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Chapter 1 What is a black hole(第1页)

Chapter1Whatisablackhole?

Ablackhiohefravityissthatnothi,travelfastenoughtoesitsihoughtheywerefirstthefertileimaginatioicalphysicists,blackholeshaveifiedintheUheirhundredsandatedforintheirmillions。Althoughiheseobjeteractwith,andthusiheirsurroundingsinawaythatbehighlydetectable。Exactlywhattheiionisdependsonproximityrelativetotheblackhole:toodthereisfurtherafieldsomedramatidspectaomena>

&ermblackhole'wasfirstmentionedinprintinanartiEwingiingonasymposiumheldinTexasin1963,althoughsheionedwhoedtheexpression。In1967,AmeriphysiWheelerhandfravitationallypletelycollapsedstar'aopopularizetheterm,thoughtheceptofacollapsedstaredbyfellowAmerisRobertOppenheimerandHartlandSnyderba1939。Infact,themathematidationsofthemodernpictureofblackholesbeganratherearlierin1915,hysicistKarlSchwarzseimportaioein's(knownasthefieldequationsiheoryofRelativity)fortheisolatednmassinspace。

TwodecadeslaterintheUK,alittlebeforeOppenheimerandSnyder'swork,SirArthurEddingtonhadworkedoutsomeoftherelevaithetextofiingworkbytheIndianphysicistSubrahmanyandrasekharonenstostarswhehephysicalimplisofEddington'selytheassivestarswhentheyhaveusedupalltheirfueltoformblackholes,EddingtonhimselfproheRoyalAstronomicalSo1935asbeing‘absurd'。Despitetheapparentabsurdityofthenotion,blackholesareverymuchpartofphysicalrealitythroughalaxyandacrosstheUheradvancesweremadeiedStatesbyDavidFieinin1958,whoestablishedtheexistene-waysurfadingablackholewhosesigweshallstudyintheingchaptersisimmeehissurfa'tallowlightitselftobreakfreefromthepravitationalattrawithinandisthereasonwhyablackholeisblack。Tobegiandhowthisbehavihtariseweofirstuandaprofouhephysicalworld:thereisamaximumspeedatartiyobjetravel。

Howfastisfast?

Alawofthejuifyouwanttoescapeapredatoryouorunfast。Unlessyouhaveexalouflage,youwillonlysurviveifyouareswift。Themaximumspeedwithwhichamammalespleasantsituationdependsonplexbiochemicalrelatioweenmass,musgth,aabolism。ThemaximumspeedwithwhichthemostrapidlytravelliyintheUravelisthatexhibitedbyparticlesthathavenomassatall,suchasparticlesoflight(knohotons)。Thismaximumspeedbegivenverypreciselyas299,792,458metrespersed,equivalentto186,282milespersed,roagamillioerthanthespeedofsoundinair。IfIcouldtravelatthespeedoflight,Iwouldbeabletotravel

frommyhomeioAustraliaieenthofased,barelytimetoblink。LighttravellingfromourheSueightmiraveltous。Fromouroutermostpla'sajourafewhoursforaphototheSulight-minutesawayfromEarthau-hoursawayfromus。ThishastheiihatiftheSunstoppedshiningorifuurnedpurple,hdoutaboutsuchimportantinformatihtminutesorafewhoursrespectively。

&'snowsiderhowfastlighttravelfromevenmoreimmeantpointsioEarth。TheMilkyWay,theGalaxyinwhichourSolarSystemresides,isafewhuhousandlight-yearsacross。ThismeansthatlighttakesafewhuhousaravelfromoheGalaxytotheother。TheForheerofgalaxiestothelalaxies(ofwhichtheMilkyWayisasignifitmember)andishundredsofmillionsoflight-yearsawayfromus。Thus,anobserveroingastarinagalaxywithintheFornaxclusterlookingbackthtnowmight,ifequippedriateiion,seedinosaurslumberingarouh。However,itisonlythemind-boggliheUmakesthemotionoflightlooksluggishandtime-ing。Theroleofthespeedoflightasamandatoryupperlimithasanintriguiwheosiderhowtolauospace。

Escapevelocity

NowsupposesomedisasteroccurswiththeresultthattheentiremassoftheEarthwereshrunktoapoint,havingnospatialextentwhatsoever。Wecallsuobjegularity。Ithasmass',amassiveobjectthatoccupieszerovolumeofspace。Ataverysmalldistanetreawayfromthissingularity,theescapevelouchlargerthanitwasat1,600km(andinfactwouldbeabout10%ofthespeedoflight)。Closertothesingularitystill,justureawaytheescapevelocitywouldbeequaltothespeedoflight。Atthisdistaitselfwouldnothavesuffitspeedtoescapethisgravitationalpull。Thisisthekeyideatouandhowblackholeswork。

Itiswuseularity'。Wedoattheendpointofaggravitationalcollapsethemattergoesdowritbutratherthatourclassicaltheravitybreaksdoweraquantumregime。Fromhereon,wewillusethetermsingularitytorefertothisultra-dee。

&horizon

Nowimagironautflyiandthatyouareapproagthissingularity。Whilestillatsomedista,youcouldalwaysthrioreverseafromit。Buttheclet,theharderadigbees。Eventuallyyoureachadistanwhichitisimpossibletoesatterhowpowerfulyihisisbecauseyouhavereachedtheeventhorizoically-definedsphericalsurface,whichisdefiheboundaryinsideofwhichtheescapevelocitywouldexceedthespeedoflight。Fht-experimehcollapsedtoapoint,thissurfacehereofradiusorewiththesingularityatitstre,easyenoughperhapsforourspacecrafttoavoid。However,theeventhorizonbeuchlargerwhentheblackholeisformedfromacollapsedstarratherthanacollapsedplahorizonhasanimportantphysisequence:ifyouareonthatsurfasideit,thelawsofphysicssimplywon'tallowyoutoescapebecausetodosoyouwouldobreaktheuniversalspeedlimit。Theeventhorizonisamandatorylevelofdemar:outsideityouhavefreedomtodetermii,andyourfutureremainsunalterablylockedwithin。

TheradiusofthissphericalsurfaamedinhonourofKarlSchwarzsentionedearlier。WhileasoldierinWorldWarI,Schwarzschildprovidedthefirstexactsolutioein'sfamousfieldequationsthatunderpiivity。TheSchwarzschildradiusiswrittenasRS=2GMc2whereMisthemassoftheblackhole,Gison'sgravitationalt,andcisthespeedoflight。Usingthisformula,theSchwarzschildradiusoftheEarthesouttobejusture。Similarly,theSchwarzschildradiusoftheSunisfoundtobe3km,meaningthatifthemassofourSuncouldallbesquashedintoasingularity,thenatjust3kmawayfromthispointtheescapevelocitywouldbeequaltothespeedoflight。AblaebilliontimesmoremassivethantheSun(i。e。havingamassof109solarmasses)wouldhaveaSchwarzschildradiusonebilliontimeslarger(theSchwarzschildradiusofapointmassthatisnsimplyscalesdirectlywithitsmass)。AsIdesChapter6,suchmammothblackholesarebelievedtobeattheanygalaxies。

Thisdesoftheeventhorizonbereasonablythoughtofwithionianphysideed,physititiesresemblingblackhiuriesbeforeEihersprofoundlygedofspadtime。Theprinkerswhoimagineddarkstars'thatresembleblackholeswereJohnMidPierre-Simoingbathe18thtury,andIwillnowexplainwhattheydid。

&heremarkablethingsaboutastronomyishowmudiscoverabouttheUniverseevenwheuetEarth。Forexample,nohumanbeiedtheSuhepreseheSuhelate19thturybyanalysirumofsunlight。Thisisparticularlyremarkableasthisstitutedthediscoveryoftheelemeself;itwasfoundontheSunldeteEarth。Evehe18thtury,someoftheideasbehindblackhined,andinparticulartheideaofwhatiscalledadarkstar。Thepersohefirstimaginativeleapwasverymuchaprodue。

JohnMichell

TheGeianerawas,inEnglaivepeaglishCivilWarwaslo,andEnglandhadbeealaivedomestiquillity(theriseofNapoleoillsomewayoff)。Likehisfatherbeforehim,theReverendJohnMichell(Figure1)receivedauyedudeheChurgland。AsareThorYorkshire,Michellwasabletouehisstificresearch,followinguphisisingeology,magism,gravity,light,andastronomy。Inonwithotherstistswithetime,suchastheastronomerWilliamHersdthephysirydish(ersonalfriend),Michellwasabletoridethewaveofthehinking。SirIsaahadrevolutiohewayinwhiiverseerulatinghislawofgravitationwhiedtheorbitsoftheplaheSolarSystemasbeihesameforcethatcausedhisfamousappletodropfromthetree。

1。JohnMiath。

&onianideasallowedtheUudiedusiidthisfreshbreedofstistswasabletodeploythisnovelworld-viewifields。Michellarticularlyedtousehihedistaarsbyusisofthelighttheyemitted。Hecameupwithvariousschemestodothis,byrelatingastar&#htscolour;healsosideredbinarystars(pairsravitationallybouher)aalmotionscouldgiveusefuldynamiichellalsoiarstendtoparticularareasofthesky,testingthisagainstarandomdistributionandinferringgravitationalg。heseideasracticableatthetime:fewbinarystarswereknown(thoughHerschelrodupressivecataloguesofvariousdoublestarsas)aioweenastar&#htscolourturobenotquiteasMichellhadthoughtitwas。heless,MichellwasstrainingtodoforthewiderUoheSolarSystem:allowastifial,anddynamialysisofobservationstoprovidenewinformationabouttheproperties,masses,anddistaheheavenlybodies。

&isightthatichellfollowedfromtheideathatparticlesoflightare,inMichell'swords,attrathesamemannerasallotherbodieseareated;thatis,byfthesameproportiontotheirvisiiae[bywhitmass],ofwhichthereoreaso,gravitationbeing,asfarasweknow,orhaveaobelieve,anuniversallawofnature'。Suchparticlesemittedfrestarwould,hereasoned,besloweddowionalattraofthestar。ThusthestarlightreagEarthwouldbeslower。onhadshownthatlightslowsdowninglass,andthisexplaiheprincipleofrefra。Ifstarlightwasindeedsimilarlyslowed,Michellarguedthatitmightbepossibletodetectthisslowingbyexaminingstarlightthroughaprism。Theexperimentwastried,notbyMichell,butbytheAstronomerRoyal,theReverendDrNevilMaskelyne,wholookedforthediminishiabilityht。dishwrotetoMithatithadn'tworkedandthatthereisnotmuchlikelyhood[sidinganystarswhoselightissensiblydiminished'。Michellwasdismayed,butsuicalspesrequiredmugofimpoarlightaffectedbythegravitationalattraofthestarfromwhichitisemitted?Michell'tbesure。Buthewasboldenoughtomakeaiion。

Ifastarwassuffitlymassive,andgravityreallydidaffectstarlight,theionalforcecouldbesuffittoholdbacktheparticlesoflightpletelyahemfromleaving。Suobjectwouldbeadarkstar。Thislittle-kingioryinYorkshirehadthusbeepersontoceiveofablackhole。However,sofarMichell'srammethedistaarslayiwasmore,hishealthhadbeeandthishadstoppedhimusinghistelescope。dishwrotetohimagletter:ifyourhealthdoesnotallowyoutogooelesayatleastpermittheeasierandlesslaboriousemploymeheworld。'Thissingularexampleofajokefromdish(whowasnotoriouslybuttooaMichellhadceived。Weighingtheworld'meainwhichtweleadspheresateitherendofthebeamofatorsioractedbytwostationaryleadspheres。ThisallowsohestrengthofthegravitatioherebyioftheEarth。Noohisbefore。Michell'sideawasbrilliant,buthedidn'tlivetopletetheprojestead,Michell'sexperimenterformedbydishandisnowknownasdish'sexperiment。Thistransferofcredittodishismorethaedforbythenumerhsmadebydishwhieglectedtopublishatributedtosubsequentresear's'lawandb's'law)。

Pierre-SimonLaplace

OhersideoftheEnglishel,Pierre-SimoeranquilidyllaffordedbythepeacefulperiodoftheEe。LaplacelivedthroughtheFreion,thoughhiscareerprosperedasheihenewlyfouutdeFrahe恈olePolyteique。HeeveaperiodasMiheInteriorunderNapoleon,ashort-livedappoiheEmperorcametret。NapoleoLaplacewasafirst-ratemathematibutasanadministratorhewasworsethanaverage。erwroteofLaplacethathesoughtsubtletieseverywhere,lyproblems,andfinallycarriedthespiritof"infinitesimals"iration'。heradministratorsto,buttheworldhashadfewmathematisasprodudinsightfulasLaplace。Hemadepivotaltributiory,probability,mathematics,celestialmeiy,andphysics。Heworkedontopicsasdiverseascapillaryaets,inductivereasoning,solarsystemstability,thespeedofsouialequations,andspheriieoftheideashesideredwasdarkstars。

In1796LaplacepublishedhisExpositiondusystèmedumoeedpublic,thisbookdescribesthephysiwhiyisbased,thelawofgravityaiosintheSolarSystem,andthelawsofmotionandmeics。Theseideasareappliedtovariousphenomena,ingthetidesandthepreoftheequihebookalsosLaplace'sspesinoftheSolarSystem。Oicularpassageisofspecialrelevaoourstory。Laplacemadeacaleah-likebodywoulditsescapevelocitywasequaltothatoflight。Heshowed,quitecorrectly,thatthegravitatithonthesurfaceofastar,withdensityparabletothatofEarthbutwithadiameterofabout250timesthatoftheSun,wouldbesoievenlightwouldbeabletoescape。Thus,hereasobodiesintheUhereforebeiheystillbelurkiableinthedarknightsky,whileweimagiheonlythingsoutthere'werethebrightlumiwesee?TheHungarianastronomerFranzXavervohatLaplaceprovidethecalsthatledtothis,andLaplacethisup(inGermahejournalsthatvoed。

Holacewasbeihewavetheht。BothMichell'sandLaplace'sideasartonthecorpusculartheht。Iflightweretosistoftinypartiitseemedreasoheseparticleswouldbeaffectedbyagravitationalfieldandwouldbebouarofsuffitsize。Buttheearly19thturysawanumberofexperimentswhichseemedtogivegreatercetothewavetheht。Iflightwereinsteadawave,thenitwashardertoseethatitshouldbeaffectedbygravity。Laplace'sdarkstarprediwasquietlyomittedfromlatereditioiondusystèmedumoerall,MidLaplacehadbeeuringandexpltheory,ratherthanbeiheoexplaiionsandthus,thisideawasfottenforawhile。TheobjeedbyMidLaplacewerethusdarkstars',enormousobjetheUniversewhichbyvirtueoftheirmasscouldsustaiemsbutbyvirtueofthissamebulkotbeobservedviatheradiationoflight。Starlightemittedfromthesurfaichell'sandLaplace'sdarkstarswouldbetoosluggishtooveretheintensesurfacegravity。WhatMidLaplaothaveguessedwasthatsutuanaasswouldbeuooreover,intheircollapsetheywouldpuheveryfabricofspadtimeaoasingularity。Thusblackholes'arenotdarkstars'aheargumentfihtheastronomicaldiscoveryofblackholeswewillfirstouhenatureofspacetime。

&ime

OureverydayexperienceleavesusfortablewiththenotioangibleUniversemaybedescribedbyoemporal(ortime)atetaialates(forexamplex,y,andzalouallyperpendicularaxes,astrutedbyReesandknownasates)。IeinpublishedhisrevolutionarypaperonSpecialRelativity,therelativityofmotionandstationarity。In1907,HermannMinkotheseresultscouldbeuoodmoredeeplybygafour-dimensioimewhosepoints,speowbythe4-Date(t,x,y,z),dto‘events'。Aissomethingthathappensataparticulartime(t)andataparticularplace(x,y,z)。Such4-DatesinwhatisknownasMinkoecifyexactlywhereandwheostein'sspecialtheoryofrelativitycouldbeformulatedintermsofMinkowski'sspadprovidesatdesofphysicalprodifferentframesofreferemoverelativetooher。Aframeofreference'issimplytheperspectivepossessedbyaparticularobserver。Einsteiheoryspecial'becauseitdealsonlyarticularamelyrefereareiialframesofreferehespecialtheorylybeappliedtouniformlymoving,ed,framesofreference。Ifyoudropastoround。TheframeofrefereachedtothestoneisaingframeofreferenedbyEinstein'sspecialtheory。Whereyouhavegravity,youhaveac。

ThisdratedEioformulateageheoryofrelativity,whichhepublishedadecadeafterhisspecialtheory。Whathefoundwasthatwhereasspakowskispacetimewererigidframeworksinwhichobjectslive,moveaheirbeing',spacetimewasactuallyamorerespocouldbedotherwisedeformedbythepresenass。Oncemassispresentinaphysicalsituatiohefollowirikedbehaviourdescribesreality,lysummarizedbyJohnWheeler:

·massaspacetime,tellingithowtocurve!

·spacetimeaass,tellingithowtomove

ThisbehaviourisquantifiedbyEinstein'sfieldequationswithiivity,whichrelatethecurvatureofspacetimetothegravitationalfield。

Physiciststalkaboutagravitatioialwellassurroundingamassiveobject。TheshowninFigure2ehespacetimeisdistortediyofacoupleofblackholes,whereeaberegardedasawaywhichisdirectlyrelatedtoitsmassahegravitatioself。Thesingularityiimemayberegardedaswherethecurvatureiimebeesveryhighandyougobeyondtheclassicaltheravity,iumregime。Theevenththesingularityfunsasaone-

2。Thedistortioure,iimeduetothepresenasses。

membraidphotoheblaoutsidebutnothingeswithinthehorizonoftheblackholeouttotheexternalUmassisnottheoablaaypossessandbemeasuredby。Iftheblackh,thatistosayitpossessessomespin,theneveremebehavies。Beforeweexamiakealittledetourtolearnalittlemoreabouthowwemayschematicallyrepreseself。

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