Work Done on a System by an External Force — Question 1

Section 8-6 · Physics pages 1112–1113

Question 1 Applied work shared by motion and elastic deformation Assume no heat transfer across the stated system boundary during the process unless otherwise specified. A 2 kg slider and its ideal horizontal spring form a system. The spring support is fixed. Initially the slider is at rest and the spring relaxed. An external agent does 25 J of work; final spring extension is 0.50 m and k=40 N/m. There is no friction. system Wext The system includes the slider and spring; its fixed support does no work. (a) Find the change in spring potential energy. (b) Find final kinetic energy and speed. (c) Why would setting the external work equal to kinetic-energy change alone fail?
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Question 1 - Solution Applied work shared by motion and elastic deformation system Wext (a) Evaluate the elastic store. The spring begins relaxed, so ∆Us = 1 2kx2 f = 1 2(40)(.50)2 = 5 J . (b) Account for both system energy forms. External work changes both system stores: 25 = ∆K + 5 ⇒Kf = 20 J , vf = √ 2Kf/m = √ 20 = 4.472 m/s . (c) Distinguish external from net particle work. For the chosen slider–spring system, Wext = ∆K + ∆Us. For the slider alone, the equivalent relation is ∆K = Wa + Ws = 25 −5. Equating external input to kinetic gain alone would omit the 5 J stored in deformation.

Question 1

Applied work shared by motion and elastic deformation

Assume no heat transfer across the stated system boundary during the process unless otherwise specified. A 2 kg slider and its ideal horizontal spring form a system. The spring support is fixed. Initially the slider is at rest and the spring relaxed. An external agent does 25 J of work; final spring extension is 0.50 m and k=40 N/m. There is no friction.

Diagram shown in the original SVG worksheet.

  1. Find the change in spring potential energy.

  2. Find final kinetic energy and speed.

  3. Why would setting the external work equal to kinetic-energy change alone fail?

Question 1 - Solution

Applied work shared by motion and elastic deformation

Diagram shown in the original SVG worksheet.

(a) Evaluate the elastic store.

The spring begins relaxed, so ΔUs=12kxf2=12(40)(.50)2=5J.\boxed{\Delta U_s=\tfrac12kx_f^2=\tfrac12(40)(.50)^2=5\ \mathrm J}.

(b) Account for both system energy forms.

External work changes both system stores: 25=ΔK+5⇒Kf=20J,25=\Delta K+5\Rightarrow\boxed{K_f=20\ \mathrm J}, vf=2Kf/m=20=4.472m/s.\boxed{v_f=\sqrt{2K_f/m}=\sqrt{20}=4.472\ \mathrm{m/s}}.

(c) Distinguish external from net particle work.

For the chosen slider–spring system, Wext=ΔK+ΔUs.W_{\mathrm{ext}}=\Delta K+\Delta U_s. For the slider alone, the equivalent relation is ΔK=Wa+Ws=25−5\Delta K=W_a+W_s=25-5. Equating external input to kinetic gain alone would omit the 5 J stored in deformation.