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Hard-sphere model phase diagram

For the adhesive hard-sphere model, the theoretical phase diagram in the Tg-0 plane has been partially calculated (Watts et al. 1971 Barboy 1974 Grant and Russel 1993). According to this model, there is a critical point r. c = 0.0976 below which the suspension is predicted to phase separate into a phase dilute in particles and one concentrated in them (see Fig. 7-4). The particle concentration at the critical point of this phase transition is 0c = 0.1213. This phase transition is analogous to the gas-liquid transition of ordinary... [Pg.334]

Our purpose in these last two subsections has been to show how the simplest fundamental description of SEE for van der Waals solids can emerge from the hard-sphere model and mean field theory. Much of the remainder of the chapter deals with how we extend this kind of approach using simple molecular models to describe more complex solid-fiuid and solid-solid phase diagrams. In the next two sections, we discuss the numerical techniques that allow us to calculate SEE phase diagrams for molecular models via computer simulation and theoretical methods. In Section IV we then survey the results of these calculations for a range of molecular models. We offer some concluding remarks in Section V. [Pg.121]

An improvement of a classical repulsive expression (2) for one dimensional system of hard sphere by the very accurate presentation of the Liu s EoS (Figure 7) doesn t change a topologic picture of phase diagram in comparison with classical van der Waals expression for repulsive term. It seems that an improvement of repulsive term makes more plausible of isotherm behavior near second critical point. To analyze a qualitative behavior of thermod5mamic surface anomalies in whole via simpler model is preferable due to a topological equivalence of models under consideration. [Pg.225]

Many of the papers on DFT have focused primarily on the hard-sphere system, and it is for this system that most success has been achieved. However, DFT has also been applied to the Lennard-Jones 12-6 system, binary mixtures, nonspherical molecules, and coulombic systems. We will discuss some of these applications later in the chapter as we review what is known about the phase diagrams of various models systems. [Pg.147]

IV. PHASE DIAGRAMS FOR MOLECULAR MODELS A. Hard Spheres... [Pg.152]


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