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    SeeingEarthsOrbitintheStars:ParallaxandAberrationToddTimberlake,BerryCollege,MountBerry,GA

    Duringthe17thcenturytheideaofanorbitingandrotatingEarthbecame

    increasinglypopular,butopponentsofthisviewcontinuedtopointoutthatthe

    theoryhadobservableconsequencesthathadnever,infact,beenobserved.1Why,

    forinstance,hadastronomersfailedtodetecttheannualparallaxofthestarsthatmustoccurifEarthorbitstheSun?

    Toaddressthisproblem,astronomersofthe17thand18thcenturiessoughtto

    measuretheannualparallaxofstarsusingtelescopes.Noneofthemsucceeded.

    Annualstellarparallaxwasnotsuccessfullymeasureduntil1838,whenFriedrich

    Besseldetectedtheparallaxofthestar61Cygni.2

    Buttheearlyfailurestodetectannualstellarparallaxledtothediscoveryofanew(andentirelyunexpected)

    phenomenon:theaberrationofstarlight.Thispaperrecountsthestoryofthe

    discoveryofstellaraberration.Itisaccompaniedbyasetofactivitiesandcomputer

    simulationsthatallowstudentstoexplorethisfascinatinghistoricalepisodeand

    learnimportantlessonsaboutthenatureofscience.3

    Parallax

    Holdupyourthumbinfrontofyourfaceatarmslength.Closeyourrighteyeand

    viewyourthumbagainstthebackground.Nowopenyourrighteyeandcloseyour

    left:youwillseeyourthumbappeartomoveagainstthebackground.Theapparentdisplacementofyourthumbisreallycausedbythedisplacementofyourobservinglocation(fromyourlefteyetoyourright).Thisphenomenon,knownasparallax,

    playsanimportantroleinastronomy.

    TheAncientGreekswereawarethatcelestialobjectsviewedfromdifferent

    locationsonEarthmightappearinslightlydifferentlocationsrelativetothebackgroundstars.Theyusedthiseffect,knownasdiurnalparallax,toaccurately

    estimatethedistancetotheMoon.Figure1illustratesthegeometryofthis

    measurement.ForsimplicitywewillassumetheMoonliesintheequatorialplane

    andobservationsaremadefromoppositesidesofEarthsequator(thepointsO1

    andO2).ThetwoobserversseetheMoonatdifferentlocationsontheCelestialSphere(orthestarrybackground,tousemoremodernterminology).These

    apparentlocationsareseparatedbyanangle2.Fromtrigonometry(andusingthe

    smallangleapproximation)wefind:

    =!"!

    !", (1)

    whereistheparallaxangleindegrees,bisthebaseline(inthiscasethediameter

    ofEarth),anddisthedistancefromthecenterofEarthtothecenteroftheMoon.

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    Notethatifyoucanmeasuretheparallaxangle,andyouknowthebaseline,youcan

    determinethedistancetotheobject.ThisishowtheAncientGreeksdeterminedthe

    distancetotheMoon.Buttheycouldnotdetectanyparallaxinthestars.Thiswas

    easilyexplained:thestarswereveryfarawaycomparedtotheEarthsdiameter

    (b

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    beengreatlyexaggeratedinordertomaketheeffectvisibleinthesimulation,but

    theplotillustratesthecorrectpatternofchangesinDeclinationresultingfrom

    annualparallax.

    In1674Hookepublishedhisresultsandclaimedtohavedetectedannualparallax.5

    Althoughhegaveadetaileddiscussionofhiscarefulmeasurementprocedure,hepresentedonlyfourobservations.Problemswiththetelescopeandhisownhealth

    preventedhimfromcontinuingthework.HookesdataisshowninFigure3.A

    comparisonwiththeparallaxpredictioninFig.2showsthatHookesdataseemsto

    matchtheexpectedpatternforannualparallax,buthiscontemporariesdidnotfindfourobservationsmadewithanunreliabletelescopeveryconvincing.Theracefor

    parallaxwasnotyetover.

    AberrationofStarlight

    SeveralastronomersattemptedtofollowuponHookesmeasurement.G.D.Cassini

    andJeanPicardmeasuredvariationsinthepositionofPolaris,butwithinconclusiveresults.AstronomerRoyalJohnFlamsteedthoughthehadmeasuredanannual

    parallaxforPolarisuntilCassinipointedoutthatFlamsteedsdatadidnotfitthe

    expectedpattern.6

    In1725,SamuelMolyneuxandJamesBradleysetouttorepeatHookes

    measurementsofGammaDraconisbyconstructingazenithtelescopeinMolyneuxs

    mansionatKewnearLondon.Theyfoundthatthestarvarieditsposition,butnotin

    thewayreportedbyHooke.Bradleyfolloweduponthisworkbymeasuringseveral

    morestarsusingashorterzenithtelescopeinhisresidenceatWanstead.Fig.3

    showsBradleysdataforGammaDraconisandAlkaid(EtaUrsaMajoris).Thedata

    showthesinusoidalvariationexpectedforparallax,butthephaseis3monthsofffromthepredictionsshowninFig.2!

    BradleyknewofOleRmers1676estimateofthefinitespeedoflight,andeventuallyusedthisideatodeviseanexplanationforhisdata.Bradleyrealizedthat

    ittakesthelightfromastarafinitetimetotravelthroughatelescopetube,andduringthistimethetubemovesslightlybecauseofthemotionofEarth.Bradleys

    theoryisillustratedinFigure4forthecaseofastarthatliesdirectlyoverhead.The

    starlightentersthetopofthetubeatp1.Itthentravelsadistancehbeforereaching

    theeyepieceatp3.Ifcisthespeedoflight,thenittakesatimeh/cforthelightto

    travelthisdistance.Duringthistimethetelescopehasmovedadistancevh/c,

    wherevisthevelocityofEarthsorbitalmotion.7Asaresult,thetelescopecannotbeaimeddirectlyuptowardthestar.Itmustbetiltedslightlytowardthedirection

    ofthetelescopesmotion.Thisphenomenonisnowcalledtheaberrationofstarlight.

    ApplyingtrigonometrytoFig.4wefindthat

    tan =!

    !

    , (2)whereistheangleoftilt.ForaninteractiveanimatedversionofFig.4seethe

    StellarAberration2Dprogram.3

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    Fig.4illustratestheapparentdisplacementofthestarduetoaberrationatasingle

    moment in time. As the Earth moves around in its orbit, its velocity changes

    direction and therefore the displacementof starsdue toaberrationwill change.8

    Thepatternofapparentmovementdependsonthelocationof thestarin thesky.

    These patterns are illustrated in the StellarAberration3D program.3

    ThisprogramwasusedtoconstructplotsoftheapparentdeclinationofGammaDraconis

    and Alkaid, usingBradleys theory ofstellar aberration, as shown inFigure 5. A

    comparisonwithFig.4showsthatthepatternpredictedbyBradleystheoryfitshis

    observationaldata.

    Bradleysdataindicatesadisplacementof20.2secondsofarcforastarthatliesina

    directionperpendiculartoEarthsmotion.UsingEquation2Bradleyfoundthatthespeedoflightmustbe10,210timesasgreatasEarthsorbitalspeed,solighttakes8

    minutes,12secondstotravelfromtheSuntoEarth.9

    BradleystheoryexplainedthemovementofPolarisobservedbyCassini,Picard,andFlamsteed,buthecouldnotgiveanexplanationforHookesmeasurementsofGammaDraconis.Hookeapparentlysawwhathewantedtoseeamidstastormof

    instrumentalerror.Bradleyshowedthathisdatafittheaberrationtheorysowell

    thatanydifference,whichmightbeduetoannualparallax,wasprobablylessthan

    onehalfsecondofarc.ThismeantthatGammaDraconiswasmorethan400,000

    timesfartherfromusthantheSun.

    ItwasimpossibletomeasureparallaxusingHookesmethodwithoutfirstknowing

    aboutaberration.AsEq.2shows,theangulardisplacementduetoaberrationdoes

    notdependonthedistancetoastar.ButasEq.1shows,theparallaxangle

    decreaseswithdistance.SinceGammaDraconisisrelativelybright,andthusprobablynearby,itmightbeexpectedtohaveoneofthelargerparallaxes.Evenso,BradleyhadshownthataberrationcompletelyswampedparallaxforGamma

    Draconis,andformoredistantstarsthesituationwouldonlygetworse.Itwasonlybymeasuringtherelativemotionsoftwostars,closetogetherinourskybutfar

    apartinspace,thatastronomerslikeBessel,Struve,andHendersonwouldfinally

    measuretheannualparallaxofstarsinthe1830s.Thisdoublestarmethod,however,wouldnothaveledtothediscoveryofaberrationbecauseaberration

    affectsbothstarsequally.10

    Lessons

    ThereareseverallessonsthatcanbelearnedfromthestoriesofHookeand

    Bradley.11Hookesclaimtohavemeasuredparallaxshowsusthatreliable

    conclusionscannotbedrawnfromasmallnumberofmeasurements.Aconclusive

    demonstrationrequiresaseriesofmanymeasurements,allofwhichfitadefinite

    patternliketheoneestablishedbyBradley.Bradleysstoryalsoshowsusthat

    scientistssometimessucceedinunexpectedways.Bradleysoughttoconfirm

    Earthsorbitalmotionbydetectingannualparallax.Instead,heconfirmeditby

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    detectingandexplainingstellaraberration.Buthissuccesswasnotcomplete:a

    parallaxmeasurementwouldhavegiventhedistancetothestar,whilea

    measurementofaberrationprovidesnoinformationaboutstellardistances.

    Bradleystheoryofaberrationalsoshowsusthatgoodscientificexplanationscan

    drawtogetheruntestedhypothesestoexplainsomethinginawaythatgivessupporttoallofthehypotheses.NeithertheorbitofEarthnorthefinitespeedof

    lighthadbeenindependentlyconfirmedbefore1725(althoughNewtonsPrincipia

    hadleftlittledoubtaboutEarthsorbit),butBradleyshowedthathisdatawere

    easilyexplainedifbothofthesehypothesesweretrue.

    Finally,thesestoriesshowthatassigningcreditforadiscoveryistrickybusiness.Hookeclaimedtomeasureparallax,buthisclaimisnowdiscredited.Flamsteed

    measuredaberrationbutthoughthewasmeasuringparallax.Cassinirecognized

    thatFlamsteedwasmeasuringsomethingotherthanparallax,butitwasBradleywhoexplainedhisdataandthereforeiscreditedwiththediscoveryofaberration.

    TheactivitiesandcomputersimulationsinRef.3,whicharedesignedtoguide

    studentsthroughanexplorationofthishistoricalepisode,illustratetheseimportant

    lessonsaboutthenatureofscience.

    Figures

    Figure1:Parallaxofthemoon,viewedfromoppositesidesofEarth.NOTTOSCALE!

    2b

    d

    O1

    O2

    M1

    M2

    EarthMoon

    Celestial

    Sphere

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    Figure2:PredictedvariationinDeclinationresultingfromtheannualparallaxofGammaDraconis(magenta)andAlkaid(blue).Theamplitudeofthevariationis

    greatlyexaggeratedsoastobevisibleinthesimulation.

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    Figure3:Observednorthwarddeviationofstars.ThedatapointsshowHookes

    dataforGammaDraconis(blacktriangles)andBradleysdataforGammaDraconis

    (magentasquares)andAlkaid(bluetriangles).

    0"

    5"

    10"

    15"

    20"

    25"

    30"

    35"

    40"

    0" 0.25" 0.5" 0.75" 1"

    NorthwardDevia.on(''

    Time)of)Year)(years)from)Vernal)Equinox)

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    Figure4:Illustrationoftheaberrationeffect,showingthetelescopetubeTatthree

    differenttimes.Becausethetelescopemovesadistancevh/cduringthetimeit

    takeslighttotraveldownthetube,thetubemustbetiltedinthedirectionofmotioninorderforthelighttomovealongtheopticalaxisofthetube.SoastaratSwill

    appeartobeatS.

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    Figure5:PredictedvariationinDeclinationresultingfromaberrationforGammaDraconis(magenta)andAlkaid(blue).Theamplitudeofthevariationisgreatly

    exaggeratedsoastobevisibleinthesimulation.

    1ChristopherM.Graney,TeachingGalileo?GettoKnowRiccioli!WhataForgotten

    ItalianAstronomerCanTeachStudentsAboutHowScienceWorks,Phys.Teach.50,18-21(2012).2AlanHirshfeld,Parallax:TheRacetoMeasuretheCosmos(WHFreeman,2001).3Aself-containedJavaprogramcontainingallofthesimulationsisavailableat

    www.opensourcephysics.org/items/detail.cfm?ID=12029.The

    activityhandoutsareavailableassupplementarydocumentsonthesamepage.4HookeobservedgammaDraconisindaylight,aswellasatnight.Hemayhave

    beenthefirstpersontoobserveastarthroughatelescopeduringtheday.5RobertHooke,AnAttempttoProvetheMotionsofEarthbyObservations(London,

    1674).Availableonlineat

    http://www.roberthooke.com/motion_of_the_earth_001.htm.6

    M.E.W.Williams,FlamsteedsAllegedMeasurementofAnnualParallaxforthePoleStar,J.Hist.Astron.10,102-116(1979).7ThetelescopealsomovesduetoEarthsrotation,buttherotationalvelocityis

    about64timessmallerthantheorbitalvelocity,sotoagoodapproximationwecanignoretheeffectofrotation.InanycasetheeffectBradleywastryingtoexplainhad

    anannualperiod.

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    8Notethatafixedaberrationanglewouldbeundetectable.Foradiscussionofthis

    point,andhowaberrationrelatestospecialrelativity,seeThomasE.Phipps,Jr.

    Relativityandaberration,Am.J.Phys.57,549-551(1989).9JamesBradley,ALettertoDr.EdmondHalleyAstronom.Reg.&c.givingan

    AccountofanewdiscoveredMotionoftheFixdStars,Phil.Trans.35,637-661(1729).10IdliketothankCharlieHolbrowofColgateUniversityforthisinsight.11MichaelHoskin,StellarAstronomy:HistoricalStudies(ScienceHistoryPublications,

    1986),pp.29-36.