Titlebook: Bifurcation Dynamics of a Damped Parametric Pendulum; Yu Guo,Albert C. J. Luo Book 2020 Springer Nature Switzerland AG 2020

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Diffus verteiltes interstellares Gas,“PD” represent the saddle-node and period-doubling bifurcations, respectively. The symmetric and asymmetric periodic motions are labeled by “S” and “A”, respectively. All bifurcations trees are predicted with varying excitation frequency Ω. Other parameters are chosen as

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2573-3168 derstand the complex world...Even though the parametrically excited pendulum is one of the simplest nonlinear systems, until now, complex motions in such a parametric pendulum cannot be achieved. In this book, the bifurcation dynamics of periodic motions to chaos in a damped, parametrically excited

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Book 2020he complex world...Even though the parametrically excited pendulum is one of the simplest nonlinear systems, until now, complex motions in such a parametric pendulum cannot be achieved. In this book, the bifurcation dynamics of periodic motions to chaos in a damped, parametrically excited pendulum i

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Bifurcation Trees,“PD” represent the saddle-node and period-doubling bifurcations, respectively. The symmetric and asymmetric periodic motions are labeled by “S” and “A”, respectively. All bifurcations trees are predicted with varying excitation frequency Ω. Other parameters are chosen as

BOOR

Harmonic Frequency-Amplitude Characteristics,od. for non-travelable periodic motions. For the travelable period-m motions, the harmonic analysis of periodic node velocities are presented. Because of . the periodic node displacements cannot be used for the harmonic analysis of the periodic motions.

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Introduction,st nonlinear systems. This is because the inherent complex dynamics of the parametrically excited pendulum helps one better understand the complex world. However, until now, complex motions in the parametrical pendulum cannot be achieved yet through the traditional analysis. What are the mechanism a

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