“…Consider the limiting case of a highly shallow specimen in which only one fringe order is observed when the shearing distance equals half the specimen width. Then, using a finite difference relation for the phase change in the optical wave front, aS = S (xl,x2 + ~) -S(xl,x2) = X, (6) where d/2 is half the specimen width and represents the shearing distance and k is the wavelengrth of light. Thus, normal curvature is approximated as Therefore, for a typical specimen width of 50 mm and wavelength of light of 632.8 rim, we obtain a limiting minimum value of curvature, ~:22 ~ 0.001 m -1, that is, a maximum radius of curvature of 1000 m. Thus, the technique needs to be enhanced for its application to very fiat specimens with curvatures k: < 0.001 m -].…”