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Transient Analysis of Three-Phase Wound Rotor (Slip-Ring) Induction Motor Under Operating Condition
International Journal of Recent Engineering Research and Development (IJRERD) ISSN: 2455-8761 www.ijrerd.com || Volume 02 – Issue 07 || July 2017 || PP. 19-32 Transient Analysis of Three-Phase Wound Rotor (Slip-Ring) Induction Motor under Operating Condition Obute K.C.1, Enemuoh F.O.1 1 – Department of Electrical Engineering Nnamdi Azikiwe University Awka, Anambra State Nigeria Corresponding Author - Obute Kingsley Chibueze Department of Electrical Engineering Nnamdi Azikiwe University Awka, Anambra State Nigeria Abstract: This work investigates the transient behaviours of a three phase wound rotor type induction motor, running on load. When starting a motor under load condition becomes paramount, obviously a wound rotor (slip ring) induction becomes the best choice of A.C. motor. This is because maximum torque at starting can be achieved by adding external resistance to the rotor circuit through slip-rings. Normally a face-plate type starter is used, and as the resistance is gradually reduced, the motor characteristics at each stage changes from the other (John Bird 2010). Hence, the three phase wound rotor (slip ring) induction motor competes favourably with the squirrel cage induction motor counterpart as the most widely used three-phase induction motor for industrial applications. The world-wide popularity and availability of this motor type has attracted a deep – look and in-depth research including its transient behavior under plugging (operating) condition. This paper unveils, through mathematical modeling, followed by dynamic simulation, the transient performance of this peculiar machine, analyzed based on Park’s transformation technique. That is with direct-quadrature-zero (d-q-o) axis based modeling in stationary reference frame. -
Nikola Tesla
Nikola Tesla Nikola Tesla Tesla c. 1896 10 July 1856 Born Smiljan, Austrian Empire (modern-day Croatia) 7 January 1943 (aged 86) Died New York City, United States Nikola Tesla Museum, Belgrade, Resting place Serbia Austrian (1856–1891) Citizenship American (1891–1943) Graz University of Technology Education (dropped out) ‹ The template below (Infobox engineering career) is being considered for merging. See templates for discussion to help reach a consensus. › Engineering career Electrical engineering, Discipline Mechanical engineering Alternating current Projects high-voltage, high-frequency power experiments [show] Significant design o [show] Awards o Signature Nikola Tesla (/ˈtɛslə/;[2] Serbo-Croatian: [nǐkola têsla]; Cyrillic: Никола Тесла;[a] 10 July 1856 – 7 January 1943) was a Serbian-American[4][5][6] inventor, electrical engineer, mechanical engineer, and futurist who is best known for his contributions to the design of the modern alternating current (AC) electricity supply system.[7] Born and raised in the Austrian Empire, Tesla studied engineering and physics in the 1870s without receiving a degree, and gained practical experience in the early 1880s working in telephony and at Continental Edison in the new electric power industry. He emigrated in 1884 to the United States, where he became a naturalized citizen. He worked for a short time at the Edison Machine Works in New York City before he struck out on his own. With the help of partners to finance and market his ideas, Tesla set up laboratories and companies in New York to develop a range of electrical and mechanical devices. His alternating current (AC) induction motor and related polyphase AC patents, licensed by Westinghouse Electric in 1888, earned him a considerable amount of money and became the cornerstone of the polyphase system which that company eventually marketed. -
Electrical Machines
1 Electrical Machines 1. The left hand rule is applicable to (a) generator ( b) motor (c) transformer ( d) ( a) and ( b) both (e) ( a) or ( b) 2. The eddy current losses in the transformer will be reduced if (a) the laminations are thick (b) number of turns in the primary winding is reduced (c) the number of turns in the secondary winding is reduced (d) the laminations are thin 3. The speed of d.c. series motor at no load is (a) zero ( b) 1500 r.p.m. (c) infinity ( d) 3000 r.p.m. (e) none of the above 4. A sinusoidal voltage of frequency 1 Hz is applied to the field of d.c. generator. The armature voltage will be (a) 1 Hz square wave ( b) 1 Hz sinusoidal voltage (c) d.c. voltage ( d) none of the above 5. The function of the commutator in a d.c. machine is (a) to change alternating current to a direct current (b) to improve commutation (c) for easy control (d) to change alternating voltage to direct voltage 6. The phase sequence of voltage generated in the alternator can be reversed by reversing its field current. (a) true ( b) false 7. The rotation of three phase induction motor can be reversed by interchanging any two of the supply phases. (a) true ( b) false 2 ELECTRICAL ENGINEERING 8. The starting torque of the three phase induction motor can be increased by (a) increasing the rotor reactance (b) increasing the rotor resistance (c) increasing the stator resistance (d) none of the above 9. -
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. -
Rotating Magnetic Field in Induction Motor
Rotating Magnetic Field in AC Machines 1 Introduction In a DC machine, the stator winding is excited by DC current and hence the field produced by this wind- ing is time invariant in nature. In this machine the conversion of energy from electrical to mechanical form or vice versa is possible by one of the following ways: 1. rotating the rotor in the field produced by the stator 2. feeding external dc current through carbon brushes to the rotor 2 Pre-lab questions Let, XX = Last two digits of your roll number g1(t) = cos(!t) and g2(t; θ) = cos(!t) cos(θ) 1. Take ! = 2πf, where f = XX × 50. Vary !t from 0 to 2π. Plot g1(t) vs t using MATLAB (or any other suitable software) 2. Take ! = 2πf, where f = XX × 50. Vary !t from 0 to 2π. Take θ = 0 to 2π. Plot g2(t; θ) vs t; for θ = XX Plot g2(t; θ) vs θ; for !t = 0; π=4; π=2; 2π=3 3 Theory Now consider three coils A, B and C of N turns each, displaced in space by 120◦ and connected to a balanced 3 phase system as shown in Fig. 1. (Note that the stator winding of 3 phase induction machine is distributed in a large number of slots as shown in Fig. 2). The expressions for the current Figure 1: Coil arrangement to produce rotating magnetic field 1 drawn by these coils are given by: ia = I sin(!st) o ib = I sin(!st + 120 ) (1) o ic = I sin(!st + 240 ) where !s = 2πF1 is supply frequency in rad/s and F1 is supply frequency in Hertz. -
Evaluation of Direct Torque Control with a Constant-Frequency Torque Regulator Under Various Discrete Interleaving Carriers
electronics Article Evaluation of Direct Torque Control with a Constant-Frequency Torque Regulator under Various Discrete Interleaving Carriers Ibrahim Mohd Alsofyani and Kyo-Beum Lee * Department of Electrical and Computer Engineering, Ajou University, 206, World cup-ro, Yeongtong-gu Suwon 16499, Korea * Correspondence: [email protected]; Tel.: +82-31-219-2376 Received: 25 June 2019; Accepted: 20 July 2019; Published: 23 July 2019 Abstract: Constant-frequency torque regulator–based direct torque control (CFTR-DTC) provides an attractive and powerful control strategy for induction and permanent-magnet motors. However, this scheme has two major issues: A sector-flux droop at low speed and poor torque dynamic performance. To improve the performance of this control method, interleaving triangular carriers are used to replace the single carrier in the CFTR controller to increase the duty voltage cycles and reduce the flux droop. However, this method causes an increase in the motor torque ripple. Hence, in this work, different discrete steps when generating the interleaving carriers in CFTR-DTC of an induction machine are compared. The comparison involves the investigation of the torque dynamic performance and torque and stator flux ripples. The effectiveness of the proposed CFTR-DTC with various discrete interleaving-carriers is validated through simulation and experimental results. Keywords: constant-frequency torque regulator; direct torque control; flux regulation; induction motor; interleaving carriers; low-speed operation 1. Introduction There are two well-established control strategies for high-performance motor drives: Field orientation control (FOC) and direct torque control (DTC) [1–3]. The FOC method has received wide acceptance in industry [4]. Nevertheless, it is complex because of the requirement for two proportional-integral (PI) regulators, space-vector modulation (SVM), and frame transformation, which also needs the installation of a high-resolution speed encoder. -
Alternator Winding Temperature Rise in Generator Systems
TM Information Sheet # 55 Alternator Winding Temperature Rise in Your Reliable Guide for Power Solutions Generator Systems 1.0 Introduction: When a wire carries electrical current, its temperature will increase due to the resistance of the wire. The factor that mostly influences/ limits the acceptable level of temperature rise is the insulation system employed in an alternator. So the hotter the wire, the shorter the life expectancy of the insulation and thus the alternator. This information sheets discusses how different applications influence temperature rise in alternator windings and classification standards are covered by the National electrical Manufacturers Association (NEMA). (Continued over) Table 1 - Maximum Temperature Rise (40°C Ambient) Continuous Temperature Rise Class A Class B Class F Class H Temp. Rise °C 60 80 105 125 Temp. Rise °F 108 144 189 225 Table 2 - Maximum Temperature Rise (40°C Ambient) Standby Temperature Rise Class A Class B Class F Class H Temp. Rise °C 85 105 130 150 Temp. Rise °F 153 189 234 270 Typical Windings Within a Generator Set’s Alternator Excitor windings Stator windings Rotor windings To fulfill our commitment to be the leading supplier and preferred service provider in the Power Generation Industry, the Clifford Power Systems, Inc. team maintains up-to-date technology and information standards on Power Industry changes, regulations and trends. As a service, our Information Sheets are circulated on a regular basis, to existing and potential Power Customers to maintain awareness of changes and -
High Speed Linear Induction Motor Efficiency Optimization
Calhoun: The NPS Institutional Archive Theses and Dissertations Thesis Collection 2005-06 High speed linear induction motor efficiency optimization Johnson, Andrew P. (Andrew Peter) http://hdl.handle.net/10945/11052 High Speed Linear Induction Motor Efficiency Optimization by Andrew P. Johnson B.S. Electrical Engineering SUNY Buffalo, 1994 Submitted to the Department of Ocean Engineering and the Department of Electrical Engineering and Computer Science in Partial Fulfillment of the Requirements for the Degree of Naval Engineer and Master of Science in Electrical Engineering and Computer Science at the Massachusetts Institute of Technology June 2005 ©Andrew P. Johnson, all rights reserved. MIT hereby grants the U.S. Government permission to reproduce and to distribute publicly paper and electronic copies of this thesis document in whole or in part. Signature of A uthor ................ ............................... D.epartment of Ocean Engineering May 7, 2005 Certified by. ..... ........James .... ... ....... ... L. Kirtley, Jr. Professor of Electrical Engineering // Thesis Supervisor Certified by......................•........... ...... ........................S•:• Timothy J. McCoy ssoci t Professor of Naval Construction and Engineering Thesis Reader Accepted by ................................................. Michael S. Triantafyllou /,--...- Chai -ommittee on Graduate Students - Depa fnO' cean Engineering Accepted by . .......... .... .....-............ .............. Arthur C. Smith Chairman, Committee on Graduate Students DISTRIBUTION -
Introduction to Power Quality
CHAPTER 1 INTRODUCTION TO POWER QUALITY 1.1 INTRODUCTION This chapter reviews the power quality definition, standards, causes and effects of harmonic distortion in a power system. 1.2 DEFINITION OF ELECTRIC POWER QUALITY In recent years, there has been an increased emphasis and concern for the quality of power delivered to factories, commercial establishments, and residences. This is due to the increasing usage of harmonic-creating non linear loads such as adjustable-speed drives, switched mode power supplies, arc furnaces, electronic fluorescent lamp ballasts etc.[1]. Power quality loosely defined, as the study of powering and grounding electronic systems so as to maintain the integrity of the power supplied to the system. IEEE Standard 1159 defines power quality as [2]: The concept of powering and grounding sensitive equipment in a manner that is suitable for the operation of that equipment. In the IEEE 100 Authoritative Dictionary of IEEE Standard Terms, Power quality is defined as ([1], p. 855): The concept of powering and grounding electronic equipment in a manner that is suitable to the operation of that equipment and compatible with the premise wiring system and other connected equipment. Good power quality, however, is not easy to define because what is good power quality to a refrigerator motor may not be good enough for today‟s personal computers and other sensitive loads. 1.3 DESCRIPTIONS OF SOME POOR POWER QUALITY EVENTS The following are some examples and descriptions of poor power quality “events.” Fig. 1.1 Typical power disturbances [2]. ■ A voltage sag/dip is a brief decrease in the r.m.s line-voltage of 10 to 90 percent of the nominal line-voltage. -
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]. -
Introduction to Direct Current (DC) Theory
PDHonline Course E235 (4 PDH) Electrical Fundamentals - Introduction to Direct Current (DC) Theory Instructor: A. Bhatia, B.E. 2012 PDH Online | PDH Center 5272 Meadow Estates Drive Fairfax, VA 22030-6658 Phone & Fax: 703-988-0088 www.PDHonline.org www.PDHcenter.com An Approved Continuing Education Provider CHAPTER 3 DIRECT CURRENT LEARNING OBJECTIVES Upon completing this chapter, you will be able to: 1. Identify the term schematic diagram and identify the components in a circuit from a simple schematic diagram. 2. State the equation for Ohm's law and describe the effects on current caused by changes in a circuit. 3. Given simple graphs of current versus power and voltage versus power, determine the value of circuit power for a given current and voltage. 4. Identify the term power, and state three formulas for computing power. 5. Compute circuit and component power in series, parallel, and combination circuits. 6. Compute the efficiency of an electrical device. 7. Solve for unknown quantities of resistance, current, and voltage in a series circuit. 8. Describe how voltage polarities are assigned to the voltage drops across resistors when Kirchhoff's voltage law is used. 9. State the voltage at the reference point in a circuit. 10. Define open and short circuits and describe their effects on a circuit. 11. State the meaning of the term source resistance and describe its effect on a circuit. 12. Describe in terms of circuit values the circuit condition needed for maximum power transfer. 13. Compute efficiency of power transfer in a circuit. 14. Solve for unknown quantities of resistance, current, and voltage in a parallel circuit.