“…Clearly, the inverse relationship between K and the induced specular flow u indicates that the magnitude of the specular flow grows dramatically as surface curvature decreases. Second, while specular flows exhibit magnitude singularities at (for orthographic observer [1]) or near (for perspective observer [21]) the projection of parabolic points, at these points they also exhibit orientation singularities. Formally, if m(x, y) and θ (x, y) are the magnitude and orientation components of the specular flow at each point, respectively, α(s) is a parametric representation of the singularity cirve and β (t) is an image curve that intersects α(s) non transversely at time t = 0, then the one sided limits at that point of intersection satisfy…”