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Modeling the MOC Ronald J Stouffer Geophysical Fluid Dynamics Laboratory NOAA The views described...

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Modeling the MOC Ronald J Stouffer Geophysical Fluid Dynamics Laboratory NOAA The views described here are solely those of the presenter and not of GFDL/NOAA/DOC or any other agency or institution. http:// www.andrill.org/ iceberg/blogs/ julian/images/ greatoceanconveyor. jpg
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Page 1: Modeling the MOC Ronald J Stouffer Geophysical Fluid Dynamics Laboratory NOAA The views described here are solely those of the presenter and not of GFDL/NOAA/DOC.

Modeling the MOC

Ronald J StoufferGeophysical Fluid Dynamics Laboratory

NOAAThe views described here are solely those of the presenter and not of GFDL/NOAA/DOC or any other agency or institution.

http://www.andrill.org/iceberg/blogs/julian/images/greatoceanconveyor.jpg

Page 2: Modeling the MOC Ronald J Stouffer Geophysical Fluid Dynamics Laboratory NOAA The views described here are solely those of the presenter and not of GFDL/NOAA/DOC.

Modeling the MOCOutline

• Role of MOC in maintaining mean climate– Northward Heat Transport – Northward Salt transport

• Role of MOC in Abrupt Climate Change– Unforced– Forced

• Predictability

Page 3: Modeling the MOC Ronald J Stouffer Geophysical Fluid Dynamics Laboratory NOAA The views described here are solely those of the presenter and not of GFDL/NOAA/DOC.

How well do models simulate the T, S structure in the ocean?

AR4 ensemble mean error Temperature

IPCC WGI Chapter 8

-2.5 +2.5

Page 4: Modeling the MOC Ronald J Stouffer Geophysical Fluid Dynamics Laboratory NOAA The views described here are solely those of the presenter and not of GFDL/NOAA/DOC.

AR4 ensemble mean errorSalinity

90N 90S

-0.2 0.2-0.4 0.4

IPCC WGI Chapter 8 Suppl. Material

EQ

PSU-1.0 +1.0

Page 5: Modeling the MOC Ronald J Stouffer Geophysical Fluid Dynamics Laboratory NOAA The views described here are solely those of the presenter and not of GFDL/NOAA/DOC.

Role of MOC in Heat Transport

Page 6: Modeling the MOC Ronald J Stouffer Geophysical Fluid Dynamics Laboratory NOAA The views described here are solely those of the presenter and not of GFDL/NOAA/DOC.

Impact of MOC on Climate(SAT)

AOGCMs

EMICs

MOC “on” minus “off” oC

Conclusion – MOC warms NH, locally large values, MOC cools SH

Page 7: Modeling the MOC Ronald J Stouffer Geophysical Fluid Dynamics Laboratory NOAA The views described here are solely those of the presenter and not of GFDL/NOAA/DOC.

Impact of MOC on Climate

Zonally averaged Precipitation differences(mm/day)

Red lines controlBlue lines difference

Dashed – EMICsSolid - AOGCMs

Conclusion – MOC on => ITCZ toward north

Page 8: Modeling the MOC Ronald J Stouffer Geophysical Fluid Dynamics Laboratory NOAA The views described here are solely those of the presenter and not of GFDL/NOAA/DOC.

Impact of MOC on ClimateSalinity MOC “on” minus “off”

(PSU)

Page 9: Modeling the MOC Ronald J Stouffer Geophysical Fluid Dynamics Laboratory NOAA The views described here are solely those of the presenter and not of GFDL/NOAA/DOC.

Role of MOC in maintaining mean climate

• North Atlantic saltier than without MOC– Rest of world ocean surface more fresh

• Northern Hemisphere warmer than without– Particularly the N Atlantic– Role of atmosphere mixing heat

Page 10: Modeling the MOC Ronald J Stouffer Geophysical Fluid Dynamics Laboratory NOAA The views described here are solely those of the presenter and not of GFDL/NOAA/DOC.

Ocean MOC Role in Abrupt Climate Changes

• Unforced – Hall and Stouffer Nature

• Forced– Idealized (Hosing ) - Stouffer et al. JoC 2006

Page 11: Modeling the MOC Ronald J Stouffer Geophysical Fluid Dynamics Laboratory NOAA The views described here are solely those of the presenter and not of GFDL/NOAA/DOC.

TransientAn Anomalous Event (Unforced)

Page 12: Modeling the MOC Ronald J Stouffer Geophysical Fluid Dynamics Laboratory NOAA The views described here are solely those of the presenter and not of GFDL/NOAA/DOC.

Maximum Negative Anomaly

Page 13: Modeling the MOC Ronald J Stouffer Geophysical Fluid Dynamics Laboratory NOAA The views described here are solely those of the presenter and not of GFDL/NOAA/DOC.

Maximum Positive Anomaly

Page 14: Modeling the MOC Ronald J Stouffer Geophysical Fluid Dynamics Laboratory NOAA The views described here are solely those of the presenter and not of GFDL/NOAA/DOC.

Surface Air TemperatureDecadal Mean Difference

Page 15: Modeling the MOC Ronald J Stouffer Geophysical Fluid Dynamics Laboratory NOAA The views described here are solely those of the presenter and not of GFDL/NOAA/DOC.

Surface variables/THC

Page 16: Modeling the MOC Ronald J Stouffer Geophysical Fluid Dynamics Laboratory NOAA The views described here are solely those of the presenter and not of GFDL/NOAA/DOC.

Summary of Physical

Mechanism

Page 17: Modeling the MOC Ronald J Stouffer Geophysical Fluid Dynamics Laboratory NOAA The views described here are solely those of the presenter and not of GFDL/NOAA/DOC.

Unforced MOC variability

• If model if “realistic”– Can we predict this event?– Complicating GHG changes– Possible explanation of some parts of paleo-

record

Page 18: Modeling the MOC Ronald J Stouffer Geophysical Fluid Dynamics Laboratory NOAA The views described here are solely those of the presenter and not of GFDL/NOAA/DOC.

Experimental DesignManabe Climate Model “MCM”

• R30 AOGCM coupled model

• Idealized Water hosing– 1 Sv for 100 years– After 100 years, stop hosing - allow recovery

• Case 1: Hosing 50N to 70N in Atlantic

• Case 2: Hosing south of 60S in Southern Ocean

• Compare to long control integration

Page 19: Modeling the MOC Ronald J Stouffer Geophysical Fluid Dynamics Laboratory NOAA The views described here are solely those of the presenter and not of GFDL/NOAA/DOC.

Simulated Global MOC

SH Index box NH Index box

Page 20: Modeling the MOC Ronald J Stouffer Geophysical Fluid Dynamics Laboratory NOAA The views described here are solely those of the presenter and not of GFDL/NOAA/DOC.

Atlantic THC Response

SV

Years

Atlantic THCdoes notrespond in aseesaw-likemanner

NH Hosing –NH THCshuts down

Page 21: Modeling the MOC Ronald J Stouffer Geophysical Fluid Dynamics Laboratory NOAA The views described here are solely those of the presenter and not of GFDL/NOAA/DOC.

SH THC Response

SV

Years

SH Hosing –

SH THCweakens.

SH THCdoes notshut down

Page 22: Modeling the MOC Ronald J Stouffer Geophysical Fluid Dynamics Laboratory NOAA The views described here are solely those of the presenter and not of GFDL/NOAA/DOC.

SAT Difference mapSH hosing

K

Years 51-100 hosing minus 1-200 control

Page 23: Modeling the MOC Ronald J Stouffer Geophysical Fluid Dynamics Laboratory NOAA The views described here are solely those of the presenter and not of GFDL/NOAA/DOC.

Surface Salinity Response

0 100 200 Years

0 100 200 Years

NH

SH

NH SSS anomaly –Intense and confined

SH SSS anomaly –Weaker and spreads

PSU

Page 24: Modeling the MOC Ronald J Stouffer Geophysical Fluid Dynamics Laboratory NOAA The views described here are solely those of the presenter and not of GFDL/NOAA/DOC.

Differences in Sea Surface Salinity (PSU)

Southern Freshwater Escape

25 years 100 years

Hosing minus Control

Page 25: Modeling the MOC Ronald J Stouffer Geophysical Fluid Dynamics Laboratory NOAA The views described here are solely those of the presenter and not of GFDL/NOAA/DOC.

Sea Surface Temperature Response

0 100 200 Years

0 100 200 Years

NH

SH

Response more symmetrical than SSSMagnitude also becoming more similar

K

Page 26: Modeling the MOC Ronald J Stouffer Geophysical Fluid Dynamics Laboratory NOAA The views described here are solely those of the presenter and not of GFDL/NOAA/DOC.

Surface Air Temperature Response

0 100 200 Years

0 100 200 Years

NH

SH

Response remarkably symmetrical (first 100 yrs)Magnitude very similar

K

Page 27: Modeling the MOC Ronald J Stouffer Geophysical Fluid Dynamics Laboratory NOAA The views described here are solely those of the presenter and not of GFDL/NOAA/DOC.

Precipitation Response

0 100 200 Years

0 100 200 Years

NH

SH

Response very symmetricMagnitude very similarITCZ shifts toward warmer hemisphere

Cm/day

Page 28: Modeling the MOC Ronald J Stouffer Geophysical Fluid Dynamics Laboratory NOAA The views described here are solely those of the presenter and not of GFDL/NOAA/DOC.

Hosing Experiment Summary

• Symmetrical Atmospheric Response

• Much less symmetry in ocean

• Why?– Strong Circum-Antarctica winds– Northward flowing surface waters– Freshwater “escapes” into other basins

• Far a field impacts• Less local impacts

Page 29: Modeling the MOC Ronald J Stouffer Geophysical Fluid Dynamics Laboratory NOAA The views described here are solely those of the presenter and not of GFDL/NOAA/DOC.

MOC Predictability

• Unforced Changes– Are MOC predictable?– How long into future– Manifest in surface changes?

• Forced - GHG increase – Does MOC weaken?– How much?– Likelihood of complete shutdown?

Page 30: Modeling the MOC Ronald J Stouffer Geophysical Fluid Dynamics Laboratory NOAA The views described here are solely those of the presenter and not of GFDL/NOAA/DOC.

Predictability Investigations just starting

• Perfect model experiments

• Use ICs from long control– Ocean ICs unchanged from control– Atmosphere ICs shifted in time by day or 2

• Probably “best case” for predictability– No model errors– Ocean ICs perfectly known

Page 31: Modeling the MOC Ronald J Stouffer Geophysical Fluid Dynamics Laboratory NOAA The views described here are solely those of the presenter and not of GFDL/NOAA/DOC.

Predictability ofAtlantic MeridionalOverturning Circulation(AMOC) in GFDLCM2.1 Climate Model

Page 32: Modeling the MOC Ronald J Stouffer Geophysical Fluid Dynamics Laboratory NOAA The views described here are solely those of the presenter and not of GFDL/NOAA/DOC.
Page 33: Modeling the MOC Ronald J Stouffer Geophysical Fluid Dynamics Laboratory NOAA The views described here are solely those of the presenter and not of GFDL/NOAA/DOC.

Are past ocean observations good enough to constrain MOC?

• Past ocean observations mainly XBTs– Temperature only– Upper 700 m or so

• Since 2003 or so – ARGO– T, S– Upper 2 km

Page 34: Modeling the MOC Ronald J Stouffer Geophysical Fluid Dynamics Laboratory NOAA The views described here are solely those of the presenter and not of GFDL/NOAA/DOC.

Can Observations constrain the MOC?

Need ARGOand atmosphericdata to constrain MOC

Other research suggests this may be too pessimistic.

Page 35: Modeling the MOC Ronald J Stouffer Geophysical Fluid Dynamics Laboratory NOAA The views described here are solely those of the presenter and not of GFDL/NOAA/DOC.

A

AR4 WG1 Assessment: MOC very likely to weaken MOC shutdown very unlikely

MOC and Forced Climate Change

Page 36: Modeling the MOC Ronald J Stouffer Geophysical Fluid Dynamics Laboratory NOAA The views described here are solely those of the presenter and not of GFDL/NOAA/DOC.

Why does MOC slow down as GHG increase?

• Role of surface fluxes– Heat fluxes– Water fluxes

Page 37: Modeling the MOC Ronald J Stouffer Geophysical Fluid Dynamics Laboratory NOAA The views described here are solely those of the presenter and not of GFDL/NOAA/DOC.

Design of Partially Coupled Experiments

Gregory et al. 2006 GRL

• Run control and 1% per year CO2 increase experiment– Save out surface fluxes

• Use water fluxes from control in 1% run– TRAD_CH2O

• Use water fluxes from 1% in control– CRAD_TH2O

• Isolates role of heat and water fluxes

Page 38: Modeling the MOC Ronald J Stouffer Geophysical Fluid Dynamics Laboratory NOAA The views described here are solely those of the presenter and not of GFDL/NOAA/DOC.

Summary of Partially Coupled Experiment

Conclusions:

1. Heat fluxes changes always weaken MOC

2. Water fluxes changes mixed, but usually weaken MOC

3. Response to heat flux changes fairly uniform

Page 39: Modeling the MOC Ronald J Stouffer Geophysical Fluid Dynamics Laboratory NOAA The views described here are solely those of the presenter and not of GFDL/NOAA/DOC.

Warming greatest over land and at most high northern latitudes and least over Southern

Ocean and parts of the North Atlantic Ocean

• Weakening of MOC contributes to minimum in cooling in N Atlantic => smaller climate change => a positive impact?

Surface Warming Pattern

A1B, 2090-2099 relative to 1980-1999

IPCC WGI SPM

Page 40: Modeling the MOC Ronald J Stouffer Geophysical Fluid Dynamics Laboratory NOAA The views described here are solely those of the presenter and not of GFDL/NOAA/DOC.

Summary:Ocean’s Role in Abrupt Climate

Change• Unforced

– Possible to have large abrupt climate changes in AOGCMs

• Forced– Idealized

• Allows easy study of climate response• Application to paleo-data and future climate changes

– GHG increase

• Predictability of MOC changes

Page 41: Modeling the MOC Ronald J Stouffer Geophysical Fluid Dynamics Laboratory NOAA The views described here are solely those of the presenter and not of GFDL/NOAA/DOC.

Questions

• Basic Issues– Why does the MOC exist?– How much mixing is there in the ocean?

• Do models have too much/too little? • Impacts of mixing on the MOC• What are the physical processes?

– What is the role of ocean eddies?– How does MOC changes impact biology and

associated changes in atmospheric pCO2?

Page 42: Modeling the MOC Ronald J Stouffer Geophysical Fluid Dynamics Laboratory NOAA The views described here are solely those of the presenter and not of GFDL/NOAA/DOC.

Questions

• Variability– Are observations good enough to constrain MOC? – Are the MOC changes predictable?

• Time scale?• Does it matter for where people live?• Paleo-data tests?

– What is role of MOC variability/changes in tropical Atlantic SST/hurricane changes?

• Future– Is future weakening of the MOC “bad”?– Interactions with Greenland/Antarctic ice melting

Page 43: Modeling the MOC Ronald J Stouffer Geophysical Fluid Dynamics Laboratory NOAA The views described here are solely those of the presenter and not of GFDL/NOAA/DOC.

Thank you


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