JPH11308824A - Magnetization method of permanent magnet - Google Patents

Magnetization method of permanent magnet

Info

Publication number
JPH11308824A
JPH11308824A JP11466298A JP11466298A JPH11308824A JP H11308824 A JPH11308824 A JP H11308824A JP 11466298 A JP11466298 A JP 11466298A JP 11466298 A JP11466298 A JP 11466298A JP H11308824 A JPH11308824 A JP H11308824A
Authority
JP
Japan
Prior art keywords
permanent magnet
yoke
magnetized
magnetizing
auxiliary yoke
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
JP11466298A
Other languages
Japanese (ja)
Inventor
Masafumi Kumoi
將文 雲井
Kenichi Watanabe
健一 渡邉
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.)
Panasonic Holdings Corp
Original Assignee
Matsushita Electric Industrial Co Ltd
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 Matsushita Electric Industrial Co Ltd filed Critical Matsushita Electric Industrial Co Ltd
Priority to JP11466298A priority Critical patent/JPH11308824A/en
Publication of JPH11308824A publication Critical patent/JPH11308824A/en
Pending legal-status Critical Current

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  • Permanent Field Magnets Of Synchronous Machinery (AREA)

Abstract

PROBLEM TO BE SOLVED: To provide a magnetization method and magnetization device of a permanent magnet by which a perfect magnetization level intensity is achieved, while a waveform for magnetization such as a sine wave, etc., is controlled. SOLUTION: Protruding parts 16a and recessed parts 16b are provided on the surface of an auxiliary yoke 12 on a permanent magnet side material 11. A magnetization yoke 13 is provided on the side of the permanent magnet material 11 opposite to the side facing the auxiliary yoke 12. As a result of this constitution, The magnetism inducing direction of a whole magnet can be controlled by the positions of the protruding parts 16a and angles between the protruding parts 16a in a circumferential direction, so that an arbitrary waveform such as a sine wave, etc., of a magnetic flux density can be obtained without causing decline in a magnetization intensity.

Description

【発明の詳細な説明】DETAILED DESCRIPTION OF THE INVENTION

【0001】[0001]

【発明の属する技術分野】本発明は、モータ等のアクチ
ュエータに使用される永久磁石の着磁方法に関するもの
である。
The present invention relates to a method for magnetizing a permanent magnet used in an actuator such as a motor.

【0002】[0002]

【従来の技術】従来の永久磁石の着磁方法は、磁石材を
完全着磁状態にする場合は、着磁磁界を発生するための
着磁コイルが巻回された着磁ヨークに加えて、着磁対象
である永久磁石材を挟んで反対側の位置に、磁性体で構
成された補助ヨークが配置されていた。上記補助ヨーク
は、着磁ヨークで発生した着磁磁界を磁石材の深部まで
引き込む役割をはたしており、上記補助ヨークにより、
磁石材の全領域にわたって磁化を誘起させ、磁石材が持
つ最大限のレベルまで着磁することが可能となる。すな
わち、磁石材を完全着磁状態にすることができるが、こ
の時、上記永久磁石がモータに組まれた時にモータの空
隙内に発生させる磁束密度は必然的に台形波または矩形
波形状になった。
2. Description of the Related Art A conventional method of magnetizing a permanent magnet includes a magnetizing yoke in which a magnetizing coil for generating a magnetizing magnetic field is wound in order to completely magnetize a magnet material. An auxiliary yoke made of a magnetic material is arranged at a position opposite to the permanent magnet material to be magnetized. The auxiliary yoke serves to draw the magnetizing magnetic field generated by the magnetized yoke to a deep portion of the magnet material.
It is possible to induce magnetization over the entire region of the magnet material and magnetize it to the maximum level of the magnet material. That is, the magnet material can be completely magnetized, but at this time, the magnetic flux density generated in the air gap of the motor when the permanent magnet is assembled to the motor necessarily has a trapezoidal or rectangular wave shape. Was.

【0003】よって、例えば、モータの空隙内に発生す
る磁束密度波形を正弦波状にしたい場合は、前記補助ヨ
ークを取り除き、着磁磁界が磁石材の深部まで流れにく
くしていた。
Therefore, for example, when it is desired to make the magnetic flux density waveform generated in the air gap of the motor into a sine wave shape, the auxiliary yoke is removed to make it difficult for the magnetizing magnetic field to flow deep into the magnet material.

【0004】以上のように従来の着磁方法では、着磁後
の磁石表面磁束密度波形を使用するモータ等の電気機器
に所望な波形にしようとした場合、磁石材を部分的に着
磁させる必要があった。
As described above, in the conventional magnetizing method, when a desired magnetic waveform is applied to an electric device such as a motor using a magnet surface magnetic flux density waveform after magnetizing, the magnet material is partially magnetized. Needed.

【0005】[0005]

【発明が解決しようとする課題】しかしながら、上記の
方法で磁石材を正弦波着磁する場合、磁石材を部分的に
着磁させることになり、完全着磁した場合と比較して、
永久磁石が発生する磁束量が減少する課題があった。
However, when the sine-wave magnetizing of the magnet material is performed by the above-described method, the magnet material is partially magnetized.
There is a problem that the amount of magnetic flux generated by the permanent magnet is reduced.

【0006】本発明は、このような従来の課題を解決す
るものであり、正弦波形着磁などの波形制御をしつつ、
完全着磁レベルの強度する永久磁石の着磁方法及び着磁
装置を提供することを目的とする。
The present invention is to solve such a conventional problem, and performs waveform control such as sine waveform magnetization.
It is an object of the present invention to provide a method and apparatus for magnetizing a permanent magnet having a strength of a complete magnetization level.

【0007】[0007]

【課題を解決するための手段】上記の課題を解決するた
めに本発明は、着磁コイル線をスロットに配設した着磁
ヨークと、永久磁石材を挟んで前記着磁ヨークと反対側
に位置する補助ヨークとを備え、前記永久磁石材に面す
る補助ヨークには凹凸部を設けた状態で着磁する永久磁
石の着磁方法であり、磁石材の全領域を最適な状態に着
磁することができ、例えば正弦波形着磁に代表される任
意な波形制御を行った時に生じる着磁強度の低下を解消
することができる。
SUMMARY OF THE INVENTION In order to solve the above-mentioned problems, the present invention provides a magnetized yoke having a magnetized coil wire disposed in a slot, and a magnetized yoke opposite to the magnetized yoke across a permanent magnet material. An auxiliary yoke that is positioned, and the auxiliary yoke facing the permanent magnet material is a method of magnetizing a permanent magnet in which the auxiliary yoke is provided with an uneven portion, and the entire region of the magnet material is magnetized in an optimal state. For example, it is possible to eliminate a decrease in the magnetization intensity that occurs when arbitrary waveform control represented by, for example, a sine waveform magnetization is performed.

【0008】[0008]

【発明の実施の形態】本発明は、着磁コイル線をスロッ
トに配設した着磁ヨークと、永久磁石材を挟んで前記着
磁ヨークと反対側に位置する補助ヨークとを備え、前記
永久磁石に面する補助ヨークには凹凸部を設けた状態で
着磁する永久磁石の着磁方法である。
DETAILED DESCRIPTION OF THE PREFERRED EMBODIMENTS The present invention comprises a magnetized yoke having a magnetized coil wire disposed in a slot, and an auxiliary yoke located on the opposite side of the magnetized yoke with a permanent magnet material interposed therebetween. This is a method of magnetizing a permanent magnet that is magnetized in a state in which the auxiliary yoke facing the magnet is provided with an uneven portion.

【0009】また、永久磁石材と補助ヨークの凸部とを
密着した構成である。また、着磁ヨークのスロットに対
向する位置に補助ヨークの凹部を設けた構成である。
Further, the structure is such that the permanent magnet material and the projection of the auxiliary yoke are in close contact with each other. Further, the configuration is such that a concave portion of the auxiliary yoke is provided at a position facing the slot of the magnetized yoke.

【0010】また、着磁ヨークのスロットに対向する位
置に補助ヨークの凸部を設けた構成である。
[0010] Further, a projection of the auxiliary yoke is provided at a position facing the slot of the magnetized yoke.

【0011】また、補助ヨークの凸部を永久磁石材と密
着させた構成である。また、補助ヨークの凸部と永久磁
石材と所定の空隙を持たせた構成である。
[0011] Further, the auxiliary yoke has a configuration in which the convex portion is brought into close contact with the permanent magnet material. Further, the auxiliary yoke has a configuration in which a convex portion, a permanent magnet material, and a predetermined gap are provided.

【0012】また、着磁ヨークのスロットと同一法線上
に補助ヨークの凹部を設け、かつ補助ヨークの凸部の比
率を0.8以上にした構成である。
Further, the auxiliary yoke is provided with a concave portion on the same normal line as the slot of the magnetized yoke, and the ratio of the convex portion of the auxiliary yoke is set to 0.8 or more.

【0013】また、着磁ヨークのスロットと同一法線上
に補助ヨークの凸部を設け、かつ補助ヨーク凹部の比率
を0.3以上にした構成である。
[0013] Further, the auxiliary yoke is provided on the same normal line as the slot of the magnetized yoke, and the ratio of the auxiliary yoke recess is set to 0.3 or more.

【0014】また、補助ヨークを磁性体である金属体で
構成した構成である。また、補助ヨークを磁性体である
薄板材を積層構造にて構成したものである。
Further, the auxiliary yoke is made of a magnetic metal. Further, the auxiliary yoke is made of a thin plate made of a magnetic material and has a laminated structure.

【0015】このように、補助ヨークに凹凸部を設けた
ものでは、補助ヨークの凸部に着磁磁界を誘導すること
ができ、凸部の位置、大きさに応じて、着磁コイルによ
り発生する着磁磁界の方向を制御することが可能であ
り、目的とする方向に磁石材中の磁気モーメントとを誘
起させ回転させる結果、永久磁石の着磁方向と着磁強度
を任意にコントロールすることが可能となり、最終的に
任意形状の着磁が実現できる。
As described above, with the auxiliary yoke provided with the concavo-convex portion, a magnetizing magnetic field can be induced in the convex portion of the auxiliary yoke and generated by the magnetizing coil in accordance with the position and size of the convex portion. It is possible to control the direction and direction of magnetization of the permanent magnet as a result of inducing and rotating the magnetic moment in the magnet material in the desired direction. , And finally an arbitrary shape of magnetization can be realized.

【0016】また、着磁ヨークのスロットに対向する位
置に補助ヨークの凹部を設けることにより、正弦波形着
磁が可能である。
Further, by providing a concave portion of the auxiliary yoke at a position facing the slot of the magnetized yoke, it is possible to magnetize a sinusoidal waveform.

【0017】また、着磁ヨークのスロットに対向する位
置に補助ヨークの凸部を設けることにより、台形波形ま
たは矩形波形着磁が可能である。
By providing a projection of the auxiliary yoke at a position facing the slot of the magnetized yoke, trapezoidal waveform or rectangular waveform magnetization is possible.

【0018】また、補助ヨークに凹凸を設け、かつ補助
ヨークを磁性体で積層した構成することにより、着磁磁
界に誘導される補助ヨーク内の渦電流を低減でき、着磁
磁界を効率良く利用でき、省エネルギーで着磁が可能で
ある。
Further, by providing the auxiliary yoke with irregularities and laminating the auxiliary yoke with a magnetic material, the eddy current in the auxiliary yoke induced by the magnetization magnetic field can be reduced, and the magnetization magnetic field can be used efficiently. It can be magnetized with energy saving.

【0019】また、補助ヨークに凹凸を設けたもので
は、着磁磁界の磁路を高精度に決定することができるた
め、ばらつきの無い極めて安定な永久磁石の着磁が可能
である。
In the case where the auxiliary yoke is provided with irregularities, the magnetic path of the magnetizing magnetic field can be determined with high accuracy, so that extremely stable permanent magnet magnetization with no variation is possible.

【0020】[0020]

【実施例】(実施例1)図1は、本発明の第1の実施例
における永久磁石の着磁方法を示したものである。
(Embodiment 1) FIG. 1 shows a method of magnetizing a permanent magnet according to a first embodiment of the present invention.

【0021】図1において、11は永久磁石材、12は
補助ヨーク、13は着磁ヨークである。永久磁石材11
は着磁ヨーク13と所定の空隙を設けて配置されてい
る。着磁ヨーク13は電磁鋼板や純鉄等の磁性材で構成
されており、また前記着磁ヨーク13には、着磁コイル
14が1ターン以上巻回されており、前記着磁コイル1
4を着磁電源に接続することで、永久磁石材11を着磁
させる着磁磁界を発生させている。
In FIG. 1, reference numeral 11 denotes a permanent magnet material, 12 denotes an auxiliary yoke, and 13 denotes a magnetized yoke. Permanent magnet material 11
Are arranged with a predetermined gap from the magnetized yoke 13. The magnetized yoke 13 is made of a magnetic material such as an electromagnetic steel plate or pure iron. The magnetized yoke 13 is wound with a magnetized coil 14 for at least one turn.
4 is connected to a magnetizing power supply to generate a magnetizing magnetic field for magnetizing the permanent magnet material 11.

【0022】補助ヨーク12は、電磁鋼板や純鉄等の磁
性材で構成されており、永久磁石材11を介して着磁ヨ
ーク13と反対側に配置してある。補助ヨーク12の永
久磁石材11側の面上には凸部16a,凹部16bが設
けられており、前記凸部16aは永久磁石材11と所定
のギャップを介して配設されている。補助ヨーク12
は、凸部16aの中心は、着磁ヨーク13に設けている
スロット、すなわち着磁コイル14の中心と同一法線上
に配設されている。
The auxiliary yoke 12 is made of a magnetic material such as an electromagnetic steel plate or pure iron, and is disposed on the side opposite to the magnetized yoke 13 via the permanent magnet material 11. A projection 16a and a recess 16b are provided on the surface of the auxiliary yoke 12 on the permanent magnet material 11 side, and the projection 16a is arranged with the permanent magnet material 11 via a predetermined gap. Auxiliary yoke 12
The center of the convex portion 16a is disposed on the same normal line as the center of the slot provided in the magnetized yoke 13, that is, the center of the magnetized coil 14.

【0023】以上のように構成された本実施例における
永久磁石の着磁方法について説明する。
A description will be given of a method of magnetizing the permanent magnet according to the present embodiment configured as described above.

【0024】着磁コイル14に電流を通電させることで
発生した着磁磁界は、永久磁石材11を横切り、補助ヨ
ーク12の方向へ流れる。このとき、着磁ヨーク13か
らみて、凸部16aは磁気抵抗が低く、反対に凹部16
bは磁気抵抗が高くなっている。したがって、前記着磁
磁界は、凹部16bよりも凸部16aの方に流れやすく
なる。永久磁石材11の着磁状態は、前記着磁磁界の分
布に依存することから、永久磁石材11は凸部16aの
位置、大きさにより決定することになる。
A magnetizing magnetic field generated by applying a current to the magnetizing coil 14 crosses the permanent magnet material 11 and flows in the direction of the auxiliary yoke 12. At this time, when viewed from the magnetized yoke 13, the protrusion 16a has a low magnetic resistance, and
b has a high magnetic resistance. Therefore, the magnetizing magnetic field is more likely to flow to the convex portion 16a than to the concave portion 16b. Since the magnetized state of the permanent magnet material 11 depends on the distribution of the magnetizing magnetic field, the permanent magnet material 11 is determined by the position and the size of the projection 16a.

【0025】図1に示す本実施例の場合、永久磁石11
が着磁ヨーク13側の表面に生成する磁束密度分布は、
台形波形状になる。ちなみに、本実施例において、台形
波形状に着磁する場合、凸部16aと凹部16bにおけ
る円周方向の角度幅の比率を8:2にするか、あるいは
凸部16aの比率を8より大きくすると良い。
In the case of this embodiment shown in FIG.
The magnetic flux density distribution generated on the surface of the magnetized yoke 13 by
It has a trapezoidal wave shape. Incidentally, in the present embodiment, when magnetizing in a trapezoidal wave shape, the ratio of the angular width in the circumferential direction between the convex portion 16a and the concave portion 16b is set to 8: 2, or the ratio of the convex portion 16a is made larger than 8. good.

【0026】さらに、上記着磁された永久磁石材11を
モータに組み込んだ場合、凸部16aと凹部16bの位
置、大きさにより、モータのエアギャップ中の磁束密度
波形を自由に設計できる。また、本実施例では、永久磁
石内部の全磁化を最適な方向、強度に着磁できるので、
永久磁石材固有の性能を最大限利用できる。本実施例に
おいては、着磁磁界は永久磁石材11を完全着磁するの
に十分な大きさとすると、本発明の効果はより確実に得
られる。
Further, when the magnetized permanent magnet material 11 is incorporated in a motor, the magnetic flux density waveform in the air gap of the motor can be freely designed depending on the positions and sizes of the convex portions 16a and the concave portions 16b. Further, in this embodiment, since the entire magnetization inside the permanent magnet can be magnetized in the optimal direction and strength,
The performance inherent in permanent magnet materials can be used to the maximum. In the present embodiment, the effect of the present invention can be more reliably obtained if the magnetizing magnetic field is set to be large enough to completely magnetize the permanent magnet material 11.

【0027】なお、凸部16a及び凹部16bの法線方
向の深さは着磁ヨーク13と補助ヨーク12との最小距
離と同じ、あるいはそれ以上あれば十分である。また、
凸部16a及び凹部16bの形状は、法線方向の深さ、
及び円周方向の角度幅の比率が、前記した値である限
り、特に制限はない。
It is sufficient that the depth of the convex portion 16a and the concave portion 16b in the normal direction is equal to or longer than the minimum distance between the magnetized yoke 13 and the auxiliary yoke 12. Also,
The shape of the convex portion 16a and the concave portion 16b is the depth in the normal direction,
There is no particular limitation as long as the ratio of the angular width in the circumferential direction is the above-mentioned value.

【0028】なお、本実施例では凸部16aと永久磁石
材11間に所定のギャップを設けているが、必ずしもこ
の限りではなく、凸部16aと永久磁石材11とを密着
させてもかまわない。
In this embodiment, a predetermined gap is provided between the convex portion 16a and the permanent magnet material 11. However, the present invention is not limited to this, and the convex portion 16a and the permanent magnet material 11 may be in close contact. .

【0029】(実施例2)図2は、本発明の第2の実施
例における永久磁石の着磁方法を示したものである。
(Embodiment 2) FIG. 2 shows a method of magnetizing a permanent magnet according to a second embodiment of the present invention.

【0030】図2において、補助ヨーク12に設けてい
る凸部16aの中心は、着磁コイル14の中心と同一法
線上に配置されている。
In FIG. 2, the center of the projection 16a provided on the auxiliary yoke 12 is arranged on the same normal line as the center of the magnetized coil 14.

【0031】以上のように構成された本実施例における
永久磁石の着磁方法によれば、凸部16aの方向へ着磁
磁界が流れやすくなり、永久磁石材11内の磁気モーメ
ントは、着磁後の表面磁束密度波形が正弦波形になるよ
うに最適な方向に誘導できる。この時、凸部16a、凹
部16bにおける周方向の角度幅の比率を3:7にする
か、もしくは凸部16aの比率を3以上にすればよい。
According to the method of magnetizing the permanent magnet in the present embodiment configured as described above, the magnetizing magnetic field easily flows in the direction of the convex portion 16a, and the magnetic moment in the permanent magnet material 11 is It can be guided in an optimal direction so that the subsequent surface magnetic flux density waveform becomes a sine waveform. At this time, the ratio of the angular width in the circumferential direction between the convex portion 16a and the concave portion 16b may be set to 3: 7, or the ratio of the convex portion 16a may be set to 3 or more.

【0032】なお、本発明においては、永久磁石の内周
側を着磁し、永久磁石の外周側と補助ヨークとに空隙を
設けた構成について説明したが、必ずしもこの限りでは
ない。例えば、永久磁石の外周側を着磁し、永久磁石の
内周側に補助ヨークを配置し、前記補助ヨークに凹凸を
設けた構成でも本発明は適用できることは言うまでもな
い。
Although the present invention has been described with respect to a configuration in which the inner peripheral side of the permanent magnet is magnetized and a gap is provided between the outer peripheral side of the permanent magnet and the auxiliary yoke, the present invention is not limited to this. For example, it goes without saying that the present invention can be applied to a configuration in which the outer peripheral side of the permanent magnet is magnetized, the auxiliary yoke is arranged on the inner peripheral side of the permanent magnet, and the auxiliary yoke is provided with irregularities.

【0033】また、永久磁石材はリング形状である必要
はない。例えば、C型の磁石を複数個用いることで、リ
ング状に配置しても構わない。永久磁石材の材質も制約
はなく本発明を適用できる。また、着磁ヨーク及び補助
ヨークは磁性材料であれば特に制約はない。さらに、着
磁ヨーク及び補助ヨークは積層構造でも、非積層構造で
も構わない。
The permanent magnet material does not need to be ring-shaped. For example, a plurality of C-shaped magnets may be used and arranged in a ring shape. There is no limitation on the material of the permanent magnet material, and the present invention can be applied. The magnetized yoke and the auxiliary yoke are not particularly limited as long as they are magnetic materials. Further, the magnetized yoke and the auxiliary yoke may have a laminated structure or a non-laminated structure.

【0034】[0034]

【発明の効果】本願請求項1記載の発明は、補助ヨーク
に凹凸を設けたので、磁束密度波形を任意波形に自由に
設計できる。また、永久磁石内部の全磁化を最適な方
向、強度に着磁できるので、永久磁石材固有の性能を最
大限利用できる効果があると共に、着磁磁界の省エネル
ギー化が図れ、着磁設備の小型化にもつながる。また、
補助ヨークに凹凸を設けたものでは、着磁磁界の磁路を
高精度に決定することができるため、ばらつきの無い極
めて安定な永久磁石の着磁が可能である。
According to the first aspect of the present invention, since the auxiliary yoke is provided with irregularities, the magnetic flux density waveform can be freely designed to have an arbitrary waveform. In addition, since the entire magnetization inside the permanent magnet can be magnetized in the optimal direction and strength, the performance unique to the permanent magnet material can be used to the maximum, and the energy of the magnetizing magnetic field can be reduced. Also leads to Also,
When the auxiliary yoke is provided with irregularities, the magnetic path of the magnetizing magnetic field can be determined with high accuracy, and therefore, extremely stable permanent magnet magnetization without variation is possible.

【0035】また、請求項2記載の実施例によれば、永
久磁石の表面磁束密度波形を台形波状にすることができ
る。
According to the embodiment of the present invention, the surface magnetic flux density waveform of the permanent magnet can be formed into a trapezoidal waveform.

【0036】また、請求項3記載の実施例によれば、永
久磁石の表面磁束密度波形を正弦波状にすることができ
る。特に、磁束密度の強度を台形波・矩形波にした時と
比べて低下することなく、正弦波形着磁が可能となる。
よって、着磁された永久磁石をモータに用いた場合、モ
ータの出力を低下させること無く、モータのエアギャッ
プを正弦波状にすることができ、トルク脈動の小さい、
低振動なモータを実現することができる。
According to the third embodiment, the surface magnetic flux density waveform of the permanent magnet can be made sinusoidal. In particular, it is possible to perform sine waveform magnetization without lowering the intensity of the magnetic flux density than when trapezoidal or rectangular waves are used.
Therefore, when the magnetized permanent magnet is used for the motor, the air gap of the motor can be made sinusoidal without lowering the output of the motor, and the torque pulsation is small.
A low-vibration motor can be realized.

【0037】また、請求項4記載の実施例によれば、補
助ヨークの凸部と永久磁石材とを密着できるため、必要
とする着磁磁界の大きさを最低減におさめることができ
る。
Further, according to the embodiment of the present invention, since the projection of the auxiliary yoke can be in close contact with the permanent magnet material, the required magnitude of the magnetizing magnetic field can be minimized.

【0038】また、請求項9記載の実施例によれば、磁
性体を積層構造にしているため、着磁磁界に誘導されて
補助ヨーク内に流れる渦電流の発生を抑えることがで
き、着磁磁界の大きさを最低減におさめることができ
る。
According to the ninth embodiment, since the magnetic body has a laminated structure, the generation of an eddy current induced in the magnetizing magnetic field and flowing in the auxiliary yoke can be suppressed. The magnitude of the magnetic field can be minimized.

【0039】また請求項11記載の実施例によれば、着
磁波形をモータの鉄心形状に応じて自在に設計できるた
め、モータで発生するコギングトルクを容易に低減でき
たり、モータの巻線での誘起電圧を巻線に通電される電
流波形に対して最適化できるため、トルクリップルの小
さい低振動なモータが実現できる。さらに、永久磁石材
を完全に着磁し、さらに、着磁波形を最適に制御できる
ため、モータの小型化を図れるとともに磁気損失の少な
い高効率なモータを実現できる。
According to the eleventh embodiment, since the magnetization waveform can be freely designed according to the shape of the iron core of the motor, the cogging torque generated in the motor can be easily reduced, and the winding of the motor can be reduced. Can be optimized with respect to the waveform of the current flowing through the winding, so that a low-vibration motor with small torque ripple can be realized. Further, since the permanent magnet material can be completely magnetized and the magnetization waveform can be optimally controlled, the motor can be reduced in size and a highly efficient motor with less magnetic loss can be realized.

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

【図1】本発明の第1の実施例を示す着磁方法を示す説
明図
FIG. 1 is an explanatory view showing a magnetizing method according to a first embodiment of the present invention.

【図2】本発明の第2の実施例を示す着磁方法を示す説
明図
FIG. 2 is an explanatory view showing a magnetizing method according to a second embodiment of the present invention.

【符号の説明】[Explanation of symbols]

11 永久磁石材 12 補助ヨーク 13 着磁ヨーク 14 着磁コイル 15 空隙 16a 凸部 16b 凸部 17 スロット Reference Signs List 11 permanent magnet material 12 auxiliary yoke 13 magnetized yoke 14 magnetized coil 15 air gap 16a convex portion 16b convex portion 17 slot

Claims (11)

【特許請求の範囲】[Claims] 【請求項1】 着磁コイル線をスロットに配設した着磁
ヨークと、永久磁石材を挟んで前記着磁ヨークと反対側
に位置する補助ヨークとを備え、前記永久磁石材に面す
る補助ヨークには凹凸部を設けた状態で着磁する永久磁
石の着磁方法。
1. A magnetized yoke having a magnetized coil wire disposed in a slot, and an auxiliary yoke located on the opposite side of the magnetized yoke with a permanent magnet material interposed therebetween, and an auxiliary yoke facing the permanent magnet material is provided. A method of magnetizing a permanent magnet that is magnetized in a state in which the yoke is provided with an uneven portion.
【請求項2】 着磁ヨークのスロットと同一法線上に補
助ヨークの凹部を設けた状態で着磁する請求項1記載の
永久磁石の着磁方法。
2. The method for magnetizing a permanent magnet according to claim 1, wherein the magnet is magnetized in a state in which a recess of the auxiliary yoke is provided on the same normal line as the slot of the magnetized yoke.
【請求項3】 着磁ヨークのスロットと同一法線上に補
助ヨークの凸部を設けた状態で着磁する請求項1記載の
永久磁石の着磁方法。
3. The method for magnetizing a permanent magnet according to claim 1, wherein the magnet is magnetized in a state where a projection of the auxiliary yoke is provided on the same normal line as a slot of the magnetized yoke.
【請求項4】 補助ヨークの凸部を永久磁石と密着させ
た状態で着磁を行う請求項1記載の永久磁石の着磁方
法。
4. The method for magnetizing a permanent magnet according to claim 1, wherein the magnetizing is performed in a state where the convex portion of the auxiliary yoke is in close contact with the permanent magnet.
【請求項5】 永久磁石と所定の空隙を持たせて補助ヨ
ークの凸部を配設した請求項1記載の永久磁石の着磁方
法。
5. The method for magnetizing a permanent magnet according to claim 1, wherein the convex portion of the auxiliary yoke is provided so as to have a predetermined gap with the permanent magnet.
【請求項6】 着磁ヨークのスロットと同一法線上に補
助ヨークの凹部を設け、かつ補助ヨークの凸部の比率を
0.8以上にした状態で着磁する請求項1記載の永久磁
石の着磁方法。
6. The permanent magnet according to claim 1, wherein the concave portion of the auxiliary yoke is provided on the same normal line as the slot of the magnetic yoke, and the ratio of the convex portion of the auxiliary yoke is set to 0.8 or more. Magnetization method.
【請求項7】 着磁ヨークのスロットと同一法線上に補
助ヨークの凸部を設け、かつ補助ヨーク凹部の比率を
0.3以上にした状態で着磁する請求項1記載の永久磁
石の着磁方法。
7. The permanent magnet as claimed in claim 1, wherein the auxiliary yoke is provided with a convex portion on the same normal line as the slot of the magnetic yoke and the ratio of the auxiliary yoke concave portion is set to 0.3 or more. Magnetic method.
【請求項8】 補助ヨークを磁性体である金属体で構成
した請求項1記載の永久磁石の着磁方法。
8. The method for magnetizing a permanent magnet according to claim 1, wherein the auxiliary yoke is made of a metal material that is a magnetic material.
【請求項9】 補助ヨークを磁性体である薄板材を積層
することにより構成した請求項1記載の永久磁石の着磁
方法。
9. The method for magnetizing a permanent magnet according to claim 1, wherein the auxiliary yoke is formed by laminating thin plates made of a magnetic material.
【請求項10】 請求項1記載の永久磁石の着磁方法に
より、永久磁石材を着磁したことを特徴とする永久磁
石。
10. A permanent magnet, wherein a permanent magnet material is magnetized by the method for magnetizing a permanent magnet according to claim 1.
【請求項11】 請求項1記載の永久磁石の着磁方法に
より、着磁された永久磁石を使用した光メディア用スピ
ンドルモータ。
11. A spindle motor for optical media using a permanent magnet magnetized by the method for magnetizing a permanent magnet according to claim 1.
JP11466298A 1998-04-24 1998-04-24 Magnetization method of permanent magnet Pending JPH11308824A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP11466298A JPH11308824A (en) 1998-04-24 1998-04-24 Magnetization method of permanent magnet

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP11466298A JPH11308824A (en) 1998-04-24 1998-04-24 Magnetization method of permanent magnet

Publications (1)

Publication Number Publication Date
JPH11308824A true JPH11308824A (en) 1999-11-05

Family

ID=14643443

Family Applications (1)

Application Number Title Priority Date Filing Date
JP11466298A Pending JPH11308824A (en) 1998-04-24 1998-04-24 Magnetization method of permanent magnet

Country Status (1)

Country Link
JP (1) JPH11308824A (en)

Cited By (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
CN107017711A (en) * 2017-03-21 2017-08-04 横店集团东磁股份有限公司 A kind of method for solving electric car cooling water pump rotor stall
JP2019212743A (en) * 2018-06-04 2019-12-12 株式会社ダイドー電子 Method of magnetizing multipolar magnet

Cited By (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
CN107017711A (en) * 2017-03-21 2017-08-04 横店集团东磁股份有限公司 A kind of method for solving electric car cooling water pump rotor stall
JP2019212743A (en) * 2018-06-04 2019-12-12 株式会社ダイドー電子 Method of magnetizing multipolar magnet

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