highly effective for reducing the error present in the physical-optics diffraction coefficients. 4 Convergence of the physical-optics diffraction coefficients f J w ) to the exact pattern p J w ) of E = 53 as E increases from 2 to 1000 for 0, = 60", 8, = 300", and 0, = 330" and O1 = 330" in Figure 1. The diffraction coefficients fl(w) and f, ("(w) are calculated by using Eqs. (7) and (12), respectively, and then compared to each other. Figure 4 illustrates the PODC f , ( w ) for E = 2, 10, 100, and 1000. The curves of f J w ) cross over the exact diffraction coefficients of the perfectly conducting wedge of E = m, p , ( w ) as E increases from 2 to 1000. According to the formulation of the dual integral equations, the exact diffraction coefficients become zero in the complementary wedge region [4]. However, the curves of f , ( w ) reveal large deviations from zero in S, and S,. Figure 5 shows the corrected diffraction coefficients of the composite wedge, f:"(w) in Eq. (12). The curves of f:"(w) approach monotonically to the exact diffraction coefficients of the perfectly conducting wedge ( E = m) as E increases from 2 to 1000 in the physical region of 0, I w I 0,. For any value of E , one finds that f!')(w) is closer to zero than f , ( w ) in the complementary regions of 0 I w < 0, and 0, < w I 2~. This implies that the suggested correction algorithm is