𝔖 Bobbio Scriptorium
✦   LIBER   ✦

High-Order Compact-Difference Schemes for Time-Dependent Maxwell Equations

✍ Scribed by J.S Shang


Publisher
Elsevier Science
Year
1999
Tongue
English
Weight
228 KB
Volume
153
Category
Article
ISSN
0021-9991

No coin nor oath required. For personal study only.

✦ Synopsis


Two high-order compact-difference schemes have been developed for solving three-dimensional, time-dependent Maxwell equations. Spurious high-frequency oscillatory components of the numerical solution, which are considered to be among the principal sources of time instability, are effectively suppressed by a spatial filter. The present numerical schemes are validated by calculations of three-dimensional transient electromagnetic waves within a waveguide, an oscillating electric dipole, and the radar cross section of perfectly electrical conducting sphere.


πŸ“œ SIMILAR VOLUMES


A new parallelization strategy for solvi
✍ Eugene Kashdan; Barak Galanti πŸ“‚ Article πŸ“… 2006 πŸ› John Wiley and Sons 🌐 English βš– 332 KB

With progress in computer technology there has been renewed interest in a time-dependent approach to solving Maxwell equations. The commonly used Yee algorithm (an explicit central difference scheme for approximation of spatial derivatives coupled with the Leapfrog scheme for approximation of tempor

High-Order Time-Stable Numerical Boundar
✍ J.F. Nystrom πŸ“‚ Article πŸ“… 2002 πŸ› Elsevier Science 🌐 English βš– 196 KB

High-order time-stable boundary operators for perfectly electrically conducting (PEC) surfaces are presented for a 3 Γ— 3 hyperbolic system representing electromagnetic fields T E to z. First a set of operators satisfying the summation-by-parts property are presented for a 2 Γ— 2 hyperbolic system rep

Higher order explicit time integration s
✍ Holger Spachmann; Rolf Schuhmann; Thomas Weiland πŸ“‚ Article πŸ“… 2002 πŸ› John Wiley and Sons 🌐 English βš– 284 KB

## Abstract The finite integration technique (FIT) is an efficient and universal method for solving a wide range of problems in computational electrodynamics. The conventional formulation in time‐domain (FITD) has a second‐order accuracy with respect to spatial and temporal discretization and is co