Plasma and Fusion Research
Volume 5, S2053 (2010)
Regular Articles
- National Institute for Fusion Science, 322-6 Oroshi-cho, Toki, Gifu 509-5292, Japan
- 1)
- UAKEA Fusion Association, Culham Science Center, Oxfordshire OX14 3 DB, United Kingdom
- 2)
- Budker Institute of Nuclear Physics, 630090, Novosibirsk, Russia
- 3)
- Department of Nuclear Engineering, Kyoto University, Kyoto 606-8501, Japan
Abstract
A high ion temperature (Ti) was achieved using a combination of perpendicular and parallel injected neutral beams in the Large Helical Device (LHD). Microturbulence spatial profiles in a high-Ti discharge were measured by two-dimensional phase contrast imaging (2D-PCI) through almost the entire vertical central chord. The 2D-PCI microturbulence spectral ranges covered wavenumbers (k) of 0.1-1 mm−1 and frequencies (f) of 20-500 kHz. The ion thermal conductivity (χi) increased in the entire region with increasing Ti. However, the difference between the experimental and neoclassical values of χi became smaller at ρ < 0.5, where ρ is the normalized position, in the high-Ti phase. Increasing fluctuation was not observed at this location, suggesting improved ion energy transport in this region. On the other hand, at ρ > 0.5, χi deviated from the neoclassical value due to enhancement of the experimental χi and reduction in the neoclassical χi by a positive radial electric field. Increasing turbulence was observed at ρ = 0.6-0.8, with fluctuations likely propagated to the ion diamagnetic direction in the plasma frame, suggesting that the observed turbulence degrades the ion energy transport at this location in the high-Ti phase.
Keywords
LHD, turbulence, phase contrast imaging, ion temperature gradient mode, neoclassical transport
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References
- [1] O. Kaneko et al., Plasma Fusion Res. 4, 027 (2009).
- [2] K. Ida et al., Phys. Plasmas 16, 056111 (2009).
- [3] K. Tanaka, C. Michael, L. N. Vyacheslavov et al., Rev. Sci. Instrum. 79, 10E702 (2008).
- [4] H. C. Howe, 1993 Proctr nid user and numerical guide Oak Ridge, Tennesee 37831 Oak ridge national laboratory.
- [5] C. D. Beidler and W. N. G. Hitchon, Plasma Phys. Control. Fusion 36, 317 (1994).
- [6] H. E. Mynick and W. N. G. Hitchon, Nucl. Fusion 23, 1053 (1983).
- [7] K. Tanaka et al., Fusion Sci. Tech. 51, 97 (2007).
- [8] T. H. Watanabe et al., Nucl. Fusion 47, 1383 (2007).
This paper may be cited as follows:
Kenji TANAKA, Clive MICHAEL, Leonid VYACHESLAVOV, Hisamichi FUNABA, Masayuki YOKOYAMA, Katsumi IDA, Mikiro YOSHINUMA, Kenichi NAGAOKA, Sadayoshi MURAKAMI, Arimitsu WAKASA, Takeshi IDO, Akihiro SHIMIZU, Masaki NISHIURA, Yasuhiko TAKEIRI, Osamu KANEKO, Katsuyoshi TSUMORI, Katsunori IKEDA, Masaki OSAKABE, Kazuo KAWAHATA and LHD Experiment Group, Plasma Fusion Res. 5, S2053 (2010).