2001
DOI: 10.1002/mop.1198
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Wind direction azimuthal signature in the Stokes emission vector from the ocean surface at microwave frequencies

Abstract: An ocean polarimetric emission model is presented. It is found that skewness and upwind/cross‐wind rms slopes are responsible for the first and second azimuthal harmonic, respectively. Atmospheric effects contribute significantly at low wind speeds, and at horizontal polarization at certain observation angles. Simulation results compare favorably with reported JPL–WINDRAD measurements. © 2001 John Wiley & Sons, Inc. Microwave Opt Technol Lett 29: 426–432, 2001.

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Cited by 12 publications
(9 citation statements)
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“…However, these models have been developed or tuned at higher frequencies, typically 19 and 37 GHz. Therefore, the solid lines have been computed using a simple, fast, and accurate extended Kirchhoff model under the stationary phase approximation [14] that describes well the incidence angle dependence at L-band, and also the 19 and 37 GHz Jet Propulsion Laboratory measurements. The sea foam effects at L-band are hard to model.…”
Section: A Incidence Angle and Azimuth Signaturesmentioning
confidence: 99%
“…However, these models have been developed or tuned at higher frequencies, typically 19 and 37 GHz. Therefore, the solid lines have been computed using a simple, fast, and accurate extended Kirchhoff model under the stationary phase approximation [14] that describes well the incidence angle dependence at L-band, and also the 19 and 37 GHz Jet Propulsion Laboratory measurements. The sea foam effects at L-band are hard to model.…”
Section: A Incidence Angle and Azimuth Signaturesmentioning
confidence: 99%
“…. Although not very accurate at L-band, an extended Kirchhoff model under the stationary phase approximation [9] has been used to plot the solid lines overlaid in Fig. 7.…”
Section: Low-to-moderate Wind Conditions-mentioning
confidence: 99%
“…The percentage errors as a result of assuming constant atmospheric downwelling temperature are less than 2% and 5% of the incidence angle sensitivities, and , respectively. After accounting for the reflected downwelling radiation, the incidence angle sensitivities of the measured ocean surface emission were modeled using the Kirchhoff method with the stationary phase approximation as formulated by Camps and Reising [7]. To avoid the need to calculate for every measured incidence angle, and since the variations in incidence angle were less than , the values were assumed to be constant over this range, and equal to their average values.…”
Section: B Pitch Angle Correctionmentioning
confidence: 99%