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E - Bibliothèque et Archives Canada

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to be based upon to

to be based upon to establish UTD results su- at low frequency. After all, currents are the building blocks for a multitude of practical resulfs used by industry and research. lt is important to note at this stage the discontinuity at the edges in Figure 2.3. Sinœ the d e used depends on e d e l of two simple half plane diffractions (back to back), if cp = O deg and Q = 3600 the diffracted fields are very difbrent. The sam dge, as part of a strip. is expected to be continuous as we go from cp = 359.Q0 to cp = 0.1 O. Double diffraction will eliminate this problem, but this. with additional details on cornputer codes used, will be discussed in later sections.

Ffgun, 2.2: Radiation pattern (Normalized pairiiier in dB) for a rnagnetic line source above (hetight = 0.0012) a strip (Mm = 0.2A , solid line) and a rectangular cyiinder (by 0.2 A ) using moment method.

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