Effect of toroidal field ripple on plasma rotation in JET

  • P. C. De Vries
  • , A. Salmi
  • , V. Parail
  • , C. Giroud
  • , Y. Andrew
  • , T. M. Biewer
  • , K. Crombé
  • , I. Jenkins
  • , T. Johnson
  • , V. Kiptily
  • , A. Loarte
  • , J. Lönnroth
  • , A. Meigs
  • , N. Oyama
  • , R. Sartori
  • , G. Saibene
  • , H. Urano
  • , K. D. Zastrow

    Research output: Contribution to journalArticlepeer-review

    60 Scopus citations

    Abstract

    Dedicated experiments on TF ripple effects on the performance of tokamak plasmas have been carried out at JET. The TF ripple was found to have a profound effect on the plasma rotation. The central Mach number, M, defined as the ratio of the rotation velocity and the thermal velocity, was found to drop as a function of TF ripple amplitude (δ) from an average value of M = 0.40-0.55 for operations at the standard JET ripple of δ = 0.08% to M = 0.25-0.40 for δ = 0.5% and M = 0.1-0.3 for δ = 1%. TF ripple effects should be considered when estimating the plasma rotation in ITER. With standard co-current injection of neutral beam injection (NBI), plasmas were found to rotate in the co-current direction. However, for higher TF ripple amplitudes (δ ∼ 1%) an area of counter rotation developed at the edge of the plasma, while the core kept its co-rotation. The edge counter rotation was found to depend, besides on the TF ripple amplitude, on the edge temperature. The observed reduction of toroidal plasma rotation with increasing TF ripple could partly be explained by TF ripple induced losses of energetic ions, injected by NBI. However, the calculated torque due to these losses was insufficient to explain the observed counter rotation and its scaling with edge parameters. It is suggested that additional TF ripple induced losses of thermal ions contribute to this effect.

    Original languageEnglish
    Article number035007
    JournalNuclear Fusion
    Volume48
    Issue number3
    DOIs
    StatePublished - Mar 1 2008

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