seeing earth's orbit in the stars
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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.