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2. Outline. IntroductionMeasurements in LTPTComparison with RFOIL calculations(Maximum) liftDrag Roughness effectsConclusions. 3. Introduction. Large machines have blades performing at Reynolds numbers up to 9 to 10 millionMany dedicated wt airfoils have not been tested at these Re-numbersTesting at these Re-numbers is relatively expensiveIf blade designers do not want to spend this amount of money they have to rely on the predictive value of codes like XFOIL and/or CFD.
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1. 1 An overview of NACA 6-digit airfoil series characteristics with reference to airfoils for large wind turbine Nando Timmer
DUWIND
Delft University Wind Energy Institute
The Netherlands
2. 2 Outline Introduction
Measurements in LTPT
Comparison with RFOIL calculations
(Maximum) lift
Drag
Roughness effects
Conclusions
3. 3 Introduction Large machines have blades performing at Reynolds numbers up to 9 to 10 million
Many dedicated wt airfoils have not been tested at these Re-numbers
Testing at these Re-numbers is relatively expensive
If blade designers do not want to spend this amount of money they have to rely on the predictive value of codes like XFOIL and/or CFD
4. 4 Introduction (cntd) NACA airfoils were tested in the Langley LTPT up to Re=9x106 and can be used to verify the predictions.
Main question in this presentation is:
How good are these data anyway and how well can we predict them with RFOIL.
(as a typical example we investigate the 18% thick airfoil from the NACA 63 and 64 series)
5. 5 LTPT measurements Test section 3x7.5 feet (0.914 m x 2.29 m)
Model chord 2 feet (0.61 m)
Maximum velocity at atmospheric pressure is 130 m/s
Maximum Mach number during the tests was 0.17
Models were made of laminated mahogany
Lift from the pressure reaction on the walls (over a length of 13 feet – 3.96 m), drag from a wake rake.
Basic wind tunnel wall corrections were applied
6. 6 RFOIL Basically XFOIL
Improvement of the numerical stability by using the Schlichting velocity profiles for the turbulent boundary layer instead of Swafford’s
the shear lag coefficient in Green’s lag entrainment equation of the turbulent boundary layer model was adjusted
Deviation from the equilibrium flow was coupled to the shape factor of the boundary layer
7. 7 Lift
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36. 36 Roughness configurations NACA wrap-around roughness (no. 60 grid distributed sparsely from 8% at the lower surface to 8% on the upper surface (worst case?)
NASA roughness (no. 80 grid strips , 2.5 cm wide at both the upper and lower surface 8% chord stations
Zigzag tape, various thicknesses and positions
Fixed transition on the leading edge in calculations
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40. 40 Conclusions The measured zero-lift angle of several NACA airfoils needs to be adjusted with absolute values ranging from 0.4 to 1 degree
The maximum lift coefficients predicted with RFOIL match the LTPT data well at Re=3x106, but under predict the Cl,max at 6x106 by 3.5% up to 6.5% at Re=9x106
Though it may be possible that the higher Cl,max in the LTPT data partly originates from the wall pressure method, RFOIL also under predicts the maximum lift measured with surface pressures.
41. 41 Conclusions (cntd) RFOIL consistently under predicts the drag coefficient with about 9% for a wide range of airfoils and Reynolds numbers
NACA standard roughness causes a reduction in the lift coefficient of 18% to 20% for 18% thick airfoils from the NACA 64-series
The effect on airfoil performance of various types of roughness has been measured in the past, but it is unclear what type of roughness may be expected, though wrap-round roughness may serve as a worst-case scenario
42. 42 How to proceed? Roughness investigations in the wind tunnel at the appropriate Reynolds numbers and field tests with zigzag tape on the blades are necessary to be able to better quantify the effect of blade soiling on the rotor performance
Side-by side tests are necessary to better understand the amount of soiling during operation.