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VERIF/2DANW: 2D Airfoil Near-Wake Verification Case (20c) - Intro Page

Note: the results on this page (and its links) are no longer "official" because the farfield grid extent of only 20c was considered too small for verification purposes. The "official" page is now at: New official page for VERIF/2DANW.

The purpose here is to provide a large sequence of nested grids of the same family, along with results from existing CFD codes that employ specific forms of particular turbulence models, in order to help programmers verify their implementations of these same models. On a given grid, there may be differences between the results from different codes, but presumably as the grid is refined the results should approach the same answer (if the flow conditions and boundary conditions are the same). With verification, the purpose is not to establish the "goodness" of a model compared to experiment, but rather to establish that a model has been implemented correctly, as intended according to the equations and boundary conditions. (It is through validation that a model's "goodness" is established.) The purpose here is primarily verification.

The 2-D airfoil near-wake case involves flow over an airfoil. Experiment exists for this case, but the main purpose here (for verification) is NOT comparison with experiment. Comparison with experiment for this case can be found under the validation section, at the 2DANW: 2D Airfoil Near-Wake page. This case was run fully turbulent at angle of attack of zero degrees, M = 0.088, and a Reynolds number of Re = 1.2 million based on airfoil chord length. The outer boundary of the grid in this case is only 20c from the airfoil, where farfield Riemann boundary conditions are imposed. Because of the relative nearness of the outer boundaries, use of a different farfield boundary condition other than Riemann-type may influence the comparisons with the reference results presented in the pages linked below.

Note that the current set of grids for this case were based on airfoil coordinates extracted from the reference: Nakayama, A., "Characteristics of the Flow around Conventional and Supercritical Airfoils," J. Fluid Mech. (1985), Vol. 160, pp. 155-179, https://doi.org/10.1017/S0022112085003433. The airfoil is a DSMA661(MODEL A). The airfoil shape does not have an analytic definition; the original airfoil point definition can be found in DSMA661 original point definition. The original airfoil has a blunt trailing edge, but this has been altered to be sharp for the purposes of this study. Also, as created, the current grids display some non-smoothness on the surface. Therefore, for the purpose of verification, you must use these same grids, or else create grids with exactly the same airfoil surface shape. The as-created airfoil surface points (from the finest grid) are given in DSMA661 as-created point definition.

Another important note: although M=0.088 is low enough that the flow is "essentially" incompressible, this is a compressible flow verification case. Therefore, if you run this case with an incompressible code, your results may be close - but not quite the same - as the grid is refined.

This case was used as a verification test case for High Lift Prediction Workshop 3 (HiLiftPW-3).

2D airfoil wake case layout & BCs


 

What to Expect:
RESULTS
LINK TO EQUATIONS
MRR Level
SA
SA eqns
4
SST
SST eqns
3

(Other turbulence model results may be added in the future.)
 
 

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Responsible NASA Official: Ethan Vogel
Page Curator: Clark Pederson
Last Updated: 03/11/2025