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A MHD invariant and the confinement regimes in a tokamak

机译:托卡马克中的MHD不变性和约束机制

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Fundamental Lagrangian, frozen-in and topological invariants can be useful to explain systematic connections between plasma parameters. At high plasma temperature the dissipation is small and the robust invariances are manifested. We invoke a frozen-in invariant which is an extension of Ertel's theorem, and connects the vorticity of the large scale motions with the profile of the safety factor and of particle density. Assuming ergodicity of the small scale turbulence we consider the approximative preservation of the invariant for changes of the vorticity in an annular region of finite radial extension (i.e. poloidal rotation). We find that the ionization-induced rotation triggered by a pellet requires a reversed-q profile. In the H-mode, the invariance requires an accumulation of the current density in the rotation layer. Then this becomes a vorticity-current sheet which may explain experimental observations related to the penetration of the resonant magnetic perturbation and the filamentation during the edge localized modes.
机译:基本的拉格朗日,冻结和拓扑不变量可用于解释血浆参数之间的系统联系。在较高的等离子体温度下,耗散很小,并且表现出鲁棒的不变性。我们调用冻结不变式,它是Ertel定理的扩展,并将大尺度运动的涡度与安全系数和粒子密度的分布联系起来。假设小尺度湍流的遍历性,我们考虑了在有限径向延伸的环形区域(即,极向旋转)中涡度变化的不变量的近似保留。我们发现,由颗粒触发的电离诱导的旋转需要反向q轮廓。在H模式下,不变性需要在旋转层中积累电流密度。然后,这成为一个涡流表,可以解释与在边缘局部模式期间谐振磁扰动和细丝化的渗透有关的实验观察。

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