Virial coefficients of model systems: Difference between revisions
		
		
		
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| density or the pressure. In the first case: | density or the pressure. In the first case: | ||
| <math> \frac{p V}{N k_B T } = Z = 1 + \sum_{k=2}^{\infty} B_k(T) \rho^{k-1} | :<math> \frac{p V}{N k_B T } = Z = 1 + \sum_{k=2}^{\infty} B_k(T) \rho^{k-1}</math>. | ||
| </math> | |||
| where   | where   | ||
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| *[[hard sphere: virial equation of state|Hard spheres]] | *[[hard sphere: virial equation of state|Hard spheres]] | ||
| *[[hard sphere: virial equation of state|Hard disks]] | *[[hard sphere: virial equation of state|Hard disks]] | ||
| [[Category:Virial coefficients]] | |||
Revision as of 12:04, 27 February 2007
The virial equation of state is used to describe the behavior of diluted gases. It is usually written as an expansion of the compresiblity factor, , in terms of either the density or the pressure. In the first case:
- .
where
- is the pressure
- is the volume
- is the number of molecules
- is the (number) density
- is called the k-th virial coefficient