TY - JOUR
T1 - Effect of the large-scale convection electric field structure on the formation of thin ionization layers at high latitudes
AU - Bristow, W. A.
AU - Watkins, B. J.
N1 - Funding Information:
Ar,kno~/rdgements~This work was supported by NSF grants ATM-8713215 and ATM-9213969.
PY - 1994/3
Y1 - 1994/3
N2 - A three-dimensional simulation of the high-latitude ionosphere was applied to investigate the geographical distribution of E-region thin ionization layers which may be formed by the action of the convection electric field. The simulation model computes the ion densities (O+, O+2, N+, N+2, NO+, Fe+), and temperatures as a function of altitude, latitude, and longitude. The stationary state momentum and continuity equations are solved for each ion species, then the energy equation is solved for electrons, neutrals, and a generic ion having the mean ion mass and velocity. The various electric field patterns of the Heppner and Maynard [(1987) J. geophys. Res. 92, 4467-4489] convection electric field model were applied and the ionization density pattern was examined after a time sufficient for the formation of thin layers (≈2000 s). It was found that large areas of thin ionization layers were formed for each of the electric field patterns examined. Southward IMF Bz conditions resulted in thin layers forming in the pre-midnight sector in the latitude range north of about 70° to about 80°, and after midnight between 60 and 70°. For northward Bz conditions, the layers were mainly in the pre-midnight sector and covered a latitude range from about 60 to 80°.
AB - A three-dimensional simulation of the high-latitude ionosphere was applied to investigate the geographical distribution of E-region thin ionization layers which may be formed by the action of the convection electric field. The simulation model computes the ion densities (O+, O+2, N+, N+2, NO+, Fe+), and temperatures as a function of altitude, latitude, and longitude. The stationary state momentum and continuity equations are solved for each ion species, then the energy equation is solved for electrons, neutrals, and a generic ion having the mean ion mass and velocity. The various electric field patterns of the Heppner and Maynard [(1987) J. geophys. Res. 92, 4467-4489] convection electric field model were applied and the ionization density pattern was examined after a time sufficient for the formation of thin layers (≈2000 s). It was found that large areas of thin ionization layers were formed for each of the electric field patterns examined. Southward IMF Bz conditions resulted in thin layers forming in the pre-midnight sector in the latitude range north of about 70° to about 80°, and after midnight between 60 and 70°. For northward Bz conditions, the layers were mainly in the pre-midnight sector and covered a latitude range from about 60 to 80°.
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U2 - 10.1016/0021-9169(94)90221-6
DO - 10.1016/0021-9169(94)90221-6
M3 - Article
AN - SCOPUS:38149147998
SN - 0021-9169
VL - 56
SP - 401
EP - 415
JO - Journal of Atmospheric and Terrestrial Physics
JF - Journal of Atmospheric and Terrestrial Physics
IS - 3
ER -