Effect of the shape of simulation box on the Van der Waals loop of a Lennard-Jones fluid (original) (raw)

1998, Chemical Physics Letters

It is demonstrated that the Van der Waals loop appearing in the computer simulations almost vanishes by modifying the shape of the simulation cell even when small size systems are treated. After a long molecular dynamics simulation, it was found that the complete phase separation into vapor and liquid took place in the unstable region. The surface free energy of the interface between the liquid and vapor phases is suggested to be a major reason why the artificial loop has been observed in molecular dynamics simulations. We show that the loop depth diminishes as the box ratio of the simulation cell is enlarged.

Determination of curvature corrections to the surface tension of a liquid–vapor interface through molecular dynamics simulations

The Journal of Chemical Physics, 2002

We use molecular dynamics simulations of particles interacting through a truncated Lennard-Jones potential to study the surface properties of the curved liquid–vapor interface. We determine the Tolman length δ, investigate its critical behavior, and provide first results for the rigidity constants of bending, k, and of Gaussian curvature, k̄. The rigidity constant of bending, determined at three different temperatures, is found to be positive and of the order of one-half kBT. The rigidity constant of Gaussian curvature, determined at a single temperature, is of the same order of magnitude.

The coexistence region in the Van der Waals fluid and the liquid-liquid phase transitions

Frontiers in Chemistry

Cellular membraneless organelles are thought to be droplets formed within the two-phase region corresponding to proteinaceous systems endowed with the liquid-liquid transition. However, their metastability requires an additional constraint—they arise in a certain region of density and temperature between the spinodal and binodal lines. Here, we consider the well-studied van der Waals fluid as a test model to work out criteria to determine the location of the spinodal line for situations in which the equation of state is not known. Our molecular dynamics studies indicate that this task can be accomplished by considering the specific heat, the surface tension and characteristics of the molecular clusters, such as the number of component chains and radius of gyration.

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