College of Engineering
Aerodynamic Effects of Painted Surface Roughness on Wind Turbine Blade
Performance
06/09/2015 Liselle A. Joseph
Aurelien Borgoltz Matthew Kuester
William Devenport
Julien Fenouil
Special thanks to Wind Turbine Aerodynamics Team of GE Power and Water
Joseph et al. NAWEA Symposium 2015
• Roughness is known to § decrease lift (Abbott and Von Doenhoff, 1959; Jones, 1936) § Increase drag (Abbott and Von Doenhoff, 1959; Jones, 1936) § Move transition forward (Timmer, 2004)
• Roughness on wind turbine blades (icing, soiling, coat deterioration etc.) reduces performance (Sagol, 2013; Ehrmann, 2014; Dalili et al., 2009)
• These are the main types of roughness currently under study
• No work into the effect of orange-peel type roughness § Likened to surface of an orange § More wavy than peaky § Produced from painting techniques and manufacturing processes
Importance of Roughness Effects
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Joseph et al. NAWEA Symposium 2015
• Created by painting Contact© paper with latex paint using rollers of various types
• Number of coats and painting direction were also varied
• 3 configurations created and tested
(a) (b) (c)
Images of the Roughness Configurations (a) S1 (b) S2 and (c) S3. The scale of the roughness features is illustrated using the 12.5-mm grid superimposed on the S1 roughness
12.5mm 12.5mm
Roughness Fetches
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Joseph et al. NAWEA Symposium 2015
• Approximate values of roughness parameters measured using Mahr PS1
• In order of increasing roughness heights: baseline, S1, S2, S3
Baseline
(Unpainted Contact© Paper)
S1 S2 S3
𝑅↓𝑎 , µμm 1.6 4.0 6.1 10.7
𝑅↓𝑡 , µμm 13.5 28.6 38.7 62.9
𝑅↓𝑞 , µμm 2.9 10.1 17.7 23.4
Roughness Fetches
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Joseph et al. NAWEA Symposium 2015
Chord (m) Re (x106) Configuration Rek1
0.8
2
baseline 0.4
S1 4.4
S2 12.7
S3 21.3
3
baseline 0.7
S1 7.9
S2 22.5
S3 37.5
0.46
1.5 baseline 0.7
S3 24.0
2 baseline 1.1
S2 48.2
• Two DU96-W-180 models tested, each at 2 chord Reynolds Numbers
• Smooth and rough cases tested for each model
• Roughness Reynolds Number formulations:
• Below Rek1,crit effects are small, above Rek1,crit effects become more noticeable
Re↓k1 = 𝑅↓𝑞 𝑢↓k /𝜈
Test Matrix
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Joseph et al. NAWEA Symposium 2015
• Experiments done in VT stability Wind Tunnel
• Lift and drag obtained from pressure measurements from test section wall and drag rake
• Transition obtained from infrared transition detection system
• Model wrapped in contact paper, 0.8-mm insulator, then roughness fetch
Experimental Set Up
0.8-mm silicone rubber insulator Starboard
m o u n t e d IR camera
Drag rake
Port mounted IR camera
Downstream View of 0.80-m DU96-W-180 Mounted in Wind Tunnel with Infrared Thermography System
Aluminum model with internally mounted heaters
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Joseph et al. NAWEA Symposium 2015
• Positive stall: αc~ 9°to10°
• Negative stall: αc~-14°
• Zero-lift αc~ -2°
• Baseline cases for two models of different chord lengths agree
Results
-20 -15 -10 -5 0 5 10 15 20-1
-0.8
-0.6
-0.4
-0.2
0
0.2
0.4
0.6
0.8
1
αc
Clw
c
0.80-m DU96 Re=2.0M, baseline, Rek1=0.4
0.46-m DU96, Re=2.0M, baseline, Rek1=1.1
Variation of Lift and Drag for Different Chord Length Models, in Baseline Configuration, at Fixed Chord Reynolds Number of 2.0x106
-15 -10 -5 0 5 100
0.005
0.01
0.015
0.02
0.025
0.03
0.035
0.04
αc
Cdw
c
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Joseph et al. NAWEA Symposium 2015
• Max lift and lift curve slope decrease with increasing Rek1
• effect most apparent at positive αc, especially above αc=5°
• Above Rek1 ~ 23 effect of roughness becomes much larger than below this value
• Rek1crit ~ 23
Effect of Roughness on Lift
Lift Plots for Varying 𝑅𝑒↓𝑘1 for the DU96-W-180 (0.46-m and 0.80-m chords) at 𝑅𝑒↓𝑐 between 1.5x106 and 3.0x106
-15 -10 -5 0 5 10
-1
-0.8
-0.6
-0.4
-0.2
0
0.2
0.4
0.6
0.8
1
αc
Clw
c
c=0.80m, Rec=2.0.M, baseline, Rek1=0.4
c=0.80m, Rec=3.0M, baseline, Rek1=0.7
c=0.46m, Rec=1.5M, baseline, Rek1=0.7
c=0.46m, Rec=2.0M, baseline, Rek1=1.1
c=0.80m, Rec=3.0M, S1, Rek1=7.9
c=0.80m, Rec=2.0M, S2, Rek1=12.7
c=0.80m, Rec=2.0M, S3, Rek1=21.3
c=0.80m, Rec=3.0M, S2, Rek1=22.5
c=0.46m, Rec=1.5M, S3, Rek1=24.0
c=0.80m, Rec=3.0M, S3, Rek1=37.5
c=0.46m, Rec=2.0M, S2, Rek1=48.2
6 8 10 120.65
0.7
0.75
0.8
0.85
0.9
0.95
1
1.05
1.1
1.15
αc
Clw
c
6 8 10 120.65
0.7
0.75
0.8
0.85
0.9
0.95
1
1.05
1.1
1.15
αc
Clw
c
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Joseph et al. NAWEA Symposium 2015
• Drag in bucket increases with increasing Rek1
• effect most dominant at positive αc
• Above Rek1 ~ 24 effect of roughness becomes much larger than below this value
• Rek1crit is between 20-25 (accounting for 10% uncertainty)
Effect of Roughness on Drag
-15 -10 -5 0 5 100
0.005
0.01
0.015
0.02
0.025
0.03
αc
Cdw
c
c=0.80m, Rec=2.0.M, Rek1=0.4
c=0.80m, Rec=3.0M, Rek1=0.7
c=0.46m, Rec=1.5M, Rek1=0.7
c=0.46m, Rec=2.0M, Rek1=1.1
c=0.80m, Rec=3.0M, Rek1=7.9
c=0.80m, Rec=2.0M, Rek1=12.7c=0.80m, Rec=2.0M, Rek1=21.3
c=0.80m, Rec=3.0M, Rek1=22.5
c=0.46m, Rec=1.5M, Rek1=24.0
c=0.80m, Rec=3.0M, Rek1=37.5
c=0.46m, Rec=2.0M, Rek1=48.2
Drag Plots for Varying 𝑅𝑒↓𝑘1 for the DU96-W-180 (0.46-m and 0.80-m chords) at 𝑅𝑒↓𝑐
between 1.5x106 and 3.0x106
-15 -10 -5 0 5 100
0.005
0.01
0.015
0.02
0.025
0.03
αc
Cdw
c
c=0.80m, Rec=2.0.M, Rek1=0.4
c=0.80m, Rec=3.0M, Rek1=0.7
c=0.46m, Rec=1.5M, Rek1=0.7
c=0.46m, Rec=2.0M, Rek1=1.1
c=0.80m, Rec=3.0M, Rek1=7.9
c=0.80m, Rec=2.0M, Rek1=12.7c=0.80m, Rec=2.0M, Rek1=21.3
c=0.80m, Rec=3.0M, Rek1=22.5
c=0.46m, Rec=1.5M, Rek1=24.0
c=0.80m, Rec=3.0M, Rek1=37.5
c=0.46m, Rec=2.0M, Rek1=48.2
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Joseph et al. NAWEA Symposium 2015
• Below Rek1~23 L/Dmax slowly declines
• Large decrease in L/Dmax after Rek1~23
• Rek1crit ~ 20-25
Effect of Roughness on Lift-to-Drag Ratio
0 10 20 30 40 500
20
40
60
80
100
120
Rek1
L/D m
ax
datacurve fit
Variation of Maximum Lift-to-Drag Ratio with 𝑅𝑒↓𝑘1 for the DU96-W-180 (0.46-m and 0.80-m chords) at 𝑅𝑒↓𝑐 between 1.5x106 and
3.0x106 10/14
Joseph et al. NAWEA Symposium 2015
• Infrared transition detection system used to detect transition
• Gradient observed in images is onset of transition
• Image processing techniques used to extract %chord location AOA=0
IR Trans region ~56%(8.5" from TE)
AOA=0
IR Trans region ~61%(7.5" from TE)
Infrared Images of the Pressure Side of the 0.46-m DU96-W-180 at AoA=0° showing the Forward Movement of the Transition Front from the (a) Baseline case with Ra=1.58 to (b) S3 Roughness
case with Ra=6.78
FLOW
(a) (b)
Effect of Roughness on Transition
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Joseph et al. NAWEA Symposium 2015
-10 -5 0 5 100
10
20
30
40
50
60
70
80
α, dg
x/c,
%
Rec=2.0M, Rek1=0.4
Rec=3.0M, Rek1=0.7
Rec=2.0M, Rek1=4.4
Rec=3.0M, Rek1=7.9
Rec=2.0M, Rek1=12.7
Rec=2.0M, Rek1=21.3
Rec=3.0M, Rek1=22.5
Rec=3.0M, Rek1=37.5
-8 -6 -4 -2 0 2 4 6 8 10 1210
20
30
40
50
60
70
80
90
100
α, dg
x/c,
%
Rec=2.0M, Rek1=0.4
Rec=3.0M, Rek1=0.7
Rec=2.0M, Rek1=4.4
Rec=3.0M, Rek1=7.9
Rec=2.0M, Rek1=12.7
Rec=2.0M, Rek1=21.3
Rec=3.0M, Rek1=22.5
Variation of transition location with angle of attack on the (a) Suction and (b) Pressure Side of the 0.8-m for all Rek1
Effect of Roughness on Transition
Suction Side Pressure Side
0.8-m DU96-W-180
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Joseph et al. NAWEA Symposium 2015
-10 -5 0 5 100
10
20
30
40
50
60
70
80
α, dg
x/c,
%
Rec=1.5M, Rek1=0.7
Rec=1.5M, Rek1=24.0
Rec=2.0M, Rek1=48.2
-10 -5 0 5 100
10
20
30
40
50
60
70
80
α, dg
x/c,
%
Rec=1.5M, Rek1=0.7
Rec=2.0M, Rek1= 1.1
Rec=1.5M, Rek1= 24.0
Rec=2.0M, Rek1= 48.2
Variation of transition location with angle of attack on the (a) Suction and (b) Pressure Side of the 0.46-m for all Rek1
Effect of Roughness on Transition Suction Side Pressure Side
0.46-m DU96-W-180
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Joseph et al. NAWEA Symposium 2015
Orange-peel type painted surface roughness on wind turbine blades have an effect on the performance
It was found that: • Roughness effects show dependence on Rec and Rek
• The effect of the roughness is more pronounced at positive angles of attack
• Lift decreases gradually with increasing Rek, up to the critical Rek
• Drag increases gradually with increasing Rek, up to the critical Rek
• Transition moves forward slightly with increasing Rek, up to the critical Rek
• Critical Rek for orange-peel roughness is between 20 and 25.
Conclusions
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Joseph et al. NAWEA Symposium 2015
Q&A
Joseph et al. NAWEA Symposium 2015
Supporting Slides
Joseph et al. NAWEA Symposium 2015
Effect of Roughness on T-S Waves
• Roughness induced disturbances grow and overtake natural T-S waves
• Roughness-induced T-S waves cause linear transition front upstream of natural transition
0 2 4 6 8 10 12 14 16 180
0.2
0.4
0.6
0.8
1
1.2
1.4x 10
-3
Wavelength, mm
Nor
mal
ized
PSD
S1S2S3
Averaged wavelength spectra of the painted roughness surfaces
0 5 10 15 20 25 30 35 400
0.1
0.2
0.3
0.4
0.5
0.6
0.7
0.8
0.9
1
Wavelength, mm
Norm
alize
d Inte
grate
d Gro
wth
0.46-m chord, Re = 1.5x106
0 5 10 15 20 25 30 35 400
0.1
0.2
0.3
0.4
0.5
0.6
0.7
0.8
0.9
1
Wavelength, mm
Norm
alize
d Inte
grate
d Gro
wth
0.46-m chord Re = 2.0x106
0 5 10 15 20 25 30 35 400
0.1
0.2
0.3
0.4
0.5
0.6
0.7
0.8
0.9
1
Wavelength, mm
Norm
alize
d Inte
grate
d Gro
wth
0.80-m chord, Re = 2.0x106
0 5 10 15 20 25 30 35 400
0.1
0.2
0.3
0.4
0.5
0.6
0.7
0.8
0.9
1
Wavelength, mm
Norm
alize
d Inte
grate
d Gro
wth
0.80-m chord, Re = 3.0x106
α = -5 deg., Pressure Side: x/c=10%α = 0 deg., Pressure Side: x/c=50%α = 5 deg., Pressure Side: x/c=70%α = -5 deg., Suction Side: x/c=55%α = 0 deg., Suction Side: x/c=50%α = 5 deg., Suction Side: x/c=40%
Wavelengths of unstable Tollmien-Schlichting disturbances for (a) 0.46-m DU96-W-180 at Re=1.5x106 and (b) 0.80-m DU96-W-180 at Re=1.5x106
(a)
(b)
Joseph et al. NAWEA Symposium 2015
Analysis of Effect on Performance • XFOIL used to investigate whether changes in lift and drag are from changes in transition
• XFOIL ‘tripped’ at where transition is observed on IRT images for rough cases
• Differences compared to that observed between clean and rough results
-10 -5 0 5 10-1
-0.5
0
0.5
1
1.5
α, deg.
Cl
-10 -5 0 5 100.006
0.008
0.01
0.012
0.014
0.016
0.018
0.02
α, deg.
Cd
-10 -5 0 5 10-0.5
0
0.5
1
1.5
2
2.5
3
3.5x 10
-3
α, deg.
ΔC
d
-10 -5 0 5 10-0.07
-0.06
-0.05
-0.04
-0.03
-0.02
-0.01
0
0.01
α, deg.
ΔC
l
Clean - ExperimentS3 - ExperimentClean - XFOILS3 - XFOIL
ΔCl - ExperimentΔCl - XFOIL
ΔCd - ExperimentΔCd - XFOIL
XFOIL analysis of the effect of transition location on lift and drag. XFOIL transition locations were set from IR transition measurements for the 0.46-m DU96-W-180 Model at Re = 1.5x106. Differences in (a)
lift and (b) drag are between the clean model (covered in insulator) and the S3 roughness condition.
(a) (b)