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6、^üV ³,þ‰Ñü«êŠ¦)•{^±é'`²·‚•{Œ15Ú(5.5.éˆaØÓ>.^‡,‰Ñ>.È©•§äNÑL§Úäk“L5ꊎ~.'…cµXJÅêHelmholtz•§,³nØ,Nystr¨om{,KressC†,>.È©•§,nŠ.IAbstractFromoriginalFiniteE
7、lementMethod(FEM)topresentpopularBoundaryEl-ementmethod(BEM),ithasbeenalongtimeforstudyingthenumericalsolutionofHelmholtzequation.Giventypesofellipticpartialdifferentialequations,whichcanbetransformedintoequivalentintegralequationtosolvebypotentialtheory,sincetheme
8、ritofintegralequationinnumericalsolution,whichmakespoten-tialtheorytosolvesuchboundaryvalueproblembecomesaclassicalnumericalmethod.Forthefollowingtypicalellipticpartialdifferentialequationsontheplanarboundary,suchasLaplaceequation,Helmholtzequation,basedontheprevio
9、uspeople’swork,professorRainerKressreformulatedthemasintegralequationsbypotentialtheory,inthefinalstep,whodirectlyusedweightquadratureformula(Nystr¨ommethod)approximatingthekernelofintegralequation,obtainingthenicenumericalresult,headoptsthemethodalmostinhisallpape
10、rsaboutthenumericalsolutionsofintegralequationandrecommendsthismethodjustasthesimplicityandoperabilityofthismethod.TherehasbeenalargeofpapersaboutthenumericalsolutionsofHelmholtzequationwithpositivewavenumberforvariousboundaryconditions,butalmostnopaperfocusingonH
11、elmholtzequationwithpureimaginarywavenumber,forthiscase,theauthorattemptstogivesystemstudyonthenumericalsolutionsofHelmholtzequationwithpureimaginarywav