English

Fluid-fluid demixing and density anomaly in a ternary mixture of hard spheres

Soft Condensed Matter 2020-06-02 v1 Statistical Mechanics

Abstract

We report the grand-canonical solution of a ternary mixture of discrete hard spheres defined on a Husimi lattice built with cubes, which provides a mean-field approximation for this system on the cubic lattice. The mixture is composed by point-like particles (0NN) and particles which exclude up to their first (1NN) and second neighbors (2NN), with activities z0z_0, z1z_1 and z2z_2, respectively. Our solution reveals a very rich thermodynamic behavior, with two solid phases associated with the ordering of 1NN (S1S1) or 2NN particles (S2S2), and two fluid phases, being one regular (RFRF) and the other characterized by a dominance of 0NN particles (F0F0 phase). However, in most part of the phase diagram these fluid (FF) phases are indistinguishable. Discontinuous transitions are observed between all the four phases, yielding several coexistence surfaces in the system, among which a fluid-fluid and a solid-solid demixing surface. The former one is limited by a line of critical points and a line of triple points (where the phases RFRF-F0F0-S2S2 coexist), both meeting at a special point, after which the fluid-fluid coexistence becomes metastable. Another line of triple points is found, connecting the FF-S1S1, FF-S2S2 and S1S1-S2S2 coexistence surfaces. A critical FF-S1S1 surface is also observed meeting the FF-S1S1 coexistence one at a line of tricritical points. Furthermore, a thermodynamic anomaly characterized by minima in isobaric curves of the total density of particles is found, yielding three surfaces of minimal density in the activity space, depending on which activity is kept fixed during its calculation.

Keywords

Cite

@article{arxiv.2005.07307,
  title  = {Fluid-fluid demixing and density anomaly in a ternary mixture of hard spheres},
  author = {Nathann T. Rodrigues and Tiago J. Oliveira},
  journal= {arXiv preprint arXiv:2005.07307},
  year   = {2020}
}