Titlebook: Boundary and Interior Layers, Computational and Asymptotic Methods - BAIL 2014; Petr Knobloch Conference proceedings 2015 Springer Interna

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J. L. Heaton MA(Cantab) FInstPetmodel that includes general non-linear wall laws. We introduce Lagrange finite element spaces adapted to approximate the slip condition. The sub-grid effects are modeled by an eddy diffusion term that acts only on a range of small resolved scales. Moreover, high-order stabilization terms are conside

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G. G. Evans,V. M. Galvin,W. F. Waller31, 1998), to analyze the uniform convergence of some numerical methods which have been used to solve successfully two dimensional parabolic singularly perturbed problems of convection-diffusion type. For getting this, we split the discretization methods in a two stage procedure where, firstly, we s

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reflection

TIA742

Luc Reychler’s Comprehensive Bibliographyged Navier-Stokes equations are closed by the SST eddy-viscosity turbulence model or by explicit algebraic Reynolds stress turbulence model (EARSM) with the .-. transition model of Lodefier and Dick. The mathematical model is solved by implicit AUSM-type finite volume method. The implementation of t

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Armando Malheiro da Silva,Fernanda Ribeiropressible Navier-Stokes equations. We consider inf-sup stable finite element methods with grad-div stabilization and symmetric stabilization of local projection type. The approach is based on a proper scale separation and only the small unresolved scales are modeled. Error estimates for the spatiall

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Luciano Floridi’s Philosophy of Technology for computing the stabilization parameter . in the streamline upwind/Petrov–Galerkin (SUPG) method based on minimizing the value of a functional called error indicator. Particularly, we present results for conforming finite element spaces up to the order 5 with the parameter . from the piecewise di

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