Symmetry-preserving discretization of the incompressible form of the Navier-Stokes equations under turbulent conditions. LES simulation of a turbulent channel flow

The incompressible form of the Navier-Stokes equations (conservation of mass, momentum and energy) is solved by applying a second-order symmetry-preserving spatial discretization which allows to preserve the symmetry of the operators. The physics behind turbulent flows and how those can be modelled...

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Detalles Bibliográficos
Autor: Luque Barcons, Jordi
Tipo de recurso: tesis de maestría
Fecha de publicación:2021
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:2117/361656
Acceso en línea:https://hdl.handle.net/2117/361656
Access Level:acceso abierto
Palabra clave:Fluid dynamics -- Computer simulation
Navier-Stokes equations
Turbulence
CFD
Computational Fluid Dynamics
Dinàmica de Fluids Computacional
LES
Turbulència
Dinàmica de fluids -- Simulació per ordinador
Equacions de Navier-Stokes
Àrees temàtiques de la UPC::Enginyeria mecànica::Mecànica de fluids
Descripción
Sumario:The incompressible form of the Navier-Stokes equations (conservation of mass, momentum and energy) is solved by applying a second-order symmetry-preserving spatial discretization which allows to preserve the symmetry of the operators. The physics behind turbulent flows and how those can be modelled is studied, considering both the RANS equations and the LES model. The Taylor-Green vortex problem is solved with no model and compared with the results of van Rees et al. [4], obtaining very good agreement regarding the time evolution of the volume-averaged kinetic energy, but higher discrepancies in the time evolution of the kinetic energy dissipation rate. Additionally, DNS results for a turbulent channel flow at Reτ “ 180 are obtained with coarse meshes. The same problem is also solved by applying the Smagorinsky, S3PR and Vreman’s LES models. DNS results obtained with a 323 mesh show relatively good agreement with the reference results of Moser et al. [5], while LES simulations employing the S3PR and Vreman’s model allow to improve the results in the buffer-layer region.