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1.
通过与地基气溶胶观测数据的对比,确认了SeaWiFS气溶胶光学厚度产品用于研究中国海域气溶胶分布和变化特征的有效性。在此基础上,分析了中国海域气溶胶光学厚度的季节变化和地理分布特征。研究结果表明,中国东部海域平均气溶胶光学厚度存在以中纬度为中心的纬向分布;受沙尘、季风气候的影响,中国海域气溶胶光学厚度存在季节变化,不同海区有不同的季节变化和分布特征。渤海、黄海及东海有类似的变化特征,春季都受到沙尘气溶胶的影响,使中国东部海域气溶胶光学厚度普遍高于0.160,且对东海的影响最大;夏、秋季逐渐减小,冬季有所回升。南海气溶胶光学厚度均值为0.150,随时间变化不明显,但地理分布变化显著;受季风气候的影响,从春季到冬季,气溶胶光学厚度高值中心从高纬海域向低纬海域转移,范围也逐渐扩大。冬季南海大部分海域气溶胶光学厚度都达到0.160以上,是整个中国海域冬季气溶胶光学厚度最大的海区。气溶胶光学厚度的季节变化和地理分布特征为研究中国海区域气候变化和海洋生态提供了依据。  相似文献   

2.
南海中部海域障碍层特征及其形成机制   总被引:2,自引:0,他引:2  
南海中部海域(10°~19°N,108°~122°E)存在显著的季节变化的障碍层.障碍层发生概率夏季最大(52.8%),秋季次之(41.0%),春季最小(10.5%).夏季(2000年8~9月)障碍层最显著,平均厚度约为14.2m;除114°E以东、吕宋岛以西海域为障碍层的多发区外,中南半岛东南海域(12°~14°N,110°~114°E)也存在显著的障碍层;春季(1998年4~6月)和秋季(1998年12月)障碍层平均厚度分别为6.8和11.2m,障碍层多位于114°E以东、吕宋岛以西海域.此外,吕宋岛以西海域(12°~16°N,116°~120°E)及中沙和西沙群岛附近(16°~18°N,110°~116°E)海域障碍层年发生几率超过20%,相对而言,其他海域障碍层年发生几率偏小.降水机制和层结机制分别是南海中部海域春、夏季和秋季障碍层形成的主要原因.其中,降水机制及东南向的Ekman平流较好的解释了春、夏季吕宋岛以西附近海域成为障碍层多发区的原因;此外,强降水是夏季中南半岛东南海域(12°~14°N,110°~114°E)障碍层产生的关键,反气旋涡(暖涡)有助于形成更强的障碍层,上升流对障碍层的影响有待进一步研究.  相似文献   

3.
在卫星数据反演气溶胶光学厚度产品的基础上,讨论了二次反演大气柱中气溶胶粒子密度的问题.通过理论分析,利用多波段气溶胶光学厚度提取大气柱中气溶胶粒子密度是可行的,并指出能否准确确定多波段气溶胶光学厚度会直接影响粒子密度的反演结果.定义并分析了气溶胶粒子消光体积权重系数随粒子半径的变化,表明从气溶胶光学厚度中反演大气柱中气溶胶积聚模态和粗模态粒子密度的结果是可信的.利用SeaWiFS气溶胶光学厚度产品,运用蒙特卡罗法反演了2002年我国海域上空大气柱中积聚模态和粗模态气溶胶粒子密度,结果表明,积聚模态粒子密度比粗模态的高2~3个量级,它们的空间分布趋势一致;我国近岸海域大气柱中气溶胶粒子密度高于离岸海域的;春季气溶胶粒子密度高于其他季节的,特别在黄海、东海海区是如此.  相似文献   

4.
利用CE318型自动太阳光度计在2010年3~5月期间的观测数据,分析了沿海城市——天津市在沙尘与灰霾天气条件下大气气溶胶的光学与物理特性。主要参数包括:气溶胶光学厚度、Angstrom波长指数、散射相函数、单次散射反照率、复折射指数以及粒子体积谱分布。观测结果表明,在该季节的大气气溶胶光学特性主要受到人为和陆地沙尘的共同作用,不同天气条件下,大气气溶胶的光学与物理特性差异明显。  相似文献   

5.
中西太平洋金枪鱼围网高产渔区年间变化及其原因分析   总被引:1,自引:1,他引:0  
金枪鱼类是中西太平洋海域重要的经济鱼种,其中鲣产量约占到总产量的50%。本研究利用1995-2010年16年的中西太平洋(20°S~20°N,120°E~155°W)鲣围网生产统计数据和Niño3.4海区(5°S~5°N,120°~170°W)海表温度异常数据,对这16年鲣产量最高的十大渔区(5°×5°)进行时空格局分析,讨论渔场分布差异及CPUE与ENSO指数的关系。结果表明:16年间十大作业渔区主要分布在5°S~5°N、130°~175°E区域,这十大渔区产量占总产量的比重达47.5%,其中5°S~0°、155°~160°E,0°~5°N、130°~135°E,0°~5°N、135°~140°E及5°S~0°、160°~165°E等4个渔区产量占高产渔区产量的比重均超过10%,是中西太平洋重要的鲣产区。高产渔区的分布受海表温度影响较大,在厄尔尼诺时期,高产渔区分布明显偏东,主要分布在155°~180°E海域;在拉尼娜时期,高产渔区分布明显偏西,主要分布在130°~160°E海域。  相似文献   

6.
以渤海海域为试验区,对经过时间、空间和波段匹配的 MODIS/Aqua 550 nm 气溶胶光学厚度产品与 CALIOP 532 nm 通道反演得到的气溶胶信息在五种不同空间采样窗口(10 km ×10 km,30 km ×30 km,50 km ×50 km,70 km ×70 km 和90 km ×90 km)、三种不同时间尺度(日、月、季度)下进行了相关性拟合分析.研究发现,较小的空间采样窗口可以更准确地反映气溶胶的局部变化特征,而以季度为时间统计单元能更好地体现气溶胶的季节变化特性.实验结果表明,在10 km ×10 km 采样窗口中,春季的日数据之间相关性较高;春季和秋季的月均值之间高度相关(R 均大于0.950).从而证明,在特定时间和空间尺度下,上述两种数据之间确存在良好的相关性,为利用遥感数据反演渤海海域气溶胶光学厚度信息提供了新的途径.  相似文献   

7.
黄海、东海上空春季气溶胶光学特性观测分析   总被引:11,自引:5,他引:11  
2003年春季国家卫星海洋应用中心等几家单位在黄海和东海海区进行了为期40 d的二类水体信息测量试验,试验中使用手持太阳辐射计对海区上空大气光学特性进行了观测,并获得了大量晴空天气条件下的大气光学数据.利用本次试验获取的测量数据得到了黄海、东海海区春季的大气气溶胶光学特性,其中包括气溶胶光学厚度和气溶胶粒子谱分布.采用Langley方法对测量得到的太阳直射辐射量进行处理得到了海区上空气溶胶光学厚度,利用得到的气溶胶光学厚度来反演气溶胶粒子谱分布.反演结果表明无云情况下黄海、东海上空的气溶胶光学厚度在0.2~0.4左右,且气溶胶粒子谱分布的变化趋势也很接近;海区上空霾层较厚时测量得到的气溶胶光学厚度明显增大,最大接近0.8;气溶胶粒子谱分布的变化趋势发生了明显的变化.  相似文献   

8.
中国东部海域大气气溶胶入海通量的研究   总被引:18,自引:2,他引:16  
刘毅  周明煜 《海洋学报》1999,21(5):38-45
根据中国东部海域气溶胶浓度及分级采样资料,计算得出黄海、东海及日本以南海域沙尘气溶胶的代表元素铝(Al)每月干沉降通量分别为42.8、18.3、5.2mg/m2;其中各海域春季的干沉降通量均占全年干沉降通量的40%以上.相应每月总沉降通量分别为54.1、29.8、10.5mg/m2.渤海、黄海、东海及日本以南海域每年沙尘气溶胶总沉降通量分别为26.4、9.3、5.1、1.8g/m2.东海污染元素总沉降通量以春季最大,夏、秋季次之,冬季最小.日本以南海域锑(Sb)元素总沉降通量的季节分布为冬季最大,夏、秋季次之,秋季最小;硒(Se)元素总沉降通量的最大值出现在夏季,其他季节分布比较均匀.  相似文献   

9.
利用设立于厦门岛西南部沿海的气溶胶地基观测站点2008年1月7日至2009年4月30日的观测资料,对厦门海域气溶胶光学厚度的每日逐时变化、逐日变化、逐月变化进行了分析研究,并利用观测结果对MODIS L2级气溶胶光学厚度(AOT)产品进行检验。结果表明,厦门海域气溶胶光学厚度每日逐时变化和逐月变化有一定的季节规律,而逐日变化随气象条件的不同有很大差异。一年中气溶胶光学厚度月平均值呈现春秋季双峰分布趋势,4月份最大,超过0.9,空气较为混浊;6月份呈现谷值,AOT小于0.3,空气相对清洁。夏季气溶胶主控粒子的粒径较大,而其余各月份的波长指数在平均值1.21附近波动,混浊系数年平均值为0.25。利用该地基观测资料对MODIS L2级AOD产品进行检验,MODIS反演的厦门海域气溶胶光学厚度逐月变化趋势和地基观测结果完全一致,表明MODIS卫星遥感气溶胶光学厚度能比较好地反映厦门海域的气溶胶季节变化特征。  相似文献   

10.
南海北部气溶胶光学厚度观测研究   总被引:5,自引:0,他引:5  
利用2004年南海北部开放航次全程使用多波段太阳光度计观测获得的气溶胶光学厚度资料,对南海北部气溶胶光学厚度(AOD)的时空分布特征、气溶胶类型和来源等进行了分析。结果显示,近岸海域AOD值大,基本在0.5(500nm)以上,远离大陆的区域AOD值小,基本在0.2(500nm)以下。AOD值与污染源区丁业生产水平和气流输送密切相关,受珠三角地区丁业高度发展和冷空气南下的影响,在珠江口南部出现AOD高值中心;由于受台湾西南部工业区和东北信风的影响,台湾岛西南部海域AOD值偏大。3天的个例分析显示,海洋上空的AOD值上午和下午略高,中午最小,AOD与大气水汽含量呈正相关。Angstrom波长指数分析显示,大陆沿海海域气溶胶以小粒子为主,远离大陆海域以海盐粒子为主。  相似文献   

11.
The shortwave radiative forcings of smoke aerosol in the cloudless atmosphere during the summer fires of 2010 in European Russia were quantitatively estimated for the land surface and the atmospheric upper boundary from measurement data obtained at the Zvenigorod Scientific Station of the Obukhov Institute of Atmospheric Physics (OIAP ZSS), Russian Academy of Sciences. Variations in the temperature of the surface air layer due to the smoke-induced attenuation of incoming solar radiation were estimated. The most intensive smoke generation in the atmosphere was observed on August 7–9, 2010, when the maximum aerosol optical thickness amounted to more than 4.0 at a wavelength of 550 nm. In this case, the albedo of single aerosol scattering amounted to ∼0.95–0.96 and the asymmetry factor amounted to ∼0.69–0.70. The maximum shortwave radiative forcing of aerosol amounted to about −360 W/m2 for the land surface and almost −150 W/m2 for the atmospheric upper boundary. During the period of intensive smoke generation, the cooling of the atmospheric surface layer over daylight hours (12 h) amounted, on average, to ∼6°C. The power character of the dependence of the shortwave radiative forcing of aerosol for the land surface on aerosol optical thickness up to its values exceeding 4.0, which was revealed earlier on the basis of data on aerosol optical thickness (up to 1.5) obtained at the OIAP ZSS during the summer forest and peatbog fires of 2002 in the region of Moscow, was supported.  相似文献   

12.
We analyze the space-and-time variability of the meridional heat transport in the North Atlantic. The contribution of various mechanisms to the integral meridional heat transport (MHT) is estimated. The key role played by the drift transport of the Tropical Atlantic in the formation of the meridional oceanic heat transport is confirmed. On the basis of the general analysis of estimations obtained by various authors according to the data accumulated for 1870–2008 and the results of numerical analyses based on the data of NCEP/NCAR reanalysis, we show that the long-term average meridional drift heat (mass) transport attains its maximum values equal to (1.6 ± 0.1) PW [(17.4 ± 1.5) Sv] in the vicinity of 12.5°N in the Tropical Atlantic. The contribution of the heat transport caused by the horizontal Sverdrup circulation to the integral meridional heat transport is maximum in the vicinity of 30° N. On the average, it is equal to ∼ 40%. In the Subtropical Atlantic, the meridional heat transport varies with a period of ∼ 50–70 yr. The minimum value of the integral meridional heat transport was attained in the mid-1960s and its maximum value was at attained at the beginning of the 1990s. The location of the center of Azores pressure maximum makes it possible to conclude that the intensification of the total meridional heat transport in the Subtropical Atlantic on these time scales is accompanied by the displacement of the center of the North Subtropical anticyclonic gyre in the southwest direction.  相似文献   

13.
The South China Sea(SCS) and the Arabian Sea(AS) are both located roughly in the north tropical zone with a range of similar latitude(0°–24°N). Monsoon winds play similar roles in the upper oceanic circulations of the both seas. But the distinct patterns of chlorophyll a(Chl a) concentration are observed between the SCS and the AS.The Chl a concentration in the SCS is generally lower than that in the AS in summer(June–August); the summer Chl a concentration in the AS shows stronger interannual variation, compared with that in the SCS; Moderate resolution imaging spectroradiometer(MODIS)-derived data present higher atmospheric aerosol deposition and stronger wind speed in the AS. And it has also been found that good correlations exist between the index of the dust precipitation indicated by aerosol optical thickness(AOT) and the Chl a concentration, or between wind and Chl a concentration. These imply that the wind and the dust precipitation bring more nutrients into the AS from the sky, the sub-layer or coast regions, inducing higher Chl a concentration. The results indicate that the wind velocity and the dust precipitation can play important roles in the Chl a concentration for the AS and the SCS in summer. However aerosol impact is weak on the biological productivity in the west SCS and wind-induced upwelling is the main source.  相似文献   

14.
The parameters of heavily dusty air in an aerosol chamber under the conditions of an arid zone are studied. The transmission, optical density, Angstrom parameter, aerosol absorption coefficient, and visibility range are calculated. The temporal and spectral dependences of the optical parameters are analyzed. The regularities of the particle-size distribution function in strongly inhomogeneous dust aerosol are studied for coarsely (with a diameter more than 1 μm) and finely dispersed (with a diameter of less than 1 μm) fractions. The sizes and concentrations of the aerosol particles in air were determined using a photoelectric aerosol counter together with a 15-channel analyzer. We present the absorption spectra of coarsely and finely dispersed dust aerosol collected under different meteorological conditions. The possible mechanisms of variations in the aerosol disperse composition are analyzed.  相似文献   

15.
The meridional heat transport in the ocean is computed according to the data of zonal sections of the World Ocean Circulation Experiment made in the North Atlantic in 1992–1998. We perform the generalized analysis of the estimates of meridional heat transport obtained by different authors by direct methods on the basis of the data of sections made between 7.5 and 48°N in the second half of the last century. The meridional heat transport averaged over the entire period of observations attains its maximum (1.38 ± 0.19 PW) in the Subtropical Atlantic. The meridional heat transport is characterized by fairly intense seasonal variability. Its maximum (about 1.9 PW) is observed in the Subtropical Atlantic at the end of summer and its minimum (about 0.8 PW) is attained at the end of winter. A significant trend toward the intensification of meridional heat transport is revealed near 36°N in 1959–1993 (from 0.75 to 1.1 PW). This is an indication of the intensification of meridional oceanic circulation in the North Atlantic. Dedicated to the 75th birthday of N. A. Timofeev, Honored Scientist of the Ukraine, Doctor of Geographical Sciences __________ Translated from Morskoi Gidrofizicheskii Zhurnal, No. 1, pp. 45–58, January–February, 2007.  相似文献   

16.
This paper first describes the atmospheric correction algorithm for OCTS visible band data used at NASDA/EOC. Sharing a basic structure with Gordon and Wang’s Sea WiFS algorithm, it uses 10 candidate aerosol models including the “Asian dust model” introduced in consideration of the unique feature of aerosols over the east Asian waters. Based on the observations at 670 and 865 nm bands, the algorithm selects a pair of aerosol models that account best for the observed spectral reflectances, and synthesizes the aerosol reflectance used for the atmospheric correction. Two different schemes for determining the value of the parameter for the aerosol model selection are presented and their anticipated estimation error is analyzed in terms of retrieved water reflectance at 443 nm. The results of our numerical simulation show that the standard deviation of the estimation error of the “weighted average” scheme is mostly within the permissible level of ±0.002, reducing the error by 18% on average compared to the “simple average” scheme. The paper further discusses the expected error under the old CZCS-type atmospheric correction, which assumes constant aerosol optical properties throughout the given image. Although our algorithm has a better performance than the CZCS algorithm, further analysis shows that the error induced by the assumption taken in the algorithm that the water-leaving radiance at 670 nm band is negligibly small may be large in high pigment concentration waters, indicating the necessity for future improvements.  相似文献   

17.
Seasonal variation in the tropical Pacific is studied by use of climatological monthly mean data of upper layer thickness of a linear reduced-gravity model with realistic basin geometry. Complex empirical orthogonal function (CEOF) analysis is applied to the data on a closed circuit which consists of the equator, eastern boundary, 7° latitude, and western boundary. The first and second CEOF represent the annual and semiannual variations, respectively. At the equator, absolute maximum anomalies associated with the first CEOF can be found near 160°W in spring and fall. Westward propagation of the annual variation is remarkable west of 130°W. However, similar westward propagation cannot be detected in either the eastern or western part of the equator. Maximum anomalies at 7° and the equator can be found in similar longitude and time. These maxima at both latitudes originate from the annual variation of Ekman pumping associated with the meridional movement of wind fields. We also decomposed the model results into Kelvin and Rossby modes. The Kelvin mode is characterized by seminnual variation, while first and third-mode Rossby waves have annual variations. In the present results, first and third-mode Rossby waves do not appear to be a trigger for Kelvin waves.  相似文献   

18.
The objective of the paper is to use the data collected along two meridional sections (45° E and 57°30′ E) during the austral summer (January–March) 2004 to understand the influence of seabed topography across the Madagascar and Southwest Indian Ridges on hydrographic parameters. The study was supplemented by World Ocean Circulation Experiment (WOCE) Conductivity-Temperature-Depth data collected during February–March 1996 along 30° E, as well as Levitus climatology. A southward shift of 2° latitude (between 45° E and 57°30′ E) was recorded for the two predominant frontal structures, i.e., the Agulhas Return Front and Southern Subtropical Front, which is attributed to the influence of seabed topography on hydrographic parameters. No significant spatial variation of these fronts was noted between the 30° E and 45° E meridional sections. Between latitudes 31° S and 42° S, the temperature and salinity structures show deepening over the ridges. The Antarctic Circumpolar Current core was detected between 40°15′ S and 43° S.  相似文献   

19.
The temporal variability of the chemical composition of surface aerosol with particle diameters of 0.7–2 μm is analyzed. This analysis is based on the results of measurements of infrared transmission spectra of aerosol samples collected with the use of a cascade impactor at the Zvenigorod Scientific Station of the Institute of Atmospheric Physics (IAP) in 1999–2005. Seasonal features of the aerosol chemical composition and its dependence on the particle size are revealed. The interdiurnal variability of the aerosol composition depends on the season, and it manifests itself more strongly in winter and spring. Air-mass changes lead to changes in the relation of sulfates and nitrates in the micron fraction of aerosol. The enrichment of samples in nitrates is especially characteristic of the winter and spring seasons. Compounds containing the NO2 group are often met in the samples of aerosol with particle sizes of 0.7–1.3 μm during the cold time of the year. The estimates of the optical thickness of micron aerosol in the sulfate absorption band are obtained, and optical-thickness variations of some scales are detected. The quantitative characteristics of statistical relations between different chemical components of aerosol inside individual fractions and between chemical components of the micron and submicron fractions are obtained and analyzed.  相似文献   

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