Nonlinear MHD modeling of n = 1 RMP-induced pedestal transport and mode coupling effects on ELM suppression in KSTAR

S.K. Kim (Corresponding author), S. Pamela, N. Logan, Y.S. Na, C. Lee, J.K. Park, S. Yang, Q. Hu, M. Becoulet, G. Huijsmans, M. Hoelzl, Y. In, M.W. Kim, H.H. Lee, J.H. Lee, J. H. Lee, O. Kwon, E. Kolemen

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Samenvatting

Fully suppressing edge-localized modes (ELMs), e.g., with resonant magnetic perturbations (RMPs), is essential to reach and sustain high-performance steady-state H-mode plasmas because large ELMs can significantly reduce the lifetime of divertor components in future tokamak reactors. RMP-driven ELM suppression in KSTAR has been modeled by coupling the neoclassical transport code PENTRC to the nonlinear 3D MHD code JOREK. We have found that the radial transport from the combined effects of the kink-peeling, tearing response, and neoclassical toroidal viscosity can explain the pedestal degradation observed in experiments. In addition, it has been found that the RMP response can increase the inter-ELM heat flux on the lower outer divertor by redistributing the heat transport between the divertor plates. In addition to the degraded pedestal, ELM suppression is also attributable to the RMP-induced mode interactions. While the linear stability of peeling-ballooning mode (PBMs) improves owing to the degraded pedestal, the PBM and RMP interaction increases the spectral transfer between edge harmonics, preventing catastrophic growth and the crash of unstable modes. Here, it turns out that the magnetic islands near the pedestal top can play a vital role in mediating the mode interactions.

Originele taal-2Engels
Artikelnummer106021
Aantal pagina's13
TijdschriftNuclear Fusion
Volume62
Nummer van het tijdschrift10
DOI's
StatusGepubliceerd - dec. 2022

Bibliografische nota

Publisher Copyright:
© 2022 IAEA, Vienna.

Financiering

The authors would like to express their deepest gratitude to KSTAR Team for the extensive supports on the RMP-ELM suppression experiment. This material was supported by the U.S. Department of Energy, under Awards DE-SC0020372 & DE-AC52-07NA27344. This work was also supported by the U.S. Department of Energy under contract number DE-AC02-09CH11466 (Princeton Plasma Physics Laboratory). The United States Government retains a non-exclusive, paid-up, irrevocable, worldwide license to publish or reproduce the published form of this manuscript or allow others to do so for United States Government purposes. This research was also supported by R&D Program of ‘KSTAR Experimental Collaboration and Fusion Plasma Research (EN2201-13)’ through the Korea Institute of Fusion Energy (KFE) funded by the Government funds. Computing resources were provided on the KFE computer, KAIROS, funded by the Ministry of Science and ICT of the Republic of Korea (KFE-EN2241-8). Part of this work has been carried out within the framework of the EUROfusion Consortium and has received funding from the Euratom research and training program 2014-2018 and 2019-2020 under Grant Agreement No. 633053. The views and opinions expressed herein do not necessarily reflect those of the European Commission. This work was partly carried out the Marconi-Fusion supercomputer operated by CINECA. The authors would like to express their deepest gratitude to KSTAR Team for the extensive supports on the RMP–ELM suppression experiment. This material was supported by the U.S. Department of Energy, under Awards DE-SC0020372 & DE-AC52-07NA27344. This work was also supported by the U.S. Department of Energy under contract number DE-AC02-09CH11466 (Princeton Plasma Physics Laboratory). The United States Government retains a non-exclusive, paid-up, irrevocable, worldwide license to publish or reproduce the published form of this manuscript or allow others to do so for United States Government purposes. This research was also supported by R&D Program of ‘KSTAR Experimental Collaboration and Fusion Plasma Research (EN2201-13)’ through the Korea Institute of Fusion Energy (KFE) funded by the Government funds. Computing resources were provided on the KFE computer, KAIROS, funded by the Ministry of Science and ICT of the Republic of Korea (KFE-EN2241-8). Part of this work has been carried out within the framework of the EUROfusion Consortium and has received funding from the Euratom research and training program 2014–2018 and 2019–2020 under Grant Agreement No. 633053. The views and opinions expressed herein do not necessarily reflect those of the European Commission. This work was partly carried out the Marconi-Fusion supercomputer operated by CINECA.

FinanciersFinanciernummer
CINECA
Euratom Research and Training Programme 2014-2018
KSTAR Experimental Collaboration and Fusion Plasma ResearchEN2201-13
Korea Institute of Fusion Energy
Ministry of Science and ICT of the Republic of KoreaKFE-EN2241-8
U.S. Department of EnergyDE-SC0020372, DE-AC02-09CH11466, DE-AC52-07NA27344
European Union’s Horizon Europe research and innovation programme633053
H2020 Euratom
Princeton Plasma Physics Laboratory (PPPL)

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