Study of Fueling 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
- Takeuchi, M.1
- Hanatani, K.1
- Konoshima, S.1
- Oshima, S.2
- Nakamura, Y.2
- Mukai, K.3
- Lee, H.3
- Zang, L.3
- Yamamoto, K.3
- Arai, S.3
- Kagawa, T.3
- Mizuno, K.3
- Minami, T.3
- Wada, Y.3
- Watada, H.3
- Yashiro, H.3
- Nishino, N.4
- Nakashima, Y.5
- Kado, S.6
- 1. Institute of Advanced Energy, Kyoto University, Gokasho, Uji (Japan)
- 2. Graduate School of Energy Science, Kyoto University, Uji (Japan)
- 3. Kyoto University Pioneering Research Unit for Next Generation, Uji (Japan)
- 4. Graduate School of Engineering, Hiroshima University, Higashi-Hiroshima (Japan)
- 5. Plasma Research Center, University of Tsukuba, Tsukuba (Japan)
- 6. School of Engineering, University of Tokyo, Bunkyo (Japan)
Description
Full text: This paper discusses the effects of fueling control on plasma performance in Heliotron J, a helical-axis heliotron device with an L/M = 1/4 helical coil (R0 = 1.2 m, (ap) = 0.12 - 0.17 m, (B0) ≤ 1.5 T). Here, L and M are the pole number of the helical coil and its helical pitch number, respectively. Based on recent installation/improvement of diagnostics, which give us plasma profile database for detailed transport analyses, the confinement study has been accelerated. Here fueling and recycling control is not only one of the key issues for high density and high performance plasma but also plays important roles in diagnostics. Effectiveness of supersonic molecular beam injection (SMBI) fueling has been studied based on profile data. A peaked density profile is realized by SMBI in NBI plasma, while a conventional gas puff (GP) fueling results in rather flat profile for the same heating condition. This is qualitatively consistent with the edge density profile reconstructed from an AM microwave reflectometer data. Since the amount of gas to obtain the same increment of the line-averaged density is about 30 - 40% higher in GP compared to SMBI, the expected difference in the neutral density outside the plasma after SMBI or GP might contribute to make the observed different density profile at ∼ 20 ms after the fueling. SMBI can also affect plasma fluctuations. Fast camera observation for filament structure in the edge turbulence has revealed that SMBI can change its rotation direction and/or speed. Similar change is observed at L-H transition in Heliotron J. In addition, recent density fluctuation measurement at different radial positions with a beam-emission spectroscopy (BES) system suggests SMBI affects the fluctuation inside the last-closed flux surface. Here, the observed fluctuation may be some MHD mode relating to high-energy ions. During about 10 ms after SMBI, the fluctuation is not observed in BES data and the Mirnov-coil signal is decreased, suggesting change of excitation condition of the mode. These observations suggest more preferable control scenario of NBI deposition profile toward core heating through ne(r) modification caused by SMBI. (author)
Additional details
Publishing Information
- Imprint Title
- 24. IAEA Fusion Energy Conference. Programme and Book of Abstracts
- Imprint Pagination
- 789 p.
- Journal Page Range
- p. 98
- Report number
- IAEA-CN--197
Conference
- Title
- 24. IAEA Fusion Energy Conference
- Acronym
- FEC 2012
- Dates
- 8-13 Oct 2012
- Place
- San Diego, CA (United States)
INIS
- Country of Publication
- International Atomic Energy Agency (IAEA)
- Country of Input or Organization
- International Atomic Energy Agency (IAEA)
- INIS RN
- 44060399
- Subject category
- S70: PLASMA PHYSICS AND FUSION TECHNOLOGY;
- Resource subtype / Literary indicator
- Conference
- Descriptors DEI
- CONFINEMENT; DEPOSITION; EMISSION SPECTROSCOPY; EXCITATION; FILAMENTS; FLUCTUATIONS; HELIOTRON; INJECTION; INSTALLATION; MAGNETIC SURFACES; MAGNETOHYDRODYNAMICS; MICROWAVE RADIATION; MOLECULAR BEAMS; PERFORMANCE; PITCHES; PLASMA; PLASMA RADIAL PROFILES; TURBULENCE
- Descriptors DEC
- BEAMS; CLOSED PLASMA DEVICES; ELECTROMAGNETIC RADIATION; ENERGY-LEVEL TRANSITIONS; FLUID MECHANICS; HYDRODYNAMICS; INTAKE; MAGNETIC FIELD CONFIGURATIONS; MECHANICS; ORGANIC COMPOUNDS; OTHER ORGANIC COMPOUNDS; RADIATIONS; SPECTROSCOPY; THERMONUCLEAR DEVICES; VARIATIONS
Optional Information
- Secondary number(s)
- EX/P3--07