4,415
edits
TJ-II:Electron Cyclotron Emission: Difference between revisions
Jump to navigation
Jump to search
TJ-II:Electron Cyclotron Emission (view source)
Revision as of 11:35, 28 October 2009
, 28 October 2009no edit summary
No edit summary |
No edit summary |
||
| Line 2: | Line 2: | ||
by means of a 16 channel heterodyne radiometer, | by means of a 16 channel heterodyne radiometer, | ||
covering the frequency range 50–60 GHz, corresponding to the second harmonic of electron cyclotron emission (ECE) in X-mode polarization at a magnetic field of 0.95 T on the plasma axis. | covering the frequency range 50–60 GHz, corresponding to the second harmonic of electron cyclotron emission (ECE) in X-mode polarization at a magnetic field of 0.95 T on the plasma axis. | ||
The measurements are performed from the low field side (LFS) in the horizontal midplane. | The measurements are performed from the low field side (LFS) in the horizontal midplane ([[TJ-II:Sectors|sector]] C4). | ||
Each frequency corresponds to a different value of the major radius ''R''. | Each frequency corresponds to a different value of the major radius ''R''. | ||
The system is operated close to the strong [[TJ-II:Electron Cyclotron Resonant Heating|ECR heating source]] (f<sub>ECRH</sub> = 53.2 GHz). | The system is operated close to the strong [[TJ-II:Electron Cyclotron Resonant Heating|ECR heating source]] (f<sub>ECRH</sub> = 53.2 GHz). | ||