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Electron cyclotron heating scenario and experimental results in LHD

Authors :
S. Kubo
Kazutaka Ikeda
O. Motojima
Y. Takeiri
Satoshi Ito
Sadayoshi Murakami
Osamu Kaneko
Y. Nagayama
Hiroshi Yamada
Satoru Kobayashi
K. Narihara
Y. Takita
P. de Vries
M. Sato
Sadatsugu Muto
B.J. Peterson
Shigeru Inagaki
H. Sasao
Y. Yoshimura
Tomohiro Morisaki
Takashi Notake
Shinichiro Kado
Hiroshi Idei
Hideya Nakanishi
Satoru Sakakibara
S. Morita
Katsumi Ida
Kazuo Kawahata
A. Komori
Yoshinori Mizuno
K.Y. Watanabe
Kuninori Sato
T. Kobuchi
Ichihiro Yamada
T. Watari
J. Miyazawa
T. Shimozuma
Motoshi Goto
Kunizo Ohkubo
Masami Fujiwara
Katsuyoshi Tsumori
T. Minami
Kenji Tanaka
Source :
Fusion Engineering and Design. 53:329-336
Publication Year :
2001
Publisher :
Elsevier BV, 2001.

Abstract

A large helical device (LHD) experiment began at the end of March 1998. Fundamental and second harmonic electron cyclotron heating (ECH) are used as a plasma production and heating method with six gyrotrons whose frequencies are 82.6/84 and 168 GHz, respectively. Up to 0.9 MW power has been injected in LHD with long distance corrugated waveguide transmission systems. The maximum pulse width is achieved to 3.0 s/240 kW for the LHD experiments. Six antenna systems have been prepared at the horizontally and vertically elongated poloidal sections. The maximum stored energy using all six gyrotrons is 70 kJ at the averaged density of n e = 4 × 10 18 m -3 . The maximum central electron temperature T e0 = 3.5 keV is achieved at n e = 3 × 10 18 m -3 . The magnetic field structure in heliotron type devices like LHD, notably near the coil, is complicated. For this oblique injection, a wave is launched from the antenna, and then crosses the plasma in the complex field structure near the coil. The polarization ellipse of the wave is changed along the ray-path. The wave propagation in heliotron type devices has been analyzed in an ideal case that the magnetic field component along the propagation direction can be neglected. Even for perpendicular injection with our antenna systems, the field component along the propagation direction is not so small. Another treatment of the wave-propagation is introduced. Some calculations for the heating scenario with this treatment are shown.

Details

ISSN :
09203796
Volume :
53
Database :
OpenAIRE
Journal :
Fusion Engineering and Design
Accession number :
edsair.doi...........70fc69311d4bcdea52f7ddbfcf22977f
Full Text :
https://doi.org/10.1016/s0920-3796(00)00505-6