Abstract:The behavior of TM-wave scattering from both semi-circular channels and bosses in a conducting plane is investigated. The scattered field is represented in terms of an infinite series of radial modes with unknown coefficients. By applying separation of variables and employing the partial orthogonality of sine functions, the unknown coefficients are obtained. The boundary conditions are checked for semi-circular channels and bosses to verify the algorithm proposed. Plotted results for the radar cross sections r… Show more
“…(Note that although in the latter case L and M are smooth functions, these functions are in fact nearly singular, for t near the endpoints of the parameter interval (0, 2π) for the curve x, and for τ around the corresponding endpoint of the parameter interval for the curve y.) Letting K denote one of the integral kernels L or M in equation (19), in view of the discussion above K may be expressed in the form K(t, τ ) = K 1 (t, τ ) log r 2 (t, τ )+K 2 (t, τ ) for smooth kernels K 1 and K 2 . For a fixed t then, there are two types of integrands for which high-order quadratures must be provided, namely integrands that are smooth in (0, 2π) but have singularities at the endpoints of the interval (that arise from corresponding singularities of the densities φ at the endpoints of the open curves; cf.…”
Section: Discretization Of Integral Equationsmentioning
confidence: 99%
“…Related semi-analytical separation-of-variables solutions are available for other simple configurations, such as semi-circular cavities and rectangular bumps and cavities (e.g. [8,9,13,19,24,23,25,31,32,39] and references therein), while solutions based on Fourier-type integral representations, mode matching techniques and staircase approximation of the geometry are available for more general domains (e.g. [5] and references therein).…”
This paper presents high-order integral equation methods for the evaluation of electromagnetic wave scattering by dielectric bumps and dielectric cavities on perfectly conducting or dielectric half-planes. In detail, the algorithms introduced in this paper apply to eight classical scattering problems, namely, scattering by a dielectric bump on a perfectly conducting or a dielectric half-plane, and scattering by a filled, overfilled, or void dielectric cavity on a perfectly conducting or a dielectric half-plane. In all cases field representations based on single-layer potentials for appropriately chosen Green functions are used. The numerical far fields and near fields exhibit excellent convergence as discretizations are refined-even at and around points where singular fields and infinite currents exist.
“…(Note that although in the latter case L and M are smooth functions, these functions are in fact nearly singular, for t near the endpoints of the parameter interval (0, 2π) for the curve x, and for τ around the corresponding endpoint of the parameter interval for the curve y.) Letting K denote one of the integral kernels L or M in equation (19), in view of the discussion above K may be expressed in the form K(t, τ ) = K 1 (t, τ ) log r 2 (t, τ )+K 2 (t, τ ) for smooth kernels K 1 and K 2 . For a fixed t then, there are two types of integrands for which high-order quadratures must be provided, namely integrands that are smooth in (0, 2π) but have singularities at the endpoints of the interval (that arise from corresponding singularities of the densities φ at the endpoints of the open curves; cf.…”
Section: Discretization Of Integral Equationsmentioning
confidence: 99%
“…Related semi-analytical separation-of-variables solutions are available for other simple configurations, such as semi-circular cavities and rectangular bumps and cavities (e.g. [8,9,13,19,24,23,25,31,32,39] and references therein), while solutions based on Fourier-type integral representations, mode matching techniques and staircase approximation of the geometry are available for more general domains (e.g. [5] and references therein).…”
This paper presents high-order integral equation methods for the evaluation of electromagnetic wave scattering by dielectric bumps and dielectric cavities on perfectly conducting or dielectric half-planes. In detail, the algorithms introduced in this paper apply to eight classical scattering problems, namely, scattering by a dielectric bump on a perfectly conducting or a dielectric half-plane, and scattering by a filled, overfilled, or void dielectric cavity on a perfectly conducting or a dielectric half-plane. In all cases field representations based on single-layer potentials for appropriately chosen Green functions are used. The numerical far fields and near fields exhibit excellent convergence as discretizations are refined-even at and around points where singular fields and infinite currents exist.
“…The methods mentioned in Ref. [9][10][11][12][13][14][15] have been developed for semi-circular and shallow circular cavities, and therefore they are not a general method that can be utilised for variants of circular cavities. In addition to the described approaches, meshing methods such as the finite element method (FEM) and MoM may also be used to analyse scattering from circular cavities.…”
Section: Introductionmentioning
confidence: 99%
“…In this paper, an efficient method based on the modal expansion technique is developed to determine the scattered wave from a circular cavity of arbitrary shape. This meshless technique is more time-efficient than fully numerical methods such as FEM and MoM and does not have the limitations of the methods proposed in [9][10][11][12][13][14][15].…”
Section: Introductionmentioning
confidence: 99%
“…In recent years, various efficient techniques have been developed for the problem of the scattering by gaps and cavities to improve both accuracy and speed of simulations [1][2][3][4][5][6][7][8][9][10][11][12][13][14][15]. In line with previous studies conducted on scattering from open cavities, we study the problem of the scattering from a circular cavity of arbitrary shape subjected to a plane wave of arbitrary polarisation.…”
An efficient modal expansion technique for scattering by a circular cavity with an arbitrary arc in a perfect electric conductor is developed. In contrast to the existing methods proposed for a shallow or semi‐circular cavity, the proposed method can be utilised for a circular cavity of arbitrary shape while is computationally efficient. The authors first introduce an auxiliary circular border that divides half‐space above the cavity into two separate subregions. Then, the tangential fields in the two subregions, which satisfy the Helmholtz equation, are expanded in terms of an infinite series of radial wave functions. The fields are matched at the auxiliary border to construct three independent equations in two different coordinate systems. By employing the addition theorem, all equations are transferred into the same coordinate system. Finally, the equations are converted into a system of linear equations and then solved through regular matrix techniques for the expansion coefficients. The solution is verified by the Method of Moments used in FEKO electromagnetic simulation software. This method is employed to study the effects of cavity shape and incident wave polarisation on the scattering signature.
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