具有Van der Pol非线性的新型4d超跳自主混沌系统的动力学与同步

R. Kengne, J. T. Mbé, Janvier Fotsing, A. Mezatio, Francine July Ntsafack Manekeng, R. Tchitnga
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摘要

在文献中,超跳系统以其简单优美的结构和复杂的动力学特性引起了人们的广泛关注。在这项工作中,我们提出了一种新的四维自主超跳系统,其特殊性在于其非线性类型,即Van der Pol非线性。利用时间序列、分岔图、李雅普诺夫指数谱、双参数相图和相图等众所周知的非线性动力学工具对该超跳系统的动力学进行了评估。作为重要的结果,我们确定了系统呈现一种特殊的滞回动力学现象,导致吸引子共存。其次,通过计算哈密顿能量,我们证明后者依赖于新超跳系统的所有变量。在此基础上,基于目标为误差系统状态函数的自适应反演方法,设计了一种新的控制器,用于从t = 30开始对相同的新型超跳混沌系统进行完全混沌同步。同样,基于PSpice(9.2完整版)的详细仿真验证了理论模型的可行性。本工作的重点之一是在PSpice环境下设计这种新的自适应反步控制器,以验证理论和数值同步结果。最后,我们在实验室的实验测量结果与数值和模拟结果吻合得很好。
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Dynamics and synchronization of a novel 4D-hyperjerk autonomous chaotic system with a Van der Pol nonlinearity
Abstract In the literature, hyperjerk systems raised up meaningful interest due to their simple and elegant structure as well as their complex dynamical features. In this work, we propose a novel 4D autonomous hyperjerk system which the particularity resides on the type of its nonlinearity namely the Van der Pol nonlinearity. The dynamics of this hyperjerk system is assessed thanks to the well-known nonlinear dynamic tools such as time series, bifurcation diagrams, Lyapunov exponent spectrum, two-parameter phase diagram, and phase portraits. As important result, it is established that the system presents a particular phenomenon of hysteretic dynamics that leads to the coexistence of attractors. Next, through the calculation of the Hamiltonian energy, we show that this latter depends on all the variables of the novel hyperjerk system. Furthermore, basing on an adaptive backstepping method whose target is a function of the states of the error system, a new controller is designed to carry out from t = 30, complete chaotic synchronization of the identical novel hyperjerk chaotic systems. Likewise, PSpice (9.2 full version) based simulations are presented in detail to confirm the feasibility of the theoretical model. One of the key points of this work is the designing in PSpice environment of this new adaptive backstepping controller to validate both theoretical and numerical synchronization results. Finally, our experimental measurements in the laboratory are in good agreement with the numerical and analog results.
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