2003
DOI: 10.1134/1.1538502
|View full text |Cite
|
Sign up to set email alerts
|

Numerical simulations of tangential microwave launching for EC heating in a tokamak

Help me understand this report

Search citation statements

Order By: Relevance

Paper Sections

Select...
1
1
1
1

Citation Types

0
19
0

Year Published

2006
2006
2016
2016

Publication Types

Select...
9

Relationship

2
7

Authors

Journals

citations
Cited by 14 publications
(19 citation statements)
references
References 10 publications
0
19
0
Order By: Relevance
“…far from the cut-off, the finite derivatives of the weakly relativistic Hamiltonian do not produce any significant error. This result has been supported by the benchmark against the WR RTC code [49]. Furthermore, in most typical ECRH/ECCD scenarios for tokamaks and stellarators, where the kinetic effects in wave propagation are negligible, the "cold" Hamiltonian can be applied.…”
Section: Ray-tracing Equationsmentioning
confidence: 61%
“…far from the cut-off, the finite derivatives of the weakly relativistic Hamiltonian do not produce any significant error. This result has been supported by the benchmark against the WR RTC code [49]. Furthermore, in most typical ECRH/ECCD scenarios for tokamaks and stellarators, where the kinetic effects in wave propagation are negligible, the "cold" Hamiltonian can be applied.…”
Section: Ray-tracing Equationsmentioning
confidence: 61%
“…The TRAVIS code has been benchmarked against the old W7-AS code [10], the code WR RTC [19] and the code TORBEAM [20]. Additionally, the code was successfully tested on the ITER reference Scenario-2 [15] against several other predictions collected by R. Prater [6,7] (the results of this benchmark are not included in the cited papers).…”
Section: Description Of the Travis Codementioning
confidence: 99%
“…contours is fairly small [37,38] (small gradient of B along the rays) leading to high absorption, and the deposition is very sensitive to small changes of B, but also to the local electron temperatures due to the relativistic down-shift of the resonant cyclotron frequency (this effect is expected to be very important for the CERC scenarios at LHD with the very high T e , but low n e ). An "anomalous dispersion" effect [39], which can lead to the bending of the rays away from the resonance and is only obtained in the tracing with the weakly relativistic (hot) dispersion [40], is negligible for the low densities in LHD. Ray-tracing calculations [38,41] for the LHD inward-shifted configurations (with fairly high B-gradient along the rays, i.e.…”
Section: B Ech Operation Modes and Depositionmentioning
confidence: 99%