Confinement and stability of DIII-D negative central shear discharges

被引:4
|
作者
Lao, LL
Burrell, KH
Casper, TS
Chan, VS
Chu, MS
Forest, CB
Groebner, RJ
Hinton, FL
Kawano, Y
Lazarus, EA
LinLiu, YR
Mauel, ME
Meyer, WH
Miller, RL
Navratil, GA
Osborne, TH
Rettig, CL
Rewoldt, G
Rice, BW
Stallard, BW
Strait, EJ
Taylor, TS
Tang, WM
Turnbull, AD
Waltz, RE
机构
[1] LAWRENCE LIVERMORE NATL LAB,LIVERMORE,CA
[2] JAPAN ATOM ENERGY RES INST,NAKA,IBARAKI 31101,JAPAN
[3] OAK RIDGE NATL LAB,OAK RIDGE,TN
[4] COLUMBIA UNIV,NEW YORK,NY
[5] UNIV CALIF LOS ANGELES,LOS ANGELES,CA
[6] PRINCETON PLASMA PHYS LAB,PRINCETON,NJ 08543
关键词
D O I
10.1088/0741-3335/38/8/051
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
Negative central magnetic shear (NCS) discharges with beta(N) less than or equal to 4, H less than or equal to 3 and up to 80% of the current non-inductively driven are reproducibly produced in the DIII-D tokamak. Strong peaking of T-i, plasma rotation and, in some cases, n(e) are observed inside the NCS region. Transport analysis shows that the core ion thermal diffusivity is substantially reduced and near the neoclassical value after the formation of the internal transport barrier. The negative central shear is necessary but not sufficient for the formation of this transport barrier. The power required for the formation appears to increase with the toroidal magnetic field. The high performance phase of H-mode NCS discharges often ends with an ELM-like collapse initiated from the edge whereas the L-mode discharges which have a more peaked pressure profile tend to end with a more global n = 1 MHD event.
引用
收藏
页码:1439 / 1443
页数:5
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