DRAFT Empirical models of the plasma density in the plasmasphere and polar cap Xueqin Huang, Bodo W. Reinisch, Paul Song, Gary S. Sales, Patrick Nsumei Environmental, Earth, & Atmospheric Sciences Department., Center for Atmospheric Research University of Massachusetts Lowell James J. Green, Robert F. Benson, Shing Fung NASA Goddard Space Flight Center Dennis L. Gallagher NASA Marshal Space Flight Center Jiannan Tu, James Horwitz Department of Physics, Center for Space Plasma and Aeronomic Research University of Alabama in Huntsville The Radio Plasma Imager (RPI) on the Imager for Magnetopause-to-Aurora Global Exploration (IMAGE) satellite [Burch et al., EOS Trans. American Geophys. Union, 82, 241-145, 2001] performs sounding in the frequency range from 3 kHz to 3 MHz using three orthogonal antennas, 500-m long dipoles in the spin plane, and a 20-m dipole along the spin axis. IMAGE is on an elliptical polar orbit with an altitude of 7.2 RE at apogee, and 1,200 km at perigee. Echo traces recorded on plasmagrams in the polar cap and the plasmasphere have been inverted into electron density profiles. When sounding from inside or outside the plasmapause, the echoes received from the plasmasphere are often diffuse in nature exhibiting substantial range spread and it is difficult to exactly determine the electron density profile. The direct echoes received from the topside ionosphere when IMAGE is in the polar cap, however, form very well defined traces that can be inverted to profiles. When IMAGE is sounding inside or close to the plasmapause there are very often clear echo traces with virtual ranges of up to 7 RE. Reinisch et al. [Geophys. Res. Lttrs., 28(24), 4521-4524, 2001] have shown that the waves producing these traces have propagated along the magnetic field lines and are reflected in the topside ionosphere. A newly developed profile inversion program calculates the electron density distribution either along the direct path from the spacecraft to the topside ionosphere in the polar cap, or along the magnetic field line through the spacecraft in the plasmasphere. The RPI sounding observations of the field aligned propagation echoes make it possible to measure the entire field-aligned profile from the satellite location to the ends of the field line in the topside ionosphere. This measurement is made within the time it takes to step through the frequencies that cover the plasma frequencies, generally less than 20 seconds. The polar cap soundings show the plasma density distribution from ~1Ð5 RE. The measurements show a clear dependence of the densities on magnetic activity. For the plasmasphere density distribution, we analyzed sounding data for two different periods: equinox and solstice. For June 2001, a sequence of eight consecutive profiles was determined for one morning pass when IMAGE changed position from L = 2.2 to L = 3.3. Soundings were made every two minutes. In March 2001, noon profiles were determined for L values between 2.4 and 3.6. Each sounding provides a complete hemisphere-to-hemisphere density profile. By piecing together these profiles along different L shells we were able to construct two-dimensional density distributions as a function of latitude and L-shell. The results show a symmetric north-south profile during the equinox period, and an asymmetric distribution at solstice with higher densities in the winter hemisphere. _______________ To be presented at the 27th General Assembly of International Union of Radio Science (URSI), Maastricht, The Netherlands, August 17-24, 2002.