第76章 对火星轨道变化问题的最后解释(10/12)
rationlenh.>
ealyantoeachofthedatafragments,andobtainnfrequencydiagrams.>
neachfrequencydiagramobtainedabove,thestrenhoferiodicitycanberelacedbyagrey-scale(orcolour)chart.>
eerformtherelacement,andconnectallthegrey-scale(orcolour)chartsintoonegrahforeachintegration.hehorizontalaxisofthesenegrahsshouldbethetime,i.e.thestartingtimesofeachfragmentofdata(ti,herei=1,…,n).heverticalaxisreresentstheeriod(orfrequency)oftheoscillationoforbitalelements.>
ehaveadotedanbecauseofitsoverhelmingseed,sincetheamountofnumericaldatatobedeosedintofrequencyonentsisterriblyhuge(severaltensofbytes).>
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tyicalexamleofthetime–frequencymacreatedbytheaboveroceduresisshoninagrey-scalediagramasig.5,hichshosthevariationoferiodicityintheeentricityandinclinationofarthin+2integration.nig.5,thedarkareashosthatatthetimeindicatedbythevalueontheabscissa,theeriodicityindicatedbytheordinateisstrongerthaninthelighterareaaroundit.ecanrecognizefromthismathattheeriodicityoftheeentricityandinclinationofarthonlychangesslightlyovertheentireeriodcoveredbythe+2integration.hisnearlyregulartrendisqualitativelythesameinotherintegrationsandforotherlas,althoughtyicalfrequenciesdifferlabylaandelementbyelement.>
4.2ong-termexchangeoforbitalenergyandangularmomentum>
ecalculateverylong-eriodicvariationandexchangeoflaaryorbitalenergyandangularmomentumusingfilteredelaunayelements,,.andareequivalenttothelaaryorbitalangularmomentumanditsverticalonenterunitmass.isrelatedtothelaaryorbitalenergyerunitmassas=?μ222.fthesystemisletelylinear,theorbital
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