{"title":"螺旋聚焦表面构象转变的数值模拟","authors":"R. Steenblik, D. Ho","doi":"10.1145/99633.99653","DOIUrl":null,"url":null,"abstract":"A new class of focusing reflectors was created by modeling the conformational transitions between a wound spiral focusing surface and its planar, non-focusing, unwound spiral state. Two solutions to the problem were found; one by modeling the process of unwinding the focusing spiral surface, the other by modeling the winding of the planar spiral surface. Both the mathematical derivations and the resulting equations relating the two states of the spiral surface proved markedly different for the two approaches. Implementation of each solution was accomplished by specifying the locations of marker points and tracking them through the conformational transitions. Although the mathematics and the algorithms employed are completely different between the two solutions, both result in identical sets of marker points for a given spiral. However, the solution based on the winding conformational transition is completely general, while the solution based on unwinding is limited to a narrow set of focusing geometries.","PeriodicalId":399502,"journal":{"name":"1990 Eastern Multiconference. Record of Proceedings. The 23rd Annual Simulation Symposium","volume":"25 1","pages":"0"},"PeriodicalIF":0.0000,"publicationDate":"1990-04-03","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"2","resultStr":"{\"title\":\"Numerical Modeling Of The Conformational Transition Of A Spiral Focusing Surface\",\"authors\":\"R. Steenblik, D. Ho\",\"doi\":\"10.1145/99633.99653\",\"DOIUrl\":null,\"url\":null,\"abstract\":\"A new class of focusing reflectors was created by modeling the conformational transitions between a wound spiral focusing surface and its planar, non-focusing, unwound spiral state. Two solutions to the problem were found; one by modeling the process of unwinding the focusing spiral surface, the other by modeling the winding of the planar spiral surface. Both the mathematical derivations and the resulting equations relating the two states of the spiral surface proved markedly different for the two approaches. Implementation of each solution was accomplished by specifying the locations of marker points and tracking them through the conformational transitions. Although the mathematics and the algorithms employed are completely different between the two solutions, both result in identical sets of marker points for a given spiral. However, the solution based on the winding conformational transition is completely general, while the solution based on unwinding is limited to a narrow set of focusing geometries.\",\"PeriodicalId\":399502,\"journal\":{\"name\":\"1990 Eastern Multiconference. Record of Proceedings. The 23rd Annual Simulation Symposium\",\"volume\":\"25 1\",\"pages\":\"0\"},\"PeriodicalIF\":0.0000,\"publicationDate\":\"1990-04-03\",\"publicationTypes\":\"Journal Article\",\"fieldsOfStudy\":null,\"isOpenAccess\":false,\"openAccessPdf\":\"\",\"citationCount\":\"2\",\"resultStr\":null,\"platform\":\"Semanticscholar\",\"paperid\":null,\"PeriodicalName\":\"1990 Eastern Multiconference. Record of Proceedings. The 23rd Annual Simulation Symposium\",\"FirstCategoryId\":\"1085\",\"ListUrlMain\":\"https://doi.org/10.1145/99633.99653\",\"RegionNum\":0,\"RegionCategory\":null,\"ArticlePicture\":[],\"TitleCN\":null,\"AbstractTextCN\":null,\"PMCID\":null,\"EPubDate\":\"\",\"PubModel\":\"\",\"JCR\":\"\",\"JCRName\":\"\",\"Score\":null,\"Total\":0}","platform":"Semanticscholar","paperid":null,"PeriodicalName":"1990 Eastern Multiconference. Record of Proceedings. The 23rd Annual Simulation Symposium","FirstCategoryId":"1085","ListUrlMain":"https://doi.org/10.1145/99633.99653","RegionNum":0,"RegionCategory":null,"ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"","JCRName":"","Score":null,"Total":0}
Numerical Modeling Of The Conformational Transition Of A Spiral Focusing Surface
A new class of focusing reflectors was created by modeling the conformational transitions between a wound spiral focusing surface and its planar, non-focusing, unwound spiral state. Two solutions to the problem were found; one by modeling the process of unwinding the focusing spiral surface, the other by modeling the winding of the planar spiral surface. Both the mathematical derivations and the resulting equations relating the two states of the spiral surface proved markedly different for the two approaches. Implementation of each solution was accomplished by specifying the locations of marker points and tracking them through the conformational transitions. Although the mathematics and the algorithms employed are completely different between the two solutions, both result in identical sets of marker points for a given spiral. However, the solution based on the winding conformational transition is completely general, while the solution based on unwinding is limited to a narrow set of focusing geometries.