Change in Entropy — Question 7

Section 20-2 · Physics pages 3264–3265

Question 7 Unequal thermal capacities require an energy-weighted final temperature Two insulated-together bodies have constant heat capacities CA = 100 J/K and CB = 300 J/K. Initial temperatures are 600 K and 300 K. They do no work and finally equilibrate. 100 J/K 300 J/K Q The arrow defines positive heat transfer from left to right. (a) Find final temperature from energy conservation and total entropy generation. (b) Calculate the entropy changes separately and show why averaging the initial temperatures without heat-capacity weights gives an inconsistent energy balance.
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Question 7 - Solution Unequal thermal capacities require an energy-weighted final temperature 100 J/K 300 J/K Q (a) Method and calculation Tf = CATA + CBTB CA + CB = 100(600) + 300(300) 400 = 375 K. Sgen = 100 ln(375/600) + 300 ln(375/300) ≈19.9427 J/K. (b) Interpretation and further calculation ∆SA = 100 ln(5/8) ≈−47.0004 J/K, ∆SB = 300 ln(5/4) ≈66.9431 J/K. ∆Uif Tf = 450 = 100(450 −600) + 300(450 −300) = 30000 J̸ = 0. The unweighted temperature would require an unprovided energy input. Physical check The equilibrium temperature lies closer to the initial temperature of the body with greater heat capacity.

Question 7

Unequal thermal capacities require an energy-weighted final temperature

Two insulated-together bodies have constant heat capacities CA=100C_A=100 J/K and CB=300C_B=300 J/K. Initial temperatures are 600 K and 300 K. They do no work and finally equilibrate.

Diagram shown in the original SVG worksheet.

  1. Find final temperature from energy conservation and total entropy generation.

  2. Calculate the entropy changes separately and show why averaging the initial temperatures without heat-capacity weights gives an inconsistent energy balance.

Question 7 - Solution

Unequal thermal capacities require an energy-weighted final temperature

Diagram shown in the original SVG worksheet.

(a) Method and calculation

Tf=CATA+CBTBCA+CB=100(600)+300(300)400=375K.T_f=\frac{C_AT_A+C_BT_B}{C_A+C_B}=\frac{100(600)+300(300)}{400}=375\,\mathrm K.Sgen=100ln⁡(375/600)+300ln⁡(375/300)≈19.9427J/K.S_{\mathrm{gen}}=100\ln(375/600)+300\ln(375/300)\approx19.9427\,\mathrm{J/K}.

(b) Interpretation and further calculation

ΔSA=100ln⁡(5/8)≈−47.0004J/K,ΔSB=300ln⁡(5/4)≈66.9431J/K.\Delta S_A=100\ln(5/8)\approx-47.0004\,\mathrm{J/K},\quad\Delta S_B=300\ln(5/4)\approx66.9431\,\mathrm{J/K}.ΔUifTf=450=100(450−600)+300(450−300)=30000J≠0.\Delta U_{\mathrm{if\ }}T_f=450=100(450-600)+300(450-300)=30000\,\mathrm J\ne0.The unweighted temperature would require an unprovided energy input.

Physical check

The equilibrium temperature lies closer to the initial temperature of the body with greater heat capacity.