MLT dependence in the relationship between plasmapause, solar wind, and geomagnetic activity based on CRRES: 1990–1991

Using the database of CRRES in situ observations of the plasmapause crossings, we develop linear and more complex plasmapause models parametrized by (a) solar wind parameters V (solar wind velocity), BV (where B is the magnitude of the interplanetary magnetic field (IMF)), and dΦmp/dt (which combine...

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Veröffentlicht in:Journal of geophysical research. Space physics 2016-05, Vol.121 (5), p.4397-4408
Hauptverfasser: Bandić, Mario, Verbanac, Giuli, Moldwin, Mark B., Pierrard, Viviane, Piredda, Giovanni
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container_end_page 4408
container_issue 5
container_start_page 4397
container_title Journal of geophysical research. Space physics
container_volume 121
creator Bandić, Mario
Verbanac, Giuli
Moldwin, Mark B.
Pierrard, Viviane
Piredda, Giovanni
description Using the database of CRRES in situ observations of the plasmapause crossings, we develop linear and more complex plasmapause models parametrized by (a) solar wind parameters V (solar wind velocity), BV (where B is the magnitude of the interplanetary magnetic field (IMF)), and dΦmp/dt (which combines different physical mechanisms which run magnetospheric activity), and (b) geomagnetic indices Dst, Ap, and AE. The complex models are built by including a first harmonic in magnetic local time (MLT). Our method based on the cross‐correlation analyses provides not only the plasmapause shape for different levels of geomagnetic activity but additionally yields the information of the delays in the MLT response of the plasmapause. All models based on both solar wind parameters and geomagnetic indices indicate the maximal plasmapause extension in the postdusk side at high geomagnetic activity. The decrease in the convection electric field places the bulge toward midnight. These results are compared and discussed in regard to past works. Our study shows that the time delays in the plasmapause response are a function of MLT and suggests that the plasmapause is formed by the mechanism of interchange instability motion. We observed that any change quickly propagates across dawn to noon, and then at lower rate toward midnight. The results further indicate that the instability may propagate much faster during solar maximum than around solar minimum. This study contributes to the determination of the MLT dependence of the plasmapause and to constrain physical mechanism by which the plasmapause is formed. Key Points The delay times of Lpp to the arrival of Lpp indicators is a function of MLT The MLT dependence of plasmapause formation is in agreement with the mechanism of interchange instability At high geomagnetic activity the Lpp bulge is formed in the postdusk; at low geomagnetic activity the bulge is located close to midnight
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The complex models are built by including a first harmonic in magnetic local time (MLT). Our method based on the cross‐correlation analyses provides not only the plasmapause shape for different levels of geomagnetic activity but additionally yields the information of the delays in the MLT response of the plasmapause. All models based on both solar wind parameters and geomagnetic indices indicate the maximal plasmapause extension in the postdusk side at high geomagnetic activity. The decrease in the convection electric field places the bulge toward midnight. These results are compared and discussed in regard to past works. Our study shows that the time delays in the plasmapause response are a function of MLT and suggests that the plasmapause is formed by the mechanism of interchange instability motion. We observed that any change quickly propagates across dawn to noon, and then at lower rate toward midnight. The results further indicate that the instability may propagate much faster during solar maximum than around solar minimum. This study contributes to the determination of the MLT dependence of the plasmapause and to constrain physical mechanism by which the plasmapause is formed. Key Points The delay times of Lpp to the arrival of Lpp indicators is a function of MLT The MLT dependence of plasmapause formation is in agreement with the mechanism of interchange instability At high geomagnetic activity the Lpp bulge is formed in the postdusk; at low geomagnetic activity the bulge is located close to midnight</description><identifier>ISSN: 2169-9380</identifier><identifier>EISSN: 2169-9402</identifier><identifier>DOI: 10.1002/2015JA022278</identifier><language>eng</language><publisher>Washington: Blackwell Publishing Ltd</publisher><subject>Charged particles ; Convection ; Correlation analysis ; CRESS satellite ; CRRES (satellite) ; Delay ; Dependence ; Electric fields ; Geomagnetic activity ; Geomagnetism ; Instability ; Interplanetary magnetic field ; Interplanetary magnetic fields ; Magnetic fields ; Magnetism ; Magnetospheres ; Mathematical models ; Motion stability ; Parameters ; Plasmapause ; Solar cycle ; Solar maximum ; Solar minimum ; Solar wind ; Solar wind parameters ; Solar wind velocity ; Stability ; Wind speed</subject><ispartof>Journal of geophysical research. 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Space physics</title><description>Using the database of CRRES in situ observations of the plasmapause crossings, we develop linear and more complex plasmapause models parametrized by (a) solar wind parameters V (solar wind velocity), BV (where B is the magnitude of the interplanetary magnetic field (IMF)), and dΦmp/dt (which combines different physical mechanisms which run magnetospheric activity), and (b) geomagnetic indices Dst, Ap, and AE. The complex models are built by including a first harmonic in magnetic local time (MLT). Our method based on the cross‐correlation analyses provides not only the plasmapause shape for different levels of geomagnetic activity but additionally yields the information of the delays in the MLT response of the plasmapause. All models based on both solar wind parameters and geomagnetic indices indicate the maximal plasmapause extension in the postdusk side at high geomagnetic activity. 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subjects Charged particles
Convection
Correlation analysis
CRESS satellite
CRRES (satellite)
Delay
Dependence
Electric fields
Geomagnetic activity
Geomagnetism
Instability
Interplanetary magnetic field
Interplanetary magnetic fields
Magnetic fields
Magnetism
Magnetospheres
Mathematical models
Motion stability
Parameters
Plasmapause
Solar cycle
Solar maximum
Solar minimum
Solar wind
Solar wind parameters
Solar wind velocity
Stability
Wind speed
title MLT dependence in the relationship between plasmapause, solar wind, and geomagnetic activity based on CRRES: 1990–1991
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