H. Zushi et al 2003 Nucl. Fusion 43 1600 doi:10.1088/0029-5515/43/12/006
H. Zushi1, S. Itoh1, K. Hanada1, K. Nakamura2, M. Sakamoto1, E. Jotaki1, M. Hasegawa2, Y.D. Pan3, S.V. Kulkarni4, A. Iyomasa1, S. Kawasaki1, H. Nakashima1, N. Yoshida1,2, K. Tokunaga2, T. Fujiwara2, M. Miyamoto5, H. Nakano5, M. Yuno5, A. Murakami5, S. Nakamura5, N. Sakamoto5, K. Shinoda5, S. Yamazoe5, H. Akanishi5, K. Kuramoto5, Y. Matsuo5, A. Iwamae6, T. Fuijimoto6, A. Komori7, T. Morisaki7, H. Suzuki7, S. Masuzaki7, Y. Hirooka7, Y. Nakashima8 and O. Mitarai9
Show affiliationsAn overview of steady state tokamak studies in TRIAM-1M (R0 = 0.8 m, a × b = 0.12 m × 0.18 m and B = 8 T) is presented. The current ramp-up scenario without using centre solenoid coils is reinvestigated with respect to controllability of the current ramp-up rate at the medium density region of (1–2) × 1019 m−3. The plasma is initiated by ECH (fundamental o-mode at 170 GHz with 200 kW) at B = 6.7 T, and the ramp-up rate below the technical limit of 150 kA s−1 for ITER can be achieved by keeping the LH power less than 100 kW during the current ramp-up phase. The physics understanding of the enhanced current drive (ECD) mode around the threshold power level has progressed from a viewpoint of transition probability. A transition frequency, ftrans, for the ECD transition is determined as a function of PCD. At ~70 kW no transition occurs for an ftrans value of ~0.017 Hz, meaning almost zero transition probability. With increasing PCD > Pth, ftrans increases up to 10 Hz, and the transition tends to occur with high probability. The record value of the discharge duration is updated to 3 h 10 min in a low
and low power (<10 kW) discharge. The global particle balance in long duration discharges is investigated, and the temporal change in wall pumping rate is determined. Although the density was low, the gas supply had to be stopped at 30 min after the plasma initiation to maintain the density constant. After that the density was sustained by the recycling flux alone until the end of the discharges. In addition to the recycling problem, in the high power and high density experiments, the localized PWI affects the SSO of the tokamak plasma. The effects of enhanced influx of metal impurities (Fe, Cr, Ni, Mo) on sustainment of the high performance ECD plasma are investigated. In order to evaluate the helium bombarding effects on the plasma facing component and hydrogen recycling in the future burning plasma, microscopic damage of metals exposed to long duration helium discharges was studied. The total exposure time was 128 s. From thermal desorption experiments for the specimens the amount of retained helium was evaluated as 3.9 × 1020 He m−2 and the scale length to be ~1 mm in the SOL.
52.55.Fa Tokamaks, spherical tokamaks
52.40.Hf Plasma-material interactions; boundary layer effects
52.55.Wq Current drive; helicity injection
52.50.Sw Plasma heating by microwaves; ECR, LH, collisional heating
Issue 12 (December 2003)
Received 25 November 2002, accepted for publication 13 November 2003
Published 1 December 2003
H. Zushi et al 2003 Nucl. Fusion 43 1600
Jonah Busch et al 2009 Environ. Res. Lett. 4 044006
Uma P. Vijh et al 2004 ApJ 606 L65
K. Sugitani et al. 2000 The Astronomical Journal 119 323
J Ancsin 1996 Metrologia 33 117
M. A. P. Torres et al. 2008 ApJ 672 1079
Ignasi Ribas et al. 2005 ApJ 622 680
Mohammad A Ahad et al 2009 Physiol. Meas. 30 1415
Juri Poutanen et al 2009 ApJ 706 L129
P. Panuzzo et al. 2007 ApJ 656 206