Mayer f-function

The Mayer f-function, or f-bond is defined as:

$f_{12}=f({\mathbf{r}}_{12})=\exp (-\frac{{\mathrm{\Phi }}_{12}(r)}{k_{B}T})-1$

where

• $k_B$ is the Boltzmann constant.
• $T$ is the temperature.
• ${\mathrm{\Phi }}_{12}(r)$ is the intermolecular pair potential.

Diagrammatically the Mayer f-function is written as

Hard sphere model

For the hard sphere model the Mayer f-function becomes:

$f_{12}=\{\begin{array}{ccc}-1& ;& r_{12}\le \sigma (\mathrm{o}\mathrm{v}\mathrm{e}\mathrm{r}\mathrm{l}\mathrm{a}\mathrm{p})\\ 0& ;& r_{12}>\sigma (\mathrm{n}\mathrm{o}\mathrm{o}\mathrm{v}\mathrm{e}\mathrm{r}\mathrm{l}\mathrm{a}\mathrm{p})\end{array}$

where $\sigma$ is the hard sphere diameter.

References

1. Joseph Edward Mayer and Maria Goeppert Mayer "Statistical Mechanics" John Wiley and Sons (1940)
2. Joseph E. Mayer "Contribution to Statistical Mechanics", Journal of Chemical Physics 10 pp. 629-643 (1942)