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1 - Nuclear Sciences and Applications - IAEA

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0.20<br />

0.15<br />

0.10<br />

Rp= 2.45 m<br />

a = 0.79 m<br />

BT = 4.7-5.0T<br />

<strong>IAEA</strong>-CN-50/A-I-2 37<br />

0.05<br />

0.5 1.0 1.5<br />

PLASMA CURRENT (MA)<br />

O<br />

L-Mode<br />

Scaling<br />

FIG. 7. Scaling of the energy confinement time with plasma current for discharges with nearly<br />

balanced NBI <strong>and</strong> well-conditioned limiters. Data for lower current (< 1 MA) supershots from 1986 <strong>and</strong><br />

1987 are included. The upper bound of the L-mode region, which encompasses data for all NBIpowers<br />

in the data set, is determined by the lowest power at each current.<br />

comparison for the range of current <strong>and</strong> power in the data set; the upper<br />

boundary corresponds to discharges at 1.6 MA.<br />

The confinement time is shown in Fig. 7 as a function of plasma current.<br />

This data set includes not only the recent data (Fig. 6) but also data from<br />

1986 <strong>and</strong> 1987 to include the lower currents (/p < 1 MA). The constraints<br />

which were applied to the data shown in Fig. 6 were applied here. The<br />

local peak in the confinement time at 0.9 MA reflects the situation in 1986<br />

<strong>and</strong> 1987 when attempts to increase the plasma current resulted in a rapid<br />

degradation of performance. The improvement in conditioning in 1988,<br />

coupled with the higher balanced NBI power, has improved the performance<br />

at 1.4 <strong>and</strong> 1.6 MA (the currents at which experimental running has been<br />

concentrated) to levels comparable to that achieved in the early supershot<br />

experiments. The upper limit to the b<strong>and</strong> representing L-mode data is<br />

calculated for the minimum power included for each current.<br />

The QDD (= PDD/PNBI) for a subset of discharges satisfying the same<br />

constraints on co/counter-injection balance <strong>and</strong> target density is shown in<br />

Fig. 8 as a function of NBI power. As expected on the basis of Fig. 2, QDD<br />

increases strongly with power, but again there is no obvious scaling with<br />

current at each power level. There is a small but significant group of shots<br />

with QDD substantially higher than the envelope of the bulk of the data.<br />

These discharges occur at the lowest extremes of the target density range. It<br />

is possible, therefore, that further improvements in conditioning techniques<br />

will allow reliable access to these exceptional conditions.<br />

2.0

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