A new family of mixed finite elements in IR3
Numerische Mathematik
On a finite-element method for solving the three-dimensional Maxwell equations
Journal of Computational Physics
A parallel time-domain Maxwell solver using upwind schemes and triangular meshes
IMPACT of Computing in Science and Engineering
Journal of Computational Physics
The origin of spurious solutions in computational electromagnetics
Journal of Computational Physics
Journal of Computational Physics
Convergence analysis of a covolume scheme for Maxwell's equations in three dimensions
Mathematics of Computation
A finite volume method for the approximation of diffusion operators on distorted meshes
Journal of Computational Physics
Journal of Computational Physics
Divergence correction techniques for Maxwell solvers based on a hyperbolic model
Journal of Computational Physics
A Finite-Volume Method for the Maxwell Equations in the Time Domain
SIAM Journal on Scientific Computing
Explicit Finite Element Methods for Symmetric Hyperbolic Equations
SIAM Journal on Numerical Analysis
SIAM Journal on Numerical Analysis
The Mortar Finite Element Method for 3D Maxwell Equations: First Results
SIAM Journal on Numerical Analysis
Nodal high-order methods on unstructured grids
Journal of Computational Physics
Locally divergence-free discontinuous Galerkin methods for the Maxwell equations
Journal of Computational Physics
A Discontinuous Galerkin Method for Linear Symmetric Hyperbolic Systems in Inhomogeneous Media
Journal of Scientific Computing
SIAM Journal on Numerical Analysis
SIAM Journal on Numerical Analysis
High-order nodal discontinuous Galerkin particle-in-cell method on unstructured grids
Journal of Computational Physics
SIAM Journal on Numerical Analysis
A finite volume method for approximating 3D diffusion operators on general meshes
Journal of Computational Physics
Hi-index | 31.45 |
A new finite volume method is presented for discretizing the two-dimensional Maxwell equations. This method may be seen as an extension of the covolume type methods to arbitrary, possibly non-conforming or even non-convex, n-sided polygonal meshes, thanks to an appropriate choice of degrees of freedom. An equivalent formulation of the scheme is given in terms of discrete differential operators obeying discrete duality principles. The main properties of the scheme are its energy conservation, its stability under a CFL-like condition, and the fact that it preserves Gauss' law and divergence free magnetic fields. Second-order convergence is demonstrated numerically on non-conforming and distorted meshes.