Experimental study of the role of the edge radial electric field on the access to H-mode at ASDEX Upgrade
ORAL · Invited
Abstract
In this study the edge parameters of L-mode plasmas which have significantly different LH power thresholds were compared. Plasmas with favorable and unfavorable drift configuration, deuterium versus hydrogen, and plasmas with the outer divertor leg on the horizontal target versus on the vertical target were examined. Special focus was put on the measurement of the outer Er gradient, which connects the confined plasma and the scrape-off layer (SOL). For this a new diagnostics, based on the active spectroscopy of HeII, was used.
It is found that prior to the LH transition the outer Er gradient normally shows little variation and only steepens once the LH transition has occurred. The evolution of the edge Er profile follows the main ion pressure gradient. In L-mode also the toroidal plasma rotation has a non-negligible impact on the Er profile. In particular, the intrinsic rotation increases with increasing edge collisionality, while Er in the confined plasma decreases. The Er profile in the SOL changes concomitantly, which indicates a strong interaction between SOL flows and the edge toroidal rotation. The direction of the intrinsic edge rotation follows the Pfirsch-Schlüter flows on the high field side of the SOL. A comparison with neoclassical theory suggests that the main ion poloidal rotation is on the neoclassical level, although in detail deviations are observed. In particular, the impact of rotation cannot explain the observed shallower Er well in unfavorable compared to favorable drift configuration. Er measurements in hydrogen show no dominant role of the inner or the outer Er gradient in the LH transition.
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Presenters
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Ulrike Plank
Max Planck Insitute for Plasma Physics, Garching, Germany, Max Planck Institute for Plasma Physics
Authors
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Ulrike Plank
Max Planck Insitute for Plasma Physics, Garching, Germany, Max Planck Institute for Plasma Physics
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Dominik Brida
Max Planck Insitute for Plasma Physics, Garching, Germany, Max Planck Institute for Plasma Physics
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Garrard D Conway
Max-Planck-Institut für Plasmaphysik, Garching, Germany, Max Planck Institute for Plasma Physics, Garching, Germany, Max Planck Institute for Plasma Physics
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Tim Happel
Max-Planck-Institut für Plasmaphysik, Garching, Germany, Max Planck Institute for Plasma Physics, Garching, Germany, Max-Planck-Institut für Plasmaphysik, 85748 Garching, Germany
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Pascale Hennequin
Laboratoire de Physique des Plasmas, Ecole Polytechnique, Palaiseau, France, LPP, Ecole Polytechnique, Palaiseau, France
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Amanda E Hubbard
Massachusetts Institute of Technology MIT, MIT PSFC, Massachusetts Institute of Technology MIT, Cambridge, MA, USA
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Hendrik Meyer
CCFE, Culham Science Centre, Abingdon, Oxon, UK, Culham Centre for Fusion Energy, UKAEA, UK
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Thomas Pütterich
Max Planck Institute for Plasma Physics, Garching, Germany, Max-Planck-Institut für Plasmaphysik
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Clemente Angioni
Max Planck Institute for Plasma Physics, Garching, Germany, Max Planck Institute for Plasma Physics
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Marco Cavedon
Max Planck Institute for Plasma Physics, Dipartimento di Fisica "G. Occhialini", Università di Milano-Bicocca, Milano, Italy
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Ralph Dux
Max Planck Institute for Plasma Physics, Max Planck Institute for Plasma Physics, Garching, Germany, Max-Planck-Institut fur Plasmaphysik
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Rainer Fischer
Max-Planck-Institut für Plasmaphysik, Garching, Germany, Max Planck Institute for Plasma Physics, Garching, Germany
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Rachael M McDermott
Max-Planck-Institut für Plasmaphysik, Garching, Germany, Max Planck Institute for Plasma Physics, Garching, Germany, Max Planck Institute for Plasma Physics
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Philip A Schneider
Max-Planck-Institut für Plasmaphysik, Garching, Germany, Max Planck Institute for Plasma Physics, Garching, Germany, Max Planck Institute for Plasma Physics