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E - Bibliothèque et Archives Canada

E - Bibliothèque et Archives Canada

-On the shadow side: H'

-On the shadow side: H' = H' = 0 since 0°< Q'

As shown in the previous section, computing a is a matter of multiplying two 3~ tem out of the four temnr of the dope dimaaion codicient by a minus sign. It should be noted hem that no multiple difiadion is considered in aie present case, since the diflracted field is zero at the surface. From equation 4.9 to 4.14, the total tangential magnetic field is and the current density can be evaluated from - n x H j, - 4.2.2 Code and Resuîts A cornputer code TMzGTD1 .FOR was created based on the formulation of saaion 4.2.1. It uses the modified slope difbaction coefficient subroutine to A large number of plots were produced to verify the de, only few will be induded here. As an independent check with open litemture, the code reproduced exadly Figure 12.15 in [2]. Results from the moment mcthod solution desuibed in section 4.3 are plotted (in small circlea) also for cornparison. it is worth noting that muitiple diffraction was not neœssary to get a good result for the TMz case.

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