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Mesoscale eddies and shelf-basin exchange in the western Arctic Ocean
AOMIP Workshop WHOI Oct. 22, 2009 Mesoscale eddies and shelf-basin exchange in the western Arctic Ocean Eiji Watanabe International Arctic Research Center, Univ. of Alaska Fairbanks
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Pacific Water Transport
Introduction Pacific Water Transport Pacific water is predominant sources of heat, freshwater and nutrients Mesoscale Eddies Spall et al. (2008)
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Our Interest Introduction
When and Where are Beaufort shelfbreak eddies generated ? What controls generation period and place ? Are these elements interannually varing ? Satellite Model
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Beaufort Shelfbreak Eddies
Result Beaufort Shelfbreak Eddies Numerous eddy-like warm water cores appear along Beaufort shelf break MODIS 8-day-mean level-3 sea surface temperature [degC] Sep. 9, 2003 70 km Sea Ice Eddy-like warm cores Alaska Sep. 6-13, 2003
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Eddy Pair from Global Imager (GLI)
Result Eddy Pair from Global Imager (GLI) GLI Level 1B radiance (460, 545, 660 nm) Eddy Pair ? Sea Ice Beaufort shelfbreak Alaska Coastal Current Ocean Pt. Barrow Cloud Land Jul. 8, 2003
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Model Description Method
Coupled sea ice-ocean model : COCO (developed at Univ. of Tokyo) Sea ice part - momentum equation based on Mellor and Kantha (1989) - 0-layer thermodynamics (Semtner, 1976) / two thickness category - EVP rheology (Hunke and Duckowicz, 1997) Ocean part :COCO 3.4 (CCSR ocean component model version 3.4) - free surface general circulation model (OGCM) - UTOPIA/QUICKEST for trace advection (Leonard et al., 1994) - turbulent closure scheme (Noh and Kim, 1999) - Smagorinsky’s biharmonic viscosity (Griffies and Hallberg, 2000) - enstrophy preserving scheme (Ishizaki and Motoi, 1999) Model parameter (background value [m2/s] ) - horizontal viscosity : 5.0×10, horizontal diffusivity : 1.0 - vertical viscosity : 1.0×10-4, vertical diffusivity : (0.1 ~ 3.0)×10-4
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Experimental Design Method
Watanabe and Hasumi (2009, JPO) Model domain : Chukchi Sea and southern Canada Basin - horizontal resolution : about 2.5 km (eddies are explicitly resolved) - vertical level : (25L) [m] Boundary condition - NCEP/NCAR reanalysis daily data (wind, temperature, radiation etc.) - lateral : sponge for ocean open for sea ice - Pacific water inflow at Bering Strait Model bathymetry [m] Canada Basin Chukchi Sea Alaska Barrow Canyon Chukchi Plateau Bering Strait Initial condition - T, S : PHC in March - ocean circulation : static - sea ice : derived from NIC Integrated for 1 year from Mar to Feb
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Sea Ice and Sea Surface Temperature
Result Sea Ice and Sea Surface Temperature Sea ice area [ - ] and sea surface temperature [degC] AMSR-E & MODIS Sep. 6-13, 2003 CTL Sep. 22 Barrow Canyon Alaska Bering St. Warm water cores Sea Ice The model reproduces warm water cores along the Beaufort shelf break
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Pacific Water Pathway Result Eddy-induced transport Alaska Oct. 10 CTL
Pacific water content [m] Canada Basin Eddy-induced transport Herald Canyon Barrow Canyon Alaska Oct. 10 CTL Bering St. Eddy-induced transport of Pacific water seems to be dominant
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Beaufort Shelfbreak Eddies
Result Beaufort Shelfbreak Eddies Ocean velocity [cm s-1] and relative vorticity [s-1] (30 m depth) 50 km Barrow Canyon Oct. 10 CTL
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Beaufort Shelfbreak Eddies
Result Beaufort Shelfbreak Eddies Ocean velocity [cm s-1] and relative vorticity [s-1] (30 m depth) ED5 ED4 ED2 ED3 ED1 50 km Barrow Canyon Jet Jul. 22 CTL
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Beaufort Shelfbreak Eddies
Result Beaufort Shelfbreak Eddies Ocean velocity [cm s-1] and relative vorticity [s-1] (30 m depth) ED5 ED6 ED4 ED3 ED1 ED2 50 km Barrow Canyon Jet Aug. 6 CTL
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Beaufort Shelfbreak Eddies
Result Beaufort Shelfbreak Eddies Ocean velocity [cm s-1] and relative vorticity [s-1] (30 m depth) ED4 ED5 ED1 ED3 ED12 ED7 ED8 ED11 ED9 ED10 50 km Barrow Canyon Jet Sep. 15 CTL
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Variation of Relative Vorticity
Result Variation of Relative Vorticity Time series of relative vorticity field [s-1] (30 m depth) Continuous Two event Oct Type I Type III ED8 Sep ED9 ED11 ED12 ED13 ED7 Type II ED6 Aug ED2 ED3 ED4 ED5 Jul ED1 Barrow Canyon Simultaneous 160W 140W
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Type I Eddy Result Lateral shear of ocean velocity [s-1] (30 m depth)
Jet strength [m s-1] Rossby Number > O(0.1) ED6 ED3 ED1 ED2 24 Jet is frequently intensified throughout summer season Aug. 6 CTL Continuous generation of Type I eddy
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Background PV Condition
Result Background PV Condition Vertical structure of potential vorticity [109 m-1 s-1], relative vorticity [s-1] and potential density [kg m-3] ED3 CTL Jul. 12 Type II 26σ 27σ 28σ -0.1f [m] N ED9 Type III CTL Sep. 4 25σ 26σ 27σ 28σ -0.2 f N 30 km Generated from shelfbreak wall at mid-depth Generated from PV front in surface layer
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Beaufort Shelfbreak Jet
Result Beaufort Shelfbreak Jet Potential temperature [degC] and eastward velocity [cm s-1] [m] Type II Type III 30 10 20 Warm jet Cold jet 10 5 30 km Jul. 12 Sep. 4 N N CTL CTL Bottom-intensified cold jet Surface-intensified warm jet Shelfbreak jet is capable of producing eddies by baroclinic instability
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Nonlinear Evolution of Coastal Current
Discuss Nonlinear Evolution of Coastal Current Low PV water outflow from a strait could form anti-cyclonic eddies Kubokawa (1991) Bussol St. Yasuda et al. (2000) Shimada et al. (2001) Barrow Canyon
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Potential Vorticity Front
Result Potential Vorticity Front PV time series on both sides of shelfbreak [107 m-1 s-1] (0 - 30m) Type II Type III Barrow Canyon Sep. 4 Type III eddies are generated when the PV difference becomes maximum PVS << PVB PVS >> PVB Frontal wave influences Type III eddy generation ?
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Summary Summary Origin of Beaufort shelfbreak eddies and timing of their generation Type II Two event Jul Continuous Jul ~ Sep Type III Sep Type I Sea Ice Cover PV front ? Shelfbreak Jet Wind Barrow Canyon Jet Eddy Decay Process Interannual Variation Basin-scale Impact Future Work Coastal Current
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