ies(cf.brouwerboccalettipucacco1998).thismeansthattheplanetaryorbitalenergy(whichisdirectlyrelatedtothesemimajoraxisa)mightbemuchlessaffectedbyperturbingplanetsthanistheangularmomentumexchange(whichrelatestoe).hence,theeccentricitiesofvenusandearthcanbedisturbedeasilybyjupiterandsaturn,whichresultsin'itivecorrelationintheangularmomentumexchange.ontheotherhand,thesemimajoraxesofvenusandeartharelesslikelytobedisturbedbythejovianplanets.thustheenergyexchangemaybelimitedonlywithinthevenus–earthpair,whichresultsinanegativecorrelationintheexchangeoforbitalenergyinthepair. asfortheouterjovianplanetarysubsystem,jupiter–saturnanduranus–neptuneseemtomakedynamicalpairs.however,thestrenhoftheircouplingisnotasstrongcomparedwiththatofthevenus–earthpair. 5±5x1010-yrintegrationsofouterplanetaryorbits sincethejovianplanetarymassesaremuchlargerthantheterrestrialplanetarymasses,,weaddedacoupleoftrialintegrationsthatspan±5x1010yr,includingonlytheouterfiveplanets(thefourjovianplanetspluspluto).theresultsexhibittherigorousstabilityoftheouterplanetarysystemoverthislongtime-span.orbitalconfigurations(fig.12),andvariationofeccentricitiesandinclinations(fig.13)showthisverylong-termstabilityoftheouterfiveplanetsinboththetimeandthefrequencydomains.althoughwedonotshowmapshere,thetypicalfrequencyoftheorbitaloscillationofplutoandtheotherouterplanetsisalmostconstantduringtheseverylong-termintegrationperiods,whichisdemonstratedinthetime–frequencymapsonourwebpage. inthesetwointegrations,therelativenumericalerrorinthetotalenergywas~10?6andthatofthetotalangularmomentumwas~10?10. 5.1resonancesintheneptune–plutosystem kinoshitanakai(1996)integratedtheouterfiveplanetaryorbitsover±5.5x109yr.theyfoundthatfourmajorresonancesbetweenneptuneandplutoaremaintainedduringthewholeintegrationperiod,andthattheresonancesmaybethemaincausesofthestabilityoftheorbitofpluto.themajorfourresonancesfoundinpreviousresearchareasfollows.inthefollowingdescription,λdenotesthemeanlongitude,ΩisthelongiM.XIApe.cOM