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Generation of electromotive force in igneous rocks subjected to non-uniform loading

Generation of electromotive force in igneous rocks subjected to non-uniform loading
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摘要 When one end of an air-dry igneous rock block was uniaxially loaded in laboratory, there appeared an electromotive force that made electric currents flow from the stressed volume to the unstressed volume. Quartz-free rocks such as gabbro also generated this force, stronger than quartz-bearing rocks such as granite. This indicates that the piezoelectric effect of quartz and the electrokinetic effect of pore water do not make a large contribution toward generating the electromotive force. We focus on peroxy bond that is one of the abundant lattice defects in igneous rock-forming minerals. When mechanical loading deforms the lattice structure around this defect and breaks its bond, its energy levels change and act like an accepter. As an electron is trapped at this defect from a neighbor 02- site, a positive hole is activated there. They attempt to diffuse toward the unstressed volume through the valence band and are simultaneously affected by the attractive electric force with the electrons trapped in peroxy bonds. This leads to a polarization in the stressed volume and the generation of electromotive force between the stressed and unstressed volumes. Similar electromotive force may be generated in the Earth's crust where inhomogeneous stress/strain is changing. When one end of an air-dry igneous rock block was uniaxially loaded in laboratory, there appeared an electromotive force that made electric currents flow from the stressed volume to the unstressed volume. Quartz-free rocks such as gabbro also generated this force, stronger than quartz-bearing rocks such as granite. This indicates that the piezoelectric effect of quartz and the electrokinetic effect of pore water do not make a large contribution toward generating the electromotive force. We focus on peroxy bond that is one of the abundant lattice defects in igneous rock-forming minerals. When mechanical loading deforms the lattice structure around this defect and breaks its bond, its energy levels change and act like an accepter. As an electron is trapped at this defect from a neighbor 02- site, a positive hole is activated there. They attempt to diffuse toward the unstressed volume through the valence band and are simultaneously affected by the attractive electric force with the electrons trapped in peroxy bonds. This leads to a polarization in the stressed volume and the generation of electromotive force between the stressed and unstressed volumes. Similar electromotive force may be generated in the Earth's crust where inhomogeneous stress/strain is changing.
出处 《Earthquake Science》 CSCD 2011年第6期593-600,共8页 地震学报(英文版)
基金 partially supported by"Observation and Research Program for Prediction of Earthquakes and Volcanic Eruptions"of the Ministry of Education,Culture,Sports,Science and Technology of Japan,"FY2010 Research Incentive Assistance Program"of Educational System General Research Organization,Tokai University "Individual Research Projects"of Institute of Oceanic Development of Science and Technology,Tokai University
关键词 electromotive force igneous rock non-uniform loading positive hole electromotive force igneous rock non-uniform loading positive hole
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  • 1Aydan O, Kyoya T, Ichikawa Y, Kawamoto T, Ito T and Shimizu Y (1988). Three-dimensional simulation of an advancing tunnel supported with forepoles, shotcrete, steel ribs and rockbolts. In: Swoboda G eds. Numeri- cal Methods in Geomechanics, Innsbruck 1988. Proceed- ings of the Sixth International Conference on Numerical Methods in Geomechanics. Balkema Publications, Rot- terdam, Netherlands, 1 481 1 486.
  • 2Aydan O, Uehara F and Kawamoto T (2011). A numer- ical study on the long-term performance of an under- ground powerhouse subjected to varying initial stress state, cyclic water head and temperature variations. In- ternational Journal of Geomechanics (in press).
  • 3Aydin A, Prance R J, Prance H and Harland C J (2009). Observation of pressure stimulated voltages in rock us- ing an electric potential sensor. Appl Phys Lett 95(12): 124102.
  • 4Balk M, Bose M, Ertem G, Rogoff D A, Rothschild L J and Freund F T (2009). Oxidation of water to hydrogen per- oxide at the rock-water interface due to stress-activated electric currents in rocks. Earth Planet Sci Lett 283(1-4): 87-92.
  • 5Finkelstein D, Hill R D and Powell J R (1973). The piezo- electric theory of earthquake lightning. J Geophys Res 78(6): 992-993.
  • 6Fitterman D V (1978). Electrokinetic and magnetic anoma- lies associated with dilatant regions in a layered earth. J Geophys Res 83(B12): 5 923- 5 928.
  • 7Freund F T (2010). "Toward a unified solid state theory for pre-earthquake signals. Acta Geophysica 58(5): 719-766.
  • 8Freund F T, Kulahci I G, Cyr G, Ling J, Winnick M, Tregloan-Reed J and Freund M M (2009). Air ioniza- tion at rock surfaces and pre-earthquake signals. Journal of Atmospheric and Solar-Terrestrial Physics 71(17-18): 1 824-1 834.
  • 9Grant R A, Halliday T, Balderer W P, Leuenberger F, New- comer M, Cyr G and Freund F T (2011). Ground water chemistry changes before major earthquakes and possible effects on animals. International Journal of Environrnen- tal Research and Public Health 8(6): 1 936-1 956.
  • 10Ishido T and Mizutani H (1981). Experimental and theo- retical basis of electrokinetic phenomena in rock-water systems and its applications to geophysics. Journal of Geophvsics 86(B3): 1 763- 1 775.

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