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1/20
Numerical and Theoretical Study on the Wind Response of Wind Turbine
June 11th, 2005The University of TokyoPham Van Phuc
2/20Wind turbine (WT)
• Wind turbines are getting bigger• Turbine rotor size increases• Hub height increases• Tower are getting higher
Time
Scale
Tower
NacelleBlade
Hub
Rotor
Wind turbine
3/20The largest wind turbine• 5000kW Wind turbine
– Manufacturer : Repower (Germany)– Rotor diameter :126m– Tower height :120m
4/20WT transportations
5/20WT constructions (1)
6/20WT constructions (2)
7/20Wind energy development
• Wind energy:– pure, clean, and inexhaustible.
• Installed turbines (in 2003)– All of the world: 40000 turbines.
– Germany : 12000.– USA : 4600– Spain : 3550– Denmark : 2880– Japan : 600
• Target by 2010– Japan: 3000 turbines. Wind farm at Tomamae, Hokaido, northern of Japan
8/20Damages of wind turbine in Japan
The damage of turbines in the Okinawa Island by typhoon Maemi in 2003
• Many damages of WT tower, blades have been reported consecutively.
• . It is strongly required to enhance the wind resistant design of wind turbines.
Collapsed due to foundation destruction
Blades broken Blades broken
Collapsed due to the buckling of the tower
9/20Wind turbine design & problems• Concepts of WT design (IEC61400-1)
– Controlled by adjusting the pitch angle of blade (Fig.1) and direction of nacelle (Fig.2)
• to get maximum wind power during their operations
• to minimize the wind load during the strong wind
(Fig.1)
(Fig.2)
• Japan has various types of typhoons and complex mountains– Control system becomes ineffective especially during
blackout which often occurs during typhoon– Control system is insensitive especially in the site with a large
turbulence.
Wind resistant design is required to consider the critical wind load
10/20Objectives of study
• Carrying out a field investigation and measurement to obtain structural data and characteristics of wind turbine.
• Numerical study– Constructing the wind turbine model of beam element. Comparing
the eigenfrequencies of analytical model with measured natural frequencies.
– Developing a FEM code to simulate the wind load. The performance of code is compared with field measurement results.
• Theoretical study– Proposing an equivalent static load formulas that can estimate
the wind load. The performance of formula is compared with the results from FEM.
11/20Field Investigation
Cutting
Blade
Cut and measure sections
Wind turbine model
Blade
HubNacelle
Tower
Investigate the collapsed turbines in the Okinawa I l d
12/20Field measurements
Modem
② ③
①⑥
Strain gaugeInternet
ISP
Mail server
amplifier
Tel. line
Monitoring PC
The Tokyo University, Bridge Lab.
A/D TransformNTT
Tel. line
Anemometer Accelerometer
• Measurement Period : Jan. 16th 2004~Mar. 16th 2004 ( 2 months)• Sampling frequency :20Hz• Record time : every 10-minute
Measure the survived turbine in
the Okinawa Island
13/20Wind turbine model contribution
10-2
10-1
100
101
102
103
0 2 4 6 8 10
nS(n)/σ2
n(Hz)
0.81Hz6.4Hz
4.6Hz
5.6Hz
7.6Hz
2.4Hz
6.9Hz
X
Y
X
Y
23m
10-2
10-1
100
101
102
103
0 2 4 6 8 10
X DirectionY Direction
nS(n)/σ2
n(Hz)
0.81Hz
2.4Hz4.6Hz
7.6Hz
7.6 (Y)
6.9 (X)
6.4 (Y)
5.6 (X)
5.6 (Y)
4.6 (Y)
-
-
2.4 (X)
0.81 (X)
0.81 (Y)
Measurements
Frequencies (Hz)
WT model
7.6 (Y)11
6.3 (X)10
6.2 (Y)9
5.7 (X)8
5.3 (Y)7
4.5 (Y)6
2.6 (X)5
2.5 (X)4
2.4 (X)3
0.81 (X)2
0.81 (Y)1
No
Power Spectral density of accelerations
Good agreement between the eigenfrequencies of WT model and measured natural frequencies of WT
35m
Wind turbine target
Eigenvalues analysis for WT model
14/20Development of wind response analysis
• Aerodynamic force
• Motion of equation
– [K]: stiffness matrix– [M]: Mass matrix– F: Aerodynamic force vector– [C]: Rayleigh damping
MX CX KX F+ + =&& &
Node i
Node j
Wind load
Load[K]
Mi
M j
Load
Discretiations
X−uur&
Vur
Uur
Wind Vel.:Element Vel.Relative Vel.
FLFD
FM
θ
U
VX&
( ) ( )20.5 fF AC U Xρ θ= × −uurur&
Quasi-steady aerodynamic theory
15/20Wind response simulation
Y, My
X, Mx
12/17
Tower coordinateSimulation results show a good agreement with measurement
-600
0
600
1200
0 200 400 600
Mx My
Moment(kNm)
Time(s)
-600
0
600
1200
0 200 400 600
Mx My
Moment(kNm)
Time(s)
10
100
1000
1 10 100
Max(Obs.)
Ave(Obs.)
Sdev(Obs.)
Max(Cal.)
Ave(Cal.)
Dev(Cal.)
Moment Mx(kN・m)
Velocity(m/s)
10
100
1000
1 10 100
Moment My(kN・m)
Velocity(m/s)
Measured bending moment time series Simulation bending moment time series
Bending moments against Wind speed
16/20
• Proposed formula – Wind loads of along-wind direction and across-wind direction
– Considering Freq.(n)、Damping(ξ)to present the characteristic of wind load on WT. Where θ:wind direction
( )max , ,fM M G n ξ θ= ×
Proposed equivalent static load formula
• Old formula by Building Standard Law of Japan
– Gf is constant
max fM M G= × (Mean×Gust effect coef.)
17/20Combinations of wind loads
( ) 2 2, ,,DL D Max L MaxMaxM M Mθ = +
ML,Max
MD,Max
MDL,Max
Wind θ
Along-wind load
Across-wind load
Flapwise
Edgewise
(Combined load)
• Blade case– Vibrating only in flapwise
( ) ( )
( )
22, ,,
22, ,
,DL D Max L Mean LMax
L Max D Mean D
M Max M M
M M
θ σ
σ
⎛= + +⎜⎝
⎞+ + ⎟⎠
Wind θ
My
Mx
(Along-wind load)(Across-wind load)
ML,Max MD,Max
MDL,Max
(Combined load)
• Tower case
18/20The Results of the Proposed equivalent static load
0 100
3 102
6 102
-180 -90 0 90 180
MDL,max
(数値解析)
MDL,max
(本提案式)
MDL,max
(建築基準法)
Moment (kNm)
Wind directionθ(deg)
0 100
6 103
1.2 104
-180 -90 0 90 180
MDL,max
(数値解析)
MDL,max
(本提案式)
MDL,max
(建築基準法)
Moment (kNm)
Wind directionθ(deg)
(Simulation)(Formula)(Old Formula)
(Simulation)(Formula)
(Old Formula)
• Blade case • Tower case
Proposed formula results show a good agreement with simulation results
19/20Further study
The interaction among typical criteria of Japan– Complex terrain criteria– Seismic criteria
to determine the relative importance of each aspect and to further assess structural optimization of wind turbine in Japan.
20/20
Thank you!