Transient response modelling for wind turbines based on synthetic wind speeds. DEL Presentation. Thomas Woolmington 28th February 2014
|
|
- Peter Cunningham
- 5 years ago
- Views:
Transcription
1 Transient response modelling for wind turbines based on synthetic wind speeds. DEL Presentation Thomas Woolmington 28th February 2014
2 Overview Introduction to Wind Energy Data Acquisition and Statistical Summarisation The Generation of Power Curves Current Power Prediction Techniques. Artificial Wind Speeds System Response Modeling Acknowledgements
3 Overview Introduction to Wind Energy Data Acquisition and Statistical Summarisation The Generation of Power Curves Current Power Prediction Techniques. Artificial Wind Speeds System Response Modeling Acknowledgements
4 Introduction to Wind Energy Kinetic wind energy is harnessed by converting to mechanical energy via the turbine rotor and then into electrical energy through the generator: Wind Energy if fundamentally derived from an extension of kinetic energy formula! P = C. p ρ. A. u 2 3 where the mechanical output power (P) is a function of the performance coefficient of the turbine C p, the density of air (ρ), the area swept by the turbine projected in the direction of the wind (A) and wind-speed (u).
5 Introduction to Wind Energy It is worth considering that Cp is limited by Betz limit of 59.3% efficiency however an important fact that is often missed is that this is strictly speaking only applicable in laminar kinetic mass flow systems. (N.B. Turbulence and Pressure drop are not considered!) As wholly laminar environments are rarely present in real world scenarios it is evident that further investigation is required when trying to bound the likely coefficient of performance in a turbulent environment.
6 Introduction to Wind Energy
7 Introduction to Wind Energy VAWT Functions in wind from any direction Functions in Turbulent or gusty Wind 12/03/hawt-and-vawt.jpg HAWT Can only accept wind from a single direction 12/03/hawt-and-vawt.jpg
8 Introduction to Wind Energy Numerous Field studies have shown that for similar size VAWT and HAWT turbine installations in similar environments that the VAWT outperform compared to their HAWT counterpart. Question: Why does the prescribed standard and or general research acceptancein this area not have different power prediction calculations based on VAWT and HAWT classification?
9 Overview Introduction to Wind Energy Data Acquisition and Statistical Summarisation The Generation of Power Curves Current Power Prediction Techniques. Artificial Wind Speeds System Response Modeling Acknowledgements
10 Data Acquisition and Statistical Summarisation DUBLex (Dublin, Urban Boundary Layer Experiment) UCD, DIT and NUI Maynooth. High resolution data for multiple purposes e.g. CO 2 monitoring / temp / moisture / wind speed Has multiple applications air quality / litter dumping / temp. hot spots / urban wind generation. A mast installation is on top of DIT Kevin Street for approximately 1 year also Marrowbone Lane URB1 St Pius SUB2
11 Data Acquisition and Statistical Summarisation Longitudinal (Cosine corrected) wind speed in a 10 minute sample. (Red arrows) Met Mast 6000 wind (speed/direction) observations or one window of 10 minutes Meteorological equipment measures 3D 10Hz wind data Then converted to conform with IEC Mean Wind Direction (over duration of observatrion window) w Individual wind vector u Longtitudinal wind velocity vector v Lateral wind velocity vector Vertical wind velocity vector However should we be using polar wind speeds (black arrows) for VAWTs w u v Cosine Corrected Wind Vector Mean of all cosine corrected wind speeds along the mean (window) direction line (Interpreted from IEC, 2006)
12 Data Acquisition and Statistical Summarisation From this industrial standard 10 minute bins are drawn based on longitudinal values of mean TI and a proposed new metric T Df This metric essentially measures how noisy a signal is. T Df = unbounded Fractal Dimension by Fourier means Analysis
13 Data Acquisition and Statistical Summarisation 1 Df = 1.00 Black Noise Df = 1.50 Brown Noise Df = 2.00 Pink Noise Df = 2.50 White Noise 0.5 Analysis
14 Df =1 is effectively 0% turbulence by the T Df metric Data Acquisition and Statistical Summarisation However the current TI metric would classify this sample as having 31% turbulence The current TI metric does not allow for trends within the wind speed sample N.B.the T Df metric does not cater for the spread of the erratic signal Therefore there is a need for both metrics when describing a wind speed signal
15 Overview Introduction to Wind Energy Data Acquisition and Statistical Summarisation The Generation of Power Curves Current Power Prediction Techniques. Artificial Wind Speeds System Response Modeling Acknowledgements
16 The Generation of Power Curves The ability to predict the power from a micro wind turbine has long been a source of controversy within industry. Inaccuracies in excess of 30% have been recorded but rarely quoted due to commercial sensitivity. Common issues that have been quoted have been the lack of accurate data / poor site assessment / overestimated manufacturers data. Also there is an ever increasing argument as to the inaccuracy of power curves so much so that IEC (2006) has specified strict criteria as to how and what needs to be measured. However this involves the use of regressive averaging which has an unknown statistical error for each turbine tested
17 The Generation of Power Curves 6 5kW demo model Power Curve 5 Power output t kw This particular study was for a 5kW turbine in a rural environment. Why is there such a spread for the power per wind speed division? Wind Speed m/s
18 The Generation of Power Curves 5kW demo model Power Curve 6 5 Power output t kw Note this power curve is only representative for this particular environment i.e. Typically tested in a low turbulence environment Wind Speed m/s
19 Overview Introduction to Wind Energy Data Acquisition and Statistical Summarisation The Generation of Power Curves Current Power Prediction Techniques. Artificial Wind Speeds System Response Modeling Acknowledgements
20 Current Power Prediction Methods 10 minute wind speed distributions can be fitted into Weibull distributions even in turbulent environments! High Turbulence (Urban/suburban) Med Turbulence (Suburban/Rural) Low Turbulence (Rural/Off-shore) Low ū Logarithmic PDF Logarithmic / Rayleigh PDF Rayleigh PDF Medium ū Logarithmic / Rayleigh PDF Rayleigh PDF Rayleigh / Gaussian PDF High ū Rayleigh PDF Rayleigh / Gaussian PDF Gaussian PDF The shape and/or scale of the distribution will change due to the turbulence measured in the sample. This gives a different spread of wind speeds and therefore adjusts the power curve based on turbulence. Probability Sample Weibull Distributions sh=0.5 sc=1 sh=1.0 sc=1 Exponential sh=1.5 sc=1 sh=2.0 sc=1 Reyleigh sh=2.5 sc=1 sh=3.0 sc=1 sh=3.5 sc=1 sh=4.0 sc=1 sh=4.5 sc=1 sh=5.0 sc=1 Gaussian
21 Current Power Prediction Methods Dynamic modelling based on best fit Gaussian histogram model for each 10 minute window Av erage Turbine Pwr. Power [kw] TI=10% TI=15% TI=20% TI=25% TI=30% TI=35% TI=40% TI=45% TI=50% TI=55% TI=60% TI=65% TI=70% TI=75% Wind Speed [m/s]
22 Current Power Prediction Methods Dynamic modelling based on best fit Weibull histogram model for each 10 minute window Power [kw] Wind Speed [m/s] Av erage Turbine Pwr. TI=10% TI=15% TI=20% TI=25% TI=30% TI=35% TI=40% TI=45% TI=50% TI=55% TI=60% TI=65% TI=70% TI=75%
23 The Generation of Power Curves Previous works have investigated the statistical accuracy of both of the above processes. Both the Weibull and the Albers (Gaussian) approximations have high mathematical accuracies. >95% of all values lie within 0.05 of Prated of the turbine even when using narrow wind speed bins (0.5m/s). Major Assumption! This model relies on an instantaneous response model! Mechanical inertia, Blade response, Generator pick up, inverter pick up is not considered in a frequency based power prediction model! A time series model needs to be developed in order to consider the above!
24 Overview Introduction to Wind Energy Data Acquisition and Statistical Summarisation The Generation of Power Curves Current Power Prediction Techniques. Artificial Wind Speeds System Response Modeling Acknowledgements
25 Artificial Wind Speeds Generation of Artificial wind speed signals based on TI, T Df and mean speed If we consider a 10 minute bin of 10Hz data summarised to mean, TI and T Df Question: What can we do with it? It is pointless in proposing a new metric (T Df ) unless it has some practical application So lets consider mixing Gaussian statistics with non Gaussian statistics!
26 Artificial Wind Speeds Consider a series of 600 random numbers (n x ) between 0-1 subjected to the following convolution ( ) in the frequency domain. Where: T Df (Turbulent Fourier Dimension)=(5-q)/2 Frequency domain equivalent with i indexing filter For this example lets take a T Df of 1.8, a TI of 0.45 (45%), and a u mean of 7.5 m/s
27 Artificial Wind Speeds Generating a fractal curve of known T Df gives the following graph. u m/s 10 TDf = mean fractal curve Fractal noise is scale invariant and as such has the same fractal properties at any scale Note the amplitude is not defined! 2 If we zoom in the concept becomes clearer! time in seconds
28 Artificial Wind Speeds Zooming in shows the fractal self symmetry within the curve. However this is not scaled and as such is of no use on its own. If we normalise to unit Standard deviation (divide by standard deviation) uniform scaling is maintained giving; u m/s TDf = mean fractal curve time in seconds
29 Artificial Wind Speeds Now that the curve is normalised around zero a known spread can be applied. u m/s 10 TDf = 1.80 normalised 0 mean fractal curve Standard dev is = mean x TI 8 6 So multiply across to give the next slide time in seconds
30 Artificial Wind Speeds Now that the curve has a spread indicative of the standard u m/s 10 TDf = 1.80 TI = 0.45 TI spread fractal curve deviation it is now time to add in an 8 average time in seconds
31 Artificial Wind Speeds This artificial wind speed has the same statistical properties as an original recording of T Df, TI and u mean. u m/s 10 8 Fractal curve with TDf = 1.80, TI = 0.45, Umean = 7.5 Early comparisons have shown this model to have a 97% statistical accuracy compared to a frequency bin equivalent However this is not over the full data set time in seconds
32 Overview Introduction to Wind Energy Data Acquisition and Statistical Summarisation The Generation of Power Curves Current Power Prediction Techniques. Artificial Wind Speeds System Response Modeling Acknowledgements
33 System Response Modelling If we consider the seriality of wind speeds as consecutive first order transients based on how quick will the system be able to respond to a change in wind speed. If we assume that these transients have a natural growth / decay curve as influencing the input response function (wind speed). In simple terms how quickly can the system respond to a change in input parameter? Adapted Heaviside step function De-convolution theory normally could be used as a means of acquiring an input response function however in this instance the base point (u start ) is constantly changing. This new model can then be benchmarked etc.
34 System Response Modelling If we consider the first 25 points of the previous artificial time series. u m/s Artificial Time Series Note strictly speaking this should only be displayed as points as they are specific datums at a known time time in seconds
35 System Response Modelling Also strictly speaking we do not know what happens between each of these points. u m/s Artificial Time Series at datum points This can be used then as an input argument What time constant whether growth or decay is suitable? time in seconds
36 System Response Modelling Where: U res = u per unit time U start = initial u at start of transient window u = change in u over transient window As τ increases e.g. larger turbines have greater inertia u m/s τ =1 simulation of system response Time Series Modelling Incorporating System Inertia Wind Speed Recordings System Responce time in seconds
37 System Response Modelling Where: U res = u per unit time U start = initial u at start of transient window u = change in u over transient window As τ increases e.g. larger turbines have greater inertia u m/s τ =5 simulation of system response Time Series Modelling Incorporating System Inertia Wind Speed Recordings System Responce time in seconds
38 System Response Modelling Where: U res = u per unit time U start = initial u at start of transient window u = change in u over transient window As τ increases e.g. larger turbines have greater inertia u m/s τ =25 simulation of system response Time Series Modelling Incorporating System Inertia Wind Speed Recordings System Responce time in seconds
39 System Response Modelling Statistical accuracy of the system response model.
40 Overview Introduction to Wind Energy Data Acquisition and Statistical Summarisation The Generation of Power Curves Current Power Prediction Techniques. Artificial Wind Speeds System Response Modeling Acknowledgements
41 Acknowledgements The author(s) would like to acknowledge Dr. Rowan Fealy, of the National University of Ireland, Maynooth (NUIM) and Dr. Gerald Mills, University College Dublin, (UCD) for providing the wind data employed in this analysis and also Axel Albers, for helpful comments at the early stages of the research.
42 Thank you
Analysis of Wind Velocity Signals for Estimating the Wave Power Density of Ireland s Coastal Resource
ISSC 2012, NUI Maynooth, June 28 29 Analysis of Wind Velocity Signals for Estimating the Wave Power Density of Ireland s Coastal Resource Jonathan Blackledge, Eugene Coyle, Ronan McGuirk and Derek Kearney
More informationCorrelation, discrete Fourier transforms and the power spectral density
Correlation, discrete Fourier transforms and the power spectral density visuals to accompany lectures, notes and m-files by Tak Igusa tigusa@jhu.edu Department of Civil Engineering Johns Hopkins University
More informationObserved Reduction of Sensitivities of Windcube Measurements by Vector Averaging
Observed Reduction of Sensitivities of Windcube Measurements by Vector Averaging Workshop on Vector Averaging Versus Scalar Averaging Vilnius, 2018-05-14 Outlook Background: Encountered Difficulties Difference
More informationComputer Vision & Digital Image Processing
Computer Vision & Digital Image Processing Image Restoration and Reconstruction I Dr. D. J. Jackson Lecture 11-1 Image restoration Restoration is an objective process that attempts to recover an image
More informationFrequency Dependent Aspects of Op-amps
Frequency Dependent Aspects of Op-amps Frequency dependent feedback circuits The arguments that lead to expressions describing the circuit gain of inverting and non-inverting amplifier circuits with resistive
More informationOn the impact of non-gaussian wind statistics on wind turbines - an experimental approach
On the impact of non-gaussian wind statistics on wind turbines - an experimental approach Jannik Schottler, N. Reinke, A. Hölling, J. Peinke, M. Hölling ForWind, Center for Wind Energy Research University
More informationMechanical Engineering for Renewable Energy Systems. Wind Turbines
ENGINEERING TRIPOS PART IB PAPER 8 - ELECTIVE (2) Mechanical Engineering for Renewable Energy Systems Wind Turbines Lecture 3: Aerodynamic fundamentals Hugh Hunt Fundamental fluid mechanics limits to energy
More informationDennis: SODAR-Based Wind Resource Assessment
Dennis: SODAR-Based Wind Resource Assessment Prepared by: Utama Abdulwahid, PhD James F. Manwell, PhD February 3, 2011 www.umass.edu/windenergy Wind Energy Center wec@ecs.umass.edu Table of Contents Executive
More informationStandard Practices for Air Speed Calibration Testing
Standard Practices for Air Speed Calibration Testing Rachael V. Coquilla Bryza Wind Lab, Fairfield, California Air speed calibration is a test process where the output from a wind measuring instrument
More informationReview of Anemometer Calibration Standards
Review of Anemometer Calibration Standards Rachael V. Coquilla rvcoquilla@otechwind.com Otech Engineering, Inc., Davis, CA Anemometer calibration defines a relationship between the measured signals from
More informationPerformance of a Vertical Axis Wind Turbine under Accelerating and Decelerating Flows
Available online at www.sciencedirect.com Procedia CIRP 00 (2013) 000 000 www.elsevier.com/locate/procedia 2 nd International Through-life Engineering Services Conference Performance of a Vertical Axis
More informationTheoretical Aerodynamic analysis of six airfoils for use on small wind turbines
Proceedings of the 1st International Conference on Emerging Trends in Energy Conservation - ETEC Tehran, Tehran, Iran, 20-21 November 2011 Theoretical Aerodynamic analysis of six airfoils for use on small
More informationCommunication Engineering Prof. Surendra Prasad Department of Electrical Engineering Indian Institute of Technology, Delhi
Communication Engineering Prof. Surendra Prasad Department of Electrical Engineering Indian Institute of Technology, Delhi Lecture - 3 Brief Review of Signals and Systems My subject for today s discussion
More informationDeviations between wind speed data measured with nacelle-mounted anemometers on small wind turbines and anemometers mounted on measuring masts
Agronomy Research 12(2), 433 444, 2014 Deviations between wind speed data measured with nacelle-mounted anemometers on small wind turbines and anemometers mounted on measuring masts A. Allik*, J. Uiga
More informationImproving S5P NO 2 retrievals
Institute of Environmental Physics and Remote Sensing IUP/IFE-UB Department 1 Physics/Electrical Engineering Improving S5P NO 2 retrievals ESA ATMOS 2015 Heraklion June 11, 2015 Andreas Richter, A. Hilboll,
More informationFluctuating Heat Transfer to an Impinging Air Jet in the Transitional Wall Jet Region
Fluctuating Heat Transfer to an Impinging Air Jet in the Transitional Wall Jet Region Tadhg S. O Donovan, Darina B. Murray Department of Mechanical & Manufacturing Engineering, Trinity College Dublin,
More informationAnalysis of one- and two-dimensional mean gust shapes using a largeeddy simulation model
Analysis of one- and two-dimensional mean gust shapes using a largeeddy simulation model Knigge, Christoph* 1), Raasch, Siegfried 1) 1) Institut für Meteorologie und Klimatologie, Leibniz Universität Hannover,
More informationNUMERICAL STUDY OF FLOW STREAM IN A MINI VAWT WITH RELATIVE ROTATING BLADES
NUMERICAL STUDY OF FLOW STREAM IN A MINI VAWT WITH RELATIVE ROTATING BLADES Bayeul-Lainé Annie-Claude, Simonet Sophie, Dockter Aurore, Bois Gérard LML, UMR CNRS 8107, Arts et Metiers PARISTECH 8, Boulevard
More informationLecture 7: Statistics and the Central Limit Theorem. Philip Moriarty,
Lecture 7: Statistics and the Central Limit Theorem Philip Moriarty, philip.moriarty@nottingham.ac.uk NB Notes based heavily on lecture slides prepared by DE Rourke for the F32SMS module, 2006 7.1 Recap
More informationConvolution and Linear Systems
CS 450: Introduction to Digital Signal and Image Processing Bryan Morse BYU Computer Science Introduction Analyzing Systems Goal: analyze a device that turns one signal into another. Notation: f (t) g(t)
More informationA Procedure for Classification of Cup-Anemometers
Downloaded from orbit.dtu.dk on: Dec, 17 A Procedure for Classification of Cup-Anemometers Friis Pedersen, Troels; Paulsen, Uwe Schmidt Published in: Proceedings of EWEC 97 Publication date: 1997 Link
More informationDocument No 10/6298/001/GLA/O/R/001 Issue : B2. Kingspan Renewables Ltd. Kingspan KW6 Wind Turbine Noise Performance Test
Document No 10/6298/001/GLA/O/R/001 Issue : B2 Kingspan Renewables Ltd Kingspan KW6 Wind Turbine Noise Performance Test December 11 2 Bath Street, Glasgow, G2 4GZ Telephone: +44 (0) 141 227 1700 www.sgurrenergy.com
More informationJustin Appleby CS 229 Machine Learning Project Report 12/15/17 Kevin Chalhoub Building Electricity Load Forecasting
Justin Appleby CS 229 Machine Learning Project Report 12/15/17 Kevin Chalhoub Building Electricity Load Forecasting with ARIMA and Sequential Linear Regression Abstract Load forecasting is an essential
More informationStatistics for Data Analysis. Niklaus Berger. PSI Practical Course Physics Institute, University of Heidelberg
Statistics for Data Analysis PSI Practical Course 2014 Niklaus Berger Physics Institute, University of Heidelberg Overview You are going to perform a data analysis: Compare measured distributions to theoretical
More information1 Wind Turbine Acoustics. Wind turbines generate sound by both mechanical and aerodynamic
Wind Turbine Acoustics 1 1 Wind Turbine Acoustics Wind turbines generate sound by both mechanical and aerodynamic sources. Sound remains an important criterion used in the siting of wind farms. Sound emission
More informationWelcome to the world of wind energy. Wind Potential. Dr. D. V. Kanellopoulos OPWP Renewable Energy Training Program December 2016 Muscat, Oman
Welcome to the world of wind energy Wind Potential Dr. D. V. Kanellopoulos OPWP Renewable Energy Training Program 11-14 December 2016 Muscat, Oman 1 Solar radiation powers up the wind 2 Surface air temperatures
More information2d-Laser Cantilever Anemometer
2d-Laser Cantilever Anemometer Introduction Measuring principle Calibration Design Comparative measurement Contact: Jaroslaw Puczylowski University of Oldenburg jaroslaw.puczylowski@forwind.de Introduction
More informationProbability & Statistics: Infinite Statistics. Robert Leishman Mark Colton ME 363 Spring 2011
Probability & Statistics: Infinite Statistics Robert Leishman Mark Colton ME 363 Spring 0 Large Data Sets What happens to a histogram as N becomes large (N )? Number of bins becomes large (K ) Width of
More informationMachine Learning in Modern Well Testing
Machine Learning in Modern Well Testing Yang Liu and Yinfeng Qin December 11, 29 1 Introduction Well testing is a crucial stage in the decision of setting up new wells on oil field. Decision makers rely
More informationLECTURE 22 WIND POWER SYSTEMS. ECE 371 Sustainable Energy Systems
LECTURE 22 WIND POWER SYSTEMS ECE 71 Sustainable Energy Systems 1 AVG POWER IN WIND WITH RAYLEIGH STATISTICS The average value of the cube of wind speed can be calculated with Raleigh probability density
More informationDynamics of Ocean Structures Prof. Dr Srinivasan Chandrasekaran Department of Ocean Engineering Indian Institute of Technology, Madras
Dynamics of Ocean Structures Prof. Dr Srinivasan Chandrasekaran Department of Ocean Engineering Indian Institute of Technology, Madras Module - 1 Lecture - 7 Duhamel's Integrals (Refer Slide Time: 00:14)
More informationLecture 8: Differential Equations. Philip Moriarty,
Lecture 8: Differential Equations Philip Moriarty, philip.moriarty@nottingham.ac.uk NB Notes based heavily on lecture slides prepared by DE Rourke for the F32SMS module, 2006 8.1 Overview In this final
More informationThe Solar Nozzle a possible approach for
The Solar Nozzle a possible approach for Efficient, Large Scale, Solar Electricity Summary The author proposes a new method for conversion of solar energy into electricity using natural convection in an
More informationAEROELASTICITY IN AXIAL FLOW TURBOMACHINES
von Karman Institute for Fluid Dynamics Lecture Series Programme 1998-99 AEROELASTICITY IN AXIAL FLOW TURBOMACHINES May 3-7, 1999 Rhode-Saint- Genèse Belgium STRUCTURAL DYNAMICS: BASICS OF DISK AND BLADE
More informationNew York Tutorials are designed specifically for the New York State Learning Standards to prepare your students for the Regents and state exams.
Tutorial Outline New York Tutorials are designed specifically for the New York State Learning Standards to prepare your students for the Regents and state exams. Math Tutorials offer targeted instruction,
More informationThe effect of environmental and operational variabilities on damage detection in wind turbine blades
The effect of environmental and operational variabilities on damage detection in wind turbine blades More info about this article: http://www.ndt.net/?id=23273 Thomas Bull 1, Martin D. Ulriksen 1 and Dmitri
More informationDigital Signal Processing Module 1 Analysis of Discrete time Linear Time - Invariant Systems
Digital Signal Processing Module 1 Analysis of Discrete time Linear Time - Invariant Systems Objective: 1. To understand the representation of Discrete time signals 2. To analyze the causality and stability
More informationMaximum Power Point Tracking for Photovoltaic Optimization Using Extremum Seeking
Maximum Power Point Tracking for Photovoltaic Optimization Using Extremum Seeking Steve Brunton 1, Clancy Rowley 1, Sanj Kulkarni 1, and Charles Clarkson 2 1 Princeton University 2 ITT Space Systems Division
More informationSECTION 7: CURVE FITTING. MAE 4020/5020 Numerical Methods with MATLAB
SECTION 7: CURVE FITTING MAE 4020/5020 Numerical Methods with MATLAB 2 Introduction Curve Fitting 3 Often have data,, that is a function of some independent variable,, but the underlying relationship is
More informationprobability of k samples out of J fall in R.
Nonparametric Techniques for Density Estimation (DHS Ch. 4) n Introduction n Estimation Procedure n Parzen Window Estimation n Parzen Window Example n K n -Nearest Neighbor Estimation Introduction Suppose
More informationLecture 27 Frequency Response 2
Lecture 27 Frequency Response 2 Fundamentals of Digital Signal Processing Spring, 2012 Wei-Ta Chu 2012/6/12 1 Application of Ideal Filters Suppose we can generate a square wave with a fundamental period
More informationWIND FARM PERFORMANCE MONITORING WITH ADVANCED WAKE MODELS
Summary WIND FARM PERFORMANCE MONITORING WITH ADVANCED WAKE MODELS N. Mittelmeier 1, S. Amelsberg 3, T. Blodau 1, A. Brand 4, S. Drueke 2, M. Kühn 2, K. Neumann 1, G. Steinfeld 2 1) REpower Systems SE,
More informationDetector Characterization of the 40m Interferometer. Eve Chase Mentors: Koji Arai & Max Isi August 20, 2015 LIGO-T
Detector Characterization of the 40m Interferometer Eve Chase Mentors: Koji Arai & Max Isi August 20, 2015 LIGO-T1500123 Overview Detector Characterization- an effort to identify, understand, and eliminate
More informationSite assessment for a type certification icing class Fraunhofer IWES Kassel, Germany
Site assessment for a type certification icing class Kai Freudenreich 1, Michael Steiniger 1, Zouhair Khadiri-Yazami 2, Ting Tang 2, Thomas Säger 2 1 DNV GL Renewables Certification, Hamburg, Germany kai.freudenreich@dnvgl.com,
More informationEliminating the Influence of Harmonic Components in Operational Modal Analysis
Eliminating the Influence of Harmonic Components in Operational Modal Analysis Niels-Jørgen Jacobsen Brüel & Kjær Sound & Vibration Measurement A/S Skodsborgvej 307, DK-2850 Nærum, Denmark Palle Andersen
More informationPhysics 132- Fundamentals of Physics for Biologists II
Physics 132- Fundamentals of Physics for Biologists II Statistical Physics and Thermodynamics A confession Temperature Object A Object contains MANY atoms (kinetic energy) and interactions (potential energy)
More informationPHYSICS 9646/02. NANYANG JUNIOR COLLEGE Science Department JC 2 PRELIMINARY EXAMINATION Higher 2. Candidate Name. Tutor Name.
NANYANG JUNIOR COLLEGE Science Department JC PRELIMINARY EXAMINATION Higher Candidate Name Class Tutor Name PHYSICS 9646/0 Paper Structured Questions 4 September 013 1 hour 45 minutes Candidates answer
More informationSignal types. Signal characteristics: RMS, power, db Probability Density Function (PDF). Analogue-to-Digital Conversion (ADC).
Signal types. Signal characteristics:, power, db Probability Density Function (PDF). Analogue-to-Digital Conversion (ADC). Signal types Stationary (average properties don t vary with time) Deterministic
More informationStructural changes detection with use of operational spatial filter
Structural changes detection with use of operational spatial filter Jeremi Wojcicki 1, Krzysztof Mendrok 1 1 AGH University of Science and Technology Al. Mickiewicza 30, 30-059 Krakow, Poland Abstract
More informationRisø-R-1133(EN) Mean Gust Shapes. Gunner Chr. Larsen, Wim Bierbooms and Kurt S. Hansen
Risø-R-33(EN) Mean Gust Shapes Gunner Chr. Larsen, Wim Bierbooms and Kurt S. Hansen Risø National Laboratory, Roskilde, Denmark December 3 Abstract The gust events described in the IEC-standard are formulated
More information13 SHADOW FLICKER Introduction Methodology
Table of contents 13 SHADOW FLICKER... 13-1 13.1 Introduction... 13-1 13.2 Methodology... 13-1 13.2.1 Factors Influencing Shadow Flicker Occurrence... 13-2 13.2.2 Shadow Flicker Analysis Methodology...
More informationIntertek Test Report No CRT-002 Project No. G Johan Kuikman Phone: Fortis Wind Energy BV
3933 US Route 11 Cortland, NY 13045 Telephone: (607) 753-6711 Facsimile: (607) 753-1045 www.intertek.com Intertek Project No. G100146060 Johan Kuikman Phone: 310505515666 Fortis Wind Energy BV Aduarderdiepsterweg
More informationSCIENTIFIC REPORT. Host: Sven-Erik Gryning (DTU Wind Energy, Denmark) Applicant: Lucie Rottner (Météo-France, CNRM, France)
SCIENTIFIC REPORT ACTION: ES1303 TOPROF STSM: COST-STSM-ES1303-30536 TOPIC: Validation of real time turbulence estimation and measurement of wind gust using Doppler lidar. VENUE: Technical University of
More informationCommunications and Signal Processing Spring 2017 MSE Exam
Communications and Signal Processing Spring 2017 MSE Exam Please obtain your Test ID from the following table. You must write your Test ID and name on each of the pages of this exam. A page with missing
More informationEPPING HIGH SCHOOL ALGEBRA 2 COURSE SYLLABUS
Course Title: Algebra 2 Course Description This course is designed to be the third year of high school mathematics. The material covered is roughly equivalent to that covered in the first Algebra course
More informationDynamic Multipath Estimation by Sequential Monte Carlo Methods
Dynamic Multipath Estimation by Sequential Monte Carlo Methods M. Lentmaier, B. Krach, P. Robertson, and T. Thiasiriphet German Aerospace Center (DLR) Slide 1 Outline Multipath problem and signal model
More informationChapter 1, Section 1.2, Example 9 (page 13) and Exercise 29 (page 15). Use the Uniqueness Tool. Select the option ẋ = x
Use of Tools from Interactive Differential Equations with the texts Fundamentals of Differential Equations, 5th edition and Fundamentals of Differential Equations and Boundary Value Problems, 3rd edition
More informationOver-enhancement Reduction in Local Histogram Equalization using its Degrees of Freedom. Alireza Avanaki
Over-enhancement Reduction in Local Histogram Equalization using its Degrees of Freedom Alireza Avanaki ABSTRACT A well-known issue of local (adaptive) histogram equalization (LHE) is over-enhancement
More informationOn the Use of Hot-Film Sensors in the Investigation of Fluid Dynamic Phenomena in the Near-Wall Region
UNIVERSITY of LIMERICK OLLSCOIL LUIMNIGH On the Use of Hot-Film Sensors in the Investigation of Fluid Dynamic Phenomena in the Near-Wall Region Philip C. Griffin & Mark R.D. Davies Stokes Research Institute
More informationA TEST OF THE PRECIPITATION AMOUNT AND INTENSITY MEASUREMENTS WITH THE OTT PLUVIO
A TEST OF THE PRECIPITATION AMOUNT AND INTENSITY MEASUREMENTS WITH THE OTT PLUVIO Wiel M.F. Wauben, Instrumental Department, Royal Netherlands Meteorological Institute (KNMI) P.O. Box 201, 3730 AE De Bilt,
More informationSite Description: Tower Site
Resource Summary for Fort Collins Site Final Report Colorado Anemometer Loan Program Monitoring Period: /0/00 11/03/007 Report Date: January 1, 00 Site Description: The site is located adjacent to the
More informationLab 3: Model based Position Control of a Cart
I. Objective Lab 3: Model based Position Control of a Cart The goal of this lab is to help understand the methodology to design a controller using the given plant dynamics. Specifically, we would do position
More informationBasic Fluid Mechanics
Basic Fluid Mechanics Chapter 6A: Internal Incompressible Viscous Flow 4/16/2018 C6A: Internal Incompressible Viscous Flow 1 6.1 Introduction For the present chapter we will limit our study to incompressible
More informationAlg2H Ch6: Investigating Exponential and Logarithmic Functions WK#14 Date:
Alg2H Ch6: Investigating Exponential and Logarithmic Functions WK#14 Date: Purpose: To investigate the behavior of exponential and logarithmic functions Investigations For investigations 1 and 2, enter
More informationLecture 4: Wind energy
ES427: The Natural Environment and Engineering Global warming and renewable energy Lecture 4: Wind energy Philip Davies Room A322 philip.davies@warwick.ac.uk 1 Overview of topic Wind resources Origin of
More informationName: INSERT YOUR NAME HERE. Due to dropbox by 6pm PDT, Wednesday, December 14, 2011
AMath 584 Name: INSERT YOUR NAME HERE Take-home Final UWNetID: INSERT YOUR NETID Due to dropbox by 6pm PDT, Wednesday, December 14, 2011 The main part of the assignment (Problems 1 3) is worth 80 points.
More informationCommunication Engineering Prof. Surendra Prasad Department of Electrical Engineering Indian Institute of Technology, Delhi
Communication Engineering Prof. Surendra Prasad Department of Electrical Engineering Indian Institute of Technology, Delhi Lecture - 41 Pulse Code Modulation (PCM) So, if you remember we have been talking
More informationRejection of Data. Kevin Lehmann Department of Chemistry Princeton University
Reection of Data by Kevin Lehmann Department of Chemistry Princeton University Lehmann@princeton.edu Copyright Kevin Lehmann, 997. All rights reserved. You are welcome to use this document in your own
More informationSingle-Trial Neural Correlates. of Arm Movement Preparation. Neuron, Volume 71. Supplemental Information
Neuron, Volume 71 Supplemental Information Single-Trial Neural Correlates of Arm Movement Preparation Afsheen Afshar, Gopal Santhanam, Byron M. Yu, Stephen I. Ryu, Maneesh Sahani, and K rishna V. Shenoy
More informationThe Hilbert Transform
The Hilbert Transform David Hilbert 1 ABSTRACT: In this presentation, the basic theoretical background of the Hilbert Transform is introduced. Using this transform, normal real-valued time domain functions
More informationAdvanced 3G and 4G Wireless Communication Prof. Aditya K. Jagannatham Department of Electrical Engineering Indian Institute of Technology, Kanpur
Advanced 3G and 4G Wireless Communication Prof. Aditya K. Jagannatham Department of Electrical Engineering Indian Institute of Technology, Kanpur Lecture - 12 Doppler Spectrum and Jakes Model Welcome to
More information1 Using standard errors when comparing estimated values
MLPR Assignment Part : General comments Below are comments on some recurring issues I came across when marking the second part of the assignment, which I thought it would help to explain in more detail
More informationExtraction of Individual Tracks from Polyphonic Music
Extraction of Individual Tracks from Polyphonic Music Nick Starr May 29, 2009 Abstract In this paper, I attempt the isolation of individual musical tracks from polyphonic tracks based on certain criteria,
More information1.5 Continuity Continued & IVT
1.5 Continuity Continued & IVT A continuous function A non-continuous function To review the 3-step definition of continuity at a point, A function f ( x) is continuous at a point x = c if lim ( ) = (
More informationDifferent approaches to model wind speed based on stochastic differential equations
1 Universidad de Castilla La Mancha Different approaches to model wind speed based on stochastic differential equations Rafael Zárate-Miñano Escuela de Ingeniería Minera e Industrial de Almadén Universidad
More informationAvailable online at Paper ISSN International Journal of Energy Applications and Technologies
Available online at www.academicpaper.org Academic @ Paper ISSN 246-967 International Journal of Energy Applications and Technologies Vol. 3, Issue, pp. 9 3, 26 Research Article www.academicpaper.org/index.php/ijeat
More informationFiltering and Edge Detection
Filtering and Edge Detection Local Neighborhoods Hard to tell anything from a single pixel Example: you see a reddish pixel. Is this the object s color? Illumination? Noise? The next step in order of complexity
More information_Algebra 2 Marking Period 1
_Algebra 2 Marking Period 1 Topic Chapters Number of Blocks Dates Equations and Inequalities 1 8 9/9-9/27 PRE-TEST 1 9/27-10/2 Linear Relations and Functions 2 10 12/3-10/25 System of Equations and Inequalities
More informationLaboratory handouts, ME 340
Laboratory handouts, ME 340 This document contains summary theory, solved exercises, prelab assignments, lab instructions, and report assignments for Lab 4. 2014-2016 Harry Dankowicz, unless otherwise
More informationUnknown input observer based scheme for detecting faults in a wind turbine converter Odgaard, Peter Fogh; Stoustrup, Jakob
Aalborg Universitet Unknown input observer based scheme for detecting faults in a wind turbine converter Odgaard, Peter Fogh; Stoustrup, Jakob Published in: Elsevier IFAC Publications / IFAC Proceedings
More informationCheng Soon Ong & Christian Walder. Canberra February June 2018
Cheng Soon Ong & Christian Walder Research Group and College of Engineering and Computer Science Canberra February June 2018 Outlines Overview Introduction Linear Algebra Probability Linear Regression
More informationINTRODUCTION TO THE DFS AND THE DFT
ITRODUCTIO TO THE DFS AD THE DFT otes: This brief handout contains in very brief outline form the lecture notes used for a video lecture in a previous year introducing the DFS and the DFT. This material
More informationEnergy Resource Group, DIT
Energy Resource Group, DIT Wind Urchin: An Innovative Approach to Wind Resource Measurement Dr. Derek Kearney 11.05 am E: derek.kearney@dit.ie Introduction Energy Resource Group (ERG) The problem with
More informationDamage detection in wind turbine blades using time-frequency analysis of vibration signals
Dublin Institute of Technology From the SelectedWorks of Breiffni Fitzgerald Damage detection in wind turbine blades using time-frequency analysis of vibration signals Breiffni Fitzgerald, Dublin Institute
More informationEPPING HIGH SCHOOL ALGEBRA 2 Concepts COURSE SYLLABUS
Course Title: Algebra 2 Concepts Course Description Algebra 2 Concepts is designed for students who wish to take an Algebra 2 course at a non college prep level. The class will begin with a review of Algebra
More informationApplications. Remote Weather Station with Telephone Communications. Tripod Tower Weather Station with 4-20 ma Outputs
Tripod Tower Weather Station with 4-20 ma Outputs Remote Weather Station with Telephone Communications NEMA-4X Enclosure with Two Translator Boards and Analog Barometer Typical Analog Output Evaporation
More informationA system that is both linear and time-invariant is called linear time-invariant (LTI).
The Cooper Union Department of Electrical Engineering ECE111 Signal Processing & Systems Analysis Lecture Notes: Time, Frequency & Transform Domains February 28, 2012 Signals & Systems Signals are mapped
More informationNON-CAUSAL FIR FILTERS FOR THE MAXIMUM RETURN FROM CAPITAL MARKETS
NON-CAUSAL FIR FILTERS FOR THE MAXIMUM RETURN FROM CAPITAL MARKETS ANDRZEJ DYKA Gdańsk University of Technology Narutowicza 11/12, 80-952 Gdańsk, Poland In this paper we consider a trading strategy, which
More informationApplication of Neural Network for Long-Term Correction of Wind Data
Application of Neural Network for Long-Term Correction of Wind Data [2008-12-WD-004] Application of Neural Network for Long-Term Correction of Wind Data Franz Vaas and Hyun-Goo Kim*, ** Abstract Wind farm
More informationTowards an Optimal Noise Versus Resolution Trade-off in Wind Scatterometry
Towards an Optimal Noise Versus Resolution Trade-off in Wind Scatterometry Brent Williams Jet Propulsion Lab, California Institute of Technology IOWVST Meeting Utrecht Netherlands June 12, 2012 Copyright
More informationToward Isolation of Salient Features in Stable Boundary Layer Wind Fields that Influence Loads on Wind Turbines
Energies 5, 8, 977-3; doi:.339/en84977 OPEN ACCESS energies ISSN 996-73 www.mdpi.com/journal/energies Article Toward Isolation of Salient Features in Stable Boundary Layer Wind Fields that Influence Loads
More informationTopic 7. Convolution, Filters, Correlation, Representation. Bryan Pardo, 2008, Northwestern University EECS 352: Machine Perception of Music and Audio
Topic 7 Convolution, Filters, Correlation, Representation Short time Fourier Transform Break signal into windows Calculate DFT of each window The Spectrogram spectrogram(y,1024,512,1024,fs,'yaxis'); A
More informationSite Description: Tower Site
Resource Summary for Elizabeth Site Final Report Colorado Anemometer Loan Program Monitoring Period: 7/3/06 /26/07 Report Date: January, 0 Site Description: The site is.6 miles northeast of the town of
More informationEngineering Tripos Part IB. Part IB Paper 8: - ELECTIVE (2)
Engineering Tripos Part IB SECOND YEAR Part IB Paper 8: - ELECTIVE (2) MECHANICAL ENGINEERING FOR RENEWABLE ENERGY SYSTEMS Examples Paper 2 Wind Turbines, Materials, and Dynamics All questions are of Tripos
More information2.4 Real Zeros of Polynomial Functions
SECTION 2.4 Real Zeros of Polynomial Functions 197 2.4 Real Zeros of Polynomial Functions What you ll learn about Long Division and the Division Algorithm Remainder and Factor Theorems Synthetic Division
More informationProbabilistic forecasting of solar radiation
Probabilistic forecasting of solar radiation Dr Adrian Grantham School of Information Technology and Mathematical Sciences School of Engineering 7 September 2017 Acknowledgements Funding: Collaborators:
More informationConfidence Intervals. Confidence interval for sample mean. Confidence interval for sample mean. Confidence interval for sample mean
Confidence Intervals Confidence interval for sample mean The CLT tells us: as the sample size n increases, the sample mean is approximately Normal with mean and standard deviation Thus, we have a standard
More informationInvestigation of fan vibration
Investigation of fan vibration Jacques Muiyser 1, Frank Weissbuch 2, Trung Luu 3, Pascal Malpoix 3 and Hanno Reuter 1,3 1 Department of Mechanical and Mechatronic Engineering, Stellenbosch University 2
More informationWindcube TM Pulsed lidar wind profiler Overview of more than 2 years of field experience J.P.Cariou, R. Parmentier, M. Boquet, L.
Windcube TM Pulsed lidar wind profiler Overview of more than 2 years of field experience J.P.Cariou, R. Parmentier, M. Boquet, L.Sauvage 15 th Coherent Laser Radar Conference Toulouse, France 25/06/2009
More informationEvolution of the Average Synaptic Update Rule
Supporting Text Evolution of the Average Synaptic Update Rule In this appendix we evaluate the derivative of Eq. 9 in the main text, i.e., we need to calculate log P (yk Y k, X k ) γ log P (yk Y k ). ()
More information