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Fundamentals

A Dash of Maxwell’s: A Maxwell’s Equations Primer – Part 6: The Method of Moments

The Method of Moments has become one of the most powerful tools in the RF engineer’s arsenal. In this chapter, we make the transition from theory to practice, first by attempting to compute the characteristics of a “short dipole” by hand, and then by demonstrating that a computer can do that in just a few seconds.

 

A Dash of Maxwell’s: A Maxwell’s Equations Primer – Part 5: Radiation from a Small Wire Element

It is time to put these equations to work by computing the radiation from a simple structure, a short wire element.

 

A Dash of Maxwell’s: A Maxwell’s Equations Primer – Part 4: Equations Even a Computer Can Love

In the preceding chapters we have derived Maxwell’s Equations and expressed them in their “integral” and “differential” form. In different ways, both forms lend themselves to a certain intuitive understanding of the nature of electromagnetic fields and waves. In this installment, we will express Maxwell’s Equations in their “computational form,” a form that allows our computers to do the work.

The Future of Battery Technologies

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In God We Trust… All Others Bring Data

All ESD control products are not created equal. In fact, there are products on...
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Circuit Models Make Shield Design Simple

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Know The Theory of Partial Inductance to Control Emissions

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Minimizing Ringing and Crosstalk

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EMI: Why Digital Devices Radiate

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A Dash of Maxwell’s: A Maxwell’s Equations Primer – Part 3: The Difference a Del Makes

In Chapter 2, I introduced Maxwell’s Equations in their “integral form.” Simple in concept, the integral form can be devilishly difficult to work with. To overcome that, scientists and engineers have evolved a number of different ways to look at the problem, including this, the “differential form of the Equations.” The differential form makes use of vector operations.
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