JPH0688159A - Rare earth magnet and rare earth magnet alloy powder as well as production therefor - Google Patents

Rare earth magnet and rare earth magnet alloy powder as well as production therefor

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Publication number
JPH0688159A
JPH0688159A JP5085290A JP8529093A JPH0688159A JP H0688159 A JPH0688159 A JP H0688159A JP 5085290 A JP5085290 A JP 5085290A JP 8529093 A JP8529093 A JP 8529093A JP H0688159 A JPH0688159 A JP H0688159A
Authority
JP
Japan
Prior art keywords
rare earth
earth magnet
phase
alloy powder
heat treatment
Prior art date
Legal status (The legal status is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the status listed.)
Granted
Application number
JP5085290A
Other languages
Japanese (ja)
Other versions
JP2999648B2 (en
Inventor
Hirokazu Kanekiyo
裕和 金清
Satoru Hirozawa
哲 広沢
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.)
Hitachi Metals Ltd
Original Assignee
Sumitomo Special Metals Co Ltd
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Classifications

    • HELECTRICITY
    • H01ELECTRIC ELEMENTS
    • H01FMAGNETS; INDUCTANCES; TRANSFORMERS; SELECTION OF MATERIALS FOR THEIR MAGNETIC PROPERTIES
    • H01F1/00Magnets or magnetic bodies characterised by the magnetic materials therefor; Selection of materials for their magnetic properties
    • H01F1/01Magnets or magnetic bodies characterised by the magnetic materials therefor; Selection of materials for their magnetic properties of inorganic materials
    • H01F1/03Magnets or magnetic bodies characterised by the magnetic materials therefor; Selection of materials for their magnetic properties of inorganic materials characterised by their coercivity
    • H01F1/032Magnets or magnetic bodies characterised by the magnetic materials therefor; Selection of materials for their magnetic properties of inorganic materials characterised by their coercivity of hard-magnetic materials
    • H01F1/04Magnets or magnetic bodies characterised by the magnetic materials therefor; Selection of materials for their magnetic properties of inorganic materials characterised by their coercivity of hard-magnetic materials metals or alloys
    • H01F1/047Alloys characterised by their composition
    • H01F1/053Alloys characterised by their composition containing rare earth metals
    • H01F1/055Alloys characterised by their composition containing rare earth metals and magnetic transition metals, e.g. SmCo5
    • H01F1/057Alloys characterised by their composition containing rare earth metals and magnetic transition metals, e.g. SmCo5 and IIIa elements, e.g. Nd2Fe14B
    • H01F1/0571Alloys characterised by their composition containing rare earth metals and magnetic transition metals, e.g. SmCo5 and IIIa elements, e.g. Nd2Fe14B in the form of particles, e.g. rapid quenched powders or ribbon flakes

Abstract

PURPOSE:To stably produce rare earth magnet alloy powder having excellent magnetic properties at low cost by subjecting the molten metal of an alloy having a specified compsn. constituted of Fe, Co, B and Pr or Nd, Ag or the like to ultrarapid solidification and executing specified heat treatment. CONSTITUTION:The molten metal of an alloy expressed by Fe100-x-y-zCoxByRzMw (R denotes Pr or Nd and M denotes Ag, Al Si as well as 0.05<=x<=15at%, 1.6<=y<=22%, 3<=z<=5.5% and 0.1<=w<=3% are satisfied) is subjected to ultrarapid solidification to form its structure into a one in which >=90% is substantially constituted of amorphous one. The temp. of this alloy is raised at 1 to 15 deg.C/min temp. rising rate from 500 deg.C, and it is held at 550 to 700 deg.C for 30sec to 6hr. By this heat treatment, the aggregate of fine crystals consisting of Fe3B type compounds as the main phase, having a ferromagnetic phase with an Nd2Fe14B type crystalline structure and having 0.01 to 0.1mum average crystalline grains is obtd., which is thereafter pulverized to regulate its average grain size into 3 to 500mum. In this way, the rare earth magnet alloy powder having magnetic properties of iHc<=3kOe, Br>=8kG and (BH)max>=8MGOe can be obtd.

Description

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

【0001】[0001]

【産業上の利用分野】この発明は、モーターやアクチュ
エーターなどに最適な希土類焼結磁石やボンド磁石に係
り、希土類元素の含有量が少ない特定組成のFe−Co
−B−R合金溶湯を超急冷法にてアモルファス組織とな
し、特定の熱処理にて微細結晶集合体を得ることによ
り、ハードフェライト磁石では得られなかった5kG以
上の残留磁束密度Brを有するボンド磁石に最適の希土
類磁石合金粉末を得る製造方法に関する。
BACKGROUND OF THE INVENTION 1. Field of the Invention The present invention relates to a rare earth sintered magnet or a bonded magnet most suitable for a motor, an actuator, etc., and Fe-Co of a specific composition containing a small amount of rare earth elements.
-A bond magnet having a residual magnetic flux density Br of 5 kG or more, which cannot be obtained by a hard ferrite magnet, by forming an amorphous structure of a molten BR alloy by a super-quenching method and obtaining a fine crystal aggregate by a specific heat treatment. The present invention relates to a manufacturing method for obtaining an optimal rare earth magnet alloy powder.

【0002】[0002]

【従来の技術】電装品用モーターやアクチュエーターな
どに使用される永久磁石は主にハードフェライト磁石に
限定されていたが、低温でのiHc低下に伴う低温減
磁、セラミックス材質のために機械的強度が低くて割
れ、欠けが発生し易いこと、複雑な形状が得難いことな
どの問題があった。
2. Description of the Related Art Permanent magnets used in motors and actuators for electrical equipment have been mainly limited to hard ferrite magnets, but they have low mechanical strength due to low temperature demagnetization accompanying iHc reduction at low temperatures and ceramic materials. However, there were problems such as low hardness, easy cracking and chipping, and difficulty in obtaining a complicated shape.

【0003】今日、自動車は省資源のため車両の軽量化
による燃費の向上が強く要求されており、自動車用電装
品はより一層の小型、軽量化が求められている。また、
自動車用電装品以外の家電用モーターなどの用途におい
ても、性能対重量比を最大にするための設計が検討され
ており、現在のモーター構造では磁石材料としてBrが
5〜7kG程度のものが最適とされている。すなわち、
使用する磁石材料のBrが8kG以上の場合、現在のモ
ーター構造では磁路となる回転子やステーターの鉄板の
断面積を増大させる必要があり、重量の増大を招来する
が、Brが5〜7kGであれば性能対重量比を最大にす
ることができる。
Nowadays, automobiles are strongly required to reduce fuel consumption in order to save resources and to improve fuel efficiency, and electric components for automobiles are required to be further reduced in size and weight. Also,
Designs for maximizing the performance-to-weight ratio are also being considered for applications such as home electric motors other than automobile electrical components. In the current motor structure, magnet materials with Br of about 5 to 7 kG are optimal. It is said that. That is,
When the magnet material used has a Br of 8 kG or more, the current motor structure requires an increase in the cross-sectional area of the iron plate of the rotor or stator that becomes the magnetic path, which causes an increase in weight. If so, the performance-to-weight ratio can be maximized.

【0004】従って、小型モーター用の磁石材料は磁気
特性的には特に5kG以上の残留磁束密度Brが要求さ
れているが、従来のハードフェライト磁石では得ること
ができない。例えばNd−Fe−B系ボンド磁石ではか
かる磁気特性を満足するが、金属の分離精製や還元反応
に多大の工程並びに大規模な設備を要するNd等を10
〜15at%含有しているため、ハードフェライト磁石
に比較して著しく高価であり、現在のところ大量生産が
可能で安価に提供できるBrが5〜7kG程度の磁石材
料は、見出されていない。
Therefore, a magnetic material for a small motor is required to have a residual magnetic flux density Br of 5 kG or more in terms of magnetic characteristics, but it cannot be obtained with a conventional hard ferrite magnet. For example, Nd-Fe-B based bonded magnets satisfy such magnetic characteristics, but Nd, etc., which require a large number of steps and a large-scale facility for separation and purification of metals and reduction reaction.
Since it is contained at ˜15 at%, it is remarkably expensive as compared with a hard ferrite magnet, and at present, a magnet material with a Br of about 5 to 7 kG that can be mass-produced and can be provided at low cost has not been found.

【0005】[0005]

【発明が解決しようとする課題】一方、Nd−Fe−B
系磁石において、最近、Nd4Fe7719(at%)近
傍でFe3B型化合物を主相とする磁石材料が提案
(R.Coehoorn等、J.de Phys.、C
8,1988,669〜670頁)された。この磁石材
料はアモルファスリボンを熱処理することにより、Fe
3BとNd2Fe14Bの結晶集合組織を有する準安定構造
であるが、iHcが2〜3kOe程度と高くなく、また
このiHcを得るための熱処理条件が狭く限定され、工
業生産上実用的でない。
On the other hand, Nd-Fe-B
Recently, a magnet material having a Fe 3 B type compound as a main phase in the vicinity of Nd 4 Fe 77 B 19 (at%) has been proposed (R. Coehorn et al., J. de Phys., C).
8, 1988, pp. 669-670). This magnet material is made of Fe by heat treatment of the amorphous ribbon.
Although it is a metastable structure having a crystal texture of 3 B and Nd 2 Fe 14 B, iHc is not so high as about 2 to 3 kOe, and the heat treatment conditions for obtaining this iHc are narrowly limited, which is practical for industrial production. Not.

【0006】このFe3B型化合物を主相とする磁石材
料に添加元素を加えて多成分化し、性能向上を図った研
究が発表されている。その1つは希土類元素にNdのほ
かにDyとTbを用いてiHcの向上を図るものである
が、高価な元素を添加する問題のほか、添加希土類元素
はその磁気モーメントがNdやFeの磁気モーメントと
反平行して結合するため磁化が減少する問題がある
(R.Coehoorn、J.Magn,Magn,M
at、83(1990)228〜230頁)。
[0006] A study has been published in which an additive element is added to the magnetic material having the Fe 3 B type compound as a main phase to make it a multi-component to improve the performance. One of them is to improve iHc by using Dy and Tb in addition to Nd as a rare earth element. However, in addition to the problem of adding an expensive element, the added rare earth element has a magnetic moment of Nd or Fe. There is a problem that the magnetization decreases due to coupling in antiparallel to the moment (R. Coehoorn, J. Magn, Magn, M
at, 83 (1990) 228-230).

【0007】他の研究(Shen Bao−genら、
J.Magn,Magn,Mat、89(1991)3
35〜340頁)として、 Feの一部をCoにて置換
してキュリー温度を上昇させ、iHcの温度係数を改善
するものであるが、Coの添加にともないBrを低下さ
せる問題がある。
Other studies (Shen Bao-gen et al.,
J. Magn, Magn, Mat, 89 (1991) 3
35 to 340), a part of Fe is replaced with Co to raise the Curie temperature and improve the temperature coefficient of iHc, but there is a problem that Br is lowered with the addition of Co.

【0008】いずれにしてもFe3B型Nd−Fe−B
系磁石は、超急冷法によりアモルファス化した後、熱処
理してハード磁石材料化できるが、iHcが低く、かつ
前記熱処理条件が苛酷であり、添加元素にて高iHc化
を図ると磁気エネルギー積が低下するなど、安定した工
業生産ができず、ハードフェライト磁石の代替えとして
安価に提供することができない。
In any case, Fe 3 B type Nd-Fe-B
The system magnet can be made into a hard magnet material by heat treatment after it is made amorphous by the ultra-quenching method, but iHc is low and the heat treatment conditions are severe, and when the iHc is increased by the additive element, the magnetic energy product is increased. It is not possible to provide stable industrial production such as deterioration, and it cannot be provided at a low cost as an alternative to the hard ferrite magnet.

【0009】また、Nd−Fe−B系合金をアモルファ
ス化するためには、超急冷時のロール周速度を著しく速
くする必要があり、製品の回収率や歩留りが低下する問
題があり、さらにFe基合金であることから、保存時の
腐食が進行し易く、長期間の保存により初期の磁気特性
が維持できずに劣化する問題があった。
Further, in order to amorphize the Nd-Fe-B system alloy, it is necessary to remarkably increase the roll peripheral speed during the ultra-quenching, which causes a problem that the product recovery rate and the yield decrease. Since it is a base alloy, there is a problem that corrosion during storage tends to proceed, and the initial magnetic characteristics cannot be maintained and deteriorates after long-term storage.

【0010】この発明は、Fe3B型Fe−B−R系磁
石(Rは希土類元素)に着目して、iHcと(BH)m
axを向上させ、安定した工業生産が可能な製造方法の
確立と、5kG以上の残留磁束密度Brを有しハードフ
ェライト磁石の代替えとして安価に提供できるFe3
型Nd−Fe−B系磁石を目的としている。
The present invention focuses on an Fe 3 B type Fe-BR magnet (R is a rare earth element), iHc and (BH) m
Fe 3 B that can improve the ax and establish a manufacturing method that enables stable industrial production and has a residual magnetic flux density Br of 5 kG or more and can be provided at a low cost as an alternative to a hard ferrite magnet.
Aims to be a type Nd-Fe-B system magnet.

【0011】[0011]

【課題を解決するための手段】この発明は、Fe3B型
系Fe−B−R磁石のiHcと(BH)maxを向上さ
せ、安定した工業生産が可能な製造方法を目的に種々検
討した結果、希土類元素の含有量が少なく、Co及びA
g、Al、Siの少なくとも1種を少量添加した鉄基の
特定組成の合金溶湯を超急冷法にてアモルファス組織と
なし、特定の昇温速度による熱処理にて微細結晶集合体
を得ることにより、ハードフェライト磁石では得られな
かった5kG以上の残留磁束密度Brを有するボンド磁
石に最適の希土類磁石合金粉末が得られることを知見
し、この発明を完成した。
The present invention has been variously studied for the purpose of improving the iHc and (BH) max of Fe 3 B type Fe-B-R magnets and enabling a stable industrial production. As a result, the content of rare earth elements is low, and Co and A
g, Al, by forming a small amount of at least one of Si, an alloy melt of a specific iron-based composition into an amorphous structure by the ultra-quenching method, and obtaining a fine crystal aggregate by heat treatment at a specific heating rate, The inventors have found that an optimum rare earth magnet alloy powder can be obtained for a bond magnet having a residual magnetic flux density Br of 5 kG or more, which could not be obtained with a hard ferrite magnet, and completed the present invention.

【0012】この発明は、組成式をFe100-x-y-zCox
yzw (但しRはPrまたはNdの1種または2
種、MはAg、AlまたはSiの1種または2種以上)
と表し、組成範囲を限定する記号x、y、z、wが下記
値を満足し、Fe3B型化合物を主相とし、Nd2Fe14
B型結晶構造を有する強磁性相を有し、平均結晶粒径が
0.01〜0.1μmの微細結晶集合体からなることを
特徴とする希土類磁石である。 0.05≦x≦15at% 16≦y≦22at% 3≦z≦5.5at% 0.1≦w≦3at%
This invention uses the composition formula Fe 100-xyz Co x
B y R z M w (where R is Pr or Nd, one or two)
Seed, M is Ag, Al or Si, one or more kinds)
And the symbols x, y, z, and w that limit the composition range satisfy the following values, the Fe 3 B type compound is the main phase, and Nd 2 Fe 14
A rare earth magnet having a ferromagnetic phase having a B-type crystal structure and comprising a fine crystal aggregate having an average crystal grain size of 0.01 to 0.1 μm. 0.05 ≦ x ≦ 15 at% 16 ≦ y ≦ 22 at% 3 ≦ z ≦ 5.5 at% 0.1 ≦ w ≦ 3 at%

【0013】また、この発明は、組成式をFe
100-x-y-zCoxyzw (但しRはPrまたはNd
の1種または2種、MはAg、AlまたはSiの1種ま
たは2種以上)と表し、組成範囲を限定する記号x、
y、z、wが上述の値を満足し、Fe3B型化合物を主
相とし、Nd2Fe14B型結晶構造を有する強磁性相を
有し、平均結晶粒径が0.01〜0.1μmの微細結晶
集合体からなり、平均粒径が3〜500μm、磁気特性
がiHc≧3kOe、Br≧8kG、(BH)max≧
8MGOeであることを特徴とする希土類磁石合金粉末
である。
Further, the present invention uses the composition formula Fe
100-xyz Co x B y R z M w ( where R is Pr or Nd
1 or 2 of M, 1 or 2 or more of Ag, Al or Si), and a symbol x for limiting the composition range,
y, z and w satisfy the above values, Fe 3 B type compound as a main phase, a ferromagnetic phase having an Nd 2 Fe 14 B type crystal structure, and an average crystal grain size of 0.01 to 0. It is composed of a fine crystal aggregate of 1 μm, has an average grain size of 3 to 500 μm, and has magnetic properties of iHc ≧ 3 kOe, Br ≧ 8 kG, (BH) max ≧.
It is a rare earth magnet alloy powder characterized by being 8 MGOe.

【0014】また、この発明は、(1)組成式をFe
100-x-y-zCoxyzw (但しRはPrまたはNd
の1種または2種、MはAg、AlまたはSiの1種ま
たは2種以上)と表し、組成範囲を限定する記号x、
y、z、wが上述の値を満足する合金溶湯を超急冷法に
て実質的に90%以上をアモルファス組織となし、
(2)さらに熱処理に際し500℃からの昇温速度を1
〜15℃/分で昇温して550〜700℃で30秒〜6
時間保持する熱処理を施し、(3)Fe3B型化合物を
主相とし、Nd2Fe14B型結晶構造を有する強磁性相
を有し、平均結晶粒径が0.01〜0.1μmの微細結
晶集合体を得たのち、(4)これを粉砕して磁石合金粉
末を得ることを特徴とする希土類磁石合金粉末の製造方
法である。
Further, according to the present invention, the composition formula (1) is represented by Fe
100-xyz Co x B y R z M w ( where R is Pr or Nd
1 or 2 of M, 1 or 2 or more of Ag, Al or Si), and a symbol x for limiting the composition range,
The alloy melt in which y, z, and w satisfy the above-mentioned values is made into an amorphous structure by substantially 90% or more by the superquenching method,
(2) In the heat treatment, the temperature rising rate from 500 ° C is set to 1
Temperature rises at -15 ° C / min and 550-700 ° C for 30 seconds-6
A heat treatment for holding for a period of time (3) having a ferromagnetic phase having a Fe 3 B type compound as a main phase and an Nd 2 Fe 14 B type crystal structure and an average crystal grain size of 0.01 to 0.1 μm A method for producing a rare earth magnet alloy powder, comprising: (4) pulverizing the fine crystal aggregate to obtain a magnet alloy powder.

【0015】[0015]

【作用】この発明は、希土類元素の含有量が少ない特定
組成のFe−Co−B−R−M系合金溶湯を超急冷法に
て実質的に90%以上をアモルファス組織となすと、特
定量のCoを含有するためアモルファス薄帯の回収率が
著しく向上し、さらに得られたフレーク、リボンを50
0℃以上から1〜15℃/分の昇温速度で昇温した後、
550〜700℃で30秒〜6時間保持する熱処理を施
すことにより、平均結晶粒径が0.01〜0.1μmの
微細結晶集合体となり、主相のFe3B型化合物相のほ
か、Nd2Fe14B型結晶構造相を有する強磁性相の量
比が増大し、α−Fe相が減少し、Ag、Al、Siを
含有するためCoを含有してもBrの低下がなく、さら
に減磁曲線の角型性が改善されることにより、iHc≧
3kOe、Br≧8kG、(BH)max≧8MGOe
の磁気特性が得られ、さらにこれを粉砕して磁石合金粉
末化することによって、5kG以上の残留磁束密度Br
を有するボンド磁石に最適のFe−Co−B−R−M系
磁石合金粉末を得ることができ、また焼結磁石化するこ
とにより従来のアルニコ系磁石と同等以上の磁気特性を
得ることができる。
According to the present invention, when a Fe-Co-B-R-M type alloy melt having a specific composition containing a small amount of rare earth elements is made to have an amorphous structure in an amount of substantially 90% or more by an ultra-quenching method, the specific amount is Since it contains Co, the recovery rate of amorphous ribbon is significantly improved, and the obtained flakes and ribbons are
After raising the temperature from 0 ° C. or higher at a heating rate of 1 to 15 ° C./min,
By performing a heat treatment of holding at 550 to 700 ° C. for 30 seconds to 6 hours, a fine crystal aggregate having an average crystal grain size of 0.01 to 0.1 μm is formed, and in addition to the Fe 3 B type compound phase of the main phase, Nd The amount ratio of the ferromagnetic phase having the 2 Fe 14 B-type crystal structure phase is increased, the α-Fe phase is decreased, and since Ag, Al, and Si are contained, even if Co is contained, Br does not decrease. Since the squareness of the demagnetization curve is improved, iHc ≧
3 kOe, Br ≧ 8 kG, (BH) max ≧ 8 MGOe
Magnetic properties are obtained, and by further pulverizing this to make a magnetic alloy powder, the residual magnetic flux density Br of 5 kG or more is obtained.
The optimum Fe-Co-B-R-M based magnet alloy powder can be obtained for the bonded magnet having the above-mentioned properties, and it is possible to obtain the magnetic characteristics equal to or higher than those of the conventional alnico based magnet by making the sintered magnet. .

【0016】組成の限定理由 希土類元素RはPrまたはNdの1種また2種を特定量
含有のときのみ、高い磁気特性が得られ、他の希土類、
例えばCe、LaではiHcが2kOe以上の特性が得
られず、またSm以降の中希土類元素、重希土類元素は
磁気特性の劣化を招来するとともに磁石を高価格にする
ため好ましくない。Rは、3at%未満では2kOe以
上のiHcが得られず、また6at%を超えるとFe3
B相が生成せず、硬磁性を示さない準安定相のR2Fe
233相が折出しiHcは著しく低下するので好ましく
ないため、3〜5.5at%の範囲とする。
Reasons for limiting the composition The rare earth element R has high magnetic properties only when it contains one or two Pr or Nd in a specific amount.
For example, in the case of Ce and La, the characteristic that iHc is 2 kOe or more cannot be obtained, and medium rare earth elements and heavy rare earth elements after Sm cause deterioration of magnetic characteristics and make the magnet expensive, which is not preferable. If R is less than 3 at%, iHc of 2 kOe or more cannot be obtained, and if it exceeds 6 at%, Fe 3
A metastable phase R 2 Fe that does not form B phase and does not exhibit hard magnetism
23 B 3 phase is unfavorable because the iHc is significantly lowered, and the range is 3 to 5.5 at%.

【0017】Bは、16at%未満および22at%を
超えると2kOe以上のiHcが得られないため、16
〜22at%の範囲とする。
When B is less than 16 at% or more than 22 at%, iHc of 2 kOe or more cannot be obtained.
The range is -22 at%.

【0018】Coは、iHc及び減磁曲線の角型性の向
上改善に有効であるが、0.05at%未満ではかかる
効果が得られず、15at%を超えるとiHcは著しく
低下し、2kOe以上のiHcが得られないため、0.
05〜15at%の範囲とする。
Co is effective for improving the squareness of iHc and the demagnetization curve, but if it is less than 0.05 at%, such an effect cannot be obtained, and if it exceeds 15 at%, iHc is remarkably reduced and 2 kOe or more. IHc cannot be obtained, so 0.
The range is from 05 to 15 at%.

【0019】Ag、Al、Siは熱処理温度範囲を拡大
して減磁曲線の角型性を改善し、磁気特性のBr、(B
H)maxを増大させる効果を有し、かかる効果を得る
には少なくとも0.1at%以上の添加が必要である
が、3at%を超えるとかえって角型性を劣化させ、
(BH)maxも低下するため、0.1〜3at%の範
囲とする。
Ag, Al, and Si improve the squareness of the demagnetization curve by expanding the heat treatment temperature range, and Br, (B
H) max has the effect of increasing, and at least 0.1 at% or more must be added to obtain such an effect, but if it exceeds 3 at%, the squareness is rather deteriorated,
Since (BH) max also decreases, the range is set to 0.1 to 3 at%.

【0020】Feは、上述の元素の含有残余を占める。Fe occupies the remaining content of the above elements.

【0021】製造条件の限定理由 この発明において、上述の特定組成の合金溶湯を超急冷
法にてアモルファスとなし、500℃以上から1〜15
℃/分の昇温速度で昇温した後、550〜700℃で3
0秒〜6時間保持する熱処理を施すことにより、熱力学
的には準安定相であるFe3B型化合物とNd2Fe14
型結晶構造を有する強磁性相を有し、平均結晶粒径が
0.01〜0.1μmの微細結晶集合体として得ること
が最も重要であり、合金溶湯の超急冷処理には公知の回
転ロールを用いた超急冷法を採用することができるが、
実質的に90%以上をアモルファスとなす必要がある。
例えばCu製ロールを用いる場合は、そのロール表面周
速度が10〜50m/秒の範囲が好適な組織が得られる
ため好ましい。すなわち周速度が10m/秒未満ではア
モルファスとならずα−Fe相の析出量が増大して好ま
しくなく、ロール表面周速度が50m/秒を超えると、
急冷された合金が連続的なリボンとして生成せず、合金
片が飛散し、装置から合金を回収する際の回収率や回収
能率が低下して好ましくない。ただし、微量のα−Fe
相が急冷薄帯中に存在しても特性を著しく低下させるも
のでなく許容される。
Reasons for Limiting Manufacturing Conditions In the present invention, the molten alloy having the above-mentioned specific composition is made amorphous by the ultra-quenching method, and the temperature is from 500 ° C. or higher to 1-15.
After raising the temperature at a temperature rising rate of ℃ / min, 3 at 550 ~ 700 ℃
By performing a heat treatment for holding for 0 seconds to 6 hours, the Fe 3 B type compound and Nd 2 Fe 14 B which are thermodynamically metastable phases are obtained.
It is most important to obtain a fine crystal aggregate having a ferromagnetic phase having a type crystal structure and an average crystal grain diameter of 0.01 to 0.1 μm. Although it is possible to adopt the ultra-quenching method using
It is necessary to make substantially 90% or more amorphous.
For example, when a Cu roll is used, a roll surface peripheral velocity in the range of 10 to 50 m / sec is preferable because a suitable structure can be obtained. That is, when the peripheral speed is less than 10 m / sec, it does not become amorphous and the amount of α-Fe phase deposited increases, which is not preferable, and when the roll surface peripheral velocity exceeds 50 m / sec,
The rapidly cooled alloy does not form as a continuous ribbon, the alloy pieces scatter, and the recovery rate and recovery efficiency when recovering the alloy from the apparatus are reduced, which is not preferable. However, a small amount of α-Fe
The presence of phases in the quenched ribbon is acceptable as it does not significantly degrade the properties.

【0022】この発明において、上述の特定組成の合金
溶湯を超急冷法にてアモルファスとなした後、磁気特性
が最高となる熱処理は組成に依存するが、熱処理温度が
550℃未満ではアモルファス相のままで2kOe以上
のiHcが得られず、また700℃を超えると熱平衡相
であるα−Fe相とFe2BまたはNd1.1Fe44相が
生成してiHcが発源しないため、熱処理温度は550
〜700℃に限定する。熱処理雰囲気はArガス中など
の不活性ガス雰囲気が好ましい。
In the present invention, the heat treatment for maximizing the magnetic properties after the alloy melt of the above-mentioned specific composition is made amorphous by the ultra-quenching method depends on the composition, but if the heat treatment temperature is less than 550 ° C. Until iHc of 2 kOe or more cannot be obtained, and if the temperature exceeds 700 ° C, the α-Fe phase and the Fe 2 B or Nd 1.1 Fe 4 B 4 phase that are thermal equilibrium phases are generated and iHc does not originate, so the heat treatment temperature Is 550
Limited to ~ 700 ° C. The heat treatment atmosphere is preferably an inert gas atmosphere such as Ar gas.

【0023】熱処理時間は短くてもよいが、30秒未満
では十分なミクロ組織の生成が行われず、iHc及び減
磁曲線の角型性が劣化し、また6時間を超えると2kO
e以上のiHcが得られないので、熱処理保持時間を3
0秒〜6時間に限定する。
The heat treatment time may be short, but if it is less than 30 seconds, a sufficient microstructure is not formed, iHc and the squareness of the demagnetization curve are deteriorated, and if it exceeds 6 hours, it is 2 kO.
Since iHc above e cannot be obtained, the heat treatment holding time is set to 3
Limited to 0 seconds to 6 hours.

【0024】この発明において重要な特徴として、熱処
理に際して500℃以上からの昇温速度があり、1℃/
分未満の昇温速度では、昇温中にNd2Fe14B相とF
3B相の結晶粒径が大きく成長しすぎてiHcが劣化
し、2kOe以上のiHcが得られない。また、15℃
/分を超える昇温速度では、500℃を通過してから生
成するNd2Fe14B相の析出が十分に行われず、α−
Fe相の析出量が増大して、磁化曲線の第2象限にBr
点近傍に磁化の低下のある減磁曲線となり、(BH)m
axが劣化するため好ましくない。ただし、微量のα−
Fe相の存在は許容できる。なお、熱処理に際して50
0℃未満までは急速加熱などその昇温速度は任意であ
る。
An important feature of the present invention is the rate of temperature increase from 500 ° C. or higher during heat treatment, which is 1 ° C. /
If the heating rate is less than a minute, the Nd 2 Fe 14 B phase and the F
Since the crystal grain size of the e 3 B phase grows too large and iHc deteriorates, iHc of 2 kOe or more cannot be obtained. Also, 15 ℃
If the heating rate exceeds / min, the Nd 2 Fe 14 B phase generated after passing 500 ° C. is not sufficiently precipitated, and α-
The amount of precipitation of the Fe phase increases and Br falls to the second quadrant of the magnetization curve.
It becomes a demagnetization curve with a decrease in magnetization near the point, (BH) m
It is not preferable because ax is deteriorated. However, a small amount of α-
The presence of the Fe phase is acceptable. In addition, at the time of heat treatment, 50
The rate of temperature increase such as rapid heating up to 0 ° C. is arbitrary.

【0025】結晶構造 この発明による希土類磁石並びに希土類磁石合金粉末の
結晶相は、Fe3B型化合物を主相とし、Nd2Fe14
型結晶構造を有する強磁性相を有し、平均結晶粒径が
0.01〜0.1μmの微細結晶集合体からなることを
特徴としている。
Crystal Structure The crystal phase of the rare earth magnet and the rare earth magnet alloy powder according to the present invention is Fe 3 B type compound as a main phase and Nd 2 Fe 14 B.
It is characterized by having a ferromagnetic phase having a type crystal structure and comprising a fine crystal aggregate having an average crystal grain size of 0.01 to 0.1 μm.

【0026】この発明において、磁石合金の平均結晶粒
径が0.1μmを超えると、減磁曲線の角型性が著しく
劣化し、Br≧7kG、(BH)max≧8MGOeの
磁気特性を得ることができない。また、平均結晶粒径は
細かいほど好ましいが、0.01μm未満の平均結晶粒
径を得ることは工業生産上困難であるため、下限を0.
01μmとする。
In the present invention, when the average grain size of the magnet alloy exceeds 0.1 μm, the squareness of the demagnetization curve is significantly deteriorated, and the magnetic properties of Br ≧ 7 kG and (BH) max ≧ 8 MGOe are obtained. I can't. Further, the smaller the average crystal grain size is, the more preferable, but it is difficult to obtain the average crystal grain size of less than 0.01 μm in industrial production.
It is set to 01 μm.

【0027】磁石化方法 特定組成の合金溶湯を超急冷法にてアモルファスとな
し、500℃以上からの昇温速度を1〜10℃/分で昇
温した後、550〜700℃で30秒〜6時間保持する
熱処理を施すことにより、平均結晶粒径が0.01〜
0.1μmの微細結晶集合体として得たこの発明による
希土類磁石合金粉末を用いて磁石化するには、700℃
以下で固化、圧密化できる公知の焼結磁石化方法並びに
ボンド磁石化方法の何れも採用することができ、特に、
当該合金を平均粒径が3〜500μmの合金粉末に粉砕
したのち、公知のバインダーと混合して所要のボンド磁
石となすことにより、5kG以上の残留磁束密度Brを
有するボンド磁石を得ることができる。
Magnetization method A molten alloy having a specific composition is made amorphous by a super-quenching method, the temperature is raised from 500 ° C. or more at a rate of 1 to 10 ° C./minute, and then at 550 to 700 ° C. for 30 seconds to. By performing a heat treatment of holding for 6 hours, the average crystal grain size is 0.01 to
To magnetize using the rare earth magnet alloy powder according to the present invention obtained as a 0.1 μm fine crystal aggregate, 700 ° C.
Any of known sintering magnetizing methods and bond magnetizing methods that can be solidified and consolidated below can be adopted, and in particular,
After crushing the alloy into alloy powder having an average particle size of 3 to 500 μm and mixing it with a known binder to form a required bond magnet, a bond magnet having a residual magnetic flux density Br of 5 kG or more can be obtained. .

【0028】[0028]

【実施例】【Example】

実施例1 表1のNo.1〜5の組成となるように、純度99.5
%以上のFe、Co、B、Nd、Pr、Ag、Al、S
iの金属を用いて、総量が30grとなるように秤量
し、底部に直径0.8mmのオリフィスを有する石英る
つぼ内に投入し、圧力56cmHgのAr雰囲気中で高
周波加熱により溶解し、溶解温度を1400℃にした
後、湯面をArガスにより加圧して室温にてロール周速
度20m/秒にて高速回転するCu製ロールの外周面に
0.7mmの高さから溶湯を噴出させて、幅2〜3m
m、厚み30〜40μmの超急冷薄帯を作製した。得ら
れた超急冷薄帯をCuKαの特性X線によりアモルファ
スであることを確認した。
Example 1 No. 1 in Table 1 Purity 99.5 so that the composition is 1 to 5
% Or more of Fe, Co, B, Nd, Pr, Ag, Al, S
The metal i was weighed so that the total amount was 30 gr, put into a quartz crucible having an orifice with a diameter of 0.8 mm at the bottom, and melted by high-frequency heating in an Ar atmosphere with a pressure of 56 cmHg to set the melting temperature. After the temperature was set to 1400 ° C., the molten metal surface was pressurized with Ar gas, and the molten metal was ejected from a height of 0.7 mm onto the outer peripheral surface of a Cu roll which was rotated at a high speed at a roll peripheral speed of 20 m / sec at room temperature. 2-3m
An ultra-quenched ribbon having a thickness of m and a thickness of 30 to 40 μm was produced. The obtained ultra-quenched ribbon was confirmed to be amorphous by the characteristic X-ray of CuKα.

【0029】この超急冷薄帯をArガス中で500℃ま
で急速加熱した後、500℃以上を表1に示す昇温速度
で昇温し、表1に示す熱処理温度で10分間保持し、そ
の後室温まで冷却して薄帯を取り出し、幅2〜3mm、
厚み30〜40μm、長さ3〜5mmの試料を作製し、
VSHを用いて磁気特性を測定した。測定結果を表2に
示す。なお、試料の測定結果は、正方晶と斜方晶が混在
するFe3B相が主相で、Nd2Fe14B相とα−Fe相
が混在する多相組織であり、平均結晶粒径はいずれも
0.1μm以下であった。なお、Coはこれらの各相で
Feの一部を置換するが、Ag、Al、Siについては
添加量が少ない上、超微細結晶であるため分析不能であ
った。
After rapidly heating the ultra-quenched ribbon in Ar gas to 500 ° C., the temperature was raised to 500 ° C. or higher at the heating rate shown in Table 1 and kept at the heat treatment temperature shown in Table 1 for 10 minutes. Cool to room temperature, take out the ribbon, width 2-3 mm,
A sample having a thickness of 30 to 40 μm and a length of 3 to 5 mm is prepared,
The magnetic properties were measured using VSH. The measurement results are shown in Table 2. The measurement result of the sample is a multiphase structure in which the main phase is the Fe 3 B phase in which the tetragonal crystal and the orthorhombic crystal are mixed and the Nd 2 Fe 14 B phase and the α-Fe phase are mixed, and the average crystal grain size is Was 0.1 μm or less. Co replaces part of Fe in each of these phases, but Ag, Al, and Si could not be analyzed because the addition amount was small and the crystals were ultrafine.

【0030】比較例 実施例1と同条件で得られた実施例1の組成No.2の
超急冷薄帯をArガス中で500℃まで急速加熱した
後、500℃以上を11℃/分で昇温し、680℃で1
0分間保持する熱処理を施し、冷却後に実施例1と同条
件で試料化(比較例No.9)してVSMを用いて磁気
特性を測定した。測定結果を表2に示す。
Comparative Example Composition No. 1 of Example 1 obtained under the same conditions as in Example 1. After rapidly heating the ultra-quenched ribbon of No. 2 in Ar gas to 500 ° C., the temperature is raised to 500 ° C. or more at 11 ° C./min, and the temperature is increased to 1 at 680 ° C.
A heat treatment of holding for 0 minutes was performed, and after cooling, a sample was made under the same conditions as in Example 1 (Comparative Example No. 9) and the magnetic characteristics were measured using VSM. The measurement results are shown in Table 2.

【0031】実施例1と同条件で得られた実施例1の組
成No.2の超急冷薄帯をArガス中で500℃まで急
速加熱した後、比較例No.10は500℃で10分間
保持する熱処理を施し、比較例No.11は500℃以
上を4℃/分で昇温し、750℃で10分間保持する熱
処理を施し、冷却後に実施例1と同条件で試料化してV
SMを用いて磁気特性を測定した。測定結果を表2に示
す。比較例No.10はアモルファス組織、同No.1
1はFe2B相とα−Fe相が混在する多相組織であっ
た。
Composition No. 1 of Example 1 obtained under the same conditions as in Example 1 After rapidly heating the ultra-quenched ribbon of No. 2 to 500 ° C. in Ar gas, Comparative Example No. No. 10 was subjected to heat treatment of holding at 500 ° C. for 10 minutes, and Comparative Example No. No. 11 was heated to 500 ° C. or higher at 4 ° C./min, heat-treated at 750 ° C. for 10 minutes, cooled, sampled under the same conditions as in Example 1, and V
The magnetic characteristics were measured using SM. The measurement results are shown in Table 2. Comparative Example No. No. 10 is an amorphous structure, and No. 10 is the same. 1
No. 1 had a multi-phase structure in which Fe 2 B phase and α-Fe phase were mixed.

【0032】実施例1の組成No.2と同様組成で、S
iを含有しない比較例No.9を、組成No.2と同条
件で製造しかつ試料化してVSHを用いて磁気特性を測
定した。測定結果を表2に示す。
Composition No. of Example 1 Same composition as 2
Comparative Example No. containing no i. 9 is the composition No. The magnetic properties were measured by using VSH after manufacturing under the same conditions as in Example 2 and sampling. The measurement results are shown in Table 2.

【0033】実施例2 実施例1で得られた表1の組成No.4の超急冷薄帯
を、表1の熱処理後に平均粒径150μm以下に粉砕
し、エポキシ樹脂なるバインダーを2wt%の割合で混
合したのち、15mm×15mm×7mm寸法のボンド
磁石を作成した。得られたボンド磁石の磁気特性は、i
Hc=3.5kOe、Br=7.0kG、(BH)ma
x=5.5MGOeであった。
Example 2 Composition No. of Table 1 obtained in Example 1 The ultra-quenched ribbon of No. 4 was crushed to have an average particle size of 150 μm or less after the heat treatment shown in Table 1 and mixed with a binder of epoxy resin at a ratio of 2 wt%, and then a bonded magnet having a size of 15 mm × 15 mm × 7 mm was prepared. The magnetic properties of the obtained bonded magnet are i
Hc = 3.5 kOe, Br = 7.0 kG, (BH) ma
x was 5.5 MGOe.

【0034】[0034]

【表1】 [Table 1]

【0035】[0035]

【表2】 [Table 2]

【0036】[0036]

【発明の効果】この発明は、特定組成のFe−Co−B
−R−M系合金溶湯を超急冷法にてアモルファス組織と
なし、これに特定条件の熱処理を施すことにより、平均
結晶粒径が0.01〜0.1μmの微細結晶集合体とな
り、主相のFe3B型化合物相のほか、Nd2Fe14B型
結晶構造相の量比が増大し、α−Fe相が減少すること
により、永久磁石薄帯となり、さらにこれを粉砕して磁
石合金粉末化することによって、iHc≧3kOe、B
r≧8kG、(BH)max≧8MGOeの磁気特性が
得られ、8kG以上の残留磁束密度Brを有するボンド
磁石に最適のFe−Co−B−R−M系磁石合金粉末を
得ることができ、また焼結磁石化することにより従来の
アルニコ系磁石と同等以上の磁気特性を得ることができ
る。また、この発明は、希土類元素の含有量が少なく、
製造方法が簡単で大量生産に適しているため、8kG以
上の残留磁束密度Brを有し、ハードフェライト磁石を
超える磁気的性能を有し、磁気部品と磁石体との一体成
型を採用することによって工程を短縮することができ、
焼結ハードフェライトを凌ぐ性能対コスト比を実現し得
るボンド磁石を提供することができる。
INDUSTRIAL APPLICABILITY The present invention has a specific composition of Fe-Co-B.
-The RM alloy melt is formed into an amorphous structure by the ultra-quenching method, and by subjecting this to a heat treatment under specific conditions, a fine crystal aggregate having an average crystal grain size of 0.01 to 0.1 μm is formed, and the main phase is formed. Fe 3 other B compound phase, the amount ratio of Nd 2 Fe 14 B crystal structure phase is increased by alpha-Fe phase decreases, becomes permanent magnet ribbon, magnet alloy was further pulverized into a By powdering, iHc ≧ 3 kOe, B
Magnetic properties of r ≧ 8 kG and (BH) max ≧ 8 MGOe are obtained, and an optimal Fe—Co—B—R—M magnet alloy powder for a bond magnet having a residual magnetic flux density Br of 8 kG or more can be obtained, Further, by using a sintered magnet, it is possible to obtain magnetic characteristics equal to or higher than those of conventional alnico magnets. Further, the present invention has a low content of rare earth elements,
Since the manufacturing method is simple and suitable for mass production, it has a residual magnetic flux density Br of 8 kG or more, has magnetic performance exceeding that of a hard ferrite magnet, and adopts integral molding of a magnetic component and a magnet body. The process can be shortened,
It is possible to provide a bonded magnet that can achieve a performance-to-cost ratio that exceeds that of sintered hard ferrite.

───────────────────────────────────────────────────── フロントページの続き (51)Int.Cl.5 識別記号 庁内整理番号 FI 技術表示箇所 H01F 1/08 B ─────────────────────────────────────────────────── ─── Continuation of the front page (51) Int.Cl. 5 Identification code Office reference number FI technical display location H01F 1/08 B

Claims (3)

【特許請求の範囲】[Claims] 【請求項1】 組成式をFe100-x-y-zCoxyzw
(但しRはPrまたはNdの1種または2種、MはA
g、AlまたはSiの1種または2種以上)と表し、組
成範囲を限定する記号x、y、z、wが下記値を満足
し、Fe3B型化合物を主相とし、Nd2Fe14B型結晶
構造を有する強磁性相を有し、平均結晶粒径が0.01
〜0.1μmの微細結晶集合体からなることを特徴とす
る希土類磁石。 0.05≦x≦15at% 16≦y≦22at% 3≦z≦5.5at% 0.1≦w≦3at%
The method according to claim 1] composition formula Fe 100-xyz Co x B y R z M w
(However, R is one or two of Pr or Nd, M is A
g, Al or Si), and symbols x, y, z and w that limit the composition range satisfy the following values, Fe 3 B type compound as the main phase, and Nd 2 Fe 14 It has a ferromagnetic phase with a B-type crystal structure and an average crystal grain size of 0.01
A rare earth magnet comprising a fine crystal aggregate of 0.1 μm. 0.05 ≦ x ≦ 15 at% 16 ≦ y ≦ 22 at% 3 ≦ z ≦ 5.5 at% 0.1 ≦ w ≦ 3 at%
【請求項2】 組成式をFe100-x-y-zCoxyzw
(但しRはPrまたはNdの1種または2種、MはA
g、AlまたはSiの1種または2種以上)と表し、組
成範囲を限定する記号x、y、z、wが下記値を満足
し、Fe3B型化合物を主相とし、Nd2Fe14B型結晶
構造を有する強磁性相を有し、平均結晶粒径が0.01
〜0.1μmの微細結晶集合体からなり、平均粒径が3
〜500μm、磁気特性がiHc≧3kOe、Br≧8
kG、(BH)max≧8MGOeであることを特徴と
する希土類磁石合金粉末。 0.05≦x≦15at% 16≦y≦22at% 3≦z≦5.5at% 0.1≦w≦3at%
2. A method composition formula Fe 100-xyz Co x B y R z M w
(However, R is one or two of Pr or Nd, M is A
g, Al or Si), and symbols x, y, z and w that limit the composition range satisfy the following values, Fe 3 B type compound as the main phase, and Nd 2 Fe 14 It has a ferromagnetic phase with a B-type crystal structure and an average crystal grain size of 0.01
Consisting of fine crystal aggregates of ~ 0.1 μm and having an average particle size of 3
~ 500 μm, magnetic characteristics iHc ≧ 3 kOe, Br ≧ 8
A rare earth magnet alloy powder characterized in that kG and (BH) max ≧ 8 MGOe. 0.05 ≦ x ≦ 15 at% 16 ≦ y ≦ 22 at% 3 ≦ z ≦ 5.5 at% 0.1 ≦ w ≦ 3 at%
【請求項3】 組成式をFe100-x-y-zCoxyzw
(但しRはPrまたはNdの1種または2種、MはA
g、AlまたはSiの1種または2種以上)と表し、組
成範囲を限定する記号x、y、z、wが下記値を満足す
る合金溶湯を超急冷法にて実質的に90%以上をアモル
ファス組織となし、さらに熱処理に際し500℃からの
昇温速度を1〜15℃/分で昇温して550〜700℃
で30秒〜6時間保持する熱処理を施し、Fe3B型化
合物を主相とし、Nd2Fe14B型結晶構造を有する強
磁性相を有し、平均結晶粒径が0.01〜0.1μmの
微細結晶集合体を得たのち、これを粉砕して磁石合金粉
末を得ることを特徴とする希土類磁石合金粉末の製造方
法。 0.05≦x≦15at% 16≦y≦22at% 3≦z≦5.5at% 0.1≦w≦3at%
The 3. A composition formula Fe 100-xyz Co x B y R z M w
(However, R is one or two of Pr or Nd, M is A
g, Al or Si, or two or more of them), and the alloy melts in which the symbols x, y, z, and w which limit the composition range satisfy the following values, are substantially 90% or more by the superquenching method. Amorphous structure, further heat treatment at a heating rate from 500 ℃ at 1 to 15 ℃ / min to 550 ~ 700 ℃
At a temperature of 30 seconds to 6 hours, a Fe 3 B type compound as a main phase, a ferromagnetic phase having an Nd 2 Fe 14 B type crystal structure, and an average crystal grain size of 0.01 to 0. A method for producing a rare earth magnet alloy powder, which comprises obtaining a 1 μm fine crystal aggregate and then pulverizing this to obtain a magnet alloy powder. 0.05 ≦ x ≦ 15 at% 16 ≦ y ≦ 22 at% 3 ≦ z ≦ 5.5 at% 0.1 ≦ w ≦ 3 at%
JP5085290A 1992-03-19 1993-03-19 Rare earth magnet, rare earth magnet alloy powder and method for producing the same Expired - Lifetime JP2999648B2 (en)

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Cited By (3)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
EP0652572A1 (en) * 1993-11-05 1995-05-10 General Motors Corporation Hot-pressed magnets
JP2007027428A (en) * 2005-07-15 2007-02-01 Neomax Co Ltd Rare earth sintered magnet and its manufacturing method
DE10045704B4 (en) * 1999-09-16 2015-11-05 Hitachi Metals, Ltd. Process for producing a nanocomposite magnetic powder and process for producing a nanocomposite magnet

Cited By (4)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
EP0652572A1 (en) * 1993-11-05 1995-05-10 General Motors Corporation Hot-pressed magnets
DE10045704B4 (en) * 1999-09-16 2015-11-05 Hitachi Metals, Ltd. Process for producing a nanocomposite magnetic powder and process for producing a nanocomposite magnet
JP2007027428A (en) * 2005-07-15 2007-02-01 Neomax Co Ltd Rare earth sintered magnet and its manufacturing method
JP4645336B2 (en) * 2005-07-15 2011-03-09 日立金属株式会社 Rare earth sintered magnet and manufacturing method thereof

Also Published As

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