Formation of electron internal transport barrier and achievement of high ion temperature in Large Helical Device
Creators
- Takeiri, Y.1, 2, 3, 4, 5, 6
- Shimozuma, T.1, 2, 3, 4, 5, 6
- Kubo, S.1, 2, 3, 4, 5, 6
- Morita, S.1, 2, 3, 4, 5, 6
- Osakabe, M.1, 2, 3, 4, 5, 6
- Kaneko, O.1, 2, 3, 4, 5, 6
- Tsumori, K.1, 2, 3, 4, 5, 6
- Oka, Y.1, 2, 3, 4, 5, 6
- Ikeda, K.1, 2, 3, 4, 5, 6
- Nagaoka, K.1, 2, 3, 4, 5, 6
- Ohyabu, N.1, 2, 3, 4, 5, 6
- Ida, K.1, 2, 3, 4, 5, 6
- Yokoyama, M.1, 2, 3, 4, 5, 6
- Miyazawa, J.1, 2, 3, 4, 5, 6
- Goto, M.1, 2, 3, 4, 5, 6
- Narihara, K.1, 2, 3, 4, 5, 6
- Yamada, I.1, 2, 3, 4, 5, 6
- Idei, H.1, 2, 3, 4, 5, 6
- Yoshimura, Y.1, 2, 3, 4, 5, 6
- Ashikawa, N.1, 2, 3, 4, 5, 6
- and others
- 1. Graduate School of Frontier Sciences, The University of Tokyo, Tokyo 113-0033 (Japan)
- 2. Graduate School of Energy Science, Kyoto University, Uji 611-0011 (Japan)
- 3. Department of Fusion Science, School of Mathematical and Physical Science, Graduate University for Advanced Studies, Hayama 240-0193 (Japan)
- 4. Research Laboratory for Nuclear Reactors, Tokyo Institute of Technology, Tokyo 152-8550 (Japan)
- 5. Department of Energy Engineering and Science, Nagoya University, Nagoya 464-8603 (Japan)
- 6. National Institute for Fusion Science, Toki 509-5292 (Japan)
Description
An internal transport barrier (ITB) was observed in the electron temperature profile in the Large Helical Device [O. Motojima et al., Phys. Plasmas 6, 1843 (1999)] with a centrally focused intense electron cyclotron resonance microwave heating. Inside the ITB the core electron transport was improved, and a high electron temperature, exceeding 10 keV in a low density, was achieved in a collisionless regime. The formation of the electron-ITB is correlated with the neoclassical electron root with a strong radial electric field determined by the neoclassical ambipolar flux. The direction of the tangentially injected beam-driven current has an influence on the electron-ITB formation. For the counter-injected target plasma, a steeper temperature gradient, than that for the co-injected one, was observed. As for the ion temperature, high-power NBI (neutral beam injection) heating of 9 MW has realized a central ion temperature of 5 keV with neon injection. By introducing neon gas, the NBI absorption power was increased in low-density plasmas and the direct ion heating power was much enhanced with a reduced number of ions, compared with hydrogen plasmas
Additional details
Identifiers
- DOI
- 10.1063/1.1560613;
Publishing Information
- Journal Title
- Physics of Plasmas
- Journal Volume
- 10
- Journal Issue
- 5
- Journal Page Range
- p. 1788-1795
- ISSN
- 1070-664X
- CODEN
- PHPAEN
Conference
- Title
- 44. annual meeting of the Division of Plasma Physics of the American Physical Society
- Dates
- 11-15 Nov 2002
- Place
- Ontario, FL (United States)
INIS
- Country of Publication
- United States
- Country of Input or Organization
- International Atomic Energy Agency (IAEA)
- INIS RN
- 35034032
- Subject category
- S70: PLASMA PHYSICS AND FUSION TECHNOLOGY;
- Resource subtype / Literary indicator
- Conference
- Descriptors DEI
- BEAM INJECTION HEATING; CHARGED-PARTICLE TRANSPORT; ECR HEATING; ELECTRON TEMPERATURE; ION TEMPERATURE; LHD DEVICE; MAGNETIC CONFINEMENT; NEUTRAL ATOM BEAM INJECTION; PLASMA CONFINEMENT; PLASMA DENSITY; TOROIDAL CONFIGURATION
- Descriptors DEC
- ANNULAR SPACE; BEAM INJECTION; CLOSED CONFIGURATIONS; CLOSED PLASMA DEVICES; CONFIGURATION; CONFINEMENT; HEATING; HIGH-FREQUENCY HEATING; MAGNETIC FIELD CONFIGURATIONS; PLASMA CONFINEMENT; PLASMA HEATING; RADIATION TRANSPORT; SPACE; THERMONUCLEAR DEVICES
Optional Information
- Notes
- (c) 2003 American Institute of Physics.