AMApplied Mathematics2152-7385Scientific Research Publishing10.4236/am.2012.37115AM-19865ArticlesPhysics&Mathematics Limit Cycle Bifurcations in a Class of Cubic System near a Nilpotent Center iaoJiang1*Department of Mathematics, Shanghai Maritime University, 1550 Haigang Avenue in New Harbor City, Shanghai 201306, PR China* E-mail:jiaojiang08@yahoo.cn300720120307772777April 25, 2012June 4, 2012 June 11, 2012© Copyright 2014 by authors and Scientific Research Publishing Inc. 2014This work is licensed under the Creative Commons Attribution International License (CC BY). http://creativecommons.org/licenses/by/4.0/

In this paper we deal with a cubic near-Hamiltonian system whose unperturbed system is a simple cubic Hamiltonian system having a nilpotent center. We prove that the system can have 5 limit cycles by using bifurcation theory.

Near-Hamiltonian System; Nilpotent Center; Hopf Bifurcation; Limit Cycle
1. Introduction

In the International Congress of Mathematics held in Paris in 1900, Hilbert made a list of 23 problems. The second part of Hilbert’s 16th problem is still an open and difficult question: to find a upper bound of the number of limit cycles and their relative locations in polynomial vector fields of order n.

If the singular point of the system is a non-saddle, nor nilpotent, the related Hopf bifurcations are elementary, see [1-3] and their references. Hopf bifurcations from the elementary focus type of singularities have found broad and important applications in biology, chemistry and physics and engineering, see [4-7] for examples. Yet for the bifurcation of limit cycles from a non-elementary center in a more general planar vector field, its intrinsic dynamics is still far away from understanding due to the complexity and technical difficulties in dealing with such bifurcations.

Then it was natural to restrict the study of the nilpotent center by assuming the system is a perturbation of a Hamiltonian system. Consider the following system

where , and are functions, is small and with D a compact set.

When , system (1.1) becomes

which is Hamiltonian system. Now suppose that the Hamiltonian system (1.2) has a nilpotent center at the origin, namely the function H satisfies the following conditions:

(H1) is a function, satisfying ;

(H2) , the equation defines a closed curve Lh surrounding the origin and Lh approaches the origin as h goes to zero;

(H3) , .

It follows that the expansion of H at the origin has the form Assume that the equation intersects the positive x-axis at . Let denote the first intersection point of the positive orbit of (1.1) starting at with the positive x-axis. Then, we have

where

The Abelian integral M above is called the first order Melnikov function of system (1.1). From Han , we have a general theorem as follows.

Theorem 1.1. Suppose that the origin is nilpotent singular point and that approaches the origin as h goes to zero. If there exist an integer and such that and then we have 1) has at most k zeros near for and all near , and k zeros can appear for some near .

2) System (1.1) has at least k limit cycles near the origin for some near .

2. Main Results and Proof

Consider the following near-Hamiltonian system:

where and p and q are cubic polynomials. We can write

Then unperturbed system is a Hamiltonian system with Hamiltonian

system has a nilpotent center at the origin. Let be the closed curve defined by . Then it can be presented as

Assume that the positive solution of the above equation in y is

where and . Then by (2.4) and (2.5) we obtain     By  the negative solution of (2.4) in y satisfies . Thus, two solutions of (2.4) are

On the other hand, the intersection points of Lh and xaxis have the x-coordinates and . Then by (2.2) we can write

where

Here, Introduce

Then, similar to the method of Han  we have

Therefore, in turn by (2.6)-(2.10) we have   Noting that , then similarly we have  In the same way, using , we have Hence, we have where And      Now it is direct that  Here, if let , , , then for some cubic system (2.1) we can obtain the above determinant is not zero, then the function M can have 5 simple zeros in h > 0 near h = 0 for some near . For example, let , , , we obtain from the above formula Here,            then we can obtain

By Theorem 1.1 we have:

Theorem 2.1. The function has at most 5 zeros in near , and for small the cubic system (2.1) can have 5 limit cycles near the origin.

REFERENCESNOTESReferencesA. Andronov, E. Leontovich, I. Gordon and A. Maier, “Theory of Bifurcations of Dynamical Systems on a Plane,” Israel Program for Scientific Translations, Jerusalem, 1971.M. Han, “On Hopf Cyclicity of Planar Systems,” Journal of Mathematical Analysis and Applications, Vol. 245, No. 2, 2000, pp. 404-422. doi:10.1006/jmaa.2000.6758Y. A. Kuznetsov, “Elements of Applied Bifurcation Theory,” Springer-Verlag, New York, 1995.T. Carmon, R. Uzdin, C. Pigier, Z. Musslimani, M. Segev and A. Nepomnyashchy, “Rotating Propeller Solitons,” Physical Review Letters, Vol. 87, No. 14, 2001, p. 143901. doi:10.1103/PhysRevLett.87.143901J. Guckenheimer and P. Holmes, “Non-Linear Oscillations, Dynamical Systems and Bifurcation of Vector Fields,” Springer-Verlag, New York, 1983.B. D. Hassard, N. D. Kazarinoff and Y. H. Wan, “Theory and Applications of Hopf Bifurcation,” Cambridge University Press, Cambridge, 1981.S. Wiggins, “Global Bifurcations and Chaos: Analytical Methods,” Springer-Verlag, New York, 1988.M. Han J. Jiang and H. Zhu, “Limit Cycle Bifurcations in Near-Hamiltonian Systems by Perturbing a Nilpotent Center,” International Journal of Bifurcation and Chaos, Vol. 18, No. 10, 2008, pp. 3013-3027. doi:10.1142/S0218127408022226