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MT与WFEM二维联合反演在山西大同地热区的应用

谢子豪 陈宇峰 刘磊 周文龙 廖卫阳 杨鑫

谢子豪,陈宇峰,刘磊,等. MT与WFEM二维联合反演在山西大同地热区的应用[J]. 地质科技通报,2025,44(4):368-378 doi: 10.19509/j.cnki.dzkq.tb20250048
引用本文: 谢子豪,陈宇峰,刘磊,等. MT与WFEM二维联合反演在山西大同地热区的应用[J]. 地质科技通报,2025,44(4):368-378 doi: 10.19509/j.cnki.dzkq.tb20250048
XIE Zihao,CHEN Yufeng,LIU Lei,et al. Application of MT and WFEM two-dimensional joint inversion in Datong geothermal area, Shanxi Province[J]. Bulletin of Geological Science and Technology,2025,44(4):368-378 doi: 10.19509/j.cnki.dzkq.tb20250048
Citation: XIE Zihao,CHEN Yufeng,LIU Lei,et al. Application of MT and WFEM two-dimensional joint inversion in Datong geothermal area, Shanxi Province[J]. Bulletin of Geological Science and Technology,2025,44(4):368-378 doi: 10.19509/j.cnki.dzkq.tb20250048

MT与WFEM二维联合反演在山西大同地热区的应用

doi: 10.19509/j.cnki.dzkq.tb20250048
基金项目: 湖北省地质局地质科研项目“地下空间地质结构与资源探测技术应用研究”(KJ2023-37);资源与生态环境地质湖北省重点实验室开放基金资助项目(HBREGKFJJ-202310)
详细信息
    作者简介:

    谢子豪:E-mail:931036711@qq.com

    通讯作者:

    E-mail:23632956@qq.com

  • 中图分类号: P631.3

Application of MT and WFEM two-dimensional joint inversion in Datong geothermal area, Shanxi Province

More Information
  • 摘要:

    地热能凭借其稳定性、经济性等优势已成为新型清洁能源体系构建的关键方向。电磁法作为解析地热系统电性结构的核心地球物理手段,其方法体系呈现显著互补特征:大地电磁法(magnetotelluric,简称MT)利用天然交变电磁场,具有探测深度大、对深部低阻异常体灵敏等特点,但极易受到电磁环境噪声的影响;广域电磁法(wide-field electromagnetic method,简称WFEM)采用人工场源,抗干扰性能强、对浅部异常体及细小断裂分辨率较高。为充分发挥MT和WFEM的优势互补效应,采用二维联合反演方法,探讨了MT与WFEM联合反演在地热勘探过程中的可行性和有效性。理论模型合成数据测试表明,相比于单独反演结果,MT与WFEM二维联合反演能够更为清晰地刻画地热系统的盖层及热储层分布特征。最后,对山西大同地热区实测MT及WFEM数据分别单独反演和联合反演,并进行了对比分析。研究结果显示联合反演结果要显著优于MT或WFEM单独反演结果,有助于圈定出地热系统的重要组成部分。根据联合反演所得的电阻率分布结构,结合测区地质及其他资料,推断出了该地区地热系统的概念模型。

     

  • 图 1  高温地热系统示意图

    Figure 1.  Schematic diagram of high-temperature geothermal system

    图 2  单独反演与联合反演的数据RMS收敛曲线

    Figure 2.  RMS convergence curve of data for individual inversion and joint inversion

    图 3  单独反演与联合反演结果(黑线为真实模型边界)

    Figure 3.  Individual inversion and joint inversion results

    图 4  大地电磁与广域电磁测点布置图

    Figure 4.  Position map of MT and WFEM survey points

    图 5  2个代表性点的大地电磁观测数据视电阻率和相位曲线

    Figure 5.  Apparent resistivity and phase curve of MT observation data from two representative points

    图 6  2个代表性点的广域电磁观测数据振幅−频率曲线图

    Figure 6.  Amplitude-frequency curve of WFEM observation data from two representative points

    图 7  相位张量椭圆剖面图

    Figure 7.  Phase tensor elliptic profile

    图 8  大地电磁单独反演时TE极化模式视电阻率拟断面图

    Figure 8.  Apparent resistivity pseudo section of TE polarization mode during MT individual inversion

    图 9  大地电磁单独反演时TM极化模式视电阻率拟断面图

    Figure 9.  Apparent resistivity pseudo section of TM polarization mode during MT individual inversion

    图 10  广域电磁单独反演时电场数据拟断面图

    Figure 10.  Pseudo section of electric field data during WFEM individual inversion

    图 11  实测数据单独反演与联合反演平均拟合误差分布曲线图

    Figure 11.  Distribution curves of average fitting error for individual inversion and joint inversion of measured data

    图 12  实测数据反演结果

    Figure 12.  Inversion results of measured data

    图 13  研究区地电解译模型

    Q. 第四系;N2. 上新统;Ar. 太古宇;下同

    Figure 13.  Geoelectric and geological model of the study area

    图 14  基于联合反演结果推断的简易地热概念模型

    Figure 14.  A simple geothermal conceptual model based on joint inversion results inference

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  • 收稿日期:  2025-02-06
  • 录用日期:  2025-06-09
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