Computing Flux via Divergence Theorem - Calculus 3

  1. Consider the vector field F⃗=⟨x+y2z,y+x2z,z+x2y2⟩\vec{F} = \langle x + y^2z, y + x^2z, z + x^2y^2 \rangle and the closed surface SS that bounds the region between two concentric spheres: 1≤x2+y2+z2≤41 \leq x^2 + y^2 + z^2 \leq 4. The surface SS consists of the outer sphere (radius 2) with outward normal and the inner sphere (radius 1) with inward normal. If we want to apply the Divergence Theorem directly to find the flux through SS, what is the correct setup?
    Answer: ∭1≤x2+y2+z2≤4(1+1+1) dV=3⋅28π3=28π\iiint_{1 \leq x^2+y^2+z^2 \leq 4} (1 + 1 + 1) \, dV = 3 \cdot \frac{28\pi}{3} = 28\pi To apply the Divergence Theorem, we need ∇⋅F⃗=∂∂x(x+y2z)+∂∂y(y+x2z)+∂∂z(z+x2y2)=1+1+1=3\nabla \cdot \vec{F} = \frac{\partial}{\partial x}(x + y^2z) + \frac{\partial}{\partial y}(y + x^2z) + \frac{\partial}{\partial z}(z + x^2y^2) = 1 + 1 + 1 = 3. The region is the spherical shell with volume 4π3(23−13)=4π3⋅7=28π3\frac{4\pi}{3}(2^3 - 1^3) = \frac{4\pi}{3} \cdot 7 = \frac{28\pi}{3}. So the flux is 3⋅28π3=28π3 \cdot \frac{28\pi}{3} = 28\pi. Choice B incorrectly includes x2y2x^2y^2 from the original field. Choice C incorrectly doubles the x2y2x^2y^2 term. Choice D incorrectly computes partial derivatives, getting terms from the original components rather than their derivatives.
  2. A vector field F⃗\vec{F} has the property that its divergence is ∇⋅F⃗=x2+y2+z2\nabla \cdot \vec{F} = x^2 + y^2 + z^2. Consider three regions: (I) the unit ball x2+y2+z2≤1x^2 + y^2 + z^2 \leq 1, (II) the cube [−1,1]3[-1,1]^3, and (III) the cylindrical region x2+y2≤1,−1≤z≤1x^2 + y^2 \leq 1, -1 \leq z \leq 1. If ΦI\Phi_I, ΦII\Phi_{II}, and ΦIII\Phi_{III} represent the outward flux through the boundaries of regions I, II, and III respectively, which ordering is correct?
    Answer: ΦI<ΦIII<ΦII\Phi_I < \Phi_{III} < \Phi_{II} When you encounter a vector field with known divergence and need to compare flux through different surfaces, immediately think of the Divergence Theorem: ∬SF⃗⋅dA⃗=∭V∇⋅F⃗ dV\iint_S \vec{F} \cdot d\vec{A} = \iiint_V \nabla \cdot \vec{F} \, dV. The outward flux through each boundary equals the triple integral of the divergence over the enclosed volume. Since ∇⋅F⃗=x2+y2+z2\nabla \cdot \vec{F} = x^2 + y^2 + z^2, you need to evaluate ∭V(x2+y2+z2) dV\iiint_V (x^2 + y^2 + z^2) \, dV for each region. Notice that this integrand is always non-negative and increases with distance from the origin. For the unit ball (I), using spherical coordinates: ΦI=∫02π∫0π∫01ρ2⋅ρ2sin⁡ϕ dρ dϕ dθ=4π5\Phi_I = \int_0^{2\pi} \int_0^{\pi} \int_0^1 \rho^2 \cdot \rho^2 \sin\phi \, d\rho \, d\phi \, d\theta = \frac{4\pi}{5}. For the cube (II), the integrand reaches its maximum value of 3 at corners like (1,1,1)(1,1,1), and the volume is 8, giving ΦII=8\Phi_{II} = 8. For the cylinder (III), the integrand reaches maximum value 2 at points like (1,0,1)(1,0,1), and the volume is 2π2\pi, giving ΦIII=2π≈6.28\Phi_{III} = 2\pi \approx 6.28. Therefore: ΦI=4π5≈2.51<ΦIII=2π≈6.28<ΦII=8\Phi_I = \frac{4\pi}{5} \approx 2.51 < \Phi_{III} = 2\pi \approx 6.28 < \Phi_{II} = 8. Choice A incorrectly orders the cylinder and cube. Choice C completely reverses the order. Choice D incorrectly places the cylinder as smallest. Strategy tip: For divergence problems, always use the Divergence Theorem to convert surface integrals to volume integrals. Compare how the divergence function behaves over each region's volume and extent.
  3. Let F⃗=⟨P(x,y,z),Q(x,y,z),R(x,y,z)⟩\vec{F} = \langle P(x,y,z), Q(x,y,z), R(x,y,z) \rangle be a vector field where ∇⋅F⃗=6\nabla \cdot \vec{F} = 6 throughout a region EE. The boundary surface SS of EE consists of two parts: S1S_1 with area 10 and S2S_2 with area 15. If the flux of F⃗\vec{F} through S1S_1 is 30 (outward), and the volume of EE is 20, what is the flux through S2S_2 (outward)?
    Answer: 90 When you encounter a problem involving flux through boundary surfaces with known divergence, immediately think of the Divergence Theorem, which connects surface integrals to volume integrals. The Divergence Theorem states that ∬SF⃗⋅n^ dS=∭E∇⋅F⃗ dV\iint_S \vec{F} \cdot \hat{n} \, dS = \iiint_E \nabla \cdot \vec{F} \, dV for a closed surface SS bounding region EE. Since ∇⋅F⃗=6\nabla \cdot \vec{F} = 6 is constant throughout EE with volume 20, the total outward flux through the entire boundary is 6×20=1206 \times 20 = 120. The complete boundary SS consists of S1S_1 and S2S_2, so the total flux equals the sum of fluxes through each part: Flux through S1+Flux through S2=120\text{Flux through } S_1 + \text{Flux through } S_2 = 120. Given that the flux through S1S_1 is 30 (outward), we have 30+Flux through S2=12030 + \text{Flux through } S_2 = 120, yielding Flux through S2=90\text{Flux through } S_2 = 90. Answer choice A (150) incorrectly adds the divergence to the area of S2S_2: 6×15+6×106 \times 15 + 6 \times 10. Choice B (120) represents the total flux through the entire boundary, not just S2S_2. Choice C (-30) might come from incorrectly assuming the flux through S2S_2 has opposite sign to S1S_1, but both are outward fluxes. Study tip: When you see divergence problems with multiple boundary surfaces, always apply the Divergence Theorem to find total flux first, then use the constraint that individual surface fluxes must sum to this total.
  4. Let F⃗=⟨yz,xz,xy+2z⟩\vec{F} = \langle yz, xz, xy + 2z \rangle and let SS be the boundary of the region E={(x,y,z):x2+y2≤1,0≤z≤x2+y2}E = \{(x,y,z) : x^2 + y^2 \leq 1, 0 \leq z \leq x^2 + y^2\}, oriented with outward normals. The surface SS consists of three parts: the bottom disk, the top paraboloid, and a curved connecting surface. What is the flux of F⃗\vec{F} through SS?
    Answer: π\pi Using the Divergence Theorem, the flux equals ∭E∇⋅F⃗ dV\iiint_E \nabla \cdot \vec{F} \, dV. We compute ∇⋅F⃗=∂∂x(yz)+∂∂y(xz)+∂∂z(xy+2z)=0+0+2=2\nabla \cdot \vec{F} = \frac{\partial}{\partial x}(yz) + \frac{\partial}{\partial y}(xz) + \frac{\partial}{\partial z}(xy + 2z) = 0 + 0 + 2 = 2. The region EE has volume ∭E1 dV=∫02π∫01∫0r2r dz dr dθ=∫02π∫01r⋅r2 dr dθ=∫02π∫01r3 dr dθ=2π⋅14=π2\iiint_E 1 \, dV = \int_0^{2\pi} \int_0^1 \int_0^{r^2} r \, dz \, dr \, d\theta = \int_0^{2\pi} \int_0^1 r \cdot r^2 \, dr \, d\theta = \int_0^{2\pi} \int_0^1 r^3 \, dr \, d\theta = 2\pi \cdot \frac{1}{4} = \frac{\pi}{2}. Therefore, the flux is 2⋅π2=π2 \cdot \frac{\pi}{2} = \pi.
  5. Consider the vector field F⃗=⟨x3,y3,z3⟩\vec{F} = \langle x^3, y^3, z^3 \rangle and the surface SS consisting of the portion of the sphere x2+y2+z2=9x^2 + y^2 + z^2 = 9 where z≥0z \geq 0, together with the disk x2+y2≤9x^2 + y^2 \leq 9 in the xyxy-plane. Both surfaces are oriented with outward-pointing normals. Which expression correctly represents the flux of F⃗\vec{F} through SS using the Divergence Theorem?
    Answer: ∭E(3x2+3y2+3z2) dV\iiint_E (3x^2 + 3y^2 + 3z^2) \, dV where EE is the upper hemisphere The Divergence Theorem states that flux through a closed surface equals ∭E∇⋅F⃗ dV\iiint_E \nabla \cdot \vec{F} \, dV. Here, ∇⋅F⃗=∂∂x(x3)+∂∂y(y3)+∂∂z(z3)=3x2+3y2+3z2\nabla \cdot \vec{F} = \frac{\partial}{\partial x}(x^3) + \frac{\partial}{\partial y}(y^3) + \frac{\partial}{\partial z}(z^3) = 3x^2 + 3y^2 + 3z^2. The region EE is the upper hemisphere (the region enclosed by SS). Choice A has the wrong divergence expression. Choice B uses the wrong region (full sphere instead of upper hemisphere). Choice C gives the flux integral setup but doesn't use the Divergence Theorem as requested.
  6. Let SS be the closed surface of the tetrahedron with vertices at (0,0,0)(0,0,0), (2,0,0)(2,0,0), (0,3,0)(0,3,0), and (0,0,1)(0,0,1), oriented with outward normals. For the vector field F⃗=⟨x2,y2,z2⟩\vec{F} = \langle x^2, y^2, z^2 \rangle, a student attempts to use the Divergence Theorem but makes an error in setting up the integral. Which of the following represents the most likely incorrect setup?
    Answer: ∫02∫03∫01(2x+2y+2z) dz dy dx\int_0^2 \int_0^3 \int_0^1 (2x + 2y + 2z) \, dz \, dy \, dx The correct application of the Divergence Theorem requires ∇⋅F⃗=2x+2y+2z\nabla \cdot \vec{F} = 2x + 2y + 2z and integration over the tetrahedron region. The tetrahedron is defined by x≥0,y≥0,z≥0x \geq 0, y \geq 0, z \geq 0 and x2+y3+z≤1\frac{x}{2} + \frac{y}{3} + z \leq 1. Choice A gives the correct integrand and bounds. Choice B reorders the integration correctly with proper bounds. Choice C is the most likely student error: using a rectangular box [0,2]×[0,3]×[0,1][0,2] \times [0,3] \times [0,1] instead of the actual tetrahedron region, which significantly overestimates the integration domain. Choice D uses the wrong integrand (the original field instead of its divergence).
  7. Consider the vector field F⃗=⟨ex+y,sin⁡(xy),z3−z⟩\vec{F} = \langle e^{x+y}, \sin(xy), z^3 - z \rangle and the cube [0,1]×[0,1]×[0,1][0,1] \times [0,1] \times [0,1] with outward orientation. A student correctly identifies that ∇⋅F⃗=ex+y+xcos⁡(xy)+3z2−1\nabla \cdot \vec{F} = e^{x+y} + x\cos(xy) + 3z^2 - 1 but then claims the Divergence Theorem cannot be applied because "the divergence is too complicated to integrate." What is the flaw in this reasoning?
    Answer: The Divergence Theorem can still be applied; computational difficulty doesn't invalidate the theorem's applicability The Divergence Theorem applies to any vector field with continuous partial derivatives on a region bounded by a piecewise smooth closed surface, regardless of how complicated the divergence expression is. The computational difficulty of evaluating ∭(ex+y+xcos⁡(xy)+3z2−1) dV\iiint (e^{x+y} + x\cos(xy) + 3z^2 - 1) \, dV doesn't affect the theorem's validity. Choice A is incorrect - the divergence calculation is correct (∂∂y(sin⁡(xy))=xcos⁡(xy)\frac{\partial}{\partial y}(\sin(xy)) = x\cos(xy)). Choice B is wrong - the divergence can be any function. Choice D is incorrect - cubes are standard examples of valid regions for the Divergence Theorem.
  8. Consider the vector field F⃗=⟨f(x),g(y),h(z)⟩\vec{F} = \langle f(x), g(y), h(z) \rangle where f′(x)=xf'(x) = x, g′(y)=2yg'(y) = 2y, and h′(z)=3z2h'(z) = 3z^2. Let SS be the boundary of the region E={(x,y,z):0≤x≤2,0≤y≤3,0≤z≤1}E = \{(x,y,z) : 0 \leq x \leq 2, 0 \leq y \leq 3, 0 \leq z \leq 1\}, oriented outward. What additional information is needed to compute the flux of F⃗\vec{F} through SS using the Divergence Theorem?
    Answer: No additional information is needed; the flux can be computed as ∫02∫03∫01(x+2y+3z2) dz dy dx\int_0^2 \int_0^3 \int_0^1 (x + 2y + 3z^2) \, dz \, dy \, dx The Divergence Theorem states that flux = ∭E∇⋅F⃗ dV\iiint_E \nabla \cdot \vec{F} \, dV. Here, ∇⋅F⃗=f′(x)+g′(y)+h′(z)=x+2y+3z2\nabla \cdot \vec{F} = f'(x) + g'(y) + h'(z) = x + 2y + 3z^2. This depends only on the derivatives of the component functions, not the functions themselves. The integral ∫02∫03∫01(x+2y+3z2) dz dy dx\int_0^2 \int_0^3 \int_0^1 (x + 2y + 3z^2) \, dz \, dy \, dx can be evaluated to get the flux. Choice A is incorrect because only the derivatives matter for divergence. Choice C is wrong because the Divergence Theorem handles the surface orientation automatically. Choice D is unnecessary since the derivatives are given as simple polynomials, implying sufficient smoothness.

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