Electric dipole fields over an anisotropic seafloor: theory and application to the structure of 40 ma pacific ocean lithosphere

SUMMARY Seismic anisotropy has been detected in the oceanic crust and upper mantle, and likewise it is geologically reasonable to expect that a certain amount of lateral anisotropy exists in sea£oor electrical properties. Anisotropy in Earth properties can often lead to surprising eiects on geophysical responses that are not anticipated from simple isotropic theories. Here, we investigate the eiects of lateral anisotropy on the frequency-domain, controlled-source electromagnetic (CSEM) response of a uniaxially conducting, non-magnetic sea£oor excited by a horizontal electric dipole whose moment is oriented obliquely with respect to the electrical strike direction. A ‘paradox of anisotropy’ is observed, in which the sea£oor electric ¢eld strength is enhanced in the most conductive direction of the sea£oor. This enhancement is opposite to what one would expect based on naive isotropic theory. We also show that it is possible in certain circumstances to extract the along-strike electrical conductivity from marine controlled-source electromagnetic data using only isotropic modelling. The extraction of across-strike conductivity, however, requires full anisotropic modelling. The physical insight into electromagnetic induction in uniaxial media that is presented here should greatly assist the geological interpretation of marine CSEM experimental data. Applying our algorithm to the PEGASUS data set (CSEM data collected over 40 Ma Paci¢c Ocean lithosphere) produces a model with conductivity in the fossil spreading direction that is seven times greater than the conductivity perpendicular to spreading. Strain-aligned mineralogical fabric, as predicted by tectonic modelling, would explain our result, with enhanced conductivities caused by hydrogen conduction along the olivine a-axis or connected accumulations of trace conductors such as graphite or magnetite.

[1]  E. Appleton Temperature Changes in the Higher Atmosphere , 1935, Nature.

[2]  Alan D. Chave,et al.  Numerical integration of related Hankel transforms by quadrature and continued fraction expansion , 1983 .

[3]  D. Oldenburg,et al.  Subspace inversion of electromagnetic data: application to mid‐ocean‐ridge exploration , 1995 .

[4]  Rob L. Evans,et al.  On the electrical nature of the axial melt zone at 13° N on the East Pacific Rise , 1994 .

[5]  C. S. Cox,et al.  Controlled-source electromagnetic sounding of the oceanic lithosphere , 1986, Nature.

[6]  S. Constable Conduction by mantle hydrogen , 1993, Nature.

[7]  G. Keller,et al.  Frequency and transient soundings , 1983 .

[8]  A. Duba,et al.  Free carbon & electrical conductivity in the Earth's mantle , 1982 .

[9]  G. Vasseur,et al.  ELECTROMAGNETIC FIELD OF SOURCES AT THE SURFACE OF A HOMOGENEOUS CONDUCTING HALFSPACE WITH HORIZONTAL ANISOTROPY: APPLICATION TO FISSURED MEDIA* , 1981 .

[10]  R. N. Edwards,et al.  Transient marine electromagnetics: the 2.5-D forward problem , 1993 .

[11]  R. N. Edwards,et al.  A time domain electromagnetic survey of the TAG Hydrothermal Mound , 1996 .

[12]  L. Gasperini,et al.  Stratigraphic numerical modelling of a carbonate platform on the Romanche transverse ridge, equatorial Atlantic , 1997 .

[13]  Alan D. Chave,et al.  On the theory of sea-floor conductivity mapping using transient electromagnetic systems , 1987 .

[14]  Alan D. Chave,et al.  Electromagnetic induction by a finite electric dipole source over a 2-D earth , 1993 .

[15]  S. Karato,et al.  Lattice preferred orientation of olivine aggregates deformed in simple shear , 1995, Nature.

[16]  S. Constable,et al.  Marine magnetotellurics for petroleum exploration Part I: A sea-floor equipment system , 1998 .

[17]  Steven Constable,et al.  Marine controlled‐source electromagnetic sounding: 1. Modeling and experimental design , 1996 .

[18]  R. Evans,et al.  The Shallow Porosity Structure Of The Continental Shelf Off Humboldt Bay, California: Results Of A Towed Electromagnetic Survey , 1997 .

[19]  C. S. Cox,et al.  Marine controlled-source electromagnetic sounding. 2. The PEGASUS experiment , 1996 .

[20]  R. N. Edwards,et al.  Transient electromagnetic responses in seafloor with triaxial anisotropy , 1997 .

[21]  M. Unsworth,et al.  An active source electromagnetic sounding system for marine use , 1990 .

[22]  Zonghou Xiong Electromagnetic fields of electric dipoles embedded in a stratified anisotropic Earth , 1989 .

[23]  P. Dawson,et al.  Teleseismic imaging of subaxial flow at mid-ocean ridges: traveltime effects of anisotropic mineral texture in the mantle , 1996 .

[24]  L. Law,et al.  A porosity mapping survey in Hecate Strait using a seafloor electro-magnetic profiling system , 1993 .

[25]  D. McKenzie,et al.  Finite deformation during fluid flow , 1979 .

[26]  S. Karato,et al.  The role of hydrogen in the electrical conductivity of the upper mantle , 1990, Nature.

[27]  P. Clemmow The theory of electromagnetic waves in a simple anisotropic medium , 1963 .

[28]  R. Parker,et al.  Occam's inversion; a practical algorithm for generating smooth models from electromagnetic sounding data , 1987 .

[29]  L. Pedersen,et al.  The electromagnetic response of an azimuthally anisotropic half-space , 1991 .

[30]  Steven Constable,et al.  The RAMESSES experiment—III. Controlled-source electromagnetic sounding of the Reykjanes Ridge at 57°45′N , 1998 .

[31]  Alan D. Chave,et al.  Controlled electromagnetic sources for measuring electrical conductivity beneath the oceans: 1. Forward problem and model study , 1982 .

[32]  R. N. Edwards,et al.  The detection of lateral anisotropy of the ocean floor by electromagnetic methods , 1992 .

[33]  C. Cox,et al.  Electromagnetic active source sounding near the East Pacific Rise , 1981 .