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Theory and FE-analysis for structures with large deformation under magnetic loading

机译:磁性载荷下大变形结构的理论与有限元分析

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We introduce and discuss a reduced micropolar continuum theory to simulate structures with large deformations under magnetic loading. Three numerical examples show the motivation of this model and its use in practical applications. The question of how to choose the micropolar material parameters is addressed. We use that a finite strain micropolar model would reduce to classical elasticity in the absence of curvature effects and body couples and for certain parameter ranges. This gives us information about a proper choice of material parameters. Thus, we introduce in fact a nearly classical model, but with the feature to cover large deformations and non-classical types of loading. As in shell theories, our continuum theory treats angular momentum as an explicit complementary principle. Thus, net couples—the typical loading of magnetized bodies in a magnetic field—can be modelled. Note that, in this case, the possibility for nonsymmetric Cauchy stresses is required for equilibrium, unlike classical shell theories. Micropolar theories are not commonly used, by comparison to the Boltzmann continuum. One reason may be that micropolar theories often require greater modelling effort without significant advantage. However, the simplicity of introducing physical effects like magnetic loading compensates those efforts.
机译:我们介绍并讨论了简化的微极连续理论,以模拟在磁载荷下具有大变形的结构。三个数值示例说明了该模型的动机及其在实际应用中的使用。解决了如何选择微极性材料参数的问题。我们认为,在没有曲率效应和体耦合的情况下,对于某些参数范围,有限应变微极性模型将减小为经典弹性。这为我们提供了有关正确选择材料参数的信息。因此,我们实际上引入了一种近乎经典的模型,但具有覆盖大变形和非经典载荷类型的功能。与壳理论一样,我们的连续统理论将角动量视为明确的补充原理。因此,可以模拟净耦合,即磁场中磁化体的典型负载。请注意,在这种情况下,与经典壳理论不同,需要非对称柯西应力来实现平衡。与玻耳兹曼连续体相比,微极理论并不常用。原因之一可能是微极性理论通常需要更多的建模工作而没有明显的优势。但是,引入物理效应(如磁性负载)的简单性弥补了这些努力。

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