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On the nature of global plasma oscillations in a tokamak. Part II: Spatial structure and propagation of perturbations observed at the T-10 tokamak

机译:关于托卡马克中整体等离子体振荡的性质。第二部分:T-10托卡马克观测到的空间结构和扰动传播

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Large-scale plasma oscillations (so-called MHD oscillations) observed at the T-10 tokamak are investigated. The central electron cyclotron heating was used to enhance oscillations at the m = 1/1 mode with the goal of determining the internal characteristics of the process. The spatially resolved electron cyclotron emission diagnostics allowed analyzing the propagation characteristics of plasma perturbations. The experiments have revealed that excitation of oscillations in a particular mode occur simultaneously in the entire area located within the corresponding rational magnetic surface. The propagation of plasma perturbations along the torus is found to be inhomogeneous. The electron cyclotron emission diagnostics allowed finding eigen (resonance) frequencies of plasma oscillations from the parameters of their inhomogeneous propagation in the plasma core and comparing them with spectra of oscillations of the magnetic field induced by the plasma current in the edge plasma, which were recorded by magnetic probes. It is established that the frequencies of eigenmodes are independent of the electron temperature, plasma density, and auxiliary heating power. Even spatial harmonics of the principal magnetic surface are observed under strong excitation of oscillations. The rational magnetic surfaces that determine oscillation harmonics retain their position during the entire steady-state phase of the total plasma current in spite of the strong sharpening of the temperature profile due to central heating.
机译:研究了在T-10托卡马克上观察到的大规模等离子体振荡(所谓的MHD振荡)。中央电子回旋加速器加热用于增强m / n = 1/1模式下的振荡,目的是确定过程的内部特性。通过空间分辨的电子回旋加速器诊断,可以分析等离子体扰动的传播特性。实验表明,在特定模式下的振动激发同时发生在位于相应有理磁表面内的整个区域中。发现等离子体扰动沿着圆环的传播是不均匀的。电子回旋加速器发射诊断程序可以从等离子核在等离子核中非均匀传播的参数中找到等离子振荡的本征(共振)频率,并将其与边缘等离子中等离子电流引起的磁场振荡光谱进行比较。通过磁性探针。已经确定本征模的频率与电子温度,等离子体密度和辅助加热功率无关。在强振动激发下,甚至观察到主磁性表面的空间谐波。尽管由于中央加热而使温度曲线急剧变强,但确定振荡谐波的合理磁性表面在总等离子体电流的整个稳态阶段仍保持其位置。

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