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1 - Nuclear Sciences and Applications - IAEA

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1<br />

10"<br />

<strong>IAEA</strong>-CN-50/A-VI1-12<br />

LCFS LCFS<br />

(magnetics) (exper.)<br />

# 15431<br />

20 40 60 80<br />

SOL Distance (mm)<br />

} 3 MA; 3.4 T<br />

OHMIC<br />

ICRH<br />

(12 MW)<br />

100<br />

ICRH<br />

(12 MW)<br />

OHMIC<br />

20 40 60 80 100<br />

SOL Distance (mm)<br />

FIG. 3. Reciprocating probe measurements ofne(r) <strong>and</strong> Tc(r) in one Ohmic <strong>and</strong> one Ohmic + ICRH<br />

discharge of /„ = 3 MA; BT = 3.4 T, PICRH = 12 MW.<br />

telescopes <strong>and</strong> transmitted by means of a quartz optical fibre<br />

(100 m) to spectrometers or detectors equipped with narrow b<strong>and</strong><br />

interference filters. Using atomic constants the influx can be<br />

derived from the spectroscopic line intensities <strong>and</strong> the measured<br />

density <strong>and</strong> temperature profiles. The telescopes observe only a<br />

small part of the interaction area. Usually simultaneous<br />

measurements of hydrogen, impurities <strong>and</strong> continuum (for<br />

are taken [7] .<br />

The ratio of carbon to deuterium influx is also obtained<br />

experimentally from spectroscopy (Fig. 5). In steady state the<br />

local recycling must be close to R=l <strong>and</strong> the deuterium influx<br />

must be equal to the flux onto the surface. The data refer to a<br />

series of discharges where density flat-tops at various values<br />

were obtained after pellet injection. Both calculated <strong>and</strong><br />

spectroscopic results show a decreasing trend with<br />

471

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