The normalized radar cross section of the sea at 10° incidence

Measurements of the normalized radar cross section of the sea at K/sub u/ band at an incidence angle of 10/spl deg/ were performed from a manned airship off the Oregon coast in September and October of 1993. The cross section at this incidence angle is often assumed to have little dependence on windspeed and direction. Their measurements, however, indicate that at windspeeds below 6-7 m/s, the cross section is in fact dependent on these quantities, and the azimuthal modulation can reach values on the order of 5-8 dB. Comparisons of the measured values with the predictions of the quasispecular scattering model are presented. The theory is shown to be accurate in predicting the azimuthal modulation and the strength of the backscatter if the effects of swell are included or if measured wind directions are ignored and the upwind direction is forced to be near the maximum cross section. Values of mean-square wind-wave slope and effective-reflection coefficient required to obtain these fits are very close to those obtained by previous investigators. In particular, mean-square wind-wave slopes are about 70-80% of those of Cox and Munk (1954) because the radar responds only to facets larger than about 10 cm, with smaller ripples acting to reduce the reflection coefficient. If swell is included, they find that mean-square slopes in the direction of the swell, that are as much as ten times the measured swell slopes, are required to fit the model to the cross-section data at low windspeeds. They suggest that this may be due to high-order effects of the hydrodynamic modulation of short waves by the swell. They believe that this explanation is more likely than assuming that wind directions were incorrectly measured.

[1]  L. Schroeder,et al.  AAFE RADSCAT 13.9-GHz measurements and analysis: Wind-speed signature of the ocean , 1985, IEEE Journal of Oceanic Engineering.

[2]  Michael S. Longuet-Higgins On the Skewness of Sea-Surface Slopes , 1982 .

[3]  J. Apel An improved model of the ocean surface wave vector spectrum and its effects on radar backscatter , 1994 .

[4]  G. Valenzuela Theories for the interaction of electromagnetic and oceanic waves — A review , 1978 .

[5]  J. Mitchell,et al.  Aircraft measurements of the microwave scattering signature of the ocean , 1977, IEEE Journal of Oceanic Engineering.

[6]  M. Donelan,et al.  Radar scattering and equilibrium ranges in wind‐generated waves with application to scatterometry , 1987 .

[7]  W. Pierson,et al.  The relationship between wind vector and normalized radar cross section used to derive SEASAT‐A satellite scatterometer winds , 1982 .

[8]  N. Roy,et al.  The wind-speed measurement capability of spaceborne radar altimeters , 1981 .

[9]  Donald E. Barrick,et al.  Rough Surface Scattering Based on the Specular Point Theory , 1968 .

[10]  William J. Plant,et al.  Measurements of the Marine Boundary Layer from an Airship , 1998 .

[11]  D. E. Hines,et al.  Sea surface mean square slope from K u ‐band backscatter data , 1992 .

[12]  A.K. Fung,et al.  Radar determination of winds at sea , 1979, Proceedings of the IEEE.

[13]  John Daley An Empirical Sea Clutter Model. , 1973 .

[14]  William J. Plant,et al.  A wave tank study of the dependence of X band cross sections on wind speed and water temperature , 1992 .

[15]  C. Cox Statistics of the sea surface derived from sun glitter , 1954 .

[16]  W. Plant A two-scale model of short wind-generated waves and scatterometry , 1986 .