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DESIGN STUDY OF HYBRID EXCITATION FLUX SWITCHING MOTOR FOR ELECTRIC VEHICLES SALMIZA BINTI SAID A project report submitted in partial fulfillment of the requirement for the award of the Degree of Master of Electrical Engineering Faculty of Electric and Electronic Engineering Universiti Tun Hussein Onn Malaysia JULY 2014

Thesis PS MIZA

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Page 1: Thesis PS MIZA

DESIGN STUDY OF HYBRID EXCITATION FLUX SWITCHING MOTOR FOR

ELECTRIC VEHICLES

SALMIZA BINTI SAID

A project report submitted in partial

fulfillment of the requirement for the award of the

Degree of Master of Electrical Engineering

Faculty of Electric and Electronic Engineering

Universiti Tun Hussein Onn Malaysia

JULY 2014

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ABSTRACT

Hybrid excitation flux switching motor (HEFSM) is an attractive features compared

to interior permanent magnet synchronous motor (IPMSM). The hybrid excitation is

applied in this project to gain the high torque of the system. This is because the flux

was achieved from both permanent magnet and field excitation coil. The design of 6

slot 7 pole inner rotor hybrid excitation motor is analyse by using the JMAG

Designer Software which is a simulation software that easily utilized by the user.

The analysis of no load, with load and improvement of the motor design is done.

The objective of the project of obtaining 207 Nm torque of the motor is succesful

since the improvement of the design give the torque of 228.70 Nm at speed

9161r/min from the initial torque of 171.04 Nm at speed 12580r/min. The

performance of motor is also improved when the maximum power is increase from

155kW to 173kW. The characteristic represent the high torque, low speed motor

performance. An improved design is to gain a better performance in its maximum

torque and power production. As the design results, the improved motor enables to

keep the better power density in the initial design.

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ABSTRAK

Hybrid excitation flux switching motor (HEFSM) mempunyai ciri-ciri yang menarik

berbanding interior permanent magnet synchronous motor (IPMSM). Pengujaan

hibrid digunakan dalam projek ini untuk menghasilkan tork yang tinggi bagi sistem.

Ini kerana fluks dicapai dari kedua-dua magnet kekal dan medan pengujaan

gegelung. Reka bentuk 6 slot 7 pole rotor dalaman pengujaan hibrid motor dianalisis

menggunakan Designer Software JMAG yang merupakan perisian simulasi yang

mudah digunakan oleh pengguna. Analisis tanpa beban, dengan beban dan

peningkatan reka bentuk motor itu dilakukan. Objektif projek memperoleh tork

motor 207 Nm tercapai kerana peningkatan reka bentuk memberikan tork 228,70

Nm pada kelajuan 9161r/min berbanding tork permulaan 171,04 Nm pada kelajuan

12580r/min. Prestasi motor juga bertambah baik apabila kuasa maksimum

mengalami peningkatan dari 155kW kepada 173kW. Ciri ini memberikan prestasi

motor dalam keadaan tork yang tinggi pada kelajuan rendah. Peningkatan reka

bentuk adalah untuk mendapatkan prestasi yang lebih baik dalam tork dan kuasa

pengeluaran maksimum. Motor dalam reka bentuk ini bertambah baik dan

mempunyai ketumpatan kuasa yang lebih baik berbanding reka bentuk awal.

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TABLE OF CONTENTS

TITLE i

DECLARATION ii

DEDICATION iii

ACKNOWLEDGEMENT iv

ABSTRACT v

CONTENTS vii

LIST OF FIGURES x

LIST OF TABLES xiii

CHAPTER 1 INTRODUCTION 1

1.1 Introduction 1

1.2 Problem statement 3

1.3 Objectives 3

1.4 Scopes 3

CHAPTER 2 LITERATURE REVIEW 5

2.1 Introduction of Electric Motor 5

2.2 Classification of Flux Switching Motor (FSM) 6

2.2.1 Permanent Magnet Flux Switching Motor

(PMFSM)

6

2.2.2 Field Excitation Flux Switching Motor

(FEFSM)

7

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2.2.3 Hybrid Excitation Flux Switching Motor

(HEFSM)

9

CHAPTER 3 METHODOLOGY 12

3.1 Introduction 12

3.2 Geometry Editor 15

3.2.1 Rotor design 16

3.2.2 Stator design 18

3.2.3 Permanent Magnet (PM) design 19

3.2.4 Field Excitation Coil (FEC) design 21

3.2.5 Armature Coil (AC) design 21

3.3 JMAG-Designer 22

3.3.1 Materials setting 22

3.3.2 Conditions setting 23

3.3.3 Circuit design 24

3.4 JMAG Analysis 24

3.4.1 No load analysis 24

3.4.2 Load analysis 25

3.4.3 Torque-Speed Analysis 25

3.4.4 The Improvement Of The Motor 25

CHAPTER 4 RESULT 27

4.1 Initial results 27

4.2 No-Load Analysis: Armature Coil test 27

4.2.1 6 coil test 29

4.2.2 3 coil test 29

4.2.3 UVW coil test 30

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4.3 Field Strengthening 33

4.4 Load Analysis 33

4.4.1 Torque at various Je/Ja 33

4.4.2 Speed Characteristic 34

4.5 Improved results 35

4.5.1 Torque at various Je/Ja for Improved

Design

38

4.5.2 Torque-Speed Characteristic for Improved

Design

38

4.6 Flux Linkage and Flux Distribution 39

4.7 Cogging Torque 45

CHAPTER 5 CONCLUSION 46

5.1 Discussion and Conclusion 46

5.2 Suggestion and Future Work 49

REFERENCES 50

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LIST OF FIGURES

1.1 The geometry of 6S-7P motor (a) Stator (b) Rotor 4

2.1 Types of Electric Motors 5

2.2 General Classification of FSM 6

2.3 Principle Operation of PMFSM 7

2.4 Principle operation of FEFSM (a) θe=0° and (b)

θe=180° flux moves from stator to rotor (c) θe=0° and

(d) θe=180° flux moves from rotor to stator

9

2.5 The operating principle of the proposed HEFSM (a)

θe=0° - more excitation (b) θe=180° - more excitation

(c) θe=0° - less excitation (d) θe=180° - less excitation

10

3.1 Design of 6S-7P HEFSM 13

3.2 Work flow of project implementation 14

3.3 Dimension of 6S-7P HEFSM Inner Rotor 14

3.4 Shortcut menu/Toolbar of Geometry Editor 16

3.5 Design of rotor (a) Sketch the design (b) Create region

(c) Region mirror copy (d) Full sketch

17

3.6 Design of stator (a) Stator sketch and create a region

(b) Region radial copy (c) Full sketch

19

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3.7 Design of PM part (a) PM sketch and create a region

(b) Full sketch

20

3.8 Design of FEC part 21

3.9 AC design of 6S-7P HEFSM 22

3.10 FEC and AC coil link 23

3.11 FEC Circuit implementation 24

3.12 The flow chart of improvement process 26

4.1 Graph of 6 coil test (a) Graph for flux pattern 1(b)

Graph of flux pattern 2 (c) Graph of flux pattern 3

29

4.2 Graph of 3 coil test (a) Flux pattern 1 represent V (b)

Flux pattern 2 represent U (c) Flux pattern 3 represent

W

30

4.3 UVW Circuit Connection 31

4.4 Graph of UVW fluxes (a) Flux pattern for UVW Test

(b) U Flux pattern for 3 conditions

32

4.5 Field Strengthening 33

4.6 The torque characteristic at various Je/Ja for Initial

Design

34

4.7 The Torque/Power-speed characteristic for Initial

Design

35

4.8 Graph of Improvement Process (a) Improvement of D1

(b) Improvement of D3

37

4.9 The torque characteristic at various Je/Ja for Improved

Design

38

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4.10 The Torque/Power-speed characteristic for Initial

Design and Improved Design

39

4.11 Flux Linkage of the Design 6S-7P Motor (a) & (b)

Initial Design (c) & (d) Improved Design

41

4.12 Flux Distribution of the Design 6S-7P Motor (a) & (b)

Initial Design (c) & (d) Improved Design (e) Magnetic

Flux Density Indicator

44

4.13 Flux flow for both PM and FEC in the motor design 44

4.14 Cogging torque of the 6S-7P design 45

5.1 Dimension of 6S-7P Inner Rotor HEFSM Improved

Design

47

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LIST OF TABLES

1.1 Parameters of Design 6S-7P HEFSM 4

2.1 Advantages and disadvantages of FSM 11

3.1 Design restrictions and specifications of the proposed

6S-7P HEFSM

13

3.2 Parameters of Design 6S-7P HEFSM 15

3.3 Materials setting 22

4.1 Connection between FEM coil and circuit 31

5.1 Initial and final design parameters of 6S-7P Inner Rotor

HEFSM

48

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CHAPTER 1

INTRODUCTION

1.1 Introduction

A demand for vehicles using electrical propulsion drives is getting higher and higher

from the stand points of preventing global warming and saving fossil fuel recently.

As one of the vehicles, many automotive companies have commercialized Hybrid

Electric Vehicles (HEVs) in which Interior Permanent Magnet Synchronous Motors

(IPMSM) have been employed as a main traction motor in terms of high torque

and/or power density, and high efficiency over most of operating torque-speed range

[1] . This is due to the restriction of motor size to ensure enough passenger space

and the limitation of motor weight to reduce fuel consumption. As one of effective

strategies for increasing the motor power density, the technological tendency to

employ the combination of a high-speed machine and a reduction gear would be

accelerated.

With the significant achievements and improvements of permanent magnet

materials and power electronics devices, the brushless machines excited by PM

associated with FEC are developing dramatically. This type of machine is called

hybrid excitation machine (HEM) that can be classified into four categories. The

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first type consists of both PM and FEC at rotor side such as combination rotor

hybrid excitation (CRHE) machine and synchronous/PM hybrid AC machine. The

second type consists of PM in the rotor while FEC is in the stator. The third type

consists of PM in the rotor while the FEC is in the machine end. Finally, the fourth

type of HEM is the machine, which has both PM and FEC in the stator. It should be

emphasized that all HEMs mentioned in the first three have a PM in the rotor and

can be categorized as “hybrid rotor-PM with field excitation machines” while the

fourth machine can be referred as “hybrid stator-PM with field excitation machines”.

Based on its principles of operation, the fourth machine is also known as “hybrid

excitation flux switching machine (HEFSM)” which is getting more popular recently

[2]- [3].

In this study, a 6S-7P HEFSM in which the arrangement of FEC in radial

direction is proposed for HEV applications. The proposed machine is composed of 6

PMs and 6 FECs distributed uniformly in the midst of each armature coil. The three-

phase armature coils are accommodated in the 6 slots for each 1/3 stator body

periodically. As the rotor rotates, the fluxes generated by PMs and mmf of FECs

link with the armature coil alternately. Generally, the relation between the

mechanical rotation frequency and the electrical frequency for this machine can be

expressed as: fe= Nr.fm

where fe is the electrical frequency, fm is the mechanical rotation frequency and Nr is

the number of rotor poles respectively. The presence of excitation coil makes these

types of machines more attractive in terms of modulating the PM flux.

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1.2 Problem statement

Hybrid excitation machines (HEMs) consist of permanent magnet (PM) and field

excitation coil (FEC) as their main flux sources. It has several attractive features

compared to interior permanent magnet synchronous machines (IPMSM) which

conventionally employed in hybrid electric vehicles (HEVs). Among various types

of HEM, the machine with both permanent magnet and excitation coil located on the

stator has the advantage of robust rotor structure similar as switch reluctance

machine (SRM) and make this machine to be applied for high speed motor drive

systems.

1.3 Objectives

The objectives of this study are:

i. To design the 6S-7P HEFSM inner rotor motor.

ii. To analyze the performance of the designed motor under no load condition,

with load condition, the torque, power and speed of the motor.

iii. To improve the performance of initial design of 6S-7P HEFSM.

1.4 Scopes

The design of 6S-7P motor is by using the JMAG Designer Software. JMAG

Designer is the electromagnetic simulation software than be easily utilized by the

user because of its CAD like usability. Application of CAD data makes it possible to

introduce magnetic field analysis into the existing design process.

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By using the parameter as in Table 1.1 and Figure 1.1(a) and (b), the

designing of 6S-7P motor is made in the Geometry Editor of the JMAG Designer.

The drawing process take place with the specification needed.

Table 1.1: Parameters of Design 6S-7P HEFSM

D1 Rotor inner radius(mm)

D2 Rotor pole depth(mm)

D3 Rotor pole width(mm)

D4 PM length (mm)

D5 Excitation coil pitch(mm)

D6 Stator outer core thickness(mm)

D7 AC width(mm)

D8 AC height(mm)

(a) Design of stator (b) Design of rotor

Figure 1.1: The geometry of 6S-7P motor (a) Stator (b) Rotor

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CHAPTER 2

LITERATURE REVIEW

2.1 Introduction of Electric Motor

Figure 2.1: Types of Electric Motors

An electric motor is an electrochemical device that converts electrical energy into

mechanical energy. Most electric motors operate through the interaction of

magnetic and current-carrying conductor to generate force. Electric motors may be

classified by the source of electric power, by their internal construction, by their

application, or by the type of motion they give. As shown in Figure 2.1, electric

motor can be divided into several types which have their own advantages and

disadvantages.

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2.2 Classification of Flux Switching Motor (FSM)

Generally, the FSMs can be categorized into three groups that are Permanent

Magnet Flux Switching Motor (PMFSM), Field Excitation Flux Switching Motor

(FEFSM), and Hybrid Excitation Flux Switching Motor (HEFSM). Both PM and FE

has only Permanent Magnet and Field Excitation Coil (FEC), respectively as their

main flux sources, while HE combines both PM and FEC as their main flux sources.

Figure 2.2 illustrates the general classification of FSMs.

Figure 2.2: General Classification of FSM

2.2.1 Permanent Magnet Flux Switching Motor (PMFSM)

PM motors based on the principle of flux switching have been studied for several

decades. Generally, such motors have a salient pole rotor and the PMs which are

housed in the stator. The salient pole rotor is similar to that of SRMs, which is more

robust and suitable for high speed applications and the difference in the number of

rotor poles and stator teeth is two. In contrast with conventional IPMSM, the slot

area is reduced when the magnets are moved from the rotor to the stator, it is easier

to dissipate the heat from the stator and the temperature rise in the magnet can be

controlled by proper cooling system.

Flux Switching Motor (FSM)

Permanent Magnet (PM) Field Excitation (FE) Hybrid Excitation (HE)

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The general operating principle of the PMFSM is illustrated in Figure 2.3,

where the black arrows show the flux line of PM as an example. From the figure,

when the relative position of the rotor poles and a particular stator tooth are as in

Figure 2.3 (a), the flux-linkage corresponds to one polarity. However, the polarity of

the flux-linkage reverses as the relative position of the rotor poles and the stator

tooth changes as shown in Figure 2.3(b), which the flux linkage switches polarity as

the salient pole rotor rotates.

Figure 2.3: Principle Operation of PMFSM

2.2.2 Field Excitation Flux Switching Motor (FEFSM)

FEFSM is a form of salient-rotor reluctance motor with a novel topology, combining

the principles of the inductor generator and the SRMs [4]- [5]. The concept of the

FEFSM involves changing the polarity of the flux linking with the armature

winding, with respect to the rotor position. The viability of this design was

demonstrated in applications requiring high power densities and a good level of

durability [6]- [7]. The novelty of the invention was that the single-phase AC

configuration could be realized in the armature windings by deployment of DC FEC

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and armature winding, to give the required flux orientation for rotation. The torque

is produced by the variable mutual inductance of the windings. The single-phase

FEFSM is very simple motor to manufacture, coupled with a power electronic

controller and it has the potential to be extremely low cost in high volume

applications. Furthermore, being an electronically commutated brushless motor, it

inherently offers longer life and very flexible and precise control of torque, speed,

and position at no additional cost.

The operating principle of the FEFSM is illustrated in Figure 2.4. Figure

2.4(a) and (b) show the direction of the FEC fluxes into the rotor while Figure 2.4(c)

and (d) illustrate the direction of FEC fluxes into the stator which produces a

complete one cycle flux. Similar with PMFSM, the flux linkage of FEC switches its

polarity by following the movement of salient pole rotor which creates the term

“flux switching”. Each reversal of armature current shown by the transition between

Figure 2.4(a) and (b), causes the stator flux to switch between the alternate stator

teeth. The flux does not rotate but shifts clockwise and counter clockwise with each

armature-current reversal. With rotor inertia and appropriate timing of the armature

current reversal, the reluctance rotor can rotate continuously at a speed controlled by

the armature current frequency. The armature winding requires an alternating

current reversing in polarity in synchronism with the rotor position. For automotive

applications the cost of the power electronic controller must be as low as possible.

This is achieved by placing two armature coils in every slot so that the armature

winding comprises a set of closely coupled (bifilar) coils [8]- [9].

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Figure 2.4: Principle operation of FEFSM (a) θe=0° and (b) θe=180° flux moves from stator to rotor (c) θe=0° and (d) θe=180° flux moves from rotor to stator

2.2.3 Hybrid Excitation Flux Switching Motor (HEFSM)

Hybrid excitation flux switching motors (HEFSMs) are those which utilize primary

excitation by PMs as well as DC FEC as a secondary source. Conventionally,

PMFSMs can be operated beyond base speed in the flux weakening region by means

of controlling the armature winding current. HEFSM is an alternative option where

the advantages of both PM motors and DC FEC motors are combined. As such

HEFSMs have the potential to improve flux weakening performance, power and

torque density, variable flux capability, and efficiency which have been researched

extensively over many years [10]- [11].

The operating principle of the proposed HEFSM is illustrated in Figure 2.5,

where the red and blue line indicate the flux from PM and FEC, respectively. In

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Figure 2.5(a) and (b), since the direction of both PM and FEC fluxes are in the same

polarity, both fluxes are combined and move together into the rotor, hence

producing more fluxes with a so called hybrid excitation flux. Furthermore in Figure

2.5(c) and (d), where the FEC is in reverse polarity, only flux of PM flows into the

rotor while the flux of FEC moves around the stator outer yoke which results in less

flux excitation. As one advantage of the DC FEC, the flux of PM can easily be

controlled with variable flux control capabilities as well as under field weakening

and or field strengthening excitation. The advantages and disadvantages of FSM

discussed in this chapter are listed in Table 2.1.

Figure 2.5: The operating principle of the proposed HEFSM (a) θe=0° - more excitation (b) θe=180° - more excitation (c) θe=0° - less excitation (d) θe=180° - less excitation.

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Table 2.1: Advantages and disadvantages of FSM

Advantages Disadvantages

1. Simple and robust rotor structure

suitable for high speed applications

2. (Easy to manage magnet temperature

rise as all active parts are located in

the stator

3. Flux focusing / low cost ferrite

magnets can also be used

4. Sinusoidal back-emf waveform

which is suitable for brushless AC

operation

1. Reduced copper slot area in stator

2. Low over-load capability due to

heavy saturation

3. Complicated stator

4. Flux leakage outside stator

5. High magnet volume for PMFSM

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CHAPTER 3

METHODOLOGY

3.1 Introduction

Methodology of this research is by using JMAG-Designer version 13.0 software to

design the motor. JMAG is simulation software for the development and design of

electrical devices. JMAG was originally release in 1983 as a tool to support design

for devices such as motors, actuators, circuit component, and antennas. The design

of 6S-7P HEFSM is divide into two parts which is by using Geometry Editor and it

is continued by using JMAG-Designer. The work flow of the geometry editor and

JMAG-Designer are illustrated in Figure 3.2(a) and (b) respectively.

To design a motor, there are some restrictions and specifications need to

follow. This is to ensure the designed motor will be around the recommended

details, thus the output performance as requested is achieved. The summary of

overall restrictions and specifications are as shown in Table 3.1. The Figure 3.1

shows the design of 6S-7P Inner Rotor HEFSM. The dimension of the motor is

shown in Figure 3.3. All these requirements are need in designing the motor.

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Figure 3.1: Design of 6S-7P HEFSM

Table 3.1: Design restrictions and specifications of the proposed 6S-7P HEFSM

Items Unit HEFSM

Geometrical dimension and volume

Stator outer diameter mm 264 Motor stack length mm 70 Shaft radius mm 30 Air gap length mm 0.8 PM weight kg 0.7

Input voltage and current

Max. DC-bus voltage inverter V 650 Max. inverter current Arms 360 Maximum Ja Arms/mm2 30 Maximum Je A/mm2 30

Output performances

Maximum torque Nm 207 Reduction gear ratio - 2.478 Max. axle torque via GR Nm > 825 Maximum speed r/min 12,400 Maximum power kW > 123 Motor weight kg < 35 Power density kW/kg > 3.5

Ja = armature current density, Je = FEC current density, GR = gear ratio

Armature Coil

Permanent Magnet

Field Excitation Coil

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(a)Flow chart of geometry editor (b) Flow chart of JMAG-Designer

Figure 3.2: Work flow of project implementation

Figure 3.3: Dimension of 6S-7P HEFSM Inner Rotor

Start

Rotor design

Stator design

Permanent Magnet design

Field Excitation Coil design

Armature coil design

End

Start

Materials

Condition

Circuit

Mesh

Run

End

Graph

Study properties

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Design parameters of 6Slot-7Poles HEFSSM for HEV applications are shown in

Table 3.2 below.

Table 3.2: Parameters of Design 6S-7P HEFSM

Parameters Initial

D1 Rotor inner radius (mm) 87.2

D2 Rotor pole depth (mm) 16.6

D3 Rotor pole arc (mm) 27.2

D4 PM length (mm) 14

D5 Excitation coil pitch (mm) 30

D6 Stator outer core thickness (mm) 8

D7 AC width (mm) 17.8

D8 AC height (mm) 14.2

ag Air gap length (mm) 0.8

3.2 Geometry Editor

Geometry editor is used to design the rotor and stator part of the motor. The drawing

of PM, FEC and AC parts at the stator can also be done here. The Figure 3.4 shows

the toolbar which used in designing the motor parts.

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aa

Figure 3.4: Shortcut menu/Toolbar of Geometry Editor

3.2.1 Rotor design

i. By click the [Edit Sketch] button, the design on the work plane is started.

ii. Three circles are drawn by using [circle] button. The radius values

adjusted according to the measurement before.

iii. A straight line ([line] button) at about 30ᵒ is drawn from the center point

and another line is parallel to it with distance 16.6mm.

iv. The part that is not being used is cut by using [Trim sketch] button. The

drawing is shown in Figure 3.5(a).

v. Create region for the drawing and must be in enclosed shape. It is shown

in Figure 3.5 (b).

vi. After that, by click the [Region Mirror Copy] the drawing is merging

with one line is set as the reference for the mirror copy. Refer Figure

3.5(c)

vii. The [Region Radial Copy] is used to complete the 7 poles of rotor model.

The full sketch of rotor design is shown in Figure 3.5(d).

Region mirror copy

Region Radial copy Edit sketch

Trim sketch

Line Circle

Create region

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(a) Sketch the design (b) Create region

(c) Region mirror copy

(d) Full sketch

Figure 3.5: Design of rotor (a) Sketch the design (b) Create region (c) Region mirror copy (d) Full sketch

Work plane

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3.2.2 Stator design

i. Same as rotor part, all steps are repeated to draw the stator part.

ii. The enclosed shape which can be merge and copy is drawn. The angle is

about 25.72o.

iii. A region is created and one line is chose as the reference. It was

illustrated in Figure 3.6(a).

iv. Copy the sketch in mirror and radial pattern. The instance of this design

is 6 with angle 60o. It can be referred in Figure 3.6(b). Figure 3.6(c)

shows the full sketch for stator part.

(a) Stator sketch and create a region (b) Region radial copy

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(c) Full sketch

Figure 3.6: Design of stator (a) Stator sketch and create a region (b) Region radial copy (c) Full sketch

3.2.3 Permanent Magnet (PM) design

i. After the stator and rotor part are drawn, all the parts that is still blank is

filled up.

ii. For permanent magnet part, all the same steps as before are repeated.

iii. One line is drawn and parallel with another line. The parameter for the

length and width is followed as in Table III and the sketch is shown in

Figure 3.7(a).

iv. Figure 3.7(b) shows the PM filled in the stator.

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(a) PM sketch and create a region

(b) Full sketch

Figure 3.7: Design of PM part (a) PM sketch and create a region (b) Full sketch

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3.2.4 Field Excitation Coil (FEC) design

i. 6S-7P consists of 6 pairs of FEC. The same steps are repeated.

ii. 4 perpendicular lines are drawn and create the region.

iii. Copy and merge the shape to fill all the 12 FEC. Figure 3.8 shows the

full sketch of FEC when it fill up the stator.

Figure 3.8: Design of FEC part

3.2.5 Armature Coil (AC) design

i. AC part is drawn. By repeated the same steps as before, the 6 pairs of AC

completed the HEFSM design in geometry editor.

ii. Figure 3.8 shows the full drawing of AC for 6S-7P HEFSM.

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Figure 3.9: AC design of 6S-7P HEFSM.

3.3 JMAG-Designer

JMAG-Designer is used to continue the design of 6S-7P HEFSM. It used to

set the materials and conditions, construct a circuit and mesh the motor part.

3.3.1 Materials setting

The materials for HEFSM parts are set as shown in Table 3.3. The materials

are choose from the toolbox located at the right side.

Table 3.3: Materials setting

Parts Material use

Rotor, Stator Nippon Steel 35H210

Permanent Magnet (PM) NEOMAX-35AH (irreversible)

Armature coil, FEC Conductor Copper

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3.3.2 Conditions setting

The condition setting for HEFSM design, for the rotation at the rotor that can be

found from the conditions toolbox and the constant revolution speed is set to 1200

r/min. The Force: Nodal force is set to the rotor to calculate the electromagnetic

force acting on magnetic materials. Rotation axis is in upward. While for the

Torque: Nodal force, it is specifies to calculate the torque acting on magnetic

materials. It set to the rotor part in upward rotation axis. FEM coil is specifies in the

model to link to an FEM coil component in the circuit when the current distribution

is assumed to be uniform in the coil. The full coil link in the FEC and AC is shown

in Figure 3.10.

Figure 3.10: FEC and AC coil link

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3.3.3 Circuit design

Figure 3.11 shows the circuit implementation for HEFSM design. For FEC 1

and FEC 2 as shown in Figure 3.10, the value of turns based on calculation is set to

190 turns while the constant is 1 ohm. The current source (I1) is set to 0 A.

Figure 3.11: FEC Circuit implementation

3.4 JMAG Analysis

3.4.1 No load analysis

The analysis is done to identify the characteristics of the magnetic flux. This is

called armature coil test. The no load analysis also include the flux characteristic by

setting the current flow through FEC with different values. Beginning from Je=0

A/mm2 until maximum Je=30 A/mm2. This analysis is named as flux strengthening.

Both armature coil test and flux strengthening shows the maximum flux that can be

generated by the motor.

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REFERENCES

[1] E. Sulaiman, T. Osaka, Y. Tsujimori, and N. Matsui, "Performance Analysis of Permanent Magnet Flux Switching Machine with Hybrid Excitation," in Proc. International Conf. on Electrical Energy and Industrial Electronics System (EEIES 2009), 2009.

[2] E. Sulaiman, T. Osaka, Y. Tsujimori, and N. Matsui, "Design optimization of 12Slot-10Pole hybrid excitation flux switching synchronous machine with 0.4kg permanent magnet for hybrid electric vehicles," in Proc. 8th Int. Conference on Power Electronics -ECCE Asia, (ICPE 2011), 2011.

[3] E. Sulaiman, T. Osaka, Y. Tsujimori, and N. Matsui, "Design of 12Slot-10Pole Permanent Magnet Flux Switching Machine with Hybrid Excitation for Hybrid electric Vehicle," in Proc. The 5th IET International Conference on Power Electronics, Machine and Drives (PEMD 2010), 2010.

[4] H. Pollock, C. Pollock, R. T. Walter, and B. V. Gorti, "Low cost, high power density, flux switching machines and drives for power tools," in Proc. Conf. Rec. IEEE IAS Annual Meeting, 2003.

[5] C. Pollock, H. Pollock, R. Barron, J. R. Coles, D. Moule, A. Court, and R. Sutton, "Flux-switching motors for automotive applications," IEEE Trans. Ind. Appl, vol. 42, no. 5, pp. 1177-1184, Sep/Oct 2006.

[6] C. Pollock and M. Brackley, "Comparison of the acoustic noise of a flux switching and a switched reluctance drive," in Proc. Conf. Rec. IEEE IAS Annual Meeting, 2001.

[7] R. L. Owen, Z.Q. Zhu, and G.W. Jewell, "Hybrid excited flux-switching permanent magnet machines," in Proc. 13th European Conf. on Power Electronics and Applications, Barcelona, Spain, 2009.

[8] C. Zhao, and Y. Yan, "A review of development of hybrid excitation synchronous machine," in Proc. of the IEEE International Symposium on Industrial Electronics, 2005.

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[9] J. H. Walker, "The theory of the inductor alternator," J. IEE, vol. Vol. 89, no. No. 9, p. pp.227– 241, June 1942.

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[11] Y. Amara, L. Vido, M. Gabsi, E. Hoang, M. Lecrivain, and F. Chabot, "Hybrid Excitation Synchronous Machines: Energy Efficient Solution for Vehicle Propulsion," in IEEE Vehicle Power and Propulsion Conference, VPPC 06, 2006.

[12] S. E. Rauch, and L. J. Johnson, "Design principles of flux-switch alternators," Trans.AIEE, vol. Vol 74, no. Pt 3, No 3, pp. 1261-1268, Jan 1995.

[13] C. Pollock, H. Pollock, and M. Brackley, "Electronically controlled flux switching motors: A comparison with an induction motor driving an axial fan," in Proc. Conf. Rec. IEEE IAS Annual Meeting, 2003.

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[16] E. Sulaiman, "Design Studies on Less Rare-Earth and High Power Density Flux Switching Motors with Hybrid Excitation/ Wound Field Excitation for HEV Drives," Nagoya Institute of Technology, Nagoya, 2012.

[17] E. Sulaiman, T. Osaka, and N. Matsui, "Design and Performance of 6-Slot 5-Pole PMFSM with Hybrid Excitation for Hybrid Electric Vehicle Applications," in International Power Electronics Conference, 2010.

[18] Y. Amara, L. Vido, M. Gabsi, E. Hoang, M. Lecrivain, and F. Chabot, "Hybrid Excitation Synchronous Machines: Energy Efficient Solution for Vehicle Propulsion”,," in IEEE Vehicle Power and Propulsion Conference, 2006.

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