Abstract

The components of pair distribution function in different directions with respect to the coordinate system defined by the simulation box are determined for Lennard-Jones fluid simulated using the Monte Carlo technique in cubic boxes of various size. The approach of Pratt and Haan is employed to analyze the distortion of isotropic fluid structure due to the periodic boundary conditions and qualitative agreement is found between the theoretical and simulated course of particular angular components of distribution function. The relation between the anisotropy of correlation functions and the system size dependency of residual energy and compressibility factor is analyzed. The finite size effects become significantly pronounced in systems with size lower than 5 particle diameters, especially if the length of the box-edge is equal to a non-integer multiple of molecular diameter. With increasing temperature the implicit finite size effects on fluid structure as well as on the thermodynamic properties become less important. The primary cause of the structure deformation lies in the short-range interparticle correlations and the long-range interactions are not important; therefore, the implicit finite size effects influence all kinds of atomistic simulations, including those using the interactions of finite range and in the molecular dynamics simulations. However, at present the simulated systems are usually of sufficiently large size and ignoring the implicit finite size does not lead to serious problems, except for the determination of surface properties using the inhomogeneous simulations which are more sensitive to the lateral dimension of simulation box.

Highlights

  • For a long time, the molecular simulations of fluids served dominantly as a tool which helped to validate the quality of theoretical models and to gain understanding of the behaviour of simulated systems at molecular level

  • The thin short-dashed black line shows the radial distribution function obtained in simulation box with dimension Lx = 12σ

  • By applying running average method calculated from three points

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Summary

INTRODUCTION

The molecular simulations of fluids served dominantly as a tool which helped to validate the quality of theoretical models and to gain (qualitative) understanding of the behaviour of simulated systems at molecular level. Mandell [31] determined the orientationally dependent pair correlation function for Lennard-Jones fluid and used the Born–Green equation to analyze the influence of the periodic error on thermodynamic and structural properties. Kolafa [36] studied the influence of implicit finite size effects on thermodynamic properties of Lennard-Jones fluid using the molecular dynamics simulations and compared the simulated values of internal energy and compressibility factor with the values obtained by solving the OrnsteinZernike (OZ) equation under periodic boundary conditions. The observed oscillatory dependence of simulated thermodynamic properties on the system size with the period equal approximately to the particle diameter was in agreement with the results obtained by solving the OZ relation. J. Janecek / Influence of the Periodic Boundary Conditions on the Fluid Structure and on the Thermodynamic Properties 273 Computed from the Molecular Simulations of the simulation box.

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