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对火星轨道变化问题的最后解释

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    作者君在作品相关中其实已经解释过这个问题。

    不过仍然有人质疑——“你说得太含糊了”,“火星轨道的变化比你想象要大得多!”

    那好吧,既然作者君的简单解释不够有力,那咱们就看看严肃的东西,反正这本书写到现在,嚷嚷着本书bug一大堆,用初高中物理在书中挑刺的人也不少。

    以下是文章内容:

    long-teraryorbitsinoursolarsystem

    abstract

    ,atleastinoursis,±5x–plutosystemhavebeenmaintainedoverthe1011-yrtime-span.

    1introduction

    thequestionofthestabilityofoursolarsystersystem.

    admp;amp;boss1996;itoamp;amp;tanikawa1999).,about±,.ofcoursethisstatementcannotbesimplyappliedtosystemswithstableorbitalresonancessuchastheneptune–plutosystem.

    inadditiontothevaguenessoftheconceptofstability,theplanetsinoursolarsystearysystesforaperiodcoveringseveral10gyrtothoroughlyunderstandthelong-teraryorbits,sincechaoticdynamicalsystemsarecharacterizedbytheirstrongdependenceoninitialconditions.

    fros,whichcoveraspanof~,butitseesalsoreroscillations.

    ontheotherhand,inhisaccurateses,especiallyofskar1996).theresultsoflaskarssecularperturbationtheoryshouldbeconfirmedandinvestigatedbyfullynumericalintegrations.

    inthispaperwepresentpreliaryorbits,coveringaspanofseveral109yr,andoftwootherintegrationscoveringaspanof±5x,,atleastoveratiaryorbitaleleunayelermomentumdeficit,andresultsofoursimpletime–frequencyanalysisonallofourintegrations.

    insection2webrieflyexplainourdynasthatspans±5x.

    2descriptionofthenumericalintegrations

    (本部分涉及比较复杂的积分计算,作者君就不贴上来了,贴上来了起点也不一定能成功显示。)

    weutilizeasecond-orderwisdom–holmansymplecticmapasourmainintegrationmethodwithaspecialstart-upproceduretoreducethetruncationerrorofanglevariables,‘warmstart’.

    thestepsizeforthenuparetheseintegrationssimplyintermsofstepsizes.

    intheintegrationoftheouterfiveplanets,wefixedthestepsizeat400d.

    weadoptgaussfandgfunctionsinthesymplecticmaptogetherwiththethird-orderhalleymethodsmethodis15,buttheyneverreachedthemaximuminanyofourintegrations.

    theintervalofthedataoutputisdforthecalculationsofallnineplanets,andaboutdfortheintegrationoftheouterfiveplanets.

    althoughnooutputfilteringwasdonewhenthenumericalintegrationswereinprocess,.

    accordingtooneofthebasicpropertiesofsyrngulartiveerrorintotalenergybyaboutoneorderofmagnitudeormore.

    relativenungularngularmomentum,respectively,.

    notethatdifferentoperatingsysternungularmomentum,whichshouldberigorouslypreserveduptomachine-eprecision.

    sincethesyparethetestintegrationwiththetedtothevalue~8700°,about25rotationsofearthafter5gyr,,thelongitudeerrorofplutocanbeestimatedas~12°.thisvalueforplutoismuchbetterthantheresultinkinoshitaamp;amp;nakaiwherethedifferenceisestimatedas~60°.

    3numericalresults–

    :noorbitalcrossingsnorcloseencountersbetweenanypairofplanetstookplace.

    first,,orbitalpositionsoftheterrestrialplanetsdifferlittlebetweentheinitialandfinalpartofeachnuaryorbitalmotionremainnearlythesameastheyareatpresent.

    verticalviewofthefourinnerplanetaryorbitstheinitialpartofn+1.thefinalpartofn+1.theinitialpartofn?1.thefinalpartofn?1.ineachpanel,x.

    thevariationofeccentricitiesandorbitalinclinationsfortheinnerfourplanetsintheinitialandfinalpartoftheintegrationn+,thecharacterofthevariationofplanetaryorbitaleles;s,.

    theorbitalsseeroverthistime-span.

    –frequencymaps

    althoughtheplanetaryrlyinthecaseofearth,canpotentiallyhaveasignificanteffectonitssurfaceclirinsolationvariation().

    togiveanoverviewofthelong-teraryorbitalskarsfrequencyanalysis.

    .

    eachfragrgeoverlappingpart:forexample,whentheithdatabeginsfromt=tiandendsatt=ti+t,thenextdatasegmentrangesfromti+δt≤ti+δt+t,whereδt?+treachesthetotalintegrationlenh.

    weapplyanffttoeachofthedatafragments,andobtainnfrequencydiagrams.

    ineachfrequencydiagracedbyagrey-scalechart.

    weperforcexisrepresentstheperiodoftheoscillationoforbitalelements.

    wehaveadoptedanfftbecauseofitsoverwhelposedintofrequencyponentsisterriblyhuge.

    atypicalexabyplanetandelementbyelement.

    wecalculateverylong-periodicvariationandexchangeofplanetaryorbitalenergyandangularunayelementsl,g,=?,,suchasymptomofinstabilityisnotprominentinourlong-termintegrations.

    ,thetotalorbitalenergyandangularponent,g0,,.

    cosandallnineplanets,itisapparentthattheasares::,,wecannotneglectthecontributionfros,aswewillseeinsubsequentsections.

    +1andn?,,,wecanseethatarysubsystem.

    itisnotclearatthearyorbitalenergy.hence,theeccentricitiesofvenusandearthcanbedisturbedeasilybyjupiterandsaturn,,–earthpair,whichresultsinanegativecorrelationintheexchangeoforbitalenergyinthepair.

    asfortheouterjovianplanetarysubsysteparedwiththatofthevenus–earthpair.

    5±5x1010-yrintegrationsofouterplanetaryorbits

    sincethejovianplanetaryarys.,thetypicalfrequencyoftheorbitaloscillationofplutoandtheotherouterplanetsisalmostconstantduringtheseverylong-termintegrationperiods,whichisdemonstratedinthetime–frequencymapsonourwebpage.

    inthesetwointegrations,therelativenungularmomentumwas~10?10.

    –plutosystem

    kinoshitaaaryorbitsover±x,,λdenotesthemeanlongitude,Ωisthelongitudeoftheascendingnodeand?.

    rgumentθ1=3λp?2λn??plibratesaround180°withanamplitudeofabout80°andalibrationperiodofabout2x104yr.

    theargumentofperihelionofplutowp=θ2=?p?Ωplibratesaround90°x.

    thelongitudeofthenodeofplutoreferredtothelongitudeofthenodeofneptune,θ3=Ωp?Ωn,,,theinclinationofplutobecoeses90°.whenθ3becoeseses90°;aterconfirni,nobiliamp;amp;carpino.

    anargumentθ4=?p??n+3libratesaround180°withalongperiod,~x108yr.

    inournurgurduringthewholeintegrationperiod.however,thefourthresonanceappearstobedifferent:thecriticalargutionovera1010-yrtime-scaleshorterintegrationswerenotabletodisclose.

    6discussion

    whatkindofdynaarysystearysystearysubsystearyseparationsbythesaregreaterthan26rh,,,.

    ,thewideseparationandsrendersthedisturbanceineffective;thedegreeofdisturbancebyjovianplanetsiso.heighteningofeccentricity,forexampleo~,.

    althoughournursystem,.

    ——以上文段引自ito,;tanikawa,,483–500

    这只是作者君参考的一篇文章,关于太阳系的稳定性。

    还有其他论文,不过也都是英文的,相关课题的中文文献很少,那些论文下载一篇要九美元(《nature》真是暴利),作者君写这篇文章的时候已经回家,不在检测中心,所以没有数据库的使用权,下不起,就不贴上来了。
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