Abstract

We establish sufficient criteria for the existence of a limit cycle in the Liénard system x[over ̇]=y-ɛF(x),y[over ̇]=-x, where F(x) is odd. In their simplest form the criteria lead to the result that, for all finite nonzero ɛ, the amplitude of the limit cycle is less than ρ and 0≤a≤ρ≤u, where F(a)=0 and ∫(0)(u)F(x)dx=0. We take the van der Pol oscillator as a specific example and establish that for all finite, nonzero ɛ, the amplitude of its limit cycle is less than 2.0672, a value whose precision is limited by the capacity of our symbolic computation software package. We show how the criterion for the upper bound can be extended to establish a bound on the amplitude of a limit cycle in systems where F(x) contains both odd and even components. We also show how the criteria can be used to establish bounds for bifurcation sets.

Highlights

  • Oscillatory phenomena occur widely in nature [1] and they arise in engineered systems [2]

  • We show that for α = 0 + α ( α > 0) the system given by Eq (30) has a limit cycle α bounded by 0

  • Let HN∗ (x,y) designate the GN polynomial of degree N in y generated with a nonzero constant of integration k for the integral of dgK,N dx

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Summary

Introduction

Oscillatory phenomena occur widely in nature [1] and they arise in engineered systems [2]. Some of the simplest mathematical descriptions of nonlinear sustained oscillations are based on limit cycles in second-order systems [3]. An area of early research in relation to specific nonlinear systems was the identification of whether limit cycles could occur and, if so, the determination of their amplitude and frequency [4,5,6]. The behavior of coupled systems of nonlinear oscillators has attracted attention, since the development of the Kuramoto model for synchronisation in oscillator ensembles [7]. A recent development in relation to the analysis of oscillatory dynamics which are stable under continuous perturbations includes a generalization of the limit-cycle concept, the “chronotaxic limit cycle” [11]

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