SMALL WTND—POWERED ELECTRIC GENERATORS and SYSTEMS Vassilis Clitou Nicodemou, M.Sc. (Eng.) July 1979 a Thesis Submitted

Total Page:16

File Type:pdf, Size:1020Kb

SMALL WTND—POWERED ELECTRIC GENERATORS and SYSTEMS Vassilis Clitou Nicodemou, M.Sc. (Eng.) July 1979 a Thesis Submitted SMALL WTND—POWERED ELECTRIC GENERATORS AND SYSTEMS by Vassilis Clitou Nicodemou, M.Sc. (Eng.) July 1979 A thesis submitted for the degree of Doctor of Philosophy of the University of London and for the Diploma of Membership of the Imperial College of Science and Technology Department of Electrical Engineering Imperial College of Science and Technology London SW7 2AZ 2. ABSTRACT This thesis examines some electrical aspects of small wind power systems. The first part of the thesis deals briefly with the historical background and with a number of basic technical factors.. associated with wind power exploitation. The second part deals with generators for small wind plants and with aspects of the associated power and control circuits. In the final part, an energy yield estimation method is presented and used to compare a number of different schemes. Most of the second part concerns the design, manufacture_ and test of several specially built P.M. generators, but sections also deal with the operation and performance of generating systems based on wound field and capacitor-excited induction machines. Control and power matching aspects are considered. The four special P.M. machines comprise two low speed designs intended for direct coupling to windmill rotors and two ferrite-field machines designed primarily for operation with step-up transmissions. The disadvantages and advantages of a number of design features including choice of rated speed, P.M. material and layout are detailed. Preliminary results in part three of the thesis seem to show that the use of a P.M. generator increases energy yield by only 5-15% compared with that produced by a carefully-chosen wound field machine and that windmill design, windmill operating mode, site, etc. are likely to be more crucial factors in maximising energy yield per total capital cost. 3, 'ATLcpwµavo 6'6o0c ' yovctt µov xat oXouc oaouc ayacw zdao itoXŪ. Dedicated to my parents and all whom I love 4. "Gt;)cc t.~ ;.c ' Ē)cbe tpa ca)cbv f3o6~ ev0a ūĒ j ux'L%CJ V &Vtl1WV Ya-cgowe )cEXcu&a. xeivov ynp tatitnv rvēµwv 7cotnae Itpovtwv, Bjµ:v ;tr..utilEvat, 1jb' ōpvūµCV, Ov )c ' Ē,9gAtJat v." oi jpoY xep. I: (20). "be (Aeolus) gave it willingly and presented me with a leather bag, made from the flayed skin of a full-grown ox, in which he had imprisoned the boisterous energies of all the Winds. For you must know that Zeus has made him Warden of the Gales, with power to lay or rouse them each at will." Homer, Odysseia, X 5. ACKNOWLEDGEMENTS This work has been carried out under the supervision of Dr. H.R. Bolton. For the invaluable help, inspiration, as well as keen interest, valuable guidance and constant encouragement during the course of the work described in this thesis, the author expresses his sincere gratitude to Dr. Bolton. The author also gratefully acknowledges the valuable and stimulating discussions, useful suggestions and the keen interest maintained during the progress of this work by Dr. L.L. Freris. Thanks are also due to Dr. E.M,Freeman for his continuous encouragement and the active interest he maintained in the project. The author wishes to extend appreciation to all his colleagues in the Electrical Machines and Power Systems Section who kindly revised the typescript of this thesis, and especially to Dr. C. Papageorgiou, Dr. R.A. Ashen and Mr. I.K. Buehring, for their useful discussions and assistance. He would also like to acknowledge the help of Miss. E. Boden throughout the course of this work. The author greatly acknowledges the manufacturing work on the Mark I, Mark II and several test rigs carried out by Mr. R. Moore under the supervision of Mr. C. Jones in the Electrical Engineering Workshop at Imperial College. Thanks are also due to Messrs. R.B. Owen and C. Johnson for their practical assistance and advice during the work. The author wishes to thank'. the British Council and the S.R.C. for financial support of the project and a large number of individuals at Imperial College, Rutherford Laboratory, and elsewhere,, for their help, suggestions and opportunities for discussion. 6. Thanks for financial support are also due to a number of individuals, and in particular my parents. Finally, the author thanks Mr. R. Puddy for drawing the figures and Mrs. S. Murdock for typing the manuscript. 7. LIST OF CONTENTS Page Abstract 2 Acknowledgements 5 List of Contents 7 List of Principal Symbols 13 CHAPTER 1: INTRODUCTION 18 1.1 Brief Historical Review on the Future of Energy, 18 and Wind Power in Particular 1.2 Introduction to the Work described in the Thesis 22 CHAPTER 2: ENERGY RESOURCES AND REQUIREMENTS FOR 23 DOMESTIC APPLICATIONS 2.1 Introduction 23 2.2 Energy Resources and Energy Consumption for 23 Domestic Applications 2.3 Other Applications of Wind-powered Systems 30 CHAPTER 3: MACHINES AND SYSTEMS FOR TRANSFORMATION 36 OF WIND ENERGY INTO ELECTRICAL ENERGY 3.1 Introduction 36 3.2 Wind Power and Windmills 36 3.2.1 Available power in the wind 36 3.2.2 Windmill operation and characteristics 38 3.2.3 Types of windmills 44 3.2.4 Windmills for generation of electricity 49 3.3 Electrical Generators and Systems for Small-Scale 53 Wind Power Application 3.3.1 Effect of operating speed on generator 56 design 3.3.2 Use of special electric generators for 63 small-scale wind-powered systems 3.3.3 Control systems of wind-powered electric 71 generators for maximum extraction of power from the wind 3.4 Capacitor-excited Induction Generator 83 3.4.1 Wind-powered Induction Generator for 88 Maximum Extraction of Wind Power with Variable Capacitor Excitation 3.5 Concluding Remarks 94 8. Page CHAPTER 4: SMALL WIND-POWERED WOUND FIELD GENERATORS 95 4.1 Introduction 95 4.2 Rewinding the Armature of the Lorry Alternator 96 4.2.1 Details of the machine 97 4.2.2 Test rig 98 4.3 Tests on the Lorry Alternator 100 4.4 Results and Comments 102 4.4.1 No-load voltage (e.m.f.) Ef, versus field 102 current at constant rotational speed. (Magnetization curve.) 4.4.2 Iron, windage and friction losses (no-load 102 losses) versus field current at 1500 rev.min1 4.4.3 Armature winding temperature rise 104 4.4.4 Constant speed load characteristics of the 106 machine connected to a.c. and•d.c. resistive loads at 1500 rev.min-1 4.4.5 Load characteristics of the machine connected 111 to a d.c. load through a three-phase, half- controlled rectifier bridge 4.4.6 Effect of field current variation on the load 113 characteristics with and without diode bridge rectification 4.5 Operation with a Self-Excited Shunt-Connected Generator 115 4.5.1 Operation with generator 117 4.5.2 Effect of generator imperfections 121 4.5.3 Ideal performance curves 126 4.5.4 Generation using a self-excited generator 128 4.5.5 Determination of coefficient k 128 4.5.6 Experimental measurements 130 4.6 Field Tests on the Lorry Alternator 137 4.7 Concluding Remarks 139 CHAPTER 5: PERMANENT MAGNET ALTERNATORS: LOW SPEED TYPE WITH 140 CIRCUMFERENTIALLY-ORIENTATED PERMANENT MAGNETS ON THE ROTOR 5.1 Introduction 140 5.2 Review of Literature relating to Permanent Magnet Machines 140 5.3 Choice of Principal Features of the First Experimental 145 Generator for Wind Power Application 9. Page 5.4 Construction of the Mark I Circumferential Rotor 151 Permanent Magnet (P.M.) Alternator 5.4.1 Stator 151 5.4.2 Rotor 153 5.5 Theory 159 5.5.1 Geometry of the alternator 160 5.5.2 The equivalent circuit and phasor diagram of 162 the CRPMA connected to a resistive load 5.5.3 Calculation of the current I and voltage V 166 of the alternator from its phasor diagram 5.5.4 Synchronous reactances of the machine 169 5.5.5 Calculation of the direct-axis magnetizing 172 reactance X ad 5.5.6 Calculation of the quadrature-axis magnetizing 175 reactance X aq 5.5.7 Inductive leakage reactance of the alternator Xe 175 5.5.8 The resistance of the winding of the alternator 176 5.5.9 Equivalent magnetic circuit of the circumferential 177 rotor p.m. alternator at no-load 5.5.10, Magnetic circuit of the alternator and the 183 calculation of the resultant flux in the airgap for-on-load conditions 5.5.11 The e.m.f. of the armature winding of the 185 alternator 5.5.12 No-load e.m.f. of the alternator 186 5.5.13 Definition of the direct-axis demagnetizing 188 m.m.f. of a three-phase winding 5.5.14 The resultant e.m.f. in the airgap of the 189 alternator 5.6 Calculation of the Regulation, Output Power Curves, Load 191 Angle EL and Efficiency Characteristics of the Machine 5.7 Theoretical and Experimental .Results and their Correlation 192 5.8 Saturation of the Stator Teeth of the Alternator and its 197 Influence on the Performance 5.8.1 Calculation of the performance of the alternator 203 with lower line of return of the magnet 5.9 Tests on the Mark I P.M. Alternator 208 5.9.1 Test rig 209 5.9.2 Test procedures 211 5.10 Results and Discussion of Actual Performances of the Mark I 215 P.M. Alternator 5.10.1 Section A results (unskewed machine with 20 turns 215 per coil and an airgap of 0.41 mm) 10. Page 5.10.2 Section B results (unskewed machine with 20 turns 218 per coil and a new airgap of 0.483 mm) 5.10.3 Section C results (skewed machine with 21 turns 221 per coil and the airgap of 0.483 mm) 5.11 Design and Construction of the "Rutherford" Low Speed, 230 Permanent Magnet Alternator 5.11.1 Double—layer fractional—slot windings 236 5.11.2 Design of the double—layer fractional—slot 238 winding of the "Rutherford" p.m.
Recommended publications
  • Axial Field Permanent Magnet Machines with High Overload Capability for Transient Actuation Applications
    THE UNIVERSITY OF SHEFFIELD Axial field permanent magnet machines with high overload capability for transient actuation applications By Jiangnan Gong A Thesis submitted for the degree of Doctor of Philosophy Department of Electronic and Electrical Engineering The University of Sheffield. JANUARY 2018 ABSTRACT This thesis describes the design, construction and testing of an axial field permanent magnet machine for an aero-engine variable guide vane actuation system. The electrical machine is used in combination with a leadscrew unit that results in a minimum torque specification of 50Nm up to a maximum speed of 500rpm. The combination of the geometry of the space envelope available and the modest maximum speed lends itself to the consideration of an axial field permanent magnet machines. The relative merits of three topologies of double-sided permanent magnet axial field machines are discussed, viz. a slotless toroidal wound machine, a slotted toroidal machine and a yokeless axial field machine with separate tooth modules. Representative designs are established and analysed with three-dimensional finite element method, each of these 3 topologies are established on the basis of a transient winding current density of 30A/mm2. Having established three designs and compared their performance at the rated 50Nm point, further overload capability is compared in which the merits of the slotless machine is illustrated. Specifically, this type of axial field machine retains a linear torque versus current characteristic up to higher torques than the other two topologies, which are increasingly affected by magnetic saturation. Having selected a slotless machine as the preferred design, further design optimization was performed, including detailed assessment of transient performance.
    [Show full text]
  • PLL Approach to Mitigate Symmetrical Faults in Weak AC Grid of DFIG Based Wind Turbine for Voltage Stability Analysis
    International Journal of Electrical Electronics & Computer Science Engineering Volume 5, Issue 2 (April, 2018) | E-ISSN : 2348-2273 | P-ISSN : 2454-1222 Available Online at www.ijeecse.com PLL Approach to Mitigate Symmetrical Faults in Weak AC Grid of DFIG Based Wind Turbine for Voltage Stability Analysis Cholleti Sriram1, O. Rakesh2, M. Harish3, A. Sridhar4 1Assistant Professor, 2-4UG Scholars, EEE Department, Guru Nanak Institute of Technology, Hyderabad, India [email protected], [email protected] Abstract: Study of Instability issues of the grid-connected of wind turbines (WTs) based on doubly fed induction doubly fed induction generator (DFIG) based wind turbines generators (DFIG) that intends to improve its low- (WTs) during low-voltage ride-through (LVRT) have got voltage ride through(LVRT) capability. The main little attention yet. In this paper, the small-signal behavior of objective of this work is to design an algorithm that DFIG WTs attached to weak AC grid with high impedances would enable the system to control the initial over during the period of LVRT is investigated, with special attention paid to the rotor-side converter (RSC). Firstly, currents that appear in the generator during voltage based on the studied LVRT strategy, the influence of the sags, which can damage the RSC, without tripping it. high-impedance grid is summarized as the interaction As a difference with classical solutions, based on the between phase-looked loop (PLL) and rotor current installation of crowbar circuits, this operation mode controller (RCC). As modal analysis result indicates that the permits to keep the inverter connected to the generator, underdamped poles are dominated by PLL, complex torque something that would permit the injection of power to coefficient method (CTCM), which is conventionally applied the grid during the fault, as the new grid codes demand.
    [Show full text]
  • Doubly Fed Induction Motor
    © 2018 JETIR April 2018, Volume 5, Issue 4 www.jetir.org (ISSN-2349-5162) Doubly fed induction motor For speed control of motor 1 2 3 4 Rushikesh pandya , Hingrajiya jaydeep , Goswami rajan , Nandaniya hiral Sarvaiya kinjal5, 1 Assistant Professor 2, 3, 4, 5, students 1, 2, 3, 4, 5, Department of Electrical engineering Dr Subhash technical campus, junagadh, Gujarat, India Abstract—Doubly-fed electric machines are electric motors or electric generators where both the field magnet windings and armature windings are separately connected to equipment outside the machine. This is useful, for instance, for generators used in wind turbines. By feeding adjustable frequency AC power to the field windings, the magnetic field can be made to rotate, allowing variation in motor or generator speed. Index Terms—doubly fed induction motor, speed control, different regulator _____________________________________________________________________________________________________ I. INTRODUCTION a three-phase wound-rotor induction machine operates as a synchronous speed nS obtained during normal singly-fed synchronous machine when ac currents are fed into one set of operation. This is illustrated in Figure 8a. In this case, the windings and dc current is fed into the other set of windings. When resulting synchronous speed of the doubly-fed induction motor ac currents are fed into both the stator and rotor windings of a is equal to: three-phase wound-rotor induction machine, the machine also operates as a synchronous machine. In this situation, when the nS (DF) 120 × (fStator — fRotor) wound-rotor induction machine operates as a synchronous motor, it = is referred to as a doubly-fed induction motor since electrical NPoSe power from the power network is converted into mechanical power available at the machine shaft via both the stator and rotor Where nS (DF) is the synchronous speed of the windings of the machine.
    [Show full text]
  • Rotating DC Motors Part I
    Rotating DC Motors Part I The previous lesson introduced the simple linear motor. Linear motors have some practical applications, but rotating DC motors are much more prolific. The principles which explain the operation of linear motors are the same as those which explain the operation of practical DC motors. The fundamental difference between linear motors and practical DC motors is that DC motors rotate rather than move in a straight line. The same forces that cause a linear motor to move “right or left” in a straight line cause the DC motor to rotate. This chapter will examine how the linear motor principles can be used to make a practical DC motor spin. 16.1 Electrical machinery Before discussing the DC motor, this section will briefly introduce the parts of an electrical machine. But first, what is an electrical machine? An electrical machine is a term which collectively refers to motors and generators, both of which can be designed to operate using AC (Alternating Current) power or DC power. In this supplement we are only looking at DC motors, but these terms will also apply to the other electrical machines. 16.1.1 Physical parts of an electrical machine It should be apparent that the purpose of an electrical motor is to convert electrical power into mechanical power. Practical DC motors do this by using direct current electrical power to make a shaft spin. The mechanical power available from the spinning shaft of the DC motor can be used to perform some useful work such as turn a fan, spin a CD, or raise a car window.
    [Show full text]
  • The Design of Turbo Field Magnets for Alternate-Current Generators with Special Reference to Large Units at High Speeds
    1910.] WALKER: DESIGN OF TURBO FIELD MAGNETS. 319 THE DESIGN OF TURBO FIELD MAGNETS FOR ALTERNATE-CURRENT GENERATORS WITH SPECIAL REFERENCE TO LARGE UNITS AT HIGH SPEEDS. By MILES WALKER, Member. (Paper received November 10, 1909, and read in London on March 10, 1910.) SUMMARY. This paper re-opens the controversy, between the salient pole type of field magnet and the cylindrical type. Reasons are given why the latter type is better suited for obtaining the greatest possible output from a given diameter. The methods adopted by various makers of supporting the windings are described, and the possible limits of output considered. THE NECESSITY OF PROVIDING LARGE GENERATING UNITS OF HIGH SPEED. In the discussion which followed the paper by Dr. Kloss, " Practical Considerations in the Selection of Turbo Alternators," before the Manchester Section of the Institution of Electrical Engineers in November, 1908, an argument arose as to whether the field magnets of turbo-generators should be made with salient poles or should be of the cylindrical type with a distributed winding. Some difference of opinion exists among designers on this point, and each method has been adopted in quite a large number of successful turbo-generators. In the opinion of the author the matter is one of great importance, because, in the future, makers of turbo-generators will be called upon to build machines of larger capacity than ever before contemplated, and the makers of steam turbines to drive them will call for extremely high speeds, so that the turbo-generator of the future will have to be capable of giving an extremely large output from a diameter which is not excessive, and will have to be constructed in a manner which permits of a high factor of safety.
    [Show full text]
  • How Electric Motors Work by Marshall Brain Introduction to How Electric Motors Work
    How Electric Motors Work by Marshall Brain Introduction to How Electric Motors Work Electric motors are everywhere! In your house, almost every mechanical movement that you see around you is caused by an AC (alternating current) or DC (direct current) electric motor. A simple motor has six parts:Armature or rotor, Commutator, Brushes, Axle, Field magnet, DC power supply of some sort By understanding how a motor works you can learn a lot about magnets, electromagnets and electricity in general. In this article, you will learn what makes electric motors tick. Inside an Electric Motor An electric motor is all about magnets and magnetism: A motor uses magnets to create motion. If you have ever played with magnets you know about the fundamental law of all magnets: Opposites attract and likes repel. So if you have two bar magnets with their ends marked "north" and "south," then the north end of one magnet will attract the south end of the other. On the other hand, the north end of one magnet will repel the north end of the other (and similarly, south will repel south). Inside an electric motor, these attracting and repelling forces create rotational motion. In the above diagram, you can see two magnets in the motor: The armature (or rotor) is an electromagnet, while the field magnet is a permanent magnet (the field magnet could be anelectromagnet as well, but in most small motors it isn't in order to save power). Toy Motor The motor being dissected here is a simple electric motor that you would typically find in a toy.
    [Show full text]
  • GCSE Physics Edexcel Physics Magnetism, the Motor Effect And
    The PiXL Club The PiXL Club The PiXL Club The PiXL Club The PiXL Club The PiXL Club The PiXL Club The PiXL Club The PiXL Club The PiXL Club The PiXL Club The PiXL Club The PiXL Club The PiXL Club The PiXL Club The PiXL Club The PiXL Club The PiXL Club The PiXL Club The PiXL Club The PiXL Club The PiXL Club The PiXL Club The PiXL Club The PiXL Club The PiXL Club The PiXL Club The PiXL Club The PiXL Club The PiXL Club The PiXL Club The PiXL Club The PiXL Club The PiXL Club The PiXL Club The PiXL Club The PiXL Club The PiXL Club The PiXL Club The PiXL Club The PiXL Club The PiXL Club The PiXL Club The PiXL Club The PiXL Club XL Club The PiXL Club The PiXL Club The PiXL Club The PiXL Club The PiXL Club The PiXL Club The PiXL Club The PiXL Club The PiXL Club The PiXL Club The PiXL Club The PiXL Club The PiXL Club The PiXL Club The PiXL Club The PiXL Club The PiXL Club The PiXL Club The PiXL Club The PiXL Club The PiXL Club The PiXL Club The PiXL Club The PiXL Club The PiXL Club The PiXL Club The PiXL Club The PiXL Club The PiXL Club The PiXL Club The PiXL Club The PiXL Club The PiXL Club The PiXL Club The PiXL Club The PiXL Club The PiXL Club The PiXL Club The PiXL Club The PiXL Club The PiXL Club The PiXL Club The PiXL Club The PiXL Club The PiXL Club The PiXL Club The PiXL Club The PiXL Club The PiXL Club The PiXL Club The PiXL Club The PiXL Club The PiXL Club The PiXL Club The PiXL Club The PiXL Club The PiXL Club The PiXL Club The PiXL Club The PiXL Club The PiXL Club The PiXL Club The PiXL Club The PiXL Club The PiXL Club The PiXL Club
    [Show full text]
  • High Magnetic Fields for Fundamental Physics
    High magnetic fields for fundamental physics R´emy Battesti,1 Jerome Beard,1 Sebastian B¨oser,2 Nicolas Bruyant,1 Dmitry Budker,2, 3, 4, 5, ∗ Scott A. Crooker,6 Edward J. Daw,7 Victor V. Flambaum,2, 3, 8 Toshiaki Inada,9 Igor G. Irastorza,10 Felix Karbstein,11, 12 Dong Lak Kim,13 Mikhail G. Kozlov,14, 15 Ziad Melhem,16 Arran Phipps,17 Pierre Pugnat,18 Geert Rikken,1, y Carlo Rizzo,1, z Matthias Schott,2 Yannis K. Semertzidis,13, 19 Herman H. J. ten Kate,20 and Guido Zavattini21 1Laboratoire National des Champs Magn´etiquesIntenses (UPR 3228, CNRS-UPS-UGA-INSA), F-31400 Toulouse Cedex, France 2Johannes Gutenberg University, 55099 Mainz, Germany 3Helmholtz Institute Mainz, 55099 Mainz, Germany 4Department of Physics, University of California, Berkeley, Berkeley, California 94720- 7300, USA 5Nuclear Science Division, Lawrence Berkeley National Laboratory, Berkeley, California 94720-7300, USA 6National High Magnetic Field Laboratory, Los Alamos, New Mexico 87545, USA 7Department of Physics and Astronomy, The University of Sheffield, Hicks Building, Hounsfield Road, Sheffield S3 7RH, United Kingdom 8School of Physics, University of New South Wales, Sydney, New South Wales 2052, Australia 9International Center for Elementary Particle Physics, The University of Tokyo, 7-3-1 Hongo, Bunkyo, Tokyo 113-0033, Japan 10Grupo de Fisica Nuclear y Astroparticulas. Departamento de Fisica Teorica. Universidad de Zaragoza, 50009 Zaragoza, Spain 11Helmholtz-Institut Jena, Fr¨obelstieg 3, 07743 Jena, Germany 12Theoretisch-Physikalisches Institut, Abbe Center of Photonics, Friedrich-Schiller-Universit¨atJena, Max-Wien-Platz 1, 07743 Jena, Germany 13Center for Axion and Precision Physics Research, IBS, Daejeon 34051, Republic of Korea 14Petersburg Nuclear Physics Institute of NRC \Kurchatov Institute", Gatchina 188300, Russia 15St.
    [Show full text]
  • Unit 3 Electric Motors
    Unit 3 Electric motors Vocabulary Match the words with their Polish equivalents. 1. armature a) cewka, zezwój 2. axle b) wirnik 3. coil c) bocznik 4. field winding d) uzwojenie wzbudzające 5. induced voltage e) wał 6. permanent magnet f) moment obrotowy 7. resistor g) stojan 8. rotor h) napięcie indukowane 9. shaft i) twornik 10. shunt j) magnes trwały 11. stator k) uzwojenie 12. torque l) oś 13. winding m) opornik Lead-in In groups list applications of electric motors in common household. Electric motors quiz 1. The basis of an electric motor is: a) a spark plug b) magnets c) a battery 2. A motor's motion comes from which property of magnets? a) Like poles repel each other. b) Opposite poles attract each other. c) both A and B 3. The six basic parts of a simple two-pole motor are: a) the armature, the commutator, the brushes, the axle, a field magnet and a DC power supply b) the armature, the brushes, the battery, the axle, the anchor and a field magnet c) the commutator, the brushes, the casing, a DC power supply and the wires 4. A motor's armature acts as: a) a rotor b) an anchor c) an axle 5. When a small motor turns on, the armature spins because of: a) gravity b) magnetism c) inertia By Justyna Plezia and Magdalena Potręć (AGH UST) 1 For classroom use at AGH UST . You can distribute the copies in paper and electronic form among fellow teachers and second cycle students at AGH UST only.
    [Show full text]
  • Solenoids, Electromagnets and Electromagnetic Windings
    This is a reproduction of a library book that was digitized by Google as part of an ongoing effort to preserve the information in books and make it universally accessible. https://books.google.com Solenoids,electromagnetsandelectro-magneticwindings... CharlesReginaldUnderhill .<rw\ , M tit nc>o SOLENOIDS ELECTROMAGNETS AND ELECTROMAGNETIC WINDINGS BY CHARLES R: UNDERHILL CONSULTINg ELECTRICaL ENgINEER aSSOCIaTE MEMBER aMERICaN INSTITUTE OF ELECTRICaL ENgINEERS 223 ILLUSTRATIONS NEW YORK D. VAN NOSTRAND COMPANY 1910 COPYRIGHT, 1910, BY D. VAN NOSTRAND COMPANY. PREFACE Since nearly all of the phenomena met with in elec trical engineering in connection with the relations between electricity and magnetism are involved in the action of electromagnets, it is readily recognized that a careful study of this branch of design is necessary in order to predetermine any specific action. With the rapid development of remote electrical con trol, and kindred electro-mechanical devices wherein the electromagnet is the basis of the system, the want of accurate data regarding the design of electromagnets has long been felt. With a view to expanding the knowledge regarding the action of solenoids and electromagnets, the author made numerous tests covering a long period, by means of which data he has deduced laws, some of which have been published in the form of articles which appeared in the technical journals. In this volume the author has endeavored to describe the evolution of the solenoid and various other types of electromagnets in as perfectly connected a manner as possible. In view of the meager data hitherto obtainable it is believed that this book will be welcomed, not only by the electrical profession in general, but by the manu facturer of electrical apparatus as well.
    [Show full text]
  • (12) United States Patent (10) Patent No.: US 7,359,166 B2 Skauen (45) Date of Patent: Apr
    USOO7359166B2 (12) United States Patent (10) Patent No.: US 7,359,166 B2 Skauen (45) Date of Patent: Apr. 15, 2008 (54) METHOD AND CONTROL SYSTEM FOR 5,128,500 A * 7/1992 Hirschfeld .................. 2OOfS R CONTROLLING ELECTRIC MOTORS 5,189,412 A * 2/1993 Mehta et al. .......... 340/825.22 5,661,625 A * 8/1997 Yang ........................... 361.92 (75) Inventor: Ronny Skauen, Gressvik (NO) 6,169,648 B1* 1/2001 Denvir et al. ................. 361.25 6,234,100 B1* 5/2001 Fadeley et al. ......... 114/144 R (73) Assignee: Sleipner Motor AS, Fredrikstad (NO) 6,570,272 B2 * 5/2003 Dickhoff..................... 307 113 (*) Notice: Subject to any disclaimer,- 0 the term of this (Continued) patent is extended or adjusted under 35 FOREIGN PATENT DOCUMENTS U.S.C. 154(b) by 493 days. EP O 651 489 5, 1995 (21) Appl. No.: 10/618,265 (Continued) (22) Filed: Jul. 11, 2003 Primary Examiner Michael Sherry Assistant Examiner—Ann T. Hoang (65) Prior Publication Data (74) Attorney, Agent, or Firm—Lipsitz & McAllister LLC US 2004/OO85695A1 May 6, 2004 (57) ABSTRACT (30) Foreign Application Priority Data There is described a method for controlling an electric motor comprising an operating relay having relay windings with Oct. 30, 2002 (NO) ................................. 2002 52O7 respective first and second relay contacts and a control (51) Int. Cl. means, which motor via current conductors is connected to HO2H 7/08 (2006.01) said relay and a power source wherein an operator by using (52) U.S. Cl. ........................................................ 361A23 said control means controls the application of current to the (58) Field of Classification Search .................
    [Show full text]
  • Lecture 27: Doubly Fed Induction Motors
    Lecture 27: Doubly fed induction motors One of the most recent rotor-side-control schemes is the doubly fed induction generator. The method uses bi-directional AC-AC converters in the rotor circuit to control the currents injected into the rotor. The converters, being bi-directional, can be used to feed the rotor power back to the grid, reducing rotor power losses and surmounting the main drawback of the rotor resistance control. Doubly-fed electric machines are electric motors or electric generators where both the field magnet windings and armature windings are separately connected to equipment outside the machine. By feeding adjustable frequency AC power to the field windings, the magnetic field can be made to rotate, allowing variation in motor or generator speed. This is useful, for instance, for generators used in wind turbines. Doubly fed electrical generators are similar to AC electrical generators, but have additional features which allow them to run at speeds slightly above or below their natural synchronous speed. This is useful for large variable speed wind turbines, because wind speed can change suddenly. When a gust of wind hits a wind turbine, the blades try to speed up, but a synchronous generator is locked to the speed of the power grid and cannot speed up. So large forces are developed in the hub, gearbox, and generator as the power grid pushes back. This causes wear and damage to the mechanism. If the turbine is allowed to speed up immediately when hit by a wind gust, the stresses are lower and the power from the wind gust is converted to useful electricity.
    [Show full text]