JPS629658B2 - - Google Patents
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- JPS629658B2 JPS629658B2 JP57008035A JP803582A JPS629658B2 JP S629658 B2 JPS629658 B2 JP S629658B2 JP 57008035 A JP57008035 A JP 57008035A JP 803582 A JP803582 A JP 803582A JP S629658 B2 JPS629658 B2 JP S629658B2
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Description
利用産業分野
この発明は、R2M17系(Rは希土類元素、Mは
遷移金属元素)希土類コバルト永久磁石の製造方
法の改良に係り、製造工程における磁石合金溶
解、鋳造後に、新たに液体化処理工程を導入し、
その後粉砕、圧縮成型、焼結を行ない、さらに、
特定温度以下まで特定の冷却速度にて冷却するこ
とにより、磁石特性の向上、安定化をはかり、時
効処理工程の省略を計つた永久磁石の製造方法に
関する。
背景技術
希土類コバルト磁石は、今日多量に製造されて
いるアルニコ系磁石、フエライト磁石と比較し、
極めて高い保磁力と大きなエネルギー積を有する
永久磁石材料として、近年急速にその需要が高ま
り、その利用分野は電子工業界を中心に多岐にわ
たつている。
この希土類コバルト系磁石合金はいずれも十分
に高い飽和磁化の強さ(4ΠIs)と、結晶磁気異
方性(K)を兼ね備えているため、高い保持力と
エネルギー積を有するすぐれた永久磁石材料であ
ることが知られている。上記合金のなかで、特に
RM5系およびR2M17系合金が注目され、その工業
化が進められてきた。
このうち、RM5系合金組成を有する希土類コバ
ルト磁石については、現在すでにエネルギー積理
論値に近い20MGOeの最大エネルギー積を有する
磁石材料が得られている。
従つて、さらに高い磁石特性を得るためには、
飽和磁化の高い、すなわち、Mのモル比が高い
R2M17系希土類コバルト磁石が、注目されるよう
になつた。
しかし、単にMの量を増加させるのみでは、磁
石本基本特性のうち保磁力が著しく低下し、実用
的な永久磁石としての特性が十分に得られない。
そこで、従来はR成分とし主としてSmを用い、
Mの構成成分について、各成分の組合せおよびそ
の割合を種々変化させて高性能化を計る試みが、
数多くなされてきた。
ここで、従来のR2M17系希土類コバルト磁石合
金の製造方法を説明すると、この磁石合金は溶
解、粉砕、磁界中プレス成型、焼結および時効処
理の各製造工程を経て作製されている。
溶解は、アークボタン溶解炉や高周波溶解炉な
どを用いてアルゴンガスなどの不活性雰囲気中で
行なわれる。
粉砕は、粗粉砕と微粉砕工程からなり、ジヨー
クラツヤー鉄製乳鉢などによる粗粉砕後、ボー
ル・ミル、バイブレーシヨン・ミル、ジエツト・
ミルなどにより微粉砕を行なう。
磁界中プレス成型では、金型を用い8kOe〜
15kOeの磁界中に於て粉末を配向しながら圧縮成
型体を作る。
焼結は、アルゴン、水素等の非酸化性雰囲気中
あるいは真空中で、1100℃〜1250℃の温度範囲に
おいて行なう。続いて、300℃〜950℃の温度範囲
において時効処理を行ない、最終の永久磁石金を
得る。
ところが、上記の従来製法で得られた永久磁石
の磁石特性は低くかつばらつきも多く、また金属
組織的に種々の相が混在し、場合によつて減磁曲
線上にクニツクを生ずるため、有用な実用永久磁
石材料とならず、また多くの製造工程を必要とす
る問題があつた。
発明の目的
この発明は、上述の従来製法による問題を解消
し、さらに高い保持力、高エネルギー積を有する
R2M17系希土類コバルト永久磁石材料を提供する
と共に時効処理工程を省略することを目的として
いる。
発明の構成
この発明は、
希土類元素Rと遷移金属MからなるR2M17系磁
石合金(但し、RはY、La、Ce、Pr、Nb、Sm
及びミツシユメタルの1種または2種以上の組合
せ、MはCu、FeもしくはNiのうち1種または2
種以上の組合せ及び該Mの一部をMn、Ti、Nb、
Zr、Ta、Hfの各元素のうち1種以上の元素と置
換した組合わせ)を、
溶解して鋳造した後、1150℃〜1210℃、1時間
〜12時間の溶体化処理を施したのち、急速冷却を
行つて、金属相RM7相を90%以上生成させ、
さらに、該合金を粉砕、圧縮成型し、この圧縮
成型体を真空中または不活性雰囲気中で焼結し、
その後800℃以下まで20℃/min〜500℃/minの
冷却速度にて冷却することにより、従来の時効処
理工程を省略して金属相的にはR2M17相を55%〜
85%、残余RM5相を有する永久磁石を得ることを
特徴とするものである。
発明の効果
この発明の特徴である溶解、鋳造後の本系磁石
合金に、液体化処理および急速冷却処理し、かつ
焼結後、880℃以下まで特定の冷却速度にて冷却
することにより、以下のような永久磁石の磁気特
性向上に著しい効果がある。
R2M17系本磁石合金における高い磁石特性の出
現機構は、本磁石合金を構成する金属相が焼結時
に、一旦、TbCu7結晶構造(RM7相)の単相とな
り、焼結後特定温度以下まで最適な冷却速度で冷
却することにより、Th2Zn17結晶構造相(R2M17
相)ならびにCaCu5結晶構造相(RM5相)が微細
に分解・析出することにある。
このTbCu7結晶構造相は、本系合金に不可欠な
金属相であり、溶解後あるいは焼結後において、
TbCu7結晶構造相の少ない場合には、その後、い
かなる磁石化工程を採つても高い磁気特性は得ら
れない。
これは、TbCu7結晶構造相が高温で、しかもあ
る狭い組成域でのみ安定な金属相であり、溶解、
鋳造過程等における温度低下とともに、直ちに
Th2Zn17結晶構造相とCaCu5結晶構造相に分解・
析出するためであり、一旦、TbCu7結晶構造相が
分解・析出すれば、容易には元のTbCu7結晶構造
相に回復しないためである。
しかも、通常、用いられる溶解、鋳造の磁石化
工程においては、溶解インゴツトの急速冷却は工
業的に困難であり、冷却速度の違いによる凝固過
程が異なるため、鋳造後すでにTbCu7結晶構造相
の他に、磁気的に好ましくないTh2Zn17結晶構造
相、Fe−Corichな初晶、CaCu5結晶構造相をか
なり含有する。
また、希土類元素は蒸気圧が高く、化学的に活
性であるため、通常のプロセスで得られたインゴ
ツトでは組成変動が著しく、上記の好まざる金属
相を生成しやすい。
そのため、この発明の1の特徴である溶解・鋳
造したインゴツトの溶体化処理工程とは、溶解、
鋳造後のインゴツトを1150℃〜1210℃の温度域で
1時間〜12時間保持し、処理後、液体窒素、水等
を用いて急速冷却し、金属相的にはRM7相90%以
上となすことである。
限定理由
ここで溶体化処理温度を1150℃〜1210℃に限定
した理由は、1150℃未満では高温でのみ安定であ
るTbCu7結晶構造相が規則化を起こし、直ちに
Th2Zn17結晶構造相ならびにCaCu5結晶構造相を
析出するためであり、1210℃を超える温度では、
金属相で約10%以上の過剰の融液相を生じ、ミク
ロ的な組成変動が大きくなり、磁石特性は著しく
劣化するので、TbCu7結晶構造相の十分な形成と
過剰の融液相の発生を防ぐためには溶体化処理温
度を1150℃〜1210℃とする。
次に溶体化処理時間を1時間〜12時間としたの
は以下の理由による。
一般に大型のインゴツトの製作においては、鋳
造時に徐冷されるため、Th2Zn17結晶構造相やFe
−Corichな初晶の磁気的に有害な金属相を形成
しやすく、そのため溶体化処理時間は長くなる。
溶体化処理時間は1時間未満ではTbCu7結晶構造
相が十分得られない。12時間を超える時間では工
業的に長時間を要しすぎ、またRの蒸発ならびに
酸化による組成変動並びに磁気的に有害な金属相
の生成が著しい。そこで溶体化処理時間を1時間
〜12時間とする。
以上の1150℃〜1210℃、1時間〜12時間の最適
溶体化処理により金属相的にRM7相90%以上とな
し得る。RM7相90%未満の金属相を呈するインゴ
ツトは、以下いかなる磁石工程を取つてもすぐれ
た磁石特性は得られない。
次に、製造工程の焼結は、アルゴン、水素等の
非酸化性雰囲気中あるいは空気中で、1150℃〜
1210℃の温度範囲で行ない焼結密度、さらに磁石
特性を向上させる。ここで焼結後の金属相中の
RM7相の量は70%以上、好ましくは90%以上であ
ることが高い磁石特性を得るには不可欠である。
また、下記条件で焼結を行なうと更に磁石特性
の改善に有効である。
すなわち、その焼結方法とは、前述の得られた
圧縮成型体を1×10-2Torr以下の真空雰囲気中
で、室温から800℃まで4〜20℃/minの割合で
昇温する焼結方法である。
ここで昇温速度に関しては、4℃/min未満の
昇温速度では、800℃までに3時間以上を要し工
業的に不適であり、20℃/minを超える昇温速度
では、成型体中の吸着ガス、水分等を十分に除去
できない。
また、昇温中の真空度は圧縮成型体の昇温過程
中の酸化を防止するため、1×10-2Torr以下の
真空度が望ましい。
次に焼結雰囲気は、上記脱ガス昇温処理後の
800℃以上から焼結温度までの10分〜120分の昇温
時間ならびに0.5時間〜4時間の焼結温度保持時
間において、R、Mの各成分の相互拡散を促進さ
せ、TbCu7結晶構造相を安定化せしめ、なおかつ
焼結密度を高めて磁石特性を向上させるため、
50Torr〜350Torrに減圧したアルゴンガス雰囲気
とする。
アルゴンガス雰囲気圧力は、50Torr未満の場
合、Rの成分が優先的に蒸発し、最終磁石組成よ
りかなり異なる組成となり、磁石特性を著しく損
なうため好ましくなく、350Torrを超える圧力下
では、R、Mの各成分の相互拡散が不十分であ
り、焼結密度も低く磁石特性も低くなる。
続いてこの発明の1特徴である焼結後の冷却条
件であるが、20〜500℃/minの範囲の冷却速度
で800℃以下の温度まで冷却する場合は通常行な
われる焼結後の時効処理を行なう必要はない。
上記の冷却速度を限定した理由は、20℃/min
未満の冷却速度ではRM7相が規則化を急激に起こ
すため、得られる磁石特性は著しく低くなり、
500℃/minを超える冷却速度ではRM7相がR2M17
相・RM5相へ十分に分解しないため好ましくな
い。
この発明において、R2M17相とRM5相の微細な
分解・析出を起こさせるために、最適の冷却速度
としては50〜200℃/minが望ましい。
この発明において、前記最適冷却条件にて冷却
することは、金属相的にR2M17相55〜85%、残余
RM5相であつて、すぐれた磁石特性を得るために
不可欠であり、本金属相以外の金属相を有する磁
石の磁気特性は著しく低い。
実施例
以下に、この発明による実施例を示しその効果
を明らかにする。
実施例 1
純度99.9%以上のSm26.9wt%、
純度99.8%以上のCo47.6wt%、Fe12.1wt%、
Ni5.5wt%、Cu7.9wt%からなる合金を、アルゴ
ンガス雰囲気中で高周波溶解し、鋳造して得られ
たインゴツトに1180℃、6時間の溶体化処理を施
し、処理後、液体窒素中で急速冷却することによ
り金属相的にRM7相を94%となした。
得られた合金を鉄乳鉢中で粗粉砕し、さらに有
機溶剤中でボール・ミル微粉砕を行ない、2〜10
μmの粉末とした。この粉末を12kOeの磁界中で
プレス成型し、圧縮成型体を得た。
次に、圧縮成型体を水素雰囲気中1200℃、2時
間の焼結を行ない、焼結後、100℃/minの冷却
速度で800℃以下の温度まで冷却することによ
り、この発明による永久磁石を得た。
また、比較例として、上記と同じの鋳造後のイ
ンゴツトに溶体化処理を施さずに、上記と同じ条
件の粗粉砕、微粉砕、プレス成型、焼結した後、
焼結後の溶体化処理を1160℃、8時間で行い、比
較永久磁石を得た。
得られた2種の永久磁石の磁気特性を第1表に
示す。
Field of Application This invention relates to an improvement in the manufacturing method of rare earth cobalt permanent magnets of the R 2 M 17 series (R is a rare earth element, M is a transition metal element). Introducing a treatment process,
After that, pulverization, compression molding, sintering, and
The present invention relates to a method for manufacturing a permanent magnet, which improves and stabilizes magnetic properties by cooling to a specific temperature or lower at a specific cooling rate, and which eliminates an aging treatment step. Background technology Rare earth cobalt magnets have a higher
As a permanent magnet material with an extremely high coercive force and a large energy product, demand for it has increased rapidly in recent years, and its applications are wide-ranging, mainly in the electronics industry. These rare earth cobalt magnet alloys have both sufficiently high saturation magnetization strength (4ΠIs) and crystal magnetic anisotropy (K), making them excellent permanent magnet materials with high coercive force and energy product. It is known that there is. Among the above alloys, especially
RM 5 series and R 2 M 17 series alloys have attracted attention, and their industrialization has been progressing. Among these, for rare earth cobalt magnets having an RM 5 alloy composition, a magnet material with a maximum energy product of 20 MGOe, which is close to the theoretical energy product value, has already been obtained. Therefore, in order to obtain even higher magnetic properties,
High saturation magnetization, that is, high molar ratio of M
R 2 M 17 rare earth cobalt magnets have started to attract attention. However, if the amount of M is simply increased, the coercive force, which is one of the basic characteristics of the magnet, will be significantly reduced, and the characteristics of a practical permanent magnet will not be sufficiently obtained.
Therefore, conventionally, Sm was mainly used as the R component,
Regarding the constituent components of M, attempts were made to improve performance by varying the combinations and proportions of each component.
Many things have been done. Here, to explain the conventional manufacturing method of R 2 M 17- based rare earth cobalt magnet alloy, this magnet alloy is manufactured through the following manufacturing steps: melting, crushing, press molding in a magnetic field, sintering, and aging treatment. Melting is performed in an inert atmosphere such as argon gas using an arc button melting furnace, a high frequency melting furnace, or the like. Grinding consists of coarse grinding and fine grinding processes, and after coarse grinding in a Jyokratuar iron mortar, etc., it is processed using a ball mill, vibration mill, jet mill,
Finely pulverize using a mill or the like. Press molding in a magnetic field uses a mold to produce 8kOe~
A compression molded body is made by orienting the powder in a 15kOe magnetic field. Sintering is performed in a non-oxidizing atmosphere such as argon, hydrogen, etc. or in vacuum at a temperature range of 1100°C to 1250°C. Subsequently, aging treatment is performed in a temperature range of 300°C to 950°C to obtain the final permanent magnet gold. However, the magnetic properties of the permanent magnets obtained by the above-mentioned conventional manufacturing method are low and highly variable, and various phases coexist in the metallographic structure, sometimes causing a knick on the demagnetization curve. There was a problem that it could not be used as a practical permanent magnet material and required many manufacturing steps. Purpose of the Invention The present invention solves the problems caused by the conventional manufacturing method described above, and has even higher holding power and higher energy product.
The purpose is to provide an R 2 M 17 -based rare earth cobalt permanent magnet material and to omit the aging treatment process. Composition of the Invention This invention consists of an R 2 M 17- based magnetic alloy consisting of a rare earth element R and a transition metal M (where R is Y, La, Ce, Pr, Nb, Sm
and a combination of two or more of Mitsushi metals, M is one or two of Cu, Fe, or Ni.
Combinations of more than one species and a part of the M include Mn, Ti, Nb,
After melting and casting a combination of Zr, Ta, and Hf (substituted with one or more of the elements), solution treatment is performed at 1150°C to 1210°C for 1 to 12 hours, and then Rapid cooling is performed to generate 90% or more of the metallic phase RM 7 phase, and the alloy is further crushed and compression molded, and this compression molded body is sintered in a vacuum or in an inert atmosphere,
After that, by cooling to below 800°C at a cooling rate of 20°C/min to 500°C/min, the conventional aging treatment process is omitted and the R 2 M 17 phase is reduced by 55% to 55% in terms of metal phase.
It is characterized by obtaining a permanent magnet with a residual RM of 85% and 5 phases. Effects of the Invention By subjecting the present magnet alloy after melting and casting, which is a feature of this invention, to liquefaction treatment and rapid cooling treatment, and cooling it at a specific cooling rate to 880°C or less after sintering, the following can be achieved. It has a remarkable effect on improving the magnetic properties of permanent magnets such as. The mechanism by which the high magnetic properties of this R 2 M 17 -based magnet alloy appear is that the metal phase that makes up this magnet alloy becomes a single phase with a TbCu 7 crystal structure (RM 7 phase) during sintering. The Th 2 Zn 17 crystal structure phase (R 2 M 17
phase) and the CaCu 5 crystal structure phase (RM 5 phase) are finely decomposed and precipitated. This TbCu 7 crystal structure phase is an essential metal phase for this alloy, and after melting or sintering,
If there is a small amount of TbCu 7 crystal structure phase, high magnetic properties cannot be obtained no matter what magnetization process is performed afterwards. This is because the TbCu 7 crystal structure phase is a metallic phase that is stable only at high temperatures and within a certain narrow composition range, and it cannot be dissolved or
As the temperature drops during the casting process, etc., the
Decomposed into Th 2 Zn 17 crystal structure phase and CaCu 5 crystal structure phase.
This is because the TbCu 7 crystal structure phase is precipitated, and once the TbCu 7 crystal structure phase is decomposed and precipitated, it does not easily recover to the original TbCu 7 crystal structure phase. Moreover, in the normally used magnetization process of melting and casting, rapid cooling of the molten ingot is industrially difficult, and the solidification process differs depending on the cooling rate, so that other than the TbCu 7 crystal structure phase already forms after casting. In addition, it contains a considerable amount of magnetically unfavorable Th 2 Zn 17 crystal structure phase, Fe-Corich primary crystal, and CaCu 5 crystal structure phase. Furthermore, since rare earth elements have a high vapor pressure and are chemically active, ingots obtained by normal processes have significant compositional fluctuations and are likely to produce the above-mentioned undesirable metal phases. Therefore, the solution treatment process for melted and cast ingots, which is the first feature of the present invention, includes melting,
After casting, the ingot is held in a temperature range of 1150℃ to 1210℃ for 1 to 12 hours, and after treatment, it is rapidly cooled using liquid nitrogen, water, etc., and the metal phase is RM 7 phase of 90% or more. That's true. Reason for limitation The reason why the solution treatment temperature was limited to 1150°C to 1210°C is that below 1150°C, the TbCu 7 crystal structure phase, which is stable only at high temperatures, becomes ordered and immediately
This is to precipitate the Th 2 Zn 17 crystal structure phase and the CaCu 5 crystal structure phase, and at temperatures above 1210℃,
An excess of about 10% or more of the melt phase is generated in the metallic phase, which increases microscopic compositional fluctuations and significantly deteriorates the magnetic properties. In order to prevent this, the solution treatment temperature should be between 1150°C and 1210°C. Next, the reason why the solution treatment time was set to 1 hour to 12 hours is as follows. Generally, when producing large ingots, the ingots are slowly cooled during casting, so the Th 2 Zn 17 crystal structure phase and Fe
-Corich primary crystals tend to form a magnetically harmful metallic phase, which increases the solution treatment time.
If the solution treatment time is less than 1 hour, a sufficient TbCu 7 crystal structure phase cannot be obtained. If the time exceeds 12 hours, it will take too long for industrial purposes, and compositional fluctuations due to evaporation and oxidation of R and generation of magnetically harmful metal phases will be significant. Therefore, the solution treatment time is set to 1 to 12 hours. By the above optimum solution treatment at 1150°C to 1210°C for 1 hour to 12 hours, the metal phase can be made into a RM 7 phase of 90% or more. Ingots exhibiting a metallic phase of less than 90% of the RM7 phase will not exhibit excellent magnetic properties no matter what magnetic process is performed. Next, sintering in the manufacturing process is performed at 1150°C or higher in a non-oxidizing atmosphere such as argon or hydrogen, or in air.
Sintering is carried out in a temperature range of 1210℃ to improve sintering density and magnetic properties. Here, in the metal phase after sintering,
It is essential for the amount of RM7 phase to be at least 70%, preferably at least 90%, in order to obtain high magnetic properties. Further, sintering under the following conditions is effective in further improving the magnetic properties. That is, the sintering method is a sintering process in which the compression molded body obtained above is heated from room temperature to 800°C at a rate of 4 to 20°C/min in a vacuum atmosphere of 1 × 10 -2 Torr or less. It's a method. Regarding the temperature increase rate, if the temperature increase rate is less than 4℃/min, it will take more than 3 hours to reach 800℃, which is industrially unsuitable, and if the temperature increase rate exceeds 20℃/min, cannot sufficiently remove adsorbed gases, moisture, etc. Further, the degree of vacuum during heating is preferably 1×10 −2 Torr or less in order to prevent oxidation of the compression molded body during the heating process. Next, the sintering atmosphere is changed to
During the heating time of 10 to 120 minutes from 800℃ or higher to the sintering temperature and the sintering temperature holding time of 0.5 to 4 hours, mutual diffusion of R and M components is promoted, and the TbCu 7 crystal structure phase is formed. In order to stabilize the sintering density and improve magnetic properties by increasing the sintering density,
Create an argon gas atmosphere with a reduced pressure of 50 Torr to 350 Torr. If the argon gas atmosphere pressure is less than 50 Torr, the R component will evaporate preferentially, resulting in a composition that is considerably different from the final magnet composition, which will significantly impair the magnetic properties. The mutual diffusion of each component is insufficient, and the sintered density is low, resulting in poor magnetic properties. Next, regarding the cooling conditions after sintering, which is a feature of this invention, when cooling to a temperature of 800°C or less at a cooling rate in the range of 20 to 500°C/min, aging treatment after sintering, which is usually performed. There is no need to do this. The reason for limiting the cooling rate above is 20℃/min.
At a cooling rate of less than
At cooling rates exceeding 500°C/min, the RM 7 phase becomes R 2 M 17
Phase/RM Unfavorable because it does not fully decompose into 5 phases. In this invention, in order to cause fine decomposition and precipitation of the R 2 M 17 phase and the RM 5 phase, the optimum cooling rate is preferably 50 to 200° C./min. In this invention, cooling under the optimum cooling conditions means that the R 2 M 17 phase is 55 to 85% in terms of metal phase, and the remaining
The RM 5 phase is essential for obtaining excellent magnetic properties, and the magnetic properties of magnets with metal phases other than this metal phase are extremely low. Examples Examples according to the present invention will be shown below to clarify its effects. Example 1 Sm26.9wt% with a purity of 99.9% or more, Co47.6wt% with a purity of 99.8% or more, Fe12.1wt%,
An alloy consisting of 5.5wt% Ni and 7.9wt% Cu was high-frequency melted in an argon gas atmosphere and cast. The resulting ingot was subjected to solution treatment at 1180℃ for 6 hours. After treatment, it was placed in liquid nitrogen. By rapid cooling, 94% of the metal phase was RM7 . The obtained alloy was coarsely ground in an iron mortar and further finely ground in a ball mill in an organic solvent.
It was made into a μm powder. This powder was press-molded in a magnetic field of 12 kOe to obtain a compression-molded body. Next, the compression molded body is sintered at 1200°C for 2 hours in a hydrogen atmosphere, and after sintering, the permanent magnet according to the present invention is cooled at a cooling rate of 100°C/min to a temperature of 800°C or less. Obtained. In addition, as a comparative example, the same cast ingot as above was subjected to coarse pulverization, fine pulverization, press molding, and sintering under the same conditions as above without being subjected to solution treatment.
A comparative permanent magnet was obtained by solution treatment after sintering at 1160°C for 8 hours. Table 1 shows the magnetic properties of the two types of permanent magnets obtained.
【表】
実施例 2
純度99.9%以上のSm25.6wt%、Y1.5wt%、
純度99.8%以上のCo43.9wt%、Fe15.3wt%、
Ni6.6wt%、Cu7.1wt%からなる合金を、アルゴ
ンガス雰囲気中でアーク溶解し、鋳造して得られ
たインゴツトに、1150℃、8時間の溶体化処理を
施し、処理後液体窒素中に急速冷却することによ
り金属相的にRM7相を97%となした。
得られた合金を、鉄乳鉢中で粗粉砕し、さらに
有機溶剤中でボール・ミル微粉砕を行ない、2〜
10μmの粉末とした。この粉末を15kOeの磁界中
でプレス成型し、圧縮成型体を得た。つぎに圧縮
成型体を200Toorの減圧アルゴン雰囲気中で、
1200℃、2時間の焼結を行ない、焼結後、180
℃/minの冷却速度で、800℃以下の温度まで冷
却し、この発明による永久磁石を得た。
また、比較例として、鋳造後のインゴツトの溶
体化処理を施さずに、上記条件の粗粉砕、微粉
砕、プレス成型、焼結した後、1160℃、6時間の
焼結後溶体化した後、800℃、3時間の熱処理を
施すことにより比較永久磁石を得た。
得られた2種の永久磁石の磁気特性を第2表に
示す。[Table] Example 2 Sm25.6wt%, Y1.5wt% with a purity of 99.9% or higher, Co43.9wt%, Fe15.3wt% with a purity of 99.8% or higher,
An alloy consisting of 6.6wt% Ni and 7.1wt% Cu was arc melted and cast in an argon gas atmosphere.The obtained ingot was subjected to solution treatment at 1150℃ for 8 hours, and after treatment was placed in liquid nitrogen. By rapid cooling, 97% of the metal phase was RM7 . The obtained alloy was roughly pulverized in an iron mortar, and further finely pulverized with a ball mill in an organic solvent.
It was made into a powder of 10 μm. This powder was press-molded in a magnetic field of 15 kOe to obtain a compression-molded body. Next, the compression molded body is placed in a reduced pressure argon atmosphere of 200Toor.
Sintered at 1200℃ for 2 hours, after sintering, 180℃
A permanent magnet according to the present invention was obtained by cooling to a temperature of 800°C or less at a cooling rate of °C/min. In addition, as a comparative example, the ingot was not subjected to solution treatment after casting, but was subjected to coarse pulverization, fine pulverization, press molding, and sintering under the above conditions, followed by solution treatment after sintering at 1160 ° C. for 6 hours. A comparative permanent magnet was obtained by heat treatment at 800°C for 3 hours. The magnetic properties of the two types of permanent magnets obtained are shown in Table 2.
【表】
以上の実施例から明らかな如く、鋳造後のイン
ゴツトに溶体化処理し、焼結後特定温度以下に特
定の冷却速度にて冷却するこの発明方法により、
磁気特性の著しい向上が計られ、すぐれた希土類
コバルト永久磁石が製造できる。[Table] As is clear from the above examples, by the method of the present invention, in which the ingot after casting is subjected to solution treatment, and after sintering, it is cooled to a specific temperature or less at a specific cooling rate.
The magnetic properties have been significantly improved, and excellent rare earth cobalt permanent magnets can be manufactured.
Claims (1)
磁石合金(但し、RはY、La、Ce、Pr、Nb、
Sm及びミツシユメタルの1種または2種以上の
組合せ、MはCuとCo、FeもしくはNiのうち1種
または2種以上の組合せ及び該Mの一部をMn、
Ti、Nb、Zr、Ta、Hfの各元素のうち1種以上の
元素と置換した組合せ)を、 溶解して鋳造し、 1150℃〜1210℃、1時間〜12時間の溶体化処理
を施したのち、急速冷却を行つて、金属相RM7相
を90%以上生成させ、 さらに、該合金を粉砕、圧縮成型し、この圧縮
成型体を真空中または不活性雰囲気中で焼結後、 800℃以下まで20℃/min〜500℃/minの冷却
速度で冷却することを特徴とする永久磁石の製造
方法。[Claims] 1 R 2 M 17- based magnetic alloy consisting of rare earth element R and transition metal M (wherein R is Y, La, Ce, Pr, Nb,
A combination of one or more of Sm and Mitsushi metal, M is a combination of one or more of Cu and Co, Fe or Ni, and a part of M is Mn,
A combination of Ti, Nb, Zr, Ta, and Hf in which one or more elements are substituted) was melted and cast, and solution treatment was performed at 1150°C to 1210°C for 1 to 12 hours. Afterwards, rapid cooling is performed to generate 90% or more of the metallic RM 7 phase, and the alloy is further crushed and compression molded. After sintering this compression molded body in vacuum or in an inert atmosphere, the alloy is heated to 800°C. A method for manufacturing a permanent magnet, characterized by cooling at a cooling rate of 20°C/min to 500°C/min.
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP57008035A JPS58126944A (en) | 1982-01-21 | 1982-01-21 | Manufacture of permanent magnet |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP57008035A JPS58126944A (en) | 1982-01-21 | 1982-01-21 | Manufacture of permanent magnet |
Publications (2)
| Publication Number | Publication Date |
|---|---|
| JPS58126944A JPS58126944A (en) | 1983-07-28 |
| JPS629658B2 true JPS629658B2 (en) | 1987-03-02 |
Family
ID=11682076
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP57008035A Granted JPS58126944A (en) | 1982-01-21 | 1982-01-21 | Manufacture of permanent magnet |
Country Status (1)
| Country | Link |
|---|---|
| JP (1) | JPS58126944A (en) |
Cited By (1)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| JPWO2017061126A1 (en) * | 2015-10-08 | 2018-09-13 | 国立大学法人九州工業大学 | Rare earth cobalt permanent magnet |
Family Cites Families (2)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| JPS53106624A (en) * | 1977-03-02 | 1978-09-16 | Hitachi Metals Ltd | Method of making permant magnet |
| JPS5625941A (en) * | 1979-08-11 | 1981-03-12 | Namiki Precision Jewel Co Ltd | Manufacture of permanent magnet alloy |
-
1982
- 1982-01-21 JP JP57008035A patent/JPS58126944A/en active Granted
Cited By (1)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| JPWO2017061126A1 (en) * | 2015-10-08 | 2018-09-13 | 国立大学法人九州工業大学 | Rare earth cobalt permanent magnet |
Also Published As
| Publication number | Publication date |
|---|---|
| JPS58126944A (en) | 1983-07-28 |
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