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1 - Nuclear Sciences and Applications - IAEA

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108 OKABAYASHI et al.<br />

-2<br />

1 • • • • • • • • • • '<br />

Time (ms)<br />

FIG. 8. Raw signals from two Mirnov coils showing the change in broadb<strong>and</strong> activity across the<br />

H-mode transition. The top trace is from a Mimov coil on an upper passive plate near the x-point, <strong>and</strong><br />

the lower trace is from a coil situated in the midplane.<br />

mode plasmas must be investigated as the injected power is increased in the<br />

near future.<br />

VI) Summary <strong>and</strong> Conclusions<br />

Even these early results from PBX-M at low- <strong>and</strong> moderate-p have<br />

produced tantalizing suggestions of the effects of the close fitting passive<br />

plates. The overall MHD properties in PBX-M plasmas appear to be improved<br />

from those in PBX in that operation in the present device routinely extends to<br />

such lower q-values at moderate indentations (15%) without strong current<br />

ramps. Other indications of this are the long period sawteeth, seen in PBX-M<br />

without current ramps, while the long period sawteeth seen in PBX could be<br />

produced only with strong current ramps. Additionally, the power threshold to<br />

the H-mode has been reduced by about a factor of two going from PBX to<br />

PBX-M. While currents induced on the passive plates by n = 1 magnetic<br />

perturbations are indeed comparable in strength to those seen by the nearby<br />

Mimov coils, these fluctuations are nevertheless still seen in the plasma core on

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