The improvement in H-mode confinement in the JFT-2M tokamak shows the difference between CO- and counter-neutral beam (CTR-NB) heating. The improvement in the CO is larger than that in the CO + CTR or CTR H-mode. The reason for is considered not to be the effect of the sheared toroidal rotation, , in the core. at the last closed flux surface shows a finite value (about 20-40 and the direction is dependent on the beam injection angle) in a divertor H-mode. The finite toroidal rotation at the edge plays a role in the observed . Since the radial electric field formed by the poloidal rotation is negative, the electric field shear at the edge is increased by the positive electric field of . In contrast, the electric field from is negative, which reduces the electric field shear. Therefore, the difference in the improvement between the CO and CO + CTR H-mode, which comes from the difference in the pedestal height, may be related to the electric field shear at the edge.
[1]
T. Petrie,et al.
Recent VH-mode results on DIII-D
,
1994
.
[2]
Mori,et al.
Density peaking in the JFT-2M tokamak plasma with counter neutral-beam injection.
,
1991,
Physical review letters.
[3]
K. Itoh,et al.
REVIEW ARTICLE: The role of the electric field in confinement
,
1996
.
[4]
Fujita,et al.
Edge electric-field profiles of H-mode plasmas in the JFT-2M tokamak.
,
1990,
Physical review letters.
[5]
David P. Schissel,et al.
ITER H mode confinement database update
,
1994
.
[6]
F. Wagner,et al.
Regime of Improved Confinement and High Beta in Neutral-Beam-Heated Divertor Discharges of the ASDEX Tokamak
,
1982
.