Irreversible Processes and Entropy — Question 8

Section 20-1 · Physics pages 3246–3247

Question 8 Reversing a gas state does not erase the entropy made in a free expansion One mole of ideal gas at 300 K first expands freely and adiabatically from V to 2V . It is then compressed reversibly and isothermally back to V by a 300 K reservoir and a work source. Use R = 8.314 J/(mol K) and ∆S = nR ln(Vf/Vi) for an isothermal ideal-gas change. V p reversible return compression Axes and labels specify the model; the sketch is schematic. (a) Find gas entropy changes for both legs and the net gas change. (b) Find net reservoir entropy change and work input over the complete protocol. Has the whole environment returned to its starting state?
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Question 8 - Solution Reversing a gas state does not erase the entropy made in a free expansion V p reversible return compression (a) Method and calculation ∆Sg,1 = R ln 2 ≈5.76283 J/K, ∆Sg,2 = −R ln 2. ∆Sg,cycle = 0. (b) Interpretation and further calculation Won,2 = RT ln 2 ≈1728.85 J, Qr,2 = RT ln 2. ∆Sr = Qr,2/300 = R ln 2 > 0, Sgen,total = R ln 2. The work source loses energy and the reservoir gains heat. Restoring the gas alone does not reverse every change in the composite. Physical check A cyclic subsystem has zero net entropy change; its surroundings need not.

Question 8

Reversing a gas state does not erase the entropy made in a free expansion

One mole of ideal gas at 300 K first expands freely and adiabatically from VV to 2V2V. It is then compressed reversibly and isothermally back to VV by a 300 K reservoir and a work source. Use R=8.314R=8.314 J/(mol K) and ΔS=nRln⁡(Vf/Vi)\Delta S=nR\ln(V_f/V_i) for an isothermal ideal-gas change.

Diagram shown in the original SVG worksheet.

  1. Find gas entropy changes for both legs and the net gas change.

  2. Find net reservoir entropy change and work input over the complete protocol. Has the whole environment returned to its starting state?

Question 8 - Solution

Reversing a gas state does not erase the entropy made in a free expansion

Diagram shown in the original SVG worksheet.

(a) Method and calculation

ΔSg,1=Rln⁡2≈5.76283J/K,ΔSg,2=−Rln⁡2.\Delta S_{g,1}=R\ln2\approx5.76283\,\mathrm{J/K},\quad\Delta S_{g,2}=-R\ln2.ΔSg,cycle=0.\Delta S_{g,\mathrm{cycle}}=0.

(b) Interpretation and further calculation

Won,2=RTln⁡2≈1728.85J,Qr,2=RTln⁡2.W_{\mathrm{on,2}}=RT\ln2\approx1728.85\,\mathrm J,\quad Q_{r,2}=RT\ln2.ΔSr=Qr,2/300=Rln⁡2>0,Sgen,total=Rln⁡2.\Delta S_r=Q_{r,2}/300=R\ln2>0,\quad S_{\mathrm{gen,total}}=R\ln2.The work source loses energy and the reservoir gains heat. Restoring the gas alone does not reverse every change in the composite.

Physical check

A cyclic subsystem has zero net entropy change; its surroundings need not.