Comparison of Induction and PM Synchronous Motor Drives for EV
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Direct Torque Control of Induction Motors
DIRECT TORQUE CONTROL FOR INDUCTION MOTOR DRIVES MAIN FEATURES OF DTC · Decoupled control of torque and flux · Absence of mechanical transducers · Current regulator, PWM pulse generation, PI control of flux and torque and co-ordinate transformation are not required · Very simple control scheme and low computational time · Reduced parameter sensitivity BLOCK DIAGRAM OF DTC SCHEME + _ s* s j s + Djs _ Voltage Vector s * T + j s DT Selection _ T S S S s Stator a b c Torque j s s E Flux vs 2 Estimator Estimator 3 s is 2 i b i a 3 Induction Motor In principle the DTC method selects one of the six nonzero and two zero voltage vectors of the inverter on the basis of the instantaneous errors in torque and stator flux magnitude. MAIN TOPICS Þ Space vector representation Þ Fundamental concept of DTC Þ Rotor flux reference Þ Voltage vector selection criteria Þ Amplitude of flux and torque hysteresis band Þ Direct self control (DSC) Þ SVM applied to DTC Þ Flux estimation at low speed Þ Sensitivity to parameter variations and current sensor offsets Þ Conclusions INVERTER OUTPUT VOLTAGE VECTORS I Sw1 Sw3 Sw5 E a b c Sw2 Sw4 Sw6 Voltage-source inverter (VSI) For each possible switching configuration, the output voltages can be represented in terms of space vectors, according to the following equation æ 2p 4p ö s 2 j j v = ç v + v e 3 + v e 3 ÷ s ç a b c ÷ 3 è ø where va, vb and vc are phase voltages. -
Single-Phase Line Start Permanent Magnet Synchronous Motor with Skewed Stator*
POWER ELECTRONICS AND DRIVES Vol. 1(36), No. 2, 2016 DOI: 10.5277/PED160212 SINGLE-PHASE LINE START PERMANENT MAGNET SYNCHRONOUS MOTOR WITH SKEWED STATOR* MACIEJ GWOŹDZIEWICZ, JAN ZAWILAK Wrocław University of Science and Technology, Wybrzeże Stanisława Wyspiańskiego 27, 50-370 Wrocław, Poland, e-mail: [email protected], [email protected] Abstract: The article deals with single-phase line start permanent magnet synchronous motor with skewed stator. Constructions of two physical motor models are presented. Results of the motors run- ning properties are analysed. Keywords: single-phase motor, permanent magnet, skew, vibration 1. INTRODUCTION Single-phase induction motors almost always have skewed rotors. It is a simple and effective solution in limitation of the motor vibration, noise and torque pulsation. In the case of line start permanent magnet synchronous motors skewed rotor is ex- tremely difficult to manufacture due to interior permanent magnets. Skewed stator is less complicated in comparison with skewed rotor [3], [4], [7], [8]. During many tests of single-phase line start permanent magnet synchronous motor physical models The authors noticed that vibration is one of the main drawbacks of these motors [1], [2]. It prompted them to construct and build a single-phase line start permanent magnet motor with skewed stator. 2. MOTOR CONSTRUCTION Two dimensional field-circuit models of the single-phase line start permanent magnet synchronous motor were applied in Maxwell software. The models are based on the mass production single-phase induction motor Seh 80-2B type: rated power Pn = 1.1 kW, rated voltage Un = 230 V, rated frequency fn = 50 Hz, number of pole * Manuscript received: September 7, 2016; accepted: December 7, 2016. -
The Fundamentals of Ac Electric Induction Motor Design and Application
THE FUNDAMENTALS OF AC ELECTRIC INDUCTION MOTOR DESIGN AND APPLICATION by Edward J. Thornton Electrical Consultant E. I. du Pont de Nemours Houston, Texas and J. Kirk Armintor Senior Account Sales Engineer Rockwell Automation The Woodlands, Texas Edward J. (Ed) Thornton is an Electrical Electrical Mechanical Consultant in the Electrical Technology Coupling System Field System Consulting Group in Engineering at DuPont, in Houston, Texas. His specialty is the design, operation, and maintenance of electric power distribution systems and large motor installations. He has 20 years E , I T , w of consulting experience with DuPont. Mr. Thornton received his B.S. degree Figure 1. Block Representation of Energy Conversion for Motors. (Electrical Engineering, 1978) from Virginia Polytechnic Institute and State University. The coupling magnetic field is key to the operation of electrical He is a registered Professional Engineer in the State of Texas. apparatus such as induction motors. The fundamental laws associated with the relationship between electricity and magnetism were derived from experiments conducted by several key scientists J. Kirk Armintor is a Senior Account in the 1800s. Sales Engineer in the Rockwell Automation Houston District Office, in The Woodlands, Basic Design and Theory of Operation Texas. He has 32 years’ experience with The alternating current (AC) induction motor is one of the most motor applications in the petroleum, rugged and most widely used machines in industry. There are two chemical, paper, and pipeline industries. major components of an AC induction motor. The stationary or He has authored technical papers on motor static component is the stator. The rotating component is the rotor. -
Abstract Controlling Ac Motor Using Arduino
ABSTRACT CONTROLLING AC MOTOR USING ARDUINO MICROCONTROLLER Nithesh Reddy Nannuri, M.S. Department of Electrical Engineering Northern Illinois University, 2014 Donald S Zinger, Director Space vector modulation (SVM) is a technique used for generating alternating current waveforms to control pulse width modulation signals (PWM). It provides better results of PWM signals compared to other techniques. CORDIC algorithm calculates hyperbolic and trigonometric functions of sine, cosine, magnitude and phase using bit shift, addition and multiplication operations. This thesis implements SVM with Arduino microcontroller using CORDIC algorithm. This algorithm is used to calculate the PWM timing signals which are used to control the motor. Comparison of the time taken to calculate sinusoidal signal using Arduino and CORDIC algorithm was also done. NORTHERN ILLINOIS UNIVERSITY DEKALB, ILLINOIS DECEMBER 2014 CONTROLLING AC MOTOR USING ARDUINO MICROCONTROLLER BY NITHESH REDDY NANNURI ©2014 Nithesh Reddy Nannuri A THESIS SUBMITTED TO THE GRADUATE SCHOOL IN PARTIAL FULFILLMENT OF THE REQUIREMENTS FOR THE DEGREE MASTER OF SCIENCE DEPARTMENT OF ELECTRICAL ENGINEERING Thesis Director: Dr. Donald S Zinger ACKNOWLEDGEMENTS I would like to express my sincere gratitude to Dr. Donald S. Zinger for his continuous support and guidance in this thesis work as well as throughout my graduate study. I would like to thank Dr. Martin Kocanda and Dr. Peng-Yung Woo for serving as members of my thesis committee. I would like to thank my family for their unconditional love, continuous support, enduring patience and inspiring words. Finally, I would like to thank my friends and everyone who has directly or indirectly helped me for their cooperation in completing the thesis. -
Electric Motors
SPECIFICATION GUIDE ELECTRIC MOTORS Motors | Automation | Energy | Transmission & Distribution | Coatings www.weg.net Specification of Electric Motors WEG, which began in 1961 as a small factory of electric motors, has become a leading global supplier of electronic products for different segments. The search for excellence has resulted in the diversification of the business, adding to the electric motors products which provide from power generation to more efficient means of use. This diversification has been a solid foundation for the growth of the company which, for offering more complete solutions, currently serves its customers in a dedicated manner. Even after more than 50 years of history and continued growth, electric motors remain one of WEG’s main products. Aligned with the market, WEG develops its portfolio of products always thinking about the special features of each application. In order to provide the basis for the success of WEG Motors, this simple and objective guide was created to help those who buy, sell and work with such equipment. It brings important information for the operation of various types of motors. Enjoy your reading. Specification of Electric Motors 3 www.weg.net Table of Contents 1. Fundamental Concepts ......................................6 4. Acceleration Characteristics ..........................25 1.1 Electric Motors ...................................................6 4.1 Torque ..............................................................25 1.2 Basic Concepts ..................................................7 -
Improvement of Electromagnetic Railgun Barrel Performance and Lifetime By
IMPROVEMENT OF ELECTROMAGNETIC RAILGUN BARREL PERFORMANCE AND LIFETIME BY METHOD OF INTERFACES AND AUGMENTED PROJECTILES A Thesis Presented to the Faculty of California Polytechnic State University San Luis Obispo In Partial Fulfillment of the Requirements for the Degree Master of Science in Aerospace Engineering by Aleksey Pavlov June 2013 c 2013 Aleksey Pavlov ALL RIGHTS RESERVED ii COMMITTEE MEMBERSHIP TITLE: Improvement of Electromagnetic Rail- gun Barrel Performance and Lifetime by Method of Interfaces and Augmented Pro- jectiles AUTHOR: Aleksey Pavlov DATE SUBMITTED: June 2013 COMMITTEE CHAIR: Kira Abercromby, Ph.D., Associate Professor, Aerospace Engineering COMMITTEE MEMBER: Eric Mehiel, Ph.D., Associate Professor, Aerospace Engineering COMMITTEE MEMBER: Vladimir Prodanov, Ph.D., Assistant Professor, Electrical Engineering COMMITTEE MEMBER: Thomas Guttierez, Ph.D., Associate Professor, Physics iii Abstract Improvement of Electromagnetic Railgun Barrel Performance and Lifetime by Method of Interfaces and Augmented Projectiles Aleksey Pavlov Several methods of increasing railgun barrel performance and lifetime are investigated. These include two different barrel-projectile interface coatings: a solid graphite coating and a liquid eutectic indium-gallium alloy coating. These coatings are characterized and their usability in a railgun application is evaluated. A new type of projectile, in which the electrical conductivity varies as a function of position in order to condition current flow, is proposed and simulated with FEA software. The graphite coating was found to measurably reduce the forces of friction inside the bore but was so thin that it did not improve contact. The added contact resistance of the graphite was measured and gauged to not be problematic on larger scale railguns. The liquid metal was found to greatly improve contact and not introduce extra resistance but its hazardous nature and tremendous cost detracted from its usability. -
Chapter # 2 Cylindrical Synchronous Generator and Motor 1
Benha University Electrical Engineering Department Faculty of Engineering at Shubra Electric Machines II Chapter # 2 Cylindrical Synchronous Generator and Motor 1. Introduction Synchronous machines are named by this name as their speed is directly related to the line frequency. Synchronous machines may be operated either as motor or generator. Synchronous generators are called alternators. Synchronous motors are used mainly for power factor correction when operate at no load. Synchronous machines are usually constructed with stationary stator (armature) windings that carrying the current and rotating rotor (field) winding that create the magnetic flux. This flux is produced by DC current from a separate source (e.g. DC shunt generator). 2. Types of Synchronous Generators The type of synchronous generators depends on the prime mover type as: a) Steam turbines: synchronous generators that driven by steam turbine are high speed machines and known as turbo alternators. The maximum rotor speed is 3600 rpm corresponding 60 Hz and two poles. b) Hydraulic turbines: synchronous generators that driven by water turbine are with speed varies from 50 to 500 rpm. The type of turbine to be used depends on the water head. For water head of 400m, Pelton wheel turbines are used. But for water head up to 350 m, Francis Turbines are used. For water head up to 50 m, Kaplan Turbines are used. 1 Chapter #2 Cylindrical Synchronous Machines Dr. Ahmed Mustafa Hussein Benha University Electrical Engineering Department Faculty of Engineering at Shubra Electric Machines II c) Diesel Engines: they are used as prime movers for synchronous generator of small ratings. For the type a) and c) the rotor shape is cylindrical as shown in Fig. -
Hybrid Synchronous Motor Electromagnetic Torque Research
MATEC Web of Conferences 19, 01026 (2014) DOI: 10.1051/matecconf/201419 01 026 C Owned by the authors, published by EDP Sciences, 2014 Hybrid synchronous motor electromagnetic torque research Elena E. Suvorkovaa, Lev K. Burulko National Research Tomsk Polytechnic University, 634050 Tomsk, Russia Abstract. Electromagnetic field distribution models in reluctance and permanent magnet parts were made by means of Elcut. Dependences of electromagnetic torque on torque angle were obtained. 1. Introduction Present-day position is inextricably connected with developing process in all components of electric drive: electrical machines, power semiconductors and converters on its base. One of the main electric motors development directions is expanding special motors’ construction range for applying in modern competitive object-orientated systems. Electric machines prospects of promotion lead to its non-traditional usage such as hybrid synchronous motor (HSM). HSM main principles of operation make it possible to use as executive engine in a number of production plants, such as artificial fiber production [1]. Electric drive projecting involves verification and regulation method choice which are determined by main electric machine characteristics. Thus main goals of this paper are hybrid synchronous motor air-gap magnetic field research and electromagnetic torque main parts determination. 2. Problem statement HSM is a machine with stator created on basis of serial asynchronous motor and rotor consisting on two parts. The main rotor part is a reluctance machine which is 70% of active rotor length [2], the other is synchronous permanent-magnet machine which is 30% [1]. Power is developed by reluctance machine as the cheapest and simple in design, and energy of constant magnets poles is used for increasing power and improving operational characteristics. -
Permanent Magnet Servomotor and Induction Motor Considerations
Permanent Magnet Servomotor and Induction Motor Considerations Kollmorgen B-104 PM Brushless Servomotor at 0.4 HP Kollmorgen M-828 PM Brushless Rotor Kollmorgen B-802 PM Brushless Servomotor at 15 HP Kollmorgen B-808 PM Brushless Rotor Permanent Magnet Servomotor and Induction Motor Considerations 1 Lee Stephens, Senior Motion Control Engineer Permanent Magnet Servomotor and Induction Motor Considerations Motion long considered a mainstay of induction motors, encroachment in the area of 50 HP and greater have been seen recently for some applications by permanent magnet (PM) servomotors. These applications usually have dynamic considerations that require position-time closed loop and high accelerations. When accelerating large loads, permanent magnet servomotors can work with very high load to inertia ratios and still maintain performance requirements. Having a lower inertia typically will allow for less permanent magnet motor can result in a greater torque energy wasted within the motor. Torque (τ), is the density than an equivalent induction system. If size product of inertia (j) and rotary acceleration (α). If you matters, then perhaps a system should use one require inertia matching, ½ of your energy is wasted technology over another. Speaking of size, the inertia accelerating the motor alone. If the inertia ratio from ratio can be an important figure of merit should motor to load is large, then control schemes must be dynamic needs arise. If you are going to have high dynamic enough to prevent the larger load from driving accelerations and decelerations, the size of the rotor the motor as opposed to the motor controlling the load. will significantly increase the inertia and decrease the Tradeoffs and knowing what can be negotiated. -
Hyperloop Accelerator Design Review
Hyperloop Accelerator Design Review TA: Benjamin Cahill ECE 445 February 25, 2015 Mohammad Jaber Michael Eraci Shivam Sharma Group #24 Table of Contents 1.0 Introduction............................................................................................................... 3 1.1 Statement of Purpose................................................................................. 3 1.2 Objectives...................................................................................................... 3 1.2.1 Benefits ........................................................................................... 3 1.2.2 Features .......................................................................................... 3 2.0 Design......................................................................................................................... 4 2.1 Block Diagram .............................................................................................. 4 2.2 Block Descriptions...................................................................................... 5 3.0 Schematics and Simulation .................................................................................. 6 3.1 Circuit Diagram ............................................................................................ 6 3.2 Control Flow Diagram ................................................................................ 7 3.3 Simulations ................................................................................................... 7 4.0 Requirements -
Rita MBAYED Contribution to the Control of the Hybrid Excitation
Année 2012 UNIVERSITE DE CERGY PONTOISE THESE Présentée pour obtenir le grade de DOCTEUR DE L’UNIVERSITE DE CERGY PONTOISE Ecole doctorale: Sciences et Ingénierie Spécialité: Génie Electrique Soutenance publique prévue le 12 Décembre 2012 Par Rita MBAYED Contribution to the Control of the Hybrid Excitation Synchronous Machine for Embedded Applications JURY Rapporteurs : Prof. Gérard CHAMPENOIS Université de Poitiers Prof. Eric SEMAIL Ecole Nationale d'Arts et Métiers ParisTech Examinateurs : Prof. Francis LABRIQUE Université Catholique de Louvain Prof. Mohamed GABSI Ecole Normale Supérieure Cachan Dr. Vincent LANFRANCHI Université de Technologie de Compiègne Directeur de thèse : Prof. Eric MONMASSON Université de Cergy Pontoise Co-directeurs : Prof. GeorgesSALLOUM Université Libanaise Dr. Lionel VIDO Université de Cergy Pontoise Laboratoire SATIE - UCP/UMR 8029, 1 rue d’Eragny, 95031 Neuville sur Oise France The secret is comprised in three words: Work, finish, publish. Michael Faraday Ere many generations pass, our machinery will be driven by a power obtainable at any point of the universe. This idea is not novel. Men have been led to it long ago by instinct or reason; it has been expressed in many ways, and in many places, in the history of old and new. We find it in the delightful myth of Antheus, who derives power from the earth; we find it among the subtle speculations of one of your splendid mathematicians and in many hints and statements of thinkers of the present time. Throughout space there is energy. Is this energy static or kinetic? If static our hopes are in vain; if kinetic - and this we know it is, for certain - then it is a mere question of time when men will succeed in attaching their machinery to the very wheelwork of nature. -
Linear Shaft Motor Vs
Linear Shaft Motor vs. Other Linear Technologies Linear Shaft Motor Traditionally, linear electric motors have been designed by Linear Shaft Motor “opening out flat” their rotary counterparts. For every rotary motor there is a linear motion counterpart, although the opposite of this No influence from Coil Magnets statement may not always be true. Thus, corresponding to the change in gap DC motor and AC induction, stepper and synchronous motor, we Standard Linear Motor have the Linear DC Motor (DCLM), Linear Induction Motor (LIM), Linear Pulse Motor (LPM), and Linear Synchronous Motor (LSM), respectively. Although this does provide a solution, a number of Cogging by concentration of flux inherent disadvantages arise. Absorption force Like the voice coil motor, the force velocity (FV) curve of the Linear Shaft Motor is a straight line from peak velocity to peak force. The Linear Shaft Motor’s FV curves are split into three regions. The first is what we call Continuous Force. It is the region in which the motor can operate indefinitely without the need for any external cooling, including heat sinks. The second is Acceleration Force, which is the amount of force that can be delivered by the motor for 40 seconds without the need for any external cooling. The third region, the Peak Force, is limited only by the power which can be supplied and the duty cycle. It is limited to 1 to 2 seconds. Your local Nippon Pulse application engineer can help you map this for your particular application. The Linear Shaft Motor is a very simple design that consists of a coil assembly (forcer), which encircles a patented round magnetic shaft.