Dynamics and control of separated flow over small-scale surface deformations with slip
Surface slip was employed to control flow separation induced by small-scale Gaussian-shaped surface deformations on a two-dimensional flat plate. Single-surface deformations, including bumps and gaps, were modeled, which generated separated flow along the rear side of the bump and within the gap con...
| Autores: | , , , |
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| Tipo de recurso: | artículo |
| Fecha de publicación: | 2024 |
| País: | España |
| Institución: | Universitat Politècnica de Catalunya (UPC) |
| Repositorio: | UPCommons. Portal del coneixement obert de la UPC |
| Idioma: | inglés |
| OAI Identifier: | oai:upcommons.upc.edu:2117/405895 |
| Acceso en línea: | https://hdl.handle.net/2117/405895 https://dx.doi.org/10.1103/PhysRevFluids.9.033902 |
| Access Level: | acceso abierto |
| Palabra clave: | Aerodynamics Turbomachines--Aerodynamics Navier-Stokes equations Boundary layer receptivity Stability & separation Fluid dynamics Simulació per ordinador Àrees temàtiques de la UPC::Informàtica::Aplicacions de la informàtica::Aplicacions informàtiques a la física i l‘enginyeria |
| Sumario: | Surface slip was employed to control flow separation induced by small-scale Gaussian-shaped surface deformations on a two-dimensional flat plate. Single-surface deformations, including bumps and gaps, were modeled, which generated separated flow along the rear side of the bump and within the gap concavity for a Reynolds number Re = 100 000 when the plate surface was subject to the no-slip condition. Surface slip was modeled using a Navier-slip condition and quantified by a slip length λ . Bump deformations had a greater impact on the flow dynamics than gap concavities, generating more intense regions of reversed flow and requiring larger slip lengths to inhibit flow separation. In addition, double-bump configurations were modeled, with the location of the two bumps playing a critical role in the evolution of the flow. When the bumps were close together, the first bump controlled the size of the separation bubble that developed downstream of the second bump. Whereas when bumps ware far apart, a moderate slip length λ excited nonlinear oscillatory flow. However, increasing the slip length suppressed this phenomenon and ultimately eliminated all pockets of separated flow. |
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