6. The squirrel cage induction machine

Size: px
Start display at page:

Download "6. The squirrel cage induction machine"

Transcription

1 6. The quiel cage induction achine TECHSCHE VERSTÄT Pof. A. Binde : Electical Machine and Dive 6/1 ntitut f Eletiche Enegieandlung FB 18

2 Squiel cage induction achine Coe quiel cage: fo big oe achine > W and fo taction achine: Maive non-inulated coe ba in oto lot. At both font end hot-cicuited by to coe end ing by elding. Soetie coe die cat oto fo alle achine to inceae efficiency. Aluiniu coe quiel cage: Die cat cage fo alle achine < W: The hole cage i cat a one iece ith liquid aluiniu. Additional fan blade fo cooling at the end ing and balancing bolt ae cat at the ae tie. To adjacent ba fo ith the in beteen ing egent oto loo hee tato otating field induce the oto voltage. Thi caue oto ba cuent & end ing egent cuent. Roto ba cuent togethe ith tato field ceate electoagnetic toque. TECHSCHE VERSTÄT Pof. A. Binde : Electical Machine and Dive 6/ ntitut f Eletiche Enegieandlung FB 18

3 Aluiniu die cat quiel cage induction achine Cage induction achine oen ventilated ai cooling Ai flo Shaft-ounted fan Cage end ing ith fan blade Fan hood fo guidance of ai Aluiniu die cat quiel cage oto eed by one tato lot to educe loe caued by lot haonic TECHSCHE VERSTÄT Pof. A. Binde : Electical Machine and Dive 6/3 ntitut f Eletiche Enegieandlung FB 18

4 nduced oto voltage e ba Stato fundaental ai ga ave (alitude ˆ ) ove elatively to the oto ith eed v yn = v yn - v. To oto ba ditanced by ole itch = oto loo". Magnetic flux e loo: l ˆ Magnetic flux e loo Φ B nduced voltage e loo induced ith fequency f = f : ˆ f lbˆ ( f ) l Bˆ v l Bˆ i c Pe ba = half loo: half voltage ˆ i ba = Roto ba voltage ˆ v Bˆ i ba yn l ˆ i c / B yn TECHSCHE VERSTÄT Pof. A. Binde : Electical Machine and Dive 6/4 ntitut f Eletiche Enegieandlung FB 18

5 Roto ba voltage fo egula bundle of hao Ditance beteen to ba = oto lot itch Q. t yield hae hift beteen adjacent ba voltage = = Roto lot angle Q Q Facit: Voltage hao of all oto ba fo on colex lane a egula bundle of hao. Exale: Fou ole cage oto ith Q /= 14 ba e ole ai. To adjacent ba voltage hao ae hae hifted by oto lot angle Q / 7 Q 8 Afte ole hae bundle i eeated: The ba voltage of ba 1 and 15 and 16 etc. ae in hae. TECHSCHE VERSTÄT Pof. A. Binde : Electical Machine and Dive 6/5 ntitut f Eletiche Enegieandlung FB 18

6 Ba cuent ba foce toque Roto ba cuent fo egula cuent hao bundle hich excite a oto ai ga field ave. Only fundaental futhe conideed. Togethe ith tato fundaental field it fo the eulting ai ga agnetic field. The ba cuent and the tato fundaental ai ga field ceate e ba e ba the tangential ORETZ-foce: F ˆ ba ˆ balb ˆ All ba foce fo ith the leve d / the electoagnetic toque M e. c) TECHSCHE VERSTÄT Pof. A. Binde : Electical Machine and Dive 6/6 ntitut f Eletiche Enegieandlung FB 18

7 Ring cuent Ring cuent flo in the ing egent: e. g. beteen ba o. (ba cuent ) and o. 3 (ba cuent 3 ) a ing ection cuent 3. KRCHHOFF node ule: Hence the ing ection cuent ae alo hae hifted by oto lot angle Q and fo a egula bundle of ing ection cuent. c) 1 in( Q / ) ba Ring in( / Q ) Reitance e ing ection R Ring : the equivalent eitance eitance R ba : P * R Ring i added to ba * Cu Q Rbaba QRRing Ring Q ( Rba RRing ) ba * RRing RRing 1/(in ( / Q )) TECHSCHE VERSTÄT Pof. A. Binde : Electical Machine and Dive 6/7 ntitut f Eletiche Enegieandlung FB 18

8 ntitut f Eletiche Enegieandlung FB 18 TECHSCHE VERSTÄT Pof. A. Binde : Electical Machine and Dive 6/8 Cage tanfe atio Each ba ay be egaded a a eaate hae: nube of inding e hae: 1/ nube of oto hae = Q inding coefficient = 1. Voltage and cuent tanfe atio ae diffeent: Roto elf and utual inductance e hae (= e ba): ith tanfe atio: Reult: Q ba h h l l 0 0 h l l M 0 0 h l l M 0 0 R R h h M M

9 ntitut f Eletiche Enegieandlung FB 18 TECHSCHE VERSTÄT Pof. A. Binde : Electical Machine and Dive 6/9 Equivalent cicuit fo cage induction achine e of tanfe atio in the tato and oto voltage equation: T-Equivalent cicuit e tato hae: Facit: We get the SAME equivalent cicuit a ith ound oto induction achine. h R j j M j ) / ( 0 ) / ( ) / ( ) / ( h R j j M j h h R j j j h h R j j j 0 ) ( h jx jx R ) ( 0 h jx jx R

10 Field line B of a cage induction achine Stato Main flux ORTH POE Main flux: in tato and oto inding; field line co the ai ga eaage flux (tay flux): only lined ith eithe tato o oto inding; field line DO OT co the ai ga Roto Ai ga Roto lot leaage flux Exale: Fou-ole edge ba oto: Field line at tand till (n = 0) - Roto fequency = Stato fequency - Roto cuent i EARY in hae ooition to tato cuent Stato lot leaage flux TECHSCHE VERSTÄT Pof. A. Binde : Electical Machine and Dive 6/10 ntitut f Eletiche Enegieandlung FB 18

11 Roto lot tay flux f oto cuent denity J ba ba / Aba i hoogeneouly ditibuted ove ba co ection then lot tay field hich coe lot eendicula to lot axi inceae linea ith ba height x! H d HQ ( x) C x bba ba x Q ( x) 0 J 0 b b hba AMPERE la: B b J x b 0 x h ba ba BQ 0 b ba o x > h ba TECHSCHE VERSTÄT Pof. A. Binde : Electical Machine and Dive 6/11 ntitut f Eletiche Enegieandlung FB 18

12 Cuent dilaceent in oto ba Slot flux denity i ulating ith oto fequency enetating the oto ba fo the ide. High oto ba fo a "aive hot cicuit loo". FARADAY la yield: B Q induce voltage u i = -d/dt in ba hich caue eddy cuent flo Ft. Self field of that eddy cuent B QFt i diected ooite to B Q due to EZ ule. Hence the eddy cuent Ft flo in ue ba egion diection of ba cuent ba and in loe ba egion OPPOSTE to ba cuent. Facit 1: Due to Ft the eulting ba cuent denity i HGHER in ue ba egion: Cuent dilaceent toad ue ba egion ( Sin effect ). Facit : The eulting lot tay flux denity B Q~ i due to B QFt educed. Cuent dilaceent CREASES ith inceaing oto fequency f ith inceaing electic ba-conductivity ith inceaing ba height h ba and ith inceaing eeability of conducto. (ote: Coe and aluiniu eeability i = 0!) TECHSCHE VERSTÄT Pof. A. Binde : Electical Machine and Dive 6/1 ntitut f Eletiche Enegieandlung FB 18

13 Effect of oto cuent dilaceent - At high oto fequency (e. g. = 1) ajo at of ba cuent flo in ue ba egion: o only educed ba co ection i ued fo cuent flo. Thu AC ba eitance R ba~ i highe than DC ba eitance R ba=. -Due to eduction of lot tay flux denity the lot leaage flux i educed. Hence the AC ba inductance ba~ i alle than the DC ba inductance ba=. R ba ~ RRba Rba ba~ ba ba - At lo oto fequency (e. g. = ) nealy O cuent dilaceent occu! TECHSCHE VERSTÄT Pof. A. Binde : Electical Machine and Dive 6/13 ntitut f Eletiche Enegieandlung FB 18

14 Reitance inceae R and inductance deceae Reduced conducto height : Pe-unit value containing all elevant aaete: R fo dee ba ( ectangula co ection") deend on: h ba f b b ba TECHSCHE VERSTÄT Pof. A. Binde : Electical Machine and Dive 6/14 ntitut f Eletiche Enegieandlung FB 18

15 Exale: Cuent dilaceent in dee ba Coe dee ba: - At 75 C ba teeatue coe conductivity i Cu = S/. - Ba idth = lot idth: ba b 7 - Peeability: Cu V/(A) - Stating of induction achine: = 1: Roto fequency f =50Hz - Ba height: h ba = 3 c h ba f b b ba b Fo cuve R () e get: R (3) = 3 and fo () follo: (3) = 0.5. Facit: - Roto ba eitance inceae u to 3-fold! - Roto ba inductance deceae don to 50%. Thub ule: At 50 Hz the inceae of eitance of coe dee ba i h c R.98 3 ba TECHSCHE VERSTÄT Pof. A. Binde : Electical Machine and Dive 6/15 ntitut f Eletiche Enegieandlung FB 18

16 nceae of tating toque by cuent dilaceent nceae of oto loe lead to inceae of tating toque M 1 : P PCu / PCu M e( ) M1 M e( 1) Ω Ω Ω yn yn Secial ba co ection fo all and big tating toque: yn SMA cuent dilaceent = M 1 all: a) Round ba b) Oval ba BG cuent dilaceent = M 1 inceaed: c) Dee ba d) Wedge ba e) -ba VERY BG cuent dilaceent = M 1 big: f) and h): Double ba g) altenating ba: Round ue bonze ba (high eitance) caue along ith cuent dilaceent fo loe in ue ba high oto loe M 1 i big. oe ba nealy ithout cuent (STARTG OF MOTOR = 1). At ated li all cuent dilaceent: Cuent flo ainly in loe ba: lo loe! TECHSCHE VERSTÄT Pof. A. Binde : Electical Machine and Dive 6/16 ntitut f Eletiche Enegieandlung FB 18

17 Toque chaacteitic of induction achine M(n)-chaacteitic of induction achine ith diffeent oto ba co ection n the figue toque i given e unit of ated toque eed e unit of ynchonou eed! Wound oto ith ound ie: Roto inding conit of any thin ie: no cuent dilaceent; iila: Round ba oto Wedge and dee ba oto: inceaed tating toque of about 40%... 80%M ; Double cage oto: Stating toque eache 160% M. Big cuent dilaceent need dee ba = high dc ba inductance = big leaage coefficient. Hence bea don toque deceae. 1 Mb X TECHSCHE VERSTÄT Pof. A. Binde : Electical Machine and Dive 6/17 ntitut f Eletiche Enegieandlung FB 18

18 Dee ba oto: nfluence of cuent dilaceent Calculated tato cuent and toque in deendence of eed: 550 W 4 ole thee hae dee ba oto cage 6.6 V 50 Hz With cuent dilaceent ( R ) in the oto ba Without cuent dilaceent ( = 1 R = 1): Toque and cuent ae alle at = 1. TECHSCHE VERSTÄT Pof. A. Binde : Electical Machine and Dive 6/18 ntitut f Eletiche Enegieandlung FB 18

19 nfluence of cuent dilaceent on cicle diaga nceae of eitance: Coefficient R : Shae of cicle eain unchanged but li cale i hifted to the left toad no-load oint P 0. Reduction of tay inductance: Coefficient : inceae cicle diaete! Facit: Each li value define by R () () a eaate cicle. Hence eulting cuent locu i no longe a cicle! TECHSCHE VERSTÄT Pof. A. Binde : Electical Machine and Dive 6/19 ntitut f Eletiche Enegieandlung FB 18

20 Flux denity line ithout / ith cuent dilaceent Wedge oto cage a) b) a) o-load: Roto fequency zeo: o oto cuent no cuent dilaceent. b) oced oto ( = 1): Roto fequency = tato fequency: Big cuent dilaceent. Roto cuent hae ooite to tato cuent; flo ainly in ue at of oto ba eule tato field to ai ga. TECHSCHE VERSTÄT Pof. A. Binde : Electical Machine and Dive 6/0 ntitut f Eletiche Enegieandlung FB 18

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

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

EE8412 Advanced AC Drive Systems. Topic 6 Field Oriented control (FOC)

EE8412 Advanced AC Drive Systems. Topic 6 Field Oriented control (FOC) Advanced AC Dive Syte Topic 6 Field Oiented contol (FOC) Souce: ABB 1 Advanced AC Dive Syte Field Oiented Contol (FOC) ectue Topi Geneal Block Diaga of FOC Diect Field Oiented Contol Diect FOC with Cuent

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

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

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 31 Faraday s Law

Chapter 31 Faraday s Law Chapte 31 Faaday s Law Change oving --> cuent --> agnetic field (static cuent --> static agnetic field) The souce of agnetic fields is cuent. The souce of electic fields is chage (electic onopole). Altenating

More information

Phys-272 Lecture 17. Motional Electromotive Force (emf) Induced Electric Fields Displacement Currents Maxwell s Equations

Phys-272 Lecture 17. Motional Electromotive Force (emf) Induced Electric Fields Displacement Currents Maxwell s Equations Phys-7 Lectue 17 Motional Electomotive Foce (emf) Induced Electic Fields Displacement Cuents Maxwell s Equations Fom Faaday's Law to Displacement Cuent AC geneato Magnetic Levitation Tain Review of Souces

More information

FARADAY'S LAW. dates : No. of lectures allocated. Actual No. of lectures 3 9/5/09-14 /5/09

FARADAY'S LAW. dates : No. of lectures allocated. Actual No. of lectures 3 9/5/09-14 /5/09 FARADAY'S LAW No. of lectues allocated Actual No. of lectues dates : 3 9/5/09-14 /5/09 31.1 Faaday's Law of Induction In the pevious chapte we leaned that electic cuent poduces agnetic field. Afte this

More information

FARADAY'S LAW dt

FARADAY'S LAW dt FAADAY'S LAW 31.1 Faaday's Law of Induction In the peious chapte we leaned that electic cuent poduces agnetic field. Afte this ipotant discoey, scientists wondeed: if electic cuent poduces agnetic field,

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

Mon , (.12) Rotational + Translational RE 11.b Tues.

Mon , (.12) Rotational + Translational RE 11.b Tues. Mon..-.3, (.) Rotational + Tanlational RE.b Tue. EP0 Mon..4-.6, (.3) Angula Momentum & Toque RE.c Tue. Wed..7 -.9, (.) Toque EP RE.d ab Fi. Rotation Coue Eval.0 Quantization, Quiz RE.e Mon. Review fo Final

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

SPH4U Magnetism Test Name: Solutions

SPH4U Magnetism Test Name: Solutions SPH4U Magneti et Nae: Solution QUESION 1 [4 Mak] hi and the following two quetion petain to the diaga below howing two cuent-caying wie. wo cuent ae flowing in the ae diection (out of the page) a hown.

More information

PHYSICS 151 Notes for Online Lecture 2.6

PHYSICS 151 Notes for Online Lecture 2.6 PHYSICS 151 Note fo Online Lectue.6 Toque: The whole eaon that we want to woy about cente of ma i that we ae limited to lookin at point mae unle we know how to deal with otation. Let eviit the metetick.

More information

18 Problem 1. 7 d Sketch a cross section of a switched reluctance machine and explain the principle of operation.

18 Problem 1. 7 d Sketch a cross section of a switched reluctance machine and explain the principle of operation. Exam Electrical Machine and Drive (ET4117) 9 November 01 from 14.00 to 17.00. Thi exam conit of 3 roblem on 3 age. Page 5 can be ued to anwer roblem 4 quetion a. The number before a quetion indicate how

More information

CHAPTER 17. Solutions for Exercises. Using the expressions given in the Exercise statement for the currents, we have

CHAPTER 17. Solutions for Exercises. Using the expressions given in the Exercise statement for the currents, we have CHATER 7 Slutin f Execie E7. F Equatin 7.5, we have B gap Ki ( t ) c( θ) + Ki ( t ) c( θ 0 ) + Ki ( t ) c( θ 40 a b c ) Uing the expein given in the Execie tateent f the cuent, we have B gap K c( ωt )c(

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

Module 18: Outline. Magnetic Dipoles Magnetic Torques

Module 18: Outline. Magnetic Dipoles Magnetic Torques Module 18: Magnetic Dipoles 1 Module 18: Outline Magnetic Dipoles Magnetic Toques 2 IA nˆ I A Magnetic Dipole Moment μ 3 Toque on a Cuent Loop in a Unifom Magnetic Field 4 Poblem: Cuent Loop Place ectangula

More information

EE595S: Class Lecture Notes Chapter 2* / QD Models for Permanent Magnet Synchronous Machines

EE595S: Class Lecture Notes Chapter 2* / QD Models for Permanent Magnet Synchronous Machines EE595S: Class ectue Notes Chapte * / QD Models fo Peanent Magnet Synchonous Machines S.D. Sudhoff Fall 5 *Analysis and Design of Peanent Magnet Synchonous Machines S.D. Sudhoff, S.P. Pekaek B. Fahii .1

More information

3-Axis Vector Magnet: Construction and Characterisation of Split Coils at RT. Semester Project Petar Jurcevic

3-Axis Vector Magnet: Construction and Characterisation of Split Coils at RT. Semester Project Petar Jurcevic 3-Axis Vecto Magnet: Constuction and Chaacteisation of Split Coils at RT Semeste Poject Peta Jucevic Outline Field Calculation and Simulation Constuction Details Field Calculations Chaacteization at RT

More information

MTE2 Wed 26, at 5:30-7:00 pm Ch2103 and SH 180. Contents of MTE2. Study chapters (no 32.6, 32.10, no 32.8 forces between wires)

MTE2 Wed 26, at 5:30-7:00 pm Ch2103 and SH 180. Contents of MTE2. Study chapters (no 32.6, 32.10, no 32.8 forces between wires) MTE Wed 6, at 5:30-7:00 pm Ch03 and SH 80 Contents of MTE Wok of the electic foce and potential enegy Electic Potential and ield Capacitos and capacitance Cuent and esistance, Ohm s la DC Cicuits and Kichoff

More information

MAGNETIC FIELD INTRODUCTION

MAGNETIC FIELD INTRODUCTION MAGNETIC FIELD INTRODUCTION It was found when a magnet suspended fom its cente, it tends to line itself up in a noth-south diection (the compass needle). The noth end is called the Noth Pole (N-pole),

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

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

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

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

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

Vector Control. Application to Induction Motor Control. DSP in Motion Control - Seminar

Vector Control. Application to Induction Motor Control. DSP in Motion Control - Seminar Vecto Contol Application to Induction Moto Contol Vecto Contol - Pinciple The Aim of Vecto Contol is to Oient the Flux Poducing Component of the Stato Cuent to some Suitable Flux Vecto unde all Opeating

More information

( )( )( ) ( ) + ( ) ( ) ( )

( )( )( ) ( ) + ( ) ( ) ( ) 3.7. Moel: The magnetic fiel is that of a moving chage paticle. Please efe to Figue Ex3.7. Solve: Using the iot-savat law, 7 19 7 ( ) + ( ) qvsinθ 1 T m/a 1.6 1 C. 1 m/s sin135 1. 1 m 1. 1 m 15 = = = 1.13

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

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

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

More information

Circular Motion. Mr. Velazquez AP/Honors Physics

Circular Motion. Mr. Velazquez AP/Honors Physics Cicula Motion M. Velazquez AP/Honos Physics Objects in Cicula Motion Accoding to Newton s Laws, if no foce acts on an object, it will move with constant speed in a constant diection. Theefoe, if an object

More information

15 B1 1. Figure 1. At what speed would the car have to travel for resonant oscillations to occur? Comment on your answer.

15 B1 1. Figure 1. At what speed would the car have to travel for resonant oscillations to occur? Comment on your answer. Kiangsu-Chekiang College (Shatin) F:EasteHolidaysAssignmentAns.doc Easte Holidays Assignment Answe Fom 6B Subject: Physics. (a) State the conditions fo a body to undego simple hamonic motion. ( mak) (a)

More information

Exam 3, vers Physics Spring, 2003

Exam 3, vers Physics Spring, 2003 1 of 9 Exam 3, ves. 0001 - Physics 1120 - Sping, 2003 NAME Signatue Student ID # TA s Name(Cicle one): Michael Scheffestein, Chis Kelle, Paisa Seelungsawat Stating time of you Tues ecitation (wite time

More information

Thrust Control of Traction Linear Induction Motors in Switch Areas

Thrust Control of Traction Linear Induction Motors in Switch Areas Thut Contol of Taction inea Induction Moto in Switch Aea Cai-Xia Tao,Dan Zhang,Xiao i School of Autoation and Electical engineeing anzhou JiaoTong Unieity 88 Wet Anning Rd.anzhou Ganu China 0130418@tu.lzjtu.edu.cn

More information

Can a watch-sized electromagnet deflect a bullet? (from James Bond movie)

Can a watch-sized electromagnet deflect a bullet? (from James Bond movie) Can a peon be blown away by a bullet? et' ay a bullet of a 0.06 k i ovin at a velocity of 300 /. And let' alo ay that it ebed itelf inide a peon. Could thi peon be thut back at hih peed (i.e. blown away)?

More information

15 Problem 1. 3 a Draw the equivalent circuit diagram of the synchronous machine. 2 b What is the expected synchronous speed of the machine?

15 Problem 1. 3 a Draw the equivalent circuit diagram of the synchronous machine. 2 b What is the expected synchronous speed of the machine? Exam Electrical Machine and Drive (ET4117) 6 November 009 from 9.00 to 1.00. Thi exam conit of 4 problem on 4 page. Page 5 can be ued to anwer problem quetion b. The number before a quetion indicate how

More information

Lecture Set 6 Brushless DC Machines

Lecture Set 6 Brushless DC Machines Lectue Set 6 Bushless DC Machines S.D. Sudhoff Sping 2018 Reading Chapte 8, Electomechanical Motion Devices, 2 nd Edition 2 A Bushless DC Machine 3 Sample Applications Low Powe: Disk dive motos Medium

More information

Content 5.1 Angular displacement and angular velocity 5.2 Centripetal acceleration 5.3 Centripetal force. 5. Circular motion.

Content 5.1 Angular displacement and angular velocity 5.2 Centripetal acceleration 5.3 Centripetal force. 5. Circular motion. 5. Cicula otion By Liew Sau oh Content 5.1 Angula diplaceent and angula elocity 5. Centipetal acceleation 5.3 Centipetal foce Objectie a) expe angula diplaceent in adian b) define angula elocity and peiod

More information

Overview Electrical Machines and Drives

Overview Electrical Machines and Drives Overview Electrical Machine and Drive 7-9 1: Introduction, Maxwell equation, magnetic circuit 11-9 1.-3: Magnetic circuit, Princile 14-9 3-4.: Princile, DC machine 18-9 4.3-4.7: DC machine and drive 1-9

More information

ELECTROSTATICS::BHSEC MCQ 1. A. B. C. D.

ELECTROSTATICS::BHSEC MCQ 1. A. B. C. D. ELETROSTATIS::BHSE 9-4 MQ. A moving electic chage poduces A. electic field only. B. magnetic field only.. both electic field and magnetic field. D. neithe of these two fields.. both electic field and magnetic

More information

A moving charged particle creates a magnetic field vector at every point in space except at its position.

A moving charged particle creates a magnetic field vector at every point in space except at its position. 1 Pat 3: Magnetic Foce 3.1: Magnetic Foce & Field A. Chaged Paticles A moving chaged paticle ceates a magnetic field vecto at evey point in space ecept at its position. Symbol fo Magnetic Field mks units

More information

Lecture 13. Rotational motion Moment of inertia

Lecture 13. Rotational motion Moment of inertia Lectue 13 Rotational motion Moment of inetia EXAM 2 Tuesday Mach 6, 2018 8:15 PM 9:45 PM Today s Topics: Rotational Motion and Angula Displacement Angula Velocity and Acceleation Rotational Kinematics

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

Electromagnetic Waves

Electromagnetic Waves Chapte 32 Electomagnetic Waves PowePoint Lectues fo Univesity Physics, Twelfth Edition Hugh D. Young and Roge A. Feedman Lectues by James Pazun Modified P. Lam 8_11_2008 Topics fo Chapte 32 Maxwell s equations

More information

16.1 Permanent magnets

16.1 Permanent magnets Unit 16 Magnetism 161 Pemanent magnets 16 The magnetic foce on moving chage 163 The motion of chaged paticles in a magnetic field 164 The magnetic foce exeted on a cuent-caying wie 165 Cuent loops and

More information

V V The circumflex (^) tells us this is a unit vector

V V The circumflex (^) tells us this is a unit vector Vecto Vecto have Diection and Magnitude Mike ailey mjb@c.oegontate.edu Magnitude: V V V V x y z vecto.pptx Vecto Can lo e Defined a the oitional Diffeence etween Two oint 3 Unit Vecto have a Magnitude

More information

Formula Formula symbols Units. s = F A. e = x L. E = s ε. k = F δ. G = t γ. e = at. maximum load original cross sectional area. s M E = = N/m.

Formula Formula symbols Units. s = F A. e = x L. E = s ε. k = F δ. G = t γ. e = at. maximum load original cross sectional area. s M E = = N/m. A Lit of foulae fo ecanical engineeing pinciple Foula Foula ybol Unit Ste Stain applied foce co ectionalaea cange in lengt oiginal lengt F A e x L Young odulu of elaticity te tain Stiffne foce extenion

More information

SPEED CONTROL OF LINEAR INDUCTION MOTOR USING DTFC METHOD CONSIDERING END-EFFECT PHENOMENON

SPEED CONTROL OF LINEAR INDUCTION MOTOR USING DTFC METHOD CONSIDERING END-EFFECT PHENOMENON Intenational Jounal on Technical Phyical Poble of Engineeing (IJTPE) Publihed by Intenational Oganization of IOTPE ISSN 77-358 IJTPE Jounal www.iote.co ijte@iote.co Decebe 14 Iue 1 Volue 6 Nube 4 Page

More information

Ch 30 - Sources of Magnetic Field! The Biot-Savart Law! = k m. r 2. Example 1! Example 2!

Ch 30 - Sources of Magnetic Field! The Biot-Savart Law! = k m. r 2. Example 1! Example 2! Ch 30 - Souces of Magnetic Field 1.) Example 1 Detemine the magnitude and diection of the magnetic field at the point O in the diagam. (Cuent flows fom top to bottom, adius of cuvatue.) Fo staight segments,

More information

Electrostatics (Electric Charges and Field) #2 2010

Electrostatics (Electric Charges and Field) #2 2010 Electic Field: The concept of electic field explains the action at a distance foce between two chaged paticles. Evey chage poduces a field aound it so that any othe chaged paticle expeiences a foce when

More information

Static equilibrium requires a balance of forces and a balance of moments.

Static equilibrium requires a balance of forces and a balance of moments. Static Equilibium Static equilibium equies a balance of foces and a balance of moments. ΣF 0 ΣF 0 ΣF 0 ΣM 0 ΣM 0 ΣM 0 Eample 1: painte stands on a ladde that leans against the wall of a house at an angle

More information

6.641 Electromagnetic Fields, Forces, and Motion Spring 2005

6.641 Electromagnetic Fields, Forces, and Motion Spring 2005 MIT OpenouseWae http://ocw.mit.edu 6.641 Electomagnetic Fields, Foces, and Motion Sping 2005 Fo infomation about citing these mateials o ou Tems of Use, visit: http://ocw.mit.edu/tems. 6.641 Electomagnetic

More information

rad / sec min rev 60sec. 2* rad / sec s

rad / sec min rev 60sec. 2* rad / sec s EE 559, Exa 2, Spig 26, D. McCalley, 75 iute allowed. Cloed Book, Cloed Note, Calculato Peitted, No Couicatio Device. (6 pt) Coide a.5 MW, 69 v, 5 Hz, 75 p DFG wid eegy yt. he paaete o the geeato ae give

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

( ) ( )( ) ˆ. Homework #8. Chapter 27 Magnetic Fields II.

( ) ( )( ) ˆ. Homework #8. Chapter 27 Magnetic Fields II. Homewok #8. hapte 7 Magnetic ields. 6 Eplain how ou would modif Gauss s law if scientists discoveed that single, isolated magnetic poles actuall eisted. Detemine the oncept Gauss law fo magnetism now eads

More information

3 Performance estimation for a three-phase PM synchronous machine

3 Performance estimation for a three-phase PM synchronous machine Assignent 3-9 3 Pefoance estiation fo a thee-phase PM synchonous achine The goal of the thid assignent is to get expeience of equivalent cicuit ethod (ECM) used fo ough sizing of a sevo oto. The estiated

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

PMSM. Mechanical Design

PMSM. Mechanical Design PMSM Indutial Electical Engineeing and Autoation Lund Univeity, Sweden Mechanical Deign Indutial Electical Engineeing and Autoation 1 Indutial Electical Engineeing and Autoation y i b i β Matheatical Model

More information

(a) Calculate the apparent weight of the student in the first part of the journey while accelerating downwards at 2.35 m s 2.

(a) Calculate the apparent weight of the student in the first part of the journey while accelerating downwards at 2.35 m s 2. Chapte answes Heineann Physics 1 4e Section.1 Woked exaple: Ty youself.1.1 CALCULATING APPARENT WEIGHT A 79.0 kg student ides a lift down fo the top floo of an office block to the gound. Duing the jouney

More information

A New Type of Capacitive Machine

A New Type of Capacitive Machine Enegy and Powe Engineeing, 015, 7, 31-40 Published Online Febuay 015 in SciRes. http://www.scip.og/jounal/epe http://dx.doi.og/10.436/epe.015.7003 A New Type of Capacitive achine Aie Shenkan, Saad Tapuchi,

More information

FI 2201 Electromagnetism

FI 2201 Electromagnetism FI 2201 Electomagnetism Alexande A. Iskanda, Ph.D. Physics of Magnetism and Photonics Reseach Goup Electodynamics ELETROMOTIVE FORE AND FARADAY S LAW 1 Ohm s Law To make a cuent flow, we have to push the

More information

Magnetic Field. Conference 6. Physics 102 General Physics II

Magnetic Field. Conference 6. Physics 102 General Physics II Physics 102 Confeence 6 Magnetic Field Confeence 6 Physics 102 Geneal Physics II Monday, Mach 3d, 2014 6.1 Quiz Poblem 6.1 Think about the magnetic field associated with an infinite, cuent caying wie.

More information

Spiral Magnetic Gradient Motor Using Axial Magnets

Spiral Magnetic Gradient Motor Using Axial Magnets Spial Magnetic Gadient Moto Using Axial Magnets Cedit: Tom Schum fo spial stato constuction Thomas Valone, PhD, PE Integity Reseach Institute Pape on Science Diect, Physics Gadients Ae Used fo All Powe

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

$ i. !((( dv vol. Physics 8.02 Quiz One Equations Fall q 1 q 2 r 2 C = 2 C! V 2 = Q 2 2C F = 4!" or. r ˆ = points from source q to observer

$ i. !((( dv vol. Physics 8.02 Quiz One Equations Fall q 1 q 2 r 2 C = 2 C! V 2 = Q 2 2C F = 4! or. r ˆ = points from source q to observer Physics 8.0 Quiz One Equations Fall 006 F = 1 4" o q 1 q = q q ˆ 3 4" o = E 4" o ˆ = points fom souce q to obseve 1 dq E = # ˆ 4" 0 V "## E "d A = Q inside closed suface o d A points fom inside to V =

More information

Unit 7: Sources of magnetic field

Unit 7: Sources of magnetic field Unit 7: Souces of magnetic field Oested s expeiment. iot and Savat s law. Magnetic field ceated by a cicula loop Ampèe s law (A.L.). Applications of A.L. Magnetic field ceated by a: Staight cuent-caying

More information

Course Updates. Reminders: 1) Assignment #8 will be able to do after today. 2) Finish Chapter 28 today. 3) Quiz next Friday

Course Updates. Reminders: 1) Assignment #8 will be able to do after today. 2) Finish Chapter 28 today. 3) Quiz next Friday Couse Updates http://www.phys.hawaii.edu/~vane/phys272-sp10/physics272.html Remindes: 1) Assignment #8 will be able to do afte today 2) Finish Chapte 28 today 3) Quiz next Fiday 4) Review of 3 ight-hand

More information

Magnetic Dipoles Challenge Problem Solutions

Magnetic Dipoles Challenge Problem Solutions Magnetic Dipoles Challenge Poblem Solutions Poblem 1: Cicle the coect answe. Conside a tiangula loop of wie with sides a and b. The loop caies a cuent I in the diection shown, and is placed in a unifom

More information

RE 11.e Mon. Review for Final (1-11) HW11: Pr s 39, 57, 64, 74, 78 Sat. 9 a.m. Final Exam (Ch. 1-11)

RE 11.e Mon. Review for Final (1-11) HW11: Pr s 39, 57, 64, 74, 78 Sat. 9 a.m. Final Exam (Ch. 1-11) Mon. Tue. We. ab i..4-.6, (.) ngula Momentum Pincile & Toque.7 -.9, (.) Motion With & Without Toque Rotation Coue Eval.0 Quantization, Quiz RE.c EP RE. RE.e Mon. Review fo inal (-) HW: P 9, 57, 64, 74,

More information

Calculate the electric potential at B d2=4 m Calculate the electric potential at A d1=3 m 3 m 3 m

Calculate the electric potential at B d2=4 m Calculate the electric potential at A d1=3 m 3 m 3 m MTE : Ch 13 5:3-7pm on Oct 31 ltenate Exams: Wed Ch 13 6:3pm-8:pm (people attending the altenate exam will not be allowed to go out of the oom while othes fom pevious exam ae still aound) Thu @ 9:-1:3

More information

Tidal forces. m r. m 1 m 2. x r 2. r 1

Tidal forces. m r. m 1 m 2. x r 2. r 1 Tidal foces Befoe we look at fee waves on the eath, let s fist exaine one class of otion that is diectly foced: astonoic tides. Hee we will biefly conside soe of the tidal geneating foces fo -body systes.

More information

( ) Physics 1401 Homework Solutions - Walker, Chapter 9

( ) Physics 1401 Homework Solutions - Walker, Chapter 9 Phyic 40 Conceptual Quetion CQ No Fo exaple, ey likely thee will be oe peanent deoation o the ca In thi cae, oe o the kinetic enegy that the two ca had beoe the colliion goe into wok that each ca doe on

More information

Induction Motor Drive

Induction Motor Drive Induction Motor Drive 1. Brief review of IM theory.. IM drive characteritic with: Variable input voltage Variable rotor reitance Variable rotor power Variable voltage and variable frequency, VVVF drive

More information

An Optimized Ride through Protection Method for DFIG Wind Turbine during Asymmetrical Disturbance

An Optimized Ride through Protection Method for DFIG Wind Turbine during Asymmetrical Disturbance 578 J. Baic. Appl. Sci. Re., ()578-58,, TextRoad Publication ISSN 9- Jounal of Baic and Applied Scientific Reeach www.textoad.co An Optiized Ride though Potection Method fo DFIG Wind Tubine duing Ayetical

More information

Impulse and Momentum

Impulse and Momentum Impule and Momentum 1. A ca poee 20,000 unit of momentum. What would be the ca' new momentum if... A. it elocity wee doubled. B. it elocity wee tipled. C. it ma wee doubled (by adding moe paenge and a

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

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

( ) rad ( 2.0 s) = 168 rad

( ) rad ( 2.0 s) = 168 rad .) α 0.450 ω o 0 and ω 8.00 ω αt + ω o o t ω ω o α HO 9 Solution 8.00 0 0.450 7.8 b.) ω ω o + αδθ o Δθ ω 8.00 0 ω o α 0.450 7. o Δθ 7. ev.3 ev π.) ω o.50, α 0.300, Δθ 3.50 ev π 7π ev ω ω o + αδθ o ω ω

More information

MAGNETIC FIELD AROUND TWO SEPARATED MAGNETIZING COILS

MAGNETIC FIELD AROUND TWO SEPARATED MAGNETIZING COILS The 8 th Intenational Confeence of the Slovenian Society fo Non-Destuctive Testing»pplication of Contempoay Non-Destuctive Testing in Engineeing«Septembe 1-3, 5, Potoož, Slovenia, pp. 17-1 MGNETIC FIELD

More information

Homework Set 4 Physics 319 Classical Mechanics. m m k. x, x, x, x T U x x x x l 2. x x x x. x x x x

Homework Set 4 Physics 319 Classical Mechanics. m m k. x, x, x, x T U x x x x l 2. x x x x. x x x x Poble 78 a) The agangian i Hoewok Set 4 Phyic 319 Claical Mechanic k b) In te of the cente of a cooinate an x x1 x x1 x xc x x x x x1 xc x xc x x x x x1 xc x xc x, x, x, x T U x x x x l 1 1 1 1 1 1 1 1

More information

This is because magnetic lines of force are closed lines and free magnetic poles do not exist.

This is because magnetic lines of force are closed lines and free magnetic poles do not exist. 1 Ch: lectromagnetic nduction Class X Physics Chater Notes Magnetic Flux Magnetic flux through a lane of area da laced in a uniform magnetic field B = B.dA f the surface is closed, then B. d.a 0 This is

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

Fields and Waves I Spring 2005 Homework 8. Due: 3 May 2005

Fields and Waves I Spring 2005 Homework 8. Due: 3 May 2005 Fields and Waves I Sping 005 Homewok 8 Tansmission Lines Due: 3 May 005. Multiple Choice (6) a) The SWR (standing wave atio): a) is a measue of the match between the souce impedance and line impedance

More information

Physics 2020, Spring 2005 Lab 5 page 1 of 8. Lab 5. Magnetism

Physics 2020, Spring 2005 Lab 5 page 1 of 8. Lab 5. Magnetism Physics 2020, Sping 2005 Lab 5 page 1 of 8 Lab 5. Magnetism PART I: INTRODUCTION TO MAGNETS This week we will begin wok with magnets and the foces that they poduce. By now you ae an expet on setting up

More information

Induction machines and drives

Induction machines and drives Chapte 1 Induction machines and dives Table of Contents 1.1 Induction machine basics... 1. Machine model and analysis... 6 1.3 No load and blocked oto tests... 15 1.4 Induction machine moto dives... 16

More information

Static Electric Fields. Coulomb s Law Ε = 4πε. Gauss s Law. Electric Potential. Electrical Properties of Materials. Dielectrics. Capacitance E.

Static Electric Fields. Coulomb s Law Ε = 4πε. Gauss s Law. Electric Potential. Electrical Properties of Materials. Dielectrics. Capacitance E. Coulomb Law Ε Gau Law Electic Potential E Electical Popetie of Mateial Conducto J σe ielectic Capacitance Rˆ V q 4πε R ρ v 2 Static Electic Field εe E.1 Intoduction Example: Electic field due to a chage

More information

Rigid Body Dynamics 2. CSE169: Computer Animation Instructor: Steve Rotenberg UCSD, Winter 2018

Rigid Body Dynamics 2. CSE169: Computer Animation Instructor: Steve Rotenberg UCSD, Winter 2018 Rigid Body Dynamics 2 CSE169: Compute Animation nstucto: Steve Rotenbeg UCSD, Winte 2018 Coss Poduct & Hat Opeato Deivative of a Rotating Vecto Let s say that vecto is otating aound the oigin, maintaining

More information

Ch 11 Particulate suspensions

Ch 11 Particulate suspensions Ch 11 Paticulate upenion Iue Stability (dipeion) edientation igation wall lip Had phee Only igid epulion peent when paticle coe into contact Zeo hea vicoity ( 1+. φ) 5 1+.5φ + 6.φ d.5 ( φ) dφ exp( 5φ /

More information

Chapter 28: Magnetic Field and Magnetic Force. Chapter 28: Magnetic Field and Magnetic Force. Chapter 28: Magnetic fields. Chapter 28: Magnetic fields

Chapter 28: Magnetic Field and Magnetic Force. Chapter 28: Magnetic Field and Magnetic Force. Chapter 28: Magnetic fields. Chapter 28: Magnetic fields Chapte 8: Magnetic fiels Histoically, people iscoe a stone (e 3 O 4 ) that attact pieces of ion these stone was calle magnets. two ba magnets can attact o epel epening on thei oientation this is ue to

More information

Forging Analysis - 2. ver. 1. Prof. Ramesh Singh, Notes by Dr. Singh/ Dr. Colton

Forging Analysis - 2. ver. 1. Prof. Ramesh Singh, Notes by Dr. Singh/ Dr. Colton Foging Analysis - ve. 1 Pof. ames Sing, Notes by D. Sing/ D. Colton 1 Slab analysis fictionless wit fiction ectangula Cylindical Oveview Stain adening and ate effects Flas edundant wo Pof. ames Sing, Notes

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

Section 25 Describing Rotational Motion

Section 25 Describing Rotational Motion Section 25 Decibing Rotational Motion What do object do and wh do the do it? We have a ve thoough eplanation in tem of kinematic, foce, eneg and momentum. Thi include Newton thee law of motion and two

More information

Rotational Motion. Lecture 6. Chapter 4. Physics I. Course website:

Rotational Motion. Lecture 6. Chapter 4. Physics I. Course website: Lectue 6 Chapte 4 Physics I Rotational Motion Couse website: http://faculty.uml.edu/andiy_danylov/teaching/physicsi Today we ae going to discuss: Chapte 4: Unifom Cicula Motion: Section 4.4 Nonunifom Cicula

More information

THE MAGNETIC FIELD. This handout covers: The magnetic force between two moving charges. The magnetic field, B, and magnetic field lines

THE MAGNETIC FIELD. This handout covers: The magnetic force between two moving charges. The magnetic field, B, and magnetic field lines EM 005 Handout 7: The Magnetic ield 1 This handout coes: THE MAGNETIC IELD The magnetic foce between two moing chages The magnetic field,, and magnetic field lines Magnetic flux and Gauss s Law fo Motion

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