Switching FOC Method for Vector Control of Single-Phase Induction Motor Drives

Similar documents
MODELING AND SIMULATION OF SENSORLESS CONTROL OF PMSM WITH LUENBERGER ROTOR POSITION OBSERVER AND SUI PID CONTROLLER

Load Equations. So let s look at a single machine connected to an infinite bus, as illustrated in Fig. 1 below.

Applications of Lagrange Equations

Rectification and Depth Computation

J. Milli Monfared K. Abbaszadeh E. Fallah Assistant Professor P.H.D Student P.H.D Student

Evaluation of Back-EMF Estimators for Sensorless Control of Permanent Magnet Synchronous Motors


EFFICIENCY OPTIMIZATION OF INDUCTION MOTOR DRIVES

) 3. 3 i. 2π ) 3. sin(

PF nce. Conferen. is, FRANC. ectronics Pari. ber 6-10, 2. ustrial Ele. Novemb. EEE Indu

Dynamic Modelling and Simulation of Five Phase Induction Motor

Homework: Due

CERTAIN RESULTS ON TIGHTENED-NORMAL-TIGHTENED REPETITIVE DEFERRED SAMPLING SCHEME (TNTRDSS) INDEXED THROUGH BASIC QUALITY LEVELS

5- Scattering Stationary States

Localisation of partial discharges sources using acoustic transducers arrays

A New Bargaining Game Model for Measuring Performance of Two-Stage Network Structures

Modeling and implementation of vector control for Induction motor Drive

Simulation of Indirect Vector Controlled Induction Motor Drive

Fuzzy Logic Speed Control of Three Phase Induction Motor Drive

Electric Machines. Leila Parsa Rensselaer Polytechnic Institute

E F. and H v. or A r and F r are dual of each other.

Analysis of Stresses and Strains in a Rotating Homogeneous Thermoelastic Circular Disk by using Finite Element Method

( V ) 0 in the above equation, but retained to keep the complete vector identity for V in equation.

9/12/2013. Microelectronics Circuit Analysis and Design. Modes of Operation. Cross Section of Integrated Circuit npn Transistor

Structure and Features

The angle between L and the z-axis is found from

High Performance Speed Control of Single-Phase Induction Motors Using Switching Forward and Backward EKF Strategy

ILSim A compact simulation tool for interferometric lithography

CIVL 7/ D Boundary Value Problems - Axisymmetric Elements 1/8

Novel Axial Flux Brushless Resolver Analysis and Optimization using 3D Finite Element and D-Q Model Method

PO with Modified Surface-normal Vectors for RCS calculation of Scatterers with Edges and Wedges

Inertia identification based on adaptive interconnected Observer. of Permanent Magnet Synchronous Motor

III. Electromechanical Energy Conversion

A Comparative Study and Analysis of an Optimized Control Strategy for the Toyota Hybrid System

Systemic design and modelling of a coiled rotor synchronous motor dedicated to electric traction

for the magnetic induction at the point P with coordinate x produced by an increment of current

Variable Structure Control ~ Motor Control

Period vs. Length of a Pendulum

Week 11: Differential Amplifiers

Analysis of a M/G/1/K Queue with Vacations Systems with Exhaustive Service, Multiple or Single Vacations

FFT Based Spectrum Analysis of Three Phase Signals in Park (d-q) Plane

Statics. Consider the free body diagram of link i, which is connected to link i-1 and link i+1 by joint i and joint i-1, respectively. = r r r.

CDS 101: Lecture 7.1 Loop Analysis of Feedback Systems

Induction Motor Speed Control using Fuzzy Logic Controller

Multi-linear Systems and Invariant Theory. in the Context of Computer Vision and Graphics. Class 4: Mutli-View 3D-from-2D. CS329 Stanford University

MODELING AND CONTROL OF DOUBLY FED INDUCTION GENERATOR FOR WIND POWER

Physics 111. Lecture 38 (Walker: ) Phase Change Latent Heat. May 6, The Three Basic Phases of Matter. Solid Liquid Gas

Sliding Mode Control of Surface-Mount Permanent-Magnet Synchronous Motor Based on Error Model with Unknown Load

Unit 3: Transistor at Low Frequencies

3. A Review of Some Existing AW (BT, CT) Algorithms

Massachusetts Institute of Technology Introduction to Plasma Physics

Instruction Execution

Electromagnetics: The Smith Chart (9-6)

Physics 240: Worksheet 15 Name

(8) Gain Stage and Simple Output Stage

Particle Swarm Optimized Fuzzy Controller for Indirect Vector Control of Multilevel Inverter Fed Induction Motor

Molecules and electronic, vibrational and rotational structure

Guo, James C.Y. (1998). "Overland Flow on a Pervious Surface," IWRA International J. of Water, Vol 23, No 2, June.

Mitigating Balanced and Unbalanced Voltage Sag Via Shunt-Connected Voltage Source Convertor (VSC) by using Double Vector Controller

Extinction Ratio and Power Penalty

Space Vector Double Frame Field Oriented Control of Six Phase Induction Motors

6. Introduction to Transistor Amplifiers: Concepts and Small-Signal Model

Basic Electrical Engineering for Welding [ ] --- Introduction ---

Loss Minimization Control for Doubly-Fed Induction Generators in Variable Speed Wind Turbines

( r) E (r) Phasor. Function of space only. Fourier series Synthesis equations. Sinusoidal EM Waves. For complex periodic signals

Controlling Swarms of Bandit Inspector Spacecraft

Hydrogen atom. Energy levels and wave functions Orbital momentum, electron spin and nuclear spin Fine and hyperfine interaction Hydrogen orbitals

24 th International Conference on Electricity Distribution Glasgow, June Paper 0045 ABSTRACT INTRODUCTION

Grid Transformations for CFD Calculations

Using Complex Numbers in Circuit Analysis and Review of the Algebra of Complex Numbers

International Journal of Mechanical Engineering and Applications

3. MODELING OF PARALLEL THREE-PHASE CURRENT-UNIDIRECTIONAL CONVERTERS 3. MODELING OF PARALLEL THREE-PHASE CURRENT-

Speed Control of Direct Torque Controlled Induction Motor By using PI, Anti-Windup PI and Fuzzy Logic Controller

Dynamics of Rigid Bodies

The Forming Theory and the NC Machining for The Rotary Burs with the Spectral Edge Distribution

The Random Phase Approximation:

FREQUENCY DETECTION METHOD BASED ON RECURSIVE DFT ALGORITHM

N-Channel 20-V (D-S) MOSFET

NEW ATTACKS ON TAKAGI CRYPTOSYSTEM

SYMMETRICAL COMPONENTS

UGC POINT LEADING INSTITUE FOR CSIR-JRF/NET, GATE & JAM. are the polar coordinates of P, then. 2 sec sec tan. m 2a m m r. f r.

Chapter 3 Binary Image Analysis. Comunicação Visual Interactiva

The Fourier Transform

Rotary motion

CHAPTER 13. Exercises. E13.1 The emitter current is given by the Shockley equation:

Signal Circuit and Transistor Small-Signal Model

Studying the Steady State Performance Characteristics of Induction Motor with Field Oriented Control Comparing to Scalar Control

( ) = ( ) + ( 0) ) ( )

Diffraction. Diffraction: general Fresnel vs. Fraunhofer diffraction Several coherent oscillators Single-slit diffraction. Phys 322 Lecture 28

II.3. DETERMINATION OF THE ELECTRON SPECIFIC CHARGE BY MEANS OF THE MAGNETRON METHOD

multipath channel Li Wei, Youyun Xu, Yueming Cai and Xin Xu

Rigid Bodies: Equivalent Systems of Forces

Physics Exam II Chapters 25-29

ORBITAL TO GEOCENTRIC EQUATORIAL COORDINATE SYSTEM TRANSFORMATION. x y z. x y z GEOCENTRIC EQUTORIAL TO ROTATING COORDINATE SYSTEM TRANSFORMATION

APPENDIX H CONSTANT VOLTAGE BEHIND TRANSIENT REACTANCE GENERATOR MODEL

( ) + is the distance from the point of interest to the location of the charge q i

Performance Improvement Technique for Induction Motor Driven by a Matrix Converter under Abnormal Input Conditions

A Novel Method for Vector Control of Three-Phase Induction Motor under Open-Phase Fault

Noise in electronic components.

Transcription:

Intnatonal Jounal of Elctcal an Comput Engnng (IJECE) Vol. 6, No., Apl 16, pp. 474~483 ISSN: 88-878, DOI: 1.11591/jc.6.9146 474 Swtchng FOC tho fo Vcto Contol of Sngl-Phas Inucton oto Ds ohamma Jannat*, Nk Rumz Nk Is*, oh Juna Abul Azz*, Tol Sutkno**,. Ghanba*** * UT-PROTON Futu D aboatoy, Faculty of Elctcal Engnng, Unst Tknolog alaysa, 8131 Skua, Joho Bahu, alaysa ** Dpatmnt of Elctcal Engnng, Faculty of Inustal Tchnology, Unstas Ahma Dahlan, Yogyakata 55164, Inonsa *** Dpatmnt of Elctcal Engnng, Alaba Katoul Banch, Islamc Aza Unsty, Alaba Katoul, Ian Atcl Info Atcl hstoy: Rc Oct 1, 15 Rs Dc 8, 15 Accpt Jan 1, 16 Kywo: AC Ds Hgh pfomanc applcatons Sngl-phas nucton moto Swtchng FOC Vcto contol ABSTRACT Ths pap poposs a nol cto contol mtho bas on Roto flux Fl-Ont Contol (RFOC) fo sngl-phas Inucton oto (I) s. It s shown that n a otatng fnc fam, th sngl-phas I uatons can b spaat nto fowa an backwa uatons wth balanc stuctus. In o to accommoat fo ths fowa an backwa uatons, a systm consstng of two RFOCs that a swtch ntchangably, s popos. Altnatly, ths two RFOC algothms can b smplf as a sngl FOC algothm. Th analyss, contoll sgn an smulaton of th popos tchnu show that t s fasbl fo sngl-phas I fo hgh pfomanc applcatons. Copyght 16 Insttut of Aanc Engnng an Scnc. All ghts s. Cosponng Autho: ohamma Jannat, UT-PROTON Futu D aboatoy, Faculty of Elctcal Engnng, Unst Tknolog alaysa, 8131 Skua, Joho Bahu, alaysa. Emal: jannatm94@yahoo.com 1. INTRODUCTION Sngl-phas Inucton oto (I) s on of th most applcabl lctcal machns whch a us n low pow omstc an nustal applcatons. Ths lctcal moto can b us n acuum clans, washs, compssos, fans an tc. Gnally, a sngl-phas I has two man an auxlay wnngs an ts opaton ns on o two capactos. To guaant th ffcnt us of ngy, th nstgaton of ffnt sngl-phas I schms ha bn ncas by sachs. In ths s th sngl-phas I, wthout capacto, s tat as an asymmtc -phas I [1]. Dffnt cont topologs ha bn popos to supply sngl-phas machn, fo xampl, on-lg nt [], -lg nt [1], [3] 3-lg nt [4], [5] an 4-lg nt [6]. Ths pap nstgats th us of -lg nt as shown n Fgu 1 fo fng th sngl-phas I. Ths confguaton s ncat fo hgh pfomanc applcatons [1], [3] (It shoul b pont out that th focus gn h s on th tal analyss an sgn of th cto contol statgy fo sngl-phas I s). Fl-Ont Contol (FOC) mtho s wly us fo mplmntng hgh pfomanc cto contol of sngl-phas I s. Ths mtho has bn ncasngly aopt as th stana contol tchnu fo nustal mans [1], [3], [7]-[16]. On of th man awbacks n th psnt FOC mthos to contol sngl-phas I s s usng th supposton of ( / ) = s / ( s,,, ncat th stato an oto - axs slf an mutual Jounal hompag: http://asjounal.com/onln/nx.php/ijece

475 ISSN: 88-878 nuctancs) [1], [3], [7]-[15]. It can b not that fo smplfyng cto contol uatons n sngl-phas I th supposton of ( / ) = s / s us. It was shown n [16] usng ths assumpton s flct n th tou spons of th sngl-phas I systm. In [16], a mtho fo Inct Roto flux FOC (IRFOC) of sngl-phas I wthout usng ( / ) = s / has bn psnt. How, th ntouc mtho n [16] s xtmly pns on moto paamts aatons. Ths stuy shows th sngl-phas I can b mol as two balanc ccuts (fowa an backwa ccuts). Bas on ths smplfyng, a nol cto contol mtho fo sngl-phas I bas on FOC algothm an wthout usng ( / ) = s / s psnt (swtchng FOC). Ths pap s oganz as follows: Aft ntoucton n scton 1, n scton, - mol of sngl-phas I s psnt. Nxt, scton 3 scbs th lopmnt of th FOC algothm, follow by psntng popos swtchng FOC schm fo cto contol of sngl-phas I s. Th pfomanc of th psnt mtho s analyz an chck usng atlab/smulnk softwa n scton 4 an scton 5 conclus th pap. Fgu 1. Sngl-phas I systm (-lg nt). ODEING OF SINGE-PHASE I Nglctng th co satuaton, th - mol of th sngl-phas I n th statonay fnc fam (supscpt s ) can b shown as th followng uatons [15]: (1) In (1), s s, s a th stato - axs oltags, s s, s a th stato - axs cunts, s, s a th oto - axs cunts, λ s s, λ s a th stato - axs fluxs an λ s, λ s a th oto - axs fluxs. s,, ncat th stato an oto - axs sstancs. s,,,, not th stato an oto - axs slf an mutual nuctancs. s th moto sp. τ, τ l a lctomagntc tou an loa tou. J, F a th momnt of nta an scous fcton coffcnt spctly. 3. SWITCHING FOC ETHOD FOR VECTOR CONTRO OF SINGE-PHASE I In ths scton, a nol mtho fo cto contol of sngl-phas I s bas on IRFOC s popos. In th RFOC statgy t s ncssay that th machn uatons tansf to th otatng fnc IJECE Vol. 6, No., Apl 16 : 474 483

IJECE ISSN: 88-878 Swtchng FOC tho fo Vcto Contol of Sngl-Phas Inucton oto Ds (. Jannat) 476 fam. Fo ths pupos, th tansfomaton matx as shown n uaton () s appl to th machn uatons [17]: T s sn sn () In (), supscpt ncats that th uatons a n th otatng fnc fam. oo, θ s th angl btwn th statonay an otatng fnc fams. By applyng () to th uatons of th sngl-phas I (uatons (1)), uatons (3a) an (3b) a obtan: s s s s s s s s s s s s s s s s s t t t t t t t t t t t t t t (3a) s s s s s s s sn sn sn sn sn sn sn sn (3b) In (3a), ω s th angula locty of th oto fl ont fnc fam. As can b sn, n gnal, uaton (3a) nclus two tms (fowa tm: supscpt + an backwa tm: supscpt - ). Each tm psnts a balanc uaton wh otats n th fowa o backwa cton as shown n Fgu.

477 ISSN: 88-878 Fgu. Fowa, backwa an statonay fnc fams ( + : fowa, - : backwa an s : statonay) As can b sn fom (3a), th stuctu of th fowa an backwa tms s smla to th conntonal 3-phas I uatons. Th only ffnc btwn fowa tms an conntonal 3-phas I uatons s that, n th fowa tms th a: ( s + )/, ( s + )/ an ( + )/ but n th conntonal 3-phas I w ha: s, s = ls +1.5 ms an =1.5 ms. oo, th ffnc btwn backwa tms an conntonal 3-phas I uatons s that, n th backwa tms th a: ( s - )/, ( s - )/, ( - )/, =, = an th a - an - but n th conntonal 3-phas I w ha: s = ls +1.5 ms, =1.5 ms,, an th a an. Th block agam of fowa an backwa IRFOC can b shown as Fgu 3 an Fgu 4 spctly. Fgu 3. Block agam of fowa IRFOC IJECE Vol. 6, No., Apl 16 : 474 483

IJECE ISSN: 88-878 478 Fgu 4. Block agam of backwa IRFOC Thfo, two lop IRFOC algothms wth two fowa an backwa cunts can b us fo cto contol of a sngl-phas I. Th block agam of th popos IRFOC fo sngl-phas I s s shown n Fgu 5. In Fgu 5, n o to altnatly swtch btwn th fowa an backwa stats, a swtch s us whby ths swtch wll conscutly chang postons n ach samplng tm. Fgu 5. Block agam of th popos IRFOC fo cto contol of sngl-phas I s In Fgu 5, to tansfomaton matx ([T s ]) s obtan as (4): 1 T (4) s 1 Swtchng FOC tho fo Vcto Contol of Sngl-Phas Inucton oto Ds (. Jannat)

479 ISSN: 88-878 Consuntly, to smplfy popos FOC n Fgu 5, sngl FOC algothm wth only changs n th moto paamts can b us fo cto contol of sngl-phas I s (s Fgu 6). Fgu 6. Block agam of th smplf popos FOC fo cto contol of sngl-phas I s 4. SIUATION RESUTS In ths scton, th smulaton sults bas on Fgu 5 an Fgu 6 s ca out to alat th popos contol statgy. A.5Hp sngl-phas I s n by a -lg oltag souc nt. Th smulaton nstgaton s manly focus on th moto sp an tou sponss. Th moto paamts a shown n Tabl 1. Tabl 1. Ratngs an paamts of th sngl-phas I Voltag 9V Funcy (f) 6Hz No. of Pols 4 Pow.5Hp s 7.14 as. a.177h 4.1 s.1885h as.1844h J.146kg.m F.N.m.s Fgu 7 shows th smulaton sults of th popos contoll fo a tapzoal fnc sp fom 5 pm to -5 pm. It s sn that th al sp sgnal a so accuat that haly can b stngush fom th ponng fnc sp sgnal. As can b sn fom Fgu 7, th maxmum sp o s about 1.5 pm. Th man an auxlay stato cunts an lctomagntc tou fo tapzoal fnc sp a also shown n Fgu 7. As shown fom Fgu 7, th snusoal fom of th stato cunts s mantan n th ffnt sp. oo, t can b sn that th lctomagntc tou has a uck spons wth no pulsatons. IJECE Vol. 6, No., Apl 16 : 474 483

IJECE ISSN: 88-878 48 Fgu 7. Smulaton sults of th popos contoll fo th tapzoal fnc sp fom top to bottom: Stato Cunts, Zoom of Stato Cunts, Sp, Sp Eo, Tou Swtchng FOC tho fo Vcto Contol of Sngl-Phas Inucton oto Ds (. Jannat)

481 ISSN: 88-878 Fgu 8 shows smulaton sults of th popos statgy fo cto contol of th sngl-phas I n th nomnal an zo fnc sps an un loa conton. In Fgu 8, th moto s unnng at th fnc sp of pm. Thn at t=3s a stp chang of 18pm s ntouc. In aton, at t=9s, a stp loa of 1.N.m s ntouc an at t=11s s mo. It s nt fom Fgu 8 that although at th momnt of applyng loa th s a small sp p but thn t s sto uckly. Bas on psnt sults n Fgu 8, usng popos systm, th maxmum sp o n nomnal sp an ung loa conton s about.4 pm. oo, th maxmum sp o n zo fnc sp s about.1 pm. As shown fom Fgu 8 th tou ncass accongly to nsu that th sp s mantan at 18pm. It can b sn fom Fgu 7 an Fgu 8 that th ynamc pfomanc of th popos contoll fo th sngl-phas I s xtmly accptabl. Fgu 8. Smulaton sults of th popos contoll n th nomnal an zo fnc sps an un loa conton fom top to bottom: Sp, Tou IJECE Vol. 6, No., Apl 16 : 474 483

IJECE ISSN: 88-878 48 Fgu 9 shows th compason btwn th stay-stat tou spons of th RFOC at th nomnal fnc sp by consng ( / ) = s / (.g., [1], [3], [7]-[15]) an wthout consng ( / ) = s / (swtchng FOC). ag tou ppl can b sn whn th assumpton ( / ) = s / s us. It s conclu n compason wth th pous schms fo RFOC of sngl-phas I s, th popos contoll n ths stuy gs btt pfomanc. Fgu 9. Smulaton sults of th compason btwn tou spons at th nomnal fnc sp; lft: assumng ( / ) = s /, ght: not assumng ( / ) = s /. 5. CONCUSION In ths pap, a cto contol statgy fo sngl-phas I s bas on Inct Roto flux Fl- Ont Contol s popos an tst. It was shown that th sngl-phas I uatons n th otatng fnc fam can b classf as th balanc uatons. Bas on ths smplcty, a nol cto contol mtho usng two lop IRFOC algothms was popos. As a sult, ths two algothms w smplf as sngl IRFOC algothm. Smulaton sults show that th popos swtchng FOC statgy woks wll o most sp angs an un loa conton. REFERENCES [1].R. Coa, t al., "Roto-flux-ont contol of a sngl-phas nucton moto ", IEEE Tansactons on Inustal Elctoncs, ol. 47, pp. 83-841, Aug.. []. Chomat an T.A. po, "Ajustabl-sp sngl-phas I wth uc numb of swtchs", IEEE Tansacton on Inustal Applcatons, ol. 39, pp. 819-85, ay/jun. 3. [3].B. Rosst Coêa, t al., "Vcto contol statgs fo sngl-phas nucton moto systms", IEEE Tansactons on Inustal Elctoncs, ol. 51, pp. 173-18, 4. [4].A. Jabba, t al., "Spac-cto moulaton n a two-phas nucton moto fo constant-pow opaton", IEEE Tansactons on Inustal Elctoncs, ol. 51, pp. 181-188, 4. [5]. Guo, t al., "A Sp Contoll fo a Two-Wnng Inucton oto Bas on Damtcal Inson", IEEE Tansacton on Inustal Applcatons, ol. 57, pp. 449-456, 1. [6] C. Young, t al., "Nw Int-Dn Dsgn an Contol tho fo Two-Phas Inucton oto Ds", IEE Pocngs on Elctc Pow Applcaton, ol. 143, pp. 458-466, 1996. [7] S. Rcy an S. Vaz-Zah, "Vcto contol of sngl-phas nucton machn wth maxmum tou opaton", In Pocngs of th IEEE Intnatonal Symposum on Inustal Elctoncs, ISIE 5, pp. 93-98, 5. [8]. Jml, t al., "Ral-tm mplmntaton of IRFOC fo sngl-phas nucton moto usng Spac DS 114 contol boa", Smulaton ollng Pactc an Thoy, ol. 17, pp. 171-18, 9. [9] H.B. Azza, t al., "Hgh pfomanc snsolss sp cto contol of SPI Ds wth on-ln stato sstanc stmaton", J. Smulat. Pactc Thoy, ol. 19, pp. 71-8, 11. [1] H. Bn Azza, t al., "Full-Dgtal Implmntaton of ISFOC fo Sngl-Phas Inucton oto D Usng Spac DS 114 Contol Boa", Intnatonal Rw of Elctcal Engnng, ol. 3, pp. 71-79, 8. [11] H.B. Azza, t al., "Implmntaton of Snsol Sp Contol fo Two-Phas Inucton oto D Usng ISFOC Statgy", Tansactons of Elctcal Engnng, ol. 35, pp. 63-74, Jun. 11. [1]. Jannat, t al., "Sp Snsolss Dct Roto Fl-Ont Contol of Sngl-Phas Inucton oto Usng Extn Kalman Flt", Intnatonal Jounal of Pow Elctoncs an D Systms (IJPEDS), ol. 4, pp. 43-438, 14. [13]. Jannat an E. Fallah, "A nw mtho fo sp snsolss cto contol of sngl-phas nucton moto usng Extn Kalman Flt", In 19th Ianan Confnc on Elctcal Engnng (ICEE), pp. 1-5, 11. [14]. Jannat, t al., "A nw mtho fo RFOC of sngl-phas nucton moto bas on otatonal tansfomatons", In 13 IEEE Stunt Confnc on Rsach an Dlopmnt (SCORD), pp. 15-, 13. Swtchng FOC tho fo Vcto Contol of Sngl-Phas Inucton oto Ds (. Jannat)

483 ISSN: 88-878 [15] D.H. Jang, "Poblms Incu n a Vcto-Contoll Sngl-Phas Inucton oto, an a Poposal fo a Vcto- Contoll Two-Phas Inucton oto as a Rplacmnt", IEEE Tansacton on Pow Elctoncs, ol. 8, pp. 56-536, Jan. 13. [16]. Jannat, t al., "An Exact ol fo Roto Fl-Ont Contol of Sngl-Phas Inucton otos", TEKONIKA Inonsan Jounal of Elctcal Engnng, ol. 1, pp. 511-51, 14. [17] P. Vas, "Vcto Contol of AC achns", Oxfo scnc publcaton, 199. IJECE Vol. 6, No., Apl 16 : 474 483