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首页> 外文期刊>Physical review, E. Statistical physics, plasmas, fluids, and related interdisciplinary topics >Statistical simulations of diffusional coarsening in finite clusters
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Statistical simulations of diffusional coarsening in finite clusters

机译:有限簇中扩散粗化的统计模拟

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The problem of diffusional interactions in a finite-sized cluster of spherical particles is studied. Simulations of diffusional interactions with size distribution and volume fraction V-v, as input parameters, referred to as snapshot (static) simulations, are compared with dynamic (time-dependent) simulation results. The precise size distribution information in the snapshot simulations is obtained on the basis of a perturbation technique proposed recently by Fradkov et al. [Phys. Rev. E 53, 3925 (1996)]. Robust iterative solution schemes for the quasistatic diffusion equation facilitate investigations of coarsening systems comprised of one million particles at ultralow (10(-13)) to moderate (0.25) volume fractions. The objective of carrying out simulations at such low volume fractions is to analyze the first-order volume-fraction-dependent correction to the effective coarsening rate predicted by the Todes, Lifshitz, and Slyozov (TLS) theory at infinite dilution. When volume fraction is considered as an input parameter, the deviation of coarsening rates from that of the infinite dilution limit of TLS varies as (3)root V-nu for a finite cluster and root V-nu (Debye screening) for an infinite system. Accurate numerical investigations of the rollover volume fraction ( V-nu*) above which the (3)root V-nu behavior changes to root V-nu showed that V-nu* varies as n(-2),where n is the number of particles in the spherical cluster. The deviation of coarsening rates from TLS observed from dynamic simulations agrees with that predicted by snapshot simulations for V-nu <0.01. The dynamic results are higher than the snapshot results for V-nu>0.01. The coarsening rate of the average particle can be calculated directly from dynamic simulations and indirectly from snapshot simulations by a perturbation relation. A different type of snapshot-ensemble averaging is suggested on the basis of the functional nature of the individual particle monopole source or sink strengths. Dynamic and snapshot simulations with dipoles were carried out up to a volume fraction of 0.25, and departure from Debye screening behavior was observed. The inclusion of dipole terms affects the deviations noticeably only above a volume fraction of 0.1. [References: 36]
机译:研究了球形颗粒的有限尺寸簇中的扩散相互作用问题。将具有大小分布和体积分数V-v的扩散相互作用的模拟作为输入参数(称为快照(静态)模拟)与动态(时间相关)模拟结果进行比较。快照模拟中的精确尺寸分布信息是基于Fradkov等人最近提出的摄动技术获得的。 [物理E.E.53,3925(1996)]。准静态扩散方程的鲁棒迭代求解方案有助于研究包括一百万个处于超低(10(-13))至中等(0.25)体积分数的颗粒的粗化系统。在如此低的体积分数下进行模拟的目的是分析无限稀释时Todes,Lifshitz和Slyozov(TLS)理论预测的对有效粗化率的一阶体积分数相关校正。当将体积分数作为输入参数时,粗化速率与TLS无限稀释极限的偏差随(3)有限簇的根V-nu和无限系统的根V-nu(德拜筛选)而变化。对(3)根V-nu行为更改为根V-nu的翻转体积分数(V-nu *)的精确数值研究表明,V-nu *随n(-2)变化,其中n是数字球形簇中的粒子数量。动态模拟观察到的与TLS的粗化率偏差与快照模拟预测的V-nu <0.01一致。对于V-nu> 0.01,动态结果高于快照结果。平均粒子的粗化率可以直接从动态模拟计算,也可以通过摄动关系间接从快照模拟计算。根据各个粒子单极子源或宿强度的功能性质,建议使用另一种类型的快照集合平均。使用偶极子进行动态和快照模拟,直到体积分数达到0.25,并且观察到偏离了德拜屏蔽行为。包含偶极子项仅在体积分数大于0.1时才会明显影响偏差。 [参考:36]

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