Multiple limit cycles and centers on center manifolds for Lorenz system
Introduction
In this paper, we consider Lorenz system which is taken the following formwhere . It is well-known, since Lorenz found the classical chaotic attractor in 1963, chaos become more and more attractive theoretical subject, especially in the nonlinear science. In the past decades, extensive investigations on chaotic systems have been carried out, particularly, for Lorenz system (see [1], [2], [3], [4], [5] and the references therein). Nevertheless, some dynamics properties of Lorenz system have not been completely understood by mathematicians, for example, the multiple Hopf bifurcation. Usually the single Hopf bifurcations of chaotic systems can be seen in many works, yet for the multiple one there exist only a few papers, as we know, Mello and Coelho [6] for Lü system, Messias et al. [7] for Chua’s system, Wang and Huang [8] for Chen system. Here we investigate this problem of Lorenz system. At the same time, we also discuss the center-focus problem for the flow of Lorenz system restricted to the center manifold, which closely relates to the maximum number of limit cycles bifurcating from the equilibria.
For the center-focus problem on the center manifold of a system in , the authors of [9] fully studied the center-focus determination method in terms of an inverse Jacobi multiplier. The authors of [10], [11] gave respectively the formal series method and the formal first integral method of determining the existence of a center. In addition, about this problem we also see [12], [13]. In our process, mainly the method given by Wang et al. [10] is applied to compute the singular point quantities of the equilibria for Lorenz system, which has been proved to be algebraic equivalent to the corresponding focal values. In contrast to the more usual ones such as Liapunov functions-Poincaré normal form and integral averaging method (see [14]), it is convenient to compute the higher order focal values and solve the center-focus problem of the equilibrium (the more details can be seen in [15]).
The rest of this paper is organized as follows. In Section 2, the corresponding singular point quantities are computed and the center conditions on the center manifold are determined. In Section 3, the multiple Hopf bifurcations at the two symmetrical equilibria for Lorenz system are investigated, six limit cycles from them are obtained, and it is proved at most 6 small limit cycles from them via Hopf bifurcation. The results are not only identical with and complementary to the previous work on Hopf bifurcation in Lorenz system, but also helpful to compare the three related chaotic systems: Lorenz system, Chen system and Lü system.
Section snippets
Singular point quantities and center conditions
In this part, we investigate the singular point quantities of the corresponding equilibria. Evidently, Lorenz system (1) always has the equilibrium . Suppose that holds, for system (1) there exist other two fixed points and . The equations in (1) are invariant under the transformation:which means that if is a solution, then is a solution too. Therefore for the two
Limit cycle bifurcation of Lorenz system
In this section, we apply the focal values obtained in last section to discuss multiple Hopf bifurcation of the equilibria, and demonstrate there exist at least 6 limit cycles. The main idea is that for certain equilibrium, when the first focal values vanish while the mth does not vanish, we can change the parameters slightly to make the equilibrium undergo a generic Hopf bifurcation, and the equilibrium is surrounded by m at most small limit cycles.
Now we investigate whether the first two
Conclusion and discussion
Based on precise symbolic computation of singular point quantities, we have investigated deeply multiple Hopf bifurcation of Lorenz system with , and obtained at most 6 small amplitude limit cycles for the two symmetric equilibria. However, according to the previous work [8], [15], we know that Chen system and L system have respectively 4 at most small limit cycles via Hopf bifurcation for the two symmetric equilibria. Therefore, we conclude that though the three chaotic systems are
Acknowledgments
The authors thank the referees for helpful suggestions of improving the paper. This work was supported by Research Foundation of Hezhou University (No. HZUBS201302), Guangxi Key Laboratory of Trusted Software (No. KX201336) and Nature Science Foundation of Guangxi (No. 2012GXNSFAA053003).
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