基于HICO模拟数据的杭州湾水体悬浮物浓度遥感反演
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Retrieval of total suspended matter concentration in Hangzhou Bay based on simulated HICO from in situ hyperspectral data
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通讯作者: 马万栋(1977-),男,正高级工程师,博士,主要从事水环境遥感研究。Email:mawdcn@163.com。
责任编辑: 陈理
收稿日期: 2017-04-6 修回日期: 2017-05-23 网络出版日期: 2018-12-15
基金资助: |
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Received: 2017-04-6 Revised: 2017-05-23 Online: 2018-12-15
作者简介 About authors
禹定峰(1986-),男,副研究员,博士,主要从事水色遥感研究。Email:
以杭州湾及其邻近海域为研究区,利用现场实测光谱模拟了近海高光谱成像仪(hyperspectral imager for the coastal ocean,HICO)波段,并在光谱特征分析的基础上确定特征波段,通过比较单波段、波段比值和反射峰面积等算法,建立了该海域悬浮物的遥感反演模型,并采用均方根误差和相对误差进行精度评价。研究结果表明,利用724.84 nm与461.36 nm波段光谱反射率比值建立的模型精度较高; 模型的决定系数为0.925 2,反演得到的悬浮物浓度与实测悬浮物浓度之间的均方根误差为14.09 mg/L,平均相对误差为5.2%。本研究对利用HICO模拟数据反演近海岸水体悬浮物具有一定的参考意义。
关键词:
In this study, field data such as the concentration of total suspended matter (TSM) in Hangzhou Bay and its adjacent areas in Hangzhou’s coastal waters were observed, meanwhile, hyperspectral remote snesing data were measured with SVC GER1500 spectrometer during four cruises carried out on 20th, 22nd, 23rd and 24th July 2010. The coastal water-leaving refectance of HICO was simulated from in situ hyperspectral remote sensing spectra. The normalized peak area of remote sensing reflectance in the near-infrared region was applied to retrieving TSM after the spectra of simulated HICO were analyzed, as well as the application of single band model and band ratio model. The result indicated that the band ratio algorithm of Rrs(724.84)/Rrs(461.36) of HICO could be used to retrieve TSM in Hangzhou Bay. This study is helpful to retrieving TSM in coastal waters using HICO.
Keywords:
本文引用格式
禹定峰, 周燕, 马万栋, 盖志刚, 刘恩晓.
YU Dingfeng, ZHOU Yan, MA Wandong, GAI Zhigang, LIU Enxiao.
0 引言
悬浮物浓度遥感反演算法主要分为经验算法和半分析算法2类。经验算法利用遥感数据与实时或准实时的地面观测悬浮物浓度数据,建立其间的统计回归模型[4]。该算法具有简单易用,估算精度较高的优点,但2类水体的光学特性复杂多变,具有很强的季节性和区域性特点。半分析算法基于光在水下的辐射传输理论,通过光谱反射率推算水体组分的吸收系数和散射系数,构建悬浮物含量和水体固有光学参数的关系,以估算水体悬浮物浓度,该算法具有较好的物理解释和适用性。但是,受到各种观测仪器的限制,该算法中很多参数以现有的设备无法获取,因此很难广泛应用[5]。此外,模型中某些参数常通过经验或半经验的方法计算,从而影响模型的精度[6]。由于近岸水体光学性质复杂及悬浮物组分多变,应用半分析算法反演水体悬浮物浓度仍然存在难度,目前仍以经验算法为主[7],常用算法有单波段算法、波段比值算法、多波段算法与光谱微分法。Ahn等[8]利用625 nm波段成功地估算了我国黄海外海的悬浮物浓度; 宋庆君等[9]对比研究了悬浮物浓度与实测遥感反射波谱数据之间的相关性大小,发现750 nm处的反射率值与其相关性最高,据此构建了适用于秋季太湖的单波段反演算法,取得了较好的效果; Ma等[10]通过对珠江口水体悬浮物浓度与实测高光谱反射率的关系研究发现,利用810 nm波段处的反射峰及其邻近的吸收谷所围成的面积反演水体悬浮物浓度具有较高的反演精度。
1 数据与方法
1.1 数据获取
图1
图2
1.2 数据处理
由于350~1 000 nm以外的波段易受仪器本身的影响,可能含有噪声,故选用400~900 nm波段光谱进行研究。采用累加平均方法将仪器所测的原始光谱模拟计算出HICO数据的光谱,计算公式为
式中:
表1 HICO主要参数
Tab.1
参数 | 性能 |
---|---|
轨道 | 近圆形轨道 |
倾角/(°) | 51.6 |
轨道高度/km | 343 |
重返周期/d | 3 |
视场角/(°) | 6.92 |
幅宽/km | 42 |
波谱范围/nm | 360~1 080 |
波段数/个 | 128 |
光谱分辨率/nm | 5.7 |
空间分辨率/m | 100 |
信噪比 | >200 |
偏振灵敏度/% | <5(430~1 000 nm) |
数据格式 | BIL,BSQ,HDF5 |
1.3 精度评价
采用统计方法作为检验反演值和实测值是否一致的标准。统计标准分别采用均方根误差(root-mean-square error,RMSE)和相对误差(relative error,RE)2种,表达式分别为
式中:
2 结果与分析
2.1 光谱特征分析
由实测光谱模拟得到的HICO光谱曲线如图3所示。
图3
图3
19个站点的模拟HICO光谱反射率曲线
Fig.3
Spectral cuves of simulated HICO at 19 stations in Hangzhou Bay
2.2 单波段算法
单波段算法适用于光谱反射率与悬浮物浓度密切相关的情况,实测悬浮物浓度与模拟HICO光谱反射率的相关系数如图4所示。
图4
图4
模拟HICO光谱反射率与悬浮物浓度之间的相关系数
Fig.4
Correlation coefficients between TSM concentration and single bands of simulated HICO
由图4可以看出,悬浮物浓度与HICO光谱反射率呈明显的正相关,这是因为当水体中的悬浮物浓度较高时,水体的后向散射较大,从而离水辐射也增加,光谱反射率也会相应增加。随着波长的增加,光谱反射率与悬浮物浓度的相关性也在逐渐增大,这是因为随着波长的增加,水体中悬浮颗粒物和有色可溶性有机物的吸收系数占总吸收系数的比例在逐渐减小。
根据杭州湾海域现场测量得到的水体光谱数据和同步实测的悬浮物浓度,通过分析模拟HICO光谱所有波段与悬浮物浓度之间的相关性。结果表明,HICO第72波段即810.76 nm处的相关系数最大,据此建立了悬浮物浓度的反演模型,该模型的决定系数R2为0.356 9,反演得到的悬浮物浓度与实测悬浮物浓度之间的RMSE为36.09 mg/L,平均RE为37.5%(图5)。
图5
图5
不同光谱反射率与悬浮物浓度之间的关系
Fig.5
Relationship between the different remote sensing reflectance and TSM concentration
2.3 波段比值算法
波段比值算法是利用2个波段反射率的比值反演水质参数,有利于校正大气和光照等环境背景对测量结果的影响[20]。本文为寻找模拟HICO反演悬浮物浓度的最佳波段比值,在Matlab软件的支持下,分析了所有波段比值与悬浮物浓度的相关性。结果表明,相关系数较高的区域基本集中在蓝绿光波段,其中第57波段(724.84 nm)与第12波段(461.36 nm)光谱反射率的比值与悬浮物浓度相关性最高。故基于这2个波段建立了反演该海域悬浮物浓度的比值模型,模型的决定系数为0.925 2,反演得到的悬浮物浓度与实测悬浮物浓度之间的RMSE为14.09 mg/L,平均RE为5.2%(图6)。实测悬浮物浓度与反演值对比如图7所示。
图6
图7
由图7可以看出,反演得到的悬浮物浓度与实测悬浮物浓度基本均匀地分布在1∶1线附近,表明该模型可有效反演该海域该时间段的悬浮物浓度。
2.4 近红外波段反射峰面积反演算法
图8
图8
水体悬浮物在近红外波段的反射峰面积示意图
Fig.8
Illustration of normalized peak area in near-infrared region
通过研究水体悬浮物在近红外波段反射峰的面积与悬浮物浓度之间的关系表明,反射峰面积与水体悬浮物浓度之间的决定系数为0.719 3,利用反射峰面积算法反演得到的悬浮物浓度与实测悬浮物浓度之间的RMSE为21.63 mg/L,平均RE为23.6%(图9)。
图9
图9
反射峰面积与悬浮物浓度的相关关系
Fig.9
Relationship between normalized peak area and TSM concentration
3 结论
2010年7月下旬,本研究在杭州湾及其邻近海域进行野外光谱与同步悬浮物采样,采用累加平均的方法将实测原始光谱模拟成HICO光谱,对模拟光谱与悬浮物浓度之间的相关性进行了分析并构建模型。
1)利用724.84 nm与461.36 nm波段光谱反射率的比值建立的悬浮物浓度反演模型可获得较高的精度。
2)二类水体的组分是比较复杂的,不同区域水体,其光学特性各不相同,对于同一海域,季节不同,水体光学性质往往也是不同的。因此,利用光谱模型精确反演近海岸水体悬浮物浓度面临着巨大挑战。HICO作为全球第一颗针对近海岸遥感而设计的星载高光谱传感器,在水体悬浮物遥感方面具有极大的应用潜力。本研究成果对利用HICO模拟数据反演近海岸水体悬浮物具有一定的参考意义和应用价值。
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61We investigate challenges faced in temporal analysis of HICO derived bathymetry.61Optimized shallow water inversion model yields precise retrievals in bathymetry.61Retrieved bathymetry can detect temporal changes in depth of less than 1m.61HICO geolocation requires sub-pixel accuracy before use in time series analysis.61New post-processing techniques to image enhancements and tide correction are given.
Remote Sensing of Ocean Colour in Coastal,and Other Optically-complex,Waters[R].Dartmouth:the International Ocean-
Optical properties of the clearest natural waters(200-800 nm)
[J].
DOI:10.1364/AO.20.000177
URL
PMID:20309088
[本文引用: 1]
A new UV submersible spectroradiometer has been employed to determine the diffuse attenuation coefficient for irradiance in the clearest natural waters [K(w)(lambda)] with emphasis on the spectral region from 300 to 400 nm. K(w)(lambda) can be related to the inherent optical properties of pure water, in particular the total absorption coefficient a(w)(lambda) and the molecular scattering coefficient b(m)(lambda), by means of equations derived from radiative transfer theory. We present an analysis showing that limiting values of K(w)(lambda) can be estimated from a(w)(lambda) and vice versa. Published a(w)(lambda) data, which show discrepancies much larger than their estimated accuracies, are briefly reviewed and then compared, via our analysis, with K(w)(lambda) data (our own new and previously published data as well as relevant data of others). This comparative analysis and new data allow a consistent and accurate set of optical properties for the clearest natural waters and for pure fresh water and saltwater to be estimated from 300 to 800 nm.
Absorption spectrum (380-700 nm) of pure water.II.Integrating cavity measurements
[J].DOI:10.1364/AO.36.008710 URL [本文引用: 1]
Lake water quality classification with airborne hyperspectral spectrometer and simulated MERIS data
[J].
DOI:10.1016/S0034-4257(01)00238-3
URL
[本文引用: 1]
We study the use of airborne and simulated satellite remote sensing data for classification of three water quality variables: Secchi depth, turbidity, and chlorophyll a. An extensive airborne spectrometer and ground truth data set obtained in four lake water quality measurement campaigns in southern Finland during 1996 1998 was used in the analysis. The class limits for the water quality variables were obtained from two operational classification standards. When remote sensing data is used, a combination of them proved to be the most suitable. The feasibility of the system for operational use was tested by training and testing the retrieval algorithms with separate data sets. In this case, the classification accuracy is 90% for three Secchi depth classes, 79% for five turbidity classes, and 78% for five chlorophyll a classes. When Airborne Imaging Spectrometer for Applications (AISA) data was spectrally averaged corresponding to Envisat Medium Resolution Imaging Spectrometer (MERIS) channels, the classification accuracy was about the same as in the case of the original AISA channels.
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