4.6 Article

3D sequential inversion of frequency-domain airborne electromagnetic data to determine conductive and magnetic heterogeneities

Journal

GEOPHYSICS
Volume 83, Issue 5, Pages E357-E369

Publisher

SOC EXPLORATION GEOPHYSICISTS
DOI: 10.1190/GEO2017-0668.1

Keywords

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Funding

  1. Human Resources Program in Energy Technology of the Korea Institute of Energy Technology Evaluation and Planning
  2. Ministry of Trade, Industry & Energy, Republic of Korea [20164010201120, 20174010201170]
  3. Korea Evaluation Institute of Industrial Technology (KEIT) [20164010201120, 20174010201170] Funding Source: Korea Institute of Science & Technology Information (KISTI), National Science & Technology Information Service (NTIS)

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We have developed two inversion workflows that sequentially invert conductivity and susceptibility models from a frequencydomain controlled-source electromagnetic data set. Both workflows start with conductivity inversion using electromagnetic (EM) kernel and out-of-phase component data, which is mainly sensitive to conductivity, and then we adopt the susceptibility inversion using in-phase component data. The difference between these two workflows is in the susceptibility inversion algorithm: One uses an EM kernel and a conductivity model as the input model; the other uses a magnetostatic kernel and a conductivity model to generate the appropriate input data. Because the appropriate input data for magnetostatic inversion should not contain the EM induction effect, the in-phase induction effect is simulated through the conductivity model obtained by inverting out-of-phase data and subtracting them from observed in-phase data to generate an induction-subtracted in-phase data set that becomes input data for magnetostatic inversion. For magnetostatic inversion, we used a linear magnetostatic kernel to enable rapid computation. Then, we applied the two inversion workflows to a field data set of a DIGHEM survey, and we successfully reconstructed the conductivity and susceptibility models from each workflow using two zones within the data sets, in which conductive and susceptible anomalies were present. One important finding is that the susceptibility inversion results obtained from two different workflows are very similar to each other. However, computational time can be significantly saved with linear magnetostatic inversion. We found out how the results of the conductivity and susceptibility models could be well-imaged using a sequential inversion workflow and also how magnetostatic inversion could be used efficiently for airborne EM data inversion.

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