Abstract

In this study, we develop the energy-phase method to deal with the high-dimensional non-autonomous nonlinear dynamical systems. Our generalized energy-phase method applies to integrable, two-degree-of freedom non-autonomous resonant Hamiltonian systems. As an example, we investigate the multi-pulse orbits and homoclinic trees for a parametrically excited, simply supported rectangular thin plate of two-mode approximation. In both the Hamiltonian and dissipative case we find homoclinic trees, which describe the repeated bifurcations of multi-pulse solutions, and we present visualizations of these complicated structures.

Highlights

  • IntroductionThe energy-phase method, which was first presented by Haller and Wiggins [1-10], was used to reveal fa milies of mu lti-pulse solutions and predict the parameter region for chaotic motion may occur

  • The energy-phase method, which was first presented by Haller and Wiggins [1-10], was used to reveal fa milies of mu lti-pulse solutions and predict the parameter region for chaotic motion may occur. the energy-phase method has been applied widely to engineering problems, it was used to solve autonomous perturbed Hamiltonian systems

  • We have generalized the energy-phase method to deal with the non-autonomous nonlinear system and derive the explicit formu las of the energydifferent function

Read more

Summary

Introduction

The energy-phase method, which was first presented by Haller and Wiggins [1-10], was used to reveal fa milies of mu lti-pulse solutions and predict the parameter region for chaotic motion may occur. The energy-phase method has been applied widely to engineering problems, it was used to solve autonomous perturbed Hamiltonian systems. It is worth to mention that the energy-phase method has never used in non-autonomous nonlinear dynamical systems. We develop the energy-phase method to deal with non-autonomous nonlinear dynamical systems for the first time. This paper develops the energy-phase method to deal with the high-dimensional non-autonomous nonlinear dynamical systems.

Generalized of the energy-phase method
Equations of motion of the buckled thin plate
The unperturbed dynamics
HPI 2HfI sin 2J cos I0
Conclusion
Full Text
Published version (Free)

Talk to us

Join us for a 30 min session where you can share your feedback and ask us any queries you have

Schedule a call