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Critical for stability of viscoresistive tearing modes
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10.1063/1.2957916
/content/aip/journal/pop/15/7/10.1063/1.2957916
http://aip.metastore.ingenta.com/content/aip/journal/pop/15/7/10.1063/1.2957916
View: Figures

Figures

Image of FIG. 1.
FIG. 1.

Critical as a function of the Prandtl number for the equilibrium . The solid line represents the relation given by Eq. (31), while the crosses are the numerical data.

Image of FIG. 2.
FIG. 2.

Comparison between the original equilibrium function (dashed line) and the modified one (solid line). The modified one agrees perfectly with the original one, apart for the fact that the modified one goes to zero perfectly at the boundary, so satisfying the periodic boundary conditions.

Image of FIG. 3.
FIG. 3.

Critical as function of the Prandtl number for the equilibrium . The solid line represents the relation given by Eq. (31), while the crosses are the numerical data.

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/content/aip/journal/pop/15/7/10.1063/1.2957916
2008-07-21
2014-04-20
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752b84549af89a08dbdd7fdb8b9568b5 journal.articlezxybnytfddd
Scitation: Critical Δ′ for stability of viscoresistive tearing modes
http://aip.metastore.ingenta.com/content/aip/journal/pop/15/7/10.1063/1.2957916
10.1063/1.2957916
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