2005
DOI: 10.1051/m2an:2005009
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A posteriorierror estimates for a nonconforming finite element discretization of the heat equation

Abstract: Abstract. The paper presents an a posteriori error estimator for a (piecewise linear) nonconforming finite element approximation of the heat equation in R d , d = 2 or 3, using backward Euler's scheme. For this discretization, we derive a residual indicator, which use a spatial residual indicator based on the jumps of normal and tangential derivatives of the nonconforming approximation and a time residual indicator based on the jump of broken gradients at each time step. Lower and upper bounds form the main re… Show more

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Cited by 18 publications
(37 citation statements)
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“…In this paper, first, we extend the results from [15] applying the approach from [12] to the high-order discontinuous Galerkin discretization. Then, we derive a lower error bound using a technique based on testing with suitable cut-off functions.…”
Section: Introductionmentioning
confidence: 95%
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“…In this paper, first, we extend the results from [15] applying the approach from [12] to the high-order discontinuous Galerkin discretization. Then, we derive a lower error bound using a technique based on testing with suitable cut-off functions.…”
Section: Introductionmentioning
confidence: 95%
“…See, e.g., [12] on how to handle the right-hand side oscillation. The solution of (3.1) is called the semi-discrete solution.…”
Section: Problem Definitionmentioning
confidence: 99%
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“…Some other results on a posteriori error estimates for parabolic problems in a conforming setting can also be found in [24] using the so-called functional approach where a flux reconstruction is also considered, but without enforcing any local condition; furthermore, only error upper bounds are derived. Finally, we observe that contrary to conforming finite elements, a posteriori energy-norm error estimates for the heat equation discretized by nonconforming methods are less explored; we mention, in particular, [10] for mixed finite elements, [23] for nonconforming finite elements, [17] for discontinuous Galerkin methods, and [3] for finite volume schemes. This paper is organized as follows.…”
mentioning
confidence: 99%