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MOTION MOUNTAIN

LIGHT, CHARGES AND BRAINS - Motion Mountain

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226 5 electromagnetic effects<br />

Challenge 223 s<br />

Page 46<br />

Challenge 224 s<br />

Vol. I, page 340<br />

Challenge 225 s<br />

Challenge 226 s<br />

Challenge 227 s<br />

Ref. 198<br />

Challenge 228 e<br />

Ref. 199<br />

Can you guess whatNis physically? (Hint: think about quantum theory.)<br />

∗∗<br />

Faraday discovered, as told above, how to change magnetism into electricity, knowing<br />

that electricity could be transformed into magnetism.The issue is subtle. Faraday’s law<br />

is not the dual of Ampère’s, as that would imply the use of magnetic monopoles; neither<br />

is it the reciprocal, as that would imply the displacement current. But he was looking for<br />

a link and he found a way to relate the two observations – in a novel way, as it turned<br />

out.<br />

Faraday also discovered how to transform electricity into light and into chemistry. He<br />

then tried to change gravitation into electricity. But he was not successful. Why not?<br />

∗∗<br />

At high altitudes (60 km to1000 km) above the Earth, gases are partly or completely<br />

ionized; no atom is neutral. One speaks of the ionosphere, as space is full of positive<br />

ions and free electrons. Even though both charges appear in exactly the same number, a<br />

satellite moving through the ionosphere acquires a negative charge. Why? How does the<br />

charging stop?<br />

∗∗<br />

A capacitor of capacityCis charged with a voltageU. The stored electrostatic energy is<br />

E=CU 2 /2. The capacitor is then detached from the power supply and branched on to<br />

an empty capacitor of the same capacity. After a while, the voltage obviously drops to<br />

U/2. However, the stored energy now isC(U/2) 2 , which is half the original value. Where<br />

did the energy go?<br />

How can you give somebody an electric shock using a4.5 V battery and some wire?<br />

∗∗<br />

∗∗<br />

An old puzzle about electricity results from the equivalence of mass and energy. It is<br />

known from experiments that the sizedof electrons is surely smaller than10 −22 m. This<br />

means that the electric field surrounding it has an energy contentEgiven by at least<br />

E nergy = 1 2 ε 0∫E 2 ∞<br />

lectric field dV=1 2 ε 0∫ ( 1 2<br />

q<br />

d 4πε o r 2) 4πr 2 dr<br />

= q2 1<br />

>1.2 µJ . (88)<br />

8πε o d<br />

On the other hand, the mass of an electron, usually given as511 keV/c 2 , corresponds<br />

to an energy of only82 fJ, ten million times less than the value just calculated. In other<br />

words, classical electrodynamics has considerable difficulty describing electrons.<br />

In fact, a consistent description of charged point particles within classical electrodynamicsisimpossible.<br />

Thistopicreceives only a rare – but then often passionate – interest<br />

nowadays, because the puzzle is solved in a different way in the quantum parts of ourad-<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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