Entropy in the Real World: Engines — Question 7

Section 20-4 · Physics pages 3304–3305

Question 7 A finite cold body warms as a reversible engine rejects heat to it A reversible cyclic engine receives heat from a 600 K reservoir and rejects it to a finite body of constant heat capacity 500 J/K. The body warms from 300 K to 400 K. Assume heat is transferred reversibly at the instantaneous body temperature. 600 K engine Tbody Qh Qc W Heat and work labels denote positive magnitudes in the arrow directions. (a) Find total rejected heat and the cold-body entropy increase. (b) Use entropy balance to find total hot heat input and work. Compare the overall efficiency with the efficiencies at the beginning and end.
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Question 7 - Solution A finite cold body warms as a reversible engine rejects heat to it 600 K engine Tbody Qh Qc W (a) Method and calculation Qc = C(400 −300) = 50000 J. ∆Sc = C ln(400/300) = 500 ln(4/3) ≈143.841 J/K. (b) Interpretation and further calculation Qh/600 = ∆Sc ⇒Qh ≈86304.6 J, W = Qh −Qc ≈36304.6 J. ηoverall = 1 − 100 600 ln(4/3) ≈.420657. ηstart = .500, ηend = 1/3. The overall efficiency falls between its instantaneous endpoint values. Physical check Total rejected heat divided by the final sink temperature would underestimate the sink entropy increase.

Question 7

A finite cold body warms as a reversible engine rejects heat to it

A reversible cyclic engine receives heat from a 600 K reservoir and rejects it to a finite body of constant heat capacity 500 J/K. The body warms from 300 K to 400 K. Assume heat is transferred reversibly at the instantaneous body temperature.

Diagram shown in the original SVG worksheet.

  1. Find total rejected heat and the cold-body entropy increase.

  2. Use entropy balance to find total hot heat input and work. Compare the overall efficiency with the efficiencies at the beginning and end.

Question 7 - Solution

A finite cold body warms as a reversible engine rejects heat to it

Diagram shown in the original SVG worksheet.

(a) Method and calculation

Qc=C(400−300)=50000J.Q_c=C(400-300)=50000\,\mathrm J.ΔSc=Cln⁡(400/300)=500ln⁡(4/3)≈143.841J/K.\Delta S_c=C\ln(400/300)=500\ln(4/3)\approx143.841\,\mathrm{J/K}.

(b) Interpretation and further calculation

Qh/600=ΔSc⇒Qh≈86304.6J,W=Qh−Qc≈36304.6J.Q_h/600=\Delta S_c\ \Rightarrow\ Q_h\approx86304.6\,\mathrm J,\quad W=Q_h-Q_c\approx36304.6\,\mathrm J.ηoverall=1−100600ln⁡(4/3)≈.420657.\eta_{\mathrm{overall}}=1-\frac{100}{600\ln(4/3)}\approx.420657.ηstart=.500,ηend=1/3.\eta_{\mathrm{start}}=.500,\quad\eta_{\mathrm{end}}=1/3.The overall efficiency falls between its instantaneous endpoint values.

Physical check

Total rejected heat divided by the final sink temperature would underestimate the sink entropy increase.