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MOTION MOUNTAIN

LIGHT, CHARGES AND BRAINS - Motion Mountain

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350 challenge hints and solutions<br />

b<br />

a<br />

c<br />

β<br />

Ref. 97<br />

Input and output beams are antiparallel,<br />

β determines the polarization rotation.<br />

Input and output beams are parallel,<br />

the length ratios a : b : c determine the<br />

polarization rotation.<br />

F I G U R E 174 Two mirror arrangements that rotate the polarization of a light beam by a predetermined<br />

angle.<br />

Challenge 147, page 138: Three mirrors is the minimum. Two such mirror arrangements are<br />

shown in Figure 174. There is also a three-mirror arrangement with parallel input and output<br />

beams;canyoufindit?Theideasbehindthesearrangementsarewellexplainedinthepapers by<br />

EnriqueGalvez andhiscollaborators.<br />

Challenge 148, page 138: In the left interferometer, light exits in direction B, in the right one,<br />

indirectionA.Theproblemcanalsobegeneralized toarbitrary interferometer shapes.Theway<br />

to solve it in this case is the use of Berry’s phase. If you are interested, explore this interesting<br />

conceptwiththehelpofyourfavourite library.<br />

Challenge 149, page 143: The average temperature of the Earth is thus287 K. The energy from<br />

the Sun is proportionalto the fourth power of the temperature. The energy is spread (roughly)<br />

overhalftheEarth’ssurface.Thesameenergy,attheSun’ssurface,comesfromamuchsmaller<br />

surface,given bythesameangleastheEarth subtendsthere.WethushaveE∼2πR 2 Earth T4 Earth =<br />

T 4 Sun R2 Earth α2 ,whereαishalftheangle subtendedbytheSun.Asaresult, thetemperatureof the<br />

SunisestimatedtobeT Sun =(T 4 Earth /α2 ) 0.25 =4 kK.<br />

Challenge 153, page 144: Because themaximumof a spectruminwavelengths andin frequenciesisnotthesame,thusdoesnot<br />

andcannotfollowc=fλ.<br />

Challenge 156, page 145: At high temperature, all bodies approach black bodies. The colour is<br />

moreimportantthanothercoloureffects. Theoven andtheobjectshavethesametemperature.<br />

Thus they cannot bedistinguishedfrom each other. Todo so nevertheless, illuminate the scene<br />

withpowerful lightand thentake apicturewith small sensitivity.Thusonealwaysneeds bright<br />

lighttotakepicturesofwhathappensinsidefires.<br />

Challenge 157, page 146: Achievingahighertemperaturewouldallowtobreakthesecondprincipleofthermodynamics.Toexplorethisquestionfurther,readintextbooksabouttheso-called<br />

Kirchhofflaws.<br />

Challenge 158, page 147: Theeffectivetemperatureoflaserlightcanalsobedescribedashigher<br />

thaninfinite;thisallowsalsotoheattargets toextremely hightemperatures.<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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