Demonstration with optical fibres by Smart Fibres Ltd. Task 15

Similar documents
Performance Testing of Composite Bearing Materials for Large Hydraulic Cylinders

EMS ELONGATION MEASUREMENT SYSTEM. Strain measurement system for wind turbines optimizing the control & condition monitoring

Experimental Verification of the Implementation of Bend-Twist Coupling in a Wind Turbine Blade

The strain sensor is available with integrated electronic evaluator.

Assemblies for Parallel Kinematics. Frank Dürschmied. INA reprint from Werkstatt und Betrieb Vol. No. 5, May 1999 Carl Hanser Verlag, München

Carbon Fiber Parts Performance In Crash SITUATIONS - CAN WE PREDICT IT?

RTM COMPOSITE LUGS FOR HIGH LOAD TRANSFER APPLICATIONS

EE5940: Wind Essen.als. Materials and Structural Reliability Sue Mantell Mechanical Engineering

ONLINE NON-CONTACT TORSION SENSING METHOD USING FIBER BRAGG GRATING SENSORS AND OPTICAL COUPLING METHOD. Yoha Hwang and Jong Min Lee

Technical Documentation

MANTECH ELECTRONICS. Stepper Motors. Basics on Stepper Motors I. STEPPER MOTOR SYSTEMS OVERVIEW 2. STEPPING MOTORS

Understanding the benefits of using a digital valve controller. Mark Buzzell Business Manager, Metso Flow Control

Load Cell for Manually Operated Presses Model 8451

Application of DSS to Evaluate Performance of Work Equipment of Wheel Loader with Parallel Linkage

Estimation of Turbine Reliability figures within the DOWEC project

Hybrid Architectures for Automated Transmission Systems

METEOROLOGICAL INSTRUMENTS

SJSU ENGR 10 Wind Turbine Power Measurement Procedure

VARIABLE DISPLACEMENT OIL PUMP IMPROVES TRACKED VEHICLE TRANSMISSION EFFICIENCY

MODEL 27106DT GILL PROPELLER ANEMOMETER JANUARY 2003 MANUAL PN 27106DT-90 R. M. YOUNG COMPANY

Tension and Compression Load Cell Model 8435

LEVER OPTIMIZATION FOR TORQUE STANDARD MACHINES

Rotary Inclinometer. User Manual: (Draft Version)

Bosko Rasuo University of Belgrade, Faculty of Mechanical Engineering, Aeronautical Department, Belgrade 35, Serbia

Field test for the comparison of LNG static and dynamic mass measurement methods

Overload tests of Eilersen web tension sensor type SLCA 500 N

Inverter control of low speed Linear Induction Motors

DIY balancing. Tony Foale 2008

inter.noise 2000 The 29th International Congress and Exhibition on Noise Control Engineering August 2000, Nice, FRANCE

ABSTRACT INTRODUCTION

Skid against Curb simulation using Abaqus/Explicit

Designing Drive Systems for Low Web Speeds

PERFORMANCE AND ACCEPTANCE OF ELECTRIC AND HYBRID VEHICLES

Racing Tires in Formula SAE Suspension Development

Gun Port Patterns (Part 1 of 2)

Application of Airborne Electro-Optical Platform with Shock Absorbers. Hui YAN, Dong-sheng YANG, Tao YUAN, Xiang BI, and Hong-yuan JIANG*

Troubleshooting. Wind Gearbox Problems

Spin Rig for NSMS Probe Development and Strain Gage Correlation

Engine Power and Fueling Comparison Between Vessels with Conventional Transmissions and Controllable Speed Propeller Transmissions During Dynamic

High Speed Gears - New Developments

USER MANUAL FOR AREX DIGI+ SYSTEMS

MONTANA TEEN DRIVER CURRICULUM GUIDE Lesson Plan & Teacher Commentary. Module 2.2 Basic Control and Vehicle Location

Test bed for hydrostatic bearing gap

Technical Article. How improved magnetic sensing technology can increase torque in BLDC motors. Roland Einspieler

Chapter 4. Vehicle Testing

Hybrid Materials and Construction Principles for Aero Engine Components. Materials 2006

Quantification of Lateral Forces in Concrete Crosstie Fastening Systems

DETERMINATION OF MINIMUM PULLEY DIAMETERS FOR BELT CONVEYORS

Armature Reaction and Saturation Effect

Throwback Thursday :: Bently Nevada Dual Probe Versus Shaft Rider

Based on the findings, a preventive maintenance strategy can be prepared for the equipment in order to increase reliability and reduce costs.

inter.noise 2000 The 29th International Congress and Exhibition on Noise Control Engineering August 2000, Nice, FRANCE

Modelling and Assembly of Single Plate Clutch

The X-Rotor Offshore Wind Turbine Concept

Measurement of induction motor characteristics

Dynamic characteristics of railway concrete sleepers using impact excitation techniques and model analysis

Wind Tunnel Measurement Of Aerodynamic Characteristics Of A Generic Eurocopter Helicopter

Implementation and Thickness Optimization of Perpetual Pavements in Ohio

COATING YOUR WAY TO LOWER EMISSIONS

The validation of MBS multi-megawatt gearbox models on a 13.2 MW test rig

Monitoring of a full-scale wing fatigue test - RNLAF F-16 aircraft, 4200 FH -

Helicopter Noise and Vibration (EU Project "HELINOVI")

Improved roll pass design for long products with WICON

"Tension Control in a Turret Winder" Clarence Klassen, P.Eng. Abstract:

Force Based Condition Monitoring of Railway Infrastructure

Measuring equipment for the development of efficient drive trains using sensor telemetry in the 200 C range

Microcellular polyurethane as steering coupling element

Impact, Torsion, and Crush Tests for 477 kcmil and 795 kcmil 3M Brand Composite Conductor. 3M Company Purchase Order

MOTORS. Part 2: The Stepping Motor July 8, 2015 ELEC This lab must be handed in at the end of the lab period

STEALTH INTERNATIONAL INC. DESIGN REPORT #1001 IBC ENERGY DISSIPATING VALVE FLOW TESTING OF 12 VALVE

Bistable Rotary Solenoid

On Control Strategies for Wind Turbine Systems

Study on Flow Fields in Variable Area Nozzles for Radial Turbines

Modeling, Structural & CFD Analysis and Optimization of UAV

Heat Engines Lab 12 SAFETY

Special edition paper

SPMM OUTLINE SPECIFICATION - SP20016 issue 2 WHAT IS THE SPMM 5000?

Aeroelastic Modelling of the LMH64-5 Blade. C. Lindenburg

Asynchronous Generators with Dynamic Slip Control

STRUCTURAL BEHAVIOUR OF 5000 kn DAMPER

Wind Energy Science Conference WESC 2017

MODEL 27106T GILL PROPELLER ANEMOMETER

METEOROLOGICAL INSTRUMENTS

Ball Rail Systems RE / The Drive & Control Company

Adelaide Wind Power Project Turbine T05 (AD117) IEC Edition 3.0 Measurement Report

Reliable and Application specific. Slewing Drives for Wind Turbines

Power Voltage Transformers for Air Insulated Substations

COMPARISON OF ENERGY EFFICIENCY DETERMINATION METHODS FOR THE INDUCTION MOTORS

BY: Paul Behnke ITT Industries, Industrial Process. Juan Gamarra Mechanical Solutions, Inc.

Hydraulic energy control, conductive part

Figure 1 Linear Output Hall Effect Transducer (LOHET TM )

Thank you for purchasing a kit from SparKIT. Your support is greatly appreciated.

A STUDY OF HUMAN KINEMATIC RESPONSE TO LOW SPEED REAR END IMPACTS INVOLVING VEHICLES OF LARGELY DIFFERING MASSES

Higher performance. through longer life of gear units

Bearings and steel balls

CONVEYOR SYSTEM COMMISSIONING, MAINTENANCE AND FAILURE ANALYSIS USING BLACK BOX TECHNIQUES. By A. J. Surtees Conveyor Watch (Pty) Ltd

TCS Axis Motor Tachometer. Replacement

Please pay attention to all Cautions and Notes within these instructions.

Stopping Accuracy of Brushless

Oregon DOT Slow-Speed Weigh-in-Motion (SWIM) Project: Analysis of Initial Weight Data

Transcription:

Demonstration with optical fibres by Smart Fibres Ltd. Task 15 Dutch Offshore Wind Energy Converter project DOWEC 10021 rev1 Name: Signature: Date: Written by: J.F. Kooij (LMGH) 30-09-03 version Date No of pages 1 30-09-03 18 New document in PDF DOWEC 10021 rev1 Page: 1 of 18 30-09-2003

Summary: One of the techniques to do load registration is the use of optical fibres in a blade. Smart Fibres Ltd. in England has developed an optical fibre strain sensing system that can measure strain in a composite structure. To give a feeling about the capabilities of this system a demonstration has been held on an existing structure. This structure was the sectional blade as tested at TU Delft. This document gives an outline of this demonstration. The demonstration gave promising results: The differences between strain gauges and optical fibre sensors are severe for lower load levels; The differences for higher load levels give a constant difference (5 %); The results for a single and a multiplexed optical sensor are comparable; In the dynamic testing the results in the low strain region differ more than 10 %. For the high strain region the differences are comparable to the differences seen at the static test (3-5 %). Contents 1 Introduction... 3 2 Mounting of optical fibres...4 2.1 Test blade... 4 2.2 Alignment of fibres... 4 2.3 Lamination specification for demonstration... 4 3 Mounting strain gauges...6 4 Testing... 8 4.1 Static testing... 8 4.1.1 Comparison between strain gauges and optical fibre sensor... 8 4.1.2 Comparison between single and multiplexed fibre... 10 4.2 Dynamic testing... 11 5 Conclusions & recommendations... 12 5.1 Conclusions... 12 5.2 Recommendations... 12 Appendix A: Strain gauges vs. Optical fibres (pos. strains)... 14 DOWEC 10021 rev1 Page: 2 of 18 30-09-2003

1 Introduction In the DOWEC project a task described in the knowledge development is the load registration and condition monitoring for an offshore rotor. One of the techniques to do load registration is the use of optical fibres in a blade. Smart Fibres Ltd. in England has made a commercial system to implement this. They have developed an optical fibre strain sensing system that can measure strain in a composite structure. To get a feeling about the capabilities of this system a demonstration has been held on an existing structure. This structure was the sectional blade as tested at TU Delft. This document gives an outline of this demonstration. The demonstration contained the following: Mounting of optical fibres on an existing structure (handling, etc); Comparison of single grating in fibre and a few gratings in series (multiplexed); Comparison between optical fibres and strain gauges (conventional method). Test performed in co-ordination with TU Delft and ECN. In chapter 2 an outline of the mounting of the optical fibres (SF) is given and in chapter 3 the mounting of the electric strain gauges (ESG). The comparison between strain gauges and between the single and multiplexed fibres is given in chapter 4. Finally the conclusions are drawn in chapter 5. DOWEC 10021 rev1 Page: 3 of 18 30-09-2003

2 Mounting of optical fibres 2.1 Test blade The structure on which the demonstration was performed was the 23m sectional blade developed in a European project (JOR3970167, Design, structural testing and cost effectiveness of sectional wind turbine blades ). The blade is divided into two parts and they are mounted together with an Ikea (T-bolt) connection. This blade was already mounted in a test rig at TU Delft and the testing was finished when the demonstration was held. 2.2 Alignment of fibres To do a good comparison, two locations were selected at which measurements were performed. These locations are a location where low strain levels occur and one where high strain levels occur. The low strains occurred near the trailing and leading edge of a cross section if loaded in flapwise direction. As the trailing edge was easier to use for mounting this side was used to mount the optical fibres. High strain levels occurred at a cross section located at L = 5300 mm. A layout of the locations where the optical fibres sensors were mounted is shown in Figure 2.1. Figure 2.1: Locations for mounting optical fibres At each location two gratings were mounted, one in line with another grating in the same fibre and one single grating in a fibre. This is useful to compare the measurements between a single grating and one in line with another grating. The optical fibres, and of course the gratings, are located on the outside of the blade. The gratings are mounted parallel to the neutral axis of the blade. This all lead to 3 optical fibres with in total 4 gratings (2 gratings in line, and two in a single fibre). 2.3 Lamination specification for demonstration The laminating specifications for the post embedment of fibre optical strain sensors are used as recommended by Smart Fibres. Unidirectional 450g/m 2 E-glass tape is used to laminate optical fibres onto the blade surface using the following lay-up (see Figure 2.2). The method of applying resin is hand lay-up. DOWEC 10021 rev1 Page: 4 of 18 30-09-2003

Figure 2.2: Lay-up for mounting optical fibres The 1 st layer was 100 mm wide UD-tape, then the optical fibres are embedded into place, followed by a second layer of 60 mm wide UD-tape. E-glass tape (0-90º) is placed on top of these two layers to have a better protection if the strain gauges are mounted and finally a layer of peel ply is placed to suck out the redundant resin. The distance between the sensors was 10mm. Polyester resin has been used and a slow hardener to give plenty of working time before setting of the laminate by heating it up. Special care had to be taken of the location where the optical fibre runs out of the laminate. During lamination resin with added silica had to be added to the surroundings of this vulnerable area. To make sure the protected part of the fibre (blue in figures) did not stick to the resin it was rubbed with a release wax. The peel ply had to be between the laminate and the optical cable (see Figure 2.3). Figure 2.3: Ending of optical fibre in laminate A complete patch with optical fibres mounted in a laminate is shown in Figure 2.4. DOWEC 10021 rev1 Page: 5 of 18 30-09-2003

Figure 2.4: Complete patch 3 Mounting strain gauges When the resin of the laminate was fully hardened, strain gauges were mounted on the locations where the gratings are present. Four strain gauges were enough to give a good comparison (one strain gauge on top of each grating). Now it became clear that the last layer of glass (0-90º tape) was necessary as the surface had to be sanded to give a good adhesion between the strain gauges and the laminate. A detail is given in Figure 3.1. A systematic sketch of layout is shown in Figure 3.2 and the complete layout is shown in Figure 3.3. In the sketch the two different measurement systems are separated to give a better overview, but in reality they are located on top of each other. DOWEC 10021 rev1 Page: 6 of 18 30-09-2003

Figure 3.1: Strain gauges on surface Figure 3.2: Layout of test set-up DOWEC 10021 rev1 Page: 7 of 18 30-09-2003

Figure 3.3: Complete test set-up on the blade 4 Testing Two types of tests were performed: static and dynamic. The static test was done with a few different steps to have a good comparison for different loading levels (and thus strain levels). The dynamic test took place for 5 minutes as the data storage of the optical fibre strain sensing system only had a limited capability. These few minutes were also sufficient to give enough data to do a comparison. 4.1 Static testing The static testing was done on six load levels: four levels with positive strain (F = -15 kn, -30 kn, -45 kn & -60 kn) and 2 levels with negative strain (F = +30 kn & +60 kn). In this line-up a positive sign of the force results in negative strains (compression on measured side of blade) and a negative force thus results in positive strains (tension on measured side of blade). The force applied in six different steps and after each load level the force was reduced to zero. The time range was 20 seconds building-up of force, 20 (or 30) seconds of continuous force and 20 seconds building-down of force. 4.1.1 Comparison between strain gauges and optical fibre sensor The results of the strain gauges are listed in table 4.1 and the results of the optical fibre sensors in table 4.2 and the graphs in appendix A and B. Force 57.472 kn 29.167 kn -14.368 kn -28.736 kn -43.104 kn -57.095 kn DOWEC 10021 rev1 Page: 8 of 18 30-09-2003

Nr 1. c *-313.238-165.832 82.916 *165.832 **239.534 322.450 Nr 2. -331.663 **-175.044 82.916 165.832 248.747 331.633 Nr 3. -1142.395-580.410 294.812 *580.410 866.009 1142.395 Nr 4. -1151.608 **-589.623 *294.812 580.410 **866.009 1151.610 Table 4.1: Results of strain gauges c: corrected with an offset of 9.213 µε *: fluctuations between 0 and -9.213 µε **: fluctuations between 0 and +9.213 µε On the two locations (high and low strain) the results of the strain gauges are comparable (difference is not more than 10 µε). This is not surprising as the distance is only 10 mm apart. In the static test the measurements do not fluctuate heavily. Only the most occurring value is listed in the table. If a fluctuation is present this result is marked with a *. Strain gauge number 1 gave a strain of 9.213 µε if the blade was unloaded. Therefore all the results of this strain gauge were corrected with this value. Force 57.472 kn 29.167 kn -14.368 kn -28.736 kn -43.104 kn -57.095 kn Nr 1. -332.543-168.353 82.106 170.854 251.365 333.403 Nr 2. -354.100-177.668 89.825 175.119 261.237 355.287 Nr 3. -1210.006-609.912 269.409 585.324 893.640 1172.072 Nr 4. -1224.456-627.112 302.659 606.353 905.683 1203.115 Table 4.2: Results of optical fibre sensors *: the standard deviation was approx. ± 10 µε, with maximums reaching ± 20 µε. The results of the optical fibre sensors give similar behaviour as the strain gauges; only the values are slightly higher. The listed values are the average values during the static test. The standard deviation differed between ±2 and ±20 µε with an average of ±10 µε. The differences between the optical fibre sensors and the strain gauges are listed in table 4.3. Force 57.472 kn 29.167 kn -14.368 kn -28.736 kn -43.104 kn -57.095 kn Nr 1. 6 % (19µε) 2 %(3µε) -1 %(1µε) 3 %(5µε) 5 %(12µε) 3 %(11µε) Nr 2. 7 %(22µε) 1 %(3µε) 8 %(7µε) 6 %(9µε) 5 %(13µε) 7 %(24µε) Nr 3. 6 %(68µε) 5 %(30µε) -9 %(25µε) 1 %(5µε) 3 %(28µε) 3 %(30µε) Nr 4. 6 %(73µε) 6 %(37µε) 3 %(8µε) 4 %(26µε) 5 %(40µε) 4 %(52µε) Table 4.3: Differences between optical fibre sensors and strain gauges (percentage and absolute) For the lower load levels (F = 29.167 kn, -14.368 kn & -28.736 kn) the percentage differences between strain gauges and optical fibre sensors are severe, especially for F = -14.368 kn, but the absolute values are low (except for nr 3.). The results for higher load levels give a more constant difference (5 %). Three reasons can be found for this difference: 1. The strain transfer between the optical fibres is different than for strain gauges. The optical fibres are more or less embedded into the structure and the strain gauges are mounted on top by an adhesive. These different types of mounting are likely to give different results. 2. Due to the embedment of the optical fibres they can also sense a portion of e.g. transverse strains. This is likely to occur in highly curved structures. Strain gauges only measure in one direction and in this case in the direction of the neutral axis. 3. The optical fibres are calibrated by a factor of 2.66 on the raw data. This is used by Smart Fibres as calibration for the raw data in their experience. For this structure or embedment the factor can be adjusted to fine-tune the results. DOWEC 10021 rev1 Page: 9 of 18 30-09-2003

4.1.2 Comparison between single and multiplexed fibre As mentioned earlier at one location two types of optical fibre sensors are present: a fibre with a single sensor and a fibre with multiplexed sensors. In this section the results of the two sensors are compared. In table 4.4 the mean, maximum and minimum values of the difference between the optical fibre sensors are shown as well as the difference between the strain gauges at one location. In appendix C the results are shown graphically. Force 57.4 kn 29.1 kn -14.3 kn -28.7 kn -43.1 kn -57.0 kn Average Difference between nr 1 and 2 Mean 6 % 6 % 9 % 2 % 4 % 7 % 6 % Min 9 % 10 % 10 % 3 % 3 % 6 % 7 % Max 3 % 5 % 5 % -3 % 5 % 7 % 4 % ESG 6 % 6 % 0 % 0 % 4 % 3 % 3 % Difference between nr 3 and 4 Mean 1 % 3 % 12 % 4 % 1 % 3 % 4 % Min 1 % 3 % 10 % 4 % 1 % 2 % 4 % Max 1 % 2 % 14 % 2 % 2 % 3 % 4 % ESG 1 % 2 % 0 % 0 % 1 % 0 % 1 % Table 4.4: Comparison between single and multiplexed fibre The table shows clearly that the results of the optical fibre sensors in the low strain area (nr 1. and 2.) differ more than at the high strain area (nr 3. and 4.). As the locations of the sensors differ 10 mm the results are likely to be different, especially in the tail area. This can also be concluded out of the results of the strain gauges. The difference between the two optical fibre sensors is approximately 3 % higher than the difference of the strain gauges at the same location. For the lower loading levels (especially in the low strain area) the differences are the greatest (10-12 %). The specifications of the Smart Fibres system list a resolution of ±10µε so it will not be surprisingly that for a low strain level the same absolute magnitude of fluctuation gives higher deviations in percentage than for higher strain levels. Therefore it is also necessary to look at the absolute differences (see table 4.5). This shows that at the low strain location the absolute difference is less than at the high stress location. Force 57.4 kn 29.1 kn -14.3 kn -28.7 kn -43.1 kn -57.0 kn Average Difference between nr 1 and 2 SF 22 µε 9 µε 8 µε 4 µε 11 µε 22 µε 13 µε ESG 18 µε 9 µε 0 µε 0 µε 9 µε 14 µε 8 µε Difference between nr 3 and 4 SF 14 µε 17 µε 33 µε 21 µε 12 µε 31 µε 22 µε ESG 9 µε 9 µε 0 µε 0 µε 0 µε 9 µε 5 µε Table 4.5: Comparison between single and multiplexed fibre DOWEC 10021 rev1 Page: 10 of 18 30-09-2003

4.2 Dynamic testing In the dynamic testing two load amplitudes were used: -5 to -30 kn and -5 to -60 kn. The results of the optical fibre sensors were stored in the "black-box" of the optical fibre strain sensing system. Due to the internal capacity of this system the disk was full after 7 minutes (86 Hz of measurement frequency). Therefore the dynamic tests only ran for 5 minutes to avoid overwriting of old data. In the second dynamic test the initial load was already -5 kn and therefore the strain gauge already gave results. Due to the downloading of old results obtained by the optical fibre strain sensing system, the optical fibre sensors gave zero strain at the start of this dynamic test. Therefore the results have to be corrected to obtain results that can be compared. Comparing the data for the dynamic testing was very comprehensive as the measuring frequencies differed (88 Hz vs. 20 Hz). To do a good comparison not the absolute maximums have to be compared as this, but the average values of all the measured maximums. The maximum values may be true for only one cycle. As there was a large amount of results only the first few cycles were compared, which may conclude in larger deviations than expected. These results are listed in table 4.6. F = -30 kn F = -60 kn Optical Strain Diff. Optical Strain Diff. fibres gauges fibres gauges Nr 1. 187.33 165.83 13 % 347.31 331.66 5 % Nr 2. 189.63 170.44 11 % 365.27 322.45 12 % Nr 3. 602.81 587.78 3 % 1170.88 1133.18 3 % Nr 4. 620.45 589.62 5 % 1198.38 1142.40 5 % Table 4.6: Average maximum values of first few cycles in dynamic testing The results show clearly that in the low stress region (nr 1. and 2.) the results differ mostly more than 10 %. For the high stress region (nr 3. and 4.) the differences are comparable to the differences seen at the static test (3-5 %). Some reasons for the large difference are the following: The influence of the geometry has a larger impact at the low region (tail) than at the high stress region (main spar). Due to the different embedment of the optical fibres they can also sense a portion of e.g. transverse strains. This is likely to occur in highly curved structures (tail). DOWEC 10021 rev1 Page: 11 of 18 30-09-2003

5 Conclusions & recommendations 5.1 Conclusions On the two locations (high and low strain) the results of the strain gauges are comparable (difference is not more than 10 µε). The results of the optical fibre sensors give a similar behaviour as the strain gauges; only the values are slightly higher. The standard deviation differed between ±2 and ±20 µε with an average of ±10 µε. For lower load levels the differences between strain gauges and optical fibre sensors are severe, especially for the lowest load level. The results for higher load levels give a more constant difference (5 %). Three reasons can be found for this difference: The strain transfer between the optical fibres is different than for strain gauges. The optical fibres are more or less embedded into the structure and the strain gauges are mounted on top by an adhesive. These different types of mounting are likely to give different results. Due to the embedment of the optical fibres they can also sense a portion of e.g. transverse strains. This is likely to occur in highly curves structures. The optical fibres are calibrated by a factor of 2.66 on the raw data. This is used by Smart Fibres as calibration for the raw data in their experience. For this structure or embedment the factor can be adjusted to fine-tune the results. The difference between the single and multiplexed fibre in the low strain area (nr 1. and 2.) is more than at the high strain area (nr 3. and 4.) but still comparable. This is cause by the fact that the sensors are located 10 mm apart, which is also seen at the results of the strain gauges. The difference however between the two optical fibre sensors is approximately 3 % higher than the difference of the strain gauges at the same location. For the lower loading levels (especially in the low strain area) the differences are the greatest (10-12 %). The specifications of the Smart Fibres system list a resolution of ±10µε so it will not be surprisingly that for a low strain level the same absolute magnitude of fluctuation gives higher deviations in percentage than for higher strain levels. Looking at the absolute values it can be seen that the difference at the low stress region is less than at the high stress location. In the dynamic testing the results in the low stress region (nr 1. and 2.) differ more than 10 %. For the high stress region (nr 3. and 4.) the differences are comparable to the differences seen at the static test (3-5 %). Some reasons for the large difference are the following: The influence of the geometry has a larger impact at the low region (tail) than at the high stress region (main spar). Due to the different embedment of the optical fibres they can also sense a portion of e.g. transverse strains. This is likely to occur in highly curves structures (tail). 5.2 Recommendations This demonstration shows that optical fibres give comparable results for strain gauges and optical fibre sensors. Therefore recommendations will be given for further research if they are going to be used for load registration in a rotor blade. Some of those recommendations are the following: Find out the accuracy of both types of measurements. How much influence has the structure on the measurements of the optical fibres and do transverse strains have an influence also; How is the difference when the fibre is completely embedded in a structure and not almost at the top (internal strains); DOWEC 10021 rev1 Page: 12 of 18 30-09-2003

How has embedding to be done using vacuum infusion and how can the location be fixed; How can optical fibre sensors be used in a test; Can optical fibres be used as production monitoring? These are only a few recommendations but more will certainly exist. For each partner in the DOWEC project however the priority will be different e.g. a blade manufacturer is more concerned about the embedding process, but a research institute will be more interested in the signal reading of the optical fibres and test facilities are willing to know if they are reliable enough for test results. DOWEC 10021 rev1 Page: 13 of 18 30-09-2003

Appendix A: Strain gauges vs. Optical fibres (pos. strains) DOWEC 10021 rev1 Page: 14 of 18 30-09-2003

DOWEC 10021 rev1 Page: 15 of 18 30-09-2003

Appendix B: Strain gauges vs. Optical fibres (neg. strains) DOWEC 10021 rev1 Page: 16 of 18 30-09-2003

DOWEC 10021 rev1 Page: 17 of 18 30-09-2003

Appendix C: Single vs. multiplexed optical fibres DOWEC 10021 rev1 Page: 18 of 18 30-09-2003