Virial coefficients of model systems: Difference between revisions

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m (New page: <math> \frac{p V}{N k_B T } = Z = 1 + \sum_{k=2} B_k(T) \rho^{k-1}. </math> where * <math> p </math> is the pressure *<math> V </math> is the volume *<math> N </math> is the number o...)
 
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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, <math> Z </math> in terms of either the
density or the pressure. In the first case:
<math> \frac{p V}{N k_B T } = Z = 1 + \sum_{k=2} B_k(T) \rho^{k-1}.
<math> \frac{p V}{N k_B T } = Z = 1 + \sum_{k=2} B_k(T) \rho^{k-1}.
</math>
</math>
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*<math> N </math> is the number of molecules
*<math> N </math> is the number of molecules
*<math> \rho \equiv \frac{N}{V} </math> is the (number) density
*<math> B_k </math> is called the k-th virial coefficient


* to be continued ...
* to be continued ...

Revision as of 11:42, 20 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, Z in terms of either the density or the pressure. In the first case:

pVNkBT=Z=1+∑k=2Bk(T)ρk−1.

where

  • p is the pressure
  • V is the volume
  • N is the number of molecules
  • ρ≡NV is the (number) density
  • Bk is called the k-th virial coefficient


  • to be continued ...