Spatio-temporal evolution of the H → L back transition

被引:20
作者
Miki, K. [1 ,2 ]
Diamond, P. H. [1 ,3 ]
Schmitz, L. [4 ]
McDonald, D. C. [5 ]
Estrada, T. [6 ]
Guercan, Oe. D. [7 ]
Tynan, G. R. [3 ]
机构
[1] Natl Fus Res Inst, WCI Ctr Fus Theory, Taejon 305333, South Korea
[2] Japan Atom Energy Agcy, Ctr Computat Sci & Syst E, Chiba 2778587, Japan
[3] Univ Calif San Diego, Ctr Momentum Transport & Flow Org, La Jolla, CA 92093 USA
[4] Univ Calif Los Angeles, Los Angeles, CA 90095 USA
[5] Culham Ctr Fus Energy, JET EFDA, Arbingdon, England
[6] Asociac Euratom CIEMAT, Lab Nacl Fus, Madrid, Spain
[7] CNRS, LPP Ecole Polytech, F-75700 Paris, France
基金
英国工程与自然科学研究理事会; 新加坡国家研究基金会;
关键词
D O I
10.1063/1.4812555
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
Since ITER will operate close to threshold and with limited control, the H -> L back transition is a topic important for machine operations as well as physics. Using a reduced mesoscale model [Miki et al., Phys. Plasmas 19, 092306 (2012)], we investigate ELM-free H -> L back transition dynamics in order to isolate transport physics effects. Model studies indicate that turbulence spreading is the key process which triggers the back transition. The transition involves a feedback loop linking turbulence and profiles. The I-phase appears during the back transition following a slow power ramp down, while fast ramp-downs reveal a single burst of zonal flow during the back transition. The I-phase nucleates at the pedestal shoulder, as this is the site of the residual turbulence in H-mode. Hysteresis in the profile gradient scale length is characterized by the Nusselt number, where Nu = chi(i,turb)/chi(i,neo). Relative hysteresis of temperature gradient vs density gradient is sensitive to the pedestal Prandtl number, where Pr-ped = D-ped/chi(i,neo). We expect the H-mode to be somewhat more resilient in density than in temperature. (C) 2013 AIP Publishing LLC.
引用
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页数:9
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