Abstract
We consider the electron distribution in current sheets observed by Cluster mission in the Earth magnetotail. We use the statistics of 70 fast (less than 20 minutes) and 12 slow (more than one hour) crossings of horizontal current sheets. We demonstrate that for both types electron temperature decreases with increase of magnetic field ∣Bx∣ away from the current sheet center. We use the approximations Te⊥/Te⊥ max ≈ 1 − αT⊥(Bx/Bext)2 and Te∥/Te∥ max ≈ 1 − αT∥(Bx/Bext)2, where Bext is value of Bx in the lobes. For statistics of thin current sheets (fast crossings) we obtain mean values 〈αT⊥〉 ≈ 〈αT∥〉 ≈ 1. For thick current sheets (slow crossings) we also obtain 〈αT⊥〉 ≈ 〈αT∥〉, but 〈αT⊥〉, 〈αT∥〉 > 1. The electron temperature anisotropy is about Te∥/Te⊥ = 1.1 − 1.2 and vertical profiles Te∥/Te⊥ ≈ const. Observed vertical distributions of Te∥ and Te⊥ are described by the analytical model of electron heating in the course of the earthward convection in thin current sheets with (Bx(z), Bz(x)) and in thick current sheets with (Bx(x, z), Bz(x, z)). We also show that the observed electron temperature anisotropy is provided by the electron population in the energy range between 50 ev and 3 keV. The cold core of electron distribution (<50 eV) is isotropic and the hot tail (>5 keV) has Te∥/Te⊥ ∼ 1 or even Te∥/Te⊥ < 1. We consider electron pressure tensor in observed thin current sheets and demonstrate that electron velocity distribution is gyrotropic with high accuracy.
Talk to us
Join us for a 30 min session where you can share your feedback and ask us any queries you have
Disclaimer: All third-party content on this website/platform is and will remain the property of their respective owners and is provided on "as is" basis without any warranties, express or implied. Use of third-party content does not indicate any affiliation, sponsorship with or endorsement by them. Any references to third-party content is to identify the corresponding services and shall be considered fair use under The CopyrightLaw.