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Modeling Sun‐aligned polar cap arcs
Author(s) -
Crain D. J.,
Sojka J. J.,
Schunk R. W.,
Zhu L.
Publication year - 1994
Publication title -
radio science
Language(s) - English
Resource type - Journals
SCImago Journal Rank - 0.371
H-Index - 84
eISSN - 1944-799X
pISSN - 0048-6604
DOI - 10.1029/93rs01512
Subject(s) - tec , arc (geometry) , ionosphere , electron temperature , physics , plasma , atmospheric sciences , electron density , flow (mathematics) , electron precipitation , electron , precipitation , altitude (triangle) , computational physics , mechanics , meteorology , geophysics , geometry , mathematics , quantum mechanics , magnetosphere
We present results of a new model of the time‐dependent ionospheric response to a generalized steady state Sun‐aligned (SA) arc structure. The thermal and plasma structure of a “prototype” arc is compared to the general features of observed SA arcs. We find that the general features of electron density, N e , electron temperature, T e , and ion temperature, T i , are determined by the distribution of the particle precipitation and E × B convection associated with the SA arc. The model results are extended to predict the possible variation of N e , T e , and T i due to such arcs at Defense Meteorological Satellite Program altitude. An important parameter in determining the overall density enhancement produced by a SA arc is the speed of plasma flow across the arc. This is demonstrated by calculating the delta total electron content, ΔTEC, enhancement for various values of cross flow. Since cross‐flow is a relatively hard measurement to make, observations of ΔTEC associated with SA arcs can help place limits on the magnitude of the cross‐flow velocities for SA arcs. In conjunction with the National Science Foundation Coupling Energetic Dynamics of the Atmospheric Regions/High‐Latitude Plasma Structure initiative, we compare the results of the model with coordinated observations of several SA arcs which were observed at Qanaq, Greenland, on December 11, 1990. Comparison of our results and observations indicates a relatively low value for the cross‐flow speed (less than 25 m s −1 ) for these SA arcs.