Electromagnetic Performance due to Tooth-tip Des

International Journal of Power Electronics and Drive System (IJPEDS)
Vol. 6, No. 4, December 2015, pp. 860~868
ISSN: 2088-8694  860
Journal homepage: http://iaesjournal.com/online/index.php/IJPEDS
Electromagnetic Performance due to Tooth-tip Design in
Fractional-slot PM Brushless Machines
Mohd Luqman Mohd Jamil1
, Zulfikri Zaki Zolkapli2
, Auzani Jidin3
,
Raja Nor Firdaus Raja Othman4
, Tole Sutikno5
1,2,3,4
Power Electronics & Drive Research Group (PEDG), Universiti Teknikal Malaysia Melaka, Malaysia
5
Department of Electrical Engineering, Universitas Ahmad Dahlan, Yogyakarta, Indonesia
Article Info ABSTRACT
Article history:
Received Aug 20, 2015
Revised Nov 15, 2015
Accepted Nov 28, 2015
Permanent Magnet (PM) machines are favorable as an alternative to other
machine topologies due to simpler construction and high torque density.
However, it may result hight torque ripple due to an influence of cogging
torque and electronic commutation. In this paper, comparisons of phase
back-emf, static torque and cogging torque due to influence of tooth-tip
asymmetry in 12-slot/10-pole double-layer and 12-slot/10-pole single layer
winding machines are carried out using 2D Finite-Element Analysis. At rated
condition, the stator asymmetry has great influence on the torque
performance as there is significant reduction of torque ripple in 12-slot/10-
pole mahine equipped with single layer winding than one equipped with
double layer winding machine. It si confirmed that an optimum torque
performance is desirable via stator iron modification in PM machines.
Keyword:
Cogging Torque
Fractional-slot
Tooth Notch
Tooth-tip Asymmetry
Torque Ripple Copyright © 2015 Institute of Advanced Engineering and Science.
All rights reserved.
Corresponding Author:
Mohd Luqman Mohd Jamil,
Power Electronics and Drives Research Group (PEDG),
Universiti Teknikal Malaysia Melaka,
Hang Tuah Jaya, 76100 Durian Tunggal, Melaka, Malaysia.
Email: luqman@utem.edu.my
1. INTRODUCTION
PM brushless machines have been used in many applications due to the advantages of low copper
loss [1], high winding factor [2]-[4], high torque density [1],[4]-[5], as well as simpler structure [6].
However, high torque ripple [8], high cogging torque [9],[10], large unbalanced magnetic pull [5] and high
rotor loss [11] are some of the drawbacks which may causes of undesirable noise and vibration especially in
small permanent magnet machines [12]. For high performance applications, these parasitic effects should be
minimized as much as possible. In design stage, cogging torque minimization is needed especially for a low
speed application. Previous researches have shown there are various effective techniques used for the
cogging torque minimization that change the geometric shapes of the machine such as stator or rotor skewing
[13], magnet pole shape [14],[15], pole arc coefficient [16], magnet shifting [17], stator teeth notching [18]
and etc. It is also possible to combine two design optomization methods i.e. stator teeth notching and rotor
magnet skewing in order to eliminate the cogging torque. Teeth notching helps to reduce skewing angle of
rotor magnet that solve various manufacturing problem and retains the shape of back EMF waveform [19]-
[21]. Many researchers as mentioned found that reduction in cogging torque inherently reduce the torque
ripple as the cogging torque is one of the components of torque pulsation in principle. However in many
cases, torque pulsation is still high even the cogging torque is significantly reduced. This is because due to
no-load reluctance torque that exists during open-circuit, while the torque ripple at rated condition exists due
discrepancy of back EMF and winding current [22]. Torque ripple in PM brushless machines also mainly due
to harmonics in back-EMF, winding MMF, commutation of current and cogging torque [23] as well as

IJPEDS ISSN: 2088-8694 
Electromagnetic Performance due to Tooth-tip Design in Fractional-slot .... (Mohd Luqman Mohd Jamil)
861
saturation in magnetic circuit path of electric machine. The torque ripple is also can be reduced effectively
which depends on other factors instead of cogging torque [21].
In this paper, further investigation is carried out by coupling the influence of tooth–notching with
the influence of stator modification from previuos work [24] which main parameter is tabulated as in Table 1.
These works are mainly focused on the output torque performance in single and double layers fractional slot
surface mounted PM machines. Factors such as notch depth, notch width, notch numbers and notch position
on stator tooth-tip are included in the investigation. All results are predicted by the Ansys Finite Element
Analysis software. Significant findings in this research are discussed in the later sections.
Table 1. Design specifications for 12-slot/10-pole machine
Parameter Specifications
Supply voltage (V) 24
Rated torque (Nm) 10
Rated speed (rpm) 100
Stator outer diameter (mm) 120
Rotor outer diameter (mm) 72
Axial length (mm) 20
Magnet thickness (mm) 5
Airgap length 1
Slot Opening 1.9
Tooth tip thickness 3.3
Rated current (A) 10.8
Magnetization type Parallel
Operating mode BLDC
2. STATOR MODIFICATION
Symmetrical stator tooth-tip width is in relation to the stator slot opening. A winding process will be
much easier when bigger space of copper winding is available. By increasing the slot opening width, a
change on slot permeance results a bigger cogging torque. If a wider tooth-tip width is implemented,
magnetic interaction between permanent magnet and slot permeance is minimized leading to a smaller
cogging torque and eventually the torque ripple. Therefore, stator tooth-tip should be as close as possible to
minimize the cogging torque and stator slot should be wide enough to accommodate copper windings. In this
study, the first asymmetry stator is implemented by having strange tooth-tip geometry as marked with dashed
circle in Figure 1.
a) double layer winding b) single layer winding
Figure 1. 12-slot/10-pole machine with alternate asymmetric tooth-tip [24]
2.1. Effect on Back EMF
The phase back-emfs of 12-slot/10-pole machines with the influence of different winding topologies
and modification on alternate tooth-tip are compared in Figure 2. The modified stator distort developed stator
magnetic path thus resulting an unsymmetrical phase back-emf. In other way, the developed stator magnetic
path has been interfered by the localized flux due to the asymmetric geometry, leading to a severe saturation
condition in the stator tooth-tip. The phenomena can be explained by the harmonics content as shown in
Figure 2b). The modified stator – single layer winding has higher fundamental and 3rd order harmonics
while at the same time boost the 5th and 7th order harmonics compare to modified stator – double layer
winding. It is also shown that the modified stator – double layer winding has boost the 2nd order harmonics.

 ISSN: 2088-8694
IJPEDS Vol. 6, No. 4, December 2015 : 860 – 868
862
In general, the modified stator affects the phase back-emfs in both double layer and single layer winding
machines.
-8
-6
-4
-2
0
2
4
6
8
0 60 120 180 240 300 360
PhasebackEMF(V)
Rotor position (elect. degree)
Double layer
Single layer
0
1
2
3
4
5
6
7
1 2 3 4 5 6 7 8 9 10 11
Magnitude
Harmonic order
Double layer
Single layer
a) Phase back-emf b) Harmonics
Figure 2. Phase back-emf of 12-slot/10-pole machine with modified stator
2.2. Effect on Output Torque
Figure 3 compares the rated output torque in 12-slot/10-pole machines with the influence of
different winding topologies and modification on stator tooth-tip. The modified machine that employs single
layer winding results superior torque performance than the double layer winding as its torque ripple is only
6% while having similar average output torque. The modified machine that employs double layer winding
results a bigger torque ripple i.e. 17.2% while maintaining average output torque of 10Nm. The harmonic
content of output torque in all machines are shown in Figure 3b). The reduction of fundamental and higher
multiple harmonics order corresponding to the torque files as shown in Figure 3a). The rise of other lower
sub-harmonics order results in more dc from of torque in the single layer winding machine. This would
results minimum noise and vibration. The average output torque and torque ripple in all respective machines
are tabulated in Table 2.
0
2
4
6
8
10
12
0 60 120 180 240 300 360
Outputtorque(Nm)
Double layer
Single layer
0
0.1
0.2
0.3
0.4
0.5
0.6
0.7
1 3 5 7 9 11 13 15 17 19 21 23 25 27 29
Magnitude
Harmonic order
Double layer
Single layer
a) Torque profile b) Harmonics
Figure 3. Output torque of 12-slot/10-pole machine with modified stator
Table 2. Rated output torque in 12-slot/10-pole machine with modified stator
Machines Average torque (Nm) Torque ripple (%)
Double layer 10 17.2
Single layer 9.8 6
2.3. Effect on Cogging Torque
Figure 4 compares the cogging torque in the respective machines. Theoretically, the 12-slot
machines have identical cogging torque although they employ different winding configurations. However,

863
machines that have modified stator result bigger cogging torques and new cogging torque cycles but their
output torque ripple reduced [24].
-250
-150
-50
50
150
250
0 60 120 180 240 300 360
Coggingtorque(mNm)
Double layer Single layer
Figure 4. Cogging torque of 12-slot/10-pole machine with modified stator
3. TOOTH-TIP NOTCH
Further investigation of stator modification is followed by tooth notching. This technique is
implemented by introducing auxiliary slots along the tooth tip periphery. In most cases, cogging torque can
be effectively reduced when notches have same width as slot-opening. Fractional-slot machines in which slot
per pole per phase, q is a fraction would be preferable instead of integral-slot type because notch numbers is
pointless and does not affect the reduction of cogging torque when q is an integer. Suitable notch number, Nn
must be carefully chosen for a minimum pulsating torque.
Figure 5 illustrates stator tooth notching with different numbers of notch at stator tooth-tip. Here, the
notches are introduced at stator teeth that are alternately symmetric to the modified ones as marked with
dashed circle in Figure 6. The machine equipped with singler layer winding is selected for further analysis of
stator tooth-tip notch due to its performance in term of back EMF and less torque ripple. Tooth-tip notch may
cause the magnetic flux distribution to depart from its ideal path as in turn changes the output performance of
the motor. By varying the notch depth, Nd, notch width, Nw, notch position, Np and suitable number of
notches, Np., the machine performance are analysed and compared with the machine equipped with single
layer winding and having modified stator as shown in Figure 1.
a) Nn = 1 b) Nn = 2
c) Nn = 3
Figure 5. Stator tooth asymmetry

 ISSN: 2088-8694
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Figure 6. Stator tooth asymmetry
3.1. Notch Number and Notch Position
The influences of notch position on torque ripple are investigated for different notch numbers. Tooth
notch with Nn = 1 are positioned on the center of the tooth-tip. However, tooth notch also can be positioned
apart from tooth-tip center when it has Nn = 2 or Nn = 3. The influence of notch position is investigated by
varying its positions from Np = 4° up to Np = 12° starting from the centre of the tooth-tip. It should be noted
that tooth notches are relatively effective on cogging torque reduction when they have same width as winding
slot opening. Thus, the notch dimension in this study resembles as winding slot opening which is 1.9 mm.
Figure 7 shows torque ripple of different notch positions for Nn = 1, Nn = 2 and Nn = 3. A similar torque
performance is obtained in two different conditions; when i) Nn = 1 and Np = 0° and ii) Nn = 3 and Np = 10°.
It can be seen that torque ripple reaches it maximum at Np = 6° and minimum when notches are positioned at
Np = 10° for both Nn = 2 and Nn = 3. It is also can be seen that stator with Nn = 3 results less torque ripple
than when Nn = 2.
1
2
3
4
5
0 2 4 6 8 10 12 14
Torqueripple(Nm)
Notch position (degree)
Nn = 1
Nn = 2
Nn = 3
Figure 7. Torque ripple for different degree of notch position
3.2. Notch Depth and Notch Width
A compromise between the notch depth and notch width has to be considered to acheieve optimum
torque i.e. higher average torque but less torque ripple. Figure 8 shows torque ripple due to various notch
depth and notch width when Nn = 1. There is not much change of torque ripple when notch depth inreases.
Notches in the stator tooth-tip change the behavior of magnetic field in the stator tooth body and hence
affecting machine torque capability. The smallest torque ripple is obtained when Nw = 5 mm and Nd = 4 mm .

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0.5
1
1.5
2
2.5
3
2 3 4 5 6 7
TorqueRipple(Nm)
Notch Depth (mm)
w= 1mm w= 2mm
w= 3mm w= 4mm
w= 5mm w= 6mm
w= 7mm
Figure 8. Torque ripple for various notch depth and notch width when Nn = 1
Investigation of torque ripple due to variation of notch depth and notch width for Nn = 2 and Nn = 3
are presented in Figure 9 and Figure 10 respectively. The investigation focus at two different position i.e. Np
= 5° and Np = 10°. From Figure 9, there is similar trend i.e. the torque ripple increase as notches getting
deeper and wider. Saturation in tooth body could be increased due to the bigger size of notch dimension,
leading to a slight reduction of average torque but bigger torque ripple. This phenomenon is confirmed by
Figure 9, when Np = 5°.
2
4
6
8
10
12
0 1 2 3 4 5 6
TorqueRipple(Nm)
Notch Depth (mm)
w= 1mm w= 2mm
w= 3mm w= 4mm
w= 5mm
2.5
3
3.5
4
4.5
5
0 1 2 3 4 5 6
TorqueRipple(Nm)
Notch Depth (mm)
w= 1mm w= 2mm
w= 3mm
a) Nn = 2 b) Nn = 3
Figure 9. Torque ripple due to different dimension of notch depth and notch width when Np = 5°
Figure 10 shows a similar trend as in Figure 9 as the torque ripple increases when the notch depth
and notch width are increased. Regardless of Nn = 2 or Nn = 3, a condition of Nw = 1mm results the smallest
range of torque ripple and it relatively remains constant over various notch depth.
1.5
2
2.5
3
3.5
4
0.5 1 1.5 2 2.5 3 3.5
TorqueRipple(Nm)
Notch Depth (mm)
w= 1mm w= 2mm
w= 3mm w= 4mm
0
1
2
3
4
5
6
7
0.5 1 1.5 2 2.5 3 3.5
TorqueRipple(Nm)
Notch Depth (mm)
w= 1mm w= 2mm
w= 3mm w= 4mm
a) Nn = 2 b) Nn = 3
Figure 10. Torque ripple due to different dimension of notch depth and notch width when Np = 10°

 ISSN: 2088-8694
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3.3. Effect on Back EMF
The phase back-emfs of 12-slot/10-pole, single-layer machines with the influence of stator
modifications, i) asymmetric tooth-tips (M1); ii) asymmetric tooth-tips + alternate tooth notching (M2); are
compared in Figure 11a). These auxiliary slot i.e. tooth notching distorts the developed stator magnetic path
and establishes high localized magnetic flux saturation. For M2 stator, there is little mis-match between
positive and negative portions of phase-back emf for every 180° elect. degree. However the M2 stator, results
similar harmonics content with M1 stator as shown in Figure 11b).
-8
-6
-4
-2
0
2
4
6
8
0 60 120 180 240 300 360
PhasebackEMF(V)
modified stator
tooth notch
0
1
2
3
4
5
6
7
1 2 3 4 5 6 7 8 9 10 11Magnitude
Harmonic order
modified stator tooth notch
a) Phase back-emf b) Harmonics
Figure 11. Phase back-emfs due to asymmetric tooth tip in 12-slot/10-pole machines
3.4. Effect on Output Torque
In general, both M1 and M2 stator result similar torque performance, but M2 is slightly better than
M1 as shown in Figure 12. The harmonic content of each respective models are illustrated in Figure 12
b),and it is shown that the fundamental and higher multiple harmonics orders of M2 are reduced. The
average torque and torque ripple at rated condition is tabulated in Table 3.
0
2
4
6
8
10
12
0 60 120 180 240 300 360
Outputtorque(Nm)
modified stator
tooth notch 0
0.05
0.1
0.15
0.2
0.25
1 3 5 7 9 11 13 15 17 19 21 23 25 27 29
Magnitude
Harmonic order
modified stator
tooth notch
a) Torque profile b) Harmonics
Figure 12. Output torque due to asymmetric tooth tip in 12-slot/10-pole machines
Table 1. Output torque of asymmetries stator 12-slot/10-pole machines
Machines Average torque (Nm) Torque ripple (%)
Modified stator 9.8 6
Tooth nooth 10 5.2
3.5. Effect on Cogging Torque
Figure 13 compares cogging torque between the two stator models. The M2 model has a slight
increase of cogging torque than the M2 where the cogging torque cycle is unchanged. Although the tooth-

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notch is tiny, it results localized flux saturation due to interaction between rotor permanent magnet and the
stator tooth. In general, non-uniform design of stator tooth may change cogging torque characteristics.
-250
-150
-50
50
150
250
350
0 60 120 180 240 300 360
Coggingtorque(mNm)
modified stator tooth notch
Figure 13. Cogging torque due to asymmetric tooth tip in 12-slot/10-pole machines
4. CONCLUSION
From the investigation, the stator asymmetry has great influence on the torque performance as there
is significant reduction of torque ripple in 12-slot/10-pole single layer winding machine equipped than the
ones equipped with double layer winding topology. Although a distorted back-emf exists when auxiliary
notches and asymmetry stator tooth-tip are employed, an optimum torque performance i.e. less torque ripple
is desirable.
ACKNOWLEDGEMENTS
The authors would like to thank Universiti Teknikal Malaysia Melaka (UTeM) for providing the
research grant PJP/2012/CERIA/Y00002 for this research.
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