Name ID MATH 253 Exam 2 Sections 201-202 Solutions ∫0 ∫0 ∫0 2 z /45 12 /12 10 /12 13 /12 11 /12 14 /12 Fall 2006 P. Yasskin Multiple Choice: (5 points each. No part credit.) 1. Compute 1-9 Total /105 xz 15x dy dx dz. a. 4 b. 8 c. 16 Correct Choice d. 32 e. 64 ∫0 ∫0 ∫0 2 z xz 15x dy dx dz = 2 = z5 2. Compute z=0 ∫0 ∫y 2 4 2 ∫0 ∫0 2 z 15xy xz dx dz = y=0 ∫ 0 ∫ 0 15x 2 z dx dz = ∫ 0 2 z 2 5x 3 z z dz = x=0 ∫ 0 5z 4 dz 2 = 32 y sinx 2 dx dy by interchanging the order of integration. a. − cos 16 2 cos 16 − 1 2 1 − cos 16 4 cos 16 8 cos 16 − 1 4 b. c. d. e. Correct Choice Plot the region. y In the original order: For each y between 1 0 and 2, x runs from y 2 to 4. In the reversed order: For each x between 0 and 4, y runs from 0 to ∫0 ∫y 2 4 y sinx 2 dx dy = 2 = 2 ∫0 ∫0 4 − cosx 2 4 x y sinx 2 dy dx = 4 0 0 x. 0 ∫0 4 y2 sinx 2 2 x 0 dx = 1 2 2 4 x ∫ 0 x sinx 2 dx 4 = 1 − cos 16 4 1 3. Which of the following is the polar plot of r = cos3θ? y a. b. 1 c. 0 2 4 6 x -1 ←Correct Choice d. e. (c) is the rectangular plot of r = cos3θ. (d) is its polar plot because there are 3 positive loops and 3 negative loops which retrace the positive loops. 4. Find the area of the region inside the circle r = 4 y 4 outside the polar curve r = 3 + 2 cos2θ with y ≥ 0. 2 The area is given by the integral: -4 a. A = ∫ π/3 ∫ 3+2 cos2θ r dr dθ b. A = ∫ π/3 ∫ 4 c. A = ∫ π/3 ∫ 3+2 cos2θ dr dθ d. A = ∫ π/6 ∫ 3+2 cos2θ dr dθ e. A = ∫ π/6 ∫ 3+2 cos2θ r dr dθ 5π/3 5π/3 5π/3 5π/6 5π/6 0 2 4 x 4 3+2 cos2θ dr dθ 4 4 4 r = 3 + 2 cos2θ = 4 A= -2 Correct Choice cos2θ = 1 2 ∫∫ dA = ∫ π/6 ∫ 3+2 cos2θ r dr dθ 5π/6 4 2θ = π 3 θ = π , 5π 6 6 by symmetry 2 5. Find the volume of the apple given in spherical coordinates by ρ = 3ϕ. The volume is given by the integral: a. 54π ∫0 b. 54π ∫ 0 ϕ 2 sin ϕ dϕ c. 27π ∫0 d. 27π ∫ 0 ϕ 2 sin ϕ dϕ e. 18π ∫ 0 ϕ 3 sin ϕ dϕ 2π ϕ 2 sin ϕ dϕ π 2π ϕ 2 sin ϕ dϕ π π V= π Correct Choice ∫∫∫ dV = ∫ 0 ∫ 0 ∫ 0 2π 3ϕ ρ 2 sin ϕ dρ dϕ dθ = 2π ∫ π 0 ρ3 3 3ϕ ρ=0 π sin ϕ dϕ = 18π ∫ ϕ 3 sin ϕ dϕ 0 ⃗ = y − z, x + z, y − x + 2z. 6. Find a scalar potential f for the vector field F Then evaluate f1, 1, 1 − f0, 0, 0: a. 1 b. 2 Correct Choice c. 4 d. 5 e. 7 ∂xf = y − z f = xy − xz + gy, z ∂yf = x + z x + ∂yg = x + z −x + y + dh = y − x + 2z dz ∂ z f = y − x + 2z ∂yg = z dh = 2z dz g = yz + hz f = xy − xz + yz + hz h = z2 f = xy − xz + yz + z 2 f1, 1, 1 − f0, 0, 0 = 1 − 1 + 1 + 1 − 0 − 0 + 0 + 0 = 2 3 ⃗ for any vector field F ⃗. 7. Which vector field cannot be written as ⃗ ∇×F ⃗ = xz, yz, z 2 a. A ⃗ ⃗ = z + z + 2z = 4z ≠ 0 ∇⋅A Correct Choice ⃗ = x, y, −2z b. B ⃗ ⃗ = 1+1−2 = 0 ∇⋅B ⃗ = xz, yz, −z 2 c. C ⃗ ⃗ = z + z − 2z = 0 ∇⋅C ⃗ ⃗ = z cos x − z cos x = 0 ∇⋅D ⃗ = z sin x, −yz cos x, y sin x d. D ⃗ ⃗ = sin y − sin y = 0 ∇⋅E ⃗ = x sin y, cos y, x cos y e. E ⃗ cannot be A ⃗ =⃗ ⃗ = 0, A ⃗. ∇⋅⃗ ∇×F ∇×F Since it is always true that ⃗ ⃗, D ⃗, C ⃗ and E ⃗ probably have vector potentials. On the other hand, B 8. Find the total mass of a plate occupying the region between x = y 2 and x = 4 if the mass density is ρ = x. a. 64 b. c. d. e. 5 128 5 256 5 32 3 32 9 x = y2 = 4 M= Correct Choice y = ±2 ∫∫ ρ dA = ∫ −2 ∫ y 2 4 2 x dx dy = ∫ −2 2 x2 2 4 dy = 1 2 2 x=y 5 ∫ −2 16 − y dy = 12 16y − y5 2 2 4 y=−2 = 128 5 9. Find the center of mass of a plate occupying the region between x = y 2 and x = 4 if the mass density is ρ = x. a. b. c. d. e. 20 , 0 7 12 , 0 5 512 , 0 7 128 , 0 5 14 , 0 5 M = 128 5 Correct Choice By symmetry, ȳ = 0. x-mom = M y = ∫∫ xρ dA = ∫ −2 ∫ y = 2 128 − 128 7 3 2 = 512 7 4 7 1 ∫ 2 64 − y 6 dy = 1 64y − y dy = 7 3 −2 3 x=y 2 My x-mom x̄ = = = 512 5 = 20 M M 7 128 7 x 2 dx dy = 2 ∫ −2 2 x3 3 4 2 y=−2 4 Work Out: (12 points each. Part credit possible. Show all work.) 10. Find the dimensions and volume of the largest box which sits on the xy-plane and whose upper vertices are on the elliptic paraboloid z = 12 − 2x 2 − 3y 2 . You do not need to show it is a maximum. You MUST eliminate the constraint. Do not use Lagrange multipliers. Maximize V = 2x2yz = 4xy12 − 2x 2 − 3y 2 = 48xy − 8x 3 y − 12xy 3 V x = 48y − 24x 2 y − 12y 3 = −12y2x 2 + y 2 − 4 = 0 V y = 48x − 8x 3 − 36xy 2 = −4x2x 2 + 9y 2 − 12 = 0 Since x = 0 or y = 0 gives V = 0, we can assume x ≠ 0 and y ≠ 0. 2x 2 + y 2 = 4 2x 2 + 9y 2 = 12 and 8y 2 = 8 Subtract: y=1 x2 = 3 x= 3 2 2 z = 12 − 2x 2 − 3y 2 = 12 − 2 3 − 31 = 6 2 2x 2 + 1 = 4 Substitute back: Substitute back: The dimensions are: L = 2x = V = LWH = The volume is: W = 2y = 2 6 H=z=6 6 26 = 12 6 11. A pot of water is sitting on a stove. The pot is a cylinder of radius 3 inches and height 4 inches. If the origin is located at the center of the bottom, then the temperature of the water is ∫∫∫ T dV T = 102 + x 2 + y 2 − z. Find the average temperature of the water: T ave = . ∫∫∫ dV ∫∫∫ dV = ∫ 0 ∫ 0 ∫ 0 r dz dr dθ = 2π 3 4 θ 2π 0 r2 2 3 z 0 4 0 = 2π 9 4 = 36π 2 ∫∫∫ T dV = ∫ 0 ∫ 0 ∫ 0 102 + r 2 − zr dz dr dθ = 2π ∫ 0 2π 3 4 3 2 102z + r 2 z − z 2 = πr 2 h 4 r dr z=0 = 2π ∫ 408 + 4r 2 − 8r dr = 2π ∫ 400r + 4r 3 dr = 2π200r 2 + r 4 3r=0 = 2π1881 = 3762π 3 3 0 0 T ave = 3762π = 209 36π 2 5 12. Compute ∫∫ x dx dy over the "diamond" y D 6 shaped region bounded by the curves y = x2 y = 3 + x2 y = 4 − x2 4 y = 6 − x2 2 Use the curvilinear coordinates u = y + x 2 and v = y − x 2 . 0 0.0 (Half credit for using rectangular coordinates.) 0.5 1.0 1.5 2.0 x The boundary curves are v = 0, v = 3, u = 4, u = 6 We solve for x and y and compute the Jacobian factor: u + v = 2y J= u − v = 2x 2 ∂y ∂u ∂y ∂v ∂x ∂u ∂x ∂v = ∫∫ x dx dy = ∫ 0 ∫ 4 3 u − v −1/2 2 2 1 2 u − v −1/2 2 2 1 2 − The integrand is x = 6 D x= u−v y = u+v 2 2 = u − v −1/2 u − v −1/2 + 4 2 4 2 = u − v −1/2 2 2 u−v . So 2 u − v u − v −1/2 du dv = 2 2 2 ∫0 ∫4 3 6 1 du dv = 1 32 = 3 4 4 2 13. The sides of a cylinder C of radius 3 and height 4 may be parametrized by Rh, θ = 3 cos θ, 3 sin θ, h for 0 ≤ θ ≤ 2π and 0 ≤ h ≤ 4. ⃗ for F ⃗ ⋅ dS ⃗ = −yz 2 , xz 2 , z 3 and outward normal. Compute ∫∫ ⃗ ∇×F C ⃗ = ⃗e h × ⃗e θ , ⃗ ⃗ and HINT: Find ⃗e h , ⃗e θ , N ∇×F ⃗ ⃗ ∇×F ⃗ h, θ . R Rh, θ = 3 cos θ, 3 sin θ, h ⃗e h = ⃗e θ = î 0, − 3 sin θ, ̂ 0, 3 cos θ, k̂ 1 0 ⃗ = ⃗e h × ⃗e θ = î−3 cos θ − ̂ 3 sin θ + k̂ 0 = −3 cos θ, −3 sin θ, 0 N ⃗ = 3 cos θ, 3 sin θ, 0 Reverse N 6 ⃗ ⃗ = ∇×F î ̂ k̂ ∂x ∂y ∂z = î0 − 2xz − ̂ 0 − −2yz + k̂ z 2 − −z 2 = −2xz, −2yz, 2z 2 −yz 2 xz 2 z 3 ⃗ ⃗ ∇×F ⃗ h, θ R = −6h cos θ, −6h sin θ, 2h 2 ⃗ ⃗⋅N ⃗ = −18h cos 2 θ − 18h sin 2 θ = −18h ∇×F ∫∫ ⃗∇ × F⃗ ⋅ dS⃗ = ∫ ∫ ⃗∇ × F⃗ ⋅ N⃗ dh dθ = ∫ 0 ∫ 0 −18h dh dθ = −2π9h 2 40 = −288π 2π 4 C 14. The hemispherical surface x 2 + y 2 + z 2 = 9 has surface density ρ = x 2 + y 2 . ⃗ ϕ, θ = 3 sin ϕ cos θ, 3 sin ϕ sin θ, 3 cos ϕ. The surface may be parametrized by R Find the mass and center of mass of the surface. ⃗ = ⃗e ϕ × ⃗e θ , HINT: Find ⃗e ϕ , ⃗e θ , N ⃗ N ⃗ ϕ, θ . and ρ R ⃗ ϕ, θ = 3 sin ϕ cos θ, 3 sin ϕ sin θ, 3 cos ϕ R î ̂ k̂ ⃗e ϕ = 3 cos ϕ cos θ, 3 cos ϕ sin θ, −3 sin ϕ ⃗e θ = −3 sin ϕ sin θ, 3 sin ϕ cos θ, 0 ⃗ = ⃗e ϕ × ⃗e θ = î9 sin 2 ϕ cos θ − ̂ −9 sin 2 ϕ sin θ + k̂ 9 sin ϕ cos ϕ cos 2 θ + 9 sin ϕ cos ϕ sin 2 θ N ⃗ = 9 sin 2 ϕ cos θ, 9 sin 2 ϕ sin θ, 9 sin ϕ cos ϕ N ⃗ = N 2 2 9 sin 2 ϕ cos θ + 9 sin 2 ϕ sin θ + 9 sin ϕ cos ϕ 2 = 9 sin 4 ϕ + sin 2 ϕ cos 2 ϕ = 9 sin ϕ ⃗ ϕ, θ ρ R = 3 sin ϕ cos θ 2 + 3 sin ϕ sin θ 2 = 9 sin 2 ϕ M= ∫∫ ρ dS = ∫∫ ρ Let u = cos ϕ ⃗ ϕ, θ R ⃗ dϕ dθ = N π/2 ∫0 ∫0 2π 9 sin 2 ϕ9 sin ϕ dϕ dθ = 2π81 ∫ π/2 0 1 − cos 2 ϕ sin ϕ dϕ du = − sin ϕ dϕ 0 3 M = −162π ∫ 1 − u 2 du = −162π u − u 3 1 0 1 = 162π 1 − 1 3 = 324π = 108π 3 By symmetry x̄ = ȳ = 0 z-mom = M xy = ∫∫ z ρ dS = ∫∫ 3 cos ϕ ρ = 2π243 ∫ z̄ = π/2 0 ⃗ ϕ, θ R cos ϕ sin 3 ϕ dϕ = 486π ⃗ dϕ dθ = N sin 4 ϕ 4 π/2 0 π/2 ∫0 ∫0 2π 3 cos ϕ9 sin 2 ϕ9 sin ϕ dϕ dθ = 243π 2 z-mom = 243π 1 = 9 M 2 108π 8 7