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An exact conserving algorithm for nonlinear dynamics with rotational DOFs and general hyperelasticity. Part 2: shells

机译:具有旋转自由度和一般超弹性的非线性动力学的精确守恒算法。第2部分:贝壳

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摘要

Following the approach developed for rods in Part 1 of this paper (Pimenta et al. in Comput. Mech. 42:715–732, 2008), this work presents a fully conserving algorithm for the integration of the equations of motion in nonlinear shell dynamics. We begin with a re-parameterization of the rotation field in terms of the so-called Rodrigues rotation vector, allowing for an extremely simple update of the rotational variables within the scheme. The weak form is constructed via non-orthogonal projection, the time-collocation of which ensures exact conservation of momentum and total energy in the absence of external forces. Appealing is the fact that general hyperelastic materials (and not only materials with quadratic potentials) are permitted in a totally consistent way. Spatial discretization is performed using the finite element method and the robust performance of the scheme is demonstrated by means of numerical examples.
机译:遵循本文第1部分(Pimenta et al。in Comput.Mech.42:715-732,2008)中为杆开发的方法,这项工作提出了一种完全保守的算法,用于将运动方程积分到非线性壳动力学中。我们首先根据所谓的Rodrigues旋转矢量对旋转场进行重新参数化,从而可以在方案中非常简单地更新旋转变量。弱形式是通过非正交投影构造的,其时间配置可确保在没有外力的情况下精确保留动量和总能量。令人着迷的事实是,一般超弹性材料(不仅是具有二次电势的材料)以完全一致的方式被允许使用。使用有限元方法进行空间离散化,并通过数值示例证明了该方案的鲁棒性能。

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