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首页> 外文期刊>Technical physics >Structure of Magnetic Plasma Fluctuations in the Uragan-3M Torsatron at Rare Collision Frequencies
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Structure of Magnetic Plasma Fluctuations in the Uragan-3M Torsatron at Rare Collision Frequencies

机译:在罕见碰撞频率下骨盆-3M躯干磁等离子体波动的结构

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摘要

Fluctuations of the poloidal component of the plasma magnetic field in the frequency range of 0.5-50 kHz are studied in the Uragan-3M (U-3M) torsatron. Hydrogen plasma is produced and heated by RF fields at frequencies close to that of the ion cyclotron. The studies are carried out using a set of 15 magnetic sensors installed in one of the torus cross sections. RF heating provided the plasma with rare collision frequencies and the presence of the bootstrap current. The study is carried out when the maximum amplitude of magnetic fluctuations is observed and their connection with the plasma energy content is noticeable. Two types of vibrations are observed. In the first type, the current structure rotates with a certain frequency mainly in the direction of the rotation of electrons in the magnetic field, and the amplitude varies slowly with time (the rotating structure). For the second type, the spatial structure does not rotate, but its amplitude changes with a certain frequency (the standing structure). The frequencies of fluctuations and rotations are close for structures with a given poloidal wave number. The standing vibration structures with different poloidal wave numbers in this frequency range are correlated. The maximum amplitude of the rotating structures is observed with m = 2, and for the standing structures with m = 3 and reaches the values of 0.3 G in the confinement region. The vibration frequency does not depend on poloidal wave number m for the studied cases; m = 0, 1, 2, 3.
机译:在Uragan-3M(U-3M)躯干中研究了0.5-50kHz频率范围内等离子体磁场的单位磁场的波动。通过靠近离子回旋加速器的频率的RF场产生并加热氢等离子体。使用安装在一个圆环横截面中的一组15磁传感器进行研究。 RF加热提供了较少的碰撞频率的等离子体以及自举电流的存在。当观察到磁波动的最大幅度并且它们与等离子体能量含量的连接是明显的时,执行该研究。观察到两种类型的振动。在第一类型中,电流结构主要旋转,主要频率主要在磁场中电子的旋转方向上,并且幅度随时间(旋转结构)而变化。对于第二种类型,空间结构不旋转,但其幅度随特定频率(常设结构)而变化。波动和旋转的频率接近具有给定针状量波数的结构。具有在该频率范围内具有不同针状波数的站立振动结构是相关的。用M = 2观察旋转结构的最大幅度,并且对于具有M = 3的常设结构,并且达到限制区域中的0.3g的值。振动频率不依赖于研究案例的针状波数M; m = 0,1,2,3。

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  • 来源
    《Technical physics》 |2019年第5期|共9页
  • 作者单位

    Kharkiv Inst Phys &

    Technol Natl Sci Ctr Inst Plasma Phys UA-61108 Kharkov Ukraine;

    Kharkiv Inst Phys &

    Technol Natl Sci Ctr Inst Plasma Phys UA-61108 Kharkov Ukraine;

    Kharkiv Inst Phys &

    Technol Natl Sci Ctr Inst Plasma Phys UA-61108 Kharkov Ukraine;

    Kharkiv Inst Phys &

    Technol Natl Sci Ctr Inst Plasma Phys UA-61108 Kharkov Ukraine;

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  • 正文语种 eng
  • 中图分类 Tb13;
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