Premium
THEMIS two‐point measurements of the cross‐tail current density: A thick bifurcated current sheet in the near‐Earth plasma sheet
Author(s) -
Saito Miho
Publication year - 2015
Publication title -
journal of geophysical research: space physics
Language(s) - English
Resource type - Journals
eISSN - 2169-9402
pISSN - 2169-9380
DOI - 10.1002/2015ja021142
Subject(s) - current sheet , heliospheric current sheet , current (fluid) , current density , plasma sheet , solar wind , physics , plane (geometry) , geophysics , interplanetary magnetic field , geometry , plasma , magnetosphere , magnetohydrodynamics , mathematics , quantum mechanics , thermodynamics
Abstract The basic properties of the near‐Earth current sheet from 8 R E to 12 R E were determined based on Time History of Events and Macroscale Interactions during Substorms (THEMIS) observations from 2007 to 2013. Ampere's law was used to estimate the current density when the locations of two spacecraft were suitable for the calculation. A total of 3838 current density observations were obtained to study the vertical profile. For typical solar wind conditions, the current density near (off) the central plane of the current sheet ranged from 1 to 2 nA/m 2 (1 to 8 nA/m 2 ). All the high current densities appeared off the central plane of the current sheet, indicating the formation of a bifurcated current sheet structure when the current density increased above 2 nA/m 2 . The median profile also showed a bifurcated structure, in which the half thickness was about 3 R E . The distance between the peak of the current density and the central plane of the current sheet was 0.5 to 1 R E . High current densities above 4 nA/m 2 were observed in some cases that occurred preferentially during substorms, but they also occurred in quiet times. In contrast to the commonly accepted picture, these high current densities can form without a high solar wind dynamic pressure. In addition, these high current densities can appear in two magnetic configurations: tail‐like and dipolar structures. At least two mechanisms, magnetic flux depletion and new current system formation during the expansion phase, other than plasma sheet compression are responsible for the formation of the bifurcated current sheets.