MODELING SYNTHETIC-APERTURE RADAR (SAR) SCATTERING FROM A SEASONALLY VARYING SNOW-COVERED SEA-ICE VOLUME AT 5.3 AND 9.25 GHZ

Citation
Dg. Barber et Ef. Ledrew, MODELING SYNTHETIC-APERTURE RADAR (SAR) SCATTERING FROM A SEASONALLY VARYING SNOW-COVERED SEA-ICE VOLUME AT 5.3 AND 9.25 GHZ, Polar research, 13(1), 1994, pp. 35-54
Citations number
23
Categorie Soggetti
Geosciences, Interdisciplinary",Geology,Oceanografhy
Journal title
ISSN journal
08000395
Volume
13
Issue
1
Year of publication
1994
Pages
35 - 54
Database
ISI
SICI code
0800-0395(1994)13:1<35:MSR(SF>2.0.ZU;2-8
Abstract
A series of sensitivity analyses using dielectric, mixture and microwa ve scattering models is presented. Data from the Seasonal Sea Ice Moni toring and Modeling Site (SIMMS) in 1990 and 1991 are used to initiali ze the models. The objective of the research is to investigate the rol e of various geophysical and electrical properties in specifying the t otal relative scattering cross section (sigma0) of snow covered first- year sea ice during the spring period. The seasonal transition period from the Winter SAR scattering season to Early Melt was shown to signa l a transition in dielectric properties which caused the snow volume t o become a factor in the microwave scattering process. The effect of t he thermal insulation of a snow cover on sea ice was shown to be signi ficant for both epsilon' and epsilon''. Higher atmospheric temperature s caused proportionally greater changes in the dielectric properties o f the sea ice at the base of the snow cover. Model sigma0 was computed for a range of sensor, sensor-earth geometry, and geophysical propert ies. In the Winter season the surface roughness terms (sigma(h) and L) were shown to have a significant impact on sigma(0) when the ice surf ace was the primary scattering mechanism. Once the snow cover began to warm and water was available in a liquid phase, the ice surface becam e masked because of the decrease in microwave penetration depths. Duri ng this period the water volume variable dominated sigma(0), both from its impact on sigma(v)0, and due to its control over the dielectric m ismatch created at the air/snow interface.