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Harvesting the Wind Energy Trond Kvamsdal Dept. of Mathematical Sciences Norwegian University of Science & Technology
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Jun 29, 2018

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Page 1: Harvesting the Wind Energy - NORCOWE for web/SS2015-presentasonar... · Harvesting the Wind Energy . ... • Wind turbine rotors convert the kinetic energy in the wind ... (no losses)

Harvesting the Wind Energy

Trond Kvamsdal Dept. of Mathematical Sciences

Norwegian University of Science & Technology

Page 2: Harvesting the Wind Energy - NORCOWE for web/SS2015-presentasonar... · Harvesting the Wind Energy . ... • Wind turbine rotors convert the kinetic energy in the wind ... (no losses)

Contents

• Introduction • Converting kinetical wind energy to

mechanical energy • HAWT vs VAWT • Converting mechanical energy to electrical

energy • Offshore wind turbines

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Introduction

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• Temperatures vary according to the amount of sun it gets

• Uneven heating of the Earth's atmosphere and surface

• Balance between warm and cool air is constantly changing, creating wind.

How Wind is Created?

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• The terms "wind energy" or "wind power" describe the process by which the wind is used to generate mechanical power or electricity.

• Wind turbine rotors convert the kinetic energy in the wind into mechanical power.

• Wind power is the conversion of wind energy into a useful form of energy, such as using: • wind turbines to make electricity, • wind mills for mechanical power, • wind pumps for water pumping • etc.

Wind Energy

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• Wind turbines turn in the moving air

and power an electric generator that supplies an electric current.

• Simply stated, a wind turbine is the opposite of a fan. Instead of using electricity to make wind, like a fan, wind turbines use wind to make electricity.

• The wind turns the blades, which spin a shaft, which connects to a generator and makes electricity.

Wind Turbine

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Two types of turbine design: Horizontal axis and Vertical axis. Horizontal axis turbines: Can reach higher altitude wind but requires a substantial tower structure. Used in most modern wind turbine designs. Vertical axis turbines: No need to turn into wind (yaw), easier construction and maintenance (generator and gear box are on the ground) level, lower efficiency.

Vertical axis turbine

Horizontal axis turbine

Wind Turbine Design

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HAWT

VAWT

Boyle, G., Renewable Energy, 2nd ed., Oxford University Press, 2004

Wind Turbine Configurations

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Wind Turbine Components

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Converting Kinetic Wind Energy to Mechanical Energy

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Aerodynamics of wind turbines

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We need wind loads to produce power !

To extract power from kinetic energy

NT p dr= ∫R TM rp dr= ∫

Tangential load to harness the available energy as useful power.

( )22

212

1 vvmP −=

v1 v2

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1-D Momentum theory for ideal rotor (no losses)

Conservation of mass, energy and momentum in flow direction:

Thrust

Power

Wind speed at rotor plane

v1 v2

v1

2' 21 vvv +=

)(21)('

21 2

221

22

21 vvmvvAvP −=−= ρ

)()(' 2121 vvmvvAvT −=−= ρ

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Ideal Extractor Derivation Due to Albert Betz

Continuity, energy balance, and force balance across rotor area

Main assumptions • Ideal rotor

– No hub – Infinite number of blades – Blades without drag

• Pure axial flow • Incompressible flow • Uniform thrust over the rotor • Equal far-field pressures

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Ideal Extractor Derivation (2)

22'

11 AvAvAvm ρρρ ===

Due to Albert Betz

Continuity and force balance across rotor area

)(' 21 vvAvvmdtdvmmaF −=∆=== ρ

Mass conservation:

Forces on the rotor:

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Ideal Extractor Derivation (3)

FvdtdxF

dtdEP ===

Power computed based on force balance

)(' 21 vvAvvmdtdvmmaF −=∆=== ρ

Power (rate of work):

Forces on the rotor:

)()'( 212

1 vvvAP −= ρExtracted power (1):

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Ideal Extractor Derivation (4)

)(21 2

221 vvm

tE

dtdEP −=

∆∆

==

Power computed based on energy balance across rotor area

Power (rate of energy):

)('21 2

2212 vvAvP −= ρExtracted power (2):

Kinetic energy: 2

21 mvE =

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Ideal Extractor Derivation (5)

"Power = Power"

21 PP =

Rotor speed:

)('21)()'( 2

22121

2 vvAvvvvA −=− ρρ

))(('21

2121 vvvvAv +−= ρ

)(21' 21 vvv +=

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Ideal Extractor Derivation (6)

221' vvv +

=

AvP 310 2

1 ρ=

( ) )(41 2

22121 vvvvAP −+= ρ

We have found that:

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Ideal Extractor Derivation (7)

593.02716~

1121

max

2

1

2

1

2

0

=

+==

−p

p

C

vv

vv

PPC

• Irrotational system • No boundary layer or compression flow • Creeping flow (Re << 1) • Uniform power extraction • No geometry boundary conditions • Never true!

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More Rigor: Deviation from Betz Limit

1vR

Aωλ ≡

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Blade Pitch: Trade-offs Since most designs use twisted blades, power quality is never ideal across the entire rotor blade.

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“Why you should choose three blades”

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Rotor Speed Control Active Stall Control Passive Stall Control

Advantages: Dynamic, reduces train complexity Disadvantages: Costly

Advantages: Simple, self regulating Disadvantages: Requires strength in high winds, hard to start-up, complex brake systems

Page 26: Harvesting the Wind Energy - NORCOWE for web/SS2015-presentasonar... · Harvesting the Wind Energy . ... • Wind turbine rotors convert the kinetic energy in the wind ... (no losses)

By definition (axial induction factor)

then gives

If this is used in the equations for power and thrust

2' 21 vvv +=

Induction factor (a)

1)1(' vav −=

12 )21( vav −=

31

2)1(2 vaAaP −= ρ 21)1(2 vaAaT −= ρ

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312

po

PCV Aρ

=21

2T

o

TCV Aρ

=

Definition of power and thrust coefficients

24 (1 )pC a a= − 4 (1 )TC a a= −

,max T16 8 10.59 for C at27 9 3pC a= ≈ = =

Betz limit

Induction factor (a) (continued)

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1.0

0.8

0.6 CP

0.4

0.2

0.0

Dim

ensi

onle

ss m

agni

tude

1.0 0.8 0.4 0.6 Axial induction factor

0.2 0.0

U4/U CT

Betz theory invalid

Relation between Tp CCvv ,,/ 12

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The wanted loads is created by the lift and drag from the local flow past the blade

cos sinsin cos

N

T

p L Dp L D

φ φφ φ

= += −

L and D depends on • Angle of attack • Airfoil geometry • Reynold number

Loads on a turbine blade

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= + −rel o bladeV V W V

In Vblade is included elastic velocities, translations and stiff body rotation

α φ θ= −

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Several options, as e.g. ● Full CFD ● Vortex methods (unsteady panel methods, lifting line etc.) ● BEM But since we are solving in the time domain with Δt small a fast model is needed and BEM is almost always used. The more advanced models are mostly used to check the various submodels in the BEM method

Computational methods

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BEM Blade Element Moment Method

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BEM method gives the equilibrium of the aerodynamic loads and the induced velocity W Knowing, W, the flowangle and thus the angle of attack, α, is known and new loads can be found from table look up in airfoil data, Cl(α) and Cd(α)

212

212

( )

( )rel l

rel d

L V cC

D V cC

ρ α

ρ α

=

=

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For zero yaw the conservation of linear and angular momentum in a streamtube intersecting the rotor plane at radial position, r, yields

cos4 ( )n

o n

BLWrF V W

φπρ−

=−

sin4 ( )t

o n

BLWrF V W

φπρ−

=−

These equations can be rewritten to (Wn=aVo and Wt=a’ωr)

21

4 sin 1n

aF

σ

=+

14 sin cos 1

t

a FCφ φ

σ

′ =−

Page 35: Harvesting the Wind Energy - NORCOWE for web/SS2015-presentasonar... · Harvesting the Wind Energy . ... • Wind turbine rotors convert the kinetic energy in the wind ... (no losses)

Prandtl’s tip loss factor In the BEM method we assume no azimuthal variation of W corresponding to infinitely many blades For a finite number of blades the flow is different, especially near the tip, as shown using a simple vortex model with constant circulation and using Biot-Savart

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312

po

PCAVρ

=

o

RVωλ =

With the use of the BEM code the theoretical optimal rotor can be computed for various number of blades

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”Glauert” correction for high values of 212

To

TCAVρ

=

Mostly for low wind speed

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13

1 14 3

4 (1 )4 (1 (5 3 ) )T

a a F aC

a a a F a− ≤

= − − >2

4 (1 )4( (1 2 ) )

cT

c c c

a a F a aC

a a a F a a− ≤

= + − >

For large values of CT the momentum equations are replaced by empirical relationships

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HAWT vs VAWT

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Advantages • Omnidirectional

– Accepts wind from any angle • Components can be mounted

at ground level – Ease of service – Lighter weight towers

• Can theoretically use less materials to capture the same amount of wind

Disadvantages • Rotors generally near ground

where wind poorer • Centrifugal force stresses

blades • Poor self-starting capabilities • Requires support at top of

turbine rotor • Requires entire rotor to be

removed to replace bearings • Overall poor performance and

reliability • Have never been commercially

successful

Vertical Axis Wind Turbine

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Advantages • Blades are to the side of the

turbines center of gravity, helping stability

• Ability to pitch the rotor blades in a storm to minimize damage

• Tall tower allows access to stronger wind in sites with wind shear

• Tall tower allows placement on uneven land or in offshore locations

• Can be sited in forest above tree-line

• Most are self-starting

Disadvantages • Difficulty operating in near

ground winds • Difficult to transport (20% of

equipment costs) • Difficult to install(require tall

cranes and skilled operators) • Effect radar in proximity • Local opposition to aesthetics • Difficult maintenance

Horizontal Axis Wind Turbine

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HAWT vs. VAWT

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• Drag designs – Savonius

Type of Wind Turbine Design Wind turbines are designed based on either aerodynamic Drag or Lift force.

• Lift designs – VAWT Darrieus – Most HAWT designs

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• Blade is essentially an airfoil (like wings of airplanes).

• When air flows past the blade, a wind speed and pressure differential is created between the upper and lower blade surfaces. The pressure at the lower surface is greater and thus acts to "lift" the blade.

• The lift force is translated into rotational motion.

• Lift design generally has higher efficiency and is used in most modern turbines.

Lift

Lift design

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Ken Youssefi / Hsu Engineering 10, SJSU 45

• The wind literally pushes the blades out of the way.

• Slower rotational speeds and high torque capabilities. Useful for providing mechanical work (water pumping).

Drag design

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Converting Mechanical Energy to Electrical Energy

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Electromagnetic induction

tNe

∂∂

−=φ

tBE∂∂

−=×∇Maxwell-Faraday

Faraday's law

E – electric field strenght B – flux density e – Induced Voltage N – number of turns φ – total magnetic flux

"Relative motion"

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A simple generator • Armateur: A conductor in the stationary portion, i.e. "stator" • Rotor: Permanent magnet in the moving part • Need mechanical force to move the magnetic field!

Mechanical Input Electrical Output

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AC Generation

How fast should the rotor turn ?

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Rotation rate If we want to generate 60 Hz frequency:

When a rotor has more poles:

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How to create magnetic field • Use permanent magnet for small generator • Use DC current passing through a coil

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Self induced magnetic field Create rotating magnetic field in stator • Coils imbedded in a 3-phase

generator • Need AC-voltage

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Major types of generators

Synchronous generator • Operate at constant rational

speed to create constant voltage

• Need magnetic field • Permanent magnet rotor for

small machine • Almost all WT creates

magnetic field by DC current

Asynchronous generator • Induction generator • Do not operate at fixed

speed • Magnetic field is induced

from AC voltage

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Synchronous generator

To supply DC current for field winding

To increase rotational speed in order to produce 50/60 Hz voltage frequency

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Induction machine

• Require rotating magnetic field, supplied by AC voltage

• Use (squirrel) cage rotor made from a number of aluminium bars shorted together at their ends, forming a cage

• Rotor have to spin with a slower speed than sychronous speed

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0 ~ 5 m/s --- Wind speed is too low for generating power. Turbine is not operational. Rotor is locked.

5 ~ 15 m/s ---- 5 m/s is the minimum operational speed. It is called “Cut-in speed”.

In 10 ~ 25 mps wind, generated power increases with the wind speed.

15 ~ 25 m/s ---- Typical wind turbines reach the rated power (maximum operating

power) at wind speed of 15 m/s (called Rated wind speed). Further increase in wind speed will not result in substantially higher generated power by design. This is accomplished by, for example, pitching the blade angle to reduce the turbine efficiency.

> 25 m/s ---- Turbine is shut down when wind speed is higher than 25m/s (called

“Cut-out” speed) to prevent structure failure.

Typical Wind Turbine Operation

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Small (10 kW) • Homes • Farms • Remote Application

Intermediate (10-250 kW) • Village Power • Hybrid Systems • Distributed Power

Large (660 kW - 2+MW) • Central Station Wind Farms • Distributed Power • Community Wind

Size and Applications

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Offshore wind turbines

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What is an Offshore Wind Turbine? A wind turbine shall be considered as an offshore wind turbine

if the support structure is subject to hydrodynamic loading.

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More energy than from the Middle East ! Potential of North Sea

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Wind energy annual installation 2000-2020 (GW)

Source: EWEA/GWEC

Potential

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Bottom Fixed Offshore Wind Turbine

• Includes: – Rotor/nacelle

assembly (RNA) – Support

structure • Tower • Substructure • Foundation

s u b - s t r u c t u r e

p i l e

f o u n d a t i o n

p i l e

p l a t f o r m

t o w e r t o w e r

s u b - s t r u c t u r e

sea floor

s u p p o r t s t r u c t u r e

rotor-nacelle assembly

seabed

water level

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Floating Offshore Wind Turbine

• Includes: – Rotor/nacelle

assembly (RNA) – Support

structure • Tower • Floating

substructure • Mooring

system

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Foundations Design with Changing Depth

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Common Types of Fixed Bottom Support Structures

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Common Types of Fixed Bottom Support Structures

• Monopiles • Tripods • Jackets • Gravity based

http://www.theengineer.co.uk/in-depth/the-big-story/wind-energy-gets-serial/1012449.article

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• Wind turbines and foundation structures • Underwater high voltage cables • Offshore substations and operations

• Onshore substations • Onshore high voltage transmission

Equipment Needed: Onshore to Offshore

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External Conditions

• Wind conditions • Marine

conditions Waves, sea currents, water level, sea ice, marine growth, seabed movement and scour

• Other environmental conditions

• Soil properties at the site

Including time variation due to seabed movement, scour and other elements of seabed instability

“Metocean” Conditions

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Assessment of Metocean External Conditions for Offshore Wind Turbines

• Wind speeds and directions • Significant wave heights, wave periods and directions • Correlation of wind and wave statistics • Current speeds and directions • Water levels • Occurrence and properties of sea ice • Occurrence of icing • Other parameters: air, water temperatures, densities;

water salinity; bathymetry, marine growth, etc

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Offshore Turbines: Energy Integration

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Things to Consider While Designing Offshore Wind Turbines

• Wave models • Hurricanes/cyclones • Wind shear as affected by waves • Floating ice • Boat (service vessel) impact • Soil characterization • Vortex induced vibrations

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Active Area of Research in Offshore Technology Development

• Aerodynamic design-FSI (blades/structure) • Foundation design (soil/structure interaction) • Material properties • Offshore data collection • Environmental impact

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Technology Trend for Wind Turbines

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Transport & Installation

Consequences of Up-Scaling

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Marine Transport

Required Port Facilities

Floating hotel during construction of offshore wind farm

Consequences of Up-Scaling Installation Methods

Heavy Machinery

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Consequences of Up-Scaling

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Consequences of Upscaling

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Assessment of Soil Conditions

• Geological survey of the site

• Bathymetric survey of the sea floor including registration of boulders, sand waves or obstructions on the sea floor

Consequences of Upscaling

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Sounds and Vibrations