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Reducible and irreducible forms of stabilised gradient elasticity in dynamics

机译:动力学中稳定梯度弹性的可还原形式和不可还原形式

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The continualisation of discrete particle models has been a popular tool to formulate higher-order gradient elasticity models. However, a straightforward continualisation leads to unstable continuum models. Padé approximations can be used to stabilise the model, but the resulting formulation depends on the particular equation that is transformed with the Padé approximation. In this contribution, we study two different stabilised gradient elasticity models; one is an irreducible form with displacement degrees of freedom only, and the other is a reducible form where the primary unknowns are not only displacements but also the Cauchy stresses — this turns out to be Eringen’s theory of gradient elasticity. Although they are derived from the same discrete model, there are significant differences in variationally consistent boundary conditions and resulting finite element implementations, with implications for the capability (or otherwise) to suppress crack tip singularities.
机译:离散粒子模型的连续化已经成为制定高阶梯度弹性模型的流行工具。但是,直接连续化会导致不稳定的连续模型。可以使用Padé逼近来稳定模型,但是得出的公式取决于使用Padé逼近转换的特定方程式。在这项贡献中,我们研究了两种不同的稳定梯度弹性模型;一种是仅具有位移自由度的不可约形式,另一种是可约形式,其中主要未知数不仅是位移,还包括柯西应力—这就是艾林根的梯度弹性理论。尽管它们来自相同的离散模型,但在变化一致的边界条件和所得的有限元实现方面存在显着差异,这对(或以其他方式)抑制裂纹尖端奇异性的能力产生了影响。

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