Abstract
The present work deals with the numerical long-time integration of damped Hamiltonian systems. The method that we analyze combines a specific Strang splitting, that separates linear dissipative effects from conservative ones, with an energy-preserving averaged vector field (AVF) integrator for the Hamiltonian subproblem. This construction faithfully reproduces the energy-dissipation structure of the continuous model, its equilibrium points and its natural Lyapunov function. As a consequence of these structural similarities, both the convergence to equilibrium and, more interestingly, the energy decay rate of the continuous dynamical system are recovered at a discrete level. The possibility of replacing the implicit AVF integrator by an explicit Störmer-Verlet one is also discussed, while numerical experiments illustrate and support the theoretical findings.
| Original language | English |
|---|---|
| Pages (from-to) | 3319-3341 |
| Number of pages | 23 |
| Journal | Discrete and Continuous Dynamical Systems |
| Volume | 41 |
| Issue number | 7 |
| DOIs | |
| Publication status | Published - 1 Jul 2021 |
| Externally published | Yes |
Keywords
- Dissipative system
- Lojasiewicz inequality
- Optimization
- Structure-preserving integrator