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(8 pts) Let f be a continuous function on R such that ∫ x3 0 f (t) dt = x3⋅cos(πx) for all x

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(1)

1091!D06-12í ®M2 ãTŒU–

1. (8 pts) Let f be a continuous function on R such that

x3 0

f (t) dt = x3⋅cos(πx) for all x.

Find f (1).

Solution:

Since f is continuous on R, by Fundamental Theorem of Calculus (2%), we have d

dx∫

x3 0

f (t) dt = d

dx(x3⋅cos(πx))

⇒ f (x3) ⋅3x2 (2%) = 3x2⋅cos(πx) − πx3⋅sin(πx) (1%) To find f (1), we solve x3=1 to obtain that x = 1 (1%). For x = 1, we have

f (1) ⋅ 3 = 3 ⋅ cos(π) − π ⋅ sin(π) = −3 ⇒ f (1) = −1 (2%).

(2)

2. (16 pts) Evaluate the following definite integrals.

(a) ∫

1 0

√x dx (1 +√

x)4. (b) ∫

1 0

sin−1(

√x) dx.

Solution:

Answer: Must show clearly the steps of substitution and integration by parts (a) Method-1:

– (2%) Set y =√

x ⇒ dx = 2ydy ⇒∫

1 0

x (1+

x)4dx =∫

1 0

2y2 (1+y)4dy (1%) = 2∫

1 0

1−(1−y2)

(1+y)4 dy = 2∫

1 0[ 1

(1+y)4(1−y)

(1+y)3]dy (2%) = 2∫

1 0[ 1

(1+y)42−(1+y)

(1+y)3 ]dy = 2∫

1 0[ 1

(1+y)42

(1+y)3 + 1

(1+y)2]dy (2%) = −2[3(1+y)1 31

(1+y)2 + 1

(1+y)]10 = 1

12 ⋯ Method-2:

– (2%) Set y = 1 +√

x ⇒ dx = 2(y − 1)dy (3%) ⇒∫

1 0

x (1+

x)4dx =∫

2 1

2(y−1)2

y4 dy = 2∫

2

1[y12y23 +y14]dy (2%) = −2[1y1

y2 + 1

3y3]21 = 1

12 ⋯ (b) Method-1:

– (2%) Set y =√

x ⇒ dx = 2ydy ⇒∫

1 0 sin−1(

√x)dx =∫

1

0 sin−1(y) 2ydy (2%) =∫

1

0 sin−1(y) (y2)dy = [y2sin−1(y)]10− ∫01 y

2

1−y2dy (2%) = π2 − ∫011−(1−y

2)

1−y2 dy = π2 − ∫01[1

1−y2 +

1 − y2]dy (2%) = π2 − [sin−1(y)]10+ ∫0π/2cos2(θ)dθ where y = sin θ (1%) = 12[θ +sin(2θ)2 ]π/20 = π

4 ⋯ Method-2:

– (4%) Set y = sin−1(

√x) ⇒ x = sin2(y) and dx = sin(2y)dy (2%) ⇒∫

1 0 sin−1(

√x)dx =∫

π/2

0 y sin(2y)dy (2%) =∫

π/2

0 y (−cos(2y)2 )dy =−12 [y cos(2y)]π/20 +1

2

π/2

0 cos(2y)dy (1%) = π4 +14[sin(2y)]π/20 = π4

Page 2 of 10

(3)

3. (13 pts)

(a) Decompose x2+4x + 5

(x + 1)2(x2+2x + 3) into partial fractions.

(b) Evaluate the indefinite integral ∫

x2+4x + 5

(x + 1)2(x2+2x + 3)dx.

Solution:

(a) Let

x2+4x + 5

(x + 1)2(x2+2x + 3) = A x + 1 +

B (x + 1)2 +

Cx + D

x2+2x + 3. (2 pts) By clearing the denominator we have

x2+4x + 5 = A(x + 1)(x2+2x + 3) + B(x2+2x + 3) + (Cx + D)(x + 1)2. (1 pt) By comparing the coefficients, we have

⎧⎪

⎪⎪

⎪⎪

⎪⎪

⎪⎪

⎪⎩

A +C =0,

3A +B +2C +D =1, 5A +2B +C +2D = 4,

3A +3B +D =5,

(4 pts) ⇒

⎧⎪

⎪⎪

⎪⎪

⎪⎪

⎪⎪

⎪⎩

A =1, B =1, C = −1, D = −1.

(1 pts)

Therefore, we get

x2+4x + 5

(x + 1)2(x2+2x + 3) = 1

x + 1+ 1 (x + 1)2 +

−x − 1

x2+2x + 3. (1 pt) (b) By (a) we have the indefinite integral

x2+4x + 5

(x + 1)2(x2+2x + 3)dx =∫ [ 1

x + 1+ 1

(x + 1)2 − x + 1

x2+2x + 3]dx (1 pt)

=ln ∣x + 1∣ − 1 x + 1 −

1

2ln(x2+2x + 3) + C. (3 pts)

(4)

4. (16 pts)

(a) Find the orthogonal trajectories of the family of curves y = K ⋅ tan2x, where K is an arbitrary constant.

(b) Solve the initial value problem : x(x + 1)dy

dx+y = (x + 1)2sin x cos x, y (π 2) =0.

Solution:

(a) (i) The slope of each point on the family of curves is dy

dx =K ⋅ 2 tan x ⋅ sec2x (2 pts) = y

tan2x⋅2 tan x ⋅ sec2x

=2y ⋅ sec2x ⋅ cot x = 2y

sin x ⋅ cos x. (2 pts) (ii) Solve dy

dx =

−sin x ⋅ cos x

2y . (2 pts) We have

dy dx =

−sin x ⋅ cos x 2y

⇒ ∫ 2ydy = ∫ (− sin x ⋅ cos x)dx = −1

2 ∫ sin(2x)dx

⇒y2= cos(2x)

4 +C. (2 pts)

The orthogonal trajectories of the family of curves y2 =

cos(2x) 4 +C.

(b) The standard form of the differential equation is dy

dx + 1

x(x + 1)⋅y = x + 1

x ⋅sin x ⋅ cos x.

Since

e x(x+1)1 dx=e∫ (1xx+11 )dx=eln ∣x+1x = ∣ x x + 1∣, we can take the integration factor as I(x) = x+1x . (3 pts)

Then we have

I(x) ⋅ [dy dx +

1

x(x + 1) ⋅y] = I(x) ⋅ [x + 1

x ⋅sin x ⋅ cos x]

⇒ [ x

x + 1⋅y]= [I(x) ⋅ y]= 1

2sin(2x)

⇒ x

x + 1 ⋅y = I(x) ⋅ y =∫ 1

2sin(2x)dx = −1

4 cos(2x) + C

⇒y = x + 1 x ⋅ [

−1

4 cos(2x) + C]. (3 pts) Since y(π2) =0, we get −14 =C. So the solution is y = x + 1

x ⋅ [

−1

4 cos(2x) −1

4]. (2 pts)

Page 4 of 10

(5)

5. (14 pts) Let C be a curve whose parametrisation is given by

⎧⎪

⎪⎪

x = etcos t

y = etsin t with 0 ≤ t ≤ π.

(a) Find the arclength of C.

(b) Find dy

dx in terms of t and find the point Q in x-y coordinates at which the tangent to C is perpendicular to the x-axis.

Solution:

(a)

dx

dt =et(cos t − sin t) dy

dt =et(sin t + cos t).

Arc length is then computed by the formula

π 0

√ (dx

dt)2+ (dx

dt)2 dt =∫

π 0

2et dt =

2(eπ−1).

Grading Guideline. Arc length formula (including lower and upper limits) 3pt differentiation computation 2pt

integral computation 2pt.

(b) With the computation above

dy

dx =sin t + cos t cos t − sin t.

Vertical tangents occur, if exists, when cos t − sin t = 0, that is t = π4. We need to check if it is indeed a vertical tangent. We can either compute

±

lim

t→π4

dy dx = ±∞

or just say the numerator is non-zero. Finally, converting it into cartesian coordinates, we get Q = eπ4(1

2,1

2).

Grading Guideline. dydx (2pt= chain rule (1pt) + computation (1pt)) vertical tangent (3pt)=denominator=0 (1pt)+t-value(1pt)+limit(1pt) converting to cartesian coordinates (1pt).

(6)

6. (10 pts) Consider two polar curves C1 and C2 defined by

C1 ∶r2 =4 sin(4θ), C2 ∶r2 =4 cos(2θ).

Find the area of the region that lies inside both C1 and C2.

Solution:

By symmetry, we compute the intersection of curves C1 and C2 when 0 ≤ θ ≤ π4.

{ r2=4 sin(4θ)

r2 =4 cos(2θ), ⇒4 cos(2θ) ⋅ (sin(2θ) − 1) = 0 (2 pts)

⇒cos(2θ) = 0 or sin(2θ) = 1 2

⇒2θ = π 2 or π

6 ⇒θ = π 4 or π

12. (3 pts) So we have

Area of the region inside C1 and C2

=2 ⋅ [∫

π 12

0

1

2⋅4 sin(4θ)dθ +∫

π 4 π 12

1

2⋅4 cos(2θ)dθ] (3 pts)

= (−cos(4θ)) ∣

π 12

0

+(2 sin(2θ)) ∣

π 4

π 12

= (−1

2+1) + 2(1 − 1 2) = 3

2. (2 pts)

Page 6 of 10

(7)

7. (10 pts) The ellipse

x2+y2 5 =1

is rotated about the x-axis to form a surface called an oblate spheroid. Find the surface area of this oblate spheroid.

Solution:

Marking scheme.

(2M) *Evaluation of ds (2M) ** Integrand (1M) Integration limits

(2M) ***Convert the integral into C ⋅∫ sec3θdθ by a suitable substitution (2M) ****Correct evaluation of ∫ sec3θdθ

(1M) Correct answer Partial credits.

(*) 1M is awarded as long as the candidate attempts to compute ds (**) Here a candidate will receive at most 1M for

ˆ making mistakes up to a constant factor

ˆ mentioning∫ 2πy ⋅ ds (or any equivalent form)

(***) 1M is taken away if a student makes mistakes in the integration limits after conducting a substitution

(****) No derivation is required. At most 1M can be awarded to a candidate with an incorrect evaluation who (1) attempts to derive ∫ sec3θdθ or (2) makes minor/obvious typos.

Sample Solution 1.

One can obtain an ellipsoid by using the upper half of the ellipse y =

5(1 − x2)for which dy

dx =

5 ⋅ −x

1 − x2 and

1 + (dy dx)

2

=

1 + 5x2 1 − x2 =

1 + 4x2 1 − x2

´¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¸¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¶

(2M )

By symmetry, the surface area is given by

2 ⋅∫

1 0

5(1 − x2)

´¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¸¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¶

y

1 + 4x2 1 − x2 dx

´¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¸¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¶

ds

´¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¸¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¶

(3M )

=4

√ 5π∫

1 0

1 + 4x2dx

To evaluate ∫

1 + 4x2dx, we substitute x = 12tan θ, then

1 + 4x2dx = 1

2∫ sec3θdθ (2M)

= 1

4(sec θ tan θ + ln ∣ sec θ + tan θ∣) + C (2M)

1 2x

1 + 4x2 ln(2x +

1 + 4x2 C

(8)

Hence, the surface area equals to √

5π(2√

5 + ln(2 +√

5)). (1M) Sample Solution 2 (Parametric way).

The ellipse can be parametrised by x = cos t and y =√ 5 sin t.

Then

√ (

dx dt)

2

+ ( dy dt)

2

=

sin2t + 5 cos2t =√

1 + 4 cos2t

´¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¸¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¶

(2M )

.

By symmetry, the surface area thus equals to 2 ⋅∫

π/2 0

2π√ 5 sin t

´¹¹¹¹¹¹¹¹¹¹¸¹¹¹¹¹¹¹¹¹¹¶

y

1 + 4 cos2tdt

´¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¸¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¶

ds

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(3M )

=4√ 5π∫

π/2 0

sin t

1 + 4 cos2tdt

To evaluate ∫ sin t

1 + 4 cos2tdt, we let 2 cos(t) = tan θ

∫ sin t

1 + 4 cos2tdt = −1

2∫ sec3θdθ (2M)

= − 1

4(sec θ tan θ + ln ∣ sec θ + tan θ∣) + C (2M)

= − 1

4(2 cos t

1 + 4 cos2t + ln(2 cos t +

1 + 4 cos2t)) + C

Hence, the surface area equals to √

5π(2√

5 + ln(2 +√

5)). (1M) Alternative form of the final answer : 10π +√

5π ln(2 +√ 5).

Page 8 of 10

(9)

8. (13 pts) Consider the region bounded by the curve y = 1

e2x+1, the x-axis and x = 1.

(a) Find the volume of the solid obtained by revolving the region about the x-axis.

(b) Student A claims that ‘The volume of the solid obtained by revolving the region about the y-axis is also finite.’. Give a proof to Student A’s claim by using the comparison test for improper integrals.

Solution:

(a)

Marking scheme.

(2M) *Integrand

(1M) Integration limits

(1M) Writing down the definition of improper integrals (3M) **Using a suitable substitution to evaluate the integral (1M) Correct answer

Partial credits.

(*) At most 1M is taken away for any missing/extra scalar factors.

(**) A candidate will receive

ˆ 2M for having done a correct substitution but incomplete evaluation of the integral

ˆ 3M as long as he/she integrates ∫

b a

1

e2x+1dx correctly - does not matter his/her choice of integration limits.

Sample solution.

By disk method, the volume of the solid equals to

1

π ⋅ 1

e2x+1dx

´¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¸¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¶

(2+1M )

= lim

t→∞

t 1

π ⋅ 1

e2x+1dx

´¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¸¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¶

(1M )

.

To evaluate ∫ 1

e2x+1dx, we let u = e2x. Then

∫ 1

e2x+1dx = 1 2∫

du u(u + 1) =

1 2∫

1 u −

1

u + 1du = 1

2ln ∣ u

u + 1∣ +C = 1

2ln ∣ e2x e2x+1∣ +C

´¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¸¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¹¶

(3M )

.

Hence, the volume equals to

π e2t e2 1

(10)

Alternative form of the final answer : −π

2ln e2 e2+1 =

π

2lne2+1 e2 =π ln

√ e2+1

e2 . (b)

Marking scheme.

(2M) *Setting up the correct integral (1M) Any correct upper bound for x

e2x+1

(2M) **Correct argument using the comparison test Partial credits.

(*) At most 1M is taken away for any missing/extra scalar factors.

(**) 1M can be awarded to candidates with an incorrect upper bound, but with some attempts of an argument using the comparison test.

In an extreme situation that a candidate didn’t set up a correct integral (not of the form C ⋅∫ e2xx+1dx) but demonstrated some understandings of the comparison test, at most 1M will be awarded.

Sample solution.

By shell method, the volume of the solid equals to ∫

1

2πx ⋅ 1

e2x+1dx. (2M)

Since 0 ≤ x

e2x+1 ≤ x

ex (1M)

and ∫

1

x

exdx = lim

t→∞

t 1

x

exdx = lim

t→∞(−te−t−e−t+2e−1) =2e−1 is convergent, (2M) the comparison test implies that ∫

1

x

e2x+1dx is convergent. This verifies the claim of Student A.

Alternative argument.

By shell method, the volume of the solid equals to ∫

1

2πx ⋅ 1

e2x+1dx. (2M)

Since 0 ≤ x

e2x+1 ≤ 1

x2 for x sufficiently large (1M)

and ∫

1

1

x2dx converges as a p-integral with p > 1, (2M)

the comparison test implies that ∫

1

x

e2x+1dx is convergent. This verifies the claim of Student A.

Remark. 1/x2 can be replaced by 1/xp for any p > 1 in the above argument.

Page 10 of 10

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