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A numerical scheme for impact problems II: The multidimensional case

机译:冲击问题的数值方案II:多维案例

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摘要

We consider a mechanical system with impact and n degrees of freedom, written in generalized coordinates. The system is not necessarily Lagrangian. The representative point is subject to a constraint: it must stay inside a closed set K with boundary of class C-3. We assume that, at impact, the tangential component of the impulsion is conserved, while its normal coordinate is reflected and multiplied by a given coefficient of restitution e is an element of [0,1] : the mechanically relevant notion of orthogonality is defined in terms of the local metric for the impulsions (local cotangent metric). We de ne a numerical scheme which enables us to approximate the solutions of the Cauchy problem: this is a generalization of the scheme presented in the companion paper [L. Paoli and M. Schatzman, SIAM J. Numer. Anal., 40 (2002), pp. 702-733]. We prove the convergence of this numerical scheme to a solution, which also yields an existence result. Without any a priori estimates, the convergence and the existence are local; with some a priori estimates, the convergence and the existence are proved on intervals depending exclusively on these estimates. The technique of proof uses a localization of the scheme close to the boundary of K; this idea is classical for a differential system studied in the framework of flows of a vector field. It is much more difficult to implement here because finite differences schemes are only approximately local: straightening the boundary creates quadratic terms which cause all the difficulties of the proof. [References: 18]
机译:我们考虑用广义坐标编写的具有冲击力和n个自由度的机械系统。该系统不一定是拉格朗日系统。代表点受到约束:它必须停留在边界为C-3类的封闭集合K内。我们假设在撞击时,脉冲的切向分量是守恒的,而其法向坐标则被反射并乘以给定的恢复系数e是[0,1]的元素:正交的机械相关概念定义为冲量的局部量度(局部余切量度)项。我们定义了一个数值方案,使我们能够近似解决柯西问题的解决方案:这是对伴随论文中提出的方案的概括。 Paoli和M. Schatzman,SIAM J. Numer。 Anal。,40(2002),pp.702-733]。我们证明了该数值方案对一个解的收敛性,这也产生了一个存在的结果。没有任何先验估计,收敛和存在是局部的;借助一些先验估计,仅取决于这些估计,就可以证明其收敛性和存在性。证明技术使用靠近K边界的方案本地化;对于在矢量场流框架中研究的微分系统,该思想是经典的。由于有限差分方案仅是近似局部的,因此在这里实施起来要困难得多:拉直边界会产生二次项,这会引起证明​​的所有困难。 [参考:18]

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