Irreversible Processes and Entropy — Question 6

Section 20-1 · Physics pages 3242–3243

Question 6 Smaller temperature steps reduce entropy generation during heating A body of constant heat capacity C = 100 J/K starts at 300 K and finishes at 600 K. Compare direct contact with a 600 K reservoir to two stages: first equilibration with a 450 K reservoir, then with a 600 K reservoir. Neglect work and all other heat capacities. 300 K 450 K 600 K Successive body temperatures in the two-stage protocol. (a) Find the body entropy change and total entropy generation for direct heating. (b) Find entropy generation for the two-stage protocol and its reduction. Explain the limit of infinitely many reservoirs with infinitesimal temperature differences.
Show solutionHide solution
Question 6 - Solution Smaller temperature steps reduce entropy generation during heating 300 K 450 K 600 K (a) Method and calculation ∆Sb = C ln 2 = 69.3147 J/K, Q = 30000 J. Sgen,direct = C ln 2 −30000/600 = 100 ln 2 −50 ≈19.3147 J/K. (b) Interpretation and further calculation Sgen,two = 100 ln 2 −15000 450 −15000 600 ≈10.9814 J/K. reduction = 8.33333 J/K, lim Sgen = C ln 2 − ∫600 300 C dT T = 0. The body entropy change is unchanged; reservoir entropy loss approaches its magnitude as heat transfer becomes reversible. Physical check A reversible limit removes entropy generation, not the entropy change of the heated body.

Question 6

Smaller temperature steps reduce entropy generation during heating

A body of constant heat capacity C=100C=100 J/K starts at 300 K and finishes at 600 K. Compare direct contact with a 600 K reservoir to two stages: first equilibration with a 450 K reservoir, then with a 600 K reservoir. Neglect work and all other heat capacities.

Diagram shown in the original SVG worksheet.

  1. Find the body entropy change and total entropy generation for direct heating.

  2. Find entropy generation for the two-stage protocol and its reduction. Explain the limit of infinitely many reservoirs with infinitesimal temperature differences.

Question 6 - Solution

Smaller temperature steps reduce entropy generation during heating

Diagram shown in the original SVG worksheet.

(a) Method and calculation

ΔSb=Cln⁡2=69.3147J/K,Q=30000J.\Delta S_b=C\ln2=69.3147\,\mathrm{J/K},\quad Q=30000\,\mathrm J.Sgen,direct=Cln⁡2−30000/600=100ln⁡2−50≈19.3147J/K.S_{\mathrm{gen,direct}}=C\ln2-30000/600=100\ln2-50\approx19.3147\,\mathrm{J/K}.

(b) Interpretation and further calculation

Sgen,two=100ln⁡2−15000450−15000600≈10.9814J/K.S_{\mathrm{gen,two}}=100\ln2-\frac{15000}{450}-\frac{15000}{600}\approx10.9814\,\mathrm{J/K}.reduction=8.33333J/K,lim⁡Sgen=Cln⁡2−∫300600CdTT=0.\text{reduction}=8.33333\,\mathrm{J/K},\quad\lim S_{\mathrm{gen}}=C\ln2-\int_{300}^{600}\frac{C\,dT}{T}=0.The body entropy change is unchanged; reservoir entropy loss approaches its magnitude as heat transfer becomes reversible.

Physical check

A reversible limit removes entropy generation, not the entropy change of the heated body.