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Isotope Geochemistry: CO2 Variations and Atmospheric Concentrations Through Geologic Time, Study notes of Geochemistry

The findings from a study using isotope geochemistry to estimate atmospheric co2 concentrations throughout the miocene and late oligocene periods. The study, based on the analysis of planktonic foraminifera shells, revealed surprising results showing that co2 levels were near pre-industrial modern levels during most of this time. The document also explains the relationship between co2, temperature, and photosynthesis, as well as the role of silicate weathering in regulating atmospheric co2 levels.

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Geol. 656 Isotope Geochemistry
Chapter 10
318 8/22/12
solved CO2; Pagani et al. (1999) determined this from the isotopic composition of planktonic fora-
minifera shells in the same layer. Combining paleotemperature estimates based on δ18O discussed in
the previous section with estimated [CO2]aq estimated using equation 10.04, they estimated atmospheric
CO2 through most of the Miocene and late Oligocene (Figure 10.40). The results were surprising be-
cause they showed that CO2 has been near its pre-industrial modern level throughout most of the Mio-
cene. Thus the cooling that occurred in the late Miocene seen in Figure 10.38 was not due to decreasing
atmospheric CO2 as was widely suspected. PCO2 does appear to declined sharply at the Oligocene-
Miocene boundary, coinciding with a known glacial event, but otherwise there is relationship to appar-
ent climate change over this period. As we shall see in the next chapter, boron isotopic measurements
largely confirm these results.
We should also caution that these results do not negate the now well-established control that CO2 ex-
erts on climate. We have seen that atmospheric CO2 correlates strongly with temperature through the
Pleistocene climate extremes. And, as we shall see, atmospheric CO2 was higher in the early Tertiary
and Cretaceous when climate was warm. As of 2011, atmospheric CO2 stood at over 390 ppmv. That
this is higher than it has been at any time over the last 25 million years is very much reason for concern.
The Phanerozoic Carbon Isotope Record and Models of Atmospheric CO2
Figure 10.41 shows the Phanerozoic variation of δ13C in and δ34S in marine carbonates, both of which
presumably record the isotopic composition of seawater at the time of deposition. (This long-term re-
cord misses some short-term events, such as dramatic negative shifts in δ13C associated with the Permo-
Triassic and Cretaceous-Tertiary extinctions that are captured by detailed sampling such as that shown
in Figure 10.39.) The record does reveal a gradual increase in δ13C and decrease in δ34S through much of
the Paleozoic and a more dramatic increase in δ13C (and decrease in δ34S) associated with the expansion
of land plants and high rates of
burial of organic carbonic in
the Carboniferous.
We expect the isotopic com-
positions of carbon and sulfur
to be linked because burial and
erosion of reduced sediment
(organic carbon and sulfide)
affect the concentration of at-
mospheric oxygen. Because of
mass balance, photosynthesis
and subsequent burial of or-
ganic carbon increases δ13C in
the ocean-atmosphere system
and also increases atmospheric
O2 concentration. The latter
enhances sulfide oxidation.
Sulfide (and other forms of re-
duced sulfur) is isotopically
light, so when it is oxidized to
sulfate and added to the ocean,
it lowers seawater δ34S. This
mechanism accounts for the
shift to more positive δ13C and
more negative δ34S in the Car-
boniferous, when the terres-
Figure 10.41. Isotopic compositions of carbon and sulfur in the oceans
through Phanerozoic time. δ34S from Kampschute and Strauss (2004);
δ13C from the compilation of Berner (2006a).
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Chapter 10

solved CO 2 ; Pagani et al. (1999) determined this from the isotopic composition of planktonic fora- minifera shells in the same layer. Combining paleotemperature estimates based on δ^18 O discussed in the previous section with estimated [CO 2 ] (^) aq estimated using equation 10.04, they estimated atmospheric CO 2 through most of the Miocene and late Oligocene (Figure 10.40). The results were surprising be- cause they showed that CO 2 has been near its pre-industrial modern level throughout most of the Mio- cene. Thus the cooling that occurred in the late Miocene seen in Figure 10.38 was not due to decreasing atmospheric CO 2 as was widely suspected. P (^) CO 2 does appear to declined sharply at the Oligocene- Miocene boundary, coinciding with a known glacial event, but otherwise there is relationship to appar- ent climate change over this period. As we shall see in the next chapter, boron isotopic measurements largely confirm these results. We should also caution that these results do not negate the now well-established control that CO 2 ex- erts on climate. We have seen that atmospheric CO 2 correlates strongly with temperature through the Pleistocene climate extremes. And, as we shall see, atmospheric CO 2 was higher in the early Tertiary and Cretaceous when climate was warm. As of 2011, atmospheric CO 2 stood at over 390 ppmv. That this is higher than it has been at any time over the last 25 million years is very much reason for concern.

The Phanerozoic Carbon Isotope Record and Models of Atmospheric CO 2

Figure 10.41 shows the Phanerozoic variation of δ^13 C in and δ^34 S in marine carbonates, both of which presumably record the isotopic composition of seawater at the time of deposition. (This long-term re- cord misses some short-term events, such as dramatic negative shifts in δ^13 C associated with the Permo- Triassic and Cretaceous-Tertiary extinctions that are captured by detailed sampling such as that shown in Figure 10.39.) The record does reveal a gradual increase in δ^13 C and decrease in δ^34 S through much of the Paleozoic and a more dramatic increase in δ^13 C (and decrease in δ^34 S) associated with the expansion of land plants and high rates of burial of organic carbonic in the Carboniferous. We expect the isotopic com- positions of carbon and sulfur to be linked because burial and erosion of reduced sediment (organic carbon and sulfide) affect the concentration of at- mospheric oxygen. Because of mass balance, photosynthesis and subsequent burial of or- ganic carbon increases δ^13 C in the ocean-atmosphere system and also increases atmospheric O 2 concentration. The latter enhances sulfide oxidation. Sulfide (and other forms of re- duced sulfur) is isotopically light, so when it is oxidized to sulfate and added to the ocean, it lowers seawater δ^34 S. This mechanism accounts for the shift to more positive δ^13 C and more negative δ^34 S in the Car- boniferous, when the terres-

Figure 10. 41. Isotopic compositions of carbon and sulfur in the oceans through Phanerozoic time. δ^34 S from Kampschute and Strauss (2004); δ^13 C from the compilation of Berner (2006a).

Chapter 10

trial biota rapidly expanded and organic carbon (later to become coal) accumulated in vast swamps in what would become North America and parts of Europe and Asia. The sedimentary record of δ^34 S and δ^13 C has given rise to various attempts to model the variation of atmospheric CO 2 and O 2 though geologic time. Berner, Lasaga and Garrels (1983, 1985) (often referred to as the BLAG model) pointed out that silicate weathering is another important control on atmospheric CO 2 as it removes CO 2 from the ocean-atmosphere system through weathering reactions such as

CaAl 2 Si 2 O 8 + H 2 CO 3 + H 2 O ↔ Ca2+^ + CO 3 2–^ + Al 2 Si 2 O 5 (OH) 4

and subsequent precipitation of carbonate from seawater:

Ca2+^ CO 3 2–^ ↔ CaCO 3

Berner (1991) developed these ideas further in the GEOCARB model and its subsequent versions (e.g., Berner and Kothavala, 2001; Berner, 2006a; Berner, 2006b). We’ll consider only the gross aspects of this complex model here. The following is based mainly on Berner (2006). Berner considered the fluxes between the ocean-atmosphere, carbonate, and organic carbon reservoirs (Figure 10.42). He as- sumed that the system was in steady-state at any given time, an assumption justified by the small size of the atmosphere-ocean reser- voir compared to the sedimentary ones. Thus one can write the following equation:

F wc + F mc + F wg + F mg = F bc + F bg 10.

where F is a flux, subscript w denotes weath- ering, subscript m magmatic or metamorphic release of carbon, subscript b burial, sub- script c the carbonate reservoir, and subscript g denotes organic sediments. Equation 10. states the steady-state condition that the rate of release of carbon from organic or carbon- ate sediment through metamorphism, mag- matism, and weathering equals the rate bur- ial of organic carbon and carbonate sedi- ment. The isotopic composition of the oceans and atmosphere depends on these fluxes:

δo F bc + (δo – αc )F bg = δo (F wc + F mc ) + δg (F wg + F mg ) 10.

where the subscript o denotes the ocean and α c is the fractionation during photosynthesis. Because the isotopic composition of the oceans (δ^13 C (^) o) through time can be estimated from δ^13 C in carbonate (e.g., Figure 10.41), equation 10.06 provides a constraint on these fluxes. Berner and Kothavala (2006) expressed rate of uptake of CO 2 via the weathering of Ca and Mg sili- cates over time (F (^) wsi) as:

Fwsi = F bc – F wc = f B (T, CO 2 ) fR ( t ) f E ( t ) f AD ( t ) 0.65^ F wsi (0) 10.

where f (^) B is the feedback factor for silicates expressing the dependence of weathering on temperature and on CO 2 , f (^) R is the mountain uplift factor (ratio of land relief at time t to present relief), f (^) E is a factor expressing the dependence of weathering on soil biological activity due to land plants (=1 at present), f (^) AD is the change in the ratio river discharge at time t to present river discharge due to change in pale- ogeography ( a function of change in both land area and river runoff; the power of 0.65 reflects dilution of dissolved load at high runoff), and F (^) wsi(0) is the present weathering uptake of CO 2.

Figure 10.42. Simple model of carbon flow consid- ered by Berner (1991). Masses of carbon are given in units of 10^18 moles. Fluxes are described in the text. After Berner (1991).

Chapter 10

and d( δ c C)/dt = δo F bc – δc (F wm + F mc ) 10.

The results of the latest version of the model (Berner, 2006b), which distinguishes weathering of vol- canic and non-volcanic rocks (the former are richer in Ca and Mg and hence more effective at removing atmospheric CO 2 ) shown in Figure 10.43. The results correspond more or less with what is known from the geologic record about temperature changes during the Phanerozoic. To begin with, the Early Pa- leozoic was warm compared with the late Precambrian, which was a time of several major glaciations. The late Paleozoic, on the other hand, was cool, and the time of the last major glacial epoch before the late Tertiary/Quaternary glaciation. The Cretaceous is well known as a remarkably warm period. Berner’s model shows generally high CO 2 during warm periods of the early Paleozoic, low CO 2 (result- ing from organic carbon burial in the Carboniferous) associated with glaciation in the late Paleozoic,

Figure 10.4 3. Ratio of modeled atmospheric CO 2 concentration to present at- mospheric CO 2. Dashed line is the GEOCARB III model of Berner and Kotha- vala ( 2001 ), circles with solid line is the GEOCARBULF model of Berner (2006b).