Abstract

The structural properties of fluids whose molecules interact via potentials with a hard-core plus n piece-wise constant sections of different widths and heights are derived using a (semi-analytical) rational-function approximation method. The results are illustrated for the cases of a square-shoulder plus square-well potential and a shifted square-well potential and compared both with simulation data and with those that follow from the (numerical) solutions of the Percus-Yevick integral equation.

Highlights

  • Simple models of intermolecular interaction have proven to be useful tools in understanding diverse phenomena in real fluids

  • In this paper we have proposed a method of deriving the structural properties of a particular kind of discrete-potential fluids, namely the ones in which molecules interact via a potential consisting of a hard-core plus n-step constant sections of different heights and widths

  • Two approximations were considered: one in which some unknown constants are fixed at their zero density value (RFA1) and one which enforces the continuity of the derivative of the cavity function (RFA2)

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Summary

Introduction

Simple models of intermolecular interaction have proven to be useful tools in understanding diverse phenomena in real fluids. In previous papers [22, 40], following a methodology that, approximate, has proven successful for many other systems [41], the structural properties of the square-well and the square-shoulder fluids were derived. The main aim of this paper is to use a similar methodology, referred to as the method of rational-function approximation (RFA), to generalize the previous results and derive the structural properties of fluids whose molecules interact via potentials with a hard-core plus piece-wise constant sections of different widths and heights. The consistency of the present approach with the results for both the square-well and square-shoulder results is proven in an appendix

Fundamental relations
The general n-step case
Particularization to two-step potentials
Illustration of the approximation for two-step potentials
Conclusions
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