Alasdair McDonald & Markus Mueller Edinburgh University

Slides:



Advertisements
Similar presentations
1. Induction Machines 1.1 Introduction
Advertisements

Superconducting and Conventional Machines A.M.Campbell IRC in Superconductivity Cambridge.
50Hz N S Load All Actions A1  A weight is balanced at equilibrium position of a spring and produce a Simple Harmonic Motion with acceleration Which.
Wind Turbine Session 4.
Lecture 30 November 4, 2013 ECEN 2060 Lecture 30 Fall 2013.
Advances in Condition Monitoring – Linking the Input to the Output Martin Jones Insensys.
Electric Motors and Generators
Staffan Engström, Ägir Konsult AB Stefan Lindgren, VG Power AB
Department of Electrical Engineering Southern Taiwan University Robot and Servo Drive Lab. 2015/5/19 Reduction of Torque Ripple Due to Demagnetization.
October 30, 2007 © SKF Group Slide 0. Why is there no ideal bearing concept EWEC 2012 Presented by Reiner Wagner, Application Engineering Manager Renewable.
® A MAGNETICALLY-GEARED COMPACT 3MW DIRECT DRIVE GENERATOR EWEC 2010.
1 Florence Libert NORPIE 2004 Design Study of Different Direct-Driven Permanent–Magnet Motors for a Low Speed Application.
Overview of different wind generator systems and their comparisons 2-4~2-7 陳昱希.
AC Machine.
When two gears make contact at the Pitch Point, the areas of contact on the face of each gear will have the same instantaneous tangential velocity Vt.
Alternate Energy Activities A look at Wind Power.
PARMENANT MAGNET SYNCHRONOUS GENERATOR BY JA’FAR R.A. AZIM Assem M.A. Al ighrair.
Superconducting Generators for Wind Turbines Abrahem Al-afandi Hamad Almutawa Majed Ataishi Advisor & Client Dr. James McCalley 1.
Importance of advanced simulations of electrical system in wind turbines April 2010.
PMSM Design and Loss Analysis Liping Zheng 07/23/2003.
PMSM at the Cryogenic Temperature
Introduction to Electrical Machines
THE POWER OF THE WIND. The wind: a key factor in world economy Wind needs clean, renewable and competitive sources of energy; wind is a very competitive.
1 11 A review of wind energy technologies part two. Adviser : Dr. Yuan-Kang Wu Student : Po-Kai Lin Date :
WIND POWER. Introduction  Energy is a major input for overall socio- economic development of any society  The prices of the fossil fuels steeply increasing.
Reciprocating Saw Dissection: Motor Description Thomas Snowdon.
Compound Gears Unit 6.
INTRODUCTION  The higher current density achievable in many superconducting materials tends to make them smaller compared with non- superconducting machines.
APEX Institute of Technology &Management Mr. SAURAV KUMAR (EEE # ) Mr. GAURAV KUMAR (ECE # ) B.TECH. PROJECT PRESENTATION-2012 [1]
Renewable Energy Research Laboratory University of Massachusetts Wind Energy: State-of-the Art and Future Trends Southwest Renewable Energy Conference.
Dr. Longya Xu The Ohio State University April, 2010.
Three-phase Cage Rotor Induction Motors Resource 2 Three-Phase AC machines.
MODELING AND SIMULATION OF WIND TURBINE –DOUBLY FED INDUCTION GENERATOR (WT-DFIG) IN WIND FARM USE MATLAB/SIMPOWERSYSTEM Student : TRUONG XUAN LOC.
Study of TFPM machines with toothed rotor applied to direct-drive generators for wind turbines Maxime R. Dubois LEEPCI, Dept. of Electrical Engineering.
Electric Machine Introduction
How do wind turbines work? A wind turbine looks closely to a household fan but very larger. The huge blades move slowly against the wind.
Superconducting Generators for Large Wind Turbines Markus Mueller Ozan Keysan – Joe Burchell Institute for Energy.
Electricity and Magnetism Magnetism is the force of attraction or repulsion of magnetic materials.  Magnets are surrounded by a magnetic field that applies.
Wind Energy. How does wind energy work? The wind blows on the blades and makes them turn. The blades turns a shaft inside the nacelle (the box at the.
Energy for people, energy for enterprise, energy for life Presentation to SEI: Renewable Energy for the Developing World Carbondale, CO - June 17, 2009.
Magnetic field due to an electric current
NORPIE June, Trondheim, Norway Analysis of a PM Machine with Concentrated Fractional Pitch Windings Freddy Magnussen, Dmitry Svechkarenko, Peter.
INDUCTION MOTOR.
Aerodynamic forces on the blade, COP, Optimum blade profiles
Future Electrical Generator Technologies for Offshore Wind Turbines Dennis Morosoff The Siberian Federal University.
CONSTRUCTION  The dc machines used for industrial electric drives have three major parts. Field system Armature and Commutator. Field system  The field.
INTRODUCTION TO ROBOTICS Part 3: Propulsion System Robotics and Automation Copyright © Texas Education Agency, All rights reserved. 1.
Study the following :  Theory of the induction motors (single and three phase).  Methods of speed control of induction motors.  Circuit diagram.
DC MOTOR. Magnetism Opposites Attract / Likes Repel.
Department of Electrical Engineering Southern Taiwan University Robot and Servo Drive Lab. 2016/6/13 Design of a Synchronous Reluctance Motor Drive T.
Induction Motor (Asynchronous Motor)
 How does a windmill create energy?.  You should be able to understand the purpose of gearing in a windmill.  You should understand how electricity.
Miscellaneous Hydraulic Machine
A Field Construction Technique to Efficiently Model the Dynamic Vector Forces within Induction Machines Dezheng Wu, Steve Pekarek School of Electrical.
CNC FEED DRIVES.
Equations, Performance, Electrical Equivalent Circuits
Electric Motors and Generators
VERTICAL AXIS WIND TURBINE:
Electric Machine Induction Motor
RECIPROCATING COMPRESSORS BY DEEPA M S VARUNA TANDON
Electric Machine Introduction
Wind turbine technology
Axial Flux Core Technology
Equivalent Circuit of a Single Phase Induction Motor
H. Polinder, S.W.H. de Haan, J.G. Slootweg, M.R. Dubois
Permanent Magnet Synchronous Motors
ME 252 Thermal-Fluid Systems G. Kallio
Equations, Performance, Electrical Equivalent Circuits
Motor Applications.
Presentation transcript:

Alasdair McDonald & Markus Mueller Edinburgh University Structural Mass in Direct-drive Permanent Magnet Electrical Generators Alasdair McDonald & Markus Mueller Edinburgh University Henk Polinder Delft University of Technology alasdair.mcdonald@ed.ac.uk

Direct-drive electrical generators McDonald, Mueller & Polinder, Structural mass in direct-drive permanent magnet electrical generators Direct-drive electrical generators Direct-drive Advantages and challenges Reducing generator mass Normal methods, looking at ‘active’ material What is structural mass? How can we include it? How can we reduce structural mass in the generators.

Advantages of direct-drive McDonald, Mueller & Polinder, Structural mass in direct-drive permanent magnet electrical generators Advantages of direct-drive Reliability and maintenance Efficiency Direct drive Geared DFIG Efficiency Power

Direct-drive difficulties McDonald, Mueller & Polinder, Structural mass in direct-drive permanent magnet electrical generators Direct-drive difficulties T ω Gearbox steps up speed and steps down torque Power = torque x speed T ω Direct-drive means that generator must produce large torque Torque = 2 x π x R2 x l x τ Need large radius, R or large shear stress, τ Large and heavy generator l R τ

Reducing generator mass McDonald, Mueller & Polinder, Structural mass in direct-drive permanent magnet electrical generators Reducing generator mass Active mass Optimise within each generator topology Compare different generator topology types But active mass is only third of total mass Structural mass Model structural mass, integrate into optimisation Generator topologies with reduced forces Structural shape optimisation Lightweight materials

Optimise within each generator topology McDonald, Mueller & Polinder, Structural mass in direct-drive permanent magnet electrical generators Optimise within each generator topology Copper Steel Permanent Magnet Maximise the torque density by reducing copper, steel and permanent magnet material

Choose different topology types McDonald, Mueller & Polinder, Structural mass in direct-drive permanent magnet electrical generators Choose different topology types Permanent magnet and electrically-excited topologies Axial-flux, radial-flux and transverse-flux topologies

Address structural mass McDonald, Mueller & Polinder, Structural mass in direct-drive permanent magnet electrical generators Address structural mass Structural mass maintains airgap clearance between rotor and stator, does not play an active role in electromagnetic circuits A number of forces at play: Shear stress Normal stress Forces from rotor blades Weight of active material Thermal stresses

Shear stress Shear stress is the useful torque-producing force McDonald, Mueller & Polinder, Structural mass in direct-drive permanent magnet electrical generators Shear stress Shear stress is the useful torque-producing force Rotor structure must transmit torque from rotor shaft to airgap Stator structure also experiences shear stress Increasing shear stress gives smaller machine

Normal stress Normal stress, q acts to close air gap clearance McDonald, Mueller & Polinder, Structural mass in direct-drive permanent magnet electrical generators Normal stress B 2 φ q = g B 2μ g o Normal stress, q acts to close air gap clearance It can be an order of magnitude bigger than shear stress Shear stress = f (Bg); Normal stress = f (Bg2) Copper Steel PM

Normal stress modelling McDonald, Mueller & Polinder, Structural mass in direct-drive permanent magnet electrical generators Normal stress modelling Simple analytical models used early on in design process Axial-flux machines: rotor and stator structure modelled as circular discs Radial-flux type machines: rotor and stator structures modelled as disc and wheel structures Stress, q Stress, q

Forces from the rotor blades McDonald, Mueller & Polinder, Structural mass in direct-drive permanent magnet electrical generators Forces from the rotor blades Yaw error, wind shear, aeroelastic vibrations, blade weight Depends on connection to rotor blades and bearing arrangement “Static” and dynamic Effects shear and normal stress Ripe for further investigation, not modelled here

McDonald, Mueller & Polinder, Structural mass in direct-drive permanent magnet electrical generators Gravity Weight of active and structural material can deflect rotor and stator structures Can be modelled in disc and wheel structures

Centripetal and thermal effects McDonald, Mueller & Polinder, Structural mass in direct-drive permanent magnet electrical generators Centripetal and thermal effects Centripetal acceleration can deflect rotor cylinder into airgap. Differences in rotor and stator temperature rise can lead to closing/opening of airgap.

Active and structural mass McDonald, Mueller & Polinder, Structural mass in direct-drive permanent magnet electrical generators Active and structural mass Active mass Structural mass

McDonald, Mueller & Polinder, Structural mass in direct-drive permanent magnet electrical generators Air-cored machines

Air-cored machines Axial-flux machines 2, 3 and 5 MW machines McDonald, Mueller & Polinder, Structural mass in direct-drive permanent magnet electrical generators Air-cored machines Axial-flux machines 2, 3 and 5 MW machines 2 different aspect ratio, kr = 0.7 and kr = 0.9

Iron- and air-cored machines McDonald, Mueller & Polinder, Structural mass in direct-drive permanent magnet electrical generators Iron- and air-cored machines Iron-cored machines: Bg = 0.9 T, shear stress = 45 kN/m2 and normal stress = 320 kN/m2. Small radius. Air-cored machines: Bg = 0.5 T, shear stress = 25 kN/m2 and normal = 100 kN/m2. Larger radius.

McDonald, Mueller & Polinder, Structural mass in direct-drive permanent magnet electrical generators Air-cored results For greater power ratings, structural mass is a greater percentage of total mass. Structural mass will become more important. When including structural mass, kr = 0.7 is lighter and cheaper than when kr = 0.9. Need to include structural mass in decision making. Air-cored machines are lighter than iron-cored machines. Air-cored machines are larger. Air-cored machines have about 50% more copper, iron and PM than the iron-cored machines and are more expensive.

McDonald, Mueller & Polinder, Structural mass in direct-drive permanent magnet electrical generators Evolutionary methods Rotor ? Stator ?

Use of lightweight materials McDonald, Mueller & Polinder, Structural mass in direct-drive permanent magnet electrical generators Use of lightweight materials Composite materials are used in wind turbine blades and other weight sensitive structures Why not use materials with high E/ρ in electric machine structures?

Summary We can reduce generator mass McDonald, Mueller & Polinder, Structural mass in direct-drive permanent magnet electrical generators Summary We can reduce generator mass Using normal methods, looking at ‘active’ material By addressing structural mass. Shown how this can be linked to the active material design. Including structural mass changes our decision making. Air-cored generators, structural optimisation and lightweight materials may help further reduce generator mass.