Related Experiment Video
Updated: Jun 20, 2026

Orientational Transition in a Liquid Crystal Triggered by the Thermodynamic Growth of Interfacial Wetting Sheets
Published on: May 15, 2017
Determination of the solid-liquid interfacial free energy along a coexistence line by Gibbs-Cahn integration
Brian B Laird1, Ruslan L Davidchack, Yang Yang
1Department of Chemistry, University of Kansas, Lawrence, Kansas 66045, USA. blaird@ku.edu
Abstract:
We calculate the solid-liquid interfacial free energy gamma(sl) for the Lennard-Jones (LJ) system at several points along the pressure-temperature coexistence curve using molecular-dynamics simulation and Gibbs-Cahn integration. This method uses the excess interfacial energy (e) and stress (tau) along the coexistence curve to determine a differential equation for gamma(sl) as a function of temperature. Given the values of gamma(sl) for the (100), (110), and (111) LJ interfaces at the triple-point temperature (T( *)=kT/varepsilon=0.618), previously obtained using the cleaving method by Davidchack and Laird [J. Chem. Phys. 118, 7657 (2003)], this differential equation can be integrated to obtain gamma(sl) for these interfaces at higher coexistence temperatures. Our values for gamma(sl) calculated in this way at T( *)=1.0 and 1.5 are in good agreement with those determined previously by cleaving, but were obtained with significantly less computational effort than required by either the cleaving method or the capillary fluctuation method of Hoyt, Asta, and Karma [Phys. Rev. Lett. 86, 5530 (2001)]. In addition, the orientational anisotropy in the excess interface energy, stress and entropy, calculated using the conventional Gibbs dividing surface, are seen to be significantly larger than the relatively small anisotropies in gamma(sl) itself.
Related Concept Videos
Area Between Curves: Integrating With Respect to y
Liquid–Solid Solutions
Chemical and Solubility Equilibria
Two Components: Liquid–Liquid Systems
Theories of Dissolution: The Danckwerts' Model and Interfacial Barrier Model
Intermolecular Forces in Solutions
When the strengths of the intermolecular forces of attraction between solute and solvent species in a solution are no different than those present in the separated components, the solution is formed with no accompanying energy change. Such a solution is called an ideal solution. A mixture of ideal gases (or gases such as helium and argon,...
