Chapter2GravityintheSolarSystem
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)。
&hreegroupsofexperimehaveledthewayinlaboratorytestsofgravityiimes:oheUyofWashingtoheUyofColorado,andathirdatStanfordUheWashingtongrouptookapendulumwithteoitaoveradiskthatedaofholes。Thependulumwasfoundtotwistduetothemissinggravitatiohemissingmassihisallowedgravitytobemeasureddowntoscalesassmallasatwehofamillimetre。ThegroupsatColoradoandStanford,oherhahegravitationalfieldmass,ahisinformatiravityallthewaydownto140ofamillimetre。Theresultsoftheselaboratoryexperimentshavesofarallbeeirelytwithon’sinversesquarelawofgravity,evenontheverysmallestofscales。