{"created":"2021-03-01T05:58:52.279302+00:00","id":6436,"links":{},"metadata":{"_buckets":{"deposit":"b1a757ab-12d4-4c32-a851-dced4a755de9"},"_deposit":{"id":"6436","owners":[],"pid":{"revision_id":0,"type":"depid","value":"6436"},"status":"published"},"_oai":{"id":"oai:kitami-it.repo.nii.ac.jp:00006436","sets":["7:15:30"]},"item_2_alternative_title_18":{"attribute_name":"その他のタイトル","attribute_value_mlt":[{"subitem_alternative_title":"Analysis of Steady- State Characteristics of Static Kramer System by Circle Diagram Method (Part 2)"}]},"item_2_biblio_info_6":{"attribute_name":"書誌情報","attribute_value_mlt":[{"bibliographicIssueDates":{"bibliographicIssueDate":"1977-11","bibliographicIssueDateType":"Issued"},"bibliographicIssueNumber":"1","bibliographicPageEnd":"65","bibliographicPageStart":"57","bibliographicVolumeNumber":"9","bibliographic_titles":[{"bibliographic_title":"北見工業大学研究報告"}]}]},"item_2_description_14":{"attribute_name":"フォーマット","attribute_value_mlt":[{"subitem_description":"application/pdf","subitem_description_type":"Other"}]},"item_2_description_4":{"attribute_name":"抄録","attribute_value_mlt":[{"subitem_description":"Already, we reported the circle diagram methods of analyzing the characteristics of a static Kramer system by using an L-type equivalent circuit and a T-type equivalent circuit. In order to calculate the characteristics, it is necessary to separate the primary leakage reactance from the secondary leakage reactance. But, in case of determining the constants of the equivalent circuits by the experimental results, it is theoretically impossible to separate the leakage reactances. Then, we analyzed the characteristics by a new T-type circle diagram method by applying the new T-type equivalent circuit suggested by Dr. Yamamura to the static Kramer system. As a result of the analysis, we pointed out that the values obtained from the results using this new T-type circle diagram method give fairly good agreement with the experimental results.","subitem_description_type":"Abstract"}]},"item_2_full_name_3":{"attribute_name":"著者別名","attribute_value_mlt":[{"nameIdentifiers":[{"nameIdentifier":"32583","nameIdentifierScheme":"WEKO"}],"names":[{"name":"Toshiaki, MURATA"}]},{"nameIdentifiers":[{"nameIdentifier":"32584","nameIdentifierScheme":"WEKO"}],"names":[{"name":"Ikuo, TAKEDA"}]}]},"item_2_publisher_32":{"attribute_name":"出版者","attribute_value_mlt":[{"subitem_publisher":"北見工業大学"}]},"item_2_select_15":{"attribute_name":"著者版フラグ","attribute_value_mlt":[{"subitem_select_item":"publisher"}]},"item_creator":{"attribute_name":"著者","attribute_type":"creator","attribute_value_mlt":[{"creatorNames":[{"creatorName":"村田, 年昭"}],"nameIdentifiers":[{"nameIdentifier":"32581","nameIdentifierScheme":"WEKO"}]},{"creatorNames":[{"creatorName":"武田, 郁夫"}],"nameIdentifiers":[{"nameIdentifier":"32582","nameIdentifierScheme":"WEKO"}]}]},"item_files":{"attribute_name":"ファイル情報","attribute_type":"file","attribute_value_mlt":[{"accessrole":"open_date","date":[{"dateType":"Available","dateValue":"2016-11-22"}],"displaytype":"detail","filename":"9-1-7.pdf","filesize":[{"value":"3.3 MB"}],"format":"application/pdf","licensetype":"license_note","mimetype":"application/pdf","url":{"label":"9-1-7.pdf","url":"https://kitami-it.repo.nii.ac.jp/record/6436/files/9-1-7.pdf"},"version_id":"2d33e528-a368-4b38-80b3-dfca4c2d519f"}]},"item_language":{"attribute_name":"言語","attribute_value_mlt":[{"subitem_language":"jpn"}]},"item_resource_type":{"attribute_name":"資源タイプ","attribute_value_mlt":[{"resourcetype":"departmental bulletin paper","resourceuri":"http://purl.org/coar/resource_type/c_6501"}]},"item_title":"静止クレーマ方式の円線図による定常特性の解析 （第２報）*","item_titles":{"attribute_name":"タイトル","attribute_value_mlt":[{"subitem_title":"静止クレーマ方式の円線図による定常特性の解析 （第２報）*"}]},"item_type_id":"2","owner":"1","path":["30"],"pubdate":{"attribute_name":"公開日","attribute_value":"2007-04-09"},"publish_date":"2007-04-09","publish_status":"0","recid":"6436","relation_version_is_last":true,"title":["静止クレーマ方式の円線図による定常特性の解析 （第２報）*"],"weko_creator_id":"1","weko_shared_id":3},"updated":"2022-12-13T02:19:48.621406+00:00"}