Validation Analysis of the 0.72˚ HYCOM/CICE 4.0 2003-2006 run Dmitry Dukhovskoy, Pam Posey, Joe Metzger, Alan Wallcraft, and Eric Chassignet.

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Validation Analysis of the 0.72˚ HYCOM/CICE run Dmitry Dukhovskoy, Pam Posey, Joe Metzger, Alan Wallcraft, and Eric Chassignet

Participant in the International partnership program funded by NSF: Arctic Ocean Model Intercomparison Project (AOMIP). AOMIP Goals: (1) Validate and improve Arctic Ocean models in coordinated fashion - identify the most consistent errors across models - propose solutions - select the most reliable and consistent Arctic Ocean / Sea Ice models (2) Investigate processes using observations and model results - How to avoid restoring and flux correction? - Formation of the Arctic Ocean halocline - Parameterization of stress-driven and convection-driven mixing (3) Climate change - 50-year experiment under “observed” forcing and 100-year experiment under reconstructed forcing Arctic Study at COAPS FSU

AOMIP Models InstitutionAWIGSFCUWNPSUMASS / WHOI FSU (ARCc0.72 / ARCc0.08) Ocean Model MOMPOMMOM FVCOMHYCOM Ice CoupledYes Vertical Levels Z levelssigma30 Z levels 40 s-layers32 hybrid Resolution>20 km~22 km~18 km1 km shelf ~15 km deep ~30 km / ~3 km Min Depth15 m45 m5 m50 m / 10 m

Developed at NRL coupled HYCOM/CICE applicationDeveloped at NRL coupled HYCOM/CICE application - ESMF-based HYCOM provided by NRL-SSC - ESMF-based HYCOM provided by NRL-SSC - ESMF-based CICE 4.0 provided by LANL - ESMF-based CICE 4.0 provided by LANL - All coupling by NRL-SSC - All coupling by NRL-SSC HYCOM/CICE at NRLHYCOM/CICE at NRL - Initially for Arctic-only domain and a Bering Sea - Initially for Arctic-only domain and a Bering Sea domain for testing data assimilation domain for testing data assimilation - Soon for fully global domain - Soon for fully global domain HYCOM/CICE 4.0 Overview

State of the art sea-ice modelState of the art sea-ice model - Multi-category ice thickness - Multi-category ice thickness - Energy conserving thermodynamics - Energy conserving thermodynamics - Energy-based ridging scheme - Energy-based ridging scheme - Elastic-viscous-plastic (EVP) ice dynamics - Elastic-viscous-plastic (EVP) ice dynamics Open Source ice modelOpen Source ice model Los Alamos Sea Ice Model (CICE 4.0)

0.72° Arctic P-grid DX (km) Run for Run for Arctic-only grid is a sub-region of the tripole gridArctic-only grid is a sub-region of the tripole grid - Bottom in the Atlantic, top in the Pacific - Bottom in the Atlantic, top in the Pacific Atlantic and Pacific boundariesAtlantic and Pacific boundaries - Closed (no-ice) in CICE - Closed (no-ice) in CICE - Closed but with relaxation to climatology in HYCOM - Closed but with relaxation to climatology in HYCOM The model coastline is at the 50 m isobath (closing the Bering Strait)The model coastline is at the 50 m isobath (closing the Bering Strait) 3 hourly NOGAPS 0.5˚ atmospheric forcing fields3 hourly NOGAPS 0.5˚ atmospheric forcing fields HYCOM/CICE ARCc 0.72˚

HYCOM/CICE ARCc0.08 Run for The model coastline is at the 10 m isobath (Bering Strait open). 3 hourly NOGAPS 0.5 degree atmospheric forcing fields OBs are forced by the 1/12° global HYCOM Ocean model is initialized from 1/12˚ non-assimilative global HYCOM 0.08° Arctic grid resolution (km)

Background: Arctic Ocean

60N 80N 0 45W 90E 180W Fram Strait Bering Strait Alaska Lomonosov Ridge CB EB GIN Sea Arctic Ocean Bathymetry (NGDC ETOPO-2) Canada Russia

Arctic Ocean Circulation WHOI:

Temperature, February 250 m, PHC 3.0 Beaufort Gyre Signature Signature of Deep Convection in the Greenland Gyre

GDEM3, Salinity at 3000 m The deep Canadian Basin is saltier than the Eurasian Basin >34.95 <34.95

Analysis of ARCc 0.72° Run

HYCOM/CICEARCc 0.72˚ grid HYCOM/CICE ARCc 0.72˚ grid PHC 3.0 Near-Surface Temperature, February

Near-Surface Salinity, February HYCOM/CICEARCc 0.72˚ grid HYCOM/CICE ARCc 0.72˚ grid PHC 3.0

WHOI: Annual Mean Near-Surface Velocity Field North Atlantic Gyre does not seem to be reproduced in the model Beaufort Gyre is in place Transpolar Current is in place

250 m Fields from HYCOM/CICE ARCc 0.72˚ HYCOM/CICE ARCc 0.08˚

Temperature 250 m, February 2006 Atlantic water flow along the shelf break ARCc 0.72˚ grid PHC ARCc 0.08˚ grid

Salinity 250 m, February 2006 ARCc 0.72˚ grid PHC ARCc 0.08˚ grid

Depth of the Upper Atlantic Water (Depth of 0˚ Surface) Atlantic water flow along the shelf break 2006 ARCc 0.72˚ grid PHC ARCc 0.08˚ grid

Arctic Ocean – Greenland – Norwegian Seas cross-section HYCOM/CICE ARCc 0.72° 60N 80N 0 45W 90E 180W

GDEM 3 HYCOM/CICE ARCc 0.72˚ Salinity, February 0 45W

GDEM 3 HYCOM/CICE ARCc 0.72˚ Temperature, February

GDEM 3 HYCOM/CICE ARCc 0.08˚, 2006 Salinity, February

GDEM 3 HYCOM/CICE ARCc 0.08˚, 2006 Temperature, February

Summary Coupled HYCOM/CICE 4.0 in placeCoupled HYCOM/CICE 4.0 in place - ARCc0.72: ran for 4 years ( ) initialized using PHC 3.0 (ARCc0.72) - ARCc0.72: ran for 4 years ( ) initialized using PHC 3.0 (ARCc0.72) - ARCc0.08: ran for 4 years ( ) initialized using 1/12° Global HYCOM - ARCc0.08: ran for 4 years ( ) initialized using 1/12° Global HYCOM Surface and deep water mass distribution modeled in ARCc 0.72˚ (and 0.08˚) is similar to climatologySurface and deep water mass distribution modeled in ARCc 0.72˚ (and 0.08˚) is similar to climatology In both ARCc 0.72˚ and 0.08˚, the Atlantic layer in the Arctic Ocean is dislocated compared to observations:In both ARCc 0.72˚ and 0.08˚, the Atlantic layer in the Arctic Ocean is dislocated compared to observations: - Atlantic layer is too deep in ARCc 0.72˚ - Atlantic layer is too deep in ARCc 0.72˚ - Atlantic water does not penetrate into the Canadian Basin in ARCc 0.08˚ - Atlantic water does not penetrate into the Canadian Basin in ARCc 0.08˚

Sea Ice from ARCc 0.08˚,

Sea Ice Simulation from HYCOM/CICE ARCc 0.72°

Sea Ice Drift Field HYCOM/CICE ARCc0.72 grid, 2006 Proshutinsky et al.,

arctic.atmos.uiuc.edu/cryosphere Sea Ice Concentration, ARCc 0.72˚ September 1, 2006

Potential Temperature Salinity Aaagaard et al., Thermohaline circulation in the Arctic Mediterranean Seas, JGR, 1985 Distribution of potential T and S along the section

Seasonal Sea Ice Thickness (m) Winter Summer

Seasonal Sea Ice Concentration (m) Winter Summer

Salinity, 10 m, PHC 3.0 Anticyclonic Beaufort Gyre February August

Seasonal Signal Simulated in HYCOM/CICE ARCc 0.72°

Seasonal Near-Surface Temperature PHC 3.0 HYCOM/CICE ARCc0.72 grid, Winter Summer

Seasonal Near-Surface Salinity PHC 3.0 HYCOM/CICE ARCc0.72 grid, Winter Summer

1) Analysis of 0.72 and 0.08 model runs performed by NRL SSC 2) Test runs with ARCc0.72 3) Transition to ARCc0.08 4) AOMIP coordinated 50-year run of ARCc0.08 COAPS Plans

Two-way coupled HYCOM/CICE – exchanges fields every 3 hours HYCOM uses a 18 minute time step and exports:HYCOM uses a 18 minute time step and exports: - SST - SST - SSS - SSS - Surface currents - Surface currents CICE uses a 45 minute time step and exports:CICE uses a 45 minute time step and exports: - Ice concentration - Ice concentration - Ice-ocean stresses - Ice-ocean stresses - Actual Freeze/Melt Heat/Salt/Mass Flux - Actual Freeze/Melt Heat/Salt/Mass Flux - Solar radiation at ice base - Solar radiation at ice base ** Runs on three HPC systems: IBM p655+, SGI Origin 3900 and Cray XT3

Stand-alone vs Coupled Stand-alone - CICE has simple bulk ocean mixed layer Relaxes to climatological SST and SSS Calculates an ice-ocean stress, based on zero ocean currents - HYCOM treats sea-ice as an “energy bank” No ice advection No ice-ocean stress (wind stress applied directly to the ocean) Best possible coupling: - HYCOM’s ocean CICE’s sea-ice - Ice-Ocean Stress identical in HYCOM and CICE - Ice-Ocean Fluxes identical in HYCOM and CICE Actual 2-way coupling: - Ice-Ocean Stress identical in HYCOM and CICE - Similar, but not identical, Ice-Ocean Fluxes CICE’s SST strongly relaxed to HYCOM SST HYCOM’s sea-ice concentration strongly relaxed to CICE sea-ice concentration - Fields exchanged every 3 hours

Arctic dipole patch on standard Mercator globeArctic dipole patch on standard Mercator globe This tripole grid has many good propertiesThis tripole grid has many good properties - Rectilinear grid south of the Arctic patch - Rectilinear grid south of the Arctic patch - Grid aligned with the equator - Grid aligned with the equator - Same resolution in Arctic and Antarctic – if Arctic patch starts - Same resolution in Arctic and Antarctic – if Arctic patch starts about 47N about 47N - relatively smooth transition across the patch boundary - relatively smooth transition across the patch boundary The “full” tripole grid contains all locations twiceThe “full” tripole grid contains all locations twice - Just as a “full” periodic domain contains all locations an - Just as a “full” periodic domain contains all locations an infinite number of times infinite number of times Global: use the lower copy of each locationGlobal: use the lower copy of each location - Logically rectangular arrays - Logically rectangular arrays - Needs a special halo exchange on the top edge - Needs a special halo exchange on the top edge -- Includes a sign change for v-velocity -- Includes a sign change for v-velocity -- Some points still included twice (both copies must be -- Some points still included twice (both copies must be identical – consistency check) identical – consistency check) Global Tripole Grid

Zhang and Steele (JGR, 2007) POP model, 1978 HYCOM/CICE ARCc0.72 grid, 2006 Mean Horizontal Velocity Across Fram Strait |U|<0.2

GDEM3 PHC 3.0 Salinity, February 250 m

Temperature, 10 m, PHC 3.0 February August

Near-Surface Temperature, August HYCOM/CICEARCc 0.72˚ grid HYCOM/CICE ARCc 0.72˚ grid PHC 3.0

Near-Surface Salinity, August HYCOM/CICEARCc 0.72˚ grid HYCOM/CICE ARCc 0.72˚ grid PHC 3.0

Initial Field: Temperature at 250 m, January PHC 3.0 HYCOM/CICE ARCc 0.72 grid

Initial Depth of the Upper Atlantic Water (Depth of 0˚ Surface) PHC 3.0, June Initial Field, ARCc 0.72, June