Change in Entropy — Question 10

Section 20-2 · Physics pages 3270–3271

Question 10 Equal-entropy endpoints do not determine the heat-transfer history For a fixed amount of ideal gas with constant molar capacities, use ∆S = nCV ln(Tf/Ti) + nR ln(Vf/Vi) and Cp = CV + R, with R = 8.314 J/(mol K). A .500 mol monatomic gas starts at 300 K. Its final volume is half its initial volume and its final entropy equals its initial entropy. V T Vi Vi/2 Axes and labels specify the model; the sketch is schematic. (a) Find the required final temperature. (b) Construct a reversible two-leg path: first isothermal compression at 300 K, then fixed-volume heating. Calculate entropy changes on the legs and determine whether zero net entropy change forces zero heat on every leg.
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Question 10 - Solution Equal-entropy endpoints do not determine the heat-transfer history V T Vi Vi/2 (a) Method and calculation 0 = 3 2nR ln(Tf/300) + nR ln(1/2). Tf = 300 22/3 ≈476.220 K. (b) Interpretation and further calculation ∆S1 = −nR ln 2, ∆S2 = 3 2nR ln(22/3) = nR ln 2. Q1 = −nR(300) ln 2, Q2 = 3 2nR(Tf −300) > 0. Each leg transfers heat although the endpoint entropy difference is zero. A reversible adiabatic path is another route to these endpoints, not the only possible route. Physical check Isentropic endpoints do not establish that the actual process was adiabatic.

Question 10

Equal-entropy endpoints do not determine the heat-transfer history

For a fixed amount of ideal gas with constant molar capacities, use ΔS=nCVln⁡(Tf/Ti)+nRln⁡(Vf/Vi)\Delta S=nC_V\ln(T_f/T_i)+nR\ln(V_f/V_i) and Cp=CV+RC_p=C_V+R, with R=8.314R=8.314 J/(mol K). A .500 mol monatomic gas starts at 300 K. Its final volume is half its initial volume and its final entropy equals its initial entropy.

Diagram shown in the original SVG worksheet.

  1. Find the required final temperature.

  2. Construct a reversible two-leg path: first isothermal compression at 300 K, then fixed-volume heating. Calculate entropy changes on the legs and determine whether zero net entropy change forces zero heat on every leg.

Question 10 - Solution

Equal-entropy endpoints do not determine the heat-transfer history

Diagram shown in the original SVG worksheet.

(a) Method and calculation

0=32nRln⁡(Tf/300)+nRln⁡(1/2).0=\tfrac32nR\ln(T_f/300)+nR\ln(1/2).Tf=30022/3≈476.220K.T_f=300\,2^{2/3}\approx476.220\,\mathrm K.

(b) Interpretation and further calculation

ΔS1=−nRln⁡2,ΔS2=32nRln⁡(22/3)=nRln⁡2.\Delta S_1=-nR\ln2,\quad\Delta S_2=\tfrac32nR\ln(2^{2/3})=nR\ln2.Q1=−nR(300)ln⁡2,Q2=32nR(Tf−300)>0.Q_1=-nR(300)\ln2,\quad Q_2=\tfrac32nR(T_f-300)>0.Each leg transfers heat although the endpoint entropy difference is zero. A reversible adiabatic path is another route to these endpoints, not the only possible route.

Physical check

Isentropic endpoints do not establish that the actual process was adiabatic.