Finite Element Models for Flexible Cosserat Solids

O. Bauchau, M. Shan
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Abstract

The application of the finite element method to the modeling of Cosserat solids is investigated in detail. In two- and three-dimensional elasticity problems, the nodal unknowns are the components of the displacement vector, which form a linear field. In contrast, when dealing with Cosserat solids, the nodal unknowns form the special Euclidean group SE(3), a nonlinear manifold. This observation has numerous implications on the implementation of the finite element method and raises numerous questions: (1) What is the most suitable representation of this nonlinear manifold? (2) How is it interpolated over one element? (3) How is the associated strain field interpolated? (4) What is the most efficient way to obtain the discrete equations of motion? All these questions are, of course intertwined. This paper shows that reliable schemes are available for the interpolation of the motion and curvature fields. The interpolated fields depend on relative nodal motions only, and hence, are both objective and tensorial. Because these schemes depend on relative nodal motions only, only local parameterization is required, thereby avoiding the occurrence of singularities. For Cosserat solids, it is preferable to perform the discretization operation first, followed by the variation operation. This approach leads to considerable computation efficiency and simplicity.
柔性cosat固体的有限元模型
详细研究了有限元法在Cosserat固体模型中的应用。在二维和三维弹性问题中,节点未知数是位移矢量的分量,它们形成一个线性场。相反,当处理coserat固体时,节点未知数形成特殊的欧几里得群SE(3),一个非线性流形。这一观察结果对有限元方法的实施有许多影响,并提出了许多问题:(1)这种非线性流形的最合适表示是什么?(2)如何在一个元素上插值?(3)如何插值相关的应变场?(4)获得离散运动方程的最有效方法是什么?当然,所有这些问题都是相互交织的。本文给出了运动场和曲率场插值的可靠方案。内插的场只依赖于相对的节点运动,因此,它既是客观的又是张量的。由于这些方案只依赖于相对节点运动,因此只需要局部参数化,从而避免了奇点的出现。对于Cosserat固体,最好先进行离散化操作,然后进行变分操作。这种方法具有相当的计算效率和简单性。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
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