2013
DOI: 10.5194/angeo-31-1297-2013
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Cross-field flow and electric potential in a plasma slab

Abstract: We consider cross-field plasma flow inside a field-aligned plasma slab embedded in a uniform background in a 1-dimensional geometry. This situation may arise, for instance, when long-lasting reconnection pulses inject plasma into the inner magnetosphere. The present paper presents a detailed analysis of the structure of the interfaces that separate the slab from the background plasma on either side; a fully kinetic model is used to do so. Since the velocity shear across both interfaces has opposite signs, and … Show more

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Cited by 14 publications
(13 citation statements)
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“…Although there is a set of analytical models describing observed C‐ and S‐type magnetopause current sheets (Allanson et al, 2017; Artemyev, 2011; De Keyser et al, 2013; Harrison & Neukirch, 2009; Panov et al, 2011), investigation of plasma transport across the magnetopause require numerical simulations of dynamical systems. A small (kinetic) thickness of the magnetopause current sheet gives preference for such simulations to global hybrid models (Lin et al, 2014, 2017, Omidi et al, 2009, 2016), but combination of MHD simulations and test particle tracing (Peroomian, 2003; Peroomian & El‐Alaoui, 2008; Raeder et al, 2000) is also useful tool for such investigations.…”
Section: Discussionmentioning
confidence: 99%
“…Although there is a set of analytical models describing observed C‐ and S‐type magnetopause current sheets (Allanson et al, 2017; Artemyev, 2011; De Keyser et al, 2013; Harrison & Neukirch, 2009; Panov et al, 2011), investigation of plasma transport across the magnetopause require numerical simulations of dynamical systems. A small (kinetic) thickness of the magnetopause current sheet gives preference for such simulations to global hybrid models (Lin et al, 2014, 2017, Omidi et al, 2009, 2016), but combination of MHD simulations and test particle tracing (Peroomian, 2003; Peroomian & El‐Alaoui, 2008; Raeder et al, 2000) is also useful tool for such investigations.…”
Section: Discussionmentioning
confidence: 99%
“…According to MHD theory, plasma discontinuities are classified into tangential discontinuities (which separate two plasmas with different characteristics), rotational discontinuities (which move relative to the plasmas on the two sides, accelerating the plasma population that crosses them), and shock waves (Hudson, ; Landau & Lifshitz, ). This classification, however, does not describe a discontinuity's internal (kinetic) structure, which can vary, even for the same discontinuity type (see, e.g., Artemyev, ; De Keyser et al, ; Harrison & Neukirch, ; Panov et al, ; Vasko et al, ). Therefore, investigation of a discontinuity's contribution to charged particle heating and acceleration in the solar wind requires detailed observational information about its configuration.…”
Section: Introductionmentioning
confidence: 99%
“…These flow shears directly lead to multiple FAC sheets that join together in the cusp region in both hemispheres and field-aligned acceleration of electrons which create multiple cusp-aligned auroral arcs both in the polar cap and auroral oval. This is a general mechanism for the formation of auroral arcs due to field-aligned acceleration of electrons through the Knight’s current-voltage process ( 36 , 37 ) caused by the FAC sheets that are generated by the strong flow shears in the magnetosphere ( 31 , 32 , 39 41 ). With a roughly stable IMF and fast solar wind speed conditions, the stable and multiple transpolar arcs, presented in this paper, cannot be fully explained by the previous models or theories, for example, the twisting magnetotail model due to IMF B y switching ( 3 , 21 , 22 ), the model of tail reconnection during IMF northward nonsubstorm intervals ( 4 , 7 ), and the interchange instability model ( 18 , 19 ), as well as the simulation model of small-scale sun-aligned arcs on closed field lines ( 25 ).…”
mentioning
confidence: 99%