A High Resolution Coupled Sea-Ice/Ocean Model for the Antarctic Peninsula Region

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A High Resolution Coupled A High Resolution Coupled Sea-Ice/Ocean Model for the Sea-Ice/Ocean Model for the Antarctic Peninsula Region Antarctic Peninsula Region Michael S. Dinniman Michael S. Dinniman John M. Klinck John M. Klinck Andrea Piñones Andrea Piñones Center for Coastal Physical Center for Coastal Physical Oceanography Oceanography Old Dominion University Old Dominion University

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A High Resolution Coupled Sea-Ice/Ocean Model for the Antarctic Peninsula Region. Michael S. Dinniman John M. Klinck Andrea Piñones Center for Coastal Physical Oceanography Old Dominion University. Outline of Presentation. Introduction and Model Description Ice Shelf Modeling - PowerPoint PPT Presentation

Transcript of A High Resolution Coupled Sea-Ice/Ocean Model for the Antarctic Peninsula Region

Page 1: A High Resolution Coupled Sea-Ice/Ocean Model for the Antarctic Peninsula Region

A High Resolution Coupled A High Resolution Coupled Sea-Ice/Ocean Model for the Sea-Ice/Ocean Model for the Antarctic Peninsula RegionAntarctic Peninsula Region

Michael S. DinnimanMichael S. DinnimanJohn M. KlinckJohn M. Klinck

Andrea PiñonesAndrea PiñonesCenter for Coastal Physical Center for Coastal Physical

OceanographyOceanographyOld Dominion UniversityOld Dominion University

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Outline of PresentationOutline of Presentation

• Introduction and Model Description

• Ice Shelf Modeling

• Sea Ice Modeling

• Cross-shelf Transport

• Future plans

• Conclusions

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Research QuestionsResearch Questions• What is the magnitude and extent of cross-shelf exchange?

• What is the structure of the circulation on the WAP shelf?

• What are the circulation dynamics that drive the coastal current?

• Which physical processes are responsible for exchanges across the permanent pycnocline?

•What processes control sea ice in the region?

What do we need in a circ. model to help answer?

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Antarctic Peninsula ModelAntarctic Peninsula Model• ROMS: 4 km horizontal resolution, 24 levelsROMS: 4 km horizontal resolution, 24 levels• Ice shelves (mechanical and Ice shelves (mechanical and

thermodynamic)thermodynamic)• Dynamic sea iceDynamic sea ice• Bathymetry: ETOPO2v2 + WHOI SOGLOBEC Bathymetry: ETOPO2v2 + WHOI SOGLOBEC

region + region + Padman gridPadman grid + BEDMAP + Maslanyj+ BEDMAP + Maslanyj• Open boundaries: T + S set to SODA, Open boundaries: T + S set to SODA,

barotropic V relaxed to SODA, baroclinic V barotropic V relaxed to SODA, baroclinic V pure radiationpure radiation

• Daily wind forcing from a blend of QSCAT Daily wind forcing from a blend of QSCAT data and NCEP reanalyses or Antarctic data and NCEP reanalyses or Antarctic Mesoscale Prediction System (AMPS) windsMesoscale Prediction System (AMPS) winds

• Other atmospheric parameters from several Other atmospheric parameters from several sources (including AMPS)sources (including AMPS)

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Ice Shelf ModelingIce Shelf Modeling • Ice Shelf basal melt can add large Ice Shelf basal melt can add large

amounts of freshwater to the system (e.g. amounts of freshwater to the system (e.g. George VI estimated basal melt: 2-5 m/yr) George VI estimated basal melt: 2-5 m/yr) which can affect circulation (AP coastal which can affect circulation (AP coastal current?)current?)

• Ice Shelf does not change in time in modelIce Shelf does not change in time in model

• Three equation viscous sub-layer model Three equation viscous sub-layer model for heat and salt fluxes (Holland and for heat and salt fluxes (Holland and Jenkins 1999)Jenkins 1999)

• PGF calculation assumes the ice shelf has PGF calculation assumes the ice shelf has no flexural rigidity and pressure at the no flexural rigidity and pressure at the base comes from the floating icebase comes from the floating ice

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Warm CDW entering theice shelf cavity => Large basal melt:

2.1 m/yr (Potter and Paren, 1985)2.8 m/yr (Corr et al., 2002)3.1-4.8 m/yr (Jenkins and Jacobs,2008)

Model average basal melt under GVI: 6.0 m/yrJenkins and Jacobs, 2008

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Model average velocity(net through flow: 0.13 Sv.)

Potter and Paren (top,1985) andJenkins and Jacobs (bottom, 2008, netS to N through flow 0.17-0.27 Sv.)

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Sea Ice ModelingSea Ice Modeling

•Budgell (2005) model (built into ROMS)

- Thermodynamics based on Mellor and Kantha (1989) with two ice layers, a snow layer, surface melt ponds and a molecular sub layer at the ice/ocean interface

- Dynamics based on an elastic-viscous-plastic rheology after Hunke and Dukowicz (1997) and Hunke (2001)

•Los Alamos CICE available, but not using yet due to time constraints

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Model daily ice

concentration

(12/24/03 – 5/23/04)

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January 2001

January 2002

model ice concentration

SSM/I ice concentration

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QSCAT/NCEP winds

AMPS winds

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Model ice concentrati

on:November

2004

SSM/I:November

2004

QSCAT/NCEP windsAMPS winds

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Maximum temperature below 200mfrom model (average).

Maximum temperature below 200 mfrom observations.

Klinck et al., 2004

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Trajectories of model floats releasedalong the shelf break to show cross-shelf exchange.

Average model velocity at 400m

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Future PlansFuture Plans

• Validation of this modelValidation of this model• 1 km nested model in MB1 km nested model in MB• CICE sea ice model?CICE sea ice model?• Bathymetry: new Smith and Sandwell, Bathymetry: new Smith and Sandwell,

other updates?other updates?• Different atmospheric forcing experimentsDifferent atmospheric forcing experiments• Lower trophic level ecosystem modelLower trophic level ecosystem model• Any suggestions?Any suggestions?

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ConclusionsConclusions• Model is still a work in progressModel is still a work in progress

• Winds are important and good bathymetry Winds are important and good bathymetry is criticalis critical

• Several model features appear to be Several model features appear to be working wellworking well

- George VI Ice Shelf and supply of fresh water to - George VI Ice Shelf and supply of fresh water to Marguerite BayMarguerite Bay

- Sea ice model and interannual variability of ice - Sea ice model and interannual variability of ice concentrationconcentration

- CDW intrusion location- CDW intrusion location

• Lower trophic level ecosystem processes Lower trophic level ecosystem processes are now being added to the modelare now being added to the model

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AcknowledgementsAcknowledgements

• AMPS winds courtesy of John Cassano AMPS winds courtesy of John Cassano (U. Colorado)(U. Colorado)

• Computer facilities and support Computer facilities and support provided by the Center for Coastal provided by the Center for Coastal Physical OceanographyPhysical Oceanography

• Financial support from the U.S. Financial support from the U.S. National Science Foundation (ANT-National Science Foundation (ANT-0523172)0523172)

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July 2001

July 2002

model ice concentration

SSM/I ice concentration

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AMPS ForcingAMPS Forcing

•Antarctic Mesoscale Prediction System: Quasi-Operational atmospheric forecast system in use for the Antarctic

•Currently based on PMM5, but transitioning to WRF

•We have an archive of analyses and forecasts from 30km grid for 2001-2005 (but much of our model domain not covered before 11/02)

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Model ice concentrati

on:August 2004

SSM/I:August 2004

QSCAT/NCEP windsAMPS winds

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Model ice concentrati

on:October

2004

SSM/I:October

2004

QSCAT/NCEP windsAMPS winds

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Feb-Apr 2004 surface velocityQSCAT/NCEP winds

Feb-Apr 2004 surface velocityAMPS winds

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Xie and Arkin Precipitation(m/yr)

AMPS Precipitation(9/03-9/05, m/yr)

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Feb-Apr 2004 surface velocityAMPS winds

Feb-Apr 2004 surface velocityAMPS winds + runoff

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Trajectories of model floats releasedalong the shelf break to show cross-shelf exchange.

Average model velocity at 400m

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Based on Smith and Sandwell(v8.2, only north of 72S)

Smith and Sandwell(v 10.1)