T 'tl I CO2 GREENHOUSE UPDATE 1985 o Lamont-Doherty Research . CRSL Research + Contribution to DOE State of the Art Report * Oceanic effects on transient climate change o Budget Status, Proposal o DOE and other reports o Recent research developments October 4, 1985 New York City B. P. Flannery rt LAMONT-DOHERTY PROGRAM 1985 PROGRESS REPORT SEASONAL STUDY OF THE CO2 AND TRACER DISTRIBUTIONS IN THE HIGH LATITUDE ATLANTIC, W. Broecker and T. Takahashi . Goal: gain better understanding of the air-sea exchange of CO2 in high latitude surface waters . First systematic study of seasonal CO2 chemistry in North Atlantic o Field studies complete March 1985 . Related studies + North Pacific (DOE support) + South Pacific (EXXON, DOE) .t SAMPLING POSITIONS IN THE NORTH ATLANTIC . Transport Freight Limited ships, Greenland stations EXXON/IFL N()BIH RILRNIIC PNOJECI LARGE SEASONAL VARTATTON rN P(CO2) r9 MAMJ E o :L AI 83 t984 - ----*7t"*-----14 EFFECT OF CIIANGE IN o o oBs€RV TETllP CORR€CTED E { N o () ar . --+I----+-- 4-r---i-::--------n- €FFECT OF CHANGE IN ESERVE0 6B.N Previously only summer data available, low values assumed to persist all year PRINCIPAL FINDINGS, CONCLUSIONS . Large, unexpected seasonal variation in P(CO2) in high latitude surface waters . Standard thermodynamic models for CO2 variation cannot explain observations + Biology and mixing required . lmplication for CO2 uptake by ocean two sided + Lower exchange from air to surface ocean + Higher exchange from surface to deep water . Results need to be assessed in quantitative oceanic carbon cycle models of AVATLABLE COMPTLATTON OF OCEANTC p(CO2) . GEOSECS data (Atlantic 72, Pacific 73, lndian 78) ff ffi 60 80s . No information on seasonal variation . Much additional data acquired, but not compiled " LAMONT PROPOSAL 1986: SEASONAL AND GEOGRAPHICAL MAP OF P(CO2) tN SURFACE WATERS o Compilation of seasonal P(CO2)map + All available data + 10 x 10 degree grid * February, August . Objectives + Differentiate regional behavior, important effects + Develop a seasonal modelto explain variation + Re-examine oceanic carbon cycle DOE STATE-OF-THE-ART REPORT MODEL PROJECTIONS OF TIME DEPENDENT RESPONSE TO INCREASING CARBON DIOXIDE MJ. HOFFRERT (NYU) and B.P. FLANNERY . Observational data for modern climate (1850-1980) . Elements of transient climate models . Disagreement among results for steady state models . Hindcasting for model verification e Forecasting of future change, first effects r Conclusions and Recommendations HISTORICAL DATA FOR TRANSIENT MODEL VERIFICATION VARIATION OF GLOBAL MEAN TEMPERATURE 1880.1980 i[iv o to :i..: iYj ..--.- 5r.rn.l.ltB2l r/'tnnltr n.l- ltsol -{r3 1880 r89s r0t0 t025 r0a0 rg55 r0ro r0E5 YEAR . . Temperature change +0.5 C (1980-1880) Factors besides CO2 must operate * volcanoes, solar variability, oceanic upwelling o Other archived data exist, Sea lce, Regional Temperature, + Less reliably predicted by models + Display more variability, as measured ... ELEMENTS OF STEADY STATE AND TRANSIENT MODELS ATMOSPHERE fa.ra3l.r!l Sadranon Haor t{t, o!, corr orr atc. Ar..brornass .tand A .rc! CouPhng Couol'n! H€ar €rcha.g€ ll lc€.Oc..n'f v w,nd Str€ss gtot ASS Armosph.r€.Oc€lnCoupt, Ch.ngos ol L.^d Fs.lv.es. Oro!'.phy. Veg€r.r'on. Ch.nges ot Oc.an aas'n Shap.. Saln'lt. alc Steady State response CO2 addition lR decreases, temperature rises + Additionalfeedbacks - Atmospheric water vapor - Snow/ice cover - Cloudiness amounts, types * r Transient evolution, timescales +Land, 1 week +Atmosphere, 1 month +Ocean mixed layer, 8 yrs +Deep ocean,(1 -.10) thousand yrs GENERAL CIRCULATION MODELS DISAGREE ON STEADY STATE RESPONSE 2xCO2 DOUBLED CO2 -----.-.-. -.trl (, sz(J !.r t F d. u.l c! a L..L l rtr...f rFl. I t r-t 3.I{a. a IOr CFr. Curl td-tn a r...t tr..a Cba.t Ll.-.ar ltatl Itfnt lttll arlll, ,irb.. rtat, t ltrr , I , I I , it . Basic results + Global mean temperature rise 1.5-4.S C * Warming greater at poles . Major disagreement between models . Sources of disagreement + Treatment of oceanic transport * Treatment of cloudiness feedback ar, = F . Recent models show 4-5 C Global warming + lnclude other trace gasses HTNDCASTTNG RESULTS/ VER F CAT ON Nod.l Obla.vationt Modsl F. , a o O - Obaorvetion. t i.a 't (J -0 r, )- I I 4.2 \t.' o Modal: aun + CO2 + volcrno.r tro oo \J HANSoN -0.4 !+, o9 a o (r980) a a o a GILLILAND (I982) a aa -0.5 a 1880 1900 1920 1940 YEAR r Models claim to detect CO2 effect, but required other types of forcing volcanoes, solar variation, (oceanic upwelling) * o Spurious agreement in conclusions + Treatment of forcing differs * Observational data differs o Consensus view CO2 warming not yet confirmed by observation 1960 1980 FORECASTING RESULTS/ PREDICTION AND FIRST EFFECTS . Requires forecast of future CO2 emissions . Ocean delays CO2 warming + As yet unrealized warming could be substantial %)v:*::"i". v%1////t o Results from General Circulation Model still unavailable + lnclusion oceanic transport challenging task coNcLUS roNS/RECOMMENDATTONS o Modern climate is forced by factors other than CO2 . . Oceanic response delays warming by at least 10 years Consensus prediction 1 C warming (1860-200 O), 2-5 C (2100) o To date models do not provide unique forecasts . Model development: + * + GCM results display substantial discrepancies Research requires a hierarchy of climate models Reliable GCM results are at least 10 years away o Must develop improved understanding of oceanic transport o Must develop observationally based strategies for model verification CR RESEARCH 1984-85 . Continuing role in the environmental impact assessment of the Natuna Gas Project . Preparation of the "Transient Climate Models" chapter of the DOE State of the Art Report on CO2 Research . Role of oceanic effects on climate change + Collaborative development of a sophisticated + Balance Climate model (Livermore, NYU) Studies of thermal lag from oceanic effects Energy EMERGING DILEMMA FOR CLIMATE MODELS: WHY HASN'T WARMING BEEN OBSERVED? . Recent GCM models predict greater sensitivity warming 2xCO2 (1 850-1 980) 2-3 0.8 C marginally detectable 4-5 1.6 C readily detectable C C . Proposed solution, delay from oceanic thermal buffering much greater than found in previous studies . Requires strong thermal coupling between surface and deep ocean MODELS INCLUDING ENERGY TRANSFER TO DEEP OCEAN PREDICT LONG DELAYS FOR ATMOSPHERIC WARMING . Purely Diffusive (PD) Model (Hansen 1984) 5 Response to lnslant Ooubling ol COz (squrlibllum sensalivlty : 4 zoo) 4 65 g' / z-2 ./rr}^-/.a / ....'. mrr.d loy.r hlot copocily mrrad loycr + lhcrrnochna (t,icmzs-rl ,/ //...........,::j I ..::;. ' j::j:j-'..::::..::::.... "' 15 35 20 Yeors o Pattern of global response Average lag time 125 years * 90 60 50 o -!o -60 -lto -r80 ::::::' -rao -60 0 Lonqrlirde (degrees) 60 THE UPWELLING DIFFUSION MODEL FOR HEAT TRANSFER INTO THE MIXED LAYER AND DEEP OCEAN . Schematic of model (Hoffert, Callegari, Hseih 1gg0) l-.4D. -r I . Timescales + Mixed layer heat exchange, + Diffussion time 5000 years + Upwelling time 1000 years 10 years (heat capacity) b ta@o uPWzulNG DlFFusloN (uD) nxo punEr-v orrrusrvE (pD) M.DELS o Orrent climate, average surface temperature 15 C u a, ,r a o L cl A E Fa, Doptb (mobrs) e lvlodels with 3 C strface warming IJ a, r. a 6 L e, A E e, F Dopth (mcton) COMPARISON OF STEADY STATE SOLUTIONS UPWzuING DIFFUSION (UD) AND PUREr-V Orr_rUSrVE(PD) MODELS o Curent climate, average surface temperature 15 C U: ) o9 K= 3000 A E Dopth (m€tors) o Temperature change vs depth for 3 C surface warrning + PD models require maximum heating o q I u a o t E llDlns l-_- Deptb (motors) TRANSIENT EVOLUTION, COMPARISON WITH HANSEN o Addition of upwelling decreases response time rJ t: E u t) J a a, E Tlmc (:rccrr) . Recalibrate Diffusion coefficient using UD model () at g a A u . Lag time decades o t t, a, E llmc (ycars) HISTORICAL AND FORECAST CO2 INCREASE 1850-2100 o CO2 record and forecasts from Weubbles (SOA Report) E A A a o () Hi& o Corresponding change in equilibrium temperature +AT=AT(2xCO2)xln(CO2 ppm/540 ppm) u F Lor Datc TEMPERATURE CHANGE WITH UD MODEL W=4 K= 3000 AT(2xCor)= 2.5 . Surface temperature variation + Lag time 30 years in 1983 but increases with time (poorly defined concept) O ol CO, ! a 6 L e, A E ql F IJ (, . Profile of ocean warming (year 2100) Nominal U q 6 E () lY= 4 K= 3000 AT(2xCor)= 2.5 Nominal CO" Year 21OO ' i,,r a d L a, A E 0, F Depth (meters) TEMPERATURE CHANGE FOR VARIOUS CO2 FORECASTS . Surface temperature variation + (1850-1985) 0.52 C + 1 C warming (2007, 2018,2033) . Lag time decades, not hundreds of years W=4 K= 3000 AT(2xCO.)= 2.5 CONCLUSIONS FROM 1D OCEAN MODEL . Purely diffusive models overestimate response time lmproper steady state solution + Overestimate diffusion coefficient . Lag time poorly defined concept to express delay in warming caused by oceans * . Response delayed by decades, 30 years, not centuries . Simple models can contribute to understanding of oceanic effects CR PROGRAM 1986 . Present results Transient Climate models Ocean modelling conference Woods Hole late 1985 Manuscript in preparation 0 Continuing development of Coupled atmosphere ocean EBM . Menitor research and reports (80A) I I CO2 GREENHOI.JSE BUDGET, PROPOSAL Projected CR EFFOFf, Professional time Consultants/R.rchased Research Travel Other TotalCR Lamont-Doherty Total 1985 K$ Proposed 1986 K$ 132 '140 14 7 35 4 10 5 157 190 93 60 250 250