Appendix to Section 7.9.2 Field
Radiated by Modified Uniform Currents
Induced on Elementary Strips
Here we investigate the field radiated by the currents
induced by the incident wave (7.128) on the finite elementary strips (0 ⩽ ξ1, 2 ⩽ l) belonging to the finite plane faces of a scattering object (Fig. 7.3). These currents are defined as those induced on the illuminated faces of the tangential half-planes (φ = 0 and φ = α); that is,
.
In this investigation we employ the right-hand Cartesian coordinates x, y, z and x′, y′, z associated with faces 1 and 2, respectively. The axes x and x′ belong to faces 1 and 2, respectively, and they are parallel to tangents τ1 and τ2. According to the solution of the half-plane diffraction problem presented in Chapter 2, the current on strip 1 is described as
with
The current components and on strip 2 are ...
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