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DESIGN OPTIMIZATION OF SINGLE-PHASE INNER-ROTOR AND OUTER-ROTOR HYBRID EXCITATION FLUX SWITCHING MACHINE FOR EV APPLICATIONS MOHAMED MUBIN AIZAT BIN MAZLAN UNIVERSITI TUN HUSSEIN ONN MALAYSIA

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Page 1: MOHAMED MUBIN AIZAT BIN MAZLANeprints.uthm.edu.my/id/eprint/8839/1/MOHAMED_MUBIN_AIZAT... · 2017-02-02 · Kenderaan elektrik dianggap sebagai kereta yang mesra alam dan ini dijangka

DESIGN OPTIMIZATION OF SINGLE-PHASE

INNER-ROTOR AND OUTER-ROTOR HYBRID

EXCITATION FLUX SWITCHING MACHINE FOR

EV APPLICATIONS

MOHAMED MUBIN AIZAT BIN MAZLAN

UNIVERSITI TUN HUSSEIN ONN MALAYSIA

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DESIGN OPTIMIZATION OF SINGLE-PHASE INNER-ROTOR AND

OUTER-ROTOR HYBRID EXCITATION FLUX SWITCHING MACHINE

FOR EV APPLICATIONS

MOHAMED MUBIN AIZAT BIN MAZLAN

A thesis submitted in

fulfillment of the requirement for the award of the

Master of Electrical Engineering

Faculty of Electric and Electronic Engineering

Universiti Tun Hussein Onn Malaysia

MARCH, 2016

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For my beloved mother and father,

Che Zarah Binti Mohd Zain and Mazlan bin Mamat,

my siblings,

Muizzuddin Azfar Mazlan and Murtaza Asmuin Mazlan

my friends,

and my lovely family

Thank you for your prayers, support, guidance and love

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ACKNOWLEDGEMENT

In the name of Allah s.w.t, Most Gracious Most Merciful. I would like to

express my sincere appreciation to my supervisor, Dr. Erwan bin Sulaiman for the

support given throughout the duration of this master project.

The cooperation given by lecturer and technician, especially from Faculty of

Electrical and Electronic is also appreciated. Discussion and guidance with the

respect of their knowledge are valuable and cannot be forgotten. A lot of thank as

well to my members, laboratory mates, who willing to help in the making of

completing this project.

Furthermore, sincere thanks to my father, Mazlan Bin Mamat and my mother,

Che Zarah Binti Mohd Zain as being the source of inspiration. These

acknowledgements would be incomplete without my special thanks to my family and

members for their prayers, encouragement, love and emotional supports.

Last but not least, appreciation goes to everyone who has contributed directly

or indirectly towards the compilation of this thesis and may your charity and

goodwill will be blessed.

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ABSTRACT

Electric Vehicle (EV) is considered as an ultimate eco-friendly car and this is highly

expected to be popularized in the future. One of the main candidates of electric

machine for an EV drive is a flux switching machine (FSM). However, since the

designed machine consists of three-phase complicated winding, the copper loss

which contributes to efficiency of the machine is expected to be increased.

Furthermore, the three-phase armature winding has a large area size of the total

system. Due to the complicated three-phase armature winding that contribute to high

copper losses, a single-phase inner-rotor and outer-rotor Hybrid Excitation Flux

Switching Machine (HEFSM) with much simpler structure and less armature coil

consumption are introduced in this research. Various characteristics of HEFSM are

investigated by analytical approaching based in finite element analysis using JMAG

software. The project implementation of this research is divided into three parts

including design, analyze and optimize. Firstly, the impact of a rotor pole number of

the proposed is investigated for inner-rotor and outer-rotor configuration in order to

determine the optimal performances of the rotor poles combinations. Then 8S-4P and

8S-8P HEFSM are chosen for optimization analysis. The combination of 8S-8P

inner-rotor HEFSM have best performance with 284Nm maximum torque, 62.98kW

maximum power and 90% efficiency. Then 8S-8P HEFSM have been compared with

three-phase 12S-14P HEFSM in term of copper loss, weight and efficiency. As

conclusion, the final design machine produce 12.45% less copper loss, 8.88% less

weight and with almost similar efficiency compared to three-phase configuration.

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ABSTRAK

Kenderaan elektrik dianggap sebagai kereta yang mesra alam dan ini dijangka sangat

popular pada masa akan datang. Calon utama mesin elektrik untuk kegunaan

kenderaan elektrik adalah mesin pensuisan fluks. Walau bagaimanapun, oleh kerana

mesin direka terdiri daripada penggulungan tiga-fasa yang rumit, kehilangan

tembaga yang menyumbang kepada kecekapan mesin dijangka akan meningkat.

Tambahan pula, penggulungan angker tiga-fasa mempunyai saiz yang besar daripada

jumlah sistem. Disebabkan angker penggulungan tiga-fasa yang rumit menyumbang

kepada kerugian tinggi tembaga, pemutar dalam fasa tunggal dan pemutar luar

HEFSM dengan struktur lebih mudah dan kurang penggunaan gegelung angker

diperkenalkan dalam kajian ini. Dalam tesis ini, pengoptimuman reka bentuk

konfigurasi pemutar dalam dan luar rotor HEFSM dianalisis. Pelbagai ciri-ciri

HEFSM disiasat oleh analisis berdasarkan Perisian JMAG-Designer. Pelaksanaan

projek penyelidikan ini dibahagikan kepada tiga bahagian termasuk reka bentuk,

analisis dan mengoptimumkan rekaan. Pertama, kesan bilangan kutub motor yang

dicadangkan dengan lapan slot pemegun disiasat untuk konfigurasi pemutar dalam

dan luar bagi menentukan prestasi optimum untuk persembahan gabungan kutub

pemutar. Kemudian 8S-4P dan 8S-8P HEFSM dipilih untuk analisis pengoptimuman.

Gabungan 8S-8P pemutar dalam HEFSM mempunyai prestasi terbaik dengan tork

maksimum 284Nm, kuasa maksimum 62.98kW dan kecekapan 90%. Kemudian 8S-

8P HEFSM telah dibandingkan dengan tiga fasa 12S-14P HEFSM dari segi

kehilangan tembaga, berat dan kecekapan. Kesimpulannya, fasa tunggal

penggulungan menghasilkan 12.45% kurang kehilangan tembaga, 0.67%, 8.88%

kurang berat dan kecekapan hampir sama berbanding dengan tiga fasa penggulungan.

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CONTENTS

TITLE i

DECLARATION ii

DEDICATION iii

ACKNOWLEDGEMENT iv

ABSTRACT v

ABSTRAK vi

CONTENTS vii

LIST OF TABLES xii

LIST OF FIGURES xiii

LIST OF ABBREVIATIONS xv

LIST OF PUBLICATIONS

LIST OF AWARDS

xvi

xviii

CHAPTER 1 INTRODUCTION

1.1 Introduction 1

1.2 Problem Statement 3

1.3 Objectives 4

1.4 Scope 5

1.5 Outlines of Thesis 6

CHAPTER 2 LITERATURE REVIEW

2.1 Introduction to Flux Switching Machine 8

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2.1.1 Permanent Magnet FSM 9

2.1.2 Field-Excitation FSM 10

2.1.3 Hybrid Excitation FSM 11

2.2 Outer-Rotor vs. Inner-Rotor Configuration 12

2.3 Reviews on Three-Phase Winding of Flux Switching 14 Machine (FSM)

2.4 Reviews on Single-Phase Winding of Flux Switching 17

Machine (FSM)

2.5 Summary 19

CHAPTER 3 METHODOLOGY

3.1 Project Methodology 20

3.2 Part 1: Design 21

3.3 Part 2: Analysis 25

3.4 Part 3: Optimize 26

3.5 Summary 29

CHAPTER 4 RESULTS

4.1 Various Rotor Pole Analysis 30

4.1.1 Inner-rotor and Outer-rotor HEFSM Various Rotor 30 Pole Analysis

4.1.2 No Load Analysis 32

4.1.2.1 Flux Linkage at Maximum DC FEC 32

Current Density, JE

4.1.2.2 Induced Voltage at Open Circuit Condition 33

4.1.2.3 Cogging Torque 34

4.1.3 Load Analysis 35

4.1.3.1 Torque and Power vs. JE at Maximum 35 Armature Coil Current Density, JA

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4.1.4 Summary of Rotor Poles Study 37

4.2 Design Optimization Single-Phase Inner-Rotor 37 and Outer-Rotor 8S-4P and 8S-8P HEFSM

4.2.1 No Load Analysis 45

4.2.1.1 Flux Linkage at PM and Maximum 45

DC FEC Current Density, JE

4.2.1.2 Cogging Torque 46

4.2.1.3 Induced Voltage/Back EMF of PM 48

with DC FEC

4.2.2 Load Analysis 49

4.2.2.1 Torque versus FEC Current Density, JE 49

at Maximum Armature Coil Current Density, JA

4.2.2.2 Instantaneous Torque Characteristic of 52

Maximum JE and JA

4.2.2.5 Rotor Mechanical Strength 53

4.2.2.4 Torque and Power Vs. Speed 56

Characteristic

4.2.2.5 Motor Losses and Efficiencies 59

4.2.3 Summary of Optimization 64

CHAPTER 5 CONCLUSION AND RECOMMENDATION

5.1 Introduction 66

5.2 Conclusion 66

5.3 Future Work 67

REFERENCES 68

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LIST OF TABLES

1.1 Design Restrictions and Specifications of HEFSM 5

3.1 Material for Rotor, Stator, Armature Coil, Permanent 25

Magnet and FEC

4.1 Parameter of Inner-Rotor and Outer-Rotor HEFSM 32

4.2 Summary of Rotor Pole Study for Inner-Rotor HEFSM 37

4.3 Summary of Rotor Pole Study for Outer-Rotor HEFSM 37

4.4 Design Parameters of Initial and Final 8S-4P Inner- 42

Rotor and Outer-Rotor HEFSM

4.5 Design Parameters of Initial and Final 8S-8P Inner- 42

Rotor and Outer-Rotor HEFSM

4.6 Input Current of FEC of Initial and Final 8S-4P Inner- 50

Rotor and Outer-Rotor HEFSM

4.7 Input Current of FEC of Initial and Final 8S-4P Inner- 50

Rotor and Outer-Rotor HEFSM

4.8 Summary of Instantaneous Torque for Final Design 52

HEFSMs

4.9 Weight, Power and Torque Density of Final Design 59

HEFSM

4.10 Loss and Efficiency of Inner0Rotor and Outer-Rotor 63

8S-4P HEFSM

4.11 Loss and Efficiency of Inner0Rotor and Outer-Rotor 63

8S-8P HEFSM

4.12 Overall Performances of The Design of Single-Phase 64

8S-4P and 8S-8P Inner-Rotor and Outer-Rotor HEFSM

4.13 Comparison Single-Phase 8S-8P and Three-Phase 12S- 65

14P Inner-Rotor and Outer-Rotor Configuration

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LIST OF FIGURES

1.1 Four Main Candidates of Electric Machine for HEV 2

Drives

2.1 Classification of Flux Switching Machine (FSM) 8

2.2 Operating Principle of Permanent Magnet Flux 9

Switching Machine (PMFSM)

2.3 Operating Principle of Field Excitation Flux Switching 10

Machine (FEFSM)

2.4 Operating Principle of Hybrid Excitation Flux 12

Switching Machine (HEFSM)

2.5 Operating Principle of Outer-rotor HEFSM 13

2.6 Example of Three-Phase FSM 16

2.7 Example of Single-Phase FSM 18

3.1 Project Implementation 20

3.2 Design and Condition Setting Proposed Inner-Rotor 21

and Outer-Rotor HEFSM

3.3 Initial Design of HEFSM 22

3.4 Direction of Permanent Magnet 23

3.5 Direction of FEC 24

3.6 The Direction of Armature Coil 25

3.7 Analysis Procedure 26

3.8 Optimization Procedure 27

3.9 Design Parameter of Inner-Rotor and Outer-Rotor 27

HEFSM

4.1 Initial Design of the IR-HEFSM Configurations 31

4.2 Initial Design of the OR-HEFSM Configurations 31

4.3 Magnetic Flux Linkage at Various Rotor Pole Numbers 33

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4.4 Induced Voltage at Various Rotor Pole Numbers 34

4.5 Cogging Torque 35

4.6 Torque versus JE at Maximum JA 36

4.7 Power versus JE at Maximum JA 36

4.8 Comparison of Torque and Power at Various 38

Topologies

4.9 Design Parameter 38

4.10 Torque versus D1 Characteristic 39

4.11 Torque versus D2 and D3 Characteristic 39

4.12 Torque versus D5 and D6 Characteristic 40

4.13 Torque versus D7 and D8 Characteristic 40

4.14 Torque versus D9 and D10 Characteristic 41

4.15 Torque versus Cycle 41

4.16 Design of Single-Phase 8S-4P 43

4.17 Design of Single-Phase 8S-8P 44

4.18 Flux Linkage of PM with DC FEC 46

4.19 Cogging Torque 47

4.20 Induced Voltage/ Back EMF of PM with DC FEC 48

4.21 Torque versus FEC Current Density, JE at Maximum 51

Armature Coil Current Density, JA

4.22 Instantaneous Torque of the Design HEFSMs 53

4.23 Rotor Mechanical Stress Distribution at 20,000r/min 54

4.24 Torque versus Speed Characteristics 57

4.25 Power versus Speed Characteristics 58

4.26 Estimated Coil End Volume of Final Design HEFSM 59

4.27 HEFSMs Losses and Efficiencies 61

4.28 Iron Loss and Copper Loss Distributions 62

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LIST OF ABBREVIATIONS

A Ampere

AC Alternating Current

Dy Dysprosium DC

Direct Current

EV Electric Vehicle

FEA Finite Element Analysis

FEC Field Excitation Coil

FEFSM Field Excitation Flux Switching Motor

HEFSM Hybrid Excitation Flux Switching Motor

HEV Hybrid Electric Vehicle

EV Electric Vehicle

IMs Induction Motors

IPMSMs Interior Permanent Magnet Synchronous Motors

ICE Internal Combustion Engine

JE FEC current density

JA Armature coil current density

kg Kilogram

Mm Millimeter

Nm Newton meter

Nd Neodymium

PM Permanent Magnet

PMFSM Permanent Magnet Flux Switching Motor

r/min Revolution per minute

V Volt

Wb Weber

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LIST OF PUBLICATIONS

Journals:

(i)

Mohamed Mubin Aizat Mazlan, Erwan Sulaiman, Md Zarafi Ahmad,

Zhafir Aizat Husin and Hassan Ali Soomro, “Design Optimization of

Single-Phase Outer-Rotor 8S-8P Hybrid Excitation Flux Switching Motor

for Electric Vehicle”, Journal of Applied Mechanics and Materials, Vol.

695, pp. 761-764, Nov 2014.

(ii) Mohamed Mubin Aizat Mazlan, Erwan Sulaiman, Md Zarafi Ahmad,

Zhafir Aizat Husin, Siti Nur Umira Zakaria, “Performance Comparison of

Optimum 8S-4P and 8S-8P of Single-Phase Hybrid Excitation Flux

Switching Machine with Outer-Rotor Configuration’’, Journal of Applied

Science and Agriculture, Vol. 9, pp 112-118, Oct 2014.

Proceedings:

(i)

Mohamed Mubin Aizat Bin Mazlan, Erwan Bin Sulaiman, and Takeshi

Kosaka “Design Study of Single-Phase Outer-Rotor Hybrid Excitation Flux

Switching Machine for Hybrid Electric Vehicles”, IEEE 8th International

Power Engineering and Optimization Techniques, Mar. 2014.

(ii) Mohamed Mubin Aizat Mazlan, Zhafir Aizat Husin, Syed Muhammad

Naufal Syed Othman and Erwan Sulaiman “Design Study of Single-Phase

Inner-Rotor Hybrid Excitation Flux Switching Machine for Hybrid Electric

Vehicles”, 2nd Power and Energy Conversion Symposium (PECS 2014),

May 2014.

(iii) Mohamed Mubin Aizat Mazlan, Erwan Sulaiman, Zhafir Aizat Husin, Syed

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Muhammad Naufal Syed Othman and Faisal Khan “Design Comparison of

Single Phase Outer and Inner-Rotor Hybrid Excitation Flux Switching

Motor for Hybrid Electric Vehicles”, International Conference on

Mathematics, Engineering & Industrial Applications (ICoMEIA), May

2014.

(iv) Mohamed Mubin Aizat Mazlan, Erwan Sulaiman, Md Zarafi Ahmad, Syed

Mohammad Naufal Syed Othman, “Topologies of Single-Phase Outer-

Rotor Hybrid Excitation Flux Switching Motor for In Wheel Drive

Applications”, IEEE Conference on Energy Conversion (CENCON), Oct.

2014.

(v) Mohamed Mubin Aizat Mazlan, Md Zarafi Ahmad, Syed Mohammad

Naufal Syed Othman and Erwan Sulaiman, “Design Studies and

Performance of Single-Phase HEFSM with Various Rotor Pole Number for

Hybrid Electric Vehicle Applications”, Malaysian Technical Universities

Conference on Engineering and Technology (MUCET), Nov. 2014.

(vi) Mohamed Mubin Aizat Mazlan, Erwan Sulaiman, Md Zarafi Ahmad,

Zhafir Aizat Husin, Siti Nur Umira Zakaria, “Performance Comparison of

Optimum 8S-4P and 8S-8P of Single-Phase Hybrid Excitation Flux

Switching Machine with Outer-Rotor Configuration”, International

Postgraduate Conference on Engineering and Technology Research

(IPCETR), Oct. 2014.

(vii) Mohamed Mubin Aizat Mazlan, Erwan Sulaiman, Md Zarafi Ahmad, Syed

Muhammad Naufal Syed Othman, “Design Optimization of Single-Phase

Outer-Rotor Hybrid Excitation Flux Switching Motor For Electric

Vehicles”, IEEE Student Conferences on Research and Development (IEEE

SCoRED), Dec. 2014.

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LIST OF AWARDS

(i)

(ii)

(iii)

(iv)

Bronze medal “Outer-Rotor Hybrid Excitation Flux Switching Machine for

In-Wheel Drive Electric Vehicle”, UTHM Research and Innovative Festival

2013, Dec 2013.

Best paper award “Performances Comparison of 12S-10P and 12S-14P of

Field Excitation Flux Switching Motor for Hybrid Electric Vehicle”, 2nd

Power and Energy Conversion Symposium (PECS 2014), May 2014.

Best paper award “Performance Analysis of 12Slot-14Pole for HEFSM and

FEFSM with Outer-Rotor Configuration”, 2014 Malaysian Technical

Universities Conference on Engineering and Technology (MUCET 2014),

Nov. 2014.

Bronze medal ‘In-Wheel HEFSM’, Malaysian Technology Expo 2015, 12-14

Feb. 2015.

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CHAPTER 1

INTRODUCTION

1.1 Introduction

With the increasing number of world population, the demand for vehicles for

personal transportation has increased dramatically in the past decades. This leads to

serious problems called ‘global warming’. One of the main causes of global warming

is Internal Combustion Engine (ICE). From the report in year 2013 [1], about 26% of

global carbon dioxide (CO2) emission in year 2013 came from the vehicles. By the

year 2020, it is expected that CO2 emission rate from vehicles will increase two times

with economic growth.

Hybrid Electric Vehicle (HEV) is considered as an ultimate eco-friendly car

and this is highly expected to be popularized in the future [2]-[4]. The important of

the basic characteristic requirements of an electric motor for HEV drive systems are

high torque at low speed, high power density, and constant power at high speed as

well as high efficiency [5].

Electric vehicles (EVs) seem like an ideal solution to deal with the energy

crisis and global warming since they have zero oil consumption and zero emissions.

EVs have several advantages over HEV such as EVs emit no tailpipe pollutants,

although the power plant producing the electricity may emit them and EV provide

quiet, smooth operation and stronger acceleration and require less maintenance than

HEV. Therefore, EV is now regarded as an ultimate eco-friendly car and is widely

expected to become more popular in the very near future [6]-[8].

Various electric motors used in HEV and EV have been designed and

successfully installed in the vehicles such as Honda Jazz, Toyota Prius, Mitsubishi

Mirage and Nissan Leaf as illustrated in Figure 1.1. Figure 1.1(a) illustrates an

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example of Permanent Magnet Synchronous Machine (PMSMs) installed in Lexus,

Prius and Nissan Leaf. Although PMSM has the advantage of high torque density

and high efficiency, still it has the problem of PM demagnetization, mechanical

damage of rotor’s magnet and uncontrolled flux of PM [9]-[11].

(a) (b)

(c) (d)

Figure1.1: Four Main Candidates of Electric Machine for HEV Drives

(a) Permanent Magnet Synchronous Machines (b) DC motor (c) Induction Motor

(d) Switched Reluctant Motor

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Furthermore, Figure 1.1(b) depicts an example of Direct Current (DC) motor

used in HEV and EV. Since DC motor utilizes DC supply battery, the control

principle becomes simpler that makes it widely accepted in electric propulsion

system. However, DC motor drives have major disadvantages such as low reliability

and high maintenance [12]. Thus DC motors are unsuitable for maintenance-free

drives.

At present, induction motor (IM) as shown in Figure 1.1(c), are generally

established as the most potential candidate for the electric propulsion of EV and

HEVs, due to their reliability, ruggedness, low maintenance, and low cost [13]-[14].

However, IM drives have demerits such as high loss, low efficiency and low power

factor [15]-[17].

Figure 1.1(d) shows the structure of a switched reluctant motor (SRM) which

is invented to overcome the permanent magnet motor problem. SRM has no PM and

robust rotor structure but it is not suitable for HEV and EV due to large torque

ripples and noisy [18]-[19]. Although the SRMs have been successfully installed in

HEV and EV, the drawbacks of each electric motor can further be improved and

optimized.

In order to overcome the previous motor problems, hybrid excitation flux

switching machine (HEFSM) in which all flux source are located in stator body is

introduced in this research. Proposed HEFSM that consists of permanent magnet

(PM) and field excitation coil (FEC) as main flux sources is more advantageous

compared to existing electric motor [20]-[21]. HEFSM with a robust rotor structure

similar with SRM is suitable for extreme driving condition. Additionally, an extra

advantage of locating PM and FEC at the stator core provide a simple cooling system

for this machines. In addition, the FEC can control constant PM flux to produce

variable flux capabilities, which can enhance more torque and power.

1.2 Problem Statement

Several invention of HEFSM for EV application has been proposed. Three-phase

HEFSM have been developed for various EV drives applications with strong

performance in term of high torque, high power and high speed ability. This is

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proven by three-phase inner-rotor HEFSM [2] and outer-rotor HEFSM [21].

However, the proposed machines have problems of high torque ripple and high

induced voltage [22]-[24]. Moreover, since the designed machine consists of three-

phase complicated winding, the copper loss which contributes to efficiency of the

machine is expected to be increased. Furthermore, the three-phase winding has high

voltage supply and use big battery size and complex inverter. Therefore the three-

phase armature winding has a large area of the total system [25]. Due to complicated

three-phase armature winding that contribute to high copper losses, a single-phase

inner-rotor and outer-rotor HEFSM with much simpler structure and less armature

coil consumption are introduced in this research. It is obvious that both inner rotor

and outer-rotor configurations can be applied for normal and direct drive HEV and

EV system respectively. Moreover, single-phase also requires low voltage supply,

uses small battery size and simple inverter. Therefore the single-phase armature

winding has a small area of the total system.

The performances of the proposed machine under some restrictions and

specifications will be analyzed and evaluated. The proposed machine is expected to

provide high efficiency, high durability and less copper losses compared to the three-

phase winding of HEFSM.

1.3 Objectives of Project

The objectives of this research are:

(i) To design a single-phase inner-rotor and outer-rotor hybrid excitation flux

switching motor for electric vehicle applications.

(ii) To analyze a single-phase inner-rotor and outer-rotor hybrid excitation flux

switching motor for electric vehicle applications.

(iii) To optimize the performances of the 8S-4P and 8S-8P single-phase inner-

rotor and outer-rotor hybrid excitation flux switching motor for electric

vehicle applications.

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1.4 Scopes of Project

The scopes of this research are divided into three parts based on the objectives. The

scopes are:

(i) The design restrictions, target specifications and parameters of the proposed

HEFSM for EV applications are listed in Table 1.1 [26]. The electrical

restrictions related with the inverter such as maximum 240V DC bus voltage

and maximum 360A inverter current are set. Assuming water jacket system is

employed as the cooling system for the machine, the limit of the current

density is set to the maximum 30Arms/mm2 for armature winding and 30A/mm2 for FEC, respectively. The outer diameter, the motor stack length,

the shaft radius and the air gap of the main part of the machine design being

264mm, 70mm, 30mm and 0.8mm respectively. The target of maximum

torque and power for proposed single-phase are 111Nm and 41kW

respectively which are one third of three-phase HEFSM.

(ii) The performances of rotor poles study are investigated in order to determine

the optimal performances. The no load and load analysis such as flux linkage,

cogging torque, induced voltage and torque and power vs. JE are determined.

Table 1.1: Design Restrictions and Specifications of HEFSM [26]

Items Unit Three-Phase

HEFSM

Single-Phase

HEFSSM

Max. DC-bus voltage inverter V 650 240

Max. inverter current Arms 360 360

Max. current density in armature winding, Ja Arms/mm2 30 30

Max. current density in excitation winding, Je A/mm2 30 30

Stator outer diameter mm 264 264

Motor stack length mm 70 70

Shaft radius mm 30 30

Air gap length mm 0.80 0.80

PM weight kg 1 1

Maximum torque Nm >333 >111

Maximum power kW >123 >41

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(iii) The motor 8S-4P and 8S-8P single-phase inner-rotor and outer-rotor

configuration are chosen from rotor pole analysis and are optimized by using

deterministic optimization method [27] and treated to all parameters until the

optimum performances are achieved. Then the outer-rotor motor is compared

to inner-rotor 8S-4P and 8S-8P HEFSM with the same design restrictions and

specifications. Finally, loss analysis, structural analysis and efficiency are

analyzed and compared for 8S-4P and 8S-8P inner-rotor and outer-rotor

configuration HEFSM.

1.5 Outlines of Thesis

This thesis deals with the design studies on single-phase inner-rotor and outer-rotor

hybrid excitation flux switching machine (HEFSM) for EV applications. The thesis

is divided into 5 chapters and the summary of each chapter are listed as follows:

(i) Chapter 1: Introduction

The first chapter gives some introduction about the research including

research background, related works on EV and some explanation regarding

inner-rotor and outer-rotor configuration used in EV. Then problems of

current three-phase winding used in EV are highlighted and the research

objectives are set to solve the problems.

(ii) Chapter 2: Literature Review

The second chapter explains some introduction and classifications of FSM

including the example of PMFSM, HEFSM and FEFSM, the operating

principle and the proposed HEFSM for HEV applications. Then the review of

single-phase for all FSM is explained.

(iii) Chapter 3: Methodology

The third chapter describes the project implementation of this research. The

project implementation is divided into three parts including design, analysis

and optimization. The design is divided into two parts that are geometry

editor and JMAG-Designer. Then the design is analyzed at no load and load

analysis such as flux linkage, cogging torque, induced voltage and torque and

power vs. maximum JE. Finally the “deterministic optimization method” is

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used and treated to all parameters until the optimum performances are

achieved.

(iv) Chapter 4: Result

In this chapter, various combinations of slot-pole inner-rotor and outer-rotor

HEFSMs such as 8S-4P, 8S-8P, 8S-12P, 8S-16P and 8S-20P are designed and

analyzed. Among various slot-pole combinations of HEFSM, the combination

of 8S-4P and 8S-8P of inner-rotor and outer-rotor configuration has better

performance and chosen for design optimization. The design is optimized by

using deterministic optimization method and treated to all parameters until

the optimum performances are achieved. The results of the initial and final

design which met the target performances such as maximum flux linkage,

cogging torque, induced voltage, instantaneous torque characteristic, rotor

mechanical stress and motor losses and efficiency are analyzed and discussed.

(v) Chapter 5: Conclusion

The final chapter describes and concludes the summary of the research and

pointed out some future works for design improvements.

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CHAPTER 2

LITERATURE REVIEW

2.1 Introduction to Flux Switching Motor

Generally, the flux switching motor (FSM) 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 PMFSM and FEFSM has only PM and field excitation coil (FEC), respectively

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

flux sources. Figure 2.1 illustrates the general classification of FSM.

Flux Switching Motor (FSM)

Permanent Magnet (PM) FSM

Field Excitation (FE) FSM

Hybrid Excitation (HE) FSM

Figure 2.1: Classification of Flux Switching Machine (FSM)

FSM consists of the rotor and stator. The rotor consist of only single structure

which is iron core thus allowing its simple construction and inherent robustness to be

retained while both field and armature windings are on the stator. The operation of

the motor is based on the principle of switching flux. The term “flux switching” is

coined to describe machines in which the stator tooth flux switches polarity

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following the motion of a salient pole rotor [28-29]. All excitation sources are on the

stator with the armature and field allocated to alternate stator teeth.

Flux is produced in the stator of the machine by permanent magnet or by dc

current flowing in the field winding. The orientation of the field flux is then simply

switched from one set of stator poles to another of stator poles by reversing the

polarity of the current in the armature winding.

2.1.1 Permanent Magnet Flux Switching Motor

Permanent magnet flux switching motor (PMFSM) is a simple construction. The

stator consists of PM and armature windings and due to this it provides some

advantages such easy cooling and better suitability for high speed applications [30].

PMFSM is popular due to high power density, efficiency and it uses PM to generate

flux. Unfortunately, the generated flux produced is fixed and will not change-

diverged which means it is constant flux because of characteristics of the PM.

Stator Stator

PM PM

Armature Coil

Rotor Rotor

(a) (b)

Figure 2.2: Operating Principle of PMFSM (a) Flux Linkage Correspond to One

Polarity (b) Flux Linkage Switch Polarity as the Salient Pole Rotates [31]-[33]

Figure 2.2 demonstrates the general ideal of the operating principle of the

PMFSM where the red arrows indicate the flux line of PM as an instance. The flux-

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linkage corresponds to one polarity is when the relative position of the rotor poles

and a particular stator tooth are as in Figure 2.2 (a). But in Figure 2.2 (b) the polarity

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

tooth changes. The salient pole rotor rotates when the flux linkage switches polarity

[31]-[33].

2.1.2 Field Excitation Flux Switching Motor

In spite of the fact that permanent magnet (PM) machines exhibit high torque density

and high efficiency, the rare earth magnet material, is expensive and the working

environmental temperature may limit its application [34]-[36].

Stator Stator

FEC FEC FEC FEC

Armature Coil

Rotor Rotor

(a) (b)

Stator Stator

FEC FEC FEC FEC

Armature Coil

Rotor Rotor

(c) (d)

Figure 2.3: Operating Principle 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

[37]-[39]

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A Flux-switching machine with field excitation coil is recommended in order

to reduce the cost. The conventional DC winding excited synchronous machine

employs the field winding on the rotor and the slip-rings are required to supply the

field current [33].

Figure 2.3 (a) reveals the operating principle of the FEFSM and Figure 2.3 (b)

reveals the direction of the FEC fluxes into the rotor. Figure 2.3 (c) and (d) indicate

the direction of FEC fluxes into the stator which produces a complete one cycle flux.

Alike 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 2.3(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

[37]-[39].

2.1.3 Hybrid Excitation Flux Switching Motor

Hybrid Excitation Flux Switching Motor (HEFSM) is the combination of PM and

FE. HEFSM has significantly less magnet and higher torque density than those of a

conventional PMFSM.

By applying negative d-axis current, the PM flux can be counteracted but

with the disadvantage of increase in copper loss and thereby reducing the efficiency,

reduced power capability, and also possible irreversible demagnetization of the PMs.

Thus, HEFSM is an alternative option where the advantages of both PM machines

and DC FEC synchronous machines 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 [40].

The operating principle of the proposed HEFSM is illustrated in Figure 2.4,

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

Figure 2.4(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 2.4(c) and

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(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 [41]-[42].

Stator Stator

FEC FEC

PM PM

Armature Coil

Rotor Rotor

Stator

(a) (b) Stator

FEC FEC

PM PM

Armature Coil

Rotor (c) (d)

Rotor

Figure 2.4: Operating Principle of HEFSM (a) θe=0°-More Excitation

(b) θe=180°-More Excitation (c) θe=0°-Less Excitation

(d) θe=180°-Less Excitation [41]-[42]

2.2 Outer-Rotor vs. Inner-Rotor Configurations

Most of commercial EV used single motor and transmission gears coupled to the

wheels. This system leads to the transmission losses and reduce the efficiency and

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reliability of the motor [43]-[44]. Therefore, in-wheel direct drive mechanism is

introduced to overcome this problem. In-wheel direct drive eliminates the

mechanical transmission, differential gears and drive belts.

Rotor Rotor

Armature Coil

PM PM

FEC FEC Stator Stator

(a) (b)

Rotor Rotor

Armature Coil

PM PM

FEC FEC Stator Stator

(c) (d)

Figure 2.5: Operating Principle of Outer-rotor HEFSM (a) θe = 0º (b) θe = 180º

More Excitation, (c) θe = 0º (b) θe = 180º Less Excitation [56]-[57]

Since the in-wheel direct drive with outer-rotor configuration is more

practical for direct drive application, several invention of in-wheel mechanism for

EV application has been proposed. For example 12S-22P outer-rotor permanent-

magnet flux-switching machine (PMFSM) for electric propulsion in a lightweight

electric vehicle has been proposed [45]. The proposed machine is a highly possible

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candidate for in-wheel direct-drives. This PMFSM has physical compactness, robust

rotor structure, higher torque and power density and high efficiency. However

PMFSM has several disadvantages of uncontrolled flux and demagnetization [46].

The operating principle of OR-HEFSM is illustrated in Figure 2.5. The single

piece of rotor that makes the motor more robust similar to SRM is shown in the

upper part, while the stator that consists of PMs, FECs, and armature coils are

located in the lower part. The PM and FEC are placed between two stator poles to

generate excitation fluxes that create the term of “hybrid excitation flux”. Figure 2.5

(a) and (b) demonstrate the flux generated by PM and FEC flow from the stator into

the rotor and from the rotor into the stator, respectively, to produce a complete one

flux cycle. The combined flux generated by PM and FEC established more excitation

fluxes that are required to produce higher torque of the motor. When the rotor rotate

clockwise, the rotor pole goes to the next stator tooth, hence switching the magnitude

and polarities of the flux linkage. The flux does not rotate but shifts clockwise and

counter clockwise in direction with each armature current reversal. According to

Figure 2.5 (c) and (d), only the PM flux flows from the stator into the rotor and from

the rotor into the stator, respectively, while the FEC flux is only circulating on its

particular winding slots. This condition establishes less excitation flux and generates

less torque [47]-[48].

2.3 Reviews on Three-Phase Winding of Flux Switching Machine (FSM)

Early examples of three-phase Flux Switching Machine (FSM), the three-phase

PMFSM, FEFSM and HEFSM are developed as shown in Figure 2.6 (a), (b) and (c),

respectively. Figure 2.6(a) shows a typical three-phase 12S-10P PMFSM, where the

salient pole stator core consists of modular U-shaped laminated segments placed next

to each other with circumferentially magnetized PMs placed in between them. For

the flux switching principles, the PM magnetization polarity is being reversed from

one magnet to another [49]-[51].

The stator armature winding consists of concentrated coils and each coil

being wound around the stator tooth formed by two adjacent laminated segments and

a magnet. The salient pole rotor is similar to that of SRMs, which is more robust and

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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.

In addition, since the flux path generated by mmf of the armature windings

and PMs are magnetically in parallel, rather than in series as in conventional

IPMSM, the influence of the armature reaction field on the working point of the PMs

is almost eliminated. As a result, the specific electric loading and the specific torque

capability of a PMFSM can be increased. In addition, a high per-unit winding

inductance can be readily achieved. Thus, such machines are eminently suitable for

constant power operation over a wide speed range, i.e., they can have a high flux-

weakening capability [52].

The 12S-10P FEFSM in Figure 2.6(b) is redesigned from the 12S-10P

PMFSM in Figure 2.6(a) in which the PM is removed from the stator and half of the

armature coil slots in the upper layer are placed with the FEC windings as explained

in [53]. The FEC are arranged with alternate DC current source polarity to produce

two flux polarities, similar with PM polarity of 12S-10P PMFSM discussed in Figure

2.6(a). However, since the isolated and unused stator teeth reduce the performance of

the machine, further investigations into improvements of the machine design of three

phase FEFSMs should be made.

Meanwhile, the HEFSM shown in Figure 2.6(c) is a 3-phase 12S-10P

PMFSM which incorporates the FEC at outer extremity of the stator [54]-[55].

However, the outer diameter of the machine is significantly enlarged for the FEC

winding, which in turn reduces torque density. In addition, the PMs in the PMFSM

can be partially replaced by the DC FEC windings and consequently, several

HEFSM topologies were developed as in [56]-[57]. Although they have no

overlapped between the armature coil and FEC, the torque capability is significantly

reduced due to less PM volume.

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FEC PM

Rotor Rotor

Stator Armature

Coil

Stator

Armature Coil

(a) (b)

FEC PM

Rotor

Stator (c)

Armature Coil

Figure 2.6: Example of Three-Phase FSM (a) Three-Phase PMFSM

(b) Three-Phase FEFSM (c) Three-Phase HEFSM

Furthermore, it is clear that to realize the hybrid topology of Figure 2.6(c),

both PM and armature coil volume should be sacrificed, when compared with the

conventional 3-phase 12S-10P PMFSM of Figure 2.6(a), while keeping the machine

stator outer radios as constant. From the conventional PMFSM topology, it is

possible to replace some of the magnet material with DC FECs and therefore create

several HEFSM topologies without loss of armature coil. This represents the simplest

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method of hybridizing the conventional PMFSM topology with FEC as it retains the

existing stator and rotor dimensions and structure.

Based on the overview of various three-phase FSMs that have been discussed,

three-phase FSM produce high instant power, high power density, and high power at

high speed for cruising. Three-phase FSM also produce fast torque response and high

torque at low speed for starting and climbing.

2.4 Reviews on Single-Phase Winding of Flux Switching Machine (FSM)

Although a few three-phase FSM have been designed in recent years, the

fundamental three-phase drawbacks such as high copper loss, complicated winding,

high cost and high supply voltage are yet to be overcome. Thus a single-phase FSM

have been fundamentally design. The advantages of single-phase FSM are simple

design due to single winding, less copper loss and easy to manufacture. Single-phase

FSM also less controlled circuit and simple control system compared to three-phase

Figure 2.7 illustrates the single-phase of FSMs.

Figure 2.7(a) shows a typical single-phase 6S-4P PMFSM, where the salient

pole stator ore consists of modular U-shaped laminated segments placed next to each

other with circumferentially magnetized PMs placed in between them. For the flux

switching principles, the PM magnetization polarity is being reversed from one

magnet to another [58]-[59]. The stator armature winding consists of concentrated

coils and each coil being wound around the stator tooth formed by two adjacent

laminated segments and a magnet. In the same figure, all armature coil phases have

the same winding configuration and are placed in the stator core to form 6 slots of

windings. 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. In addition, since the flux path generated by mmf of the

armature windings and PMs are magnetically in parallel, rather than in series as in

conventional IPMSM, the influence of the armature reaction field on the working

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point of the PMs is almost eliminated. As a result, the specific electric loading and

the specific torque capability of a PMFSM can be increased. In addition, a high per-

unit winding inductance can be readily achieved. Thus, such machines are eminently

suitable for constant power operation over a wide speed range, i.e., they can have a

high flux-weakening capability [60].

Stator Stator FEC

Rotor

Rotor

PM Armature Coil

(a) (b)

Armature Coil

FEC

PM Rotor

Stator Armature

Coil

(c)

Figure 2.7: Example of Single-Phase FSM (a) Single-Phase PMFSM

(b) Single-Phase FEFSM (c) Single-Phase HEFSM

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The concept of the FEFSM involves changing the polarity of the flux linking

with the armature winding, with respect to the rotor position. Early examples of

single-phase 4S-2P FEFSM that employs with a DC FEC on the stator, a toothed-

rotor structure and fully-pitched windings on the stator is shown in Figure 2.7(b)

[61]. From the figure, it is clear that two armature coil and FEC windings are placed

in the stator which overlapped each other. The viability of this design was

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

durability [62]–[64]. The novelty of the invention was that the single-phase ac

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

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.

Hybrid excitation flux switching machines (HEFSMs) are those which utilize

primary excitation by PMs as well as DC FEC as a secondary source. HEFSM is an

alternative option where the advantages of both PM machines and DC FEC

synchronous machines are combined. Figure 2.7(c) shows a single-phase 6S-4P

HEFSM in which the active parts are arranged in three layers in the stator. The inner

stator consists of the armature windings, followed by the FECs in the middle layer,

while the PMs are placed in outer stator as discussed in [65]-[66]. However, the

machine has low torque density and long end winding for the DC FECs, which

overlaps the armature windings, and increase copper loss.

2.6 Summary

In this chapter, the overview and classifications of various FSMs are discussed. The

PMFSM, FEFSM and HEFSM have their own advantages and disadvantages which

requires further investigations to extract higher performances for several

applications.

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CHAPTER 3

METHODOLOGY

3.1 Project Methodology

The project implementation of this research is divided into three parts based on

objectives including design, analyze and optimize. The general process of research

methodology is illustrated in Figure 3.1. An analytical study, Finite Element

Analysis (FEA) study based on reluctant network is used to evaluate magnetic flux is

needed to design the inner-rotor and outer-rotor HEFSM. Using FEA based on

JMAG-Designer Software allows obtaining information that is not available through

an actual device test because it gives us substantially greater insight into the device's

performance. JMAG is simulation software for electromechanical design striving to

be easy to use while providing versatility to support users from conceptual design to

comprehensive analyses. JMAG can accurately capture and quickly evaluate

complex physical phenomena inside of machine.

Start

Part 1: Design

Part 2: Analyze

Part 3: Optimize

End

Figure 3.1: Project Implementation

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3.2 Part 1: Design

The project implementation is divided into two parts that are geometry editor and

JMAG-Designer. The design process of single-phase inner-rotor and outer-rotor

HEFSM parts is demonstrated in Figure 3.2.

START

Sketch of Rotor

Sketch of

Stator

Sketch of

Armature coil

Sketch of

FEC

Sketch of Permanent

Magnet

GEOMETRY EDITOR

DESIGNER

Set materials

Set the conditions

Set the NO

circuits

Set the mesh & study

properties

Run and Simulate

YES

END

Figure 3.2: Design and Condition Setting of the Proposed Inner-Rotor

and Outer-Rotor HEFSM

In this design study, the motor are divided into two groups, namely, those

related to stator iron core and rotor iron core. On the stator iron core, it is subdivided

into three components which are the PM shape, FEC slot shape, and armature slot

shape. The rotor parameters involved are the inner rotor radius, rotor pole depth, and

rotor pole arc width. The PM slot shape parameters are the PM depth and the PM

width, while for the FEC slot parameters are FEC slot depth and FEC slot width, and

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respectively. Finally, the armature coil parameters are armature coil slot depth and

the armature coil slot width. The initial designs are demonstrated in Figure 3.3.

Rotor

Rotor

FEC

PM Stator

PM FEC

Armature Coil

Stator Armature

Coil

(a) (b)

Figure 3.3: Initial Design of HEFSM (a) Inner-Rotor HEFSM (b) Outer-Rotor HEFSM

The selections of the initial design single-phase HEFSMs are based on the

main geometrical dimensions identical to existing three-phase HEFSM in which the

stator outer diameter, stack length and shaft are set respectively to 132mm, 70mm

and 30mm as mentioned earlier in Table 1.1 with following assumptions follows:

(i) The rotor radius is 70% for inner rotor and 83% for outer rotor of the size of

motor and both within the range of general machine split ratio [67]-[68].

(ii) The rotor pole depth is half of the rotor to give much depth for the flux to

flow while keeping the suitable distance of the rotor inner part to avoid flux

saturation and to keep the acceptable rotor mechanical strength,

simultaneously.

(iii) The rotor pole width is defined as in equation (3.1) [69].

∑ Stator Tooth Width = ∑ Rotor Tooth Width (3.1)

(iv) The PM depth and width is calculated based on the volume of 1kg permanent

magnet. The PM depth is approximately one third of stator depth and

expecting give more space for flux to flow from stator to rotor. The direction

of permanent magnet are shown in Figure 3.4.

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Rotor

PM

FEC

(a)

Stator Armature

Coil

(b)

Figure 3.4: Direction of Permanent Magnet

(a) Inner-Rotor HEFSM (b) Outer-Rotor HEFSM

(v) The FEC depth and width is calculated based on 147mm2 area of FEC. The

area of FEC, Se is defined by equations 3.2, with the filling factor of motor, α,

and number of turn, Ne set as 0.5 and 44 respectively.

N = J eαS e

e I

(3.2)

e

Where Ne, Je (A/mm2), α, Se (mm2), and Ie (A) are number of turns, current

density, filling factor, slot area and input current, respectively. Assuming

only one water-jackets system is employed as a cooling system, the current

density threshold is set to be 30A/mm2, for FEC winding and the input

current is set 50A as the maximum input current for FEC [71]. The FEC slot

depth is one third of stator depth to give an appropriate distance between two

FEC slot areas for the flux to flow in this area. FEC for the inner-rotor and

outer-rotor HEFSM design contains two parts namely F1 and F2. Both parts

inner and outer-rotor HEFSM for FEC1 and FEC2 is illustrated in Figure 3.5.

(vi) The armature coil depth and width are calculated based on 168mm2 area of

armature coil. The area of armature coil, Sa is defined by equations 3.3, with

the filling factor of motor, α, and number of turn, Na set as 0.5 and 7

respectively.

N = J aαS a

a I

(3.3)

a

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Where Na, Ja (A/mm2), α, Sa (mm2) and Ia (Arms) are number of turns, current

density, filling factor, slot area and input current, respectively. Assuming

only one water-jackets system is employed as a cooling system, the current

density threshold is set to be 30A/mm2, for armature coil winding and the

input current is set 360Arms as the maximum input current for FEC [71]. The

depth of armature coil is set two third of the stator in order to avoid

overlapping between armature coil winding and FEC winding. The direction

of armature coil is shown in Figure 3.6 respectively. The direction of

armature coils is in alternate direction.

F1 o

F1 F2 x x

F2 F1 o o

F1 x

xx oo

F2 o x F2 F1 F2 F2 F1

x oo F1 F1 x F2 F2 F2 F2

x o F2 x o F2 x F1 F1 o

x F1

F1 o o

F2

o F1

x x F1

F2

F1 F1 oo F2F2 xx

(a) (b)

Figure 3.5: Direction of FEC

(a) Inner-Rotor HEFSM (b) Outer-Rotor HEFSM

The design contains stator, rotor, armature coil, permanent magnet and FEC

for inner-rotor and outer-rotor HEFSM uses the different materials. Stator and rotor

use electrical steel 35H210 [69]. The armature coil and FEC use copper as their

material. The PM material used for this motor is Neomax 35AH whose residual flux

density and coercive force at 20°C are 1.2T and 932kA/m, respectively. Table 3.1

shows the material of the motor part.

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