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Hyperelastic Deformations of Smallest Total Energy

机译:总能量最小的超弹性变形

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Throughout this article X and Y will be nonempty bounded domains in R-n, n >= 2. The term deformation of X subset of R-n onto Y subset of R-n refers to an orientation preserving homeomorphism h : X ->(onto) Y in the Sobolev class W-1,W-1(X, Y) whose inverse f : Y ->(onto) X lies in W-1,W-1(Y, X). The general law of hyperelasticity asserts that there exists an energy integral epsilon(X)[h] = integral(X) E(x, h, Dh) dx such that the elastic deformations have the smallest energy. We assume here that E is conformally coerced and polyconvex. Some additional regularity conditions are also imposed. Under those conditions we establish the existence and global invertibility of the minimizers. The key tools in obtaining an extremal deformation h : X ->(onto) Y, regardless of its boundary values, are the free Lagrangians. Finding suitable free Lagrangians and using them for a specific stored-energy function E is truly a work of art. We have done it here for the so-called total harmonic energy and a pair of annuli in the plane. In fact this challenging problem illustrates rather clearly the strength of the concept of free Lagrangians.
机译:在本文中,X和Y将是Rn中的非空有界域,n> =2。术语Rn的X子集到Rn的Y子集上的变形是指保持同胚性的方向h:X->(在)Sobolev中的Y W-1,W-1(X,Y)类,其逆f:Y->(onto)X位于W-1,W-1(Y,X)中。超弹性的一般定律认为,存在一个能量积分epsilon(X)[h] =积分(X)E(x,h,Dh)dx,从而使弹性变形具有最小的能量。我们在这里假设E是保角强制的和多凸的。还强加了一些其他规则性条件。在这些条件下,我们确定了最小化子的存在性和全局可逆性。无论其边界值如何,获得极值变形h的关键工具都是自由拉格朗日式。找到合适的自由拉格朗日派并将其用于特定的储能函数E确实是一件艺术品。我们在这里针对所谓的总谐波能量和平面中的一对环进行了此操作。实际上,这个具有挑战性的问题非常清楚地说明了自由拉格朗日派概念的力量。

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