GEOPHYSICAL RESEARCH LETTERS, VOL. 23, NO. 1, PAGES 57-60, JANUARY 1, 1996 The 1990-1995 El Nifio-Southern Oscillation event: Longest on record Kevin E. TrenberthandTimothyJ. Hoar NationalCenterfor Atmospheric Research, Boulder,Colorado Abstract. The tendencyfor morefrequentE1 Nifio events and fewer La Nifia eventssincethe late 1970's has been linked to decad•l changesin climatethroughoutthe Pacific basin. Aspectsof the most recentwarmingin the tropical Pacific from 1990 to 1995, which are connectedto but not Americato the InternationalDateline. It is the basin-scale phenomenon,however,that is linked to globaJatmospheric circulationand associatedweatheranomalies.The primary responsein the atmospherecoupledto EN is the SO and, together,the tropical Pacific warm eventsare often referred synonymouswith E1 Nifio, are unprecedentedin the climate to as ENSO events. record of the past 113 years. There is a distinction between E1 Nifio (EN), the SouthernOscillation(SO)in the atmo- The Southern Oscillation sphere, and ENSO, where the two are strongly linked, that emergesclearly on decadal time scaJes.In the traditional E1 The SO has a time scaleof 2-7 yearsand consistsof a globalscale, predominantly standing wave with centersof action in Nifio region,seasurfacetemperatureanomalies (SSTAs)have waxed and waned, while SSTAs in the centra• equatorial Pa- surfacepressureover Indonesia and the tropical South Pacific cific, which are better linked to the SO, remained positive (seeFig. I of Trenberth and Shea1987). The nature of the from 1990 to June 1995. We carry out severalstatisticaJtests oscillation can be seenfrom the inversevariations in pressures at Darwin (12.4øS130.9øE)in northernAustraliaand Tahiti (17.5øS149.6øW) in the South Pacificwhoseannualmean part of a natural decadal-timesca•evariation. One test fits an pressures are correlatedat -0.79 (Trenberth1984). Thesetwo autoregressive-moving average(ARMA) modelto a measure stationscan be optimally combinedinto a SO index, $0I -of the SO given by the first hundred years of the pressuresat TN- DN whereT andD referto the departurefromthe long- to assess the likelihood that the recent behavior of the SO is Darwin, Australia, beginningin 1882. Both the recenttrend term monthly mean sea level pressuresat Tahiti and Darwin, for more ENSO events since 1976 and the prolonged1990respectively,and the subscriptN refers to an appropriate 1995 ENSO event are unexpectedgiven the previous record, normaJization. with a probability of occurrenceabout once in 2,000 years. Becausethere are many small scale and high frequency This opensup the possibilitythat the ENSO changesmay be phenomena.in the atmosphere that can influence the prespartly causedby the observedincreasesin greenhousegases. suresat Tahiti and Darwin, such an index contains noisethat doesnot reflect the global-scaleSO. A primary sourceof high frequency variability arises from the 30-60 day intraseasonaJ Introduction The recent warm event related to E1 Nifio in the tropical Pacific from 1990 to June 1995, is the longest on record since 1882 by some measures. It occurs in the context of a tendency for more frequent E1 Nifio events and fewer La Nifia oscillation(Madden and Julian 1994). A measureof noise SON - T•v 4- D•v (Trenberth1984)indicatestimeswhen Tahiti and Darwin are not varying in opposition as observed in the SO (Fig. 1). Taking accountof the signal-to-noise ra- tio and the coherenceof the Darwin and Tahiti time series, the SOI is optimized as an indicator of the SO by applying changesin climate throughoutthe Pacific basin (Trenberth a low-pass 11 term filter that eliminates fluctuations of less 1990, Trenberth and Huttell 1994, Kumar et al. 1994, Gra- than 8 monthsperiod but mostly retains periodsexceeding24 events since the late 1970's that has been linked to decad•l ham 1995). In assessing how unusualthe recentevent and months(Trenberth1984). The ratio of the variances of these the past two decadesare, due considerationmust be given to two serieschangesfrom 2.0 for monthly data to 6.4 with the whichregionsof the tropical'Pacific seasurfacetemperatures filtering, and the filtered SOI retains56% of the monthlyvari(SSTs)are mostimportant,their link to the atmospheric cir- ance. Accordingly, an appropriate normalization is the annual culationcomponent knownasthe SouthernOscillation(SO), meanstandarddeviationof eachtime series(Trenberth1984). and the integrity and signaJ-versus-noise ratio of any index or measureof the SO. Given that the changesare unlikely in the context of the natural variability as revealed by the previous record, this may be evidenceof climate changerather than simply an unusually long fluctuation. The Tahiti recordis lessreliable and containsmissingdata prior to 1935. Tahiti and Darwin monthly(annual)pressure anomaliesare correlated-0.35 (-0.77) for 1935 to 1995 but -0.19 (-0.36) for 1882to 1934yet the SO wasstronglyin evidencefrom otherstationsduringthe earlierperiod(Trenberth E1Nifio (EN) refersto the occasional %nomaJous" warming and Shea1987). Th• only long-termhomogeneous recordof of the eastern tropical Pacific Ocean but is commonly linked the SO is givenby tie appropriatelyfilteredpressures at Darto a basin-scalewarming extending from the coast of South win (Fig. 2). This recordis usedto judgethe degreeto which the behavior in recent years is anomalous. Copyright1996by theAmericanGeophysical Union. E1 Nifio-Southern Papernumber95GL03602 Oscillation To explore the coupling between the atmosphereand the ocean in ENSO events, we make use of the "Nifio" regions 0094-8534/96/95 GL-03602503.00 57 $8 TRENBERTH AND HOAR: THE 1990-1995 ENSO EVENT: LONGEST ON RECORD 0.5 .0.5 -1.5 1.5 0.5 -0.5 -1.5 Raw noise 1.5 t 0.5 -0.5 :• -3 1930 ,, i, .... i,,,,1 1940 .... Smoothed noise i,,, 1950 1,,,,, I,,,,, .... 1960 i,,, 1970 -1.5 .... ,, I,'''''''' 1980 I ''1''- 1990 1055 Year Figure 1. Time seriesof the SOI (normalizedTahiti minus Darwin sea level pressureanomalies)signaland a measure of noisein the SOI given by SON (normalizedTahiti plus Darwin) with baseperiod 1950-1979.The top two showthe SOI, monthly and filtered, the lower two showthe SON. The filtered seriesreveal the interannual fluctuations;note the different scalingson the ordinate. 1960 1965 1070 1075 1980 1985 1990 1995 Year Figure 3. Time seriesof Nifio areasSST anomaliesfrom 1950 through September 1995. The areas coveredare Nifio [1+2]: 0ø-10øS 90øW-80øW, Nifio 3: 5øN-5øS, 150?W90øW, and Nifio 4: 5øN-5øS, 160øE-150øW. tivelyregardedasindependent thenthe 5%significance levelis 0.30. Alsoapparent(Fig. 4) is the strikingboomerang-shaped oppositeSST anomaliesextendinginto the extratropicsof from the Climate DiagnosticsBulletin and SSTs from the each hemisphereand the coastalinfluencealong the AmerClimate AnalysisCenter. In the traditional E1 Nifio region, icaswith the samesignas the tropicalPacific. Therefore,the Nifio [1+2] SST anomalies (SSTAs)havewaxedandwaned, SSTs most involved in ENSO are in the central Pacific, not while Nifio 4 SSTAs,like the SOI, haveremainedpersistently in the coastalwatersoff of Peru and Ecuador(Trenberthand anomalous in recentyears(Fig. 3). Correlation coefficientsfor 1951 to April 1995 betweenthe Shea1987,Deserand Wallace1987,Ropelewskiet al. 1992). The importanceof the SO has variedin the past hundred years: strong variations'from 1880 to the 1920sand after smoothed (rawmonthly)SOIandthemonthlySSTAs(Fig. 3) are-0.61(-0.48),-0.81(-0.65)and-0.84(-0.68)forNifio[1+2], about 1950 and, except for strong event during 1939-1942, weakervariationsfrom the mid-1920sto 1950(Trenberthand Shea1987) (Fig. 2). Note the lackof decadalor longer-term equatorialPacific. Nifio 4 and Nifio [1+2] SSTAsare corre- variability until recentyears. The trend for a negativeSOI aflated 0.49 over the same period. Commonly, SST increases ter 1976is apparent(Figs. I and 2) andsetsthe stagefor the occurred almost simultaneously from South America to the very persistentwarmingoverthe past five yearsin the vicinity Dateline} so the distinctionbetweenwhich regionmost influ- of the equatorand the Dateline (Fig. 3). It is importantto encesthe atmosphere has not been easy to make. In recent distinguishthis phenomenonfrom the coastalE1 Nifio. years,this has not beenthe case(Fig. 3). The correlations Usingthe smoothedSOI time seriesin Fig. 2, the previous Nifio 3 and Nifio 4, respectively,demonstratinghighly statistically significantcorrelationsthat are strongestin the central between the smoothed SOI and monthly SST anomaliesfrom longest continuous ENSOevent,fromearly-1911 to mid-1915, 1950to 1994(45 years)(rig. 4) are strongest, exceeding -0.8, lasted 4.1 years. The longestinterval of oppositesign lasted in the region120øWto 180,5øNto 10øS,whichstraddlespart 5.0 years,from May 1906to April 1911. The currentevent,by of the Nifio 3 and Nifio 4 regionsand extendsfarther into the this measure,beganin October1989 and continuedthrough Southern Hemisphere. If only one value per year is conserva- June 1995, 5 years 8 months. When the Nifio 4 SSTAs are used as a measure,positive valuesbegan in September1989 andcontinuedthroughJuly 1995;valuesexceeded 0.3øCfrom January1990throughJuly 1995exceptfor a shortbreakfrom Februaryto April 1994(relativeto a 1950-79mean). ,o. S•••••:•i•:...'-:•.'..• [:!: B•i:•:!:•-'.'•-!• :•!-:•.. :i: , I ' '"''"':•!...:'•i i::i•ii*:'"•j• ::"'*':"':'•:'•:•. •i::'.'!:i:!:i•'.-.: " 20N Figure 2. Time seriesof the monthlynormalizedSouthern Oscillation Index(minusDarwinsealevelpressure anomalies) smoothedwith the l 1-term filter and with a low passsmoothing spline filter that removesperiodslessthan 10 years. A 1-2-1 filter is used on the end points and the last value is September 1995. 40SI00E 120[140[160[ 180 160W 140W 120W 100W 60W60W' Figure 4. Correlationsof the smoothedSOI with monthly SST anomaliesfor January 1950 to December1994 (540 months).Magnitudesexceeding0.3 are shadedor stippled. TRENBERTHAND HOAR:THE 1990-1995ENSOEVENT: LONGESTON RECORD Statistical 59 tests To test whether the recent SO behavior is statistically un- likely,a numberof testsare performed.We identifythe seasonsas December-January-February, DJF, and so on. The 22 I ! I If I I I I seasonalmean anomalies at Darwin from DJF 1989 to MAM 1995are all positiverelativeto the 1882-1981mean. The next longestpositiverunsobserved are15seasons fromMAM 1894 to SON 1897,12 fromDJF 1981-82to SON 1984,and 11 from 0 50 1O0 150 200 250 300 350 400 Season SON 1939 to MAM 1942. The longest run of oppositesign Figure 6. lasted 13 seasons from MAM 1973 to MAM 1976. We first use a t test for the difference between the means of Observed (top) from 1882to 1981and simu.. lated(bottom)100yearsequences of Darwinseasonal pressure anomalies. Note the additional noisecomparedwith the two periodsunderthe null hypothesis that they arethe same, filtered values in Fig. 2. modifiedto accountfor the strongpersistencein the SO time series.In determiningthe standarderror of the meanfor the SOI, the time neededto gain an extra degreeof freedomor, wherethe at is a Gaussianwhite noiseprocessat time t with effectivelythe time betweenindependentobservations,is 6 zero mean and variance era 2 _ 0.435 mb2, andthe y is the months(Trenberth1984). For December1989to May 1995 syntheticDarwinseriesof seasonal anomalies, t is in unitsof (66 months)versusJanuary1882to November 1989(1295 seasons,and all units are in mb. months),the resultis t - 2.82with an estimated225degrees The estimatedpower spectrumof the Darwin seasonal of freedom,significantat 0.5% with a two-tailedtest. anomalies for 1882-1981(Fig. 5), whichrevealsa broadspecSimilarly,for March 1977-May 1995 (219 months),the t tral peakfrom3 to 7 yearsperiodin the SOI, is seento havea statistic is 2.68; significantlydifferentfrom the mean for the verygoodfit with the theoretical ARMA spectrum (c.f. Chu 1142 months in the rest of the series at • 1%. andKatz 1989),whichfeaturesa broadpeakat 4.2 yearspeThese tests provide a ballpark indication, but are con- riodicity. Of particularnote for the currentexercise,is the founded somewhat by the persistencein the time series. A excellentagreement in powerat very low frequencies.This more comprehensive test fits an autoregressive (AR) mov- modelis usedto generateover 1,000,000yearsof synthetic ing average(MA) or ARMA modelto the time seriesof sea- recordand the first 1,000yearsare discardedbecauseof possonalDarwin pressureanomaliesfor the first hundredyears siblespinupeffects. The remainderis usedto estimatethe of record(1882to 1981). The modelis then usedto generate probabilityof eventssuchasthoserecentlyobserved. A comsynthetic time seriesfor testing. parisonof 100 yearsof modeloutputwith the observed first The ARMA model for Darwin can be compared with one 100 yearsof Darwin (Fig. 6) revealsthe similarcharacterof based on a much shorter period for the SOI Tahiti minus the variations;notethreesequential strongsimulated"ENSO Darwin by Chu and Katz (1985) who found a best fit with events"3.5 yearsapart betweenseasons200 and 250, quite an AR(3) processfor seasonal values.Our bestfit modelwas similar to the observed1939-42event (near season240, top foundusinga maximumlikelihoodfitting procedure(Jones curve). 1980)andAkaike's Information Criterion(AIC)(Akaike1974) Because the results indicated we were dealing with rare which invokesa performanceand penalty functionrelatedto the number of parameters in the model; the most parsimo- events,we testedthe sensitivityof the resultsto variantsin the model. Minor changesarisingfrom differentinitial states nious model is one with a minimum in the search for the ARMA coefficientsmade insignificant in the AIC. The model selectedis an ARMA (3,1) (of order3 for the AR process and 1 for the MA), givenby Yt -- 1.278yt_• - 0.318yt-2 - 0.136yt_a+ at - 0.712at_1 Period 101 ß/ / - Seasons ,'-- 1•;00 ,5.?0 ;•.,3;• 2.,50 2.00 • • Bandwidth differences.Somewhatlarger differences wereproducedwhen the model was based on either the first 95 or 105 years of record instead of the first 100. In both cases,the spectrumof the ARMA best-fit model had slightlymorepowerat periods longerthan 20 years. The 105-yearmodelis basedon data through1986 whichincludesthe 1982-83ENSO event, the largeston record. Becauseit overlapsconsiderably with the 1977-1995periodthat we wish to test, it is considered less reliable. \l \•, /- /'• 10 • / \/ \ ..-.• ---/ /'\ \/ I ' The longestrun of simulatedvaluesof one sign was 31 seasonsand 113 .runs of either sign equalledor exceeded22 seasons, indicatingan incidenceof 1 "observed" eventin about 8,850 years. From this standpoint,the model suggeststhat the continuouspositiverun for the most recent22 seasonsis extremelyrare. In the alternatemodels,the numbersof runs of 22 seasonsor more were 144 and 154, so that the most Frequency- Cycles/Season Figure 5. Estimatedpowerspectrafor Darwinseasonal conservative estimate is for one such run about every 6,500 years. anomaliesfrom 1882-1981(heavy) and the corresponding The mean Darwin anomaly relative to 1882-1981 for the spectraof the ARMA(3,1)bestfit model(thin) . A loga- the last 22 seasonsis 0.94 mb. From the model, it was deterrithmic vertical scaleis usedso that the 95% confidenceband mined that the median 1 in 1000 year threshold for 22-season (dashed) is constant in width,whiletheabscissa is linearin eventsof either sign was 0.88 mb, and the 1 in 10,000 year frequency. The bandwidth of the Parzenwindow(with 60 threshold .was0.99 mb, indicating a frequencyof occurrence lags)is plotted. of the observedvalue of 1 in 3,000 years; or about 1 in 545 60 TRENBERTH AND HOAR: THE 1990-1995ENSO EVENT.: LONGEST ON RECORD 22-season intervals(0.18%). Given100trials of 10,000years, in greenhousegasesin the atmosphere?Or is this pattern the samplingfor 1,000year eventsindicatesan interquartile natural decadal-timescale variation? We have shown that the rangeof 0.86 to 0.91 mb, and the rangeis 0.80 to 0.99 mb. The latter is highly unlikely. median return periods of the observedvalue in the alternate modelswere 1,648 and 1,137 years. Acknowledgments. NCAR is sponsored by the National For the last 73 seasons from MAM 1977to MAM 1995,the Science Foundation. We thank Dennis Shea and Chris Guillemot observedmeananomalyis 0.50mb. From73-season sequences for help with the figures and datasets, and Richard Jones for help in the model, valuesof 0.48 mb and 0.52 mb are reachedonce in fitting the ARMA models. This researchis partly sponsoredby every 1,000 and 10,000 years, respectively,and the observed NOAA under grant NA56GP0247 and by the GeophysicalStatistics valueis obtainedabout onceevery 2,000 yearsor about I in Project at NCAR under grant NSF DMS9312686. 110 suchsequences (0.9%). The resultsfrom the alternative References modelsgivereturn periodsof 2,400 and 1,390years. In all cases,the shortestreturn periodsoccurfor the model Akaike, H., A new look at the statistical model identificabasedupon 1882-1986,as expected.For the 73-season case, tion. IEEE Trans. Auto. Control, 19, 716-723, 1974. the longestreturn periodis for the modelbasedupon 1882- Chu, P-S., and R. W. Katz, Modelingand forecastingthe 1976,the onlymodelthat wasnot basedonpart ofthe period Southern Oscillation: A time-domainapproach. Mon. of interest. Wea. Rev. 113 1876-1888, 1985. Chu, P-S., and R. W. Katz, Spectralestimationfrom time series models with relevance to the Southern Oscillation. Discussion J. Climate 2, 86-90, 1989. The resultsfromthe t testsindicatethat the lowfrequency Deser C., and J. M. Wallace, E1 Nifio events and their revariability and the negativetrend in the SOI in recentdecades lation to the SouthernOscillation.J. Geophys.Res.,92, 14189-14196, 1987. are quiteunusual;the recentsequence wouldbe expectedonly aboutoncein 1,100years.The ARMA modelingrefinesthis Graham, N. E., Simulationof recent global temperature estimate and indicates that the likelihood of occurrence of trends. Science,267, 666-671, 1995. the 1990-95ENSO, gi•:enthe first hundredyearsof record, Jones,R. H., Maximum likelihoodfitting of ARMA models is aboutoncein 1,500to 3,000years.The changebeginning to time serieswith missingobservations.Technometrics, 22, 389-395, 1980. about 1976 toward more frequentENSO eventsis also unlikely,abouta oncein 2,000yearexpectation.Clearlythe two Knutson,T. R., and S. Manabe, Time-meanresponseover are not independentand the resultssuggesta non-stationary the tropicalPacificto increasedCO2 in a coupledoceaninfluencesuchas wouldarisefrom a changein climate. atmospheremodel. J. Climate 8, 2181-2199, 1995. Severalaspectsof the decadalchangebeginningaround Kumar, A., A. Leetmaa and M. Ji, Simulations of atmo1976 have been simulatedwith atmospheric modelsusing sphericvariability inducedby sea surfacetemperatures and implicationsfor globalwarming. Science,266, 632specifiedSSTs (Kumar et al. 1994, Graham1995)includ634, 1994. ing patternsof surfacetemperaturechangeobserved in recent years over land. These and other studiesconfirm that the atmosphericchangesare tied to the changes in SSTsand, fur- Madden, R. A., and P. R. Julian, Observationsof the 40-50 daytropicaloscillation-A review. Mon. Wea. Rev. 122, ther,that the changes overthe NorthPacificandsurrounding 814-837, 1994. areas are substantially controlled by the anomalousSST forc- Ropelewski, C. F., M. S. Halpert, and X. Wang,Observed ing from the tropicalPacific,and thuslinkedto the changes troposphericbiennialvariabilityandits relationshipto the in ENSO. Accordingly, the key questionis whythe SSTs,and SouthernOscillation. J. Climate5, 594-614, 1992. especiallythe tropicalPacificSSTs,havechangedin the way Trenberth, K. E., Signal versusnoisein the SouthernOscilthey have? lation. Mon. Wea. Rev., 112, 326-332, 1984. No currentcoupledglobalclimatemodelprovidesa fully Trenberth, K. E., Recent observed interdecadal climate realisticsimulationof ENSO eventsalthoughsomemodelsrechangesin the Northern Hemisphere. Bull. Amer. Meproduce aspectsof the observedbehavior but with reduced teor. Soc., 71,988-993, 1990. amplitude.Thusthereis little basisfor expecting that there Trenberth,K. E., and J. W. Hurrell,Decadalatmospherewill be an increasein the numberand/or lengthof ENSO oceanvariationsin the Pacific. Clim. Dyn., 9, 303-319, 1994. eventsfromcoupledatmosphere-ocean models,although modelsdo predictSSTwarmingwith increased greenhouse gases Trenberth, K. E., and D. J. Shea, On the evolution of the (KnutsonandManabe1995),sothat the background mean SouthernOscillation.Mon. Wea. Rev.,115, 3078-3096, 1987. is changed.In morelimitedmodelsdesigned specifically for simulatingENSO in the Pacific,the prolongedENSO hasnot been well predicted by models which have otherwisedemonstratedskill in predictingENSO events(seerecentissuesof NOAA's Experimental long-lead Forecast Bulletin and Climate DiagnosticsBulletin). These results raise questions about the role of climate change.Is this patternof changea manifestationof the global warmingand related climate changeassociatedwith increases K. E. Trenberth and T. J. Hoar. Climate and Global Dynamics Division, National Center for Atmospheric Research, P.O. Box 3000, Boulder, CO 80307-3000. (e-mail: [email protected]) (received August,21, 1995;revised October9, 1995; acceptedNovember13, 1995.)
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