The ABC's of Synchronous Motors
Total Page:16
File Type:pdf, Size:1020Kb
Load more
Recommended publications
-
The Role of MHD Turbulence in Magnetic Self-Excitation in The
THE ROLE OF MHD TURBULENCE IN MAGNETIC SELF-EXCITATION: A STUDY OF THE MADISON DYNAMO EXPERIMENT by Mark D. Nornberg A dissertation submitted in partial fulfillment of the requirements for the degree of Doctor of Philosophy (Physics) at the UNIVERSITY OF WISCONSIN–MADISON 2006 °c Copyright by Mark D. Nornberg 2006 All Rights Reserved i For my parents who supported me throughout college and for my wife who supported me throughout graduate school. The rest of my life I dedicate to my daughter Margaret. ii ACKNOWLEDGMENTS I would like to thank my adviser Cary Forest for his guidance and support in the completion of this dissertation. His high expectations and persistence helped drive the work presented in this thesis. I am indebted to him for the many opportunities he provided me to connect with the world-wide dynamo community. I would also like to thank Roch Kendrick for leading the design, construction, and operation of the experiment. He taught me how to do science using nothing but duct tape, Sharpies, and Scotch-Brite. He also raised my appreciation for the artistry of engineer- ing. My thanks also go to the many undergraduate students who assisted in the construction of the experiment, especially Craig Jacobson who performed graduate-level work. My research partner, Erik Spence, deserves particular thanks for his tireless efforts in modeling the experiment. His persnickety emendations were especially appreciated as we entered the publi- cation stage of the experiment. The conversations during our morning commute to the lab will be sorely missed. I never imagined forging such a strong friendship with a colleague, and I hope our families remain close despite great distance. -
Appendix B: Soft Starter Application Considerations BBB
AAPPENDIXPPENDIX APPENDIX B: SOFT STARTER APPLICATION CONSIDERATIONS BBB TABLE OF CONTENTS Appendix B: Soft Starter Application Considerations �� � � � � � � � � � � � � � � � � � � � � � � B–1 B�1 – Motor Suitability and Associated Considerations� � � � � � � � � � � � � � � � � � � � � B–2 B�1�1 – Suitability� � � � � � � � � � � � � � � � � � � � � � � � � � � � � � � � � � � � � � � � � � � � � � B–2 B�1�2 – Induction Motor Characteristics �� � � � � � � � � � � � � � � � � � � � � � � � � � � � � � � � � B–2 B�1�3 – Rating� � � � � � � � � � � � � � � � � � � � � � � � � � � � � � � � � � � � � � � � � � � � � � � � B–2 B�1�4 – Maximum Motor Cable Length� � � � � � � � � � � � � � � � � � � � � � � � � � � � � � � � � � B–3 B�1�5 – Power Factor Correction Capacitors �� � � � � � � � � � � � � � � � � � � � � � � � � � � � � � � B–3 B�1�6 – Lightly Loaded Small Motors � � � � � � � � � � � � � � � � � � � � � � � � � � � � � � � � � � � B–3 B�1�7 – Motors Installed with Integral Brakes � � � � � � � � � � � � � � � � � � � � � � � � � � � � � � B–3 B�1�8 – Older Motors� � � � � � � � � � � � � � � � � � � � � � � � � � � � � � � � � � � � � � � � � � � � B–3 B�1�9 – Wound-rotor or Slip-ring Motors � � � � � � � � � � � � � � � � � � � � � � � � � � � � � � � � B–3 B�1�10 – Enclosures � � � � � � � � � � � � � � � � � � � � � � � � � � � � � � � � � � � � � � � � � � � � B–3 B�1�11 – Efficiency �� � � � � � � � � � � � � � � � � � � � � � � � � � � � � � � � � � � � � � � � � � � � � B–4 B�1�12 – High-Efficiency Motors � � � � � � -
Parameters Effects on Force in Tubular Linear Induction Motors with Blocked Rotor
Proc. of the 5th WSEAS/IASME Int. Conf. on Electric Power Systems, High Voltages, Electric Machines, Tenerife, Spain, December 16-18, 2005 (pp92-97) Parameters Effects on Force in Tubular Linear Induction Motors with Blocked Rotor REZA HAGHMARAM(1,2), ABBAS SHOULAIE(2) (1) Department of Electrical Engineering, Imam Hosein University, Babaie Highway, Tehran (2) Department of Electrical Engineering, Iran University of Science & Technology, Narmak, Tehran IRAN Abstract: This paper is concerned with the study of several parameters effects on longitudinal force applied on the rotor in the generator driven air-core tubular linear induction motors with blocked rotor. With developing the motor modeling by involving temperature equations in the previous computer code, we first study variations of the coils and rings temperatures and the effect of the temperature on the rotor force. In the next section, the effect of the rotor length on the rotor force is studied and it is shown that there is an almost linear relation between the rotor length and the rotor force. Finally we have given the optimum time step for solving the state equations of the motor and calculating the force. By this time step the code will have reasonable speed and accuracy. These studies can be useful for the force motors and for finding a view for dynamic state analysis of the acceleration motors. Keywords: - Air Core Tubular Linear Induction Motor, Coilgun, Linear Induction Launcher 1 Introduction the value of coils and rings currents and calculating Tubular Linear Induction Motors (TLIMs) may the gradient of mutual inductance between coils and have unique applications as electromagnetic rings, we can calculate the force applied on the launchers with very high speed and acceleration rotor [3]. -
Performance of Superconductor Dynamic Synchronous Condenser on an Electric Grid Swarn Kalsi, David Madura and Mike Ross1
2005 IEEE/PES Transmission and Distribution Conference & Exhibition: Asia and Pacific 1 Dalian, China Performance of Superconductor Dynamic Synchronous Condenser on an Electric Grid Swarn Kalsi, David Madura and Mike Ross1 Abstract — High-temperature superconductor (HTS) dynamic synchronous condensers have been developed for applications in II. INTRODUCTION an electric grid. The HTS dynamic synchronous condensers, also hile conventional dynamic synchronous condensers based called SuperVAR®, are similar to conventional synchronous W condensers, but the copper field winding has been replaced with on copper field coils have been widely used in the power an HTS field winding. The HTS dynamic synchronous grid, their relatively low efficiency has limited their potential condensers have some very attractive features, such as a small applications, and their lifetime has been limited by insulation footprint, transportability, high reliability, and peak and degradation caused by field current heating during cyclic dynamic reactive compensation capability for leading or lagging operation. They have been replaced by electronic solutions VARS. These HTS dynamic synchronous condenser machines such as Static VAR Compensators (SVCs), and Flexible AC are also inherently stable to close-in faults and can provide up to Transmission System (FACTS) devices. Although other twice the nominal rating for about one minute (peak rating) during depressed voltage events. These machines also use about reactive compensation devices, such as SVC are capable of one-half -
Based Resources Into Low Short Circuit Strength Systems Reliability Guideline
Integrating Inverter- Based Resources into Low Short Circuit Strength Systems Reliability Guideline December 2017 NERC | Report Title | Report Date I Table of Contents Preface ...................................................................................................................................................................... iv Preamble .................................................................................................................................................................... v Acknowledgements ................................................................................................................................................... vi Executive Summary .................................................................................................................................................. vii Introduction .............................................................................................................................................................. ix Qualitative Description of System Strength ........................................................................................................... x Variable Energy Resources ..................................................................................................................................... x Wind Turbine Generator Technologies ............................................................................................................. xi Solar Photovoltaic Generator Technologies ................................................................................................... -
Pulsed Rotating Machine Power Supplies for Electric Combat Vehicles
Pulsed Rotating Machine Power Supplies for Electric Combat Vehicles W.A. Walls and M. Driga Department of Electrical and Computer Engineering The University of Texas at Austin Austin, Texas 78712 Abstract than not, these test machines were merely modified gener- ators fitted with damper bars to lower impedance suffi- As technology for hybrid-electric propulsion, electric ciently to allow brief high current pulses needed for the weapons and defensive systems are developed for future experiment at hand. The late 1970's brought continuing electric combat vehicles, pulsed rotating electric machine research in fusion power, renewed interest in electromag- technologies can be adapted and evolved to provide the netic guns and other pulsed power users in the high power, maximum benefit to these new systems. A key advantage of intermittent duty regime. Likewise, flywheels have been rotating machines is the ability to design for combined used to store kinetic energy for many applications over the requirements of energy storage and pulsed power. An addi - years. In some cases (like utility generators providing tran- tional advantage is the ease with which these machines can sient fault ride-through capability), the functions of energy be optimized to service multiple loads. storage and power generation have been combined. Continuous duty alternators can be optimized to provide Development of specialized machines that were optimized prime power energy conversion from the vehicle engine. for this type of pulsed duty was needed. In 1977, the laser This paper, however, will focus on pulsed machines that are fusion community began looking for an alternative power best suited for intermittent and pulsed loads requiring source to capacitor banks for driving laser flashlamps. -
An Engineering Guide to Soft Starters
An Engineering Guide to Soft Starters Contents 1 Introduction 1.1 General 1.2 Benefits of soft starters 1.3 Typical Applications 1.4 Different motor starting methods 1.5 What is the minimum start current with a soft starter? 1.6 Are all three phase soft starters the same? 2 Soft Start and Soft Stop Methods 2.1 Soft Start Methods 2.2 Stop Methods 2.3 Jog 3 Choosing Soft Starters 3.1 Three step process 3.2 Step 1 - Starter selection 3.3 Step 2 - Application selection 3.4 Step 3 - Starter sizing 3.5 AC53a Utilisation Code 3.6 AC53b Utilisation Code 3.7 Typical Motor FLCs 4 Applying Soft Starters/System Design 4.1 Do I need to use a main contactor? 4.2 What are bypass contactors? 4.3 What is an inside delta connection? 4.4 How do I replace a star/delta starter with a soft starter? 4.5 How do I use power factor correction with soft starters? 4.6 How do I ensure Type 1 circuit protection? 4.7 How do I ensure Type 2 circuit protection? 4.8 How do I select cable when installing a soft starter? 4.9 What is the maximum length of cable run between a soft starter and the motor? 4.10 How do two-speed motors work and can I use a soft starter to control them? 4.11 Can one soft starter control multiple motors separately for sequential starting? 4.12 Can one soft starter control multiple motors for parallel starting? 4.13 Can slip-ring motors be started with a soft starter? 4.14 Can soft starters reverse the motor direction? 4.15 What is the minimum start current with a soft starter? 4.16 Can soft starters control an already rotating motor (flying load)? 4.17 Brake 4.18 What is soft braking and how is it used? 5 Digistart Soft Starter Selection 5.1 Three step process 5.2 Starter selection 5.3 Application selection 5.4 Starter sizing 1. -
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. -
LECTURE NOTES on Utilization of Electrical Energy & Traction
LECTURE NOTES ON Utilization of Electrical Energy & Traction Name of the course: Diploma in Electrical Engineering. (6th Semester) Notes Prepared by: HIMANSU BHUSAN BEHERA Designation : LECTURER IN ELECTRICAL College : UTKALMANI GOPABANDHU INSTITUTE OF ENGINEERING, ROURKELA CHAPTER-1 ELECTROLYSIS Definition and Basic principle of Electro Deposition. Electro deposition is the process of coating a thin layer of one metal on top of different metal to modify its surface properties. It is done to achieve the desire electrical and corrosion resistance, reduce wear &friction, improve heat tolerance and for decoration. Electroplating Basics Fig-1. Electrochemical Plating Figure- 1, schematically illustrates a simple electrochemical plating system. The ―electro‖ part of the system includes the voltage/current source and the electrodes, anode and cathode, immersed in the ―chemical‖ part of the system, the electrolyte or plating bath, with the circuit being completed by the flow of ions from the plating bath to the electrodes. The metal to be deposited may be the anode and be ionized and go into solution in the electrolyte, or come from the composition of the plating bath. Copper, tin, silver and nickel metal usually comes from anodes, while gold salts are usually added to the plating bath in a controlled process to maintain the composition of the bath. The plating bath generally contains other ions to facilitate current flow between the electrodes. The deposition of metal takes place at the cathode. The overall plating process occurs in the following sequence: 1. Power supply pumps electrons into the cathode. 2. An electron from the cathode transfers to a positively charged metal ion in the solution and the reduced metal plates onto the cathode. -
THE ULTIMATE Tesla Coil Design and CONSTRUCTION GUIDE the ULTIMATE Tesla Coil Design and CONSTRUCTION GUIDE
THE ULTIMATE Tesla Coil Design AND CONSTRUCTION GUIDE THE ULTIMATE Tesla Coil Design AND CONSTRUCTION GUIDE Mitch Tilbury New York Chicago San Francisco Lisbon London Madrid Mexico City Milan New Delhi San Juan Seoul Singapore Sydney Toronto Copyright © 2008 by The McGraw-Hill Companies, Inc. All rights reserved. Manufactured in the United States of America. Except as permitted under the United States Copyright Act of 1976, no part of this publication may be reproduced or distributed in any form or by any means, or stored in a database or retrieval system, without the prior written permission of the publisher. 0-07-159589-9 The material in this eBook also appears in the print version of this title: 0-07-149737-4. All trademarks are trademarks of their respective owners. Rather than put a trademark symbol after every occurrence of a trademarked name, we use names in an editorial fashion only, and to the benefit of the trademark owner, with no intention of infringement of the trademark. Where such designations appear in this book, they have been printed with initial caps. McGraw-Hill eBooks are available at special quantity discounts to use as premiums and sales promotions, or for use in corporate training programs. For more information, please contact George Hoare, Special Sales, at [email protected] or (212) 904-4069. TERMS OF USE This is a copyrighted work and The McGraw-Hill Companies, Inc. (“McGraw-Hill”) and its licensors reserve all rights in and to the work. Use of this work is subject to these terms. Except as permitted under the Copyright Act of 1976 and the right to store and retrieve one copy of the work, you may not decompile, disassemble, reverse engineer, reproduce, modify, create derivative works based upon, transmit, distribute, disseminate, sell, publish or sublicense the work or any part of it without McGraw-Hill’s prior consent. -
IEEE/PES Transformers Committee Fall 2017 Meeting Minutes
Transformers Committee Chair: Stephen Antosz Vice Chair: Sue McNelly Secretary: Bruce Forsyth Treasurer: Greg Anderson Awards Chair/Past Chair: Don Platts Standards Coordinator: Jim Graham IEEE/PES Transformers Committee Fall 2017 Meeting Minutes Louisville, KY October 30 – November 2, 2017 Unapproved (These minutes are on the agenda to be approved at the next meeting in Spring 2018) TABLE OF CONTENTS GENERAL ADMINISTRATIVE ITEMS 1.0 Agenda 2.0 Attendance OPENING SESSION – MONDAY OCTOBER 30, 2017 3.0 Approval of Agenda and Previous Minutes – Stephen Antosz 4.0 Chair’s Remarks & Report – Stephen Antosz 5.0 Vice Chair’s Report – Susan McNelly 6.0 Secretary’s Report – Bruce Forsyth 7.0 Treasurer’s Report – Gregory Anderson 8.0 Awards Report – Don Platts 9.0 Administrative SC Meeting Report – Stephen Antosz 10.0 Standards Report – Jim Graham 11.0 Liaison Reports 11.1. CIGRE – Raj Ahuja 11.2. IEC TC14 – Phil Hopkinson 11.3. Standards Coordinating Committee, SCC No. 18 (NFPA/NEC) – David Brender 11.4. Standards Coordinating Committee, SCC No. 4 (Electrical Insulation) – Paulette Payne Powell 12.0 Hot Topics for the Upcoming – Subcommittee Chairs 13.0 Opening Session Adjournment CLOSING SESSION – THURSDAY NOVEMBER 2, 2017 14.0 Chair’s Remarks and Announcements – Stephen Antosz 15.0 Meetings Planning SC Minutes & Report – Gregory Anderson 16.0 Reports from Technical Subcommittees (decisions made during the week) 17.0 Report from Standards Subcommittee (issues from the week) 18.0 New Business 19.0 Closing Session Adjournment APPENDIXES – ADDITIONAL DOCUMENTATION Appendix 1 – Meeting Schedule Appendix 2 – Semi-Annual Standards Report Appendix 3 – IEC TC14 Liaison Report Appendix 4 – CIGRE Report Page 2 of 55 ANNEXES – UNAPPROVED MINUTES OF TECHNICAL SUBCOMMITTEES NOTE: The Annexes included in these minutes are unapproved by the respective subcommittees and are accurate as of the date the Transformers Committee meeting minutes were published. -
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.