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Published byEmil Edwards Modified over 9 years ago
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Measuring the eastern boundary inflow to the Labrador Sea
Robert S. Pickart (WHOI) Outline 1. Insights on the overturning circulation of the Labrador Sea 2. Challenges associated with measuring the eastern boundary current 3. Strawman array design and remaining questions Greenland coast viewed from R/V Knorr , Oct 2008 (Photo by Ben Harden)
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Labrador Sea general circulation
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Wintertime storm tracks (from 45 years of ECMWF re-analysis data)
Mean storm track Våge et al. (2009)
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Heat loss from wintertime cold-air outbreaks
Ice Color = heat loss in Watts/m2 (from NCEP reanalysis)
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Heat loss from wintertime cold-air outbreaks
Ice Color = heat loss in Watts/m2 (from NCEP reanalysis) Contours = Absolute geostrophic pressure (Lavender et al. (2000)
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Surface eddy speed Color = surface eddy speed (cm/s)
Contours = Absolute geostrophic pressure (Lavender et al. (2000) After Lilly et al. (2003)
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Surface eddy speed and regions of deep convection
Color = surface eddy speed (cm/s) Contours = Absolute geostrophic pressure (Lavender et al. (2000)
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Surface eddy speed and regions of deep convection
Color = surface eddy speed (cm/s) Contours = Absolute geostrophic pressure (Lavender et al. (2000)
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Mixed-layer depth in winter 1997
Color = mixed layer depth (m) Contours = Absolute geostrophic pressure (Lavender et al. (2000)
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WOCE AR7W line Inverse calculation
Time period of high NAO in the early to mid 1990s
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Float data Mean circulation at 700m 1995–1999 AR7W
Lavendar et al. (2000)
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Referencing the geostrophic velocity section
Mean velocity at 700m from PALACE
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Referencing the geostrophic velocity section
Mean velocity at 700m from PALACE Mean temperature/density section X
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Referencing the geostrophic velocity section
Mean velocity at 700m from PALACE Mean temperature/density section X
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Referencing the geostrophic velocity section
Mean velocity at 700m from PALACE Total transport in: 35.4 Sv Total transport out: 35.5 Sv Mean temperature/density section X
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Absolute geostrophic velocity
AR7W
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Absolute geostrophic velocity
Throughput Overflow water transport = 12.4 Sv Recirculation transport = 2.5 Sv Total Boundary Current transport = 28.5 Sv
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Absolute geostrophic velocity
Near zero velocity! Throughput Overflow water transport = 12.4 Sv Recirculation transport = 2.5 Sv Total Boundary Current transport = 28.5 Sv
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Depth space: Overturning and horizontal components of the flow
Deviation Decompose the full velocity: Horizontal gyre Baroclinic gyre Then decompose the deviation velocity:
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Transport components Overturning Cell Horizontal cell
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Transport components 95% of sinking happens in boundary current
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Density space: Overturning transport
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Density space: Overturning transport
> 95% of the transport imbalance occurs in the boundary current
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What are the important points for OSNAP?
Seaward of the 700m isobath there is mass balance across the section (i.e. excluding the shallow shelf-edge flows). The horizontal cell is significantly larger than the overturning cell. Nearly all of the overturning, in depth space and density space, occurs along the rim of the basin. Flows in the middle of the Basin are weak. There is substantial mesoscale variability, so low-passing will be necessary.
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Ongoing Timeseries in the Labrador Sea
OSNAP-east moorings
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Ongoing Timeseries in the Labrador Sea
OSNAP-east moorings
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Considerations for OSNAP eastern boundary array
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Considerations for OSNAP eastern boundary array
1997 hydrographic Sections
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Two eastern boundary crossings in Feb 1997
North Salinity (color) overlain by density (contours) 26 Feb South
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Considerations for OSNAP eastern boundary array
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Considerations for OSNAP eastern boundary array
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Considerations for OSNAP eastern boundary array
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Considerations for OSNAP eastern boundary array
2001 hydrographic Section
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Eastern boundary crossing in Aug 2001
Salinity (color) overlain by density (contours) Absolute geostrophic velocity (color) overlain by density (contours)
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Eastern boundary crossing in Aug 2001
Salinity (color) overlain by density (contours) Absolute geostrophic velocity (color) overlain by density (contours)
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Eastern boundary crossing in Aug 2001
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Eastern boundary crossing in Aug 2001
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Considerations for OSNAP eastern boundary array
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Eastern boundary crossing in Aug 2001
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Eastern boundary crossing in Aug 2001
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Eastern boundary crossing in Aug 2001
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Eastern boundary crossing in Aug 2001
Use of current meters and Microcats is safer and allows for 2-year deployments
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Strawman OSNAP-West Boundary Arrays
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Remaining issues: shelf, near-surface, recirculation
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Remaining issues: shelf, near-surface, recirculation
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Considerations for OSNAP eastern boundary array
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Positive aspects of eastern array location
Bottom topography is gentle enough to effectively resolve the boundary current. Array will coincide with an altimeter line (providing additional surface velocity information). By moving south, the array is a true input boundary condition for the Labrador Sea (to compare to the western export array). The offshore recirculation is geographically confined, which means it can be effectively sampled with floats.
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Negative aspects of eastern array location
It is not the AR7W line! (which provides a wonderful context). Logistically more difficult to service the array. Closer to OSNAP Cape Farewell array (less contrast).
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