NANANov 25, 2014

Notes on error estimates for the standard Galerkin-finite element method for the Shallow Water equations

arXiv:1403.56992 citations
Originality Synthesis-oriented
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This work provides rigorous error bounds for a well-studied numerical method on a specific PDE system, but the results are incremental and limited to 1D smooth solutions.

The authors prove optimal-order $L^{2}$-error estimates for standard Galerkin-finite element methods applied to the shallow water equations in 1D, achieving $O(h^{2})$ for piecewise linear functions on uniform meshes. They also derive temporal error estimates for explicit Runge-Kutta methods and justify the symmetric variant of the system.

We consider a simple initial-boundary-value problem for the shallow water equations in one space dimension, and also the analogous problem for a symmetric variant of the system. Assuming smoothness of solutions, we discretize these problems in space using standard Galerkin-finite element methods and prove $L^{2}$-error estimates for the semidiscrete problems for quasiuniform and uniform meshes. In particular we show that in the case of spatial discretizations with piecewise linear continuous functions on a uniform mesh, suitable compatibility conditions at the boundary and superaccuracy properties of the $L^{2}$ projection on the finite element subspaces lead to an optimal-order $O(h^{2})$ $L^{2}$-error estimate. We also examine temporal discretizations of the semidiscrete problems by three explicit Runge-Kutta methods (the Euler, improved Euler, and the Shu-Osher scheme) and prove $L^{2}$-error estimates, which are of optimal order in the temporal variable, under appropriate stability conditions. In a final section of remarks we prove optimal-order $L^{2}$-error estimates for smooth spline spatial discretizations of the periodic initial-value problem for the systems. We also prove that small-amplitude, appropriately transformed solutions of the symmetric system are close to the corresponding solutions of the usual system while they are both smooth, thus providing a justification of the symmetric system.

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