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Coefficient of tangential restitution for viscoelastic spheres

机译:粘弹性球体的切向恢复系数

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The collision of frictional granular particles may be described by an interaction force whose normal component is that of viscoelastic spheres while the tangential part is described by the model by Cundall and Strack (Geotechnique 29, 47 (1979)) being the most popular tangential collision model in Molecular Dynamics simulations. Albeit being a rather complicated model, governed by 5 phenomenological parameters and 2 independent initial conditions, we find that it is described by 3 independent parameters only. Surprisingly, in a wide range of parameters the corresponding coefficient of tangential restitution, epsilon(t), is well described by the simple Coulomb law with a cut-off at epsilon(t) = 0. A more complex behavior of the coefficient of restitution as a function on the normal and tangential components of the impact velocity, g(n) and g(t) , including negative values of epsilon(n) , is found only for very small ratio g(t)/g(n). For the analysis presented here we neglect dissipation of the interaction in normal direction.
机译:摩擦颗粒的碰撞可以通过相互作用力来描述,该相互作用力的法向分量是粘弹性球体的正向分量,而切向部分由Cundall和Strack的模型描述(Geotechnique 29,47(1979)),是最受欢迎的切向碰撞模型。在分子动力学模拟中。尽管这是一个相当复杂的模型,受5个现象学参数和2个独立的初始条件控制,但我们发现它仅由3个独立的参数描述。令人惊讶的是,在简单的库仑定律中,在epsilon(t)= 0处有一个截止值,因此可以在很宽的参数范围内很好地描述相应的切向恢复系数epsilon(t)。作为冲击速度的法向和切向分量的函数,只有极小的比率g(t)/ g(n)才发现g(n)和g(t)(包括epsilon(n)的负值)。对于此处介绍的分析,我们忽略了法线方向上相互作用的耗散。

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