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Ocean circulation and sea ice in the MPI-M IPCC experiments Johann Jungclaus Max- Planck- Institut für Meteorologie Hamburg + M. Esch, H. Haak, F. Landerer, M. Boettinger, E. Roeckner ++

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Page 1: Ocean circulation and sea ice in the MPI-M IPCC experiments · 2005. 12. 15. · Atmospheric and oceanic heat transports total atmos ocean 90S 60S 30S EQ 30N 60N 90N 6-4 4 0-6-2 2

Ocean circulation and sea ice in the MPI-M IPCC experiments

Johann JungclausMax- Planck- Institut für Meteorologie

Hamburg

+ M. Esch, H. Haak, F. Landerer, M. Boettinger, E. Roeckner ++

Page 2: Ocean circulation and sea ice in the MPI-M IPCC experiments · 2005. 12. 15. · Atmospheric and oceanic heat transports total atmos ocean 90S 60S 30S EQ 30N 60N 90N 6-4 4 0-6-2 2

Introduction: The role of the ocean in the climate system

The oceans store and transporthuge amounts of heat

The ocean provide the slowcomponent of variability and its inertia may mask global climate change

The ocean provides also a storage and transportmeans for carbon. (25% of anthropogenic carbonemission are taken up bythe oceans)

European temperature March 2005

Page 3: Ocean circulation and sea ice in the MPI-M IPCC experiments · 2005. 12. 15. · Atmospheric and oceanic heat transports total atmos ocean 90S 60S 30S EQ 30N 60N 90N 6-4 4 0-6-2 2

Atmospheric and oceanic heat transportstotal

atmos

ocean

90S 60S 30S EQ 30N 60N 90N

6

-4

4

0

-6

-2

2

Atmosphere and oceantransport about 6 PW (1 PW=1015 W) heat from theequator to high and middlelatitudes

The global oceanaccounts for 1/3 (ca. 2 PW) of this. The Atlantic heat transport is about 1.3 PW

Page 4: Ocean circulation and sea ice in the MPI-M IPCC experiments · 2005. 12. 15. · Atmospheric and oceanic heat transports total atmos ocean 90S 60S 30S EQ 30N 60N 90N 6-4 4 0-6-2 2

The Thermohaline Circulation (THC)

Page 5: Ocean circulation and sea ice in the MPI-M IPCC experiments · 2005. 12. 15. · Atmospheric and oceanic heat transports total atmos ocean 90S 60S 30S EQ 30N 60N 90N 6-4 4 0-6-2 2

Evidence from the past

Abrupt climate changes in the past are associated withdisturbances of the Atlanic Thermohaline Circulation caused byexcessive fresh water input into the North Atlantic

Page 6: Ocean circulation and sea ice in the MPI-M IPCC experiments · 2005. 12. 15. · Atmospheric and oceanic heat transports total atmos ocean 90S 60S 30S EQ 30N 60N 90N 6-4 4 0-6-2 2

Effects of a possible sea change

Page 7: Ocean circulation and sea ice in the MPI-M IPCC experiments · 2005. 12. 15. · Atmospheric and oceanic heat transports total atmos ocean 90S 60S 30S EQ 30N 60N 90N 6-4 4 0-6-2 2

Eiszeit oder Treibhaus?

PM September 2004 Titel

Page 8: Ocean circulation and sea ice in the MPI-M IPCC experiments · 2005. 12. 15. · Atmospheric and oceanic heat transports total atmos ocean 90S 60S 30S EQ 30N 60N 90N 6-4 4 0-6-2 2

Sea ice in the climate systemSea ice effectively decouples ocean and atmosphere. Owing to its high albedo itreflects sun light back to space. Loss of seaice will enhance oceanic heat uptake (icealbedo feedback).

Therefore the sea ice covered regions arevey sensitive to global change

Sea ice stores huge amounts of fresh water. Its release under warming condition mayinfluence the THC.

The presence of sea ice influencesatmospheric circulation.

Sea ice changes will influence the marineand terrestrial ecosystems, and high latitude societies and economics.

Page 9: Ocean circulation and sea ice in the MPI-M IPCC experiments · 2005. 12. 15. · Atmospheric and oceanic heat transports total atmos ocean 90S 60S 30S EQ 30N 60N 90N 6-4 4 0-6-2 2

The coupled ocean atmosphere ModelECHam5: MPI atmosphere model (Roeckner et

al., 2003), interactive runoff and glacier calving scheme.

Resolutions: T63L31 (IPCC)

OASIS 3.0 PRISM coupler

MPI-OM (C-HOPE) (Marsland et al., 2003)C-Grid, z-level, partial cells, BBL

parameterizationHibler-type sea ice model incl. snow and

fractional ice coverConformal mapping: 1.5° with refinement in

grid pole regions

NO FLUX ADJUSTMENT

ECHam5

OASIS

MPI-OM

Page 10: Ocean circulation and sea ice in the MPI-M IPCC experiments · 2005. 12. 15. · Atmospheric and oceanic heat transports total atmos ocean 90S 60S 30S EQ 30N 60N 90N 6-4 4 0-6-2 2

Ocean model grid

Every 5th grid line is shown here; in the vertical, there are40 unevenly spaced depth levels

Page 11: Ocean circulation and sea ice in the MPI-M IPCC experiments · 2005. 12. 15. · Atmospheric and oceanic heat transports total atmos ocean 90S 60S 30S EQ 30N 60N 90N 6-4 4 0-6-2 2

Ocean model grid

Page 12: Ocean circulation and sea ice in the MPI-M IPCC experiments · 2005. 12. 15. · Atmospheric and oceanic heat transports total atmos ocean 90S 60S 30S EQ 30N 60N 90N 6-4 4 0-6-2 2

How well does the model reproduce the presentclimate ?

SST is in general agreement with observations but biases > 1º C are common owing to unresolved processes/features.

These errors are not a unique MPI-OM/ECHAM feature.Jungclaus et al., 2005

Page 13: Ocean circulation and sea ice in the MPI-M IPCC experiments · 2005. 12. 15. · Atmospheric and oceanic heat transports total atmos ocean 90S 60S 30S EQ 30N 60N 90N 6-4 4 0-6-2 2

Precipitation (modeled – observed)

[mm/day]Precipitation bias is most pronounced in equatorial region(Double ITCZ)

Jungclaus et al., 2005

Page 14: Ocean circulation and sea ice in the MPI-M IPCC experiments · 2005. 12. 15. · Atmospheric and oceanic heat transports total atmos ocean 90S 60S 30S EQ 30N 60N 90N 6-4 4 0-6-2 2

Northern hemisphere sea ice conc.Chapman & Walsh 1996 Model (T63/GR1.5 ctrl.)

March

September

Jungclaus et al., 2005

Page 15: Ocean circulation and sea ice in the MPI-M IPCC experiments · 2005. 12. 15. · Atmospheric and oceanic heat transports total atmos ocean 90S 60S 30S EQ 30N 60N 90N 6-4 4 0-6-2 2

Southern hemisphere sea ice conc.Model (T63/GR1.5)Chapman & Walsh 1996

March

September

Page 16: Ocean circulation and sea ice in the MPI-M IPCC experiments · 2005. 12. 15. · Atmospheric and oceanic heat transports total atmos ocean 90S 60S 30S EQ 30N 60N 90N 6-4 4 0-6-2 2

The Atlantic Meridional Overturning Circulation

Jungclaus et al., 2005

Page 17: Ocean circulation and sea ice in the MPI-M IPCC experiments · 2005. 12. 15. · Atmospheric and oceanic heat transports total atmos ocean 90S 60S 30S EQ 30N 60N 90N 6-4 4 0-6-2 2

Meridional heat transport in the Atlantic

ECHAMT63/L31, MPI-OM 1.5

Jungclaus et al., 2005

Page 18: Ocean circulation and sea ice in the MPI-M IPCC experiments · 2005. 12. 15. · Atmospheric and oceanic heat transports total atmos ocean 90S 60S 30S EQ 30N 60N 90N 6-4 4 0-6-2 2

Results from the IPCCscenario experiments

Atm. CO2 concentration Glob. Atm. Surface air temperature

Figure by M. Boettinger, DKRZ

Page 19: Ocean circulation and sea ice in the MPI-M IPCC experiments · 2005. 12. 15. · Atmospheric and oceanic heat transports total atmos ocean 90S 60S 30S EQ 30N 60N 90N 6-4 4 0-6-2 2

IPCC Experiments A1B: SST difference end of 21th century minus 20th century

Widespread warming, North Atlantic shows effect of weaker THC

Page 20: Ocean circulation and sea ice in the MPI-M IPCC experiments · 2005. 12. 15. · Atmospheric and oceanic heat transports total atmos ocean 90S 60S 30S EQ 30N 60N 90N 6-4 4 0-6-2 2

A1B: Sea surface salinity difference end of 21th century minus 20th century

Page 21: Ocean circulation and sea ice in the MPI-M IPCC experiments · 2005. 12. 15. · Atmospheric and oceanic heat transports total atmos ocean 90S 60S 30S EQ 30N 60N 90N 6-4 4 0-6-2 2

What is the fate of the MOC?In a warmer climate, the heating of the upper ocean is

accompanied by freshening in high latitudes and salinification in low latitudes (acceleration of thehydrological cycle). Surface waters in the deep waterformation regions become lighter and the watercolumn is more stably stratified.

This will affect the sinking of deep water and the MOC.

Feedbacks such as salt advection by the ocean maycounteract or enhance the decrease of the MOC.

The relative role of individual feedbacks appears to behighly model dependent.

Page 22: Ocean circulation and sea ice in the MPI-M IPCC experiments · 2005. 12. 15. · Atmospheric and oceanic heat transports total atmos ocean 90S 60S 30S EQ 30N 60N 90N 6-4 4 0-6-2 2

Estimates from different models (Third Assessment Report (TAR))

Figure from IPCC, 2001

Page 23: Ocean circulation and sea ice in the MPI-M IPCC experiments · 2005. 12. 15. · Atmospheric and oceanic heat transports total atmos ocean 90S 60S 30S EQ 30N 60N 90N 6-4 4 0-6-2 2

Projections for the Atlantic MOC for the 21st C

Global Atm. Surfacetemperature[ºC]

Atlantic Meridional overturningcirculation

[Sv, 1Sv=106m3s-1]

Page 24: Ocean circulation and sea ice in the MPI-M IPCC experiments · 2005. 12. 15. · Atmospheric and oceanic heat transports total atmos ocean 90S 60S 30S EQ 30N 60N 90N 6-4 4 0-6-2 2

and beyond...

Global Atm. Surfacetemperature[ºC]

Atlantic Meridional overturningcirculation

[Sv, 1Sv=106m3s-1]

Page 25: Ocean circulation and sea ice in the MPI-M IPCC experiments · 2005. 12. 15. · Atmospheric and oceanic heat transports total atmos ocean 90S 60S 30S EQ 30N 60N 90N 6-4 4 0-6-2 2

Temporal evolution of Atlantic upper oceansalinity

Difference betweenzonally averagedsalinity in the A1B experiment and the 20th

century mean

Positive salinityanomalies in the North Atlantic evolve as a resultof northward salttransport.

Page 26: Ocean circulation and sea ice in the MPI-M IPCC experiments · 2005. 12. 15. · Atmospheric and oceanic heat transports total atmos ocean 90S 60S 30S EQ 30N 60N 90N 6-4 4 0-6-2 2

Temporal evolution of zonally averagedsurface air temperature

A1B

Page 27: Ocean circulation and sea ice in the MPI-M IPCC experiments · 2005. 12. 15. · Atmospheric and oceanic heat transports total atmos ocean 90S 60S 30S EQ 30N 60N 90N 6-4 4 0-6-2 2

Future evolution of Arctic sea ice

Figure by M. Boettinger, DKRZ

Page 28: Ocean circulation and sea ice in the MPI-M IPCC experiments · 2005. 12. 15. · Atmospheric and oceanic heat transports total atmos ocean 90S 60S 30S EQ 30N 60N 90N 6-4 4 0-6-2 2

Animation by M. Boettinger, DKRZ

Page 29: Ocean circulation and sea ice in the MPI-M IPCC experiments · 2005. 12. 15. · Atmospheric and oceanic heat transports total atmos ocean 90S 60S 30S EQ 30N 60N 90N 6-4 4 0-6-2 2

Animation by M. Boettinger, DKRZ

Page 30: Ocean circulation and sea ice in the MPI-M IPCC experiments · 2005. 12. 15. · Atmospheric and oceanic heat transports total atmos ocean 90S 60S 30S EQ 30N 60N 90N 6-4 4 0-6-2 2

Impact of Arctic climate change: New seatransportation routes?

Figure by BBC

Page 31: Ocean circulation and sea ice in the MPI-M IPCC experiments · 2005. 12. 15. · Atmospheric and oceanic heat transports total atmos ocean 90S 60S 30S EQ 30N 60N 90N 6-4 4 0-6-2 2

Open water in the North East Passage (in % of the total area of the coastal corridor)

Time (yr)

% o

f ope

nw

ater

September August October March

Page 32: Ocean circulation and sea ice in the MPI-M IPCC experiments · 2005. 12. 15. · Atmospheric and oceanic heat transports total atmos ocean 90S 60S 30S EQ 30N 60N 90N 6-4 4 0-6-2 2

Great future for Arctic shipping but at whichcosts for the environment?

Ship emissions as observed from space;

will we see a similar track around Siberia?

Page 33: Ocean circulation and sea ice in the MPI-M IPCC experiments · 2005. 12. 15. · Atmospheric and oceanic heat transports total atmos ocean 90S 60S 30S EQ 30N 60N 90N 6-4 4 0-6-2 2

What are climate model results good for?ACIA, the Arctic Climate Impact Assessment

An international project of the Arctic Council and the International Arctic Science Committee (IASC), to evaluate and synthesize knowledge on climate variability, climate change, and increased ultraviolet radiation and their consequences.

The model results were mainly basedon the IPCC TAR (2001) experiments.

ACIA International Scientific Symposium held in Reykjavik, Iceland in November 2004.

http://www.acia.uaf.edu

Page 34: Ocean circulation and sea ice in the MPI-M IPCC experiments · 2005. 12. 15. · Atmospheric and oceanic heat transports total atmos ocean 90S 60S 30S EQ 30N 60N 90N 6-4 4 0-6-2 2

ConclusionsThe new coupled model simulates a reasonable climate withoutflux adjustment.Improvements in comparison with the IPCC TAR models areseen in ocean heat transport, sea ice, and other featuresIn the IPCC scenarios, the Atlantic MOC decreases over the 21st

century but slowly recovers thereafter; this is also the case ifthere is an additional fresh water input from a melting Greenlandice sheet. (This may be model dependent)The model show a considerable and rapid loss of Arctic sea icein the 21st century. While winter sea ice cover is only slightlyreduced the Arctic ocean is projected to become ice free in summer in the 2nd half of the 21st century

Page 35: Ocean circulation and sea ice in the MPI-M IPCC experiments · 2005. 12. 15. · Atmospheric and oceanic heat transports total atmos ocean 90S 60S 30S EQ 30N 60N 90N 6-4 4 0-6-2 2

Data issues

Data are available on original grid (256x220x40 grid points) and (partly) on IPCC standard 1º grid (360x180x40).

Data format is „EXTRA“ (a fortran binary) or NetCDF

10 yr monthly mean of a 3d- data field requires 1.1 GB on original (EXTRA) and 1.25 GB (NetCDF) on regular grid.

10 yr monthly mean of a 2d- data field requires 27 MB on original and 32 MB on regular grid.

Owing to technical problems not all data have beentransferred fo PCMDI.

Data will also be stored in M&D CERA data base

Page 36: Ocean circulation and sea ice in the MPI-M IPCC experiments · 2005. 12. 15. · Atmospheric and oceanic heat transports total atmos ocean 90S 60S 30S EQ 30N 60N 90N 6-4 4 0-6-2 2

Thank You….

Page 37: Ocean circulation and sea ice in the MPI-M IPCC experiments · 2005. 12. 15. · Atmospheric and oceanic heat transports total atmos ocean 90S 60S 30S EQ 30N 60N 90N 6-4 4 0-6-2 2
Page 38: Ocean circulation and sea ice in the MPI-M IPCC experiments · 2005. 12. 15. · Atmospheric and oceanic heat transports total atmos ocean 90S 60S 30S EQ 30N 60N 90N 6-4 4 0-6-2 2

No total breakdown of the MOC....What if we include the meltdown of Greenland ?

The present simulations do not include ice sheet dynamics. Icesheet model projections show a considerable loss of Greenlandice mass (with a high range of uncertainty); estimates rangefrom 0.01 to 0.1 Sv for various scenarios.

From the IPCC experiments one can deduce a melting rate of about 0.03 Sv for the A1B scenario at the end of the 21st

century.

A sensitivity experiment under A1B forcing is carried out where an additional fresh water inflow is prescribed around Greenland. The flux is ramped up from 0 Sv in 2000 to 0.09 Sv in 2100.

Page 39: Ocean circulation and sea ice in the MPI-M IPCC experiments · 2005. 12. 15. · Atmospheric and oceanic heat transports total atmos ocean 90S 60S 30S EQ 30N 60N 90N 6-4 4 0-6-2 2

Effect of additional melt water input fromGreenland on the MOC