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ACCESS Ocean and Sea Ice Model CORE II Simulations Simon Marsland CSIRO Marine and Atmospheric Research WGOMD, Exeter, May 1, 2009

ACCESS Ocean and Sea Ice Model CORE II Simulations

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ACCESS Ocean and Sea Ice Model CORE II Simulations. Simon Marsland CSIRO Marine and Atmospheric Research WGOMD, Exeter, May 1, 2009. Atmospheric Chemistry (UKCA). Land Surface CABLE (+ CASA-CNP). Atmosphere (UM). Dynamic Vegetation (LPJ). Coupler OASIS. Sea Ice (Auscom – CICE). - PowerPoint PPT Presentation

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Page 1: ACCESS Ocean and Sea Ice Model CORE II Simulations

ACCESS Ocean and Sea Ice ModelCORE II Simulations

Simon Marsland

CSIRO Marine and Atmospheric Research

WGOMD, Exeter, May 1, 2009

Page 2: ACCESS Ocean and Sea Ice Model CORE II Simulations

CSIRO. WGOMD, Exeter, May 1, 2009

ACCESSAustralian Community Climate and Earth System Simulator

• The ACCESS Model is being developed by the

Centre for Australian Weather and Climate Research,

a partnership between CSIRO and the Bureau of Meteorology

CouplerOASIS

Atmosphere(UM)

Sea Ice(Auscom – CICE)

OceanBiogeochemistry

(Matear)

AtmosphericChemistry

(UKCA)

Land SurfaceCABLE

(+ CASA-CNP)

Ocean(Auscom – MOM4)

DynamicVegetation (LPJ)

Page 3: ACCESS Ocean and Sea Ice Model CORE II Simulations

CSIRO. WGOMD, Exeter, May 1, 2009

ACCESS Ocean Model: MOM4p1 + OASIS3.2.5 + CICE4

• 46 vertical levels• Nominal 1 degree global horizontal grid

• Tripolar grid in Arctic region• Equatorial meridional refinement: 1/3 degree from 10S to 10N• Mercator grid in Southern Ocean: 1 degree at 30S to 0.25 degree at 78S

Page 4: ACCESS Ocean and Sea Ice Model CORE II Simulations

CSIRO. WGOMD, Exeter, May 1, 2009

ACCESS Implementation Plan

The Atlantic, May 2009

• 2006: choose some models

• 2007: develop some expertise

• 2009: buy a computer and couple the models

• 2010: commence IPCC/CMIP5 runs

Page 5: ACCESS Ocean and Sea Ice Model CORE II Simulations

CSIRO. WGOMD, Exeter, May 1, 2009

How can a CORE II dataset be used by the “outsiders”?

• Nobody (beyond the ocean modellers) expects much from CORE I

• The opposite is true for CORE II. Everybody expects everything.

• Interannual forcing means people want to see the real world

• Modes of variability: ENSO, NAO, IOD, SAM, …• sea ice, watermasses, convection, overturning, …• Transports: Drake, ITF, …• Seasonal variability, Interannual variability, Decadal variability• etc• Even some climate change, e.g. sea level rise

• Highly likely people will use CORE II outputs as a guide when shopping for a model

• Shoppers will look for what they want to see in a model• And then use the CORE II model run of choice as a control for whatever experiment they have been losing sleep over

• And they will want extension of dataset through to 2008, and beyond in due course?

• e.g. Arctic sea ice, Antarctic sea ice, …

Page 6: ACCESS Ocean and Sea Ice Model CORE II Simulations

CSIRO. WGOMD, Exeter, May 1, 2009

10: Initialisation - Repeat cycles or spinup?Need to account for both initial shock and model drift

• Do we want to spin up with climatology (CORE I) and then start CORE II?

• Do we want to run repeat cycles of CORE II, and how many?

COREv2 interannual

COREv1 normal year

Page 7: ACCESS Ocean and Sea Ice Model CORE II Simulations

CSIRO. WGOMD, Exeter, May 1, 2009

Model validation (I): Global Ocean Water mass transports

Page 8: ACCESS Ocean and Sea Ice Model CORE II Simulations

CSIRO. WGOMD, Exeter, May 1, 2009

12: How can we make output more accessible to community

• Central server versus individual repositories?

• If we intend to individually serve our IPCC outputs to community, then this might be a good practice exercise

• What do the AMIP community do?

Page 9: ACCESS Ocean and Sea Ice Model CORE II Simulations

CSIRO. WGOMD, Exeter, May 1, 2009

Current Australian experiences with CORE II

• We have chosen CORE for our tuning runs

• Currently doing both CORE I and CORE II runs

• Laplacian versus Biharmonic• KPP vs Chen vs GOTM• Convective overturn vs enhanced diffusion• Etc …

Page 10: ACCESS Ocean and Sea Ice Model CORE II Simulations

CSIRO. WGOMD, Exeter, May 1, 2009

ACCESS ocean/sea ice model simulation27 years 1979 - 2005

Sea surface temperatureequatorial Pacific (5°N–5°S; 170°W–120°W)

observed

AusCOM model

Upper ocean heat contentequatorial Pacific (5°N–5°S; 180°–110°W; top 300 m)

Page 11: ACCESS Ocean and Sea Ice Model CORE II Simulations

CSIRO. WGOMD, Exeter, May 1, 2009

AusCOM1.0: Long-term mean

temperature along the equator

Levitus climatology:

Temperature along the equator

Equatorial thermocline - mean 1979-2006

Problems:

• Thermocline too diffusea common model problem

•Western Pacific WarmPool too hot

Page 12: ACCESS Ocean and Sea Ice Model CORE II Simulations

CSIRO. WGOMD, Exeter, May 1, 2009

Pacific equatorial undercurrent (m/s)

A variety of problems:

• undercurrent too weak• undercurrent wrong structure

Possible solutions:

• improved Indonesian Throughflow?• need for higher resolution?• biharmonic versus Laplacian friction?

Pers. Comm. Jaci Brown (CSIRO)

Page 13: ACCESS Ocean and Sea Ice Model CORE II Simulations

CSIRO. WGOMD, Exeter, May 1, 2009

5: INSTANT Mooring Program

• Susan Wijffels and Rebecca Cowley (CAWCR)• INSTANT. International Nusantara Stratification and Transport Program

• 2004-2006 continuous moorings in key straits

• Allows direct comparison with ACCESS model transports

LombokOmbai

Timor

Total ITF

Page 14: ACCESS Ocean and Sea Ice Model CORE II Simulations

CSIRO. WGOMD, Exeter, May 1, 2009

INSTANT/ACCESS comparison - Lombok St

We are making incrementalimprovements to modelITF by tuning individualStrait transports against theobserved intra-seasonal variability

• momentum sink parameterisation is used to reduce flow where necessary

• changes to bathymetry toincrease flow wherenecessary

Page 15: ACCESS Ocean and Sea Ice Model CORE II Simulations

CSIRO. WGOMD, Exeter, May 1, 2009

INSTANT/ACCESS comparison - Lombok St

We are making incrementalimprovements to modelITF by tuning individualStrait transports against theobserved intra-seasonal variability

• momentum sink parameterisation is used to reduce flow where necessary

• changes to bathymetry toincrease flow wherenecessary

Page 16: ACCESS Ocean and Sea Ice Model CORE II Simulations

CSIRO. WGOMD, Exeter, May 1, 2009

INSTANT/ACCESS comparison - Timor St

• Model/data collaborationWe are making incrementalimprovements to modelITF by tuning individualStrait transports against theobserved intra-seasonal variability

• momentum sink parameterisation is used to reduce flow where necessary

• changes to bathymetry toincrease flow where necessary

Page 17: ACCESS Ocean and Sea Ice Model CORE II Simulations

CSIRO. WGOMD, Exeter, May 1, 2009

Opening Timor St - massive earthworks required

• Model/data collaboration

Page 18: ACCESS Ocean and Sea Ice Model CORE II Simulations

CSIRO. WGOMD, Exeter, May 1, 2009

INSTANT/ACCESS comparison - ITF (old)

INSTANT (obs)

Page 19: ACCESS Ocean and Sea Ice Model CORE II Simulations

CSIRO. WGOMD, Exeter, May 1, 2009

INSTANT/ACCESS comparison - ITF (new)

INSTANT (obs)

Page 20: ACCESS Ocean and Sea Ice Model CORE II Simulations

CSIRO. WGOMD, Exeter, May 1, 2009

INSTANT/ACCESS comparison - watermasses

Importance of resolvingcorrect watermassesin transports

Requires tuning ofindividual straits

Recent work indicatesenhanced mixing may help (e.g. tides)

Page 21: ACCESS Ocean and Sea Ice Model CORE II Simulations

CSIRO. WGOMD, Exeter, May 1, 2009

INSTANT/ACCESS comparison - vertical structure

Resolving wind drivenStrait transportreversals

Work in progress

Page 22: ACCESS Ocean and Sea Ice Model CORE II Simulations

CSIRO. WGOMD, Exeter, May 1, 2009

The INSTANT project was 2004-06: same years as the recent bug report

Delivery is delayed to these recipients or distribution lists:[email protected]:This message has not yet been delivered. Microsoft Exchange will continue to try delivering the message on your behalf.Reporting-MTA: dns; relay-central.nems.noaa.gov (tcp_intranet-daemon)Final-recipient: RFC822; [email protected]: delayedStatus: 5.4.0X-Supplementary-Info: < #4.4.7>

SHORTWAVELONGWAVE

Page 23: ACCESS Ocean and Sea Ice Model CORE II Simulations

CSIRO. WGOMD, Exeter, May 1, 2009

4: Baseline metrics: Validating an Ocean Climate Model

• Start with the Griffies et. al CORE I baseline metrics

• Global Diagnostics• Meridional overturning circulation (Global and Atlantic)

• Strength and depth of North Atlantic Deep Water cell• Atlantic outflow at 30 S• Antarctic Bottom Water Cell• Southern Ocean Cell

• Poleward heat transport (Global and Atlantic)• Gulf Stream and Kuroshio currents• Drake Passage transport• Sea ice concentration and thickness (winter and summer)• North Atlantic and Southern Ocean convection• Tropical Pacific velocity structure

Page 24: ACCESS Ocean and Sea Ice Model CORE II Simulations

CSIRO. WGOMD, Exeter, May 1, 2009

ACCESS Atlantic Meridional Overturning Circulation (Sv)

North Atlantic Deep Water (NADW)

Depth of interface

Antarctic BottomWater (AABW)

Equatorial cells

Page 25: ACCESS Ocean and Sea Ice Model CORE II Simulations

CSIRO. WGOMD, Exeter, May 1, 2009

ACCESS Global Meridional Overturning Circulation (Sv)

AntarcticIntermediate Water (AAIW)

Southern Oceancell

Page 26: ACCESS Ocean and Sea Ice Model CORE II Simulations

CSIRO. WGOMD, Exeter, May 1, 2009

ACCESS barotropic streamfunction (Sv)

KuroshioCurrent

Aghulus

GulfStream

DrakePassagetransport

Indonesian Throughflow

Page 27: ACCESS Ocean and Sea Ice Model CORE II Simulations

CSIRO. WGOMD, Exeter, May 1, 2009

Drake Passage transport (Sv)

• Common Ocean Ice Reference Experiment forcing (CORE)• corrected version of NCEP forcing (Large and Yeager, 2008)• COREv1 climatology - too weak?• COREv2 interannual - too strong?

COREv2 interannual

COREv1 normal year

Page 28: ACCESS Ocean and Sea Ice Model CORE II Simulations

CSIRO. WGOMD, Exeter, May 1, 2009

AusCOM high latitude deep convection sites

Northern Hemisphere Southern Hemisphere

• Mixed layer depth shows main sites of deep convection• Importance for water mass exchange• Importance for overturning circulation

Page 29: ACCESS Ocean and Sea Ice Model CORE II Simulations

CSIRO. WGOMD, Exeter, May 1, 2009

February (winter) August (summer)

AusCOM Arctic sea ice thickness (m)

• Arctic sea ice too thin in summer• Too strong ocean vertical mixing?• Sea ice initial condition? Collapse of Arctic halocline.

Page 30: ACCESS Ocean and Sea Ice Model CORE II Simulations

CSIRO. WGOMD, Exeter, May 1, 2009

February (summer) August (winter)

AusCOM Antarctic sea ice thickness (m)

• Too little summer sea ice• Poor representation of Western Weddell Sea• Nice representation of East Antarctic coastal polynyas

Page 31: ACCESS Ocean and Sea Ice Model CORE II Simulations

CSIRO. WGOMD, Exeter, May 1, 2009

Southern Hemisphere Sea Ice ConcentrationYear 200; climatological forcing

Page 32: ACCESS Ocean and Sea Ice Model CORE II Simulations

CSIRO. WGOMD, Exeter, May 1, 2009

Southern Hemisphere Sea Ice Thickness (m)Year 200; climatological forcing

Page 33: ACCESS Ocean and Sea Ice Model CORE II Simulations

CSIRO. WGOMD, Exeter, May 1, 2009

Surface Temperature and Salinity

Initial Condition Year 100 Year 200

SALINITY

TEMPERATURE

Page 34: ACCESS Ocean and Sea Ice Model CORE II Simulations

CSIRO. WGOMD, Exeter, May 1, 2009

Zonal Average Temperature and Salinity:Loss of Antarctic Intermediate Water

Initial Condition Year 100 Year 200

SALINITY

TEMPERATURE

AAIW