Solving the elastostatic problem by the analog equation method

Katsikadelis, JT; Kandilas, CB

dc.contributor.author	Katsikadelis, JT	en
dc.contributor.author	Kandilas, CB	en
dc.date.accessioned	2014-03-01T02:48:17Z
dc.date.available	2014-03-01T02:48:17Z
dc.date.issued	1994	en
dc.identifier.uri	https://dspace.lib.ntua.gr/xmlui/handle/123456789/33693
dc.relation.uri	http://www.scopus.com/inward/record.url?eid=2-s2.0-0028739436&partnerID=40&md5=040430d697004ebf5e7911408c038060	en
dc.subject.other	Boundary element method	en
dc.subject.other	Boundary value problems	en
dc.subject.other	Finite difference method	en
dc.subject.other	Finite element method	en
dc.subject.other	Mathematical models	en
dc.subject.other	Mathematical operators	en
dc.subject.other	Partial differential equations	en
dc.subject.other	Strain	en
dc.subject.other	Stresses	en
dc.subject.other	Analog equation method	en
dc.subject.other	Navier equations	en
dc.subject.other	Poisson equation	en
dc.subject.other	Shear modulus	en
dc.subject.other	Numerical methods	en
dc.title	Solving the elastostatic problem by the analog equation method	en
heal.type	conferenceItem	en
heal.publicationDate	1994	en
heal.abstract	A novel BEM-based method, the Analog Equation Method (AEM) [1], is employed to solve the plane elastostatic problem described by the Navier Equations. The actual problem is converted to an equivalent one described by two uncoupled Poisson's Equations with fictitious source terms, under the same boundary conditions. The fictitious sources are established using the indirect BEM method for the potential problem. The method incorporates features and advantages of FDM, FEM and BEM. Numerical examples are presented, which illustrate the merits of the method as well as its efficiency and accuracy.	en
heal.publisher	Civil-Comp Limited, Edinburgh, United Kingdom	en
heal.journalName	International Conference on Computational Structures Technology - Proceedings	en
dc.identifier.spage	269	en
dc.identifier.epage	274	en