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The equation of state for a non-ideal gas is

\[ \frac{Pv}{RT} = 1 + BP \]

where \(P\) is pressure, \(v\) is specific volume, \(R\) is the specific gas constant, \(T\) is temperature, and \(B\) is a temperature dependent parameter. For this gas, the partial derivative of enthalpy with respect to pressure at constant temperature is

  • A.\(BRT\)
  • B.\(-RT^{2}\left(\frac{dB}{dT}\right)\)
  • C.\(BRT - RT^{2}\left(\frac{dB}{dT}\right)\)
  • D.0

Answer: B

The derivative is \(-RT^{2}\left(\frac{dB}{dT}\right)\).

The general relation is \((\partial h/\partial P)_T = v - T(\partial v/\partial T)_P\). From the equation of state, \(v = RT/P + BRT\), so

\[ \begin{aligned} \left(\frac{\partial v}{\partial T}\right)_P &= \frac{R}{P} + BR + RT\frac{dB}{dT} \\ v - T\left(\frac{\partial v}{\partial T}\right)_P &= -RT^{2}\frac{dB}{dT} \end{aligned} \]

The ideal-gas part \(RT/P\) and the \(BRT\) term both cancel. BRT is what remains if B is treated as constant in only one of the two terms, and 0 is the ideal-gas result, which holds here only if B does not depend on T.

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