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1、Lecture2Lecture2ReflectionandRefraction,Snell’sLaw[Readingassignment:Hecht4.3,4.4,4.7]Animportantelementofopticsistheinterfacebetween2materialswithdifferentindexofrefractionreflectedray11n1n2refractedray2nsin=nsin1122sin1n2ifn2n121-------------=-----sin2n1ifnn122
2、1TotalReflectionIfnn,thenwecanhave121=902n2sin=-----cn1–12=90c=sinn2n1Therefractedraydisappears!Thelightistotallyreflected.Thisusuallyoccursinsideaprism,andiscalledtotalinternalreflection.=“criticalangle”.Foratypicalglasswithn=1.5,thecriticalanglecis:–11sin-------=
3、41.8.1.51©JeffreyBokor,2000,allrightsreservedLecture2Sofor=45,thelightisreflected.Averycommonprismistherightangleprism459045LightImpingingataSurfaceTheplanecontainingthelightraypropagationvectorandthesurfacenormaliscalledthe“planeofinci-dence”EE1pnormalE1p1sE1sn111nE
4、E22p2s2p-polarizations-polarization(paralleltoplaneofincidence)•Forageneralpolarizationstateincidentonasurface,wechoosesandpdirectionstodecomposethepolarizationeffects.FresnelReflectionCoefficients[Optionalreading:Hecht4.6]Themagnitudeofreflectionandtransmissionataninterfacebet
5、weennandnaregivenby12222tan–ncos4sincos212221R=---------------------------------T=--------------------------------------------------------------------------------------p2pncos22tan+11sin+cos–211212222sin–ncos4sincos212221R=-----------------------------
6、---T=--------------------------------------------------------s2sncos2sin+11sin+21122©JeffreyBokor,2000,allrightsreservedLecture2n–n221near==0RR=-----------------.Forn=1.5R4%Noticealso,if1spn+n21+=---,thentan,andR0.212pn2canbeshowntobegivenbytan=-----.Th
7、isangleisknownas“Brewster’sangle”or11n1the“Polarizingangle”.PolarizationReadingAssignment:Hecht8.1,8.2]•Lightwaveshavetransversepolarization•Theelectricfieldvectorpointsinadirectionperpendiculartothepropagationdirection(raydirection).•Themagneticfieldvectorisorthogonaltopropagat
8、iondirection.Generally,wecanignorethemag-neticf