4,378
edits
TJ-II:Electron Cyclotron Resonant Heating: Difference between revisions
TJ-II:Electron Cyclotron Resonant Heating (view source)
Revision as of 10:33, 6 August 2009
, 6 August 2009no edit summary
No edit summary |
mNo edit summary |
||
| Line 3: | Line 3: | ||
<ref>[http://dx.doi.org/10.1109/ICIMW.2000.892950 A. Fernandez et al, ''Design of the upgraded TJ-II quasi-optical transmission line'', Conference Digest, 25<sup>th</sup> International Conference on Infrared and Millimeter Waves (2000) 91 - 92]</ref> | <ref>[http://dx.doi.org/10.1109/ICIMW.2000.892950 A. Fernandez et al, ''Design of the upgraded TJ-II quasi-optical transmission line'', Conference Digest, 25<sup>th</sup> International Conference on Infrared and Millimeter Waves (2000) 91 - 92]</ref> | ||
The power is delivered to the [[TJ-II:Sectors|sector]] B3. | The power is delivered to the [[TJ-II:Sectors|sector]] B3. | ||
The gyrotron frequency is f=53.2 GHz, tuned to the 2<sup>nd</sup> harmonic, X-mode polarisation. | The gyrotron frequency is ''f''=53.2 GHz, tuned to the 2<sup>nd</sup> harmonic, X-mode polarisation. | ||
The total power that can be delivered to the plasma is ''P<sub>ECRH</sub>'' ≤ 600 kW. | The total power that can be delivered to the plasma is ''P<sub>ECRH</sub>'' ≤ 600 kW. | ||
The gyrotrons can be modulated. | The gyrotrons can be modulated. | ||