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Such a structure is intended for the deliberate curving of magnetic dynamic lines, without affecting the electric ones. For an acceptable simulation, the domain is discretized into 120 ´ 24 ´ 120 cells, and the excitation is launched at the z = 0 plane, whereas the open waveguide ends are terminated by the pertinent absorbing boundary conditions (see Chapter 4 for an elaborate explanation). 4 presents the magnitude of the Ey component at the y = 8 plane for several time-step values, revealing the smoothness of propagation and the total absence of spurious modes.

They can completely represent the profile of every field component anywhere on the FDTD lattice. Evidently, when a cubic mesh (D = Dx = Dy = Dz) is considered, storage demands can be more efficiently handled. This parametric rendition permits the easier incorporation of material attributes and enhances the compactness of the analysis. 24) may be written more elegantly. This is performed through the pertinent number (1 to 6) of integer arrays depending on the E and H components that interact with these media.

Because of the deformation of the elements in the vicinity of a geometric discontinuity or detail, their intrinsic attributes are likely to be distorted, hence affecting the consistency of the mesh. To indicate the modeling capabilities of the FDTD method, consider the simple 3-D EMC problem of an H-bend waveguide with a uniform cross section along the y-axis. Such a structure is intended for the deliberate curving of magnetic dynamic lines, without affecting the electric ones. For an acceptable simulation, the domain is discretized into 120 ´ 24 ´ 120 cells, and the excitation is launched at the z = 0 plane, whereas the open waveguide ends are terminated by the pertinent absorbing boundary conditions (see Chapter 4 for an elaborate explanation).

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