A one-dimensional hybrid satellite track model has been developed to c
alculate the high-latitude thermospheric/ionospheric structure below t
he satellite altitude using Dynamics Explorer 2 (DE 2) satellite measu
rements and theory. This model is based on Emery et al. (1985) satelli
te track code but also includes elements of Roble et al. (1987b) globa
l mean thermosphere/ionosphere model. A number of parameterizations an
d data handling techniques are used to input satellite data from sever
al DE 2 instruments into this model. Profiles of neutral atmospheric d
ensities are determined from the MSIS-90 model and measured neutral te
mperatures. Measured electron precipitation spectra are used in an amo
ral model to calculate particle impact ionization rales below the sate
llite. These rates are combined with a solar ionization rate profile a
nd used to solve the O+ diffusion equation, with the measured electron
density as an upper boundary condition. The calculated O+ density dis
tribution, as well as the ionization profiles, are then used in a phot
ochemical equilibrium model to calculate the electron and molecular io
n densities. The electron temperature is also calculated by solving th
e electron energy equation with an upper boundary condition determined
by the-DE 2 measurement. The model enables calculations of altitude p
rofiles of conductivity and Joule heating rate along and below the sat
ellite track. In a first application of the new model, a study is made
of thermospheric and ionospheric structure below the DE 2 satellite f
or a single orbit which occurred on October 25, 1981. The held-aligned
Poynting flux, which is independently obtained for this orbit, is com
pared with the model predictions of the height-integrated energy conve
rsion rate. Good quantitative agreement between these two estimates ha
s been reached. In addition, measurements taken at the incoherent scat
ter radar site at Chatanika (65.1 degrees N, 147.4 degrees W) during a
DE 2 overflight are compared with the model calculations. A good agre
ement was found in lower thermospheric conductivities and Joule heatin
g rate.