wind turbine aerodynamics optimization

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Name Technische Universität München Institute for Flight Propulsion 1 Name of presentation Presented by: Low Chee Meng Supervisor: Marc Kainz Development of a Wind Turbine Optimization Tool Using Open-Source Software

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Page 1: Wind Turbine Aerodynamics Optimization

Name

Technische Universität MünchenInstitute for Flight Propulsion

1

Name of presentationPresented by: Low Chee MengSupervisor: Marc Kainz

Development of a Wind TurbineOptimization Tool Using Open-Source Software

Page 2: Wind Turbine Aerodynamics Optimization

Low Chee Meng

Technische Universität MünchenInstitute for Flight Propulsion

Outline

2

• Project objectives• The wind environment• Aerodynamics of wind turbines• Structure of the optimization program• Validation of the wind turbine performance code• Results from optimization runs

Development of a Wind Turbine Optimization Tool Using Open-Source Software

Page 3: Wind Turbine Aerodynamics Optimization

Technische Universität MünchenInstitute for Flight Propulsion

Low Chee Meng

Project Objectives

3

• Develop and validate a wind turbine blade/rotor aerodynamics performance code

• Develop an optimization algorithm wrapped around the rotor/blade performance code

• Test the accuracy and effectiveness of the code in achieving the optimization objective: Maximize annual power capture at different wind sites

Development of a Wind Turbine Optimization Tool Using Open-Source Software

Page 4: Wind Turbine Aerodynamics Optimization

Technische Universität MünchenInstitute for Flight Propulsion

Low Chee Meng

Windspeed and Energy Density Distribution

*Plotted from shape and scale factors obtained from Christoffer and Ulbricht-Eissing (1989)

Windspeed Distribution

Energy Density Distribution

EnergyDensity (U ∞ )=f (U ∞ )×(12 ρU∞3 )

f (U ∞ )=kc

U ∞

cexp[−( U ∞

c )k

]

Page 5: Wind Turbine Aerodynamics Optimization

Technische Universität MünchenInstitute for Flight Propulsion

Low Chee Meng

Atmospheric Boundary Layer

• Weibull parameters usually for winds measured at height of 10m → correct windspeed pdf for desired turbine hub height

• Azimuthal variation of windspeed for each revolution → use a correction model proposed by Wagner (2010) to find an azimuthal mean windspeed at hub height

Source:Sørensen and Sørensen (2011)

Page 6: Wind Turbine Aerodynamics Optimization

Technische Universität MünchenInstitute for Flight Propulsion

Low Chee Meng

Source:<http://www.mstudioblackboard.tudelft.nl/duwind>

Wind Turbine Performance Map

C p=Aerodynamic Power Extracted

Total Wind Power

λ=Blade Tip Tangential Velocity

Incoming Windspeed

For a fixed RPM turbine, High λ = low windspeeds Low λ = high windspeeds

Cp,max

λCp,max

Coefficient of Power:

Tip Speed Ratio:

X

Page 7: Wind Turbine Aerodynamics Optimization

Technische Universität MünchenInstitute for Flight Propulsion

Low Chee Meng

Source:Staino et al. (2012)

Source:Hansen M. (2008)

Source:http://www.esru.strath.ac.uk

a=U ∞−U d

U ∞

a'=U Ω

2rΩ

Axial Induction Factor: Tangential Induction Factor:

Blade Element Momentum Theory (BEM)

Actuator Disk Theory Blade Element Theory

Page 8: Wind Turbine Aerodynamics Optimization

Technische Universität MünchenInstitute for Flight Propulsion

Low Chee Meng

C p,max,ideal=0 .593

aCp,max=13

Betz LimitC p=

Pextracted

Pwind

=4a (1−a )2 Derived from actuator disk theory

Lossless conversion of axial momentum of flow to power extracted by the actuator disk

Page 9: Wind Turbine Aerodynamics Optimization

Technische Universität MünchenInstitute for Flight Propulsion

Low Chee Meng

Corrections to BEM

Source: Bushong. S. (2012)

Source: Hansen (2008)

2) Turbulent Wake State

3) Tip/hub losses

1) Stall delay

Source: Yu et al. (2011)

Source: Lindenberg (2004)

Page 10: Wind Turbine Aerodynamics Optimization

Technische Universität MünchenInstitute for Flight Propulsion

Low Chee Meng

Rotor Performance Calculations

ChordMetal angle,

βRPM Airfoil

Rotor Design

2D Polars XFOILStall Delay Correction

360° Extrapolation

BEM ProcedureCalculate

Power Curve

Calculate AnnualEnergy Production

WindspeedPDF

P (U cut-in<U <U cut-out)

C p (λ)

Page 11: Wind Turbine Aerodynamics Optimization

Technische Universität MünchenInstitute for Flight Propulsion

Low Chee Meng

BEM Code ValidationReference Code: QBladeTest Cases: NREL Phase 2 and 6 Rotors

Specification Phase 2 Phase 6

RPM 72 72

Radius (m) 5.05 5.029

Airfoils S809 S809

Max. Power (kW) 20 20

Chord/Metal Angles See plots

Page 12: Wind Turbine Aerodynamics Optimization

Technische Universität MünchenInstitute for Flight Propulsion

Low Chee Meng

Validation Results

βtip

=3° βtip

=6°

βtip

=12°βtip

=9°

Page 13: Wind Turbine Aerodynamics Optimization

Technische Universität MünchenInstitute for Flight Propulsion

Low Chee Meng

Genetic Algorithms

• Inspired by biological 'survival-of-the-fittest' processes• Fitter, more highly adapted entities have better chances

of passing on their traits to successive generations• Advantages of GA compared to gradient techniques:

- More robust

- Less likely to be trapped by local minima• Disadvantages

- Requires many more iterations

Source: Beliakov and Lim (2007)

Page 14: Wind Turbine Aerodynamics Optimization

Technische Universität MünchenInstitute for Flight Propulsion

Low Chee Meng

● Individuals – Rotor design● Genes – Design variables● Genome – Collection of genes that fully describe the rotor design● Population/Generation – A batch of rotor designs● Selection – Process by which designs are chosen for gene sharing● Crossover – Sharing of genes● Mutation – Random change to genes

Nomenclature for GA-based Techniques

Gene

Gene 1 Gene 2 Gene 3

Genome

Genome 1

Genome 2

Genome 3

Genome 4

Population

Initial Population/Generation 1 Generation 2 Generation n...

Evolutionary Progress

Page 15: Wind Turbine Aerodynamics Optimization

Technische Universität MünchenInstitute for Flight Propulsion

Low Chee Meng

Airfoil combination

RPM

Chord at Blade root, 25%, 50%, 75%, blade tip

Blade metal angle at25%, 50%, 75%, bladetip

111

72

0.7369

0.5511

0.4529

0.3551

0.2435

24.848

11.151

6.210

4.370

3.000

Genes(Design Variables)

Page 16: Wind Turbine Aerodynamics Optimization

Technische Universität MünchenInstitute for Flight Propulsion

Low Chee Meng

Selection of 2 IndividualsFor gene sharing

Do Crossover /Gene sharing

Do Mutation

Insert new Individuals intonext population

Enough individuals toPopulate next generation?No

Assess fitness of eachIndividual in new generation

Termination criteria met?

Create and AssessInitial population

Yes

End

Yes

No

Page 17: Wind Turbine Aerodynamics Optimization

Technische Universität MünchenInstitute for Flight Propulsion

Low Chee Meng

Program Structure

Fitness EvaluationBEM Module

GA Module

Encoding

Selection

Crossover Mutation

User Input

Airfoil PolarPreparation

Module

Wind Turbine Rotor Optimizer

Page 18: Wind Turbine Aerodynamics Optimization

Technische Universität MünchenInstitute for Flight Propulsion

Low Chee Meng

Optimization Test Environments

Windspeed PDF

Energy Density

2 Test Environments:● High Winds – Helgoland● Low Winds - Singapore

Page 19: Wind Turbine Aerodynamics Optimization

Technische Universität MünchenInstitute for Flight Propulsion

Low Chee Meng

High Winds Environment

Evolution of AEP

Page 20: Wind Turbine Aerodynamics Optimization

Technische Universität MünchenInstitute for Flight Propulsion

Low Chee Meng

Evolution of RPM Blade Root Bending Moment, MB

High Winds Environment

● RPM ↑ to re-align flow angle as windspeeds ↑● Windspeeds ↑ thus M

B,max ↑. Increase

should be as low as possible. Ideally, no increase!

MBmax

Page 21: Wind Turbine Aerodynamics Optimization

Technische Universität MünchenInstitute for Flight Propulsion

Low Chee Meng

Cp↓ V

cutout

High Winds Environment

● Evolved blade with highest AEP has lower Cp than baseline blade across all tip speed ratios● Power output is lower for all windspeeds but operational windspeed range has widened.

Page 22: Wind Turbine Aerodynamics Optimization

Technische Universität MünchenInstitute for Flight Propulsion

Low Chee Meng

High Winds Environment

Vcutout

AccessibleEnergy ↑

Page 23: Wind Turbine Aerodynamics Optimization

Technische Universität MünchenInstitute for Flight Propulsion

Low Chee Meng

High Winds Environment

Pareto Trade-off – AEP and Blade Root Bending Moment

● Pareto-frontier delineates the max-AEP↑-for-min-M

Bmax-

penalty line along the AEP-M

Bmax curve

● ParetoBest rotor has 4% lower AEP compared to AEPmax rotor but also lower M

Bmax by 7.6%

Page 24: Wind Turbine Aerodynamics Optimization

Technische Universität MünchenInstitute for Flight Propulsion

Low Chee Meng

MBmax

Vcutout

Page 25: Wind Turbine Aerodynamics Optimization

Technische Universität MünchenInstitute for Flight Propulsion

Low Chee Meng

αstall

αstall

Page 26: Wind Turbine Aerodynamics Optimization

Technische Universität MünchenInstitute for Flight Propulsion

Low Chee Meng

● Compared to AEPmax blade, ParetoBest blade has more evenly distributed power contribution from its radial blade segments● Root region power contribution of ParetoBest blade increases as windspeed ↑

Contribution of root region to power increases significantly as windspeed ↑

Page 27: Wind Turbine Aerodynamics Optimization

Technische Universität MünchenInstitute for Flight Propulsion

Low Chee Meng

● Compared to AEPmax blade, ParetoBest blade has smaller outboard chord and enlarged inboard chord, this reduces the blade root bending moment

ParetoBest AEPmax

Page 28: Wind Turbine Aerodynamics Optimization

Technische Universität MünchenInstitute for Flight Propulsion

Low Chee Meng

ParetoBest

AEPmax

Baseline

Page 29: Wind Turbine Aerodynamics Optimization

Technische Universität MünchenInstitute for Flight Propulsion

Low Chee Meng

Low Winds Environment

● AEPmax design underwent just 1 re-design● RPM decreases → Cp curve shifts to the left● Cp curve shifts up to increase power capture over all tip speed ratios and windspeeds

Page 30: Wind Turbine Aerodynamics Optimization

Technische Universität MünchenInstitute for Flight Propulsion

Low Chee Meng

Increase in Cp due to combination of: ● Increase in chord lengths for most of the bladespan● Reduction in RPM and blade metal angle near the tip, both increase angle of attack

C(r) ↑

β↓

Page 31: Wind Turbine Aerodynamics Optimization

Technische Universität MünchenInstitute for Flight Propulsion

Low Chee Meng

Low Winds Environment

● AEPmax rotor higher power capture for entire windspeed range except very close to V

cutout

● Increase in energy capture comes from increase in angle of attack (mostly pre-stall) and blade forces● M

Bmax increases correspondingly and by a large margin of 20%

Page 32: Wind Turbine Aerodynamics Optimization

Technische Universität MünchenInstitute for Flight Propulsion

Low Chee Meng

Low Winds Environment

Vcutout

Page 33: Wind Turbine Aerodynamics Optimization

Technische Universität MünchenInstitute for Flight Propulsion

Low Chee Meng

αstall

αstall

Page 34: Wind Turbine Aerodynamics Optimization

Technische Universität MünchenInstitute for Flight Propulsion

Low Chee Meng

MBmax

remains largely unchanged

● ParetoBest blade has lower MBmax

compared to AEPmax blade mainly

due to enlargement of root region chord and reduction of tip chord

Page 35: Wind Turbine Aerodynamics Optimization

Technische Universität MünchenInstitute for Flight Propulsion

Low Chee Meng

ParetoBest

AEPmax

Baseline

Page 36: Wind Turbine Aerodynamics Optimization

Technische Universität MünchenInstitute for Flight Propulsion

Low Chee Meng

Summary of Findings

● Adaptation toward high RPM for high winds, low RPM for low winds

Strategy for high winds● Expand operational windspeed range as much as possible to tap energy available of high winds● Power limitation is a problem. For fixed RPM, non-pitchable blades, solutions may include the following:

- have high β at the root, low (negative) β at the tip- force tip to stall at high winds- enlarge root chord, reduce tip chord- power contribution shifts from tip to root as windspeed↑

Page 37: Wind Turbine Aerodynamics Optimization

Technische Universität MünchenInstitute for Flight Propulsion

Low Chee Meng

Summary of FindingsSummary of Findings

Strategy for low winds● Maximize energy capture for low winds at the sacrifice of efficiency at high winds (where wind energy density is low)● The following may be the solution:

- reduce RPM- increase metal angle β to increase angle of attack and blade forces- enlarge chord to increase axial induction factor and blade forces- enlarge chord more near root region to reduce blade root bending moment increase

Page 38: Wind Turbine Aerodynamics Optimization

Technische Universität MünchenInstitute for Flight Propulsion

Low Chee Meng

Conclusion

● An optimization program for wind turbine rotor aerodynamics has been successfully implemented● The GA is able to improve on baseline design and is robust and reliable● Identified possible good 'genes' for rotors at low and high windspeeds

Outlook

● Run the program with variable airfoil combinations● Tune the GA algorithm for a more thorough search of possible designs but more iterations needed● Improve the accuracy and speed of the BEM code● Include structural and noise factors as those are important considerations as well

Page 39: Wind Turbine Aerodynamics Optimization

Technische Universität MünchenInstitute for Flight Propulsion

Low Chee Meng

Danke schön!

Grazie