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Sustainable carbon emissions: The geologic perspective

Published online by Cambridge University Press:  26 August 2015

Donald J. DePaolo*
Affiliation:
Earth Sciences Division, Lawrence Berkeley National Laboratory, and Department of Earth and Planetary Science, University of California, Berkeley, CA 94720, USA
*
a) Address all correspondence to Donald J. DePaolo at djdepaolo@lbl.gov

Abstract

Current issues with carbon emissions need to be understood in terms of natural geologic processes that move carbon on the Earth. Comparison of modern emissions with the norms and extremes of natural processes emphasizes the enormity of the current challenge, and also the reason there are uncertainties about the future effects. Reaching sustainable emissions in the future can be viewed as a need to systematically reduce the carbon intensity of energy production.

Achieving sustainable carbon emissions requires understanding of Earth's natural carbon cycles. Geologic processes move carbon in large quantities between Earth reservoirs, including in and out of the deeper reaches of the planet, and regulate Earth's surface temperature within a narrow range suitable for life for the past 3–4 billion years. There have been large changes in atmospheric CO2 in the geologic past; the largest to offset changes in the brightness of the Sun. Atmospheric CO2 has been much higher in the past, but not since humans evolved. Geologic processes act slowly, even during times in the geologic past regarded as examples of catastrophic climate change. In contrast, over the past 100 years, Earth's carbon cycles have undergone revolutionary change as a result of a greatly accelerated transfer of carbon from geologic storage to the atmosphere. Today, about 98% of the movement of carbon out of geologic reservoirs (coal-, oil-, and gas-bearing sedimentary rocks and limestone) into the atmosphere is due to human activities; the total carbon flux is 40–50 times the geologic flux. The extremely large modern carbon flux is unprecedented in Earth history. Returning to a sustainable carbon cycle requires systematic lowering of the carbon emission intensity of energy production over the next century.

Information

Type
Review
Copyright
Copyright © Materials Research Society 2015 
Figure 0

Figure 1. Transfer rate of carbon from geologic storage as coal, oil, natural gas, and limestone to the atmosphere in units of GtC/yr. The major increases have occurred since 1850 and most of the increase has occurred since 1950.

Figure 1

Figure 2. Rates of transfer of carbon from geologic storage in rocks to the atmosphere from 1750 to 2014, plotted on a logarithmic scale and compared to natural geologic rates estimated for the modern Earth. Data on combustion and cement are from ORNL database. Geologic rates are from Ref. 11. Total geologic is the rate of carbon emission, mostly as CO2, from volcanic areas plus metamorphism in nonvolcanic mountain ranges. Estimates of total geologic emissions are close to the estimates of carbon removal from the atmosphere-ocean-biosphere system by sedimentation in the oceans56 and hence are likely to be reasonably accurate.

Figure 2

Figure 3. Simplified “box model” representation of where carbon is stored in near-surface reservoirs and the rates at which carbon is exchanged annually between the reservoirs. Fluxes, shown on the arrows, are in units of GtC/yr and are approximate to 10 Gt/yr. The soil carbon mass of 1800 GtC is in the lower range of recent estimates.15 The overall storage in the surface reservoirs is roughly 4000 GtC. The atmospheric mass represents the preindustrial amount; the current value as of 2014 is about 830 GtC. The terrestrial biosphere mass has changed over the past 200 years but not by a large amount (approximately 50 GtC). Solid arrows depict the normal geologic flux of about 0.23 Gt/yr carbon from deep geologic reservoirs to the atmosphere. To a good approximation, the reservoirs within the gray box are the ones that are most affected, over the next few hundred years, by the increased flux of carbon from deep reservoirs caused by fossil fuel burning and cement production.

Figure 3

Figure 4. The radiocarbon content of the atmosphere from 1950 to 2010, expressed in units of permil deviation (∆14C) from the approximately 1950 value of 14C/12C in the atmosphere (Figure from Ref. 45). Between the late 1950s and the mid-1960s, the 14C content of the atmosphere increased by about 60–80% (600–800‰) due to testing of nuclear weapons. The 14C is produced from nuclear blasts in much the same way it is produced naturally, by neutrons released from the explosions reacting with atmospheric nitrogen. The gradual return of the atmospheric ∆14C value to zero is a measure of the rate at which atmospheric C is exchanged with the oceans and biosphere. For a simplified model where this effect is caused by exchange between the atmosphere and surface ocean (1000 GtC) and land biosphere (600 GtC), the annual exchange rates needed to account for the approximately 10–15 year time scale of ∆14C decay are about 50–60 GtC/yr,55 which is evidence for the large magnitude of exchange fluxes shown in Fig. 3. In the last 25 years, the decreasing ∆14C is significantly influenced by fossil fuel carbon emissions, since fossil fuel carbon contains no 14C (∆14C = −1000) and hence tends to accelerate the decrease of ∆14C.

Figure 4

Figure 5. Distribution of carbon in the Earth. A large proportion of Earth's carbon is stored in the core, where it is isolated and not available to significantly affect the surface environment. The Mantle and Continents are large reservoirs of carbon that exchange with the surface slowly over millions and billions of years. The surface reservoirs, shown in blue type, are much smaller but determine the amount of carbon in the atmosphere and hence climate. The deep ocean is an intermediate storage reservoir—it exchanges carbon with the surface reservoirs on a time scale of 1000 years, much shorter than the mantle and continents, but much slower than the exchange among the surface reservoirs. The mass of the remaining fossil fuel stores (5000 GtC) that could still be extracted and burned are not precisely known, but are believed to be roughly equal to the amount of carbon stored currently in the surface reservoirs, and 5–10 times the amount currently in the atmosphere.

Figure 5

Figure 6. Diagram of the geologic carbon cycle that regulates the amount of CO2 in the atmosphere and surface reservoirs over long time scales of millions of years and has kept the Earth “habitable” over most of its 4.5 billion year lifetime. The key feature of the Earth is that carbon (from the Mantle) released to the atmosphere by volcanic emissions can be returned to the deep Earth rather than retained in the atmosphere where it would accumulate to exceedingly high levels over geologic time. The CO2 released from geologic storage by volcanoes tends to acidify rainwater (and the oceans), which slowly dissolves rocks in a process referred to as “weathering.” Weathering generates alkalinity, including aqueous Ca2+ (and Mg2+) ions, that when added to the oceans can combine with dissolved carbonate ions to form solid carbonate (mostly as shelled organisms on the modern Earth), which accumulate on the sea floor and form limestone by compaction and chemical processing over millions of years. Limestone can be added to the continents and stored as sedimentary or metamorphic rock for hundreds of millions of years, or it can be “subducted” back into the deep mantle where it can be retained for one or two billion years. The strength of the feedback between volcanic CO2 emissions, which tend to acidify the oceans and increase atmospheric CO2, and weathering which tends to make the ocean more alkaline and decrease atmospheric CO2, can change slowly over millions of years, resulting in slow swings in global climate between hotter and cooler states (see following figure).

Figure 6

Figure 7. Diagrammatic representation of the CO2-temperature feedback that regulates Earth's surface temperature. Atmospheric CO2 is supplied at a small but significant rate, currently estimated at about 0.23 GtC/yr (probably larger in the geologic past) by volcanic emissions and metamorphism. Weathering has the net effect of removing CO2 from the atmosphere-ocean system and converting it to solid carbonate minerals. Weathering reactions are accelerated by higher temperature and lower pH, so it is inferred that increased atmospheric CO2 and temperature will accelerate weathering. Hence there is feedback, where any increase in volcanic emissions, which will tend to increase atmospheric CO2 and temperature, will be counterbalanced by an increase in weathering, with a lag time of roughly 100,000 years.82 The rate of volcanic emissions can change due to the strength of the “carbon short circuit,” and the rate of weathering can change as a result of continent–continent collisions, which accelerate weathering by creating high mountain ranges where erosion is rapid, making more mineral surface area available for weathering reactions. Over millions to hundreds of millions of years, Earth's climate can drift between warmer and cooler regimes. Ultimately, the strength of the feedback is determined by the absorption of solar energy by the atmosphere, and because the brightness of the Sun has increased gradually over the past 4.5 billion years, there has been a tendency for the CO2 content of the atmosphere to decrease gradually during Earth history (Fig. 9). As the Sun's luminosity increases, less CO2 is required to balance weathering.

Figure 7

Figure 8. (a) Plausible rate of outgassing of deep mantle carbon to the atmosphere over the course of Earth history (from Ref. 89). The inferred modern rate is 0.03 GtC/yr and the rate at 3.0 billion years ago is about 0.06 GtC/yr. Other estimates are as much as twice these numbers (e.g., Ref. 19). At the rates shown, approximately all the original carbon in the mantle would have been released to the atmosphere over the past 4+ billion years. In this case, and even more so if the rates were higher, the fact that the Earth's mantle still contains a lot of carbon would suggest that there is an efficient mechanism to return carbon from the atmosphere back to the mantle. (b) Results of a simple calculation showing the partial pressure of CO2 needed in the atmosphere to maintain the Earth's surface temperature between 0 and 15 °C to compensate for the changing luminosity of the Sun.

Figure 8

Figure 9. (a) Atmospheric CO2 during the climate transition from the last glacial maximum, from 22,000 years ago to 9000 years ago.53 During the period from 17,000 to 11,000 years ago, atmospheric carbon concentration changed by about 70 ppm, corresponding to an atmospheric carbon increase of 150 GtC in 6000 years or about 0.025 GtC/yr. (b) Carbon isotope record and estimated deep ocean temperature during the Paleocene-Eocene Thermal maximum (PETM) about 50 million years ago. These signals correspond to the addition of 3000–7000 GtC in 6000 years, a rate of 0.5–1.2 GtC/yr (figures from Ref. 86).

Figure 9

Figure 10. Representation of atmospheric CO2 history from 5 to 65 million years ago based on oxygen isotopes in marine benthic foraminifera. Oxygen isotope data are from references given in Ref. 86. The formula for CO2 concentration is modified slightly from Ref. 49: (CO2) = 280 × 1.5^(2.6-δ18O). Other estimates of CO2 history are described in Refs. 5, 63, and 66, but show generally similar values. The spike to high CO2 concentrations at 55 million years is associated with the so-called PETM where a large release of carbon to the atmosphere over about 6000 years temporarily increased atmospheric CO2 concentration by as much as 1000 ppm above the ambient (already high) level of about 1000 ppm87 (Fig. 9). The Antarctic ice cap began to form at about 34–38 Ma, after atmospheric CO2 had dropped below 600–700 ppm.21 Current atmospheric CO2, at 400 ppm, is higher than it has been for about the last 10 million years. If continued fossil carbon release drives CO2 much above 1000 ppm, it will then be higher than it has been for roughly 100 million years, with the exception of the geologically brief PETM event.

Figure 10

Figure 11. (a) Three possible emission scenarios for the next 200+ years and the total integrated emissions to which they correspond. Black line is historical emissions to 2014. Redline is the IPCC “worst case” scenario to 2100. Dashed lines are other arbitrary possibilities with lower emissions. (b) Graph depicting where 5000 Gt of fossil CO2 emissions is likely to be stored over the next several thousand years, if only “natural” carbon removal mechanisms are at work (figure adapted from Ref. 15. This model assumes that 5000 GtC is added to the atmosphere at one time at time zero, which would correspond approximately to the year 2100 in the graph in Fig. 11(a) and the scenario where a total of 4700 GtC is emitted. The atmospheric amount shown is the amount in addition to the 600 GtC that was in the preindustrial atmosphere. After 2000 years (which would be the year 2100 + 2000 = 4100), there would still be 1800 + 600 = 2400 GtC in the atmosphere, equivalent to about 1100 ppm. By the year 12,000, the concentration would have decreased only to about 800 ppm and would drift down slowly after that over the subsequent 200–300 thousand years. In the next 50 years, we will choose the emission scenario that will determine the Earth's climate over the next 100,000 years or more.

Figure 11

Figure 12. Carbon cycle approximately 2014. The transfer of rate of 10 GtC/yr from geologic reservoirs now dwarfs the natural rate from volcanoes and metamorphism, and the flux of carbon into sediments as carbonate shells and buried organic material is similarly dwarfed. The only relief from accumulation of the 10 GtC/yr flux in the surface reservoirs is the transfer to the deep ocean, which is significant at about 2 GtC/yr, but much smaller than 10 GtC/yr.

Figure 12

Figure 13. Carbon intensity of global primary energy production (squares and light line) from 1800 to 2010. Prior to the early 1900s, coal and biomass were the main sources of energy, so the carbon intensity of energy production reflects their relatively low efficiency (90–100 MtC/PWh). Subsequent to about 1920, the gradual addition of petroleum, then natural gas, nuclear, hydro, and renewables, caused a systematic decrease in carbon intensity through 2000. Since 2000, the large number of new coal-fired power plants in China and India has reversed the trend.44 The carbon intensity for fossil carbon (circles and bold line) shows a different trend. From 1800 to 1920, the proportion of energy generated from coal rather than biomass increased until about half of energy production was from coal. Fossil carbon intensity continued to increase through 1960 but at a slower rate as a larger proportion of energy was generated from petroleum. Subsequent to 1960, the trend was downward as natural gas, nuclear, and hydropower played a larger role. The ultimate objective for next century is to get the fossil intensity down to below 5 MtC/PWh. This objective will require that carbon intensity decrease by 4–5 MtC/PWh each decade, which means systematically shifting to nuclear and renewables plus possibly CCS-aided coal and natural gas combustion. The recent announcement by China that it will not reach peak carbon emissions until 2030, means that the necessary steep trajectory toward low intensity will have been set back by 30–40 years. The difference between the two arrows shown represents approximately an additional 1200 GtC of total emissions. This graph also shows that while natural gas combustion is preferable to coal and petroleum, its carbon intensity is still far too high to get to the needed levels by next century. The carbon intensity numbers for the various energy sources are adapted from Ref. 58 and other sources.