JPH0736943B2 - High-permeability soft magnetic fiber and method for producing the same - Google Patents

High-permeability soft magnetic fiber and method for producing the same

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Publication number
JPH0736943B2
JPH0736943B2 JP62310261A JP31026187A JPH0736943B2 JP H0736943 B2 JPH0736943 B2 JP H0736943B2 JP 62310261 A JP62310261 A JP 62310261A JP 31026187 A JP31026187 A JP 31026187A JP H0736943 B2 JPH0736943 B2 JP H0736943B2
Authority
JP
Japan
Prior art keywords
fiber
magnetic
permeability
soft magnetic
diameter
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
Application number
JP62310261A
Other languages
Japanese (ja)
Other versions
JPH01150446A (en
Inventor
隆治 一柳
芳樹 小野
英昭 石原
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.)
Toyobo Co Ltd
Original Assignee
Toyobo Co Ltd
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 Toyobo Co Ltd filed Critical Toyobo Co Ltd
Priority to JP62310261A priority Critical patent/JPH0736943B2/en
Priority to US07/280,320 priority patent/US4946746A/en
Priority to DE3841241A priority patent/DE3841241C2/en
Publication of JPH01150446A publication Critical patent/JPH01150446A/en
Publication of JPH0736943B2 publication Critical patent/JPH0736943B2/en
Anticipated expiration legal-status Critical
Expired - Lifetime legal-status Critical Current

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    • H—ELECTRICITY
    • H01—ELECTRIC ELEMENTS
    • H01F—MAGNETS; INDUCTANCES; TRANSFORMERS; SELECTION OF MATERIALS FOR THEIR MAGNETIC PROPERTIES
    • H01F1/00—Magnets or magnetic bodies characterised by the magnetic materials therefor; Selection of materials for their magnetic properties
    • H01F1/01—Magnets or magnetic bodies characterised by the magnetic materials therefor; Selection of materials for their magnetic properties of inorganic materials
    • H01F1/03—Magnets or magnetic bodies characterised by the magnetic materials therefor; Selection of materials for their magnetic properties of inorganic materials characterised by their coercivity
    • H01F1/12—Magnets or magnetic bodies characterised by the magnetic materials therefor; Selection of materials for their magnetic properties of inorganic materials characterised by their coercivity of soft-magnetic materials
    • H01F1/14—Magnets or magnetic bodies characterised by the magnetic materials therefor; Selection of materials for their magnetic properties of inorganic materials characterised by their coercivity of soft-magnetic materials metals or alloys
    • H01F1/20—Magnets or magnetic bodies characterised by the magnetic materials therefor; Selection of materials for their magnetic properties of inorganic materials characterised by their coercivity of soft-magnetic materials metals or alloys in the form of particles, e.g. powder
    • B—PERFORMING OPERATIONS; TRANSPORTING
    • B22—CASTING; POWDER METALLURGY
    • B22D—CASTING OF METALS; CASTING OF OTHER SUBSTANCES BY THE SAME PROCESSES OR DEVICES
    • B22D11/00—Continuous casting of metals, i.e. casting in indefinite lengths
    • B22D11/005—Continuous casting of metals, i.e. casting in indefinite lengths of wire
    • C—CHEMISTRY; METALLURGY
    • C30—CRYSTAL GROWTH
    • C30B—SINGLE-CRYSTAL GROWTH; UNIDIRECTIONAL SOLIDIFICATION OF EUTECTIC MATERIAL OR UNIDIRECTIONAL DEMIXING OF EUTECTOID MATERIAL; REFINING BY ZONE-MELTING OF MATERIAL; PRODUCTION OF A HOMOGENEOUS POLYCRYSTALLINE MATERIAL WITH DEFINED STRUCTURE; SINGLE CRYSTALS OR HOMOGENEOUS POLYCRYSTALLINE MATERIAL WITH DEFINED STRUCTURE; AFTER-TREATMENT OF SINGLE CRYSTALS OR A HOMOGENEOUS POLYCRYSTALLINE MATERIAL WITH DEFINED STRUCTURE; APPARATUS THEREFOR
    • C30B15/00—Single-crystal growth by pulling from a melt, e.g. Czochralski method
    • C—CHEMISTRY; METALLURGY
    • C30—CRYSTAL GROWTH
    • C30B—SINGLE-CRYSTAL GROWTH; UNIDIRECTIONAL SOLIDIFICATION OF EUTECTIC MATERIAL OR UNIDIRECTIONAL DEMIXING OF EUTECTOID MATERIAL; REFINING BY ZONE-MELTING OF MATERIAL; PRODUCTION OF A HOMOGENEOUS POLYCRYSTALLINE MATERIAL WITH DEFINED STRUCTURE; SINGLE CRYSTALS OR HOMOGENEOUS POLYCRYSTALLINE MATERIAL WITH DEFINED STRUCTURE; AFTER-TREATMENT OF SINGLE CRYSTALS OR A HOMOGENEOUS POLYCRYSTALLINE MATERIAL WITH DEFINED STRUCTURE; APPARATUS THEREFOR
    • C30B15/00—Single-crystal growth by pulling from a melt, e.g. Czochralski method
    • C30B15/007—Pulling on a substrate
    • C—CHEMISTRY; METALLURGY
    • C30—CRYSTAL GROWTH
    • C30B—SINGLE-CRYSTAL GROWTH; UNIDIRECTIONAL SOLIDIFICATION OF EUTECTIC MATERIAL OR UNIDIRECTIONAL DEMIXING OF EUTECTOID MATERIAL; REFINING BY ZONE-MELTING OF MATERIAL; PRODUCTION OF A HOMOGENEOUS POLYCRYSTALLINE MATERIAL WITH DEFINED STRUCTURE; SINGLE CRYSTALS OR HOMOGENEOUS POLYCRYSTALLINE MATERIAL WITH DEFINED STRUCTURE; AFTER-TREATMENT OF SINGLE CRYSTALS OR A HOMOGENEOUS POLYCRYSTALLINE MATERIAL WITH DEFINED STRUCTURE; APPARATUS THEREFOR
    • C30B29/00—Single crystals or homogeneous polycrystalline material with defined structure characterised by the material or by their shape
    • C30B29/10—Inorganic compounds or compositions
    • C30B29/52—Alloys
    • C—CHEMISTRY; METALLURGY
    • C30—CRYSTAL GROWTH
    • C30B—SINGLE-CRYSTAL GROWTH; UNIDIRECTIONAL SOLIDIFICATION OF EUTECTIC MATERIAL OR UNIDIRECTIONAL DEMIXING OF EUTECTOID MATERIAL; REFINING BY ZONE-MELTING OF MATERIAL; PRODUCTION OF A HOMOGENEOUS POLYCRYSTALLINE MATERIAL WITH DEFINED STRUCTURE; SINGLE CRYSTALS OR HOMOGENEOUS POLYCRYSTALLINE MATERIAL WITH DEFINED STRUCTURE; AFTER-TREATMENT OF SINGLE CRYSTALS OR A HOMOGENEOUS POLYCRYSTALLINE MATERIAL WITH DEFINED STRUCTURE; APPARATUS THEREFOR
    • C30B29/00—Single crystals or homogeneous polycrystalline material with defined structure characterised by the material or by their shape
    • C30B29/60—Single crystals or homogeneous polycrystalline material with defined structure characterised by the material or by their shape characterised by shape
    • H—ELECTRICITY
    • H01—ELECTRIC ELEMENTS
    • H01F—MAGNETS; INDUCTANCES; TRANSFORMERS; SELECTION OF MATERIALS FOR THEIR MAGNETIC PROPERTIES
    • H01F1/00—Magnets or magnetic bodies characterised by the magnetic materials therefor; Selection of materials for their magnetic properties
    • H01F1/01—Magnets or magnetic bodies characterised by the magnetic materials therefor; Selection of materials for their magnetic properties of inorganic materials
    • H01F1/03—Magnets or magnetic bodies characterised by the magnetic materials therefor; Selection of materials for their magnetic properties of inorganic materials characterised by their coercivity
    • H01F1/12—Magnets or magnetic bodies characterised by the magnetic materials therefor; Selection of materials for their magnetic properties of inorganic materials characterised by their coercivity of soft-magnetic materials
    • H01F1/14—Magnets or magnetic bodies characterised by the magnetic materials therefor; Selection of materials for their magnetic properties of inorganic materials characterised by their coercivity of soft-magnetic materials metals or alloys
    • H01F1/147—Alloys characterised by their composition
    • H01F1/153—Amorphous metallic alloys, e.g. glassy metals
    • H01F1/15325—Amorphous metallic alloys, e.g. glassy metals containing rare earths
    • H—ELECTRICITY
    • H01—ELECTRIC ELEMENTS
    • H01F—MAGNETS; INDUCTANCES; TRANSFORMERS; SELECTION OF MATERIALS FOR THEIR MAGNETIC PROPERTIES
    • H01F1/00—Magnets or magnetic bodies characterised by the magnetic materials therefor; Selection of materials for their magnetic properties
    • H01F1/01—Magnets or magnetic bodies characterised by the magnetic materials therefor; Selection of materials for their magnetic properties of inorganic materials
    • H01F1/03—Magnets or magnetic bodies characterised by the magnetic materials therefor; Selection of materials for their magnetic properties of inorganic materials characterised by their coercivity
    • H01F1/12—Magnets or magnetic bodies characterised by the magnetic materials therefor; Selection of materials for their magnetic properties of inorganic materials characterised by their coercivity of soft-magnetic materials
    • H01F1/14—Magnets or magnetic bodies characterised by the magnetic materials therefor; Selection of materials for their magnetic properties of inorganic materials characterised by their coercivity of soft-magnetic materials metals or alloys
    • H01F1/147—Alloys characterised by their composition
    • H01F1/153—Amorphous metallic alloys, e.g. glassy metals
    • H01F1/15391—Elongated structures, e.g. wires

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  • Chemical & Material Sciences (AREA)
  • Engineering & Computer Science (AREA)
  • Crystallography & Structural Chemistry (AREA)
  • Materials Engineering (AREA)
  • Metallurgy (AREA)
  • Organic Chemistry (AREA)
  • Power Engineering (AREA)
  • Dispersion Chemistry (AREA)
  • Electromagnetism (AREA)
  • Physics & Mathematics (AREA)
  • Mechanical Engineering (AREA)
  • Inorganic Chemistry (AREA)
  • Continuous Casting (AREA)
  • Inorganic Fibers (AREA)

Description

【発明の詳細な説明】 [産業上の利用分野] 本発明は、磁化の非常に容易な高透磁率軟磁性繊維及び
その製造方法に関するものである。
Description: TECHNICAL FIELD The present invention relates to a high-permeability soft magnetic fiber having extremely easy magnetization and a method for producing the same.

[従来の技術] 珪素鋼などの磁性材料は、交流励磁に適合する様に薄肉
のものを一定の形に打ち抜いた後複数枚を積層して使用
される。即ち交流励磁における渦電流損失及びヒステリ
シス損失を小さくする主旨であり、高周波数領域で磁性
材料が励磁される場合には、磁性材料をさらに細分割し
て鉄損の低減を図ると共に、透磁率の動特性を向上させ
る必要がある。
[Prior Art] A magnetic material such as silicon steel is used by stacking a plurality of thin materials after punching a thin material into a certain shape so as to be suitable for AC excitation. That is, the purpose is to reduce eddy current loss and hysteresis loss in AC excitation, and when a magnetic material is excited in a high frequency region, the magnetic material is further subdivided to reduce iron loss and magnetic permeability. It is necessary to improve the dynamic characteristics.

ところで技術革新が進むにつれて電子・電磁機器の小型
化・軽量化に対する要請は益々強くなっており、こうし
た要望に沿うため小型磁性材料に関する改良研究も盛ん
に行なわれている。
By the way, as technological innovation progresses, demands for miniaturization and weight reduction of electronic / electromagnetic devices are increasing more and more, and in order to meet such demands, improvement studies on small magnetic materials are being actively conducted.

電磁機器を小型化し、あるいは細分割するための一つの
方法として、磁性材料を繊維状に形成することが考えら
れるが、繊維状磁性材料の磁気特性を高めるうえでは、
結晶粒界や不純物などの欠陥や内部歪を少なくして磁化
され易い構造にすることが大切である。しかも繊維軸方
向に異方性を有する高透磁性の軟磁性繊維を得るには、
結晶の磁化容易軸の方向を軟磁性繊維の繊維軸の方向に
揃えることが必要になってくる。
As one method for downsizing or subdividing an electromagnetic device, it is conceivable to form a magnetic material into a fibrous shape. In order to enhance the magnetic characteristics of the fibrous magnetic material,
It is important to reduce defects such as crystal grain boundaries and impurities and internal strain so that the structure is easily magnetized. Moreover, in order to obtain a highly permeable soft magnetic fiber having anisotropy in the fiber axis direction,
It is necessary to align the easy axis of magnetization of the crystal with the fiber axis of the soft magnetic fiber.

[発明が解決しようとする問題点] 本発明は上記のような状況の下で、磁性材料からなる繊
維状物の結晶粒界や内部歪を極力少なくすることによっ
て磁化を容易にし、また磁化容易軸の方向が繊維軸方向
に揃った構造特性を与えることによって、比透磁率が非
常に大きく高レベルの透磁性を示す様な軟磁性繊維及び
その製造方法を提供しようとするものである。
[Problems to be Solved by the Invention] Under the circumstances as described above, the present invention facilitates magnetization by minimizing crystal grain boundaries and internal strain of a fibrous material made of a magnetic material, and facilitates magnetization. An object of the present invention is to provide a soft magnetic fiber having a very large relative magnetic permeability and a high level of magnetic permeability by providing structural characteristics in which the axis direction is aligned with the fiber axis direction, and a method for producing the same.

[問題点を解決するための手段] 本発明に係る高透磁率軟磁性繊維は、直径が100μm以
下であり、且つ直流磁化状態における比透磁率が90,000
以上であるところに要旨を有するものであり、この様な
高透磁率の軟磁性繊維は、磁化の容易な磁性材料を使用
し、溶融紡糸によって、樹枝状晶の一次アームが繊維軸
方向に対して角度20度以内、好ましくは5度以内で揃っ
た樹枝状組織を有する直径100μm以下の磁性繊維を作
製し、その後熱処理によって結晶粒界や内部歪を極力少
なくすることによって得ることができる。
[Means for Solving Problems] The high-permeability soft magnetic fiber according to the present invention has a diameter of 100 μm or less and a relative magnetic permeability of 90,000 in a DC magnetized state.
The above is the gist, and such a high magnetic permeability soft magnetic fiber uses a magnetic material that is easily magnetized, and by melt spinning, the primary arm of the dendritic crystal is oriented in the fiber axis direction. It can be obtained by producing magnetic fibers having a dendritic structure with an angle within 20 degrees, preferably within 5 degrees, and having a diameter of 100 μm or less, and then performing heat treatment to reduce grain boundaries and internal strain as much as possible.

[作用及び実施例] 上記の様に本発明の高透磁率の軟磁性繊維は、直径が10
0μm以下と非常に細いものであり、直流磁化状態にお
いて90,000以上といった高レベルの比透磁率を有してい
る。ここで繊維の直径を100μm以下に定めたのは、こ
の値を超える太径繊維では、追って詳述する如く繊維組
織に十分な方向性が与えられず、上記の様な高レベルの
比透磁率を確保することができないからである。また直
流磁化状態における比透磁率の下限を90,000に定めたの
は、90,000を下回るものでは本発明の意図する高透磁率
軟磁性繊維としての要求特性を満足すことができないか
らである。
[Operations and Examples] As described above, the high magnetic permeability soft magnetic fiber of the present invention has a diameter of 10
It is very thin, 0 μm or less, and has a high level of relative magnetic permeability of 90,000 or more in a DC magnetized state. Here, the diameter of the fiber is set to 100 μm or less because, in the case of a large diameter fiber exceeding this value, sufficient directivity is not given to the fiber structure as will be described in detail later, and the high level of relative permeability as described above. This is because it cannot be secured. Further, the lower limit of the relative magnetic permeability in the direct-current magnetized state is set to 90,000 because if it is less than 90,000, the required characteristics as the high magnetic permeability soft magnetic fiber intended by the present invention cannot be satisfied.

本発明で使用される磁性材料としては種々のものが考え
られるが、中でも本発明の特徴を最も有効に発揮するの
はFe−Si系合金、Fe−Al系合金、Fe−Si−Al系合金であ
り、これらの鉄合金中に適量の希土類金属を1種または
2種以上含有させたものも好ましいものとして挙げられ
る。尚希土類金属として特に好ましいのは、原子番号が
57〜71のランタン系列から選択されるものであって、具
体的にはLa,Ce,Pr,Nd,Pm,Sm,Eu,Gd,Tb,Dy,Ho,Er,Tm,Yb,
Luであり、これらは単独で含有させてもよく、あるいは
2種以上を複合して含有させることもできる。上記希土
類金属の中でも特に好ましいのはCeである。また本発明
を実施するに当たっては、軟磁性繊維の用途や要求特性
に応じて更に他の成分を配合することも可能である。
There are various possible magnetic materials used in the present invention. Among them, Fe-Si alloys, Fe-Al alloys, and Fe-Si-Al alloys most effectively exhibit the characteristics of the present invention. Among these iron alloys, one containing one or more rare earth metals in an appropriate amount is also preferable. In addition, it is particularly preferable that the rare earth metal has an atomic number
It is selected from the lanthanum series of 57 to 71, specifically, La, Ce, Pr, Nd, Pm, Sm, Eu, Gd, Tb, Dy, Ho, Er, Tm, Yb,
Lu, which may be contained alone or in combination of two or more. Among the above rare earth metals, Ce is particularly preferable. Further, in carrying out the present invention, it is possible to further mix other components depending on the use and required characteristics of the soft magnetic fiber.

ところで前述の様な高透磁率の軟磁性繊維を製造する方
法としては、磁性材料を溶融紡糸して樹枝状晶の一次ア
ームが繊維軸方向に対して20度以内の角度で揃って成長
した軟磁性繊維(第4図(a)、(b)参照)とした
後、これを熱処理して内部歪を除去するとともに樹枝状
晶を消失せしめ、均質化する方法が挙げられる。
By the way, as a method for producing a soft magnetic fiber having a high magnetic permeability as described above, a magnetic material is melt-spun and a primary arm of a dendrite is softly grown at an angle within 20 degrees with respect to the fiber axis direction. A method in which a magnetic fiber (see FIGS. 4 (a) and 4 (b)) is heat treated to remove internal strain, and dendrites disappear to homogenize the magnetic fiber can be used.

溶融紡糸法としては、たとえガラス被覆紡糸法、水流中
紡糸法、回転液中紡糸法等が例示されるが、中でも特に
好ましいのは特開昭55−64948号公報に開示された様な
回転液中紡糸法である。第1、2図はその方法を例示す
る概略正面図及び一部断面側面図であり、回転ドラム6
を高速回転させることによってその内周面側に冷却液体
層8を形成する。そして該液体層8の液面9に向けて、
るつぼ1下面の噴出ノズル2から溶融した磁性材料を噴
出させ、磁性材料を細線状4にして急冷凝固させながら
回転ドラム6の内周壁に巻き取っていく。図中3は磁性
材料を溶融させるためのヒーター、5は溶融磁性材料噴
出用の不活性ガス、7はモータ、10はベルトを夫々示
す。そして回転する冷却液体層の周速度を、噴出ノズル
2からの溶融磁性材料の噴出速度と実質的に同一かまた
はそれよりやや早くしておけば、断面均一性の良好な磁
性繊維が得られ易い。ここで使用される冷却液体は純粋
な液体の他、溶液、エマルジョン等のいずれであっても
よいが、コスト及び冷却効率を総合すると最も好ましい
のは水である。回転ドラムは横向きでも縦向きでもよい
が、該ドラム中の冷却液体層の表面速度は300〜900m/mi
n程度、溶融磁性材料の冷却液体層への侵入角度は40〜8
0゜、噴出ノズル2と冷却液体層8の液面9との距離は
0.5〜10mm程度が夫々好適である。この場合、特に注意
しなければならないのは、噴出ノズル2の口径を100μ
m以下とし、紡糸される磁性繊維の直径が100μm以下
としなければならないことである。しかして噴出ノズル
2の口径が100μmを超える場合は、その内部組織にお
いて、繊維軸方向に対する樹枝状晶一次アームの成長方
向が20度以内の角度で揃わなくなり、後述する様な熱処
理を行なって結晶粒界や内部歪を極力少なくしたとして
も、前述の如き高透磁率の軟磁性繊維は得られない。該
繊維の直径を100μm以下とすることによって何故上述
のような組織が形成されるのか、その機構の詳細は明ら
かではないが、得られた繊維の内部組織や結晶方位等の
観察結果からすると次の様に考えることができる。即
ち、溶融磁性材料の噴出流の太さの違いによって冷却液
体層中における冷却速度が変わり、結晶の生成及び成長
状況が変化することによって結晶の成長方向が繊維軸方
向に揃い、その後の熱処理で樹枝状晶が消失した後も一
次アームの方向性が保たれており結晶の方向性に好まし
い影響を及ぼしたためと推定される。
Examples of the melt spinning method include a glass coating spinning method, a water spinning method, and a rotating liquid spinning method. Among them, particularly preferred is a spinning solution as disclosed in JP-A-55-64948. Medium spinning method. 1 and 2 are a schematic front view and a partial cross-sectional side view illustrating the method, and FIG.
By rotating at high speed, the cooling liquid layer 8 is formed on the inner peripheral surface side. Then, toward the liquid surface 9 of the liquid layer 8,
The molten magnetic material is ejected from the ejection nozzle 2 on the lower surface of the crucible 1, and the magnetic material is made into a thin wire 4 and rapidly cooled and solidified, and wound around the inner peripheral wall of the rotary drum 6. In the figure, 3 is a heater for melting the magnetic material, 5 is an inert gas for ejecting the molten magnetic material, 7 is a motor, and 10 is a belt. If the peripheral velocity of the rotating cooling liquid layer is set to be substantially the same as or slightly higher than the ejection velocity of the molten magnetic material from the ejection nozzle 2, magnetic fibers having good cross-sectional uniformity can be easily obtained. . The cooling liquid used here may be a pure liquid, a solution, an emulsion or the like, but water is most preferable in terms of cost and cooling efficiency. The rotating drum may be horizontal or vertical, but the surface velocity of the cooling liquid layer in the drum is 300 to 900 m / mi.
n, the penetration angle of the molten magnetic material into the cooling liquid layer is 40 to 8
0 °, the distance between the jet nozzle 2 and the liquid surface 9 of the cooling liquid layer 8 is
0.5 to 10 mm is suitable for each. In this case, it should be noted that the diameter of the jet nozzle 2 should be 100μ.
The diameter of the spun magnetic fiber must be 100 μm or less. However, when the diameter of the jet nozzle 2 exceeds 100 μm, the growth direction of the dendrite primary arms with respect to the fiber axis direction is not aligned within 20 degrees in the internal structure, and the heat treatment as described below is performed to crystallize. Even if grain boundaries and internal strain are reduced as much as possible, the above-mentioned soft magnetic fiber having high magnetic permeability cannot be obtained. The reason why the above-mentioned structure is formed by setting the diameter of the fiber to 100 μm or less, the details of the mechanism are not clear, but from the observation result of the internal structure and the crystal orientation of the obtained fiber, the following is obtained. You can think like. That is, the cooling rate in the cooling liquid layer changes due to the difference in the thickness of the jet flow of the molten magnetic material, and the crystal growth and growth conditions change, so that the crystal growth direction is aligned with the fiber axis direction. It is presumed that the orientation of the primary arm was maintained even after the dendrites disappeared, which had a favorable effect on the orientation of the crystals.

尚熱処理は、内部歪を解消すると共に魚冷凝固時に生成
した樹枝状晶を実質的に消失せしめ、均質化の目的を果
たし得る様、磁性材料の種類に応じて適宜定めるべきで
あるが、一般的な基準としては、繊維を溶融させること
なく短時間で均質化し得る様、[当該磁性材料の固相線
温度−10℃]よりも低く且つ[当該磁性材料の融点の1/
3]以上の温度の範囲で行なうのがよい。また熱処理
は、繊維表面の酸化を防止するため真空もしくはアルゴ
ン等の不活性ガス雰囲気で行なうことが望まれる。
The heat treatment should be appropriately determined according to the type of magnetic material so that the internal strain is eliminated and the dendrites formed during fish coagulation are substantially eliminated, and the purpose of homogenization can be achieved. As a standard, the temperature is lower than [solidus temperature of the magnetic material −10 ° C.] and [1 / the melting point of the magnetic material] so that the fibers can be homogenized in a short time without melting.
3] It is better to do it in the temperature range above. Further, it is desirable that the heat treatment is performed in a vacuum or in an atmosphere of an inert gas such as argon in order to prevent the fiber surface from being oxidized.

例えば、磁性材料としてFe−5.7重量%Si合金を使用
し、上記のような回転液中紡糸時における噴出ノズルの
口径(紡出繊維の直径に対応する)を150μmまたは95
μmに設定して磁性繊維とした後、1000℃で1時間熱処
理したものについて、繊維軸方向に直流磁場を印加した
時の室温における直流磁化曲線を調べたところによる
と、直径150μmに太径磁性繊維の比最大透磁率は53,00
0と低い値しか得られていないのに対し、直径が95μm
の細径磁性繊維の比最大透磁率は121,000と2倍以上に
大きい値が得られた。また第3図は、上記と同じ材料を
使用し、上記と同じ方法で紡糸した磁性繊維を、1100℃
で2時間熱処理した磁性繊維について、比透磁率(縦
軸)の励磁周波数(横軸)特性を示したものであり、直
径95μmの細径磁性繊維は、直径150μmの太径磁性繊
維に比べて、各周波数帯で大きな比透磁率を示してい
る。
For example, Fe-5.7 wt% Si alloy is used as the magnetic material, and the diameter of the jet nozzle (corresponding to the diameter of the spun fiber) at the time of spinning in the rotating liquid as described above is 150 μm or 95
After the magnetic fiber was set to μm and heat-treated at 1000 ° C. for 1 hour, the DC magnetization curve at room temperature when a DC magnetic field was applied in the fiber axis direction was examined. Specific maximum magnetic permeability of fiber is 53,00
The value is as low as 0, whereas the diameter is 95 μm.
The specific maximum magnetic permeability of the small-diameter magnetic fiber was 121,000, which was more than doubled. In addition, Fig. 3 shows that the magnetic fibers spun in the same manner as above using the same materials as above
Shows the magnetic permeability of the relative magnetic permeability (vertical axis) (horizontal axis) of the magnetic fiber heat-treated for 2 hours at 95 μm in diameter as compared with the thick magnetic fiber in 150 μm in diameter. , Shows a large relative permeability in each frequency band.

磁性繊維の直径を細くすることによって軟磁気特性が著
しく改善される理由を解明するため、繊維の内部組織を
調べてみたところ、次の様な事実が確認された。即ち直
径100μmを超える太径の磁性繊維は、熱処理前の状態
で樹枝状晶の一次アームの成長方向が繊維軸方向に対し
て角度20度を超えるものが多数存在しているのに対し、
直径100μm以下の細径の磁性繊維における樹枝状晶の
一次アームの成長方向は繊維軸方向に対して全てが20度
以内の角度にあった。そしてこれらをさらに熱処理して
結晶粒界や内部歪を減少させた後エッチピット法により
結晶方位を調べてみると、熱処理繊維の結晶方位は熱処
理前の組織を反映しており、太径磁性繊維には、特定の
結晶方位が繊維軸方向に対して20度を超えるものが多数
存在するのに対し、細径磁性繊維では、特定の結晶方位
が繊維軸方向に対して20度以内の角度で一様に揃ってい
ることが確認された。磁化の容易な方向は結晶方位と一
定の関係を有することが知られており、直径100μm以
下の細径磁性繊維では、前述の如く繊維軸方向に対して
20度以内の角度で揃った熱処理前の樹枝状晶一次アーム
が結晶粒界や内部歪の減少後も有効に反映されて、磁化
が容易で且つ極めて強い異方性をもつた磁性繊維とな
り、これらが透磁率の向上に好影響をもたらしたものと
考えられる。
In order to elucidate the reason why the soft magnetic properties are remarkably improved by reducing the diameter of the magnetic fiber, the internal structure of the fiber was examined, and the following facts were confirmed. That is, in the large diameter magnetic fibers having a diameter of more than 100 μm, there are many magnetic fibers in which the primary arm growth direction of the dendrites exceeds 20 ° with respect to the fiber axis direction before heat treatment.
The growth direction of the primary arms of the dendrites in the magnetic fibers having a diameter of 100 μm or less was all within 20 ° with respect to the fiber axis direction. After further heat treating these to reduce the crystal grain boundaries and internal strain, the crystal orientation of the heat treated fiber was examined by the etch pit method. The crystal orientation of the heat treated fiber reflects the structure before heat treatment. There are many specific crystal orientations that exceed 20 degrees with respect to the fiber axis direction, whereas in thin magnetic fibers, the specific crystal orientation is within 20 degrees with respect to the fiber axis direction. It was confirmed that they were even. It is known that the direction of easy magnetization has a certain relationship with the crystal orientation. For small-diameter magnetic fibers with a diameter of 100 μm or less, the direction of the fiber axis is as described above.
The dendrite primary arms before heat treatment aligned at an angle of 20 degrees or less are effectively reflected even after the reduction of grain boundaries and internal strain, resulting in a magnetic fiber with easy magnetization and extremely strong anisotropy, It is considered that these had a favorable effect on the improvement of magnetic permeability.

又、結晶粒界が非常に少ないということはとりもなおさ
ず靭性や柔軟性にも優れたものであることを意味してお
り、2次加工を含めて非常に取扱い易い材料である。
In addition, the fact that the number of crystal grain boundaries is extremely small means that the toughness and flexibility are excellent, and it is a material that is extremely easy to handle including secondary processing.

このようにして得られる高透磁率の軟磁性繊維は、一本
のままで小型軟磁性材料として利用できるだけでなく、
適当な方法で絶縁皮膜を施した当該繊維を多数束ね、高
周波特性の優れた軟磁性材料として使用すこともでき
る。
The high-permeability soft magnetic fiber thus obtained can be used as a small soft magnetic material as it is,
It is also possible to bundle a large number of the fibers coated with an insulating film by an appropriate method and use them as a soft magnetic material having excellent high frequency characteristics.

例えば、当該軟磁性材料を磁気増幅器の磁心に応用すれ
ば、時定数の非常に小さい優れた性能の磁気増幅器を作
製することができる。
For example, when the soft magnetic material is applied to the magnetic core of a magnetic amplifier, a magnetic amplifier having an excellent performance with a very small time constant can be manufactured.

[発明の効果] 本発明は以上の様に構成されており、細径で、磁化の障
害となる結晶粒界や内部歪が非常に少なく、高透磁率、
低保磁力の要求特性を共に満足する軟磁性繊維とその製
造方法を提供し得ることになった。そしてこの高透磁率
軟磁性繊維は、小型軟磁性材料として、或いは渦電流損
失やヒステリシス損失の非常に小さなものとして各種変
圧器や磁気増幅器の磁心材料として有用であり、その他
様々の電磁器分野に幅広く活用することが期待される。
[Advantages of the Invention] The present invention is configured as described above, has a small diameter, has very few crystal grain boundaries and internal strains that obstruct magnetization, and has high magnetic permeability,
It has become possible to provide a soft magnetic fiber that satisfies both the required characteristics of low coercive force and a manufacturing method thereof. And this high permeability soft magnetic fiber is useful as a small soft magnetic material or as a magnetic core material for various transformers and magnetic amplifiers with very small eddy current loss and hysteresis loss. Expected to be widely used.

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

第1、2図は回転液中紡糸法を説明するための図であ
り、第1図は概略正面図、第2図は一部断面側面図、第
3図は実施例で得た軟磁性繊維の室温における比透磁率
と励磁周波数の関係を対比して示すグラフである。また
第4図(a)および(b)は、一次アームと繊維軸との
なす角度が20度以下である樹枝状組織を有する軟磁性繊
維の説明図である。 1:るつぼ、2:噴出ノズル 3:ヒーター、4:細線 5:不活性ガス、6:回転ドラム 7:モータ、8:冷却液体 9:冷却液面、10:ベルト
FIGS. 1 and 2 are views for explaining a spinning in-liquid spinning method. FIG. 1 is a schematic front view, FIG. 2 is a partial cross-sectional side view, and FIG. 3 is a soft magnetic fiber obtained in an example. 4 is a graph showing the relationship between the relative magnetic permeability at room temperature and the excitation frequency. 4 (a) and 4 (b) are explanatory views of a soft magnetic fiber having a dendritic tissue in which the angle formed by the primary arm and the fiber axis is 20 degrees or less. 1: crucible 2: jet nozzle 3: heater, 4: fine wire 5: inert gas, 6: rotating drum 7: motor, 8: cooling liquid 9: cooling liquid level, 10: belt

───────────────────────────────────────────────────── フロントページの続き (56)参考文献 特開 昭51−138517(JP,A) 特開 昭61−123448(JP,A) 特開 昭55−64948(JP,A) ─────────────────────────────────────────────────── ─── Continuation of the front page (56) References JP-A-51-138517 (JP, A) JP-A-61-123448 (JP, A) JP-A-55-64948 (JP, A)

Claims (2)

【特許請求の範囲】[Claims] 【請求項1】直径100μm以下で、樹枝状晶の一次アー
ムが繊維軸方向に対して20度以内の角度で成長した樹枝
状組織を有する磁性繊維を、熱処理によって内部歪を除
去すると共に樹枝状組織を消失させたものであり、且つ
直流磁化状態における比透磁率が90,000以上であること
を特徴とする高透磁率軟磁性繊維。
1. A magnetic fiber having a dendritic structure with a diameter of 100 μm or less and a primary arm of the dendritic crystal grown at an angle within 20 degrees with respect to the fiber axis direction, is subjected to heat treatment to remove internal strain and to be dendritic A high-permeability soft magnetic fiber characterized by having a tissue disappeared and having a relative magnetic permeability of 90,000 or more in a DC magnetized state.
【請求項2】磁性材料を溶融紡糸し、直径100μm以下
で、樹枝状晶の一次アームが繊維軸方向に対して20度以
内の角度で成長した樹枝状組織を有する磁性繊維を得た
後、熱処理によって該繊維の内部歪を除去すると共に樹
枝状組織を消失させて、直流磁化状態における比透磁率
を90,000以上にすることを特徴とする高透磁率軟磁性繊
維の製造方法。
2. A magnetic material is melt-spun to obtain a magnetic fiber having a dendritic structure having a diameter of 100 μm or less and a primary arm of dendrite growing at an angle within 20 ° with respect to the fiber axis direction. A method for producing a high-permeability soft magnetic fiber, characterized in that the internal strain of the fiber is removed by heat treatment and the dendritic structure is eliminated so that the relative magnetic permeability in a direct current magnetized state is 90,000 or more.
JP62310261A 1987-12-08 1987-12-08 High-permeability soft magnetic fiber and method for producing the same Expired - Lifetime JPH0736943B2 (en)

Priority Applications (3)

Application Number Priority Date Filing Date Title
JP62310261A JPH0736943B2 (en) 1987-12-08 1987-12-08 High-permeability soft magnetic fiber and method for producing the same
US07/280,320 US4946746A (en) 1987-12-08 1988-12-06 Novel metal fiber and process for producing the same
DE3841241A DE3841241C2 (en) 1987-12-08 1988-12-07 Metal fiber and method of manufacturing a metal fiber

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP62310261A JPH0736943B2 (en) 1987-12-08 1987-12-08 High-permeability soft magnetic fiber and method for producing the same

Publications (2)

Publication Number Publication Date
JPH01150446A JPH01150446A (en) 1989-06-13
JPH0736943B2 true JPH0736943B2 (en) 1995-04-26

Family

ID=18003119

Family Applications (1)

Application Number Title Priority Date Filing Date
JP62310261A Expired - Lifetime JPH0736943B2 (en) 1987-12-08 1987-12-08 High-permeability soft magnetic fiber and method for producing the same

Country Status (1)

Country Link
JP (1) JPH0736943B2 (en)

Family Cites Families (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS5824924B2 (en) * 1975-05-28 1983-05-24 株式会社日立製作所 Stork

Also Published As

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JPH01150446A (en) 1989-06-13

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