Abstract:[1] A semielliptical channel flush-mounted under a metal plane and slotted along the interfocal distance of its cross section is separated from the half-space above by a multilayer diaphragm. The cavity, the diaphragm, and the half-space are all isorefractive to each other. Both the cavity and the multilayer diaphragm are filled with materials isorefractive to the medium in the half-space above. This is a two-dimensional geometry where the source is invariant with respect to the axial variable. The resulting e… Show more
“…The isorefractive condition led to many new exact analytical solutions for canonical geometries in many coordinate systems, including: the circular cylinder [5], the elliptic cylinder [6], [7], the oblate spheroidal [8], the prolate spheroidal [9], and the paraboloidal [10]. These new solutions provide additional benchmarks for the validation of computational electromagnetic software.…”
The isorefractive condition augments the set of geometries for which electromagnetic boundary value problems are solvable with the mode matching method. From a teaching viewpoint, understanding the isorefractive condition enables to appreciate the underpinnings of the special functions used in certain coordinate systems. From a research viewpoint, the isorefractive condition extends the set of problems for which an exact solution is known, thus leading to new canonical problems that can be used as challenging benchmarks to validate numerical approaches.
“…The isorefractive condition led to many new exact analytical solutions for canonical geometries in many coordinate systems, including: the circular cylinder [5], the elliptic cylinder [6], [7], the oblate spheroidal [8], the prolate spheroidal [9], and the paraboloidal [10]. These new solutions provide additional benchmarks for the validation of computational electromagnetic software.…”
The isorefractive condition augments the set of geometries for which electromagnetic boundary value problems are solvable with the mode matching method. From a teaching viewpoint, understanding the isorefractive condition enables to appreciate the underpinnings of the special functions used in certain coordinate systems. From a research viewpoint, the isorefractive condition extends the set of problems for which an exact solution is known, thus leading to new canonical problems that can be used as challenging benchmarks to validate numerical approaches.
“…A brief literature survey finds that, in addition to the known exact solutions published in [2], the introduction of the isorefractive condition by Uslenghi [3,4] allowed for the development of many new exact solutions. In particular, new geometries involving isorefractive materials are available for scattering from infinite bodies, such as shapes involving the 2D wedge [5][6][7], the elliptical cylinder [8][9][10][11][12][13][14][15][16][17][18], the paraboloid [19][20][21], and finite bodies, such as shapes involving spheroidal geometries [22][23][24][25].…”
A new exact for a solution half oblate spheroidal cavity filled with double-negative and double-positive metamaterials and surrounded by perfect electric conductor walls with a circular opening is considered. The structure is illuminated by a dipole source, either electric or magnetic, located on the axis of symmetry and axially oriented. Analytical expressions and numerical examples are provided.
“…Therefore, this article provides expressions for both radial and angular functions using the Stratton-Morse-Chu normalization. The choice of the Stratton-Morse-Chu normalization is dictated by a vast collection of analytical results that already exist, such as [5], [30], [7], [12], [13], [31], [14], [38], [39], [6].…”
Abstract. Small parameter power series expansions for both radial and angular Mathieu functions are derived. The expansions are valid for all integer orders and apply the Stratton-Morse-Chu normalization. Three new contributions are provided: (1) explicit power series expansions for the radial functions, which are not available in the literature; (2) improved convergence rate of the power series expansions of the radial functions, obtained by representing the radial functions as a series of products of Bessel functions; (3) simpler and more direct derivations for the power series expansion for both the angular and radial functions. A numerical validation is also given.
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