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E - Bibliothèque et Archives Canada

E - Bibliothèque et Archives Canada

note that a -or of H is

note that a -or of H is multiplid with fields at grazing incidence. Equations 3.1 to 3.4 are four equations mth four unknomw that can k sdved for H; .H:, Hi and Hi. Once these four unknowrw are computed. and sinœ = fi x n , the current density on the surtace of the strip can be obtaineâ from: il On the umer surface: -&---Pl + ~ H ; D ~ ( - w ~,L,,o,o,~)x 2 Jw-p

ii)On the lower surface: 3.2.2 Code and Results The formulation of sedon 3.2.1 was used to mate the MGTD1 .FOR code. It contains the generic UTD dimadion coetiicient subrouthe. The set of Iinear equations was solved by fOrwardlbackward substitution rnethod based on PO]. The code was made flexible so that the total magnetic field wuld be computed with or without mulaple diffraction. Results from the moment method solution described in section 3.3 are plotteâ (in srnall cirdas) for cornparison: al 90' anale of nlane wave incidenœ: Several cases were considerd for a 90' angle of incidenœ. The idea behind that is to be able to evaluate the causes that wuld prevent the sucœss of UTD a low fnquency. Sinœ the UTD solution for a haif plane illuminated by a incident plane waw at 90' is an enrrd one. it would be expecbd that tb UTD solution sucœss of an eldcally small stnp (illuminatad by a plam wave at 90' and wnsidereâ to be the combination of two dg-) wouW depend on how low a

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