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Runaway electron beam generation and mitigation during disruptions at JET-ILW

  • C. Reux
  • , V. Plyusnin
  • , B. Alper
  • , D. Alves
  • , B. Bazylev
  • , E. Belonohy
  • , A. Boboc
  • , S. Brezinsek
  • , I. Coffey
  • , J. Decker
  • , P. Drewelow
  • , S. Devaux
  • , P. C. De Vries
  • , A. Fil
  • , S. Gerasimov
  • , L. Giacomelli
  • , S. Jachmich
  • , E. M. Khilkevitch
  • , V. Kiptily
  • , R. Koslowski
  • U. Kruezi, M. Lehnen, I. Lupelli, P. J. Lomas, A. Manzanares, A. Martin De Aguilera, G. F. Matthews, J. Mlynář, E. Nardon, E. Nilsson, C. Perez Von Thun, V. Riccardo, F. Saint-Laurent, A. E. Shevelev, G. Sips, C. Sozzi
  • Commissariat à l'Énergie Atomique (CEA)
  • Instituto Superior Técnico
  • Culham Centre for Fusion Energy
  • KARLSRUHER INSTITUT FUER TECHNOLOGIE
  • FORSCHUNGSZENTRUM JULICH GMBH
  • Queens University
  • Max-Planck-Institut für Plasmaphysik
  • ITER
  • Ioffe Physical-Technical Institute of the Russian Academy of Sciences
  • Laboratorio Nacional de Fusión
  • Institute of Plasma Physics, Academy of Sciences of the Czech Republic
  • CNR

Résultats de recherche: Contribution à un journalArticleRevue par des pairs

126 Citations (Scopus)

Résumé

Disruptions are a major operational concern for next generation tokamaks, including ITER. They may generate excessive heat loads on plasma facing components, large electromagnetic forces in the machine structures and several MA of multi-MeV runaway electrons. A more complete understanding of the runaway generation processes and methods to suppress them is necessary to ensure safe and reliable operation of future tokamaks. Runaway electrons were studied at JET-ILW showing that their generation dependencies (accelerating electric field, avalanche critical field, toroidal field, MHD fluctuations) are in agreement with current theories. In addition, vertical stability plays a key role in long runaway beam formation. Energies up to 20 MeV are observed. Mitigation of an incoming runaway electron beam triggered by massive argon injection was found to be feasible provided that the injection takes place early enough in the disruption process. However, suppressing an already accelerated runaway electron beam in the MA range was found to be difficult even with injections of more than 2 kPa.m3 high-Z gases such as krypton or xenon. This may be due to the presence of a cold background plasma weakly coupled to the runaway electron beam which prevents neutrals from penetrating in the electron beam core. Following unsuccessful mitigation attempts, runaway electron impacts on beryllium plasma-facing components were observed, showing localized melting with toroidal asymmetries.

langue originaleAnglais
Numéro d'article093013
journalNuclear Fusion
Volume55
Numéro de publication9
Les DOIs
étatPublié - 5 août 2015

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