Ideal gas: Heat capacity: Difference between revisions
		
		
		
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| Carl McBride (talk | contribs) No edit summary | Carl McBride (talk | contribs)  No edit summary | ||
| Line 1: | Line 1: | ||
| :<math>C_p - C_V = \left.\frac{\partial V}{\partial T}\right\vert_p \left(p + \left.\frac{\partial E}{\partial V}\right\vert_T \right) </math> | :<math>C_p - C_V = \left.\frac{\partial V}{\partial T}\right\vert_p \left(p + \left.\frac{\partial E}{\partial V}\right\vert_T \right) </math> | ||
| :<math>\left.C_p -C_V \right.= | :<math>\left.C_p -C_V \right.=R</math> | ||
| ==References== | ==References== | ||
| #Donald A. McQuarrie "Statistical Mechanics" (1976) Eq. 1-1 | #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 | #Landau and Lifshitz Course of Theoretical Physics Volume 5 Statistical Physics 3rd Edition Part 1 Equation 42.11 | ||
| [[Category: Ideal gas]] | [[Category: Ideal gas]] | ||
Revision as of 13:57, 28 May 2007
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