2002
DOI: 10.5194/angeo-20-1559-2002
|View full text |Cite
|
Sign up to set email alerts
|

Origin of some anisotropic tailward flows in the plasma sheet

Abstract: Abstract. We use a test particle model to explore anisotropy and fast flows in the central plasma sheet (CPS) that are a consequence of plasma sheet boundary layer (PSBL) ion beam dynamics. Ion distributions and flows (velocity moments) in the CPS and equatorial current sheet (CS) are compared and we find that mirroring of initially earthward beams from the PSBL, and their subsequent convection to the CS region, results in strong anisotropy throughout the CPS. At higher latitudes, velocity moments are field-al… Show more

Help me understand this report

Search citation statements

Order By: Relevance

Paper Sections

Select...
2
1
1
1

Citation Types

0
7
0

Year Published

2008
2008
2019
2019

Publication Types

Select...
7

Relationship

0
7

Authors

Journals

citations
Cited by 7 publications
(7 citation statements)
references
References 89 publications
0
7
0
Order By: Relevance
“…With the equilibrium current sheet model treated as the initial condition, test‐particle simulations can now be carried out to reproduce the observed evolution of the ion distributions (shown in Figures 2d–2f) as the front approaches. As was shown by Zhou et al [2009a], the modeled ion distributions are associated with the ion distributions at later times, on the basis of Liouville's theorem [e.g., Schwartz et al , 1998; Wanliss et al , 2002]. In other words, the ion distributions f ( r , v , t ) at time t can be determined by tracing the ion trajectories backward in time to obtain their initial locations r 0 and velocities v 0 within the modeled equilibrium at t 0 and equating f with the corresponding f ( r 0 , v 0 , t 0 ) values [ Zhou et al , 2009a].…”
Section: Simulations and Discussionmentioning
confidence: 99%
“…With the equilibrium current sheet model treated as the initial condition, test‐particle simulations can now be carried out to reproduce the observed evolution of the ion distributions (shown in Figures 2d–2f) as the front approaches. As was shown by Zhou et al [2009a], the modeled ion distributions are associated with the ion distributions at later times, on the basis of Liouville's theorem [e.g., Schwartz et al , 1998; Wanliss et al , 2002]. In other words, the ion distributions f ( r , v , t ) at time t can be determined by tracing the ion trajectories backward in time to obtain their initial locations r 0 and velocities v 0 within the modeled equilibrium at t 0 and equating f with the corresponding f ( r 0 , v 0 , t 0 ) values [ Zhou et al , 2009a].…”
Section: Simulations and Discussionmentioning
confidence: 99%
“…Our approach to simulate the precursor flows ahead of DFs is based on Liouville's theorem [ Birn and Hesse , ; Schwartz et al ., ; Wanliss et al ., ; Zhou et al ., ; Marchand , ]. First, we use a two‐dimensional, Schindler‐type equilibrium [ Schindler , ] current sheet, with the magnetic field obtained from the magnetic vector potential given by…”
Section: Backward Tracing Liouville Simulationsmentioning
confidence: 99%
“…With the initial condition determined, test particle simulations can then be carried out under prescribed electric and magnetic fields, as the second step, to simulate the evolution of ion distributions [ Zhou et al , 2009a]. Here the association between the ion distributions in the initial equilibrium and those at later times is provided by Liouville's theorem [ Schwartz et al , 1998; Wanliss et al , 2002]. In other words, the ion distributions f ( r , v , t ) at time t can be obtained by tracing ion trajectories backward in time to identify their initial locations r 0 and velocities v 0 within the modeled equilibrium at t 0 and equating f ( r , v , t ) with the corresponding f ( r 0 , v 0 , t 0 ) values.…”
Section: Simulationsmentioning
confidence: 99%