JPH0441753Y2 - - Google Patents

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Publication number
JPH0441753Y2
JPH0441753Y2 JP1987047333U JP4733387U JPH0441753Y2 JP H0441753 Y2 JPH0441753 Y2 JP H0441753Y2 JP 1987047333 U JP1987047333 U JP 1987047333U JP 4733387 U JP4733387 U JP 4733387U JP H0441753 Y2 JPH0441753 Y2 JP H0441753Y2
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JP
Japan
Prior art keywords
rotor
stator
output shaft
rotors
length
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
Application number
JP1987047333U
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Japanese (ja)
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JPS63156573U (en
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Priority to JP1987047333U priority Critical patent/JPH0441753Y2/ja
Publication of JPS63156573U publication Critical patent/JPS63156573U/ja
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Expired legal-status Critical Current

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Description

【考案の詳細な説明】 [産業上の利用分野] この考案は、例えば、工業用ロボツトのアーム
駆動等に用いて好適な可変空隙型モータに係り、
特に、振動および騒音の低減を図るとともに、電
力効率の改善を図つた可変空隙型モータに関す
る。
[Detailed description of the invention] [Industrial application field] This invention relates to a variable gap type motor suitable for use, for example, in driving the arm of an industrial robot.
In particular, the present invention relates to a variable gap type motor that reduces vibration and noise and improves power efficiency.

[従来技術] 従来、一般のモータとはその動作原理が全く異
なるものとして、第3図イ〜ニに示すような可変
空隙型モータが知られている。これらの図におい
て、1は固定子であり、内周に8個の極歯(図示
略)が形成された円筒状のコア1aと、各極歯に
各々巻回されたコイル(図示略)とから構成され
ている。これにより、第3図ハに示すように固定
子1の内周面に沿つて8個の磁極a〜hが設けら
れている。そして、固定子1の各コイルに順次励
磁電流を供給することにより、磁極a〜hが順次
励磁されるようになつている。上記固定子1は第
3図ニに示すようにフレーム2内に収納されてお
り、また、このフレーム2に、固定子1の中心軸
C上に配置された2本の出力軸3,3が軸受4,
4を介して各々回転自在に支持されている。2本
の出力軸3,3の内側の各端部にはクランク板
5,5の各一端部が固定され、これらクランク板
5,5の各他端部には回転子6の支持軸7の両端
が各々固定されている。この場合、出力軸3と支
持軸7との各軸線間の距離l(第3図イ)はコア
1aの内周の半径nから回転子6の半径Rを差し
引いた長さより若干小となつている。また、上記
回転子6は、円筒状の磁性体によつて構成され、
第3図ロに示すように軸受8,8を介して支持軸
7に自転自在に支持されている。
[Prior Art] Conventionally, variable gap type motors as shown in FIGS. 3A to 3D have been known as motors whose operating principle is completely different from that of general motors. In these figures, 1 is a stator, which includes a cylindrical core 1a with eight pole teeth (not shown) formed on its inner periphery, and a coil (not shown) wound around each pole tooth. It consists of As a result, eight magnetic poles a to h are provided along the inner peripheral surface of the stator 1, as shown in FIG. 3C. By sequentially supplying an excitation current to each coil of the stator 1, the magnetic poles a to h are sequentially excited. The stator 1 is housed in a frame 2 as shown in FIG. bearing 4,
4, each is rotatably supported. One end of a crank plate 5, 5 is fixed to each inner end of the two output shafts 3, 3, and a support shaft 7 of a rotor 6 is fixed to the other end of each crank plate 5, 5. Both ends are fixed. In this case, the distance l between each axis of the output shaft 3 and the support shaft 7 (Fig. 3 A) is slightly smaller than the length obtained by subtracting the radius R of the rotor 6 from the radius n of the inner circumference of the core 1a. There is. Further, the rotor 6 is made of a cylindrical magnetic material,
As shown in FIG. 3B, it is rotatably supported by a support shaft 7 via bearings 8, 8.

以上の構成により、第3図ハに示すように回転
子6が出力軸3の軸線を中心に公転しつつ、支持
軸7を中心に自転自在となつている。この結果、
常に回転子6の外周の一部が固定子1の内周に近
接している状態で公転可能となつている。例え
ば、回転子6が第3図ハに示すように位置してい
る状態において、磁極bを励磁すると、この磁極
bと回転子6との間に磁気吸引力が発生する。こ
れにより、回転子6が磁極bとのギヤツプGをせ
ばめる方向、すなわち、矢印F方向へ吸引され
る。この結果、回転子6が出力軸3の軸線を中心
に矢印A1方向に公転を始め、この公転運動にと
もなつて、支持軸7を中心に矢印B方向に自転を
開始する。以降、磁極c、磁極d、磁極eを順次
励磁すると、回転子6が磁極c,d,e……に
次々と吸引され、これにより、回転子6が矢印A
方向に連続的に公転を続け、この公転運動が、出
力軸3によつて外部へ出力される。
With the above configuration, the rotor 6 is able to rotate around the support shaft 7 while revolving around the axis of the output shaft 3, as shown in FIG. 3C. As a result,
The rotor 6 can revolve with a part of its outer periphery always being close to the inner periphery of the stator 1. For example, when the rotor 6 is positioned as shown in FIG. 3C, when the magnetic pole b is excited, a magnetic attraction force is generated between the magnetic pole b and the rotor 6. As a result, the rotor 6 is attracted in the direction of narrowing the gap G with the magnetic pole b, that is, in the direction of the arrow F. As a result, the rotor 6 starts to revolve around the axis of the output shaft 3 in the direction of arrow A1 , and along with this revolution, starts to rotate around the support shaft 7 in the direction of arrow B. Thereafter, when the magnetic poles c, d, and e are sequentially excited, the rotor 6 is attracted to the magnetic poles c, d, e, etc. one after another, and the rotor 6 moves in the direction indicated by the arrow A.
It continues to revolve continuously in the direction, and this revolution movement is outputted to the outside by the output shaft 3.

上述した可変空隙型モータは磁極a,b,c…
…と回転子6との空隙が変化する構造になつてお
り、磁気吸引力(可変空隙力)を回転子6に直接
作用させて、回転子6を公転させ、この公転力に
よつて回転出力を得ている。一方、回転子と固定
子との空隙が常に一定である。一般のモータ、い
わゆる固定空隙型モータは、上述した磁気吸引力
を利用することなく、磁極から発生する界磁磁束
と直交する接線力(固定空隙力)のみを利用して
いる。ここで、一般的に可変空隙力は固定空隙力
に比較して極めて大であることが知られており、
これにより、可変空隙型モータは、固定空隙型モ
ータと比較して大きいトルクが得られ、したがつ
て、工業用ロボツトのアーム駆動のように、高ト
ルクが必要とされる駆動源としての利用が考えら
れる。
The variable air gap type motor described above has magnetic poles a, b, c...
It has a structure in which the air gap between ... and the rotor 6 changes, and a magnetic attraction force (variable air gap force) is applied directly to the rotor 6 to cause the rotor 6 to revolve, and this revolving force produces a rotational output. I am getting . On the other hand, the gap between the rotor and stator is always constant. A general motor, a so-called fixed air gap type motor, does not utilize the above-mentioned magnetic attraction force, but only uses a tangential force (fixed air gap force) orthogonal to the field magnetic flux generated from the magnetic poles. Here, it is generally known that the variable pore force is extremely large compared to the fixed pore force.
As a result, variable gap type motors can obtain larger torque than fixed gap type motors, and therefore can be used as drive sources that require high torque, such as arm drives of industrial robots. Conceivable.

[考案が解決しようとする問題点] ところで、上述した従来の可変空隙型モータに
おいては、回転子6の重心が出力軸3の軸線から
距離lだけ隔たつた支持軸7上にあるので、重心
が偏心した回転、すなわち偏心荷重回転となつて
いる。この結果、回転子6の公転にともなつて、
回転系全体に振動が生じ、また、この振動にとも
なつて騒音が生じるという問題があつた。
[Problems to be solved by the invention] By the way, in the conventional variable gap type motor described above, the center of gravity of the rotor 6 is located on the support shaft 7 which is separated by a distance l from the axis of the output shaft 3. is an eccentric rotation, that is, an eccentric load rotation. As a result, as the rotor 6 revolves,
There was a problem in that vibrations occurred throughout the rotating system, and noise was generated along with this vibration.

また、上述した従来の可変空隙型モータにおい
ては、回転子6は第3図ロに示すように、円筒状
に形成され、その両端部に軸受8,8が嵌入され
ているので、回転子6の内周面と支持軸7の外周
面との間には、軸受8,8の外周と内周との差に
略相当する空間Sが形成されている。このため、
回転子6の公転の際に、磁極から回転子6に流入
した磁束は空間Sより磁気抵抗の小さい軸受8,
8を通り、支持軸7へ導かれる、しかしながら、
この軸受8,8は材質、構造上の点から回転子6
と比較して磁気抵抗が大きい。この結果、励磁電
流を大としないと十分な磁気吸引力が得られず、
したがつて電力効率が低くなる。このため、本考
案者は第4図に示すように回転子6の内周面に環
状の凸部6aを設け支持軸7に近接させる構造の
可変空隙型モータを考えたが、このように構成す
ると磁極から回転子6に流入した磁束φは凸部6
aに集中し、支持軸7に導かれる。この結果、凸
部6aにおいて、磁束φの密度が高くなり、磁気
抵抗が増加する。したがつて、上記と同様に電力
効率の低下の原因となる。
Further, in the conventional variable gap type motor described above, the rotor 6 is formed in a cylindrical shape as shown in FIG. A space S is formed between the inner circumferential surface of the support shaft 7 and the outer circumferential surface of the support shaft 7, which substantially corresponds to the difference between the outer circumference and the inner circumference of the bearings 8, 8. For this reason,
When the rotor 6 revolves, the magnetic flux flowing into the rotor 6 from the magnetic poles flows through the bearings 8, which have lower magnetic resistance than the space S.
8 and is guided to the support shaft 7, however,
These bearings 8, 8 are used for the rotor 6 in terms of material and structure.
Magnetic resistance is large compared to As a result, sufficient magnetic attraction force cannot be obtained unless the excitation current is increased.
Therefore, power efficiency becomes low. For this reason, the present inventor considered a variable gap type motor having a structure in which an annular convex portion 6a is provided on the inner circumferential surface of the rotor 6 and brought close to the support shaft 7, as shown in FIG. Then, the magnetic flux φ flowing into the rotor 6 from the magnetic poles flows into the convex portion 6
a and is guided to the support shaft 7. As a result, the density of the magnetic flux φ increases in the convex portion 6a, and the magnetic resistance increases. Therefore, similar to the above, this causes a decrease in power efficiency.

この考案は、上記の事情に鑑みてなされたもの
で、その目的とするところは、振動および騒音の
低減を図るとともに、電力効率の改善をさらに図
つた可変空隙型モータを提供することにある。
This invention was made in view of the above circumstances, and its purpose is to provide a variable air gap motor that reduces vibration and noise and further improves power efficiency.

[問題点を解決するための手段] この考案は、内周面に沿つて回転磁界を発生す
る円筒状の固定子と、前記固定子の中心軸上に貫
通して配置され、かつ回転自在に支持された出力
軸と、前記出力軸と平行に、かつ前記出力軸を中
心とする仮想円周上に等間隔を隔てて配置され、
前記固定子の内周面と近接した状態で公転する複
数個の略円筒状の回転子と、前記各回転子を軸受
を介して各々自転自在に支持する支持軸と、前記
各支持軸が各々取り付けられ、前記各回転子の公
転を前記出力軸に伝達する公転板とを具備する可
変空隙型モータであつて、前記回転子の軸方向長
を前記固定子の軸方向長よりも前記軸受の長さに
相当する分だけ長く形成し、前記回転子の内周面
または前記各支持軸の外周面のいずれか一方もし
くは両方に、前記回転子と前記支持軸との間の隙
間が小となるように環状の凸部を形成し、該凸部
の軸方向の長さを前記固定子と同一長に形成した
ことを特徴としている。
[Means for Solving the Problems] This invention consists of a cylindrical stator that generates a rotating magnetic field along its inner circumferential surface, and a stator that is disposed penetratingly on the central axis of the stator and is rotatable. a supported output shaft, and arranged parallel to the output shaft and at equal intervals on a virtual circumference centered on the output shaft,
a plurality of substantially cylindrical rotors that revolve in close proximity to the inner circumferential surface of the stator; support shafts that rotatably support each of the rotors via bearings; and each of the support shafts and a revolution plate that is attached to the shaft and transmits the revolution of each of the rotors to the output shaft, the axial length of the rotor being longer than the axial length of the stator. The gap between the rotor and the support shafts is reduced on either or both of the inner peripheral surface of the rotor or the outer peripheral surface of each of the support shafts. The present invention is characterized in that an annular convex portion is formed, and the length of the convex portion in the axial direction is the same as that of the stator.

[作用] この考案によれば、複数個の回転子が出力軸と
平行に、かつ出力軸を中心とする仮想円周上に等
間隔を隔てて配置されているので、回転系全体の
重心と出力軸の軸線とが一致する。したがつて、
各回転子の公転に伴う振動およびこの振動に伴う
騒音が低減される。
[Operation] According to this invention, since the plurality of rotors are arranged parallel to the output shaft and at equal intervals on the virtual circumference centered on the output shaft, the center of gravity of the entire rotating system and The axis line of the output shaft matches. Therefore,
Vibration accompanying the revolution of each rotor and noise accompanying this vibration are reduced.

また、凸部の軸方向の長さすなわち回転子から
支持軸に導かれる磁束の通路が固定子の軸方向の
長さと等しい長さであり、かつ凸部により回転子
と支持軸との間の隙間が小となつているので、回
転磁界により固定子から回転子に流入した磁束
は、均一な密度で回転子を通過し、かつ回転子か
らわずかな隙間を介して支持軸に導かれる。した
がつて、磁気抵抗が小となる。
In addition, the axial length of the convex portion, that is, the path of the magnetic flux guided from the rotor to the support shaft, is equal to the axial length of the stator, and the convex portion allows the path between the rotor and the support shaft to Since the gap is small, the magnetic flux flowing from the stator to the rotor due to the rotating magnetic field passes through the rotor with uniform density and is guided from the rotor to the support shaft through a small gap. Therefore, magnetic resistance becomes small.

[実施例] 以下、この考案の一実施例について、図面を参
照して説明する。第1図イ、ロおよびハにおい
て、20は固定子であり、内周に12個の極歯(図
示略)が等間隔をおいて形成された円筒状のコア
20aと、各極歯に各々巻回されたコイル(図示
略)とから構成されている。これにより、固定子
1の内周面に沿つて、磁極a1〜a4,b1〜b4,c1
c4が設けられている。この固定子1の中心軸C上
には出力軸21が貫通して配置されており、この
出力軸21は軸受(図示略)を介してフレーム
(図示略)に回転自在に支持されている。また、
この出力軸21には十字状に形成された公転板2
2,22の中央部が各々固定されている。これら
公転板22,22には、その中心から四方へ距離
mだけ隔てた位置に、出力軸21と平行に配置さ
れた支持軸23a〜23dの両端が各々固定され
ている。これら支持軸23a〜23dには各軸受
24a〜24dを介して回転子25a〜25dが
各々自転自在に支持されている。これら回転子2
5a〜25dは、略円筒状の磁性体によつて各々
構成され、その全長L2は第1図ロに示すように
固定子1の軸方向長Lより軸受23a〜23d、
23aの長さL1に相当する分だけ各々両側に長
く形成され、その内周面には、軸方向長が固定子
1と同一長Lであり、かつ各支持軸23a〜23
dの外周面との間の隙間が約1/100mmとなるよ
うに、環状の凸部30が各々形成されている。ま
た、回転子25a〜25dの半径rは、第1図イ
に示すように固定子20の内周の半径nから出力
軸21と支持軸23a〜23dの各軸線間の距離
mを差し引いた長さより若干小となつている。こ
のような構成により、回転子25a〜25dは、
出力軸21を中心とする仮想円周上に等間隔(中
心角にして90度)を隔てて配置され、また出力軸
21に関して、回転子25aと回転子25cが対
称に、回転子25bと回転子25dが対称に位置
している。そして、これら回転子25a〜25d
の外周の一部が常に固定子20の内周面に近接し
た状態で出力軸26の軸線を中心に公転しつつ、
各々支持軸23a〜23dを中心に自転自在とな
つている。
[Example] Hereinafter, an example of this invention will be described with reference to the drawings. In FIGS. 1A, 1B, and 1C, 20 is a stator, which includes a cylindrical core 20a on the inner periphery of which 12 pole teeth (not shown) are formed at equal intervals, and a stator for each pole tooth. It is composed of a wound coil (not shown). As a result, magnetic poles a 1 to a 4 , b 1 to b 4 , c 1 to
c 4 is provided. An output shaft 21 is disposed to pass through the center axis C of the stator 1, and the output shaft 21 is rotatably supported by a frame (not shown) via a bearing (not shown). Also,
This output shaft 21 has a revolution plate 2 formed in a cross shape.
The central parts of 2 and 22 are each fixed. Both ends of support shafts 23a to 23d, which are arranged parallel to the output shaft 21, are fixed to the revolution plates 22, 22 at positions spaced apart from the center by a distance m in all directions. Rotors 25a to 25d are rotatably supported on these support shafts 23a to 23d via bearings 24a to 24d, respectively. These rotors 2
5a to 25d are each made of a substantially cylindrical magnetic body, and their total length L2 is longer than the axial length L of the stator 1 as shown in FIG.
23a is formed to be long on both sides by an amount corresponding to the length L1 , and on the inner peripheral surface thereof, the axial length is the same length L as the stator 1, and each support shaft 23a to 23
The annular protrusions 30 are each formed such that the gap between the protrusions 30 and the outer peripheral surface of the protrusions d is about 1/100 mm. Furthermore, the radius r of the rotors 25a to 25d is determined by subtracting the distance m between the axes of the output shaft 21 and the support shafts 23a to 23d from the radius n of the inner circumference of the stator 20, as shown in FIG. It is slightly smaller than Sayaka. With such a configuration, the rotors 25a to 25d are
The rotors 25a and 25c are arranged at equal intervals (90 degrees as a center angle) on a virtual circumference centered on the output shaft 21, and the rotors 25a and 25c are symmetrical with respect to the output shaft 21. The children 25d are located symmetrically. And these rotors 25a to 25d
While revolving around the axis of the output shaft 26 with a part of the outer circumference always being close to the inner circumferential surface of the stator 20,
Each of them is rotatable around support shafts 23a to 23d.

以上の構成において、例えば、回転子25a〜
25dが第1図ハに示すように位置している状態
において、まず、磁極a1,a2,a3,a4を励磁する
と、これにより、磁極a1と回転子25aとの間、
磁極a2と回転子25bとの間、磁極a3と回転子2
5cとの間に、磁極a4と回転子25dとの間に
各々磁気吸引力が発生し、回転子25a〜25d
が各々磁極a1〜a4との間のギヤツプをせばめる方
向、すなわち、回転子25aが矢印Fa方向に、
回転子25bが矢印Fb方向に、回転子25cが
矢印Fc方向に、回転子25dが矢印Fd方向に
各々吸引される。これにより、回転子25a〜2
5dが出力軸26の軸線を中心に矢印Q1方向に
公転を始め、この公転運動に伴つて回転子25a
〜25dが支持軸23a〜23dを中心に矢印P
方向に自転を開始する。以降、磁極b1〜b4、次に
磁極c1〜c4、再び、磁極a1〜a4と、各々中心角が
90度ずれた磁極を順次励磁することにより、回転
子25a〜25dが上記と同様に磁極b1〜b4、次
に磁極c1〜c4、再び磁極a1〜a4に各々吸引され
る。これにより、回転子25a〜25dは上記と
同様に矢印Q方向に公転を続け、この公転力が軸
受24a〜24d、支持軸23a〜23d、公転
板22からなる支持機構を介して出力軸21に伝
達され、この結果、出力軸21が回転する。
In the above configuration, for example, the rotors 25a to
25d is positioned as shown in FIG .
Between magnetic pole a 2 and rotor 25b, between magnetic pole a 3 and rotor 2
5c, a magnetic attraction force is generated between the magnetic pole a4 and the rotor 25d, and the rotors 25a to 25d
is the direction in which the gap between the magnetic poles a1 to a4 is narrowed, that is, the rotor 25a is moved in the direction of the arrow Fa,
The rotor 25b is attracted in the direction of arrow Fb, the rotor 25c is attracted in the direction of arrow Fc, and the rotor 25d is attracted in the direction of arrow Fd. As a result, the rotors 25a to 2
5d begins to revolve in the direction of arrow Q1 around the axis of the output shaft 26, and along with this revolution, the rotor 25a
~25d is an arrow P centered around the support shafts 23a~23d
Start rotating in the direction. From then on, magnetic poles b 1 to b 4 , then magnetic poles c 1 to c 4 , and again magnetic poles a 1 to a 4 , each with a central angle
By sequentially exciting the magnetic poles shifted by 90 degrees, the rotors 25a to 25d are attracted to the magnetic poles b 1 to b 4 , then to the magnetic poles c 1 to c 4 , and again to the magnetic poles a 1 to a 4 in the same manner as above. . As a result, the rotors 25a to 25d continue to revolve in the direction of the arrow Q in the same manner as described above, and this revolving force is applied to the output shaft 21 via the support mechanism consisting of the bearings 24a to 24d, the support shafts 23a to 23d, and the revolution plate 22. As a result, the output shaft 21 rotates.

しかして、上記の構成によれば、各回転子25
a〜25dの全長L2を回転子1の軸方向長Lよ
り、軸受23a〜23dの長さL1に相当する長
さL1分だけ各々両側に長く形成し、その内周面
に支持軸24a〜24dと1/100mmの隙間を有
する環状の凸部30を設け、かつ凸部30を固定
子1の軸方向長Lと同一長に形成したので、例え
ば、磁極a1から回転子25aに流入した磁束φは
第2図に示すように、回転子25aの凸部30を
直線的に均一な密度で通過し1/100mmの隙間を
介して支持軸23aに導かれる。これと同様に、
各磁極a2〜a4から各回転子25b〜25dに流入
した磁束φも各回転子25b〜25dの凸部30
を均一な密度で通過し1/100mmの隙間を介して
支持軸23b〜23dに導かれる。これにより、
従来の可変空隙型モータのように、軸受を通るこ
となく、かつ、均一な磁束密度で回転子25a〜
25dを磁束が各々通過するので、従来と比較し
て磁気抵抗が小となる。この結果、コイルの励磁
電流が少なくても十分な磁気吸引力が得られ、し
たがつて、従来より電力効率が向上する。また、
回転子25a〜25dが出力軸21に平行に、か
つ出力軸21を中心とする仮想円周上に等間隔に
配置されているので、回転系全体の重心が出力軸
の軸線と一致し、振動およびこの振動に伴う騒音
が完全に防止される。また、固定子20の中心軸
上に1本の出力軸21を貫通した構造となつてい
るので、従来のように、2本の出力軸3,3(第
3図イ参照)の軸線を合わせる必要がなく、製作
が容易となる。
According to the above configuration, each rotor 25
The total length L 2 of bearings 23 a to 25 d is longer than the axial length L of rotor 1 by a length L 1 corresponding to the length L 1 of bearings 23 a to 23 d on both sides, and a support shaft is attached to the inner circumferential surface of the bearings 23 a to 23 d. Since an annular convex portion 30 having a gap of 1/100 mm from 24a to 24d is provided, and the convex portion 30 is formed to have the same length as the axial length L of the stator 1, for example, from the magnetic pole a 1 to the rotor 25a. As shown in FIG. 2, the inflowing magnetic flux φ passes straight through the convex portion 30 of the rotor 25a with uniform density and is guided to the support shaft 23a through a gap of 1/100 mm. Similarly,
The magnetic flux φ flowing from each magnetic pole a 2 to a 4 to each rotor 25b to 25d also flows into the convex portion 30 of each rotor 25b to 25d.
It passes through with a uniform density and is guided to the support shafts 23b to 23d through a gap of 1/100 mm. This results in
Unlike conventional variable gap type motors, the rotor 25a~ does not pass through bearings and has a uniform magnetic flux density.
Since the magnetic flux passes through each of the sections 25d, the magnetic resistance becomes smaller compared to the conventional case. As a result, sufficient magnetic attraction force can be obtained even if the excitation current of the coil is small, and therefore power efficiency is improved compared to the conventional method. Also,
Since the rotors 25a to 25d are arranged parallel to the output shaft 21 and at equal intervals on a virtual circumference centered on the output shaft 21, the center of gravity of the entire rotating system coincides with the axis of the output shaft, and vibrations are reduced. And the noise associated with this vibration is completely prevented. In addition, since the structure is such that one output shaft 21 passes through the center axis of the stator 20, the axes of the two output shafts 3, 3 (see Fig. 3 A) are aligned, as in the conventional case. It is not necessary and manufacturing is easy.

なお、上記の実施例においては、回転子25a
〜25dの内周面に環状の凸部30を設けたが、
支持軸24a〜24dの外周面に環状の凸部を設
け、もしくは回転子25a〜25dおよび支持軸
24a〜24dの両方に環状の凸部を設け、回転
子25a〜25dと支持軸24a〜24dとを近
接させるような構造としてもよい。また、上述し
た実施例においては、固定子20の極歯に各々コ
イルを巻回して、磁極を構成する場合を例にして
説明したが、誘導電動機のように、コアの内周面
に等間隔に複数のスロツトを形成し、これらスロ
ツトにコイルを連続して巻回し、このコイルに交
流電流を流してコア20aの内周面に沿つて連続
的に回転磁界を発生させ、これにより、回転子を
磁気吸引させるように構成してもよい。
Note that in the above embodiment, the rotor 25a
Although an annular convex portion 30 was provided on the inner peripheral surface of ~25d,
An annular projection is provided on the outer peripheral surface of the support shafts 24a to 24d, or an annular projection is provided to both the rotors 25a to 25d and the support shafts 24a to 24d, so that the rotors 25a to 25d and the support shafts 24a to 24d It is also possible to have a structure in which the two are placed close to each other. In addition, in the above-mentioned embodiment, a case was explained in which a coil is wound around each pole tooth of the stator 20 to form a magnetic pole. A plurality of slots are formed in the core 20a, coils are continuously wound around these slots, and an alternating current is passed through the coil to continuously generate a rotating magnetic field along the inner circumferential surface of the core 20a. It may be configured so that it is magnetically attracted.

[考案の効果] 以上説明したように、この考案によれば、複数
個の回転子が出力軸と平行に、かつ出力軸を中心
とする仮想円周上に等間隔を隔てて配置されてい
るので、回転系全体の重心と出力軸の軸線とが一
致する。したがつて、各回転子の公転に伴う振動
およびこの振動に伴う騒音を低減することができ
る。
[Effects of the invention] As explained above, according to this invention, a plurality of rotors are arranged parallel to the output shaft and at equal intervals on a virtual circumference centered on the output shaft. Therefore, the center of gravity of the entire rotating system and the axis of the output shaft coincide. Therefore, the vibration accompanying the revolution of each rotor and the noise accompanying this vibration can be reduced.

また、凸部の軸方向の長さすなわち回転子から
支持軸に導かれる磁束の通路が固定子の軸方向の
長さと等しい長さであり、かつ凸部により回転子
と支持軸との間の隙間が小となつているので、回
転磁界により固定子から回転子に流入した磁束
は、均一な密度で回転子を通過し、かつ回転子か
らわずかな隙間を介して支持軸に導かれる。しが
たつて、磁気抵抗が小となるため、励磁電流を小
としても十分な磁気吸引力を得ることができ、電
力効率が向上させることができる。
In addition, the axial length of the convex portion, that is, the path of the magnetic flux guided from the rotor to the support shaft, is equal to the axial length of the stator, and the convex portion allows the path between the rotor and the support shaft to Since the gap is small, the magnetic flux flowing from the stator to the rotor due to the rotating magnetic field passes through the rotor with uniform density and is guided from the rotor to the support shaft through a small gap. As a result, the magnetic resistance becomes small, so even if the excitation current is made small, a sufficient magnetic attraction force can be obtained, and power efficiency can be improved.

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

第1図イ、ロおよびハはこの考案の一実施例の
構成を示す分解斜視図、部分断面図および正面
図、第2図は同実施例の回転子25a,25b〜
25dの磁束線図、第3図はイ、ロ、ハおよびニ
は従来の可変空隙型モータの構成を示す分解斜視
図、部分断面図、正面図および側断面図、第4図
は問題点を説明するため磁束線図である。 20……固定子、21……出力軸、22,22
……公転板、23a〜23d……支持軸、24a
〜24d……軸受、25a〜25d……回転子、
30……凸部。
Figures 1A, 2B, and 3 are exploded perspective views, partial sectional views, and front views showing the configuration of an embodiment of this invention, and Figure 2 shows rotors 25a, 25b, and 25b of the same embodiment.
25d is a magnetic flux line diagram, FIG. 3 is an exploded perspective view, partial sectional view, front view, and side sectional view showing the configuration of a conventional variable gap type motor, and FIG. 4 is a diagram showing problems. It is a magnetic flux line diagram for explanation. 20... Stator, 21... Output shaft, 22, 22
...Revolution plate, 23a to 23d...Support shaft, 24a
~24d...bearing, 25a~25d...rotor,
30...Protrusion.

Claims (1)

【実用新案登録請求の範囲】 内周面に沿つて回転磁界を発生する円筒状の固
定子と、前記固定子の中心軸上に貫通して配置さ
れ、かつ回転自在に支持された出力軸と、前記出
力軸と平行に、かつ前記出力軸を中心とする仮想
円周上に等間隔を隔てて配置され、前記固定子の
内周面と近接した状態で公転する複数個の略円筒
状の回転子と、前記各回転子を軸受を介して各々
自転自在に支持する支持軸と、前記各支持軸が
各々取り付けられ、前記各回転子の公転を前記出
力軸に伝達する公転板とを具備する可変空隙型モ
ータであつて、 前記回転子の軸方向長を前記固定子の軸方向長
よりも前記軸受の長さに相当する分だけ長く形成
し、前記回転子の内周面または前記各支持軸の外
周面のいずれか一方もしくは両方に、前記回転子
と前記支持軸との間の隙間が小となるように環状
と凸部を形成し、該凸部の軸方向の長さを前記固
定子と同一長に形成したことを特徴とする可変空
隙型モータ。
[Claims for Utility Model Registration] A cylindrical stator that generates a rotating magnetic field along its inner peripheral surface, an output shaft that is disposed penetrating the central axis of the stator and is rotatably supported. , a plurality of substantially cylindrical tubes arranged parallel to the output shaft and at equal intervals on a virtual circumference centered on the output shaft, and revolving in close proximity to the inner circumferential surface of the stator; A rotor, a support shaft that rotatably supports each of the rotors via a bearing, and a revolution plate to which each of the support shafts is attached and which transmits the revolution of each of the rotors to the output shaft. A variable gap type motor, wherein the axial length of the rotor is longer than the axial length of the stator by an amount corresponding to the length of the bearing, and the inner circumferential surface of the rotor or each of the An annular convex portion is formed on one or both of the outer circumferential surfaces of the support shaft so that the gap between the rotor and the support shaft is small, and the length of the convex portion in the axial direction is A variable gap type motor characterized by being formed to have the same length as the stator.
JP1987047333U 1987-03-30 1987-03-30 Expired JPH0441753Y2 (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP1987047333U JPH0441753Y2 (en) 1987-03-30 1987-03-30

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP1987047333U JPH0441753Y2 (en) 1987-03-30 1987-03-30

Publications (2)

Publication Number Publication Date
JPS63156573U JPS63156573U (en) 1988-10-13
JPH0441753Y2 true JPH0441753Y2 (en) 1992-09-30

Family

ID=30867840

Family Applications (1)

Application Number Title Priority Date Filing Date
JP1987047333U Expired JPH0441753Y2 (en) 1987-03-30 1987-03-30

Country Status (1)

Country Link
JP (1) JPH0441753Y2 (en)

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* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPWO2021049327A1 (en) * 2019-09-11 2021-03-18

Also Published As

Publication number Publication date
JPS63156573U (en) 1988-10-13

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