Plasma depletion layer: Magnetosheath flow structure and forces
The plasma depletion layer (PDL) is a layer on the sunward side of the magnetopause with lower plasma density and higher magnetic field compared to the corresponding upstream magnetosheath values. In a previous study, we have validated the UCLA global (MHD) model in studying the formati...
Main Authors: | , , |
---|---|
Format: | Article |
Language: | English |
Published: |
Copernicus Publications
2004-03-01
|
Series: | Annales Geophysicae |
Online Access: | https://www.ann-geophys.net/22/1001/2004/angeo-22-1001-2004.pdf |
id |
doaj-5e28766e27c745ba8b0869d424e6fe95 |
---|---|
record_format |
Article |
spelling |
doaj-5e28766e27c745ba8b0869d424e6fe952020-11-24T23:47:20ZengCopernicus PublicationsAnnales Geophysicae0992-76891432-05762004-03-01221001101710.5194/angeo-22-1001-2004Plasma depletion layer: Magnetosheath flow structure and forcesY. L. Wang0J. Raeder1C. T. Russell2Institute of Geophysics and Planetary Physics, University of California, Los Angeles, USAInstitute of Geophysics and Planetary Physics, University of California, Los Angeles, USAInstitute of Geophysics and Planetary Physics, University of California, Los Angeles, USAThe plasma depletion layer (PDL) is a layer on the sunward side of the magnetopause with lower plasma density and higher magnetic field compared to the corresponding upstream magnetosheath values. In a previous study, we have validated the UCLA global (MHD) model in studying the formation of the PDL by comparing model results, using spacecraft solar wind observations as the driver, with in situ PDL observations. In this study, we extend our previous work and examine the detailed MHD forces responsible for the PDL formation. We argue that MHD models, instead of gasdynamic models, should be used to study the PDL, because gasdynamic models cannot produce the PDL on the sunward side of the magnetopause. For northward (IMF), flux tube depletion occurs in almost all the subsolar magnetosheath. However, the streamlines closest to the magnetopause and the stagnation line show the greatest depletion. The relative strength of the various MHD forces changes along these streamlines. Forces along a flux tube at different stages of its depletion in the magnetosheath are analyzed. We find that a strong plasma pressure gradient force along the magnetic field at the bow shock and a pressure gradient force along the flux tube within the magnetosheath usually exist pushing plasma away from the equatorial plane to deplete the flux tube. More complex force structures along the flux tube are found close to the magnetopause. This new, more detailed description of flux tube depletion is compared with the results of Zwan and Wolf (1976) and differences are found. Near the magnetopause, the pressure gradient force along the flux tube either drives plasma away from the equatorial plane or pushes plasma toward the equatorial plane. As a result, a slow mode structure is seen along the flux tube which might be responsible for the observed two-layered slow mode structures. <br><br><b>Key words.</b> Magnetospheric physics (magnetosheath; solar wind-magnetosphere interactions). Space plasma physics (numerical simulations studies)https://www.ann-geophys.net/22/1001/2004/angeo-22-1001-2004.pdf |
collection |
DOAJ |
language |
English |
format |
Article |
sources |
DOAJ |
author |
Y. L. Wang J. Raeder C. T. Russell |
spellingShingle |
Y. L. Wang J. Raeder C. T. Russell Plasma depletion layer: Magnetosheath flow structure and forces Annales Geophysicae |
author_facet |
Y. L. Wang J. Raeder C. T. Russell |
author_sort |
Y. L. Wang |
title |
Plasma depletion layer: Magnetosheath flow structure and forces |
title_short |
Plasma depletion layer: Magnetosheath flow structure and forces |
title_full |
Plasma depletion layer: Magnetosheath flow structure and forces |
title_fullStr |
Plasma depletion layer: Magnetosheath flow structure and forces |
title_full_unstemmed |
Plasma depletion layer: Magnetosheath flow structure and forces |
title_sort |
plasma depletion layer: magnetosheath flow structure and forces |
publisher |
Copernicus Publications |
series |
Annales Geophysicae |
issn |
0992-7689 1432-0576 |
publishDate |
2004-03-01 |
description |
The plasma depletion layer (PDL) is a layer on the sunward side of the magnetopause with
lower plasma density and higher magnetic field compared to the corresponding
upstream magnetosheath values.
In a previous study, we have validated the UCLA global (MHD) model in studying
the formation of the PDL by comparing model results, using spacecraft
solar wind observations as the driver, with in situ PDL observations.
In this study, we extend our previous work and examine
the detailed MHD forces responsible for the PDL formation.
We argue that MHD models, instead of gasdynamic models, should be
used to study the PDL, because gasdynamic models cannot produce the PDL on
the sunward side of the magnetopause.
For northward (IMF), flux tube depletion occurs in almost all the subsolar
magnetosheath.
However, the streamlines closest to the magnetopause and
the stagnation line show the greatest depletion.
The relative strength of the various MHD forces changes along these streamlines.
Forces along a flux tube at different stages of its depletion in the
magnetosheath are analyzed.
We find that a strong plasma pressure gradient force along the magnetic field
at the bow shock and a pressure gradient force along the flux tube within the magnetosheath
usually exist pushing plasma away from the equatorial plane to deplete the flux tube.
More complex force structures along the flux tube are found close to the magnetopause.
This new, more detailed description of flux tube depletion is compared with
the results of Zwan and Wolf (1976) and differences are found.
Near the magnetopause, the pressure gradient force along the flux tube either
drives plasma away from the equatorial plane or pushes plasma toward
the equatorial plane.
As a result, a slow mode structure is seen along the flux tube
which might be responsible for the observed two-layered slow mode structures.
<br><br><b>Key words.</b> Magnetospheric physics (magnetosheath; solar
wind-magnetosphere interactions). Space plasma physics
(numerical simulations studies) |
url |
https://www.ann-geophys.net/22/1001/2004/angeo-22-1001-2004.pdf |
work_keys_str_mv |
AT ylwang plasmadepletionlayermagnetosheathflowstructureandforces AT jraeder plasmadepletionlayermagnetosheathflowstructureandforces AT ctrussell plasmadepletionlayermagnetosheathflowstructureandforces |
_version_ |
1725490328503320576 |