{"title":"Shape Reconstruction of Body of Revolution at Resonant Frequencies","authors":"Oleg Kusyy, N. N. Voitovich","doi":"10.1109/DIPED.2018.8543308","DOIUrl":null,"url":null,"abstract":"The method of obstacle shape reconstruction at its resonant frequencies is extended to the case of body of revolution. The scalar three-dimensional acoustic problem is reduced to a two-dimensional one. Connection between the field on the boundary and far field asymptotic is used for modeling a set of the scattering patterns. Resonant frequencies are defined as the frequencies at which the orthogonal complement function exists. Such a function generates the Herglotz wave function, one of whose zero lines is the boundary contour. The method is tested on several model examples.","PeriodicalId":146873,"journal":{"name":"2018 XXIIIrd International Seminar/Workshop on Direct and Inverse Problems of Electromagnetic and Acoustic Wave Theory (DIPED)","volume":"17 1","pages":"0"},"PeriodicalIF":0.0000,"publicationDate":"2018-09-01","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"2","resultStr":null,"platform":"Semanticscholar","paperid":null,"PeriodicalName":"2018 XXIIIrd International Seminar/Workshop on Direct and Inverse Problems of Electromagnetic and Acoustic Wave Theory (DIPED)","FirstCategoryId":"1085","ListUrlMain":"https://doi.org/10.1109/DIPED.2018.8543308","RegionNum":0,"RegionCategory":null,"ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"","JCRName":"","Score":null,"Total":0}
引用次数: 2
Abstract
The method of obstacle shape reconstruction at its resonant frequencies is extended to the case of body of revolution. The scalar three-dimensional acoustic problem is reduced to a two-dimensional one. Connection between the field on the boundary and far field asymptotic is used for modeling a set of the scattering patterns. Resonant frequencies are defined as the frequencies at which the orthogonal complement function exists. Such a function generates the Herglotz wave function, one of whose zero lines is the boundary contour. The method is tested on several model examples.