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JP2980254B2 - Anisotropic permanent magnet and manufacturing method thereof - Google Patents
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JP2980254B2 - Anisotropic permanent magnet and manufacturing method thereof - Google Patents

Anisotropic permanent magnet and manufacturing method thereof

Info

Publication number
JP2980254B2
JP2980254B2 JP3046135A JP4613591A JP2980254B2 JP 2980254 B2 JP2980254 B2 JP 2980254B2 JP 3046135 A JP3046135 A JP 3046135A JP 4613591 A JP4613591 A JP 4613591A JP 2980254 B2 JP2980254 B2 JP 2980254B2
Authority
JP
Japan
Prior art keywords
atomic
iron
balance
permanent magnet
magnetic properties
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.)
Expired - Fee Related
Application number
JP3046135A
Other languages
Japanese (ja)
Other versions
JPH04263403A (en
Inventor
一郎 高須
昇 原田
智宏 西山
義和 田中
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.)
Sanyo Tokushu Seiko KK
Original Assignee
Sanyo Tokushu Seiko KK
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 Sanyo Tokushu Seiko KK filed Critical Sanyo Tokushu Seiko KK
Priority to JP3046135A priority Critical patent/JP2980254B2/en
Publication of JPH04263403A publication Critical patent/JPH04263403A/en
Application granted granted Critical
Publication of JP2980254B2 publication Critical patent/JP2980254B2/en
Anticipated expiration legal-status Critical
Expired - Fee Related legal-status Critical Current

Links

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
    • H01F1/0574Alloys 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 obtained by liquid dynamic compaction

Landscapes

  • Chemical & Material Sciences (AREA)
  • Crystallography & Structural Chemistry (AREA)
  • Inorganic Chemistry (AREA)
  • Engineering & Computer Science (AREA)
  • Power Engineering (AREA)
  • Powder Metallurgy (AREA)
  • Hard Magnetic Materials (AREA)

Description

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

【0001】[0001]

【産業上の利用分野】本発明は、磁気特性の異方性を与
えた希土類−鉄−ほう素系(R−Fe−B系)永久磁石
及びその製造方法に関する。
BACKGROUND OF THE INVENTION 1. Field of the Invention The present invention relates to a rare earth-iron-boron (R-Fe-B) permanent magnet having anisotropy of magnetic properties and a method for producing the same.

【0002】[0002]

【従来の技術】希土類元素が10〜21原子%、ほう素
が3〜15原子%、残部が鉄及び不可避不純物である合
金を用いた異方性永久磁石が知られている。ここで、希
土類元素としては一般にNd、Prの一方または双方が
用いられ、両元素が製品の磁気特性に与える効果は殆ど
同一である。この合金に異方性を付与する方法には、次
の2種類がある。
2. Description of the Related Art Anisotropic permanent magnets using an alloy in which a rare earth element is 10 to 21 atomic%, boron is 3 to 15 atomic%, and the balance is iron and inevitable impurities are known. Here, one or both of Nd and Pr are generally used as the rare earth element, and both elements have almost the same effect on the magnetic properties of the product. There are the following two methods for imparting anisotropy to this alloy.

【0003】第1の製法は、所定の組成の合金塊を鋳造
し、これを3〜10μmの微粉末に粉砕し、個々の粉末
を磁場中で配向させて成形し、不活性ガス雰囲気中で焼
結処理する。
[0003] In the first production method, an alloy lump having a predetermined composition is cast, crushed into fine powder of 3 to 10 µm, and the individual powders are oriented in a magnetic field and formed, and then formed in an inert gas atmosphere. Sintering is performed.

【0004】第2の製法は、所定の組成の合金を溶融
し、メルトスピニング法により急冷凝固させてフレーク
状の薄片を得、この薄片をホットプレスにより成形し、
更に熱間据込み加工によって加圧して加圧方向に易磁化
軸を配向させる。
[0004] In a second production method, an alloy having a predetermined composition is melted and rapidly solidified by a melt spinning method to obtain a flake-like flake, and this flake is formed by hot pressing.
Further, pressure is applied by hot upsetting to orient the easy magnetization axis in the pressing direction.

【0005】これらの方法で製造させる磁石において、
その磁気性能を向上させる目的で、Rの一部をDyで置
換したり、Feの一部をCoで置換したりすることが試
みられていた。
[0005] In the magnet manufactured by these methods,
For the purpose of improving the magnetic performance, it has been attempted to substitute a part of R with Dy or a part of Fe with Co.

【0006】[0006]

【発明が解決しようとする課題】Coの添加は、磁石の
キューリー点を高めて高温での減磁率を小さくする効果
が認められたが、磁気特性、特に最大磁気エネルギー積
は殆ど改善されなかった。Dyを添加すると磁気特性を
させることができるが、Dyは、極めて高価なために実
用上の問題があった。従ってこの発明は、R−Fe−B
系の異法性永久磁石の磁気特性、特にr及びθの両方向
について最大磁気エネルギー積を向上させようとするも
のである。
The addition of Co has the effect of increasing the Curie point of the magnet and reducing the demagnetization rate at high temperatures, but the magnetic properties, especially the maximum magnetic energy product, have hardly been improved. . The magnetic properties can be improved by adding Dy, but Dy has a practical problem because it is extremely expensive. Therefore, the present invention relates to R-Fe-B
Magnetic properties of the different laws of the permanent magnet system, both of Japanese to r and θ
For it is intended to improve the maximum magnetic energy product.

【0007】[0007]

【課題を解決するための手段】この発明に用いる原料合
金の基本的な組成は、周知の希土類元素が10〜21原
子%、ほう素が3〜15原子%、残部が鉄族元素及び不
可避不純物よりなるものであり、希土類元素としてはN
d及びPrの一方または双方を使用する。この発明の特
徴として、上記合金中の鉄元素は、そのX原子%のコバ
ルトとY原子%のニッケルと残部の鉄とよりなり、これ
らX及びYは、 0≦X≦30 0≦Y≦1.5 X+10Y≧15 を満足する値である。
The basic composition of the raw material alloy used in the present invention is as follows: a well-known rare earth element is 10 to 21 atomic%, boron is 3 to 15 atomic%, and the balance is an iron group element and unavoidable impurities. And the rare earth element is N
One or both of d and Pr are used. As a feature of the present invention, the iron element in the alloy is composed of X atomic% of cobalt, Y atomic% of nickel and the balance of iron, and X and Y are 0 ≦ X ≦ 300 0 ≦ Y ≦ 1 0.5 X + 10Y ≧ 15.

【0008】この発明においては、製品にr及びθ方向
の異法性を与えるために、上記原料合金を溶融し、不活
性ガスを用いたガスアトマイズ法によってこれを球状粉
末化し、この粉末を550℃〜800℃の温度で前方押
出加工することによって、所定の形状に成形すると同時
に、異法性を与える。
[0008] In the present invention, the product in the r and θ directions
To provide a different law of, by melting the material alloy, which was spherical powder by gas atomization using an inert gas, the front pressing the powder at a temperature of 550 ° C. to 800 ° C.
By deca Engineering, when formed into a predetermined shape at the same time, it gives a different law properties.

【0009】上記の不活性ガスとしては、アルゴン、ネ
オン、ヘリウムの何れか、またはこれらの混合ガスを用
いる。塑性加工に用いる球状粉末の寸法は、極端に小さ
いと取扱中に酸化し、大きすぎると塑性加工に支障を来
すので、平均粒径が20〜100μm、最大粒径が30
0μm以下であることが望ましい。また、前方押出加
に際しては、加熱及び加工時の酸化を防ぐために、粉末
を塑性加工が可能な金属容器中に真空封入し、容器ごと
加熱及び加工を行うことが望ましい。
As the inert gas, any of argon, neon, helium, or a mixed gas thereof is used. If the size of the spherical powder used for the plastic working is extremely small, it will be oxidized during handling, and if it is too large, it will hinder the plastic working. Therefore, the average particle size is 20 to 100 μm, and the maximum particle size is 30.
It is desirable that the thickness be 0 μm or less. Further, when the forward extrusion pressure engineering, in order to prevent oxidation during heating and processing, the powder was vacuum-sealed into a metal container capable of plastic working, it is desirable to carry out together with the vessel heating and processing.

【0010】一般に、異方性を与えるためには、前方押
出加工、後方押出加工、リング状押出加工、圧延、温間
据込み加工など適宜の方法を採用することができ、その
際に生ずる歪の方向によって異方性を生ずる方向が決ま
る。r及びθ方向について顕著な異方性を得るために
、前方押出加工が適し、加工比(加工前の断面積/加
工後の断面積)が4.6以上であることが望ましい。
Generally, in order to impart anisotropy, an appropriate method such as forward extrusion, backward extrusion, ring extrusion, rolling, warm upsetting, etc. can be adopted. Determines the direction in which anisotropy occurs. In order to obtain a remarkable anisotropy for r and θ directions, suitable forward extrusion, pressurization Engineering ratio (sectional area after the cross-sectional area / processing before processing) it is desirable that 4.6 or more.

【0011】前方押出加工に際しては、加工速度が速す
ぎると、材料の歪速度が大きくなって破損するから、歪
速度を0.3以下に抑えることが必要である。歪速度V
eは、加工の態様によらず、次のようにして算出され
る。 歪E=lnK 歪速度Ve=E/T(sec -1) ここで、kは加工比であり、Tは材料中の或る部位が加
工領域に入ってからこれを出るまでの滞留時間である。
[0011] In the forward extrusion pressure engineering, the processing speed is too fast, because the strain rate of the material is damaged increases, it is necessary to suppress the strain rate below 0.3. Strain speed V
e is calculated as follows regardless of the mode of processing. Strain E = lnK Strain speed Ve = E / T (sec −1 ) where k is a working ratio, and T is a residence time from when a certain part in the material enters the working area to when it exits the working area. .

【0012】[0012]

【作用】前記した2種類の従来の製法では、原料合金中
の鉄の一部をコバルト及びニッケルの一方または双方で
置換しても、目立った磁気特性の改善が得られなかっ
た。しかし、本発明においては、原料合金の粉末化に不
活性ガスを用いたガスアトマイズ法を採用し、更にその
粉末を容器に真空封入して加熱及び前方押出加工を行う
ようにしたことにより、コバルト及び/またはニッケル
による鉄の一部置換の効果が顕著に現れて、磁気特性、
にr方向及びθ方向の最大磁気エネルギー積を大きく
改善することができた。その最大の原因は、原料合金の
粉末化から前方押出加工が完了するまでの間、原料粉末
の酸化を抑制し得たことにあると考えられる。
In the above two conventional manufacturing methods, no remarkable improvement in magnetic properties was not obtained even if a part of iron in the raw material alloy was replaced with one or both of cobalt and nickel. However, in the present invention, by a gas atomizing method using an inert gas to the powder of the material alloy is adopted, and to further perform heat及beauty forward extrusion pressure Engineering and vacuum sealed the powder into a container, The effect of partial replacement of iron by cobalt and / or nickel is remarkable, and the magnetic properties,
It was possible to greatly improve the maximum magnetic energy product of the r direction and the θ direction especially. Cause of the maximum is considered to be in the powdered material alloy or al forward extrusion machining is until the completion, it was able to suppress oxidation of the raw material powder.

【0013】Nd及びPrが製品の磁気特性に与える効
果は殆ど同じであることが知られている。換言すれば、
Ndの一部または全部をPrで置換しても、合金中で占
めるNdとPrの合計量の割合が一定である限り、製品
の磁気特性は殆ど変わらない。原料合金中の鉄をコバル
ト及びニッケルで置換する量の範囲を図1に示す。即
ち、鉄、コバルト、ニッケルの総量(100原子%)中
で、コバルト量X(原子%)とニッケル量Y(原子%)
の関係がX+10Y<15のとき、及びコバルト量Xが
30原子%を越え、或いはニッケル量Yが1.5原子%
を越えるときは、製品の磁気特性は十分改善されない。
It is known that the effects of Nd and Pr on the magnetic properties of products are almost the same. In other words,
Even if some or all of Nd is replaced with Pr, the magnetic properties of the product hardly change as long as the ratio of the total amount of Nd and Pr in the alloy is constant. FIG. 1 shows the range of the amount of iron to be replaced with cobalt and nickel in the raw material alloy. That is, in the total amount of iron, cobalt and nickel (100 atomic%), the amount of cobalt X (atomic%) and the amount of nickel Y (atomic%)
Is X + 10Y <15, and the cobalt amount X exceeds 30 at%, or the nickel amount Y is 1.5 at%.
When the value exceeds, the magnetic properties of the product are not sufficiently improved.

【0014】更に、この発明においては、極めて生産性
が良好な前方押出加工方法を採用し ているので、優れた
性能の異方性磁石を工業的に有利に生産できるようにな
った。
Furthermore, in the present invention, pole since Umate productivity is adopted good forward extrusion machining method, to be able to industrially advantageously produce an anisotropic magnet of superior performance Was.

【0015】[0015]

【実施例】実施例1 表1に試料1乃至6として示すR−Fe−B系の各種の
合金を溶製し、それぞれアルゴンガスアトマイズ法によ
り粒径298μm以下に粉末化する。これらをそれぞれ
外径28mm、長さ35mm、肉厚1mmの軟鋼製カプ
セルに充填し、内部を真空排気して電子ビーム溶接によ
り封止する。これをビレットとして下記条件で前方押出
加工した。 予熱 600℃×5分間 押出温度 650±5℃ 押出比 4.0(径28mm→径14mm) 歪速度 毎秒0.05
EXAMPLES Example 1 Various R-Fe-B-based alloys shown as samples 1 to 6 in Table 1 are melted, and each is pulverized to a particle size of 298 μm or less by an argon gas atomizing method. These are each filled in a mild steel capsule having an outer diameter of 28 mm, a length of 35 mm and a wall thickness of 1 mm, and the inside is evacuated and sealed by electron beam welding. This was extruded forward as a billet under the following conditions. Preheating 600 ° C × 5 minutes Extrusion temperature 650 ± 5 ° C Extrusion ratio 4.0 (diameter 28 mm → diameter 14 mm) Strain rate 0.05 per second

【0016】得られた磁石材の磁気特性を表1に示す。
なお、Zは押出加工方向、rは半径方向、θはrに直交
する方向である。
Table 1 shows the magnetic properties of the obtained magnet material.
Note that Z is the extrusion direction, r is the radial direction, and θ is the direction orthogonal to r.

【表1】 表1を検討すると、試料3、4、5ではCoの添加によ
って磁気特性が顕著に改善されているが、試料2及び6
ではCoの添加による磁気特性の改善が殆ど認められな
い。
[Table 1] Examination of Table 1 reveals that the magnetic properties of Samples 3, 4 and 5 were significantly improved by the addition of Co, whereas Samples 2 and 6
, There is almost no improvement in magnetic properties due to the addition of Co.

【0017】実施例2 表2に試料7乃至9として示すR−Fe−B系の各種の
合金を、それぞれ実施例1と同条件で粉末化し、かつ同
条件で磁石材に加工した。得られた磁石材の磁気特性を
表2に示す。
Example 2 Various R-Fe-B alloys shown as samples 7 to 9 in Table 2 were powdered under the same conditions as in Example 1, and processed into magnet materials under the same conditions. Table 2 shows the magnetic properties of the obtained magnet material.

【表2】 表2を検討すると、試料8はNiの添加によって磁気特
性が顕著に改善されているが、試料7及び9ではNi添
加による磁気特性の改善が殆ど認められない。
[Table 2] Examination of Table 2 reveals that the magnetic properties of Sample 8 are remarkably improved by the addition of Ni, but the magnetic properties of Samples 7 and 9 are hardly improved by the addition of Ni.

【0018】実施例3 表3に試料10乃至12として示すR−Fe−B系の各
種の合金を、それぞれ実施例1と同条件で粉末化し、か
つ同条件で磁石材に加工した。得られた磁石材の磁気特
性を表3に示す。
Example 3 Various R—Fe—B alloys shown as samples 10 to 12 in Table 3 were powdered under the same conditions as in Example 1 and processed into magnet materials under the same conditions. Table 3 shows the magnetic properties of the obtained magnet material.

【表3】 表3を検討すると、試料10及び11ではNi及びCo
の同時添加による磁気特性の改善効果が認められるが、
試料12では磁気特性が却って減退している。
[Table 3] Examination of Table 3 shows that Samples 10 and 11 have Ni and Co
The effect of improving the magnetic properties by the simultaneous addition of
In Sample 12, the magnetic properties are rather reduced.

【0019】図1は、横軸にCo量X(原子%)を、縦
軸にNi量Y(原子%)をとり、上記試料1乃至12の
分布状況を示すものである。図中の符号1乃至12は上
記試料番号を示し、括弧内の数字はr方向の最大磁気エ
ネルギー積(BH)max(MGOe)を示す。図1に
よって明らかなように、r方向の最大磁気エネルギー積
がおよそ14MGOe以上である範囲は、 X=30 Y=1.5 X+10Y=15 である3本の直線で囲まれた部分である。図2は、横軸
にCo量X(原子%)を、縦軸にr方向の最大磁気エネ
ルギー積(MGOe)をとった図であり、Ni量Yが
である試料1、2、3、4、5及び6の場合はCo量X
15〜30原子%のときにr方向の最大磁気エネルギ
ー積が最高値を示している。また、このことから、試料
7及び10のようにNi量Yが0.62原子%である場
合、試料8及び11のようにNi量Yが1.24原子%
である場合、及び試料9及び12のようにNi量Yが約
1.7原子%である場合にも、図示のようにCo量Xが
15〜30原子%のときにr方向の最大磁気エネルギー
積がピークを示すことを予想できる。
FIG. 1 shows the distribution of the above samples 1 to 12, with the horizontal axis representing the amount of Co X (atomic%) and the vertical axis representing the amount of Ni Y ( atomic%). Reference numerals 1 to 12 in the drawing indicate the sample numbers, and the numbers in parentheses indicate the maximum magnetic energy product (BH) max (MGOe) in the r direction. As is clear from FIG. 1, the range where the maximum magnetic energy product in the r direction is about 14 MGOe or more is a portion surrounded by three straight lines where X = 30 Y = 1.5 X + 10Y = 15. 2, the Co content on the horizontal axis X (atomic%), the vertical axis is a diagram taken r direction of maximum magnetic energy product (MGOe), Ni amount Y is 0
Co amount X in the case of samples 2, 3, 4, 5 and 6 is
Is 15 to 30 atomic%, the maximum magnetic energy product in the r direction shows the highest value. Also, from this , the sample
In the case where the amount of Ni Y is 0.62 atomic% as in 7 and 10,
In this case, as in Samples 8 and 11, the Ni amount Y is 1.24 atomic%.
And the amount of Ni Y is about
Even in the case of 1.7 atomic%, the Co amount X is
Maximum magnetic energy in r direction at 15-30 atomic%
The product can be expected to show a peak.

【0020】[0020]

【発明の効果】以上の実施例によって明らかなように、
本発明によれば、R−Fe−B系磁石合金の磁気特性を
Co及びNiの一方または双方の添加によって向上する
ことができ、かつ生産性の良好なガスアトマイズ法及び
生産性が良好な前方押出加工方法の採用によって、所望
形状のr、θ両方向異法性磁石を安価に量産することが
できる。
As is clear from the above embodiments,
Advantageous Effects of Invention According to the present invention, the magnetic properties of an R-Fe-B-based magnet alloy can be improved by the addition of one or both of Co and Ni, and a gas atomizing method with good productivity and forward extrusion with good productivity. the adoption of machining methods, can be inexpensively mass-produced r a desired shape, a θ bidirectional different method of magnets.

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

【図1】本発明におけるCo量XとNi量Yの範囲を示
す分布図である。
FIG. 1 is a distribution diagram showing a range of a Co amount X and a Ni amount Y in the present invention.

【図2】本発明におけるCo量Xと最大磁気エネルギー
積との関係をNi量Yごとに分けて示した線図である。
FIG. 2 is a diagram showing a relationship between a Co amount X and a maximum magnetic energy product in the present invention for each Ni amount Y.

【符号の説明】[Explanation of symbols]

1〜12 試料番号 1-12 Sample number

───────────────────────────────────────────────────── フロントページの続き (72)発明者 西山 智宏 兵庫県姫路市飾磨区中島字一文字3007番 地 山陽特殊製鋼株式会社内 (72)発明者 田中 義和 兵庫県姫路市飾磨区中島字一文字3007番 地 山陽特殊製鋼株式会社内 (56)参考文献 特開 昭63−287007(JP,A) 特開 昭60−189901(JP,A) 特開 昭63−289905(JP,A) (58)調査した分野(Int.Cl.6,DB名) H01F 1/00 - 1/08 ──────────────────────────────────────────────────続 き Continuing from the front page (72) Inventor Tomohiro Nishiyama 3007 character, Nakajima character in Shima, Ward, Himeji City, Hyogo Prefecture Inside Sanyo Special Steel Co., Ltd. Chisan Sanyo Special Steel Co., Ltd. (56) References JP-A-63-287007 (JP, A) JP-A-60-189901 (JP, A) JP-A-63-289905 (JP, A) (58) Field (Int.Cl. 6 , DB name) H01F 1/00-1/08

Claims (2)

(57)【特許請求の範囲】(57) [Claims] 【請求項1】 希土類元素が10〜21原子%、ほう素
が3〜15原子%、残部が鉄族元素及び不可避不純物よ
りなり、かつ上記鉄族元素は、そのX原子%のコバルト
と、Y原子%のニッケルと、残部の鉄とよりなり、上記
X及びYは 0≦X≦30(原子%) 0≦Y≦1.5(原子%) X+10Y≧15(原子%) である合金の不活性ガスを用いたガスアトマイズ粉末の
成形品であり、r及びθの2方向の最大磁気エネルギー
積が改善されていることを特徴とする異方性永久磁石。
1. A rare earth element is composed of 10 to 21 atomic%, boron is composed of 3 to 15 atomic%, and the balance is composed of an iron group element and an unavoidable impurity. Atomic% nickel and the balance of iron, where X and Y are 0 ≦ X ≦ 30 (atomic%) 0 ≦ Y ≦ 1.5 (atomic%) X + 10Y ≧ 15 (atomic%) It is a molded product of gas atomized powder using active gas, and the maximum magnetic energy in two directions of r and θ
Anisotropic permanent magnet characterized in that the product is improved .
【請求項2】 希土類元素が10〜21原子%、ほう素
が3〜15原子%、残部が鉄族元素及び不可避不純物よ
りなり、かつ上記鉄族元素は、そのX原子%がコバルト
で、Y原子%がニッケルで、残部が鉄であって、上記X
及びYは 0≦X≦30(原子%) 0≦Y≦1.5(原子%) X+10Y≧15(原子%) である合金を溶融して、不活性ガスを用いたガスアトマ
イズ法により球状粉末化し、この粉末を550℃〜80
0℃の温度で前方押出加工を行うことにより所定の形状
の成形品を得ることを特徴とする異方性永久磁石の製造
方法。
2. A rare earth element comprises 10 to 21 atomic%, boron comprises 3 to 15 atomic%, and the balance comprises an iron group element and an unavoidable impurity. Atomic% is nickel and the balance is iron,
And Y are: 0 ≦ X ≦ 30 (atomic%) 0 ≦ Y ≦ 1.5 (atomic%) An alloy satisfying X + 10Y ≧ 15 (atomic%) is formed into a spherical powder by a gas atomizing method using an inert gas. 550-80 ° C.
Method for producing an anisotropic permanent magnet, characterized in that to obtain a predetermined shape of the molded article by a temperature of 0 ℃ performing forward extrusion pressure Engineering.
JP3046135A 1991-02-18 1991-02-18 Anisotropic permanent magnet and manufacturing method thereof Expired - Fee Related JP2980254B2 (en)

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JP3046135A JP2980254B2 (en) 1991-02-18 1991-02-18 Anisotropic permanent magnet and manufacturing method thereof

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP3046135A JP2980254B2 (en) 1991-02-18 1991-02-18 Anisotropic permanent magnet and manufacturing method thereof

Publications (2)

Publication Number Publication Date
JPH04263403A JPH04263403A (en) 1992-09-18
JP2980254B2 true JP2980254B2 (en) 1999-11-22

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Country Link
JP (1) JP2980254B2 (en)

Family Cites Families (3)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS60189901A (en) * 1984-03-09 1985-09-27 Sumitomo Special Metals Co Ltd Manufacture of alloy powder for rare earth-boron-iron group magnetic anisotropic permanent magnet
JPS63287007A (en) * 1987-05-19 1988-11-24 Seiko Epson Corp Permanent magnet manufacturing method
JPS63289905A (en) * 1987-05-22 1988-11-28 Kobe Steel Ltd Manufacture of rare earth-fe-b magnet

Also Published As

Publication number Publication date
JPH04263403A (en) 1992-09-18

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