The Second Law of Thermodynamics — Question 6

Section 20-3 · Physics pages 3282–3283

Question 6 The second law bounds cooling in an adiabatic gas expansion One mole of monatomic ideal gas starts at 300 K and expands adiabatically to twice its initial volume. It exchanges work but no matter or heat. Use ∆S = 3 2R ln(Tf/300) + R ln 2 and U = 3RT/2, with R = 8.314 J/(mol K). V p Axes and labels specify the model; the sketch is schematic. (a) Find the lowest allowed final temperature and corresponding maximum work done by the gas. (b) Test a proposed final temperature of 100 K. Explain when equality in the temperature bound can be achieved.
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Question 6 - Solution The second law bounds cooling in an adiabatic gas expansion V p (a) Method and calculation ∆S = Sgen ≥0 ⇒ln(Tf/300) ≥−2 3 ln 2. Tf ≥300 2−2/3 ≈188.988 K, Wmax = 3 2R(300 −188.988) ≈1384.43 J. (b) Interpretation and further calculation ∆S(100) = R[ 3 2 ln(1/3) + ln 2] < 0. Tf = Tmin ⇔Sgen = 0. The proposed 100 K endpoint is impossible under the stated exchanges; the limiting endpoint belongs to a reversible adiabatic expansion. Physical check At fixed final volume, irreversibility leaves more energy in the gas and reduces extracted work.

Question 6

The second law bounds cooling in an adiabatic gas expansion

One mole of monatomic ideal gas starts at 300 K and expands adiabatically to twice its initial volume. It exchanges work but no matter or heat. Use ΔS=32Rln⁡(Tf/300)+Rln⁡2\Delta S=\tfrac32R\ln(T_f/300)+R\ln2 and U=3RT/2U=3RT/2, with R=8.314R=8.314 J/(mol K).

Diagram shown in the original SVG worksheet.

  1. Find the lowest allowed final temperature and corresponding maximum work done by the gas.

  2. Test a proposed final temperature of 100 K. Explain when equality in the temperature bound can be achieved.

Question 6 - Solution

The second law bounds cooling in an adiabatic gas expansion

Diagram shown in the original SVG worksheet.

(a) Method and calculation

ΔS=Sgen≥0⇒ln⁡(Tf/300)≥−23ln⁡2.\Delta S=S_{\mathrm{gen}}\ge0\ \Rightarrow\ln(T_f/300)\ge-\tfrac23\ln2.Tf≥3002−2/3≈188.988K,Wmax=32R(300−188.988)≈1384.43J.T_f\ge300\,2^{-2/3}\approx188.988\,\mathrm K,\quad W_{\max}=\tfrac32R(300-188.988)\approx1384.43\,\mathrm J.

(b) Interpretation and further calculation

ΔS(100)=R[32ln⁡(1/3)+ln⁡2]<0.\Delta S(100)=R[\tfrac32\ln(1/3)+\ln2]<0.Tf=Tmin⇔Sgen=0.T_f=T_{\min}\ \Leftrightarrow\ S_{\mathrm{gen}}=0.The proposed 100 K endpoint is impossible under the stated exchanges; the limiting endpoint belongs to a reversible adiabatic expansion.

Physical check

At fixed final volume, irreversibility leaves more energy in the gas and reduces extracted work.