Computer Methods in Applied Mechanics and Engineering
Computer Methods in Applied Mechanics and Engineering - Special edition on the 20th Anniversary
The characteristic streamline diffusion method for convection-diffusion problems
Computer Methods in Applied Mechanics and Engineering
Computer Methods in Applied Mechanics and Engineering
A new approach to algorithms for convection problems which are based on exact transport + projection
Computer Methods in Applied Mechanics and Engineering
Solving ordinary differential equations I (2nd revised. ed.): nonstiff problems
Solving ordinary differential equations I (2nd revised. ed.): nonstiff problems
Convergence Analysis for a Class of High-Order Semi-Lagrangian Advection Schemes
SIAM Journal on Numerical Analysis
The Lagrange-Galerkin spectral element method on unstructured quadrilateral grids
Journal of Computational Physics
A semi-Lagrangian high-order method for Navier-Stokes equations
Journal of Computational Physics
Finite Element Method for Elliptic Problems
Finite Element Method for Elliptic Problems
A Semi-Lagrangian Method for Turbulence Simulations Using Mixed Spectral Discretizations
Journal of Scientific Computing
Journal of Computational and Applied Mathematics
Strong and Auxiliary Forms of the Semi-Lagrangian Method for Incompressible Flows
Journal of Scientific Computing
Galerkin Finite Element Methods for Parabolic Problems (Springer Series in Computational Mathematics)
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We present in this paper an analysis of a semi-Lagrangian second order Backward Difference Formula combined with hp-finite element method to calculate the numerical solution of convection diffusion equations in 驴2. Using mesh dependent norms, we prove that the a priori error estimate has two components: one corresponds to the approximation of the exact solution along the characteristic curves, which is $O(\Delta t^{2}+h^{m+1}(1+\frac{\mathopen{|}\log h|}{\Delta t}))$ ; and the second, which is $O(\Delta t^{p}+\| \vec{u}-\vec{u}_{h}\|_{L^{\infty}})$ , represents the error committed in the calculation of the characteristic curves. Here, m is the degree of the polynomials in the finite element space, $\vec{u}$ is the velocity vector, $\vec{u}_{h}$ is the finite element approximation of $\vec{u}$ and p denotes the order of the method employed to calculate the characteristics curves. Numerical examples support the validity of our estimates.