Interpreting Local and Remote RPI/IMAGE Plasmaspheric Electron Density Measurements using a Global Plasmasphere-Ionosphere Model Phillip A. Webb NRC NASA/Goddard Space Flight Center, Code 692 Greenbelt, Maryland 20771 USA Robert F. Benson NASA/Goddard Space Flight Center, Code 692 Greenbelt, Maryland 20771 USA Bodo W. Reinisch Center for Atmospheric Research University of Massachusetts at Lowell Lowell, Massachusetts 01854 USA The Imager for Magnetopause-to-Aurora Global Exploration (IMAGE) satellite is currently in a highly inclined elliptical orbit that takes it between altitudes of 1000 km and seven Earth radii. During each 14.2 hour orbit, IMAGEÕs instruments have the opportunity to observe the plasma distribution from the topside ionosphere to beyond the plasmapause. One such instrument carried by IMAGE is the Radio Plasma Imager (RPI). Using the RPI, the local electron density Ne can be separately calculated from plasma resonances stimulated during active soundings and natural emissions received during the passive recording of dynamic spectrograms. An along-orbit Ne profile can be obtained for each orbit by calculating Ne from these active and passive measurements. Furthermore, the active RPI soundings often produce reflection traces that can be converted into Ne profiles along the local field line into both hemispheres using inversion and ray-tracing techniques. Both these types of Ne profiles can be compared to the predictions of plasmaspheric models. The theoretical-based Global Plasmasphere Ionosphere Density (GPID) model has been developed by the first author to simulate the global scale evolution of the ion and electron number densities in the plasmasphere. Combined with the latest version of the International Reference Ionosphere (IRI), GPID can model the dynamic emptying caused by geomagnetic storms and the following refilling of the plasmasphere. The accuracy of the GPID will be ascertained by comparing the models predictions with RPI derived Ne profiles across a variety of geomagnetic L-shells and various geomagnetic storm conditions. _______________ To be presented at the Western Pacific Geophysical Meeting, Wellington, New Zealand, 9-12 July 2002.