# A structure-preserving split finite element discretization of the split 1D wave equations

## TL;DR

This paper presents a novel structure-preserving finite element discretization framework for split 1D wave equations, enabling stable and accurate numerical schemes that respect the equations' geometric properties.

## Contribution

It introduces a new discretization approach that preserves geometric structure and explores different Galerkin projection schemes, including a novel unstable scheme and stable mixed schemes.

## Key findings

- The scheme with twice GP1 is unstable and mimics P1-P1 behavior.
- Mixed GP1 and GP0 schemes are stable, resembling P1-P0 schemes.
- All schemes exhibit second-order convergence for key quantities.

## Abstract

We introduce a new finite element (FE) discretization framework applicable for covariant split equations. The introduction of additional differential forms (DF) that form pairs with the original ones permits the splitting of the equations into topological momentum and continuity equations and metric-dependent closure equations that apply the Hodge-star operator. Our discretization framework conserves this geometrical structure and provides for all DFs proper FE spaces such that the differential operators hold in strong form. We introduce lowest possible order discretizations of the split 1D wave equations, in which the discrete momentum and continuity equations follow by trivial projections onto piecewise constant FE spaces, omitting partial integrations. Approximating the Hodge-star by nontrivial Galerkin projections (GP), the two discrete metric equations follow by projections onto either the piecewise constant (GP0) or piecewise linear (GP1) space. Our framework gives us three schemes with significantly different behavior. The split scheme using twice GP1 is unstable and shares the dispersion relation with the P1-P1 FE scheme that approximates both variables by piecewise linear spaces (P1). The split schemes that apply a mixture of GP1 and GP0 share the dispersion relation with the stable P1-P0 FE scheme that applies piecewise linear and piecewise constant (P0) spaces. However, the split schemes exhibit second order convergence for both quantities of interest. For the split scheme applying twice GP0, we are not aware of a corresponding standard formulation to compare with. Though it does not provide a satisfactory approximation of the dispersion relation as short waves are propagated much too fast, the discovery of the new scheme illustrates the potential of our discretization framework as a toolbox to study and find FE schemes by new combinations of FE spaces.