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Supplementary information to chapter 5.8: Modelling the end of an interglacial (MIS 1, 5, 7, 9, 11)...

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Supplementary information to chapter 5.8: Modelling the end of an interglacial (MIS 1, 5, 7, 9, 11) Claudia Kubatzki*, Martin Claussen**, Reinhard Calov, Andrey Ganopolski Potsdam-Institute for Climate Impact Research PO Box 601203, 14412 Potsdam *now at Alfred Wegener Institute Bussestr. 24, 27570 Bremerhaven www.awi-bremerhaven.de /People/ show?ckubatzk ( www.pik-potsdam.de /~ kubi ) [email protected] **now at University of Hamburg and Max Planck Institute for Meteorology
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Page 1: Supplementary information to chapter 5.8: Modelling the end of an interglacial (MIS 1, 5, 7, 9, 11) Claudia Kubatzki*, Martin Claussen**, Reinhard Calov,

Supplementary information to chapter 5.8:

Modelling the end of an interglacial(MIS 1, 5, 7, 9, 11)

Claudia Kubatzki*, Martin Claussen**, Reinhard Calov, Andrey Ganopolski

Potsdam-Institute for Climate Impact ResearchPO Box 601203, 14412 Potsdam

 *now at Alfred Wegener InstituteBussestr. 24, 27570 Bremerhaven

www.awi-bremerhaven.de/People/show?ckubatzk ( www.pik-potsdam.de/~kubi )

[email protected] **now at University of Hamburg and Max Planck Institute for Meteorology

Page 2: Supplementary information to chapter 5.8: Modelling the end of an interglacial (MIS 1, 5, 7, 9, 11) Claudia Kubatzki*, Martin Claussen**, Reinhard Calov,

Figures I

This first part contains the figures of our book chapter.

Page 3: Supplementary information to chapter 5.8: Modelling the end of an interglacial (MIS 1, 5, 7, 9, 11) Claudia Kubatzki*, Martin Claussen**, Reinhard Calov,
Page 4: Supplementary information to chapter 5.8: Modelling the end of an interglacial (MIS 1, 5, 7, 9, 11) Claudia Kubatzki*, Martin Claussen**, Reinhard Calov,
Page 5: Supplementary information to chapter 5.8: Modelling the end of an interglacial (MIS 1, 5, 7, 9, 11) Claudia Kubatzki*, Martin Claussen**, Reinhard Calov,
Page 6: Supplementary information to chapter 5.8: Modelling the end of an interglacial (MIS 1, 5, 7, 9, 11) Claudia Kubatzki*, Martin Claussen**, Reinhard Calov,
Page 7: Supplementary information to chapter 5.8: Modelling the end of an interglacial (MIS 1, 5, 7, 9, 11) Claudia Kubatzki*, Martin Claussen**, Reinhard Calov,
Page 8: Supplementary information to chapter 5.8: Modelling the end of an interglacial (MIS 1, 5, 7, 9, 11) Claudia Kubatzki*, Martin Claussen**, Reinhard Calov,
Page 9: Supplementary information to chapter 5.8: Modelling the end of an interglacial (MIS 1, 5, 7, 9, 11) Claudia Kubatzki*, Martin Claussen**, Reinhard Calov,
Page 10: Supplementary information to chapter 5.8: Modelling the end of an interglacial (MIS 1, 5, 7, 9, 11) Claudia Kubatzki*, Martin Claussen**, Reinhard Calov,
Page 11: Supplementary information to chapter 5.8: Modelling the end of an interglacial (MIS 1, 5, 7, 9, 11) Claudia Kubatzki*, Martin Claussen**, Reinhard Calov,

Figures II

This second part contains supplementary material.

Page 12: Supplementary information to chapter 5.8: Modelling the end of an interglacial (MIS 1, 5, 7, 9, 11) Claudia Kubatzki*, Martin Claussen**, Reinhard Calov,

Model:

CLIMBER-2.3• is an Earth system model of intermediate complexity („weather“ parameterized, coarse spatial resolution except for the inland-ice module);• couples atmosphere, ocean, vegetation, inland ice, carbon cycle;• is driven by changes in insolation and CO2;• simulation period: several thousands of years.

Page 13: Supplementary information to chapter 5.8: Modelling the end of an interglacial (MIS 1, 5, 7, 9, 11) Claudia Kubatzki*, Martin Claussen**, Reinhard Calov,
Page 14: Supplementary information to chapter 5.8: Modelling the end of an interglacial (MIS 1, 5, 7, 9, 11) Claudia Kubatzki*, Martin Claussen**, Reinhard Calov,

Glacial inception:

At the end of the Eemian interglacial decreasing summer insolation in the northern hemisphere; glacial inception in Northern America at about 117 kyBP; bifurcation (strong positive snow-albedo feedback); sea-level change about 40m until 100 kyBP.

Page 15: Supplementary information to chapter 5.8: Modelling the end of an interglacial (MIS 1, 5, 7, 9, 11) Claudia Kubatzki*, Martin Claussen**, Reinhard Calov,

CO2 and insolation (Last Glacial Inception):

Page 16: Supplementary information to chapter 5.8: Modelling the end of an interglacial (MIS 1, 5, 7, 9, 11) Claudia Kubatzki*, Martin Claussen**, Reinhard Calov,

longitude longitude

latitude

latitude

Last Glacial Inception:

ice thickness [m]

(Changessince Eemian)

2000 years

Page 17: Supplementary information to chapter 5.8: Modelling the end of an interglacial (MIS 1, 5, 7, 9, 11) Claudia Kubatzki*, Martin Claussen**, Reinhard Calov,

Last glacial inceptionas bifurcation

(max. volume lags area by ~ 3 ky)

Page 18: Supplementary information to chapter 5.8: Modelling the end of an interglacial (MIS 1, 5, 7, 9, 11) Claudia Kubatzki*, Martin Claussen**, Reinhard Calov,

128 kyBP 117 kyBP

100 kyBP

Atlantic oceanmeridional overturningcirculation

Page 19: Supplementary information to chapter 5.8: Modelling the end of an interglacial (MIS 1, 5, 7, 9, 11) Claudia Kubatzki*, Martin Claussen**, Reinhard Calov,

125 kyBP 115 kyBP

100 kyBP

10% 90% Tree fraction

Page 20: Supplementary information to chapter 5.8: Modelling the end of an interglacial (MIS 1, 5, 7, 9, 11) Claudia Kubatzki*, Martin Claussen**, Reinhard Calov,

Amplification factors:

• The last glacial inception in the model is mainly caused by changes in the precession.• Changes in the ocean surface as well as of vegetation provide a crucial additional, positive albedo feedback.• Variations in the atmospheric CO2 only act as an amplification factor.

Page 21: Supplementary information to chapter 5.8: Modelling the end of an interglacial (MIS 1, 5, 7, 9, 11) Claudia Kubatzki*, Martin Claussen**, Reinhard Calov,

Ice-area (North America):

Temperature (global annual):

Last Glacial Inception:

- Precession initiates ice-sheet growth

- Obliquity / CO2

act as amplifiers

Page 22: Supplementary information to chapter 5.8: Modelling the end of an interglacial (MIS 1, 5, 7, 9, 11) Claudia Kubatzki*, Martin Claussen**, Reinhard Calov,

Fixed pre-ind. ... ... or Eemian surface conditions

Atm.+ oce.+veg.Atm.+ oce.Atm.+ veg.Atm.interactivelysimulated,othercomponentsfixed

Page 23: Supplementary information to chapter 5.8: Modelling the end of an interglacial (MIS 1, 5, 7, 9, 11) Claudia Kubatzki*, Martin Claussen**, Reinhard Calov,

Cold events:

At the end of the Eemian interglacial:• data show abrupt cooling events, and forest decline in central Europe;• reproducable in the model due to changes in the Atlantic overturning circulation,• caused by disturbing the North Atlantic freshwater balance.

Page 24: Supplementary information to chapter 5.8: Modelling the end of an interglacial (MIS 1, 5, 7, 9, 11) Claudia Kubatzki*, Martin Claussen**, Reinhard Calov,

Stadials

D-O events

Temperature in Greenland: CLIMBER-2 and NGRIP

NGRIP members 2004

Freshwaterdisturbances(„IRDs“)

Page 25: Supplementary information to chapter 5.8: Modelling the end of an interglacial (MIS 1, 5, 7, 9, 11) Claudia Kubatzki*, Martin Claussen**, Reinhard Calov,

• An ice-free Greenland is a possible second equilibrium state in the model under the insolation forcing of 128 kyr BP. • Timing and extent of northern American glaciation at the end of the Eemian, however, do not depend on the size of the Greenland ice sheet during the Eemian.

Page 26: Supplementary information to chapter 5.8: Modelling the end of an interglacial (MIS 1, 5, 7, 9, 11) Claudia Kubatzki*, Martin Claussen**, Reinhard Calov,

Sea-level change (difference to pre-industrial):

Difference between the two runsresulting from two possible equilibrium statesof the Greenland ice sheet

Page 27: Supplementary information to chapter 5.8: Modelling the end of an interglacial (MIS 1, 5, 7, 9, 11) Claudia Kubatzki*, Martin Claussen**, Reinhard Calov,

The end of the current interglacial:

In the next 50,000 years („natural“ forcing) only small changes in solar insolation; insolation variations comparably low as during MIS 11 but no significant expansion of inland ice in the model.

Page 28: Supplementary information to chapter 5.8: Modelling the end of an interglacial (MIS 1, 5, 7, 9, 11) Claudia Kubatzki*, Martin Claussen**, Reinhard Calov,

Maximum insolation at 65oN

11975MIS 1

CO2 from Vostok

Petit et al. 1999

11975MIS

Berger 1978

Page 29: Supplementary information to chapter 5.8: Modelling the end of an interglacial (MIS 1, 5, 7, 9, 11) Claudia Kubatzki*, Martin Claussen**, Reinhard Calov,

meters

Inland-ice area

MIS 10 MIS 11 50 kyAP Present

Height of inland ice at the end of MIS 10 (343kyBP)

Future glaciation ?Sea-level change

Page 30: Supplementary information to chapter 5.8: Modelling the end of an interglacial (MIS 1, 5, 7, 9, 11) Claudia Kubatzki*, Martin Claussen**, Reinhard Calov,

Application of our model to a ‘typical GCM setup’:

• The extent to which time-slice simulations of 115 kyr BP are able to reproduce a transient simulation of the last glacial inception is significantly influenced by use of a high-resolution orography and the atmospheric CO2 concentration applied.• Certain combinations of synchronously-run periods and acceleration of the climate model as compared to the ice-sheet module enable a reasonable reproduction of a fully synchronous run.

Page 31: Supplementary information to chapter 5.8: Modelling the end of an interglacial (MIS 1, 5, 7, 9, 11) Claudia Kubatzki*, Martin Claussen**, Reinhard Calov,

Annual temperature (difference to pre-industrial):

the transient simulation of the

fully coupled model at 115 ka BP,

a time slice simulation of 115 ka BPwith fixed pre-industrial ice sheets,

a time slice simulation of 115 ka BP

with interactive inland ice model.

Page 32: Supplementary information to chapter 5.8: Modelling the end of an interglacial (MIS 1, 5, 7, 9, 11) Claudia Kubatzki*, Martin Claussen**, Reinhard Calov,

Simulation of the last glacial inceptionapplying different levels of climate vs. ice-sheet model acceleration

(coupling period / presetting run time, the black line gives the control run).

Global ice volume:


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