simplified lorenz system
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Author(s):  
Mengxin Jin ◽  
Kehui Sun ◽  
Huihai Wang


2021 ◽  
Author(s):  
Mengxin Jin ◽  
Kehui Sun ◽  
Huihai Wang

Abstract In this paper, the complex simplified Lorenz system is proposed. It is the complex extension of the simplified Lorenz system. Dynamics of the proposed system are investigated by theoretical analysis as well as numerical simulation, including bifurcation diagram, Lyapunov exponent spectrum, phase portraits, Poincaré section, and basins of attraction. The results show that the complex simplified Lorenz system has non-trivial circular equilibria and displays abundant and complicated dynamical behaviors. Particularly, the coexistence of infinitely many attractors, i.e., extreme multistability, is discovered in the proposed system. Furthermore, the adaptive complex generalized function projective synchronization between two complex simplified Lorenz systems with unknown parameter is achieved. Based on Lyapunov stability theory, the corresponding adaptive controllers and parameter update law are designed. The numerical simulation results demonstrate the effectiveness and feasibility of the proposed synchronization scheme. It provides a theoretical and experimental basis for the applications of the complex simplified Lorenz system.



2015 ◽  
Vol 25 (06) ◽  
pp. 1550085 ◽  
Author(s):  
Huihai Wang ◽  
Kehui Sun ◽  
Shaobo He

By adopting Adomian decomposition method, the fractional-order simplified Lorenz system is solved and implemented on a digital signal processor (DSP). The Lyapunov exponent (LE) spectra of the system is calculated based on QR-factorization, and it accords well with the corresponding bifurcation diagrams. We analyze the influence of the parameter and the fractional derivative order on the system characteristics by color maximum LE (LEmax) and chaos diagrams. It is found that the smaller the order is, the larger the LEmax is. The iteration step size also affects the lowest order at which the chaos exists. Further, we implement the fractional-order simplified Lorenz system on a DSP platform. The phase portraits generated on DSP are consistent with the results that were obtained by computer simulations. It lays a good foundation for applications of the fractional-order chaotic systems.



2015 ◽  
Vol 259 ◽  
pp. 53-60 ◽  
Author(s):  
Fuchen Zhang ◽  
Yonglu Shu


2014 ◽  
Vol 223 (8) ◽  
pp. 1591-1600 ◽  
Author(s):  
Yan Wang ◽  
Kehui Sun ◽  
Shaobo He ◽  
Huihai Wang


2014 ◽  
Vol 24 (03) ◽  
pp. 1450034 ◽  
Author(s):  
Chunbiao Li ◽  
J. C. Sprott

A new simple four-dimensional equilibrium-free autonomous ODE system is described. The system has seven terms, two quadratic nonlinearities, and only two parameters. Its Jacobian matrix everywhere has rank less than 4. It is hyperchaotic in some regions of parameter space, while in other regions it has an attracting torus that coexists with either a symmetric pair of strange attractors or with a symmetric pair of limit cycles whose basin boundaries have an intricate fractal structure. In other regions of parameter space, it has three coexisting limit cycles and Arnold tongues. Since there are no equilibria, all the attractors are hidden. This combination of features has not been previously reported in any other system, especially one as simple as this.



2014 ◽  
Vol 63 (12) ◽  
pp. 120511
Author(s):  
Ai Xing-Xing ◽  
Sun Ke-Hui ◽  
He Shao-Bo ◽  
Wang Hui-Hai


2012 ◽  
Vol 69 (3) ◽  
pp. 1383-1391 ◽  
Author(s):  
Keihui Sun ◽  
Xuan Liu ◽  
Congxu Zhu ◽  
J. C. Sprott


2010 ◽  
Vol 20 (04) ◽  
pp. 1209-1219 ◽  
Author(s):  
KEHUI SUN ◽  
XIA WANG ◽  
J. C. SPROTT

The dynamics of fractional-order systems have attracted increasing attention in recent years. In this paper, we numerically study the bifurcations and chaotic behaviors in the fractional-order simplified Lorenz system using the time-domain scheme. Chaos does exist in this system for a wide range of fractional orders, both less than and greater than three. Complex dynamics with interesting characteristics are presented by means of phase portraits, bifurcation diagrams and the largest Lyapunov exponent. Both the system parameter and the fractional order can be taken as bifurcation parameters, and the range of existing chaos is different for different parameters. The lowest order we found for this system to yield chaos is 2.62.



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