Computing the Tolman length for solid-liquid interfaces
arXiv:1803.09140 · doi:10.1063/1.5038396
Abstract
The curvature dependence of interfacial free energy, which is crucial in quantitatively predicting nucleation kinetics and the stability of bubbles and droplets, can be described in terms of the Tolman length δ. For solid-liquid interfaces, however,δ has never been computed directly due to various theoretical and practical challenges. Here we present a general method that enables the direct evaluation of the Tolman length from atomistic simulations of a solid-liquid planar interface in out-of-equilibrium conditions. This method works by first measuring the surface tension from the amplitude of thermal capillary fluctuations of a localized version of Gibbs dividing surface, and bythen computing the free energy difference between the surface of tension and the equimolar dividing surface. For benchmark purposes, we computed δfor a model potential, and compared the results to less rigorous indirect approaches.
References in corpus (6)
- Canonical sampling through velocity-rescaling
- Crystal Nucleation in Liquids: Open Questions and Future Challenges in Molecular Dynamics Simulations
- Systematic Improvement of Classical Nucleation Theory
- Crystal-liquid interfacial free energy via thermodynamic integration
- Premelting, fluctuations and coarse-graining of water-ice interfaces
- Why Are Alkali Halide Solid Surfaces Not Wetted By Their Own Melt?
Cited by in corpus (5)
- Interfacial free energy and Tolman length of curved liquid-solid interfaces from equilibrium studies
- Theoretical prediction of the homogeneous ice nucleation rate: disentangling thermodynamics and kinetics
- Finite-temperature materials modeling from the quantum nuclei to the hot electrons regime
- Equivalence between condensation and boiling in a Lennard Jones fluid
- Classical nucleation theory predicts the shape of the nucleus in homogeneous solidification