{"title":"由曲率跳变引起的衍射:在中等距离上接近极限射线的波场","authors":"E. Zlobina","doi":"10.1109/DD49902.2020.9274586","DOIUrl":null,"url":null,"abstract":"We are concerned with deriving formulas that describe high-frequency diffraction by a contour with a jump of curvature. In earlier research [1] we have shown that the rigorous boundary-layer approach allows obtaining an asymptotic expression for the wavefield near the limit ray in terms of the parabolic cylinder function D−3. This result is valid in a small neighborhood of the singular point of the contour. In this note we extend formulas for the vicinity of the limit ray to a larger distance.","PeriodicalId":133126,"journal":{"name":"2020 Days on Diffraction (DD)","volume":"29 1","pages":"0"},"PeriodicalIF":0.0000,"publicationDate":"2020-05-25","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"0","resultStr":"{\"title\":\"Diffraction by a jump of curvature: wavefield near the limit ray at a moderate distance\",\"authors\":\"E. Zlobina\",\"doi\":\"10.1109/DD49902.2020.9274586\",\"DOIUrl\":null,\"url\":null,\"abstract\":\"We are concerned with deriving formulas that describe high-frequency diffraction by a contour with a jump of curvature. In earlier research [1] we have shown that the rigorous boundary-layer approach allows obtaining an asymptotic expression for the wavefield near the limit ray in terms of the parabolic cylinder function D−3. This result is valid in a small neighborhood of the singular point of the contour. In this note we extend formulas for the vicinity of the limit ray to a larger distance.\",\"PeriodicalId\":133126,\"journal\":{\"name\":\"2020 Days on Diffraction (DD)\",\"volume\":\"29 1\",\"pages\":\"0\"},\"PeriodicalIF\":0.0000,\"publicationDate\":\"2020-05-25\",\"publicationTypes\":\"Journal Article\",\"fieldsOfStudy\":null,\"isOpenAccess\":false,\"openAccessPdf\":\"\",\"citationCount\":\"0\",\"resultStr\":null,\"platform\":\"Semanticscholar\",\"paperid\":null,\"PeriodicalName\":\"2020 Days on Diffraction (DD)\",\"FirstCategoryId\":\"1085\",\"ListUrlMain\":\"https://doi.org/10.1109/DD49902.2020.9274586\",\"RegionNum\":0,\"RegionCategory\":null,\"ArticlePicture\":[],\"TitleCN\":null,\"AbstractTextCN\":null,\"PMCID\":null,\"EPubDate\":\"\",\"PubModel\":\"\",\"JCR\":\"\",\"JCRName\":\"\",\"Score\":null,\"Total\":0}","platform":"Semanticscholar","paperid":null,"PeriodicalName":"2020 Days on Diffraction (DD)","FirstCategoryId":"1085","ListUrlMain":"https://doi.org/10.1109/DD49902.2020.9274586","RegionNum":0,"RegionCategory":null,"ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"","JCRName":"","Score":null,"Total":0}
Diffraction by a jump of curvature: wavefield near the limit ray at a moderate distance
We are concerned with deriving formulas that describe high-frequency diffraction by a contour with a jump of curvature. In earlier research [1] we have shown that the rigorous boundary-layer approach allows obtaining an asymptotic expression for the wavefield near the limit ray in terms of the parabolic cylinder function D−3. This result is valid in a small neighborhood of the singular point of the contour. In this note we extend formulas for the vicinity of the limit ray to a larger distance.