Study of fuelling control for confinement experiments in Heliotron J
Creators
- Mizuuchi, T.1
- Sano, F.1
- Nagasaki, K.1
- Okada, H.1
- Minami, T.1
- Kobayashi, S.1
- Yamamoto, S.1
- Oshima, S.1
- Konoshima, S.1
- Shi, N.1
- Nakamura, Y.2
- Lee, H.Y.2
- Zang, L.2
- Watada, H.2
- Arai, S.2
- Fukushima, H.2
- Hashimoto, K.2
- Kenmochi, N.2
- Nagae, Y.2
- Nakamura, Y.I.2
- Sha, M.2
- Sugimoto, Y.2
- Yasuda, K.2
- Kasajima, K.2
- Yamamoto, K.2
- Kagawa, T.2
- Mizuno, K.2
- Minami, T.Y.2
- Wada, Y.2
- Yashiro, H.2
- Mukai, K.3
- Nishino, N.4
- Kado, S.5
- Takeuchi, Masaki6
- Nakashima, Y.7
- Weir, G.8
- Volpe, F.9
- Yan, L.10
- Estrada, T.11
- 1. Kyoto University, Institute of Advanced Energy, Uji, Kyoto (Japan)
- 2. Kyoto University, Graduate School of Energy Science, Uji, Kyoto (Japan)
- 3. National Inst. for Fusion Science, Toki, Gifu (Japan)
- 4. Hiroshima University, Graduate School of Engineering, Higashi-Hiroshima, Hiroshima (Japan)
- 5. Tokyo University, School of Engineering, Tokyo (Japan)
- 6. Japan Atomic Energy Agency, Naka Fusion Institute, Naka, Ibaraki (Japan)
- 7. University of Tsukuba, Plasma Research Center, Tsukuba, Ibaraki (Japan)
- 8. University of Wisconsin, Madison, WI (United States)
- 9. Columbia University, New York, NY (United States)
- 10. Southwestern Institute of Physics, Chendu (China)
- 11. Laboratorio Nacional de Fusión, EURATOM-CIEMAT, Madrid (Spain)
Description
The optimization of gas-fuelling scenario has been studied to examine the plasma confinement in Heliotron J. Gas fuelling effects on plasma profile are discussed by comparing two fuelling methods, a short pulse H2-beam fuelling with a supersonic molecular-beam injection (SMBI) technique and a high-intensity gas-puff fuelling (HIGP) with a conventional gas puff technique. The maximum plasma stored energy Wp after SMBI is about 20% higher than that after HIGP in this NBI-only sustained plasma experiment, where the line-averaged density is almost the same (∼3x1019 m-3) for both cases. The core electron and ion temperatures for the SMBI case are higher than those in the HIGP case at the timing of maximum Wp. A peaked density profile is observed after SMBI, while it is flat or a slightly hollow for the case of HIGP. These observations point out the importance of SMBI fuelling for plasma density control to obtain better plasma performance. The effects of fuelling on plasma fluctuations and effectiveness of fuelling control for triggering of the L-H transitions are also reported. (author)
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45097518.pdf
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Additional details
Publishing Information
- Imprint Pagination
- 9 p.
- Report number
- NIFS--1059
Conference
- Title
- 24. IAEA Fusion Energy Conference
- Dates
- 8-13 Oct 2012
- Place
- San Diego, CA (United States)
INIS
- Country of Publication
- Japan
- Country of Input or Organization
- Japan
- INIS RN
- 45097518
- Subject category
- S70: PLASMA PHYSICS AND FUSION TECHNOLOGY;
- Resource subtype / Literary indicator
- Conference
- Descriptors DEI
- BALMER LINES; ELECTRON TEMPERATURE; EMISSION SPECTRA; GAS INJECTION; HELICAL CONFIGURATION; HELIOTRON; H-MODE PLASMA CONFINEMENT; HYDROGEN; ION TEMPERATURE; JETS; PLASMA; PLASMA DENSITY; PLASMA PRODUCTION; PLASMA RADIAL PROFILES; SPATIAL DISTRIBUTION; SUPERSONIC FLOW; THERMONUCLEAR FUELS; THERMONUCLEAR REACTOR FUELING
- Descriptors DEC
- CLOSED PLASMA DEVICES; CONFIGURATION; CONFINEMENT; DISTRIBUTION; ELEMENTS; FLUID FLOW; FLUID INJECTION; FUELS; MAGNETIC CONFINEMENT; NONMETALS; PLASMA CONFINEMENT; SPECTRA; THERMONUCLEAR DEVICES
Optional Information
- Notes
- 18 refs., 7 figs.
- Secondary number(s)
- IAEA-CN--197; EX/P3--07