Filament structures at the plasma edge on MAST

A Kirk, NB Ayed, G Counsell, B Dudson… - Plasma physics and …, 2006 - iopscience.iop.org
A Kirk, NB Ayed, G Counsell, B Dudson, T Eich, A Herrmann, B Koch, R Martin, A Meakins
Plasma physics and controlled fusion, 2006iopscience.iop.org
The boundary of the tokamak core plasma, or scrape-off layer, is normally characterized in
terms of average parameters such as density, temperature and e-folding lengths suggesting
diffusive losses. However, as is shown in this paper, localized filamentary structures play an
important role in determining the radial efflux in both L mode and during edge localized
modes (ELMs) on MAST. Understanding the size, poloidal and toroidal localization and the
outward radial extent of these filaments is crucial in order to calculate their effect on power …
Abstract
The boundary of the tokamak core plasma, or scrape-off layer, is normally characterized in terms of average parameters such as density, temperature and e-folding lengths suggesting diffusive losses. However, as is shown in this paper, localized filamentary structures play an important role in determining the radial efflux in both L mode and during edge localized modes (ELMs) on MAST. Understanding the size, poloidal and toroidal localization and the outward radial extent of these filaments is crucial in order to calculate their effect on power loading both on the first wall and the divertor target plates in future devices. The spatial and temporal evolution of filaments observed on MAST in L-mode and ELMs have been compared and contrasted in order to confront the predictions of various models that have been proposed to predict filament propagation and in particular ELM energy losses.
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