Multivariable-Calculus Ā· Unit 18 Ā· Video 1 Ā· Interactive Practice

Work Around a Closed Curve: Integrating Piece by Piece

IKey Formulas

FormulaNameWhat it says
∮CFāƒ—ā‹…drāƒ—=∫C1+∫C2+∫C3\displaystyle\oint_C \vec F \cdot d\vec r = \int_{C_1} + \int_{C_2} + \int_{C_3}Piece by pieceSplit CC at its corners; each piece gets its own parametrisation
āˆ«āˆ’CFāƒ—ā‹…drāƒ—=āˆ’āˆ«CFāƒ—ā‹…drāƒ—\displaystyle\int_{-C} \vec F \cdot d\vec r = -\int_C \vec F \cdot d\vec rReversing a pathEvery step drāƒ—d\vec r flips, so the work changes sign
x=cos⁔θ,Ā y=sin⁔θ:y dx+x dy=cos⁔2θ dĪøx = \cos\theta,\ y = \sin\theta:\quad y\,dx + x\,dy = \cos 2\theta\,d\thetaThe arc C2C_2∫0Ļ€/4cos⁔2θ dĪø=12\int_0^{\pi/4} \cos 2\theta\,d\theta = \tfrac12
0+12āˆ’12=00 + \tfrac12 - \tfrac12 = 0Total for Fāƒ—=y ı^+x ȷ^\vec F = y\,\hat\imath + x\,\hat\jmathAround the sector from 00 to Ļ€/4\pi/4

Key Insight: on every piece the integrand is the same expression y dx+x dyy\,dx + x\,dy; only the substitution changes.

IIWalking the Loop

The work of Fāƒ—=⟨y,x⟩\vec F = \langle y, x\rangle around the sector builds up piece by piece: 00, then 12\tfrac12, then āˆ’12-\tfrac12.

IIIReversing the Diagonal

Along āˆ’C3-C_3 the steps drāƒ—d\vec r point the other way, so every Fāƒ—ā‹…drāƒ—\vec F \cdot d\vec r changes sign.

IVQuiz Questions

Problem 1 Ā· A Single Segment

Given: Fāƒ—=y ı^+x ȷ^\vec F = y\,\hat\imath + x\,\hat\jmath and CC the segment from (0,0)(0, 0) to (1,2)(1, 2) — find ∫Cy dx+x dy\int_C y\,dx + x\,dy.

āœ… Correct! With x=tx = t, y=2ty = 2t the integrand is 4t dt4t\,dt, and ∫014t dt=2\int_0^1 4t\,dt = 2.
āŒ Only one of the two terms. y dx=2t dty\,dx = 2t\,dt and x dy=tā‹…2 dtx\,dy = t \cdot 2\,dt each give 11; the integral is their sum.
āŒ That is the integrand, not the integral. y dx+x dy=4t dty\,dx + x\,dy = 4t\,dt, and integrating from 00 to 11 gives 22.
āŒ The parameter range is right, the integrand is not. Both dx=dtdx = dt and dy=2 dtdy = 2\,dt must be substituted: 2t dt+2t dt2t\,dt + 2t\,dt.
Show solution

Parametrise: x=tx = t, y=2ty = 2t, 0≤t≤10 \le t \le 1, so dx=dtdx = dt and dy=2 dtdy = 2\,dt. Then

∫Cy dx+x dy=∫012t dt+tā‹…2 dt=∫014t dt=[2t2]01=2.\int_C y\,dx + x\,dy = \int_0^1 2t\,dt + t \cdot 2\,dt = \int_0^1 4t\,dt = \big[2t^2\big]_0^1 = 2.

Problem 2 Ā· Backwards Along the Same Curve

Given: for some field Fāƒ—\vec F and curve CC, ∫CFāƒ—ā‹…drāƒ—=34\int_C \vec F \cdot d\vec r = \tfrac34 — find āˆ«āˆ’CFāƒ—ā‹…drāƒ—\int_{-C} \vec F \cdot d\vec r.

āœ… Correct! Reversing the path reverses every step drāƒ—d\vec r, so the work changes sign.
āŒ The direction matters. āˆ’C-C has the same points but every drāƒ—d\vec r points the other way, so each Fāƒ—ā‹…drāƒ—\vec F \cdot d\vec r flips sign.
āŒ That would be CC followed by āˆ’C-C. Going out and coming back gives 34āˆ’34=0\tfrac34 - \tfrac34 = 0; the question asks for āˆ’C-C alone.
āŒ The parametrisation does not matter. Any parametrisation of āˆ’C-C in its direction gives the same value, āˆ’āˆ«CFāƒ—ā‹…drāƒ—-\int_C \vec F \cdot d\vec r.
Show solution

āˆ’C-C is the same set of points traversed in the opposite direction. Each small step drāƒ—d\vec r is replaced by āˆ’drāƒ—-d\vec r, so

āˆ«āˆ’CFāƒ—ā‹…drāƒ—=āˆ’āˆ«CFāƒ—ā‹…drāƒ—=āˆ’34.\int_{-C} \vec F \cdot d\vec r = -\int_C \vec F \cdot d\vec r = -\tfrac34.

Problem 3 Ā· A Longer Arc

Given: Fāƒ—=y ı^+x ȷ^\vec F = y\,\hat\imath + x\,\hat\jmath and CC the arc of the unit circle from Īø=0\theta = 0 to Īø=Ļ€/3\theta = \pi/3, counterclockwise — find ∫Cy dx+x dy\int_C y\,dx + x\,dy.

āœ… Correct! ∫0Ļ€/3cos⁔2θ dĪø=12sin⁔2Ļ€3=34\int_0^{\pi/3} \cos 2\theta\,d\theta = \tfrac12 \sin\tfrac{2\pi}{3} = \tfrac{\sqrt3}{4}.
āŒ Missing the factor 12\tfrac12. An antiderivative of cos⁔2Īø\cos 2\theta is 12sin⁔2Īø\tfrac12 \sin 2\theta, not sin⁔2Īø\sin 2\theta.
āŒ Check the sign of the integrand. y dx=āˆ’sin⁔2θ dĪøy\,dx = -\sin^2\theta\,d\theta and x dy=cos⁔2θ dĪøx\,dy = \cos^2\theta\,d\theta, so the integrand is cos⁔2Īøāˆ’sin⁔2Īø=cos⁔2Īø\cos^2\theta - \sin^2\theta = \cos 2\theta, not its negative.
āŒ That is the value for the arc up to Ļ€/4\pi/4. Here the upper limit is Ļ€/3\pi/3, so 2Īø2\theta ends at 2Ļ€/32\pi/3.
Show solution

On the unit circle x=cos⁔θx = \cos\theta, y=sin⁔θy = \sin\theta, so dx=āˆ’sin⁔θ dĪødx = -\sin\theta\,d\theta and dy=cos⁔θ dĪødy = \cos\theta\,d\theta:

∫Cy dx+x dy=∫0Ļ€/3(cos⁔2Īøāˆ’sin⁔2Īø) dĪø=∫0Ļ€/3cos⁔2θ dĪø.\int_C y\,dx + x\,dy = \int_0^{\pi/3} (\cos^2\theta - \sin^2\theta)\,d\theta = \int_0^{\pi/3} \cos 2\theta\,d\theta. =[12sin⁔2Īø]0Ļ€/3=12sin⁔2Ļ€3=34.= \Big[\tfrac12 \sin 2\theta\Big]_0^{\pi/3} = \tfrac12 \sin\tfrac{2\pi}{3} = \tfrac{\sqrt3}{4}.

Problem 4 Ā· The Rotation Field Around the Sector

Given: Gāƒ—=āˆ’y ı^+x ȷ^\vec G = -y\,\hat\imath + x\,\hat\jmath and the same closed curve as the video: C1C_1 along the xx-axis from (0,0)(0,0) to (1,0)(1,0), C2C_2 along the unit circle to (12,12)(\tfrac{1}{\sqrt2}, \tfrac{1}{\sqrt2}), C3C_3 back along the diagonal — find ∮CGāƒ—ā‹…drāƒ—\oint_C \vec G \cdot d\vec r.

āœ… Correct! Only the arc contributes: Gāƒ—ā‹…T^=1\vec G \cdot \hat T = 1 there, times the arc length Ļ€/4\pi/4.
āŒ The zero total was special to ⟨y,x⟩\langle y, x\rangle. For Gāƒ—\vec G the arc gives Ļ€/4\pi/4 and nothing cancels it.
āŒ That is the work around the whole unit circle. The curve here contains only an eighth of the circle.
āŒ The diagonal contributes nothing. On y=x=ty = x = t, āˆ’y dx+x dy=āˆ’t dt+t dt=0-y\,dx + x\,dy = -t\,dt + t\,dt = 0: Gāƒ—\vec G is perpendicular to the diagonal.
Show solution

The integrand is āˆ’y dx+x dy-y\,dx + x\,dy.

C1C_1: y=0y = 0, dy=0dy = 0, so the integrand is 00.

C2C_2: x=cos⁔θx = \cos\theta, y=sin⁔θy = \sin\theta: āˆ’sin⁔θ(āˆ’sin⁔θ) dĪø+cos⁔θcos⁔θ dĪø=dĪø-\sin\theta(-\sin\theta)\,d\theta + \cos\theta\cos\theta\,d\theta = d\theta, so the work is ∫0Ļ€/4dĪø=Ļ€4\int_0^{\pi/4} d\theta = \tfrac{\pi}{4}.

C3C_3: on y=xy = x, dy=dxdy = dx, so āˆ’y dx+x dy=āˆ’x dx+x dx=0-y\,dx + x\,dy = -x\,dx + x\,dx = 0.

∮CGāƒ—ā‹…drāƒ—=0+Ļ€4+0=Ļ€4.\oint_C \vec G \cdot d\vec r = 0 + \tfrac{\pi}{4} + 0 = \tfrac{\pi}{4}.

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