Abstract
The aim of this paper is to present a method for solving the time-domain three-dimensional Maxwell equations, which can be coupled with a particle solver. For this purpose, Maxwell's equations are reformulated as a constrained wave equation system, with Lagrange multipliers associated to the conditions ∇ · β - 0 and ∇ · E - ρ/ε 0. We approximate both the fields and the Lagrange multipliers with a finite element method using a Taylor Hood element.
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