Abstract:Abstract. The Kobe earthquake of January 17, 1995, which had a weathered granite fault wall as shown by arrow B in Figure lb; magnitude of 7.2, was accompanied by earthquake hghtning and 3) the clayey fault gouge under the part where the charred (EQL). The fault gouge near ground level at the Nojima fault, roots were found was highly lithified and showed a lamellar near where the EQL was witnessed, was highly lithified and structure. anomalously mag-netized. The characterization of the fault gouge and the muds… Show more
“…Recently, a number of examples of high magnetic susceptibility within fault gouges have been described from several faults related to large earthquakes (Enomoto and Zheng 1998;Nakamura and Nagahama 2001;Fukuchi et al 2005;Hirono et al 2006;Mishima et al 2006Mishima et al , 2009. Similarly, some core gouges with high magnetic susceptibility occur within the WFSD-1 core.…”
Section: Relationship Between Magnetic Susceptibility and Fault Rocksmentioning
confidence: 99%
“…Magnetic susceptibility and rock magnetism have commonly been used to understand the physical characteristics and chemical processes of fault slip zones (Enomoto and Zheng 1998;Nakamura and Nagahama 2001;Ferré et al 2005Ferré et al , 2012. Correlations have been reported between magnetic susceptibility anomalies in borehole log data and the presence of cataclastic zones and faults in the main drill borehole of the German Deep Drilling Project (KTB) (Bosum et al 1997), but the magnetic susceptibility of drill cuttings in the KTB do not support this correlation (Rauen et al 2000).…”
We measured the magnetic susceptibility of the core from the first borehole of the Wenchuan Earthquake (May 12, 2008, Mw7.9) Fault Scientific Drilling Project (WFSD-1) at 1-cm intervals. The correlations between magnetic susceptibility anomalies and fault rock occurrence are shown by a few fault zones in the WFSD-1 core. The values for the mass and ferromagnetic material magnetic susceptibility for the sample at 589.25-m depth are higher than those for the other samples. All the thermomagnetic curves display a rapid increase in slope after 380°C, and a marked peak occurs at about 510°C in the heating curves. The cooling curves are clearly higher than the heating curves. The saturation magnetization (Ms) shows a significant peak at a depth of 589.25 m, as do the mass magnetic susceptibility and the ferrimagnetic magnetic susceptibility. The mechanism principally responsible for the high magnetic susceptibility at a depth of 589.25 m might be the production of new magnetite from iron-bearing silicates (e.g., chlorite) or clays caused by frictional heating during seismic slip. Therefore, we suggest that the presence of high magnetic susceptibility fault gouges in the same country rock can be considered as an indicator of earthquakes or seismic signatures.
“…Recently, a number of examples of high magnetic susceptibility within fault gouges have been described from several faults related to large earthquakes (Enomoto and Zheng 1998;Nakamura and Nagahama 2001;Fukuchi et al 2005;Hirono et al 2006;Mishima et al 2006Mishima et al , 2009. Similarly, some core gouges with high magnetic susceptibility occur within the WFSD-1 core.…”
Section: Relationship Between Magnetic Susceptibility and Fault Rocksmentioning
confidence: 99%
“…Magnetic susceptibility and rock magnetism have commonly been used to understand the physical characteristics and chemical processes of fault slip zones (Enomoto and Zheng 1998;Nakamura and Nagahama 2001;Ferré et al 2005Ferré et al , 2012. Correlations have been reported between magnetic susceptibility anomalies in borehole log data and the presence of cataclastic zones and faults in the main drill borehole of the German Deep Drilling Project (KTB) (Bosum et al 1997), but the magnetic susceptibility of drill cuttings in the KTB do not support this correlation (Rauen et al 2000).…”
We measured the magnetic susceptibility of the core from the first borehole of the Wenchuan Earthquake (May 12, 2008, Mw7.9) Fault Scientific Drilling Project (WFSD-1) at 1-cm intervals. The correlations between magnetic susceptibility anomalies and fault rock occurrence are shown by a few fault zones in the WFSD-1 core. The values for the mass and ferromagnetic material magnetic susceptibility for the sample at 589.25-m depth are higher than those for the other samples. All the thermomagnetic curves display a rapid increase in slope after 380°C, and a marked peak occurs at about 510°C in the heating curves. The cooling curves are clearly higher than the heating curves. The saturation magnetization (Ms) shows a significant peak at a depth of 589.25 m, as do the mass magnetic susceptibility and the ferrimagnetic magnetic susceptibility. The mechanism principally responsible for the high magnetic susceptibility at a depth of 589.25 m might be the production of new magnetite from iron-bearing silicates (e.g., chlorite) or clays caused by frictional heating during seismic slip. Therefore, we suggest that the presence of high magnetic susceptibility fault gouges in the same country rock can be considered as an indicator of earthquakes or seismic signatures.
“…Fukuchi (2003) indicated that Nojima fault gouge contains antiferromagnetic minerals such as kaolinite or smectite that can be changed into ferrimagnetic minerals such as maghemite by thermal dehydration. Nojima fault gouge contains siderite (FeCO 3 ) (Enomoto and Zheng 1998), which thermally decomposes into magnetite with carbon dioxide at 470 °C under reducing conditions (French 1971). Mishima et al (2009) showed that paramagnetic minerals such as siderite in Taiwan Chelungpu fault gouge changed into ferrimagnetic magnetite through thermal decomposition above about 400 °C.…”
Section: Introductionmentioning
confidence: 99%
“…First, ferrimagnetic minerals in the fault slip zone may acquire a thermal remanent magnetization (TRM) upon cooling (Piper and Poppleton 1988;Ferré et al 2014). Second, earthquake lightning may constitute an additional magnetization process (Enomoto and Zheng 1998;Ferré et al 2005). Third, a fault slip zone may acquire chemical remanent magnetization (CRM) due to neoformation of ferrimagnetic minerals by thermal decomposition during seismic slips (Nakamura et al 2002;Fukuchi 2003;Fukuchi et al 2005;Hirono et al 2006;Chou et al 2012); it can be explained that many kinds of antiferromagnetic or paramagnetic minerals are thermally decomposed into ferrimagnetic minerals.…”
Microscopic billow-like wavy folds have been observed along slip planes of the Nojima active fault, southwest Japan. The folds are similar in form to Kelvin-Helmholtz (KH) instabilities occurring in fluids, which implies that the slip zone underwent "lubrication" such as frictional melting or fluidization of fault gouge materials. If the temperature range for generation of the billow-like wavy folds can be determined, we can constrain the physical properties of fault gouge materials during seismic slip. Here, we report on rock magnetic studies that identify seismic slip zones associated with the folds, and their temperature rises during ancient seismic slips of the Nojima active fault. Using a scanning magneto-impedance magnetic microscope and a scanning superconducting quantum interference device microscope, we observed surface stray magnetic field distributions over the folds, indicating that the folds and slip zones are strongly magnetized. This is due to the production of magnetite through thermal decomposition of antiferromagnetic or paramagnetic minerals in the gouge at temperatures over 350 °C. The presence of micrometer-sized finely comminuted materials in the billow-like wavy folds, along with our rock magnetic results, suggests that frictional heatinginduced fluidization was the driving mechanism of faulting. We found that the existence of the magnetized KH-type billow-like wavy folds supports that the low-viscosity fluid induced by fluidization after frictional heating decreased the frictional strength of the fault slip zone.
“…But the melted zones do not constitute the continuos, non-interrupted barrier to charge spreading. Moreover, the most intense light flashes (lightning-like discharges) were seen above the strait with sea water having electric conductivity much higher than the typical conductivity of wet rocks (Enomoto and Zheng, 1998). So we propose alternative mechanism -the skin effect, invoking diffusion of electric currents and magnetic fields in the highly conductive medium from the current generation zone due to nonstationary magnetoelectrodynamic processes (Nemtchinov, 2002;Nemtchinov and Losseva, 2002;Losseva and Nemtchinov, 2002).…”
Abstract.A physical model of earthquake lights is proposed. It is suggested that the magnetic diffusion from the electric and magnetic fields source region is a dominant process, explaining rather high localization of the light flashes. A 3D numerical code allowing to take into account the arbitrary distribution of currents caused by ground motion, conductivity in the ground and at its surface, including the existence of sea water above the epicenter or (and) near the ruptured segments of the fault have been developed. Simulations for the 1995 Kobe earthquake were conducted taking into account the existence of sea water with realistic geometry of shores. The results do not contradict the eyewitness reports and scarce measurements of the electric and magnetic fields at large distances from the epicenter.
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