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A new truncation scheme for BBGKY hierarchy: conservation of energy and time reversibility

Published 8 Aug 2016 in cond-mat.stat-mech, math-ph, and math.MP | (1608.02338v1)

Abstract: We propose a new truncation scheme for Bogoliubov-Born-Green-Kirkwood-Yvon (BBGKY) hierarchy. We approximate the three particle distribution function f3(1,2,3,t)f_{3}(1,2,3,t) in terms of f2(1,2,t)f_{2}(1,2,t), f1(3,t)f_{1}(3,t) and two point correlation functions {g2(1,3,t),g2(2,3,t)}\left\lbrace g_{2}(1,3,t), g_{2}(2,3,t)\right\rbrace . Further f2f_{2} is expressed in terms of f1(1,t)f_{1}(1,t) and g2(1,2,t)g_{2}(1,2,t) to close the hierarchy, resulting a set of coupled kinetic equations for f1f_{1} and g2g_{2}. In this paper we show that, for velocity independent correlations, the kinetic equation for f1f_{1} reduces to the model proposed by Martys[Martys N S 1999 \textit{IJMPC} \textbf{10} 1367-1382]. In the steady state limit, the kinetic equation for g2g_{2} reduces to Born-Green-Yvon (BGY) hierarchy for homogeneous density. We also prove that the present scheme respects the energy conservation and under specific circumstances, time symmetry \textit{i.e.,} dH(t)dt=0\displaystyle \frac{dH(t)}{dt} = 0 where H(t)H(t) refers to the Boltzmann's H-function.

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