Journal of Scientific Computing
Exact projections and the Lagrange-Galerkin method: a realistic alternative to quadrature
Journal of Computational Physics
Spline-characteristic method for simulation of convective turbulence
Journal of Computational Physics
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
SIAM Journal on Numerical Analysis
A semi-Lagrangian high-order method for Navier-Stokes equations
Journal of Computational Physics
Terascale spectral element dynamical core for atmospheric general circulation models
Proceedings of the 2001 ACM/IEEE conference on Supercomputing
SIAM Journal on Scientific Computing
A Semi-Lagrangian Method for Turbulence Simulations Using Mixed Spectral Discretizations
Journal of Scientific Computing
Nonlinear operator integration factor splitting for the shallow water equations
Applied Numerical Mathematics
Hybrid Eulerian-Lagrangian Semi-Implicit Time-Integrators
Computers & Mathematics with Applications
A regularized Lagrangian finite point method for the simulation of incompressible viscous flows
Journal of Computational Physics
Accurate interface-tracking for arbitrary Lagrangian-Eulerian schemes
Journal of Computational Physics
Nonlinear operator integration factor splitting for the shallow water equations
Applied Numerical Mathematics
An unconditionally stable rotational velocity-correction scheme for incompressible flows
Journal of Computational Physics
Journal of Computational Physics
Journal of Scientific Computing
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We present a review of the semi-Lagrangian method for advection---diffusion and incompressible Navier---Stokes equations discretized with high-order methods. In particular, we compare the strong form where the departure points are computed directly via backwards integration with the auxiliary form where an auxiliary advection equation is solved instead; the latter is also referred to as Operator Integration Factor Splitting (OIFS) scheme. For intermediate size of time steps the auxiliary form is preferrable but for large time steps only the strong form is stable.