Work and Potential Energy — Question 10

Section 8-1 · Physics pages 1030–1031

Question 10 Relative extension when both ends of a spring move An ideal spring of k = 100 N/m initially has extension 0.20 m. Its left end moves right 0.05 m while its right end moves right 0.15 m. The moves are controlled quasistatically. L R 0.05 m 0.15 m Both ends move right; the difference of their displacements changes the extension. (a) Find the final extension. (b) Find the spring potential-energy change and the total spring work on both ends. (c) Would translating both ends right 0.15 m instead produce the same potential change?
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Question 10 - Solution Relative extension when both ends of a spring move L R 0.05 m 0.15 m (a) Subtract the two endpoint displacements. Spring extension changes with the relative endpoint displacement: ∆x = ∆rR −∆rL = .15 −.05 = .10 m, xf = .20 + .10 = .30 m . (b) Use the relative configuration. The potential change fixes the sum of spring endpoint works: ∆Us = 1 2(100)(.302 −.202) = 2.5 J , Ws,L + Ws,R = −2.5 J . Their separate values require the endpoint motion histories. (c) Check rigid translation. For equal translations, ∆x = .15 −.15 = 0 ⇒∆Us = 0, Ws,L + Ws,R = 0 . Rigid translation leaves the relative configuration unchanged, even though each endpoint may exchange work.

Question 10

Relative extension when both ends of a spring move

An ideal spring of k=100k=100 N/m initially has extension 0.20 m. Its left end moves right 0.05 m while its right end moves right 0.15 m. The moves are controlled quasistatically.

Diagram shown in the original SVG worksheet.

  1. Find the final extension.

  2. Find the spring potential-energy change and the total spring work on both ends.

  3. Would translating both ends right 0.15 m instead produce the same potential change?

Question 10 - Solution

Relative extension when both ends of a spring move

Diagram shown in the original SVG worksheet.

(a) Subtract the two endpoint displacements.

Spring extension changes with the relative endpoint displacement: Δx=ΔrR−ΔrL=.15−.05=.10m,xf=.20+.10=.30m.\Delta x=\Delta r_R-\Delta r_L=.15-.05=.10\ \mathrm m,\qquad\boxed{x_f=.20+.10=.30\ \mathrm m}.

(b) Use the relative configuration.

The potential change fixes the sum of spring endpoint works: ΔUs=12(100)(.302−.202)=2.5J,Ws,L+Ws,R=−2.5J.\boxed{\Delta U_s=\tfrac12(100)(.30^2-.20^2)=2.5\ \mathrm J},\qquad\boxed{W_{s,L}+W_{s,R}=-2.5\ \mathrm J}. Their separate values require the endpoint motion histories.

(c) Check rigid translation.

For equal translations, Δx=.15−.15=0⇒ΔUs=0,Ws,L+Ws,R=0.\Delta x=.15-.15=0\Rightarrow\boxed{\Delta U_s=0,\quad W_{s,L}+W_{s,R}=0}. Rigid translation leaves the relative configuration unchanged, even though each endpoint may exchange work.