Abstract
Granular gases are systems in which macroscopic particles lose a
fraction of their kinetic energy at each collision. When an external
energy supply is continuously brought to the particles, the system may
reach a non-equilibrium steady state, whose properties differ
significantly from those of thermal equilibrium (breakdown of the
equipartition, non-gaussian statistics, modified hydrodynamics). All
those characteristics are intimately related to the dissipative nature
of collisions.
The studies of granular gases have focused mainly on spherical
particles. However, anisotropy for granular particles is ubiquitous
in nature, and one expects that the anisotropy introduces additional
effects.
We analyze, both numerically and analytically by means of the
Boltzmann equation, the kinetics of a granular planar rotator with a
fixed center undergoing inelastic collisions with bath particles. The
angular velocity distribution displays a large variety of behavior:
when the mass of the rotator is much larger than the mass of the bath
particles, a perturbative method allows to solve the Boltzmann
equation and shows that the distribution is quasi-Gaussian in this
Brownian limit. Conversely, in the limit of an infinitely light
particle, an exact solution is obtained when the coefficient of
restitution is equal to zero. Intermediate cases are obtained by a
precise numerical method showing strong deviations to gaussian
behavior.
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