Abstract

The Lie-Poisson Hamiltonian structure of the special-relativistic electromagnetic fluid equations is derived. This Hamiltonian structure provides synthesis and insight leading to new conservation laws and stability conditions for the equilibrium solutions. A corollary of the stability results generalizes Rayleigh's inflectional instability criterion for ideal incompressible fluids to the present case. Another alternative. Hamiltonian formulation of relativistic electromagnetic fluid dynamics is constructed systematically via Lie-algebraic considerations of the Poisson bracket. (In particular, relativistic magnetohydrodynamics emerges naturally from these considerations.) The nonrelativistic limits of these two formulations are also determined and are shown to be regular and to preserve the corresponding Lie-Poisson structures.

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