TJ-II:Electron Cyclotron Resonant Heating: Difference between revisions
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<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 | 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. | ||
Revision as of 10:33, 6 August 2009
TJ-II disposes of two gyrotrons for Electron Cyclotron Resonance Heating (ECRH). [1] The power is delivered to the sector B3. The gyrotron frequency is f = 53.2 GHz, tuned to the 2nd harmonic, X-mode polarisation. The total power that can be delivered to the plasma is PECRH ≤ 600 kW. The gyrotrons can be modulated.