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Please use this identifier to cite or link to this item: https://digital.lib.ueh.edu.vn/handle/UEH/62193
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dc.contributor.authorNgoc L.T.P.-
dc.contributor.otherTruong L.X.-
dc.contributor.otherLong N.T.-
dc.date.accessioned2021-08-30T04:58:11Z-
dc.date.available2021-08-30T04:58:11Z-
dc.date.issued2010-
dc.identifier.issn0420-1213-
dc.identifier.urihttp://digital.lib.ueh.edu.vn/handle/UEH/62193-
dc.description.abstractIn this paper we consider the following nonlinear wave equation (1) {utt-α/αx(μ(x,t,∥ux(t)∥2)ux) = f(x,t,u), 0 < x < 1,0 < t < T, u(0,t) = u(1,t) = 0, u(x,0) = ũ0(x),ut(x,0) = ũ1(x), where n, μ, f, ũ0,ũ1 are given functions satisfying conditions specified later. In Eq. (l)1, the nonlinear term μ,(x,t, ∥ux∥2) depends on the integral ∥ux(t) ∥2 = ∫10ux(x,i)|2 dx. In this paper we associate with equation (l)1 a recurrent sequence {um} defined by (2) α2um/αt2 - α/ αx (μ(x,t,∥umx(t)∥2umx) = N-1Σi=01/zi αi∫/ αui (x,t, um-1) um - um-1)i,0 < x < 1, 0 < t < T, with um satisfying (1)2,3. The first term uo is chosen as uo ≡ 0. If ∫ ∈ CN([0,1] × ℝ+ × ℝ), we prove that the sequence {um} converges at a rate of order N to a unique weak solution of problem (1).en
dc.formatPortable Document Format (PDF)-
dc.language.isoeng-
dc.publisherWalter de Gruyter GmbH-
dc.relation.ispartofDemonstratio Mathematica-
dc.relation.ispartofseriesVol. XLIII, No. 3-
dc.rightsWarsaw University-
dc.subjectFaedo-Galerkin methoden
dc.subjectNonlinear Kirchhoff-Carrier wave equationen
dc.subjectThe convergence of order Nen
dc.titleHigh-order iterative methods for a nonlinear kirchhoff wave equationen
dc.typeJournal Articleen
dc.identifier.doihttps://doi.org/10.1515/dema-2010-0310-
dc.format.firstpage605-
dc.format.lastpage634-
ueh.JournalRankingScopus-
item.languageiso639-1en-
item.openairecristypehttp://purl.org/coar/resource_type/c_18cf-
item.cerifentitytypePublications-
item.openairetypeJournal Article-
item.grantfulltextnone-
item.fulltextOnly abstracts-
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