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E - Bibliothèque et Archives Canada

E - Bibliothèque et Archives Canada

Now sinœ [5] which

Now sinœ [5] which after expansion in sine and cosine ternis becornes =A ; 4x12) then taking into consideration equation 2.7 this will lead to a diffraction The diffracteci field of equations 2.3 and 2.4 reduœs to

and the final fomulation of equations 2.3 and 2.4 is: 2.3.2 Sommerbld Exact Solution for the case of a half plane illuminated by a pcrpendiwlar plane wave (rd. to Cg. 2.1) Sommerfbld [6]m 1=8~0Ivecl the problm by mahods basd on the concept of a two-sheeted Riemann surface. The solution for total field (for a unity incident field) is:

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