Title of article :
Electron cyclotron heating scenario and experimental results in LHD
Author/Authors :
Idei، نويسنده , , H and Kubo، نويسنده , , S and Shimozuma، نويسنده , , T and Sato، نويسنده , , M and Ohkubo، نويسنده , , K and Yoshimura، نويسنده , , Y and Takita، نويسنده , , Y and Kobayashi، نويسنده , , S and Ito، نويسنده , , S and Mizuno، نويسنده , , Y and Tsumori، نويسنده , , K and Ikeda، نويسنده , , K and Notake، نويسنده , , T and Watari، نويسنده , , T and Kaneko، نويسنده , , O and Komori، نويسنده , , A and Yamada، نويسنده , , H and de Vries، نويسنده , , P.C and Goto، نويسنده , , M and Ida، نويسنده , , K and Inagaki، نويسنده , , S and Kado، نويسنده , , S and Kawahata، نويسنده , , K and Kobuchi، نويسنده , , T and Minami، نويسنده , , T and Miyazawa، نويسنده , , J and Morisaki، نويسنده , , T and Morita، نويسنده , , S and Murakami، نويسنده , , S and Muto، نويسنده , , S and Nagayama، نويسنده , , Y and Nakanishi، نويسنده , , H and Narihara، نويسنده , , K and Peterson، نويسنده , , B.J and Sakakibara، نويسنده , , S and Sasao، نويسنده , , H and Sato، نويسنده , , K and Tanaka، نويسنده , , K and Takeiri، نويسنده , , Y and Watanabe، نويسنده , , K.Y and Yamada، نويسنده , , I and Motojima، نويسنده , , O and Fujiwara، نويسنده , , M، نويسنده ,
Issue Information :
روزنامه با شماره پیاپی سال 2001
Pages :
8
From page :
329
To page :
336
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 n̄e=4×1018 m−3. The maximum central electron temperature Te0=3.5 keV is achieved at n̄e=3×1018 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.
Keywords :
Electron cyclotron heating , Wave propagation , Large helical device
Journal title :
Fusion Engineering and Design
Serial Year :
2001
Journal title :
Fusion Engineering and Design
Record number :
2351109
Link To Document :
بازگشت