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首页> 外文期刊>International journal of bifurcation and chaos in applied sciences and engineering >Bifurcations and Chaos in the Duffing Equation with Parametric Excitation and Single External Forcing
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Bifurcations and Chaos in the Duffing Equation with Parametric Excitation and Single External Forcing

机译:带有参数激励和单一外部强制的Duffing方程中的分叉和混沌

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摘要

We study the Duffing equation with parametric excitation and single external forcing and obtain abundant dynamical behaviors of bifurcations and chaos. The criteria of chaos of the Duffing equation under periodic perturbation are obtained through the Melnikov method. And the existence of chaos of the averaged system of the Duffing equation under the quasi-periodic perturbation Omega = n omega + epsilon nu (where nu is not rational relative to omega) and n = 1, 2, 4, 6 is shown, but the existence of chaos of averaged system of the Duffing equation cannot be proved when n = 3, 5, 7- 15, whereas the occurrence of chaos in the original system can be shown by numerical simulation. Numerical simulations not only show the correctness of the theoretical analysis but also exhibit some new complex dynamical behaviors, including homoclinic or heteroclinic bifurcation surfaces, bifurcation diagrams, Lyapunov exponent diagrams, phase portraits and Poincare maps. We find a large chaotic region with some solitary period parameter points, a large period and quasi-period region with some solitary chaotic parameter points, period-doubling to chaos and chaos to inverse period-doubling, nondense curvilinear chaotic attractor, nonattracting chaotic motion, nonchaotic attracting set, fragmental chaotic attractors. Almost chaotic motion and almost nonchaotic motion appear through adjusting the parameters of the Duffing system, which can be taken as a strategy of chaotic control or a strategy of chaotic motion to nonchaotic motion.
机译:我们研究了带有参数激励和单一外部强制的Duffing方程,并获得了丰富的分叉和混乱的动态行为。通过Melnikov方法获得了周期性扰动下Duffing方程的混沌标准。在准周期性扰动ωωω+ n omega + epsilon nu(其中nu相对于Omega不合理)和n = 1,2,4,6的情况下,存在的混沌的存在的存在的平均系统的存在的混沌。当N = 3,5,7-15时,不能证明Duffing方程的平均系统的混乱的存在,而原始系统中的混沌发生在数值模拟中可以示出。数值模拟不仅显示了理论分析的正确性,而且还表现出一些新的复杂动态行为,包括同性律或杂循环的分叉表面,分叉图,Lyapunov指数图,相位肖像和庞纳罗地图。我们发现一个具有一些孤独时期参数点的大混沌区域,一个孤立的混乱参数点,混沌和混乱的时期加倍,逆时间加倍,不矛盾的混沌运动,不矛盾的混沌运动, nonchanotic吸引套装,碎片混沌吸引子。几乎混乱的运动和几乎非混沌运动通过调整Duffing系统的参数来看出来,可以作为混沌控制的策略或混沌运动策略到非混沌运动。

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