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2019
DOI: 10.1002/asna.201913644
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Stability of a force‐free Hall equilibrium and release of magnetic energy

Abstract: Conservation of magnetic helicity by the Hall drift does not prevent Hall instability of helical fields. This conclusion follows from stability analysis of a force‐free spatially periodic Hall equilibrium. The growth rates of the instability scale as σ ∝ B3/4η1/4 with the field strength B and magnetic diffusivity η and can be large compared to the rate of resistive decay of the background field. The instability deviates the magnetic field from the force‐free configuration. The unstable eigenmodes include a fin… Show more

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Cited by 6 publications
(6 citation statements)
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References 23 publications
(38 reference statements)
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“…This heuristic condition for the instability is satisfied by any force-free field of ∇ × B = α(r)B. Instability of a 1-D force-free field with maximum helicity was confirmed by Kitchatinov (2019). The instability can be active with the force-free fields of the solar corona where the Hall number R H ∼ 10 7 is large.…”
Section: Discussionmentioning
confidence: 78%
See 1 more Smart Citation
“…This heuristic condition for the instability is satisfied by any force-free field of ∇ × B = α(r)B. Instability of a 1-D force-free field with maximum helicity was confirmed by Kitchatinov (2019). The instability can be active with the force-free fields of the solar corona where the Hall number R H ∼ 10 7 is large.…”
Section: Discussionmentioning
confidence: 78%
“…A decrease of the field scale cannot therefore be balanced by diffusion. Release of magnetic energy on the nonlinear stage of the instability proceeds in a sequence of spikes or bursts, where each spike releases several percent of magnetic energy (Kitchatinov 2017(Kitchatinov , 2019.…”
Section: Discussionmentioning
confidence: 99%
“…Closely related to this feature is the idea of a Hall equilibrium-a magnetic field configuration where the Hall term is identically equal to zero. Such equilibria were first proposed by [71], and have been extensively studied further [65,66,72,73]. In most of these works, the field is computed directly from the requirement that the Hall term ∇ × 1 4πen e (∇ × B) × B = 0, in which case one must additionally consider the question of whether the solution is stable or not.…”
Section: Hall Evolutionmentioning
confidence: 99%
“…These models have successfully addressed observational properties of NSs and they have revealed, moreover, rich effects in terms of magnetohydrodynamical evolution, arising from the non-linear nature of the equations. These effects include instabilities and turbulent cascades and are of broader applications within the realm of magnetohydrodynamics [53][54][55][56][57][58][59][60][61][62][63][64][65][66][67][68].…”
Section: Introductionmentioning
confidence: 99%