Excluded volume and molecular field in the Lennard-Jones fluid: a modified first-order perturbation theory
A. Trokhymchuk, V. Hordiichuk, R. Melnyk, I. Nezbeda

TL;DR
This paper evaluates a modified first-order perturbation theory for Lennard-Jones fluids, showing it accurately predicts thermodynamics by emphasizing the reference system's physical content and consistent state dependence treatment.
Contribution
It introduces a range-based decomposition in perturbation theory that improves accuracy by focusing on the reference system's short-range interactions.
Findings
The modified theory reproduces high-accuracy reference data.
Range-based decomposition makes the perturbation contribution near-mean-field.
Success depends on the reference system's physical content and state dependence handling.
Abstract
The equation of state and, more generally, the thermodynamics of the Lennard-Jones fluid have long served as a benchmark problem in the statistical theory of fluids. Among available theoretical approaches, first-order perturbation theory occupies a special position: only at this level does the correction to the Helmholtz free energy admit an exact statistical-mechanical expression. In this work, we present a systematic, simulation-based assessment of a non-classical first-order perturbation theory in which the reference system incorporates the entire short-range part of the interaction, while the perturbation is confined to the remaining long-range tail. We show that this range-based decomposition transforms the perturbation contribution into a small, smoothly varying, near-mean-field quantity over a broad supercritical thermodynamic domain. When its density and temperature derivatives…
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