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Global gyrokinetic simulations of the H-mode tokamak edge pedestal
被引:21
|作者:
Wan, Weigang
[1
]
Parker, Scott E.
[1
]
Chen, Yang
[1
]
Groebner, Richard J.
[2
]
Yan, Zheng
[3
]
Pankin, Alexei Y.
[4
]
Kruger, Scott E.
[4
]
机构:
[1] Univ Colorado, Dept Phys, Boulder, CO 80309 USA
[2] Gen Atom Co, San Diego, CA 92186 USA
[3] Univ Wisconsin, Madison, WI 53706 USA
[4] Tech X Corp, Boulder, CO 80305 USA
关键词:
REGIME;
PROFILES;
PHYSICS;
D O I:
10.1063/1.4803890
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:
Global gyrokinetic simulations of DIII-D H-mode edge pedestal show two types of instabilities may exist approaching the onset of edge localized modes: an intermediate-n, high frequency mode which we identify as the "kinetic peeling ballooning mode (KPBM)," and a high-n, low frequency mode. Our previous study [W. Wan et al., Phys. Rev. Lett. 109, 185004 (2012)] has shown that when the safety factor profile is flattened around the steep pressure gradient region, the high-n mode is clearly kinetic ballooning mode and becomes the dominant instability. Otherwise, the KPBM dominates. Here, the properties of the two instabilities are studied by varying the density and temperature profiles. It is found that the KPBM is destabilized by density and ion temperature gradient, and the high-n mode is mostly destabilized by electron temperature gradient. Nonlinear simulations with the KPBM saturate at high levels. The equilibrium radial electric field (E-r) reduces the transport. The effect of the parallel equilibrium current is found to be weak. (C) 2013 AIP Publishing LLC.
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