Quan>fyingtheTransportofAirintoMesoscaleConvec>veSystemUpdraVs 1 2 2 RachelPhinney ,PeterMarinescu ,SusanvandenHeever 1 2 UniversityofNebraska-Lincoln ,ColoradoStateUniversity Results:Lowvs.Mid-levelTracers Introduc>on Results:CaseComparison Figure4.ThefracFonoftheiniFaltracer amountasafuncFonofheight(m)where theverFcalvelocityisgreaterthan5ms-1 at10:30UTC. Scien>ficQues>on:Howmuchmid-levelairisge3ng intoMCSupdra:s? Methods TheRegionalAtmosphericModelingSystem(RAMS)1wasusedto simulatetwocasesfromtheMid-la>tudeCon>nentalConvec>veCloud Experiment(MC3E)2,3:May20,2011andMay23-24,2011. Figure1.NEXRADradarreflecFvity(dBZ)at2.5kmabovegroundfor(le6)20Mayat10:30UTC and(right)24Mayat05:00UTC Crosssec>ons 0900UTC Figure5.Bargraphcomparisonof T01-T02andT05-T06between7and8 kilometerson20Mayat10:30UTC. 1045UTC TheRAMSsimula>onsu>lizedaredescribedinMarinescuetal.(2016). Theyused1.2kmhorizontalgridspacingandver>calgridspacingof75 mnearthesurface,stretchedto500mnear4kmabovegroundlevel. Forthestudyhere,thesesimula>onswererestartedduringtheMCS maturestagesandrunfor2hours.Tracerswereplacedinfrontand behindtheMCSatmul>pleal>tudestostudyairtransportwithin MCSs. TracerIni>aliza>on T03 T02 T01 Therewere16tracer heights,each1kminthe ver>cal,and150kmx150 kminthehorizontal(Figures 2and3).Eachlayerwas populatedwiththesame totalnumberoftracers. Figure2.(top).CrosssecFonofthe20May caseat09:00UTCshowingthelocaFonof thetraceriniFalizaFon.EachsecFonis1km thickand150kmx150kminthehorizontal. Totalcondensateiscontouredinblack. Figure3.(bo\om).Planviewofthe20Mayat 09:00UTCwithverFcallyintegrated condensatecontouredandthetracerlocaFons outlinedinblack. Figure7.SameasFigure4,but for24Mayat03:30UTC. Resultsofthisgraphare comparedwiththatofFigure4. Notethechangeinx-axisscale. 1) Greateramountsoftracersareobservedinthe24Maycase. 2) Thedifferencebetweenlow-levelandmid-leveltracersis smallerinthe20Maycasei.e.mid-levelairprovidesalarger frac>onoftheairwithinupdraVsinthe20Maycase comparedtothe24Maycase. • Toseehowmanytracerswereenteringintotheupper regionsofthestormthetotalquan>>esoftracersbetween 7and8kilometerswereevaluated.Itwasdiscoveredthatin thisregiontherewere1.5>mesmorelow-leveltracersthan mid-leveltracers(Figure5).Thisisconsistentwithour findingswhenlookingatthetracerquan>>esforalheights. height(m) • Thetotalquan>>esofthe tracerswithintheupdraV showthat6%ofairfromthe low-levels(T01-T02)and3%of airfromthemid-levels(T05T06)arecontainedwithinthe MCSupdraVs(w>5ms-1)aVer 1.5hours. • Resultsfromthe24Maycase aswellasother>messhow similarresults. height(m) AnMCS(MesoscaleConvec>veSystem)isdefinedasathunderstorm withacon>nuousprecipita>onregionatleast100kilometersinthe horizontaldirec>on(AMSGlossary). Airhasdis>nctcharacteris>csatdifferentlevelsthroughoutthe atmosphere.It’sknownthatairnearthesurfaceentersintoMCS updraVs,butwhataboutairfromthemid-levels?Thecharacteris>csof airintheselayers,suchasthedrynessofthelayerortheaerosol content,couldimpacttheMCSmicrophysicsanddynamics. height(m) Bothoftheseobserva>onsarethoughttobepartlyduetothe strongerupdraVsaswellasthelargerupdraVregioninthe24May casewhichhassignificantlymoreupdraVsthan20Maycase (Figure8).Thegreateramountoftracersobservedwithinthe convec>velineinthe24Maycasewerealsopartlyduetothe northernadvec>onoftracersbywindsinthe20Maycasewhich meantthatthesetracersdidnotbecomeentrainedintothe updraV. 24May,2011 20May,2011 T01-T02 T05-T06 T09-T10 Figure6.CrosssecFonat35.1oNfor20Maycaseat(le6) 09:00UTCand(right)10:45UTC.T01-T02iscontouredinblue, T05-T06iscontouredingreen,andT09-T10iscontouredinred atavalueof9e-6.Totalcondensateiscontouredinblack. Conclusions • Asexpected,morelow-levelairiswithinMCSupdraVs(6%comparedto3%).Thisalsoshows, howeverthatmid-leveltracersarepresentwithinMCSupdraVsinamountsthatcouldhaveimpacts onthemicrophysicsanddynamicsofthesystem. • UpdraVstrengthandwidthoftheupdraVregionmayimpacttheamountofmid-leveltracers ge[ngintoMCSupdraVs. FutureWork • AnalyzetracersplacedbehindtheMCS • ComparetracerstoCCNconcentra>ontodeterminehowmanyaerosolsgetac>vatedandwhereinac>vated aerosolsendup. Figure8.Planviewplotsfor(le6)20Maycaseat10:30UTCand(right)24Maycaseat03:30 UTCwithverFcalvelocitygreaterthan5ms-1contouredinred.Totalcondensateiscontouredin black. Acknowledgements ThisworkhasbeensupportedbytheNa>onalScienceFounda>onResearchExperiencesfor UndergraduatesSiteinClimateScienceatColoradoStateUniversityunderthecoopera>ve agreementNo.AGS-1461270andtheDepartmentofEnergy.GrantNumber:DE-SC0010569. References 1.Saleeby,S.M.,andS.C.vandenHeever,2013:DevelopmentsintheCSU-RAMSaerosolmodel:Emissions, nuclea>on,regenera>on,deposi>on,andradia>on.J.Appl.Meteor.Climatol.,inpress. 2.Jensen,M.P.,etal.,2015:TheMidla>tudeCon>nentalConvec>veCloudExperiment(MC3E).Bull.Am.Meteorol. Soc. 3.Marinescu,P.J.,andCoauthors,2016:MicrophysicalStructureandEvolu>onofLatentHea>ngProfilesinTwo SimulatedMC3EMCS.J.Geophys.Res. Formoreinforma>on,[email protected]
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