Predictive capability of MHD stability limits in high performance DIII-D discharges

被引:37
作者
Turnbull, AD [1 ]
Brennan, DP
Chu, MS
Lao, LL
Ferron, JR
Garofalo, AM
Snyder, PB
Bialek, J
Bogatu, IN
Callen, JD
Chance, MS
Comer, K
Edgell, DH
Galkin, SA
Humphreys, DA
Kim, JS
La Haye, RJ
Luce, TC
Navratil, GA
Okabayashi, M
Osborne, TH
Rice, BW
Strait, EJ
Taylor, TS
Wilson, HR
机构
[1] Gen Atom Co, San Diego, CA 92138 USA
[2] UKAEA, Culham Lab, Abingdon OX14 3DB, Oxon, England
[3] Lawrence Livermore Natl Lab, Livermore, CA USA
[4] Univ Calif San Diego, La Jolla, CA 92093 USA
[5] Princeton Univ, Princeton Plasma Phys Lab, Princeton, NJ 08543 USA
[6] Univ Wisconsin, Madison, WI USA
[7] FARTECH, San Diego, CA USA
[8] Columbia Univ, New York, NY USA
[9] Oak Ridge Inst Sci Educ, Oak Ridge, TN USA
关键词
D O I
10.1088/0029-5515/42/7/315
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
Results from an array of theoretical and computational tools developed to treat the instabilities of most interest for high performance tokamak discharges are described. The theory and experimental diagnostic capabilities have now been developed to the point where detailed predictions can be productively tested so that competing effects can be isolated and either eliminated or confirmed. The linear MHD stability predictions using high quality discharge equilibrium reconstructions are tested against the observations for the principal limiting phenomena in DIII-D: L mode negative central shear (NCS) disruptions, H mode NCS edge instabilities, and tearing and resistive wall modes (RWMs) in long pulse discharges. In the case of predominantly ideal plasma MHD instabilities, agreement between the code predictions and experimentally observed stability limits and thresholds can now be obtained to within several per cent, and the predicted fluctuations and growth rates to within the estimated experimental errors. Edge instabilities can be explained by a new model for edge localized modes as predominantly ideal instabilities with low to intermediate toroidal mode number. Accurate ideal calculations are critical to demonstrating RWM stabilization by plasma rotation, and the ideal eigenfunctions provide a good representation of the RWM structure when the plasma rotation slows. Ideal eigenfunctions can then be used to predict stabilization using active feedback. For non-ideal modes, the agreement in some cases is promising. Delta' calculations, for example, indicate that some discharges are linearly unstable to classical tearing modes, consistent with the observed growth of islands in those discharges. Nevertheless, there is still a great deal of improvement required before the non-ideal predictive capability can routinely approach levels similar to those for the ideal comparisons.
引用
收藏
页码:917 / 932
页数:16
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