نمایش مختصر رکورد

dc.contributor.authorHeidarinejad, Ghassemen_US
dc.contributor.authorDelfani, S.en_US
dc.date.accessioned1399-07-09T08:07:05Zfa_IR
dc.date.accessioned2020-09-30T08:07:05Z
dc.date.available1399-07-09T08:07:05Zfa_IR
dc.date.available2020-09-30T08:07:05Z
dc.date.issued2000-08-01en_US
dc.date.issued1379-05-11fa_IR
dc.identifier.citationHeidarinejad, Ghassem, Delfani, S.. (2000). Direct Numerical Simulation of the Wake Flow Behind a Cylinder Using Random Vortex Method in Medium to High Reynolds Numbers. International Journal of Engineering, 13(3), 33-50.en_US
dc.identifier.issn1025-2495
dc.identifier.issn1735-9244
dc.identifier.urihttp://www.ije.ir/article_71264.html
dc.identifier.urihttps://iranjournals.nlai.ir/handle/123456789/335263
dc.description.abstractDirect numerical simulation of turbulent flow behind a cylinder, wake flow, using the random vortex method for an incompressible fluid in two dimensions is presented. In the random vortex method, the primary variable is vorticity of the flow field. After generation on the cylinder wall, it is followed in two fractional time step in a Lagrangian system of coordinates, namely convection and diffusion. No closure model is used and the instantaneous results are calculated without any a priori modeling. Regarding the Lagrangian nature of the method, there is a very good compatibility between the numerical method and physics of the flow. The numerical results are presented for a wide range of Reynolds number, 40-9500. In the initial stages, there is only an unstable symmetrical flow behind the cylinder and the vortex sheding is not started yet. But, in the high Reynolds number flows, two distinctive flow patterns, namely α and β are detected. The mechanism of generation of the primary and the secondary eddies can be related to the production, convection and diffusion of the vorticity field and the time dependent structure of the flow field in the wake zone behind the cylinder. The length of the computational domain, downstream of the cylinder, is selected 25 times of the cylinder's diameter. Regarding such a lengthy computational domain it is possible to detect the mechanism of generation, pairing and growth of the large scale structure, eddies. Although the instantaneous numerical results are calculated, no coresponding comparable results are available. Therefore, the validity of the results in this stage is only qualitative. For the quantitative comparison of the results, after the establishment of the stationary state, time averaged based indicators such as separation angle, drag coefficient, lift coefficient, Strouhal number and ... are calculated. The numerical results accurately fall within the range of the experimental measurements.en_US
dc.format.extent1276
dc.format.mimetypeapplication/pdf
dc.languageEnglish
dc.language.isoen_US
dc.publisherMaterials and Energy Research Centeren_US
dc.relation.ispartofInternational Journal of Engineeringen_US
dc.subjectCylinderen_US
dc.subjectWakeen_US
dc.subjectTurbulent Flowen_US
dc.subjectVortexen_US
dc.subjectRandom Walken_US
dc.subjectLagrangianen_US
dc.subjectDragen_US
dc.subjectLiften_US
dc.subjectSeparation Angleen_US
dc.titleDirect Numerical Simulation of the Wake Flow Behind a Cylinder Using Random Vortex Method in Medium to High Reynolds Numbersen_US
dc.typeTexten_US
dc.contributor.departmentMechanical Engineering, Tarbiat Modares Universityen_US
dc.contributor.department, Tarbiat Modarres Universityen_US
dc.citation.volume13
dc.citation.issue3
dc.citation.spage33
dc.citation.epage50


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