(This paper was rapporteured in lecture TH1/7)
B. N. Rogers , J. F. Drake
Institute for Plasma Research, University of Maryland, College
Park, MD 20742, USA
A. Zeiler
Max-Planck-Institut für Plasmaphysik, EURATOM Association,
85748 Garching, Germany
Abstract
Based on three-dimensional simulations of the Braginskii equations ,
we identify two main parameters which control transport in the edge of
tokamaks: the MHD ballooning parameter and a diamagnetic parameter. The space
defined by these parameters delineates regions where typical L-mode levels of
transport arise, where the transport is catastrophically large (density limit )
and where the plasma spontaneously forms a transport barrier (H-mode ). Ion
diamagnetic effects allow the edge pedestal to steepen well beyond the first
ideal MHD stability boundary.
IAEA 1999