Fluid-fluid phase behaviour in the explicit solvent ionic model: hard spherocylinder solvent molecules

TL;DR

This study investigates the fluid-fluid phase transition in a model combining ionic fluids and hard spherocylinder solvent molecules, using theoretical approaches to understand how molecular shape affects phase behavior.

Contribution

It introduces a combined theoretical framework using SPT and AMSA to analyze phase behavior in ionic mixtures with anisotropic solvent molecules, highlighting the impact of molecular shape.

Findings

Broader phase coexistence region with spherocylinder solvents.

Higher critical temperature in the RPM-HSC model compared to RPM-HS.

Different concentration dependences predicted by AMSA and MSA.

Abstract

We study a fluid-fluid phase transition of the explicit solvent model represented as a mixture of the restricted primitive model (RPM) of ionic fluid and neutral hard spherocylinders (HSC). To this end, we combine two theoretical approaches, i.e., the scale particle theory (SPT) and the associative mean spherical approximation (AMSA). Whereas the SPT is sufficient to provide a rather good description of a reference system taking into account hard-core interactions, the AMSA is known to be efficient in treating the Coulomb interactions between the ions. Alternatively, we also use the mean spherical approximation (MSA) for comparison. In general, both approximations lead to similar qualitative results for the phase diagrams: the region of coexisting envelope becomes broader and shifts towards larger densities and higher temperatures when the pressure increases. However, the AMSA and the MSA produce different concentration dependences, i.e., contrary to the MSA, the AMSA phase diagrams show that the high-density phase mostly consists of the ions for all pressures considered. To demonstrate the effect of asphericity of solvent molecules on the fluid-fluid phase transition, we consider an "equivalent" mixture in which the HSC particles are replaced by hard spheres (HS) of the same volume. It is observed that in the case of HSC solvent (RPM-HSC model), the region of phase coexistence is wider than for the case of the solvent molecules being of spherical shape (RPM-HS model). It is also found that the critical temperature is higher in the RPM-HSC model than in the RPM-HS model, though it becomes the same at higher pressures in the MSA, while in the AMSA this difference remains essential.