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MOTION MOUNTAIN

LIGHT, CHARGES AND BRAINS - Motion Mountain

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346 challenge hints and solutions<br />

Poynting vector field<br />

cable,<br />

forward<br />

current<br />

Resistance-free<br />

cable<br />

cable,<br />

backward<br />

Loss-free<br />

transformer<br />

Poynting vector field<br />

F I G U R E 172 The Poynting vector field for a cable without electrical resistance and the situation a long<br />

transformer without losses.<br />

Challenge 77, page 79: Field lines and equipotential surfaces are always orthogonal to each<br />

other.Thusafield linecannotcrossanequipotentialsurfacetwice.<br />

Challenge 85, page 83: See Figure 172. If the cable is resistance-free, most of the energy flows<br />

justoutsidethetwoconductorsandparallel tothem.Ifthecabledoeshaveresistance,thePoynting<br />

vectors point slightly towards the conductors. For the case of a transformer, which can be<br />

deduced fromthecaseofthecablevia theanalogy sketched inthepicture,seethebeautiful paperbyF.<br />

Herrmann & G.B. Schmid, The Ponyting vector fieldand the energy flow withina<br />

transformer,AmericanJournalofPhysics54,pp.528–531,1986.<br />

Challenge 90, page 86: Theargumentisthesameasfortheincreaseinentropy:reverseprocesses<br />

arepossible,buttheprobabilityissolowthattheydonotappearinpractice.Theextremely low<br />

probabilityisduetothefluctuationsinduced bytheenvironment.<br />

Challenge 91, page 86: Justdrawacurrentthroughacoilwithitsmagneticfield,thendrawthe<br />

mirrorimageofthecurrent andredraw themagneticfield.<br />

Challenge 92, page 87: Other asymmetries in nature include the helicity of the DNA molecules<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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