Optimization of DIII-D advanced tokamak discharges with respect to the β limit

Author:

Ferron J. R.1,Casper T. A.2,Doyle E. J.3,Garofalo A. M.4,Gohil P.1,Greenfield C. M.1,Hyatt A. W.1,Jayakumar R. J.2,Kessel C.5,Kim J. Y.6,Luce T. C.1,Makowski M. A.7,Menard J.5,Murakami M.8,Petty C. C.1,Politzer P. A.1,Taylor T. S.1,Wade M. R.8

Affiliation:

1. General Atomics , P.O. Box 85608, San Diego, California 92186-5608

2. Lawrence Livermore National Laboratory , Livermore, California 94550

3. University of California—Los Angeles , Los Angeles, California 90024

4. Columbia University , New York, New York 10027

5. Princeton Plasma Physics Laboratory , Princeton, New Jersey 08543

6. Korea Basic Science Institute , 52 Yeoeundong Yusungku, Daejeon 305-333, Korea

7. Lawrence Livermore National Laboratory , Livermore, California 74550

8. Oak Ridge National Laboratory , Oak Ridge, Tennessee 37831

Abstract

Results are presented from comparisons of modeling and experiment in studies to assess the best choices of safety factor q profile, pressure profile, and discharge shape for high β, steady-state, noninductive advanced tokamak operation in the DIII-D device [J. L. Luxon, Nucl. Fusion 42, 614 (2002)]. These studies are motivated by the need for high qminβN to maximize the self-driven bootstrap current while maintaining high toroidal β to increase fusion gain. Modeling shows that increases in the normalized beta βN stable to ideal, low toroidal mode number (n=1,2), instabilities can be obtained through broadening of the pressure profile and use of a symmetric double-null divertor shape. Experimental results are in agreement with this prediction. The general trend is for qminβN to increase with the minimum q value (qmin) although βN decreases as qmin increases. By broadening the pressure profile, βN≈4 is obtained with qmin≈2. Modeling of equilibria with near 100% bootstrap current indicates that operation with βN≈5 should be possible with a sufficiently broad pressure profile.

Publisher

AIP Publishing

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