the faint young sun problem

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The Faint Young Sun Problem

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The Faint Young Sun Problem. Systems Notation. = system component. = positive coupling. = negative coupling. Positive Feedback Loops (Destabilizing). Water vapor feedback. Surface temperature. Atmospheric H 2 O. (+). Greenhouse effect. Positive Feedback Loops (Destabilizing). - PowerPoint PPT Presentation

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Page 1: The Faint Young Sun Problem

The Faint Young Sun Problem

Page 2: The Faint Young Sun Problem

Systems Notation

= system component

= positive coupling

= negative coupling

Page 3: The Faint Young Sun Problem

Positive Feedback Loops(Destabilizing)

Surfacetemperature

AtmosphericH2O

Greenhouseeffect

Water vapor feedback

(+)

Page 4: The Faint Young Sun Problem

Positive Feedback Loops(Destabilizing)

Surfacetemperature

Snow and icecover

Planetaryalbedo

Snow/ice albedo feedback

(+)

Page 5: The Faint Young Sun Problem

Negative Feedback Loops(Stabilizing)

Surfacetemperature

IR flux feedback

(-) OutgoingIR flux

Page 6: The Faint Young Sun Problem

Runaway Greenhouse: FIR and FS

J. F. Kasting, Icarus (1988)

Page 7: The Faint Young Sun Problem

The Carbonate-Silicate Cycle

Page 8: The Faint Young Sun Problem

Negative Feedback Loops(Stabilizing)

The carbonate-silicate cycle feedback

(-)

Surfacetemperature

Rainfall

Silicateweathering

rate

AtmosphericCO2

Greenhouseeffect

Page 9: The Faint Young Sun Problem

Model pCO2 vs. Time

J. F. Kasting, Science (1993)

Page 10: The Faint Young Sun Problem

pCO2 from Paleosols (2.8 Ga)

Rye et al., Nature (1995)

Page 11: The Faint Young Sun Problem

Geological O2 Indicators

H. D. Holland, 1994

Page 12: The Faint Young Sun Problem

The Universal Tree of Life

Page 13: The Faint Young Sun Problem
Page 14: The Faint Young Sun Problem

Kasting and Brown (1998)

Page 15: The Faint Young Sun Problem

Pavlov et al., JGR (2000)

Page 16: The Faint Young Sun Problem

CH4-Climate Feedback Loop

Surfacetemperature

CH4

productionrate

Greenhouseeffect

(+)

Page 17: The Faint Young Sun Problem

CH4-Climate Feedback Loop

• Doubling times for thermophilic methan-ogens are shorter than for mesophiles

• Thermophiles will therefore tend to outcompete mesophiles, producing more CH4, and further warming the climate But

• If CH4 becomes more abundant than CO2, organic haze begins to form...

Page 18: The Faint Young Sun Problem

Titan’s Organic Haze Layer

Page 19: The Faint Young Sun Problem

The Anti-greenhouse Effect

Page 20: The Faint Young Sun Problem

Archean Climate Control Loop

Surfacetemperature

CH4

production

Hazeproduction

AtmosphericCH4/CO2

ratio

CO2 loss(weathering)

(–)

(–)

Page 21: The Faint Young Sun Problem

Huronian Supergroup (2.2-2.45 Ga)

Redbeds

Detrital uraniniteand pyrite

Glaciations

Page 22: The Faint Young Sun Problem

Snowball Earth Glaciations

• Paleomagnetic data indicate low-latitude glaciation at 2.3 Ga, 0.75 Ga, and 0.6 Ga

• Huronian glaciation (2.3 Ga) may be triggered by the rise of O2 and the corresponding loss of CH4

• Late Precambrian glaciations studied by Hoffman et al., Science 281, 1342 (1998)

Page 23: The Faint Young Sun Problem

Model pCO2 vs. Time

J. F. Kasting, Science (1993)

Page 24: The Faint Young Sun Problem

Late Precambrian Geography

Hyde et al., Nature, 2000* glacial deposits

Page 25: The Faint Young Sun Problem

Triggering a Snowball Earth episode

• Hoffman et al.: Continental rifting created new shelf area, thereby promoting burial of organic carbon

• Marshall et al. (JGR, 1988): Clustering of continents at low latitudes allows silicate weathering to proceed even as the global climate gets cold

Page 26: The Faint Young Sun Problem

Caldeira and Kasting, Nature, 1992

Page 27: The Faint Young Sun Problem

Recovering from a Snowball Earth episode

• Volcanic CO2 builds up to ~0.1 bar

• Ice melts catastrophically (within a few thousand years)

• Surface temperatures climb briefly to 50-60oC

• CO2 is rapidly removed by silicate weathering, forming cap carbonates

Page 28: The Faint Young Sun Problem

Hoffman et al.,Science, 1998

‘Cap’ carbonate(400 m thickness)

Page 29: The Faint Young Sun Problem

How did the biota survive the Snowball Earth?

• Refugia such as Iceland?

• Hyde et al. (Nature, 2000): Tropical oceans were ice free

• C. McKay (GRL, 2000): Tropical sea ice may have been thin

Page 30: The Faint Young Sun Problem

Snowball EarthIce Thickness

Fg

Ts

Toc 0oC

Let k = thermal conductivity of ice z = ice thickness T = Toc – Ts

Fg = geothermal heat flux

z

Page 31: The Faint Young Sun Problem

Ice Thickness (cont.)

The diffusive heat flux is: Fg = kT / z Solving for z gives:

z = kT / Fg

2.5 W/m/K(27 K)/ 6010-3 W/m2

= 1100 m

Page 32: The Faint Young Sun Problem

Heat Flow Through Semi-transparent, Ablating Ice

Ref: C. P. McKay, GRL 27, 2153 (2000)

k dT/dz = S(z) + L + Fg

where k = thermal conductivity of ice S(z) = solar flux at depth z in the ice L= latent heat flux (balancing ablation) Fg = geothermal heat flux

Page 33: The Faint Young Sun Problem

Comparative Heat Fluxes

Geothermal heat flux: Fg = 6010-3 W/m2

Solar heat flux (surface average):Fs = 1370 W/m2(1 – 0.3)/4 240 W/m2

Equatorial heat flux:Feq 1.2 Fs 300 W/m2

Ratio of equatorial heat flux (from Sun) vs. geothermal heat flux: Feq/Fg 300/0.006 = 5000

Page 34: The Faint Young Sun Problem

Ice Transmissivity

C. McKay, GRL (2000)

Page 35: The Faint Young Sun Problem

Heat Fluxes (cont.)

Now, lettR = ice transmissivity

Then, scaling ice thickness inversely withtransmitted heat flux yields:

tR z10-3 ~200 m10-2 ~20 m10-1 ~2 m

Page 36: The Faint Young Sun Problem

CONCLUSIONS

• Earth’s climate is stabilized on long time-scales by the carbonate-silicate cycle

• Higher atmospheric CO2 levels are a good way of compensating for the faint young Sun

• CH4 probably made a significant contribution to the greenhouse effect during the Archean when O2 levels were low

Page 37: The Faint Young Sun Problem

CONCLUSIONS (cont.)

• Earth’s climate is theoretically susceptible to episodes of global glaciation. It can recover from these by buildup of volcanic CO2

• The first such “Snowball Earth” episode at ~2.4 Ga may have been triggered by the rise of O2 and loss of the methane component of the atmospheric greenhouse

Page 38: The Faint Young Sun Problem

CONCLUSIONS (cont.)

• The true “Snowball Earth” model (complete glacial ice cover) best explains the geological evidence, particularly the presence of cap carbonates