武汉上空大气密度温度的激光雷达探测

介绍了中国科学院武汉物理与数学研究所瑞利散射激光雷达的结构和性能,报道了该激光雷达观测所得到的我国武汉上空30～70 km范围内大气密度和30～60 km范围内温度廓线的反演结果。     

海洋工程勘察的实践与探索

为全面了解海洋工程地质资料,本次工作采用收集区域地质资料、物理探测、工程钻探、土工试验等手段,对辽东湾北部的某海洋石油平台及海底管线路由进行了工程勘察,在实践的基础上取得了一些海洋工程勘察经验,获得了较好的效果。介绍海洋工程勘察的工作方法与主要内容的同时,对区域地质评价、管道路由场地地质评价、平台防沉板的工程分析、钢管桩的分析与评价等内容进行了简要阐述,同时也发现了一些目前在海洋工程勘察领域存在的问题。     

Raman激光雷达探测对流层中上部大气温度分布

介绍了一台氮分子(N2)Raman激光雷达系统.利用N2分子Raman散射和气溶胶及分子的Mie-Rayleigh散射信号,通过同时订正分子、气溶胶和臭氧的衰减,反演出对流层中上部大气密度和温度的垂直分布,其结果与常规球载无线电探空仪探测资料对比,在8～18 km范围内表现了较好的一致性.其中,二者测量的温度在9～15 km高度内相对差别小于4 K.     

Potassium Doppler-resonance lidar for the study of the mesosphere and lower thermosphere at the Arecibo Observatory

We have developed a lidar to study the temperature structure of the nighttime mesopause region over the Arecibo Observatory (18.35°N, 66.75°W) by measuring the lineshape of the fluorescence spectrum of atomic potassium that is deposited in the mesosphere and lower thermosphere (MLT) by meteors. To demonstrate how the potassium lidar can enhance MLT studies at Arecibo, we show recent results for: (1) comparisons with airglow temperature measurements; (2) simultaneous operations with stratospheric and mesospheric temperature profiling by Rayleigh lidar; (3) simultaneous observations of K, Ca⁺, and E-region electron density profiles; and (4) occurrences of sporadic K layers, and relationships to sporadic E layers.     

随机取向沙尘气溶胶激光雷达线退偏比特性研究

利用离散偶极子近似法,数值计算分析了随机取向旋转椭球体沙尘气溶胶粒子在尺度参数为0.1~23时（波长0.55 μm对应有效半径为0.01~2 μm）的激光雷达线退偏比特性,通过比较其不同旋转椭球体轴半径比下的差别,研究了粒子非球形性程度对单分散和多分散沙尘气溶胶激光雷达线退偏比特性的影响.单分散旋转椭球体沙尘气溶胶的激光雷达线退偏比对粒子的轴半径比和尺度参数有很强的依赖性;对于长旋转椭球体,沙尘激光雷达线退偏比较小值出现在瑞利散射区,而较大的值出现在米散射区;对于扁旋转椭球体,在米散射区较大沙尘粒子也可以产生较小的激光雷达线退偏比,例如,轴半径比为1/16,尺度参数为3时的沙尘激光雷达线退偏比仅为0.1%.就随机取向旋转椭球体沙尘粒子而言,对于单分散系,仅当尺度参数小于0.5时,非球形特征越明显,其激光雷达线退偏比越大;而对多分散系,非球形特征越明显,其激光雷达线退偏比越大.     

华北香河站一次霾污染事件的综合观测研究

利用激光雷达、太阳光度计、系留气艇低空探测数据及MODIS卫星数据等多源资料,对2007年2月初发生在我国中东部地区的一次大范围霾污染事件进行了综合分析,重点分析了华北香河站垂直向气溶胶光学特性的变化特征,并初步讨论了气溶胶区域输送。分析结果表明:霾污染中心位于大城市、城市群或者盆地等污染物源排放强度大或者地形不利于污染物扩散的地区,形成了6个污染中心;2日霾最严重时,近地面气溶胶消光系数(355nm)达到1.8 km~(-1),是霾发生前的3倍;霾最严重时气溶胶光学厚度(340 nm)为1.4,较前后日的高;随着边界层高度的下降,底层气溶胶快速积累;香河站气溶胶在垂直向存在明显的分层现象,上层600—1000 m高度气溶胶受区域输送的影响,其光学厚度占整层气溶胶的比值能达到43.6%,甚至更高;本次霾过程以细粒子为主;弱高压系统、低至100 m左右的逆温层高度及低风速等气象条件对此次霾的形成起到了重要的作用;而3日出现的大风则很可能是驱散霾的重要因子。     

大气遥感双视场米散射激光雷达信号拼接

介绍了一种双视场米散射激光雷达信号拼接方法。主要思想是寻找近场和远场信号都具有高信噪比的最佳拼接区域,求解该区域两种信号之间的函数关系,自动实现激光雷达近场信号与远场信号的有效拼接和反演。拼接结果兼具近场信号探测盲区低和远场信号探测高度高的优点。反演结果表明,该方法能够准确有效地实现双视场信号拼接,并能反演得到高精度的气溶胶光学特性。     

新一代水位测量系统—空气声学水位计

本文介绍了空气声学水位计的工作原理、技术指标及现场使用比测结果。结果证明用该仪器来更新水位测量系统是合适的。     

The Application of Sea-Surface Wind Detection with Doppler Lidar in Olympic Sailing

The mobile incoherent Doppler lidar(MIDL),which was jointly developed by State Key Laboratory of Severe Weather(LaSW) of the Chinese Academy of Meteorological Sciences(CAMS) and Ocean University of China,provided meteorological services during the Olympic sailing events in Qingdao in 2008.In this study,two experiments were performed based on these measurements.First,the capabilities of MIDL detection of sea-surface winds were investigated by comparing its radial velocities with those from a sea buoy.MIDL radial velocity was almost consistent with sea-buoy data;both reflected the changes in wind with time.However,the MIDL data was 0.5 m s 1 lower on average than the sea-buoy data due to differences in detection principle,sample volume,sample interval,spatial and temporal resolution.Second,the wind fields during the Olympic sailing events were calculated using a four-dimensional variation data assimilation(4DVAR) algorithm and were evaluated by comparing them with data from a sea buoy.The results show that the calculations made with the 4DVAR wind retrieval method are able to simulate the fine retrieval of sea-surface wind data-the retrieved wind fields were consistent with those of sea-buoy data.Overall,the correlation coefficient of wind direction was 0.93,and the correlation coefficient of wind speed was 0.70.The distribution of retrieval wind fields was consistent with that of MIDL radial velocity;the root-mean-square error between them had an average of only 1.52 m s 1.