Nonlinear MHD modeling of neon doped shattered pellet injection with JOREK and its comparison to experiments in KSTAR

Abstract 3D nonlinear MHD simulations of neon-doped single shattered pellet injection (SPI) conducted with the JOREK code reveal rich physics during SPI-induced disruptions in KSTAR. In the early phase, pressure-driven modes dominate, and the perturbation of the plasma current is largely consistent with the perturbation of the Pfirsch–Schlüter current. As shards reach the q = 1 surface, resistive current perturbations by helical electron cooling start to dominate, and the electron temperature in the core begins to collapse with convective mixing of the density driven by the internal <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" overflow="scroll"> <mml:mrow> <mml:mn>1</mml:mn> <mml:mrow> <mml:mo>/</mml:mo> </mml:mrow> <mml:mn>1</mml:mn> </mml:mrow> </mml:math> kink mode. The confinement of the plasma is later completely destroyed as a cold bubble convects into the core via quasi-interchange mode. Comparisons with available experimental data demonstrate qualitative agreements between JOREK results and experiments, and possible reasons for deviations are discussed.

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Publication Details

Journal
Nuclear Fusion
Published
2024-08-13
DOI
https://doi.org/10.1088/1741-4326/ad6ea1
Citations
5
Primary Topic
Magnetic confinement fusion research
Type
article
Field-Weighted Citation Impact
3.30

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article

Nonlinear MHD modeling of neon doped shattered pellet injection with JOREK and its comparison to experiments in KSTAR

M. Hoelzl, D. Bonfiglio, Di Hu, F.J. Artola et al.
5 citations
Nuclear Fusion
Magnetic confinement fusion research
3.30
article

Nonlinear MHD modeling of neon doped shattered pellet injection with JOREK and its comparison to experiments in KSTAR

M. Hoelzl, D. Bonfiglio, Di Hu, F.J. Artola, E. Nardon, M. Lehnen, S.-J. Lee, Yong-Su Na, Jayhyun Kim
article en
5 citations

Abstract

Abstract 3D nonlinear MHD simulations of neon-doped single shattered pellet injection (SPI) conducted with the JOREK code reveal rich physics during SPI-induced disruptions in KSTAR. In the early phase, pressure-driven modes dominate, and the perturbation of the plasma current is largely consistent with the perturbation of the Pfirsch–Schlüter current. As shards reach the q = 1 surface, resistive current perturbations by helical electron cooling start to dominate, and the electron temperature in the core begins to collapse with convective mixing of the density driven by the internal <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" overflow="scroll"> <mml:mrow> <mml:mn>1</mml:mn> <mml:mrow> <mml:mo>/</mml:mo> </mml:mrow> <mml:mn>1</mml:mn> </mml:mrow> </mml:math> kink mode. The confinement of the plasma is later completely destroyed as a cold bubble convects into the core via quasi-interchange mode. Comparisons with available experimental data demonstrate qualitative agreements between JOREK results and experiments, and possible reasons for deviations are discussed.

Nuclear FusionVol. 64(10)
ITER (FR), Seoul National University (KR), Commissariat à l'Énergie Atomique et aux Énergies Alternatives (FR), Korea Institute of Fusion Energy (KR), CEA Cadarache (FR), Max Planck Institute for Plasma Physics (DE), Consorzio per la Ricerca Sanitaria (IT), Beihang University (CN)
National Research Foundation of Korea, Euratom Research and Training Programme
Openalex Percentile: Top 6%
Magnetic confinement fusion research
3.30
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