Impact of resistive MHD plasma response on perturbation field sidebands

  • D. M. Orlov
  • , T. E. Evans
  • , R. A. Moyer
  • , B. C. Lyons
  • , N. M. Ferraro
  • , G. Y. Park

Research output: Contribution to journalArticlepeer-review

2 Scopus citations

Abstract

Single fluid linear simulations of a KSTAR RMP ELM suppressed discharge with the M3D-C1 resistive magnetohydrodynamic code have been performed for the first time. The simulations show that the application of the n = 1 perturbation using the KSTAR in-vessel control coils (IVCC), which apply modest levels of n = 3 sidebands (∼20% of the n = 1), leads to levels of n = 3 sideband that are comparable to the n = 1 when plasma response is included. This is due to the reduced level of screening of the rational-surface-resonant n = 3 component relative to the rational-surface-resonant n = 1 component. The n = 3 sidebands could play a similar role in ELM suppression on KSTAR as the toroidal sidebands (n = 1, 2, 4) in DIII-D n = 3 ELM suppression with missing I-coil segments (Paz Soldan et al 2014 Nucl. Fusion 54 073013). This result may help to explain the uniqueness of ELM suppression with n = 1 perturbations in KSTAR since the effective perturbation is a mixed n = 1/n = 3 perturbation similar to n = 3 ELM suppression in DIII-D.

Original languageEnglish (US)
Article number075009
JournalPlasma Physics and Controlled Fusion
Volume58
Issue number7
DOIs
StatePublished - Jun 3 2016

All Science Journal Classification (ASJC) codes

  • Nuclear Energy and Engineering
  • Condensed Matter Physics

Keywords

  • edge stochastic layer
  • ELM control
  • plasma response
  • resonant magnetic perturbation
  • tokamak

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