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  • The penetration dynamics of the resonant magnetic perturbation (RMP) field is simulated in the full toroidal geometry, under realistic plasma conditions in MAST experiments. The physics associated with several aspects of the RMP penetration-the plasma response and rotational screening, the resonant and non-resonant torques and the toroidal momentum balance-are highlighted. In particular, the plasma response is found to significantly amplify the non-resonant component of the RMP field for some of the MAST plasmas. A fast rotating plasma, in response to static external magnetic fields, experiences a more distributed electromagnetic torque due to the resonance with continuum waves in the plasma. At fast plasma flow (such as for the MAST plasma), the electromagnetic torque is normally dominant over the neoclassical toroidal viscous (NTV) torque. However, at sufficiently slow plasma flow, the NTV torque can play a significant role in the toroidal momentum balance, thanks to the precession
  • The penetration dynamics of the resonant magnetic perturbation (RMP) field is simulated in the full toroidal geometry, under realistic plasma conditions in MAST experiments. The physics associated with several aspects of the RMP penetration-the plasma response and rotational screening, the resonant and non-resonant torques and the toroidal momentum balance-are highlighted. In particular, the plasma response is found to significantly amplify the non-resonant component of the RMP field for some of the MAST plasmas. A fast rotating plasma, in response to static external magnetic fields, experiences a more distributed electromagnetic torque due to the resonance with continuum waves in the plasma. At fast plasma flow (such as for the MAST plasma), the electromagnetic torque is normally dominant over the neoclassical toroidal viscous (NTV) torque. However, at sufficiently slow plasma flow, the NTV torque can play a significant role in the toroidal momentum balance, thanks to the precession (en)
Title
  • Toroidal modeling of plasma response and resonant magnetic perturbation field penetration
  • Toroidal modeling of plasma response and resonant magnetic perturbation field penetration (en)
skos:prefLabel
  • Toroidal modeling of plasma response and resonant magnetic perturbation field penetration
  • Toroidal modeling of plasma response and resonant magnetic perturbation field penetration (en)
skos:notation
  • RIV/61389021:_____/12:00388717!RIV13-AV0-61389021
http://linked.open...avai/predkladatel
http://linked.open...avai/riv/aktivita
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  • Z(AV0Z20430508)
http://linked.open...iv/cisloPeriodika
  • 12
http://linked.open...vai/riv/dodaniDat
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  • 174637
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  • RIV/61389021:_____/12:00388717
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  • tokamak; resonant magnetic perturbation; neoclassical toroidal viscosity (en)
http://linked.open.../riv/klicoveSlovo
http://linked.open...odStatuVydavatele
  • GB - Spojené království Velké Británie a Severního Irska
http://linked.open...ontrolniKodProRIV
  • [B1FD5CB230F5]
http://linked.open...i/riv/nazevZdroje
  • Plasma Physics and Controlled Fusion
http://linked.open...in/vavai/riv/obor
http://linked.open...ichTvurcuVysledku
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http://linked.open...UplatneniVysledku
http://linked.open...v/svazekPeriodika
  • 54
http://linked.open...iv/tvurceVysledku
  • Sun, Y.
  • Kirk, A.
  • Cahyna, Pavel
  • Denner, P.
  • Liu, Y. Q.
  • Nardon, E.
  • Chapman, I. T.
  • Harrison, J. R.
  • Fishpool, G.
  • Garofalo, A. M.
http://linked.open...ain/vavai/riv/wos
  • 000312579500016
http://linked.open...n/vavai/riv/zamer
issn
  • 0741-3335
number of pages
http://bibframe.org/vocab/doi
  • 10.1088/0741-3335/54/12/124013
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