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An interactive boundary layer modeling methodology for aerodynamic flows[Presentation]

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dc.contributor.author Smith, L
dc.contributor.author Meyer, JP
dc.contributor.author Oxtoby, Oliver F
dc.contributor.author Malan, AG
dc.date.accessioned 2012-04-19T14:29:28Z
dc.date.available 2012-04-19T14:29:28Z
dc.date.issued 2011-11
dc.identifier.citation Smith, L, Meyer, JP, Oxtoby, OF and Malan, AG. An interactive boundary layer modeling methodology for aerodynamic flows. ASME 2011 International Mechanical Engineering Congress & Exposition (IMECE), Denver, Colorado, USA, 11-17 November 2011 en_US
dc.identifier.uri ftp://202.38.89.18/incoming/ASME/data/pdfs/trk-17/IMECE2011-62075.pdf
dc.identifier.uri http://asmedl.org/vsearch/servlet/VerityServlet?KEY=ASMEDL
dc.identifier.uri http://hdl.handle.net/10204/5802
dc.description Copyright: 2011 ASME. This is an ABSTRACT ONLY. en_US
dc.description.abstract The authors propose to develop a new method to couple Drela’s twointegral equations with a generic outer flow solver in an iterative fashion. They introduce an auxiliary equation which is solved along with the displacement thickness to overcome the Goldstein singularity without the need to solve the entire flow domain simultaneously. In this work the incompressible Navier- Stokes equations will be used for the outer flow. In the majority of previous studies the boundary layer thickness is simulated using a wall transpiration boundary condition at the interface between viscous and inviscid flows. This boundary condition is inherently non-physical since it adds extra mass into the system to simulate the effects of the boundary layer. Here, the authors circumvent this drawback by the use of a mesh movement algorithm to shift the surface of the body outward without regridding the entire mesh. This replaces the transpiration boundary condition. The results obtained show that accurate modeling is possible for laminar incompressible flow and that the solutions obtained compare well to similarity solutions in the cases of flat and inclined plates and to the results of a NACA 0012 airfoil produced by the validated XFOIL code. en_US
dc.language.iso en en_US
dc.publisher ASME en_US
dc.relation.ispartofseries Workflow;8586
dc.subject Boundary layer modelling en_US
dc.subject Coupling en_US
dc.subject Interactive method en_US
dc.subject Airfoil drag prediction en_US
dc.subject Aerodynamic flows en_US
dc.title An interactive boundary layer modeling methodology for aerodynamic flows[Presentation] en_US
dc.type Conference Presentation en_US
dc.identifier.apacitation Smith, L., Meyer, J., Oxtoby, O. F., & Malan, A. (2011). An interactive boundary layer modeling methodology for aerodynamic flows[Presentation]. ASME. http://hdl.handle.net/10204/5802 en_ZA
dc.identifier.chicagocitation Smith, L, JP Meyer, Oliver F Oxtoby, and AG Malan. "An interactive boundary layer modeling methodology for aerodynamic flows[Presentation]." (2011): http://hdl.handle.net/10204/5802 en_ZA
dc.identifier.vancouvercitation Smith L, Meyer J, Oxtoby OF, Malan A, An interactive boundary layer modeling methodology for aerodynamic flows[Presentation]; ASME; 2011. http://hdl.handle.net/10204/5802 . en_ZA
dc.identifier.ris TY - Conference Presentation AU - Smith, L AU - Meyer, JP AU - Oxtoby, Oliver F AU - Malan, AG AB - The authors propose to develop a new method to couple Drela’s twointegral equations with a generic outer flow solver in an iterative fashion. They introduce an auxiliary equation which is solved along with the displacement thickness to overcome the Goldstein singularity without the need to solve the entire flow domain simultaneously. In this work the incompressible Navier- Stokes equations will be used for the outer flow. In the majority of previous studies the boundary layer thickness is simulated using a wall transpiration boundary condition at the interface between viscous and inviscid flows. This boundary condition is inherently non-physical since it adds extra mass into the system to simulate the effects of the boundary layer. Here, the authors circumvent this drawback by the use of a mesh movement algorithm to shift the surface of the body outward without regridding the entire mesh. This replaces the transpiration boundary condition. The results obtained show that accurate modeling is possible for laminar incompressible flow and that the solutions obtained compare well to similarity solutions in the cases of flat and inclined plates and to the results of a NACA 0012 airfoil produced by the validated XFOIL code. DA - 2011-11 DB - ResearchSpace DP - CSIR KW - Boundary layer modelling KW - Coupling KW - Interactive method KW - Airfoil drag prediction KW - Aerodynamic flows LK - https://researchspace.csir.co.za PY - 2011 T1 - An interactive boundary layer modeling methodology for aerodynamic flows[Presentation] TI - An interactive boundary layer modeling methodology for aerodynamic flows[Presentation] UR - http://hdl.handle.net/10204/5802 ER - en_ZA


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