JPS58170347A - Rotor magnet - Google Patents
Rotor magnetInfo
- Publication number
- JPS58170347A JPS58170347A JP57050570A JP5057082A JPS58170347A JP S58170347 A JPS58170347 A JP S58170347A JP 57050570 A JP57050570 A JP 57050570A JP 5057082 A JP5057082 A JP 5057082A JP S58170347 A JPS58170347 A JP S58170347A
- Authority
- JP
- Japan
- Prior art keywords
- plate face
- permanent magnet
- circumferential direction
- shaped permanent
- surface side
- 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
Links
Classifications
-
- H—ELECTRICITY
- H02—GENERATION; CONVERSION OR DISTRIBUTION OF ELECTRIC POWER
- H02K—DYNAMO-ELECTRIC MACHINES
- H02K1/00—Details of the magnetic circuit
- H02K1/06—Details of the magnetic circuit characterised by the shape, form or construction
- H02K1/22—Rotating parts of the magnetic circuit
- H02K1/27—Rotor cores with permanent magnets
- H02K1/2793—Rotors axially facing stators
- H02K1/2795—Rotors axially facing stators the rotor consisting of two or more circumferentially positioned magnets
Abstract
Description
【発明の詳細な説明】
本発明は例えばブラシレス・コアレス・7ラツトモータ
に使用されるp−タマグネットの改良に関する。DETAILED DESCRIPTION OF THE INVENTION The present invention relates to improvements in p-ta magnets used, for example, in brushless, coreless, 7-rat motors.
従来、この種のロータマグネットは8極とか10極とか
に多極磁化された中空円板状の永久磁石板からなり、磁
化方向はその板面に対し垂直で円周方向上で交互に逆方
向に磁化されており、これに対向して配置される電機子
コイル(ステータ)の形成する回転磁界でもって駆動さ
れるものである0ロータマグネツトのステータ側の表面
磁束密度は速度変動を少なくするために円周方向におい
て正弦波分布するのが理想とされている。Conventionally, this type of rotor magnet consists of a hollow disk-shaped permanent magnet plate that is magnetized with multiple poles such as 8 or 10 poles, and the magnetization direction is perpendicular to the plate surface and alternately in opposite directions in the circumferential direction. The surface magnetic flux density on the stator side of the 0-rotor magnet, which is magnetized and driven by the rotating magnetic field formed by the armature coil (stator) placed opposite to it, reduces speed fluctuations. Therefore, it is considered ideal to have a sinusoidal distribution in the circumferential direction.
従来のロータマグネットは第1図に示すように等厚の中
空円板状永久磁石板を使用し、これを着磁器にはさんで
磁化して形成しているが、前述の磁束密度分布に正弦波
曲線を得るための着磁器のヨーク形状の設計や励磁コイ
ル電流の制御などは非常に難かしく、実際には第2図に
示すように正弦波からはかなりずれた分布曲線のものし
か得られなかった。As shown in Figure 1, conventional rotor magnets are formed by using hollow circular permanent magnet plates of equal thickness and magnetizing them by sandwiching them between magnetizers. It is extremely difficult to design the yoke shape of the magnetizer and control the excitation coil current in order to obtain a wave curve, and in reality, the only way to obtain a distribution curve is one that deviates considerably from a sine wave, as shown in Figure 2. There wasn't.
第2図は従来のロータマグネットの円周方向の断面図(
、)と、これに対応する位置の表面磁束密度の分布曲線
(b)を示すもので、1はロータマグネット、2は理想
とされる正弦波曲線、3は実際の分布曲線、φは回転角
、Bは表面磁束密度である。Figure 2 is a circumferential cross-sectional view of a conventional rotor magnet (
) and the distribution curve (b) of the surface magnetic flux density at the corresponding position, where 1 is the rotor magnet, 2 is the ideal sine wave curve, 3 is the actual distribution curve, and φ is the rotation angle. , B is the surface magnetic flux density.
本発明の目的は上記のような欠点を除去したロータマグ
ネットを提供することにある。An object of the present invention is to provide a rotor magnet that eliminates the above-mentioned drawbacks.
上記の目的を達成するため本発明p−タマグネットは、
表側板面が平面で裏側板面が曲面からなリ、上記表側板
面に垂直な方向に飽和磁化されてなる扇状永久磁石板片
と、上記磁石板片と同形同質だが逆方向に飽和磁化され
てなる扇状永久磁石板片とが、上記表側板面を一平面上
に揃えて円周方向に交互に位置して中空円板状に構成さ
れ、上記表側板面の表面磁束密度分布が円周方向におい
て正弦波曲線になるようにしたものである。In order to achieve the above object, the p-ta magnet of the present invention has the following features:
A fan-shaped permanent magnet plate whose front plate surface is flat and whose back plate surface is curved and is saturated magnetized in the direction perpendicular to the front plate surface; fan-shaped permanent magnet plates are arranged alternately in the circumferential direction with the front plate surfaces aligned on one plane to form a hollow disk shape, and the surface magnetic flux density distribution of the front plate surfaces is arranged circumferentially. It is designed to form a sinusoidal curve in the direction.
次に本発明の実施例について説明する。Next, examples of the present invention will be described.
第3図は本発明ロータマグネットの一実施例を示す斜視
図で、4は例えばプラスチック磁石で形成された扇形永
久磁石板片で、その下側板面が平面で上側板面が曲面か
らなり、上記下側板面に垂直な方向に飽和磁化されてい
る。5は磁石板片4と同形同質だが逆方向に飽和磁化さ
れてなる磁石板片で、この二種類の磁石板片をその下側
板面を一平面上に揃えるようにして円周方向に順次交互
に位置させて中空円板状に構成したものである。FIG. 3 is a perspective view showing an embodiment of the rotor magnet of the present invention, and 4 is a sector-shaped permanent magnet plate made of, for example, a plastic magnet, the lower plate surface of which is flat and the upper plate surface of which is curved. It is saturated magnetized in the direction perpendicular to the lower plate surface. Reference numeral 5 indicates a magnet plate piece having the same shape and the same quality as the magnet plate piece 4, but which is saturated magnetized in the opposite direction. It is located in the shape of a hollow disk.
上記下側板面はモータの中でステータに対向する面にす
るので機能的には表側板面と言える。Since the lower plate surface is the surface facing the stator in the motor, it can be functionally called the front plate surface.
上記上側板面の曲面の形状は板厚を次のようにとること
により決定される。The shape of the curved surface of the upper plate surface is determined by determining the plate thickness as follows.
板面に垂直に飽和磁化された同一材質の永久磁石板の厚
さ1のときの表面磁束密度II′b(1)は第4図のよ
うな曲線で示され、回転角φにおける上記磁石板片の厚
さ?1(φ)が
′E1(φ)=Aeinφ/yb(1) (A +定
数)となるように上側板面の曲面が決定される。The surface magnetic flux density II'b(1) when the thickness of a permanent magnet plate of the same material, which is saturation magnetized perpendicular to the plate surface, is 1 is shown by a curve as shown in Fig. 4. Thickness of the piece? The curved surface of the upper plate surface is determined so that 1(φ) becomes 'E1(φ)=Aeinφ/yb(1) (A + constant).
こうすることにより上記中空円板状レータマグネットの
下側(表側)板面の表面磁束密度の円周方向の分布状態
は第5図に示すようになる。第5図(、)は本発明ロー
タマグネット乙の円周方向断面図、(b)はこれに対応
する位置の下側(表側)板面の表面磁束密度の分布曲線
で、理想的な正弦波を示している。磁化方向が逆転する
境界は板厚が最も薄い部分であるから正確に形成されや
すく、このことが正弦波分布の得られやすい条件になっ
ている。By doing so, the distribution state of the surface magnetic flux density in the circumferential direction on the lower (front) plate surface of the hollow disc-shaped rotor magnet becomes as shown in FIG. Figure 5 (,) is a circumferential cross-sectional view of the rotor magnet B of the present invention, and (b) is a distribution curve of the surface magnetic flux density of the lower (front) plate surface at the corresponding position, which is an ideal sine wave. It shows. Since the boundary where the magnetization direction is reversed is the thinnest part of the plate, it is easy to form it accurately, and this is a condition that makes it easy to obtain a sinusoidal distribution.
本発明ロータマグネットに使用する着磁器は、従来のよ
うに正弦波磁束密度分布を得るための特殊な磁場を形成
する必要がなく、単純な飽和磁場を形成してやればよい
ので非常に簡単に準備できる。The magnetizer used in the rotor magnet of the present invention does not need to create a special magnetic field to obtain a sinusoidal magnetic flux density distribution as in the past, and can be prepared very easily because it only needs to create a simple saturation magnetic field. .
又、本発明ロータマグネットは各磁石板片を別々に形成
したのち中空円板状に一本化してなるもの、或いは最初
から中空円板状に一体化成形してなるもののいずれでも
かまわない。プラスチック磁石材などを用いて各磁石板
片が別々に形成される場合は、磁場中成型により飽和磁
化されて別設の着磁器の使用が省略でき、又、各磁石板
片の一体化は超音波溶接や高周波溶接などにより変形を
伴なわずに接合可能である。Further, the rotor magnet of the present invention may be formed by forming each magnet plate piece separately and then integrating them into a hollow disk shape, or may be formed by integrally molding them into a hollow disk shape from the beginning. When each magnet plate piece is formed separately using a plastic magnet material, etc., it is saturated magnetized by molding in a magnetic field, and the use of a separate magnetizer can be omitted, and the integration of each magnet plate piece is extremely easy. They can be joined without deformation by sonic welding or high-frequency welding.
本発明ロータマグネットには回転時の空気抵抗を減らす
ためと補強の目的を兼ねて、第6図に示すように無着磁
の内周リング7や外周リング8を付設してもよく、又、
曲面を有する上側板面にはバックヨークや非磁性カバー
板を垣ねでもよい。The rotor magnet of the present invention may be provided with a non-magnetized inner ring 7 and outer ring 8, as shown in FIG. 6, for the purpose of reducing air resistance during rotation and for reinforcement purposes.
A back yoke or a non-magnetic cover plate may be placed around the curved upper plate surface.
以上の説明から明らかなように、本発明によれば板面に
垂直な方向に磁化されて且つ円周方向の表面磁束密度分
布が正弦波状のロータマグネットが確実に、しかも簡単
に得られ、その産業上の利(5)
用効果は極めて高い。As is clear from the above description, according to the present invention, a rotor magnet that is magnetized in the direction perpendicular to the plate surface and has a sinusoidal surface magnetic flux density distribution in the circumferential direction can be obtained reliably and easily. Industrial Use (5) The effects of use are extremely high.
第1図及び第2図は従来の四−タマグネットの説明図、
第3図及び第5図、第6図は本発明p−タマグネットの
説明図、第4図は板厚対表面磁束密度関係曲線図である
。
1的・従来のロータマグネット、2争軸正弦波分布曲線
、3…実際の分布曲線、4.5・軸層状永久磁石板片、
611・・本発明ロータマグネット、7拳軸内周リング
、8・・争外周リング。
代理人 弁理士 永田武三部
(6)Figures 1 and 2 are explanatory diagrams of conventional four-ta magnets,
FIG. 3, FIG. 5, and FIG. 6 are explanatory diagrams of the p-ta magnet of the present invention, and FIG. 4 is a diagram showing the relationship between plate thickness and surface magnetic flux density. 1. Conventional rotor magnet, 2. Axis sinusoidal distribution curve, 3. Actual distribution curve, 4.5. Axial layered permanent magnet plate piece.
611: Rotor magnet of the present invention, 7: Inner circumferential ring of fist shaft, 8: Outer circumferential ring. Agent: Patent attorney Takezo Nagata (6)
Claims (1)
面に垂直な方向に飽和磁化されてなる扇状永久磁石板片
と、上記磁石板片と同形同質だが逆方向に飽和磁化され
てなる扇状永久磁石板片とが、上記表側板面を一平面上
に揃えて円周方向に交互に位置して中空円板状に構成さ
れることを特徴とするロータマグネット。A fan-shaped permanent magnet plate whose front plate surface is flat and whose back plate surface is curved and is saturated magnetized in a direction perpendicular to the front plate surface; A rotor magnet characterized in that the fan-shaped permanent magnet plate pieces are arranged alternately in the circumferential direction with the front plate surfaces aligned on one plane and configured in the shape of a hollow disk.
Priority Applications (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP57050570A JPS58170347A (en) | 1982-03-29 | 1982-03-29 | Rotor magnet |
Applications Claiming Priority (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP57050570A JPS58170347A (en) | 1982-03-29 | 1982-03-29 | Rotor magnet |
Publications (1)
Publication Number | Publication Date |
---|---|
JPS58170347A true JPS58170347A (en) | 1983-10-06 |
Family
ID=12862656
Family Applications (1)
Application Number | Title | Priority Date | Filing Date |
---|---|---|---|
JP57050570A Pending JPS58170347A (en) | 1982-03-29 | 1982-03-29 | Rotor magnet |
Country Status (1)
Country | Link |
---|---|
JP (1) | JPS58170347A (en) |
Cited By (4)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
WO2002023701A1 (en) * | 2000-09-18 | 2002-03-21 | S.H.R. Limited Bvi | Synchronous machine with permanent magnets |
JP2007215291A (en) * | 2006-02-08 | 2007-08-23 | Honda Motor Co Ltd | Rotor for motor |
WO2017098094A1 (en) * | 2015-12-10 | 2017-06-15 | Whylot Sas | Rotor of an axial-flow electromagnetic motor having a corrugated-shape integral magnet |
GB2589582A (en) * | 2019-12-02 | 2021-06-09 | Peter Devereux Christopher | Electrical generator |
Citations (1)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
JPS5553164A (en) * | 1978-10-14 | 1980-04-18 | Sony Corp | Permanent magnet rotor |
-
1982
- 1982-03-29 JP JP57050570A patent/JPS58170347A/en active Pending
Patent Citations (1)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
JPS5553164A (en) * | 1978-10-14 | 1980-04-18 | Sony Corp | Permanent magnet rotor |
Cited By (6)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
WO2002023701A1 (en) * | 2000-09-18 | 2002-03-21 | S.H.R. Limited Bvi | Synchronous machine with permanent magnets |
JP2007215291A (en) * | 2006-02-08 | 2007-08-23 | Honda Motor Co Ltd | Rotor for motor |
WO2017098094A1 (en) * | 2015-12-10 | 2017-06-15 | Whylot Sas | Rotor of an axial-flow electromagnetic motor having a corrugated-shape integral magnet |
FR3045233A1 (en) * | 2015-12-10 | 2017-06-16 | Whylot | ROTOR OF AN AXIAL FLUX ELECTROMAGNETIC MOTOR HAVING AT LEAST ONE WAVED FORM MAGNET |
GB2589582A (en) * | 2019-12-02 | 2021-06-09 | Peter Devereux Christopher | Electrical generator |
GB2589582B (en) * | 2019-12-02 | 2021-12-08 | Peter Devereux Christopher | Electrical generator |
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