Line Integrals of Vector Fields โ€” Question 4

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Question 4

Let CC be the unit circle and let ๐‘ญ(x,y)=โŸจโˆ’y,xโŸฉ.\mathbf F(x,y)=\langle-y,x\rangle. Compute โˆฎC๐‘ญโ‹…d๐’“\displaystyle\oint_C\mathbf F\cdot d\mathbf r when CC is traversed (a) counterclockwise and (b) clockwise.

Tasks

  1. Parametrize the counterclockwise circle and evaluate the integral.

  2. Use orientation reversal to obtain the clockwise value.

  3. Interpret the signs using the direction of the field.

Original worksheet page 1: question and worked solution for 5-4-004
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Question 4 โ€“ Solution

Strategy. On the unit circle this field is the counterclockwise unit tangent, making the dot product especially simple.

Step 1: Counterclockwise traversal Take ๐’“(t)=โŸจcos⁡t,sin⁡tโŸฉ,0โ‰คtโ‰ค2ฯ€.\mathbf r(t)=\langle\cos t,\sin t\rangle,\quad 0\le t\le 2\pi. Then ๐‘ญ(๐’“(t))=โŸจโˆ’sin⁡t,cos⁡tโŸฉ=๐’“โ€ฒ(t).\mathbf F(\mathbf r(t))=\langle-\sin t,\cos t\rangle=\mathbf r'(t).

See the diagram in the original worksheet below.

Consequently, โˆฎC๐‘ญโ‹…d๐’“=โˆซ02ฯ€๐’“โ€ฒ(t)โ‹…๐’“โ€ฒ(t)dt=โˆซ02ฯ€1dt=2ฯ€.\oint_C\mathbf F\cdot d\mathbf r =\int_0^{2\pi}\mathbf r'(t)\cdot\mathbf r'(t)\,dt =\int_0^{2\pi}1\,dt=\boxed{2\pi}.

Step 2: Reverse the orientation Reversing a vector-field line integral changes its sign, so the clockwise value is โˆ’2ฯ€.\boxed{-2\pi}.

Verification The field assists counterclockwise motion at every point and opposes clockwise motion at every point, so the respective signs must be positive and negative.

Original worksheet page 2: question and worked solution for 5-4-004

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