REVIEW OF RECENT ADVANCES IN HEATING AND CURRENT DRIVE ON TEXTOR

Citation
Am. Messiaen et al., REVIEW OF RECENT ADVANCES IN HEATING AND CURRENT DRIVE ON TEXTOR, Plasma physics and controlled fusion, 35, 1993, pp. 15-34
Citations number
25
Categorie Soggetti
Phsycs, Fluid & Plasmas
ISSN journal
07413335
Volume
35
Year of publication
1993
Supplement
A
Pages
15 - 34
Database
ISI
SICI code
0741-3335(1993)35:<15:RORAIH>2.0.ZU;2-C
Abstract
Co-injection (DO --> D+) applied to TEXTOR leads to a hot ion node reg ime with enhanced confinement. A synergistic increase of the beam effe cts is observed with the addition of ICRH at omega = 2omega(cD) = omeg a(cH) (H minority heating scenario) resulting, beside other reviewed e ffects, in a significant increase of the ion temperature and of the be am driven current (respectively larger than 30 % and 50 % for the addi tion of an RF power comparable to the NBI one). The large ion heating efficiency of ICRH also remains when ICRH is added to balanced injecti on and the hot ion mode regime remains up to the maximum achieved beta (=2/3 of the Troyan limit with more than 6MW of auxiliary heating). I CRH also leads to the formation of a more 'isotropic' tail. These resu lts are interpreted with the help of a Fokker-Planck code which comput es the beam distribution function in presence of RF and of TRANSP simu lations. The amount of RF absorption by the H minority by the ion beam and die bulk plasma is theoretically evaluated. It is shown that a la rge part of the synergistic effects can be explained by the rise of th e electron temperature due to the minority heating which increases the beam slowing down time and its critical energy. A smaller contributio n to the effects is due to direct coupling of the RF power to the beam (less than 10 % of the total RF absorbed power) and to the decrease o f the plasma toroidal rotation induced by the RF. ICRH has also been a dded to co-injection at omega = 3omega(CD). In this case no minority h eating is present and the RF energy coupling to the beam is one of the dominant effects. It leads to the formation of a very energetic tail of the ion beam with a strong increase of the beam-target neutron reac tivity.