From Electrostatics to Optics A Concise Electrodynamics Course [Paperback]

After a historical introduction and mathematical preliminaries the book turns to electrostatics in vacuum, whereby Maxwells equations are not postulated as axioms, but deduced from electrostatics plus Lorentz invariance. These general ideas are then illustrated by many applications, radiation phenomena in particular. Chapter 4 is devoted to the completely different subject of phenomenological electrodynamics of matter, with the equations derived by spatial averaging, assuming a classical model for the atomic structure of matter. The chapter on optics is not treated as an independent field, but rather an application of Chapter 4, where significant themes such as wave optics, light scattering, geometrical optics, diffraction theory, and the laser are discussed. Finally, an epilogue relates the classical theory to modern quantum electrodynamics.We live in the electronic age. Millions of people stare at television sets; com? puters penetrate our working life; and the heartbeat of many older people is regulated by a pace-maker. Even music is becoming electric. The good old mechanical Swiss watch has meanwhile been replaced by an electronic watch made in Hong Kong, which is ten times as accurate and costs a tenth of the price. (The cheap Swiss watches are today also electric and the parts are probably made in Hong Kong. ) In physics, the retirement of mechanics as the basis of science already took place in the 19th century, when it was found that light and electromag? netism must be described by a field theory and not by a mechanical theory. That was a radically new idea: The basic objects in Newton's mechanics are point particles with coordinates qi(t) and momenta Pi(t) depending on time. If the index i runs from 1 to f, the system has finitely many (f or 2f) degrees of freedom. The basic quantities of field theory, on the otl1. er hand, are a few vector fields E(t,x), B(t,x), v(t,x) which depend on ti~e and space. The velocity field v( t, x) is fundamental in continuum lsŒ