hypoxia in the bottom water of the st. lawrence estuary: is this ecosystem on borrowed time?
DESCRIPTION
Hypoxia in the bottom water of the St. Lawrence Estuary: Is this ecosystem on borrowed time?. Stelly Lefort , Y. Gratton , A. Mucci , I. Dadou & D. Gilbert. McGill University & GEOTOP Department of Earth & Planetary Sciences. Problem. Hypoxic Systems Around the World. - PowerPoint PPT PresentationTRANSCRIPT
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Hypoxia in the bottom water of the St. Lawrence Estuary:
Is this ecosystem on borrowed time?
Stelly Lefort, Y. Gratton, A. Mucci, I. Dadou & D. Gilbert
McGill University & GEOTOPMcGill University & GEOTOP
Department of Earth & Planetary SciencesDepartment of Earth & Planetary Sciences
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Adapted from Diaz and Rosenberg (2008) and Falkowski et al. (2011)
PROBLEMPROBLEM
Hypoxic Systems Around the World
Hypoxic system [O2] < 60 µmol/kg ~ 62.5 mmol/m3
Oxygen concentrations (µmol/kg) at 200 m depth
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Near-bottom oxygen concentration in 2004-2005
Spatial distribution of dissolved oxygen concentration in the deep water
2524
2322
2120 19
18
17
16
Cabot
PROBLEMPROBLEM
Gilbert et al. (2007)
Hypoxia in the St. Lawrence System
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Density and dissolved oxygen concentration measured in July 2010 along the central axis of the Laurentian Channel
Density (kg m-3)
Oxygen (mmol m-3)
Seaward distance from STN 25 (km)
Dep
th (
m)
Dep
th (
m)
permanent pycnocline
ubottom
usurface
Hypoxia in the St. Lawrence System
LSLE Gulf of St. Lawrence
PROBLEMPROBLEM
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LSLE
Cabot
Gilbert et al. (2005)
In the LSLE At Cabot Strait
Hypoxic Waters
62.5 Severe hypoxia threshold
PROBLEMPROBLEM
Temporal changes in the source water properties
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Density and dissolved oxygen concentration measured in July 2010 along the central axis of the Laurentian Channel
Density (kg m-3)
Oxygen (mmol m-3)
Seaward distance from STN 25 (km)
Dep
th (
m)
Dep
th (
m)
Hypoxia in the St. Lawrence System
LSLE Gulf of St. Lawrence
PROBLEMPROBLEM
Explain the vertical distribution of O2
Identify the driving mechanisms of hypoxia
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PREVIOUS MODEL DESCRIPTIONPREVIOUS MODEL DESCRIPTION
Modified from Benoit et al. (2006)
A simple advective-diffusive conceptual model
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NEW MODEL DESCRIPTIONNEW MODEL DESCRIPTION
1. A realistic bathymetry: generation of an upward vertical advection2. A pelagic sink
Improvements of the simple advective-diffusive conceptual model
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MODEL OUTPUTSMODEL OUTPUTS
STN 25 Cabot
Observations
Respiration in sediments & water columnNew model
Previous model Flat bathymetry & Respiration in sediments only
Model Results & Observations
Adapted from Benoit et al. (2006)
Lefort et al. (accepted)
Climatology from 2002 to 2010
[O2 ] (m
mo
l m-3)
[O2 ] (m
mo
l m-3)
[O2 ] (m
mo
l m-3)
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DiffV > AdvH
u1
u2
u3
u1 < u2 < u3
IDENTIFYING THE DRIVING IDENTIFYING THE DRIVING MECHANISMSMECHANISMS
The oxygen minimum: A physical explanation
DiffV > AdvH
DiffV < AdvH
New model (1/2)
Previous model
New model (2/2)
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SUMMARY OF FINDINGSSUMMARY OF FINDINGS
• The oxygen minimum is mostly generated by physical processes as the oxygen tongue is induced by changes in bathymetry.
Which processes control the oxygen distribution in the deep waters and what are the causes of the persistent hypoxia
in the LSLE?
• Hypoxia in the LSLE results from a combination of physical and biogeochemical processes, but oxygen concentration is much more sensitive to variations in physical than biogeochemical processes.
• Water properties at the continental shelf edge in the North Atlantic Ocean are mostly responsible for the establishment of hypoxia in the LSLE.
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CONCLUSIONSCONCLUSIONS
Organic Carbon Flux Bottom Water TemperatureIncrease
& source water [O2] Decrease
Respiration Rate
Persistent and Severe Hypoxia
++
+
Is the St. Lawrence ecosystem on borrowed time?
Lefort S., Y. Gratton, A. Mucci, I. Dadou and D. Gilbert (accepted) Hypoxia in the Lower St. Lawrence Estuary: How physics controls spatial patterns, JGR-Oceans.