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E - Bibliothèque et Archives Canada

E - Bibliothèque et Archives Canada

3.4 RECTANGULAR CYLlNDER

3.4 RECTANGULAR CYLlNDER SURFACE CURRENT USlNG UTD After evaluaüng the strip. the rectangular cyiinder illumïnated by a T G plane wave (refar to Figure 3.23) was chosen for evaluation. The droits of the rectangular cylinder was considered because 1 is halfinmy betwem the exad half plane solution (n=2) and no difiradon at al1 (n=l). It is al- a sime geornetry subject to multiple dihction. This section will formulate the solution of the problem fimt and cover the d e and results afterward. 3.4.1 Formulation of the GO Fields Let's suppose the TEz plane wave (refsr to Figure 3.23) has a unit magnitude magnetic field at the origin and the incidenœ angk 9' can Vary between 0' and 90'. This means that the incident fields on points A. B. C. and O am: a1 On surface AB (tefer to fia 3.241: The incident field at any point is:

Figure 3.23: TEz plane wave incident on rcctangular cylin&r. Figure 3.21: Cginder sides geornety.

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