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Variational analysis of topological stationary barotropic MHD in the case of single-valued magnetic surfaces

机译:单值磁表面的情况下拓扑静止的拓扑静止的拓扑静脉分析分析分析

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Variational principles for magnetohydrodynamics have been introduced by previous authors both in Lagrangian and Eulerian form. Yahalom & Lynden-Bell (2008) have previously introduced simpler Eulerian variational principles from which all the relevant equations of barotropic magnetohydrodynamics can be derived. These variational principles were given in terms of six independent functions for non-stationary barotropic flows with given topologies and three independent functions for stationary barotropic flows. This is less then the seven variables which appear in the standard equations of barotropic magnetohydrodynamics which are the magnetic field B the velocity field v and the density p. Later, Yahalom (2010) introduced a simpler variational principle in terms of four functions for non-stationary barotropic magnetohydrodynamics. It was shown that the above variational principles are also relevant for flows of non-trivial topologies and in fact using those variational variables one arrives at additional topological conservation laws in terms of cuts of variables which have close resemblance to the Aharonov-Bohm phase (Yahalom (2013)). In previous examples (Yahalom & Lynden-Bell (2008); Yahalom (2013)) the magnetic field lines with non-trivial topology were at the intersection of two surface one of which was always multivalued; in this paper an example is introduced in which the magnetic helicity is not zero yet both surfaces are single-valued.
机译:磁性流动动力学的变分原理是通过拉格朗日和欧拉形式的先前作者引入的。 yahalom&lynden-bell(2008)以前推出了简单的欧拉变分原理,可以从中获得任何相关的压力学磁力学动力学的相关方程。根据具有给定拓扑和三个独立功能的非平稳的波波波波波波波波波特和静止的管腔流动的三个独立功能来给出这些变分原理。这少于位于波高的磁力流体动力学的标准方程中出现的七个变量,其是磁场B速度场V和密度P。后来,Yahalom(2010)就非静止管道磁力流体动力学的四个功能引入了更简单的变分原理。结果表明,上述变分原理也与非普通拓扑的流量相关,实际上使用这些变分变量在与Aharonov-Bohm阶段相比相似的变量的削减方面到达额外的拓扑保护法(yahalom (2013))。在前面的例子中(Yahalom&Lynden-Bell(2008); Yahalom(2013))具有非琐碎拓扑的磁场线在两个表面的交叉点处总是多值的;在本文中,引入了一个例子,其中磁螺旋不是零的,但两个表面都是单值的。

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