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1 - Nuclear Sciences and Applications - IAEA

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584 NOTERDAEME et al.<br />

in the start-up phase of the ICRH, made possible long pulses with ICRH alone at high power. These<br />

experiments allowed the investigation of the plasma evolution on previously inaccessible time-scales. For the<br />

first time, ICRH in the second harmonic hydrogen regime (2 Wcn) <strong>and</strong> repetitive pellet refueling were<br />

successfully combined. The density profiles became peaked (ne(0)/ = 1.75) <strong>and</strong> the confinement time<br />

increased from 50 to 70 ms. H° <strong>and</strong> D° neutral beam healing were added to second harmonic heating. D° neutral<br />

injection occasionally resulted in large density increases, with only slight confinement lime improvement.<br />

Minority heating with D° injection produced similar density increases, but with peaked profiles <strong>and</strong><br />

confinement time improvement. H modes lasting 0.5 s were also obtained with D° neutrdl injection <strong>and</strong> D(H)<br />

minority heating. The ICRH power triggered the transition.<br />

1. INTRODUCTION<br />

Between April 1986 <strong>and</strong> April 1987, ASDEX was modified [1] to allow long pulse<br />

additional heating. The ICRH system was also upgraded : the generators can deliver Pgcn = 2 x<br />

2 MW [2], the two low field side antennas are now water cooled [3], <strong>and</strong> the voltage st<strong>and</strong>-off<br />

of transmission line components has been improved [4].<br />

The actual operating space has to date been extended from Pgen = 2.5 MW [5] to 3 MW<br />

for 0.5 s <strong>and</strong>, at Pgen = 2MW, from a pulse length of 1 s [5] to presently 2 s. The coupled<br />

power (PIC) is estimated to be 0.85 x P Experiments were performed at the second<br />

harmonic frequency of hydrogen (67 MHz) in various H/D mixtures, with <strong>and</strong> without H° or<br />

DO neutral injection <strong>and</strong> at the fundamental frequency (33.5 MHz) in D+ plasmas (npj/np = 10<br />

%) with D° injection. The vessel wall was carbonized <strong>and</strong> the parameters were: R = 1.67 m, a<br />

= 0.4 m, Ip = 380 kA, Bt (at 1.65 m ) = 2.42 T.<br />

In mis paper we report a novel scenario used to couple high power at 2 cH for long<br />

pulses, <strong>and</strong> for the first time results obtained in combination with repetitive pellet refueling.<br />

The confinement in the second harmonic <strong>and</strong> minority heating regimes is analysed. Finally H<br />

mode transitions obtained with ICRH + NI are discussed.<br />

2. BRIEF APPLICATION OF NI AT THE BEGINNING OF THE ICRH PULSE<br />

The turn-on of the ICRH is usually accompanied by a density increase, which leads, at<br />

high power, to a disruption. The effect can be partly alleviated by operation of ICRH in<br />

combination with NI. At a given ICRH power, the density increase is smaller with NI, <strong>and</strong><br />

the maximum RF power that can be coupled increases. However, combination with NI makes<br />

ICRH specific properties st<strong>and</strong> out less clearly. Recent experiments have shown that only a<br />

short NI pulse is required at the beginning of the ICRH pulse. At the turn-off of the Nl-pulse,<br />

the density still increases somewhat, but this density increase (also present without ICRH) is<br />

independent of the ICRH power. The reason for the favourable influence of the NI on the<br />

ICRH is still unclear although a number of explanations have been put forward [6-9].<br />

A further interesting observation [1] was that, after the NI is turned off, the antenna resistance<br />

<strong>and</strong> the reflected power change slowly on a long (Is) time-scale. This could be due to a slowly<br />

changing isotope concentration (the decrease in resistance, with increasing H concentration,<br />

would then indicate that eigenmodes play a role). However, a slow change of boundary<br />

density gradients cannot be excluded.<br />

3. RF HEATING AND PELLET REFUELING<br />

The long ICRH pulse, described above, that can be applied to an OH plasma after an<br />

initial NI pulse, was used to combine ICRH (PjC =1.4 MW; the absorbed power, for ICRH<br />

alone, is about 0.6 of PjC ) <strong>and</strong> pellet refueling (up to 15 pellets, every 67 ms, velocity 600<br />

m/s, mass = 1 x 10 20 D atoms). In contrast to other attempts to heat a pellet refueled plasma,<br />

we started pellet injection during the RF pulse. The resonance layer was located at r = 15 cm<br />

(with q = 1 at r = 13 cm <strong>and</strong> q = 2 at about r = 22 cm). Figure 1 presents some of the<br />

experimental traces on which two phases are clearly observed.

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