The asymptotic response of three-dimensional basin offsets to magnetotelluric fields at long periods; the effects of current channeling

A simple, inexpensive numerical algorithm is used to analyze the asymptotic long-period behavior of magnetotelluric (MT) fields in the vicinity of lateral offsets in sedimentary basins. The model is based on the distortion or channeling of telluric currents in a horizontal thin sheet. Although a gross oversimplification of nature, the model represents a class of structures which, because of excessive computer costs, have been relatively unstudied previously. Within, and closely adjacent to, the region of the three-dimensional (3-D) offset, significant distortion of the MT parameters occurs. Skewness coefficients vary from negligible values to over 0.7. Principal resistivities vary by an order of magnitude. On the other hand, there is not a clear correlation between the degree of distortion of the parameters usually evaluated during MT surveys and the magnitude of conventional 3-D indicators (e.g., the skewness coefficient). Calculations have simulated the technique of averaging resistivity parameters from a large number of field sites in order to arrive at a regionally representative one-dimensional (1-D) model. The results indicate that unless care is taken in adapting the nature of the averaging algorithm to the class of distortions encountered, significant bias of the averaged parameters may result. These results also suggest that formore » this class of structures grave problems may be associated with using the principal resistivity perpendicular to geologic strike, the so-called transverse magnetic (TM) mode, to infer an equivalent two-dimensional (2-D) model for the region. A 2-D model would likely show significant modulations in the physical character of the basement which are, in fact, an artifact of telluric distortion caused by current channeling in the surficial heterogeneity. 10 figures, 4 tables.« less

[1]  C. Swift,et al.  A magnetotelluric investigation of an electrical conductivity anomaly in the southwestern United States , 1967 .

[2]  G. W. Hohmann,et al.  Magnetotelluric models of the Roosevelt hot springs thermal area, Utah. , 1980 .

[3]  G. W. Hohmann,et al.  Integral equation modeling of three-dimensional magnetotelluric response , 1981 .

[4]  D. Rankin,et al.  Three-dimensional modelling in magnetotelluric and magnetic variational sounding , 1977 .

[5]  M. Berdichevskiĭ Electrical prospecting with the telluric current method , 1965 .

[6]  F. W. Jones,et al.  The Perturbation of Alternating Geomagnetic Fields by Three-Dimensional Conductivity Inhomogeneities , 1972 .

[7]  G. W. Hohmann Three-Dimensional Induced Polarization and Electromagnetic Modeling , 1975 .

[8]  Refined finite-difference simulations using local integral forms: Application to telluric fields in two dimensions , 1982 .

[9]  The perturbation of geomagnetic fields by two-dimensional and three-dimensional conductivity inhomogeneities , 1974 .

[10]  T. Madden,et al.  Generalized thin sheet analysis in magnetotellurics: an extension of Price's analysis , 1980 .

[11]  A. Raiche An Integral Equation Approach to Three-Dimensional Modelling , 1974 .

[12]  J. Hermance,et al.  The telluric-magnetotelluric method , 1975 .

[13]  G. W. Hohmann,et al.  The telluric‐magnetotelluric method in two‐ and three‐dimensional environments , 1981 .

[14]  F. W. Jones,et al.  The calculation of magnetotelluric quantities for three‐dimensional conductivity inhomogeneities , 1978 .