Closed-loop phase equilibria of a symmetrical associating mixture of square-well molecules examined by Gibbs ensemble Monte Carlo simulation

Citation
La. Davies et al., Closed-loop phase equilibria of a symmetrical associating mixture of square-well molecules examined by Gibbs ensemble Monte Carlo simulation, PHYS REV E, 61(3), 2000, pp. 2245-2256
Citations number
60
Categorie Soggetti
Physics
Journal title
PHYSICAL REVIEW E
ISSN journal
1063651X → ACNP
Volume
61
Issue
3
Year of publication
2000
Pages
2245 - 2256
Database
ISI
SICI code
1063-651X(200003)61:3<2245:CPEOAS>2.0.ZU;2-6
Abstract
A closed loop of liquid-liquid immiscibility for a simple model binary symm etrical mixture of square-well monomers with a single short-ranged interact ion site has been recently observed using the Gibbs ensemble Monte Carlo te chnique [L. A. Davies, G. Jackson, and L. F. Rull, Phys. Rev. Lett. 82, 528 5 (1999)]. This model system has unfavorable mean-field interactions betwee n unlike components which leads to phase separation at intermediate tempera tures; the addition of a directional bonding site leads to association and miscibilty of the system at low temperatures. In this work we present a det ailed study of the effect of a variation in pressure and of the strength of the bonding interaction on the phase equilibria of such a model system by Gibbs ensemble simulation. The phase diagram is dominated by regions of liq uid-liquid immiscibility which are bounded at high temperatures by an upper critical solution temperature and by a lower critical solution temperature (LCST) for specific values of the pressure and association strength. This closed-loop region is seen to increase in size as the pressure of the syste m is increased. For weak bonding interaction strengths the system does not possess a LCST and is seen to exhibit regions of two-phase vapor-liquid coe xistence which are separated from the region of liquid-Liquid immiscibility by a three-phase line. The phase equilibria of the same model system is al so determined using the statistical associating fluid theory as adapted for potentials of variable range; the theory provides a good description df th e closed-loop immiscibility and other features of the phase diagram.