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WHAT NEW OBSERVATIONS AND KINETIC SIMULATIONS OF THE PLASMASPHERE REVEAL ON THE INNER MAGNETOSPHERE

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proceedings of the conference-165 GRINGAUZ 100: PLASMAS IN THE SOLAR SYSTEM, 2018 165

WHAT NEW OBSERVATIONS AND KINETIC SIMULATIONS OF THE PLASMASPHERE REVEAL ON THE INNER MAGNETOSPHERE

V. Pierrard

1,2

, F. Darrouzet

1

, G. Lopez Rosson

1,2

, J. Lemaire

1,2

1

Royal Belgian Institute for Space Aeronomy (IASB-BIRA), Space Physics,  Belgium; [email protected]

2

Université Catholique de Louvain (UCL), Center for Space Radiations  (CSR), ELI-C, Belgium

KEYWORDS

plasmasphere, radiation belts, kinetic model, plasmapause, geomagnetic storms

Using CRRES, Cluster and THEMIS observations, we analyzed how the plas- mapause is formed in the post-midnight sector when the geomagnetic activity is enhanced; the plasmasphere is first eroded deeper in the magnetosphere, and its newly formed outer Plasmapheric Boundary Layer (PBL) is subse- quently transmitted to other MLT sectors by co-rotation. The results of these satellites measurements are generally in excellent agreement with the pre- diction of plasmapause formation mechanism based on plasma quasi-inter- change process [1] which is implemented in the numerical simulations codes developed at IASB-BIRA.

Our Kp-dependent 3D-model of the plasmasphere enables not only to calcu- late the equatorial position of the plasmapause as a function of MLT and UT, but it gives also the cold plasma density and temperature within as well as out- side the plasmasphere [2]. Our 3D time-dependent model of the plasmasphere is coupled to a standard model of the ionosphere [3]. It enables to simulate the dynamical development of plasmaspheric plumes. The latter are initially generated as growing shoulders formed in the dawn sector at the onset of geomagnetic storms; then they propagate into the afternoon MLT sector where they stretch radially toward the magnetopause to form an extended plume.

The continuous radial flow of plasma known as Plasmaspheric Wind [4] has also been implemented in our 3D-numerical model. Plasma densities and drift velocities from the THEMIS mission will be used as initial conditions to model the overall distribution of the plasmaspheric wind velocity.

Using CLUSTER particle flux measurements for different energy ranges, we

found that the observed plasmapause positions and the observed boundaries

of the radiations belts are correlated with each other [5]. These connections are

currently studied in greater details by using the observations available from the

Energetic Particle Telescope (EPT), the specific instrument that has been de-

veloped in Belgium by IASB-BIRA, CSR/UCL, and QinetiQ-Space. The EPT is

a high time-resolution (2 sec.) spectrometer which was launched in May 2013

onboard of the PROBA-V satellite of ESA [6]. This energetic particle detector

is still operating at the altitude of 820 km on a LEO polar orbit. This unique new

type of detector has a field of view angle of 52°, and is providing continuously

for already 5 years valuable electrons count rates in 7 energy channels (0.5 –

8 MeV), in 11 channels (9.5 – 248 MeV) for the protons, and in 11 channels

(38 – 900 MeV) for the helium ions. The detailed observations of EPT confirm

that the calibrated fluxes of outer belt electrons drop drastically and abruptly

during the main phase of geomagnetic storms [7]; these fluxes recoup eventu-

ally gradually over 1 or 2 days during the subsequent recovery phases. Some-

times at the end of such recovery periods, the fluxes of relativistic electrons

can have smaller values, or else they reach values orders of magnitude larger

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166-proceedings of the conference

GRINGAUZ 100: PLASMAS IN THE SOLAR SYSTEM, 2018

166

than their pre-storm intensities. Furthermore, our EPT measurements clearly confirm that following geomagnetic storm events the outer belt fluxes slowly decrease with a time constant ranging between 6 and 18 days. The positions of the maximum flux of relativistic electrons shift toward the Earth during the enhanced geomagnetic activity events, in a rather similar way as the surface of the plasmapause does it also during such enhancements. The fluxes of parti- cles in the Inner Radiation Belt and South Atlantic Anomaly can also be signifi- cantly affected by geomagnetic activity, but only during the strongest storms.

REFERENCES

[1] Lemaire J., Pierrard V. Comparison between two theoretical mechanisms for the formation of the plasmapause and relevant observations, Geomagnetizm I Aer- onomiya. 2008. V. 48, No. 5, P. 579-597.

[2] Pierrard V., Stegen K. A three dimensional dynamic kinetic model of the plasma- sphere, Journal Geophys. Res. 2008. V. 113, A10209, doi: 10.1029/2008ja013060.

[3] Pierrard V., Voiculescu M. The 3D model of the plasmasphere coupled to the ion- osphere, Geophys. Res. Lett. 2011. V. 38, L12104, doi:10.1029/2011GL047767.

[4] Lemaire J., Schunk R.W. Plasmaspheric wind, Journal of Atmospheric and Terres- trial Physics, 1992. 54, 467-477.

[5] Darrouzet F. et al. Links between the plasmapause and the radiation belts bound- aries as observed by the instruments CIS, RAPID and WHISPER on CLUS- TER, J. Geophys. Res.: Space Phys., 2013. V. 118, P. 4176-4188, doi: 10.1002/

jgra.50239.

[6] Pierrard V. et al. The Energetic Particle Telescope: First results, Space Science Rev., 2014. V. 184, P. 87-106, DOI: 10.1007/s11214-014-0097-8.

[7] Pierrard V., Lopez Rosson G. The effects of the big storm events in the first half

of 2015 on the radiation belts observed by EPT/PROBA-V. Annales Geophysi-

cae. 2016. V. 34 P. 75-84, doi:10.5194/angeo-34-75-2016.

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