JPH04314315A - Manufacture of bond magnet - Google Patents

Manufacture of bond magnet

Info

Publication number
JPH04314315A
JPH04314315A JP3105199A JP10519991A JPH04314315A JP H04314315 A JPH04314315 A JP H04314315A JP 3105199 A JP3105199 A JP 3105199A JP 10519991 A JP10519991 A JP 10519991A JP H04314315 A JPH04314315 A JP H04314315A
Authority
JP
Japan
Prior art keywords
semi
sintered
molded
permanent magnet
magnetic field
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.)
Granted
Application number
JP3105199A
Other languages
Japanese (ja)
Other versions
JP2963786B2 (en
Inventor
Haruhiro Yukimura
治洋 幸村
Takaaki Yasumura
隆明 安村
Yoshio Matsuo
良夫 松尾
Tomoyuki Hayashi
智幸 林
Teruo Kiyomiya
照夫 清宮
Kazuo Matsui
一雄 松井
Current Assignee (The listed assignees may be inaccurate. Google has not performed a legal analysis and makes no representation or warranty as to the accuracy of the list.)
FDK Corp
Original Assignee
FDK Corp
Priority date (The priority date is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the date listed.)
Filing date
Publication date
Application filed by FDK Corp filed Critical FDK Corp
Priority to JP3105199A priority Critical patent/JP2963786B2/en
Publication of JPH04314315A publication Critical patent/JPH04314315A/en
Application granted granted Critical
Publication of JP2963786B2 publication Critical patent/JP2963786B2/en
Anticipated expiration legal-status Critical
Expired - Fee Related legal-status Critical Current

Links

Classifications

    • HELECTRICITY
    • H01ELECTRIC ELEMENTS
    • H01FMAGNETS; INDUCTANCES; TRANSFORMERS; SELECTION OF MATERIALS FOR THEIR MAGNETIC PROPERTIES
    • H01F1/00Magnets or magnetic bodies characterised by the magnetic materials therefor; Selection of materials for their magnetic properties
    • H01F1/01Magnets or magnetic bodies characterised by the magnetic materials therefor; Selection of materials for their magnetic properties of inorganic materials
    • H01F1/03Magnets or magnetic bodies characterised by the magnetic materials therefor; Selection of materials for their magnetic properties of inorganic materials characterised by their coercivity
    • H01F1/032Magnets or magnetic bodies characterised by the magnetic materials therefor; Selection of materials for their magnetic properties of inorganic materials characterised by their coercivity of hard-magnetic materials
    • H01F1/04Magnets or magnetic bodies characterised by the magnetic materials therefor; Selection of materials for their magnetic properties of inorganic materials characterised by their coercivity of hard-magnetic materials metals or alloys
    • H01F1/047Alloys characterised by their composition
    • H01F1/053Alloys characterised by their composition containing rare earth metals
    • H01F1/055Alloys characterised by their composition containing rare earth metals and magnetic transition metals, e.g. SmCo5
    • H01F1/057Alloys characterised by their composition containing rare earth metals and magnetic transition metals, e.g. SmCo5 and IIIa elements, e.g. Nd2Fe14B
    • H01F1/0571Alloys characterised by their composition containing rare earth metals and magnetic transition metals, e.g. SmCo5 and IIIa elements, e.g. Nd2Fe14B in the form of particles, e.g. rapid quenched powders or ribbon flakes
    • H01F1/0575Alloys 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 pressed, sintered or bonded together
    • H01F1/0578Alloys 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 pressed, sintered or bonded together bonded together

Landscapes

  • Chemical & Material Sciences (AREA)
  • Crystallography & Structural Chemistry (AREA)
  • Inorganic Chemistry (AREA)
  • Engineering & Computer Science (AREA)
  • Power Engineering (AREA)
  • Manufacturing Cores, Coils, And Magnets (AREA)
  • Hard Magnetic Materials (AREA)

Abstract

PURPOSE:To provide a bond magnet which is made of baked type permanent magnet bulk which is cheap and excellent in magnetic characteristics. CONSTITUTION:A permanent magnet bulk consisting of partially baked alloy whose basic components are rare earth elements, iron and boron is molded by magnetic field applied molding and the resulting compact is impregnated with resin. Or, the same permanent magnet bulk is molded by after magnetic field applied molding and then thermally treated in an inert atmosphere, and the resulting compact is impregnated with resin. The partially baked alloy is thermally treated in a vacuum or inert atmosphere. The treatment is made at 700-1000 deg.C for 3 hours or less so that the density may be 60-95% of theoretical one.

Description

【発明の詳細な説明】[Detailed description of the invention]

【0001】0001

【産業上の利用分野】本発明は、希土類元素(R)、鉄
及びボロンを基本成分とする磁性材料を合成樹脂により
結合させたボンド磁石の製造方法に関し、特に、焼結型
のR−Fe−B系の永久磁石バルク体を原料として、高
い磁気特性を発揮するボンド磁石を製造する方法に関す
るものである。
[Industrial Application Field] The present invention relates to a method for manufacturing bonded magnets in which magnetic materials whose basic components are rare earth elements (R), iron, and boron are bonded together using synthetic resin, and in particular, sintered R-Fe. The present invention relates to a method of manufacturing a bonded magnet exhibiting high magnetic properties using a B-based permanent magnet bulk body as a raw material.

【0002】0002

【従来の技術】従来、希土類磁石として、R−Fe−B
系の永久磁石が開発されている。このR−Fe−B系磁
石には、焼結法と高速急冷型とがあり、現在のところ、
焼結型が低コストで高い磁気特性を有するものとして最
も優れているとされている。一方、ボンド磁石は、従来
、例えば、次ぎのような方法で製造されていた。
[Prior Art] Conventionally, as a rare earth magnet, R-Fe-B
permanent magnets have been developed. There are two types of R-Fe-B magnets: sintering method and high-speed quenching method.Currently,
The sintered type is said to be the most excellent as it is low cost and has high magnetic properties. On the other hand, bonded magnets have conventionally been manufactured, for example, by the following method.

【0003】上記の高速急冷型のR−Fe−B系永久磁
石バルク体を原料とし、これを粉砕し、粒径毎に分級す
る。分級された粉体に、この粉体の接着剤である合成樹
脂(例えば、エポキシ樹脂等)を添加混合し、均一に混
練する。混練物を磁場中で所定の形状に成型した後、得
られた成形体をキュア―する。
[0003] The above-mentioned high-speed quenching type R-Fe-B permanent magnet bulk body is used as a raw material, which is pulverized and classified according to particle size. A synthetic resin (such as an epoxy resin) as an adhesive for the powder is added to and mixed with the classified powder, and the mixture is uniformly kneaded. After the kneaded material is molded into a predetermined shape in a magnetic field, the obtained molded product is cured.

【0004】なお、上記の磁場中成型は、一般に、圧縮
成型法が採用され、成型体の密度を高めて、良好な磁気
特性を有するボンド磁石を製造している。このように、
従来のボンド磁石は、高速急冷型のR−Fe−B系永久
磁石バルク体を原料としており、これまで上記の焼結型
のR−Fe−B系永久磁石バルク体を原料としたボンド
磁石は知られていない。
[0004] In the above-mentioned magnetic field molding, a compression molding method is generally employed to increase the density of the molded body and produce a bonded magnet having good magnetic properties. in this way,
Conventional bonded magnets are made from high-speed quenched bulk R-Fe-B permanent magnets; unknown.

【0005】そこで、前述のように、焼結型のR−Fe
−B系永久磁石バルク体は、コストが低く、高い磁気特
性を有することから、これを原料としたボンド磁石の開
発が望まれているが、この種の磁石バルク体を原料とす
るボンド磁石の製造には、以下に説明する技術的課題が
あった。
Therefore, as mentioned above, sintered R-Fe
- B-based permanent magnet bulk bodies are low in cost and have high magnetic properties, so it is desired to develop bonded magnets using them as raw materials. The manufacturing had technical challenges as explained below.

【0006】[0006]

【発明が解決しようとする課題】すなわち、焼結型のも
のを原料とするボンド磁石の製造方法では、これを粉砕
すると、得られる粉体(粒子)には、粉砕による機械的
な歪みが発生し、また粒子粉砕面の化学的活性に起因す
る酸化が生じ、これら歪みや酸化の影響により、粒子の
磁気特性(保持力iHc)が激減する。このように磁気
特性の激減した粒子を使用して得られるボンド磁石は、
当然に磁気特性が充分でなく、本発明者等の実験によれ
ば、iHcが2KOe程度、最大エネルギ積(BH)m
ax が3MGOe程度でしかなく、実用性に欠けるも
のしか得られなかった。
[Problem to be Solved by the Invention] In other words, in a method for manufacturing a bonded magnet using a sintered type as a raw material, when the material is crushed, mechanical distortion occurs in the resulting powder (particles) due to the crushing. In addition, oxidation occurs due to chemical activity on the particle crushing surface, and the magnetic properties (coercive force iHc) of the particles are drastically reduced due to the effects of distortion and oxidation. Bonded magnets obtained using particles with drastically reduced magnetic properties are
Naturally, the magnetic properties are not sufficient, and according to the experiments of the present inventors, the iHc is about 2KOe, and the maximum energy product (BH) m
The ax was only about 3MGOe, which meant that it was not practical.

【0007】本発明は、以上の諸点に鑑みてなされたも
のであって、その目的とするところは、従来はボンド磁
石の原料とされていなかった焼結型のR−Fe−B系永
久磁石バルク体を原料として、簡素で低コスト、しかも
高磁気特性を有するボンド磁石を安定して製造する方法
を提供することにある。
The present invention has been made in view of the above points, and its purpose is to develop a sintered R-Fe-B permanent magnet, which has not been used as a raw material for bonded magnets in the past. It is an object of the present invention to provide a method for stably manufacturing bonded magnets that are simple, low cost, and have high magnetic properties using bulk materials as raw materials.

【0008】[0008]

【課題を解決するための手段】上記目的を達成するため
に、本発明は、希土類元素,鉄及びボロンを基本成分と
する半焼結合金からなる永久磁石バルク体を磁場中成型
し、得られた成型体に樹脂を含浸させることを特徴とす
る。
[Means for Solving the Problems] In order to achieve the above object, the present invention forms a permanent magnet bulk body made of a semi-sintered alloy whose basic components are rare earth elements, iron and boron in a magnetic field, and It is characterized by impregnating the molded body with resin.

【0009】また、第2の発明として、希土類元素,鉄
及びボロンを基本成分とする半焼結合金からなる永久磁
石バルク体を、磁場中成型した後、真空又は不活性雰囲
気中で熱処理し、次いで得られた熱処理成型体に樹脂を
含浸させることを特徴とする。上記半焼結合金は、真空
又は不活性雰囲気中で700〜1000℃の温度で3時
間以内の半焼結をおこない、その密度を理論密度の60
〜95%にすることが望ましい。上記真空又は不活性雰
囲気中での熱処理は、400〜1000℃の温度で3時
間以内とすることが望ましい。
In addition, as a second invention, a permanent magnet bulk body made of a semi-sintered alloy whose basic components are rare earth elements, iron and boron is molded in a magnetic field, then heat treated in a vacuum or an inert atmosphere, and then The method is characterized by impregnating the obtained heat-treated molded body with a resin. The above-mentioned semi-sintered alloy is semi-sintered at a temperature of 700 to 1000°C in a vacuum or an inert atmosphere for less than 3 hours, and its density is reduced to 60% of the theoretical density.
It is desirable to set it to ~95%. The heat treatment in vacuum or in an inert atmosphere is preferably performed at a temperature of 400 to 1000° C. for less than 3 hours.

【0010】0010

【作用】本発明は、前述のようにボンド磁石の磁気特性
が、原料となる焼結型R−Fe−B系永久磁石バルク体
粉末の酸化や機械的歪みの影響を大きく受けることに着
目したもので、この酸化や機械的歪みといった欠点を、
焼結温度を限定(以後、半焼結という)し、その半焼結
バルク体を所望形状の金型に入れ、粉砕と成型を兼ねる
形で磁場中成型することにより軽減し、必要に応じて熱
処理を行うことにより解消するものである。
[Operation] As mentioned above, the present invention focuses on the fact that the magnetic properties of bonded magnets are greatly affected by the oxidation and mechanical distortion of the sintered R-Fe-B permanent magnet bulk powder, which is the raw material. However, this defect such as oxidation and mechanical distortion can be eliminated by
This can be reduced by limiting the sintering temperature (hereinafter referred to as semi-sintering), placing the semi-sintered bulk body in a mold of the desired shape, and molding it in a magnetic field in a form that combines pulverization and molding, and heat treatment as necessary. It can be resolved by doing something like this.

【0011】従来の焼結体の組織と、本発明の半焼結体
の組織を比較した状態を図1に示す。同図により、本発
明では粒成長が抑制されていることがわかる。また、同
図に示すように、本発明のものは、空孔をかなり含んだ
組織であるため密度が低く、さらにその空孔は亀裂発展
さらには破壊の核となるため、小さな応力で容易に粉砕
できる。具体的には、従来の焼結体の抗折強度が2.5
ton /cm2 以上であるのに対し、本発明の半焼
結体は1ton /cm2 未満と非常に小さい。
FIG. 1 shows a comparison between the structure of a conventional sintered body and the structure of the semi-sintered body of the present invention. The figure shows that grain growth is suppressed in the present invention. In addition, as shown in the same figure, the structure of the present invention has a low density because it has a structure that contains a large number of pores, and since the pores become the core of crack development and even fracture, it can be easily processed by small stress. Can be crushed. Specifically, the bending strength of the conventional sintered body is 2.5
ton/cm2 or more, whereas the semi-sintered body of the present invention has a very small weight of less than 1 ton/cm2.

【0012】本発明は上記の利点を生かしたものである
。つまり、半焼結体を粉砕を行なわずにバルクの状態で
所望の形状の金型に入れ、粉砕と成型を兼ねる形で磁場
中成型を行なうものである。
The present invention takes advantage of the above advantages. That is, the semi-sintered body is put into a mold of a desired shape in a bulk state without being pulverized, and molding is performed in a magnetic field in a manner that combines pulverization and molding.

【0013】従来の技術では、粉砕、分級工程において
、機械的歪みや酸化の影響をうけやすく、磁気特性(特
にiHc)の劣化やばらつきが大きかった。しかし、本
発明ではそれらの影響を受けにくいため、磁気特性が高
く、ばらつきもすくない。上述のような利点を生かすと
、以下に示す低コスト化が可能である。半焼結により所
望の特性を満たしていれば、時効処理を省略できる。ま
た、半焼結体を磁場中成型後、所望の特性を満たしてい
れば、図2において熱処理を省略できる。さらに、熱処
理を省略せずに行なった場合には、非常に高特性なボン
ド磁石を得ることができる。また、粉砕、分級工程はな
いため大幅なコストダウンとなる。
[0013] In the conventional technology, the grinding and classification processes are easily affected by mechanical distortion and oxidation, and the magnetic properties (particularly iHc) deteriorate and vary greatly. However, the present invention is less susceptible to these influences, so the magnetic properties are high and there are few variations. By taking advantage of the advantages described above, it is possible to reduce costs as shown below. If the desired characteristics are satisfied by semi-sintering, aging treatment can be omitted. Further, if the semi-sintered body satisfies the desired characteristics after being molded in a magnetic field, the heat treatment in FIG. 2 can be omitted. Furthermore, if heat treatment is carried out without omitting it, a bonded magnet with extremely high characteristics can be obtained. In addition, there is no pulverization or classification process, resulting in significant cost reductions.

【0014】ここで本発明において、上記の作用をより
有効に発揮させる上で、上記の半焼結温度は700〜1
000℃(理論密度の60〜95%に相当する)で、特
に800〜950℃(理論密度の70〜85%に相当す
る)とするのが良い。すなわち、700℃より低温であ
ると半焼結体にiHcがほとんど発生せず上記のような
作用が生じない。1000℃より高温であると理論密度
の95%及び、抗折強度2ton /cm2 を越えて
しまい、機械的歪みが少ない、粒成長が抑制されるとい
った長所が失われるので700〜1000℃とした。
[0014] In the present invention, in order to more effectively exhibit the above-mentioned effects, the above-mentioned semi-sintering temperature is 700 to 1
000°C (corresponding to 60 to 95% of the theoretical density), particularly preferably 800 to 950°C (corresponding to 70 to 85% of the theoretical density). That is, if the temperature is lower than 700° C., almost no iHc is generated in the semi-sintered body, and the above-mentioned effect does not occur. If the temperature is higher than 1000°C, the theoretical density exceeds 95% and the bending strength exceeds 2 ton/cm2, and the advantages such as little mechanical distortion and suppressed grain growth are lost, so the temperature was set at 700 to 1000°C.

【0015】また、上記の半焼結の時間は、上記の半焼
結温度に応じて適宜選択されるが、結晶粒径の粗大化に
より磁気特性を劣化させるため、本発明では3時間以内
とすることが望ましい。なお、この場合、1時間より短
時間であると、半焼結の効果が不十分となることがある
ため半焼結時間の下限は1時間とすることが好ましい。
[0015] Further, the above-mentioned semi-sintering time is appropriately selected depending on the above-mentioned semi-sintering temperature, but in the present invention, it should be within 3 hours because the coarsening of the crystal grain size deteriorates the magnetic properties. is desirable. In this case, if the time is shorter than 1 hour, the effect of semi-sintering may be insufficient, so it is preferable that the lower limit of the semi-sintering time is 1 hour.

【0016】さらに、図2において熱処理温度は400
〜1000℃で、特に600〜800℃とするのが良い
。すなわち400℃より低温であると、粒子間及び結晶
粒界面での原子拡散が不十分でiHc向上の効果が得ら
れない。一方、1000℃より高温であると、結晶粒径
が粗大化したり、酸化が生じて、磁気特性がかえって劣
化するばかりでなく成型体の形状変化が生じる等の不都
合が生じる。
Furthermore, in FIG. 2, the heat treatment temperature is 400
The temperature is preferably 600 to 800°C, particularly 600 to 800°C. That is, if the temperature is lower than 400° C., atomic diffusion between particles and at crystal grain interfaces is insufficient, and the effect of improving iHc cannot be obtained. On the other hand, if the temperature is higher than 1000° C., the crystal grain size becomes coarse and oxidation occurs, which not only deteriorates the magnetic properties but also causes problems such as changes in the shape of the molded product.

【0017】また、熱処理の時間は、上記熱処理温度に
応じて適宜選択されるが、3時間を超えると、結晶粒径
の粗大化及び酸化により磁気特性を劣化させるため、本
発明では3時間以内とするののが望ましい。なお、1時
間より短時間であると、粒子間及び結晶粒界面の原子拡
散が不十分となることがあるため熱処理時間の下限は1
時間とすることが好ましい。さらにまた、上記の半焼結
及び熱処理を真空または不活性雰囲気中で行えば、酸化
が熱により促進されれず、この酸化を防止するために有
効である。
Further, the heat treatment time is appropriately selected depending on the above heat treatment temperature, but if it exceeds 3 hours, the magnetic properties will deteriorate due to coarsening of crystal grain size and oxidation, so in the present invention, the time is within 3 hours. It is desirable to do so. Note that if the heat treatment time is shorter than 1 hour, atomic diffusion between particles and at grain interfaces may become insufficient, so the lower limit of the heat treatment time is 1 hour.
It is preferable to set it as time. Furthermore, if the above-mentioned semi-sintering and heat treatment are performed in a vacuum or an inert atmosphere, oxidation is not promoted by heat and is effective for preventing this oxidation.

【0018】以上の作用を発現させるための原料である
焼結型R−Fe−B系永久磁石バルク体として、本発明
では、R(Rは、Nd,Pr,Dy,Ho,Tbのうち
少なくとも1種又は更にLa,Ce,Sm,Gd,Er
,Eu,Tm,Yb,Lu,Yのうち少なくとも1種か
らなる)8〜30原子%、B2〜28原子%、Fe42
〜90原子%の組成からなりものが好ましく使用される
。更に、キュ―リ―点の向上等を目的として、Feに対
してCoを50%まで置換しても良い。
In the present invention, as a sintered R-Fe-B permanent magnet bulk body which is a raw material for exhibiting the above effects, R (R is at least one of Nd, Pr, Dy, Ho, and Tb) is used. One or more La, Ce, Sm, Gd, Er
, Eu, Tm, Yb, Lu, Y) 8 to 30 at%, B2 to 28 at%, Fe42
Those having a composition of 90 atomic % are preferably used. Furthermore, for the purpose of improving the Curie point, etc., up to 50% of Co may be substituted for Fe.

【0019】[0019]

【実施例】*ボンド磁石用バルク体の製造組成式Nd1
6Fe78B6 及びNd18Fe76B6 で表わさ
れるNd−Fe−B系合金をジェットミルにより粉砕し
、平均粒径3μmの微粉体とし、この微粉体を磁場中成
型後、表1に示す条件により半焼結、時効処理を施した
[Example] *Production of bulk body for bonded magnet Composition formula Nd1
Nd-Fe-B alloys represented by 6Fe78B6 and Nd18Fe76B6 were ground using a jet mill to form fine powder with an average particle size of 3 μm. After molding this fine powder in a magnetic field, it was semi-sintered and aged under the conditions shown in Table 1. provided.

【0020】得られたバルク体のそれぞれの条件での磁
気特性を表2に示す。また、比較例として、同組成にて
通常の焼結、時効処理を施したものもあわせて示す。 (なお、平均粒径とは、得られたバルク体を鏡面研磨し
金属顕微鏡にて測定したものである。)表2より、半焼
結合金では粒成長が抑制され、iHcが大きいことがわ
かる。
Table 2 shows the magnetic properties of the obtained bulk body under each condition. In addition, as a comparative example, a sample having the same composition but subjected to normal sintering and aging treatment is also shown. (Note that the average grain size is the value measured by mirror polishing the obtained bulk body and using a metallurgical microscope.) From Table 2, it can be seen that grain growth is suppressed and iHc is large in the semi-sintered alloy.

【0021】[0021]

【0022】[0022]

【0023】*半焼結温度範囲の確認 組成Nd18Fe76B6 (半焼結条件800℃×2
h,時効条件600℃×1h)について、半焼結温度を
種々変えた以外は上記バルク体の製造方法とまったく同
様にして複数の半焼結体試料を作製し、得られた半焼結
体の諸特性を測定した。この結果を図3に示す。
* Confirmation of semi-sintering temperature range Composition Nd18Fe76B6 (semi-sintering condition 800°C x 2
h, aging conditions (600°C x 1 h), a plurality of semi-sintered samples were produced in exactly the same manner as the bulk body manufacturing method described above, except that the semi-sintering temperature was variously changed, and various properties of the obtained semi-sintered bodies were determined. was measured. The results are shown in FIG.

【0024】同図により、iHcは半焼結温度に依存し
ており、700℃より低温ではiHcはほとんど発現せ
ず、700℃以上で十分なiHcが得られる。1000
℃を超えると、理論密度の95%を越えてしまい、半焼
結合金の利点(機械的歪みが少ない等)が失われる。以
上により半焼結温度は700〜1000℃、好ましくは
800〜950℃であることがわかる。
[0024] The figure shows that iHc depends on the semi-sintering temperature, iHc hardly appears at temperatures lower than 700°C, and sufficient iHc is obtained at temperatures above 700°C. 1000
When the temperature exceeds 95% of the theoretical density, the advantages of semi-sintered alloys (low mechanical strain, etc.) are lost. From the above, it can be seen that the semi-sintering temperature is 700 to 1000°C, preferably 800 to 950°C.

【0025】*半焼結時間の確認 組成Nd18Fe76B6 (半焼結条件800℃×2
h,時効条件600℃×1h)について、半焼結時間を
種々変えた以外は上記バルク体の製造方法とまったく同
様にして複数の半焼結体試料を作製し、得られた半焼結
体の磁気特性を測定した。
*Confirmation of semi-sintering time Composition Nd18Fe76B6 (semi-sintering condition 800°C x 2
h, aging conditions (600°C x 1 h), a plurality of semi-sintered samples were produced in exactly the same manner as the bulk body manufacturing method described above, except that the semi-sintering time was varied, and the magnetic properties of the obtained semi-sintered bodies were was measured.

【0026】この結果を図4に示す。同図から明らかな
ように、3時間より長時間であるとiHcの低下が見ら
れ、また1時間より短時間であるとやはりiHcの低下
が見られる。
The results are shown in FIG. As is clear from the figure, when the time is longer than 3 hours, a decrease in iHc is observed, and when the time is shorter than 1 hour, a decrease in iHc is also observed.

【0027】*実施例1 上記表1で得られた各バルク体を15KOeの磁場中で
配向させながら3ton/cm 2で圧縮成型し、この
成型体を粘度10cps のエポキシ樹脂中に浸漬し、
デシケ―タに移し、約3分間真空状態とし、成型体中に
エポキシ樹脂を十分含浸させた。次いで100℃、60
分間のアフタ―キュア―を行い試料を作製した(図2の
うち熱処理を省いた製造方法)。
*Example 1 Each bulk body obtained in Table 1 above was compression molded at 3 tons/cm 2 while being oriented in a magnetic field of 15 KOe, and this molded body was immersed in an epoxy resin with a viscosity of 10 cps.
The molded product was transferred to a desiccator and kept in a vacuum state for about 3 minutes to sufficiently impregnate the epoxy resin into the molded product. Then 100℃, 60℃
A sample was prepared by performing an after-cure for 1 minute (manufacturing method in which heat treatment was omitted in Figure 2).

【0028】得られたボンド磁石の磁気特性を表3に示
す。表3より半焼結バルク体という機械的強度の小さい
ものにのみ成型が可能であって、比較例はいずれも成型
できなかった。また、磁気特性についても、成型時のi
Hcの劣化が小さいため十分実用可能であることがわか
る。
Table 3 shows the magnetic properties of the bonded magnet obtained. From Table 3, it is possible to mold only semi-sintered bulk bodies with low mechanical strength, and none of the comparative examples could be molded. In addition, regarding magnetic properties, i
It can be seen that since the deterioration of Hc is small, it is sufficiently practical.

【0029】[0029]

【0030】*角型性:0.9BrのときのHc/iH
c *比較例A,比較例Bともに成型不可能
*Squareness: Hc/iH at 0.9Br
c *Both Comparative Example A and Comparative Example B cannot be molded.

【0031】*
実施例2 上記表1で得られた各バルク体を15KOeの磁場中で
配向させながら3ton/cm 2で圧縮成型し、この
成型体を1×10−6Torrの真空中、700℃1時
間で熱処理した。この成型体を粘度10cps のエポ
キシ樹脂中に浸漬し、デシケ―タに移し、約3分間真空
状態とし、成型体中にエポキシ樹脂を十分含浸させた。 次いで100℃、60分間のアフタ―キュア―を行った
。以上のようにして試料を作製した(図2参照)。
[0031]*
Example 2 Each bulk body obtained in Table 1 above was compression molded at 3 ton/cm 2 while oriented in a magnetic field of 15 KOe, and the molded body was heat treated at 700°C for 1 hour in a vacuum of 1 x 10 -6 Torr. did. This molded body was immersed in an epoxy resin having a viscosity of 10 cps, transferred to a desiccator, and kept under vacuum for about 3 minutes to sufficiently impregnate the epoxy resin into the molded body. Next, after-cure was performed at 100°C for 60 minutes. A sample was prepared as described above (see FIG. 2).

【0032】比較のため、同組成の焼結バルク体をジョ
―クラッシャ―により粉砕し、分級して125〜300
μmの合金粉体とし、この分級粉体を15KOeの磁場
中で配向させながら3ton /cm 2で圧縮成型し
、この成型体を上述の手法にてボンド化して試料を作製
した。
For comparison, a sintered bulk body of the same composition was crushed with a jaw crusher and classified to have a particle size of 125 to 300.
The classified powder was compression molded at 3 ton/cm 2 while being oriented in a magnetic field of 15 KOe, and the molded body was bonded using the method described above to prepare a sample.

【0033】各試料の磁気特性を表4に示す。表4より
本発明である半焼結−成型−熱処理の操作により、非常
に高特性なボンド磁石が得られることがわかる。
Table 4 shows the magnetic properties of each sample. Table 4 shows that bonded magnets with very high characteristics can be obtained by the semi-sintering-molding-heat treatment operation of the present invention.

【0034】[0034]

【0035】*角型性:0.9BrのときのHc/iH
c *比較例A:■,■と同組成 *比較例B:■,■と同組成
*Squareness: Hc/iH at 0.9Br
c * Comparative example A: Same composition as ■, ■ * Comparative example B: Same composition as ■, ■

【0036】*実施例3 組成Nd18Fe76B6 (半焼結条件800℃×2
h,時効条件600℃×1h)について、半焼結温度を
種々変えた以外は実施例2とまったく同様にして本発明
に係る製造方法を実施し、得られたボンド磁石の磁気特
性を測定した。
*Example 3 Composition Nd18Fe76B6 (semi-sintering condition 800°C x 2
The manufacturing method according to the present invention was carried out in exactly the same manner as in Example 2, except that the semi-sintering temperature was variously changed, and the magnetic properties of the obtained bonded magnets were measured.

【0037】この結果を図5に示す。同図から明らかな
ように、磁気特性は熱処理温度にかなり依存しており、
400℃以上でその効果が現れる。また、温度が上がる
にしたがい、iHc,(BH)max ともに増加して
いき、700℃で(BH)max が最高になり、10
00℃を超えると激減する。iHcは、1000℃まで
増加していき、1000℃を超えると激減する(iHc
と(BH)max のピ―ク位置の違いは角型性が若干
違うからである。)。
The results are shown in FIG. As is clear from the figure, the magnetic properties are highly dependent on the heat treatment temperature.
The effect appears at temperatures above 400°C. Also, as the temperature rises, both iHc and (BH)max increase, and (BH)max reaches its maximum at 700°C, reaching 10
It decreases sharply when the temperature exceeds 00℃. iHc increases up to 1000°C and decreases sharply when it exceeds 1000°C (iHc
The difference in peak position between and (BH)max is due to a slight difference in squareness. ).

【0038】以上により熱処理効果は400〜1000
℃、好ましくは600〜800℃であることがわかる。
[0038] As a result of the above, the heat treatment effect is 400 to 1000
℃, preferably 600 to 800℃.

【0039】*実施例4 組成Nd18Fe76B6 (半焼結条件800℃×2
h,時効条件600℃×1h)について、熱処理時間を
種々変えた以外は実施例3とまったく同様にして本発明
に係る方法を実施し、得られたボンド磁石の磁気特性を
測定した。
*Example 4 Composition Nd18Fe76B6 (semi-sintering condition 800°C x 2
The method according to the present invention was carried out in exactly the same manner as in Example 3, except that the heat treatment time was varied under the aging conditions (600° C. x 1 h), and the magnetic properties of the obtained bonded magnets were measured.

【0040】この結果を図6に示す。同図から明らかな
ように、3時間より長時間であると磁気特性の低下が見
られ、また1時間より短時間であるとやはり磁気特性の
低下が見られる。
The results are shown in FIG. As is clear from the figure, when the time is longer than 3 hours, the magnetic properties are degraded, and when the time is shorter than 1 hour, the magnetic properties are also degraded.

【0041】[0041]

【発明の効果】以上詳述した本発明に係る方法によれば
、ボンド磁石の原料であるバルク体に関し、半焼結状態
で大きなiHcを得ることが可能なので、ここで所望の
iHcを満たしていれば時効処理の省略が可能である。 また、ボンド磁石作製に関して、粉砕後もiHcの劣化
が小さいため、ここで所望特性を満たしていれば熱処理
の省略が可能である。さらに、粉砕、分級工程は省かれ
る。よって、これらにより良好な磁気特性を有するボン
ド磁石を低コストで提供することができる。
[Effects of the Invention] According to the method according to the present invention described in detail above, it is possible to obtain a large iHc in a semi-sintered state with respect to the bulk body, which is a raw material of a bonded magnet, so that the desired iHc can be satisfied. For example, the aging process can be omitted. Furthermore, regarding the production of bonded magnets, since the deterioration of iHc is small even after pulverization, heat treatment can be omitted if the desired characteristics are satisfied. Furthermore, the grinding and classification steps are omitted. Therefore, a bonded magnet having good magnetic properties can be provided at low cost.

【0042】また、時効処理、熱処理を省かずに行なっ
た場合、現状技術では達し得ない非常に高性能な磁石を
作製することができる。
[0042] Furthermore, if the aging treatment and heat treatment are not omitted, it is possible to produce a magnet with extremely high performance that cannot be achieved with the current technology.

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

【図1】従来及び本発明の製造方法で用いるバルク体の
表面拡大模式説明図である。
FIG. 1 is an enlarged schematic explanatory view of the surface of a bulk body used in the conventional manufacturing method and the manufacturing method of the present invention.

【図2】本発明の製造方法の工程を順に示すブロック図
である。
FIG. 2 is a block diagram sequentially showing the steps of the manufacturing method of the present invention.

【図3】焼結温度とiHcおよび密度との関係を示すグ
ラフである。
FIG. 3 is a graph showing the relationship between sintering temperature, iHc, and density.

【図4】焼結時間とiHcとの関係を示すグラフである
FIG. 4 is a graph showing the relationship between sintering time and iHc.

【図5】熱処理温度とiHcとの関係を示すグラフであ
る。
FIG. 5 is a graph showing the relationship between heat treatment temperature and iHc.

【図6】熱処理時間と(BH)max との関係を示す
グラフである。
FIG. 6 is a graph showing the relationship between heat treatment time and (BH)max.

Claims (4)

【特許請求の範囲】[Claims] 【請求項1】  希土類元素,鉄及びボロンを基本成分
とする半焼結合金からなる永久磁石バルク体を磁場中成
型し、得られた成型体に樹脂を含浸させることを特徴と
するボンド磁石の製造方法。
[Claim 1] Production of a bonded magnet characterized by molding a permanent magnet bulk body made of a semi-sintered alloy whose basic components are rare earth elements, iron, and boron in a magnetic field, and impregnating the obtained molded body with a resin. Method.
【請求項2】  希土類元素,鉄及びボロンを基本成分
とする半焼結合金からなる永久磁石バルク体を、磁場中
成型した後、真空又は不活性雰囲気中で熱処理し、次い
で得られた熱処理成型体に樹脂を含浸させることを特徴
とするボンド磁石の製造方法。
[Claim 2] A permanent magnet bulk body made of a semi-sintered alloy whose basic components are rare earth elements, iron, and boron is molded in a magnetic field, and then heat treated in a vacuum or inert atmosphere, and then the resulting heat-treated molded product A method for manufacturing a bonded magnet, which comprises impregnating a bonded magnet with a resin.
【請求項3】  上記半焼結合金は、真空又は不活性雰
囲気中で700〜1000℃の温度で3時間以内の半焼
結をおこない、その密度を理論密度の60〜95%にす
ることを特徴とする請求項1,2記載のボンド磁石の製
造方法。
3. The semi-sintered alloy is semi-sintered in a vacuum or an inert atmosphere at a temperature of 700 to 1000°C for up to 3 hours, and the density thereof is made to be 60 to 95% of the theoretical density. The method for manufacturing a bonded magnet according to claim 1 or 2.
【請求項4】  上記真空又は不活性雰囲気中での熱処
理は、400〜1000℃の温度で3時間以内とするこ
とを特徴とする請求項2記載のボンド磁石の製造方法。
4. The method of manufacturing a bonded magnet according to claim 2, wherein the heat treatment in vacuum or an inert atmosphere is carried out at a temperature of 400 to 1000° C. for less than 3 hours.
JP3105199A 1991-04-11 1991-04-11 Manufacturing method of bonded magnet Expired - Fee Related JP2963786B2 (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP3105199A JP2963786B2 (en) 1991-04-11 1991-04-11 Manufacturing method of bonded magnet

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP3105199A JP2963786B2 (en) 1991-04-11 1991-04-11 Manufacturing method of bonded magnet

Publications (2)

Publication Number Publication Date
JPH04314315A true JPH04314315A (en) 1992-11-05
JP2963786B2 JP2963786B2 (en) 1999-10-18

Family

ID=14401000

Family Applications (1)

Application Number Title Priority Date Filing Date
JP3105199A Expired - Fee Related JP2963786B2 (en) 1991-04-11 1991-04-11 Manufacturing method of bonded magnet

Country Status (1)

Country Link
JP (1) JP2963786B2 (en)

Cited By (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JP2014116589A (en) * 2012-12-11 2014-06-26 Samsung Electro-Mechanics Co Ltd Electronic component and method of manufacturing the same

Cited By (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JP2014116589A (en) * 2012-12-11 2014-06-26 Samsung Electro-Mechanics Co Ltd Electronic component and method of manufacturing the same

Also Published As

Publication number Publication date
JP2963786B2 (en) 1999-10-18

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