JPH10271723A - Permanent magnet field type rotating electric machine and method of manufacturing the same - Google Patents

Permanent magnet field type rotating electric machine and method of manufacturing the same

Info

Publication number
JPH10271723A
JPH10271723A JP9069570A JP6957097A JPH10271723A JP H10271723 A JPH10271723 A JP H10271723A JP 9069570 A JP9069570 A JP 9069570A JP 6957097 A JP6957097 A JP 6957097A JP H10271723 A JPH10271723 A JP H10271723A
Authority
JP
Japan
Prior art keywords
magnet
rotor
electric machine
rotating electric
stator
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
JP9069570A
Other languages
Japanese (ja)
Inventor
Masahiro Mita
正裕 三田
Fumio Kimura
文雄 木村
Toshiko Takahashi
俊子 高橋
Takashi Sasaki
崇 佐々木
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.)
Proterial Ltd
Original Assignee
Hitachi Metals 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 Hitachi Metals Ltd filed Critical Hitachi Metals Ltd
Priority to JP9069570A priority Critical patent/JPH10271723A/en
Publication of JPH10271723A publication Critical patent/JPH10271723A/en
Pending legal-status Critical Current

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Classifications

    • Y—GENERAL TAGGING OF NEW TECHNOLOGICAL DEVELOPMENTS; GENERAL TAGGING OF CROSS-SECTIONAL TECHNOLOGIES SPANNING OVER SEVERAL SECTIONS OF THE IPC; TECHNICAL SUBJECTS COVERED BY FORMER USPC CROSS-REFERENCE ART COLLECTIONS [XRACs] AND DIGESTS
    • Y02—TECHNOLOGIES OR APPLICATIONS FOR MITIGATION OR ADAPTATION AGAINST CLIMATE CHANGE
    • Y02T—CLIMATE CHANGE MITIGATION TECHNOLOGIES RELATED TO TRANSPORTATION
    • Y02T10/00—Road transport of goods or passengers
    • Y02T10/60—Other road transportation technologies with climate change mitigation effect
    • Y02T10/64—Electric machine technologies in electromobility

Landscapes

  • Permanent Field Magnets Of Synchronous Machinery (AREA)
  • Iron Core Of Rotating Electric Machines (AREA)
  • Permanent Magnet Type Synchronous Machine (AREA)

Abstract

(57)【要約】 【課題】 界磁用R−Fe−B磁石を良好に着磁可能な
永久磁石界磁型回転電機およびその製造方法を提供する
ことである。また、界磁用磁石として焼結磁石を用いた
場合において安価でかつ高性能を維持した永久磁石界磁
型回転電機を提供する。 【解決手段】 回転子コア内部にR−Fe−B磁石(R
はYを含めたNd,Dy等の希土類元素の1種または2
種以上)を有した内部磁石型回転子を備えた永久磁石界
磁型回転電機であって、前記回転子単独の状態における
R−Fe−B磁石のパーミアンス係数(Pcm)と残留
磁束密度(Br:kG)とが、(Pcm+1)>Br/
7 の関係を満たすことを特徴とする永久磁石界磁型回
転電機。
(57) [Problem] To provide a permanent magnet field type rotating electric machine capable of satisfactorily magnetizing a field R-Fe-B magnet and a method of manufacturing the same. Further, there is provided a permanent magnet field type rotating electric machine which is inexpensive and maintains high performance when a sintered magnet is used as a field magnet. SOLUTION: An R-Fe-B magnet (R
Is one or two of rare earth elements such as Nd and Dy including Y
), Wherein the permeance coefficient (Pcm) and the residual magnetic flux density (Br) of the R-Fe-B magnet in the state of the rotor alone are provided. : KG) and (Pcm + 1)> Br /
7. A permanent magnet field type rotating electric machine characterized by satisfying the relationship of 7.

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】本発明は配設された界磁用R
−Fe−B磁石の着磁性が良好な回転電機およびその製
造方法に関する。また、本発明は配設された界磁用焼結
磁石の加工が簡略化されて安価であるとともに高性能を
保持した永久磁石界磁型回転電機に関する。
BACKGROUND OF THE INVENTION 1. Field of the Invention The present invention relates to an R
The present invention relates to a rotating electric machine with good magnetization of an Fe-B magnet and a method for manufacturing the same. The present invention also relates to a permanent magnet field type rotating electric machine in which the processing of the provided field magnet is simplified, inexpensive, and has high performance.

【0002】[0002]

【従来の技術】最近の永久磁石材料の特性改良には目覚
ましいものがあり、例えばR−Fe−B系の希土類磁石
(RはYを含めたNd,Dy等の希土類元素の1種また
は2種以上の元素であり、以後R−Fe−B磁石と略
す。)はその非常に高い磁石特性によって、主に軽薄短
小の分野(例えば、ハードディスクドライブのヘッドア
クチュエータ駆動用モータ等。)に広く用いられてき
た。近年、高温に耐えるR−Fe−B磁石が開発され、
出力が10kWを越すような大型の回転電機(例えば、
電気自動車駆動用モータ等。)にも使用されるようにな
ってきた。しかし、R−Fe−B磁石は磁石特性が高い
反面、回転電機に界磁用磁石として配設された状態で着
磁を行う際にその固有の優れた磁石特性を100%引き
出すことが可能な十分な着磁磁界強度を確保できない場
合が実用上多く見られる。
2. Description of the Related Art Recent improvements in the properties of permanent magnet materials are remarkable. For example, R-Fe-B based rare earth magnets (R is one or two of rare earth elements such as Nd and Dy including Y) These elements, hereinafter abbreviated as R-Fe-B magnets) are widely used mainly in light, thin and small fields (for example, motors for driving a head actuator of a hard disk drive) because of their extremely high magnetic properties. Have been. In recent years, R-Fe-B magnets that can withstand high temperatures have been developed,
A large rotating electric machine whose output exceeds 10 kW (for example,
Motors for driving electric vehicles. ) Has also begun to be used. However, while the R-Fe-B magnet has high magnet properties, it is possible to bring out 100% of its unique excellent magnet properties when magnetizing it while being arranged as a field magnet in a rotating electric machine. There are many cases where a sufficient magnetizing magnetic field strength cannot be secured.

【0003】本発明者らは永久磁石界磁型回転電機に組
み込まれたR−Fe−B磁石の着磁条件を鋭意検討した
結果、R−Fe−B磁石の残留磁束密度(Br)が90
00G以上のときに着磁不良が多く発生していることを
確認した。
[0003] The inventors of the present invention have conducted intensive studies on the magnetizing conditions of the R-Fe-B magnet incorporated in the permanent magnet field type rotating electric machine. As a result, the residual magnetic flux density (Br) of the R-Fe-B magnet was 90%.
It was confirmed that a large number of magnetization failures occurred at 00G or more.

【0004】図11の斜視図に示される従来の表面磁石
型回転子105では回転子コア102の外周面にNd−
Fe−B磁石103を配置しているが、この磁石103
を単体で着磁した後その回転子105に配置する場合、
この磁石103の単体着磁におけるパーミアンス係数は
0.5以下であることが多く着磁の印加磁界を大きくし
てもこの磁石103の内部に不完全着磁部分が残存する
可能性があり、好ましくない。他方、未着磁のNd−F
e−B磁石103を配置した表面磁石型回転子105の
状態でそのNd−Fe−B磁石103を着磁する方法が
あるが、回転子105の仕様変更毎に着磁用の専用治具
を設計、製作する必要があり、コスト高となるため実用
的でない。さらに、この方法で着磁した回転子105を
図12に示した回転電機200に組み込む際に回転子1
05と固定子104との間に強力な磁気吸引力が作用す
るので、この組み込み作業には困難が伴い、回転電機2
00が大型化するとさらに適切な組み込み用治具を使用
しないと非常に危険である。
[0004] In a conventional surface magnet type rotor 105 shown in a perspective view of FIG.
Although the Fe-B magnet 103 is arranged, this magnet 103
Is placed on the rotor 105 after magnetizing the
The permeance coefficient in magnetizing the magnet 103 alone is often 0.5 or less, and even if the applied magnetic field is increased, an incompletely magnetized portion may remain inside the magnet 103. Absent. On the other hand, unmagnetized Nd-F
There is a method of magnetizing the Nd-Fe-B magnet 103 in a state of the surface magnet type rotor 105 on which the e-B magnet 103 is arranged. It is necessary to design and manufacture, and it is not practical because of high cost. Further, when the rotor 105 magnetized by this method is incorporated into the rotating electric machine 200 shown in FIG.
Since a strong magnetic attraction force acts between the electric motor 05 and the stator 104, this assembling operation involves difficulty, and the rotating electric machine 2
If the size of 00 becomes large, it is very dangerous unless an appropriate mounting jig is used.

【0005】上記組み込み作業の困難性を改善した提案
として、完成した回転電機の状態で固定子巻線の発生磁
界を利用して着磁を行う方法があり、図12により説明
する。図12の回転電機200では、固定子104の例
えばU相巻線115とV相巻線116に電流を流し、回
転子105の界磁用磁石103にこれら固定子巻線から
発生した着磁磁界を印加せしめ、着磁を行うことができ
る。固定子104の各U,V,W相巻線を施す部分10
8がスロットと呼ばれる固定子鉄芯に設けられた凹部で
ある。また、スロット108に挟まれた凸部109を歯
あるいは歯部と呼んでいる。この着磁方法によれば着磁
用の専用治具は必要ないが、巻線で発生した磁束は鉄芯
の歯部109に集中するため、スロット108と対向す
る界磁用磁石103の部分では着磁磁界が低く、歯部
(固定子磁極)109と対向する界磁用磁石103の部
分では着磁磁界が高いので、界磁用磁石103に部分的
な着磁率の変動が生じて均一な着磁磁石が得られないこ
とになる。この着磁不良の界磁用磁石103を配置した
永久磁石界磁型回転電機200ではこの界磁用磁石10
3の発生磁束量が局部的に変動するので、回転電機の性
能低下を招来してしまう。
As a proposal for improving the difficulty of the assembling work, there is a method of performing magnetization using a magnetic field generated in a stator winding in a state of a completed rotating electric machine, which will be described with reference to FIG. In the rotating electric machine 200 shown in FIG. 12, a current flows through, for example, the U-phase winding 115 and the V-phase winding 116 of the stator 104, and the magnetizing magnetic field generated from these stator windings flows through the field magnet 103 of the rotor 105. And magnetizing can be performed. Portion 10 for applying U, V, and W phase windings of stator 104
Reference numeral 8 denotes a recess provided in the stator iron core called a slot. Further, the convex portion 109 sandwiched between the slots 108 is called a tooth or a tooth portion. According to this magnetizing method, a dedicated jig for magnetizing is not required, but the magnetic flux generated by the winding concentrates on the teeth 109 of the iron core. Since the magnetizing magnetic field is low, and the magnetizing magnetic field is high in the portion of the field magnet 103 facing the tooth portion (stator magnetic pole) 109, the magnetizing rate of the field magnet 103 partially varies and uniformity occurs. A magnetized magnet cannot be obtained. In the permanent magnet field type rotary electric machine 200 in which the field magnet 103 having poor magnetization is arranged, the field magnet 10
Since the amount of generated magnetic flux of No. 3 locally fluctuates, the performance of the rotating electric machine is reduced.

【0006】次に、界磁用磁石として公知の焼結磁石
(例えば、Nd−Fe−B系異方性焼結磁石等。)を使
用する際には、姿砥石等を用いた砥石研削や平面研削等
の機械研削により焼結あがりの磁石体表面の黒皮部分を
除去して所定の寸法精度を付与しているのが実状であ
り、焼結磁石の加工効率の悪さに基因した加工費がかさ
んで永久磁石界磁型回転電機のコスト低減を阻んでいる
一因となっている。他方、未加工の焼結磁石(全面黒皮
品)を界磁用磁石103として上記図12の回転電機2
00に配設すると寸法精度不足からエアギャップ106
の厚みが不均一になることや発生磁束量にばらつきを生
じて、高性能の回転電機を実現することが困難である。
Next, when a known sintered magnet (for example, an Nd-Fe-B-based anisotropic sintered magnet or the like) is used as a field magnet, a grinding wheel using a grinding wheel or the like is used. The actual condition is that the black scale on the surface of the magnet body after sintering is removed by mechanical grinding such as surface grinding to give a predetermined dimensional accuracy, and the processing cost due to the poor processing efficiency of the sintered magnet This is one of the factors that hinders the cost reduction of permanent magnet field type rotating electric machines. On the other hand, an unprocessed sintered magnet (entire black scale) is used as the field magnet 103 for the rotating electric machine 2 shown in FIG.
If it is arranged at 00, the air gap 106
It is difficult to realize a high-performance rotating electric machine because the thickness of the magnetic head becomes uneven and the amount of generated magnetic flux varies.

【0007】[0007]

【発明が解決しようとする課題】したがって、本発明の
課題は装着された界磁用R−Fe−B磁石を良好に着磁
可能な永久磁石界磁型回転電機およびその製造方法を提
供することである。また、界磁用磁石として用いる焼結
磁石の焼結上がりのもの(全面黒皮品)の寸法ばらつき
と加工性の悪さとを考慮して、高性能を維持しながら焼
結磁石の加工コストを抑えた安価な永久磁石界磁型回転
電機を提供することである。
SUMMARY OF THE INVENTION Accordingly, an object of the present invention is to provide a permanent magnet field type rotating electric machine capable of satisfactorily magnetizing the mounted field R-Fe-B magnet and a method of manufacturing the same. It is. In addition, taking into account the dimensional variation and poor processability of the sintered magnet used as the field magnet (the entire surface is black scale), the processing cost of the sintered magnet is maintained while maintaining high performance. An object of the present invention is to provide an inexpensive permanent magnet field type rotating electric machine that is suppressed.

【0008】[0008]

【課題を解決するための手段】上記課題を解決した本発
明の永久磁石界磁型回転電機は、回転子コア内部にR−
Fe−B磁石(RはYを含めたNd,Dy等の希土類元
素の1種または2種以上)を有した内部磁石型回転子を
備えた永久磁石界磁型回転電機であって、前記回転子単
独の状態における前記R−Fe−B磁石のパーミアンス
係数(Pcm)と残留磁束密度(Br:kG)とが、
(Pcm+1)>Br/7 の関係を満たすことを特徴
とする。本発明によれば、永久磁石界磁型回転電機の界
磁用R−Fe−B磁石に印加される有効磁界強度を常温
環境で15kOe以上とすれば、そのR−Fe−B磁石
にほぼ着磁率100%の良好な着磁を付与できて永久磁
石界磁型回転電機特性を安定して高水準に維持すること
ができる。すなわち、従来の回転電機の着磁において発
生し易い界磁用磁石の着磁むらの発生を抑制でき、回転
電機としての特性を安定に向上できる。ここで、回転子
単独の状態とは地球磁場以外に実質的にその回転子に外
部磁場が印加されていない状態、すなわちその回転子近
傍に磁性体が存在していない状態をいう。
SUMMARY OF THE INVENTION In order to solve the above-mentioned problems, a permanent magnet field type rotating electric machine according to the present invention has an R-type rotor inside a rotor core.
A permanent magnet field type rotating electric machine including an internal magnet type rotor having an Fe-B magnet (R is one or two or more rare earth elements such as Nd and Dy including Y), The permeance coefficient (Pcm) and the residual magnetic flux density (Br: kG) of the R-Fe-B magnet in the state of the child alone are:
(Pcm + 1)> Br / 7. According to the present invention, if the effective magnetic field intensity applied to the field R-Fe-B magnet of the permanent magnet field type rotating electric machine is set to 15 kOe or more in a normal temperature environment, the magnetic field is almost completely attached to the R-Fe-B magnet. Good magnetization with a magnetic susceptibility of 100% can be provided, and the characteristics of the permanent magnet field type rotating electric machine can be stably maintained at a high level. That is, it is possible to suppress the occurrence of uneven magnetization of the field magnet, which tends to occur in the magnetization of the conventional rotating electric machine, and to stably improve the characteristics of the rotating electric machine. Here, the state of the rotor alone refers to a state in which an external magnetic field is not substantially applied to the rotor other than the earth magnetic field, that is, a state in which a magnetic substance does not exist near the rotor.

【0009】また、本発明は、複数の固定子磁極とこの
固定子磁極に回転磁界を発生する巻線とを有した固定子
と、回転軸とこの回転軸に設けられて前記固定子磁極に
対向して回転するとともに回転子コア内部にR−Fe−
B磁石(RはYを含めたNd,Dy等の希土類元素の1
種または2種以上)とそのR−Fe−B磁石の端部に空
間を有した内部磁石型回転子と、前記固定子磁極に対向
する前記回転子の磁極位置を検出してその位置に応じて
前記巻線に電流を供給する制御回路とを有し、前記回転
子単独の状態におけるR−Fe−B磁石のパーミアンス
係数(Pcm)と残留磁束密度(Br:kG)とが、
(Pcm+1)>Br/7 の関係を満たすことを特徴
とする永久磁石界磁型回転電機である。本発明によれ
ば、従来構成の固定子の制限された回転磁界強度でもっ
て本発明の回転電機の界磁用R−Fe−B磁石の着磁率
を、従来構成の回転電機に組み込まれた界磁用R−Fe
−B磁石の着磁率よりも良好にすることができ、実用性
に富むものである。
Further, the present invention provides a stator having a plurality of stator magnetic poles and a winding for generating a rotating magnetic field on the stator magnetic pole, a rotating shaft and a stator shaft provided on the rotating shaft. The rotor rotates in opposition and the R-Fe-
B magnet (R is one of rare earth elements such as Nd and Dy including Y
And two or more types), an internal magnet type rotor having a space at an end of the R-Fe-B magnet, and a magnetic pole position of the rotor facing the stator magnetic pole, and according to the detected position. A permance coefficient (Pcm) and a residual magnetic flux density (Br: kG) of the R-Fe-B magnet in the state of the rotor alone,
A permanent magnet field type rotating electric machine characterized by satisfying a relationship of (Pcm + 1)> Br / 7. According to the present invention, the magnetizing rate of the field R-Fe-B magnet of the rotating electric machine of the present invention is determined by the limited rotating magnetic field strength of the stator of the conventional structure. R-Fe for magnet
The magnetism can be made better than the magnetization rate of the -B magnet, and the magnet is highly practical.

【0010】また、本発明は、回転子コア内部に焼結磁
石を有した内部磁石型回転子を備えた永久磁石界磁型回
転電機であって、前記焼結磁石の表面に未加工の黒皮部
分を有するとともに、その黒皮部分が前記回転子コア内
部に設けられた空間に対向配置されることを特徴とする
永久磁石界磁型回転電機である。本発明により、寸法精
度に劣る焼結磁石の未加工黒皮部分の寸法ばらつきを回
転子コア内の回転軸長手方向に設けた空間部で吸収する
ことができるので焼結磁石の加工が簡略化でき、回転電
機の高性能を保持したコストダウンが可能である。ここ
で、この空間部は焼結磁石の磁化方向側には設けないこ
とが回転電機の高特性を維持するために好ましい。した
がって、黒皮を有した部分は焼結磁石の磁化方向側以外
の部分にあることが好ましい。
The present invention is also directed to a permanent magnet field type rotating electric machine having an internal magnet type rotor having a sintered magnet inside a rotor core, wherein the surface of the sintered magnet has an unprocessed black magnet. A permanent magnet field type rotating electric machine having a skin portion, wherein the black skin portion is arranged to face a space provided inside the rotor core. According to the present invention, the dimensional variation of the unprocessed black scale portion of the sintered magnet having inferior dimensional accuracy can be absorbed by the space provided in the rotor core in the longitudinal direction of the rotating shaft, thereby simplifying the processing of the sintered magnet. It is possible to reduce the cost while maintaining the high performance of the rotating electric machine. Here, it is preferable that this space is not provided on the magnetization direction side of the sintered magnet in order to maintain high characteristics of the rotating electric machine. Therefore, it is preferable that the portion having the black scale is a portion other than the magnetization direction side of the sintered magnet.

【0011】本発明の回転電機に組み込まれる内部磁石
型回転子を構成する回転子コアは、珪素鋼、磁性ステン
レス鋼、軟鉄、パーマロイ、非晶質軟磁性合金、ナノ結
晶粒軟磁性合金のいずれか1種または2種以上を用いて
形成することが好ましい。回転子コアは厚さ0.05〜
1mmの薄板を回転軸の長手方向に積層して形成するこ
とが耐渦電流損の点から好ましい。
The rotor core constituting the internal magnet type rotor incorporated in the rotating electric machine of the present invention is made of any one of silicon steel, magnetic stainless steel, soft iron, permalloy, amorphous soft magnetic alloy, and nanocrystalline soft magnetic alloy. It is preferable to use one or two or more of them. Rotor core thickness 0.05 ~
It is preferable from the viewpoint of eddy current resistance that a 1 mm thin plate is formed by laminating in the longitudinal direction of the rotating shaft.

【0012】また、内部磁石型回転子におけるR−Fe
−B磁石と回転子コアの外周面との間の回転子コアの最
小厚みを0.5〜5mmとすることが好ましい。この厚
みが0.5mm未満であると上記回転子単独状態におけ
る関係式を満足するように構成することが困難となりR
−Fe−B磁石の局部に着磁不良部分を発生し易くなる
ので着磁率が顕著に低下し、5mmを超えると着磁され
たR−Fe−B磁石から発した磁束がその最小厚みの回
転子コア部分で短絡して鎖交磁束量が減少し、いずれも
好ましくない。
Further, R-Fe in the internal magnet type rotor is used.
It is preferable that the minimum thickness of the rotor core between the -B magnet and the outer peripheral surface of the rotor core is 0.5 to 5 mm. If the thickness is less than 0.5 mm, it is difficult to configure the rotor so as to satisfy the relational expression in the rotor alone state.
-Magnetization rate is remarkably reduced because a poorly magnetized portion is easily generated in a local portion of the Fe-B magnet, and when it exceeds 5 mm, the magnetic flux generated from the magnetized R-Fe-B magnet is rotated with the minimum thickness. A short circuit occurs in the daughter core portion, and the amount of interlinkage magnetic flux is reduced, which is not preferable.

【0013】また、本発明は、複数の固定子磁極とこの
固定子磁極に回転磁界を発生する巻線を有した固定子
と、回転軸とこの回転軸に設けられて前記固定子磁極に
対向して回転するとともに回転子コア内部にR−Fe−
B磁石(RはYを含めたNd,Dy等の希土類元素の1
種または2種以上)を有した内部磁石型回転子と、前記
固定子磁極に対向する前記回転子の磁極位置を検出して
その位置に応じて前記巻線に電流を供給する制御回路と
を有した永久磁石界磁型回転電機の製造方法において、
前記回転子単独状態におけるR−Fe−B磁石のパーミ
アンス係数(Pcm)と残留磁束密度(Br:kG)と
が、 (Pcm+1)>Br/7 の関係を満足するよ
うに前記回転子を構成した後、その回転子をエアギャッ
プを介して前記固定子に対向配置して永久磁石界磁型回
転電機を構成し、その後前記巻線に通電することにより
発生する磁界で前記R−Fe−B磁石を着磁することを
特徴とする永久磁石界磁型回転電機の製造方法である。
本発明によれば、従来構成の固定子の発生する回転磁界
で界磁用のR−Fe−B磁石にほぼ100%の着磁率を
付与できるとともに、着磁された界磁用磁石を単体ある
いは部品として回転電機に組み込む従来の回転電機の製
造方法に比べて組立工数が削減できかつ安全である。さ
らに、回転バランスをとるために回転子の一部を削る必
要を生じた場合に削られた切り粉や削り屑が磁石回転子
の周囲に磁気吸着する不具合を避けることができる。
Further, the present invention provides a stator having a plurality of stator magnetic poles, a winding for generating a rotating magnetic field in the stator magnetic pole, a rotating shaft, and a rotating shaft provided to face the stator magnetic pole. And the rotor core has R-Fe-
B magnet (R is one of rare earth elements such as Nd and Dy including Y
(Or two or more types), and a control circuit that detects a magnetic pole position of the rotor facing the stator magnetic pole and supplies a current to the winding according to the position. In a method of manufacturing a permanent magnet field type rotating electric machine having
The rotor was configured such that the permeance coefficient (Pcm) and the residual magnetic flux density (Br: kG) of the R-Fe-B magnet in the rotor alone state satisfied the relationship of (Pcm + 1)> Br / 7. Thereafter, the rotor is disposed opposite to the stator via an air gap to form a permanent magnet field type rotating electric machine, and then the R-Fe-B magnet is formed by a magnetic field generated by energizing the winding. And a method for manufacturing a permanent magnet field type rotating electric machine characterized by magnetizing.
According to the present invention, the rotating magnetic field generated by the stator having the conventional configuration can impart a magnetizing rate of almost 100% to the field R-Fe-B magnet, and the magnetized field magnet can be used alone or The number of assembling steps can be reduced and safer than a conventional method of manufacturing a rotating electric machine that is incorporated into a rotating electric machine as a part. Furthermore, it is possible to avoid a problem that the shavings and shavings are magnetically attracted around the magnet rotor when it is necessary to cut a part of the rotor in order to balance the rotation.

【0014】[0014]

【発明の実施の形態】以下、本発明を詳説する。回転電
機の界磁用R−Fe−B磁石における着磁の困難さにつ
いて本発明者らが検討し、得た知見は下記の通りであ
る。図8に、磁石特性の異なる同一形状の3つのNd−
Fe−B磁石(日立金属(株)製の異方法焼結磁石):
イ、ロ、ハを用いて着磁率を評価した結果を示した。着
磁率は、(着磁率)=(着磁された永久磁石が発生する
磁束量)÷(その永久磁石の最大磁束密度が飽和する状
態にフル着磁された場合に発生する磁束量)×100
(%)で定義される値である。図8の横軸は空芯型のソ
レノイドコイルによる磁石単体着磁における着磁磁界強
度をとっている。図8において、ハ、ロ、イの順で右側
のものほど固有保磁力(iHc)が小さく、残留磁束密
度(Br)が大きいNd−Fe−B磁石となっている。
各磁石単体でのパーミアンス係数(Pc)は1に設定し
てある。パーミアンス係数(Pc)は、永久磁石が発生
する磁界方向と逆方向の磁界強度を−H、その−Hが永
久磁石に印加された場合に永久磁石内部に発生する磁束
密度をBとすると、Pc=B/Hで定義される。その磁
界強度−Hは、外部から電流などで加えられる磁界のみ
ならず、磁石内部で発生するいわゆる反磁界も含めた値
である。図8から、イ、ロ、ハの磁石特性の差によって
磁石単体で着磁した場合の着磁特性が異なることがわか
る。
DESCRIPTION OF THE PREFERRED EMBODIMENTS The present invention will be described below in detail. The present inventors have studied the difficulty of magnetizing the field R-Fe-B magnet of the rotating electric machine, and obtained the following findings. FIG. 8 shows three Nd-
Fe-B magnet (another method sintered magnet manufactured by Hitachi Metals, Ltd.):
The results of evaluating the magnetizability using a, b, and c are shown. Magnetization rate is (magnetization rate) = (magnetic flux generated by magnetized permanent magnet) / (magnetic flux generated when full magnetization is performed so that the maximum magnetic flux density of the permanent magnet is saturated) × 100
It is a value defined by (%). The horizontal axis in FIG. 8 represents the magnetizing magnetic field strength when the magnet alone is magnetized by the air-core type solenoid coil. In FIG. 8, the Nd-Fe-B magnet has a smaller intrinsic coercive force (iHc) and a larger residual magnetic flux density (Br) as the rightmost one in the order of c, b, and b.
The permeance coefficient (Pc) of each magnet alone is set to 1. The permeance coefficient (Pc) is defined as Pc, where -H is the magnetic field strength in the direction opposite to the magnetic field direction generated by the permanent magnet, and B is the magnetic flux density generated inside the permanent magnet when -H is applied to the permanent magnet. = B / H. The magnetic field strength -H is a value including not only a magnetic field applied by an external current or the like but also a so-called demagnetizing field generated inside the magnet. From FIG. 8, it can be seen that the magnetization characteristics when the magnets are magnetized alone differ depending on the difference in the magnet characteristics of A, B and C.

【0015】従来、このイ、ロ、ハの差は、固有保磁力
(iHc)の差によるものと考えられていたが、実際は
異なることがわかった。以下、その得られた知見につい
て説明する。上記Nd−Fe−B磁石イ、ロ、ハの単体
着磁特性の差について反磁界を考慮すると、この差は各
磁石内部での有効な着磁磁界の大きさの差に起因するこ
とが後述の通りわかった。永久磁石は磁化されると内部
で反磁界を形成する性質があり、例えば空芯型のソレノ
イドコイルによる磁石単体の着磁では、この反磁界を外
部印加磁界から差し引いたものが永久磁石の着磁に利用
される有効な磁界の強さとなる。この磁石内部で着磁に
有効利用される磁界の強さを、本発明では有効磁界と呼
ぶことにする。有効磁界の強さは下記関係式で定義され
る。 (有効磁界の強さ)=(外部印加磁界の強さ)−(反磁界の強さ) (1)
Conventionally, the difference between a, b, and c has been considered to be due to a difference in intrinsic coercive force (iHc). However, it has been found that the difference is actually different. Hereinafter, the obtained knowledge will be described. Considering the demagnetizing field for the difference between the individual magnetizing characteristics of the Nd-Fe-B magnets a, b, and c, it will be described later that this difference is caused by the difference in the magnitude of the effective magnetizing magnetic field inside each magnet. I understood as follows. Permanent magnets have the property of forming a demagnetizing field when magnetized.For example, when magnetizing a single magnet with an air-core solenoid coil, the demagnetizing field is subtracted from the externally applied magnetic field. The effective magnetic field strength used for In the present invention, the strength of the magnetic field effectively used for magnetization inside the magnet is referred to as an effective magnetic field. The strength of the effective magnetic field is defined by the following relational expression. (Effective magnetic field strength) = (Externally applied magnetic field strength)-(Demagnetizing field strength) (1)

【0016】反磁界の強さは、例えば図9の初期磁化曲
線から求めることができる。図9では上記Nd−Fe−
B磁石イ、ロ、ハを各々閉じた磁気回路中に挿入してパ
ーミアンス係数を大とし、着磁過程における反磁界の発
生を無視できる程度として初期磁化曲線を測定してい
る。横軸には印加磁界強度H(kOe)、縦軸には磁化
の強さ:4πI(kG)をとっている。所定の磁気回路
内で任意のパーミアンス係数Pcを持つ永久磁石を着磁
する場合の反磁界の強さは(2)式で与えられる。 (反磁界の強さ)=(永久磁石の磁化の強さ)×{1/(Pc+1)} (2) (1)、(2)式から、 (有効磁界の強さ)=(外部印加磁界の強さ)− (永久磁石の磁化の強さ)×{1/(Pc+1)}(3) の関係が得られる。
The strength of the demagnetizing field can be determined, for example, from the initial magnetization curve shown in FIG. In FIG. 9, the Nd-Fe-
The initial magnetization curve is measured by inserting the B magnets A, B, and C into a closed magnetic circuit to increase the permeance coefficient, and neglecting the generation of a demagnetizing field during the magnetization process. The horizontal axis indicates the applied magnetic field intensity H (kOe), and the vertical axis indicates the magnetization intensity: 4πI (kG). The strength of the demagnetizing field when a permanent magnet having an arbitrary permeance coefficient Pc is magnetized in a predetermined magnetic circuit is given by equation (2). (Strength of demagnetizing field) = (Strength of magnetization of permanent magnet) × {1 / (Pc + 1)} (2) From equations (1) and (2), (Effective field strength) = (Externally applied magnetic field) (Intensity of magnetization) − (magnetization intensity of permanent magnet) × {1 / (Pc + 1)} (3)

【0017】上記図8のデータを(3)式を用いて求め
た有効磁界の強さと着磁率との関係に再プロットしたの
が図10である。図10より、Nd−Fe−B磁石イ、
ロ、ハのいずれも有効磁界に対してほぼ一致した着磁率
を有しており、着磁率が約100%となる有効磁界は常
温において約15kOeであることがわかる。さらに、
本発明者らの検討によってこのように有効磁界が約15
kOe以上で着磁率がほぼ飽和することはR−Fe−B
磁石の共通の特性であることを確認した。実際に、図1
0の結果を検証するために上記Nd−Fe−B磁石イ、
ロ、ハを各々、Pc>10である磁気回路に組み込んで
反磁界の影響を排除した状態で着磁特性を測定すると、
ほぼ図10と同様の着磁特性を得ることができた。上記
知見をまとめると次のようになる。 R−Fe−B磁石の着磁率は有効磁界に対してほぼ一
定である。 永久磁石特性の差によって外部からの印加着磁磁界の
大きさに応じて誘起される反磁界の大きさが異なるた
め、磁石単体着磁等の低パーミアンス係数の着磁では見
掛け上(Br)の小さい永久磁石の着磁特性が良好に見
える。これらの知見を基に、本発明者らはR−Fe−B
磁石の着磁を良好にする磁気回路について検討を行っ
た。(3)式を変形して、 (外部印加磁界の強さ)−(有効磁界の強さ)=(永久磁石の磁化の強さ) ×{1/(Pc+1)} (4) となる。 (4)式の(有効磁界の強さ)はR−Fe−B磁石では
15kOe以上必要であることは前述の通りである。ま
た、回転電機の回転磁界発生用巻線により界磁用R−F
e−B磁石を着磁する場合において、発生できる着磁磁
界の強さは実用上常温(例えば20℃)において22k
Oe程度が最大である。すなわち、(4)式の(外部印
加磁界の強さ)は22kOe以下である。これらを考慮
すると、(4)式から(5)式が導かれる。 22−15=7(kOe)=(R−Fe−B磁石の磁化の強さ) ×{1/(Pc+1)} (5) (5)式の(R−Fe−B磁石の磁化の強さ)は最大で
残留磁束密度Brになることがわかっているため、この
条件を入れて(5)式を変形することにより(6)式を
得る。 (Pc+1)>Br(kG)/7(kOe) (6) (6)式を満たす場合に、界磁用R−Fe−B磁石の磁
気特性を十分に引き出すことのできる良好な着磁がなさ
れる回転電機を実現できる。なお、回転電機の巻線を利
用した界磁用R−Fe−B磁石の着磁の際には、スロッ
トの断面積を確保するために巻線を施している歯部の断
面積自体が小さな値となっている。このため、着磁に際
して巻線に流れる電流によって誘起される磁束により歯
部が飽和状態となるので、界磁用R−Fe−B磁石のパ
ーミアンス係数を計算する場合は歯部の磁性体は考慮に
入れず、そのR−Fe−B磁石が設置してある回転子コ
ア単独で計算することが必要である。
FIG. 10 is a re-plot of the data of FIG. 8 to the relationship between the strength of the effective magnetic field and the magnetization rate obtained by using the equation (3). From FIG. 10, Nd-Fe-B magnet b,
Both (b) and (c) have a magnetization rate substantially coincident with the effective magnetic field, and it can be seen that the effective magnetic field at which the magnetization rate becomes about 100% is about 15 kOe at room temperature. further,
According to the study of the present inventors, the effective magnetic field is about 15
At kOe or more, the magnetizability is almost saturated with R-Fe-B
It was confirmed that it was a common property of magnets. In fact, FIG.
In order to verify the result of 0, the Nd-Fe-B magnet b
(B) and (c) are each incorporated into a magnetic circuit with Pc> 10, and the magnetization characteristics are measured in a state where the influence of the demagnetizing field is eliminated.
Magnetization characteristics similar to those in FIG. 10 were obtained. The above findings are summarized as follows. The magnetization rate of the R-Fe-B magnet is almost constant with respect to the effective magnetic field. Since the magnitude of the demagnetizing field induced according to the magnitude of the externally applied magnetizing magnetic field varies depending on the difference in the permanent magnet characteristics, the apparent (Br) of the magnetization has a low permeance coefficient such as the magnet alone. The magnetizing characteristics of the small permanent magnet look good. Based on these findings, the present inventors have found that R-Fe-B
A magnetic circuit for improving the magnetization of the magnet was studied. Equation (3) is modified so that (the strength of the externally applied magnetic field) − (the strength of the effective magnetic field) = (the strength of the magnetization of the permanent magnet) × {1 / (Pc + 1)} (4). As described above, the value of (effective magnetic field strength) in the expression (4) is required to be 15 kOe or more for the R-Fe-B magnet. In addition, the field R-F
When magnetizing an e-B magnet, the intensity of the magnetizing magnetic field that can be generated is 22 k at room temperature (for example, 20 ° C.) for practical use.
Oe is the largest. That is, (the strength of the externally applied magnetic field) in the equation (4) is 22 kOe or less. In consideration of these, the expression (5) is derived from the expression (4). 22-15 = 7 (kOe) = (magnetization strength of R-Fe-B magnet) × {1 / (Pc + 1)} (5) (5) Equation (5): Magnetization strength of (R-Fe-B magnet) ) Is known to be the residual magnetic flux density Br at the maximum, and the equation (6) is obtained by modifying the equation (5) with this condition. (Pc + 1)> Br (kG) / 7 (kOe) (6) When the expression (6) is satisfied, good magnetization that can sufficiently bring out the magnetic characteristics of the field R-Fe-B magnet is performed. Rotating electric machine can be realized. When magnetizing the field R-Fe-B magnet using the windings of the rotating electrical machine, the cross-sectional area itself of the teeth on which the windings are applied is small in order to secure the cross-sectional area of the slot. Value. For this reason, the teeth become saturated due to the magnetic flux induced by the current flowing through the winding at the time of magnetization. Therefore, when calculating the permeance coefficient of the field R-Fe-B magnet, the magnetic material of the teeth is considered. It is necessary to calculate only the rotor core on which the R-Fe-B magnet is installed, without using the R-Fe-B magnet.

【0018】次に、本発明を実施例を交えて説明する。
図1は本発明の回転電機の一態様を示す要部断面図であ
る。図1において、図14と同一構成部分には同一の符
号を付している。図1の永久磁石界磁型回転電機10は
電動機として構成した一例であり、内部磁石型回転子5
0と固定子104とを有している。内部磁石型回転子5
0は回転軸5(例えばSUS304製)のまわりに軟磁
性の回転子コア2を配置し、さらに回転子コア2の内部
に図示の磁極を有した板状のNd−Fe−B磁石1(例
えば、日立金属(株)製の異方性焼結磁石;HS−35
CHで横20mm×縦4mm×軸方向50mmの長方形
板状のもの。)が略四角形状に4個埋設されて、内部磁
石型回転子50の外周面回転方向に等間隔に対称4極が
形成可能に構成されている。また、Nd−Fe−B磁石
1の両端部には略三角形状の空間3が形成されていて、
点線で模式的に示される隣接磁極間の短絡磁束Фsを抑
えられるとともに、Nd−Fe−B磁石1の端面1aが
未加工部分である黒皮仕様のものであって寸法がばらつ
いたものでも空間3でその端面1aの寸法ばらつきを吸
収できるようになっている。したがって、Nd−Fe−
B磁石1の磁極面である1b両面を平面研削する等の簡
略な機械加工のみでNd−Fe−B磁石1の最終形状に
仕上げられるのでコスト低減に有利であり、かつ下記関
係式のように回転子50を構成している。回転子コア2
内で空間3はNd−Fe−B磁石1の固設状況に応じて
軸方向に必要分が形成されて、その形状寸法は黒皮部分
1aの寸法ばらつき程度および内部磁石型回転子50の
磁気回路の拘束条件から適宜設定される。なお、黒皮を
有した焼結磁石としては公知のものを用いることがで
き、端面1aに軽度の加工を施して部分的に黒皮が残る
ようにしたものを用いても良い。この回転子50単独状
態でのNd−Fe−B磁石1のパーミアンス係数(Pc
m)と残留磁束密度(Br:kG)との関係は、 (P
cm+1)=Br/3.5 であり、回転電機10とし
て良好な特性を示した。さらに、Nd−Fe−B磁石1
と回転子コア2の外周面との間の最小厚み部の厚みt1
は0.5〜5mmとしている。この構成下で、Nd−F
e−B磁石1の着磁面(磁極面)1bとエアギャップ4
との間に回転子コア2が存在するので、上記従来の回転
電機200においてスロット部108と歯部109とで
生じる着磁磁界強度のむらが抑えられて軟磁性の回転子
コア2内部で平準化され、Nd−Fe−B磁石1の着磁
特性が向上する。しかし、t1寸法が0.5mm未満で
は、 (Pcm+1)>Br/7 を満足できなかっ
た。また、t1寸法が5mmを越えると着磁後のNd−
Fe−B磁石1から発生する磁束が回転子コア2のt1
部を通って回転子コア2の内部で容易に短絡してしま
い、固定子104に導かれる有効な鎖交磁束量が極端に
減少するので、回転電機の特性向上が難しい。
Next, the present invention will be described with reference to examples.
FIG. 1 is a cross-sectional view of a principal part showing one embodiment of the rotating electric machine of the present invention. 1, the same components as those in FIG. 14 are denoted by the same reference numerals. The permanent magnet field type rotary electric machine 10 of FIG. 1 is an example configured as an electric motor, and an internal magnet type rotor 5
0 and a stator 104. Internal magnet type rotor 5
Numeral 0 denotes a plate-like Nd-Fe-B magnet 1 (for example, a soft magnetic rotor core 2 having a magnetic pole shown in the drawing) arranged around a rotation axis 5 (for example, made of SUS304). Anisotropic sintered magnet manufactured by Hitachi Metals, Ltd .; HS-35
A rectangular plate having a width of 20 mm, a length of 4 mm, and an axial direction of 50 mm. ) Are buried in a substantially square shape so that symmetrical four poles can be formed at equal intervals in the rotation direction of the outer peripheral surface of the internal magnet type rotor 50. A substantially triangular space 3 is formed at both ends of the Nd—Fe—B magnet 1,
The short-circuit flux Фs between adjacent magnetic poles, which is schematically shown by a dotted line, can be suppressed, and even if the end face 1a of the Nd-Fe-B magnet 1 is an unprocessed part of a black scale specification and its dimensions vary, the space can be reduced. 3 allows the dimensional variation of the end face 1a to be absorbed. Therefore, Nd-Fe-
Since the Nd-Fe-B magnet 1 can be finished to the final shape only by simple mechanical processing such as surface grinding of both surfaces 1b, which are the pole faces of the B magnet 1, it is advantageous for cost reduction, and as in the following relational expression: The rotor 50 is constituted. Rotor core 2
A space 3 is formed in the space 3 in an axial direction according to the fixed state of the Nd-Fe-B magnet 1, and its shape and dimension are about the degree of dimensional variation of the black scale portion 1 a and the magnetic force of the internal magnet type rotor 50. It is set as appropriate from the constraint conditions of the circuit. A known magnet can be used as the sintered magnet having a black scale, and a magnet in which the end face 1a is lightly processed to partially leave the black scale may be used. The permeance coefficient (Pc) of the Nd—Fe—B magnet 1 in the rotor 50 alone state
m) and the residual magnetic flux density (Br: kG) are given by (P
cm + 1) = Br / 3.5, and showed good characteristics as the rotating electric machine 10. Further, the Nd-Fe-B magnet 1
T1 of the minimum thickness portion between the rotor core 2 and the outer peripheral surface thereof
Is 0.5 to 5 mm. Under this configuration, Nd-F
Magnetized surface (magnetic pole surface) 1b of eB magnet 1 and air gap 4
, The unevenness in the intensity of the magnetizing magnetic field generated in the slot portion 108 and the tooth portion 109 in the above-described conventional rotary electric machine 200 is suppressed, and leveling is performed inside the soft magnetic rotor core 2. As a result, the magnetization characteristics of the Nd—Fe—B magnet 1 are improved. However, if the t1 dimension was less than 0.5 mm, (Pcm + 1)> Br / 7 could not be satisfied. If the t1 dimension exceeds 5 mm, the Nd-
The magnetic flux generated from the Fe-B magnet 1 is equal to t1 of the rotor core 2.
The short circuit easily occurs inside the rotor core 2 through the portion, and the amount of effective interlinkage magnetic flux guided to the stator 104 is extremely reduced, so that it is difficult to improve the characteristics of the rotating electric machine.

【0019】図1の固定子104側には三相スター結線
した巻線:(U相115、V相116、W相117)が
設けてあり、これらの巻線によって回転磁界を発生せし
め、その回転磁界に同期させて下記本発明の着磁方法で
良好に着磁されたNd−Fe−B磁石1を有した内部磁
石型回転子50が回転するようになっている。この回転
子50の直径は約50mm,回転軸5の軸方向長さは約
80mmにしてある。また回転子コア2と固定子コア1
10は3.5%珪素鋼板を用いて形成してある。回転子
コア2と固定子コア110とを上記珪素鋼板の薄板(例
えば厚み0.45mmのもの)で積層して形成すると耐
渦電流損の点から好ましい。
On the stator 104 side in FIG. 1, three-phase star-connected windings (U-phase 115, V-phase 116, W-phase 117) are provided, and these windings generate a rotating magnetic field. In synchronization with the rotating magnetic field, the internal magnet type rotor 50 having the Nd-Fe-B magnet 1 which is well magnetized by the magnetizing method of the present invention described below rotates. The diameter of the rotor 50 is about 50 mm, and the axial length of the rotating shaft 5 is about 80 mm. The rotor core 2 and the stator core 1
10 is formed using a 3.5% silicon steel plate. It is preferable from the viewpoint of eddy current resistance that the rotor core 2 and the stator core 110 are formed by laminating the above silicon steel sheets (for example, those having a thickness of 0.45 mm).

【0020】図2は、上記U,V,W相各巻線と、着磁
用電源として使用するコンデンサとの結線構成の一例を
示す模式図である。図2ではコンデンサ21を1個とし
て模式的に表わしているが、上記回転電機10では実際
には多数のコンデンサ群を直列および/または並列に接
続し、所定の耐電圧とキャパシタンスとを得ている。
FIG. 2 is a schematic diagram showing an example of a connection configuration between the U, V, and W phase windings and a capacitor used as a power supply for magnetization. Although FIG. 2 schematically shows one capacitor 21, in the rotary electric machine 10, a large number of capacitor groups are actually connected in series and / or in parallel to obtain predetermined withstand voltage and capacitance. .

【0021】図1の回転電機10において、未着磁状態
の界磁用Nd−Fe−B磁石1に実用に供し得るに十分
な所定の磁力を付与して図示するような4極構成の回転
子50とするための本発明の着磁方法について以下に説
明する。 (実施例)図2のコンデンサ21のキャパシタンスを2
500μFに固定し、このコンデンサ2に所定の電圧を
印加し、十分時間が経った後にスイッチSを閉じて図1
の巻線(U相およびV相)に約4msecの半値幅電流
を流し、Nd−Fe−B磁石1を着磁した。このNd−
Fe−B磁石1として上記図8〜図10のNd−Fe−
B磁石イ、ロ、ハと各々同一の材質、磁石特性を有した
Nd−Fe−B磁石イ、ロ、ハを用いて着磁している。
前記巻線に流れる電流は印加電圧により異なり、ピーク
値で約200〜600Aである。この着磁における回転
電機10のコンデンサ充電電圧に対するNd−Fe−B
磁石1としてのイ、ロ、ハとの着磁率の関係を図3に示
した。図3より、コンデンサ充電電圧が2500V以上
で本発明における界磁用Nd−Fe−B磁石イ、ロ、ハ
が十分な着磁率を有していることがわかった。また、図
3において、イは(Pcm+1)>Br/3.8であ
り、ロは(Pcm+1)>Br/3.5であり、ハは
(Pcm+1)>Br/3.25の関係にある。
In the rotating electric machine 10 shown in FIG. 1, a predetermined magnetic force sufficient for practical use is applied to the non-magnetized field Nd-Fe-B magnet 1 so as to form a 4-pole rotating motor as shown in FIG. The magnetizing method of the present invention for forming the element 50 will be described below. (Embodiment) The capacitance of the capacitor 21 of FIG.
It is fixed at 500 μF, a predetermined voltage is applied to this capacitor 2, and after a sufficient time has passed, the switch S is closed and FIG.
A half-width current of about 4 msec was passed through the windings (U-phase and V-phase) to magnetize the Nd-Fe-B magnet 1. This Nd-
As the Fe-B magnet 1, the Nd-Fe-
Magnetization is performed using Nd-Fe-B magnets A, B, and C having the same material and magnetic properties as the B magnets A, B, and C, respectively.
The current flowing through the winding varies depending on the applied voltage, and has a peak value of about 200 to 600A. Nd-Fe-B with respect to the capacitor charging voltage of the rotating electric machine 10 in this magnetization
FIG. 3 shows the relationship between the magnetization rates of A, B, and C as the magnet 1. From FIG. 3, it was found that when the capacitor charging voltage was 2500 V or higher, the field Nd-Fe-B magnets A, B, and C of the present invention had sufficient magnetization rates. In addition, in FIG. 3, A has a relationship of (Pcm + 1)> Br / 3.8, B has a relationship of (Pcm + 1)> Br / 3.5, and C has a relationship of (Pcm + 1)> Br / 3.25.

【0022】(比較例)比較例として上記図12の回転
電機200において、表面磁石型回転子105に配置さ
れたNd−Fe−B磁石103(日立金属(株)製のH
S−35CH)の着磁率を評価した結果を図4に示し
た。図4より、このNd−Fe−B磁石103の着磁率
は初期電圧2500(V)でも十分とは言えず、実施例
のイ、ロ、ハのものに比べて着磁性が非常に悪く、(P
cm+1)>Br/7 の関係を満たしていない。この
着磁性の悪さの要因として、以下の2つがあげられる。 1)回転電機200の巻線にNd−Fe−B磁石103
を着磁するためのできるだけ多くの電流を流すと、回転
電機200の巻線が施されている鉄芯の歯部109が飽
和状態となり、歯部109とエアギャップ106を隔て
て対向しているNd−Fe−B磁石103部分のパーミ
アンス係数を上げるための鉄芯としての役割を十分果た
すことができなくなる。 2)歯部109にNd−Fe−B磁石103を着磁する
ための磁束が集中し、Nd−Fe−B磁石103のうち
歯部109に対向している部分が選択的に着磁され、均
一に着磁されない。これらの不具合要因を踏まえて、上
記の通り本発明ではR−Fe−B磁石を回転子コア内部
に配置した特長ある内部磁石型の回転子構成としたの
で、従来の着磁不具合を避けることができる。
(Comparative Example) As a comparative example, in the rotating electric machine 200 shown in FIG. 12, the Nd-Fe-B magnet 103 (Hitachi Metal Co., Ltd.)
The result of evaluating the magnetization rate of (S-35CH) is shown in FIG. From FIG. 4, the magnetizing rate of the Nd—Fe—B magnet 103 cannot be said to be sufficient even at the initial voltage of 2500 (V), and the magnetizing rate is very poor as compared with those of the examples a, b, and c. P
cm + 1)> Br / 7. The following two factors can be cited as factors of the poor magnetization. 1) Nd-Fe-B magnet 103 in winding of rotating electric machine 200
When as much current as possible is passed to magnetize the rotor, the teeth 109 of the iron core on which the windings of the rotating electric machine 200 are wound become saturated, and face the teeth 109 with the air gap 106 therebetween. The Nd—Fe—B magnet 103 cannot sufficiently serve as an iron core for increasing the permeance coefficient of the portion. 2) The magnetic flux for magnetizing the Nd-Fe-B magnet 103 concentrates on the teeth 109, and the portion of the Nd-Fe-B magnet 103 facing the teeth 109 is selectively magnetized, Not uniformly magnetized. In view of these inconvenience factors, as described above, the present invention employs a unique internal magnet type rotor configuration in which the R-Fe-B magnet is disposed inside the rotor core, so that the conventional magnetization failure can be avoided. it can.

【0023】本発明では平板状のNd−Fe−B磁石を
回転子コア内部に配置した内部磁石型回転子の構成に限
定されず、図5に示した弧状の界磁磁石71を配置した
内部磁石型回転子70、図6に示したブロック状の界磁
磁石81を同磁極反発型に配置した内部磁石型回転子8
0、図7に示した逆弧状の界磁磁石91を用いた内部磁
石型回転子90の構成等、用途に応じて自在に採用可能
である。さらに、図5〜図7において点線で示される略
三角形の空間74,84,94を各界磁磁石の磁極面以
外に対向させて配設するとともに、各界磁磁石を端面7
1a,81a,91aが黒皮面または部分的に黒皮面で
ある異方性焼結磁石としても良い。この場合、各焼結磁
石71,81,91における磁極面71b,81b,9
1bは所定の寸法公差内に加工されているので加工コス
トの低減とともに回転電機特性を全面加工した異方性焼
結磁石を用いた場合と略同等に維持可能である。
The present invention is not limited to the configuration of the internal magnet type rotor in which the plate-like Nd-Fe-B magnet is disposed inside the rotor core, but is not limited to the configuration in which the arc-shaped field magnet 71 shown in FIG. Magnet type rotor 70, internal magnet type rotor 8 in which block-shaped field magnet 81 shown in FIG. 6 is arranged in the same magnetic pole repulsion type
0, the configuration of the internal magnet type rotor 90 using the reverse arc-shaped field magnet 91 shown in FIG. Further, substantially triangular spaces 74, 84, and 94 shown by dotted lines in FIGS. 5 to 7 are arranged so as to face each other than the pole faces of the field magnets, and each field magnet is connected to the end face 7 thereof.
The anisotropic sintered magnets 1a, 81a, and 91a may be black scale or partially black scale. In this case, the pole faces 71b, 81b, 9 of the respective sintered magnets 71, 81, 91
1b is processed within a predetermined dimensional tolerance, so that it is possible to reduce the processing cost and maintain substantially the same as the case of using an anisotropic sintered magnet in which the rotating electrical machine characteristics are entirely processed.

【0024】上記態様では永久磁石を内包した回転子を
固定子の内側に対向配置したインナーロータ型の回転電
機の例を示したがアウターロータ型にも適用可能である
ことは勿論である。また、本発明は発電機にも適用可能
である。さらに、具体的に例示すると、(a)永久磁石
が固定子に配置されており、かつ、回転子が固定子の内
側に配置されている構成、(b)永久磁石が固定子に配
置されており、かつ、回転子が固定子の外側に配置され
ている構成、(c)永久磁石が回転子に配置されてお
り、かつ、回転子が固定子の外側に配置されている構
成、(d)永久磁石が回転子に配置されており、かつ、
固定子と回転子が軸方向に対向する構成、(e)永久磁
石が固定子に配置されており、かつ、固定子と回転子が
軸方向に対向する構成、等にも広く本発明を適用可能で
ある。
In the above embodiment, the example of the inner rotor type rotating electric machine in which the rotor containing the permanent magnet is arranged inside the stator to face each other has been described, but it is needless to say that the present invention can be applied to the outer rotor type. The present invention is also applicable to a generator. Further specifically, when (a) the permanent magnet is arranged on the stator and the rotor is arranged inside the stator, (b) the permanent magnet is arranged on the stator (C) a configuration in which the rotor is disposed outside the stator, and (c) a configuration in which the rotor is disposed outside the stator, and (c) a configuration in which the rotor is disposed outside the stator. ) A permanent magnet is arranged on the rotor, and
The present invention can be widely applied to a configuration in which a stator and a rotor face in the axial direction, (e) a configuration in which a permanent magnet is disposed on the stator, and a configuration in which the stator and the rotor face in the axial direction. It is possible.

【0025】上記態様では、界磁用永久磁石としてNd
−Fe−B系の異方性焼結磁石を用いた回転電機の構成
および製造方法を記載したが、本発明は公知のR−Fe
−B磁石であって従来の回転電機に組み込まれた状態で
その固有の高い磁石特性までのフル着磁が難しい材質に
適用可能である。本発明を適用可能なR−Fe−B磁石
を例示すると、R−Fe−B系であれば良いが、望まし
くはR−Fe−(Co)−B−M系が良く、RはYを含
む希土類元素のうちの1種または2種以上を25〜35
重量%、Bは0.8〜1.2重量%、MはAl、Nb、
Ti、V、Zr、Mo、W、Ga、Cu、Zn、Ge、
Snのうちの1種または2種以上を5重量%以下、残部
が不可避な混合物を除きFeまたはFeとCoからな
る。合金系として、Nd−Fe−B−Al−Nb、Nd
−Fe−Co−B−Al−Nb、Nd−Fe−B−Al
−Ga、Nd−Fe−Co−B−Al−Ga、Nd−D
y−Fe−B−Al−Nb、Nd−Dy−Fe−Co−
B−Al−Nb、Nd−Dy−Fe−B−Al−Ga、
Nd−Fe−Dy−Co−B−Al−Ga等の異方性焼
結磁石、およびこれらの粉末の1種または2種以上を用
いたボンド磁石等が例示されるが、限定されるものでは
ない。
In the above embodiment, Nd is used as the field permanent magnet.
Although the configuration and manufacturing method of a rotating electric machine using an anisotropic sintered magnet of the Fe-B type have been described, the present invention relates to a known R-Fe
The present invention is applicable to a material which is a -B magnet which is difficult to fully magnetize to its inherent high magnet characteristics in a state where the magnet is incorporated in a conventional rotating electric machine. As an example of an R-Fe-B magnet to which the present invention can be applied, an R-Fe-B system may be used, but an R-Fe- (Co) -BM system is preferable, and R includes Y. One or more of the rare earth elements is 25 to 35
% By weight, B is 0.8 to 1.2% by weight, M is Al, Nb,
Ti, V, Zr, Mo, W, Ga, Cu, Zn, Ge,
One or more of Sn is 5% by weight or less, and the balance is Fe or Fe and Co excluding an unavoidable mixture. Nd-Fe-B-Al-Nb, Nd
-Fe-Co-B-Al-Nb, Nd-Fe-B-Al
-Ga, Nd-Fe-Co-B-Al-Ga, Nd-D
y-Fe-B-Al-Nb, Nd-Dy-Fe-Co-
B-Al-Nb, Nd-Dy-Fe-B-Al-Ga,
Examples include anisotropic sintered magnets such as Nd-Fe-Dy-Co-B-Al-Ga, and bonded magnets using one or more of these powders, but are not limited thereto. Absent.

【0026】上記態様では内部磁石型回転子の外周面回
転方向に等間隔で対称4極の磁極を形成した例を記載し
たが、磁極間隔が異なる非対称の磁極構成としても良
い。また、磁極数は限定されるものはないが、例えば2
〜100極の構成が非常に有用である。
In the above-described embodiment, an example has been described in which four symmetrical magnetic poles are formed at equal intervals in the rotation direction of the outer peripheral surface of the internal magnet type rotor, but an asymmetrical magnetic pole configuration having different magnetic pole intervals may be used. Further, the number of magnetic poles is not limited.
A configuration of ~ 100 poles is very useful.

【0027】[0027]

【発明の効果】以上記述の通り、本発明は下記の優れた
効果を奏し得る。 (1)Brが9kG以上の界磁用R−Fe−B磁石を配
置した回転電機において、従来構成の固定子巻線の形成
磁界を利用してそのR−Fe−B磁石をほぼ均一かつ良
好に着磁できるように構成したので、そのR−Fe−B
磁石固有の磁石特性に非常に近い磁石特性レベルまで着
磁可能となり、回転電機としての特性ばらつきおよび耐
熱性の改善に大きく寄与する。 (2)永久磁石界磁型回転電機に未着磁状態で組み込ま
れた界磁用R−Fe−B磁石をほぼ均一かつ安全に着磁
できるので高性能の回転電機を安定して製作できるとと
もに組み立て作業の安全性が確保される有用なものであ
る。 (3)回転電機特性を良好に維持しながら界磁用磁石と
して用いる焼結磁石の加工コストを低減することができ
る。
As described above, the present invention has the following excellent effects. (1) In a rotating electric machine in which an R-Fe-B magnet for field having Br of 9 kG or more is arranged, the R-Fe-B magnet is made almost uniform and good by utilizing a magnetic field formed by a stator winding having a conventional configuration. So that the R-Fe-B
Magnetization can be performed up to the magnet characteristic level very close to the magnet characteristics inherent to the magnet, which greatly contributes to the characteristics variation and improvement of heat resistance as a rotating electric machine. (2) The R-Fe-B magnet for field incorporated in the unmagnetized state in the permanent magnet field type rotating electric machine can be almost uniformly and safely magnetized, so that a high-performance rotating electric machine can be stably manufactured. This is a useful tool that ensures the safety of assembly work. (3) The working cost of the sintered magnet used as the field magnet can be reduced while maintaining good characteristics of the rotating electric machine.

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

【図1】本発明の回転電機の一態様を示す要部断面図で
ある。
FIG. 1 is a sectional view of a main part showing one embodiment of a rotating electric machine according to the present invention.

【図2】図1の固定子側巻線および着磁用電源として使
用したコンデンサの結線の模式図を示している。
FIG. 2 is a schematic diagram of connection between a stator-side winding and a capacitor used as a power supply for magnetization in FIG. 1;

【図3】本発明におけるコンデンサ充電電圧と着磁率と
の関係を示す図である。
FIG. 3 is a diagram showing a relationship between a capacitor charging voltage and a magnetization rate in the present invention.

【図4】比較例におけるコンデンサ充電電圧と着磁率と
の関係を示す図である。
FIG. 4 is a diagram showing a relationship between a capacitor charging voltage and a magnetization rate in a comparative example.

【図5】本発明に組み込まれる回転子の他の態様を示す
要部断面図である。
FIG. 5 is a sectional view of a main part showing another embodiment of a rotor incorporated in the present invention.

【図6】本発明に組み込まれる回転子のさらに他の態様
を示す要部断面図である。
FIG. 6 is a cross-sectional view of a main part showing still another embodiment of a rotor incorporated in the present invention.

【図7】本発明に組み込まれる回転子のさらに他の態様
を示す要部断面図である。
FIG. 7 is a cross-sectional view of a main part showing still another embodiment of the rotor incorporated in the present invention.

【図8】磁石単体着磁における着磁磁界の強さと着磁率
との関係を示す図である。
FIG. 8 is a diagram showing the relationship between the strength of a magnetizing magnetic field and the magnetizing rate in magnetizing a single magnet.

【図9】初期磁化曲線を説明する図である。FIG. 9 is a diagram illustrating an initial magnetization curve.

【図10】有効磁界の強さと着磁率との関係を示す図で
ある。
FIG. 10 is a diagram showing the relationship between the strength of the effective magnetic field and the magnetization rate.

【図11】従来の回転子を示す斜視図である。FIG. 11 is a perspective view showing a conventional rotor.

【図12】従来の回転電機を示す要部断面図である。FIG. 12 is a sectional view of a main part showing a conventional rotating electric machine.

【符号の説明】[Explanation of symbols]

1 界磁用磁石、1a,71a,81a,91a 端
面、1b,71b,81b,91b 着磁対向面、2,
72,82,92 回転子コア(鉄芯)、3,74,8
4,94 空間、4 エアギャップ、5,73,83,
93 回転軸、10 回転電機、21 コンデンサ、5
0,70,80,90 回転子、71 弧状磁石、81
ブロック磁石、91 断面U字形磁石、101 回転
軸、102回転子コア、103 界磁用磁石、104
固定子、105 回転子、106エアギャップ、108
凹部、109,109U,109V,109W 歯、
110 固定子コア、115 U相巻線、116 V相
巻線、117 W相巻線、200 回転電機。
1 magnet for field, 1a, 71a, 81a, 91a end face, 1b, 71b, 81b, 91b
72, 82, 92 Rotor core (iron core), 3, 74, 8
4,94 spaces, 4 air gaps, 5,73,83,
93 rotating shaft, 10 rotating electric machine, 21 capacitor, 5
0, 70, 80, 90 rotor, 71 arc-shaped magnet, 81
Block magnet, 91 section U-shaped magnet, 101 rotating shaft, 102 rotor core, 103 field magnet, 104
Stator, 105 rotor, 106 air gap, 108
Recess, 109, 109U, 109V, 109W teeth,
110 stator core, 115 U-phase winding, 116 V-phase winding, 117 W-phase winding, 200 rotating electric machine.

───────────────────────────────────────────────────── フロントページの続き (72)発明者 佐々木 崇 埼玉県熊谷市三ケ尻5200番地日立金属株式 会社磁性材料研究所内 ──────────────────────────────────────────────────続 き Continuing on the front page (72) Inventor Takashi Sasaki 5200 Mikajiri, Kumagaya-shi, Saitama Magnetic Materials Research Laboratory, Hitachi Metals, Ltd.

Claims (6)

【特許請求の範囲】[Claims] 【請求項1】 回転子コア内部にR−Fe−B磁石(R
はYを含めたNd,Dy等の希土類元素の1種または2
種以上)を有した内部磁石型回転子を備えた永久磁石界
磁型回転電機であって、 前記回転子単独の状態におけるR−Fe−B磁石のパー
ミアンス係数(Pcm)と残留磁束密度(Br:kG)
とが、(Pcm+1)>Br/7 の関係を満たすこと
を特徴とする永久磁石界磁型回転電機。
An R-Fe-B magnet (R) is provided inside a rotor core.
Is one or two of rare earth elements such as Nd and Dy including Y
And a permanent magnet field type rotating electric machine provided with an internal magnet type rotor having a permeance coefficient (Pcm) and a residual magnetic flux density (Br) of the R-Fe-B magnet in a state of the rotor alone. : KG)
Satisfies the following relationship: (Pcm + 1)> Br / 7.
【請求項2】 複数の固定子磁極とこの固定子磁極に回
転磁界を発生する巻線とを有した固定子と、 回転軸とこの回転軸に設けられて前記固定子磁極に対向
して回転するとともに回転子コア内部にR−Fe−B磁
石(RはYを含めたNd,Dy等の希土類元素の1種ま
たは2種以上)とそのR−Fe−B磁石の端部に空間を
有した内部磁石型回転子と、 前記固定子磁極に対向する前記回転子の磁極位置を検出
してその位置に応じて前記巻線に電流を供給する制御回
路とを有し、 前記回転子単独の状態におけるR−Fe−B磁石のパー
ミアンス係数(Pcm)と残留磁束密度(Br:kG)
とが、 (Pcm+1)>Br/7 の関係を満たすこ
とを特徴とする永久磁石界磁型回転電機。
A stator having a plurality of stator magnetic poles and a winding for generating a rotating magnetic field in the stator magnetic pole; a rotating shaft and a rotating shaft provided on the rotating shaft and opposed to the stator magnetic pole; At the same time, there is an R-Fe-B magnet (R is one or two or more rare earth elements such as Nd and Dy including Y) inside the rotor core and a space at the end of the R-Fe-B magnet. And a control circuit for detecting a magnetic pole position of the rotor facing the stator magnetic pole and supplying a current to the winding according to the position, and Permeance coefficient (Pcm) and residual magnetic flux density (Br: kG) of the R-Fe-B magnet in the state
Satisfies the following relationship: (Pcm + 1)> Br / 7.
【請求項3】 回転子コア内部に焼結磁石を有した内部
磁石型回転子を備えた永久磁石界磁型回転電機であっ
て、 前記焼結磁石の表面に未加工の黒皮部分を有するととも
に、その黒皮部分が前記回転子コア内部に設けられた空
間に対向配置されることを特徴とする永久磁石界磁型回
転電機。
3. A permanent magnet field type rotating electric machine having an internal magnet type rotor having a sintered magnet inside a rotor core, wherein the surface of the sintered magnet has a raw black scale portion. A permanent magnet field type rotating electric machine, wherein a black skin portion is arranged to face a space provided inside the rotor core.
【請求項4】 前記回転子コアは珪素鋼、磁性ステンレ
ス鋼、軟鉄、パーマロイ、非晶質軟磁性合金、ナノ結晶
粒軟磁性合金のいずれか1種または2種以上を用いて形
成されることを特徴とする請求項1乃至3のいずれかに
記載の永久磁石界磁型回転電機。
4. The rotor core is formed using one or more of silicon steel, magnetic stainless steel, soft iron, permalloy, amorphous soft magnetic alloy, and nanocrystalline soft magnetic alloy. The permanent magnet field type rotating electric machine according to any one of claims 1 to 3, characterized in that:
【請求項5】 前記の界磁用磁石と回転子コアの外周面
との間の回転子コアの最小厚みを0.5〜5mmとした
ことを特徴とする請求項1乃至4のいずれかに記載の永
久磁石界磁型回転電機。
5. The rotor core according to claim 1, wherein a minimum thickness of the rotor core between the field magnet and an outer peripheral surface of the rotor core is 0.5 to 5 mm. A permanent magnet field type rotating electric machine as described in the above.
【請求項6】 複数の固定子磁極とこの固定子磁極に回
転磁界を発生する巻線を有した固定子と、 回転軸とこの回転軸に設けられて前記固定子磁極に対向
して回転するとともに回転子コア内部にR−Fe−B磁
石(RはYを含めたNd,Dy等の希土類元素の1種ま
たは2種以上)を有した内部磁石型回転子と、 前記固定子磁極に対向する前記回転子の磁極位置を検出
してその位置に応じて前記巻線に電流を供給する制御回
路とを有した永久磁石界磁型回転電機の製造方法におい
て、 前記回転子単独状態におけるR−Fe−B磁石のパーミ
アンス係数(Pcm)と残留磁束密度(Br:kG)と
が、(Pcm+1)>Br/7 の関係を満足するよう
に前記回転子を構成した後、その回転子をエアギャップ
を介して前記固定子に対向配置して永久磁石界磁型回転
電機を構成し、その後前記巻線に通電することにより発
生する磁界で前記R−Fe−B磁石を着磁することを特
徴とする永久磁石界磁型回転電機の製造方法。
6. A stator having a plurality of stator magnetic poles, a stator having a winding for generating a rotating magnetic field at the stator magnetic poles, a rotating shaft and a rotating shaft provided to rotate opposite to the stator magnetic poles. And an internal magnet type rotor having an R-Fe-B magnet (R is one or two or more rare earth elements such as Nd and Dy including Y) inside the rotor core, and facing the stator magnetic pole. And a control circuit for detecting a magnetic pole position of the rotor and supplying a current to the winding according to the detected position. After the rotor is configured so that the permeance coefficient (Pcm) and the residual magnetic flux density (Br: kG) of the Fe-B magnet satisfy the relationship of (Pcm + 1)> Br / 7, the rotor is air-gapped. And placed opposite to the stator via A method of manufacturing a permanent magnet field type rotating electric machine, comprising: constructing a permanent magnet field type rotating electric machine, and thereafter magnetizing the R-Fe-B magnet with a magnetic field generated by energizing the winding. .
JP9069570A 1997-03-24 1997-03-24 Permanent magnet field type rotating electric machine and method of manufacturing the same Pending JPH10271723A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP9069570A JPH10271723A (en) 1997-03-24 1997-03-24 Permanent magnet field type rotating electric machine and method of manufacturing the same

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP9069570A JPH10271723A (en) 1997-03-24 1997-03-24 Permanent magnet field type rotating electric machine and method of manufacturing the same

Publications (1)

Publication Number Publication Date
JPH10271723A true JPH10271723A (en) 1998-10-09

Family

ID=13406585

Family Applications (1)

Application Number Title Priority Date Filing Date
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Country Link
JP (1) JPH10271723A (en)

Cited By (8)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JP2001327130A (en) * 2000-05-18 2001-11-22 Aichi Emerson Electric Co Ltd Permanent magnet motor stator
JP2002369478A (en) * 2001-06-05 2002-12-20 Yaskawa Electric Corp Permanent magnet synchronous motor
WO2003081748A1 (en) * 2002-03-22 2003-10-02 Ebm-Papst St. Georgen Gmbh & Co. Kg Inner rotor motor
JP2005304178A (en) * 2004-04-12 2005-10-27 Ichinomiya Denki:Kk Rotor for brushless motor and brushless motor
JP2015019504A (en) * 2013-07-10 2015-01-29 住友重機械工業株式会社 Permanent magnet motor and magnetizing method thereof
JP2015208134A (en) * 2014-04-21 2015-11-19 日産自動車株式会社 Method for manufacturing sintered magnet
JP2019221127A (en) * 2018-06-19 2019-12-26 トヨタ自動車株式会社 Magnet embedded motor and manufacturing method thereof
JP2020039251A (en) * 2019-10-29 2020-03-12 日立金属株式会社 Sintered magnet for motor, method of manufacturing the same, and permanent magnet type synchronous motor

Cited By (8)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JP2001327130A (en) * 2000-05-18 2001-11-22 Aichi Emerson Electric Co Ltd Permanent magnet motor stator
JP2002369478A (en) * 2001-06-05 2002-12-20 Yaskawa Electric Corp Permanent magnet synchronous motor
WO2003081748A1 (en) * 2002-03-22 2003-10-02 Ebm-Papst St. Georgen Gmbh & Co. Kg Inner rotor motor
JP2005304178A (en) * 2004-04-12 2005-10-27 Ichinomiya Denki:Kk Rotor for brushless motor and brushless motor
JP2015019504A (en) * 2013-07-10 2015-01-29 住友重機械工業株式会社 Permanent magnet motor and magnetizing method thereof
JP2015208134A (en) * 2014-04-21 2015-11-19 日産自動車株式会社 Method for manufacturing sintered magnet
JP2019221127A (en) * 2018-06-19 2019-12-26 トヨタ自動車株式会社 Magnet embedded motor and manufacturing method thereof
JP2020039251A (en) * 2019-10-29 2020-03-12 日立金属株式会社 Sintered magnet for motor, method of manufacturing the same, and permanent magnet type synchronous motor

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