Sound velocities of Lennard-Jones systems near the liquid-solid phase transition
arXiv:2008.00858 · doi:10.3390/molecules25153498
Abstract
Longitudinal and transverse sound velocities of Lennard-Jones systems are calculated at the liquid-solid coexistence using the additivity principle. The results are shown to agree well with the ``exact'' values obtained from their relations to excess energy and pressure. Some consequences, in particular, in the context of the Lindemann's melting rule and Stokes-Einstein relation between the self-diffusion and viscosity coefficients are discussed. Comparison with available experimental data on the sound velocities of solid argon at melting conditions is provided.
7 pages, 5 figures, published in Molecules
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- The instantaneous shear modulus in the shoving model
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- Freezing density scaling of fluid transport properties: Application to liquefied noble gases
- Bridgman formula for the thermal conductivity of atomic and molecular liquids
- When do soft spheres become hard spheres?
- Elementary vibrational model for thermal conductivity of Lennard-Jones fluids: Applicability domain and accuracy level
- Quasi-universal behaviour of shear relaxation times in simple fluids
- Note: Sound velocities of generalized Lennard-Jones () fluids near freezing
- Speed of sound in dense simple liquids
- Modified Bridgman formula for the thermal conductivity of complex (dusty) plasma fluids
- Variational approach to Yukawa fluids. II. Instantaneous elastic moduli and sound velocities
- Excess entropy scaling of the transverse sound speed in simple fluids