Virial equation of state
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
Virial coefficients
The second virial coefficient represents the initial departure from ideal-gas behavior
where Failed to parse (Conversion error. Server ("https://wikimedia.org/api/rest_") reported: "Cannot get mml. Server problem."): {\displaystyle N_{0}} is Avogadros number and and are volume elements of two different molecules in configuration space. The integration is to be performed over all available phase-space; that is, over the volume of the containing vessel. For the special case where the molecules posses spherical symmetry, so that Failed to parse (Conversion error. Server ("https://wikimedia.org/api/rest_") reported: "Cannot get mml. Server problem."): {\displaystyle u} depends not on orientation, but only on the separation of a pair of molecules, the equation can be simplified to
- Failed to parse (Conversion error. Server ("https://wikimedia.org/api/rest_") reported: "Cannot get mml. Server problem."): {\displaystyle B_{2}(T)=-{\frac {1}{2}}\int _{0}^{\infty }\left(\langle \exp \left(-{\frac {u(r)}{k_{B}T}}\right)\rangle -1\right)4\pi r^{2}dr}
Using the Mayer f-function
- Failed to parse (SVG (MathML can be enabled via browser plugin): Invalid response ("Math extension cannot connect to Restbase.") from server "https://wikimedia.org/api/rest_v1/":): {\displaystyle f_{ij}=f(r_{ij})= \exp\left(-\frac{u(r)}{k_BT}\right) -1 }
one can write the third virial coefficient more compactly as
- Failed to parse (SVG (MathML can be enabled via browser plugin): Invalid response ("Math extension cannot connect to Restbase.") from server "https://wikimedia.org/api/rest_v1/":): {\displaystyle B_{3}(T)= - \frac{1}{3V} \int \int \int f_{12} f_{13} f_{23} dr_1 dr_2 dr_3 }