Issue |
ESAIM: M2AN
Volume 51, Number 5, September-October 2017
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Page(s) | 1663 - 1689 | |
DOI | https://doi.org/10.1051/m2an/2017032 | |
Published online | 20 October 2017 |
Numerical analysis of the Oseen-type Peterlin viscoelastic model by the stabilized Lagrange–Galerkin method. Part II: A linear scheme
1 Institute of Mathematics, University of Mainz, Mainz 55099, Germany
lukacova@uni-mainz.de; mizerova@uni-mainz.de
2 Faculty of Mathematics and Physics, Kanazawa University, Kanazawa 920-1192, Japan
notsu@se.kanazawa-u.ac.jp
3 Japan Science and Technology Agency (JST), PRESTO, Kawaguchi 332-0012, Japan
4 Department of Mathematics, Waseda University, 3-4-1, Ohkubo, Shinjuku, Tokyo 169-8555, Japan
tabata@waseda.jp
Received: 22 March 2016
Revised: 1 February 2017
Accepted: 19 June 2017
This is the second part of our error analysis of the stabilized Lagrange–Galerkin scheme applied to the Oseen-type Peterlin viscoelastic model. Our scheme is a combination of the method of characteristics and Brezzi–Pitkäranta’s stabilization method for the conforming linear elements, which leads to an efficient computation with a small number of degrees of freedom especially in three space dimensions. In this paper, Part II, we apply a semi-implicit time discretization which yields the linear scheme. We concentrate on the diffusive viscoelastic model, i.e. in the constitutive equation for time evolution of the conformation tensor a diffusive effect is included. Under mild stability conditions we obtain error estimates with the optimal convergence order for the velocity, pressure and conformation tensor in two and three space dimensions. The theoretical convergence order is confirmed by numerical experiments.
Mathematics Subject Classification: 65M12 / 65M25 / 65M60 / 76A10
Key words: Error estimates / Peterlin viscoelastic model / Lagrange–Galerkin method / Pressure-stabilization
© EDP Sciences, SMAI 2017
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