Change in Entropy — Question 2

Section 20-2 · Physics pages 3254–3255

Question 2 Pressure-temperature data give an equivalent entropy formula 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). One mole has CV = 5R/2. Its temperature doubles while its pressure quadruples. T p Axes and labels specify the model; the sketch is schematic. (a) Eliminate the volume ratio and derive ∆S = nCp ln(Tf/Ti) −nR ln(pf/pi). Evaluate it. (b) For a temperature doubling, find the pressure ratio giving zero entropy change. Can pressure increase while entropy also increases?
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Question 2 - Solution Pressure-temperature data give an equivalent entropy formula T p (a) Method and calculation Vf/Vi = (Tf/Ti)/(pf/pi). ∆S = n(CV + R) ln(Tf/Ti) −nR ln(pf/pi) = R[ 7 2 ln 2 −ln 4] ≈8.64424 J/K. (b) Interpretation and further calculation ∆S = 0 ⇒pf/pi = (Tf/Ti)Cp/R = 27/2 ≈11.3137. 1 < pf/pi < 27/2 ⇒∆S > 0 (Tf/Ti = 2). Compression and heating contribute oppositely; pressure increase alone cannot determine the entropy sign. Physical check The use of Cp follows algebraically from the ideal equation of state; it does not imply a constant-pressure process.

Question 2

Pressure-temperature data give an equivalent entropy formula

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). One mole has CV=5R/2C_V=5R/2. Its temperature doubles while its pressure quadruples.

Diagram shown in the original SVG worksheet.

  1. Eliminate the volume ratio and derive ΔS=nCpln⁡(Tf/Ti)−nRln⁡(pf/pi)\Delta S=nC_p\ln(T_f/T_i)-nR\ln(p_f/p_i). Evaluate it.

  2. For a temperature doubling, find the pressure ratio giving zero entropy change. Can pressure increase while entropy also increases?

Question 2 - Solution

Pressure-temperature data give an equivalent entropy formula

Diagram shown in the original SVG worksheet.

(a) Method and calculation

Vf/Vi=(Tf/Ti)/(pf/pi).V_f/V_i=(T_f/T_i)/(p_f/p_i).ΔS=n(CV+R)ln⁡(Tf/Ti)−nRln⁡(pf/pi)=R[72ln⁡2−ln⁡4]≈8.64424J/K.\Delta S=n(C_V+R)\ln(T_f/T_i)-nR\ln(p_f/p_i)=R[\tfrac72\ln2-\ln4]\approx8.64424\,\mathrm{J/K}.

(b) Interpretation and further calculation

ΔS=0⇒pf/pi=(Tf/Ti)Cp/R=27/2≈11.3137.\Delta S=0\ \Rightarrow\ p_f/p_i=(T_f/T_i)^{C_p/R}=2^{7/2}\approx11.3137.1<pf/pi<27/2⇒ΔS>0(Tf/Ti=2).1<p_f/p_i<2^{7/2}\ \Rightarrow\Delta S>0\quad(T_f/T_i=2).Compression and heating contribute oppositely; pressure increase alone cannot determine the entropy sign.

Physical check

The use of CpC_p follows algebraically from the ideal equation of state; it does not imply a constant-pressure process.