THE FLUID STRUCTURES FOR SOFT-SPHERE POTENTIALS VIA THE ZERO-SEPARATION THEOREMS ON MOLECULAR-DISTRIBUTION FUNCTIONS

Citation
Ll. Lee et al., THE FLUID STRUCTURES FOR SOFT-SPHERE POTENTIALS VIA THE ZERO-SEPARATION THEOREMS ON MOLECULAR-DISTRIBUTION FUNCTIONS, The Journal of chemical physics, 104(20), 1996, pp. 8058-8067
Citations number
54
Categorie Soggetti
Physics, Atomic, Molecular & Chemical
ISSN journal
00219606
Volume
104
Issue
20
Year of publication
1996
Pages
8058 - 8067
Database
ISI
SICI code
0021-9606(1996)104:20<8058:TFSFSP>2.0.ZU;2-Y
Abstract
We present a class of closures specifically designed to satisfy the ze ro-separation theorems for the correlation functions y(r) (the cavity function), gamma(r)=h(r)-C(r) (the indirect correlation), and B(r) (th e bridge function) at coincidence r=0 for soft-sphere pair potentials. The rationale is to ensue the correct behavior of these correlation f unctions inside the core r<sigma. Since the coincidence theorems impli cate the thermodynamic properties of the bulk fluid: the isothermal co mpressibility, the internal energy and the chemical potentials, we can hopefully enforce consistency between the structure and thermodynamic properties. We solve the Ornstein-Zernike equation for the Lennard-Jo nes molecules where plentiful Monte Carlo data are available for testi ng. It turns out that not only consistency is achieved, we also obtain accurate structures: the pair correlation function g(r), the cavity f unction, and the bridge function for wide ranges of fluid states (0.72 < T< 1.5, rho*< 0.9). Comparison with MC data attests to the accurac y. The closure of the zero-separation type (ZSEP), is sufficiently rob ust and flexible to ensure not only fulfillment of the zero-separation theorems but also pressure consistency. Success with the Lennard-Jone s potential implies its applicability to other similar soft-sphere pot entials. (C) 1996 American Institute of Physics.