Alfred Wegener Institute
for Polar and Marine Research Bremerhaven, Germany
The Carbon Cycle during the Pleistocene
Peter K¨ohler
Institute for Applied Geosciences, Darmstadt University of Technology
—
13 November 2007
In cooperation with:
Hubertus Fischer, Alfred Wegener Institute, Bremerhaven, Germany Richard E. Zeebe, University of Hawaii, USA
Guy Munhoven, Universit´e de L`ıege, Belgium
Outline
The global record of atmospheric CO
2EPICA — European Project for Ice Coring in Antarctica The global carbon cycle and the box model BICYCLE
Time-dependent processes: motivations and simulation results Combined scenarios
Open questions
Conclusions
200 250 300 350
CO
2[ppmv]
700 400 100 Time [kyr BP]
13C CO2
10 7 4 1 Time [kyr BP]
1000 1500 2000 Time [yr AD]
2000 198019902000 Time [yr AD]
-8.5 -8.0 -7.5 -7.0 -6.5 -6.0
13
C [
o/
oo]
200 250 300 350
CO
2[ppmv]
700 400 100 Time [kyr BP]
13C CO2
10 7 4 1 Time [kyr BP]
1000 1500 2000 Time [yr AD]
2000 198019902000 Time [yr AD]
-8.5 -8.0 -7.5 -7.0 -6.5 -6.0
13
C [
o/
oo]
20 y:
seasonal
Point Barrow
Keeling and Whorf, 2005; Keeling et al., 2005.
200 250 300 350
CO
2[ppmv]
700 400 100 Time [kyr BP]
13C CO2
10 7 4 1 Time [kyr BP]
1750 AD
1000 1500 2000 Time [yr AD]
2000 198019902000 Time [yr AD]
-8.5 -8.0 -7.5 -7.0 -6.5 -6.0
13
C [
o/
oo]
20 y:
seasonal
1 kyr:
anthrop.
Point Barrow Law Dome
Francey et al., 1998; Trudinger et al., 1999
200 250 300 350
CO
2[ppmv]
700 400 100 Time [kyr BP]
13C CO2
10 7 4 1 Time [kyr BP]
1750 AD
1000 1500 2000 Time [yr AD]
2000 198019902000 Time [yr AD]
-8.5 -8.0 -7.5 -7.0 -6.5 -6.0
13
C [
o/
oo]
20 y:
seasonal
1 kyr:
anthrop.
10 kyr:
Holocene
Point Barrow Law Dome
Taylor D.
Smith et al., 1999
200 250 300 350
CO
2[ppmv]
700 400 100 Time [kyr BP]
13C CO2
10 7 4 1 Time [kyr BP]
1750 AD
1000 1500 2000 Time [yr AD]
2000 198019902000 Time [yr AD]
-8.5 -8.0 -7.5 -7.0 -6.5 -6.0
13
C [
o/
oo]
20 y:
seasonal
1 kyr:
anthrop.
10 kyr:
Holocene 700 kyr:
glacial/
interglacial
Point Barrow Law Dome
Taylor D.
Vostok
EPICA DC
Petit et al., 1999; Siegenthaler et al., 2005
Radiative Forcing of Greenhouse Gases — Today
Gas Current Increase Radiative forcing (W m−2)
Amount < 1750 1750-2007
H2O 94 -
CO2 383 ppm 105 ppm (38%) 50 1.71
CH4 1745 ppb 1045 ppb(150%) 1.1 0.48 N2O 314 ppb 44 ppb (16%) 1.25 0.16
CFCs 268 ppt 0.31
Preindustrial Greenhouse Forcing 146
Anthropogenic Greenhouse Forcing 2.66 Total Greenhouse Forcing 148.66
Global surface temperature (energy balance without GHG): –18◦C Global surface temperature (measured in 20th century): +16◦C Total Greenhouse Forcing (148.66 W/m2) explains ∆T of 34 K.
⇒ Anthropogenic Forcing (2.66 W/m2) explains ∆T of 0.6 K.
(which is in agreement with observations during the last 150 years)
Radiative Forcing of Greenhouse Gases — LGM
Agent Radiative forcing
(W m−2) Preindustrial Greenhouse Gases +146 Anthropogenic Greenhouse Gases +2.66
LGM
GHG (CO2 +CH4 +N2O) –2.8
Dust –1.4
Ice sheets (Albedo) –3.0
Vegetation (Albedo) –1.2
LGM sum –8.4
⇒ Anthropogenic GHG forcing is of the same order but opposite sign than GHG foring during LGM.
The global record of atmospheric CO
2EPICA — European Project for Ice Coring in Antarctica
The global carbon cycle and the box model BICYCLE
Time-dependent processes: motivations and simulation results Combined scenarios
Open questions
Conclusions
EPICA drilling sites:
Dome C (EDC): low accumulation rate; long time series (∼8 glacial cycles) Dronning Maud Land (EDML): high accumulation rate, high resolution
Kohnen station in Dronning Maud Land
Drilling team 2005/06 with last section of EDML (from 2774 m depth)
Scientific lab in Kohnen station
200 250 300 350
CO
2[ppmv]
700 400 100 Time [kyr BP]
13C CO2
10 7 4 1 Time [kyr BP]
1750 AD
1000 1500 2000 Time [yr AD]
2000 198019902000 Time [yr AD]
-8.5 -8.0 -7.5 -7.0 -6.5 -6.0
13
C [
o/
oo]
20 y:
seasonal
1 kyr:
anthrop.
10 kyr:
Holocene 700 kyr:
glacial/
interglacial
Point Barrow Law Dome
Taylor D.
Vostok
EPICA DC
The EPICA challenge
Predicting pCO2 prior to Vostok (Wolff et al., 2004, 2005, EOS) 8 contributions: from regression analysis to full carbon cycle model
-450 -420 -390 -360
D(o /oo)
EDC D
1 5
7 9
11 13
15 17
MIS
0 500 1000
dust(ppbv) 1500
EDC dust
700 600 500 400 300 200 100 0
Time (kyr BP)
160 200 240 280
pCO2(ppmv)
Vostok pCO
2I II
III
?
IVEPICA, 2004; Petit et al., 1999
The EPICA challenge
Predicting pCO2 prior to Vostok (Wolff et al., 2004, 2005, EOS) 8 contributions: from regression analysis to full carbon cycle model
-450 -420 -390 -360
D(o /oo)
EDC D
1 5
7 9
11 13
15 17
MIS
0 500 1000
dust(ppbv) 1500
EDC dust
700 600 500 400 300 200 100 0
Time (kyr BP)
160 200 240 280
pCO2(ppmv)
Vostok pCO
2EDC pCO
2I II
III IV
V VI
VII
EPICA, 2004; Petit et al., 1999 Siegenthaler et al., 2005
The EPICA challenge
Our contribution to the EPICA challenge:
Carbon cycle model simulations based on results for Termination I
-450 -420 -390 -360
D(o /oo)
EDC D
Termination I
1 5
7 9
11 13
15 17
MIS
0 500 1000
dust(ppbv) 1500
EDC dust
700 600 500 400 300 200 100 0
Time (kyr BP)
160 200 240 280
pCO2(ppmv)
Vostok pCO
2EDC pCO
2I II
III IV
V VI
VII
EPICA, 2004; Petit et al., 1999 Siegenthaler et al., 2005
Atmospheric carbon during Termination I
Interprete the temporal evolution of atmospheric CO2, δ13C, 14C records
by carbon cycle simulations.
Smith et al., 1999; Monnin et al., 2001;
Stuiver et al., 1998; Hughen et al., 2004
-7.0 -6.8 -6.6 -6.4 -6.2
13 C[o / oo]
Interval I II III IV H1 BA YD 13
C
180 200 220 240 260 280
pCO2[ppmv]
pCO
220 18 16 14 12 10 GISP2 Age [kyr BP]
0 100
200 300 400 500
14 C[o /oo]
14
C
The global record of atmospheric CO
2EPICA — European Project for Ice Coring in Antarctica The global carbon cycle and the box model BICYCLE
Time-dependent processes: motivations and simulation results Combined scenarios
Open questions
Conclusions
THC
THC
The global
carbon cycle
60 PgC/yr 60 PgC/yr
1 PgC/yr 10 PgC/yr
ATMOSPHERE (600 PgC)
ROCK
TERR. BIOSPHERE (2200 PgC)
0.8 PgC/yr
0.2 PgC/yr
0.2 PgC/yr
DEEP OCEAN (38000 PgC)
SEDIMENT
soft tissues | hard shells marine biosphere SURFACE OCEAN (700 PgC)
preindustrial reservoir sizes and annual fluxes
Carbonate System in the Ocean
Dissolved Inorganic Carbon (DIC) = CO2 + HCO−3 + CO=3
Atmosphere
CO2 + H20 ⇀↽K1 HCO−3 + H+ ⇀↽K2 CO=3 + 2H+
1% 89% 10%
m
K0CO2(g)
m
CO2(g)
Ocean
K0, K1, K2 = f(temperature,salinity,depth)
after Zeebe and Wolf-Gladrow, 2001
000000 000000 000000 000000 000000 000000 000000 000000 000000
111111 111111 111111 111111 111111 111111 111111 111111 111111
00000 00000 00000 00000 00000 00000 00000 00000 00000
11111 11111 11111 11111 11111 11111 11111 11111 11111 0000
0000 1111 1111
00000000 00000000 00000000 11111111 11111111 11111111
Box model of the Isotopic Carbon cYCLE BICYCLE
Rock
C3
FS SS
NW W D
C4
Atmosphere
Atlantic Indo−Pacific
Sediment SO
Biosphere
mediate inter−
surface
deep
water carbon
K¨ohler, et al., 2005, Global Biogeochemical Cycles.
000000 000000 000000 000000 000000 000000 000000 000000 000000
111111 111111 111111 111111 111111 111111 111111 111111 111111
00000 00000 00000 00000 00000 00000 00000 00000 00000
11111 11111 11111 11111 11111 11111 11111 11111 11111 0000
0000 1111 1111
00000000 00000000 00000000 11111111 11111111 11111111
Box model of the Isotopic Carbon cYCLE BICYCLE
Rock
C3
FS SS
NW W D
C4
Atmosphere
Atlantic Indo−Pacific
Sediment SO
Biosphere
water carbon
Prognostic variables:
10 oceanic boxes: DIC,
7 terrestrial boxes: C, 13C, 14C 1 atmospheric box:
14C, ALK, PO4, O2 13C,
CO2, 13C, 14C
K¨ohler, et al., 2005, Global Biogeochemical Cycles.
000000 000000 000000 000000 000000 000000 000000 000000 000000
111111 111111 111111 111111 111111 111111 111111 111111 111111
00000 00000 00000 00000 00000 00000 00000 00000 00000
11111 11111 11111 11111 11111 11111 11111 11111 11111 0000
0000 1111 1111
00000000 00000000 00000000 11111111 11111111 11111111
Box model of the Isotopic Carbon cYCLE BICYCLE
Rock
C3
FS SS
NW W D
C4
Atmosphere
Atlantic Indo−Pacific
Sediment SO
Biosphere
water carbon
Prognostic variables:
10 oceanic boxes: DIC,
7 terrestrial boxes: C, 13C, 14C 1 atmospheric box:
14C, ALK, PO4, O2 13C,
CO2,
DIC + ALK −> CO2, HCO3, CO3, 13C, 14C
pH
K¨ohler, et al., 2005, Global Biogeochemical Cycles.
The global record of atmospheric CO
2EPICA — European Project for Ice Coring in Antarctica The global carbon cycle and the box model BICYCLE
Time-dependent processes: motivations and simulation results
Combined scenarios Open questions
Conclusions
Overall objective and procedure for time-dependent simulations
Novelty:
• BICYCLE runs forward in time (no inverse studies)
• Transient simulations based on and forced with available paleo records
Three steps:
1. Which time-dependent processes were changing the carbon cycle on glacial/interglacial timescales?
2. How can we prescribe / force these processes in BICYCLE?
3. What are the impacts on CO2?
Time-dependent processes:
Which How What ?
Physics (without ocean circulation) 1 Temperature
2 Sea level / salinity
3 Gas exchange / sea ice Ocean circulation
4 NADW formation
5 Southern Ocean ventilation Biogeochemistry
6 Marine biota / iron fertilisation 7 Terrestrial carbon storage
8 CaCO3 chemistry
1 Temperature
Simulation with the climate model CCSM3 LGM–Preindustrial: light blue: –(2-4)K
Otto-Bliesner et al., 2006
Time-dependent processes:
Which How (T I) What (ppmv) ?
Physics (without ocean circulation)
1 Temperature +(3–5) K +30 !
2 Sea level / salinity
3 Gas exchange / sea ice Ocean circulation
4 NADW formation
5 Southern Ocean ventilation Biogeochemistry
6 Marine biota / iron fertilisation 7 Terrestrial carbon storage
8 CaCO3 chemistry
2 Sea Level / Salinity
Sea level rose during Termination I by 125 m; salinity dropped by 3%
50 100 150 200 250 300 350
Longitude [o]
-90 -60 -30 0 30 60 90
Latitude[o ]
Area flooded from LGM to present
Bathymetry from Scripps Institiute of Oceanography from ICE-5G, Peltier, 2004
Time-dependent processes:
Which How (T I) What (ppmv) ?
Physics (without ocean circulation)
1 Temperature +(3–5) K +30 !
2 Sea level / salinity +125 m –15 !
3 Gas exchange / sea ice Ocean circulation
4 NADW formation
5 Southern Ocean ventilation Biogeochemistry
6 Marine biota / iron fertilisation 7 Terrestrial carbon storage
8 CaCO3 chemistry
3 Gas Exchange / Sea Ice
Annual mean sea ice area shrunk by ∼50% (Termination I)
Dynamics coupled to temperature in the high latitude surface boxes
Arctic (present): The Cryosphere Today (www) Antarctic (LGM) Gersonde et al., 2005
3 Gas Exchange / Sea Ice
Model comparions came to ambiguous results
Box models: full sea ice cover in SO reduces CO2 General Circulation Models: only small changes
Archer et al., 2003 BICYCLE
3 Gas Exchange / Sea Ice
BICYCLE: Sea ice change in N and S N is sink for CO2; S is source for CO2
S as in box models, but N dominates over S
700 600 500 400 300 200 100 0 Time (kyr BP)
250 260 270 280
CO 2(ppmv)
S only (90% coverage) S only (60% coverage) S only (30% coverage) N and S
Archer et al., 2003 BICYCLE
Time-dependent processes:
Which How (T I) What (ppmv) ?
Physics (without ocean circulation)
1 Temperature +(3–5) K +30 !
2 Sea level / salinity +125 m –15 !
3 Gas exchange / sea ice –50% –15 ?
Ocean circulation 4 NADW formation
5 Southern Ocean ventilation Biogeochemistry
6 Marine biota / iron fertilisation 7 Terrestrial carbon storage
8 CaCO3 chemistry
4 North Atlantic Deep Water (NADW) Formation
Conveyor belt Changes in Atlantic THC
Rahmstorf, 2002
4 North Atlantic Deep Water (NADW) Formation
Preindustrial circulation: World Ocean Circulation Experiment (WOCE) data Temporal changes: NADW reduce from 16 Sv to 10 Sv (0 Sv)
Box model of the Isotopic Carbon cYCLE
BICYCLE
100 m
1000 m
DEEP SURFACE
MEDIATEINTER−
Rock
carbon
water
C3
FS SS
NW W D
C4
Atmosphere
Atlantic Indo−Pacific
Sediment
40°N
50°N 40°S 40°S
SO
Biosphere
16
22 5
10 1
4 16
9 6
3 30
9 16
20 1
18 19
15
6
9 9
16
12 5 2 1
3
Circulation after Ganachaud & Wunsch, 2000
Time-dependent processes:
Which How (T I) What (ppmv) ?
Physics (without ocean circulation)
1 Temperature +(3–5) K +30 !
2 Sea level / salinity +125 m –15 !
3 Gas exchange / sea ice –50% –15 ?
Ocean circulation
4 NADW formation +6 Sv +15 !
5 Southern Ocean ventilation Biogeochemistry
6 Marine biota / iron fertilisation 7 Terrestrial carbon storage
8 CaCO3 chemistry
4 Indirect effects of shutdown of NADW (not in BICYCLE)
Additionally, a NADW shutdown would lead to cooling in Eurasia Temperature anomalies simulated with climate model ECBILT-CLIO
K¨ohler et al., 2005, Climate Dynamics (after Knutti et al., 2004)
4 Indirect effects of shutdown of NADW (not in BICYCLE)
Reduction of marine export production (blue) in North Atlantic by 50%
Schmittner, 2005
4 Indirect effects of shutdown of NADW (not in BICYCLE)
Cooling leads to southwards shift of treeline (LPJ-DGVM) Competing effect of soil respiration and vegetation growth
275 280 285 290 295 300
CO 2 (ppmv)
CO2 fert. feedbacks off CO2 fert feedbacks on
230 235 240 245 250
CO 2 (ppmv)
195 200 205 210 215
CO 2 (ppmv)
0 1000 2000 3000 Simulation time (yr) 175
180 185 190 195 200
CO 2 (ppmv)
1 kyr BP
13 kyr BP
21 kyr BP 17 kyr BP
K¨ohler et al., 2005, Climate Dynamics
Time-dependent processes:
Which How (T I) What (ppmv) ?
Physics (without ocean circulation)
1 Temperature +(3–5) K +30 !
2 Sea level / salinity +125 m –15 !
3 Gas exchange / sea ice –50% –15 ?
Ocean circulation
4 NADW formation +6 Sv +15 !/? (off)
5 Southern Ocean ventilation Biogeochemistry
6 Marine biota / iron fertilisation 7 Terrestrial carbon storage
8 CaCO3 chemistry
5 Southern Ocean Ventilation
How to explain ∆δ13C(PRE-LGM)=+1.2/◦◦◦ in deep Southern Ocean?
SO mixing reduced by 2/3 coupled to SO SST = f(EDC δD)
Different hypotheses on the physical cause behind it (work in progress)
20 18 16 14 12 10 Time [kyr BP]
-0.6 -0.4 -0.2 0.0 0.2 0.4 0.6 0.8
13
C in deep SO [
o/
oo]
SO stratification breakdown
at 17 kyr BP no SO stratification breakdown
Hodell et al, 2003 K¨ohler, et al., 2005, Global Biogeochemical Cycles
Time-dependent processes:
Which How (T I) What (ppmv) ?
Physics (without ocean circulation)
1 Temperature +(3–5) K +30 !
2 Sea level / salinity +125 m –15 !
3 Gas exchange / sea ice –50% –15 ?
Ocean circulation
4 NADW formation +6 Sv +15 !/? (off)
5 Southern Ocean ventilation +20 Sv +35 o
Biogeochemistry
6 Marine biota / iron fertilisation 7 Terrestrial carbon storage
8 CaCO3 chemistry
6 Marine Biota / Iron fertilisation
Marine biological productivity might be Fe limited
in high nitrate low chlorophyll (HNLC) areas (Martin, 1990)
surface nitrate (µmol kg−1) (Conkright et al, 1994)
6 Marine Biota / Iron fertilisation
Aeolian dust input to Antarctica LGM export production:
+ 20% (12 PgC yr−1) Dust/iron input is reduced before rise in CO2 starts
Monnin et al., 2001;
R¨othlisberger et al., 2002
Interval I II III IV
180 200 220 240 260
CO 2[ppmv]
EPICA Dome C CO2
20 18 16 14 12 10
GISP2 age [kyr BP]
0 10 20 30 40 50 nss-Ca2+ [ppb]
EPICA Dome C nss-Ca2+
iron limitation no iron limitation
Time-dependent processes:
Which How (T I) What (ppmv) ?
Physics (without ocean circulation)
1 Temperature +(3–5) K +30 !
2 Sea level / salinity +125 m –15 !
3 Gas exchange / sea ice –50% –15 ?
Ocean circulation
4 NADW formation +6 Sv +15 !/? (off)
5 Southern Ocean ventilation +20 Sv +35 o
Biogeochemistry
6 Marine biota / iron fertilisation –2 PgC yr−1 +20 ? 7 Terrestrial carbon storage
8 CaCO3 chemistry
7 Terrestrial carbon storage
Model and data-based estimates range from 300 to 800 PgC Example from LPJ-DGVM (Preindustrial–LGM)
K¨ohler et al., 2005, Climate Dynamics
Time-dependent processes:
Which How (T I) What (ppmv) ?
Physics (without ocean circulation)
1 Temperature +(3–5) K +30 !
2 Sea level / salinity +125 m –15 !
3 Gas exchange / sea ice –50% –15 ?
Ocean circulation
4 NADW formation +6 Sv +15 !/? (off)
5 Southern Ocean ventilation +20 Sv +35 o
Biogeochemistry
6 Marine biota / iron fertilisation –2 PgC yr−1 +20 ? 7 Terrestrial carbon storage +500 PgC –15 ! 8 CaCO3 chemistry
8 Carbonate compensation
Dissolution / accumulation of CaCO3 depends on deep ocean [CO23− ]
Zeebe and Westbroeck, 2003
8 Carbonate compensation
Anomalies in deep ocean [CO23− ] caused by carbon cycle variations relax to initial state with an e-folding time τ of 1.5 to 6 kyr
100 80 60 40 20 0
Depth (cm) -20
-10 0 10 20 30
CO 32- (molkg-1 )
-20 -10 0 10 20 30
CO 32- (molkg-1 )
25 20 15 10 5
Time (cal kyr BP)
= 6.0 kyr
= 1.5 kyr
8.314 CkyrBP 9.4calkyrBP 3.314 CkyrBP 3.5calkyrBP
τ = 6.0 kyr:
process-based sediment model
(Archer et al., 1997) τ = 1.5 kyr:
reconstruction of deep ocean [CO23− ]
(Marchitto et al., 2005)
after Marchitto et al., 2005
Time-dependent processes:
Which How (T I) What (ppmv) ?
Physics (without ocean circulation)
1 Temperature +(3–5) K +30 !
2 Sea level / salinity +125 m –15 !
3 Gas exchange / sea ice –50% –15 ?
Ocean circulation
4 NADW formation +6 Sv +15 !/? (off)
5 Southern Ocean ventilation +20 Sv +35 o
Biogeochemistry
6 Marine biota / iron fertilisation –2 PgC yr−1 +20 ? 7 Terrestrial carbon storage +500 PgC –15 !
8 CaCO3 chemistry τ=1.5 kyr +20 ?
Time-dependent processes:
Which How (T I) What (ppmv) ?
1 Temperature +(3–5) K +30 !
2 Sea level / salinity +125 m –15 !
3 Gas exchange / sea ice –50% –15 ?
4 NADW formation +6 Sv +15 !/? (off)
5 Southern Ocean ventilation +20 Sv +35 o
6 Marine biota / iron fertilisation –2 PgC yr−1 +20 ? 7 Terrestrial carbon storage +500 PgC –15 !
8 CaCO3 chemistry τ=1.5 kyr +20 ?
Sum +75
Sum (without sea ice) +90
Vostok (incl. Holocene rise) +103
The global record of atmospheric CO
2EPICA — European Project for Ice Coring in Antarctica The global carbon cycle and the box model BICYCLE
Time-dependent processes: motivations and simulation results Combined scenarios
Open questions
Conclusions
Atmospheric carbon during Termination I
Interprete the temporal evolution of atmospheric CO2, δ13C, 14C records
by carbon cycle simulations.
Smith et al., 1999; Monnin et al., 2001;
Stuiver et al., 1998; Hughen et al., 2004
-7.0 -6.8 -6.6 -6.4 -6.2
13 C[o / oo]
Interval I II III IV H1 BA YD 13
C
180 200 220 240 260 280
pCO2[ppmv]
pCO
220 18 16 14 12 10 GISP2 Age [kyr BP]
0 100
200 300 400 500
14 C[o /oo]
14
C
Atmospheric carbon during Termination I
Not only the amplitudes but also the timing of the changes in CO2, δ13C,
14C seems to be appropriate.
Smith et al., 1999; Monnin et al., 2001;
Stuiver et al., 1998; Hughen et al., 2004 K¨ohler et al., 2005,
Global Biogeochemical Cycles
-7.0 -6.8 -6.6 -6.4 -6.2
13 C[o / oo]
Interval I II III IV H1 BA YD 13
C
180 200 220 240 260 280
pCO2[ppmv]
pCO
220 18 16 14 12 10 GISP2 Age [kyr BP]
0 100
200 300 400 500
14 C[o /oo]
20 18 16 14 12 10 GISP2 Age [kyr BP]
0 100
200 300 400 500
14 C[o /oo]
14
C
The EPICA challenge
Working hypothesis:
Our findings for Termination I are of general nature.
Approach:
Use same assumptions and extend forcing data set back in time.
-450 -420 -390 -360
D(o /oo)
EDC D
1 5
7 9
11 13
15 17
MIS
0 500 1000
dust(ppbv) 1500
EDC dust
700 600 500 400 300 200 100 0
Time (kyr BP)
160 200 240 280
pCO2(ppmv)
Vostok pCO2 EDC pCO2
I II
III IV
V VI
VII
0 20 40 60 80 100
IRD(%) (a)
5 10 15
SST(o C)
(b)
5 4 3 2
18 O(o /oo)
(c)
0 -1 -2
18 O(o /oo)
(d)
-15 -10 -5 0
T(K)
(e)
1.0 0.5 0.0
18 O(o /oo)
(f)
-100 -50 0
sealevel(m)
(g)
-450 -420 -390 -360
D(o /oo)
(h)
1 5
7 9
11 13
15 17
500 400 300 200 100 0
Feflux(gm-2 yr-1 )
(i)
700 600 500 400 300 200 100 0
Time (kyr BP)
180 200 220 240 260 280
CO2(ppmv)
700 600 500 400 300 200 100 0
Time (kyr BP)
180 200 220 240 260 280 300
CO2(ppmv)
(j)
S6.0k S1.5k S0.0k
I II
III IV
V VI
VII VIII
a: Heinrich b: N-SST c: NADW d: EQ-SST
e: NH ∆T
f: deep sea ∆T g: sea level
h: SO SST i: Fe fert.
j: CO2
K¨ohler and Fischer, 2006, Climate of the Past
The EPICA challenge
800 700 600
180 200 220 240 260 280 300
CO2(ppmv) S6.0k
S1.5k S0.0k
800 700 600
180 200 220 240 260 280 300
CO2(ppmv)
(a)
VII
"VIII"
17
600 500 400
180 200 220 240 260 280 300
CO2(ppmv)
600 500 400
180 200 220 240 260 280 300
CO2(ppmv)
(b)
V VI
11 13
15
400 300 200
180 200 220 240 260 280 300
CO2(ppmv)
400 300 200
180 200 220 240 260 280 300
CO2(ppmv)
(c)
III IV
7 9
200 100 0
Time (kyr BP) 180
200 220 240 260 280 300
CO2(ppmv)
200 100 0
Time (kyr BP) 180
200 220 240 260 280 300
CO2(ppmv)
(d)
I II
1 5
K¨ohler and Fischer, 2006, Climate of the Past
The EPICA challenge
800 700 600
180 200 220 240 260 280 300
CO2(ppmv) S6.0k
S1.5k S0.0k
800 700 600
180 200 220 240 260 280 300
CO2(ppmv)
(a)
VII
"VIII"
17
600 500 400
180 200 220 240 260 280 300
CO2(ppmv)
600 500 400
180 200 220 240 260 280 300
CO2(ppmv)
(b)
V VI
11 13
15
400 300 200
180 200 220 240 260 280 300
CO2(ppmv)
400 300 200
180 200 220 240 260 280 300
CO2(ppmv)
(c)
III IV
7 9
200 100 0
Time (kyr BP) 180
200 220 240 260 280 300
CO2(ppmv)
200 100 0
Time (kyr BP) 180
200 220 240 260 280 300
CO2(ppmv)
(d)
I II
1 5
1. Terminations I, III, IV, V
K¨ohler and Fischer, 2006, Climate of the Past
The EPICA challenge
800 700 600
180 200 220 240 260 280 300
CO2(ppmv) S6.0k
S1.5k S0.0k
800 700 600
180 200 220 240 260 280 300
CO2(ppmv)
(a)
VII
"VIII"
17
600 500 400
180 200 220 240 260 280 300
CO2(ppmv)
600 500 400
180 200 220 240 260 280 300
CO2(ppmv)
(b)
V VI
11 13
15
400 300 200
180 200 220 240 260 280 300
CO2(ppmv)
400 300 200
180 200 220 240 260 280 300
CO2(ppmv)
(c)
III IV
7 9
200 100 0
Time (kyr BP) 180
200 220 240 260 280 300
CO2(ppmv)
200 100 0
Time (kyr BP) 180
200 220 240 260 280 300
CO2(ppmv)
(d)
I II
1 5
1. Terminations I, III, IV, V 2. Maximum peaks
K¨ohler and Fischer, 2006, Climate of the Past
The EPICA challenge
800 700 600
180 200 220 240 260 280 300
CO2(ppmv) S6.0k
S1.5k S0.0k
800 700 600
180 200 220 240 260 280 300
CO2(ppmv)
(a)
VII
"VIII"
17
600 500 400
180 200 220 240 260 280 300
CO2(ppmv)
600 500 400
180 200 220 240 260 280 300
CO2(ppmv)
(b)
V VI
11 13
15
400 300 200
180 200 220 240 260 280 300
CO2(ppmv)
400 300 200
180 200 220 240 260 280 300
CO2(ppmv)
(c)
III IV
7 9
200 100 0
Time (kyr BP) 180
200 220 240 260 280 300
CO2(ppmv)
200 100 0
Time (kyr BP) 180
200 220 240 260 280 300
CO2(ppmv)
(d)
I II
1 5
1. Terminations I, III, IV, V 2. Maximum peaks
3. Timing inconsistencies
K¨ohler and Fischer, 2006, Climate of the Past
The EPICA challenge
800 700 600
180 200 220 240 260 280 300
CO2(ppmv) S6.0k
S1.5k S0.0k
800 700 600
180 200 220 240 260 280 300
CO2(ppmv)
(a)
VII
"VIII"
17
600 500 400
180 200 220 240 260 280 300
CO2(ppmv)
600 500 400
180 200 220 240 260 280 300
CO2(ppmv)
(b)
V VI
11 13
15
400 300 200
180 200 220 240 260 280 300
CO2(ppmv)
400 300 200
180 200 220 240 260 280 300
CO2(ppmv)
(c)
III IV
7 9
200 100 0
Time (kyr BP) 180
200 220 240 260 280 300
CO2(ppmv)
200 100 0
Time (kyr BP) 180
200 220 240 260 280 300
CO2(ppmv)
(d)
I II
1 5
1. Terminations I, III, IV, V 2. Maximum peaks
3. Timing inconsistencies
Solutions:
A: Synchronisation errors?
B: Missing processes?
C: Are our findings for Termination I
of general nature?
K¨ohler and Fischer, 2006, Climate of the Past
Terminations I-VIII
combined simulation vs. ice core data
∼20 ppmv per Termination are missing
VIII VII VI V IV III II I Number of Termination
0 10 20 30 40 50 60 70 80 90 100 110 120 130
CO 2rise(ppmv)
Vostok and EDC data scenario S1.5K
sum of one-at-a-time sum of all-but-one
Vostok pre-Vostok
K¨ohler and Fischer, 2006, Climate of the Past
Terminations I-VIII
combined simulation vs. ice core data
Termination VI, VII: smaller contributions from OCEAN CIRCULATION and SST
VIII VII VI V IV III II I Number of Termination
0 10 20 30 40 50 60 70 80 90 100 110 120 130
CO 2rise(ppmv)
Vostok and EDC data scenario S1.5K
sum of one-at-a-time sum of all-but-one
Vostok pre-Vostok
K¨ohler and Fischer, 2006, Climate of the Past
pH
pH from δ11B in surface waters of equatorial Atlantic only pH reconstruction available so far
700 600 500 400 300 200 100 0 Time (kyr BP)
8.1 8.15
8.2 8.25 8.3 8.35
pH
S6.0k S1.5k S0.0k
1 5
7 9
11 13
15 17
pH from H¨onisch & Hemming 2005
The global record of atmospheric CO
2EPICA — European Project for Ice Coring in Antarctica The global carbon cycle and the box model BICYCLE
Time-dependent processes: motivations and simulation results Combined scenarios
Open questions
Conclusions
Missing processes
• process-based sediment model (work in progress)
• riverine input of continental weathering
THC
THC
The global carbon cycle
60 PgC/yr 60 PgC/yr
1 PgC/yr 10 PgC/yr
ATMOSPHERE (600 PgC)
ROCK
TERR. BIOSPHERE (2200 PgC)
0.8 PgC/yr
0.2 PgC/yr
0.2 PgC/yr
DEEP OCEAN (38000 PgC)
SEDIMENT
soft tissues | hard shells marine biosphere SURFACE OCEAN (700 PgC)
Continental Weathering
Two effects of continental weathering:
1. a sink for atmospheric CO2
2. a source of HCO−3 and alkalinity to the ocean
For steady state conditions :
riverine input = sedimentation output
Changes in the riverine input lead to changes in the sedimentation output (carbonate compensation) until a new equlibrium with equal input and output is established.
For investigations under changing climates (either 21st century or LGM) one would need :
1. a climate model coupled to a model of continenal weathering 2. riverine inputs in an ocean carbon cycle model (incl sediments)
Continental Weathering II
Two different processes:
• Carbonate weathering: C supply from atmosphere and continental crust
• Silicate weathering: C supply from atmospheric CO2 only
⇒: Outgassing from ocean. Changes in alkalinity are more important than for the changes in the C budget itself.
(Munhoven 1997)
Continental Weathering III
Work on changes in continental weathering during the last 20 000 yr:
• Munhoven 2002: CO2 changes by 6 to 12 ppmv
• Jones et al 2002: CO2 changes by less than 6 ppmv
Shortcomings:
• Weathering: underlying lithology (incl resolution)
• Carbon cycle: simplified model
The global record of atmospheric CO
2EPICA — European Project for Ice Coring in Antarctica The global carbon cycle and the box model BICYCLE
Time-dependent processes: motivations and simulation results Combined scenarios
Open questions
Conclusions
Take Home Messages
1. There are reasonable data- and model-based evidences which processes were influencing the global carbon cycle on glacial/interglacial timescales.
2. The way how they are treated in a model depends on its architecture.
Prescribing climate (box models) vs. internally calculated climate variability (climate models). More important is the agreement with paleo data sets.
3. Not only the amplitudes, but also the timing of changes need to be addres- sed to quantify what impacts individual processes have on CO2.
4. Simulation results are always model-dependent, but the amplitudes of indivi- dual contributions can be estimated with simple models such as BICYCLE.
5. Are our findings for Termination I of general nature?
Take Home Messages
1. There are reasonable data- and model-based evidences which processes were influencing the global carbon cycle on glacial/interglacial timescales.
2. The way how they are treated in a model depends on its architecture.
Prescribing climate (box models) vs. internally calculated climate variability (climate models). More important is the agreement with paleo data sets.
3. Not only the amplitudes, but also the timing of changes need to be addres- sed to quantify what impacts individual processes have on CO2.
4. Simulation results are always model-dependent, but the amplitudes of indivi- dual contributions can be estimated with simple models such as BICYCLE.
5. Are our findings for Termination I of general nature?
Take Home Messages
1. There are reasonable data- and model-based evidences which processes were influencing the global carbon cycle on glacial/interglacial timescales.
2. The way how they are treated in a model depends on its architecture.
Prescribing climate (box models) vs. internally calculated climate variability (climate models). More important is the agreement with paleo data sets.
3. Not only the amplitudes, but also the timing of changes need to be addres- sed to quantify what impacts individual processes have on CO2.
4. Simulation results are always model-dependent, but the amplitudes of indivi- dual contributions can be estimated with simple models such as BICYCLE.
5. Are our findings for Termination I of general nature?
Take Home Messages
1. There are reasonable data- and model-based evidences which processes were influencing the global carbon cycle on glacial/interglacial timescales.
2. The way how they are treated in a model depends on its architecture.
Prescribing climate (box models) vs. internally calculated climate variability (climate models). More important is the agreement with paleo data sets.
3. Not only the amplitudes, but also the timing of changes need to be addres- sed to quantify what impacts individual processes have on CO2.
4. Simulation results are always model-dependent, but the amplitudes of indivi- dual contributions can be estimated with simple models such as BICYCLE.
5. Are our findings for Termination I of general nature?
Take Home Messages
1. There are reasonable data- and model-based evidences which processes were influencing the global carbon cycle on glacial/interglacial timescales.
2. The way how they are treated in a model depends on its architecture.
Prescribing climate (box models) vs. internally calculated climate variability (climate models). More important is the agreement with paleo data sets.
3. Not only the amplitudes, but also the timing of changes need to be addres- sed to quantify what impacts individual processes have on CO2.
4. Simulation results are always model-dependent, but the amplitudes of indivi- dual contributions can be estimated with simple models such as BICYCLE.
5. Are our findings for Termination I of general nature?
Take Home Messages
1. There are reasonable data- and model-based evidences which processes were influencing the global carbon cycle on glacial/interglacial timescales.
2. The way how they are treated in a model depends on its architecture.
Prescribing climate (box models) vs. internally calculated climate variability (climate models). More important is the agreement with paleo data sets.
3. Not only the amplitudes, but also the timing of changes need to be addres- sed to quantify what impacts individual processes have on CO2.
4. Simulation results are always model-dependent, but the amplitudes of indivi- dual contributions can be estimated with simple models such as BICYCLE.
5. Are our findings for Termination I of general nature?
Future δ13C data might verify or falsify our approach.
200 250 300 350
CO 2[ppmv]
700 400 100 Time [kyr BP]
13C CO2
10 7 4 1 Time [kyr BP]
1750 AD
1000 1500 2000 Time [yr AD]
2000 198019902000 Time [yr AD]
-8.5 -8.0 -7.5 -7.0 -6.5 -6.0
13 C[o / oo]