J. Otterman et al., SCATTERING BY LAMBERTIAN-LEAVES CANOPY - DEPENDENCE ON LEAF-AREA PROJECTIONS, International journal of remote sensing, 16(6), 1995, pp. 1107-1125
A single-scattering model is constructed for a canopy with Lambertian
leaves. The azimuthal distribution of the leaves is represented by fra
ctional abundances of the leaf-area in the cardinal directions with re
spect to the Sun. The canopy bi-directional reflectances are found to
be controlled by the projections of the leaf-areas onto horizontal and
vertical planes. The sum of the leaf-area projections onto the horizo
ntal plane determines the reflectance to the zenith when the Sun is at
the zenith. For a complete canopy this reflectance is [GRAPHICS] wher
e w(xh) is the fractional projection onto the horizontal plane of leaf
-area of leaf-category x, g(x) is the leaf reflectance (assumed equal
to the leaf transmittance), and Psi(x) is the zenith angle of the leaf
normal for this category. As the view and solar zenith angles deviate
from the nadir, the change in the reflectance in the principal plane
of the Sun is controlled by the difference in the leaf-area projection
s onto the vertical plane of the leaves with leaf-normals in opposite
quadrants in the principal plane. When these two leaf-categories are i
dentical (other than in their azimuths), a large region around the zen
ith exhibits the Lambertian viewing property, that is, the reflectance
does not change with the view or illumination directions. Forward sca
ttering and backscattering, which become intense when both the illumin
ation zenith angle theta 0, and the view zenith angle theta v, are lar
ge (approach 90 degrees) while Psi is not small (or when Psi is large
while theta 0, and theta v, are not small), are controlled by the slim
of these two leaf-area projections. The reflectance has then the limi
ting value g sin Psi'(cot theta 0 + cot theta v), where g and Psi char
acterize the two leaf categories with normals in the principal plane.
This expression represents a generalization of a result obtained for a
field of thin vertical cylinders,