+ All Categories
Home > Documents > Modeling the Earth System: Different Approaches for Different Problems James Kasting Department of...

Modeling the Earth System: Different Approaches for Different Problems James Kasting Department of...

Date post: 18-Jan-2016
Category:
Upload: nelson-grant
View: 215 times
Download: 0 times
Share this document with a friend
Popular Tags:
39
Modeling the Earth System: Different Approaches for Different Problems James Kasting Department of Geosciences Penn State University
Transcript
Page 1: Modeling the Earth System: Different Approaches for Different Problems James Kasting Department of Geosciences Penn State University.

Modeling the Earth System:Different Approaches for Different Problems

James KastingDepartment of Geosciences

Penn State University

Page 2: Modeling the Earth System: Different Approaches for Different Problems James Kasting Department of Geosciences Penn State University.

What is the Earth System?

• The Earth contains many different ‘systems’ that we might wish to simulate. These include (but are not limited to):– The climate system– Atmospheric composition– Geochemical cycles– Human populations– Human economic systems

• I’ll talk about modeling the first two of these systems

https://www.youtube.com/watch?v=T6JIE8e2LhQ

Page 3: Modeling the Earth System: Different Approaches for Different Problems James Kasting Department of Geosciences Penn State University.

Talk Outline

• Part 1: Modeling the climate system• Part 2: (Very brief) Modeling atmospheric

composition and photochemistry

Page 4: Modeling the Earth System: Different Approaches for Different Problems James Kasting Department of Geosciences Penn State University.

Hierarchies of Climate Models

• First, one needs to define the problem in which one is interested– Is it global or regional?– What is the time scale of interest? Decades? Centuries?

Millennia? Billions of years?– How firm are the constraints? Are we simulating

observations? Predicting the future? Speculating about other Earth-like planets?

• High levels of modeling complexity are justified only when the constraints are tight and/or the stakes are large (as in modern global warming)

Page 5: Modeling the Earth System: Different Approaches for Different Problems James Kasting Department of Geosciences Penn State University.

Hierarchies of Climate Models

• I’ll talk about three levels of climate models1. 1-D radiative-convective models

• These are what I’ve spent most of my own time studying

2. Energy-balance models (EBMs)• These are useful for a limited class of problems in which

latitudinal resolution is needed, as well as long time scales

3. 3-D global climate models (GCMs)• These are how climate really ought to be modeled, but

they are time-consuming to construct, expensive to run, and they contain many parameters (e.g., continental geography) that need to be known

Page 6: Modeling the Earth System: Different Approaches for Different Problems James Kasting Department of Geosciences Penn State University.

Hierarchies of Climate Models

• I’ll talk about three levels of climate models1. 1-D radiative-convective models

• These are what I’ve spent most of my own time studying

2. Energy-balance models (EBMs)• These are useful for a limited class of problems in which

latitudinal resolution is needed, as well as long time scales

3. 3-D global climate models (GCMs)• These are how climate really ought to be modeled, but

they are time-consuming to construct, expensive to run, and they contain many parameters (e.g., continental geography) that need to be known

Page 7: Modeling the Earth System: Different Approaches for Different Problems James Kasting Department of Geosciences Penn State University.

Hierarchies of Climate Models

• I’ll talk about three levels of climate models1. 1-D radiative-convective models

• These are what I’ve spent most of my own time studying

2. Energy-balance models (EBMs)• These are useful for a limited class of problems in which

latitudinal resolution is needed, as well as long time scales

3. 3-D global climate models (GCMs)• These are how climate really ought to be modeled, but

they are time-consuming to construct, expensive to run, and they contain many parameters (e.g., continental geography) that need to be known

Page 8: Modeling the Earth System: Different Approaches for Different Problems James Kasting Department of Geosciences Penn State University.

1-D Radiative-convective models

• For many problems of interest, it is sufficient to calculate globally averaged vertical temperature profiles

• One needs to include both radiation and convection

Radiation

Convection

Page 9: Modeling the Earth System: Different Approaches for Different Problems James Kasting Department of Geosciences Penn State University.

1-D Radiative-convective models

• One problem that these models can be used for, for example, is to determine what greenhouse gas, or combination of gases, could have compensated for the faint young Sun problem

Page 10: Modeling the Earth System: Different Approaches for Different Problems James Kasting Department of Geosciences Penn State University.

The faint young Sun problem

Kasting et al., Scientific American (1988)

Te = effective radiating temperature = [S(1-A)/4]1/4

TS = average surface temperature

Page 11: Modeling the Earth System: Different Approaches for Different Problems James Kasting Department of Geosciences Penn State University.

• But we know that the early Earth was not frozen. Indeed, if anything the climate was generally warmer than today

Page 12: Modeling the Earth System: Different Approaches for Different Problems James Kasting Department of Geosciences Penn State University.

Geologic time

Rise of atmospheric O2 (Ice age)

First shelly fossils (Cambrian explosion)Snowball Earth ice ages

Warm (The ‘Boring Billion’)

Ice ages

Warm (?) Origin of life

‘Conventional’ interpretationof the Precambrian climaterecord

Page 13: Modeling the Earth System: Different Approaches for Different Problems James Kasting Department of Geosciences Penn State University.

Greenhouse gases and CO2-climate feedbacks

• So, one needs more greenhouse gases, especially during the Archean

• CO2 is a prime candidate because it is part of a negative feedback loop (see panel at right)

• Atmospheric CO2 increases when the climate cools because of slower rates of silicate weathering on land

Diagram illustrating the (modern)carbonate-silicate cycle

Page 14: Modeling the Earth System: Different Approaches for Different Problems James Kasting Department of Geosciences Penn State University.

Is CO2 the solution to the FYS problem?

• 1-D radiative-convective climate model calculations can be used to estimate past CO2 concentrations that would be consistent with the geologic record

• Unfortunately, geochemists have made this problem more difficult by attempting to measure paleo-CO2 concentrations

J. F. Kasting, Science (1993)

Page 15: Modeling the Earth System: Different Approaches for Different Problems James Kasting Department of Geosciences Penn State University.

Precambrian pCO2 from paleosols

• At first, these paleosol studies showed significantly lower Precambrian CO2 levels

• If Sheldon and Driese are right about Precambrian CO2 levels, then other greenhouse gases would have been needed to keep the early Earth from freezing

• But, more recent analyses show less of a discrepancy…

N. Sheldon, Precambrian Res. (2006)

Driese et al.,2011

(10-50 PAL)

Page 16: Modeling the Earth System: Different Approaches for Different Problems James Kasting Department of Geosciences Penn State University.

Precambrian pCO2 from paleosols

• If the new paleosol analysis is correct, then CO2 could have been high enough to solve the faint young Sun problem by itself

• I’ll return to this story at the end because it remains unlikely that CO2 was the only important greenhouse gas during the Archean

• Atmospheric O2 levels were low, and so reduced greenhouse gases (e.g., CH4) should have been more abundant

Kanzaki & Murakami, GCA (2015)

Page 17: Modeling the Earth System: Different Approaches for Different Problems James Kasting Department of Geosciences Penn State University.

1-D models of the habitable zone

• Another problem that can be addressed with 1-D climate models is to try to define the habitable zone around the Sun and other stars

• Definition: The habitable zone (HZ) is the region around a star in which liquid water can exist on a planet’s surface

Figure based on Kasting et al. (Icarus, 1993)

Page 18: Modeling the Earth System: Different Approaches for Different Problems James Kasting Department of Geosciences Penn State University.

Calculating HZ boundaries• The inner edge of the HZ is defined by either a

runaway or moist greenhouse– Runaway greenhouse: The planet’s ocean evaporates

entirely– ‘Moist ‘greenhouse: The ocean remains present, but

water is lost anyway because the stratosphere becomes wet, allowing H2O to be photodissociated, after which the H escapes to space

• The outer edge of the HZ is defined by the ‘maximum greenhouse’ limit, beyond which the surface can no longer be warmed above the freezing point by a CO2-H2O atmosphere

Page 19: Modeling the Earth System: Different Approaches for Different Problems James Kasting Department of Geosciences Penn State University.

Calculating HZ boundaries

• Calculating the boundaries of the habitable zone is difficult because one must be able to deal with dense H2O-rich atmospheres on the inner edge and dense CO2-rich atmospheres on the outer edge

• Both CO2 and H2O have hundreds of thousands of absorption lines across the thermal- and near-infrared

• Including these in a climate model requires that they be parameterized using correlated-k coefficients

Page 20: Modeling the Earth System: Different Approaches for Different Problems James Kasting Department of Geosciences Penn State University.

Habitable zone updates• Within the past two

years, our group has recalculated HZ boundaries using updated 1-D climate models

• The main thing that has changed is the development of a new HITEMP database for H2O absorption coefficients (replacing the older HITRAN database)– The new database gives

more absorption of incoming sunlight at visible/near-IR wavelengths, thereby lowering a planet’s albedo

Goldblatt et al., Nature Geosciences (2013)

Page 21: Modeling the Earth System: Different Approaches for Different Problems James Kasting Department of Geosciences Penn State University.

Revised conventional HZ limits

• The runaway and moist greenhouse limits on the inner edge of the HZ have recently been revised. They now lie perilously close to Earth’s orbit• Note that the horizontal axis has been changed to show effective stellar luminosity, Seff = S/S0

Kasting et al., PNAS, 2014 (Figure by Sonny Harman)

Page 22: Modeling the Earth System: Different Approaches for Different Problems James Kasting Department of Geosciences Penn State University.

• But these 1-D climate model calculations may be too pessimistic, for at least two reasons1. They typically assume that the

troposphere is fully saturated2. Cloud feedback is typically ignored

(Neither of these processes can be modeled effectively in 1-D)

Page 23: Modeling the Earth System: Different Approaches for Different Problems James Kasting Department of Geosciences Penn State University.

3-D modeling of habitable zone boundaries

• Fortunately, new studies using 3-D climate models predict that the runaway greenhouse threshold is increased by ~10% because the tropical Hadley cells act like radiator fins– This behavior was pointed

out 20 years ago by Ray Pierrehumbert (JAS, 1995) in a paper dealing with Earth’s tropics

• We have adjusted our (1-D) HZ inner edge inward to account for this behavior

Leconte et al., Nature (2013)

Outgoing IR radiation

Page 24: Modeling the Earth System: Different Approaches for Different Problems James Kasting Department of Geosciences Penn State University.

Updated habitable zone(Kopparapu et al., 2013, 2014)

• When the 3-D climate calculations are taken into account, the inner edge of the HZ moves back to ~0.95 AU around the Sun

Credit: Sonny Harman

Page 25: Modeling the Earth System: Different Approaches for Different Problems James Kasting Department of Geosciences Penn State University.

Tidal locking for planets around M stars

• 3-D models are also needed to simulate tidally locked planets orbiting M stars

• Such planets are likely to be syncronously rotating, i.e., they always show the same face to the star– The 1-D

approximation is not very good in this case

Figure based on Kasting et al. (1993)

Page 26: Modeling the Earth System: Different Approaches for Different Problems James Kasting Department of Geosciences Penn State University.

3-D climate model calculations for M- and K-

star planets• Clouds dominate the

sunny side of tidally locked planets orbiting M and late-K stars, raising their albedos

• The inner edge of the HZ is therefore pushed way in– Seff 2 for a

synchronously rotating planet around a K star (dark blue curves)

Yang et al., ApJ Lett (2013)

Page 27: Modeling the Earth System: Different Approaches for Different Problems James Kasting Department of Geosciences Penn State University.

Most recent habitable zone

• Thus, our current estimate of the habitable zone looks something like this. The inner edge is still highly uncertain

Kopparapu et al., ApJ Lett (2014)

Page 28: Modeling the Earth System: Different Approaches for Different Problems James Kasting Department of Geosciences Penn State University.

• Recent work shows that the outer edge of the HZ may be similarly complex, requiring the use of climate models of at least EBM complexity…

Page 29: Modeling the Earth System: Different Approaches for Different Problems James Kasting Department of Geosciences Penn State University.

• A new paper by Kristen Menou shows that planets near the outer edge of the habitable zone should not have stable, warm climates, despite the influence of the carbonate-silicate cycle

• See also Kadoya and Tajika (ApJ, 2014), along with earlier papers by Tajika, referenced therein

• Energy balance models (EBMs) are needed to simulate this behavior because it involves polar glaciation

Page 30: Modeling the Earth System: Different Approaches for Different Problems James Kasting Department of Geosciences Penn State University.

Limit cycling near the HZ outer edge

• Our own EBM predicts limit cycles near the outer edge of the HZ

• A planet in this region remains frozen much of the time, but warms occasionally near the equator

• Calculation of the ice line is needed to study this phenomenon

Haqq-Misra et al., PNAS, submitted

Page 31: Modeling the Earth System: Different Approaches for Different Problems James Kasting Department of Geosciences Penn State University.

Limit cycling near the HZ outer edge

• This phenomenon may have implications for the existence of complex (animal) life, including intelligent life• It is hard to see how such life could evolve in a limit-cycling environment

Page 32: Modeling the Earth System: Different Approaches for Different Problems James Kasting Department of Geosciences Penn State University.

• Part 2: (Very brief) Modeling atmospheric composition and photochemistry

Finally, on long time scales, the composition of the atmosphere may change in ways that affect the Earth’s climate. This requires the use of a photochemical model..

Page 33: Modeling the Earth System: Different Approaches for Different Problems James Kasting Department of Geosciences Penn State University.

1-D photochemical models• Divide the atmosphere into

vertical layers (typically 1001 km)

• Calculate absorption and scattering of incident solar UV radiation

• Calculate photochemical reaction rates and (vertical) transport for the relevant atmospheric species (typically 50-60)

• Integrate the model in time until it converges using an implicit an implicit numerical method, such as the reverse Euler method

Segura et al., Astrobiology (2003)

Page 34: Modeling the Earth System: Different Approaches for Different Problems James Kasting Department of Geosciences Penn State University.

1-D photochemical models

• For example, one can calculate the vertical profiles of CH4 and N2O for different atmospheric O2 levels• A constant upward flux of each gas is assumed

Segura et al., Astrobiology (2003)

Page 35: Modeling the Earth System: Different Approaches for Different Problems James Kasting Department of Geosciences Penn State University.

1-D photochemical models

Segura et al., Astrobiology (2003)

• One can also calculate vertical ozone profiles• Then, by feeding this output back into the 1-D climate model, and iterating back and forth, one can calculate the effect on vertical temperature profiles

Page 36: Modeling the Earth System: Different Approaches for Different Problems James Kasting Department of Geosciences Penn State University.

The faint young Sun problem revisited

• Finally, to return briefly to the faint young Sun problem, mentioned earlier, it is easy to demonstrate that atmospheric CH4 concentrations could have been up to 1000 times higher than today (~1000 ppmv, compared to 1.7 ppmv today) prior to the rise of atmospheric O2

• This could have provided an additional 10-12 degrees of greenhouse warming

A. A. Pavlov et al., JGR (2001)Volume mixing ratio

Page 37: Modeling the Earth System: Different Approaches for Different Problems James Kasting Department of Geosciences Penn State University.

Archean CH4-CO2 greenhouse

• Diagram shows a hypothetical Archean atmosphere at 2.8 Ga

• The black curves show predicted surface temperatures with zero and 1000 ppm of CH4

• The loss of much of this CH4 at ~2.5 Ga could plausibly have triggered the Paleoproterozoic glaciations

2.8 GaS/So = 0.8

J.F. Kasting, Science (2013)

Driese et al. (2011)

Page 38: Modeling the Earth System: Different Approaches for Different Problems James Kasting Department of Geosciences Penn State University.

Geologic time

Rise of atmospheric O2 (Ice age)

First shelly fossils (Cambrian explosion)Snowball Earth ice ages

Warm (The ‘Boring Billion’)

Ice ages

Warm (?) Origin of life

‘Conventional’ interpretationof the Precambrian climaterecord

Page 39: Modeling the Earth System: Different Approaches for Different Problems James Kasting Department of Geosciences Penn State University.

Conclusions• Different types of climate models are useful for different problems

– 1-D models are useful for studying weakly constrained problems like the faint young Sun problem and the boundaries of the circumstellar habitable zone

– 3-D models are useful for refining such calculations and for investigating problems like modern day global warming, for which both tight constraints and lots of funding are available

– EBMs are useful for long-timescale problems for which latitudinal information, e.g. ice lines, are essential

• 1-D photochemical models, sometimes coupled to 1-D climate models, are useful for studying problems (like the faint young Sun problem) in which changes in atmospheric composition are important


Recommended