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A relationship of mean-field theory for a driven lattice gas to an exact equilibrium density functional

W S Brams Dwandaru1,2 and Matthias Schmidt1,3

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We consider the totally asymmetric exclusion process (TASEP) of particles on a one-dimensional lattice that interact with site exclusion and are driven into one direction only. The mean-field approximation of the dynamical equation for the one-particle density of this model is shown to be equivalent to the exact Euler–Lagrange equations for the equilibrium density profiles of a binary mixture. In this mixture particles occupy one (two) lattice sites and correspond to resting (moving) particles in the TASEP. Despite the strict absence of bulk phase transitions in the equilibrium mixture, the influence of density-dependent external potentials is shown to induce abrupt changes in the one-body density that are equivalent to the exact out-of-equilibrium phase transitions between steady states in the TASEP with open boundaries.


PACS

05.50.+q Lattice theory and statistics (Ising, Potts, etc.)

47.11.Qr Lattice gas

05.60.-k Transport processes

05.70.Ln Nonequilibrium and irreversible thermodynamics

05.70.Fh Phase transitions: general studies

MSC

82B26 Phase transitions (general)

82C26 Dynamic and nonequilibrium phase transitions (general)

82C70 Transport processes

82C20 Dynamic lattice systems (kinetic Ising, etc.) and systems on graphs

Subjects

Fluid dynamics

Computational physics

Statistical physics and nonlinear systems

Dates

Issue 44 (2 November 2007)

Received 17 July 2007, in final form 18 July 2007

Published 16 October 2007



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