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For an ideal gas with constant properties undergoing a quasi-static process, which one of the following represents the change of entropy (Δs) from state 1 to 2?

  • A.\(\Delta s = C_p\ln(\frac{T_2}{T_1}) - R\ln(\frac{P_2}{P_1})\)
  • B.\(\Delta s = C_V\ln(\frac{T_2}{T_1}) - C_p\ln(\frac{V_2}{V_1})\)
  • C.\(\Delta s = C_P\ln(\frac{T_2}{T_1}) - C_V\ln(\frac{P_2}{P_1})\)
  • D.\(\Delta s = C_V\ln(\frac{T_2}{T_1}) + R\ln(\frac{V_1}{V_2})\)

Answer: A

The correct expression is \(\Delta s = C_{p}\ln\frac{T_{2}}{T_{1}} - R\ln\frac{P_{2}}{P_{1}}\).

From the Gibbs relation \(T\,ds = dh - v\,dP\), with \(dh = C_{p}\,dT\) and \(v = RT/P\) for an ideal gas:

\[ \begin{aligned} ds &= C_{p}\frac{dT}{T} - R\frac{dP}{P} \\ \Delta s &= C_{p}\ln\frac{T_{2}}{T_{1}} - R\ln\frac{P_{2}}{P_{1}} \end{aligned} \]

The volume form is \(\Delta s = C_{V}\ln\frac{T_{2}}{T_{1}} + R\ln\frac{V_{2}}{V_{1}}\). Option D has \(R\ln(V_{1}/V_{2})\), which reverses the sign of the volume term. Options B and C put a heat capacity where R belongs.

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