Surface Integrals of Vector Fields β€” Question 7

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Question 7

Let SS be the upper hemisphere x2+y2+z2=4x^2+y^2+z^2=4, zβ‰₯0z\ge 0, oriented outward. Compute the flux of the constant field 𝑭=⟨0,0,1⟩\mathbf F=\langle 0,0,1\rangle across SS.

Tasks

  1. Express the hemisphere as a graph and find its upward vector element.

  2. Evaluate the flux using projection onto the xyxy-plane.

  3. State the result for the opposite orientation.

Original worksheet page 1: question and worked solution for 6-4-007
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Question 7 – Solution

Strategy. A constant vertical field dotted with the upward graph element leaves exactly the projected area element.

Step 1: Graph orientation Write z=g(x,y)=4βˆ’x2βˆ’y2z=g(x,y)=\sqrt{4-x^2-y^2} over the disk D:x2+y2≀4D:x^2+y^2\le 4. The outward orientation on the upper hemisphere is upward, so 𝒏dS=βŸ¨βˆ’gx,βˆ’gy,1⟩dA.\mathbf n\,dS=\langle-g_x,-g_y,1\rangle\,dA.

See the diagram in the original worksheet below.

Step 2: Project Since 𝑭=π’Œ\mathbf F=\mathbf k, 𝑭⋅𝒏dS=π’Œβ‹…βŸ¨βˆ’gx,βˆ’gy,1⟩dA=dA.\mathbf F\cdot\mathbf n\,dS =\mathbf k\cdot\langle-g_x,-g_y,1\rangle\,dA=dA. Thus ∬S𝑭⋅𝒏dS=∬DdA=Ο€(22)=4Ο€.\boxed{\iint_S\mathbf F\cdot\mathbf n\,dS =\iint_DdA=\pi(2^2)=4\pi}.

Step 3: Reverse orientation With the inward orientation the vector element changes sign, so the flux is βˆ’4Ο€\boxed{-4\pi}.

Verification The graph derivatives become unbounded at the equator, but their components are annihilated by the dot product with π’Œ\mathbf k. Truncating to radius R<2R<2 and taking Rβ†’2βˆ’R\to 2^- yields the same result.

Original worksheet page 2: question and worked solution for 6-4-007

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