{"created":"2021-03-01T06:23:35.576111+00:00","id":20485,"links":{},"metadata":{"_buckets":{"deposit":"5adb6a30-70dc-4af3-8146-9c9ecf83a7ea"},"_deposit":{"id":"20485","owners":[],"pid":{"revision_id":0,"type":"depid","value":"20485"},"status":"published"},"_oai":{"id":"oai:soar-ir.repo.nii.ac.jp:00020485","sets":["1221:1222"]},"author_link":["107510","107511","107512"],"item_1628147817048":{"attribute_name":"\u51fa\u7248\u30bf\u30a4\u30d7","attribute_value_mlt":[{"subitem_version_resource":"http://purl.org/coar/version/c_970fb48d4fbd8a85","subitem_version_type":"VoR"}]},"item_6_alternative_title_1":{"attribute_name":"\u305d\u306e\u4ed6\uff08\u5225\u8a00\u8a9e\u7b49\uff09\u306e\u30bf\u30a4\u30c8\u30eb","attribute_value_mlt":[{"subitem_alternative_title":"NUMERICAL SIMULATION OF FLUID FLOWS WITH A SOLID PARTICLE IN A T-SHAPED PIPE BY THE IMMERSED BOUNDARY-IMPROVED LATTICE KINETIC SCHEME"}]},"item_6_biblio_info_6":{"attribute_name":"\u66f8\u8a8c\u60c5\u5831","attribute_value_mlt":[{"bibliographicIssueDates":{"bibliographicIssueDate":"2016-12","bibliographicIssueDateType":"Issued"},"bibliographicPageEnd":"36","bibliographicPageStart":"31","bibliographicVolumeNumber":"16","bibliographic_titles":[{"bibliographic_title":"\u8a08\u7b97\u6570\u7406\u5de5\u5b66\u8ad6\u6587\u96c6"}]}]},"item_6_description_20":{"attribute_name":"\u6284\u9332","attribute_value_mlt":[{"subitem_description":"An immersed boundary\u2013improved lattice kinetic scheme is formulated for numerical simulations of fluid flows with a solid particle in a T-shaped pipe. The improved lattice kinetic scheme is an extended version of the lattice Boltzmann method and is more accurate and stable than the single relaxation time-lattice Boltzmann method. In this study, we combine the improved lattice kinetic scheme with the multi direct forcing method, which enforces the no-slip boundary condition accurately by determining the body force iteratively. In addition, the present method includes a collision technique in which a repulsive force occurs when the gap between a particle and a wall is lower than a given threshold. By using the present method, we simulate fluid flows with a circular cylinder in a two-dimensional T-shaped pipe and investigate the effects of the initial position of the cylinder, the pressure difference between two outlets, and the ratio of the diameter of the cylinder to the width of the pipe.","subitem_description_type":"Abstract"}]},"item_6_description_30":{"attribute_name":"\u8cc7\u6e90\u30bf\u30a4\u30d7\uff08\u30b3\u30f3\u30c6\u30f3\u30c4\u306e\u7a2e\u985e\uff09","attribute_value_mlt":[{"subitem_description":"Article","subitem_description_type":"Other"}]},"item_6_description_5":{"attribute_name":"\u5f15\u7528","attribute_value_mlt":[{"subitem_description":"\u8a08\u7b97\u6570\u7406\u5de5\u5b66\u8ad6\u6587\u96c6.16:31-36(2016)","subitem_description_type":"Other"}]},"item_6_link_3":{"attribute_name":"\u4fe1\u5dde\u5927\u5b66\u7814\u7a76\u8005\u7dcf\u89a7\u3078\u306e\u30ea\u30f3\u30af","attribute_value_mlt":[{"subitem_link_text":"\u5409\u91ce, \u6b63\u4eba","subitem_link_url":"http://soar-rd.shinshu-u.ac.jp/profile/ja.ONkpbpkh.html"},{"subitem_link_text":"\u9234\u6728, \u5eb7\u7950","subitem_link_url":"http://soar-rd.shinshu-u.ac.jp/profile/ja.uayebUkh.html"}]},"item_6_publisher_4":{"attribute_name":"\u51fa\u7248\u8005","attribute_value_mlt":[{"subitem_publisher":"\u65e5\u672c\u8a08\u7b97\u6570\u7406\u5de5\u5b66\u4f1a"}]},"item_6_rights_62":{"attribute_name":"\u6a29\u5229","attribute_value_mlt":[{"subitem_rights":"\u00a9 2016 \u65e5\u672c\u8a08\u7b97\u6570\u7406\u5de5\u5b66\u4f1a (CC BY-NC-ND 4.0) "}]},"item_6_source_id_35":{"attribute_name":"ISSN","attribute_value_mlt":[{"subitem_source_identifier":"1348-5245","subitem_source_identifier_type":"ISSN"}]},"item_creator":{"attribute_name":"\u8457\u8005","attribute_type":"creator","attribute_value_mlt":[{"creatorNames":[{"creatorName":"\u5409\u91ce, \u6b63\u4eba"}],"nameIdentifiers":[{}]},{"creatorNames":[{"creatorName":"\u767d, \u6db5\u592b"}],"nameIdentifiers":[{}]},{"creatorNames":[{"creatorName":"\u9234\u6728, \u5eb7\u7950"}],"nameIdentifiers":[{}]}]},"item_files":{"attribute_name":"\u30d5\u30a1\u30a4\u30eb\u60c5\u5831","attribute_type":"file","attribute_value_mlt":[{"accessrole":"open_date","date":[{"dateType":"Available","dateValue":"2019-02-22"}],"displaytype":"detail","filename":"26420105_01.pdf","filesize":[{"value":"469.5 kB"}],"format":"application/pdf","licensefree":"\u00a9 2016 \u65e5\u672c\u8a08\u7b97\u6570\u7406\u5de5\u5b66\u4f1a (CC BY-NC-ND 4.0)","licensetype":"license_note","mimetype":"application/pdf","url":{"label":"26420105_01.pdf","url":"https://soar-ir.repo.nii.ac.jp/record/20485/files/26420105_01.pdf"},"version_id":"6a17e301-7d28-4b15-bf25-9220576c3996"}]},"item_keyword":{"attribute_name":"\u30ad\u30fc\u30ef\u30fc\u30c9","attribute_value_mlt":[{"subitem_subject":"Immersed Boundary\u2013Improved Lattice Kinetic Scheme","subitem_subject_scheme":"Other"},{"subitem_subject":"Solid Particle","subitem_subject_scheme":"Other"},{"subitem_subject":"Repulsive Force","subitem_subject_scheme":"Other"},{"subitem_subject":"T-Shaped Pipe","subitem_subject_scheme":"Other"}]},"item_language":{"attribute_name":"\u8a00\u8a9e","attribute_value_mlt":[{"subitem_language":"jpn"}]},"item_resource_type":{"attribute_name":"\u8cc7\u6e90\u30bf\u30a4\u30d7","attribute_value_mlt":[{"resourcetype":"journal article","resourceuri":"http://purl.org/coar/resource_type/c_6501"}]},"item_title":"\u57cb\u3081\u8fbc\u307f\u5883\u754c : \u6539\u826fLattice Kinetic Scheme\u3092\u7528\u3044\u305fT\u5b57\u7ba1\u5185\u306b\u304a\u3051\u308b\u56fa\u4f53\u7c92\u5b50\u3092\u542b\u3080\u6d41\u308c\u306e\u6570\u5024\u8a08\u7b97","item_titles":{"attribute_name":"\u30bf\u30a4\u30c8\u30eb","attribute_value_mlt":[{"subitem_title":"\u57cb\u3081\u8fbc\u307f\u5883\u754c : \u6539\u826fLattice Kinetic Scheme\u3092\u7528\u3044\u305fT\u5b57\u7ba1\u5185\u306b\u304a\u3051\u308b\u56fa\u4f53\u7c92\u5b50\u3092\u542b\u3080\u6d41\u308c\u306e\u6570\u5024\u8a08\u7b97","subitem_title_language":"ja"}]},"item_type_id":"6","owner":"1","path":["1221/1222"],"pubdate":{"attribute_name":"PubDate","attribute_value":"2019-02-22"},"publish_date":"2019-02-22","publish_status":"0","recid":"20485","relation_version_is_last":true,"title":["\u57cb\u3081\u8fbc\u307f\u5883\u754c : \u6539\u826fLattice Kinetic Scheme\u3092\u7528\u3044\u305fT\u5b57\u7ba1\u5185\u306b\u304a\u3051\u308b\u56fa\u4f53\u7c92\u5b50\u3092\u542b\u3080\u6d41\u308c\u306e\u6570\u5024\u8a08\u7b97"],"weko_creator_id":"1","weko_shared_id":-1},"updated":"2021-10-12T00:45:58.846376+00:00"}