Line Integrals of Vector Fields โ€” Question 9

Section 18-4 ยท Calculus pages 3417โ€“3418

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Question 9

Let CC be the line segment from (0,0)(0,0) to (1,2)(1,2) in the field ๐‘ญ(x,y)=โŸจxโˆ’y,x+yโŸฉ.\mathbf F(x,y)=\langle x-y,x+y\rangle. Compute โˆซC๐‘ญโ‹…d๐’“\displaystyle\int_C\mathbf F\cdot d\mathbf r using both ๐’“1(t)=โŸจt,2tโŸฉ,0โ‰คtโ‰ค1,and๐’“2(u)=โŸจu2,2u2โŸฉ,0โ‰คuโ‰ค1.\mathbf r_1(t)=\langle t,2t\rangle,\ 0\le t\le 1, \quad\text{and}\quad \mathbf r_2(u)=\langle u^2,2u^2\rangle,\ 0\le u\le 1.

Tasks

  1. Evaluate the integral with each parametrization.

  2. Explain why the zero velocity of ๐’“2\mathbf r_2 at u=0u=0 causes no problem.

  3. State the invariance illustrated by the equal answers.

Question 9 โ€“ Solution

Strategy. Carry the parameter derivative through both computations; the slower start must be included in d๐’“d\mathbf r.

Step 1: First parametrization Here ๐‘ญ(๐’“1(t))=โŸจโˆ’t,3tโŸฉ,๐’“1โ€ฒ(t)=โŸจ1,2โŸฉ.\mathbf F(\mathbf r_1(t))=\langle-t,3t\rangle,\qquad \mathbf r_1'(t)=\langle 1,2\rangle. Thus โˆซ01(โˆ’t+6t)dt=โˆซ015tdt=52.\int_0^1(-t+6t)\,dt=\int_0^1 5t\,dt=\boxed{\frac 52}.

Step 2: Nonuniform parametrization Now ๐‘ญ(๐’“2(u))=โŸจโˆ’u2,3u2โŸฉ,๐’“2โ€ฒ(u)=โŸจ2u,4uโŸฉ.\mathbf F(\mathbf r_2(u))=\langle-u^2,3u^2\rangle,\qquad \mathbf r_2'(u)=\langle 2u,4u\rangle. Therefore โˆซ01(โˆ’2u3+12u3)du=โˆซ0110u3du=52.\int_0^1(-2u^3+12u^3)\,du =\int_0^1 10u^3\,du=\boxed{\frac 52}.

Step 3: Interpret Although ๐’“2โ€ฒ(0)=๐ŸŽ\mathbf r_2'(0)=\mathbf 0, the curve pauses only at one endpoint and then traces the segment once with the same orientation. The derivative factor compensates for its varying speed.

Verification Both maps begin at (0,0)(0,0), end at (1,2)(1,2), and move monotonically along the same segment, so parameter independence requires the matching values obtained above.