JPH0137462B2 - - Google Patents

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Publication number
JPH0137462B2
JPH0137462B2 JP55094355A JP9435580A JPH0137462B2 JP H0137462 B2 JPH0137462 B2 JP H0137462B2 JP 55094355 A JP55094355 A JP 55094355A JP 9435580 A JP9435580 A JP 9435580A JP H0137462 B2 JPH0137462 B2 JP H0137462B2
Authority
JP
Japan
Prior art keywords
alloy
crystal structure
mold
shows
cast
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.)
Expired
Application number
JP55094355A
Other languages
Japanese (ja)
Other versions
JPS5719345A (en
Inventor
Masahiro Takehana
Itaru Okonogi
Tatsuya Shimoda
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.)
Seiko Epson Corp
Original Assignee
Seiko Epson 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 Seiko Epson Corp filed Critical Seiko Epson Corp
Priority to JP9435580A priority Critical patent/JPS5719345A/en
Publication of JPS5719345A publication Critical patent/JPS5719345A/en
Publication of JPH0137462B2 publication Critical patent/JPH0137462B2/ja
Granted legal-status Critical Current

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  • Hard Magnetic Materials (AREA)
  • Powder Metallurgy (AREA)

Description

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

本発明は、Sm2Co17型結晶を主体とする希土類
コバルト永久磁石合金の製造方法に関するもので
ある。 例を樹脂結合型希土類コバルト磁石にとつて説
明する。この磁石は、第1図に示すような製造方
法、すなわち合金を溶解、鋳造し、容体化処理及
び時効処理によつて磁気的に硬化させた後、粉砕
して粉末にし、その後バインダーを混合、被覆し
て成形するか、成形後バインダーを含浸するとい
う2種類の製造方法により磁石化される。 この磁石の磁気性能は、合金組成、熱処理、粉末
の粒度ならびに粉末の形状、バインダーの種類、
磁場中プレス時の磁場の強さおよびプレス圧、そ
れから成形法により左右されることが以前から知
られていた。今回は新たに、鋳造インゴツトのマ
クロ組織により、磁石の磁気性能が大きく変化す
ることを発見した。 一般に溶融金属が、るつぼから鋳型に鋳込まれ
た時、金属融液は最初、鋳型壁と接触して、おび
ただしい核生成が起る程度まで急冷されチル晶組
織を生じる。その次には、鋳型へ熱が流れるた
め、鋳型壁と垂直に内部へ向つて柱状晶組織が伸
びてくる。しだいに熱の流れがなくなると、柱状
晶組織に変り等軸晶組織が現われ、鋳型内での凝
固は完了する。 鋳込まれた磁性合金を用い上述の三種類の組織
について、種々の実験をしてみたところ、柱状晶
組織を有するものが最も磁気的にすぐれているこ
とを見い出した。これらの実験は、Sm−Co−Cu
−Fe−Nbの5元系の組成の合金で行つた。この
とき柱状晶組織の効果が顕徴に現われたのは、
Smの含有量が21〜28wt%のSm2Co17型の結晶構
造を有する組成であつた。 実施例 1 第1表の合金1の組成を有する合金を高周波溶
The present invention relates to a method for producing a rare earth cobalt permanent magnet alloy mainly composed of Sm 2 Co 17 type crystals. An example will be explained using a resin bonded rare earth cobalt magnet. This magnet is produced by the manufacturing method shown in Figure 1, in which the alloy is melted and cast, hardened magnetically through container treatment and aging treatment, and then crushed into powder, after which a binder is mixed, Magnetization can be achieved by two methods: coating and molding or impregnation with a binder after molding. The magnetic performance of this magnet depends on the alloy composition, heat treatment, powder particle size and shape, binder type,
It has long been known that pressing in a magnetic field is affected by the strength of the magnetic field, the pressing pressure, and the molding method. This time, we newly discovered that the magnetic performance of a magnet changes significantly depending on the macrostructure of the cast ingot. Generally, when molten metal is poured into a mold from a crucible, the metal melt first contacts the walls of the mold and is rapidly cooled to the extent that extensive nucleation occurs, creating a chilled crystalline structure. Next, as heat flows into the mold, the columnar crystal structure extends inward perpendicular to the mold wall. When the heat flow gradually stops, the crystal structure changes to a columnar crystal structure and an equiaxed crystal structure appears, and solidification in the mold is completed. When we conducted various experiments on the three types of structures mentioned above using cast magnetic alloys, we found that the one with a columnar crystal structure was the most magnetically superior. These experiments were carried out using Sm−Co−Cu
An alloy with a five-element composition of -Fe-Nb was used. At this time, the effect of the columnar crystal structure became evident.
The composition had a Sm 2 Co 17 type crystal structure with an Sm content of 21 to 28 wt%. Example 1 An alloy having the composition of Alloy 1 in Table 1 was subjected to induction welding.

【表】 解炉を用いて、1Kgをアルミナるつぼ中で溶解し
肉厚10mmの第2図に示すような鉄製の金型に、
1500℃の温度で鋳込んだ。その時、第3図に示す
ような、組織の形態を取つた。第3図はインゴツ
トを中心で切断したときの組織を示す。これらの
部分のうちで、チル晶組織をA、柱状晶組織をB
そして等軸晶組織をCとする。本実施例では合金
1の鋳造塊のA,B,Cからそれぞれインゴツト
を切り出し、それを1140〜1180℃の間の最適な温
度で溶体化処理を行い、続いて800℃で時効処理
をし、磁気硬化させた。それを、砕いて粉末にし
た後、有機バインダーと混練した。その混練した
混合物を磁場中でプレス成形し、成形体の中の樹
脂を適度な熱を加えて硬化させ(キユア処理)
で、磁石を完成させた。磁気性能と合金の組織と
の関係との関係を第4図と第5図に示す。第4図
は、保持力iHcと800℃における時効時間との関
係を示し、図中のA,B,Cの記号はそれぞれチ
ル晶組織、柱状晶組織、等軸晶組織の部分を示
す。第5図は、飽和磁化Msと時効時間の関係を
示す。第4図、第5図から分るように柱状晶組織
の部分が他の部分よりも高い磁気性能が得られ
た。 実施例 2 第1表に示される合金2,3を実施例1と同じ
方法で溶解し、第6図に示す鉄製の鋳型に1500℃
の温度で鋳込んだ。第6図のbは、鋳型を水冷で
きるように外側に銅パイプをまいてある。第6図
aは空冷の鋳型である。両鋳型は水冷装置を除け
ば、大きさも形も材質も同じものである。また合
金2,3を実施例1と同じ方法で溶解し、るつぼ
中でそのまま除冷されたインゴツトも得た。これ
ら3種類の冷却速度の異つたインゴツトの組織を
観察すると、合金1,3ともに水冷のものは殆ん
ど全体がチル晶で、空冷のものは90vol%以上が
柱状晶で、るつぼ内除冷のものは粗大化した等軸
晶であつた。合金1,3について、それぞれ3種
のインゴツトを1140〜1180℃の間で最適の条件で
溶体化処理し、続いて800℃で2時間、加えて700
℃で時4時間時効処理した。そして、実施例1と
同様な方法で樹脂結合磁石を製造した。その結果
を第2表と第3表に示す。第2表は合金2につい
て、第3表は合金3についての結果である。
[Table] Using a melting furnace, 1 kg was melted in an alumina crucible and placed in an iron mold with a wall thickness of 10 mm as shown in Figure 2.
It was cast at a temperature of 1500℃. At that time, it took the form of an organization shown in Figure 3. FIG. 3 shows the structure when the ingot is cut at the center. Among these parts, the chill crystal structure is called A, and the columnar crystal structure is called B.
And let C be the equiaxed crystal structure. In this example, ingots were cut from cast ingots A, B, and C of Alloy 1, and they were solution-treated at an optimal temperature between 1140 and 1180°C, and then aged at 800°C. Magnetically hardened. It was crushed into powder and then kneaded with an organic binder. The kneaded mixture is press-molded in a magnetic field, and the resin in the molded body is cured by applying appropriate heat (cure treatment).
So, I completed the magnet. The relationship between the magnetic performance and the structure of the alloy is shown in FIGS. 4 and 5. FIG. 4 shows the relationship between the coercive force iHc and the aging time at 800°C, and the symbols A, B, and C in the figure indicate the chill crystal structure, columnar crystal structure, and equiaxed crystal structure, respectively. FIG. 5 shows the relationship between saturation magnetization Ms and aging time. As can be seen from FIGS. 4 and 5, higher magnetic performance was obtained in the columnar crystal structure area than in other areas. Example 2 Alloys 2 and 3 shown in Table 1 were melted in the same manner as in Example 1, and heated to 1500°C in the iron mold shown in Figure 6.
It was cast at a temperature of In Figure 6b, copper pipes are placed on the outside so that the mold can be cooled with water. Figure 6a shows an air-cooled mold. Both molds are the same size, shape, and material, except for the water cooling system. In addition, alloys 2 and 3 were melted in the same manner as in Example 1, and an ingot was obtained which was left to cool slowly in a crucible. Observing the structures of these three types of ingots with different cooling rates, we find that for both Alloys 1 and 3, the water-cooled ones are almost entirely chilled crystals, while the air-cooled ones are made up of columnar crystals at over 90 vol%. The crystals were coarse equiaxed crystals. For Alloys 1 and 3, three types of ingots were solution-treated at optimal conditions between 1140 and 1180°C, followed by 2 hours at 800°C and an additional 700°C.
It was aged at ℃ for 4 hours. Then, a resin-bonded magnet was manufactured in the same manner as in Example 1. The results are shown in Tables 2 and 3. Table 2 shows the results for Alloy 2, and Table 3 shows the results for Alloy 3.

【表】【table】

【表】 第2表、第3表より分るように、合金1も3も
柱状晶のできている空冷型のインゴツトが最も磁
気性能がすぐれているということができる。 以上説明してきたように、柱状晶組織を利用す
ることにより、Sm2Co17型の磁石の磁気性能を従
来より高めることができ、安価で高性能な磁石の
製造が可能になつた。
[Table] As can be seen from Tables 2 and 3, it can be said that for Alloys 1 and 3, the air-cooled ingots made of columnar crystals have the best magnetic performance. As explained above, by utilizing the columnar crystal structure, the magnetic performance of Sm 2 Co 17 type magnets can be improved compared to conventional magnets, making it possible to manufacture inexpensive and high-performance magnets.

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

第1図は、樹脂結合型磁石の製造工程を示す。
第2図は、鉄製の丸型の鋳型を示す。肉厚は全て
10mmである。長さの単位はmmである。第3図は、
第2図で示された鋳型に鋳込んだインゴツトの中
心を縦方向に切断したときの断面である。A,B
そしてCは、それぞれチル晶、柱状晶そして等軸
晶の各組織を示す。Dは金型の断面である。第4
図は、チル晶A、柱状晶B、等軸晶Cのインゴツ
トから得た磁石の磁気性能で時効時間と保磁力
(iHc)の関係を示す。第5図は、第4図と同様
の磁石における時効時間と飽和磁化(Ms)との
関係を示す。第6図は、角型の鉄鋳型を示す。A
は鉄、Bは水冷の銅パイプである。図中の単位は
全てmmである。
FIG. 1 shows the manufacturing process of a resin-bonded magnet.
Figure 2 shows a round iron mold. Thickness is everything
It is 10mm. The unit of length is mm. Figure 3 shows
This is a cross section taken in the longitudinal direction through the center of the ingot cast into the mold shown in FIG. 2. A, B
And C indicates each structure of chill crystal, columnar crystal, and equiaxed crystal. D is a cross section of the mold. Fourth
The figure shows the relationship between aging time and coercive force (iHc) in the magnetic performance of magnets obtained from ingots of chill crystal A, columnar crystal B, and equiaxed crystal C. FIG. 5 shows the relationship between aging time and saturation magnetization (Ms) in a magnet similar to that in FIG. 4. Figure 6 shows a square iron mold. A
is iron, and B is water-cooled copper pipe. All units in the figure are mm.

Claims (1)

【特許請求の範囲】[Claims] 1 Sm2Co17型結晶を主体とする合金を溶解、鋳
造し、粉砕して粉末にした後バインダーを混合、
被覆もしくは含浸して成形する希土類コバルト永
久磁石合金の製造方法において、前記合金として
サマリウム(Sm)、コバルト(Co)、銅(Cu)、
鉄(Fe)およびニオブ(Nb)からなり、Smの
含有量が重量比で21〜28%の範囲にあり、かつマ
クロ組織が柱状晶組織である合金を使用したこと
を特徴とする希土類コバルト永久磁石合金の製造
方法。
1 An alloy mainly composed of Sm 2 Co 17 type crystals is melted, cast, crushed into powder, and then mixed with a binder.
In the method for producing a rare earth cobalt permanent magnet alloy by coating or impregnating and forming, the alloy includes samarium (Sm), cobalt (Co), copper (Cu),
A rare earth cobalt permanent alloy consisting of iron (Fe) and niobium (Nb), with an Sm content in the range of 21 to 28% by weight, and a macrostructure having a columnar crystal structure. Method of manufacturing magnetic alloy.
JP9435580A 1980-07-10 1980-07-10 Manufacture of permanent magnet alloy of rare earth element and cobalt Granted JPS5719345A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP9435580A JPS5719345A (en) 1980-07-10 1980-07-10 Manufacture of permanent magnet alloy of rare earth element and cobalt

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP9435580A JPS5719345A (en) 1980-07-10 1980-07-10 Manufacture of permanent magnet alloy of rare earth element and cobalt

Publications (2)

Publication Number Publication Date
JPS5719345A JPS5719345A (en) 1982-02-01
JPH0137462B2 true JPH0137462B2 (en) 1989-08-07

Family

ID=14107974

Family Applications (1)

Application Number Title Priority Date Filing Date
JP9435580A Granted JPS5719345A (en) 1980-07-10 1980-07-10 Manufacture of permanent magnet alloy of rare earth element and cobalt

Country Status (1)

Country Link
JP (1) JPS5719345A (en)

Also Published As

Publication number Publication date
JPS5719345A (en) 1982-02-01

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