Abstract:A numerical approach for investigating the bandwidth of ridged circular waveguides is described in this article. This approach is the combination of the boundary element method (BEM) and modifying the boundary, which is first proposed here. By this approach, high convergence of numerical solution and good agreement between experimental results and theoretical results can both be achieved.
“…Equation (13) represents the boundary condition. Equations (12) and (13) are formulated only for one element, then the coefficient matrices E 0 , E 1 , E 2 and M 0 are assembled into overall matrices of the whole structure, as in the standard FEM.…”
Section: Scaled Boundary Finite Element Methods For Waveguide Problemsmentioning
confidence: 99%
“…The transmission characteristics of quadruple‐ridged waveguides have been obtained by using various numerical approaches including the FEM , the magnetic field integral equation method , the multilayer perceptron NN model , the mode‐matching method , the transverse resonance technique , the Ritz–Galerkin approach , the BEM , the multipole theory and so on. It is well accepted that, among those methods, the FEM is undoubtedly the dominant one for modelling waveguide problems at present because of its powerful capability of simulating a large variety of problems with complex structural geometries, complicated material properties and various boundary conditions.…”
“…Equation (13) represents the boundary condition. Equations (12) and (13) are formulated only for one element, then the coefficient matrices E 0 , E 1 , E 2 and M 0 are assembled into overall matrices of the whole structure, as in the standard FEM.…”
Section: Scaled Boundary Finite Element Methods For Waveguide Problemsmentioning
confidence: 99%
“…The transmission characteristics of quadruple‐ridged waveguides have been obtained by using various numerical approaches including the FEM , the magnetic field integral equation method , the multilayer perceptron NN model , the mode‐matching method , the transverse resonance technique , the Ritz–Galerkin approach , the BEM , the multipole theory and so on. It is well accepted that, among those methods, the FEM is undoubtedly the dominant one for modelling waveguide problems at present because of its powerful capability of simulating a large variety of problems with complex structural geometries, complicated material properties and various boundary conditions.…”
“…Equation 23is in the same form as the definition of the dynamic stiffness matrix in Equation (19). Denoting ϕ (0) = ϕ.…”
Section: Formulation Of the Generalized Eigenvalue Equation For Wavegmentioning
confidence: 99%
“…Among them, quadruple-ridge waveguides find wide applications, especially in antenna and radar systems [4,5] because of their supporting dual-polarization capabilities. The transmission characteristics of quadruple ridged waveguides have been obtained by employing various numerical approaches including the finite element method (FEM) [13], the magnetic field integral equation (MFIE) method [14], multilayer perceptron neural network model (MLPNN) [15], mode-matching method (MMM) [16] transverse resonance technique [17], Ritz-Galerkin approach [18], boundary element method (BEM) [19], Multipole Theory (MT) [20]. In practical applications, the quadruple ridges in a square waveguide are usually cut at their corners [21] as shown in Figure 1, which contains reentrant corners.…”
This paper presents an extension of the recently-developed efficient semi-analytical method, namely scaled boundary finite element method (SBFEM) to analyze quadruple corner-cut ridged circular waveguide. Owing to its symmetry, only a quarter of its crosssection needs to be considered. The entire computational domain is divided into several sub-domains. Only the boundaries of each subdomain are discretized with line elements leading to great flexibility in mesh generation, and a variational approach is used to derive the scaled boundary finite element equations. SBFEM solution converges in the finite element sense in the circumferential direction, and more significantly, is analytical in the radial direction. Consequently, singularities around re-entrant corners can be represented exactly and automatically. By introducing the "dynamic stiffness" of waveguide, using the continued fraction solution and introducing auxiliary variables, a generalized eigenvalue equation with respect to wave number is obtained without introducing an internal mesh. Numerical results illustrate the accuracy and efficiency of the method with very few elements and much less consumed time. Influences of corner-cut ridge dimensions on the wave numbers of modes are examined in detail. The single mode bandwidth of the waveguide is also discussed. Therefore, these results provide an extension to the existing design data for ridge waveguide and are considered helpful in practical applications.
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