# Difference between revisions of "Ideal gas: Heat capacity"

Carl McBride (talk | contribs) |
Carl McBride (talk | contribs) |
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− | :<math>C_p - C_V = \left.\frac{\partial V}{\partial T}\right\vert_p \left(p + \left.\frac{\partial | + | :<math>C_p - C_V = \left.\frac{\partial V}{\partial T}\right\vert_p \left(p + \left.\frac{\partial U}{\partial V}\right\vert_T \right) </math> |

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+ | for an [[ideal gas]] this becomes: | ||

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:<math>\left.C_p -C_V \right.=R</math> | :<math>\left.C_p -C_V \right.=R</math> | ||

==References== | ==References== |

## Revision as of 13:28, 21 June 2007

for an ideal gas this becomes:

## References

- Donald A. McQuarrie "Statistical Mechanics" (1976) Eq. 1-1
- Landau and Lifshitz Course of Theoretical Physics Volume 5 Statistical Physics 3rd Edition Part 1 Equation 42.11