Intermolecular distance and density scaling of dynamics in molecular liquids
arXiv:1904.02026 · doi:10.1063/1.5098455
Abstract
A broad variety of liquids conform to density scaling: relaxation times expressed as a function of the ratio of temperature to density, the latter raised to a material constant γ. For atomic liquids interacting only through simple pair potentials, the exponent γ is very nearly equal to n/3, where n is the steepness of the intermolecular potential, while for molecular liquids having rigid bonds and built using the same interatomic potential, γ>n/3. We find that for this class of molecular liquids γ=n/δ, where the parameter δ relates the intermolecular distance to the density along an isomorph (line of approximately constant dynamics and structure). δ depends only on the molecular structure and not the interatomic potential.
References in corpus (4)
- Theoretical perspective on the glass transition and amorphous materials
- Pressure-energy correlations in liquids. II. Analysis and consequences
- Thermodynamic scaling of diffusion in supercooled Lennard-Jones liquids
- Feasibility of single-order parameter description of equilibrium viscous liquid dynamics
Cited by in corpus (7)
- Transport properties of Lennard-Jones fluids: Freezing density scaling along isotherms
- An extreme case of density scaling: The Weeks-Chandler-Andersen system at low temperatures
- Isomorph theory beyond thermal equilibrium
- Connecting Entropy Scaling and Density Scaling
- Unified scaling model for viscosity of crude oil over extended temperature range
- Scaling properties of liquid dynamics predicted from a single configuration: Small rigid molecules
- Isomorph invariance in the liquid and plastic-crystal phases of asymmetric-dumbbell models