The Second Law of Thermodynamics — Question 8

Section 20-3 · Physics pages 3286–3287

Question 8 An irreversible path and a reversible return produce a negative Clausius integral A closed system follows path A to B, absorbing 800 J through a 400 K boundary and rejecting 300 J through a 300 K boundary. Its entropy increases by 1.50 J/K. It returns from B to A reversibly, with whatever changing-temperature heat contacts are needed. A B actual reversible return Schematic; labels, not drawing lengths, specify the data. (a) Find entropy transfer and entropy generation on the outward path. (b) Find R δQrev/T on the return and H δQ/Tb over the cycle. Verify the cyclic inequality.
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Question 8 - Solution An irreversible path and a reversible return produce a negative Clausius integral A B actual reversible return (a) Method and calculation Z B A δQ Tb = 800/400 −300/300 = 1.00 J/K. Sgen,AB = ∆SAB − Z B A δQ/Tb = .500 J/K. (b) Interpretation and further calculation Z A B δQrev T = SA −SB = −1.50 J/K. I δQ Tb = 1.00 −1.50 = −.500 J/K = −Sgen,cycle ≤0. The return removes the system entropy increase but cannot undo the generation from the outward leg. Physical check The closed integral of dS is zero; the closed integral of actual heat divided by boundary temperature need not be.

Question 8

An irreversible path and a reversible return produce a negative Clausius integral

A closed system follows path A to B, absorbing 800 J through a 400 K boundary and rejecting 300 J through a 300 K boundary. Its entropy increases by 1.50 J/K. It returns from B to A reversibly, with whatever changing-temperature heat contacts are needed.

Diagram shown in the original SVG worksheet.

  1. Find entropy transfer and entropy generation on the outward path.

  2. Find ∫δQrev/T\int\delta Q_{\mathrm{rev}}/T on the return and ∮δQ/Tb\oint\delta Q/T_b over the cycle. Verify the cyclic inequality.

Question 8 - Solution

An irreversible path and a reversible return produce a negative Clausius integral

Diagram shown in the original SVG worksheet.

(a) Method and calculation

∫ABδQTb=800/400−300/300=1.00J/K.\int_A^B\frac{\delta Q}{T_b}=800/400-300/300=1.00\,\mathrm{J/K}.Sgen,AB=ΔSAB−∫ABδQ/Tb=.500J/K.S_{{\mathrm{gen}},AB}=\Delta S_{AB}-\int_A^B\delta Q/T_b=.500\,\mathrm{J/K}.

(b) Interpretation and further calculation

∫BAδQrevT=SA−SB=−1.50J/K.\int_B^A\frac{\delta Q_{\mathrm{rev}}}T=S_A-S_B=-1.50\,\mathrm{J/K}.∮δQTb=1.00−1.50=−.500J/K=−Sgen,cycle≤0.\oint\frac{\delta Q}{T_b}=1.00-1.50=-.500\,\mathrm{J/K}=-S_{\mathrm{gen,cycle}}\le0.The return removes the system entropy increase but cannot undo the generation from the outward leg.

Physical check

The closed integral of dSdS is zero; the closed integral of actual heat divided by boundary temperature need not be.