Home

About

Advanced Search

Browse by Discipline

Scientific Societies

E-print Alerts

Add E-prints

E-print Network
FAQHELPSITE MAPCONTACT US


  Advanced Search  

 
Theory for non-equilibrium statistical mechanics Phil Attard*
 

Summary: Theory for non-equilibrium statistical mechanics
Phil Attard*
Received 23rd March 2006, Accepted 8th May 2006
First published as an Advance Article on the web 7th July 2006
DOI: 10.1039/b604284h
This paper reviews a new theory for non-equilibrium statistical mechanics. This gives the non-
equilibrium analogue of the Boltzmann probability distribution, and the generalization of entropy
to dynamic states. It is shown that this so-called second entropy is maximized in the steady state,
in contrast to the rate of production of the conventional entropy, which is not an extremum. The
relationships of the new theory to Onsager's regression hypothesis, Prigogine's minimal entropy
production theorem, the Langevin equation, the formula of Green and Kubo, the Kawasaki
distribution, and the non-equilibrium fluctuation and work theorems, are discussed. The theory is
worked through in full detail for the case of steady heat flow down an imposed temperature
gradient. A Monte Carlo algorithm based upon the steady state probability density is
summarized, and results for the thermal conductivity of a Lennard-Jones fluid are shown to be in
agreement with known values. Also discussed is the generalization to non-equilibrium mechanical
work, and to non-equilibrium quantum statistical mechanics. As examples of the new theory two
general applications are briefly explored: a non-equilibrium version of the second law of
thermodynamics, and the origin and evolution of life.
1. Introduction

  

Source: Attard, Phil - School of Chemistry, University of Sydney

 

Collections: Chemistry