Entropy in the Real World: Engines — Question 10

Section 20-4 · Physics pages 3310–3311

Question 10 A required engine output sets the share of heat needed from a hotter source A cyclic engine receives total heat 1000 J per cycle: fraction x from 600 K and fraction 1 −x from 400 K. It rejects heat only to 300 K. The desired output is 350 J per cycle. x W solid: reversible work limit Axes and labels specify the model; the sketch is schematic. (a) Find the minimum x compatible with reversible operation. (b) If total entropy generation is .200 J/K per cycle, find the required x and rejected heat. State whether the result lies in the physical fraction range.
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Question 10 - Solution A required engine output sets the share of heat needed from a hotter source x W solid: reversible work limit (a) Method and calculation Qc,min = 300 (1000x 600 + 1000(1 −x) 400 ) = 750 −250x. Wmax = 1000 −Qc,min = 250 + 250x ⇒x ≥.400. (b) Interpretation and further calculation Qc = 750 −250x + 300(.200), W = 190 + 250x. 350 = 190 + 250x ⇒x = .640, Qc = 650 J. The fraction is admissible, 0 ≤x ≤1. Irreversibility requires a greater contribution from the hotter source for the same work output. Physical check The required high-temperature heat share is a design constraint derived jointly from energy and entropy.

Question 10

A required engine output sets the share of heat needed from a hotter source

A cyclic engine receives total heat 1000 J per cycle: fraction xx from 600 K and fraction 1−x1-x from 400 K. It rejects heat only to 300 K. The desired output is 350 J per cycle.

Diagram shown in the original SVG worksheet.

  1. Find the minimum xx compatible with reversible operation.

  2. If total entropy generation is .200 J/K per cycle, find the required xx and rejected heat. State whether the result lies in the physical fraction range.

Question 10 - Solution

A required engine output sets the share of heat needed from a hotter source

Diagram shown in the original SVG worksheet.

(a) Method and calculation

Qc,min=300(1000x600+1000(1−x)400)=750−250x.Q_{c,\min}=300\left(\frac{1000x}{600}+\frac{1000(1-x)}{400}\right)=750-250x.Wmax=1000−Qc,min=250+250x⇒x≥.400.W_{\max}=1000-Q_{c,\min}=250+250x\ \Rightarrow\ x\ge.400.

(b) Interpretation and further calculation

Qc=750−250x+300(.200),W=190+250x.Q_c=750-250x+300(.200),\quad W=190+250x.350=190+250x⇒x=.640,Qc=650J.350=190+250x\ \Rightarrow\ x=.640,\quad Q_c=650\,\mathrm J.The fraction is admissible, 0≤x≤10\le x\le1. Irreversibility requires a greater contribution from the hotter source for the same work output.

Physical check

The required high-temperature heat share is a design constraint derived jointly from energy and entropy.