EWEC 2006, AthensMartin Geyler 1 Hardware-in-the-Loop Development and Testing of New Pitch Control Algorithms EWEC 2006 Athens Martin Geyler, Jochen Giebhardt,

Slides:



Advertisements
Similar presentations
National Aeronautics and Space Administration Wind turbines generate electric power from clean renewable sources. They must be robust and.
Advertisements

Lecture 20 Dimitar Stefanov. Microprocessor control of Powered Wheelchairs Flexible control; speed synchronization of both driving wheels, flexible control.
Delft University of Technology Aeroelastic Modeling and Comparison of Advanced Active Flap Control Concepts for Load Reduction on the Upwind.
ASME 2002, Reno, January VIBRATIONS OF A THREE-BLADED WIND TURBINE ROTOR DUE TO CLASSICAL FLUTTER Morten Hartvig Hansen Wind Energy Department Risø.
European Wind Energy Conference and Exhibition 2010 Warsaw, Poland EWEC 2010 Warsaw April 2010 Aeroelastic Analysis of Pre-Curved Rotor Blades V.A.Riziotis,S.G.Voutsinas.
Presentation outline Product development process: =>Design for Six Sigma =>Advanced modelling tools Practical examples => SKF quiet running bearing.
Beams and Frames.
Advances in Condition Monitoring – Linking the Input to the Output Martin Jones Insensys.
AeroAcoustics & Noise Control Laboratory, Seoul National University
A Comparison of Multi-Blade Coordinate Transformation and Direct Periodic Techniques for Wind Turbine Control Design Karl Stol Wind Energy Symposium AIAA.
Load Assumptions for the Design of electro mechanic Pitch Systems
Controller design for a wind farm, considering both power and load aspects Maryam Soleimanzadeh Controller design for a wind farm, considering both power.
Challenge the future Delft University of Technology Blade Load Estimations by a Load Database for an Implementation in SCADA Systems Master Thesis.
Determining Mechanical Loads for Wind Turbines
1 TRC 2008 The Effect of (Nonlinear) Pivot Stiffness on Tilting Pad Bearing Dynamic Force Coefficients – Analysis Jared Goldsmith Research Assistant Dr.
PROJECTS WITH POTENTIAL FUNDING
1 Residual Vectors & Error Estimation in Substructure based Model Reduction - A PPLICATION TO WIND TURBINE ENGINEERING - MSc. Presentation Bas Nortier.
Design of Motion Systems N. Delson. Analysis in 156A Project  Initial Design  Measurement of Performance  Mathematical Modeling  Optimization  Re-Design.
Aeroelastic Stability and Control of Large Wind Turbines
March 2006 Development and Test of a 5 kW Wind Turbine for Modular Autonomous Supply Systems Berthold Hahn Paul Kühn Institut für Solare Energieversorgungstechnik.
Computational Modelling of Unsteady Rotor Effects Duncan McNae – PhD candidate Professor J Michael R Graham.
Experimental Aerodynamics & Concepts Group Micro Renewable Energy Systems Laboratory Georgia Institute of Technology Validation of.
Design Process Supporting LWST 1.Deeper understanding of technical terms and issues 2.Linkage to enabling research projects and 3.Impact on design optimization.
Wind Modeling Studies by Dr. Xu at Tennessee State University
Where: I T = moment of inertia of turbine rotor.  T = angular shaft speed. T E = mechanical torque necessary to turn the generator. T A = aerodynamic.
1 11 A review of wind energy technologies part two. Adviser : Dr. Yuan-Kang Wu Student : Po-Kai Lin Date :
Aerodynamics and Aeroelastics, WP 2
Some effects of large blade deflections on aeroelastic stability Bjarne S. Kallesøe Morten H. Hansen.
Smart Rotor Control of Wind Turbines Using Trailing Edge Flaps Matthew A. Lackner and Gijs van Kuik January 6, 2009 Technical University of Delft University.
Recent and Future Research for Bird-like Flapping MAVs of NPU Prof. B.F.Song Aeronautics School of Northwestern Polytechnical University.
Innovation for Our Energy FutureNational Renewable Energy Laboratory 1 Gunjit Bir National Renewable Energy Laboratory 47 th AIAA Aerospace Meetings Orlando,
Dave Corbus, Craig Hansen Presentation at Windpower 2005 Denver, CO May 15-18, 2005 Test Results from the Small Wind Research Turbine (SWRT) Test Project.
LOAD ALLEVIATION ON WIND TURBINE BLADES USING VARIABLE AIRFOIL GEOMETRY Thomas Buhl, Mac Gaunaa, Peter Bjørn Andersen and Christian Bak ADAPWING.
Voltage grid support of DFIG wind turbines during grid faults
EWEC2007 Milano, 8 May 2007 Extrapolation of extreme loads acc. to IEC Ed.3 in comparison with the physics of real turbine response Dirk Steudel,
Integrated Dynamic Analysis of Floating Offshore Wind Turbines EWEC2007 Milan, Italy 7-10 May 2007 B. Skaare 1, T. D. Hanson 1, F.G. Nielsen 1, R. Yttervik.
REDUCTION OF TEETER ANGLE EXCURSIONS FOR A TWO-BLADED DOWNWIND ROTOR USING CYCLIC PITCH CONTROL Torben Juul Larsen, Helge Aagaard Madsen, Kenneth Thomsen,
European Wind Energy Conference and Exhibition 2006 Athens, Greece EWEC’06 Athens 27 February-2 March 20061/16 Advanced Aeroelastic Modeling of Complete.
EWEC 2007, MilanoMartin Geyler 1 Individual Blade Pitch Control Design for Load Reduction on Large Wind Turbines EWEC 2007 Milano, 7-10 May 2007 Martin.
An Introduction to Rotorcraft Dynamics
Control systems KON-C2004 Mechatronics Basics Tapio Lantela, Nov 5th, 2015.
Title and Contents Contents:
Advanced Simulation Techniques for the coupled Fatigue and NVH Optimization of Engines. K+P Software, Schönbrunngasse 24, A Graz / Austria Tel.:
Supervisor: Dr David Wood Co-Supervisor: Dr Curran Crawford
High Speed Balancing in the Service Industry – Deformed Rotors
WIND TURBINE CONTROL DESIGN TO REDUCE CAPITAL COSTS P. Jeff Darrow(Colorado School of Mines) Alan Wright(National Renewable Energy Laboratory) Kathryn.
Modal Dynamics of Wind Turbines with Anisotropic Rotors Peter F
DEWEK 2004 Lecture by Aero Dynamik Consult GmbH, Dipl. Ing. Stefan Kleinhansl ADCoS – A Nonlinear Aeroelastic Code for the Complete Dynamic Simulation.
Samcef ROTORS versus MSC NASTRAN V**
Aerodynamic forces on the blade, COP, Optimum blade profiles
Bird Strike on Jet Fan. Introduction Modelling of Bird Strike using EUROPLEXUS Full Lagrangian Approach Bird modelled by SPH elements (porous gelatine.
Evan Gaertner University of Massachusetts, Amherst IGERT Seminar Series October 1st, 2015 Floating Offshore Wind Turbine Aerodynamics.
Advanced Controls Research Alan D. Wright Lee Fingersh Maureen Hand Jason Jonkman Gunjit Bir 2006 Wind Program Peer Review May 10, 2006.
ROBOTICS 01PEEQW Basilio Bona DAUIN – Politecnico di Torino.
Date of download: 6/1/2016 Copyright © ASME. All rights reserved. From: Numerical Simulation of the Aerodynamics of Horizontal Axis Wind Turbines under.
SECTION 3 Components part 2. DIFFERENTIALS Adams/Driveline has two differential related components –Entire Differential Unit (Differential Assembly) ●
Chapter 8, pp (*figures from text)
Model Reduction & Interface Modeling in Dynamic Substructuring Application to a Multi-Megawatt Wind Turbine MSc. Presentation Paul van der Valk.
Wind Turbine Control System
INVESTIGATION OF IDLING INSTABILITIES IN WIND TURBINE SIMULATIONS
DYNAMIC STALL OCCURRENCE ON A HORIZONTAL AXIS WIND TURBINE BLADE
Rotors in Complex Inflow, AVATAR, WP2
Dynamic Controllers for Wind Turbines
1C9 Design for seismic and climate changes
QUANSER Flight Control Systems Design 2DOF Helicopter 3DOF Helicopter 3DOF Hover 3DOF Gyroscope Quanser Education Solutions Powered by.
Conceptual research of a downwind turbine, based on a Suzlon 2
Design of a C – Clamp Asanga Ratnaweera Dept of Mechanical Engineering
Exploring the limits in Individual Pitch Control S. Kanev and T
High Speed Balancing in the Service Industry – Deformed Rotors
Eulerization of Betz theory: Wind Turbines
Presentation transcript:

EWEC 2006, AthensMartin Geyler 1 Hardware-in-the-Loop Development and Testing of New Pitch Control Algorithms EWEC 2006 Athens Martin Geyler, Jochen Giebhardt, Bahram Panahandeh Institut für Solare Energieversorgungstechnik (ISET e.V.) Phone:

EWEC 2006, AthensMartin Geyler 2 Project Objectives -Individual blade pitch control -compensation for unsymmetrical inflow conditions due to turbulence or deterministic effects -active damping for tower and blades Project Partners Development of advanced pitch control algorithms for load reduction in large wind turbines -Modular controller design -Development of safety algorithms -stability monitoring, -handling of sensor faults -Identification of requirements for the pitch system using a Hardware-in-the-Loop test bed setup -dynamics, -loads, wear, -power consumption, thermal losses, -load sensors -communication requirements

EWEC 2006, AthensMartin Geyler 3 Control Problem Schematic of Control Loop

EWEC 2006, AthensMartin Geyler 4 Test Bed: Schematic Overview

EWEC 2006, AthensMartin Geyler 5 Test Bed: Control Concept

EWEC 2006, AthensMartin Geyler 6 Test Bed: Laboratory Setup Load Drive Inverter Cabinet Pitch Drive Inverter Cabinet Pitch Motors Load Machines Controller Rack with Simulation PCs Host PC

EWEC 2006, AthensMartin Geyler 7 Block structure of Simulink model Real-Time Simulation: Overall Wind Turbine Model

EWEC 2006, AthensMartin Geyler rigid bodies connected by joints: (1)Universal joints with torsional stiffness and damping representing flexibility of the structure (2)Revolute joints with external torque input representing actuators Mechanical model Real-Time Simulation: Mechanical Model (1) -fully recursive algorithm: „Method of Articulated Inertia“: -tree-like structure is exploited -avoids need for inverting large mass matrices -O(N) method: computational effort increases linearly with number of DOF -Mass forces (gravity, inertia) inherently included by the algorithm. -Solver: 3 rd -order Runge-Kutta solver at 1ms time step -ca. 450 µs calculation time on Athlon PC Multibody approach:

EWEC 2006, AthensMartin Geyler 9 Mechanical model Real-Time Simulation: Mechanical Model (2) -Parameters for multi body model were calculated using a optimisation algorithm to find a best fit to a given finite elements (FE) model: 1st mode and static deflection of simplified blade model with 2 rigid sections; Comparison with FE model 1.Step: Optimisation of joint locations in order to allow for best representation of first 3 mode shapes 2.Step: Optimisation of stiffness parameters and joint twist angles in order to fit eigen frequencies and mode shapes -Validation: Comparison of static deflection due to a constant line load (blade) or constant tower top force

EWEC 2006, AthensMartin Geyler 10 Load torque reference values for load drives will include the following effects: Example simulation for pitch load situation in turbulent wind conditions Real-Time Simulation: Pitch System Model -pitch gear ratio 1:1000 -tooth clearance at fast side of pitch gears -blade bearing friction -DRE/CON-formula for large bearings: M R = µ D /2 * k * M blade root -Four point contact bearings: µ D = 0.006, k = Components for axial and radial force have been neglected. -changing inertia due to blade deflection inherently included by mechanical model

EWEC 2006, AthensMartin Geyler 11 Real-Time Simulation: Aerodynamic Model (1) -Blade Element Momentum Theory (BEM) -12 blade elements per blade -semi-empirical corrections: state-of-the-art implementation of - dynamic inflow - yawed inflow - dynamic stall -total 240 aerodynamic states -Solver: simple Forward-Euler integration at 1ms time step calculation time ca. 45 µs on Athlon PC

EWEC 2006, AthensMartin Geyler 12 Dynamic Inflow Model (ECN): -Local inflow condition at blade sections depend on free wind speed and load situation of the rotor in a dynamic manner. -Example: Overshoot in blade root bending moment for fast step on pitch angle Simulation Tjaereborg Experiment Real-Time Simulation: Aerodynamic Model (2)

EWEC 2006, AthensMartin Geyler 13 Dynamic Stall Model (Beddoes-Leishmann-Type): -Effect: dynamic lift forces can be considerable bigger than predicted by stationary c L -  -curve for fast changes in pitch angle. Simulation Measurement (Risø) Real-Time Simulation: Aerodynamic Model (3)

EWEC 2006, AthensMartin Geyler 14 2-D turbulent Wind Field is simulated off-line and read from a file during real time simulation  reproducible time series -8 x 8 points in the rotor plane, -linear interpolation -only mean wind direction Real-Time Simulation: Turbulent Wind Field Input (1) Method by Mann - wind field is assembled in a 3D-box by means of inverse FFT - Fourier Coefficients calculated from spectral-tensor ( only  11 used ) -„frozen turbulence“ : dimension L1 is used as time axis Parameter fitting to Kaimal spectrum Input parameters: - mean wind speed, - mean wind shear, - turbulence intensity Extreme gust events can be embedded into stochastic turbulent wind field: - Most likely gust shape calculated from correlation matrix R and a given criterion e.g. total jump in wind speed at given location

EWEC 2006, AthensMartin Geyler 15 Real-Time Simulation: Turbulent Wind Field Input (2) Averaged auto-power spectrum for simulated wind fields Example for extreme gust event Criterion:  v = 10 m/s,  t = 16 s, location

EWEC 2006, AthensMartin Geyler 16 -3D visualisation tool for motion and load situation of simulated wind turbine -VRML based -Visualisation coupled to real-time simulation via TCP/IP based communication channel Visualisation with VRML Real-Time Simulation: Visualisation

EWEC 2006, AthensMartin Geyler 17 First Results (1) -Algorithm for yaw and tilt moment compensation implemented and tested simulated reduction in 1p component of flapwise blade root bending moment -(simulated) 1p component in flapwise blade root bending moments is almost cancelled, -pitch drive rating seems sufficient for producing required 1p cyclic pitch offsets, however, considerably increased motion as compared to normal collective pitch operation -simple fuzzy scheme for supervision and controller gain adjustment

EWEC 2006, AthensMartin Geyler 18 First Results (2) Measurement of Pitch Drive Load Torques

EWEC 2006, AthensMartin Geyler 19 Conclusions -Hardware-in-the-Loop test bed for Pitch Drives has been developed and successfully taken into operation. -Real-Time Simulation Environment allows for providing realistic load conditions as well as all required feedback signals to the tested Pitch Control System. -First simulation results and measurements for a Yaw- and Tilt-Moment Compensation Controller (Proof-Of-Concept). -It is believed, that the test bed will greatly improve the understanding of the system aspects of advanced pitch control strategies. Thank You.