JPWO2017159576A1 - Method for producing RTB-based sintered magnet - Google Patents

Method for producing RTB-based sintered magnet Download PDF

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JPWO2017159576A1
JPWO2017159576A1 JP2018505902A JP2018505902A JPWO2017159576A1 JP WO2017159576 A1 JPWO2017159576 A1 JP WO2017159576A1 JP 2018505902 A JP2018505902 A JP 2018505902A JP 2018505902 A JP2018505902 A JP 2018505902A JP WO2017159576 A1 JPWO2017159576 A1 JP WO2017159576A1
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倫太郎 石井
倫太郎 石井
鉄兵 佐藤
鉄兵 佐藤
國吉 太
太 國吉
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    • BPERFORMING OPERATIONS; TRANSPORTING
    • B22CASTING; POWDER METALLURGY
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    • B22F3/00Manufacture of workpieces or articles from metallic powder characterised by the manner of compacting or sintering; Apparatus specially adapted therefor ; Presses and furnaces
    • BPERFORMING OPERATIONS; TRANSPORTING
    • B22CASTING; POWDER METALLURGY
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    • B22FWORKING METALLIC POWDER; MANUFACTURE OF ARTICLES FROM METALLIC POWDER; MAKING METALLIC POWDER; APPARATUS OR DEVICES SPECIALLY ADAPTED FOR METALLIC POWDER
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    • B22F3/24After-treatment of workpieces or articles
    • CCHEMISTRY; METALLURGY
    • C22METALLURGY; FERROUS OR NON-FERROUS ALLOYS; TREATMENT OF ALLOYS OR NON-FERROUS METALS
    • C22CALLOYS
    • C22C33/00Making ferrous alloys
    • C22C33/02Making ferrous alloys by powder metallurgy
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    • C22CALLOYS
    • C22C38/00Ferrous alloys, e.g. steel alloys
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    • H01ELECTRIC ELEMENTS
    • H01FMAGNETS; INDUCTANCES; TRANSFORMERS; SELECTION OF MATERIALS FOR THEIR MAGNETIC PROPERTIES
    • H01F1/00Magnets or magnetic bodies characterised by the magnetic materials therefor; Selection of materials for their magnetic properties
    • H01F1/01Magnets or magnetic bodies characterised by the magnetic materials therefor; Selection of materials for their magnetic properties of inorganic materials
    • H01F1/03Magnets or magnetic bodies characterised by the magnetic materials therefor; Selection of materials for their magnetic properties of inorganic materials characterised by their coercivity
    • H01F1/032Magnets or magnetic bodies characterised by the magnetic materials therefor; Selection of materials for their magnetic properties of inorganic materials characterised by their coercivity of hard-magnetic materials
    • H01F1/04Magnets or magnetic bodies characterised by the magnetic materials therefor; Selection of materials for their magnetic properties of inorganic materials characterised by their coercivity of hard-magnetic materials metals or alloys
    • H01F1/047Alloys characterised by their composition
    • H01F1/053Alloys characterised by their composition containing rare earth metals
    • H01F1/055Alloys characterised by their composition containing rare earth metals and magnetic transition metals, e.g. SmCo5
    • H01F1/057Alloys characterised by their composition containing rare earth metals and magnetic transition metals, e.g. SmCo5 and IIIa elements, e.g. Nd2Fe14B
    • HELECTRICITY
    • H01ELECTRIC ELEMENTS
    • H01FMAGNETS; INDUCTANCES; TRANSFORMERS; SELECTION OF MATERIALS FOR THEIR MAGNETIC PROPERTIES
    • H01F41/00Apparatus or processes specially adapted for manufacturing or assembling magnets, inductances or transformers; Apparatus or processes specially adapted for manufacturing materials characterised by their magnetic properties
    • H01F41/02Apparatus or processes specially adapted for manufacturing or assembling magnets, inductances or transformers; Apparatus or processes specially adapted for manufacturing materials characterised by their magnetic properties for manufacturing cores, coils, or magnets

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Abstract

R:28.5〜33.0質量%(Rは希土類元素のうち少なくとも1種であり、NdおよびPrの少なくとも1種を含む)、B:0.850〜0.910質量%、Ga:0.2〜0.7質量%、Cu:0.05〜0.50質量%、およびAl:0.05〜0.50質量%、を含有し、残部がT(TはFeとCoであり、Tの90質量%以上がFeである)および不可避的不純物であり、式(1)(14[B]/10.8<[T]/55.85([B]は質量%で示すBの含有量であり、[T]は質量%で示すTの含有量である))を満足するR−T−B系焼結磁石の製造方法であって、粒径D50および粒径D99が式(2)(3.8μm≦D50≦5.5μm)および式(3)(D99≦10μm)を満足する合金粉末を準備する工程と、前記合金粉末を成形して成形体を得る成形工程と、前記成形体を焼結して焼結体を得る焼結工程と、前記焼結体に熱処理を施す熱処理工程と、を含む、R−T−B系焼結磁石の製造方法である。R: 28.5 to 33.0% by mass (R is at least one rare earth element and includes at least one of Nd and Pr), B: 0.850 to 0.910% by mass, Ga: 0 2 to 0.7% by mass, Cu: 0.05 to 0.50% by mass, and Al: 0.05 to 0.50% by mass, the balance being T (T is Fe and Co, 90% by mass or more of T is Fe) and inevitable impurities, and the formula (1) (14 [B] /10.8 <[T] /55.85 ([B] is the mass% of B a content, the [T] is a is)) a method for producing R-T-B based sintered magnet that satisfies the content of the T represented by mass%, particle size D 50 and particle size D 99 a step of preparing an alloy powder which satisfies the equation (2) (3.8μm ≦ D 50 ≦ 5.5μm) and formula (3) (D 99 ≦ 10μm ) R-, comprising: a molding step of molding the alloy powder to obtain a molded body; a sintering step of sintering the molded body to obtain a sintered body; and a heat treatment step of applying a heat treatment to the sintered body. It is a manufacturing method of a TB type sintered magnet.

Description

本開示は、R−T−B系焼結磁石の製造方法に関する。   The present disclosure relates to a method for manufacturing an RTB-based sintered magnet.

R−T−B系焼結磁石(Rは希土類元素のうち少なくとも一種であり、NdおよびPrの少なくとも一種を含む、Tは遷移金属元素のうち少なくとも一種でありFeを必ず含む)は、R14B型結晶構造を有する化合物からなる主相と、この主相の粒界部分に位置する粒界相とから構成されており、永久磁石の中で最も高性能な磁石として知られている。An R-T-B sintered magnet (R is at least one of rare earth elements and includes at least one of Nd and Pr, T is at least one of transition metal elements and must always contain Fe), R 2 It is composed of a main phase composed of a compound having a T 14 B-type crystal structure and a grain boundary phase located at the grain boundary portion of this main phase, and is known as the most powerful magnet among permanent magnets. .

このため、ハードディスクドライブのボイスコイルモータ(VCM)、電気自動車(EV、HV、PHV)用モータ、産業機器用モータなどの各種モータや家電製品など多種多様な用途に用いられている。   For this reason, it is used for various applications such as various motors such as voice coil motors (VCM) for hard disk drives, motors for electric vehicles (EV, HV, PHV), motors for industrial equipment, and home appliances.

このように用途が広がるにつれ、例えば電気自動車用モータは、100℃〜160℃のような高温下に曝される場合があり、高温下においても安定した動作が要求されている。   As the application expands in this way, for example, electric motors for motor vehicles may be exposed to high temperatures such as 100 ° C. to 160 ° C., and stable operation is required even at high temperatures.

しかし、従来のR−T−B系焼結磁石は、高温になると保磁力HcJ(以下、単に「HcJ」と記載する場合がある)が低下し、不可逆熱減磁が起こるという問題がある。電気自動車用モータにR−T−B系焼結磁石が使用される場合、高温下での使用によりHcJが低下し、モータの安定した動作が得られない恐れがある。そのため、室温において高いHcJを有し、かつ高温においても高いHcJを有するR−T−B系焼結磁石が求められている。However, the conventional RTB -based sintered magnet has a problem that the coercive force H cJ (hereinafter sometimes simply referred to as “H cJ ”) decreases at a high temperature and irreversible thermal demagnetization occurs. is there. When an R-T-B sintered magnet is used for a motor for an electric vehicle, HcJ decreases due to use at a high temperature, and there is a possibility that stable operation of the motor cannot be obtained. Therefore, an RTB -based sintered magnet having high H cJ at room temperature and high H cJ even at high temperature is required.

従来、室温におけるHcJ向上のために、R−T−B系焼結磁石に重希土類元素RH(主としてDy)を添加していたが、残留磁束密度B(以下、単に「B」と記載する場合がある)が低下するという問題があった。さらに、Dyは、産出地が限定されている等の理由から、供給が不安定であり、また価格が大きく変動することがあるなどの問題を有している。そのため、Dyなどの重希土類元素RHをできるだけ使用せずにR−T−B系焼結磁石のHcJを向上させる技術が求められている。Conventionally, in order to improve HcJ at room temperature, a heavy rare earth element RH (mainly Dy) has been added to an RTB-based sintered magnet, but residual magnetic flux density B r (hereinafter simply referred to as “B r ”) There is a problem that it may decrease). Furthermore, Dy has problems such as supply being unstable and price fluctuating due to the limited production area. Therefore, there is a demand for a technique for improving HcJ of an R-T-B based sintered magnet without using a heavy rare earth element RH such as Dy as much as possible.

このような技術として、例えば特許文献1は、通常のR−T−B系合金よりもB量を低くするとともに、Al、GaおよびCuのうちから選ばれる1種以上である金属元素Mを含有させることによりR17相を生成させ、該R17相を原料として生成させた遷移金属リッチ相(R−T−Ga相)の体積率を充分に確保することにより、Dyの含有量を抑制しつつ、保磁力の高いR−T−B系焼結磁石が得られることを開示している。As such a technique, for example, Patent Document 1 contains a metal element M that is one or more selected from Al, Ga, and Cu while lowering the B amount than a normal RTB-based alloy. The R 2 T 17 phase is generated by the process, and the volume fraction of the transition metal rich phase (R-T-Ga phase) generated using the R 2 T 17 phase as a raw material is sufficiently ensured to contain Dy. It discloses that an RTB-based sintered magnet having a high coercive force can be obtained while suppressing the amount.

国際公開第2013/008756号公報International Publication No. 2013/008756

しかし、特許文献1に記載されるR−T−B系焼結磁石はHcJが向上しているものの、近年の要求を満足するには不十分である。However, although the RTB -based sintered magnet described in Patent Document 1 has improved HcJ , it is insufficient to satisfy recent requirements.

そこで本発明の実施形態は、高い保磁力HcJを有するR−T−B系焼結磁石の製造方法を提供することを目的とする。Then, embodiment of this invention aims at providing the manufacturing method of the RTB type | system | group sintered magnet which has high coercive force HcJ .

本発明の態様1は、R:28.5〜33.0質量%(Rは希土類元素のうち少なくとも1種であり、NdおよびPrの少なくとも1種を含む)、B:0.850〜0.910質量%、Ga:0.2〜0.7質量%、Cu:0.05〜0.50質量%、Al:0.05〜0.50質量%、を含有し、残部がT(TはFeとCoであり、Tの90質量%以上がFeである)および不可避的不純物であり、下記式(1)を満足するR−T−B系焼結磁石の製造方法であって、

14[B]/10.8<[T]/55.85 (1)
([B]は質量%で示すBの含有量であり、[T]は質量%で示すTの含有量である)

粒径D50および粒径D99が下記式(2)および(3)を満足する合金粉末を準備する工程と、前記合金粉末を成形して成形体を得る成形工程と、前記成形体を焼結して焼結体を得る焼結工程と、前記焼結体に熱処理を施す熱処理工程と、を含む、R−T−B系焼結磁石の製造方法である。

3.8μm≦D50≦5.5μm (2)
99≦10μm (3)
In aspect 1 of the present invention, R: 28.5 to 33.0 mass% (R is at least one rare earth element and includes at least one of Nd and Pr), B: 0.850 to 0.00. 910% by mass, Ga: 0.2 to 0.7% by mass, Cu: 0.05 to 0.50% by mass, Al: 0.05 to 0.50% by mass, the balance being T (T is Fe and Co, 90% by mass or more of T is Fe) and inevitable impurities, and a method for producing an RTB-based sintered magnet satisfying the following formula (1),

14 [B] /10.8 <[T] /55.85 (1)
([B] is the B content in mass%, and [T] is the T content in mass%)

A step of preparing an alloy powder having a particle size D 50 and a particle size D 99 satisfying the following formulas (2) and (3); a forming step of forming the alloy powder to obtain a formed product; It is a manufacturing method of the R-T-B system sintered magnet including the sintering process which couple | bonds together and obtains a sintered compact, and the heat processing process which heat-processes the said sintered compact.

3.8 μm ≦ D 50 ≦ 5.5 μm (2)
D 99 ≦ 10 μm (3)

本発明の態様2は、前記R−T−B系焼結磁石におけるBが0.870〜0.910質量%である、態様1に記載のR−T−B系焼結磁石の製造方法である   Aspect 2 of the present invention is the method for producing an RTB-based sintered magnet according to aspect 1, wherein B in the RTB-based sintered magnet is 0.870 to 0.910 mass%. is there

本発明の態様3は、前記粒径D50および粒径D99がさらに下記式(4)および(5)を満足する、態様1又は2に記載のR−T−B系焼結磁石の製造方法である。
3.8μm≦D50≦4.5μm (4)
99≦9μm (5)
Aspect 3 of the present invention is the production of the RTB-based sintered magnet according to aspect 1 or 2, wherein the particle diameter D 50 and the particle diameter D 99 further satisfy the following formulas (4) and (5): Is the method.
3.8 μm ≦ D 50 ≦ 4.5 μm (4)
D 99 ≦ 9 μm (5)

本発明の実施形態によれば、高い保磁力HcJを有するR−T−B系焼結磁石を製造できる方法を提供することができる。According to the embodiment of the present invention, it is possible to provide a method capable of producing an RTB -based sintered magnet having a high coercive force HcJ .

図1は、実施例における、保磁力の向上幅ΔHcJとB量との関係を表す図である。FIG. 1 is a diagram illustrating the relationship between the coercivity improvement width ΔH cJ and the B amount in the embodiment.

以下に示す実施形態は、本発明の技術思想を具体化するためのR−T−B系焼結磁石の製造方法を例示するものであって、本発明を以下に限定するものではない。   Embodiment shown below illustrates the manufacturing method of the RTB type sintered magnet for materializing the technical idea of this invention, Comprising: This invention is not limited below.

本発明者らは鋭意検討した結果、本発明の実施形態に記載するような特定の組成範囲、特に極めて狭い特定範囲のB含有量を有するR−T−B系焼結磁石の製造において、分級機等を用いて比較的大きな粒径を有する微粉末を取り除くことによって、合金粉末の粒度分布を調整することで、最終的に得られるR−T−B系焼結磁石のHcJを大幅に上昇できることを見出した。As a result of intensive studies, the present inventors have conducted classification in the production of an RTB-based sintered magnet having a specific composition range as described in the embodiment of the present invention, particularly an extremely narrow specific range of B content. By adjusting the particle size distribution of the alloy powder by removing fine powder having a relatively large particle size using a machine or the like, the HcJ of the finally obtained R-T-B system sintered magnet is greatly increased. I found that I could rise.

従来のR−T−B系焼結磁石の製造においても比較的大きな粒径を有する微粉末を取り除くことは行われてきた。しかし、後述する実施例に示す通り、本発明の特定の組成範囲外では最終的に得られるR−T−B系焼結磁石のHcJの向上幅が小さい。さらに比較的大きな粒径を有する微粉末を取り除くためには粉砕時間を長くしなければならず、粉砕能率が低下し、その結果、量産効率の悪化を招く。すなわち、従来は量産効率の悪化を招くにしてはHcJの向上幅が小さすぎるため、実際の量産では積極的に行われることは無かった。In the production of conventional RTB-based sintered magnets, fine powder having a relatively large particle size has been removed. However, as shown in the examples to be described later, outside the specific composition range of the present invention, the improvement width of HcJ of the finally obtained RTB -based sintered magnet is small. Furthermore, in order to remove fine powder having a relatively large particle size, the pulverization time must be lengthened, and the pulverization efficiency is lowered, resulting in deterioration of mass production efficiency. That is, conventionally, since the improvement in HcJ is too small to cause deterioration in mass production efficiency, it has not been actively performed in actual mass production.

しかし、本発明者らは、後述するように、本発明の実施形態の特定の組成範囲(特にB含有量が0.850〜0.910質量%)であるR−T−B系焼結磁石の製造において、平均粒径D50が3.8μm以上5.5μm以下、かつD99が10μm以下(好ましくは、平均粒径D50が3.8μm以上4.5μm以下、かつD99が9μm以下)となるように原料合金粉末を調整し、このような合金粉末を成形、焼結および熱処理することにより得られたR−T−B系焼結磁石は、粉砕時間が長くなることによる量産効率の悪化を招いたとしても積極的に行うことができるほど、大幅にHcJが向上することを見出し、本発明に至ったものである。
以下に本発明の実施形態に係る製造方法について詳述する。
However, as will be described later, the inventors of the present invention have a specific composition range (particularly, the B content is 0.850 to 0.910% by mass) according to the embodiment of the present invention. The average particle diameter D 50 is 3.8 μm or more and 5.5 μm or less, and D 99 is 10 μm or less (preferably, the average particle diameter D 50 is 3.8 μm or more and 4.5 μm or less, and D 99 is 9 μm or less. The R-T-B system sintered magnet obtained by adjusting the raw material alloy powder so as to be, and molding, sintering, and heat-treating such alloy powder has a mass production efficiency due to the longer pulverization time. As a result, the inventors have found that HcJ is greatly improved to the extent that it can be actively carried out even if the deterioration of the temperature is caused .
The manufacturing method according to the embodiment of the present invention will be described in detail below.

[R−T−B系焼結磁石]
まず、本発明の実施形態に係る製造方法により得られるR−T−B系焼結磁石について説明する。
[RTB-based sintered magnet]
First, the RTB system sintered magnet obtained by the manufacturing method according to the embodiment of the present invention will be described.

[R−T−B系焼結磁石の組成]
本実施形態に係るR−T−B系焼結磁石の組成は、
R:28.5〜33.0質量%(Rは希土類元素のうち少なくとも1種であり、NdおよびPrの少なくとも1種を含む)、
B:0.850〜0.910質量%、
Ga:0.2〜0.7質量%、
Cu:0.05〜0.50質量%、
Al:0.05〜0.50質量%、を含有し、
残部がT(TはFeとCoであり、Tの90質量%以上がFeである)および不可避的不純物であり、下記式(1)を満足する。

14[B]/10.8<[T]/55.85 (1)
([B]は質量%で示すBの含有量であり、[T]は質量%で示すTの含有量である。)
[Composition of RTB-based sintered magnet]
The composition of the RTB-based sintered magnet according to this embodiment is
R: 28.5 to 33.0% by mass (R is at least one rare earth element and includes at least one of Nd and Pr),
B: 0.850-0.910 mass%,
Ga: 0.2-0.7 mass%,
Cu: 0.05 to 0.50 mass%,
Al: 0.05 to 0.50 mass%,
The balance is T (T is Fe and Co, 90% by mass or more of T is Fe) and inevitable impurities, and satisfies the following formula (1).

14 [B] /10.8 <[T] /55.85 (1)
([B] is the B content in mass%, and [T] is the T content in mass%.)

上記組成により、一般的なR−T−B系焼結磁石よりもB量を少なくするとともに、Ga等を含有させているので、二粒子粒界にR−T−Ga相が生成して、高いHcJを得ることができる。ここで、R−T−Ga相とは、代表的にはNdFe13Ga化合物である。R13Ga化合物は、LaCo11Ga型結晶構造を有する。また、R13Ga化合物は、その状態によっては、R13−δGa1+δ化合物(δは典型的には2以下)になっている場合がある。例えば、R−T−B系焼結磁石中にCu、Alが比較的多く含有される場合、R13−δ(Ga1−x−yCuAl1+δになっている場合がある。
以下に、各組成について詳述する。
With the above composition, the amount of B is smaller than that of a general RTB-based sintered magnet, and Ga and the like are contained. Therefore, an RT-Ga phase is generated at the two-grain grain boundary, High H cJ can be obtained. Here, the R—T—Ga phase is typically an Nd 6 Fe 13 Ga compound. The R 6 T 13 Ga compound has a La 6 Co 11 Ga 3 type crystal structure. Moreover, the R 6 T 13 Ga compound may be an R 6 T 13-δ Ga 1 + δ compound (δ is typically 2 or less) depending on the state. For example, Cu in R-T-B based sintered magnet, if the Al is contained relatively large, may have been the R 6 T 13-δ (Ga 1-x-y Cu x Al y) 1 + δ is there.
Below, each composition is explained in full detail.

(R:28.5〜33.0質量%)
Rは、希土類元素のうち少なくとも1種であり、NdおよびPrの少なくとも1種を含む。Rの含有量は、28.5〜33.0質量%である。Rが28.5質量%未満であると焼結時の緻密化が困難となるおそれがあり、33.0質量%を超えると主相比率が低下して高いBを得られないおそれがある。Rの含有量は、好ましくは29.5〜32.5質量%である。Rがこのような範囲であれば、より高いBを得ることができる。
(R: 28.5-33.0% by mass)
R is at least one of rare earth elements and includes at least one of Nd and Pr. Content of R is 28.5-33.0 mass%. R is may become difficult to densification during sintering is less than 28.5% by mass may main phase proportion exceeds 33.0% by weight can not be obtained a high B r drops . The content of R is preferably 29.5 to 32.5% by mass. If R is in such a range, higher Br can be obtained.

(B:0.850〜0.910質量%)
Bの含有量は、0.850〜0.910質量%である。本発明の実施形態では特にBの含有量がこのような狭い範囲であれば、後述する合金粉末を得る工程において、合金粉末の粒度D50およびD99が本発明の実施形態で規定する所定の範囲になるように管理することで、最終的に得られるR−T−B系焼結磁石のHcJを大幅に向上することができる。Bの含有量が0.850質量%未満及び0.910質量%を超えると、高いHcJ向上効果を得ることができない。好ましくは、Bの含有量は、0.870〜0.910質量%である。より高いHcJ向上効果が得られる。
(B: 0.850 to 0.910 mass%)
Content of B is 0.850-0.910 mass%. Especially if narrow range content, such as the B-in the embodiment of the present invention, in the step of obtaining the alloy powder to be described later, the particle size D 50 and D 99 of the alloy powder is in a predetermined specified in the embodiment of the present invention By managing so that it may become a range, HcJ of the RTB system sintered magnet finally obtained can be improved significantly. When the B content is less than 0.850 mass% and exceeds 0.910 mass%, a high HcJ improvement effect cannot be obtained. Preferably, the content of B is 0.870 to 0.910 mass%. A higher HcJ improvement effect can be obtained.

さらに、Bの含有量は下記式(1)を満たす。

14[B]/10.8<[T]/55.85 (1)

式(1)を満足することにより、Bの含有量が一般的なR−T−B系焼結磁石よりも少なくなる。一般的なR−T−B系焼結磁石は、主相であるR14B相以外に軟磁性相であるR17相が生成しないように、[T]/55.85(Feの原子量)は14[B]/10.8(Bの原子量)よりも少ない組成となっている([T]は、質量%で示すTの含有量である)。本発明の実施形態のR−T−B系焼結磁石は、一般的なR−T−B系焼結磁石と異なり、[T]/55.85が14[B]/10.8よりも多くなるように式(1)で規定している。なお、本発明の実施形態のR−T−B系焼結磁石におけるTの主成分はFeであるため、Feの原子量を用いた。
Furthermore, the content of B satisfies the following formula (1).

14 [B] /10.8 <[T] /55.85 (1)

By satisfying the formula (1), the content of B becomes smaller than that of a general RTB-based sintered magnet. A general R-T-B type sintered magnet has [T] /55.85 (so that an R 2 T 17 phase, which is a soft magnetic phase, is not generated in addition to an R 2 T 14 B phase, which is a main phase. The atomic weight of Fe is less than 14 [B] /10.8 (the atomic weight of B) ([T] is the content of T expressed in mass%). The R-T-B system sintered magnet of the embodiment of the present invention differs from a general R-T-B system sintered magnet in that [T] /55.85 is greater than 14 [B] /10.8. It is defined by equation (1) so as to increase. In addition, since the main component of T in the RTB-based sintered magnet of the embodiment of the present invention is Fe, the atomic weight of Fe was used.

(Ga:0.2〜0.7質量%)
Gaの含有量は、0.2〜0.7質量%である。Gaが0.2質量%未満であると、R−T−Ga相の生成量が少なすぎて、R17相を消失させることができず、高いHcJを得ることができないおそれがあり、0.7質量%を超えると不要なGaが存在することになり、主相比率が低下してBが低下するおそれがある。
(Ga: 0.2-0.7 mass%)
The Ga content is 0.2 to 0.7% by mass. If Ga is less than 0.2% by mass, the amount of R—T—Ga phase produced is so small that R 2 T 17 phase cannot be lost and high H cJ may not be obtained. It will be present unnecessary Ga exceeds 0.7 weight%, there is a possibility that B r decreases to decrease the main phase proportion.

(Cu:0.05〜0.50質量%)
Cuの含有量は、0.05〜0.50質量%である。Cuが0.05質量%未満であると高いHcJを得ることができないおそれがあり、0.50質量%を超えると焼結性が悪化して高いHcJが得られないおそれがある。
(Cu: 0.05 to 0.50 mass%)
The content of Cu is 0.05 to 0.50 mass%. If Cu is less than 0.05% by mass, high H cJ may not be obtained, and if it exceeds 0.50% by mass, sinterability may deteriorate and high H cJ may not be obtained.

(Al:0.05〜0.50質量%)
Alの含有量は、0.05〜0.50質量%である。Alを含有することによりHcJを向上させることができる。Alは通常、製造工程で不可避的不純物として0.05質量%以上含有されるが、不可避的不純物で含有される量と意図的に添加した量の合計で0.5質量%以下含有してもよい。
(Al: 0.05 to 0.50 mass%)
The Al content is 0.05 to 0.50 mass%. By containing Al, HcJ can be improved. Al is usually contained in an amount of 0.05% by mass or more as an inevitable impurity in the production process, but it may be contained in an amount of 0.5% by mass or less in total of the amount contained by the inevitable impurity and the amount intentionally added. Good.

(残部:Tおよび不可避的不純物)
残部はTおよび不可避的不純物である。ここでTはFeとCoであり、Tの90質量%以上がFeである。Coを含有することにより耐食性を向上させることができるが、Coの置換量がFeの10質量%を超えると、高いBが得られないおそれがある。
さらに、本発明の実施形態のR−T−B系焼結磁石は、ジジム合金(Nd−Pr)、電解鉄、フェロボロンなどに通常含有される不可避的不純物としてCr、Mn、Si、La、Ce、Sm、Ca、Mgなどを含有することができる。さらに、製造工程中の不可避的不純物として、O(酸素)、N(窒素)およびC(炭素)などを例示できる。また、少量(0.1質量%程度)のV、Ni、Mo、Hf、Ta、W、Nb、Zrなどを含有してもよい。
(Remainder: T and inevitable impurities)
The balance is T and inevitable impurities. Here, T is Fe and Co, and 90% by mass or more of T is Fe. Although the corrosion resistance can be improved by containing Co, if the substitution amount of Co exceeds 10% by mass of Fe, high Br may not be obtained.
Furthermore, the RTB-based sintered magnet of the embodiment of the present invention includes Cr, Mn, Si, La, Ce as inevitable impurities usually contained in didymium alloy (Nd—Pr), electrolytic iron, ferroboron, and the like. , Sm, Ca, Mg and the like can be contained. Furthermore, O (oxygen), N (nitrogen), C (carbon), etc. can be illustrated as an inevitable impurity in a manufacturing process. Moreover, you may contain a small amount (about 0.1 mass%) of V, Ni, Mo, Hf, Ta, W, Nb, Zr, etc.

以下に、本発明の実施形態に係るR−T−B系焼結磁石の製造方法の詳細を説明する。   Below, the detail of the manufacturing method of the RTB type | system | group sintered magnet which concerns on embodiment of this invention is demonstrated.

[R−T−B系焼結磁石の製造方法]
上述した組成を有するR−T−B系焼結磁石の製造方法を説明する。R−T−B系焼結磁石の製造方法は、合金粉末を得る工程、成形工程、焼結工程、熱処理工程を有する。
以下、各工程について説明する。
[Method for producing RTB-based sintered magnet]
The manufacturing method of the RTB system sintered magnet which has the composition mentioned above is explained. The manufacturing method of a RTB system sintered magnet has a process of obtaining alloy powder, a forming process, a sintering process, and a heat treatment process.
Hereinafter, each step will be described.

(1)合金粉末を得る工程
この工程において、上述したR−T−B系焼結磁石と同じ組成を有し、粒径D50が3.8μm以上5.5μm以下であり、かつ粒径D99が10μm以下の合金粉末を得る。粒径D50およびD99がこのような範囲であり、また、本実施形態に係るR−T−B系焼結磁石の組成となるように調整した合金粉末を用いることにより、最終的に得られるR−T−B系焼結磁石は、高い保磁力HcJを有することができる。
(1) Step of obtaining alloy powder In this step, it has the same composition as the RTB-based sintered magnet described above, the particle size D 50 is 3.8 μm or more and 5.5 μm or less, and the particle size D An alloy powder with 99 of 10 μm or less is obtained. Particle size D 50 and D 99 is such a range, In addition, by using the prepared alloy powder having the composition of the R-T-B based sintered magnet according to the present embodiment, the finally obtained The obtained RTB -based sintered magnet can have a high coercive force HcJ .

このような合金粉末は、例えば次のように得ることができる。
上述したR−T−B系焼結磁石の組成となるように各元素の金属または合金(溶解原料)を準備し、ストリップキャスティング法等によりフレーク状の原料合金を作製する。次に、前記フレーク状の原料合金から合金粉末を作製する。得られたフレーク状の原料合金を水素粉砕し、例えば1.0mm以下の粗粉砕粉を得る。次に、粗粉砕粉を不活性ガス中でジェットミル等により微粉砕し、分級機を用いて、粒径の大きな微粉砕粉を取り除き、粒径D50が3.8μm以上5.5μm以下であり、かつ粒径D99が10μm以下の微粉砕粉(合金粉末)を得る。このような粒度分布を有する合金粉末を用いて上述した組成を有するR−T−B系焼結磁石を製造することにより、高い保磁力HcJを有するR−T−B系焼結磁石を得ることができる。合金粉末は、粒径D50が3.8μm以上4.5μm以下であり、かつD99が9μm以下であることがより好ましい。このような範囲であれば、最終的に得られるR−T−B系焼結磁石のHcJをより向上することができる。
Such an alloy powder can be obtained, for example, as follows.
A metal or alloy (melting raw material) of each element is prepared so as to have the composition of the above-described RTB-based sintered magnet, and a flaky raw material alloy is produced by a strip casting method or the like. Next, an alloy powder is produced from the flaky raw material alloy. The obtained flaky raw material alloy is pulverized with hydrogen to obtain coarsely pulverized powder of, for example, 1.0 mm or less. Next, the coarsely pulverized powder was finely pulverized by a jet mill or the like in an inert gas, by using a classifier to remove a large finely pulverized powder particle size, the particle size D 50 is not more than 5.5μm or 3.8μm There is obtained finely pulverized powder (alloy powder) having a particle size D 99 of 10 μm or less. An RTB -based sintered magnet having a high coercive force HcJ is obtained by manufacturing an RTB -based sintered magnet having the above-described composition using an alloy powder having such a particle size distribution. be able to. Alloy powder had a particle size D 50 is at 4.5μm or less than 3.8 .mu.m, and more preferably D 99 is 9μm or less. If it is such a range, HcJ of the RTB system sintered magnet finally obtained can be improved more.

合金粉末は、1種類の合金粉末(単合金粉末)を用いてもよいし、2種類以上の合金粉末を混合することにより合金粉末(混合合金粉末)を得る、いわゆる2合金法を用いてもよく、公知の方法などを用いて本発明の実施形態の組成となるように合金粉末を作製すればよい。なお、ジェットミル粉砕前の粗粉砕粉、ジェットミル粉砕中およびジェットミル粉砕後の合金粉末に助剤として公知の潤滑剤を添加してもよい。   As the alloy powder, one kind of alloy powder (single alloy powder) may be used, or a so-called two alloy method may be used in which an alloy powder (mixed alloy powder) is obtained by mixing two or more kinds of alloy powder. The alloy powder may be produced using a known method or the like so as to obtain the composition of the embodiment of the present invention. A known lubricant may be added as an auxiliary agent to the coarsely pulverized powder before jet mill pulverization, and the alloy powder during and after jet mill pulverization.

上述のように、本実施形態に係る合金粉末は特定の範囲の粒径D50およびD99を有するが、粒径D50およびD99は、気流分散式レーザー回折法(JIS Z 8825:2013年改訂版に準拠する)により測定することができる。すなわち、本明細書において、D50は、小粒径側からの積算粒度分布(体積基準)が50%となる粒径(メジアン径)を意味し、D99は、小粒径側からの積算粒度分布(体積基準)が99%となる粒径を意味する。
なお本発明の実施形態におけるD50とD99は、Sympatec社製の粒度分布測定装置「HELOS&RODOS」において
分散圧:4bar
測定レンジ:R2
計算モード:HRLD
の条件にて測定されたD50とD99のことを示す。
As described above, the alloy powder according to the present embodiment has a specific range of particle diameters D 50 and D 99 , and the particle diameters D 50 and D 99 are determined based on the air flow dispersion type laser diffraction method (JIS Z 8825: 2013). According to the revised version). That is, in the present specification, D 50 means a particle size (median diameter) at which the integrated particle size distribution (volume basis) from the small particle size side is 50%, and D 99 is an integration from the small particle size side. It means the particle size at which the particle size distribution (volume basis) is 99%.
Note D 50 and D 99 in the embodiment of the present invention, dispersing pressure in Sympatec Co. particle size distribution measuring apparatus "HELOS &RODOS": 4 bar
Measurement range: R2
Calculation mode: HRLD
It shows D 50 and D 99 measured under the following conditions.

(2)成形工程
得られた合金粉末を用いて磁界中成形を行い、成形体を得る。磁界中成形は、金型のキャビティー内に乾燥した合金粉末を挿入し、磁界を印加しながら成形する乾式成形法、金型のキャビティー内に該合金粉末を分散させたスラリーを注入し、スラリーの分散媒を排出しながら成形する湿式成形法を含む既知の任意の磁界中成形方法を用いてよい。
(2) Forming step Using the obtained alloy powder, forming in a magnetic field is performed to obtain a formed body. In the magnetic field molding, a dry alloy method in which a dry alloy powder is inserted into a mold cavity and molded while applying a magnetic field, a slurry in which the alloy powder is dispersed is injected into the mold cavity, Any known forming method in a magnetic field may be used, including a wet forming method of forming while discharging the slurry dispersion medium.

(3)焼結工程
成形体を焼結することにより焼結体(焼結磁石)を得る。成形体の焼結は既知の方法を用いることができる。なお、焼結時の雰囲気による酸化を防止するために、焼結は、真空雰囲気中または雰囲気ガス中で行うことが好ましい。雰囲気ガスは、ヘリウム、アルゴンなどの不活性ガスを用いることが好ましい。
(3) Sintering process A sintered compact (sintered magnet) is obtained by sintering a molded object. A known method can be used for sintering the molded body. In addition, in order to prevent the oxidation by the atmosphere at the time of sintering, it is preferable to perform sintering in a vacuum atmosphere or atmospheric gas. The atmosphere gas is preferably an inert gas such as helium or argon.

(4)熱処理工程
得られた焼結磁石に対し、磁気特性を向上させることを目的とした熱処理を行うことが好ましい。熱処理温度、熱処理時間などは既知の条件を用いることができる。例えば、比較的低い温度(400℃以上600℃以下)のみでの熱処理(一段熱処理)をしてもよく、あるいは比較的高い温度(700℃以上焼結温度以下(例えば1050℃以下))で熱処理を行った後比較的低い温度(400℃以上600℃以下)で熱処理(二段熱処理)をしてもよい。好ましい条件は、730℃以上1020℃以下で5分から500分程度の熱処理を施し、冷却後(室温まで冷却後、または440℃以上550℃以下まで冷却後)、さらに440℃以上550℃以下で5分から500分程度熱処理をすることが挙げられる。熱処理雰囲気は、真空雰囲気あるいは不活性ガス(ヘリウムやアルゴンなど)で行うことが好ましい。
(4) Heat treatment process It is preferable to perform the heat processing for the purpose of improving a magnetic characteristic with respect to the obtained sintered magnet. Known conditions can be used for the heat treatment temperature, the heat treatment time, and the like. For example, heat treatment (one-step heat treatment) only at a relatively low temperature (400 ° C. or more and 600 ° C. or less) may be performed, or heat treatment is performed at a relatively high temperature (700 ° C. or more and sintering temperature or less (eg, 1050 ° C. or less)). After performing, heat treatment (two-stage heat treatment) may be performed at a relatively low temperature (400 ° C. or more and 600 ° C. or less). Preferable conditions are as follows: heat treatment at 730 ° C. to 1020 ° C. for 5 minutes to 500 minutes, cooling (after cooling to room temperature or after cooling to 440 ° C. to 550 ° C.), and further at 440 ° C. to 550 ° C. Heat treatment for about 500 minutes to 500 minutes. The heat treatment atmosphere is preferably a vacuum atmosphere or an inert gas (such as helium or argon).

最終的な製品形状にするなどの目的で、得られた焼結磁石に研削などの機械加工を施してもよい。その場合、熱処理は機械加工前でも機械加工後でもよい。さらに、得られた焼結磁石に、表面処理を施してもよい。表面処理は、既知の表面処理であってもよく、例えばAl蒸着や電気Niめっきや樹脂塗料などの表面処理を行うことができる。   For the purpose of obtaining a final product shape, the obtained sintered magnet may be subjected to machining such as grinding. In that case, the heat treatment may be performed before or after machining. Furthermore, you may surface-treat to the obtained sintered magnet. The surface treatment may be a known surface treatment, and for example, a surface treatment such as Al deposition, electric Ni plating, or resin coating can be performed.

本発明を実施例によりさらに詳細に説明するが、本発明はそれらに限定されるものではない。   The present invention will be described in more detail with reference to examples, but the present invention is not limited thereto.

・実施例1
表1の試料No.1〜27に示すR−T−B系焼結磁石の組成となるように各元素を秤量し、ストリップキャスト法により合金を作製した。得られた各合金を水素粉砕法により粗粉砕し粗粉砕粉を得た。前記粗粉砕粉を、以下に説明するA〜Cのいずれかの条件で、それぞれジェットミルにより微粉砕を行った(但し、条件Cで微粉砕を行ったのは試料No.13のみ)。
Example 1
Sample No. in Table 1 Each element was weighed so as to have the composition of the RTB-based sintered magnet shown in 1-27, and an alloy was produced by strip casting. Each obtained alloy was coarsely pulverized by a hydrogen pulverization method to obtain a coarsely pulverized powder. The coarsely pulverized powder was finely pulverized by a jet mill under any of conditions A to C described below (however, only sample No. 13 was finely pulverized under condition C).

(条件A)
条件Aは、ジェットミルへの原料供給量を200g/分、分級ロータ回転数を4500rpmにして微粉砕を行った。粉砕時間は約10分であった。条件Aは通常の粉砕条件であり、狙い値は粒径D50:4μm、粒径D99:12μmである。尚、前記D50及び前記D99は、それぞれ、気流分散法によるレーザー回折法で得られる粒度分布において、小粒径側からの積算粒度分布(体積基準)が50%となる粒径及び小粒径側からの積算粒度分布(体積基準)が99%となる粒径である。また、D50及びD99は、Sympatec社製の粒度分布測定装置「HELOS&RODOS」を用いて、分散圧:4bar、測定レンジ:R2、計算モード:HRLDの条件にて測定した。
(Condition A)
Condition A was that fine pulverization was performed at a feed rate of 200 g / min to the jet mill and a classification rotor rotation speed of 4500 rpm. The grinding time was about 10 minutes. Condition A is normal pulverization conditions, and target values are a particle size D 50 : 4 μm and a particle size D 99 : 12 μm. The D 50 and the D 99 are respectively a particle size and a small particle in which the cumulative particle size distribution (volume basis) from the small particle size side is 50% in the particle size distribution obtained by the laser diffraction method by the air flow dispersion method. The particle size at which the cumulative particle size distribution (volume basis) from the diameter side is 99%. D 50 and D 99 were measured under the conditions of dispersion pressure: 4 bar, measurement range: R2, and calculation mode: HRLD using a particle size distribution measuring apparatus “HELOS & RODOS” manufactured by Sympatec.

(条件B)
条件Bは、ジェットミルへの原料供給量を50g/分、分級ロータ回転数を5500rpmにして微粉砕を行った。粉砕時間は約40分であった。条件Bは、本発明の実施形態の粒径(D50及びD99)を得るために行うものであり、狙い値は粒径D50:4μm、粒径D99:9.5μmである。条件Cは、ジェットミルへの原料供給量を50g/分、分級ロータ回転数を6000rpmにして微粉砕を行った。粉砕時間は約40分であった。
(Condition B)
Condition B was fine pulverization with the raw material supply rate to the jet mill set to 50 g / min and the classification rotor rotation speed set to 5500 rpm. The grinding time was about 40 minutes. Condition B is performed to obtain the particle diameters (D 50 and D 99 ) of the embodiment of the present invention, and the target values are the particle diameter D 50 : 4 μm and the particle diameter D 99 : 9.5 μm. Condition C was that fine pulverization was performed with the raw material supply rate to the jet mill set to 50 g / min and the classification rotor rotation speed set to 6000 rpm. The grinding time was about 40 minutes.

(条件C)
条件Cは、本発明の実施形態の好ましい粒径(D50及びD99)を得るために行うものであり、狙い値は粒径D50:4μm、粒径D99:8.5μmである。
(Condition C)
Condition C is performed in order to obtain preferable particle diameters (D 50 and D 99 ) of the embodiment of the present invention, and target values are a particle diameter D 50 : 4 μm and a particle diameter D 99 : 8.5 μm.

各条件で微粉砕して得られた微粉砕粉の粒径(D50及びD99)の実測値を表2及び表3に示す。表2の「条件A」には、試料No.1〜27を条件Aで微粉砕して得られた微粉砕粉の粒径の実測値が示されている。表2の「条件B」には、試料No.1〜27を条件Bで微粉砕して得られた微粉砕粉の粒径の実測値が示されている。表3の「条件A」には、試料No.13を条件Aで微粉砕して得られた粒径の実測値が示されている。表3の「条件C」には、試料No.13を条件Cで微粉砕して得られた粒径の実測値が示されている。Tables 2 and 3 show the actual measured values of the particle diameters (D 50 and D 99 ) of the finely pulverized powder obtained by pulverizing under each condition. In “Condition A” of Table 2, sample No. Measured values of the particle size of finely pulverized powder obtained by finely pulverizing 1-27 under condition A are shown. In “Condition B” in Table 2, sample No. The measured value of the particle size of the finely pulverized powder obtained by pulverizing 1-27 under the condition B is shown. In “Condition A” of Table 3, sample No. The actual measured value of the particle size obtained by pulverizing 13 under condition A is shown. In “Condition C” of Table 3, sample No. The measured value of the particle size obtained by pulverizing 13 under the condition C is shown.

得られた微粉砕粉(合金粉末)に、潤滑剤としてステアリン酸亜鉛を微粉砕粉100質量部に対して0.05質量部添加、混合した後、磁界中で成形し、成形体を得た。なお、成形装置には、磁界印加方向と加圧方向とが直交する、いわゆる直角磁界成形装置(横磁界成形装置)を用いた。得られた成形体を、真空中で組成に応じて1030〜1070℃で4時間焼結し、R−T−B系焼結磁石を得た。焼結磁石の密度は7.5Mg/m以上であった。さらに焼結後のR−T−B系焼結磁石に対し、800℃で2時間保持した後室温まで急冷し、次いで500℃で2時間保持した後室温まで冷却する熱処理を施した。After adding and mixing 0.05 parts by mass of zinc stearate as a lubricant with respect to 100 parts by mass of finely pulverized powder, the resulting finely pulverized powder (alloy powder) was molded in a magnetic field to obtain a molded body. . In addition, what was called a right-angle magnetic field shaping | molding apparatus (lateral magnetic field shaping | molding apparatus) in which the magnetic field application direction and the pressurization direction orthogonally cross was used for the shaping | molding apparatus. The obtained molded body was sintered in vacuum at 1030 to 1070 ° C. for 4 hours according to the composition to obtain an RTB-based sintered magnet. The density of the sintered magnet was 7.5 Mg / m 3 or more. Further, the sintered RTB-based sintered magnet was held at 800 ° C. for 2 hours, then rapidly cooled to room temperature, then held at 500 ° C. for 2 hours and then cooled to room temperature.

得られた焼結磁石の成分を求めるために、Nd、Pr、Tb、B、Co、Al、Cu、Ga、Nb、Zr、Feの含有量をICP発光分光分析法により測定した。さらに、O(酸素量)はガス融解−赤外線吸収法、N(窒素量)はガス融解−熱伝導法、C(炭素量)は燃焼−赤外線吸収法、によるガス分析装置を使用して測定した。結果を表1に示す。   In order to determine the components of the obtained sintered magnet, the contents of Nd, Pr, Tb, B, Co, Al, Cu, Ga, Nb, Zr, and Fe were measured by ICP emission spectroscopy. Further, O (oxygen amount) was measured using a gas melting-infrared absorption method, N (nitrogen amount) was measured using a gas melting-heat conduction method, and C (carbon amount) was measured using a combustion-infrared absorption method. . The results are shown in Table 1.

熱処理後の焼結磁石に機械加工を施し、縦7mm、横7mm、厚み7mmの試料を作製し、B−Hトレーサによって各試料の特性(B及びHcJ)を測定した。測定結果を表2及び表3に示す。
なお、表2および表3の備考欄に記載された「本発明例」とは、本発明の実施形態に規定する要件を満たす実施例であることを意味する。
The sintered magnet after the heat treatment was machined to prepare samples having a length of 7 mm, a width of 7 mm, and a thickness of 7 mm, and the characteristics (B r and H cJ ) of each sample were measured with a BH tracer. The measurement results are shown in Tables 2 and 3.
The “examples of the present invention” described in the remarks column of Tables 2 and 3 mean examples that satisfy the requirements defined in the embodiments of the present invention.

表2の「条件A」には、表1の試料No.1〜27の組成を有する合金を条件Aで微粉砕し、得られた微粉砕粉を焼結、熱処理して得られた焼結磁石の特性値が示されている。表2の「条件B」には、表1の試料No.1〜27の組成を有する合金を条件Bで微粉砕し、得られた微粉砕粉を焼結、熱処理して得られた焼結磁石の特性値(B及びHcJの値)が示されている。また、表2の「条件B−条件A」には、微粉砕の条件を条件Aから条件Bに変更したことによる焼結磁石のHcJの向上幅(ΔHcJ)を示されている。つまり、表2におけるΔHcJは、微粉砕粉を条件Aまたは条件Bで作製することにより得られたR−T−B系焼結磁石におけるHcJの差(条件Bを用いて得られたR−T−B系焼結磁石のHcJの値から条件Aを用いて得られたR−T−B系焼結磁石のHcJの値を引いたもの)である。In “Condition A” of Table 2, the sample No. The characteristic values of sintered magnets obtained by pulverizing an alloy having a composition of 1 to 27 under condition A and sintering and heat-treating the obtained finely pulverized powder are shown. In “Condition B” in Table 2, the sample No. Alloy was milled in condition B the having a composition of 1 to 27, sintering the finely pulverized powder obtained, the characteristic values of the sintered magnet obtained by heat treatment (the value of B r and H cJ) is shown ing. Further, “Condition B—Condition A” in Table 2 shows the improvement width (ΔH cJ ) of the sintered magnet by changing the pulverization condition from Condition A to Condition B. That is, ΔH cJ in Table 2 is the difference in H cJ in the R-T-B system sintered magnet obtained by producing finely pulverized powder under Condition A or Condition B (R obtained using Condition B). The value obtained by subtracting the value of HcJ of the RTB -based sintered magnet obtained using Condition A from the value of HcJ of the TB-based sintered magnet).

表3の「条件A」には、表1の試料No.13の組成を有する合金を条件Aで微粉砕し、得られた微粉砕粉を焼結、熱処理して得られた焼結磁石の特性値が示されている。表3の「条件C」には、表1の試料No.13の組成を有する合金を条件Cで微粉砕し、得られた微粉砕粉を焼結、熱処理して得られた焼結磁石の特性値が示されている。表3の「条件C−条件A」には、微粉砕の条件を条件Aから条件Cに変更したことによる焼結磁石のHcJの向上幅(ΔHcJ)が示されている。つまり、表3におけるΔHcJは、微粉砕粉を条件Aまたは条件Cで作製することにより得られたR−T−B系焼結磁石におけるHcJの差(条件Cを用いて得られたR−T−B系焼結磁石のHcJの値から条件Aを用いて得られたR−T−B系焼結磁石のHcJの値を引いたもの)である。In “Condition A” of Table 3, the sample No. The characteristic values of a sintered magnet obtained by finely pulverizing an alloy having a composition of 13 under condition A and sintering and heat-treating the finely pulverized powder obtained are shown. In “Condition C” of Table 3, the sample No. The characteristic values of a sintered magnet obtained by finely pulverizing an alloy having a composition of 13 under condition C and sintering and heat-treating the obtained finely pulverized powder are shown. “Condition C—Condition A” in Table 3 shows the improvement width (ΔH cJ ) of H cJ of the sintered magnet by changing the pulverization condition from Condition A to Condition C. That is, ΔH cJ in Table 3 is the difference in H cJ in the R-T-B system sintered magnet obtained by producing finely pulverized powder under condition A or condition C (R obtained using condition C). The value obtained by subtracting the value of HcJ of the RTB -based sintered magnet obtained using Condition A from the value of HcJ of the TB-based sintered magnet).

Figure 2017159576
Figure 2017159576

Figure 2017159576
Figure 2017159576

Figure 2017159576
Figure 2017159576

表2に示すように、試料No.1〜27のいずれの焼結磁石も、使用する微粉砕粉(合金粉末)の粒径D50及び粒径D99を本発明の実施形態の粒径(条件Bで作製した微粉砕粉)にすることにより、通常の粒径(条件Aで作製)の場合と比べて、Bの低下なしにHcJが向上(ΔHcJが0を超えている)している。しかし、本発明の実施形態の組成を満たしていない試料No.15〜26の比較例は、焼結磁石のHcJの向上幅(ΔHcJ)が36〜57kA/mと十分ではなかった。これ対し、本発明の実施形態の組成範囲(試料No.1〜14及び27)であると、ΔHcJが87〜101kA/mとなり、比較例の約1.5〜2.5倍と大幅に向上した。このように、本発明の実施形態の組成を満たすことにより、高いBと高いHcJが得られている。上述したように、条件A(通常の粒度)から条件B(本発明の実施形態の粒度)にすることにより、粉砕時間が10分から40分と長くなる。よって、本発明の実施形態の組成を満たしていない場合はHcJの向上幅が小さいため、本発明の実施形態の粒度で粉砕は行わない。しかし、本発明の実施形態の組成範囲であると大幅にHcJが向上するので、粉砕時間が長くなったとしても行う価値が十分にある。As shown in Table 2, sample no. Any of the sintered magnet 1-27, the finely pulverized powder used (finely pulverized powder produced in the condition B) The particle size of the embodiment of the present invention the particle size D 50 and particle size D 99 of the (alloy powder) by, as compared to a regular particle size (prepared under the conditions a), H cJ without loss of B r is improved ([Delta] H cJ is greater than 0). However, the sample No. which does not satisfy the composition of the embodiment of the present invention. In the comparative examples of 15 to 26 , the improvement width (ΔH cJ ) of H cJ of the sintered magnet was not sufficient at 36 to 57 kA / m. On the other hand, in the composition range of the embodiment of the present invention (sample Nos. 1 to 14 and 27), ΔH cJ is 87 to 101 kA / m, which is significantly about 1.5 to 2.5 times that of the comparative example. Improved. Thus, by satisfying the composition of an embodiment of the present invention, a high B r and high H cJ are achieved. As described above, when the condition A (normal particle size) is changed to the condition B (particle size of the embodiment of the present invention), the pulverization time is increased from 10 minutes to 40 minutes. Therefore, when the composition of the embodiment of the present invention is not satisfied, the improvement width of HcJ is small, so that the pulverization is not performed with the particle size of the embodiment of the present invention. However, since the HcJ is greatly improved within the composition range of the embodiment of the present invention, it is sufficiently worth even if the pulverization time is increased.

ここで、表1に示すB量と、表2および3に示した保磁力の向上幅ΔHcJとの関係を図1に示す。図1は、縦軸に本発明例及び比較例のΔHcJを、横軸にB量を示したものである。図1における四角のプロット(■)が本発明例であり、三角のプロット(▲)が比較例である。図1に示すように、B量が0.850〜0.910質量%と極めて狭い範囲において高いΔHcJが得られていることが分かる。また、B量が0.870〜0.910質量%の方がさらに高い(90kA/m以上)ΔHcJが得られている。Here, FIG. 1 shows the relationship between the B amount shown in Table 1 and the coercivity improvement width ΔH cJ shown in Tables 2 and 3. In FIG. 1, the vertical axis represents ΔH cJ of the inventive example and the comparative example, and the horizontal axis represents the B amount. A square plot (■) in FIG. 1 is an example of the present invention, and a triangular plot (▲) is a comparative example. As shown in FIG. 1, it can be seen that a high ΔH cJ is obtained in a very narrow range of B amount of 0.850 to 0.910 mass%. In addition, a higher B content (90 kA / m or more) ΔH cJ is obtained when the B content is 0.870 to 0.910 mass%.

また、表3に示すように、微粉砕粉(合金粉末)における粒径D50及び粒径D99が本発明の実施形態の好ましい範囲(3.8μm≦D50≦4.5μm及びD99≦9μm)であると、Bの低下なしにΔHcJが173kA/mと、さらに高いBと高いHcJが得られている。Moreover, as shown in Table 3, the particle size D 50 and the particle size D 99 in the finely pulverized powder (alloy powder) are preferably in the preferred embodiments of the present invention (3.8 μm ≦ D 50 ≦ 4.5 μm and D 99 ≦ If it is 9 .mu.m), without loss of B r is [Delta] H cJ and 173kA / m, even higher B r and high H cJ are achieved.

本出願は、出願日が2016年3月17日である日本国特許出願、特願第2016−054153号を基礎出願とする優先権主張を伴う。特願第2016−054153号は参照することにより本明細書に取り込まれる。   This application is accompanied by a priority claim based on a Japanese patent application filed on March 17, 2016, Japanese Patent Application No. 2006-054153. Japanese Patent Application No. 2006-054153 is incorporated herein by reference.

Claims (3)

R:28.5〜33.0質量%(Rは希土類元素のうち少なくとも1種であり、NdおよびPrの少なくとも1種を含む)、
B:0.850〜0.910質量%、
Ga:0.2〜0.7質量%、
Cu:0.05〜0.50質量%、
Al:0.05〜0.50質量%、を含有し、
残部がT(TはFeとCoであり、Tの90質量%以上がFeである)および不可避的不純物であり、下記式(1)を満足するR−T−B系焼結磁石の製造方法であって、

14[B]/10.8<[T]/55.85 (1)
([B]は質量%で示すBの含有量であり、[T]は質量%で示すTの含有量である)

粒径D50および粒径D99が下記式(2)および(3)を満足する合金粉末を準備する工程と、
3.8μm≦D50≦5.5μm (2)
99≦10μm (3)
前記合金粉末を成形して成形体を得る成形工程と、
前記成形体を焼結して焼結体を得る焼結工程と、
前記焼結体に熱処理を施す熱処理工程と、
を含む、R−T−B系焼結磁石の製造方法。
R: 28.5 to 33.0% by mass (R is at least one rare earth element and includes at least one of Nd and Pr),
B: 0.850-0.910 mass%,
Ga: 0.2-0.7 mass%,
Cu: 0.05 to 0.50 mass%,
Al: 0.05 to 0.50 mass%,
The balance is T (T is Fe and Co, 90% by mass or more of T is Fe) and inevitable impurities, and a method for producing an R-T-B system sintered magnet satisfying the following formula (1) Because

14 [B] /10.8 <[T] /55.85 (1)
([B] is the B content in mass%, and [T] is the T content in mass%)

Preparing an alloy powder having a particle size D 50 and a particle size D 99 satisfying the following formulas (2) and (3);
3.8 μm ≦ D 50 ≦ 5.5 μm (2)
D 99 ≦ 10 μm (3)
A molding step of molding the alloy powder to obtain a molded body;
Sintering step for obtaining a sintered body by sintering the molded body;
A heat treatment step for heat-treating the sintered body;
The manufacturing method of the RTB type | system | group sintered magnet containing this.
前記R−T−B系焼結磁石におけるBが0.870〜0.910質量%である、請求項1に記載のR−T−B系焼結磁石の製造方法。   The manufacturing method of the RTB system sintered magnet according to claim 1 whose B in said RTB system sintered magnet is 0.870-0.910 mass%. 前記粒径D50および粒径D99がさらに下記式(4)および(5)を満足する、請求項1又は2に記載のR−T−B系焼結磁石の製造方法。
3.8μm≦D50≦4.5μm (4)
99≦9μm (5)
Satisfies the particle diameter D 50 and particle size D 99 is further following formula (4) and (5) The method of manufacturing a R-T-B based sintered magnet according to claim 1 or 2.
3.8 μm ≦ D 50 ≦ 4.5 μm (4)
D 99 ≦ 9 μm (5)
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