Reduced-order Modeling of Laminar Boundary Layers
ORAL
Abstract
In external aerodynamic applications such as flow over an airfoil, the number of computational volumes
in the laminar and transitional region can be greater than that of the turbulent region by up to two
orders of magnitude in a wall-modeled large-eddy simulation (WMLES) (Slotnick, et al., 2014). The high
computational cost of this region is a barrier to the application of WMLES to transitional flows of
engineering interest, such as the flow near the leading edge of wings. Prior work (Gonzalez, et al., 2020)
implemented a reduced order model for laminar boundary layers based on the Falkner-Skan similarity
solution. This model was then tested in stagnation flow and a spatially varying pressure gradient
boundary layer and the results were in good agreement with the Navier Stokes solutions. In this
investigation, we present a further assessment of the model when applied to a NACA0012 airfoil. We
evaluate the accuracy of engineering quantities of interest, such as wall-stress, lift, and drag. In addition,
the model is integrated with the parabolized stability equations in order to identify the onset of
transition.
in the laminar and transitional region can be greater than that of the turbulent region by up to two
orders of magnitude in a wall-modeled large-eddy simulation (WMLES) (Slotnick, et al., 2014). The high
computational cost of this region is a barrier to the application of WMLES to transitional flows of
engineering interest, such as the flow near the leading edge of wings. Prior work (Gonzalez, et al., 2020)
implemented a reduced order model for laminar boundary layers based on the Falkner-Skan similarity
solution. This model was then tested in stagnation flow and a spatially varying pressure gradient
boundary layer and the results were in good agreement with the Navier Stokes solutions. In this
investigation, we present a further assessment of the model when applied to a NACA0012 airfoil. We
evaluate the accuracy of engineering quantities of interest, such as wall-stress, lift, and drag. In addition,
the model is integrated with the parabolized stability equations in order to identify the onset of
transition.
*Supported by NASA
–
Presenters
-
Carlos A Gonzalez
- Center for Turbulence Research, Stanford University