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E - Bibliothèque et Archives Canada

E - Bibliothèque et Archives Canada

Bessel fundions

Bessel fundions subrouüne[25]. Figures 4.1 and 4.5 am identical even at the edge. Meimer [6] has studied this singularity for the TMz case and has introduced a suitable condition to rnake sure the solution is unique. Meimr's edge condition requires the energy density to be integrable at the edge. Figure 4.6 shows the current density (representing only Ha) mullplied by fi for the case of Figure 4.1. the value converges and is finite near the edge. The code EEDGEFOR is considead adequate for the present evaluation and its formulation will be used as a building block for the solution of more cornplex shapes in the next secüons.

2 2.5 3 RH0 in Lambdas ïMz plane wave T ----- n=2 Figure 4.1: Magnitude of current distribution on the surface of a haif plane (n=2) illuminated by a TMz plane wave at 9' =90 O (J in Afn1.p in k)-UTD.

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