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| Heat capacity | Work |
|---|---|
| $c_p=\left(\frac{\partial H}{\partial T}\right)_p$ | $dW=-pdV$ |
| $c_V=\left(\frac{\partial U}{\partial T}\right)_V$ |
Laws of thermodynamics
| 1st | $dU=dQ+dW$ |
|---|---|
| 2nd | $ dS= \frac{dQ}{T} $ |
| 3rd | $\lim_{T \to 0}=0$ |
Simplified definitions of energies
| $dU=dQ+dW$ | |
| $ dH= dU+d(pV) $ | |
| $dF=dU-d(TS)$ | |
| $dG=dH-d(TS)$ | |
| $dH=TdS-pdV+pdV+Vdp$ | |
| $dF=TdS-pdV-TdS-SdT$ | |
| $dG=TdS+Vdp-TdS-SdT$ | |
| $dH=TdS+Vdp$ | |
| $dF=-pdV-SdT$ | |
| $dG=Vdp-SdT$ | |
| $dU=TdS-pdV$ | |
| $ dH= TdS+Vdp $ | |
| $ dF=-SdT-pdV$ | |
| $dG=-Sdt+Vdp$ |
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