{"title":"New types of TLM nodes for the analysis of axially symmetric structures","authors":"S. Le Maguer, M. Ney","doi":"10.1109/ANTEM.1998.7861732","DOIUrl":null,"url":null,"abstract":"The Transmission Line Matrix (TLM) method is a well-known numerical time-domain technique which has been widely used for solving electromagnetic field problems. Axially symmetric structures are frequently encountered in microwave engineering. For this purpose, a first memory-saving TLM algorithm was developed in the particular case of uniform guiding structures [1]. Based on the classical Symmetrical Condensed Node (SCN) [2], this approach leads to a 1D mesh array using 18 complex voltages. Low memory requirement and simple algorithm make this method a very versatile tool. Extension of this model to general axially symmetric structure (2D mesh array) is not memory competitive compared to other time domain methods as BoR-FDTD [3,4].","PeriodicalId":334204,"journal":{"name":"1998 Symposium on Antenna Technology and Applied Electromagnetics","volume":"29 1","pages":"0"},"PeriodicalIF":0.0000,"publicationDate":"1998-08-01","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"0","resultStr":null,"platform":"Semanticscholar","paperid":null,"PeriodicalName":"1998 Symposium on Antenna Technology and Applied Electromagnetics","FirstCategoryId":"1085","ListUrlMain":"https://doi.org/10.1109/ANTEM.1998.7861732","RegionNum":0,"RegionCategory":null,"ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"","JCRName":"","Score":null,"Total":0}
引用次数: 0
Abstract
The Transmission Line Matrix (TLM) method is a well-known numerical time-domain technique which has been widely used for solving electromagnetic field problems. Axially symmetric structures are frequently encountered in microwave engineering. For this purpose, a first memory-saving TLM algorithm was developed in the particular case of uniform guiding structures [1]. Based on the classical Symmetrical Condensed Node (SCN) [2], this approach leads to a 1D mesh array using 18 complex voltages. Low memory requirement and simple algorithm make this method a very versatile tool. Extension of this model to general axially symmetric structure (2D mesh array) is not memory competitive compared to other time domain methods as BoR-FDTD [3,4].