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      Discontinuous change of shear modulus for frictional jammed granular materials

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          Abstract

          The shear modulus of jammed frictional granular materials with the harmonic repulsive interaction under an oscillatory shear is numerically investigated. It is confirmed that the storage modulus, the real part of the shear modulus, for frictional grains with sufficiently small strain amplitude \(\gamma_0\) discontinuously emerges at the jamming transition point. The storage modulus for small \(\gamma_0\) differs from that of frictionless grains even in the zero friction limit, while they are almost identical with each other for sufficiently large \(\gamma_0\), where the transition becomes continuous. The stress-strain curve exhibits a hysteresis loop even for a small strain, which connects a linear region for sufficiently small strain to another linear region for relatively larger strain. We propose a new scaling law to interpolate between the states of small and large \(\gamma_0\).

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          Jamming is not just cool any more

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            Jamming of frictional spheres and random loose packing

            The role of friction coefficient, \(\mu\), on the jamming properties of disordered, particle packings is studied using computer simulations. Compressed, soft-sphere packings are brought towards the jamming transition - the point where a packing loses mechanical stability - by decreasing the packing fraction. The values of the packing fraction at the jamming transition, \(\phi^{\mu}_{c}\), gradually decrease from the random close packing point for zero friction, to a value coincident with random loose packing as the friction coefficient is increased over several orders of magnitude. This is accompanied by a decrease in the coordination number at the jamming transition, \(z^{\mu}_{c}\), which varies from approximately six to four with increasing friction. Universal power law scaling is observed in the pressure and coordination number as a function of distance from the generalised, friction-dependent jamming point. Various power laws are also reported between the \(\phi^{\mu}_{\rm c}\), \(z^{\mu}_{\rm c}\), and \(\mu\). Dependence on preparation history of the packings is also investigated.
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              Gutenberg Richter and Characteristic Earthquake Behavior in Simple Mean-Field Models of Heterogeneous Faults

              The statistics of earthquakes in a heterogeneous fault zone is studied analytically and numerically in the mean field version of a model for a segmented fault system in a three-dimensional elastic solid. The studies focus on the interplay between the roles of disorder, dynamical effects, and driving mechanisms. A two-parameter phase diagram is found, spanned by the amplitude of dynamical weakening (or ``overshoot'') effects (epsilon) and the normal distance (L) of the driving forces from the fault. In general, small epsilon and small L are found to produce Gutenberg-Richter type power law statistics with an exponential cutoff, while large epsilon and large L lead to a distribution of small events combined with characteristic system-size events. In a certain parameter regime the behavior is bistable, with transitions back and forth from one phase to the other on time scales determined by the fault size and other model parameters. The implications for realistic earthquake statistics are discussed.
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                Author and article information

                Journal
                2016-12-03
                Article
                1612.00961
                b4f341bd-76c9-4826-ba74-442c79ff05e8

                http://arxiv.org/licenses/nonexclusive-distrib/1.0/

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                Custom metadata
                10 pages, 13 figures
                cond-mat.soft

                Condensed matter
                Condensed matter

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