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An explanation for hard MHD stability limits in low-q95 diverted tokamak plasmas

D Brunetti, J P Graves, C J Ham, S Saarelma2025年8月Plasma Physics and Controlled FusionIF 2.2出版社

This paper proposes a model attempting to explain the appearance of fast growing global disruptive instabilities in diverted configurations when the safety factor near the magnetic separatrix approaches two. We show that if edge density and pressure gradients are strong enough, although external kink modes are stable, poloidal harmonics may couple allowing for a global fluid perturbation to become unstable. The instability window is approached sharply as the mode resonance occurs in the edge region, and is characterised by rather large growth rates even with modest gradients.

日本語訳

本論文は、磁気セパラトリックス近傍の安全係数が2に近づくとき、ダイバータ配位において高速成長する全局的破壊的不安定性の出現を説明しようとするモデルを提案する。我々は、周辺密度と圧力勾配が十分に強い場合、外部キンクモードが安定であるにもかかわらず、ポロイダル高調波が結合し、全局的な流体摂動が不安定になり得ることを示す。不安定性ウィンドウは、モード共鳴が周辺領域で生じるにつれて急峻に近づき、緩やかな勾配でもかなり大きな成長率によって特徴づけられる。

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MagnetohydrodynamicsMHD stability

AIによる論文要約

低q95分断トカマク プラズマにおける強力MHD安定性限界の説明
JAこの論文は、トカマク装置の設計・運転に携わる研究者や学生に役立つでしょう。不安定性の発生メカニズムを理解することで、高性能プラズマの実現につながります。#トカマク #MHD安定性 #プラズマ不安定性 #プラズマ閉じ込め
LLM向け: {'Title': '低q95分断トカマクプラズマにおける強力MHD安定性限界の説明', 'Author(s)': '不明', 'Research Object…

この論文は、分断構成で安全係数q95が2に近づくときに発生する高速成長する大域的破壊的不安定性の出現を説明するモデルを提案しています。強い密度・圧力勾配があると、外部キンクモードは安定でも、ポロイダル調和が結合し、グローバルな流体擾乱が不安定になることを示しています。

An explanation for hard MHD stability limits in low-q95 diverted tokamak plasmas
ENThis paper should be read by fusion researchers and students interested in understanding the stability limits of tokamak plasmas, particularly in diverted configurations with low safety factor.#tokamak #stability #MHD #disruption #diverted
LLM向け: {'Title': 'An explanation for hard MHD stability limits in low-q95 diverted toka…

This paper proposes a model to explain the appearance of fast-growing global disruptive instabilities in diverted tokamak configurations when the safety factor near the magnetic separatrix approaches two. The instability is caused by the coupling of poloidal harmonics, which can lead to a global fluid perturbation becoming unstable, even when external kink modes are stable.

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