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Chapter2GravityintheSolarSystem
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TheSolarSystem,ingtheEarth,isourmostimmediatelaboratoryfthecesofgravity.ThegravitatioheSolarSystemisdomiheSun,whichisfarmoremassivethanas.
InorbitsthatarerelativelyclosetotheSuhefoursmallestplas:Merus,Earth,andMars.Furtherout,therearefourmuchlargerplaer,Saturn,Uranus,aheSolarSystemsaherobjects,suets,asteroids,moons,andman-madespacecraft.Bythemotios,andinsomecasesbyiingwiththem,weagreatdealaboutthebehaviravity.
&udyofexperimentalaionalgravityintheSolarSystemtookofidurierhalfofthe20thtury.Whileastronomershadbeentragthemotiosforturies,thedevelopmeeologiesahodsihturyallowedobservatiostobecarriedoutinwaysthathadneverpreviouslybeenpossible.Iryaheresultsofthisworkinsomekindofsensibleorder,Iwillclassifythemihatprobethefoundationalassumptionsofgravitytheories;experimentsthatprobeon’slaerimentsthatprobethesubtleefectsthatresultfromEiheory.
&ingfoundationalassumptions
Thereareanumberoffoundationalassumptionsthatgoiheravity.Theseihattherestmassofashouldbeisposition,aofitsmotioootherbodies.Otherassumptiohatthespeedoflightshouldbethesameiion,andthatallobjectsshouldfallatthesamerate(intheabsen-gravitationalforces).Overthecourseofthepastturyalltheseideashavebeeremelyhighaccuracy.I’lloutlihebestofthesetestshere,beforewemoveontothinkisthattesttheparticularsofoein’stheravity.
&ofbythinkingaboutmass.Recallthatmassisthequantitythattellsushowmuchforeedtoapplytoaiomakeitacceleratebyafixedamount.It’sthoughttobeapropertyoftheobjectitself.Thisisdifere,whichisthehedownwardsforobjectexertsonyourhandwhenyouholdit,andwhichwouldbediferentifyouheldthesameobjectwhilestandingo.Itismassthatappearsion’slawofgravity,anditismassthatwasshowtyiein’sfamousformula(E=mc2).Becausethesetwoequatioraltogravity,weohavesomeideaofwhetherornotthemassofareallyisispositionandmotioninagravitatiohislybedoally.
Oddlyeestofendsonpositionistolookathowlightgescolourasittravelsthroughagravitatiohebasicideabehihatphotons(particlesoflight)shouldlyastheyesthegravitationalfieldsofmassiveobjectssuchasstarsorplahisisbecauseittakeseopullsomethingupwardsthroughagravitationalfield.So,justasyouwouldhavetytorunupaflightofstairs,ittakesaphotoytotravelupwardsfromthesurfaceoftheEarth,orawayfromthesurfaceoftheSun.Aenergyofaphotosiscolour(itswavelength),andsoabeamoflighttravellingthroughagravitationalfieldshouldbeexpectedtohaveadiferentcolourdependingonhowfaritisabovethesourceofthatfield.Thisisthereasonwhylightdetectedfarfromthesurfaceofastarisfoulyredder,erihanitasemitted.Theefeowioingoflight.
So,howthegravitatioingoflightbeexpectedtotellusanythingaboutwhetherthemassofadependsonitspositioninagravitatiooahis,let’ssiderthemostdireeasuringthemassofainagravitatioingitupiheamouooktodoso.Thisenergyshouldbedirectlyrelatedtothemassoftheobject,stheeolifttheobjetwhtsshouldtellussomethiaboutitsmassat,ahosetwopositions.U’sdiculttoaccuratelymeasuretheamountyusedbyawinch,astheyteeiheygiveyi,aheropeandtheirowhisiswherethegravitatioingoflightesin.Thefrequencyoflightbemeasuredthpredtheeonslosebygoutofthegravitationalfieldisexpectedtobeexactlythesameasthatwhichwouldbeusedtoliftahamassthatdstothesameenergy(ascalculatedusingE=mc2).Ifwemeasuretheredshiftingoflight,wethereforehaveahighlyaccurateproxyexperiment,whichisexpectedtoveyexactlythesameinformationasthewi.
&desighegravitatioingoflighterformedforthefirsttimebythestistsRobertPoundaheearly1960s.TheyusedatowerattheJefersonPhysicalLaboratoryatHarvardUy,aheredshiftingofphotoravelledupitsheight.Theyfoundthatthelightdidindeedgecolourasittravelledupwards,andbyanamountthatwasentirelytwithmassbeiofposition.Theoionspossiblewouldhavetobesmallerthantheaccuracyoftheexperimentitself,whichwasatthelevelofabout1pert.AsimilarexperimenthassincarriedoutusiemittedfromtheSun,whichalsohadresultsthatweretwithmassbeiofposition,againatanaccuracyofabout1pert.
&ly,atomicclockshavebeeoprobethesameefect.Theideabehisisthatbeamsoflightarethemselves,insomesense,likeclocks.Thechtisdetermihewavelengthofthephotonsthatmakeupthelight,whichisitselfrelatedtothefrequencyatwhichtheyoscillate.Ifweweretotaketheseosstobethebasisofaclock,bysayingthateachosisooftime,thenweseethattheredshiftingoflightisequivalenttotheappearanceofclocksatdiferentpatdiferentrates.Ieveomeasurethefrequencyoflighttoperformthisexperiment,becauseifaclockbasedoionsofaphotoorunslow,thensomusteveryotherclock.Allwehavetodoisputtwoclocksattwhtsahemtotraheydisplayviaradiosignals.Thediferewhichtheyappeartotick,agtnalsthatareobserved,istheirelyequivalewhichalightsighemshouldberedshifted.
&hereforetaketwohighlyacicdputoneowhileleaviourfeet.Ifthetherosmitsitstimeviaradiosignals,thenarethissigimedisplayedbytheclockwekeptbesideus.Theyshould,inge:aknownasgravitatioiowascarriedoutforthefirsttimebyRobertVessotandMartinLevinein1976.Theyobservedthetimedilatioly,andfoundittobetwithmassbeiofpositiontoanaccuracyofabout1partin10,000(aboutahuimesmoreaccuratethantheHarvardexperiment).Thisexperimentthereforeprevidemassisiofpositioninagravitatiohaccuracy.
Movingonfrompositioispossibletostructexperimentsthattestwhetherthespeedoflight,orthemassofa,aredepeoheseexperimeoricallyveryimportant,becausebeforeEinsteiheravityitwaswidelybelievedthattherewasasubstaherthatpermeatedthewholeofspace.Theetherwasihemediumthroughwhichwavesoflighttravelled,andhysitilaslateasthe20thtury.Iftheetherexisted,thenthespeedoflightthatanobservermeasuredshoulddepeioravelledthroughit.Eiheoryisinpatiblewiththeexisteher,ashehadstructeditsothatallobserversmeasurethesamespeedoflight,iheirstateofmtestsfortheexisteherwasthereforeanimportantparthistheory.ThemostfamousofthesetestswastheMiorleyexperimein1887.Itisatesttoseeifthespeedoflightdependsoiation.
TheMiorleyexperimentusedadeviasaer,goftwoarms,builtatright-aher.Thisisillustratedifromalaserisshohearms,aedbaitselfbymirrorspositioheirehereflectedlightreachedtheiiowoarmsitwasallowedtoi.Aslightisknoropertiesofawave,itwouldbepossibletoletthetwobeamsoflightioformapattersofwavesiingonthesurfaceofapond).Theformofthepatternthatisprodutheierdepehofeas,atakesthelaserlighttotravelalohespeedoflightwasdiferedires,thenMiorleyshouldhaveseenthecesofthisbyusingtheirapparatus.
6.Aschematicdiagramofaer.Thebeamsplitterseparatesthelaserlightintotwobeams,eachofwhichisre’eirrhttheh,as,befdiretothedetector.
Miorley’sexperimenthada.Nodiferencewasobservedinthespeedoflight,asittravellediwodiferehisectedbymathetime,astheEarthosedtobeinmotiootheether.Iflightwasawaveihespeedoflightshouldhavebeeioonlyinalaboratorythatwasstationarywithrespecttotheether.Thiswasn’tthoughttobethecasefortheEarth,whichorbitstheSunataround30,000metrespersed.TheexperimentperformedbyMiorleyisthereforetakerongevidetheexisteher,andinfavourofaspeedoflightthatistrulythesameiion.Thiswasveryimportaein’stheory.
&hediredependenasswasgivesthatwereilyperformedbyVernonHughesandRoheearly1960s.Theseiorssideredtheelesthatexistwithinlithiumatoms,andthatorbitthevelocitiesofaroundamillioresperseow,thegravitatioioheseeledaheirimmediatee,isextremelysmall.Thisisbecauseeleshavesuymasses.isstillpossiblethtboundsonanypossiblediredepeheirmass.Thisisbecauseelesgiveoutphotoheyergylevelswithinatoms,ahesephotonshaveaveryspecificsetoffrequenastransitiohemassoftheelesdepeheirdireotiohisrecisepositioioresultedfromenergylevels.Carefulstudies,bybothHughesandDrever,foundhediredepehemassoftheeleelyhighaccuracy.
&’sheideaoftheUyofFreeFall.Rememberthatthisistheheideathatallobjectsfallatthesamerate,asdemalileo.ButGalileo’sexperiment,whilegr,robablynotveryaccurate(bymodernstandards).So,giventheenheUyofFreeFallforbothoeiherehassubsequeofeforttoverifyittothehighestpossiblelevelofaccuracy.Thishasnowbeendoneinanumberofdiferentes,inumerouslaboratoryexperimentsasace-basedobservations.
So,tosummarize,theresgoodevidenavarietyofdiferes,thatthemassofaisihitspositioionofitsmotion.Thereisalsevidehespeedoflightisthesameiion,andthatallobjectsfalluyatthesamerate.Thesearethefoundationalassumptionsunderwhi’saheorieswerestructed.Let’soexperimentsthataimtoiheoriesthemselves.
&hatprobeon’slaw
&hischapterwewillsiderthepredisofEiheory,whiotedtosupplantthatofon.Hothaton’sinversesquarelawofgravityisagoodenoughapproximatioeiodescribeawidevarietyofbothterrestrialandastronomiena.It’sthereforeverymuchworthwhiletestion’slawtoseeexactlyhowwellitdescribesgravity.Herewewillsidersomeofthemostimportahavebeenperformedsofar.
&laboratorytestoftheinversesquarelaerformedbyHetheehtury.dish’sexperimentmadeuseofatorsioheov’s(illustratedinFigure7).Uv’s,hoositioramassesiomakethetorsioe.Heputthesemassesclosetotheowereattachedtothetravitatioweeshangingfromthetorsioheextramassesthatdishintroduced,beiherateofrotatious.Theneulledatthemassesattachedtotheththegravitatioweenthem,ahebartorotate.Theresultsofdish’sexperimentthusallravitatioobeprobedoveradistances.Hefoundthatgravityoperatedonthesesawaythatwasentirelytwithon’sinversesquarelaerimehesesameideasonmuchsmallerdistancescales.
Thegesiion’slawofgravityioryariseprincipallyduetotheweakhegravitationalforparedtotheotherforature.Thisweakeveresidualelectricapieetotallyoverwhelmthegravitationalforgitimpossibletomeasure.Allexperimethereforeobepreparedwiththegreatestofdtheiricchargesthatshroughhavetobesedbyintrodugmetalshieldsthatreducetheirihismakesthestruoflaboratoryexperimeyextremelydidexplainswhywehavesofarravitydowlebelow1mm(thisparedtoaroundabillionthofabillionthofamillimetrefortheelectricforce).
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