2001
DOI: 10.1103/physreve.64.056217
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Variational approach to a class of nonlinear oscillators with several limit cycles

Abstract: We study limit cycles of nonlinear oscillators described by the equationẍ + νF (ẋ) + x = 0 with F an odd function. Depending on the nonlinearity, this equation may exhibit different number of limit cycles. We show that limit cycles correspond to relative extrema of a certain functional.Analytical results in the limits ν → 0 and ν → ∞ are in agreement with previously known criteria.For intermediate ν numerical determination of the limit cycles can be obtained.

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Cited by 10 publications
(8 citation statements)
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“…A method that gives a sequence of algebraic approximations to the equation of each limit cycle can be found in [10], and a variational method showing that limit cycles correspond to relative extrema of certain functionals is explained in [14]. Here, we are interested in the application of another non-perturbative technique, the homotopy analysis method (HAM), to this problem.…”
Section: Introductionmentioning
confidence: 99%
“…A method that gives a sequence of algebraic approximations to the equation of each limit cycle can be found in [10], and a variational method showing that limit cycles correspond to relative extrema of certain functionals is explained in [14]. Here, we are interested in the application of another non-perturbative technique, the homotopy analysis method (HAM), to this problem.…”
Section: Introductionmentioning
confidence: 99%
“…25,22 Conditions for existence of a limit cycle have been shown in the case of both f and g are functions of position 25 and work exists on determining the numbers and locations of limit cycles. 26,27,28,29,30 Numerous authors have studied stability of Equation 2 as: 1) f and g being functions of position, 25,31,21 which has been generalized for n of this type of equations, 32,33 2) f and g being functions of time only, 34,35 3) f (t, x) = c(t)h(x) and g is a function of time and position, 36 and 4) general forms:ẍ + f (x,ẋ, t) |ẋ| αẋ + g(x) = 0 studied by Andreyev and Yurjeva 37 and a (t)ẍ + b (t) f (x,ẋ) + c (t) g (x) h (ẋ) = e (t, x,ẋ) by Athanassov. 38 A gap exists between existing semi-active vibration models and application of these results.…”
Section: Modeling the Vibration Isolation Problem And Insightsmentioning
confidence: 99%
“…They include numerical integration [27] (see Table I), harmonic balance [28,29], variational analysis [30], the Melnikov method [31], empirical analyis [23], piecewise approximation [32], and bifurcation analysis [33]. Most of the methods (Melnikov, piece-wise approximation, bifurcation, and harmonic balance) are valid only for specific ranges of the strength parameter ε.…”
Section: Introductionmentioning
confidence: 99%
“…(1) have also been employed with success to approximate the amplitude of limit cycles in other Liénard systems where F (x) is an odd polynomial of degree greater than 3. Among these methods are the variational method of Depassier and Mura [30] and the empirical, nonperturbative method of Giacomini and Neukirch [23].…”
Section: Introductionmentioning
confidence: 99%