erdistancescales,however,thereareavarietyofotherteststhatwemustsider。Toorderthedisofthesetestsseofallsiderdistaeres,uptoabouttoaboutafewkilometres。Thesescalesmayseemliketheyshouldbetheeasiesttoprobeastheyareclosesttothetypeofdistansiderinoureverydaylives。Theyare,however,quiteproblematic。
&hebesttsthathassofarbeenagravityovertheseeverydaydistancescalesisduetomeasuremeioaexperievariousheightsupatalltower。Towardstheendofthe1980s,ateamofstistsperformedthistestusire-highWTVDtarha。Thegravityexpeon’sinversesquarelawatdiferentpoioweriseasytocaldtheexperimeoodaccuracy。Atarouime,otherresearchersweremeasuriiohewaterinareservoirfilledtodiferentlevels。Ihisallowedthewatertobeweighedaon’sinversesquarelawofgravitytobetested。Furthertests,acoupleofyearslater,wereperformedbymeasuriionalattraofseawateratdifereheo。Theseexperimentsallproducedresultsthatweretwithon’sinversesquarelaw,andallatalevelofaccuracyofarou。
erscalesitstartstobeepossibletouseastronomicaldata,whichismuchmoreaccuratethantryihegravitatiohewaterinreservoirsaaweenamillionandafewhundredsofmillioresbeprobedbystudyisofmaesarouheorbitoftheMoosoftheplasarouheLAGEOSsatellites,laun1976and1992,areparticularlyusefulforexperimentsofthistype’asaretheorbitsoftheplas,whiclosedellipses(tofirstapproximatiohegravitationalattraisiveon’sinversesquarelaw。Observationsofallofthesebodies,as,haveshowhon’slawataccuraciesofbetweeinamillioinabillion。
&hereforehaveverygoodevideon’sinversesquarelaroximationtogravityoverawideraahesesgefromafraillimetre,tohundredsofmillioheaccuracyoftheexperimentsthatprobegravityoverthesedistancesvarieswildly,betartin1,000(forscalesofteoaboutoinabillion(fordistadtotheorbitsoftheplahisisagreatsuccess,butit’shestory。Let’son’slawandstartgthearisefromEiheory。
&hatprobeEiheory
&sdiscussedearlierhaveallisthatarefamiliartomostpeoplewhohavestudiedphysicsatschool:theass;theUyofFreeFall;aon’sinversesquarelawofgravity。Iion,Iwillisthatprobethemoreunfamiliargrouein’stheravity。Thespecificefectsthatresultfromthistheoryareoftensmallanddiculttodetectexperimeheless,theyareveryimportant,astheyprovideusthatbeusedtoviewaandgravityatadeeperlevel。
TherearealargenumberofefectsthatresultfromEiheoingtolimitmyselftfourofthem。ThesearetheanomalousorbitoftheplahebendinghtarouhetimedelaynalsastheypassbytheSun;andthebehaviyrosorbitarouhesearefourofthemostpromiicgravitatiobeobservedintheSolarSystem。Furtherefects,whieappareremeastrophysients,willbedisChapter3。
&withtheanomalousorbitofMercury。Earlieroninthisbook,IstatedthatheoryexplainedKepler’sobservatiosfollowellipticalorbitsarouhisistruefleplahingsstarttogetabitmorepliwesidertheorbitsofmultipleplaahisisbecausethereexistgravitatioweesthemselvesandnotjustbetlaheSunindividually。Theseiarygravitationalforcesaresmallerbutmeasurable,aheefectofpullisoftheplasofwhatmightotherwisebeperfectellipses。
Physicistshaveknownabouttheefeterplaarygravitationalftime。Theseforbeeasilycalculatedwithiheory,andastronomershavemeasuredtheirtheorbitsoftheplasforturies。Infact,theexisteunewasdeduthemid-19thturybycarefullystudyiofUratotheSuofUraurbedalittlefromwhereastroedittobe,aioncouldbeexplaiherewasaslightlylargerplalebitfurtheroutintheSolarSystem。UrbainLeVerrierandJohnsbothpredictedtheexistehisplain1845’andby1846ithadbeehiswasclearlyamomentousat。
Itthereforewasn’ttoomuchofasho,in1859,LeVerrieraheorbitofMercury(theplaheSuodeviatealittlefromthepaththatitectedtotake。Nodoubtbuoyedbyhispredioftheexisteune,LeVerrierpredictedthattheremustbeastillclosertotheSunthanMercury。Heeve’Vul。Thistime,however,thediscoveryofthepredietneveroccurred。Despitemuchefort,couldbeseeweenMerdtheSuheless,theanomalousorbitofMercurypersisted。ItseemedasifitsorbitwasbeingdraggedaroundtheSunbyagravitatiohadnoin。
&eryoftheanomalousorbitofMercurywassolvedin1915,notbythediscoveryofanynewmassivebodiesintheSolarSystem,butbyEinsteiioheory。Yousee,agtoEinsteiheory,theoniangravitationalforlyaroughapproximatioureofgravity。Aswellastheinversesquarelaw,Eihatthereshouldbenew,smallertributioionalforcelahysicalsystemdominatedbyalargemassatthetre,liketheSureoftheSolarSystem,Einsteincalculatedthatthelargestofthesenewforcesshouldvaryastheihedistaherefore,theeistotheSuhetributionfromthisnewforceshouldbe,relativetoon’sinversesquarelaw。
Mercurywas,andstillis,theowheSun,aeiationalfororeiialonMercury’sorbitthasofaherplas。
&eincalculatedthatMercury’sorbitshedaroundtheSura43ardspertury(1ardis1360ofadegree)。Thisisatinyamount,butitisenoughtobeobservedbyastroisalsotwiththeanomalousobservationsmadebyLeVerrier。SoEiheravityhaditsfirstobservationalsuccessasearlyas1915,byexplainingtheanomalousorbitoftheplaMercury。
ModersoftheorbitofMercuryaremuchbetterthaexistedihtury。theorbitsofalltheplahaccuracy,whichisessentialforgthedeviationofMeraradragcausedbyVenusalone,forexample,ismorethaoftheduetoEinstein’sgravity。Itspositionthereforeobeknhaccuracy。Thisissourtyinmoderionsthough。ThatdistiheuyassociatedwiththeshapeoftheSunitself。AionsfromaperfectlysphericalshapecauseefetheorbitofMercurythatcouldbefusedwithEinsteiatioheshapeoftheSunishardtokly,sothebestwetlydoistosaythattheanomalousorbitofMercuryistwithEiheorytoanaccuracyofabout1partin1,000。
&ionofMercury’sorbitisimpressivebutprobablydoesn’ttasapredi,becausetheanomalyitselfwasknownaboutloeinwasevenborn。WhatdoestasageioeihebendinghtaroundtheSunbyitsgravitatioreviouslyuailightshouldbeafectedbygravity,beewtravitationalforlybetweehavemass(whichlightdoesnot)。Thisambiguitywasremovedihehtsimplyfollowstheshortestpathsavailableinthecurvedspace-time,justlikeeverythihereforepredictedthatlightshouldbebeionalfieldsofmassiveobjects。
&ein’scalsshowedthatthedefleoflightwouldbegreatestforbeamsthatjustskimthesurfaassiveobjects。ThemostmassiveobjetheSolarSystemistheSun。ButthtthatpassesveryclosetotheSuforasolareclipse,otherwisetheSun’sownlightoverwhelmsthatofthemuterstars。ThefirstgoodopportuheideaofbendingstarlightcameaftertheendofWorldWarI,in1919。TheexpeditiohepositioarsheSuotestEiheravity,wasledbySirArthurEddington。
&oioheislandofPrínAfrica,wherethesolareclipsethatwasgoingtohappenthatyearwouldbetotal。Hemadecarefulmeasurements,usiographicplatesthatwereavailableatthetime。TheswerelessthaEddingtonsumeasuriioarsduringtheeclipse。Hefoundthattheyhadied,justasEinsteied,becausethetrajectoryofthelighthadbeehegravitatioheSuosweresuiEiheory,butonlywithinanaccuracyofarou。
On,moderionshaveimprovedthisresultdramatically。Thishasbeelybythefactthatthereare,tally,anumberhtobjeasquasars,whijusttherightpartoftheskytotestEinsteiiospassbehihede’eofthelightthattheyemitbemeasured。Severalmillioionsofthesequasarshavenowbeenmadeusingverylargebaseliers(thisisatypeoftelesixesthesignalsfromanumberofdifereocreateahigh-resolutioheresultofthisworkshowsperfesisteeialevelofaccuracyofabout1partin10,000。
AmoreretprediEiheoryisthetimedelaynalsthatpassbymassiveobjeereason,ittookuntil1964forstiststohisefeeeofEinstein’sgravity,butithasnowbeenmeasuredinanumberofdiferentsituations。ThesehaveiheobservatinalsthatbounetsastheyareabouttopassbehindtheSun,aswellasbylookingatthesignalsthatareemittedfromman-madeprobesastheydothesame。Thefirstofthesemethodshasthebehepositiosbeingverywellknowrajecteasytopredict。Thisstabilitymakesthemaget,buttheimperfetheirshapeeproblemsihere’eals。Man-madeprobes,oherhaveryeasilypredictablesignals,buttheirtrajectoriesewhatless。
RadietsthathavebeeomeasurethetimedelayefecludetheplasMerdVenus,andthespaariners6and7,Voyager2,theVikingMarsLanderaheiprobe。Themostredmostaccurate,oftheseobservationswasmadeusingi。TheprimarymissionofthisspacecraftwastoobserveSaturn,butitsrelevahestudyofgravitysbestservedin2003,whenitwasahadedtheexisteimedelayefeaccuracyof1partin100,000。Thisectaatioein’stheory,andonewhichwasachievedathigheraccuraypreviousexperiment。Thisart,duetotheobservationsnalsbeiiplefrequencies,whichallowedinterfereheSun’satobeextracted。
’smoveontothefiIwanttodisthisse:thebehaviyrosorbitarouh。Agyroscopeisessentiallyaspinningtop,whosetralaxisisallowedtopointiitoEiheravity,thereshouldbetwobeobservedeisputinorbitarouhefirstoftheseisadireofthegyroscope’saxisofrotation,asitorbitstheEarth。Thisefeasgeodeticpre,isduetothecurvatureofspace-timearouhesedefeing,aherotatiohefectivelypullingspadwithitasitrotates。Thisisaypeofgravitatioion,andsoitisofgreatioseeifitedexperimentally。
AlthoughtheprediiwasmadeonlyafewyearsafterEinsteinpublishedhisheravity,ittookuntilthe1960sbeforetheefegyrosorbitwascalculated,aalobservatiohemselvesdidnottakeplatilthe21sttury。TheLAGEOSsatelliteworkprovidedaionibymeasuringthetheorbitofitssatellitesastheywentarEarth。Thelong-awaitedgyroscopeexperimenterformedbyamissioyProbeB,in2011。Thegeodeticpredframe-draggisweremeasuredbythisexperimentwithaccuraciesofabout0。3perd20pert,respectively。TheaccuracyofthedisfromtheLAGEOSsatellitesareestimatedatbetert。Allresultswereonfoueein’stheory。
SotheoverallpictureweareleftwithisveryengforEiheravity。Thefoundationalassumptionsofthistheory,suchastheassandtheUyofFreeFall,havebeeremelyhighaccuraversesquarelawthatformedthebasisofheory,andwhichisagoodfirstapproximatioein’stheory,hasbeehesub-millimetrescaleallthetoastrophysicalscales。WearealsonowinpossessionofanumberofaccurateexperimehatprobethetihatresultfromEiheoryspecifically。Thisdataallowsusdirectexperimentalinsightiioteraureofspace-time,andallofitissoodagreemeeiions。Thisisatrulyspectaatiowasborofalmht。Eiedtomakeatheravitythatatibleeedoflightthatwasmeasuredtobethesamebyeveryobserver。Hedidso,andwehavehenumerouscesofhisrevolutioureoftheUniverse。
Thisishesth:Einstein’sgravityhasmaasequences,illdisthefollo