Electromagnetic scattering from 3-D curved dielectric bodies using time-domain integral equations

A boundary integral equation (BIE) approach is developed to calculate transient scattering from dielectric bodies. The treatment is directly in terms of the E and H fields rather than magnetic and electric currents. It employs curvilinear (quadratic) modeling, which allows accurate representation of arbitrarily shaped curved bodies. The treatment is isoparametric with the same quadratic representation of the spatial field variation and with the temporal variation modeled by similar quadratic elements. Integration employs high-order Gaussian quadrature with special treatment of the singular and hypersingular integrals that arise. The treatment is implicit, requiring the solution of a sparse matrix equation at each timestep. This adds only trivially to the cost at each timestep and, by freeing the timestep from the constraint that it be smaller than the smallest nodal spacing, can greatly reduce the number of timesteps that must be employed. Additionally, it produces stable results without resort to the averaging processes proposed elsewhere. Example calculations of scattering from a sphere, a cube, and an almond are presented and compared with earlier published transient results and with results from a frequency domain treatment. Good agreement and improved accuracy is found.

[1]  M. Bluck Integral equation methods for transient wave propagation , 1993 .

[2]  M. Bluck,et al.  Time-domain BIE analysis of large three-dimensional electromagnetic scattering problems , 1997 .

[4]  M. J. Schuh,et al.  EM programmer's notebook-benchmark plate radar targets for the validation of computational electroma , 1992 .

[5]  J. Watson,et al.  Effective numerical treatment of boundary integral equations: A formulation for three‐dimensional elastostatics , 1976 .

[6]  M. D. Pocock,et al.  An accurate method for the calculation of singular integrals arising in time-domain integral equation analysis of electromagnetic scattering , 1997 .

[7]  Roger F. Harrington,et al.  Field computation by moment methods , 1968 .

[8]  H. Mieras,et al.  Space-time integral equation approach to dielectric targets , 1982 .

[9]  E. K. Miller,et al.  A selective survey of computational electromagnetics , 1988 .

[10]  Simon P. Walker,et al.  ANALYSIS OF THREE-DIMENSIONAL TRANSIENT ACOUSTIC WAVE PROPAGATION USING THE BOUNDARY INTEGRAL EQUATION METHOD , 1996 .

[11]  M. D. Pocock,et al.  Radar Cross Section Prediction Using Boundary Integral Equation Methods with Isoparametric Quadratic Surface Modeling and Iterative Solvers , 1996 .

[12]  D. Wilton,et al.  Electromagnetic scattering by surfaces of arbitrary shape , 1980 .

[13]  Tapan K. Sarkar,et al.  Transient scattering from three-dimensional arbitrarily shaped dielectric bodies , 1994 .

[14]  Andrew J. Poggio,et al.  CHAPTER 4 – Integral Equation Solutions of Three-dimensional Scattering Problems , 1973 .

[15]  S. Walker,et al.  Parallel computation of integral equation methods for three‐dimensional transient wave propagation , 1995 .

[16]  E. Marx,et al.  Integral equation for scattering by a dielectric , 1984 .

[17]  B. P. Rynne,et al.  Time Domain Scattering from Arbitrary Surfaces Using the Electric Field Integral Equation , 1991 .

[18]  D. Wilton,et al.  Transient scattering by conducting surfaces of arbitrary shape , 1991 .

[19]  A. C. Woo,et al.  Benchmark radar targets for the validation of computational electromagnetics programs , 1993 .