Annals ofGlaciology 27 1998 © International Glaciological Society Implications for the interpretation of ice-core isotope data from analysis of modelled Antarctic precipitation D. NOO NE, I. SIMMON DS School of Earth Sciences, University of Melbourne, Parkville, Victoria 3052, Australia ABSTRACT. By co nsider a tion of m odel- ge ne ra ted a tmosph eric da ta, domin a nt anom alies in th e synoptic circul ation patterns a re observed under conditions of high Antarctic precipitation. T hi s is associated with strong moisture advecti on of m a rine origin. Examining precipi ta tion at individu al locations reveals a strong rel a ti onship between local surface temperat ure a nd precipitation a mount. Days with > 5 mm of precipita tion (which, on average, corresponds to about 8 % of days over Anta rctica) have surface temperatures that a re a round 10°C warmer tha n the mean. This bias suggest that abnormal conditi ons a re captured in the ice-core record and that interpretation or reconstruction of palaeotemperatures will succeed only under the possibly fl awed assumption th at similar abnormal condi tions existed at the time of deposition. Although isotopic a na lysis of Anta rctic ice cores has been used successfull y in pa laeocl imate studi es, a compl ete understa nding of the underl ying processes affecting the deposition of the core rem ains to be found. It is reaso ned that by obtaining such a n understanding, it m ay be possible to reconstruct the synoptic cond itions under which accumulation occurred. INTRODUCTION Th e work of Da nsgaard (1964) o n the behaviour of stable water isotopes in precipitation has prompted m any studies of pa laeocl im ates from ice-core data. It is genera lly accepted that the high correlati on between the annual D/H or 18 0 / 6 0 ratios a nd mean ambient temperature can be used directly to infer palaeoclim atic temperatures from ice-core samples (e.g. J ohnsen and others, 1995; Jouzel a nd others, 1996). J ones a nd others (1993) point out, however, that la rge-scale temperature trend s cannot be extrapolated much beyond the locality of the drill-site. T his empirical approach reli es solely on the observationa l d ata rather tha n the physical processes involved. An understa nding of the role of atmos pheric circulation in influencing the isotopic sig nat ure revealed in Anta rctic d rill cores is crucia l to the interp retation of th e core d ata. Wi thout such knowledge, conclusions rega rding palaeoenvironments from a ny typ e of proxy data could be seriously misleading (Taylor a nd others, 1995). T he key to understanding and inte rpreting the isotopic signa ls in ice cores over time is two-fold. First, we must consider the a tmospheric processes th at transport water from a region of evaporati on to the place of precipitation, and secondly, we need to understa nd the processes governing the isotope concentration of th e accumulated water. We wo uld expect, for example, tha t days with precipitation wo uld have greater than average cloud cover and stronger therm a l ad vec tion from lower latitudes. T hi s would influence the local surface temperature. Such co nditi ons are by defini tion anomalous a nd p erhaps not fully representative of mean temperature. Whil e thi has been appreciated for some time in principle (e.g. K ato, 1978; A rista rain a nd others, 1986), littl e a ttempt has been m ade to explain or quantify the uncertainties to which 398 the interpretation of the isotope- temperature relationship is subj ect. To highlight the important as pects of interpretation of the palaeoclimatic signa l at a given locality, we examine here some of the processes invo lved in deposition of water at the drill-site. To perform such a n ana lysis, we need highresoluti on (both spatial a nd temporal) data. Meas urements of d aily precipitation and other atmospheric para meters a re un avail able from the observational network. Therefore, to perform this analysis, we must m a ke use of output from a global climate model with a complex physical representation of the atmosphere. The implications that a comprehensive understanding of the synoptic processes influencing the isoto pic signatu re has for existing pa laeotemperature reco nstructions, and for successfull y estimating the synoptic vari ability of palaeoclimate systems from the ice-core data, a re disc ussed. OVERVIEW OF THE NUMERICAL MODEL The Melbourne University general circulation model (G CM ) is a non-linear, physically based, spectral, primitive equation model and is discussed in detail elsewh ere (Simm ond s, 1985; Simmond s a nd others, 1988; Simm onds a nd Law, 1995). The spatial resolution is defined by truncation of the spectral series at wavenumber 21, roughly corresponding to a 5.6° x 3.3° grid. In the vertical, there are nine d iscrete levels in the terrain following "sigma" coordinates, with the lowest level about 75 m above the surface. For th e m odel run at this resoluti on th ere are approximately 350 points ove r the Antarctic continent. Many physical processes not governed by the primitive equations are included via appropriate para meterisations. These include the radiati on scheme of Fels and Schwar zkopf (1975) and Schwa rzkopf a nd Fels (1991), the convecti ve scheme suggested by Noone and Simmonds: Precipitation analysis and interpretation qf ice-core data Manabe and others (1965), a soil hydrology scheme following Deardorff's (1977) model and a parameterisation of heat fluxes over sea ice applied by Simmonds and Budd (1990). Clouds are included interactively at three levels (Argete and Simmonds, 1996) to affect the radiation, and snow cover is prescribed as the climatology from passive-microwave observations by the Nimbus 7 satellite. The topography originates from continental heights of Smith and others (1966) and there is forcing at the lower boundary from the sea-surface temperatures ofReynolds (1988). Although modelling Antarctic moisture is a difficult task in practice, Simmonds (1990) showed that the modelgenerated accumulation rates over the Antarctic are representative of the accumulation estimated from stake measurements in both amount and spatial distribution. As such, it is thought that the Antarctic precipitation is modelled with sufficient accuracy and is appropriate for use in this study. The model results from the second decade of a 20 year control integration are used in this study. (a .. . . ... c;;;~ : ~ i . L_ t.,3,,~ .. :/ Cl .". ' ' 0 O~:~~;~j SYNOPTIC CONDITIONS Precipitation is obviously an integral part of ice-core analysis through accumulation at a drill-site. To determine what synoptic conditions lead to precipitation, we examine the mean sea-level pressure (MSLP) anomalies for each day in the model dataset. One calculates the anomalies by subtracting, from the given pattern, the monthly climatology temporally interpolated to the appropriate calendar day. A subset of the anomalies is chosen and averaged for the days on which more than a specified amount of precipitation fell at a given grid location. The amount chosen here is 5 mm d- \ as it represents high-precipitation conditions and occurs on roughly one in ten days at coastal locations. This fraction varies depending on precisely which grid point is considered. Further, even the most arid points (e.g. Vostok) show a number of tota ls over 5 mm because model data are used. Figure 1 shows the averaged MSLP anomaly pattern for the coastal point near Casey base (67.7" S, 112.5 E ) and the inland Vostok base (77.6 ° S, 106.9° E ). Coastal sites (e.g. Casey ) commonly show a local feature associated with the approach of a "cyclonic system". This dipolar structure, seen clearly in Figure la, suggests a northerly air stream which would advect relatively warm, moist marine air over the site. Upon cooling, this air would easi ly become saturated and condense into the modelled precipitation and release latent heat at the site. For inland cases (e.g. Fig. Ib ), such a dipolar feature is not usually present, and indeed it is more common for a single cyclonic feature to be present. This low-pressure anomaly is probably associated with precipitation formed by ascend ing air associated with surface convergence. Kinematic trajectories were generated in three dimensions for the 6 days prior to arrival at the site under consideration, for each day on which more than 5mm of precipitation occurred. Figure 2 shows the density of the origin of air parcels 6 days prior to precipitation, together with the calculated mean trajectory path. This trajectory reveals that indeed the air is of marine origin for the coastal site. The direction of approach deviates from that suggested by the geostrophic assumption as the driving winds from the GCM include the effects of katabatic flow. Few of the individual trajectories penetrate the region of the circumpolar 0 Fig. 1. MSLPanomaly on days with> 5 mm precipitationfor ( a) Casey and (b) Vastok locations. The contour interval is 0.5 hPa and the zero contour is shown in bold. trough. The MSLP anomalies and the trajectory analysis suggest that there are active links between the precipitation and the local synoptic conditions on any given day, Analysis of precipitation We now turn to consider the precipitation over the Antarctic continent in more detail by examining the daily precipitation totals at the 350 model points located over Antarctica. Although more precipitation events tended to occur in winter months, individual precipitation events with high totals occurred throughout the year. These data revealed that about half of the days showed no or negligible precipitation, From the same 10 year model dataset, we also extract the surface temperatures. For each model point, we calcu late the surface-temperature anomaly as the difference between the daily temperature at the site and the climatolo399 Noone and Simmonds: Precipitation analysis and interpretation if ice-core data test days are warmer than the average by up to 15°C, and days with over 5 mm of precipitation (around 8% of days ) are over 10°C warmer. If the dataset is broken down seasonally (Fig. 3b), we Gnd that the trend is stronger in autumn and winter (up to 20 ° and l8 °C, respectively) than in summer and spring (5° and 12°C). The gradient of this trend is also slightly larger if only coastal locations are considered. A similar trend is found at other model temperature Gelds although it is not as pronounced. For example, the lowest atmospheric level in the model (sigma level 0.991) displays warm tendencies up to 2°C. During precipitation events warm air is advected from the north, and the coastal regions of the continent are subject to greater cloud cover. Hence, it is not clear a priori whether the warm surface conditions of high-rainfall days are associated more closely with the extra southward sensible-heat transport or the additional trapping of longwave 25 20 15 ........ Cb) ...........-. 20 2:' '0" E 10 •..•... c: 5 .§ ...;::l'" Q) 15 0 j -;;; ... 0. Q) c:; Q) ... 0. 6 -5 10 ~ -10<1.1 "... ~ - 15 ,.' x ;::::s m - 20 . - 25 ...... \ .. a .... 3650 rank by precipitation amounl .... .,...... .... -" " " 20 ,.../ -':'" 15 102 to E Fig. 2. Average trajectory paths and density if trajectory originsfor the 6 days prior to precipitation at ( a) Casey and ( b) Vostok locations. Dark regions show higher density in arbitrary units if trajectory origins per unit area. An asterisk marks model locations. 0 5 c: ...'" Q) 0 ..,;::l ...'" Q) -5 0. E ~ - JOQ.) gical mean interpolated to the appropriate time of the year. Thus, for each of the 350 Antarctic points, a 10 year time series of both the precipitation and surface temperature was available. Ordering the precipitation totals at each point by amount from lowest to highest shows a distribution of an exponential nature, common in precipitation data (e.g. Noone and Stern, 1995). This highlights the fact that only a small percentage of precipitation events have high precipitation totals. The shaded region of Figure 3 shows the average of these distributions. ,,ye plot the surface-temperature anomaly corresponding Lo th e precipitation amounts and then average across the 350 points. Figure 3a shows a clear monotonic trend in the associated surface-temperature anomalies. We see that the wet400 "... ~ -15:::l m -20 -25 b 910 rank by precipilalion amount Fig. 3. M ean precipitation amount ( shaded region ) and corresponding mean surface-temperature anomaly (curve). The x axis is ranked by precipitation amount from lowest to highestJor ( a) all data (3650 days ) and (b ) seasonal comparison (910 days). Surface-temperature anomaly is marked on the right axis in o ~ and precipitation is on the lift axis in mm a'. Noone and Simmonds: Precipitation analysis and interpretation qf ice-core data ra diatio n by the cha nged clo ud conditions. This question can be a nswered simply by p erforming experiments in a GeM in which we prescribe cloud cover of give n amounts. Specificall y, we set the cloud concentration at all three cloud levels to have, first, 100 % a nd, second, 0 % a nd perform a 3 year integration. T he close simil a rit y in th e temperature trends res ulting from these two runs (not shown) suggests tha t indeed th e u nderl ying mecha nism is wa rm advection rather than radiation associated with greater cloud a mounts. This conclusion is supported by the earlier result that days with p recipi tation have a predomin ant north erl y air stream advecting moistu re to the precipitati on site. Simila rl y, the reduction in the temperature trend for inl and sites results from both weaker a dvection and a drier ai r mass. The trend seen in Figure 3 has a n obvious co nsequence for recreating pa laeoclimates from ice-core records. Specifically, as it is the d ays with high-precipitation events which a re recorded in the ice cores, a nd these days are shown to have sig nificantl y higher th an ave rage temperatures, the core isotope data will refl ect these warmer temperatures. DISCUSSION The naive interp retation of the above result suggests that a ny reconstruction of palaeoclimates from core isotope d ata will overestimate the temperatures if one does not include this warm bias. H owever, the relationship between the isotope concentratio n a nd temperature is determin ed by emp irical means fo r a give n site or a rea. Th erefore, the bias on a ny give n d ay has a lready been included in the regression. We note tha t such a method foc uses on the annu al m ean temperatu re, and that d aily informati on associated with individua l precipita tion events is lost. The appropri ate interpretati on is that th e co re data represent conditions tha t a re in some way abnorm a l. This is true in the simple case of surface temperature a nd in the more complex case of the synoptic situation as seen above with the example of MSLP a noma li es. Th at is, the ice-core sig nal will refl ect a circulation regime that is significantly different from the mean conditions. An importa nt consider atio n that foll ows from thi s is the tempora l va riation of the bi as. We saw in Fig ure 3b that th e temperature a nomali es on precipitation d ays in the autumn a nd winter differ significantly from th ose in the warmer summer and spring months. "Ve attribute this difference to more intense baroclinic acti vity leading to stronge r norther ly advec tion of wa rm, moist air during autumn and winter. As very littl e is known about th e ci rcul ation conditions of various pa laeoclim ates, it is difficult to say whether such a seasonal variation would prevail. Simil a rl y, it is likely tha t the stre ng th of circulati on was different from th at of tod ay. Thi s is importa nt insomuch as we cannot be sure that the co nditions under which acc umul a ti on can occ ur have the same bi as over time. P. Valdes and others (p ersonal communicati on, 1997) indicate from simul ations with a GeM that there is a reduction in streng th of polar ba roclinicity during th e L as t G lacia l M aximum . Foll owing th e above a rgument, we wo uld ex pect a reduced slope in the temperat ure bias. This wo uld resul t in a n underestim ate of pa laeotemperatures from the regression relation deri ved from experimental d ata coll ected under tod ay's conditi ons. Thi s scena ri o is incomplete, in th at altering the circul ation strength will a lso intro- duce changes in oth er complex atm ospheric processes like evaporati on, transport a nd precipitation. It m ay be possible to qu antify, to some extent, the differences be tween var ious globa l circul ati on regimes by considering the vari ati on in acc umulati on rates in ice cores. One could focus on times when there is a shift from glacial to interglacial periods. If there is a pa rticula r peri od of cha nge that is tempora lly consistent over a la rge geographical domain, it is possible there was a sig nificant change in the circulation regime a nd that empirical te mperature reconstruction would be less reliable. 10 obtain detailed inform ation abo ut the vari a tions in isoto pic content from a n ice co re on short time-scales wo uld be very difficult, a nd indeed m ay be impossible. Th e u e of fll0delling techniques, instead of observationa l data, m ay yield a valu abl e approach. Running a n ensembl e of si mu lations th at re present a number of pa laeoclimate systems would give a n indicati on of the range of circulation regimes that m ay ex ist. Incorporating a hydrological cycle that allows for the stable-isotopic forms of water wo uld then give a n indication of the spati a l a nd te mporal vari ations in th e isotopic concentrations, along with estim ates for accumul ati on rates. This wo uld p rovide a useful tool in linking the measured isotope d ata in ice co res to the synoptic conditi ons via the precipit ation signal. This wo uld a llow one to gain more informati on than is give n simply by the m ean conditions. CONCLU DING R EMARKS It is of g reat importa nce to obtain a complete understa nding of the precipi tatio n p rocesses leading to acc umulation before analyzing ice-core data. The exa mpl e shown here highli ghts how, without such knowledge, th e regress ion techni q ues com mo nl y used to reconstruct pa laeo temperatures a re q uesti onable, in that the ass umed rela tionship may be different under a pa laeoclima tic regime. Through precipi tati on, it is possibl e to associate the meas urements in th e 18 0 record with the prevailing synoptic condi tions of the day. As there is onl y one d ay in ten th at exhibits a high-precipitati on event leading to sig nificant accumul ation, th ere will be a bi as in the ice-core compositi on towa rd conditions that a re in so me way abnorm al. In th e results given here, these conditions ar e warmer. Th e increased synoptic activity shown in the MSLP a noma li es is a lso not representati ve of th e "average" condi tions a round a ny single Anta rctic site. An extension of th e a rg ument of bi as in ice-co re records presented ass umes a simila r bias wo uld have been evident in a da tase t represe nting the circul ati on patterns of pa laeoclimate systems. Specificall y, one can infer from the ice-core measurements only the condi tions of the abnorma l synoptic situ ati on tha t lead to precipitation. Nonetheless, it m ay be possible to assess th e expected vari ability of vari ous palaeoclim ates by co nsidering the extreme conditi ons expected during precipitati on. G e M experiments th at recreate th ese extreme conditi ons of precipi tation will also co ntain informati on about d a il y circulation that does not result in precipitati on. Th e difference between th ese two conditions will give a n indicati on of the atm ospheric vari abili ty on a daily time-scale prese nt under a given pa laeoclimatic circulation regime. 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