The Second Law of Thermodynamics — Question 4

Section 20-3 · Physics pages 3278–3279

Question 4 The cyclic condition distinguishes a forbidden engine from a work store A proposed cyclic machine absorbs 500 J from a single 300 K reservoir and converts all of it to work, with no other effect. Compare this with an ideal descending weight delivering 500 J of mechanical work while its gravitational energy decreases by 500 J. weight descent Schematic; labels, not drawing lengths, specify the data. (a) Calculate the entropy change of the machine–reservoir composite for the cyclic claim. (b) Write energy and entropy balances for the ideal weight. Explain why its work delivery does not contradict the prohibition on a single-reservoir cyclic heat engine.
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Question 4 - Solution The cyclic condition distinguishes a forbidden engine from a work store weight descent (a) Method and calculation ∆Smachine = 0, ∆Sr = −500/300 = −5/3 J/K. ∆Scomposite < 0 ⇒the cyclic claim is impossible. (b) Interpretation and further calculation Qweight = 0, Wweight = 500 J, ∆Egrav = −500 J. ∆Sideal work store = 0. The weight does not return to its starting height. It consumes stored mechanical energy rather than cyclically converting heat from one reservoir into work. Physical check The phrase “with no other effect is essential to the single-reservoir statement.

Question 4

The cyclic condition distinguishes a forbidden engine from a work store

A proposed cyclic machine absorbs 500 J from a single 300 K reservoir and converts all of it to work, with no other effect. Compare this with an ideal descending weight delivering 500 J of mechanical work while its gravitational energy decreases by 500 J.

Diagram shown in the original SVG worksheet.

  1. Calculate the entropy change of the machine–reservoir composite for the cyclic claim.

  2. Write energy and entropy balances for the ideal weight. Explain why its work delivery does not contradict the prohibition on a single-reservoir cyclic heat engine.

Question 4 - Solution

The cyclic condition distinguishes a forbidden engine from a work store

Diagram shown in the original SVG worksheet.

(a) Method and calculation

ΔSmachine=0,ΔSr=−500/300=−5/3J/K.\Delta S_{\mathrm{machine}}=0,\quad\Delta S_r=-500/300=-5/3\,\mathrm{J/K}.ΔScomposite<0⇒the cyclic claim is impossible.\Delta S_{\mathrm{composite}}<0\ \Rightarrow\text{the cyclic claim is impossible}.

(b) Interpretation and further calculation

Qweight=0,Wweight=500J,ΔEgrav=−500J.Q_{\mathrm{weight}}=0,\quad W_{\mathrm{weight}}=500\,\mathrm J,\quad\Delta E_{\mathrm{grav}}=-500\,\mathrm J.ΔSidealworkstore=0.\Delta S_{\mathrm{ideal\ work\ store}}=0.The weight does not return to its starting height. It consumes stored mechanical energy rather than cyclically converting heat from one reservoir into work.

Physical check

The phrase “with no other effect is essential to the single-reservoir statement.