A New Design of Permanent Magnets Reluctance Generator Andi Pawawoi, Syafii
|
|
|
- Georgiana Cox
- 9 years ago
- Views:
Transcription
1 A New Design of Permanent Magnets Reluctance Generator Andi Pawawoi, Syafii Abstract Instantaneous electromagnetic torque of simple reflectance generator can be positive at a time and negative at other time. It is utilized to design a permanent magnet reluctance generator specifically. Generator is designed by combining two simple reluctance generators, consists of two rotors mounted on the same shaft, two output-windings and a field source of the permanent magnet. By this design, the electromagnetic torque on both rotor will be eliminated each other, so the input torque generator can be smaller. Rotor is expected only to regulate the flux flow to both output windings alternately, until the magnetic energy is converted into electrical energy, such as occurs in the transformer energy conversion. The prototype trials have been made to test this design. The test result show that the new design of permanent magnets reluctance generator able to convert energy from permanent magnets into electrical energy, this is proven by the existence 167% power output compared to the shaft input power. Keywords Energy, Magnet permanent, Reluctance generator. O I. INTRODUCTION NE source of new and renewable energy has recently discovered is a permanent magnet. Permanent magnet is long known and used in various fields of electrical engineering, for example, dynamos, motors, speakers, etc. However, its use as an energy source, newly discovered, and these energy conversion devices currently no commercially produced. Previous studies, associated with the permanent magnet, showed that the permanent magnet can be used as an energy source. The energy conversions from permanent magnets have been done [1], which made Parendev Permanent Magnet Motor (PPMM). Accordance with its name, this engine produces mechanical rotation energy derived from permanent magnet energy of motor that build it. Several other researchers also have made a permanent magnet motor with a different design from the motor Varendev. Research to get a permanent magnet machine energy conversion into electricity is very promising and gives great hope. A study aimed to get a permanent magnet machine energy conversion into electrical energy has been studied in [2] as pioneered research. In that study successfully designed a New Model Reluctance Generator (NMRG) with excess capable of converting energy from a constant magnetic field into electric energy. NMRG output energy is not reflected by the input shaft, but from given constant input fields. In the Andi Pawawoi is with the Electrical Engineering Department, Andalas University, Padang, Indonesia ( [email protected]). Syafii is with the Electrical Engineering Department, Andalas University, Padang, Indonesia ( [email protected] ) conducted experiments, when NMRG loaded at different load levels, the input power was constant, and the power was same as the generator in no-load conditions. However, the changes according to the load change are the power input field excitation. It shows that there has been a conversion of energy from the generator field source into electrical energy [2]. The next problem to be studied is to develop design NMRG, by changing the source field from the coil electric DC current into permanent magnet. This NMRG development targets, is obtained an engine design that is able to convert energy from permanent magnet into the electrical energy. II. BASIC THEORY A. Simple Reluctance Generator Reluctance generator is a generator that utilizes the air gap reluctance changes due to rotation of the rotor to generate voltage. At this generator, both field winding and armature fixed and operations depend on the period of the air gap changes. The generator is allowed to be operated at high speed to generate a voltage, typically used as a wind turbine or micro gas turbine generator. Fig. 1 shows the operating principle of a simple reluctance generator. Two permanent magnets are placed on the stator core, serves as a major source of field. A salient pole rotor is made of silicon steel. Stator windings are placed on poles. When the rotor rotated, the reluctance changes will occur in the core of the stator flux changes along with changes in the position of the rotor. Because the flux changes are summarized by the stator winding on the winding voltage will be induced [3], [4]. Fig. 1 Simple reluctance generator By considering simple reluctance motors as shown in Fig.1, which is a function of the assumed magnetic rotor position angle by (1) and the graph illustrated in Fig
2 R R R R R cos 2σ (1) Emf induced is generated in the windings if the resistance is negligible: wherein: and 2 cos ω φ φ φ sin ω Electromagnetic torque simple of reluctance generator expressed by (5) and the graph illustrated in Fig. 2 [4], [6], [7]. φ R σ Fig. 2 The relationship between reflectance position B. Permanent Magnet Permanent magnet is a material that able to generate its own magnetic field without energy supply, in contrast to the winding can generate magnetic fields only if there is electrical energy supplied (voltage and current). The magnetic field is a form of energy. The magnetic field of the permanent magnet has the same character with the magnetic field generated from electrical current-carrying winding [5]. The ability of permanent magnet moving mass of a body of evidence ferromagnetic hat proves permanent magnets have the real energy. Energy in permanent magnets has not been widely used. On conventional generators / motors, permanent magnet is used as an imaginary energy source only. Permanent magnets are generally made of a mixture metal and or non-metal created by buffed with another magnet in the same direction, induced magnet, or magnetic material is placed in a solenoid (a long tubular coil of wire with very tightly turned) and electrified by direct current (DC). Currently there are several types of permanent magnets include: n Neodymium magnets, samarium-cobalt magnets, ceramic magnets, plastic magnets, alnico magnets, ferrite φ. π ω and torque vs. rotor (2) (3) (4) (5) magnets, etc. The permanent magnet shape can be adjusted as needed. The form a permanent magnet available is: U magnet, horseshoe magnet, rod magnet, circles magnet, etc. The magnetic properties of permanent magnets can be eliminated by means of, among other things: burned, slamslam, pounded, or placed on the solenoid magnet and electrified by alternating current. III. METHOD A. Design of Permanent Magnet Reluctance Generator 1. Design of Rotor Rotor of the generator, designed according to Fig. 3. It is consists of 2 pieces and both are connected by a shaft with a different angle of 180 as shown in Fig. 4. By this way the electromagnetic torque of the two rotors are able to reduce. The rotor which made of silicon steel laminations is arranged radials intended to reduce eddy current losses in the rotor. Fig. 3 Design of rotor Fig. 4 Composite rotor By rotor designed above, the electromagnetic torque of each rotor is a different phase of 180, so that the total sum of both rotor electromagnetic torques s will be zero. 2. Design of Stator The generator stator consists of 3 main parts: stator core, permanent magnet and armature windings. Fig. 5 shows a sketch of stator design. Stator core made of laminated silicon steel U-shaped, with each core leg right and left mounted armature windings which are the output voltage V out1 and V out2 are generated with different angle 180 o. In the middle of arrangement plate, mounted permanent magnet is served as a major source of field so that in the stator formed 2 stator gaps i.e. left and right gap, as shown in Fig. 5. At this gap will be mounted rotor. 462
3 that if both torque summed the result is equal to zero. This means that if the two rotors mounted on the same shaft then there would be no electromagnetic torque on the rotor shaft. Fig. 5 Stator design 3. Design of Combined Stator and Rotor Rotor that has been made is placed in the contained gap at the stator. In this generator design, the magnitude of the air gap must be considered because effecting on the flux flow result (Fig. 6). The air gap between the rotor and stator kept minimum to achieve small reluctance, while between the shaft and the stator should not be too close so that the flux does not pass through the shaft. If the rotor is rotated past the stator gap, when the rotor is right on the stator gap (Fig. 6), the flux from the permanent magnet will flow through the rotor and into the stator core. Line with the movement of the rotor through the stator gap, the magnetic flux passing through the stator winding core will change from the minimum value before the rotor into the stator gap until it reaches the maximum value when the stator gap is closed by the rotor, and this value will be returned to its minimum value when the rotor exit of stator gap. This condition occurs alternately on both core winding. Magnetic flux changes as described above occur because of changes in Reluctance stator gap. The resulting flux from the permanent magnet will tend to flow on the section that has a low Reluctance values. Minimum Reluctance value of stator gap will occur when the rotor is directly on the gap, at the time of flux flow will reach its maximum value. The maximum reluctance occurs when the rotor outside the stator gap, at the time the flux reaches its minimum value. Graphically it can be represented as shown in Fig. 7. Description: 1 = air gap between stator-rotor 2 = air gap between the stator-shaft Fig. 6 Model of permanent magnet reluctance generator According to (5), the electromagnetic torque on both rotors can be described as shown in Fig. 7. From the picture shown Fig. 7 Reluctance and electromagnetic torque in a permanent magnet reluctance generator new design B. Generator Voltage Due to the change in flux in the core of the armature windings are placed where it will be raised the voltage on the armature windings. To determine the maximum total flux windings, necessary to determine the broad surface of the rotor and stator assembly are effective through the magnetic flux. The maximum effective area occurs when the rotor is right on the stator gap; in this condition the magnitude of the magnetic flux reaches its maximum. The equation used to calculate the area, is the equation of a circle sector wide. For more details can be seen in the Fig. 8 below. Surface of the stator pole Fig. 8 The effective area crossed magnetic flux Effective area is approximated by the equation: π 2 0 A = (r ) α (6) where: A = Effective surface area (m2) π = 3.14 r = R 2 R 1 (m) 463
4 α = Angle (degrees) Effective areas are used to calculate the reluctance between the stator and the rotor with the following equations: R (7) (8) where: R = Reluctance (A. turn/weber) l = Path length (m) A = Surface area (m2) µ = Permeability (H/m) = Material permeability = Vacuum permeability The values that have been obtained are used to calculate the magnitude of the magnetic flux and flux density according to the following equation: φ F R (9) (10) where: φ = Magnetic flux (Weber) F = Mmf (A. Turn) B = Flux density (Weber/m 2 ) The voltage generated can be calculated using the following equation: where: So that: where: So that: φ e = -N t (11) φ (12) BdA Brdθ e = - N = -N (13) dt dt dθ = ω ; kecepatan sudut dt e = - N. B. r.ω (14) C. Dimensional Trial Prototype To test the above generator design, the trial generator is created with the rotor and stator dimensions as shown in Figs. 9 and 10 below. Fig. 9 Specifications rotor R 1 = 3 cm, R 2 = 5.7 cm, L = 2.4 cm, α = 90 0 Fig. 10 Specifications stator P s = 15.2 cm, T s = 10.1 cm, L s = 6.3 cm, P s1 = P s3 = 2.5 cm, P s2 = 5 cm, T s1 = 7.6 cm, Number of winding = 530 turn, Size of copper = 0.5 mm D. Permanent Magnet Permanent magnets are used in this design are grade N35 neodymium magnets with length 22mm, width 13mm and thickness of 2.5mm, a total of 90 pieces arranged to form a 3x3 matrix as high as 15 pieces. The magnetic field generated from the permanent magnet in the air can be seen in Fig. 11 below: Fig. 11 Magnetic flux of neodymium magnet N35 E. Simulation of Magnetic Flux The proposed design, ideally desired all magnetic flux from the permanent magnet applied to the right and left leg of stator core, alternately. The leakage flux is undesired, such as the flux that flows into the left side core when all flux is directed 464
5 by rotor to the right side core. To minimize the flux leakage magnetic flux mapping needs to be done so that the design could be made more perfect. The simulation of magnetic field mapping and flux density at each component is done using Visimag 3:18. The results are shown in Figs. 12 and 13 below. P inm0 = No load motor input power (W) P inm-g0 = Motor input power after coupled with generator at no load (145 W) I a = Motor armature current (A) R a = Motor armature resistance (13 Ohm) Generator shaft input power under loaded can be defined by equation below: Fig. 12 The mapping of magnetic flux Fig. 13 Flux density field at each component F. Testing Plan Shunt DC motor is used in testing of this generator as a motor drive. There are two types of tests performed, namely; 1. No-load test, intended to look at the characteristics of the voltage as a function of rotational speed of the generator. 2. Load testing, intended to get the effect of the load curve of the generator output voltage. Input-output power measurements were also performed on this test. G. Calculation Method of Input-Output Power The power flow scheme of these experiments is shown in Fig. 18. The generator shaft input power with no load (P ing0 ) can be determined by calculating the difference between the motor input power after coupled with generator (P inm-g0 ) and the motor input power before coupled to a generator (P inm0 ) reduced by Cu losses due to the motor load, or equations can be written as below: P ing0 = P inm-g0 (PinM0 + I 2 a R a ) (15) where: P ing0 = No load generator shaft input power (W) P ingx = P inmx ( P ing0 + ( I ax ) 2 Ra ) (16) where: P ingx = Generator shaft input power of x loaded (W) P inmx = Motor input power at x loaded (W) P ing0 = Generator input power at no load I AX = Motor armature current at loaded (A) R a = Armature resistance (13 Ohm) Power is converted into electrical energy by generator can be determined as equation below: P ConGx = P outgx (I gx ) 2 Rg (17) where: P ConGx = Converted power by generator (W) P outgx = Output power of generator on x loaded (W) I gx = Generator armature current at x loaded (A) R g = Generator armature resistance (37 Ohm) Conversion efficiency (ηc) of generator to shaft input power can be calculated by comparing the output power with the shaft input power on the generator, is calculated by equation below: η (18) IV. RESULTS AND DISCUSSION A. The Design Results The generators that has been made shown in Fig. 14 below: Fig. 14 Permanent magnet reluctance generator prototype new designs trials B. Generator Testing 1. Generator Testing at No Load Before testing the generator with no load, the motor power is measured first at the conditions before and after coupled to the generator. The results are shown in Table I below: 465
6 Condition Before coupled with a generator After coupled with a generator TABLE I POWER MOTOR AT NO LOAD I (Amp) P (Watt) The effects of loaded to output voltage graphics are shown in Fig. 16. The output voltage at the load condition is decreased with increasing given load. No-load voltage measurement is done by vary of generator rotation. The data obtained show that, the increased of generator rotation speed make voltage generated also increased. Complete test results on graph are shown in Fig. 15 below. Fig. 15 Characteristics of the output voltage to the rotation speed 2. Generator Testing Under Load Testing under load carried by the generator operates a constant speed 2000 rpm, and given a variable load resistance. The test result data are shown in Table II below: TABLE II LOAD TEST RESULTS Motor Generator No I V I V Load R P (Watt) P (Amp.) (Volt) (Amp.) (Volt) out (W) (Ohm) No. Motor I (Amp.) V (Volt) P (Watt) I (Amp.) V (Volt) P out (W) P ConGx (W) P ingx (W) Efficiency (%) TABLE III POWER INPUT - OUTPUT GENERATOR Fig. 16 Characteristics output voltage on load conditions 3. Input Output Power Analysis Motor input power, before being connected to the generator (no load motor) on the nominal rotation 2000 rpm, measured: P inm0 = 91 Watt After the coupled to a permanent magnet generator with no load and operated at nominal rotation (2000 rpm), the motor power input is measured by: P inm-g0 = 145 Watt. Shaft input power generator with no load (P ing0 ) or no load loses is obtained by the use of (15); P ing0 = P inm-g0 ( P inm0 + I 2 a R a ) P ing0 = [(0.71) 2 x 13] = Watt Generator shaft input power under loaded (P ingx ) is calculated by (16) and converted power generator (P ConGx ) is calculated by (17). According the data in Table II, can be calculated P ingx, P ConG and conversion efficiency of generator, the results are shown in Table III below: Generator
7 energy. When the permanent magnet reluctance generator new model is loaded, it will be generated magnetic field of the output coil. The magnetic field will oppose the magnetic field of the permanent magnet, so that if the continuous load plus the magnetic field in the core is reduced, consequently the converted energy will also be reduced, with its own generator output will drop. This is consistent with the experimental results as shown in the input-output curve in Fig. 17. Scheme on the power flow when it reaches 167% conversion efficiency is shown in Fig. 18 below. On the scheme shows that 83 W of power that is converted into electrical energy, 80.9 W (98%) comes from permanent magnet. Fig. 17 Graphic shaft input power and output power of the generator In Fig. 17, it is seen that the generator shaft power input is relatively constant at various load levels. This result is caused of using two rotors with intersecting rotors mounted. When the generator is operated, the electromagnetic torque of the two rotors will always opposite (destructively) at any time. The impact of the rotor design is the generator shaft power input will tend to constant despite increased load. The comparison between power output and the power input of generator shaft, as shown in the input-output curve in Fig. 17 and Table III, there has been a condition where the generator output power greater than the power input shaft up to 167%. With is applying the law of conservation of energy in the generator can be assured that the energy source of the generator is not entirely derived from the input shaft. If we note the reluctance generator working principle of this new model, the velocity of the rotor actually serve only divert the direction of magnetic flux flow from the permanent magnet to the right and left foot of stator core, alternately. Diversion of flux flow direction leads to changes in the magnetic flux in the core of both the stator armature windings so that induced voltage. By considering on the process of transformer energy conversion, electrical energy initially converted into energy in the form of a magnetic field on the primary side, and then the magnetic field energy is converted back into electrical energy on the secondary side. Energy conversion system with a magnetic field media is possible only if the magnetic field changes with time. On the transformer, electrical source changes with time so that the magnetic field generated also changes with time. Magnetic field changes with time are passed to the secondary coil, and the secondary coil magnetic field energy is converted back into electrical energy [4]-[7]. On permanent magnet reluctance generator of this new model, a constant magnetic field of the permanent magnet is converted into magnetic field varies with time by the rotation of the rotor, the magnetic field by flowing to the right and left foot of stator core, alternately. Output coil is placed on the right and left leg stator feel the time-varying fields, so that in the coil, the magnetic field energy is converted into electrical Fig. 18 Power flow scheme V. CONCLUSION 1. Permanent magnets reluctance generator new model has been developed. The reluctance generator was able to convert energy from permanent magnets into electrical energy. 2. The permanent magnets reluctance generator new models was able to produce power 167%, compared to the shaft input power. 3. The permanent magnets reluctance generator new models, only serves as a regulator of the flow of magnetic flux from the source in the form of permanent magnetic field to one to two feet alternately stator core. ACKNOWLEDGMENT The author gratefully acknowledges the assistance rendered by the Faculty of Engineering, Andalas University for partially funding this research in DIPA FT Unand 2013 (Contract No.034/PL/SPK/PNP/FT Unand/2013). REFERENCES [1] V.Roschin and S. Godin, New Energy Technologies, Faraday Lab Ltd, Russia,
8 [2] Pawawoi, A Generator reluctance model baru, Polirekayasa Vol. 6 No. 1. Padang. [3] Tsukerman, D. Rabinovici, R. New Power Factor and Current Harmonic Mitigation for AC Variable Reluctance Generator with DC Excitation. Israel. Department of Electrical and Computer Engineering. University of The Negev. [4] Ichinokura, O., Ono, T., Takahashi, A., Nakamura, K., and Watanabe, T Three Phase Reluctance Generator with Permanent Magnet Buried in Stator Core. Japan. Universities Tohoku. [5] Peter Campbell, Permanent Magnet Materials and Their Application, New York: Cambridge University Press, 1994 [6] Matsch.L, W. Electromagnetic and Electromechanical Machines. Third Ed. John Wiley & Son. Inc [7] I, J, Nagrath Electric Machines. Tata McGraw Hill. New Delhi. 468
DIRECT CURRENT GENERATORS
DIRECT CURRENT GENERATORS Revision 12:50 14 Nov 05 INTRODUCTION A generator is a machine that converts mechanical energy into electrical energy by using the principle of magnetic induction. This principle
Motors and Generators
Motors and Generators Electro-mechanical devices: convert electrical energy to mechanical motion/work and vice versa Operate on the coupling between currentcarrying conductors and magnetic fields Governed
Direct Current Motors
Direct Current Motors DC MOTORS The DC machine can operate as a generator and as a motor. Chap 5. Electrical Machines by Wildi, 6 e Lecturer: R. Alba-Flores Alfred State College Spring 2008 When a DC machine
Induction Motor Theory
PDHonline Course E176 (3 PDH) Induction Motor Theory Instructor: Jerry R. Bednarczyk, P.E. 2012 PDH Online PDH Center 5272 Meadow Estates Drive Fairfax, VA 22030-6658 Phone & Fax: 703-988-0088 www.pdhonline.org
Motor Fundamentals. DC Motor
Motor Fundamentals Before we can examine the function of a drive, we must understand the basic operation of the motor. It is used to convert the electrical energy, supplied by the controller, to mechanical
Principles and Working of DC and AC machines
BITS Pilani Dubai Campus Principles and Working of DC and AC machines Dr Jagadish Nayak Constructional features BITS Pilani Dubai Campus DC Generator A generator consists of a stationary portion called
Lab 8: DC generators: shunt, series, and compounded.
Lab 8: DC generators: shunt, series, and compounded. Objective: to study the properties of DC generators under no-load and full-load conditions; to learn how to connect these generators; to obtain their
13 ELECTRIC MOTORS. 13.1 Basic Relations
13 ELECTRIC MOTORS Modern underwater vehicles and surface vessels are making increased use of electrical actuators, for all range of tasks including weaponry, control surfaces, and main propulsion. This
1. The diagram below represents magnetic lines of force within a region of space.
1. The diagram below represents magnetic lines of force within a region of space. 4. In which diagram below is the magnetic flux density at point P greatest? (1) (3) (2) (4) The magnetic field is strongest
CHAPTER 4 DESIGN OF INTEGRAL SLOT AND FRACTIONAL SLOT BRUSHLESS DC MOTOR
47 CHAPTER 4 DESIGN OF INTEGRAL SLOT AND FRACTIONAL SLOT BRUSHLESS DC MOTOR 4.1 INTRODUCTION This chapter deals with the design of 24 slots 8 poles, 48 slots 16 poles and 60 slots 16 poles brushless dc
DHANALAKSHMI COLLEGE OF ENGINEERING DEPARTMENT OF ELECTRICAL AND ELECTRONICS ENGINEERING EE2302 - ELECTRICAL MACHINES II UNIT-I SYNCHRONOUS GENERATOR
1 DHANALAKSHMI COLLEGE OF ENGINEERING DEPARTMENT OF ELECTRICAL AND ELECTRONICS ENGINEERING Constructional details Types of rotors EE2302 - ELECTRICAL MACHINES II UNIT-I SYNCHRONOUS GENERATOR PART A 1.
DC GENERATOR THEORY. LIST the three conditions necessary to induce a voltage into a conductor.
DC Generators DC generators are widely used to produce a DC voltage. The amount of voltage produced depends on a variety of factors. EO 1.5 LIST the three conditions necessary to induce a voltage into
Basics of Electricity
Basics of Electricity Generator Theory PJM State & Member Training Dept. PJM 2014 8/6/2013 Objectives The student will be able to: Describe the process of electromagnetic induction Identify the major components
SYNCHRONOUS MACHINES
SYNCHRONOUS MACHINES The geometry of a synchronous machine is quite similar to that of the induction machine. The stator core and windings of a three-phase synchronous machine are practically identical
HIGH SPEED PERMANENT MAGNET SYNCHRONOUS MOTOR / GENERATOR DESIGN FOR FLYWHEEL APPLICATIONS
HIGH SPEED PERMANENT MAGNET SYNCHRONOUS MOTOR / GENERATOR DESIGN FOR FLYWHEEL APPLICATIONS Aleksandr Nagorny, Ph.D. National Research Council Outline Introduction Selection of the Rated Point The major
Lab 14: 3-phase alternator.
Lab 14: 3-phase alternator. Objective: to obtain the no-load saturation curve of the alternator; to determine the voltage regulation characteristic of the alternator with resistive, capacitive, and inductive
The purposes of this experiment are to test Faraday's Law qualitatively and to test Lenz's Law.
260 17-1 I. THEORY EXPERIMENT 17 QUALITATIVE STUDY OF INDUCED EMF Along the extended central axis of a bar magnet, the magnetic field vector B r, on the side nearer the North pole, points away from this
Electric Motors and Drives
EML 2322L MAE Design and Manufacturing Laboratory Electric Motors and Drives To calculate the peak power and torque produced by an electric motor, you will need to know the following: Motor supply voltage,
2. A conductor of length 2m moves at 4m/s at 30 to a uniform magnetic field of 0.1T. Which one of the following gives the e.m.f. generated?
Extra Questions - 2 1. A straight length of wire moves through a uniform magnetic field. The e.m.f. produced across the ends of the wire will be maximum if it moves: a) along the lines of magnetic flux
Inductance. Motors. Generators
Inductance Motors Generators Self-inductance Self-inductance occurs when the changing flux through a circuit arises from the circuit itself. As the current increases, the magnetic flux through a loop due
AC generator theory. Resources and methods for learning about these subjects (list a few here, in preparation for your research):
AC generator theory This worksheet and all related files are licensed under the Creative Commons Attribution License, version 1.0. To view a copy of this license, visit http://creativecommons.org/licenses/by/1.0/,
Simple Analysis for Brushless DC Motors Case Study: Razor Scooter Wheel Motor
Simple Analysis for Brushless DC Motors Case Study: Razor Scooter Wheel Motor At first glance, a brushless direct-current (BLDC) motor might seem more complicated than a permanent magnet brushed DC motor,
Equipment: Power Supply, DAI, Universal motor (8254), Electrodynamometer (8960), timing belt.
Lab 12: The universal motor. Objective: to examine the construction of the universal motor; to determine its no-load and full-load characteristics while operating on AC; to determine its no-load and full-load
Direction of Induced Current
Direction of Induced Current Bar magnet moves through coil Current induced in coil A S N v Reverse pole Induced current changes sign B N S v v Coil moves past fixed bar magnet Current induced in coil as
Force on Moving Charges in a Magnetic Field
[ Assignment View ] [ Eðlisfræði 2, vor 2007 27. Magnetic Field and Magnetic Forces Assignment is due at 2:00am on Wednesday, February 28, 2007 Credit for problems submitted late will decrease to 0% after
Application Information
Moog Components Group manufactures a comprehensive line of brush-type and brushless motors, as well as brushless controllers. The purpose of this document is to provide a guide for the selection and application
Edmund Li. Where is defined as the mutual inductance between and and has the SI units of Henries (H).
INDUCTANCE MUTUAL INDUCTANCE If we consider two neighbouring closed loops and with bounding surfaces respectively then a current through will create a magnetic field which will link with as the flux passes
DC motors: dynamic model and control techniques
DC motors: dynamic model and control techniques Luca Zaccarian Contents 1 Magnetic considerations on rotating coils 1 1.1 Magnetic field and conductors.......................... 1 1.2 The magneto-motive
5. Measurement of a magnetic field
H 5. Measurement of a magnetic field 5.1 Introduction Magnetic fields play an important role in physics and engineering. In this experiment, three different methods are examined for the measurement of
Magnetic Field of a Circular Coil Lab 12
HB 11-26-07 Magnetic Field of a Circular Coil Lab 12 1 Magnetic Field of a Circular Coil Lab 12 Equipment- coil apparatus, BK Precision 2120B oscilloscope, Fluke multimeter, Wavetek FG3C function generator,
Lecture 6: AC machinery fundamentals
Lecture 6: AC machinery fundamentals 1 Instructor: Dr. Gleb V. Tcheslavski Contact: [email protected] Office Hours: TBD; Room 030 Class web site: http://ee.lamar.edu/gleb/ind ex.htm Preliminary notes AC
ElectroMagnetic Induction. AP Physics B
ElectroMagnetic Induction AP Physics B What is E/M Induction? Electromagnetic Induction is the process of using magnetic fields to produce voltage, and in a complete circuit, a current. Michael Faraday
A METHOD OF CALIBRATING HELMHOLTZ COILS FOR THE MEASUREMENT OF PERMANENT MAGNETS
A METHOD OF CALIBRATING HELMHOLTZ COILS FOR THE MEASUREMENT OF PERMANENT MAGNETS Joseph J. Stupak Jr, Oersted Technology Tualatin, Oregon (reprinted from IMCSD 24th Annual Proceedings 1995) ABSTRACT The
THE LUCAS C40 DYNAMO & ITS ARMATURE.
THE LUCAS C40 DYNAMO & ITS ARMATURE. H. Holden, March 2011. The Dynamo as a DC generating machine was used extensively in the pre- Alternator era, from the early 1900 s up to the late 1960 s and early
Equipment: Power Supply, DAI, Wound rotor induction motor (8231), Electrodynamometer (8960), timing belt.
Lab 13: Wound rotor induction motor. Objective: to examine the construction of a 3-phase wound rotor induction motor; to understand exciting current, synchronous speed and slip in this motor; to determine
*ADVANCED ELECTRIC GENERATOR & CONTROL FOR HIGH SPEED MICRO/MINI TURBINE BASED POWER SYSTEMS
*ADVANCED ELECTRIC GENERATOR & CONTROL FOR HIGH SPEED MICRO/MINI TURBINE BASED POWER SYSTEMS Jay Vaidya, President Electrodynamics Associates, Inc. 409 Eastbridge Drive, Oviedo, FL 32765 and Earl Gregory,
INSTRUMENTATION AND CONTROL TUTORIAL 2 ELECTRIC ACTUATORS
INSTRUMENTATION AND CONTROL TUTORIAL 2 ELECTRIC ACTUATORS This is a stand alone tutorial on electric motors and actuators. The tutorial is of interest to any student studying control systems and in particular
Design and Analysis of Switched Reluctance Motors
Design and Analysis of Switched Reluctance Motors İbrahim ŞENGÖR, Abdullah POLAT, and Lale T. ERGENE Electrical and Electronic Faculty, İstanbul Technical University, 34469, Istanbul, TURKEY [email protected],
The DC Motor/Generator Commutation Mystery. Commutation and Brushes. DC Machine Basics
The DC Motor/Generator Commutation Mystery One small, yet vital piece of the DC electric motor puzzle is the carbon brush. Using the correct carbon brush is a key component for outstanding motor life,
Digital Energy ITI. Instrument Transformer Basic Technical Information and Application
g Digital Energy ITI Instrument Transformer Basic Technical Information and Application Table of Contents DEFINITIONS AND FUNCTIONS CONSTRUCTION FEATURES MAGNETIC CIRCUITS RATING AND RATIO CURRENT TRANSFORMER
8 Speed control of Induction Machines
8 Speed control of Induction Machines We have seen the speed torque characteristic of the machine. In the stable region of operation in the motoring mode, the curve is rather steep and goes from zero torque
Magnetic electro-mechanical machines
Magnetic electro-mechanical machines Lorentz Force A magnetic field exerts force on a moving charge. The Lorentz equation: f = q(e + v B) f: force exerted on charge q E: electric field strength v: velocity
Mathematical Modelling of PMSM Vector Control System Based on SVPWM with PI Controller Using MATLAB
Mathematical Modelling of PMSM Vector Control System Based on SVPWM with PI Controller Using MATLAB Kiran Boby 1, Prof.Acy M Kottalil 2, N.P.Ananthamoorthy 3 Assistant professor, Dept of EEE, M.A College
USER MANUAL THE RESOLVER
USR MANUAL TH RSOLVR ICP Department 4 has developed and produced a wide range of transmitter type resolvers for military and industrial applications. From a mechanical viewpoint, these products have been
Vehicle Design Summit Electric Hub Motor (V2) Eric Conner Harvey Tang Matthew Peddie
Vehicle Design Summit Electric Hub Motor (V2) Eric Conner Harvey Tang Matthew Peddie Motivation The AHPV from VDS 1.0 used an expensive, NGM electric hub motor, costing roughly $8000. (picture on right)
Magnetic Circuits. Outline. Ampere s Law Revisited Review of Last Time: Magnetic Materials Magnetic Circuits Examples
Magnetic Circuits Outline Ampere s Law Revisited Review of Last Time: Magnetic Materials Magnetic Circuits Examples 1 Electric Fields Magnetic Fields S ɛ o E da = ρdv B V = Q enclosed S da =0 GAUSS GAUSS
Modelling, Simulation and Performance Analysis of A Variable Frequency Drive in Speed Control Of Induction Motor
International Journal of Engineering Inventions e-issn: 78-7461, p-issn: 319-6491 Volume 3, Issue 5 (December 013) PP: 36-41 Modelling, Simulation and Performance Analysis of A Variable Frequency Drive
Linear DC Motors. 15.1 Magnetic Flux. 15.1.1 Permanent Bar Magnets
Linear DC Motors The purpose of this supplement is to present the basic material needed to understand the operation of simple DC motors. This is intended to be used as the reference material for the linear
Chapter 22: Electric motors and electromagnetic induction
Chapter 22: Electric motors and electromagnetic induction The motor effect movement from electricity When a current is passed through a wire placed in a magnetic field a force is produced which acts on
2. Permanent Magnet (De-) Magnetization 2.1 Methodology
Permanent Magnet (De-) Magnetization and Soft Iron Hysteresis Effects: A comparison of FE analysis techniques A.M. Michaelides, J. Simkin, P. Kirby and C.P. Riley Cobham Technical Services Vector Fields
Permanent Magnetic Generator Construction Manual
Permanent Magnetic Generator Construction Manual http://hojomotor.com Our Team Doing an On-site Assembly in Peru http://hojomotor.com Section 1) Introduction This manual describes how to build a 'permanent
Circuits with inductors and alternating currents. Chapter 20 #45, 46, 47, 49
Circuits with inductors and alternating currents Chapter 20 #45, 46, 47, 49 RL circuits Ch. 20 (last section) Symbol for inductor looks like a spring. An inductor is a circuit element that has a large
Equipment: Power Supply, DAI, Synchronous motor (8241), Electrodynamometer (8960), Tachometer, Timing belt.
Lab 9: Synchronous motor. Objective: to examine the design of a 3-phase synchronous motor; to learn how to connect it; to obtain its starting characteristic; to determine the full-load characteristic of
Magnetic Fields and Their Effects
Name Date Time to Complete h m Partner Course/ Section / Grade Magnetic Fields and Their Effects This experiment is intended to give you some hands-on experience with the effects of, and in some cases
Massachusetts Institute of Technology Department of Electrical Engineering and Computer Science
Massachusetts Institute of Technology Department of Electrical Engineering and Computer Science 6.685 Electric Machines Class Notes 6: DC (Commutator) and Permanent Magnet Machines c 2005 James L. Kirtley
Brush DC Motor Basics. by Simon Pata Business Unit Manager, Brushless DC
thinkmotion Brush DC Motor Basics by Simon Pata Business Unit Manager, Brushless DC Ironless DC Motor Basics Technical Note Brushed DC ironless motors are found in a large variety of products and applications
Chen. Vibration Motor. Application note
Vibration Motor Application note Yangyi Chen April 4 th, 2013 1 Table of Contents Pages Executive Summary ---------------------------------------------------------------------------------------- 1 1. Table
Principles of Adjustable Frequency Drives
What is an Adjustable Frequency Drive? An adjustable frequency drive is a system for controlling the speed of an AC motor by controlling the frequency of the power supplied to the motor. A basic adjustable
EEE1001/PHY1002. Magnetic Circuits. The circuit is of length l=2πr. B andφ circulate
1 Magnetic Circuits Just as we view electric circuits as related to the flow of charge, we can also view magnetic flux flowing around a magnetic circuit. The sum of fluxes entering a point must sum to
Chapter 7. Magnetism and Electromagnetism ISU EE. C.Y. Lee
Chapter 7 Magnetism and Electromagnetism Objectives Explain the principles of the magnetic field Explain the principles of electromagnetism Describe the principle of operation for several types of electromagnetic
Drive circuit basics + V. τ e. Industrial Circuits Application Note. Winding resistance and inductance
ndustrial Circuits Application Note Drive circuit basics For a given size of a stepper motor, a limited space is available for the windings. n the process of optimizing a stepper motor drive system, an
Chapter 10. AC Inductor Design. Copyright 2004 by Marcel Dekker, Inc. All Rights Reserved.
Chapter 10 AC Inductor Design Table of Contents 1. Introduction 2. Requirements 3. Relationship of, A p, to the Inductor Volt-Amp Capability 4. Relationship of, K g, to the Inductor Volt-Amp Capability
STUDY GUIDE: ELECTRICITY AND MAGNETISM
319 S. Naperville Road Wheaton, IL 60187 www.questionsgalore.net Phone: (630) 580-5735 E-Mail: [email protected] Fax: (630) 580-5765 STUDY GUIDE: ELECTRICITY AND MAGNETISM An atom is made of three
Low Cost Design Study of Brushless DC Motor for Electric Water Pump Application
J Electr Eng Technol Vol. 9, No.?: 742-?, 2014 http://dx.doi.org/10.5370/jeet.2014.9.?.742 ISSN(Print) 1975-0102 ISSN(Online) 2093-7423 Low Cost Design Study of Brushless DC Motor for Electric Water Pump
DC generator theory. Resources and methods for learning about these subjects (list a few here, in preparation for your research):
DC generator theory This worksheet and all related files are licensed under the Creative Commons Attribution License, version 1.0. To view a copy of this license, visit http://creativecommons.org/licenses/by/1.0/,
Synchronous motor. Type. Non-excited motors
Synchronous motor A synchronous electric motor is an AC motor in which the rotation rate of the shaft is synchronized with the frequency of the AC supply current; the rotation period is exactly equal to
SLOT FRINGING EFFECT ON THE MAGNETIC CHARACTERISTICS OF ELECTRICAL MACHINES
Journal of ELECTRICAL ENGINEERING, VOL. 60, NO. 1, 2009, 18 23 SLOT FRINGING EFFECT ON THE MAGNETIC CHARACTERISTICS OF ELECTRICAL MACHINES Mohammad B. B. Sharifian Mohammad R. Feyzi Meysam Farrokhifar
ABB ! CAUTION. Type COQ Negative Sequence Generator Relay. (50/60 Hertz) 41-161J. Instruction Leaflet
ABB Instruction Leaflet 41-161J Effective: May 1997 Supersedes I.L. 41-161H Dated July 1984 ( ) Denotes Change Since Previous Issue Type COQ Negative Sequence Generator Relay (50/60 Hertz)! CAUTION Before
1150 hp motor design, electromagnetic and thermal analysis
115 hp motor design, electromagnetic and thermal analysis Qasim Al Akayshee 1, and David A Staton 2 1 Mawdsley s Ltd., The Perry Centre, Davey Close, Waterwells, Gloucester GL2 4AD phone: +44 1452 888311
Keywords: synchronous generator, synchronous motor, automatic voltage regulator, V- curves, synchronizing power, hunting, excitation system
SYNCHRONOUS MACHINES Tze-Fun Chan Hong Kong Polytechnic University, Hong Kong, China Keywords: synchronous generator, synchronous motor, automatic voltage regulator, V- curves, synchronizing power, hunting,
Chapter 16. Current Transformer Design. Copyright 2004 by Marcel Dekker, Inc. All Rights Reserved.
Chapter 16 Current Transformer Design Table of Contents 1. Introduction 2. Analysis of the Input Current Component 3. Unique to a Current Transformer 4. Current Transformer Circuit Applications 5. Current
UTILIZATION OF MECHANICAL ENERGY FROM ROTATION OF CEILING FAN TO GENERATE ELECTRICITY (Mini Generator Using Conventional Machine)
UTILIZATION OF MECHANICAL ENERGY FROM ROTATION OF CEILING FAN TO GENERATE ELECTRICITY (Mini Generator Using Conventional Machine) Vinay Pattanashetti 1, Angelo L Noronha 2, Prashant D Hulaji 3 1, 2, 3
Chapter 11. Inductors ISU EE. C.Y. Lee
Chapter 11 Inductors Objectives Describe the basic structure and characteristics of an inductor Discuss various types of inductors Analyze series inductors Analyze parallel inductors Analyze inductive
SECTION 4 ELECTRIC MOTORS UNIT 17: TYPES OF ELECTRIC MOTORS
SECTION 4 ELECTRIC MOTORS UNIT 17: TYPES OF ELECTRIC MOTORS UNIT OBJECTIVES After studying this unit, the reader should be able to Describe the different types of open single-phase motors used to drive
Permanent Magnetic Couplings and Brakes for Drive Technology
Tridelta Magnetsysteme A Tridelta Group Company Permanent Magnetic Couplings and Brakes for Drive Technology Raw Materials Magnets Systems and Components Magnet N1 Soft iron N2 Resin Introduction and principals
UNIT 3 AUTOMOBILE ELECTRICAL SYSTEMS
UNIT 3 AUTOMOBILE ELECTRICAL SYSTEMS Automobile Electrical Structure 3.1 Introduction Objectives 3.2 Ignition System 3.3 Requirement of an Ignition System 3.4 Types of Ignition 3.4.1 Battery or Coil Ignition
OVERCURRENT & EARTH FAULT RELAYS. To study the protection of equipment and system by relays in conjunction with switchgear.
OVERCURRENT & EARTH FAULT RELAYS Objective: To study the protection of equipment and system by relays in conjunction with switchgear. Theory: The function of a relay is to detect abnormal conditions in
How to Optimize Performance and Minimize Size in High Speed Applications High Performance Brushless DC Motors
thinkmotion How to Optimize Performance and Minimize Size in High Speed Applications High Performance Brushless DC Motors I. Introduction II. III. IV. Optimization of a Brushless DC motor for high speed
PS-6.2 Explain the factors that determine potential and kinetic energy and the transformation of one to the other.
PS-6.1 Explain how the law of conservation of energy applies to the transformation of various forms of energy (including mechanical energy, electrical energy, chemical energy, light energy, sound energy,
Theory of Heating by Induction
CHAPTER 2 Theory of Heating by Induction INDUCTION HEATING was first noted when it was found that heat was produced in transformer and motor windings, as mentioned in the Chapter Heat Treating of Metal
CONTINUOUS AUTOMATED FLUX MONITORING FOR TURBINE GENERATOR ROTOR CONDITION ASSESSMENT
CONTINUOUS AUTOMATED FLUX MONITORING FOR TURBINE GENERATOR ROTOR CONDITION ASSESSMENT Abstract J. Kapler, S. Campbell, M. Credland Iris Power Engineering Inc. Toronto, Canada Flux monitoring via permanently
ELECTRODYNAMICS 05 AUGUST 2014
ELECTRODYNAMICS 05 AUGUST 2014 In this lesson we: Lesson Description Discuss the motor effect Discuss how generators and motors work. Summary The Motor Effect In order to realise the motor effect, the
Preview of Period 16: Motors and Generators
Preview of Period 16: Motors and Generators 16.1 DC Electric Motors What causes the rotor of a motor to spin? 16.2 Simple DC Motors What causes a changing magnetic field in the simple coil motor? 16.3
Development Of High Efficiency Brushless DC Motor With New Manufacturing Method Of Stator For Compressors
Purdue University Purdue e-pubs International Compressor Engineering Conference School of Mechanical Engineering 2002 Development Of High Efficiency Brushless DC Motor With New Manufacturing Method Of
Build A Simple Electric Motor (example #1)
PHY115 Experiment 11 Build A Simple Electric Motor (example #1) MATERIAL This is the necessary equipment. Present any list of material in your written lab report. 1.5 V battery in series 1 ceramic magnet
Magnetism Basics. Magnetic Domains: atomic regions of aligned magnetic poles Random Alignment Ferromagnetic Alignment. Net Effect = Zero!
Magnetism Basics Source: electric currents Magnetic Domains: atomic regions of aligned magnetic poles Random Alignment Ferromagnetic Alignment Net Effect = Zero! Net Effect = Additive! Bipolar: all magnets
How To Understand And Understand The Electrical Power System
DOE-HDBK-1011/4-92 JUNE 1992 DOE FUNDAMENTALS HANDBOOK ELECTRICAL SCIENCE Volume 4 of 4 U.S. Department of Energy Washington, D.C. 20585 FSC-6910 Distribution Statement A. Approved for public release;
Introduction. Three-phase induction motors are the most common and frequently encountered machines in industry
Induction Motors Introduction Three-phase induction motors are the most common and frequently encountered machines in industry - simple design, rugged, low-price, easy maintenance - wide range of power
Performance Comparison of Dual-Rotor Radial-Flux and Axial-Flux Permanent-Magnet BLDC Machines
Performance Comparison of Dual-Rotor Radial-Flux and Axial-Flux Permanent-Magnet BLDC Machines Ronghai Qu, Member, IEEE Electronic & Photonic Systems Technologies General Electric Company Bldg EP, Rm 110-B,
BASIC ELECTRONICS AC CIRCUIT ANALYSIS. December 2011
AM 5-202 BASIC ELECTRONICS AC CIRCUIT ANALYSIS December 2011 DISTRIBUTION RESTRICTION: Approved for Pubic Release. Distribution is unlimited. DEPARTMENT OF THE ARMY MILITARY AUXILIARY RADIO SYSTEM FORT
CNC Machine Control Unit
NC Hardware a NC Hardware CNC Machine Control Unit Servo Drive Control Hydraulic Servo Drive Hydraulic power supply unit Servo valve Servo amplifiers Hydraulic motor Hydraulic Servo Valve Hydraulic Servo
45. The peak value of an alternating current in a 1500-W device is 5.4 A. What is the rms voltage across?
PHYS Practice Problems hapters 8- hapter 8. 45. The peak value of an alternating current in a 5-W device is 5.4 A. What is the rms voltage across? The power and current can be used to find the peak voltage,
Faraday s Law of Induction
Chapter 10 Faraday s Law of Induction 10.1 Faraday s Law of Induction...10-10.1.1 Magnetic Flux...10-3 10.1. Lenz s Law...10-5 10. Motional EMF...10-7 10.3 Induced Electric Field...10-10 10.4 Generators...10-1
THREE-PHASE INDUCTION MOTOR March 2007
THREE-PHASE INDUCTION MOTOR March 2007 A. PREPARATION 1. Introduction 2. The Rotating Field 3. Rotor Currents 4. Induction Motor Equivalent Circuit 5. Torque and Power Characteristics 6. Operation Beyond
Force on a square loop of current in a uniform B-field.
Force on a square loop of current in a uniform B-field. F top = 0 θ = 0; sinθ = 0; so F B = 0 F bottom = 0 F left = I a B (out of page) F right = I a B (into page) Assume loop is on a frictionless axis
ELECTRICAL ENGINEERING Vol. III - Induction Motor and Self-Excited Induction Generator - Tze-Fun Chan
INDUCTION MOTOR AND SELFEXCITED INDUCTION GENERATOR TzeFun Chan The Hong Kong Polytechnic University, Hung Hom, Kowloon, Hong Kong, China Keywords: threephase induction motor, singlephase induction motor,
Conceptual: 1, 3, 5, 6, 8, 16, 18, 19. Problems: 4, 6, 8, 11, 16, 20, 23, 27, 34, 41, 45, 56, 60, 65. Conceptual Questions
Conceptual: 1, 3, 5, 6, 8, 16, 18, 19 Problems: 4, 6, 8, 11, 16, 20, 23, 27, 34, 41, 45, 56, 60, 65 Conceptual Questions 1. The magnetic field cannot be described as the magnetic force per unit charge
SOLID MECHANICS TUTORIAL MECHANISMS KINEMATICS - VELOCITY AND ACCELERATION DIAGRAMS
SOLID MECHANICS TUTORIAL MECHANISMS KINEMATICS - VELOCITY AND ACCELERATION DIAGRAMS This work covers elements of the syllabus for the Engineering Council exams C105 Mechanical and Structural Engineering
