Mixed layer heat and freshwater budgets: Improvements during TACE Rebecca Hummels 1, Marcus Dengler 1, Peter Brandt 1, Michael Schlundt 1 1 GEOMAR Helmholtz.

Slides:



Advertisements
Similar presentations
1 ICES/NAFO Symposium Santander May Seasonal to interannual variability of temperature and salinity in the Nordic Seas: heat and freshwater budgets.
Advertisements

Preliminary results on Formation and variability of North Atlantic sea surface salinity maximum in a global GCM Tangdong Qu International Pacific Research.
About the contribution of the diapycnal heat flux to the heat budget of the mixed layer Rebecca Hummels 1, Marcus Dengler 1, Bernard Bourles 2 1 GEOMAR.
Published in 2007 Cited 15 times Keywords: North Pacific, PDO-related air forcing, Eddy permitting model, Model heat/SST budget analysis.
Maria Valdivieso Department of Meteorology, University of Reading, UK ▶ Focus on surface heat fluxes ▶ Timeseries comparison at buoy sites
Equatorial Atlantic Circulation and Tropical Climate Variability
Semyon A. Grodsky and James A. Carton, University of Maryland, College Park, MD The PIRATA (PIlot Research Array moored in the Tropical Atlantic) project.
Salinity Structure of the Indian Ocean Dipole: Perspectives from Aquarius and SMOS satellite missions Ebenezer Nyadjro NOAA PMEL Seattle, WA Bulusu Subrahmanyam.
Section 3.4 Introduction to the West African Monsoon.
Thermohaline Circulation
Yukio Masumoto (RIGC, JAMSTEC). Outline  Indian Ocean Observing System - Background and present status  Examples of key phenomena observed by IndOOS.
LOW FREQUENCY VARIATION OF SEA SURFACE SALINITY IN THE TROPICAL ATLANTIC Semyon A. Grodsky 1, James A. Carton 1, and Frederick M. Bingham 2 1 Department.
Evaporative heat flux (Q e ) 51% of the heat input into the ocean is used for evaporation. Evaporation starts when the air over the ocean is unsaturated.
Potential temperature ( o C, Levitus 1994) Surface Global zonal mean.
Graduate Course: Advanced Remote Sensing Data Analysis and Application SURFACE HEAT BUDGETS IN THE PACIFIC WARM POOL DURING TOGA COARE Shu-Hsien Chou Dept.
SHNHCEF EI ind c-5.3±0.24.5±0.1−0.8±0.1 EI dir c-5.4±0.24.8± ±0.2 E40 ind c−5.7±0.34.9±0.3−0.9±0.2 E40 dir c-4.9±0.64.7± ±0.2 FT08−4.9±0.25.1±0.5-
The Caribbean Low Level Jet variability during August and September and its relation with the regional hydroclimate Ernesto Muñoz.
Evaporative heat flux (Q e ) 51% of the heat input into the ocean is used for evaporation. Evaporation starts when the air over the ocean is unsaturated.
Two research cruises were successfully conducted in 2013 and Shipboard and moored observations show that: at first glance no significant decadal.
Mode (Eighteen Degree) Water V.Y. Chow EPS Dec 2005.
Western boundary circulation in the tropical South Atlantic and its relation to Tropical Atlantic Variability Rebecca Hummels 1, Peter Brandt 1, Marcus.
Ventilation of the Equatorial Atlantic P. Brandt, R. J. Greatbatch, M. Claus, S.-H. Didwischus, J. Hahn GEOMAR Helmholtz Centre for Ocean Research Kiel.
Sara Vieira Committee members: Dr. Peter Webster
Estimating Diffusivity from the Mixed Layer Heat and Salt Balances Meghan F Cronin 1, et al. 1 NOAA Pacific Marine Environmental Laboratory 4 April 2013.
EFFECTS OF OCEAN MIXING ON HURRICANE HEAT CONTENT ESTIMATES: A NUMERICAL STUDY S. DANIEL JACOB and LYNN K. SHAY Meteorology and Physical Oceanography Rosenstiel.
Clivar - Pune The Vasco-Cirene experiment J.Ph. Duvel J. Vialard and R. Molcard J.Ph. Duvel J. Vialard and R. Molcard LMD-ENS Paris, France LODYC, UPMC,
Equatorial Circulation and Tropical Atlantic Variability during the Tropical Atlantic Climate Experiment Peter Brandt 1, Andreas Funk 2, Alexis Tantet.
Southern Ocean Surface Measurements and the Upper Ocean Heat Balance Janet Sprintall Sarah Gille Shenfu Dong Scripps Institution of Oceanography, UCSD.
Mixing on the Western Antarctic Peninsula Shelf: A Component of Southern Ocean GLOBEC Susan L. Howard, Laurence Padman, Earth and Space Research and Jason.
The Linear and Non-linear Evolution Mechanism of Mesoscale Vortex Disturbances in Winter Over Western Japan Sea Yasumitsu MAEJIMA and Keita IGA (Ocean.
Western boundary circulation and the role of deep eddies in the tropical South Atlantic Overview Western Boundary Circulation (Schott et al. 2004) - shipboard.
Eastern WP Gap winds April 2013 Dec 2013 SST warmest coldest Local gap wind effect Regional conditions, comments by Gordon and Sprintall SST 6 April 2014.
Annual and semi-annual variations of equatorial Atlantic circulation associated with basin mode resonance Peter Brandt 1, Martin Claus 1, Richard J. Greatbatch.
Ventilation of the Equatorial Atlantic P. Brandt, R. J. Greatbatch, M. Claus, S.-H. Didwischus, J. Hahn GEOMAR Helmholtz Centre for Ocean Research Kiel.
An evaluation of satellite derived air-sea fluxes through use in ocean general circulation model Vijay K Agarwal, Rashmi Sharma, Neeraj Agarwal Meteorology.
Investigation of Mixed Layer Depth in the Southern Ocean by using a 1-D mixed layer model Chin-Ying Chien & Kevin Speer Geophysical Fluid Dynamics Institute,
Typical Distributions of Water Characteristics in the Oceans.
Mixed Layer Ocean Model: Model Physics and Climate
1 Marginal Thermobaric Stability in the Weddell Sea Miles McPhee McPhee Research Company.
TOGA Pan-Pacific Surface Current Study NOAA Atlantic Oceanographic and Meteorological Laboratory (AOML) April 1988 Miami, Florida.
Oceanic mixed layer heat budget in the Eastern Equatorial Atlantic using ARGO floats and PIRATA buoys M. Wade (1,2,3), G. Caniaux (1) and Y. du Penhoat.
Ocean Surface heat fluxes
Contributions to SST Anomalies in the Atlantic Ocean [Ocean Control of Air-Sea Heat Fluxes] Kathie Kelly Suzanne Dickinson and LuAnne Thompson University.
An evaluation of a hybrid satellite and NWP- based turbulent fluxes with TAO buoys ChuanLi Jiang, Kathryn A. Kelly, and LuAnne Thompson University of Washington.
The CHIME coupled climate model Alex Megann, SOC 26 January 2005 (with Adrian New, Bablu Sinha, SOC; Shan Sun, NASA GISS; Rainer Bleck, LANL)  Introduction.
Estimating Vertical Eddy Viscosity in the Pacific Equatorial Undercurrent Natalia Stefanova Masters Thesis Defense October 31, 2008 UW School of Oceanography.
Western boundary circulation in the tropical South Atlantic and its relation to Tropical Atlantic Variability Rebecca Hummels1, Peter Brandt1, Marcus Dengler1,
By S.-K. Lee (CIMAS/UM), D. Enfield (AOML/NOAA), C. Wang (AOML/NOAA), and G. Halliwell Jr. (RSMAS/UM) Objectives: (1)To assess the appropriateness of commonly.
Air-Sea Fluxes: A New Approach for Validation and Estimation Huai-Min Zhang NOAA/NESDIS/NCDC/ScSD John M. Toole and Michael J. Caruso Woods Hole Oceanographic.
Combining Altimeter-derived Currents With Aquarius Salinity To Study The Marine Freshwater Budget Gary Lagerloef Aquarius Principal Investigator Yi Chao.
On the role of circulation and mixing in the ventilation of the oxygen minimum zone of the eastern tropical North Atlantic Peter Brandt with contributions.
Changes in the South American Monsoon and potential regional impacts L. Carvalho, C. Jones, B. Bookhagan, D. Lopez-Carr UCSB, USA A.Posadas, R. Quiroz.
Interannual Variability (Indian Ocean Dipole) P. N. Vinayachandran Centre for Atmospheric and Oceanic Sciences (CAOS) Indian Institute of Science (IISc)
Ocean Data Assimilation for SI Prediction at NCEP David Behringer, NCEP/EMC Diane Stokes, NCEP/EMC Sudhir Nadiga, NCEP/EMC Wanqiu Wang, NCEP/EMC US GODAE.
November 28, 2006 Representation of Skin Layer and Diurnal Warming Effects Gary Wick 1 and Sandra Castro 2 1 NOAA Earth System Research Laboratory 2 CCAR,
Nansen Environmental and Remote Sensing Center Modifications of the MICOM version used in the Bergen Climate Model Mats Bentsen and Helge Drange Nansen.
SPURS Synthesis Research Objectives: Budget calculations Resolve important terms of the freshwater and heat budgets of the upper 1000 m on temporal scales.
Tropical Atlantic SST in coupled models; sensitivity to vertical mixing Wilco Hazeleger Rein Haarsma KNMI Oceanographic Research The Netherlands.
Seasonal Variations of MOC in the South Atlantic from Observations and Numerical Models Shenfu Dong CIMAS, University of Miami, and NOAA/AOML Coauthors:
TAV / PIRATA-17 Meeting, Kiel, Germany
ASCOS ocean boundary layer measurements Anders Sirevaag Sara de la Rosa
I. Objectives and Methodology DETERMINATION OF CIRCULATION IN NORTH ATLANTIC BY INVERSION OF ARGO FLOAT DATA Carole GRIT, Herlé Mercier The methodology.
Argo’s role in closing the oceanic heat and freshwater budgets Dean Roemmich, Josh Willis, and John Gilson Scripps Institution of Oceanography, La Jolla.
OCEAN RESPONSE TO AIR-SEA FLUXES Oceanic and atmospheric mixed
Intraseasonal latent heat flux based on satellite observations
TAV / PIRATA-17 Meeting, Kiel, Germany
Monsoonal impacts on the Pacific climate and its
Annual mean precipitation (colour), SST (contours) & surface wind
TAV / PIRATA-17 Meeting, Kiel, Germany
Numerical Mixing in the COSIMA Models
Presentation transcript:

Mixed layer heat and freshwater budgets: Improvements during TACE Rebecca Hummels 1, Marcus Dengler 1, Peter Brandt 1, Michael Schlundt 1 1 GEOMAR Helmholtz Zentrum für Ozeanforschung, Kiel, Germany Ocean Sciences Meeting 2014, Honolulu, Hawaii USA,

Motivation : Why look at Mixed Layer (ML) heat budgets in Tropics?  Annual-mean heat flux through sea surface calculated from the ECMWF 40-year reanalysis (Kallberg et al., 2005) Annual-mean Sea Surface Temperature (SST) from TMI satellite observations

Which processes drive seasonal SST variability ? Motivation: SST variability in the Atlantic Cold Tongue (ACT) Interannual variability of ACT SSTs is tied to interannual variations in rainfall over the adjacent continents

Foltz et. al 2003 Motivation: Mixed layer heat budget Contributions to residual: coarse resolution of surface velocity climatology bad data coverage for relative humidity neglection of diapycnal heat flux out of the ML individual contributions to heat balance Sum and local storage

Observational program repetitive microstructure sections within the cold tongue region: 11 cruises during different seasons individual stations with at least 3 profiles (>2000 profiles) shipboard ADCP measurements

Data Treatment CTD sensors  T, C, p  Shear sensors  Dissipation rate of turbulent kinetic energy for isotropic turbulence is given by: ( Osborn and Cox, 1972) (Osborn, 1980) Eddy diffusivities for mass can be estimated as : From MSS measurements to diapycnal heat fluxes

Background settings within the ACT 3°S-1.5°N (equatorial ACT): elevated shear levels ( due to strong currents (EUC,cSEC,nSEC) enhanced dissipation rates below MLD EUC cSEC nSEC moderate shear levels due to the lack of strong currents background dissipation rates below MLD 10°S-4°S (southern ACT):

Diapycnal heat flux: Layer of interest Divergent profile of diapycnal heat flux heat loss due to diapycnal mixing is characterized by diapycnal heat flux in thin layer below the ML this value is included in the ML heat budget MLD

Mixed layer heat budget 3 phases of ACT development: 1)Absence (January-April) 1)Development (May-August) 2)Mature phase (September- December) 0°N, 10°W Evaluation at the 4 PIRATA buoy locations within the ACT

Mixed layer heat budget local storage = net surface - advection – eddy advection - entrainment – diapycnal ML heat loss 0°N, 23°W

Mixed layer heat budget Warming: Cooling: local storage = net surface - advection – eddy advection - entrainment – diapycnal ML heat loss 0°N, 23°W net surface heat flux

zonal and meridional heat advection Mixed layer heat budget Warming: Cooling: local storage = net surface - advection – eddy advection - entrainment – diapycnal ML heat loss 0°N, 23°W net surface heat flux

Mixed layer heat budget Warming: Cooling: local storage = net surface - advection – eddy advection - entrainment – diapycnal ML heat loss 0°N, 23°W net surface heat flux zonal and meridional heat advection, eddy advection

Mixed layer heat budget Warming: Cooling: local storage = net surface - advection – eddy advection - entrainment – diapycnal ML heat loss 0°N, 23°W net surface heat flux zonal and meridional heat advection, eddy advection, entrainment

, diapycnal Mixed layer heat budget Warming: Cooling: local storage = net surface - advection – eddy advection - entrainment – diapycnal ML heat loss 0°N, 23°W net surface heat flux zonal and meridional heat advection, entrainment

Mixed layer heat budget Warming: Cooling: local storage = net surface - advection – eddy advection - entrainment – diapycnal ML heat loss 0°N, 23°W net surface heat flux zonal and meridional heat advection, eddy advection, entrainment, diapycnal

Mixed layer heat budget Warming: Cooling: local storage = net surface - advection – eddy advection - entrainment – diapycnal ML heat loss 0°N, 23°W net surface heat flux zonal and meridional heat advection, eddy advection, entrainment, diapycnal

Mixed layer heat budget local storage = net surface - advection – eddy advection - entrainment – diapycnal ML heat loss 0°N, 10°W Warming: net surface heat flux, eddy advection Cooling: zonal and meridional heat advection, entrainment, diapycnal

Mixed layer heat budget local storage = net surface - advection – eddy advection - entrainment – diapycnal ML heat loss 0°N, 0°E Warming: net surface heat flux (strongly reduced), eddy advection, meridional Cooling: zonal heat advection, entrainment, diapycnal

Mixed layer heat budget local storage = net surface - advection – eddy advection - entrainment – diapycnal ML heat loss 10°S, 10°W Warming: eddy advection and meridional heat advection Cooling: net surface heat flux, zonal heat advection, entrainment, diapycnal

Mixed layer heat budget closed ML heat budget within uncertainties during sampled periods 0°N, 10°W0°N, 23°W diapycnal heat flux and zonal advection are the terms dominating the cooling within the equatorial ACT 0°N, 0°E 10°S, 10°W

Salinification:E-P>0, entrainment, meridional heat advection and diapycnal salt flux Freshening:eddy advection and zonal heat advection Freshwater budget 0°N, 23°W 0°N, 10°W

Salinification:evaporation, entrainment, meridional heat advection and diapycnal salt flux Freshening:precipitation, eddy advection and zonal heat advection Freshwater budget 0°N, 23°W 0°N, 10°W during ACT development mixed layer salinity increases largest terms: entrainment and diapycnal salt flux

Summary and Outlook improvement of the ML heat budget a higher resolved surface velocity climatology improved net surface heat fluxes (TropFlux) estimates of the diapycnal ML heat loss closure of the budgets within the incertainties within the ACT identification of main cooling terms during ACT development: diapycnal heat flux (partly zonal advection) in the entire equatorial ACT region further required improvements (specially for investigations of inter annual variability of ML budget contributions): surface velocities resolution of diapycnal ML heat loss 

Uncertainties Drifter and ARGO (used here) OSCAR Lumpkin et al., 2005 choice of surface velocity product 0°N, 23°W seasonal variability of diapycnal ML heat loss not sufficiently resolved

Mixed layer heat budget closed ML heat budget within uncertainties during sampled periods 0°N, 10°W0°N, 23°W 10°W, 10°S diapycnal heat flux and zonal advection are the terms dominating the cooling within the equatorial ACT Improvements  0°N, 0°E

Diapycnal ML heat loss: Seasonal and regional variability Heat loss of the MLD due to turbulent mixing is elevated : within the equatorial region in the western equatorial ACT compared to the east in early summer compared to September and November MLD

Diapycnal ML heat loss: Seasonal and regional variability Heat loss of the MLD due to turbulent mixing is elevated : within the equatorial region in the western equatorial ACT compared to the east

Diapycnal ML heat loss: Seasonal and regional variability MLD Heat loss of the MLD due to turbulent mixing is elevated : within the equatorial region in the western equatorial ACT compared to the east in early summer compared to September and November

Uncertainties Comparison of zonal and meridional velocity of different surface velocity products

Parametrization

Existing parametrization schemes for the equatorial region are based on a simple Ri (N²/S²) dependence: Pacanowski and Philander 1981 Peters 1988 (2 different formulations) KPP (Large et al 1994) Zaron and Moum 2009 (2 different formulations) Propose a simple dependence fitted to the observational data of this study

Parametrization 10°W, 0°N Parametrizations

Parametrization  Most existing parametrization schemes cleary overestimate the heat loss of the mixed layer due to diapycnal mixing  Seasonal parametrized heat loss based on independent data set with new fit is closest to observations MLD

Parametrization All individual terms of the mixed layer heat budget at 10°W on the equator are estimated from observations of the PIRATA buoy and climatological products 10°W, 0°N