2008
DOI: 10.1103/physrevlett.100.015001
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Competing Mechanisms of Plasma Transport in Inhomogeneous Configurations with Velocity Shear: The Solar-Wind Interaction with Earth’s Magnetosphere

Abstract: Two-dimensional simulations of the Kelvin-Helmholtz instability in an inhomogeneous compressible plasma with a density gradient show that, in a transverse magnetic field configuration, the vortex pairing process and the Rayleigh-Taylor secondary instability compete during the nonlinear evolution of the vortices. Two different regimes exist depending on the value of the density jump across the velocity shear layer. These regimes have different physical signatures that can be crucial for the interpretation of sa… Show more

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Cited by 61 publications
(83 citation statements)
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“…From Eqs. (14) & (15) in Ref. 25 using parameters ν1 = 0.007, ν2 = 0.007 and ν3 = 0.4, the resistivity is η ≈ 10 −3 for both the adiabatic and isothermal cases with the setup described below.…”
Section: Mhd Stagger Codementioning
confidence: 99%
“…From Eqs. (14) & (15) in Ref. 25 using parameters ν1 = 0.007, ν2 = 0.007 and ν3 = 0.4, the resistivity is η ≈ 10 −3 for both the adiabatic and isothermal cases with the setup described below.…”
Section: Mhd Stagger Codementioning
confidence: 99%
“…1). In the sub-magnetosonic case, instead, the vortices are composed of spiralling arms of alternating right-side and left-side values of the density, as discussed in Faganello et al (2008a) and in Tenerani et al (2010) in configurations with and, respectively, without an in-plane magnetic field component. The characteristic value of the vortex density is of the order of the magnetospheric density.…”
Section: Simulation Resultsmentioning
confidence: 99%
“…Moreover, they showed that the onset of secondary reconnection instabilities can disrupt the vortex structure and change the large scale evolution of the configuration significantly. In the low latitude magnetopause context, the Rayleigh Taylor (RT) instability (Matsumoto and Hoshino, 2004;Faganello et al, 2008a) is another important secondary instability that can develop inside the KH vortices. This instability is driven by the alternating density layers consisting of solar wind and of magnetosphere plasma respectively which are rolled up in the KH vortex arms.…”
Section: Introductionmentioning
confidence: 99%
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“…Nonlinear simulations of the KH instability have been performed in MHD by Malagoli et al [38], Frank et al [27], Keppens et al [39], Ryu et al [28], Otto and Fairfield [14], Baty et al [29], Faganello et al [15], among others. These studies have frequently identified vortex formation in the early nonlinear regime, followed by field-induced vortex disruption, magnetic reconnection, turbulent breakdown, and relaxation to an equilibrium state.…”
Section: Prior Researchmentioning
confidence: 99%