1. (10%) Evaluate the iterated integral Z a
0
Z a x
sin (y2) dy dx, a > 0.
Sol:
Z a 0
Z a x
sin y2dy dx = Z a
0
Z y 0
sin y2dx dy
= Z a
0
y sin y2dy
= − cos y2 2
y=a y=0
= 1 − cos a2 2
2. (12%) Compute the area of the domain in the first quadrant bounded by the four curves xy = 1, xy = 4, y
x2 = 1, and y x2 = 2.
Sol:
Method 1
(i) Find the four vertices of the region:
(2−13, 213), (1, 1), (213, 253), (223, 243).
(From left to right.) (ii)
Area = Z 1
2−
1 3
(2x2− 1 x) dx +
Z 213 1
(2x2− x2) dx
+ Z 223
213
(4
x − x2) dx
= ln 2
or
Area = Z 213
1
(y12 − y−1) dy
+ Z 243
213
(y12 − (y 2)12) dy +
Z 253 243
(4 y − (y
2)12) dy
= ln 2.
Method 2
(i) Make the change of variables:
u = xy v = yx2
⇒
x = (uv)13 y = u23v13 (ii)
Area = Z 2
1
Z 4
1 |∂(x, y)
∂(u, v)|dudv = ln 2.
3. (12%) Find the region E ⊂ R3 for which the triple integral Z Z Z
E
(4 − x2− 4y2 − 9z2) dV is a maximum, and compute this maximum value.
Sol:
First we note that the region E which maximize the integralR 4 −x2− 4y2− 9z2 is the ellipsoid (x, y, z) : 4 − x2− 4y2− 9z2 > 0
Here we use the ”change of coordinate”, that is x = r sin φ cos θ, y = 1
2r sin φ sin θ, z = 1 3r cos φ and the corresponding Jacobian is
∂(x, y, z)
∂(r, φ, θ) = 1
6r2sin φ
With the above transformation, the original integral R
x2+4y2+9z2<44 − x2− 4y2− 9z2dxdydz is now changed to
Z 2π 0
Z π 0
Z 2
0 (4 − r2)1
6r2sin φ drdφdθ = 128 45π 4. (14%) Let F(x, y, z) = yzi +
xz + y
y2+ z2+ 1
j+
xy + z
y2+ z2+ 1 + cos z k.
(a) Find a function f such that F = ∇f.
(b) Compute the line integral Z
C
F· dr, where C is the curve starting from the origin given by r(θ) = hθ cos θ, θ sin θ, θi, 0 ≤ θ ≤ π.
Sol:
(a) ∂f
∂x = yz ⇒ f = xyz + g(y, z)
∂f
∂x = xz + y
y2+ z2+ 1 ⇒ f = xyz +1
2ln(y2+ z2+ 1) + h(z)
∂f
∂x = xy + z
y2+ z2 + 1 + cos y ⇒ f = xyz + 1
2ln(y2+ z2+ 1) + sin z (b)
Z
CF · dr = f(x, y, z)
r(π)=(−π,0,π) r(0)=(0,0,0) = 1
2ln(π2+ 1) 5. (14%) Compute the line integral
I
C
(3xy + 1) dx + (x2+ x) dy, where the closed curve C is the cardioid given by the polar equation r = 1 + sin θ, and is oriented counterclockwise (see figure).
Sol:
Since 3xy + 1, x2+ x are smooth on C and smooth in D ,where D is the region enclosed by C.
Hence using Green’s theorem we have I
c
(3xy + 1)dx + (x2+ x)dy = Z Z
D
∂(x2+ x)
∂x − ∂(3xy + 1)
∂y dA =
Z Z
D(1 − x)dA
by using polar coordinates we have Z Z
D(1 − x)dA = Z 2π
0
Z 1+sin θ
0 (1 − r cos θ)rdrdθ Z 2π
0
Z 1+sin θ
0 (1 − r cos θ)rdrdθ = Z 2π
0
[(1 + sin θ)2
2 −1
3cos θ(1 + sin θ)3]dθ
= Z 2π
0
(1
2 + sin θ +1
2sin2θ)dθ
= π + π 2 = 3π
2 6. (10%) Evaluate
Z Z
S
p1 + x2+ y2dS, where S is the helicoid parametrized as r(u, v) = u cos v i+
u sin v j + v k, 0 ≤ u ≤ 1, 0 ≤ v ≤ π.
Sol:
r(u, v) = (u cos v, u sin v, v)
∂r
∂u = (cos v, sin v, v)
∂r
∂v = (−u sin v, u cos v, 1)
∂r
∂u × ∂r
∂v = (sin v, − cos v, u)
∂r
∂u × ∂r
∂v =
√1 + u2
Z Z
S
p1 + x2+ y2dS = Z 1
0
Z π 0
√1 + u2√
1 + u2dvdu = (u + 1 3u3)
1 0(v)
π 0 = 4
3π
7. (14%) Let closed curve C be the intersection of the plane x + y + z = 1 and the cylinder x2+ y2 = 9, oriented counterclockwise as viewed from above, and F(x, y, z) = x2zi + xy2j+ z2k.
Find I
C
F· dr.
Sol:
Compute the curl of vector field F. Find curl(F) = x2j+ y2k. Using Stoke’s Theorem, we have
I
C
F· dr = Z Z
S
curl(F)dS
where S is the surface with boundary C which is parametrized with counterclockwise orienta- tion. And C is the intersection of x2+ y2= 9 and x + y + z = 1. Now observe that the normal
vector of S is (1, 1, 1)/√
3 and that dS =√
3 dA. So Z Z
S
curl(F) = Z Z
A
(x2+ y2)dA
where A is the projection of S on xy plane., that is, x2 + y2 = 9. Hence by using polar coordinates. We have
Z Z
A
(x2+ y2)dA = Z 3
0
Z 2π 0
r2rdrdθ = 81 2 π
8. (14%) Let F(x, y, z) =
xy2+py2+ z4 i+
tan−1x + x2y
j+z3
3 − ex2+y2 k.
(a) Find div F.
(b) Find Z Z
S
F· dS, where the surface S is the top half of the sphere x2+ y2+ z2 = 1 with the unit normal vectors pointing away from the origin. Warning. S is not a closed surface!
Sol:
(a) divF = x2+ y2+ z2
(b) 1◦ By divergence theorem, we have Z Z
S
F· dS + Z Z
E
F· dS = Z Z Z
x2+ y2+ z2dxdydz
where E is the disk with radius 1 on xy-plane and with the unit normal vectors (0, 0, −1).
2◦
Z Z
E
F· dS = Z Z
x2+y2≤1
ex2+y2 −
0 z3
3dxdy = Z 2π
0
Z 1 0
er2 · rdrdθ = π(e − 1) 3◦
Z Z Z
x2+ y2+ z2dxdydz = Z 2π
0
Z π/2 0
Z 1 0
ρ2 · ρ2sin φdρdφdθ = 2π 5 4◦ Thus
Z Z
S
F· dS = 2π
5 − π(e − 1)