首页> 外文期刊>Journal of Statistical Physics >Asymptotic behavior of a stationary silo with absorbing walls
【24h】

Asymptotic behavior of a stationary silo with absorbing walls

机译:具有吸收壁的固定筒仓的渐近行为

获取原文
获取原文并翻译 | 示例
           

摘要

We study the nearest neighbors one dimensional uniform q-model of force fluctuations in bead packs,((1)) a stochastic model to simulate the stress of granular media in two dimensional silos. The vertical coordinate plays the role of time, and the horizontal coordinate the role of space. The process is a discrete time Markov process with state space R-{1,R-...N}. At each layer (time), the weight supported by each grain is a random variable of mean ones (its own weight) plus the sum of random fractions of the weights supported by the! nearest neighboring grains at the previous layer. The fraction of the weight given to the right neighbor of the successive layer is a uniform random variable in [0, 1] independent of everything. The remaining weight is given to the left neighbor. In the boundaries, a uniform fraction of the weight leans on the wall of the silo. This corresponds to absorbing boundary conditions. For this model we show that there exists a unique invariant measure. The mean weight at site i under the invariant measure is i(N+1-i); we prove that its variance is 1/2(i(N+1-i))(2) + O(N-3) and the covariances between grains i not equal j are of order O(N-3). Moreover, as N --> infinity, the law under the invariant measure of the weights divided by N 2 around site (integer part of) rN, r is an element of (0, 1), converges to a product of gamma distributions with parameters 2 and 2(r(1-r))(-1) (sum of two exponentials of mean r(1-r)/2). Liu et al.((2)) proved that for a silo with infinitely many weightless grains, any product of gamma distributions with parameters 2 and 2/p with rho is an element of [0,infinity) are invariant. Our result shows that as the silo grows, the model selects exactly one of these Gamma's at each macroscopic place. [References: 14]
机译:我们研究了珠包中力波动的最近邻一维均匀q模型,((1))随机模型来模拟二维筒仓中颗粒介质的应力。垂直坐标起时间的作用,水平坐标起空间的作用。该过程是状态时间为R- {1,R -... N}的离散时间马尔可夫过程。在每个层(时间),每个谷物所支持的权重是均值(其自身的权重)的随机变量加上!所支持的权重的随机分数之和。前一层最近的相邻晶粒。赋予连续层右邻的权重分数是[0,1]中的均匀随机变量,与所有事物无关。剩余的权重将分配给左邻居。在边界处,均匀重量的一部分靠在筒仓的壁上。这对应于吸收边界条件。对于该模型,我们表明存在唯一的不变性度量。在不变度量下,第i个站点的平均体重为i(N + 1-i);我们证明其方差为1/2(i(N + 1-i))(2)+ O(N-3),且晶粒i不等于j的协方差为O(N-3)。此外,当N->无穷大时,定律在权重的不变度量下除以r 2围绕位置r(整数部分)的N 2,r是(0,1)的元素,收敛为伽玛分布的乘积参数2和2(r(1-r))(-1)(均值r(1-r)/ 2的两个指数之和)。 Liu et al。((2))证明,对于具有无限多失重晶粒的筒仓,参数为2和2 / p与rho的伽马分布的任何乘积都是[0,无穷大]的元素。我们的结果表明,随着筒仓的增长,模型会在每个宏观位置精确选择这些Gamma之一。 [参考:14]

著录项

相似文献

  • 外文文献
  • 中文文献
  • 专利
获取原文

客服邮箱:kefu@zhangqiaokeyan.com

京公网安备:11010802029741号 ICP备案号:京ICP备15016152号-6 六维联合信息科技 (北京) 有限公司©版权所有
  • 客服微信

  • 服务号