“…For an object placed a distance f-d behind a lens of focallength f, and assurning that the object is of smaller spatial extent than the illurnination, the field distribution at the focal plane, Ur ( Xr, y f), can be written as a function of the object's spatial frequency spectrum T(f.,fy) [4]: The irradiance distribution at the focal plane will be proportional to the magnitude squared of the sum of the field distributions, which can be cast into a general irradiance distribution expression: (2) where Ibis the average value ofthe intensity, M is the modulation index ofthe irradiance pattem, and g(xr ,y r) is the phase variation across the film plane. For the specific case described here, it can be shown that [11]: The resulting transmittance recorded on the film can be approximated to the first order as [12]: (6) where Tb is the transmission of the film associated with the biasing exposure, ß is the slope of the Transmission-Exposure (T-E) curve at the biasing point, and M is the modulation.…”