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Partial Differential Equations - Modelling and ... - ResearchGate

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Comparison of Two Explicit Time Domain<br />

Unstructured Mesh Algorithms<br />

for Computational Electromagnetics<br />

Igor Sazonov, Oubay Hassan, Ken Morgan, <strong>and</strong> Nigel P. Weatherill<br />

Civil <strong>and</strong> Computational Engineering Centre, School of Engineering, University of<br />

Wales, Swansea SA2 8PP, Wales, UK<br />

{i.sazonov,O.Hassan,K.Morgan,N.P.Weatherill}@swansea.ac.uk<br />

Summary. An explicit finite element time domain method <strong>and</strong> a co-volume approach,<br />

based upon a generalization of the well-known finite difference time domain<br />

scheme of Yee to unstructured meshes, are employed for the solution of Maxwell’s<br />

curl equations in the time domain. A stitching method is employed to produce<br />

meshes that are suitable for use with a co-volume algorithm. Examples, involving<br />

EM wave propagation <strong>and</strong> scattering, are included <strong>and</strong> the numerical performance<br />

of the two techniques is compared.<br />

Key words: computationalelectromagnetics,Delaunaytriangulation,Voronoï<br />

tessellation,co-volumemeshgeneration,explicitschemes,finiteelementmethod,<br />

co-volume method, EM wave propagation <strong>and</strong> scattering<br />

1 Introduction<br />

Computational methods are widely employed for the solution of Maxwell’s<br />

equations in a variety of different application areas that fall within the general<br />

field of electromagnetics. For practical applications, the requirement of modelling<br />

complex geometries means that unstructured mesh methods are particularly<br />

attractive, as fully automatic unstructured mesh generation procedures<br />

are now widely available [Geo91, WH94, PPM99]. Following this philosophy<br />

requires the identification of a suitable unstructured mesh-based solution algorithm<br />

<strong>and</strong> several low-order time domain procedures have been proposed<br />

[MSH91, PLD92, CFS93, DL97, MWH + 99]. These methods are readily implemented,<br />

but may require a significant computational resource to undertake<br />

accurate simulations involving wave propagation over a large number of<br />

wavelengths [DBB99]. On the other h<strong>and</strong>, the Yee scheme [Yee66] is a covolume<br />

solution technique, on a structured Cartesian mesh, that exhibits a<br />

high degree of computationally efficiency, in terms of both CPU <strong>and</strong> memory<br />

requirements.

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