Dynamical analysis of a simple autonomous jerk system with multiple attractors

In recent years, tremendous research efforts have been devoted to simple chaotic oscillators based on jerk equation that involves a third-time derivative of a single variable. In the present paper, we perform a systematic analysis of a simple autonomous jerk system with cubic nonlinearity. The system is a linear transformation of Model MO5 first introduced in Sprott (Elegant chaos: algebraically simple flow. World Scientific Publishing, Singapore, 2010) prior to the more detailed study by Louodop et al. (Nonlinear Dyn 78:597–607, 2014). The basic dynamical properties of the model are investigated including equilibria and stability, phase portraits, frequency spectra, bifurcation diagrams, and Lyapunov exponent plots. It is shown that the onset of chaos is achieved via the classical period-doubling and symmetry-restoring crisis scenarios. One of the key contributions of this work is the finding of a window in the parameter space in which the jerk system experiences the unusual and striking feature of multiple attractors (e.g. coexistence of four disconnected periodic and chaotic attractors). Basins of attraction of various coexisting attractors are computed showing complex basin boundaries. Among the very few cases of lower-dimensional systems (e.g. Newton–Leipnik system) capable of displaying such type of behaviour reported to date, the jerk system with cubic nonlinearity considered in this work represents the simplest and the most ‘elegant’ prototype. An appropriate electronic circuit describing the jerk system is designed and used for the investigations. Results of theoretical analyses are perfectly traced by laboratory experimental measurements.

[1]  Julien Clinton Sprott,et al.  Multistability in a Butterfly Flow , 2013, Int. J. Bifurc. Chaos.

[2]  A. Nayfeh,et al.  Applied nonlinear dynamics : analytical, computational, and experimental methods , 1995 .

[3]  Sergey P. Kuznetsov,et al.  Co-existing hidden attractors in a radio-physical oscillator system , 2015 .

[4]  Michael Small,et al.  On a Dynamical System with Multiple Chaotic attractors , 2007, Int. J. Bifurc. Chaos.

[5]  Julien Clinton Sprott,et al.  Coexisting Hidden Attractors in a 4-D Simplified Lorenz System , 2014, Int. J. Bifurc. Chaos.

[6]  Sajad Jafari,et al.  Three-dimensional chaotic autonomous system with only one stable equilibrium: Analysis, circuit design, parameter estimation, control, synchronization and its fractional-order form , 2014 .

[7]  Julien Clinton Sprott,et al.  Simplest dissipative chaotic flow , 1997 .

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

[9]  Steven H. Strogatz,et al.  Nonlinear Dynamics and Chaos , 2024 .

[10]  A. Wolf,et al.  Determining Lyapunov exponents from a time series , 1985 .

[11]  Masoller Coexistence of attractors in a laser diode with optical feedback from a large external cavity. , 1994, Physical review. A, Atomic, molecular, and optical physics.

[12]  K. Kyamakya,et al.  On the analysis of semiconductor diode-based chaotic and hyperchaotic generators—a case study , 2014 .

[13]  R. Leipnik,et al.  Double strange attractors in rigid body motion with linear feedback control , 1981 .

[14]  Christophe Letellier,et al.  Symmetry groups for 3D dynamical systems , 2007 .

[15]  Julien Clinton Sprott,et al.  A New Chaotic Jerk Circuit , 2011, IEEE Transactions on Circuits and Systems II: Express Briefs.

[16]  Ralf Eichhorn,et al.  Simple polynomial classes of chaotic jerky dynamics , 2002 .

[17]  U. Feudel,et al.  Control of multistability , 2014 .

[18]  Julien Clinton Sprott,et al.  Simple chaotic systems and circuits , 2000 .

[19]  Martin Rosalie,et al.  Systematic template extraction from chaotic attractors: I. Genus-one attractors with an inversion symmetry , 2013 .

[20]  Mohammad Ghasem Mahjani,et al.  Multiple attractors in Koper–Gaspard model of electrochemical periodic and chaotic oscillations , 2010 .

[21]  S. K. Dana,et al.  Extreme multistability: Attractor manipulation and robustness. , 2015, Chaos.

[22]  Martin Rosalie,et al.  Systematic template extraction from chaotic attractors: II. Genus-one attractors with multiple unimodal folding mechanisms , 2015 .

[23]  Julien Clinton Sprott,et al.  Amplitude control approach for chaotic signals , 2013 .

[24]  Vaithianathan Venkatasubramanian,et al.  Coexistence of four different attractors in a fundamental power system model , 1999 .

[25]  J.-M. Malasoma What is the simplest dissipative chaotic jerk equation which is parity invariant , 2000 .

[26]  Shandelle M Henson,et al.  Multiple mixed-type attractors in a competition model , 2007, Journal of biological dynamics.

[27]  Jan Danckaert,et al.  Dissipative chaos, Shilnikov chaos and bursting oscillations in a three-dimensional autonomous system: theory and electronic implementation , 2013 .

[28]  Ranjit Kumar Upadhyay,et al.  Multiple attractors and crisis route to chaos in a model food-chain , 2003 .

[29]  Julien Clinton Sprott,et al.  Precision measurements of a simple chaotic circuit , 2004 .

[30]  F. Busse An exploration of chaos: J. Argyris, G. Faust and M. Haase, Elsevier, Amsterdam, 1994, 722 pp., ISBN 0-444-82002-7 (hardbound), 0-444-82003-5 (paperback) , 1994 .

[31]  Samuel Bowong,et al.  Practical finite-time synchronization of jerk systems: Theory and experiment , 2014, Nonlinear Dynamics.

[32]  Chai Wah Wu,et al.  Chua's oscillator: A compendium of chaotic phenomena , 1994 .

[33]  Julien Clinton Sprott,et al.  Multistability in symmetric chaotic systems , 2015 .

[34]  Jacques Kengne,et al.  Coexistence of Chaos with Hyperchaos, Period-3 Doubling Bifurcation, and Transient Chaos in the Hyperchaotic Oscillator with Gyrators , 2015, Int. J. Bifurc. Chaos.