The Efficiencies of Real Engines — Question 2

Section 20-6 · Physics pages 3334–3335

Question 2 A heat leak lowers efficiency even when the working engine is reversible A source at 800 K supplies 1000 J per cycle to an installation rejecting heat to 400 K. Of the source heat, 200 J bypasses the engine and leaks directly to the cold reservoir. The remaining 800 J enters an internally reversible engine between the two reservoirs. 800 K engine 400 K 200 J leak W Schematic; labels, not drawing lengths, specify the data. (a) Find engine work, total rejected heat and installation efficiency. (b) Calculate total entropy generation and compare the work with the reversible limit for all 1000 J passing through the engine.
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Question 2 - Solution A heat leak lowers efficiency even when the working engine is reversible 800 K engine 400 K 200 J leak W (a) Method and calculation W = (1000 −200)(1 −400/800) = 400 J. Qc,total = 400 + 200 = 600 J, ηinstallation = 400/1000 = .400. (b) Interpretation and further calculation Sgen = 600/400 −1000/800 = .250 J/K. Wno leak = 500 J, ∆W = 100 J = 400Sgen. All entropy generation comes from bypass heat transfer; the internally reversible core does not make the installation reversible. Physical check Use total source heat in the installation efficiency denominator.

Question 2

A heat leak lowers efficiency even when the working engine is reversible

A source at 800 K supplies 1000 J per cycle to an installation rejecting heat to 400 K. Of the source heat, 200 J bypasses the engine and leaks directly to the cold reservoir. The remaining 800 J enters an internally reversible engine between the two reservoirs.

Diagram shown in the original SVG worksheet.

  1. Find engine work, total rejected heat and installation efficiency.

  2. Calculate total entropy generation and compare the work with the reversible limit for all 1000 J passing through the engine.

Question 2 - Solution

A heat leak lowers efficiency even when the working engine is reversible

Diagram shown in the original SVG worksheet.

(a) Method and calculation

W=(1000−200)(1−400/800)=400J.W=(1000-200)(1-400/800)=400\,\mathrm J.Qc,total=400+200=600J,ηinstallation=400/1000=.400.Q_{c,\mathrm{total}}=400+200=600\,\mathrm J,\quad\eta_{\mathrm{installation}}=400/1000=.400.

(b) Interpretation and further calculation

Sgen=600/400−1000/800=.250J/K.S_{\mathrm{gen}}=600/400-1000/800=.250\,\mathrm{J/K}.Wnoleak=500J,ΔW=100J=400Sgen.W_{\mathrm{no\ leak}}=500\,\mathrm J,\quad\Delta W=100\,\mathrm J=400S_{\mathrm{gen}}.All entropy generation comes from bypass heat transfer; the internally reversible core does not make the installation reversible.

Physical check

Use total source heat in the installation efficiency denominator.