In this section, we test locally conformal PML technique via a three-dimensional scatterer, which is a conesphere whose halfcone angle is 45°, base radius is 1.6, and length is 1.6. The edge size is set to approximately /10. The thicknesses of the PML and the free-space regions are both /5. The mesh cross-section and the bistatic RCS pattern of the conesphere are plotted in Figures 6 and 7, respectively, assuming an axial (nose-on) plane-wave incidence. The mesh cross-section in Figure 7 is just a coarse mesh given for the purpose of visualization. The different gray-shades in the mesh correspond to the scatterer, free-space and PML regions, respectively.
CONCLUSIONSIn this article, we have introduced the locally conformal PML technique in terms of a complex coordinate transformation. The technique is very simple to implement an ordinary FEM software.We have investigated the accuracy of the technique via comparisons with the MoM and literature data. REFERENCES 1. J.P. Berenger, A perfectly matched layer for the absorption of electromagnetic waves,