A complete form is presented of the physical optics Solution to the diffraction by an arbitrary-angled dielectric wedge with any relative dielectric constant in both cases of E-and H-polarized plane wave incidences upon one side of two dielecphysical optics approximation to the dual integral equation formulated in the spatial frequency domain, is constructed by the geometrical optics terms, including multiple reflection inside the wedge and the edge diffracted field. The diffraction coefficients of the edge diffracted field are represented in a quite simple form as two finite series of cotangent functions weighted by the Fresnel's reflection coefficients. Far-field patterns of the some authors [ll], [12] to apply perturbation schemes, but their solutions were valid only for the restricted dielectric constant or wedge angle. ~~~~~~l there have been polarized wave diffraction by dielectric wedges with right [13] and general angles [14]. In this paper, a complete form of the physical optics solution to diffraction by a dielectric wedge with arbitrary dielectric constant and wedge angle is presented. By applying the Fourier transformation to the well-known Fredholm inte-tric interfaces. The solution, which is obtained by performing in Obtaining asymptotic to the Ephysical optics solutions for wedge angle 45", relative dielectric constants 2, 10, and 100, and E-polarized incident angle 150" are plotted in figures, where abrupt discontinuities appear at dielectric interfaces. The error of the physical optics solution is also interpreted explicitly by nonzeroness of the edge diffracted field in the complementary plane where two media inside and outside the dielectric wedge are exchanged with each other.