Mayer f-function
From Wikipedia, the free encyclopedia
| This article does not cite any references or sources. (October 2007) Please help improve this article by adding citations to reliable sources. Unverifiable material may be challenged and removed. |
The Mayer f-function is an auxiliary function that often appears in the series expansion of thermodynamical quantities related to classical many-particle systems.
[edit] Definition
Consider a system of classical particles interacting through a pair-wise potential
where the bold labels
and
denote the continuous degrees of freedom associated with the particles e.g.
for spherically symmetric particles and
for rigid non-spherical particles where
denotes position and Ω the orientation parametrized e.g. by Euler angles. The Mayer f-function is then defined as
where β = (kBT) − 1 the inverse absolute temperature in units of (Temperature times the Boltzmann constant kB)-1 .
See Statistical Mechanics, Donald A McQuarrie, page 228





