1998
DOI: 10.1103/physreve.58.931
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Magnetic islands in a magnetized plasma with electron flow

Abstract: A system of two coupled nonlinear equations describing magnetic electron modes in a magnetized inhomogeneous plasma with a spatially dependent electron flow is derived. For a homogeneous basic state electron concentration, the two equations can be decoupled, and a nonlinear solution for the magnetic field in the form of a traveling stationary vortex chain of magnetic islands is found.

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Cited by 12 publications
(6 citation statements)
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“…When μ = 0, we find that is satisfied by the Ansatz where ϕ 0 , C 0 , and A 0 are arbitrary constants. The solution of is We note that for A 0 > 1, the vortex profile resembles the Kelvin‐Stuart “cat's eyes” that are chains of vortices [ Petviashvili and Pokhotelov , 1992; Stenflo , 1994; Shukla et al , 1995; , 1998]. The vortex chain speed is U 0 = ( V a * + μ z u 0 )/2± [( V a * + μ z u 0 ) 2 + 4 C a 2 μ z (α + μ z )] 1/2 /2.…”
Section: Lower Hybrid Drift Vorticesmentioning
confidence: 99%
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“…When μ = 0, we find that is satisfied by the Ansatz where ϕ 0 , C 0 , and A 0 are arbitrary constants. The solution of is We note that for A 0 > 1, the vortex profile resembles the Kelvin‐Stuart “cat's eyes” that are chains of vortices [ Petviashvili and Pokhotelov , 1992; Stenflo , 1994; Shukla et al , 1995; , 1998]. The vortex chain speed is U 0 = ( V a * + μ z u 0 )/2± [( V a * + μ z u 0 ) 2 + 4 C a 2 μ z (α + μ z )] 1/2 /2.…”
Section: Lower Hybrid Drift Vorticesmentioning
confidence: 99%
“…Choosing where ϕ 0 and ϕ c are arbitrary constants, one easily finds that the solution of takes the form [ Mallier and Maslowe , 1993] which represents a street of counterrotating vortices, where ϵ (<1) is a constant. Furthermore, choosing where α 0 , K 0 , and γ 0 are constants, one finds that the solution [, 1998] of with is which is an even (in the x direction) row of identical vortices for γ 0 2 > 1.…”
Section: Lower Hybrid Drift Vorticesmentioning
confidence: 99%
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“…In the spatial regions where the streamlines are closed the function G in principle may have di †erent forms, and besides of the boundary conditions at inÐnity it would be necessary to Ðnd the appropriate form of the function in these regions and match solutions at separatrices but this would be a difficult task. Consequently, we shall assume that the corresponding asymptotic expression of the above function is valid on the whole (x, y) plane [9].…”
Section: Basic Equations Derivations and Solutionsmentioning
confidence: 99%
“…where the function g is arbitrary, and following the procedure from our Ref. [9] we take it in the form :…”
Section: Basic Equations Derivations and Solutionsmentioning
confidence: 99%