We study the bounded quadratic systems with either two weak foci or a weak focus of order 2. From the first case we obtain (1,1)-configuration of limit cycles, and in the second case we prove that there is no limit cycle surrounding the weak focus of order 2. Also, we unfold the bounded quadratic sy
Higher Order Bifurcations of Limit Cycles
β Scribed by I.D. Iliev; L.M. Perko
- Publisher
- Elsevier Science
- Year
- 1999
- Tongue
- English
- Weight
- 242 KB
- Volume
- 154
- Category
- Article
- ISSN
- 0022-0396
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β¦ Synopsis
This paper shows that asymmetrically perturbed, symmetric Hamiltonian systems of the form
with analytic * j (=)=O(=), have at most two limit cycles that bifurcate for small ={0 from any period annulus of the unperturbed system. This fact agrees with previous results of Petrov, Dangelmayr and Guckenheimer, and Chicone and Iliev, but shows that the result of three limit cycles for the asymmetrically perturbed, exterior Duffing oscillator, recently obtained by Jebrane and Z 4 o*aΓ dek, is incorrect. The proofs follow by deriving an explicit formula for the kth-order Melnikov function, M k (h), and using a Picard Fuchs analysis to show that, in each case, M k (h) has at most two zeros. Moreover, the method developed in this paper for determining the higher-order Melnikov functions also applies to more general perturbations of these systems.
π SIMILAR VOLUMES
The perturbation-incremental method is applied to the study of stability bifurcations of limit cycles and homoclinic (heteroclinic) bifurcations of strongly non-linear oscillators. The bifurcation parameters can be determined to any desired degree of accuracy.
Bifurcation of limit cycles from the class \(Q_{3}^{N H}\) of quadratic systems possessing centers is investigated. Bifurcation diagrams for various systems in this class are constructed, and are used to locate systems possessing a period annulus whose closure has cyclicity three. "1995 Acidenic Pre