Oxygen variability in the eastern tropical North Atlantic oxygen minimum zone
Peter Brandt
with contributions from
Johannes Hahn, Florian Schütte, Tim Fischer, Johannes Karstensen,
Richard J. Greatbatch, Marcus Dengler, Arne Körtzinger, Gerd Krahmann,
Sunke Schmidtko, Lothar Stramma, Toste Tanhua, and Martin Visbeck
T,S,v N,P,Fe
O2
SFB754
tOxygen Depletion in the North Atlantic OMZ
Oxygen data show a reduction of dissolved oxygen in the North Atlantic OMZ over the last 40 years.
Stramma et al. 2008
mmol/kg
Motivation
Habitat Reduction for Pelagic Fishes
Stramma et al. 2011
Motivation
Global Model Simulations
Oschlies, pers. comm.
Annual mean oxygen [μmol/kg] at 300m in observations (WOA) and different state-of-the-art global models
Motivation
Stramma et al. 2013
Mismatch between Observed and Modeled Trends
Pattern correlation between simulated (upper right) and observed (bottom) patterns of past oxygen change over the last 50 yr is negative
Oxygen (left,
μmol/kg) and oxygen trend (right, μmol/kg/yr) at 300m.
Motivation
Outline
Structure of the
Eastern Tropical North Atlantic (ETNA) Oxygen Minimum Zone (OMZ)
• Mean structure
• Shallow OMZ
• Equatorial oxygen maximum
Oxygen Budget
• Consumption
• Diapycnal mixing
• Lateral mixing
• Advection
Long-term Oxygen Changes
Summary
Ventilated Thermocline
Transport processes at the boundary between ventilated and
unventilated thermocline:
advection (solid arrow) and diffusive flux (open
arrow) Luyten et al. 1983
FLAME simulation, C. Eden
Simulation of OMZs involve physical
processes from large to small scales: circulation, jets, eddies, filaments, turbulent mixing.
Structure of the ETNA OMZ: Mean Structure
Oxygen Distribution at 600m [ccm/l]
Left: From METEOR expedition 1925/27
(Wattenberg 1939)
Right: From WOA’09 (same style, courtesy Florian Schütte)
Note, oxygen maximum at the equator
Wattenberg 1939 WOA‘09
Structure of the ETNA OMZ: Mean Structure
Mean Circulation and Oxygen Distribution
Complex zonal current system connects high-oxygen western boundary regime with sluggish flow in the eastern basin.
Brandt et al. 2015
Structure of the ETNA OMZ: Mean Structure
Measurement Programme
Repeat ship section along 23°W; moored observations;
microstructure measurements; 2 tracer release experiments
Brandt et al. 2015
Structure of the ETNA OMZ: Mean Structure
Mean 23°W Section
Equatorial oxygen maximum Deep
oxycline at about 300m or sq=26.8 kg/m3
OMZ is ventilated from the west by zonal currents
Structure of the ETNA OMZ: Mean Structure
Oxygen at Deep Oxygen Minimum
Deep OMZ (below 200m) located in the interior with slightly enhanced oxygen
concentration
toward the eastern boundary
Structure of the ETNA OMZ: Mean Structure
From shipboard CTD/O2 profiles taken during more than 30 research cruises
Oxygen at Shallow Oxygen Minimum
Shallow OMZ
(above 200m) close to the eastern
boundary upwelling region
Single low oxygen events also in the region of the deep OMZ
Structure of the ETNA OMZ: Mean Structure
Mean 18°N Section
More More SACW
NACW
Shallow OMZ
Structure of the ETNA OMZ: Shallow OMZc
Oxygen at CVOO Mooring
Oxygen at 40-60m (black), 140m (grey) and
oxygen saturation (red) Karstensen et al., 2015
Structure of the ETNA OMZ: Shallow OMZc
CVOO
Passage of a Mode-Water Eddy at the CVOO Mooring
Low oxygen zones present just below the mixed-layer of a high productive anticyclonic modewater eddies (oxygen at 42m and 170m, salinity, meridional velocity [m/s])
Karstensen et al., 2015
Structure of the ETNA OMZ: Shallow OMZc
Low Oxygen Eddies Identified in Available Hydrographic Data
Schütte et al., 2016 Anticyclonic
modewater eddies
(ACME) Cyclonic eddies
Eddy tracking using SLA data
Mean Surface Signatures
Structure of the ETNA OMZ: Shallow OMZc
Mean Vertical Structure
Structure of the ETNA OMZ: Shallow OMZc
Obtained from oxygen anomaly profiles, i.e. difference between profiles inside and outside of an eddy.
Summary: Shallow OMZ
Inside of cyclones and ACMEs very low oxygen environment are found just below the mixed layer
Eddy cores are well-isolated, i.e., hydrographically constant, while respiration is elevated and
reduces oxygen during westward eddy migration
Locally increased consumption (aOUR) within these eddies represents an
essential part of the total consumption and is partly responsible for the
formation of the shallow oxygen minimum zone
Schütte et al., 2016; and Biogeosciences special issue on Hydrography, biogeochemistry, and biology of
"dead-zone eddies" in the eastern tropical North Atlantic aOUR (µmol kg-1 y-1)
-15 -10 -5 0
Depth (m)
0 50 100 150 200 250 300 350 400 450 500
ACME Cyclone Total
Consumption after Kartsensen et al. 2008
Structure of the ETNA OMZ: Shallow OMZc
Equatorial oxygen and velocity distribution
Why there is on oxygen maximum at the equator?
Why it is largely missing in global Earth System Models?
Oschlies, pers. comm.
Structure of the ETNA OMZ: Equatorial oxygen maximum
Zonal Velocity in the Equatorial Atlantic at 23°W
Equatorial Deep Jets are a dominant flow feature below the Equatorial Undercurrent and oscillate with a period of about 4.5 years
Downward phase and
upward energy propagation
Structure of the ETNA OMZ: Equatorial oxygen maximum
Shipboard mean and
moored time series
Energy of Zonal Flow at 23°W:
Basin Mode Oscillations
Most of the energy is concentrated on only three frequencies
All peaks are associated with resonant linear equatorial basin modes
Black line: basin mode characteristic
from PhD thesis, M. Claus, 2016
25 Cane and Moore (1981)
described low-
frequency standing equatorial modes
composed of equatorial Kelvin and long Rossby waves
T = 4 L
c
gwEquatorial Basin Mode
Greatbatch et al.
(2012) used a reduced- gravity model to
simulate regular high- baroclinic-mode
oscillations with a period of 4.5 years
Width of the EDJs could be correctly
simulated by including lateral eddy viscosity of about 200-300m2/s
Structure of the ETNA OMZ: Equatorial oxygen maximum
Greatbatch et al. 2012
Advection-Diffusion Model
Model is forced by the velocity field of basin mode of EDJs
It includes a restoring to western boundary oxygen concentrations within a boundary layer and oxygen consumption (van Geen et al.
2006)
Simulation are performed until a constantly oscillating state is reached (about 160 yr)
Mean relative oxygen shows ventilation of the equatorial band due to basin mode oscillations
Equator
Structure of the ETNA OMZ: Equatorial oxygen maximum
Brandt et al. 2012
Reduced-Gravity Model with EDJ and Mean Advection
a) Mean zonal flow field, i.e.
latitudinally
alternating zonal jets
b) Mean oxygen distribution
c) Oxygen anomaly along 23°W
d) Mean Oxygen along the equator
Structure of the ETNA OMZ: Equatorial oxygen maximum
Summary: Equatorial Atlantic Ventilation
Equatorial Deep Jets and the mean eastward flow at 2°N/S with westward flow in between results in
strong mixing between western boundary regime and eastern equatorial Atlantic producing the equatorial oxygen maximum
High-resolution models with better representation of equatorial circulation allow simulation of more
realistic oxygen distribution (e.g. Duteil et al. 2014)
Structure of the ETNA OMZ: Equatorial oxygen maximum
Oxygen Budget of the ETNA OMZ
Oxygen tendency
Oxygen sink
• Heterotrophic respiration
Oxygen source or sink:
• Diapycnal mixing
• Meridional eddy fluxes
• Advection by latitudinally alternating zonal jets
Oxygen Budget
¶O
2¶t = -C z ( ) + K
r¶
2O
2¶z
2+ K
y¶
2O
2¶y
2- u ¶O
2¶x + ...
Respiration Estimates
AOUR: apparent oxygen utilization rate
Derived as the ratio of AOU and CFC11 ages (data from the subtropics)
Exponential decay of AOUR downward is assumed
Karstensen et al. 2008
Oxygen Budget: Consumption
OUR from Different Tracer-Based Age Concepts
Mean age from the transit time distribution (TTD) is calculated by D/G=1, with D the width and G the mean age of the TTD
„classical“ tracer age is with D/G=0
Problems: very old water masses, mixing of different water masses
Large uncertainty
Mean age (TTD)
Mean age (TTD)
“classical”
tracer age
“classical”
tracer age
Oxygen Budget: Consumption
Diapycnal Mixing
Microstructure measurements yield a diapycnal diffusivity, K, that is relatively
constant with
depth in the depth range of the OMZ
Fischer et al. 2013
Oxygen Budget: Diapycnal Mixing
Tracer Release Experiment
Diapycnal and lateral mixing estimated from tracer spreading:
Kr = (1.19±0.18) x 10-5 m2 s-1
Kx = 1200±600 m2 s-1, Ky = 500±200 m2 s-1
Banyte et al. 2012, 2013
Oxygen Budget: Diapycnal Mixing
Hahn et al. 2014
Meridional Eddy Fluxes
Two Methods
Eddy correlation method applied to moored observations of oxygen and meridional velocity (here at 5°N,
23°W)
Flux gradient parameterization based on repeat ship sections
Oxygen Budget: Lateral Mixing
FO
2 = v'O2 '
dy K dO
F = - e 2
Mean Eddy Diffusivity Profile K
eBrandt et al. (2010)
NATRE: Ferrari and Polzin (2005)
GUTRE: Banyte et al. (2013) TNEA: Hahn et al. (2014)
Oxygen Budget: Lateral Mixing
Eddy Flux Divergence
Oxygen supply due to
meridional eddy flux
Hahn et al. 2014
Meridional eddy diffusivity
Oxygen Budget: Lateral Mixing
Oxygen Budget of the ETNA OMZ
Hahn et al. 2014
Oxygen Budget
Mean 23°W Section
Equatorial oxygen maximum Deep
oxycline at about 300m or sq=26.8 kg/m3
OMZ is ventilated from the west by zonal currents
Structure of the ETNA OMZ: Mean Structure
Oxygen Depletion in the North
Atlantic OMZ = Climate Change?
Oxygen data show a reduction of dissolved oxygen in the North Atlantic OMZ over the last 40 years.
Stramma et al. 2008
mmol/kg
Long-term Oxygen Changes
Ocean Deoxygenation
Increased stratification and a corresponding reduction of ventilation, or solubility changes associated with a warming of subducted water masses (Bopp et al. 2002; Matear and Hirst 2003)
Increase in heterotrophic respiration along the pathways of ventilating water masses due to excess organic carbon
formed at higher CO2 levels (Oschlies et al. 2008)
Simulated global O2 changes in response to external forcing (90% confidence), but Atlantic O2 changes undistinguishable from internal variability (Andrews et al. 2013)
Observations indicate circulation changes:
e.g. weakening of zonal jets (Brandt et al. 2010)
Long-term Oxygen Changes
150-300m, 9-15°N, 20-26°W
350-700m, 9-15°N, 20-26°W
Oxygen Budget with Trends
Long-term Oxygen Changes
Hahn et al. 2016, in preparation
Decadal Water Mass Changes
Salinity increase (more high-saline NAW)
associated with oxygen decrease and vice versa
Oxygen Trend 2006-2014
Hahn et al. 2016, in preparation
Salinity Trend 2006-2014
Summary
Advection dominates ventilation in the upper 300m
Deoxygenation associated with anthropogenic
climate change might not be the dominant signal on regional scale
Strong decadal
oxygen changes likely associated with
circulation variability
Exact mechanisms are still unknown
Trend 2006-2014
Hahn et al. 2016, in preparation
Acknowledgements
This study was supported by the German Science Foundation (DFG) as part of the
Sonderforschungsbereich 754 “Climate-
Biogeochemistry Interactions in the Tropical Ocean” , by the German Federal Ministry of
Education and Research as part of the co-operative projects “NORDATLANTIK”, “RACE”, “SOPRAN”, and “AWA” as well as by the Cluster of Excellence
“The Future Ocean”