Note: Sound velocities of generalized Lennard-Jones () fluids near freezing
arXiv:2110.09139 · doi:10.3390/molecules26061660
Abstract
In a recent paper [S. Khrapak, Molecules {\bf 25}, 3498 (2000)] the longitudinal and transverse sound velocities of conventional Lennard-Jones systems at the liquid-solid coexistence were calculated. It was shown that the sound velocities remain almost invariant along the liquid-solid coexistence boundary lines and that their magnitudes are comparable with those of repulsive soft sphere and hard sphere models at the fluid-solid phase transition. This implies that attraction does not affect the magnitude of sound velocities at the fluid-solid phase transition. This paper provides further evidence to this by examining the generalized Lennard-Jones -6 fluids with ranging from to and demonstrating that the steepness of repulsive term has only a minor effect on the magnitude of the sound velocities.
arXiv comment4 pages, 1 figure
References in corpus (8)
- Lindemann melting criterion in two dimensions
- A new view of the Lindemann criterion
- Universality of the melting curves for a wide range of interaction potentials
- Sound velocities of Lennard-Jones systems near the liquid-solid phase transition
- Unified description of sound velocities in strongly coupled Yukawa systems of different spatial dimensionality
- Note: Sound velocity of a soft sphere model near the fluid-solid phase transition
- Note: Melting criterion for soft particle systems in two dimensions
- Freezing and melting equations for the -6 Lennard-Jones systems