Nambu-bracket for three-dimensional ideal fluid dynamics and magnetohydrodynamics

IF 4.3 3区 材料科学 Q1 ENGINEERING, ELECTRICAL & ELECTRONIC ACS Applied Electronic Materials Pub Date : 2024-02-17 DOI:10.1093/ptep/ptae025
Yasuhide Fukumoto, Rong Zou
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Abstract

The ideal magnetohydrodynamics (MHD) as well as the ideal fluid dynamics is governed by the Hamilton equation with respect to the Lie-Poisson bracket. The Nambu bracket manifestly represents the Lie-Poisson structure in terms of derivative of the Casimir invariants. We construct a compact Nambu-bracket representation for the three-dimensional ideal MHD equations, with use of three Casimirs for the second Hamiltonians, the total entropy and the magnetic and cross helicities, whose coefficients are all constant. The Lie-Poisson bracket induced by this Nambu bracket does not coincide with the original one, but supplemented by terms with an auxiliary variable. The supplemented Lie-Poisson bracket qualifies the cross-helicity as the Casimir. By appealing to Noether’s theorem, we show that the cross-helicity is the integral invariant associated with the particle-relabeling symmetry. Employing the Lagrange label function, as the independent variable in the variational framework, facilitates implementation of the relabeling transformation. By incorporating the divergence symmetry, other known topological invariants are put on the same ground of Noether’s theorem.
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用于三维理想流体动力学和磁流体动力学的 Nambu 支架
理想磁流体动力学(MHD)和理想流体动力学都受关于 Lie-Poisson 方括号的汉密尔顿方程支配。南布括号通过卡西米尔不变式的导数来表示列-泊松结构。我们为三维理想 MHD 方程构建了一个紧凑的南布括号表示法,使用三个卡西米尔来表示第二哈密顿、总熵以及磁螺旋和交叉螺旋,其系数均为常数。这个南布括号所诱导的李-泊松括号并不与原始括号重合,而是由带有辅助变量的项所补充。补充后的李-泊松括号将交叉螺旋限定为卡西米尔。利用诺特定理,我们证明了交叉螺旋是与粒子标记对称性相关的积分不变量。采用拉格朗日标注函数作为变分框架中的自变量,有助于实现重标注变换。通过纳入发散对称性,其他已知拓扑不变式也被置于诺特定理的同一基础之上。
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CiteScore
7.20
自引率
4.30%
发文量
567
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