MISC

2001年4月

Impact of pellet injection on extension of the operational region in LHD

NUCLEAR FUSION
  • R Sakamoto
  • H Yamada
  • K Tanaka
  • K Narihara
  • S Morita
  • S Sakakibara
  • S Masuzaki
  • S Inagaki
  • LR Baylor
  • PW Fisher
  • SK Combs
  • MJ Gouge
  • S Kato
  • A Komori
  • O Kaneko
  • N Ashikawa
  • P de Vries
  • M Emoto
  • H Funaba
  • M Goto
  • K Ida
  • H Idei
  • K Ikeda
  • M Isobe
  • S Kado
  • K Kawahata
  • K Khlopenkov
  • S Kubo
  • R Kumazawa
  • T Minami
  • J Miyazawa
  • T Morisaki
  • S Murakami
  • S Muto
  • T Mutoh
  • Y Nagayama
  • Y Nakamura
  • H Nakanishi
  • K Nishimura
  • N Noda
  • T Notake
  • T Kobuchi
  • Y Liang
  • S Ohdachi
  • N Ohyabu
  • Y Oka
  • M Osakabe
  • T Ozaki
  • RO Pavlichenko
  • BJ Peterson
  • A Sagara
  • K Saito
  • H Sasao
  • M Sasao
  • K Sato
  • M Sato
  • T Seki
  • T Shimozuma
  • M Shoji
  • S Sudo
  • H Suzuki
  • M Takechi
  • Y Takeiri
  • N Tamura
  • K Toi
  • T Tokuzawa
  • Y Torii
  • K Tsumori
  • Yamada, I
  • S Yamaguchi
  • S Yamamoto
  • Y Yoshimura
  • KY Watanabe
  • T Watari
  • K Yamazaki
  • Y Hamada
  • O Motojima
  • M Fujiwara
  • 全て表示

41
4
開始ページ
381
終了ページ
386
記述言語
英語
掲載種別
DOI
10.1088/0029-5515/41/4/304
出版者・発行元
INT ATOMIC ENERGY AGENCY

Pellet injection has been used as a primary fuelling scheme in the Large Helical Device. With pellet injection, the operational region of NBI plasmas has been extended to higher densities while maintaining a favourable dependence of energy confinement on density, and several important values, such as plasma stored energy of 0.85 MJ, energy confinement time of 0.3 s, beta of 2.4% at 1.3 T and density of 1.1x10(20) m(-3), have been achieved. These parameters cannot be attained by gas puffing. Ablation and the subsequent behaviour of the plasma have been investigated. The measured pellet penetration depth estimated on the basis of the duration of the H-alpha emission is shallower than the depth predicted from the simple neutral gas shielding (NGS) model. It can be explained by the NGS model with inclusion of the effect of fast ions on the ablation. Just after ablation, the redistribution of the ablated pellet mass was observed on a short timescale (similar to 400 ms). The redistribution causes shallow deposition and low fuelling efficiency.

リンク情報
DOI
https://doi.org/10.1088/0029-5515/41/4/304
Web of Science
https://gateway.webofknowledge.com/gateway/Gateway.cgi?GWVersion=2&SrcAuth=JSTA_CEL&SrcApp=J_Gate_JST&DestLinkType=FullRecord&KeyUT=WOS:000169682600004&DestApp=WOS_CPL
URL
https://www.scopus.com/inward/record.uri?partnerID=HzOxMe3b&scp=0035323784&origin=inward
ID情報
  • DOI : 10.1088/0029-5515/41/4/304
  • ISSN : 0029-5515
  • SCOPUS ID : 0035323784
  • Web of Science ID : WOS:000169682600004

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