非对称约束容器中压力梯度不消失的对称理想磁流平衡

N. Sato
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引用次数: 1

摘要

我们研究了在不对称约束容器中构造具有切向边界条件的满足理想磁流体力学力平衡方程的稳定磁场的可能性,即在连续欧几里得等距(平移、旋转或它们的组合)下不是不变的有界区域。这个问题在下一代聚变反应堆的设计中经常遇到。我们表明,如果放宽容器边界对应于压力等值面的标准假设,这种配置是可能的。我们展示了一个光滑的解决方案,它具有欧几里得对称性,但在不对称椭球域解决了边值问题,同时保持了不消失的压力梯度。这一结果为非对称有界区域中存在规则理想磁流平衡问题提供了一个明确的答案。边值问题的正则非对称解是否存在,仍然是一个悬而未决的问题。
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Symmetric ideal magnetofluidostatic equilibria with nonvanishing pressure gradients in asymmetric confinement vessels
We study the possibility of constructing steady magnetic fields satisfying the force balance equation of ideal magnetohydrodynamics with tangential boundary conditions in asymmetric confinement vessels, i.e. bounded regions that are not invariant under continuous Euclidean isometries (translations, rotations, or their combination). This problem is often encountered in the design of next-generation fusion reactors. We show that such configurations are possible if one relaxes the standard assumption that the vessel boundary corresponds to a pressure isosurface. We exhibit a smooth solution that possesses an Euclidean symmetry and yet solves the boundary value problem in an asymmetric ellipsoidal domain while sustaining a non-vanishing pressure gradient. This result provides a definitive answer to the problem of existence of regular ideal magnetofluidostatic equilibria in asymmetric bounded domains. The question remains open whether regular asymmetric solutions of the boundary value problem exist.
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