JpGU-AGU Joint Meeting 2017

Presentation information

[JJ] Oral

P (Space and Planetary Sciences) » P-EM Solar-Terrestrial Sciences, Space Electromagnetism & Space Environment

[P-EM21] [JJ] Space Plasma Physics: Theory and Simulation

Wed. May 24, 2017 3:30 PM - 5:00 PM A01 (Tokyo Bay Makuhari Hall)

convener:Takayuki Umeda(Institute for Space-Earth Environmental Research, Nagoya University), Yasuhiro Nariyuki(Faculty of Human Development, University of Toyama), Yohei Miyake(Education Center on Computational Science and Engineering, Kobe University), Tadas Nakamura(Fukui Prefectural University), Chairperson:Takayuki Umeda(Institute for Space-Earth Environmental Research, Nagoya University), Chairperson:Yasuhiro Nariyuki(Faculty of Human Development, University of Toyama)

3:30 PM - 3:45 PM

[PEM21-01] Electron dynamics surrounding the X-line in magnetopause-type asymmetric reconnection

*Seiji Zenitani1, Hiroshi Hasegawa2, Tsugunobu Nagai3 (1.NAOJ National Astronomical Observatory of Japan, 2.Institute of Space and Astronautical Science, Japan Aerospace Exploration Agency, 3.Department of Earth and Planetary Sciences, Tokyo Institute of Technology)

Keywords:magnetic reconnection, magnetopause, particle dynamics

Electron dynamics surrounding the X-line in magnetopause-type asymmetric reconnection is investigated using a two-dimensional particle-in-cell (PIC) simulation. We study electron properties of three characteristic regions in the vicinity of the X-line. The fluid properties, velocity distribution functions (VDFs), and orbits are studied and cross-compared. In the low-beta side of the X-line, the normal electric field enhances the electron meandering motion from the high-beta side. The motion leads to a crescent-shaped component in the electron VDF, in agreement with recent studies. In the high-beta side of the X-line, the magnetic field line is highly stretched in the third dimension. As a result, its curvature radius is comparable with a typical electron Larmor radius. The electron motion becomes chaotic, and therefore the electron idealness is no longer expected to hold. Around the middle of the outflow regions, the electron nonidealness is coincident with the region of the nonadiabatic motion.

Reference:
- Zenitani, S., H. Hasegawa, and T. Nagai, submitted to J. Geophys. Res. (MMS special issue)