{"created":"2023-06-20T15:16:34.020155+00:00","id":10301,"links":{},"metadata":{"_buckets":{"deposit":"1de9e4c3-8ec3-4273-b241-688724555aae"},"_deposit":{"created_by":3,"id":"10301","owners":[3],"pid":{"revision_id":0,"type":"depid","value":"10301"},"status":"published"},"_oai":{"id":"oai:nifs-repository.repo.nii.ac.jp:00010301","sets":["8:32"]},"author_link":["64721","64722","64723"],"item_5_biblio_info_7":{"attribute_name":"書誌情報","attribute_value_mlt":[{"bibliographicIssueDates":{"bibliographicIssueDate":"2001-02-01","bibliographicIssueDateType":"Issued"},"bibliographic_titles":[{},{"bibliographic_title":"Research Report NIFS-Series","bibliographic_titleLang":"en"}]}]},"item_5_description_5":{"attribute_name":"抄録","attribute_value_mlt":[{"subitem_description":"\"Two semi-Lagrangian schemes that guarantee exactly mass conservation are proposed.  Although they are in a non-conservative form, the mass of each cell is employed as an additional variable that is advaced in a conservative form.  One of them (CIP-CSL4) is the direct extension of the CIP method into the 4-th order polynomial to incorporate mass conservation.  In another scheme (CIP-CSL2), the CIP principle is applied to integrated mass and the interpolation of the value becomes quadratic.  The latter one can be readily extended to multi-dimensions.  These schemes are applied to the non-linear advection problem with large CFL number.\"","subitem_description_type":"Abstract"}]},"item_5_source_id_10":{"attribute_name":"ISSN","attribute_value_mlt":[{"subitem_source_identifier":"0915-633X","subitem_source_identifier_type":"ISSN"}]},"item_5_text_8":{"attribute_name":"報告書番号","attribute_value_mlt":[{"subitem_text_value":"NIFS-685"}]},"item_access_right":{"attribute_name":"アクセス権","attribute_value_mlt":[{"subitem_access_right":"metadata only access","subitem_access_right_uri":"http://purl.org/coar/access_right/c_14cb"}]},"item_creator":{"attribute_name":"著者","attribute_type":"creator","attribute_value_mlt":[{"creatorNames":[{"creatorName":"\"Tanaka,  R.","creatorNameLang":"en"}],"nameIdentifiers":[{}]},{"creatorNames":[{"creatorName":"Nakamura,  T.","creatorNameLang":"en"}],"nameIdentifiers":[{}]},{"creatorNames":[{"creatorName":"Yabe,  T.\"","creatorNameLang":"en"}],"nameIdentifiers":[{}]}]},"item_keyword":{"attribute_name":"キーワード","attribute_value_mlt":[{"subitem_subject":"Semi-Lagrangian Schemes","subitem_subject_language":"en","subitem_subject_scheme":"Other"},{"subitem_subject":"Conservation","subitem_subject_language":"en","subitem_subject_scheme":"Other"},{"subitem_subject":"CIP","subitem_subject_language":"en","subitem_subject_scheme":"Other"},{"subitem_subject":"CFL","subitem_subject_language":"en","subitem_subject_scheme":"Other"},{"subitem_subject":"Berger's Equation","subitem_subject_language":"en","subitem_subject_scheme":"Other"}]},"item_language":{"attribute_name":"言語","attribute_value_mlt":[{"subitem_language":"eng"}]},"item_resource_type":{"attribute_name":"資源タイプ","attribute_value_mlt":[{"resourcetype":"research report","resourceuri":"http://purl.org/coar/resource_type/c_18ws"}]},"item_title":"Exactly Conservative Semi-Lagrangian Scheme (CIP-CSL)  in One-Dimension","item_titles":{"attribute_name":"タイトル","attribute_value_mlt":[{"subitem_title":"Exactly Conservative Semi-Lagrangian Scheme (CIP-CSL)  in One-Dimension","subitem_title_language":"en"}]},"item_type_id":"5","owner":"3","path":["32"],"pubdate":{"attribute_name":"公開日","attribute_value":"2010-02-05"},"publish_date":"2010-02-05","publish_status":"0","recid":"10301","relation_version_is_last":true,"title":["Exactly Conservative Semi-Lagrangian Scheme (CIP-CSL)  in One-Dimension"],"weko_creator_id":"3","weko_shared_id":-1},"updated":"2023-06-20T20:51:28.657050+00:00"}