Abstract

Abstract. The four Cluster s/c passed over Northern Scandinavia on 6 February 2001 from south-east to north-west at a radial distance of about 4.4 RE in the post-midnight sector. When mapped along geomagnetic field lines, the separation of the spacecraft in the ionosphere was confined to within 110km in latitude and 50km in longitude. This constellation allowed us to study the temporal evolution of plasma with a time scale of a few minutes. Ground-based instrumentation used involved two all-sky cameras, magnetometers and the EISCAT radar. The main findings were as follows. Two auroral arcs were located close to the equatorward and poleward edge of a large-scale density cavity, respectively. These arcs showed a different kind of a temporal evolution. (1) As a response to a pseudo-breakup onset, both the up- and downward field-aligned current (FAC) sheets associated with the equatorward arc widened and the total amount of FAC doubled in a time scale of 1–2min. (2) In the poleward arc, a density cavity formed in the ionosphere in the return (downward) current region. As a result of ionospheric feedback, a strongly enhanced ionospheric southward electric field developed in the region of decreased Pedersen conductance. Furthermore, the acceleration potential of ionospheric electrons, carrying the return current, increased from 200 to 1000eV in 70s, and the return current region widened in order to supply a constant amount of return current to the arc current circuit. Evidence of local acceleration of the electron population by dispersive Alfvén waves was obtained in the upward FAC region of the poleward arc. However, the downward accelerated suprathermal electrons must be further energised below Cluster in order to be able to produce the observed visible aurora. Both of the auroral arcs were associated with broad-band ULF/ELF (BBELF) waves, but they were highly localised in space and time. The most intense BBELF waves were confined typically to the return current regions adjacent to the visual arc, but in one case also to a weak upward FAC region. BBELF waves could appear/disappear between s/c crossings of the same arc separated by about 1min. Key words. Ionosphere (electric fields and currents) – Magnetospheric physics (auroral phenomena; magnetosphereionosphere interactions)

Highlights

  • Satellite and rocket observations in the auroral zone below and within the auroral acceleration region have been performed by many spacecraft since the discovery of the region in the 1970’s (Mozer et al, 1977)

  • The acceleration potential of ionospheric electrons, carrying the return current, increased from 200 to 1000 eV in 70 s, and the return current region widened in order to supply a constant amount of return current to the arc current circuit

  • The DC electric field is calculated as a spin fit to a probe-pair measurement with 4-s resolution and it is presented in the field-aligned current (FAC) coordinate system, where the positive Z-axis points in the direction of the Earth’s magnetic field at the spacecraft’s location, the positive X-axis lies in the plane of the Earth’s magnetic field line, perpendicular to the Z-axis, and points inwards, i.e. towards the magnetic equator and the positive Y-axis completes the orthogonal right-handed system

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Summary

Introduction

Satellite and rocket observations in the auroral zone below and within the auroral acceleration region have been performed by many spacecraft since the discovery of the region in the 1970’s (Mozer et al, 1977). The DC electric field is calculated as a spin fit to a probe-pair measurement with 4-s resolution and it is presented in the FAC (field-aligned) coordinate system, where the positive Z-axis points in the direction of the Earth’s magnetic field at the spacecraft’s location, the positive X-axis lies in the plane of the Earth’s magnetic field line, perpendicular to the Z-axis, and points inwards, i.e. towards the magnetic equator and the positive Y-axis completes the orthogonal right-handed system (it points towards west during the studied time interval). To study the electric field fluctuations, we use high time resolution, 450 samples/s, electric field data from the EFW instrument These data are presented in the BSC (Magnetic Spacecraft Coordinates) coordinate system, where the Z-axis is along the satellite spin axis, the X-axis is along the projection of the magnetic field vector on the spin plane and the Y-axis closes the right-handed coordinate system.

Ground optical and magnetic observations
Cluster observations of field-aligned currents
Cluster electric field and potential observations
Cluster observations of electric field fluctuations
EISCAT observations
Cluster observations of particles
Temporal evolution of the arcs
Electric field fluctuations
Conclusions
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