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TOWARDS UNIFORMLY Γ-EQUIVALENT THEORIES FOR NONCONVEX DISCRETE SYSTEMS

机译:非凸离散系统的一致Γ等效理论

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In this paper we consider a one-dimensional chain of atoms which interact with their nearest and next-to-nearest neighbours via a Lennard-Jones type potential. We prescribe the positions in the deformed configuration of the first two and the last two atoms of the chain. We are interested in a good approximation of the discrete energy of this system for a large number of atoms, i.e., in the continuum limit. We show that the canonical expansion by Γ-convergence does not provide an accurate approximation of the discrete energy if the boundary conditions for the deformation are close to the threshold between elastic and fracture regimes. This suggests that a uniformly Γ-equivalent approximation of the en ergy should be made, as introduced by Braides and Truskinovsky, to overcome the drawback of the lack of accuracy of the standard Γ-expansion. In this spirit we provide a uniformly Γ-equivalent approximation of the discrete energy at first order, which arises as the Γ-limit of a suitably scaled functional.
机译:在本文中,我们考虑一维原子链,这些原子通过Lennard-Jones型势能与其最近和最接近的邻居相互作用。我们规定了链的前两个原子和后两个原子在变形构型中的位置。我们感兴趣的是对于大量原子,即在连续极限中,该系统的离散能量的良好近似。我们表明,如果形变的边界条件接近弹性和断裂状态之间的阈值,则通过Γ收敛的正则展开式不会提供离散能量的准确近似值。这表明,如Braides和Truskinovsky所介绍的那样,应该对能量进行均等的Γ等效近似,以克服缺乏标准Γ扩展精度的缺点。本着这种精神,我们提供了一阶离散能量的均匀Γ当量近似值,该近似值作为适当缩放的泛函的Γ极限值出现。

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