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Deutsche Physikalische Gessellschaft IOP Institute of Physics

Brownian motion in a granular fluid

Focus on Brownian Motion and Diffusion in the 21st Century

James W Dufty1 and J Javier Brey2

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Part of Focus on Brownian Motion and Diffusion in the 21st Century

The Fokker–Planck equation for a heavy particle in a granular fluid is derived from the Liouville equation. The host fluid is assumed to be in its homogeneous cooling state and all interactions are idealized as smooth, inelastic hard spheres. The similarities and differences between the Fokker–Planck equation for elastic and inelastic collisions are discussed in detail. Although the fluctuation–dissipation relation is violated and the reference fluid is time-dependent, it is shown that diffusion occurs at long times for a wide class of initial conditions. The results presented here generalize previous results based on the Boltzmann–Lorentz equation to higher densities.


PACS

05.40.Jc Brownian motion

47.57.Gc Granular flow

05.10.Gg Stochastic analysis methods (Fokker-Planck, Langevin, etc.)

Subjects

Soft matter, liquids and polymers

Fluid dynamics

Computational physics

Statistical physics and nonlinear systems

Dates

Issue 1 (January 2005)

Received 6 September 2004

Published 31 January 2005



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