Onset of instability with collapse observed in relatively high density and medium beta regions of LHD

Author:

Takemura Yuki1ORCID,Watanabe Kiyomasa12,Sakakibara Satoru13,Ohdachi Satoshi14,Narushima Yoshiro13,Tanaka Kenji15,Tokuzawa Tokihiko13ORCID

Affiliation:

1. National Institute for Fusion Science, National Institutes of Natural Sciences, Toki, Gifu 509-5292, Japan

2. Department of Energy Engineering, Graduate School of Engineering, Nagoya University, Nagoya, Aichi 464-8603, Japan

3. The Graduate University for Advanced Studies, SOKENDAI, Toki, Gifu 509-5292, Japan

4. Graduate School of Frontier Sciences, The University of Tokyo, Kashiwa, Chiba 277-8561, Japan

5. Interdisciplinary Graduate School of Engineering Sciences, Kyushu University, Kasuga, Fukuoka 816-8580, Japan

Abstract

Edge MHD instabilities with pressure collapse are found in relatively high beta and low magnetic Reynolds number regions with a magnetic axis torus outward-shifted configuration of the large helical device (LHD), and characteristics and onset conditions of the instability are investigated. The instability has a radial structure with an odd parity around the resonant surface, which is different from that of the interchange instability typically observed in the LHD. The onset condition dependence on the magnetic axis location shows that the onset beta increases as the magnetic axis location moves more torus inwardly, and the instability appears only in limited configurations where the magnetic axis is located between 3.65 and 3.775 m. In such configurations, the resonant surface location is close to an index of the plasma boundary. This fact suggests that the distance between the resonant surface location and the plasma boundary plays an important role in the onset, and a possibility that the instability is driven by an external mode.

Funder

Japan Society for the Promotion of Science

Future Energy Research Association

National Institute for Fusion Science

Publisher

AIP Publishing

Subject

Condensed Matter Physics

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