By Kantartzis N.V., TsiboukisT.D.
The target of this two-volume booklet is the systematic and finished description of the main aggressive time-domain computational equipment for the effective modeling and actual answer of contemporary real-world EMC difficulties. meant to be self-contained, it plays an in depth presentation of all recognized algorithms, elucidating on their benefits or weaknesses, and accompanies the theoretical content material with a number of functions. Outlining the current quantity, numerical investigations delve into revealed circuit forums, monolithic microwave built-in circuits, radio frequency microelectromechanical platforms in addition to to the serious problems with electromagnetic interference, immunity, protecting, and sign integrity. Biomedical difficulties and EMC try out facility characterizations also are completely coated through different time-domain types and exact implementations. additionally, the research covers the case of large-scale functions and electrostatic discharge difficulties, whereas exact realization is attracted to the impression of up to date fabrics within the EMC international, equivalent to double damaging metamaterials, bi-isotropic media, and a number of other others.
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Extra resources for Modern EMC Analysis Techniques. Vol. 2
Device, Fields, vol. 22, pp. 299–321, 2004. 9. J. Fan, J. L. Drewniak, H. Shi, and J. Knighten, “DC power-bus modeling and design with a mixed-potential integral-formulation and circuit extraction,” IEEE Trans. Electromagn. , vol. 43, no. 4, pp. 426–436, Nov. 2001. 10. Y. Kayano, M. Tanaka, J. L. Drewniak, and H. Inoue, “Common-mode current due to a trace near a PCB edge and its suppression by a guard band,” IEEE Trans. Electromagn. , vol. 46, no. 1, pp. 46–53, Feb. 2004. 823609 11. N. V. Kantartzis, T.
Vol. 50, no. 5, May 2002. 35. J. Gómez-Tagle, P. F. Wahid, M. T. Chryssomallis, and C. G. Christodoulou, “FDTD analysis of finite-sized phased array microstrip antennas, IEEE Trans. , vol. 51, no. 8, pp. 2057–2062, Aug. 2003. 813640 36. N. V. Kantartzis and T. D. Tsiboukis, “A higher order nonstandard FDTD-PML method for the advanced modeling of complex EMC problems in generalized 3-D curvilinear coordinates,” IEEE Trans. Electromagn. , vol. 46, pp. 2–11, Feb. 2004. 823606 37. M. N. Vouvakis, C.
1) where (xi, yj, zk) points are defined by the i, j, k indices along the three axes of the grid. Also in G, the nonempty faces Am (m = 1, 2, ¼, NA) are the intersections of two cells, edges Lm (m = 1, 2, ¼, NL) signify the intersection of faces, and nodes Pm (m = 1, 2, ¼, NP) are created by the intersection of edges. Next, Maxwell’s laws and the related constitutive equations are discretized by allocating electric voltages, e, on the edges and magnetic fluxes, b, on the faces of a primary lattice and magnetic voltages, h, on the edges and electric fluxes, d, on the faces of a secondary (dual) lattice.