Nonequilibrium Phase Transition for a Heavy Particle in a Granular Fluid

Details Nonequilibrium Phase Transition for a Heavy Particle in a Granular Fluid Nonequilibrium Phase Transition for a Heavy Particle in a Granular Fluid

2001-06-11

arxiv.org/abs/cond-mat/0106205v2

Phys. Rev. E 64, 051305 (2001)

Physics

Condensed Matter

Statistical Mechanics

28 pages, 12 figures included

Scientific paper

10.1103/PhysRevE.64.051305

It is shown that the homogeneous cooling state (HCS) for a heavy impurity particle in a granular fluid supports two distinct phases. The order parameter $\phi$ is the mean square velocity of the impurity particle relative to that of a fluid particle, and the control parameter $\xi$ is the fluid cooling rate relative to the impurity collision rate. For $\xi<1$ there is a ``normal'' phase for which $\phi$ scales as the fluid/impurity mass ratio, just as for a system with elastic collisions. For $\xi>1$ an ``ordered'' phase occurs in which $\phi$ is finite even for vanishingly small mass ratio, representing an extreme violation of energy equipartition. The phenomenon can be described in terms of a Landau-like free energy for a second order phase transition. The dynamics leading to the HCS is studied in detail using an asymptotic analysis of the Enskog-Lorentz kinetic equation near each phase and the critical domain. Critical slowing is observed with a divergent relaxation time at the critical point. The stationary velocity distributions are determined in each case, showing a crossover from Maxwellian in the normal phase to an exponential quartic function of the velocity that is sharply peaked about the non-zero $\phi$ for the ordered phase. It is shown that the diffusion coefficient in the normal phase diverges at the critical point and remains so in the ordered phase. This is interpreted as a transition from diffusive to ballistic dynamics between the normal and ordered phases.

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