U.S. patent application number 15/772433 was filed with the patent office on 2019-12-26 for a method to reduce torque ripple of permanent magnet synchronous motor.
This patent application is currently assigned to Jiangsu University. The applicant listed for this patent is Qian Chen, Xinxin Du, Deshui Hu, Guohai Liu, Wenxiang Zhao. Invention is credited to Qian Chen, Xinxin Du, Deshui Hu, Guohai Liu, Wenxiang Zhao.
Application Number | 20190393811 15/772433 |
Document ID | / |
Family ID | 58865990 |
Filed Date | 2019-12-26 |
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United States Patent
Application |
20190393811 |
Kind Code |
A1 |
Liu; Guohai ; et
al. |
December 26, 2019 |
A METHOD TO REDUCE TORQUE RIPPLE OF PERMANENT MAGNET SYNCHRONOUS
MOTOR
Abstract
A method named as Magnet Shifting to reduce torque ripple of
permanent magnet synchronous motor is disclosed. A way of
reasonably choosing the repeating unit of magnetic pole, the
shifting ways and the shifting angle calculation of the first and
second magnet shifting is described, which are carried on the
repeating unit of magnetic poles individually or repeatedly to
improve the performance of the motor. The method can be applied to
surface, surface-inset and inner-embedded permanent magnet motors,
which can reduce torque ripple caused by different torque
components, including cogging torque, reluctance torque or
permanent magnet torque. It also can quickly calculate the shifting
angle of the magnetic pole by choosing repeating unit reasonably.
Magnet shifting can effectively enhance the sinusoidal degree of
back electrodynamic force (back-EMF) waveform, where the repeating
units can offset the torque ripple between the maximum and the
minimum value to reduce the different torque harmonics. Also, the
output torque can be maintained nearly to the original value while
less vibration noise of the motor is inevitably introduced.
Inventors: |
Liu; Guohai; (Zhenjiang,
Jiangsu, CN) ; Du; Xinxin; (Zhenjiang, Jiangsu,
CN) ; Zhao; Wenxiang; (Zhenjiang, Jiangsu, CN)
; Chen; Qian; (Zhenjiang, Jiangsu, CN) ; Hu;
Deshui; (Zhenjiang, Jiangsu, CN) |
|
Applicant: |
Name |
City |
State |
Country |
Type |
Liu; Guohai
Du; Xinxin
Zhao; Wenxiang
Chen; Qian
Hu; Deshui |
Zhenjiang, Jiangsu
Zhenjiang, Jiangsu
Zhenjiang, Jiangsu
Zhenjiang, Jiangsu
Zhenjiang, Jiangsu |
|
CN
CN
CN
CN
CN |
|
|
Assignee: |
Jiangsu University
Zhenjiang, Jiangsu
CN
|
Family ID: |
58865990 |
Appl. No.: |
15/772433 |
Filed: |
February 6, 2017 |
PCT Filed: |
February 6, 2017 |
PCT NO: |
PCT/CN2017/072924 |
371 Date: |
April 30, 2018 |
Current U.S.
Class: |
1/1 |
Current CPC
Class: |
H02P 6/10 20130101 |
International
Class: |
H02P 6/10 20060101
H02P006/10 |
Foreign Application Data
Date |
Code |
Application Number |
Nov 29, 2016 |
CN |
201611066962.2 |
Claims
1. A method of reducing torque ripple of a permanent magnet
synchronous motor, the method comprising: Step one: analyzing
torque of a target motor with different combinations between poles
and slots, wherein according to the relationship between pole
number and slot number, a fluctuation period number of torque
ripple in one electric cycle is calculated to determine a general
trend of its fluctuation; Step two: calculating a minimum number of
magnetic poles (N.sub.0) in each module to modularize rotor and
magnets of the motor, wherein through modular analysis, the
magnetic poles in each module produce the same torque with
consistency in waveform and phase, then each module containing
fewest magnetic poles is recognized as one basic repeating unit;
Step three: merging two or more basic repeating units to form a new
repeating unit, which can also produce same torque with consistency
in waveform and phase, wherein a different number of new repeating
units has an effect on magnet shifting; Step four: analyzing and
modularizing main source of torque and torque ripple so as to
determine the basic repeating unit to produce main source of torque
and torque ripple, and to calculate a minimum pole number
(N.sub.i0) in each basic repeating unit; Step five: choosing a
reasonable repeating unit to shift by considering N.sub.0 and
N.sub.i0 comprehensively, according to number of poles (b) in the
selected repeating unit, and respectively determining number of
repeating units (q) and maximum shifting times (N); Step six:
calculating accurate angle (.theta..sub.1) of magnet shifting a
first time in order to weaken a first main harmonic of torque
ripple, and shifting the selected repeating unit counterclockwise
by .theta..sub.1 degrees, wherein the selected repeating unit is
the first repeating unit, and the first application is the first
magnet shifting; Step seven: calculating accurate angle
(.theta..sub.2) of magnet shifting for a second time in order to
weaken the second main harmonic of torque ripple, based upon the
first magnet shifting, new repeating unit is reconsidered, formed,
and then shifted by .theta..sub.2 degrees, wherein the new
repeating unit is the second repeating unit, and the second
application is the second magnet shifting; and Step eight:
calculating accurate angle (.theta..sub.n) of magnet shifting for
n.sup.th time to weaken n.sup.th order main harmonic of torque
ripple on basis of (n-1).sup.th magnet shifting, new repeating unit
is reconsidered for n.sup.th time and then shifted by .theta..sub.n
degrees, the newest repeating unit is the n.sup.th repeating
unit.
2. The method according to claim 1, wherein the fluctuation period
number of torque ripple in one electric cycle in Step one is
calculated by T ripple = N p s N p , ##EQU00026## wherein
T.sub.ripple is the fluctuation period number of torque ripple in
one electric cycle, N.sub.s is slot number, N is pole-pair number,
and N.sub.ps is least common multiple of slot number (N.sub.s) and
pole number (2N.sub.p), N.sub.ps=LCM(N.sub.s, 2N.sub.p).
3. The method according to claim 1, wherein the basic repeating
unit in Step two is a group of poles that produces torques with
consistency in waveforms and phases.
4. The method according to claim 1, wherein the minimum number of
magnetic poles in each basic repeating unit in Step two is
calculated by N 0 = N p s N s , ##EQU00027## where N.sub.0 is
minimum number of magnetic poles in each basic repeating unit, and
N.sub.s is slot number.
5. The method according to claim 1, wherein the new repeating unit
in Step three is combined with k basic repeating units, then the
number of magnetic poles in one new repeating unit is kN.sub.0.
6. The method according to claim 1, wherein the main source of
torque ripple in Step four influences cogging torque, reluctance
torque and permanent magnet torque, and wherein corresponding
minimum numbers of magnetic poles (N.sub.0) in each basic repeating
unit are N.sub.10, N.sub.20, N.sub.30, respectively.
7. The method according to claim 1, wherein, in Step five, the
number of poles (b) in the selected repeating unit, the number of
repeating units (q) and the maximum shifting times (N) are
respectively determined by 1 ) { b = k N 0 b m ax .ltoreq. N p ,
##EQU00028## k belongs to integer; 2 ) q = 2 N p b ; 3 ) N = log 2
( 2 N p b ) , ##EQU00029## N belongs to integer; when the number of
poles (b) in the selected repeating unit, the number of repeating
units (q) and the maximum shifting times (N) in Step five are
determined, the total torque is composed of partial torque produced
by each repeating unit, i.e., T = i = 1 q T i , ##EQU00030## where
T.sub.i is torque produced by the i.sup.th repeating unit.
8. The method according to claim 1, in Step six, wherein the
accurate angle (.theta..sub.n) of magnet shifting for the n.sup.th
time are calculated by Step 6.1, expressing torque expression of
the motor as sum of average torque and torque ripple, as follows: {
T = T all _ av + T all _ rip T all _ rip = n = 1 .infin. T rn sin N
p s n .alpha. = q n = 1 .infin. T prn sin N p s n .alpha.
##EQU00031## wherein T.sub.all_av represents average torque and
T.sub.all_rip represents torque ripple, according to periodicity of
torque ripple expressed as a form of the Fourier series; Step 6.2,
torque T of the motor is sum of partial torque component T.sub.i
produced by i.sup.th repeating unit, and partial torque component
T.sub.i is sum of corresponding partial average value component and
corresponding partial torque ripple, and when one repeating unit is
shifted by .theta. degrees, the corresponding partial torque ripple
produced by the shifted repeating unit changes only in phase, as
follows: T rip ' = n = 1 .infin. T prn sin N p s n ( .alpha. +
.theta. ) ; ##EQU00032## Step 6.3, the total torque ripple is
superposed by the torque ripple produced by shifted repeating units
and that of fixed repeated units: T all _ rip = q 2 j = 1 2 n = 1
.infin. T prjn sin N p s n ( .alpha. + .theta. ) ; ##EQU00033##
Step 6.4, based on these, the output torque is expressed as T = q 2
j = 1 2 ( T pavj + n = 1 .infin. T prjn sin N p s n ( .alpha. + ( j
- 1 ) .theta. ) ) ##EQU00034## where, T.sub.pavj represents the
average torque produced by j.sup.th repeating unit before the
magnet shifting, the partial average torque produced by each
repeating unit is the same as each other, i.e.,
T.sub.pavj=T.sub.pav; Step 6.5, after the magnet shifting, the
rotor is caused to be slightly asymmetrical, therefore, the partial
average torque of each repeating unit makes a change far lower than
value of torque ripple, the specific relationship being expressed
as { T pavj = T pav + .DELTA. T j T prjn = T prn + .DELTA. T rj
where { .DELTA. T = q 2 j = 1 2 .DELTA. T j + q 2 j = 1 2 n = 1
.infin. .DELTA. T rj sin N ps n ( .alpha. + ( j - 1 ) .theta. ) T r
= q 2 j = 1 2 n = 1 .infin. T prn sin N ps n ( .alpha. + ( j - 1 )
.theta. ) ##EQU00035## T.sub.r is the main component of the torque
ripple, which is recognized as the main study object by using the
trigonometric function formula simplified as T r = q 2 n = 1
.infin. T prn sin N ps n .theta. sin N ps n .theta. 2 sin ( N ps n
( .alpha. + 3 2 .theta. ) ) ; ##EQU00036## Step 6.6, in order to
reduce torque ripple, T.sub.r is minimized, then, the shifting
angle is .theta. n = 180 .degree. nN ps or .theta. n = .pi. nN ps ,
##EQU00037## where .theta..sub.n represents the shifting angle that
eliminates the n.sup.th main subharmonic of the torque ripple, when
n=1, magnet shifting by .theta..sub.1 degrees reduces the first
main harmonic of the torque ripple, and when n=2, magnet shifting
by .theta..sub.2 degrees reduces the second main harmonic of the
torque ripple.
9. The method according to claim 1, wherein the first magnet
shifting in Step six has the selected basic repeating unit is
alternately shifted by .theta..sub.1 degrees.
10. The method according to claim 1, wherein the second magnet
shifting in Step seven has the shifted basic repeating unit and the
adjacent fixed basic repeating unit chosen as one new repeating
unit, wherein for every pair of adjacent new repeating units, one
new repeating unit is fixed, and the other new repeating unit is
alternately shifted by .theta..sub.2 degrees, and wherein the
second magnet shifting in Step seven keeps the same the shifting
direction as the first magnet shifting in Step six.
11. A method of reducing torque ripple in a permanent magnet
synchronous motor, the method comprising: Step (a): analyzing
torque of a target motor with different combinations between poles
and slots, wherein according to relationship between pole number
and slot number, a fluctuation period number of torque ripple in
one electric cycle is calculated to determine a general trend of
its fluctuation; Step (b): calculating a minimum number of magnetic
poles (N.sub.0) in each module to modularize rotor and magnets of
the motor, wherein through modular analysis, the magnetic poles in
each module produce the same torque with consistency in waveform
and phase, then, each module containing fewest magnetic poles is
recognized as one basic repeating unit; Step (c): merging at least
two basic repeating units to form a new repeating unit, which can
also produce same torque with consistency in waveform and phase,
wherein a different number of new repeating units has an effect on
magnet shifting; Step (d): analyzing and modularizing main source
of torque and torque ripple so as to determine the basic repeating
unit to produce main source of torque and torque ripple, and to
calculate a minimum pole number (N.sub.i0) in each basic repeating
unit; Step (e): choosing a reasonable repeating unit to shift by
considering N.sub.0 and N.sub.i0 comprehensively, according to
number of poles (b) in the selected repeating unit, respectively
determining number of repeating units (q) and maximum shifting
times (N); Step (f): calculating accurate angle (.theta..sub.1) of
magnet shifting a first time in order to weaken a first main
harmonic of torque ripple, and shifting the selected repeating unit
counterclockwise by .theta..sub.1 degrees, wherein the selected
repeating unit is the first repeating unit, and the first
application is the first magnet shifting; Step (g): calculating
accurate angle (.theta..sub.2) of magnet shifting for a second time
in order to weaken the second main harmonic of torque ripple, based
upon the first magnet shifting, new repeating unit is reconsidered,
formed, and then shifted by .theta..sub.2 degrees, wherein the new
repeating unit is the second repeating unit, and the second
application is the second magnet shifting; and Step (h):
calculating accurate angle (.theta..sub.n) of magnet shifting for
n.sup.th time to weaken n.sup.th order main harmonic of torque
ripple on basis of (n-1).sup.th magnet shifting, new repeating unit
is reconsidered for n.sup.th time and then shifted by .theta..sub.n
degrees, the newest repeating unit is the n.sup.th repeating
unit.
12. The method according to claim 11, wherein the fluctuation
period number of torque ripple in one electric cycle in Step (a) is
calculated by T ripple = N ps N p , ##EQU00038## wherein
T.sub.ripple is the fluctuation period number of torque ripple in
one electric cycle, N.sub.s is slot number, N.sub.p is pole-pair
number, and N.sub.ps is least common multiple of slot number
(N.sub.s) and pole number (2N), N.sub.ps=LCM(N.sub.s, 2N).
13. The method according to claim 11, wherein the basic repeating
unit in Step (b) is a group of poles that produces torques with
consistency in waveforms and phases.
14. The method according to claim 11, wherein the minimum number of
magnetic poles in each basic repeating unit in Step (b) is
calculated by N 0 = N ps N s , ##EQU00039## wherein N.sub.0 is
minimum number of magnetic poles in each basic repeating unit, and
N.sub.s is slot number.
15. The method according to claim 11, wherein when the new
repeating unit in Step (c) is combined with k basic repeating
units, then the number of magnetic poles in one new repeating unit
is kN.sub.0.
16. The method according to claim 11, wherein the main source of
torque ripple in Step (d) influences cogging torque, reluctance
torque, and permanent magnet torque, and wherein corresponding
minimum numbers of magnetic poles (No) in each basic repeating unit
are N.sub.10, N.sub.20, N.sub.30, respectively.
17. The method according to claim 11, wherein, in Step (e), the
number of poles (b) in the selected repeating unit, the number of
repeating units (q) and the maximum shifting times (N) are
respectively determined by { b = kN 0 b max .ltoreq. N p , 1 )
##EQU00040## k belongs to integer; q = 2 N p b ; 2 ) N = log 2 ( 2
N p b ) , 3 ) ##EQU00041## N belongs to integer; when the number of
poles (b) in the selected repeating unit, the number of repeating
units (q) and the maximum shifting times (N) in Step (e) are
determined, the total torque is composed of partial torque produced
by each repeating unit, i.e., T = i = 1 q T i , ##EQU00042## where
T.sub.i is torque produced by the i.sup.th repeating unit.
18. The method according to claim 11, in Step (f), wherein the
accurate angle (.theta..sub.n) of magnet shifting for the n.sup.th
time are calculated by: Step (f)-1, expressing torque expression of
the motor as sum of average torque and torque ripple, as follows: {
T = T all _ av + T all _ rip T all _ rip = n = 1 .infin. T rn sin N
ps n .alpha. = q n = 1 .infin. T prn sin N ps n .alpha.
##EQU00043## wherein T.sub.all_av represents average torque and
T.sub.all_rip represents torque ripple, according to periodicity of
torque ripple expressed as a form of the Fourier series; Step
(f)-2, torque T of the motor is sum of partial torque component
T.sub.i produced by i.sup.th repeating unit, and partial torque
component T.sub.i is sum of corresponding partial average value
component and corresponding partial torque ripple, and when one
repeating unit is shifted by .theta. degrees, the corresponding
partial torque ripple produced by the shifted repeating unit
changes only in phase, as follows: T rip ' = n = 1 .infin. T prn
sin N ps n ( .alpha. + .theta. ) ; ##EQU00044## Step (f)-3, the
total torque ripple is superposed by the torque ripple produced by
shifted repeating units and that of fixed repeated units: T all _
rip = q 2 j = 1 2 n = 1 .infin. T prjn sin N ps n ( .alpha. + ( j -
1 ) .theta. ) ; ##EQU00045## Step (f)-4, based on these, the output
torque is expressed as T = q 2 j = 1 2 ( T pavj + n = 1 .infin. T
prjn sin N ps n ( .alpha. + ( j - 1 ) .theta. ) ) ##EQU00046##
where, T.sub.pavj represents the average torque produced by
j.sup.th repeating unit before the magnet shifting, the partial
average torque produced by each repeating unit is the same as each
other, i.e., T.sub.pavj=T.sub.pav; Step (f)-5, after the magnet
shifting, the rotor is caused to be slightly asymmetrical,
therefore, the partial average torque of each repeating unit makes
a change far lower than value of torque ripple, the specific
relationship being expressed as { T pavj = T pav + .DELTA. T j T
prjn = T prn + .DELTA. T rj where { .DELTA. T = q 2 j = 1 2 .DELTA.
T j + q 2 j = 1 2 n = 1 .infin. .DELTA. T rj sin N ps n ( .alpha. +
( j - 1 ) .theta. ) T r = q 2 j = 1 2 n = 1 .infin. T prn sin N ps
n ( .alpha. + ( j - 1 ) .theta. ) ##EQU00047## T.sub.r is the main
component of the torque ripple, which is recognized as the main
study object by using the trigonometric function formula simplified
as T r = q 2 n = 1 .infin. T prn sin N ps n .theta. sin N ps n
.theta. 2 sin ( N ps n ( .alpha. + 3 2 .theta. ) ) ; ##EQU00048##
Step (f)-6, in order to reduce torque ripple, T.sub.r is minimized,
then, the shifting angle is .theta. n = 180 .degree. nN ps or
.theta. n = .pi. nN ps , ##EQU00049## where .theta..sub.n
represents the shifting angle that eliminates the n.sup.th main
subharmonic of the torque ripple, when n=1, magnet shifting by
.theta..sub.1 degrees reduces the first main harmonic of the torque
ripple, and when n=2, magnet shifting by .theta..sub.2 degrees
reduces the second main harmonic of the torque ripple.
19. The method according to claim 11, wherein the first magnet
shifting in Step (f) has the selected basic repeating unit
alternately shifted by .theta..sub.1 degrees.
20. The method according to claim 11, wherein the second magnet
shifting in Step (g) has the shifted basic repeating unit and the
adjacent fixed basic repeating unit chosen as one new repeating
unit, wherein for every pair of adjacent new repeating units, one
new repeating unit is fixed, and the other new repeating unit is
alternately shifted by .theta..sub.2 degrees, and wherein the
second magnet shifting in Step (g) keeps the same shifting
direction as the first magnet shifting in Step (f).
Description
CROSS-REFERENCE TO RELATED APPLICATIONS
[0001] This application is a national phase entry under 35 U.S.C.
.sctn. 371 of International Patent Application PCT/CN2017/072924,
filed Feb. 6, 2017, designating the United States of America, which
claims the benefit under Article 8 of the Patent Cooperation Treaty
to Chinese Patent Application Serial No. 201611066962.2, filed Nov.
29, 2016.
TECHNICAL FIELD
[0002] The application relates to the technology of permanent
magnet synchronous motors, in particular, for reducing torque
ripple of permanent magnet synchronous motors, which belongs to the
field of motor manufacturing.
BACKGROUND
[0003] Permanent magnet synchronous motors have been widely used in
various occasions due to their high efficiency and high torque
density. Meanwhile, permanent magnet synchronous motors utilize
magnetic material with high magnetic energy, instead of traditional
excitation winding. This not only avoids the negative effects
resulting from traditional excitation winding, but also simplifies
the mechanical structure of the motor, which improves the
reliability of the motor and reduces the mechanical loss.
[0004] Some demanding applications need smooth output torque and
high operating stability, such as an electric steering system and
servo motor. That is, torque ripple of the motor should be
maintained as small as possible, so as to achieve a smooth and
accurate thrust drive. However, due to the concavity and convexity
of motor structure and the coupling effect of magnetic field,
permanent magnet synchronous motors suffer from relatively large
torque ripple, which limits the application of these motors.
Therefore, it is greatly significant to study the torque ripple
suppression strategy for these motors, thus improving the
smoothness of the torque.
[0005] In order to reduce the torque ripple, various methods have
been proposed. Generally, these methods can be classified into
three main strategies: involving stator slots and teeth, windings
and rotor magnets. First, skewing is widely used to reduce torque
ripple, in which the stator slots or rotor poles are skewed to
reduce the cogging torque. However, the skewed stator or rotor is
harder to build as for manufacturing, which also increases the cost
of production. Then, the auxiliary slots or teeth are used to
replace the skewing to avoid the disadvantages from skewing at the
loss of efficiency. Moreover, optimization of the slot or
slot-opening is also used to reduce torque ripple. Second, due to
the influence between the stator winding and the cogging torque,
the stator magnetic modification has been proposed to minimize the
ripple, such as fractional-slot pitch windings. However, the odd
and even magnetomotive force harmonics are incorporated in those
windings. This means that the improper selection of the fractional
slot can lead to the vibration of the stator core. Also, these
methods pay much attention to reduction of torque ripple but ignore
loss of output torque. Therefore, how to maintain torque density
and minimize torque ripple at the same time is one key research
direction.
[0006] In addition, optimization of magnets has been developed as
one of the effective methods, such as reshaping magnets, using
different magnet widths and asymmetry magnets. These studies result
in asymmetric magnets or change the distribution of magnets by
poles shifting or other methods. However, these methods only
consider the reduction for cogging torque while ignoring the
effects of reluctance torque on torque smoothness in inset and
interior permanent magnet synchronous motors. Sometimes in inset or
interior motors, the cogging torque occupies a very small
proportion in the total torque ripple because of the existence of
the reluctance torque. The total torque ripple was not always
reduced effectively with an acceptable torque loss by the
conventional magnet shifting. Therefore, how to reduce the main
source of torque ripple quickly and effectively is another key
research direction.
BRIEF SUMMARY
[0007] The disclosure notably describes a method to reduce total
torque ripple and maintain torque density at the same time by
magnets shifting. On the basis of accurately analyzing source of
torque ripple, this method is realized by reasonably choosing a
repeating unit that indicates a group of poles producing torques
with consistency in waveform and phase. Under the premise of
reducing torque ripple effectively, comprehensive consideration of
permanent magnet torque and reluctance torque is helpful to weaken
the effect of asymmetric rotor on output torque, vibration and
noise of motor.
[0008] The technical scheme of the disclosure is the method to
reduce torque ripple of permanent magnet synchronous motors,
including the following steps:
[0009] Step one: Torque of target motor with different combination
between poles and slots is analyzed. According to the relationship
between the pole number and slot number, the fluctuation period
number of torque ripple in one electric cycle is calculated to
determine the general trend of its fluctuation.
[0010] Step two: The rotor and magnets of the motor are modularized
by calculating the minimum number of magnetic poles (N.sub.0) in
each module. Through modular analysis, the magnetic poles in each
module can produce the same torque with consistency in waveform and
phase. Then, each module containing the fewest magnetic poles is
recognized as one basic repeating unit.
[0011] Step three: Two or more of basic repeating units can be
merged to form a new repeating unit, which can also produce the
same torque with consistency in waveform and phase. A different
number of new repeating units has an effect on magnet shifting.
[0012] Step four: The main source of torque and torque ripple are
analyzed, and their generation is modularized and analyzed. The
basic repeating unit to produce the main source of torque and
torque ripple is determined, and the minimum pole number (N.sub.i0)
in each basic repeating unit is calculated.
[0013] Step five: Considering the N.sub.0 and N.sub.i0
comprehensively, a reasonable repeating unit is chosen to shift.
According to the number of poles (b) in the selected repeating
unit, the number of repeating units (q) and the maximum shifting
times (N) are determined respectively.
[0014] Step six: In order to weaken the first main harmonic of
torque ripple, the accurate angle (.theta..sub.1) of magnet
shifting for the first time is calculated, and the selected
repeating unit is shifted anti-clockwise by .theta..sub.1 degrees.
The selected repeating unit is named "first repeating unit," and
the first application is recognized as "first magnet shifting."
[0015] Step seven: In order to weaken the second main harmonic of
torque ripple, the accurate angle (.theta..sub.2) of magnet
shifting for the second time is calculated. Based on the first
magnet shifting, a new repeating unit is reconsidered, formed, and
then shifted by .theta..sub.2 degrees. The new repeating unit is
named "second repeating unit," and the second application is
recognized as "second magnet shifting."
[0016] Step eight: If motor structure is allowed, the accurate
angle (.theta..sub.n) of magnet shifting for the n.sup.th time is
calculated to weaken the n.sup.th order main harmonic of torque
ripple. On the basis of the (n-1).sup.th magnet shifting, a new
repeating unit is reconsidered for the n.sup.th time and then
shifted by .theta..sub.n degrees. The newest repeating unit is
named "n.sup.th repeating unit."
[0017] Further, in Step one, the fluctuation period number of
torque ripple in one electric cycle is calculated by
T ripple = N p s N p , ##EQU00001##
where T.sub.ripple is the fluctuation period number of torque
ripple in one electric cycle, N.sub.s is the slot number, N.sub.p
is the pole-pair number, and N.sub.ps is the least common multiple
of slot number (N.sub.s) and pole number (2N.sub.p),
N.sub.ps=LCM(N.sub.s, 2N.sub.p).
[0018] Further, in Step two, the basic repeating unit indicates a
group of poles producing the same torques with consistency in
waveforms and phases.
[0019] Further, in Step two, the minimum number of magnetic poles
(N.sub.0) in each basic repeating unit is calculated by
N 0 = N p s N s , ##EQU00002##
where N.sub.0 is the minimum number of magnetic poles in each basic
repeating unit, and N.sub.s is the slot number.
[0020] Further, in Step three, the new repeating unit is combined
with k basic repeating units and the number of magnetic poles in
the new basic repeating unit is kN.sub.0.
[0021] Further, in Step four, the main source of torque ripple may
be involved in cogging torque, reluctance torque and permanent
magnet torque. Their minimum numbers of magnetic poles (N.sub.0) in
each basic repeating unit are marked as N.sub.10, N.sub.20,
N.sub.30, respectively.
[0022] Further, in Step five, the number of poles (b) in the
selected repeating unit, the number of repeating units (q) and the
maximum shifting times (N) are respectively determined by
1 ) { b = k N 0 b m ax .ltoreq. N p , ##EQU00003##
k belongs to integer.
2 ) q = 2 N p b . 3 ) N = log 2 ( 2 N p b ) , ##EQU00004##
N belongs to integer.
[0023] When the number of poles (b) in the selected repeating unit,
the number of repeating units (q) and the maximum shifting times
(N) in Step five are determined, the total torque can be composed
of partial torque produced by each repeating unit. That is
T = i = 1 q T i , ##EQU00005##
where T.sub.i is torque produced by the i.sup.th repeating
unit.
[0024] Further, in Step six, wherein the accurate angle
(.theta..sub.n) of magnet shifting for the n.sup.th time are
calculated by
[0025] Step 6.1, the torque expression of the motor can be
expressed as the sum of the average torque and torque ripple, which
is as follows:
{ T = T all _ av + T all _ rip T all _ rip = n = 1 .infin. T rn sin
N p s n .alpha. = q n = 1 .infin. T prn sin N p s n .alpha.
##EQU00006##
where the T.sub.all_av represents the average torque and the
T.sub.all_rip represents the torque ripple. According to the
periodicity of torque ripple, it can be expressed as the form of
the Fourier series.
[0026] Step 6.2, the torque T of a motor can be expressed as the
sum of the partial torque component T.sub.i produced by the
i.sup.th repeating unit. And the partial torque component T.sub.i
can also be expressed as the sum of the corresponding partial
average value component and the corresponding partial torque
ripple. When one repeating unit is shifted by .theta. degrees, the
corresponding partial torque ripple produced by the shifted
repeating unit changes only in phase. That is
T rip ' = n = 1 .infin. T prn sin N p s n ( .alpha. + .theta. )
##EQU00007##
[0027] Step 6.3, the total torque ripple is superposed by the
torque ripple produced by shifted repeating units and that of fixed
repeated units:
T all _ rip = q 2 j = 1 2 n = 1 .infin. T prjn sin N p s n (
.alpha. + ( j - 1 ) .theta. ) ##EQU00008##
[0028] Step 6.4, based on these, the output torque can be further
expressed as
T = q 2 j = 1 2 ( T pavj + n = 1 .infin. T prjn sin N p s n (
.alpha. + ( j - 1 ) .theta. ) ) ##EQU00009##
where, the T.sub.pavj represents the average torque produced by the
j.sup.th repeating unit. Before the magnet shifting, the partial
average torque produced by each repeating unit is the same as each
other, that is, T.sub.pavj=T.sub.pav.
[0029] Step 6.5, after the magnet shifting, the rotor is caused to
be slightly asymmetrical. Therefore, the partial average torque of
each repeating unit makes a tiny change that is far lower than
value of torque ripple. The specific relationship is expressed
as
{ T pavj = T pav + .DELTA. T j T prjn = T prn + .DELTA. T rj where
{ .DELTA. T = q 2 j = 1 2 .DELTA. T j + q 2 j = 1 2 n = 1 .infin.
.DELTA. T rj sin N p s n ( .alpha. + ( j - 1 ) .theta. ) T r = q 2
j = 1 2 n = 1 .infin. T p rn sin N p s n ( .alpha. + ( j - 1 )
.theta. ) ##EQU00010##
[0030] In the formula, T.sub.r is the main component of the torque
ripple, which is recognized as the main study object. By using the
trigonometric function formula, it is simplified as
T r = q 2 n = 1 .infin. T prn sin N p s n .theta. sin N p s n
.theta. 2 sin ( N p s n ( .alpha. + 3 2 .theta. ) )
##EQU00011##
[0031] Step 6.6, in order to reduce torque ripple, T.sub.r is
supposed to be as small as possible and, in the extreme, to be
zero. Then, the shifting angle is
.theta. n = 180 .degree. nN p s or .theta. n = .pi. nN p s ,
##EQU00012##
where .theta..sub.n represents the shifting angle that eliminates
the n.sup.th main subharmonic of the torque ripple. When n=1,
magnet shifting by .theta..sub.1 degrees can eliminate the first
main harmonic of the torque ripple. When n=2, magnet shifting by
.theta..sub.2 degrees can eliminate the second main harmonic of the
torque ripple.
[0032] Further, in Step six, the first magnet shifting in Step six
means that the selected basic repeating unit is alternately shifted
by .theta..sub.1 degrees.
[0033] Further, in Step seven, the second magnet shifting in Step
seven means that the shifted basic repeating unit and the adjacent
fixed basic repeating unit are chosen as one new repeating unit.
For every pair of adjacent new repeating units, one new repeating
unit is fixed, and the other new repeating unit is alternately
shifted by .theta..sub.2 degree. The second magnet shifting in Step
seven is supposed to keep the same the shifting direction as the
first magnet shifting in Step six.
[0034] The beneficial effect of the disclosure:
[0035] a) In the disclosure, the magnet shifting method not only
reduces the torque ripple component caused by cogging torque, but
also effectively reduces the torque ripple caused by permanent
magnet torque or reluctance torque. Also, optimization of back-EMF
and reduction of output torque ripple can significantly improve the
stability of permanent magnet synchronous motors.
[0036] b) In the disclosure, the magnet shifting method
comprehensively considers the minimum number of magnetic poles in
each basic repeating unit that produces total torque (N.sub.0) and
the minimum number of magnetic poles in each basic repeating unit
that produces partial torque ripple component (N.sub.i0). Under the
premise of reducing torque ripple significantly, the average output
torque is maintained to be nearly the same as the original
value.
[0037] c) In the disclosure, the magnet shifting method contains
different choices of shifted repeating units. According to the main
source of torque ripple, the shifted repeating unit can be
reasonably chosen so that different kinds of motors can achieve
similar and effective results.
[0038] d) In the disclosure, the magnet shifting method contains
superposed effects from several magnets shifting. According to the
requirements, the different subharmonics of torque ripple can be
deeply weakened.
[0039] e) In the disclosure, the described magnet shifting method
introduces less harmonic components of radial force density, which
are inevitable. Compared with traditional magnet shifting methods,
it can ease vibration and noise.
BRIEF DESCRIPTION OF THE DRAWINGS
[0040] The disclosure can be better understood by reading the
following detailed description of non-restrictive illustrative
embodiments while examining the appended drawings, wherein:
[0041] FIG. 1 schematically and partially illustrates, in
perspective, magnet shifting ways and choices of a repeating unit
according to an illustrative embodiment of the disclosure. Panel
(a): Schematic diagram of the permanent magnet distribution of the
original motor. Panel (b): Schematic diagram of the permanent
magnet distribution of the first shifted motor. Panel (c):
Schematic diagram of the permanent magnet distribution of the
second shifted motor.
[0042] FIG. 2 schematically and partially illustrates structure
cross-section of an inset-mounted permanent magnet synchronous
motor (an original motor).
[0043] FIG. 3 shows a comparison diagram of reluctance torques
between the original motor and the modified motor with magnet
shifting of one embodiment of the motor disclosed herein.
[0044] FIG. 4 shows harmonic analysis of reluctance torques between
the original motor and one embodiment of the motor disclosed
herein.
[0045] FIG. 5 shows a comparison diagram of permanent magnet
torques between the original motor and one embodiment of the motor
disclosed herein.
[0046] FIG. 6 shows harmonic analysis of permanent magnet torques
between the original motor and one embodiment of the motor
disclosed herein.
[0047] FIG. 7 shows a comparison diagram of back-EMFs between the
original motor and one embodiment of the motor disclosed
herein.
[0048] FIG. 8 shows harmonic analysis of back-EMFs between the
original motor and one embodiment of the motor disclosed
herein.
[0049] FIG. 9 shows a comparison diagram of output torques between
the original motor and one embodiment of the motor disclosed
herein.
[0050] FIG. 10 shows harmonic analysis of output torques between
the original motor and one embodiment of the motor disclosed
herein.
[0051] FIG. 11 shows harmonic analysis of radial force densities
between the existing technology and this disclosure.
[0052] FIG. 12 shows a flow chart of magnet shifting as disclosed
herein.
DETAILED DESCRIPTION
[0053] With reference to the appended drawings in the embodiment of
the disclosure, the detailed embodiment of the disclosure is
clearly and completely described in the following.
[0054] The following embodiments are for example only and not as a
limitation to the disclosure.
[0055] As shown in FIG. 2, an inset-mounted permanent magnet
synchronous motor with three phases comprising an outer stator (1)
and an inner rotor (2). The outer stator (1) includes forty-eight
stator slots and embedded armature windings (4), and the inner
rotor (2) includes a rotor core, eight magnetic poles (3) and six
ventilation holes (5).
[0056] A three-phase inset-mounted permanent magnet synchronous
motor is taken as an example, whose implementation steps are shown
in FIG. 12.
[0057] 1) Torque of target motor with different combination between
poles and slots is analyzed. According to the relationship between
the number of poles and slots, the fluctuation period number of
torque ripple in one electric cycle is calculated to determine the
general trend of its fluctuation. The fluctuation period number of
torque ripple in one electric cycle is calculated by
T ripple = N p s N p . ##EQU00013##
The calculating result is
T ripple = N p s N p = 48 4 = 12 , ##EQU00014##
where N.sub.s=48, N.sub.p=4; N.sub.ps=LCM(N.sub.s,
2N.sub.p)=LCM(48, 8)=48. The target motor includes a surface
mounted motor, a surface-inset motor and an interior embedded
motor.
[0058] 2) The rotor and magnets of the motor are modularized by
calculating the minimum number of magnetic poles (N.sub.0) in each
module. Through modular analysis, the magnetic poles in each module
can produce the same torque with consistency in waveform and phase.
Then, each module containing the fewest magnetic poles is
recognized as one basic repeating unit. The minimum number of
magnetic poles (N.sub.0) in each basic repeating unit is calculated
by
N 0 = N p s N s , ##EQU00015##
where N.sub.0 is the minimum number of magnetic poles in each basic
repeating unit, and N.sub.s is the slot number.
[0059] In the described step 2), the minimum number of magnetic
poles in each basic repeating unit equals to one. That is
N.sub.0=1.
[0060] In the described step 2), the number of magnetic poles is
eight (2N.sub.p=8). According to the pole number of repeating
units, the rotor of the target motor is modularized as eight basic
partial modules. Each basic module is recognized as one basic
repeating unit.
[0061] As shown in FIG. 1, Panel (a), a rotor of the original motor
has eight magnetic poles. They are divided into eight groups
(M1-M8), and each pole (Mi) is recognized as one basic repeating
unit.
[0062] 3) Two or more of basic repeating units can be merged to
form some new repeating units, all of which can also produce the
same torques with consistency in waveform and phase. A different
number of new repeating units can be combined to generate different
magnet shifting ways.
[0063] In the described step 3), the "new repeating unit" consists
of k basic repeating units, and the pole number of a "new repeating
unit" is kN.sub.0 (k=1, 2, 4). Three different repeating units are
available for selection in all.
[0064] 4) The main source of torque and torque ripple are analyzed,
and their generation is modularized and analyzed. The basic
repeating unit to produce the main source of torque and torque
ripple is determined, and the minimum pole number (N.sub.i0) in
each basic repeating unit is calculated.
[0065] Table I gives the torque performances of the original motor.
It can be seen that the total torque ripple is 35.9%. The
percentage of cogging torque is only 1.3% while the peak-to-peak
value of reluctance torque is high, approximately 52.5 Nm, which
accounts for 22% of total average torque. In addition, the
peak-to-peak value of permanent magnet torque accounts for 12% of
total average torque. Therefore, the reluctance torque ripple and
the permanent magnet torque ripple are the main source of total
torque ripple.
[0066] In the described step 4), the minimum pole number in each
basic repeating unit that produces the same reluctance torque is
calculated and equals to one, and that of permanent magnet torque
equals to two. That is N.sub.20=1, N.sub.30=2.
TABLE-US-00001 TABLE I Torque Performances of the target motor
Parameter Value Average output torque (Nm) 244 Peak-to-peak value
of cogging torque (Nm) 1.7 Peak-to-peak value of reluctance torque
(Nm) 52.5 Torque ripple (%) 35.9 Cogging torque ripple ratio (%)
1.3 Reluctance torque ripple ratio (%) 22 Permanent magnet torque
ripple ratio (%) 12
[0067] 5) Considering the N.sub.0 and N.sub.i0 comprehensively,
shifting repeating unit is chosen reasonably. According to the
number of poles in the selected repeating unit (b), the number of
repeating units (q) and the maximum shifting times (N) are
determined respectively. When the number of poles (b) in the
selected repeating unit, the number of repeating units (q) and the
maximum shifting times (N) in Step five are determined, the total
torque can be composed of partial torque produced by each repeating
unit. That is
T = i = 1 q T i , ##EQU00016##
where T.sub.i is torque produced by the i.sup.th repeating unit.
Here, the number of poles (b) in the selected repeating unit, the
number of repeating units (q) and the maximum shifting times (N)
are respectively determined by
1 ) { b = kN 0 b ma x .ltoreq. N p , ##EQU00017##
k belongs to integer.
2 ) q = 2 N p b . 3 ) N = log 2 ( 2 N p b ) , ##EQU00018##
N belongs to integer.
[0068] In the described step 2), N.sub.0=1.
[0069] In the described step 4), N.sub.20=, N.sub.30=2.
[0070] Considering the N.sub.0, N.sub.20 and N.sub.30
comprehensively, two basic repeating units are chosen as first
repeating unit to comprehensively consider crossing effect between
reluctance torque and permanent magnet torque. That is b=2.
[0071] On this basis, the number of repeating unit equals to four
and the maximum shifting times equals to two. That is q=4, N=2.
[0072] As shown in FIG. 1, Panel (b), one pair of magnetic poles
(two basic repeating units) is chosen as first repeating unit and
they are (M1, M2), (M3, M4), (M5, M6), and (M7, M8), respectively.
All of these are chosen to eliminate the first main harmonic of
torque ripple.
[0073] In order to weaken the first main harmonic of torque ripple,
the accurate angle (.theta..sub.1) of magnet shifting for the first
time is calculated, and the selected first repeating unit is
shifted anti-clockwise by .theta..sub.1 degrees for the first time.
The shifting angles are calculated by
[0074] Step 6.1, the torque expression of the motor can be
expressed as the sum of the average torque and torque ripple, which
is as follows:
{ T = T all _ av + T all _ rip T all _ rip = n = 1 .infin. T rn sin
N p s n .alpha. = q n = 1 .infin. T prn sin N p s n .alpha.
##EQU00019##
where the T.sub.all_av represents the average torque and the
T.sub.all_rip represents the torque ripple. According to the
periodicity of torque ripple, it can be expressed as the form of
the Fourier series.
[0075] Step 6.2, the torque T of the motor can be expressed as the
sum of the partial torque component T produced by the i.sup.th
repeating unit. And the partial torque component T.sub.i can also
be expressed as the sum of the corresponding partial average value
component and the corresponding partial torque ripple. When one
repeating unit is shifted by .theta. degrees, the corresponding
partial torque ripple produced by the shifted repeating unit
changes only in phase. That is
T rip ' = n = 1 .infin. T prn sin N p s n ( .alpha. + .theta. )
##EQU00020##
[0076] Step 6.3, the total torque ripple is superposed by the
torque ripple produced by shifted repeating units and that of fixed
repeated units:
T all _ rip = q 2 j = 1 2 n = 1 .infin. T prjn sin N p s n (
.alpha. + ( j - 1 ) .theta. ) ##EQU00021##
[0077] Step 6.4, based on these, the output torque can be further
expressed as
T = q 2 j = 1 2 ( T pavj + n = 1 .infin. T prjn sin N p s n (
.alpha. + ( j - 1 ) .theta. ) ) ##EQU00022##
where, the T.sub.pavj represents the average torque produced by the
j.sup.th repeating unit. Before the magnet shifting, the partial
average torque produced by each repeating unit is the same as each
other, that is, T.sub.pavj=T.sub.pav.
[0078] Step 6.5, after the magnet shifting, the rotor is caused to
be slightly asymmetrical. Therefore, the partial average torque of
each repeating unit makes a tiny change that is far lower than
value of torque ripple. The specific relationship is expressed
as
{ T pavj = T pav + .DELTA. T j T prjn = T prn + .DELTA. T rj where
{ .DELTA. T = q 2 j = 1 2 .DELTA. T j + q 2 j = 1 2 n = 1 .infin.
.DELTA. T rj sin N p s n ( .alpha. + ( j - 1 ) .theta. ) T r = q 2
j = 1 2 n = 1 .infin. T prn sin N p s n ( .alpha. + ( j - 1 )
.theta. ) ##EQU00023##
[0079] In the formula, T.sub.r is the main component of the torque
ripple, which is recognized as the main study object. By using the
trigonometric function formula, it is simplified as
T r = q 2 n = 1 .infin. T prn sin N p s n .theta. sin N p s n
.theta. 2 sin ( N p s n ( .alpha. + 3 2 .theta. ) ) .
##EQU00024##
[0080] Step 6.6, in order to reduce torque ripple, T.sub.r is
supposed to be as small as possible and, in the extreme, to be
zero. Then, the shifting angle is
.theta. n = 180 .degree. n N p s or .theta. n = .pi. n N p s ,
##EQU00025##
where .theta..sub.n represents the shifting angle that eliminates
the n.sup.th main subharmonic of the torque ripple. When n=1,
magnet shifting by .theta..sub.1 degrees can eliminate the first
main harmonic of the torque ripple. When n=2, magnet shifting by
.theta..sub.2 degrees can eliminate the second main harmonic of the
torque ripple.
[0081] Here, the accurate angle of magnet shifting for the first
time (.theta..sub.1) is calculated and equals to 3.75 degrees. That
is .theta..sub.1=180.degree./48=3.75.degree.. As shown in FIG. 1,
Panel (b), for every pair of adjacent repeating units, one
repeating unit ((M1, M2) or (M5, M6)) is alternately shifted by
.theta..sub.1 degree, and the other repeating unit ((M3, M4) or
(M7, M8)) is fixed.
[0082] 6) In order to weaken the second main harmonic of torque
ripple, the accurate angle (.theta..sub.2) of magnet shifting for
the second time is calculated. Based on the first magnet shifting,
the shifted basic repeating unit and the adjacent fixed basic
repeating unit are chosen as one new repeating unit. The new
repeating units are reconsidered and then alternately shifted by
.theta..sub.2 degrees. The new repeating unit is named "second
repeating unit."
[0083] In the described step 7), the accurate angle of magnet
shifting for the second time (.theta..sub.2) is calculated and
equals to 1.875 degrees. That is
.theta..sub.2=1800/2.times.48=1.875.degree..
[0084] As shown in FIG. 1, Panel (c), based on the first magnet
shifting, the shifted basic repeating unit (M1, M2) and the
adjacent fixed basic repeating unit (M3, M4) are chosen as one new
repeating unit. That is (M1, M2, M3, M4), named "second repeating
unit." Similarly, the other second repeating unit is (M5, M6, M7,
M8). For every pair of adjacent new repeating units, one new
repeating unit (M5, M6, M7, M8) is fixed, and the other new
repeating unit (M1, M2, M3, M4) is shifted by .theta..sub.2 degree
and named the "second magnet shifting." The second magnet shifting
in Step seven is supposed to keep the same shifting direction as
the first magnet shifting in Step six.
[0085] Table II lists the angles of magnets shifting for reducing
first main and second main harmonics.
TABLE-US-00002 TABLE II Shifting Angle of Every Repeating Unit
Shifting Angle of Reduction n.sup.th Main Repeating Harmonics
(deg.) Unit 1.sup.st 2.sup.nd (M1, M2) .theta..sub.1 (3.75)
.theta..sub.1 (3.75) + .theta..sub.2 (1.875) (M3, M4) 0
.theta..sub.2 (1.875) (M5, M6) .theta..sub.1 (3.75) .theta..sub.1
(3.75) (M7, M8) 0 0
[0086] FIG. 2 illustrates the cross-sectional structure of an
inset-mounted permanent magnet synchronous motor (the original
motor). Based on the original motor, magnetic poles are shifted to
obtain one embodiment of the motor disclosed herein. Comparing the
torque performance between the original and the embodiments of the
motors disclosed herein, the beneficial effect of the disclosure
can be clearly shown.
[0087] FIG. 3 and FIG. 4 show comparison diagrams and their
harmonic analysis of reluctance torques (main source of torque
ripple) between the original motor and the modified motor with
magnet shifting (one embodiment of the motor disclosed herein). It
can be seen from FIG. 3 that the peak-to-peak value of reluctance
torque has been greatly reduced from 52.5 Nm to 25.2 Nm after the
first magnet shifting. Moreover, the peak-to-peak value of
reluctance torque has been further reduced to 14.2 Nm after the
second magnet shifting. At the same time, it can be seen from the
FIG. 4 that the first main harmonic (6.sup.th harmonic) and the
second main harmonic (12.sup.th harmonic) are successively
eliminated.
[0088] FIG. 5 and FIG. 6 show comparison diagrams and their
harmonic analysis of permanent magnet torques (the other main
source of torque ripple) between the original motor and one
embodiment of the motor disclosed herein. It can be seen from FIG.
5 that the peak-to-peak value of permanent magnet torque has been
greatly reduced from 49.1 Nm to 11.9 Nm after magnet shifting
twice. At the same time, it can be seen from the FIG. 6 that the
first main harmonic (6.sup.th harmonic) is eliminated.
[0089] FIG. 7 and FIG. 8 show comparison diagrams and their
harmonic analysis of back electromotive force (EMF) between the
original motor and one embodiment of the motor disclosed herein. It
can be seen from FIG. 7 that the sinusoidal characteristic of the
back-EMF has been greatly improved, compared with the original
motor. In addition, it can be seen from FIG. 8 that not only some
harmonics are greatly eliminated, but the amplitude of fundamental
back-EMF is almost constant with that of the original motor. That
is, the torque ripple can be greatly reduced while the torque
density can be nearly maintained.
[0090] FIG. 9 and FIG. 10 show comparison diagrams and their
harmonic analysis of output torques between the original motor and
one embodiment of the motor disclosed herein. It can be seen that
the torque performance has been effectively improved. After the
first magnet shifting, torque ripple is greatly reduced from 35.9%
to 12.7%. After the second magnet shifting, torque ripple is
reduced further to 7.9%. Also, it can be seen from FIG. 10 that the
first main harmonic (6.sup.th harmonic) and the second main
harmonic (12.sup.th harmonic) are successively eliminated.
[0091] FIG. 11 shows harmonic analysis of radial force densities
between the existing magnet shifting technology and the disclosure.
It can be seen from FIG. 11 that the lowest order harmonic of
radial force density in the disclosure is the fifth order harmonic
while that of the existing magnet shifting technology are the third
order harmonic. The former is higher than the latter. Moreover,
harmonic amplitude of the disclosure is lower than that of the
existing magnet shifting technology, and the contained harmonic
content in the disclosure is less than that of the existing magnet
shifting technology. This means, magnets shifting in the disclosure
may cause relatively less vibration and acoustic noise.
[0092] In summary, the application discloses a method named "Magnet
Shifting" to reduce torque ripple of permanent magnet synchronous
motors. Reasonable repeating unit is chosen to shift, so as to
reduce the main source of torque ripple, optimize the back-EMF, and
maintain torque density. It is involved in the way of reasonably
choosing the repeating unit of magnetic pole, the shifting ways and
the shifting angle calculation of the first and second magnet
shifting, which are carried on the repeating unit of magnetic poles
individually or repeatedly to improve the performance of the motor.
It also can quickly calculate the shifting angle of the magnetic
pole by reasonably choosing the repeating unit. Magnet shifting can
effectively enhance the sinusoidal degree of back electrodynamic
force (back-EMF) waveform, where the repeating units can offset the
torque ripple between the maximum and the minimum value to reduce
the different torque harmonics. Also, the output torque can be
maintained nearly to the original value while less vibration noise
of the motor is inevitably introduced.
[0093] While the method herein described, and the forms of
apparatus for carrying this method into effect, constitute
preferred embodiments of this disclosure, it is to be understood
that the invention is not limited to this precise method and forms
of apparatus, and that changes may be made in either without
departing form the scope of the invention, which is defined in the
appended claims.
* * * * *