Effect of Toroidal Current on Rotational Transform Profile by MHD Activity Measurement in Heliotron J
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概要
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The effect of toroidal current on the rotational transform was investigated in Heliotron J by measuring magnetohydrodynamic (MHD) activities at two configurations with a rotational transform (ι/2π) close to 0.5. The resonant m/n = 2/1 mode was observed in an ECH + co-NBI plasma in the configuration with ι/2π = 0.48 at ρ = 0.7. Here, m and n are the poloidal and toroidal mode numbers, respectively. ρ is the normalized minor radius. The rotational transform is increased presumably due to the toroidal current. The location of the ι/2π = 0.50 rational surface was determined to be ρ = 0.8-0.9 by soft X-ray (SX) fluctuations related to the MHD mode. An equilibrium calculation considering the toroidal current showed that the increase in the rotational transform due to the toroidal current was consistent with experimental results. The resonant mode structure was also investigated in an ECH + counter-NBI plasma at the ι/2π = 0.50 configuration. The location of the ι/2π = 0.50 rational surface, as determined by SX signals, did not change significantly compared with that obtained under a vacuum configuration. There is no significant difference between the rotational transform profile that considers toroidal currents by equilibrium calculation and that of the vacuum configuration. These results suggest that the change in the rotational transform profile caused by the toroidal current was small, owing to the balance between the bootstrap current and counter-flowing NB driven current.
著者
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SAKAKIBARA Satoru
National Insitute for Fusion Science
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WATANABE Kiyomasa
National Insitute for Fusion Science
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Mizuuchi Tohru
Institute Of Advanced Energy Kyoto University
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Hanatani Kiyoshi
Institute Of Advanced Energy Kyoto University
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NAGASAKI Kazunobu
Institute of Advanced Energy, Kyoto University
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OKADA Hiroyuki
Institute of Advanced Energy, Kyoto University
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KONDO Katsumi
Graduate School of Energy Science, Kyoto University
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Suzuki Yasuhiro
National Agriculture And Food Res. Organization (naro) National Inst. Of Crop Sci.
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Nakamura Yuji
Graduate School Of Energy Science Kyoto University
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Kobayashi Shinji
Institute Of Advanced Energy Kyoto Univ.
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Watanabe Shinya
Graduate School of Dentistry (First Department of Oral and Maxillofacial Surgery), Osaka Dental University
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ARIMOTO Hajime
Graduate School of Energy Science, Kyoto Univ., Gokasho, Uji 611-0011, Japan
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MOTOJIMA Gen
Graduate School of Energy Science, Kyoto Univ., Gokasho, Uji 611-0011, Japan
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SANO Fumimichi
Institute of Advance Energy, Kyoto University
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SANO Fumimichi
Institute of Advanced Energy, Kyoto University, Uji 611-0011, Japan
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BLACKWELL Boyd
Plasma Research Laboratory, Research School of Physical Sciences and Engineering, The Australian National University, Canberra ACT 0200, Australia
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YAMAMOTO Satoshi
Kyoto University Pioneering Research Unit for Next Generation, Uji 611-0011, Japan
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KONDO Katsumi
Graduate School of Energy Science, Kyoto Univ., Gokasho, Uji 611-0011, Japan
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YAMAMOTO Satoshi
Kyoto University Pioneering Research Unit for Next Generation, Gokasho, Uji 611-0011, Japan
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HANATANI Kiyoshi
Institute of Advanced Energy, Kyoto University, Uji 611-0011, Japan
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NAGASAKI Kazunobu
Institute of Advanced Energy, Kyoto University, Uji 611-0011, Japan
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NAGASAKI Kazunobu
Institute of Advance Energy, Kyoto University
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MIZUUCHI Tohru
Institute of Advance Energy, Kyoto University
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MIZUUCHI Tohru
Institute of Advanced Energy, Kyoto University, Uji 611-0011, Japan
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OKADA Hiroyuki
Institute of Advance Energy, Kyoto University
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KOBAYASHI Shinji
Institute of Advance Energy, Kyoto University
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