Wall stabilization of high beta plasmas in DIII-D

  • T. S. Taylor
  • , E. J. Strait
  • , L. Lao
  • , M. Mauel
  • , A. D. Turnbull
  • , K. H. Burrell
  • , M. S. Chu
  • , J. R. Ferron
  • , R. J. Groebner
  • , R. J. La Haye
  • , B. W. Rice
  • , R. T. Snider
  • , S. J. Thompson
  • , D. Wròblewski
  • , D. J. Lightly

Research output: Contribution to journalArticlepeer-review

86 Citations (Scopus)

Abstract

Detailed analysis of recent high beta discharges in the DIII-D [Plasma Physics Controlled Nuclear Fusion Research, 1986 (International Atomic Energy Agency, Vienna, 1987), Vol. I, p. 159] tokamak demonstrates that the resistive vacuum vessel can provide stabilization of low n magnetohydrodynamic (MHD) modes. The experimental beta values reaching up to βT=12.6% are more than 30% larger than the maximum stable beta calculated with no wall stabilization. Plasma rotation is essential for stabilization. When the plasma rotation slows sufficiently, unstable modes with the characteristics of the predicted "resistive wall" mode are observed. Through slowing of the plasma rotation between the q=2 and q=3 surfaces with the application of a nonaxisymmetric field, it has been determined that the rotation at the outer rational surfaces is most important, and that the critical rotation frequency is of the order of Ω/2π=1 kHz.

Original languageEnglish
Pages (from-to)2390-2396
Number of pages7
JournalPhysics of Plasmas
Volume2
Issue number6
DOIs
Publication statusPublished - 1995

All Science Journal Classification (ASJC) codes

  • Condensed Matter Physics

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