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1 - Nuclear Sciences and Applications - IAEA

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344 DeGRASSIE et al.<br />

CJ<br />

CO<br />

a<br />

23<br />

21<br />

19<br />

APERTURE<br />

229kA<br />

lp = 209 kA<br />

v ;<br />

c ' Y - • ' •• ; •••..•••••••':•-.•*.<br />

0 30 60 90 120 150 180 0 30 60 90 120 150 180<br />

POLOIDAL ANGLE (DEGREE) POLOIDAL ANGLE (DEGREE)<br />

FIG. 3. Mappings of field structure at the two times indicated in Fig. 2. The m = 7/n = 2 isl<strong>and</strong> is<br />

seen to pass by the limiter aperture during the period of increased plasma collection.<br />

This effect is clearly a resonant phenomenon, as expected, in that<br />

the increase occurs only at q values near the resonant q value. (At<br />

q — 3.2 on the limiter front face, q ~ 3.5 at the limiter aperture.) Varying<br />

the limiter radius requires a different Ip to achieve the resonant q as<br />

expected. Reversing the direction of In places an x point on the aperture<br />

rather than the o point for all conditions the same. This reversed<br />

situation gives no observable pressure rise.<br />

Interestingly, the pressure increase is greater in helium discharges<br />

than in hydrogen. Empirically, TEXT has found better particle confinement<br />

time with helium compared to hydrogen, indicating a lower intrinsic<br />

cross-field transport in helium. Any transport mechanism which<br />

moves particles across the field lines competes with the desired RID<br />

particle control.<br />

Measurements with the infrared camera confirm that heat is diverted<br />

off the limiter face in the presence of the magnetic isl<strong>and</strong>. Also,<br />

a fiber optic threaded down the limiter shaft viewing the region inside<br />

the aperture collector shows a significant increase in the ha recycling<br />

h'ght due to the enhanced plasma collection.<br />

Although the pumped limiter enhancements are qualitatively as<br />

predicted, one cannot justify the magnitude given the small isl<strong>and</strong><br />

widths in TEXT. The measured intrinsic cross-field diffusion should<br />

transport an ion across an isl<strong>and</strong> long before it circulates the isl<strong>and</strong><br />

due to motion parallel to the field lines, thus washing out any particle<br />

channeling action. Presently, our working model is that isl<strong>and</strong> induced<br />

perturbations in the electrostatic field cause ions to circulate the isl<strong>and</strong>s<br />

much more rapidly due to the SE X B drift, being independent<br />

of parallel motion <strong>and</strong> transporting impurities as rapidly as the pro-

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