GTC Simulation of Ideal Ballooning Mode in Tokamak Plasmas

被引：0

作者：

李泽彬 ^{[1
]}

孙国亚 ^{[1
]}

Ihor HOLOD ^{[2
]}

肖湧 ^{[3
]}

张文禄 ^{[4
]}

林志宏 ^{[5
,6
]}

机构：

[1] Department of Physics and Institute of Theoretical Physics and Astrophysics,Xiamen University

[2] Department of Physics and Astronomy,University of California,Irvine,California ,USA

[3] Institute of Fusion Theory and Simulation,Zhejiang University

[4] CAS Key Laboratory of Basic Plasma Physics,University of Science and Technology of China

[5] Department of Physics and Astronomy,University of California

[6] Fusion Simulation Center,Peking

来源：

PlasmaScienceandTechnology | 2013年 / 15卷 / 06期

关键词：

D O I：

暂无

中图分类号：

TL631.24 [];

学科分类号：

摘要：

<正>In the present paper,we first derive the eigenmode equation of the ideal ballooning mode in tokamak plasmas using a gyrokinetic equation.It is shown that the gyrokinetic eigenmode equation can be reduced to the magnetohydrodynamic(MHD) form in the long wavelength limit when kinetic effects are ignored.Then,the global gyrokinetic toroidal code(GTC) is applied for simulations of the edge-localized ideal ballooning modes.The obtained mode structures are compared with the results of ideal MHD simulations.The observed scaling of the linear growth rate with the toroidal mode number is consistent with the ideal MHD theory.The simulation results verify the GTC capability of simulating MHD processes in toroidal plasmas.

引用

页码：499 / 505

页数：7

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