Self-consistent simulation of resistive kink instabilities with runaway electrons

被引:11
|
作者
Liu, Chang [1 ]
Zhao, Chen [1 ]
Jardin, Stephen C. [1 ]
Ferraro, Nathaniel M. [1 ]
Paz-Soldan, Carlos [2 ]
Liu, Yueqiang [3 ]
Lyons, Brendan C. [3 ]
机构
[1] Princeton Plasma Phys Lab, POB 451, Princeton, NJ 08543 USA
[2] Columbia Univ, New York, NY USA
[3] Gen Atom, San Diego, CA USA
关键词
disruption; MHD; runaway electron;
D O I
10.1088/1361-6587/ac2af8
中图分类号
O35 [流体力学]; O53 [等离子体物理学];
学科分类号
070204 ; 080103 ; 080704 ;
摘要
A new fluid model for runaway electron (RE) simulation based on fluid description is introduced and implemented in the magnetohydrodynamics (MHD) code M3D-C1, which includes self-consistent interactions between plasma and REs. The model utilizes the method of characteristics to solve the continuity equation for the RE density with large convection speed, and uses a modified Boris algorithm for pseudo particle pushing. The model was employed to simulate MHD instabilities happening in a RE final loss event in the DIII-D tokamak. Nonlinear simulation reveals that a large fraction of REs get lost to the wall when kink instabilities are excited and form stochastic field lines in the outer region of the plasma. Plasma current converts from RE current to Ohmic current. Given the agreements with experiment on RE loss ratio and mode growing time, the simulation model provides a reliable tool to study macroscopic plasma instabilities in existence of RE current, and can be used to support future studies of RE mitigation strategies in ITER.
引用
收藏
页数:14
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