Effect of deep-sea sedimentary calcite preservation on atmospheric CO2 concentration

D. Archer1

Lamont-Doherty Earth Observatory

Palisades, NY 10964

and

E. Maier-Reimer

Max-Plank-Institut für Meteorologie

Bundesstra[[beta]]e 7, D-2000 Hamburg 54

1Presently at: Department of Geophysical Sciences

5734 South Ellis Avenue

University of Chicago

Chicago, Ill 60637

The partial pressure of CO2 (pCO2) of the glacial atmosphere was 30% lower than pre-anthropogenic interglacial values1. While the cause of this change is generally accepted to be oceanographic, the mechanism has not been determined. We present a global ocean/sediment circulation and carbon cycle model, and explore the relationship between deep sea sediment chemistry and atmospheric pCO2. On time frames of thousands of years, the pH of the ocean (and hence atmospheric pCO2) is determined by a steady state balance between the supply rate of carbonate alkalinity from terrestrial weathering and alteration and removal by calcium carbonate burial in sediments2, 3, 4. Degradation of organic carbon in sediments promotes dissolution of calcium carbonate5, 6, so that a change in the ratio of rain rates of organic carbon and calcite to the sea floor drives a compensating change in ocean pH to maintain steady state. When organic-driven calcite dissolution is included in our carbon cycle model, a 40% decrease in the calcite precipitation rate (production) is sufficient to decrease pCO2 to glacial values. The response time of model pCO2 to a change in calcite production is similar to the observed pCO2 transition time following the last glacial termination1.

The solubility of calcite (CaCO3) in sea water increases with pressure, so that the ocean is typically supersaturated at shallow and intermediate depths and undersaturated in the deepest waters. Only a fraction of the global calcite production is buried, and this proportion depends on the area of the sea floor that is shallower than the depth of calcite saturation. Any imbalance in the sources (terrestrial weathering and alteration) and sinks (deep sea and shallow water deposition) for CaCO3 will change the ocean dissolved carbonate ion concentration ([CO3=]) in the direction of restoring throughput balance. Through this mechanism, called "CaCO3 compensation" 2, 3, 4, the steady state deep sea calcite burial rate is a slave to weathering less shallow water deposition, which we refer to as the "deep sea carbonate influx". The pH equilibrium reaction

maintains an inverse relationship between [CO3=] and pCO2.

We simulate the coupled ocean / sediment carbon cycle using the global ocean circulation / carbon cycle model of Maier-Reimer7, 8, to which we have coupled the sediment calcite dissolution model of Archer6. Without the detailed sedimentary component the ocean model is unable to drive the atmospheric pCO2 to lower glacial values without violating paleoceanographic data7. Here we predict the ocean alkalinity ([HCO3-] + 2[CO3=] + [B(OH)4-]) and total CO2 ([CO2] + [HCO3-] + [CO3=]), rather than specifying present-day values, based on the constraint that the deep sea calcite burial rate equals the deep sea carbonate influx (which is imposed as a source of alkalinity and total CO2 to the surface ocean, in the ratio of 2:1). The deep sea alkalinity influx for the "standard case" (intended to mimic present-day conditions) is 1.2 GT CaCO3 yr-1( Ref. 9, 10). The model distributions of alkalinity and total CO2, and therefore the calcite saturation state of deep water, compare well with oceanic observations (Figure 1a and Refs. 7 and 8). Although the glacial distributions of nutrients, d13C, and sedimentary calcite were influenced by changes in circulation, we use the present-day ocean circulation field throughout.

The calcite diagenesis model6 calculates the calcite dissolution rate from the steady-state concentration profiles of the carbonate species CO2, HCO3-, and CO3= in the diffusive sediment pore water. Within the constraints of in situ microelectrode data11, sediment trap data, pore water chemical data, and calcite accumulation rates, the model predicts the observed patterns of calcite preservation in the ocean6 ( Figure 1b). The steady state sedimentary calcite distribution in the "standard case" model is compared with observations in Figures 2a and 2b. The model calcite distribution is smoother than observations because of the smoothness of the model topography.

One proposed explanation for lower glacial pCO2 is called the "coral reef hypothesis"12, 13. In the present day ocean, up to half of the total oceanic CaCO3 removal may be by growth of coral reef complexes13. The rate of coral growth might be tied to fluctuations in sea level relative to the level of the continental shelves, with low coral growth rates during glacial times when the shelves are exposed and surface temperatures are cooler. A shift of the "locus of CaCO3 deposition" to the deep sea would require a higher ocean [CO3=], and hence a lower pCO212, 13. The steady state pCO2 predicted by our model appears to respond linearly to variations in the deep sea carbonate influx (Figure 3a and 3b). In order for our model to achieve the magnitude of the observed glacial / interglacial pCO2 changes, the glacial deep sea calcite burial rate has to be 2-3 times higher than today's value. Under these conditions, high-calcite sediments dominate the sea floor (Figure 2c). This prediction is clearly at odds with the sedimentary record14, 15. Although a better test of the coral reef hypothesis would be a time dependent calculation13, and we present a steady state, the atmospheric pCO2 recorded by the Vostok ice core was depressed to the 180 - 220 uatm range for 50 kyr16. This time period is long enough for sediments to have approached their steady state condition. Our results support the conclusion that cycles in the global growth rate of corals would have a significant impact on pCO2; however, we show that the coral-reef mechanism by itself cannot account for the entire glacial / interglacial pCO2 signal.

We propose a new explanation for lower glacial pCO2 that relies in part on the effect of sedimentary organic carbon degradation on calcite dissolution. Diagenetic models for calcite dissolution predict that a significant fraction of the calcite rain to the sediments dissolves in response to the addition of CO2 to the pore water by oxic organic carbon degradation5, 6 (a process we will refer to as "respiratory calcite dissolution", see Figure 1b and 1c). If sedimentary calcite dissolution is represented as the sum of respiratory dissolution and dissolution driven by the overlying water [CO3=], an increase in one, globally, will require a decrease in the other to maintain steady state. Therefore an increase in the organic carbon to calcite rain rate ratio to the sediments will drive an increase in [CO3=], and a corresponding decrease in pCO2, through the mechanism of CaCO3 compensation.

We test this hypothesis by altering the fraction of organic carbon and calcite production that reaches the sea floor (Figure 3b, c). Since only a small fraction of production reaches the ocean bottom, altering this fraction has only a minor impact on the tracer source/sink functions in the water column. In order to isolate the effect of respiratory calcite dissolution, we ran model simulations both with and without the effect of respiratory calcite dissolution. When respiratory calcite dissolution is neglected in the simulations, we find that pCO2 is somewhat sensitive to calcite rain to the sea floor, and insensitive to organic carbon rain, consistent with previous studies17. In contrast, when respiratory calcite dissolution is included in the simulation, pCO2 becomes much more sensitive to organic carbon and calcite rain rates (Figure 3b-d, solid lines). We also simulate an ecological shift from calcitic to silicious organisms by varying the production ratio of calcite to organic carbon. For example, a decrease in calcite production by 40% globally drives the pCO2 of the atmosphere near glacial values.

The required shifts in organic carbon and calcite dissolution are qualitatively supported by observations from glacial sediments. An increase in organic carbon production is suggested by an increased benthic-planktonic gradient in d13C18, increased sedimentary organic carbon concentration19 and burial rates20, and a change in foraminiferal assemblages21. In general, calcitic organisms are replaced by siliceous diatoms in regions of high productivity and lower temperatures22. Both conditions are thought to be generally more prevalent under the glacial climate. In high latitudes, the front between silica and calcite production moved equatorward23 during the glacial. Thus we see a general increase in organic production, and a potential shift from calcite toward siliceous production during the last glacial. We conclude that, in contrast to the coral reef hypothesis, the requirements of a "change in production" hypothesis seem to fit more comfortably within the constraints of the available data.

The model predicts that the alkalinity and pH of the whole ocean were higher during glacial time than at present. One test of this hypothesis will be paleo-pH estimates derived from isotopic signature of boron24 in sedimentary calcite (A. Sanyal and G. Hemming, personal communication). Another test of the hypothesis can be made by comparing model time-dependent behavior to atmospheric pCO2 recorded in ice cores. The ~10 kyr time scale of data from Byrd1 is clearly longer than would be expected from a glacial / interglacial change in surface ocean chemistry 25, 26 or ocean circulation17. The model experiment in Figure 4 started at 18 kyr BP with a low value for calcite production relative to organic carbon, and simulated the removal of carbon from the ocean by forest re-growth (as inferred from the d13C values of benthic foraminifera27) by removing 0.055 GT C yr-1 from the atmosphere, from 17.5-7.5 kyr BP, for a total of 550 GT C. The model captures the long term behavior of the observed CO2 record, but misses short-term excursions (e.g. at 12 Kyr BP) that are probably associated with fast changes in ocean circulation, sea surface temperature, or terrestrial biomass, that are not simulated by the model. The model also neglects changes in terrestrial weathering intensity and coral growth that may be significant to the global alkalinity budget. However, we conclude that the similarity between the model pCO2 and data from Byrd supports the possibility that lower glacial pCO2 values were caused by a higher glacial whole ocean alkalinity. While the "coral reef" hypothesis (a higher deep sea calcite burial rate during glacials) appears by itself to be inadequate as an explanation for high glacial alkalinity, we look instead to a change in the relative production rates of calcite and organic carbon.

Acknowledgements. This work supported by the Lamont Doherty Earth Observatory, and benefitted from discussion with Wally Broecker, Steve Emerson, Lloyd Burkle, Robin Keir, Mitch Lyle, Doug MacAyeal, and several other anonymous reviewers.

Citations

1. Neftel, A., Oeschger, H., Staffelbach, T. & Stauffer, B. Nature 331, 609-611 (1988).

2. Broecker, W.S. & Peng, T.H. Global Biogeochemical Cycles 1, 15-29 (1987).

3. Boyle, E.A. Nature 331, 55-56 (1988).

4. Emerson, S.R. & Archer, D.E. Paleoceanography 7, 319-332 (1992).

5. Emerson, S. & Bender, M.L. J. Mar. Res. 39, 139-162 (1981).

6. Archer, D.E. J. Geophys. Res. 96, 17,037-17,050 (1991).

7. Heinze, C., Maier-Reimer, E. & Winn, K. Paleoceanogr. 6, 395-430 (1991).

8. Maier-Reimer, E. Global Biogeochem. Cycles 7, 645-678 (1993).

9. Milliman, J.D. Marine Carbonates 1-375 (Springer-Verlag, Heidelberg, 1974).

10. Davies, T.A. & Worsley, T.R. Soc. Econ. Paleontologists and Mineralogists Spec. Pub. 32, 169-179 (1981).

11. Archer, D., Emerson, S. & Reimers, C. Geochim. Cosmochim. Acta 53, 2831-2846 (1989).

12. Berger, W.H. Naturwissenschaften 69, 87-88 (1982).

13. Opdyke, B.N. & Walker, J.C.G. Geology 20, 733-736 (1992).

14. Berger, W.H. & Keir, R.S. in Climate Processes and Climate Sensitivity (eds. Hansen J.E., a.T.T.) 337-351 (AGU, Washington, D.C., 1984).

15. Peterson, L.C. & Prell, W.L. in The carbon cycle and atmospheric CO2: natural variations archean to present (eds. Sundquist E.T., a.B.W.S.) 251-269 (American Geophysical Union, Washington, D,C,, 1985).

16. Barnola, J.M., Raynaud, D., Korotkevich, Y.S. & Lorius, C. Nature 329, 408-414 (1987).

17. Keir, R.S. Paleoceangr. 5, 253-277 (1990).

18. Sarnthein, M., Winn, K., Duplessy, J.C. & Fontugne, M.R. Paleoceangraphy 3, 361-399 (1988).

19. Lyle, M., Murray, D.W., Finney, B.P., Dymond, J., Robbins, J.M. & Brooksforce, K. Paleoceanography 3, 39-59 (1988).

20. Lyle, M. Nature 335, 529-532 (1988).

21. Mix, A.C. Nature 337(6207), 541-544 (1989).

22. Lisitzin, A.P. in The Micropaleontology of Oceans (eds. Funnell, B.M. & Reidel, W.r.) 173-195 (Cambridge University Press, London, 1971).

23. Howard, W.R. & Prell, W.L. Paleoceanogr. 7, 79-118 (1992).

24. Spivack, A.J., You, C.-F. & Smith, H.J. Nature 363, 149-151 (1993).

25. Broecker, W.S. & Peng, T.-H. Global Biogeochem. Cycles 3, 215-239 (1989).

26. Sarmiento, J.L., Toggweiler, J.R. & Najjar, R. Phil. Trans. R. Soc. Lond. A 325, 3-21 (1988).

27. Leuenberger, M., Siegenthaler, U. & Langway, C.C. Nature 357, 488-490 (1992).

28. Bacastow, R. & Maier-Reimer, E. Clim. Dyn. 4, 95-125 (1990).

29. Martin, J.H., Knauer, G.A., Karl, D.M. & Broenkow, W.M. Deep Sea Res. 34(2), 267-285 (1987).

30. Keir, R.S. Geochim. Cosmochim. Acta 44, 241-252 (1980).

31. Biscaye, P.E., Kolla, V. & Turekian, K.K. J. Geophys. Res. 81, 2595 (1976).

32. Berger, W.H., Adelseck, C.G. & Mayer, L.A. J. Geophys. Res. 81, 2617 (1976).

33. Kolla, V., Bé, A.W.H. & Biscaye, P. J Geophys. Res. 81, 2605-2616 (1976).