Overview of L-H power threshold studies in NSTX

  • R. Maingi
  • , S. M. Kaye
  • , R. E. Bell
  • , T. M. Biewer
  • , C. S. Chang
  • , D. A. Gates
  • , S. P. Gerhardt
  • , J. Hosea
  • , B. P. Leblanc
  • , H. Meyer
  • , D. Mueller
  • , G. Y. Park
  • , R. Raman
  • , S. A. Sabbagh
  • , T. A. Stevenson
  • , J. R. Wilson

Research output: Contribution to journalArticlepeer-review

41 Scopus citations

Abstract

A summary of results from recent L-H power threshold (PLH) experiments in the National Spherical Torus Experiment is presented. First PLH (normalized linearly by plasma density) was found to be a minimum in double-null configuration, tending to increase as the plasma was shifted more strongly towards lower- or upper-single null configuration with either neutral beam or rf heating. The measured PLH/ne was comparable with neutral beam or rf heating, suggesting that rotation was not playing a dominant role in setting the value of PLH. The role of triangularity (δbot) in setting PLH/ne is less clear: while 50% less auxiliary heating power was required to access H-mode at low δbot than at high δbot, the high δbot discharges had lower ohmic heating and higher dW/dt, leading to comparable loss of power over a range of δbot. In addition, the dependences of PLH on the density, species (helium versus deuterium), plasma current, applied non-axisymmetric error fields and lithium wall conditioning are summarized.

Original languageEnglish
Article number064010
JournalNuclear Fusion
Volume50
Issue number6
DOIs
StatePublished - 2010

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