浅部约束的地磁测深C-响应一维反演

李世文, 翁爱华, 李建平, 唐裕, 张艳辉, 杨悦, 李大俊, 李斯睿. 2017. 浅部约束的地磁测深C-响应一维反演. 地球物理学报, 60(3): 1201-1210, doi: 10.6038/cjg20170330
引用本文: 李世文, 翁爱华, 李建平, 唐裕, 张艳辉, 杨悦, 李大俊, 李斯睿. 2017. 浅部约束的地磁测深C-响应一维反演. 地球物理学报, 60(3): 1201-1210, doi: 10.6038/cjg20170330
LI Shi-Wen, WENG Ai-Hua, LI Jian-Ping, TANG Yu, ZHANG Yan-Hui, YANG Yue, LI Da-Jun, LI Si-Rui. 2017. 1-D inversion of C-response data from geomagnetic depth sounding with shallow resistivity constraint. Chinese Journal of Geophysics (in Chinese), 60(3): 1201-1210, doi: 10.6038/cjg20170330
Citation: LI Shi-Wen, WENG Ai-Hua, LI Jian-Ping, TANG Yu, ZHANG Yan-Hui, YANG Yue, LI Da-Jun, LI Si-Rui. 2017. 1-D inversion of C-response data from geomagnetic depth sounding with shallow resistivity constraint. Chinese Journal of Geophysics (in Chinese), 60(3): 1201-1210, doi: 10.6038/cjg20170330

浅部约束的地磁测深C-响应一维反演

  • 基金项目:

    国家重大科研仪器专项(2011YQ05006010)资助

详细信息
    作者简介:

    李世文, 男, 1988年生, 在读博士, 主要从事地球电磁法及电磁勘探正反演理论研究.E-mail:lisw15@mails.jlu.edu.cn

    通讯作者: 翁爱华, 男, 1968年生, 教授, 主从事电磁法勘探方法技术、正反演理论研究.E-mail:wengah@jlu.edu.cn
  • 中图分类号: P631

1-D inversion of C-response data from geomagnetic depth sounding with shallow resistivity constraint

More Information
  • 地磁测深研究的周期范围通常为105~107s,缺少反映浅部电性结构的短周期信息,而C-响应受浅部电阻率影响明显,因此本文提出在反演中增加浅部(约200 km)电阻率约束以提高深部反演的稳定性和可靠性.在磁层环状电流满足P10假设的条件下,球坐标系中一维导电薄球层状地球的C-响应和电导率分布关系由边界条件通过递推的方法计算得到.反演采用有限内存拟牛顿(L-BFGS)法;浅部电阻率约束通过将目标函数对模型参数的梯度设为零来实现;通过置信区间分析评价约束反演结果的可靠性.合成数据的无约束反演虽然最终的拟合效果很好,但浅部电阻率受初始模型影响,差异较大;采用浅部约束后,反演结果对初始模型依赖性明显减小,同时还能显著提高200~600 km范围内反演结果的准确性.对全球近地轨道卫星观测的C-响应数据约束反演后结果与前人一致,表现为地幔电导率整体上随着深度的增加而增加.参数置信区间分析表明,由于约束反演加入了浅部信息,电阻率的变化范围更加紧致,说明反演结果更加可靠.因此,有必要通过其他地球物理方法,如长周期大地电磁测深等获得浅部电阻率分布,作为先验信息参加反演,进行浅部约束的C-响应反演,获得更可靠的一维全深度电性结构,为地磁测深数据解释奠定基础.

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  • 图 1 

    地球的薄层球状模型及球坐标系下的磁场三分量

    Figure 1. 

    Spherical thin-shell Earth model and three components of magnetic field decomposed in spherical coordinates

    图 2 

    浅部 (0~200 km) 电阻率不同时的C-响应

    Figure 2. 

    The C-response of models with different resistivity in shallow layers (0~200 km)

    图 3 

    不同初始模型的1-D反演结果

    Figure 3. 

    The inversion results of different starting models

    图 4 

    理论模型有无浅部约束的反演结果

    Figure 4. 

    Inversion results with and without shallow resistivity constraint

    图 5 

    近地轨道卫星观测数据的反演结果

    Figure 5. 

    The 1-D inversion results of low Earth orbit satellite′s data

    表 1 

    用于C-响应数值模拟的理论模型

    Table 1. 

    Model used to calculate C-response

    Resistivity/ΩmThickness/km
    76200
    76320
    4.5126
    5.9145
    0.6622099
    Core3481
    下载: 导出CSV

    表 2 

    有限内存拟牛顿反演法的基本流程

    Table 2. 

    Inversion diagram of L-BFGS method

    k=0
    初始化模型mk、正则化参数λ和对称正定矩阵Hk, 指定迭代终止条件
    循环
    计算导数向量gk, 并计算修正梯度方向dk=-Hkgk
    搜索最优步长αk
    更新模型mk+1=mk+αkdk
    下载: 导出CSV

    表 3 

    用于合成反演数据的模型

    Table 3. 

    Model for inversion test

    Resistivity/ΩmThickness/km
    100200
    50300
    5300
    0.52090
    Core3481
    下载: 导出CSV
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出版历程
收稿日期:  2016-07-12
修回日期:  2016-12-05
上线日期:  2017-03-01

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