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A quasi-elastic regime for vibrated granular gases

Abstract

Using simple scaling arguments and two-dimensional numerical simulations of a granular gas excited by vibrating one of the container boundaries, we study a double limit of small 1r1-r and large LL, where rr is the restitution coefficient and LL the size of the container. We show that if the particle density n0n_0 and (1r2)(n0Ld)(1-r^2)(n_0 Ld) where dd is the particle diameter, are kept constant and small enough, the granular temperature, i.e. the mean value of the kinetic energy per particle, /N/N, tends to a constant whereas the mean dissipated power per particle, /N/N, decreases like 1/N1/\sqrt{N} when NN increases, provided that (1r2)(n0Ld)2<1(1-r^2)(n_0 Ld)^2 < 1. The relative fluctuations of EE, DD and the power injected by the moving boundary, II, have simple properties in that regime. In addition, the granular temperature can be determined from the fluctuations of the power I(t)I(t) injected by the moving boundary.

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