Magnetic and Electric Fields Produced in the Sea During Geomagnetic Disturbances

Abstract — To understand geomagnetic effects on systems with long conductors it is necessary to know the electric field those systems experience. For surface conductors such as power systems and pipelines this can easily be calculated from the magnetic field variations at the surface using the surface impedance of the earth. However, for calculating the electric fields in pipelines and submarine cables at the seafloor it is necessary to take account of the attenuating effect of the conducting seawater. Assuming that the fields are vertically propagating plane waves, we derive the transfer functions between the electric and magnetic fields at the seafloor and the magnetic field variations at the sea surface. These transfer functions are then used, with surface magnetic field data, to determine the power spectra of the seafloor magnetic and electric fields in a shallow sea (depth 100 m) and in the deep ocean (depth 5 km) for different values of the Kp magnetic activity index . For the period range considered (2 min to 3 hrs) the spectral characteristics of the seafloor magnetic and electric fields for a 100 m deep sea are very similar to those of the surface fields. For the deep ocean the seafloor spectra show a faster decrease in spectral density with increasing frequency compared to the surface fields. The results obtained are shown to be consistent with seafloor observations. Assessment of the seafloor electric fields produced by different levels of geomagnetic activity can be useful in the design of the power feed equipment for submarine cables and cathodic protection for undersea pipelines.

[1]  G. W. Hohmann,et al.  4. Electromagnetic Theory for Geophysical Applications , 1987 .

[2]  James R. Wait,et al.  Wave Propagation Theory , 1981 .

[3]  R. Shapka Geomagnetic Effects on Modern Pipeline Systems , 1993 .

[4]  G. Fischer Electromagnetic induction effects at an ocean coast , 1979, Proceedings of the IEEE.

[5]  Alan G. Jones,et al.  Resistivity cross section through the Juan de Fuca Subduction System and its tectonic implications , 1989 .

[6]  Louis J. Lanzerotti,et al.  Induction of Currents in Long Submarine Cables by Natural Phenomena (Paper 2R1945) , 1983 .

[7]  Antti Pulkkinen,et al.  Recordings and occurrence of geomagnetically induced currents in the Finnish natural gas pipeline network , 2001 .

[8]  P Eng,et al.  GIC effects on pipeline corrosion and corrosion control systems , 2002 .

[9]  J. T. Weaver Mathematical methods for geo-electromagnetic induction , 1994 .

[10]  G. Heinson,et al.  An application of thin-sheet electromagnetic modelling to the Tasman Sea , 1993 .

[11]  J. Filloux,et al.  Geomagnetic induction in the Tasman Sea and electrical conductivity structure beneath the Tasman Seafloor , 1990 .

[12]  N. Bindoff,et al.  The Tasman Project of Seafloor Magnetotelluric Exploration: experiment and observations , 1989 .

[13]  J. P. Greenhouse,et al.  Geomagnetic variation sounding of the asthenosphere beneath the Juan de Fuca Ridge , 1981 .

[14]  J.G. Kappenman,et al.  Geomagnetic Storms and Their Impact on Power Systems , 1996, IEEE Power Engineering Review.

[15]  R. Kurtz,et al.  Magnetotelluric measurements over the Alpha Ridge , 1987 .

[16]  S. Constable,et al.  In defence of a resistive oceanic upper mantle: reply to a Comment by Tarits, Chave and Schultz , 1993 .

[17]  A. Viljanen,et al.  Geomagnetically induced currents in the Finnish high-voltage power system , 1994 .

[18]  R. V. Herzen,et al.  Electrical resistivity structure beneath the North-west Atlantic Ocean , 1976 .

[19]  Henty Root Earth-Current Effects on Communication-Cable Power Subsystems , 1979, IEEE Transactions on Electromagnetic Compatibility.

[20]  Carol G. Maclennan,et al.  Geoelectric power spectra over oceanic distances , 1995 .