H-MODE CONFINEMENT IN JET WITH ENHANCED PERFORMANCE BY PELLET PEAKED DENSITY PROFILES

被引:92
作者
TUBBING, BJD
BALET, B
BARTLETT, DV
CHALLIS, CD
CORTI, S
GILL, RD
GORMEZANO, C
GOWERS, CW
VONHELLERMANN, M
HUGON, M
JACQUINOT, JJ
JAECKEL, H
KUPSCHUS, P
LAWSON, K
MORSI, H
OROURKE, J
PASINI, D
RIMINI, FG
SADLER, G
SCHMIDT, GL
START, DFH
STUBBERFIELD, PM
TANGA, A
TIBONE, F
机构
[1] JET Joint Undertaking Abingdon Oxfordshire, United Kingdom Princeton Plasma Physics Laboratory, Princeton, NJ
关键词
D O I
10.1088/0029-5515/31/5/003
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
The combination of two regimes of enhanced performance, the H-mode and the pellet enhanced performance (PEP) mode, has been achieved in JET. The strong enhancement of the central plasma parameters, obtained with pellet injection and subsequent auxiliary heating, is found to persist well into the H-mode phase. A characteristic of the PEP regime is that an improvement of the fusion reactivity over non-pellet discharges is obtained under the condition of nearly equal electron and ion temperatures. A maximum neutron production rate of 0.95 x 10(16) s-1 was obtained in a double-null X-point discharge with 2.5 MW of neutral beam heating and 9 MW of ion cyclotron resonance heating, with central ion and electron temperatures of about 10 keV and a central deuterium density of 8.0 x 10(19) m-3. The corresponding fusion product n(D)(0)tau-EPSILON-T(i)(0) is between 7.0 and 8.6 x 10(20) m-3.s.keV. The enhanced neutron production is predominantly of thermonuclear (Maxwellian) origin. The compatibility of these regimes is an important issue in the context of tokamak ignition strategies. Several technical developments on JET have played a role in the achievement of this result: (1) the use of low voltage plasma breakdown (0.15 V/m) to permit pellet injection in an X-point configuration before the formation of a q = 1 surface; (2) the elimination of ICRH specific impurities with antenna Faraday screens made of solid beryllium; (3) the use of a novel system of plasma radial position control that stabilizes the coupling resistance of the ion cyclotron heating system.
引用
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页码:839 / 850
页数:12
相关论文
共 49 条
[1]  
BELL MG, 1989, PLASMA PHYS CONTROLL, V1, P27
[2]  
BOSIA G, 1988, FUSION ENG DES, V11, P459
[3]   OBSERVATION OF AN IMPROVED ENERGY-CONFINEMENT REGIME IN NEUTRAL-BEAM-HEATED DIVERTOR DISCHARGES IN THE DIII-D TOKAMAK [J].
BURRELL, KH ;
EJIMA, S ;
SCHISSEL, DP ;
BROOKS, NH ;
CALLIS, RW ;
CARLSTROM, TN ;
COLLERAINE, AP ;
DEBOO, JC ;
FUKUMOTO, H ;
GROEBNER, RJ ;
HILL, DN ;
HONG, RM ;
HOSOGANE, N ;
JACKSON, GL ;
JAHNS, GL ;
JANESCHITZ, G ;
KELLMAN, AG ;
KIM, J ;
LAO, LL ;
LEE, P ;
LOHR, JM ;
LUXON, JL ;
MAHDAVI, MA ;
MOELLER, CP ;
OHYABU, N ;
OSBORNE, TH ;
OVERSKEI, D ;
PETERSEN, PI ;
PETRIE, TW ;
PHILLIPS, JC ;
PRATER, R ;
SCOVILLE, JT ;
SERAYDARIAN, RP ;
SHIMADA, M ;
SLEAFORD, BW ;
SNIDER, RT ;
STAMBAUGH, RD ;
STAV, RD ;
STJOHN, HE ;
STOCKDALE, R ;
STRAIT, EJ ;
TAYLOR, T ;
TOOKER, JF ;
YAMAGUCHI, S .
PHYSICAL REVIEW LETTERS, 1987, 59 (13) :1432-1435
[4]   CONFINEMENT PHYSICS OF H-MODE DISCHARGES IN DIII-D [J].
BURRELL, KH .
PLASMA PHYSICS AND CONTROLLED FUSION, 1989, 31 (10) :1649-1664
[5]  
BUSH CE, 1991, PLASMA PHYS CONTROLL, V1, P309
[6]  
CHARLTON LA, UNPUB NUCL FUSION
[7]  
CHEETHAM AD, 1987, CONTROLLED FUSIO D 1, V11, P205
[8]  
COPPI B, 1989, PLASMA PHYS CONTROLL, V3, P357
[9]   IMPURITY RELEASE BY ICRF ANTENNAS IN JET [J].
DIPPOLITO, DA ;
MYRA, JR ;
BURES, M ;
STAMP, M ;
JACQUINOT, J .
FUSION ENGINEERING AND DESIGN, 1990, 12 (1-2) :209-216
[10]   ENHANCEMENT OF CONFINEMENT IN TOKAMAKS [J].
FURTH, HP .
PLASMA PHYSICS AND CONTROLLED FUSION, 1986, 28 (9A) :1305-1317