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首页> 外文期刊>Journal of Sound and Vibration >Deformation modes in the finite element absolute nodal coordinate formulation
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Deformation modes in the finite element absolute nodal coordinate formulation

机译:有限元绝对节点坐标公式中的变形模式

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摘要

The objective of this study is to provide interpretation of the deformation modes in the finite element absolute nodal coordinate formulation using several strain definitions. In this finite element formulation, the nodal coordinates consist of absolute position coordinates and gradients that can be used to define a unique rotation and deformation fields within the element as well as at the nodal points. The results obtained in this study clearly show cross-section deformation modes eliminated when the number of the finite element nodal coordinates is systematically and consistently reduced. Using the procedure discussed in this paper one can obtain a reduced order dynamic model, eliminate position vector gradients that introduce high frequencies to the solution of some problems, achieve the continuity of the remaining gradients at the nodal points, and obtain a formulation that automatically satisfies the principle of work and energy. Furthermore, the resulting dynamic model, unlike large rotation finite element formulations, leads to a unique rotation field, and as a consequence, the obtained formulation does not suffer from the problem of coordinate redundancy that characterizes existing large deformation finite element formulations. In order to accurately define strain components that can have easy physical interpretation, a material coordinate system is introduced to define the material element rotation and deformation. Using the material coordinate system, the Timoshenko-Reissner and Euler-Bernoulli beam models can be systematically obtained as special cases of the absolute nodal coordinate formulation beam models. While a constraint approach is used in this study to eliminate the cross-section deformation modes, it is important to point out as mentioned in this paper that lower-order finite elements, some of which already presented in previous investigations, can be efficiently used in thin and stiff structure applications. (c) 2006 Elsevier Ltd. All rights reserved.
机译:这项研究的目的是使用几种应变定义来解释有限元绝对节点坐标公式中的变形模式。在这种有限元公式中,节点坐标由绝对位置坐标和梯度组成,可用于定义元素内以及节点处的唯一旋转场和变形场。在这项研究中获得的结果清楚地表明,当有限元节点坐标的数目被系统且一致地减少时,横截面变形模式被消除。使用本文讨论的过程,可以得到降阶动态模型,消除了将高频引入某些问题的解决方案的位置矢量梯度,实现了节点处其余梯度的连续性,并获得了自动满足要求的公式工作和精力的原则。此外,与大的旋转有限元公式不同,所得的动力学模型导致唯一的旋转场,因此,所获得的公式不存在表征现有大变形有限元公式的坐标冗余问题。为了精确定义可以容易地物理解释的应变分量,引入了材料坐标系来定义材料元素的旋转和变形。使用材料坐标系,可以作为绝对节点坐标公式化梁模型的特殊情况,系统地获得Timoshenko-Reissner和Euler-Bernoulli梁模型。尽管在本研究中使用约束方法消除了截面变形模式,但重要的是要指出,如本文所述,可以有效地使用低阶有限元(其中一些在先前的研究中已经提出)可以有效地用于分析。薄而硬的结构应用。 (c)2006 Elsevier Ltd.保留所有权利。

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