From equilibrium to non-equilibrium statistical mechanics of liquids
O. Joaqu\'in-Jaime, R. Peredo-Ortiz, M. Medina-Noyola, L.F., Elizondo-Aguilera

TL;DR
This paper reviews the fundamental concepts of statistical mechanics for liquids, emphasizing the extension from equilibrium to non-equilibrium states, with applications to rheology and viscoelasticity of glass- and gel-forming liquids.
Contribution
It provides a general framework and a concrete example for describing non-equilibrium properties of liquids from first principles.
Findings
Extension of equilibrium relations to non-equilibrium conditions.
Application to rheological and viscoelastic properties.
Insights into aging and transient states in liquids.
Abstract
Relevant and fundamental concepts of the statistical mechanical theory of classical liquids are ordinarily introduced in the context of the description of thermodynamic equilibrium states. This makes explicit reference to probability distribution functions of \emph{equilibrium} statistical ensembles (canonical, microcanonical, ...) in the derivation of general and fundamental relations between inter-particle interactions and measurable macroscopic properties of a given system. This includes, for instance, expressing the internal energy and the pressure as functionals of the radial distribution function, or writing transport coefficients (diffusion constant, linear viscosity, ...) in terms of integral relations involving both, static and dynamic auto-correlation functions (density-density, stress-stress, ...). Most commonly, however, matter is not in thermodynamic equilibrium, and this…
Peer Reviews
No public reviews on file for this paper yet. If you reviewed it on a platform where reviews are public (OpenReview, ICLR, NeurIPS, ICML), you can paste yours below so the community can read it here.
Videos
No videos yet. Explain this paper in a talk, walkthrough, or lecture? Add one.
Taxonomy
TopicsAdvanced Thermodynamics and Statistical Mechanics · Material Dynamics and Properties · Phase Equilibria and Thermodynamics
