Relaxation dynamics of non-Brownian spheres below jamming
arXiv:2007.09418 · doi:10.1007/s10955-021-02710-8
Abstract
We numerically study the relaxation dynamics and associated criticality of non-Brownian frictionless spheres below jamming in spatial dimensions , , , and , and in the mean-field Mari-Kurchan model. We discover non-trivial finite-size and volume fraction dependences of the relaxation time associated to the relaxation of unjammed packings. In particular, the relaxation time is shown to diverge logarithmically with system size at any density below jamming, and no critical exponent can characterise its behaviour approaching jamming. In mean-field, the relaxation time is instead well-defined: it diverges at jamming with a critical exponent that we determine numerically and differs from an earlier mean-field prediction. We rationalise the finite logarithmic divergence using an extreme-value statistics argument in which the relaxation time is dominated by the most connected region of the system. The same argument shows that the earlier proposition that relaxation dynamics and shear viscosity are directly related breaks down in large systems. The shear viscosity of non-Brownian packings is well-defined in all in the thermodynamic limit, but large finite-size effects plague its measurement close to jamming.
11 pages, 8 figures
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- Introduction to the dynamics of disordered systems: equilibrium and gradient descent
- Jamming, relaxation, and memory in a structureless glass former
- Critical Scaling of Compression-Driven Jamming of Athermal Frictionless Spheres in Suspension
- Non-Affine Displacements Below Jamming under Athermal Quasi-Static Compression
- Universality of stress-anisotropic and stress-isotropic jamming of frictionless spheres in three dimensions: Uniaxial vs isotropic compression
- Gradient descent dynamics and the jamming transition in infinite dimensions
- Relaxation dynamics and long-time tails explain shear-induced diffusion of soft athermal particles near jamming