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W transport and accumulation control in the termination phase of JET H-mode discharges and implications for ITER

  • JET Contributors
  • Culham Centre for Fusion Energy
  • Austrian Academy of Science
  • Vienna University of Technology
  • ITER
  • Laboratorio Nacional de Fusión
  • Instituto Superior Técnico
  • Commissariat à l'Énergie Atomique (CEA)
  • FORSCHUNGSZENTRUM JULICH GMBH
  • Institute for Plasma Research
  • Queens University
  • University of Helsinki
  • VTT Technical Research Centre of Finland
  • National Institutes for Quantum and Radiological Science and Technology
  • University of Napoli 'Federico II'
  • Universidad Nacional de Educación a Distancia
  • Istituto di Fisica del Plasma Piero Caldirola
  • Consorzio Rfx
  • Kurchatov Institute
  • University of Napoli Parthenope
  • University of Ghent
  • Université Libre de Bruxelles
  • ENEA Centro Ricerche Frascati
  • Troitsk Insitute of Innovating and Thermonuclear Research (TRINITI)
  • Uppsala University
  • The National Institute for Cryogenics and Isotopic Technology
  • Max-Planck-Institut für Plasmaphysik
  • Università degli Studi di Catania
  • Fusion for Energy
  • National Institute for Fusion Science
  • Massachusetts Institute of Technology
  • Aalto University
  • University of Latvia
  • Imperial College London
  • University of Oxford
  • EUROfusion
  • Oak Ridge National Laboratory
  • KARLSRUHER INSTITUT FUER TECHNOLOGIE
  • University of York
  • KTH Royal Institute of Technology
  • Maritime University of Szczecin
  • Institute of Nuclear Physics PAN
  • Institute of Plasma Physics, Academy of Sciences of the Czech Republic
  • University of Trento
  • Ecole Polytechnique Federale de Lausanne
  • Wigner Research Centre for Physics
  • University Mlynska
  • Lviv Polytechnic National University
  • University of Milano-Bicocca
  • The National Institute for Optoelectronics
  • Fourth State Research
  • University of Texas at Austin
  • STUDIECENTRUM VOOR KERNENERGIE / CENTRE D'ETUDE DE L'ENERGIE NUCLEAIRE
  • Narodowe Centrum Badań Jadrowych
  • Princeton Plasma Physics Laboratory
  • Université Aix Marseille
  • University of Cagliari
  • University of Warwick
  • Institute of Plasma Physics and Laser Microfusion
  • FOM Institute DIFFER
  • National Institute for Laser, Plasma and Radiation Physics
  • Jozef Stefan Institute
  • Université de Lorraine
  • Institute of Plasma Physics Chinese Academy of Sciences
  • Center for Energy Research
  • The 'Horia Hulubei' National Institute for Physics and Nuclear Engineering
  • Chalmers University of Technology
  • European Commission
  • Universidad Politécnica de Madrid
  • Second University of Napoli
  • Warsaw University of Technology
  • University of Basilicata
  • Barcelona Supercomputer Centre
  • University of Seville
  • Centro Brasileiro de Pesquisas Fisicas
  • University of Rome Tor Vergata
  • Ioffe Physical-Technical Institute of the Russian Academy of Sciences
  • General Atomics
  • Universitat Innsbruck
  • University of Toyama
  • University of Strathclyde
  • National Technical University of Athens
  • University of Tuscia
  • Technical University of Denmark
  • KAIST
  • Seoul National University
  • UNIVERSITY COLLEGE CORK, NATIONAL UNIVERSITY OF IRELAND, CORK
  • University of Opole
  • Daegu University
  • National Fusion Research Institute (NFRI)
  • Dublin City University
  • Pelin Llc
  • Arizona State University
  • Universidad Complutense de Madrid
  • University of Basel
  • Universidad Carlos III de Madrid
  • Consorzio CREATE
  • NCSR 'Demokritos'
  • Purdue University
  • University of California
  • Universidade de São Paulo
  • Lithuanian Energy Institute
  • HRS Fusion
  • Politecnico di Torino
  • University of Cassino
  • University of Electronic Science and Technology of China

Résultats de recherche: Contribution à un journalArticleRevue par des pairs

49 Citations (Scopus)

Résumé

Tokamak operation with W PFCs is associated with specific challenges for impurity control, which may be particularly demanding in the transition from stationary H-mode to L-mode. To address W control issues in this phase, dedicated experiments have been performed at JET including the variation of the decrease of the power and current, gas fuelling and central ion cyclotron heating (ICRH), and applying active ELM control by vertical kicks. The experimental results obtained demonstrate the key role of maintaining ELM control to control the W concentration in the exit phase of H-modes with slow (ITER-like) ramp-down of the neutral beam injection power in JET. For these experiments, integrated fully predictive core+edge+SOL transport modelling studies applying discrete models for the description of transients such as sawteeth and ELMs have been performed for the first time with the JINTRAC suite of codes for the entire transition from stationary H-mode until the time when the plasma would return to L-mode focusing on the W transport behaviour. Simulations have shown that the existing models can appropriately reproduce the plasma profile evolution in the core, edge and SOL as well as W accumulation trends in the termination phase of JET H-mode discharges as function of the applied ICRH and ELM control schemes, substantiating the ambivalent effect of ELMs on W sputtering on one side and on edge transport affecting core W accumulation on the other side. The sensitivity with respect to NB particle and momentum sources has also been analysed and their impact on neoclassical W transport has been found to be crucial to reproduce the observed W accumulation characteristics in JET discharges. In this paper the results of the JET experiments, the comparison with JINTRAC modelling and the adequacy of the models to reproduce the experimental results are described and conclusions are drawn regarding the applicability of these models for the extrapolation of the applied W accumulation control techniques to ITER.

langue originaleAnglais
Numéro d'article074008
journalPlasma Physics and Controlled Fusion
Volume60
Numéro de publication7
Les DOIs
étatPublié - 5 juin 2018

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