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基于遥感数据和表层声速的全海深声速剖面反演

李倩倩 李宏琳 曹守莲 严娴 马志川

李倩倩,李宏琳,曹守莲,等. 基于遥感数据和表层声速的全海深声速剖面反演[J]. 海洋学报,2022,44(12):84–94 doi: 10.12284/hyxb2022149
引用本文: 李倩倩,李宏琳,曹守莲,等. 基于遥感数据和表层声速的全海深声速剖面反演[J]. 海洋学报,2022,44(12):84–94 doi: 10.12284/hyxb2022149
Li Qianqian,Li Honglin,Cao Shoulian, et al. Inversion of the full-depth sound speed profile based on remote sensing data and surface sound speed[J]. Haiyang Xuebao,2022, 44(12):84–94 doi: 10.12284/hyxb2022149
Citation: Li Qianqian,Li Honglin,Cao Shoulian, et al. Inversion of the full-depth sound speed profile based on remote sensing data and surface sound speed[J]. Haiyang Xuebao,2022, 44(12):84–94 doi: 10.12284/hyxb2022149

基于遥感数据和表层声速的全海深声速剖面反演

doi: 10.12284/hyxb2022149
基金项目: 中国博士后科学基金(2020M670891);山东科技大学科研创新团队支持计划(2019TDJH103);山东省高等学校青年创新团队人才引育计划;山东省自然科学基金(ZR2020MA090,ZR2022MA051)
详细信息
    作者简介:

    李倩倩(1984-),女,山东省青岛市人,副教授,主要从事研究海洋环境声学反演和水下声源定位等水声逆问题。E-mail:liqianqian@sdust.edu.cn

  • 中图分类号: P733.2

Inversion of the full-depth sound speed profile based on remote sensing data and surface sound speed

  • 摘要: 海洋声速剖面严重影响着水下声传播特性,近实时地获取声速剖面对水下声通信、水下定位、鱼群探测等都有重要意义。单经验正交函数回归(single Empirical Orthogonal Function regression,sEOF-r)方法通过建立声速剖面的经验正交系数与海面遥感数据之间的线性回归关系来反演声速剖面。但是,海洋是一个复杂的动力系统,声速与海面遥感数据并不是简单的线性关系,因此,本文基于Argo历史网格数据,通过自组织映射(Self-Organizing Map,SOM)生成海平面高度异常(Sea Level Anomaly,SLA)、海表面温度(Sea Surface Temperature,SST)等海表遥感数据以及表层声速仪测量的表层声速与声速剖面异常之间的非线性映射;然后利用近实时的海表遥感数据和表层声速反演三维海洋声速场。声速剖面反演的结果表明,在多源信息融合的优势下,本文方法的反演性能最稳定且精度最高,声速剖面的平均反演精度比经典sEOF-r方法提高约2 m/s,比未考虑表层声速的经典SOM方法提高约1 m/s。
  • 图  1  Argo网格数据与海表面温度、海平面高度异常数据位置匹配示意图

    Fig.  1  Schematic diagram of location matching between Argo grid data and sea surface temperature and sea level anomaly data

    图  2  声速剖面反演流程

    黑色虚线框表示增加的先验信息,红色虚线框表示测试集中已知信息与输出层参考向量匹配

    Fig.  2  Flow of sound speed profile inversion

    The black dashed box indicates the added prior information, and the red dashed box indicates that the known information in the test set matches the reference vector of the output layer

    图  3  训练集中的声速剖面(灰色线为实测剖面,黑色线为平均剖面)(a)、声速扰动(b)和前6阶经验正交函数(EOF)的累积方差贡献率(c)

    Fig.  3  The sound speed profile in the training set (gray lines are the measured profile, black line is the average profile) (a), residual sound speed (b) and the cumulative variance contribution rates of the first 6-order empirical orthogonal function (EOF) (c)

    图  4  训练集和测试集的经验正交函数基函数之间的相关系数

    Fig.  4  Correlation coefficient between empirical orthogonal function (EOF) basis functions of training set and test set

    图  5  训练集和测试集的前两阶基函数(a)、测试集前6阶经验正交函数(EOF)的累积方差贡献率(b)和训练集和测试集的平均声速误差(c)

    Fig.  5  The first two order basis functions of the training set and the test set (a), the cumulative variance contribution rate of the first six orders of empirical orthogonal function (EOF) in the test set (b) and the average sound speed error of the training set and test set (c)

    图  6  声速剖面重构误差

    白色虚线为重构声速剖面的均方根误差

    Fig.  6  The reconstruction error of the sound speed profile

    The white dashed line is the root mean square error of the reconstructed sound speed profile

    图  7  平均声速剖面的声速梯度(a),海表面温度(SST)、海表面高度异常(SLA)和声速剖面(SSP)的相关性(b)

    Fig.  7  Sound speed gradient of mean sound speed profile (a), correlation between sea surface temperature (SST), sea level anomally (SLA) and sound speed profile (SSP) (b)

    图  8  测试集中声速剖面反演误差

    a. SOM-c10方法;b. SOM方法;c. sEOF-r方法

    Fig.  8  The inversion error of the sound speed profiles in the test set

    a. SOM-c10 method; b. SOM method; c. sEOF-r method

    图  9  不同方法的均方根误差

    Fig.  9  The root mean square error for different methods

    图  10  测试集中的13~18号声速剖面

    Fig.  10  The 13th−18th sound speed profiles in the test set

    图  11  测试集中第13号剖面(a)和第16号剖面(b)的反演情况

    Fig.  11  The inversion of 13th profile (a) and 16th profile (b) in the test set

    图  12  不同平均声速剖面下sEOF-r和SOM-c10方法的反演结果

    Fig.  12  Prediction results of sEOF-r and SOM-c10 method with different mean sound speed profiles

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出版历程
  • 收稿日期:  2022-02-17
  • 修回日期:  2022-05-23
  • 网络出版日期:  2022-09-19
  • 刊出日期:  2023-01-17

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