IEEE TRANSACTIONS ON MAGNETICS, VOL. 50, NO. 2, FEBRUARY 2014 7019704
Quasi-Zero Torque Pulsation of Surface Permanent Magnet
Synchronous Motor for Ship Gyro Stabilizer by
Pole/Slot Number and Air-Gap Designs
Sun-Kwon Lee
1,2
, Gyu-Hong Kang
1
, Jin Hur
2
, and Byoung-Woo Kim
2
1
Korea Marine Equipment Research Institute, Busan 1631-10, Korea
2
Department of Electrical Engineering, University of Ulsan, Ulsan 680-749, Korea
This paper deals with the reduction of torque pulsation including torque ripple and cogging torque in surface PM brushless
ac motors. The fractional combination and air-gap shape design by shaping the PM and stator core are studied to reduce torque
pulsation. Torque ripple reduction is achieved by adjusting the magnetic flux density in air-gap contour by cutting magnet outer
shape. Quasi-zero torque pulsation in this paper means the ripple ratio to average torque <0.5%. The magnetic field and torque
characteristics are analyzed by 2-D finite element analysis and prototype to validate is manufactured and measured.
Index Terms—Finite element analysis, permanent magnet, SPMSM, torque pulsation.
I. I NTRODUCTION
M
ARINE applications have strict limits on vibrations and
interference for electromagnetic comparability, and so
high efficiency and low vibrations are key requirements [1].
The reduction of vibration is a very important design issue
for ship gyro stabilizers to operate reliably due to their heavy
mass flywheel. PM machines with a fractional number of
slots per pole and a concentrated winding have shorter end
windings and lower overall length and yet have high efficiency,
torque, and power density [1]–[3]. Furthermore, fractional slot
machines have extremely low cogging torque without the need
for design features such as skew [2].
Torque ripple caused by rotor field and stator current is
affected by harmonic components of radial flux density. The
cogging torque is generated from the interaction between the
air-gap flux density distribution and stator slotting. The torque
pulsation reduction can be achieved by minimizing torque
ripple and cogging torque [3].
Thus, many previous studies [1]–[11] dealt with torque
pulsation reduction approaches of PM machines. Hur et al.
[4] proposed a third harmonic elimination method to reduce
cogging torque. The analytical approach was introduced to
calculate the cogging torque of an interior permanent magnet
(IPM) motor [5]. Some researchers [6]–[9], studied the torque
pulsation reduction of IPM machines and PM assisted reluc-
tance machine including optimization problems. Kwon [10]
studied the sinusoidal PM shape to the axial direction to
obtain sinusoidal back EMF and low torque pulsation. The
sensitivity of harmonics caused by manufacturing tolerance is
also studied [11].
In this paper, torque pulsation reduction is introduced by
poles/slots combination and air-gap structure design using
magnet shapes and stator core structure. The torque ripple
Manuscript received June 29, 2013; revised August 12, 2013; accepted
September 24, 2013. Date of current version February 21, 2014.
Corresponding author: G.-H. Kang (e-mail: kang@komeri.re.kr).
Color versions of one or more of the figures in this paper are available
online at http://ieeexplore.ieee.org.
Digital Object Identifier 10.1109/TMAG.2013.2284004
Fig. 1. Designed and analysis models. (a) 8p12s model. (b) 10p12s model1.
(c) 10p12s model2. (d) Magnet shape difference between 10p12s model1 and
model2.
TABLE I
SPECIFICATIONS OF ANALYZED MODELS
reduction principle by adjusting air-gap magnetic flux density
distribution is also discussed. The flux density on the air-gap
contor is investigated to compare the relationship between
torque pulsation and air-gap flux density in detail. Close
to torque pulsation is achieved compared with the average
generated torque. 2-D finite element analysis using Maxwell
is used to calculate the magnetic field of the designed motor.
II. ANALYSIS MODEL DESCRIPTIONS
Fig. 1 shows the cross sections of the analyzed models.
An identical stator with 12 slots concentrated windings is
employed for each model. The detailed descriptions of ana-
lyzed models are listed in Table I. The differences between
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