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MA4006: Exercise Sheet 4: Solutions
H 2 2
1. Verify Green's theorem in the plane for C(xy + y )dx + x dy where C is the closed
2
curve of the region bounded by y = x and y = x .
Solution. Now
I (xy+y2)dx+x2dy =I f ·dr=I f ·dr+I f ·dr,
C C C C
1 2
where f = (xy+y2,x2) and C and C are given in Figure 1. We parameterise C as x = t,
1 2 1
y = t2, 0 ≤ t ≤ 1. Then
2 ′ 3 4 2
r(t) = (t,t ) =⇒ r (t) = (1,2t) & f(r(t)) = (t +t ,t ).
Thus I Z Z
1 1 19
′ 3 4 3
C f · dr = 0 f(r(t))·r (t)dt = 0 (t +t +2t )dt = 20.
1
We parameterise C as r(t) = r +(r −r )t, 0 ≤ t ≤ 1, where r = (1,1) and r = (0,0).
2 0 1 0 0 1
Then
′ 2 2
r(t) = (1 − t,1 − t) =⇒ r (t) = (−1,−1) & f(r(t)) = (2(1 − t) ,(1 − t) ).
Thus I Z
1
f · dr = −3(1−t)2dt=−1,
C 0
2
and so I
f · dr = 19 − 1 = − 1 .
C 20 20
Green's theorem says
I ZZ µ∂f ∂f ¶
f dx+f dy = 2 − 1 dxdy,
1 2 ∂x ∂y
C R
2 2
where f = xy +y and f = x . So
1 2
∂f ∂f
2 = 2x , 1 = x+2y,
∂x ∂y
and so By Green's theorem
I 2 2 ZZ Z 1Z x Z 1 4 3 1
(xy+y )dx+x dy = (2x−x−2y)dxdy = 2(x−2y)dydx = (x −x )dx = −20.
C R 0 x 0
1
y
y = x
C 2
2 y = x
R C1
x
Figure 1: Question 1.
2. Verify the divergence theorem for the vector eld F = 4xi − 2y2j + z2k taken over the
region bounded by the cylinder x2 +y2 = 4, z = 0 and z = 3.
Solution. The divergence theorem says RRS F·dS = RRRV ∇·FdV. Now
∇·F= ∂ (4x)+ ∂ (−2y2)+ ∂ (z2)=4−4y+2z.
∂x ∂y ∂z
So ZZZ ZZZ
V ∇·FdV = V(4−4y+2z)dV.
Use cylindrical co-ordinates
x=rcosθ, y=rsinθ, z=z, 0 ≤ θ ≤ 2π, 0 ≤ r ≤ 2, 0 ≤ z ≤ 3.
So
ZZZ ∇·FdV =Z 3Z 2πZ 2(4−4rsinθ+2z)rdrdθdz
V 0 0 0
Z 3Z 2π£ ¤
= 2r2 −2r2sinθ+zr2 2dθdz
0 0 0
Z 3Z 2π¡ ¢
= 0 0 8−8sinθ+4z dθdz
=Z 3£8θ+8cosθ+4zθ¤2πdz
0 0
Z 3¡ ¢ £ ¤
= 16π+8πz dz = 16πz+4πz3 3 =84π.
0 0
We now calculate RR F·dS. See Figure 2.
S
2
S z
2
S3
2
x y
S1
Figure 2: Question 2.
b
On S (z =0): n = −k. So
1
b 2 2 2
F·n=(4x,−2y ,z )·(0,0,−1)=−z =0,
RR RR b
since z = 0. So S F·dS= S F·ndS=0.
1 1
b
On S (z =3): n = k. So
2
b 2 2 2
F·n=(4x,−2y ,z )·(0,0,1) = z = 9,
since z = 3. So ZZ ZZ ZZ
b
S F·dS= S F·ndS =9 S dS = 36π,
2 2 2
since the area of S is 4π.
2
2 2
Finally, on S (x +y = 4): Parameterise cylinder as
3
x=2cosθ, y=2sinθ, z=z, 0 ≤ θ ≤ 2π, 0 ≤ z ≤ 3.
So r(θ,z) = (2cosθ,2sinθ,z). Also
¯ ¯
¯ ¯
¯ i j k ¯
¯ ¯
¯ ¯
r ×rz =¯ −2sinθ 2cosθ 0 ¯=(2cosθ,2sinθ,0),
θ ¯ ¯
¯ ¯
¯ 0 0 1 ¯
and ¯ ¯
2 2
F(r(θ,z)) = (8cosθ,−8sin θ,z ).
3
So
ZZ F·dS=ZZ F(r(θ,z))·(r ×r )dθdz
θ z
S3 R
Z 3Z 2π¡ 2 3 ¢
= 0 0 16cos θ−16sin θ dθdz
Z 2π ¡ 2 3 ¢
=48 0 cos θ −sin θ dθ = 48π.
Thus
ZZ F·dS=ZZ F·dS+ZZ F·dS+ZZ F·dS=36π+48π=84π.
S S S S
1 2 3
3. Verify Stokes' theorem for the vector eld F = zi − 3xj + 2zk, where S is the surface
2 2 2 2
z = 1−x −y , z ≥ 0, C is the boundary circle x +y = 1. Assume that S is oriented in
the positive z-direction.
Solution. Stokes' Theorem states H F·dr = RR (∇×F)·dS. See Figure 3.
C S
z
1
x y
2 2
C: x + y = 1
Figure 3: Question 3.
Parameterise C as
x=cosθ, y=sinθ, z=0, 0 ≤ θ ≤ 2π.
Thus r(θ) = (cosθ,sinθ,0) and so
′
r (θ) = (−sinθ,cosθ,0), F(r(θ)) = (0,−3cosθ,0).
4
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