Advanced Modeling in Computational Electromagnetic by Dragan Poljak PDF

By Dragan Poljak

ISBN-10: 0470036656

ISBN-13: 9780470036655

This article combines the basics of electromagnetics with numerical modeling to take on a wide variety of present electromagnetic compatibility (EMC) difficulties, together with issues of lightning, transmission strains, and grounding structures. It units forth an outstanding origin within the fundamentals sooner than advancing to really expert themes, and permits readers to advance their very own EMC computational versions for purposes in either study and undefined.

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Extra resources for Advanced Modeling in Computational Electromagnetic Compatibility

Example text

The second Maxwell equation is the differential form of Ampere’s law stating ~ that either an electric current density ~ J or a time-varying electric flux density D ~ . This can be expressed as gives rise to a magnetic field H ~ ¼~ rxH Jþ q~ D qt ð2:2Þ ~=qt was added by Maxwell to the original expresIt is worth noting that the term qD sion of Ampere’s law to make the law consistent with the conservation of electric charge. The third Maxwell equation states that electric monopoles exist, so that r~ D¼r ð2:3Þ That is, charge densities r are the sources of the electric field.

144) using the Lorentz gauge and it is given by A À ms r2~ q~ A q2 ~ A À me 2 ¼ 0 qt qt ð2:161Þ The boundary conditions imposed by this choice of gauge are the same as in the diffusion gauge. 92). 162) results in the well-known Poisson potential equation r2 j ¼ À r e ð2:164Þ It is worth noting that the major part of computational electrostatics problems is based on this equation. 164) simplifies into the Laplace equation r2 j ¼ 0 ð2:165Þ which is also widely used in a major part of electrostatic problems.

Also, in the vicinity of a perfect conductor, there is a zero tangential component normal to the conductor and there cannot be power flow into the perfect conductor. Therefore, the final integral form of the conservation law in the electromagnetic field is then given by q qt Z V 1 ~ ~ ~ ~ ðE Á D þ H Á BÞdV ¼ À 2 Z ~ E Á~ J dVþ V I ~ Þ Á d~ ð~ E xH S ð2:70Þ S In other words, the rate of increase of electromagnetic energy in the domain equals the rate of flow of energy in through the domain surface less the Joule heat production in the domain.

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Advanced Modeling in Computational Electromagnetic Compatibility by Dragan Poljak


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