paper

Ratio of effective temperature to pressure controls the mobility of sheared hard spheres

arXiv:1103.3704 · doi:10.1103/PhysRevE.85.011503

Abstract

Using molecular dynamics simulation, we calculate fluctuations and response for steadily sheared hard spheres over a wide range of packing fractions and shear strain rates , using two different methods to dissipate energy. To a good approximation, shear stress and density fluctuations are related to their associated response functions by a single effective temperature that is equal to or larger than the kinetic temperature . We find a crossover in the relationship between the relaxation time and the the nondimensionalized effective temperature , where is the pressure and is the sphere diameter. In the solid response regime, the behavior at fixed packing fraction satisfies , where depends weakly on , suggesting that the average local yield strain is controlled by the effective temperature in a way that is consistent with shear transformation zone theory. In the fluid response regime, the relaxation time depends on as it depends on in equilibrium. This regime includes both near-equilibrium conditions where and far-from-equilibrium conditions where . We discuss the implications of our results for systems with soft repulsive interactions.

9 pages, 6 figures. Major revision: added results and analysis for sheared inelastic hard spheres to complement the previous results for sheared thermostatted hard spheres, increasing the available range of and strengthening the conclusions; added discussion of results relative to the jamming phase diagram

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