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Ka-Band Dual Copolarized Empirical Model for the Sea Surface Radar Cross Section

机译:海面雷达截面的Ka波段双共极化经验模型

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This paper presents dual copolarized (PP) (VV and HH) Ka-band sea surface backscattering measurements taken from the Black Sea research platform at incidence angles ranging from 25° to 65° and in the wind speed range from 3 to 18 m/s. These measurements are corrected for radar antenna pattern and geometry of observations. The resulting normalized radar cross section (NRCS) is parameterized in a form of truncated azimuthal Fourier series with coefficients dependent on the incidence angle and wind speed. This dual PP empirical model (KaDPMod) is consistent with the Ku-band NSCAT-4 model. However, some remarkable differences are revealed. They are apparent when analyzed using a decomposition of VV and HH measurements into polarized Bragg backscattering (polarization difference, PD = VV−HH) and nonpolarized (NP) backscattering from breaking waves. The polarization difference (PD) has strong azimuth and wind dependencies, with the wind exponent ranging from 2.5 to 3. The saturation wave spectra derived from multifrequency PD (based on KaDPMod and Ku- and C-band empirical models) have a notable peak in the capillary-gravity range. The relative contribution of NP radar return to the Ka-band NRCS is significant. In the upwind direction, it reaches up to 60%–80% and 25%–50% for HH and VV, respectively. It is found that the NP wind exponent is lower than that for Bragg backscattering. Therefore, the relative contribution of the NP to Ka-band NRCS decreases with increasing wind speed at both polarizations. Such a behavior is the opposite of that observed in the Ku-band.
机译:本文介绍了从黑海研究平台进行的双共极化(PP)(VV和HH)Ka波段海面后向散射测量,入射角范围为25°至65°,风速范围为3至18 m / s 。这些测量已针对雷达天线方向图和观测几何进行了校正。所得的归一化雷达横截面(NRCS)以截顶方位傅立叶级数的形式进行参数化,其系数取决于入射角和风速。这种双重PP经验模型(KaDPMod)与Ku波段NSCAT-4模型一致。但是,揭示了一些显着差异。当使用VV和HH测量值分解为极化布拉格反向散射(极化差,PD = VV-HH)和来自破碎波的非极化(NP)反向散射时,它们很明显。极化差(PD)具有很强的方位角和风力依赖性,风力指数在2.5到3之间。多频PD(基于KaDPMod以及Ku和C波段经验模型)得出的饱和波谱在毛细管重力范围。 NP雷达返回对Ka波段NRCS的相对贡献是重要的。在逆风方向,HH和VV分别达到60%–80%和25%–50%。发现NP风指数低于布拉格反向散射的风指数。因此,NP对Ka波段NRCS的相对贡献随着在两个极化方向上风速的增加而减小。这种行为与在Ku波段观察到的行为相反。

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