Field Detection of Microcracks to Define the Nucleation Stage of Earthquake Occurrence

Main shocks of natural earthquakes are known to be accompanied by preshocks which evolve following the modified Ohmori’s law in average over many samples. Individual preshock activity, however, is far less systematic for predictive purposes. On the other hand, the microcracks in laboratory rock experiments are always preceded to final rupture. And, previous investigations of field acoustic emissions showed that the activity increases prominently before and after the main shock. But there is no detection of any phenomena to identify the nucleation stage. Here we show that a special underground electric field measurement could detect microcracks. Pulse-like variations were classified into three groups (A, B, C) by frequency. The B-type is suggested to define the nucleation period: activity increases sharply following the modified Omori’s law before the main shock and there is no activity afterward. The B-type is subgrouped into three types possibly corresponding to crack-rupture modes. The variations are supposed to be induced by crack occurrence through electrokinetic effects in the elastic-porous medium. The detection distance is suggested to be several orders larger than that of the acoustic emission due to the effective smallness of dissipation rate, and the waveform can be used to infer the rupture mode.

[1]  Bijan Nourbehect,et al.  Irreversible thermodynamic effects in inhomogeneous media and their applications in certain geoelectric problems , 1963 .

[2]  J Oliver,et al.  Earthquake Prediction , 1987, Journal of the World Association for Emergency and Disaster Medicine.

[3]  David V. Fitterman,et al.  Electrokinetic and magnetic anomalies associated with dilatant regions in a layered Earth , 1978 .

[4]  Lucile M. Jones,et al.  Some characteristics of foreshocks and their possible relationship to earthquake prediction , 1979 .

[5]  Vincent P. Drnevich,et al.  Acoustic emissions in geotechnical engineering practice , 1981 .

[6]  T. Ishido,et al.  Experimental and theoretical basis of electrokinetic phenomena in rock‐water systems and its applications to geophysics , 1981 .

[7]  T. Rikitake Earthquake forecasting and warning , 1982 .

[8]  David J. Varnes,et al.  Predicting earthquakes by analyzing accelerating precursory seismic activity , 1989 .

[9]  Christopher H. Scholz,et al.  Elastic properties of contacting surfaces under normal and shear loads: 2. Comparison of theory with experiment , 1989 .

[10]  Y. Fujinawa,et al.  Emission of electromagnetic radiation preceding the Ito seismic swarm of 1989 , 1990, Nature.

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

[12]  Y. Fujinawa,et al.  A study of anomalous underground electric field variations associated with a volcanic eruption , 1992 .

[13]  F. Dale Morgan,et al.  Electromagnetic precursors to earthquakes in the Ulf band: A review of observations and mechanisms , 1993 .

[14]  Pride,et al.  Governing equations for the coupled electromagnetics and acoustics of porous media. , 1994, Physical review. B, Condensed matter.

[15]  早川 正士,et al.  Electromagnetic phenomena related to earthquake prediction , 1994 .

[16]  Didier Sornette,et al.  Complex Critical Exponents from Renormalization Group Theory of Earthquakes: Implications for Earthquake Predictions , 1995 .

[17]  M. Ohnaka A shear failure strength law of rock in the brittle-plastic transition regime , 1995 .

[18]  J. Byerlee,et al.  Magnetic and electric fields associated with changes in high pore pressure in fault zones : Application to the Loma Prieta ULF emissions , 1995 .

[19]  Y. Fujinawa,et al.  Experiments to Locate Sources of Earthquake-related VLF Electromagnetic Signals , 1997 .

[20]  Steven R. Pride,et al.  Electroseismic waves from point sources in layered media , 1997 .

[21]  Y. Fujinawa,et al.  Electromagnetic radiations associated with major earthquakes , 1998 .

[22]  P. Sammonds,et al.  Electric potential changes prior to shear fracture in dry and saturated rocks , 1998 .

[23]  Masashi Hayakawa,et al.  Atmospheric and ionospheric electromagnetic phenomena associated with earthquakes , 1999 .

[24]  K. Maeda Time Distribution of Immediate Foreshocks Obtained by a Stacking Method , 1999 .

[25]  T. Nagao,et al.  Co‐seismic geoelectric potential changes observed in Japan , 2000 .

[26]  D. Sornette,et al.  Reexamination of log periodicity observed in the seismic precursors of the 1989 Loma Prieta earthquake , 2000 .

[27]  O. Nishizawa,et al.  Quasi‐static fault growth and cracking in homogeneous brittle rock under triaxial compression using acoustic emission monitoring , 2000 .

[28]  Naum I. Gershenzon,et al.  Modeling of Seismo-Electromagnetic Phenomena , 2001 .

[29]  T. Doi,et al.  Electric Field Variations Related to Seismic Swarms , 2002 .

[30]  Y. Fujinawa,et al.  Modeling confined pressure changes inducing anomalous electromagnetic fields related with earthquakes , 2002 .

[31]  Philippe Labazuy,et al.  The volcano‐electric effect , 2003 .

[32]  Lindsay M. Linzer,et al.  Source parameters of acoustic emission events and scaling with mining‐induced seismicity , 2003 .

[33]  S. Yoshida,et al.  Electromagnetic emissions from dry and wet granite associated with acoustic emissions , 2004 .

[34]  Xinglin Lei,et al.  Detailed analysis of acoustic emission activity during catastrophic fracture of faults in rock , 2004 .

[35]  K. Nomicos,et al.  Distinguished seismological and electromagnetic features of the impending global failure: Did the 7/9/1999 M5.9 Athens earthquake come with a warning? , 2005 .

[36]  Alexander Schekotov,et al.  Near-seismic effects in ULF fields and seismo-acoustic emission: statistics and explanation , 2005 .

[37]  F. Lefeuvre,et al.  The magnetic field experiment IMSC and its data processing onboard DEMETER: Scientific objectives, description and first results , 2006 .

[38]  Steven D. Glaser,et al.  Self-potential observations during hydraulic fracturing , 2007 .

[39]  C. Shieh,et al.  Evaluation of the effects of ground shaking and static volumetric strain change on earthquake-related groundwater level changes in Taiwan , 2010 .

[40]  D. Prior,et al.  Effects of crystallographic anisotropy on fracture development and acoustic emission in quartz , 2010 .

[41]  Hengshan Hu,et al.  Seismoelectromagnetic waves radiated by a double couple source in a saturated porous medium , 2010 .

[42]  Haruko Sekiguchi,et al.  Rupture process of the 2011 Tohoku‐Oki mega‐thrust earthquake (M9.0) inverted from strong‐motion data , 2011 .

[43]  Yoichi Noda,et al.  Remote Detection of the Electric Field Change Induced at the Seismic Wave Front from the Start of Fault Rupturing , 2011 .

[44]  M. Karaoulis,et al.  Imaging with cross-hole seismoelectric tomography , 2012 .

[45]  Evert Slob,et al.  Experimental Validation of the Electrokinetic Theory and Development of Seismoelectric Interferometry by Cross-Correlation , 2012 .

[46]  Qinghua Huang,et al.  Numerical simulation of coseismic electromagnetic fields associated with seismic waves due to finite faulting in porous media , 2012 .

[47]  Katsumi Hattori,et al.  Investigation of ULF Seismo-Magnetic Phenomena in Kanto, Japan During 2000–2010: Case Studies and Statistical Studies , 2013, Surveys in Geophysics.

[48]  K. Eftaxias,et al.  On the puzzling feature of the silence of precursory electromagnetic emissions , 2013 .

[49]  K. Eftaxias,et al.  Current challenges for pre-earthquake electromagnetic emissions: shedding light from micro-scale plastic flow, granular packings, phase transitions and self-affinity notion of fracture process , 2013 .

[50]  Yoshimori Honkura,et al.  Rapid changes in the electrical state of the 1999 Izmit earthquake rupture zone , 2013, Nature Communications.