JPH0239082B2 - - Google Patents
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- Publication number
- JPH0239082B2 JPH0239082B2 JP53079049A JP7904978A JPH0239082B2 JP H0239082 B2 JPH0239082 B2 JP H0239082B2 JP 53079049 A JP53079049 A JP 53079049A JP 7904978 A JP7904978 A JP 7904978A JP H0239082 B2 JPH0239082 B2 JP H0239082B2
- Authority
- JP
- Japan
- Prior art keywords
- glass
- wire
- ferromagnetic
- iron
- ferromagnetic metal
- 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 - Lifetime
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- Hard Magnetic Materials (AREA)
- Soft Magnetic Materials (AREA)
Description
本発明は磁気的に比較的軟質な強磁性金属細線
の表面を、磁気的に比較的硬質な強磁性酸化物を
含むガラス層で被覆した強磁性細線及びその製造
方法に関するもので、内部の強磁性金属細線の保
磁力を高め、或いは、B−Hループを変形させ或
いはB−Hループをシフトさせ、永久磁石・磁気
センサー・磁気記憶素子・スイツチング素子・自
己回復機能を有する各種素子等の製造に有用な磁
性金属細線を提供する事を目的とするものであ
る。本発明にいう強磁性金属としては、良く知ら
れた鉄・コバルト、ニツケルから成る群から選ば
れた少なくとも一種の元素を含み、他に必要に応
じてチタン、バナジウム、クロム、マンガン、
銅、亜鉛、アルミニウム、ジルコニウム、ニオ
ブ、モリブデン、タングステン、珪素、炭素、硼
素、リン等から成る群から選ばれた少なくとも一
種の元素を添加した金属組成物であり、常温に於
て強磁性を有しているものである。具体的には、
パーマロイ・インバー合金等の鉄・ニツケル系合
金;高コバルト合金・パーメンデユア等の鉄・コ
バルト合金;パーミンバー等の鉄・ニツケル・コ
バルト系合金;いわゆる電気鉄板等の鉄及び鉄・
珪素合金;アルパーム等の鉄・アルミニウム系合
金;センダスト等の鉄・珪素・アルミニウム系合
金;バイカロイ等の鉄・コバルト・バナジウム系
合金;キユニフエ・キユニコ等の鉄・ニツケル・
銅及びコバルト・ニツケル・銅系合金;鉄・クロ
ム・コバルト系合金;アルニコ等の鉄・ニツケ
ル・コバルト・アルミニウム系合金;鉄・炭素系
合金;鉄・コバルト・ニツケルから成る群から選
ばれた少なくとも一種の元素及び硼素・珪素・リ
ン・炭素・アルミニウム・等から成る群から選ば
れた少なくとも一種の元素を含むいわゆる非晶質
合金等通常の磁性関係の文献に書かれている強磁
性体を意味している。
また本発明にいうガラスとは、バリウム;スト
ロンチウム;鉛から成る群から選ばれた少なくと
も一種の元素及び鉄を含む酸化物とB2O3・
S1O2・P2O5・GeO2・As2O3・TeO2・Sb2O3等の
いわゆるガラス形成酸化物と必要に応じて加えら
れた添加物との混合物をガラス化したものであ
り、ガラス形成後の熱処理に依り、いわゆるバリ
ウムフエライトに代表されるマグネトプランバイ
ト型構造を有する強磁性相微結晶を析出させたも
のである。ガラス化の熱処理の温度はガラス組成
にも依存するが、300℃〜1000℃が望ましい。
また本発明にいう微結晶とは直径にして約100
Å〜約1μmに相当する大きさの結晶粒を意図して
おり、約100Å以下では超常磁性的振舞いが顕著
になり、約1μm以上では多磁区構造を有する粒と
なる為共に磁気特性の面から好ましくない。ガラ
ス中に占める微結晶相の割合(占積率)は0.1〜
0.8、より好ましくは0.4〜0.7が望ましいが、アル
ニコ等と違つてさほど敏感ではない。
またガラス被覆層の厚さは金属細線の相当する
径の0.05倍〜0.4倍、より好ましくは0.1倍〜0.3倍
が望ましい。ガラス被覆層が薄すぎる場合、被覆
層の内部強磁性金属に与える効果が小さくなり、
ガラス被覆層が厚すぎる場合、内部強磁性金属の
効果が顕著ではなくなる。
本発明の磁性材料は、いわゆる熔融紡糸法・テ
ーラー法等の様に熔融或いは十分に軟化せしめた
ガラス材料及び熔融せしめた金属組成物を同時に
押出し或いは引き出し、約102℃/秒以上の冷却
速度で急冷して得たガラスで強磁性金属表面を被
覆した細線を上述の様に300℃〜1000℃でマグネ
トプランバイト型微結晶が析出するに十分な時間
0.5〜50時間熱処理する事に依つても得られるが、
この他にも、通常の線引きに依つて得られた金属
細線を熔融せしめた該ガラス組成物中に浸漬し引
き上げてガラス被覆強磁性金属細線を得、後に前
述の熱処理を行なつてマグネトプランバイト型微
結晶を析出させる等の容易に考え得る方法に依り
製造する事が出来る。
また本発明にいう細線は、各種の製造方法があ
る事からも判る様に特に指定した太さ形状は無い
が、熔融紡糸法・テーラー法等に依り製造する場
合には0.1μm〜100μmより好ましくは1μm〜
50μm相当の線径を有するものが望ましい。また、
必要に応じて本発明の細線を更に通常のガラス材
料に依つて被覆する事も出来る。
以下実施例によつて説明する。
実施例 1
B2O312g,BaCO353g,Fe2O335gを白金ルツボ
中1350℃で熔解し銅板上に急冷して得たガラス及
びFe90g,Si10gを真空中・高周波炉で溶解後急
冷して得たFe−Si合金を各々二重ルツボの外及
び内側に入れ、加熱・熔解しいわゆるテーラー法
(G.W.F.Pardoe,E.Butler,D.Gelder;Journal
of Materials Scievce13(1978)786等)に依り
細線化し、ガラス被覆した強磁性金属細線を得
た。線の断面はほゞ円形であり直径は約20μm、
ガラス層の厚さは約2μmであつた。この細線に
500℃〜1000℃で20時間の熱処理を施し、測定を
行なつた。X線回折の結果では、約600℃から
BaO・6Fe2O3の相が析出しているのが見られる。
また、20KOeの磁場で測定した試料の磁束密度
及び20KOeの振巾で振つた時の保磁力を第1表
に示す。
The present invention relates to a ferromagnetic wire in which the surface of a magnetically relatively soft ferromagnetic metal wire is coated with a glass layer containing a magnetically relatively hard ferromagnetic oxide, and a method for manufacturing the same. Manufacture permanent magnets, magnetic sensors, magnetic memory elements, switching elements, various elements with self-recovery functions, etc. by increasing the coercive force of magnetic thin metal wires, or by changing or shifting the B-H loop. The purpose of this invention is to provide a thin magnetic metal wire useful for. The ferromagnetic metal referred to in the present invention includes at least one element selected from the well-known group consisting of iron, cobalt, and nickel, and optionally includes titanium, vanadium, chromium, manganese,
A metal composition containing at least one element selected from the group consisting of copper, zinc, aluminum, zirconium, niobium, molybdenum, tungsten, silicon, carbon, boron, phosphorus, etc., and exhibiting ferromagnetic properties at room temperature. This is what we are doing. in particular,
Iron/nickel alloys such as permalloy and invar alloys; iron/cobalt alloys such as high cobalt alloys and permendure; iron/nickel/cobalt alloys such as perminvar; iron and iron/iron alloys such as so-called electric iron plates
Silicon alloys; iron/aluminum alloys such as Alperm; iron/silicon/aluminum alloys such as Sendust; iron/cobalt/vanadium alloys such as Vicaloy; iron/nickel/nickel alloys such as Kiunihue and Kiyunico.
Copper and cobalt/nickel/copper alloys; iron/chromium/cobalt alloys; iron/nickel/cobalt/aluminum alloys such as alnico; iron/carbon alloys; at least one selected from the group consisting of iron, cobalt, and nickel. A ferromagnetic material described in ordinary magnetism-related literature such as a so-called amorphous alloy containing one type of element and at least one element selected from the group consisting of boron, silicon, phosphorus, carbon, aluminum, etc. are doing. Furthermore, the glass referred to in the present invention refers to an oxide containing at least one element selected from the group consisting of barium, strontium, and lead, and iron, and B 2 O 3 .
Vitrified mixture of so-called glass-forming oxides such as S 1 O 2 , P 2 O 5 , GeO 2 , As 2 O 3 , TeO 2 , Sb 2 O 3 , and additives added as necessary. By heat treatment after glass formation, ferromagnetic phase microcrystals having a magnetoplumbite structure represented by so-called barium ferrite are precipitated. The temperature of the heat treatment for vitrification depends on the glass composition, but is preferably 300°C to 1000°C. In addition, the microcrystal referred to in the present invention is about 100 mm in diameter.
Crystal grains with a size equivalent to approximately 1 μm are intended; below approximately 100 Å, superparamagnetic behavior becomes noticeable, and above approximately 1 μm, grains have a multi-domain structure, both of which are important in terms of magnetic properties. Undesirable. The proportion of microcrystalline phase in the glass (space factor) is 0.1~
A value of 0.8, more preferably 0.4 to 0.7 is desirable, but unlike Alnico etc., it is not very sensitive. The thickness of the glass coating layer is preferably 0.05 to 0.4 times, more preferably 0.1 to 0.3 times, the diameter of the thin metal wire. If the glass coating layer is too thin, it will have less effect on the internal ferromagnetic metal of the coating layer,
If the glass coating layer is too thick, the effect of the internal ferromagnetic metal will not be significant. The magnetic material of the present invention can be produced by simultaneously extruding or drawing out a melted or sufficiently softened glass material and a melted metal composition using the so-called melt spinning method, Taylor method, etc., at a cooling rate of about 10 2 °C/second or more. A fine wire with a ferromagnetic metal surface coated with glass obtained by quenching at 300°C to 1000°C for a sufficient time to precipitate magnetoplumbite-type microcrystals as described above.
It can also be obtained by heat treatment for 0.5 to 50 hours,
In addition, a thin metal wire obtained by ordinary wire drawing is immersed in the melted glass composition and pulled up to obtain a glass-coated ferromagnetic thin metal wire, which is then subjected to the above-mentioned heat treatment to form a magnetoplumbite. It can be manufactured by an easily conceivable method such as precipitation of type microcrystals. In addition, the thin wire referred to in the present invention does not have a specified thickness or shape as can be seen from the fact that there are various manufacturing methods, but when manufacturing by melt spinning method, Taylor method, etc., it is preferably 0.1 μm to 100 μm. is 1μm~
It is desirable to have a wire diameter equivalent to 50 μm. Also,
If necessary, the thin wire of the present invention can be further coated with a conventional glass material. This will be explained below using examples. Example 1 Glass obtained by melting 12 g of B 2 O 3 , 53 g of BaCO 3 , and 35 g of Fe 2 O 3 at 1350°C in a platinum crucible and rapidly cooling it on a copper plate, and 90 g of Fe and 10 g of Si were melted in a high frequency furnace in a vacuum and then rapidly cooled. The Fe-Si alloy obtained by
of Materials Scievce 13 (1978) 786, etc.) to obtain glass-coated ferromagnetic metal thin wires. The cross section of the wire is approximately circular and the diameter is approximately 20 μm.
The thickness of the glass layer was approximately 2 μm. to this thin line
Heat treatment was performed at 500°C to 1000°C for 20 hours, and measurements were taken. According to the results of X-ray diffraction, from about 600℃
It can be seen that the BaO・6Fe 2 O 3 phase is precipitated.
In addition, Table 1 shows the magnetic flux density of the sample measured in a magnetic field of 20 KOe and the coercive force when shaken with an amplitude of 20 KOe.
【表】
実施例 2
実施例1と同じ組成のガラス及び合金材料を用
い同じ装置を使用して、直径約21μm、ガラス層
の厚さが約3μmの細線を得た。この細線に850℃
で20時間の熱処理を施し、測定を行なつた。
20KOeの磁場で測定した結果は試料の磁束密度
約10KG、保磁力は700Oeであつた。
実施例 3
実施例1と同じ組成のガラス及びFe21.2g,
Ni78.5g,Mn0.3g(いわゆる78パーマロイの組成)
を真空中・高周波炉で溶解後急冷して得たFe−
Ni系合金を用いて、実施例1と同じ装置を使用
して、直径25μm、ガラス層の厚さが約1μmの細
線を得た。この細線を700℃で20時間の熱処理を
施し、室温まで急冷して測定した。20KOeでの
試料の磁束密度は約9KG、保磁力は約80Oeであ
つた。
また、正方向に20KOeの磁場をかけた後、磁
場を0Oeとし、次に負方向に200Oeの磁場をかけ
磁化を反転せしめた。その後磁場を再び0Oeに戻
すと磁化は再度反転し正方向を向いた。これは−
200Oeの磁場では被覆ガラス中のバリウムフエラ
イトは反転しない為、−200Oe→0Oeとしても、
内部のパーマロイ層にかかる磁場は、20KOe→
0O2の場合とほゞ同一となつている為と考えら
れ、この現象を用いれば自己回復機能を有する素
子への応用が可能である。[Table] Example 2 Using the same glass and alloy materials as in Example 1 and using the same equipment, a thin wire with a diameter of about 21 μm and a glass layer thickness of about 3 μm was obtained. 850℃ for this thin wire
After heat treatment was performed for 20 hours, measurements were taken.
The results of measurements in a magnetic field of 20KOe showed that the magnetic flux density of the sample was approximately 10KG and the coercive force was 700Oe. Example 3 Glass with the same composition as Example 1 and Fe21.2g,
Ni78.5g, Mn0.3g (composition of so-called 78 permalloy)
Fe-
Using a Ni-based alloy and using the same equipment as in Example 1, a thin wire with a diameter of 25 μm and a glass layer thickness of about 1 μm was obtained. This thin wire was heat-treated at 700°C for 20 hours, rapidly cooled to room temperature, and then measured. The magnetic flux density of the sample at 20KOe was approximately 9KG, and the coercive force was approximately 80Oe. Furthermore, after applying a magnetic field of 20 KOe in the positive direction, the magnetic field was set to 0 Oe, and then a magnetic field of 200 Oe was applied in the negative direction to reverse the magnetization. After that, when the magnetic field was returned to 0Oe, the magnetization reversed again and pointed in the positive direction. This is-
Since the barium ferrite in the coated glass does not reverse in a magnetic field of 200Oe, even if -200Oe → 0Oe,
The magnetic field applied to the internal permalloy layer is 20KOe→
This is thought to be because it is almost the same as in the case of 0O 2 , and if this phenomenon is used, it is possible to apply it to an element with a self-healing function.
Claims (1)
性微結晶粒を析出させたガラスで強磁性金属細線
表面を被覆した事を特徴とする強磁性金属細線。 2 熔融或いは十分に軟化せしめたガラス材料及
び熔融せしめた金属組成物を、同時に押出し或い
は引き出し、102℃/秒以上の冷却速度で急冷し
て得たガラスで強磁性金属表面を被覆した細線を
600℃〜1000℃でマグネツトプランバイト型微結
晶が析出するに十分な時間熱処理する事を特徴と
する強磁性金属細線の製造方法。[Scope of Claims] 1. A ferromagnetic metal wire characterized in that the surface of the ferromagnetic metal wire is coated with glass in which ferromagnetic microcrystalline grains having a magnetoplumbite structure are precipitated. 2 A thin wire whose ferromagnetic metal surface is coated with glass obtained by simultaneously extruding or drawing a melted or sufficiently softened glass material and a melted metal composition and rapidly cooling at a cooling rate of 10 2 °C/sec or more.
A method for producing a ferromagnetic metal thin wire, characterized by heat treatment at 600°C to 1000°C for a sufficient time to precipitate magnetoplumbite type microcrystals.
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP7904978A JPS556858A (en) | 1978-06-29 | 1978-06-29 | Ferromagnetic, metallic thin wire and its preparation |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP7904978A JPS556858A (en) | 1978-06-29 | 1978-06-29 | Ferromagnetic, metallic thin wire and its preparation |
Publications (2)
| Publication Number | Publication Date |
|---|---|
| JPS556858A JPS556858A (en) | 1980-01-18 |
| JPH0239082B2 true JPH0239082B2 (en) | 1990-09-04 |
Family
ID=13679037
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP7904978A Granted JPS556858A (en) | 1978-06-29 | 1978-06-29 | Ferromagnetic, metallic thin wire and its preparation |
Country Status (1)
| Country | Link |
|---|---|
| JP (1) | JPS556858A (en) |
Families Citing this family (1)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| JPS59211841A (en) * | 1983-05-18 | 1984-11-30 | Machida Giken Kogyo:Kk | Pressure expansion testing machine of high pressure gas container |
-
1978
- 1978-06-29 JP JP7904978A patent/JPS556858A/en active Granted
Also Published As
| Publication number | Publication date |
|---|---|
| JPS556858A (en) | 1980-01-18 |
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