Kinetic theory for finite inhomogeneous gravitational systems

Physics – Condensed Matter – Statistical Mechanics

Scientific paper

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Astronomical Models, Gravitational Effects, Kinetic Theory, Stellar Motions, Two Body Problem, Approximation, Distribution Functions, Fokker-Planck Equation, Particle Interactions, Statistical Mechanics

Scientific paper

Chandrasekhar's (1942) kinetic theory of binary encounters in an infinite homogeneous gravitational system is extended to a finite isolated nonrotating stable inhomogeneous system of gravitating point particles. Proceeding from a systematic approximation based on the BBGKY hierarchy of equations for the reduced distribution functions, a description of encounters is obtained which corresponds to two-particle scattering in a strong quasi-steady mean field. A proximate-encounter approximation is formulated so that the mean field can be considered as uniform, and a collision integral is found whose form does not depend on field effects but retains nonlocal effects associated with the system's inhomogeneity. A kinetic equation is derived which contains corrective terms allowing for delocalization of the encountering particles. It is shown that the classical encounter description based on the standard Fokker-Planck kinetic equation is valid in the limit where log N is much greater than unity (N being the population of the system).

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