Department of Mechanical Engineering and Materials Science, Yale University, New Haven, Connecticut 06520, USA.
Laboratoire Jean Perrin UMR 8237 CNRS/UPMC, Université Pierre et Marie Curie, 75255 Paris Cedex, France.
Phys Rev E. 2017 Dec;96(6-1):062902. doi: 10.1103/PhysRevE.96.062902. Epub 2017 Dec 1.
We focus on the response of mechanically stable (MS) packings of frictionless, bidisperse disks to thermal fluctuations, with the aim of quantifying how nonlinearities affect system properties at finite temperature. In contrast, numerous prior studies characterized the structural and mechanical properties of MS packings of frictionless spherical particles at zero temperature. Packings of disks with purely repulsive contact interactions possess two main types of nonlinearities, one from the form of the interaction potential (e.g., either linear or Hertzian spring interactions) and one from the breaking (or forming) of interparticle contacts. To identify the temperature regime at which the contact-breaking nonlinearities begin to contribute, we first calculated the minimum temperatures T_{cb} required to break a single contact in the MS packing for both single- and multiple-eigenmode perturbations of the T=0 MS packing. We find that the temperature required to break a single contact for equal velocity-amplitude perturbations involving all eigenmodes approaches the minimum value obtained for a perturbation in the direction connecting disk pairs with the smallest overlap. We then studied deviations in the constant volume specific heat C[over ¯]{V} and deviations of the average disk positions Δr from their T=0 values in the temperature regime T{C[over ¯]{V}}<T<T_{r}, where T_{r} is the temperature beyond which the system samples the basin of a new MS packing. We find that the deviation in the specific heat per particle ΔC[over ¯]_{V}^{0}/C[over ¯]_{V}^{0} relative to the zero-temperature value C[over ¯]_{V}^{0} can grow rapidly above T_{cb}; however, the deviation ΔC[over ¯]_{V}^{0}/C[over ¯]_{V}^{0} decreases as N^{-1} with increasing system size. To characterize the relative strength of contact-breaking versus form nonlinearities, we measured the ratio of the average position deviations Δr^{ss}/Δr^{ds} for single- and double-sided linear and nonlinear spring interactions. We find that Δr^{ss}/Δr^{ds}>100 for linear spring interactions is independent of system size. This result emphasizes that contact-breaking nonlinearities are dominant over form nonlinearities in the low-temperature range T{cb}<T<T_{r} for model jammed systems.
我们关注无摩擦、双分散圆盘的力学稳定(MS)填充的热涨落响应,目的是量化非线性如何在有限温度下影响系统性质。相比之下,许多先前的研究在零温度下描述了无摩擦球形粒子的 MS 填充的结构和力学性质。具有纯排斥接触相互作用的圆盘填充具有两种主要类型的非线性,一种来自于相互作用势的形式(例如,线性或赫兹弹簧相互作用),另一种来自于粒子间接触的断裂(或形成)。为了确定接触断裂非线性开始贡献的温度范围,我们首先计算了 T=0 MS 填充的单特征模态和多特征模态扰动下打破单个 MS 填充接触所需的最小温度 T_{cb}。我们发现,对于涉及所有特征模态的具有相同速度幅度的扰动,打破单个接触所需的温度接近在圆盘对之间具有最小重叠的方向上进行的扰动获得的最小温度。然后,我们在 T_{C[over ¯]{V}}<T<T_{r}温度范围内研究了恒容比热 C[over ¯]_{V}的偏差以及平均圆盘位置 Δr 与其 T=0 值的偏差。T_{r}是系统采样新 MS 填充基池的温度。我们发现,相对于零温度值 C[over ¯]_{V}^{0},每个粒子的比热偏差 ΔC[over ¯]_{V}^{0}/C[over ¯]_{V}^{0}可以在 T_{cb}以上快速增长;然而,随着系统尺寸的增加,偏差 ΔC[over ¯]_{V}^{0}/C[over ¯]_{V}^{0}会以 N^{-1}的速度减小。为了表征接触断裂与形式非线性的相对强度,我们测量了单边和双边线性和非线性弹簧相互作用的平均位置偏差 Δr^{ss}/Δr^{ds}的比值。我们发现,对于线性弹簧相互作用,Δr^{ss}/Δr^{ds}>100与系统尺寸无关。这个结果强调了在模型堵塞系统中,T{cb}<T<T_{r}的低温范围内,接触断裂非线性相对于形式非线性是主导的。