Entropy in the Real World: Refrigerators — Question 9

Section 20-5 · Physics pages 3328–3329

Question 9 A reversible engine can power cooling without external electrical work A reversible engine operates between 600 K and 300 K. All its work drives a reversible refrigerator lifting heat from 250 K to 300 K. The engine receives 1000 J per cycle; the devices are scaled to exchange equal work. engine refrigerator WE = WR 600 K input 250 K cooling common 300 K sink Schematic; labels, not drawing lengths, specify the data. (a) Find engine work, refrigerator cooling, and total heat delivered to the 300 K reservoir. (b) Check the composite energy and entropy balances. Explain why cooling can exceed the high-temperature heat input without violating either law.
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Question 9 - Solution A reversible engine can power cooling without external electrical work engine refrigerator WE = WR 600 K input 250 K cooling common 300 K sink (a) Method and calculation ηE = 1 −300/600 = .500 ⇒WE = 500 J. KR = 250/(300 −250) = 5 ⇒Qc,R = 2500 J. Q300 = (1000 −500) + (2500 + 500) = 3500 J. (b) Interpretation and further calculation Q300 = Q600 + Q250 = 1000 + 2500, Wexternal = 0. ∆Sreservoirs = 3500/300 −1000/600 −2500/250 = 0. The cooling heat comes from the 250 K reservoir, while high-temperature heat supplies the ability to drive that transfer. Physical check Internal work cancels only after both complete device balances are included.

Question 9

A reversible engine can power cooling without external electrical work

A reversible engine operates between 600 K and 300 K. All its work drives a reversible refrigerator lifting heat from 250 K to 300 K. The engine receives 1000 J per cycle; the devices are scaled to exchange equal work.

Diagram shown in the original SVG worksheet.

  1. Find engine work, refrigerator cooling, and total heat delivered to the 300 K reservoir.

  2. Check the composite energy and entropy balances. Explain why cooling can exceed the high-temperature heat input without violating either law.

Question 9 - Solution

A reversible engine can power cooling without external electrical work

Diagram shown in the original SVG worksheet.

(a) Method and calculation

ηE=1−300/600=.500⇒WE=500J.\eta_E=1-300/600=.500\ \Rightarrow\ W_E=500\,\mathrm J.KR=250/(300−250)=5⇒Qc,R=2500J.K_R=250/(300-250)=5\ \Rightarrow\ Q_{c,R}=2500\,\mathrm J.Q300=(1000−500)+(2500+500)=3500J.Q_{300}=(1000-500)+(2500+500)=3500\,\mathrm J.

(b) Interpretation and further calculation

Q300=Q600+Q250=1000+2500,Wexternal=0.Q_{300}=Q_{600}+Q_{250}=1000+2500,\quad W_{\mathrm{external}}=0.ΔSreservoirs=3500/300−1000/600−2500/250=0.\Delta S_{\mathrm{reservoirs}}=3500/300-1000/600-2500/250=0.The cooling heat comes from the 250 K reservoir, while high-temperature heat supplies the ability to drive that transfer.

Physical check

Internal work cancels only after both complete device balances are included.