The diffraction by a dielectric wedge of an arbitrary aperture angle is studied by means of the generalized Wiener-Hopf technique. Generalized Wiener- Hopf equations are deduced that apparently cannot be solved in closed form. The factorization of the kernels can be reduced to Fredholm equations of the second kind by using a standard procedure (Fredholm factorization). The solutions of the Fredholm equations are obtained through a simple quadrature technique that very quickly yields a numerically stable evaluation of the unknowns of the generalizedWiener-Hopf equa- tions. The generalized Wiener-Hopf technique provides a representation of the fields only in certain regions of the spectral domain. To obtain valid solutions everywhere, a process of analytical continuation is required. This latter task is accomplished in the companion paper
The Wiener-Hopf formulation of the dielectric wedge problem.Part I / Daniele, Vito. - In: ELECTROMAGNETICS. - ISSN 0272-6343. - STAMPA. - 30:8(2010), pp. 625-643. [10.1080/02726343.2010.524878]
The Wiener-Hopf formulation of the dielectric wedge problem.Part I
DANIELE, Vito
2010
Abstract
The diffraction by a dielectric wedge of an arbitrary aperture angle is studied by means of the generalized Wiener-Hopf technique. Generalized Wiener- Hopf equations are deduced that apparently cannot be solved in closed form. The factorization of the kernels can be reduced to Fredholm equations of the second kind by using a standard procedure (Fredholm factorization). The solutions of the Fredholm equations are obtained through a simple quadrature technique that very quickly yields a numerically stable evaluation of the unknowns of the generalizedWiener-Hopf equa- tions. The generalized Wiener-Hopf technique provides a representation of the fields only in certain regions of the spectral domain. To obtain valid solutions everywhere, a process of analytical continuation is required. This latter task is accomplished in the companion paperPubblicazioni consigliate
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https://hdl.handle.net/11583/2422128
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