electromagnetic analysis of hysteresis synchronous motor based...

6
88 Iranian Journal of Electrical & Electronic Engineering, Vol. 9, No. 2, June 2013 Electromagnetic Analysis of Hysteresis Synchronous Motor Based on Complex Permeability Concept S. M. Mirimani*, A. Vahedi*, M. R. Ghazanchaei* and A. Baktash* Abstract: Hysteresis motor is self-starting synchronous motor that uses the hysteresis characteristics of magnetic materials to make torque. There are different methods to model this kind of motor and take into account the magnetic hysteresis characteristic of the rotor hysteresis ring. In this investigation the application of complex permeability concept is implemented to model the hysteresis loop and the hysteresis loop in inclined ellipse shape is adopted. To the best knowledge of the authors, this has not been studied before. Based on this concept, simulation of hysteresis motor in conventional configuration is done in order to obtain the output values of motor using 3D Finite Element Model (FEM). This 3D finite element model has high level accuracy and gives better insight of motor performance. Meanwhile, in order to validate the simulation results an experimental set-up is provided and the output values of typical motor are measured. It is shown that there is a good agreement between experimental and simulation results. Keywords: 3-D Finite Element Method, Complex Permeability, Hysteresis Motor. 1 Introduction1 Hysteresis motors have some good characteristics such as soft torque, simple construction with conventional three phase stator windings and self-starting torque. These advantages make the hysteresis motor suitable for some applications such as compressors, pumps, timing, and recording equipment. Although, hysteresis motor in contrast to Permanent Magnet Synchronous Motor (PMSM) has lower output power per unit volume, lower power factor and efficiency and higher magnetizing current [1], But limitation such as zero starting torque, needs to auxiliary winding for line starting and closed loop control systems have confined the usage of PMSM for special applications. Hysteresis motor overcomes these limitations by using the hysteresis characteristics of the magnetic materials. It should be noted that the magnetic characteristics of the motor could be easily affected by hysteresis material, structural dimensions and winding distributions [2]. To have a good designing for these parameters of machine, it would be desirable to adopt an accurate model for the motor. Analytical methods have been used to study the hysteresis motors frequently. However, these methods are very complex when accurate evaluation of the saturation effects, and Iranian Journal of Electrical & Electronic Engineering, 2013. Paper first received 9 Jan. 2012 and in revised form 13 Jan. 2013. * The Authors are with the Center of Excellence for Power Systems Automation and Operation, Iran University of Science & Technology (IUST), Tehran, Iran. E-mails: [email protected], [email protected], [email protected] and [email protected]. stator and rotor slotting is needed. These problems are overcome by applying numerical methods. Finite element method allows a precise analysis of magnetic devices taking into account geometric details and magnetic nonlinearity. In previous studies, 2D finite element (FEM) techniques for simulating of hysteresis motors have been developed [2-4]. In this paper, the performance characteristics of hysteresis motor through a 3D finite element analysis (FEA) are provided. 3D model has high level of accuracy and gives us a better insight of motor characteristics. Such simulation is based upon Maxwell’s field equations considering the case of a circumferential flux type machine at synchronous speed. There are mainly three methods to take into account the magnetic hysteresis of the rotor hysteresis ring. One is based on the approximation of a parallelogram [5] and the second one is the Preisach model [2, 6, 7] and the last one is based on elliptical model [8]. In this study, the application of complex permeability concept is implemented in order to model the hysteresis loop in the shape of inclined ellipse. To the best knowledge of the authors, this has not been studied before. Finally, in order to validate the simulation an experimental set-up is provided and output characteristics of conventional hysteresis motor are measured. There exists a reasonably close agreement between the FEM results and experimental set-up output characteristics. Furthermore, this study can be used in the design approach and precise analysis of hysteresis motors. Downloaded from ijeee.iust.ac.ir at 5:49 IRST on Wednesday December 30th 2020

Upload: others

Post on 09-Sep-2020

4 views

Category:

Documents


0 download

TRANSCRIPT

Page 1: Electromagnetic Analysis of Hysteresis Synchronous Motor Based …ijeee.iust.ac.ir/article-1-481-en.pdf · hysteresis motor through a 3D finite element analysis (FEA) are provided

88 Iranian Journal of Electrical & Electronic Engineering, Vol. 9, No. 2, June 2013

Electromagnetic Analysis of Hysteresis Synchronous Motor Based on Complex Permeability Concept S. M. Mirimani*, A. Vahedi*, M. R. Ghazanchaei* and A. Baktash*

Abstract: Hysteresis motor is self-starting synchronous motor that uses the hysteresis characteristics of magnetic materials to make torque. There are different methods to model this kind of motor and take into account the magnetic hysteresis characteristic of the rotor hysteresis ring. In this investigation the application of complex permeability concept is implemented to model the hysteresis loop and the hysteresis loop in inclined ellipse shape is adopted. To the best knowledge of the authors, this has not been studied before. Based on this concept, simulation of hysteresis motor in conventional configuration is done in order to obtain the output values of motor using 3D Finite Element Model (FEM). This 3D finite element model has high level accuracy and gives better insight of motor performance. Meanwhile, in order to validate the simulation results an experimental set-up is provided and the output values of typical motor are measured. It is shown that there is a good agreement between experimental and simulation results. Keywords: 3-D Finite Element Method, Complex Permeability, Hysteresis Motor.

1 Introduction1 Hysteresis motors have some good characteristics such as soft torque, simple construction with conventional three phase stator windings and self-starting torque. These advantages make the hysteresis motor suitable for some applications such as compressors, pumps, timing, and recording equipment. Although, hysteresis motor in contrast to Permanent Magnet Synchronous Motor (PMSM) has lower output power per unit volume, lower power factor and efficiency and higher magnetizing current [1], But limitation such as zero starting torque, needs to auxiliary winding for line starting and closed loop control systems have confined the usage of PMSM for special applications. Hysteresis motor overcomes these limitations by using the hysteresis characteristics of the magnetic materials. It should be noted that the magnetic characteristics of the motor could be easily affected by hysteresis material, structural dimensions and winding distributions [2]. To have a good designing for these parameters of machine, it would be desirable to adopt an accurate model for the motor. Analytical methods have been used to study the hysteresis motors frequently. However, these methods are very complex when accurate evaluation of the saturation effects, and Iranian Journal of Electrical & Electronic Engineering, 2013. Paper first received 9 Jan. 2012 and in revised form 13 Jan. 2013. * The Authors are with the Center of Excellence for Power Systems Automation and Operation, Iran University of Science & Technology (IUST), Tehran, Iran. E-mails: [email protected], [email protected], [email protected] and [email protected].

stator and rotor slotting is needed. These problems are overcome by applying numerical methods. Finite element method allows a precise analysis of magnetic devices taking into account geometric details and magnetic nonlinearity. In previous studies, 2D finite element (FEM) techniques for simulating of hysteresis motors have been developed [2-4].

In this paper, the performance characteristics of hysteresis motor through a 3D finite element analysis (FEA) are provided. 3D model has high level of accuracy and gives us a better insight of motor characteristics. Such simulation is based upon Maxwell’s field equations considering the case of a circumferential flux type machine at synchronous speed. There are mainly three methods to take into account the magnetic hysteresis of the rotor hysteresis ring. One is based on the approximation of a parallelogram [5] and the second one is the Preisach model [2, 6, 7] and the last one is based on elliptical model [8]. In this study, the application of complex permeability concept is implemented in order to model the hysteresis loop in the shape of inclined ellipse. To the best knowledge of the authors, this has not been studied before.

Finally, in order to validate the simulation an experimental set-up is provided and output characteristics of conventional hysteresis motor are measured. There exists a reasonably close agreement between the FEM results and experimental set-up output characteristics. Furthermore, this study can be used in the design approach and precise analysis of hysteresis motors.

Dow

nloa

ded

from

ijee

e.iu

st.a

c.ir

at 5

:49

IRS

T o

n W

edne

sday

Dec

embe

r 30

th 2

020

Page 2: Electromagnetic Analysis of Hysteresis Synchronous Motor Based …ijeee.iust.ac.ir/article-1-481-en.pdf · hysteresis motor through a 3D finite element analysis (FEA) are provided

Mirimani et al: Electromagnetic Analysis of Hysteresis Synchronous Motor Based on … 89

2 Structure and Winding Configuration Hysteresis motor is a kind of special motor with

outstanding structural features. This type of motor has not slot on its rotor and the rotor structure is quite simple. The structure of a typical two pole hysteresis motor is shown in Fig. 1. The inside surface of the stator has teeth and slots and the conventional three phase windings is implemented in stator. Rotor is generally designed as a cylindrical type motor and made up of two parts. Firstly, hysteresis ring which is the basic element for the torque providing that is made of semi hard magnetic material and can conduct flux circumferentially. Secondly, the hysteresis ring holder; which almost is made of the nonmagnetic material such as aluminum and its alloys. This part of rotor has not any effect on the torque providing and only is the copulative between the rotor and the motor shaft. 3 FEM Model

Since the presentation of the theory of hysteresis torque by Steinmetz in 1908, many authors analyzed the hysteresis machine based on the approximation of representing the hysteresis loop. The hysteresis loop was replaced by inclined ellipse by Teare, Roberts, Miyairi and Robertson in their analysis of the hysteresis motor.

Fig. 1 different parts of hysteresis motor (1) Holder, (2) Hysteresis ring, (3) Stator and winding

In this study, a complex permeability is used to predict the hysteresis loop in hysteresis motor for first time. The aim of the following discussion is to investigate the validity of such application. A useful tool for dealing with magnetic effects is the complex permeability. While at low frequencies in a linear material the magnetic field and the auxiliary magnetic field are simply proportional to each other through some scalar permeability, at high frequencies these quantities will react to each other with some lag time [9]. These fields can be written as phasors, such that:

ω , ω δ (1)

where δ is the phase delay of B from H. Understanding permeability as the ratio of the magnetic field to the auxiliary magnetic field, the ratio of the phasors can be written and simplified as:

μω δ

ωδ (2)

So that the permeability becomes a complex

number. By Euler's formula, the complex permeability can be translated from polar to rectangular form:

μ cos δ δ μ μ (3)

The ratio of the imaginary to the real part of the

complex permeability is called the loss tangent:

δ (4)

which provides a measure of how much power is lost in a material versus how much is stored.

Fig. 2 helps us to exploit desired parameter as a function of Hmax, HC and Bmax [9, 10].

µµµ µ

(5)

δ (6)

µ ′ µ cos δ (7)

µ ′′ µ sin δ (8)

where δ is hysteresis lag angle between flux density and magnetic field intensity, rμ is the relative permeability,

'rμ and ''

rμ are the real and imaginary parts of complex permeability.

Dow

nloa

ded

from

ijee

e.iu

st.a

c.ir

at 5

:49

IRS

T o

n W

edne

sday

Dec

embe

r 30

th 2

020

Page 3: Electromagnetic Analysis of Hysteresis Synchronous Motor Based …ijeee.iust.ac.ir/article-1-481-en.pdf · hysteresis motor through a 3D finite element analysis (FEA) are provided

90

Fig. 2 Inclined As shown

different hysloop regardmaterial is illustrated witeration, a rahysteresis rinFrom the Fcircumferentcan be obtaobtained fromthis proceduris satisfied. Ican be evaluhysteresis loproportional Eq. (5).

rVpT ..21π

=

where, p is nvolume and that this promodeling wagreement w3D finite elsimulate of level of accuperformance

d hysteresis loo

n in Fig. 2, fosteresis loop. Iding to magn

in, an iteratwith a flow candom hystereng elements hFEA, the matial direction ained. Now, m FEA is chere continues uIf the analysis ated. It is so iop since the to the area of

hE.

number of poEh is the area

ocedure is so with comple

with real motorement modelproposed mo

uracy and give[9]. Finite

I

p approximatio

or a hysteresisIn order to chnetic circuit tion method chart in Fig.esis ring is sel

have the arbitraximum flux

in the hysterthe maximu

ecked with pruntil the conv is completedimportant to soutput torque

f hysteresis loo

le pairs, Vr tha of hysteresi

accurate andex permeabir tests. As mel is implemen

otor. This 3D es us a better element meth

Iranian Journ

on

material therhoose an accur

that hysteris used that

. 3. In the flected. So, all ary permeabildensity for

resis ring regum flux denevious value

vergence criter, torque of mo

select an accure of the motoop [10] regard

he hysteresis rs loop. It is s

d hysteresis lility has clentioned befornted in ordermodel has hinsight of mo

hod is based

nal of Electrica

re is rate esis t is first the

lity. the

gion nsity and rion otor rate

or is ding

(9)

ring seen oop lose re, a r to high otor

on

Maare

B =

madeshexthe900forconenccirquause

Fig

Fig

×∇

.∇B

al & Electron

axwell’s equae relevant to st

.A×∇=

In order to hash diagram signed manuaxagonal elemee mesh diagra000 that lead r boundary cndition is compasses thcuit coupled mantity. Fig. 4ed in this stud

F

Set new loaccording to

g. 3 Flow chart

g. 4 Circuit coup

,JH=×

,0=B

nic Engineerin

ations. The folteady state app

ave high leveis not used ally. Pentagoent is used in am. The total

to high leveconditions, thadopted on

he motor. Thimodel that theshows the cir

dy.

Initia

ind HC, Hmax ,cregardin

Finite

Bma

Calculatehy

oop Bmax1

NO

for accurate hy

pled model use

ng, Vol. 9, No.

llowing Maxwplications [11

l of accuracy and a mesh

on element irotor in ordernumber of nl of accuracyhe homogeno

the infinitis simulation e phase voltagrcuit coupled

al guess for Bma

complex permeng to selected

element analy

ax1 – Bmax<eps.

END

e Bmax1 from FEysteresis ring

Yes

ysteresis selectio

ed in simulation

2, June 2013

well equations].

(10

(11

(12

the automatich diagram isin stator andr to constituteodes is about

y. Meanwhile,ous Dirichlette box that

is based onge is the inputmodel that is

ax

eability terms loop

ysis

EM on

on

n

3

s

0)

1)

2)

c s d e t , t t n t s

Dow

nloa

ded

from

ijee

e.iu

st.a

c.ir

at 5

:49

IRS

T o

n W

edne

sday

Dec

embe

r 30

th 2

020

Page 4: Electromagnetic Analysis of Hysteresis Synchronous Motor Based …ijeee.iust.ac.ir/article-1-481-en.pdf · hysteresis motor through a 3D finite element analysis (FEA) are provided

Mirimani et a

4 ExperimThe tes

circumferentshown on FiTable 1.

In this sehigh resoluti0.011(Nm) toare shown in

5 Simulatio

Based osimulation fomotor has bemotor is analthe motor. Fi

Table 1 Motor

LRa

A

R

Outer

Inner

Sta

Nu

Phase

Table 2 Outpu

Qu

Steady stat(

Steady sta

P inpPow

Effici

al: Electroma

mental Set-Upts have betial hysteresisig. 1. The par

et-up voltage,ion oscilloscoorque. Output

n Table 2.

on Results on the abovor prototype ceen done. It mlyzed becauseig. 5 shows th

r features Quantity

Line RMS voltaated phase curre

Frequency(H

Speed(rpm

Phase connect

Pole pairs

Holder thickn

Air gap length (

Ring thickness (

r diameter of sta

r diameter of sta

ator stack heigh

Number of slo

mber of turns p

Fill factor

e resistance at 4

ut quantities of

uantity

te Load torque (Nm)

ate current (A)

put(Watt) er factor iency (%)

agnetic Analys

een done os synchronourameters of m

, current are mope for a cont quantities of

ve respects, circumferentiamust be notede of the magnehe mesh diagra

age(V) ent (A)

Hz)

)

tion

ness

(mm)

(mm)

ator(mm)

ator(mm)

ht(mm)

ots

per coil

400Hz(Ω)

prototype moto

Hysteresis

0

0

604

sis of Hysteres

on a prototus motor that

motor are given

measured witnstant load wf prototype mo

finite elemal flux hysterd that half of etic periodicityam of motor.

Value 150 0.6

400

24000

Y

1

1

1.5

1

93

50.4

25

24

115

0.5

30

or

motor outputs

.0110

0.443

68.6 0.596 40.2

sis Synchrono

type t is n in

th a with otor

ment esis the

y of

s

Fig

Fig

befhys

Sta

us Motor Bas

g. 5 Mesh diagr

g. 6 distribution

Fig. 6 show

fore, flux linsteresis ring. Fig. 7 shows

ator and rotor.

ed on …

ram of simulated

n of the circumf

ws the flux denes are circu

s the isovalues.

d motor

ferential flux

ensity of motumferentially

s diagram of f

91

tor. As saidthrough the

flux density in

d e

n

Dow

nloa

ded

from

ijee

e.iu

st.a

c.ir

at 5

:49

IRS

T o

n W

edne

sday

Dec

embe

r 30

th 2

020

Page 5: Electromagnetic Analysis of Hysteresis Synchronous Motor Based …ijeee.iust.ac.ir/article-1-481-en.pdf · hysteresis motor through a 3D finite element analysis (FEA) are provided

92

Fig. 7 Isovalue

Table 3 Simul

Steady

Steady

PP

Ef As seen

speed is exacdensity distrobtained and

As seen agreement band simulate 6 Conclusi

In this pais presentedmotor. The were calculashape is adopAn iterationaccurate looptypical motoaccuracy ofprovided andmeasured. Iagreement bquantities.

References [1] Rahma

Synchr

es diagram of f

lation results foQuantity

y state torque (N

y state current (

P input(Watt) Power Factor fficiency (%)

in Fig. 7, hyctly like a permibutions the o

d shown in Tabfrom Tables

between outpud one.

ion aper, a novel

d for accuratsteady state

ated. A hysterepted to approxn method is p. The simulaor is done. f the model d output quanIt was showbetween sim

an M. A. aronization of

I

flux density of r

or Hysteresis mv

Nm) 0

(A)

ysteresis ringmanent magnoutput quantitble 3. s 2 and 3, tut quantities

finite elemente analysis o

characteristicesis loop in anximate the rea

implementedation based on

In order to an experim

ntities of protwn that theremulation resu

and Qin R.Permanent M

Iranian Journ

rotor and stator

otor values

0.0112

0.435

66.7 0.59 42

g at synchronnet. Based on fties of motor

there is a clof actual mo

nt analysis moof the hystercs of the mon inclined elli

al hysteresis lod to model n dimensions o

investigate mental set-uptotype motor e is reasonaults and mo

, "Starting Magnet Hyster

nal of Electrica

nous flux are

lose otor

odel esis otor ipse oop.

the of a the

p is are

ably otor

and esis

[2]

[3]

[4]

[5]

[6]

[7]

[8]

[9]

[10

[11

eng

al & Electron

Motors", Applicatio

] Kim H. KElement AVector MTransactio3495-3498

] Hong S. KK., “TorqUsing VTransactio1932-1935

] Kim H. Kof HysteMethod aIEEE Trapp. 685-68

] Rahman MHysteresisApparatus237-242,

] Rahman MPerard Jalgorithmprocesses Transactio3253-3255

] Hong S., HysteresisMaterials”Vol. 30, N

] Horii T., HysteresisComplex Journal o135-142,

] Getzlaff MSpringer-V

0] Zaher F.Field of aPermeabilConversio

1] Wilcox LSolving EquationsPhilosophMathemat

gineering in the

nic Engineerin

IEEE Tron, Vol. 32, NK., Jung H. KAnalysis of H

Magnetization-ons on Magn8, 1998. K., Kim H. Kque CalculatVector Hysons on Magn5, 2000.

K., Hong S. K.eresis Motorand Magneti

ansaction on M88, 2000. M. A., “Analys Motor”, IEEs and Systems1973. M. A., PoloujJ. and Gows for digital in semi hard

opn on Magn5, 1981. Kim D., Jung

s Model fo”, IEEE Tra

No. 5, pp. 337Yuge N. and s Motor on A

Permeabilitn Magnetics i1994. M., FundamenVerlag, 2008. A. A., “An Aa Hysteresis lity”, IEEE on, Vol. 5, No. C., “High-or

the Tims”, for the hy in the tics at Brown

Seyyed MBabol, Iradegree fMazandaraM.Sc. degrmachines Science anin 2010, wtoward the

e Department o

ng, Vol. 9, No.

ransaction oNo. 5, pp. 1183K. and Hong SHysteresis Mo-Dependent Mnetics, Vol. 34

K., Kim H. S.tion of Hyststeresis Monetics, Vol. 3

and Jung H. r Using Finzation-dependMagnetics, Vo

ytical Models fEE Transactios, Vol. PAS-9

ujadoff M., Jawada S. D.,

simulation magnetic matnetics., Vol.

g H. and Woor Unorienteansactions on1-3374, Sep. Wakui G., “A

Asynchronous ty”, IEEE in Japan, Vol

ntals of magn

Analytical Solmotor Based Transaction

o. 1, pp. 156-1rder Accurate

me-Harmonic degree of Division

University, M

Mehdi Mirimanan. He receivfrom the Uan, Babol, in ree on the subje

from Iran nd Technologywhere he is cure Ph.D. degreof Electrical En

2, June 2013

on Industry3-1189, 1996.S. K., “Finitetor Using the

Model”, IEEE4, No. 5, pp.

and Jung H.teresis Motorodel”, IEEE6, No. 4, pp.

K., “Analysisnite Elementdent Model”,ol. 36, No. 4,

for Polyphaseons on Power92, No. 1, pp.

ackson R. D.,, “Improvedof hysteresisterials”, IEEE17, Nov. pp.

on J., “Vectored Magneticn Magnetics,1994. Analysis of aSpeed UsingTransaction

. 9, No. 2, pp.

etism, Berlin:

lution for theon Complexon Energy

63, 1990. e Methods for

Maxwell’sf Doctor of

of AppliedMay 2006.

ni was born inved the B.Sc.University of

2007 and theect of electricalUniversity of, Tehran, Iran,

rrently workinge in electricalngineering. His

3

y

e e E .

. r

E .

s t , ,

e r .

, d s E .

r c ,

a g n .

:

e x y

r s f d

n . f e l f ,

g l s

Dow

nloa

ded

from

ijee

e.iu

st.a

c.ir

at 5

:49

IRS

T o

n W

edne

sday

Dec

embe

r 30

th 2

020

Page 6: Electromagnetic Analysis of Hysteresis Synchronous Motor Based …ijeee.iust.ac.ir/article-1-481-en.pdf · hysteresis motor through a 3D finite element analysis (FEA) are provided

Mirimani et a

research interefinite-element electromagnet

Optimization, He is currenEngineering ais also membautomation &

al: Electroma

ests include thanalysis of

tic devices.

Abolfaz1989 froand MrespectiPolytechFrance) has direof Elecresearch

Monitoring anntly Professor

at Iran Universiber of Center o

Operation.

agnetic Analys

he design, modelectrical ma

zl Vahedi receom Ferdowsi M

M.Sc & Ph.D ively from Ihnique de all in Electrica

ected several pctrical Machineh interests arend Control of Er in Departmity of Science &of Excellence

sis of Hysteres

eling, control, achines and o

eived his B.ScMashhad Univerin 1992 and 1Institute Natio

Lorraine (INal Engineering.

projects in the es & Drives. e mainly DesElectric Machi

ment of Electr& Technology.for Power Sys

sis Synchrono

and other

c in rsity 1996 onal

NPL-. He area His

sign, ines. rical . He stem

appma

pul

us Motor Bas

plication of FEachines.

lsed power tech

ed on …

Mohammaborn in 1received hiof Iran TechnologyElectrical Efinishing hUniversity (IUST), Teinterests in

EM to design

Amir Baktin ElectUniversity Electrical University (IUST) in Now he is research indrives, Ele

hnology.

adreza Ghaz1986 in Tehris B.S. degree frUniversity ofy (IUST), IranEngineering. Phis Msc. pro

of Science &ehran, Iran. Hisnclude dynamic

and modeling

tash received htronic Engin

of Yazd anEngineering

of Science &2004 and 2007a PhD studen

nterests include ectrical motor

93

zanchaei wasran, Iran. Hefrom Universityf Science &n, in 2007 in

Presently, he isogram in Iran& Technologys main researchc modeling andg of electrical

his BS degreesneering fromd his MS in

from Iran& Technology7, respectively.t in IUST. Hisvariable speed

s design, and

s e y

& n s n y h d l

s m n n y . s d d

Dow

nloa

ded

from

ijee

e.iu

st.a

c.ir

at 5

:49

IRS

T o

n W

edne

sday

Dec

embe

r 30

th 2

020