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Asymptotic and hybrid methods in electromagnetics Let us turn now to the boundary condition on E1a and H1a . From (2.23) we have E1a = 0 for = 0. Chapter 1: Asymptotic theory of diffractionChapter 2: Electromagnetic creeping wavesChapter 3: Hybrid diffraction coefficientsChapter 4: Asymptotic currentsChapter 5: Hybrid methods: Series Title: IEE electromagnetic waves series, 51. Responsibility: Iran [i.e. Ivan] Andronov, Daniel Bouche, and Frédéric Molinet. Fugle fra oceanet