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請用此 Handle URI 來引用此文件: http://scholars.ntou.edu.tw/handle/123456789/2378
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dc.contributor.authorJeng-Tzong Chenen_US
dc.contributor.authorHuang, W. S.en_US
dc.contributor.authorFan, Y.en_US
dc.contributor.authorKao, S. K.en_US
dc.date.accessioned2020-11-17T03:22:34Z-
dc.date.available2020-11-17T03:22:34Z-
dc.date.issued2015-10-
dc.identifier.issn1811-8216-
dc.identifier.urihttp://scholars.ntou.edu.tw/handle/123456789/2378-
dc.description.abstractThe boundary element method (BEM) is easier than the finite element method (FEM) on the viewpoint of the discretization of one dimension reduction rather than the domain discretization of finite element method. The disadvantage of BEM is the rank deficiency in the influence matrix, e.g., degenerate boundary, degenerate scale, spurious eigenvalues and fictitious frequencies, which do not occur in the FEM. The conventional BEM can not be straightforward applied to solve a problem which contains a degenerate boundary without decomposing the domain to multi-regions. A hypersingular integral equation is used to ensure a unique solution for the problem containing a degenerate boundary. By combining the singular and hypersingular equations, it’s termed the dual BEM due to its dual frame. Following the successful experience on the retrieval of information using the singular value decomposition (SVD) updating term and updating document, this technique is also used to extract out the degenerate-boundary information and the rigid-body information in the dual BEM. It is interesting to find that true information due to a rigid-body mode in physics is found in the right singular vector with respect to the corresponding zero singular value while the degenerate-boundary mode (geometry degeneracy) in mathematics is imbedded in the left singular vector with respect to the corresponding zero singular value. The role of the common right and left singular vectors of SVD for the four influence matrices in the dual BEM is also discussed in this paper. Two examples, a potential flow problem across a cutoff wall and a cracked bar under torsion were demonstrated to see the mathematical SVD structure of four influence matrices in the dual BEM.en_US
dc.language.isoen_USen_US
dc.publisherOXFORD ACADEMICen_US
dc.relation.ispartofJournal of Mechanicsen_US
dc.subjectDegenerate boundaryen_US
dc.subjectDual BEMen_US
dc.subjectSVD updating techniqueen_US
dc.titleRevisit of the Dual Bem using SVD Updating Techniqueen_US
dc.typejournal articleen_US
dc.identifier.doi10.1017/jmech.2015.12-
dc.relation.journalvolume31en_US
dc.relation.journalissue5en_US
dc.relation.pages505-514en_US
item.fulltextno fulltext-
item.openairecristypehttp://purl.org/coar/resource_type/c_6501-
item.cerifentitytypePublications-
item.grantfulltextnone-
item.languageiso639-1en_US-
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.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-
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