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Theory of Atomic Motions in Simple Classical Liquids

K. S. Singwi

A. Sjölander

  • Institute of Theoretical Physics, Sven Hultins gata, Göteborg, Sweden and Solid State Science Division, Argonne National Laboratory, Argonne, Illinois

  • Institute of Theoretical Physics, Sven Hultins gata, Göteborg, Sweden

Phys. Rev. 167, 152 – Published 5 March, 1968

DOI: https://doi.org/10.1103/PhysRev.167.152

Abstract

This paper is an attempt towards developing a theory of the self-motion of atoms in monatomic classical fluids, based on a simplified Liouville equation and on a knowledge of the interaction potential V(r) and the static pair correlation function g(r). A nonlinear integral equation for the velocity autocorrelation function Φ(t) is derived which under certain approximations can be written as dΦ(t)dt+0tK(tt)Φ(t)dt=0 where the kernel K(t) is an implicit function of Φ(t). An expression for K(t) in terms of V(r) and g(r) has been given. Explicit numerical calculations for the "memory" function K(t) have been made for liquid argon at T=85.9°K, and the results have been compared with those obtained by Rahman from his machine computations.

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