Long-Period Magnetotelluric Measurements Near the Central California Coast: A Land-Locked View of the Conductivity Structure Under the Pacific Ocean

SUMMARY Telluric data from Hollister, California were combined with magnetic data from the Fresno, California magnetic observatory to determine the MT response at long periods. The shifted eigenstate analysis of LaTorraca et al. (1986) was used to determine the maximum apparent resistivities and corresponding EIH phases for periods from 1 to 30 h. The apparent resistivity and phase at Hollister are greatly influenced by the ocean, with the mantle branch beginning at a period of about 12 h. In typical continental areas, the mantle branch usually begins at periods of 10s or less. A maximum likelihood inversion algorithm was used to invert the observed data and to determine the sensitivity of the model parameters. The data required a resistivity-thickness product of approximately 1 x lo9 Q-m2 (1 x lo6 Q-m-km) for the oceanic lower crust and upper mantle. The oceanic mantle shows a rather small gradient of conductivity from approximately 200 to 640 km in depth, and a rapid conductivity increase below 640km. The sensitivity analysis shows the data are most sensitive to the oceanic parameters, except for the electric field amplitudes which are also sensitive to the resistivities under the observation site.

[1]  A. Tarantola Inverse problem theory : methods for data fitting and model parameter estimation , 1987 .

[2]  W. Mooney,et al.  Two-dimensional velocity structure along the synclinal axis of the Great Valley, California , 1986 .

[3]  Theodore R. Madden,et al.  An analysis of the magnetotelluric impedance for three-dimensional conductivity structures , 1986 .

[4]  P. Tarits Conductivity and fluids in the oceanic upper mantle , 1986 .

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

[6]  B. Bennett A long-period magnetotelluric study in California , 1985 .

[7]  Gerald W. Hohmann,et al.  Magnetotelluric responses of three-dimensional bodies in layered earths , 1982 .

[8]  D. Oldenburg,et al.  Inversion of ocean bottom magnetotelluric data revisited , 1984 .

[9]  John F. Hermance,et al.  Electromagnetic induction studies , 1983 .

[10]  Stephen K. Park,et al.  Three-dimensional magnetotelluric modelling and inversion , 1983 .

[11]  A. Tarantola,et al.  Generalized Nonlinear Inverse Problems Solved Using the Least Squares Criterion (Paper 1R1855) , 1982 .

[12]  A. Chave,et al.  Electromagnetic induction fields in the deep ocean north-east of Hawaii: implications for mantle conductivity and source fields , 1981 .

[13]  T. Jordan,et al.  Continents as a chemical boundary layer , 1981, Philosophical Transactions of the Royal Society of London. Series A, Mathematical and Physical Sciences.

[14]  G. Latorraca Differential tellurics with applications to mineral exploration and crustal resistivity monitoring , 1981 .

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

[16]  B. Lienert,et al.  Long Term Variations in Magnetotelluric Apparent Resistivities Observed near the San Andreas Fault in Southern California , 1980 .

[17]  J. Filloux Magnetotelluric soundings over the northeast Pacific may reveal spatial dependence of depth and conductance of the asthenosphere , 1980 .

[18]  John Clarke,et al.  Magnetotellurics with a remote magnetic reference , 1979 .

[19]  John Clarke,et al.  Magnetotelluric data analysis; removal of bias , 1978 .

[20]  R. P. Ranganayaki Generalized thin sheet approximation for magnetotelluric modelling. , 1978 .

[21]  T. Shankland,et al.  Partial melting and electrical conductivity anomalies in the upper mantle , 1977 .

[22]  J. Filloux Ocean-floor magnetotelluric sounding over North Central Pacific , 1977, Nature.

[23]  David L.B. Jupp,et al.  Two-dimensional magnetotelluric inversion , 1977 .

[24]  R. Phillips,et al.  Electrical structure in a region of the Transverse Ranges, southern California. [for earthquake prediction] , 1977 .

[25]  P. Kasameyer Low-frequency magnetotelluric survey of New England. , 1974 .

[26]  H. C. Heard,et al.  Electrical conductivity of olivine at high pressure and under controlled oxygen fugacity , 1974 .

[27]  J. Filloux Techniques and instrumentation for study of natural electromagnetic induction at sea , 1973 .

[28]  J. Hermance Processing of magnetotelluric data , 1973 .

[29]  A. Duba Electrical conductivity of olivine , 1972 .

[30]  K. Vozoff,et al.  The Magnetotelluric Method in the Exploration of Sedimentary Basins , 1972 .

[31]  F. X. Bostick,et al.  THE ESTIMATION OF MAGNETOTELLURIC IMPEDANCE TENSOR ELEMENTS FROM MEASURED DATA , 1971 .

[32]  Joel Franklin,et al.  Well-posed stochastic extensions of ill-posed linear problems☆ , 1970 .

[33]  Ulrich Schmucker,et al.  Anomalies of geomagnetic variations in the Southwestern United States , 1970 .

[34]  J. S. V. van Zijl A DEEP SCHLUMBERGER SOUNDING TO INVESTIGATE THE ELECTRICAL STRUCTURE OF THE CRUST AND UPPER MANTLE IN SOUTH AFRICA , 1969 .

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

[36]  A. Orange,et al.  Further deep resistivity measurements in the Pacific Northwest , 1965 .

[37]  P. Nelson,et al.  Deep resistivity measurements in the Pacific Northwest , 1965 .

[38]  W. D. Parkinson The Influence of Continents and Oceans on Geomagnetic Variations , 1962 .

[39]  R. W. Webb,et al.  Geology of California , 1934, Nature.