JPH07111767A - Power generating apparatus - Google Patents

Power generating apparatus

Info

Publication number
JPH07111767A
JPH07111767A JP5317249A JP31724993A JPH07111767A JP H07111767 A JPH07111767 A JP H07111767A JP 5317249 A JP5317249 A JP 5317249A JP 31724993 A JP31724993 A JP 31724993A JP H07111767 A JPH07111767 A JP H07111767A
Authority
JP
Japan
Prior art keywords
magnetic field
rotating
magnetic
output shaft
rotating magnetic
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.)
Granted
Application number
JP5317249A
Other languages
Japanese (ja)
Other versions
JP2796237B2 (en
Inventor
Teruo Kawai
輝男 河合
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.)
NIPPON RIKEN KK
Original Assignee
NIPPON RIKEN KK
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 NIPPON RIKEN KK filed Critical NIPPON RIKEN KK
Priority to JP5317249A priority Critical patent/JP2796237B2/en
Publication of JPH07111767A publication Critical patent/JPH07111767A/en
Application granted granted Critical
Publication of JP2796237B2 publication Critical patent/JP2796237B2/en
Anticipated expiration legal-status Critical
Expired - Fee Related legal-status Critical Current

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  • Permanent Magnet Type Synchronous Machine (AREA)
  • Permanent Field Magnets Of Synchronous Machinery (AREA)

Abstract

PURPOSE:To obtain a power generating apparatus having a high torque and a high energy efficiency, without any increase of its size. CONSTITUTION:A power generating apparatus has an electromagnet 11 generating a rotating magnetic field in the case of its excitation caused by the application of a three-phase AC current to it, a rotary output shaft 12 mounted in a rotatable way on a supporting member 10 so as to be placed in the rotating magnetic field, permanent magnets 14a, 14b which are so provided around the rotary output shaft 12 that the polarity of the rotating magnetic field generated by them is inverse to the one of the rotating magnetic field generated by the electromagnet 11 and which are rotated together with the output shaft 12, and magnetic substances 15a, 15b which are provided respectively on the outsides of the permanent magnets 14a, 14b and are rotated together with the rotary output shaft 12. Through the magnetic substances 15a, 15b, the magnetic fluxes of the permanent magnets 14a, 14b are passed respectively, and the magnetic substances 15a, 15b have respectively on their outer peripheral parts magnetic tooth parts 150a, 150b whose width are nearly equal to the ones of the rotating magnetic field. In case of the excitation of the electromagnet 11, the magnetic fluxes are converged on the side of the rotating magnetic field and are rotated together with the rotating magnetic field. Thereby, the rotary output shaft 12 receives a rotating torque.

Description

【発明の詳細な説明】Detailed Description of the Invention

【0001】[0001]

【産業上の利用分野】本発明は、固定子として交流電流
により回転磁界を発生する電磁石を使用し、回転子とし
て永久磁石と軟鋼等の磁性体とを組み合わせて使用した
動力変換装置に関するものである。
BACKGROUND OF THE INVENTION 1. Field of the Invention The present invention relates to a power conversion device which uses an electromagnet which generates a rotating magnetic field by an alternating current as a stator and uses a permanent magnet and a magnetic material such as mild steel in combination as a rotor. is there.

【0002】[0002]

【従来の技術】これまで、固定子として交流電流により
回転磁界を発生する電磁石を使用し、回転子として永久
磁石を使用した同期モータが知られている。この同期モ
ータでは、固定子の電磁石に交流電流を印加して回転磁
界を発生させ、この回転磁界で回転子を引っ張って回転
するようにしてある。
2. Description of the Related Art Up to now, there has been known a synchronous motor which uses an electromagnet for generating a rotating magnetic field by an alternating current as a stator and a permanent magnet as a rotor. In this synchronous motor, an alternating current is applied to the electromagnet of the stator to generate a rotating magnetic field, and the rotating magnetic field pulls and rotates the rotor.

【0003】[0003]

【発明が解決しようとする課題】しかしながら、この同
期モーターでは、永久磁石のエネルギが電気エネルギ同
様の入力エネルギとして活用されていない。さらにこの
同期モーターでは、自己始動が困難であり、このためか
ご型回転子を併置して誘導モーターの原理で加速するよ
うにしているが、寸法的に大型化する問題がある。
However, in this synchronous motor, the energy of the permanent magnet is not used as the input energy like the electrical energy. Further, in this synchronous motor, self-starting is difficult, and for this reason, a squirrel-cage rotor is arranged side by side to accelerate by the principle of an induction motor, but there is a problem in that it becomes large in size.

【0004】そこで、同期状態を得易いように、この同
期モーターの鉄心に多数の歯を設けて見かけ上の極数を
増加させることにより同期速度を低くし、かご型回転子
を併置することなく停止状態から同期状態に直接引き込
むことができるようにした同期モーター(インダクタ型
同期モーター)が提案されている。この同期モーター
は、ステッピングモーターと類似したものであるが、ス
テッピングモーターと同様に磁極の半分しかトルクに寄
与することができず、電磁石に引加する電流エネルギの
観点からみても、また永久磁石の磁気エネルギが入力エ
ネルギとして付加されていないという点からみても、エ
ネルギ効率が低い問題がある。
Therefore, in order to easily obtain the synchronized state, a large number of teeth are provided on the iron core of the synchronous motor to increase the apparent number of poles, thereby lowering the synchronous speed and eliminating the squirrel cage rotor. A synchronous motor (inductor type synchronous motor) has been proposed which can be directly pulled from a stopped state to a synchronous state. This synchronous motor is similar to the stepping motor, but like the stepping motor, only half of the magnetic poles can contribute to the torque. From the viewpoint of the current energy applied to the electromagnet, the synchronous motor is also There is a problem that the energy efficiency is low even from the viewpoint that magnetic energy is not added as input energy.

【0005】したがって、本発明は、永久磁石の磁気エ
ネルギを入力エネルギに変換し、これを電気エネルギに
付加活用することにより、大型化せず、エネルギ効率が
よく、高トルクが得られる動力発生装置を提供すること
を目的とする。
Therefore, according to the present invention, the magnetic energy of the permanent magnet is converted into the input energy, and the energy is added to the electric energy to be utilized. The purpose is to provide.

【0006】[0006]

【課題を解決しようとするための手段】上記目的を達成
するため本発明では、磁気エネルギを動力に変換する動
力発生装置にして、支持部材に固定配置され、交流電流
を印加して励磁したときに回転磁界を発生する電磁石
と、前記回転磁界中に位置するようにして前記支持部材
に回転自在に装備された回転出力軸と、前記回転磁界の
極性と逆極性となる関係で前記回転出力軸の回りに配置
され、該回転出力軸とともに回転する永久磁石と、前記
永久磁石の外側に配置され、前記回転出力軸とともに回
転する磁性体とを具備し、前記磁性体は前記永久磁石の
磁束が通り、前記電磁石を励磁したときに、前記永久磁
石の磁束が前記回転磁界側に収束されながら回転磁界と
ともに回転することにより、前記回転出力軸が回転トル
クを受けるように構成してなることを特徴としている。
In order to achieve the above object, the present invention provides a power generation device for converting magnetic energy into power, which is fixedly arranged on a support member and is excited by applying an alternating current. An electromagnet that generates a rotating magnetic field, a rotating output shaft that is rotatably mounted on the supporting member so as to be positioned in the rotating magnetic field, and the rotating output shaft having a polarity opposite to the polarity of the rotating magnetic field. A permanent magnet disposed around the rotary output shaft and rotating with the rotary output shaft, and a magnetic body disposed outside the permanent magnet and rotating with the rotary output shaft, wherein the magnetic body has a magnetic flux of the permanent magnet. As described above, when the electromagnet is excited, the magnetic flux of the permanent magnet converges to the rotating magnetic field side and rotates together with the rotating magnetic field, so that the rotating output shaft receives the rotating torque. Is characterized in that the composed.

【0007】[0007]

【作用】上記発明によれば、電磁石に交流電流を印加し
ないときには、磁性体を通る永久磁石の磁束は磁性体全
体に広がっているが、電磁石に交流電流を印加して回転
磁界を発生させると、磁束が回転磁界側に収束されるこ
とにより初期回転トルクが発生する。同時に、磁性体磁
歯部において回転磁界と反対側の端部では、永久磁石に
よる磁束が極端に弱められか、ほとんど無くなってしま
う現象が起こり、このため、この部分とステーター側鉄
心との関わりにおいて回転方向に逆らう力が大きく減じ
られる。従って、順次励磁される回転磁界によって、永
久磁石からは回転力にプラスする力のみが一方的に提供
されることになる。また、これにより回転子(磁性体及
び永久磁石)が瞬時に同期状態になり、同期運転、すな
わち、回転磁界と回転子の磁気軸との負荷角θによって
発生する回転トルクによる運転に移行する。
According to the above invention, when no alternating current is applied to the electromagnet, the magnetic flux of the permanent magnet passing through the magnetic body is spread over the entire magnetic body. However, when an alternating current is applied to the electromagnet to generate a rotating magnetic field. The initial rotation torque is generated by the magnetic flux being converged on the rotating magnetic field side. At the same time, a phenomenon occurs in which the magnetic flux from the permanent magnet is extremely weakened or almost disappeared at the end of the magnetic body magnetic tooth opposite to the rotating magnetic field. The force against the direction of rotation is greatly reduced. Therefore, due to the rotating magnetic field that is sequentially excited, only the force that is in addition to the rotating force is unilaterally provided from the permanent magnet. Further, by this, the rotor (the magnetic body and the permanent magnet) is instantaneously brought into the synchronous state, and the synchronous operation, that is, the operation by the rotational torque generated by the load angle θ between the rotating magnetic field and the magnetic axis of the rotor is started.

【0008】[0008]

【実施例】以下、本発明の好ましい実施例を、添付図面
を参照して詳細に説明する。
DETAILED DESCRIPTION OF THE PREFERRED EMBODIMENT A preferred embodiment of the present invention will now be described in detail with reference to the accompanying drawings.

【0009】本実施例によれば、第1図及び第2図に示
すように、支持部材10の前後側板10a間に固定子と
なる電磁石11が装備されている。この電磁石11は、
例えば、24個のスロットを設けた円筒状の鉄心11a
に12組のコイル11bを巻回して構成してあり、3相
の交流電流を印加したときに回転磁界を発生する。この
回転磁界は、図4に示すように、後述する回転出力軸1
2に対して垂直な平面内に分布し、例えば図1の時計方
向に回転する。
According to this embodiment, as shown in FIGS. 1 and 2, an electromagnet 11 serving as a stator is provided between the front and rear side plates 10a of the support member 10. This electromagnet 11 is
For example, a cylindrical iron core 11a provided with 24 slots
It is configured by winding 12 sets of coils 11b, and generates a rotating magnetic field when a three-phase alternating current is applied. This rotating magnetic field, as shown in FIG.
It is distributed in a plane perpendicular to 2 and rotates, for example, clockwise in FIG.

【0010】支持部材10の前後側板10a間であって
電磁石11の回転磁界中には、回転出力軸12が軸受1
3を介して回転自在に装備されている。この回転出力軸
12の外周には、それを囲むようにして半円筒状の永久
磁石14a、14bが配置されている。図1及び図3で
は、一方の永久磁石14aは回転磁界の一方の磁極(S
極)と反対のN極に、他方の永久磁石14bは回転磁界
の他方の磁極(N極)と反対のS極になるようにそれぞ
れ着磁してある。これら永久磁石14a、14bを組み
合わせて円筒状にしたときに作り出す磁界は,電磁石1
1の回転磁界と同様に回転出力軸11に対して垂直な平
面内に分布している。また、永久磁石14a、14bの
磁力は電磁石11の作り出す回転磁界の磁力にとらわれ
ることなく設定することができる。
Between the front and rear side plates 10a of the support member 10 and in the rotating magnetic field of the electromagnet 11, the rotary output shaft 12 has the bearing 1
It is equipped rotatably through 3. Semi-cylindrical permanent magnets 14a and 14b are arranged on the outer circumference of the rotation output shaft 12 so as to surround it. In FIG. 1 and FIG. 3, one permanent magnet 14a is one magnetic pole (S
The other permanent magnet 14b is magnetized so as to be an S pole opposite to the other magnetic pole (N pole) of the rotating magnetic field. The magnetic field created when these permanent magnets 14a, 14b are combined into a cylindrical shape is
Similar to the rotating magnetic field of 1, the magnetic field is distributed in a plane perpendicular to the rotation output shaft 11. Further, the magnetic forces of the permanent magnets 14a and 14b can be set without being restricted by the magnetic force of the rotating magnetic field generated by the electromagnet 11.

【0011】永久磁石14aの外側にはそれを囲むよう
にして一方の磁性体15aが配置され、また永久磁石1
4bの外側にはそれを囲むようにして他方の磁性体15
bが配置されており、これら磁性体15a、15bには
永久磁石14a、14bの磁束が通る。磁性体15a、
15bの外周部には、電磁石11の回転磁界と略等しい
幅を有して径方向に突出する磁歯部150a、150b
がそれぞれ一体に設けられている。ここで、磁性体15
aと磁性体15bとを互いに接合せず、図1に示すよう
に両者間に隙間を設けたのは、仮に両者を接合した場合
には永久磁石14a、14bの磁束の大部分が磁性体1
5a、15bの外側に出ず、磁性体15a、15b内に
閉じ込められてしまい、回転磁界に引っ張られて回転ト
ルクを生み出しにくくなるからである。
On the outside of the permanent magnet 14a, one magnetic body 15a is arranged so as to surround the permanent magnet 14a.
On the outside of 4b, the other magnetic body 15 is formed so as to surround it.
b is arranged, and the magnetic flux of the permanent magnets 14a and 14b passes through these magnetic bodies 15a and 15b. Magnetic body 15a,
Magnetic tooth portions 150a, 150b having a width substantially equal to the rotating magnetic field of the electromagnet 11 and protruding in the radial direction are provided on the outer peripheral portion of 15b.
Are provided integrally with each other. Here, the magnetic body 15
1a and the magnetic body 15b are not joined to each other, and a gap is provided between them as shown in FIG. 1, if the two are joined, most of the magnetic flux of the permanent magnets 14a and 14b is the magnetic body 1.
This is because they do not come out of the outer side of 5a and 15b, are confined in the magnetic bodies 15a and 15b, and are difficult to generate the rotating torque by being pulled by the rotating magnetic field.

【0012】永久磁石14a、14bと磁性体15a、
15bは、同軸状態で回転出力軸12の外側に取り付け
られており、電磁石11の回転磁界中で該回転磁界に引
っ張られて回転出力軸12とともに回転する回転子をな
している。
The permanent magnets 14a, 14b and the magnetic body 15a,
15b is attached to the outside of the rotary output shaft 12 in a coaxial state, and forms a rotor that is pulled by the rotary magnetic field in the rotating magnetic field of the electromagnet 11 and rotates together with the rotary output shaft 12.

【0013】また、本実施例では、電磁石11は、単一
の回転磁界を発生し、極数が2極で作動する。また、磁
歯部150a、150bの一方の端部、すなわち回転子
の回転方向側の端部151a、151bを鋭角に設定
し、磁性体15a、15bを通る永久磁石14a、14
bの磁束が回転磁界側に収束されたとき、大きな回転ト
ルクを生み出すように(磁歯部150a、150bと電
磁石11の鉄心11aとの間の隙間において磁力線の傾
斜が大きくなるように)してある。換言すれば、始動時
に回転トルクが効率よく得られるようにしてある。磁性
体15a、15bは例えば各種鉄材、ケイ素鋼板、パー
マロイ等の透磁率の高い磁性体材料により形成すること
ができるが、本実施例では軟磁性材料により形成してあ
る。
Further, in this embodiment, the electromagnet 11 generates a single rotating magnetic field and operates with two poles. Further, one end of the magnetic tooth portions 150a and 150b, that is, the end portions 151a and 151b on the rotation direction side of the rotor are set to an acute angle, and the permanent magnets 14a and 14 passing through the magnetic bodies 15a and 15b are set.
When the magnetic flux of b is converged to the rotating magnetic field side, a large rotating torque is generated (inclination of magnetic force line becomes large in the gap between the magnetic tooth portions 150a and 150b and the iron core 11a of the electromagnet 11). is there. In other words, the rotation torque is efficiently obtained at the time of starting. The magnetic bodies 15a and 15b can be made of, for example, various iron materials, silicon steel sheets, magnetic materials having a high magnetic permeability such as permalloy, but in this embodiment, they are made of a soft magnetic material.

【0014】次に上記実施例の作用を説明する。Next, the operation of the above embodiment will be described.

【0015】電磁石11に3相交流電流を印加しないと
き、磁性体15a、15bを通る永久磁石14a、14
bの磁束は、磁性体15a、15b全体に広がっている
が、電磁石11に3相交流電流を印加して回転磁界を発
生させると、磁束は回転磁界側に収束され、磁歯部15
0a、150bの端部151a、151bに集中するこ
とにより(図5の濃墨部分参照)、磁歯部150a、1
50bと電磁石11の鉄心11aとの間の隙間部分で磁
力線が大きく傾斜して時計方向の初期回転トルクが発生
する。これにより、回転子が瞬時に同期状態になり、同
期運転、すなわち回転磁界の磁気軸と回転子の磁気軸と
の間の負荷角θによって発生する回転トルクによる運転
状態に移行する。
When a three-phase alternating current is not applied to the electromagnet 11, the permanent magnets 14a, 14 passing through the magnetic bodies 15a, 15b.
The magnetic flux of b is spread over the entire magnetic bodies 15a and 15b, but when a three-phase alternating current is applied to the electromagnet 11 to generate a rotating magnetic field, the magnetic flux is converged to the rotating magnetic field side and the magnetic tooth portion 15 is formed.
0a, 150b by concentrating on the end portions 151a, 151b (see dark ink portion in FIG. 5), the magnetic tooth portions 150a, 1
The magnetic lines of force largely incline in the gap between the iron core 11a of the electromagnet 11 and 50b, and an initial rotational torque in the clockwise direction is generated. As a result, the rotor is instantaneously brought into a synchronous state, and a synchronous operation, that is, an operating state due to the rotational torque generated by the load angle θ between the magnetic axis of the rotating magnetic field and the magnetic axis of the rotor is entered.

【0016】換言すれば、回転磁界と磁歯部150a、
150bとの引き合いにより回転トルクを発生させる
際、回転子内部の永久磁石14a、14bの磁束が回転
磁界によって磁性体15a、15bを透過する過程で収
束されるために、瞬時に同期運転に入ることができる。
In other words, the rotating magnetic field and the magnetic tooth portion 150a,
When a rotating torque is generated by an inquiry with 150b, the magnetic flux of the permanent magnets 14a, 14b inside the rotor is converged in the process of passing through the magnetic bodies 15a, 15b by the rotating magnetic field, so that the synchronous operation is instantaneously performed. You can

【0017】ここで、本実施例のモータの運転初期時の
試験結果について説明する。
Here, the test results of the motor of this embodiment at the initial operation will be described.

【0018】磁性体として軟鉄を使用した。磁性体の形
状は図1に示す通りである。永久磁石にはサマリウム・
コバルト(SmCo)を使用した。その磁力は12,0
00ガウスであった。電磁石は市販の誘導モータ(3相
日立インダクションモータTFO−OK、最大出力31
0W)と同じものを使用した。モータ回転数の測定には
小野測器(株)製のデジタルタコメーターHT−410
0を使用した。
Soft iron was used as the magnetic material. The shape of the magnetic body is as shown in FIG. Samarium for permanent magnets
Cobalt (SmCo) was used. Its magnetic force is 12,0
It was 00 gauss. The electromagnet is a commercially available induction motor (3-phase Hitachi induction motor TFO-OK, maximum output 31
The same one was used. Digital tachometer HT-410 manufactured by Ono Sokki Co., Ltd.
0 was used.

【0019】上記の条件の下で運転し、所定回転数にな
るまでの時間を測定したところ、瞬時に回転数1,43
0rpmに達した。この試験結果は、前記の市販の誘導
モータと同じであった。この試験から、本実施例のモー
タは、同期モータでありながらかご型回転子を併置する
ことなく自己始動できることが確認された。
When the engine was operated under the above conditions and the time required to reach a predetermined rotation speed was measured, the rotation speed was 1,43 instantly.
Reached 0 rpm. The test results were the same as the commercial induction motor described above. From this test, it was confirmed that the motor of the present example could be self-started without arranging the squirrel cage rotor side by side, although it was a synchronous motor.

【0020】本実施例では、かご型回転子を使用せず、
磁性体を使用しているために大幅に小型化を図ることが
できる。また、自己始動の問題を解消するために、ステ
ッピングモータと類似した構造をとらないことから、エ
ネルギ効率が良い。さらに、永久磁石型同期モータと異
なり、永久磁石の磁力と回転磁界の磁力の比は1:1に
限定されず、永久磁石の磁力を回転磁界の磁力よりも大
きく設定し、トルクを高めることも可能である。すなわ
ち、高磁力の永久磁石を用いるほどに高トルクを得るこ
とができる。
In this embodiment, a cage rotor is not used,
Since a magnetic material is used, the size can be greatly reduced. Further, since the structure similar to that of the stepping motor is not adopted in order to solve the problem of self-starting, energy efficiency is good. Further, unlike the permanent magnet type synchronous motor, the ratio of the magnetic force of the permanent magnet and the magnetic force of the rotating magnetic field is not limited to 1: 1. The magnetic force of the permanent magnet can be set larger than the magnetic force of the rotating magnetic field to increase the torque. It is possible. That is, as the permanent magnet of high magnetic force is used, high torque can be obtained.

【0021】なお、磁性体を回転出力軸12に対して偏
心させて取り付けることにより、磁歯部を設けなくても
永久磁石の磁束を収束させて回転始動時に回転トルクを
得るようにすることも可能である。
The magnetic body may be eccentrically attached to the rotary output shaft 12 so that the magnetic flux of the permanent magnet can be converged to obtain the rotary torque at the start of rotation without providing the magnetic tooth portion. It is possible.

【0022】[0022]

【発明の効果】以上説明したように本発明によれば、回
転磁界中の永久磁石の外側に該永久磁石の磁束が通る磁
性体を配置し、電磁石を励磁したときに、永久磁石の磁
束が回転磁界側に収束されて回転磁界とともに回転する
ようにしてあるので、磁性体磁歯部の回転磁界と反対側
の端部では、通常ステーター側電磁石の鉄心との間で起
こるところの回転方向に逆行する力が無力に近い状態と
なり、永久磁石から回転方向に働く力のみが活用できる
ようになった。つまり、永久磁石の磁気エネルギを入力
側の作業エネルギとして変換し、電気エネルギと併合し
て出力を生ずることが可能になった。また、かご型回転
子を使用しなくても自己始動が可能で、小形化を図るこ
とができるし、自己始動の問題を解消するために、ステ
ッピングモータと類似した構造をとらないことからも、
エネルギ効率がよく、さらに高磁力の永久磁石を使用す
ることにより高トルクが得られる。
As described above, according to the present invention, a magnetic body through which the magnetic flux of the permanent magnet passes is arranged outside the permanent magnet in the rotating magnetic field, and when the electromagnet is excited, the magnetic flux of the permanent magnet is reduced. Since the magnetic field converges on the rotating magnetic field side and rotates together with the rotating magnetic field, at the end opposite to the rotating magnetic field of the magnetic body magnetic tooth part, in the direction of rotation that normally occurs between the iron core of the stator side electromagnet, The reverse force is almost powerless, and only the force acting in the rotation direction from the permanent magnet can be utilized. In other words, it has become possible to convert the magnetic energy of the permanent magnet into work energy on the input side and combine it with the electric energy to generate an output. In addition, self-starting is possible without using a squirrel-cage rotor, downsizing can be achieved, and in order to solve the problem of self-starting, a structure similar to that of a stepping motor is not adopted.
High torque is obtained by using a permanent magnet having high energy efficiency and high magnetic force.

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

【図1】本発明のモータの実施例を概略的に示す一部切
断、省略して示した一側面図である。
FIG. 1 is a side view schematically showing an embodiment of a motor of the present invention with a part cut and abbreviated.

【図2】図1に示すモータの縦断面図である。FIG. 2 is a vertical sectional view of the motor shown in FIG.

【図3】永久磁石の端面図である。FIG. 3 is an end view of a permanent magnet.

【図4】図1のモータの電磁石の作る回転磁界を説明す
る説明図である。
4 is an explanatory diagram illustrating a rotating magnetic field created by an electromagnet of the motor of FIG. 1. FIG.

【図5】図1のモータの電磁石を励磁したときの永久磁
石の磁束の収束状態を説明する説明図である。
5 is an explanatory diagram illustrating a converged state of magnetic flux of a permanent magnet when an electromagnet of the motor of FIG. 1 is excited.

【符号の説明】[Explanation of symbols]

10 支持部材 11 電磁石 11a 鉄心 11b コイル 14a、14b 永久磁石 15a、15b 磁性体 150a、150b 磁歯部 DESCRIPTION OF SYMBOLS 10 Support member 11 Electromagnet 11a Iron core 11b Coil 14a, 14b Permanent magnet 15a, 15b Magnetic body 150a, 150b Magnetic tooth part

Claims (3)

【特許請求の範囲】[Claims] 【請求項1】 磁気エネルギを動力に変換する動力発生
装置にして、 支持部材に固定配置され、単相、三単等(以下、単に交
流という)交流電流を印加して励磁したときに回転磁界
を発生する電磁石と、 前記回転磁界中に位置するようにして前記支持部材に回
転自在に装備された回転出力軸と、 前記回転磁界の極性と逆極性となる関係で前記回転出力
軸の回りに配置され、該回転出力軸とともに回転する永
久磁石と、 前記永久磁石の外側に配置され、前記回転出力軸ととも
に回転する磁性体とを具備し、 前記磁性体は、前記永久磁石の磁束が通り、前記電磁石
を励磁したときに、該磁束が前記回転磁界側に収束され
ながら回転磁界とともに回転することにより、前記回転
出力軸が回転トルクを受けるように構成してなることを
特徴とする動力発生装置。
1. A rotating magnetic field when used as a power generation device for converting magnetic energy into power, which is fixedly arranged on a support member and is excited by applying a single-phase, three-single, etc. (hereinafter simply referred to as AC) alternating current. A rotating output shaft rotatably mounted on the support member so as to be positioned in the rotating magnetic field, and a rotating output shaft having a polarity opposite to that of the rotating magnetic field. A permanent magnet that is arranged and rotates together with the rotation output shaft, and a magnetic body that is arranged outside the permanent magnet and that rotates together with the rotation output shaft, wherein the magnetic body has a magnetic flux of the permanent magnet passing therethrough; When the electromagnet is excited, the magnetic flux converges on the rotating magnetic field side and rotates together with the rotating magnetic field, so that the rotating output shaft receives a rotating torque. Generating device.
【請求項2】 請求項1に記載の動力発生装置にして、 前記磁性体の外周に、前記回転磁界とほぼ同じ幅の磁歯
部を設けてなることを特徴とする動力発生装置。
2. The power generator according to claim 1, wherein a magnetic tooth portion having substantially the same width as the rotating magnetic field is provided on the outer circumference of the magnetic body.
【請求項3】 請求項2に記載の動力発生装置にして、 前記磁歯部の回転方向側の端部を鋭角に形成してなるこ
とを特徴とする動力発生装置。
3. The power generator according to claim 2, wherein an end of the magnetic tooth portion on the rotation direction side is formed at an acute angle.
JP5317249A 1993-10-12 1993-10-12 Power generator Expired - Fee Related JP2796237B2 (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP5317249A JP2796237B2 (en) 1993-10-12 1993-10-12 Power generator

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP5317249A JP2796237B2 (en) 1993-10-12 1993-10-12 Power generator

Publications (2)

Publication Number Publication Date
JPH07111767A true JPH07111767A (en) 1995-04-25
JP2796237B2 JP2796237B2 (en) 1998-09-10

Family

ID=18086149

Family Applications (1)

Application Number Title Priority Date Filing Date
JP5317249A Expired - Fee Related JP2796237B2 (en) 1993-10-12 1993-10-12 Power generator

Country Status (1)

Country Link
JP (1) JP2796237B2 (en)

Cited By (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
CN111711299A (en) * 2020-08-04 2020-09-25 珠海格力电器股份有限公司 Single-phase permanent magnet self-starting motor and electric equipment with same

Citations (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPH05176487A (en) * 1991-10-24 1993-07-13 Toshiba Corp Permanent magnet type motor

Patent Citations (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPH05176487A (en) * 1991-10-24 1993-07-13 Toshiba Corp Permanent magnet type motor

Cited By (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
CN111711299A (en) * 2020-08-04 2020-09-25 珠海格力电器股份有限公司 Single-phase permanent magnet self-starting motor and electric equipment with same
CN111711299B (en) * 2020-08-04 2023-01-24 珠海格力电器股份有限公司 Single-phase permanent magnet self-starting motor and electric equipment with same

Also Published As

Publication number Publication date
JP2796237B2 (en) 1998-09-10

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