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A Numerical Scheme for Impact Problems II: The Multidimensional Case
69
Citations
9
References
2002
Year
Numerical AnalysisMathematical ProgrammingEngineeringImpact (Mechanics)Structural CrashworthinessImpact LoadingGeometric Singular Perturbation TheoryStructural OptimizationComputational MechanicsImpact Problems IiCalculus Of VariationOperations ResearchNumerical ComputationNumerical SimulationSystems EngineeringHypervelocity ImpactGlobal AnalysisNonlinear Hyperbolic ProblemGeometric Partial Differential EquationGeneralized CoordinatesNumerical SchemeMechanical SystemMultiscale Modeling
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 C3 . 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 $e\in[0,1]$: the mechanically relevant notion of orthogonality is defined in terms of the local metric for the impulsions (local cotangent metric). We define 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.
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