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Mayer f-function
The Mayer f-function is an auxiliary function that often appears in the series expansion of thermodynamic quantities related to classical many-particle systems.Donald Allan McQuarrie, Statistical Mechanics (HarperCollins, 1976), page 228 It is named after chemist and physicist Joseph Edward Mayer.
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 \Omega 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 \beta=(k{B}T)^{-1} the inverse absolute temperature in units of energy−1 .
Notes
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