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An empirical sea clutter model for low grazing angles

机译:低掠角的经验海杂波模型

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The most fundamental characteristic of sea clutter, as used in radar performance evaluation, is its apparent reflectivity defined as sigma0 (m2/m2). The word apparent is used here as a reminder that any measurement of sea clutter reflectivity inevitably includes the effects of propagation close to the sea surface. Sea clutter reflectivity depends on many factors including sea state, wind velocity, grazing angle, polarization, and radar frequency. A comprehensive tabulation of measurements from around 60 sources were included in the 1991 edition of Nathanson's book and this probably represents the most complete database of sea clutter reflectivity available. Also included in this book by Nathanson was a detailed description of an empirical sea clutter model proposed by Horst et. al., the so-called Georgia Technical Institute (GTI) model. This model has found widespread acceptance in the radar community although its technical basis may be somewhat vague. As pointed out by Nathanson, his tabulated measured sea clutter data does not agree too well with the GTI model, in particular at low sea states. While this difference qualitatively can be explained by measurement inaccuracies, unknown propagation conditions (such as ducting), and uncertainties in defining the underlying sea state, these discrepancies are at times quite large and may lead to overly optimistic radar performance predictions if the GTI sea clutter model is used. In this paper a new empirical model for sea clutter reflectivity at low grazing angles is developed. The model is defined as a function of radar frequency, polarization, sea-state, and grazing angle. The parameters of the empirical equation have been optimized such that the average absolute dB-deviation between the model and the experimental data tabulated by Nathanson is minimized for grazing angles up to 10 degrees. Subsequently we shall refer to this new model as the NRL sea clutter model.
机译:雷达性能评估中使用的海杂波的最基本特征是其表观反射率定义为sigma 0 (m 2 / m 2 )。这里使用“明显”一词来提醒人们,任何对海杂波反射率的测量都不可避免地包括靠近海面传播的影响。海杂波反射率取决于许多因素,包括海况,风速,掠角,极化和雷达频率。 1991年版的Nathanson的书中包含了来自大约60个来源的全面测量表,这可能代表了可用的最完整的海杂波反射率数据库。内森森(Nathanson)的这本书中还包括对霍斯特(Horst)等人提出的经验性海杂波模型的详细描述。等,所谓的佐治亚技术学院(GTI)模型。尽管该模型的技术基础可能有些含糊,但已在雷达界获得广泛接受。正如纳森森(Nathanson)所指出的那样,他的列表化测量海杂波数据与GTI模型不太吻合,尤其是在低海州。虽然可以通过测量的不准确性,未知的传播条件(例如管道)和确定潜在海况的不确定性来定性地解释这种差异,但是这些差异有时会很大,如果GTI海杂波会导致雷达性能预测过于乐观使用模型。本文针对低掠角的海杂波反射率建立了新的经验模型。该模型被定义为雷达频率,极化,海况和掠射角的函数。优化了经验方程的参数,以使模型和Nathanson列表的实验数据之间的平均绝对dB偏差在掠角最大10度时最小化。随后,我们将此新模型称为NRL海杂波模型。

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