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Destabilization of poloidal plasma rotation during electron cyclotron resonance heating in tokamaks

机译:托卡马克中电子回旋加速器共振加热过程中极性等离子体旋转的不稳定

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The poloidal plasma rotation destabilized by electron cyclotron resonance heating (ECRH) is proposed in both collision and banana regions of tokamak plasmas. The poloidal electric field, which results in poloidally inhomogeneous ion accumulation, can be produced by ECRH due to either the resonance localization or the asymmetric rf power deposition. When the ion accumulation rate overwhelms the damping rate of the ion-ion collision on the poloidal plasma rotation, the poloidal plasma rotation will be destabilized. Based on the linearized drift kinetic equation and the fluid equations, including a model term of the density perturbation driven by rf waves, the criterion of the destabilization of the poloidal plasma rotation is analytically derived. It is shown chat the poloidal plasma rotation in tokamaks can be generated by ECRH in the practical rf power level by this manner. (C) 1998 American Institute of Physics. [S1070-664X(98)02307-6] [References: 26]
机译:在托卡马克等离子体的碰撞区和香蕉区中,都提出了通过电子回旋共振加热(ECRH)不稳定的极向等离子体旋转。由于共振局部化或不对称的射频功率沉积,可通过ECRH产生极向电场,从而导致极向离子不均匀积累。当离子积累速率使离子-离子碰撞的阻尼率在极性等离子体旋转上不堪重负时,极性等离子体旋转将变得不稳定。基于线性化的漂移动力学方程和流体方程,包括一个由rf波驱动的密度扰动的模型项,可以解析地推导出极性等离子体旋转失稳的判据。可以看出,通过这种方式,ECRH可以在实际的射频功率水平下产生托卡马克中的极向等离子体旋转。 (C)1998美国物理研究所。 [S1070-664X(98)02307-6] [参考:26]

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