JPS6331087B2 - - Google Patents

Info

Publication number
JPS6331087B2
JPS6331087B2 JP54088069A JP8806979A JPS6331087B2 JP S6331087 B2 JPS6331087 B2 JP S6331087B2 JP 54088069 A JP54088069 A JP 54088069A JP 8806979 A JP8806979 A JP 8806979A JP S6331087 B2 JPS6331087 B2 JP S6331087B2
Authority
JP
Japan
Prior art keywords
examples
alloy
plate
thickness
same
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
JP54088069A
Other languages
Japanese (ja)
Other versions
JPS5612705A (en
Inventor
Kenichiro Momose
Kyoshi Kumagai
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.)
Toshiba Corp
Original Assignee
Tokyo Shibaura Electric 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 Tokyo Shibaura Electric Co Ltd filed Critical Tokyo Shibaura Electric Co Ltd
Priority to JP8806979A priority Critical patent/JPS5612705A/en
Publication of JPS5612705A publication Critical patent/JPS5612705A/en
Publication of JPS6331087B2 publication Critical patent/JPS6331087B2/ja
Granted 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
    • H01F1/12Magnets 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
    • H01F1/14Magnets 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
    • H01F1/16Magnets 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 sheets

Landscapes

  • Chemical & Material Sciences (AREA)
  • Dispersion Chemistry (AREA)
  • Engineering & Computer Science (AREA)
  • Power Engineering (AREA)
  • Heat Treatment Of Nonferrous Metals Or Alloys (AREA)
  • Magnetic Heads (AREA)
  • Soft Magnetic Materials (AREA)

Description

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

本発明は、鉄−ニツケル系合金からなる磁気ヘ
ツドコア用素材に関するものであり、さらに詳し
くは鉄−ニツケル系合金を熱間加工又は冷間加工
により2層以上にクラツドしてなる磁気ヘツドコ
ア用素材に関するものである。 パーマロイと呼ばれる鉄−ニツケル系合金は初
透磁率(μo)及び最大透磁率(μm)が高く、
保磁力が小さい特性を有しており、磁気テープレ
コーダ等の磁気ヘツド用材料として用いられてい
るが、パーマロイ自身は固有抵抗が低く460μ
Ω・cm程度)、高周波に使用した場合、うず電流
が発生しやすく、いわゆるうず電流損出が生ずる
という欠点を有している。そのため、パーマロイ
を磁気ヘツド用材料として使用するには、パーマ
ロイの薄板を幾層にも積層し、かつ層間を絶縁し
た積層構造とすることが多い。しかしながらこれ
らの薄板を幾層にも積層しかつ層間を絶縁する工
程には多くの労力と時間を要し、この工程を短縮
する材料ないし方法が強く要望されている。 本発明の目的はかかる要望に応えて積層磁気コ
ア材料として高い透磁率を示すとともに、積層構
造とする際に積層する薄板の枚数を減らしてもう
ず電流損出等の欠点が少ない磁気ヘツドコア用素
材を提供することである。 本発明の素材は、70〜90重量%のニツケル
(Ni)、10重量%以下のモリブデン(Mo)、タン
グステン(W)、クロム(Cr)、ニオブ(Nb)、
タンタル(Ta)、チタン(Ti)、銅(Cu)、コバ
ルト(Co)、ケイ素(Si)、マンガン(Mn)及び
アルミニウム(Al)から選ばれた少なくとも一
種の金属並びに残部が鉄からなる合金を二層以上
にクラツドして(合わせ板として)なる磁気ヘツ
ドコア用素材である。 本発明に用いる合金としては、例えばFe−Ni
−Mo、Fe−Ni−Nb、Fe−Ni−Cu−Mo等が好
ましく成分組成としては、Ni70〜90重量%、
Mo、W、Cr、Nb、Ta、Ti、Cu、Co、Si、Mn
及びAlから選ばれた少なくとも一種の金属は10
重量%以下好ましくは0.1〜7重量%であること
が好ましい。 Niは70%未満及び90%を超えると、透磁率が
小さくなり、保磁率が大きくなるので好ましくな
い。また、Mo、W、Cr、Nb、Ta、Ti、Cu、
Co、Si、Mn、Al等の金属は電気抵抗を上げ、透
磁率を改善する成分であり、特に、Nb、Taは耐
摩耗性を向上することができる。しかし、10%を
超えると飽和磁束密度が低下するため実用に供さ
なくなる。 本発明のエレメント・プレートは上記した合金
を熱間加工又は冷間加工により2層以上にクラツ
ドすることにより製造される。層構造は多層であ
ればあるほど磁気ヘツド用材料として優れた特性
を示すが、実用性から考えて2〜3層構造とする
のが有利である。加工は、例えば、熱間又は冷間
で二層以上に積層した合金を圧延することにより
厚さ0.1〜0.3mmの薄板とすることにより行なうこ
とができる。 かくして得られた本発明の薄板はそれ単独で又
は従来の薄板と組合わせて積層することにより磁
気ヘツドコア用材料として使用でき、従来のパー
マロイからなる磁気ヘツドコアに比較して、その
積層枚数を例えば6枚から4枚に減じても優れた
高周波特性を示す。 以上実施例、比較例を掲げて本発明をさらに詳
しく説明するが本発明はこれにより何ら制限を受
けるものではない。なお実施例において%は重量
%を意味する。 実施例 1〜3 Ni77%、Cu5%、Mo4%、Mn0.5%および残部
がFeからなる合金を熱間(1100℃)又は冷間
(常温雰囲気)でクラツドし、圧延して0.1mm厚の
板を得た。比較例として同じ合金をクラツドする
ことなく圧延して0.1mm厚の板を得た。得られた
板について、マツクスウエルブリツジを用いて
100kHzにおける初実効透磁率(μe)を測定した。 結果を第1表に示す。
The present invention relates to a material for a magnetic head core made of an iron-nickel alloy, and more particularly to a material for a magnetic head core made of an iron-nickel alloy clad in two or more layers by hot working or cold working. It is something. The iron-nickel alloy called permalloy has high initial magnetic permeability (μo) and maximum magnetic permeability (μm).
Permalloy has a characteristic of having a low coercive force and is used as a material for magnetic heads in magnetic tape recorders, etc. However, permalloy itself has a low specific resistance of 460 μm.
When used at high frequencies (approximately Ω cm), eddy currents are likely to occur, resulting in so-called eddy current loss. Therefore, in order to use permalloy as a material for a magnetic head, a laminated structure is often created in which a number of thin permalloy plates are laminated and the layers are insulated. However, the process of laminating these thin plates into many layers and insulating the layers requires a lot of labor and time, and there is a strong demand for materials or methods that can shorten this process. The object of the present invention is to meet such demands as a material for magnetic head cores that exhibits high magnetic permeability as a laminated magnetic core material, and that also reduces the number of laminated thin plates when forming a laminated structure and has fewer drawbacks such as eddy current loss. The goal is to provide the following. The material of the present invention includes 70 to 90% by weight of nickel (Ni), 10% by weight or less of molybdenum (Mo), tungsten (W), chromium (Cr), niobium (Nb),
An alloy consisting of at least one metal selected from tantalum (Ta), titanium (Ti), copper (Cu), cobalt (Co), silicon (Si), manganese (Mn) and aluminum (Al) and the balance being iron. This is a material for magnetic head cores made of two or more layers clad (as a laminated plate). Examples of alloys used in the present invention include Fe-Ni
-Mo, Fe-Ni-Nb, Fe-Ni-Cu-Mo, etc. are preferred as component compositions: Ni 70 to 90% by weight,
Mo, W, Cr, Nb, Ta, Ti, Cu, Co, Si, Mn
and at least one metal selected from Al is 10
It is preferably 0.1 to 7% by weight or less. If Ni is less than 70% or more than 90%, the magnetic permeability decreases and the coercivity increases, which is not preferable. Also, Mo, W, Cr, Nb, Ta, Ti, Cu,
Metals such as Co, Si, Mn, and Al are components that increase electrical resistance and improve magnetic permeability, and in particular, Nb and Ta can improve wear resistance. However, if it exceeds 10%, the saturation magnetic flux density decreases, making it impractical. The element plate of the present invention is manufactured by cladding the above-mentioned alloy into two or more layers by hot working or cold working. The more layers the material has, the better the characteristics it exhibits as a material for a magnetic head, but from the viewpoint of practicality, it is advantageous to have a two to three layer structure. The processing can be carried out, for example, by hot or cold rolling an alloy laminated in two or more layers to form a thin plate having a thickness of 0.1 to 0.3 mm. The thus obtained thin plate of the present invention can be used as a material for a magnetic head core by laminating it alone or in combination with a conventional thin plate.Compared to a conventional magnetic head core made of permalloy, the number of laminated sheets is, for example, 6. Excellent high frequency characteristics are exhibited even when the number of sheets is reduced from one to four. The present invention will be described in more detail with reference to Examples and Comparative Examples, but the present invention is not limited thereto in any way. Note that in the examples, % means weight %. Examples 1 to 3 An alloy consisting of 77% Ni, 5% Cu, 4% Mo, 0.5% Mn, and the balance Fe is clad in hot (1100°C) or cold (room temperature atmosphere) and rolled into a 0.1 mm thick material. Got the board. As a comparative example, a 0.1 mm thick plate was obtained by rolling the same alloy without cladding. The obtained board was tested using a Maxwell bridge.
The initial effective permeability (μe) at 100kHz was measured. The results are shown in Table 1.

【表】 実施例 4〜6 合金としてNi80%、Mo5%および残部がFeか
らなるものを用いた他は、実施例1〜3と同様に
して0.2mm厚の板を得た。比較例として、同じ厚
さの単層の板を得た。かくして得られた薄板の初
実効透磁率(μe)を実施例1〜3と同様にして
測定した。 結果を第2表に示した。
[Table] Examples 4 to 6 Plates with a thickness of 0.2 mm were obtained in the same manner as in Examples 1 to 3, except that an alloy consisting of 80% Ni, 5% Mo, and the balance Fe was used. As a comparative example, a single layer plate of the same thickness was obtained. The initial effective magnetic permeability (μe) of the thus obtained thin plate was measured in the same manner as in Examples 1-3. The results are shown in Table 2.

【表】 実施例 7〜9 合金として、Ni80%、Nb7%及び残部Feから
なるものを用いた他は実施例1〜3と同様にして
0.1mm厚の板を製造した。比較例として、同じ合
金とクラツドすることなく同じ厚さに圧延したも
のを製造した。初実効透磁率(μe)を実施例1
〜3と同様にして測定した。 結果を第3表に示した。
[Table] Examples 7 to 9 The same procedure as Examples 1 to 3 was used except that an alloy consisting of 80% Ni, 7% Nb, and the balance Fe was used.
A plate with a thickness of 0.1 mm was manufactured. As a comparative example, one was produced that was rolled to the same thickness without being clad with the same alloy. Example 1 Initial effective permeability (μe)
Measurements were made in the same manner as in 3. The results are shown in Table 3.

【表】 実施例 10〜12 合金として、Ni80%、W4%、Cr3%及び残部
Feからなるものを用いた他は実施例1〜3と同
様にして0.1mm厚の板を製造した。比較例として、
同じ合金をクラツドすることなく同じ厚さに圧延
したものを製造した。初実効透磁率(μe)を実施
例1〜3と同様にして測定した。 結果を第4表に示した。
[Table] Examples 10 to 12 Alloy: 80% Ni, 4% W, 3% Cr, and the balance
A plate having a thickness of 0.1 mm was manufactured in the same manner as in Examples 1 to 3, except that a plate made of Fe was used. As a comparative example,
The same alloy was rolled to the same thickness without cladding. The initial effective permeability (μ e ) was measured in the same manner as in Examples 1-3. The results are shown in Table 4.

【表】 実施例 13〜15 合金として、Ni80%、Ta4%、Ti1%及び残部
Feからなるものを用いた他は実施例1〜3と同
様にして0.1mm厚の板を製造した。比較例として、
同じ合金をクラツドすることなく同じ厚さに圧延
したものを製造した。初実効透磁率(μe)を実施
例1〜3と同様にして測定した。 結果を第5表に示した。
[Table] Examples 13 to 15 Alloy: 80% Ni, 4% Ta, 1% Ti, and the balance
A plate having a thickness of 0.1 mm was manufactured in the same manner as in Examples 1 to 3, except that a plate made of Fe was used. As a comparative example,
The same alloy was rolled to the same thickness without cladding. The initial effective permeability (μ e ) was measured in the same manner as in Examples 1-3. The results are shown in Table 5.

【表】 実施例 16〜18 合金として、Ni80%、Cu5%、Co1%及び残部
Feからなるものを用いた他は実施例1〜3と同
様にして0.1mm厚の板を製造した。比較例として、
同じ合金をクラツドすることなく同じ厚さに圧延
したものを製造した。初実効透磁率(μe)を実施
例1〜3と同様にして測定した。 結果を第6表に示した。
[Table] Examples 16 to 18 Alloys: 80% Ni, 5% Cu, 1% Co, and the balance
A plate having a thickness of 0.1 mm was manufactured in the same manner as in Examples 1 to 3, except that a plate made of Fe was used. As a comparative example,
The same alloy was rolled to the same thickness without cladding. The initial effective permeability (μ e ) was measured in the same manner as in Examples 1-3. The results are shown in Table 6.

【表】 実施例 19〜21 合金として、Ni80%、Si2%、Al2%及び残部
Feからなるものを用いた他は実施例1〜3と同
様にして0.1mm厚の板を製造した。比較例として、
同じ合金をクラツドすることなく同じ厚さに圧延
したものを製造した。初実効透磁率(μe)を実施
例1〜3と同様にして測定した。 結果を第7表に示した。
[Table] Examples 19 to 21 Alloy: 80% Ni, 2% Si, 2% Al, and the balance
A plate having a thickness of 0.1 mm was manufactured in the same manner as in Examples 1 to 3, except that a plate made of Fe was used. As a comparative example,
The same alloy was rolled to the same thickness without cladding. The initial effective permeability (μ e ) was measured in the same manner as in Examples 1-3. The results are shown in Table 7.

【表】【table】

Claims (1)

【特許請求の範囲】[Claims] 1 70〜90重量%のニツケル、10重量%以下のモ
リブデン、タングステン、クロム、ニオブ、タン
タル、チタン、銅、コバルト、ケイ素、マンガン
及びアルミニウムから選ばれた少なくとも一種の
金属並びに残部が鉄からなる合金材を二層以上に
クラツドしてなる磁気ヘツドコア用素材。
1 An alloy consisting of 70 to 90% by weight of nickel, 10% by weight or less of molybdenum, tungsten, chromium, niobium, tantalum, titanium, copper, cobalt, silicon, manganese and aluminum, and the balance consisting of iron. A material for magnetic head cores made of two or more layers of cladding.
JP8806979A 1979-07-13 1979-07-13 Raw material for magnetic head core Granted JPS5612705A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP8806979A JPS5612705A (en) 1979-07-13 1979-07-13 Raw material for magnetic head core

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP8806979A JPS5612705A (en) 1979-07-13 1979-07-13 Raw material for magnetic head core

Publications (2)

Publication Number Publication Date
JPS5612705A JPS5612705A (en) 1981-02-07
JPS6331087B2 true JPS6331087B2 (en) 1988-06-22

Family

ID=13932554

Family Applications (1)

Application Number Title Priority Date Filing Date
JP8806979A Granted JPS5612705A (en) 1979-07-13 1979-07-13 Raw material for magnetic head core

Country Status (1)

Country Link
JP (1) JPS5612705A (en)

Cited By (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPH0434279U (en) * 1990-07-18 1992-03-23

Families Citing this family (4)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
FR2560711B1 (en) * 1984-03-02 1987-03-20 Metalimphy COMPOSITE MAGNETIC CIRCUIT AND METHOD FOR MANUFACTURING SAID CIRCUIT
JP2502633B2 (en) * 1987-11-16 1996-05-29 日産自動車株式会社 Vehicle drive force control device
DE4423622A1 (en) * 1994-07-06 1996-01-11 Vacuumschmelze Gmbh Total current transformer for electronic protective devices
US6744342B2 (en) 2000-07-27 2004-06-01 Decristofaro Nicholas J. High performance bulk metal magnetic component

Cited By (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPH0434279U (en) * 1990-07-18 1992-03-23

Also Published As

Publication number Publication date
JPS5612705A (en) 1981-02-07

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