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TRANSCRIPT
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Technische Universitt Mnchen
Prof. Dr.-Ing. H.-P. Kau Module Fluid Machinery 12 - 1
Chapter 12
12.Wind power plants
1. Environmental conditions2. Examples
3. Specifications
4. Advantages and Disadvantages
5. Realised designs
6. Design
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Technische Universitt Mnchen
Prof. Dr.-Ing. H.-P. Kau Module Fluid Machinery 12 - 2
Environmental conditions of wind turbines
Approx. 1.5 to 2.5% of the sunss energy is transformed to wind giving a theoretical windpotential
of 35 * 1011
kWh/a for Germany. From this amount of wind energy only 2 * 1011
kWh/a aretechnically usable since the wind velocity has to be between 4 and 24 m/s. This results in a wind
energy of40 to 8000 W/m2.
Resulting from the required wind
velocities the typical operational area of
wind turbines in Germany is north of the
line Aachen-Kassel-Erfurt-Chemnitz-
Dresden.
The wind velocity is more permanent
above a height of 50m over groundwhich eases the efficient use of wind
turbines.
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Technische Universitt Mnchen
Prof. Dr.-Ing. H.-P. Kau Module Fluid Machinery 12 - 3
Wind conditions Europe and Germany
StrombasiswissenNr.109,Informationszentraleder
Elektrizittsw
irtschafte.V.FrankfurtamMain1995
Averaged wind
velocity in 10m
above ground
to
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Prof. Dr.-Ing. H.-P. Kau Module Fluid Machinery 12 - 4
Munich waste disposal site
Hub height: 67m
Nominal power: 1500kW
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Prof. Dr.-Ing. H.-P. Kau Module Fluid Machinery 12 - 5
Offshore Windpark Middelgrunden
20 wind turbines (2MW Bonus Energy A/S,
rotor diameter: 76m) 180m distance
4-8m Water Depth
Wind speed at 50m: 7.2m/s
3,4km overall length
Per Year Output: 89 GWh
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Prof. Dr.-Ing. H.-P. Kau Module Fluid Machinery 12 - 6
Specifications of a wind turbine
Simple design and low manufacturing costs
Rugged construction (gust and storm-proof
design)
Low maintenance
Low-noise operation
High efficiency
Turnable tower
Rotor blades are adjustable at hub
Interconnected operation or possibilities to store
the obtained energy
For example pumped or compressed air
storage plants
Rotor blade
Connection to
power supplyFoundation
Tower
Rotor hub and
blade adjustment Wind tracking
Generator
Nacelle
Gear boxBrake
Switschboard &
control system
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Technische Universitt Mnchen
Prof. Dr.-Ing. H.-P. Kau Module Fluid Machinery 12 - 7
Advantages and disadvantages of a wind turbine
Hydropower plant Wind turbine Oil / coal / gas
power plant
Nuclear power plant
Fuel reserve + Renewable energy:
timely unlimited
+ Renewable energy:
timely unlimited
- approx. 50 years - approx. 50 years =>
fast breeder reactor?
Local existence - Often not at the
location where
energy is needed
- Often not at the
location where energy
is needed
+ easily transportable + Comparatively easy to
transport
Upgradability - Limitied - Limitied + short-term
unlimited
+ short-term hardly
unlimited
Emissions no emission from
power plant, but CO2-
emission from
reservoir
Noise emission,
shadow strike
- Waste heat, CO2-
and NOx-emission
- Waste heat, radiation
near to the plant?
Efficiency + approx. 90% approx. 45% - approx. 35 60% - approx. 35%
Disposal problems + no + no - Disposal of ash and
gypsum
- Final disposal
unsolved!
Accident hazard,
probability
+ very low + very low medium + with corresponding
monitoring effort very
low
Consequences - Dam breaks: very
huge damages,
short-term
+ very low + limited range,
short-term
- Explosion: extreme
consequences, short-
and long-term
+good
medium
-poor
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Technische Universitt Mnchen
Prof. Dr.-Ing. H.-P. Kau Module Fluid Machinery 12 - 8
Advantages and disadvantages of a wind turbine
Hydropower plant Wind turbine Oil / coal / gas power
plant
Nuclear power plant
Land consumption River power station
small, storage powerplant maybe very
high
Comparatively high,
land remains arable
+ small + small
Environmental impact + managable, overall
nearly neutral
+ managable, overall
nearly neutral
- managable, clearly
negative
- ??
Dismanteling + possible, maybe
complex
+ very easy + easy - Very complex
Operation: Contro l + Very fast adjustable - Not adjustable Coal slow, CCGT fast - Only slowly
adjustable
Avail ib il ity + Very high + Very high medium + Very high
Investment costs - Very high + medium + medium high
Amortisat ion Approx. 20 years Approx. 5 to 10 y. Approx. 5 to 15 y. Approx. 15 y.
Maintenance + low + low medium medium - high
Life + 40 to 100 years - 10 to 20 y. - 10 to 30 y. approx. 30 y.
Construction time 2 to 10 years Approx. 1 year 1 to 3 y. 5 to 10 y.
+good
medium
-poor
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Technische Universitt Mnchen
Prof. Dr.-Ing. H.-P. Kau Module Fluid Machinery 12 - 9
Basic classification of wind turbines
Horizontal spool machinery Vertical spool machinery
Lift using machinery Drag using machinery
Most common design: Horizontal spool machinery with lift using blades
a) Mul tiblade converter b) Twoblade turbine c) Threeblade turbine
d) Cased turbine e) Darrieus machine f) H-Rotor
g) Savonius rotor h) Flettner rotor i) Cup rotor
j) Half cased drag rotor
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Technische Universitt Mnchen
Prof. Dr.-Ing. H.-P. Kau Module Fluid Machinery 12 - 10
Arrangement of the geared power train in horizontal machinery
Gearbox and
generator in thenacelle (common
design)
Generator
verticallymounted in the
tower head
Gearbox and
generator in thetower base
Gearbox in the
tower head andgenerator in the
tower base
Generator in the
tower baseGearbox is split
Directly driven
generatorwithout gearbox
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Technische Universitt Mnchen
Prof. Dr.-Ing. H.-P. Kau Module Fluid Machinery 12 - 11
Vertical spool machinery
Parabolic rotorCylindrical rotor
Advantages and
disadvantages in
comparison with a horizontal
spool machinery:
+ less moving parts
+ no driven orientation
necessary
+ smaller forces
- lower efficiency
- poorer performance
Blade
BearingCirculargenerator
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Technische Universitt Mnchen
Prof. Dr.-Ing. H.-P. Kau Module Fluid Machinery 12 - 13
Example Nordex N80 / 2500 kW
1. Rotor blades
2. Hub
3. Engine frame
4. Bearing, established in double-row spherical roller bearings
5. Shaft
6. Twostage planetary drive
7. Disc brake
8. Generator coupling
9. Water-cooled generator.
10. Cooling-system for generator and gearbox
11. Cooling-system for generator
12. Redundant wind measuring system
13. Control
14.Hydraulic system for the hydraulic pressure of the brake cylinders
and the yaw brakes15. Azimuth drive
16. Azimuth bearing
17. Nacelle made of glassfibre reinforced plastic
18. Tubular steel tower
19. Pitchsystem (three independant, electrically driven pitch gear units)
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Technische Universitt Mnchen
Prof. Dr.-Ing. H.-P. Kau Module Fluid Machinery 12 - 14
Data sheet Nordex N80Rotor GeneratorNumber of blades 3 Power 2.500 kW
Speed 10.9 bis 19.1 /min Currency 660V
Rotordiameter 80 m Typ Double-fed induction generator, liquid-
cooledSwept ares 5.026 m2 Speed 740-1.310 /min
Power control Pitch Protection class IP 54
Startwind 3 m/s Mass ca. 12.000 kg
Stopwind 25 m/s
Orientation controlRated power at approx. 15 m/s
Surviving wind speed 65 m/s according tp GL class 1 / 70 m/saccording IEC Tclass 1
Azimuth bearing Ball bearing
Pitch control Single blade pitch Brake hydraulic, Disc brakeMass approx. 50.000 kg Drive Two induction motors with integrated
brakes
Speed approx. 0.5 0/s
Gearbox TowerTyp Threestage planetary spur gearbox Design Modular tubular steel tower, cylindrical /
top segment conical or truss tower, hot-dipped
Gear ratio 02:08.1 Hub height Tubular steel tower 60 m, certificate IEC1a, DIBt 3
Mass approx. 18.500 kg Truss tower 80 m, certificate IEC 1a, NVN1a, DIBt 3
Status: 09/2005 (subject to technical modifications)
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Technische Universitt Mnchen
Prof. Dr.-Ing. H.-P. Kau Module Fluid Machinery 12 - 15
Energy transformation: Stream theory
The wind flowing into the wind turbine (1) with the velocity v1is decelerated. Kinetic energy is withdrawn from the wind to
drive the rotor (A). The deceleration of the air stream in the
rotor causes a stream expansion (dilatation) (2).
A pressure increase occurs downstream at the inside of the
stream. Inside the rotor (A) a pressure decrease takes place.
At some distance upstream and downstream of the rotor atposition (1) and (2) the pressure is equal to the ambient
pressure p0 on the entire cross-section. Hence for a annular
cross-section the relative velocity becomes |w1| = | w2|.
pt
A
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Technische Universitt Mnchen
Prof. Dr.-Ing. H.-P. Kau Module Fluid Machinery 12 - 16
Formulas of the stream theory
Power withdrawn from the stream at the massflow :
Thrust of the rotor:
Actio = Reactio Thrust of the rotor corresponds to
the force which the rotor exerts on the fluid
Average velocity in the rotor plane:
Massflow through the rotor:
Mechanical power of the rotor:
)(2
1 22
2
1 vvmP m
)( 21 vvmF
vvvmvFP )( 21
vvvmvvmP )()(
2
121
2
2
2
1
2
)( 21 vvv
)(21 21 vvAm
))((4
121
2
2
2
1 vvvvAP
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Technische Universitt Mnchen
Prof. Dr.-Ing. H.-P. Kau Module Fluid Machinery 12 - 17
Betz theory about the power of a wind turbine
Betz coefficient:
AvP 3
102
1
1
2
2
1
2
3
1
212
22
1
0
112
1...
2
1
))((41
v
v
v
v
Av
vvvvA
P
PcP
The maximum of the Betz coefficient is at for (Betz factor) for
an ideal, frictionless flow.
593,027
16Pc
3
1
1
2 v
v
Power of the airflow at the cross-section A without any power withdrawn:
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Technische Universitt Mnchen
Prof. Dr.-Ing. H.-P. Kau Module Fluid Machinery 12 - 18
Power characteristics of wind turbines
R
Rotor power as a function of the wind velocity: with cPR = Betz coefficient of the rotor
Betz factor cp
AvcP PRR3
12
Betzcoefficient Fast runner
Theoretic power coefficient of an ideal wind turbine
3-blade
rotor
2-blade rotor
Single blade
rotorSlow runner
Darrieus
rotor
Dutchmans windmill
American w indmil l
Tip speed ratio
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Technische Universitt Mnchen
Prof. Dr.-Ing. H.-P. Kau Module Fluid Machinery 12 - 19
Real characteristics according to the number of blades
Gradual approximation of
the real rotor characteristic
with the help of the theory
23
R
Number of
blades
Powercoefficient
Tip speed ratio at design point
Capability of the air flow
Ideal Betz factor
Swirl losses Profile losses
Finite number of blades
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Technische Universitt Mnchen
Prof. Dr.-Ing. H.-P. Kau Module Fluid Machinery 12 - 20
Power control through pitch
The power generated by the wind turbine has to be controlled due to the technically limited capacity
of the generator, due to safety aspects and to the purpose of keeping the power generation constant.
One possibility is to decrease the pitch angle of the rotor blades (pitch control).
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Prof. Dr.-Ing. H.-P. Kau Module Fluid Machinery 12 - 21
Power control through stall
The rotor blades stall at a fixed pitch angle and at a
constant circumferential velocity when the wind velocity
raises. This effect limits the power output of the windturbine so this can be used to control the plant (stall
control).
The design of the plant has to be modified:
Increased stiffness and ruggedness of the entire plant isnecessary to withstand the higher aerodynamic loading
Comparatively high generator power necessary to cover
peak power
Improved starting capabilities of the rotor (2-blade rotorneeds an electrical starter)
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Prof. Dr.-Ing. H.-P. Kau Module Fluid Machinery 12 - 22
Power
Factor Formula
Theoretical maximum possible power coefficient of the rotor:(Betz factor)
Rotor efficiency:
(caused by aerodynamic losses of the rotor)
Betz coefficient:(modern rotor designs obtain a Betz coefficient of approx. 0.5)
Efficiency of all mechanical and electrical components:
From the efficiency of the rotor and all remaining components the effciency
of the wind turbine is calculated:
Effective power of the wind turbine:
(Electrical power of the plant)
593.0Pc
gRPPR cc ,
85.07.0, gR
elmech,
elmechPRPlantP cc ,,
RotorPlantPel AvcP
3
1,2
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Technische Universitt Mnchen
Prof. Dr.-Ing. H.-P. Kau Module Fluid Machinery 12 - 23
Principal sequence of the wind turbine desing
Iterative proces(maximum energy
supply)
Design wind
data
Rotor
diameter
Generator
power
Tower
height
Rotor performancemap
Av. wind velocity and frequency
distribution in hub height
Management
and control
Optimum rotor
speed
effective rotor
characteristic
Mech. and el. losses
in power trainWind data at
installation location
Power characteristic of
plant Pel
Energy supply