首页> 外文期刊>International Journal of Modern Physics, C. Physics and Computers >Stability limits of the single relaxation-time advection–diffusion lattice Boltzmann scheme
【24h】

Stability limits of the single relaxation-time advection–diffusion lattice Boltzmann scheme

机译:单一放松时间平流扩散格子Boltzmann计划的稳定性限制

获取原文
获取原文并翻译 | 示例
       

摘要

In many cases, multi-species and/or thermal flows involve large discrepancies between the different diffusion coefficients involved — momentum, heat and species diffusion. In the context of classical passive scalar lattice Boltzmann (LB) simulations, the scheme is quite sensitive to such discrepancies, as relaxation coefficients of the flow and passive scalar fields are tied together through their common lattice spacing and time-step size. This in turn leads to at least one relaxation coefficient, τ being either very close to 0.5 or much larger than unity which, in the case of the former (small relaxation coefficient), has been shown to cause instability. The present work first establishes the stability boundaries of the passive scalar LB method in the sense of von Neumann and as a result shows that the scheme is unconditionally stable, even for τ=0.5, provided that the nondimensional velocity does not exceed a certain threshold. Effects of different parameters such as the distribution function and lattice speed of sound on the stability area are also investigated. It is found that the simulations diverge for small relaxation coefficients regardless of the nondimensional velocity. Numerical applications and a study of the dispersion–dissipation relations show that this behavior is due to numerical noise appearing at high wave numbers and caused by the inconsistent behavior of the dispersion relation along with low dissipation. This numerical noise, known as Gibbs oscillations, can be controlled using spatial filters. Considering that noise is limited to high wave numbers, local filters can be used to control it. In order to stabilize the scheme with minimal impact on the solution even for cases involving high wave number components, a local Total Variation Diminishing (TVD) filter is implemented as an additional step in the classical LB algorithm. Finally, numerical applications show that this filter eliminates the unwanted oscillations while closely reproducing
机译:在许多情况下,多物种和/或热流涉及涉及的不同扩散系数之间的大致差异 - 动量,热和物种扩散。在古典被动标量晶格Boltzmann(LB)模拟的背景下,该方案对这种差异非常敏感,因为流动和被动标量场的放松系数通过它们的常见晶格间隔和时间步长被捆绑在一起。这又导致至少一个松弛系数,τ非常接近0.5或远远大于团结,在前者(小松弛系数)的情况下已经显示出不稳定性。本工作首先在von Neumann的感觉中建立被动标量标题方法的稳定边界,结果表明该方案是无条件稳定的,即使对于τ= 0.5,即使不升级速度不超过一定阈值。还研究了不同参数的影响,例如分布函数和声音速度的稳定区域。结果发现,无论不升级的速度如何,模拟都针对小的松弛系数发散。分散耗散关系的数值应用及其研究表明,这种行为是由于在高波数处出现的数值噪声,并且由色散关系的不一致行为以及低耗散引起。可以使用空间滤波器控制这种称为Gibbs振荡的数值噪声。考虑到噪声限于高波数,本地滤波器可用于控制它。为了使该方案稳定在诸如涉及高波数分量的情况下的溶液的最小影响,局部总变化减少(TVD)滤波器被实现为经典LB算法中的附加步骤。最后,数值应用表明,该过滤器消除了不需要的振荡,同时密切恢复

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