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1 - Nuclear Sciences and Applications - IAEA

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280 ASHRAF et al.<br />

Modulation amplitude vs resonance position<br />

30<br />

Phase delay vs resonance position<br />

-30 -20 -10 0 10<br />

rres(cm)<br />

FIG. 3. Amplitude <strong>and</strong> phase of the ion saturation current <strong>and</strong> radial field fluctuations as a function<br />

ofECRH resonance position for second harmonic heating.<br />

5. CONCLUSION<br />

X e J* values deduced from power balance <strong>and</strong> sawtooth propagation are similar<br />

<strong>and</strong> both fall with increasing ne. Modulation experiments give somewhat<br />

higher values of x e j* • There are indications that the effective thermal conductivity<br />

nex e j* rises away from the central regions of the plasma. The<br />

amplitudes <strong>and</strong> delay times of the edge response are consistent with diffusive<br />

energy transport from the power deposition region. Off-diagonal terms<br />

in the transport matrix appear to be small.<br />

REFERENCES<br />

[1] ASHRAF, M., et al., Paper <strong>IAEA</strong>-CN-5O/E-I-3, these Proceedings, Vol. 1.<br />

[2] JAHNS, G.L., et al., Nucl. Fusion 26 (1986) 226.<br />

[3] DELIYANAKIS, N., et al., in Electron Cyclotron Emission <strong>and</strong> Electron Cyclotron Resonance<br />

Heating (Proc. 6th Joint Workshop Oxford, 1987), UKAEA, Culham Lab., Abingdon (1987)<br />

247.

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