Dependence of edge stability on plasma shape and local pressure gradients in the DIII-D and JT-60U tokamaks

  • L. L. Lao
  • , Y. Kamada
  • , T. Oikawa
  • , L. R. Baylor
  • , K. H. Burrell
  • , V. S. Chan
  • , M. S. Chance
  • , M. S. Chu
  • , J. R. Ferron
  • , T. Fukuda
  • , T. Hatae
  • , A. Isayama
  • , G. J. Jackson
  • , A. W. Leonard
  • , M. A. Makowski
  • , J. Manickam
  • , M. Murakami
  • , M. Okabayashi
  • , T. H. Osborne
  • , P. B. Snyder
  • E. J. Strait, S. Takeji, T. Takizuka, T. S. Taylor, A. D. Turnbull, K. Tsuchiya, M. R. Wade

Research output: Contribution to journalArticlepeer-review

73 Scopus citations

Abstract

The dependence of edge stability on plasma shape and local pressure gradients P′ in the DIII-D and JT-60U tokamaks is studied. The stronger plasma shaping in DIII-D allows the edge region of DIII-D discharges with type I (giant) ELMs to have access to the second region of stability for ideal ballooning modes and a larger edge pedestal pressure gradient P′ than JT-60U type I ELM discharges. These JT-60U discharges are near the ballooning mode first regime stability limit. The DIII-D results support an ideal stability based working model of type I ELMs as low to intermediate toroidal mode number, n, MHD modes. The results from a stability analysis of JT-60U type I ELM discharges indicate that the predictions of this model are also consistent with JT-60U edge stability observations.

Original languageEnglish
Pages (from-to)295-300
Number of pages6
JournalNuclear Fusion
Volume41
Issue number3
DOIs
StatePublished - Mar 2001

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