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基于频域电磁法反演喀斯特表层土-岩结构研究

程凭 程勤波 陈喜 刘金涛 张志才 高满

程 凭,程勤波,陈 喜,等. 基于频域电磁法反演喀斯特表层土-岩结构研究[J]. 中国岩溶,2022,41(5):675-683 doi: 10.11932/karst20220501
引用本文: 程 凭,程勤波,陈 喜,等. 基于频域电磁法反演喀斯特表层土-岩结构研究[J]. 中国岩溶,2022,41(5):675-683 doi: 10.11932/karst20220501
CHENG Ping, CHENG Qinbo, CHEN Xi, LIU Jintao, ZHANG Zhicai, GAO Man. Exploration of superficial soil-rock structure for karst area based on frequency domain electromagnetic method[J]. CARSOLOGICA SINICA, 2022, 41(5): 675-683. doi: 10.11932/karst20220501
Citation: CHENG Ping, CHENG Qinbo, CHEN Xi, LIU Jintao, ZHANG Zhicai, GAO Man. Exploration of superficial soil-rock structure for karst area based on frequency domain electromagnetic method[J]. CARSOLOGICA SINICA, 2022, 41(5): 675-683. doi: 10.11932/karst20220501

基于频域电磁法反演喀斯特表层土-岩结构研究

doi: 10.11932/karst20220501
基金项目: 国家自然科学基金项目(42030506, 42071039)
详细信息
    作者简介:

    程凭(1997-),男,理学硕士,主要研究方向为水文地球物理。E-mail:chengping0221@163.com

    通讯作者:

    陈喜(1964-),男,教授,主要研究方向为流域水文模拟、地下水数值计算等。E-mail: xi_chen@tju.edu.cn

  • 中图分类号: P631

Exploration of superficial soil-rock structure for karst area based on frequency domain electromagnetic method

  • 摘要: 喀斯特地区浅表层土壤分布极不均匀,探测土-岩界面和土壤分布对区域水文以及生态环境研究具有重要意义。文章基于麦克斯韦方程组构建了频域电磁法(FDEM)探测的电导率(EC)一维反演模型,实现了喀斯特浅表剖面EC可视化表述。根据设定的理想地层EC数据以及南方喀斯特峰丛洼地两个剖面和出露的三个实测剖面的FDEM实测视电导率,结合高密度电法、剖面实测土-岩界面,检验了反演模型可靠性。结果表明:FDEM法反演结果能较好的描述理想地层EC变化,以及土壤与灰岩、白云岩界面EC分布,进而可辨识土壤厚度分布,但基于反演的EC值判别尺度较小的溶沟(槽)以及泥岩区土-岩界面误差较大。

     

  • 图  1  CMD Explorer频域电磁仪示意图(改自Jadoon et al[12])

    Figure  1.  Diagram of CMD Explorer frequency domain electromagnetic induction instrument (modified from Jadoon et al[12])

    图  2  频域电磁感应仪工作原理图(改自SELEPENG[13]

    Figure  2.  Working principle diagram of frequency domain electromagnetic induction instrument (FDEM) (modified from SELEPENG[13])

    图  3  土壤或岩石分层示意图(改自Deidda et al., 2017[19]

    Figure  3.  Schematic diagram of soil or rock stratification (modified from Deidda et al., 2017[19])

    图  4  地层EC反演(虚线)与设定(实线)分布对比图

    Figure  4.  Comparison of the inversion EC line (dotted line) and the set line (solid line) of the profiles

    图  5  研究断面位置示意图

    Figure  5.  Schematic diagram of the location of the study sections

    图  6  高密度电法(a)与频域电磁法反演结果(b)对比图 (Line 1)

    Figure  6.  Comparison of the electric resistivity distribution measured by ERT (a) and the EC distribution inversed by FDEM at the line 1

    图  7  高密度电法(a)与频域电磁法反演结果(b)对比图(line 2)

    Figure  7.  Comparison of the electric resistivity values measured by ERT (a) and the EC values inversed by FDEM at the section of line 2

    图  8  FDEM反演的视电导率与观测值相关关系

    Figure  8.  Comparison of the measured and the inverted ECa values

    图  9  厚层灰岩剖面(a.实景照片,b.反演的EC,c.探测的ECa)

    Figure  9.  Thick limestone profile (a. real photo, b. inverted EC, c. measured ECa)

    图  10  黄土-白云岩/泥岩互层剖面(a.实景照片,b.反演的EC,c.探测的ECa

    Figure  10.  Loess-Dolomite/Mudstone interbed profile (a. real photo, b. inverted EC, c. detected ECa)

    图  11  黄土-白云岩/泥灰岩剖面(a.实景照片,b.反演的EC,c.探测的ECa

    Figure  11.  Loess-Dolomite/Marl profile (a. real photo, b. inverted EC, c. detected ECa)

    图  12  各剖面反演与实测ECa对比图

    Figure  12.  Comparison of inverted and measured ECa of each profile

    表  1  正演模型模拟与反演ECa结果对比

    Table  1.   Comparison of the simulated and inverted ECa values

    线圈模式 HCP VCP 残差
    线圈距离/m 1.48 2.82 4.49 1.48 2.82 4.49
    a 模拟
    ECa/S·m−1
    0.059 2 0.051 8 0.043 8 0.059 3 0.057 5 0.053 8 0.000 2
    反演
    ECa/S·m−1
    0.058 8 0.051 7 0.0441 0.059 5 0.057 5 0.053 9
    b 模拟
    ECa/S·m−1
    0.064 1 0.055 9 0.048 6 0.071 5 0.065 9 0.060 7 0.000 3
    反演
    ECa/S·m−1
    0.064 1 0.055 8 0.048 7 0.071 5 0.065 8 0.060 7
    c 模拟
    ECa/S·m−1
    0.064 1 0.055 9 0.0486 0.0715 0.065 9 0.060 7 0.000 2
    反演
    ECa/S·m−1
    0.064 1 0.055 8 0.048 7 0.071 5 0.065 8 0.060 7
    d 模拟
    ECa/S·m−1
    0.076 9 0.082 8 0.077 4 0.061 2 0.070 7 0.074 4 0.000 0
    反演
    ECa/S·m−1
    0.076 7 0.083 1 0.077 2 0.061 2 0.070 8 0.074 5
    下载: 导出CSV
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出版历程
  • 收稿日期:  2021-12-09
  • 刊出日期:  2022-12-02

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