EE 350 Radioscience Seminar
Professor Umran S. Inan
Winter 2003-2004
Date: Wednesday, February 25, 2004
Time: 4:15 PM – Refreshments at 4:00
Location: Bldg. 160, Room 323
Radio Sounding of Geospace Plasmas
Prof. Bodo W. Reinisch Environmental, Earth, and Atmospheric Sciences Department Center for Atmospheric
Research, University of Massachusetts Lowell
Abstract
Radio sounding is a well-established technique that was first deployed in the 1920's for ionospheric sounding from the ground. In recent
years, advanced digital sounders were developed that use multi-antenna Doppler imaging for ground-based and satellite observations of geospace plasmas providing detailed
information about its structure and dynamics. These modern sounders measure more than just the time of flight and amplitude of the reflected echo pulses, they also
determine the arrival angle, wave polarization, and Doppler frequency. Radio sounding relies on total (specular) reflection of radio waves from plasma structures that
have plasma frequencies fN equal to the radio frequencies f for the ordinary wave mode. It is, therefore, not possible on the ground to receive echoes reflected from the
topside ionosphere -unlike the incoherent scatter radar echoes- or the magnetosphere/plasmasphere since the F2 layer prevents all transmitted waves with frequencies f <
foF2 (the maximum plasma frequency) from propagating beyond the height of the F2 layer peak. This presentation will review the state of the art in interferometric
Doppler imaging on the ground for routine measurement of F region plasma drifts and show observational results from the polar and equatorial ionosphere. Recently, the
radio plasma imager (RPI) on NASA's IMAGE satellite started using modern radio sounding techniques for measurements in the magnetosphere, sounding with frequencies from
3 kHz to 3 MHz, corresponding to electron densities of Ne " 105 to 1011 m-3. This talk will show how the plasma density distribution in the plasmasphere is derived from
echo signals with f > fpe that propagate along magnetic field lines.
|