Spatial error estimates for a finite element viscosity-splitting scheme for the Navier-Stokes equations

In this paper, we obtain optimal first order error estimates for a fully discrete fractional-step scheme applied to the Navier-Stokes equations. This scheme uses decomposition of the viscosity in time and finite elements (FE) in space. In [15], optimal first order error estimates (for velocity and p...

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Detalles Bibliográficos
Autores: Guillén González, Francisco Manuel, Redondo Neble, María Victoria
Tipo de recurso: artículo
Estado:Versión publicada
Fecha de publicación:2013
País:España
Institución:Universidad de Sevilla (US)
Repositorio:idUS. Depósito de Investigación de la Universidad de Sevilla
OAI Identifier:oai:dnet:idus________::bfdc8ba0a086c55a8dee5c9bd539c7aa
Acceso en línea:https://hdl.handle.net/11441/187141
Access Level:acceso abierto
Palabra clave:Navier-Stokes Equations
Splitting in time schemes
Fully discrete schemes
Error estimates
Mixed formulation
Stable finite elements
Descripción
Sumario:In this paper, we obtain optimal first order error estimates for a fully discrete fractional-step scheme applied to the Navier-Stokes equations. This scheme uses decomposition of the viscosity in time and finite elements (FE) in space. In [15], optimal first order error estimates (for velocity and pressure) for the corresponding time-discrete scheme were obtained, using in particular H2XH1 estimates for the approximations of the velocity and pressure. Now, we use this time-discrete scheme as an auxiliary problem to study a fully discrete finite element scheme, obtaining optimal first order approximation for velocity and pressure with respect to the max-norm in time and the H1XL2-norm in space. The proof of these error estimates are based on three main points: a) provide some new estimates for the time-discrete scheme (not proved in [15]) which must be now used, b) give a discrete version of the H2XH1 estimates in FE spaces, using stability in the W1,6XL6-norm of the FE Stokes projector, and c) the use of a weight function vanishing at initial time will let to hold the error estimates without imposing global compatibility for the exact solution.