| Issue |
EPJ Web Conf.
Volume 157, 2017
22 Topical Conference on Radio-Frequency Power in Plasmas
|
|
|---|---|---|
| Article Number | 03020 | |
| Number of page(s) | 4 | |
| Section | Standard Papers | |
| DOI | https://doi.org/10.1051/epjconf/201715703020 | |
| Published online | 23 October 2017 | |
https://doi.org/10.1051/epjconf/201715703020
Sequential modelling of ICRF wave near RF fields and asymptotic RF sheaths description for AUG ICRF antennas
1 Max-Planck-Institut für Plasmaphysik, Boltzmannstrasse 2, D-85748 Garching, Germany
2 Ghent University, Sint-Pietersnieuwstraat 41, Gent, Belgium
3 CEA, IRFM, F-13108 Saint Paul-lez-Durance, France
* e-mail: wouter.tierens@ipp.mpg.de
Published online: 23 October 2017
A sequence of simulations is performed with RAPLICASOL and SSWICH to compare two AUG ICRF antennas. RAPLICASOL outputs have been used as input to SSWICH-SW for the AUG ICRF antennas. Using parallel electric field maps and the scattering matrix produced by RAPLICASOL, SSWICH-SW, reduced to its asymptotic part, is able to produce a 2D radial/poloidal map of the DC plasma potential accounting for the antenna input settings (total power, power balance, phasing). Two models of antennas are compared: 2-strap antenna vs 3-strap antenna. The 2D DC potential structures are correlated to structures of the parallel electric field map for different phasing and power balance. The overall DC plasma potential on the 3-strap antenna is lower due to better global RF currents compensation. Spatial proximity between regions of high RF electric field and regions where high DC plasma potentials are observed is an important factor for sheath rectification.
© The authors, published by EDP Sciences, 2017
This is an Open Access article distributed under the terms of the Creative Commons Attribution License 4.0, which permits unrestricted use, distribution, and reproduction in any medium, provided the original work is properly cited.
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