Work — Question 4

Section 7-3 · Physics pages 898–899

Question 4 A force schedule matters even when displacement cancels An actuator exerts +8 N while a slider moves from x=0 to x=3 m, then exerts +2 N while it moves back to x=0. Forces are along x and constant within each leg. out: Fx = +8 N back: Fx = +2 N x = 0 x = 3 m Path arrows show motion; the actuator force points right on both legs. (a) Find work in each leg and the cycle total. (b) What work would result if +8 N acted on both legs? (c) Can zero net displacement alone establish zero work for the original schedule?
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Question 4 - Solution A force schedule matters even when displacement cancels out: Fx = +8 N back: Fx = +2 N x = 0 x = 3 m (a) Pair each force with its own displacement. The governing relation is Wcycle = Fout∆xout + Fback∆xback W1 = 8(3) = 24 J, W2 = 2(−3) = −6 J; total is 18 J. (b) Apply one unchanged force. With +8 N both ways, total work is 24 −24 = 0 J. (c) Keep the history of the interaction. No. The original force is not constant across the complete trip. Different force-displacement pairings give different work even when the particle returns to its starting point.

Question 4

A force schedule matters even when displacement cancels

An actuator exerts +8 N while a slider moves from x=0 to x=3 m, then exerts +2 N while it moves back to x=0. Forces are along x and constant within each leg.

Diagram shown in the original SVG worksheet.

  1. Find work in each leg and the cycle total.

  2. What work would result if +8 N acted on both legs?

  3. Can zero net displacement alone establish zero work for the original schedule?

Question 4 - Solution

A force schedule matters even when displacement cancels

Diagram shown in the original SVG worksheet.

(a) Pair each force with its own displacement.

The governing relation is Wcycle=FoutΔxout+FbackΔxback\boxed{W_{\mathrm{cycle}}=F_{\mathrm{out}}\Delta x_{\mathrm{out}}+F_{\mathrm{back}}\Delta x_{\mathrm{back}}}

W1=8(3)=24J,W2=2(−3)=−6J;W_1=8(3)=24\ \mathrm J,\qquad W_2=2(-3)=-6\ \mathrm J; total is 18 J.

(b) Apply one unchanged force.

With +8 N both ways, total work is 24−24=0J.24-24=0\ \mathrm J.

(c) Keep the history of the interaction.

No. The original force is not constant across the complete trip. Different force-displacement pairings give different work even when the particle returns to its starting point.