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Recent results on modeling the refractive-index structure parameter over the ocean surface using bulk methods

机译:使用散装方法对海洋表面的折射率结构参数进行建模的最新结果

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Infrared scintillation measurements were obtained along a 7.2 km path over San Diego Bay, concurrently with mean meteorological and turbulence measurements obtained from a buoy located along the path. Bulk estimates and turbulence measurements of C_n~2 were computed from the buoy data and compared with the optical scintillation-derived C_n~2 values. Similar to the results of previous experiments, the bulk C_n~2 estimates agreed well with both the scintillation and turbulence measurements in unstable conditions, increasingly underestimated C_n~2 as conditions approached neutral, and agreed less well with scintillation and turbulence C_n~2 values in stable conditions. The mean differences between bulk C_n~2 estimates and both the turbulence and scintillation measurements when conditions were not near-neutral exhibited an air-sea temperature difference and wind speed dependence, possibly indicating that the forms of the empirical stability functions used by the bulk model are incorrect. The turbulent C_n~2 measurements from the buoy showed excellent agreement with the scintillation values in unstable conditions, but had surprisingly large differences in weakly stable conditions. This disagreement may be related to the fact that humidity fluctuations begin to increasingly influence refractive index fluctuations when the air-sea temperature difference is small and are not properly taken into account by the sonic temperature measurements. As the absolute air-sea temperature difference approaches zero the bulk C_n~2 estimates decrease much more rapidly and to much smaller values than either the scintillation or turbulence measurements. Fortunately, in such near-neutral conditions scintillation is usually small enough to have little effect on many optical system applications.
机译:在圣地亚哥湾沿7.2公里的路径获得了红外闪烁测量值,同时从沿该路径放置的浮标获得了平均气象和湍流测量值。根据浮标数据计算出C_n〜2的体积估计值和湍流测量值,并将其与光学闪烁衍生的C_n〜2值进行比较。与以前的实验结果相似,C_n〜2的总体估算值与不稳定条件下的闪烁和湍流测量结果吻合得很好,随着接近中性条件,C_n〜2的估算值越来越低,而在不稳定条件下,闪烁和湍流C_n〜2值的吻合程度则不太条件稳定。当条件不是接近中性时,体C_n〜2估计值与湍流和闪烁测量之间的平均差异表现出海-海温度差和风速依赖性,这可能表明体模型使用的经验稳定性函数的形式是不正确的。在不稳定条件下,浮标的湍流C_n〜2测量值与闪烁值显示出极好的一致性,但在弱稳定条件下却具有惊人的大差异。这种分歧可能与以下事实有关:当空气-海洋温度差较小且声波温度测量未适当考虑到湿度波动时,湿度波动就开始逐渐影响折射率波动。随着绝对海气温度差接近零,与闪烁或湍流测量相比,体积C_n〜2估计值将更快地减小并且减小到更小的值。幸运的是,在这种接近中性的条件下,闪烁通常很小,对许多光学系统应用几乎没有影响。

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