| dc.contributor.author | Yüca, E. | |
| dc.contributor.author | Kavsaoğlu, Mehmet Şerif | |
| dc.date.accessioned | 2019-10-20T19:32:34Z | |
| dc.date.available | 2019-10-20T19:32:34Z | |
| dc.date.issued | 2018 | |
| dc.identifier.isbn | 9781538672297 | |
| dc.identifier.uri | https://dx.doi.org/10.1109/ICMAE.2018.8467677 | |
| dc.identifier.uri | https://hdl.handle.net/11421/18559 | |
| dc.description | 9th International Conference on Mechanical and Aerospace Engineering, ICMAE 2018 -- 10 July 2018 through 13 July 2018 -- -- 139971 | en_US |
| dc.description.abstract | The flow field around a 6:1 prolate spheroid is numerically solved. The freestream velocity is 45 m/s. The angle between the principal axis of the prolate spheroid and the free flow direction is 30 degrees. Reynolds number based on length is 6.7 million. The k-omega and k-epsilon turbulence models are applied for two different solution meshes. The present numerical results are compared with the available experimental data | en_US |
| dc.language.iso | eng | en_US |
| dc.publisher | Institute of Electrical and Electronics Engineers Inc. | en_US |
| dc.relation.isversionof | 10.1109/ICMAE.2018.8467677 | en_US |
| dc.rights | info:eu-repo/semantics/closedAccess | en_US |
| dc.subject | K-Epsilon | en_US |
| dc.subject | K-Omega | en_US |
| dc.subject | Navier Stokes | en_US |
| dc.subject | Prolate Spheroid | en_US |
| dc.title | Numerical Solution of the Flow Field Around a Prolate Spheroid | en_US |
| dc.type | conferenceObject | en_US |
| dc.relation.journal | Proceedings of 2018 9th International Conference on Mechanical and Aerospace Engineering, ICMAE 2018 | en_US |
| dc.contributor.department | Anadolu Üniversitesi, Havacılık ve Uzay Bilimleri Fakültesi | en_US |
| dc.identifier.startpage | 451 | en_US |
| dc.identifier.endpage | 456 | en_US |
| dc.relation.publicationcategory | Konferans Öğesi - Uluslararası - Kurum Öğretim Elemanı | en_US] |
| dc.contributor.institutionauthor | Kavsaoğlu, Mehmet Şerif | |
