IS THERE A HIGHER CANT STORAGE

Slides:



Advertisements
Similar presentations
Age and AOU increases at the North Pacific subtropical-subpolar gyre boundary PICES 13th Annual Meeting, Honolulu, HI Sabine Mecking Woods Hole Oceanographic.
Advertisements

Global climate responses to perturbations in Antarctic Intermediate Water Jennifer Graham Prof K. Heywood, Prof. D. Stevens, Dr Z. Wang (BAS)
- Perspectivas actuales en el estudio de la evolución del CO2 en la superficie del océano => case studies - Perspectivas actuales en el estudio de la.
Essentials of Oceanography
Oceanography Chapter Heating of Earth’s surface and atmosphere by the sun drives convection within the atmosphere and oceans, producing winds and.
Ocean Circulation And Current Carbon Cycle For more detail see the course materials for Lynne Talley’s Course at SIO.
Lecture 2 - Major Ions in Sea Water Why do we care about the major ions? What is the composition of seawater? What defines Major Ions? What are their concentrations?
GEOF236 CHEMICAL OCEANOGRAPHY (HØST 2012) Christoph Heinze University of Bergen, Geophysical Institute and Bjerknes Centre for Climate Research Prof. in.
Sarmiento and Gruber (2002) Sinks for Anthropogenic Carbon Physics Today August
Density - density is a key property of seawater - one of the most important parameters in ocean dynamics - the ocean forms layers by density (denser waters.
Lecture 16 Oxygen distributions and ocean ventilation Thermocline Ventilation and Deep Water Formation Oxygen Utilization rates.
Global Conveyor Belt. Conveyor Belt Circulation Diagnose conveyor belt pathways – Mass, volume, heat & salt budgets (inverse analysis) Water mass analysis.
The Anthropogenic Ocean Carbon Sink Alan Cohn March 29, 2006
SIO 210 Typical distributions (2 lectures) Fall 2014
Chapter 9.
NADW AABW AAIW Itay Halevy
A Multiple Linear Regression of pCO2 against Sea Surface Temperature, Salinity, and Chlorophyll a at Station BATS and its Potential for Estimate pCO2 from.
Core Theme 4 : Biogeochemical Feedbacks on the Oceanic Carbon Sink. M. Gehlen (CEA/DSM/LSCE) CarboOcean Annual Meeting Bremen 4-7/12/2007.
FIGURE 4.1 (a) Surface temperature (°C) of the oceans in winter (January, February, March north of the equator; July, August, September south of the equator)
1/6 Palma, March 2012 ODV practical: water masses and C ANT distribution In the Indian Ocean OCEAN DATA VIEW
WP13: Regional assessment for the Mediterranean Sea Partner 22: University of Perpignan, France Catherine Goyet. CARBOOCEAN.
DECADAL CHANGES IN OCEAN CARBON UPTAKE C.L. Sabine, R.A. Feely, G.C. Johnson, R. Wanninkhof, F.J. Millero, A.G. Dickson, N. Gruber, R. Key and P. Covert.
Two research cruises were successfully conducted in 2013 and Shipboard and moored observations show that: at first glance no significant decadal.
1.Introduction 2.Description of model 3.Experimental design 4.Ocean ciruculation on an aquaplanet represented in the model depth latitude depth latitude.
CarboOcean 2009 CARINA - Carbon dioxide in the Atlantic Ocean Will allow for improved estimates of ocean carbon inventory and transport Data rescue project.
1-Slide Summary Explicit Southern Ocean eddies respond to forcing differently than parameterizations.  We need eddy resolving ocean climate models. Spurious.
Towards higher resolution, global-ocean, tracer simulations
Arrigo (2005) Marine Microorganisms and Global Nutrient Cycles Nature 437: Issues: Redfield stoichiometry Co-limitation N 2 -Fixation Anammox.
1/30 IS THERE A HIGHER C ANT STORAGE IN THE INDIAN OCEAN? Estimating the storage of anthropogenic carbon in the subtropical Indian Ocean: a comparison.
WOCE hydrographic Atlas, 1 As a result of the World Ocean Circulation Experiment (WOCE), a hydrographic survey of the world oceans occurred from
Introduction to Ecosystem Monitoring and Metabolism
Novel features in this model: - - Ten million solutions for random values of the 10 circulation and productivity parameters are obtained. - - The preformed.
 Instrumentation  CTD  Dissolved Oxygen Sensor  ADCP/ Current Meters  Oxygen Titrations  Nutrient Concentrations Circulation and Chemical Tracer.
Ciclo global del carbono Land use change Land sink y su perturbación antropogénica.
Chapter 15 Earth’s Oceans. The Global Ocean One vast body of water covering more than two thirds of Earth’s surface Oceans contain 97% of the water on.
First results from the isopycnic ocean carbon cycle model HAMOCC & MICOM/BCM Karen Assmann, Christoph Heinze, Mats Bentsen, Helge Drange Bjerknes Centre.
1 Claire Lo Monaco, Andrew Lenton and Nicolas Metzl (LOCEAN-IPSL, Paris) Natural and Anthropogenic Carbon Changes in the South Indian Ocean.
CO 2 and Climate Change. Lisiecki & Raymo,
An example of vertical profiles of temperature, salinity and density.
Water Mass Distribution OEAS 604 Lecture Outline 1)Thermohaline Circulation 2)Spreading pathways in ocean basins 3)T-S diagrams 4)Mixing on T-S diagrams.
OC3230-Paduan images Copyright © McGraw Hill Chap 7-8: Distributions SPECIAL DATES: MPA meeting…6 Jul R/V Pt Sur Cruise…14 Jul R/V Pt Sur Cruise…25 Jul.
ANTHROPOGENIC CARBON IN THE ATLANTIC OCEAN: COMPARISON OF FIVE DATA-BASED CALCULATION METHODS Marcos Vázquez-Rodríguez 1, Franck Touratier 2, Claire Lo.
Sverdrup Lecture 2008 Chlorofluorocarbons: The Oceans’ Inadvertent Canary Rana A. Fine Rosenstiel School of the University of Miami.
Salinity and Density Differences VERTICAL STRUCTURE, THERMOHALINE CIRCULATION & WATER MASSES.
IPCC AR4 Chapter 5 Oxygen decline at base of pycnocline throughout subpolar and subtropical N. Pacific: reduced ventilation Deutsch et al. (2005) IPCC.
Michael J. McPhaden & Dongxiao Zhang NOAA/PMEL Decadal Variability and Trends of the Pacific Shallow Meridional Overturning Circulation and Their Relation.
SMOC Brazil 2010 Monitoring the Formation Rate of NADW Components Using Tracer Inventories Rana A. Fine Rosenstiel School, University of Miami Studies.
Quantifying the Mechanisms Governing Interannual Variability in Air-sea CO 2 Flux S. Doney & Ivan Lima (WHOI), K. Lindsay & N. Mahowald (NCAR), K. Moore.
Oceans & Anthropogenic CO 2 V.Y. Chow EPS 131.  CO 2 exchange across sea surfaces in the oceans  Measurement methods of anthropogenic CO 2  Distributions.
Global ocean uptake and storage of anthropogenic carbon estimated using transit-time distributions Samar Khatiwala Collaborators: Tim Hall (NASA/GISS)
FIGURE 4.1 TALLEY Copyright © 2011 Elsevier Inc. All rights reserved (a) Surface temperature (°C) of the oceans in winter (January, February, March north.
I. Objectives and Methodology DETERMINATION OF CIRCULATION IN NORTH ATLANTIC BY INVERSION OF ARGO FLOAT DATA Carole GRIT, Herlé Mercier The methodology.
Franck Touratier & Catherine Goyet EA 1947 BDSI, Université de Perpignan, France UNIVERSITE DE PERPIGNAN BIOPHYSIQUE ET DYNAMIQUE DES SYSTEMES INTEGRES.
Our water planet and our water hemisphere
Density-Driven Downwelling and Thermohaline Circulation
OCEAN RESPONSE TO AIR-SEA FLUXES Oceanic and atmospheric mixed
Essentials of Oceanography
Music today: Little Mermaid, “Under the Sea” WELCOME OSU MOMS!!
Erin McCabe Alison Gray, Keith Rodgers, Ping Zhai
The Oceanic Sink Uptake in the mixed layer
Doney (2010) The Growing Human Footprint on Coastal
Heat Transport by the Atmosphere and ocean
MERIDIONAL TRANSECTS AIMS
Ocean Circulation based on Density: Temperature and Salinity
Warm-up What is ocean water made of?
Impacto del cambio global en los ciclos del N, P, C y metales
Eutrophication indicators PSA & EUTRISK
Lauren Santi and Alison Gray
Deep Ocean Circulation
Presentation transcript:

IS THERE A HIGHER CANT STORAGE IN THE INDIAN OCEAN? Estimating the storage of anthropogenic carbon in the subtropical Indian Ocean: a comparison of five different approaches M. Álvarez, C. Lo Monaco, T. Tanhua, A. Yool, A. Oschlies, J. L. Bullister, C. Goyet, N. Metzl, F. Touratier, E. McDonagh, and H. L. Bryden, Biogeosciences, 6, 681-703, 2009. http://www.biogeosciences-discuss.net/6/729/2009/bgd-6-729-2009.html

CANT inventory referred to 1994 = 110 ± 13 Pg C CANT ALONG CD139 CRUISE (2002) 32ºS INDIAN OCEAN CANT inventory referred to 1994 = 110 ± 13 Pg C Indian Ocean contains - 21% of the total CANT inventory - half of the Atlantic CANT inventory despite having only 20% less area Indian Ocean Pacific Ocean Atlantic Ocean 44.8  6 Pg 20.3  3 Pg 44.5  5 Pg (Sabine et al, Science 2004)

Indian Ocean CANT vertical distribution mmol/kg CANT ALONG CD139 CRUISE (2002) 32ºS INDIAN OCEAN Indian Ocean CANT vertical distribution mmol/kg RedSea /Persian Gulf Intermediate Water Antarctic Intermediate Water (AAIW) AAIW marks the deepest CANT penetration in the Subtropical gyre No CANT in deep and bottom waters (Sabine et al, Science 2004)

CANT ALONG CD139 CRUISE (2002) 32ºS INDIAN OCEAN Hypothesis: CANT penetrates deeper than 1000-1500 m How to assess this question: compare different CANT methods -> difficult: every method has high uncertainties help: relation of CANT with tracers (CFC12, CCl4)

CANT ALONG CD139 CRUISE (2002) 32ºS INDIAN OCEAN On board R/V Charles Darwin, CD139 cruise, 1/3 – 15/4/2002, from Durban to Freemantle P.I.: Harry Bryden (National Oceanographic Centre, Southampton, UK) Physics: temperature, salinity, ADCP, LADCP Chemistry: oxygen, salinity, nutrients, CO2 (pH & TA, TIC), CFCs (11, 12, 113), CCl4.

CANT ALONG CD139 CRUISE (2002) 32ºS INDIAN OCEAN Salinity (psu) Africa Australia SAMW SAMW SAMW SAMW AAIW AAIW AAIW AAIW NADW NADW NADW CDW AABW AABW

CANT ALONG CD139 CRUISE (2002) 32ºS INDIAN OCEAN Australia Africa CFC-12 (pmol/kg) SAMW SAMW SAMW AAIW AAIW AAIW CDW NADW CDW AABW AABW

CANT ALONG CD139 CRUISE (2002) 32ºS INDIAN OCEAN CANT TECHNIQUES CANT SAB99: method by Sabine et al. (GBC,1999), using their DCDis CANT LM05: method by LoMonaco et al. (JGR, 2005) CANT TrOCA: Touratier & Goyet (Tellus, 2007) CANT TTD CANT from OCCAM model

CANT ALONG CD139 CRUISE (2002) 32ºS INDIAN OCEAN Back-calculation technique by Sabine et al. (GBC, 1999) to estimate CANT. CANT = DC* - DCDis = C – AOU/RC – ½(TA + AOU/RN ) + 106/104 · N* - C280 – DCDis C is the current total inorganic carbon  TA = TA - TA0, current alkalinity - preformed alkalinity TA0= 378.1 + 55.22 · Sal + 0.0716 · PO - 1.236 · Tpot AOU is the Apparent Oxygen Utilization, assuming oxygen saturation C280 is the inorganic carbon in equilibrium with the preindustrial atmosphere. C280 = f (Tpot, Sal, TA0, pCO2280) from thermodynamic equations pCO2280 = CO2 fugacity at a 100% of water vapor pressure in uatm = f(Tpot, Sal, 280) C280 in GSS96 => constants by Goyet & Poisson (1989) & a constant pCO2280 = 280 uatm linearilized equation: C280 = 2072 - 8.982 · (Tpot - 9) - 4.931 · (Sal - 35) + 0.842 · (TA0- 2320) N* = (0.87 · (NO3 - 16 · PO4 + 2.9)) term accounting for the denitrification

CANT ALONG CD139 CRUISE (2002) 32ºS INDIAN OCEAN

CANT ALONG CD139 CRUISE (2002) 32ºS INDIAN OCEAN DCDis is obtained with own CD139 data using CFC12 ages and limit at 40 years a) Old deep waters, CANT = 0 => DC* = DCDis b) In upper waters, having the age: DCDis = DC*t|σ=cte DC*t = C - CBio - C t where Ct = f (Tpot, Sal, TA0, pCO2t) pCO2 in the atmosphere at 2002 – age (t) c) In between => weigthed mean DC* and DC*t|s=cte

CANT ALONG CD139 CRUISE (2002) 32ºS INDIAN OCEAN Fig. 4. Air-sea CO2 disequilibrium (mmol kg-1) by  density intervals. Blue points correspond to the values taken directly from SAB99 work, light blue and orange points correspond to the values estimated using the CD139 biogeochemical data, following SAB99 (orange) and combined (light blue) methods. Interpolated points are highlighted with black open circles.

CANT ALONG CD139 CRUISE (2002) 32ºS INDIAN OCEAN Back-calculation technique by Lo Monaco et al. (JGR, 2005): CANT = CT – CBio - CT0 obs – (CT– CBio – C0 obs) REF CT = measured TIC CBio = 0.73·(O20 – O2) + 0.5·(TA – TA0) => biological activity variation in TIC TA0 => preformed TA O20 = O2sat – a·K·O2Sat => aO2 = 12% undersaturation K = > mixing ratio of ice-covered water (OMP) C0 obs => preformed TIC currently observed in the formation area water masses REF = reference water where no CANT should be detected.

CANT ALONG CD139 CRUISE (2002) 32ºS INDIAN OCEAN Back-calculation technique by Lo Monaco et al. (JGR, 2005) TA0 = k(S) TA0(S) + k(N) TA0(NADW) C0,obs = k(S) C0,obs(S) + k(N) C0,obs(NADW) southern relationships: winter surface data from the Atlantic and Indian oceans (WOCE and OISO cruises) TA0(S) = 0.0685 PO + 59.787 S - 1.448  + 217.15 (± 5.5 µmol/kg, r2 = 0.96, n = 243) C0,obs(S) = -0.0439 PO + 42.79 S - 12.019  + 739.83 (± 6.3 µmol/kg, r2 = 0.99, n = 428) northern relationships subsurface data from the North Atlantic and Nordic Seas (WOCE and KNORR cruises) TA0(N) = 42.711 S + 1.265  + 804.6 (± 9.3 µmol/kg, r2 = 0.92, n = 297) C0,obs(N) = 10.69 S + 0.306 NO + 1631.6 (± 9.2 µmol/kg, r2 = 0.79, n = 364) mixing ratios of southern and northern waters: k(S) + k(NADW) = 1 determined from OMP analysis

CANT ALONG CD139 CRUISE (2002) 32ºS INDIAN OCEAN Back-calculation technique by Lo Monaco et al. (JGR, 2005): OMP analysis modified from Lo Monaco et al. (JGR, 2005) Endmembers: AAIW, NADW-E, NIDW, Indian Water, WDS/CDW, ISW Weddell Variables: Sal, Tpot, SiO2 and NO Salinity SiO2 NO Tpot

CANT ALONG CD139 CRUISE (2002) 32ºS INDIAN OCEAN Back-calculation technique by Lo Monaco et al. (JGR, 2005): OMP Tpot, Sal, SiO2 NO STD Res. 0.0481 0.0051 1.3 3 R2 0.9979 0.9967 0.9973 0.9611 (n=1299)

CANT ALONG CD139 CRUISE (2002) 32ºS INDIAN OCEAN 2. Back-calculation technique by Lo Monaco et al. (JGR, 2005): OMP Africa Africa Australia Australia NADW contribution Ice-covered SW contribution

CANT ALONG CD139 CRUISE (2002) 32ºS INDIAN OCEAN Back-calculation technique by Lo Monaco et al. (JGR, 2005): CANT = CT – CBio - CT0 obs – (CT– CBio – C0 obs) REF REF = NADW= reference water where no CANT should be detected. Applied to samples with more 50% NADW from OMP analysis (CT – CBio – C0 obs) REF = - 54.4 ± 1.4 umol/kg (LoMonaco JGR2005 -51 umol/kg) CANT = CT – CBio - CT0 obs – (- 54.4)

CANT ALONG CD139 CRUISE (2002) 32ºS INDIAN OCEAN CANT TrOCA, Touratier et al (Tellus B, 2007): TrOCA = O2 + a · (CT -1/2 ·TA) a = ψO2 / [ψCO2 + ½ ·( ψ H+ − ψHPO24−)] CANT (TrOCA) = (TrOCA – TrOCA280) / a CANT = (O2 + 1.279 · (CT – 0.5 · TA) – exp (7.511-0.01087· θ -781000/TA2))/1.279)

CANT ALONG CD139 CRUISE (2002) 32ºS INDIAN OCEAN 4. CANT TTD (Waugh et al., 2004; 2006; Tanhua et al., 2008): - each water sample has its own “age”, i.e. time since it was last in contact with the atmosphere. The sum of all these ages makes the TTD of a water sample - the mean age ( ) and the width of the TTD () are assumed to be of equal magnitude: realistic assumption of the relation between advective and diffusive transport in the Ocean - CANT is an inert passive tracer where air-sea disequilibrium hasn’t changed over time.

CANT ALONG CD139 CRUISE (2002) 32ºS INDIAN OCEAN 5. CANT OCCAM global, medium-resolution, primitive equation ocean general circulation model (Marsh et al., 2005).  OCCAM's vertical resolution is 66 levels (5 m thickness at the surface, 200 m at depth), with a horizontal resolution of typically 1 degree. Advection is 4th order accurate, and the model is time-integrated using a forward leapfrog scheme with a 1 hour time-step.  Surface fluxes of heat and freshwater not specified but are calculated empirically using NCEP-derived atmospheric boundary quantities (Large and Yeager, 2004).  OCCAM incorporates a NPZD plankton ecosystem (Oschlies, 2001; Yool et al., 2007) which drives the biogeochemical cycles of nitrogen, carbon, oxygen and alkalinity. 

CANT ALONG CD139 CRUISE (2002) 32ºS INDIAN OCEAN CANT vertical distributions Troca TTD OCCAM pCFC12 & pCCl4 SAB99 LM05

CANT ALONG CD139 CRUISE (2002) 32ºS INDIAN OCEAN CANT mean profile differences

CANT ALONG CD139 CRUISE (2002) 32ºS INDIAN OCEAN Neutral density layers & salinity Australia Africa Surface SAMW AAIW Deep Bottom

CANT ALONG CD139 CRUISE (2002) 32ºS INDIAN OCEAN CANT mean inventories

CANT ALONG CD139 CRUISE (2002) 32ºS INDIAN OCEAN Surface, SAMW waters and upper AAIW Revelle = 10 Revelle = 13 Fig. 10. Partial pressure of CFC-12 (ppt) and CANT estimates (mmol kg-1) for upper waters with potential temperature higher than 5ºC, pressure higher than 200 dbar and CFC-12 age less than 30 years. Also shown in black is the atmospheric evolution of CFC-12 and CANT using Revelle factors of 10 and 13 (see text for details), some time markers are shown. pCFC-12

CANT ALONG CD139 CRUISE (2002) 32ºS INDIAN OCEAN Deep and bottom waters Fig. 11. a) Partial pressure of CFC-12 (ppt) and b) partial pressure of CCl4 (ppt) versus CANT (mmol kg-1) estimates for deep waters with potential temperature lower than 5ºC, pressure higher than 200 dbar and CFC-12 age higher than 40 years. In the case of CCl4, the temperature limit is 3ºC. Also shown in black are the atmospheric evolution of CFC-12, CCl4 and CANT using Revelle factors of 10 and 13 (see text for details), some time markers are shown.

CANT ALONG CD139 CRUISE (2002) 32ºS INDIAN OCEAN Inventories Table 1. Mean  standard deviation CANT specific inventory (molC m-2) by water masses in the subtropical Indian Ocean for the different methods here evaluated. Mean and standard deviation values were obtained randomly modifying the initially calculated single CANT values by 5 mmol kg-1. A set of 100 perturbations were done for the five methods. The standard deviation for each layer is weighted by the layer contribution to the total section area. See text for the acronyms. N/D stands for not determined. Values between brackets correspond to the LM05 method assuming a 100% oxygen saturation in equation (7), =0. Upper SAMW AAIW Deep Bottom Total* SAB99 N/D 8.50.5 8.10.4 00.5 0.30.2 23.9 2 LM05 110.7 110.5 0.60.4 (0.50.4) 1.20.3 (0.00.3) 30.82.5 (29.52.5) TrOCA 8.40.5 9.40.5 1.90.5 1.40.3 28.12.2 TTD 7.2 0.7 9.30.6 9.30.5 20.4 1.30.2 28.92.3 OCCAM 6.91.5 9.30.8 7.60.5 0.50.1 00 24.4 2.8 * The total specific inventory is calculated as the sum of the SAMW, AAIW, Deep and Bottom contributions plus 7 molC m-2, i.e., the TTD and OCCAM mean specific inventory for the upper layer.

CANT ALONG CD139 CRUISE (2002) 32ºS INDIAN OCEAN Conclusions This work investigates the CANT penetration and inventory in the subtropical Indian Ocean along 32ºS calculated with data collected in 2002. Five different methods are compared and discussed: three carbon-based methods (DC*, LM05 and TrOCA), TTD and a simulation from the OCCAM global model. Comparatively, the DC* method seems to yield too shallow penetration of CANT, with no or very low CANT detected in deep or bottom waters, mainly due to the formulation and assumptions of DCTdis. Our results indicate that SAB99 DCTdis values are inconsistent with the current air-sea CO2 disequilibrium found in current Indian Ocean winter DCTdis values. Although this could also be misleading taking into account that water masses are usually formed in particular times and areas of the ocean. Previous estimates of CANT inventory in the subtropical Indian Ocean with the DC* method appear to be underestimates. Considering the CANT estimates derived from those methods consistent with the tracer distributions and the knowledge about water masses, our best estimate for the mean CANT specific inventory is 282 molC m-2 which compares with 242 molC m-2 from DC*, 17% higher.

CANT ALONG CD139 CRUISE (2002) 32ºS INDIAN OCEAN Hypothesis: CANT penetrates deeper than 1000 m (Sabine et al 1999) How to assess this question: difficult: every method has uncertainties help: relation of CANT with tracers (CFC12, CCl4) seems to be hinted by any other method absolutely true, no method is perfect questions still arise, saturation, mixing, etc.. community should combine methods and time-evolution studies at specially sensitive regions OPEN DISCUSSION: KEY REGION ….. THE SO

CANT ALONG CD139 CRUISE (2002) 32ºS INDIAN OCEAN Discusión: ¿Cuáles son las asunciones de cada método? ¿nos creemos el desequilibrio? ¿Qué método os parece el más fiable? ¿Se os ocurre como evaluar los métodos de otra manera?