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

Commit id: bf4f9c59de762ae8cb6ddd54d6916420eb22b3ed

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For an ideal gas  \begin{align}  d\epsilon &= \frac{R}{\gamma -1}dT \\  PdV &= -\left(\gamma -1\right)\epsilon \frac{d \rho}{\rho} = RT -RT\frac{d \rho}{\rho}  \end{align}  Then  \begin{equation} 

\end{equation}  so that  \begin{align}  dQ &= R\left( 1 + \frac{1}{\gamma-1}\right)dT - \frac{d \rho}{\rho} P}{\rho}  \\ &= \frac{\gamma R}{\gamma-1}dT - \frac{d P}{\rho}  \end{align}