Abstract
The standard reflectance model for inhomogeneous materials suggests that to a good approximation the reflectance function can be described as the weighted sum of two functions1,2. One function represents the interface (specular) reflection, and the second function represents the subsurface (diffuse) reflection. Let SI(λ) and SS(λ) be the surface spectral reflectances for the two components of interface and subsurface reflections, and let E(λ) be the spectral power distribution of the incident light. Then reflected light is where cI(θ) and cS(θ) are the geometric scale factors. The parameters θ vary with the viewing geometry. In a previous paper2 we have evaluated this model and shown how to use light reflected from pairs of surfaces to estimate the spectral power distribution of the illuminant.
© 1989 Optical Society of America
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