On the criteria guiding the design of the upper electron-cyclotron launcher for ITER
Electron cyclotron waves injected from an antenna located in the upper part of the vessel will be employed in ITER to controlMHD instabilities, particularly neoclassical tearingmodes (NTMs). The derivation of the NTM stabilization criteria used up to now to guide the optimization of the launcher is...
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2015-01-01
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Series: | EPJ Web of Conferences |
Online Access: | http://dx.doi.org/10.1051/epjconf/20158701008 |
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doaj-60f9f9b1fd7d41a6b982b557266b25c72021-08-02T06:01:07ZengEDP SciencesEPJ Web of Conferences2100-014X2015-01-01870100810.1051/epjconf/20158701008epjconf_ec2015_01008On the criteria guiding the design of the upper electron-cyclotron launcher for ITERPoli E.0Angioni C.1Casson F. J.2Farina D.3Figini L.4Goodman T. P.5Maj O.6Sauter O.7Weber H.8Zohm H.9Saibene G.10Henderson M. A.11Max-Planck-Institut für PlasmaphysikMax-Planck-Institut für PlasmaphysikMax-Planck-Institut für PlasmaphysikIstituto di Fisica del Plasma CNR, EURATOM-ENEA-CNR AssociationIstituto di Fisica del Plasma CNR, EURATOM-ENEA-CNR AssociationCentre de Recherches en Physique des Plasmas, CRPP-EPFLMax-Planck-Institut für PlasmaphysikCentre de Recherches en Physique des Plasmas, CRPP-EPFLMax-Planck-Institut für PlasmaphysikMax-Planck-Institut für PlasmaphysikFusion for EnergyITER Organization Electron cyclotron waves injected from an antenna located in the upper part of the vessel will be employed in ITER to controlMHD instabilities, particularly neoclassical tearingmodes (NTMs). The derivation of the NTM stabilization criteria used up to now to guide the optimization of the launcher is reviewed in this paper and their range of validity elucidated. Possible effects leading to a deterioration of the predicted performance through a broadening of the EC deposition profile are discussed. The most detrimental effect will likely be the scattering of the EC beams from density fluctuations, resulting in a beam broadening in the 100% range. The combined impact of these effects with that of beam misalignment (with respect to the targeted surface) is discussed for a time slice of the standard Q = 10 H-mode scenario. http://dx.doi.org/10.1051/epjconf/20158701008 |
collection |
DOAJ |
language |
English |
format |
Article |
sources |
DOAJ |
author |
Poli E. Angioni C. Casson F. J. Farina D. Figini L. Goodman T. P. Maj O. Sauter O. Weber H. Zohm H. Saibene G. Henderson M. A. |
spellingShingle |
Poli E. Angioni C. Casson F. J. Farina D. Figini L. Goodman T. P. Maj O. Sauter O. Weber H. Zohm H. Saibene G. Henderson M. A. On the criteria guiding the design of the upper electron-cyclotron launcher for ITER EPJ Web of Conferences |
author_facet |
Poli E. Angioni C. Casson F. J. Farina D. Figini L. Goodman T. P. Maj O. Sauter O. Weber H. Zohm H. Saibene G. Henderson M. A. |
author_sort |
Poli E. |
title |
On the criteria guiding the design of the upper electron-cyclotron launcher for ITER |
title_short |
On the criteria guiding the design of the upper electron-cyclotron launcher for ITER |
title_full |
On the criteria guiding the design of the upper electron-cyclotron launcher for ITER |
title_fullStr |
On the criteria guiding the design of the upper electron-cyclotron launcher for ITER |
title_full_unstemmed |
On the criteria guiding the design of the upper electron-cyclotron launcher for ITER |
title_sort |
on the criteria guiding the design of the upper electron-cyclotron launcher for iter |
publisher |
EDP Sciences |
series |
EPJ Web of Conferences |
issn |
2100-014X |
publishDate |
2015-01-01 |
description |
Electron cyclotron waves injected from an antenna located in the upper part of the vessel will be employed in ITER to controlMHD instabilities, particularly neoclassical tearingmodes (NTMs). The derivation of the NTM stabilization criteria used up to now to guide the optimization of the launcher is reviewed in this paper and their range of validity elucidated. Possible effects leading to a deterioration of the predicted performance through a broadening of the EC deposition profile are discussed. The most detrimental effect will likely be the scattering of the EC beams from density fluctuations, resulting in a beam broadening in the 100% range. The combined impact of these effects with that of beam misalignment (with respect to the targeted surface) is discussed for a time slice of the standard Q = 10 H-mode scenario.
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url |
http://dx.doi.org/10.1051/epjconf/20158701008 |
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