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模拟的对流边界层光学湍流的特征尺度分析
引用本文:卢超,袁仁民,罗涛,吴徐平,孙鉴泞. 模拟的对流边界层光学湍流的特征尺度分析[J]. 光学学报, 2012, 32(2): 201002-23
作者姓名:卢超  袁仁民  罗涛  吴徐平  孙鉴泞
作者单位:卢超:深圳市国家气候观象台, 广东 深圳 518040中国科学技术大学地球和空间科学学院, 安徽 合肥 230026
袁仁民:中国科学技术大学地球和空间科学学院, 安徽 合肥 230026
罗涛:中国科学技术大学地球和空间科学学院, 安徽 合肥 230026
吴徐平:中国科学技术大学地球和空间科学学院, 安徽 合肥 230026
孙鉴泞:南京大学大气科学学院, 江苏 南京 210093
基金项目:国家自然科学基金(40975006,40975004)和中国科学院知识创新工程重要方向(KZCX2-YW-QN502)资助课题。
摘    要:边界层作为地面与自由大气的过渡带对人类活动影响很大。边界层湍流结构尤其是夹卷层的湍流特征,是边界层研究的一个重要方面,这对于加深对边界层的认识以及研究边界层参数化具有十分重要的意义。由于边界层上部位置较高,难以进行精细结构观测。在室内对流水槽(150cm×150cm×60cm)中模拟了大气对流边界层的发生发展。将准直光通过模拟对流边界层得到光斑图像数据。利用改进协方差法对光斑图像进行功率谱分析,找出功率谱密度最大值所对应的频率即峰值频率,峰值频率对应的波长为涡的特征尺度。研究结果表明,在混合层,峰值波长较小,说明此处混合比较均匀,小尺度结构占主导地位。而夹卷层的峰值波长较大。夹卷层的平均峰值波长与对流Richardson数存在一定的关系,这种关系受下垫面类型以及对流状况的双重影响。

关 键 词:大气光学  峰值波长  功率谱分析  水槽模拟  混合层和夹卷层  非均匀下垫面
收稿时间:2011-07-22

Characteristic Scale Analysis of Atmospheric Optical Turbulence in Simulating Convective Boundary Layer with Water Tank
Lu Chao,Yuan Renmin,Luo Tao,Wu Xuping,Sun Jianning. Characteristic Scale Analysis of Atmospheric Optical Turbulence in Simulating Convective Boundary Layer with Water Tank[J]. Acta Optica Sinica, 2012, 32(2): 201002-23
Authors:Lu Chao  Yuan Renmin  Luo Tao  Wu Xuping  Sun Jianning
Affiliation:1 Shenzhen National Climate Observatory,Shenzhen,Guangdong 518040,China 2 School of Earth and Space Sciences,University of Science and Technology of China,Hefei,Anhui 230026,China 3 School of Atmospheric Sciences,Nanjing University,Nanjing,Jiangsu 210093,China
Abstract:The boundary layer is very important to human activity as the transition zone between the surface and free atmosphere. Turbulence structure of the boundary layer especially the entrainment layer is an important aspect for the boundary layer research, which is very important to improve understanding of the boundary layer and the research of the boundary layer parameterization. Because of the high level of the top of the boundary layer, it is difficult to detect extensively. Generation and evolution of the atmospheric convective layer are simulated in laboratory convective water tank with the dimension of 150 cm×150 cm×60 cm . When the collimated light beam propagates through the simulated atmospheric convective boundary layer, facula image data can be obtained. Using improved covariance method for power spectrum analysis on the facula image, the peak frequency can be found by finding the maximum power spectral density corresponding to the frequency, which is needed to obtain the peak wavelength as the characteristic scale of eddy. It is found that, in the mixed layer, peak wavelength is small, which means that the mixed layer is homogeneously mixed and small scale dominated there. But in entrainment layer the peak wavelength was larger. The average peak wavelength in the entrainment zone has some relation with the convective Richardson number, and the relation are influenced by surface types and convection condition.
Keywords:atmospheric optics  peak wavelength  power spectrum analysis  water-tank simulation  mixed layer and entrainment layer  inhomogeneous land surface
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