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Describing the Components of the Water Transport in the Martian Atmosphere PDF

2 Pages·2003·0.04 MB·English
by  MontmessinF.
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Preview Describing the Components of the Water Transport in the Martian Atmosphere

Third Mars Polar Science Conference (2003) 8089.pdf DESCRIBINGTHECOMPONENTSOFTHEWATERTRANSPORTINTHEMARTIANATMOSPHERE..F.Montmessin, R.M.Haberle,NASAAmesResearchCenter-MoffettField,F.Forget,LaboratoiredeMeteorologieDynamique-France,P.Rannou, M.Cabane,Serviced’Aeronomie-France. Introduction: Inthispaper,weexaminethemeteorolog- andmid-latitudesprecedestheincorporationofwaterwithin icalcomponentsdrivingwatertransportintheMartianatmo- theascendingbranchoftheHadleycellinthenortherntropics. sphere. Aparticularemphasisisgiventotheroleofresidual Likewise,themechanismbywhichwaterreturnstothenorth meancirculationandwatericecloudsindeterminingthegeo- residualcapincludeswatertrappingintheseasonalCO cap, 2 graphicalpartitioningofwatervaporandfrost. thankstoanintensemixingofairmassesacrossthecapedge. Modeldescription: Foroursimulations,weusetheGen- Duringtherecessionofthecap,seasonalwaterfrostiscarried eralCirculationModel(GCM)developpedatLaboratoirede polewardbyasuccessionofsublimation/recondensationpro- MeteorologieDynamique(Paris/France)[1]tosimulateMar- cesses occuring within poleward warm fronts and equatorial tianhydrologicalcycleforvariousorbitalconfigurations. The coldfronts. model includes usual representations of processes like sur- With this in mind, describing water transport in terms of its facesublmation,cloudformationandsedimentation(withpre- meteorological components becomes a necessary task in or- dictedcloudparticlesizes)[2]. Mostofoursimulations dertofullyappreciatethemechanismscontrollingtheMartian Watercycleandcirculation: Usingthesamedecompo- watercyclestability. sition as that found in [3], it is possible to recast the water Results of our analysis on an annual average and at specific transport in terms of circulation components. Indeed, it is seasonswillthusbepresented. staightforwardtodemonstratethatthetotalmeridionaltrans- Watercycleandclouds:Followingtheirfirstobservation portofatracerspeciesincludesthecontributionofthemean ofwhathasbeensincecalledthe"Aphelioncloudbelt",i.e. a meridionalcirculation,thatoftransienteddiesandthatofsta- cloudystructureencirclingtheequatorduringnorthernspring tionarywaves. andsummer,[7]proposedamechanism,involvingclouds,to Followingthisapproach,weexpressthetotaltransportofwa- predict preferred storage location of water with changes of tervaporatagivenlatitudeandatagivenheightas[q¯v],where periheliondate. Theso-calledClancyeffectcomesfromthe theq¯vsymboldenotesthetimeaverageand[]symbolsdenotes potential ability of clouds to sequester water below the re- thezonalmeanoftheproductqv,qbeingthemassmixingra- turning branch of the equinoctial Hadley cell if the latter is tioofwaterandvthemeridionalwind. Accordingto[3],[q¯v] synchronized with the aphelion season. In practice, aphe- canbewrittenas: lion season implies decreasing atmospheric temperatures in [q¯v]=[q¯][v¯]+[q0¯v0]+[q¯∗v¯∗] (1) thetropicsandthuslowerlevelsofcondensation/precipitation. Perihelionseason,onthecontrary,comeswithenhancedsolar with the prime symbol 0 expressing the departure from the forcingandwarmertemperatureswhichallowwatertobecar- timeaverage(q0 = q−q¯andv0 = v−v¯)whereasthestar riedbytheHadleycelltowardsthewinterhemispherewithout experiencingtheeffectsofcloudsedimentation. symbolbeingrelatedtothedeparturefromthezonalaverage (q∗ =q−[q]andv∗ =v−[v]). Onanannualaverage,[7]suggestsanetfluxofwatertowards the hemisphere for which summer is timing with aphelion. In short, total water transport [q¯v] is the sum of the mean Whereasthecurrentorbitalconfigurationshouldthereforefa- meridionalcirculationcomponent[q¯][v¯],thatoftransiented- dies [q0¯v0] and that of non-travelling waves [q¯∗v¯∗]. Eq. (1) vorthenorthernhemisphere,italsoimpliesthatthissituation isreversedwhentheperihelionisshiftedof180o. canbeintegratedoverheighttoyield [7]evensuggestedthatthecurrentpositionofthepermanent Z 0 dp Z 0 dp Z 0 dp Z 0 dp watericecapisaconsequenceofthiseffect. Accordingly,the [q¯v] = [q¯][v¯] + [q0¯v0] + [q¯∗v¯∗] permanentwatericecapshouldmovetothesouthpolewhen g g g g ps ps ps ps aphelionoccursduringsouthernsummer. (2) Ontheotherhand,[8]showedthat,regardlessofexcentricity Thelatterequation,akintoazonal-andvertical-meanexpres- andapheliondate,thesouthtonorthtopographicslopeapplies sionofthewatermeridionaltransport,synthetizesthegeneral a major component to the general circulation biasing cross- behaviorofthemeridionalfluxfields. Giventhatqisthesum equatorialmassflowstowardsthenorthhemisphere. ofbothatmosphericwatervaporandwaterice(clouds),eqs. The purpose of our study is to confront the Clancy effect to (1)and(2)canbefurtherrecastedtoyieldtherespectivecon- thatinducedbytopographicforcingwithinthecontextofGCM tributionsofvaporandclouds. Mostofthewatercyclestudies simulations. Ultimately,wewilldiscussthestabilityofaper- todate[4,5]havefocusedonthesoleroleoftheHadleycellin manent cap in the south pole that recent observations may cross-equtorialflowsofmoisture. However,[4]and[5]have confirm[9]. shownthatbaroclinicactivityplaysakeyroleincyclingwater inandoutthenorthresidualcap. Indeed,[6]concludedthat Reference theobservedextractionofwaterfromthenorthpolarcapcan [1]F.Forgetetal.,JGR104,24155(1999) notbereproducedwithatwo-dimensionnalcirculationmodel. [2]F.Montmessinetal., proceedingsofthemarsVIconfer- Accordingto[5],horizontalmixingofmoisturebetweenhigh ence,Pasadena(2003) Third Mars Polar Science Conference (2003) 8089.pdf Watertransportcomponents: F.Montmessinetal. [3]J.P.PeixotoandA.Oort,PhysicsofClimate,Amer. Inst. [6]R.HaberleetB.Jakosky,JGR95,1423(1992) ofPhysics(1992) [7]T.Clancyetal.,Icarus122,36(1996) [4]H.Houbenetal.,JGR102,9069(1997) [8]M.RichardsonandJ.Wilson,Nature416,298(2002) [5]M.RichardsonandJ.Wilson,JGR107,10.129/2001JE001536 [9]T.Titusetal.,Science299,1048(2003) (2002)

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