Loading…
A Stabilized Time-Domain Combined Field Integral Equation Using the Quasi-Helmholtz Projectors
This article introduces a time-domain combined field integral equation (TD-CFIE) for electromagnetic scattering by a perfect electric conductor (PEC). The new equation is obtained by leveraging the quasi-Helmholtz projectors, which separate both the unknown and the source fields into solenoidal and...
Saved in:
Published in: | IEEE transactions on antennas and propagation 2024-07, Vol.72 (7), p.5852-5864 |
---|---|
Main Authors: | , , , |
Format: | Article |
Language: | English |
Subjects: | |
Citations: | Items that this one cites |
Online Access: | Get full text |
Tags: |
Add Tag
No Tags, Be the first to tag this record!
|
Summary: | This article introduces a time-domain combined field integral equation (TD-CFIE) for electromagnetic scattering by a perfect electric conductor (PEC). The new equation is obtained by leveraging the quasi-Helmholtz projectors, which separate both the unknown and the source fields into solenoidal and irrotational components. These two components are then appropriately rescaled to cure the solution from a loss of accuracy occurring when the time step is large. Yukawa-type integral operators of a purely imaginary wavenumber are also used as a Calderón preconditioner to eliminate the ill-conditioning of matrix systems. The stabilized time-domain electric and magnetic field integral equations are linearly combined in a Calderón-like fashion, then temporally discretized using an appropriate pair of trial functions, resulting in a marching-on-in-time (MOT) linear system. The novel formulation is immune to spurious resonances, dense discretization breakdown, large-time step breakdown, and dc instabilities stemming from non-trivial kernels. Numerical results for both simply-connected and multiply-connected scatterers corroborate the theoretical analysis. |
---|---|
ISSN: | 0018-926X 1558-2221 |
DOI: | 10.1109/TAP.2024.3410709 |