The vapor–liquid phase equilibria of square‐well systems with hard‐sphere diameters σ,
well‐depths ε, and ranges λ= 1.25, 1.375, 1.5, 1.75, and 2 are determined by Monte Carlo …

Since the formulation of the so-called high temperature series expansion (HTSE) by
Zwanzig, 1 thermodynamic perturbation theories developed along this line have been one of …

The binary liquid phase separation of aqueous solutions of γ‐crystallins is utilized to gain
insight into the microscopic interactions between these proteins. The interactions are …

We present an analytic equation of state, without any adjustable parameters, for the square-
well fluid of variable well width (1⩽ λ⩽ 2) based on perturbation theory using the real …

The vapor-liquid phase behavior and the critical behavior of the square-well (SW) fluid are
investigated as a function of the interaction range, λ∊[1.25, 3], by means of the self …

Fluids formed by molecules interacting with discrete potentials are examined in the context
of perturbation theory and the reference hypernetted chain equation (RHNC) solution to the …

The vapor-liquid equilibrium of the square-well (SW) fluid of variable range is studied. The
analysis focuses on the dependence on the SW range, which exhibits deviations from …

The free energy of square-well (SW) systems of hard-core diameter σ with ranges 1≤ λ≤ 3
is expanded in a perturbation series. This interval covers most ranges of interest, from short …

An equation of state for square-well fluids of short and long potential range λ is presented
and compared with Gibbs ensemble and canonical Monte Carlo simulation data; vapour …

The Helmholtz free-energy of a square-well fluid is studied as a function of the range of the
well. A high-temperature perturbation expansion is carried out to second order, which is …