glen dash

Please view the Digital Edition to read the article (click here).

Please view the Digital Edition to read the article (click here).

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.

In this chapter, Dash makes the modifications to Maxwell’s Equations necessary to encompass the “dynamic” case, that is, where magnetic and electric fields are changing.

Maxwell’s Equations are eloquently simple yet excruciatingly complex. These equations just don’t give the scientist or engineer insight; they are literally the answer to everything RF.