Energy analysis of Sprott-A system and generation of a new Hamiltonian conservative chaotic system with coexisting hidden attractors

Abstract The paper firstly investigates energy cycle of the Sprott-A system by transforming the Sprott-A system into the Kolmogorov-type system. We found the dynamics of the Sprott-A system are influenced by the change along the energy exchange between the conservative energy and the external supplied energy. And the action of the external supplied torque is the main reason that the Sprott-A system generates chaos. Secondly, based on energy analysis of the Sprott-A system, a new four-dimension (4-D) chaotic system is obtained. The new 4-D chaotic system is a conservative system with a constant Hamiltonian energy. Besides, it is also a no-equilibrium system, this means that the new 4-D chaotic system can exhibit hidden characteristics. Further, the coexisting hidden attractors are found when selecting different initial points. Finally, the new 4-D chaotic system is implemented by FPGA, and the coexisting attractors observed are consistent with those found in numerical analysis, which in experiment verifies the existence of coexisting hidden attractors of the new 4-D chaotic system from physical point of view.

[1]  Qiang Lai,et al.  Coexisting attractors and circuit implementation of a new 4D chaotic system with two equilibria , 2018 .

[2]  Zengqiang Chen,et al.  A new class of Hamiltonian conservative chaotic systems with multistability and design of pseudo-random number generator , 2019, Applied Mathematical Modelling.

[3]  Xiyin Liang,et al.  Mechanical Analysis and Energy Cycle of Chen Chaotic System , 2017 .

[4]  Jiangfeng Zhang,et al.  Energy cycle and bound of Qi chaotic system , 2017 .

[5]  Guoyuan Qi,et al.  Comparing mechanical analysis with generalized-competitive-mode analysis for the plasma chaotic system , 2019, Physics Letters A.

[6]  Junkang Ni,et al.  Multi-scroll hidden attractors in improved Sprott A system , 2016 .

[7]  Hoover Remark on "Some simple chaotic flows" , 1995, Physical review. E, Statistical physics, plasmas, fluids, and related interdisciplinary topics.

[8]  Jacques Kengne,et al.  Dynamical analysis of a simple autonomous jerk system with multiple attractors , 2016 .

[9]  Julien Clinton Sprott,et al.  Some simple chaotic jerk functions , 1997 .

[10]  Zenghui Wang,et al.  Four-dimensional autonomous dynamical systems with conservative flows: two-case study , 2017 .

[11]  Xiyin Liang,et al.  Mechanism and Energy Cycling of the Qi Four-Wing Chaotic System , 2017, Int. J. Bifurc. Chaos.

[12]  Ai-Guo Wu,et al.  Conservative Chaos in a Class of Nonconservative Systems: Theoretical Analysis and Numerical Demonstrations , 2018, Int. J. Bifurc. Chaos.

[13]  Antonello Pasini,et al.  A unified view of Kolmogorov and Lorenz systems , 2000 .

[14]  Hoover,et al.  Canonical dynamics: Equilibrium phase-space distributions. , 1985, Physical review. A, General physics.

[15]  Bocheng Bao,et al.  Hidden extreme multistability in memristive hyperchaotic system , 2017 .

[16]  J. Sprott,et al.  Some simple chaotic flows. , 1994, Physical review. E, Statistical physics, plasmas, fluids, and related interdisciplinary topics.

[17]  Marcelo Messias,et al.  On the formation of hidden chaotic attractors and nested invariant tori in the Sprott A system , 2017 .

[18]  Xiyin Liang,et al.  Force Analysis of Qi Chaotic System , 2016, Int. J. Bifurc. Chaos.

[19]  Binoy Krishna Roy,et al.  Five new 4-D autonomous conservative chaotic systems with various type of non-hyperbolic and lines of equilibria , 2018, Chaos, Solitons & Fractals.

[20]  Licai Liu,et al.  Dynamics and Entropy Analysis for a New 4-D Hyperchaotic System with Coexisting Hidden Attractors , 2019, Entropy.

[21]  Vesely,et al.  Canonical dynamics of the Nosé oscillator: Stability, order, and chaos. , 1986, Physical review. A, General physics.

[22]  Zengqiang Chen,et al.  Mechanics Analysis and Hardware Implementation of a New 3D Chaotic System , 2018, Int. J. Bifurc. Chaos.

[23]  M. Gamal,et al.  Analysis of chaotic and hyperchaotic conservative complex nonlinear systems , 2017 .

[24]  Marcelo Messias,et al.  On the existence of periodic orbits and KAM tori in the Sprott A system: a special case of the Nosé–Hoover oscillator , 2018 .

[25]  Xiao-Song Yang,et al.  A vast amount of various invariant tori in the Nosé-Hoover oscillator. , 2015, Chaos.

[26]  Guoyuan Qi,et al.  Modelings and mechanism analysis underlying both the 4D Euler equations and Hamiltonian conservative chaotic systems , 2018, Nonlinear Dynamics.

[27]  Guoyuan Qi,et al.  Energy cycle of brushless DC motor chaotic system , 2017 .

[28]  Antonello Pasini,et al.  Energy cycle for the Lorenz attractor , 2014 .

[29]  Xiyin Liang,et al.  Mechanical analysis of Qi four-wing chaotic system , 2016 .

[30]  Julien Clinton Sprott,et al.  Recent new examples of hidden attractors , 2015 .