Diffraction By a Circular Aperture At High Frequencies

$Cover Diffraction By a Circular Aperture At High Frequencies$

Harold Levine

The book Diffraction By a Circular Aperture At High Frequencies was written by author Harold Levine Here you can read free online of Diffraction By a Circular Aperture At High Frequencies book, rate and share your impressions in comments. If you don't know what to write, just answer the question: Why is Diffraction By a Circular Aperture At High Frequencies a good or bad book?

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7Uii . 505 1. 8 . 850 . 6U2 1. 9 . 9U5 . 783 2. 0 i. 029 . 922 2. 1 i. LOO 1. 0U2 2. 2 1. 158 1. 135 2. 3 1. 202 1. 200 2. U 1. 233 1. 235 2. 5 1. 251 1. 2U8 ti- tr' 1. 257 1. 2Uii 1. 253 1. 227 1. 2U0 1. 202 1. 218 1. 173 1. 190 1. 1U2 1. 158 I0I09 1. 122 1. 078 1. 085 i. 0U8 1. 0U8 1. 020 1. 012 0. 99U . 978 0. 969 . 9U8 0. 9U6 . 923 . 926 . 902 . 908 . 887 . 893 . 877 . 880 . 873 . 872 . 87U . 867 . 879 . 866 . 889 . 869 . 907 . 878 . 920 . 895 . 939 . 915 . 959 . 937 . 979 . 958 1. 075 1. 0...65 . 963 . 96U . 976 . 967 1. 0U2 1. 039 . 987 . 987 - Hi - 3* Screen integral equation In this section we base our fonnulation of the boundary-value problem on the representation (U). This leads naturally to an integral equation for the normal derivative of the wave function at the screen* Designating (23) ik K(p) - - ^ T(x, y, 0), p in S, and recalling that 3 T(x, y, 0) ■ 3 y^ (x, y, 0) in A, we rewrite (U) as 4 Ir - p'l /g |r - p'l From the requirement that the wave function vanish at the screen, the basic integral equation for K(p) followsi (25) K(p) 2-3 — 3— dS'- 2__ ;^-dS', p in S.

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