Renellys C. Perez 12, Silvia L. Garzoli 2, Ricardo P. Matano 3, Christopher S. Meinen 2 1 UM/CIMAS, 2 NOAA/AOML, 3 OSU/COAS.

Slides:



Advertisements
Similar presentations
Open-ocean sustained time series observation sites run/co-run by NOAA/AOML Western Boundary Time Series: Florida Current transport (Meinen & Baringer)
Advertisements

Yoichi Ishikawa 1, Toshiyuki Awaji 1,2, Teiji In 3, Satoshi Nakada 2, Tsuyoshi Wakamatsu 1, Yoshimasa Hiyoshi 1, Yuji Sasaki 1 1 DrC, JAMSTEC 2 Kyoto University.
Preliminary results on Formation and variability of North Atlantic sea surface salinity maximum in a global GCM Tangdong Qu International Pacific Research.
Role of the Southern Ocean in controlling the Atlantic meridional overturning circulation Igor Kamenkovich RSMAS, University of Miami, Miami RSMAS, University.
C. A. Collins 1, R. Castro Valdez 2, A.S. Mascarenhas 2, and T. Margolina 1 Correspondence: Curtis A. Collins, Department of Oceanography, Naval Postgraduate.
Propagation of wave signals along the western boundary and their link to ocean overturning in the North Atlantic Vassil Roussenov 1, Ric Williams 1 Chris.
Propagation of wave signals in models and altimetry for the North Atlantic Vassil Roussenov 1, Chris Hughes 2, Ric Williams 1, David Marshall 3 and Mike.
1 of 27 Moored Current Observations from Nares Strait: Andreas Münchow College of Marine and Earth Studies University of Delaware Collaborators: Drs. Melling.
A monitoring design for the Atlantic meridional overturning circulation Joël Hirschi, Johanna Baehr, Jochem Marotzke, John Stark School of Earth and Ocean.
SAMOC: South Atlantic Meridional Overturning Circulation International Programs and Plans
Wave communication of high latitude forcing perturbations over the North Atlantic Vassil Roussenov, Ric Williams & Chris Hughes How changes in the high.
Define Current decreases exponentially with depth. At the same time, its direction changes clockwise with depth (The Ekman spiral). we have,. and At the.
Measurements in the Ocean Peter Challenor University of Exeter and National Oceanography Centre.
The meridional coherence of the North Atlantic meridional overturning circulation Rory Bingham Proudman Oceanographic Laboratory Coauthors: Chris Hughes,
“ New Ocean Circulation Patterns from Combined Drifter and Satellite Data ” Peter Niiler Scripps Institution of Oceanography with original material from.
Define Current decreases exponentially with depth and. At the same time, its direction changes clockwise with depth (The Ekman spiral). we have,. and At.
Two research cruises were successfully conducted in 2013 and Shipboard and moored observations show that: at first glance no significant decadal.
“ Combining Ocean Velocity Observations and Altimeter Data for OGCM Verification ” Peter Niiler Scripps Institution of Oceanography with original material.
Model LSW formation rate (2 yr averages) estimated from: (red) CFC-12 inventories, (black) mixed layer depth and (green) volume transport residual. Also.
1.Introduction 2.Description of model 3.Experimental design 4.Ocean ciruculation on an aquaplanet represented in the model depth latitude depth latitude.
Renellys C. Perez 12, Silvia L. Garzoli 2, Ricardo P. Matano 3, Christopher S. Meinen 2 1 UM/CIMAS, 2 NOAA/AOML, 3 OSU/COAS.
Western boundary circulation in the tropical South Atlantic and its relation to Tropical Atlantic Variability Rebecca Hummels 1, Peter Brandt 1, Marcus.
Deep circulation and meridional overturning Steve Rintoul and many others ….
Assuming 16 cm standard deviation. The final result – 5 of these records were noisy Halifax Grand Banks Line W 4100 m 2700 m 3250 m 2250 m 1800 m.
Sara Vieira Committee members: Dr. Peter Webster
OCEAN CURRENTS.
Impact of partial steps and momentum advection schemes in a global ocean circulation model at eddy-premitting resolution Barnier Bernard et al.
1DMS/USM, 2SERF, 3NRL/SSC, 4COAPS/FSU
Contribution Contribution to monitoring the cold water route is constructed along 3 axes: 1- monitoring transport of the Malvinas Current 2- documenting.
The Gent-McWilliams parameterization of ocean eddies in climate models Peter Gent National Center for Atmospheric Research.
Southern Ocean Surface Measurements and the Upper Ocean Heat Balance Janet Sprintall Sarah Gille Shenfu Dong Scripps Institution of Oceanography, UCSD.
NOAA/CPO Climate Observation Division 6th Annual System Review, September 3-5, 2008 AOML South Atlantic MOC related Observations and Plans Silvia L. Garzoli.
Antarctic Climate Response to Ozone Depletion in a Fine Resolution Ocean Climate Mode by Cecilia Bitz 1 and Lorenzo Polvani 2 1 Atmospheric Sciences, University.
Monitoring Heat Transport Changes using Expendable Bathythermographs Molly Baringer and Silvia Garzoli NOAA, AOML What are time/space scales of climate.
“Very high resolution global ocean and Arctic ocean-ice models being developed for climate study” by Albert Semtner Extremely high resolution is required.
National Oceanography Centre
Ventilation of the Equatorial Atlantic P. Brandt, R. J. Greatbatch, M. Claus, S.-H. Didwischus, J. Hahn GEOMAR Helmholtz Centre for Ocean Research Kiel.
MOC related activities at NOC Joël Hirschi, Elaine McDonagh, Brian King, Gerard McCarthy Stuart Cunningham, Harry Bryden, Adam Blaker SAMOC workshop, Rio.
North Atlantic dynamical response to high latitude perturbations in buoyancy forcing Vassil Roussenov, Ric Williams & Chris Hughes How changes in the high.
Measuring the South Atlantic MOC – in the OCCAM ocean model Povl AbrahamsenJoel Hirschi Emily ShuckburghElaine McDonagh Mike MeredithBob Marsh British.
A Synthetic Drifter Analysis of Upper-Limb Meridional Overturning Circulation Interior Ocean Pathways in the Tropical/Subtropical Atlantic George Halliwell,
Measuring the eastern boundary inflow to the Labrador Sea
Cross-Gyre Thermohaline Transport in the Tropical Atlantic: The role of NBC Rings Bill Johns Zulema Garraffo Division of Meteorology and Physical Oceanography.
South Atlantic deep water circulation Stramma & England 1999.
Western boundary circulation in the tropical South Atlantic and its relation to Tropical Atlantic Variability Rebecca Hummels1, Peter Brandt1, Marcus Dengler1,
The relationship between sea level and bottom pressure in an eddy permitting ocean model Rory Bingham and Chris Hughes Proudman Oceanographic Laboratory.
On the effect of the Greenland Scotland Ridge on the dense water formation in the Nordic Seas Dorotea Iovino NoClim/ProClim meeting 4-6 September 2006.
Propagation of wave signals along the western boundary and their link to ocean overturning in the North Atlantic Vassil Roussenov 1, Ric Williams 1 Chris.
Mesoscale eddies and deep upwelling in the Southern Ocean
Forces and accelerations in a fluid: (a) acceleration, (b) advection, (c) pressure gradient force, (d) gravity, and (e) acceleration associated with viscosity.
Sharing the results of high- resolution ocean general circulation model under a multi-discipline frame work-a review of OFES activities Yukio Masumoto.
Seasonal Variations of MOC in the South Atlantic from Observations and Numerical Models Shenfu Dong CIMAS, University of Miami, and NOAA/AOML Coauthors:
Gent-McWilliams parameterization: 20/20 Hindsight Peter R. Gent Senior Scientist National Center for Atmospheric Research.
I. Objectives and Methodology DETERMINATION OF CIRCULATION IN NORTH ATLANTIC BY INVERSION OF ARGO FLOAT DATA Carole GRIT, Herlé Mercier The methodology.
RTOFS Monitoring and Evaluation Metrics Avichal Mehra MMAB/EMC/NCEP/NWS.
Intraseasonal to interannual variability of the Brazil Current transport measured at 34.5°S M. P. Chidichimo* 1, A. R. Piola 1, C. S. Meinen 3, E. Campos.
Wind-driven halocline variability in the western Arctic Ocean
Define and we have • At the sea surface (z=0), the surface current flows at 45o to the right of the wind direction Depends on constant Az => • Current.
Define and we have • At the sea surface (z=0), the surface current flows at 45o to the right of the wind direction Depends on constant Az => • Current.
Define and we have • At the sea surface (z=0), the surface current flows at 45o to the right of the wind direction Depends on constant Az => • Current.
A Comparison of Profiling Float and XBT Representations of Upper Layer Temperature Structure of the Northwestern Subtropical North Atlantic Robert L.
OCEAN RESPONSE TO AIR-SEA FLUXES Oceanic and atmospheric mixed
The relationship between MVT & MHT of AMOC:
Shelf-basin exchange in the Western Arctic Ocean
Deep Western Boundary Current
Y. Xue1, C. Wen1, X. Yang2 , D. Behringer1, A. Kumar1,
Characteristics of mesoscale eddies in the Southwest Pacific
The Role of Inter-ocean Exchanges on Long-term Variability of the Northward Heat Transport in the South Atlantic Shenfu Dong CIMAS/UM and NOAA/AOML S.
by M. A. Srokosz, and H. L. Bryden
CURRENT Energy Budget Changes
Presentation transcript:

Renellys C. Perez 12, Silvia L. Garzoli 2, Ricardo P. Matano 3, Christopher S. Meinen 2 1 UM/CIMAS, 2 NOAA/AOML, 3 OSU/COAS

South Atlantic MOC (SAM) array Deployed 3 PIES/1 CPIES in March 2009 Figure from SAM Cruise report (Chief Scientist: Chris Meinen) PIES (CPIES) = inverted echo sounder with bottom pressure sensor (and current meter) As part of BONUS-GOODHOPE project 2 CPIES were deployed near South African coast in February 2008 (Chief Scientist: Sabrina Speich)

Existing observations in the South Atlantic To better resolve the western boundary currents along the northern boundary of the SAMOC box, a pilot array was started along 34.5°S Infrastructure considerations largely determined the latitude Figure obtained from

Questions: What do Observing System Experiments (OSEs) tell us about where a MOC monitoring array should be located? Can a PIES/CPIES array be used to monitor the MOC? Can the SAM and Bonus-Goodhope arrays be incorporated into a MOC monitoring array?

Motivation There is only one quasi-comprehensive MOC monitoring system in North Atlantic: the RAPID/MOCHA array at 26.5°N (Cunningham et al. 2007; Kanzow et al. 2007) Given global extent of the MOC, it is important to take into account changes in other basins Otherwise, we cannot determine the causality of changes observed by the RAPID/MOCHA array Heat and salt fluxes from the SA to NA are important for North Atlantic Deep Water (NADW) formation From XBT measurements we know that there is strong connection between the MOC and heat transport in the SA (Dong et al. 2009) Garzoli and Matano 2010

Observed connection between NHT and MOC Signals are positively correlated (r=0.76) 1 Sv increase in MOC = 0.05 ± 0.01 PW increase in NHT Dong et al. 2009

Array development Deploy virtual arrays into two high-resolution ocean models Evaluate the ability of the arrays to reproduce the MOC and NHT Perfect array of T, S profiles Perfect array of CPIES* SAM array + Bonus-Goodhope array (+ additional) At each time step, velocity estimated as v g + v b + v e + v c Velocity adjusted by v c to give zero net volume transport MOC(t) = maximum northward volume transport at each time step (integrate from velocity surface to ~1000 m) Focus on five latitudes: 15°S, 20°S, 25°S, 30°S, 34.5°S * IES travel times are combined with model T, S to produce time series of dynamic height and geostrophic velocity (similar to Gravest Empirical Mode methodology, e.g., Meinen et al. 2006)

Models POCM: Parallel Ocean Circulation Model (Tokmakian and Challenor 1999) Bryan (1969) primitive equation, hydrostatic, z-level model ECMWF/ERA40 reanalysis fluxes Horizontal resolution is 0.4° longitude x 1/4° latitude* 20 z-levels OFES: OGCM For the Earth Simulator (JAMSTEC) Based on MOM3 NCEP/NCAR reanalysis fluxes Horizontal resolution is 0.1° longitude x 0.1° latitude 54 z-levels

Models POCM 1 Well studied, but has coarser resolution and older numerics Successfully simulates vertically integrated flow and diapycnal overturning in Southern Ocean, low-frequency variability of ACC and Malvinas Current Does not reproduce correct location of Malvinas Confluence nor Zapiola Eddy, only sheds 2 Agulhas rings/year, overestimates ACC transport through Drake Passage OFES 2 High resolution and advanced numerics, but needs further validation Reproduces large scale SSHA variability in Southern Ocean Underestimates increasing tendency of SSHA in South Atlantic, Agulhas rings propagate too far north 1 Matano & Beier (2003),Schouten & Matano (2006),Baringer & Garzoli (2007),Fetter & Matano (2008) 2 Sasaki et al. (2007), Giarolla & Matano (Ocean Sciences 2010)

MOC computed using perfect v array “Truth” Black = OFES Blue = POCM Left: MOC time series Right: Mean vertical structure

MOC computed using perfect v array “Truth” Lumpkin and Speer (2007) 11°S 16.2 ± 3.0 Sv 32°S 12.4 ± 2.6 Sv Dong et al. (2009) 35°S 17.9 ± 2.2 Sv

High correlation, but zonal structure different Black = OFES Blue = POCM Left: Mean Right: Standard Deviation

NHT computed using perfect v array “Truth” Correlation between NHT and MOC exceeds 0.85 for all latitudes and both models (consistent with Dong et al. 2009)

Can a perfect T,S or CPIES array reconstruct the MOC in OFES? Black = “Truth” array Blue = Perfect T,S array Red = Perfect CPIES array Left: MOC time series Right: Mean vertical structure

Can a perfect T,S or CPIES array reconstruct the MOC in OFES? Less than 0.4 Sv bias at all latitudes High RMSE at 15°S Perfect T, S: high correlation at all latitudes Perfect CPIES: high correlation at 20°S, 30°S, 35°S

Can a perfect T,S or CPIES array reconstruct the MOC in POCM? Black = “Truth” array Blue = Perfect T,S array Red = Perfect CPIES array Left: MOC time series Right: Mean vertical structure

Can a perfect T,S or CPIES array reconstruct the MOC in POCM? Bias exceeds 1 Sv at low latitudes High RMSE at low latitudes Perfect T, S: high correlation at all latitudes Perfect CPIES: high correlation at 25°S, 30°S, 35°S

Summary of perfect arrays In general, better reconstructions are achieved in OFES compared with POCM at higher latitudes compared with lower latitudes with a perfect T, S array compared with a perfect CPIES array for volume transport (MOC) compared with heat transport (NHT) Recommendation: higher latitudes (25°S to 35°S) better for placement of the SAMOC array, especially if array consists of PIES/CPIES

What happens if we degrade the array at 34.5°S in OFES? Color contours: Mean v White contours: Std v

What happens if we degrade the array at 34.5°S in OFES? Color contours: Mean v White contours: Std v

What happens if we degrade the array at 34.5°S in OFES? Color contours: Mean v White contours: Std v

What happens if we degrade the array at 34.5°S in OFES? Color contours: Mean v White contours: Std v

What happens if we degrade the array at 34.5°S in OFES? Color contours: Mean v White contours: Std v

What happens if we degrade the array at 34.5°S in POCM? Color contours: Mean v White contours: Std v

OFES 34.5°SPOCM 34.5°S in OFES? Blue = Degraded T,S array Red = Degraded CPIES array

What happens if we degrade the array at 30°S in OFES? Color contours: Mean v White contours: Std v

What happens if we degrade the array at 30°S in POCM? Color contours: Mean v White contours: Std v

OFES 30°SPOCM 30°S Blue = Degraded T,S array Red = Degraded CPIES array

Why do less instruments do a better job? Large meso-scale variability east of Walvis Ridge poorly represented by a handful of moorings [Need to filter out meso-scale variability] MOC is strongly correlated with Ekman transport at high latitudes POCM: 0.66 at 25°S, 0.75 at 30°S, 0.85 at 35°S OFES: 0.51 at 25°S, 0.82 at 30°S, 0.88 at 35°S RAPID/MOCHA array correlation is ~0.6* Questions: Can altimetric data be used to resolve regions of large meso-scale variability and set geographic limits for a SAMOC array? How many moorings are needed to reconstruct heat and salt transport by Agulhas rings? * RAPID/MOCHA data obtained from

Summary of degraded arrays For reconstructions of the MOC, it is important to have interior measurements Present arrays + 2 interior points perform surprisingly well Energetic Agulhas eddy region must be treated carefully Degraded CPIES array and T, S array are comparable for MOC reconstructions Need ~15 measurements to reproduce mean vertical structure of the MOC and have low biases in the OFES model Degrading the array is less successful in the POCM model

Can a perfect T,S or CPIES array reconstruct the NHT in OFES? Black = “Truth” array Blue = Perfect T,S array Red = Perfect CPIES array plus mean T,S relationship Left: NHT time series Right: Mean vertical structure

Can a perfect T,S or CPIES array reconstruct the NHT in OFES? Less than 0.07 PW bias at all latitudes High RMSE at 15°S Perfect T, S: high correlation at all latitudes Perfect CPIES: modest correlation 20°S, 30°S, 35°S

Can a perfect T,S or CPIES array reconstruct the NHT in POCM? Black = “Truth” array Blue = Perfect T,S array Red = Perfect CPIES array plus mean T,S relationship Left: NHT time series Right: Mean vertical structure

Can a perfect T,S or CPIES array reconstruct the NHT in POCM? Large biases at 20°S, 25°S, 30°S High RMSE at 20°S, 30°S Perfect T, S: high correlation at all latitudes Perfect CPIES: modest correlation 25°S, 35°S

OFES 34.5°S longer term trend

Example of v g reconstruction: OFES 34.5°S

Agulhas rings go to far north in the OFES Giarolla & Matano (Ocean Sciences 2010)