Interannual variability in sea surface temperature and fCO2 changes in the Cariaco Basin

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Interannual variability in sea surface temperature and fCO 2 changes in the Cariaco Basin Y.M. Astor a,n , L. Lorenzoni b , R. Thunell c , R. Varela a , F. Muller-Karger b , L. Troccoli d , G.T. Taylor e , M.I. Scranton e , E. Tappa c , D. Rueda b a Fundacio ´n La Salle de Ciencias Naturales, EDIMAR, Punta de Piedras, Edo. Nueva Esparta, Venezuela b University of South Florida, College of Marine Science, 140 7th Ave. S., St. Petersburg, FL 33701, USA c University of South Carolina, Department of Earth and Ocean Sciences, Columbia, SC 29208, USA d Universidad de Oriente, ECLAM, Boca del Rı ´o, Edo. Nueva Esparta, Venezuela e Stony Brook University, School of Marine and Atmospheric Sciences, Stony Brook, NY 11794-5000, USA article info Keywords: CO 2 fugacity Upwelling Cariaco Basin Sea surface temperature Climate variability abstract We examined the variability of sea surface carbon dioxide fugacity (fCO 2sea ) and its relation to temperature at the Cariaco Basin ocean time-series location (10130 0 N, 64140 0 W) for the period from 1996 through 2008. Periods of warm (positive) and cold (negative) anomalies at the station were related to variability in coastal upwelling intensity. A positive temporal trend in monthly- deseasonalized sea surface temperatures (SST) was observed, leading to an overall increase of 1.13 1C over 13 years. Surface fCO 2sea displayed significant short-term variation (month to month) with a range of 330–445 matm. In addition to a large seasonal range (58 717 matm), deseasonalized fCO 2sea data showed an interannual positive trend of 1.77 70.43 matm yr 1 . In the Cariaco Basin, positive and negative anomalies of temperature and fCO 2sea are in phase. An increase/decrease of 1 1C coincides with an increase/decrease of 16–20 matm of fCO 2sea . Deseasonalized fCO 2sea normalized to 26.05 1C, the mean Cariaco SST, shows a lower rate of increase (0.51 70.49 matm yr 1 ). Based on these observations, 72% of the increase in fCO 2sea in Cariaco Basin between 1996 and 2008 can be attributed to an increasing temperature trend of surface waters, making this the primary factor controlling fugacity at this location. During this period, a decrease in upwelling intensity was also observed. The phytoplankton community changed from large diatom-dominated blooms during upwelling in the late 1990’s to blooms dominated by smaller cells in the first decade of the 21st century. The average net sea-air CO 2 flux over the study period is 2.0 72.6 mol C m 2 yr 1 employing the Wanninkhof parameterization, and 2.1 72.5 mol C m 2 yr 1 based on Nightingale’s model. To further understand the connection between the changes observed in the Cariaco Basin, the relationships between interannual variability in the temperature anomaly with three modes of climate variability (AMO, NAO and ENSO) were examined. The correlations between SSTA and two of these climate modes (AMO and ENSO) only show very weak relationships, although they were significant. & 2013 Elsevier Ltd. All rights reserved. 1. Introduction Although continental margins represent only about 0.5% of the ocean volume and occupy less than 8% of the seafloor, they play an important role in regulating the exchange of carbon dioxide (CO 2 ) and the storage of carbon within the global ocean (Doney et al., 2009; Liu et al., 2000; Muller-Karger et al., 2005). Due to high primary production and carbon storage rates in sediments, many continental margin areas are considered CO 2 sinks (Chen and Borges, 2009). However, the balance between biogeochemical processes (CO 2 uptake/production, CaCO 3 fixation/dissolution), transport (advection/turbulent diffusion), convective mixing, air- sea gas exchange, and riverine input determine whether a particular region functions as a net source or sink of CO 2 . Long-term and frequent observations of fugacity of seawater CO 2 (fCO 2sea ) are required to help reduce the large uncertainties in the global estimates of CO 2 flux (Nemoto et al., 2009). Indeed, both seasonal and spatial variability of CO 2 concentrations in the ocean may mask any long-term changes if careful observations are not conducted within a time series framework (Bates, 2001). Contents lists available at SciVerse ScienceDirect journal homepage: www.elsevier.com/locate/dsr2 Deep-Sea Research II 0967-0645/$ - see front matter & 2013 Elsevier Ltd. All rights reserved. http://dx.doi.org/10.1016/j.dsr2.2013.01.002 n Corresponding author. Tel.: þ58 295 808 3804; fax: þ58 295 239 8051. E-mail addresses: [email protected] (Y.M. Astor), [email protected] (L. Lorenzoni), [email protected] (R. Thunell), [email protected] (R. Varela), [email protected] (F. Muller-Karger), [email protected] (L. Troccoli), [email protected] (G.T. Taylor), [email protected] (M.I. Scranton), [email protected] (E. Tappa), [email protected] (D. Rueda). Please cite this article as: Astor, Y.M., et al., Interannual variability in sea surface temperature and fCO 2 changes in the Cariaco Basin. Deep-Sea Res. II (2013), http://dx.doi.org/10.1016/j.dsr2.2013.01.002i Deep-Sea Research II ] (]]]]) ]]]]]]

Transcript of Interannual variability in sea surface temperature and fCO2 changes in the Cariaco Basin

Deep-Sea Research II ] (]]]]) ]]]–]]]

Contents lists available at SciVerse ScienceDirect

Deep-Sea Research II

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journal homepage: www.elsevier.com/locate/dsr2

Interannual variability in sea surface temperature and fCO2 changesin the Cariaco Basin

Y.M. Astor a,n, L. Lorenzoni b, R. Thunell c, R. Varela a, F. Muller-Karger b, L. Troccoli d, G.T. Taylor e,M.I. Scranton e, E. Tappa c, D. Rueda b

a Fundacion La Salle de Ciencias Naturales, EDIMAR, Punta de Piedras, Edo. Nueva Esparta, Venezuelab University of South Florida, College of Marine Science, 140 7th Ave. S., St. Petersburg, FL 33701, USAc University of South Carolina, Department of Earth and Ocean Sciences, Columbia, SC 29208, USAd Universidad de Oriente, ECLAM, Boca del Rıo, Edo. Nueva Esparta, Venezuelae Stony Brook University, School of Marine and Atmospheric Sciences, Stony Brook, NY 11794-5000, USA

a r t i c l e i n f o

Keywords:

CO2 fugacity

Upwelling

Cariaco Basin

Sea surface temperature

Climate variability

45/$ - see front matter & 2013 Elsevier Ltd. A

x.doi.org/10.1016/j.dsr2.2013.01.002

esponding author. Tel.: þ58 295 808 3804; f

ail addresses: [email protected] (Y.M. A

marine.usf.edu (L. Lorenzoni), [email protected]

[email protected] (R. Varela), carib@marine

[email protected] (L. Troccoli), gordon.taylor@s

[email protected] (M.I. Scranton), tapp

[email protected] (D. Rueda).

e cite this article as: Astor, Y.M., et a-Sea Res. II (2013), http://dx.doi.org

a b s t r a c t

We examined the variability of sea surface carbon dioxide fugacity (fCO2sea) and its relation to

temperature at the Cariaco Basin ocean time-series location (101300N, 641400W) for the period from

1996 through 2008. Periods of warm (positive) and cold (negative) anomalies at the station were

related to variability in coastal upwelling intensity. A positive temporal trend in monthly-

deseasonalized sea surface temperatures (SST) was observed, leading to an overall increase of 1.13 1C

over 13 years. Surface fCO2sea displayed significant short-term variation (month to month) with a range

of 330–445 matm. In addition to a large seasonal range (58717 matm), deseasonalized fCO2sea data

showed an interannual positive trend of 1.7770.43 matm yr�1. In the Cariaco Basin, positive and

negative anomalies of temperature and fCO2sea are in phase. An increase/decrease of 1 1C coincides with

an increase/decrease of 16–20 matm of fCO2sea. Deseasonalized fCO2sea normalized to 26.05 1C, the mean

Cariaco SST, shows a lower rate of increase (0.5170.49 matm yr�1). Based on these observations, 72% of

the increase in fCO2sea in Cariaco Basin between 1996 and 2008 can be attributed to an increasing

temperature trend of surface waters, making this the primary factor controlling fugacity at this

location. During this period, a decrease in upwelling intensity was also observed. The phytoplankton

community changed from large diatom-dominated blooms during upwelling in the late 1990’s to

blooms dominated by smaller cells in the first decade of the 21st century. The average net sea-air CO2

flux over the study period is 2.072.6 mol C m�2 yr�1 employing the Wanninkhof parameterization,

and 2.172.5 mol C m�2 yr�1 based on Nightingale’s model. To further understand the connection

between the changes observed in the Cariaco Basin, the relationships between interannual variability in

the temperature anomaly with three modes of climate variability (AMO, NAO and ENSO) were

examined. The correlations between SSTA and two of these climate modes (AMO and ENSO) only

show very weak relationships, although they were significant.

& 2013 Elsevier Ltd. All rights reserved.

1. Introduction

Although continental margins represent only about 0.5% of theocean volume and occupy less than 8% of the seafloor, they playan important role in regulating the exchange of carbon dioxide(CO2) and the storage of carbon within the global ocean (Doney

ll rights reserved.

ax: þ58 295 239 8051.

stor),

.edu (R. Thunell),

.usf.edu (F. Muller-Karger),

tonybrook.edu (G.T. Taylor),

[email protected] (E. Tappa),

l., Interannual variability in/10.1016/j.dsr2.2013.01.002

et al., 2009; Liu et al., 2000; Muller-Karger et al., 2005). Due tohigh primary production and carbon storage rates in sediments,many continental margin areas are considered CO2 sinks (Chenand Borges, 2009). However, the balance between biogeochemicalprocesses (CO2 uptake/production, CaCO3 fixation/dissolution),transport (advection/turbulent diffusion), convective mixing, air-sea gas exchange, and riverine input determine whether aparticular region functions as a net source or sink of CO2.

Long-term and frequent observations of fugacity of seawaterCO2 (fCO2sea) are required to help reduce the large uncertainties inthe global estimates of CO2 flux (Nemoto et al., 2009). Indeed,both seasonal and spatial variability of CO2 concentrations in theocean may mask any long-term changes if careful observationsare not conducted within a time series framework (Bates, 2001).

sea surface temperature and fCO2 changes in the Cariaco Basin.i

Y.M. Astor et al. / Deep-Sea Research II ] (]]]]) ]]]–]]]2

Long time-series are a powerful tool for investigating biogeo-chemical cycles and marine ecosystems and their role in andresponse to climate variability. This important concept has led tothe initiation of a number of biogeochemical ocean time-seriesstations, both in open ocean and continental margin sites. Forexample, in the deep North Pacific Ocean at ocean time-seriesstation ALOHA (A Long-term Oligotrophic Habitat Assessment;221450N, 1581000W), observations have revealed an increase of2.8470.28 mmol kg�1 yr�1 in surface total carbon dioxide (TCO2)between 1989 and 2001 (Dore et al., 2003). In the deep sub-tropical North Atlantic, at the Bermuda Atlantic Time-series Study(BATS; 311450N, 641100W), surface TCO2 increased by1.3770.16 mmol kg�1 yr�1 between 1983 and 2005 (Bates,2007), with surface and atmospheric pCO2 increasing at1.6770.28 matm yr�1 and 1.7870.02 matm yr�1 respectivelyover this 22 year period (Bates, 2007).

However, whether surface water CO2 varies over similar timescales in continental margin settings within the tropics are yetunknown. Since November 1995, the Cariaco Basin ocean time-series program (CARIACO) has conducted biogeochemical andecological observations at a location on the northern Venezuelanmargin (101300N, 641400W, Fig. 1) to examine the linkagesbetween water column processes and the flux of particles settlingto the seafloor. The Cariaco Basin is an ideal location to examinethis question because past changes in surface ocean processes arewell preserved in the sediment record accumulating in the basin.The Cariaco Basin has a unique set of oceanographic character-istics. The open exchange of water and materials with theCaribbean Sea only occurs above a 140 m deep sill. Consequently,there is a restriction (or limitation) of deep water circulation andmixing, which allows the formation of anoxic waters below320 m. The restricted circulation within the basin isolates it fromthe open ocean and makes it a trap for sinking materials. Theseasonally alternating coastal wind-driven upwelling controls thehigh seasonal biological productivity and particulate sedimentflux.

Fig. 1. Map depicting the Cariaco Basin and indicating

Please cite this article as: Astor, Y.M., et al., Interannual variability inDeep-Sea Res. II (2013), http://dx.doi.org/10.1016/j.dsr2.2013.01.002

While the Cariaco Basin has a long history of oceanographicstudies, very few have focused on the carbon dioxide system.Avila-Melean (1976) analyzed the relationship between TCO2 anddissolved oxygen in the nearby Gulf of Santa Fe. Hastings andEmerson (1988) measured TCO2 and total alkalinity (TA) in astudy of sulfate reduction above the O2–H2S interface. Zhang andMillero (1993) measured TCO2, pH, and TA in the eastern andwestern basins of the Cariaco Basin. Astor et al. (2005a,b)observed the interactions between physical and biochemicalparameters that lead to temporal variations in fCO2sea, findingthat even during periods of high production, the CO2 flux betweenthe ocean and the atmosphere decreased but remained positive,i.e. CO2 escaped from the ocean to the atmosphere.

In this paper, we report the results of CO2 observations at theCARIACO time-series station. We look at changes observed duringperiods of upwelling (dry season) and non-upwelling (rainyseason). We evaluate the rates of change of several hydrographicparameters over the period 1996–2008, and examine possibleconnections with different modes of climate variability.

1.1. Study area

The Cariaco Basin, located on the continental margin of Vene-zuela, is a tectonic depression (�1400 m deep) subject to seasonalchanges in atmospheric forcing that affect the water column’s upperlayers. Intermittent easterly trade winds (46 m s�1) are responsi-ble for offshore surface Ekman transport and wind-driven coastalupwelling during winter and early spring (January–April). Rainyconditions and weak winds are typical between September andDecember, the months of non-upwelling. A transition period occursbetween June and August when a short and relatively weaksecondary upwelling event occurs with characteristics and timingthat vary from year to year (Astor et al., 2003). The causes of thissecondary upwelling event are linked to variations in the wind curl(Rueda-Roa, 2012). During the primary upwelling event, high

the location of the CARIACO time series station.

sea surface temperature and fCO2 changes in the Cariaco Basin.i

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salinity (S436.8) Subtropical Underwater (SUW) reaches the sur-face (Morrison and Smith, 1990). This nutrient- and carbon-richwater stimulates primary production (41.5 gC m�2 d�1, Muller-Karger et al., 2001) during the period of upwelling. The reminer-alization of the sinking particulate organic matter and limitedcirculation maintain a suboxic zone (dissolved oxygen and sulfideo5 mM) between 200 and 320 m, with anoxic conditions fullydeveloped deeper than about 320 m.

2. Methods

Observations of the inorganic carbon system were made betweenJanuary 1996 and December 2000, and from March 2002 to Decem-ber 2008 on board the R/V Hermano Gines (Fundacion La Salle deCiencias Naturales de Venezuela). All data, including the time series ofpH (pH on the total hydrogen ion concentration, pHT), total alkalinity(TA), TCO2, and fCO2sea are publicly available on the CARIACO webpage (/http://www.imars.usf.edu/CAR/index.htmlS) and through theOcean Carbon and Biogeochemistry (OCB) Data Management Office(/http://mapservice.bco-dmo.org/mapsbin/global/mapS). Continu-ous hydrographic profiles and water samples were collected using aCTD system (SeaBird SBE-19 from January to September 1996; SBE-25 for all subsequent cruises). Sampling details were described inAstor et al. (2003, 2005a).

The parameters measured to characterize the various compo-nents of the carbonate system are pH and TA. TA samples werecollected in 250-mL glass amber bottles and poisoned with 50 mLof saturated HgCl2 solution (final Hg concentration of about50 mM). Samples were stored at 4 1C and analyzed in the labora-tory. For pH, seawater samples were drawn directly from eachNiskin bottle into a 10 cm spectrophotometer cell. Colorimetricanalyses were made on board ship within 1 h of sample collec-tion. Samples for pH were measured using the spectrophoto-metric method of Clayton and Byrne (1993) as modified byDelValls and Dickson (1998) and Dickson et al. (2007). TAanalyses followed the method of Breland and Byrne (1993), andYao and Byrne (1998), with modifications suggested by Dr.Wensheng Yao (personal communication). Further details on thealkalinity and pH methods can be found in Astor et al. (2005a).The precision of the alkalinity and pH measurements are4 mmol kg�1 and 0.003 units of pH, respectively. Certified alkali-nity reference materials (CRM’s) supplied by A.G. Dickson (ScrippsInstitute of Oceanography) were analyzed for TA with each batchof samples for each cruise. The standard deviation between themean value of alkalinity measurements of the standards and thecertified value was 2 mmol kg�1.

TCO2 and fCO2sea were calculated using CO2SYS (Lewis andWallace, 1998), applying the carbonic acid dissociation constantsof Mehrbach et al. (1973) as modified by Dickson and Millero(1987), and equilibrium constants from Millero (1995). Theprecision of TCO2 and fCO2sea measurements were estimatedthrough 1000 Monte Carlo simulations using the average andstandard deviation for each input parameter. The uncertaintyassociated with TCO2 was about 2 mmol kg�1 and for fCO2sea

about 4 matm. Surface TA and TCO2 data were normalized (nTAand nTCO2) to the mean surface salinity (36.8) at the Cariacotime-series site (nTA¼36.8TA/S; nTCO2¼36.8TCO2/S) to removethe effects of local precipitation and evaporation. To normalizethe fCO2sea data (nfCO2sea), fCO2sea was recalculated at a constantT (using CO2SYS). The temperature used was 26.05 1C, which isthe mean of SST observations at the Cariaco station. Then, therecalculated fCO2sea was deseasonalized, and this data set wasregressed linearly against time (year).

The shallow cast (1–160 m) was always collected as close tolocal noon (16:30 UTC) as possible; therefore, heating effects on

Please cite this article as: Astor, Y.M., et al., Interannual variability inDeep-Sea Res. II (2013), http://dx.doi.org/10.1016/j.dsr2.2013.01.002

the ocean’s surface are strong. The effect of daytime warmingtogether with low wind speeds may enhance air-sea CO2 flux(Ward et al., 2004). Therefore, we used the average of fCO2sea

estimates at 1 and 7 m to minimize the temperature effect and toassess air-sea CO2 flux. TCO2, TA, salinity and temperature werealso averaged between 1 and 7 m, and the average was used asrepresentative of surface layer values.

Estimates of the mixed-layer depth (MLD) were determined asthe depth where the difference between in situ density andsurface density exceeded 0.125 kg m�3. The coastal upwellingindex was estimated as the cross-shore Ekman transport per100 m coastline (M, m3 s�1 per 100 m of coastline; Bakun, 1973;Schwing et al., 1996) as follows:

M¼ tx=f ð1Þ

where M is the meridional Ekman transport resulting from thezonal wind stress (tx), and f is the Coriolis parameter. Because thezonal wind at the CARIACO site is negative by convention, the signof the offshore component of the Ekman transport estimatedalong the Venezuelan shoreline was modified to reflect thatnegative (offshore) Ekman transport leads to positive (upwelling)vertical transport. Thus, transport values reported here are shownas positive.

Wind data were derived from two meteorological stations locatedto the northeast of the CARIACO time-series station on MargaritaIsland, Venezuela (one at 101560N 641060W in Punta de Piedras, andthe other at a nearby station at 101540N 631580W in PorlamarInternational Airport). Zonal wind stress was estimated from themonthly mean wind speed since wind speeds are relatively stableover periods of weeks to months in this tropical setting.

Phytoplankton biomass was estimated as chlorophyll a (Chla)extracted in methanol and measured on a Turner Designs fluorom-eter using standard methods (Falkowski and Kiefer, 1985; Holm-Hansen et al., 1965). Primary productivity observations were made atthe same depths as Chla using a modified Steeman Nielsen (1952)NaH14CO3 uptake assay. Further details on the primary productionmethod can be found in Muller-Karger et al. (2001). Primaryproductivity and Chla values were integrated from 1 to 7 m forconsistency with all other parameters. Phytoplankton samples fortaxonomy were fixed with neutralized formalin and were analyzedin the laboratory with the Utermohl technique (Hasle, 1978).

A single mooring containing five automated sediment traps isused to measure the vertical flux of particles at various depths inthe Cariaco Basin water column. Further details on the character-istics of this mooring can be found in Thunell et al. (2008). Theratio of organic to inorganic carbon (Co/Ci) in the total carbon fluxderived from sediment trap samples collected at 225 m at thestudy site was calculated.

The sea-air CO2 flux, F, was calculated according to:

F ¼ kaDf CO2 ð2Þ

where k is the transfer velocity for sea-air CO2 exchange, a is thesolubility of CO2 and DfCO2 is the sea-air fCO2 difference (fCO2sea–fCO2 atm). DfCO2 was calculated from the difference between theaverage value of fCO2sea and the fugacity of CO2 in the atmosphere(fCO2 atm). Data for atmospheric CO2 was taken from Conway et al.(2009) for Ragged Point in Barbados (131100N 591260W) withinthe period of 1996 and 2008. An average value of atmosphericCO2 at this site for each month was used for calculations.

The solubility of CO2 is a function of temperature and salinityand was calculated according to Weiss (1974). The CO2 gastransfer velocity is the exchange parameter between the oceanand the atmosphere, and different parameterizations yieldroughly a factor of two differences in gas transfer values overthe oceans (Wanninkhof et al., 2004); therefore, to assess the

sea surface temperature and fCO2 changes in the Cariaco Basin.i

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uncertainty in the estimates of sea-air CO2 fluxes, two parame-terizations were considered, namely Nightingale et al. (2000) andWanninkhof (1992)

k¼ 0:31u2 Sc=660� ��0:5

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k¼ 0:222u2þ0:333u� �

Sc=600� ��0:5

Nightingale et al: ð2000Þ

ð4Þ

where Sc is the Schmidt number and u is the monthly meanwind speed measured at 10 m above the ground. The Schmidtnumber is the ratio of the kinematic viscosity of seawater to theaqueous diffusion coefficient of CO2 in water, and it was calcu-lated using the Wanninkhof (1992).

Three indices designed to assess climate variability (the NorthAtlantic Oscillation (NAO), the Southern Oscillation Index (SOI),and the Atlantic Multidecadal Oscillation (AMO) index) wereobtained from NOAA’s Climate Prediction Center (/http://www.cpc.noaa.govS) and compared to the time series of CARIACO seasurface temperature anomalies (SSTA). The NAO describes a large-scale meridional oscillation in atmospheric mass between theAzores High and the Iceland Low. The Southern Oscillation Index(SOI), an indicator of large-scale variability in the Pacific Oceanassociated with the El Nino phenomenon, is calculated frommonthly fluctuations of atmospheric sea level pressure betweenDarwin, Australia and Tahiti. The AMO is an index that tracksvariability in temperatures of the North Atlantic Ocean.

2.1. Statistical analyses

The annual cycle was statistically removed (deseasonalized)from SST, salinity, pH, TA, TCO2, and fCO2 by subtracting monthlyobservations from 13-yr means (for SST and salinity) and 11-yrmeans (for CO2 parameters) and adding the overall mean (e.g.,Bates, 2007). The years 2001 and 2002 were excluded from CO2

statistics in this analysis because all CO2 data from 2001 and sixmonths from 2002 were missing due to equipment failure. Theobserved and deseasonalized monthly values were regressedlinearly against time (year) to obtain the rate of change. Anoma-lies were derived by subtracting the climatological mean frommonthly observations. The relationship among 10 environmentalvariables (TCO2, temperature, salinity, MLD, chlorophyll a, fCO2sea,primary production, upwelling index, ratio of organic to inorganiccarbon (Co/Ci), and diatom/coccolithophore (D/C) ratio) wereanalyzed by Principal Coordinate Analysis (PCO or PCoA). PCO isan ordination method similar to Principal Component Analysis(PCA). The PCO is an eigenanalysis routine where the analysisplaces the samples onto Euclidean axes using only a matrix ofinter-point dissimilarities, rather than from a correlation orcovariance matrix. The values for each variable were normalizedby having their mean subtracted and were divided by theirstandard deviation. Euclidean distances among centroids in thespace were calculated to normalized data to produce a resem-blance matrix that formed the basis of the analyses. This matrixwas used as an ordination method to visually compare groupdifferences and patterns through a projection of the data ontoaxes (Anderson et al., 2008). The analysis was performed usingPermanovaþ add-on package for Primer software.

1 1 1 1 2 2 2 2 2 2 2 2 2 2

Fig. 2. Time-series of monthly observations of (a) SST (1C), (b) SSS, and

(c) upwelling index (m3 s�1 per 100 m of coastline, black line-closed diamonds)

and wind speed (m s�1, dashed line-open triangles) at the CARIACO time-series

station from January 1996 to December 2008. In (a) and (b), the thin black line and

dashed line-open squares indicate monthly individual and deseasonalized mea-

surements, respectively. Linear trends are indicated in a and b for individual

values (black solid line) and deseasonalized data (dashed line). Trends are given in

Table 1. In (c), linear trend for upwelling index is indicated by the black line and

for wind speed by the dashed line.

3. Results and discussion

3.1. Hydrography

Several authors have documented the seasonal hydrographic,biological, and chemical characteristics of the water column at theCARIACO station (Astor et al., 1998, 2003, 2005a,b, 2006; Muller-

Please cite this article as: Astor, Y.M., et al., Interannual variability inDeep-Sea Res. II (2013), http://dx.doi.org/10.1016/j.dsr2.2013.01.002

Karger et al., 2001, 2010; Scranton et al., 2001, 2006a,b; Taylor et al.,2012; Virmani and Weisberg, 2009). Fig. 2 shows time-series of seasurface temperature (SST), sea surface salinity (SSS), wind speed andupwelling index. The highest SST typically occurred in associationwith the lowest SSS in September and October (Fig. 2a and b).Conversely, the lowest SST and highest SSS were observed fromJanuary through April, when stronger winds resulted in greatervertical mixing and upwelling. In addition to this pronouncedseasonal cycle, there was significant interannual variability in SSTand SSS, particularly in the seasonal minima for both parameters. Anaverage seasonal SST range 670.6 1C, and a seasonal range of SSSof 0.6370.22 were observed between 1996 and 2008. The MLD

sea surface temperature and fCO2 changes in the Cariaco Basin.i

CARIACO Time Series

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basis of Euclidean distances of normalized data of the CARIACO time-series

station. The upwelling periods are represented by triangles and non-upwelling

by squares. The years corresponding to the cold periods are circled in blue and

years of warm periods in red. Both axes combined explain 77.9% of the total

variation.

Y.M. Astor et al. / Deep-Sea Research II ] (]]]]) ]]]–]]] 5

was typically shallow with an average seasonal range of2177.6 m. Occasionally, eddies drifting near the shelf breakinjected oxygenated nutrient rich water into the basin enhancingbiological activity that resulted in a drawdown of CO2 (Astor et al.,2003, 2005a). Unfortunately, our data on the influence of eddieson the biogeochemistry of the basin is limited and precludes usfrom drawing further conclusions on the importance of thesesporadic events.

The wind speed also showed strong seasonal and interannualfluctuations, leading to variations in the strength of the upwelling(Fig. 2c). Periods with stronger upwelling (1996–1998, 2001–2003) were followed by years of weak upwelling (1999–2000,2004–2008). A linear fit model between SST and the upwellingindex shows a correlation coefficient equals to �0.60 (R2

¼0.37)indicating a moderately strong relationship between the twovariables.

Fig. 3 illustrates the SSTA from 1996 to 2008. A 12-monthrunning mean was applied to the monthly values. The SSTA datarevealed two cold periods (January 1996–March 1998, June 2000–December 2003) and two warm periods (April 1998–May 2000,January 2004–December 2008). Between 1996 and 2008, SSTAvalues oscillated 71 1C around the mean. When compared to theupwelling index, the periods of cold and warm anomalies coin-cided with periods of strong and weak upwelling intensities,respectively (Fig. 2c). A PCO analysis shows similar patterns inthe distribution. The years with similar characteristics occupy thesame location in multivariate space separating the years into coldand warm periods. The first axis (PCO1) is strongly associatedwith the separation between the upwelling and the non-upwelling season, and it explains 63% of the total variation(Fig. 4). Temperature differences among periods (warm and coldyears) are discernible along the second axis (PCO2), whichaccounts for an additional 14.9%. Together, both axes explain77.9% of the total variation. Overall, there is a clear separationbetween the upwelling and the non-upwelling season duringboth the cold and warm periods.

3.2. CO2 parameters: Surface values

Over the 13-year study period, surface pH fluctuated from 8.014to 8.113 (Fig. 5a). This range is similar to what we had observedpreviously over the shorter period of 1996–2000 (Astor et al.,2005a). Surface TA and nTA (Fig. 5b, nTA not shown) had meanvalues of 2413719 and 2416715 mmol kg�1, respectively.

-3

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1996 1997 1998 1999 2000 2001 2002 2003 2004 2005 2006 2007 2008 2009

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(o C)

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ace fC

O2s

ea a

nom

aly

(µat

m)

Fig. 3. Time-series of anomalies of sea surface temperature (SSTA) and surface

fCO2sea at the CARIACO time-series station from January 1996 to December 2008.

Anomalies were derived by subtracting the climatological mean from monthly

observations. Anomalies were smoothed using a 12-month running mean where

black line is for SSTA and gray line for fCO2sea anomaly.

Please cite this article as: Astor, Y.M., et al., Interannual variability inDeep-Sea Res. II (2013), http://dx.doi.org/10.1016/j.dsr2.2013.01.002

The high standard deviation at CARIACO reflects the higher envir-onmental variability of coastal waters, where controlling factorssuch as upwelling of a water mass and changing productivity areimportant. At the CARIACO station, TA changes may also occur dueto biogenic precipitation of calcium carbonate and the dissolutionof calcareous shells or skeletons. Biogenic precipitation was evidenton January 1997, January 1999, March 2007, and February 2008,when nTA values dropped by more than 20 mmol kg�1 and thenumber of coccolithophore cells in surface waters increased sig-nificantly (Luis Troccoli, pers. comm., Universidad de Oriente).Elevated TA values were usually associated to salinities greaterthan 36.8 which identifies Subtropical Underwater (Astor et al.,2003). This water mass may reach the surface during the peak ofupwelling (February–March) with high TA values.

Surface TCO2 and nTCO2 (Fig. 5c, nTCO2 not shown) variedbetween 1988 and 2137 (mean value 2072726 mmol kg�1), and1978 and 2132 mmol kg�1 (mean value 2074721 mmol kg�1),respectively, over the 13-year study period. Higher surface values(42100 mmol kg�1) were typical during periods of high upwel-ling and low precipitation. The relationship between TCO2 andsalinity was significant (R2

¼0.38, po0.01). In 2004, surfacevalues throughout the year were closer to the overall mean(2070 mmol kg�1). Seasonal variation of TCO2 over the entirestudy period had an average range of 83718 mmol kg�1. Sincedifferences between surface TA and nTA, and TCO2 and nTCO2 areminimal, we can say that changes in salinity due to mixing,evaporation, and precipitation had minimal effects on the CO2

parameters at the CARIACO station.Fig. 6a and b shows surface fCO2sea and normalized fCO2sea

(nfCO2sea) at a constant temperature at the CARIACO station overthe study period. Average surface fCO2sea was 395722 matmconsistent with our previous calculations for the period 1996–2000 (Astor et al., 2005a). Over the entire period, we observevalues that range from 330 to 445 matm, which is in the rangeobserved for the western tropical North Atlantic and the Carib-bean Sea (320–400 matm; Park and Wanninkhof, 2012;Wanninkhof et al., 2007).

3.3. Interannual trends from 1996 to 2008 at the CARIACO

Time-series station

3.3.1. Observed hydrographic and CO2 parameters.

Salinity, pH, TCO2, nTCO2, TA and nTA did not show significantchanges through time. For all these parameters, seasonality

sea surface temperature and fCO2 changes in the Cariaco Basin.i

8.00

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2009

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O2

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ol k

g-1)

Fig. 5. Time-series of monthly observations (individual and deseasonalized) of

(a) pH; (b) total alkalinity (mmol kg�1) and (b) total CO2 (mmol kg�1) at the

CARIACO time-series station from January 1996 to December 2008. The thin line

and dashed line-open squares indicate monthly individual and deseasonalized

measurements, respectively. Linear trends are indicated for individual and

deseasonalized data (black and dashed lines). Trends are given in Table 1.

300

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2sea

(µa

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nf C

O2s

ea (

µatm

)

Fig. 6. Time-series of monthly individual and deseasonalized of: (a) surface CO2

fugacity, (fCO2sea, matm) and (b) normalized CO2 fugacity (nfCO2sea, matm) at the

CARIACO time-series station from January 1996 to December 2008. The thin line

and dashed line-open squares indicate monthly individual and deseasona-

lized measurements, respectively. Linear trends are indicated for individual

values (black line) and deseasonalized data (dashed black line). Trends are given

in Table 1.

Table 1Summary linear least squares statistics for observations (1996�2008) at the

CARIACO time-series station. Both observed and deseasonalized statistics are

presented. The years 2001 and 2002 were excluded from CO2 statistics because all

CO2 data from 2001 and six months from 2002 were missing due to equipment

failure.

Parameter Slope Intercept Standard error n R2 p-value

ObservedT 0.1 �174.5 0.04 150 0.04 o0.01

S �0.01 49.9 0.004 150 0.01 0.14

pH �0.0004 8.825 0.0005 118 0.01 0.44

TA �0.37 3161 0.44 114 0.01 0.39

nTA 0.10 2216 0.33 114 o0.01 0.76

TCO2 �0.19 2451 0.61 112 o0.01 0.76

nTCO2 0.23 1622 0.49 112 o0.02 0.64

fCO2 1.95 �3505 0.48 112 0.13 o0.01

nfCO2 0.40 �406 0.61 112 o0.01 0.51

Upwelling index �29.3 60050 12.3 151 0.04 o0.02

Wind speed �0.05 111.9 0.02 151 0.03 o0.03

DeseasonalizedT 0.09 �148.2 0.02 150 0.09 o0.01

S 0.11 �177.8 0.06 150 0.03 0.1

pH �0.0005 8.974 0.0004 118 0.01 0.25

TA �0.29 2988 0.35 114 0.01 0.41

nTA 0.12 2175 0.31 114 o0.01 0.70

TCO2 �0.04 2143 0.46 112 o0.01 0.94

nTCO2 0.30 1480 0.44 112 o0.02 0.50

fCO2 1.77 �3142 0.43 112 0.13 o0.01

nfCO2 0.51 �631 0.49 112 o0.01 0.29

Y.M. Astor et al. / Deep-Sea Research II ] (]]]]) ]]]–]]]6

dominates variability, thus increasing the uncertainty in calculat-ing interannual trends. In contrast, the observed SST, the upwel-ling index, and fCO2sea at the CARIACO time-series station alldisplay linear interannual trends for the period 1996–2008(Figs. 2 and 6, and Table 1).

A statistically significant change was observed for SST. The rate ofchange of measured SST at CARIACO was 0.170.04 1C yr�1

(R2¼0.04, po0.01; Fig. 2a, Table 1). This is similar to the surface

warming (0.1170.03 1C yr�1) reported by Padin et al. (2010) for theequatorial upwelling system of the Atlantic Ocean. During this time,upwelling intensity (measured through the Bakun upwelling index)

Please cite this article as: Astor, Y.M., et al., Interannual variability in sea surface temperature and fCO2 changes in the Cariaco Basin.Deep-Sea Res. II (2013), http://dx.doi.org/10.1016/j.dsr2.2013.01.002i

Y.M. Astor et al. / Deep-Sea Research II ] (]]]]) ]]]–]]] 7

and wind speed at CARIACO have been decreasing (Fig. 2c). Theseparameters showed a rate of change of �29.3712.3 m3 s�1 per100 m of coastline yr�1 (R2

¼0.04, po0.02) and �0.0570.02m s�1 yr�1 (R2

¼0.03, po0.03), respectively. Upwelling intensityand wind speed are closely related and have a great influence on SSTat the station.

The fCO2sea data also showed a statistical significant positivetrend of 1.9570.48 matm yr�1 (R2

¼0.13, po0.01; Fig. 6a,Table 1). The total observed variation in fCO2sea at the CARIACOstation from 1996 to 2008 was �24 matm, representing a changeof 6% during the study period. If the effect of temperature isremoved, the nfCO2sea shows a lower rate of increase of0.4070.61 matm yr�1, which yields a statistically insignificanttrend (R2

¼o0.01, p40.5, Fig. 6b and Table 1). Therefore, theeffect of SST on fCO2sea at CARIACO is very significant.

3.3.2. Deseasonalized hydrographic and CO2 parameters

The amplitude of the seasonal variability in many of themeasured parameters is large and can easily mask low-amplitude,low-frequency interannual changes. Therefore, the annual cyclewas removed (deseasonalized) to evaluate long-term trends (e.g.,Bates, 2007). Deseasonalized SST and fCO2sea trends were statis-tically significant (Table 1, Figs. 2 and 6a). SST increased0.0970.02 1C yr�1 (R2

¼0.09, po0.01), and fCO2sea increased at1.7770.43 matm yr�1(R2

¼0.13, po0.01). Deseasonalized nfCO2

data showed an increase of 0.5170.49 matm yr�1 (R2¼o0.01,

p40.3), but this change was not statistically significant.

3.4. Factors controlling fCO2 variability

From thermodynamics considerations, temperature changesmay cause variations of 4.13–4.23% fCO2sea per 1 1C (Gordon andJones, 1973; Takahashi et al., 1993). Therefore, surface warming of1 1C would drive a �16 matm increase in fCO2sea at CARIACO.Fig. 3 shows that SSTA and fCO2sea anomalies are mostly in phasewith each other. An increase/decrease of 1 1C is usually followedby an increase/decrease of 16–20 matm of fCO2sea. Thus, the SSTincrease of 1.3 1C between 1996 and 2008 accounted for 16 matmincrease in fCO2sea explaining around 72% of the fCO2sea observedvariation. This suggests that the changes measured in fCO2sea

were primarily the result of surface-ocean warming inCariaco Basin.

Upwelling of subsurface water plays an important role in bring-ing high concentrations of TCO2 to the surface, favoring an increaseof fCO2sea. However, upwelling also brings low-temperature, high-nutrient waters to the surface, which can counter the effect of highTCO2 concentrations by lowering fCO2sea through an increase in CO2

solubility and changes in H2CO3 dissociation constants, togetherwith an increase in carbon fixation that enhances the removal of CO2

from surface waters. There is a strong inverse relationship betweenchlorophyll a concentration and SST (R2

¼0.45, po0.01). The highestchlorophyll a levels were observed at the surface in 1996 and 2001in conjunction with temperatures below 22 1C. After 2004, surfacewater temperatures were consistently above the annual mean, whilechlorophyll a levels were low and TCO2 concentrations were high.

The decrease in intensity of upwelling events since 2004,associated with a weakening in wind stress during boreal winter,resulted in the upwelling of waters from shallower depths.However, higher concentrations of TCO2, likely from subsurfacewaters, still reach the surface during this period, as noted in asharp increase in TCO2 below 15 m during the upwelling season.Changes in SST, nutrients and TCO2 concentrations observed insurface waters depend not only on upwelling intensity, but alsoon the vertical gradients of these parameters beneath the mixed

Please cite this article as: Astor, Y.M., et al., Interannual variability inDeep-Sea Res. II (2013), http://dx.doi.org/10.1016/j.dsr2.2013.01.002

layer (Mahadevan et al., 2004). Surface waters at CARIACOnormally show consistently low nutrients levels in the upper35–55 m and only occasionally during strong upwelling events,when upwelled waters come from 60–80 m, do they have nitrateconcentrations above 1 mM (Scranton et al., 2006b). The weakupwelling that prevailed between 2004 and 2008 at the CARIACOstation only brought shallow subsurface water (20–30 m) to thesurface. Hence, the low nutrient concentration effectively reducedcarbon fixation, which led to an accumulation of CO2 in surfacewaters. Additionally, weaker winds decreased vertical mixing,exposing the recently upwelled water to heating for a longerperiod. The warming of this upwelled subsurface water with highTCO2 concentration strengthened the thermally driven evasion ofCO2 from the sea to the atmosphere.

Another source of CO2 to surface waters is the respiration ofdissolved organic carbon (DOC) by bacteria (Jiao et al., 2010). DOCconcentrations at the CARIACO site are controlled by biologicaland physical processes, mainly extracellular release of DOC byphytoplankton, grazing by zooplankton, and decomposition bybacteria, and upwelling/stratification of the water column(Lorenzoni et al., submitted for publication). The CARIACO sitedoes not receive significant input of DOC from land (Lorenzoniet al., 2009). Variations in the concentration of DOC between theupwelling and rainy season is �6%, with higher DOC concentra-tions during the rainy season due to the strong thermal stratifica-tion the basin experiences. During upwelling, the SubtropicalUnderwater that is injected into the surface is DOC-poor (averageof �57 mMC, Del Castillo, 1998; CLIVAR-Repeat Hydrography,transect 22). It is possible that a fraction of the surface DOC iseventually degraded by bacteria upwelled with the underlyingwater. Carlson et al. (2004) showed that bacteria in the uppermesopelagic can consume surface accumulated DOM. Unfortu-nately, we currently have no estimate of what fraction of surfaceDOC can be degraded by microbial respiration, but it is our beliefthat this process is not one of the most significant controls ofsurface fCO2 in the Cariaco Basin.

Diatoms historically dominated the phytoplankton populationat the CARIACO station during the upwelling season (Goni et al.,2003; Thunell et al., 2000). Carbon fixation by these organismsreduces TCO2 and fCO2sea. When upwelling decreases and surfacewaters warm smaller phytoplankton, such as coccolithophores,become more abundant. These organisms can affect surface waterfCO2sea through calcification, leading to depletion of dissolvedcarbonate ion (CO2�

3 ) and an increase in CO2 (Archer, 2003)according to the reactions:

CO2þCO2�3 þH2O22HCO�3 þCa2þ2CaCO3þH2OþCO2

In order to evaluate the influence of this biological process onfugacity, we examined the ratio of organic to inorganic carbon(Co/Ci) in the total carbon flux derived from sediment trapsamples collected at 225 m at the study site. This ratio was thencompared to the ratio of diatom to coccolithophore (D/C) cellnumbers in surface water samples collected monthly at the studysite. Previous work has shown that a decrease in surface fCO2sea

occurs when the Co/Ci ratio is larger than about 0.7 due to CO2

uptake during net photosynthesis (Honda et al., 1997). Conver-sely, a Co/Ci ratio below 0.7 is associated with the prevalence ofcalcification processes in surface waters that increases fCO2sea.Before 2005, Co/Ci values were above 0.7 in 48% of the sedimenttrap samples, while after 2005 only 13% of the samples had Co/Ci

ratios above 0.7. This is consistent with a shift in the phytoplank-ton community from diatoms to CaCO3-fixing organisms in thearea. Before 2005, the D/C ratio was 41 in 68% of the watersamples, suggesting that diatoms were dominant in most of thesamples. This number decreased to 52% after 2005. In addition toa shift in the composition of the phytoplankton community at the

sea surface temperature and fCO2 changes in the Cariaco Basin.i

-60

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ta f

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CO

2 fl

ux (

mm

ol C

m-2

d-1

)

Fig. 7. Time-series of (a) DfCO2 (matm, DfCO2sea¼ fCO2sea� fCO2atm) and (b) CO2

fluxes (mmol C m�2 d�1) at the CARIACO time-series station from January 1996 to

December 2008. In (b), black line-closed circles denote flux estimated based on the

formulation for the gas exchange constant, k, of Wanninkhof (1992). Gray line-

closed diamonds denote flux estimated with k based on Nightingale et al. (2000).

Y.M. Astor et al. / Deep-Sea Research II ] (]]]]) ]]]–]]]8

station, there was also a significant decrease in overall phyto-plankton biomass. The increase in calcifying organisms likelycontributed to the observed increase in surface water CO2;additionally, the decrease in upwelling observed after 2005 alsoaffected the efficiency of the biological pump’s ability to removeCO2. The coupling of these processes (i.e., the lack of removal ofthe upwelled TCO2 due to a decrease in carbon fixation and theshift in phytoplankton population) may explain the remaining28% increase observed in fCO2sea, and these two processes,together with temperature, potentially contributed to the highfCO2sea values observed during 2005–2008.

3.5. Sea-air CO2 fluxes

At the CARIACO station, the monthly DfCO2sea (DfCO2sea¼

fCO2sea� fCO2atm) values (Fig. 7a) for 1996–2008 did not showsignificant differences relative to what was found for 1996–2000(Astor et al., 2005a). The average value for the entire period was23721.5 matm. High positive values were present most of theyear except during months of maximum upwelling (Februaryand/or March). These observations confirm that this area is aconsistent source of CO2 to the atmosphere. Smaller variabilitywas observed during months of relaxation, when temperatureswere high (428 1C) and primary production was low(o1 gC m�2 d�1). Strong negative DfCO2sea were associated withthe drawdown of CO2 during strong upwelling events and anincrease in net primary production above 3 gC m�2 d�1. Duringthese events, the area becomes a sink of CO2.

Fig. 7b illustrates the sea-air CO2 fluxes at the CARIACO station.Negative CO2 flux values denote net air to sea CO2 flux, whereaspositive values denote net evasion from the sea. Over the entire

Please cite this article as: Astor, Y.M., et al., Interannual variability inDeep-Sea Res. II (2013), http://dx.doi.org/10.1016/j.dsr2.2013.01.002

time series, values ranged between �16.2 mmol C m�2 d�1 inFebruary 2003 and 16.9 mmol C m�2 d�1 in March 2007. Only16% of the observations (n¼112) have negative values. The lowwind speeds (5.271.1 m s�1) and the large positive DfCO2 values(0oDfCO2sea matmo60) led to moderate supersaturation withrespect to atmospheric CO2 most of the time. Only during times ofvery high primary production was the system undersaturated.Due to the large difference in DfCO2sea, the average net sea-airCO2 flux over the study period was 2.072.6 mol C m�2 yr�1

employing the Wanninkhof (1992) parameterization, and2.172.5 mol C m�2 yr�1 based on Nightingale et al. (2000). Thesevalues were large compared to fluxes calculated in other upwellingsystems (0.56 mol C m�2 yr�1 in the north of the Benguela system;Santana-Casiano et al., 2009; 0.9 mol C m�2 yr�1 in the Gulf ofOman; Goyet et al., 1998). However, they were lower than the ratecalculated by Astor et al. (2005a), 2.873.6 mol C m�2 yr�1 withthe Wanninkhof (1992) parameterization for a shorter period ofCARIACO observations. In the Cariaco Basin, the primary factorsregulating sea-air CO2 flux are the high seasonal variability ofupwelling and its direct effect on both oceanographic conditionsand biological production.

3.6. Effects of modes of climate variability on SST

Major changes have been observed from year to year inmeteorological and oceanographic conditions in the CariacoBasin. In order to establish whether the interannual variabilityobserved in the SST at the CARIACO station is associated withmodes of low-frequency climate variability, the SSTA time serieswas compared with several indices of climatic variability, includ-ing the North Atlantic Oscillation (NAO), the Atlantic MeridionalOscillation (AMO) and the El Nino/Southern Oscillation (ENSO).

Although the dominant mode of atmospheric variability in theNorth Atlantic region appears to be the NAO (Bates, 2001), wefound very weak correlation between NAO and the SSTA at theCARIACO station. Crosscorrelation analysis between SSTA and theNAO index shows no significant relationship at a number ofdifferent lags. However, a visual examination of a 12-monthrunning mean for SSTA and the NAO index (Fig. 8) does suggestthat NAO and SSTA show a similar behavior between 2000 and2004, and between 2007 and 2008.

The AMO (Enfield et al., 2001) is a global signal that is mostintense in the North Atlantic, affecting the entire basin. The AMOindex shows a cool phase when negative and a warm phase whenpositive. For our entire study period, AMO was in a cool phase.However, a well-defined periodicity in this index still needs to beestablished (Poore et al., 2009). The index has been linked tomulti-year precipitation anomalies over North America, andappears to modulate ENSO teleconnections (Enfield et al., 2001;McCabe et al., 2004). When compared to the SSTA of the CARIACOstation, a weak but significant relationship (R2

¼0.06, po0.01)was observed.

Changes in the tropical Atlantic Ocean lag the ENSO variabilityin the tropical Pacific Ocean by 3–9 months (Enfield and Mayer,1997; Giannini et al., 2000; Klein et al., 1999; Saravanan andChan, 2000). More specifically, modes of climate variabilityoriginating in the Atlantic and Pacific affect the Intra-AmericasSea (IAS, Gulf of Mexico-Caribbean Sea; Giannini and Cane,2001a). ENSO teleconnections affect multiple processes in theCaribbean Sea, including geostrophic transport (Alvera-Azcarateet al., 2009), precipitation (Jury et al., 2007), and the phytoplank-ton community structure within the Cariaco Basin (Romero et al.,2009). When the Southern Oscillation index (SOI) was comparedto SSTA at CARIACO, no statistically significant relationship wasobserved. However, when a 9-month running mean was appliedto both the SSTA and SOI, a pattern was observed where periods

sea surface temperature and fCO2 changes in the Cariaco Basin.i

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Fig. 8. (a) Time-series of the (a) NAO index (gray line) and SSTA (black line) and

(b) of the SO index (gray line) and SSTA (black line) at the CARIACO time-series

station. The time-series of SSTA and NAO index were smoothed by a 12-month

running mean. The time-series of SSTA and SOI were smoothed by a 9-month

running mean.

Y.M. Astor et al. / Deep-Sea Research II ] (]]]]) ]]]–]]] 9

of warm SSTA followed a negative SOI with a 3–6 months lag,while cold SSTA lagged a positive SOI (Fig. 8b). A very strongnegative SOI event occurred in 1997 and part of 1998, and warmtemperatures were recorded at the CARIACO station between1998 and 2000. ENSO-related atmospheric anomalies are knownto force a warming of tropical North Atlantic SST through theweakening of the northeasterly trade winds (Giannini et al.,2001b). When comparing the wind speed anomaly in the regionto SOI, a relatively weak but significant relationship (R2

¼0.06,po0.01) was observed. A crosscorrelation analysis showed ahigher relationship (R2

¼0.12, po0.01) at one month lag.The interaction among several modes of climate variability and

forcing mechanisms seem to modulate interannual SST variabilityin the Caribbean region (Munoz et al., 2010); however, thecorrelations between SSTA and these climate signals in CARIACOonly show very weak relationships. Nevertheless, the CARIACOtime-series seems to be recording the signals generated fromthese interactions, and may prove invaluable in time for under-standing the impacts of large-scale processes on regional bio-chemical and ecological changes.

4. Conclusions

The observations collected between 1996 and 2008 at theCARIACO time-series station provide new insight into seasonaland interannual controls of the inorganic carbon system in thisupwelling-dominated tropical continental margin. The main

Please cite this article as: Astor, Y.M., et al., Interannual variability inDeep-Sea Res. II (2013), http://dx.doi.org/10.1016/j.dsr2.2013.01.002

process controlling the long-term changes in surface fCO2sea atCARIACO was temperature, with net community productionplaying a secondary role. Over the study period, deseasonalizedSST increased by 0.0970.02 1C yr�1, representing an overallincrease of 1.13 1C in 13 years. Despite large seasonal variability,the deseasonalized fCO2sea data for the CARIACO time-seriesstation also showed a statistically significant interannual increaseof 1.7770.43 matm yr�1. Thermodynamic effects explained 72%of the fCO2sea variability in surface waters. A decrease in upwel-ling intensity between 2004 and 2008 also contributed to thischange. Warmer waters with low primary production and highTCO2 and fCO2 prevailed for much of the period of observation. Atthe CARIACO site, the ocean is primarily a source of CO2 to theatmosphere, except during strong upwelling events.

The relationship between SST and wind speed anomalies andmodes of climate variability, such as NAO, AMO and SOI were alsoassessed. Weak but significant relationships between SSTA andthe AMO (R2

¼0.06, po0.01) and wind speed anomaly and SOI atone month lag (R2

¼0.12, po0.01) were found. A weakening ofthe winds measured around the Cariaco Basin lagged a negativeSOI by 1–3 months. Future studies should attempt to furtherunderstand the relationship among these modes of climate andtheir connection with the changes in hydrography in the CariacoBasin, an important archive of past tropical climate change.

Acknowledgments

The Consejo Nacional de Investigaciones Cientificas y Tecno-logicas(CONICIT, VENEZUELA, Grant 96280221) and Fondo Nacio-nal de Ciencia y Tecnologıa (FONACIT, Venezuela, Grant2000001702) to RV, the National Science Foundation (NSF GrantsOCE-0752139, OCE-9216626, OCE-9729284, OCE-9401537, OCE-9729697, OCE-9415790, OCE-9711318, and OCE 0963028 to FMK;OCE-9415790, OCE-9711318, OCE-9730278 and OCE-0118491,OCE-0326175, and OCE-0752014 to MIS and GTT; OCE-0752037and OCE-1039503 to RT), and NASA (NASA Grants NAG5-6448 yNAS5-97128 to FMK) supported this work. We are indebted to thepersonnel of the Fundacion La Salle de Ciencias Naturales, Esta-cion de Investigaciones Marinas, Isla Margarita (FLASA/EDIMAR)who have been responsible for the collection, analysis, and qualitycontrol of the data presented here, and the crew of the R/VHermano Gines for their enthusiasm and professional support. Inparticular we thank Dr. Pablo Mandazen (Hermano Gines, FLASAfounder) for his confidence in our activities. Kent Fanning fromthe University of South Florida provided nutrient data. Theauthors are grateful to Dr. Chris Sabine for his help in theintercalibrations, and we are also thankful to Andrew Dicksonfor the continued supply of certified references materials forTCO2. A special thanks to all the students from Instituto Uni-versitario de Tecnologıa del Mar (IUTEMAR), Universidad deOriente (UDO), University of South Florida (USF), University ofSouth Carolina (USC) and Stony Brook University for their colla-boration in the field sampling of different cruises.

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