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Stability of dynamical systems

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Zeeman, E. C. (Erik Christopher), 1925- . (1988) Stability of dynamical systems. NONLINEARITY, 1 (1). pp. 115-155. ISSN 0951-7715

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Abstract

A new definition of the stability of ordinary differential equations is proposed as an alternative to structural stability. It is particularly aimed at dissipative nonlinear systems, including those with chaos or strange attractors. The definition is as follows. Given a vector field v on an oriented manifold X, and given epsilon > 0, let u be the steady state of the Fokker-Planck equation for v with epsilon-diffusion. The existence, uniqueness and global attraction of v is proved in the case when Xis compact (in the non-compact case a suitable boundary condition on v is required for the existence of U). Vector fields are defined to be equivalent, or stable, according to whether their steady states are. A similar theory is developed for diffeomorphisms. The new definition has a number of advantages over structural stability. Stable systems are dense, and therefore most strange attractors are stable, including non-hyperbolic ones. The equivalence extends the Thom classification of gradient systems to non-gradient systems. The theory is closely related to applications, because the steady state v is an epsilon-smoothing of the measure on the attractors of the flow of v, and therefore in numerical and physical experiments v can be used to model the data with epsilon-error.

Item Type: Journal Article
Subjects: Q Science > QA Mathematics
Q Science > QC Physics
Journal or Publication Title: NONLINEARITY
Publisher: IOP PUBLISHING LTD
ISSN: 0951-7715
Date: February 1988
Volume: 1
Number: 1
Number of Pages: 41
Page Range: pp. 115-155
Publication Status: Published
URI: http://wrap.warwick.ac.uk/id/eprint/24614

Data sourced from Thomson Reuters' Web of Knowledge

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