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Dependence of the high‐latitude lower thermospheric wind vertical vorticity and horizontal divergence on the interplanetary magnetic field
Author(s) -
Kwak Y.S.,
Richmond A. D.
Publication year - 2014
Publication title -
journal of geophysical research: space physics
Language(s) - English
Resource type - Journals
eISSN - 2169-9402
pISSN - 2169-9380
DOI - 10.1002/2013ja019589
Subject(s) - vorticity , physics , thermosphere , interplanetary magnetic field , advection , atmospheric sciences , vorticity equation , potential vorticity , positive vorticity advection , geophysics , ionosphere , magnetic field , vortex , solar wind , mechanics , quantum mechanics , thermodynamics
We analyze the vertical component of vorticity and the horizontal divergence of the high‐latitude neutral wind field in the lower thermosphere during the southern summer time for different interplanetary magnetic field (IMF) conditions with the aid of the National Center for Atmospheric Research thermosphere ionosphere electrodynamics general circulation model, with the following results. (1) The mean neutral wind pattern in the high‐latitude lower thermosphere is dominated by rotational flow, imparted primarily through the ion drag force rather than by horizontally divergent flow. (2) The vertical vorticity depends on the IMF. (3) The difference vertical vorticity, obtained by subtracting values with zero IMF from those with nonzero IMF, is much larger than the difference horizontal divergence for all IMF conditions. (4) The effects of IMF penetrate down to 106 km altitude. To determine the processes forcing strong rotational flow in the high‐latitude lower thermospheric wind fields, a term analysis of the vorticity equation is also performed, with the following results. (1) The primary forcing term that determines variations of the vertical vorticity is ion drag. This forcing is closely related to the flow of field‐aligned current between the ionosphere and magnetosphere. Significant contributions to variations of the vorticity, however, can be made by the horizontal advection term. (2) The effects of the IMF on the ion drag forcing are seen down to around 106 km altitude. (3) The continual forcing of magnetic zonal mean B y ‐dependent vertical vorticity by ion drag can lead to strong polar vortices.