JPS6326808A - Magnetic head - Google Patents

Magnetic head

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Publication number
JPS6326808A
JPS6326808A JP17122286A JP17122286A JPS6326808A JP S6326808 A JPS6326808 A JP S6326808A JP 17122286 A JP17122286 A JP 17122286A JP 17122286 A JP17122286 A JP 17122286A JP S6326808 A JPS6326808 A JP S6326808A
Authority
JP
Japan
Prior art keywords
magnetic
divided piece
magnetic flux
magnetic head
permeability
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.)
Pending
Application number
JP17122286A
Other languages
Japanese (ja)
Inventor
Junichi Horikawa
順一 堀川
Kazuhiko Okita
和彦 沖田
Toshiharu Hoshi
星 敏春
Haruo Saji
佐治 晴夫
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.)
Panasonic Holdings Corp
Original Assignee
Matsushita Electric Industrial 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 Matsushita Electric Industrial Co Ltd filed Critical Matsushita Electric Industrial Co Ltd
Priority to JP17122286A priority Critical patent/JPS6326808A/en
Publication of JPS6326808A publication Critical patent/JPS6326808A/en
Pending legal-status Critical Current

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  • Magnetic Heads (AREA)

Abstract

PURPOSE:To increase the leakage magnetic flux and to prevent the permeability from being deteriorated by forming a magnetic head by split pieces made of two kinds of ferrite materials with different saturation density and permeability. CONSTITUTION:The magnetic head core forming a main magnetic path consists of two split pieces 1a, 1b to form an operating gap 2. A wiring window 3 is formed in the inside of the gap 2. In utilizing the window 3, an electromagnetic conversion wire 6 is applied to the core 1. The split piece 1a is made of a ferrite material having a higher saturated magnetic flux density then that of the split piece 1b, and the split piece 1b is made by a ferrite material having a higher permeability then that for the split piece 1a. In the magnetic recording/ reproduction using a high coercive force medium, the leakage magnetic flux near the operating gap generated at recoding is increased and an excellent reproduction output is obtained without lowering the permeability.

Description

【発明の詳細な説明】 産業上の利用分野 本発明は、磁気記録再生装置に用いる磁気ヘッドに関す
るものである。
DETAILED DESCRIPTION OF THE INVENTION Field of Industrial Application The present invention relates to a magnetic head used in a magnetic recording/reproducing device.

従来の技術 近年、磁気ヘッドは、VTR,オーディオテープレコー
ダ、フロッピーディスク、ハートティスフ、磁気カード
などを始めとする磁気記録分野で盛んに利用されている
。以下、第3図及び第4図を参照しながら従来の磁気ヘ
ッドの概要について説明する。
2. Description of the Related Art In recent years, magnetic heads have been widely used in the field of magnetic recording, including VTRs, audio tape recorders, floppy disks, heart disks, magnetic cards, and the like. Hereinafter, an overview of the conventional magnetic head will be explained with reference to FIGS. 3 and 4.

第4図に示すように主磁器を形成する磁気ヘッドコア2
1は通常、第3図に示すように2つの分割片21a、2
1bよりなり、作動ギャップ対峠部22により作動ギャ
ップ23が形成さ牡ている。
As shown in Fig. 4, the magnetic head core 2 forming the main ceramic
1 usually has two divided pieces 21a and 2 as shown in FIG.
1b, and an operating gap 23 is formed by the operating gap pair portion 22.

作動ギヤノブ23は単なる空隙でも良いが、機械的安定
性を得るため、通常はガラスなどの磁気的絶縁材料が狭
−1している。作動ギヤノブ23の内方には巻線窓24
が形成され、この巻線窓2,1は磁気へラドコア21を
構成する分割片21a、21bの少なくとも一方に形成
されている。磁気へラドコア21には巻線官24を利用
して電磁変換用巻線25が施されている。
The actuating gear knob 23 may be a simple gap, but is usually filled with a magnetically insulating material such as glass to provide mechanical stability. There is a winding window 24 inside the operating gear knob 23.
The winding windows 2, 1 are formed in at least one of the divided pieces 21a, 21b constituting the magnetic helad core 21. An electromagnetic conversion winding 25 is provided on the magnetic helad core 21 using a winding member 24 .

周知のように、磁気記録においては、強磁性体を含有す
る薄層からなる記録媒体表面を磁気ヘッドの記録再生ト
ラック26により走査し、上記作動ギャップ23近傍の
漏れ磁束によ磁化ず右記録磁界により、上記記録媒体に
入力信号に対応した残留磁化のパターンを記録する。再
生においては、磁気ヘッドの記録再生トラック26によ
り上記記録媒体表面を走査し、上記残留磁化の状態を検
知することにより行なう。
As is well known, in magnetic recording, the surface of a recording medium made of a thin layer containing a ferromagnetic material is scanned by a recording/reproducing track 26 of a magnetic head, and the leakage magnetic flux near the working gap 23 causes the right recording magnetic field to remain unmagnetized. As a result, a residual magnetization pattern corresponding to the input signal is recorded on the recording medium. Reproduction is performed by scanning the surface of the recording medium with the recording/reproducing track 26 of the magnetic head and detecting the state of the residual magnetization.

最近、磁気記録密度を向上させるために、記録媒体の高
抗磁力化が活発に進められている。周知のように、記録
媒体の抗磁力を高くすると、記録する磁気ヘッドの漏れ
磁束をより大きくするために磁気へラドコアの飽和磁束
密度を大きくする必要がある。磁気ヘッドコア材料とし
てよく用いられているMn−Zn フェライトの飽和磁
束密度は4000〜5000ガウスであるが、よシ高い
飽和磁束密度を実現するための三元組成の検討が盛んに
進めらn1飽和磁束密度が6000ガウスを越える材料
が発表されておシ(例えば、D、5TOPPELS  
et  al、JMMM  37  (1983)12
3−1301あるいは堀用他 1985年 秋季応用物
理学会学術講演会講演予稿集4a−ZE−8など)、磁
気ヘッドへの応用が考えられている。
Recently, efforts have been made to increase the coercive force of recording media in order to improve magnetic recording density. As is well known, when the coercive force of the recording medium is increased, it is necessary to increase the saturation magnetic flux density of the magnetic helad core in order to increase the leakage flux of the magnetic head for recording. The saturation magnetic flux density of Mn-Zn ferrite, which is often used as a magnetic head core material, is 4,000 to 5,000 Gauss, but studies on ternary compositions to achieve even higher saturation magnetic flux density are actively progressing. Materials with a density exceeding 6000 Gauss have been announced (for example, D, 5TOPPELS).
et al, JMMM 37 (1983) 12
3-1301 or Horiyo et al. 1985 Autumn Academic Conference of Japan Society of Applied Physics Proceedings 4a-ZE-8), applications to magnetic heads are being considered.

発明が解決しようとする問題点 しかし、磁気へラドコア21を構成する分割片21a 
、21bに上記のような6000ガウスを越える高飽和
磁束密度のMn−Znフェライトを用いた場合、従来よ
く用いられていた飽和磁束密度4000〜5000ガウ
スのMn’Znフzライトよりなる磁気ヘッドコア21
に比べて、再生出力が20%以上低下するという問題が
ある。飽和磁束密度が高く、記録を行うのに有利であり
ながら再生出力が低下するというこの現象の原因として
は、高飽和磁束密度のM n −Z nフェライト材料
を用いた磁気へラドコアの透磁率が低下しているため、
再生時の電磁変換効率が低下するものと考えられる。
Problems to be Solved by the Invention However, the divided pieces 21a constituting the magnetic herad core 21
, 21b, when Mn-Zn ferrite with a high saturation magnetic flux density exceeding 6000 Gauss as described above is used, the magnetic head core 21 made of Mn'Zn ferrite with a saturation magnetic flux density of 4000 to 5000 Gauss, which has been commonly used in the past.
There is a problem in that the playback output is reduced by 20% or more compared to the above. The reason for this phenomenon, in which the reproduction output decreases even though the saturation magnetic flux density is high and is advantageous for recording, is that the magnetic permeability of the magnetic herad core made of Mn-Zn ferrite material with high saturation magnetic flux density is low. Because it is decreasing,
It is thought that the electromagnetic conversion efficiency during reproduction is reduced.

本発明は、上記従来例の問題を解決するもので、記録に
有利となるように漏れ磁束を大きくすることができ、し
かも透磁率低下を生じないようにして良好な再生出力を
得ることができるようにした磁気ヘッドを提供しようと
するものである。
The present invention solves the above-mentioned problems of the conventional example, and makes it possible to increase the leakage magnetic flux to be advantageous for recording, and also to obtain good reproduction output without causing a decrease in magnetic permeability. It is an object of the present invention to provide such a magnetic head.

問題点を解決するための手段 そして上記問題点を解決するための本発明の技術的な手
段は、磁気ヘッドコアが作動ギャップ対峠部を有し、主
磁路を形成する第1と第2の2つの分割片よりなり、第
1の分割片が第2の分割片よりも高い飽和磁束密度を有
するフェライト材料により形成され、第2の分割片が第
1の分割片よシも高い透磁率を有するフェライト材料に
より形成さnたものである。
Means for solving the problems and the technical means of the present invention for solving the above problems are that the magnetic head core has an operating gap pair part and a first and second part forming a main magnetic path. It consists of two divided pieces, the first divided piece is made of a ferrite material having a higher saturation magnetic flux density than the second divided piece, and the second divided piece has a higher magnetic permeability than the first divided piece. It is made of a ferrite material having the following characteristics.

作用 本発明は上記構成により、高抗磁力媒体を使用した磁気
記録再生において、記録時に発生する作動ギヤノブ近傍
の漏れ磁束を大きくし、しかも透磁率を低下せず、良好
な再生出力を得ることができる。
Effect of the Invention With the above configuration, the present invention can increase the leakage magnetic flux near the operating gear knob that occurs during recording in magnetic recording and reproduction using a high coercive force medium, and can obtain good reproduction output without reducing magnetic permeability. can.

実施例 以下、本発明の実施例について図面を参照しながら説明
する。
EXAMPLES Hereinafter, examples of the present invention will be described with reference to the drawings.

第1図は本発明の一実施例における磁気ヘッドの斜視図
である。
FIG. 1 is a perspective view of a magnetic head in one embodiment of the present invention.

第1図に示すように主磁路を形成する磁気へラドコア1
は第1と第2の2つの分割片1a、lbよりなり、作動
ギャップ対峠部にガラススパッタ膜よりなる作動ギャッ
プ2が形成されている。作動ギャップ2の内方には巻線
窓3が形成され、この巻線窓3は磁気へラドコア1を構
成する第1と第2の分割片1a11bの少なくとも一方
に形成されている。第1と第2の分割片1a、1bにお
ける作動ギヤツブ3の両側部には作動ギャップ3と記録
再生トラック4の機械的強度を保つための補強ガラス5
a、5bが設けられている。磁気へラドコア1には巻線
窓3を利用して電磁変換用巻線6が施されている。上記
第1の分割片1aは飽和磁束密度6300ガウスのM 
n −Z n フェライト材料により形成され、第2の
分割片1bは飽和磁束密度5000ガウスで、上記第1
の分割片1bのM n −Z nフェライト材料よりも
透磁率が使用周波数帯である5MHzにおいて、20%
高いMn−Znフェライト材料により形成されている。
Magnetic helad core 1 forming the main magnetic path as shown in Figure 1
consists of two divided pieces 1a and 1b, a first and a second, and a working gap 2 made of a glass sputtered film is formed at the pass portion of the working gap. A winding window 3 is formed inside the working gap 2, and this winding window 3 is formed on at least one of the first and second divided pieces 1a11b constituting the magnetic herad core 1. On both sides of the operating gear 3 in the first and second divided pieces 1a and 1b, there is a reinforcing glass 5 for maintaining the mechanical strength of the operating gap 3 and the recording/reproducing track 4.
a and 5b are provided. An electromagnetic conversion winding 6 is provided on the magnetic helad core 1 using a winding window 3. The first divided piece 1a has a saturation magnetic flux density of 6300 Gauss.
n - Z n ferrite material, the second divided piece 1b has a saturation magnetic flux density of 5000 Gauss, and has a saturation magnetic flux density of 5000 Gauss,
The magnetic permeability is 20% higher than that of the M n -Z n ferrite material of the divided piece 1b at 5 MHz, which is the frequency band used.
It is made of high Mn-Zn ferrite material.

上記実施例の磁気ヘッドの記録再生特性を比較するため
の比較実施例として、第1と第2の分割片1aと1bを
それぞれ飽和磁束密度5000ガウスで、同じ透磁率の
Mn−Znフェライトによシ形成し、その他は上記実施
例と同一に構成した。
As a comparative example for comparing the recording and reproducing characteristics of the magnetic head of the above example, the first and second divided pieces 1a and 1b were each made of Mn-Zn ferrite with a saturation magnetic flux density of 5000 Gauss and the same magnetic permeability. The structure was otherwise the same as that of the above embodiment.

そして本発明実施例と比較実施例を用い、抗磁力143
0エルステツドの塗布型金属テープへの記録再生特性を
相対速度5.8 m / secで試験した結果は第2
図に示す通シである。第2図において、7は本発明実施
例による磁気ヘッドの再生出力を示し、8は比較実施例
による磁気ヘッドの再生出力を示す。なお、第2図の縦
軸は本発明実施例による磁気ヘッドの0.5MHzにお
ける再生出力電圧を規準として規格化しである。第2図
に示した試験結果から明らかなように、本発明実施例に
よる磁気ヘッドは、高抗磁力媒体を使用する際に高再生
出力を得ることができた。
Then, using the present invention example and the comparative example, coercive force 143
The results of testing the recording and reproducing characteristics of 0 Oersted coated metal tape at a relative speed of 5.8 m/sec are as follows.
This is the passage shown in the figure. In FIG. 2, numeral 7 indicates the reproduction output of the magnetic head according to the embodiment of the present invention, and numeral 8 indicates the reproduction output of the magnetic head according to the comparative example. Note that the vertical axis in FIG. 2 is normalized based on the reproduction output voltage at 0.5 MHz of the magnetic head according to the embodiment of the present invention. As is clear from the test results shown in FIG. 2, the magnetic head according to the example of the present invention was able to obtain high reproduction output when using a high coercive force medium.

上記本発明実施例の構成で、第1の分割片1aに飽和磁
束密度が5000ガウスから6800ガウスまでの各種
M n −Z nフェライト材料を用い、抗磁力143
0エルステツドの塗布型金属テープへの記録再生特性に
ついて相対速度5.8m/secで試験した。その結果
、飽和磁束密度が5800ガウスよりも小さい材料では
、第2図に示す比較実施例8の出力値との差が10%よ
υも小さく、優位性は認められなかった。従って本発明
においては、第1の分割片1aに飽和磁束密度が580
0〜6800ガウスとなるMn−Znフェライト材料を
用いるのが望ましい。
In the configuration of the embodiment of the present invention described above, various Mn-Zn ferrite materials having a saturation magnetic flux density of 5000 Gauss to 6800 Gauss are used for the first divided piece 1a, and the coercive force is 143.
The recording and reproducing characteristics of a coated metal tape of 0 oersted were tested at a relative speed of 5.8 m/sec. As a result, for materials with a saturation magnetic flux density smaller than 5800 Gauss, the difference from the output value of Comparative Example 8 shown in FIG. 2 was as small as 10%, and no superiority was recognized. Therefore, in the present invention, the first divided piece 1a has a saturation magnetic flux density of 580
It is desirable to use a Mn-Zn ferrite material with a 0 to 6800 Gauss.

また上記本発明実施例の構成で、第2の分割片1bに透
磁率が第1の分割片1aよりも10%〜40%高い種々
のMn−Znフェライト材料を用い、抗磁力1430エ
ルステツドの塗布型金属テープへの記録再生特性につい
て相対速度5.8m/secで試験した。その結果、第
1と第2の分割片1aと1bの透磁率の差が15%よシ
小さい場合には、第2図に示す比較実施例8の出力値と
の差が10%よりも小さく、優位性は認められなかった
。従って本発明においては、第2の分割片1bの透磁率
が第1の分割片1aの透磁率よりも15%〜40%大き
いMn−Znフェライト材料を用いるのが望ましい。
In addition, in the configuration of the embodiment of the present invention, the second segment 1b is made of various Mn-Zn ferrite materials whose magnetic permeability is 10% to 40% higher than that of the first segment 1a, and a coercive force of 1430 oersted is applied. The recording and reproducing characteristics of the molded metal tape were tested at a relative speed of 5.8 m/sec. As a result, when the difference in magnetic permeability between the first and second divided pieces 1a and 1b is smaller than 15%, the difference from the output value of Comparative Example 8 shown in FIG. 2 is smaller than 10%. , no superiority was observed. Therefore, in the present invention, it is desirable to use an Mn-Zn ferrite material in which the magnetic permeability of the second divided piece 1b is 15% to 40% higher than that of the first divided piece 1a.

さらに本発明実施例の構成で、第1の分割片1aに飽和
磁束密度が5000ガウスから6800ガウスまでの各
種Mn−Zn フェライト材料を用い、第2の分割片1
bに飽和磁束密度が第1の分割片1aよりも200から
1000ガウス小さい各種MnZnフェライト材料を用
いた。この比較実施例として、第2の分割片1bと同じ
M n −Z nフェライト材料によシ第1の分割片1
aを形成した。これら本発明実施例と比較実施例を抗磁
力11130 エルステッドの塗布型金属テープへの記
録再生特性について相対速度5.8 m / secで
比較試験した。その結果、第1と第2の分割片1aと1
bの飽和磁束密度の差が500ガウスより小さいと、第
1と第2の分割片1aと1bに同じ〜1n−Znフェラ
イト材料のみを用いた比較実施例との出力の差が10%
よシも小さくなり、優位性が認められなかった。従って
第1の分割片1aに用いるMn−Znフェライト材料と
第2の分割片1bに用いるMn −Z n フェライト
材料の飽和磁束密度の差が500〜1000ガウスにな
るように選定するのが望ましい。
Further, in the configuration of the embodiment of the present invention, various Mn-Zn ferrite materials having a saturation magnetic flux density of 5000 Gauss to 6800 Gauss are used for the first divided piece 1a, and the second divided piece 1
Various MnZn ferrite materials whose saturation magnetic flux density is 200 to 1000 Gauss smaller than that of the first divided piece 1a were used for b. As a comparative example, the first divided piece 1 is made of the same M n -Z n ferrite material as the second divided piece 1 b.
A was formed. These inventive examples and comparative examples were tested for recording and reproducing characteristics on a coated metal tape with a coercive force of 11130 Oersted at a relative speed of 5.8 m/sec. As a result, the first and second divided pieces 1a and 1
When the difference in the saturation magnetic flux density of b is smaller than 500 Gauss, the difference in output from the comparative example in which only the same ~1n-Zn ferrite material is used for the first and second divided pieces 1a and 1b is 10%.
Yoshi also became smaller and his superiority was no longer recognized. Therefore, it is desirable to select the Mn-Zn ferrite material used for the first divided piece 1a and the Mn-Zn ferrite material used for the second divided piece 1b so that the difference in saturation magnetic flux density is 500 to 1000 Gauss.

発明の効果 以上述べたように本発明によnば、磁気へラドコアを第
1と第2の2つの分割片により構成し、第1の分割片を
第2の分割片よりも高い飽和磁束密度を有するフェライ
ト材料により形成し、第2の分割片を第1の分割片より
も高い透磁率を有するフェライト材料により形成してい
るので、高抗磁力媒体を使用した磁気記録再生において
、記録時に発生する作動ギャップ近傍の漏れ磁束を太き
くシ、シかも透磁率を低下させず、良好な再生出力を得
ることができる。
Effects of the Invention As described above, according to the present invention, the magnetic herad core is composed of two divided pieces, the first and second divided pieces, and the first divided piece has a higher saturation magnetic flux density than the second divided piece. Since the second divided piece is made of a ferrite material that has a higher magnetic permeability than the first divided piece, there is no possibility of occurrence during recording during magnetic recording and reproduction using a high coercive force medium. By increasing the leakage magnetic flux near the working gap, good reproduction output can be obtained without reducing the magnetic permeability.

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

第1図は本発明の一実施例における磁気ヘッドの斜視図
、第2図は本発明実施例と比較実施例の再生出力の周波
数特性図、第3図及び第4図は従来の磁気ヘッドを示し
、第3図は製造途中の斜視図、第4図は製造完成状態の
斜視図である。 1・・・磁気ヘッドコア、1a・・・第1の分割片、1
b・・・第2の分割片、2・・・作動ギャップ、3・・
・巻線窓、4・・・記録再生トラック、5a、5b・・
・補強ガラス゛、6・・・電磁変換用巻線。 代理人の氏名 弁理士 中 尾 敏 男 ほか1名Mx
  図 第2図 關”21−4ダ(MHz)
FIG. 1 is a perspective view of a magnetic head according to an embodiment of the present invention, FIG. 2 is a frequency characteristic diagram of reproduction output of an embodiment of the present invention and a comparative example, and FIGS. 3 and 4 are diagrams of a conventional magnetic head. 3 is a perspective view of the product in the middle of manufacture, and FIG. 4 is a perspective view of the product in the completed state. 1... Magnetic head core, 1a... First divided piece, 1
b...Second divided piece, 2...Operating gap, 3...
・Winding window, 4...recording/reproducing track, 5a, 5b...
・Reinforced glass ゛, 6...Winding for electromagnetic conversion. Name of agent: Patent attorney Toshio Nakao and 1 other Mx
Figure 2: 21-4 da (MHz)

Claims (4)

【特許請求の範囲】[Claims] (1)磁気ヘッドコアが作動ギャップ対峠部を有し、主
磁路を形成する第1と第2の2つの分割片よりなり、第
1の分割片が第2の分割片よりも高い飽和磁束密度を有
するフェライト材料により形成され、第2の分割片が第
1の分割片よりも高い透磁率を有するフェライト材料に
より形成されていることを特徴とする磁気ヘッド。
(1) The magnetic head core has an operating gap pair part and consists of two divided pieces, a first and a second divided piece, forming a main magnetic path, and the first divided piece has a higher saturation magnetic flux than the second divided piece. A magnetic head characterized in that it is formed of a ferrite material having a high density, and the second divided piece is formed of a ferrite material that has a higher magnetic permeability than the first divided piece.
(2)第1の分割片の飽和磁束密度が5800ガウス以
上である特許請求の範囲第1項記載の磁気ヘッド。
(2) The magnetic head according to claim 1, wherein the first divided piece has a saturation magnetic flux density of 5,800 Gauss or more.
(3)第2の分割片の透磁率が第1の分割片の透磁率よ
りも使用周波数帯で、15%以上大きい特許請求の範囲
第1項記載の磁気ヘッド。
(3) The magnetic head according to claim 1, wherein the magnetic permeability of the second divided piece is 15% or more higher than the magnetic permeability of the first divided piece in the operating frequency band.
(4)第1の分割片と第2の分割片の飽和磁束密度の差
が500ガウス以上である特許請求の範囲第1項記載の
磁気ヘッド。
(4) The magnetic head according to claim 1, wherein the difference in saturation magnetic flux density between the first divided piece and the second divided piece is 500 Gauss or more.
JP17122286A 1986-07-21 1986-07-21 Magnetic head Pending JPS6326808A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP17122286A JPS6326808A (en) 1986-07-21 1986-07-21 Magnetic head

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP17122286A JPS6326808A (en) 1986-07-21 1986-07-21 Magnetic head

Publications (1)

Publication Number Publication Date
JPS6326808A true JPS6326808A (en) 1988-02-04

Family

ID=15919306

Family Applications (1)

Application Number Title Priority Date Filing Date
JP17122286A Pending JPS6326808A (en) 1986-07-21 1986-07-21 Magnetic head

Country Status (1)

Country Link
JP (1) JPS6326808A (en)

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