Peeling-Ballooning Model: Difference between revisions
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The Peeling-Ballooning Model is a description of MHD stability in the edge region of tokamaks. It predicts where | The Peeling-Ballooning Model is a description of MHD stability in the edge region of tokamaks. It predicts operational regimes where pedestal pressure and bootstrap current lead to peeling unstable or ballooning unstable modes | ||
<ref> | <ref>J.W. Connor et al, ''Magnetohydrodynamic stability of tokamak edge plasmas'', [[doi:10.1063/1.872956|Phys. Plasmas '''5''' (1998) 2687]] | ||
</ref> | </ref> | ||
<ref> | <ref>P.B. Snyder et al, ''Edge localized modes and the pedestal: A model based on coupled peeling–ballooning modes'', [[doi:10.1063/1.1449463|Phys. Plasmas '''9''' (2002) 2037]] | ||
</ref>. The peeling-ballooning model is one possible mechanism for the formation of [[Edge Localized Modes]]. | |||
</ref>. | |||
==References== | ==References== | ||
<references/> | <references/> | ||
Latest revision as of 14:45, 3 April 2018
The Peeling-Ballooning Model is a description of MHD stability in the edge region of tokamaks. It predicts operational regimes where pedestal pressure and bootstrap current lead to peeling unstable or ballooning unstable modes [1] [2]. The peeling-ballooning model is one possible mechanism for the formation of Edge Localized Modes.
References
- ↑ J.W. Connor et al, Magnetohydrodynamic stability of tokamak edge plasmas, Phys. Plasmas 5 (1998) 2687
- ↑ P.B. Snyder et al, Edge localized modes and the pedestal: A model based on coupled peeling–ballooning modes, Phys. Plasmas 9 (2002) 2037