{"created":"2023-05-15T08:55:10.717942+00:00","id":212,"links":{},"metadata":{"_buckets":{"deposit":"c6bc0add-cd32-46d9-b07e-af51a8034dac"},"_deposit":{"created_by":10,"id":"212","owners":[10],"pid":{"revision_id":0,"type":"depid","value":"212"},"status":"published"},"_oai":{"id":"oai:tsurumi-u.repo.nii.ac.jp:00000212","sets":["8:123:14:39"]},"author_link":["189"],"item_10002_biblio_info_7":{"attribute_name":"書誌情報","attribute_value_mlt":[{"bibliographicIssueDates":{"bibliographicIssueDate":"2018-02","bibliographicIssueDateType":"Issued"},"bibliographicIssueNumber":"55","bibliographicPageEnd":"151","bibliographicPageStart":"145","bibliographic_titles":[{"bibliographic_title":"鶴見大学紀要. 第4部, 人文・社会・自然科学編","bibliographic_titleLang":"ja"},{"bibliographic_title":"The bulletin of Tsurumi University. Pt. 4, Studies in humanities, social and natural sciences","bibliographic_titleLang":"en"}]}]},"item_10002_description_5":{"attribute_name":"抄録","attribute_value_mlt":[{"subitem_description":"Newtonの運動方程式は、F=maともma=Fとも表記される。等式の左右には意味があるので、加速度aと力Fの因果関係からすればma=Fだというのは納得できる。教育現場でも利便性が高い。しかしma=Fが見られるのは日本のみで、海外ではもっぱらF=maである。ma=Fには欠点もあり、質量mについての因果関係を考えると、mが左辺に位置するのは不自然である。いっぽうF=maにも、W=mgとの対応関係など利点がある。運動方程式が力の定義式か加速度の定義式か、という議論は世界中で行われているのだが、国際的にはこれが方程式の表記法に反映されない理由は、今のところ分からない。","subitem_description_language":"ja","subitem_description_type":"Abstract"}]},"item_10002_identifier_registration":{"attribute_name":"ID登録","attribute_value_mlt":[{"subitem_identifier_reg_text":"10.24791/00000193","subitem_identifier_reg_type":"JaLC"}]},"item_10002_publisher_8":{"attribute_name":"出版者","attribute_value_mlt":[{"subitem_publisher":"鶴見大学","subitem_publisher_language":"ja"}]},"item_10002_source_id_11":{"attribute_name":"書誌レコードID","attribute_value_mlt":[{"subitem_source_identifier":"AN10179064","subitem_source_identifier_type":"NCID"}]},"item_10002_source_id_9":{"attribute_name":"ISSN","attribute_value_mlt":[{"subitem_source_identifier":"03898032","subitem_source_identifier_type":"PISSN"}]},"item_10002_version_type_20":{"attribute_name":"著者版フラグ","attribute_value_mlt":[{"subitem_version_resource":"http://purl.org/coar/version/c_970fb48d4fbd8a85","subitem_version_type":"VoR"}]},"item_creator":{"attribute_name":"著者","attribute_type":"creator","attribute_value_mlt":[{"creatorNames":[{"creatorName":"安藤, 準","creatorNameLang":"ja"},{"creatorName":"アンドウ, ヒトシ","creatorNameLang":"ja-Kana"},{"creatorName":"ANDO, Hitoshi","creatorNameLang":"en"}],"nameIdentifiers":[{"nameIdentifier":"189","nameIdentifierScheme":"WEKO"},{"nameIdentifier":"189","nameIdentifierScheme":"WEKO著者ID","nameIdentifierURI":" "}]}]},"item_files":{"attribute_name":"ファイル情報","attribute_type":"file","attribute_value_mlt":[{"accessrole":"open_date","date":[{"dateType":"Available","dateValue":"2019-01-18"}],"displaytype":"detail","filename":"55_4_07.pdf","filesize":[{"value":"5.2 MB"}],"format":"application/pdf","licensetype":"license_6","mimetype":"application/pdf","url":{"label":"55_4_07","url":"https://tsurumi-u.repo.nii.ac.jp/record/212/files/55_4_07.pdf"},"version_id":"cd1de5b3-80a9-4f70-ac3f-5fda557dcd0a"}]},"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":"Newton の運動方程式は F=ma か ma=F か 第一報　―日本では ma=F が優位である―","item_titles":{"attribute_name":"タイトル","attribute_value_mlt":[{"subitem_title":"Newton の運動方程式は F=ma か ma=F か 第一報　―日本では ma=F が優位である―","subitem_title_language":"ja"},{"subitem_title":"F=ma or ma=F, Which is Suitable Formula for the Newton's Equation of Motion? 1. -ma=F is common in Japan-","subitem_title_language":"en"}]},"item_type_id":"10002","owner":"10","path":["39"],"pubdate":{"attribute_name":"PubDate","attribute_value":"2019-01-18"},"publish_date":"2019-01-18","publish_status":"0","recid":"212","relation_version_is_last":true,"title":["Newton の運動方程式は F=ma か ma=F か 第一報　―日本では ma=F が優位である―"],"weko_creator_id":"10","weko_shared_id":-1},"updated":"2023-11-07T07:07:46.822416+00:00"}