1989
DOI: 10.1109/tgrs.1989.1398241
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Leaf-shape effects in electromagnetic wave scattering from vegetation

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Cited by 148 publications
(43 citation statements)
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“…It is possible to model the behavior of an incident waveĒ i in the direction (θ i , φ i ), of the incidence and look angle, using (1). The model follows the finite cylinder approximation [32,33] for stems, tillers and panicles and the physical optics approximation [34] for leaves. Additionally, the model variables are listed as: type of the morphological structure, t; scattering matrix element where q and p are polarization channels (q, p for H,V) for scattered and incident waves, f t qp ; propagation vector of the incident and scattered wave,k i,s p ; Fresnel reflection coefficients, R p (θ) and R q (θ).…”
Section: Backscattering Modelmentioning
confidence: 99%
“…It is possible to model the behavior of an incident waveĒ i in the direction (θ i , φ i ), of the incidence and look angle, using (1). The model follows the finite cylinder approximation [32,33] for stems, tillers and panicles and the physical optics approximation [34] for leaves. Additionally, the model variables are listed as: type of the morphological structure, t; scattering matrix element where q and p are polarization channels (q, p for H,V) for scattered and incident waves, f t qp ; propagation vector of the incident and scattered wave,k i,s p ; Fresnel reflection coefficients, R p (θ) and R q (θ).…”
Section: Backscattering Modelmentioning
confidence: 99%
“…The scatterers are then characterized by extinction and scattering properties, as a function of shape and size, using different approaches. The scattering amplitudes and the extinction cross sections of needles (representing coniferous forest leaves) were computed by using the model proposed by Karam et al [1989]. For cylinders (representing trunks and branches in forest) the "infinite length" approximation can be adopted.…”
Section: The Snow-vegetation Modelmentioning
confidence: 99%
“…The scattering of an arbitrarily polarized wave incident on the cylinder can be described in terms of the scattering amplitude tensor, F(k s ,k i ) [9]. If the field inside the cylinder is estimated as the field inside a similar, but infinite cylinder, then F(k s ,k i ) can be expressed as in [9, Equation (47)].…”
Section: Reflection and Scatteringmentioning
confidence: 99%