Abstract
Given any finite dimensional autonomous first order system of ordinary differential equations and any one step discretization method consistent of order p ≥ 1, the diffeomorphism associated to step size a is the period map of the autonomous system with a certain periodic forcing.The forcing amplitude is of order O(ε p) as ε tends to zero, and the forcing frequency is 1/ε. In this sense, the forcing is rapid. We give a proof of this lemma (from Fiedler and Scheurle [1991]. Also, based on recent work on splitting of separatrices for rapidly forced systems, we discuss consequences concerning the numerical simulation of the long-time behaviour of autonomous systems near homo-clinic orbits. Especially, we want to make the point that discretizing a homoclinic orbit, generically breaks the homoclinic orbit and can lead to chaos. This will be discussed for both Hamiltonian and general systems. Also, upper bounds in terms of ε for the splitting effects are presented. Under appropriate smoothness assumptions, those are of arbitrarily high algebraic order in ε, as ε tends to zero. In particular, in the analytic case, they are exponentially small. A proof of these results is outlined at the end of the paper.
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© 1995 Springer-Verlag New York, Inc.
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Scheurle, J. (1995). Discretization of Autonomous Systems and Rapid Forcing. In: Dumas, H.S., Meyer, K.S., Schmidt, D.S. (eds) Hamiltonian Dynamical Systems. The IMA Volumes in Mathematics and its Applications, vol 63. Springer, New York, NY. https://doi.org/10.1007/978-1-4613-8448-9_22
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DOI: https://doi.org/10.1007/978-1-4613-8448-9_22
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