8.1 DC Motor

Total Page:16

File Type:pdf, Size:1020Kb

8.1 DC Motor IV B. Tech I semester (JNTUH-R15) Prepared By Ms. Lekha Chandran, Assistant Professor Unit-1 ELECTRIC DRIVE ELECTRICAL ENERGY It is flexible Easilyavailable Can be converted to other forms of energy. Can be easily transported to required location Economical Mature technology Saves manual labor in industry and domestic applications UTILISATION Electrical energy is used in variousapplications: 1. Electric Drives; DC and ACmotors 2. Electric heating and welding 3. Illumination 4. Electric Traction 5. Electric Vehicles DC MOTOR • The direct current (dc) machine can be used asa motor or as agenerator. • DC Machine is most often used for amotor. • The major advantages of dc machines are theeasy speed and torqueregulation. • However, their application is limited to mills, mines and trains. As examples, trolleys and underground subway cars may use dcmotors. • In the past, automobiles were equipped withdc dynamos to charge theirbatteries. DC MOTOR • Eventoday the starter is a series dc motor • However, the recent development of power electronics has reduced the use of dc motorsand generators. • The electronically controlled ac drives aregradually replacing the dc motor drives infactories. • Nevertheless, a large number of dc motors arestill used by industry and several thousand are sold annually. CONSTRUCTI ON DC MACHINE CONSTRUCTION General arrangement of a dc machine DC MACHINES • Thestator of the dc motor has poles, which are excited by dc current to produce magnetic fields. • Inthe neutral zone, in the middle between the poles,commutating poles are placed to reduce sparking of the commutator. The commutating poles are supplied by dccurrent. • Compensating windings are mounted on the main poles. These short-circuitedwindings damp rotor oscillations. DC MACHINES • The poles are mounted onan iron core that provides a closed magneticcircuit. • The motor housing supports the iron core, the brushesand thebearings. • The rotor has a ring-shaped laminated iron core withslots. • Coils with several turns are placed in the slots. The distance between the twolegs of the coil is about 180 electric degrees. DC MACHINES • The coils are connected inseries through the commutator segments. • The ends of each coil are connected to acommutator segment. • The commutator consists of insulated copper segments mounted on an insulatedtube. • Twobrushesare pressedto the commutator to permit current flow. • The brushes are placed in the neutral zone, where themagnetic field is close to zero, to reduce arcing. DC MACHINES • The rotor has a ring-shaped laminated iron core withslots. • The commutator consists of insulated copper segments mounted onan insulated tube. • Two brushes are pressedto the commutator to permit currentflow. • The brushes are placed in the neutral zone, where the magneticfield is close to zero, to reducearcing. DC MACHINES • The commutator switches the current from one rotor coil to the adjacentcoil, • The switching requiresthe interruption of the coil current. • The sudden interruption ofan inductive current generates high voltages. • The high voltage produces flashover and arcingbetween the commutator segmentand thebrush. DC MACHINE CONSTRUCTION Rotation I /2 Ir_dc/2 I r_dc Brush r_dc Pole winding Shaft | 1 2 8 N 7 3 S 6 4 5 Insulation Copper Rotor segment Ir_dc Winding Fig:Commutator with the rotor coils connections. DC MACHINE CONSTRUCTION Fig: Details of the Commutator ofa dc motor. DC MACHINE CONSTRUCTION Fig:DC motor stator with polesvisible. DC MACHINE CONSTRUCTION Fig:Rotor of adc motor. DC MACHINE CONSTRUCTION Fig: Cutaway view of a dc motor. DC MOTOR OPERATION DC MOTOR OPERATION • In a dc motor, the stator poles are supplied by dc Rotation I I /2 Ir_dc/2 r_dc r_dc excitation current,which Brush Pole winding produces a dc magnetic Shaft field. 1 2 • The rotor is supplied by 8 dc current through the N 7 3 S 6 4 brushes, commutatorand 5 coils. • The interaction of the Insulation Copper Rotor I segment magnetic field and rotor Winding r_dc current generates aforce that drives themotor DC MOTOROPERATION v B • The magnetic field linesenter a into the rotor from the north S 30 N pole (N) and exit toward the Vdc south pole(S). b • The poles generate a v magnetic field that is Ir_dc perpendicular to thecurrent (a) Rotor current flow from segment 1 to 2 (slot a to b) carryingconductors. • The interaction betweenthe B field and the current a produces a Lorentzforce, S N v 30 v V • The force is perpendicular to dc both the magnetic field and b conductor Ir_dc (b) Rotor current flow from segment 2 to 1 (slot b to a) DC MOTOROPERATION v B • The generated force turns therotor a until the coil reaches the neutral S 30 N point between thepoles. Vdc • At this point, the magnetic field b becomes practically zerotogether v with theforce. Ir_dc • However, inertia drives the motor (a) Rotor current flow from segment 1 to 2 (slot a to b) beyond theneutral zone where the direction of the magnetic field B reverses. a • To avoid the reversal of the force S N 30 V direction, the commutatorchanges v v dc the current direction, which b maintains the counterclockwise rotation. Ir_dc (b) Rotor current flow from segment 2 to 1 (slot b to a) DC MOTOROPERATION v B • Before reaching the neutral zone, a the current enters insegment 1 and exits from segment2, S 30 N Vdc • Therefore, current enters the coil end at slot a and exits from slot b b during thisstage. v I • After passing the neutral zone, the r_dc current enters segment 2 and exits (a) Rotor current flow from segment 1 to 2 (slot a to b) from segment1, B • This reverses the currentdirection a through the rotor coil, when the S 30 N coil passes the neutral zone. v v Vdc • The result of this currentreversal is b the maintenance of therotation. Ir_dc (b) Rotor current flow from segment 2 to 1 (slot bto a) DC GENERATO R OPERATIO N DC GENERATOROPERATION v B • The N-S poles produce adc a magnetic field and the S N rotorcoil turns in thisfield. 30 Vdc • Aturbine or othermachine b drives therotor. v Ir_dc • The conductors in the (a) Rotor current flow from segment 1 to 2 (slot ato slots cut the magnetic flux b) lines, which inducevoltage B in the rotorcoils. a S N • The coil has two sides: 30 v v Vdc one is placed in slot a, the other in slotb. b Ir_dc (b) Rotor current flow from segment 2 to 1 (slot b to a) DC GENERATOROPERATION • In Figure 8.11A, the v B conductorsin slot aare a cutting the field lines S N entering into the rotor 30 Vdc from the northpole, b • The conductors in slot b v are cutting the fieldlines Ir_dc exiting from the rotor to (a) Rotor current flow from segment 1 to 2 (slot ato the south pole. b) • The cutting of the field B lines generates voltagein a theconductors. S 30 N • The voltages generatedin v v Vdc the two sides of the coil areadded. b Ir_dc (b) Rotor current flow from segment 2 to 1 (slot b to a) DC GENERATOROPERATION • The induced voltage is v B connected to thegenerator a S N terminals through the 30 V commutator andbrushes. dc • In Figure 8.11A, the induced b voltage in b is positive, and in v Ir_dc a isnegative. (a) Rotor current flow from segment 1 to 2 (slot ato • The positive terminal is b) connected tocommutator B segment 2 and to the a conductors in slotb. S N v 30 V • The negative terminal is v dc connected to segment 1and b to the conductorsin slota. Ir_dc (b) Rotor current flow from segment 2 to 1 (slot b to a) DC GENERATOROPERATION • When the coil passesthe v B neutralzone: a S N 30 – Conductors in slot a arethen Vdc moving toward the south pole and cut flux lines b exiting from therotor v – Conductors in slot b cut the Ir_dc flux lines entering the inslot (a) Rotor current flow from segment 1 to 2 (slot ato b. b) • This changes the polarity B of the induced voltage in a thecoil. S 30 N • The voltage induced in ais v v Vdc now positive, and in b is b negative. Ir_dc (b) Rotor current flow from segment 2 to 1 (slot b to a) DC GENERATOROPERATION v B • The simultaneously the a S N 30 commutator reverses its Vdc terminals, which assures b that the output voltage v I (Vdc) polarity is unchanged. r_dc (a) Rotor current flow from segment 1 to 2 (slot ato • In Figure 8.11B b) – the positive terminal is B connected to commutator a segment 1 and to the S N 30 V conductors in slota. v v dc – The negative terminal is b connected to segment 2 and to the conductors in slotb. Ir_dc (b) Rotor current flow from segment 2 to 1 (slot b to a) DC MACHINE EQUIVALENT CIRCUIT GENERATOR DC GENERATOR EQUIVALENTCIRCUIT • The magnetic field produced by the stator poles induces a voltage in the rotor (or armature) coils when the generator is rotated. • This induced voltage is represented by a voltagesource. • Thestator coil has resistance, which is connected inseries. • Thepole flux is produced by the DC excitation/field current, which is magnetically coupled to therotor • Thefield circuit has resistanceand asource • Thevoltagedrop on the brushes represented by abattery DC GENERATOR EQUIVALENTCIRCUIT V brush R Rf a Load max I If ag Vf Vdc Eag Mechanical Electrical power in power out Equivalent circuitof a separatelyexcited dc generator. DC GENERATOR EQUIVALENTCIRCUIT • The magnetic field produced by the stator poles induces a voltage in the rotor (or armature) coils when the generator isrotated. • The dc field current of the poles generatesa magneticflux • Theflux is proportional with the field current if the iron core is notsaturated: ag K1 I f DC GENERATOR EQUIVALENTCIRCUIT • The rotor conductors cut the field linesthat generate voltage in thecoils.
Recommended publications
  • 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.
    [Show full text]
  • DRM105, PM Sinusoidal Motor Vector Control with Quadrature
    PM Sinusoidal Motor Vector Control with Quadrature Encoder Designer Reference Manual Devices Supported: MCF51AC256 Document Number: DRM105 Rev. 0 09/2008 How to Reach Us: Home Page: www.freescale.com Web Support: http://www.freescale.com/support USA/Europe or Locations Not Listed: Freescale Semiconductor, Inc. Technical Information Center, EL516 2100 East Elliot Road Tempe, Arizona 85284 1-800-521-6274 or +1-480-768-2130 www.freescale.com/support Europe, Middle East, and Africa: Freescale Halbleiter Deutschland GmbH Technical Information Center Information in this document is provided solely to enable system and Schatzbogen 7 software implementers to use Freescale Semiconductor products. There are 81829 Muenchen, Germany no express or implied copyright licenses granted hereunder to design or +44 1296 380 456 (English) fabricate any integrated circuits or integrated circuits based on the +46 8 52200080 (English) information in this document. +49 89 92103 559 (German) +33 1 69 35 48 48 (French) www.freescale.com/support Freescale Semiconductor reserves the right to make changes without further notice to any products herein. Freescale Semiconductor makes no warranty, Japan: representation or guarantee regarding the suitability of its products for any Freescale Semiconductor Japan Ltd. particular purpose, nor does Freescale Semiconductor assume any liability Headquarters arising out of the application or use of any product or circuit, and specifically ARCO Tower 15F disclaims any and all liability, including without limitation consequential or 1-8-1, Shimo-Meguro, Meguro-ku, incidental damages. “Typical” parameters that may be provided in Freescale Tokyo 153-0064 Semiconductor data sheets and/or specifications can and do vary in different Japan applications and actual performance may vary over time.
    [Show full text]
  • 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.
    [Show full text]
  • 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.
    [Show full text]
  • 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
    [Show full text]
  • Single Phase to Single Phase Step-Down Cycloconverter for Electric Traction Applications
    American-Eurasian Journal of Scientific Research 11 (4): 271-274, 2016 ISSN 1818-6785 © IDOSI Publications, 2016 DOI: 10.5829/idosi.aejsr.2016.11.4.22905 Single Phase to Single Phase Step-Down Cycloconverter for Electric Traction Applications Mrs. J. Suganthi vinodhini and R. Samuel Rajesh Babu Research Scholar, Sathyabama University, India Abstract: In electric traction application electrical energy used was: 1.direct current and 2.alternating current. In this world already a constant voltage constant frequency single phase and three phase AC readily available. For some applications it is needed to have variable voltage and variable frequency for this conversions need between dc and ac sources and this conversion can be carried out by power converters. For converting AC–AC cycloconverter are widely used as a converter. The ns of alternating current drives relates with the frequency (f) and number of poles (p) present in the induction motor. It is not feasible by changing the poles of a motor under running processes, so the only one way during running condition the frequency can be varied. In the absence of direct current (DC) link with constant voltage constant frequency alternating current to variable voltage variable frequency alternating current is needed to run the electric traction applications, so the cycloconverter will make this as possible with reliable and economical. This work explains how to control the speed of single phase induction motor and single phase to single phase Cycloconverter using different frequency conversions with R Load was carried out using MATLAB / Simulink. Key words: Cycloconverter Electric traction Pulse width modulation Synchronous speed (ns ) INTRODUCTION switches instead of thyristors.
    [Show full text]
  • Report of Contributions
    MT25 Conference 2017 - Timetable, Abstracts, Orals and Posters Report of Contributions https://indico.cern.ch/e/MT25-2017 MT25 Conferenc … / Report of Contributions 3D Electromagnetic Analysis of Tu … Contribution ID: 5 Type: Poster Presentation of 1h45m 3D Electromagnetic Analysis of Tubular Permanent Magnet Linear Launcher Tuesday, 29 August 2017 13:15 (1h 45m) A short stroke and large thrust axial magnetized tubular permanent magnet linear launcher (TPMLL) with non-ferromagnetic rings is presented in this paper. Its 3D finite element (FE) models are estab- lished for sensitivity analyses on some parameters, such as air gap thickness, permanent magnet thickness, permanent magnet width, stator yoke thickness and four types of permanent magnet material, ferrite, NdFeB, AlNiCO5 and Sm2CO17 are conducted to achieve greatest thrust. Then its 2D finite element (FE) models are also established. The electromagnetic thrusts calculated by 2D and 3D finite element method (FEM) and got from prototype test are compared. Moreover, the prototype static and dynamic tests are conducted to verify the 2D and 3D electromagnetic analysis. The FE software FLUX provides the interface with the MATLAB/Simulink to establish combined simulation. To improve the accuracy of the simulation, the combined simulation between the model of the control system in Matlab/Simulink and the 3D FE model of the TPMLL in FLUX is built in this paper. The combined simulation between the control system and the 3D FE modelof the TPMLL is built. A prototype is manufactured according to the final designed dimensions. The photograph of the developed TPMLL prototype with thrust sensor and the magnetic powder brake as the load are shown.
    [Show full text]
  • Course Description Bachelor of Technology (Electrical Engineering)
    COURSE DESCRIPTION BACHELOR OF TECHNOLOGY (ELECTRICAL ENGINEERING) COLLEGE OF TECHNOLOGY AND ENGINEERING MAHARANA PRATAP UNIVERSITY OF AGRICULTURE AND TECHNOLOGY UDAIPUR (RAJASTHAN) SECOND YEAR (SEMESTER-I) BS 211 (All Branches) MATHEMATICS – III Cr. Hrs. 3 (3 + 0) L T P Credit 3 0 0 Hours 3 0 0 COURSE OUTCOME - CO1: Understand the need of numerical method for solving mathematical equations of various engineering problems., CO2: Provide interpolation techniques which are useful in analyzing the data that is in the form of unknown functionCO3: Discuss numerical integration and differentiation and solving problems which cannot be solved by conventional methods.CO4: Discuss the need of Laplace transform to convert systems from time to frequency domains and to understand application and working of Laplace transformations. UNIT-I Interpolation: Finite differences, various difference operators and theirrelationships, factorial notation. Interpolation with equal intervals;Newton’s forward and backward interpolation formulae, Lagrange’sinterpolation formula for unequal intervals. UNIT-II Gauss forward and backward interpolation formulae, Stirling’s andBessel’s central difference interpolation formulae. Numerical Differentiation: Numerical differentiation based on Newton’sforward and backward, Gauss forward and backward interpolation formulae. UNIT-III Numerical Integration: Numerical integration by Trapezoidal, Simpson’s rule. Numerical Solutions of Ordinary Differential Equations: Picard’s method,Taylor’s series method, Euler’s method, modified
    [Show full text]
  • Power Processing, Part 1. Electric Machinery Analysis
    DOCONEIT MORE BD 179 391 SE 029 295,. a 'AUTHOR Hamilton, Howard B. :TITLE Power Processing, Part 1.Electic Machinery Analyiis. ) INSTITUTION Pittsburgh Onii., Pa. SPONS AGENCY National Science Foundation, Washingtcn, PUB DATE 70 GRANT NSF-GY-4138 NOTE 4913.; For related documents, see SE 029 296-298 n EDRS PRICE MF01/PC10 PusiPostage. DESCRIPTORS *College Science; Ciirriculum Develoiment; ElectricityrFlectrOmechanical lechnology: Electronics; *Fagineering.Education; Higher Education;,Instructional'Materials; *Science Courses; Science Curiiculum:.*Science Education; *Science Materials; SCientific Concepts ABSTRACT A This publication was developed as aportion of a two-semester sequence commeicing ateither the sixth cr'seventh term of,the undergraduate program inelectrical engineering at the University of Pittsburgh. The materials of thetwo courses, produced by a ional Science Foundation grant, are concernedwith power convrs systems comprising power electronicdevices, electrouthchanical energy converters, and associated,logic Configurations necessary to cause the system to behave in a prescribed fashion. The emphisis in this portionof the two course sequence (Part 1)is on electric machinery analysis. lechnigues app;icable'to electric machines under dynamicconditions are anallzed. This publication consists of sevenchapters which cW-al with: (1) basic principles: (2) elementary concept of torqueand geherated voltage; (3)tile generalized machine;(4i direct current (7) macrimes; (5) cross field machines;(6),synchronous machines; and polyphase
    [Show full text]
  • DC Motor Workshop
    DC Motor Annotated Handout American Physical Society A. What You Already Know Make a labeled drawing to show what you think is inside the motor. Write down how you think the motor works. Please do this independently. This important step forces students to create a preliminary mental model for the motor, which will be their starting point. Since they are writing it down, they can compare it with their answer to the same question at the end of the activity. B. Observing and Disassembling the Motor 1. Use the small screwdriver to take the motor apart by bending back the two metal tabs that hold the white plastic end-piece in place. Pull off this plastic end-piece, and then slide out the part that spins, which is called the armature. 2. Describe what you see. 3. How do you think the motor works? Discuss this question with the others in your group. C. Mounting the Armature 1. Use the diagram below to locate the commutator—the split ring around the motor shaft. This is the armature. Shaft Commutator Coil of wire (electromagnetic) 2. Look at the drawing on the next page and find the brushes—two short ends of bare wire that make a "V". The brushes will make electrical contact with the commutator, and gravity will hold them together. In addition the brushes will support one end of the armature and cradle it to prevent side- to-side movement. 1 3. Using the cup, the two rubber bands, the piece of bare wire, and the three pieces of insulated wire, mount the armature as in the diagram below.
    [Show full text]
  • Design Procedure of a Permanent Magnet D.C. Commutator Motor
    International Journal of Engineering Research and Technology. ISSN 0974-3154 Volume 9, Number 1 (2016), pp. 53-60 © International Research Publication House http://www.irphouse.com Design Procedure of A Permanent Magnet D.C. Commutator Motor Ritunjoy Bhuyan HOD Electrical Engineering, HRH The Prince of Wales Institute of Engg & Technology (Govt.), Jorhat, Assam, India. Abstract Electrical machine with electro magnet as excitation system many problems out of which, less efficiency is a major one. Self excited dc machine has to sacrifice some power for excitation system as a result, power available for useful work become less. This problem can be solved to some extent whatever may be the amount , by using permanent magnet for the excitation system of dc machine and there by contributing towards the conservation of conventional energy sources which are alarmingly decrease day by day . Using of permanent magnet in the electrical machine helps in burning of less conventional fossil fuel and contributes indirectly in conservation of air- pollution free environment. With permanent magnet dc motor, the efficiency of the machine also rise up considerably. This paper is an effort to give a computer aided design procedure of permanent magnet dc motor. Keywords: permanent magnet dc motor, yoke, pole pitch, commutator, magnetic loading, electric loading, output coefficient. Introduction It can be stated without any dispute that for the ever developing modern civilization electric motor become an unavoidable part both in industrial product as well as domestic applications. But ever since the growing threat of running out of the conventional energy source used by the mankind by the middle of the next century, the scientists have very desperately engaged themselves for last few decades in molding suitable devices for conservation of different form of conventional energy.
    [Show full text]
  • Brushless DC Electric Motor
    Please read: A personal appeal from Wikipedia author Dr. Sengai Podhuvan We now accept ₹ (INR) Brushless DC electric motor From Wikipedia, the free encyclopedia Jump to: navigation, search A microprocessor-controlled BLDC motor powering a micro remote-controlled airplane. This external rotor motor weighs 5 grams, consumes approximately 11 watts (15 millihorsepower) and produces thrust of more than twice the weight of the plane. Contents [hide] 1 Brushless versus Brushed motor 2 Controller implementations 3 Variations in construction 4 AC and DC power supplies 5 KM rating 6 Kv rating 7 Applications o 7.1 Transport o 7.2 Heating and ventilation o 7.3 Industrial Engineering . 7.3.1 Motion Control Systems . 7.3.2 Positioning and Actuation Systems o 7.4 Stepper motor o 7.5 Model engineering 8 See also 9 References 10 External links Brushless DC motors (BLDC motors, BL motors) also known as electronically commutated motors (ECMs, EC motors) are electric motors powered by direct-current (DC) electricity and having electronic commutation systems, rather than mechanical commutators and brushes. The current-to-torque and frequency-to-speed relationships of BLDC motors are linear. BLDC motors may be described as stepper motors, with fixed permanent magnets and possibly more poles on the rotor than the stator, or reluctance motors. The latter may be without permanent magnets, just poles that are induced on the rotor then pulled into alignment by timed stator windings. However, the term stepper motor tends to be used for motors that are designed specifically to be operated in a mode where they are frequently stopped with the rotor in a defined angular position; this page describes more general BLDC motor principles, though there is overlap.
    [Show full text]