“…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).…”