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Meiji University
Title
Warm-Core Events of the Arctic Winters Appeared
in the Annual March of the Monthly Mean Air
Temperatures北極域の月平均気温変化に現れる冬季の
ウォームコア現象
Author(s) 梅本,亨
Citation 駿台史學, 103: 79-94
URL http://hdl.handle.net/10291/6101
Rights
Issue Date 1998-03-26
Text version publisher
Type Departmental Bulletin Paper
DOI
https://m-repo.lib.meiji.ac.jp/
駿 台 史 学 第103号79-94頁,1998年3月
SUNDAISHIGAKU(SundaiHistoricalReview)
No.103,Mar.1998,pp.79-94.
Warm-CoreEventsoftheArcticWintersAppearedinthe
AnnualMarchoftheMonthlyMeanAirTemperatures
TohruUMEMOTO
DepartmentofGeography,MeijiUniversity
Abstract:Awarm-coreeventisthewarmspellobservedduringthecoreless
typewinteroftheannualmarchofsurfacetemperatureinthehighlatitudes .Wecanexplainsomepossiblecausesforthewarmspell:1)thelargescale
warmadvectionaroundtheactioncenterssuchastheAleutianandthe
Icelandiclows,2)passingofcyclonicdisturbancesthatbreakthestrong
surfacetemperatureinversion,and,3)existenceofcut-offwarmanticyclones
thatderivedfromblockingridges.Thispapershowsthegeographical
distributionofoccurrencefrequencyofthewarm-coreeventsinthenorthern
hemispherebyusingthemonthlymeantemperaturedataofNMCoctagonal
grids.Warm-coreeventsarefoundnotonlyonthesurfacegridsbutalsoonthe700hPaand500hPagrids.Thegeographicaldistributionofeachgrid
systemshowsasamepattern,sothatthelargescalewarmadvectionisthe
mostlmportantcauseforthewarm-coreevents.
Keywords:warmcore,corelesswinter,Arctic,blocking ,airtemperature.
1 Introduction
Theannualmarchofmonthlymeansurfacetemperaturesinthehigh
latitudesoftenshowsthecorelesstypeinwinter.IntheAntarctic ,wecan
observethetypicalcorelesswintersthatassociatewiththestrongsurface
temperatureinversion.Kawaguchi(1979)pointedoutonepossiblecausethatthe
upwardterrestrialradiationbalanceswiththedownwardatmosphericradiation
duringthepolarnight,sothatthemonthlymeansurfacetemperaturesstagnate
aroundabottomvalue.
AlthoughthelargescaletopographyoftheArcticisquitereversetothe
Antarctic,corelesswintersalsooccurinthenorthernhemisphere .Inthis
situation,theverticaltemperatureprofileshowsastrongsurfaceinversion(Lg .,
Streten,1969;Kahl,1990).Therefore,oneofthemostimportantfactors
controllingtheArcticwintertemperaturefieldisthedownwardlongwave
79
T.UMEMOTO
radiation.Thisfactorisstronglyinfluencedbythebehaviorofthepolarvortex
throughthevariationoftemperature,humidity,andcloudiness(Overlandetal.,
1997).
VowinckelandOrvig(1970)statedthatcoldspellsovertheArcticOceanare
notcausedbythecoldadvectionbutbytheradiativecooling,andwarmspells
arecausedbycyclonesthatdistracttheinversion.Theyalsomentionedthatthis
surfaceinversionisordinarilyintensifiedbytheupper-levelwarmadvection.
Thewarmadvection,however,occasionallyraisessurfacetemperatureand
causesawarmspell.ThereforetheyconcludedthattheArcticsurfaceinversion
isacomplexphenomenon.Recently,Serrezeetal.(1992)ana.1yzedstationdata
includingaerologicalsoundingsandtheRussiandrifting-icestations.Theyshowed
thattemperatureinversionsusuallyappearintheEurasiansideoftheArctic
BasinandthethicknessofinversionlayerisaboutlOOOminwinter.
Figurelshowsthethreetypesofsurfacetemperaturechangeinwinter.
Thecold-coretypeisordinaryinthemiddlelatitudes,andthecorele∬typeis
typicalinthepolarregion.Whenawarmspellofrelativelylongtermisobserved
inthepolarwinter,itmakesawarm-coreupontheflatcorelessline(hereafter
referredtoaswarm-coreez/ent).
SomemeteorologicalstationsaroundtheBeringSea(inJanuary)andthe
BarentsSea(inFebruary)showthewarm-coreastheclimaticvaluesofmonthly
meansurfacetemperature.Forexample,ShiraiwaandSawagaki(1992)observed
awarm-coreeventduringthewinterofl990inSpitsbergen.
Rubinshteyn(1962)showedtheoccurrencefrequencymapofthewarm-core
eventsbyusingmonthlymeantemperatureofllOstationsaroundtheArctic
Basin.Hefiguredouttwohighfrequencyareas:theNorwegianSea(fromthe
eastcoastofGreenlandtothewestcoastofNovayaZemlya),andtheBering
Sea.Healsoreviewedthediscussionofthecauseforwarm-coreevents.He
summarizedthreeprincipalmechanisms:
●thewarmadvectionfromthelowerlatitudes,
●thesensibleheattransportfromtheArcticOceanthroughtheseaice,
●thereleaseoflatentheatattheseaiceformation .
Thewarmadvectionistheonlyonepossiblecauseforthewarm-coreamong
them,becausewecanobservewarm-coreeventsoutsidetheArcticBasinand
80
Warm-CoreEventsoftheArcticWinters
Φ」⊃ρ"5」Φ○∈
Φト
⊂円ΦΣ
〉一エピ⊂OΣ
エ9エ
≧OL
Cold-core
Warm-core
Coreless
EarlyWinterMidWinterLateWinter
Season
FigurelSchematicsforthewarm-coretypetemperaturechange.Thecold-coretypeisotdinaryinthemiddlelatitudesandthecorelessistypicalintheArcticregion.
evenintheinlandregionofthecontinents.
Thepurposeofthispaperistoshowthetemporalandspatialcharacteristics
ofthewarm-coreeventsintheArcticregion.Inordertodiscussthestructureof
large-scalewarmadvection,theauthorpaidaspecialattentiontorecognizethe
geographicaldistributionofoccurrencefrequencyintheupPertroposphere,andhe
extendstheareaofanalysisuptothemiddlelatitudesofthenorthern
hemisphere.
2Dataandthewarm-coredefinition
ThedatausedinthisstudyaretheNMC(NationalMeteorologicalCenter,
USA)octagonalgridsofthemonthlymeantemperatureofthenorthern
hemisphere.Theauthorusedthetemperatureofthreelevels(surface,700hPa,
and500hPa)for22winterseasonsfroml965-66tol986-87.Thewinterseasonis
definedasthe5-monthperiodfromNovembertoMarch.Weordinarilydefinethe
81
T.UMEMOTO
northernhemispherewinterseasonasthe3-monthperiodfromDecemberto
February.Inthepresentanalysistheauthorfocusedontheannualmarchof
temperatureintheArcticregion,sothatheaddedNovemberandMarch.
Ofcourse,thetermwarm-coremeansawarm-coreり ρρArcticwinter,then
thetermistobeusedonlyforthehighlatitudes.Awarm-coreeventinthe
Arcticregionimpliestheexistenceofthelarge-scalepositivetemperature
anomalythatmayextendintothemiddlelatitudes.Thismeansthatwarmspells
ofthemiddlelatitudescloselyrelatetotheArcticwarm-core.Theauthornamed
bothArcticwarm-coresandwarmspellsinthemiddlelatitudesashigh
temperatureevents.Ahightemperatureeventforamonthinawinterseasonat
agivengridpointmeetsthefollowingsimplecondition:
tm.1trn+1.
Intheaboveexpression,tisthemonthlymeantemperatureofonegridpoint,
andthesubscriptsm-1,m,andm十ldenotethepreviousmonth,theverymonth
(fromNovembertoMarch),andthefollowingmonthrespectively.
Theaboveproceduiemaybetoodescriptivetomakeaphysicalimage.The
authorgivesanexamplethatshowsthespatialrelationshipsamongthe
geopotentialheight,temperatureanomaly,andhightemperatureevents.Figure2
showsthemonthlymeanheightandtemperatureanomalyof500hPasurfacefor
Januaryl977.Themoststrikingfeatureofthismonthwasthesimultaneously
developedblockingridgesintheAtlanticandthePacific.Thesetworidges
coupledovertheArcticOceanandbecameintoasingleanticyclonicsystem
(Fig.21eft).
Byusingthestationdata,Umemoto(1985)showedthatthissynopticevent
producedanextremelycoldweatheroverthebroadareaofEastAsia,andatthe
sametime,awarmweatheroverthehighlatitudes.TheNMCgridsof500hPa
levelforJanuaryl977alsoindicatethelargepositivetemperatureanomalyover
thehighlatitudes(Fig.2right).Relativelylargeanomalyareas(forexample,above
十6degree)aresituatedinthepositionsofthetwoblockingridges(theNortheast
PacificandtheNorthwestAtlantic)andofthecutoffhighovertheArcticBasin.
Figure3showsthegeographicaldistributionofhightemperatureeventsfor
Januaryl977.Hightemperatureeventsofthe500hPalevelshowseveral
82
Warm-CoreEventsoftheArcticWinters
500hPa={
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●MonthlyMeanHeight●MonthlyMeanTemp.Anomaly
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Figure2Themonthlymeangeopotentialheightandmonthlymeantemperatureanomaly
ofthe500hPasurfaceforJanuaryl977:(1eft)heightinmeter,andthedottedlinesshow
theridges,(right)contoursdrowninevery2degrees,shadedareashowspositive
anomalies。
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Figure3HightemperatureeventsoccurredinJanuaryl977.Thegridpoints
recordofhightemperatureeventwereenclosedbylinesandshaded .
δ
withthe
expansionsofareascorrespondingtothelargepositivetemperatureanomalyover
thehighlatitudes(Fig.2right).Bothofthesurfaceandthe500hPachartsshow
averysimilarimageovertheArctic,thereforetheauthorconsidersthatthe
83
T.UMEMOTO
statisticallydefinedhightemperatureevents(thismeanswarm-coreeventsinthe
Arctic)reflectasubstantialatmosphericsystemofthesynopticscale.
3GeographicalDistributionofWarm-coreEvents
HightemperatureeventsaredetectedatallpointsoftheNMCoctagonalgrid
systemfor22winters.Oneoctagonalgridcontains1977points,butsomepoints
outsidethelatitudinalcircleof20Nareomittedbecauseofpresentation.Figures
4,5,and6showthegeographicaldistributionofoccurrencefrequencies.Inthese
figures,theauthordidnotuseanykindsofarea-normalizationorspatial
smoothingbutjustcalculatedtheoccurrenceratio(timesofoccurrenceare
dividedby22).ContoursaredrawnineverylO%andshadedpartsshowthearea
withthevalueabove30%.
a)Surface
Manyhightempetatureeventsoccurredthroughoutthewinter,butthe
frequencyisverylowinNovember.Therearetwohighfrequencyareasinthe
ArcticregionforJanuary(Fig.4c):thefirstonecentersontheBeringStraitand
itcoversabroadareaoftheEastSiberiaandAlaskasector,thesecondis
situatedaroundGreenland.Bothoftheseshowthevaluesof40%ormore.
AsmallpeakcanbeseentothenorthofNovayaZemlya.Ontheother
hand,hightemperatur6eventsofthemiddlelatitudesoccurredintheEast
PacificandtheEastAtlanticOceans.ThepeakoftheEastPacificseemstobe
apartofthehighlatitudeswarm-corearea.However,thepeakoftheEast
Atlanticseemstohavenorelationtothewarm-corearoundGreenland.
InFebruary(Fig.4d),thesituationistotallydifferent.Onlyonemajorareaof
thewarm-coreappearsovertheNorwegianSeaandtheGreenlandSea.Another
smallpeakisintheeastpartofAlaskaanditcoversthecoastalareaoftheGulf
ofAlaska.Besidesthis,wecannotfindanynotableareasofhightemperature
event.Inothermonths,thefrequencyofwarm-coreislow.Oneexceptionisthe
BarentsSeainMarch(Fig.4e).
Wecanseesomehighfrequencyareasofhightemperatureeventsinthelow
latitudestoo(forexample,theEastPacificOceanofNovember,themiddle
84
`
Warm-CoreEventsoftheArcticWinters
鱗
●SURFACE(1966-1987)●
Occurrencefrequency(×10%)
ofthehightemperatureevents
definedas
tm.,tm+1
t:monthlymeantemperatureofgrid・points
(subscripts}
m:month(fromNovembertoMarch)
m-1:thepreviousmonth,m+1:thefollowingmonth
(Data:NMCoctagonalgrids)
a)November,b)Decemberc)January,d)Februarye)March
Figure4Surfaceoccurrencefrequencyofthe
hemisphere.ContoursweredrawnineverylO
30%.
hightemperatureeventsinthenorthern
percent,andashadedareashowsabove
85
T.UMEMOTO
.
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●700hPa(1966-1987)●
Occurrencefrequency(×10%)
ofthehightemperatureevents
definedas
tm .ftm+t
f:monthlymeantemperatureofgrid・points
(subscripts)
m:month(lromNovembertoMarch)
m・1:thepreviousmonth,m+1:thefollowingmonth
(Data:NMCoctagonalgrids)
a)November,b)Decemberc)January,d)Februarye)March
Figure5700hPaleveloccurrencefrequencyofthehightemperatureeventsinthe
northernhemisphere.ContoursweredrawnineverylOpercent,andashadedareashows
above30%.
86
Warm-CoreEventsoftheArcticWinters
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Occurrencefrequency(×10%)
ofthehightemperatureevents
definedas
fm-1fm+1
「:monthlymeantemperatureofgrid・points
(subscripts)m:month(fromNovembertoMarch)
m-1二thepreviousmonth,m+1:thefollowingmonth
(Data:NMCoctagonalgrids)
a)November,b)Decemberc)January,d)Februarye)March
Figure6500hPaleveloccurrencefrequencyofthehightemperatureeventsinthe
northernhemisphere.ContoursweredrawnineverylOpercent,andashadedareashows
above30%.
87
T.UMEMOTO
AtlanticOceanofFebruary,etc.).Buttheseareashavenodirectrelationstothe
atmosphericcirculationoftheArctic.Moreover,theprocedureforfindinghigh
temperatureeventsusedinthispapermaybemeaninglessfortheTropics.The
author,thereforedidnottakethesepeaksintoconsiderationonthewarm-core
events.
b)Upperlevels
Thedistributionofhightemperatureeventsof700hPaand500hPain
Novembershowsafamiliarpatternthatrecallsustothecifcumpolarflowof
zonalwave-numberthree(Figs.5aand6a).Highfrequencyareasaresituatedin
theEastPacificsectorcenteredinAlaska,tothesouthofGreenland,andalong
theUralMountains.
InDecember,wecanseetwomajorareasofhighfrequencyinthemiddle
latitudesof500hPalevel(Fig.6b):theNorthAtlanticOceanandtheNorth
PacificOcean.TheNorthAtlanticoneismarkedinthe700hPaleveltoo,butthe
NorthPacificoneissomewhatobscureinthatlevel(Fig.5b).Thesetwoareas
arenotnotableinthesurfacechart(Fig.4b).
InJanuary,ahighfrequencyareaofwarm-coreeventsexistsintheArctic
(Figs.5cand6c).Thedistributionpatternissimilartothesurfacechart.Inthe
middlelatitudes,ahighvalueareainthenortheasternPacificextendstothe
ArcticthroughAlaska.Twootherhighfrequencyareasaredistinguishedover
MongoliaandthesouthwestpartofEurope.
InFebruary(Figs.5dand6d),wecanseeabroadareawiththehighervalue
ofwarm-coreeven .tsovertheNorthAmericansideoftheArctic.Itcoversfrom
AlaskatothenorthwesternEuropethroughtheCanadianArctic.The
westernmostpartofthearea(i.e.,aroundAlaska)of700hPachart(Fig.5d)
extendssoUthwardtothemiddlelatitudesofthewestcoastoftheNorth
America.
ThedistributionofhightemperatureeventsofMarchshowsthreepeaks
(Figs.3eand6e).Arelativelysmallareaofthewarm-coreeventsappearsover
theBarentsSea.TheothertwoaresituatedinthemiddlelatitudesoftheNorth
PacificandtheNorthAtlantic.Eachofthepeakstakessomewhateastpositions
incomparisonwithJanuary.
88
Warm-CoreEventsoftheArcticWinters
4Discussions
Thedistributionofwarm-coreeventsintheArcticshowsastrikingfeature
thatthepositionofhighvalueareaseemstosiftanticlockwisebyabout60
degreesfromJanuarytoFebruary.TheAtlanticside(theeasternmostpart)
changesitspositionfromGreenlandtotheNorwegianSea,andthePacificside
(thewesternmostpart)changesitfromtheBeringSeatoAlaska.Inotherwords,
bothsideschangetheirpositionseastward.
PerlwitzandGraf(1995)showedasimilargeographicalpattern.They
performedthecanonicalcorrelationanalysisandtheempiricalorthogonalfunction
analysisforthethreewintermonths(December,January,andFebruary)inorder
toinvestigate"barotropic"relationbetweenthetroposphericandthestratospheric
variationingeopotentialheightandtemperaturefields.Theirfirstandsecond
modeof850hPatemperature(Figs9candlOcoftheirpaper)areconsideredto
correspondtotheJanuaryandtheFebruarypatternsofthepresentpaper.This
impliesthatthevarianceoflowertropospherictemperature.fieldisstatistically
connectedwiththeuppertroposphericpersistentpositivetemperatureanomalyof
JanuaryandFebruary.
Thesefeaturessuggestthatsomelargescaleatmosphericsystemswiththe
durationofatleastonemonthmaycontrolthetemperaturefields.Wecaneasily
indicatetwoofsuchsystems,theoneistheAleutianLowandtheotheristhe
IcelandicLow.Thesesystemshavethecharacteristicsofstandingwavesinthe
northernhemisphericwesterlies,sothattheytransportsensibleheatpoleward
continuouslyforalongperiod.Ifthesesystemschangethosepositionsslightly,
thentheyproduceadrasticchangeinthetemperaturefield(Umemoto,1985).
Forexample,Mosesetat.(1987)showedthereversalpositionalrelationship
betweentheIcelandicLowandtheAzoresHighfromtheviewpointoftheNorth
AtlanticOscillation.
Overlandetal.(1996)showedthreepathwaysofpolewardheatfluxacross
thelatitudinalcircleof70N:theGreenlandSea,theBeringStrait,andthe
northernCanada.Theformertwoarethemainpathwaysandshowrelatlvely
largeinterannualvariability.Theyalsoindicatedthatabout50%ofthetotalheat
89
T.UMEMOTO
fluxisbroughtbythetransienteddies,andabout25%ofitisduetothe
standingeddies.Thetransientandstandingeddiesoftheiranalysisareconsidered
tobeincludingblockingactivitiesandactioncentersrespectively.
Ontheotherhand,theNorthPacificblockingmadethelarge-scalepositive
(negative)surfacetemperatureanomalyoverthehigh(middle)latitudesinwinter
(DoleandGordon,1983;Umemoto,1986).Blockingphenomenafrequentlyoccur
evenintheArcticBasininwinter(e.g.,KnoxandHay,1985;Mullen,1994).
Colucci(1985)showedthatblockinganticycloneshastwokindsofthewarming
effect:
●theadvectivewarmingofwinds,
●theadiabaticwarmingofthesinkingair.
Therefore,thewarmadvectionbythepersistentblockingridgeoranticyclonecan
produceawarm-coreevent.Blockingphenomenatakeplaceespeciallyinthe
NorthAtlantic,theNorthPacificandthewesternSiberia.Butthecut-offwarm
highsfromblockingridgesdonotalwaysstayintheoccurrencearea.
Thetermblocleingisoriginallyderivedfromitseffecttoblockthemovingof
synopticorsub-synopticscaledisturbances.Inmanycases,ablockingflow
patterndoesnotreallyblockthecyclonepassage,butfixesitstracks.Thiseffect
exertsanimportantinfluenceuponthede『tructionofthestrongsurface
temperaturelnverSlon.
ConsequentlytheblockingphenomenaintheArctichavethreekindsof
contributiontoproducewarm-coreevents:1)thewarmairmassinsidethe
blockinghighanditssubsidence,2)thestronghorizontalwarmadvectionalong
persistentblockingridges,and3)thefixingofthecyclonetrackthatbreaksthe
surfacetemperatureinversion.
InFebruary,aqueerphenomenoncanbefoundinthenorthwesternpartof
Canadanearthemeridianofl20W.Thisareadoesnotshowahighvaluein
surfacechart(Fig.4d),butitshowsabout40%intheupperlevels(Figs5dand
6d).AsimilarphenomenoncanbeseenoverMongoliainJanuary.Arelatively
largeareaofhighfrequency(above30%ormore)isanalyzedatupperlevels.
Bothareasaresituatedintheinlandregionofthecontinents,andatthesame
time,inthecoreareaofwintercontinentalhighs.Theauthor,thereforeconsiders
thatthisphenomenonmaybecausedbythegradualformationofthicklayerof
90
Warm-CoreEventsoftheArcticWinters
temperaturelnverslon.
Ontheotherhand,wecanseesomeareaswithhighfrequencyvaluesover
theoceans.Theseareascanbedistinguishedclearlyintheupperlevels.One
markedhighvalueareaappearsovertheAtlanticOceanoffthecoastofEurope
inDecember,January,andMarch,butitappearsovertheSubtropicsin
February.Iftheseareashaveanysubstantialrelationsoneanother,itis
noteworthythatthesepeakschangetheirpositiongraduallyfromthenorthtothe
south.Thesepositionsare:
・November:thesouthofGreenland,
●December:thewestofthenorthwesternEurope,
●January:thesouthwestoftheWestEurope,
・February:thewestofAfrica,
・March:thesouthwestoftheWestEuropeagain.
OvertheEastPacificOcean,thesituationisalmostthesameasabove:
●November:thewestofAlaska,
.December:thesouthoftheAleutianIslands,
●January:thewestoftheUSA,
●February:aroundCaliforniaPeninsula,
●March:thewestoftheUSAagain.
Thissituationmaybeastatisticalimageofthemagnitudeofmonthlymean
temperaturevariance.Theauthorthinksthatthisgradualdisplacementofthe
hightemperatureeventsreflectstheseasonalsiftoftheactioncentersandthe
magnitudeofcoldoutbreaks.Thisviewmaybesupportedbythefactthatthe
positionofthefrequencypeakreturnsfromthesouthtothenorthinMarch,the
endofwinter.
5Concludingrernarks
Thewarm-coreeventsoftheArcticwinterappearedintheannualmarchof
monthlymeanairtemperaturesweredetectedbyusingtheNMCoctagonalgrid
dataofthenorthernhemispherefroml966tol987.Thegeographicaldistribution
ofthewarm-coreoccurrencefrequencywasmappedforthesurface,700hPa,and
500hPalevels.Theresultsoftheanalysisissummarizedasfollows;
91
T.UMEMOTO
・Mostcasesofhightemperatureevents(relativelywarmerspellsrepresentedby
monthlymeantemperatures)appearinthemiddleandhighlatitudesofthe
northernhemisphere.Theoccurrencefrequencyismuchhigherinthehigh
latitudesthanthemiddlelatitudes.
・IntheArctic,warm-coreeventsoccurintensivelyinJanuaryandFebruary,but
thedistributionofoccurrencefrequencyisdifferentineachmonth.InJanuary,
thehighfrequencyareaisfromtheBeringSeatoGreenlandthroughthe
CanadianArctic.InFebruary,itisfromAlaskatotheNorwegianSeathrough
Iceland.
・Theabovegeographicalfeaturesareincommonamongthreelevelsofthe
troposphere(surface,700hPa,and500hPa).
Theauthorproposestwocausesofwarmspellsmakingwarm-coreevents:
1)warmanticyclonescutofffromblockingridgesthatdriftintotheArctic
Basin,and2)thelarge-s6alewarmadvectioninthenortheasternsideofthe
IcelandicandAleutianlows.
REFERENCES
Colucci,S.J.,1985:Explosivecyclogenesisandlarge-scalecirculationchanges:
Implicationsforatmosphericblocking。 ノottrnaloftheAtmosphericS`iences,42,
2701-2717.
Dole,R.M.andN.D.Gordon,1983:Persistentanomaliesoftheextratropicalnorthern
hemispherewintertimecirculation:Geographicaldistributionandregionalpersistence
characteristics.ルfonthlyIpVeather1~et/iew,ll1,1567-1586.
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93
T.UMEMOTO
【要旨】
北極域の月平均気温変化に現れる冬季のウォームコア現象
梅 本 亨
極地 の 冬 は長 い が,気 温 が 低 下 し続 け るわ け で は な い。 中緯 度 で は 真 冬 の一 ヶ月 を 谷 底 とす
るV字 型 の 気温 変化 グ ラ フ とな るが,極 地 で は早 い時 期 に気 温 が底 を 打 ち,鍋 底 状 のU字 型 と
な る。 これ を コ ア レス ウ ィ ン タ ー とい うが,そ の 中 に暖 か い 月 が 出現 す る こ とが あ り,ウ ォー
ム コア現 象 と呼 ん で い る。北 極 圏 で は 探検 時 代か ら気 象 学 者 に注 目 され た 現象 だが ,こ れ まで
に提 出 され た成 因 に は 多 くの難 点 が あ る。 また,南 極 大 陸 に も ウ ォー ム コ アが 出現 す る が,大
陸 氷 床 上 の斜 面 滑降 風 に よ る逆 転 層 の破 壊 が 主 因で あ る点 で 北 極 域 とは異 な る。 本 論 で は,北
極 域 の ウ ォー ム コア を,中 緯 度 の大 規 模 な寒 波 と対 を 為 す 現 象 と して捉 え る。 そ の発 生 原 因 は
大 気 の作 用 中心 とブ ロ ッキ ング リッジ が も た らす 総 観 規 模 の 暖 気 移 流 で あ る と の仮 説 を立 て,
ウ ォー ム コア の 出現 頻 度 の地 理 的 分 布 に よ って これ を 検 証 す る。
使 用 した 気 温 デ ー タ は,北 極 圏 の対 流 圏 全 体 で 長 期 に わ た り信 頼 の お け るNMC(National
MeteorologicalCenter,USA)の 北 半 球 八 角 形 グ リ ッ ドデ ー タ で あ る。 冬 季 に お い て前 後 の 月
よ り高 温 と な った 格 子 点 を1965-66年 か ら1986-87年 の22冬 に つ いて 求 め,そ の 出 現 頻 度 を 地
上,700hPa面,500hPa面 につ い て月 別 に 示 した。 そ の結 果,ウ ォー ム コ アは 北 極 域 の1月 と
2月 に よ く発 生 す るが,1月 に は 北 ア メ リカ大 陸寄 りに,ま た2月 に は ヨ ー ロ ッパ 寄 りに,い
ず れ もブ ロ ッキ ン グが 多 発 す る領 域 を 中 心 に 分 布 す る傾 向 が 明 らか で あ る。 この 特 徴 は,各 高
度 に 共通 す るの で,必 然 的 に 総 観 ス ケ ール で 背 が高 く順 圧 的 な構 造 を もつ 暖気 移 流場 の存 在 を
示 唆 す る 。 よ って,ウ ォ ー ム コア の 主 因 は ブ ロ ッキ ング と作 用 中心 の相 互作 用 に よ る暖 気 移 流
効 果 で あ る と結 論 した。
な お,本 論 は 人為 的 な 温 室効 果 ガ ス の放 出 に よる いわ ゆ る地 球 温 暖化 問題 と は視 点 を異 に す
る こ とを 明記 して お く。
キ ー ワー ド:ウ ォー ム コア,コ ア レス ・ウ ィ ンタ ー,北 極 圏,ブ ロ ッキ ン グ,気 温
94