Abstract

Abstract. We introduce a new model for the plasmapause location in the equatorial plane. The determination of the L-shell bounding the plasmasphere is based on magnetic field observations made by the CHAMP satellite in the topside ionosphere. Related signals are medium-scale field-aligned currents (MSFAC) (some 10 km scale size). The mid-latitude boundary of these MSFACs is used for determining the plasmapause. We are presenting a procedure for detecting the MSFAC boundary. Reliable L-values are obtained on the night side, whenever the solar zenith angle is below 90°. This means, the boundary is not determined well in the 08:00 to 16:00 magnetic local time (MLT) sector. The radial distance of the boundary is closely controlled by the magnetic activity index Kp. Over the Kp range 0 to 9, the L-value varies from 6 to 2 RE. Conversely, the dependence on solar flux is insignificant. For a fixed Kp level, the obtained L-values of the boundary form a ring on an MLT dial plot with a centre somewhat offset from the geomagnetic pole. This Kp and local time dependent feature is used for predicting the location of the MSFAC boundary at all MLTs based on a single L-value determination by CHAMP. We compared the location of the MSFAC boundary during the years 2001–2002 with the L-value of the plasmapause, determined from in situ observations by the IMAGE spacecraft. The mean difference in radial distance is within a 1 RE range for all local times and Kp values. The plasmapause is generally found earthward of the FAC boundary, except for the duskside. By considering this systematic displacement and by taking into account the diurnal variation and Kp-dependence of the residuals, we are able to construct an empirical model of the plasmapause location that is based on MSFAC measurements from CHAMP. Our new model PPCH-2012 agrees with IMAGE in situ observations within a standard deviation of 0.79 RE.

Highlights

  • RKtthhapdeisivFasalAyldsuCtieessbtm.aonTaucthniecediadpsrilysaw,psimletahxcaicepnemapautes1nfeotRirasEntghdreaenbnMdeygureatsoalfklkodysirindfeaogellu.linnDBlGodtyoceeaecaalvocrottcneihmosswliuocedanseritprdeaitmnnhongdefteifnict1ofsro9fon6mt7h(1)eg.9rIT9oS2huE)enEwdfrasebsaqatudseeeellndriittvelVyesdLcaFifntredoMwdmfhmroioesolmdteldeceertelrllooeonDbcfGstdCreeoeeranvnvroaspeditetiseyonlnocntmDessiipri.etesiacamTennusshusdteesriineiAfonmmfinnecstoerdrdneeetrds-l diurnal variation and Kp-dependence of the residuals, we are gives the PP location as a function of geomagnetic Kp inable to construct an empirical model of the plasmapause lo- dices prevailing some hours before

  • The CHAMP satellite was launched on 15 July 2000 into an almost circular, near-polar orbit with an initial altitude of 454 km which has decreased to ∼300 km after 9 years

  • We have developed an empirical approach for detecting the medium-scale field-aligned currents (MSFAC) boundary

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Summary

CHAMP magnetic data

The CHAMP satellite was launched on 15 July 2000 into an almost circular, near-polar (inclination 87.3◦) orbit with an initial altitude of 454 km which has decreased to ∼300 km after 9 years An advantage of this orbit is its precession through local time (LT) that makes it possible to investigate the LT dependence of various phenomena. The satellite data used in this study are the pre-processed (level 2) fluxgate magnetometer vector data from CHAMP in sensor frame (product identifier CH-ME-2-FGM-FGM). The mean field was estimated by the CHAMP based field model POMME 4.1s (Potsdam Magnetic Model of the Earth) developed by Maus et al (2006) This model includes the main field, the crustal anomalies up to spherical harmonic degree/order 90, the field of the ring current, and large-scale magnetospheric fields.

Detection method
Observations
Discussion
Correlation analysis
Comparison with IMAGE observations
Findings
Proposal of a plasmapause model
Conclusions
Full Text
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