Hamiltonian formulations for perturbed dissipationless plasma equations

Abstract

The Hamiltonian formulations for the perturbed Vlasov-Maxwell equations and the perturbed ideal magnetohydrodynamics (MHD) equations are expressed in terms of the perturbation derivative $\partial \mathcal{F}/\partial \epsilon \equiv [\mathcal{F},\mathcal{S}]$ of an arbitrary functional ${\cal F}[\vbψ]$ of the Vlasov-Maxwell fields $\vbψ = ({\sf f},{\bf E},{\bf B})$ or the ideal MHD fields $\vbψ = (ρ,{\bf u},s,{\bf B})$, which are assumed to depend continuously on the (dimensionless) perturbation parameter $\epsilon$. Here, $[,]$ denotes the functional Poisson bracket for each set of plasma equations and the perturbation {\it action} functional $\mathcal{S}$ is said to generate dynamically accessible perturbations of the plasma fields. The new Hamiltonian perturbation formulation introduces a framework for functional perturbation methods in plasma physics and highlights the crucial roles played by polarization and magnetization in Vlasov-Maxwell and ideal MHD perturbation theories. One application considered in this paper is a formulation of plasma stability that guarantees dynamical accessibility and leads to a natural generalization to higher-order perturbation theory.

arXiv comment15 pages

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Cited by in corpus (3)

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• A Tale of Two Polarization Paradoxes I: the Diamagnetic Polarization Paradox