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請用此 Handle URI 來引用此文件: http://scholars.ntou.edu.tw/handle/123456789/24547
DC 欄位值語言
dc.contributor.authorChen, Jeng-Tzongen_US
dc.contributor.authorKao, Jeng-Hongen_US
dc.contributor.authorKao, Shing-Kaien_US
dc.contributor.authorWu, Ting-Annen_US
dc.date.accessioned2024-03-04T08:53:12Z-
dc.date.available2024-03-04T08:53:12Z-
dc.date.issued2023-10-01-
dc.identifier.issn0955-7997-
dc.identifier.urihttp://scholars.ntou.edu.tw/handle/123456789/24547-
dc.description.abstractFor a long time, direct and indirect BEM/BIEMs were always unified and seemed equivalent in real implementation for ensuring the solution. Regarding the solution space and the numerical aspects in linear algebra, it is interesting to find that they are not fully equivalent. To demonstrate this finding, antiplane shear problems containing the elliptical rigid inclusion and hole as well as rigid-line inclusion and line crack were given to demonstrate the non-equivalence between the direct and indirect BEM/BIEMs. It is interesting to find that nonunique boundary densities may yield the unique field solution in both analytical derivation and numerical implementation. The mechanism was analytically studied and numerically performed by using the degenerate kernel and the singular value decomposition technique, respectively. Besides, the Fredholm alternative theorem was employed to examine the solvability condition in both the indirect boundary integral equation method and indirect boundary element method. For continuous system and discrete system, we can explain why the boundary density does not match the exact solution but the field solution is always acceptable when setting xi 0 = 0 in the beginning of the derivation of BIE. Two approaches, direct and indirect BEM/BIEMs, show the non-equivalence of solution in case of degenerate boundary and degenerate scale.en_US
dc.language.isoEnglishen_US
dc.publisherELSEVIER SCI LTDen_US
dc.relation.ispartofENGINEERING ANALYSIS WITH BOUNDARY ELEMENTSen_US
dc.subjectAntiplane shearen_US
dc.subjectLine cracken_US
dc.subjectRigid -line inclusionen_US
dc.subjectSingle layer potentialen_US
dc.subjectDouble layer potentialen_US
dc.subjectBEM/BIEMen_US
dc.titleAre the direct and indirect BEM/BIEMs equivalent?en_US
dc.typejournal articleen_US
dc.identifier.doi10.1016/j.enganabound.2023.08.026-
dc.identifier.isiWOS:001087175800001-
dc.relation.journalvolume157en_US
dc.relation.pages441-461en_US
dc.identifier.eissn1873-197X-
item.openairecristypehttp://purl.org/coar/resource_type/c_6501-
item.cerifentitytypePublications-
item.languageiso639-1English-
item.fulltextno fulltext-
item.grantfulltextnone-
item.openairetypejournal article-
crisitem.author.deptCollege of Engineering-
crisitem.author.deptDepartment of Harbor and River Engineering-
crisitem.author.deptNational Taiwan Ocean University,NTOU-
crisitem.author.deptCenter of Excellence for Ocean Engineering-
crisitem.author.deptBasic Research-
crisitem.author.deptNational Taiwan Ocean University,NTOU-
crisitem.author.deptCollege of Engineering-
crisitem.author.deptDepartment of Harbor and River Engineering-
crisitem.author.orcid0000-0001-5653-5061-
crisitem.author.parentorgNational Taiwan Ocean University,NTOU-
crisitem.author.parentorgCollege of Engineering-
crisitem.author.parentorgNational Taiwan Ocean University,NTOU-
crisitem.author.parentorgCenter of Excellence for Ocean Engineering-
crisitem.author.parentorgNational Taiwan Ocean University,NTOU-
crisitem.author.parentorgCollege of Engineering-
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