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Alternative Derivation of the Partition Function for Generalized Ensembles

A pedagogical approach for deriving the statistical mechanical partition function, in a manner that emphasizes the key role of entropy in connecting the microscopic states to thermodynamics, is introduced. The connections between the combinatoric formula $S= k \ln W$ applied to the Gibbs construction, the Gibbs entropy, $S = -k \sum\limits_i p_i \ln p_i$, and the microcanonical entropy expression $S= k \ln Ω$ are clarified. The condition for microcanonical equilibrium, and the associated role of the entropy in the thermodynamic potential is shown to arise naturally from the postulate of equal {\itshape a priori} states. The derivation of the canonical partition function follows simply by invoking the Gibbs ensemble construction at constant temperature and using the first and second law of thermodynamics (\emph{via} the fundamental equation $dE = TdS - PdV + μdN$) that incorporate the conditions of conservation of energy and composition without the needs for explicit constraints; other ensemble follow easily. The central role of the entropy in establishing equilibrium for a given ensemble emerges naturally from the current approach. Connections to generalized ensemble theory also arise and are presented in this context.