Generalized van der Waals theory. IX. Excess properties of simple fluid mixtures

1982 ◽  
Vol 35 (2) ◽  
pp. 247 ◽  
Author(s):  
S Nordholm ◽  
PR Harrowell ◽  
K Cheung

The generalized van der Waals theory, recently developed and applied to a wide range of problems involving simple single component fluids, is here extended to uniform simple fluid mixtures. Binary mixtures of hard spheres or particles interacting by Lennard-Jones pair potentials are considered, the Lorentz-Berthelot rules being used to generate the between-species pair-potential. The basic theory is very simple, combining features of cell and mean field theories. Yet it differs considerably from the presently favoured theories of mixtures. The new GvdW theory is implemented at four levels of sophistication but the calculations remain very simple by present standards even for the most accurate form of the theory wherein the effective hard-sphere diameters are determined variationally. The results obtained for the equation of state and thermodynamic excess properties indicate that the very favourable accuracy relative to the simplicity of the theory observed for single component fluids is retained for mixtures. In the case of excess properties calculations for a wide range of equimolar mixtures suggest that the GvdW accuracy is substantially better than that obtained by random mixture or average potential theories but not as good as that obtained by the best theories based on the estimation of the radial distribution functions of the fluid.

2001 ◽  
Vol 235 (2) ◽  
pp. 334-343 ◽  
Author(s):  
Hans Greberg ◽  
Gaia Valeria Paolini ◽  
John Satherley ◽  
Robert Penfold ◽  
Sture Nordholm

Materials ◽  
2019 ◽  
Vol 13 (1) ◽  
pp. 84 ◽  
Author(s):  
Gianmarco Munaò ◽  
Franz Saija

We perform Monte Carlo simulations of a simple hard-soft dimeric model constituted by two tangent spheres experiencing different interactions. Specifically, two hard spheres belonging to different dimers interact via a bare hard-core repulsion, whereas two soft spheres experience a softly repulsive Hertzian interaction. The cross correlations are soft as well. By exploring a wide range of temperatures and densities we investigate the capability of this model to document the existence of structural inhomogeneities indicating the possible onset of aggregates, even if no attraction is set. The fluid phase behavior is studied by analyzing structural and thermodynamical properties of the observed structures, in particular by computing radial distribution functions, structure factors and cluster size distributions. The numerical results are supported by integral equation theories of molecular liquids which allow for a finer and faster spanning of the temperature-density diagram. Our results may serve as a framework for a more systematic investigation of self-assembled structures of functionalized hard-soft dimers able to aggregate in a variety of structures widely oberved in colloidal dispersion.


1980 ◽  
Vol 33 (10) ◽  
pp. 2139 ◽  
Author(s):  
S Nordholm ◽  
M Johnson ◽  
BC Freasier

This article is devoted to further development of the generalized van der Waals theory and its application to non-uniform hard sphere fluids. A coarse-graining assumption included in the original derivation is replaced by a weaker assumption recognizing the non-zero range of hard core interactions. The new fine-grained theory thus contains a non-local entropy functional and allows fluid structure on a length scale shorter than the hard core diameter to be resolved. Moreover, it contains a simplified representation of the mechanism leading to hard sphere structure due essentially to geometrical packing constraints. This is shown by application of the theory to hard sphere adsorption profiles in the case of a hard wall and to radial distribution functions of a hard sphere fluid. The amount of structure is underestimated partly due to the use of a density-independent excluded volume. It is shown that this flaw can be remedied by use of a hard- sphere entropy functional which successfully interpolates between the original high density estimate and the known behaviour in the low density limit.


1973 ◽  
Vol 51 (11) ◽  
pp. 1216-1226 ◽  
Author(s):  
E. W. Grundke ◽  
D. Henderson ◽  
R. D. Murphy

This paper reports zero-pressure excess properties of binary fluid mixtures of Lennard-Jones 6:12 molecules calculated from the Percus–Yevick (PY) theory and the energy equation. The PY theory, used this way, gives results that are in excellent agreement with simulation studies.In addition, results obtained from the compressibility equation are discussed for comparison. The geometrical structure of the mixture, as indicated by the PY pair distribution functions, is described. Error estimates are provided for the calculated excess properties.


Sign in / Sign up

Export Citation Format

Share Document