JPH02104632A - Manufacture of permanent magnetic alloy - Google Patents
Manufacture of permanent magnetic alloyInfo
- Publication number
- JPH02104632A JPH02104632A JP63256616A JP25661688A JPH02104632A JP H02104632 A JPH02104632 A JP H02104632A JP 63256616 A JP63256616 A JP 63256616A JP 25661688 A JP25661688 A JP 25661688A JP H02104632 A JPH02104632 A JP H02104632A
- Authority
- JP
- Japan
- Prior art keywords
- powder
- permanent magnet
- aging treatment
- temperature
- fine powder
- 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
Links
- 238000004519 manufacturing process Methods 0.000 title claims description 8
- 229910001004 magnetic alloy Inorganic materials 0.000 title 1
- 239000000843 powder Substances 0.000 claims abstract description 40
- 230000032683 aging Effects 0.000 claims abstract description 19
- 229910052751 metal Inorganic materials 0.000 claims abstract description 13
- 239000002184 metal Substances 0.000 claims abstract description 13
- 229910052761 rare earth metal Inorganic materials 0.000 claims abstract description 8
- 239000011261 inert gas Substances 0.000 claims abstract description 7
- 238000005245 sintering Methods 0.000 claims abstract description 5
- 229910052726 zirconium Inorganic materials 0.000 claims abstract description 5
- 229910052759 nickel Inorganic materials 0.000 claims abstract description 3
- 229910052758 niobium Inorganic materials 0.000 claims abstract description 3
- 229910052715 tantalum Inorganic materials 0.000 claims abstract description 3
- 229910052735 hafnium Inorganic materials 0.000 claims abstract 2
- 229910052719 titanium Inorganic materials 0.000 claims abstract 2
- 239000000956 alloy Substances 0.000 claims description 20
- 229910045601 alloy Inorganic materials 0.000 claims description 20
- 238000001816 cooling Methods 0.000 claims description 9
- 230000001590 oxidative effect Effects 0.000 claims 1
- 238000002844 melting Methods 0.000 abstract description 9
- 230000008018 melting Effects 0.000 abstract description 9
- 238000007712 rapid solidification Methods 0.000 abstract description 7
- 229910052802 copper Inorganic materials 0.000 abstract description 4
- 229910052742 iron Inorganic materials 0.000 abstract description 3
- 229910052720 vanadium Inorganic materials 0.000 abstract description 2
- 229910000531 Co alloy Inorganic materials 0.000 abstract 2
- 230000001105 regulatory effect Effects 0.000 abstract 1
- 230000005291 magnetic effect Effects 0.000 description 22
- 238000000034 method Methods 0.000 description 17
- 239000002994 raw material Substances 0.000 description 14
- 239000000203 mixture Substances 0.000 description 13
- 230000004907 flux Effects 0.000 description 10
- 230000005415 magnetization Effects 0.000 description 8
- 239000002245 particle Substances 0.000 description 7
- 238000009792 diffusion process Methods 0.000 description 6
- 238000007664 blowing Methods 0.000 description 5
- 230000007423 decrease Effects 0.000 description 5
- 239000013078 crystal Substances 0.000 description 4
- 238000010438 heat treatment Methods 0.000 description 4
- 239000000047 product Substances 0.000 description 4
- 230000000052 comparative effect Effects 0.000 description 3
- 238000010586 diagram Methods 0.000 description 3
- 230000006698 induction Effects 0.000 description 3
- 230000008569 process Effects 0.000 description 3
- 230000009467 reduction Effects 0.000 description 3
- PNEYBMLMFCGWSK-UHFFFAOYSA-N aluminium oxide Inorganic materials [O-2].[O-2].[O-2].[Al+3].[Al+3] PNEYBMLMFCGWSK-UHFFFAOYSA-N 0.000 description 2
- 238000004458 analytical method Methods 0.000 description 2
- 238000007796 conventional method Methods 0.000 description 2
- 238000011978 dissolution method Methods 0.000 description 2
- 230000005294 ferromagnetic effect Effects 0.000 description 2
- 239000007789 gas Substances 0.000 description 2
- 230000006872 improvement Effects 0.000 description 2
- 230000005381 magnetic domain Effects 0.000 description 2
- 239000000463 material Substances 0.000 description 2
- 238000000465 moulding Methods 0.000 description 2
- 238000005191 phase separation Methods 0.000 description 2
- 238000010298 pulverizing process Methods 0.000 description 2
- 241001663154 Electron Species 0.000 description 1
- 230000005374 Kerr effect Effects 0.000 description 1
- 229910052772 Samarium Inorganic materials 0.000 description 1
- 230000015572 biosynthetic process Effects 0.000 description 1
- 239000003638 chemical reducing agent Substances 0.000 description 1
- 239000000470 constituent Substances 0.000 description 1
- 238000009826 distribution Methods 0.000 description 1
- 230000000694 effects Effects 0.000 description 1
- 238000005516 engineering process Methods 0.000 description 1
- 238000002474 experimental method Methods 0.000 description 1
- 230000007774 longterm Effects 0.000 description 1
- 239000011159 matrix material Substances 0.000 description 1
- 230000007246 mechanism Effects 0.000 description 1
- 239000002244 precipitate Substances 0.000 description 1
- 238000001556 precipitation Methods 0.000 description 1
- 238000010791 quenching Methods 0.000 description 1
- 230000000171 quenching effect Effects 0.000 description 1
- 150000002910 rare earth metals Chemical group 0.000 description 1
- 230000009291 secondary effect Effects 0.000 description 1
- 230000007704 transition Effects 0.000 description 1
- XLYOFNOQVPJJNP-UHFFFAOYSA-N water Substances O XLYOFNOQVPJJNP-UHFFFAOYSA-N 0.000 description 1
- 239000002023 wood Substances 0.000 description 1
Landscapes
- Powder Metallurgy (AREA)
- Hard Magnetic Materials (AREA)
Abstract
Description
【発明の詳細な説明】
〔産業上の利用分野〕
本発明はR1Co、、系永久磁石(ただしRは希土類元
素)の磁気特性の改良に関するものである。DETAILED DESCRIPTION OF THE INVENTION [Field of Industrial Application] The present invention relates to the improvement of the magnetic properties of R1Co permanent magnets (where R is a rare earth element).
2相分離型RgCo、?系永久磁石(ただしRは希土、
類元素)の保磁力発生機構は微細な強磁性の2つの
相を共存させることにより磁壁の移動が妨げられること
に起因している。この2つの相を共存させるためにはC
uの存在が不可欠であり、また残留磁束密度を高めるた
めにはFeの添加が有効であることから、−船釣にはC
oの一部をCuとFeで置換したものが実用化されてい
る。また近年、これにさらにZr (特開昭52−11
5000)あるいは11f(特開昭53−106326
)などの遷移元素を微量添加することによって保磁力1
Hcと最大エネルギー積(BH)+sを高めた磁石合金
が提案されている。Two-phase separation type RgCo,? system permanent magnet (where R is rare earth,
The coercive force generation mechanism of ferromagnetic elements) is due to the coexistence of two fine ferromagnetic phases, which prevents the movement of domain walls. In order for these two phases to coexist, C
Since the presence of u is indispensable and the addition of Fe is effective in increasing the residual magnetic flux density, -C is used for boat fishing.
One in which part of o is replaced with Cu and Fe has been put into practical use. In addition, in recent years, Zr (Japanese Unexamined Patent Publication No. 52-11
5000) or 11f (JP-A-53-106326
) by adding a small amount of transition elements such as
Magnet alloys with increased Hc and maximum energy product (BH)+s have been proposed.
この2相分離型のR,Co、、系永久磁石では、熱処理
である時効処理によってマトリクスに析出する微細な析
出相の状態がその保磁力の水準や第2象限の角型性を大
きく左右するため、この時効処理を最適な条件下で実施
することが製造上のポイントとなる。このためRtCo
、7系永久磁石の磁気特性の改良は時効処理を中心に行
なわれてきた。例えば特開昭50−133106には7
00〜900℃の温度から400℃近傍まで多段時効す
る方法が、特開昭53−106624には700〜90
0℃の温度から400℃近傍の温度まで徐冷する方法が
示されている。また特開昭57−161044には40
0〜750℃の温度で等温処理し、次いで600〜10
00℃を開始温度として300〜600℃まで冷却する
方法が、特開昭59−153873には750〜950
℃の温度から700℃以下の温度まで冷却する熱処理を
2回以上(り返す方法が示されている。その結果今日で
は、合金組成に応じた適切な時効処理を施すことによっ
て、1Qkoe以上の高い保磁力、11cが得られるよ
うになっている。In this two-phase separated R, Co, and permanent magnet, the state of the fine precipitated phase that precipitates in the matrix during aging treatment, which is heat treatment, greatly influences the level of coercive force and the squareness of the second quadrant. Therefore, it is important in manufacturing to carry out this aging treatment under optimal conditions. For this reason, RtCo
, 7 series permanent magnets have been improved mainly by aging treatment. For example, in JP-A-50-133106, 7
A method of multi-stage aging from 00 to 900 degrees Celsius to around 400 degrees Celsius is described in JP-A-53-106624.
A method of slowly cooling from a temperature of 0°C to a temperature around 400°C is shown. In addition, 40
Isothermal treatment at a temperature of 0-750 °C, then 600-10
A method of cooling from 300 to 600 degrees Celsius with a starting temperature of 00 degrees Celsius is disclosed in JP-A-59-153873.
℃ to 700℃ or less.As a result, today, by applying appropriate aging treatment according to the alloy composition, high A coercive force of 11c can be obtained.
ところがこのようなR2Co、7系永久磁石の磁化曲線
の第2象限にはクニックが存在し、このため残留磁束密
度の値から期待される水準に比較して得られる最大エネ
ルギー積(Bll)mの水準がかなり低下するという問
題があった。このクニックは保磁力1Hcが大きくなる
ほど顕著になる傾向がある。However, there is a knick in the second quadrant of the magnetization curve of such R2Co, 7 series permanent magnet, and therefore the maximum energy product (Bll) m obtained from the value of residual magnetic flux density is The problem was that the standard had dropped considerably. This knick tends to become more pronounced as the coercive force 1Hc increases.
従ってこのクニックは時効条件を変更し保磁力、llc
を抑制することでその程度を緩和することは可能である
。しかし時効条件の変更のみでは完全に解消することは
できない。Therefore, this knick changes the aging conditions and increases the coercive force, llc
It is possible to reduce the extent of the problem by suppressing it. However, changing the statute of limitations alone cannot completely resolve the issue.
本発明の目的は、上記問題点を解消し、高い保磁力とエ
ネルギー積を有する磁化曲線の第2象限の角型性の良い
R,Co、、系永久磁石を提供することにある。An object of the present invention is to solve the above-mentioned problems and provide an R, Co, permanent magnet having high coercive force and energy product and good squareness in the second quadrant of the magnetization curve.
本発明者等はR2Co1t系永久磁石に関し第2象限の
角型性を改善する方法について種々検討した結果、原料
粉末の製造方法に改良を加えることによって前記目的を
達成できることを見い出し、本発明を完成させるに至っ
たものである。As a result of various studies on methods for improving the squareness of the second quadrant of R2Co1t-based permanent magnets, the present inventors discovered that the above object could be achieved by improving the manufacturing method of the raw material powder, and completed the present invention. This is what led to this.
一般にI?zCoIt系永久磁石の製造においては、原
料メタルを高周波誘導溶解等で溶解して合金インゴット
を作製しそれを粉砕して原料粉末を得る溶解法と、酸化
物原料を還元剤で還元してCo粉、?粉等へ拡散させ合
金原料粉末を得るいわゆる還元拡散法とが採用されてい
る。本発明者等は研究の過程でこれら従来の製造方法で
R,Co、、系の原料粉末を作製しその磁気特性を評価
した。第1図に、実験結果の1例として、溶解法で作製
した5ra25.5wt%、Fe14.0wt%、Cu
4.4wt%、Zr2.7wt%、残部Coの永久磁石
合金の第2象限の磁化曲線(4πI−H曲線)を示す。Generally I? In the production of zCoIt-based permanent magnets, there are two methods: melting the raw metal by high-frequency induction melting to create an alloy ingot, and pulverizing it to obtain the raw material powder, and the other method by reducing the oxide raw material with a reducing agent to produce Co powder. ,? A so-called reduction diffusion method is used to obtain alloy raw material powder by diffusing it into powder or the like. In the course of research, the present inventors produced R, Co, and raw material powders using these conventional manufacturing methods and evaluated their magnetic properties. Figure 1 shows, as an example of experimental results, 5ra25.5wt%, Fe14.0wt%, Cu
The magnetization curve (4πI-H curve) in the second quadrant of a permanent magnet alloy containing 4.4 wt% Zr, 2.7 wt% Zr, and the balance Co is shown.
時効処理の条件によって保磁力の水準は変化するが、い
ずれの条件においても磁化曲線にクニックが存在し角型
性が悪いことがわかる。また、還元拡散法で作製した同
一組成の合金原料粉末を用いた場合も、第1図とほぼ同
じ結果を得た。Although the level of coercive force changes depending on the aging treatment conditions, it can be seen that under all conditions, there is a knick in the magnetization curve and the squareness is poor. Also, when alloy raw material powders of the same composition prepared by the reduction diffusion method were used, almost the same results as in FIG. 1 were obtained.
第1図の磁化曲線から、磁石内部の磁壁のピンニングの
大きさが必ずしも一様ではなく不均一であることがわか
る。またその不均一性は時効処理条件の変更に伴う保磁
力の増加に従って拡大する傾向があることがわかる。発
明者等はこのピンニングの大きさが不均一な原因を明ら
かにするために、第1図の試料に焼結温度より20℃低
い温度まで加熱し次いで室温まで急冷するという溶体化
処理を再度節こした後、S E M (Scannin
g Elect−ron Microanalyzer
)、 E P MA (Electron Prob
eMicroanalyzer LTEM (Anal
ytica’l ElectronMicroscop
e )等の機器を用いてそのミクロ組成分析をおこなっ
た。その結果、同一の結晶粒の内部においてもCuを中
心とした構成各元素の組成的な不均一性が微小ではある
が存在することが明らかになった。さらに同じ試料を時
効処理し、Kerr効果を利用した磁区観察を行なった
結果、第2象限りこおける逆磁区の発生は結晶粒界の特
定部から始まること、また上記のミクロ組成分析との対
応ではこの特定部近傍の組成は同一結晶粒内部の他の部
位に比較して相対的にはCuとSmが若干少ないことな
どが判明した。From the magnetization curve in FIG. 1, it can be seen that the magnitude of pinning of the domain wall inside the magnet is not necessarily uniform, but is non-uniform. It can also be seen that the non-uniformity tends to expand as the coercive force increases with changes in the aging treatment conditions. In order to clarify the cause of the non-uniformity in the size of this pinning, the inventors once again applied the solution treatment to the sample shown in Figure 1 by heating it to a temperature 20°C lower than the sintering temperature and then rapidly cooling it to room temperature. After straining, SEM (Scannin
g Elect-ron Microanalyzer
), E P MA (Electron Prob
eMicroanalyzer LTEM (Anal
ytica'l Electron Microscope
The microcomposition was analyzed using a device such as e). As a result, it has been revealed that even within the same crystal grain, there is slight compositional non-uniformity among the constituent elements centered on Cu. Furthermore, as a result of aging the same sample and observing magnetic domains using the Kerr effect, we found that the generation of reversed magnetic domains in the second quadrant begins from a specific part of the grain boundary, and that there is no correspondence with the above microcomposition analysis. It has been found that the composition near this specific part is relatively slightly lower in Cu and Sm than other parts within the same crystal grain.
以上の検討結果から、永久磁石の結晶粒内部のミクロ的
な組成の不均一性が時効処理によるSmCo5相の析出
状態の不均一性を誘起し、それが磁壁のピンニングの不
均一性しいては第2象限のクニックの発生をもたらすも
のと考えられる。本発明者らのその後の研究によって、
上記の永久磁石の結晶粒内部の組成の不均一性は原料粉
末内部の組成の不均一性に由来し、それはまた溶解法で
は合金インゴットの冷却過程での冷却速度の不均一性と
相分離に、還元拡散法では拡散の不均一性に起因するこ
とが明らかになった。そのため本発明者らは合金インゴ
ットあるいば永久磁石焼結体の熱処理による組成的な均
一化、焼結条件の検討による組成的な均一化を試行した
が良好な結果を得るには至らなかった。第2図に、実験
結果の1例として、溶解法で作製したがSm25.0i
yt%、Fe14.0−t%、Cu4.8ivt%、Z
r3.Qwt%、残部Coの永久磁石合金の焼結体を種
々の条件で溶体化処理した場合の時効処理後の第2象限
の磁化曲線(4πI−H曲線)を示す。溶体化処理時間
の増加に伴う第2象限のクニックの若干の改善が認めら
れ、このことからクニックの発生原因に対する先の考察
の妥当性が裏づけられる。一方間時に、長時間の溶体化
処理においてもクニックは根本的には無くならず、この
ことから熱処理による原子の拡散程度では一度発生した
組成的な不均一性は解消されないことがわかる。From the above study results, the non-uniformity of the microscopic composition inside the crystal grains of the permanent magnet induces the non-uniformity of the precipitation state of the SmCo5 phase due to aging treatment, and this causes the non-uniformity of the pinning of the domain wall. It is thought that this causes the formation of a knick in the second quadrant. Through subsequent research by the present inventors,
The non-uniformity of the composition inside the crystal grains of the above-mentioned permanent magnet originates from the non-uniformity of the composition inside the raw material powder, and in the melting method, it is also due to the non-uniformity of the cooling rate and phase separation during the cooling process of the alloy ingot. , it became clear that this is due to the non-uniformity of diffusion in the reduction-diffusion method. Therefore, the present inventors attempted to make the alloy ingot or permanent magnet sintered body uniform in composition by heat treatment and by examining the sintering conditions, but they were unable to obtain good results. . Figure 2 shows, as an example of experimental results, Sm25.0i, which was produced by the dissolution method.
yt%, Fe14.0-t%, Cu4.8ivt%, Z
r3. % Qwt%, the balance being Co, the magnetization curve (4πI-H curve) in the second quadrant after the aging treatment when the sintered body of the permanent magnet alloy was solution-treated under various conditions. A slight improvement in the knicks in the second quadrant was observed as the solution treatment time increased, and this confirms the validity of the above discussion of the cause of the knicks. On the other hand, even after long-term solution treatment, the nicks do not fundamentally disappear, and this shows that compositional non-uniformity once generated cannot be eliminated by the degree of atomic diffusion caused by heat treatment.
以上の研究結果から本発明者等は組成的に均一な原料粉
末の使用が本系永久磁石の第2象限のクニックを解消し
角型性を改善するポイントであるとの結論に達した。種
々の検討の結果、具体的には特許請求の範囲に示す組成
の溶湯を不活性ガスの高速気流中に滴下またはノズルで
吹き出して急冷凝固させて粉末化し、この粉末を原料と
してこれを通常の粉末冶金的手法によって永久磁石化す
ることにより前記目的を達成できることを見い出した。From the above research results, the present inventors have come to the conclusion that the use of a compositionally uniform raw material powder is the key to eliminating the second quadrant knick and improving the squareness of this permanent magnet. As a result of various studies, specifically, the molten metal having the composition shown in the claims is dropped into a high-speed stream of inert gas or blown out with a nozzle to rapidly solidify it into a powder, and this powder is used as a raw material to form a powder. It has been discovered that the above object can be achieved by forming a permanent magnet using a powder metallurgical method.
不活性ガス圧力は溶湯の滴下量や吹き出し量に応じてそ
の適値を選ぶ必要があるため特に限定されるものではな
いが、例えば木系溶湯をφ5のノズル穴から30kg/
分の速度で吹き出す場合には不活性ガスの行の圧力は3
0aLm以上好ましくは50〜1100at程度が適当
である。溶湯の滴下穴あるいはノズル穴の径は溶湯の量
と滴下および吹き出し速度に応じて適宜決定する必要が
あるが、例えば本系溶湯10〜100kgを10〜50
kg/分の速度で吹き出す場合にはノズル穴の径はφ3
〜10程度が適当である。また溶湯を溶解するにあたっ
てのルツボの材質はA l zOs、Mg。The inert gas pressure is not particularly limited, as it is necessary to select an appropriate value depending on the amount of dripping and blowing of the molten metal, but for example, when molten wood is 30 kg/kg from a φ5 nozzle hole,
When blowing out at a speed of 1 minute, the pressure in the inert gas line is 3
A suitable value is 0 aLm or more, preferably about 50 to 1100 at. The diameter of the molten metal dripping hole or nozzle hole needs to be determined appropriately depending on the amount of molten metal and the dropping and blowing speed.
When blowing at a speed of kg/min, the diameter of the nozzle hole is φ3.
~10 is appropriate. In addition, the material of the crucible for melting the molten metal is AlzOs and Mg.
などが使用される。ノズルの材質もルツボの材質と同一
のものが好ましい。本方法で急冷凝固して作製する粉末
は最終的には機械的粉砕によって微粉砕されるためその
粒径は特に限定されるものではないが300μ以下のも
のが全粉末の70−t%以上であることが望ましい。粒
径が大きな粉末では急冷速度が低下し本発明の目的であ
る組成的な均一性が得られにくくなるからである。粒径
の制御は溶湯の滴下あるいは吹き出し速度と不活性ガス
の圧力および流量の条件を適宜組合せることによって行
なわれる。なお、溶湯の滴下穴あるいはノズル穴の近傍
に加振装置を取り付は溶湯を加振しながら滴下あるいは
吹き出すことによって粒度分布をより狭い範囲に制御す
ることも可能である。etc. are used. It is preferable that the nozzle is made of the same material as the crucible. The powder produced by rapid solidification using this method is ultimately finely pulverized by mechanical pulverization, so its particle size is not particularly limited, but particles of 300μ or less account for 70-t% or more of the total powder. It is desirable that there be. This is because powder with a large particle size reduces the quenching rate and makes it difficult to achieve compositional uniformity, which is the object of the present invention. The particle size is controlled by appropriately combining the dropping or blowing rate of the molten metal and the pressure and flow rate of the inert gas. It is also possible to control the particle size distribution to a narrower range by installing a vibration device near the molten metal dripping hole or nozzle hole so that the molten metal is dripped or blown out while being vibrated.
また後で述べる本発明の実施例と比較例の対比からも明
らかなように、本方法で急冷凝固して作製した粉末の0
□量は従来の溶解法又は還元拡散法で作製した粗粉の0
2量に比べて低いため、同一組成の合金においてはより
高い残留磁束密度が得られる。Furthermore, as is clear from the comparison between the examples of the present invention and comparative examples described later, it is clear that the powder produced by rapid solidification by this method has a zero
□Amount is 0 of coarse powder produced by conventional dissolution method or reduction diffusion method.
Since the amount of residual magnetic flux is lower than that of 2, higher residual magnetic flux density can be obtained in alloys with the same composition.
第3図に、実験結果の1例として、本方法で急冷凝固し
て作製したSm25.5iyt%、Fe14.Owt%
。FIG. 3 shows, as an example of experimental results, Sm25.5iyt%, Fe14. Owt%
.
Cu4.4ivt%、Zr2.7wt%、残部Coの合
金粉末を永久磁石化した場合の第2象限の磁化曲線(4
πI−H曲線)を示す。本発明のR2GO+?系永久磁
石合金の具体的な製造方法については後で実施例にて詳
細な説明を加えるが、この第3図の実験シt、同じ製造
方法によっている。第3図を先の第1図と比較すること
によって、急冷凝固して作製した粉末を用いこれを永久
磁石化した場合クニックの無い角型性に優れた磁化曲線
が得られることがわかる。The magnetization curve in the second quadrant (4
πI-H curve). R2GO+ of the present invention? A detailed explanation will be given later in Examples regarding a specific manufacturing method of the permanent magnet alloy, but the same manufacturing method was used in the experiment shown in FIG. Comparing FIG. 3 with FIG. 1 above, it can be seen that when a powder produced by rapid solidification is used and made into a permanent magnet, a magnetization curve with excellent squareness and no nicks can be obtained.
この第3図の試料に溶体化処理を再度族こし、先に第1
図の試料に対しておこなったのと同じ方法でそのミクロ
組成分析をおこなったが、先の場合とは異なり同一の結
晶粒内での組成的な不均一性は検知されなかった。The sample shown in Figure 3 was subjected to solution treatment again, and first
Microcompositional analysis was carried out using the same method as for the sample shown in the figure, but unlike in the previous case, no compositional inhomogeneity within the same grain was detected.
最後に本発明のR,Go、7系永久磁石合金の組成限定
理由を説明する。希土類元素Rは22〜30wtXとさ
れる。希土類元素の含有量が22−t%未満では十分な
保磁力が得られない。また希土類元素の含有量が304
%より多い場合には残留磁束密度が低下する。Feは1
0〜25−1%とされる。10wt%未満では残留磁束
密度が低下する。25wt%より多い場合には保磁力お
よび角型性が低下する。Finally, the reasons for limiting the composition of the R, Go, 7-based permanent magnet alloy of the present invention will be explained. The rare earth element R is 22 to 30 wtX. If the rare earth element content is less than 22-t%, sufficient coercive force cannot be obtained. In addition, the content of rare earth elements is 304
%, the residual magnetic flux density decreases. Fe is 1
It is considered to be 0 to 25-1%. If it is less than 10 wt%, the residual magnetic flux density decreases. When the amount is more than 25 wt%, coercive force and squareness decrease.
Cuは1=lOwt%とされる。1wt%未満では十分
な保磁力が得られない。10wt%より多い場合には残
留磁束密度が低下する。M元素(Zr、肘、 Ti。Cu is assumed to be 1=lOwt%. If it is less than 1 wt%, sufficient coercive force cannot be obtained. When the amount is more than 10 wt%, the residual magnetic flux density decreases. M elements (Zr, elbow, Ti.
Ta、 Nb、 Ni、 Vの内の少(とも1種)は
0.2〜5wt%とされる。0.24%未満では十分な
保磁力が得られず、5wt%より多い場合には残留磁束
密度が低下する。The amount of at least one of Ta, Nb, Ni, and V is 0.2 to 5 wt%. If it is less than 0.24%, sufficient coercive force cannot be obtained, and if it is more than 5wt%, the residual magnetic flux density decreases.
以下本発明の実施例と比較例を説明するがこれによって
本発明の範囲が制限されるものではない。Examples and comparative examples of the present invention will be described below, but the scope of the present invention is not limited thereby.
(実施例1)
合計で10kgの原料をアルミナルツボに装入し、これ
を実質的な真空中で高周波誘導溶解により溶解した。次
いで溶湯をルツボ底部に設けたφ4のノズル穴から10
kg715秒の速度で80atmの圧力のAfガス気流
中に吹き出して粉末化した。この作業をくり返しおこな
って表1のNo、 1− No、 5に示す組成と0□
量を有する5種類の粉末を作製した。(Example 1) A total of 10 kg of raw materials were charged into an alumina crucible and melted by high frequency induction melting in a substantial vacuum. Next, the molten metal was passed through a φ4 nozzle hole provided at the bottom of the crucible.
kg was blown into a flow of Af gas at a pressure of 80 atm at a speed of 715 seconds to powder. By repeating this process, the compositions shown in Table 1 No. 1- No. 5 and 0□
Five types of powder were made with different amounts.
5種類の粉末は全てその総重量の80wt%以上が30
0μ以下の粒径を有するものであった。次いで各々の粉
末をジェットミルで微粉砕した。微粉の粒度は約4.0
μ(F−3−3−3)であった。All five types of powder contain 30% or more of 80wt% of their total weight.
It had a particle size of 0μ or less. Each powder was then finely ground using a jet mill. The particle size of fine powder is approximately 4.0
It was μ (F-3-3-3).
微粉を配向磁界強度10kOe、成形圧3 ton/c
+flの条件下で成形して成形体とした。成形体は11
□ガス雰囲気中で1180℃X 2 Hの条件で焼結し
た。次いで焼結体を1160℃X 4 Hの条件で溶体
化処理し水中に急冷した。最後に800℃X8Hの等温
処理をおこなった後1°(:/minの冷却速度で常温
まで徐冷するという時効処理を施した。以上の処理によ
って永久磁石合金を永久磁石化しその磁気特性を測定し
たところ表2に示すような結果を得た。Magnetic field strength for orienting fine powder: 10 kOe, molding pressure: 3 ton/c
A molded article was obtained by molding under +fl conditions. The molded body is 11
□Sintering was carried out in a gas atmosphere at 1180°C x 2 H. Next, the sintered body was subjected to solution treatment at 1160°C x 4 H and rapidly cooled in water. Finally, after performing isothermal treatment at 800°C for 8 hours, aging treatment was performed by slowly cooling to room temperature at a cooling rate of 1° (:/min). Through the above treatment, the permanent magnet alloy was turned into a permanent magnet, and its magnetic properties were measured. As a result, the results shown in Table 2 were obtained.
ここでIIKはBrX0,9の点でのI−H曲線上のH
の値である。また角型性の程度を表わす角型比はH1l
/ +IIcX 100 (%)で定義した。表2から
、本発明による永久磁石合金では60%以上という良好
な角型比が得られることがわかる。Here, IIK is H on the I-H curve at the point BrX0,9
is the value of In addition, the squareness ratio, which indicates the degree of squareness, is H1l
/+IIcX 100 (%). Table 2 shows that the permanent magnet alloy according to the present invention has a good squareness ratio of 60% or more.
(比較例1)
合計で10kgの原料をアルミナルツボに装入し、これ
を実質的な真空中で高周波誘導溶解により溶解して合金
インゴットを作製した。次いで合金インゴットをショー
クラッシャで粉砕し、300μ以下の粗粉とした。この
作業をくり返しおこなって表3のNo、 6〜No、
10に示す組成と0□量を有する5種類の粗粉を作製し
た。表1と表3の比較から、急冷凝固法によって作製し
た粉末と従来の溶解法によって作製した粗粉との間には
02量の水準に差があり、前者の方が少ないことがわか
る。表3の各粗粉を実施例1と同一の条件で処理して永
久磁石化しその磁気特性を測定したところ表4に示すよ
うな結果を得た。表4の磁気特性と表2に記載の対応す
る組成の合金の磁気特性とを比較することによって、従
来の溶解法による原料を用いた永久磁石合金の磁気特性
は本発明による永久磁石合金の磁気特性に比較して角型
性が悪くまた残留磁束密度4πIrと最大エネルギー積
(BH) mも小さいことがわかる。(Comparative Example 1) A total of 10 kg of raw materials were charged into an alumina crucible and melted by high frequency induction melting in a substantial vacuum to produce an alloy ingot. Next, the alloy ingot was crushed using a show crusher to obtain a coarse powder of 300 μm or less. Repeat this process to get No. 6 to No. 6 in Table 3.
Five types of coarse powder having the composition shown in 10 and the amount of 0□ were prepared. From a comparison of Tables 1 and 3, it can be seen that there is a difference in the amount of 02 between the powder produced by the rapid solidification method and the coarse powder produced by the conventional melting method, with the former being smaller. Each coarse powder in Table 3 was treated under the same conditions as in Example 1 to become a permanent magnet, and its magnetic properties were measured, and the results shown in Table 4 were obtained. By comparing the magnetic properties in Table 4 with the magnetic properties of the alloys with the corresponding compositions listed in Table 2, the magnetic properties of the permanent magnet alloy using conventional melting raw materials can be compared to the magnetic properties of the permanent magnet alloy according to the present invention. It can be seen that the squareness is poor compared to the characteristics, and the residual magnetic flux density 4πIr and maximum energy product (BH) m are also small.
表 1
表 3
〔発明の効果]
以上述べたように、急冷凝固法によって作製した粉末を
原料として使用することによってRZCoI7系永久磁
石の組成的な不均一性が解消され、その結果第2象眼の
角型性が改善された。また同時に原料のat量の水準が
低下するという副次的な効果によって従来より高い残留
磁束密度が得られるようになった。Table 1 Table 3 [Effect of the invention] As described above, by using the powder produced by the rapid solidification method as a raw material, the compositional non-uniformity of the RZCoI7 permanent magnet is eliminated, and as a result, the second quadrant The squareness has been improved. At the same time, a higher residual magnetic flux density than before can be obtained due to the secondary effect of lowering the level of the at content of the raw material.
第1図は従来法における時効処理条件と磁気特性の関係
を示す図。
第2図は従来法における溶体化処理条件と磁気特性の関
係を示す図。
第3図は本発明における時効処理条件と磁気特性の関係
を示す図。
第1図
H(にOe)
第2図
jI3図
H(にOe)FIG. 1 is a diagram showing the relationship between aging treatment conditions and magnetic properties in a conventional method. FIG. 2 is a diagram showing the relationship between solution treatment conditions and magnetic properties in a conventional method. FIG. 3 is a diagram showing the relationship between aging treatment conditions and magnetic properties in the present invention. Figure 1 H (to Oe) Figure 2 jI3 Figure H (to Oe)
Claims (1)
),Fe10〜25%,Cu1〜10%,M0.2〜5
%(ただしMはZr,Hf,Ti,Ta,Nb,Ni,
Vの内の少なくとも1種),残部が実質的にCoの組成
を有する合金を不活性ガス雰囲気中又は実質的な真空中
で溶解して溶湯とし、この溶湯を不活性ガスの高速気流
中に滴下またはノズルで吹き出して急冷凝固させて粉末
化し、次いでこの粉末を機械的粉砕によって微粉とし、
微粉を成形して成形体を非酸化性雰囲気中又は実質的な
真空中で1100〜1250℃の温度範囲で焼結し、焼
結体を焼結温度より10〜80℃低い温度に加熱して時
効処理開始温度以下の温度まで急冷し、最後に600〜
900℃の温度を開始温度とし400℃以下の温度まで
徐冷する時効処理を施す、ことを特徴とする永久磁石合
金の製造方法。Weight percentage: R22-30% (R is a rare earth element), Fe10-25%, Cu1-10%, M0.2-5
% (where M is Zr, Hf, Ti, Ta, Nb, Ni,
(V), the remainder of which is essentially Co, is melted into a molten metal in an inert gas atmosphere or in a substantial vacuum, and the molten metal is placed in a high-velocity stream of inert gas. Drop it or blow it out with a nozzle to rapidly solidify it into a powder, then mechanically grind it into a fine powder,
The fine powder is molded and the molded body is sintered at a temperature range of 1100 to 1250°C in a non-oxidizing atmosphere or in a substantial vacuum, and the sintered body is heated to a temperature 10 to 80°C lower than the sintering temperature. Rapid cooling to a temperature below the aging treatment start temperature, and finally 600~
A method for producing a permanent magnet alloy, which comprises performing an aging treatment with a starting temperature of 900°C and gradual cooling to a temperature of 400°C or less.
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP63256616A JPH02104632A (en) | 1988-10-12 | 1988-10-12 | Manufacture of permanent magnetic alloy |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP63256616A JPH02104632A (en) | 1988-10-12 | 1988-10-12 | Manufacture of permanent magnetic alloy |
Publications (1)
| Publication Number | Publication Date |
|---|---|
| JPH02104632A true JPH02104632A (en) | 1990-04-17 |
Family
ID=17295098
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP63256616A Pending JPH02104632A (en) | 1988-10-12 | 1988-10-12 | Manufacture of permanent magnetic alloy |
Country Status (1)
| Country | Link |
|---|---|
| JP (1) | JPH02104632A (en) |
Cited By (1)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| JPH06108190A (en) * | 1992-09-25 | 1994-04-19 | Shin Etsu Chem Co Ltd | Rare earth permanent magnet alloy |
-
1988
- 1988-10-12 JP JP63256616A patent/JPH02104632A/en active Pending
Cited By (1)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| JPH06108190A (en) * | 1992-09-25 | 1994-04-19 | Shin Etsu Chem Co Ltd | Rare earth permanent magnet alloy |
Similar Documents
| Publication | Publication Date | Title |
|---|---|---|
| US7211157B2 (en) | Rare-earth alloy, rare-earth sintered magnet, and methods of manufacturing | |
| US5963774A (en) | Method for producing cast alloy and magnet | |
| JP4596645B2 (en) | High performance iron-rare earth-boron-refractory-cobalt nanocomposites | |
| JP3267133B2 (en) | Alloy for rare earth magnet, method for producing the same, and method for producing permanent magnet | |
| US5314548A (en) | Fine grained anisotropic powder from melt-spun ribbons | |
| JPH0216368B2 (en) | ||
| CN87104923A (en) | High energy ball milling method for making rare earth-transition metal-boron permanent magnets | |
| JP3505261B2 (en) | Sm-Co permanent magnet material, permanent magnet and method for producing the same | |
| US4082582A (en) | As - cast permanent magnet sm-co-cu material, with iron, produced by annealing and rapid quenching | |
| US4983230A (en) | Platinum-cobalt alloy permanent magnets of enhanced coercivity | |
| RU2174261C1 (en) | Material for rare-earth permanent magnets and its production process | |
| Branagan et al. | Developing rare earth permanent magnet alloys for gas atomization | |
| JPH024901A (en) | Manufacture of rare earth element-fe-b series alloy magnet powder | |
| Yang et al. | High coercivity of Nd–Dy–Fe–(C, B) ribbons prepared by melt spinning | |
| JP2002083705A (en) | Anisotropic rare earth sintered magnet and method of manufacturing the same | |
| JP3423965B2 (en) | Method for producing anisotropic rare earth alloy powder for permanent magnet | |
| JPS63115304A (en) | High-performance rare-earth cast magnet | |
| JPH0582319A (en) | Permanent magnet | |
| JPS5853699B2 (en) | Method for manufacturing rare earth intermetallic compound magnets | |
| JPS58186906A (en) | Permanent magnet and preparation thereof | |
| Meira et al. | PrFeB Based Alloys Obtained by Melt Spinning for the Production of Permanent Magnets | |
| JPS62122106A (en) | Sintered permanent magnet | |
| JP2000232012A (en) | Rare earth magnet manufacturing method | |
| JP3053344B2 (en) | Rare earth magnet manufacturing method | |
| JPH0796694B2 (en) | Method of manufacturing permanent magnet material |