JPS62268339A - Three-phase synchronous motor - Google Patents

Three-phase synchronous motor

Info

Publication number
JPS62268339A
JPS62268339A JP8252086A JP8252086A JPS62268339A JP S62268339 A JPS62268339 A JP S62268339A JP 8252086 A JP8252086 A JP 8252086A JP 8252086 A JP8252086 A JP 8252086A JP S62268339 A JPS62268339 A JP S62268339A
Authority
JP
Japan
Prior art keywords
harmonic
harmonics
synchronous motor
influence
phase synchronous
Prior art date
Legal status (The legal status is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the status listed.)
Pending
Application number
JP8252086A
Other languages
Japanese (ja)
Inventor
Hiroshi Iijima
飯島 博
Tetsuo Endo
遠藤 哲男
Yukio Miyamoto
宮本 由紀夫
Kiyokazu Okamoto
清和 岡本
Current Assignee (The listed assignees may be inaccurate. Google has not performed a legal analysis and makes no representation or warranty as to the accuracy of the list.)
NEC Corp
Nippon Electric Industry Co Ltd
Original Assignee
NEC Corp
Nippon Electric Industry Co Ltd
Priority date (The priority date is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the date listed.)
Filing date
Publication date
Application filed by NEC Corp, Nippon Electric Industry Co Ltd filed Critical NEC Corp
Priority to JP8252086A priority Critical patent/JPS62268339A/en
Publication of JPS62268339A publication Critical patent/JPS62268339A/en
Pending legal-status Critical Current

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  • Synchronous Machinery (AREA)

Abstract

PURPOSE:To reduce the occurrence of abnormal torque by removing the influential higher harmonics of high degree in particular of what is contained in the void flux which causes abnormal torque to a three-phase synchronous motor. CONSTITUTION:A three-phase synchronous motor is constituted by relatively skewing the conductor groove of a stator core by an electrics angle of 2pi/n (where n represents the degree of higher harmonics selected as an object for removing the influence) against a rotor pole 3. The rotor pole 3 arranged through an interpolar separating groove 4 skews one cycle of higher harmonics, i.e. by an electric angle of 2pi/n, using n for the higher harmonic degree. Thus, in the part corresponding to the n-th degree higher harmonics of the torque produced to the rotor pole 3, the n-th degree higher harmonic torques are induced, which have the reverse direction and size one another. Consequently, the n-th degree higher harmonic torquew of the void flux acting on the rotor pole is cancelled and no influence gets exercised. The abnormal torque by the n-th degree higher harmonics is therefore produce no longer.

Description

【発明の詳細な説明】 〔産業上の利用分野〕 本発明はトルクの平滑化をはかった比較的小容量(例え
ば出力31(W以下〉の三和同3IJl電動機に関する
ものである。
DETAILED DESCRIPTION OF THE INVENTION [Industrial Field of Application] The present invention relates to a Sanwa Do 3IJl electric motor with a relatively small capacity (for example, an output of 31 W or less) which is designed to smooth torque.

〔従来の技術〕[Conventional technology]

三相同期電動機においては、固定子(−次側)鉄心と回
転子(二次側)磁極の間の空隙に発生する磁束(以下「
空隙磁束」と言う。)に種々の高調波(第5.7,11
,13.17・・・・・・等の次数の高調波)が含まれ
ていて磁束変動が化している。
In a three-phase synchronous motor, magnetic flux (hereinafter referred to as "
air gap magnetic flux. ) to various harmonics (5.7th, 11th
, 13, 17, etc.) are included, resulting in magnetic flux fluctuations.

そのためこれら高調波の影響を受けてl−ルクリソプル
(トルクが大きくなったり小さくなったり変動すること
。以下「異常トルク」と言う。)が発生ずる。これを避
けるために、固定子鉄心の導体溝(スロット)を回転子
磁極に対しスキj〜−することが多く行なわれている。
Therefore, under the influence of these harmonics, l-lucrysopulus (torque increases or decreases or fluctuates; hereinafter referred to as "abnormal torque") occurs. In order to avoid this, the conductor grooves (slots) of the stator core are often spaced from the rotor magnetic poles.

従来、スキューは空隙磁束を平滑化するという考えに基
づき、第3図に示したように一般に固定子の1スロット
ピンチ行なうようにしている。なお、第3図において、
1は固定子鉄心、2は固定子のスロット、3は回転子磁
極、4はスキューされた磁極の間の分離溝である。
Conventionally, the skew is based on the idea that the air gap magnetic flux is smoothed, and the stator is generally pinched by one slot as shown in FIG. In addition, in Figure 3,
1 is a stator core, 2 is a stator slot, 3 is a rotor magnetic pole, and 4 is a separation groove between the skewed magnetic poles.

このようにすると、スロット2と磁極の間の分H?#4
が完全に一致して対向することがなく、また固定子と回
転子の間の磁束通路は常に確保されるので、空隙におけ
る磁束の変動が少なくなり、異常トルク発生が軽減され
る。
In this way, the distance between slot 2 and the magnetic pole H? #4
Since the stator and the rotor do not completely match and face each other, and the magnetic flux path between the stator and rotor is always secured, fluctuations in the magnetic flux in the air gap are reduced, and abnormal torque generation is reduced.

一方、空隙磁束の変動そのものを小さくするごとも考え
られており、固定子に設りるスロソ1〜数を多くしたり
、スn 、、 l・の開口を塞いだりする設計も行なわ
れている。
On the other hand, it is also being considered to reduce the fluctuation of the air gap magnetic flux itself, and designs are being made to increase the number of slots installed in the stator or to close the openings of the slots. .

〔解決しようとする問題点〕[Problem to be solved]

上述したように異常トルク発イ1−を防止するために種
々の対策が施されている。しかしながら、いずれも異常
トルク発η−の要因たる高調波に着目して直接的に対策
を施しているものでないために、どうしてもトルクリッ
プルが残ってしまうという問題がある。
As mentioned above, various measures have been taken to prevent abnormal torque generation. However, none of these methods focus on the harmonics that are the cause of abnormal torque generation and take direct countermeasures, so there is a problem in that torque ripples inevitably remain.

例えば従来行なわれている固定子の導体溝のスキューで
は、比較的高次の高#jA]波(例えば第11次以上)
の影響は除去できるが、影響力の大きい次数(例えば第
5次、第7次)の高調波はたまたま除去されている場合
もあるが、除去されずに残ってトルクリップルを発生さ
せている場合が多い。
For example, in the conventional skew of the conductor grooves of the stator, relatively high-order high #jA] waves (e.g., 11th order or higher) are generated.
The effects of harmonics can be removed, but harmonics with a large influence (for example, the 5th or 7th order) may be removed by chance, but if they remain without being removed and cause torque ripple. There are many.

また、固定子のス1コツト数を多くしてトルクの平滑化
をはかる方法は、大型の電動機の場合には可能であり効
果的であるが、小型の電動機では製造上の制約をうける
のでスロソ1〜数をあまり多くすることはてきない。
In addition, the method of increasing the number of slots in the stator to smooth the torque is possible and effective for large motors, but it is subject to manufacturing constraints for small motors, so It is not possible to increase the number from 1 to too many.

さらに、スロットの開口を塞ぐという方法は、製造工程
が複雑であり、ごく限られた分野の電動機にしか採用さ
れていない。
Furthermore, the method of closing the opening of the slot requires a complicated manufacturing process, and is only used in electric motors in a very limited field.

本発明は上記の事情を考え合わせてなされたもので、製
造上の制約が少なく、異常トルクの発生も少ない三相同
期電動機を捉供することを目的とするものである。
The present invention has been made in consideration of the above-mentioned circumstances, and aims to provide a three-phase synchronous motor with fewer manufacturing restrictions and with less occurrence of abnormal torque.

〔問題点を解決するための手段〕[Means for solving problems]

上記の目的を達成するために、本発明の三相同期電動機
は、異常トルク発生の原因となる空隙磁束に含まれる高
調波のうち特に影響の大きい次数の高調波を除去するよ
うにした。すなわち、■固定子鉄心の導体溝を回転子磁
極に対し電気角で2π/n (但しnは影響を除去する
ための対象に選んだ高調波の次数)スキューさせた。
In order to achieve the above object, the three-phase synchronous motor of the present invention removes harmonics of a particularly large order among the harmonics contained in the air gap magnetic flux that cause abnormal torque generation. That is, (1) the conductor grooves of the stator core were skewed by 2π/n in electrical angle with respect to the rotor magnetic poles (where n is the order of the harmonic selected as a target for removing the influence).

■つぎに上記の手段でn次(例えば第7次)の高調波を
除去した場合に、除去されなかったr次(例えば第5次
)の高調波の影響が残ってしまうことが考えられる。そ
のような場合には別途r次高調波を除去するχ、1策が
必要になる。その対策は固定子鉄心のスI’l y )
 (溝)数の選び方によって行なうようにした。
(2) Next, when the n-th harmonic (for example, the 7th harmonic) is removed by the above-mentioned means, the influence of the r-th harmonic (for example, the 5th harmonic) that was not removed may remain. In such a case, a separate measure for removing the r-order harmonic is required. The countermeasure is to replace the stator core.
(Groove) It was decided to do this by selecting the number.

すなわち、本願の発明者らは、先に固定子鉄心に設ける
スロット数Nをそれほど大きくしなくても、影響力の大
きい特定の次数の高調波を除去する手段を考えて別途出
願(特願昭61−1884号)しているが、この手段を
合せて採用するようにした。
In other words, the inventors of the present application have devised a method for removing harmonics of a specific order that has a large influence without first increasing the number of slots N provided in the stator core, and have filed a separate patent application (Patent Application No. 61-1884), but this method was also adopted.

その手段を具体的に示すと次の通りである。The specific means for doing so are as follows.

固定子鉄心のスロット数Nは N−極数l×相数m×毎極毎相の溝数qによって決めら
れるが、このうち毎極毎相の溝数qの値を不整数に選ぶ
ようにする。
The number of slots N in the stator core is determined by N - number of poles l x number of phases m x number of grooves for each pole and each phase q, but the value of the number of grooves q for each pole and each phase should be selected as an integer number. do.

また、影響力が大きく特に除去したい高調波の次数をr
とすると、固定子巻線ピッチSを5−(r−t)/r 
 (短節巻の場合)またはs=r/(r+t)   (
長節巻の場合)但し t:奇数 に選ぶようにする。
In addition, the order of harmonics that have a large influence and that you especially want to remove is r
Then, the stator winding pitch S is 5-(rt)/r
(for short section winding) or s=r/(r+t) (
(In the case of long section windings) However, t: Choose an odd number.

上記の関係を満足し、しかも三相平衡巻線が可能なよう
にスロット数Nを決定する。
The number N of slots is determined so that the above relationship is satisfied and three-phase balanced winding is possible.

〔作用〕[Effect]

上述した本発明の手段を採用すると、空隙磁束のうち特
に問題となる二つの次数の高調波の影響が消去される。
When the above-described means of the present invention is adopted, the effects of two harmonics of the air gap magnetic flux, which are particularly problematic, are eliminated.

すなわち、固定子鉄心の導体溝を回転子磁極に対し電気
角で2π/nだけスキューすると、空隙磁束のn次の高
調波によって回転子磁極に発生するトルクリップルは後
述の如く (第1図及び関連説明参照)打消され、n次
高調波のトルクへの影響はなくなる。
In other words, if the conductor grooves of the stator core are skewed by 2π/n in electrical angle with respect to the rotor magnetic poles, the torque ripple generated in the rotor magnetic poles by the n-th harmonic of the air gap magnetic flux will be as described below (Fig. 1 and (see related explanation), and the influence of the n-th harmonic on the torque disappears.

また、固定子のスロット数を前記の設計法に従って決定
すると、全スロット数はそれほどふやさなくても毎極毎
相の溝数qの値を大きくしたのと同じ効果が得られるし
、巻線ピンチを所定の値に選ぶことにより二次回路に特
定(次数r)の高調波電流が流れなくなる(この詳細に
ついては特願昭61−1884号を参照されたい)。
Furthermore, if the number of stator slots is determined according to the design method described above, the same effect as increasing the number of grooves q for each pole and each phase can be obtained without increasing the total number of slots that much, and the winding pinch can be reduced. By selecting a predetermined value, a harmonic current of a specific (order r) will not flow in the secondary circuit (for details, see Japanese Patent Application No. 1884/1984).

従って固定子導体溝に対する回転子磁極のスキューによ
りn次高調波(例えば第7高調波)、固定子側でr次高
調波(例えば第5高調波)の対策を施せば、異常トルク
発生に特に大きい影響を与えている2つの高調波を同時
に除去することができる。
Therefore, if measures are taken against the n-th harmonic (e.g., the 7th harmonic) due to the skew of the rotor magnetic poles with respect to the stator conductor grooves, and the r-th harmonic (e.g., the 5th harmonic) on the stator side, it is possible to prevent abnormal torque generation. Two harmonics that have a large influence can be removed at the same time.

〔実施例〕〔Example〕

次に本発明の実施例を図面を参照して説明する。 Next, embodiments of the present invention will be described with reference to the drawings.

なお、本実施例は特許請求の範囲の一例を示す。Note that this example shows an example of the scope of the claims.

第1図は本発明の詳細な説明図であり、空隙磁束の波形
と固定子導体溝の回転子磁極に対するスキューの関係を
示している。図面並に説明を簡明にするために、空隙磁
束に含まれる第7高調波の影響を除去する場合を示し、
電動機は2極の場合で説明する。
FIG. 1 is a detailed explanatory diagram of the present invention, showing the relationship between the waveform of the air gap magnetic flux and the skew of the stator conductor grooves with respect to the rotor magnetic poles. In order to simplify the drawing and explanation, a case is shown in which the influence of the seventh harmonic included in the air gap magnetic flux is removed,
The explanation will be based on the case where the electric motor has two poles.

第1図において、5は空隙磁束の基本波波形、6は同じ
く第7高調波波形である。Lは固定子磁極間隔、Wは回
転子鉄心幅(回転軸方向の長さ)を示している。基本波
波形5の半サイクル幅が磁極間隔してあり、2極電動機
の場合はπ(機械角−電気角)である。図に示したよう
に分離溝4を介して配置された回転子磁極3は、高調波
次数n(本実施例では第7高調波であるからn−7)と
すると、高調波の1サイクル分すなわち電気角で2π/
nだけスキューする。
In FIG. 1, 5 is the fundamental waveform of the air gap magnetic flux, and 6 is the seventh harmonic waveform. L indicates the stator magnetic pole spacing, and W indicates the rotor core width (length in the rotation axis direction). The half cycle width of the fundamental waveform 5 is spaced apart from the magnetic poles, which is π (mechanical angle minus electrical angle) in the case of a two-pole motor. As shown in the figure, the rotor magnetic poles 3 arranged through the separation grooves 4 correspond to one cycle of the harmonic, assuming that the harmonic order is n (in this example, it is the seventh harmonic, so n-7). In other words, the electrical angle is 2π/
Skew by n.

このようにすると、回転子磁極に発生するトルクの中の
n次高調波に対応する部分は例えば■の位置、■の位置
ではそれぞれ点線に示したようにn次高調波トルク(リ
ップルになる)が誘起され、それらは相互に逆向きの方
向と大きさをもっている。従って、回転子磁極に働く空
隙磁束のn次高調波トルクは打消されて影響がなくなる
。すなわち、このように作られた回転子を備えた同期電
動機ではn次高調波による異常トルクは発生しなくなる
In this way, the part corresponding to the n-th harmonic in the torque generated at the rotor magnetic poles will be the n-th harmonic torque (ripple) at the position ■, and at the position ■, respectively, as shown by the dotted lines. are induced, and they have mutually opposite directions and magnitudes. Therefore, the nth harmonic torque of the air gap magnetic flux acting on the rotor magnetic poles is canceled out and has no effect. That is, in a synchronous motor equipped with a rotor made in this manner, abnormal torque due to n-th harmonics will not occur.

なお、本実施例は高調波次数n=7の場合を図示して説
明したが、本発明はこれに限定されるものではなく、影
響力の大きな高調波次数のものを除去対象に選んでnの
値を決めればよく、例えば第5.7,11,13,17
.・・・・・・等の次数の高調波のうちから所望のもの
を選ぶことができる。
Although this embodiment has been described with reference to the case where the harmonic order n=7, the present invention is not limited to this, and harmonic orders with a large influence are selected to be removed. For example, the values of 5.7, 11, 13, 17
.. A desired harmonic can be selected from harmonics of orders such as .

また、本発明は2極、4極、6極等電動機の極数に関係
なく同様に適用できる。
Furthermore, the present invention can be similarly applied regardless of the number of poles of the motor, such as 2-pole, 4-pole, 6-pole, etc.

上述した固定子導体溝の回転子磁極に対するスキューに
より、異常トルクの発生は大幅に軽減されるが、消去さ
れなかった次数の高調波による異常トルクが残って問題
になる場合がある。このような時は、固定子側でも対策
を施こせばよく、次にその具体的手段を第2図によって
説明する。
Although the above-mentioned skew of the stator conductor grooves with respect to the rotor magnetic poles greatly reduces the occurrence of abnormal torque, abnormal torque due to harmonics of unerased orders may remain and become a problem. In such a case, countermeasures may be taken on the stator side as well, and specific measures will be explained below with reference to FIG.

第2図は固定子の一実施例の説明図であり、図面並に説
明を簡明にするために、空隙磁束に含まれる第5高調波
の影響を除去する場合を示し、かつ小型同期電動機で実
現可能なように固定子鉄心のスロット数Nがなるべく小
さい値をとるように設計したものを示している。
FIG. 2 is an explanatory diagram of one embodiment of the stator, and for the purpose of simplifying the drawing and explanation, it shows the case where the influence of the fifth harmonic included in the air gap magnetic flux is removed, and it is also used in a small synchronous motor. This figure shows a design in which the number N of slots in the stator core is as small as possible to be practical.

すなわち、極数l−2,相数m−3,毎極釦用の溝数q
=2.5(不整数)に選び、スロット数N−2X3X2
.5=15の場合である。そして固定子巻線ピッチは短
節巻で、t=1とした。
That is, the number of poles l-2, the number of phases m-3, the number of grooves for each pole button q
= 2.5 (inconsistent number), number of slots N-2X3X2
.. This is the case when 5=15. The stator winding pitch was short-pitch winding, and t=1.

第2図の(alは固定子のスロットを展開図で示したも
の、同図(b)は磁束分布で基本波と除去対象の第5高
調波を示したもの、同図+c+は固定?!−巻線でスロ
ットの位置及びピッチの関係を示したものである。なお
、図中の7は基本波、8は第5高調波である。
In Figure 2, (al is a developed view of the stator slots, Figure (b) is a magnetic flux distribution showing the fundamental wave and the 5th harmonic to be removed, and +c+ is fixed?! - This figure shows the relationship between slot positions and pitches in the winding. In the figure, 7 is the fundamental wave, and 8 is the fifth harmonic.

本実施例は除去対象とする高調波次数r =5の場合で
あり、固定子巻線ピッチ5−(r−1)/r=415=
0.8となる。すなわち1極当りのスロットは15/2
=7.5であり、それに対し巻線は、7.5スロツトX
 O,8= 6スロソトのところに来るようにする。こ
のようにすると、図に見られるように丁度第5高調波の
4番目の節のところに巻線が来でおり、第5高調波が誘
起されなくなる。
In this example, the harmonic order to be removed is r = 5, and the stator winding pitch is 5 - (r - 1) / r = 415 =
It becomes 0.8. In other words, the slot per pole is 15/2
= 7.5, whereas the winding has 7.5 slots
O, 8= Make it come to 6 slots. By doing this, as shown in the figure, the winding comes exactly at the fourth node of the fifth harmonic, and the fifth harmonic is no longer induced.

次に全スIコント数N−15で、6スロノト毎に巻線を
施こした場合に三相平衡巻線が可能かどうか調べて見る
Next, we will investigate whether three-phase balanced winding is possible when winding is performed every 6 slots with the total number of slots N-15.

三相平衡巻線の可否判別は次式によって行なわれる。The following equation determines whether or not a three-phase balanced winding is possible.

スロット数Nと極対数Pの最大公約数てスロット数Nを
割った値をN。とし、相数をmとすると、N87m−整
数・・・・・・、−の場合は2層巻線が可能、No /
 2 m−整数・・・・・・この場合は単層巻線、2層
巻線が可能である。いずれも不整数の場合は三和平i釦
巻線が出来す、ごのようなス+:r ソl−数は採用で
きないことになる。1 本実施例の場合はN=−15,P=1であるからN、=
15であり、相数m=3であるからNo/m=15/3
=5で整数が得られ、三相平衡巻線が可能なことが分る
N is the value obtained by dividing the number of slots N by the greatest common divisor of the number of slots N and the number of pole pairs P. If the number of phases is m, then N87m-integer..., if -, two-layer winding is possible, No/
2 m-integer...In this case, single-layer winding or two-layer winding is possible. If both are integer numbers, a Sanwahei i-button winding can be created, and a S+:r/Sol- number cannot be adopted. 1 In this example, N=-15 and P=1, so N,=
15, and the number of phases m=3, so No/m=15/3
= 5, an integer is obtained, and it can be seen that three-phase balanced winding is possible.

すなわち、本実施例は実現可能な設計例である。In other words, this example is a feasible design example.

ト述のように固定子を設計するとr次高調波(本実施例
では第5高調波)の影響が除去される。
If the stator is designed as described above, the influence of the r-order harmonic (the fifth harmonic in this embodiment) is removed.

従って、固定Y−鉄心の導体溝の回転子磁極に対するス
キューと、固定子のスロット数N及び巻線ピッチを本発
明の手段によって決めれば、n次及びr次の高調波の影
響を同時に消去することができる。
Therefore, if the skew of the conductor grooves of the fixed Y-iron core with respect to the rotor magnetic poles, the number N of stator slots, and the winding pitch are determined by the means of the present invention, the effects of the n-th and r-th harmonics can be simultaneously eliminated. be able to.

なお、このよ・)に回転子と固定子の両方に高調波対策
を施こす場合には、回転子側で高次(例えば第7高調波
)を、固定子側で低次(例えば第5高調波)のものを除
去するようにすれば、スキューする角度が小さくてすむ
ので回転子の製作が容易になり有利である。
In addition, when applying harmonic countermeasures to both the rotor and stator in this case, high-order harmonics (e.g., the 7th harmonic) are taken care of on the rotor side, and low-order harmonics (e.g., the 5th harmonic) are taken on the stator side. If harmonics) are removed, the skew angle can be small, making it easier to manufacture the rotor, which is advantageous.

〔効果〕〔effect〕

以上説明したように、本発明によれば、異常トルク発生
に大きな影響力をもつ次数の高調波を選んで直接的に消
去できるので、トルクリップルの少ない三相同期電動機
を作ることができる。従ってトルクの滑かさが特に要求
されるサーボ機構の小型駆動源を折伏することが可能に
なる。
As described above, according to the present invention, harmonics of orders that have a large influence on abnormal torque generation can be selected and directly eliminated, so a three-phase synchronous motor with less torque ripple can be manufactured. Therefore, it is possible to fold down a small drive source for a servo mechanism that requires particularly smooth torque.

【図面の簡単な説明】[Brief explanation of drawings]

第1図及び第2図は本発明の詳細な説明図である。第2
図において、(alは固定子のスロットの展開図、fb
lは磁束分布、TC)は固定子巻線の位置を示している
。第3図は従来行なわれている回転子磁極のスキューに
ついての説明図である。 l・・・固定子鉄心、 2・・・スロット、 3・・・回転子磁極、 4・・・磁極間分離溝。 Z 又ひ′人でン
1 and 2 are detailed explanatory views of the present invention. Second
In the figure, (al is a developed view of the stator slot, fb
l indicates the magnetic flux distribution, and TC) indicates the position of the stator winding. FIG. 3 is an explanatory diagram of the conventional skew of rotor magnetic poles. l... Stator core, 2... Slot, 3... Rotor magnetic pole, 4... Separation groove between magnetic poles. Z Matahi'jinden

Claims (1)

【特許請求の範囲】 1、固定子鉄心と回転子磁極の間の空隙に発生する磁束
に含まれる複数の高調波のうち異常トルク発生の要因と
なっている次数の高調波の影響を除去する対策を施こし
た三相同期電動機であって、固定子鉄心の導体溝を回転
子磁極に対し相対的に電気角で2π/n(但しnは影響
を除去するための対象に選んだ高調波の次数)スキュー
させたことを特徴とする三相同期電動機。 2、固定子鉄心と回転子磁極の間の空隙に発生する磁束
に含まれる複数の高調波のうち異常トルク発生の要因と
なっている次数の高調波の影響を除去する対策を施こし
た三相同期電動機であって、固定子鉄心の導体溝を回転
子磁極に対し相対的に電気角で2π/n(但しnは影響
を除去するための対象に選んだ高調波の次数)スキュー
させるとともに、 固定子鉄心のスロット(溝)数Nは N=極数l×相数m×毎極毎相の溝数q によって決める際に毎極毎相の溝数qの値を不整数とし
、かつ固定子巻線ピッチsが s=(r−t)/r または s=r/(r+t) t:奇数 (但しには影響を除去するための対象に選んだ高調波の
次数)の関係を満足し、しかも三相平衡巻線が可能なよ
うに選んだものであることを特徴とする三相同期電動機
。 3、特許請求の範囲第2項において、t=1とした三相
同期電動機。
[Scope of Claims] 1. Eliminate the influence of harmonics of orders that cause abnormal torque generation among multiple harmonics contained in the magnetic flux generated in the air gap between the stator core and the rotor magnetic poles. It is a three-phase synchronous motor with countermeasures, and the conductor grooves of the stator core are relative to the rotor magnetic poles in electrical angle of 2π/n (where n is the harmonics selected to remove the influence). A three-phase synchronous motor characterized by a skew (order of). 2. Measures have been taken to remove the influence of the harmonics of the order that are the cause of abnormal torque generation among the multiple harmonics contained in the magnetic flux generated in the air gap between the stator core and the rotor magnetic poles. In a phase synchronous motor, the conductor grooves of the stator core are skewed by 2π/n in electrical angle relative to the rotor magnetic poles (where n is the order of the harmonic selected as a target for removing the influence), and , The number N of slots (grooves) in the stator core is determined by N = number of poles l x number of phases m x number of grooves per pole and each phase q, where the value of the number of grooves q per pole and each phase is an integer number, and The stator winding pitch s satisfies the relationship s=(r-t)/r or s=r/(r+t) where t is an odd number (however, the order of the harmonic selected as a target for removing the influence). Moreover, a three-phase synchronous motor is selected to enable three-phase balanced winding. 3. A three-phase synchronous motor in which t=1 in claim 2.
JP8252086A 1986-04-10 1986-04-10 Three-phase synchronous motor Pending JPS62268339A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP8252086A JPS62268339A (en) 1986-04-10 1986-04-10 Three-phase synchronous motor

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP8252086A JPS62268339A (en) 1986-04-10 1986-04-10 Three-phase synchronous motor

Publications (1)

Publication Number Publication Date
JPS62268339A true JPS62268339A (en) 1987-11-20

Family

ID=13776808

Family Applications (1)

Application Number Title Priority Date Filing Date
JP8252086A Pending JPS62268339A (en) 1986-04-10 1986-04-10 Three-phase synchronous motor

Country Status (1)

Country Link
JP (1) JPS62268339A (en)

Cited By (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US6853105B2 (en) 2000-05-25 2005-02-08 Mitsubishi Denki Kabushiki Kaisha Permanent magnet motor
DE10125005B4 (en) * 2000-05-25 2018-07-12 Mitsubishi Denki K.K. Permanent magnet motor

Citations (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS5325813A (en) * 1976-08-23 1978-03-10 Mitsubishi Electric Corp Inductor type synchronous

Patent Citations (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS5325813A (en) * 1976-08-23 1978-03-10 Mitsubishi Electric Corp Inductor type synchronous

Cited By (3)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US6853105B2 (en) 2000-05-25 2005-02-08 Mitsubishi Denki Kabushiki Kaisha Permanent magnet motor
US6876116B2 (en) 2000-05-25 2005-04-05 Mitsubishi Denki Kabushiki Kaisha Permanent magnet motor
DE10125005B4 (en) * 2000-05-25 2018-07-12 Mitsubishi Denki K.K. Permanent magnet motor

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