2015
DOI: 10.1017/jfm.2015.501
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Hydrodynamics of binary mixtures of granular gases with stochastic coefficient of restitution

Abstract: A hydrodynamic description of dilute binary gas mixtures comprising smooth inelastic spheres interacting by binary collisions with a random coefficient of restitution is presented. Constitutive relations are derived using the Chapman-Enskog perturbative method, associated with a computer-aided method to allow high-order Sonine polynomial expansions. The transport coefficients obtained are checked against DSMC simulations. The resulting equations are applied to the analysis of a vertically vibrated system. It i… Show more

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Cited by 11 publications
(7 citation statements)
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“…But a significant part can go into transverse components of translational energy and rotational energy. Thus, this is a simple demonstration of the idea that β z (and β x ) must be treated as a random variable rather than a fixed quantity as in the case of the normal coefficient of restitution associated with spherical particles in a granular gas, although recent efforts have treated this quantity as a random variable (Gunkelmann et al, 2014;Serero et al, 2015).…”
Section: Resultsmentioning
confidence: 99%
“…But a significant part can go into transverse components of translational energy and rotational energy. Thus, this is a simple demonstration of the idea that β z (and β x ) must be treated as a random variable rather than a fixed quantity as in the case of the normal coefficient of restitution associated with spherical particles in a granular gas, although recent efforts have treated this quantity as a random variable (Gunkelmann et al, 2014;Serero et al, 2015).…”
Section: Resultsmentioning
confidence: 99%
“…However, this method goes beyond the Maxwellian approximation since it determines the exact velocity distribution functions f i . In this context, the comparison of DSMC results versus analytical results for very dilute systems (φ → 0) can be used to asses the accuracy of the Maxwellian approximation (32) for determining the cooling rates (34). The second method is MD simulations.…”
Section: A Temperaturesmentioning
confidence: 99%
“…One approach, when momentum is not conserved, is the stochastic thermostat, which adds a random force acting on every particle with zero correlation time, and amplitude related to the intensity of the kicks [28][29][30][31]. Other models, which are appropriate when momentum is conserved, consider random restitution coefficients (larger or smaller than 1) that lead to a homogeneous steady state [32][33][34]. In the present article we will consider the so-called model also valid for smooth plates, where the thermostat is a collisional one, so that energy is injected in every collision [35].…”
Section: Introductionmentioning
confidence: 99%
“…One approach is the stochastic thermostat, which adds a random force acting on every particle with zero correlation time, and amplitude related with the intensity of the kicks [28][29][30]. Other models consider random restitution coefficients (larger or smaller than one) that lead to a homogeneous steady state [31][32][33]. In the present article we will consider the so-called ∆-model, where the thermostat is a collisional one, so that energy is injected in every collision [34].…”
Section: Introductionmentioning
confidence: 99%