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<strong>IAEA</strong>-CN-50/E-I-2 539<br />

The ELM-free period is characterized by improved confinement of<br />

electron heat as well as density. Figure 7 shows profiles of electron temperature<br />

for the ohmic, NBI L-mode, NBI plus ECH H-mode, <strong>and</strong> ELM-free<br />

H-mode phases of the discharge of Fig. 5. These profiles show that the<br />

effect of ELMs is not just on the density, but that by suppression of ELMs<br />

the electron temperature may be increased. If the ECH is not being absorbed<br />

near the plasma center, as expected during the ELM-free period,<br />

improvement in confinement of electron heat near the center of the plasma<br />

is even greater.<br />

ACKNOWLEDGEMENT<br />

This work was supported by the U.S. Department of Energy under<br />

Contracts DE-AC03-84ER51044 <strong>and</strong> W-7405-ENG-48. The authors<br />

would like to acknowledge outst<strong>and</strong>ing engineering support by D. Bell,<br />

E. Hoffman, <strong>and</strong> A. Nerem.<br />

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(1985) 354.<br />

[2] ALIKAEV, V., et al., Plasma Phys. Control. Fusion 29 (1987) 1285.<br />

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[13] PFEIFFER, W.W., et al., ONETWO: a Computer Code for Modeling Plasma Transport in<br />

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[14] PARK, W., MONTICELLO, D.A., CHU, T.K., Phys. Fluids 30 (1987) 285.<br />

[15] WESTERHOF, E., GOEDHEER, W.J., in Controlled Fusion <strong>and</strong> Plasma Heating (Proc. 13th<br />

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