The Hamiltonian structure and Euler-Poincaré formulation of the Vlasov-Maxwell and gyrokinetic systems
arXiv:1301.6066 · doi:10.1063/1.4791664
Abstract
We present a new variational principle for the gyrokinetic system, similar to the Maxwell-Vlasov action presented in Ref. 1. The variational principle is in the Eulerian frame and based on constrained variations of the phase space fluid velocity and particle distribution function. Using a Legendre transform, we explicitly derive the field theoretic Hamiltonian structure of the system. This is carried out with a modified Dirac theory of constraints, which is used to construct meaningful brackets from those obtained directly from Euler-Poincaré theory. Possible applications of these formulations include continuum geometric integration techniques, large-eddy simulation models and Casimir type stability methods. [1] H. Cendra et. al., Journal of Mathematical Physics 39, 3138 (1998)
36 pages, 1 figure
References in corpus (6)
- A general theory for gauge-free lifting
- Multisymplectic formulation of fluid dynamics using the inverse map
- Derivation of reduced two-dimensional fluid models via Dirac's theory of constrained Hamiltonian systems
- Covariant Lagrangian Methods of Relativistic Plasma Theory
- The effect of subfilter-scale physics on regularization models
- A Lagrangian kinetic model for collisionless magnetic reconnection
Cited by in corpus (7)
- Action Principles for Extended MHD Models
- Variational approach to low-frequency kinetic-MHD in the current coupling scheme
- Explicit high-order noncanonical symplectic algorithms for ideal two-fluid systems
- Neutral Vlasov kinetic theory of magnetized plasmas
- Field theory and weak Euler-Lagrange equation for classical particle-field systems
- Koopman wavefunctions and Clebsch variables in Vlasov-Maxwell kinetic theory
- Variational mean-fluctuation splitting and drift-fluid models