Solutions to Assignment 6.2 Exercise 3 Letfaculty.atu.edu/mfinan/2924/Solution62.pdf · Arkansas...
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Transcript of Solutions to Assignment 6.2 Exercise 3 Letfaculty.atu.edu/mfinan/2924/Solution62.pdf · Arkansas...
Arkansas Tech UniversityMATH 2924: Calculus II
Dr. Marcel B. Finan
Solutions to Assignment 6.2
Exercise 3Let u = cosx then du = − sinxdx. Thus,∫ π/2
0sin7 x cos5 xdx =
∫ π/2
0(1− cos2 x)3 sinx cos5 xdx
=
∫ 1
0(1− u2)3u5du =
∫ 1
0(1− 3u2 + 3u4 − u6)u5du
=
[u6
6− 3
8u8 +
3
10u10 − 1
12u12]10
=1
120
Exercise 5Using the trigonometric identity
cos2 x =1 + cos 2x
2
we find ∫ π/2
0cos2 xdx =
∫ π/2
0
1 + cos 2x
2dx
=1
2
∫ π/2
0(1 + cos 2x)dx
=1
2
[x+
sin 2x
2
]π/20
=π
4
Exercise 7Letting u = 2x and using the trigonometric identity
cos2 u =1 + cos 2u
2
1
we find∫ π
0cos4 2xdx =
1
2
∫ 2π
0[cos2 u]2du =
1
2
∫ 2π
0
(1 + cos 2u
2
)2
du
=1
8
∫ 2π
0(1 + 2 cos 2u+ cos2 2u)du
=1
8
[u+ sin 2u+
u
2+
sin 4u
8
]2π0
=3π
8
Exercise 11Using integration by parts with u = t and v′ = sin2 t, we have∫
t sin2 tdt =t
2
(t− sin 2t
2
)−∫
1
2
(t− sin 2t
2
)dt
=t
2
(t− sin 2t
2
)− t2
4− cos 2t
8+ C
=t2
4− t
4sin 2t− cos 2t
8+ C
Exercise 17Letting u = secx so that du = tanx secxdx, we have∫
tanx sec3 xdx =
∫u2du =
u3
3+ C
=sec3 x
3+ C
Exercise 21Letting u = tanx so that du = secx2dx, we have∫
tan4 x sec6 xdx =
∫u4(u2 + 1)2du
=
∫(u8 + 2u6 + u4)du =
u9
9+
2
7u7 +
u5
5+ C
=tan9 x
9+
2
7tan7 x+
tan5 x
5+ C
2
Exercise 27Letting u = tanx so that du = sec2 xdx and using Example 7 of the book,we have ∫
tan5 xdx =
∫tan3 x tan2 xdx =
∫tan3 x(sec2 x− 1)dx
=
∫tan3 x sec2 xdx−
∫tan3 xdx
=tan4 x
4− tan2 x
2+ ln | secx|+ C
Exercise 33Using the fact that
(cscx− cotx)′ = − cscx cotx+ csc2 x = cscx(cscx− cotx)
we have ∫cscxdx =
∫cscx(cscx− cotx)
cscx− cotxdx
=
∫(cscx− cotx)′
cscx− cotxdx
= ln | cscx− cotx|+ C
Exercise 39Let x = 2 sin θ with −π
2 < θ < π2 . Then
√4− x2 = 2 cos θ. We have∫
dx
x2√
4− x2=
∫2 cos θ
4 sin2 θ(2 cos θ)dθ
=1
4
∫csc2 θdθ = −1
4cot θ
=−√
4− x24x
+ C
3
Exercise 40Let x = 2 tan θ with −π
2 < θ < π2 . Then
√x2 + 4 = 2 sec θ. We have∫
x3√x2 + 4
dx =
∫8 tan3 θ(2 sec2 θ)
2 sec θdθ
=8
∫tan3 θ sec θdθ = 8
∫(sec2 θ − 1) tan θ sec θdθ
=8
∫(u2 − 1)du = 8
[sec3 θ
3− sec θ
]+ C
=1
3(x2 + 4)
√x2 + 4− 4
√x2 + 4 + C
Exercise 41Let x = 2 sec θ with 0 < θ < π
2 or π < θ < 3π2 . Then
√x2 − 4 = 2 tan θ. We
have ∫ √x2 − 4
xdx =
∫2 tan θ(2 sec θ tan θ)
2 sec θdθ
=2
∫tan2 θdθ = 2
∫(sec2 θ − 1)dθ
=2 tan θ − 2θ + C =√x2 − 4− 2 sec−1
(x2
)+ C
4
Exercise 45Let x = a tan θ with −π
2 < θ < π2 . Then
√a2 + x2 = a sec θ and dx =
a sec2 θdθ. Hence, ∫ a
0
dx
(a2 + x2)32
=
∫ π/4
0
a sec2 θ
a3 sec3 θdθ
=1
a2sin θ]
π/40 =
√2
2a2
Exercise 49Let 2x = sin θ with −π
2 < θ < π2 . Then
√1− 4x2 = cos θ and 2dx = cos θdθ.
Thus, ∫ √1− 4x2dx =
1
2
∫cos2 θdθ
=1
4
∫(1 + cos 2θ)dθ =
θ
4+
sin 2θ
8+ C
=θ
4+
2 sin θ cos θ
8+ C
=1
4sin−1 (2x) +
x√
1− 4x2
2+ C
Exercise 51Let x = 3 sec θ so that
√x2 − 9 = 3 tan θ and dx = 3 sec θ tan θdθ. Thus,∫ √
x2 − 9
x3dx =
1
3
∫tan2 θ
sec2 θdθ
=1
3
∫sin2 θdθ =
θ
6− 1
12sin 2θ + C
=1
6sec−1
(x3
)−√x2 − 9
2x+ C
5
Exercise 53Let 5x = 3 sin θ with −π
2 < θ < π2 . Then
√9− 25x2 = 3 cos θ and 5dx =
3 cos θdθ. Thus, ∫ 0.6
0
x2√9− 25x2
dx =9
125
∫ π/2
0sin2 θdθ
=9
125
[θ
2− sin 2θ
4
]π/20
=9
125[π
4] =
9π
500
Exercise 57Let x = tan θ so that
√x2 + 1 = sec θ and dx = sec2 θdθ. Thus,∫ √
x2 + 1
xdx =
∫sec3 θ
tan θdθ
=
∫ (tan2 θ + 1
tan θ
)sec θdθ
=
∫ (tan θ +
1
tan θ
)sec θdθ
=
∫sin θ
cos2 θdθ +
∫csc θdθ
= sec θ + ln | csc θ − cot θ|+ C
=√x2 + 1 + ln
∣∣∣∣∣√x2 + 1
x− 1
x
∣∣∣∣∣+ C
Exercise 65We have
f(t) =
∫ t
0sinωs cos2 ωsds = − 1
3ωcos3 ωs
∣∣∣∣t0
=1
3ω
(1− cos3 ωt
)Exercise 66(a) Recall that the average of f(x) in [a, b] is given by
1
b− a
∫ b
af(x)dx.
6
Now, one cycle takes 160 seconds. We are asked to find[
1160 − 0
∫ 1/60
0E(t)2dt
] 12
.
We have∫ 1/60
0E(t)2dt =24, 025
∫ 1/60
0sin2 (120πt)dt =
24, 025
120π
[60πt− 1
4sin (240πt)
]1/600
=24, 025
120π(π) =
4805
24.
Thus,
RMS =
[1
160 − 0
4805
24
] 12
≈ 109.60.
(b) We must solve the equation
2202 =1
160 − 0
∫ 1/60
0A2 sin2 (120πt)dt.
That is,
2202 =60A2
120
which yields A ≈ 311.13
Exercise 67Using the substitution x = sec θ, we have
1
7− 1
∫ 7
1
√x2 − 1
xdx =
1
6
∫ sec−1 7
sec−1 1tan2 θdθ
=1
6
∫ sec−1 7
sec−1 1(sec2 θ − 1)dθ
=1
6[tan θ − θ]sec
−1 7sec−1 1
=1
6
[√x2 − 1− sec−1 x
]71
=1
6(√
48− sec−1 7)
7
Exercise 70From Exercise 45, we find∫
dx
(x2 + b2)32
=sin θ
b2+ C =
x
b2√x2 + b2
+ C.
Thus,
E(P ) =λb
4πε0
[x
b2√x2 + b2
]L−a−a
=λ
4πε0b
[L− a√
(L− a)2 + b2+
a√a2 + b2
]
8