Reconstructing ocean 3-d structure from surface measurements Bruno Buongiorno Nardelli, Olga Cavalieri, Rosalia Santoleri, Marie-Helene Rio Gruppo di Oceanografia.

Slides:



Advertisements
Similar presentations
MEsoSCale dynamical Analysis through combined model, satellite and in situ data PI: Bruno Buongiorno Nardelli 1 Co-PI: Ananda Pascual 2 & Marie-Hélène.
Advertisements

SVINØY SECTION A full-scale ocean climate laboratory in the Norwegian Atlantic Current.
Tensors and Component Analysis Musawir Ali. Tensor: Generalization of an n-dimensional array Vector: order-1 tensor Matrix: order-2 tensor Order-3 tensor.
A thermodynamic model for estimating sea and lake ice thickness with optical satellite data Student presentation for GGS656 Sanmei Li April 17, 2012.
Experiments with Monthly Satellite Ocean Color Fields in a NCEP Operational Ocean Forecast System PI: Eric Bayler, NESDIS/STAR Co-I: David Behringer, NWS/NCEP/EMC/GCWMB.
SIO 210: I. Observational methods and II. Data analysis (combined single lecture) Fall 2013 Remote sensing In situ T, S and tracers Velocity Observing.
Eleonora Rinaldi, Bruno Buongiorno Nardelli, Gianluca Volpe, Rosalia Santoleri Institute for Atmospheric Sciences and Climate (ISAC) National Research.
Maximum Covariance Analysis Canonical Correlation Analysis.
Environmental Data Analysis with MatLab Lecture 16: Orthogonal Functions.
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.
Horizontal Pressure Gradients Pressure changes provide the push that drive ocean currents Balance between pressure & Coriolis forces gives us geostrophic.
About Estuarine Dynamics
Argo Products at the Asia-Pacific Data-Research Center Konstantin Lebedev, Sharon DeCarlo, Peter Hacker, Nikolai Maximenko, James Potemra, Yingshuo Shen.
Horizontal Pressure Gradients Pressure changes provide the push that drive ocean currents Balance between pressure & Coriolis forces gives us geostrophic.
Observational evidence for propagation of decadal spiciness anomalies in the North Pacific Yoshi N. Sasaki, N. Schneider, N. Maximenko, and K. Lebedev.
Ocean warming and sea level rise D. Roemmich 1, J. Willis 2, J. Gilson 1 1 Scripps Institution of Oceanography, UCSD 2 NASA Jet Propulsion Laboratory Understanding.
Review High Resolution Modeling of Steric Sea-level Rise Tatsuo Suzuki (FRCGC,JAMSTEC) Understanding Sea-level Rise and Variability 6-9 June, 2006 Paris,
Group Meeting 2010/03/30 R Kirsten Feng. Nutrient and salinity decadal variations in the central and eastern North Pacific E. Di Lorenzo, J. Fiechter,
Sustained Ocean Observations in Support of Sea Surface Salinity Process Studies Gustavo Jorge Goni National Oceanic and Atmospheric.
Spatial coherence of interannual variability in water properties on the U.S. northeast shelf David G. Mountain and Maureen H. Taylor Presented by: Yizhen.
Extensions of PCA and Related Tools
Quality Assessment of a Mediterranean Sea Reanalysis M. Adani, G. Coppini, C.Fratianni, P.Oddo, M.Tonani, GNOO, INGV Sez Bologna N. Pinardi,
M-H Rio 1, F.Hernandez 2, J-M Lemoine 3, R. Schmidt 4, Ch. Reigber 4 AN IMPROVED MEAN DYNAMIC TOPOGRAPHY COMPUTED GLOBALLY COMBINING GRACE DATA, ALTIMETRY.
“ New Ocean Circulation Patterns from Combined Drifter and Satellite Data ” Peter Niiler Scripps Institution of Oceanography with original material from.
“ Combining Ocean Velocity Observations and Altimeter Data for OGCM Verification ” Peter Niiler Scripps Institution of Oceanography with original material.
Linear Inverse Modeling with an SVD treatment (at least the extent that I’ve learned thus far) Eleanor Middlemas.
Cambiamento attuale: Ghiaccio e mare CLIMATOLOGIA Prof. Carlo Bisci.
Sophie RICCI CALTECH/JPL Post-doc Advisor : Ichiro Fukumori The diabatic errors in the formulation of the data assimilation Kalman Filter/Smoother system.
Interannual Variabilities of High Clouds Seen by AIRS and Comparison with CAM5 simulations Yuk Yung, Hui Su, Katie, Hazel et al.
2nd GODAE Observing System Evaluation Workshop - June Ocean state estimates from the observations Contributions and complementarities of Argo,
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.
© Crown copyright Met Office The EN4 dataset of quality controlled ocean temperature and salinity profiles and monthly objective analyses Simon Good.
An example of vertical profiles of temperature, salinity and density.
OSTST March, Hobart, Tasmania Ocean Mean Dynamic Topography from altimetry and GRACE: Toward a realistic estimation of the error field Marie-Helene.
Principles of the Global Positioning System Lecture 12 Prof. Thomas Herring Room ;
Weak Constraint 4DVAR in the R egional O cean M odeling S ystem ( ROMS ): Development and application for a baroclinic coastal upwelling system Di Lorenzo,
Group Meeting 2010/03/16 R Kirsten Feng. Coupled Decadal Variability in the North Pacific: An Observationally Constrained Idealized Model* BO.
In situ evidence of deep equatorial layering due to inertial instability M. d’Orgeville, B. L. Hua & R. Schopp Laboratoire de Physique des Océans, IFREMER,
GODAE OceanView-GSOP-CLIVAR workshop June Monitoring the Ocean State from the Observations Stéphanie Guinehut Sandrine Mulet Marie-Hélène.
A signal in the energy due to planetary wave reflection in the upper stratosphere J. M. Castanheira(1), M. Liberato(2), C. DaCamara(3) and J. M. P. Silvestre(1)
The I nverse R egional O cean M odeling S ystem Development and Application to Variational Data Assimilation of Coastal Mesoscale Eddies. Di Lorenzo, E.
A. Bonaduce, N. Pinardi Mediterranean Sea level reconstruction during the last century A. Bonaduce (1), N. Pinardi (2) (1) Centro Euro-Mediterraneo per.
3 “Products” of Principle Component Analysis
G. Panteleev, P.Stabeno, V.Luchin, D.Nechaev,N.Nezlin, M.Ikeda. Estimates of the summer transport of the Kamchatka Current a variational inverse of hydrographic.
Oceanography 569 Oceanographic Data Analysis Laboratory Kathie Kelly Applied Physics Laboratory 515 Ben Hall IR Bldg class web site: faculty.washington.edu/kellyapl/classes/ocean569_.
TS 15 The Great Salt Lake System ASLO 2005 Aquatic Sciences Meeting Climatology and Variability of Satellite-derived Temperature of the Great Salt Lake.
Central limit theorem revisited Throw a dice twelve times- the distribution of values is not Gaussian Dice Value Number Of Occurrences.
The OC in GOCE: A review The Gravity field and Steady-state Ocean Circulation Experiment Marie-Hélène RIO.
An oceanographic assessment of the GOCE geoid models accuracy S. Mulet 1, M-H. Rio 1, P. Knudsen 2, F. Siegesmund 3, R. Bingham 4, O. Andersen 2, D. Stammer.
Principal Components Analysis ( PCA)
Central limit theorem - go to web applet. Correlation maps vs. regression maps PNA is a time series of fluctuations in 500 mb heights PNA = 0.25 *
EMPIRICAL ORTHOGONAL FUNCTIONS 2 different modes SabrinaKrista Gisselle Lauren.
ESA Climate Change Initiative Sea-level-CCI project A.Cazenave (Science Leader), G.Larnicol /Y.Faugere(Project Leader), M.Ablain (EO) MARCDAT-III meeting.
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.
ARGO and other observing system elements – Issues and Challenges Uwe Send IfM Kiel With contributions from P.Testor J.Karstensen M.Lankhorst J.Fischer.
Geology 6600/7600 Signal Analysis 18 Nov 2015 Last time: Deconvolution in Flexural Isostasy Tharsis loading controversy: Surface loading by volcanic extrusives?
Spatial Modes of Salinity and Temperature Comparison with PDO index
EMPIRICAL ORTHOGONAL FUNCTIONS
2016 ROMS Asia-Pacific Workshop, Hobart, Australia
Using Profiling Float Trajectories to Estimate Ocean Circulation
SEA SURFACE TEMPERATURE TRENDS IN THE MEDITERRANEAN SEA: FROM INTERANNUAL TO DECADAL VARIATIONS By S. Marullo1, R. Santoleri2, M. Guarracino1, B. Buongiorno.
OCEAN RESPONSE TO AIR-SEA FLUXES Oceanic and atmospheric mixed
Y. Xue1, C. Wen1, X. Yang2 , D. Behringer1, A. Kumar1,
Principal Component Analysis
Multivariate Analysis: Theory and Geometric Interpretation
Assessment of the Surface Mixed Layer Using Glider and Buoy Data
NOAA Objective Sea Surface Salinity Analysis P. Xie, Y. Xue, and A
in situ or Altimetry ? Arctic – Subarctic Ocean Fluxes focus topics:
Presentation transcript:

Reconstructing ocean 3-d structure from surface measurements Bruno Buongiorno Nardelli, Olga Cavalieri, Rosalia Santoleri, Marie-Helene Rio Gruppo di Oceanografia da Satellite Istituto di Scienze dell’Atmosfera e del Clima-Sezione di Roma, CNR Contact: Objective of the work: Develop and test techniques for the extrapolation of the vertical structure of the sea from satellite measurements Take advantage of the fundamental information that comes from altimeter estimates of the sea elevation, and integrate it with in situ dynamic/steric heights, keeping into account the differences between them. In facts, the true sea level is substantially a measure of volume depending on the VERTICAL STRUCTURE of the sea: total water mass variations  horizontal advection at a fixed location (barotropic terms) specific volume variations  horizontal advection along the water column (baroclinic terms)  heat and salt exchanges Strategy: Implementation : SEVERAL STEPS: Use historical/climatological hydrological in situ measurements as ‘learning/training’ sets to correlate surface and deep layers variability  statistical analyses of temperature, salinity, density, steric/dynamic heights profiles temporal variability at a fixed location (time series) spatial variability in limited time periods (selected surveys) combined temporal/spatial variability (climatology) Test the validity of the methods using surface in situ data as input and the sensitivity to errors in surface measures Analyze the differences between satellite altimeter measures of sea elevation and in situ steric heights and adapt the methodologies to effectively use satellite data as input Test the methods using satellite data as surface input training test OBSERVE D RECONSTRUCTED CLIMATOLOGY Application of CPR to DYFAMED time-series using steric height at surface as input available at: Training data set  Independent Test data set  DATA USED: Conductivity Temperature Depth (CTD) profiles collected by the service of observation DYFAMED (DYnamique des Flux de mAtière en MEDiterranée) Multivariate EOF Reconstruction (mEOF-R) The multivariate EOF reconstruction (mEOF-R) is based on: The multivariate Empirical Orthogonal Function (mEOF) decomposition  technique for the identification of the ‘multicoupled’ modes of variability between n data sets of vertical profiles (here we consider, at first, temperature T(z,t), salinity S(z,t) and steric height SH(z,t) profiles) the hypothesis that few coupled modes explain the major part of the ‘multi-variability’ Historical in situ datasets (vertical profiles) mEOF modes Independent surface measurement s mEOF Reconstructe d vertical profiles mEOF-R Coupled Pattern Reconstruction (CPR) The Coupled Pattern Reconstruction (CPR) is based on: the Coupled Pattern Analysis (CPA)  technique for the identification of the coupled modes of variability between two data sets of vertical profiles (here we will consider temperature T(z,t) and steric height SH(z,t) profiles) the hypothesis that few coupled modes explain the major part of the co-variability Historical in situ datasets (vertical profiles) Couple d modes Independent surface measurement s CPA CPR Reconstructe d vertical profiles CPA identifies pairs of vertical patterns that explain as much as possible of the mean-squared temporal covariance between the two datasets (Bretherton et al., 1992). T(z,t) and SH(z,t) are expanded in terms of a set of N orthonormal vectors, L k and R k (called patterns), that are computed as the right and left singular vectors of the cross-covariance matrix: cross-covariance matrix CR k =s k L k C T L k =s k R k In practice, L k and R k are eigenvectors of CC T and C T C respectively and s k 2 are the eigenvalues for both. s k 2 represents the covariance explained by the k th mode. singular value problems CPA finally gives: patterns amplitudes In the ocean the major part of the covariance is typically explained by few modes. If we limit to the first two modes we have: CPR bases on the idea that, as the amplitudes a k (t) and b k (t) are strongly correlated (condition imposed by CPA), one can linearly relate one to the other: a k (t)=  k ·b k (t)+  k calculating  and  for each mode, we can estimate the profiles at any instant t from independent surface values (z=0) solving the linear system for a 1 (t) and a 2 (t): Core of CPR method mEOF consists in the EOF decomposition of a ‘multivariate’ matrix of data The new matrix is constructed putting the three sets of profiles (T, S and SH anomalies, each with m vertical levels and n measurements) in a single matrix X (3m  n). Data are preliminarily normalized dividing each parameter by its standard deviation. The further step is the computation of the EOF or, equivalently, the SVD of the ‘multi- variance’ matrix  X calculated from this new data set. The SVD applied to the multi-variance matrix identifies ‘multi-coupled’ modes, each containing the three patterns corresponding to the parameters considered:  X U=U   U=(u k ) eigenvalue problem new data matrix eigenvectors mEOF decomposition Similarly to CPR, in the hypothesis that few coupled modes explain the major part of the ‘multi-variability’, we can limit the expansion to the first three modes: While in the CPA the amplitudes were computed separately for each parameter, in the mEOF, the a k coefficients are the same for T, S and SH. The vertical profiles can be thus directly estimated at any instant t from the surface values (z=0) of the three parameters, solving a linear system for a 1, a 2 and a 3 : Core of mEOF-R method available at: Training data set  Independent Test data set  DATA USED: Conductivity Temperature Depth (CTD) profiles collected within the HOT (Hawaii Ocean Time-series) program at station ALOHA (A Long-term Oligotrophic Habitat Assessment) Application of mEOF-R to HOT time-series using steric height at surface as input OBSERVED TEMPERATURE CLIMATOLOGIC TEMPERATURE RECONSTRUCTED SALINITY CLIMATOLOGIC SALINITY training test RECONSTRUCTED TEMPERATURE OBSERVED SALINITY training test First method Second method Application of mEOF-R to Topex/Poseidon data Simultaneous CTD and altimeter Sea Level along Topex/Poseidon track 059 (Sicily channel) DATA USED: Training data set Independen t TEST data T/P track 059 Infrared Image (NOAA-14) CTD collected in the Sicily channel during the ALT and SYMPLEX cruises  spring 1996, spring 1998 OBSERVEDREC. FROM STERIC HEIGHTSREC. FROM TOPEX/POSEIDON GEOSTROPHIC VELOCITY TRANSECT A synthetic mean dynamic topography computed from drifter data and altimeter data has been added to Standard altimeter Sea Level Anomalies REFERENCES: Buongiorno Nardelli B., Santoleri R., Reconstructing synthetic profiles from surface data, J. Atmos. Oceanic Tech., vol.21, 4, Buongiorno Nardelli B. and R. Santoleri, 2004:Methods for the reconstruction of vertical profiles from surface data: multivariate analyses and variable temporal signals in the north Pacific Ocean, submitted to J. Atmos. Oceanic Tech. Cavalieri O., Buongiorno Nardelli B., Santoleri R., Estimating subsurface geostrophic velocities from altimeter data: application to the Sicily Channel (Mediterranean Sea), submitted to J. Geophys. Res. Rio M.-H. and F.Hernandez, 2004: A mean dynamic topography computed over the world ocean from altimetry, in situ measurements and a geoid model, J.Geophys.Res., in press.   T/P …… ∆ steric heights