{"@context":{"@vocab":"https://cir.nii.ac.jp/schema/1.0/","rdfs":"http://www.w3.org/2000/01/rdf-schema#","dc":"http://purl.org/dc/elements/1.1/","dcterms":"http://purl.org/dc/terms/","foaf":"http://xmlns.com/foaf/0.1/","prism":"http://prismstandard.org/namespaces/basic/2.0/","cinii":"http://ci.nii.ac.jp/ns/1.0/","datacite":"https://schema.datacite.org/meta/kernel-4/","ndl":"http://ndl.go.jp/dcndl/terms/","jpcoar":"https://github.com/JPCOAR/schema/blob/master/2.0/"},"@id":"https://cir.nii.ac.jp/crid/1390282679445358080.json","@type":"Article","productIdentifier":[{"identifier":{"@type":"DOI","@value":"10.2322/jjsass.49.375"}},{"identifier":{"@type":"NDL_BIB_ID","@value":"5984705"}},{"identifier":{"@type":"URI","@value":"http://id.ndl.go.jp/bib/5984705"}},{"identifier":{"@type":"URI","@value":"https://ndlsearch.ndl.go.jp/books/R000000004-I5984705"}},{"identifier":{"@type":"URI","@value":"https://www.jstage.jst.go.jp/article/jjsass/49/574/49_574_375/_pdf"}},{"identifier":{"@type":"NAID","@value":"10007208255"}}],"dc:title":[{"@language":"en","@value":"Rotational and Vibrational Temperature of High-Speed, Nonequilibrium Nitrogen Flow along the Stagnation Streamline of Hemi-Sphere Cylinder."},{"@language":"ja","@value":"高速非平衡窒素流中における球頭物体澱み流線上の振動・回転温度"},{"@language":"ja-Kana","@value":"コウソク ヒヘイコウ チッソリュウ チュウ ニ オケル キュウトウブッタイ ヨドミ リュウ センジョウ ノ シンドウ カイテン オンド"}],"dc:language":"ja","description":[{"type":"abstract","notation":[{"@language":"en","@value":"An arc-heated wind tunnel has been used to produce nitrogen gas flow with high enthalpy to investigate physical phenomena along the stagnation streamline of a hemi-sphere cylinder with a diameter of 10 mm. The rotational and vibrational temperatures were measured by a spectroscopic method. The rotational temperature took a maximum value of 800 K at a location 2 mm upstream of the stagnation point, while the vibrational temperature showed a nearly constant value of 5, 500 K, which was much higher than the rotational temperature. This means that the present flow is in the state of thermal nonequilibrium. For comparison, the flow was numerically simulated by using the measured data as boundary conditions. As a result the calculated translational-rotational temperature was 80 K higher than the experimental data. Vibrational temperature had a tendency to decrease along the centerline of the wind tunnel, due to insufficient energy exchange between translational-rotational and vibrational energy."}],"abstractLicenseFlag":"disallow"}],"creator":[{"@id":"https://cir.nii.ac.jp/crid/1410001204615297280","@type":"Researcher","personIdentifier":[{"@type":"NRID","@value":"9000017193468"}],"foaf:name":[{"@language":"en","@value":"HAMAMOTO Naoki"},{"@language":"ja","@value":"濱本 直樹"}],"jpcoar:affiliationName":[{"@language":"ja","@value":"名古屋大学工学研究科"},{"@language":"ja","@value":"現 三菱自動車工業(株)"}]},{"@id":"https://cir.nii.ac.jp/crid/1410282679445358081","@type":"Researcher","foaf:name":[{"@language":"en","@value":"NAKAMURA Yoshiaki"},{"@language":"ja","@value":"中村 佳朗"}],"jpcoar:affiliationName":[{"@language":"ja","@value":"名古屋大学工学研究科"}]}],"publication":{"publicationIdentifier":[{"@type":"PISSN","@value":"13446460"},{"@type":"LISSN","@value":"13446460"},{"@type":"EISSN","@value":"24323691"},{"@type":"NDL_BIB_ID","@value":"000000105032"},{"@type":"ISSN","@value":"13446460"},{"@type":"NCID","@value":"AA11307372"}],"prism:publicationName":[{"@language":"ja","@value":"日本航空宇宙学会論文集"},{"@language":"en","@value":"JOURNAL OF THE JAPAN SOCIETY FOR AERONAUTICAL AND SPACE SCIENCES"},{"@language":"en","@value":"JOURNAL OF THE JAPAN SOCIETY FOR AERONAUTICAL AND SPACE SCIENCES"},{"@language":"ja","@value":"日本航空宇宙学会論文集"},{"@language":"en","@value":"Journal of the Japan Society for Aeronautical and Space Sciences"}],"dc:publisher":[{"@language":"en","@value":"THE JAPAN SOCIETY FOR AERONAUTICAL AND SPACE SCIENCES"},{"@language":"ja","@value":"一般社団法人 日本航空宇宙学会"}],"prism:publicationDate":"2001","prism:volume":"49","prism:number":"574","prism:startingPage":"375","prism:endingPage":"381"},"reviewed":"false","url":[{"@id":"http://id.ndl.go.jp/bib/5984705"},{"@id":"https://ndlsearch.ndl.go.jp/books/R000000004-I5984705"},{"@id":"https://www.jstage.jst.go.jp/article/jjsass/49/574/49_574_375/_pdf"}],"availableAt":"2001","foaf:topic":[{"@id":"https://cir.nii.ac.jp/all?q=High%20Enthalpy%20Flow","dc:title":"High Enthalpy Flow"},{"@id":"https://cir.nii.ac.jp/all?q=Spectroscopy","dc:title":"Spectroscopy"},{"@id":"https://cir.nii.ac.jp/all?q=Nonequilibrium%20Flow","dc:title":"Nonequilibrium Flow"},{"@id":"https://cir.nii.ac.jp/all?q=Arc-Heated%20Wind%20Tunnel","dc:title":"Arc-Heated Wind Tunnel"},{"@id":"https://cir.nii.ac.jp/all?q=Rotational%20Temperature","dc:title":"Rotational Temperature"},{"@id":"https://cir.nii.ac.jp/all?q=Vibrational%20Temperature","dc:title":"Vibrational Temperature"}],"relatedProduct":[{"@id":"https://cir.nii.ac.jp/crid/1360292619529201408","@type":"Article","relationType":["references","cites"],"jpcoar:relatedTitle":[{"@value":"Evaluation of Real-Gas Phenomena in High-Enthalpy Impulse Test Facilities: A Review"}]},{"@id":"https://cir.nii.ac.jp/crid/1360574095047716096","@type":"Article","relationType":["cites"],"jpcoar:relatedTitle":[{"@value":"Implicit Schemes and LU Decompositions"}]},{"@id":"https://cir.nii.ac.jp/crid/1361137044301456512","@type":"Article","relationType":["references"],"jpcoar:relatedTitle":[{"@value":"Franck-Condon factors to high vibrational quantum numbers I. N2 and N+2"}]},{"@id":"https://cir.nii.ac.jp/crid/1361981469524598144","@type":"Article","relationType":["references"],"jpcoar:relatedTitle":[{"@value":"Emission spectroscopy of SiH in a silane glow-discharge"}]},{"@id":"https://cir.nii.ac.jp/crid/1362262944364874496","@type":"Article","relationType":["references","cites"],"jpcoar:relatedTitle":[{"@value":"The interpretation of intensity distributions in the N2 second positive and N+2 first negative band systems"}]},{"@id":"https://cir.nii.ac.jp/crid/1362262945941941120","@type":"Article","relationType":["references","cites"],"jpcoar:relatedTitle":[{"@value":"A New Flux Splitting Scheme"}]},{"@id":"https://cir.nii.ac.jp/crid/1362544421424983680","@type":"Article","relationType":["references"],"jpcoar:relatedTitle":[{"@value":"Determination of gas temperature from unresolved bands in the spectrum from a nitrogen discharge"}]},{"@id":"https://cir.nii.ac.jp/crid/1363107370327891712","@type":"Article","relationType":["references"],"jpcoar:relatedTitle":[{"@value":"Constants of diatomic molecules"}]},{"@id":"https://cir.nii.ac.jp/crid/1363388843630950528","@type":"Article","relationType":["references"],"jpcoar:relatedTitle":[{"@value":"Systematics of Vibrational Relaxation"}]},{"@id":"https://cir.nii.ac.jp/crid/1363670321058236416","@type":"Article","relationType":["references","cites"],"jpcoar:relatedTitle":[{"@value":"Spectroscopic Emission Measurements Within the Blunt-Body Shock Layer in an Arcjet Flow"}]},{"@id":"https://cir.nii.ac.jp/crid/1364233268158845824","@type":"Article","relationType":["references","cites"],"jpcoar:relatedTitle":[{"@value":"Potential Curves for the Observed States of N_{2} Below 11 eV."}]},{"@id":"https://cir.nii.ac.jp/crid/1390001288129857152","@type":"Article","relationType":["isCitedBy"],"jpcoar:relatedTitle":[{"@language":"ja","@value":"航空宇宙工学におけるこれからのCFD"},{"@language":"ja-Kana","@value":"コウクウ ウチュウ コウガク ニ オケル コレカラ ノ CFD"}]},{"@id":"https://cir.nii.ac.jp/crid/1570009749640186496","@type":"Article","relationType":["cites"]},{"@id":"https://cir.nii.ac.jp/crid/1570291224616898816","@type":"Article","relationType":["cites"],"jpcoar:relatedTitle":[{"@language":"en","@value":"Constants of Diatomic Molecules"}]},{"@id":"https://cir.nii.ac.jp/crid/1570572699593606912","@type":"Article","relationType":["cites"]},{"@id":"https://cir.nii.ac.jp/crid/1570854176487815168","@type":"Article","relationType":["cites"],"jpcoar:relatedTitle":[{"@language":"en","@value":"Determination of Gas Temperature from Unresolved Bands in the Spectrum from a Nitrogen Discharge"}]},{"@id":"https://cir.nii.ac.jp/crid/1571698599500447872","@type":"Article","relationType":["cites"]},{"@id":"https://cir.nii.ac.jp/crid/1571698599500450560","@type":"Article","relationType":["cites"],"jpcoar:relatedTitle":[{"@language":"en","@value":"Frank-Condon Factors to High Vibrational Quantum Numbers I : N_2 and N^+_2"}]},{"@id":"https://cir.nii.ac.jp/crid/1571980074477159808","@type":"Article","relationType":["cites"],"jpcoar:relatedTitle":[{"@language":"en","@value":"Basic Governing Equations for the Flight Regimes of Aeroassisted Orbital Transfer Vehicles"}]},{"@id":"https://cir.nii.ac.jp/crid/1572543024430582784","@type":"Article","relationType":["cites"]},{"@id":"https://cir.nii.ac.jp/crid/1573387451272103296","@type":"Article","relationType":["cites"]},{"@id":"https://cir.nii.ac.jp/crid/1573387451534771456","@type":"Article","relationType":["cites"],"jpcoar:relatedTitle":[{"@value":"N_2 2+バンドを用いた高温プラズマの温度計測-問題点と対策-"}]},{"@id":"https://cir.nii.ac.jp/crid/1573668924337421952","@type":"Article","relationType":["cites"],"jpcoar:relatedTitle":[{"@language":"en","@value":"Uber die Struktur der Zwciten Positiven Stickstoffgruppe und die Pradissoziation des N_2-Molekults"}]},{"@id":"https://cir.nii.ac.jp/crid/1573668924337423360","@type":"Article","relationType":["cites"]},{"@id":"https://cir.nii.ac.jp/crid/1573668924337425280","@type":"Article","relationType":["cites"]},{"@id":"https://cir.nii.ac.jp/crid/1574231874290848256","@type":"Article","relationType":["cites"],"jpcoar:relatedTitle":[{"@language":"en","@value":"Systematics of Vibrational Relaxation"}]}],"dataSourceIdentifier":[{"@type":"JALC","@value":"oai:japanlinkcenter.org:0012368355"},{"@type":"NDL_SEARCH","@value":"oai:ndlsearch.ndl.go.jp:R000000004-I5984705"},{"@type":"CROSSREF","@value":"10.2322/jjsass.49.375"},{"@type":"CIA","@value":"10007208255"}]}