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Subject:Investigating the effects of numerical discretization and t b l d li th f fl l ti turbulence modeling on the accuracy of flow solution
around NACA0012 airfoil using OpenFOAM
Authors:Authors:Farshad Rezaei Ehsan Roohi Mahmood Pasandideh Frad
Ferdowsi University of Mashhad, Mashhad, Iran
Presented by:Farshad Rezaei
Contents:Contents:
IntroductionIntroduction
Grid IndependencyGrid Independency
Results and DiscussionResults and Discussion
ConclusionsConclusions
I t d tiIntroduction
Incompressible Flow around NACA0012Incompressible Flow around NACA0012
Using OpenFOAMUsing OpenFOAM
simpleFoam Solver: A Pressure-Based SolversimpleFoam Solver: A Pressure-Based Solver
SIMPLE Algorithm: The Semi-Implicit Method of Linked Equations
Turbulence Models:
Spallart-Allmaras: An one equation model
Turbulence Models:
K-ω SST: Two-equation eddy-viscosity model
Grid IndependencyGrid Independency
Grid Independency:Grid Independency:
Mesh Name Number of Thickness of Error%
Lift Coefficient for different Meshes AoA=10
Computational DomainCLmesh points around airfoil
first B.L cell (mm)
Computational DomainCL
Mesh-1 450 0.6 1.0834 1.204
Mesh-2 592 0.6 1.0897 0.631
Mesh-3 738 0.6 1.0916 0.458
Results and DiscussionResults and DiscussionDiscretization Schemes of the Momentum Equations
leastSquares Improve the CL 2 01%q p
Pressure Gradient: fourth Improve the
2.01%
CLfourth Improve the
I t l ti f l it f th ll t t ll’ f
CL
2.1%
Interpolation of velocity from the cell center to cell’s face: Linear,cubic-Correction,midpoint,linear-Upwind and CL C D
are exactly Limited-Linear-V, vanLeer-V, gamma-V, SFCDV the same
Results and DiscussionResults and DiscussionConvective term: for an Incompressible flow
)( UUdiv )( Udiv
QUICK
),( UUdiv ),( Udiv
QUICK Linear compared to linear-Upwind SFCD SFCD
The most accurate result was obtained by using linearS h f i d b 0 35%CScheme for improved by 0.35%),( UUdiv CL
Th t t ltUsing fourth order discretization scheme for presuure gradient term
The most accurate results:p g
Using linear scheme for diverjence term ),( UU
variation vs. angle of attack from the current numerical work to thin airfoil theoryCL
Results and Discussion
Investigating the effect of Reynolds number:
CL vs. angle of attack for different Reynolds number compared to Thin Airfoil TheoryL g y p y
By increasing the Reynolds number, increasers and become closer to Thin Airfoil Theory
CL
Wall‐Skin friction Coefficient using K‐ turbulence modelWall Skin friction Coefficient using K turbulence model
AOA=0 AOA=10
AOA=15
ConclusionConclusionUsing fourth order discretization scheme for presuure gradient
termterm.
U i li h f di j )(dUsing linear scheme for diverjence term .),( UUdiv
By increasing the Reynolds number increasers and become closer to Thin Airfoil Theory.
CL
K-SST model provides more accurate results for and compared to p pthe spalart-Allamras one.