Recent progress on TRIAM-1M
Authors
Zushi, H
Itoh, S
Sato, KN
Nakamura, K
Sakamoto, M
Hanada, K
Jotaki, E
Makino, K
Pan, YD
Kawasaki, S
Nakashima, H
Citation
H. Zushi et al., Recent progress on TRIAM-1M, NUCL FUSION, 40(6), 2000, pp. 1183-1196
Categorie Soggetti
Physics
Journal title
NUCLEAR FUSION
SICI code
0029-5515(200006)40:6<1183:RPOT>2.0.ZU;2-U
Abstract
A steady state plasma with high performance and high current drive efficien
cy is reported. In 2.45 GHz LHCD plasmas T-i is studied as a function of n(
e) at the edge of the high ion temperature (HIT) window. Different characte
ristic timescales are found for T-i and n(e) to enter the HIT regime and th
e observed hysteresis behaviour of T-i with respect to n(e) is attributed t
o this difference. The electromagnetic emission (<3.5 GHz) is studied in or
der to understand ion heating mechanisms in the HIT regime. The spectrum sh
ows several sidebands whose peak frequencies correspond to the ion plasma f
requency. The spectral narrowing of the width of the sideband shows a clear
correlation with ion heating. In 8.2 GHz LHCD plasmas an enhanced current
drive (ECD) regime where both current drive efficiency eta(CD) (= (n) over
bar(e)I(CD)R(o)/P-LH similar to 1 x 10(19) A m(-2)/W) and energy confinemen
t time tau(E) (similar to 8-10 ms) are simultaneously improved is obtained
at an (n) over bar(e) of 4.3 x 10(13) cm(-3) and B = 7 T under full current
drive conditions. There exists a certain threshold power above which the E
CD transition occurs. A hysteresis of eta(CD) is found around the threshold
power, which is explained by the different characteristic time for the ECD
transition in power rampup and rampdown schemes. Current profile control e
xperiments are performed by using two opposite travelling LHWs. Current com
pensation (Delta I-CD/I-CD < -10%) is clearly seen when the backward (BW) t
ravelling LHW (8.2 GHz) is added to a target plasma whose current is driven
by a forward travelling LHW (8.2 GHz). As the BW wave power is increased,
however, the current tends to flow in the forward direction. The mechanisms
of this non-linear behaviour of the driven current with respect to the BW
wave power are discussed.