Crescent-shaped electron velocity distribution functions formed at the edges of plasma jets interacting with a tangential discontinuity
<p>In this paper we discuss numerical simulations that illustrate a physical mechanism leading to the formation of crescent-shaped electron velocity distribution functions at the edges of a high-speed plasma jet impacting on a thin, steep and impenetrable tangential discontinuity with no ma...
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Copernicus Publications
2018-11-01
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Series: | Annales Geophysicae |
Online Access: | https://www.ann-geophys.net/36/1521/2018/angeo-36-1521-2018.pdf |
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doaj-82dfaa73649b42a69cc4757bb11a51832020-11-25T00:17:05ZengCopernicus PublicationsAnnales Geophysicae0992-76891432-05762018-11-01361521153510.5194/angeo-36-1521-2018Crescent-shaped electron velocity distribution functions formed at the edges of plasma jets interacting with a tangential discontinuityG. Voitcu0M. Echim1M. Echim2Institute of Space Science, Magurele, 077125, RomaniaInstitute of Space Science, Magurele, 077125, RomaniaBelgian Institute of Space Aeronomy, Brussels, 1180, Belgium<p>In this paper we discuss numerical simulations that illustrate a physical mechanism leading to the formation of crescent-shaped electron velocity distribution functions at the edges of a high-speed plasma jet impacting on a thin, steep and impenetrable tangential discontinuity with no magnetic shear. We use three-dimensional particle-in-cell simulations to compute the velocity distribution function of electrons in different areas of the plasma jet and at different phases of the interaction with the discontinuity. The simulation set-up corresponds to an idealized, yet relevant, magnetic configuration likely to be observed at the frontside magnetopause under the northward interplanetary magnetic field. The combined effect of the gradient-B drift and the remote sensing of large Larmor radius electrons leads to the formation of crescent-shaped electron velocity distribution functions. We provide examples of such distributions <q>measured</q> by a virtual satellite launched into the simulation domain.</p>https://www.ann-geophys.net/36/1521/2018/angeo-36-1521-2018.pdf |
collection |
DOAJ |
language |
English |
format |
Article |
sources |
DOAJ |
author |
G. Voitcu M. Echim M. Echim |
spellingShingle |
G. Voitcu M. Echim M. Echim Crescent-shaped electron velocity distribution functions formed at the edges of plasma jets interacting with a tangential discontinuity Annales Geophysicae |
author_facet |
G. Voitcu M. Echim M. Echim |
author_sort |
G. Voitcu |
title |
Crescent-shaped electron velocity distribution functions formed at the edges of plasma jets interacting with a tangential discontinuity |
title_short |
Crescent-shaped electron velocity distribution functions formed at the edges of plasma jets interacting with a tangential discontinuity |
title_full |
Crescent-shaped electron velocity distribution functions formed at the edges of plasma jets interacting with a tangential discontinuity |
title_fullStr |
Crescent-shaped electron velocity distribution functions formed at the edges of plasma jets interacting with a tangential discontinuity |
title_full_unstemmed |
Crescent-shaped electron velocity distribution functions formed at the edges of plasma jets interacting with a tangential discontinuity |
title_sort |
crescent-shaped electron velocity distribution functions formed at the edges of plasma jets interacting with a tangential discontinuity |
publisher |
Copernicus Publications |
series |
Annales Geophysicae |
issn |
0992-7689 1432-0576 |
publishDate |
2018-11-01 |
description |
<p>In this paper we discuss numerical simulations that illustrate a physical
mechanism leading to the formation of crescent-shaped electron velocity
distribution functions at the edges of a high-speed plasma jet impacting on a
thin, steep and impenetrable tangential discontinuity with no magnetic shear.
We use three-dimensional particle-in-cell simulations to compute the velocity
distribution function of electrons in different areas of the plasma jet and
at different phases of the interaction with the discontinuity. The simulation
set-up corresponds to an idealized, yet relevant, magnetic configuration
likely to be observed at the frontside magnetopause under the northward
interplanetary magnetic field. The combined effect of the gradient-B drift
and the remote sensing of large Larmor radius electrons leads to the
formation of crescent-shaped electron velocity distribution functions. We
provide examples of such distributions <q>measured</q> by a virtual satellite
launched into the simulation domain.</p> |
url |
https://www.ann-geophys.net/36/1521/2018/angeo-36-1521-2018.pdf |
work_keys_str_mv |
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1725381116798435328 |