JPS58170347A - Rotor magnet - Google Patents

Rotor magnet

Info

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
Application number
JP57050570A
Other languages
Japanese (ja)
Inventor
Kichi Kaiba
佶 買場
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.)
Individual
Original Assignee
Individual
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 Individual filed Critical Individual
Priority to JP57050570A priority Critical patent/JPS58170347A/en
Publication of JPS58170347A publication Critical patent/JPS58170347A/en
Pending legal-status Critical Current

Links

Classifications

    • HELECTRICITY
    • H02GENERATION; CONVERSION OR DISTRIBUTION OF ELECTRIC POWER
    • H02KDYNAMO-ELECTRIC MACHINES
    • H02K1/00Details of the magnetic circuit
    • H02K1/06Details of the magnetic circuit characterised by the shape, form or construction
    • H02K1/22Rotating parts of the magnetic circuit
    • H02K1/27Rotor cores with permanent magnets
    • H02K1/2793Rotors axially facing stators
    • H02K1/2795Rotors axially facing stators the rotor consisting of two or more circumferentially positioned magnets

Abstract

PURPOSE:To make the surface magnetic flux density distribution of a rotor magnet in the circumferential direction to form sine wave by a method wherein sector shaped permanent magnets consisting of a plane plate face on the surface side and a curved plate face on the back side are arranged in the hollow disk type as to have different polarity alternately in the circumferential direction. CONSTITUTION:Sector shaped permanent magnet segments 4 consisting of the plane plate face on the surface side (lower side) and the curved plate face on the back side (upper side), and consisting of a plastic magnet (for example) saturatedly magnetized in the perpendicular direction to the plate face on the surface side, and the sector shaped permanent magnet segments 5 having the same shape and the same quality with the sector shaped permanent magnet segments 4 thereof and saturatedly magnetized in the opposite direction are put in order alternately in the circumferential direction placing the plate faces on the surface side on the same plane to constitute the hollow disk type. At this time, the curved surface of the plate face on the back side is decided as to make thicknesses of the respective fan type permanent magnet segments 4, 5 to be in a fixed function in the circumferential direction. Accordingly, surface magnetic flux density distribution of the plate face on the surface side is apt to form the sine wave, and moreover magnetization can be attained in a simply saturated magnetic field.

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.

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

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)

【特許請求の範囲】[Claims] 表側板面が平面で裏側板面が曲面からなり、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.
JP57050570A 1982-03-29 1982-03-29 Rotor magnet Pending JPS58170347A (en)

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)

* Cited by examiner, † Cited by third party
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)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS5553164A (en) * 1978-10-14 1980-04-18 Sony Corp Permanent magnet rotor

Patent Citations (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS5553164A (en) * 1978-10-14 1980-04-18 Sony Corp Permanent magnet rotor

Cited By (6)

* Cited by examiner, † Cited by third party
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

Similar Documents

Publication Publication Date Title
JP2695332B2 (en) Permanent magnet field type rotor
JP2799209B2 (en) Electric machine
US4745312A (en) Stepping motor
US4322648A (en) Permanent magnet motor armature
JPH0479741A (en) Permanent magnet rotor
US4725752A (en) 1-phase self starting disk-type brushless motor with cogging element
JPS58170347A (en) Rotor magnet
EP0266862A1 (en) Improved brushless D.C. dynamoelectric machine
JPS63140644A (en) Rotor with permanent magnet for rotary electric machine
JPS6122751A (en) Stepping motor
JPS6335155A (en) Motor
JP3228782U (en) Motor using permanent magnet
JPH0429529Y2 (en)
JPH0122390Y2 (en)
JPS61170265A (en) Synchronous motor
JP2017131034A (en) Magnetization method of lundell type rotor
JPH0398449A (en) Rotary electric machine
JPH0410655Y2 (en)
JPH0522917A (en) Direct current motor
JP2023116318A (en) Magnet, electric motor and manufacturing method of magnet
JPH02276431A (en) Rotary electric machine having rotor with permanent magnet
JPS61176977U (en)
JPH01253216A (en) Magnetizer
JPH04340352A (en) Manufacture of movable element of thin film magnet motor
JPS58222767A (en) Flat rotary electric machine