HY-1 CCD宽波段水色要素反演算法

利用2003年春季黄海、东海区现场实测数据,建立了HY1卫星4波段CCD成像仪水色要素反演算法.由于HY1CCD的宽波段特性阻碍了黄色物质的反演,因此反演的水色要素仅包括水体表层的总悬浮物、悬浮泥沙(SS)以及叶绿素a的浓度.现场遥感反射率光谱由ASD地物波谱仪测量,对于叶绿素a的浓度利用现场萃取荧光法测量,总悬浮物、悬浮泥沙由实验室滤膜称重法获得.反演算法的拟合相关系数均大于0.88,平均相对误差在40%以下.对反演算法进行了误差灵敏度分析,结果表明对于总悬浮物、悬浮泥沙和低浊度水体中的叶绿素a的浓度反演算法能够满足日常的业务运行要求,但是对于高浊度水体中叶绿素a的浓度反演算法对某个波段组合比较敏感,仍需要进一步探讨.     

我国获得美国海星号卫星资料免费接收权

我国获得美国海星号卫星资料免费接收权海洋水色遥感是利用航天或航空传感器上对海洋水色敏感的电磁波来监测海水叶绿素浓度、悬浮泥沙浓度以及海水污染浓度等海洋水色因子，用以评估海洋初级生产力、河口海岸泥沙运输量及过程、海水有害物质含量以及污染源和污染范围，进...     

海水光谱模拟及其在黄色物质遥感反演中的应用

以海洋水色因子(悬浮泥沙、叶绿素、黄色物质)浓度的大量实测资料为主要输入，对水体光谱反射率进行模拟(正演)，进而分析黄色物质浓度与模拟光谱资料的关系，确定提取黄色物质浓度信息的最佳波段组合，并以此波段组合建立黄色物质浓度信息提取模式(反演)。对模拟光谱资料与卫星遥感光谱资料的关系进行了推导，将反演模式应用于卫星遥感资料，并利用SeaWiFS资料提取珠江口水域黄色物质浓度信息，初步实现了海水黄色物质浓度的卫星遥感信息提取。     

台湾海峡及周边海域水色光谱特性分析

利用2006—2007年4次908计划ST06区块海洋光学调查的数据和MODIS水色遥感数据,对台湾海峡及周边海域的水色光谱特性进行了研究和分析。结果显示该海域的水色光谱主要有4个类型:类型1光谱峰值出现在580 nm附近,谱峰两侧遥感反射率随波长变化迅速减小,主要分布在紧靠中国大陆的海域;类型2光谱峰值出现在540～560 nm之间,具有谱峰宽的特点,主要分布在台湾海峡靠近大陆的一侧;类型3光谱与大洋水体光谱类似,主要分布在台湾西南的南海区域和吕宋海峡区域;类型4光谱在.450 nm附近出现极小值,在500～600 nm之间出现峰值,主要出现在台湾海峡中部和靠近台湾岛的一侧。其中类型2和4水体分布具有明显的季节特征。类型3、4、2、1对应的叶绿素a浓度和悬浮泥沙浓度呈上升趋势,对应的透明度依次降低,该海域以二类水体为主。     

基于遥感反演的莱州湾水色变化的多时相分析

悬浮泥沙和叶绿素是海洋水色的重要部分,是反映河口海岸地区生态环境状况的重要指标。本文基于Landsat TM/ETM+/OLI遥感影像,在不依赖地面实测数据的条件下,结合水文气象数据,利用光谱信息建立水色遥感模型对莱州湾1996—2015年不同时期的悬浮泥沙和叶绿素变化进行研究。研究结果表明:(1)此模型可以快速反演出较大空间尺度内的水色时空分布情况。(2)1996—2015年这一时期内悬浮泥沙浓度变化明显,枯水期的悬浮泥沙扩散范围总体大于丰水期,悬浮泥沙高浓度区主要分布在黄河口附近海域和沿岸区域,泥沙主要来源于陆源输沙和海水中的泥沙再悬浮,悬浮泥沙的扩散主要受潮流的影响,风和波浪等动力因素也在一定程度上影响着悬浮泥沙的扩散;(3)此外,莱州湾叶绿素高浓度区主要分布在莱州湾东—南部海域,其分布具有明显的季节性,春季(5月)海水温度升高,水中营养物质垂直混合好使得叶绿素浓度处于较高态势。     

水下光谱辐射测量技术

海水中的叶绿素、泥沙、黄色物质等及其含量直接影响海水的光谱特性。此外，海洋水色遥感算法的建立及验证也离不开现场相关光学参数的测量，准确的海水现场光谱辐射测量，是提高海洋水色定量化遥感精度的重要环节。文章通过开展水下光谱辐射测量方法的讨论、仪器总体方案的设计及相应的试验的结果分析，提出了有关水下光谱辐射测量仪器构成的一些想法。     

基于实测数据的北海区海水表层叶绿素a浓度遥感定量反演

为提高我国海洋水色遥感技术和海水环境监测水平,文章根据北海区海水遥感现场监测数据,基于经验算法和荧光基线高度法的回归分析,开展海水表层叶绿素a浓度的遥感定量反演,并选取北黄海近岸海域样本数据进行算法检验。研究结果表明:辽东湾等9个北海区典型海域具有相同或相似海水表层光学特性,适宜建立海水表层叶绿素a浓度遥感定量反演模型;典型海域海水表层叶绿素a浓度与遥感反射率之间的相关关系较强,模型均为简单波段比值模型;二类海水研究区域海水表层叶绿素a浓度与荧光基线高度之间的相关关系不明显;北黄海近岸海域海水表层叶绿素a浓度的最优模型遥感定量反演值的相对误差的平均值为0.669μg/L。     

CMODIS资料提取叶绿素a浓度的反演算法研究

中分辨率成像光谱仪(CMODIS)是我国“神舟3号”飞船上对地观测主载荷,是我国第一台上天的具有测量海面叶绿素a浓度能力的成像光谱仪.利用宽视场海洋水色扫描仪(SeaWiFS)反演叶绿素a浓度作为参考值建立CMODIS资料处理模型,得到三个基于蓝绿波段比值法的叶绿素a浓度反演算法,平均相对误差分别为26.6%,24%和33.5%,均方根误差分别为1.16,1.15和1.23 mg/m3.在叶绿素a浓度反演误差允许范围小于35%的条件下,比值算法的适用范围为悬浮泥沙浓度小于5 g/m3的海区.悬浮泥沙的强散射作用导致比值算法在高悬浮泥沙浓度条件下产生高估叶绿素a浓度反演值的现象;在中低悬浮泥沙浓度的海区,悬浮泥沙和浮游植物对离水辐亮度的综合作用使比值算法存在低估叶绿素a浓度的趋势.     

黄、东海二类水体春季表观光谱特性与表层悬浮体浓度反演模式

利用Savitzky-Golay滤波信号处理方法,分析了南黄海、北东海2003年春季水色遥感试验所取得的遥感反射率和表层悬浮体取样数据,以期探讨该海区近岸二类水体表观光谱及其导数光谱特性,及遥感反射率及其导数与水体表层总悬浮颗粒物浓度(TSS)和悬浮泥沙浓度(SS)的关系。结果表明,遥感反射率及其一阶导数均适于水体总悬浮颗粒物浓度与悬浮泥沙浓度反演,但其更高阶导数通常会抑制悬浮泥沙的作用则不建议采用;遥感反射率及其一阶导数与ln(TSS)、ln(SS)的相关性较其与TSS和SS更为显著。基于相关分析所筛选出的较优波段,建立了南黄海、北东海水域春季总悬浮颗粒物浓度与悬浮泥沙浓度统计反演模式。     

基于Landsat8数据的舟山群岛海域悬浮泥沙浓度遥感研究

文章利用舟山近岸海域实测水体光谱及泥沙浓度数据，分析光谱反射率与悬浮泥沙浓度的相关性，并结合Landsat8遥感数据进行该海域的悬浮泥沙浓度遥感反演。研究表明：随着水体悬浮泥沙浓度的增加，各波段的反射率相应增加，且不同波段的增幅有明显不同，水体光谱曲线存在“双峰”现象；Landsat8遥感数据的波段4与波段3的比值与悬浮泥沙浓度的相关性较好；舟山群岛海域总体处于高泥沙浓度的状态，岛屿近岸悬浮泥沙浓度明显高于开阔水域，岛屿周围的悬浮泥沙浓度呈现“西高东低”的格局；一元二次方程模型（二次模型）对舟山海域水体的悬浮泥沙浓度反演精度较其他模型（线性模型，对数模型，指数模型，幂指数模型）高；Landsat8遥感数据可用于舟山海域悬浮泥沙浓度的监测。本研究成果能为近岸海域港口建设、航道安全、环境监测等研究提供数据支持。     

渤海湾海水光谱特性的数值分析——复相关分析

一、序言 从遙感信息中提取海洋信息是海洋遙感应用的核心问题。 从遙感数据提取海洋数据,现在已经有很多方法与模型。各种方法都有它们的长处和短处。从目前发表的遙感文章来看,大多还是使用数理统计模型。它的优点是方法比较简单,且比较精确。缺点是有很大的局限性,它的结果只有在特定的海区、特定的大气条件和飞行     

Estimation of chlorophyll concentration from the specific fluorescence at 685nm in the upward irradiance just below the sea surface

An algorithm for estimating the chlorophyll concentration from the fluorescence intensity at 685nm in upward irradiance observed just below the sea surface is presented and discussed. The observed chlorophyll concentration is closely related to the ratio of the fluoresced quanta to the total incident quanta (downward plus upward quanta) in the spectral range between 350nm and 600nm. The correlation between them, however, is not good and the rate of increase of the ratio decreases as the chlorophyll concentration increases. This is due to the fact that the number of fluoresced quanta varies with attenuation of the incident light by various materials in the sea.A better correlation is obtained between the ratio of the fluoresced quanta to the upward quanta at wavelengths around 480nm. This is explained by the fact that dividing by the upward quanta at the appropriate wavelength compensates for apparent variation of fluorescence intensity with attenuation by the sea water. In this method, upward quanta at the four wavelengths of 480nm, 640nm, 685nm and 740nm are necessary for estimation of chlorophyll concentration. The quanta at 640nm and 740nm are used for interpolating the quanta at 685nm in the absence of fluorescence.It is also shown that the correlation of the observed chlorophyll concentration with the ratio of upward quanta at the wavelengths of 685nm and 480nm is also good. Use of this ratio is recommended for remote sensing of chlorophyll concentration since the number of spectral channels required by the remote multispectral imager can be minimized.     

渤海湾航空遥感的图象分析——渤海湾近岸叶绿素A分布图

1980年9月6日,中国科学院组织十多个部门、几十个单位在津渤地区进行第二阶段环境污染航空遥感联合试验第二航次试验,中国科学院海洋研究所参加了在渤海湾海河、蓟运河口的海上试验。这次试验,空中由双水獺512飞机装载RMK相机进行彩色红外摄影,航高3800米。航速240公里/小时,摄影比例尺1:25000,相幅面积230毫米×230亳米,飞行航线示于图1。海上由“津塘护1号”、“交津研1号”、“海调105号”、“金星”轮等4条船只进行同步观测、取样。     

Analysis of ocean color spectra (III)

The spectral measurements of the attenuation coefficient of sea water and the absorption coefficient of suspended particles and of yellow substance were made with a spectrophotometer for the sea waters sampled in Tokyo Bay. These parameters can be used to compute the expected spectral irradiance reflectance. Some relationships between the optical properties of sea water and the concentration of dissolved organic carbon, the dry weight of suspended matter and chlorophyll-a concentration are presented. On the basis of these results, the possibility of modelling the relationship between optical and material properties is discussed.     

珠江口藻华水体总吸收系数的变化特性及高光谱反演模式

基于2007年8月海洋光学浮标在珠江口投放期间获得的近16天的实测生物光学数据, 对一次藻华过程中水体总吸收系数和水色光谱的变化特性及其相互关系进行了研究。结果表明, 藻华前后水体中非藻类物质尤其是有色溶解有机物在蓝光波段具有较强的吸收贡献, 而当藻华爆发时, 随着叶绿素a浓度的急剧增大, 浮游植物的吸收贡献明显增强; 各波段之间总吸收系数呈现出较好的线性相关关系, 吸收光谱蓝绿波段比值的变化对遥感反射率的光谱分布有重要的贡献; 据此建立了对水体总吸收系数反演的经验关系模型, 表现出较高的反演精度, 计算值与实测值之间相对偏差的均方根在可见光波段可控制在24%以内。     

海水现场水色色度及渤海水域水色色度分析

叙述了目前海水现场水色测量的弊端 ,指出数字化海洋水色的潜在应用价值 ;根据色度学及色度学的三原色基本理论 ,确定海洋现场水色的色度要素 ,使海洋现场水色标号统一为物理学中严格的颜色物理量。结合 1 996年渤海水域光谱反射测量 ,对渤海水域 4个典型站位的反射光谱做了水色色度分析 ,并进行了 2种测量方法的比较     

Relationship between the Beam Attenuation Coefficient and the Concentration of Suspended Matter in Black-Sea Waters

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.     

The vertical attenuation of light in Charlotte Harbor, a shallow, subtropical estuary, south-western Florida

The relative contribution of different components to the attenuation of photosynthetically active radiation was determined in the Charlotte Harbor estuarine system based on laboratory and in situ measurements. Agreement between laboratory and in situ measurements of the attenuation coefficient (k_t) was good (r² = 0·92). For all in situ measurements (n = 100), suspended, non-chlorophyll matter accounted for an average of 72% of k_t, dissolved matter accounted for 21%, suspended chlorophyll for 4%, and water for the remaining 3%.For individual determinations, suspended non-chlorophyll matter, dissolved matter, suspended chlorophyll, and water, each accounted for as much as 99%, 79%, 21%, and 18% of k_t. Attenuation by suspended matter was greatest near the mouth of the northern tidal rivers and was variable over the rest of the estuarine system. Attenuation by dissolved matter was greatest in the brackish tidal rivers and decreased with increasing salinity. Attenuation due to dissolved matter was positively correlated with water color. The source of the color was basin runoff. Wavelength transmittance changed along the salinity gradient. Maximum transmittance shifted from 500 to 600 nm in gulf waters to 650 to 700 nm in colored, brackish waters. Dissolved matter was primarily responsible for the large attenuation at short wavelengths (400–500 nm).     

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.