时空和任意拉格朗日-欧拉方法在流动计算中的网格移动方法

K. Takizawa, Y. Bazilevs, T. Tezduyar
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引用次数: 9

摘要

在时空法、任意拉格朗日-欧拉法等移动网格方法中,良好的网格移动方法是流动计算的重要组成部分。采用良好的网格移动方法,可以降低流固界面和流固界面发生较大位移时的网格重划分频率,减少流域中对求解精度要求较高的部分的单元畸变,并在网格沿流固界面移动时保持流固界面附近边界层网格的质量。自1990年以来,已经开发出了许多与ST计算方法相结合的良好网格移动方法,从基于雅可比矩阵的网格加筋到基于纤维增强超弹性的网格移动方法,再到无循环累积变形的线弹性网格移动方法。这些方法已用于计算流体-颗粒相互作用、流体-结构相互作用以及更一般的移动边界和界面等许多复杂流动问题。采用ST法和ALE法进行计算。我们提供了这些方法的概述,并提供了执行计算的示例。这是一篇在知识共享署名许可(http://creativecommons.org/licenses/by/4.0/)条款下发布的开放获取文章,该许可允许在任何媒介上不受限制地使用、分发和复制,只要原始作品被适当引用。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
Mesh Moving Methods in Flow Computations with the Space-Time and Arbitrary Lagrangian-Eulerian Methods
A good mesh moving method is an important part of flow computations with moving-mesh methods like the space–time (ST) and Arbitrary Lagrangian–Eulerian (ALE) methods. With a good mesh moving method, we can decrease the remeshing frequency even when the fluid–solid and fluid–fluid interfaces undergo large displacements, decrease the element distortion in parts of the flow domain where we care about the solution accuracy more, and maintain the quality of the boundary layer meshes near the fluid–solid interfaces as the mesh moves to follow those interfaces. Since 1990, quite a few good mesh moving methods have been developed for use with the ST computational methods, from the mesh Jacobian-based stiffening to a mesh moving method based on fiber-reinforced hyperelasticity to a linear-elasticity mesh moving method with no cycle-to-cycle accumulated distortion. These methods have been used in computation of many complex flow problems in the categories of fluid–particle interaction, fluid–structure interaction, and more generally, moving boundaries and interfaces. The computations were with both the ST and ALE methods. We provide an overview of these methods and present examples of the computations performed.This is an Open Access article distributed under the terms of the Creative Commons Attribution License (http://creativecommons.org/licenses/by/4.0/), which permits unrestricted use, distribution, and reproduction in any medium provided the original work is properly cited. 
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