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Figure 12.2.11 Comparison of HH bistatic scattering coefficients (dB). Results of firstorder, second-order, and independent scattering as shown (50 realizations). The parameters are N s = 10, N c = 10, a c = 6.32 em, Ep = (20 + i3)EO, q = (15 + i5)EO, N = 100, VA = 560.5 cm,a = 1 em, L = 60 em, IJ"L = 1 em, A = 20 em, Bi = 45.55 , and cPi = 0 .

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In Table 12.2.1 and Table 12.2.2 we give the absorption coefficients, as defined by (12.2.62), for the clustering case with N s = 5 cylinders randomly distributed in each of N e = 20 clusters with the cluster radius a c = 10 em, for vertically polarized and horizontally polarized incident waves, respectively. The local fractional volume is 5%. The azimuthal angle <Pi of the incident wave is kept equal to 0 for all cases. We compare the results of first-order and second-order with the independent absorption case. The independent absorption is defined as the sum of the absorption of the cylinders assuming that each cylinder exists by itself. For the wave theory, we have tabulated I~g;, the first-order result and I~bsd, the second-order theory result. The second-order theory includes the first-order and second-order scattering results. We note that for the case of clustering, there is considerable mutual interaction such that the absorption is significantly enhanced. Since the absorption cross section is proportional to the square of the magnitude of internal field, it is expected that the internal field inside each cylinder is greatly altered by the strong coherent mutual interaction between scatterers which are close to each other. The small variation of the absorption coefficient for horizontal polarization with incident angles is due to the small tangential component of the exciting field which induces a small internal

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In this section, we study the multiple scattering by cylinders placed inside a parallel plate waveguide. The problem is conveniently formulated in terms of the dyadic Green's function of vector cylindrical waves and expressed in terms of waveguide modes. The case considered here resembles the coupling problem among multiple vias in high frequency circuits. The Foldy-Lax multiple scattering equations are derived using vector cylindrical waves and waveguide mode indices as basis functions. It is important to recognize that the Foldy-Lax equations are decoupled among the waveguide modes. In terms of the matrix equation, this decoupling reduces significantly the dimension of the matrix equation as one only needs to solve Foldy-Lax equation for each waveguide mode separately. In this section we also consider ring-like magnetic sources as excitation.

Consider two perfect electric conductors (PEC) at z = d/2 and z = -d/2. Let the magnetic source z' be between the two PEes (Fig. 12.3.1). Then the primary Green's function is given by (2.1.28) of 2, Volume 1. We consider the case when the magnetic current source sheet M s flows in the horizontal plane. Let It. = + yy be the transverse dyad. Then

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dx'dy'G(r, 7") . Ms(r')

(12.3.1)

The Green's function is next decomposed into a primary part and a response part G = G p + GR. The primary Green's function is ~ dk p_ l _ (-It eikz(z-z')+in(q,-q,') 47f J kpk z n o

> z'

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