STUDY OF INDUCTION MACHINE UNDER TRANSIENT NT DUTY
|
|
- Loreen Thomas
- 5 years ago
- Views:
Transcription
1 STUDY OF INDUCTION MACHINE STUDY OF INDUCTION MACHINE UNDE TANSIENT NT DUTY AND STEADY-STATE STATE AS SYNCHONIZED MACHINE Prof. Eng. Aleandru Simion, PhD, Assoc. Prof. Eng. Leond Livadu, PhD, Assist. Prof. Eng. Adrian Munteanu, PhD Gheorghe Asachi Technical University from Iaşi, Electrical Engineering Faculty, EZUMAT. In vederea analizei minii inone trifazate in regim de mina sinona (mina inona sinonizata MAS se apeleaza la ecuatiile diferentiale de ordinul I exprimate numai în fluxuri totale si unghiul de rotatie.. Se obtine un sistem de 8 ecuatii ce se refera: la cele faze statorice, la cele faze rotorice, (dintre ce 2 sunt inseriate si sunt alimentate de la o sursa de curent continuu, constituind infurea de excitatie, i cea de-a treia constituie infurea de amortize, fiind conectata in scurtcircuit, la ce se mai adauga 2 ecuatii de misce. Acetă A aborde permite obtinerea unor informatii directe-precise despre fenomenele ce au loc în mina, inclusiv si despre directiile de actiune ale fluxurilor magnetice adică despre unghiul intern instantaneu. Pe baza acestor informatii se pot adopta strategii s adecvate si lua decizii pertinente privind momentele favorabile ale cuplării înfăsurărilor la surse. Trebuie evitata situaţia de deose, de d exemplu, cand se declansează un regim tranzitoriu electromecanic cu constantă de timp me, ce întârzie procesul cu o durată ce poate fi egala cu dublul timpului neces pornirii. Se insista upra utilizii hodografului fluxului rezultant rotoric ca instrument eficient, cu reale valente didactice în aprecierea comportii minii de inductie sinonizate in diverse regimuri: tranzitorii sau statione. Cuvinte cheie: motor inon de putere me, condiţii de pornire speciale, două colivii rotorice, simule MEF ABSTACT. For the analysis of the three-phe induction machine under synchronous operation n (the so-called synchronized induction machine, SIM one uses first order differential equations that contains nothing but total fluxes and rotation angle. The resulted 8 equations system chacterize the stator phes, the rotor phes (2 of them e series connected and fed from a DC source and the third is short-circuited and play the role of a damper winding and the movement of the rotor (the lt 2 equations. This approach allows the obtaining of direct and proper information about the intimate phenomena that take place inside the machine including the direction of magnetic fluxes, which leads to the instantaneous internal angle. On the bis of this information, one can adopt proper strategies concerning the most favourable moment for the connection of the windings to the supply sources. The pulling out must be avoided, for example when stts a transient duty with high time constant which delays the process with a length that may attain twice the value of the stting time. The hodograph of the resultant rotor flux is considered a very effective tool, also for didactic purpose, that desibe the behavior of the synchronized induction machine under different duties such transients or steady state. Keywords: high power induction motor, stt-up constraints, two squirrel cages of distinct materials, FEM simulation. INTODUCTION A pticul duty of the doubly-fed wound rotor three-phe induction machine [, 2] refers to the socalled situation of synchronized induction machine-sim [] whose schematic diagram is presented in Fig. []. The main chacteristic of this operation mode consists in the fact that it put together the qualities of induction machine (safe stting with less expensive auxiliy devices, high stting torque with the ones of the synchronous machine with electromagnetic excitation (operation with high power factor, sometimes even synchronous compensator, constant speed, high pull-out torque, etc.. Due to these advantages, the SIM is used under motoring duty for high power applications, concerning constant speed and single direction of rotation such pumps, fans, compressors and roller mills [2,, 4, 5, 6]. Coming back to the schematic diagram (Fig., a SIM operates follows. Initially, after connection to the mains of the three-phe stator winding by means of K, the rotor winding is short-circuited (or connected to an auxiliy resistance and the rotor stts and accelerates close to synchronous speed (K2 h the mobile contacts to the left side. Shortly after that, the mobile contacts of K2 e moved to the right side when the rotor phe is short-circuited and the other two phes, and become series connected and fed from a DC source. After a few oscillations, the synchronizing torque that acts between the stator rotating field and the rotor (which h a constant magnetic field a succession of magnetic poles on the perifery pulls the rotor into synchronous speed. Buletinul AGI nr. 4/22 octomie-decemie 29
2 CONFEINŢA NATIONAL NAŢIONALĂ CONFEENCE DE ACŢIONĂI OF ELECTICAL ELECTICE, DIVES ediţia XVI, CNAE SUCEAVA L L2 L Fig.. Schematic diagram of synchronized induction machine. Consequently, the machine becomes a synchronous motor, which is capable to drive a load machine. Lately, the electromechanical conversion of mio wind power plants uses frequently induction generators, which sometimes change their duty into synchronized induction generators (SIGs. 2. EQUATIONS OF THEE-PHASE INDUCTION MACHINE IN TOTAL FLUXES The analysis of three-phe machine can be generally done (including unbalanced supply systems either for stator or rotor windings by putting together the 6 equations of the electric circuits containing nothing but total fluxes and voltages and the 2 movement-torque balance equations where appes the electromagnetic torque (deduced from magnetic coenergy viation and the rotation angle of the rotor, θ [2, 7]. Under symbolic method, one obtains a first order system with 8 equations, (-8: ( s + ν st = u ν sr ( + + ν σs ( [ [ [ [ K ( 2 + ( ( s + ν st = u ν sr ( + + ν σs ( ( ( s + ν st = u ν sr ( + + ν σs ( ( ( s + ν rt = u ν rs ( + + ν σr ( 2 + ( ] f SIM n +U -U S K2 M st (2 ( (4 [ ( s + ν rt = u ν rs ( + + ν σr ( ( ( s + ν rt = ν rs ( + r + ν σr ( ( ] [ & k z p θ s + = J J + (2 + + ( dθ dt [ ( ] pλ 2 { } M st sinθ [ + (2 + ( (2 + ] + (5 (6 + (7 = & θ = ω (8 The first equations contain the values of the balanced supply voltages connected to the stator phes, that is U max =U max =U max =49V, ω s =4.rad/s; u - behind u with 2π/ rad. The synchronized induction machine h a pticulity concerns the rotor. The phe-voltage is null, u =, (this phe becomes a damper winding and the other 2 phes e series connected and fed from a DC source with a voltage of (-4, +4V.. THE SIMULATION STUDY OF THE SYNCHONIZED INDUCTION MACHINE For a three-phe machine with the following pameters (SI units: s = r =2; L hs =.9; L σs = L σr =.; J=.5; p=2; k z =.2; ω =4. one obtains the equation system: ( s + 5,5 = 2,26( + + 2,26( ,88( u ( s + 5,5 = 2,26( + + 2,26( ,88( u sinθ ( s + 5,5 = 2,26( + + 2,26( ,88( u sin θ ( s + 5,5 = 2,26( + + 2,26( ,88( u ( s + 5,5 = 2,26( + + 2,26( 2 u + 55,88( ( s + 5,5 = 2,26( + + 2,26( ,88( u 2 292
3 STUDY OF INDUCTION MACHINE UNDE TANSIENT DUTY AND STEADY-STATE STUDY OF AS INDUCTION SYNCHONIZED MACHINE MACHINE ( s +,4 = ( 4 ( 2,26 { sin θ [ ( 2 ( 2 + ( 2 ] + [ ( + ( + ( ]} M θ & θ = ω s + On the bis of these equations, the structural diagram in Matlab-Simulink environment h been ied out and numerous simulations were performed. A few representative ones e presented follows. Two distinct ces will be discussed concerning the operation synchronized induction generator (SIG. a DAGS ce. This ce used the mathematical model desibed by the equation system (-8 and the pameter values presented above. The schematic diagram corresponds to Fig.. Initially, the mobile contacts e placed to the left position and K is switched on. The machine stts at no-load, induction motor, developing a small torque, line viable with speed, necessy for frictions. The stt-up process takes less then.2 sec. The viations of the electromagnetic torque and of the angul velocity e presented in Fig. 2 and Fig., respectively. The electromagnetic torque value gets ound Nm and the angul velocity comes ne synchronous speed, 57rad/s Fig. 2. M e =f(t for a SIG with torque enforcement of -7 Nm at the moment t =.4 s and put under excitation at the moment t 2 =.6s. At the moment t =.4sec., a load torque of -7 Nm is applied and the machine becomes a SIG. The value of the speed rises with a few percents over synchronous one, the slip and developed electromagnetic torque become both negative. The stator active power changes its sign. At the moment t 2 =.6sec., K2 moves the mobile contacts to the right position. Consequently, two rotor phes e series connected and fed from a DC source (U =-4V, U =+4V. They become excitation winding. The third rotor phe stays short-circuited (U = and becomes damping winding for the machine that operates non salient pole synchronous machine. st 5 5 Ω [rad/s] Fig.. Ω =f(t for a SIG with torque enforcement of -7 Nm at the moment t =.4 s and put under excitation at the moment t 2 =.6s. Now, the electromagnetic torque determines a deceleration of the rotor and after a few oscillations the speed reaches the synchronous value. Further, the machine operates synchronized induction generator connected to the mains. Fig. 4 presents the dynamic chacteristic. The operation is desibed by the points order: A(stt-up M(the lt transit through maximum stting torque value S(cui-synchronism no-load motoring duty S(induction generator (synchronized induction generator. S - A Ω [rad/s] Fig. 4. Dynamic chacteristic Ω =f(m e for a SIG with torque enforcement of -7 Nm at the moment t =.4s and put under excitation at the moment t 2 =.6s. Fig. 5 shows the hodograph of the resultant rotor flux. Initially, the flux is null and corresponds to the A point. Than, during stt-up, the rotor flux rises and tracks a limit value (over-synchronism speed overshoot S point than goes to S and the rotor gets the synchronism no-load motoring duty. The enforcement of a load torque of -7 Nm (t =.4 sec. determines the curve S-S on the hodograph that coresponds to over-synonism generator duty. S M Buletinul AGI nr. 4/22 octomie-decemie 29
4 CONFEINŢA NATIONAL NAŢIONALĂ CONFEENCE DE ACŢIONĂI OF ELECTICAL ELECTICE, DIVES ediţia XVI, CNAE SUCEAVA A ' Fig. 5. esultant rotor for a SIG with torque enforcement of -7 Nm at the moment t =.4 s and put under excitation at the moment t 2 =.6s. The induction generator is then DC energized, at the moment t 2 =.6 sec. and the magnetic flux, the rotor flux pticully, suddenly inees. The machine becomes a synchonized generator and the hodograph tracks the S-'- sector. The operation point lays in long the load remains unmodified. A deeper investigation of the hodograph movement reveals the followings: - i for suynchronous speeds, the hodograph tracks anti-clockwise (positive spirals which e simil to transient duty but they become circles for steady-state. This behavior desibes the induction motor duty (Fig. 5 sector A-S excepting the nrow ea that corresponds to the over-speed before S point; - ii for oversynchronous speeds, the hodograph tracks clockwise (negative spirals which e simil to transient duty but they become circles for steady-state. This behavior desibes the induction generator duty (Fig. 5 sector S-S plus the nrow ea that corresponds to the over-speed before S point; - iii for synchronous speeds, at steady-state and constant load, the hodograph becomes a point and the machine operates synchronized induction generator (Fig. 5 point. The synchronization process (sector S-'-, Fig. 5 is accompanied by ocillations of the speed, of total fluxes of both rotor and stator and of the torque values. The movement of the hodograph is also esentially influenced by the moment when the rotor windings e connected to the DC source. More precisely, at the end of the transient duty, an internal angle will exist between the resultant rotor flux and the resultant stator flux. This angle depends on load degree and h a certain but constant value. Since, at the connection moment, the rotor position (and the rotor flux position too is aleatory then the synchronization process (with all the accompanying events depends on the initial S S' S moment of the transitory process. Consequently, the machine may operate from a duty to another (and the hodograph rotates towd both directions damped oscillations until it reaches the steady-state point operation, which corresponds to the load degree. The manner used in writing the equations (using quantities the applied voltages, total magnetic fluxes and rotation angle allows a deep analysis, which is very useful for didactic purposes but also for the study of transient duties that e specific to induction machines, including the unbalanced operation such SIG [2]. To justify this statement, a second study ce is presented follows. b Ce DAG. The symmetric three-phe machine (the same pameters in the previous ce with perfect symmetry both in stator and rotor (which is short-circuited is connected to the mains (t = and stts a no-load induction motor. The electromagnetic torque, M e, h significant values (Fig. 6 and after a few oscillations, the torque reaches a low value ( Nm, which corresponds to frictions Fig. 6. M e =f(t for a SIG with no-load stt-up, torque enforcement of -7 Nm at the moment t =.s, put under excitation at the moment t 2 =.42s, a second torque enforcement of -Nm at the moment t =.8s, and complete unload at the moment t 4 =s. The speed inees rapidly in approx.. sec. (gets over synchronism and then goes to a value close to synchronism, Fig. 7. On the dynamic mechanical chacteristic, Fig. 8, the representative point A stts from zero and tracks the sector A-M-As, close to synchronism. The hodograph of resultant rotor flux stts from A, Fig. 9, and tracks some anti-clockwise repetitional cycles (sector A-M-S'-As, see the rows, excepting a nrow sector by the SO point (overshoot process. - At the moment t =.sec, the induction machine operation switches to generating duty by applying an opposed torque of -7 Nm. This fact determines a response of the electromagnetic torque, which oscillates ound this value. The slip turns to a negative value and 4 294
5 STUDY OF INDUCTION MACHINE UNDE TANSIENT DUTY AND STEADY-STATE STUDY OF AS INDUCTION SYNCHONIZED MACHINE MACHINE the speed reaches oversynchronous values. On the dynamic mechanical chacteristic, Fig. 8, the representative point tracks from As to S after a few oscillations. The hodograph of the resultant rotor flux, Fig. 9, tracks the sector As-S in anti-clockwise direction (oversynchronism. 5 5 Ω [rad/s] Fig. 7. Ω =f(t for a SIG with no-load stt-up, torque enforcement of -7 Nm at the moment t =.s, put under excitation at the moment t 2 =.42s, a second torque enforcement of -Nm at the moment t =.8s, and complete unload at the moment t 4 =s. S - S Ω [rad/s] Fig. 8. Ω =f(m e for a SIG with no-load stt-up, torque enforcement of -7 Nm at the moment t =.s, put under excitation at the moment t 2 =.42s, a second torque enforcement of -Nm at the moment t =.8s, and complete unload at the moment t 4 =s. - At the moment t 2 =.42sec, the machine is connected to the DC source (the series-connected and rotor phes e fed with Ue=4V, Ue=-4V, while the phe remains short-circuited, Ue=V. The machine operation turns to synchronous generator duty when the load torque keeps constant to 7 Nm but the speed h the synchronism value. There e some torques that oscillate ound this value and get over the rotor. On the dynamic mechanical chacteristic, the representative point tracks from S to after a few oscillations, Fig. 8. The hodograph of resultant rotor flux tracks the sector S- in anti-clockwise direction and settles down to point, Fig. 9. S4 As A M +2 S4 t=.42s S A M S' As Fig. 9. otor flux for a SIG with no-load stt-up, torque enforcement of -7 Nm at the moment t =.s, put under excitation at the moment t 2 =.42s, a second torque enforcement of -Nm at the moment t =.8s, and complete unload at the moment t 4 =s. - At the moment t =.8sec, the already excited machine gets a sudden additional torque enforcement of -Nm (the total load torque is now of -Nm but lower then pull-out value. The speed tends to advance over synchronous value but after a few oscillations it returns to synchronism. The one effect of this torque enforcement is the alteration of the internal angle. There e also oscillations of the electromagnetic torque. In Fig. 8, the operation point tracks from to S after a few oscillations. The hodograph of the resultant rotor flux tracks the sector -S in anticlockwise direction and settles down to S point, Fig. 9. This rotation of the hodograph proves the alteration of the internal angle due to load modification. - At the moment t 4 =s, the machine is suddenly unloaded, by applying a positive load torque of Nm (the total torque value becomes zero. The machine operates at no-load and the speed tends to deee under synchronous value but after a few oscillations it returns to synchronism. The one notable effect is the deee of the internal angle to a value very close to zero, δ. There e also oscillations of the electromagnetic torque ound its cui-null value, Fig. 8. The representative point tracks from S to S4 point after a few oscillations. The hodograph of the resultant rotor flux tracks the sector S-S4, in clockwise direction and settles down to S4 As point, Fig. 9. This rotation of the hodograph equates the alteration of internal angle due to the load of Nm (from -Nm to Nm. The internal angle, δ, can be so established the angle between the radii AS and AS4, Fig. 9. The internal angle corresponding to the load of -7 Nm can be expressed the angle betwee the radii A and AS4, or for any other load one should plot the angul chacteristic of the induction machine under synchronized induction generator duty. δ S Buletinul AGI nr. 4/22 octomie-decemie 5 295
6 CONFEINŢA NATIONAL NAŢIONALĂ CONFEENCE DE ACŢIONĂI OF ELECTICAL ELECTICE, DIVES ediţia XVI, CNAE SUCEAVA CONCLUSIONS The mathematical model in total fluxes allows an ey analysis of the induction machines but also of synchronous machines for any duty. The mathematical model called in total fluxes is bed on the equations of the electric circuits, which derive from induced voltage law. The recommended form of this law is Ψ& = ν Ψ ( t and h viable j j j + u j quantities the total magnetic fluxes and the electric voltages. The pameters, which chacterize each machine, e present inside the factors ν j. The unity approach for both induction and synchronous machines (with electromagnetic excitation put in view pticul phenomena, which e specific to these machines with double feeding. It is mainly about the oscillations of the mechanical and electromagnetic quantities. The simulations of the AC machines (ynchronous and synchronous one, which e bed on the equations where nothing but total fluxes and rotation angle e present, allow a deep analysis upon the directions of magnetic fluxes and further upon the instantaneous internal angle. The information provided by these simulations can suggest proper strategies concerning the right moments for the connection of the windings to the supply sources. The obtained results prove that any pulling out process determines an electromechanical transient duty with high time constant, which may delay the process with a two times higer duration. BIBLIOGAPHY [] Simion Al., Maşini electrice, vol. II, Maşina sinonă, Editura Gh. Asachi Iaşi,. [2] Simion Al., Maşini electrice, vol. III, Maşina inonă, Editura PIM Iaşi, 22. [] entzsch, G., Handbuch fuer Elektromotoren,. Aufl., Verlag W. Girdet Essen, BBC Mannheim, 98. [4] Boldea, I., N S., The Induction Machine Handbook, CC Press LLC USA, 2. [5] Gier, J.F., Advancements in Electric Machines. Springer Verlag, 8. [6] Boldea, I., Tutelea, L., Electric machines - Steady state, Transients and Design with MATLAB, CC Press,. [7] Simion, Al., Livadu, L. and Munteanu, A., Mathematical Model of the Three-Phe Induction Machine for the Study of Steady-State and Transient Duty under Balanced and Unbalanced States, vol. Induction Motor, cap. XX, Ed. Intech Editor ui Asanjo, 22, (av. About the authors Prof. Eng. Aleandru SIMION, PhD. Gh. Asachi Technical University from Iaşi, Electrical Engineering Faculty, Deptment of Electrical Machines imion@ee.tuii.ro eceived the B.Sc. and Ph.D. degrees in electrical engineering from the Technical University of Iaşi, omania, in 968 and 976, respectively. He h published over 29 papers in conference proceedings and 6 books. His technical interests e electric machines and drives, simulation and design. He is the holder of 5 patents. Assoc. Prof. Eng. Leond LIVADAU, PhD. Gh. Asachi Technical University from Iaşi, Electrical Engineering Faculty, Deptment of Electrical Machines livadu@ee.tuii.ro eceived the B.Sc. and Ph.D. degrees in electrical engineering from the Technical University of Iaşi, omania, in 985 and, respectively. He h published over 5 papers in conference proceedings and 5 books. His technical interests e electric machines, simulation, design and optimization bed on finite element method. Assist. Prof. Eng. Adrian MUNTEANU, PhD. Gh. Asachi Technical University from Iaşi, Electrical Engineering Faculty, Deptment of Electrical Machines imion@ee.tuii.ro eceived the B.Sc. and Ph.D. degrees in electrical engineering from the Technical University of Iaşi, omania, in 4 and 8, respectively. He h published over 2 papers in conference proceedings. His technical interests e electric machines, simulation, design and optimization bed on finite element method
Lesson 17: Synchronous Machines
Lesson 17: Synchronous Machines ET 332b Ac Motors, Generators and Power Systems Lesson 17_et332b.pptx 1 Learning Objectives After this presentation you will be able to: Explain how synchronous machines
More informationJRE SCHOOL OF Engineering
JRE SCHOOL OF Engineering Class Test-1 Examinations September 2014 Subject Name Electromechanical Energy Conversion-II Subject Code EEE -501 Roll No. of Student Max Marks 30 Marks Max Duration 1 hour Date
More informationControl of Wind Turbine Generators. James Cale Guest Lecturer EE 566, Fall Semester 2014 Colorado State University
Control of Wind Turbine Generators James Cale Guest Lecturer EE 566, Fall Semester 2014 Colorado State University Review from Day 1 Review Last time, we started with basic concepts from physics such as
More informationStepping Motors. Chapter 11 L E L F L D
Chapter 11 Stepping Motors In the synchronous motor, the combination of sinusoidally distributed windings and sinusoidally time varying current produces a smoothly rotating magnetic field. We can eliminate
More informationINFLUENCE OF PERMANENT NT MAGNETS DESIGN OVER THE PERFORMANCE OF AXIAL FLUX SYNCHRONOUS MOTORS
Influence of permanent magnets design over the performance of axial flux synchronous motors INFLUENCE OF PERMANENT NT MAGNETS DESIGN OVER THE PERFORMANCE OF AXIAL FLUX SYNCHRONOUS MOTORS Eng. Andreea (ADAM)
More informationMotor Info on the WWW Motorola Motors DC motor» /MOTORDCTUT.
Motor Info on the WWW Motorola Motors DC motor» http://www.freescale.com/files/microcontrollers/doc/train_ref_material /MOTORDCTUT.html Brushless DC motor» http://www.freescale.com/files/microcontrollers/doc/train_ref_material
More informationRevision Guide for Chapter 15
Revision Guide for Chapter 15 Contents tudent s Checklist Revision otes Transformer... 4 Electromagnetic induction... 4 Generator... 5 Electric motor... 6 Magnetic field... 8 Magnetic flux... 9 Force on
More informationGentle synchronization of two-speed synchronous motor with asynchronous starting
Electr Eng (2012) 94:155 163 DOI 10.1007/s00202-011-0227-1 ORIGINAL PAPER Gentle synchronization of two-speed synchronous motor with asynchronous starting Paweł Zalas Jan Zawilak Received: 5 November 2009
More informationElectric Machines I Three Phase Induction Motor. Dr. Firas Obeidat
Electric Machines I Three Phase Induction Motor Dr. Firas Obeidat 1 Table of contents 1 General Principles 2 Construction 3 Production of Rotating Field 4 Why Does the Rotor Rotate 5 The Slip and Rotor
More informationModeling of Symmetrical Squirrel Cage Induction Machine with MatLab Simulink
Modeling of Symmetrical Squirrel Cage Induction Machine with MatLab Simulink Marcus Svoboda *, Lucian Tutelea *, Gheorghe Madescu **, Marius Biriescu *, Martian Mot ** * University POLITEHNICA Timisoara/Electrical
More informationMassachusetts Institute of Technology Department of Electrical Engineering and Computer Science Electric Machines
Massachusetts Institute of Technology Department of Electrical Engineering and Computer Science 6.685 Electric Machines Problem Set 10 Issued November 11, 2013 Due November 20, 2013 Problem 1: Permanent
More informationDynamic Modeling of Surface Mounted Permanent Synchronous Motor for Servo motor application
797 Dynamic Modeling of Surface Mounted Permanent Synchronous Motor for Servo motor application Ritu Tak 1, Sudhir Y Kumar 2, B.S.Rajpurohit 3 1,2 Electrical Engineering, Mody University of Science & Technology,
More informationEFFECTS OF LOAD AND SPEED VARIATIONS IN A MODIFIED CLOSED LOOP V/F INDUCTION MOTOR DRIVE
Nigerian Journal of Technology (NIJOTECH) Vol. 31, No. 3, November, 2012, pp. 365 369. Copyright 2012 Faculty of Engineering, University of Nigeria. ISSN 1115-8443 EFFECTS OF LOAD AND SPEED VARIATIONS
More informationMathematical MATLAB Model and Performance Analysis of Asynchronous Machine
Mathematical MATLAB Model and Performance Analysis of Asynchronous Machine Bikram Dutta 1, Suman Ghosh 2 Assistant Professor, Dept. of EE, Guru Nanak Institute of Technology, Kolkata, West Bengal, India
More informationAutomatic Control Systems. -Lecture Note 15-
-Lecture Note 15- Modeling of Physical Systems 5 1/52 AC Motors AC Motors Classification i) Induction Motor (Asynchronous Motor) ii) Synchronous Motor 2/52 Advantages of AC Motors i) Cost-effective ii)
More informationSpontaneous Speed Reversals in Stepper Motors
Spontaneous Speed Reversals in Stepper Motors Marc Bodson University of Utah Electrical & Computer Engineering 50 S Central Campus Dr Rm 3280 Salt Lake City, UT 84112, U.S.A. Jeffrey S. Sato & Stephen
More informationThe synchronous machine (detailed model)
ELEC0029 - Electric Power System Analysis The synchronous machine (detailed model) Thierry Van Cutsem t.vancutsem@ulg.ac.be www.montefiore.ulg.ac.be/~vct February 2018 1 / 6 Objectives The synchronous
More informationDynamics of the synchronous machine
ELEC0047 - Power system dynamics, control and stability Dynamics of the synchronous machine Thierry Van Cutsem t.vancutsem@ulg.ac.be www.montefiore.ulg.ac.be/~vct October 2018 1 / 38 Time constants and
More informationPERFORMANCE ANALYSIS OF DIRECT TORQUE CONTROL OF 3-PHASE INDUCTION MOTOR
PERFORMANCE ANALYSIS OF DIRECT TORQUE CONTROL OF 3-PHASE INDUCTION MOTOR 1 A.PANDIAN, 2 Dr.R.DHANASEKARAN 1 Associate Professor., Department of Electrical and Electronics Engineering, Angel College of
More informationDEVELOPMENT OF DIRECT TORQUE CONTROL MODELWITH USING SVI FOR THREE PHASE INDUCTION MOTOR
DEVELOPMENT OF DIRECT TORQUE CONTROL MODELWITH USING SVI FOR THREE PHASE INDUCTION MOTOR MUKESH KUMAR ARYA * Electrical Engg. Department, Madhav Institute of Technology & Science, Gwalior, Gwalior, 474005,
More information51. IWK Internationales Wissenschaftliches Kolloquium International Scientific Colloquium
51. IWK Internationales Wissenschaftliches Kolloquium International Scientific Colloquium PROCEEDINGS 11-15 September 2006 FACULTY OF ELECTRICAL ENGINEERING AND INFORMATION SCIENCE INFORMATION TECHNOLOGY
More informationIndependent Control of Speed and Torque in a Vector Controlled Induction Motor Drive using Predictive Current Controller and SVPWM
Independent Control of Speed and Torque in a Vector Controlled Induction Motor Drive using Predictive Current Controller and SVPWM Vandana Peethambaran 1, Dr.R.Sankaran 2 Assistant Professor, Dept. of
More informationEqual Pitch and Unequal Pitch:
Equal Pitch and Unequal Pitch: Equal-Pitch Multiple-Stack Stepper: For each rotor stack, there is a toothed stator segment around it, whose pitch angle is identical to that of the rotor (θs = θr). A stator
More informationEE 410/510: Electromechanical Systems Chapter 4
EE 410/510: Electromechanical Systems Chapter 4 Chapter 4. Direct Current Electric Machines and Motion Devices Permanent Magnet DC Electric Machines Radial Topology Simulation and Experimental Studies
More informationA Direct Torque Controlled Induction Motor with Variable Hysteresis Band
UKSim 2009: th International Conference on Computer Modelling and Simulation A Direct Torque Controlled Induction Motor with Variable Hysteresis Band Kanungo Barada Mohanty Electrical Engineering Department,
More informationChapter 5 Three phase induction machine (1) Shengnan Li
Chapter 5 Three phase induction machine (1) Shengnan Li Main content Structure of three phase induction motor Operating principle of three phase induction motor Rotating magnetic field Graphical representation
More informationDESIGN AND MODELLING OF SENSORLESS VECTOR CONTROLLED INDUCTION MOTOR USING MODEL REFERENCE ADAPTIVE SYSTEMS
DESIGN AND MODELLING OF SENSORLESS VECTOR CONTROLLED INDUCTION MOTOR USING MODEL REFERENCE ADAPTIVE SYSTEMS Janaki Pakalapati 1 Assistant Professor, Dept. of EEE, Avanthi Institute of Engineering and Technology,
More informationInternational Journal of Advance Engineering and Research Development SIMULATION OF FIELD ORIENTED CONTROL OF PERMANENT MAGNET SYNCHRONOUS MOTOR
Scientific Journal of Impact Factor(SJIF): 3.134 e-issn(o): 2348-4470 p-issn(p): 2348-6406 International Journal of Advance Engineering and Research Development Volume 2,Issue 4, April -2015 SIMULATION
More informationELECTRIC MACHINE TORQUE PRODUCTION 101
ELECTRIC MACHINE TORQUE PRODUCTION 101 Best Electric Machine, 014 INTRODUCTION: The following discussion will show that the symmetrical (or true dual-ported) transformer electric machine as only provided
More informationECEN 667 Power System Stability Lecture 18: Voltage Stability, Load Models
ECEN 667 Power System Stability Lecture 18: Voltage Stability, Load Models Prof. Tom Overbye Dept. of Electrical and Computer Engineering Texas A&M University, overbye@tamu.edu 1 Announcements Read Chapter
More informationModel of a DC Generator Driving a DC Motor (which propels a car)
Model of a DC Generator Driving a DC Motor (which propels a car) John Hung 5 July 2011 The dc is connected to the dc as illustrated in Fig. 1. Both machines are of permanent magnet type, so their respective
More informationGenerators for wind power conversion
Generators for wind power conversion B. G. Fernandes Department of Electrical Engineering Indian Institute of Technology, Bombay Email : bgf@ee.iitb.ac.in Outline of The Talk Introduction Constant speed
More informationMATLAB SIMULINK Based DQ Modeling and Dynamic Characteristics of Three Phase Self Excited Induction Generator
628 Progress In Electromagnetics Research Symposium 2006, Cambridge, USA, March 26-29 MATLAB SIMULINK Based DQ Modeling and Dynamic Characteristics of Three Phase Self Excited Induction Generator A. Kishore,
More informationECE 325 Electric Energy System Components 7- Synchronous Machines. Instructor: Kai Sun Fall 2015
ECE 325 Electric Energy System Components 7- Synchronous Machines Instructor: Kai Sun Fall 2015 1 Content (Materials are from Chapters 16-17) Synchronous Generators Synchronous Motors 2 Synchronous Generators
More information3 d Calculate the product of the motor constant and the pole flux KΦ in this operating point. 2 e Calculate the torque.
Exam Electrical Machines and Drives (ET4117) 11 November 011 from 14.00 to 17.00. This exam consists of 5 problems on 4 pages. Page 5 can be used to answer problem 4 question b. The number before a question
More informationFEEDBACK CONTROL SYSTEMS
FEEDBAC CONTROL SYSTEMS. Control System Design. Open and Closed-Loop Control Systems 3. Why Closed-Loop Control? 4. Case Study --- Speed Control of a DC Motor 5. Steady-State Errors in Unity Feedback Control
More informationThree phase induction motor using direct torque control by Matlab Simulink
Three phase induction motor using direct torque control by Matlab Simulink Arun Kumar Yadav 1, Dr. Vinod Kumar Singh 2 1 Reaserch Scholor SVU Gajraula Amroha, U.P. 2 Assistant professor ABSTRACT Induction
More informationMathematical Modeling and Dynamic Simulation of a Class of Drive Systems with Permanent Magnet Synchronous Motors
Applied and Computational Mechanics 3 (2009) 331 338 Mathematical Modeling and Dynamic Simulation of a Class of Drive Systems with Permanent Magnet Synchronous Motors M. Mikhov a, a Faculty of Automatics,
More informationIntroduction to Synchronous. Machines. Kevin Gaughan
Introduction to Synchronous Machines Kevin Gaughan The Synchronous Machine An AC machine (generator or motor) with a stator winding (usually 3 phase) generating a rotating magnetic field and a rotor carrying
More informationComparative Study of Synchronous Machine, Model 1.0 and Model 1.1 in Transient Stability Studies with and without PSS
Comparative Study of Synchronous Machine, Model 1.0 and Model 1.1 in Transient Stability Studies with and without PSS Abhijit N Morab, Abhishek P Jinde, Jayakrishna Narra, Omkar Kokane Guide: Kiran R Patil
More informationTexas A & M University Department of Mechanical Engineering MEEN 364 Dynamic Systems and Controls Dr. Alexander G. Parlos
Texas A & M University Department of Mechanical Engineering MEEN 364 Dynamic Systems and Controls Dr. Alexander G. Parlos Lecture 6: Modeling of Electromechanical Systems Principles of Motor Operation
More informationBehaviour of synchronous machine during a short-circuit (a simple example of electromagnetic transients)
ELEC0047 - Power system dynamics, control and stability (a simple example of electromagnetic transients) Thierry Van Cutsem t.vancutsem@ulg.ac.be www.montefiore.ulg.ac.be/~vct October 2018 1 / 25 Objectives
More information7. Transient stability
1 7. Transient stability In AC power system, each generator is to keep phase relationship according to the relevant power flow, i.e. for a certain reactance X, the both terminal voltages V1and V2, and
More informationNEURAL NETWORKS APPLICATION FOR MECHANICAL PARAMETERS IDENTIFICATION OF ASYNCHRONOUS MOTOR
NEURAL NETWORKS APPLICATION FOR MECHANICAL PARAMETERS IDENTIFICATION OF ASYNCHRONOUS MOTOR D. Balara, J. Timko, J. Žilková, M. Lešo Abstract: A method for identification of mechanical parameters of an
More informationINDUCTION MOTOR MODEL AND PARAMETERS
APPENDIX C INDUCTION MOTOR MODEL AND PARAMETERS C.1 Dynamic Model of the Induction Motor in Stationary Reference Frame A three phase induction machine can be represented by an equivalent two phase machine
More informationLecture 9: Space-Vector Models
1 / 30 Lecture 9: Space-Vector Models ELEC-E8405 Electric Drives (5 ECTS) Marko Hinkkanen Autumn 2017 2 / 30 Learning Outcomes After this lecture and exercises you will be able to: Include the number of
More informationElectrical Machines and Energy Systems: Operating Principles (Part 2) SYED A Rizvi
Electrical Machines and Energy Systems: Operating Principles (Part 2) SYED A Rizvi AC Machines Operating Principles: Synchronous Motor In synchronous motors, the stator of the motor has a rotating magnetic
More informationECE 5670/6670 Lab 8. Torque Curves of Induction Motors. Objectives
ECE 5670/6670 Lab 8 Torque Curves of Induction Motors Objectives The objective of the lab is to measure the torque curves of induction motors. Acceleration experiments are used to reconstruct approximately
More informationRobust Controller Design for Speed Control of an Indirect Field Oriented Induction Machine Drive
Leonardo Electronic Journal of Practices and Technologies ISSN 1583-1078 Issue 6, January-June 2005 p. 1-16 Robust Controller Design for Speed Control of an Indirect Field Oriented Induction Machine Drive
More informationLecture 1: Induction Motor
1 / 22 Lecture 1: Induction Motor ELEC-E8402 Control of Electric Drives and Power Converters (5 ECTS) Marko Hinkkanen Aalto University School of Electrical Engineering Spring 2016 2 / 22 Learning Outcomes
More informationRevision Guide for Chapter 15
Revision Guide for Chapter 15 Contents Revision Checklist Revision otes Transformer...4 Electromagnetic induction...4 Lenz's law...5 Generator...6 Electric motor...7 Magnetic field...9 Magnetic flux...
More informationAn Introduction to Electrical Machines. P. Di Barba, University of Pavia, Italy
An Introduction to Electrical Machines P. Di Barba, University of Pavia, Italy Academic year 0-0 Contents Transformer. An overview of the device. Principle of operation of a single-phase transformer 3.
More informationMechatronics Engineering. Li Wen
Mechatronics Engineering Li Wen Bio-inspired robot-dc motor drive Unstable system Mirko Kovac,EPFL Modeling and simulation of the control system Problems 1. Why we establish mathematical model of the control
More informationElectrical Machines and Energy Systems: Operating Principles (Part 1) SYED A Rizvi
Electrical Machines and Energy Systems: Operating Principles (Part 1) SYED A Rizvi AC Machines Operating Principles: Rotating Magnetic Field The key to the functioning of AC machines is the rotating magnetic
More informationModule 3 : Sequence Components and Fault Analysis
Module 3 : Sequence Components and Fault Analysis Lecture 12 : Sequence Modeling of Power Apparatus Objectives In this lecture we will discuss Per unit calculation and its advantages. Modeling aspects
More informationSensorless DTC-SVM of Induction Motor by Applying Two Neural Controllers
Sensorless DTC-SVM of Induction Motor by Applying Two Neural Controllers Abdallah Farahat Mahmoud Dept. of Electrical Engineering, Al-Azhar University, Qena, Egypt engabdallah2012@azhar.edu.eg Adel S.
More informationSensorless Control for High-Speed BLDC Motors With Low Inductance and Nonideal Back EMF
Sensorless Control for High-Speed BLDC Motors With Low Inductance and Nonideal Back EMF P.Suganya Assistant Professor, Department of EEE, Bharathiyar Institute of Engineering for Women Salem (DT). Abstract
More informationPRINCIPLE OF DESIGN OF FOUR PHASE LOW POWER SWITCHED RELUCTANCE MACHINE AIMED TO THE MAXIMUM TORQUE PRODUCTION
Journal of ELECTRICAL ENGINEERING, VOL. 55, NO. 5-6, 24, 138 143 PRINCIPLE OF DESIGN OF FOUR PHASE LOW POWER SWITCHED RELUCTANCE MACHINE AIMED TO THE MAXIMUM TORQUE PRODUCTION Martin Lipták This paper
More informationGeneralized Theory of Electrical Machines- A Review
Generalized Theory of Electrical Machines- A Review Dr. Sandip Mehta Department of Electrical and Electronics Engineering, JIET Group of Institutions, Jodhpur Abstract:-This paper provides an overview
More informationMathematical Modeling and Dynamic Simulation of DC Motors using MATLAB/Simulink Environment
Mathematical Modeling and Dynamic Simulation of DC Motors using MATLAB/Simulink Environment K. Kalaiselvi 1, K.Abinaya 2, P. Ramesh Babu 3 1,2 Under Graduate Scholar, Department of EEE, Saranathan College
More informationEEE3405 ELECTRICAL ENGINEERING PRINCIPLES 2 - TEST
ATTEMPT ALL QUESTIONS (EACH QUESTION 20 Marks, FULL MAKS = 60) Given v 1 = 100 sin(100πt+π/6) (i) Find the MS, period and the frequency of v 1 (ii) If v 2 =75sin(100πt-π/10) find V 1, V 2, 2V 1 -V 2 (phasor)
More informationQUESTION BANK ENGINEERS ACADEMY. Power Systems Power System Stability 1
ower ystems ower ystem tability QUETION BANK. A cylindrical rotor generator delivers 0.5 pu power in the steady-state to an infinite bus through a transmission line of reactance 0.5 pu. The generator no-load
More informationPerformance Evaluation of DFIG to Changes in Network Frequency
019 CIENCELINE Journal of World s Electrical Engineering and Technology J. World. Elect. Eng. Tech. 8(1): 01-06, 019 JWEET Performance Evaluation of DFIG to Changes in Network Frequency Ramin Tayebi-Derazkolaie
More informationA new FOC technique based on predictive current control for PMSM drive
ISSN 1 746-7, England, UK World Journal of Modelling and Simulation Vol. 5 (009) No. 4, pp. 87-94 A new FOC technique based on predictive current control for PMSM drive F. Heydari, A. Sheikholeslami, K.
More informationOverview of motors and motion control
Overview of motors and motion control. Elements of a motion-control system Power upply High-level controller ow-level controller Driver Motor. Types of motors discussed here; Brushed, PM DC Motors Cheap,
More informationAC Induction Motor Stator Resistance Estimation Algorithm
7th WSEAS International Conference on Electric Power Systems, High Voltages, Electric Machines, Venice, Italy, November 21-23, 27 86 AC Induction Motor Stator Resistance Estimation Algorithm PETR BLAHA
More informationDefinition Application of electrical machines Electromagnetism: review Analogies between electric and magnetic circuits Faraday s Law Electromagnetic
Definition Application of electrical machines Electromagnetism: review Analogies between electric and magnetic circuits Faraday s Law Electromagnetic Force Motor action Generator action Types and parts
More informationMathematical Modelling of Permanent Magnet Synchronous Motor with Rotor Frame of Reference
Mathematical Modelling of Permanent Magnet Synchronous Motor with Rotor Frame of Reference Mukesh C Chauhan 1, Hitesh R Khunt 2 1 P.G Student (Electrical),2 Electrical Department, AITS, rajkot 1 mcchauhan1@aits.edu.in
More informationNonlinear dynamic simulation model of switched reluctance linear machine
Procedia Earth and Planetary Science 1 (2009) 1320 1324 Procedia Earth and Planetary Science www.elsevier.com/locate/procedia The 6 th International Conference on Mining Science & Technology Nonlinear
More informationLAB REPORT: THREE-PHASE INDUCTION MACHINE
LAB REPORT: THREE-PHASE INDUCTION MACHINE ANDY BENNETT 1. Summary This report details the operation, modelling and characteristics of a three-phase induction machine. It attempts to provide a concise overview
More informationChapter 4. Synchronous Generators. Basic Topology
Basic Topology Chapter 4 ynchronous Generators In stator, a three-phase winding similar to the one described in chapter 4. ince the main voltage is induced in this winding, it is also called armature winding.
More informationSECTION - I. PULL-IN-OPERATION Op SYNCHRONOUS MOTORS
SECTION - I PULL-IN-OPERATION Op SYNCHRONOUS MOTORS 14 S 1.1 INTRODUCTION The starting of synchronous, reluctance and permanent magnet synchronous motors is normally carried out by damper winding. The
More informationCHAPTER 5 SIMULATION AND TEST SETUP FOR FAULT ANALYSIS
47 CHAPTER 5 SIMULATION AND TEST SETUP FOR FAULT ANALYSIS 5.1 INTRODUCTION This chapter describes the simulation model and experimental set up used for the fault analysis. For the simulation set up, the
More informationElectromagnetic fields calculation at single phase shaded pole motor
Electromagnetic fields calculation at single phase shaded pole motor Vasilija J. Šarac, Dobri M. Čundev Finite Element Method (FEM) is used for calculation of electromagnetic field inside the single phase
More informationStep Motor Modeling. Step Motor Modeling K. Craig 1
Step Motor Modeling Step Motor Modeling K. Craig 1 Stepper Motor Models Under steady operation at low speeds, we usually do not need to differentiate between VR motors and PM motors (a hybrid motor is
More informationTime-Harmonic Modeling of Squirrel-Cage Induction Motors: A Circuit-Field Coupled Approach
Time-Harmonic Modeling of Squirrel-Cage Induction Motors: A Circuit-Field Coupled Approach R. Escarela-Perez 1,3 E. Melgoza 2 E. Campero-Littlewood 1 1 División de Ciencias Básicas e Ingeniería, Universidad
More informationSynchronous Machines
Synchronous Machines Synchronous Machines n 1 Φ f n 1 Φ f I f I f I f damper (run-up) winding Stator: similar to induction (asynchronous) machine ( 3 phase windings that forms a rotational circular magnetic
More informationUNIT I INTRODUCTION Part A- Two marks questions
ROEVER COLLEGE OF ENGINEERING & TECHNOLOGY ELAMBALUR, PERAMBALUR-621220 DEPARTMENT OF ELECTRICAL AND ELECTRONICS ENGINEERING DESIGN OF ELECTRICAL MACHINES UNIT I INTRODUCTION 1. Define specific magnetic
More informationEquivalent Circuits with Multiple Damper Windings (e.g. Round rotor Machines)
Equivalent Circuits with Multiple Damper Windings (e.g. Round rotor Machines) d axis: L fd L F - M R fd F L 1d L D - M R 1d D R fd R F e fd e F R 1d R D Subscript Notations: ( ) fd ~ field winding quantities
More informationDESIGN OF ROBUST CONTROL SYSTEM FOR THE PMS MOTOR
Journal of ELECTRICAL ENGINEERING, VOL 58, NO 6, 2007, 326 333 DESIGN OF ROBUST CONTROL SYSTEM FOR THE PMS MOTOR Ahmed Azaiz Youcef Ramdani Abdelkader Meroufel The field orientation control (FOC) consists
More informationSteady State Modeling of Doubly Fed Induction Generator
Steady State Modeling of Douly Fed Induction Generator Bhola Jha 1, Dr. K. R. M Rao 2 1 Dept. of Electrical Engg., G. B. Pant Engg. College, Pauri-Garhwal, India 2 Dept. of Electrical Engg., M. J. College
More informationMathematical Modelling of an 3 Phase Induction Motor Using MATLAB/Simulink
2016 IJSRSET Volume 2 Issue 3 Print ISSN : 2395-1990 Online ISSN : 2394-4099 Themed Section: Engineering and Technology Mathematical Modelling of an 3 Phase Induction Motor Using MATLAB/Simulink ABSTRACT
More informationUnderstanding the Inductances
Understanding the Inductances We have identified six different inductances (or reactances) for characterizing machine dynamics. These are: d, q (synchronous), ' d, ' q (transient), '' d,'' q (subtransient)
More informationSynchronous Machines
Synchronous Machines Synchronous generators or alternators are used to convert mechanical power derived from steam, gas, or hydraulic-turbine to ac electric power Synchronous generators are the primary
More informationBasic parts of an AC motor : rotor, stator, The stator and the rotor are electrical
INDUCTION MOTO 1 CONSTUCTION Baic part of an AC motor : rotor, tator, encloure The tator and the rotor are electrical circuit that perform a electromagnet. CONSTUCTION (tator) The tator - tationary part
More informationComparative Analysis of Speed Control of Induction Motor by DTC over Scalar Control Technique
Comparative Analysis of Speed Control of Induction Motor by DTC over Scalar Control Technique S.Anuradha 1, N.Amarnadh Reddy 2 M.Tech (PE), Dept. of EEE, VNRVJIET, T.S, India 1 Assistant Professor, Dept.
More informationMODELING AND HIGH-PERFORMANCE CONTROL OF ELECTRIC MACHINES
MODELING AND HIGH-PERFORMANCE CONTROL OF ELECTRIC MACHINES JOHN CHIASSON IEEE PRESS ü t SERIES ON POWER ENGINEERING IEEE Press Series on Power Engineering Mohamed E. El-Hawary, Series Editor The Institute
More informationDesign of PSS and SVC Controller Using PSO Algorithm to Enhancing Power System Stability
IOSR Journal of Electrical and Electronics Engineering (IOSR-JEEE) e-issn: 2278-1676,p-ISSN: 2320-3331, Volume 10, Issue 2 Ver. II (Mar Apr. 2015), PP 01-09 www.iosrjournals.org Design of PSS and SVC Controller
More information(Refer Slide Time: 00:01:30 min)
Control Engineering Prof. M. Gopal Department of Electrical Engineering Indian Institute of Technology, Delhi Lecture - 3 Introduction to Control Problem (Contd.) Well friends, I have been giving you various
More informationDETERMINING STATIC TORQUE CHARACTERISTICS OF PERMANENT MAGNET STEP MOTOR
DETERMINING STATIC TORQUE CHARACTERISTICS OF PERMANENT MAGNET STEP MOTOR Miroslav BJEKIĆ Abstract: The paper analyzes three methods of calculating static torque of permanent magnet step motor. Analytical
More informationSCHOOL OF ELECTRICAL, MECHANICAL AND MECHATRONIC SYSTEMS. Transient Stability LECTURE NOTES SPRING SEMESTER, 2008
SCHOOL OF ELECTRICAL, MECHANICAL AND MECHATRONIC SYSTEMS LECTURE NOTES Transient Stability SPRING SEMESTER, 008 October 7, 008 Transient Stability Transient stability refers to the ability of a synchronous
More informationA High Performance DTC Strategy for Torque Ripple Minimization Using duty ratio control for SRM Drive
A High Performance DTC Strategy for Torque Ripple Minimization Using duty ratio control for SRM Drive Veena P & Jeyabharath R 1, Rajaram M 2, S.N.Sivanandam 3 K.S.Rangasamy College of Technology, Tiruchengode-637
More informationENGG4420 LECTURE 7. CHAPTER 1 BY RADU MURESAN Page 1. September :29 PM
CHAPTER 1 BY RADU MURESAN Page 1 ENGG4420 LECTURE 7 September 21 10 2:29 PM MODELS OF ELECTRIC CIRCUITS Electric circuits contain sources of electric voltage and current and other electronic elements such
More informationRobust sliding mode speed controller for hybrid SVPWM based direct torque control of induction motor
ISSN 1 746-7233, England, UK World Journal of Modelling and Simulation Vol. 3 (2007) No. 3, pp. 180-188 Robust sliding mode speed controller for hybrid SVPWM based direct torque control of induction motor
More informationThe basic principle to be used in mechanical systems to derive a mathematical model is Newton s law,
Chapter. DYNAMIC MODELING Understanding the nature of the process to be controlled is a central issue for a control engineer. Thus the engineer must construct a model of the process with whatever information
More informationPOWER SYSTEM STABILITY
LESSON SUMMARY-1:- POWER SYSTEM STABILITY 1. Introduction 2. Classification of Power System Stability 3. Dynamic Equation of Synchronous Machine Power system stability involves the study of the dynamics
More informationPrince Sattam bin Abdulaziz University College of Engineering. Electrical Engineering Department EE 3360 Electrical Machines (II)
Chapter # 4 Three-Phase Induction Machines 1- Introduction (General Principles) Generally, conversion of electrical power into mechanical power takes place in the rotating part of an electric motor. In
More informationLecture 4: Losses and Heat Transfer
1 / 26 Lecture 4: Losses and Heat Transfer ELEC-E845 Electric Drives (5 ECTS) Marko Hinkkanen Aalto University School of Electrical Engineering Autumn 215 2 / 26 Learning Outcomes After this lecture and
More informationELECTROMAGNETIC INDUCTION
ELECTROMAGNETIC INDUCTION 1. Magnetic Flux 2. Faraday s Experiments 3. Faraday s Laws of Electromagnetic Induction 4. Lenz s Law and Law of Conservation of Energy 5. Expression for Induced emf based on
More information