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Material instability with stress localization

机译:具有应力定位的材料不稳定性

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This paper is concerned with a possible material instability arising from a non-unique dependence of stress on deformation and leading to localization of stress in otherwise homogeneous deformations. A recently published work cites several constitutive theories and certain experimental evidence indicating this type of constitutive behavior, and it provides an analysis of quasi-static bifurcation of in the steady exten-sional deformation of certain idealized isotropic elastic solids and viscoelastic fluids. The principle objective is to raise the question as to whether the ubiquitous "force chains" observed in experiments and computer simulation of non-cohesive granular media represent stress localization. As a prelude to a more complete investigation, consideration is given to the question of the statistical distribution of contact forces in sphere assemblies. The maximum-entropy estimator of statistical thermodynamics is employed to derive the statistical distribution of contact forces in a static assembly of nearly-rigid grains. However, instead of the usual constraint of stationary energy, stationarity of stress is assumed. It is shown that under fairly general circumstances one obtains a distribution with exponential tail in contact-force magnitude, which is found in various experiments and numerical simulations. This result is exact for frictionless monodispcrse sphere assemblies subject to isotropic confinement. According to the present model, the exponential tail does not depend on special models of "force propagation" in granular assemblies, of the type postulated in the contemporary physics literature. According to the above principle, the precise form of the probability density for force depends on the weight (a priori probability) assigned to elementary volumes in the state-space of contact forces. Various weight functions are discussed and the resulting distributions are compared to experiment and simulation. In its present form, the analysis given here does not apply to the "two-phase" structure associated with force chains in granular media.
机译:本文涉及一种可能的材料不稳定性,来自压力对变形的非独特依赖性,并导致均匀变形中应力的定位。最近发表的工作引用了几个组成型理论和某些实验证据,表明这种类型的本构体行为,并提供了在某些理想的各向同性弹性固体和粘弹性液体的稳定延长变形中的准静态分叉的分析。原则目标是提出关于在非粘结粒度介质的实验和计算机模拟中观察到的无处不在的“力链”的问题代表了应力定位。作为更完整的调查的前奏,对球体组件中接触力的统计分布问题的审议。使用统计热力学的最大熵估计器用于在近刚性颗粒的静态组装中导出接触力的统计分布。然而,假设具有静止能量的通常限制,而是假设应力的平稳性。结果表明,在相当一般情况下,在各种实验和数值模拟中发现了一种接触力幅度的指数尾部的分布。该结果精确适用于经过各向同性监禁的摩擦摩洛莫摩西克斯球体组件。根据本模型,指数尾部不依赖于在当代物理文献中假设的粒状组件中“力传播”的特殊模型。根据上述原理,力的概率密度的精确形式取决于在接触力的状态空间中分配给基本体积的重量(优先概率)。讨论了各种重量函数,并将得到的分布与实验和仿真进行比较。在其目前的形式中,这里给出的分析不适用于与粒状介质中的力链相关的“两相”结构。

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