System-Size Dependence in Grand Canonical and Canonical Ensembles
Debajit Chakraborty, James Dufty, Valentin V. Karasiev

TL;DR
This paper investigates how thermodynamic potentials differ between canonical and grand canonical ensembles as a function of system size, providing exact relations and detailed analysis for a non-interacting Fermi gas, with implications for density functional theory.
Contribution
It derives exact size-dependent relations between thermodynamic potentials in canonical and grand canonical ensembles and analyzes their behavior for a simple Fermi gas model.
Findings
Exact relations between free energy and pressure for arbitrary system size.
Asymptotic equivalence of ensembles as system size becomes large.
Size dependence originates from inter-particle distance and quantum length scales.
Abstract
The thermodynamics for a system with given temperature, density, and volume is described by the Canonical ensemble. The thermodynamics for a corresponding system with the same temperature, volume, and average density is described by the Grand Canonical ensemble. In general a chosen thermodynamic potential (e.g., free energy) is different in the two cases. Their relationship is considered here as a function of the system size. Exact expressions relating the fundamental potential for each (free energy and pressure, respectively) are identified for arbitrary system size. A formal asymptotic analysis for large system size gives the expected equivalence, but without any characterization of the intermediate size dependence. More detailed evaluation is provided for the simple case of a homogeneous, non-interacting Fermi gas. In this case, the origin of size dependence arises from only two…
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