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get fields on the sparse grid. For the non-near-field interactions, we further expand on a canonical grid of a horizontal surface so that the fast Fourier transform (FFT) can be applied. In the lower medium, non-near-field interactions were neglected because of lossy properties of the lower medium. The approach is denoted as PBTG-BMIAjCAG. The computational complexity and the memory requirements for the present algorithm are O(N log(N)) and O(N), respectively, where N is the number of surface unknowns on the coarse grid. Using this approach, we illustrate numerical results of TE and TM wave scattering up to surface length of 500 wavelengths and 30,000 surface unknowns. The salient features of the numerical results are as follows: (1) A single coarse grid (SCG) has poorer accuracy for TM case than for TE case. (2) PBTG-BMIAjCAG speeds up CPU and preserves the accuracy. It has accuracy comparable to that of a single dense grid and yet has a CPU comparable to that of a single coarse grid. It also gives surface fields on the dense grid and can give accurate results of the surface fields even when the surface fields have large spatial variations. (3) PBTG-BMIAjCAG gives accurate results for emissivity calculations. word pdf 417 How to Encode a Tab or Function in a PDF417 in Microsoft Word ...
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