2002
DOI: 10.1016/s0010-4655(02)00269-2
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Numerical modeling of the coupling of an ICRH antenna with a plasma with self-consistent antenna currents

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Cited by 35 publications
(30 citation statements)
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“…In a variational formalism used in EVE code (Dumont & Zarzoso 2013) there is no possibility to model the antennaplasma coupling self-consistently, because at this moment the density current on the antenna is fixed and cannot be modified by the current induced on the antenna structure, which is limited to the straps description. To obtain relevant near-field computations, other ways are used to build antenna-plasma coupling codes, for example, Boundary Element Method in ICANT code, and integral method in TOPICA (see (Pécoul et al 2002;Lancellotti et al 2006)). Another one the TORIC code, using spectral decomposition, was also developed to study the ICRH scenarios (Brambilla 1999).…”
Section: Heating Simulationmentioning
confidence: 99%
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“…In a variational formalism used in EVE code (Dumont & Zarzoso 2013) there is no possibility to model the antennaplasma coupling self-consistently, because at this moment the density current on the antenna is fixed and cannot be modified by the current induced on the antenna structure, which is limited to the straps description. To obtain relevant near-field computations, other ways are used to build antenna-plasma coupling codes, for example, Boundary Element Method in ICANT code, and integral method in TOPICA (see (Pécoul et al 2002;Lancellotti et al 2006)). Another one the TORIC code, using spectral decomposition, was also developed to study the ICRH scenarios (Brambilla 1999).…”
Section: Heating Simulationmentioning
confidence: 99%
“…The main ingredient to determine the RF potential along a magnetic field line E is generally computed from conventional antenna codes in the absence of sheaths, i.e., perfect electric conductors are assumed in direct contact with the plasma. This procedure, although clearly not self-consistent, was widely implemented as the only tool able to model realistic wave-launching structures (Pécoul et al 2002;Lancellotti et al 2006). The theoretical background of the SSWICH code that considers sheath boundary condition is in (Colas et al 2012).…”
Section: Contextmentioning
confidence: 99%
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“…Ref. [1][2][3][4]) have been developed for calculation of the coupling to the plasma. However, antenna codes often use simplified plasma models, which do not always consider reflection of the wave.…”
Section: Introductionmentioning
confidence: 99%
“…Since then, there [2][3][4][5][6][7][8][9][10][11][12] have been a number of theoretical studies which have tried to remove various restrictions in the 3-D model mentioned above. In particular, the effects of including feeders [1,7,8] and the antenna configurations [10] have been discussed. In some of these studies [1][2][3][4] it has been pointed out that poloidal power spectrum and radiation pattern are asymmetric.…”
Section: Introductionmentioning
confidence: 99%