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1.
自然界各种物体,都有表征其自然属性的光谱特性。地物的光谱特性是遥感图象定性判读的依据之一,它作为一种遥感信息也直接用于定量测定和制图。 海水中悬浮物质的数量和性质影响海水的颜色和海水的光谱特性。反之,根据海水的光谱特性可以测定水中悬浮物质的数量和性质。1974年, S. D. Duntley首先从海洋叶绿素的光谱效应,提出根据海水的光谱反射率曲线,用卫星传感器测定水中叶绿素a 浓度的理论。1978年, R. W. Johnson 建立了航空遥感的光谱数据与沿岸带海洋叶绿素a 浓度之间的数学关系,并绘制了叶绿素a的分布图。1979年, R. W. Johnson建立了光谱数据与悬浮泥沙含量之间的数学关系,并绘制了悬浮泥沙的定量分布图,等等。本文的目的即是要建立一种方法,用国产101W光谱辐射计记录的遥感数据,计算海域悬浮泥沙、叶绿素a 浓度、水色等水质参数。 1980年5月16日至19日,由中国科学院组织,有中国科学院海洋研究所、国家海洋局第一海洋研究所、第二海洋研究所、交通部天津水运科学研究所、水利部天津水利科学研究所等单位参加,在天津塘沽的海河和蓟运河口进行津、渤地区第一次环境污染航空遥感监测联合试验。在此次试验中用机载101W光谱辐射计记录海水的光谱辐射曲线,作者以此计算海水的光谱反射率曲线,用逐次回归分析法建立海洋实测数据(悬浮泥沙、叶绿素a浓度、水色等)与海水光谱反射率数据之间的数学关系。实验基本是成功的,由回归方程计算的结果与海洋实测数据之间的相关系数约为0.7。如果对研究海域的每一个子域的辐射值作光谱扫瞄,作出定量的分布图也是可行的。  相似文献   

2.
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.  相似文献   

3.
Besides empirical algorithms with the blue-green ratio, the algorithms based on fluorescence are also important and valid methods for retrieving chlorophyll-a concentration in the ocean waters, especially for Case II waters and the sea with algal blooming. This study reviews the history of initial cognitions, investigations and detailed approaches towards chlorophyll fluorescence, and then introduces the biological mechanism of fluorescence remote sensing and main spectral characteristics such as the positive correlation between fluorescence and chlorophyll concentration, the red shift phenomena. Meanwhile, there exist many influence factors that increase complexity of fluorescence remote sensing, such as fluorescence quantum yield, physiological status of various algae, substances with related optical property in the ocean, atmospheric absorption etc. Based on these cognitions, scientists have found two ways to calculate the amount of fluorescence detected by ocean color sensors: fluorescence line height and reflectance ratio. These two ways are currently the foundation for retrieval of chlorophyl l - a concentration in the ocean. As the in-situ measurements and synchronous satellite data are continuously being accumulated, the fluorescence remote sensing of chlorophyll-a concentration in Case II waters should be recognized more thoroughly and new algorithms could be expected.  相似文献   

4.
The hydrographic and bio-optical properties of the Bering Sea shelf were analyzed based on in-situ measurements obtained during four cruises from 2007 to 2009. According to the temperature and salinity of the seawater, the spring water masses on the Bering Sea shelf were classified as the Alaskan Coast Water, Bering Sea Shelf Water, Anadyr Water, Spring Mixed Layer Water, Remnant Winter Water, and Winter Water, each of which had varying chlorophyll a concentrations. Among them, the highest chlorophyll a concentration occurred in the nutrient-rich Anadyr Water ((7.57±6.16) mg/m3 in spring). The spectrum-dependent diffuse attenuation coefficient (Kd(λ)) of the water column for downwelling irradiance was also calculated, exhibiting a decrease at 412–555 nm and then an increase within the range of 0.17–0.48 m–1 in spring. Furthermore, a strong correlation between the chlorophyll a concentration and the attenuation coefficient was found at visible wavelengths on the Bering Sea shelf. Spatially, the chlorophyll a concentration was higher on the northern shelf ((5.18±3.78) mg/m3) than on the southern shelf ((3.64±2.51) mg/m3), which was consistent with the distribution of the attenuation coefficient. Seasonally, the consumption of nutrients by blooms resulted in minimum chlorophyll a concentration ((0.78±0.51) mg/m3) and attenuation coefficient values in summer. In terms of the vertical structure, both the attenuation coefficient and the chlorophyll a concentration tended to reach maximum values at the same depth, and the depth of the maximum values increased as the surface temperature increased in summer. Moreover, an empirical model was fitted with a power function based on the correlation between the chlorophyll a concentration and the attenuation coefficient at 412–555 nm. In addition, a spectral model was constructed according to the relationship between the attenuation coefficients at 490 nm and at other wavelengths, which provides a method for estimating the bio-optical properties of the Bering Sea shelf.  相似文献   

5.
叶绿素荧光遥感算法为探测近岸海域二类水体叶绿素浓度开辟了新途径.基于大连湾及邻近海域的实测数据,本文研究了海水叶绿素浓度的荧光遥感算法.结果表明:随着海水叶绿素质量浓度的增高,荧光峰出现显著的红移现象,叶绿素质量浓度与荧光峰波长存在着正相关关系.此外,基于MODIS、MERIS及GLI传感器荧光波段建立的荧光基线高度算法较差,不适用于该研究海域.选择680、685、690、695、700、705nm作为荧光峰波长建立的荧光基线高度算法,随着选定波长的增大,该算法拟合的相关性逐渐增高,最大相关系数(R2)可达0.91;而以实测荧光峰波长建立的荧光基线高度算法最佳,乘幂函数拟合优于线性拟合,拟合方程为P(chl)=3.167×10^5 FLH^1.45(R2=0.93).本研究为新一代海洋水色卫星传感器的开发、建造提供了科学依据,并为已有高光谱传感器在叶绿素荧光遥感反演方面的应用打下了基础.  相似文献   

6.
珠江口水体叶绿素荧光特性研究   总被引:3,自引:0,他引:3  
利用2003年1月和2004年1月珠江口实测的遥感反射率和叶绿素浓度,建立了基于实测1nm带宽及其模拟MERIS遥感反射率数据的叶绿素荧光特征与叶绿素浓度之间的拟合关系。基于实测1nm带宽遥感反射率光谱,叶绿素荧光峰的位置和高度分别与叶绿素浓度之间存在良好的线性关系和指数关系;基于模拟MERIS遥感反射率数据,叶绿素荧光峰的高度与叶绿素浓度之间存在良好的线性关系,叶绿素荧光峰位置与叶绿素浓度之间不存在明显的相关关系,但可作为叶绿素浓度数量级的有效探针。利用2006年5月和8月的珠江口实测遥感反射率和叶绿素浓度对拟合结果进行了检验,结果表明其精度较高,说明叶绿素荧光特征在探测叶绿素浓度时效果良好且MERIS数据在近岸二类水体叶绿素浓度反演、水质监测等方面有着良好的应用前景。  相似文献   

7.
By using the results of simultaneous measurements of the beam attenuation coefficient and the concentration of suspended matter in water samples, we deduce the relationships between these parameters for wavelengths of 640, 660, and 677 nm. The proposed formulas are used for the evaluation of the concentration of suspended matter according to the data of optical measurements performed in cruises of research vessels. We present two maps of the distribution of suspended matter plotted for the north part of the sea in November–December 1991 and for the south part of the sea in July 1992.  相似文献   

8.
辐射传输模式HydroLight是研究水体辐射传输特性的有效工具,同时也是进行石油类水体辐射传输特性的有效模型。本文基于2018年8月在辽宁大连港海域实测的石油类污染水体的表观及固有光学量数据,通过设置不同浓度的配比模拟试验,利用HydroLight对油类物质和藻类物质的单一组分和两者混合水体的遥感反射比(remote sensing reflectance,Rrs)光谱进行了模拟。模拟结果表明:(1)在仅含油类物质单一组分的水体中,Rrs随着油浓度Coil的变化分为两个特征波段:400~480 nm和480~700 nm。在400~480 nm波段范围内RrsCoil的增加而减小,在480~700 nm随Coil的增大而增大;(2)在仅含藻类物质的单一成分水体中,叶绿素的光谱特性需要其浓度Cchl达到一定值才能表现出来,在低Cchl时的Rrs光谱特性反映为纯水的光谱特性;(3)在油藻混合水体中,随Coil的增加会增大叶绿素的Rrs,但不会明显改变叶绿素的Rrs随波长的变化趋势,这说明油藻混合水体的光谱形状主要受叶绿素的影响,油类物质的存在只改变光谱的量值。利用HydroLight对石油类污染水体的Rrs展开研究,有助于丰富水色遥感基础研究,对完善各类水体生物光学模型研究具有重要的理论意义。  相似文献   

9.
采用现场实测和室内培养两种方式测定了甲藻、赤潮异弯藻、叉角藻、海洋蓝绿藻等赤潮和新月菱形藻、叉鞭金藻、塔胞藻、扁藻和小球藻等非赤潮藻类光谱曲线.采用度量太阳激发的叶绿素荧光峰高度的归一化荧光高度法,建立了不同藻类归一化荧光高度与叶绿素浓度的关系.荧光高度计算方法是将红光波段的反射率最大值(Rmaxred)和R685分别归一化到560 nm处的R560和560 nm附近整个光谱曲线的最大值R560 max上或675 nm处的R675和675 nm附近的最小值R675mini上.结果表明,不同藻类的Rmaxred/R560max和Rmaxred/R675mini与叶绿素a的相关系数分别比R685/R560和R685/R675与叶绿素的相关系数高,但在海洋现场测量中由于近岸二类水体其他水色组分以及大气校正误差的影响,Rmaxred/R675mini和R685/R675更适合于实测的叶绿素浓度估算.采用三种统计回归方程建立了不同藻类归一化荧光高度与叶绿素浓度关系,除个别藻种外,大部分的相关系数在0.9以上,其中FLH=a+(Chla)b回归方程得到的相关系数优于其他两种方法,相关系数大于0.93,这表明藻类水体的荧光特性和叶绿素浓度之间的普遍关系是非线性的.  相似文献   

10.
水下光谱辐射计光学特性的测试与分析   总被引:1,自引:0,他引:1  
为适应高精度水下光学测量的需求,设计研制了多通道水下光谱辐射计。该辐射计可同步测量12波段的下行/上行光谱辐照度和7波段的上行光谱辐亮度。对该辐射计的主要性能指标,如余弦响应特性、浸没因子、光谱辐射精度、稳定性和重复性进行了室内测试和分析,用MonteCarlo方法模拟了阴影误差,给出并分析了现场实验数据及部分推导的物理量。结果表明,该光谱辐射计各波段的中心波长和带宽偏差小于1.6nm,稳定性优于5%,阴影误差可控制在5%之内,具有良好的余弦响应特性,满足当前定量化水色遥感现象光辐射测量的技术要求。  相似文献   

11.
两种荧光分析法在海洋浮游植物叶绿素测定中的应用   总被引:3,自引:0,他引:3  
以湛江叉鞭金藻为材料.用普通荧光分析法测定了chla、chic的荧光发射光谱,以四乳突扁藻为材料,用普通荧光分析法和同步荧光分析法测定了chla、chlb的荧光发射光谱,结果表明:chla、chlb、chic的荧光发射峰分别为670nm、655nm、640nm,普通荧光分析法适于进行浮游植物所含的chla、chlc的定性、定量测定,而不适于进行chla、chlb的同时测定;同步荧光法则适于进行浮游植物中chla、chlb的定性、定量的同时测定。  相似文献   

12.
基于高光谱遥感的渤海海冰厚度半经验模型   总被引:1,自引:0,他引:1  
Sea ice thickness is one of the most important input parameters for the prevention and mitigation of sea ice disasters and the prediction of local sea environments and climates. Estimating the sea ice thickness is currently the most important issue in the study of sea ice remote sensing. With the Bohai Sea as the study area, a semiempirical model of the sea ice thickness(SEMSIT) that can be used to estimate the thickness of first-year ice based on existing water depth estimation models and hyperspectral remote sensing data according to an optical radiative transfer process in sea ice is proposed. In the model, the absorption and scattering properties of sea ice in different bands(spectral dimension information) are utilized. An integrated attenuation coefficient at the pixel level is estimated using the height of the reflectance peak at 1 088 nm. In addition, the surface reflectance of sea ice at the pixel level is estimated using the 1 550–1 750 nm band reflectance. The model is used to estimate the sea ice thickness with Hyperion images. The first validation results suggest that the proposed model and parameterization scheme can effectively reduce the estimation error associated with the sea ice thickness that is caused by temporal and spatial heterogeneities in the integrated attenuation coefficient and sea ice surface. A practical semi-empirical model and parameterization scheme that may be feasible for the sea ice thickness estimation using hyperspectral remote sensing data are potentially provided.  相似文献   

13.
In order to evaluate near-surface water quality parameters from spectral irradiance reflectance observed just below the surface, models of both radiative transfer and optical properties of sea water are used. The computed water quality parameters are compared with those determined directly from concurrent surface water samples. In this comparison, efforts have been made to minimize the number of spectral irradiance reflectance used in the computation while ensuring that the computed water quality parameters fit well to the observed ones.The observed water quality parameters were found to be closely represented by those computed from the irradiance reflectance at wavelengths of 400 nm, 440 nm, 510 nm and 600 nm, and the fit is as good as the fit of observed water quality parameters to those computed from the irradiance reflectances at 151 wavelengths located between 400 nm and 700 nm at intervals of 2 nm. This implies that the water quality parameters can be evaluated from at least four radiances observed at high altitude, if the effects of the atmosphere and the sea surface can be correctly removed.  相似文献   

14.
杨广普  江涛  赵永芳  黄珏 《海洋学报》2019,41(1):183-190
水体中叶绿素a的含量是研究浮游植物生物量、初级生产力的重要指标,因此对于河口海湾区域叶绿素a的长期监测具有重要的生态学意义。借助遥感技术能够获取长时序大范围观测数据的特点,本文利用1986-2015年的Landsat TM/ETM+影像,通过构建基于实测数据的定量反演模型,得到了30年来胶州湾海域秋季叶绿素a浓度的分布情况:叶绿素a浓度的空间分布规律稳定,呈现西北高东南低的特点,叶绿素a浓度均值呈波动略有上升的趋势。本文利用遥感反演的胶州湾海表面温度及胶州湾流域的土地利用分类和景观格局指数,从自然因素和人为因素两方面对胶州湾叶绿素a浓度时空分布的影响因素进行分析,发现胶州湾秋季叶绿素a浓度与海表面温度密切相关,并且受到近海养殖区破碎化程度、修建大型人工设施等人为因素的影响。  相似文献   

15.
利用加拿大环极冰间水道系统研究项目,作者对2007年11月24日至2008年1月26日北极群岛阿蒙森湾海域秋冬季节一年冰的物理和光学性质进行了观测研究。结果显示,观测期间的海冰厚度整体在27~108 cm范围内变化,积雪厚度仅为0~6 cm。海冰温度、盐度和密度在冰内的分布特征为:海冰表层最低温度为–22.4℃,底层最高温度为–2.2℃,冰内温度随深度单调增大;盐度变化范围为3.30~11.70,冰内盐度剖面呈现“C”形,即表层和底层盐度较大,而中间层盐度较小;海冰的平均密度略大,为(0.91±0.03)g/cm3。通过观测人造光源在海冰中的透射辐射谱分布,发现一年冰的光谱透射辐射在490 nm和589 nm处呈明显的双峰结构,但随着海冰厚度的增加,双峰结构逐渐减弱,体现了海冰对于不同谱段辐射能衰减作用的差异。在可见光范围内,裸冰和雪覆冰的吸收率最小值出现在490 nm,在443~490 nm范围内二者的吸收率随波长增大而降低,在490~683 nm范围内二者的吸收率随波长增大而升高,但雪覆冰的吸收率在可见光范围内基本保持不变,体现了雪覆冰吸收率的光谱独立性。一年冰的谱衰减系数随波长呈“U”字形分布,紫光和红光谱段的衰减系数较大,中间谱段的衰减系数较小,589 nm波长的衰减系数最小,为1.7 m–1。将谱衰减系数在可见光范围内积分,得到一年冰的积分漫射衰减系数约为2.3 m–1,略高于多年浮冰的漫射衰减系数1.5 m–1。阿蒙森湾一年冰与加拿大海盆北部多年浮冰辐射光学性质的差异,主要源于陆源物质输入引起的海冰内含物组分的改变,而不同组分对光谱的吸收和散射性质不同,进一步导致了光学性质的整体变化。  相似文献   

16.
浮游植物的粒级结构是一个重要的生物参数。基于南海北部海区不同水体环境下测量的生物光学数据, 作者深入研究了粒级结构对浮游植物吸收光谱的影响。结果表明, 选择443和510nm波段计算得到的浮游植物光谱斜率S对粒级结构的变化具有较高的敏感性, 其随着小型浮游植物比例的增大呈不断增加的趋势。S与水体叶绿素a浓度、浮游植物吸收系数(aph(443))之间表现出明显的正相关特征。以40%为界对不同粒级浮游植物的优势进行定义, 发现在S与叶绿素a浓度、aph(443)的关系分布中小型(Micro)和微微型(Pico)浮游植物占据优势的水体表现出较为明显的分界, 叶绿素a浓度和aph(443)分别在0.70mg•m-3和0.05m-1附近, 相应的S在0.0004(m•nm)-1左右。基于实测数据建立的遥感反射率蓝绿波段比值与S之间的统计关系, 决定系数高达0.91, 为从水色遥感数据反演浮游植物粒级结构提供了重要手段。  相似文献   

17.
Remote sensing and surface POC concentration in the South Atlantic   总被引:1,自引:0,他引:1  
Several SeaWiFS products have been compared with shipboard data to assess the possibility of using remote sensing to estimate particulate organic carbon (POC) concentration in surface waters. Transmissometer data were collected during six South Atlantic Ventilation Experiment (SAVE) hydrographic expeditions conducted between November 1987 and March 1989 from R/V Knorr, and Melville. A total of 361 beam attenuation profiles were made with a SeaTech transmissometer interfaced with a CTD/rosette. In order to calculate the POC concentration from transmissometer profiles, a regression between beam attenuation and POC for open Atlantic Ocean waters derived from our research in the North Atlantic (North Atlantic Bloom Experiment, NABE) and enhanced by data from the Bermuda Atlantic Time Series Station (BATS) was applied. The profiles were processed and examined as vertical sections of the surface 250 m. The data were collected in two successive years, during the same season, which allowed us to compile a combined data set over the austral summer for examination. Beam attenuation/POC concentrations were integrated down to one attenuation depth with the intent of making comparisons with satellite optical data. No satellite optical data were available for 1987–1989, so the only option was to compare our integrated data with SeaWiFS-derived variables from later years averaged over the same season as SAVE data. Analysis of four SeaWiFS products acquired from 1997 to 2002 demonstrated very low variations from year to year for seasonally averaged data, suggesting that making comparisons of the beam attenuation/POC fields with averaged satellite optical products from later years is a valid (though not optimal) approach for this area. The highest correlation between beam attenuation/POC concentration and remotely derived products was found with normalized water-leaving radiance at 555 nm. Other SeaWiFS-derived variables—chlorophyll concentration, diffuse attenuation coefficient at 490 nm and integral chlorophyll (integrated over one attenuation depth)—were also compared but showed a slightly less satisfactory correlation.  相似文献   

18.
UVR and PAR wavelengths are attenuated to different extents within the water column, causing variations in spectral composition with depth. The present investigation (a) describes the variability of UVR and PAR penetration at a station in the temperate coastal waters of Sagami Bay and determines (b) the characteristics of relative UVR penetration to the euphotic zone. Examination of the seasonal irradiance profile measurements indicated eight measurements displaying two distinct attenuation coefficients (K d) for specific UVR wavelengths and PAR. The two attenuation coefficients observed from specific wavelengths in the water column may be caused not only by chlorophyll pigments, but also by dissolved organic material in the upper layer. The 1% depth of surface UVR at 305, 320, 340, and 380 nm averaged 10.8 ± 5.7, 14.9 ± 9.5, 19.8 ± 12.1, and 30.4 ± 17.6 m, respectively. The depth of euphotic layer displayed less variability averaging 62 ± 15 m throughout the entire study. Relative UVR penetration within the euphotic zone averaged 17.8 ± 8.1, 22.9 ± 10, 30.5 ± 13.8, and 46 ± 46.9% for 305, 320, 340, and 380 nm, respectively. A large variation of the relative transmission of UVR within the euphotic zone was found although the spectral composition was relatively stable in the air throughout the study.  相似文献   

19.
大亚湾水体后向散射比率的光谱变化   总被引:1,自引:0,他引:1       下载免费PDF全文
采用2007年5月大亚湾浮标定点航次采集的生物-光学数据, 分析了大亚湾水体后向散射比率的光谱变化及其影响因素。分析结果表明, 660nm处后向散射比率变化范围在0.0040—0.0245之间, 均值为0.0082±0.0032, 实测后向散射比率光谱波段间的相对变化不超过15%; 颗粒后向散射比率随着叶绿素a浓度增加呈减小的趋势, 高叶绿素浓度显著对应较低的后向散射比率; 粒径是影响大亚湾水体后向散射比率的重要因素之一, 随着水体中Junge粒级斜率的增大, 颗粒后向散射比率显著增大; 折射率的变化也对后向散射比率产生一定影响, 类似的水体粒径分布情况下, 浮游植物与非藻类物质相对贡献的变化将导致折射率的明显变化, 并将主导水体后向散射比率的变化。  相似文献   

20.
东海原甲藻(Prorocentrum donghaiense Lu)是我国东海海域的典型赤潮藻种,其在水体中通常呈垂直非均匀分布,并存在季节性和日内的垂直迁移现象。本文通过量化垂直迁移过程中东海原甲藻的分布状态,利用Hydrolight软件数值模拟各状态下的水体反射光谱,研究其光谱特征和变化规律。利用叶绿素浓度高斯垂向模型表征东海原甲藻在水体中的垂直分布,结合东海近岸海域二类水体的生物光学模型,模拟得到垂直迁移过程中东海原甲藻赤潮水体的反射光谱。对比分析叶绿素浓度垂向分布参数(背景叶绿素浓度、甲藻主体水层厚度、水体总生物量和叶绿素浓度峰值深度)对水体反射光谱的影响。研究结果表明,在东海原甲藻从次表层向表层垂直向上迁移过程中,水体反射光谱数值在蓝绿波段(400—570nm)减小,在黄红波段(570—720nm)增大,特别是在叶绿素荧光效应波段(680nm)处的变化尤为明显。  相似文献   

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