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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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