Entropy in the Real World: Refrigerators — Question 8

Section 20-5 · Physics pages 3326–3327

Question 8 Lowering a cold setpoint increases both the heat leak and work per joule A refrigerated enclosure has heat leak ˙Qc = G(Th −Tc), with G = 2.00 W/K and Th = 300 K. Its actual coefficient is one-half the reversible value: KR = .500Tc/(Th −Tc). Ignore all other loads. Tc heat leak 300 K Schematic; labels, not drawing lengths, specify the data. (a) Find cooling load and input power at Tc = 270 K. (b) Repeat at 260 K and derive the input-power dependence on Tc. Explain the more-than-linear increase in required power.
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Question 8 - Solution Lowering a cold setpoint increases both the heat leak and work per joule Tc heat leak 300 K (a) Method and calculation ˙Qc = 2(30) = 60.0 W, KR = .500(270/30) = 4.50. ˙W = 60/4.50 = 13.3333 W. (b) Interpretation and further calculation ˙Qc(260) = 80.0 W, KR(260) = 3.25, ˙W(260) ≈24.6154 W. ˙W = G(Th −Tc)2 .500Tc . A larger temperature difference admits more heat and simultaneously raises the work cost of removing each joule. Physical check The coefficient model is stipulated for these two operating points; it is not a universal real-device law.

Question 8

Lowering a cold setpoint increases both the heat leak and work per joule

A refrigerated enclosure has heat leak Q̇c=G(Th−Tc)\dot Q_c=G(T_h-T_c), with G=2.00G=2.00 W/K and Th=300T_h=300 K. Its actual coefficient is one-half the reversible value: KR=.500Tc/(Th−Tc)K_R=.500T_c/(T_h-T_c). Ignore all other loads.

Diagram shown in the original SVG worksheet.

  1. Find cooling load and input power at Tc=270T_c=270 K.

  2. Repeat at 260 K and derive the input-power dependence on TcT_c. Explain the more-than-linear increase in required power.

Question 8 - Solution

Lowering a cold setpoint increases both the heat leak and work per joule

Diagram shown in the original SVG worksheet.

(a) Method and calculation

Q̇c=2(30)=60.0W,KR=.500(270/30)=4.50.\dot Q_c=2(30)=60.0\,\mathrm W,\quad K_R=.500(270/30)=4.50.Ẇ=60/4.50=13.3333W.\dot W=60/4.50=13.3333\,\mathrm W.

(b) Interpretation and further calculation

Q̇c(260)=80.0W,KR(260)=3.25,Ẇ(260)≈24.6154W.\dot Q_c(260)=80.0\,\mathrm W,\quad K_R(260)=3.25,\quad\dot W(260)\approx24.6154\,\mathrm W.Ẇ=G(Th−Tc)2.500Tc.\dot W=\frac{G(T_h-T_c)^2}{.500T_c}.A larger temperature difference admits more heat and simultaneously raises the work cost of removing each joule.

Physical check

The coefficient model is stipulated for these two operating points; it is not a universal real-device law.