| P.H.Pathak and R.G. Kouyoumjian, "The dyadic diffraction coefficient for a perfectly conducting wedge," ElectroScience Lab., Ohio State Univ., Columbus, Rep. 21834, June 5,1970, Contract No. AF19(628)-5929. |
....[6] In the implementation of GTD, the radiated fields from the aperture antenna are first determined assuming an infinite ground plane. These fields are used to calculate the incident fields on the edges of finite ground plane. Employing the compact edge diffraction coefficients given in [7] and the incident field on the edges, the diffracted field in the forward as well as backward directions is calculated using the procedure given in [6] The total radiation field is then obtained by superposition of far field with infinite ground plane assumption and the diffracted field. To ....
....Effect of finite ground plane : The infinite ground plane solution described in the above sections yields the field radiated in the forward direction. This field is obtained by equation (11) The effect of finite ground plane is incorporated by employing the compact edge diffraction coefficients[7] and following the procedure described in [6] The radiation fields are supplemented by the additional field contributions arising from the diffraction by the edges of the finite ground plane. The diffracted field supplements the field in the forward region whereas it accounts totally for the ....
P.H.Pathak and R.G. Kouyoumjian, "The dyadic diffraction coefficient for a perfectly conducting wedge," ElectroScience Lab., Ohio State Univ., Columbus, Rep. 21834, June 5,1970, Contract No. AF19(628)-5929.
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Pathak, P. H.; and Kouyoumjian, R. G.: The Dyadic Diffraction Coefficient for a Perfectly Conducting Wedge. AFCRL-690546, U.S. Air Force, 1969. (Available from DTIC as AD 707 827.)
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