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非对称环形区域中无旋转变换的弱拟对称磁场的存在性

Existence of weakly quasisymmetric magnetic fields without rotational transform in asymmetric toroidal domains.

作者信息

Sato Naoki

机构信息

Graduate School of Frontier Sciences, The University of Tokyo, Kashiwa, Chiba, 277-8561, Japan.

出版信息

Sci Rep. 2022 Jul 5;12(1):11322. doi: 10.1038/s41598-022-15594-9.

Abstract

A quasisymmetry is a special symmetry that enhances the ability of a magnetic field to trap charged particles. Quasisymmetric magnetic fields may allow the realization of next generation fusion reactors (stellarators) with superior performance when compared with tokamak designs. Nevertheless, the existence of such magnetic configurations lacks mathematical proof due to the complexity of the governing equations. Here, we prove the existence of weakly quasisymmetric magnetic fields by constructing explicit examples. This result is achieved by a tailored parametrization of both magnetic field and hosting toroidal domain, which are optimized to fulfill quasisymmetry. The obtained solutions hold in a toroidal volume, are smooth, possess nested flux surfaces, are not invariant under continuous Euclidean isometries, have a non-vanishing current, exhibit a vanishing rotational transform, and fit within the framework of anisotropic magnetohydrodynamics. Due to the vanishing rotational transform, these solutions are however not suitable for particle confinement.

摘要

准对称性是一种特殊的对称性,它增强了磁场捕获带电粒子的能力。与托卡马克设计相比,准对称磁场可能使下一代高性能聚变反应堆(仿星器)的实现成为可能。然而,由于控制方程的复杂性,这种磁结构的存在缺乏数学证明。在此,我们通过构造具体例子证明了弱准对称磁场的存在。这一结果是通过对磁场和承载环形域进行定制参数化实现的,这些参数经过优化以满足准对称性。所得到的解存在于一个环形体积内,是光滑的,具有嵌套的磁通面,在连续欧几里得等距变换下不是不变的,具有非零电流,呈现出零旋转变换,并且符合各向异性磁流体动力学的框架。然而,由于旋转变换为零,这些解不适用于粒子约束。

https://cdn.ncbi.nlm.nih.gov/pmc/blobs/6635/9256717/e024a1b42708/41598_2022_15594_Fig1_HTML.jpg

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