Line Integrals of Vector Fields β€” Question 7

Section 18-4 Β· Calculus pages 3413–3414

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Question 7

The field 𝑭(x,y)=βŸ¨βˆ’y,x⟩\mathbf F(x,y)=\langle-y,x\rangle acts between A=(0,0)A=(0,0) and B=(1,1)B=(1,1). Compare the work along C1:𝒓(t)=⟨t,t⟩,0≀t≀1,C_1:\mathbf r(t)=\langle t,t\rangle,\quad 0\le t\le 1, and the broken path C2C_2 that goes from (0,0)(0,0) to (1,0)(1,0) to (1,1)(1,1).

Tasks

  1. Compute the work along C1C_1.

  2. Compute the work along both pieces of C2C_2.

  3. Explain what the comparison demonstrates.

Question 7 – Solution

Strategy. Evaluate the same vector-field line integral on two explicitly parametrized paths with common endpoints.

Step 1: Diagonal path On C1C_1, 𝑭(𝒓(t))=βŸ¨βˆ’t,t⟩,𝒓′(t)=⟨1,1⟩.\mathbf F(\mathbf r(t))=\langle-t,t\rangle,\qquad \mathbf r'(t)=\langle 1,1\rangle. The dot product is βˆ’t+t=0-t+t=0, so W1=0W_1=\boxed{0}.

Diagram shown in the original SVG worksheet.

Step 2: Broken path On the horizontal piece ⟨t,0⟩\langle t,0\rangle, the dot product ⟨0,tβŸ©β‹…βŸ¨1,0⟩\langle 0,t\rangle\cdot\langle 1,0\rangle is zero. On the vertical piece ⟨1,s⟩\langle 1,s\rangle, βŸ¨βˆ’s,1βŸ©β‹…βŸ¨0,1⟩=1,0≀s≀1.\langle-s,1\rangle\cdot\langle 0,1\rangle=1,\qquad 0\le s\le 1. Thus W2=0+∫011ds=1.W_2=0+\int_0^1 1\,ds=\boxed{1}.

Step 3: Compare Since W1β‰ W2W_1\ne W_2 despite identical endpoints, the work for this field depends on the path taken.

Verification Along the diagonal the field is perpendicular to the motion. Along the final vertical piece of C2C_2, its upward component is 11, explaining the extra unit of work.