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MOTION MOUNTAIN

LIGHT, CHARGES AND BRAINS - Motion Mountain

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Vol. IV, page 231<br />

Chapter 2<br />

THE DESCRIPTION OF<br />

ELECTROMAGNETIC FIELD<br />

EVOLUTION<br />

Electric and magnetic fields change: simply said, they move. How<br />

xactly does this happen? In the 1860s, James Clerk Maxwell* collected all<br />

xperimental knowledge he could find, and deduced the precise description of<br />

electromagnetic field motion. Twenty years later, Heaviside and Hertz extracted the<br />

main points of Maxwell ideas, calling their summaryMaxwell’stheoryoftheelectromagneticfield.<br />

The motion of the electromagnetic field is described by a set of evolution equations.<br />

In the relativistic description, the set consists of two equations, in the non-relativistic<br />

case of four equations. All observations of classical electrodynamics follow from these<br />

equations. In fact, if quantum effects are properly taken into account,all electromagnetic<br />

effects of nature are described.<br />

The first field equation of electrodynamics<br />

The first relativistic field equation of electrodynamics is the precise statement that electromagneticfieldsoriginateat<br />

charges,andnowhereelse.Itcan variously be written**<br />

dF=jμ 0 or<br />

∇⋅E= ρ ε 0<br />

and<br />

∇×B− 1 c 2 ∂E<br />

∂t =μ 0j . (28)<br />

*JamesClerkMaxwell(b.1831Edinburgh,d.1879Cambridge) isoneofthemostimportant andinfluential<br />

physicists.Hefoundedelectromagnetismbytheoretically unifying electricityandmagnetism,asdescribed<br />

inthischapter.Hisworkonthermodynamicsformsthesecondpillar ofhisactivity.Inaddition,hestudied<br />

the theory of colours and developed the colour triangle; he was one of the first people to make a colour<br />

photograph. He is regarded by many as the greatest physicist ever. Both ‘Clerk’ and ‘Maxwell’ were his<br />

familynames.<br />

** There is a certain freedom in writing the equations, becausedifferent authors absorb different combinations<br />

of the constantscandμ 0 into the definitions of the quantitiesF,Aandj.The one given here is the<br />

most common version. The equations can be generalized to cases where the charges are not surrounded<br />

by vacuum, but located inside matter. We will not explore these situations in our walk because,as we will<br />

discoverlater on,theseeminglyspecialcaseofvacuuminfactdescribesall ofnature.<br />

Motion Mountain – The Adventure of Physics copyright © Christoph Schiller June 1990–November 2015 free pdf file available at www.motionmountain.net

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