JPH0150182B2 - - Google Patents
Info
- Publication number
- JPH0150182B2 JPH0150182B2 JP58166308A JP16630883A JPH0150182B2 JP H0150182 B2 JPH0150182 B2 JP H0150182B2 JP 58166308 A JP58166308 A JP 58166308A JP 16630883 A JP16630883 A JP 16630883A JP H0150182 B2 JPH0150182 B2 JP H0150182B2
- Authority
- JP
- Japan
- Prior art keywords
- ring
- shaped core
- field
- toroidal coil
- toroidal
- 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.)
- Expired
Links
Classifications
-
- H—ELECTRICITY
- H02—GENERATION; CONVERSION OR DISTRIBUTION OF ELECTRIC POWER
- H02K—DYNAMO-ELECTRIC MACHINES
- H02K21/00—Synchronous motors having permanent magnets; Synchronous generators having permanent magnets
- H02K21/12—Synchronous motors having permanent magnets; Synchronous generators having permanent magnets with stationary armatures and rotating magnets
- H02K21/14—Synchronous motors having permanent magnets; Synchronous generators having permanent magnets with stationary armatures and rotating magnets with magnets rotating within the armatures
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- Engineering & Computer Science (AREA)
- Power Engineering (AREA)
- Permanent Magnet Type Synchronous Machine (AREA)
Description
【発明の詳細な説明】
本発明はトロイダルコイル型回転電機に関する
ものである。DETAILED DESCRIPTION OF THE INVENTION The present invention relates to a toroidal coil type rotating electric machine.
一般に、トロイダルコイル型回転電機は環状鉄
心の上に、例えば4極構成のものであれば約90゜
ごとに分割された4個のトロイダルコイルを有す
る電機子と、この各コイルに対し、あるギヤツプ
をへだてた磁極を有する界磁とから成り、界磁は
それに含まれる永久磁石によつて上記磁極から電
機子の環状鉄心に対し、その半径方向に磁束を生
ずるように構成されている。この4極の例では、
界磁の磁極は順にN極、S極、N極、S極という
風に交互に異極となつている。対応する電機子の
4個のコイルも、順に捲回方向が交互に逆になる
ように巻かれている。この電機子のコイルも仮り
にシリースにつながれているものとして、このコ
イルに或る大きさの電流を流すと、界磁と電機子
との間にトルクを生じ、このトルクは電流の大き
さに比例し、また電流の方向によつてトルクの方
向が定まる。今、仮りに電機子が外側にあり、界
磁がその内側にあつて、電機子を固定子として用
い、界磁を回転子として用いる場合を考えること
にしよう。このようなトロイダルコイル型回転電
機は、通常、回転子の回転の範囲がある角度、た
とえば基準位置を中心にプラス・マイナス20゜の
範囲という風に限られている場合に用いられる。
用途例としては、油圧回転弁の制御とか、限られ
た範囲の回転サーボ系のサーボモータなどの場合
があげられる。このような用途に対しトロイダル
コイル型回転電機は、整流子とかスリツプリング
とかが全くないので、直流機なのに交流誘導機の
ように摩擦トルクもなく、消耗部品もないので大
変便利である。 In general, a toroidal coil type rotating electrical machine has an armature on a ring core with four toroidal coils divided at approximately 90° intervals in the case of a four-pole configuration, and a certain gap for each coil. and a field having magnetic poles separated from each other, and the field is configured to generate a magnetic flux from the magnetic pole to the annular core of the armature in the radial direction by means of a permanent magnet contained therein. In this four-pole example,
The magnetic poles of the field are alternately different in the order of N pole, S pole, N pole, and S pole. The four coils of the corresponding armature are also wound in such a way that the winding directions are alternately reversed. Assuming that this armature coil is also connected to the series, when a certain amount of current is passed through this coil, a torque is generated between the field and the armature, and this torque is proportional to the amount of current. It is proportional, and the direction of the torque is determined by the direction of the current. Let us now consider a case where the armature is on the outside and the field is on the inside, and the armature is used as a stator and the field is used as a rotor. Such a toroidal coil type rotating electric machine is usually used when the rotation range of the rotor is limited to a certain angle, for example, within a range of plus or minus 20 degrees around a reference position.
Examples of applications include control of hydraulic rotary valves, and servo motors in limited range rotation servo systems. For such applications, toroidal coil type rotating electric machines are very convenient because they do not have any commutators or slip rings, and although they are DC machines, they do not have frictional torque or consumable parts like AC induction machines.
一方、この種のトロイダルコイル型回転電機は
界磁と電機子との相対位置関係によつて、同じ電
流によつて生ずるトルクの大きさが変化する性質
をもつている。第1図は、この性質を一般的に説
明した図であり、各トロイダルコイルの中央に界
磁の各磁極の中央が来ているときを角度の基準位
置にとり、横軸に界磁と電機子との相対回転角θ
をとり、縦軸に電流をある一定値にしたときのト
ルクをとつてある。回転角θが零のとき、即ち、
上述した基準位置のとき発生するトルクは最大値
τmとなつているが、θが左右どちらかに行くに
従つてトルクは低くなり、極数をPとすると、θ
がπ/Pラジアンのところで、トルクは零とな
る。上述の例ではPが4であるからθが45゜のと
ころで、トルクが零となる。通常この種のトロイ
ダルコイル型回転電機においては使用する角度の
範囲、たとえばプラス・マイナス20゜のところで、
トルクが最大値τmの何割迄下つてよいかを仕様
上で定め、これにあわせて設計される。第1図で
は、一般的にこの点をθがθfのときトルクがτfで
あるとしてトルクの減衰の限界を定めている。 On the other hand, this type of toroidal coil type rotating electrical machine has the property that the magnitude of torque generated by the same current changes depending on the relative positional relationship between the field and the armature. Figure 1 is a diagram that generally explains this property. The angle reference position is when the center of each magnetic pole of the field is at the center of each toroidal coil, and the horizontal axis shows the field and armature. Relative rotation angle θ
The vertical axis shows the torque when the current is set to a certain value. When the rotation angle θ is zero, that is,
The torque generated at the reference position mentioned above is the maximum value τm, but as θ moves to the left or right, the torque decreases, and if the number of poles is P, then θ
The torque becomes zero when is π/P radian. In the above example, since P is 4, the torque becomes zero when θ is 45°. Normally, in this type of toroidal coil type rotating electric machine, within the range of angles used, for example, plus or minus 20 degrees,
The specifications specify how much of the maximum value τm the torque can fall to, and the design is made accordingly. In FIG. 1, the limit of torque attenuation is generally determined at this point by assuming that when θ is θf, the torque is τf.
以上のべたのは4極のトロイダルコイル型回転
電機がトルクモータの例であるが、極数は2極か
ら相当な数の多極に渉るものまで使用されている
し、界磁が固定子で電機子が回転子の場合もあ
る。 The above is an example of a 4-pole toroidal coil type rotating electric machine, but the number of poles ranges from 2 to a considerable number of poles, and the field is connected to the stator. In some cases, the armature is a rotor.
また、トロイダルコイル型回転電機は、トルク
モータでなく、タコメータとして用いられる場合
もあり、この場合電機子には外部から電流を流し
たりせず、電機子に対する界磁の相対角速度に比
例する電圧が、トロイダルコイルから発電される
性質を利用する。この場合第1図の縦軸としてト
ルクでなく、一定角速度に対する発電電圧をとる
ならば、トルクで説明したのと全く同じ形の曲線
を示すことになる。この場合には、仕様としてθf
のところでのある角速度に対する発電電圧が規定
されることになる。 In addition, toroidal coil type rotating electric machines are sometimes used as tachometers instead of torque motors, and in this case, no current is applied to the armature from the outside, and a voltage proportional to the relative angular velocity of the field with respect to the armature is applied. , utilizes the property of generating electricity from a toroidal coil. In this case, if we take the generated voltage for a constant angular velocity instead of the torque as the vertical axis in FIG. 1, we will see a curve that is exactly the same as that described for the torque. In this case, the specification is θf
The generated voltage for a certain angular velocity is defined at .
一般に、この種のトロイダルコイル型回転電機
においては、各トロイダルコイルの間にはある角
度範囲だけコイルのないスペースをおく必要があ
る。従来は、上記コイル間のスペースtsを得るた
めに、環状鉄心に正確にマーキング等を施し、こ
れを目印に各トロイダルコイルを巻回し、所定の
スペースを設けていた。しかし、このような従来
の方法では各コイルを多層巻きにした場合、巻線
が崩れるとか、ずれるとかして所定のスペースts
が得られないという問題を生ずる欠点がある。こ
のスペースの所定巾tsが変化することは、第1図
の曲線に重大な影響を与える。即ち、例えば角θf
のとき、所望とする下限のトルクτfを正しく得ら
れないというこの種のトロイダルコイル型回転電
機としては重大な欠点があつた。 Generally, in this type of toroidal coil rotating electric machine, it is necessary to leave a space between each toroidal coil without a coil within a certain angular range. Conventionally, in order to obtain the above-mentioned space t s between the coils, markings etc. were accurately applied to the annular core, and each toroidal coil was wound using the markings as a guide to provide a predetermined space. However, with this conventional method, when each coil is wound in multiple layers, the windings may collapse or shift, resulting in a space t s
There is a drawback that causes the problem that it is not possible to obtain. Varying the predetermined width t s of this space has a significant effect on the curve of FIG. That is, for example, the angle θf
At this time, this type of toroidal coil rotating electric machine had a serious drawback in that it was not possible to correctly obtain the desired lower limit torque τf.
従つて、本発明の主目的は、上述の如き従来の
欠点を除去したトロイダルコイル型回転電機を提
供するにある。 Therefore, the main object of the present invention is to provide a toroidal coil type rotating electrical machine that eliminates the above-mentioned conventional drawbacks.
本発明の要旨は、リング状コア上に等間隔に分
割された複数個のトロイダルコイルを有する電機
子と、複数個のトロイダルコイルと同数の磁極を
有する界磁とより成るトロイダルコイル型回転電
機に於て、複数個のトロイダルコイルの隣接する
各間隙に対応し且つ界磁とは反対側のリング状コ
アの面に、リング状コアの中心軸の方向の少なく
とも全長に亘る長さの突条部を夫々形成すると共
に、突条部に対応し且つ界磁に対向するリング状
コアの面に、リング状コアの中心軸の方向の少な
くとも全長に亘る長さで、界磁に向かう方向に突
出した非磁性より成るスペーサを夫々固定したこ
とを特徴とするトロイダルコイル型回転電機にあ
る。 The gist of the present invention is to provide a toroidal coil type rotating electrical machine comprising an armature having a plurality of toroidal coils divided at equal intervals on a ring-shaped core, and a field having the same number of magnetic poles as the plurality of toroidal coils. A protrusion portion having a length extending at least the entire length in the direction of the central axis of the ring-shaped core is provided on the surface of the ring-shaped core opposite to the field and corresponding to each of the adjacent gaps between the plurality of toroidal coils. At the same time, on the surface of the ring-shaped core that corresponds to the protrusion and faces the field, it protrudes in the direction toward the field by at least the entire length in the direction of the central axis of the ring-shaped core. A toroidal coil type rotating electrical machine is characterized in that spacers made of non-magnetic material are fixed to each other.
以下、上述した特徴を有する本発明によるトロ
イダルコイル型回転電機の一例を、第2及び第3
図を参照して説明しよう。 Hereinafter, an example of the toroidal coil type rotating electrical machine according to the present invention having the above-mentioned characteristics will be explained as follows.
Let me explain with reference to the diagram.
第2図は本発明によるトロイダルコイル型回転
電機の一例の分解斜視図であり、第3図はその組
立た状態に於ける回転軸Oに垂直な面に沿つた断
面図である。図に於て、1はトロイダルコイル型
回転電機の界磁を全体として示し、2はその電機
子を全体として示す。尚、第2及び第3図に示す
本発明の例は、4極の場合であり、界磁1が電機
子2の内側に配置される場合である。従つて、こ
の場合界磁1は4極の突型界磁である。 FIG. 2 is an exploded perspective view of an example of a toroidal coil type rotating electric machine according to the present invention, and FIG. 3 is a sectional view taken along a plane perpendicular to the rotation axis O in the assembled state. In the figure, 1 shows the field of the toroidal coil type rotating electric machine as a whole, and 2 shows the armature as a whole. The example of the present invention shown in FIGS. 2 and 3 is a case of four poles, and the field 1 is arranged inside the armature 2. Therefore, in this case, the field 1 is a four-pole protruding field.
扨て、同図に示す如く、界磁1は磁性材より成
るリング状のヨーク11と、等角間隔(この場合
90゜)で、隣接するもの同志間に所定の空隙をあ
けて、リング状のヨーク11の外周面に固定され
た4個のマグネツト12,13,14及び15と
より成る。周知の如く、各マグネツトは略々同形
でその厚さ方向、即ちリング状のヨーク11の直
径方向に沿つて着磁されている。例えば、マグネ
ツト12の表面がS極にその内面(ヨーク11に
固定されている面)がN極に着磁されている場合
は、ヨーク11に対して反対側のマグネツト14
は同一極性に着磁されているが、両者間のマグネ
ツト13及び15は、夫々逆極性に着磁されてい
る。換言すれば、各マグネツト12乃至15は順
次逆極性に着磁されている。 As shown in the figure, the field 1 is connected to a ring-shaped yoke 11 made of magnetic material at equiangular intervals (in this case
It consists of four magnets 12, 13, 14 and 15 fixed to the outer circumferential surface of a ring-shaped yoke 11 with a predetermined gap between adjacent ones at an angle of 90 degrees. As is well known, each magnet has substantially the same shape and is magnetized along its thickness direction, that is, along the diameter direction of the ring-shaped yoke 11. For example, if the surface of the magnet 12 is magnetized to the south pole and the inner surface (the surface fixed to the yoke 11) is magnetized to the north pole, the magnet 14 on the opposite side to the yoke 11
are magnetized to the same polarity, but the magnets 13 and 15 between them are respectively magnetized to opposite polarities. In other words, each magnet 12 to 15 is sequentially magnetized with opposite polarity.
一方、電機子2は磁性材、例えば鉄より成るリ
ング状コア21と、このコア21に巻装された4
個のトロイダルコイル22,23,24及び25
と、隣接するトロイダルコイル22乃至25間に
位置する如く、夫々リング状コア21の外周面に
形成された突条部30,31,32及び33と、
これら突条部30,31,32及び33に夫々対
応する如く、夫々リング状コア21の内周面に固
定された非磁性材より成り所定巾tsのスペーサ2
6,27,28及び29とより成る。各トロイダ
ルコイル22………25のリング状コア21の円
周方向の長さは等しく、それ等の巻回方向は順次
逆となつている。 On the other hand, the armature 2 includes a ring-shaped core 21 made of a magnetic material such as iron, and a ring-shaped core 21 made of a magnetic material such as iron, and a
toroidal coils 22, 23, 24 and 25
and protrusions 30, 31, 32 and 33 formed on the outer peripheral surface of the ring-shaped core 21, respectively, so as to be located between the adjacent toroidal coils 22 to 25;
Spacers 2 made of a non-magnetic material and having a predetermined width ts are fixed to the inner circumferential surface of the ring-shaped core 21 so as to correspond to the protrusions 30, 31, 32 and 33, respectively.
6, 27, 28 and 29. The ring-shaped core 21 of each toroidal coil 22...25 has the same length in the circumferential direction, and the winding directions thereof are sequentially reversed.
扨て、本発明の主たる要素である突条部30〜
33及びスペーサ26〜29に就き説明する。図
示の如く、各突条部30,31,32及び33
は、略同一形状で、リング状コア21の外周面の
中心軸Oの方向の少なくとも全長に亘る長さで、
リング状コア21の外周面より界磁1とは反対に
向かう方向、即ち、中心軸Oとは反対に向かう方
向に突出している長さは、リング状コア21に巻
回されるトロイダルコイルの導線の径、コイルの
層数等を考慮して適切に選択される。 In other words, the protruding portion 30 which is the main element of the present invention
33 and spacers 26 to 29 will be explained. As shown in the figure, each protrusion 30, 31, 32 and 33
have substantially the same shape and have a length spanning at least the entire length in the direction of the central axis O of the outer peripheral surface of the ring-shaped core 21,
The length protruding from the outer peripheral surface of the ring-shaped core 21 in the direction opposite to the field 1, that is, in the direction opposite to the central axis O, is the conductor of the toroidal coil wound around the ring-shaped core 21. The diameter of the coil, the number of coil layers, etc. are selected appropriately.
又、図示の如く、各スペーサ26………29は
略略同一形状で、リング状コア21の内周面の中
心軸Oの方向の少くとも全長に亘る長さで、内周
面の円方向の巾は所定の巾tsで、リング状コア2
1の内周面より界磁1に向かう方向、即ち、中心
軸Oに向かう方向に突出している長さlは、リン
グ状コア21に巻回されるトロイダルコイルの導
線の径、コイルの層数等を考慮して適切に選択さ
れる。従つて、各トロイダルコイル22………2
5をリング状コア21に各突条部30,31,3
2及び33並びに各スペーサ26………29が従
来のマーキング(各コイルの位置決め)の役目を
果す外に、巻装された各コイルが崩れたり、ずれ
たりするのを確実に阻止し得るものであるから、
各コイルを均一に巻装し得ると共に、それ等の長
さも所定になし得る。更に、コイル間の間隔、即
ちスペーサを所定巾tsに確実に保持し得るもので
ある。 Further, as shown in the figure, each spacer 26...29 has substantially the same shape, has a length spanning at least the entire length of the inner peripheral surface of the ring-shaped core 21 in the direction of the central axis O, and has a length extending in the direction of the circular direction of the inner peripheral surface. The width is a predetermined width ts , and the ring-shaped core 2
The length l that protrudes from the inner peripheral surface of the toroidal coil in the direction toward the field 1, that is, in the direction toward the central axis O, is the diameter of the conducting wire of the toroidal coil wound around the ring-shaped core 21, and the number of layers of the coil. Appropriate selection will be made taking into account the following. Therefore, each toroidal coil 22...2
5 to the ring-shaped core 21 and each protrusion 30, 31, 3
2 and 33 and each spacer 26...29 not only serve as a conventional marking (positioning each coil), but also can reliably prevent each wound coil from collapsing or shifting. because there is,
Each coil can be wound uniformly, and its length can also be set to a predetermined value. Furthermore, the distance between the coils, that is, the spacer, can be reliably maintained at a predetermined width ts .
従つて、トロイダルコイル型回転電機の下限ト
ルクを意図した値に確実になし得、これを量産し
た場合も、特性のバラツキを極小に抑えることが
できる。 Therefore, the lower limit torque of the toroidal coil type rotating electrical machine can be reliably set to the intended value, and even when the machine is mass-produced, variations in characteristics can be kept to a minimum.
上述は、4極のトロイダルコイル型回転電機を
説明したが、本発明はこの例に限らず、2極或は
6極以上の偶数極のトロイダルコイル型回転電機
に適用できることは勿論、界磁としては上述の突
極型に限らず、例えば円筒型等でもよい。 Although the above description describes a four-pole toroidal coil type rotating electric machine, the present invention is not limited to this example, and can of course be applied to a toroidal coil type rotating electric machine with two poles or an even number of poles of six or more poles. is not limited to the above-mentioned salient pole type, but may be of a cylindrical type, for example.
又、本発明は界磁が電機子の外側に配される型
のものに適用しても、同一の効果が得られるもの
である。 Further, even if the present invention is applied to a type in which the field is disposed outside the armature, the same effect can be obtained.
その他、本発明の要旨を逸脱せずに多くの変
化、変更がなし得ることは当該業者に明らかであ
ろう。 It will be apparent to those skilled in the art that many other changes and modifications can be made without departing from the spirit of the invention.
第1図はトロイダルコイル型回転電機のトルク
分布図、第2図は本発明のトロイダルコイル型回
転電機の一例の分解斜視図、第3図はその組立状
態を示す断面図である。
図に於て、1は界磁、2は電機子、11はヨー
ク、12………15はマグネツト、21はリング
状コア、22………25はトロイダルコイル、2
6………29はスペーサを夫々示す。
FIG. 1 is a torque distribution diagram of a toroidal coil type rotating electric machine, FIG. 2 is an exploded perspective view of an example of the toroidal coil type rotating electric machine of the present invention, and FIG. 3 is a sectional view showing its assembled state. In the figure, 1 is a field, 2 is an armature, 11 is a yoke, 12...15 is a magnet, 21 is a ring-shaped core, 22...25 is a toroidal coil, 2
6...29 indicate spacers, respectively.
Claims (1)
のトロイダルコイルを有する電機子と、上記複数
個のトロイダルコイルと同数の磁極を有する界磁
とより成るトロイダルコイル型回転電機に於て、
上記複数個のトロイダルコイルの隣接する各間隙
に対応し且つ上記界磁とは反対側の上記リング状
コアの面に、該リング状コアの中心軸の方向の少
なくとも全長に亘る長さの突条部を夫々形成する
と共に、該突条部に対応し且つ上記界磁に対向す
る上記リング状コアの面に、該リング状コアの中
心軸の方向の少なくとも全長に亘る長さで、上記
界磁に向かう方向に突出した非磁性より成るスペ
ーサを夫々固定したことを特徴とするトロイダル
コイル型回転電機。1. In a toroidal coil type rotating electric machine, which is composed of an armature having a plurality of toroidal coils divided at equal intervals on a ring-shaped core, and a field having the same number of magnetic poles as the plurality of toroidal coils,
A protrusion having a length extending at least over the entire length in the direction of the central axis of the ring-shaped core is provided on a surface of the ring-shaped core opposite to the field and corresponding to each of the adjacent gaps of the plurality of toroidal coils. and at least the entire length of the ring-shaped core in the direction of the central axis of the ring-shaped core, on the surface of the ring-shaped core that corresponds to the protrusion and faces the field. A toroidal coil type rotating electrical machine characterized by fixing spacers made of non-magnetic material that protrude in the direction of .
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP16630883A JPS6059954A (en) | 1983-09-09 | 1983-09-09 | Toroidal coil type rotary electric machine |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP16630883A JPS6059954A (en) | 1983-09-09 | 1983-09-09 | Toroidal coil type rotary electric machine |
Publications (2)
| Publication Number | Publication Date |
|---|---|
| JPS6059954A JPS6059954A (en) | 1985-04-06 |
| JPH0150182B2 true JPH0150182B2 (en) | 1989-10-27 |
Family
ID=15828929
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP16630883A Granted JPS6059954A (en) | 1983-09-09 | 1983-09-09 | Toroidal coil type rotary electric machine |
Country Status (1)
| Country | Link |
|---|---|
| JP (1) | JPS6059954A (en) |
Families Citing this family (5)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| DE3532101A1 (en) * | 1985-09-09 | 1987-03-19 | Huebner Elektromasch Ag | BRUSHLESS INDUCTION MACHINE |
| US5798591A (en) * | 1993-07-19 | 1998-08-25 | T-Flux Pty Limited | Electromagnetic machine with permanent magnet rotor |
| JP3579272B2 (en) * | 1998-12-10 | 2004-10-20 | ミネベア株式会社 | Toroidal core type actuator |
| JP3445173B2 (en) * | 1998-12-11 | 2003-09-08 | ミネベア株式会社 | Actuator device with valve |
| JP2016226104A (en) * | 2015-05-28 | 2016-12-28 | 株式会社インターナショナル電子 | Generator |
Family Cites Families (1)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| JPS51118007U (en) * | 1975-03-19 | 1976-09-25 |
-
1983
- 1983-09-09 JP JP16630883A patent/JPS6059954A/en active Granted
Also Published As
| Publication number | Publication date |
|---|---|
| JPS6059954A (en) | 1985-04-06 |
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