Piezomagnetic potentials due to an inclined rectangular fault in a semi-infinite medium
Analytical solutions for the piezomagnetic potentials are derived for strike-slip, dip-slip and tensile-opening fault motions with arbitrary dip and strike angles, so as to be applicable in various types of earthquakes. These solutions are expressed as the composition of elementary functions which a...
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Veröffentlicht in: | Geophysical journal international 2000-03, Vol.140 (3), p.479-492 |
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description | Analytical solutions for the piezomagnetic potentials are derived for strike-slip, dip-slip and tensile-opening fault motions with arbitrary dip and strike angles, so as to be applicable in various types of earthquakes. These solutions are expressed as the composition of elementary functions which are identical to the magnetic potentials produced by magnetic dipoles, quadrupoles and octupoles distributed on the fault plane and other planes. Therefore, the geomagnetic field changes due to the piezomagnetic effect are expressed by the superposition of the fields produced by these equivalent sources. Examples of calculated results show characteristic features for various types of fault motions as follows: (1) the pattern of the geomagnetic field changes becomes significantly different depending on the strike direction, although the maximum amplitude is almost the same for all directions; (2) the geomagnetic field change reaches a maximum at a dip angle of 90° for strike-slip and tensile-opening fault motions and at 45° for dip-slip fault motion. |
doi_str_mv | 10.1046/j.1365-246X.2000.00953.x |
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These solutions are expressed as the composition of elementary functions which are identical to the magnetic potentials produced by magnetic dipoles, quadrupoles and octupoles distributed on the fault plane and other planes. Therefore, the geomagnetic field changes due to the piezomagnetic effect are expressed by the superposition of the fields produced by these equivalent sources. Examples of calculated results show characteristic features for various types of fault motions as follows: (1) the pattern of the geomagnetic field changes becomes significantly different depending on the strike direction, although the maximum amplitude is almost the same for all directions; (2) the geomagnetic field change reaches a maximum at a dip angle of 90° for strike-slip and tensile-opening fault motions and at 45° for dip-slip fault motion.</description><identifier>ISSN: 0956-540X</identifier><identifier>EISSN: 1365-246X</identifier><identifier>DOI: 10.1046/j.1365-246X.2000.00953.x</identifier><language>eng</language><publisher>Oxford, UK: Blackwell Science Ltd</publisher><subject>inclined fault ; piezomagnetic potential ; seismomagnetic effect</subject><ispartof>Geophysical journal international, 2000-03, Vol.140 (3), p.479-492</ispartof><rights>2000 RAS 2000</rights><lds50>peer_reviewed</lds50><oa>free_for_read</oa><woscitedreferencessubscribed>false</woscitedreferencessubscribed><citedby>FETCH-LOGICAL-a4463-6b47025de888b7cc38288f61ba90505f5b2638345c4de1d3cecf0a72b90f49843</citedby><cites>FETCH-LOGICAL-a4463-6b47025de888b7cc38288f61ba90505f5b2638345c4de1d3cecf0a72b90f49843</cites></display><links><openurl>$$Topenurl_article</openurl><openurlfulltext>$$Topenurlfull_article</openurlfulltext><thumbnail>$$Tsyndetics_thumb_exl</thumbnail><linktopdf>$$Uhttps://onlinelibrary.wiley.com/doi/pdf/10.1046%2Fj.1365-246X.2000.00953.x$$EPDF$$P50$$Gwiley$$H</linktopdf><linktohtml>$$Uhttps://onlinelibrary.wiley.com/doi/full/10.1046%2Fj.1365-246X.2000.00953.x$$EHTML$$P50$$Gwiley$$H</linktohtml><link.rule.ids>314,780,784,1417,27924,27925,45574,45575</link.rule.ids></links><search><creatorcontrib>Utsugi, Mitsuru</creatorcontrib><creatorcontrib>Nishida, Yasunori</creatorcontrib><creatorcontrib>Sasai, Yoichi</creatorcontrib><title>Piezomagnetic potentials due to an inclined rectangular fault in a semi-infinite medium</title><title>Geophysical journal international</title><addtitle>Geophys. 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Examples of calculated results show characteristic features for various types of fault motions as follows: (1) the pattern of the geomagnetic field changes becomes significantly different depending on the strike direction, although the maximum amplitude is almost the same for all directions; (2) the geomagnetic field change reaches a maximum at a dip angle of 90° for strike-slip and tensile-opening fault motions and at 45° for dip-slip fault motion.</description><subject>inclined fault</subject><subject>piezomagnetic potential</subject><subject>seismomagnetic effect</subject><issn>0956-540X</issn><issn>1365-246X</issn><fulltext>true</fulltext><rsrctype>article</rsrctype><creationdate>2000</creationdate><recordtype>article</recordtype><recordid>eNqNkEtv1DAQgC0EEtvCf_CJW9Jx_IhX4oIW-pZaIRArLpbjTCovibONHbHl1zdpUE9F4jSjmflmNB8hlEHOQKiTXc64klkh1DYvACAHWEueH16R1XPjNVlNRZVJAdu35CjGHQATTOgV-XHr8U_f2buAyTu67xOG5G0baT0iTT21gfrgWh-wpgO6ZMPd2NqBNnZs09SilkbsfOZD44NPSDus_di9I2-aaQu-_xuPyffTL98259n1zdnF5tN1ZoVQPFOVKKGQNWqtq9I5rgutG8UquwYJspFVobjmQjpRI6u5Q9eALYtqDY1Ya8GPyYdl737o70eMyXQ-OmxbG7AfoylKpUpesmlQL4Nu6GMcsDH7wXd2eDAMzGzS7MwszMzCzGzSPJk0hwn9uKC_fYsP_82Zs8uLKZlwvuD9uP8HnL10NFsoHxMenjk7_DLzQ9Kcb38apeB2oz9fma_8ESTumMg</recordid><startdate>200003</startdate><enddate>200003</enddate><creator>Utsugi, Mitsuru</creator><creator>Nishida, Yasunori</creator><creator>Sasai, Yoichi</creator><general>Blackwell Science Ltd</general><scope>BSCLL</scope><scope>AAYXX</scope><scope>CITATION</scope><scope>8FD</scope><scope>H8D</scope><scope>L7M</scope></search><sort><creationdate>200003</creationdate><title>Piezomagnetic potentials due to an inclined rectangular fault in a semi-infinite medium</title><author>Utsugi, Mitsuru ; Nishida, Yasunori ; Sasai, Yoichi</author></sort><facets><frbrtype>5</frbrtype><frbrgroupid>cdi_FETCH-LOGICAL-a4463-6b47025de888b7cc38288f61ba90505f5b2638345c4de1d3cecf0a72b90f49843</frbrgroupid><rsrctype>articles</rsrctype><prefilter>articles</prefilter><language>eng</language><creationdate>2000</creationdate><topic>inclined fault</topic><topic>piezomagnetic potential</topic><topic>seismomagnetic effect</topic><toplevel>peer_reviewed</toplevel><toplevel>online_resources</toplevel><creatorcontrib>Utsugi, Mitsuru</creatorcontrib><creatorcontrib>Nishida, Yasunori</creatorcontrib><creatorcontrib>Sasai, Yoichi</creatorcontrib><collection>Istex</collection><collection>CrossRef</collection><collection>Technology Research Database</collection><collection>Aerospace Database</collection><collection>Advanced Technologies Database with Aerospace</collection><jtitle>Geophysical journal international</jtitle></facets><delivery><delcategory>Remote Search Resource</delcategory><fulltext>fulltext</fulltext></delivery><addata><au>Utsugi, Mitsuru</au><au>Nishida, Yasunori</au><au>Sasai, Yoichi</au><format>journal</format><genre>article</genre><ristype>JOUR</ristype><atitle>Piezomagnetic potentials due to an inclined rectangular fault in a semi-infinite medium</atitle><jtitle>Geophysical journal international</jtitle><stitle>Geophys. J. Int</stitle><addtitle>Geophys. J. Int</addtitle><date>2000-03</date><risdate>2000</risdate><volume>140</volume><issue>3</issue><spage>479</spage><epage>492</epage><pages>479-492</pages><issn>0956-540X</issn><eissn>1365-246X</eissn><abstract>Analytical solutions for the piezomagnetic potentials are derived for strike-slip, dip-slip and tensile-opening fault motions with arbitrary dip and strike angles, so as to be applicable in various types of earthquakes. These solutions are expressed as the composition of elementary functions which are identical to the magnetic potentials produced by magnetic dipoles, quadrupoles and octupoles distributed on the fault plane and other planes. Therefore, the geomagnetic field changes due to the piezomagnetic effect are expressed by the superposition of the fields produced by these equivalent sources. Examples of calculated results show characteristic features for various types of fault motions as follows: (1) the pattern of the geomagnetic field changes becomes significantly different depending on the strike direction, although the maximum amplitude is almost the same for all directions; (2) the geomagnetic field change reaches a maximum at a dip angle of 90° for strike-slip and tensile-opening fault motions and at 45° for dip-slip fault motion.</abstract><cop>Oxford, UK</cop><pub>Blackwell Science Ltd</pub><doi>10.1046/j.1365-246X.2000.00953.x</doi><tpages>14</tpages><oa>free_for_read</oa></addata></record> |
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title | Piezomagnetic potentials due to an inclined rectangular fault in a semi-infinite medium |
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