TY - JOUR
T1 - Magnetosphere-Ionosphere Convection Under the Due Northward IMF
AU - Tanaka, T.
AU - Obara, T.
AU - Watanabe, M.
AU - Fujita, S.
AU - Ebihara, Y.
AU - Kataoka, R.
AU - Den, M.
N1 - Funding Information:
In the present study, we used the high-speed computing system at Polar Data Center of National Institute of Polar Research through General Collaboration Project 29-5. This study was supported by KAKENHI (Grant 15H03732) and MEXT/JSPS KAKENHI Grant 15H05815. Numerical data (coordinate data and variable data), information for graphic program, and history data necessary to reproduce drawings are available online (http://polaris.nipr.ac.jp/~reppu/reppu2/reppu2/reppu4/).
Publisher Copyright:
©2019. American Geophysical Union. All Rights Reserved.
PY - 2019/8/1
Y1 - 2019/8/1
N2 - Convection under the due northward interplanetary magnetic field (IMF) is reproduced by the global simulation. The resulting magnetosphere is closed except in the XZ plane and separated from the solar wind by the separatrix generated from cusp nulls. Inside the separatrix, there exist three plasma regimes of the cusp high-pressure region, the low-latitude boundary layer (LLBL) and the plasma sheet. In the ionosphere, the northward Bz (NBZ) current and the reverse cell occur in higher latitudes than 80°, and the fun-shaped arc-like field-aligned current and the main oval occur in lower latitudes than 80°. Magnetic field lines in the antisunward flow region of the reverse cell are connected to the LLBL that is accelerated to supersonic flow by the cusp pressure. Circulation on the reverse cell in the ionosphere is as a whole constructed to the interchange cycle in the magnetosphere. Convection is looked upon as the process to discharge stress generated by the dayside cusp reconnection. Magnetic stress generated by the reconnection is first converted to thermal energy in the cusp. This thermal energy is drained through three possible routes: release of plasma downtail through the LLBL, dissipation as electromagnetic energy through formation of the dynamo, and evacuation down to the ionosphere through the plasma sheet.
AB - Convection under the due northward interplanetary magnetic field (IMF) is reproduced by the global simulation. The resulting magnetosphere is closed except in the XZ plane and separated from the solar wind by the separatrix generated from cusp nulls. Inside the separatrix, there exist three plasma regimes of the cusp high-pressure region, the low-latitude boundary layer (LLBL) and the plasma sheet. In the ionosphere, the northward Bz (NBZ) current and the reverse cell occur in higher latitudes than 80°, and the fun-shaped arc-like field-aligned current and the main oval occur in lower latitudes than 80°. Magnetic field lines in the antisunward flow region of the reverse cell are connected to the LLBL that is accelerated to supersonic flow by the cusp pressure. Circulation on the reverse cell in the ionosphere is as a whole constructed to the interchange cycle in the magnetosphere. Convection is looked upon as the process to discharge stress generated by the dayside cusp reconnection. Magnetic stress generated by the reconnection is first converted to thermal energy in the cusp. This thermal energy is drained through three possible routes: release of plasma downtail through the LLBL, dissipation as electromagnetic energy through formation of the dynamo, and evacuation down to the ionosphere through the plasma sheet.
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U2 - 10.1029/2019JA026547
DO - 10.1029/2019JA026547
M3 - Article
AN - SCOPUS:85071221729
SN - 2169-9380
VL - 124
SP - 6812
EP - 6832
JO - Journal of Geophysical Research: Space Physics
JF - Journal of Geophysical Research: Space Physics
IS - 8
ER -