TJ-II:Electron Bernstein Wave Heating: Difference between revisions
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The system is located in [[TJ-II:Sectors|sector]] D6. | The system is located in [[TJ-II:Sectors|sector]] D6. | ||
[[File:TJII EBW diagram.jpg|400px|thumb|left|TJ-II Electron Bernstein Wave Heating system diagram.]] | |||
[[File:TJII EBW photo.jpg|400px|thumb|right|TJ-II Electron Bernstein Wave Heating system photo, as viewed from the mounting flange for the heating system corrugated waveguide.]] | |||
==References== | ==References== | ||
<references /> | <references /> | ||
Revision as of 15:51, 4 July 2010
In TJ-II, the possibility of achieving high-density plasmas using Electron Bernstein Wave Heating (EBWH), which has been used successfully in the W7-AS and H-J stellarators, is being explored. [1] [2] It offers a way of overcoming the cut-off density limit associated with ECRH methods (1.7×1019 m-3 in TJ-II). Preliminary studies highlighted several promising EBWH first harmonic schemes, i.e. at 28 GHz. [3]
The system is located in sector D6.
References
- ↑ A. Fernández et al., The design of an electron Bernstein wave heating system for the TJ-II stellarator, Fusion Sci. Tech. 46, pp. 335-341 (2004)
- ↑ A. Fernández et al., Status of the TJ-II Electron Bernstein Waves heating project, Fusion Engineering and Design 74, Issues 1-4 (2005) 325-329
- ↑ F. Castejón et al., Electron Bernstein wave heating calculations for TJII plasmas, Fusion Sci. Tech. 46, pp. 327-334 (2004)