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基于改进的接收点插值算法的频率域海洋可控源电磁法2.5维正演
引用本文:李刚,李予国,韩波,段双敏.基于改进的接收点插值算法的频率域海洋可控源电磁法2.5维正演[J].地球物理学报,2017,60(12):4887-4900.
作者姓名:李刚  李予国  韩波  段双敏
作者单位:1. 中国海洋大学海洋地球科学学院, 青岛 266100; 2. 中国海洋大学海底科学与探测技术教育部重点实验室, 青岛 266100; 3. 海洋科学与技术国家实验室, 海洋矿产资源评价与探测技术功能实验室, 青岛 266071; 4. 德国GEOMAR亥姆霍兹基尔海洋研究中心, 基尔 24148
基金项目:国家自然科学基金项目(41704075,41604063)和山东省自然科学基金项目(ZR2016DQ15,ZR2016DB31)联合资助.
摘    要:在海洋可控源电磁法勘探中,接收站常置于海底.在进行海洋电磁场模拟时,由于海水和海底介质存在显著电性差异,这给海底接收点处场值的求取带来困难.本文提出一种新的接收点插值算法,该算法考虑到海底电场法向分量不连续性问题,用法向电流分量进行插值以准确求取海底任意接收点处电磁场值.本文利用交错网格有限差分法实现了二维介质中频率域海洋可控源法(CSEM)正演.对构造走向做傅里叶变换,将三维电磁模拟问题转换为波数域2.5维问题,即三维场源激励下针对二维地电模型的电磁模拟问题.使用交错网格有限差分法,基于一次场/二次场分离方法导出波数域二次电场离散形式,并进一步求得波数域电磁场.采用本文提出的改进的插值算法可求得海底任意接收点处波数域电磁场,采用傅里叶逆变换对波数域电磁场进行积分可得到接收点处空间域电磁场.模型算例表明,与常规的线性插值和严格插值算法相比,本文提出的改进的插值算法具有更高的精度.

关 键 词:海洋可控源电磁法  2.5维  数值模拟  接收点插值  
收稿时间:2016-11-13

2.5D marine CSEM modeling in the frequency-domain based on an improved interpolation scheme at receiver positions
LI Gang,LI Yu-Guo,HAN Bo,DUAN Shuang-Min.2.5D marine CSEM modeling in the frequency-domain based on an improved interpolation scheme at receiver positions[J].Chinese Journal of Geophysics,2017,60(12):4887-4900.
Authors:LI Gang  LI Yu-Guo  HAN Bo  DUAN Shuang-Min
Institution:1. College of Marine Geosciences, Ocean University of China, Qingdao 266100, China; 2. Key Lab of Submarine Geosciences and Prospecting Techniques of Ministry of Education, Ocean University of China, Qingdao 266100, China; 3. Laboratory of Marine Mineral Resources, Qingdao National Laboratory for Marine Science and Technology, Qingdao 266071, China; 4. GEOMAR Helmholtz Centre for Ocean Research Kiel, Kiel 24148, Germany
Abstract:In the marine controlled-source electromagnetic (CSEM) survey, the receivers are usually placed at the seafloor. The resistivity contrast between the seawater and seafloor sediments is large, which can cause difficulties in numerical modeling of CSEM fields at receiver locations. In this paper, we present an improved interpolating method for calculating electric and magnetic fields at the seafloor with a resistivity contrast. This method is applied to the 2.5-dimensional (2.5D) frequency-domain CSEM modeling with towed transmitters and receivers located at the seafloor. Considering the discontinuity of the normal electric fields, we use the normal current electric density for interpolation. We simulate the 2.5D marine CSEM responses by the staggered finite-difference (SFD) method with Fourier transform to the strike direction. The final SFD equations are solved by the direct solver MUMPS (MUltifrontal Massively Parallel Sparse direct Solver). To avoid the source singularities, the secondary-field approach is used and the primary fields excited by the electric dipole source can be calculated quasi-analytically for the one-dimensional (1D) layered background model. We focus on interpolating of electric and magnetic fields in the wavenumber domain to the receiver locations at the seafloor interface between the conductive seawater and resistive seafloor formation. The secondary electric and magnetic fields are used for interpolation instead of the total fields for high numerical accuracy. After performing the inverse Fourier transform to the wavenumbers, the electric and magnetic fields in the space domain are obtained. To check the accuracy of our 2.5D marine CSEM SFD modeling algorithm with the improved receiver interpolating technique, we compare our results with both the 1D analytical results and the adaptive finite element results. The SFD numerical results are approved to be accurate. We also compare the numerical accuracy between our improved interpolation scheme and others, i.e., the conventional linear interpolation and the rigorous interpolation. The proposed interpolation only utilizes the nodes below/above the seafloor interface, and is proved to be much more accurate than the other two interpolating methods used.
Keywords:Marine CSEM  2  5D  Numerical modeling  Interpolation scheme for receiver positions
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