2012
DOI: 10.2528/pier12020205
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Multilayer Model Formulation and Analysis of Radar Backscattering From Sea Ice

Abstract: Abstract-The Antarctic continent is an extremely suitable environment for the application of remote sensing technology as it is one of the harshest places on earth. Satellite images of the terrain can be properly interpreted with thorough understanding of the microwave scattering process. The proper model development for backscattering can be used to test the assumptions on the dominating scattering mechanisms. In this paper, the formulation and analysis of a multilayer model used for sea ice terrain is presen… Show more

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Cited by 19 publications
(25 citation statements)
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“…By comparing this model with the measurements by [14] for validation, promising match is observed. In future, this model can be further improved by considering higher order scattering in the surface-volume formulation, considering the advanced IEM (AIEM) [21] in the surface scattering formulation, and considering multilayer in the model development [1].…”
Section: Resultsmentioning
confidence: 99%
“…By comparing this model with the measurements by [14] for validation, promising match is observed. In future, this model can be further improved by considering higher order scattering in the surface-volume formulation, considering the advanced IEM (AIEM) [21] in the surface scattering formulation, and considering multilayer in the model development [1].…”
Section: Resultsmentioning
confidence: 99%
“…The geometrical configuration adopted to solve the wave-scattering problem from the 2-D randomly-rough surface is given in Figure 4, where a rough interface z = h( r ), with r = (x, y), between two homogenous half-spaces, is considered [29][30][31][32]. The time dependence is assumed to be exp(−iω e t).…”
Section: Scattering Field Theorymentioning
confidence: 99%
“…In SSA, the geometrical configuration adopted to resolve the wavescattering problem from the 2-D randomly rough surface is given in Figure 3, where we consider a rough interface z = h(r ), with r = (x, y), between two homogenous half-spaces which are defined by their permittivity and permeability [26][27][28]. The time dependence is assumed to be exp (−iωt).…”
Section: Scattering Field Theory Of Rough Surface In Ssamentioning
confidence: 99%
“…Due to the random characteristics of the sea surface, the final bistatic NRCS and the backscattering coefficient are calculated as an average, i.e., σ 0 pq = σ 0 pq (27) Each NRCS is obtained over 100 realizations of sea surfaces.…”
Section: Scattering Field Theory Of Rough Surface In Ssamentioning
confidence: 99%