Stationary nonequilibrium states by molecular dynamics. Fourier's law
- 1 May 1982
- journal article
- research article
- Published by American Physical Society (APS) in Physical Review A
- Vol. 25 (5), 2778-2787
- https://doi.org/10.1103/physreva.25.2778
Abstract
We have developed a technique to produce stationary nonequilibrium states in a molecular-dynamics system; this method is based on the introduction of stochastic boundary conditions to simulate the contact with a thermal wall. The relaxation times involved in such contact are short enough (∼ sec) to make the technique suitable for computer experiments. The method allows the simulation of bulk properties in a system coupled with a heat reservoir and the study of the local thermodynamical equilibrium. Furthermore, it gives a physical description of the heat transfer near a thermal wall. The method has been applied to simulate high thermal gradients in a region of dense fluids ranging from the gas-liquid coexistence line to the freezing line, to check the validity of the linear thermal response (Fourier's law). We have found that the linear region extends at least up to gradients of the order of 1.8× K/cm for argon. In the bulk region where boundary effects are negligible we have verified the validity of the local equilibrium hypothesis for all simulated gradients.
Keywords
This publication has 8 references indexed in Scilit:
- Canonical ensemble and nonequilibrium states by molecular dynamicsJournal of Statistical Physics, 1980
- Transport properties of the Lorentz gas: Fourier's lawJournal of Statistical Physics, 1978
- Computer "Experiments" on Classical Fluids. IV. Transport Properties and Time-Correlation Functions of the Lennard-Jones Liquid near Its Triple PointPhysical Review A, 1973
- Equilibrium Theory of Simple LiquidsPhysical Review A, 1972
- The thermal conductivity of liquid and gaseous argonPhysica, 1968
- Computer "Experiments" on Classical Fluids. I. Thermodynamical Properties of Lennard-Jones MoleculesPhysical Review B, 1967
- Compressibility isotherms of argon at temperatures between −25°C and −155°C, and at densities up to 640 amagat (pressures up to 1050 atmospheres)Physica, 1958
- The Statistical Mechanical Theory of Transport Processes. IV. The Equations of HydrodynamicsThe Journal of Chemical Physics, 1950