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Material downloaded from myCBSEguide.com . 1 / 10 CBSE Class 12 Physics Revision Notes Chapter-10 Wave Optics Wave front: It is the continuous locus of all such particles of the medium which are vibrating in the same phase of oscillation at any instant. Depending upon the shape of the source of light, wavefront are of different shapes. (i) Plane wavefront (ii) Spherical wavefront (iii) Cylindrical wavefront Rays: Rays are the arrows perpendicular to the wavefront in the direction of propagation of a wave. Time Taken: The time taken for light to travel from one wavefront to another is called time taken by a ray. Huygens’ Principle: 1. According to Huygens’ Each point on the given wave front (called primary wave front) acts as a fresh source of new disturbance, called secondary wavelet, which travels in all directions with the velocity of light in the given medium. 2. A surface touching these secondary wavelets, tangentially in the forward direction at any instant gives the new wavefront at that instant. This is called secondary wavelets.

CBSE Class 12 Physics Revision Notes Chapter-10 Wave

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CBSEClass12Physics

RevisionNotes

Chapter-10

WaveOptics

Wavefront:Itisthecontinuouslocusofallsuchparticlesofthemediumwhichare

vibratinginthesamephaseofoscillationatanyinstant.

Dependingupontheshapeofthesourceoflight,wavefrontareofdifferentshapes.

(i)Planewavefront

(ii)Sphericalwavefront

(iii)Cylindricalwavefront

Rays:Raysarethearrowsperpendiculartothewavefrontinthedirectionof

propagationofawave.

TimeTaken:Thetimetakenforlighttotravelfromonewavefronttoanotheris

calledtimetakenbyaray.

Huygens’Principle:

1. AccordingtoHuygens’Eachpointonthegivenwavefront(calledprimarywavefront)

actsasafreshsourceofnewdisturbance,calledsecondarywavelet,whichtravelsinall

directionswiththevelocityoflightinthegivenmedium.

2. Asurfacetouchingthesesecondarywavelets,tangentiallyintheforwarddirectionatany

instantgivesthenewwavefrontatthatinstant.Thisiscalledsecondarywavelets.

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PrincipleofHuygens’Construction:

1. Itisbasedontheprinciplethateverypointonawavefrontisasourceofsecondary

wavefront.

2. Theenvelopeofthesewavefrontsi.e.,thesurfacetangenttoallthesecondarywavefront

givesthenewwavefront.

Snell’slawofrefraction:

ReflectionofPlaneWavesUsingHuygens’Principle:Thelawofreflection(i=

r)canbederivedusingthewavetheory.

RefractionofPlaneWavesUsingHuygens’Principle:theSnell’slawofrefraction

canbederivedusingthewavetheory.(Herev1andv2are

thespeedoflightinmedia1and2withrefractiveindex and respectively).

RelationbetweenFrequencyandSpeed:Thefrequency remainsthesameaslight

travelsfromonemediumtoanother.Thespeedvofawaveisgivenby

Where isthewavelengthofthewaveand istheperiodofoscillation.

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DopplerEffect:Wheneverthereisarelativemotionbetweenthesourceand

observerthentheapparentfrequencyofligtreceivedbytheobserverisdifferent

fromtheactualfrequencyemittedbythesourceoflight.ThiseffectiscalledDoppler's

effectinlight.Theeffectcanbeusedtomeasurethespeedofanapproachingor

recedingobject.

ChangeinFrequency:Forthesourcemovingawayfromtheobserver ,and

forthesourcemovingtowardstheobserver ,.Thechangeinfrequencyis

So,finally,

CoherentandIncoherentAdditionofWaves:

Coherentsources:-Twosourcesoflightwhichcontinouslyemitlightwavesofsame

frequency(orwavelength)withazeroorconstantphasedifferencebetweenthem,

arecalledcoherentsources.

Incoherentsources:-Twosourcesoflightwhichdonotemitlightwaveswitha

constantphasedifferencearecalledincoherentsources.

ThetotalintensityIisnotjustthesumofindividualintensitiesI1andI2duetothetwo

sourcesbutincludesaninterferenceterm-

Theinterferencetermaveragedovermanycyclesiszeroif

1. Thesourceshavedifferentfrequenciesor

2. Thesourceshavethesamefrequencybutnostablephasedifference.

3. Forsuchcoherentsources-

4. Accordingtothesuperpositionprinciplewhentwoormorewavemotionstraveling

throughamediumsuperimposeoneanother,anewwaveisformedinwhichresultant

displacementsduetotheindividualwavesatthatinstantisgivenby-

5. Theaverageofthetotalintensitywillbe

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Where istheinherentphasedifferencebetweenthetwosuperimposingwaves.

6. Thesignificanceisthattheintensityduetotwosourcesoflightisnotequaltothesumof

intensitiesduetoeachofthem.

7. Theresultantintensitydependsontherelativelocationofthepointfromthetwosources,

sincechangingitchangesthepathdifferenceaswegofromonepointtoanother.

8. Asaresult,theresultingintensitywillvarybetweenmaximumandminimumvalues,

determinedbythemaximumandminimumvaluesofthecosinefunction.Thesewillbe

=

=

Young’sExperiment

TwoparallelandverycloseslitsS1andS2(illuminatedbyanothernarrowslit)behave

liketwocoherentsourcesandproduceapatternofdarkandbrightbandsonascreen

knownasinterferencefringes.

ForapointPonthescreen,thepathdifference

Wheredistheseparationbetweentwoslits,Disthedistancebetweentheslitsand

thescreenandxisthedistanceofthepointofPfromthecentralfringe.

Forconstructiveinterference(brightband),thepathdifferencemustbeaninteger

multipleof ,i.e.-

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Theseparation betweenadjacentbright(ordark)fringesis, usingwhich

canbemeasured.

Young’sDoubleSlitInterferenceExperiment:Fringewidth,

whereDisthedistancebetweentheslits&thescreendisthedistancebetweenthe

twoslits

ConstructiveInterference:

1. Phasedifference: wherenisaninteger

2. Pathdifference: wherenisaninteger

Destructiveinterference:

1. Phasedifference: ,wherenisaninteger

2. Pathdifference: ,wherenisaninteger

Intensitydistributioncurveforinterference:

Interferencefringeswithwhitelight:-Whentheslitsareilluminatedwithwhite

light,theinterferencepatternconsistofacentralwhitefringehavingonbothsidesa

fewcolouredfringesandthenageneralillumination.

Conditionsforsustainedinterference:-

(i)Twosourcesoflightmustbecoherent.

(ii)Thefrequencies(orwavelength)ofthetwowavesshouldbeequal.

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(iii)Thelightmustbemonochromatic.

(iv)Theamplitudesoftheinterferingwavesmustbeequalornearlyequal.

(v)Thetwosourcesmustbenarrow.

Diffraction:

Thephenomenonofbendingoflightaroundthecornersofanobstacleiscalledthe

diffractionoflight.

DiffractionduetoSingleSlit:

1. Thesingle-slitdiffractionpatternshowsthecentralmaximum ,zerointensity

atangularseparation

2. Angularspreadofthecentralmaxima

3. Widthofthecentralmaxima:

WhereDisthedistanceoftheslitfromthescreen,distheslitwidth.

ConditionfortheMinimaontheeithersideoftheCentralMaxima: ,

wheren=1,2,3,….

Relationbetweenphasedifference&pathdifference:

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Where isthephasedifference& isthepathdifference.

DifferentPartsoftheWaveFrontattheSlitactasSecondarySources:

1. Diffractionpatternistheresultofinterferenceofwavesfromthesesources.

2. Theintensityplotlooksasfollows,withtherebeingabrightcentralmaximum,followed

bysmallerintensitysecondarymaxima,withtherebeingpointsofzerointensityin

between,whenever

3. Widthofcentralmaximumisdirectlyproportionaltowavelengthoflightandinversely

proportionaltothewidthoftheslit.

Emission,AbsorptionandScattering:

1. Thesearethethreeprocessesbywhichmatterinteractswithradiation.Inemission,an

acceleratedchargeradiatesandlosesenergy.

2. Inabsorption,thechargegainsenergyattheexpenseoftheelectromagneticwave.

3. Inscattering,thechargeacceleratedbyincidentelectromagneticwaveradiatesinall

direction.

Polarization:

1. Ifthevibrationsofawavearepresentinjustonedirectioninaplaneperpendicularto

thedirectionofpropagation,thewaveissaidtobepolarisedorplanepolarised.the

phenomenonofrestrictingtheoscillationsofawavetojustonedirectioninthe

transverseplaneiscalledpolarisationofwaves.

2. WhenlightpassesthroughasinglepolaroidP1lightintensityisreducedtohalf,

independentoftheorientationofP1.WhenasecondPolaroidP2isalsoincluded,atone

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specificorientationw.r.tP1,thenettransmittedintensityisreducedtozerobutis

transmittedfullywhenP1isturned900fromthatorientation.Thishappensbecausethe

transmittedpolarizationbyapolaroidisthecomponentofEparalleltoitsaxis.

3. Polariser:Adevicethatpolarisestheunpolarisedlightpassedthroughitiscalleda

polariser.

4. Unpolarizedsunlightscatteredbytheatmosphereorreflectedfromamediumgets

partiallypolarized.

OpticalActivity:Whenplanepolarisedlightpassesthroughacertainsubstances,the

planeofpolarisationofthelightisrotatedaboutthedirectionofpropagationoflight

throughacertainangle.Thisphenomenoniscalledopticalactivityoropticalrotation

andthesubstancesopticallyactive.

IntensityoftheLightduetoPolarization(LawofMalus):

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WhereIistheintensityoflightafterpolarization,Ioistheoriginalintensity, isthe

anglebetweentheaxisoftheanalyzer&thepolarizer

AgraphbetweentheintensityoflightItransmittedbytheanalyserandtheangle

betweenthepolariserandtheanalyserwillbeasshown-

Methodsofproducingplanepolarisedlight:

1. Reflection

2. Scattering

3. Doublerefraction

Polarisationbyreflection(Brewster’sLaw):Whenunpolarisedlightisincidentona

transparentsurfaceatthepolarisingangle ,thereflectedlightispolarisedwithits

electricvectorperpendiculartotheplaneofincidencewhentherefractedand

reflectedraysmakearightanglewitheachother.

PolarizationbyScattering:

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1. Lightisscatteredwhenitmeetsaparticleofsimilarsizetoitsownwavelength.The

scatteringofsunlightbydustparticlesisanexampleofpolarizationbyscattering.

Polarizationbydoublerefraction:Whenanunpolrisedraypassesthroughcertain

crystalslikequartzorcalcite,itspiltsupintotworays.Thisphenomenoniscalled

doublerefraction.

Rayleighshowedthatthescatteringoflightisproportionaltothefourthpowerofthe

frequencyofthelightorvariesas where isthewavelengthoflightincidenton

theairmoleculesofsize‘d’where .Hencebluelightisscatteredmorethan

red.Thisexplainsthebluecolourofthesky.

Polaroids:Polaroidsarethincommercialsheetswhichmakeuseofthepropertyof

selectiveabsorptiontoproduceanintensebeamofplanepolarisedlight.

Usesofpolaroids-Insunglassesandcamerafilters,Inwindscreens,Inwindow

panesofaeroplanes,InLCDsetc.