JPH0417604A - Manufacture of rare earth element magnet alloy powder having excellent magnetic characteristic - Google Patents
Manufacture of rare earth element magnet alloy powder having excellent magnetic characteristicInfo
- Publication number
- JPH0417604A JPH0417604A JP2122651A JP12265190A JPH0417604A JP H0417604 A JPH0417604 A JP H0417604A JP 2122651 A JP2122651 A JP 2122651A JP 12265190 A JP12265190 A JP 12265190A JP H0417604 A JPH0417604 A JP H0417604A
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- Prior art keywords
- alloy
- temperature
- rare earth
- atomic
- powder
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Classifications
-
- H—ELECTRICITY
- H01—ELECTRIC ELEMENTS
- H01F—MAGNETS; INDUCTANCES; TRANSFORMERS; SELECTION OF MATERIALS FOR THEIR MAGNETIC PROPERTIES
- H01F1/00—Magnets or magnetic bodies characterised by the magnetic materials therefor; Selection of materials for their magnetic properties
- H01F1/01—Magnets or magnetic bodies characterised by the magnetic materials therefor; Selection of materials for their magnetic properties of inorganic materials
- H01F1/03—Magnets or magnetic bodies characterised by the magnetic materials therefor; Selection of materials for their magnetic properties of inorganic materials characterised by their coercivity
- H01F1/032—Magnets 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
- H01F1/04—Magnets 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
- H01F1/047—Alloys characterised by their composition
- H01F1/053—Alloys characterised by their composition containing rare earth metals
- H01F1/055—Alloys characterised by their composition containing rare earth metals and magnetic transition metals, e.g. SmCo5
- H01F1/057—Alloys characterised by their composition containing rare earth metals and magnetic transition metals, e.g. SmCo5 and IIIa elements, e.g. Nd2Fe14B
- H01F1/0571—Alloys 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
- H01F1/0573—Alloys 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 reduction or by hydrogen decrepitation or embrittlement
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- Chemical & Material Sciences (AREA)
- Crystallography & Structural Chemistry (AREA)
- Inorganic Chemistry (AREA)
- Engineering & Computer Science (AREA)
- Power Engineering (AREA)
- Manufacture Of Metal Powder And Suspensions Thereof (AREA)
- 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〕
この発明は、Yを含む希土類元素(以下、Rで示す)と
、FcあるいはFeの一部をCOて置換した成分(以下
、Tで示す)と、Bを主成分としさらに、l、Sj、V
のうち少なくとも18以上: 0.01〜5.0原子%
を含有した合金(以下、R−T−B系合金という)を、
水素吸蔵−脱水素の水素処理することにより、磁気特性
、特に保磁力および角型性に優れたR−T−B系磁石合
金粉末を製造する方法に関するものである。[Detailed Description of the Invention] [Field of Industrial Application] This invention provides a rare earth element containing Y (hereinafter referred to as R) and a component in which a part of Fc or Fe is replaced with CO (hereinafter referred to as T). ), and with B as the main component, l, Sj, V
At least 18 or more of: 0.01 to 5.0 at%
(hereinafter referred to as R-T-B alloy) containing
The present invention relates to a method for producing an RTB magnet alloy powder having excellent magnetic properties, particularly coercive force and squareness, by hydrogen absorption-dehydrogenation treatment.
一般に、R−T−B系合金を水素吸蔵したのち脱水素処
理することによりR−T−B系磁石合金粉末を製造する
方法は、例えば、特開平1−132106号公報などに
開示されている。Generally, a method for manufacturing an RTB-based magnet alloy powder by absorbing hydrogen in an RT-B-based alloy and then dehydrogenating it is disclosed, for example, in JP-A No. 1-132106. .
上記特開平1−132106号公報に開示のR−T−B
系磁石合金粉末の製造方法は、
強磁性相であるR2T14B型金属間化合物相(以下、
R2T 14 B相という)を主相とする訃T−B系合
金インゴットまたはそのインゴットの粉砕粉を均質化処
理するかまたは均質化処理せずに、所定の高温度域のH
2雰囲気中に保持してH2吸蔵せしめ、引き続いて同高
温度域を保持しながら排気し、真空雰囲気下で脱H2処
理することにより再び上記R2T14B相を生成させる
方法で、その結果得られたR−T−B系磁石合金粉末は
、平均粒径: 0.05〜50μmの極めて微細なR2
T14B相の再結晶組織を主相とした集合組織を有し、
かつ高い磁気特性を有している。R-T-B disclosed in the above-mentioned Japanese Patent Application Laid-Open No. 1-132106
The manufacturing method of the magnet alloy powder is as follows: R2T14B type intermetallic compound phase (hereinafter referred to as
A T-B alloy ingot having R2T14 B phase as its main phase or a pulverized powder of the ingot is subjected to a homogenization treatment or is not homogenized and subjected to H in a predetermined high temperature range.
This is a method in which the R2T14B phase is generated again by holding in a 2 atmosphere to absorb H2, then evacuating while maintaining the same high temperature range, and removing H2 in a vacuum atmosphere. -T-B magnet alloy powder has extremely fine R2 particles with an average particle size of 0.05 to 50 μm.
It has a texture whose main phase is a recrystallized structure of T14B phase,
It also has high magnetic properties.
上記従来法で製造されたR−T−B系磁石合金粉末は、
優れた磁気特性を有するが、インゴットの合金組成、H
吸蔵および脱H2などの処理条件の微少な変動などによ
り、得られたR−T−B系磁石合金粉末の磁気特性、特
に保磁力や角型性にばらつき、低下などが生しることが
あった。かかる保磁力や角型性にばらつき、低下などが
生じたものは廃棄処分せざるを得ず、工業的に大量生産
する場合にかかる事態が発生することは多大の損害をこ
うむることになる。The R-T-B magnet alloy powder produced by the above conventional method is
Although it has excellent magnetic properties, the alloy composition of the ingot, H
Due to slight variations in processing conditions such as occlusion and H2 removal, the magnetic properties of the obtained R-T-B magnet alloy powder, especially the coercive force and squareness, may vary or deteriorate. Ta. Products in which the coercive force and squareness vary or deteriorate must be disposed of, and if such a situation occurs in the case of industrial mass production, a great deal of damage will be incurred.
そこで、本発明者等は、上記磁気特性、特に保磁力や角
型性にばらつき、低下などが生じたりすることなく、安
定して優れた磁気特性を有するR−T−B系磁石合金粉
末を製造すべく研究を行った結果、
(a) 温度=750〜950℃のH2雰囲気中にお
いて、R−T−B系合金インゴットまたは粉末のR2T
14B相は、
RTB→RH+T+T2B ・・・・・・・・・(1
)の相変態を起こし、続けて同温度の脱H2工程で、R
H2+T+T2B→R2T14B ・・・・・・・・・
(2)の相変態で再びR2T14B相の再結晶集合組織
となるが、上記(1)式の反応を、R−T−B系合金イ
ンゴットまたは粉末に、場所によるばらつきかなく均質
に行うためには、至温から温度750〜950℃に保持
するまでの昇温過程を、H2雰囲気中で行うことがよく
、また上記(2)式の反応は吸熱反応であるために温度
低下変動が発生し、この温度低下変動が発生すると、上
記(1)および(2)式の相変態を経て得られた再結晶
集合組織の磁気特性は低下し、また上記原料としてのR
−T−B系合金インゴットまたは粉末の容器内充填個所
に応じて温度の低下変動差が生ずることにより、得られ
たR−T−B系磁石合金粉末の磁気特性にばらつきや低
下が生する原因となっていることが解明された。Therefore, the present inventors have developed an R-T-B magnet alloy powder that has stable and excellent magnetic properties without causing variations or deterioration in the above-mentioned magnetic properties, especially coercive force and squareness. As a result of research to produce (a) R2T of R-T-B alloy ingot or powder in H2 atmosphere at a temperature of 750 to 950°C.
The 14B phase is RTB→RH+T+T2B (1
), followed by a deH2 step at the same temperature, R
H2+T+T2B→R2T14B ・・・・・・・・・
The phase transformation in (2) results in a recrystallized texture of the R2T14B phase again, but in order to uniformly carry out the reaction in equation (1) above on the R-T-B alloy ingot or powder without variations depending on location, The temperature raising process from the lowest temperature to the temperature of 750 to 950°C is often carried out in an H2 atmosphere, and since the reaction in equation (2) above is an endothermic reaction, temperature drop fluctuations occur. , when this temperature drop fluctuation occurs, the magnetic properties of the recrystallized texture obtained through the phase transformation of equations (1) and (2) above will decrease, and the R as the raw material
- Differences in temperature drop depending on the location where the T-B alloy ingot or powder is filled in the container causes variation and deterioration in the magnetic properties of the obtained R-T-B magnet alloy powder. It has been clarified that this is the case.
したかって、上記温度低下変動の発生を防止するために
は、上記R−T−B系合金インゴットまたは粉末を、蓄
熱材とともにH2雰囲気中高温度に加熱し、引き続いて
同温度真空雰囲気中に保持すると、上記(2)式の吸熱
反応による温度低下変動は上記蓄熱材の保温作用により
防止され、一定の高温度に維持されて、得られたR−T
−B系磁石合金粉末の磁気特性の低下およびばらつきが
なくなる。Therefore, in order to prevent the occurrence of the temperature drop fluctuation, the R-T-B alloy ingot or powder should be heated together with a heat storage material to a high temperature in an H2 atmosphere, and then held at the same temperature in a vacuum atmosphere. , the temperature drop fluctuation due to the endothermic reaction of the above equation (2) is prevented by the heat retention effect of the heat storage material, and the temperature is maintained at a constant high temperature.
- Eliminates deterioration and variation in magnetic properties of B-based magnet alloy powder.
(b) 上記原料としてのR−T−B系合金インゴッ
トまたは粉末の成分組成は、原子百分率で、R:8〜3
0%、
B:3〜15%、
An)、Sl、Vのうち少なくとも1種: 0.01〜
5.0%、
を含有し、残りがTおよび不可避不純物からなるR−T
−B系合金(但し、TはFeまたはFeの一部をCo:
o、01〜40%で置換した成分)を用いると、上記脱
H2工程の温度の低下変動に対して感受性か鈍くなり、
ばらつきの少ない安定して優れた磁気特性、特に保磁力
および角型性の一層優れたR−T−B系磁石合金粉末か
得られる。(b) The composition of the R-T-B alloy ingot or powder as the raw material is R: 8 to 3 in atomic percentage.
0%, B: 3 to 15%, At least one of An), Sl, and V: 0.01 to
5.0%, with the remainder consisting of T and unavoidable impurities.
-B-based alloy (where T is Fe or a part of Fe is Co:
o, a component substituted with 01 to 40%), the sensitivity to the temperature drop fluctuation in the deH2 process becomes insensitive,
It is possible to obtain an R-T-B magnet alloy powder that has stable and excellent magnetic properties with little variation, particularly excellent coercive force and squareness.
という上記(a)および(b)の知見を得たのである。The above findings (a) and (b) were obtained.
この発明は、上記知見にもとづいてなされたものであっ
て、
必要に応じて前処理として温度:600〜1200℃の
均質化処理したR−T−B系合金を、蓄熱材とともにH
2雰囲気中で昇温し、温度:750〜950℃のH2雰
囲気中に保持したのち、引き続いて同温度の真空雰囲気
中に保持し、ついで冷却し、粉砕する磁気特性に優れた
R−T−B系磁石合金粉末の製造法に特徴を有するもの
であり、このようにして得られたR−T−B系磁石合金
粉末は、さらに温度=300〜1000℃で熱処理する
ことにより一層優れた磁気特性が得られるのである。This invention was made based on the above knowledge, and the R-T-B alloy, which has been homogenized at a temperature of 600 to 1200°C as a pretreatment as necessary, is heated together with a heat storage material.
R-T-, which has excellent magnetic properties, is heated in a H2 atmosphere at a temperature of 750 to 950°C, then held in a vacuum atmosphere at the same temperature, and then cooled and crushed. It is characterized by the manufacturing method of B-based magnet alloy powder, and the R-T-B-based magnet alloy powder obtained in this way can be further heat-treated at a temperature of 300 to 1000°C to achieve even better magnetic properties. characteristics can be obtained.
つぎに、この発明の製造法における条件限定理由につい
て説明する。Next, the reason for limiting the conditions in the manufacturing method of the present invention will be explained.
(L)R−T−B系合金
原料として用いるR−T−B系合金は、一般にインゴッ
トまたはバルク状のものを用いるが、その他フレーク、
粉末など任意の形状を有するものでよく、その成分組成
は、原子百分率で、Ra8〜30%、
B、3〜15%、
を含有し、さらに、
AN、Sl、Vのうち少なくとも1種: 0.01〜5
.0%、
を含有し、残部Tおよび不可避不純物からなる組成を有
する。上記R−T−B系合金において、Rは、Yを含む
希土類元素のうち1種または2種以上であるか、特にN
d、Prまたはそられの混合物が好ましく、これにその
他の希土類元素を添加して用いられるが、その中でも特
にTb。(L) R-T-B alloy The R-T-B alloy used as a raw material is generally in the form of an ingot or a bulk, but other types such as flakes,
It may have any shape such as a powder, and its component composition contains, in atomic percentage, Ra 8-30%, B 3-15%, and at least one of AN, Sl, and V: 0 .01~5
.. 0%, with the remainder consisting of T and unavoidable impurities. In the above R-T-B alloy, R is one or more rare earth elements including Y, or especially N
d, Pr or a mixture thereof is preferred, and other rare earth elements are added thereto, among which Tb is particularly preferred.
Dyは保磁力を向上させる効果がある。Rの含有量が8
%より低いと、また30%より高いと保磁力が低下し、
高特性が得られない。Dy has the effect of improving coercive force. R content is 8
If it is lower than % or higher than 30%, the coercive force will decrease,
High characteristics cannot be obtained.
Bは、Bの一部をC,N、O,Fで置換してもよいが、
3%より低いと、また15%より高いと保磁力が低下し
高特性が得られない。B may be partially replaced with C, N, O, F,
If it is lower than 3% or higher than 15%, the coercive force decreases and high characteristics cannot be obtained.
Aj)、Si、Vは、保磁力および角型性を向上させる
元素であるか、これら元素は0 、0196より低いと
その効果が顕著に表われず、5.0%より高いと、磁化
の値、保磁力が低下し高特性が得られない。Aj), Si, and V are elements that improve coercive force and squareness.When these elements are lower than 0.0196, the effect is not noticeable, and when higher than 5.0%, they reduce magnetization. The value and coercive force decrease, making it impossible to obtain high characteristics.
残部のTは、FeまたはFeの一部をCoで置換した成
分で、Feの一部をo、oi〜4o%のCoで置換する
ことかでき、上記Feの一部をCoて置換することによ
り、耐食性、磁気特性、磁気温度特性を改善することが
できる。The remaining T is a component in which Fe or a part of Fe is replaced with Co. A part of Fe can be replaced with o, oi to 4o% of Co, and a part of the Fe can be replaced with Co. This makes it possible to improve corrosion resistance, magnetic properties, and magnetic temperature properties.
その他、必要に応じてTI 、Nb、Ta、Mo。In addition, TI, Nb, Ta, Mo as necessary.
Wのうち少なくとも1種以上をAN、Si、Vと共に総
量で5.0%以内で添加しても角型性を向上させる効果
が得られる。Even if at least one kind of W is added together with AN, Si, and V in a total amount of 5.0% or less, the effect of improving squareness can be obtained.
(2)均質化処理
上記R−T−B系合金は、均質化処理しなくてもよいが
、均質化処理することにより一層均−な磁気特性を有す
るR−T−B系磁石合金粉末が得られ、その温度は、8
00−1200”C1好ましくは1050〜1200℃
である。均質化処理温度がfioo”cより低いと均質
化処理に長時間を要するため、工業的に生産性が悪く、
一方、1200℃を越えると溶融するので好ましくない
。(2) Homogenization Treatment The above R-T-B alloy does not need to be homogenized, but by homogenizing it, the R-T-B magnet alloy powder can have more uniform magnetic properties. obtained and its temperature is 8
00-1200"C1 preferably 1050-1200℃
It is. If the homogenization temperature is lower than fioo"c, the homogenization process will take a long time, resulting in poor industrial productivity.
On the other hand, if the temperature exceeds 1200°C, it will melt, which is not preferable.
(3)昇温過程の雰囲気
室温から温度ゴ50〜950℃に保持するまでの昇温過
程をH2雰囲気中で行うと、他の真空およびAr等の不
活性ガス雰囲気で行うのに比べて、上記(1)式の相変
態がばらつきなく、均質に起りやすい。(3) Atmosphere during the heating process If the heating process from room temperature to maintaining the temperature at 50 to 950°C is carried out in an H2 atmosphere, compared to other vacuum or inert gas atmospheres such as Ar, The phase transformation of the above formula (1) tends to occur uniformly without variation.
(4)H2雰囲気および真空雰囲気における処理温度
500〜1000℃の範囲内の温度のH2雰囲気中にR
−T−B系合金を保持すると、上記(1)式に示される
相変態が起り、引き続いて同温度の真空雰囲気中に保持
すると上記(2)式の相変態が起り、再結晶集合組織が
得られるが、上記(1)および(2)式の相変態は、特
に750〜950℃で顕著に起り、磁気特性の優れた再
結晶集合組織が得られる。したがって、H2雰囲気およ
び真空雰囲気における処理温度は750〜950℃に定
めた。(4) Processing temperature in H2 atmosphere and vacuum atmosphere
When the -T-B alloy is held, the phase transformation shown by equation (1) above occurs, and when it is subsequently held in a vacuum atmosphere at the same temperature, the phase transformation shown by equation (2) above occurs, and the recrystallization texture changes. However, the phase transformations of formulas (1) and (2) above occur significantly, especially at 750 to 950°C, and a recrystallized texture with excellent magnetic properties is obtained. Therefore, the processing temperature in the H2 atmosphere and vacuum atmosphere was set at 750 to 950°C.
このようにして得られる再結晶集合組織は、平均再結晶
粒径: 0.05〜1.0−のR2T14B型金属間化
合物相を主相とする再結晶の集合組織であることが好ま
しい。The recrystallized texture obtained in this manner is preferably a recrystallized texture in which the main phase is an R2T14B type intermetallic compound phase with an average recrystallized grain size of 0.05 to 1.0.
(5)蓄熱材
上記(2)式は、吸熱反応であるから、750〜950
℃の一定温度に保持しても、保持温度の低下変動が生じ
る。上記保持温度の低下変動が生しると、得られるR−
T−B系磁石合金粉末の磁気的異方性の低下またはばら
つきが発生して好ましくない。上記保持温度低下変動を
防止するために、上記(2)式の相変態時に炉内温度を
制御して保持温度の低下変動を防止する手段も考えられ
るが、上記炉内温度の制御によるR−T−B系合金の保
持温度低下変動防止制御は、工業的には難しく、十分な
保持温度の低下変動を防止するために特別な設備を必要
とし、コストも高くなる。(5) Heat storage material Since the above equation (2) is an endothermic reaction, 750 to 950
Even if the temperature is held at a constant temperature of °C, the holding temperature will fluctuate downward. When the above holding temperature decreases and fluctuates, the obtained R-
This is undesirable because the magnetic anisotropy of the T-B magnet alloy powder decreases or varies. In order to prevent the above-mentioned holding temperature drop fluctuations, it is possible to control the furnace temperature during the phase transformation in equation (2) above to prevent the holding temperature drop fluctuations. Control to prevent fluctuations in lowering of the holding temperature of T-B alloys is industrially difficult, and requires special equipment to sufficiently prevent fluctuations in lowering of the holding temperature, resulting in high costs.
したがって、この発明では、R−T−B系合金原料を蓄
熱材と共に加熱し、上記750〜950℃内の一定温度
に保持する方法を採用したのである。Therefore, in this invention, a method is adopted in which the R-T-B alloy raw material is heated together with the heat storage material and maintained at a constant temperature within the above-mentioned range of 750 to 950°C.
上記R−T−B系合金が蓄熱材とともに共存すると、上
記(2)式の吸熱反応かあっても、蓄熱材の保温作用に
よりR−T−B系合金の保持温度低下は起こらず、簡単
に750〜950℃の範囲内の一定温度に保持すること
かできる。上記蓄熱材は、熱容量が大きく、750〜9
50”Cの水素および真空雰囲気においてR−T−B系
合金と反応しない高融点材料であれば、いかなる材料で
製造されてもよいが、特にアルミナ、マグネシア、ジル
コニアなどのセラミックスまたはタングステン、モリブ
デン、ステンレススチールなどの高融点金属材料が好ま
しい。また蓄熱材の形状は、板状、ブロック状、塊状、
球状など得られたR−T−B系磁石合金粉末と分離可能
な形状であればよい。When the above R-T-B alloy coexists with the heat storage material, even if the endothermic reaction of equation (2) occurs, the holding temperature of the R-T-B alloy does not decrease due to the heat retention effect of the heat storage material, and it is easy to The temperature can be maintained at a constant temperature within the range of 750 to 950°C. The heat storage material has a large heat capacity of 750 to 9
It may be made of any material with a high melting point that does not react with the R-T-B alloy in a 50"C hydrogen and vacuum atmosphere, but in particular ceramics such as alumina, magnesia, zirconia, or tungsten, molybdenum, High-melting point metal materials such as stainless steel are preferred.The shape of the heat storage material may be plate-like, block-like, lump-like,
It may have any shape as long as it can be separated from the obtained R-T-B magnet alloy powder, such as a spherical shape.
つぎに、蓄熱材を用いたこの発明の保持温度低下防止方
法を図面を用いて具体的に説明する。Next, the method for preventing a drop in holding temperature according to the present invention using a heat storage material will be specifically explained with reference to the drawings.
第1図は、蓄熱材として球状蓄熱材を用いた場合の断面
説明図、
第2図は、蓄熱材として板状蓄熱材を用いた場合の断面
説明図であり、
1は球状蓄熱材、1′は板状蓄熱材、2はR−T−B系
合金ブロック状インゴット、3は容器、4は加熱保持炉
である。FIG. 1 is a cross-sectional explanatory diagram when a spherical heat storage material is used as a heat storage material, and FIG. 2 is a cross-sectional explanatory diagram when a plate-shaped heat storage material is used as a heat storage material, 1 is a spherical heat storage material, 1 ' is a plate-shaped heat storage material, 2 is an R-T-B alloy block ingot, 3 is a container, and 4 is a heating and holding furnace.
第1図に示されるように、R−T−B系合金ブロック状
インゴット2を球状蓄熱材1とともに加熱保持炉4内の
容器3に充填し、上記加熱保持炉4内の雰囲気を水素雰
囲気にし、750〜950℃の範囲内の一定温度に保持
してR−T−B系合金インゴットにH2吸蔵せしめ、引
き続いて上記加熱保持炉4内の雰囲気を真空雰囲気にし
て脱H2処理しても、球状蓄熱材1が存在することによ
り吸熱反応による保持温度の低下変動は起らない。As shown in FIG. 1, an R-T-B alloy block ingot 2 is filled together with a spherical heat storage material 1 into a container 3 in a heating and holding furnace 4, and the atmosphere in the heating and holding furnace 4 is made into a hydrogen atmosphere. Even if the R-T-B alloy ingot is held at a constant temperature within the range of 750 to 950° C. to absorb H2, and then the atmosphere in the heating and holding furnace 4 is made into a vacuum atmosphere for H2 removal treatment, Due to the presence of the spherical heat storage material 1, the holding temperature does not decrease or fluctuate due to an endothermic reaction.
第2図は、蓄熱材として板状蓄熱材1′を用い、R−T
−B系合金ブロック状インゴット2を板状蓄熱材1′の
間に挾んで、第1図と同様にH2吸蔵−脱H2処理する
ものである。FIG. 2 shows the R-T
-B alloy block-shaped ingot 2 is sandwiched between plate-shaped heat storage materials 1' and subjected to H2 occlusion and H2 removal treatment in the same manner as shown in FIG.
第1図および第2図に示されるように、R−T−B系合
金インゴットを蓄熱材と共存させてH2処理すると、蓄
熱材の熱容量が太きいた。め、脱H2処理工程で吸熱反
応が起きても保持温度が低下変動することなく一定温度
に保持することができ、それによって得られたR−T−
B系磁石合金粉末は磁気特性の低下やばらつきが防止で
きる。As shown in FIGS. 1 and 2, when the R-T-B alloy ingot was treated with H2 in the presence of a heat storage material, the heat capacity of the heat storage material was increased. Therefore, even if an endothermic reaction occurs during the deH2 treatment process, the holding temperature can be maintained at a constant temperature without any decrease or fluctuation, and the obtained R-T-
B-based magnet alloy powder can prevent deterioration and variation in magnetic properties.
原料をプラズマ・アーク溶解炉により溶解し、鋳造して
第1表に示される成分組成のR−T−B系合金インゴッ
トA−Vを製造した。The raw materials were melted in a plasma arc melting furnace and cast to produce R-T-B alloy ingots A-V having the composition shown in Table 1.
これらR−T−B系合金インゴットA−Vをそれぞれ温
度: 1100℃のAr雰囲気中に40時間保持して均
質化処理を行った。These R-T-B alloy ingots A-V were each held in an Ar atmosphere at a temperature of 1100° C. for 40 hours to perform a homogenization treatment.
実施例 1
上記R−T−B系合金インゴットA−Vを約10〜30
mm角のブロック状に割り、R−T−B系合金ブロック
状インゴットを作製した。Example 1 About 10 to 30 of the above R-T-B alloy ingot A-V
It was divided into mm square blocks to produce R-T-B alloy block ingots.
一方純度: 99.9重量%、直径:5mmのアルミナ
ボールを用意し、このアルミナボールを蓄熱材として用
い、重量比て、R−T−B系合金ブロック状インゴット
:蓄熱材−1:1の割合で第1図に示されるようにアル
ミナ製容器内に共存せしめ、加熱炉に装入し、室温から
加熱炉の雰囲気を760Torrの水素ガスとし、温度
、850℃に3時間760Torrの水素雰囲気で保持
したのち、続けて温度=850℃に保持しながら、1時
間保持して脱水素を行って真空度+ I X 10’T
orrになるまて排気し、冷却した。On the other hand, alumina balls with a purity of 99.9% by weight and a diameter of 5 mm were prepared, and the alumina balls were used as a heat storage material, and the weight ratio of the R-T-B alloy block ingot to the heat storage material was 1:1. They were coexisted in an alumina container at the ratio shown in Figure 1, charged into a heating furnace, and the atmosphere in the heating furnace was changed from room temperature to 760 Torr hydrogen gas, and the temperature was raised to 850°C for 3 hours in a 760 Torr hydrogen atmosphere. After holding the temperature, continue to hold the temperature at 850°C for 1 hour to perform dehydrogenation and reduce the vacuum level to + I x 10'T.
The mixture was evacuated until it reached orr and cooled.
その後、蓄熱材と上記R−T−B系合金インゴットとを
ふるい分けして分離し、上記R−TB系合金インゴット
はブラウンミルにて、Ar雰囲気中、500−以下にな
るまで粉砕し、R−TB系磁石合金粉末を得た。Thereafter, the heat storage material and the R-T-B alloy ingot are separated by sieving, and the R-TB alloy ingot is ground in a brown mill in an Ar atmosphere until it has a particle size of 500 or less. A TB-based magnet alloy powder was obtained.
得られたR−T−B系磁石合金粉末を3重量%のエポキ
シ樹脂と混合し、20KOeの磁場中あるいは無磁場中
、圧カニ6Ton/c−で成形し、温度:120℃、6
0分保持して硬化させ、それぞれ磁場中成形ボンド磁石
および無磁場中成形ボンド磁石を作製した。得られたボ
ンド磁石の磁気特性(磁束密度B「、保磁力iHc、最
大エネルギー積BHfllaXおよび角型性Hk/IH
c但しHkは4πI−Hカーブ上でB rX 0.9の
ときの磁場を示す)を測定し、それらの測定結果を第2
表に示した。The obtained R-T-B magnet alloy powder was mixed with 3% by weight of epoxy resin and molded with a pressure crab of 6Ton/c- in a 20KOe magnetic field or in no magnetic field, at a temperature of 120°C, 6
The mixture was held for 0 minutes to cure, and a bonded magnet molded in a magnetic field and a bonded magnet molded in a non-magnetic field were produced, respectively. The magnetic properties of the obtained bonded magnet (magnetic flux density B', coercive force iHc, maximum energy product BHfllaX and squareness Hk/IH
(where Hk indicates the magnetic field when B rX is 0.9 on the 4πI-H curve), and those measurement results are
Shown in the table.
比較例 1
第1表のR−T−B系合金インゴットA〜■を均質化処
理し、約10〜30mm角のブロック状に割って得られ
たR−T−B系ブロック状インゴットを、蓄熱材なしで
上記実施例1と同様に処理したのち、粉砕し、R−T−
B系磁石合金粉末を作製し、このR−T−B系磁石合金
粉末を用いて実施例1と全く同様にしてボンド磁石を作
製し、得られたボンド磁石の磁気特性(磁束密度B「、
保磁力iHc、最大エネルギー積BHmaxおよび角型
性Hk/iHc但しHkは4πl−Hカーブ上でB r
X O,9のときの磁場を示す)を測定し、それらの結
果を第2表に示した。Comparative Example 1 R-T-B alloy ingots A to ■ in Table 1 were homogenized and divided into blocks of approximately 10 to 30 mm square. After processing in the same manner as in Example 1 above without the material, pulverization and R-T-
A B-based magnet alloy powder was produced, and a bonded magnet was produced using this R-T-B-based magnet alloy powder in exactly the same manner as in Example 1, and the magnetic properties of the obtained bonded magnet (magnetic flux density B',
Coercive force iHc, maximum energy product BHmax and squareness Hk/iHc However, Hk is Br on the 4πl-H curve
The magnetic field at X O,9) was measured, and the results are shown in Table 2.
第2表の結果から、R−T−B系ブロック状インゴット
を蓄熱材を用いてH2吸蔵および脱H2処理した場合は
、蓄熱材を用いない場合よりも、磁場中成形して得られ
たボンド磁石および磁場無し成形して得られたボンド磁
石の磁気特性が共に優れており、特に保磁力および角型
性が優れていることかわかる。From the results in Table 2, it can be seen that when the R-T-B block-shaped ingot was subjected to H2 occlusion and H2 desorption treatment using a heat storage material, the bond obtained by forming in a magnetic field was better than when no heat storage material was used. It can be seen that both the magnetic properties of the magnet and the bonded magnet obtained by molding without a magnetic field are excellent, particularly in coercive force and squareness.
実施例2〜7および比較例2〜3
合金組成が原子百分率てNd12.4PrO,2co1
5.5” 0.5 FeBadのR−T−B系合金イン
ゴットを一辺か15mm角の立方体となるように切断し
てR−T−B系合金ブロック状インゴットを作製し、こ
のインゴットを1150℃、20時間Ar雰囲気中で均
質化処理した。Examples 2 to 7 and Comparative Examples 2 to 3 Alloy composition is Nd12.4PrO,2co1 in atomic percentage
An R-T-B alloy block ingot of 5.5" 0.5 FeBad was cut into cubes with one side or 15 mm square, and this ingot was heated to 1150°C. , homogenization treatment was performed in an Ar atmosphere for 20 hours.
一方、純度: 99.9%、厚さ:5關の寸法を有する
ステンレス鋼板を用意し、このステンレス鋼板を蓄熱材
としてR−T−B系合金インゴットを第2図に示される
ように容器内に装入し、R−T−B系合金ブロック状イ
ンゴット、蓄熱材−1=3(重量比)、
の割合となるように容器内に配置し、この容器を加熱炉
に装入し、第3表に示されたH22吸蔵件にて3時間熱
処理し、続けて第3表の脱H2条件で1時間脱水素を行
って冷却した。その後、ステンレス鋼板状蓄熱材を除去
し、処理したRT−B系合金ブロック状インゴットをA
r雰囲気中ディスクミルにて500μm以下となるまで
粉砕し、R−T−B系磁石合金粉末を得た。On the other hand, a stainless steel plate with a purity of 99.9% and a thickness of 5 mm was prepared, and an R-T-B alloy ingot was placed in a container using this stainless steel plate as a heat storage material as shown in Figure 2. The R-T-B alloy block ingot is placed in a container at a ratio of -1 = 3 (weight ratio), and this container is charged into a heating furnace. Heat treatment was performed for 3 hours under the H22 storage conditions shown in Table 3, followed by dehydrogenation for 1 hour under the H2 removal conditions shown in Table 3, followed by cooling. After that, the stainless steel plate heat storage material was removed and the treated RT-B alloy block ingot was
The powder was pulverized in a disk mill in an r atmosphere until it had a particle size of 500 μm or less to obtain an R-T-B magnet alloy powder.
得られたR−T−B系磁石合金粉末を、2重量%のエポ
キシ樹脂と混合し、ついで圧カニ67on/cdでプレ
ス成形し、温度=120℃、60分間保持して硬化させ
、等方性ボンド磁石を作製した。The obtained R-T-B magnet alloy powder was mixed with 2% by weight of epoxy resin, then press-molded with a pressure crab of 67 on/cd, held at a temperature of 120°C for 60 minutes, and hardened. A bonded magnet was produced.
得られたボンド磁石の磁気特性を第3表に示す。The magnetic properties of the obtained bonded magnet are shown in Table 3.
第3表の結果から、H吸蔵および脱H2処理温度を75
0〜950℃の範囲内に保持することによりR−T−B
系磁石合金粉末を作製し、このR−T−B系磁石合金粉
末を用いて製造した等方性ボンド磁石は、保磁力JHc
および角型性Hk/fHc共に優れているが、H吸蔵お
よび脱H2処理温度が750℃未満では保磁力iHcが
十分に得られず、一方、950℃を越えると磁気特性が
極めで低下することがわかる。さらにR−T−B系磁石
合金粉末の製造に際して使用する蓄熱材としてセラミッ
クスのような非金属だけでなく、ステンレス鋼のような
耐熱合金を用いることができることもわかる。From the results in Table 3, the H storage and deH2 treatment temperature was set to 75
R-T-B by maintaining within the range of 0 to 950℃
An isotropic bonded magnet manufactured using this R-T-B magnet alloy powder has a coercive force JHc.
However, if the H occlusion and H2 removal treatment temperature is lower than 750°C, sufficient coercive force iHc cannot be obtained, and on the other hand, if it exceeds 950°C, the magnetic properties are extremely deteriorated. I understand. Furthermore, it can be seen that not only non-metals such as ceramics but also heat-resistant alloys such as stainless steel can be used as the heat storage material used in the production of RTB magnet alloy powder.
二の発明の製造法によると、H2吸蔵および脱H2処理
において蓄熱材を用いることにより、従来よりも簡単に
安定して優れた磁気特性、特に優れた保磁力および角型
性を有するR−T−B系磁石合金粉末を得ることがてき
、産業上澄れた効果をもたらすものである。According to the manufacturing method of the second invention, by using a heat storage material in H2 occlusion and H2 desorption processing, RT -B type magnet alloy powder can be obtained, which brings excellent industrial effects.
第1図および第2図は、R−T−B系合金ブロック状イ
ンゴットと蓄熱材を共存するように容器に充填したこの
発明の実施状態を示す断面概略図である。FIGS. 1 and 2 are schematic cross-sectional views showing an embodiment of the present invention in which a container is filled with an R-T-B alloy block ingot and a heat storage material so as to coexist.
Claims (5)
0原子%、 B:3〜15原子%、 を含有し、さらに、 Al,Si,Vのうち少なくとも1種:0.01〜5.
0原子%を含有し、残りがFeおよび不可避不純物から
なる合金を、蓄熱材と共に水素ガス雰囲気中で昇温し、
温度:750〜950℃の水素ガス雰囲気中に保持した
のち、引き続いて温度:750〜950℃の真空雰囲気
中に保持し、ついで、冷却し、粉砕することを特徴とす
る磁気特性に優れた希土類磁石粉末の製造法。(1) Rare earth elements containing Y (hereinafter referred to as R): 8 to 3
0 atomic %, B: 3 to 15 atomic %, and at least one of Al, Si, and V: 0.01 to 5.
An alloy containing 0 atomic % and the remainder consisting of Fe and unavoidable impurities is heated in a hydrogen gas atmosphere together with a heat storage material,
Rare earths with excellent magnetic properties characterized by being held in a hydrogen gas atmosphere at a temperature of 750 to 950°C, then held in a vacuum atmosphere at a temperature of 750 to 950°C, then cooled and pulverized. Manufacturing method of magnet powder.
0原子%を含有し、残りがFeおよび不可避不純物から
なる合金を、温度:600〜1200℃に保持して均質
化処理を行ない、 上記均質化処理した上記合金を、蓄熱材と共に水素ガス
雰囲気中で昇温し、温度:750〜950℃の水素ガス
雰囲気中に保持したのち、引き続いて温度:750〜9
50℃の真空雰囲気中に保持し、ついで、冷却し、粉砕
することを特徴とする磁気特性に優れた希土類磁石合金
粉末の製造法。(2) Contains R: 8 to 30 atom %, B: 3 to 15 atom %, and further contains at least one of Al, Si, and V: 0.01 to 5.
An alloy containing 0 atomic % and the remainder consisting of Fe and unavoidable impurities is homogenized at a temperature of 600 to 1200°C, and the homogenized alloy is placed in a hydrogen gas atmosphere together with a heat storage material. The temperature was raised at 750 to 950°C, and then maintained in a hydrogen gas atmosphere at a temperature of 750 to 950°C.
A method for producing rare earth magnet alloy powder with excellent magnetic properties, which comprises holding in a vacuum atmosphere at 50°C, then cooling and pulverizing.
0原子%を含有し、残りがFeおよび不可避不純物から
なる合金であることを特徴とする請求項1または2記載
の磁気特性に優れた希土類磁石粉末の製造法。(3) The above alloy contains R: 8 to 30 atomic %, B: 3 to 15 atomic %, Co: 0.01 to 40 atomic %, and further contains at least one of Al, Si, and V: 0.01-5.
3. The method for producing rare earth magnet powder with excellent magnetic properties according to claim 1 or 2, wherein the alloy contains 0 atomic % of Fe and the remainder consists of Fe and unavoidable impurities.
または粉末であることを特徴とする請求項1,2または
3記載の磁気特性に優れた希土類磁石合金粉末の製造法
。(4) The method for producing a rare earth magnet alloy powder with excellent magnetic properties according to claim 1, 2 or 3, wherein the alloy is a pulverized ingot, bulk, flake or powder.
クスまたは高融点金属材料からなることを特徴とする請
求項1,2,3または4記載の磁気特性に優れた希土類
磁石合金粉末の製造法。(5) The method for producing a rare earth magnet alloy powder with excellent magnetic properties according to claim 1, 2, 3 or 4, wherein the heat storage material is made of a high melting point material, preferably a ceramic or a high melting point metal material. .
Priority Applications (5)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP2122651A JPH0417604A (en) | 1990-05-11 | 1990-05-11 | Manufacture of rare earth element magnet alloy powder having excellent magnetic characteristic |
| US07/560,594 US5228930A (en) | 1989-07-31 | 1990-07-31 | Rare earth permanent magnet power, method for producing same and bonded magnet |
| DE69009335T DE69009335T2 (en) | 1989-07-31 | 1990-07-31 | Rare earth powder for permanent magnet, manufacturing process and bonded magnet. |
| EP90114691A EP0411571B1 (en) | 1989-07-31 | 1990-07-31 | Rare earth permanent magnet powder, method for producing same and bonded magnet |
| US07/978,911 US5338371A (en) | 1989-07-31 | 1992-11-19 | Rare earth permanent magnet powder, method for producing same and bonded magnet |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP2122651A JPH0417604A (en) | 1990-05-11 | 1990-05-11 | Manufacture of rare earth element magnet alloy powder having excellent magnetic characteristic |
Publications (2)
| Publication Number | Publication Date |
|---|---|
| JPH0417604A true JPH0417604A (en) | 1992-01-22 |
| JPH0579724B2 JPH0579724B2 (en) | 1993-11-04 |
Family
ID=14841254
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP2122651A Granted JPH0417604A (en) | 1989-07-31 | 1990-05-11 | Manufacture of rare earth element magnet alloy powder having excellent magnetic characteristic |
Country Status (1)
| Country | Link |
|---|---|
| JP (1) | JPH0417604A (en) |
Cited By (3)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| JPH06151132A (en) * | 1992-10-29 | 1994-05-31 | Mitsubishi Materials Corp | Method for producing anisotropic magnet material powder and method for producing magnet using anisotropic magnet material powder obtained by the method |
| US5643491A (en) * | 1992-12-28 | 1997-07-01 | Aichi Steel Works, Ltd. | Rare earth magnetic powder, its fabrication method, and resin bonded magnet |
| US6444052B1 (en) | 1999-10-13 | 2002-09-03 | Aichi Steel Corporation | Production method of anisotropic rare earth magnet powder |
-
1990
- 1990-05-11 JP JP2122651A patent/JPH0417604A/en active Granted
Cited By (3)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| JPH06151132A (en) * | 1992-10-29 | 1994-05-31 | Mitsubishi Materials Corp | Method for producing anisotropic magnet material powder and method for producing magnet using anisotropic magnet material powder obtained by the method |
| US5643491A (en) * | 1992-12-28 | 1997-07-01 | Aichi Steel Works, Ltd. | Rare earth magnetic powder, its fabrication method, and resin bonded magnet |
| US6444052B1 (en) | 1999-10-13 | 2002-09-03 | Aichi Steel Corporation | Production method of anisotropic rare earth magnet powder |
Also Published As
| Publication number | Publication date |
|---|---|
| JPH0579724B2 (en) | 1993-11-04 |
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