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arXiv 1807.08201cond-mat.soft
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无序颗粒材料中的旋转声

Rotational sound in disordered granular materials

Kuniyasu Saitoh, Rohit K. Shrivastava, Stefan Luding

摘要:

我们采用数值模拟来了解无序摩擦盘系统中弹性驻波的演化,其中旋转声模式的色散关系进行了详细的分析。在晶格上的摩擦粒子的情况下,旋转模式表现出“光学”的色散关系在高频率制度,代表一个肩膀的振动态密度和旋转速度的自相关的快速振荡。一个基于格子的模型描述了小波数的旋转模式的色散关系。如果接触圆盘之间的切向弹性力足够大,则该模型可以很好地解释转动模式。如果切向力与法向力相当或小于法向力,则模型在短波长下失效。然而,旋转模式的色散关系,然后遵循横向模式的模型预测,这意味着磁盘的旋转切换到声学声音行为的快速振荡。我们通过分析无序摩擦盘的本征矢量证明了这种旋转模式的转变,并确定了频带的上限和下限。我们发现,这些是不可逆的切向刚度的整个范围内作为一个显着的区别,在晶格上的摩擦粒子的旋转声音。

英文摘要:

We employ numerical simulations to understand the evolution of elastic standing waves in disordered frictional disk systems, where the dispersion relations of rotational sound modes are analyzed in detail. As in the case of frictional particles on a lattice, the rotational modes exhibit an "optical-like" dispersion relation in the high frequency regime, representing a shoulder of the vibrational density of states and fast oscillations of the autocorrelations of rotational velocities. A lattice-based model describes the dispersion relations of the rotational modes for small wave numbers. The rotational modes are perfectly explained by the model if tangential elastic forces between the disks in contact are large enough. If the tangential forces are comparable with or smaller than normal forces, the model fails for short wave lengths. However, the dispersion relation of the rotational modes then follows the model prediction for transverse modes, implying that the fast oscillations of disks' rotations switch to acoustic sound behavior. We evidence such a transition of the rotational modes by analyzing the eigen vectors of disordered frictional disks and identify upper and lower limits of the frequency-bands. We find that those are not reversed over the whole range of tangential stiffness as a remarkable difference from the rotational sound in frictional particles on a lattice.

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