K. Schröder, S. Grove, S. Tsiapoki, C.G. Gebhardt and R ... · Gebhardt and R. Rolfes. EERA...

17
Structural Change Identification at a Wind Turbine Blade using Model Updating K. Schröder, S. Grove, S. Tsiapoki, C.G. Gebhardt and R. Rolfes EERA DeepWind’18, 18.01.18

Transcript of K. Schröder, S. Grove, S. Tsiapoki, C.G. Gebhardt and R ... · Gebhardt and R. Rolfes. EERA...

Page 1: K. Schröder, S. Grove, S. Tsiapoki, C.G. Gebhardt and R ... · Gebhardt and R. Rolfes. EERA DeepWind’18, 18.01.18. DeepWind’18 18.01.18 2. Content. I. Motivation II. Optimization

Structural Change Identification at a Wind Turbine Blade using Model Updating

K. Schröder, S. Grove, S. Tsiapoki, C.G. Gebhardt and R. Rolfes

EERA DeepWind’18, 18.01.18

Page 2: K. Schröder, S. Grove, S. Tsiapoki, C.G. Gebhardt and R ... · Gebhardt and R. Rolfes. EERA DeepWind’18, 18.01.18. DeepWind’18 18.01.18 2. Content. I. Motivation II. Optimization

DeepWind’18 18.01.18 2

Content

I. Motivation

II. Optimization based model updating

III. Rotor blade test

IV. Model updating at the rotor blade1. Damage localization2. Ice accretion

V. Conclusion and Outlook

Page 3: K. Schröder, S. Grove, S. Tsiapoki, C.G. Gebhardt and R ... · Gebhardt and R. Rolfes. EERA DeepWind’18, 18.01.18. DeepWind’18 18.01.18 2. Content. I. Motivation II. Optimization

DeepWind’18 18.01.18 3

Motivation

• Remote location

• Rotor blades: costly and time-consuming repair

• Ice accretion: - Risk of ice throw

- Undesired loads

Localization and quantification of structuralchanges using model updating

Page 4: K. Schröder, S. Grove, S. Tsiapoki, C.G. Gebhardt and R ... · Gebhardt and R. Rolfes. EERA DeepWind’18, 18.01.18. DeepWind’18 18.01.18 2. Content. I. Motivation II. Optimization

DeepWind’18 18.01.18 4

Finite Element Model Updating

Damage event

Page 5: K. Schröder, S. Grove, S. Tsiapoki, C.G. Gebhardt and R ... · Gebhardt and R. Rolfes. EERA DeepWind’18, 18.01.18. DeepWind’18 18.01.18 2. Content. I. Motivation II. Optimization

DeepWind’18 18.01.18 5

Deviation between numerical model andmeasured data

Modal parameters

Transmissibility functions

• Eigenvalues• Mode shapes

Quantification of the „difference“ between model and measurement

Page 6: K. Schröder, S. Grove, S. Tsiapoki, C.G. Gebhardt and R ... · Gebhardt and R. Rolfes. EERA DeepWind’18, 18.01.18. DeepWind’18 18.01.18 2. Content. I. Motivation II. Optimization

DeepWind’18 18.01.18 6

Minimization of the deviation

• Nonlinear• Constrained• Nonconvex• Several local minima

Global optimization algorithm:Simulated Quenching

Local optimization algorithm:Sequential Quadratic Programming

Page 7: K. Schröder, S. Grove, S. Tsiapoki, C.G. Gebhardt and R ... · Gebhardt and R. Rolfes. EERA DeepWind’18, 18.01.18. DeepWind’18 18.01.18 2. Content. I. Motivation II. Optimization

DeepWind’18 18.01.18 7

Rotor blade test

• Hammer excitation

• 12 measurement channels

Page 8: K. Schröder, S. Grove, S. Tsiapoki, C.G. Gebhardt and R ... · Gebhardt and R. Rolfes. EERA DeepWind’18, 18.01.18. DeepWind’18 18.01.18 2. Content. I. Motivation II. Optimization

DeepWind’18 18.01.18 8

• Hammer excitation

• 12 measurement channels

• Ice mass

• Damage

Trailing edge bondline: Spot of damage initiation

Trailing edge – PressureSide (outside)

Rotor blade test

Page 9: K. Schröder, S. Grove, S. Tsiapoki, C.G. Gebhardt and R ... · Gebhardt and R. Rolfes. EERA DeepWind’18, 18.01.18. DeepWind’18 18.01.18 2. Content. I. Motivation II. Optimization

DeepWind’18 18.01.18 9

Numerical Modeling

•Rectangular Cross Section

•Known: EI and mass

•26 Timoshenko beam elements

•Clamping at blade root

•Material damping

Page 10: K. Schröder, S. Grove, S. Tsiapoki, C.G. Gebhardt and R ... · Gebhardt and R. Rolfes. EERA DeepWind’18, 18.01.18. DeepWind’18 18.01.18 2. Content. I. Motivation II. Optimization

DeepWind’18 18.01.18 10

Numerical validation

Stiffness reduction

Page 11: K. Schröder, S. Grove, S. Tsiapoki, C.G. Gebhardt and R ... · Gebhardt and R. Rolfes. EERA DeepWind’18, 18.01.18. DeepWind’18 18.01.18 2. Content. I. Motivation II. Optimization

DeepWind’18 18.01.18 11

Numerical validation–Modal Parameters

Parameter number

Parameter number

Page 12: K. Schröder, S. Grove, S. Tsiapoki, C.G. Gebhardt and R ... · Gebhardt and R. Rolfes. EERA DeepWind’18, 18.01.18. DeepWind’18 18.01.18 2. Content. I. Motivation II. Optimization

DeepWind’18 18.01.18 12

Numerical validation –Transmissibility Functions

Parameter number

Parameter number

Page 13: K. Schröder, S. Grove, S. Tsiapoki, C.G. Gebhardt and R ... · Gebhardt and R. Rolfes. EERA DeepWind’18, 18.01.18. DeepWind’18 18.01.18 2. Content. I. Motivation II. Optimization

DeepWind’18 18.01.18 13

Ice accretion

• 4 steps

• Variation of density

• Optimization problem:

• Step 3: 14,4kg at 32m-33m and 33m-34m

Page 14: K. Schröder, S. Grove, S. Tsiapoki, C.G. Gebhardt and R ... · Gebhardt and R. Rolfes. EERA DeepWind’18, 18.01.18. DeepWind’18 18.01.18 2. Content. I. Motivation II. Optimization

DeepWind’18 18.01.18 14

Ice localization – Modal Parameters

• Correct Localizations in runs 1, 3, 7, 9 und 11

• Verification using objective function value

• Ice localization using modal parameters is possible

Parameter number

Page 15: K. Schröder, S. Grove, S. Tsiapoki, C.G. Gebhardt and R ... · Gebhardt and R. Rolfes. EERA DeepWind’18, 18.01.18. DeepWind’18 18.01.18 2. Content. I. Motivation II. Optimization

DeepWind’18 18.01.18 15

Ice quantification – Modal ParametersSt

iffne

ssPa

ram

eter

4 in

%

Ice set (rotor blade mass in %)0.1 0.3 0.6 0.9

Page 16: K. Schröder, S. Grove, S. Tsiapoki, C.G. Gebhardt and R ... · Gebhardt and R. Rolfes. EERA DeepWind’18, 18.01.18. DeepWind’18 18.01.18 2. Content. I. Motivation II. Optimization

DeepWind’18 18.01.18 16

Conclusion & Outlook

• Updating in numerical examplesand for ice quantification successful

• Minimization using global two-step optimization algorithm• No success for damage localization using measured data• Modal parameters superior to transmissibility functions

• Investigate more advanced metrics for model updating• Application to changing conditions (in situ)

Conclusion

Outlook

Page 17: K. Schröder, S. Grove, S. Tsiapoki, C.G. Gebhardt and R ... · Gebhardt and R. Rolfes. EERA DeepWind’18, 18.01.18. DeepWind’18 18.01.18 2. Content. I. Motivation II. Optimization

DeepWind’18 18.01.18 17

Thank you for your attention!

Leibniz Universität HannoverInstitute of Structural Analysis (ISD)Appelstraße 9a, 30167 Hannover

+49 511 762 [email protected]