{"created":"2023-03-31T01:54:14.465817+00:00","id":4462,"links":{},"metadata":{"_buckets":{"deposit":"e52bf8c9-2a1a-4536-abf2-862b4d38272c"},"_deposit":{"id":"4462","owners":[1],"pid":{"revision_id":0,"type":"depid","value":"4462"},"status":"published"},"_oai":{"id":"oai:nied-repo.bosai.go.jp:00004462","sets":[]},"author_link":[],"item_10001_biblio_info_7":{"attribute_name":"書誌情報","attribute_value_mlt":[{"bibliographicIssueDates":{"bibliographicIssueDate":"2002-02"},"bibliographicIssueNumber":"B2","bibliographicVolumeNumber":"107","bibliographic_titles":[{"bibliographic_title":"JOURNAL OF GEOPHYSICAL RESEARCH-SOLID EARTH","bibliographic_titleLang":"en"}]}]},"item_10001_description_5":{"attribute_name":"抄録","attribute_value_mlt":[{"subitem_description":"[1] We study a symmetrical three-forked shear fault under simple triaxial stress. Rupture initiates in the central primary plane and propagates toward the branching point. One of the two branches is in the compressional quadrant, while the other is in the tensional domain. We study the following question: Does rupture always prefer propagating along the tensional branch because of the effect of normal stress? When the primary plane is located in the most favorable direction as determined by Mohr-Coulomb criterion, one finds that the compressional branch is almost always preferred for various dynamic coefficients and confining pressures. Simultaneous rupture propagation on both branches appears only under a very special condition found by Aochi et al. [2000b]. These results indicate that shear stress changes produced by the rupture front dominate during dynamic rupture propagation, compared to normal stress changes. This result depends completely on the orientation of the whole fault system. In all cases, we can explain the branch selection by analyzing the applied initial shear stress and the fault properties. Change of normal stress may play a role similar to shear stress change for disjoint faults since the effect of normal stress change sometimes dominates.","subitem_description_language":"en","subitem_description_type":"Other"}]},"item_10001_publisher_8":{"attribute_name":"出版者","attribute_value_mlt":[{"subitem_publisher":"AMER GEOPHYSICAL UNION","subitem_publisher_language":"en"}]},"item_10001_relation_14":{"attribute_name":"DOI","attribute_value_mlt":[{"subitem_relation_type_id":{"subitem_relation_type_id_text":"10.1029/2001JB000500"}}]},"item_10001_source_id_9":{"attribute_name":"ISSN","attribute_value_mlt":[{"subitem_source_identifier":"2169-9356","subitem_source_identifier_type":"EISSN"}]},"item_creator":{"attribute_name":"著者","attribute_type":"creator","attribute_value_mlt":[{"creatorNames":[{"creatorName":"H Aochi","creatorNameLang":"en"}]},{"creatorNames":[{"creatorName":"R Madariaga","creatorNameLang":"en"}]},{"creatorNames":[{"creatorName":"E Fukuyama","creatorNameLang":"en"}]}]},"item_language":{"attribute_name":"言語","attribute_value_mlt":[{"subitem_language":"eng"}]},"item_title":"Effect of normal stress during rupture propagation along nonplanar faults","item_titles":{"attribute_name":"タイトル","attribute_value_mlt":[{"subitem_title":"Effect of normal stress during rupture propagation along nonplanar faults","subitem_title_language":"en"}]},"item_type_id":"40001","owner":"1","path":["1670839190650"],"pubdate":{"attribute_name":"PubDate","attribute_value":"2023-03-30"},"publish_date":"2023-03-30","publish_status":"0","recid":"4462","relation_version_is_last":true,"title":["Effect of normal stress during rupture propagation along nonplanar faults"],"weko_creator_id":"1","weko_shared_id":-1},"updated":"2023-03-31T01:54:16.232263+00:00"}