Diffraction of a High Frequency Plane Electromagnetic Wave By a Perfectly Conduc
Diffraction of a High Frequency Plane Electromagnetic Wave By a Perfectly Conduc
Douglas S Jones
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Consequently 33 -la 2 . , (1)+T&e (D+^e'd)-!:^ n 2rta | n^"^^'^l6a ^n''"^'''^^ '^n'' e^(0] -V^ (67, + ■ i 3/2 n^ ^ a (16 n (0) 2 ' + o(-t; a Because of (DI6), ■la a = ^= 1 rta + IL__2li. E_ -l^^l 1 . . Trti+ia i6a - & ^ -^ XsT^ " 7X37^ + 0(a 5 2, rt^a ' ij-rt^a- and, from (Dll), (69; le -la Srra 1 - ^ -i 2^) + 0(a ^; (70) a' = 0(a-^; n ^ ' (n> 1) Combining (66), (68) - (70) ve have wd(w)dw 2e la - -Tjti 1 1 '^-k' -la jta l-?fc) + 0(a2) 16a Hence, from (63) and (65), - 3^ - 1 3 7jri-2ia i . , . ..., rtl-6ia " = - ^. -!S + 0(a W/ a^/^ ^ I6jt2a^/^ ^ J This scattering coefficient agrees with that found by Seshradi and Wu [15] except for the last term. The numerical factor of the last term is foimd by them to be T/k- instead of 2j/l6; the difference is probably due to an arithmetical slip on one of our parts but this has not, so far, been located.
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