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E - Bibliothèque et Archives Canada

E - Bibliothèque et Archives Canada

) On surface BC: At a

) On surface BC: At a certain point rn on BC: from equation (4.21) CI On surface CD: from equation (4.21) dl On surface DA: E$ = O (sinœ 0q'

from equation (4.21) On any surface, In paragraphs a) to d), HE& =HE+#& ad the evaluation of - requires the evaluation of a. As seen previously, this is 3~ %J easily obtained from the dope diffraction cdficicnt. 4.4.3 CoderndResub A cornputer code HGTDBXFOR was created baseci on the formulation of sections 4.3.1 and 4.3.2. It uses the same dope dintaction coefficient subrouüne used for the strip. As for the TEt case, cumrnt density distributions will be shown for a square cylinder illuminatd by a TMz plane wave. The diameter of the Minder =2a. The plots of the curient densities are against ph, where p is a linear distance on the surface of the Minder from edge A moving dodnnise. This mans that for pla =1, the position is h ahy behnnren A and B and if @a = 4, the position is at C. The reason for this representation is to be able to compare the results with plots alraady existent in the open literature [213[22). The nsuk f m the moment rnethod solution deswiôed in section 4.5. am plotted (in small cides) also for amparison.

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