一次典型高压型海雾过程中海上大气波导的数值模拟

2009年4月9—12日黄海海域发生了一次受高压系统影响的海雾过程。利用卫星观测与探空数据、WRF模式(Weather Research and Forecasting Model)对此次海雾过程及相伴的大气波导进行了观测分析与数值模拟。海雾与波导发展可分为3个阶段:(1)大气波导先于海雾存在于黄海海面;受高压下沉影响,黄海上空存在逆温层和较强的湿度梯度,表现为较强的贴海表面波导和非贴海表面波导。(2)海雾始于高压西部,并随高压系统逐渐东移减弱,向黄海北部扩展;辐射冷却虽然使雾顶附近逆温增强,但海雾的机械湍流使其顶部湿度梯度减小,雾顶附近对应弱悬空波导或波导消失。(3)高压系统影响使干空气下沉到雾区导致黄海海雾消散;雾顶附近逆温仍存在,同时湿度梯度增大,黄海上空逐渐变为非贴海表面波导。本研究结果表明:高压系统不仅极易为波导的发生提供有利条件,而且有利于海雾的生成,在海雾演变过程中主要是雾顶水汽梯度的变化导致了波导类型及强度的变化。     

黄海平流海雾的观测分析

利用大量的地面站点观测、卫星监测和非常规观测资料,统计分析了海雾的时空分布特征、卫星云图特征及影响黄海海雾的气象和水文因子.结果表明,黄海海雾随时间和空间而变化,在空间分布上,雾频随着纬度增高而增加;海雾与海上风速的大小和方向有密切关系;海雾出现与海表温度、气-海温差、露点温度有关;海流是影响海雾形成的水文因素之一;海雾是大气处在稳定层状态下的一种凝结现象,有海雾不一定有逆温,但是逆温层的消散却为海雾的消散提供了有利的依据.     

基于20年卫星遥感资料的黄海、渤海海雾分布季节特征分析

目前对海上雾分布的认识多基于沿岸测站和海上船舶、浮标观测,但这些数据非常稀少,且存在代表性和数据质量方面的问题,因此一直缺乏对海雾分布更全面、清晰的了解。卫星遥感数据空间均一、覆盖范围广、质量一致,具有对无云条件下大范围、离岸海雾监测的优势。本文通过分析算法检测出的1989-2008年黄渤海海雾及云的频数、分布百分率信息,得到了黄渤海海雾季节变化的较全面特征。除印证其他资料或研究的结论外,还发现:(1)黄海海雾频数随季节变化的幅度较渤海明显;(2)黄海、渤海海域存在冬季海雾多发时段;(3)海雾生消过程中有覆盖区变化的东传特征;(4)春夏雾季中存在黄海中部和西朝鲜湾两处海雾多发区,其中西朝鲜湾也是全年海雾最多的海域。另外,在样本充足的情况下,通过对检测出的低云、中高云覆盖百分率和海雾频数的分析统计,还能估算出黄海、渤海部分季节20年海雾发生的平均概率。     

第三讲 海雾的水文气象特征

海雾是在一定的水文条件和特定的天气背景下产生并维持的。世界各大洋主要雾区分布表明,冷暖海流交汇的海洋锋区,为海雾的生成提供了优越的水文条件,因为穿过锋区,水平方向的温度梯度很大;但也不是每天都有海雾发生,这与当时的天气条件如风场,近水层的大气温湿度以及空气的稳定度等有关。世界各地海雾的水文气象条件各有异同,本讲将以中国海及其临近海域海雾的水文气象特征为依据加以分析,同时介绍海雾的某些微观物理特征。 一、水文气象条件 (一)水温和水气温差 西北太平洋及其边缘海域的海雾,以平流冷却雾为主,尤其在多雾的春、夏季。产生条件是暖空气平流到冷海面上,因此它的生成与消散,必然与海表面温度,大气和海水温度差以及风场有关,当海面上的空气在平流冷却过程中,气温降到露点温度,空气方可饱和,如果露点温度恰好等于水温,那么低层空气凝结成雾是顺理成章的。但是,如果水温很高,而空     

我国东部沿海一次局地海雾抬升成云过程分析

利用洪家站L波段雷达探空资料、高分辨率海气耦合模式再分析资料、静止气象卫星云图和地面观测资料,分析了一次黄东海海雾抬升为低云,使海雾消散的过程。发现近海面偏南风速突然增强,海洋大气边界层(MABL)中机械剪切加强,湍流混合层向上发展,是导致海雾抬升转化为低云的主要原因。近海面风速突然增加与高空急流北抬、平均层槽脊振幅加大、槽前正涡度平流输入诱使地面低压系统发展、地面气压梯度力增大有关。近海面气温升高对海雾消散也有作用,气温升高的原因是暖平流、绝热下沉和海气界面热通量的综合效应。其中,东海海洋锋(STF)冷区的下沉气流可能对边界层内的绝热下沉增温和低云的形成高度有重要的影响。该研究为海雾消散预报提供了新的思路。     

青岛地区海雾分布及大气边界层条件分析

青岛地区海雾多发,观测表明海雾对沿海地区影响范围不尽相同,特别是海雾影响内陆的机理尚缺乏研究。本文利用观测资料及数值模式统计了青岛地区4月-7月海雾分布特征,并对不同影响范围海雾典型个例进行对比分析,结果表明:海雾发生日数自沿海向内陆递减。胶州湾沿岸雾日数比黄海沿岸明显减少,胶州湾东北部的雾日数要少于胶州湾西北部。海雾多发生于高空形势稳定,低层偏南流场的天气条件下。大气边界层内逆温层的的范围大致影响着海雾的分布。只影响沿海的海雾,地面为偏南风,风速在3~8 m/s之间,内陆风力减弱不明显。500 m以下大气边界层内风速切变大。湍流作用使海雾向内陆推进过程中倾斜抬升为低云,地面雾区减弱。能够影响内陆地区的海雾,多出现在地面风力较弱的情况之下,大部分在1~3 m/s之间。500 m以下大气边界层内风速切变小,大气边界层内湍流强度不强,使沿海到内陆的逆温层能够始终维持,沿海海雾在弱南风影响下延伸影响内陆地区。     

冬季黑潮延伸体区域涡旋尺度海面温度季节内变化特征

利用ERA_interim再分析资料以及OISST高分辨率海面温度(Sea surface temperature,SST)卫星观测数据,通过小波分析、二维模态相关(Pattern correlation)等方法系统地分析了黑潮延伸体区域涡旋尺度SST信号的季节内变化特征。发现涡旋尺度SST季节内变化信号在冬季最强、夏季最弱。该信号主要分布在黑潮-亲潮海洋锋面区域,在日本沿岸振幅最强、并沿黑潮、亲潮锋面向东延伸,其标准差高达1℃,是该海域冬季SST的重要变化信号。涡旋尺度SST的季节内变化周期以40～100 d周期为主,会引起大气边界层的响应,激发海气界面湍流热通量、海面气温、边界层高度等同位相的季节内变化。在该区域涡旋信号较强个数较多的时间段SST异常的季节内变化信号更明显,边界层大气与涡旋尺度SST季节内变化信号的相关程度更大。     

北部湾地区海雾特点的初步分析

利用2016年1月至2017年12月北部湾浮标站观测资料,分析了北部湾海雾的特点。结果表明,2016年北部湾出现海雾37 d,2017年为19 d; 3月海雾日数最多,4月次之,2016年12月和2017年6—10月未出现海雾;一天中出现雾的峰值时间为03:00—05:00,雾消散的峰值时间为08:00—10:00;雾的维持时间绝大部分在3 h以内。浮标站与北海站、涠洲岛站的大气能见度、相对湿度对比分析表明,在海雾日,涠洲岛站的平均大气能见度、平均相对湿度更接近浮标站,涠洲岛站平均大气能见度比浮标站大0.7～3.3 km,平均相对湿度比浮标站小1.6%～2.4%。不同的海雾过程由于影响系统不同,海上和陆地上雾的持续时间、大气能见度有所不同,当西南暖低压、高压后部影响造成大雾时,涠洲岛站的大气能见度与浮标站更接近,北海站的大气能见度与浮标站相差较大;而均压场造成海雾时,3个观测站的大气能见度变化趋势较为一致,凌晨到上午有雾,中午到下午雾消散。     

基于文氏谱的起伏海面虚反射特征研究

海洋地震记录中的虚反射会和反射波发生混叠和干涉,严重影响了海洋地震资料的质量。常规海面水平的条件假设将在海面反射系数计算过程中引入误差。本文引入文圣常提出并改进的文氏海浪谱,采用有效波高、海浪成长系数等各项参数模拟出更符合实际情况的海浪形态,并通过时频分析等方法研究起伏海面虚反射对地震记录的改造作用和起伏海面条件下的虚反射时频谱特征。结果表明：当海面起伏程度较大时,起伏海面的虚反射不仅强烈扭曲了海底一次波反射同相轴,且与一次波发生了强烈的干涉作用,导致成像结果出现很多假同相轴,严重影响了地震资料的质量。随着起伏海面有效波高的增加,地震记录受陷波效应逐渐增强,虚反射能量逐渐增加,主频幅值逐渐减小。当海面起伏变化时,随着偏移距的增加,陷波点幅值变化丰富,主频幅值逐渐减小,且向高频方向移动。随着震源或检波器沉放深度逐渐增加,有效波虚反射的能量强度逐渐增加,频带变窄,陷波改造作用强烈,主频幅值逐渐减小。     

南海北部近岸春季海雾的年际变化

利用ICOADS(International Comprehensive Ocean-Atmosphere Data Set)资料对南海北部春季海雾的年际变化特征进行研究.春季南海北部的海雾多集中在近岸海区,远离岸线的海区海雾较少发生.南海北部近岸春季海雾日数偏多年份有4个(1969、1983、1986、1987年);雾日数偏少年份有5个(1971、1999-2002年).利用NCEP/NCAR月平均再分析资料,对海雾日数偏多、偏少年份的850hPa等压面上各要素分别进行合成分析.850hPa等压面上,华南沿海上空常年存在一个由南向北的暖平流.南海上空的空气湿度较大,在海雾日数偏多年份大气湿度减小,偏少年份湿度增大.南海上空850-1 000hPa等压面之间存在一股来自西太平洋的水汽输送.在海雾日数偏多年份水汽输送增强,海雾日数偏少年份水汽输送减弱.     

Measuring solar irradiance profiles in the Arctic sea ice using fiber optic spectrometry via inclined holes

An irradiance profile measurement approach and profiling system were developed to measure the solar irradiance profile of the Arctic sea ice using fiber optic spectrometry. The approach involved using a miniature spectrometer to sense light signals collected and transmitted from a fiber probe. The fiber probe was small, and could thus move freely in inclined bore holes drilled in sea ice with its optical entrance pointing upward. The input-output relationship of the system was analyzed and built. Influence factors that determined the system output were analyzed. A correctional system output approach was proposed to correct the influence of these factors, and to obtain the solar irradiance profile based on the measurements outputted by this system. The overall performance of the system was examined in two ice floes in the Arctic during the 9 th Chinese National Arctic Research Expedition. The measured solar irradiance profiles were in good agreement with those obtained using other commercially available oceanographic radiometers. The derived apparent optical properties of sea ice were comparable to those of similar sea ice measured by other optical instruments.     

Reconstruction of regular time series from bi-monthly temperature data in the Yellow Sea and the northwestern East China Sea

Reconstruction of evenly-spaced, regular time series from routine survey serial data was investigated for precise analysis of spatio-temporal variations in a temperate sea at mid-latitudes where the seasonality dominates the interannual variability. Considering that the annual range of sea surface temperature in the Yellow Sea and the northwestern East China Sea can be as large as 15–20 °C, temperature data collected bi-monthly in these temperate seas were used for the assessment of reconstruction methodology. The cubic spline interpolation with a sampling interval of 0.5 months reconstructed the regular time series closest to the in-situ measurements among various interpolation schemes. Also, two computation methods for the interannual anomaly were compared; the residual method that the long-term monthly means are subtracted from the monthly serial data and the filtering method that high-frequency variations are removed using a low-pass filter. In that the high-frequency variations in frequencies greater than 1 cycle per year are comparable in magnitude to the interannual variation, the residual method proves inadequate in the temperate sea. High-frequency noises can be effectively removed through the use of a proper low-pass filter with bell-shaped weights.     

Measurement of the sea surface emissivity

The sea surface emissivity in the infrared region is determined on the basis of data analyses. Net radiation, surface irradiance and other oceanographical and meteorological variables are measured throughout most of the year at the oceanographical observatory tower in Tanabe Bay, Japan. We have found that 0.984±0.004 is a reliable emissivity value from the night time data. Surface emission radiates not from the subsurface water but from the sea surface. The thermal skin layer on the sea surface, however, is disturbed and disappears under high wind speed over 5 m/s through the analyses of the radiation observation using the emissivity value of 0.984. Under low wind speed, the sea surface can be cooler or warmer than the subsurface due to overlying thermal conditions and the skin layer can be neutral as the transient process between them. By using an emissivity value of 0.984, the temperature difference between the sea surface temperature and the temperature determined from surface irradiance that has been reported in the satellite data analyses is found to be reduced by half.     

Variation of diffuse attenuation coefficient of downwelling irradiance in the Arctic Ocean

The diffuse attenuation coefficient(Kd) for downwelling irradiance is calculated from solar irradiance data measured in the Arctic Ocean during 3rd and 4th Chinese National Arctic Research Expedition(CHINARE), including 18 stations and nine stations selected for irradiance profiles in sea water respectively. In this study, the variation of attenuation coefficient in the Arctic Ocean was studied, and the following results were obtained. First, the relationship between attenuation coefficient and chlorophyll concentration in the Arctic Ocean has the form of a power function. The best fit is at 443 nm, and its determination coefficient is more than 0.7. With increasing wavelength, the determination coefficient decreases abruptly. At 550 nm, it even reaches a value lower than 0.2. However, the exponent fitted is only half of that adapted in low-latitude ocean because of the lower chlorophyll-specific absorption in the Arctic Ocean. The upshot was that, in the case of the same chlorophyll concentration, the attenuation caused by phytoplankton chlorophyll in the Arctic Ocean is lower than in low-latitude ocean. Second, the spectral model, which exhibits the relationship of attenuation coefficients between 490 nm and other wavelength, was built and provided a new method to estimate the attenuation coefficient at other wavelength, if the attenuation coefficient at 490 nm was known. Third, the impact factors on attenuation coefficient, including sea ice and sea water mass, were discussed. The influence of sea ice on attenuation coefficient is indirect and is determined through the control of entering solar radiation. The linear relationship between averaging sea ice concentration(ASIC, from 158 Julian day to observation day) and the depth of maximum chlorophyll is fitted by a simple linear equation. In addition, the sea water mass, such as the ACW(Alaskan Coastal Water), directly affects the amount of chlorophyll through taking more nutrient, and results in the higher attenuation coefficient in the layer of 30–60 m. Consequently, the spectral model of diffuse attenuation coefficient, the relationship between attenuation coefficient and chlorophyll and the linear relationship between the ASIC and the depth of maximum chlorophyll, together provide probability for simulating the process of diffuse attenuation coefficient during summer in the Arctic Ocean.     

基于遥感的海表紫外辐射强度反演方法

Ultraviolet(UV) radiation has a significant influence on marine biological processes and primary productivity;however, the existing ocean color satellite sensors seldom contain UV bands. A look-up table of wavelengthintegrated UV irradiance(280–400 nm) on the sea surface is established using the coupled ocean atmosphere radiative transfer(COART) model. On the basis of the look-up table, the distributions of the UV irradiance at middle and low latitudes are inversed by using the satellite-derived atmospheric products from the Aqua satellite,including aerosol optical thickness at 550 nm, ozone content, liquid water path, and the total precipitable water.The validation results show that the mean relative difference of the 10 d rolling averaged UV irradiance between the satellite retrieval and field observations is 8.20% at the time of satellite passing and 13.95% for the daily dose of UV. The monthly-averaged UV irradiance and daily dose of UV retrieved by satellite data show a good correlation with the in situ data, with mean relative differences of 6.87% and 8.43%, respectively. The sensitivity analysis of satellite inputs is conducted. The liquid water path representing the condition of cloud has the highest effect on the retrieval of the UV irradiance, while ozone and aerosol have relatively lesser effect. The influence of the total precipitable water is not significant. On the basis of the satellite-derived UV irradiance on the sea surface, a preliminary simple estimation of ultraviolet radiation's effects on the global marine primary productivity is presented, and the results reveal that ultraviolet radiation has a non-negligible effect on the estimation of the marine primary productivity.     

海冰中侧向传播光衰减系数的解析验证

The attenuation of lateral propagating light(LPL) in sea ice was measured using an artificial light source in the Canadian Arctic during the 2007/2008 winter. The apparent attenuation coefficient μ(λ) for lateral propagating light was obtained from the measured logarithmic relative variation rate. In this study an analytical solution based on the strict optical theories is developed to validate the measured result. There is a good consistency between theoretical solution and measured data, by which a quite simple but very rigorous relationship among the light source, measurement geometry, and measured irradiance is established. The attenuation coefficients acquired by measurement and theory are the diffusion attenuation as an apparent optical property of ice, independent of the light source and shining condition. The attenuation ability of sea ice should be caused by the microstructure of sea ice, such as crystal size, ice density, brine volume, air inclusion, etc. It also includes the leak from both interfaces by directional scattering. It is verified that the measuring approach is operational and accurate to measure the attenuation of the LPL. The solution from this study did not tell the connection among the extinction and the inclusions of sea ice theoretically because of insufficient understanding.     

Analysis of the inter-annual variability and southward expansion of red tides in the Zhejiang coastal waters from 1981 to 2018

A time series dataset spanning 39 years(1981-2018) on red tide events in Zhejiang coastal waters was used to study the characteristics of inter-annual spatial and temporal variations. A distinct inter-annual pattern characterized by low frequency, explosive growth and fluctuating decline stages was found over the studied time scale. Most red tide events occurred in parallel to the bathymetric contour, and 95.4% were located to the west of the 50 m isobath. Additionally, the high-incidence area o...     

渤海冬季海冰气候变异的成因分析

选取渤海冰情等级资料和大气环流74个指数逐月资料,分别建立不同尺度(年、半年、季和月)的累积值变量作为因子,研究该地区冰情年代际变化及冰情的气候成因,结果发现以1972年为分界把1932～2000年时期冰情的变化分为两个时段,前一时段为重冰情多发阶段,1972年以后转为轻冰情时段.影响渤海海冰冰情变化主要因子是太平洋副高.     

基于长期观测的辽东湾口东部海域水动力特征研究

辽东湾口东部海域是辽东湾与渤海中部进行物质和能量交换的主要通道之一。本文利用坐底式海床基平台获取的近8个月的水动力连续观测资料,通过谱分析和调和分析方法对该海域的潮汐、潮流特征进行分析,并讨论了余流及底层温度的季节变化规律。研究结果表明:该海域潮汐属于不规则半日潮,平均潮差为0.95 m,最大可能潮差为2.27 m。潮流属于不规则半日潮流,M₂分潮流为其优势分潮流。主要分潮流运动形式为往复流,最大流速方向为西南-东北向。余流的季节性特征较为明显:秋季,余流流速在中层达到最大,流向以西南向为主;冬季,余流流速垂向变化较小,并呈西南偏西向流动;春季,流速随深度增加而减小,流向从表层至底层呈现逆时针旋转的特征。受底层潮流、水平温度梯度及海面温度日变化的影响,底层温度表现出短期的高频变化特征:秋季,短期振荡以半日周期信号为主;冬季,全日周期信号较为显著;春季,短期振荡的现象较弱。     

中国南海表层叶绿素a季节内变化特征及成因

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