{"title":"曲线坐标系下任意形状波导特征值的FD-FD算法求解","authors":"L. Zhao, R. Carter","doi":"10.1109/EUMA.1992.335762","DOIUrl":null,"url":null,"abstract":"A finite-difference frequency-domain algorithm has been developed in non-orthogonal curvilinear co-ordinates. The full vector Maxwell's equations are discretized on boundary-fitted meshes. Because the algorithm is formulated in a non-orthogonal co-ordinate system, it is not restricted to any a special orthogonal co-ordinate system, and can over the conventional FD-FD algorithm in the orthogonal co-ordinate system. To demonstrate the method, several of the lowest eigenvalues of waveguides with arbitrary cross-section shapes have been computed. The subspace iterative algorithm is used to solve the unsymmetric eigen-equation. Boundary-orthogonal meshes are introduced in order to eliminate the error generated by non-orthogonal meshes on which the boundary conditions for the electromagnetic fields are not satisfied.","PeriodicalId":317106,"journal":{"name":"1992 22nd European Microwave Conference","volume":"08 1","pages":"0"},"PeriodicalIF":0.0000,"publicationDate":"1992-10-01","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"0","resultStr":"{\"title\":\"The Solution of Waveguides Eigenvalues with Arbitrary Shapes by FD-FD Algorithm in Curvilinear Co-Ordinates\",\"authors\":\"L. Zhao, R. Carter\",\"doi\":\"10.1109/EUMA.1992.335762\",\"DOIUrl\":null,\"url\":null,\"abstract\":\"A finite-difference frequency-domain algorithm has been developed in non-orthogonal curvilinear co-ordinates. The full vector Maxwell's equations are discretized on boundary-fitted meshes. Because the algorithm is formulated in a non-orthogonal co-ordinate system, it is not restricted to any a special orthogonal co-ordinate system, and can over the conventional FD-FD algorithm in the orthogonal co-ordinate system. To demonstrate the method, several of the lowest eigenvalues of waveguides with arbitrary cross-section shapes have been computed. The subspace iterative algorithm is used to solve the unsymmetric eigen-equation. Boundary-orthogonal meshes are introduced in order to eliminate the error generated by non-orthogonal meshes on which the boundary conditions for the electromagnetic fields are not satisfied.\",\"PeriodicalId\":317106,\"journal\":{\"name\":\"1992 22nd European Microwave Conference\",\"volume\":\"08 1\",\"pages\":\"0\"},\"PeriodicalIF\":0.0000,\"publicationDate\":\"1992-10-01\",\"publicationTypes\":\"Journal Article\",\"fieldsOfStudy\":null,\"isOpenAccess\":false,\"openAccessPdf\":\"\",\"citationCount\":\"0\",\"resultStr\":null,\"platform\":\"Semanticscholar\",\"paperid\":null,\"PeriodicalName\":\"1992 22nd European Microwave Conference\",\"FirstCategoryId\":\"1085\",\"ListUrlMain\":\"https://doi.org/10.1109/EUMA.1992.335762\",\"RegionNum\":0,\"RegionCategory\":null,\"ArticlePicture\":[],\"TitleCN\":null,\"AbstractTextCN\":null,\"PMCID\":null,\"EPubDate\":\"\",\"PubModel\":\"\",\"JCR\":\"\",\"JCRName\":\"\",\"Score\":null,\"Total\":0}","platform":"Semanticscholar","paperid":null,"PeriodicalName":"1992 22nd European Microwave Conference","FirstCategoryId":"1085","ListUrlMain":"https://doi.org/10.1109/EUMA.1992.335762","RegionNum":0,"RegionCategory":null,"ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"","JCRName":"","Score":null,"Total":0}
The Solution of Waveguides Eigenvalues with Arbitrary Shapes by FD-FD Algorithm in Curvilinear Co-Ordinates
A finite-difference frequency-domain algorithm has been developed in non-orthogonal curvilinear co-ordinates. The full vector Maxwell's equations are discretized on boundary-fitted meshes. Because the algorithm is formulated in a non-orthogonal co-ordinate system, it is not restricted to any a special orthogonal co-ordinate system, and can over the conventional FD-FD algorithm in the orthogonal co-ordinate system. To demonstrate the method, several of the lowest eigenvalues of waveguides with arbitrary cross-section shapes have been computed. The subspace iterative algorithm is used to solve the unsymmetric eigen-equation. Boundary-orthogonal meshes are introduced in order to eliminate the error generated by non-orthogonal meshes on which the boundary conditions for the electromagnetic fields are not satisfied.