Quasi-periodic solutions and homoclinic bifurcation in an impact inverted pendulum

We investigate a nonlinear inverted pendulum impacting between two rigid walls under external periodic excitation. Based on KAM theory, we prove that there are three regions (corresponding to different energies) occupied by quasi-periodic solutions in phase space when the periodic excitation is small. Moreover, the rotational quasi-periodic motion is maintained when the perturbation gets larger. The existence of subharmonic periodic solutions is obtained by the Aubry-Mather theory and the boundedness of all solutions is followed by the fact that there exist abundant invariant tori near infinity. To study the homoclinic bifurcation of this system, we present a numerical method to compute the discontinuous invariant manifolds accurately, which provides a useful tool for the study of invariant manifolds under the effect of impacts.(C) 2022 Elsevier B.V. All rights reserved.

Automated summary

We investigate the impact of a nonlinear inverted pendulum between two rigid walls under external periodic excitation. By applying KAM theory, we demonstrate the existence of three regions in phase space (corresponding to different energies) occupied by quasi-periodic solutions when the periodic excitation is small. Furthermore, we observe that the rotational quasi-periodic motion persists as the perturbation increases. The Aubry-Mather theory is utilized to obtain subharmonic periodic solutions, and the boundedness of all solutions is explained by the presence of abundant invariant tori near infinity. Additionally, we propose a numerical method to accurately compute the discontinuous invariant manifolds, which serves as a useful tool for studying invariant manifolds under the effect of impacts.