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On the origin and nature of finite-amplitude instabilities in physical systems

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R Krechetnikov1 and J E Marsden2

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FAST TRACK COMMUNICATION

Finite-amplitude instabilities are ubiquitous, but their theory and precise definitions require clarification. In this work, we discuss the interrelation of various notions connected with finite-amplitude instabilities and offer a precise context for these phenomena. Then we establish a connection between non-normality of linear operators, energy conservation by nonlinear operators and the existence of finite-amplitude instabilities in finite- and infinite-dimensional dynamical systems, both in the conservative and dissipative cases. Such a connection may at first appear counter-intuitive since it relates intrinsically linear and nonlinear phenomena, but it follows naturally from the properties of linear and nonlinear operators when they appear together in a dynamical system. In particular, the main theorem of this communication proves that non-normality is a necessary condition for a finite-amplitude instability. It is demonstrated that this phenomenon is relevant to a wide class of physical systems with energy-conserving nonlinearities.


PACS

47.10.ad Navier-Stokes equations

47.27.Cn Transition to turbulence

47.20.Ky Nonlinearity (including bifurcation theory)

MSC

76D05 Navier-Stokes equations (See also 35Q30)

76F06 Transition to turbulence

37G05 Normal forms

Subjects

Fluid dynamics

Mathematical physics

Dates

Issue 41 (16 October 2009)

Received 26 May 2009, in final form 10 September 2009

Published 29 September 2009



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