INFLUENCE OF DESIGN DATA OF INDUCTION MOTOR ON EFFECTS OF CAGE ASYMMETRY

Size: px
Start display at page:

Download "INFLUENCE OF DESIGN DATA OF INDUCTION MOTOR ON EFFECTS OF CAGE ASYMMETRY"

Transcription

1 Pace Nauowe Intytutu Mazyn, Naędów i Pomiaów Eletycznych N 66 Politechnii Wocławiej N 66 Studia i Mateiały N 3 1 Alejando FERNANDEZ GOMEZ* Tadeuz J. SOBCZYK* induction moto, oto cage aymmety, cage moto diagnotic INFLUENCE OF DESIGN DATA OF INDUCTION MOTOR ON EFFECTS OF CAGE ASYMMETRY The ae eent eult of analyi of influence of choen aamete of induction cage moto on the comonent (1 )f in tato cuent, which i commonly ued fo diagnoi of cage condition. The invetigation concentate on the influence of commonly available moto data uch a oleai and oto lot numbe, eectively, but alo on elationhi between eitance of cage ba and end ing. A educed model of moto with a faulty cage i ued, in which cage fault ae eeented by aymmety coefficient of a cage. The main intention of the ae i to ovide enginee with imle etimate of effect due to cage fault fo vaiou moto given limited infomation. 1. INTRODUCTION Nowaday diagnoi of induction moto cage fault bae on the Moto Cuent Signatue Analyi (MCSA). Many ae [1] [7] ae devoted to that oblem. Pediction of effect in tato cuent due to cage fault i ovided engaging cicuital o field model of Induction Moto (IM) that ae moe o le comlicated. They equied detailed infomation on deign data of a moto, which uually ae not available fo enginee in the induty. Theefoe, it i equeted to etimate effect of cage fault uing only baic data of a moto. Thi ae i an attemt to anwe to that oblem given limiting neceay infomation to the ole-ai numbe and the oto lot numbe N. Commonly, the comonent with the fequency (1 )f in tato hae cuent i ecognized a a baic fundamental effect of cage fault. The effect can be edicted by a baic model of induction moto accounting fo the cage aymmety. One uch model wa eented in [8]. It oeate with ymmetical comonent of tato and oto quantitie, and it i a imle extenion of the claical IM model. The cage * Intitute on Electomechanical Enegy Conveion, Cacow Univeity of Technology, ul. Wazawa 4, Kaów, Poland.

2 358 aymmety i eeented in the model by the aymmety facto a and. In the cae of a healthy cage thoe facto ae equal to zeo.. ESTIMATION OF EFFECTS IN CURRENTS DUE TO CAGE FAULTS Vaiou tudie [9], [11] eented a dynamic model of IM conideing the main MFF hamonic only and a cage aymmety. When uly voltage ae balanced and teady-tate ae conideed that equation ae educed to fou algebaic equation of the fom U 1 = X σ + X μ j X μ X σ + X μ X μ X μ X' σ + X μ X μ X' σ + X μ + R + R 1 ( 1+ ) a e jα jα ae ( 1+ 1 I I I' N I' ) (1) jω t whee I denote a value of the fit ymmetical comonent i ( t) = I e of the uly fequency Ω and I j(1 ) Ω t a value of the econd comonent i ( t) = I e with the li deendent fequency ( 1 ) Ω. Thoe equation could be eeented by the equivalent cheme eented in Fig I 1 U R jxσ, jxμ jx' σ, (1+ a) a jx' σ, jxμ jx σ, R 1 I' Fig. 1. Equivalent cheme of induction moto with faulty cage Fom that equivalent cheme a elationhi between the main cuent comonent 1 I and the comonent I, geneated by a cage fault, can be found. In [11] it ha been

3 359 hown that at nomal oeating condition of a moto, i.e. fo mall li, the magnetizing eactance X μ and the leaage eactance X σ,, X' σ, can be omitted, eectively, and neglecting the eitance R, the atio between I and I 1 can be exe by the cage aymmety facto a I' 1 = 1 a () I = In Figue the value of the atio facto 1 ae hown veu li at diffeent aumtion fo equivalent cheme aamete. The cuve a i obtained fom a full cheme, the cuve b wa develoed when omitting the magnetizing eactance X μ. The cuve c i obtained when leaage eactance ae omitted a well, i.e. fo a uely eitive cheme. The dahed line (cuve d ) how the value a. Thoe cuve wee calculated fo a moto with the following ated data: P n = W, n n = 98 m, U = 6 V, I n = 7 A, = 1, N = 36. Fig.. The atio 1 veu li at diffeent imlification of the equivalent cheme in Fig. 1 [11] It i evident that the atio 1 i vey cloe to aymmety facto a fo nea ated li. 3. ESTIMATION OF ASYMMETRY FACTOR BY POLE-PAIR AND ROTOR SLOT NUMBERS To detemine the aymmety facto a, the eitance of each cage element hould be nown [8] [11], i.e. eitance of cage ba R b and end-ing egment R e.

4 36 Uually, cage fault ae modelled by inceaing the eitance of a faulty element u to time the nominal value. The aymmety facto a detemine a eitive couling between equivalent cheme fo the fit and the econd ymmetical comonent, which ae connected bac-to-bac (ee Fig. 1) in comaion to the value of the oto eitance in the equivalent cheme fo the ymmetical cae π = ( ν) Re + Rb in (3) N whee i a ole-ai numbe and N i a numbe of ba in a cage. The eitance R b and egment R e can be elated uing deign data of a moto. Knowing the elationhi between cuent in ba and end ing egment I = I in( α ), whee α = ( π ) N, and etimating the elationhi between the ba length L and the diamete of end ing D a L = ( λ π D) a well a uing the machine atio λ = L τ, whee τ i the ole itch, the elationhi between the eitance R b and R e i done by the fomula 4π Re = λ N π in N π N je γb j γ b e b 1 whee: j b, j e ae cuent denitie in ba and end-ing egment, γ b, γ e ae eective conductivitie and in i a facto fo detemining in effect in a ba. Baed on thi elation the aymmety facto a can be etimated by uing a oleai numbe and a numbe of cage lot only and, a a conequence, the atio 1. The value of the facto a deend on the fault tye. Thi ae how that it i an eential cae when one ba i boen becaue effect of multi-ba fault can be etimated by that elementay fault. in R b e (4) 4. INFUENCE OF END-RING SEGMENT RESISTANCE ON ASYMMETRY FACTOR Fom () it follow that elationhi between eitance R b and R e deend on the conductivity of a mateial ued fo cage and cuent denitie aumed fo ba and ending. Uually, mateial ued fo end-ing and ba ae the ame, o the atio γ b /γ e i equal to one. Fo mall li the in effect can be neglected a well. So, an influence of end-ing geomety on the aymmety facto can be tudied by changing the atio j e /j b. Reult of calculation of the aymmety facto a fo one boen ba ae efomed given the following aumtion: λ = 1.5, in = 1. and γ b /γ e = 1. ee Fig..

5 361 Thee ae fou gah in thi figue, when the quotient j e /j b i changing. The gah a how the facto a veu the value fo diffeent ole-ai numbe (fom = 1 till = 5) fo j e /j b = 1.. The cuve b how the ame data fo j e /j b =. and gah c fo the atio j e /j b =.5. In the gah d the eitance of end-ing egment i aumed to be zeo (R e = ). Such aumtion i ometime ued when analyzing the cage aymmety. It can be een that fo eal value of the quotient j e /j b the aymmety facto a, and alo the atio 1, deend on the numbe of lot in a cage but alo on the ole-ai numbe. It can be tated that end-ing can be omitted fo highe lot numbe and then 1..7 Gah a.7 Gah b.6.5 a.4 j e / j b =1 j e / j b =.6.5 a Gah c Gah d.6.6 j e / j b =,5 R e =.5 a.4.5 a Fig. 3. Influence of end-ing egment eitance on the aymmety facto fo diffeent ole-ai numbe

6 36 5. ESTIMATION OF RATIO K 1 FOR MULTI-BAR FAULTS In the cae of multi-ba fault the atio 1 can be etimated by the aymmety facto fo one boen ba. In liteatue the elationhi 1 n/n i often ued, whee n i a numbe of boen ba. Howeve, thi elationhi i not valid even fo imle multiba fault. A fa moe exact etimation of the atio 1 fo multi-ba fault can be obtained by umming geometically the comonent (1 )f geneated by individual boen ba a it i exlained in Fig. 4 fo the cae of two ucceive boen ba. 1- γ 1 Fig. 4. Etimation of effect due to two adjacent boen ba It follow that fo n equent boen ba the atio 1 can be etimated by the following fomula γ in n = = (5) γ n in 1 a 1,a whee 1,a i the aymmety facto fo one boen ba and γ = α = (π ) /N. That etimation i much moe meaningful than 1 n / N. The change of atio 1 = a fo neighbou boen ba veu at diffeent ole-ai numbe ae hown in Fig. 5: gah a fo two ba and gah b fo thee ba. All cuve have been obtained fo λ = 1.5, in = 1., γ b/γ e =1. and j e /j b = Gah a.18 Gah b a.5.1 a Fig. 5. Aymmety facto at and 3 neighbou ba boen fo diffeent ole-ai numbe

7 363 Thoe figue illutate difficultie in diagnotic of multi-ba fault. The geometical um of (1 )f comonent geneated at individual boen ba can tae an abitay value and can even diaea at mall numbe of cage lot and bigge oleai numbe..5.4 Evolution of a =1 = =3.3 a Pai of ole Fig. 6. Aymmety facto fo veu oition of a ai of boen ba That effect can be obeved alo in Fig. 6, in which change of the aymmety facto ae hown fo two ba ae boen located at vaiou oition. In that figue the oition of a boen ba ai ae denoted a: 1, 1 3, 1 4 etc. The calculation wee efomed fo a moto with N = 36 ba fo ole-ai numbe = 1, = and = 3, and given λ = 1.5, in = 1., γ b γ e = 1. and j e /j b = 1.. Alo, it hould be noted that fo each ole-ai numbe thee ae ai fo which aymmety facto i cloe to zeo, meaning that the effect of cage aymmety i not obeved in tato cuent. Theefoe, it i athe evident that the atio 1 i not uniquely elated to a multi-ba fault tye. The final concluion of the eented analyi i that the diagnotic of cage fault baed on (1 )f comonent in tato cuent could be unatifactoy. In actice, diagnotic ytem hould attemt to identify the onet of cage damage becaue when multi-ba fault aie the analyi could be unatifactoy. 6. CONCLUSIONS In the ae a imle analyi of effect in tato cuent due to cage fault i eented. It ha been hown how to etimate effect of multi-ba cage fault baed on the effect of one boen ba. The lit of aamete equied fo that etimation ha been

8 364 limited to the numbe of ole-ai and the cage lot numbe. The influence of ending deign data on effect due to cage damage ha been alo dicued. Etimation eented in the ae can be ueful fo enginee fo cage diagnotic. Thi ae ha been eaed a a at of eeach oject Enegy SmatO in a fame of 7FP-ITN-PEOPLE-11. REFERENCES [1] BELLINI A., FILIPPETTI F., FRANCESCHINI F., SOBCZYK T.J., TASSONI C., Diagnoi of induction machine by d-q and i..c oto model, Poc. 5th IEEE Sym. on Diagnotic of Electic Machine, Powe Electonic and Dive, (SDEMPED 5), [] DIDIER G., TERNISIEN E., CASPAREY O., RAZIK H., Fault detection of boen oto ba in induction moto uing a global fault index, IEEE Tan. Induty Alication, 6, Vol. 4, [3] FILIPPETTI F., FRANCESCHINI G., TASSONI C., VAS P., AI technique in induction machine diagnoi including the eed ile effect, IEEE Tan. Induty Alication, 1998, Vol. 34, [4] JUNG J.H., LEE J.J., KWON B.H., Online Diagnoi of Induction Moto Uing MCSA, Tan. Indutial Electonic, 6, Vol. 53, No. 6, [5] KLIMAN G.B., STEIN J., ENDICOTT R.D., KOEGL R.A., Non-invaive Detection of Boen Roto Ba in Oeating Induction Moto, IEEE Tan. Enegy Conveion., 1998, Vol. 3, [6] KRAL C., KAPELLER H., GRAGGER J.V., HAUMER A., KUBICEK B., Phenomenon Roto Fault Multile Electical Roto Aymmetie in Induction Machine, Poc. 7th IEEE Sym. on Diagnotic of Electic Machine, Powe Electonic and Dive, (SDEMPED 9), IEEE Catalog Numbe CFP9DE-CDR, TF63. [7] MIRAFZAL B., DEMERDASH N., On innovative method of induction moto intetem and boenba fault diagnoi, IEEE Tan. Induty Alication, 6, Vol. 4, [8] SOBCZYK T.J., MACIOŁEK W., Aymmety facto of induction moto oto cage, Poc. 3d IEEE Sym. on Diagnotic of Electic Machine, Powe Electonic and Dive, (SDEMPED 1), [9] SOBCZYK T.J., MACIOŁEK W., Doe the comonent (1-)f o in tato cuent i ufficient fo detection of oto cage fault?, Poc. 5th IEEE Sym. on Diagnotic of Electic Machine, Powe Electonic and Dive, (SDEMPED 5), [1] SOBCZYK T.J., MACIOŁEK W., On Reduced Model of Induction Moto with Faulty Cage, Poc. 7th IEEE Sym. on Diagnotic of Electic Machine, Powe Electonic and Dive, (SDEMPED 9), IEEE Catalog Numbe CFP9SDE-CDR, TF1. [11] SOBCZYK T.J., MACIOŁEK W., Influence of Pole-Pai Numbe and Roto Slot Numbe on Effect Caued by Cage Fault, Poc. 8th IEEE Sym. on Diagnotic of Electic Machine, Powe Electonic and Dive, (SDEMPED 11), IEEE Catalog Numbe CFP11SDE-USB, ID54.

Basic propositional and. The fundamentals of deduction

Basic propositional and. The fundamentals of deduction Baic ooitional and edicate logic The fundamental of deduction 1 Logic and it alication Logic i the tudy of the atten of deduction Logic lay two main ole in comutation: Modeling : logical entence ae the

More information

Considerations Regarding the Flux Estimation in Induction Generator with Application at the Control of Unconventional Energetic Conversion Systems

Considerations Regarding the Flux Estimation in Induction Generator with Application at the Control of Unconventional Energetic Conversion Systems Conideation Regading the Flux Etimation in Induction Geneato with Application at the Contol of Unconventional Enegetic Conveion Sytem Ioif Szeidet, Octavian Potean, Ioan Filip, Vaa Citian Depatment of

More information

one primary direction in which heat transfers (generally the smallest dimension) simple model good representation for solving engineering problems

one primary direction in which heat transfers (generally the smallest dimension) simple model good representation for solving engineering problems CHAPTER 3: One-Dimenional Steady-State Conduction one pimay diection in which heat tanfe (geneally the mallet dimenion) imple model good epeentation fo olving engineeing poblem 3. Plane Wall 3.. hot fluid

More information

Eddy Currents in Permanent Magnets of a Multi-pole Direct Drive Motor

Eddy Currents in Permanent Magnets of a Multi-pole Direct Drive Motor Acta Technica Jauineni Vol. 6. No. 1. 2013 Eddy Cuent in Pemanent Magnet of a Multi-pole Diect Dive Moto G. Gotovac 1, G. Lampic 1, D. Miljavec 2 Elaphe Ltd. 1, Univeity of Ljubljana, Faculty of Electical

More information

Chapter 8 Sampling. Contents. Dr. Norrarat Wattanamongkhol. Lecturer. Department of Electrical Engineering, Engineering Faculty, sampling

Chapter 8 Sampling. Contents. Dr. Norrarat Wattanamongkhol. Lecturer. Department of Electrical Engineering, Engineering Faculty, sampling Content Chate 8 Samling Lectue D Noaat Wattanamongkhol Samling Theoem Samling of Continuou-Time Signal 3 Poceing Continuou-Time Signal 4 Samling of Dicete-Time Signal 5 Multi-ate Samling Deatment of Electical

More information

Boise State University Department of Electrical and Computer Engineering ECE470 Electric Machines

Boise State University Department of Electrical and Computer Engineering ECE470 Electric Machines Boie State Univeity Depatment of Electical and Compute Engineeing ECE470 Electic Machine Deivation of the Pe-Phae Steady-State Equivalent Cicuit of a hee-phae Induction Machine Nomenclatue θ: oto haft

More information

The Normal Stress Dıstribution in an Infinite. Elastic Body with a Locally Curved and Hollow. Fiber under Geometrical Nonlinear Statement

The Normal Stress Dıstribution in an Infinite. Elastic Body with a Locally Curved and Hollow. Fiber under Geometrical Nonlinear Statement Nonlinea Analyi and Diffeential quation Vol. 4 06 no. 6 95-04 HIKARI td www.m-hikai.com htt://dx.doi.og/0.988/nade.06.656 The Nomal Ste Dıtibution in an Infinite latic Body with a ocally Cuved and Hollow

More information

ψ - exponential type orbitals, Frictional

ψ - exponential type orbitals, Frictional ew develoment in theoy of Laguee olynomial I. I. Gueinov Deatment of Phyic, Faculty of At and Science, Onekiz Mat Univeity, Çanakkale, Tukey Abtact The new comlete othonomal et of L -Laguee tye olynomial

More information

CHAPTER 2 MATHEMATICAL MODELING OF WIND ENERGY SYSTEMS

CHAPTER 2 MATHEMATICAL MODELING OF WIND ENERGY SYSTEMS 17 CHAPTER 2 MATHEMATICAL MODELING OF WIND ENERGY SYSTEMS 2.1 DESCRIPTION The development of wind enegy ytem and advance in powe electonic have enabled an efficient futue fo wind enegy. Ou imulation tudy

More information

Determination of Excitation Capacitance of a Three Phase Self Excited Induction Generator

Determination of Excitation Capacitance of a Three Phase Self Excited Induction Generator ISSN (Online): 78 8875 (An ISO 397: 007 Cetified Oganization) Detemination of Excitation Capacitance of a Thee Phae Self Excited Induction Geneato Anamika Kumai, D. A. G. Thoa, S. S. Mopai 3 PG Student

More information

Gravity. David Barwacz 7778 Thornapple Bayou SE, Grand Rapids, MI David Barwacz 12/03/2003

Gravity. David Barwacz 7778 Thornapple Bayou SE, Grand Rapids, MI David Barwacz 12/03/2003 avity David Bawacz 7778 Thonapple Bayou, and Rapid, MI 495 David Bawacz /3/3 http://membe.titon.net/daveb Uing the concept dicued in the peceding pape ( http://membe.titon.net/daveb ), I will now deive

More information

Above Flux Estimation Issues in Induction Generators with Application at Energy Conversion Systems

Above Flux Estimation Issues in Induction Generators with Application at Energy Conversion Systems Acta Polytechnica Hungaica Vol. 3, No. 3, 2006 Above Flux Etimation Iue in Induction Geneato with Application at Enegy Conveion Sytem Ioif Szeidet, Octavian Potean, Ioan Filip, Vaa Citian Depatment of

More information

6. The squirrel cage induction machine

6. The squirrel cage induction machine 6. The quiel cage induction achine TECHSCHE VERSTÄT Pof. A. Binde : Electical Machine and Dive 6/1 ntitut f Eletiche Enegieandlung FB 18 Squiel cage induction achine Coe quiel cage: fo big oe achine >

More information

A Generalized Two Axes Model of a Squirrel-Cage Induction Motor for Rotor Fault Diagnosis

A Generalized Two Axes Model of a Squirrel-Cage Induction Motor for Rotor Fault Diagnosis SEBIAN JOUNAL OF ELECTICAL ENGINEEING Vol. 5, No. 1, ay 2008, 155-170 A Genealized Two Axe odel of a Squiel-Cage Induction oto fo oto Fault Diagnoi Sami Hamdani 1, Oma Touhami 2, achid Ibtiouen 2 Abtact:

More information

Tutorial 5 Drive dynamics & control

Tutorial 5 Drive dynamics & control UNIVERSITY OF NEW SOUTH WALES Electic Dive Sytem School o Electical Engineeing & Telecommunication ELEC463 Electic Dive Sytem Tutoial 5 Dive dynamic & contol. The ollowing paamete ae known o two high peomance

More information

AC DRIVES. There are two type of AC motor Drives : 1. Induction Motor Drives 2. Synchronous Motor Drives

AC DRIVES. There are two type of AC motor Drives : 1. Induction Motor Drives 2. Synchronous Motor Drives AC DRIVES AC moto Dive ae ued in many indutial and dometic application, uch a in conveye, lift, mixe, ecalato etc. The AC moto have a numbe of advantage : Lightweight (0% to 40% lighte than equivalent

More information

Chapter 19 Webassign Help Problems

Chapter 19 Webassign Help Problems Chapte 9 Webaign Help Poblem 4 5 6 7 8 9 0 Poblem 4: The pictue fo thi poblem i a bit mileading. They eally jut give you the pictue fo Pat b. So let fix that. Hee i the pictue fo Pat (a): Pat (a) imply

More information

MANUFACTURING TOLERANCES AS A CAUSE FOR AUDIBLE NOISE OF INDUCTION MOTORS

MANUFACTURING TOLERANCES AS A CAUSE FOR AUDIBLE NOISE OF INDUCTION MOTORS MANUFACTURING TOLERANCES AS A CAUSE FOR AUDIBLE NOISE OF INDUCTION MOTORS Delaere K., Franen J., Hameyer K., Belman R. Katholieke Univeriteit Leuven, De. EE (ESAT) Div. ELEN, Kardinaal Mercierlaan 94,

More information

Then the number of elements of S of weight n is exactly the number of compositions of n into k parts.

Then the number of elements of S of weight n is exactly the number of compositions of n into k parts. Geneating Function In a geneal combinatoial poblem, we have a univee S of object, and we want to count the numbe of object with a cetain popety. Fo example, if S i the et of all gaph, we might want to

More information

6. The Squirrel-Cage Induction Machine . (6.2)

6. The Squirrel-Cage Induction Machine . (6.2) Electical Machine and Dive 6/1 Squiel-Cage nduction Machine Electical Machine and Dive 6/ Squiel-Cage nduction Machine 6. The Squiel-Cage nduction Machine Sliping-induction machine do not only have advantage

More information

Simulink Model of Direct Torque Control of Induction Machine

Simulink Model of Direct Torque Control of Induction Machine Ameican Jounal of Applied Science 5 (8): 1083-1090, 2008 ISSN 1546-9239 2008 Science Publication Simulink Model of Diect Toque Contol of Induction Machine H.F. Abdul Wahab and H. Sanui Faculty of Engineeing,

More information

Sinusoidal Oscillators

Sinusoidal Oscillators Sinuoidal Ocillato Signal geneato: inuoidal, ectangula, tiangula, aw-tooth, etc. Obtaining a ine wave: tiangle functional tanf. ine ine wave geneation: fequency elective netwok in a feedback loo of a PF

More information

ASTR 3740 Relativity & Cosmology Spring Answers to Problem Set 4.

ASTR 3740 Relativity & Cosmology Spring Answers to Problem Set 4. ASTR 3740 Relativity & Comology Sping 019. Anwe to Poblem Set 4. 1. Tajectoie of paticle in the Schwazchild geomety The equation of motion fo a maive paticle feely falling in the Schwazchild geomety ae

More information

Simulation of Spatially Correlated Large-Scale Parameters and Obtaining Model Parameters from Measurements

Simulation of Spatially Correlated Large-Scale Parameters and Obtaining Model Parameters from Measurements Simulation of Spatially Coelated Lage-Scale Paamete and Obtaining Model Paamete fom PER ZETTERBERG Stockholm Septembe 8 TRITA EE 8:49 Simulation of Spatially Coelated Lage-Scale Paamete and Obtaining Model

More information

Image Enhancement: Histogram-based methods

Image Enhancement: Histogram-based methods Image Enhancement: Hitogam-baed method The hitogam of a digital image with gayvalue, i the dicete function,, L n n # ixel with value Total # ixel image The function eeent the faction of the total numbe

More information

4. Induction machines. 4.1 Significance and features of induction machines

4. Induction machines. 4.1 Significance and features of induction machines Moto develoment 4/1 nduction machine 4. nduction machine 4.1 Significance and featue of induction machine a Baic function and diffeent tye of machine: nduction machine ae in the owe ange of 100 W u to

More information

5. The Slip-Ring Induction Machine

5. The Slip-Ring Induction Machine 5. Te Sli-ing nduction Macine Souce: Siemen AG TECHNSCHE UNVESTÄT DAMSTADT of. A. Binde : Electical Macine and Dive 5/1 ntitut fü Elektice Enegiewandlung FB 18 Active and eactive owe in conume aow ytem

More information

Faraday s Law. Faraday s Law. Faraday s Experiments. Faraday s Experiments. Magnetic Flux. Chapter 31. Law of Induction (emf( emf) Faraday s Law

Faraday s Law. Faraday s Law. Faraday s Experiments. Faraday s Experiments. Magnetic Flux. Chapter 31. Law of Induction (emf( emf) Faraday s Law Faaday s Law Faaday s Epeiments Chapte 3 Law of nduction (emf( emf) Faaday s Law Magnetic Flu Lenz s Law Geneatos nduced Electic fields Michael Faaday discoeed induction in 83 Moing the magnet induces

More information

Representation of a Group of Three-phase Induction Motors Using Per Unit Aggregation Model A.Kunakorn and T.Banyatnopparat

Representation of a Group of Three-phase Induction Motors Using Per Unit Aggregation Model A.Kunakorn and T.Banyatnopparat epreentation of a Group of Three-phae Induction Motor Uing Per Unit Aggregation Model A.Kunakorn and T.Banyatnopparat Abtract--Thi paper preent a per unit gregation model for repreenting a group of three-phae

More information

Speed Control of a Doubly Fed Induction Motor using Fuzzy Logic Techniques

Speed Control of a Doubly Fed Induction Motor using Fuzzy Logic Techniques Intenational Jounal on Electical Engineeing and Infomatic - Volume 2, Numbe 3, 2010 Speed Contol of a Doubly Fed Induction Moto uing Fuzzy Logic Technique D. Ben Attou and Y. Bekaka Depatment of Electical

More information

PHYS 1444 Lecture #5

PHYS 1444 Lecture #5 Shot eview Chapte 24 PHYS 1444 Lectue #5 Tuesday June 19, 212 D. Andew Bandt Capacitos and Capacitance 1 Coulom s Law The Fomula QQ Q Q F 1 2 1 2 Fomula 2 2 F k A vecto quantity. Newtons Diection of electic

More information

rad rev 60sec p sec 2 rad min 2 2

rad rev 60sec p sec 2 rad min 2 2 NAME: EE 459/559, Exa 1, Fall 2016, D. McCalley, 75 inute allowed (unle othewie diected) Cloed Book, Cloed Note, Calculato Peitted, No Counication Device. The following infoation ay o ay not be ueful fo

More information

MATHEMATICAL MODEL FOR THE BLOOD FLOW IN CAPILLARY VESSELS

MATHEMATICAL MODEL FOR THE BLOOD FLOW IN CAPILLARY VESSELS MATHEMATICAL MODEL FO THE BLOOD FLOW IN CAPILLAY VESSELS. Sonia PETILA. Bala ALBET. Tibeiu Pooviciu Infomatic Highchool Cluj-Naoca OMANIA. Univeity Babe-Bolyai Cluj-Naoca OMANIA Abtact: In thi ae we develo

More information

POWER SYSTEM SMALL SIGNAL STABILITY ANALYSIS BASED ON TEST SIGNAL

POWER SYSTEM SMALL SIGNAL STABILITY ANALYSIS BASED ON TEST SIGNAL POWE YEM MALL INAL ABILIY ANALYI BAE ON E INAL Zheng Xu, Wei hao, Changchun Zhou Zheang Univerity, Hangzhou, 37 PChina Email: hvdc@ceezueducn Abtract - In thi paper, a method baed on ome tet ignal (et

More information

Theorem 2: Proof: Note 1: Proof: Note 2:

Theorem 2: Proof: Note 1: Proof: Note 2: A New 3-Dimenional Polynomial Intepolation Method: An Algoithmic Appoach Amitava Chattejee* and Rupak Bhattachayya** A new 3-dimenional intepolation method i intoduced in thi pape. Coeponding to the method

More information

RESEARCH REPORT on MODELS for NUMERICAL EVALUATION of VARIABLE SPEED DIFFERENT WIND GENERATOR SYSTEMS

RESEARCH REPORT on MODELS for NUMERICAL EVALUATION of VARIABLE SPEED DIFFERENT WIND GENERATOR SYSTEMS Poject funded by the Euoean Commiion unde the 6th (EC) RTD Famewok Pogamme (00-006) within the famewok of the ecific eeach and technological develoment ogamme Integating and tengthening the Euoean Reeach

More information

Supplemental Materials. Advanced Thermoelectrics Governed by Single Parabolic Band Model:

Supplemental Materials. Advanced Thermoelectrics Governed by Single Parabolic Band Model: Electonic Supplementay Mateial (ESI) fo Phyical Chemity Chemical Phyic. Thi jounal i The Royal Society of Chemity 04 Supplemental Mateial Advanced Themoelectic Govened by Single Paabolic and Model: Mg

More information

Solutions Practice Test PHYS 211 Exam 2

Solutions Practice Test PHYS 211 Exam 2 Solution Pactice Tet PHYS 11 Exam 1A We can plit thi poblem up into two pat, each one dealing with a epaate axi. Fo both the x- and y- axe, we have two foce (one given, one unknown) and we get the following

More information

BASIC INDUCTION MOTOR CONCEPTS

BASIC INDUCTION MOTOR CONCEPTS INDUCTION MOTOS An induction motor ha the ame phyical tator a a ynchronou machine, with a different rotor contruction. There are two different type of induction motor rotor which can be placed inide the

More information

Piezoceramics-based Devices for Active Balancing of Flexible Shafts

Piezoceramics-based Devices for Active Balancing of Flexible Shafts Piezoceamic-baed Device fo Active Balancing of Flexible Shaft P. J. Sloetje, A. de Boe Univeity of Twente, Faculty of Engineeing Technology, Applied Mechanic Section Dienelolaan 5, 7500 AE, Enchede, The

More information

Fall 2004/05 Solutions to Assignment 5: The Stationary Phase Method Provided by Mustafa Sabri Kilic. I(x) = e ixt e it5 /5 dt (1) Z J(λ) =

Fall 2004/05 Solutions to Assignment 5: The Stationary Phase Method Provided by Mustafa Sabri Kilic. I(x) = e ixt e it5 /5 dt (1) Z J(λ) = 8.35 Fall 24/5 Solution to Aignment 5: The Stationay Phae Method Povided by Mutafa Sabi Kilic. Find the leading tem fo each of the integal below fo λ >>. (a) R eiλt3 dt (b) R e iλt2 dt (c) R eiλ co t dt

More information

SENSORLESS SPEED CONTROL SYSTEMS BASED ON ADAPTIVE OBSERVERS LUENBERGER AND GOPINATH

SENSORLESS SPEED CONTROL SYSTEMS BASED ON ADAPTIVE OBSERVERS LUENBERGER AND GOPINATH Annal of the Univeity of Caiova, Electical Engineeing eie, No. 32, 2008; ISSN 1842-4805 SENSORLESS SPEED CONTROL SYSTEMS BASED ON ADAPTIVE OBSERVERS LUENBERGER AND GOPINATH Maiu-Auelian PICIU, Lauenţiu

More information

17.1 Electric Potential Energy. Equipotential Lines. PE = energy associated with an arrangement of objects that exert forces on each other

17.1 Electric Potential Energy. Equipotential Lines. PE = energy associated with an arrangement of objects that exert forces on each other Electic Potential Enegy, PE Units: Joules Electic Potential, Units: olts 17.1 Electic Potential Enegy Electic foce is a consevative foce and so we can assign an electic potential enegy (PE) to the system

More information

LC transfer of energy between the driving source and the circuit will be a maximum.

LC transfer of energy between the driving source and the circuit will be a maximum. The Q of oscillatos efeences: L.. Fotney Pinciples of Electonics: Analog and Digital, Hacout Bace Jovanovich 987, Chapte (AC Cicuits) H. J. Pain The Physics of Vibations and Waves, 5 th edition, Wiley

More information

Estimation and Confidence Intervals: Additional Topics

Estimation and Confidence Intervals: Additional Topics Chapte 8 Etimation and Confidence Inteval: Additional Topic Thi chapte imply follow the method in Chapte 7 fo foming confidence inteval The text i a bit dioganized hee o hopefully we can implify Etimation:

More information

Earth Potential Rise (EPR) Computation for a Fault on Transmission Mains Pole

Earth Potential Rise (EPR) Computation for a Fault on Transmission Mains Pole ACN: 32586675 ABN: 8632586675 NATIONAL ELECTRICAL ENGINEERING CONULTANCY Earth otential Rie (ER) Computation for a Fault on Tranmiion Main ole repared by: M. Naereddine ACN: 32586675 ABN: 8632586675 Abtract

More information

Speed Control of Matrix Converter-Fed Five-Phase Permanent Magnet Synchronous Motors under Unbalanced Voltages

Speed Control of Matrix Converter-Fed Five-Phase Permanent Magnet Synchronous Motors under Unbalanced Voltages enegie Aticle Speed Contol of Matix Convete-Fed Five-Phae Pemanent Magnet Synchonou Moto unde Unbalanced Voltage Bozou Youefi 1 ID, Soodabeh Soleymani 1, *, Babak Mozafai 1 and Seid Agha Gholamian 2 1

More information

ROOT LOCUS. Poles and Zeros

ROOT LOCUS. Poles and Zeros Automatic Control Sytem, 343 Deartment of Mechatronic Engineering, German Jordanian Univerity ROOT LOCUS The Root Locu i the ath of the root of the characteritic equation traced out in the - lane a a ytem

More information

The Analysis of the Influence of the Independent Suspension on the Comfort for a Mine Truck

The Analysis of the Influence of the Independent Suspension on the Comfort for a Mine Truck 16 3 d Intenational Confeence on Vehicle, Mechanical and Electical Engineeing (ICVMEE 16 ISBN: 978-1-6595-37- The Analyi of the Influence of the Independent Supenion on the Comfot fo a Mine Tuck JINGMING

More information

Design By Emulation (Indirect Method)

Design By Emulation (Indirect Method) Deign By Emulation (Indirect Method he baic trategy here i, that Given a continuou tranfer function, it i required to find the bet dicrete equivalent uch that the ignal produced by paing an input ignal

More information

Development of Model Reduction using Stability Equation and Cauer Continued Fraction Method

Development of Model Reduction using Stability Equation and Cauer Continued Fraction Method Intenational Jounal of Electical and Compute Engineeing. ISSN 0974-90 Volume 5, Numbe (03), pp. -7 Intenational Reeach Publication Houe http://www.iphoue.com Development of Model Reduction uing Stability

More information

Direct Torque Control of Double Feed Induction Machine (DTC-DFIM)

Direct Torque Control of Double Feed Induction Machine (DTC-DFIM) Jounal of Advanced Reeach in Science and echnology ISSN: 232-9989 Diect oque Contol of Double Feed Induction Machine (DC-DFIM) Zemmit Abdeahim, Sadouni Radhwane 2 and Meoufel Abdelkade 2 Electical Engineeing

More information

TRAVELING WAVES. Chapter Simple Wave Motion. Waves in which the disturbance is parallel to the direction of propagation are called the

TRAVELING WAVES. Chapter Simple Wave Motion. Waves in which the disturbance is parallel to the direction of propagation are called the Chapte 15 RAVELING WAVES 15.1 Simple Wave Motion Wave in which the ditubance i pependicula to the diection of popagation ae called the tanvee wave. Wave in which the ditubance i paallel to the diection

More information

CHAPTER 3 CLASSICAL CONTROL TECHNIQUES FOR AC DRIVES

CHAPTER 3 CLASSICAL CONTROL TECHNIQUES FOR AC DRIVES 44 CHAPTER 3 CLASSICAL CONTROL TECHNIQUES FOR AC DRIVES 3.1 INTRODUCTION The contolle equied fo AC dive can be divided into two majo type: cala contol and vecto contol (Boe 1976). In cala contol, which

More information

γ from B D(Kπ)K and B D(KX)K, X=3π or ππ 0

γ from B D(Kπ)K and B D(KX)K, X=3π or ππ 0 fom and X, X= o 0 Jim Libby, Andew Powell and Guy Wilkinon Univeity of Oxfod 8th Januay 007 Gamma meeting 1 Outline The AS technique to meaue Uing o 0 : intoducing the coheence facto Meauing the coheence

More information

A Simplified Methodology for the Synthesis of Adaptive Flight Control Systems

A Simplified Methodology for the Synthesis of Adaptive Flight Control Systems A Simplified Methodology for the Synthei of Adaptive Flight Control Sytem J.ROUSHANIAN, F.NADJAFI Department of Mechanical Engineering KNT Univerity of Technology 3Mirdamad St. Tehran IRAN Abtract- A implified

More information

Induction Machine Shaft Speed Estimation using Imaginary Power

Induction Machine Shaft Speed Estimation using Imaginary Power Induction Machine Shaft Speed Etimation uing Imaginay Powe Teence Summe, Robet Eic Betz, Bendan McGath, Gaham Cliffod Goodwin School of Electical Engineeing and Compute Science Univeity of Newcatle, Callaghan,

More information

The physics of induction stoves

The physics of induction stoves The physics of uction stoves This is an aticle fom my home page: www.olewitthansen.dk Contents 1. What is an uction stove...1. Including self-uctance...4 3. The contibution fom the magnetic moments...6

More information

SOLVING THE KONDO PROBLEM FOR COMPLEX MESOSCOPIC SYSTEMS

SOLVING THE KONDO PROBLEM FOR COMPLEX MESOSCOPIC SYSTEMS SOLVING THE KONDO POBLEM FO COMPLEX MESOSCOPIC SYSTEMS V. DINU and M. ÞOLEA National Intitute of Material Phyic, Bucharet-Magurele P.O. Box MG-7, omania eceived February 21, 2005 Firt we preent the calculation

More information

Rotational Kinetic Energy

Rotational Kinetic Energy Add Impotant Rotational Kinetic Enegy Page: 353 NGSS Standad: N/A Rotational Kinetic Enegy MA Cuiculum Famewok (006):.1,.,.3 AP Phyic 1 Leaning Objective: N/A, but olling poblem have appeaed on peviou

More information

Given the following circuit with unknown initial capacitor voltage v(0): X(s) Immediately, we know that the transfer function H(s) is

Given the following circuit with unknown initial capacitor voltage v(0): X(s) Immediately, we know that the transfer function H(s) is EE 4G Note: Chapter 6 Intructor: Cheung More about ZSR and ZIR. Finding unknown initial condition: Given the following circuit with unknown initial capacitor voltage v0: F v0/ / Input xt 0Ω Output yt -

More information

Figure 1 Siemens PSSE Web Site

Figure 1 Siemens PSSE Web Site Stability Analyi of Dynamic Sytem. In the lat few lecture we have een how mall ignal Lalace domain model may be contructed of the dynamic erformance of ower ytem. The tability of uch ytem i a matter of

More information

Thin-Walled Tube Extension by Rigid Curved Punch

Thin-Walled Tube Extension by Rigid Curved Punch Engineeing,, 3, 45-46 doi:.436/eng..355 Publihed Online May (http://www.scirp.og/jounal/eng) Thin-Walled Tube Extenion by Rigid Cuved Punch Abtact Rotilav I. Nepehin Platic Defomation Sytem Depatment,

More information

Histogram Processing

Histogram Processing Hitogam Poceing Lectue 4 (Chapte 3) Hitogam Poceing The hitogam of a digital image with gay level fom to L- i a dicete function h( )=n, whee: i the th gay level n i the numbe of pixel in the image with

More information

Permanent Magnet Magnetization State Estimation Using High Frequency Signal Injection

Permanent Magnet Magnetization State Estimation Using High Frequency Signal Injection Thi aticle ha been acceted fo ublication in a futue iue of thi jounal, but ha not been fully edited. Content may change io to final ublication. Citation infomation: DOI 1.119/TIA.216.2541616, IEEE Tanaction

More information

MRAS Based Speed Sensor-less Vector Controlled Induction Motor Using Modified Adaptive Mechanism

MRAS Based Speed Sensor-less Vector Controlled Induction Motor Using Modified Adaptive Mechanism Seno & Tanduce, Vol. 55, Iue 8, Augut 23, pp. 8-85 Seno & Tanduce 23 by IFSA http://www.enopotal.com MRAS Baed Speed Seno-le Vecto Contolled Induction Moto Uing Modified Adaptive Mechanim ALIYU Eneji Iah,

More information

Determining the Best Linear Unbiased Predictor of PSU Means with the Data. included with the Random Variables. Ed Stanek

Determining the Best Linear Unbiased Predictor of PSU Means with the Data. included with the Random Variables. Ed Stanek Detemining te Bet Linea Unbiaed Pedicto of PSU ean wit te Data included wit te andom Vaiable Ed Stanek Intoduction We develop te equation fo te bet linea unbiaed pedicto of PSU mean in a two tage andom

More information

INFLUENCE OF BROKEN ROTOR BARS LOCATION IN THE SQUIRREL CAGE INDUCTION MOTOR USING FINITE ELEMENT METHOD

INFLUENCE OF BROKEN ROTOR BARS LOCATION IN THE SQUIRREL CAGE INDUCTION MOTOR USING FINITE ELEMENT METHOD Journal of Fundamental and Applied Science ISSN - Available online at http:www.jfa.info INFLUENCE OF BROKEN ROTOR BARS LOCATION IN THE SQUIRREL CAGE INDUCTION MOTOR USING FINITE ELEMENT METHOD N. Halem*,

More information

Fuzzy Speed Regulator for Induction Motor Direct Torque Control Scheme

Fuzzy Speed Regulator for Induction Motor Direct Torque Control Scheme ACEEE Int. J. on Electical and Powe Engineeing, ol., No., Dec Fuzzy peed Regulato fo Induction Moto Diect Toque Contol cheme Jagadih H. Puja,. F. Kodad Reeach chola JNTU, Anantapu & Faculty Depatment of

More information

Physics 313 Practice Test Page 1. University Physics III Practice Test II

Physics 313 Practice Test Page 1. University Physics III Practice Test II Physics 313 Pactice Test Page 1 Univesity Physics III Pactice Test II This pactice test should give you a ough idea of the fomat and oveall level of the Physics 313 exams. The actual exams will have diffeent

More information

A Novel Method for Modeling Magnetic Saturation in the Main Flux of Induction Machine

A Novel Method for Modeling Magnetic Saturation in the Main Flux of Induction Machine Poceeding of the 5th WSEAS Int. Conf. on Syte Science and Siulation in Engineeing, Teneife, Canay Ilan, Spain, Decebe 16-18, 2006 150 A Novel Method fo Modeling Magnetic Satuation in the Main Flux of Induction

More information

VECTOR CONTROL OF INDUCTION MOTOR DRIVE BY USING THE CONSTANT SWITCHING FREQUENCY CURRENT CONTROLLER FOR REDUCED RIPPLE

VECTOR CONTROL OF INDUCTION MOTOR DRIVE BY USING THE CONSTANT SWITCHING FREQUENCY CURRENT CONTROLLER FOR REDUCED RIPPLE Acta Electotechnica et Infomatica, Vol. 3, No. 3, 203, 27 33, DOI: 0.2478/aeei-203-0036 27 VECTOR CONTROL OF INDUCTION MOTOR DRIVE BY USING THE CONSTANT SWITCHING FREQUENCY CURRENT CONTROLLER FOR REDUCED

More information

How Electric Currents Interact with Magnetic Fields

How Electric Currents Interact with Magnetic Fields How Electic Cuents nteact with Magnetic Fields 1 Oested and Long Wies wote these notes to help ou with vaious diectional ules, and the equivalence between the magnetism of magnets and the magnets of electic

More information

What lies between Δx E, which represents the steam valve, and ΔP M, which is the mechanical power into the synchronous machine?

What lies between Δx E, which represents the steam valve, and ΔP M, which is the mechanical power into the synchronous machine? A 2.0 Introduction In the lat et of note, we developed a model of the peed governing mechanim, which i given below: xˆ K ( Pˆ ˆ) E () In thee note, we want to extend thi model o that it relate the actual

More information

No-load And Blocked Rotor Test On An Induction Machine

No-load And Blocked Rotor Test On An Induction Machine No-load And Blocked Rotor Tet On An Induction Machine Aim To etimate magnetization and leakage impedance parameter of induction machine uing no-load and blocked rotor tet Theory An induction machine in

More information

Shrinkage Estimation of Reliability Function for Some Lifetime Distributions

Shrinkage Estimation of Reliability Function for Some Lifetime Distributions Ameican Jounal of Computational and Applied Mathematic 4, 4(3): 9-96 DOI:.593/j.ajcam.443.4 Shinkage Etimation of eliability Function fo Some Lifetime Ditibution anjita Pandey Depatment of Statitic, niveity

More information

Basic parts of an AC motor : rotor, stator, The stator and the rotor are electrical

Basic 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 information

RESONANCE SERIES RESONANT CIRCUITS. 5/2007 Enzo Paterno 1

RESONANCE SERIES RESONANT CIRCUITS. 5/2007 Enzo Paterno 1 ESONANCE SEIES ESONANT CICUITS 5/007 Enzo Pateno ESONANT CICUITS A vey impotant cicuit, used in a wide vaiety o electical and electonic systems today (i.e. adio & television tunes), is called the esonant

More information

EXAM NMR (8N090) November , am

EXAM NMR (8N090) November , am EXA NR (8N9) Novembe 5 9, 9. 1. am Remaks: 1. The exam consists of 8 questions, each with 3 pats.. Each question yields the same amount of points. 3. You ae allowed to use the fomula sheet which has been

More information

On the Efficiency of Markets with Two-sided Proportional Allocation Mechanisms

On the Efficiency of Markets with Two-sided Proportional Allocation Mechanisms On the Efficiency of Maket with Two-ided Pootional Allocation Mechanim Volodymy Kulehov and Adian Vetta Deatment of Mathematic and Statitic, and School of Comute Science, McGill Univeity volodymy.kulehov@mail.mcgill.ca,

More information

Gain and Phase Margins Based Delay Dependent Stability Analysis of Two- Area LFC System with Communication Delays

Gain and Phase Margins Based Delay Dependent Stability Analysis of Two- Area LFC System with Communication Delays Gain and Phae Margin Baed Delay Dependent Stability Analyi of Two- Area LFC Sytem with Communication Delay Şahin Sönmez and Saffet Ayaun Department of Electrical Engineering, Niğde Ömer Halidemir Univerity,

More information

Second Order Fuzzy S-Hausdorff Spaces

Second Order Fuzzy S-Hausdorff Spaces Inten J Fuzzy Mathematical Achive Vol 1, 013, 41-48 ISSN: 30-34 (P), 30-350 (online) Publihed on 9 Febuay 013 wwweeachmathciog Intenational Jounal o Second Ode Fuzzy S-Haudo Space AKalaichelvi Depatment

More information

Section Induction motor drives

Section Induction motor drives Section 5.1 - nduction motor drive Electric Drive Sytem 5.1.1. ntroduction he AC induction motor i by far the mot widely ued motor in the indutry. raditionally, it ha been ued in contant and lowly variable-peed

More information

Linearteam tech paper. The analysis of fourth-order state variable filter and it s application to Linkwitz- Riley filters

Linearteam tech paper. The analysis of fourth-order state variable filter and it s application to Linkwitz- Riley filters Linearteam tech paper The analyi of fourth-order tate variable filter and it application to Linkwitz- iley filter Janne honen 5.. TBLE OF CONTENTS. NTOCTON.... FOTH-OE LNWTZ-LEY (L TNSFE FNCTON.... TNSFE

More information

Chapter 6. NEWTON S 2nd LAW AND UNIFORM CIRCULAR MOTION. string

Chapter 6. NEWTON S 2nd LAW AND UNIFORM CIRCULAR MOTION. string Chapte 6 NEWTON S nd LAW AND UNIFORM CIRCULAR MOTION 103 PHYS 1 1 L:\103 Phy LECTURES SLIDES\103Phy_Slide_T1Y3839\CH6Flah 3 4 ting Quetion: A ball attached to the end of a ting i whiled in a hoizontal

More information

Experiment I Voltage Variation and Control

Experiment I Voltage Variation and Control ELE303 Electicity Netwoks Expeiment I oltage aiation and ontol Objective To demonstate that the voltage diffeence between the sending end of a tansmission line and the load o eceiving end depends mainly

More information

Chapter 6. NEWTON S 2nd LAW AND UNIFORM CIRCULAR MOTION

Chapter 6. NEWTON S 2nd LAW AND UNIFORM CIRCULAR MOTION Chapte 6 NEWTON S nd LAW AND UNIFORM CIRCULAR MOTION Phyic 1 1 3 4 ting Quetion: A ball attached to the end of a ting i whiled in a hoizontal plane. At the point indicated, the ting beak. Looking down

More information

Simulation and Analysis of Linear Permanent Magnet Vernier Motors for Direct Drive Systems

Simulation and Analysis of Linear Permanent Magnet Vernier Motors for Direct Drive Systems Available online at www.ijpe-online.com vol. 3, no. 8, December 07, pp. 304-3 DOI: 0.3940/ijpe.7.08.p.3043 Simulation and Analyi of Linear Permanent Magnet Vernier Motor for Direct Drive Sytem Mingjie

More information

Steady State and Transient Performance Analysis of Three Phase Induction Machine using MATLAB Simulations

Steady State and Transient Performance Analysis of Three Phase Induction Machine using MATLAB Simulations Intenational Jounal of Recent Tends in Engineeing, Vol, No., May 9 Steady State and Tansient Pefomance Analysis of Thee Phase Induction Machine using MATAB Simulations Pof. Himanshu K. Patel Assistant

More information

EKT 345 MICROWAVE ENGINEERING CHAPTER 2: PLANAR TRANSMISSION LINES

EKT 345 MICROWAVE ENGINEERING CHAPTER 2: PLANAR TRANSMISSION LINES EKT 345 MICROWAVE ENGINEERING CHAPTER : PLANAR TRANSMISSION LINES 1 Tansmission Lines A device used to tansfe enegy fom one point to anothe point efficiently Efficiently minimum loss, eflection and close

More information

Σr2=0. Σ Br. Σ br. Σ r=0. br = Σ. Σa r-s b s (1.2) s=0. Σa r-s b s-t c t (1.3) t=0. cr = Σ. dr = Σ. Σa r-s b s-t c t-u d u (1.4) u =0.

Σr2=0. Σ Br. Σ br. Σ r=0. br = Σ. Σa r-s b s (1.2) s=0. Σa r-s b s-t c t (1.3) t=0. cr = Σ. dr = Σ. Σa r-s b s-t c t-u d u (1.4) u =0. 0 Powe of Infinite Seie. Multiple Cauchy Poduct The multinomial theoem i uele fo the powe calculation of infinite eie. Thi i becaue the polynomial theoem depend on the numbe of tem, o it can not be applied

More information

AIRCRAFT ENGINE RESPONSE DUE TO FAN UNBALANCE AND TO THE PRESENCE OF CONSUMED GAPS IN THE ENGINE DURING THE PHASE OF WINDMILLING

AIRCRAFT ENGINE RESPONSE DUE TO FAN UNBALANCE AND TO THE PRESENCE OF CONSUMED GAPS IN THE ENGINE DURING THE PHASE OF WINDMILLING ICAS CONGRESS AIRCRAF ENGINE RESPONSE DUE O FAN UNBALANCE AND O HE PRESENCE OF CONSUMED GAPS IN HE ENGINE DURING HE PHASE OF WINDMILLING B. Benay AEROSPAIALE MARA AIRBUS 316 ouloue Cedex 3 Fance Abtact

More information

LECTURE 14. m 1 m 2 b) Based on the second law of Newton Figure 1 similarly F21 m2 c) Based on the third law of Newton F 12

LECTURE 14. m 1 m 2 b) Based on the second law of Newton Figure 1 similarly F21 m2 c) Based on the third law of Newton F 12 CTU 4 ] NWTON W O GVITY -The gavity law i foulated fo two point paticle with ae and at a ditance between the. Hee ae the fou tep that bing to univeal law of gavitation dicoveed by NWTON. a Baed on expeiental

More information

3. Perturbation of Kerr BH

3. Perturbation of Kerr BH 3. Petubation of Ke BH hoizon at Δ = 0 ( = ± ) Unfotunately, it i technically fomidable to deal with the metic petubation of Ke BH becaue of coupling between and θ Nevethele, thee exit a fomalim (Newman-Penoe

More information

ECE Spring Prof. David R. Jackson ECE Dept. Notes 5

ECE Spring Prof. David R. Jackson ECE Dept. Notes 5 ECE 6345 Sping 15 Pof. David R. Jackson ECE Dept. Notes 5 1 Oveview This set of notes discusses impoved models of the pobe inductance of a coaxially-fed patch (accuate fo thicke substates). A paallel-plate

More information

MATERIAL SPREADING AND COMPACTION IN POWDER-BASED SOLID FREEFORM FABRICATION METHODS: MATHEMATICAL MODELING

MATERIAL SPREADING AND COMPACTION IN POWDER-BASED SOLID FREEFORM FABRICATION METHODS: MATHEMATICAL MODELING MATERIAL SPREADING AND COMPACTION IN POWDER-BASED SOLID FREEFORM FABRICATION METHODS: MATHEMATICAL MODELING Yae Shanjani and Ehan Toyekani Depatment of Mechanical and Mechatonic Engineeing, Univeity of

More information

Torsional Vibration Analysis of Reciprocating Compressor Trains driven by Induction Motors

Torsional Vibration Analysis of Reciprocating Compressor Trains driven by Induction Motors IOP Confeence Seie: Mateial Science and Engineeing PAPER OPEN ACCESS Toional Vibation Analyi of Recipocating Compeo Tain diven by Induction Moto To cite thi aticle: M Bunelli et al 015 IOP Conf. Se.: Mate.

More information

The Influence of the Load Condition upon the Radial Distribution of Electromagnetic Vibration and Noise in a Three-Phase Squirrel-Cage Induction Motor

The Influence of the Load Condition upon the Radial Distribution of Electromagnetic Vibration and Noise in a Three-Phase Squirrel-Cage Induction Motor The Influence of the Load Condition upon the Radial Ditribution of Electromagnetic Vibration and Noie in a Three-Phae Squirrel-Cage Induction Motor Yuta Sato 1, Iao Hirotuka 1, Kazuo Tuboi 1, Maanori Nakamura

More information

Phys-272 Lecture 18. Mutual Inductance Self-Inductance R-L Circuits

Phys-272 Lecture 18. Mutual Inductance Self-Inductance R-L Circuits Phys-7 ectue 8 Mutual nductance Self-nductance - Cicuits Mutual nductance f we have a constant cuent i in coil, a constant magnetic field is ceated and this poduces a constant magnetic flux in coil. Since

More information

Brushless Doubly-Fed Induction Machines: Magnetic Field Modelling

Brushless Doubly-Fed Induction Machines: Magnetic Field Modelling Buhle Doubly-Fed Induction Machine: Magnetic Field Modelling T. D. Stou.H. van de Blij H. Polinde J. A. Feeia Φ Abtact The buhle DFIM i a complex machine type. Though neve commecially exploited it ha a

More information