Jagla ramp particles, interacting through a ramp potential with two characteristic length scales, are known to show in their bulk phase thermodynamic and dynamic anomalies, similar to what is found in water. Jagla particles also exhibit a line of phase transitions separating a low density liquid phase and a high density liquid phase, terminating in a liquid-liquid critical point in a region of the phase diagram that can be studied by simulations. Employing molecular dynamics computer simulations, we study the thermodynamics and the dynamics of solutions of hard spheres (HS) in a solvent formed by Jagla ramp particles. We consider the cases of HS mole fraction x(HS) = 0.10, 0.15, and 0.20, and also the case x(HS) = 0.50 (a 1: 1 mixture of HS and Jagla particles). We find a liquid-liquid critical point, up to the highest HS mole fraction; its position shifts to higher pressures and lower temperatures upon increasing x(HS). We also find that the diffusion coefficient anomalies appear to be preserved for all the mole fractions studied.
Corradini, D., Buldyrev, S.v., Gallo, P., Stanley, H.e. (2010). Effect of hydrophobic solutes on the liquid-liquid critical point. PHYSICAL REVIEW E, STATISTICAL, NONLINEAR, AND SOFT MATTER PHYSICS, 81(6) [10.1103/PhysRevE.81.061504].
Effect of hydrophobic solutes on the liquid-liquid critical point
GALLO, PAOLA;
2010-01-01
Abstract
Jagla ramp particles, interacting through a ramp potential with two characteristic length scales, are known to show in their bulk phase thermodynamic and dynamic anomalies, similar to what is found in water. Jagla particles also exhibit a line of phase transitions separating a low density liquid phase and a high density liquid phase, terminating in a liquid-liquid critical point in a region of the phase diagram that can be studied by simulations. Employing molecular dynamics computer simulations, we study the thermodynamics and the dynamics of solutions of hard spheres (HS) in a solvent formed by Jagla ramp particles. We consider the cases of HS mole fraction x(HS) = 0.10, 0.15, and 0.20, and also the case x(HS) = 0.50 (a 1: 1 mixture of HS and Jagla particles). We find a liquid-liquid critical point, up to the highest HS mole fraction; its position shifts to higher pressures and lower temperatures upon increasing x(HS). We also find that the diffusion coefficient anomalies appear to be preserved for all the mole fractions studied.I documenti in IRIS sono protetti da copyright e tutti i diritti sono riservati, salvo diversa indicazione.
