Generalized Galerkin Variational Integrators
arXiv:math/0508360
Abstract
We introduce generalized Galerkin variational integrators, which are a natural generalization of discrete variational mechanics, whereby the discrete action, as opposed to the discrete Lagrangian, is the fundamental object. This is achieved by approximating the action integral with appropriate choices of a finite-dimensional function space that approximate sections of the configuration bundle and numerical quadrature to approximate the integral. We discuss how this general framework allows us to recover higher-order Galerkin variational integrators, asynchronous variational integrators, and symplectic-energy-momentum integrators. In addition, we will consider function spaces that are not parameterized by field values evaluated at nodal points, which allows the construction of Lie group, multiscale, and pseudospectral variational integrators. The construction of pseudospectral variational integrators is illustrated by applying it to the (linear) Schrodinger equation. G-invariant discrete Lagrangians are constructed in the context of Lie group methods through the use of natural charts and interpolation at the level of the Lie algebra. The reduction of these G-invariant Lagrangians yield a higher-order analogue of discrete Euler-Poincare reduction. By considering nonlinear approximation spaces, spatio-temporally adaptive variational integrators can be introduced as well.
30 pages, 7 figures
Cited by in corpus (10)
- Discrete Routh Reduction
- A Discrete Variational Integrator for Optimal Control Problems on SO(3)
- Variational Integrators for Reduced Magnetohydrodynamics
- Phase-fitted Discrete Lagrangian Integrators
- Energy-preserving Variational Integrators for Forced Lagrangian Systems
- Performance Assessment of Energy-preserving, Adaptive Time-step Variational Integrators
- Optimal Attitude Control of a Rigid Body using Geometrically Exact Computations on SO(3)
- High Order Phase-fitted Discrete Lagrangian Integrators for Orbital Problems
- Geometric structure-preserving optimal control of the rigid body
- Lie Group Variational Integrators for the Full Body Problem