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MOTION MOUNTAIN

LIGHT, CHARGES AND BRAINS - Motion Mountain

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78 2 the description of electromagnetic field evolution<br />

m, q m, q<br />

v<br />

v<br />

0 distance r<br />

F I G U R E 44 Charged particles after a collision.<br />

Challenge 75 ny<br />

Ref. 42<br />

Challenge 76 s<br />

Ref. 43<br />

Page 116<br />

antpropertythatwementionedrightatthestart:thefielditselfcanmove. In particular,<br />

the field can carry energy, linear momentum and angular momentum.<br />

Colliding charged particles<br />

Electromagnetic fields move. A simple experiment clarifies the meaning of motion for<br />

fields: When two charged particles collide, their total momentum is not conserved. Let<br />

us check this.<br />

Imagine two particles of identical mass and identical charge just after a collision, when<br />

they are moving away from one another. The situation is illustrated in Figure 44. Imagine<br />

also that the two masses are large, so that the acceleration due to their electrical<br />

repulsionissmall. Foran observer at the centre of gravity of the two, each particle feels<br />

an acceleration from the electric field of the other. This electric fieldEis given by the<br />

so-calledHeavisideformula<br />

E= q(1−v2 /c 2 )<br />

4πe 0 r 2 . (33)<br />

Inotherwords,thetotalsystemhasavanishing total momentum for this observer.<br />

Take a second observer, moving with respect to the first with velocityv, so that the<br />

first charge will be at rest. Expression (33) leads to two different values for the electric<br />

fields, one at the position of each particle. In other words, the system of the two particles<br />

is not in inertial motion, as we would expect; the total momentum is not conserved for<br />

this observer.The missing momentum is small, but where did it go?<br />

This at first surprising effect has even been put in the form of a theorem by Van Dam<br />

and Wigner. They showed that, for a system of particles interacting at a distance, the total<br />

particle energy–momentum cannot remain constant in all inertial frames.<br />

The total momentum of the system is conserved only because the electromagnetic<br />

field itself also carries some momentum. In short, momentum is conserved in the experiment,butsomeofitiscarriedbythefield.Thepreciseamountdependsontheobserver.<br />

Two colliding charged particles thus show us that electromagnetic fields have momentum.Ifelectromagneticfieldshave<br />

momentum, they are able tostrike objects and to<br />

be struck by them. As we will show below, light is also an electromagnetic field.Thus we<br />

should be able to move objects by shining light on to them. We should even be able to<br />

suspend particles in mid air by shining light on to them from below. Both predictions<br />

are correct, and some experiments will be presented shortly.<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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