1091 ®Y01-03í +ãTU
1. Compute the integrals.
(a) (6%) ∫ x(sin 2x + cos x)dx. (b) (9%) ∫
8x − 4 x2(x2+4)dx.
Solution:
(a)
∫ x (sin(2 x) + cos x) dx
= ∫ x sin(2 x) dx + ∫ x cos x dx
=
−1
2 ∫ x d cos(2 x) +∫ x d sin x d cos(2 x) = −2 sin(2 x) dx (1pt) d sin x = cos x dx (1pt)
=
−1
2 (x cos(2 x) −∫ cos(2 x) dx) IBP (2pts)
+x sin x −∫ sin x dx ∫ cos(2 x) dx = 1
2 sin(2 x) + C (0.5pt)
=
−1
2 (x cos(2 x) −1
2 sin(2 x) dx) ∫ sin x dx = − cos x + C (0.5pt) +x sin x + cos x + C C (1pt)
(b)
8x − 4 x2(x2+4)
=
A + B x x2+4 +
C x2 +
D
x partial fractions
=1 − 2x x2+4− 1
x2 +2
x Solve ⇒ A = 1, B = −2, C = −1, D = 2 (4pts)
∫
8x − 4 x2(x2+4)dx
= ∫ ( 1 x2+4−
2x x2+4 −
1 x2 +
2
x) dx use (a)
= 1
2tan−1( x
2) −ln (x2+4) + 1
x+2 ln x + C 4 integrals (4pts); C (1pt)
2. (a) (3%) Evaluate and simplify d dxln (
√
x2+1 + x).
(b) (5%) Evaluate ∫ sec x dx.
(c) (7%) Use (b) and trigonometric substitution to find ∫
1 0
1
√
x2+1dx.
(d) (7%) Use (a) and integration by parts to evaluate the integral ∫
1 0
ln (
√
x2+1 + x) dx.
Solution:
(a) d dxln (
√
x2+1 + x) =
1
2(x2+1)−12 (2 x) + 1
√
x2+1 + x (ln x)′= 1
x (1pt)and chain rule (1pt)
=
√
x2+1 + x (
√
x2+1 + x)(√
x2+1) multiply (x2+1)12 (1pt)
= 1
√ x2+1 (b)
∫ sec x dx =∫
sec x (sec x + tan x)
sec x + tan x dx multiply (sec x + tan x) (2pts)
= ∫
d(sec x + tan x) sec x + tan x
d
dxsec x = sec x tan x (1pt), d
dxtan x = sec2x (1pt)
=ln ∣ sec x + tan x∣ + C ∫ 1
xdx = ln ∣x∣ + C (1pt) (c)
∫
1 0
1
√
x2+1dx x ∶= tan θ ⇒ dx = sec2θ dθ (2pt)
x = 1 ⇒ θ = π/4 (0.5pt), x = 0 ⇒ θ = 0 (0.5pt)
= ∫
π/4 0
1
sec θ sec2θ dθ simplify (1pt)
= ∫
π/4 0
sec θ dθ use (b) (1pt)
=ln ∣ sec θ + tan θ∣ ∣
π/4
0
simplify (1pt)
=ln ∣ sec(π/4) + tan(π/4)∣ sec(π/4) =
√
2 (0.5pt); tan(π/4) = 1 (0.5pt)
=ln(
√ 2 + 1)
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(d)
∫
1 0
ln (
√
x2+1 + x) dx
=x ln (
√
x2+1 + x) ∣
1 0− ∫
1 0
x d ln (
√
x2+1 + x) IBP: u = ln (
√
x2+1 + x), v = x (2pts)
=ln(
√
2 + 1) −∫
1 0
x dx
√
x2+1 evaluate bdy. term (1pt); use (a) (1pt)
=ln(
√
2 + 1) − (x2+1)12∣
1
0 ∫
x dx
√
x2+1 = (x2+1)12 (2pts)
=ln(
√
2 + 1) −
√
2 + 1 evaluate bdy. term (1pt)
3. (a) (10%) Let R be the region bounded by y = cos x, y = sin 2x and x = 0 in the first quadrant.
Rotate R about the x-axis. Find the volume of the resulting solid.
Solution:
First, find intersection points of y = cos x and y = sin 2x for 0 ≤ x ≤ π 2. y = cos x = sin 2x = 2 sin x cos x ⇒ sin x = 1
2 or cos x = 0 i.e. x =π 6 or π
2. Hence R is bounded by y = cos x and y = sin 2x, with 0 ≤ x ≤ π
6. (2 pts for the range of x.) By the disc method, the volume is
V = π∫
π 6
0
(cos x)2− (sin 2x)2dx (2 pts for the formula.
1 pt for recognizing cos x ≥ sin 2x for 0 ≤ x ≤ π 6.)
=π∫
π 6
0
1 + cos 2x
2 −
1 − cos 4x
2 dx (2 pts for half angle formulas)
= π
2 [sin 2x
2 +sin 4x 4 ] ∣
x=π6
x=0 (2 pts for integrating cos 2x and cos 4x.)
= 3√
3
16 π (1 pt for the final answer.)
If Students write V = ∫
π 6
0
2πx(cos x − sin 2x)dx = ⋯, they get 2 pts for the range of x (0 ≤ x ≤ π
6) and 1 pt for recognizing cos x ≥ sin 2x for 0 ≤ x ≤ π 6. (b) (6%) (A) ∫
1 0
πx dx. (B) ∫
1 0
πx4dx. (C) ∫
1 0
πx2dx. (D)∫
1 0
x2dx.
Match each solid with the integral that represents its volume.
Integrals A B C D
Solid 2 1 4 3
1.5 pts for each answers.
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4. (8%) Find the length of the curve
y = f (x) =∫
x 1
√
t3−1 dt, 1 ≤ x ≤ 4.
Solution:
By the fundamental theorem of calculus f′(x) =
√
x3−1. (2%)
length =∫
4 1
√
1 + f′(x)2dx (2%)
= ∫
4 1
x3/2dx (2%)
= 62
5 (2%).
5. Let f (x) = xex. (When finding the following Taylor series, you don’t need to specify the range of x for which the series equals the function.)
(a) (4%) Find the Taylor series for f (x) at x = 0.
(b) (7%) Calculate ∫
x
0 tetdt and find its Taylor series at x = 0.
(c) (4%) Find the sum
∞
∑
n=0
1 n!(n + 2).
Solution:
(a)
f (x) = xex=x(1 + x 1!+
x2 2! + ⋯ +
xn
n! + ⋯) (2%)
=x +x2 1! +
x3 2! + ⋯ +
xn+1
n! + ⋯ (2%).
(b)
∫
x 0
tet dt =∫
x 0
t det (2%)
=xex−ex+1. (2%)
Use term-be-term integration for the Taylor expansion of tet in (a), we have
∫
x 0
tet dt =∫
x 0
t dt +∫
x 0
t2 1!dt +∫
x 0
t3
2!dx + ⋯ +∫
x 0
tn+1
n! dt + ⋯ (1%)
= x2 2 + x3
3 ⋅ 1!+ ⋯ + xn+2
(n + 2) ⋅ n!+ ⋯. (2%) (c) By (b), we have
xex−ex+1 = x2 2 + x3
3 ⋅ 1! + ⋯ + xn+2
(n + 2) ⋅ n!+ ⋯. (1%) Put x = 1 (1%), we have
1 =1 2+
1 3 ⋅ 1! +
1
4 ⋅ 2!+ ⋯ + 1
(n + 2) ⋅ n!+ ⋯. (2%)
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6. (a) (6%) Find the Taylor series for f (x) = ln(1 − x2), g(x) = cos x − 1, and h(x) = sin(2x4)at x = 0.
(You don’t need to specify the range of x for which the function equals its Taylor series.) (b) (4%) Evaluate lim
x→0
(cos x − 1) ln(1 − x2) sin(2x4)
.
Solution:
(a) ln(1 − y) = −y −y2 2 −
y3 3 − ⋯ −
yn+1
n + 1− ⋯, for −1 ≤ y < 1.
f (x) = ln(1 − x2) = −x2− x4
2 − x6
3 − ⋯ − x2x+2
n + 1 − ⋯, for −1 < x < 1
(1 pt for knowing the Taylor series for ln(1 − y). 1 pt for the Taylor series for f (x).) cos x = 1 − x2
2! + x4
4! − x6
6! + ⋯ +
(−1)nx2n
(2n)! + ⋯, for x ∈ R g(x) = cos x − 1 = −x2
2! + x4
4! − x6
6! + ⋯ +
(−1)nx2n
(2n)! + ⋯ for x ∈ R
(1 pt for knowing the Taylor series for cos x. 1 pt for the Taylor series for g(x).) sin y = y −y3
3! + y5 5! + ⋯ +
(−1)n
(2n + 1)!y2n+1+ ⋯ h(x) = sin(2x4) =2x4−
23x12 3! + ⋯ +
(−1)n22n+1
(2n + 1)! x8n+4+ ⋯
(1 pt for knowing the Taylor series for sin y. 1 pt for the Taylor series for h(x).) (b) Solution 1:
(cos x − 1) ln(1 − x2) sin(2x4)
= (−x
2
2 +x
4
4! − ⋯)(−x2−x
4
2 − ⋯) 2x4−43x12+ ⋯
(2 pts for plugging in Taylor series)
=
1
2x4+ (14 −4!1)x6⋯ 2x4−4
3x12+ ⋯
→ 1
4 as x → 0 Hence lim
x→0
(cos x − 1) ln(1 − x2) sin(2x4)
= 1
4 (2 pts for final answers)
Solution 2:
limx→0
(cos x − 1) ln(1 − x2) sin(2x4)
0 0
ÔÔ
L’H lim
x→0
−sin x ⋅ ln(1 − x2) + (cos x − 1)1−x−2x2
cos(2x4) ⋅8x3
=lim
x→0− ( sin x
x
ln(1 − x2) x2
1 8 cos(2x4)
) + (
cos x − 1 x2
−1
4(1 − x2)cos(2x4) )
= 1 8+
1 8 =
1 4.
(2 pts for using L’Hospital’s Rule and obtaining correct first derivatives. 2 pts for final answers.)
7. (a) (6%) Compute lim
x→0
∫
4x2
0 cos(√ t)dt
x2 by L’Hospital’s Rule.
(b) (8%) Compute lim
x→∞(1 + x)1/ ln x. Solution:
(a) As x → 0, ∫
4x2 0
cos(
√
t)dt → 0 and x2→0.
Hence we can apply L’Hospital’s rule.
limx→0
∫
4x2
0 cos(√ t)dt x2
0 0
ÔÔ
L’H lim
x→0
cos(2∣x∣) ⋅ 8x
2x =4
(1 pt for using L’H rule. 3 pts for d dx∫
4x2 0 cos(
√ t)dt) (2 pts for the final answer.)
(b)
ln(1 + x)ln x1 = 1
ln x⋅ln(1 + x) (2 pts)
x→∞lim
ln(1 + x) ln x
∞
∞
ÔÔ
L’H lim
x→∞
1 1+x
1 x
(2 pts)
= lim
x→∞
x
1 + x =1 (2 pts)
Hence lim
x→∞(1 + x)ln x1 =e1 =e (2 pts)
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