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模拟颗粒气体输运特性的弹性硬球系统。

System of elastic hard spheres which mimics the transport properties of a granular gas.

作者信息

Santos Andrés, Astillero Antonio

机构信息

Departamento de Física, Universidad de Extremadura, E-06071 Badajoz, Spain.

出版信息

Phys Rev E Stat Nonlin Soft Matter Phys. 2005 Sep;72(3 Pt 1):031308. doi: 10.1103/PhysRevE.72.031308. Epub 2005 Sep 30.

Abstract

The prototype model of a fluidized granular system is a gas of inelastic hard spheres (IHS) with a constant coefficient of normal restitution alpha. Using a kinetic theory description we investigate the two basic ingredients that a model of elastic hard spheres (EHS) must have in order to mimic the most relevant transport properties of the underlying IHS gas. First, the EHS gas is assumed to be subject to the action of an effective drag force with a friction constant equal to half the cooling rate of the IHS gas, the latter being evaluated in the local equilibrium approximation for simplicity. Second, the collision rate of the EHS gas is reduced by a factor (1/2)(1+alpha), relative to that of the IHS gas. Comparison between the respective Navier-Stokes transport coefficients shows that the EHS model reproduces almost perfectly the self-diffusion coefficient and reasonably well the two transport coefficients defining the heat flux, the shear viscosity being reproduced within a deviation less than 14% (for alpha > or = 0.5). Moreover, the EHS model is seen to agree with the fundamental collision integrals of inelastic mixtures and dense gases. The approximate equivalence between IHS and EHS is used to propose kinetic models for inelastic collisions as simple extensions of known kinetic models for elastic collisions.

摘要

流化颗粒系统的原型模型是具有恒定法向恢复系数α的非弹性硬球(IHS)气体。我们使用动力学理论描述来研究弹性硬球(EHS)模型为了模拟基础IHS气体的最相关输运性质必须具备的两个基本要素。首先,假设EHS气体受到有效阻力的作用,其摩擦常数等于IHS气体冷却速率的一半,为简单起见,后者在局部平衡近似中进行评估。其次,EHS气体的碰撞率相对于IHS气体降低了一个因子(1/2)(1 + α)。各自的纳维-斯托克斯输运系数之间的比较表明,EHS模型几乎完美地再现了自扩散系数,并且相当好地再现了定义热通量的两个输运系数,剪切粘度的再现偏差小于14%(对于α≥0.5)。此外,EHS模型被认为与非弹性混合物和稠密气体的基本碰撞积分一致。IHS和EHS之间的近似等效性被用于提出非弹性碰撞的动力学模型,作为已知弹性碰撞动力学模型的简单扩展。

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