
Revised ocean backscatter models at C and Ku band under high‐wind conditions
Author(s) -
Donnelly William J.,
Carswell James R.,
McIntosh Robert E.,
Chang Paul S.,
Wilkerson John,
Marks Frank,
Black Peter G.
Publication year - 1999
Publication title -
journal of geophysical research: oceans
Language(s) - English
Resource type - Journals
SCImago Journal Rank - 1.67
H-Index - 298
eISSN - 2156-2202
pISSN - 0148-0227
DOI - 10.1029/1998jc900030
Subject(s) - scatterometer , backscatter (email) , environmental science , remote sensing , wind speed , crosswind , geology , meteorology , wind direction , geography , oceanography , computer science , telecommunications , wireless
A series of airborne scatterometer experiments designed to collect C and Ku band ocean backscatter data in regions of high ocean surface winds has recently been completed. More than 100 hours of data were collected using the University of Massachusetts C and Ku band scatterometers, CSCAT and KUSCAT. These instruments measure the full azimuthal normalized radar cross section (NRCS) of a common surface area of the ocean simultaneously at four incidence angles. Our results demonstrate limitations of the current empirical models, C band geophysical model function 4 (CMOD4), SeaSat scatterometer 2 (SASS 2), and NASA scatterometer 1 (NSCAT) 1, that relate ocean backscatter to the near‐surface wind at high wind speeds. The discussion focuses on winds in excess of 15 m s −1 in clear atmospheric conditions. The scatterometer data are collocated with measurements from ocean data buoys and Global Positioning System dropsondes, and a Fourier analysis is performed as a function of wind regime. A three‐term Fourier series is fit to the backscatter data, and a revised set of coefficients is tabulated. These revised models, CMOD4HW and KUSCAT 1, are the basis for a discussion of the NRCS at high wind speeds. Our scatterometer data show a clear overprediction of the derived NRCS response to high winds based on the CMOD4, SASS 2, and NSCAT 1 models. Furthermore, saturation of the NRCS response begins to occur above 15 m s −1 . Sensitivity of the upwind and crosswind response is discussed with implications toward high wind speed retrieval.