๐”– Bobbio Scriptorium
โœฆ   LIBER   โœฆ

Corrective meshless particle formulations for time domain Maxwell's equations

โœ Scribed by G. Ala; E. Francomano; A. Tortorici; E. Toscano; F. Viola


Publisher
Elsevier Science
Year
2007
Tongue
English
Weight
298 KB
Volume
210
Category
Article
ISSN
0377-0427

No coin nor oath required. For personal study only.

โœฆ Synopsis


In this paper a meshless approximation of electromagnetic (EM) field functions and relative differential operators based on particle formulation is proposed. The idea is to obtain numerical solutions for EM problems by passing up the mesh generation usually required to compute derivatives, and by employing a set of particles arbitrarily placed in the problem domain. The meshless Smoothed Particle Hydrodynamics method has been reformulated for solving the time domain Maxwell's curl equations. The consistency of the discretized model is investigated and improvements in the approximation are obtained by modifying the numerical process. Corrective algorithms preserving meshless consistency are presented and successfully used. Test problems, dealing with even and uneven particles distribution, are simulated to validate the proposed methodology, also by introducing a comparison with analytical solution.


๐Ÿ“œ SIMILAR VOLUMES


Optimal symplectic integrators for numer
โœ Z. X. Huang; X. L. Wu; W. Sha; M. S. Chen ๐Ÿ“‚ Article ๐Ÿ“… 2007 ๐Ÿ› John Wiley and Sons ๐ŸŒ English โš– 177 KB

## Abstract Optimal symplectic integrators were proposed to improve the accuracy in numerical solution of timeโ€domain Maxwell's equations. The proposed symplectic scheme has almost the same stability and numerical dispersion as the mostly used fourthโ€order symplectic scheme, but acquires more effic

A novel high-order time-domain scheme fo
โœ Zhi-Xiang Huang; Wei Sha; Xian-Liang Wu; Ming-Sheng Chen ๐Ÿ“‚ Article ๐Ÿ“… 2006 ๐Ÿ› John Wiley and Sons ๐ŸŒ English โš– 84 KB

## Abstract A novel highโ€order timeโ€domain scheme with a fourโ€stage optimized symplectic integrator propagator is presented for 3D electromagnetic scattering problems. The scheme is nondissipative and does not require more storage than the classical finiteโ€difference timeโ€domain (FDTD) method. The

Efficient implementation issues of finit
โœ Joe Lovetri; George I. Costache ๐Ÿ“‚ Article ๐Ÿ“… 1993 ๐Ÿ› John Wiley and Sons ๐ŸŒ English โš– 956 KB

The computer implementation of time-domain finite difference methods for the solution of Maxwell's equations is considered. As the basis of this analysis, Maxwell's equations are expressed as a system of hyperbolic conservation laws. It is shown that, in this form, all the well-known differencing sc