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Session 7F - DIII-D: Edge and H-Mode.
ORAL session, Thursday morning, November 14
Vail Room, Adam's Mark

[7F.02] Attainment of High Density in \hboxDIII--D H--mode Plasmas

M.A. Mahdavi, R.J. La Haye, A.W. Leonard, T.W. Petrie, R.D. Stambaugh, W.P. West (General Atomics), R. Maingi, L.R. Baylor, T.C. Jernigan, M.R. Wade, M. Murakami (Oak Ridge National Laboratory), J.G. Watkins (Sandia National Laboratories), J. Cuthbertson (University of California, San Diego)

We report results of experiments designed to identify physical effects that define the tokamak n_e limit. Our results support the postulate that the n_e limit is defined by two generic groups of physical effects, power balance and MHD stability. Power balance limits of the core, boundary, and divertor plasmas result in a n_e limit that increases with heating power P, typically n_e\hbox(max)\propto P^0.5. MHD modes, such as ballooning or neoclassical tearing, limit P from above (through transport) with P_max\propto I_P^2. Thus the n_e limit increases with I_P. With typical H--mode density profiles, divertor and boundary plasmas dominate in the power balance. Using n_e profile control, by divertor pumping and pellet injection, we have increased the \bar n_e relative to the edge values. As a result we have succeeded in increasing the H--mode n_e limit by a factor of two and up to the core radiative limit. Densities up to 1.5 times the Greenwald limit with \tau_E^ \simeq0.9\times\tau_E (JET\slash \hboxDIII--D H--mode) have been obtained.

Part 7 of program listing