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On the parasitic absorption in FWCD experiments in JET ITB plasmas

  • T. Hellsten
  • , M. Laxåback
  • , T. Bergkvist
  • , T. Johnson
  • , F. Meo
  • , F. Nguyen
  • , C.C. Petty
  • , M. Mantsinen
  • , G. Matthews
  • , J.-M. Noterdaeme
  • , Tuomas Tala
  • , D. Van Eester
  • , P. Andrew
  • , P. Beaumont
  • , V. Bobkov
  • , M. Brix
  • , J. Brzozowski
  • , L.-G. Eriksson
  • , C. Giroud
  • , E. Joffrin
  • V. Kiptily, J. Mailloux, M-L. Mayoral, I. Monakhov, R. Sartori, A. Staebler, E. Rachlew, E. Tennfors, A. Tuccillo, A. Walden, K. D. Zastrow, JET-EFDA Contributors
    • KTH Royal Institute of Technology
    • Risø DTU National Laboratory for Sustainable Energy
    • Commissariat a l'Energie Atomique et aux Energies Alternatives (CEA)
    • General Atomics
    • Helsinki University of Technology
    • Culham Science Centre
    • Max-Planck-Institut für Plasmaphysik (IPP)
    • Ghent University
    • École Royale Militaire
    • EFDA Close Support Unit Garching
    • National Agency for New Technologies, Energy and Sustainable Economic Development (ENEA)

    Research output: Contribution to journalArticleScientificpeer-review

    Abstract

    Fast wave current drive (FWCD) experiments have been performed in JET plasmas with electron internal transport barriers produced with LHCD. Because of a large fraction of parasitic absorption, owing to weak single pass damping, the inductive nature of the plasma current and the interplay between the RF-driven current and the bootstrap current only small changes are seen in the central current profiles. The measured difference in the central current density for co- and counter-current drive is larger than the response expected from current diffusion calculations, but smaller than the driven currents, suggesting a faster current diffusion than that given by neo-classical resistivity. A large fraction of the power is absorbed by cyclotron damping on residual 3He ions while a significant fraction appears not to have been deposited in the plasma. The strong degradation of heating and current drive occurs simultaneously with strong increases in the Be II and C IV line intensities in the divertor. The degradation depends on the phasing of the antennas and increases with reduced single pass damping which is consistent with RF-power being lost by dissipation of rectified RF-sheath potentials at the antennas and walls. Asymmetries in direct electron heating, lost power and production of impurities, fast ions and gamma-rays are seen for co- and counter-current drive. These differences are consistent with the differences in the absorption on residual 3He ions owing to the RF-induced pinch. Effective direct electron heating, comparable to the indirect electron heating with H-minority heating, occurs for dipole phasing of the antennas without producing a significant fast ion pressure and with low impurity content in the divertor plasma.
    Original languageEnglish
    Pages (from-to)706 - 720
    Number of pages15
    JournalNuclear Fusion
    Volume45
    Issue number7
    DOIs
    Publication statusPublished - 2005
    MoE publication typeA1 Journal article-refereed

    UN SDGs

    This output contributes to the following UN Sustainable Development Goals (SDGs)

    1. SDG 7 - Affordable and Clean Energy
      SDG 7 Affordable and Clean Energy

    Keywords

    • JET
    • plasma
    • fusion energy
    • fusion reactors
    • ITER
    • Tokamak
    • internal transport barriers

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