Mayer f-function

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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

V(\mathbf{i},\mathbf{j})

where the bold labels \mathbf{i} and \mathbf{j} denote the continuous degrees of freedom associated with the particles e.g.

\mathbf{i}=\mathbf{r}_i

for spherically symmetric particles and

\mathbf{i}=(\mathbf{r}_i,\Omega_i)

for rigid non-spherical particles where \mathbf{r} denotes position and Ω the orientation parametrized e.g. by Euler angles. The Mayer f-function is then defined as

f(\mathbf{i},\mathbf{j})=e^{-\beta V(\mathbf{i},\mathbf{j})}-1

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