1993
DOI: 10.1088/0741-3335/35/sa/008
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Modelling of RF current drive in the presence of radial diffusion

Abstract: The kinetic theory of radiofrequency current drive in to-plasmas is investigated. The problem of the impact of anomalous uansport on the driven current profile and efficiency is considered in detail. b o n g the possible candidates for explaining anomalous transport in tokamaks, magnetic turbulence is known to have a saong influence on the dynamics of snperthemd elecaons and is assumed here to be the basic mechanism responsible for radial diffusion of therf-driven current. The 3-dimensional kinetic equation in… Show more

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Cited by 47 publications
(28 citation statements)
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“…However, it has been observed experimentally Harvey et al (2002); Coda et al (2003); Kirov et al (2002) that the deposition can actually be larger than expected from ECCD/ECRH modeling. This can be due to cross-field diffusion of the fast electrons density (constituting the EC current), for instance because of turbulence on the deposition location, leading to a broadening of the driven current density deposition and therefore to a reduction in the maximum driven current density Giruzzi and Fidone (1989); Giruzzi (1993); Coda et al (2006); Bertelli and Westerhof (2009) ;Bertelli et al (2010). It has also been shown that the electron density fluctuations near the plasma edge, or along the path of the RF-waves, might lead to a broadening of the current deposition as well as a fluctuating power deposition profile Tsironis et al (2009) ;Peysson et al (2011); Decker, J. et al (2012).…”
Section: Introductionmentioning
confidence: 99%
“…However, it has been observed experimentally Harvey et al (2002); Coda et al (2003); Kirov et al (2002) that the deposition can actually be larger than expected from ECCD/ECRH modeling. This can be due to cross-field diffusion of the fast electrons density (constituting the EC current), for instance because of turbulence on the deposition location, leading to a broadening of the driven current density deposition and therefore to a reduction in the maximum driven current density Giruzzi and Fidone (1989); Giruzzi (1993); Coda et al (2006); Bertelli and Westerhof (2009) ;Bertelli et al (2010). It has also been shown that the electron density fluctuations near the plasma edge, or along the path of the RF-waves, might lead to a broadening of the current deposition as well as a fluctuating power deposition profile Tsironis et al (2009) ;Peysson et al (2011); Decker, J. et al (2012).…”
Section: Introductionmentioning
confidence: 99%
“…2(a) have been performed, using a 3D relativistic Fokker-Planck code [22], and focusing the comparison on the synergy factor F syn . The measured temperature and density profiles as well as other experimental parameters are used as an input to the Fokker-Planck code.…”
mentioning
confidence: 99%
“…The identification of the physical phenomena corresponding to each time scale implies a comparison with detailed theoretical models, in this case with the 3D kinetic theory of the tail formation and relaxation in the presence of Coulomb collisions, radial diffusion, rf waves, and dc electric field. This has been performed using a sophisticated computational model including a 3D time-dependent Fokker-Planck code (for the evaluation of the electron distribution function), coupled to a radiation code for the evaluation of the corresponding ECE and ECA outputs in a realistic geometry [6]. This comparison demonstrates that in a large machine the relaxation of fast electrons is dominated by Coulomb collisions, in contrast with small tokamaks, where radial diffusion plays a comparable or even dominant role [7].…”
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confidence: 99%