏
𝟐
Equating Coefficient (π’™πŸ )
1
𝟏
2
𝟐
βž” 1 = A + C , 1 = A + , then: 𝐀 =
π‘₯ 2 +1
Then: (π‘₯−1)2 (π‘₯+1) =
1
1
2(π‘₯−1)
+ (π‘₯−1)2 +
1
2(π‘₯+1)
Choice D
29] The partial Fraction decomposition of
πŸπ’™+𝟏
πŸ‘
πŸπ’™+𝟏
πŸ‘
A- (π’™πŸ +𝒙+𝟐) + (πŸπ’™−𝟏)
C-
B- (π’™πŸ +𝒙+𝟐) − (πŸπ’™−𝟏)
π’™πŸ −πŸ‘π’™−πŸ•
(π’™πŸ +𝒙+𝟐)(πŸπ’™−𝟏)
πŸπ’™−𝟏
πŸ‘
πŸπ’™+𝟏
πŸ‘
− (πŸπ’™−𝟏)
(π’™πŸ +𝒙+𝟐)
D- (π’™πŸ +𝒙+𝟐) − (πŸπ’™+𝟏)
Solution:
π‘₯ 2 −3π‘₯−7
Aπ‘₯+B
(π‘₯ 2 +π‘₯+2)(2π‘₯−1)
= (π‘₯ 2
C
+π‘₯+2)
+ (2π‘₯−1)
(Proper Fraction)
By multiplying in two sides by : (π‘₯ 2 + π‘₯ + 2)(2π‘₯ − 1)
π‘₯ 2 − 3π‘₯ − 7 = (Aπ‘₯ + B)(2π‘₯ − 1) + C(π‘₯ 2 + π‘₯ + 2)
= 2Aπ‘₯ 2 − Aπ‘₯ + 2Bπ‘₯ − B + C(π‘₯ 2 + π‘₯ + 2)
𝟏
33
𝟐
4
At 𝒙 = , −
=C∗
11
4
, then: 𝐂 = −πŸ‘
Equating Coefficient (π’™πŸ )
1 = 2A + C , 1 = 2A − 3 , then: 𝐀 = 𝟐
Equating Coefficient (π’™πŸ )
−3 = −A + 2B + C , −3 = −2 + 2B − 3 , then: 𝐁 = 𝟏
Then: (π‘₯ 2
Choice B
Page | 19
π‘₯ 2 −3π‘₯−7
+π‘₯+2)(2π‘₯−1)
2π‘₯+1
= (π‘₯ 2
+π‘₯+2)
3
− (2π‘₯−1)
is
30] The partial Fraction decomposition of
πŸπŸ”
πŸ–π’™−𝟏𝟐
πŸπ’™−πŸ‘
πŸπŸ”
−πŸ–π’™+𝟏𝟐
πŸπ’™+πŸ‘
πŸπŸ”
−πŸ–π’™+𝟏𝟐
πŸπ’™+πŸ‘
πŸπŸ‘
(πŸπ’™+πŸ‘)(π’™πŸ +𝟏)𝟐
is
A- πŸπŸ‘(πŸπ’™+πŸ‘) − πŸπŸ‘(π’™πŸ +𝟏) − (π’™πŸ +𝟏)𝟐
C-
+ πŸπŸ‘(π’™πŸ +𝟏) + (π’™πŸ +𝟏)𝟐
πŸπŸ‘(πŸπ’™+πŸ‘)
B- πŸπŸ‘(πŸπ’™+πŸ‘) − πŸπŸ‘(π’™πŸ +𝟏) − (π’™πŸ +𝟏)𝟐
πŸπŸ”
−πŸ–π’™+𝟏𝟐
πŸπ’™+πŸ‘
D- − πŸπŸ‘(πŸπ’™+πŸ‘) + πŸπŸ‘(π’™πŸ +𝟏) − (π’™πŸ +𝟏)𝟐
Solution:
13
(2π‘₯+3)(π‘₯ 2 +1)2
A
Bπ‘₯+C
= (2π‘₯+3) + (π‘₯ 2
+1)
Dπ‘₯+E
+ (π‘₯ 2
(Proper Fraction)
+1)2
By multiplying in two sides by : (2π‘₯ + 3)(π‘₯ 2 + 1)2
13 = A(π‘₯ 2 + 1)2 + (Bπ‘₯ + C)(2π‘₯ + 3)(π‘₯ 2 + 1) + (Dπ‘₯ + E)(2π‘₯ + 3)
= A(π‘₯ 4 + 2π‘₯ 2 + 1) + 2Bπ‘₯ 4 + 3Bπ‘₯ 3 + 2Bπ‘₯ 2 + 3Bπ‘₯ + 2Cπ‘₯ 3
+3Cπ‘₯ 2 + 2Cπ‘₯ + 3C + 2Dπ‘₯ 2 + 3Dπ‘₯ + 2Eπ‘₯ + 3E
3 2
πŸ‘
2
At 𝒙 = − , 13 = A ((− ) + 1) , 13 = A ∗
𝟐
2
169
16
, then: 𝐀 =
πŸπŸ”
πŸπŸ‘
Equating Coefficient (π’™πŸ’ )
0 = A + 2B , 0 =
16
13
+ 2B , then: 𝐁 = −
πŸ–
πŸπŸ‘
Equating Coefficient (π’™πŸ‘ )
0 = 3B + 2C , 0 = 3 ∗ −
8
13
+ 2C , then: 𝐂 =
𝟏𝟐
πŸπŸ‘
Equating Coefficient (π’™πŸ )
0 = 2A + 2B + 3C + 2D , 0 = 2 ∗
βž” 0 = 4 + 2D , then: 𝐃 = −𝟐
Page | 20
16
13
+2∗−
8
13
+3∗
12
13
+ 2D
Equating Coefficient (π’™πŸ )
0 = 3B + 2C + 3D + 2E , 0 = 3 ∗ −
8
13
+2∗
12
13
+ 3 ∗ −2 + 2E
βž” 0 = 6 + 2E , then: 𝐄 = πŸ‘
Then:
13
(2π‘₯+3)(π‘₯ 2 +1)2
=
16
13(2π‘₯+3)
=
8
12
13
13
2
(π‘₯ +1)
− π‘₯+
+
16
13(2π‘₯+3)
+
−2π‘₯+3
+ (π‘₯ 2
−8π‘₯+12
13(π‘₯ 2 +1)
+1)2
2π‘₯−3
− (π‘₯ 2
=
+1)2
16
13(2π‘₯+3)
−
8π‘₯−12
13(π‘₯ 2 +1)
Choice A
31] The partial Fraction decomposition of
−πŸπ’™+πŸ‘
πŸ”
−πŸπ’™+πŸ‘
πŸ”
A- πŸ•(π’™πŸ −𝒙+𝟏) − πŸ•(πŸ‘π’™−𝟐)
C-
B- πŸ•(π’™πŸ −𝒙+𝟏) + πŸ•(πŸ‘π’™−𝟐)
𝒙
(π’™πŸ −𝒙+𝟏)(πŸ‘π’™−𝟐)
πŸπ’™+πŸ‘
πŸ”
−πŸπ’™−πŸ‘
πŸ”
+ πŸ•(πŸ‘π’™−𝟐)
πŸ•(π’™πŸ −𝒙+𝟏)
D- πŸ•(π’™πŸ −𝒙+𝟏) + πŸ•(πŸ‘π’™−𝟐)
Solution:
π‘₯
Aπ‘₯+B
(π‘₯ 2 −π‘₯+1)(3π‘₯−2)
= (π‘₯ 2
−π‘₯+1)
C
+ (3π‘₯−2)
(Proper Fraction)
By multiplying in two sides by : (π‘₯ 2 − π‘₯ + 1)(3π‘₯ − 2)
βž” π‘₯ = (Aπ‘₯ + B)(3π‘₯ − 2) + C(π‘₯ 2 − π‘₯ + 1)
= 3Aπ‘₯ 2 − 2Aπ‘₯ + 3Bπ‘₯ − 2B + C(π‘₯ 2 − π‘₯ + 1)
At 𝒙 =
𝟐
πŸ‘
,
2
3
=C∗
7
9
, then: 𝐂 =
πŸ”
πŸ•
Equating Coefficient (π’™πŸ )
6
𝟐
7
πŸ•
0 = 3A + C , 0 = 3A + , then: 𝐀 = −
Equating Coefficient (π’™πŸ )
2
6
πŸ‘
7
7
πŸ•
1 = −2A + 3B − C , 1 = −2 ∗ − + 3B − , then: 𝐁 =
Page | 21
is
2π‘₯−3
− (π‘₯ 2
+1)2
Then: (π‘₯ 2
2
3
−7 π‘₯+7
π‘₯
= (π‘₯ 2
−π‘₯+1)(3π‘₯−2)
=
−π‘₯+1)
+
−2π‘₯+3
7(π‘₯ 2 −π‘₯+1)
6
7(3π‘₯−2)
+
6
7(3π‘₯−2)
Choice B
32] The partial Fraction decomposition of
𝟏
𝟏
A- − π’™πŸ − (𝟏+π’™πŸ )
𝟏
C-
𝟏
𝟏
π’™πŸ +π’™πŸ’
is
𝟏
+ (𝟏+π’™πŸ)
π’™πŸ
𝟏
B- π’™πŸ − (𝟏−π’™πŸ )
𝟏
𝟏
D- π’™πŸ − (𝟏+π’™πŸ )
Solution:
1
π‘₯ 2 +π‘₯ 4
=
1
π‘₯ 2 (1+π‘₯ 2 )
=
A
π‘₯
+
B
π‘₯2
Cπ‘₯+D
+ (1+π‘₯ 2 )
(Proper Fraction)
By multiplying in two sides by : π‘₯ 2 (1 + π‘₯ 2 )
βž” 1 = A(π‘₯ )(1 + π‘₯ 2 ) + B(1 + π‘₯ 2 ) + (Cπ‘₯ + D)(π‘₯ 2 )
= A(π‘₯ + π‘₯ 3 ) + B(1 + π‘₯ 2 ) + Cπ‘₯ 3 + Dπ‘₯ 2
At 𝒙 = 𝟎 βž” 1 = B(1) βž” then: 𝐁 = 𝟏
Equating Coefficient (π’™πŸ‘ )
0 = A + C βž” A = −C
Equating Coefficient (π’™πŸ )
0 = B + D βž” D = −B βž” then: 𝐃 = −𝟏
Equating Coefficient (π’™πŸ )
0 = A βž” then: 𝐀 = 𝟎
then: 𝐂 = 𝟎
Then:
1
π‘₯ 2 (1+π‘₯ 2 )
Choice D
Page | 22
0
1
π‘₯
π‘₯
= +
0∗π‘₯−1
2 + (1+π‘₯ 2 ) =
1
π‘₯
1
2 − (1+π‘₯ 2 )
33] The partial Fraction decomposition of
𝟐
𝒙+𝟏
𝟐
𝒙+𝟏
A- πŸ‘(𝒙+𝟏) + πŸ‘(π’™πŸ +𝒙+𝟏)
C-
B- πŸ‘(𝒙+𝟏) + πŸ‘(π’™πŸ −𝒙−𝟏)
π’™πŸ +𝟏
π’™πŸ‘ +𝟏
is
𝟐
𝒙+𝟏
𝟐
𝒙+𝟏
+ πŸ‘(π’™πŸ −𝒙+𝟏)
πŸ‘(𝒙+𝟏)
D- πŸ‘(𝒙+𝟏) − πŸ‘(π’™πŸ −𝒙+𝟏)
Solution:
π‘₯ 2 +1
π‘₯ 3 +1
A
Bπ‘₯+C
= (π‘₯+1) + (π‘₯ 2
−π‘₯+1)
(Proper Fraction)
By multiplying in two sides by : π‘₯ 3 + 1
βž” π‘₯ 2 + 1 = A(π‘₯ 2 − π‘₯ + 1) + (Bπ‘₯ + C)(π‘₯ + 1)
= Aπ‘₯ 2 − Ax + A + Bπ‘₯ 2 + Bπ‘₯ + Cπ‘₯ + C
At 𝒙 = −𝟏 βž” 𝟐 = A((−1)2 − (−1) + 1) βž” 2 = 3A , then: 𝐀 =
𝟐
πŸ‘
Equating Coefficient (π’™πŸ )
2
𝟏
3
πŸ‘
1 = A + B βž” 1 = + B , then: 𝐁 =
Equating Coefficient (π’™πŸ )
2
1
𝟏
3
3
πŸ‘
0 = −A + B + C βž” 0 = − + + C , then: 𝐂 =
Then:
π‘₯ 2 +1
π‘₯ 3 +1
=
2
3(π‘₯+1)
+
1
1
π‘₯+3
3
(π‘₯ 2 −π‘₯+1)
=
2
3(π‘₯+1)
+
x+1
3(π‘₯ 2 −π‘₯+1)
Choice C
34] The partial Fraction decomposition of
𝟏
(𝒙+𝟏)(π’™πŸ −𝟏)(π’™πŸ +πŸ“)
is
πŸ“
𝟏
𝟏
𝒙−𝟏
πŸ“
𝟏
𝟏
𝒙−𝟏
A- − πŸ•πŸ(𝒙+𝟏)
−
−
−
C- − πŸ•πŸ(𝒙+𝟏)
−
+
+
𝟏𝟐(𝒙+𝟏)𝟐
πŸπŸ’(𝒙−𝟏)
πŸ‘πŸ”(π’™πŸ +πŸ“)
𝟏𝟐(𝒙+𝟏)𝟐
πŸπŸ’(𝒙−𝟏)
πŸ‘πŸ”(π’™πŸ +πŸ“)
πŸ“
𝟏
𝟏
𝒙−𝟏
πŸ“
𝟏
𝟏
𝒙−𝟏
B- − πŸ•πŸ(𝒙+𝟏)
+
+
+
D- πŸ•πŸ(𝒙+𝟏)
−
+
+
𝟏𝟐(𝒙+𝟏)𝟐
πŸπŸ’(𝒙−𝟏)
πŸ‘πŸ”(π’™πŸ +πŸ“)
𝟏𝟐(𝒙+𝟏)𝟐
πŸπŸ’(𝒙−𝟏)
πŸ‘πŸ”(π’™πŸ +πŸ“)
Page | 23
Solution:
1
1
(π‘₯+1)(π‘₯ 2 −1)(π‘₯ 2 +5)
= (π‘₯+1)(π‘₯−1)(π‘₯+1)(π‘₯ 2
A
1
+5)
B
= (π‘₯+1)2 (π‘₯−1)(π‘₯ 2
C
+5)
(Proper Fraction)
Dπ‘₯+E
= (π‘₯+1) + (π‘₯+1)2 + (π‘₯−1) + (π‘₯ 2
+5)
By multiplying in two sides by : (π‘₯ + 1)2 (π‘₯ − 1)(π‘₯ 2 + 5)
βž” 1 = A(π‘₯ + 1)(π‘₯ − 1)(π‘₯ 2 + 5) + B(π‘₯ − 1)(π‘₯ 2 + 5) + C(π‘₯ + 1)2 (π‘₯ 2 + 5)
+(Dπ‘₯ + E)(π‘₯ + 1)2 (π‘₯ − 1)
βž” 1 = A(π‘₯ 4 + 4π‘₯ 2 − 5) + B(π‘₯ 3 − π‘₯ 2 + 5π‘₯ − 5) + C(π‘₯ 4 + 2π‘₯ 3 + 6π‘₯ 2 + 10π‘₯ + 5)
+Dπ‘₯ 4 + Dπ‘₯ 3 − Dπ‘₯ 2 − Dπ‘₯ + Eπ‘₯ 3 + Eπ‘₯ 2 − Eπ‘₯ − E
At 𝒙 = −𝟏 βž” 1 = B((−1) − 1)((−1)2 + 5) βž” 1 = B(−12) , then: 𝐁 = −
𝟏
𝟏𝟐
𝟏
At 𝒙 = 𝟏 βž” 1 = C(π‘₯ + 1)2 (π‘₯ 2 + 5) βž” 1 = C(2)2 (12 + 5) = C(24) , then: 𝐂 = πŸπŸ’
Equating Coefficient (π’™πŸ’ )
0=A+C+Dβž”0= A+
1
24
+D
1
Equating Coefficient (π’™πŸ‘ )
0 = B + 2C + D + E βž” 0 = −
1
12
+2∗
1
24
+ D + E βž” D + E = 0 βž” D = −E
Equating Coefficient (π’™πŸ )
0 = 4A − B + 6C − D + E βž” 0 = 4A − (−
= 4A +
1
12
1
1
4
3
+ + 2E = 4A + + 2E = 0
From equations 1 & 2
0=A+
1
24
+ D && D = −E
βž”0=A+
Page | 24
1
24
− E , then: E = A +
1
24
1
1
) + 6 ∗ 24 − (−E) + E
12
3
2
From equation 3
1
1
1
3
3
24
4A + + 2E = 0 βž” 4A + + 2 ∗ (A +
1
1
3
12
4A + + 2A +
E=A+
1
24
5
5
πŸ“
= 0 βž” 6A + 12 = 0 βž” 6A = − 12 , then: 𝐀 = − πŸ•πŸ
βž”E=−
D = −E βž” D = − (−
Then:
)=0
5
72
+
1
24
1
=−
1
36
1
) = 36
36
1
(π‘₯+1)2 (π‘₯−1)(π‘₯ 2 +5)
=−
5
72(π‘₯+1)
=−
−
5
72(π‘₯+1)
1
12(π‘₯+1)2
−
+
1
12(π‘₯+1)
1
24(π‘₯−1)
2 +
+
1
24(π‘₯−1)
1
1
π‘₯−36
36
(π‘₯ 2 +5)
+
π‘₯−1
36(π‘₯ 2 +5)
Choice C
35] The partial Fraction decomposition of
π’™πŸ +πŸπ’™+πŸ‘
is
(𝒙−𝟏)𝟐 (𝒙−𝟐)(π’™πŸ +πŸ’)
−πŸ‘πŸ–
πŸ”
𝟏𝟏
πŸπŸ—π’™−πŸ”
−πŸ‘πŸ–
πŸ”
𝟏𝟏
πŸπŸ—π’™−πŸ”
πŸ‘πŸ–
πŸ”
𝟏𝟏
πŸπŸ—π’™−πŸ”
−πŸ‘πŸ–
πŸ”
𝟏𝟏
πŸπŸ—π’™−πŸ”
A- πŸπŸ“(𝒙−𝟏) − πŸ“(𝒙−𝟏)𝟐 + πŸ–(𝒙−𝟐) + (π’™πŸ +πŸ’) C- πŸπŸ“(𝒙−𝟏) + πŸ“(𝒙−𝟏)𝟐 + πŸ–(𝒙−𝟐) + (π’™πŸ +πŸ’)
B- πŸπŸ“(𝒙−𝟏) − πŸ“(𝒙−𝟏)𝟐 + πŸ–(𝒙−𝟐) + (π’™πŸ+πŸ’) D- πŸπŸ“(𝒙−𝟏) − πŸ“(𝒙−𝟏)𝟐 + πŸ–(𝒙−𝟐) − (π’™πŸ +πŸ’)
Solution:
π‘₯ 2 +2π‘₯+3
(π‘₯−1)2 (π‘₯−2)(π‘₯ 2 +4)
A
B
C
Dπ‘₯+E
= (π‘₯−1) + (π‘₯−1)2 + (π‘₯−2) + (π‘₯ 2
+4)
(Proper Fraction)
By multiplying in two sides by : (π‘₯ − 1)2 (π‘₯ − 2)(π‘₯ 2 + 4)
βž” π‘₯ 2 + 2π‘₯ + 3 = A(π‘₯ − 1)(π‘₯ − 2)(π‘₯ 2 + 4) + B(π‘₯ − 2)(π‘₯ 2 + 4)
+C(π‘₯ − 1)2 (π‘₯ 2 + 4) + (Dπ‘₯ + E)(π‘₯ − 1)2 (π‘₯ − 2)
= A(π‘₯ 4 − 3π‘₯ 3 + 6π‘₯ 2 − 12π‘₯ + 8) + B(π‘₯ 3 − 2π‘₯ 2 + 4π‘₯ − 8)
+ C(π‘₯ 4 − 2π‘₯ 3 + 5π‘₯ 2 − 8π‘₯ + 4)
+𝐷π‘₯ 4 − 4Dπ‘₯ 3 + 5Dπ‘₯ 2 − 2Dπ‘₯ + Eπ‘₯ 3 − 4Eπ‘₯ 2 + 5Eπ‘₯ − 2E
Page | 25
At 𝒙 = 𝟏 βž” 12 + 2 ∗ 1 + 3 = B(−1) ∗ 5 βž” 6 = −5B , then: 𝐁 = −
πŸ”
πŸ“
At 𝒙 = 𝟐 βž” 22 + 2 ∗ 2 + 3 = C(2 − 1)2 (22 + 4) βž” 11 = C(8) , then: 𝐂 =
Equating Coefficient (π’™πŸ’ )
βž”0=A+C+D=A+
11
8
+D=0βž”A+D=−
11
1
8
Equating Coefficient (π’™πŸ‘ )
6
22
5
8
βž” 0 = −3A + B − 2C − 4D + E βž” 0 = −3A − −
βž” 0 = −3A −
79
20
− 4D + E βž” 3A + 4D − E = −
− 4D + E
79
2
20
Equating Coefficient (π’™πŸ )
βž” 1 = 6A − 2B + 5C + 5D − 4E βž” 1 = 6A +
βž” 1 = 6A +
371
40
12
5
+
55
8
+ 5D − 4E
βž” 6A + 5D − 4E = −
+ 5D − 4E
331
3
40
Equating Coefficient (π’™πŸ )
βž” 2 = −12A + 4B − 8C − 2D + 5E
βž” 2 = −12A −
79
5
− 2D + 5E βž” 12A + 2D − 5E = −
89
5
4
By Solving Equations 2 , 3 , 4 together
3A + 4D − E = −
79
20
6A + 5D − 4E = −
βž” E = 3A + 4D +
331
40
79
)=−
20
βž” 6A + 5D − 12A − 16D −
79
Page | 26
301
40
20
2
βž” By substitute in E
βž” 6A + 5D − 4 (3A + 4D +
βž” −6A − 11D =
79
5
=−
3
331
40
331
40
βž” 6A + 11D = −
301
40
5
𝟏𝟏
πŸ–
12A + 2D − 5E = −
89
5
βž” By substitute in E
79
βž” 12A + 2D − 5 (3A + 4D +
)=−
20
βž” 12A + 2D − 15A − 20D −
79
βž” −3A − 18D =
39
20
=−
4
βž” A + 6D = −
4
89
5
89
5
13
6
20
Solve Equation 5 , 6 together
6A + 11D = −
A=−
13
20
301
40
13
, A + 6D = −
− 6D βž” 6 (−
βž”−
13
20
39
10
20
− 6D) + 11D = −
− 36D + 11D = −
29
βž” −25D = −
Then: 𝐀 = −
8
βž”πƒ=
301
40
301
40
πŸπŸ—
𝟐𝟎𝟎
πŸ‘πŸ–
πŸπŸ“
By Substitution in equation 2 :
3A + 4D − E = −
Then:
79
20
βž”3∗−
π‘₯ 2 +2π‘₯+3
(π‘₯−1)2 (π‘₯−2)(π‘₯ 2 +4)
π‘₯ 2 +2π‘₯+3
= (π‘₯−1)2 (π‘₯−2)(π‘₯ 2
+4)
=
=
38
25
+4∗
−38
25(π‘₯−1)
−38
25(π‘₯−1)
−
−
29
200
−E=−
6
5(π‘₯−1)2
6
5(π‘₯−1)2
+
+
79
20
11
+
8(π‘₯−2)
11
βž”π„=−
29
3
π‘₯−100
200
(π‘₯ 2 +4)
29π‘₯−6
8(π‘₯−2)
+ (π‘₯ 2
+4)
Choice A
36] The partial Fraction decomposition of
πŸ•
πŸπŸ‘
A- 𝟏 − 𝒙−𝟐 + 𝒙−πŸ‘
πŸ•
πŸπŸ‘
B- 𝟐 − 𝒙−𝟐 + 𝒙−πŸ‘
Page | 27
π’™πŸ +𝒙+𝟏
π’™πŸ −πŸ“π’™+πŸ”
πŸ•
πŸπŸ‘
πŸ•
πŸπŸ‘
C- 𝟏 + 𝒙−𝟐 + 𝒙−πŸ‘
D- 𝟏 − 𝒙−𝟐 − 𝒙−πŸ‘
is
πŸ‘
𝟏𝟎𝟎
Solution:
π‘₯ 2 +π‘₯+1
1
(Improper Fraction)
π‘₯ 2 −5π‘₯+6
π‘₯ 2 +π‘₯+1
π‘₯ 2 −5π‘₯+6
=1+
6π‘₯−5
6π‘₯−5
π‘₯ 2 − 5π‘₯ + 6
π‘₯ 2 −5π‘₯+6
π‘₯2 + π‘₯ + 1
−
π‘₯ − 5π‘₯ + 6
2
(Proper Fraction)
π‘₯ 2 −5π‘₯+6
6π‘₯−5
6π‘₯−5
π‘₯ 2 −5π‘₯+6
A
B
= (π‘₯−2)(π‘₯−3) = (π‘₯−2) + (π‘₯−3)
6π‘₯ − 5
By multiplying in two sides by : (π‘₯ − 2)(π‘₯ − 3)
βž” 6π‘₯ − 5 = A(π‘₯ − 3) + B(π‘₯ − 2)
At 𝒙 = πŸ‘ βž” 6 ∗ 3 − 5 = B(1) , then: 𝐁 = πŸπŸ‘
At 𝒙 = 𝟐 βž” 6 ∗ 2 − 5 = A(2 − 3) , 7 = A(−1) , then: 𝐀 = −πŸ•
6π‘₯−5
7
π‘₯ 2 −5π‘₯+6
Then:
13
= − (π‘₯−2) + (π‘₯−3)
π‘₯ 2 +π‘₯+1
π‘₯ 2 −5π‘₯+6
7
13
= 1 − (π‘₯−2) + (π‘₯−3)
Choice A
37] The partial Fraction decomposition of
πŸ“
𝟏
πŸ“
𝟏
A- πŸπ’™ + πŸ‘ + πŸ‘π’™+𝟏 + 𝒙−𝟏
B- πŸπ’™ − πŸ‘ + πŸ‘π’™+𝟏 + 𝒙−𝟏
πŸ”π’™πŸ‘ +πŸ“π’™πŸ −πŸ•
πŸ‘π’™πŸ −πŸπ’™−𝟏
πŸ“
3π‘₯ 2 −2π‘₯−1
6π‘₯ 3 +5π‘₯ 2 −7
3π‘₯ 2 −2π‘₯−1
𝟏
C- πŸπ’™ + πŸ‘ − πŸ‘π’™+𝟏 + 𝒙−𝟏
πŸ“
𝟏
D- πŸπ’™ + πŸ‘π’™+𝟏 + 𝒙−𝟏
Solution:
6π‘₯ 3 +5π‘₯ 2 −7
is
2π‘₯ + 3
(Improper Fraction)
= 2π‘₯ + 3 +
8π‘₯−4
3π‘₯ 2 − 2π‘₯ − 1
6π‘₯ 3 + 5π‘₯ 2 − 7
−
3
2
6π‘₯ − 4π‘₯ − 2π‘₯
3π‘₯ 2 −2π‘₯−1
9π‘₯ 2 + 2π‘₯ − 7
2
9π‘₯ − 6π‘₯ − 3
Page | 28
8π‘₯ − 4
−
4π‘₯−4
(Proper Fraction)
3π‘₯ 2 −2π‘₯−1
8π‘₯−4
8π‘₯−4
3π‘₯ 2 −2π‘₯−1
A
B
= (3π‘₯+1)(π‘₯−1) = (3π‘₯+1) + (π‘₯−1)
By multiplying in two sides by : (3π‘₯ + 1)(π‘₯ − 1)
βž” 8π‘₯ − 4 = A(π‘₯ − 1) + B(3π‘₯ + 1)
𝟏
1
1
At 𝒙 = − βž” 8 ∗ (− ) − 4 = A (− − 1) βž” −
πŸ‘
3
3
20
3
4
= A (− ) , then: 𝐀 = πŸ“
3
At 𝒙 = 𝟏 βž” 8 ∗ 1 − 4 = B(3 ∗ 1 + 1) βž” 4 = B(4) , then: 𝐁 = 𝟏
8π‘₯−4
A
3π‘₯ 2 −2π‘₯−1
Then:
B
5
1
= (3π‘₯+1) + (π‘₯−1) = (3π‘₯+1) + (π‘₯−1)
6π‘₯ 3 +5π‘₯ 2 −7
3π‘₯ 2 −2π‘₯−1
5
1
= 2π‘₯ + 3 + (3π‘₯+1) + (π‘₯−1)
Choice A
38] The partial Fraction decomposition of
πŸπ’™πŸ’ +πŸ‘π’™πŸ +𝟏
π’™πŸ +πŸ‘π’™+𝟐
−πŸ’πŸ“
πŸ”
C- πŸπ’™πŸ + πŸ”π’™ + πŸπŸ• + (𝒙+𝟐) − (𝒙+𝟏)
−πŸ’πŸ“
πŸ”
D- πŸπ’™πŸ − πŸ”π’™ + πŸπŸ• + (𝒙+𝟐) + (𝒙+𝟏)
A- πŸπ’™πŸ − πŸ”π’™ + πŸπŸ• − (𝒙+𝟐) + (𝒙+𝟏)
B- πŸπ’™πŸ − πŸ”π’™ + πŸπŸ• + (𝒙+𝟐) + (𝒙+𝟏)
Solution:
2π‘₯ 4 +3π‘₯ 2 +1
π‘₯ 2 +3π‘₯+2
2π‘₯ 4 +3π‘₯ 2 +1
π‘₯ 2 +3π‘₯+2
−39π‘₯−33
−39π‘₯−33
π‘₯ 2 +3π‘₯+2
=
−πŸ’πŸ“
πŸ”
πŸ’πŸ“
πŸ”
2π‘₯ 2 − 6π‘₯ + 17
(Improper Fraction)
= 2π‘₯ 2 − 6π‘₯ + 17 +
π‘₯ 2 + 3π‘₯ + 2
−39π‘₯−33
π‘₯ 2 +3π‘₯+2
(Proper Fraction)
π‘₯ 2 +3π‘₯+2
is
−39π‘₯−33
(π‘₯+2)(π‘₯+1)
=
A
B
+
(π‘₯+2)
(π‘₯+1)
By multiplying in two sides by : (π‘₯ + 2)(π‘₯ + 1)
βž” −39π‘₯ − 33 = A(π‘₯ + 1) + B(π‘₯ + 2)
2π‘₯ 4 + 3π‘₯ 2 + 1
4
3
2π‘₯ + 6π‘₯ + 4π‘₯
−6π‘₯ 3 − π‘₯ 2 + 1
3
2
−
−
−6π‘₯ − 18π‘₯ − 12π‘₯
17π‘₯ 2 + 12π‘₯ + 1
2
17π‘₯ + 51π‘₯ + 34
−39π‘₯ − 33
Page | 29
2
−
At 𝒙 = −𝟐 βž” −39 ∗ (−2) − 33 = A(−2 + 1) βž” 45 = −A , then: 𝐀 = −πŸ’πŸ“
At 𝒙 = −𝟏 βž” −39 ∗ (−1) − 33 = B(−1 + 2) βž” 6 = B , then: 𝐁 = πŸ”
−39π‘₯−33
π‘₯ 2 +3π‘₯+2
Then:
A
B
−45
6
= (π‘₯+2) + (π‘₯+1) = (π‘₯+2) + (π‘₯+1)
2π‘₯ 4 +3π‘₯ 2 +1
π‘₯ 2 +3π‘₯+2
45
6
= 2π‘₯ 2 − 6π‘₯ + 17 − (π‘₯+2) + (π‘₯+1)
Choice B
π’™πŸ‘ +𝟏
39] The partial Fraction decomposition of
𝟏+𝒙
C- 𝒙 − π’™πŸ +𝟏
𝟏−𝒙
𝟏−𝒙
B- πŸπ’™ + π’™πŸ +𝟏
D- 𝒙 + π’™πŸ +𝟏
Solution:
π‘₯ 2 +1
π‘₯ 3 +1
π‘₯ 2 +1
π‘₯
(Improper Fraction)
=π‘₯+
π‘₯2 + 1
1−π‘₯
π‘₯3 + 1
3
π‘₯ +π‘₯
π‘₯ 2 +1
40] The partial Fraction decomposition of
πŸ”πŸ’
𝟏
πŸ‘πŸπŸ
A- 𝒙 + 𝟐 + πŸπŸ“(𝒙−𝟏) + πŸ“(𝒙−𝟏)𝟐 + πŸπŸ“(𝒙+πŸ’)
πŸ”πŸ’
𝟏
πŸ‘πŸπŸ
B- 𝒙 − πŸπŸ“(𝒙−𝟏) + πŸ“(𝒙−𝟏)𝟐 + πŸπŸ“(𝒙+πŸ’)
πŸ”πŸ’
𝟏
πŸ‘πŸπŸ
C- 𝒙 − 𝟐 + πŸπŸ“(𝒙−𝟏) + πŸ“(𝒙−𝟏)𝟐 + πŸπŸ“(𝒙+πŸ’)
𝟏
πŸ‘πŸπŸ
D- πŸπŸ“(𝒙+𝟏) + πŸ“(𝒙−𝟏)𝟐 + πŸπŸ“(𝒙+πŸ’)
Page | 30
−
1−π‘₯
Choice D
πŸ”πŸ’
is
𝟏−𝒙
A- 𝒙 + π’™πŸ +𝟏
π‘₯ 3 +1
π’™πŸ +𝟏
π’™πŸ’ +πŸ’π’™πŸ +𝒙−πŸ“
π’™πŸ‘ +πŸπ’™πŸ −πŸ•π’™+πŸ’
is
Solution:
π‘₯ 4 +4π‘₯ 2 +π‘₯−5
(Improper Fraction)
π‘₯ 3 +2π‘₯ 2 −7π‘₯+4
π‘₯ 4 +4π‘₯ 2 +π‘₯−5
π‘₯ 3 +2π‘₯ 2 −7π‘₯+4
=π‘₯−2+
15π‘₯ 2 −17π‘₯+3
π‘₯ 3 +2π‘₯ 2 −7π‘₯+4
π‘₯ 3 +2π‘₯ 2 −7π‘₯+4
(Proper Fraction)
π‘₯ 3 +2π‘₯ 2 −7π‘₯+4
15π‘₯ 2 −17π‘₯+3
15π‘₯ 2 −17π‘₯+3
=
15π‘₯ 2 −17π‘₯+3
π‘₯ 3 +2π‘₯ 2 −3π‘₯−4π‘₯+4
=
15π‘₯ 2 −17π‘₯+3
15π‘₯ 2 −17π‘₯+3
π‘₯(π‘₯ 2 +2π‘₯−3)−4(π‘₯−1)
15π‘₯ 2 −17π‘₯+3
= (π‘₯−1)(π‘₯(π‘₯+3)−4) = (π‘₯−1)(π‘₯ 2
βž”
15π‘₯ 2 −17π‘₯+3
(π‘₯−1)2 (π‘₯+4)
A
B
+3π‘₯−4)
=
15π‘₯ 2 −17π‘₯+3
π‘₯(π‘₯+3)(π‘₯−1)−4(π‘₯−1)
15π‘₯ 2 −17π‘₯+3
= (π‘₯−1)(π‘₯+4)(π‘₯−1) =
15π‘₯ 2 −17π‘₯+3
(π‘₯−1)2 (π‘₯+4)
C
= (π‘₯−1) + (π‘₯−1)2 + (π‘₯+4)
By multiplying in two sides by : (π‘₯ − 1)2 (π‘₯ + 4)
βž” 15π‘₯ 2 − 17π‘₯ + 3 = A(π‘₯ − 1)(π‘₯ + 4) + B(π‘₯ + 4) + C(π‘₯ − 1)2
βž” 15π‘₯ 2 − 17π‘₯ + 3 = A(π‘₯ − 1)(π‘₯ + 4) + B(π‘₯ + 4) + C(π‘₯ − 1)2
= Aπ‘₯ 2 + 3Aπ‘₯ − 4A + Bπ‘₯ + 4B + Cπ‘₯ 2 − 2π‘₯ + 1
At 𝒙 = 𝟏 βž” 15 ∗ (1)2 − 17 ∗ 1 + 3 = B(1 + 4) , then: 𝐁 =
𝟏
πŸ“
At 𝒙 = −πŸ’ βž” 15 ∗ (−4)2 − 17 ∗ (−4) + 3 = C(−4 − 1)2 βž” 311 = 25C , then: 𝐂 =
Equating Coefficient (π’™πŸ )
15 = A + C βž” A = 15 −
15π‘₯ 2 −17π‘₯+3
(π‘₯−1)2 (π‘₯+4)
Then:
64
25(π‘₯−1)
π‘₯ 4 +4π‘₯ 2 +π‘₯−5
π‘₯ 3 +2π‘₯ 2 −7π‘₯+4
Choice C
Page | 31
=
+
311
25
, then: 𝐀 =
1
5(π‘₯−1)
2 +
=π‘₯−2+
πŸ”πŸ’
πŸπŸ“
311
25(π‘₯+4)
64
25(π‘₯−1)
+
1
5(π‘₯−1)2
+
311
25(π‘₯+4)
πŸ‘πŸπŸ
πŸπŸ“
41] The partial Fraction decomposition of
𝟐
𝟏
𝟐
𝟏
πŸ—π’™πŸ +πŸπŸŽπ’™−𝟏𝟎
is
(𝒙+𝟐)(πŸ‘π’™−𝟏)
𝟐
A- 𝟐 + (𝒙+𝟐) − (πŸ‘π’™−𝟏)
𝟏
C- (𝒙+𝟐) − (πŸ‘π’™−𝟏)
𝟐
B- πŸ‘ + (𝒙+𝟐) + (πŸ‘π’™−𝟏)
𝟏
D-πŸ‘ + (𝒙+𝟐) − (πŸ‘π’™−𝟏)
Solution:
9π‘₯ 2 +20π‘₯−10
(π‘₯+2)(3π‘₯−1)
=
9π‘₯ 2 +20π‘₯−10
(π‘₯+2)(3π‘₯−1)
= 3 + (π‘₯+2)(3π‘₯−1)
3π‘₯ 2 +5π‘₯−2
3
(Improper Fraction)
5π‘₯−4
3π‘₯ 2 + 5π‘₯ − 2
9π‘₯ 2 + 20π‘₯ − 10
2
5π‘₯−4
(π‘₯+2)(3π‘₯−1)
5π‘₯−4
(π‘₯+2)(3π‘₯−1)
9π‘₯ 2 +20π‘₯−10
(Proper Fraction)
=
A
(π‘₯+2)
+
9π‘₯ + 15π‘₯ − 6
5π‘₯ − 4
B
(3π‘₯−1)
By multiplying in two sides by : (π‘₯ + 2)(3π‘₯ − 1)
βž” 5π‘₯ − 4 = A(3π‘₯ − 1) + B(π‘₯ + 2)
At 𝒙 = −𝟐 βž” 5 ∗ (−2) − 4 = A(3 ∗ (−2) − 1) , then: A = 2
𝟏
1
1
πŸ‘
3
3
At 𝒙 = βž” 5 ∗ − 4 = B ( + 2) , then: B = −1
5π‘₯−4
(π‘₯+2)(3π‘₯−1)
Then:
9π‘₯ 2 +20π‘₯−10
(π‘₯+2)(3π‘₯−1)
Choice D
Page | 32
2
1
= (π‘₯+2) − (3π‘₯−1)
2
1
= 3 + (π‘₯+2) − (3π‘₯−1)
−
42] If 𝒇(𝒙, π’š) = π’™πŸ‘ + π’™πŸ π’šπŸ‘ − πŸπ’šπŸ then 𝒇𝒙 (𝟐, 𝟏) , π’‡π’š (𝟏, 𝟐)
respectively equal
A- πŸπŸ” , πŸ’
C- πŸ’ , πŸπŸ”
B- 𝟎 , πŸπŸ”
D- None of them
Solution:
𝑓π‘₯ =
πœ•π‘“
πœ•π‘₯
= 3π‘₯ 2 + 2π‘₯𝑦 3 − 0 , At (𝟐, 𝟏) βž” 3 ∗ 22 + 2 ∗ 2 ∗ 13 = 12 + 4 =
16
Then: 𝑓π‘₯ (2,1) = 16
𝑓𝑦 =
πœ•π‘“
πœ•π‘¦
= 0 + 3π‘₯ 2 𝑦 2 − 4𝑦 , At (𝟏, 𝟐) βž” 3 ∗ 12 ∗ 22 − 4 ∗ 2 = 12 − 8 = 4
Then: 𝑓𝑦 (1,2) = 4
Choice A
Page | 33
𝒙
43] If 𝒇(𝒙, π’š) = π’”π’Šπ’ (𝟏+π’š) then 𝒇𝒙 , π’‡π’š respectively equal
AB-
𝐜𝐨𝐬(
𝒙
)
𝟏+π’š
𝟏+π’š
𝐜𝐨𝐬(
𝒙
)
𝟏+π’š
𝟏+π’š
,
,
𝒙
)
𝟏+π’š
(𝟏+π’š)𝟐
C-
𝒙
)
𝟏+π’š
(𝟏+π’š)𝟐
D- None of them
−𝒙 𝐜𝐨𝐬(
−𝒙 𝐬𝐒𝐧(
𝒙
)
𝟏+π’š
(𝟏+π’š)𝟐
−𝒙 𝐜𝐨𝐬(
,
𝐜𝐨𝐬(
𝒙
)
𝟏+π’š
𝟏+π’š
Solution:
π‘₯
𝑓π‘₯ =
𝑓𝑦 =
πœ•π‘“
πœ•π‘₯
πœ•π‘“
πœ•π‘¦
π‘₯
= cos (
πœ•
1+𝑦
= cos (
π‘₯
π‘₯
π‘₯
cos(1+𝑦)
1
) ⋅ πœ•π‘₯ (1+𝑦) = cos (1+𝑦) ⋅ 1+𝑦 =
πœ•
1+𝑦
π‘₯
) ⋅ πœ•π‘¦ (1+𝑦)
1+𝑦
= cos (
π‘₯
1+𝑦
)⋅
((1+𝑦)⋅0)−(π‘₯⋅1)
(1+𝑦)2
= cos (
π‘₯
1+𝑦
−π‘₯
) ⋅ (1+𝑦)2 =
π‘₯
)
1+𝑦
(1+𝑦)2
−π‘₯ cos(
Choice A
πœ•π‘§
πœ•π‘§
44] Find πœ•π‘₯ , πœ•π‘¦ respectively if z is defined by (π‘₯, 𝑦) where
π‘₯ 3 + 𝑦 3 + 𝑧 3 + 6π‘₯𝑦𝑧 = 1
π’™πŸ +πŸπ’šπ’›
π’šπŸ +πŸπ’™π’›
π’šπŸ +πŸπ’™π’›
A- −π’›πŸ−πŸπ’™π’š , − −π’›πŸ −πŸπ’™π’š
π’™πŸ +πŸπ’šπ’›
B- −π’›πŸ−πŸπ’™π’š ,
C- −π’›πŸ −πŸπ’™π’š , −π’›πŸ −πŸπ’™π’š
π’šπŸ −πŸπ’™π’›
π’™πŸ +πŸπ’šπ’›
D- −π’›πŸ −πŸπ’™π’š ,
−π’›πŸ −πŸπ’™π’š
Solution:
𝑓π‘₯ =
πœ•π‘“
πœ•π‘₯
= 3π‘₯ 2 + 0 + 3𝑧 2 ⋅
3π‘₯ 2 + 6𝑦𝑧 +
πœ•π‘§
πœ•π‘₯
3π‘₯ 2 + 6𝑦𝑧 = −
Page | 34
πœ•π‘§
πœ•π‘₯
+ 6𝑦𝑧 + 6π‘₯𝑦 ⋅
(3𝑧 2 + 6π‘₯𝑦) = 0
πœ•π‘§
πœ•π‘₯
π’™πŸ +πŸπ’šπ’›
(3𝑧 2 + 6π‘₯𝑦)
πœ•π‘§
πœ•π‘₯
=0
π’šπŸ +πŸπ’™π’›
−π’›πŸ −πŸπ’™π’š
πœ•π‘§
=
πœ•π‘₯
𝑓𝑦 =
3π‘₯ 2 +6𝑦𝑧
−(3𝑧 2 +6π‘₯𝑦)
πœ•π‘“
πœ•π‘¦
πœ•π‘§
πœ•π‘¦
3𝑦 2 + 6π‘₯𝑧 = −
πœ•π‘¦
=
3(π‘₯ 2 +2𝑦𝑧)
−3(𝑧 2 +2π‘₯𝑦)
= 0 + 3𝑦 2 + 3𝑧 2 ⋅
3𝑦 2 + 6π‘₯𝑧 +
πœ•π‘§
=
3𝑦 2 +6π‘₯𝑧
−(3𝑧 2 +6π‘₯𝑦)
πœ•π‘§
πœ•π‘¦
=
π‘₯ 2 +2𝑦𝑧
−𝑧 2 −2π‘₯𝑦
+ 6π‘₯𝑧 + 6π‘₯𝑦 ⋅
πœ•π‘§
πœ•π‘¦
=0
(3𝑧 2 + 6π‘₯𝑦) = 0
πœ•π‘§
πœ•π‘¦
=
(3𝑧 2 + 6π‘₯𝑦)
3(𝑦 2 +2π‘₯𝑧)
−3(𝑧 2 +2π‘₯𝑦)
=
𝑦 2 +2π‘₯𝑧
−𝑧 2 −2π‘₯𝑦
Choice D
45] Find the second partial derivative of 𝒇(𝒙, π’š) = π’™πŸ‘ + π’™πŸ π’šπŸ‘ − πŸπ’šπŸ
[𝒇𝒙𝒙 , π’‡π’™π’š , π’‡π’šπ’™ , π’‡π’šπ’š ] respectively
A- πŸ”π’™ + πŸπ’šπŸ‘ / πŸ”π’™π’šπŸ / πŸ”π’™π’šπŸ / πŸ”π’™πŸ π’š − πŸ’
B- πŸ”π’™πŸ π’š − πŸ’ / πŸ”π’™π’šπŸ / πŸ”π’™π’šπŸ / πŸ”π’™ − πŸπ’šπŸ‘
C- πŸ”π’™πŸ π’š − πŸ’ / πŸ”π’™π’šπŸ / πŸ”π’™ + πŸπ’šπŸ‘ / πŸ”π’™π’šπŸ
D- None of them
Solution:
𝑓π‘₯ = 3π‘₯ 2 + 2π‘₯𝑦 3 , 𝑓𝑦 = 3π‘₯ 2 𝑦 2 − 4𝑦
𝑓π‘₯π‘₯ = 6π‘₯ + 2𝑦 3
𝑓π‘₯𝑦 = 6π‘₯𝑦 2
𝑓𝑦π‘₯ = 6π‘₯𝑦 2
𝑓𝑦𝑦 = 6π‘₯ 2 𝑦 − 4
Note
Choice A
Page | 35
Since 𝑓π‘₯𝑦 = 𝑓𝑦π‘₯ , then: the Function is continuous.
46] Find π’‡π’™π’™π’šπ’› of 𝒇(𝒙, π’š, 𝒛) = 𝐬𝐒𝐧(πŸ‘π’™ + π’šπ’›)
A- −πŸ— 𝐜𝐨𝐬(πŸ‘π’™ + π’šπ’›) − πŸ—π’šπ’› 𝐬𝐒𝐧(πŸ‘π’™ + π’šπ’›)
B- −πŸ— 𝐜𝐨𝐬(πŸ‘π’™ + π’šπ’›) + πŸ—π’šπ’› 𝐬𝐒𝐧(πŸ‘π’™ + π’šπ’›)
C- −πŸ— 𝐜𝐨𝐬(πŸ‘π’™ + π’šπ’›) + πŸ—π’šπ’› 𝐬𝐒𝐧(πŸ‘π’™ − π’šπ’›)
D- πŸ— 𝐜𝐨𝐬(πŸ‘π’™ + π’šπ’›) + πŸ—π’šπ’› 𝐬𝐒𝐧(πŸ‘π’™ + π’šπ’›)
Solution:
𝑓π‘₯ = cos(3π‘₯ + 𝑦𝑧) ∗ 3 = 3 cos(3π‘₯ + 𝑦𝑧)
𝑓π‘₯π‘₯ = −3 sin(3π‘₯ + 𝑦𝑧) ∗ 3 = − 9 sin(3π‘₯ + 𝑦𝑧)
𝑓π‘₯π‘₯𝑦 = −9 cos(3π‘₯ + 𝑦𝑧) ∗ 𝑧 = −9𝑧 cos(3π‘₯ + 𝑦𝑧)
𝑓π‘₯π‘₯𝑦𝑧 = −9 cos(3π‘₯ + 𝑦𝑧) + 9𝑦𝑧 sin(3π‘₯ + 𝑦𝑧)
Choice B
47] Find the first partial derivative of the following functions :
( I ) 𝒇(𝒙, π’š) = π’™πŸ’ π’šπŸ‘ + πŸ–π’™πŸ π’š [𝒇𝒙 , π’‡π’š ] respectively
A- πŸ’π’™πŸ‘ π’šπŸ‘ + πŸπŸ”π’™π’š , πŸ‘π± πŸ’ π’šπŸ + πŸ–π’™πŸ
B- πŸ‘π’™πŸ’ π’šπŸ + πŸ–π’™πŸ , πŸ’π’™πŸ‘ π’šπŸ‘ + πŸπŸ”π’™π’š
C- πŸ’π’™πŸ‘ π’šπŸ‘ + πŸπŸ”π’™π’š , πŸ‘π’™πŸ’ π’šπŸ − πŸ–π’™πŸ
D- None of them
Solution:
𝑓π‘₯ = 4π‘₯ 3 𝑦 3 + 16π‘₯𝑦 , 𝑓𝑦 = 3π‘₯ 4 𝑦 2 + 8π‘₯ 2
Choice A
Page | 36
πŸ“
( II ) π’ˆ(𝒖, 𝒗) = (π’–πŸ 𝒗 − π’—πŸ‘ ) [π’ˆπ’– , π’ˆπ’— ] respectively
πŸ’
πŸ’
A- πŸπŸŽπ’–π’—(π’–πŸ 𝒗 + π’—πŸ‘ ) , πŸ“(π’–πŸ 𝒗 − π’—πŸ‘ ) (π’–πŸ − πŸ‘π’—πŸ )
πŸ’
B- πŸ“(π’–πŸ 𝒗 − π’—πŸ‘ ) (π’–πŸ − πŸ‘π’—πŸ ) , πŸπŸŽπ’–π’—(π’–πŸ 𝒗 − π’—πŸ‘ )
πŸ’
πŸ’
πŸ’
C- πŸπŸŽπ’–π’—(π’–πŸ 𝒗 − π’—πŸ‘ ) , πŸ“(π’–πŸ 𝒗 − π’—πŸ‘ ) (π’–πŸ − πŸ‘π’—πŸ )
D- None of them
Solution:
𝑔𝑒 = 5(𝑒2 𝑣 − 𝑣 3 )4 ∗ 2𝑒𝑣 = 10𝑒𝑣 (𝑒2 𝑣 − 𝑣 3 )4
𝑔𝑣 = 5(𝑒2 𝑣 − 𝑣 3 )4 ∗ (𝑒2 − 3𝑣 2 )
Choice C
( III ) 𝒇(𝒙, 𝒕) = 𝒆−𝒕 𝒄𝒐𝒔 𝝅𝒙 [𝒇𝒙 , 𝒇𝒕 ] respectively
A- −𝒆−𝒕 𝒄𝒐𝒔 𝝅𝒙 , 𝝅𝒆−𝒕 π’”π’Šπ’ 𝝅𝒙
B- 𝝅𝒆−𝒕 π’”π’Šπ’ 𝝅𝒙 , −𝒆−𝒕 𝒄𝒐𝒔 𝝅𝒙
C- −𝝅𝒆−𝒕 π’”π’Šπ’ 𝝅𝒙 , −𝒆−𝒕 𝒄𝒐𝒔 𝝅𝒙
D- None of them
Solution:
𝑓π‘₯ = (−𝑒 −𝑑 𝑠𝑖𝑛 πœ‹π‘₯ ) ∗ πœ‹ = −πœ‹π‘’ −𝑑 𝑠𝑖𝑛 πœ‹π‘₯
𝑓𝑑 = −𝑒 −𝑑 π‘π‘œπ‘  πœ‹π‘₯
Choice C
Page | 37
( IV ) 𝒇(𝒙, π’š) = √𝒙 𝒍𝒏 𝒕 [𝒇𝒙 , 𝒇𝒕 ] respectively
𝒍𝒏 𝒕
A- 𝟐
C-
√
√𝒙
𝒕
,
𝒙
√𝒙 𝒍𝒏 𝒕
,
𝒕 𝟐 √𝒙
B-
𝒍𝒏 𝒕 √𝒙
,
√𝒙 𝒕
D- None of them
Solution:
𝑙𝑛 𝑑
𝑓π‘₯ =
2√π‘₯
𝑓𝑑 =
√π‘₯
𝑑
Choice A
𝒙
( V ) 𝒇(𝒙, π’š) = π’š [𝒇𝒙 , π’‡π’š ] respectively
𝟏
𝒙
A- π’š ,− π’š
𝟏
𝒙
C- π’š , π’šπŸ
B-
𝟏
πŸ“
,− π’šπŸ
π’š
D- None of them
Solution:
𝑓π‘₯ =
π‘₯
𝑦
1
𝑦
= π‘₯𝑦 −1 βž” 𝑓𝑦 = −π‘₯𝑦 −2 = −
Choice D
Page | 38
π‘₯
𝑦2
48] If 𝒇(𝒙, π’š) is a differentiable function such that 𝒙 = 𝒙(𝒓, 𝒔) and
π’š = π’š(𝒓, 𝒔) , then
𝝏𝒇
𝝏𝒇 𝝏𝒇
𝝏𝒙 ππ’š
𝝏𝒇
𝝏𝒇 𝒅𝒙
𝝏𝒇 π’…π’š
A- 𝝏𝒓 = 𝝏𝒙 ππ’š + 𝝏𝒓 𝝏𝒓
C- 𝝏𝒓 = 𝝏𝒙 𝒅𝒓 + ππ’š 𝒅𝒓
𝝏𝒇
𝒅𝒇 𝝏𝒙
𝒅𝒇 ππ’š
𝝏𝒇
𝝏𝒇 𝝏𝒙
𝝏𝒇 ππ’š
B- 𝝏𝒓 = 𝒅𝒙 𝝏𝒓 + π’…π’š 𝝏𝒓
D- 𝝏𝒓 = 𝝏𝒙 𝝏𝒓 + ππ’š 𝝏𝒓
Solution:
Since 𝑓(π‘₯, 𝑦) has 2 variables && π‘₯ and 𝑦 have 2 variables too
Then:
πœ•π‘“
πœ•π‘Ÿ
=
πœ•π‘“ πœ•π‘₯
πœ•π‘₯ πœ•π‘Ÿ
+
πœ•π‘“ πœ•π‘¦
πœ•π‘¦ πœ•π‘Ÿ
Choice D
49] If 𝒇(𝒙, π’š) is differentiable at (𝒂, 𝒃) , then
A- 𝒇(𝒙, π’š) is continuous at (𝒂, 𝒃)
B- 𝒇(𝒙, π’š) is not continuous at (𝒂, 𝒃)
C- 𝒇(𝒙, π’š) is not defined at (𝒂, 𝒃)
D- None of them
Solution:
Since 𝑓 (π‘₯, 𝑦) is differentiable at (π‘Ž, 𝑏) βž” 𝑓(π‘₯, 𝑦) is continuous at (π‘Ž, 𝑏)
Choice A
𝝏𝒖
50] If 𝒖(𝒙, π’š) = π₯𝐧(π’™πŸ + π’š + 𝟐) , then 𝝏𝒙 at (𝟏, πŸ‘) is
𝟏
A- πŸ”
𝟏
C- πŸ‘
Page | 39
𝟏
B- 𝟐
D- None of them
Solution:
πœ•π‘’
πœ•π‘₯
=
2π‘₯
π‘₯ 2 +𝑦+2
At (1,3) βž”
2π‘₯
π‘₯ 2 +𝑦+2
=
2∗1
12 +3+2
2
1
6
3
= =
Choice B
51] If 𝒇(𝒙, π’š) is a differentiable function such that 𝒙 = 𝒙(𝒓) and
π’š = π’š(𝒓) , then
𝝏𝒇
𝝏𝒇 𝝏𝒇
𝝏𝒙 ππ’š
𝝏𝒇
𝝏𝒇 𝒅𝒙
𝝏𝒇 π’…π’š
A- 𝝏𝒓 = 𝝏𝒙 ππ’š + 𝝏𝒓 𝝏𝒓
𝝏𝒇
𝒅𝒇 𝝏𝒙
𝒅𝒇 ππ’š
𝝏𝒇
𝝏𝒇 𝝏𝒙
𝝏𝒇 ππ’š
B- 𝝏𝒓 = 𝒅𝒙 𝝏𝒓 + π’…π’š 𝝏𝒓
C- 𝝏𝒓 = 𝝏𝒙 𝒅𝒓 + ππ’š 𝒅𝒓
D- 𝝏𝒓 = 𝝏𝒙 𝝏𝒓 + ππ’š 𝝏𝒓
Solution:
Since 𝑓(π‘₯, 𝑦) has 2 variables && π‘₯ and 𝑦 have 1 variable each
Then:
πœ•π‘“
πœ•π‘Ÿ
=
πœ•π‘“ 𝑑π‘₯
πœ•π‘₯ π‘‘π‘Ÿ
+
πœ•π‘“ 𝑑𝑦
πœ•π‘¦ π‘‘π‘Ÿ
Choice C
𝝏𝟐 𝒖
𝟐
52] If 𝒖(𝒙, π’š) = π₯𝐧(𝒙 + π’š + 𝟐) , then ππ’šπŸ at (𝟏, πŸ‘) is
𝟏
𝟏
A- πŸ‘πŸ”
B- πŸ”
𝟏
𝟏
C- − πŸ‘πŸ”
D- − πŸ”
Solution:
πœ•π‘’
πœ•π‘¦
=
1
π‘₯ 2 +𝑦+2
Page | 40
πœ•2 𝑒
πœ•π‘¦ 2
=
(π‘₯ 2 +𝑦+2)∗0−1∗(1)
(π‘₯ 2 +𝑦+2)2
= (12
−1
−1
+3+2)2
= (6)2 =
−1
36
Choice C
53] Determine whether each of the following functions is a solution
of the Laplace’s equation
I- 𝒖(𝒙, 𝒕) = 𝐬𝐒𝐧(𝒙 − 𝒂𝒕)
III- 𝒖(𝒙, 𝒕) = 𝒆𝒙−𝒕
II- 𝒖(𝒙, 𝒕) = 𝐬𝐒𝐧(𝒙 + 𝒕) IV- 𝒖(𝒙, 𝒕) = 𝒆𝒙 𝐬𝐒𝐧 𝒕
A] I and II
B] I , II and III
C] IV only
D] I and IV
Solution:
I ] 𝑒(π‘₯, 𝑑) = sin(π‘₯ − π‘Žπ‘‘)
𝑒π‘₯ = cos(π‘₯ − π‘Žπ‘‘)
𝑒π‘₯π‘₯ = − sin(π‘₯ − π‘Žπ‘‘)
𝑒𝑑 = cos(π‘₯ − π‘Žπ‘‘) ∗ −π‘Ž = −π‘Ž cos(π‘₯ − π‘Žπ‘‘)
𝑒𝑑𝑑 = −π‘Ž ∗ − sin(π‘₯ − π‘Žπ‘‘) ∗ −π‘Ž = −π‘Ž2 sin(π‘₯ − π‘Žπ‘‘)
𝑒π‘₯π‘₯ + 𝑒𝑑𝑑 = − sin(π‘₯ − π‘Žπ‘‘) + (−π‘Ž2 sin(π‘₯ − π‘Žπ‘‘)) ≠ 0
Then 𝒖 doesn’t satisfy Laplace’s equation
II ] 𝑒(π‘₯, 𝑑) = sin(π‘₯ + 𝑑)
𝑒π‘₯ = cos(π‘₯ + 𝑑) , 𝑒π‘₯π‘₯ = − sin(π‘₯ + 𝑑)
𝑒𝑑 = cos(π‘₯ + 𝑑) , 𝑒𝑑𝑑 = − sin(π‘₯ + 𝑑)
𝑒π‘₯π‘₯ + 𝑒𝑑𝑑 = − sin(π‘₯ + 𝑑) + (− sin(π‘₯ + 𝑑)) = −2 sin(π‘₯ + 𝑑) ≠ 0
Then 𝒖 doesn’t satisfy Laplace’s equation
Page | 41
III ] 𝑒(π‘₯, 𝑑) = 𝑒 π‘₯−𝑑
𝑒π‘₯ = 𝑒 π‘₯−𝑑 , 𝑒π‘₯π‘₯ = 𝑒 π‘₯−𝑑
𝑒𝑑 = 𝑒 π‘₯−𝑑 ∗ −1 = −𝑒 π‘₯−𝑑
𝑒𝑑𝑑 = −𝑒 π‘₯−𝑑 ∗ −1 = 𝑒 π‘₯−𝑑
𝑒π‘₯π‘₯ + 𝑒𝑑𝑑 = 𝑒 π‘₯−𝑑 + 𝑒 π‘₯−𝑑 = 2𝑒 π‘₯−𝑑 ≠ 0
Then 𝒖 doesn’t satisfy Laplace’s equation
IV ] 𝑒(π‘₯, 𝑑) = 𝑒π‘₯ sin 𝑑
𝑒π‘₯ = 𝑒 π‘₯ sin 𝑑 , 𝑒π‘₯π‘₯ = 𝑒 π‘₯ sin 𝑑
𝑒𝑑 = 𝑒 π‘₯ cos 𝑑 , 𝑒𝑑𝑑 = −𝑒 π‘₯ sin 𝑑
𝑒π‘₯π‘₯ + 𝑒𝑑𝑑 = 𝑒 π‘₯ sin 𝑑 + (−𝑒 π‘₯ sin 𝑑) = 0
Then 𝒖 satisfies Laplace’s equation
Choice C
54] Determine whether each of the following functions is a solution
of the Wave equation
I- 𝒖(𝒙, 𝒕) = (𝒙 − 𝒂𝒕)πŸ” + (𝒙 + 𝒂𝒕)πŸ”
II- 𝒖(𝒙, 𝒕) = 𝐬𝐒𝐧(𝒙 − 𝒂𝒕) + 𝒍𝒏(𝒙 + 𝒂𝒕)
III- 𝒖(𝒙, 𝒕) = 𝐬𝐒𝐧(𝒙 − 𝒂𝒕)
A] I and II
B] I , II and III
C] I
D] II and III
Page | 42
Solution:
I ] 𝑒(π‘₯, 𝑑) = (π‘₯ − π‘Žπ‘‘)6 + (π‘₯ + π‘Žπ‘‘)6
𝑒π‘₯ = 6(π‘₯ − π‘Žπ‘‘)5 + 6(π‘₯ + π‘Žπ‘‘)5
𝑒π‘₯π‘₯ = 30(π‘₯ − π‘Žπ‘‘)4 + 30(π‘₯ + π‘Žπ‘‘)4
𝑒𝑑 = 6(π‘₯ − π‘Žπ‘‘)5 ∗ (−π‘Ž) + 6(π‘₯ + π‘Žπ‘‘)5 ∗ π‘Ž = −6π‘Ž(π‘₯ − π‘Žπ‘‘)5 + 6π‘Ž(π‘₯ + π‘Žπ‘‘)5
𝑒𝑑𝑑 = −6π‘Ž(π‘₯ − π‘Žπ‘‘)4 ∗ 5 ∗ (−π‘Ž) + 6π‘Ž(π‘₯ + π‘Žπ‘‘)4 ∗ 5 ∗ π‘Ž
= 30π‘Ž2 (π‘₯ − π‘Žπ‘‘)4 + 30π‘Ž2 (π‘₯ + π‘Žπ‘‘)4
𝑒𝑑𝑑 = π‘Ž2 𝑒π‘₯π‘₯ βž” 30π‘Ž2 (π‘₯ − π‘Žπ‘‘)4 + 30π‘Ž2 (π‘₯ + π‘Žπ‘‘)4 = π‘Ž2 (30(π‘₯ − π‘Žπ‘‘)4 +
30(π‘₯ + π‘Žπ‘‘)4 )
Then 𝒖 satisfies Wave equation
II ] 𝑒(π‘₯, 𝑑) = 𝑠𝑖𝑛(π‘₯ − π‘Žπ‘‘) + 𝑙𝑛(π‘₯ + π‘Žπ‘‘)
𝑒π‘₯ = cos(π‘₯ − π‘Žπ‘‘) +
1
π‘₯+π‘Žπ‘‘
𝑒𝑑 = cos(π‘₯ − π‘Žπ‘‘) ∗ −π‘Ž +
1
, 𝑒π‘₯π‘₯ = − sin(π‘₯ − π‘Žπ‘‘) − (π‘₯+π‘Žπ‘‘)2
π‘Ž
π‘₯+π‘Žπ‘‘
π‘Ž2
𝑒𝑑𝑑 = −π‘Ž2 sin(π‘₯ − π‘Žπ‘‘) − (π‘₯+π‘Žπ‘‘)2
π‘Ž2
1
𝑒𝑑𝑑 = π‘Ž2 𝑒π‘₯π‘₯ βž” −π‘Ž2 sin(π‘₯ − π‘Žπ‘‘) − (π‘₯+π‘Žπ‘‘)2 = π‘Ž2 (− sin(π‘₯ − π‘Žπ‘‘) − (π‘₯+π‘Žπ‘‘)2 )
Then 𝒖 satisfies Wave equation
III ] 𝑒(π‘₯, 𝑑) = sin(π‘₯ − π‘Žπ‘‘)
𝑒π‘₯ = cos(π‘₯ − π‘Žπ‘‘) , 𝑒𝑑 = −π‘Ž cos(π‘₯ − π‘Žπ‘‘)
𝑒π‘₯π‘₯ = − sin(π‘₯ − π‘Žπ‘‘) , 𝑒𝑑𝑑 = −π‘Ž2 sin(π‘₯ − π‘Žπ‘‘)
𝑒𝑑𝑑 = π‘Ž2 𝑒π‘₯π‘₯ βž” −π‘Ž2 sin(π‘₯ − π‘Žπ‘‘) = π‘Ž2 (− sin(π‘₯ − π‘Žπ‘‘))
Then 𝒖 satisfies Wave equation
Page | 43
Choice B
𝒅𝒛
55] If 𝒛 = π’™πŸ π’š + πŸ‘π’™π’šπŸ’ , 𝒙 = 𝐬𝐒𝐧 πŸπ’• , π’š = 𝐜𝐨𝐬 𝒕 , find
A- πŸ”
B- −πŸ”
C- 𝟏𝟐
D- 𝟎
𝒅𝒕
when 𝒕 = 𝟎
Solution:
πœ•π‘§
𝑑π‘₯
= 2π‘₯𝑦 + 3𝑦 4 ,
πœ•π‘₯
πœ•π‘§
𝑑𝑦
= π‘₯ 2 + 12π‘₯𝑦 3 ,
πœ•π‘¦
βž”
𝑑𝑧
=
𝑑𝑑
πœ•π‘§
πœ•π‘₯
∗
𝑑π‘₯
𝑑𝑑
= 2 cos 2𝑑
𝑑𝑑
+
𝑑𝑑
πœ•π‘§
πœ•π‘¦
∗
= − sin 𝑑
𝑑𝑦
𝑑𝑑
= (2π‘₯𝑦 + 3𝑦 4 ) ∗ (2 cos 2𝑑) + (π‘₯ 2 + 12π‘₯𝑦 3 ) ∗ (− sin 𝑑)
At 𝒕 = 𝟎 βž” 2 ∗ (2π‘₯𝑦 + 3𝑦 4 ) + 0 = 4π‘₯𝑦 + 6𝑦 4
π‘₯ = sin 2𝑑 , 𝑦 = cos 𝑑 , then: 𝒙 = 𝟎 , π’š = 𝟏
Then: 4π‘₯𝑦 + 6𝑦 4 = 4 ∗ 0 ∗ 1 + 6 ∗ 14 = 6
Choice A
56] If 𝒛 = 𝒆𝒙 𝐬𝐒𝐧 π’š , 𝒙 = π’”π’•πŸ , π’š = π’”πŸ 𝒕 , find
𝝏𝒛
𝝏𝒔
,
𝝏𝒛
𝝏𝒕
respectively
A- 𝒕𝒆𝒙 (𝒕 𝐬𝐒𝐧 π’š + πŸπ’” 𝐜𝐨𝐬 π’š) , 𝒔𝒆𝒙 (πŸπ’• 𝐬𝐒𝐧 π’š + 𝒔 𝐜𝐨𝐬 π’š)
B- 𝒔𝒆𝒙 (πŸπ’•π’†π’™ 𝐬𝐒𝐧 π’š + 𝒔 𝐜𝐨𝐬 π’š) , 𝒕𝒆𝒙 (𝒕 𝐬𝐒𝐧 π’š + πŸπ’” 𝐜𝐨𝐬 π’š)
C- 𝒕𝒆𝒙 (𝒕 𝐬𝐒𝐧 π’š + πŸπ’” 𝐜𝐨𝐬 π’š)
, 𝒆𝒙 (πŸπ’•π’†π’™ 𝐬𝐒𝐧 π’š + 𝒔 𝐜𝐨𝐬 π’š)
D- None of them
Solution:
πœ•π‘§
πœ•π‘₯
πœ•π‘§
πœ•π‘ 
= 𝑒 π‘₯ sin 𝑦 ,
=
πœ•π‘§
πœ•π‘₯
∗
πœ•π‘₯
πœ•π‘ 
+
πœ•π‘₯
= 𝑑2 ,
πœ•π‘ 
πœ•π‘§
πœ•π‘¦
∗
πœ•π‘¦
πœ•π‘ 
πœ•π‘₯
πœ•π‘‘
= 2𝑠𝑑 ,
πœ•π‘§
πœ•π‘¦
= 𝑒 π‘₯ cos 𝑦 ,
πœ•π‘¦
πœ•π‘ 
= 2𝑠𝑑 ,
πœ•π‘¦
πœ•π‘‘
= 𝑠2
= (𝑒 π‘₯ sin 𝑦 ) ∗ (𝑑 2 ) + (𝑒 π‘₯ cos 𝑦) ∗ (2𝑠𝑑)
= 𝑑 2 𝑒 π‘₯ sin 𝑦 + 2𝑠𝑑𝑒 π‘₯ cos 𝑦 = 𝒕𝒆𝒙 (𝒕 𝐬𝐒𝐧 π’š + πŸπ’” 𝐜𝐨𝐬 π’š)
Page | 44
πœ•π‘§
=
πœ•π‘‘
πœ•π‘§
πœ•π‘₯
∗
πœ•π‘₯
πœ•π‘‘
+
πœ•π‘§
∗
πœ•π‘¦
πœ•π‘¦
πœ•π‘‘
= (𝑒 π‘₯ sin 𝑦 ) ∗ (2𝑠𝑑) + (𝑒 π‘₯ cos 𝑦) ∗ (𝑠 2 )
= 2𝑠𝑑𝑒 π‘₯ sin 𝑦 + 𝑠 2 𝑒 π‘₯ cos 𝑦 = 𝒔𝒆𝒙 (πŸπ’• 𝐬𝐒𝐧 π’š + 𝒔 𝐜𝐨𝐬 π’š)
Choice A
57] If 𝒖 = π’™πŸ’ π’š + π’šπŸ π’›πŸ‘ , 𝒛 = π’”π’“πŸ 𝐬𝐒𝐧 𝒕 , 𝒙 = 𝒓𝒔𝒆𝒕 , π’š = π’“π’”πŸ 𝒆−𝒕
find
𝝏𝒖
,
𝝏𝒓
𝝏𝒖
𝝏𝒔
,
𝝏𝒖
𝝏𝒕
, when 𝒓 = 𝟐 , 𝒔 = 𝟏 , 𝒕 = 𝟎 respectively
A- πŸ–πŸŽ , πŸπŸ—πŸŽ , πŸ—πŸ”
B- πŸ–πŸŽ , πŸπŸ—πŸ , πŸ—
C- πŸ–πŸŽ , πŸπŸ—πŸ , πŸ—πŸ”
D- None of them
Solution:
πœ•π‘’
πœ•π‘§
= 3𝑦 2 𝑧 2 ,
πœ•π‘§
πœ•π‘Ÿ
= 2π‘ π‘Ÿ sin 𝑑 ,
πœ•π‘’
πœ•π‘₯
= 4π‘₯ 3 𝑦 ,
πœ•π‘₯
πœ•π‘Ÿ
= 𝑠𝑒 𝑑 ,
πœ•π‘’
πœ•π‘¦
= π‘₯ 4 + 2𝑦𝑧 3 ,
𝑠 2 𝑒 −𝑑
πœ•π‘’
πœ•π‘Ÿ
=
πœ•π‘’
πœ•π‘§
∗
πœ•π‘§
πœ•π‘Ÿ
+
πœ•π‘’
πœ•π‘₯
∗
πœ•π‘₯
πœ•π‘Ÿ
+
πœ•π‘’
πœ•π‘¦
∗
πœ•π‘¦
πœ•π‘Ÿ
= (3𝑦 2 𝑧 2 ) ∗ (2π‘ π‘Ÿ sin 𝑑) + (4π‘₯ 3 𝑦 ) ∗ (𝑠𝑒 𝑑 ) + (π‘₯ 4 + 2𝑦𝑧 3 ) ∗ (𝑠 2 𝑒 −𝑑 )
At π‘Ÿ = 2 , 𝑠 = 1 , 𝑑 = 0
βž” (3𝑦 2 𝑧 2 ) ∗ (2 ∗ 1 ∗ 2 ∗ sin 0) + (4π‘₯ 3 𝑦 ) ∗ (1 ∗ 𝑒 0 ) + (π‘₯ 4 + 2𝑦𝑧 3 ) ∗
(12 𝑒 −0 )
= 0 + (4π‘₯ 3 𝑦 ) ∗ (1 ∗ 1) + (π‘₯ 4 + 2𝑦𝑧 3 ) ∗ (1 ∗ 1)
= (4π‘₯ 3 𝑦 ) + (π‘₯ 4 + 2𝑦𝑧 3 )
Page | 45
πœ•π‘¦
πœ•π‘Ÿ
=
βž” 𝑧 = π‘ π‘Ÿ 2 sin 𝑑 , At π‘Ÿ = 2 , 𝑠 = 1 , 𝑑 = 0
Then: 𝑧 = 1 ∗ 22 ∗ sin 0 = 0
βž” π‘₯ = π‘Ÿπ‘ π‘’ 𝑑 , At π‘Ÿ = 2 , 𝑠 = 1 , 𝑑 = 0
Then: π‘₯ = 2 ∗ 1 ∗ 𝑒 0 = 2
βž” 𝑦 = π‘Ÿπ‘  2 𝑒 −𝑑 , At π‘Ÿ = 2 , 𝑠 = 1 , 𝑑 = 0
Then: 𝑦 = 2 ∗ 1 ∗ 1 = 2
By Substitution in the equation :
(4π‘₯ 3 𝑦 ) + (π‘₯ 4 + 2𝑦𝑧 3 ) = (4 ∗ 23 ∗ 2) + (24 + 2 ∗ 2 ∗ 03 ) = 64 + 16 = 80
𝑒 = π‘₯ 4 𝑦 + 𝑦 2 𝑧 3 , 𝑧 = π‘ π‘Ÿ 2 sin 𝑑 , π‘₯ = π‘Ÿπ‘ π‘’ 𝑑 , 𝑦 = π‘Ÿπ‘  2 𝑒 −𝑑
πœ•π‘’
βž” πœ•π‘§ = 3𝑦 2 𝑧 2 ,
πœ•π‘§
πœ•π‘ 
= π‘Ÿ 2 sin 𝑑 ,
πœ•π‘’
πœ•π‘₯
= 4π‘₯ 3 𝑦 ,
πœ•π‘₯
πœ•π‘ 
= π‘Ÿπ‘’ 𝑑 ,
πœ•π‘’
πœ•π‘¦
= π‘₯ 4 + 2𝑦𝑧 3 ,
πœ•π‘¦
πœ•π‘ 
=
2π‘Ÿπ‘ π‘’ −𝑑
πœ•π‘’
πœ•π‘ 
=
πœ•π‘’
πœ•π‘§
∗
πœ•π‘§
πœ•π‘ 
+
πœ•π‘’
πœ•π‘₯
∗
πœ•π‘₯
πœ•π‘ 
+
πœ•π‘’
πœ•π‘¦
∗
πœ•π‘¦
πœ•π‘ 
= (3𝑦 2 𝑧 2 ) ∗ (π‘Ÿ 2 sin 𝑑 ) + (4π‘₯ 3 𝑦 ) ∗ (π‘Ÿπ‘’ 𝑑 ) + (π‘₯ 4 + 2𝑦𝑧 3 ) ∗ (2π‘Ÿπ‘ π‘’ −𝑑 )
At π‘Ÿ = 2 , 𝑠 = 1 , 𝑑 = 0
βž” (3𝑦 2 𝑧 2 ) ∗ (22 sin 0 ) + (4π‘₯ 3 𝑦 ) ∗ (2 ∗ 𝑒 0 ) + (π‘₯ 4 + 2𝑦𝑧 3 ) ∗ (2 ∗ 2 ∗ 1 ∗
𝑒 −0 )
= 0 + (4π‘₯ 3 𝑦 ) ∗ (2) + (π‘₯ 4 + 2𝑦𝑧 3 ) ∗ (4)
= 8π‘₯ 3 𝑦 + 4π‘₯ 4 + 8𝑦𝑧 3
At π‘Ÿ = 2 , 𝑠 = 1 , 𝑑 = 0
βž”π‘§=0 , π‘₯ =2 , 𝑦 =2
Then: 8 ∗ 23 ∗ 2 + 4 ∗ 24 + 8 ∗ 2 ∗ 03 = 128 + 64 + 0 = 192
Page | 46
𝑒 = π‘₯ 4 𝑦 + 𝑦 2 𝑧 3 , 𝑧 = π‘ π‘Ÿ 2 sin 𝑑 , π‘₯ = π‘Ÿπ‘ π‘’ 𝑑 , 𝑦 = π‘Ÿπ‘  2 𝑒 −𝑑
πœ•π‘’
πœ•π‘§
βž” πœ•π‘§ = 3𝑦 2 𝑧 2 ,
= π‘ π‘Ÿ 2 cos 𝑑 ,
πœ•π‘‘
πœ•π‘’
πœ•π‘₯
= 4π‘₯ 3 𝑦 ,
πœ•π‘₯
πœ•π‘‘
= π‘Ÿπ‘ π‘’ 𝑑 ,
πœ•π‘’
πœ•π‘¦
= π‘₯ 4 + 2𝑦𝑧 3 ,
πœ•π‘¦
πœ•π‘‘
=
−π‘Ÿπ‘  2 𝑒 −𝑑
πœ•π‘’
πœ•π‘‘
=
πœ•π‘’
πœ•π‘§
∗
πœ•π‘§
πœ•π‘‘
+
πœ•π‘’
πœ•π‘₯
∗
πœ•π‘₯
πœ•π‘‘
+
πœ•π‘’
πœ•π‘¦
∗
πœ•π‘¦
πœ•π‘‘
= (3𝑦 2 𝑧 2 ) ∗ (π‘ π‘Ÿ 2 cos 𝑑) + (4π‘₯ 3 𝑦) ∗ (π‘Ÿπ‘ π‘’ 𝑑 ) + (π‘₯ 4 + 2𝑦𝑧 3 ) ∗ (−π‘Ÿπ‘  2 𝑒 −𝑑 )
At π‘Ÿ = 2 , 𝑠 = 1 , 𝑑 = 0
(3𝑦 2 𝑧 2 ) ∗ (1 ∗ 22 ∗ π‘π‘œπ‘  0) + (4π‘₯ 3 𝑦) ∗ (2 ∗ 1 ∗ 𝑒 0 ) + (π‘₯ 4 + 2𝑦𝑧 3 ) ∗
(−2 ∗ 12 ∗ 𝑒 −0 )
= 12𝑦 2 𝑧 2 + 8π‘₯ 3 𝑦 − 2π‘₯ 4 − 4𝑦𝑧 3
At π‘Ÿ = 2 , 𝑠 = 1 , 𝑑 = 0
βž”π‘§=0 , π‘₯ =2 , 𝑦 =2
12 ∗ 22 ∗ 02 + 8 ∗ 23 ∗ 2 − 2 ∗ 24 − 4 ∗ 2 ∗ 03 = 0 + 128 − 32 + 0 = 96
Choice C
𝝏𝒛
𝝏𝒛
58] Use Implicit Derivative to find 𝝏𝒙 and ππ’š respectively
1] π’šπ’› + 𝒙 𝒍𝒏 π’š = π’›πŸ
𝒍𝒏 π’š
π’›π’š+𝒙
𝒍𝒏 π’š
πŸ–π’›π’š+𝒙
π’›π’š+𝒙
A- πŸπ’›−π’š , πŸπ’›π’š−π’šπŸ
𝒍𝒏 π’š
B- πŸπ’›π’š−π’šπŸ , πŸπ’›−π’š
C- πŸπ’›+πŸ—π’š , πŸπ’›π’š−π’šπŸ
D- None of them
Solution:
βž”π’š∗
𝝏𝒛
𝝏𝒙
+ 𝒍𝒏 π’š = πŸπ’› ∗
βž” 𝒍𝒏 π’š = πŸπ’› ∗
βž”
𝝏𝒛
𝝏𝒙
=
Page | 47
𝒍𝒏 π’š
πŸπ’›−π’š
𝝏𝒛
𝝏𝒙
−π’š∗
𝝏𝒛
𝝏𝒙
𝝏𝒛
𝝏𝒙
→ 𝒍𝒏 π’š =
𝝏𝒛
𝝏𝒙
(πŸπ’› − π’š)
𝝏𝒛
βž”π’›+π’š∗
ππ’š
𝒙
𝝏𝒛
π’š
ππ’š
+ = πŸπ’› ∗
𝒙
𝝏𝒛
π’š
ππ’š
βž” 𝒛 + = πŸπ’› ∗
−π’š∗
𝝏𝒛
𝒙
𝝏𝒛
π’š
ππ’š
→𝒛+ =
ππ’š
(πŸπ’› − π’š)
𝒙
βž”
𝝏𝒛
ππ’š
=
𝒛+π’š
πŸπ’›−π’š
π’›π’š+𝒙
=
πŸπ’›π’š−π’šπŸ
Choice A
2] π’™πŸ − π’šπŸ + π’›πŸ − πŸπ’› = πŸ’
π’š
−𝒙
−𝒙
π’š
𝒙
A- 𝒛−𝟏 , 𝒛−𝟏
π’š
B- 𝒛−𝟏 , 𝒛−𝟏
C- 𝒛−𝟏 , 𝒛−𝟏
D- None of them
Solution:
βž” 2π‘₯ + 2𝑧 ∗
βž” 2𝑧 ∗
βž”
πœ•π‘§
πœ•π‘₯
=
πœ•π‘§
πœ•π‘₯
πœ•π‘§
πœ•π‘₯
−2∗
−2π‘₯
2𝑧−2
=
βž” −2𝑦 + 2𝑧 ∗
βž” 2𝑧 ∗
βž”
πœ•π‘§
πœ•π‘¦
=
πœ•π‘§
πœ•π‘¦
2𝑧−2
Page | 48
=
πœ•π‘§
πœ•π‘₯
πœ•π‘§
πœ•π‘₯
=0
= −2π‘₯ →
πœ•π‘§
πœ•π‘₯
(2𝑧 − 2) = −2π‘₯
−π‘₯
𝑧−1
πœ•π‘§
πœ•π‘¦
−2∗
2𝑦
Choice C
−2∗
−2∗
πœ•π‘§
πœ•π‘¦
𝑦
𝑧−1
πœ•π‘§
πœ•π‘¦
=0
= 2𝑦 →
πœ•π‘§
πœ•π‘¦
(2𝑧 − 2) = 2𝑦
59] Find π’š′ of π’™πŸ‘ + π’šπŸ‘ = πŸ”π’™π’š
A-
πŸ‘π’™πŸ −πŸ”π’š
B- −
πŸ‘π’šπŸ −πŸ”π’™
C- −
πŸ‘π’™πŸ +πŸ”π’š
πŸ‘π’™πŸ −πŸ”π’š
πŸ‘π’šπŸ −πŸ”π’™
D- None of them
πŸ‘π’šπŸ −πŸ”π’™
Solution:
π‘₯ 3 + 𝑦 3 − 6π‘₯𝑦 = 0 βž” 𝑓π‘₯ = 3π‘₯ 2 − 6𝑦 , 𝑓𝑦 = 3𝑦 2 − 6π‘₯
𝑦′ = −
𝑓π‘₯
𝑓𝑦
=−
3π‘₯ 2 −6𝑦
3𝑦 2 −6π‘₯
Choice B
60] Find Second Partial Derivative to :
I] 𝒇(𝒙, π’š) = π’™πŸ‘ π’šπŸ“ + πŸπ’™πŸ’ π’š
Solution:
𝑓π‘₯ = 3π‘₯ 2 𝑦 5 + 8π‘₯ 3 𝑦 βž” 𝑓π‘₯π‘₯ = 6π‘₯𝑦 5 + 24π‘₯ 2 𝑦
𝑓𝑦 = 5π‘₯ 3 𝑦 4 + 2π‘₯ 4 βž” 𝑓𝑦𝑦 = 20π‘₯ 3 𝑦 3
𝑓π‘₯𝑦 = 15π‘₯ 2 𝑦 4 + 8π‘₯ 3 , 𝑓𝑦π‘₯ = 15π‘₯ 2 𝑦 4 + 8π‘₯ 3
Since 𝑓π‘₯𝑦 = 𝑓𝑦π‘₯ , Then The Function Is Continuous
II] 𝒇(𝒙, π’š) = 𝐬𝐒𝐧𝟐 (π’Žπ’™ + π’π’š)
Solution:
𝑓π‘₯ = 2 sin(π‘šπ‘₯ + 𝑛𝑦) cos(π‘šπ‘₯ + 𝑛𝑦) ∗ π‘š = π‘š sin 2(π‘šπ‘₯ + 𝑛𝑦)
𝑓π‘₯π‘₯ = π‘š ∗ cos 2(π‘šπ‘₯ + 𝑛𝑦) ∗ 2 ∗ π‘š = 2π‘š2 cos 2(π‘šπ‘₯ + 𝑛𝑦)
𝑓𝑦 = 2 sin(π‘šπ‘₯ + 𝑛𝑦) cos(π‘šπ‘₯ + 𝑛𝑦) ∗ 𝑛 = 𝑛 sin 2(π‘šπ‘₯ + 𝑛𝑦)
𝑓𝑦𝑦 = 𝑛 ∗ cos 2(π‘šπ‘₯ + 𝑛𝑦) ∗ 2 ∗ 𝑛 = 2𝑛2 cos 2(π‘šπ‘₯ + 𝑛𝑦)
𝑓π‘₯𝑦 = 2π‘šπ‘› cos 2(π‘šπ‘₯ + 𝑛𝑦) = 𝑓𝑦π‘₯ , then the function is continuous
Page | 49
61] Use the chain rule to find
𝒅𝒛
𝒅𝒕
π’…π’˜
or
𝒅𝒕
I] 𝒛 = π’™πŸ + π’šπŸ + π’™π’š , 𝒙 = 𝐬𝐒𝐧 𝒕 , π’š = 𝒆𝒕
Solution:
βž”
πœ•π‘§
πœ•π‘₯
𝑑π‘₯
𝑑𝑑
βž”
𝑑𝑧
=
𝑑𝑑
πœ•π‘§
πœ•π‘₯
∗
𝑑π‘₯
𝑑𝑑
= 2π‘₯ + 𝑦 ,
= π‘π‘œπ‘  𝑑 ,
πœ•π‘§
πœ•π‘₯
∗
𝑑π‘₯
𝑑𝑑
+
+
πœ•π‘§
πœ•π‘¦
𝑑𝑦
𝑑𝑑
πœ•π‘§
πœ•π‘¦
πœ•π‘§
πœ•π‘¦
∗
𝑑𝑦
𝑑𝑑
= 2𝑦 + π‘₯
= 𝑒𝑑
∗
𝑑𝑦
= (2π‘₯ + 𝑦 ) ∗ (π‘π‘œπ‘  𝑑) + (2𝑦 + π‘₯ ) ∗ (𝑒 𝑑 )
𝑑𝑑
= 2π‘₯ π‘π‘œπ‘  𝑑 + 𝑦 π‘π‘œπ‘  𝑑 + 2𝑦𝑒 𝑑 + π‘₯𝑒 𝑑
= 2 ∗ sin 𝑑 π‘π‘œπ‘  𝑑 + 𝑒 𝑑 π‘π‘œπ‘  𝑑 + 2 ∗ 𝑒 𝑑 ∗ 𝑒 𝑑 + sin 𝑑 ∗ 𝑒 𝑑
= 2 sin 𝑑 π‘π‘œπ‘  𝑑 + 𝑒 𝑑 π‘π‘œπ‘  𝑑 + 2𝑒 2𝑑 + 𝑒 𝑑 sin 𝑑
II] 𝒛 = 𝐜𝐨𝐬(𝒙 + πŸ’π’š) , 𝒙 = πŸ“π’•πŸ’ , π’š =
𝟏
𝒕
Solution:
βž”
πœ•π‘§
πœ•π‘₯
𝑑π‘₯
𝑑𝑑
βž”
𝑑𝑧
=
𝑑𝑑
πœ•π‘§
πœ•π‘₯
∗
𝑑π‘₯
+
𝑑𝑑
πœ•π‘§
πœ•π‘¦
∗
𝑑𝑦
𝑑𝑑
= − 𝑠𝑖𝑛(π‘₯ + 4𝑦) ,
= 20𝑑 3 ,
πœ•π‘§
πœ•π‘₯
∗
𝑑π‘₯
𝑑𝑑
+
𝑑𝑦
𝑑𝑑
πœ•π‘§
πœ•π‘¦
=−
∗
𝑑𝑦
𝑑𝑑
πœ•π‘§
πœ•π‘¦
= −4 𝑠𝑖𝑛(π‘₯ + 4𝑦)
1
𝑑2
1
= (− 𝑠𝑖𝑛(π‘₯ + 4𝑦)) ∗ (20𝑑 3 ) + (−4 𝑠𝑖𝑛(π‘₯ + 4𝑦)) ∗ (− 2 )
𝑑
= −20𝑑 3 𝑠𝑖𝑛(π‘₯ + 4𝑦) +
3
4
4 𝑠𝑖𝑛(π‘₯+4𝑦)
𝑑2
1
= −20𝑑 𝑠𝑖𝑛 (5𝑑 + 4 ∗ ) +
𝑑
Page | 50
1
4 𝑠𝑖𝑛(5𝑑 4 +4∗ 𝑑 )
𝑑2
III] π’˜ = 𝒍𝒏 √π’™πŸ + π’šπŸ + π’›πŸ , 𝒙 = π’”π’Šπ’ 𝒕 , π’š = 𝒄𝒐𝒔 𝒕 , 𝒛 = 𝒕𝒂𝒏 𝒕
Solution:
𝑑𝑀
βž”
𝑑𝑑
=
πœ•π‘€
πœ•π‘₯
∗
𝑑π‘₯
+
𝑑𝑑
πœ•π‘€
πœ•π‘¦
∗
𝑑𝑦
𝑑𝑑
+
πœ•π‘€
πœ•π‘§
𝑑𝑧
∗
𝑑𝑑
2π‘₯
πœ•π‘€
=
πœ•π‘₯
2√π‘₯2 +𝑦2 +𝑧2
√π‘₯ 2 +𝑦 2 +𝑧 2
=
π‘₯
π‘₯ 2 +𝑦2 +𝑧 2
,
𝑑π‘₯
𝑑𝑑
= π‘π‘œπ‘  𝑑
2𝑦
πœ•π‘€
=
πœ•π‘¦
2√π‘₯2 +𝑦2 +𝑧2
√π‘₯ 2 +𝑦 2 +𝑧 2
=
𝑦
π‘₯ 2 +𝑦2 +𝑧 2
,
𝑑𝑦
𝑑𝑑
= − 𝑠𝑖𝑛 𝑑
2𝑧
πœ•π‘€
=
πœ•π‘§
βž”
πœ•π‘€
πœ•π‘₯
=(
√π‘₯ 2 +𝑦 2 +𝑧 2
∗
𝑑π‘₯
𝑑𝑑
+
π‘₯
πœ•π‘¦
∗
𝑧
π‘₯ 2 +𝑦2 +𝑧 2
𝑑𝑦
𝑑𝑑
+
πœ•π‘€
πœ•π‘§
∗
,
𝑑𝑧
= 𝑠𝑒𝑐 2 𝑑
𝑑𝑑
𝑑𝑧
𝑑𝑑
𝑑)2 +(π‘π‘œπ‘  𝑑)2 +(π‘‘π‘Žπ‘› 𝑑)2
1+(π‘‘π‘Žπ‘› 𝑑)2
𝑧
) ∗ (π‘π‘œπ‘  𝑑) + (π‘₯ 2 +𝑦2 +𝑧 2 ) ∗ (− 𝑠𝑖𝑛 𝑑) + (π‘₯ 2 +𝑦2 +𝑧 2 ) ∗ (𝑠𝑒𝑐 2 𝑑)
𝑠𝑖𝑛 𝑑∗π‘π‘œπ‘  𝑑
π‘‘π‘Žπ‘› 𝑑∗𝑠𝑒𝑐 2 𝑑
Page | 51
πœ•π‘€
=
𝑦
π‘₯ 2 +𝑦 2 +𝑧 2
= (𝑠𝑖𝑛
=
2√π‘₯2 +𝑦2 +𝑧2
=
− (𝑠𝑖𝑛
π‘‘π‘Žπ‘› 𝑑∗𝑠𝑒𝑐 2 𝑑
𝑠𝑒𝑐 2 𝑑
π‘π‘œπ‘  𝑑∗𝑠𝑖𝑛 𝑑
𝑑)2 +(π‘π‘œπ‘  𝑑)2 +(π‘‘π‘Žπ‘› 𝑑)2
= π‘‘π‘Žπ‘› 𝑑
+ (𝑠𝑖𝑛
π‘‘π‘Žπ‘› 𝑑∗𝑠𝑒𝑐 2 𝑑
𝑑)2 +(π‘π‘œπ‘  𝑑)2 +(π‘‘π‘Žπ‘› 𝑑)2
62] Use the chain rule to find
𝝏𝒛
𝝏𝒔
or
𝝏𝒛
𝝏𝒕
I] 𝒛 = π’™πŸ π’šπŸ‘ , 𝒙 = 𝒔 𝒄𝒐𝒔 𝒕 , π’š = 𝒔 π’”π’Šπ’ 𝒕
Solution:
βž”
πœ•π‘§
πœ•π‘₯
βž”
πœ•π‘§
πœ•π‘ 
=
πœ•π‘§
πœ•π‘₯
πœ•π‘₯
∗
πœ•π‘ 
= 2π‘₯𝑦 3 ,
πœ•π‘§
πœ•π‘ 
+
πœ•π‘₯
πœ•π‘ 
πœ•π‘§
πœ•π‘¦
∗
πœ•π‘¦
πœ•π‘ 
= π‘π‘œπ‘  𝑑 ,
πœ•π‘§
πœ•π‘¦
= 3π‘₯ 2 𝑦 2 ,
πœ•π‘¦
πœ•π‘ 
= 𝑠𝑖𝑛 𝑑
= (2π‘₯𝑦 3 ) ∗ (π‘π‘œπ‘  𝑑) + (3π‘₯ 2 𝑦 2 ) ∗ (𝑠𝑖𝑛 𝑑)
= (2 ∗ 𝑠 π‘π‘œπ‘  𝑑 ∗ (𝑠 𝑠𝑖𝑛 𝑑)3 ) ∗ (π‘π‘œπ‘  𝑑) + (3 ∗ (𝑠 π‘π‘œπ‘  𝑑)2 ∗ (𝑠 𝑠𝑖𝑛 𝑑)2 ) ∗ (𝑠𝑖𝑛 𝑑)
= 2𝑠 4 π‘π‘œπ‘  2 𝑑 𝑠𝑖𝑛3 𝑑 + 3𝑠 4 π‘π‘œπ‘  2 𝑑 𝑠𝑖𝑛3 𝑑
= 5𝑠 4 𝑠𝑖𝑛3 𝑑 π‘π‘œπ‘  2 𝑑
βž”
πœ•π‘§
πœ•π‘‘
πœ•π‘§
πœ•π‘₯
βž”
=
πœ•π‘§
πœ•π‘₯
∗
πœ•π‘₯
πœ•π‘‘
= 2π‘₯𝑦 3 ,
πœ•π‘§
πœ•π‘‘
+
πœ•π‘₯
πœ•π‘‘
πœ•π‘§
πœ•π‘¦
∗
πœ•π‘¦
πœ•π‘‘
= −𝑠 𝑠𝑖𝑛 𝑑 ,
πœ•π‘§
πœ•π‘¦
= 3π‘₯ 2 𝑦 2 ,
πœ•π‘¦
πœ•π‘‘
= 𝑠 π‘π‘œπ‘  𝑑
= (2π‘₯𝑦 3 ) ∗ (−𝑠 𝑠𝑖𝑛 𝑑) + (3π‘₯ 2 𝑦 2 ) ∗ (𝑠 π‘π‘œπ‘  𝑑)
= (2 ∗ 𝑠 π‘π‘œπ‘  𝑑 ∗ (𝑠 𝑠𝑖𝑛 𝑑)3 ) ∗ (−𝑠 𝑠𝑖𝑛 𝑑) + (3(𝑠 π‘π‘œπ‘  𝑑)2 (𝑠 𝑠𝑖𝑛 𝑑)2 ) ∗ (𝑠 π‘π‘œπ‘  𝑑)
= −2𝑠 5 π‘π‘œπ‘  𝑑 𝑠𝑖𝑛4 𝑑 + 3𝑠 5 π‘π‘œπ‘  3 𝑑 𝑠𝑖𝑛2 𝑑
II] 𝒛 = π’”π’Šπ’ 𝜽 𝒄𝒐𝒔 ∅ , 𝜽 = π’”π’•πŸ , ∅ = π’”πŸ 𝒕
Solution:
βž”
∂z
∂θ
∂z
∂s
=
∂z
∂θ
∗
∂θ
∂s
+
∂z
∂∅
= cos θ cos ∅ ,
Page | 52
∗
∂θ
∂s
∂∅
∂s
= t2 ,
∂z
∂∅
= − sin θ sin ∅ ,
∂∅
∂s
= 2st
∂z
βž”
= (cos θ cos ∅ ) ∗ (t 2 ) + (− sin θ sin ∅) ∗ (2st)
∂s
= (cos 𝑠𝑑 2 cos 𝑠 2 𝑑 ) ∗ (t 2 ) + (− sin 𝑠𝑑 2 sin 𝑠 2 𝑑) ∗ (2st)
= π’•πŸ 𝒄𝒐𝒔 π’”π’•πŸ 𝒄𝒐𝒔 π’”πŸ 𝒕 − πŸπ’”π’• π’”π’Šπ’ π’”π’•πŸ π’”π’Šπ’ π’”πŸ 𝒕
∂z
βž”
∂z
∂θ
=
∂t
∂z
∂θ
∗
∂θ
∂t
+
∂z
∂∅
∂θ
= cos θ cos ∅ ,
βž”
∂z
∂∅
∗
∂t
∂t
= 2st ,
∂z
∂∅
∂∅
= − sin θ sin ∅ ,
∂t
= s2
= (cos θ cos ∅ ) ∗ (2st) + (− sin θ sin ∅) ∗ (s2 )
∂t
= (π‘π‘œπ‘  𝑠𝑑 2 π‘π‘œπ‘  𝑠 2 𝑑 ) ∗ (2𝑠𝑑) + (− 𝑠𝑖𝑛 𝑠𝑑 2 𝑠𝑖𝑛 𝑠 2 𝑑) ∗ (𝑠 2 )
= πŸπ’”π’• 𝒄𝒐𝒔 π’”π’•πŸ 𝒄𝒐𝒔 π’”πŸ 𝒕 − π’”πŸ π’”π’Šπ’ π’”π’•πŸ π’”π’Šπ’ π’”πŸ 𝒕
III] 𝝋 = π’†πœΆ+𝟐𝜷 , 𝜢 =
𝒔
𝒕
𝒕
, 𝜷=𝒔
Solution:
βž”
πœ•πœ‘
πœ•π›Ό
πœ•πœ‘
πœ•π‘ 
=
πœ•πœ‘
πœ•π›Ό
∗
πœ•π›Ό
πœ•π‘ 
= 𝑒 𝛼+2𝛽 ,
+
πœ•π›Ό
πœ•π‘ 
πœ•πœ‘
πœ•π›½
=
∗
1
πœ•π›½
πœ•π‘ 
πœ•πœ‘
,
𝑑
πœ•π›½
= 2𝑒 𝛼+2𝛽 ,
πœ•π›½
=−
πœ•π‘ 
𝑑
𝑠2
𝑠
βž”
πœ•πœ‘
βž”
πœ•πœ‘
πœ•πœ‘
= 𝑒 𝛼+2𝛽 ,
πœ•π›Ό
βž”
πœ•π‘ 
πœ•π‘‘
πœ•πœ‘
πœ•π‘‘
Page | 53
1
𝑑
= (𝑒 𝛼+2𝛽 ) ∗ ( ) + (2𝑒 𝛼+2𝛽 ) ∗ (− 2 ) =
𝑑
𝑠
=
πœ•πœ‘
πœ•π›Ό
∗
πœ•π›Ό
πœ•π‘‘
+
πœ•π›Ό
πœ•π‘‘
πœ•πœ‘
πœ•π›½
∗
=−
𝑒𝑑
𝑑
+2
𝑠
𝑑
−
𝑠 𝑑
+2
𝑠
2𝑑𝑒 𝑑
𝑠2
πœ•π›½
πœ•π‘‘
𝑠
𝑑2
𝑠
,
πœ•πœ‘
πœ•π›½
= 2𝑒 𝛼+2𝛽 ,
πœ•π›½
πœ•π‘‘
1
=
1
𝑠
= (𝑒 𝛼+2𝛽 ) ∗ (− 2 ) + (2𝑒 𝛼+2𝛽 ) ∗ ( ) = −
𝑑
𝑠
𝑠 𝑑
+2
𝑠
𝑠𝑒 𝑑
𝑑2
+
𝑠 𝑑
+2
𝑠
2𝑒 𝑑
𝑠
63] Find
π’…π’š
𝒅𝒙
Using Partial derivatives
I] π’š 𝒄𝒐𝒔 𝒙 = π’™πŸ + π’šπŸ
Solution:
βž”
𝑑𝑦
=−
𝑑π‘₯
𝐹π‘₯ =
πœ•πΉ
πœ•π‘₯
πœ•πΉ
𝐹𝑦 =
𝑑𝑦
𝑑π‘₯
πœ•π‘¦
=−
𝐹π‘₯
𝐹𝑦
= −𝑦 𝑠𝑖𝑛 π‘₯ = 2π‘₯ βž” −𝑦 𝑠𝑖𝑛 π‘₯ − 2π‘₯ = 0
= π‘π‘œπ‘  π‘₯ = 2𝑦 βž” π‘π‘œπ‘  π‘₯ − 2𝑦 = 0
(−𝑦 𝑠𝑖𝑛 π‘₯−2π‘₯)
(π‘π‘œπ‘  π‘₯−2𝑦)
=−
−(𝑦 𝑠𝑖𝑛 π‘₯+2π‘₯)
(π‘π‘œπ‘  π‘₯−2𝑦)
=
𝑦 𝑠𝑖𝑛 π‘₯+2π‘₯
π‘π‘œπ‘  π‘₯−2𝑦
II] 𝒕𝒂𝒏−𝟏 (π’™πŸ π’š) = 𝒙 + π’™π’šπŸ
Solution:
βž”
𝑑𝑦
=−
𝑑π‘₯
𝐹π‘₯ =
πœ•πΉ
𝐹𝑦 =
𝑑𝑦
𝑑π‘₯
πœ•π‘₯
πœ•πΉ
πœ•π‘¦
=
=
𝐹π‘₯
𝐹𝑦
1
1+(π‘₯ 2 𝑦)
2
2 ∗ 2π‘₯𝑦 = 1 + 𝑦 βž”
1
1+(π‘₯ 2 𝑦)
2
2 ∗ π‘₯ = 2π‘₯𝑦 βž”
2π‘₯𝑦
2
2 −𝑦 −1)
2
1+(π‘₯ 𝑦)
(
=−
π‘₯2
2 −2π‘₯𝑦)
1+(π‘₯2 𝑦)
(
III] π’†π’š π’”π’Šπ’ 𝒙 = 𝒙 + π’™π’š
Solution:
βž”
𝑑𝑦
𝑑π‘₯
Page | 54
=−
𝐹π‘₯
𝐹𝑦
2π‘₯𝑦
1+(π‘₯ 2 𝑦)2
π‘₯2
1+(π‘₯ 2 𝑦)2
− 𝑦2 − 1 = 0
− 2π‘₯𝑦 = 0
𝐹π‘₯ =
𝐹𝑦 =
𝑑𝑦
𝑑π‘₯
πœ•πΉ
πœ•π‘₯
πœ•πΉ
πœ•π‘¦
=−
= 𝑒 𝑦 π‘π‘œπ‘  π‘₯ = 1 + 𝑦 βž” 𝑒 𝑦 π‘π‘œπ‘  π‘₯ − 1 − 𝑦 = 0
= 𝑒 𝑦 𝑠𝑖𝑛 π‘₯ = π‘₯ βž” 𝑒 𝑦 𝑠𝑖𝑛 π‘₯ − π‘₯ = 0
(𝑒 𝑦 π‘π‘œπ‘  π‘₯−1−𝑦)
(𝑒 𝑦 𝑠𝑖𝑛 π‘₯−π‘₯)
64] If 𝒇(𝒙, π’š) where 𝒙 = 𝒆𝒖 𝒄𝒐𝒔 𝒗 & π’š = 𝒆𝒖 π’”π’Šπ’ 𝒗 , Show that
𝝏𝒇
𝝏𝒇
𝝏𝒇
𝝏𝒇
= 𝒙 𝝏𝒙 + π’š ππ’š &
𝝏𝒖
𝝏𝒇
𝝏𝒇
= −π’š 𝝏𝒙 + 𝒙 ππ’š
𝝏𝒗
Solution:
βž”
πœ•π‘“
πœ•π‘’
Since
βž”
πœ•π‘“
πœ•π‘’
Then:
βž”
πœ•π‘“
πœ•π‘£
Since
βž”
πœ•π‘“
πœ•π‘£
Then:
Page | 55
=
πœ•π‘“
πœ•π‘₯
πœ•π‘₯
πœ•π‘’
=
πœ•π‘₯
πœ•π‘’
=
πœ•π‘₯
+
πœ•π‘“
πœ•π‘¦
∗
πœ•π‘¦
πœ•π‘’
∗ 𝑒 𝑒 π‘π‘œπ‘  𝑣 +
∗
πœ•π‘“
πœ•π‘₯
πœ•π‘₯
πœ•π‘£
+𝑦
+
πœ•π‘“
πœ•π‘¦
πœ•π‘“
πœ•π‘¦
∗
πœ•π‘“
πœ•π‘¦
πœ•π‘¦
πœ•π‘’
πœ•π‘“
πœ•π‘₯
πœ•π‘“
is true
πœ•π‘¦
πœ•π‘£
πœ•π‘£
∗ (−𝑒 𝑒 𝑠𝑖𝑛 𝑣 ) +
= −𝑦
πœ•π‘“
πœ•π‘₯
+π‘₯
= 𝑒 𝑒 𝑠𝑖𝑛 𝑣 = 𝑦
∗ 𝑒 𝑒 𝑠𝑖𝑛 𝑣
= −𝑒 𝑒 𝑠𝑖𝑛 𝑣 = −𝑦 &
πœ•π‘£
=
πœ•π‘’
=π‘₯
πœ•π‘“
πœ•π‘₯
πœ•π‘₯
= 𝑒 𝑒 π‘π‘œπ‘  𝑣 = π‘₯ &
πœ•π‘“
πœ•π‘“
∗
πœ•π‘“
πœ•π‘¦
πœ•π‘“
πœ•π‘¦
πœ•π‘¦
πœ•π‘£
= 𝑒 𝑒 π‘π‘œπ‘  𝑣 = π‘₯
∗ 𝑒 𝑒 π‘π‘œπ‘  𝑣
is true
𝝏𝒛 𝝏𝒛
65] If 𝒛 = π’™πŸ + π’šπŸ when 𝒙 = 𝒓 𝐜𝐨𝐬 𝜽 , π’š = 𝒓 𝐬𝐒𝐧 𝟐𝜽 , Find 𝝏𝒓 , 𝝏𝜽
respectively
A- πŸπ’“(𝐜𝐨𝐬 𝜽)𝟐 + πŸπ’“(𝐬𝐒𝐧 𝟐𝜽)𝟐 , −π’“πŸ 𝐬𝐒𝐧 𝟐𝜽 + πŸπ’“πŸ 𝐬𝐒𝐧 πŸ’πœ½
B- πŸπ’“(𝐜𝐨𝐬 𝜽)𝟐 + πŸπ’“(𝐬𝐒𝐧 𝟐𝜽)𝟐 , π’“πŸ 𝐬𝐒𝐧 𝟐𝜽 + πŸπ’“πŸ 𝐬𝐒𝐧 πŸ’πœ½
C- 𝟐(𝐜𝐨𝐬 𝜽)𝟐 + πŸπ’“(𝐬𝐒𝐧 𝟐𝜽)𝟐 , −π’“πŸ 𝐬𝐒𝐧 𝟐𝜽 + πŸπ’“πŸ 𝐬𝐒𝐧 πŸ’πœ½
D- None of them
Solution:
πœ•π‘§
πœ•π‘Ÿ
πœ•π‘§
πœ•π‘₯
πœ•π‘§
πœ•π‘Ÿ
=
πœ•π‘§
πœ•π‘₯
∗
= 2π‘₯ ,
πœ•π‘₯
πœ•π‘Ÿ
πœ•π‘₯
πœ•π‘Ÿ
+
πœ•π‘§
πœ•π‘¦
∗
πœ•π‘¦
πœ•π‘Ÿ
= cos πœƒ ,
πœ•π‘§
πœ•π‘¦
= 2𝑦 ,
πœ•π‘¦
πœ•π‘Ÿ
= sin 2πœƒ
= (2π‘₯ ) ∗ (cos πœƒ ) + (2𝑦) ∗ (sin 2πœƒ ) = 2π‘₯ cos πœƒ + 2𝑦 sin 2πœƒ
By substitute βž” π‘₯ = π‘Ÿ cos πœƒ , 𝑦 = π‘Ÿ sin 2πœƒ
Then:
πœ•π‘§
πœ•π‘Ÿ
= 2(π‘Ÿ cos πœƒ ) ∗ cos πœƒ + 2(π‘Ÿ sin 2πœƒ ) ∗ sin 2πœƒ
= 2π‘Ÿ(cos πœƒ )2 + 2π‘Ÿ(sin 2πœƒ )2
πœ•π‘§
πœ•πœƒ
πœ•π‘§
πœ•π‘₯
πœ•π‘§
πœ•πœƒ
=
πœ•π‘§
πœ•π‘₯
∗
= 2π‘₯ ,
πœ•π‘₯
πœ•πœƒ
πœ•π‘₯
πœ•πœƒ
+
πœ•π‘§
πœ•π‘¦
∗
πœ•π‘¦
πœ•πœƒ
= −π‘Ÿ sin πœƒ ,
πœ•π‘§
πœ•π‘¦
= 2𝑦 ,
πœ•π‘¦
πœ•πœƒ
= 2π‘Ÿ cos 2πœƒ
= (2π‘₯ ) ∗ (−π‘Ÿ sin πœƒ ) + (2𝑦) ∗ (2π‘Ÿ cos 2πœƒ ) = −2π‘Ÿπ‘₯ sin πœƒ + 4π‘Ÿπ‘¦ cos 2πœƒ
By substitute βž” π‘₯ = π‘Ÿ cos πœƒ , 𝑦 = π‘Ÿ sin 2πœƒ
Then:
πœ•π‘§
πœ•πœƒ
= −2π‘Ÿ ∗ (π‘Ÿ cos πœƒ ) ∗ sin πœƒ + 4π‘Ÿ(π‘Ÿ sin 2πœƒ ) ∗ cos 2πœƒ
= −2π‘Ÿ 2 sin πœƒ cos πœƒ + 4π‘Ÿ 2 sin 2πœƒ cos 2πœƒ
= −π‘Ÿ 2 sin 2πœƒ + 2π‘Ÿ 2 sin 4πœƒ
Page | 56
𝝏𝒛
66] Find
𝝏𝒙
&
𝝏𝒛
ππ’š
if π’™πŸ‘ + π’šπŸ‘ + π’›πŸ‘ + πŸ”π’™π’šπ’› = 𝟏 respectively
(π’™πŸ +πŸπ’šπ’›) (π’šπŸ +πŸπ’™π’›)
(π’™πŸ +πŸπ’šπ’›)
A- − (π’›πŸ +πŸπ’™π’š) , (π’›πŸ +πŸπ’™π’š)
C-
(π’™πŸ +πŸπ’šπ’›)
− (π’›πŸ +πŸπ’™π’š) ,
(π’šπŸ +πŸπ’™π’›)
B- (π’›πŸ +πŸπ’™π’š) , − (π’›πŸ+πŸπ’™π’š)
(π’šπŸ +πŸπ’™π’›)
− (π’›πŸ +πŸπ’™π’š)
D- None of them
Solution:
βž” π‘₯ 3 + 𝑦 3 + 𝑧 3 + 6π‘₯𝑦𝑧 − 1 = 0
πœ•π‘§
πœ•π‘₯
=−
Then:
πœ•π‘§
πœ•π‘¦
=−
πœ•π‘“
πœ•π‘¦
πœ•π‘“
πœ•π‘§
πœ•π‘¦
𝑓𝑧
βž” 𝑓π‘₯ = 3π‘₯ 2 + 6𝑦𝑧 = 0 , 𝑓𝑧 = 3𝑧 2 + 6π‘₯𝑦 = 0
= − (3𝑧 2
πœ•π‘₯
πœ•π‘§
𝑓π‘₯
(3π‘₯ 2 +6𝑦𝑧)
πœ•π‘§
=−
Then:
πœ•π‘“
πœ•π‘₯
πœ•π‘“
πœ•π‘§
=−
𝑓𝑦
𝑓𝑧
+6π‘₯𝑦)
(π‘₯ 2 +2𝑦𝑧)
= − (𝑧 2
+2π‘₯𝑦)
βž” 𝑓𝑦 = 3𝑦 2 + 6π‘₯𝑧 = 0 , 𝑓𝑧 = 3𝑧 2 + 6π‘₯𝑦 = 0
(3𝑦 2 +6π‘₯𝑧)
= − (3𝑧 2
+6π‘₯𝑦)
(𝑦 2 +2π‘₯𝑧)
= − (𝑧 2
+2π‘₯𝑦)
67] If 𝒛 = 𝒇(𝒙, π’š) has continuous second-order partial derivatives
and 𝒙 = π’“πŸ + π’”πŸ , π’š = πŸπ’“π’” , Find :
𝝏𝒛
[1] 𝝏𝒓
𝝏𝒛
𝝏𝒛
𝝏𝒛
𝝏𝒛
𝝏𝒛
A- 𝝏𝒙 ∗ πŸπ’“ − ππ’š ∗ πŸπ’”
C- 𝝏𝒙 ∗ πŸπ’“ + ππ’š ∗ πŸπ’”
D- None of them
Solution:
πœ•π‘§
πœ•π‘Ÿ
=
πœ•π‘§
πœ•π‘₯
Page | 57
∗
πœ•π‘₯
πœ•π‘Ÿ
+
πœ•π‘§
πœ•π‘¦
∗
πœ•π‘¦
πœ•π‘Ÿ
=
𝝏𝒛
B- 𝝏𝒙 ∗ πŸπ’“ + ππ’š ∗ πŸπ’“
πœ•π‘§
πœ•π‘₯
∗ 2π‘Ÿ +
πœ•π‘§
πœ•π‘¦
∗ 2𝑠
𝝏𝟐 𝒛
[2] ππ’“πŸ
𝝏𝒛
𝟐
𝟐𝝏 𝒛
πŸ’π’“ ππ’™πŸ
𝝏𝒛
𝝏𝟐 𝒛
A- 𝟐 𝝏𝒙 +
𝝏𝟐 𝒛
𝟐
𝟐𝝏 𝒛
πŸ’π’” ππ’šπŸ
𝝏𝟐 𝒛
𝝏𝟐 𝒛
+ πŸ–π’“π’” ππ’™ππ’š +
𝝏𝒛
B- 𝟐 𝝏𝒙 +
C- 𝟐 𝝏𝒙 + πŸ’π’“πŸ ππ’™πŸ + πŸ–π’“π’” ππ’™ππ’š + πŸ’π’”πŸ ππ’šπŸ
𝟐
𝟐𝝏 𝒛
πŸ’π’“ ππ’™πŸ
D- None of them
Solution:
πœ•2 𝑧
πœ•π‘Ÿ 2
πœ•
=
πœ•π‘§
πœ•
πœ•
=
πœ•
πœ•π‘Ÿ
πœ•
=
Then:
πœ•π‘₯
πœ•
=
Then:
πœ•π‘§
πœ•π‘₯
πœ•π‘§
πœ•
+ 2π‘Ÿ ∗
πœ•
πœ•
πœ•π‘¦
πœ•
∗
πœ•π‘§
πœ•
πœ•π‘§
( ) + 2𝑠 ∗ πœ•π‘Ÿ (πœ•π‘¦ )
πœ•π‘Ÿ πœ•π‘₯
πœ•π‘₯
πœ•π‘§
πœ•
πœ•π‘¦
πœ•π‘§
πœ•
πœ•π‘₯
∗
πœ•π‘§
πœ•π‘₯
∗
πœ•2 𝑧
πœ•π‘₯
πœ•π‘₯
πœ•π‘Ÿ
2 ∗
πœ•2 𝑧
πœ•π‘₯ 2
πœ•π‘₯
πœ•π‘Ÿ
+
∗ 2π‘Ÿ +
+
πœ•
πœ•π‘¦
πœ•2 𝑧
πœ•π‘₯πœ•π‘¦
∗
πœ•2 𝑧
πœ•π‘₯πœ•π‘¦
∗
πœ•π‘§
πœ•π‘₯
∗
πœ•π‘¦
πœ•π‘Ÿ
πœ•π‘¦
πœ•π‘Ÿ
∗ 2𝑠
πœ•π‘¦
πœ•π‘Ÿ
πœ•π‘§
πœ•
πœ•π‘¦
πœ•π‘§
πœ•
πœ•π‘₯
πœ•π‘§
( ) = πœ•π‘¦ ∗ πœ•π‘Ÿ ∗ (πœ•π‘¦) + πœ•π‘₯ ∗ πœ•π‘Ÿ ∗ (πœ•π‘¦)
πœ•π‘Ÿ πœ•π‘¦
=
=
Page | 58
πœ•π‘§
( ) = πœ•π‘₯ ∗ πœ•π‘Ÿ ∗ (πœ•π‘₯) + πœ•π‘¦ ∗ πœ•π‘Ÿ ∗ (πœ•π‘₯)
πœ•π‘Ÿ πœ•π‘₯
=
πœ•π‘Ÿ
πœ•
πœ•π‘Ÿ
=
πœ•
πœ•π‘§
πœ•π‘₯
∗
=
βž”
πœ•π‘§
( ∗ 2π‘Ÿ) + πœ•π‘Ÿ (πœ•π‘¦ ∗ 2𝑠 )
πœ•π‘Ÿ πœ•π‘₯
=2
βž”
πœ•π‘§
( ) = πœ•π‘Ÿ (πœ•π‘₯ ∗ 2π‘Ÿ + πœ•π‘¦ ∗ 2𝑠 )
πœ•π‘Ÿ πœ•π‘Ÿ
πœ•
πœ•π‘¦
∗
πœ•π‘§
πœ•π‘¦
∗
πœ•π‘¦
πœ•π‘Ÿ
+
πœ•
πœ•π‘₯
πœ•2 𝑧
πœ•2 𝑧
πœ•π‘¦
πœ•π‘¦πœ•π‘₯
2 ∗ 2𝑠 +
∗
πœ•π‘§
πœ•π‘¦
∗ 2π‘Ÿ
∗
πœ•π‘₯
πœ•π‘Ÿ
=
πœ•2 𝑧
πœ•π‘¦
πœ•π‘¦
πœ•π‘Ÿ
2 ∗
+
πœ•2 𝑧
πœ•π‘¦πœ•π‘₯
∗
πœ•π‘₯
πœ•π‘Ÿ
+
𝟐
𝟐𝝏 𝒛
πŸ’π’” ππ’šπŸ
βž”2
=2
=2
=2
πœ•π‘§
πœ•π‘₯
πœ•π‘§
πœ•π‘₯
πœ•π‘§
πœ•π‘₯
πœ•π‘§
πœ•π‘₯
Page | 59
+ 2π‘Ÿ ∗
πœ•
πœ•π‘§
+ 2π‘Ÿ ∗ (
πœ•2 𝑧
πœ•π‘₯ 2
+ 4π‘Ÿ 2
+
πœ•
πœ•π‘§
( ) + 2𝑠 ∗ πœ•π‘Ÿ (πœ•π‘¦ )
πœ•π‘Ÿ πœ•π‘₯
∗ 2π‘Ÿ +
πœ•2 𝑧
πœ•π‘₯πœ•π‘¦
πœ•2 𝑧
πœ•2 𝑧
πœ•π‘₯
πœ•π‘₯πœ•π‘¦
2 + 4π‘Ÿπ‘ 
2
2πœ• 𝑧
4π‘Ÿ
πœ•π‘₯ 2
+ 8π‘Ÿπ‘ 
πœ•2 𝑧
πœ•π‘₯πœ•π‘¦
∗ 2𝑠) + 2𝑠 ∗ (
πœ•π‘¦ 2
+ 4𝑠 2
+
πœ•2 𝑧
∗ 2𝑠 +
πœ•2 𝑧
πœ•2 𝑧
πœ•π‘¦
πœ•π‘¦πœ•π‘₯
2 + 4π‘Ÿπ‘ 
2
2πœ• 𝑧
4𝑠
πœ•π‘¦ 2
πœ•2 𝑧
πœ•π‘¦πœ•π‘₯
∗ 2π‘Ÿ)
68] Find Fourier series for the function 𝒇(𝒙) , defined by
−𝟏 π’˜π’‰π’†π’ − 𝝅 ≤ 𝒙 ≤ 𝟎
𝒇(𝒙) = {
𝟏
π’˜π’‰π’†π’ 𝟎 ≤ 𝒙 ≤ 𝝅
𝟐
𝒏
A- ∑∞
𝒏=𝟏 (𝒏𝝅 [(𝟏 + (−𝟏) )] 𝐬𝐒𝐧(𝒏𝒙))
𝟐
𝒏
B- ∑∞
𝒏=𝟏 (𝒏𝝅 [(𝟏 − (−𝟏) )] 𝐬𝐒𝐧(𝒏𝒙))
𝟏
𝒏
C- ∑∞
𝒏=𝟏 (𝒏𝝅 [(𝟏 − (−𝟏) )] 𝐬𝐒𝐧(𝒏𝒙))
D- None of them
Solution:
Even or Odd or Neither Even nor Odd?
𝑓(−π‘₯ ) = {
−1
1
, −πœ‹ < −π‘₯ < 0
, 0 < −π‘₯ < πœ‹
Multiplying by −𝟏
−1
,πœ‹ > π‘₯ > 0
→{
1
, 0 > π‘₯ > −πœ‹
Then it is Odd ;
Then π’‚πŸŽ , 𝒂𝒏 = 0 & 𝒃𝒏 has a value
1
π‘›πœ‹π‘₯
2
πœ†
𝑓(π‘₯ ) = π‘Ž0 + ∑∞
𝑛=1 (π‘Žπ‘› cos (
1
2
π‘›πœ‹π‘₯
)
πœ‹
𝑓(π‘₯) = π‘Ž0 + ∑∞
𝑛=1 (π‘Žπ‘› cos (
π‘›πœ‹π‘₯
) + 𝑏𝑛 sin (
π‘›πœ‹π‘₯
))
πœ‹
+ 𝑏𝑛 sin (
πœ†
)) βž” 𝝀 = 𝝅
1
2
= π‘Ž0 + ∑∞
𝑛=1(π‘Žπ‘› cos(𝑛π‘₯ ) +
𝑏𝑛 sin(𝑛π‘₯))
1
= ∗ 0 + ∑∞
𝑛=1(0 ∗ cos(𝑛π‘₯) + 𝑏𝑛 sin(𝑛π‘₯))
2
= ∑∞
𝑛=1(𝑏𝑛 sin(𝑛π‘₯))
Page | 60
1
πœ‹
0
1
πœ‹
𝒃𝒏 = ∫−πœ‹ 𝑓(π‘₯ ) sin(𝑛π‘₯ ) 𝑑π‘₯ = [∫−πœ‹ 𝑓(π‘₯ ) sin(𝑛π‘₯ ) + ∫0 𝑓(π‘₯ ) sin(𝑛π‘₯ )]
πœ‹
πœ‹
1
= [− [
− cos(𝑛π‘₯) 0
πœ‹
1
= [[
πœ‹
=
=
=
=
1
π‘›πœ‹
1
π‘›πœ‹
1
π‘›πœ‹
1
π‘›πœ‹
]
𝑛
−πœ‹
cos(𝑛π‘₯) 0
]
𝑛
−πœ‹
−[
+[
− cos(𝑛π‘₯) πœ‹
𝑛
] ]
0
cos(𝑛π‘₯) πœ‹
] ]
𝑛
0
[(cos 0 − cos π‘›πœ‹) − (cos(−π‘›πœ‹) − cos 0)]
[(1 − (−1)𝑛 ) − ((−1)𝑛 − 1)]
[(1 − (−1)𝑛 ) − (−1)𝑛 + 1]
[(2 − 2(−1)𝑛 )] =
∞
Then: ∑∞
𝑛=1(𝑏𝑛 sin(𝑛π‘₯ )) = ∑𝑛=1 (
2
π‘›πœ‹
𝟐
𝒏𝝅
[(𝟏 − (−𝟏)𝒏 )]
[(1 − (−1)𝑛 )] sin(𝑛π‘₯ ))
Choice B
69] What are Fourier Coefficients?
A- the terms that are presented in a Fourier Series
B- the terms that are obtained through Fourier Series
C- the terms which consist of the Fourier along with their Sine or
Cosine values
D- the terms which are of resemblance to Fourier transform in a
Fourier Series are called Fourier Series Coefficients
Solution:
Choice C
Page | 61
‫ Ω‡Ωˆ كده‬Fourier Series ‫ Ψ§Ψ£Ω„Ψ΅Ω„ Ψ¨ΨͺΨ§ΨΉβ€¬ΨŒ ‫بء يا سيدي Ω„Ω„Ψͺوآيح بس‬
1
π‘›πœ‹π‘₯
2
πœ†
𝑓(π‘₯ ) = π‘Ž0 + ∑∞
𝑛=1 (π‘Žπ‘› cos (
1
0πœ‹π‘₯
2
πœ†
= π‘Ž0 cos (
π‘›πœ‹π‘₯
) + 𝑏𝑛 sin (
π‘›πœ‹π‘₯
) + ∑∞
𝑛=1 (π‘Žπ‘› cos (
1
π‘›πœ‹π‘₯
2
πœ†
1
π‘›πœ‹π‘₯
2
πœ†
= π‘Ž0 ∗ 1 + ∑∞
𝑛=1 (π‘Žπ‘› cos (
= π‘Ž0 ∗ 1 + ∑∞
𝑛=1 (π‘Žπ‘› cos (
πœ†
πœ†
))
π‘›πœ‹π‘₯
) + 𝑏𝑛 sin (
π‘›πœ‹π‘₯
) + 𝑏𝑛 sin (
πœ†
π‘›πœ‹π‘₯
) + 𝑏𝑛 sin (
πœ†
πœ†
))
))
))
Cosine terms ‫ Ωˆβ€¬Sine ‫بالΨͺΨ§Ω„ΩŠ Ψ§Ψ£Ω„Ψ΅Ω„ Ψ¨ΨͺΨ§ΨΉ Ψ§Ω„Ω…ΨͺΨ³Ω„Ψ³Ω„Ψ© دي Ψ§Ω† ΩΩŠΩ‡Ψ§β€¬
70] If the function 𝒇(𝒙) is even , then which of the following is zero?
A- 𝒂𝒏
B- π’‚πŸŽ
C- 𝒃𝒏
D- A & B
Solution:
Since 𝑓(π‘₯ ) is even , then 𝒃𝒏 = 0 βž” Choice C
71] The Fourier Series of an odd periodic function , contains only …
A- Cosine terms
C- Odd harmonics
B- Sine terms
D- Even harmonics
Solution:
Since 𝑓(π‘₯ ) is odd , then π’‚πŸŽ , 𝒂𝒏 = 0 βž” then 𝒃𝒏 has a value
Then: The Fourier Series contains Sine terms
Choice B
Page | 62
72] If the function 𝒇(𝒙) is odd , then which of the following is zero?
A- 𝒂𝒏
B- π’‚πŸŽ
C- 𝒃𝒏
D- A & B
Solution:
Since 𝑓(π‘₯ ) is odd , then π’‚πŸŽ , 𝒂𝒏 = 0
Choice D
73] The trigonometric Fourier Series of an even function does not
have …
A- Cosine terms
C- Odd harmonics
B- Sine terms
D- Even harmonics
Solution:
Since 𝑓(π‘₯ ) is even , then 𝒃𝒏 = 0
Then: The Fourier Series doesn’t contain Sine terms
Choice B
74] Fourier Series representation can be used in case non-periodic
signals too. True or False
A-True
E- False
Solution:
Choice E
Page | 63
75] The Fourier Series of a real periodic function has only
( I ) Cosine terms if it is even
( II ) Sine terms if it is even
( III ) Cosine terms if it is odd
( IV ) Sine terms if it is odd
Which of the above statement is correct ?
A- I and III
B- II and IV
C- II and III
D- I and IV
Solution:
If the function is even βž” 𝒃𝒏 = 0 , 𝒂𝒏 , π’‚πŸŽ have values
then: it consists of Cosine terms only
If the function is odd βž” 𝒂𝒏 , π’‚πŸŽ = 0 , 𝒃𝒏 has a value
then: it consists of Sine terms only
Choice D
76] Find fourier series for the function 𝒇(𝒙) , defined by 𝒇(𝒙) =
when −𝝅 ≤ 𝒙 ≤ 𝝅
π…πŸ
𝟏
π…πŸ
𝟏
π…πŸ
𝟏
𝒏
A- 𝟏𝟐 + ∑∞
𝒏=𝟏 ((−𝟏) π’πŸ 𝐬𝐒𝐧(𝒏𝒙))
𝒏
B- 𝟏𝟐 + ∑∞
𝒏=𝟏 ((−𝟏) 𝒏 𝐜𝐨𝐬(𝒏𝒙))
𝒏
C- 𝟏𝟐 + ∑∞
𝒏=𝟏 ((−𝟏) π’πŸ 𝐜𝐨𝐬(𝒏𝒙))
D- None of them
Page | 64
π’™πŸ
πŸ’
,
Solution:
Even or Odd or Neither Even nor Odd?
𝑓(−π‘₯ ) =
(−𝒙)𝟐
πŸ’
=
π’™πŸ
πŸ’
Then it is Even ; Then 𝒃𝒏 = 0 & π’‚πŸŽ , 𝒂𝒏 have values
1
π‘›πœ‹π‘₯
2
πœ†
𝑓(π‘₯ ) = π‘Ž0 + ∑∞
𝑛=1 (π‘Žπ‘› cos (
π‘›πœ‹π‘₯
) + 𝑏𝑛 sin (
πœ†
)) βž” 𝝀 = 𝝅
1
𝑓(π‘₯ ) = π‘Ž0 + ∑∞
𝑛=1(π‘Žπ‘› cos(𝑛π‘₯ ) + 𝑏𝑛 sin(𝑛π‘₯ ))
2
π’‚πŸŽ =
πœ‹
𝑓 (π‘₯ ) 𝑑π‘₯
∫
πœ‹ −πœ‹
1
=
πœ‹ π‘₯2
𝑑π‘₯
∫
πœ‹ −πœ‹ 4
1
1 π‘₯3
πœ‹
= [
πœ‹ 12
𝒂𝒏 =
=
=
Page | 65
+
πœ‹3
12
−πœ‹3
12
1 2πœ‹3
]= [
πœ‹
12
πœ‹
𝑓 (π‘₯ ) cos(𝑛π‘₯ ) 𝑑π‘₯
∫
πœ‹ −πœ‹
]=
πœ‹ π‘₯2
∫
πœ‹ −πœ‹ 4
1
=
π‘₯ 2 ∗ cos(𝑛π‘₯ ) 𝑑π‘₯
∫
−πœ‹
4πœ‹
1
4πœ‹
2
[(π‘₯ ∗
1
sin 𝑛π‘₯
𝑛
− ((2πœ‹ ∗
4πœ‹
1
4πœ‹
[
π…πŸ
πŸ”
D
∗ cos(𝑛π‘₯ ) 𝑑π‘₯
πœ‹
1
]
6
1
[
=
πœ‹ 12
−
πœ‹2
((πœ‹ 2 ∗
=
= [
πœ‹ 12 −πœ‹
1 πœ‹3
Then: π’‚πŸŽ =
1 πœ‹3
= [ ]
𝑛
− cos 𝑛π‘₯
𝑛2
𝑛2
𝑛3
) − (2 ∗
((0) − (0)) − ((2πœ‹ ∗
𝑛2
𝑛
𝑛2
𝑛3
))
) + (2πœ‹ ∗
+((0) − (0))
)]
cos 𝑛π‘₯
+
πœ‹
−πœ‹
2π‘₯
−
))
− cos 𝑛∗−πœ‹
− sin 𝑛∗−πœ‹
−(−1)𝑛
𝑛3
sin 𝑛∗−πœ‹
) − (2 ∗ −πœ‹ ∗
− sin 𝑛∗πœ‹
− sin 𝑛π‘₯
) + (2 ∗
) − ((−πœ‹)2 ∗
− cos π‘›πœ‹
+ ((2 ∗
π‘₯2
) − (2π‘₯ ∗
sin π‘›πœ‹
I
2
+
))
0
]
−(−1)𝑛
𝑛2
))
]
sin 𝑛π‘₯
𝑛
− cos 𝑛π‘₯
𝑛2
− sin 𝑛π‘₯
𝑛3
=
=
=
1
4πœ‹
1
4πœ‹
1
4πœ‹
[− (− (2πœ‹ ∗
[((2πœ‹ ∗
[
4πœ‹(−1)𝑛
𝑛2
(−1)𝑛
(−1)𝑛
𝑛2
]=
𝑛2
) − (2πœ‹ ∗
) + (2πœ‹ ∗
(−1)𝑛
𝑛2
Then: 𝒂𝒏 = (−1)𝑛
(−1)𝑛
𝑛2
(−1)𝑛
𝑛2
= (−𝟏)𝒏
))]
2πœ‹(−1)𝑛
1
))] = 4πœ‹ [(
𝑛2
+
2πœ‹(−1)𝑛
𝑛2
)]
𝟏
π’πŸ
1
𝑛2
1
𝑓(π‘₯ ) = π‘Ž0 + ∑∞
𝑛=1(π‘Žπ‘› cos(𝑛π‘₯ ) + 𝑏𝑛 sin(𝑛π‘₯ )) , 𝑏𝑛 = 0
2
1
1
𝑓(π‘₯ ) = π‘Ž0 + ∑∞
𝑛=1(π‘Žπ‘› cos(𝑛π‘₯ ) + 0 ∗ sin(𝑛π‘₯ )) = 𝑓 (π‘₯ ) = π‘Ž0 +
2
∞
∑𝑛=1(π‘Žπ‘› cos(𝑛π‘₯ ))
1
πœ‹2
2
6
= ∗
𝑛
+ ∑∞
𝑛=1 ((−1)
2
1
πœ‹2
𝑛
12
( )
2 cos 𝑛π‘₯ ) =
𝑛
+ ∑∞
𝑛=1 ((−1)
1
𝑛2
cos(𝑛π‘₯ ))
1
Then: 𝑓(π‘₯) = 2 π‘Ž0 + ∑∞
𝑛=1(π‘Žπ‘› cos(𝑛π‘₯ ) + 𝑏𝑛 sin(𝑛π‘₯ ))
=
πœ‹2
12
𝑛
+ ∑∞
𝑛=1 ((−1)
1
𝑛2
cos(𝑛π‘₯ )) Choice C
77] Find Fourier series for the function 𝒇(𝒙) , defined by
𝒇(𝒙) = {
𝟏
A- πŸ’ +
𝟏
B- +
𝟐
𝟏
C- πŸ’ +
𝟎 , −𝟏 < 𝒙 < 𝟎
𝒙, 𝟎<𝒙<𝟏
(−𝟏)𝒏 −𝟏
∞
∑𝒏=𝟏 ( ( )𝟐 𝒄𝒐𝒔(𝒏𝝅𝒙)
𝒏𝝅
(−𝟏)𝒏 −𝟏
∞
∑𝒏=𝟏 (
𝒄𝒐𝒔(𝒏𝝅𝒙)
(𝒏𝝅)𝟐
(−𝟏)𝒏 −𝟏
∞
∑𝒏=𝟏 ( ( )𝟐 𝒄𝒐𝒔(𝒏𝝅𝒙)
𝒏𝝅
D- None of them
Page | 66
−
−
+
(−𝟏)𝒏
𝒏𝝅
(−𝟏)𝒏
𝒏𝝅
(−𝟏)𝒏
𝒏𝝅
π’”π’Šπ’(𝒏𝝅𝒙))
π’”π’Šπ’(𝒏𝝅𝒙))
π’”π’Šπ’(𝒏𝝅𝒙))
Solution:
Even or Odd or Neither Even nor Odd?
𝑓(−π‘₯ ) = {
0
−π‘₯
, −1 < −π‘₯ < 0
, 0 < −π‘₯ < 1
Multiplying by −𝟏
0
→{
−π‘₯
,1 > π‘₯ > 0
, 0 > π‘₯ > −1
Then it is Neither even nor odd ; Then π‘Ž0 , π‘Žπ‘› , 𝑏𝑛 have values
1
π‘›πœ‹π‘₯
2
πœ†
𝑓(π‘₯ ) = π‘Ž0 + ∑∞
𝑛=1 (π‘Žπ‘› π‘π‘œπ‘  (
π‘›πœ‹π‘₯
) + 𝑏𝑛 𝑠𝑖𝑛 (
πœ†
))
2πœ† = 2 , πœ† = 1
π’‚πŸŽ =
πœ†
𝑓(π‘₯ ) 𝑑π‘₯
∫
πœ† −πœ†
1
=
πœ†
1
𝒂𝒏 = ∫−πœ† 𝑓(π‘₯ ) π‘π‘œπ‘  (
πœ†
0
𝑓(π‘₯ )
(
∫
1 −1
1
π‘›πœ‹π‘₯
πœ†
+
1
1
∫0 𝑓(π‘₯ )) 𝑑π‘₯
=0+
1
∫0 π‘₯ 𝑑π‘₯
π‘₯2
1
=0+[ ] =
2 0
𝟏
𝟐
1
) 𝑑π‘₯ = 1 ∫−1 𝑓(π‘₯ ) π‘π‘œπ‘ (π‘›πœ‹π‘₯ ) 𝑑π‘₯
0
1
= ∫−1 𝑓 (π‘₯ ) π‘π‘œπ‘ (π‘›πœ‹π‘₯ ) + ∫0 𝑓(π‘₯ ) π‘π‘œπ‘ (π‘›πœ‹π‘₯ )
0
1
= ∫−1 0 ∗ π‘π‘œπ‘ (π‘›πœ‹π‘₯ ) + ∫0 π‘₯ ∗ π‘π‘œπ‘ (π‘›πœ‹π‘₯ )
1
∫0 π‘₯ ∗ π‘π‘œπ‘ (π‘›πœ‹π‘₯ )
=π‘₯∗
=[
π‘₯ 𝑠𝑖𝑛(π‘›πœ‹π‘₯)
=(
π‘›πœ‹
𝑠𝑖𝑛(π‘›πœ‹)
π‘›πœ‹
+
+
𝑠𝑖𝑛(π‘›πœ‹π‘₯ )
π‘π‘œπ‘ (π‘›πœ‹π‘₯ )
π‘₯ 𝑠𝑖𝑛(π‘›πœ‹π‘₯ ) π‘π‘œπ‘ (π‘›πœ‹π‘₯ )
− (−
=
+
)
(π‘›πœ‹)2
(π‘›πœ‹)2
π‘›πœ‹
π‘›πœ‹
π‘π‘œπ‘ (π‘›πœ‹π‘₯) 1
]
(π‘›πœ‹)2 0
π‘π‘œπ‘ (π‘›πœ‹)
)
(π‘›πœ‹)2
−(
(−1)𝑛
D
0∗𝑠𝑖𝑛(π‘›πœ‹∗0)
= (0 + (π‘›πœ‹)2 ) − (0 + 1) =
=
(−𝟏)𝒏 −𝟏
(𝒏𝝅)𝟐
Then: 𝒂𝒏 =
π‘›πœ‹
(−1)𝑛
(π‘›πœ‹)2
(−𝟏)𝒏 −𝟏
+
π‘π‘œπ‘ (π‘›πœ‹∗0)
)
(π‘›πœ‹)2
+
1
−
(𝒏𝝅)𝟐
0
Page | 67
π‘π‘œπ‘ (π‘›πœ‹π‘₯ )
π‘₯
1
− (π‘›πœ‹)2
I
𝑠𝑖𝑛(π‘›πœ‹π‘₯ )
π‘›πœ‹
− π‘π‘œπ‘ (π‘›πœ‹π‘₯ )
(π‘›πœ‹)2
πœ†
1
𝒃𝒏 = ∫−πœ† 𝑓 (π‘₯ ) 𝑠𝑖𝑛 (
πœ†
π‘›πœ‹π‘₯
πœ†
1
1
) 𝑑π‘₯ = 1 ∫−1 𝑓(π‘₯ ) 𝑠𝑖𝑛(π‘›πœ‹π‘₯ ) 𝑑π‘₯
0
1
0
1
= ∫−1 𝑓(π‘₯ ) 𝑠𝑖𝑛(π‘›πœ‹π‘₯ ) + ∫0 𝑓(π‘₯ ) 𝑠𝑖𝑛(π‘›πœ‹π‘₯ ) = ∫−1 0 ∗ 𝑠𝑖𝑛(π‘›πœ‹π‘₯ ) + ∫0 π‘₯ ∗
𝑠𝑖𝑛(π‘›πœ‹π‘₯ )
1
∫0 π‘₯ ∗ 𝑠𝑖𝑛(π‘›πœ‹π‘₯ )
= π‘₯ ∗ (−
= [−
= (−
=
π‘π‘œπ‘ (π‘›πœ‹π‘₯)
π‘›πœ‹
π‘₯ π‘π‘œπ‘ (π‘›πœ‹π‘₯)
π‘›πœ‹
π‘π‘œπ‘ (π‘›πœ‹)
π‘›πœ‹
−(−1)𝑛
π‘›πœ‹
+
+
D
(π‘›πœ‹)2
) − (−
𝑠𝑖𝑛(π‘›πœ‹π‘₯ )
π‘₯
𝑠𝑖𝑛(π‘›πœ‹π‘₯) 1
]
(π‘›πœ‹)2 0
+ 0 − (0) =
Then: 𝒃𝒏 =
𝑠𝑖𝑛(π‘›πœ‹π‘₯)
)
(π‘›πœ‹)2
) − (−
𝑠𝑖𝑛(π‘›πœ‹)
I
+
0∗π‘π‘œπ‘ (π‘›πœ‹∗0)
π‘›πœ‹
+
𝑠𝑖𝑛(π‘›πœ‹∗0)
(π‘›πœ‹)2
1
)
−
−(−𝟏)𝒏
0
𝒏𝝅
−(−𝟏)𝒏
𝒏𝝅
1
Then: 𝑓(π‘₯ ) = π‘Ž0 + ∑∞
𝑛=1(π‘Žπ‘› π‘π‘œπ‘  (π‘›πœ‹π‘₯ ) + 𝑏𝑛 𝑠𝑖𝑛 (π‘›πœ‹π‘₯ ))
2
1
1
(−1)𝑛 −1
2
2
(π‘›πœ‹)2
= ∗ + ∑∞
𝑛=1 (
1
(−1)𝑛 −1
4
(π‘›πœ‹)2
= + ∑∞
𝑛=1 (
Choice A
Page | 68
∗ π‘π‘œπ‘ (π‘›πœ‹π‘₯ ) +
π‘π‘œπ‘ (π‘›πœ‹π‘₯ ) −
(−1)𝑛
π‘›πœ‹
−(−1)𝑛
π‘›πœ‹
∗ 𝑠𝑖𝑛(π‘›πœ‹π‘₯ ))
𝑠𝑖𝑛(π‘›πœ‹π‘₯ ))
− π‘π‘œπ‘ (π‘›πœ‹π‘₯ )
π‘›πœ‹
− 𝑠𝑖𝑛(π‘›πœ‹π‘₯ )
(π‘›πœ‹)2
78] Find Sin Series 𝒃𝒏 , 𝒇(𝒙) = π’†π’Œπ’™ , 𝟎 < 𝒙 < 𝝅 , π’Œ: constant
𝒏
𝒏
A- π’πŸ +π’Œ [−π’†π…π’Œ (−𝟏)𝒏 + 𝟏]
B- π’πŸ +π’ŒπŸ [−π’†π…π’Œ (−𝟏)𝒏 − 𝟏]
𝒏
C- π’πŸ +π’ŒπŸ [−π’†π…π’Œ (−𝟏)𝒏 + 𝟏]
D- None of them
Solution:
1
πœ‹
πœ‹
1
𝒃𝒏 = ∫0 𝑓 (π‘₯ ) sin(𝑛π‘₯ ) 𝑑π‘₯ = ∫0 𝑒 π‘˜π‘₯ sin(𝑛π‘₯ ) 𝑑π‘₯
πœ‹
πœ‹
∫ 𝑒 π‘˜π‘₯ sin(𝑛π‘₯ ) = I
𝑒 = 𝑒 π‘˜π‘₯ , 𝑑𝑒 = π‘˜π‘’ π‘˜π‘₯ , 𝑑𝑣 = sin(𝑛π‘₯ ) , 𝑣 = −
𝑒𝑣 − ∫ 𝑣 𝑑𝑒 = −
𝑒 π‘˜π‘₯ cos(𝑛π‘₯)
− ∫−
𝑛
π‘˜
cos(𝑛π‘₯)
𝑛
cos(𝑛π‘₯)
𝑛
∗ π‘˜π‘’
π‘˜π‘₯
=−
𝑒 π‘˜π‘₯ cos(𝑛π‘₯)
𝑛
+
π’†π’Œπ’™ 𝐜𝐨𝐬(𝒏𝒙)
∫
𝑛
∫ π’†π’Œπ’™ 𝐜𝐨𝐬(𝒏𝒙) βž” 𝑒 = 𝑒 π‘˜π‘₯ , 𝑑𝑒 = π‘˜π‘’ π‘˜π‘₯ , 𝑑𝑣 = cos(𝑛π‘₯ ) , 𝑣 =
𝑒𝑣 − ∫ 𝑣 𝑑𝑒 = 𝑒 π‘˜π‘₯ ∗
Then: −
−
βž”
−
𝑒 π‘˜π‘₯ cos(𝑛π‘₯)
𝑛
𝑒 π‘˜π‘₯ cos(𝑛π‘₯)
𝑛
−
𝑛
𝑛
𝑛
+ [
𝑛
+
+
π‘˜
𝑛2
𝑒
π‘˜π‘₯
I=
𝑛2
π‘˜π‘’ π‘˜π‘₯ sin(𝑛π‘₯)−𝑒 π‘˜π‘₯ 𝑛 cos(𝑛π‘₯)
Page | 69
𝑛2
𝑛
∗
=
𝑛
π‘˜
− ∫ 𝑒 π‘˜π‘₯ sin(𝑛π‘₯ )
𝑛
π‘˜
∫ 𝑒 π‘˜π‘₯ sin(𝑛π‘₯) = −
𝑛2
= I(
sin(𝑛π‘₯)
𝑛
− ∫ 𝑒 π‘˜π‘₯ sin(𝑛π‘₯ )] = I
𝑛
= I (1 +
𝑛2
∗ π‘˜π‘’ π‘˜π‘₯ = 𝑒 π‘˜π‘₯ ∗
π‘˜2
−𝑒 π‘˜π‘₯ 𝑛 cos(𝑛π‘₯)+π‘˜π‘’ π‘˜π‘₯ sin(𝑛π‘₯)
𝑛2 +π‘˜ 2
𝑛
sin(𝑛π‘₯ ) = I +
−𝑒 π‘˜π‘₯ 𝑛 cos(𝑛π‘₯)+π‘˜π‘’ π‘˜π‘₯ sin(𝑛π‘₯)
I=
𝑛
π‘˜π‘’ π‘˜π‘₯ sin(𝑛π‘₯)
𝑛2
sin(𝑛π‘₯)
π‘˜ 𝑒 π‘˜π‘₯ sin(𝑛π‘₯)
𝑒 π‘˜π‘₯ sin(𝑛π‘₯) −
2
𝑒 π‘˜π‘₯ cos(𝑛π‘₯)
−∫
𝑛
π‘˜
+
𝑒 π‘˜π‘₯ cos(𝑛π‘₯)
sin(𝑛π‘₯)
sin(𝑛π‘₯)
2 +
π‘˜2
𝑛2
π‘˜2
𝑛2
2 βž”I =
1
𝑛2 +π‘˜ 2
π‘˜
π‘˜2
𝑛
𝑛2
𝑒 π‘˜π‘₯ sin(𝑛π‘₯) −
2
)
𝑛2 +π‘˜ 2
) = I(
𝑛2
𝑛2 +π‘˜
𝑛
+
I
π‘˜2
𝑛2
𝑒 π‘˜π‘₯ cos(𝑛π‘₯)
𝑛2
)
π‘˜π‘’ π‘˜π‘₯ sin(𝑛π‘₯)−𝑒 π‘˜π‘₯ 𝑛 cos(𝑛π‘₯)
𝑛2 +π‘˜ 2
∗ (π‘˜π‘’ π‘˜π‘₯ sin(𝑛π‘₯ ) − 𝑒 π‘˜π‘₯ 𝑛 cos(𝑛π‘₯ ))
I=I
1
∗ [π‘˜π‘’ π‘˜π‘₯ sin(𝑛π‘₯ ) − 𝑒 π‘˜π‘₯ 𝑛 cos(𝑛π‘₯ )]πœ‹0
𝑛2 +π‘˜ 2
=
1
𝑛2 +π‘˜ 2
∗ [(π‘˜π‘’ πœ‹π‘˜ sin(π‘›πœ‹) − 𝑒 πœ‹π‘˜ 𝑛 cos(π‘›πœ‹)) − [π‘˜π‘’ 0∗π‘₯ sin(𝑛 ∗ 0) −
𝑒 π‘˜∗0 𝑛 cos(𝑛 ∗ 0)]]
=
1
𝑛2 +π‘˜
[(0 − 𝑒 πœ‹π‘˜ 𝑛(−1)𝑛 ) − (0 − 𝑛)] =
2
Then: 𝒃𝒏 =
=
𝟏
π’πŸ +π’ŒπŸ
𝒏
π’πŸ +π’ŒπŸ
𝟏
π’πŸ +π’ŒπŸ
[−π’†π…π’Œ 𝒏(−𝟏)𝒏 + 𝒏]
[−π’†π…π’Œ 𝒏(−𝟏)𝒏 + 𝒏]
[−π’†π…π’Œ (−𝟏)𝒏 + 𝟏]
Choice C
79] Find Fourier series for the function 𝒇(𝒙) , defined by
𝒇(𝒙) = {
𝟎 , −𝝅 < 𝒙 < 𝟎
𝟏, 𝟎<𝒙<𝝅
𝟏
𝟏
𝟏
𝟏
𝒏
A- 𝟐 + ∑∞
𝒏=𝟏 ((− 𝝅𝒏 [(−𝟏) − 𝟏]) 𝐜𝐨𝐬(𝒏𝒙))
𝒏
B- 𝟐 + ∑∞
𝒏=𝟏 ((− 𝝅𝒏 [(−𝟏) − 𝟏]) 𝐬𝐒𝐧(𝒏𝒙))
𝟏
𝒏
C- ∑∞
𝒏=𝟏 ((− 𝝅𝒏 [(−𝟏) − 𝟏]) 𝐬𝐒𝐧(𝒏𝒙))
D- None of them
Solution:
Even or Odd or Neither Even nor Odd?
𝑓(−π‘₯ ) = {
0
1
, −πœ‹ < −π‘₯ < 0
, 0 < −π‘₯ < πœ‹
Multiplying by −𝟏
0
→{
1
Page | 70
,πœ‹ > π‘₯ > 0
, 0 > π‘₯ > −πœ‹
Then it is Neither ; Then π‘Ž0 , π‘Žπ‘› , 𝑏𝑛 have values
1
𝑓(π‘₯ ) = π‘Ž0 + ∑∞
𝑛=1(π‘Žπ‘› cos(𝑛π‘₯ ) + 𝑏𝑛 sin(𝑛π‘₯ ))
2
1
πœ‹
1
0
πœ‹
0
1
πœ‹
π’‚πŸŽ = ∫−πœ‹ 𝑓 (π‘₯ ) 𝑑π‘₯ = [∫−πœ‹ 𝑓(π‘₯ ) + ∫0 𝑓(π‘₯ )] 𝑑π‘₯ = [∫−πœ‹ 0 + ∫0 1] 𝑑π‘₯
πœ‹
πœ‹
πœ‹
1
1
πœ‹
πœ‹
= [0 + [π‘₯ ]πœ‹0 ] = [πœ‹] = 𝟏
1
πœ‹
0
1
πœ‹
𝒂𝒏 = ∫−πœ‹ 𝑓(π‘₯ ) cos(𝑛π‘₯ ) 𝑑π‘₯ = [∫−πœ‹ 𝑓(π‘₯ ) cos(𝑛π‘₯ ) + ∫0 𝑓(π‘₯ ) cos(𝑛π‘₯ )] 𝑑π‘₯
πœ‹
πœ‹
0
1
πœ‹
= [∫−πœ‹ 0 ∗ cos(𝑛π‘₯ ) + ∫0 1 ∗ cos(𝑛π‘₯ )]
πœ‹
1
= [0 +
πœ‹
=
1
πœ‹π‘›
πœ‹
∫0 cos(𝑛π‘₯ )]
1 sin(𝑛π‘₯) πœ‹
= [
πœ‹
𝑛
] =
0
1
πœ‹π‘›
[sin(𝑛π‘₯ )]πœ‹0
[sin(π‘›πœ‹) − sin(𝑛 ∗ 0)] = 𝟎
Then: 𝒂𝒏 = 𝟎
1
πœ‹
0
1
πœ‹
𝒃𝒏 = ∫−πœ‹ 𝑓(π‘₯ ) sin(𝑛π‘₯ ) 𝑑π‘₯ = [∫−πœ‹ 𝑓(π‘₯ ) sin(𝑛π‘₯ ) + ∫0 𝑓(π‘₯ ) sin(𝑛π‘₯ )] 𝑑π‘₯
πœ‹
πœ‹
0
1
πœ‹
= [∫−πœ‹ 0 ∗ sin(𝑛π‘₯ ) + ∫0 1 ∗ sin(𝑛π‘₯ )]
πœ‹
1
= [0 +
πœ‹
=−
=−
Then: 𝒃𝒏 = −
𝟏
𝝅𝒏
1
πœ‹π‘›
𝟏
𝝅𝒏
πœ‹
∫0 sin(𝑛π‘₯ )]
1 − cos(𝑛π‘₯) πœ‹
= [
πœ‹
[cos(π‘›πœ‹) − cos(𝑛 ∗ 0)]
[(−𝟏)𝒏 − 𝟏]
[(−𝟏)𝒏 − 𝟏]
1
𝑓(π‘₯ ) = π‘Ž0 + ∑∞
𝑛=1(π‘Žπ‘› cos(𝑛π‘₯ ) + 𝑏𝑛 sin(𝑛π‘₯ ))
2
1
1
2
πœ‹π‘›
= + ∑∞
𝑛=1 ((−
Choice B
Page | 71
𝑛
[(−1)𝑛 − 1]) ∗ sin(𝑛π‘₯ ))
] =−
0
1
πœ‹π‘›
[cos(𝑛π‘₯ )]πœ‹0
80] Find Fourier series for the function 𝒇(𝒙) , defined by
𝒇(𝒙) = {
𝟎 , −𝝅 < 𝒙 < 𝟎
π’”π’Šπ’ 𝒙 , 𝟎 < 𝒙 < 𝝅
A- 𝝅 + ∑∞
𝒏=𝟏 ((
𝟏
πŸπ…
B- 𝝅 − ∑∞
𝒏=𝟏 ((
C- 𝝅 + ∑∞
𝒏=𝟏 ((
𝟏
πŸπ…
𝟏
πŸπ…
[
−(−𝟏)𝒏 −𝟏
[
[
𝟏+𝒏
−(−𝟏)𝒏 −𝟏
𝟏+𝒏
−(−𝟏)𝒏 −𝟏
𝟏+𝒏
−
−
+
(−𝟏)𝒏 +𝟏
𝟏−𝒏
]) 𝐜𝐨𝐬(𝒏𝒙))
(−𝟏)𝒏 +𝟏
𝟏−𝒏
(−𝟏)𝒏 +𝟏
𝟏−𝒏
]) 𝐜𝐨𝐬(𝒏𝒙))
]) 𝐜𝐨𝐬(𝒏𝒙))
D- None of them
Solution:
Even or Odd or Neither Even nor Odd?
𝑓(−π‘₯ ) = {
0
sin π‘₯
, −πœ‹ < −π‘₯ < 0
, 0 < −π‘₯ < πœ‹
Multiplying by −𝟏
0
→{
sin π‘₯
,πœ‹ > π‘₯ > 0
, 0 > π‘₯ > −πœ‹
Then it is Neither ; Then π‘Ž0 , π‘Žπ‘› , 𝑏𝑛 have values
1
𝑓(π‘₯ ) = π‘Ž0 + ∑∞
𝑛=1(π‘Žπ‘› cos(𝑛π‘₯ ) + 𝑏𝑛 sin(𝑛π‘₯ ))
2
1
πœ‹
1
0
πœ‹
πœ‹
1
1
π’‚πŸŽ = ∫−πœ‹ 𝑓 (π‘₯ ) 𝑑π‘₯ = [∫−πœ‹ 0 + ∫0 sin π‘₯ ] 𝑑π‘₯ = [0 + ∫0 sin π‘₯ ] = [− cos π‘₯]πœ‹0
πœ‹
πœ‹
πœ‹
πœ‹
1
1
𝟐
πœ‹
πœ‹
𝝅
= − [cos πœ‹ + cos 0] = − [−1 − 1] =
1
πœ‹
1
0
πœ‹
𝒂𝒏 = ∫−πœ‹ 𝑓(π‘₯ ) cos(𝑛π‘₯ ) 𝑑π‘₯ = [∫−πœ‹ 𝑓(π‘₯ ) cos(𝑛π‘₯ ) + ∫0 𝑓(π‘₯ ) cos(𝑛π‘₯ )] 𝑑π‘₯
πœ‹
πœ‹
1
0
πœ‹
= [∫−πœ‹ 0 ∗ cos(𝑛π‘₯ ) + ∫0 sin π‘₯ ∗ cos(𝑛π‘₯ )] 𝑑π‘₯
πœ‹
1
πœ‹
= [0 + ∫0 sin π‘₯ ∗ cos(𝑛π‘₯ )]
πœ‹
Page | 72
Since: 1] sin(A + B) = sin A cos B + cos A sin B
2] sin(A − B) = sin A cos B − cos A sin B
By Adding 1 & 2 βž” sin A cos B + cos A sin B + sin A cos B − cos A sin B = 2 sin A cos B
= sin(A + B) + sin(A − B)
Then: sin π‘₯ ∗ cos(𝑛π‘₯ ) = sin A cos B
βž” 2 sin π‘₯ ∗ cos(𝑛π‘₯ ) = 2 sin A cos B = sin(A + B) + sin(A − B)
= sin(π‘₯ + 𝑛π‘₯ ) + sin(π‘₯ − 𝑛π‘₯ )
πœ‹
1
πœ‹
1
βž” 𝒂𝒏 = ∫−πœ‹ 𝑓(π‘₯ ) cos(𝑛π‘₯ ) 𝑑π‘₯ = [∫0 (sin(π‘₯ + 𝑛π‘₯ ) + sin(π‘₯ − 𝑛π‘₯ ))]
πœ‹
2πœ‹
=
=
=
1
2πœ‹
1
2πœ‹
− cos(πœ‹+π‘›πœ‹)
[(
1+𝑛
−(−1)𝑛
[(
1+𝑛
+
+
− cos(πœ‹−π‘›πœ‹)
1−𝑛
−(−1)𝑛
1−𝑛
1
2πœ‹
[
− cos(π‘₯+𝑛π‘₯)
1+𝑛
− cos(0+𝑛∗0)
)−(
−1
1+𝑛
−1
1
𝟏
πŸπ…
[
−(−𝟏)𝒏 −𝟏
𝟏+𝒏
+
−
𝟏
πŸπ…
[
0
− cos(0−𝑛∗0)
1−𝑛
−(−1)𝑛
1
]
1−𝑛
) − (1+𝑛 + 1−𝑛)] = 2πœ‹ [(
=
Then: 𝒂𝒏 =
+
− cos(π‘₯−𝑛π‘₯) πœ‹
1+𝑛
−(−𝟏)𝒏 −𝟏
𝟏+𝒏
−
−
)]
(−1)𝑛
1−𝑛
−1
1
) + (1+𝑛 − 1−𝑛)]
(−𝟏)𝒏 +𝟏
𝟏−𝒏
]
(−𝟏)𝒏 +𝟏
𝟏−𝒏
πœ‹
1
]
0
πœ‹
𝒃𝒏 = ∫−πœ‹ 𝑓(π‘₯ ) sin(𝑛π‘₯ ) 𝑑π‘₯ = [∫−πœ‹ 𝑓(π‘₯ ) sin(𝑛π‘₯ ) + ∫0 𝑓(π‘₯ ) sin(𝑛π‘₯ )] 𝑑π‘₯
πœ‹
πœ‹
1
0
πœ‹
= [∫−πœ‹ 0 ∗ sin(𝑛π‘₯ ) + ∫0 sin π‘₯ ∗ sin(𝑛π‘₯ )]
πœ‹
πœ‹
1
= [0 + ∫0 sin π‘₯ ∗ sin(𝑛π‘₯ )]
πœ‹
Since: 1] cos(π‘₯ − 𝑦) = cos π‘₯ cos 𝑦 + sin π‘₯ sin 𝑦
2] cos(π‘₯ + 𝑦) = cos π‘₯ cos 𝑦 − sin π‘₯ sin 𝑦
By Subtracting 1 & 2 βž” (cos π‘₯ cos 𝑦 + sin π‘₯ sin 𝑦) − (cos π‘₯ cos 𝑦 − sin π‘₯ sin 𝑦)
= 2 sin π‘₯ sin 𝑦 = cos(π‘₯ − 𝑦) − cos(π‘₯ + 𝑦)
Then: sin π‘₯ sin(𝑛π‘₯ ) =
Page | 73
cos(π‘₯−𝑛π‘₯)−cos(π‘₯+𝑛π‘₯)
2
1
πœ‹
πœ‹
πœ‹ cos(π‘₯−𝑛π‘₯)−cos(π‘₯+𝑛π‘₯)
1
[∫0 sin π‘₯ ∗ sin(𝑛π‘₯ )] = [∫0
πœ‹
2
]=
1
2πœ‹
πœ‹
[∫0 (cos(π‘₯ − 𝑛π‘₯ ) −
cos(π‘₯ + 𝑛π‘₯ ))]
=
sin(π‘₯−𝑛π‘₯)
sin(π‘₯+𝑛π‘₯) πœ‹
−
]
2πœ‹
1−𝑛
1+𝑛
0
1
[
=
1
sin(πœ‹−π‘›πœ‹)
sin(πœ‹+π‘›πœ‹)
sin(0−𝑛∗0)
sin(0+𝑛∗0)
−
)−(
−
)]
1−𝑛
1+𝑛
1−𝑛
1+𝑛
= 2πœ‹ [(
1
2πœ‹
[(0 − 0) − (0 − 0)] = 𝟎
Then: 𝒃𝒏 = 𝟎
1
𝑓(π‘₯ ) = π‘Ž0 + ∑∞
𝑛=1(π‘Žπ‘› cos(𝑛π‘₯ ) + 𝑏𝑛 sin(𝑛π‘₯ ))
2
1
2
1
2
πœ‹
2πœ‹
= ∗ + ∑∞
𝑛=1 ((
=πœ‹+
[
−(−1)𝑛 −1
1+𝑛
−
(−1)𝑛 +1
1−𝑛
]) ∗ cos(𝑛π‘₯ ))
(−1)𝑛 +1
1 −(−1)𝑛 −1
∞
∑𝑛=1 (( [
−
]) cos(𝑛π‘₯ ))
2πœ‹
1+𝑛
1−𝑛
Choice A
81] What is the Fourier Series expansion of the function 𝒇(𝒙) in the
interval (𝒄, 𝒄 + πŸπ…) ?
A-
π’‚πŸŽ
𝟐
+ ∑∞
𝒏=𝟏[𝒂𝒏 𝒄𝒐𝒔 𝒏𝒙 + 𝒃𝒏 π’”π’Šπ’ 𝒏𝒙]
B- π’‚πŸŽ + ∑∞
𝒏=𝟏[𝒂𝒏 𝒄𝒐𝒔 𝒏𝒙 + 𝒃𝒏 π’”π’Šπ’ 𝒏𝒙]
C-
π’‚πŸŽ
𝟐
+ ∑∞
𝒏=𝟎[𝒂𝒏 𝒄𝒐𝒔 𝒏𝒙 + 𝒃𝒏 π’”π’Šπ’ 𝒏𝒙]
D- π’‚πŸŽ + ∑∞
𝒏=𝟎[𝒂𝒏 𝒄𝒐𝒔 𝒏𝒙 + 𝒃𝒏 π’”π’Šπ’ 𝒏𝒙]
Solution:
Choice A
Page | 74
82] Study Stationary Points of 𝒇(𝒙, π’š) = π’™πŸ + π’šπŸ − πŸπ’™ − πŸ”π’š + πŸπŸ’
Solution:
𝑓π‘₯ = 2π‘₯ − 2 = 0 , π‘₯ − 1 = 0 , then: π‘₯ = 1
𝑓𝑦 = 2𝑦 − 6 = 0 , 𝑦 − 3 = 0 , then: 𝑦 = 3
So, The Only Critical Point is (𝟏, πŸ‘)
𝑓π‘₯π‘₯ = 2 , 𝑓𝑦𝑦 = 2 , 𝑓π‘₯𝑦 = 0
2
D = 𝑓π‘₯π‘₯ (π‘Ž, 𝑏) ∗ 𝑓𝑦𝑦 (π‘Ž, 𝑏) − [𝑓π‘₯𝑦 (π‘Ž, 𝑏)] = 2 ∗ 2 − [0]2 = 4
At (𝟏, πŸ‘) → D > 0 & 𝑓π‘₯π‘₯ (1,3) = 2 > 0
Then: (𝟏, πŸ‘) is local minimum
Page | 75
83] Study Stationary Points of 𝒇(𝒙, π’š) = π’™πŸ’ + π’šπŸ’ − πŸ’π’™π’š + 𝟏
Solution:
𝑓π‘₯ = 4π‘₯ 3 − 4𝑦 = 0 βž” π‘₯ 3 − 𝑦 = 0 βž” π‘₯ 3 = 𝑦
𝑓𝑦 = 4𝑦 3 − 4π‘₯ = 0 βž” 𝑦 3 − π‘₯ = 0 βž” 𝑦 3 = π‘₯
By Solving those two equations:
𝑦 3 = π‘₯ βž” (π‘₯ 3 )3 = π‘₯ βž” π‘₯ 9 = π‘₯ βž” π‘₯ 9 − π‘₯ = 0 βž” π‘₯ (π‘₯ 8 − 1) = 0
π‘₯ = 0 ; π‘₯ 8 − 1 = 0 βž” (π‘₯ 4 − 1)(π‘₯ 4 + 1) βž” (π‘₯ 2 − 1)(π‘₯ 2 + 1)(π‘₯ 4 + 1)
βž” (π‘₯ − 1)(π‘₯ + 1)(π‘₯ 2 + 1)(π‘₯ 4 + 1)
Then: π‘₯ = 1 , π‘₯ = −1
π‘₯ = −1 , 0 , 1
π‘₯ 3 = 𝑦 βž” (𝑦 3 )3 = 𝑦 βž” 𝑦 9 = 𝑦 βž” 𝑦 9 − 𝑦 = 0 βž” 𝑦(𝑦 8 − 1) = 0
𝑦 = 0 ; 𝑦 8 − 1 = 0 βž” (𝑦 4 − 1)(𝑦 4 + 1) βž” (𝑦 2 − 1)(𝑦 2 + 1)(𝑦 4 + 1)
βž” (𝑦 − 1)(𝑦 + 1)(𝑦 2 + 1)(𝑦 4 + 1)
Then: 𝑦 = 1 , 𝑦 = −1
𝑦 = −1 , 0 , 1
The three critical points are : (−𝟏, −𝟏) & (𝟎, 𝟎) & (𝟏, 𝟏)
𝑓π‘₯π‘₯ = 12π‘₯ 2 , 𝑓𝑦𝑦 = 12𝑦 2 , 𝑓π‘₯𝑦 = −4
2
𝐷 = 𝑓π‘₯π‘₯ (π‘Ž, 𝑏) ∗ 𝑓𝑦𝑦 (π‘Ž, 𝑏) − [𝑓π‘₯𝑦 (π‘Ž, 𝑏)] = 12π‘₯ 2 ∗ 12𝑦 2 − [−4]2 = 0
144π‘₯ 2 𝑦 2 − 16 = 0
At (𝟎, 𝟎) Saddle Point βž” 𝐷 = −16
At (𝟏, 𝟏) βž” 𝐷 = 144 − 16 = 128
𝑓π‘₯π‘₯ at (1,1) = 12 > 0 βž” then it is a local minimum value
Page | 76
At (−𝟏, −𝟏) βž” 𝐷 = 144 − 16 = 128
𝑓π‘₯π‘₯ at (−1, −1) = 12 > 0 βž” then it is a local minimum value
84] Study Stationary Points of 𝒇(𝒙, π’š) = π’™πŸ + π’™π’š + π’šπŸ + π’š
Solution:
𝑓π‘₯ = 2π‘₯ + 𝑦 = 0 βž” 𝑦 = −2π‘₯
𝑓𝑦 = π‘₯ + 2𝑦 + 1 = 0 βž” π‘₯ + 2 ∗ (−2π‘₯ ) + 1 = 0 → π‘₯ − 4π‘₯ + 1 = 0 → −3π‘₯ +
1=0
Then: 1 = 3π‘₯ βž” π‘₯ =
1
3
1
−2
3
3
βž” 𝑦 = −2π‘₯ = −2 ∗ =
𝟏 −𝟐
The Critical Point is ( ,
πŸ‘
πŸ‘
)
𝑓π‘₯π‘₯ = 2 , 𝑓𝑦𝑦 = 2 , 𝑓π‘₯𝑦 = 1
2
Then: 𝐷 = 𝑓π‘₯π‘₯ (π‘Ž, 𝑏) ∗ 𝑓𝑦𝑦 (π‘Ž, 𝑏) − [𝑓π‘₯𝑦 (π‘Ž, 𝑏)] = 2 ∗ 2 − [1]2 = 3 > 0
1 −2
𝑓π‘₯π‘₯ (π‘Ž, 𝑏) = 2 > 0 βž” ( ,
3
1 −2
𝑓(π‘Ž, 𝑏) = 𝑓 ( ,
3
2
3
=
3
3
) is a local minimum point.
1 2
1
−2
3
3
3
)=( ) + ∗
−1
3
Then: The minimum Value is
Page | 77
−𝟏
πŸ‘
−2 2
−2
1
2
4
2
3
2
1
3
9
9
9
3
9
3
3
+( ) +( )= − + − = − = −
3
85] Study Stationary Points of 𝒇(𝒙, π’š) = π’™πŸ‘ + πŸ‘π’™πŸ π’š − πŸ”π’šπŸ − πŸ”π’™πŸ + 𝟐
Solution:
𝑓π‘₯ = 3π‘₯ 2 + 6π‘₯𝑦 − 12π‘₯ = 0 → 𝑓π‘₯ = π‘₯ 2 + 2π‘₯𝑦 − 4π‘₯ = 0
𝑓𝑦 = 3π‘₯ 2 − 12𝑦 βž” π‘₯ 2 − 4𝑦 = 0 , π‘₯ 2 = 4𝑦 , 𝑦 =
2
π‘₯ + 2π‘₯ ∗
π‘₯2
4
π‘₯2
4
− 4π‘₯ = 0 multiply by 𝟐
2π‘₯ 2 + π‘₯ 3 − 8π‘₯ = 0 , π‘₯ (π‘₯ 2 + 2π‘₯ − 8) = 0
Then: π‘₯ = 0 & π‘₯ 2 + 2π‘₯ − 8 = 0
π‘₯ 2 + 2π‘₯ − 8 = (π‘₯ − 2)(π‘₯ + 4) = 0 βž” π‘₯ = 2 , π‘₯ = −4
Then: π‘₯ = −4 , 0 , 2
𝑦=
π‘₯2
4
βž” at π‘₯ = −4 , 𝑦 = 4
At 𝒙 = 𝟎 , π’š = 𝟎
At 𝒙 = 𝟐 , π’š = 𝟏
Then the critical points are : (−4,4) , (0,0) , (2,1)
𝑓π‘₯π‘₯ = 6π‘₯ + 6𝑦 − 12 , 𝑓𝑦𝑦 = −12 , 𝑓π‘₯𝑦 = 6π‘₯
2
𝐷 = 𝑓π‘₯π‘₯ ∗ 𝑓𝑦𝑦 − (𝑓π‘₯𝑦 ) = (6π‘₯ + 6𝑦 − 12 ) ∗ (−12) − (6π‘₯)2 = −72π‘₯ − 72𝑦 + 144 −
36π‘₯ 2
𝐷(−4,4) = −72 ∗ −4 − 72 ∗ 4 + 144 − 36 ∗ (−4)2 = 0 + 144 + 36 ∗ 16 =
π‘£π‘Žπ‘™π‘’π‘’ < 0
𝑓π‘₯π‘₯ (−4,4) = 6 ∗ −4 + 6 ∗ 4 − 12 = −12 < 0
Then: (−4,4) is a saddle point
𝐷(0,0) = −72 ∗ 0 − 72 ∗ 0 + 144 − 36 ∗ (0)2 = 144 > 0
𝑓π‘₯π‘₯ (0,0) = 6 ∗ 0 + 6 ∗ 0 − 12 = −12 < 0
Then: (0,0) is a local maximum point
Page | 78
𝐷(2,1) = −72 ∗ 2 − 72 ∗ 1 + 144 − 36 ∗ (2)2 = π‘£π‘Žπ‘™π‘’π‘’ < 0
Then: (2,1) is a Saddle point
86] Study Stationary Points of 𝒇(𝒙, π’š) = 𝒆𝒙 𝐜𝐨𝐬 π’š
Solution:
𝑓π‘₯ = 𝑒 π‘₯ cos 𝑦 = 0 , 𝑦 = 90 , 270 && 𝑓𝑦 = −𝑒 π‘₯ sin 𝑦 = 0 , 𝑦 = 0 , 180
There is no critical points
87] If 𝒇(𝒙, π’š) = π’™πŸ + π’šπŸ − πŸπ’™ − πŸ”π’š , then has extreme value at :
A- (𝟎, 𝟎)
B- (𝟏, 𝟏)
C- (πŸ‘, 𝟏)
D- (𝟏, πŸ‘)
Solution:
𝑓π‘₯ = 2π‘₯ − 2 = 0 βž” 2(π‘₯ − 1) = 0 βž” π‘₯ = 1
𝑓𝑦 = 2𝑦 − 6 = 0 βž” 2(𝑦 − 3) = 0 βž” 𝑦 = 3
Then The critical point is : (1,3)
𝑓π‘₯π‘₯ = 2 , 𝑓𝑦𝑦 = 2 , 𝑓π‘₯𝑦 = 0
2
𝐷 = 𝑓π‘₯π‘₯ (π‘Ž, 𝑏) ∗ 𝑓𝑦𝑦 (π‘Ž, 𝑏) − [𝑓π‘₯𝑦 (π‘Ž, 𝑏)] = 2 ∗ 2 − 02 = 4 > 0
Then at (1,3) it is local minimum point
Choice D
Page | 79
88] Stationary points of the function 𝒖(𝒙, π’š) are obtained by :
A- 𝒖𝒙 = 𝟎
B- 𝒖𝒙 = 𝟎 and π’–π’š = 𝟎
C- π’–π’š = 𝟎
D- None of these
Solution:
Choice B
89] If 𝒇𝒙𝒙 (𝒂, 𝒃) = 𝒔 , π’‡π’šπ’š (𝒂, 𝒃) = 𝒕 , π’‡π’™π’š (𝒂, 𝒃) = 𝒓 , and βˆ†= 𝒔𝒕 − π’“πŸ
then 𝒇(𝒂, 𝒃) is the maximum at
A- βˆ†> 𝟎 and 𝒓 < 𝟎
B- βˆ†> 𝟎 and 𝒔 < 𝟎
C- βˆ†< 𝟎 and 𝒔 < 𝟎
D- None of these
Solution:
Suppose 𝐷 = βˆ†= 𝑓π‘₯π‘₯ (π‘Ž, 𝑏) ∗ 𝑓𝑦𝑦 (π‘Ž, 𝑏) − [𝑓π‘₯𝑦 (π‘Ž, 𝑏)]
2
= 𝑠𝑑 − π‘Ÿ 2
It is maximum at 𝐷 > 0 , 𝑓π‘₯π‘₯ (π‘Ž, 𝑏) = 𝑠 < 0
Choice B
90] If 𝒇(𝒙, π’š) = π’™πŸ + π’šπŸ , then has extreme value at :
A- (𝟎, 𝟎)
B- (𝟏, 𝟏)
C- (πŸ‘, 𝟏)
D- (𝟏, πŸ‘)
Solution:
𝑓π‘₯ = 2π‘₯ = 0 βž” π‘₯ = 0
𝑓𝑦 = 2𝑦 = 0 βž” 𝑦 = 0
Then The critical point is : (0,0)
Page | 80
Choice A
91] If 𝒇𝒙𝒙 (𝒂, 𝒃) = 𝒔 , π’‡π’šπ’š (𝒂, 𝒃) = 𝒕 , π’‡π’™π’š (𝒂, 𝒃) = 𝒓 , and βˆ†= 𝒔𝒕 − π’“πŸ
then 𝒇(𝒂, 𝒃) is the minimum at
A- βˆ†> 𝟎 and 𝒓 < 𝟎
B- βˆ†> 𝟎 and 𝒔 < 𝟎
C- βˆ†< 𝟎 and 𝒔 < 𝟎
D- None of these
Solution:
Suppose 𝐷 = βˆ†= 𝑓π‘₯π‘₯ (π‘Ž, 𝑏) ∗ 𝑓𝑦𝑦 (π‘Ž, 𝑏) − [𝑓π‘₯𝑦 (π‘Ž, 𝑏)]
= 𝑠𝑑 − π‘Ÿ 2
It is minimum at 𝐷 > 0 , 𝑓π‘₯π‘₯ (π‘Ž, 𝑏) = 𝑠 > 0
Choice D
Page | 81
2
92] If 𝒇(𝒙, π’š) = 𝒆𝒙+π’š , then find Taylor’s expansion at the point
(𝟎, 𝟎) for 𝒏 = πŸ‘
𝟏
𝟏
𝟏
𝟏
A- 𝟏 + (𝒙 + π’š) + 𝟐! (π’™πŸ + π’šπŸ + πŸπ’™π’š) + πŸ‘! [π’™πŸ‘ + πŸ‘π’™πŸ π’š + πŸ‘π’™π’šπŸ +
π’šπŸ‘ ]π’†πœ½(𝒙+π’š)
B- 𝟏 + (𝒙 + π’š) + 𝟐! (π’™πŸ + π’šπŸ + πŸπ’™π’š) + πŸ‘! [π’™πŸ‘ + πŸ‘π’™πŸ π’š + πŸ‘π’™π’šπŸ + π’šπŸ‘ ]
𝟏
C- 𝟏 + (𝒙 + π’š) + 𝟐! (π’™πŸ + π’šπŸ + πŸπ’™π’š) + [π’™πŸ‘ + πŸ‘π’™πŸ π’š + πŸ‘π’™π’šπŸ +
π’šπŸ‘ ]π’†πœ½(𝒙+π’š)
D- None of these
Solution:
𝑓(π‘₯, 𝑦) = 𝑓(π‘Ž, 𝑏) + [(π‘₯ − π‘Ž)
𝑏)
πœ•
πœ•π‘₯
+ (𝑦 − 𝑏)
πœ• 1
πœ•π‘¦
1
πœ•
] 𝑓(π‘Ž, 𝑏) + 2! [(π‘₯ − π‘Ž) πœ•π‘₯ + (𝑦 −
πœ• 2
πœ•π‘¦
] 𝑓(π‘Ž, 𝑏) + 𝑅3
At (𝒂, 𝒃) = (0,0)
πœ•
πœ• 1
1
πœ•
πœ• 2
= 𝑓(0,0) + [(π‘₯ − π‘Ž) + (𝑦 − 𝑏) ] 𝑓(0,0) + [(π‘₯ − π‘Ž) + (𝑦 − 𝑏) ] 𝑓(0,0) + 𝑅3
πœ•π‘₯
πœ•π‘¦
2!
πœ•π‘₯
πœ•π‘¦
𝑓(0,0) = 𝑒 0+0 = 𝑒 0 = 1
πœ•
πœ•π‘₯
=
πœ•
πœ•π‘¦
=
[(π‘₯ − π‘Ž)
πœ•2
πœ•π‘₯ 2
πœ•
πœ•π‘₯
=
πœ•2
πœ•π‘¦ 2
= 𝑒 π‘₯+𝑦 βž” at (0,0) 𝑒 π‘₯+𝑦 = 1
+ (𝑦 − 𝑏)
πœ• 1
πœ•π‘¦
] 𝑓(0,0) = [(π‘₯ − 0)
πœ•
πœ• 1
( 𝑦 − 0) ]
+
πœ•π‘₯
πœ•π‘¦
= ((π‘₯ − 0) ∗ 1 + (𝑦 − 0) ∗ 1) = (𝒙 + π’š)
1
πœ• 2
πœ•
1
πœ• 2
πœ•
[(π‘₯ − π‘Ž) πœ•π‘₯ + (𝑦 − 𝑏) πœ•π‘¦] 𝑓(0,0) = 2! [(π‘₯ − 0) πœ•π‘₯ + (𝑦 − 0) πœ•π‘¦]
2!
=
𝑅3 =
1
3!
[(π‘₯ − π‘Ž)
At (𝒂, 𝒃) = (0,0)
Page | 82
πœ•
πœ•π‘₯
+ (𝑦 − 𝑏)
1
2!
πœ• 3
πœ•π‘¦
[(π‘₯) ∗ 1 + (𝑦) ∗ 1]2 =
𝟏
𝟐!
(π’™πŸ + π’šπŸ + πŸπ’™π’š)
] 𝑓 ((π‘Ž + πœƒ(π‘₯ − π‘Ž)), (𝑏 + πœƒ(𝑦 − 𝑏)))
1
Then: 𝑅3 =
1
=
3!
1
=
3!
3!
πœ•
[(π‘₯ − 0)
[(π‘₯)
[(π‘₯)
πœ•
πœ•π‘₯
πœ•
πœ•π‘₯
πœ•π‘₯
+ (𝑦)
+ (𝑦)
+ (𝑦 − 0)
πœ•π‘¦
] 𝑓 ((0 + πœƒ(π‘₯ − 0)), (0 + πœƒ(𝑦 − 0)))
πœ• 3
πœ•π‘¦
] 𝑓(πœƒ(π‘₯), πœƒ(𝑦))
πœ• 2
πœ•π‘¦
] [(π‘₯)
πœ• 2
1
πœ• 3
πœ•
πœ•π‘₯
+ (𝑦)
πœ•
πœ•
πœ•π‘¦
]
πœ• 2
πœ•
πœ•
πœ•
([(π‘₯) πœ•π‘₯] + 2 [((π‘₯) πœ•π‘₯) ((𝑦) πœ•π‘¦)] + [(𝑦) πœ•π‘¦] ) ∗ [(π‘₯) πœ•π‘₯ + (𝑦) πœ•π‘¦]
3!
=
=
π‘₯2
1
3!
πœ•2
πœ•
πœ•π‘₯
πœ•π‘₯
2 ∗π‘₯
+ π‘₯2
πœ•2
πœ•π‘₯ 2
∗𝑦
πœ•
πœ•π‘¦
+ 2 [((π‘₯)
+𝑦 2
[
= π‘₯3
βž”
πœ•3
πœ•π‘₯ 3
πœ•3
πœ•3
πœ•π‘₯
πœ•π‘₯ 2 πœ•π‘¦
= 𝑓π‘₯π‘₯π‘₯ = 𝑒 π‘₯+𝑦 ,
πœ•3
𝑒 π‘₯+𝑦
+ π‘₯ 2𝑦
3
πœ•π‘¦ 2 πœ•π‘₯
πœ•3
πœ•π‘₯ 2 πœ•π‘¦
= 𝑓𝑦𝑦π‘₯ = 𝑒 π‘₯+𝑦 ,
At (𝟎, 𝟎) , then
Then: π‘₯ 3
+ 2(π‘₯ 2 𝑦)
πœ•3
πœ•π‘₯ 3
=
πœ•3
πœ•π‘₯ 2 πœ•π‘¦
πœ•3
πœ•3
πœ•π‘₯
πœ•π‘₯ 2 πœ•π‘¦
+ π‘₯ 2𝑦
3
=
πœ•
πœ•π‘₯
πœ•
πœ•2
πœ•π‘¦
2 ∗π‘₯
πœ•3
πœ•π‘₯πœ•π‘¦πœ•π‘₯
πœ•
πœ•π‘₯
+ 𝑦2
πœ•π‘¦ 3
πœ•2
πœ•π‘¦ 2
+ 2(π‘₯𝑦 2 )
πœ•3
= 𝑓π‘₯π‘₯𝑦 = 𝑒 π‘₯+𝑦 ,
πœ•3
πœ•
πœ•
πœ•
πœ•π‘₯πœ•π‘¦ 2
πœ•
∗𝑦
πœ•3
πœ•π‘₯πœ•π‘¦
]
πœ•π‘¦
+ 𝑦2π‘₯
2
πœ•3
πœ•π‘¦ 2 πœ•π‘₯
= 𝑓π‘₯𝑦𝑦 = 𝑒 π‘₯+𝑦 ,
+ 𝑦3
πœ•3
πœ•π‘₯πœ•π‘¦πœ•π‘₯
πœ•3
πœ•π‘¦ 3
= 𝑓π‘₯𝑦π‘₯ =
= 𝑓𝑦𝑦𝑦 = 𝑒 π‘₯+𝑦
πœ•3
πœ•π‘₯πœ•π‘¦ 2
+ 2(π‘₯ 2 𝑦)
=
πœ•3
πœ•π‘₯πœ•π‘¦πœ•π‘₯
πœ•3
πœ•π‘₯πœ•π‘¦πœ•π‘₯
=
πœ•3
πœ•π‘¦ 2 πœ•π‘₯
+ 2(π‘₯𝑦 2 )
=
πœ•3
πœ•π‘¦ 3
πœ•3
πœ•π‘₯πœ•π‘¦
= 𝑒 0+0 = 1
+ 𝑦2π‘₯
2
πœ•3
πœ•π‘¦ 2 πœ•π‘₯
+ 𝑦3
πœ•3
πœ•π‘¦ 3
= π‘₯ 3 (𝑒 π‘₯+𝑦 ) + π‘₯ 2 𝑦(𝑒 π‘₯+𝑦 ) + 2(π‘₯ 2 𝑦)(𝑒 π‘₯+𝑦 ) + 2(π‘₯𝑦 2 )(𝑒 π‘₯+𝑦 ) + 𝑦 2 π‘₯(𝑒 π‘₯+𝑦 ) +
𝑦 3 (𝑒 π‘₯+𝑦 )
= π‘₯ 3 (𝑒 π‘₯+𝑦 ) + 3(π‘₯ 2 𝑦)(𝑒 π‘₯+𝑦 ) + 3(π‘₯𝑦 2 )(𝑒 π‘₯+𝑦 ) + 𝑦 3 (𝑒 π‘₯+𝑦 )
= 𝑒 π‘₯+𝑦 (π‘₯ 3 + 3π‘₯ 2 𝑦 + 3π‘₯𝑦 2 + 𝑦 3 ) = 1 ∗ (π‘₯ 3 + 3π‘₯ 2 𝑦 + 3π‘₯𝑦 2 + 𝑦 3 )
Then: 𝑅3 =
=
1
3!
1
3!
[(π‘₯)
πœ•
πœ•π‘₯
+ (𝑦)
πœ• 3
πœ•π‘¦
] 𝑓(πœƒ(π‘₯), πœƒ(𝑦))
[π‘₯ 3 + 3π‘₯ 2 𝑦 + 3π‘₯𝑦 2 + 𝑦 3 ]𝑓 (πœƒ(π‘₯), πœƒ(𝑦))
βž” 𝑓(πœƒ(π‘₯), πœƒ(𝑦)) = 𝑒 πœƒπ‘₯+πœƒπ‘¦ = 𝑒 πœƒ(π‘₯+𝑦)
1
3!
[π‘₯ 3 + 3π‘₯ 2 𝑦 + 3π‘₯𝑦 2 + 𝑦 3 ]𝑓(πœƒ(π‘₯), πœƒ(𝑦)) =
Page | 83
πœ•
) ((𝑦) πœ•π‘¦)] ∗ π‘₯ πœ•π‘₯ + 2 [((π‘₯) πœ•π‘₯) ((𝑦) πœ•π‘¦)] ∗ 𝑦 πœ•π‘¦
𝟏
πŸ‘!
[π’™πŸ‘ + πŸ‘π’™πŸ π’š + πŸ‘π’™π’šπŸ + π’šπŸ‘ ]π’†πœ½(𝒙+π’š)
𝑓(π‘₯, 𝑦) = 𝑓(π‘Ž, 𝑏) + [(π‘₯ − π‘Ž)
𝑏)
πœ•
πœ•π‘₯
+ (𝑦 − 𝑏)
πœ• 1
πœ•π‘¦
1
πœ•
] 𝑓(π‘Ž, 𝑏) + 2! [(π‘₯ − π‘Ž) πœ•π‘₯ + (𝑦 −
πœ• 2
πœ•π‘¦
] 𝑓(π‘Ž, 𝑏) + 𝑅3
𝟏
= 𝟏 + (𝒙 + π’š) +
𝟐!
(π’™πŸ + π’šπŸ + πŸπ’™π’š) +
𝟏
[π’™πŸ‘ + πŸ‘π’™πŸ π’š + πŸ‘π’™π’šπŸ + π’šπŸ‘ ]π’†πœ½(𝒙+π’š)
πŸ‘!
Choice A
93] If 𝒇(𝒙, π’š) = 𝐜𝐨𝐬(𝒙 + π’š) , then find Taylor’s expansion at the
point (𝟎, 𝟎) for 𝒏 = πŸ‘
𝟏
𝟏
A- −𝟏 − 𝟐! (𝒙 + π’š)𝟐 + πŸ‘! (𝒙 + π’š)πŸ‘ 𝐬𝐒𝐧 𝜽(𝒙 + π’š)
𝟏
𝟏
B- 𝟏 − 𝟐! (𝒙 + π’š)𝟐 − πŸ‘! (𝒙 + π’š)πŸ‘ 𝐬𝐒𝐧 𝜽(𝒙 + π’š)
C- 𝟏 −
(𝒙+π’š)𝟐
𝟐!
+
(𝒙+π’š)πŸ‘
𝐬𝐒𝐧 𝜽(𝒙 + π’š)
πŸ‘!
D- None of these
Solution:
𝑓(π‘₯, 𝑦) = 𝑓(π‘Ž, 𝑏) + [(π‘₯ − π‘Ž)
𝑏)
πœ•
πœ•π‘₯
+ (𝑦 − 𝑏)
πœ• 1
1
πœ•
] 𝑓(π‘Ž, 𝑏) + 2! [(π‘₯ − π‘Ž) πœ•π‘₯ + (𝑦 −
πœ•π‘¦
πœ• 2
πœ•π‘¦
] 𝑓(π‘Ž, 𝑏) + 𝑅3
At (𝒂, 𝒃) = (0,0)
= 𝑓(0,0) + [(π‘₯ − π‘Ž)
πœ•
πœ•π‘₯
+ (𝑦 − 𝑏)
πœ• 1
1
πœ• 2
πœ•
] 𝑓(0,0) + 2! [(π‘₯ − π‘Ž) πœ•π‘₯ + (𝑦 − 𝑏) πœ•π‘¦] 𝑓(0,0) + 𝑅3
πœ•π‘¦
𝑓(0,0) = cos(0 + 0) = cos(0) = 1
πœ•
πœ•π‘₯
= − sin(π‘₯ + 𝑦) ,
πœ•2
πœ•π‘₯πœ•π‘¦
πœ•
πœ•π‘¦
= − sin(π‘₯ + 𝑦) ,
πœ•2
πœ•π‘₯ 2
= − cos(π‘₯ + 𝑦) ,
πœ•2
πœ•π‘¦ 2
= − cos(π‘₯ + 𝑦) ,
= − cos(π‘₯ + 𝑦)
At (𝟎, 𝟎) βž”
[(π‘₯ − π‘Ž)
Page | 84
πœ•
πœ•π‘₯
πœ•
πœ•π‘₯
=
πœ•
πœ•π‘¦
=0 ,
+ (𝑦 − 𝑏)
πœ• 1
πœ•π‘¦
πœ•2
πœ•π‘₯ 2
=
πœ•2
πœ•π‘¦ 2
=
πœ•2
πœ•π‘₯πœ•π‘¦
= −1
] 𝑓(0,0) = [(π‘₯ − 0) ∗ 0 + (𝑦 − 0) ∗ 0]1 = 𝟎
1
2!
[(π‘₯ − π‘Ž)
[ (𝑦 − 0)
πœ•
πœ•π‘₯
πœ• 2
+ (𝑦 − 𝑏 )
πœ•π‘¦
πœ•π‘¦
2
2 πœ•
(π‘₯ 2
2!
πœ•π‘₯
1
1
πœ•
πœ•π‘₯
πœ•π‘₯
] + 2 [((π‘₯ − 0)
) (( 𝑦 − 0 )
πœ•
πœ•π‘¦
)] +
1
Then: 𝑅3 =
1
3!
1
3!
3!
πœ•
[(π‘₯ − 0)
1
[(π‘₯)
[(π‘₯)
πœ•
πœ•π‘₯
πœ•
πœ•π‘₯
+ (𝑦)
+ (𝑦)
πœ•π‘₯πœ•π‘¦
πœ•2
] + 𝑦2
πœ•π‘¦2
)
𝟏
2!
𝟐!
πœ• 3
πœ•π‘¦
] 𝑓 ((0 + πœƒ(π‘₯ − 0)), (0 + πœƒ(𝑦 − 0)))
πœ• 3
πœ•π‘¦
] 𝑓(πœƒ(π‘₯), πœƒ(𝑦))
πœ• 2
πœ•π‘¦
] [(π‘₯)
πœ• 2
1
πœ•2
(−π‘₯ 2 − 2π‘₯𝑦 − 𝑦 2 ) = − (π’™πŸ + πŸπ’™π’š + π’šπŸ )
+ (𝑦 − 0)
πœ•π‘₯
+ 2 [π‘₯𝑦
(π‘₯2 ∗ −1 + 2[π‘₯𝑦 ∗ −1] + 𝑦2 ∗ −1)
2!
=
=
πœ• 2
] )
=
=
2!
([(π‘₯ − 0)
πœ• 2
=
=
1
] 𝑓 (0,0) =
πœ•
πœ•π‘₯
+ (𝑦)
πœ•
πœ•
πœ•π‘¦
]
πœ• 2
πœ•
πœ•
πœ•
([(π‘₯) πœ•π‘₯] + 2 [((π‘₯) πœ•π‘₯) ((𝑦) πœ•π‘¦)] + [(𝑦) πœ•π‘¦] ) ∗ [(π‘₯) πœ•π‘₯ + (𝑦) πœ•π‘¦]
3!
=
π‘₯2
1
3!
πœ•2
πœ•π‘₯
2 ∗π‘₯
πœ•
πœ•π‘₯
+ π‘₯2
πœ•2
πœ•π‘₯ 2
∗𝑦
πœ•
πœ•π‘¦
+𝑦 2
[
= π‘₯3
βž”
+ 2 [((π‘₯)
πœ•3
πœ•π‘₯ 3
πœ•3
πœ•π‘₯πœ•π‘¦πœ•π‘₯
πœ•3
πœ•3
πœ•π‘₯
πœ•π‘₯ 2 πœ•π‘¦
+ π‘₯ 2𝑦
3
+ 2(π‘₯ 2 𝑦)
= 𝑓π‘₯π‘₯π‘₯ = sin(π‘₯ + 𝑦) ,
= 𝑓π‘₯𝑦π‘₯ = sin(π‘₯ + 𝑦)
At ((𝜽(𝒙), 𝜽(π’š))) , then
πœ•3
πœ•π‘₯ 3
πœ•3
πœ•π‘₯ 2 πœ•π‘¦
πœ•3
πœ•π‘¦ 2 πœ•π‘₯
=
πœ•
πœ•
πœ•
πœ•2
πœ•
πœ•π‘¦
πœ•π‘₯
2 ∗π‘₯
πœ•3
πœ•π‘₯πœ•π‘¦πœ•π‘₯
+ 𝑦2
πœ•2
πœ•π‘¦ 2
∗𝑦
πœ•3
+ 2(π‘₯𝑦 2 )
πœ•π‘₯πœ•π‘¦
= 𝑓π‘₯π‘₯𝑦 = sin(π‘₯ + 𝑦) ,
= 𝑓𝑦𝑦π‘₯ = sin(π‘₯ + 𝑦) ,
πœ•3
πœ•π‘₯ 2 πœ•π‘¦
=
πœ•
πœ•
πœ•3
πœ•π‘₯πœ•π‘¦ 2
=
πœ•3
πœ•π‘₯πœ•π‘¦πœ•π‘₯
=
πœ•
]
πœ•π‘¦
+ 𝑦2π‘₯
2
πœ•3
πœ•π‘₯πœ•π‘¦ 2
πœ•3
πœ•π‘¦ 3
πœ•3
πœ•π‘¦ 2 πœ•π‘₯
+ 𝑦3
πœ•3
πœ•π‘¦ 3
= 𝑓π‘₯𝑦𝑦 = sin(π‘₯ + 𝑦) ,
= 𝑓𝑦𝑦𝑦 = sin(π‘₯ + 𝑦)
πœ•3
πœ•π‘¦ 2 πœ•π‘₯
=
πœ•3
πœ•π‘¦ 3
= sin(πœƒ(π‘₯) + πœƒ(𝑦)) = sin πœƒ(π‘₯ + 𝑦)
Then: π‘₯ 3
πœ•3
πœ•3
πœ•π‘₯
πœ•π‘₯ 2 πœ•π‘¦
+ π‘₯ 2𝑦
3
+ 2(π‘₯ 2 𝑦)
πœ•3
πœ•π‘₯πœ•π‘¦πœ•π‘₯
+ 2(π‘₯𝑦 2 )
πœ•3
πœ•π‘₯πœ•π‘¦
+ 𝑦2π‘₯
2
πœ•3
πœ•π‘¦ 2 πœ•π‘₯
= π‘₯ 3 ∗ sin πœƒ(π‘₯ + 𝑦) + π‘₯ 2 𝑦 ∗ sin πœƒ(π‘₯ + 𝑦) + 2(π‘₯ 2 𝑦) ∗ sin πœƒ(π‘₯ + 𝑦)
+2(π‘₯𝑦 2 ) ∗ sin πœƒ(π‘₯ + 𝑦) + 𝑦 2 π‘₯ ∗ sin πœƒ(π‘₯ + 𝑦) + 𝑦 3 ∗ sin πœƒ(π‘₯ + 𝑦)
= sin πœƒ(π‘₯ + 𝑦) [π‘₯ 3 + 3π‘₯ 2 𝑦 + 3π‘₯𝑦 2 + 𝑦 3 ]
Page | 85
πœ•
) ((𝑦) πœ•π‘¦)] ∗ π‘₯ πœ•π‘₯ + 2 [((π‘₯) πœ•π‘₯) ((𝑦) πœ•π‘¦)] ∗ 𝑦 πœ•π‘¦
πœ•π‘₯
+ 𝑦3
πœ•3
πœ•π‘¦ 3
Then: 𝑅3 =
=
𝟏
πŸ‘!
1
3!
[(π‘₯)
πœ•
πœ•π‘₯
+ (𝑦)
πœ• 3
πœ•π‘¦
[π’™πŸ‘ + πŸ‘π’™πŸ π’š + πŸ‘π’™π’šπŸ + π’šπŸ‘ ] 𝐬𝐒𝐧 𝜽(𝒙 + π’š)
𝑓(π‘₯, 𝑦) = 𝑓(π‘Ž, 𝑏) + [(π‘₯ − π‘Ž)
𝑏)
] 𝑓(πœƒ(π‘₯), πœƒ(𝑦))
πœ•
πœ•π‘₯
+ (𝑦 − 𝑏)
πœ• 1
πœ•π‘¦
1
πœ•
] 𝑓(π‘Ž, 𝑏) + 2! [(π‘₯ − π‘Ž) πœ•π‘₯ + (𝑦 −
πœ• 2
πœ•π‘¦
] 𝑓(π‘Ž, 𝑏) + 𝑅3
1
1
= 1 + 0 + (− (π‘₯ 2 + 2π‘₯𝑦 + 𝑦 2 )) + [π‘₯3 + 3π‘₯2 𝑦 + 3π‘₯𝑦2 + 𝑦3 ] sin πœƒ(π‘₯ + 𝑦)
2!
3!
𝟏
= 𝟏 − (π’™πŸ + πŸπ’™π’š + π’šπŸ ) +
𝟐!
𝟏
= 𝟏 − (𝒙 + π’š )𝟐 +
𝟐!
𝟏
[π’™πŸ‘
πŸ‘!
+ πŸ‘π’™πŸ π’š + πŸ‘π’™π’šπŸ + π’šπŸ‘ ] 𝐬𝐒𝐧 𝜽(𝒙 + π’š)
𝟏
(𝒙 + π’š)πŸ‘ 𝐬𝐒𝐧 𝜽(𝒙 + π’š)
πŸ‘!
Choice C
94] Expand 𝒇(𝒙, π’š) = π’™πŸ + π’™π’š + π’šπŸ in powers of (𝒙 − 𝟐) , (π’š − πŸ‘)
A- πŸ•π’™ + πŸ—π’š + (𝒙 − 𝟐)𝟐 + (𝒙 − 𝟐)(π’š − πŸ‘) + (π’š − πŸ‘)𝟐
B- −πŸπŸ— + πŸ•π’™ + πŸ–π’š + (𝒙 − 𝟐)𝟐 + (𝒙 − 𝟐)(π’š − πŸ‘) + (π’š − πŸ‘)𝟐
C- πŸπŸ— + πŸ•π’™ + πŸ—π’š + (𝒙 − 𝟐)𝟐 + (𝒙 − 𝟐)(π’š − πŸ‘) + (π’š − πŸ‘)𝟐
D- None of these
Solution:
π‘₯−2=0βž”π‘₯ =2
𝑦−3=0βž”π‘¦ =3
𝑓(2,3) = 19
Then point is (𝟐, πŸ‘)
𝑓π‘₯ = 2π‘₯ + 𝑦 , 𝑓π‘₯ (2,3) = 7
𝑓𝑦 = π‘₯ + 2𝑦 , 𝑓π‘₯ (2,3) = 8
𝑓π‘₯π‘₯ = 2 , 𝑓π‘₯ (2,3) = 2
Page | 86
𝑓𝑦𝑦 = 2 , 𝑓π‘₯ (2,3) = 2
𝑓π‘₯𝑦 = 1 , 𝑓π‘₯ (2,3) = 1
𝑓𝑦π‘₯ = 1 , 𝑓π‘₯ (2,3) = 1
𝑓π‘₯π‘₯π‘₯ = 𝑓𝑦𝑦𝑦 = 𝑓π‘₯𝑦𝑦 = 𝑓𝑦𝑦π‘₯ = 0
All The third higher order partial derivatives is Zero
Then 𝒏 = 𝟐
𝑓(π‘₯, 𝑦) = 𝑓(2,3) + [(π‘₯ − π‘Ž)
πœ•
πœ•π‘₯
+ (𝑦 − 𝑏 )
πœ• 1
πœ•π‘¦
1
πœ•
2!
πœ•π‘₯
] 𝑓 (2,3) + [(π‘₯ − π‘Ž)
+
πœ• 2
(𝑦 − 𝑏 )
πœ•π‘¦
] 𝑓(2,3)
𝑓(2,3) = 19
πœ•
πœ•
= 2π‘₯ + 𝑦 βž” at (𝟐, πŸ‘) , 2 ∗ 2 + 3 = 7
πœ•π‘₯
πœ•2
πœ•π‘₯ 2
πœ•2
= 2 βž” at (𝟐, πŸ‘) , equals 2
πœ•2
πœ•π‘₯πœ•π‘¦
πœ•π‘¦
πœ•π‘¦ 2
= π‘₯ + 2𝑦 βž” at (𝟐, πŸ‘) , 2 + 2 ∗ 3 = 8
= 2 βž” at (𝟐, πŸ‘) , equals 2
= 1 βž” at (𝟐, πŸ‘) , equals 1
[(π‘₯ − π‘Ž)
πœ•
πœ•π‘₯
+ (𝑦 − 𝑏)
πœ• 1
πœ•π‘¦
] 𝑓(2,3) = [(π‘₯ − 2) ∗ 7 + (𝑦 − 3) ∗ 8]1 = 7π‘₯ − 14 + 8𝑦 − 24
= 7π‘₯ + 8𝑦 − 38
1
2!
[(π‘₯ − π‘Ž)
[ (𝑦 − 3)
πœ•
πœ•π‘₯
+ (𝑦 − 𝑏 )
πœ• 2
πœ•π‘¦
] 𝑓(2,3) =
1
2!
([(π‘₯ − 2)
πœ• 2
πœ•
πœ•π‘₯
πœ•π‘₯
] + 2 [((π‘₯ − 2)
) (( 𝑦 − 3 )
)] +
πœ• 2
πœ•π‘¦
] )
=
=
1
2!
1
2!
((π‘₯ − 2)2
πœ•2
πœ•π‘₯2
+ 2 [(π‘₯ − 2)(𝑦 − 3)
πœ•2
] + (𝑦
πœ•π‘₯πœ•π‘¦
− 3)2
πœ•2
)
πœ•π‘¦2
((π‘₯ − 2)2 ∗ 2 + 2[(π‘₯ − 2)(𝑦 − 3) ∗ 1] + (𝑦 − 3)2 ∗ 2)
= (π‘₯ − 2)2 + (π‘₯ − 2)(𝑦 − 3) + (𝑦 − 3)2
Page | 87
πœ•
πœ•π‘¦
Then: 𝑓(2,3) + [(π‘₯ − π‘Ž)
πœ•
πœ•π‘₯
+ (𝑦 − 𝑏)
πœ• 1
πœ•π‘¦
1
πœ•
2!
πœ•π‘₯
] 𝑓(2,3) + [(π‘₯ − π‘Ž)
+ (𝑦 − 𝑏)
πœ• 2
πœ•π‘¦
] 𝑓(2,3)
= 19 + 7π‘₯ + 8𝑦 − 38 + (π‘₯ − 2)2 + (π‘₯ − 2)(𝑦 − 3) + (𝑦 − 3)2
= −πŸπŸ— + πŸ•π’™ + πŸ–π’š + (𝒙 − 𝟐)𝟐 + (𝒙 − 𝟐)(π’š − πŸ‘) + (π’š − πŸ‘)𝟐
Choice B
95] Find the first and second degree Taylor polynomial of 𝒇(𝒙, π’š) =
𝟐
𝟐
𝒆−𝒙 −π’š at (𝟎, 𝟎)
A- 𝟏 − π’™πŸ − π’šπŸ‘
B- 𝟏 − π’™πŸ − π’šπŸ
C- 𝟏𝟏 − π’™πŸ + π’šπŸ
D- None of these
Solution:
𝑓(π‘₯, 𝑦) = 𝑓(0,0) + [(π‘₯ − π‘Ž)
(𝑦 − 𝑏 )
πœ•π‘₯
πœ•
πœ•π‘¦
πœ•π‘₯
+ (𝑦 − 𝑏 )
πœ•π‘¦
2 −02
∗ −2π‘₯ βž” at (𝟎, 𝟎) , 𝑒 −0
= 𝑒 −π‘₯
2 −𝑦 2
∗ −2𝑦 βž” at (𝟎, 𝟎) , 𝑒 −0
= (𝑒 −π‘₯
2 −𝑦 2
πœ•π‘¦ 2
= (𝑒 −π‘₯
2 −𝑦2
πœ•π‘₯πœ•π‘¦
= 𝑒 −π‘₯
Page | 88
2!
πœ•π‘₯
+
2 −𝑦2
2 −02
− 2𝑒 −0
2 −02
− 2𝑒 −0
∗ −2 ∗ 0 = 0
2 −02
2 −𝑦 2
2 −02
∗ −2𝑦 ∗ −2𝑦) + (𝑒 −π‘₯
At (𝟎, 𝟎) , 4 ∗ 02 ∗ 𝑒 −0
πœ•2
2 −02
∗ −2π‘₯ ∗ −2π‘₯) + (𝑒 −π‘₯
At (𝟎, 𝟎) , 4 ∗ 02 ∗ 𝑒 −0
πœ•2
πœ•
=1
2 −𝑦 2
πœ•π‘₯ 2
πœ•π‘¦
1
] 𝑓 (0,0) + [(π‘₯ − π‘Ž)
] 𝑓(0,0)
= 𝑒 −π‘₯
πœ•2
πœ• 1
πœ• 2
𝑓(0,0) = 𝑒 −0
πœ•
πœ•
∗ −2) = 4π‘₯ 2 𝑒 −π‘₯
2 −𝑦2
− 2𝑒 −π‘₯
2 −𝑦 2
2 −𝑦2
− 2𝑒 −π‘₯
= 0 − 2 = −2
2 −𝑦 2
2 −02
∗ −2 ∗ 0 = 0
∗ −2) = 4𝑦 2 𝑒 −π‘₯
= 0 − 2 = −2
∗ −2π‘₯ ∗ −2𝑦 βž” at (0,0) , 𝑒 −π‘₯
2 −𝑦 2
∗ −2π‘₯ ∗ −2𝑦 = 0
2 −𝑦 2
[ (π‘₯ − π‘Ž )
1
2!
πœ•
πœ•π‘₯
[(π‘₯ − π‘Ž)
[ (𝑦 − 0)
πœ•
πœ•π‘₯
+ (𝑦 − 𝑏 )
+ (𝑦 − 𝑏 )
πœ• 1
πœ•π‘¦
] 𝑓 (0,0) = [(π‘₯ − 0) ∗ 0 + (𝑦 − 0) ∗ 0]1 = 0
πœ• 2
πœ•π‘¦
] 𝑓(0,0) =
2!
([(π‘₯ − 0)
πœ• 2
πœ•
πœ•π‘₯
πœ•π‘₯
] + 2 [((π‘₯ − 0)
) (( 𝑦 − 0 )
πœ•
πœ•π‘¦
)] +
πœ• 2
πœ•π‘¦
] )
=
=
=
Then: 𝑓(0,0) + [(π‘₯ − π‘Ž)
𝑏)
1
πœ•
πœ•π‘₯
1
2!
1
2!
1
2!
(π‘₯ 2
πœ•2
πœ•2
πœ•π‘₯
πœ•π‘₯πœ•π‘¦
+ 2 [π‘₯𝑦
2
] + 𝑦2
πœ•2
πœ•π‘¦ 2
)
(π‘₯ 2 ∗ −2 + 2[π‘₯𝑦 ∗ 0] + 𝑦 2 ∗ −2)
(−2π‘₯ 2 − 2𝑦 2 ) = −π‘₯ 2 − 𝑦 2
+ (𝑦 − 𝑏 )
πœ• 1
πœ•π‘¦
1
πœ•
2!
πœ•π‘₯
] 𝑓 (0,0) + [(π‘₯ − π‘Ž)
+ (𝑦 −
πœ• 2
πœ•π‘¦
] 𝑓(0,0)
= 1 + 0 + (−π‘₯ 2 − 𝑦 2 )
= 𝟏 − π’™πŸ − π’šπŸ
Choice B
96] Find the first and second degree Taylor polynomial of 𝒇(𝒙, π’š) =
π’™π’†π’š at (𝟏, 𝟎)
𝟏
A- 𝒙 − π’š + 𝟐! (πŸπ’™π’š − πŸπ’š + π’šπŸ )
𝟏
B- 𝒙 + π’š + 𝟐 (πŸπ’™π’š − πŸπ’š + π’šπŸ )
C- 𝒙 + π’š +
𝟏
πŸ‘!
(πŸπ’™π’š − πŸπ’š + π’šπŸ )
D- None of these
Solution:
𝑓(π‘₯, 𝑦) = 𝑓(1,0) + [(π‘₯ − π‘Ž)
(𝑦 − 𝑏 )
Page | 89
πœ• 2
πœ•π‘¦
] 𝑓(1,0)
πœ•
πœ•π‘₯
+ (𝑦 − 𝑏 )
πœ• 1
πœ•π‘¦
1
πœ•
2!
πœ•π‘₯
] 𝑓 (1,0) + [(π‘₯ − π‘Ž)
+
𝑓(1,0) = π‘₯𝑒 𝑦 = 1 ∗ 𝑒 0 = 1
πœ•
πœ•π‘₯
πœ•
πœ•π‘¦
= 𝑒 𝑦 βž” at (𝟏, 𝟎) , 𝑒 0 = 1
= π‘₯𝑒 𝑦 βž” at (𝟏, 𝟎) , 1 ∗ 𝑒 0 = 1
πœ•2
πœ•π‘₯ 2
πœ•2
πœ•π‘¦ 2
=0
= π‘₯𝑒 𝑦 βž” at (𝟏, 𝟎) , 1 ∗ 𝑒 0 = 1
πœ•2
πœ•π‘₯πœ•π‘¦
= 𝑒 𝑦 βž” at (𝟏, 𝟎) , 𝑒 0 = 1
πœ•
[(π‘₯ − π‘Ž)
1
2!
[(π‘₯ − π‘Ž)
[ (𝑦 − 0)
πœ•π‘₯
πœ•
πœ•π‘₯
+ (𝑦 − 𝑏)
+ (𝑦 − 𝑏 )
πœ• 1
πœ•π‘¦
] 𝑓(1,0) = [(π‘₯ − 1) ∗ 1 + (𝑦 − 0) ∗ 1]1 = π‘₯ − 1 + 𝑦
πœ• 2
πœ•π‘¦
] 𝑓(1,0) =
2!
([(π‘₯ − 1)
πœ•π‘¦
=
=
Then: 𝑓(1,0) + [(π‘₯ − π‘Ž)
πœ•
πœ•π‘₯
1
2!
1
2!
1
2!
1
2!
(( π‘₯ − 1 ) 2
πœ•2
πœ•π‘₯ 2
πœ•π‘₯
] + 2 [((π‘₯ − 1)
) (( 𝑦 − 0 )
πœ•
πœ•π‘¦
+ (𝑦 − 𝑏 )
1
2!
Choice B
𝟐!
πœ•π‘₯πœ•π‘¦
] + 𝑦2
πœ•2
πœ•π‘¦ 2
)
(2π‘₯𝑦 − 2𝑦 + 𝑦 2 )
πœ• 1
πœ•π‘¦
(πŸπ’™π’š − πŸπ’š + π’šπŸ )
1
πœ•
2!
πœ•π‘₯
] 𝑓 (1,0) + [(π‘₯ − π‘Ž)
= 1 + π‘₯ − 1 + 𝑦 + (2π‘₯𝑦 − 2𝑦 + 𝑦 2 )
𝟏
πœ•2
(0 + 2[(π‘₯ − 1)𝑦] + 𝑦 2 )
] 𝑓(1,0)
=𝒙+π’š+
+ 2 [ (π‘₯ − 1)𝑦
((π‘₯ − 1)2 ∗ 0 + 2[(π‘₯ − 1)𝑦 ∗ 1] + 𝑦 2 ∗ 1)
πœ• 2
Page | 90
πœ•
πœ•π‘₯
] )
=
πœ•π‘¦
πœ• 2
πœ• 2
=
𝑏)
1
+ (𝑦 −
)] +
97] Obtain Taylor’s expansion of 𝒇(𝒙, π’š) = 𝒆𝒙 𝐜𝐨𝐬 π’š at point (𝟎, 𝟎)
for 𝒏 = πŸ‘
𝟏
𝟏
A- π’™πŸ + 𝟐! (π’™πŸ − π’šπŸ ) + πŸ‘! [π’†πœ½(𝒙) ((𝒄𝒐𝒔 𝜽(π’š) (π’™πŸ‘ − πŸ‘π’™π’šπŸ )) + (π’”π’Šπ’ 𝜽(π’š) (π’šπŸ‘ −
πŸ‘π’™πŸ π’š)))]
𝟏
B- 𝒙 + 𝟐! (π’™πŸ − π’šπŸ ) + [π’†πœ½(𝒙) ((𝒄𝒐𝒔 𝜽(π’š) (π’™πŸ‘ − πŸ‘π’™π’šπŸ )) + (π’”π’Šπ’ 𝜽(π’š) (π’šπŸ‘ −
πŸ‘π’™πŸ π’š)))]
𝟏
𝟏
C- 𝟏 + 𝟐! (π’™πŸ − π’šπŸ ) + πŸ‘! [π’†πœ½(𝒙) ((𝒄𝒐𝒔 𝜽(π’š) (π’™πŸ‘ − πŸ‘π’™π’šπŸ )) + (π’”π’Šπ’ 𝜽(π’š) (π’šπŸ‘ −
πŸ‘π’™πŸ π’š)))]
D- None of these
Solution:
𝑓(π‘₯, 𝑦) = 𝑓(0,0) + [(π‘₯ − π‘Ž)
πœ•
πœ•π‘₯
𝑅3
𝒇(𝟎, 𝟎) = 𝑒 0 cos 0 = 1
πœ•
πœ•π‘₯
= 𝑒 π‘₯ cos 𝑦
At (𝟎, 𝟎) βž” 𝑒 0 cos 0 = 1
πœ•
πœ•π‘¦
= −𝑒 π‘₯ sin 𝑦
At (𝟎, 𝟎) βž” −𝑒 0 sin 0 = 0
πœ•2
πœ•π‘₯ 2
= 𝑒 π‘₯ cos 𝑦
At (𝟎, 𝟎) βž” 𝑒 0 cos 0 = 1
πœ•2
πœ•π‘¦ 2
= −𝑒 π‘₯ cos 𝑦
Page | 91
+ (𝑦 − 𝑏)
πœ• 1
1
πœ•
πœ• 2
] 𝑓(0,0) + 2! [(π‘₯ − π‘Ž) πœ•π‘₯ + (𝑦 − 𝑏) πœ•π‘¦] 𝑓(0,0) +
πœ•π‘¦
At (𝟎, 𝟎) βž” −𝑒 0 cos 0 = −1
πœ•2
πœ•π‘₯πœ•π‘¦
= −𝑒 π‘₯ sin 𝑦
At (𝟎, 𝟎) βž” −𝑒 0 sin 0 = 0
πœ•
[(π‘₯ − π‘Ž)
1
2!
[(π‘₯ − π‘Ž)
[ (𝑦 − 0)
πœ•π‘₯
πœ•
+ (𝑦 − 𝑏)
+ (𝑦 − 𝑏 )
πœ•π‘₯
πœ• 1
πœ•π‘¦
] 𝑓(0,0) = [(π‘₯ − 0) ∗ 1 + (𝑦 − 0) ∗ 0]1 = 𝒙
πœ• 2
πœ•π‘¦
] 𝑓(1,1) =
πœ•π‘¦
=
Then: π‘ΉπŸ‘ =
=
πœ• 2
πœ•
πœ•π‘₯
πœ•π‘₯
] + 2 [((π‘₯ − 0)
) (( 𝑦 − 0 )
πœ•
πœ•π‘¦
)] +
] )
=
=
2!
([(π‘₯ − 0)
πœ• 2
=
=
1
1
3!
1
3!
1
3!
[(π‘₯)
[(π‘₯)
[(π‘₯ − 0)
πœ•
πœ•π‘₯
πœ•
πœ•π‘₯
+ (𝑦)
+ (𝑦)
πœ•
πœ•π‘₯
2!
1
2!
𝟏
𝟐!
(( π‘₯ ) 2
πœ•2
πœ•2
πœ•π‘₯
πœ•π‘₯πœ•π‘¦
+ 2 [(π‘₯)(𝑦)
2
] + (𝑦 )2
πœ•2
πœ•π‘¦ 2
)
((π‘₯)2 ∗ 1 + 2[(π‘₯)(𝑦) ∗ 0] + (𝑦)2 ∗ −1)
(π’™πŸ − π’šπŸ )
+ (𝑦 − 0)
πœ• 3
πœ•π‘¦
] 𝑓 ((0 + πœƒ(π‘₯ − 0)), (0 + πœƒ(𝑦 − 0)))
πœ• 3
πœ•π‘¦
] 𝑓(πœƒ(π‘₯), πœƒ(𝑦))
πœ• 2
πœ•π‘¦
] [(π‘₯)
πœ• 2
1
1
πœ•
πœ•π‘₯
+ (𝑦)
πœ•
πœ•
πœ•π‘¦
]
πœ• 2
πœ•
πœ•
πœ•
([(π‘₯) πœ•π‘₯] + 2 [((π‘₯) πœ•π‘₯) ((𝑦) πœ•π‘¦)] + [(𝑦) πœ•π‘¦] ) ∗ [(π‘₯) πœ•π‘₯ + (𝑦) πœ•π‘¦]
3!
=
π‘₯2
1
3!
πœ•2
πœ•π‘₯
2 ∗π‘₯
πœ•
πœ•π‘₯
+ π‘₯2
πœ•2
πœ•π‘₯ 2
∗𝑦
πœ•
πœ•π‘¦
+ 2 [((π‘₯)
+𝑦 2
[
= π‘₯3
Page | 92
πœ•3
πœ•3
πœ•π‘₯
πœ•π‘₯ 2 πœ•π‘¦
+ π‘₯ 2𝑦
3
+ 2(π‘₯ 2 𝑦)
πœ•
πœ•
πœ•
πœ•
πœ•
πœ•
) ((𝑦) πœ•π‘¦)] ∗ π‘₯ πœ•π‘₯ + 2 [((π‘₯) πœ•π‘₯) ((𝑦) πœ•π‘¦)] ∗ 𝑦 πœ•π‘¦
πœ•π‘₯
πœ•2
πœ•
πœ•π‘¦
πœ•π‘₯
2 ∗π‘₯
πœ•3
πœ•π‘₯πœ•π‘¦πœ•π‘₯
+ 𝑦2
πœ•2
πœ•π‘¦ 2
+ 2(π‘₯𝑦 2 )
∗𝑦
πœ•3
πœ•π‘₯πœ•π‘¦
πœ•
]
πœ•π‘¦
+ 𝑦2π‘₯
2
πœ•3
πœ•π‘¦ 2 πœ•π‘₯
+ 𝑦3
πœ•3
πœ•π‘¦ 3
πœ•3
πœ•π‘₯ 3
= 𝑒 π‘₯ cos 𝑦 ,
πœ•3
πœ•π‘¦ 2 πœ•π‘₯
3
3 πœ•
π‘₯
πœ•π‘₯ 3
πœ•3
πœ•π‘₯ 2 πœ•π‘¦
= −𝑒 π‘₯ cos 𝑦 ,
πœ•3
2
+π‘₯ 𝑦
πœ•π‘₯ 2 πœ•π‘¦
= −𝑒 π‘₯ sin 𝑦 ,
πœ•3
πœ•π‘¦ 3
πœ•3
πœ•π‘₯πœ•π‘¦πœ•π‘₯
= −𝑒 π‘₯ sin 𝑦 ,
πœ•3
πœ•π‘₯πœ•π‘¦ 2
= −𝑒 π‘₯ cos 𝑦
= 𝑒 π‘₯ sin 𝑦
+ 2( π‘₯ 2 𝑦 )
πœ•3
πœ•π‘₯πœ•π‘¦πœ•π‘₯
+ 2(π‘₯𝑦 2 )
πœ•3
πœ•π‘₯πœ•π‘¦ 2
πœ•3
2
+𝑦 π‘₯
πœ•π‘¦ 2 πœ•π‘₯
+
3
3 πœ•
𝑦
πœ•π‘¦ 3
= π‘₯ 3 ∗ 𝑒 π‘₯ cos 𝑦 + π‘₯ 2 𝑦 ∗ (−𝑒 π‘₯ sin 𝑦) + 2(π‘₯ 2 𝑦) ∗ (−𝑒 π‘₯ sin 𝑦)
+2(π‘₯𝑦 2 ) ∗ (−𝑒 π‘₯ cos 𝑦) + 𝑦 2 π‘₯ ∗ (−𝑒 π‘₯ cos 𝑦) + 𝑦 3 ∗ 𝑒 π‘₯ sin 𝑦
= π‘₯ 3 𝑒 π‘₯ cos 𝑦 − 3π‘₯ 2 𝑦𝑒 π‘₯ sin 𝑦 − 3π‘₯𝑦 2 𝑒 π‘₯ cos 𝑦 + 𝑦 3 𝑒 π‘₯ sin 𝑦
= 𝑒 π‘₯ cos 𝑦 (π‘₯ 3 − 3π‘₯𝑦 2 ) + 𝑒 π‘₯ sin 𝑦 (𝑦 3 − 3π‘₯ 2 𝑦)
At ((𝟎 + 𝜽(𝒙 − 𝟎)), (𝟎 + 𝜽(π’š − 𝟎))) = (𝜽(𝒙), 𝜽(π’š))
Substitute in 𝑒 π‘₯ cos 𝑦 & 𝑒 π‘₯ sin 𝑦 Only
βž” 𝑒 πœƒ(π‘₯) cos πœƒ (𝑦) (π‘₯ 3 − 3π‘₯𝑦 2 ) + 𝑒 πœƒ(π‘₯) sin πœƒ (𝑦) (𝑦 3 − 3π‘₯ 2 𝑦)
Then: 𝑅3 =
1
3!
[𝑒 πœƒ(π‘₯) ((cos πœƒ (𝑦) (π‘₯ 3 − 3π‘₯𝑦 2 )) + (sin πœƒ (𝑦) (𝑦 3 − 3π‘₯ 2 𝑦)))]
πœ•
πœ• 1
1
πœ•
Then: 𝑓(0,0) + [(π‘₯ − π‘Ž) πœ•π‘₯ + (𝑦 − 𝑏) πœ•π‘¦] 𝑓(0,0) + 2! [(π‘₯ − π‘Ž) πœ•π‘₯ + (𝑦 −
𝑏)
πœ• 2
] 𝑓(0,0) +
πœ•π‘¦
=𝟏+
𝟏
𝟐!
(π’™πŸ − π’šπŸ ) +
πŸ‘π’™πŸ π’š)))]
Choice C
Page | 93
𝑅3
𝟏
πŸ‘!
[π’†πœ½(𝒙) ((𝒄𝒐𝒔 𝜽(π’š) (π’™πŸ‘ − πŸ‘π’™π’šπŸ )) + (π’”π’Šπ’ 𝜽(π’š) (π’šπŸ‘ −
∞
98] Determine ∫𝒂 𝒆−𝒙 𝒅𝒙 converges or diverges , if converges Find
its value .
A- Converged at 𝒆−𝒂
B- Diverged at ∞
D- Converged at 𝒆𝒂
C- Diverged at −∞
Solution:
∞
𝑑
∫π‘Ž 𝑒 −π‘₯ 𝑑π‘₯ = lim ∫π‘Ž 𝑒 −π‘₯ 𝑑π‘₯ = lim [−𝑒 −π‘₯ ]π‘‘π‘Ž = lim [(−𝑒 −𝑑 ) − (−𝑒 −π‘Ž )]
𝑑→∞
𝑑→∞
𝑑→∞
= lim [(−𝑒 −𝑑 ) + 𝑒 −π‘Ž ] = (−𝑒 −∞ ) + 𝑒 −π‘Ž = −
𝑑→∞
1
𝑒∞
+ 𝑒 −π‘Ž
= 0 + 𝑒 −π‘Ž = 𝑒 −π‘Ž
Since the result is a number not ∞ or −∞ , then it converged
Then: this improper integral Converged
∞ 𝟏
99] Determine ∫πŸ’
𝒙−𝟐
Choice A
𝒅𝒙 converges or diverges , if converges Find
its value .
A- Converged
B- Diverged at ∞
C- Diverged at −∞
D- None of these
Solution:
∞ 1
∫4
π‘₯−2
𝑑 1
𝑑π‘₯ = lim ∫4
𝑑→∞
π‘₯−2
𝑑π‘₯ = lim [ln|π‘₯ − 2|]𝑑4 = lim [(ln|𝑑 − 2|) − (ln|4 − 2|)]
𝑑→∞
𝑑→∞
= lim [(ln|𝑑 − 2|) − (ln|2|)]
𝑑→∞
= [(ln|∞ − 2|) − (ln|2|)] = [(ln|∞|) − (ln|2|)]
= [∞ − (ln|2|)] = ∞
Then: this improper integral Diverged
Page | 94
Choice B
∞
𝟏
100] Determine ∫−∞ 𝟏+π’™πŸ 𝒅𝒙 converges or diverges , if converges
Find its value .
A- Converged at 𝝅
B- Diverged at ∞
C- Diverged at −∞
D- Converged at 𝟐
𝝅
Solution:
∞
𝑐
1
−1
lim [tan
𝑑→∞
π‘₯ ]𝑑𝑐
𝑑
1
∫−∞ 1+π‘₯ 2 𝑑π‘₯ = lim ∫𝑑
1+π‘₯
𝑑→−∞
2 𝑑π‘₯ + lim ∫𝑐
𝑑→∞
1
1+π‘₯ 2
𝑑π‘₯ = lim [tan−1 π‘₯ ]𝑐𝑑 +
𝑑→−∞
= lim [tan−1 𝑐 − tan−1 𝑑] + lim [tan−1 𝑑 − tan−1 𝑐 ]
𝑑→−∞
𝑑→∞
Let 𝑐 = 0 or any number in the Domain of tan
βž” lim [tan−1 0 − tan−1 𝑑] + lim [tan−1 𝑑 − tan−1 0]
𝑑→−∞
𝑑→∞
= lim [0 − tan−1 𝑑] + lim [tan−1 𝑑 − 0] = − tan−1 −∞ + tan−1 ∞
𝑑→−∞
𝑑→∞
πœ‹
πœ‹
= − (− ) + = πœ‹
2
2
Then: this improper integral Converged
πŸ–
101] Determine ∫𝟎
πŸ‘π’™
πŸ‘
√πŸ”πŸ’−π’™πŸ
Choice A
𝒅𝒙 converges or diverges , if converges
Find its value .
A- Converged at πŸ‘πŸ”
B- Diverged at ∞
C- Diverged at −∞
D- Converged at −πŸ‘πŸ”
Solution:
8
∫0
3π‘₯
3
√64−π‘₯
𝑑
3 lim− ∫0
𝑑→8
Page | 95
𝑑
𝑑π‘₯ = lim− ∫0
2
π‘₯
𝑑→8
1
(64−π‘₯ 2 )3
𝑑π‘₯
3π‘₯
3
√64−π‘₯
𝑑
𝑑π‘₯ = 3 ∗ lim− ∫0
2
𝑑→8
π‘₯
3
√64−π‘₯ 2
𝑑π‘₯ =
=
𝑑
3 lim− ∫0 π‘₯
𝑑→8
∗ (64 − π‘₯
1
2 )−3
𝑑π‘₯ = 3 ∗
1
−3
𝑑
3
= − lim− ∫0 −2π‘₯ (64 − π‘₯ 2 )
2 𝑑→8
3
3
= − lim− [(64 − π‘₯
2 𝑑→8 2
9
= − lim− [(64 − 𝑑
4 𝑑→8
2
2 )3
2
2 )3
3
𝑑π‘₯ = − lim− [
∗ −2 ∗ (64 − π‘₯
1
− +1
2
(64−π‘₯ ) 3
2
3
2 𝑑→8
𝑑
9
] = − lim− [(64 − π‘₯
4 𝑑→8
0
− (64 − 0
2
9
𝑑
− lim− ∫0 π‘₯
2 𝑑→8
1
2
2
2 )3
2
2 )3
1
2 )−3
𝑑π‘₯
𝑑
]
0
𝑑
]
0
]
2
9
3
= − [(64 − 82 )3 − (64)3 ] = − [(0)3 − √(64)2 ]
4
4
9
9
3
= − [− √4096 ] = − ∗ −16 = +36
4
4
Then: this improper integral Converged
Choice A
πŸ‘ 𝟏
102] Determine ∫−𝟏 π’™πŸ 𝒅𝒙 converges or diverges , if converges Find
its value .
A- Converged
B- Diverged
C- Diverged at −∞
D- None of these
Solution:
3 1
0 1
3 1
∫−1 π‘₯ 2 𝑑π‘₯ = ∫−1 π‘₯ 2 𝑑π‘₯ + ∫0
π‘₯
𝑑
2 𝑑π‘₯ = lim− ∫−1
𝑑→0
3 1
1
π‘₯
2 𝑑π‘₯ + lim+ ∫𝑑
𝑑→0
𝑑
3
π‘₯2
𝑑π‘₯
= lim− ∫−1(π‘₯ )−2 𝑑π‘₯ + lim+ ∫𝑑 (π‘₯ )−2 𝑑π‘₯
𝑑→0
𝑑→0
1 𝑑
1 3
= lim− [− ]
𝑑→0
1
1
π‘₯ −1
1
+ lim+ [− ]
π‘₯ 𝑑
𝑑→0
1
= lim− [(− ) − (− )] + lim+ [(− ) − (− )]
𝑑
−1
3
𝑑
𝑑→0
Page | 96
𝑑→0
1
1
1
= lim− [(− ) − 1] + lim+ [(− ) + ]
𝑑
3
𝑑
𝑑→0
𝑑→0
1
1
1
= lim− (− ) − lim−(1) + lim+ (− ) + lim+ ( )
𝑑
3
𝑑
𝑑→0
𝑑→0
1
𝑑→0
1
𝑑→0
1
1
1
1
= lim− (− ) − 1 − + lim+ ( ) = lim− (− ) − 1 − + lim+ ( )
𝑑
3
𝑑
0
3
0
𝑑→0
𝑑→0
𝑑→0
𝑑→0
1
= −∞ − 1 − + ∞
3
Then: this improper integral Diverged
𝟏
103] Determine ∫𝟎
𝟏
√𝟏−π’™πŸ
Choice B
𝒅𝒙 converges or diverges , if converges
Find its value .
𝝅
A- Converged at 𝟐
B- Diverged
C- Diverged at −∞
D- Converged at 𝝅
Solution:
1
∫0
1
√1−π‘₯ 2
𝑑
𝑑π‘₯ = lim− ∫0
𝑑→1
1
√1−π‘₯ 2
𝑑π‘₯ = lim−[sin−1 π‘₯ ]𝑑0 = lim−[sin−1 𝑑 − sin−1 0]
𝑑→1
𝑑→1
πœ‹
πœ‹
2
2
= [sin−1 1 − sin−1 0] = − 0 =
Then: this improper integral Converged
𝟐
104] Determine ∫𝟏
𝟏
𝒙 π₯𝐧 𝒙
Choice A
𝒅𝒙 converges or diverges , if converges Find
its value .
A- Converged
B- Diverged at ∞
C- Diverged at −∞
D- None of these
Page | 97
Solution:
2 1
∫1 π‘₯ ln π‘₯ 𝑑π‘₯
=
2 1
lim+ ∫𝑑
𝑑π‘₯
π‘₯ ln π‘₯
𝑑→1
1
=
2
lim+ ∫𝑑 π‘₯
ln π‘₯
𝑑→1
𝑑π‘₯ = lim+[ln|ln|π‘₯ ||]2𝑑
𝑑→1
= lim+[(ln|ln|2||) − (ln|ln|𝑑||)]
𝑑→1
= (ln|ln|2||) − (ln|ln|1||)
= ln|ln|2|| − ln|0|
= ln|ln|2|| − (−∞) = ∞
Then: this improper integral Diverged
Choice B
πŸπŸ• 𝟏
105] Determine ∫𝟎
πŸ‘
√π’™πŸ
𝒅𝒙 converges or diverges , if converges Find
its value .
A- Converged at −πŸ—
B- Diverged at ∞
C- Diverged at −∞
D- Converged at πŸ—
Solution:
27 1
∫0
3
√π‘₯
27 1
𝑑π‘₯ = ∫0
2
27 1
∫0 2 𝑑π‘₯
π‘₯3
=
2
𝑑π‘₯
π‘₯3
27 1
π‘™π‘–π‘š+ ∫𝑑 2 𝑑π‘₯
𝑑→0
π‘₯3
1
=
27 −2
π‘™π‘–π‘š ∫ π‘₯ 3 𝑑π‘₯
𝑑→0+ 𝑑
2
− +1
π‘₯ 3
= π‘™π‘–π‘š+ [
𝑑→0
2
−3+1
1
27
]
= π‘™π‘–π‘š+ [3π‘₯ ]
𝑑
1
= π‘™π‘–π‘š+ [(3 ∗ 273 ) − (3 ∗ 𝑑 3 )] = π‘™π‘–π‘š+ [(3 ∗ 3) − (3 ∗ 𝑑 3 )]
𝑑→0
𝑑→0
1
3
1
3
= π‘™π‘–π‘š+ [9 − (3 ∗ 𝑑 )] = 9 − (3 ∗ 0 ) = 9
𝑑→0
Then: this improper integral Converged
Page | 98
Choice D
1
3
𝑑→0
27
𝑑
πŸ’ 𝟏
106] Determine ∫𝟎
√𝒙
𝒅𝒙 converges or diverges , if converges Find
its value .
A- Converged at 𝟎
B- Diverged at ∞
C- Converged at πŸ’
D- Converged at −πŸ’
Solution:
4 1
∫0 π‘₯ 𝑑π‘₯
√
=
4 1
π‘™π‘–π‘š+ ∫𝑑
𝑑π‘₯
√π‘₯
𝑑→0
4
1
= π‘™π‘–π‘š+ [
𝑑→0
− +1
π‘₯ 2
1
−2+1
=
4 1
π‘™π‘–π‘š+ ∫𝑑 1 𝑑π‘₯
𝑑→0
π‘₯2
1
] = π‘™π‘–π‘š+ [
𝑑→0
𝑑
π‘₯2
1
2
=
4 −1
π‘™π‘–π‘š ∫ π‘₯ 2 𝑑π‘₯
𝑑→0+ 𝑑
1
− +1
π‘₯ 2
= π‘™π‘–π‘š+ [
𝑑→0
1
2
− +1
4
]
𝑑
4
4
] = π‘™π‘–π‘š+[2√π‘₯]𝑑 = π‘™π‘–π‘š+[(2√4) − (2√𝑑)]
𝑑→0
𝑑
𝑑→0
= π‘™π‘–π‘š+[4 − (2√𝑑)] = 4 − (2√0) = 4
𝑑→0
Then: this improper integral Converged
Choice C
πŸ—
107] Determine ∫𝟎
𝟏
√πŸ—−𝒙
𝒅𝒙 converges or diverges , if converges Find
its value .
A- Converged at −πŸ”
B- Diverged at ∞
C- Converged at πŸ”
D- Converged at πŸ’
Solution:
9 1
∫0 √9−π‘₯ 𝑑π‘₯
=
𝑑 1
π‘™π‘–π‘š− ∫0
𝑑π‘₯
√9−π‘₯
𝑑→9
1
− +1
(9−π‘₯) 2
1
𝑑→9− (−2+1)∗(−1)
= π‘™π‘–π‘š [
=
𝑑
𝑑
π‘™π‘–π‘š− ∫0
𝑑→9
1
1
1
(9−π‘₯)2
1
−2
𝑑→9−
] = π‘™π‘–π‘š [
0
1
2
𝑑π‘₯ =
(9−π‘₯)2
1
2
𝑑
π‘™π‘–π‘š− ∫0 (9
𝑑→9
− π‘₯)
𝑑
Page | 99
𝑑π‘₯
1
2
] = −2 π‘™π‘–π‘š− [(9 − π‘₯ ) ]
0
𝑑→9
1
2
1
2
= −2 π‘™π‘–π‘š− [(9 − 𝑑) − (9 − 0) ] = −2 [(9 − 9) − (9) ]
𝑑→9
1
−2
𝑑
0
1
1
= −2 [(0)2 − (9)2 ] = −2[−√9] = −2[−3] = 6
Then: this improper integral Converged
Choice C
πŸ’ πŸ’π’™
108] Determine ∫𝟏
π’™πŸ −𝟏
𝒅𝒙 converges or diverges , if converges Find
its value .
A- Converged at −πŸ”
B- Diverged at ∞
C- Converged at πŸ”
D- Converged at πŸ’
Solution:
4 4π‘₯
∫1
4 4π‘₯
π‘₯ 2 −1
𝑑π‘₯ = π‘™π‘–π‘š+ ∫𝑑
𝑑→1
π‘₯ 2 −1
𝑑π‘₯
Let π‘₯ 2 − 1 = 𝑒 , 2π‘₯ 𝑑π‘₯ = 𝑑𝑒 βž” 𝑑π‘₯ =
4 4π‘₯
π‘™π‘–π‘š+ ∫𝑑
𝑑→1
π‘₯ 2 −1
4 4π‘₯
𝑑π‘₯ = π‘™π‘–π‘š+ ∫𝑑
𝑑→1
𝑒
∗
𝑑𝑒
2π‘₯
𝑑𝑒
2π‘₯
42
= π‘™π‘–π‘š+ ∫𝑑
𝑑→1
𝑒
𝑑𝑒 = 2 ∗ π‘™π‘–π‘š+[ln|𝑒|]4𝑑
𝑑→1
= 2 π‘™π‘–π‘š+[ln|π‘₯ 2 − 1|]4𝑑 = 2 π‘™π‘–π‘š+[ln|42 − 1| − ln|𝑑 2 − 1|]
𝑑→1
𝑑→1
= 2 π‘™π‘–π‘š+[ln|15| − ln|𝑑 2 − 1|] = 2[ln|15| − ln|12 − 1|]
𝑑→1
= 2[ln|15| − ln|0|] = 2 ln|15| − 2 ln|0| = 2 ln|15| − (−∞) = ∞
Then: this improper integral Diverged
Choice B
∞
109] Determine ∫𝟎 𝒙 𝒆−𝒙 𝒅𝒙 converges or diverges , if converges
Find its value .
A- Converged at −𝟏
B- Diverged at −∞
C- Converged at 𝟏
D- Converged at 𝟎
Page | 100
Solution:
∞
𝑑
∫0 π‘₯ 𝑒 −π‘₯ 𝑑π‘₯ = π‘™π‘–π‘š− ∫0 π‘₯ 𝑒 −π‘₯ 𝑑π‘₯
𝑑→∞
= π‘™π‘–π‘š−[π‘₯ ∗ (−𝑒 −π‘₯ ) − 𝑒 −π‘₯ ]𝑑0
𝑑→∞
𝐈
π‘₯
𝑒 −π‘₯
1
= π‘™π‘–π‘š−[−π‘₯𝑒 −π‘₯ − 𝑒 −π‘₯ ]𝑑0 = π‘™π‘–π‘š−[−𝑒 −π‘₯ (π‘₯ + 1)]𝑑0
𝑑→∞
𝐃
𝑑→∞
+
−
−𝑒 −π‘₯
𝑒 −π‘₯
0
= π‘™π‘–π‘š−[(−𝑒−𝑑 (𝑑 + 1)) − (−𝑒−0 (0 + 1))]
𝑑→∞
= π‘™π‘–π‘š−[(−𝑒−𝑑 (𝑑 + 1)) − (−1)] = π‘™π‘–π‘š−[(−𝑒−𝑑 (𝑑 + 1)) + 1]
𝑑→∞
𝑑→∞
= π‘™π‘–π‘š−(−𝑒−𝑑 (𝑑 + 1)) + π‘™π‘–π‘š− 1 = π‘™π‘–π‘š− (−
𝑑→∞
𝑑→∞
𝑑+1
= − π‘™π‘–π‘š− (
𝑑→∞
𝑒𝑑
𝑑→∞
𝑑+1
𝑒𝑑
)+1
)+1
∞+1
By Substitution in limits βž” (
𝑒∞
∞
)=∞
Then We will Use L’hopital Rule
𝑑+1
− π‘™π‘–π‘š− (
𝑑→∞
1+0
) + 1 = − π‘™π‘–π‘š− (
𝑒𝑑
𝑑→∞
𝑒𝑑
1
) + 1 = − π‘™π‘–π‘š− (𝑒∞) + 1 = −0 + 1 = 1
𝑑→∞
Then: this improper integral Converged
Choice C
∞
110] Determine ∫𝟏
𝟏
(πŸ’π’™+𝟏)πŸ‘
𝒅𝒙 converges or diverges , if converges
Find its value .
𝟏
A- Converged at 𝟐𝟎𝟎
B- Diverged at −∞
C- Converged at −πŸ“ ∗ 𝟏𝟎−πŸ‘
D- Converged at 𝟐𝟎𝟎
Solution:
∞
∫1
1
𝑑π‘₯
(4π‘₯+1)3
𝑑
𝑑
1
= π‘™π‘–π‘š− ∫1 (4π‘₯+1)3 𝑑π‘₯ = π‘™π‘–π‘š− ∫1 (4π‘₯ + 1)−3 𝑑π‘₯
𝑑→∞
(4π‘₯+1)−3+1
𝑑→∞
𝑑
= π‘™π‘–π‘š− [ (−3+1)∗(4) ] = π‘™π‘–π‘š− [
𝑑→∞
Page | 101
1
𝑑→∞
(4π‘₯+1)−2
−8
𝑑
] = π‘™π‘–π‘š− [−
1
𝑑→∞
1
𝑑
]
8(4π‘₯+1)2 1
= π‘™π‘–π‘š− [(−
𝑑→∞
1
1
8(4𝑑+1)2
= π‘™π‘–π‘š− [(−
𝑑→∞
1
1
) − (− 8(4∗1+1)2)] = π‘™π‘–π‘š− [(− 8(4𝑑+1)2 ) − (− 8∗25)]
𝑑→∞
1
1
1
1
) + 200] = π‘™π‘–π‘š− [(− 8(4∗∞+1)2 ) + 200]
8(4𝑑+1)2
𝑑→∞
1
1
1
1
1
1
= π‘™π‘–π‘š− [(− ) + ] = π‘™π‘–π‘š− (− ) + π‘™π‘–π‘š−
=0+
=
∞
200
∞
200
200
200
𝑑→∞
𝑑→∞
𝑑→∞
Then: this improper integral Converged
Choice A
𝟐
111] Determine ∫−𝟐
𝟏
√𝟐+𝒙
𝒅𝒙 converges or diverges , if converges
Find its value .
A- Converged at 𝟎
B- Diverged at −∞
C- Converged at −πŸ’
D- Converged at πŸ’
Solution:
2
1
∫−2 √2+π‘₯ 𝑑π‘₯
=
2 1
π‘™π‘–π‘š+ ∫𝑑
𝑑π‘₯
√2+π‘₯
𝑑→−2
1
(2+π‘₯)−2+1
= π‘™π‘–π‘š+ [
𝑑→−2
1
−2+1
=
2
π‘™π‘–π‘š+ ∫𝑑
𝑑→−2
2
1
(2+π‘₯)2
𝑑→−2
1
2
1
2
𝑑π‘₯ =
(2+π‘₯)2
1
] = π‘™π‘–π‘š+ [
𝑑
1
2
π‘™π‘–π‘š+ ∫𝑑 (2
𝑑→−2
2
+ π‘₯)
1
2
] = 2 π‘™π‘–π‘š+ [(2 + π‘₯ ) ]
𝑑→−2
𝑑
1
2
1
−2
𝑑π‘₯
2
𝑑
= 2 π‘™π‘–π‘š+ [((2 + 2) ) − ((2 + 𝑑) )] = 2 π‘™π‘–π‘š+[(√4) − (√2 + 𝑑)]
𝑑→−2
𝑑→−2
= 2[(√4) − (√2 − 2)] = 2[(2) − (0)] = 4
Then: this improper integral Converged
Choice D
Page | 102
𝟎
112] Determine ∫−𝝅 𝐬𝐞𝐜 𝟐 𝒙 𝒅𝒙 converges or diverges , if converges
𝟐
Find its value .
A- Converged at ∞
B- Diverged at −∞
𝝅
C- Converged at − 𝟐
D- Diverged at ∞
Solution:
0
∫−πœ‹ sec 2 π‘₯ 𝑑π‘₯
2
0
0
1
πœ‹
1
1
1
Since ∫−πœ‹ sec 2 π‘₯ 𝑑π‘₯ = ∫−πœ‹ 2 𝑑π‘₯ then: at π‘₯ = − βž” 2 = 2 πœ‹ =
cos π‘₯
2
cos π‘₯
0
cos −
2
2
2
0
0
Then: ∫−πœ‹ sec 2 π‘₯ 𝑑π‘₯ = π‘™π‘–π‘š+ ∫𝑑 sec 2 π‘₯ 𝑑π‘₯ = π‘™π‘–π‘š+[tan π‘₯ ]0𝑑
πœ‹
2
πœ‹
𝑑→− 2
𝑑→− 2
= π‘™π‘–π‘š+[(tan 0) − (tan 𝑑)] = π‘™π‘–π‘š+[0 − (tan 𝑑)]
πœ‹
πœ‹
𝑑→− 2
𝑑→− 2
= π‘™π‘–π‘š+ 0 − π‘™π‘–π‘š+ tan 𝑑 = 0 − π‘™π‘–π‘š+ tan −
πœ‹
𝑑→− 2
πœ‹
1
2
0
πœ‹
𝑑→− 2
Since tan − = = 𝑒𝑛𝑑𝑒𝑓𝑖𝑛𝑒𝑑
πœ‹
Then: π‘™π‘–π‘š+ tan − = ∞
πœ‹
𝑑→− 2
2
πœ‹
βž” 0 − π‘™π‘–π‘š+ tan − = 0 − ∞ = −∞
πœ‹
𝑑→− 2
2
Then: this improper integral Diverged
Choice B
Page | 103
πœ‹
𝑑→− 2
πœ‹
2
∞
𝟏
113] Determine ∫𝟎
πŸ’+π’™πŸ
𝒅𝒙 converges or diverges , if converges Find
its value .
𝝅
A- Converged at 𝟐
C- Converged at
B- Diverged at −∞
πŸπ…
D- None of them
πŸ’
Solution:
∞
∫0
1
4+π‘₯ 2
∞
∫0
1
4+π‘₯ 2
𝑑π‘₯ at π‘₯ = ∞ βž”
𝑑
1
4+∞2
=
1
∞
1
𝑑π‘₯ = π‘™π‘–π‘š− ∫0
𝑑π‘₯
4+π‘₯ 2
𝑑→∞
1
π‘₯
1
∫ 4+π‘₯ 2 𝑑π‘₯ βž” Suppose 𝑒 = 2 βž” π‘₯ = 2𝑒 , 𝑑𝑒 = 2 𝑑π‘₯ βž” 2𝑑𝑒 = 𝑑π‘₯
1
1
2
1
1
∫ 4+π‘₯ 2 𝑑π‘₯ = ∫ 4+(2𝑒)2 ∗ 2𝑑𝑒 = ∫ 4+4𝑒2 𝑑𝑒 = 2 ∫ 4+4𝑒2 𝑑𝑒 = 2 ∫ 4(1+𝑒2 ) 𝑑𝑒
= 2∫
1
2
1
1
1
1
−1
𝑑𝑒
=
𝑑𝑒
=
𝑑𝑒
=
tan
𝑒
∫
∫
2
2
2
4(1+𝑒 )
4 1+𝑒
2 1+𝑒
2
1
π‘₯
= tan−1 ( )
2
2
𝑑 1
π‘™π‘–π‘š− ∫0
𝑑π‘₯
4+π‘₯ 2
𝑑→∞
=
=
1
π‘₯
tan−1 (2)
= π‘™π‘–π‘š− [
𝑑→∞
] =
2
0
𝑑
π‘₯
1
π‘₯
π‘™π‘–π‘š− [tan−1 ( )]
2
2 𝑑→∞
1
𝑑
0
𝑑→∞
∞
2 𝑑→∞
1
𝑑→∞
1
πœ‹
πœ‹
2
2
4
Then: this improper integral Converged
Page | 104
0
π‘™π‘–π‘š− [(tan−1 ( )) − (0)] = π‘™π‘–π‘š−(tan−1 (∞))
2
2
= ∗ =
Choice D
𝑑
0
π‘™π‘–π‘š− [tan−1 ( )] = π‘™π‘–π‘š− [(tan−1 ( )) − (tan−1 ( ))]
2
2
2
2
2 𝑑→∞
1
𝑑
∞ 𝒍𝒏 𝒙
114] Determine ∫𝟏
𝒅𝒙 converges or diverges , if converges Find
π’™πŸ‘
its value .
𝟏
A- Converged at 𝟐
B- Diverged at ∞
𝟏
C- Converged at πŸ’
D- Converged at 𝟎
Solution:
∞ 𝑙𝑛 π‘₯
∫1
π‘₯3
∞ 𝑙𝑛 π‘₯
∫1
∫
π‘₯3
𝑙𝑛 π‘₯
π‘₯3
𝑑π‘₯ at π‘₯ = ∞ βž”
𝑙𝑛 ∞
𝑑 𝑙𝑛 π‘₯
𝑑π‘₯ = π‘™π‘–π‘š− ∫1
= ∫ 𝑙𝑛 π‘₯ ∗ π‘₯
𝟏
−3
βž” 𝒖 = 𝒍𝒏 𝒙 , 𝒅𝒖 = , 𝒅𝒗 = 𝒙
2
−πŸ‘
𝒙
𝒖𝒗 − ∫ 𝒗 𝒅𝒖 = 𝑙𝑛 π‘₯ ∗ (−
1
∞
𝑑π‘₯
π‘₯3
𝑑→∞
∞
=
∞3
1
1
2π‘₯ 2
1
,𝒗=
𝑙𝑛 π‘₯
1
𝒙−𝟐
−𝟐
=−
1
𝟏
πŸπ’™πŸ
𝑙𝑛 π‘₯
) − ∫ (− 2π‘₯ 2 ∗ π‘₯) = − 2π‘₯ 2 + 2 ∫ π‘₯ 3 = − 2π‘₯ 2 +
∫ π‘₯ −3
=−
Then: ∫
𝑙𝑛 π‘₯
π‘₯3
𝑙𝑛 π‘₯
2π‘₯
=−
1
2 + ∗
2
π‘₯ −2
−2
𝑙𝑛 π‘₯
1
2π‘₯
4π‘₯ 2
𝑑 𝑙𝑛 π‘₯
βž” π‘™π‘–π‘š− ∫1 3 𝑑π‘₯
π‘₯
𝑑→∞
𝑙𝑛 1
1
2 −
=−
= π‘™π‘–π‘š− [−
𝑑→∞
𝑙𝑛 π‘₯
2π‘₯ 2
−
𝑙𝑛 π‘₯
1
2π‘₯
4π‘₯
2 −
1
4π‘₯ 2
𝑑
2 ] = π‘™π‘–π‘š− [(−
𝑑→∞
1
𝑙𝑛 𝑑
1
2𝑑
4𝑑 2
2 −
)−
(− 2∗12 − 4∗12 )]
= π‘™π‘–π‘š− [(−
𝑑→∞
= π‘™π‘–π‘š− (−
𝑑→∞
= − π‘™π‘–π‘š−
𝑑→∞
Since π‘™π‘–π‘š−
𝑙𝑛 ∞
𝑑→∞ 2∞2
𝑙𝑛 𝑑
2𝑑 2
βž”
Page | 105
1
𝑑
4𝑑
=
1
4𝑑 2
=
∞
∞
𝑙𝑛 𝑑
2𝑑
2 −
𝑙𝑛 𝑑
2𝑑 2
𝑙𝑛 𝑑
2𝑑 2
−
1
1
𝑙𝑛 𝑑
1
4𝑑 2
𝑑→∞
1
) + π‘™π‘–π‘š− 4
− π‘™π‘–π‘š−
𝑑→∞
1
4𝑑 2
1
𝑑→∞
𝑑→∞
1
4𝑑 2
1
𝑙𝑛 ∞
𝑑→∞ 4
2∞2
+ π‘™π‘–π‘š− = − π‘™π‘–π‘š−
, then Use L’hopital rule
, then π‘™π‘–π‘š−
1
) − (0 − 4)] = π‘™π‘–π‘š− [(− 2𝑑 2 − 4𝑑 2 ) + 4]
4𝑑 2
= π‘™π‘–π‘š−
1
𝑑→∞ 4∗∞2
=0
𝑑→∞
− π‘™π‘–π‘š−
𝑑→∞
1
4∞2
+
1
4
1
π‘™π‘–π‘š−
𝑑→∞ 4∞2
=0
Then: − π‘™π‘–π‘š−
𝑑→∞
𝑙𝑛 ∞
2∞2
− π‘™π‘–π‘š−
𝑑→∞
1
4∞2
1
1
1
4
4
4
+ =0+0+ =
Then: this improper integral Converged
Choice C
𝟏
𝟏
115] Determine ∫−πŸ‘ (𝒙+𝟐)𝟐 𝒅𝒙 converges or diverges , if converges
Find its value .
𝟏
A- Converged at 𝟐
B- Diverged
𝟏
C- Converged at πŸ’
D- Converged at 𝟎
Solution:
1
1
1
∫−3 (π‘₯+2)2 𝑑π‘₯ , at π‘₯ = −2 βž” 0
1
−2
1
∫−3 (π‘₯+2)2 𝑑π‘₯ = ∫−3
1
1
(π‘₯+2)2
−2
1
𝑑π‘₯ + ∫−2 (π‘₯+2)2 𝑑π‘₯ = π‘™π‘–π‘š− ∫−3
𝑑→−2
−2
1
1
(π‘₯+2)2
𝑑→−2
1
= π‘™π‘–π‘š− ∫−3 (π‘₯ + 2)−2 𝑑π‘₯ + π‘™π‘–π‘š+ ∫−2(π‘₯ + 2)−2 𝑑π‘₯
𝑑→−2
𝑑→−2
= π‘™π‘–π‘š− [
(π‘₯+2)−2+1
𝑑→−2
−2+1
= π‘™π‘–π‘š− [−
𝑑→−2
1
𝑑→−2
= π‘™π‘–π‘š− [(−
= π‘™π‘–π‘š− (−
𝑑→−2
= π‘™π‘–π‘š− (−
𝑑→−2
4
𝑑
π‘₯+2 −3
= π‘™π‘–π‘š− [(−
𝑑→−2
]
𝑑
]
1
−3
Page | 106
(π‘₯+2)−2+1
−2+1
𝑑→−2
+ π‘™π‘–π‘š+ [−
𝑑→−2
1
]
1
]
𝑑
1
π‘₯+2 𝑑
1
1
1
𝑑+2
) − (− −3+2)] + π‘™π‘–π‘š+ [(− 1+2) − (− 𝑑+2)]
1
1
𝑑→−2
1
) − (1)] + π‘™π‘–π‘š+ [(− 3) + 𝑑+2]
𝑑+2
𝑑→−2
1
1
1
) − π‘™π‘–π‘š−(1) + π‘™π‘–π‘š+ (− 3) + π‘™π‘–π‘š+ 𝑑+2
𝑑+2
𝑑→−2
1
𝑑→−2
1
𝑑→−2
1
1
4
1
) − 1 − 3 + π‘™π‘–π‘š+ −2+2 = π‘™π‘–π‘š− (− 0) − 3 + π‘™π‘–π‘š+ 0
−2+2
= −∞ − + ∞ ≠ 0
3
+ π‘™π‘–π‘š+ [
𝑑→−2
𝑑→−2
1
𝑑π‘₯ + π‘™π‘–π‘š+ ∫−2 (π‘₯+2)2 𝑑π‘₯
𝑑→−2
Then: this improper integral Diverged
Choice B
𝟏
116] Determine ∫𝟎 𝒙 𝒍𝒏 𝒙 𝒅𝒙 converges or diverges , if converges
Find its value .
πŸ•
A- Converged at − πŸπŸ–
B- Diverged at ∞
𝟏
𝟏
C- Converged at πŸ’
D- Converged at − 𝟐
Solution:
1
∫0 π‘₯ 𝑙𝑛 π‘₯ 𝑑π‘₯ at π‘₯ = 0 βž” 0 𝑙𝑛 0 = 0 ∗ 𝑒𝑛𝑑𝑒𝑓𝑖𝑛𝑒𝑑
1
1
∫0 π‘₯ 𝑙𝑛 π‘₯ 𝑑π‘₯ = π‘™π‘–π‘š+ ∫𝑑 π‘₯ 𝑙𝑛 π‘₯ 𝑑π‘₯
𝑑→0
π’™πŸ
𝟏
∫ π‘₯ 𝑙𝑛 π‘₯ βž” 𝒖 = 𝒍𝒏 𝒙 , 𝒅𝒖 = 𝒙 , 𝒅𝒗 = 𝒙 , 𝒗 =
𝒖𝒗 − ∫ 𝒗 𝒅𝒖 = 𝑙𝑛 π‘₯ ∗
π‘₯2
2
−∫
π‘₯2
2
1
π‘₯ 2 𝑙𝑛 π‘₯
π‘₯
2
∗ =
𝟐
1
− ∫π‘₯ =
2
=
1
π‘™π‘–π‘š+ ∫𝑑 π‘₯ 𝑙𝑛 π‘₯ 𝑑π‘₯
𝑑→0
= π‘™π‘–π‘š+ [
𝑑→0
π‘₯ 2 𝑙𝑛 π‘₯
2
−
π‘₯2
1
2
2
𝑑→0
1
4
2
𝑑→0 4
𝑑→0
1
π’•πŸ 𝒍𝒏 𝒕
= − − π’π’Šπ’Ž+
4
1
𝒕→𝟎
𝟐
Page | 107
2
𝑑2
+ ]
4
𝑑2
+ ]
4
𝑑 2 𝑙𝑛 𝑑
2
+0
= − − (−∞) = ∞
4
𝑑 2 𝑙𝑛 𝑑
2
𝑑 2 𝑙𝑛 𝑑
= − π‘™π‘–π‘š+ − π‘™π‘–π‘š+
2
4
𝑑 2 𝑙𝑛 𝑑
1
1
2
π‘₯2
12
𝑑→0
𝑑→0
π‘₯2
− )−(
4
= π‘™π‘–π‘š+ [(0 − ) −
4
= π‘™π‘–π‘š+ [− −
−
1
− ∗
2
π‘₯ 2 𝑙𝑛 π‘₯
12 𝑙𝑛 1
] = π‘™π‘–π‘š+ [(
4 𝑑
π‘₯ 2 𝑙𝑛 π‘₯
+ π‘™π‘–π‘š+
𝑑→0
𝑑2
4
𝑑2
− )]
4
Then: this improper integral Diverged
Choice B
𝝅
𝟐
117] Determine ∫𝟎
𝟏
𝟏−𝐬𝐒𝐧 𝒙
𝒅𝒙 converges or diverges , if converges
Find its value .
πŸ•
A- Converged at − πŸπŸ–
B- Diverged at ∞
𝟏
𝟏
C- Converged at πŸ’
D- Converged at − 𝟐
Solution:
πœ‹
2
∫0
βž”
1
1−𝑠𝑖𝑛 π‘₯
1
1−𝑠𝑖𝑛 π‘₯
πœ‹
1
2
πœ‹
1−𝑠𝑖𝑛 2
𝑑π‘₯ , at π‘₯ = βž”
∗
1+𝑠𝑖𝑛 π‘₯
1+𝑠𝑖𝑛 π‘₯
=
1+𝑠𝑖𝑛 π‘₯
1−𝑠𝑖𝑛2 π‘₯
=
1+𝑠𝑖𝑛 π‘₯
π‘π‘œπ‘  2 π‘₯
=
=
1
=
1−1
1
π‘π‘œπ‘  2 π‘₯
+
1
0
𝑠𝑖𝑛 π‘₯
π‘π‘œπ‘  2 π‘₯
= 𝑠𝑒𝑐 2 π‘₯ +
𝑠𝑖𝑛 π‘₯
π‘π‘œπ‘  π‘₯
∗
π‘‘π‘Žπ‘› π‘₯ 𝑠𝑒𝑐 π‘₯
Then: ∫(𝑠𝑒𝑐2 π‘₯ + π‘‘π‘Žπ‘› π‘₯ 𝑠𝑒𝑐 π‘₯) = π‘‘π‘Žπ‘› π‘₯ + 𝑠𝑒𝑐 π‘₯
πœ‹
2
∫0
𝑑
1
1−𝑠𝑖𝑛 π‘₯
𝑑π‘₯ = π‘™π‘–π‘š
∫
πœ‹− 0
𝑑→ 2
1
1−𝑠𝑖𝑛 π‘₯
[π‘‘π‘Žπ‘› π‘₯ + 𝑠𝑒𝑐 π‘₯ ]𝑑0
𝑑π‘₯ = π‘™π‘–π‘š
πœ‹−
𝑑→ 2
[(π‘‘π‘Žπ‘› 𝑑 + 𝑠𝑒𝑐 𝑑) − (π‘‘π‘Žπ‘› 0 + 𝑠𝑒𝑐 0)]
= π‘™π‘–π‘š
πœ‹−
𝑑→ 2
= π‘™π‘–π‘š
π‘‘π‘Žπ‘› 𝑑 + π‘™π‘–π‘š
𝑠𝑒𝑐 𝑑 − π‘™π‘–π‘š
π‘‘π‘Žπ‘› 0 − π‘™π‘–π‘š
𝑠𝑒𝑐 0
πœ‹−
πœ‹−
πœ‹−
πœ‹−
𝑑→ 2
𝑑→ 2
πœ‹
𝑑→ 2
𝑑→ 2
πœ‹
= π‘™π‘–π‘š
π‘‘π‘Žπ‘› + π‘™π‘–π‘š
𝑠𝑒𝑐 − 0 − π‘™π‘–π‘š
πœ‹−
πœ‹−
πœ‹−
𝑑→
2
2
𝑑→
2
2
πœ‹
πœ‹
𝑑→
2
πœ‹
𝑑→ 2
πœ‹
π‘™π‘–π‘š
π‘‘π‘Žπ‘› = ∞ , π‘™π‘–π‘š
𝑠𝑒𝑐 = ∞
πœ‹−
πœ‹−
𝑑→ 2
2
𝑑→ 2
2
=∞+∞−1=∞
Page | 108
2
cos 0
2
= π‘™π‘–π‘š
π‘‘π‘Žπ‘› + π‘™π‘–π‘š
𝑠𝑒𝑐 − 0 − π‘™π‘–π‘š
πœ‹−
πœ‹−
πœ‹−
𝑑→ 2
1
1
𝑑→ 2 cos 0
1
π‘π‘œπ‘  π‘₯
= 𝑠𝑒𝑐 2 π‘₯ +
Then: this improper integral Diverged
Choice B
∞
118] Determine ∫𝟎
𝟏
(𝒙−πŸ‘)𝟐
𝒅𝒙 converges or diverges , if converges
Find its value .
πŸ•
A- Converged at − πŸπŸ–
B- Diverged at ∞
𝟏
𝟏
C- Converged at πŸ’
D- Converged at − 𝟐
Solution:
∞
∫0
∞
∫0
1
𝑑π‘₯
(π‘₯−3)2
, at π‘₯ = 3 βž” (3−3)2 = = 𝑒𝑛𝑑𝑒𝑓𝑖𝑛𝑒𝑑
1
𝑑π‘₯
(π‘₯−3)2
= π‘™π‘–π‘š− ∫0 (π‘₯−3)2 𝑑π‘₯ + π‘™π‘–π‘š+ ∫𝑑
1
∫ (π‘₯−3)2 𝑑π‘₯
𝑑
1
0
𝑑
∞
1
𝑑→3
𝑑→3
= ∫(π‘₯ − 3)−2 𝑑π‘₯ =
∞
1
π‘™π‘–π‘š− ∫0 (π‘₯−3)2 𝑑π‘₯ + π‘™π‘–π‘š+ ∫𝑑
𝑑→3
1
𝑑→3
𝑑→3
= π‘™π‘–π‘š− [(−
= π‘™π‘–π‘š− (−
𝑑→3
= π‘™π‘–π‘š− (−
𝑑→3
−2+1
1
𝑑π‘₯
(π‘₯−3)2
= π‘™π‘–π‘š− [(−
𝑑→3
(π‘₯−3)−2+1
𝑑→3
1
1
π‘₯−3
𝑑
1
] + π‘™π‘–π‘š+ [−
π‘₯−3 0
1
𝑑→3
1
1
]
∞
π‘₯−3 𝑑
1
) − (− 0−3)] + π‘™π‘–π‘š+ [(− ∞−3) − (− 𝑑−3)]
𝑑−3
𝑑→3
1
1
1
1
) − 3] + π‘™π‘–π‘š+ [(− ∞−3) + 𝑑−3]
𝑑−3
𝑑→3
1
1
1
1
) − π‘™π‘–π‘š− 3 − π‘™π‘–π‘š+ ∞−3 + π‘™π‘–π‘š+ 𝑑−3
𝑑−3
𝑑→3
1
𝑑→3
1
𝑑→3
1
) − 3 − 0 + π‘™π‘–π‘š+ 3−3
3−3
1
3
Then: this improper integral Diverged
Page | 109
= −(π‘₯ − 3)−1 = −
= π‘™π‘–π‘š− [−
=∞− −0+∞=∞
Choice B
1
𝑑π‘₯
(π‘₯−3)2
𝑑→3
πŸ”
119] Determine ∫𝟎
𝒙
(π’™πŸ −πŸ’)𝟐
𝒅𝒙 converges or diverges , if converges
Find its value .
πŸ•
A- Converged at − πŸπŸ–
B- Diverged
𝟏
𝟏
C- Converged at πŸ’
D- Converged at − 𝟐
Solution:
6
∫0
π‘₯
(π‘₯ 2 −4)
2 𝑑π‘₯ , at π‘₯ = 2 βž” (22
2
2
−4)2
= = 𝑒𝑛𝑑𝑒𝑓𝑖𝑛𝑒𝑑
0
π‘₯
𝑑𝑒
∫ (π‘₯ 2 −4)2 𝑑π‘₯ , π‘₯ 2 − 4 = 𝑒 , 2π‘₯ 𝑑π‘₯ = 𝑑𝑒 , 𝑑π‘₯ =
π‘₯
∫ (𝑒)2
6
∫0
∗
𝑑𝑒
2π‘₯
π‘₯
(π‘₯ 2 −4)2
=∫
1
1
𝑑𝑒 = ∫ 𝑒
2𝑒2
2
𝑑
𝑑π‘₯ = π‘™π‘–π‘š− ∫0 (π‘₯ 2
𝑑→2
= π‘™π‘–π‘š− [−
𝑑→2
= π‘™π‘–π‘š− [(−
= π‘™π‘–π‘š− (−
𝑑→2
= π‘™π‘–π‘š− (−
𝑑→2
𝑒−2+1
2
−2+1
𝑑𝑒 = ∗
6
π‘₯
−4)2
𝑑π‘₯ + π‘™π‘–π‘š+ ∫𝑑
𝑑→2
] + π‘™π‘–π‘š+ [−
2(π‘₯ 2 −4) 0
𝑑→2
1
𝑑
1
= π‘™π‘–π‘š− [(−
𝑑→2
−2
2π‘₯
𝑑→2
1
π‘₯
(π‘₯ 2 −4)2
1
]
2
2𝑒
=−
1
2(π‘₯ 2 −4)
𝑑π‘₯
6
1
1
1
) − (− 2(02 −4))] + π‘™π‘–π‘š+ [(− 2(62 −4)) − (− 2(𝑑 2 −4))]
2(𝑑 2 −4)
𝑑→2
1
1
1
1
) − 8] + π‘™π‘–π‘š+ [(− 64) + 2(𝑑 2 −4)]
2(𝑑 2 −4)
𝑑→2
1
1
1
1
) − π‘™π‘–π‘š− 8 − π‘™π‘–π‘š− 64 + π‘™π‘–π‘š− 2(𝑑 2 −4)
2(𝑑 2 −4)
𝑑→2
1
1
𝑑→2
𝑑→2
1
1
) − 8 − 64 + π‘™π‘–π‘š− 2(22 −4)
2(22 −4)
𝑑→2
1
1
𝑑→2
1
1
𝑑→2
1
1
8
64
= −∞ − −
+∞
Then: this improper integral Diverged
Page | 110
1
2(π‘₯ 2 −4) 𝑑
= π‘™π‘–π‘š− (−
) − 8 − 64 + π‘™π‘–π‘š− 2∗(0)
2∗(0)
Choice B
1
= − 𝑒−1 = −
∞ 𝟏
120] Determine ∫𝟏
π’™πŸ
𝒅𝒙 converges or diverges , if converges Find
its value .
A- Converged at −𝟏
B- Diverged at −∞
πŸ’
C- Converged at πŸ’
D- Converged at 𝟎
Solution:
∞ 1
∫1
π‘₯2
𝑑π‘₯ , at π‘₯ = ∞ βž”
∞ 1
∫1 π‘₯ 2 𝑑π‘₯
=
1
= 𝑒𝑛𝑑𝑒𝑓𝑖𝑛𝑒𝑑
∞2
𝑑 1
π‘™π‘–π‘š− ∫1 2 𝑑π‘₯
π‘₯
𝑑→∞
=
𝑑
π‘™π‘–π‘š− ∫1 π‘₯ −2 𝑑π‘₯
𝑑→∞
1
1
1
= π‘™π‘–π‘š− [
𝑑→∞
π‘₯ −2+1
𝑑
1 𝑑
] = π‘™π‘–π‘š− [− ]
−2+1 1
𝑑→∞
π‘₯ 1
= π‘™π‘–π‘š− [(− ) − (− )] = π‘™π‘–π‘š− [(− ) + 1]
𝑑
1
𝑑
𝑑→∞
𝑑→∞
1
1
= π‘™π‘–π‘š− (− ) + π‘™π‘–π‘š− 1 = − π‘™π‘–π‘š− ( ) + 1
𝑑
∞
𝑑→∞
𝑑→∞
𝑑→∞
=0+1=1
Then: this improper integral Converged
Choice C
∞ 𝟏
121] Determine ∫𝟏
πŸ’
√𝒙
𝒅𝒙 converges or diverges , if converges Find
its value .
A- Converged at −𝟏
B- Diverged at −∞
C- Converged at πŸ’
D- Diverged at ∞
Solution:
∞ 1
∫1
4
√π‘₯
∞ 1
∫1
4
√π‘₯
𝑑π‘₯ , at π‘₯ =
1
∞
𝑑 1
𝑑π‘₯ = π‘™π‘–π‘š− ∫1
Page | 111
𝑑→∞
4
√π‘₯
𝑑 1
𝑑π‘₯ = π‘™π‘–π‘š− ∫1
𝑑→∞
1
π‘₯4
𝑑
𝑑π‘₯ = π‘™π‘–π‘š− ∫1 π‘₯
𝑑→∞
1
−4
1
− +1
π‘₯ 4
1
𝑑→∞− −4+1
𝑑π‘₯ = π‘™π‘–π‘š [
𝑑
]
1
𝑑
3
= π‘™π‘–π‘š− [
π‘₯4
𝑑→∞
3
4
] =
1
4
3
4
𝑑
π‘™π‘–π‘š [π‘₯ ] =
3 𝑑→∞−
1
4
3
4
3
4
π‘™π‘–π‘š [(𝑑 ) − (1 )] = ∞
3 𝑑→∞−
Then: this improper integral Diverged
Choice D
∞
𝟏
122] Determine ∫𝟐𝟐 𝒆𝒙 +πŸ• 𝒅𝒙 converges or diverges , if converges Find
its value .
A- Converged at −𝟏
B- Diverged at −∞
C- Converged at πŸ’
D- Diverged
Solution:
∞
1
1
1
∫22 𝑒 π‘₯+7 𝑑π‘₯ , at π‘₯ = ∞ βž” 𝑒 ∞ +7 = ∞ = 𝑒𝑛𝑑𝑒𝑓𝑖𝑛𝑒𝑑
1
∫ 𝑒 π‘₯ +7 𝑑π‘₯ , 𝑒 = 𝑒 π‘₯ + 7 , 𝑒 π‘₯ = 𝑒 − 7 , 𝑑𝑒 = 𝑒 π‘₯ 𝑑π‘₯ , 𝑑π‘₯ =
1
1
𝑑𝑒
𝑑𝑒
𝑒π‘₯
1
∫ 𝑒 π‘₯ +7 𝑑π‘₯ = ∫ 𝑒 ∗ 𝑒 π‘₯ = ∫ 𝑒(𝑒−7) 𝑑𝑒
1
=
𝑒(𝑒−7)
A
𝑒
+
B
𝑒−7
By multiplying in two sides by : 𝑒(𝑒 − 7)
βž” 1 = A(𝑒 − 7) + B𝑒
At 𝒖 = πŸ• βž” 1 = 0 + B ∗ 7 , then: B =
1
7
At 𝒖 = 𝟎 βž”1 = A(0 − 7) , then: A = −
Then:
1
𝑒(𝑒−7)
=−
1
1
+
7𝑒
1
1
7
1
7(𝑒−7)
1
1
1
∫ 𝑒(𝑒−7) 𝑑𝑒 = ∫ (− 7𝑒 + 7(𝑒−7)) 𝑑𝑒 = − ∫ 7𝑒 𝑑𝑒 + ∫ 7(𝑒−7)
1
1
1
1
= − ∫ 𝑑𝑒 + ∫ (𝑒−7)
7 𝑒
7
Page | 112
1
1
1
1
7
7
7
7
= − ln|𝑒| + ln|𝑒 − 7| = − ln|𝑒 π‘₯ + 7| + ln|𝑒 π‘₯ + 7 − 7|
1
1
7
7
= − ln|𝑒 π‘₯ + 7| + ln|𝑒 π‘₯ |
∞ 1
βž”∫22 π‘₯ 𝑑π‘₯
𝑒 +7
=
𝑑
1
π‘™π‘–π‘š− ∫22 π‘₯ 𝑑π‘₯
𝑒 +7
𝑑→∞
1
1
π‘₯
π‘₯|
= π‘™π‘–π‘š− [− ln|𝑒 + 7| + ln|𝑒 ]
𝑑→∞
7
7
1
1
1
7
7
7
𝑑
22
= π‘™π‘–π‘š− [(− ln|𝑒 ∞ + 7| + ln|𝑒 ∞ |) − (− ln|𝑒 22 + 7| +
𝑑→∞
1
7
ln|𝑒 22 |)]
1
1
7
7
= π‘™π‘–π‘š− [(−∞ + ∞) − ( ln|𝑒 22 + 7| − ln|𝑒 22 |)]
𝑑→∞
Then: this improper integral Diverged
Choice D
∞ 𝟏
123] Determine ∫𝟐
𝒙−𝟏
𝒅𝒙 converges or diverges , if converges Find
its value .
A- Converged at −𝟏
B- Diverged at ∞
C- Converged at πŸ’
D- None of them
Solution:
∞ 1
∫2
π‘₯−1
𝑑π‘₯ , at π‘₯ = ∞ βž”
1
∞−1
=
1
∞
= 𝑒𝑛𝑑𝑒𝑓𝑖𝑛𝑒𝑑
1
∫ π‘₯−1 = ln|π‘₯ − 1|
∞ 1
∫2
π‘₯−1
𝑑 1
𝑑π‘₯ = π‘™π‘–π‘š− ∫2
𝑑→∞
π‘₯−1
𝑑π‘₯ = π‘™π‘–π‘š−[ln|π‘₯ − 1|]𝑑2 = π‘™π‘–π‘š−[(ln|𝑑 − 1|) −
𝑑→∞
𝑑→∞
(ln|2 − 1|)]
= π‘™π‘–π‘š−[(ln|𝑑 − 1|) − (ln|2 − 1|)] = ∞ − 0 = ∞
𝑑→∞
Then: this improper integral Diverged
Choice B
Page | 113
𝟎
𝟏
124] Determine ∫−∞ πŸ“π’™ 𝒅𝒙 converges or diverges , if converges Find
its value .
A- Converged at −𝟏
B- Diverged at ∞
C- ∞
D- None of them
Solution:
0
1
5−π‘₯
0
∫−∞ 5π‘₯ 𝑑π‘₯ = ∫−∞ 5−π‘₯ 𝑑π‘₯ = [−1∗ln 5]
= [(−
= [(−
0
−∞
= [−
1
ln 5∗5
π‘₯]
0
−∞
1
) − (− ln 5∗5−∞)]
ln 5∗50
1
1
1
5∞
1
) + ln 5∗5−∞] = − ln 5 + ln 5 = − ln 5 + ∞ = ∞
ln 5
Then: this improper integral Diverged
Page | 114
1
Choice C
125] Write the equation πŸ•π’™πŸ + πŸ‘π’šπŸ = πŸ”πŸ‘ in standard form and
sketch a graph of the ellipse
A-
π’™πŸ
π’šπŸ
+ 𝟐𝟏 = 𝟏
B-
C- πŸ•π’™πŸ + πŸ‘π’šπŸ = 𝟏
D-
πŸ—
π’™πŸ
πŸ—
π’™πŸ
πŸ—
π’šπŸ
− 𝟐𝟏 = 𝟏
π’š
+ 𝟐𝟏 = 𝟏
Solution:
7π‘₯ 2 + 3𝑦 2 = 63 , By dividing 63 in two sides
7π‘₯ 2 +3𝑦2 =63
63
7π‘₯ 2
63
+
3𝑦 2
63
=
=
π‘₯2
9
7π‘₯ 2
63
+
+
𝑦2
21
3𝑦 2
63
=1
= 1 βž” its called Standard Form
π‘Ž2 = 21 βž” π‘Ž = √21
𝑏 2 = 9 βž” 𝑏 = √9 = 3
𝑐 = √π‘Ž2 − 𝑏 2 = √21 − 9 = √12 = 2√3
(𝟎, √𝟐𝟏)
π’—πŸ
1] Center = (0,0)
2] Major axis βž” 𝑦 − π‘Žπ‘₯𝑖𝑠
π’‡πŸ
3] π‘Ž = √21 ≈ 4.58 , 𝑏 = 3
4] 𝑐 = 2√3 ≈ 3.46
(𝟎, 𝟐√πŸ‘)
(𝟎, 𝟎)
(πŸ‘, 𝟎)
(−πŸ‘, 𝟎)
Choice A
(𝟎, −𝟐√πŸ‘)
π’‡πŸ
(𝟎, −√𝟐𝟏)
Page | 115
π’—πŸ
126] If the length of the horizontal axis of an ellipse is 20 and the
length of the vertical axis is 16 , Write the equation of the ellipse
centered at the origin in standard form .
π’™πŸ
π’šπŸ
π’™πŸ
πŸ–π’šπŸ
π’™πŸ
A- 𝟏𝟎𝟎 − πŸ”πŸ’ = 𝟏
C- 𝟏𝟎𝟎 +
πŸ”πŸ’
π’šπŸ
B- 𝟏𝟎𝟎 + πŸ”πŸ’
=𝟏
D- None of them
Solution:
The horizontal axis = 20
Then : 2π‘Ž = 20 , π‘Ž = 10
The vertical axis = 16
Then : 2𝑏 = 16 , 𝑏 = 8
βž” 𝑐 = √π‘Ž2 − 𝑏 2 = √102 − 82 = 6
Center = (0,0)
Then: The Standard Form =
Choice D
Page | 116
π‘₯2
100
+
𝑦2
64
= 1 , Because π‘₯ π‘Žπ‘₯𝑖𝑠 is the major axis
127] Write the equation πŸπ’™πŸ + πŸ–π’šπŸ − πŸπŸŽπ’™ + πŸ’πŸ–π’š = −πŸπŸŽπŸ” in
Standard Form .
AC-
π’™πŸ
+
πŸ–
(π’š+πŸ‘)𝟐
(𝒙−πŸ“)𝟐
πŸ–
=𝟏
𝟐
+
(π’š+πŸ‘)𝟐
𝟐
B-
=𝟏
(𝒙−πŸ“)𝟐
πŸ–
−
(π’š+πŸ‘)𝟐
𝟐
D- None of them
Solution:
→ 2π‘₯ 2 + 8𝑦 2 − 20π‘₯ + 48𝑦 = −106
→ 2π‘₯ 2 − 20π‘₯ + 8𝑦 2 + 48𝑦 = −106
βž” 2(π‘₯ 2 − 10π‘₯ ) + 8(𝑦 2 + 6𝑦) = −106
By Completing Squaring
2((π‘₯ − 5)2 − 25) + 8((𝑦 + 3)2 − 9)
2(π‘₯ − 5)2 − 50 + 8(𝑦 + 3)2 − 72 = −106
2(π‘₯ − 5)2 + 8(𝑦 + 3)2 = −106 + 72 + 50
2(π‘₯ − 5)2 + 8(𝑦 + 3)2 = 16
By Dividing 16
(π‘₯−5)2
8
(π‘₯−5)2
8
+
+
(𝑦+3)2
2
(𝑦+3)2
2
= 1 βž” Standard Form of the ellipse
=
(π‘₯−5)2
8
2
+
(𝑦−(−3))
2
=
(π‘₯−β„Ž)2
π‘Ž2
+
(𝑦−π‘˜)2
𝑏2
Then: β„Ž = 5 , π‘˜ = −3 , π‘Ž2 = 8 βž” π‘Ž = √8 = 2√2 , 𝑏 2 = 2 βž” 𝑏 = √2
𝑐 = √π‘Ž2 − 𝑏 2 = √8 − 2 = √6
Then: Major axis is Parallel to X-axis
Length of major axis = 2π‘Ž = 4√2
Length of minor axis = 2𝑏 = 2√2
Page | 117
Choice C
128] Write the equation of the ellipse in Standard Form of the
vertices of the ellipse (𝟐, πŸπŸ—) , (𝟐, −πŸ•) and Co vertices of the Ellipse
(−πŸ‘, πŸ”) , (πŸ•, πŸ”)
(𝒙−𝟐)𝟐
AC-
(πŸπŸ‘)𝟐
(𝒙−𝟐)𝟐
(πŸ“ )𝟐
+
+
(π’š−πŸ”)𝟐
(πŸ“ )𝟐
(π’š−πŸ”)𝟐
(πŸπŸ‘)𝟐
(𝒙−𝟐)𝟐
=𝟏
B-
=𝟏
D- None of them
(πŸ“ )𝟐
+
(π’š−πŸ”)𝟐
(πŸπŸ‘)𝟐
Solution:
Since the vertices is (2,19) , (2, −7) , Then the major axis is Parallel to Y-axis
Co-vertices is (−3,6) , (7,6) , Then the minor axis is parallel to X-axis
π‘₯1 +π‘₯2 𝑦1 +𝑦2
Midpoint = (
2
,
2
2+2 19−7
)=(
,
2
2
4 12
) = (2 ,
2
) = (2,6)
OR
π‘₯1 +π‘₯2 𝑦1 +𝑦2
Midpoint = (
2
,
2
−3+7 6+6
)=(
2
,
2
4 12
) = (2 ,
2
) = (2,6)
Then: Center = (2,6) βž” β„Ž = 2 , π‘˜ = 6
(2,19)
Length of major axis = 2π‘Ž = 19 + 7 = 26 βž” π‘Ž = 13
Length of minor axis = 2𝑏 = 3 + 7 = 10 βž” 𝑏 = 5
The Standard Form is
βž”
(π‘₯−β„Ž)2
𝑏2
Choice C
Page | 118
+
(𝑦−π‘˜)2
π‘Ž2
=
(π‘₯−β„Ž)2
𝑏2
(π‘₯−2)2
(5)2
+
+
(𝑦−π‘˜)2
π‘Ž2
(𝑦−6)2
(13)2
=1
=1
(−3,6)
(β„Ž, π‘˜)
(7,6)
129] If the length of the horizontal axis is πŸ– and the length of the
vertical axis is 𝟏𝟎 , what is the equation of the ellipse centered at the
origin ?
π’™πŸ
A- πŸπŸ“ +
π’™πŸ
π’šπŸ
πŸ’
=𝟏
π’™πŸ
π’šπŸ
B- πŸπŸ“ − πŸπŸ” = 𝟏
π’šπŸ
C- πŸπŸ” + πŸπŸ“ = 𝟏
D- None of them
Solution:
The vertical axis = 10 , then: 2π‘Ž = 10 βž” π‘Ž = 5
The horizontal axis = 8 , then: 2𝑏 = 8 βž” 𝑏 = 4
𝑐 = √π‘Ž2 − 𝑏 2 = √52 − 42 = 3
Center = (0,0)
Then : The Standard equation =
Choice C
Page | 119
π‘₯2
𝑦2
𝑏
π‘Ž2
2 +
=1βž”
π‘₯2
𝑦2
4
52
2 +
=1
130] Write the equation of the ellipse with vertices (−πŸ‘, 𝟏) , (𝟏, 𝟏)
and co-vertices (−𝟏, 𝟐) , (−𝟏, 𝟎) .
AC-
(𝒙+𝟏)𝟐
πŸ’
(𝒙+𝟏)𝟐
πŸ’
+
(π’š−𝟏)𝟐
𝟏
= 𝟐𝟎
B-
(𝒙+𝟏)𝟐
πŸ’
+ (π’š − 𝟏)𝟐 = 𝟏
−
(π’š−𝟏)𝟐
𝟏
=𝟏
D- None of them
Solution:
Since The vertex is (−3,1) , (1,1) , then: the major axis is parallel to X-axis
The co-vertex is (−1,2) , (−1,0) , then: the major axis is parallel to Y-axis
Midpoint = (
π‘₯1 +π‘₯2 𝑦1 +𝑦2
2
,
2
)=(
−3+1 1+1
2
,
2
−1+(−1) 2+0
) = (−1,1) OR (
2
βž” Center = (−1,1) , then: β„Ž = −1 , π‘˜ = 1
The length of the major axis = 2π‘Ž = 3 + 1 = 4 βž” π‘Ž = 2
The length of the minor axis = 2𝑏 = 1 + 1 = 2 βž” 𝑏 = 1
The Standard Form =
βž”
(π‘₯−β„Ž)2
π‘Ž2
Choice C
Page | 120
+
(𝑦−π‘˜)2
𝑏2
(π‘₯−β„Ž)2
π‘Ž2
+
(𝑦−π‘˜)2
2
=
(π‘₯−(−1))
22
+
𝑏2
(𝑦−1)2
12
=1
=
(π‘₯+1)2
4
+
(𝑦−1)2
1
=1
,
2
) = (−1,1)
131] Write the equation π’™πŸ + πŸ’π’šπŸ = πŸ– in Standard Form .
AC-
π’™πŸ
πŸ–
π’™πŸ
πŸ–
+
−
π’šπŸ
𝟐
π’šπŸ
𝟐
π’™πŸ
+
π’šπŸ‘
=𝟏
B-
=𝟏
D- None of them
πŸ–
𝟐
=𝟏
Solution:
βž”
π‘₯ 2 +4𝑦 2 =8
8
=
π‘₯2
8
+
4𝑦 2
8
8
π‘₯2
8
8
= βž”
+
𝑦2
=1
2
Choice A
132] Write the equation πŸπŸ“π’™πŸ + πŸ’π’šπŸ + πŸ“πŸŽπ’™ − πŸ‘πŸπ’š = 𝟏𝟏 in
Standard Form .
AC-
(𝒙+𝟏)𝟐
πŸ’
(𝒙+𝟏)𝟐
πŸ’
+
+
(π’š−πŸ’)𝟐
πŸπŸ“
=𝟏
(π’š−πŸ’)𝟐
πŸ’
B-
(𝒙+𝟏)𝟐
𝟏𝟎𝟎
+
(π’š−πŸ’)𝟐
πŸπŸ“
=𝟏
D- None of them
Solution:
25π‘₯ 2 + 4𝑦 2 + 50π‘₯ − 32𝑦 = 11 βž” 25π‘₯ 2 + 50π‘₯ + 4𝑦 2 − 32𝑦 = 11
→ 25(π‘₯ 2 + 2π‘₯ ) + 4(𝑦 2 − 8𝑦) = 11
→ 25((π‘₯ + 1)2 − 1 ) + 4((𝑦 − 4)2 − 16) = 11
→ 25(π‘₯ + 1)2 − 25 + 4(𝑦 − 4)2 − 4 ∗ 16 = 11
→ 25(π‘₯ + 1)2 − 25 + 4(𝑦 − 4)2 − 64 − 11 = 0
→ 25(π‘₯ + 1)2 + 4(𝑦 − 4)2 − 100 = 0
→ 25(π‘₯ + 1)2 + 4(𝑦 − 4)2 = 100
Page | 121
→ 25(π‘₯ + 1)2 + 4(𝑦 − 4)2 = 100
→
→
25(π‘₯+1)2
100
(π‘₯+1)2
4
Choice A
Page | 122
+
+
4(𝑦−4)2
100
(𝑦−4)2
25
=
=1
100
100
Dividing by 𝟏𝟎𝟎
133] Find the vertex, focus and directrix of the parabola π’šπŸ = πŸπŸ”π’™
respectively
A- (𝟎, 𝟎) , (−πŸ’, 𝟎) , πŸ’
B- (𝟎, 𝟎) , (πŸ’, 𝟎) , −πŸ’
C- the origin point , (πŸ’, 𝟎) , πŸ’
D- None of them
Solution:
Axis of Symmetry is on π‘₯ − π‘Žπ‘₯𝑖𝑠
βž” (𝑦 − π‘˜)2 = ±4𝑝(π‘₯ − β„Ž) βž” 𝑦 2 = 16π‘₯
Then: (𝑦 − π‘˜)2 = 𝑦 2 βž” π‘˜ = 0
Then: 4𝑝(π‘₯ − β„Ž) = 16π‘₯ βž” β„Ž = 0 , 4𝑝 = 16 → 𝑝 = 4
Then: 𝒗𝒆𝒓𝒕𝒆𝒙 = (β„Ž, π‘˜) = (0,0)
Since 𝑝 = 4 & Sign (+)
Then: 𝒇𝒐𝒄𝒖𝒔 = (β„Ž + 𝑝, π‘˜) = (0 + 4,0) = (4,0)
The π‘«π’Šπ’“π’†π’„π’•π’“π’Šπ’™ βž” π‘₯ = β„Ž − 𝑝 → π‘₯ = 0 − 4 = −4
Choice B
Page | 123
134] Find the vertex, focus and directrix of the parabola
respectively
A- (𝟎, 𝟎) , (−πŸ’, πŸ–) , −πŸ’
B- (𝟎, 𝟏) , (πŸ“, 𝟎) , −𝟐
C- the origin point , (−𝟐, 𝟎) , 𝟐
D- None of them
Solution:
βž”
−𝑦 2
8
= π‘₯ → −𝑦 2 = 8π‘₯ → 𝑦 2 = −8π‘₯
Axis of Symmetry is on 𝒙 − π’‚π’™π’Šπ’”
βž” (𝑦 − π‘˜)2 = ±4𝑝(π‘₯ − β„Ž) βž” 𝑦 2 = −8π‘₯
Then: (𝑦 − π‘˜)2 = 𝑦 2 βž” π‘˜ = 0
Then: 4𝑝(π‘₯ − β„Ž) = −8π‘₯ βž” β„Ž = 0 , 4𝑝 = 8 → 𝑝 = 2
Then: 𝒗𝒆𝒓𝒕𝒆𝒙 = (β„Ž, π‘˜) = (0,0)
Since 𝑝 = 2 & Sign (−)
Then: 𝒇𝒐𝒄𝒖𝒔 = (β„Ž − 𝑝, π‘˜) = (0 − 2,0) = (−2,0)
The π‘«π’Šπ’“π’†π’„π’•π’“π’Šπ’™ βž” π‘₯ = β„Ž + 𝑝 → π‘₯ = 0 + 2 = 2
Choice C
Page | 124
−π’šπŸ
πŸ–
=𝒙
135] Find the vertex, focus and directrix of the equation
𝟏
π’š = (π’™πŸ − πŸ’π’™ + 𝟐𝟐) respectively
πŸ”
A- (𝟎, 𝟎) , (−πŸ’, πŸ–) , −πŸ’
πŸ•
B- (𝟎, 𝟎) , (𝟐 , πŸ‘) , 𝟎
πŸ—
πŸ‘
C- (𝟐, πŸ‘) , (πŸ‘, 𝟐) , 𝟐
D- None of them
Solution:
1
𝑦 = (π‘₯ 2 − 4π‘₯ + 22) → 6𝑦 = π‘₯ 2 − 4π‘₯ + 22
6
π‘₯ 2 − 4π‘₯ + 22 = [(π‘₯ − 2)2 − 4] + 22
βž” 6𝑦 = π‘₯ 2 − 4π‘₯ + 22
By Completing Squaring
= [(π‘₯ − 2)2 − 4] + 22 = (π‘₯ − 2)2 + 18
6
3
4
2
6𝑦 − 18 = (π‘₯ − 2)2 → 6(𝑦 − 3) = (π‘₯ − 2)2 βž” 4𝑝 = 6 → 𝑝 = =
Then: 𝒗𝒆𝒓𝒕𝒆𝒙 = (β„Ž, π‘˜) = (2,3)
3
Since 𝑝 = & Sign (+)
2
3
9
Then: 𝒇𝒐𝒄𝒖𝒔 = (β„Ž, π‘˜ + 𝑝) = (2,3 + ) = (2, )
2
2
3
3
2
2
The π‘«π’Šπ’“π’†π’„π’•π’“π’Šπ’™ βž” 𝑦 = π‘˜ − 𝑝 → 𝑦 = 3 − =
Choice D
Page | 125
136] The point (𝟎, πŸ•) is the focus of a parabola that its vertex (𝟐, πŸ•).
Find the equation of the parabola.
A- (π’š − πŸ•)𝟐 = −πŸ–(𝒙 − 𝟐)
B- (π’š − πŸ•)𝟐 = πŸ–(𝒙 − 𝟐)
C- (π’š − πŸ•)𝟐 = −πŸ–(𝒙 + 𝟐)
D- None of them
Solution:
𝒗𝒆𝒓𝒕𝒆𝒙 = (β„Ž, π‘˜) = (2,7)
𝒇𝒐𝒄𝒖𝒔 = (0,7)
1] Axis of symmetry is parallel to π‘₯ − π‘Žπ‘₯𝑖𝑠
2] π‘£π‘’π‘Ÿπ‘‘π‘’π‘₯ = (2,7)
3] Since π‘£π‘’π‘Ÿπ‘‘π‘’π‘₯ = (2,7) & πΉπ‘œπ‘π‘’π‘  = (0,7) , then 2 → 0 βž” Sign (−)
4] πΉπ‘œπ‘π‘’π‘  = (2 − 𝑝, 7) → 𝑝 = 2
(𝑦 − π‘˜)2 = ±4𝑝(π‘₯ − β„Ž)
(𝑦 − π‘˜)2 = ±4𝑝(π‘₯ − β„Ž) → (𝑦 − 7)2 = −4 ∗ 2(π‘₯ − 2)
→ (π’š − πŸ•)𝟐 = −πŸ–(𝒙 − 𝟐)
Choice A
Page | 126
137] The point (πŸ”, 𝟐) is the vertex of a parabola that its Directrix
equals 𝒙 = πŸ’ . Find the equation of the parabola.
A- (π’š − 𝟐)𝟐 = πŸ–(𝒙 − πŸ”)
B- (π’š − 𝟐)𝟐 = −πŸ–(𝒙 − πŸ”)
C- (π’š − 𝟐)𝟐 = 𝟐(𝒙 − πŸ”)
D- None of them
Solution:
Since the Directrix βž” π‘₯ = 4
Then: the equation βž” (𝑦 − π‘˜)2 = ±4𝑝(π‘₯ − β„Ž)
Since the 𝒗𝒆𝒓𝒕𝒆𝒙 = (6,2) βž” β„Ž = 6 , π‘˜ = 2
π‘«π’Šπ’“π’†π’„π’•π’“π’Šπ’™ βž” π‘₯ = 4
From the sketch
(πŸ”, 𝟐)
Then: 𝑝 → (+) 𝑠𝑖𝑔𝑛
π‘«π’Šπ’“π’†π’„π’•π’“π’Šπ’™ βž” π‘₯ = 4 = β„Ž − 𝑝 → 6 − 𝑝 = 4
Then: 𝑝 = 2
𝑻𝒉𝒆 π’†π’’π’–π’‚π’•π’Šπ’π’
βž” (𝑦 − 2)2 = 4 ∗ 2(π‘₯ − 6)
→ (𝑦 − 2)2 = 8(π‘₯ − 6)
Choice A
Page | 127
Equation: 𝒙 = πŸ’
(𝟎, 𝟎)
(πŸ’, 𝟎)
138] Find the vertex, focus and directrix of the parabola
π’šπŸ = πŸπŸπ’™ − πŸ–π’š + πŸ– respectively .
A- (−𝟐, −πŸ’) , (−𝟏, πŸ’) , −πŸ“
B- (−𝟐, −πŸ’) , (𝟏, −πŸ’) , πŸ“
C- (−𝟐, −πŸ’) , (𝟏, −πŸ’) , −πŸ“
D- None of them
Solution:
𝑦 2 = 12π‘₯ − 8𝑦 + 8 βž” 𝑦 2 + 8𝑦 = 12π‘₯ + 8
𝑦 2 + 8𝑦
By Completing Squaring
→ (𝑦 + 4)2 − 16
Then: (𝑦 + 4)2 − 16 = 12π‘₯ + 8 βž” (𝑦 + 4)2 = 12π‘₯ + 8 + 16
βž” (𝑦 + 4)2 = 12π‘₯ + 24 βž” (𝑦 + 4)2 = 12(π‘₯ + 2)
Since the equation: (𝑦 − π‘˜)2 = ±4𝑝(π‘₯ − β„Ž) → (𝑦 + 4)2 = 12(π‘₯ + 2)
π‘˜ = −4 , β„Ž = −2 , 𝑝 =
12
4
= 3 , 𝑠𝑖𝑔𝑛 = (+)
Then: 𝒗𝒆𝒓𝒕𝒆𝒙 = (β„Ž, π‘˜) = (−2, −4)
Since 𝑝 = 3 & Sign (+)
Then: 𝒇𝒐𝒄𝒖𝒔 = (β„Ž + 𝑝, π‘˜) = (−2 + 3, −4) = (1, −4)
The π‘«π’Šπ’“π’†π’„π’•π’“π’Šπ’™ βž” π‘₯ = β„Ž − 𝑝 → π‘₯ = −2 − 3 = −5
Choice C
Page | 128
139] Find the vertex, focus and directrix of the parabola π’š =
π’™πŸ
respectively .
A- (𝟎, 𝟎) , (𝟏, 𝟎) , −πŸ“
B- the origin point , (𝟎, 𝟏) , −𝟐
C- (𝟎, 𝟎) , (𝟏, 𝟎) , −𝟏
D- None of them
Solution:
𝑦=
π‘₯2
4
βž” π‘₯ 2 = 4𝑦
(π‘₯ − β„Ž)2 = ±4𝑝(𝑦 − π‘˜) → β„Ž = 0 , π‘˜ = 0 , 4𝑝 = 4 βž” 𝑝 = 1 & Sign (+)
Then: 𝒗𝒆𝒓𝒕𝒆𝒙 = (β„Ž, π‘˜) = (0,0)
Since 𝑝 = 1 & Sign (+)
Then: 𝒇𝒐𝒄𝒖𝒔 = (β„Ž, π‘˜ + 𝑝) = (0,0 + 1) = (0,1)
The π‘«π’Šπ’“π’†π’„π’•π’“π’Šπ’™ βž” 𝑦 = π‘˜ − 𝑝 → 𝑦 = 0 − 1 = −1
Choice D
Page | 129
πŸ’
140] Find the sum of the first n-terms of series : 𝟏 ∗ πŸ‘ + 𝟐 ∗ πŸ’ + πŸ‘ ∗ πŸ“ + β‹―
Solution:
π‘’π‘˜ = π‘˜ (π‘˜ + 2) βž” π‘’π‘˜ = π‘˜ 2 + 2π‘˜
∑π‘›π‘˜=1 π‘’π‘˜ = ∑π‘›π‘˜=1 π‘˜ 2 + 2 ∑π‘›π‘˜=1 π‘˜
∑π‘›π‘˜=1 π‘’π‘˜ =
𝑛(𝑛+1)(2𝑛+1)
∑π‘›π‘˜=1 π‘’π‘˜ =
𝑛(𝑛+1)(2𝑛+1)
6
6
+2∗
+
𝑛(𝑛+1)
2
6∗𝑛(𝑛+1)
6
=
𝑛(𝑛+1)(2𝑛+1)
6
+ 𝑛(𝑛 + 1)
𝑛(𝑛+1)(2𝑛+1)+6𝑛(𝑛+1)
=
6
=
=
(𝑛(𝑛+1))[(2𝑛+1)+6]
6
(𝑛(𝑛+1))(2𝑛+7)
6
141] Find the sum of the first n-terms of series : πŸ‘ ∗ 𝟏𝟐 + πŸ’ ∗ 𝟐𝟐 + πŸ“ ∗ πŸ‘πŸ + β‹―
Solution:
π‘’π‘˜ = (π‘˜ + 2)π‘˜ 2 βž” π‘’π‘˜ = π‘˜ 3 + 2π‘˜ 2
∑π‘›π‘˜=1 π‘’π‘˜ = ∑π‘›π‘˜=1 π‘˜ 3 + 2 ∑π‘›π‘˜=1 π‘˜ 2
∑π‘›π‘˜=1 π‘’π‘˜
=
=
=
Page | 130
𝑛2 (𝑛+1)2
4
+2∗
𝑛(𝑛+1)(2𝑛+1)
6
=
3∗(𝑛2 (𝑛+1)2 )+4(𝑛(𝑛+1)(2𝑛+1))
4∗3
𝑛(𝑛+1)[3𝑛(𝑛+1)+4(2𝑛+1)]
12
=
𝑛2 (𝑛+1)2
=
4
+
𝑛(𝑛+1)(2𝑛+1)
3
3𝑛2 (𝑛+1)2 +4𝑛(𝑛+1)(2𝑛+1)
12
𝑛(𝑛+1)[3𝑛2 +3𝑛+8𝑛+4]
12
=
𝑛(𝑛+1)[3𝑛2 +11𝑛+4]
12
𝟏
𝟏
𝟏
𝟏
𝟏
142] Test the convergence of the series : ∑∞
𝒏=𝟏 πŸπ’−𝟏 = 𝟏 + 𝟐 + πŸ’ + πŸ– + β‹― + πŸπ’−𝟏
Solution:
∑∞
𝑛=1
1
2𝑛−1
1
1
1
1
2
4
8
2𝑛−1
= 1 + + + + β‹―+
1
1
1
1
1
1
2
4
2
8
4
2
Then: π‘Ž = 1 , π‘Ÿ = ÷ 1 = ÷ = ÷ =
1
Since |π‘Ÿ| = < 1 βž” then it is converge
2
S𝑛 =
π‘Ž
1−π‘Ÿ
=
1
1
1−2
=
1
1
2
=2
143] Discuss the nature of the series : ∑∞𝒏=𝟏(−𝟏)𝒏−𝟏 = 𝟏 − 𝟏 + 𝟏 − 𝟏 + β‹― + (−𝟏)𝒏−𝟏 + β‹―
Solution:
S1 = 1
0 𝑒𝑣𝑒𝑛
S2 = 1 − 1 = 0
S𝑛 = {
S3 = 1 − 1 + 1 = 1
1 π‘œπ‘‘π‘‘
S4 = 1 − 1 + 1 − 1 = 0
Then the given series is Oscillating
−𝒏+𝟐
144] Discuss the nature of the series : ∑∞
∗ πŸ’π’+𝟏
𝒏=𝟏 πŸ—
Solution:
−𝑛+2
−(𝑛−2)
∑∞
∗ 4𝑛+1 = ∑∞
∗ 4𝑛+1 = ∑∞
𝑛=1 9
𝑛=1 9
𝑛=1
= ∑∞
𝑛=1
Then: π‘Ž = 16 ∗ 9 , π‘Ÿ =
Page | 131
4
9
4𝑛−1 ∗42 ∗91
9𝑛−1
4𝑛+1
9𝑛−2
= ∑∞
𝑛=1
4𝑛−1 ∗42
9𝑛−1 ∗9−1
4 𝑛−1
= ∑∞
𝑛=1 16 ∗ 9 ∗ (9)
4 𝑛−1
∑∞
𝑛=1 16 ∗ 9 ∗ (9)
βž” S𝑛 =
π‘Ž
1−π‘Ÿ
=
16∗9
4
1−9
𝑛−1
= ∑∞
[Geometric Series]
𝑛=1 π‘Ž (π‘Ÿ)
16∗9
=
5
9
=
16∗92
5
=
1296
5
= 259.2
4
16∗92
9
5
Since |π‘Ÿ| = < 1 βž” then it is converge and its value equals
145] Determine if series converge or diverge , if converge find its
𝟏
value : ∑∞
𝒏=𝟎 𝟐
𝒏 +πŸ‘π’+𝟐
Solution:
∑∞
𝑛=0
1
1
𝑛2 +3𝑛+2
1
(𝑛+1)(𝑛+2)
= ∑∞
𝑛=0 (𝑛+1)(𝑛+2)
A
B
= (𝑛+1) + (𝑛+2)
By multiplying in two sides by : (𝒏 + 𝟏)(𝒏 + 𝟐)
1 = A(𝑛 + 2) + B(𝑛 + 1)
At 𝒏 = −𝟏 βž”1 = A(−1 + 2) + 0 → 1 = A(1) , then: A = 1
At 𝒏 = −𝟐 βž”1 = 0 + B(−2 + 1) → 1 = B(−1) , then: B = −1
1
1
1
Then: (𝑛+1)(𝑛+2) = (𝑛+1) − (𝑛+2)
1
1
−
)
(𝑛+1)
(𝑛+2)
∑∞
𝑛=0 (
1
(𝑛+1)
∑∞
𝑛=0 (
1
1
1
1
1
1
1
1
1
1
2
2
3
3
4
4
5
βž” S𝑛 = 1 −
1
𝑛+2
get the limit where 𝒏 approaches to ∞
1
lim S𝑛 = lim (1 −
) = 1 − lim
𝑛+2
𝑛→∞
Page | 132
1
1
− (𝑛+2)) = ( − ) + ( − ) + ( − ) + ( − ) + β‹― + ((𝑛+1) − (𝑛+2))
𝑛→∞
1
𝑛→∞ 𝑛+2
= 1 − 0 = 1 [Converges]
146] Determine if series converge or diverge , if converge find its
𝟏
value : ∑∞
𝒏=𝟏 𝟐
𝒏 +πŸ’π’+πŸ‘
Solution:
∑∞
𝑛=1
1
1
𝑛2 +4𝑛+3
1
(𝑛+1)(𝑛+3)
= ∑∞
𝑛=1 (𝑛+1)(𝑛+3)
A
B
= (𝑛+1) + (𝑛+3)
By multiplying in two sides by : (𝒏 + 𝟏)(𝒏 + πŸ‘)
1 = A(𝑛 + 3) + B(𝑛 + 1)
At 𝒏 = −πŸ‘ βž”1 = 0 + B(−3 + 1) → 1 = B(−2) , then: B = −
At 𝒏 = −𝟏 βž”1 = A(−1 + 3) → 1 = A(2) , then: A =
1
Then: (𝑛+1)(𝑛+3) =
1
∑∞
𝑛=1 (
2(𝑛+1)
−
1
2(𝑛+1)
1
2(𝑛+3)
−
1
2(6)
βž” S𝑛 =
1
2( 2
+
)
1
2( 3
1
1
+
)
2(𝑛+1)
1
1
−
−
−
1
)+(
2(4)
1
2(8)
1
2(3)
1
−
)+(
2(5)
Page | 133
5
12
+0−0=
1
2(4)
−
1
2(𝑛+3)
12
)+(
2(6)
1
2(5)
−
1
2(7)
)
get the limit where 𝒏 approaches to ∞
1
5
1
𝑛→∞ 2(𝑛+1)
5
1
1
1
−
)
2(𝑛+1)
2(𝑛+3)
𝑛→∞
=
2
) + β‹―+ (
lim S𝑛 = lim ( + +
−
) = 12 + lim
4
6
2(𝑛+1)
2(𝑛+3)
𝑛→∞
1
2(𝑛+3)
2(2)
+(
2
1
1
)=(
1
[Converges]
− lim
1
𝑛→∞ 2(𝑛+3)
πŸ–
πŸπŸ•
πŸ”πŸ’
147] Test Series 𝟏 − πŸ— + πŸπŸ– − πŸ”πŸ“ + β‹―
Solution:
𝑒𝑛 =
𝑛3
𝑛3 +1
βž” lim 𝑒𝑛 = lim
𝑛→∞
𝑛→∞
3
𝑛
= lim
𝑛3 +1
𝑛→∞
𝑛3
𝑛3
3
𝑛
1
+
𝑛3 𝑛3
= lim
𝑛→∞
1
1
1+ 3
𝑛
1
= 1+0 = 1 ≠ 0
[Diverges]
𝟏
148] Test Convergence ∑∞
𝒏=𝟏 𝒏
Solution:
∑∞
𝑛=1
1
𝑛1
, Since 𝑛 > 0 && 𝑝 = 1
Then: it is divergence
149] Test Convergence ∑∞
𝒏=𝟏
𝟏
√𝒏
Solution:
∑∞
𝑛=1
1
√𝑛
= ∑∞
𝑛=1
1
1
𝑛2
Then: it is divergence
Page | 134
1
, Since 𝑛 > 0 && 𝑝 = < 1
2
𝒏
150] Test Convergence ∑∞
𝒏=𝟏 π’πŸ −𝐜𝐨𝐬𝟐 𝒏
Solution:
∑∞
𝑛=1
𝑛
𝑛2 −cos2 𝑛
𝑛
𝑛2 −cos2 𝑛
1
𝑛
𝑛
>
𝑛2
=
1
𝑛
by using p-test
Since 𝒑 = 𝟏 , then: it is divergence
Then: ∑∞
𝑛=1
𝑛
𝑛2 −cos2 𝑛
is divergence
151] Test Convergence ∑∞
𝒏=𝟏
π’πŸ +𝟐
π’πŸ’ +πŸ“
Solution:
𝑛2 +2
𝑛4 +5
1
𝑛2
+
<
2
𝑛4
𝑛2 +2
𝑛4
𝑛2
=(
𝑛4
+
2
𝑛4
=
𝟏
π’πŸ
+
𝟐
π’πŸ’
)
by using p-test
Since 𝒑 = 𝟐 & 𝒑 = πŸ’ , then: convergence + convergence = convergence
Then:
𝑛2 +2
𝑛4 +5
Page | 135
is convergence
152] Test Convergence ∑∞
𝒏=𝟏
𝐬𝐒𝐧 𝒏
π’πŸ‘
Solution:
∑∞
𝑛=1
sin 𝑛
𝑛3
Since : −1 < sin 𝑛 < 1 βž” |sin 𝑛| = 1
∑∞
𝑛=1
|sin 𝑛|
𝑛3
= ∑∞
𝑛=1
1
𝑛3
By using p test
Since 𝒑 = πŸ‘ > 𝟏 , then: it is convergence
𝟏
𝟏
𝟏
𝟏
153] Test Convergence 𝟐 + πŸ“ + 𝟏𝟎 + πŸπŸ• + β‹―
Solution:
Then: π‘Žπ‘› =
∑∞
𝑛=1
1
𝑛2
1
𝑛2 +1
1
𝑛2 +1
, by using comparison βž”
1
𝑛2 +1
by using p test
Since 𝒑 = 𝟐 > 𝟏 , then: it is convergence
βž” ∑∞
𝑛=1
Page | 136
1
𝑛2 +1
is convergence
<
1
𝑛2
πŸπŸ’
𝟏
πŸ‘πŸ’
154] Test Convergence 𝒆 + π’†πŸ’ + π’†πŸ— + β‹― +
π’πŸ’
𝒆𝒏
𝟐
Solution:
π‘Žπ‘› =
π‘Žπ‘›+1
π‘Žπ‘›
𝑛4
𝑒𝑛
=
2
, π‘Žπ‘›+1 =
(𝑛+1)4
𝑒
(𝑛+1)2
÷
(𝑛+1)4
𝑒 (𝑛+1)
𝑛4
𝑒
=
𝑛2
2
(𝑛+1)4
𝑒
(𝑛+1)2
∗
𝑒𝑛
2
𝑛4
=(
𝑛+1 4
𝑛
) ∗
𝑒𝑛
𝑒
2
(𝑛+1)2
𝑛+1 4
=(
𝑛+1 4
=(
lim |
𝑛→∞
π‘Žπ‘›+1
π‘Žπ‘›
𝑛+1 4
| = lim |(
𝑛+1 4
) ∗ 𝑒 −2𝑛−1 = (
1+
1
) ∗ 𝑒 2𝑛+1 | = lim |(
𝑛
𝑛→∞
𝑛
𝑛→∞
𝒙
π’™πŸ
π’™πŸ‘
1
1
𝑛
Solution:
π‘Žπ‘› =
π‘Žπ‘›+1
π‘Žπ‘›
=
lim |
𝑛→∞
𝑛!
, π‘Žπ‘›+1 =
π‘₯ 𝑛+1
π‘₯𝑛
÷
(𝑛+1)!
𝑛!
π‘Žπ‘›+1
π‘Žπ‘›
Page | 137
π‘₯ 𝑛+1
(𝑛+1)!
=
| = lim |
π‘₯ 𝑛 ∗π‘₯
(𝑛+1)𝑛!
π‘₯
𝑛→∞ 𝑛+1
|=0
∗
𝑛!
π‘₯𝑛
=
π‘₯
𝑛+1
[converge]
𝑛
2 −(𝑛2 +2𝑛+1)
1
) ∗ 𝑒 2𝑛+1
4
1
) ∗ 𝑒 2𝑛+1 | = 0
155] Test Convergence 𝟏 + 𝟏! + 𝟐! + πŸ‘! + β‹―
π‘₯𝑛
𝑛
) ∗ 𝑒𝑛
[converge]
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