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A two-term model of the confinement in Elmy H-modes using the global confinement and pedestal databases

  • J. G. Cordey
  • , J. A. Snipes
  • , M. Greenwald
  • , F. Ryter
  • , O. J.W.F. Kardaun
  • , J. Stober
  • , M. Valovic
  • , A. Sykes
  • , A. Dnestrovskij
  • , M. Walsh
  • , J. C. DeBoo
  • , T. N. Carlstrom
  • , G. Bracco
  • , E. Righi
  • , J. G. Cordey
  • , K. Thomsen
  • , D. McDonald
  • , Y. Miura
  • , K. Shinohara
  • , K. Tsuzuki
  • T. Fukuda, Y. Kamada, T. Takizuka, H. Urano, S. M. Kaye, C. Bush, Y. Martin, A. Cote, G. Pacher, J. Ongena, S. Lebedev, A. Chudnovskiy, A. Hubbard, W. Suttrop, L. D. Horton, T. H. Osborne, G. Janeschitz, M. Sugihara, T. Hatae, Y. Kamada

Research output: Contribution to journalArticlepeer-review

Abstract

Two different physical models of the H-mode pedestal are tested against the joint pedestal-core database. The first is a confinement model in which the transport down the steep edge gradient is assumed to be dominated by thermal conduction. The second model is a magnetohydrodynamics (MHD) limit model in which it is assumed that the dominant loss mechanism is by the edge localized modes (ELMs), the pressure gradient being determined by a MHD stability limit. These models are then combined with models for the core and shown to give a good fit to the ELMy H-mode database. The resulting two-term scaling expressions are shown to give very similar predictions for the confinement time, in the next step machines ITER and FIRE, to that of the one-term model IPB98(y,2). The predicted stored energy in the pedestal is 28-50% of the total stored energy.

Original languageEnglish (US)
Pages (from-to)670-674
Number of pages5
JournalNuclear Fusion
Volume43
Issue number8
DOIs
StatePublished - Aug 2003

All Science Journal Classification (ASJC) codes

  • Nuclear and High Energy Physics
  • Condensed Matter Physics

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