The limit cycles in a generalized Rayleigh-Liénard oscillator

Abstract

We compute the cyclicity of open period annuli of the following generalized Rayleigh-Liénard equation \begin{document}$ \ddot{x}+ax+bx^3-(\lambda_1+\lambda_2 x^2+\lambda_3\dot{x}^2+\lambda_4 x^4+\lambda_5\dot{x}^4+\lambda_6 x^6)\dot{x} = 0 $\end{document} and the equivalent planar system $ X_\lambda $, where the coefficients of the perturbation $ \lambda_j $ are independent small parameters and $ a, b $ are fixed nonzero constants. Our main tool is the machinery of the so called higher-order Poincaré-Pontryagin-Melnikov functions (Melnikov functions $ M_n $ for short), combined with the explicit computation of center conditions and the corresponding Bautin ideal.We consider first arbitrary analytic arcs $ \varepsilon \to \lambda(\varepsilon) $ and explicitly compute all possible Melnikov functions $ M_n $ related to the deformation $ X_{ \lambda(\varepsilon)} $. At a second step we obtain exact bounds for the number of the zeros of the Melnikov functions (complete elliptic integrals depending on parameter) in an appropriate complex domain, using a modification of Petrov's method.To deal with the general case of six-parameter deformations $ \lambda \to X_\lambda $, we compute first the related Bautin ideal. To do this we carefully study the Melnikov functions up to order three, and then use Nakayama lemma from Algebraic geometry. The principalization of the Bautin ideal (achieved after a blow up) reduces finally the study of general deformations $ X_{ \lambda } $ to the study of one-parameter deformations $ X_{ \lambda(\varepsilon)} $.