学术文献库

Invariant manifolds play an important role in organizing global dynamical behaviors. For example, it is found that in multi-well conservative systems where the potential energy wells are connected by index-1 saddles, the motion between potential wells is governed by the invariant manifolds of a periodic orbit around the saddle. In two degree of freedom systems, such invariant manifolds appear as cylindrical conduits which are referred to as transition tubes. In this study, we apply the concept of invariant manifolds to study the transition between potential wells in not only conservative systems, but more realistic dissipative systems, by solving respective proper boundary-value problems. The example system considered is a two mode model of the snap-through buckling of a shallow arch. We define the transition region, $\mathcal{T}_h$, as a set of initial conditions of a given initial Hamiltonian energy $h$ with which the trajectories can escape from one potential well to another, which in the example system corresponds to snap-through buckling of a structure. The numerical results reveal that in the conservative system the boundary of the transition region, $\partial \mathcal{T}_h$, is a cylinder, while in the dissipative system, $\partial \mathcal{T}_h$ is an ellipsoid. The algorithms developed in the current research from the perspective of invariant manifold provides a robust theoretical-computational framework to study escape and transition dynamics.