The Origin of the Refraction Index文献及翻译.docx
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The Origin of the Refraction Index文献及翻译.docx
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TheOriginoftheRefractionIndex文献及翻译
外文文献:
TheOriginoftheRefractionIndex
Wehavesaidbeforethatlightgoesslowerinwaterthaninair,andslower,slightly,inairthaninvacuum.Thiseffectisdescribedbytheindexofrefractionn.Nowwewouldliketounderstandhowsuchaslowervelocitycouldcomeabout.Inparticular,weshouldtrytoseewhattherelationistosomephysicalassumptions,orstatements,wemadeearlier,whichwerethefollowing:
(a)Thatthetotalelectricfieldinanyphysicalcircumstancecanalwaysberepresentedbythesumofthefieldsfromallthechargesintheuniverse.
(b)Thatthefieldfromasinglechargeisgivenbyitsaccelerationevaluatedwitharetardationatthespeedc,always(fortheradiationfield).
But,forapieceofglass,youmightthink:
"Oh,no,youshouldmodifyallthis.Youshouldsayitisretardedatthespeedc/n."That,however,isnotright,andwehavetounderstandwhyitisnot.
Itisapproximatelytruethatlightoranyelectricalwavedoesappeartotravelatthespeedc/nthroughamaterialwhoseindexofrefractionisn,butthefieldsarestillproducedbythemotionsofallthecharges-includingthechargesmovinginthematerial-andwiththesebasiccontributionsofthefieldtravellingattheultimatevelocityc.Ourproblemistounderstandhowtheapparentlyslowervelocitycomesabout.
Weshalltrytounderstandtheeffectinaverysimplecase.Asourcewhichweshallcall"theexternalsource"isplacedalargedistanceawayfromathinplateoftransparentmaterial,sayglass.Weinquireaboutthefieldatalargedistanceontheoppositesideoftheplate.ThesituationisillustratedbythediagramofFig.31-1,whereSandPareimaginedtobeveryfarawayfromtheplate.Accordingtotheprincipleswehavestatedearlier,anelectricfieldanywherethatisfarfromallmovingchargesisthe(vector)sumofthefieldsproducedbytheexternalsource(atS)andthefieldsproducedbyeachofthechargesintheplateofglass,everyonewithitsproperretardationatthevelocityc.Rememberthatthecontributionofeachchargeisnotchangedbythepresenceoftheothercharges.Theseareourbasicprinciples.ThefieldatPcanbewrittenthus:
(31.1)
or
,(31.2)
whereEsisthefieldduetothesourcealoneandwouldbepreciselythefieldatPiftherewerenomaterialpresent.WeexpectthefieldatPtobedifferentfromEsifthereareanyothermovingcharges.
Whyshouldtherebechargesmovingintheglass?
Weknowthatallmaterialconsistsofatomswhichcontainelectrons.Whentheelectricfieldofthesourceactsontheseatomsitdrivestheelectronsupanddown,becauseitexertsaforceontheelectrons.Andmovingelectronsgenerateafield-theyconstitutenewradiators.ThesenewradiatorsarerelatedtothesourceS,becausetheyaredrivenbythefieldofthesource.ThetotalfieldisnotjustthefieldofthesourceS,butitismodifiedbytheadditionalcontributionfromtheothermovingcharges.Thismeansthatthefieldisnotthesameastheonewhichwastherebeforetheglasswasthere,butismodified,anditturnsoutthatitismodifiedinsuchawaythatthefieldinsidetheglassappearstobemovingatadifferentspeed.Thatistheideawhichwewouldliketoworkoutquantitatively.
Nowthisis,intheexactcase,prettycomplicated,becausealthoughwehavesaidthatalltheothermovingchargesaredrivenbythesourcefield,thatisnotquitetrue.Ifwethinkofaparticularcharge,itfeelsnotonlythesource,butlikeanythingelseintheworld,itfeelsallofthechargesthataremoving.Itfeels,inparticular,thechargesthataremovingsomewhereelseintheglass.Sothetotalfieldwhichisactingonaparticularchargeisacombinationofthefieldsfromtheothercharges,whosemotionsdependonwhatthisparticularchargeisdoing!
Youcanseethatitwouldtakeacomplicatedsetofequationstogetthecompleteandexactformula.Itissocomplicatedthatwepostponethisproblemuntilnextyear.
Insteadweshallworkoutaverysimplecaseinordertounderstandallthephysicalprinciplesveryclearly.Wetakeacircumstanceinwhichtheeffectsfromtheotheratomsisverysmallrelativetotheeffectsfromthesource.Inotherwords,wetakeamaterialinwhichthetotalfieldisnotmodifiedverymuchbythemotionoftheothercharges.Thatcorrespondstoamaterialwhichtheindexofrefractionisverycloseto1,whichwillhappen,forexample,ifthedensityoftheatomsisverylow.Ourcalculationwillbevalidforanycaseinwhichtheindexisforanyreasonverycloseto1.Inthiswayweshallavoidthecomplicationsofthemostgeneral,completesolution.
Incidentally,youshouldnoticethatthereisanothereffectcausedbythemotionofthechargesintheplate.ThesechargeswillalsoradiatewavesbacktowardthesourceS.Thisbackward-goingfieldisthelightweseereflectedfromthesurfacesoftransparentmaterials.Itdoesnotcomefromjustthesurface.Thebackwardradiationcomesfromeverywhereintheinterior,butitturnsoutthatthetotaleffectisequivalenttoareflectionfromthesurfaces.Thesereflectioneffectsarebeyondourapproximationatthemomentbecauseweshallbelimitedtoacalculationforamaterialwithanindexsocloseto1thatverylittlelightisreflected.
Beforeweproceedwithourstudyofhowtheindexofrefractioncomesabout,weshouldunderstandthatallthatisrequiredtounderstandrefractionistounderstandwhytheapparentwavevelocityisdifferentindifferentmaterials.Thebendingoflightrayscomesaboutjustbecausetheeffectivespeedofthewavesisdifferentinthematerials.ToremindyouhowthatcomesaboutwehavedrawninFig.31-2severalsuccessivecrestsofanelectricwavewhicharrivesfromavacuumontothesurfaceofablockofglass.Thearrowperpendiculartothewavecrestsindicatesthedirectionoftravelofthewave.Nowalloscillationsinthewavemusthavethesamefrequency.(Wehaveseenthatdrivenoscillationshavethesamefrequencyasthedrivingsource.)Thismeans,also,thatthewavecrestsforthewavesonbothsidesofthesurfacemusthavethesamespacingalongthesurfacebecausetheymusttraveltogether,sothatachargesittingattheboundarywillfeelonlyonefrequency.Theshortestdistancebetweencrestsofthewave,however,isthewavelengthwhichisthevelocitydividedbythefrequency.Fromthefigurewecanseethattheonlywayforthewavesto"fit"properlyattheboundaryisforthewavesinthematerialtobetravellingatadifferentanglewithrespecttothesurface,fromthegeometryofthefigureyoucanseethatfora"fit"wemusthave
or
whichisSnell'slaw.Weshall,fortherestofourdiscussion,consideronlywhylighthasaneffectivespeedofc/ninmaterialofindexn,andnolongerworry,inthischapter,aboutthebendingofthelightdirection.
WegobacknowtothesituationshowninFig.31-1.WeseethatwhatwehavetodoistocalculatethefieldproducedatPbyalltheoscillatingchargesintheglassplate.WeshallcallthispartofthefieldEa,anditisjustthesumwrittenasthesecondterminEq.(31.2).WhenweaddittothetermEs,duetothesource,wewillhavethetotalfieldatP.31-2Thisisprobablythemostcomplicatedthingthatwearegoingtodothisyear,butitiscomplicatedonlyinthattherearemanypiecesthathavetobeputtogether;eachpiece,however,isverysimple.Unlikeotherderivationswherewesay,"Forgetthederivation,justlookattheanswer!
"inthiscasewedonot
needtheanswersomuchasthederivation.Inotherwords,thethingtounderstandnowisthephysicalmachineryfortheproductionoftheindex.
Toseewherewearegoing,letusfirstfindoutwhatthecorrectionfield"EawouldhavetobeifthetotalfieldatPisgoingtolooklikeradiationfromthesourcethatissloweddownwhilepassingthroughthethinplate.Iftheplatehadnoeffectonit,thefieldofawavetravellingtotheright(alongthez-axis)wouldbe
or,usingtheexponentialnotation,
Nowwhatwouldhappenifthewavetravelledmoreslowlyingoingthroughtheplate?
Letuscallthethicknessoftheplate
.Iftheplatewerenottherethewavewouldtravelthedistance
inthetime
Butifitappearstotravelatthespeedc/nthenitshouldtakethelongertime
ortheadditionaltime
.Afterthatitwouldcontinuetotravelatthespeedcagain.WecantakeintoaccounttheextradelayingettingthroughtheplatebyreplacinginEq.(31.4)by
orby
.Sothewaveafterinsertionoftheplateshouldbewritten
(31.5)
Wecanalsowritethisequationas
(31.6)
31-3Dispersion
Noticethatintheaboveprocesswehaveobtainedsomethingveryinteresting.Forwehavenotonlyanumberfortheindexofrefractionwhichcanbecomputedfromthebasicatomicquantities,butwehavealsolearnedhowtheindexofrefractionshouldvarywiththefrequencycofthelight.Thisissomethingwewouldneverunderstandfromthesimplestatementthat"lighttravelsslowerinatransparentmaterial."Westillhavetheproblem,ofcourse,ofknowinghowmanyatomsperunitvolumethereare,andwhatistheirnaturalfrequencyw0.Wedonotknowthisjustyet,becauseitisdifferentforeverydifferentmaterial,andwecannotgetageneraltheoryofthatnow.Formulationofageneraltheoryofthepropertiesofdifferentsubstances-theirnaturalfrequencies,andsoon-ispossibleonlywithquantumatomicmechanics.Also,differentmaterialshavedifferentpropertiesanddifferentindexes,sowecannotexpect,anyway,togetageneralformulafortheindexwhichwillapplytoallsubstances.
However,weshalldiscusstheformulawehaveo
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