Entropy in the Real World: Engines — Question 6

Section 20-4 · Physics pages 3302–3303

Question 6 A cooling finite source cannot maintain its initial Carnot efficiency A finite body of constant heat capacity C = 1000 J/K starts at 600 K. A succession of reversible cyclic engines extracts work while cooling it to a fixed 300 K environment. At instantaneous source temperature T, the engine absorbs dQh = −C dT and has efficiency 1 −300/T. T 1 −T0/T Axes and labels specify the model; the sketch is schematic. (a) Integrate to find maximum work and total rejected heat. (b) Find overall work divided by total source heat loss. Compare with the estimate obtained by applying the initial efficiency to all heat.
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Question 6 - Solution A cooling finite source cannot maintain its initial Carnot efficiency T 1 −T0/T (a) Method and calculation Wmax = C ∫600 300 ( 1 −300 T ) dT = C[300 −300 ln 2] ≈92055.8 J. Qh = C(600 −300) = 300000 J, Qc = C(300) ln 2 ≈207944 J. (b) Interpretation and further calculation ηoverall = Wmax/Qh = 1 −ln 2 ≈.306853. Winitial efficiency = .500(300000) = 150000 J > Wmax. The source temperature falls continuously, reducing the available work per joule of heat. Physical check The available-work integral vanishes as the source approaches the environmental temperature.

Question 6

A cooling finite source cannot maintain its initial Carnot efficiency

A finite body of constant heat capacity C=1000C=1000 J/K starts at 600 K. A succession of reversible cyclic engines extracts work while cooling it to a fixed 300 K environment. At instantaneous source temperature TT, the engine absorbs dQh=−CdTdQ_h=-C\,dT and has efficiency 1−300/T1-300/T.

Diagram shown in the original SVG worksheet.

  1. Integrate to find maximum work and total rejected heat.

  2. Find overall work divided by total source heat loss. Compare with the estimate obtained by applying the initial efficiency to all heat.

Question 6 - Solution

A cooling finite source cannot maintain its initial Carnot efficiency

Diagram shown in the original SVG worksheet.

(a) Method and calculation

Wmax=C∫300600(1−300T)dT=C[300−300ln⁡2]≈92055.8J.W_{\max}=C\int_{300}^{600}\left(1-\frac{300}{T}\right)dT=C[300-300\ln2]\approx92055.8\,\mathrm J.Qh=C(600−300)=300000J,Qc=C(300)ln⁡2≈207944J.Q_h=C(600-300)=300000\,\mathrm J,\quad Q_c=C(300)\ln2\approx207944\,\mathrm J.

(b) Interpretation and further calculation

ηoverall=Wmax/Qh=1−ln⁡2≈.306853.\eta_{\mathrm{overall}}=W_{\max}/Q_h=1-\ln2\approx.306853.Winitialefficiency=.500(300000)=150000J>Wmax.W_{\mathrm{initial\ efficiency}}=.500(300000)=150000\,\mathrm J>W_{\max}.The source temperature falls continuously, reducing the available work per joule of heat.

Physical check

The available-work integral vanishes as the source approaches the environmental temperature.