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JPS61194607A - magnetic head - Google Patents

magnetic head

Info

Publication number
JPS61194607A
JPS61194607A JP3263085A JP3263085A JPS61194607A JP S61194607 A JPS61194607 A JP S61194607A JP 3263085 A JP3263085 A JP 3263085A JP 3263085 A JP3263085 A JP 3263085A JP S61194607 A JPS61194607 A JP S61194607A
Authority
JP
Japan
Prior art keywords
head
noise
core
less
magnetic head
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
JP3263085A
Other languages
Japanese (ja)
Inventor
Yoshihiro Shiroishi
芳博 城石
Kazuo Shiiki
椎木 一夫
Takayuki Kumasaka
登行 熊坂
Moichi Otomo
茂一 大友
Takeo Yamashita
武夫 山下
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.)
Hitachi Ltd
Original Assignee
Hitachi 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 Hitachi Ltd filed Critical Hitachi Ltd
Priority to JP3263085A priority Critical patent/JPS61194607A/en
Publication of JPS61194607A publication Critical patent/JPS61194607A/en
Pending legal-status Critical Current

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  • Magnetic Heads (AREA)

Abstract

PURPOSE:To reduce a head resistance which is the main cause of a thermal noise and to reduce a head noise even when a head is made into multicoil by making the core width smaller. CONSTITUTION:The core width of a head coil window part in at least one head core part is set to a value range more than 0.05mm and less than 0.7mm, and the number of coils are more than 25. Thus the thermal noise due to the practical resistance of the head can be reduced, whereby a noise level can lie within the range of a conventional head even if the number of head coils is set to more than 25.

Description

【発明の詳細な説明】 〔発明の利用分野〕 本発明はフロッピ装置などの高密度記録用の磁気ヘッド
に係り、特にヘッド熱雑音の小さな磁気ヘッドに関する
DETAILED DESCRIPTION OF THE INVENTION [Field of Application of the Invention] The present invention relates to a magnetic head for high-density recording in floppy devices and the like, and particularly to a magnetic head with low head thermal noise.

〔発明の背景〕[Background of the invention]

従来、磁気ヘッドに関しては、再生出力の向上。 Conventionally, with regard to magnetic heads, improvements in playback output.

摺動ノイズ、変調ノイズの低減等について検討がなされ
、宮カノイズ比の向上がなされて来た。一方、ヘッド自
身に帰因するノイズには、テープ摺動雑音、熱雑音など
があるが(これについては、松本光功著、「磁気記録J
 pisa、共立出版に記載されている。これらは媒体
ノイズ、アンプノイズなどに比べて小さく、従来あまり
配慮されてはいなかった。ところが近年、記録密度の向
上と共に、トラック幅が狭くなり、再生出力の不足を補
うため、ヘッドを多巻線化することが必要になって来た
。このとき1発明者らの予備的な実験によると、第9図
に示すようにヘッドの熱雑音は巻線数と共に増大し、ヘ
ッド媒体、アンプ系のノイズの大部分を占めてしまう恐
れがあることが明らかになった。このためこのヘッド熱
雑音を低減することは非常に重要である。
Studies have been conducted on reducing sliding noise, modulation noise, etc., and efforts have been made to improve the noise ratio. On the other hand, noise attributable to the head itself includes tape sliding noise and thermal noise.
pisa, published by Kyoritsu Shuppan. These are smaller than media noise, amplifier noise, etc., and have not been given much consideration in the past. However, in recent years, as recording density has improved, track width has become narrower, and in order to compensate for the lack of reproduction output, it has become necessary to increase the number of windings in the head. At this time, according to preliminary experiments conducted by the inventors, the thermal noise of the head increases with the number of windings, as shown in Figure 9, and there is a possibility that it may account for most of the noise of the head medium and amplifier system. It became clear. Therefore, it is very important to reduce this head thermal noise.

〔発明の目的〕[Purpose of the invention]

本発明の目的は、ヘッドの熱雑音が小さな、高密度記録
用磁気ヘッドを提供することにある。
An object of the present invention is to provide a magnetic head for high-density recording in which the head has low thermal noise.

〔発明の概要〕[Summary of the invention]

発明者らは、ヘッド熱雑音とヘッド寸法、ヘッド形状、
を線数との関係を詳細に検討し、ヘッド熱雑音はヘッド
巻線部でのヘッドコア体積を小さくすることで著しく低
減できることを見い出した。
The inventors investigated head thermal noise, head dimensions, head shape,
We investigated the relationship between the number of wires and the number of wires in detail, and found that head thermal noise can be significantly reduced by reducing the head core volume at the head winding section.

すなわち1巻線部周辺におけるコア幅を0.7閣以下、
より望ましくは0.5an以下とするものである。ここ
で、コアの機械的強度を保つためには。
In other words, the core width around the first winding is 0.7 mm or less,
More preferably, it is 0.5 an or less. Here, in order to maintain the mechanical strength of the core.

このコア幅は0.0511111以上、より望ましくは
0.1m以上であることが望ましい。さらに、ヘッドの
ギャップ深さを20μm以下1μm以上。
The core width is desirably 0.0511111 or more, more preferably 0.1 m or more. Furthermore, the head gap depth is 20 μm or less and 1 μm or more.

より望ましくは10μm以下2μm以上とすることでノ
イズの低減と共に記録再生効率も向上することができる
。なお、ここでギャップ深さに対する下限は、耐摺動に
対する信頼性を保つために必要である。
More preferably, by setting the thickness to 10 μm or less and 2 μm or more, it is possible to reduce noise and improve recording and reproducing efficiency. Note that the lower limit for the gap depth is necessary here in order to maintain reliability with respect to sliding resistance.

〔発明の実施例〕[Embodiments of the invention]

以下本発明の一実施例を第1図により説明する。 An embodiment of the present invention will be described below with reference to FIG.

すなわちM n −Z nフェライト単結晶を磁気コア
材とし、各部寸法Cコア側面コア幅t、Iコア側面コア
幅U、コアリア部コア幅V及びギャップ深さg、を表1
に示す値としたものである。ここでコア厚Tはいずれも
50,100,150,200゜400μmの4種とし
、ヘッド巻線は25,30゜50.70,100の5種
とした。
That is, M n -Z n ferrite single crystal is used as the magnetic core material, and the dimensions of each part C core side core width t, I core side core width U, core rear part core width V and gap depth g are shown in Table 1.
The values shown are as follows. Here, the core thickness T was set to four types: 50, 100, 150, 200° and 400 μm, and the head winding was set to five types: 25, 30°, 50.70, and 100°.

第2図には別の実施例を示す。すなわちM n −Zn
フェライト基板上に高飽和磁束密度磁性合金を形成した
リングヘッドで、その各部寸法は表2に示した通りであ
る。
FIG. 2 shows another embodiment. That is, M n −Zn
This is a ring head in which a high saturation magnetic flux density magnetic alloy is formed on a ferrite substrate, and the dimensions of each part are as shown in Table 2.

表   1 表  2 ここで、高飽和磁束密度磁性合金としては、膜厚40μ
mのCo −Z r −N b系非晶質磁性合金などの
非晶質磁性合金を用いたが、Fe−Aρ−8i合金、N
i−Fe合金、Fe−5i−Ru合金や、それらの積層
膜などでも良く、基板もAQ、03−TiC,非磁性Z
n−フェライトなどの非磁性基板でも良い。
Table 1 Table 2 Here, as a high saturation magnetic flux density magnetic alloy, the film thickness is 40 μm.
We used an amorphous magnetic alloy such as Co-Zr-Nb-based amorphous magnetic alloy of m, but Fe-Aρ-8i alloy, N
i-Fe alloy, Fe-5i-Ru alloy, or a laminated film of these may be used, and the substrate may also be AQ, 03-TiC, or non-magnetic Z.
A nonmagnetic substrate such as n-ferrite may also be used.

本実施例によれば、ヘッドの実効的な抵抗に基づく熱ノ
イズを低減できるので、ヘッド巻線数を25以上に多巻
化してもノイズレベルを従来ヘッド程度に抑えることが
できる。第3図には、第1図の構造でヘッドギャップ深
さを20μm、uを0.7m 、v=0.6mm 、T
を0.15mとし。
According to this embodiment, thermal noise based on the effective resistance of the head can be reduced, so even if the number of head windings is increased to 25 or more, the noise level can be suppressed to the level of a conventional head. Figure 3 shows the structure shown in Figure 1 with a head gap depth of 20 μm, u = 0.7 m, v = 0.6 mm, and T.
is 0.15m.

tを0.1w〜2−と変えた場合のヘッドノイズを示す
、コア幅tを0.7mm以下、より望ましくは0.5閣
とすることでヘッドノイズを低減できることがわかる。
It can be seen that the head noise can be reduced by setting the core width t to 0.7 mm or less, more preferably 0.5 mm, which indicates the head noise when t is changed from 0.1 w to 2 -.

t=0.5mm 、u=0.6rm+ 。t=0.5mm, u=0.6rm+.

T=0.2mmとしてVを変えた場合、あるいは、t=
0.4+m 、 v=0.8+m 、 T=0.13m
oとしてUを変えた場合も、第2図の構造の場合も同様
の結果が得られた。ただしt g u @ Vの各幅を
0.1mm以下にするとコアの機械的強度が著しく低下
し、実用上好ましくなかった。
If T=0.2mm and V is changed, or t=
0.4+m, v=0.8+m, T=0.13m
Similar results were obtained when U was changed as o and in the case of the structure shown in FIG. However, when each width of t g u @ V was set to 0.1 mm or less, the mechanical strength of the core decreased significantly, which was not preferred in practice.

第4図には、t=0.4IIIII、 u=o、4mm
 、 v= 0 、7 mm 、 T = 0 、14
 m とし、ギャップ深さを1μm〜100μmと変え
た第2図に示した構造のヘッドの熱ノイズと、ビデオテ
ープを用いて記録再生を行った時の再生出力を示す。こ
れから、ギャップ深さを20μm以下とするとノイズは
著しく小さくなり、さらに10μm以下にすると再生出
力も著しく増大することがわかる。ただしギャップ深さ
を1〜2μm以下にすると、摩耗のためヘッド寿命が短
かくなり、実用上好ましくない。
In Figure 4, t=0.4III, u=o, 4mm
, v = 0, 7 mm, T = 0, 14
The thermal noise of the head having the structure shown in FIG. 2 with the gap depth changed from 1 μm to 100 μm and the reproduction output when recording and reproduction is performed using a video tape are shown. From this, it can be seen that when the gap depth is set to 20 μm or less, the noise is significantly reduced, and when the gap depth is set to 10 μm or less, the reproduction output is also significantly increased. However, if the gap depth is less than 1 to 2 μm, the life of the head will be shortened due to wear, which is not preferred in practice.

以上の結果は、第1図の構造のヘッドでも同様であった
The above results were the same for the head having the structure shown in FIG.

一方、第5図にはu=0.6mm+ 、t=0.4mm
 。
On the other hand, in Fig. 5, u=0.6mm+, t=0.4mm
.

v=0.6m++ とじ、Tを50〜1000μmと変
えた場合における、第2図に示した構造のヘッドのノイ
ズを示す。コア厚を400μm以下とするとノイズは低
減できることがわかる。ただし30μm以下とすると強
度が低下するのであまり望ましくはない。
The noise of the head having the structure shown in FIG. 2 is shown when v=0.6m++ and T is varied from 50 to 1000 μm. It can be seen that noise can be reduced when the core thickness is 400 μm or less. However, if the thickness is less than 30 μm, the strength will decrease, which is not very desirable.

第6図、第7図にはそれぞれ本発明の第1図。FIG. 6 and FIG. 7 respectively show the first diagram of the present invention.

第2図の構造のヘッドチップを非磁性スライダに埋め込
んだ磁気ディスク、フロッピディスク装置用のヘッドの
実施例を示す。いずれの場合も従来の大型ヘッドに比べ
てノイズは小さくなったが、アンプノイズ、媒体ノイズ
との関係で、特に巻線数を25とした時に装置のS/N
比が著しく向上した。第7図のヘッドチップとしては、
各コア幅寸法、ギャップ深さコア厚が表2に示した値で
An embodiment of a head for a magnetic disk or floppy disk device in which a head chip having the structure shown in FIG. 2 is embedded in a non-magnetic slider is shown. In both cases, the noise was lower than that of conventional large heads, but due to the relationship with amplifier noise and media noise, the S/N of the device was particularly high when the number of windings was set to 25.
The ratio has improved significantly. As the head chip in Figure 7,
Each core width dimension, gap depth and core thickness are the values shown in Table 2.

コア形状を第8図に示した構造のものでもよい。The core may have a structure shown in FIG. 8.

〔発明の効果〕〔Effect of the invention〕

以上のように、コア幅を小さくするという本発明によれ
ば、熱ノイズの最大の原因であるヘッド抵抗を低減でき
るため、ヘッドを多巻線化した場合にもヘッドノイズ分
を小さくできる。特に、アンプノイズ、媒体ノイズとの
兼ね合いから、巻線数を25以上とした時に本発明の効
果は著′しい。
As described above, according to the present invention in which the core width is reduced, the head resistance, which is the biggest cause of thermal noise, can be reduced, so that even when the head has multiple windings, the head noise can be reduced. In particular, the effects of the present invention are remarkable when the number of windings is set to 25 or more in consideration of amplifier noise and medium noise.

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

第1図、第2図はそれぞれ本発明の実施例としてのヘッ
ドの上面、側面図、第6図、第7図はそれぞれ本発明の
別の実施例としての磁気ヘッドの鳥轍図、第3図、第4
図、第5図はヘッドノイズとコア幅、ギャップ深さ、コ
ア厚との関係を示す図、第8図は本発明の一実施例であ
るヘッドコア形状を示した図、第9図は、ヘッドノイズ
と巻線数との関係を示す図。 1・・・磁気コア、2・・・巻線窓、3・・・ガラス、
4・・・基板、5・・・高飽和磁束密度材、6・・・磁
気ヘッド、7・・・非磁性スライダ、8・・・ヘッド、
9・・・非磁性スラぞ 3 固 i ′f14 図 入゛ヤッ71斥さ3ty彬 Vl 5 目 第を口    第7図
1 and 2 are top and side views of a magnetic head as an embodiment of the present invention, respectively. FIGS. 6 and 7 are bird track diagrams of a magnetic head as another embodiment of the present invention, respectively. Figure, 4th
5 is a diagram showing the relationship between head noise and core width, gap depth, and core thickness. FIG. 8 is a diagram showing a head core shape according to an embodiment of the present invention. FIG. A diagram showing the relationship between noise and the number of windings. 1... Magnetic core, 2... Winding window, 3... Glass,
4... Substrate, 5... High saturation magnetic flux density material, 6... Magnetic head, 7... Nonmagnetic slider, 8... Head,
9...Non-magnetic slot 3 Solid i 'f14 Illustration 71 Rejection 3ty Akira Vl 5 Eye open Figure 7

Claims (1)

【特許請求の範囲】 1、少なくとも一方のヘッドコア部におけるヘッド巻線
窓部のコア幅が0.7mm以下、0.05mm以上であ
り、巻線数を25以上としたことを特徴とする磁気ヘッ
ド。 2、上記コア幅が0.5mm以下、0.1mm以上であ
ることを特徴とする特許請求の範囲第1項記載の磁気ヘ
ッド。 3、ヘッドコア両側部及びリヤ部のコア幅のいずれも0
.5mm以下、0.1mm以上としたことを特徴とする
特許請求の範囲第1項記載の磁気ヘッド。 4、ギャップ深さを20μm以下、1μm以上としたこ
とを特徴とする特許請求の範囲第1項または特許請求の
範囲第2項または特許請求の範囲第3項記載の磁気ヘッ
ド。 5、上記ギャップ深さを10μm以下、2μm以上とし
たことを特徴とする特許請求の範囲第1項または特許請
求の範囲第2項または特許請求の範囲第3項記載の磁気
ヘッド。 6、コア厚が400μm以下であることを特徴とする特
許請求の範囲第1項ないし第5項記載の磁気ヘッド。 7、上記磁気ヘッドを非磁性材から成るスライダに埋め
込んだことを特徴とする特許請求の範囲第1項記載の磁
気ヘッド。
[Claims] 1. A magnetic head characterized in that the core width of the head winding window in at least one head core part is 0.7 mm or less and 0.05 mm or more, and the number of windings is 25 or more. . 2. The magnetic head according to claim 1, wherein the core width is 0.5 mm or less and 0.1 mm or more. 3. Both sides of the head core and rear core width are 0.
.. The magnetic head according to claim 1, wherein the magnetic head is 5 mm or less and 0.1 mm or more. 4. The magnetic head according to claim 1, claim 2, or claim 3, characterized in that the gap depth is 20 μm or less and 1 μm or more. 5. The magnetic head according to claim 1, claim 2, or claim 3, wherein the gap depth is 10 μm or less and 2 μm or more. 6. A magnetic head according to claims 1 to 5, characterized in that the core thickness is 400 μm or less. 7. The magnetic head according to claim 1, wherein the magnetic head is embedded in a slider made of a non-magnetic material.
JP3263085A 1985-02-22 1985-02-22 magnetic head Pending JPS61194607A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP3263085A JPS61194607A (en) 1985-02-22 1985-02-22 magnetic head

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP3263085A JPS61194607A (en) 1985-02-22 1985-02-22 magnetic head

Publications (1)

Publication Number Publication Date
JPS61194607A true JPS61194607A (en) 1986-08-29

Family

ID=12364169

Family Applications (1)

Application Number Title Priority Date Filing Date
JP3263085A Pending JPS61194607A (en) 1985-02-22 1985-02-22 magnetic head

Country Status (1)

Country Link
JP (1) JPS61194607A (en)

Cited By (4)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPH0271411A (en) * 1988-09-07 1990-03-12 Nippon Mining Co Ltd Copper wire wrapped around the head core
JPH07169017A (en) * 1993-10-22 1995-07-04 Nec Corp Magnetic head and magnetic recording apparatus employing the same
WO2001039181A1 (en) * 1999-11-24 2001-05-31 Matsushita Electric Industrial Co., Ltd. Method of manufacturing magnetic head, and magnetic recording and reproducing apparatus
US6640418B2 (en) 1999-12-03 2003-11-04 Matsushita Electric Industrial Co., Ltd. Method of manufacturing a head unit

Cited By (5)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPH0271411A (en) * 1988-09-07 1990-03-12 Nippon Mining Co Ltd Copper wire wrapped around the head core
JPH07169017A (en) * 1993-10-22 1995-07-04 Nec Corp Magnetic head and magnetic recording apparatus employing the same
WO2001039181A1 (en) * 1999-11-24 2001-05-31 Matsushita Electric Industrial Co., Ltd. Method of manufacturing magnetic head, and magnetic recording and reproducing apparatus
US6783435B1 (en) 1999-11-24 2004-08-31 Matsushita Electric Industrial Co., Ltd. Method of manufacturing magnetic head, and magnetic recording and reproducing apparatus
US6640418B2 (en) 1999-12-03 2003-11-04 Matsushita Electric Industrial Co., Ltd. Method of manufacturing a head unit

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