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On the canonical Hamiltonian structure of the drift equations of motion for a charged particle in a magnetic field

R O Dendy1987年Plasma Physics and Controlled FusionIF 2.2出版社

The equations which describe the combined E*B, Del B*B, and curvature drifts, the magnetic gradient force along magnetic field lines, the existence of the first adiabatic invariant, and the rapid cyclotron motion are shown to have a canonical Hamiltonian structure which relates directly to the local spatial coordinates. The use of Poisson brackets leads immediately to the drift kinetic equation, expressed in local spatial coordinates rather than magnetic field coordinates. When the magnetic field geometry is such as to give rise to mirroring, and the second and third adiabatic invariants exist, their physical identification follows at once from the canonical formulation.

日本語訳

磁場勾配に沿った磁力線方向の力、第一断熱不変量の存在、および高速サイクロトロン運動と組み合わせたE×Bドリフト、曲率ドリフト、および∇Bドリフトを記述する方程式は、局所空間座標に直接関連する正準ハミルトン構造を持つことが示される。ポアソン括弧の使用により、磁場座標ではなく局所空間座標で表されたドリフト運動論方程式が直ちに導かれる。磁場の幾何学的形状がミラー効果を生じさせる場合、第二および第三断熱不変量が存在し、その物理的意味は正準形式から直ちに明らかになる。

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