1995
DOI: 10.1016/0022-3115(94)00474-9
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Formation of oscillating perpendicular electric field by AC limiter biasing on HYBTOK-II tokamak

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Cited by 3 publications
(2 citation statements)
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“…In the case of resistive plasmas (Lundquist number S ~ 230), the redistribution of the plasma current due to magnetic field reconnection induced by RHF was predominantly observed [9,10]. We have started a new DED experiment on a small tokamak device, HYBTOK-II [11,12] to study the fundamental processes of DED in a higher-temperature region (S ~ 5000) compared with CSTN-IV. It is expected that the shielding current against the externally excited RHF around the resonance surface will drive the plasma poloidal rotation.…”
Section: Introductionmentioning
confidence: 99%
“…In the case of resistive plasmas (Lundquist number S ~ 230), the redistribution of the plasma current due to magnetic field reconnection induced by RHF was predominantly observed [9,10]. We have started a new DED experiment on a small tokamak device, HYBTOK-II [11,12] to study the fundamental processes of DED in a higher-temperature region (S ~ 5000) compared with CSTN-IV. It is expected that the shielding current against the externally excited RHF around the resonance surface will drive the plasma poloidal rotation.…”
Section: Introductionmentioning
confidence: 99%
“…Recently, a biased electrode was used to actively control MHD mode rotation on the HBT-EP tokamak [19]. Electrode biasing has also been used to achieve the high confinement H-mode regime as was done in the CCT [20] and HBT-EP [21] tokamaks as well as broaden heat loads at the plasma edge as done in the HYBTOK-II [22] and DIII-D [23] tokamaks. Static electrode biasing has been shown to suppress mode amplitudes in several tokamaks [24][25][26][27][28].…”
mentioning
confidence: 99%