JPS6321188Y2 - - Google Patents

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Publication number
JPS6321188Y2
JPS6321188Y2 JP1979040012U JP4001279U JPS6321188Y2 JP S6321188 Y2 JPS6321188 Y2 JP S6321188Y2 JP 1979040012 U JP1979040012 U JP 1979040012U JP 4001279 U JP4001279 U JP 4001279U JP S6321188 Y2 JPS6321188 Y2 JP S6321188Y2
Authority
JP
Japan
Prior art keywords
permanent magnet
ring
rotor
shaft
motor
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
JP1979040012U
Other languages
Japanese (ja)
Other versions
JPS55141277U (en
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
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Priority to JP1979040012U priority Critical patent/JPS6321188Y2/ja
Publication of JPS55141277U publication Critical patent/JPS55141277U/ja
Application granted granted Critical
Publication of JPS6321188Y2 publication Critical patent/JPS6321188Y2/ja
Expired legal-status Critical Current

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  • Permanent Field Magnets Of Synchronous Machinery (AREA)

Description

【考案の詳細な説明】 本考案は、連続回転で使用される同期モータの
起動特性を大幅に向上させることのできる永久磁
石ロータに関し、更に詳しくは、リング状永久磁
石がロータシヤフトに対して回転振動可能に、弾
性的に支持されてなる永久磁石ロータに関する。
[Detailed Description of the Invention] The present invention relates to a permanent magnet rotor that can significantly improve the starting characteristics of a synchronous motor used in continuous rotation. The present invention relates to a permanent magnet rotor that is elastically supported so as to be able to vibrate.

永久磁石ロータ型の同期モータは、周知のよう
に、ステータの巻線に通電することによつて形成
される回転磁界と、永久磁石ロータの磁極との相
互作用で生じる同期トルクによつて、永久磁石ロ
ータが同期速度で回転するモータである。なお、
本考案において「同期モータ」とは、基本的には
同じ動作原理を応用しているステツプモータ(階
動電動機)をも含めた広い概念を示す用語として
用いている。
As is well known, a permanent magnet rotor type synchronous motor uses a rotating magnetic field created by energizing the stator windings and a synchronous torque generated by the interaction with the magnetic poles of the permanent magnet rotor to generate a permanent motor. This is a motor in which the magnet rotor rotates at a synchronous speed. In addition,
In the present invention, the term "synchronous motor" is used to refer to a broad concept that includes step motors (step motors) that basically apply the same operating principle.

ところで同期速度が高く、ロータの慣性がある
程度大きい場合あるいはロータ自身の慣性がある
程度小さくてもロータ軸が背負う負荷の慣性があ
る程度大きい場合には、ロータとして永久磁石の
みを使つた狭義の同期モータでは、電源スイツチ
を入れても振動トルクが生じるだけで始動トルク
は存在しない。これは、モータの最大トルクをも
つてしても短時間内にロータを同期速度まで加速
しえないからである。しかし電源周波数が低い場
合には瞬時にして同期速度に達することができ、
これを利用して始動時に電源周波数を低い周波数
から所定の周波数まで掃引して起動させるのが周
波数制御形永久磁石同期モータである。だが、こ
のような速度制御をしようとすると高価な電子装
置が必要となる。
By the way, when the synchronous speed is high and the inertia of the rotor is large to some extent, or even if the inertia of the rotor itself is small to some extent but the inertia of the load carried by the rotor shaft is large to some extent, a narrowly defined synchronous motor that uses only permanent magnets as the rotor Even if the power switch is turned on, only vibration torque is generated and there is no starting torque. This is because even the maximum torque of the motor cannot accelerate the rotor to synchronous speed within a short period of time. However, if the power supply frequency is low, synchronous speed can be reached instantaneously.
A frequency-controlled permanent magnet synchronous motor takes advantage of this and starts the motor by sweeping the power supply frequency from a low frequency to a predetermined frequency. However, such speed control requires expensive electronic equipment.

なお、ステツプモータの場合も同様である。ス
テツプモータは狭義の同期モータと異なり、回転
子の慣性を小さく、多極にして磁極間隔を小さく
して同期トルクのみでも起動するようになつてい
るが、それでも連続回転領域内では一旦停止する
と再起動回路を動作させないかぎり起動しない
し、負荷がある程度以上大きい場合にも起動しに
くい。
Note that the same applies to the step motor. A step motor differs from a synchronous motor in the narrow sense in that it has a small rotor inertia and has multiple poles with a small spacing between magnetic poles so that it can be started with only synchronous torque. It will not start unless the startup circuit is activated, and it will be difficult to start even if the load is large beyond a certain level.

狭義の同期モータにおいては、上記のような起
動の困難性を解決するため、ステータヨークを弾
性支持体によつて外部外付用ブラケツト内面に取
付け、該ステータヨークが円周方向に振動できる
ようにしたものも案出されている。しかし、ステ
ータ側は慣性モーメントが大きく、振動しにくい
し、振動させるにはかなりの力が必要となるほ
か、円周方向のみに振動させることは困難であ
る。
In a narrowly defined synchronous motor, in order to solve the above-mentioned difficulty in starting, the stator yoke is attached to the inner surface of the external bracket with an elastic support, so that the stator yoke can vibrate in the circumferential direction. Some have also been devised. However, the stator side has a large moment of inertia and is difficult to vibrate, requires considerable force to vibrate, and is difficult to vibrate only in the circumferential direction.

本考案は、このような従来技術の実情に鑑みな
されたものであつて、その目的とするところは、
構造極めて簡単であつて、従来よりもはるかに起
動の容易な同期モータ用の永久磁石ロータを提供
することにある。
The present invention was developed in view of the actual state of the prior art, and its purpose is to:
An object of the present invention is to provide a permanent magnet rotor for a synchronous motor which has an extremely simple structure and is much easier to start than conventional ones.

即ち、従来の永久磁石ロータは、例えば第1図
に示すように、リング状永久磁石1と、シヤフト
2と、介在部材3(アルミニウムや硬質プラスチ
ツク製のロータリング)を用意し、圧入あるいは
接着等により固定一体化されていたのであるが、
介在部材として剛性のロータリングの代りに高分
子材料からなるクツシヨン材を用い、それによつ
てリング状の永久磁石がシヤフトに対して回転振
動可能に支持されているところに本考案の特徴が
ある。
That is, as shown in FIG. 1, for example, a conventional permanent magnet rotor includes a ring-shaped permanent magnet 1, a shaft 2, and an intervening member 3 (a rotor ring made of aluminum or hard plastic), which are press-fitted or bonded together. It was fixedly integrated by
The present invention is characterized in that a cushion material made of a polymeric material is used as an intervening member instead of a rigid rotor ring, and thereby a ring-shaped permanent magnet is supported so as to be able to rotate and vibrate with respect to the shaft.

以下、本考案について更に詳しく説明する。第
2図は本考案に係る永久磁石ロータの一実施例を
示す一部破断斜視図である。リング状の永久磁石
ロータ11とその中心軸部に位置するシヤフト1
2とを結合する介在部材としてゴムやポリウレタ
ンフオーム等の高分子材料からなるクツシヨン材
13aを用いている。シヤフト12にリング状永
久磁石11の高さにほぼ等しい間隔おいて、該リ
ング状永久磁石11の内径よりもやや小径の端円
板14,15を配置し、リング状永久磁石11で
覆う。そして、内部空間にクツシヨン材13aを
充填する。つまり、シヤフト12はクツシヨン材
13aを介してリング状永久磁石11と弾性的に
結合されているが、端円板14,15とは非接着
の状態にある。ただし、この関係は逆、つまりリ
ング状永久磁石11がクツシヨン材13aを介し
てシヤフト12と弾性的に結合し、端円板14,
15とは非接着の状態であつてもよい。したがつ
て、シヤフト12が固定されていても、リング状
永久磁石11はシヤフトの周囲を回転振動しう
る。端円板14,15はリング状永久磁石11の
回転振動の軌道の案内となり、ラジアル方向への
不要な振動を阻止すると共に、シヤフト12が水
平方向を向いて配置された場合でも該シヤフト1
2が偏心するのを防止し、またクツシヨン材13
aを充填する場合の型枠としても機能する。勿
論、クツシヨン材13aを予め成形しておいて、
接着等により組立てることも自由である。
The present invention will be explained in more detail below. FIG. 2 is a partially cutaway perspective view showing an embodiment of the permanent magnet rotor according to the present invention. A ring-shaped permanent magnet rotor 11 and a shaft 1 located at its central axis.
A cushion material 13a made of a polymeric material such as rubber or polyurethane foam is used as an intervening member that connects the parts 2 and 2. End disks 14 and 15 having a diameter slightly smaller than the inner diameter of the ring-shaped permanent magnet 11 are disposed on the shaft 12 at intervals approximately equal to the height of the ring-shaped permanent magnet 11, and are covered with the ring-shaped permanent magnet 11. Then, the interior space is filled with cushion material 13a. That is, the shaft 12 is elastically coupled to the ring-shaped permanent magnet 11 via the cushion material 13a, but is not bonded to the end discs 14, 15. However, this relationship is reversed, that is, the ring-shaped permanent magnet 11 is elastically coupled to the shaft 12 via the cushion material 13a, and the end disc 14,
15 may be in a non-adhesive state. Therefore, even if the shaft 12 is fixed, the ring-shaped permanent magnet 11 can rotate and vibrate around the shaft. The end disks 14 and 15 serve as guides for the trajectory of the rotational vibration of the ring-shaped permanent magnet 11, preventing unnecessary vibration in the radial direction, and even when the shaft 12 is arranged horizontally, the shaft 1
2 from eccentricity, and the cushion material 13
It also functions as a mold for filling a. Of course, the cushion material 13a is formed in advance,
It is also free to assemble by gluing or the like.

このような構造の永久磁石ロータを同期モータ
に組込むと、たとえその負荷が大きくても、リン
グ状永久磁石11の回転振動の際の慣性モーメン
トは極く小さく、それ故起動当初はシヤフト12
があまり動かなくてもリング状永久磁石11が円
周方向に振動し、クツシヨン材13aが弾性変形
した際の弾性復元力と同期トルクとの方向、タイ
ミングが一致した時、両者が強め合つて非常に大
きなトルクとなり、ロータ全体が加速回転し、同
期回転へと至る。従つて起動が極めて容易とな
る。
When a permanent magnet rotor with such a structure is incorporated into a synchronous motor, even if the load is large, the moment of inertia during rotational vibration of the ring-shaped permanent magnet 11 is extremely small, and therefore the shaft 12 is
Even if the ring-shaped permanent magnet 11 does not move much, it vibrates in the circumferential direction, and when the direction and timing of the elastic restoring force when the cushion material 13a is elastically deformed and the synchronizing torque match, the two strengthen each other and generate an extremely A large torque is generated, and the entire rotor rotates at an accelerated rate, leading to synchronous rotation. Therefore, startup becomes extremely easy.

この様子は、第3図のトルク−周波数特性曲線
図によつてより一層明確になるであろう。図中、
破線Aは、第1図に示す従来構造のロータを用い
た起動特性、すなわちステツプ(歩進)が入力信
号周波数と完全に1対1に対応して起動できるモ
ータの負荷トルクを測定したものであり、破線B
は連続特性、すなわち同期運転してるモータが同
期を脱する脱出周波数と負荷トルクの関係を示し
たものである。これに対して上記本考案実施例の
構造のロータを用いた場合、起動特性は曲線Cに
示すように連続回転領域に大きく延び、連続特性
に極めて近い特性となる。つまり、同じ負荷を背
負つている場合でも、本考案品は従来品に比しよ
り高い周波数で起動することができるし、実質的
に拡大された起動特性領域内(斜線及び符号Dで
示す)ならば、従来品の起動特性領域外であつて
も、再起動回路を使用せずに再起動させることが
できる。
This situation will become even clearer from the torque-frequency characteristic curve diagram in FIG. In the figure,
The broken line A shows the starting characteristic using the rotor of the conventional structure shown in Fig. 1, that is, the load torque of a motor that can be started in a completely one-to-one correspondence with the input signal frequency. Yes, dashed line B
is a continuous characteristic, that is, the relationship between the escape frequency at which a synchronously operating motor loses synchronization and the load torque. On the other hand, when the rotor having the structure according to the embodiment of the present invention is used, the starting characteristic greatly extends into the continuous rotation region as shown by curve C, and becomes a characteristic that is extremely close to the continuous rotational characteristic. In other words, even when carrying the same load, the product of this invention can be started at a higher frequency than the conventional product, and within the substantially expanded starting characteristic range (indicated by diagonal lines and symbol D). For example, even if the product is outside the startup characteristic range of conventional products, it can be restarted without using a restart circuit.

従つて本考案は、起動時あるいは再起動時に、
クロツクパルスに対して必ずしも1対1で完全に
同期して回転しなくてもよいような場合の定速回
転用途にステツプモータを用いるとき、例えばフ
オノモータ、に好適である。勿論、通常の同期モ
ータにも適用できる。
Therefore, the present invention, upon startup or restart,
When a step motor is used for constant-speed rotation applications where it does not necessarily have to rotate completely in one-to-one synchronization with clock pulses, it is suitable for use as a phono motor, for example. Of course, it can also be applied to ordinary synchronous motors.

本考案は上記のような永久磁石ロータであるか
ら、構造極めて簡単で、永久磁石がシヤフトに対
して回転振動自在に支持されているから、従来よ
りもはるかに起動が容易であり、実質的に起動特
性を大幅に拡大することができ、再起動に際して
も特別の再起動回路を必要としないなどすぐれた
実用的効果がある。
Since the present invention is a permanent magnet rotor as described above, the structure is extremely simple, and since the permanent magnet is supported on the shaft so that it can rotate and vibrate freely, it is much easier to start up than conventional methods, and it is substantially The starting characteristics can be greatly expanded, and there are excellent practical effects such as no need for a special restart circuit when restarting.

クツシヨン材の内側面はシヤフトに、外側面は
永久磁石にそれぞれ固着されているから軸方向の
振動は阻止され、またクツシヨン材の端面には永
久磁石に嵌合する端板が配置されているからラジ
アル方向への不要な振動が阻止される。つまり永
久磁石とシヤフトとは回転振動のみが許容される
ため、ロータがステータと衝突して騒音を生じた
り破損する虞れはないし、ロータとステータとを
近接配置できるからモータ効率を向上させること
ができる効果がある。
The inner surface of the cushion material is fixed to the shaft, and the outer surface is fixed to the permanent magnet, so vibration in the axial direction is prevented, and end plates that fit into the permanent magnets are arranged on the end surfaces of the cushion material. Unnecessary vibration in the radial direction is prevented. In other words, only rotational vibration is allowed between the permanent magnet and the shaft, so there is no risk of the rotor colliding with the stator and causing noise or damage, and since the rotor and stator can be placed close together, motor efficiency can be improved. There is an effect that can be done.

クツシヨン材は全周にわたつて均一に設けら
れ、しかも粘弾性挙動を呈するから、同期モータ
の脈流駆動に対して円滑な回転動作を行わせるこ
とができる。
Since the cushion material is uniformly provided over the entire circumference and exhibits viscoelastic behavior, it is possible to perform smooth rotational motion in response to the pulsating flow drive of the synchronous motor.

永久磁石とシヤフトとの間には特別なストツパ
部材等は設けられておらず回転振動可能な範囲に
は特に制限はない。専らクツシヨン材の性能のみ
に依存している。そのため起動や停止に際してス
トツパ部材が他の部材と衝突して騒音が生じるこ
ともなく、スムーズな起動が行われる。またこの
ことはトルク範囲や駆動周波数範囲を広くできる
ことにつながり、同一仕様のモータを様々な使用
条件で使えるという極めて好ましい効果ももたら
される。
No special stopper member or the like is provided between the permanent magnet and the shaft, and there is no particular limit to the range in which rotational vibration can occur. It depends exclusively on the performance of the cushion material. Therefore, the stopper member does not collide with other members and generate noise when starting or stopping, and smooth starting is performed. This also leads to the ability to widen the torque range and drive frequency range, which brings about the extremely favorable effect of being able to use a motor with the same specifications under various operating conditions.

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

第1図は従来のロータの縦断面図、第2図は本
考案に係るロータの一実施例の一部破断斜視図、
第3図は従来品と本考案品との特性比較曲であ
る。 11……リング状永久磁石、12……シヤフ
ト、13a……クツシヨン材。
FIG. 1 is a longitudinal sectional view of a conventional rotor, and FIG. 2 is a partially cutaway perspective view of an embodiment of the rotor according to the present invention.
Figure 3 is a comparison song of the characteristics of the conventional product and the product of the present invention. 11...Ring-shaped permanent magnet, 12...Shaft, 13a...Cushion material.

Claims (1)

【実用新案登録請求の範囲】[Scope of utility model registration request] 介在部材によつてリング状永久磁石とその中心
軸部に位置するシヤフトとを結合してなる永久磁
石ロータにおいて、前記介在部材は高分子材料か
らなるクツシヨン材であり、その内側面がシヤフ
トに、外側面がリング状永久磁石にそれぞれ固着
され、端面には前記リング状永久磁石に嵌合する
端板が配置されていて、リング状永久磁石がシヤ
フトに対して回転振動自在に支持されている同期
モータの永久磁石ロータ。
In a permanent magnet rotor in which a ring-shaped permanent magnet and a shaft located at its central axis are connected by an intervening member, the intervening member is a cushion material made of a polymeric material, and the inner surface thereof is connected to the shaft. A synchronous motor in which the outer surfaces are each fixed to a ring-shaped permanent magnet, an end plate that fits into the ring-shaped permanent magnet is arranged on the end surface, and the ring-shaped permanent magnet is supported with respect to a shaft so as to be able to rotate and vibrate freely. Permanent magnet rotor of motor.
JP1979040012U 1979-03-29 1979-03-29 Expired JPS6321188Y2 (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP1979040012U JPS6321188Y2 (en) 1979-03-29 1979-03-29

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP1979040012U JPS6321188Y2 (en) 1979-03-29 1979-03-29

Publications (2)

Publication Number Publication Date
JPS55141277U JPS55141277U (en) 1980-10-08
JPS6321188Y2 true JPS6321188Y2 (en) 1988-06-10

Family

ID=28907925

Family Applications (1)

Application Number Title Priority Date Filing Date
JP1979040012U Expired JPS6321188Y2 (en) 1979-03-29 1979-03-29

Country Status (1)

Country Link
JP (1) JPS6321188Y2 (en)

Families Citing this family (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPH0431814Y2 (en) * 1985-07-30 1992-07-30

Citations (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS52116815A (en) * 1976-03-25 1977-09-30 Sundstrand Corp Structure for mounting permanent magnet at rotary shaft

Patent Citations (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS52116815A (en) * 1976-03-25 1977-09-30 Sundstrand Corp Structure for mounting permanent magnet at rotary shaft

Also Published As

Publication number Publication date
JPS55141277U (en) 1980-10-08

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