2005
DOI: 10.1007/s11202-005-0030-1
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On error estimates in the Galerkin method for hyperbolic equations

Abstract: We consider the Cauchy problem in a Hilbert space for a second-order abstract quasilinear hyperbolic equation with variable operator coefficients and nonsmooth (but Bochner integrable) free term. For this problem, we establish an a priori energy error estimate for the semidiscrete Galerkin method with an arbitrary choice of projection subspaces. Also, we establish some results on existence and uniqueness of an exact weak solution. We give an explicit error estimate for the finite element method and the Galerki… Show more

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Cited by 5 publications
(8 citation statements)
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“…The proof of this theorem is carried out mainly by the available methods; therefore, here we only sketch the main steps. The assertion on existence of a unique weak solution to (0.1), (0.2) is a consequence of the corresponding result of [1] (which is proven under somewhat more general conditions on B as compared with those of this article). The proof of unique strong solvability of (1.7), (1.8) is carried out by the scheme of [11, Chapter 1, Sections 1.4-1.6] combined with some technical elements of [1].…”
Section: The Initial Conditions Projection-difference Scheme and Ausupporting
confidence: 53%
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“…The proof of this theorem is carried out mainly by the available methods; therefore, here we only sketch the main steps. The assertion on existence of a unique weak solution to (0.1), (0.2) is a consequence of the corresponding result of [1] (which is proven under somewhat more general conditions on B as compared with those of this article). The proof of unique strong solvability of (1.7), (1.8) is carried out by the scheme of [11, Chapter 1, Sections 1.4-1.6] combined with some technical elements of [1].…”
Section: The Initial Conditions Projection-difference Scheme and Ausupporting
confidence: 53%
“…The assertion on existence of a unique weak solution to (0.1), (0.2) is a consequence of the corresponding result of [1] (which is proven under somewhat more general conditions on B as compared with those of this article). The proof of unique strong solvability of (1.7), (1.8) is carried out by the scheme of [11, Chapter 1, Sections 1.4-1.6] combined with some technical elements of [1]. For construction of a strong solution to (1.7), (1.8), we use semidiscrete Galerkin approximations and establish a priori estimates of the form (1.11) and (1.12) for them; their proof relies upon the Bihari lemma [18, p. 189, Theorem 3] and the Gronwall lemma [19, p. 191], respectively.…”
Section: The Initial Conditions Projection-difference Scheme and Ausupporting
confidence: 53%
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