Coupled interaction of earthquake nucleation with deep Earth gases: a possible mechanism for seismo-electromagnetic phenomena

SUMMARY The mechanisms of seismo-electromagnetic phenomena remain largely unexplained. To address this issue, we introduce a fault model that takes account of a coupled interaction between earthquake nucleation and deep Earth gases. This interaction causes a negatively electrified gas flow due to an exo-electron attachment reaction, as the gases pass through fractured asperities. This transient activity may be regarded to be a pressure-impressed electric current generator. In the model, the current and frequency are formulated as functions of earthquake parameters. The estimated current is sufficient to explain the seismic electromagnetic signals observed at ground level. A physical model of how current generation is coupled with ionospheric electromagnetic disturbances is explained in terms of magnetic induction coupling for strong offshore earthquakes, which may provide a plausible explanation of observed ionospheric electron enhancement prior to some recent offshore earthquakes. The model also suggests that geomagnetic observations close to an epicentre of a strong offshore earthquake may provide an effective means of detecting clear and identifiable precursor signals.

[1]  P. Bernard Plausibility of long distance electrotelluric precursors to earthquakes , 1992 .

[2]  H. Hashimoto,et al.  Emission of charged particles from indentation fracture of rocks , 1990, Nature.

[3]  M. M. Chaudhri,et al.  Fracto‐emission during Fracture of Engineering Ceramics , 1993 .

[4]  D. L. Anderson,et al.  Theoretical Basis of Some Empirical Relations in Seismology by Hiroo Kanamori And , 1975 .

[5]  D. J. Strauss,et al.  SOME OBSERVATIONS ABOUT THE STATISTICAL SIGNIFICANCE AND PHYSICAL MECHANISMS OF THE VAN METHOD OF EARTHQUAKE PREDICTION, GREECE , 1996 .

[6]  M. Butala,et al.  On the reported ionospheric precursor of the 1999 Hector Mine, California earthquake , 2012 .

[7]  A. Duba,et al.  Carbon‐enhanced electrical conductivity during fracture of rocks , 1999 .

[8]  D. Wells,et al.  New empirical relationships among magnitude, rupture length, rupture width, rupture area, and surface displacement , 1994, Bulletin of the Seismological Society of America.

[9]  Masashi Kamogawa,et al.  Short-term earthquake prediction: Current status of seismo-electromagnetics , 2009 .

[10]  K. Heki Ionospheric electron enhancement preceding the 2011 Tohoku‐Oki earthquake , 2011 .

[11]  S. Pulinets,et al.  Lithosphere-Atmosphere-Ionosphere Coupling (LAIC) Model - An Unified Concept for Earthquake Precursors Validation , 2011 .

[12]  Sergey Pulinets,et al.  Recent progress in seismo electromagnetics and related phenomena , 2006 .

[13]  Cheng-Ling Kuo,et al.  Ionosphere plasma bubbles and density variations induced by pre‐earthquake rock currents and associated surface charges , 2011 .

[14]  M. Parrot Statistical analysis of the ion density measured by the satellite DEMETER in relation with the seismic activity , 2011 .

[15]  The electrification of flowing gases by mechanical abrasion of mineral surfaces , 1998 .

[16]  Y. Kagan,et al.  Earthquakes Cannot Be Predicted , 1997, Science.

[17]  Stephen B. M. Beck,et al.  Measurement of fluid flow rates through cracks , 1997 .

[18]  B. Shibazaki,et al.  Transition process from nucleation to high-speed rupture propagation: scaling from stick-slip experiments to natural earthquakes , 2002 .

[19]  M. Ladd,et al.  Low‐frequency magnetic field measurements near the epicenter of the Ms 7.1 Loma Prieta Earthquake , 1990 .

[20]  Geomagnetic field changes in response to the 2011 off the Pacific Coast of Tohoku Earthquake and Tsunami , 2011 .

[21]  A. Viljanen,et al.  Induction effects on ionospheric electric and magnetic fields , 2005 .

[22]  Efthimios S. Skordas,et al.  On the recent advances in the study of seismic electric signals (VAN method) , 2006 .

[23]  Hiroo Kanamori,et al.  Earthquake Prediction: An Overview , 2003 .

[24]  F. Wenzel,et al.  Seismic results at Kola and KTB deep scientific boreholes: velocities, reflections, fluids, and crustal composition , 2000 .

[25]  Clifford C. Walters,et al.  The Origin of Petroleum , 2006 .

[26]  D. Mogk,et al.  Carbonaceous films in midcrustal rocks from the KTB borehole, Germany, as characterized by time‐of‐flight secondary ion mass spectrometry , 2000 .