Virial equation of state: Difference between revisions
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*<math> B_k\left( T \right) </math> is called the k-th virial coefficient | *<math> B_k\left( T \right) </math> is called the k-th virial coefficient | ||
==Virial coefficients== | |||
The second virial coefficient represents the initial departure from ideal-gas behavior | |||
<math>B_{2}(T)= \frac{N_0}{2V} \int .... \int (1-e^{-u/kT}) ~d\tau_1 d\tau_2 | |||
</math> | |||
where <math>N_0</math> is [[Avogadro constant | Avogadros number]] and <math>d\tau_1</math> and <math>d\tau_2</math> 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 <math>u</math> depends not on | |||
orientation, but only on the separation <math>r</math> of a pair of molecules, the equation can be simplified to | |||
:<math>B_{2}(T)= - \frac{1}{2} \int_0^\infty \left(\langle \exp\left(-\frac{u(r)}{k_BT}\right)\rangle -1 \right) 4 \pi r^2 dr</math> | |||
Using the [[Mayer f-function]] | |||
:<math>f_{ij}=f(r_{ij})= \exp\left(-\frac{u(r)}{k_BT}\right) -1 </math> | |||
one can write the third virial coefficient more compactly as | |||
:<math>B_{3}(T)= - \frac{1}{3V} \int \int \int f_{12} f_{13} f_{23} dr_1 dr_2 dr_3 | |||
</math> | |||
==References== | |||
#[http://dx.doi.org/10.1088/0034-4885/7/1/312 James A Beattie and Walter H Stockmayer "Equations of state",Reports on Progress in Physics '''7''' pp. 195-229 (1940)] | |||
[[category:equations of state]] | [[category:equations of state]] | ||
Revision as of 11:29, 22 May 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
Virial coefficients
The second virial coefficient represents the initial departure from ideal-gas behavior
where 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
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 }