Green's Theorem: Circulation & Flux - Calculus 3

  1. A vector field F(x,y)=(excos⁡y−y,−exsin⁡y+x)\mathbf{F}(x,y) = (e^x \cos y - y, -e^x \sin y + x) is given in a simply connected domain. To determine whether the circulation around any simple closed curve in this domain is zero, which condition should be verified using Green's theorem?
    Answer: Check if ∂Q∂x−∂P∂y=0\frac{\partial Q}{\partial x} - \frac{\partial P}{\partial y} = 0 everywhere in the domain For circulation to be zero around any simple closed curve in a simply connected domain, the vector field must be conservative. By Green's theorem, ∮CF⋅dr=∬D(∂Q∂x−∂P∂y)dA\oint_C \mathbf{F} \cdot d\mathbf{r} = \iint_D \left(\frac{\partial Q}{\partial x} - \frac{\partial P}{\partial y}\right) dA. For this to equal zero for any region DD, we need ∂Q∂x−∂P∂y=0\frac{\partial Q}{\partial x} - \frac{\partial P}{\partial y} = 0 everywhere, which is equivalent to ∂Q∂x=∂P∂y\frac{\partial Q}{\partial x} = \frac{\partial P}{\partial y}. Choice A tests the condition for flux, not circulation. Choice C reverses the order (∂P∂y−∂Q∂x=0\frac{\partial P}{\partial y} - \frac{\partial Q}{\partial x} = 0 is equivalent to choice B). Choice D uses the wrong combination of partial derivatives.
  2. A vector field F(x,y)=(P(x,y),Q(x,y))\mathbf{F}(x,y) = (P(x,y), Q(x,y)) has the property that ∂P∂x+∂Q∂y=6xy\frac{\partial P}{\partial x} + \frac{\partial Q}{\partial y} = 6xy throughout a simply connected region DD. If the outward flux of F\mathbf{F} through the boundary of the square with vertices at (0,0)(0,0), (2,0)(2,0), (2,2)(2,2), and (0,2)(0,2) is computed using Green's theorem, what is the result?
    Answer: 2424 For outward flux through a closed curve, Green's theorem gives ∮CF⋅n ds=∬D(∂P∂x+∂Q∂y)dA\oint_C \mathbf{F} \cdot \mathbf{n} \, ds = \iint_D \left(\frac{\partial P}{\partial x} + \frac{\partial Q}{\partial y}\right) dA. We're given that ∂P∂x+∂Q∂y=6xy\frac{\partial P}{\partial x} + \frac{\partial Q}{\partial y} = 6xy. The region DD is the square [0,2]×[0,2][0,2] \times [0,2]. Therefore, the flux is ∬D6xy dA=∫02∫026xy dx dy=∫026y[x22]02dy=∫026y⋅2 dy=∫0212y dy=12[y22]02=12⋅2=24\iint_D 6xy \, dA = \int_0^2 \int_0^2 6xy \, dx \, dy = \int_0^2 6y \left[\frac{x^2}{2}\right]_0^2 dy = \int_0^2 6y \cdot 2 \, dy = \int_0^2 12y \, dy = 12 \left[\frac{y^2}{2}\right]_0^2 = 12 \cdot 2 = 24.
  3. The vector field F(x,y)=(2x−y,x+3y)\mathbf{F}(x,y) = (2x - y, x + 3y) is defined in the plane. A student wants to compute the circulation of F\mathbf{F} around a triangle with vertices at (1,0)(1,0), (4,0)(4,0), and (2,3)(2,3), oriented counterclockwise. Using Green's theorem, which of the following expressions correctly represents this circulation?
    Answer: ∬D(1−(−1)) dA=∬D2 dA\iint_D (1 - (-1)) \, dA = \iint_D 2 \, dA For circulation using Green's theorem: ∮CF⋅dr=∬D(∂Q∂x−∂P∂y)dA\oint_C \mathbf{F} \cdot d\mathbf{r} = \iint_D \left(\frac{\partial Q}{\partial x} - \frac{\partial P}{\partial y}\right) dA. Here P(x,y)=2x−yP(x,y) = 2x - y and Q(x,y)=x+3yQ(x,y) = x + 3y. Computing the partial derivatives: ∂Q∂x=∂∂x(x+3y)=1\frac{\partial Q}{\partial x} = \frac{\partial}{\partial x}(x + 3y) = 1 and ∂P∂y=∂∂y(2x−y)=−1\frac{\partial P}{\partial y} = \frac{\partial}{\partial y}(2x - y) = -1. Therefore ∂Q∂x−∂P∂y=1−(−1)=2\frac{\partial Q}{\partial x} - \frac{\partial P}{\partial y} = 1 - (-1) = 2. Choice B incorrectly adds the partial derivatives instead of subtracting. Choice C uses the wrong partial derivatives (3 and 2). Choice D also uses wrong values and computes 2−32-3 instead of the correct expression.
  4. Consider the region DD bounded by x2+y2=4x^2 + y^2 = 4 and the vector field F(x,y)=(yx2+y2,−xx2+y2)\mathbf{F}(x,y) = \left(\frac{y}{x^2+y^2}, \frac{-x}{x^2+y^2}\right). A student attempts to use Green's theorem to compute ∮CF⋅dr\oint_C \mathbf{F} \cdot d\mathbf{r} where CC is the circle x2+y2=4x^2 + y^2 = 4 oriented counterclockwise. What is the fundamental issue with this approach?
    Answer: Green's theorem doesn't apply because the vector field is not continuously differentiable throughout the region DD When applying Green's theorem to compute a line integral, you must verify that all conditions are met. Green's theorem states that ∮CF⋅dr=∬D(∂Q∂x−∂P∂y)dA\oint_C \mathbf{F} \cdot d\mathbf{r} = \iint_D \left(\frac{\partial Q}{\partial x} - \frac{\partial P}{\partial y}\right) dA when the vector field F=(P,Q)\mathbf{F} = (P, Q) is continuously differentiable on a simply connected region DD. Here, P(x,y)=yx2+y2P(x,y) = \frac{y}{x^2+y^2} and Q(x,y)=−xx2+y2Q(x,y) = \frac{-x}{x^2+y^2}. The critical issue is that both PP and QQ have denominators of x2+y2x^2+y^2, making them undefined at the origin (0,0)(0,0). Since the region DD is the disk x2+y2≤4x^2 + y^2 \leq 4, it includes the origin where the vector field is not continuously differentiable. This violates a fundamental requirement for Green's theorem. Option A is incorrect because counterclockwise orientation is actually the correct orientation for Green's theorem. Option B is wrong since the circle x2+y2=4x^2 + y^2 = 4 is indeed a simple, closed curve. Option C misidentifies the issue—the region DD (a disk) is simply connected, but that's not the problem here. The correct answer is D because the vector field fails to be continuously differentiable throughout the region due to the singularity at the origin. Study tip: Always check that vector fields are well-defined and differentiable throughout the entire region before applying Green's theorem. Look for denominators that could equal zero within your domain—this is a common trap in circulation problems.
  5. A vector field F(x,y)=(P(x,y),Q(x,y))\mathbf{F}(x,y) = (P(x,y), Q(x,y)) satisfies ∂Q∂x−∂P∂y=x+y\frac{\partial Q}{\partial x} - \frac{\partial P}{\partial y} = x + y in a region DD. If the boundary ∂D\partial D consists of two simple closed curves: an outer curve C1C_1 oriented counterclockwise and an inner curve C2C_2 oriented clockwise, what is ∮C1F⋅dr+∮C2F⋅dr\oint_{C_1} \mathbf{F} \cdot d\mathbf{r} + \oint_{C_2} \mathbf{F} \cdot d\mathbf{r} in terms of the given information?
    Answer: ∬D(x+y) dA\iint_D (x + y) \, dA where DD is the region between C1C_1 and C2C_2 When you encounter a vector field with given curl and multiple boundary curves, you're dealing with Green's theorem in a region with holes. The key insight is understanding how orientations work with the divergence theorem. Green's theorem states that ∮∂DF⋅dr=∬D(∂Q∂x−∂P∂y)dA\oint_{\partial D} \mathbf{F} \cdot d\mathbf{r} = \iint_D \left(\frac{\partial Q}{\partial x} - \frac{\partial P}{\partial y}\right) dA, where ∂D\partial D represents the complete boundary of region DD with proper orientation. For a region with holes, the "positive orientation" means the outer boundary goes counterclockwise while inner boundaries go clockwise - both orientations keep the region to your left as you traverse the boundary. Since C1C_1 is oriented counterclockwise (correct for outer boundary) and C2C_2 is oriented clockwise (correct for inner boundary), both curves have the proper orientation for the region between them. Therefore, ∮C1F⋅dr+∮C2F⋅dr=∬D(x+y)dA\oint_{C_1} \mathbf{F} \cdot d\mathbf{r} + \oint_{C_2} \mathbf{F} \cdot d\mathbf{r} = \iint_D (x + y) dA where DD is the region between the curves. Answer A incorrectly uses the entire region bounded by C1C_1, ignoring the hole created by C2C_2. Answer B has the wrong sign, which would occur if one of the orientations were reversed. Answer D reflects the misconception that opposite orientations automatically cancel - this ignores that the curves bound different parts of the region's boundary. Remember: for regions with holes, Green's theorem applies to the actual region (between boundaries), and "positive orientation" means outer curves go counterclockwise while inner curves go clockwise.

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