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 the parameter space where pedestal pressure and bootstrap current lead to peeling unstable or ballooning unstable modes
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>
[http://link.aip.org/link/?PHPAEN/5/2687/1 J.W. Connor et al, ''Magnetohydrodynamic stability of tokamak edge plasmas'', Phys. Plasmas '''5''' (1998) 2687]
[http://link.aip.org/link/?PHPAEN/5/2687/1 J.W. Connor et al, ''Magnetohydrodynamic stability of tokamak edge plasmas'', Phys. Plasmas '''5''' (1998) 2687]
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<ref>
<ref>
[http://link.aip.org/link/?PHPAEN/9/2037/1 P.B. Snyder et al, ''Edge localized modes and the pedestal: A model based on coupled peeling–ballooning modes'', Phys. Plasmas '''9''' (2002) 2037]
[http://link.aip.org/link/?PHPAEN/9/2037/1 P.B. Snyder et al, ''Edge localized modes and the pedestal: A model based on coupled peeling–ballooning modes'', Phys. Plasmas '''9''' (2002) 2037]
</ref>. Therefore the peeling-ballooning model is one possible mechanism for the formation of [[Edge Localized Modes]].  
</ref>. The peeling-ballooning model is one possible mechanism for the formation of [[Edge Localized Modes]].  




==References==
==References==
<references/>
<references/>

Revision as of 23:58, 3 October 2013

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