Empirical Orthogonal Function Analysis of Ocean Surface Currents Using Complex and Real-Vector Methods*

Empirical orthogonal function (EOF) analysis has been widely used in meteorology and oceanography to extract dominant modes of behavior in scalar and vector datasets. For analysis of two-dimensional vector fields, such as surface winds or currents, use of the complex EOF method has become widespread. In the present paper, this method is compared with a real-vector EOF method that apparently has previously been unused for current or wind fields in oceanography or meteorology. It is shown that these two methods differ primarily with respect to the concept of optimal representation. Further, the real-vector analysis can easily be extended to threedimensional vector fields, whereas the complex method cannot. To illustrate the differences between approaches, both methods are applied to Ocean Surface Current Radar data collected off Cape Hatteras, North Carolina, in June and July 1993. For this dataset, while the complex analysis ‘‘converges’’ in fewer modes, the real analysis is better able to isolate flows with wide cross-shelf structures such as tides.

[1]  D E Barrick,et al.  Ocean surface currents mapped by radar. , 1977, Science.

[2]  Duncan B. Ross,et al.  Mesoscale Ocean Surface Current Structure Detected by High-Frequency Radar , 1995 .

[3]  M. Merrifield,et al.  Detecting Propagating Signals with Complex Empirical Orthogonal Functions: A Cautionary Note , 1990 .

[4]  Donald R. Thompson,et al.  Ocean surface features and currents measured with synthetic aperture radar interferometry and HF radar , 1996 .

[5]  Lawrence Sirovich,et al.  An empirical eigenfunction analysis of sea surface temperatures in the western North Atlantic , 1997 .

[6]  P. Holmes,et al.  Turbulence, Coherent Structures, Dynamical Systems and Symmetry , 1996 .

[7]  L. Shay Internal Wave-Driven Surface Currents From HF Radar , 1997 .

[8]  L. Sirovich,et al.  Propagating structures in wall-bounded turbulent flows , 1991 .

[9]  D. Inman,et al.  Description of seasonal beach changes using empirical eigenfunctions , 1975 .

[10]  B. Ng The Prediction of Nearshore Wind-induced Surface Currents from Wind Velocities Measured at Nearby Land Stations , 1993 .

[11]  R. Preisendorfer,et al.  Principal Component Analysis in Meteorology and Oceanography , 1988 .

[12]  Donald R. Thompson,et al.  Correlation of oceanographic signatures appearing in synthetic aperture radar and interferometric synthetic aperture radar imagery with in situ measurements , 1997 .

[13]  L. Sirovich Turbulence and the dynamics of coherent structures. I. Coherent structures , 1987 .

[14]  David M. Legler,et al.  Empirical Orthogonal Function Analysis of Wind Vectors over the Tropical Pacific Region , 1983 .

[15]  P. K. Kundu,et al.  Some Three-Dimensional Characteristics of Low-Frequency Current Fluctuations near the Oregon Coast , 1976 .

[16]  Donald E. Barrick,et al.  Ocean Surface Currents Mapped by Radar , 1977, Science.

[17]  John E. Kutzbach,et al.  Empirical Eigenvectors of Sea-Level Pressure, Surface Temperature and Precipitation Complexes over North America , 1967 .

[18]  Lawrence Sirovich,et al.  The Karhunen–Loéve decomposition of minimal channel flow , 1997 .

[19]  D. M. Hardy,et al.  Empirical eigenvector analysis of vector observations , 1977 .

[20]  John L. Lumley,et al.  Viscous Sublayer and Adjacent Wall Region in Turbulent Pipe Flow , 1967 .

[21]  John L. Lumley,et al.  Large Eddy Structure of the Turbulent Wake behind a Circular Cylinder , 1967 .

[22]  John M. Klinck,et al.  EOF Analysis of Central Drake Passage Currents from DRAKE 79 , 1985 .

[23]  H. Graber,et al.  Current Structure Variations Detected by High-Frequency Radar and Vector-Measuring Current Meters , 1998 .