2005
DOI: 10.1051/0004-6361:20041624
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A stability property of a force-free surface bounding a vacuum gap

Abstract: Abstract.A force-free surface (FFS) S is a sharp boundary separating a void from a region occupied by a charge-separated force-free plasma. It is proven here under very general assumptions that there is on S a simple relation between the charge density µ on the plasma side and the derivative of δ = E · B along B on the vacuum side (with E denoting the electric field and B the magnetic field). Combined with the condition δ = 0 on S, this relation implies that a FFS has a general stability property, already conj… Show more

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Cited by 4 publications
(3 citation statements)
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“…The quasi-static dynamics of coronal fields is often modeled as a sequence of instabilities followed by relaxation and current sheets formation (Ng & Bhattacharjee 1998), in which equilibria play an important role (Aly 2005).…”
Section: Discussionmentioning
confidence: 99%
“…The quasi-static dynamics of coronal fields is often modeled as a sequence of instabilities followed by relaxation and current sheets formation (Ng & Bhattacharjee 1998), in which equilibria play an important role (Aly 2005).…”
Section: Discussionmentioning
confidence: 99%
“…Note that Eq. (15) imposes σE < 0 just above Σ (with E the component of E along B), while in a true equilibrium electrosphere we would have µE > 0 just above the upper surface of the equatorial belt (approximated by Σ in our model) where the volume charge density is µ (see Aly 2005, for a general proof of this statement). However, this should not cause too much trouble here, as the problems we are interested in are essentially dominated by the radial structure of the electric field (remember that we do not allow vertical distortions of Σ).…”
Section: Some Relations For the Electrostatic Potential And Fieldmentioning
confidence: 84%
“…On the force-free side, the charges ensure that E = 0 (and if any lapse in shielding occurs, the electric field direction is such that it drives charges towards the trap surface, which is why the cloud fills at least up to this surface), but on the vacuum side, E is non-vanishing and points in the expedient direction to collect and transport stray particles of the same (sign of) charge into the force-free side, while repelling particles of the undesirable opposite charge. This ensures that the charge clouds, and in turn the electrosphere solutions, are stable [120,126] 12 . Such a self-maintenance feature also prevents clouds from dissipating if they spill over beyond the trap surfaces, as would be the case when there is too much charge and the electric repulsion is severe.…”
Section: Appendix A3 With Plasma: the Charge-separated Electrospheresmentioning
confidence: 99%