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1 - Nuclear Sciences and Applications - IAEA

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<strong>IAEA</strong>-CN-50/A-II-2 109<br />

the soft X-rays. It is reasonable to believe, however, that the modes seen in<br />

the plasma during this time are modified from those that would have been<br />

observed in the absence of the plates. Some of the disruption characteristics,<br />

such as the slow growth <strong>and</strong> locking of low frequency modes just prior to the<br />

disruption, appear to be resistive in nature, <strong>and</strong> the separation between the<br />

passive plates <strong>and</strong> the plasma edge must be reduced closer to the design value<br />

of a few cm in order to suppress these "resistive" instabilities.<br />

While the MHD activity at low P has not yet been fully explored <strong>and</strong><br />

controlled, these early results suggest positive benefits of the new geometry to<br />

attain <strong>and</strong> study very high-(3 tokamak plasmas.<br />

After optimization of plasma parameters with large current ramping <strong>and</strong><br />

strong shaping, the future addition of RF techniques shold allow the fine scale<br />

control of the plasma pressure <strong>and</strong> current profiles to optimize access to the<br />

second stability regime.<br />

ACKNOWLEDGEMENT<br />

The authors are pleased to acknowledge discussions with N. Suzuki.<br />

REFERENCES<br />

[1] GREENWALD, M., et ah, Phys. Rev. Lett. 53 (1984) 352.<br />

[2] STRACHAN, J., Phys. Rev. Lett 58 (1987) 1004.<br />

[3] BOL, K., et al., Phys. Rev. Lett. 57 (1986) 1891.<br />

[4] REWOLDT, G., TANG, W.M., HASTIE, R.J., Phys. Fluids 30 (1987) 807.<br />

[5] REWOLDT, G., Princeton Univ., personal communications, 1988.

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