{"created":"2023-06-20T15:08:09.212602+00:00","id":430,"links":{},"metadata":{"_buckets":{"deposit":"20465165-7947-40e1-8198-f9dfc451f0ee"},"_deposit":{"created_by":3,"id":"430","owners":[3],"pid":{"revision_id":0,"type":"depid","value":"430"},"status":"published"},"_oai":{"id":"oai:nifs-repository.repo.nii.ac.jp:00000430","sets":["6:7"]},"author_link":["123952","123954","123955","123951","123950","123953","123956"],"item_2_biblio_info_7":{"attribute_name":"書誌情報","attribute_value_mlt":[{"bibliographicIssueDates":{"bibliographicIssueDate":"2008-01-01","bibliographicIssueDateType":"Issued"},"bibliographicPageStart":"S1059-1 - S1059-7","bibliographicVolumeNumber":"Vol.3","bibliographic_titles":[{},{"bibliographic_title":"Plasma and Fusion Research","bibliographic_titleLang":"en"}]}]},"item_2_description_5":{"attribute_name":"抄録","attribute_value_mlt":[{"subitem_description":"Previously reported benchmarking examples of the analytical formulae of neoclassical viscosities were presented implicitly assuming applications in a future integrated simulation system of the Large Helical Device (LHD). Therefore, the assumed toroidal period numbers were mainly N = 10. However, in this type of calculation, an implicit (or sometimes explicit) assumption of ι/N 1 is sometimes included. This assumption is included not only in simplified bounce-averaged drift kinetic equations for ripple diffusions, but also in the equation before the averaging for non-bounce-averaged effects determining neoclassical parallel viscosity and banana-plateau diffusions. For clarifying the applicability of the analytical methods for configurations with extremely low toroidal period numbers (required for low aspect ratios), we show recent benchmarking examples in the National Compact Stellarator Experiment (NCSX) with N = 3 and the Quasi-Poloidal Stellarator (QPS) with N = 2.","subitem_description_type":"Abstract"}]},"item_2_publisher_8":{"attribute_name":"出版者","attribute_value_mlt":[{"subitem_publisher":"プラズマ・核融合学会"}]},"item_2_relation_14":{"attribute_name":"DOI","attribute_value_mlt":[{"subitem_relation_type_id":{"subitem_relation_type_id_text":"10.1585/pfr.3.S1059","subitem_relation_type_select":"DOI"}}]},"item_2_rights_15":{"attribute_name":"権利","attribute_value_mlt":[{"subitem_rights":"? 2008 The Japan Society of Plasma Science and Nuclear Fusion Research"}]},"item_creator":{"attribute_name":"著者","attribute_type":"creator","attribute_value_mlt":[{"creatorNames":[{"creatorName":"NISHIMURA,  Shin","creatorNameLang":"en"}],"nameIdentifiers":[{}]},{"creatorNames":[{"creatorName":"MIKKELSEN,  David R.","creatorNameLang":"en"}],"nameIdentifiers":[{}]},{"creatorNames":[{"creatorName":"SPONG,  Donald A.","creatorNameLang":"en"}],"nameIdentifiers":[{}]},{"creatorNames":[{"creatorName":"HIRSHMAN,  Steven P.","creatorNameLang":"en"}],"nameIdentifiers":[{}]},{"creatorNames":[{"creatorName":"KU,  Long-Poe","creatorNameLang":"en"}],"nameIdentifiers":[{}]},{"creatorNames":[{"creatorName":"MYNICK,  Henry E.","creatorNameLang":"en"}],"nameIdentifiers":[{}]},{"creatorNames":[{"creatorName":"ZARNSTORF,  Michael C.","creatorNameLang":"en"}],"nameIdentifiers":[{}]}]},"item_files":{"attribute_name":"ファイル情報","attribute_type":"file","attribute_value_mlt":[{"accessrole":"open_date","date":[{"dateType":"Available","dateValue":"2016-03-23"}],"displaytype":"detail","filename":"pfr2008_03-S1059.pdf","filesize":[{"value":"992.2 kB"}],"format":"application/pdf","licensetype":"license_note","mimetype":"application/pdf","url":{"label":"pfr2008_03-S1059.pdf","url":"https://nifs-repository.repo.nii.ac.jp/record/430/files/pfr2008_03-S1059.pdf"},"version_id":"333602b5-0a78-41c5-b03a-81894dd56b39"}]},"item_keyword":{"attribute_name":"キーワード","attribute_value_mlt":[{"subitem_subject":"neoclassical transport","subitem_subject_language":"en","subitem_subject_scheme":"Other"},{"subitem_subject":"neoclassical viscosity","subitem_subject_language":"en","subitem_subject_scheme":"Other"},{"subitem_subject":"moment equation approach","subitem_subject_language":"en","subitem_subject_scheme":"Other"},{"subitem_subject":"drift kinetic equation","subitem_subject_language":"en","subitem_subject_scheme":"Other"},{"subitem_subject":"nonsymmetric toroidal plasma","subitem_subject_language":"en","subitem_subject_scheme":"Other"},{"subitem_subject":"low aspect ratio stellarator","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":"journal article","resourceuri":"http://purl.org/coar/resource_type/c_6501"}]},"item_title":"Neoclassical Viscosities in NCSX and QPS with Few Toroidal Periods and Low Aspect Ratios","item_titles":{"attribute_name":"タイトル","attribute_value_mlt":[{"subitem_title":"Neoclassical Viscosities in NCSX and QPS with Few Toroidal Periods and Low Aspect Ratios","subitem_title_language":"en"}]},"item_type_id":"2","owner":"3","path":["7"],"pubdate":{"attribute_name":"公開日","attribute_value":"2011-04-05"},"publish_date":"2011-04-05","publish_status":"0","recid":"430","relation_version_is_last":true,"title":["Neoclassical Viscosities in NCSX and QPS with Few Toroidal Periods and Low Aspect Ratios"],"weko_creator_id":"3","weko_shared_id":-1},"updated":"2023-06-20T16:42:48.248015+00:00"}