Change in Entropy — Question 1

Section 20-2 · Physics pages 3252–3253

Question 1 Temperature and volume contributions to gas entropy add independently 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 gas has CV = 5R/2. It changes from (300 K, Vi) to (450 K, 2Vi). V T Vi 2Vi Axes and labels specify the model; the sketch is schematic. (a) Calculate the temperature and volume contributions and their sum. (b) Construct two reversible reference legs that give the same sum, first heating at fixed volume and then expanding isothermally. Find the pressure ratio between the actual endpoints.
Show solutionHide solution
Question 1 - Solution Temperature and volume contributions to gas entropy add independently V T Vi 2Vi (a) Method and calculation ∆ST = .500(5 2)R ln(450/300), ∆SV = .500R ln 2. ∆S = 1 2R[ 5 2 ln(3/2) + ln 2] ≈7.09521 J/K. (b) Interpretation and further calculation ∆S1 = ∫450 300 nCV T dT, ∆S2 = ∫2Vi Vi nR V dV. ∆S1 + ∆S2 = ∆S, pf/pi = (450/300)/2 = .750. The endpoint formula applies even if the actual process is irreversible; the reference legs only evaluate the state-function difference. Physical check Temperature rises while pressure falls here because volume grows by a larger factor.

Question 1

Temperature and volume contributions to gas entropy add independently

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 gas has CV=5R/2C_V=5R/2. It changes from (300K,Vi)(300\,\mathrm K,V_i) to (450K,2Vi)(450\,\mathrm K,2V_i).

Diagram shown in the original SVG worksheet.

  1. Calculate the temperature and volume contributions and their sum.

  2. Construct two reversible reference legs that give the same sum, first heating at fixed volume and then expanding isothermally. Find the pressure ratio between the actual endpoints.

Question 1 - Solution

Temperature and volume contributions to gas entropy add independently

Diagram shown in the original SVG worksheet.

(a) Method and calculation

ΔST=.500(52)Rln⁡(450/300),ΔSV=.500Rln⁡2.\Delta S_T=.500(\tfrac52)R\ln(450/300),\quad\Delta S_V=.500R\ln2.ΔS=12R[52ln⁡(3/2)+ln⁡2]≈7.09521J/K.\Delta S=\tfrac12R[\tfrac52\ln(3/2)+\ln2]\approx7.09521\,\mathrm{J/K}.

(b) Interpretation and further calculation

ΔS1=∫300450nCVTdT,ΔS2=∫Vi2VinRVdV.\Delta S_1=\int_{300}^{450}\frac{nC_V}{T}dT,\quad\Delta S_2=\int_{V_i}^{2V_i}\frac{nR}{V}dV.ΔS1+ΔS2=ΔS,pf/pi=(450/300)/2=.750.\Delta S_1+\Delta S_2=\Delta S,\quad p_f/p_i=(450/300)/2=.750.The endpoint formula applies even if the actual process is irreversible; the reference legs only evaluate the state-function difference.

Physical check

Temperature rises while pressure falls here because volume grows by a larger factor.