thermallydrivenflows-2017steenburgh/classes/6250/lectures/... · 2017. 9. 15. · •winds tend to...
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ThermallyDrivenFlows
Atmos 6250:MountainMeteorologyJimSteenburgh
DepartmentofAtmosphericSciencesUniversityofUtah
[email protected]:greatmontanabeertrek.com
Reading
Zardi,D.,andC.D.Whiteman,2013:Diurnalmountainwindsystems.MountainWeatherResearchandForecasting:RecentProgressandCurrentChallenges.T.Chow,S.deWekker,andB.
Snyder,Eds.,Springer,35–119.
Discussion
• Whydoterrainheterogeneities(mountains,valleys,slopes)leadtocirculationsinthepresenceofuniformsurfaceheatingorcooling?
• Canyouprovidesomeexamplesofthermallydrivenmountain,valley,orslopecirculationsinUtah?
TypesofMountainWinds
• Dynamicallydrivenflows producedbytheinteractionofthelarge-scaleflowwithtopography
• Thermallydrivenflows (a.k.a.diurnalmountainwinds)producedbyhorizontalcontrastsinheatingandcoolingthatarisefromtopographicandland-surfacecontrasts
• Frequentlycombinedtosomeextent
TypesofMountainWinds
• Dynamicallydrivenflows producedbytheinteractionofthelarge-scaleflowwithtopography
• Thermallydrivenflows (a.k.a.diurnalmountainwinds)producedbyhorizontalcontrastsinheatingandcoolingthatarisefromtopographicandland-surfacecontrasts
• Frequentlycombinedtosomeextent
ThisLecture
ThermallyDrivenMountainWinds• Slopeflows(upslopeanddownslope)
– Producedbyhorizontaltemperaturecontrastsbetweenairoveravalleyandairoveritssidewalls
• Valleyflows(up-valleyanddown-valley)– Producedbyhorizontaltemperaturecontrastsalongavalleyaxisorbetween
airinthevalleyandoveranadjacentplain
• Cross-valleyflows– Producedbyhorizontaltemperaturedifferencesbetweentwoopposingvalley
sidewalls
• Mountain-plainwindsystem– Producedbyhorizontaltemperaturedifferencesbetweenairoveramountain
massifandairoverthesurroundingplains
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ThermallyDrivenMountainWinds• Diurnalmountainwindsystems
– ThermallydrivenwindsystemsassociatedwiththediurnalcycleofheatingandcoolingattheEarth’ssurface
– Exhibitdiurnalreversal
• Anabaticflows– Upslope,upvalley
• Katabaticflows– Downslope,downvalley
• Anabaticandkatabaticflowsdonotnecessarilyexhibitdiurnalreversal– Katabaticmorecommonlythananabatic
SlopeandValleyFlows
Whiteman(2000)
DaytimeNighttime*Diurnalreversalcommon,butnotrequired(e.g.,glacialflows)
CrossValleyFlow
BaderandWhiteman(1989),Whiteman(2000)
Mountain-PlainWindSystem
H
L
H
L
Daytime
Nighttime
Regional-scalecirculationbetweenmountain/plateaumassiff andsurroundinglowlands
Mountain-PlainWindSystem
Reiter & Tang (1984); Whiteman (2000)
MeanJuly850mbheight(0500MST) MeanJuly850mbheight(1700MST)
ReiterandTang(1984),Whiteman(2000)
Multiscale Interactions
Whiteman(2000)
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Multiscale Interactions
Whiteman(2000)
SlopeFlows
Photo:http://oldbearnews.blogspot.com/
Discussion
• Lateintheday,flowsthatmovedirectlydowntheterraingradienttypicallydevelopalongslopes
• Whatmechanismsdrivetheseflows?
• Whydon’ttheycontinuetogetstrongerduringthenight(inmostinstances,theydon’t)
SlopeFlows
• Gravityorbuoyancyflowsthatfollowtheterraingradient
• Drivingforceisbuoyancygeneratedbythecoolingorwarmingofairadjacenttotheslope
• Bestdevelopedinclear,undisturbedweather
• Difficulttofindinpureform
SlopeFlows
Whiteman(2000)
Along-SlopeForceBalance
S
n
u =velocityparalleltoslope(alongs),positivedownslope
ρ0 =referencedensitywithoutcooling
Pa =Ambientpressure
θ’=perturbationθ nearslope
θ0 =referenceθ
α=slopeangle
u’w’=turbulentmomentumflux
DuDt
= −gθ 'θ0sinα − 1
ρ0
∂(p− pa )∂s
−∂(u 'w ')∂n
HorstandDoran(1986),Whiteman(2000)
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Along-SlopeForceBalance
S
n
DuDt
−1ρ0
∂(p− pa )∂s
−gθ 'θ0sinα
−∂(u 'w ')∂n
DuDt
= −gθ 'θ0sinα − 1
ρ0
∂(p− pa )∂s
−∂(u 'w ')∂n
Along-slopeacceleration
Buoyancycomponentalongslope
Along-slopepressuredifferencegradient(differencerelativetoambient)
Turbulentmomentumflux(a.k.a.,friction)
HorstandDoran(1986),Whiteman(2000)
SlopeFlows
U
B
PGFF Assumingsteadystate,buoyancybalancedby:
1.Friction/entrainment2.Pressuregradient(relativetoambient)producedbychangesindepthofcoldpoolalongslope
DuDt
= −gθ 'θ0sinα − 1
ρ0
∂(p− pa )∂s
−∂(u 'w ')∂n
HorstandDoran(1986),Whiteman(2000)
SlopeFlows• Typically1–5ms-1,butspeedincreaseswithslopelength
– Antarctica15–30ms-1
• Decreaseindepthwithincreasingstaticstability
• Downslopeflows– Strongestatorjustfollowingsunset
• DeepeningcoldpoolcreatesadversePGFlateratnightandlimitsbuoyancyeffect
• Convergeintogullies,basins,etc.
• Upslopeflows– Strongestmidmorning– Increaseindepthasonemovesupslope– Convergeoverhigherground(e.g.,ridges,plateaus,etc.)
SlopeFlows• Verysensitivetospatialvariationsinsurfaceradiation– Persistentcloudcover,timeofsunrise/sunset– Slopeaspect,topographicshading,etc.
Whiteman(2000)
UpslopeFlowaboveForest
Whiteman(2000)
Heatingincanopylayercanproduceupslopeflowaboveshallowdownslopeinthesnow-cooledsub-canopylayer
ValleyFlows
https://cleanairfairbanks.files.wordpress.com/2011/01/helios-fire_2011-1-16_nh_1453_duringfire.jpg
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ValleyFlows
• Drivenbystrongerheatingandcoolingofthevalleyatmospherecomparedtotheadjacentplain
• Bestdevelopedinclear,undisturbedweather
Whiteman(2000)
Discussion
• Basedonthecrosssectionspictured,whichofthevalleysbelowwouldhaveastrongerdaytimeup-valleyflow?
ValleyWinds
ValleyVolumeEffectValley-to-plain
temperaturecontrastsdevelopbecauseairvolumeinvalleyissmallerthanthatinplain
Valleydoesn’thavetoslopetoproducealong-valley
winds
Whiteman(2000)
SeasonalEffectonDiurnalReversal
Reiteretal.(1983),Whiteman(2000)
NocturnalValleyExitJet• Windstendtobehighernearmouthofavalleybecause– Windsacceleratewithdistancedownthevalley– Horizontalpressuregradientlargestnearexitwherethereisanabrupttransitionfromhighpressureinvalleytolowpressureoverplain
– Bycontinuity,windspeedincreasesascoldvalleyairsinksandfansoutoverplain
• Greatestimpactfordeepvalleysthatendabruptlyataplain
NocturnalValleyExitJet
ExitjetfromAustria’sInnValley
Pamperin andStilke (1985),Whiteman(2000)
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ValleyWindVariability
• Along-valleytemperatureandwindvariabilitycanbeproducedby– Contrastinshort- orlon-waveradiationlossesorgainsalongvalley
– Rateofconversionofnetradiationtosensibleheat• Concerns:Heterogeneoussnowcover,soilmoisture,vegetation
Whiteman(2000)
ValleyShape
• Along-valleytemperatureandwindvariabilitycanbeproducedbychangesinvalleyvolume– Heatingofairinvalleyisproportionaltovalleyvolume(Whiteman1990)
– AreaswithconvexvalleysidewallsheatmorequicklythanU-shapedareas
Whiteman(2000)
Discussion
ThisphotoofupperLittleCottonwoodCanyonwastakenshortlyaftersunriseAssumingcalmlarge-scalewinds,whatlocalflowsdoyouexpect?
Cross-ValleyWinds
• Blowacrossvalleywhenairononesidebecomeswarmerthanothersid)• Compensatoryflowsinoppositedirectionaloft• Culprits:Unequalsidewallexposuretosun,heterogeneoussnowcover,
vegetation,soilmoisture
Whiteman(2000)
Cross-ValleyWinds
BaderandWhiteman(1989),Whiteman(2000)
TheDiurnalPBLCycle
• Nighttime(decoupled)period• Morningtransition• DaytimeCBL• Eveningtransition
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DiurnalPBLEvolutionoveraPlain
Whiteman(2000)
DiurnalPBLEvolutionoverValley
Whiteman(2000)
NighttimeDecoupledPeriod
• ValleyflowdecoupledfromresidualCBLaloft
• Downvalleyanddownslopewindsprevail
Whiteman(2000)
Discussion
• WhatisgoingonintheWasatchWeatherWeeniesbannerbelow?Describethecloudsandhypothesizewhytheylookthewaytheydo
MorningTransition• CBLbeginstodevelopoverheated
slopes
• Upslopeflowsdevelopalongvalleysidewals,thenshallowup-valleyflowalongvalleyaxis
• Topofinversionsinksduetocompensatingsubsidence
• Downvalley flowpersistsinshrinkingstable-corealoft
• StablecoreeventuallydestroyedbyCBLgrowthandup-valleyflowextendsthroughvalleydepth
• Valleymayeventuallycouplewithambientsynopticfloworplain-mountaincirculation
Whiteman(2000)
MorningTransition
Whiteman(1980)
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DaytimeCBL• Convectionoccursaboveall
slopes
• Upslopeandup-valleyflowspredominatewithinvalley
• Windstransitiontothelarge-scaleflowabovethevalley
• Windsinthevalleymaybecometurbulentandupperwindsmayoccasionallychannelintovalley
Whiteman(2000)
EveningTransition
• Beginsinlateafternoon• Downslopeflowsbeginfirstinshadedareasonsidwalls andvalley
floor,thenoverallsidewals• Valleyinversionwithdown-valleyflowgrowsindepth
Whiteman(1986)
DiurnalCycleHodograms
RightBankwindsturnclockwise
LeftBankwindsturn
counterclockwise
Hawkes(1947),Whiteman(2000)
Discussion
Howwelldothemeansummerwindsatthestationsabovematchthetheoryonthepriorslide?Explaindiscrepancies(Fullandhalfbarbdenote1and0.5ms-1,respectively)
Stewartetal.(2002)
DiurnalCycleofValleyDivergence
Convergence
Divergence
October2000
CourtesyMikeSplitt
BasinCirculationsNASA
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Discussion
Describethediurnalevolutionofwindsyouexpectinabasin.HowaretheyDifferentthaninavalley?Why?
NASA
BasinCirculations• Unlessperturbedbythelarger-scaleflow,enclosed
terrainfeaturesdevelopslopeflowsbutweakalong-basincirculations– Slopeflowstypicallyweakenasbasincoldpooldeepens
• Theabsenceofalong-basinadvectionandassociatedturbulenceresultsinalargerdiurnaltemperaturerange– Overnightminimumsareespeciallylow
• Basincoldpoolscanbediurnal(i.e.,developatnight)orpersistfordaysorweeks
Examples
Whiteman(2000)
Examples
CourtesyDaveWhiteman
PeterSinks
Clements(2001)
Utahall-timerecordlowof-57°C
NorthSink
Clements(2001)
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NorthSink
Clements(2001)
Vegetation“inversion”
Perimeter
Clements(2001)
Instrumentation
Clements(2001)
SurfaceTemperature
Clements(2001)
BigdiurnalcycleColdestairinbottomofbasin
Airtemperatureincreasesupwardalongbasinsidewalls
VerticalStructure
• Gradualcoolingofbasinairmass throughnight
• Downslopeflowearly,thenwindsbecomeweak
• Inversionattopofbasinstrengthens
Clements(2001)
Summary• Largespectrumofthermallydrivenflowsincomplexterrain
– Slopeflows– Valleyflows– Cross-valleyflows– Mountain-plaincirculations
• Typicaldiurnalevolutionunderlightforcingincludes– Nocturnalregime
• Downslopeanddown-valleyflows– Morningtransition
• Rapiddevelopmentofslopeandshallowup-valleyflows• Gradualerosionofelevateddown-valleyflowandstablecorealoft
– Afternoonregime• Upslopeandup-valley;possiblecouplingwithlarge-scaleflowaloft
– Eveningregime• Rapidonsetofdownslopethendownvalley withgradualdeepeningofcoldcore
• Basins– Weakslopeflowsinitiallyineveningthatweaken– Attainverycoldnocturnaltemperaturesduetolimitedflowsandturbulence
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ReferencesBader,D.C.,andC.D.Whiteman,1989:Numericalsimulationofcross-valleyplumedispersionduringthemorningtransitionperiod.J.Appl.Meteor.,28,652-664.
Clements,C.B.2001:ColdAirPoolEvolutionandDynamicsinaMountainBasin.UniversityofUtahM.S.Thesis,100pp.
Hawkes,H.B.,1947:Mountainandvalleywindswithspecialreferance tothediurnalmountainswindsoftheGreatSaltLakeregion.Ph.D.dissertation,OhioStateUniversity,312pp.
Horst,T.W.,andJ.C.Doran,1986:Nocturnaldrainageflowonsimpleslopes.Bound.-LayerMeteor.,34,263–286.
Pamperin,H.,andG.Stilke,1985:NocturnalboundarylayerandLLJinthepre-alpineregionneartheoutletoftheInnValley.Meteor.Rundsch.,38,145–156.
Reiter,E.R.,andM.Tang,1984:Plateaueffectsondiurnalcirculationpatterns.Mon.Wea.Rev.,112,638–651.
Stewart,J.Q.,C.D.Whiteman,W.J.Steenburgh,andX.Bian,2002:AclimatologicalstudyofthermallydrivenwindsystemsoftheUSIntermountainWest.Bull.Amer.Meteor.Soc.,83,699-708.
Whiteman,C.D.,1980.BreakupofTemperatureInversionsinColoradoMountainValleys.Ph.D.dissertation,ColoradoStateUniversity. AvailablefromUniversityMicrofilms,AnnArbor,MichiganorasAtmosphericSciencePaperNo.328fromDepartmentofAtmosphericScience,ColoradoStateUniversity,FortCollins,Colorado80523.
Whiteman,C.D.,1986:TemperatureinversionbuildupinColorado'sEaglevalley.Meteor.Atmos.Physics,35,220-226.
Whiteman,C.D.,2000:MountainMeteorology:FundamentalsandApplications.OxfordUniversityPress,355pp.
Zardi,D.,andC.D.Whiteman,2013:Diurnalmountainwindsystems.MountainWeatherResearchandForecasting:RecentProgressandCurrentChallenges.T.Chow,S.deWekker,andB.Snyder,Eds.,Springer,35–119.