Daniel D'Orazio edited untitled.tex  over 9 years ago

Commit id: b496f9f47f9279bef52d4e9bc030593a4be55838

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so that  \begin{align}  dQ &= R\left( 1 + \frac{1}{\gamma-1}\right)dT - \frac{d \rho}{\rho} \\  &= \frac{\gamma R}{\gamma-1}dT - \frac{d \rho}{\rho} P}{\rho}  \end{align}  Let's also introduce the enthalpy $h$ in the limit that the number of particles in the system is constant,