Abstract
We study theoretically the global chaotic behavior of the generalized Chen–Wang differential system
where \(a,b \in {\mathbb {R}}\) are parameters and \(b\ne 0\). This polynomial differential system is relevant because is the first polynomial differential system in \({\mathbb {R}}^3\) with two parameters exhibiting chaotic motion without having equilibria. We first show that for \(a>0\) sufficiently small it can exhibit up to three small amplitude periodic solutions that bifurcate from a zero-Hopf equilibrium point located at the origin of coordinates when \(a=0\). We also show that the system exhibits two limit cycles emerging from two classical Hopf bifurcations at the equilibrium points \(({\pm }\sqrt{2a}, 0,0)\), for \(a>0, b=1/2\). We also give a complete description of its dynamics on the Poincaré sphere at infinity by using the Poincaré compactification of a polynomial vector field in \({\mathbb {R}}^3\), and we show that it has no first integrals neither in the class of analytic functions nor in the class of Darboux functions.
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Acknowledgments
The first author is partially supported by the Project FP7-PEOPLE-2012-IRSES Number 316338, a CAPES Grant Number 88881.030454/2013-01 and Projeto Temático FAPESP Number 2014/00304-2. The second author is supported by FCT/Portugal through the Project UID/MAT/04459/2013.
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Oliveira, R., Valls, C. Global dynamical aspects of a generalized Chen–Wang differential system. Nonlinear Dyn 84, 1497–1516 (2016). https://doi.org/10.1007/s11071-015-2584-1
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DOI: https://doi.org/10.1007/s11071-015-2584-1
Keywords
- Hopf bifurcation
- Zero-Hopf bifurcation
- Poincaré compactification
- Invariant algebraic surface
- Analytic first integral
- Chen–Wang system