2005
DOI: 10.1016/j.physleta.2005.06.002
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Plasma vortexes induced by an external rotating helical magnetic perturbation in tokamaks

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Cited by 3 publications
(11 citation statements)
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“…In these experiments it was found that |B ∼ r | was amplified almost over the whole radial range by up to a few ten per cent of the vacuum field, while |B ∼ θ | was attenuated at around the resonant surface and amplified at r < 6.5 cm. Our calculations show that in these experiments a very wide interaction region occurred ( figure 1(a)) and the plasma response was not so strong (see also [11]).…”
Section: Tokamaks Cstn-iv and Hybtok-iimentioning
confidence: 59%
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“…In these experiments it was found that |B ∼ r | was amplified almost over the whole radial range by up to a few ten per cent of the vacuum field, while |B ∼ θ | was attenuated at around the resonant surface and amplified at r < 6.5 cm. Our calculations show that in these experiments a very wide interaction region occurred ( figure 1(a)) and the plasma response was not so strong (see also [11]).…”
Section: Tokamaks Cstn-iv and Hybtok-iimentioning
confidence: 59%
“…In that paper the analytic solution of equations (9) and (10) was found assuming that the vacuum DED coil perturbation of the magnetic field plays a dominant role and the plasma response is small. But for f = 10 kHz and f = 20 kHz the plasma response is very strong and the approximations of the paper [11] are not valid.…”
Section: Textor-dedmentioning
confidence: 90%
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“…The first nonlinearity enters in the conventional way namely due to the nonlinear terms of the equation. It has been estimated by Pankratov et al [23], that the nonlinear terms become important for a DED current higher than 5 kA. It is expected that the nonlinearities lead to a growth of modes as, e.g.…”
Section: Discussionmentioning
confidence: 97%