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Measurement of optical turbulence in the u

机译:光学湍流的测量

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Abstract: Horizontal path temperature fluctuation measurements were made on board a KC-135 aircraft, at altitudes ranging from 30,000 to 40,000 feet, such that the altitudes below, in, and above the tropopause were sampled. In general, we find that there is a low background level of turbulence, and there appear to be superimposed o this background higher level turbulent 'patches.' These patches are a few km in extent, and the boundaries of these patches are abrupt with the transition to background taking place in distances of approximately 50 meters. These abrupt boundaries are consistent with the optical measurements taken at the same time. The measured structure functions of the form D(r) is approximate to r$+n$/ with o.2$LSEQ@n$LSEQ@2 down to scale sized of 20 cm, which was the limiting resolution of the instrumentation. Each flight segment was conducted under constant conditions (i.e., speed, temperature, altitude). Contrary to expectations, the log slopes of either the power spectral densities or of the structure functions are often non-Kolmogorov, as characterized by a k$+$MIN@5/3$/ power spectral density, or by a structure function of the form r$+2/3$/. This statement must be tempered, however, by uncertainties in the frequency response of the temperature sensor. In addition, the data show regions in which the expected functional relation between the structure function and power spectral density does not hold. These characteristics of high-altitude turbulence suggest that past measurement techniques used to measure c$-n$/$+2$/ may be inapplicable in the high-altitude regime, and c$-n$/$+2$/ as a sole descriptor of turbulence may be incomplete. !5
机译:摘要:在KC-135飞机上海拔30,000到40,000英尺的高度上进行了水平路径温度波动的测量,从而对了对流层顶下方,上方和上方的海拔高度进行了采样。通常,我们发现湍流的背景水平较低,并且此背景较高的湍流“斑块”似乎叠加了。这些斑块的范围只有几公里,并且这些斑块的边界会突然过渡到背景,距离大约为50米。这些突变边界与同时进行的光学测量结果一致。形式D(r)的测量结构函数近似为r $ + n $ /,其中o.2 $ LSEQ @ n $ LSEQ @ 2缩小到20厘米,这是仪器的极限分辨率。每个飞行段均在恒定条件(即速度,温度,高度)下进行。与预期相反,功率谱密度或结构函数的对数斜率通常不是Kolmogorov,其特征在于ak $ + MIN @ 5/3 $ /功率谱密度,或形式为r $ 2/2/3 $ /。但是,必须通过温度传感器的频率响应中的不确定性来调节该陈述。此外,数据显示的区域中,结构功能和功率谱密度之间的预期功能关系不成立。高海拔湍流的这些特征表明,过去用于测量c $ -n $ / $ + 2 $ /的测量技术可能不适用于高海拔地区,而c $ -n $ / $ + 2 $ /作为湍流的唯一描述可能不完整。 !5

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