期刊文献+

用边有限元法计算三维各向异性介质的电磁响应 被引量:9

Modeling of the 3-D Electromagnetic Responses to the Anisotropic Medium by the Edge Finite Element Method
下载PDF
导出
摘要 用边有限元基函数导出了各向异性介质中麦克斯韦 (Maxwell)方程的边有限元关系式 ,计算了三维各向异性介质中多分量电磁测井的响应。将总场分离成背景场和二次场的处理技术 ,使该方法适应于有限尺寸和任意方向的源以及倾斜井眼。离散化得到的方程用加不完全乔累斯基分解预处理的Krylov子空间迭代算法实现。利用多层模型检验了该方法。模拟结果表明 ,不同的发射和接收方式在各向异性介质中电磁测井响应有较大差别 ,共面垂直线圈发射和接收 ,视电导率介于各向异性的垂直电导率和水平电导率之间 ;同轴水平线圈发射和接收 ,视电导率等于各向异性的水平电导率 ,用多分量电磁测井可以给出更多和更准确的地层电阻率信息。 The finite element formulation of the Maxwell equation in 3-D anisotropic formation was derived by using the edge finite element interpolation and it was used to simulate the 3-D electromagnetic well logging responses to the subsurface anisotropic formation. The separation of the total electric field into the background and the secondary fields makes it possible that the technique proposed is suitable for the magnetic dipole in any direction and finite size and the deviated borehole. The discrete large sparse linear equation was solved by using the Krylov subspace iterative solver, and its convergence rate was improved by the in-complete Cholesky decomposition preconditioner. Calculation of the simple model shows that, different types of transmitters and receivers have obvious differences of the electromagnetic responses to the anisotropic formation. In thick bed, configuration of co-planar coils in vertical plane shows apparent conductivity between the vertical conductivity and horizontal conductivity in the anisotropic formation; configuration of co-axial coils responses to horizontal conductivity in the anisotropic formation. By using all the information of the multi-component electromagnetic well logging tool, it is possible to derive the true conductivity in the anisotropic formation.
作者 沈金松
出处 《测井技术》 CAS CSCD 2004年第1期11-15,共5页 Well Logging Technology
基金 国家自然科学基金 (40 2 740 1 8) 留学回国人员科研启动基金 (J0 2 0 1 )
关键词 电磁测井 电磁响应 边有限元法 三维各向异性 Krylov子空间迭代算法 edge finite element method 3-D anisotropy electromagnetic response Krylov subspace iterative solver
  • 相关文献

参考文献19

  • 1沈金松.用交错网格有限差分法计算三维频率域电磁响应[J].地球物理学报,2003,46(2):280-288. 被引量:74
  • 2Weaver J, Agarwal A K, Pu X H. 3-D Finite Difference Modeling of the Magnetic Field in Geoelectromagnetic Induction, in Oristaglio, M. , and Spies, B. , Eds, Three-diemnsional Electromagnetics[M]: Soc. Expl. Geophys. 1999.
  • 3Richard B, Michael B, Tony F C, James D, June D, Jack D,Victor E, Roldan P, Charles R, Henk V. Templates for the Solution of Linear Systems: Building Blocks for Iterative Methods[M], Society for Industrial and Applied Mathematics, Philadelphia USA: Tuttle
  • 4Klein J D. Induction Log Anisotropy Corrections[J]. The Log Analyst, 1993,34: 18- 27.
  • 5Jin Jianming. The Finite Element Method in Electromagnetics [M]. John Wiley and Sons Inc, 1993 : 11 - 31.
  • 6Wong Y S. Preconditioned Conjugate Gradient Methods Applied to Certain Symmetric Linear Systems, Intem[J]. J.Computer Math., 1986, 19:177-200.
  • 7Ward S H, Hohmann G W. Electromagnetic Theory for Geophysical Applications, in Nabighian, M. N. , Ed. , Electromagnetic Methods in Applied Geophysics-theory [M]. Soc.Explor. Geophys, 1988, Vol. 1: 131-311.
  • 8Fujino S, Zhang S L. The Mathematics of the Iterative Methods[M]. Tokyo : Asakura Publishing House, 1996: 23-126.
  • 9Van der Vorst H A. ICC G and Related Methods for 3D Problems on Vector Computers [J]. Comput. Phys.Comm. , 1989, 53: 223-235.
  • 10Lee K H. EM1D Fortran Code Research Report of Lawrence Berkeley Laboratory[J]. Nov. 1988. Califomia: United States.

二级参考文献21

  • 1Newman G A, Alumbaugh D L. Three dimensional massively parallel electromagnetic inversion_Theory. Geophys. J. Int., 1997, 128:345~354
  • 2Hohmann G W. Three dimensional induced polarization and electromagnetic modeling. Geophysics, 1975,40:309~324
  • 3Wannamaker P E, Hohmann G W, San Fulipo W A. Electromagnetic modelingof three dimensional bodies in layered earths using integral equations. Geophysics, 1984,49:60~74
  • 4Pridmore D F, Hohmann G W, Ward S H, et al. An investigation of finite element method. Geophysics, 1981, 46:1009~1024
  • 5Alumbaugh D L, Newman G A, Lydie Prevost, et al. Three dimensional wideband electromagnetic modeling on massively parallel computers. Radio Science, 1996, 31:1~23
  • 6Mackie R L, Madden T R. Three dimensional magnetotelluric inversion using conjugate gradient. Geophys. J. Int., 1993, 115: 215~229
  • 7Druskin V, Knizhnerman L. A spectral approach to solving three dimensional Maxwell's diffusion equations in the time and frequency domain. Radio Science. 1994, 29:937~953
  • 8Smith J T. Conservative modeling of 3 D electromagnetic fields, PartⅡ:Bi conjugate gradient solution and an accelerator. Geophysics, 1996, 61:1319~1324
  • 9Yee K S. Numerical solution of initial boundary problems involving Maxwell's equations in isotropic media. IEEE Transaction on Antennas Propagation,1966,AP 14:302~309
  • 10Chew W C, Weedom W H. A 3 D perfectly matched medium from modified Maxwell's equations with stretched coordinates. Microwave and Optical Technology Letters, 1994,7: 599~604

共引文献78

同被引文献96

引证文献9

二级引证文献107

相关作者

内容加载中请稍等...

相关机构

内容加载中请稍等...

相关主题

内容加载中请稍等...

浏览历史

内容加载中请稍等...
;
使用帮助 返回顶部