JPS63247902A - Magnetic head - Google Patents
Magnetic headInfo
- Publication number
- JPS63247902A JPS63247902A JP7754387A JP7754387A JPS63247902A JP S63247902 A JPS63247902 A JP S63247902A JP 7754387 A JP7754387 A JP 7754387A JP 7754387 A JP7754387 A JP 7754387A JP S63247902 A JPS63247902 A JP S63247902A
- Authority
- JP
- Japan
- Prior art keywords
- magnetic
- core
- magnetic core
- half body
- ferrite
- 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
Links
- 229910000521 B alloy Inorganic materials 0.000 claims abstract description 11
- 239000000696 magnetic material Substances 0.000 claims abstract description 9
- 238000011144 upstream manufacturing Methods 0.000 claims abstract description 4
- 229910000859 α-Fe Inorganic materials 0.000 abstract description 22
- 230000004907 flux Effects 0.000 abstract description 13
- 238000004804 winding Methods 0.000 abstract description 10
- 239000011521 glass Substances 0.000 abstract description 7
- 229910045601 alloy Inorganic materials 0.000 abstract description 3
- 239000000956 alloy Substances 0.000 abstract description 3
- 238000003466 welding Methods 0.000 abstract description 3
- 230000035699 permeability Effects 0.000 abstract description 2
- 239000011162 core material Substances 0.000 description 67
- 229910000702 sendust Inorganic materials 0.000 description 12
- 238000010586 diagram Methods 0.000 description 2
- 230000000694 effects Effects 0.000 description 2
- 238000005299 abrasion Methods 0.000 description 1
- 239000002131 composite material Substances 0.000 description 1
- 238000000034 method Methods 0.000 description 1
Abstract
Description
【発明の詳細な説明】
[産業上の利用分野]
本発明は磁気記録媒体に磁気コアを相対的に摺動させて
情報の記録、再生または消去を行なう磁気ヘッドに関し
、特に例えば8 mmV T Rに用いられる回転消去
ヘッド等の磁気コアに高飽和磁束密度と高耐摩耗性が要
求され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 that records, reproduces, or erases information by sliding a magnetic core relative to a magnetic recording medium, and particularly relates to a magnetic head that records, reproduces, or erases information by sliding a magnetic core relative to a magnetic recording medium. The present invention relates to a magnetic head such as a rotary erase head used in a magnetic core that requires high saturation magnetic flux density and high wear resistance.
[従来の技術]
VTRに用いられるシングルギャップの回転消去ヘッド
では以ドのことが要求される。[Prior Art] A single-gap rotary erasing head used in a VTR requires the following.
a)高抗磁力の磁気テープに高密度記録を行なうため磁
気コアの飽和磁束密度が高いこと。a) The saturation magnetic flux density of the magnetic core is high because high-density recording is performed on a magnetic tape with high coercive force.
b)消去消費電力を少なくするために渦電流損失が小さ
く磁気コアのQが高く、磁気回路の共振が取り易いこと
。b) In order to reduce erase power consumption, eddy current loss is small and the Q of the magnetic core is high, making it easy to obtain resonance in the magnetic circuit.
C)高速で磁気テープに摺接するため磁気コアの耐摩耗
性が優れていること。C) The magnetic core has excellent wear resistance because it comes into sliding contact with the magnetic tape at high speed.
このような要求に対して従来のシングルギャップ回転消
去ヘッドでは、磁気コアの構造として第4図〜第6図に
示すような構造が採用されている。すなわち、まず第4
図の構造ではそれぞれ磁気コア半体として酸化物磁性体
のフェライi・からなるフェライトコア半体l、1′を
磁気ギャップ4を介して突き合わせ接合して磁気コアが
構成されている。また、第5図の構造では磁気コア字体
としてそれぞれセンダストから成るセンタヌトコア半体
7,7′を磁気ギヤング4を介し接合して磁気コアが構
成されている。また、第6図のコアはいわゆる複合型の
コアであり、フェライトから成るフェライトコア半体l
とセンダストから成るセンダストコア半体7′とを磁気
ギャップ4を介[2接合して磁気コアが構成されている
。In order to meet these demands, conventional single-gap rotary erasing heads employ structures as shown in FIGS. 4 to 6 as the structure of the magnetic core. That is, first, the fourth
In the structure shown in the figure, the magnetic core is constructed by butt-joining ferrite core halves l and 1' made of ferrite i, which are oxide magnetic materials, through a magnetic gap 4, respectively. Further, in the structure shown in FIG. 5, the magnetic core is constructed by joining center core halves 7 and 7' made of sendust through a magnetic ganging 4 as magnetic core fonts. The core shown in Figure 6 is a so-called composite core, with a ferrite core half made of ferrite.
A magnetic core is constructed by joining a Sendust core half body 7' made of Sendust and a Sendust core half 7' through a magnetic gap 4.
それぞれのコア半体の突き合わせ面において磁気キャン
プ4の両側には磁気ギャップ4のトラック幅を決めるト
ラック溝6,6′が形成されており、このトランク溝6
.6′にガラス3を充填し、このガラス3の溶着により
コア半体どうしが接合される、また、一方の磁気コア半
体には巻線窓5か形成されており、この巻線窓を介して
不図示のコイル!j3線を磁気コアに巻回して磁気ヘッ
ドが構成される。Track grooves 6 and 6' are formed on both sides of the magnetic camp 4 at the abutting surfaces of the respective core halves to determine the track width of the magnetic gap 4, and this trunk groove 6 is formed on both sides of the magnetic camp 4.
.. 6' is filled with glass 3, and the core halves are joined by welding the glass 3. Also, a winding window 5 is formed in one of the magnetic core halves, and the winding window 5 is used to connect the core halves. A coil (not shown)! A magnetic head is constructed by winding the J3 wire around a magnetic core.
[発明が解決しようとする問題点]
ところが、このような構造では上に述べたa〜Cの要求
に対して以下のような問題がある。[Problems to be Solved by the Invention] However, such a structure has the following problems with respect to the requirements a to C described above.
すなわち、まず第4図の構造ではフェライトの特性ト飽
和磁束密度が不足する6また、第5図の磁気コアアはセ
ンダストの比抵抗が低いため渦電流損失が大きく、Qが
低くなってしまう6また、センダストはフェライトに比
べて耐摩耗性に劣るという問題がある。そして第6図の
構造では飽和f磁束密度とQについては満足されるもの
の、耐摩耗性に劣るセンダストコア半体7′の方が片減
りし、磁気テープ摺動面の形状が変形してヘッドタッチ
が劣化するという問題があった。That is, first, the structure shown in Fig. 4 lacks the saturation magnetic flux density due to the characteristics of ferrite.6 Also, in the magnetic core shown in Fig. 5, the eddy current loss is large due to the low specific resistance of sendust, resulting in a low Q. , Sendust has a problem in that it has inferior wear resistance compared to ferrite. Although the structure shown in Fig. 6 satisfies the saturation f magnetic flux density and Q, the sendust core half 7', which has poor wear resistance, wears on one side, and the shape of the magnetic tape sliding surface deforms, causing the head There was a problem that the touch deteriorated.
[問題点を解決するだめの手段]
このような問題点を解決するため本発明によれば、一対
のmスコア半体を磁気ギャップを介し接合してなる磁気
コアを磁気記録媒体に相対的に摺動させて情報の記録、
再生または消去を行なう磁気ヘッドにおいて、前記媒体
の摺動力向の」1流側の磁気コア半体はFe−B系合金
から形成し、下流側の磁気コア半体は酸化物磁性体から
形成した構造を採用した。[Means for Solving the Problems] In order to solve these problems, according to the present invention, a magnetic core formed by joining a pair of m-score halves through a magnetic gap is fixed relative to a magnetic recording medium. Record information by sliding,
In a magnetic head for reproducing or erasing, the magnetic core half on the first stream side of the sliding direction of the medium is formed from an Fe-B alloy, and the magnetic core half on the downstream side is formed from an oxide magnetic material. structure was adopted.
[作 用]
Fe−B系合金のコア材によれば、耐摩耗性については
センダストより大幅に高く、酸化物磁性体のフェライト
に近い、また飽和磁束密度については、フェライトより
大幅に高く、センダストに近い。従ってこのようなFe
−B系合金と酸化物磁性体のフェライトを組み合わせて
用いた上述の磁気コアの構j告によれば、先に述べた従
来構造よりも飽和磁束密度と耐摩耗性の両方を共に向ト
することができる。[Function] According to the Fe-B alloy core material, wear resistance is significantly higher than Sendust and close to ferrite, which is an oxide magnetic material, and saturation magnetic flux density is significantly higher than ferrite, which is similar to Sendust. Close to. Therefore, such Fe
- According to the above-mentioned magnetic core structure using a combination of B-based alloy and ferrite, which is an oxide magnetic material, both saturation magnetic flux density and wear resistance are improved compared to the conventional structure described above. be able to.
[実施例]
以ド、第1図以下を参照して本発明実施例の詳mllを
説明する。[Embodiment] Hereinafter, details of an embodiment of the present invention will be explained with reference to FIG. 1 and subsequent figures.
第1図は、本発明の実施例として先に述べたVTRのシ
ングルキャンプ回転消去ヘッドの磁気コアの構造を示し
ている。FIG. 1 shows the structure of the magnetic core of the single camp rotary erase head of the VTR described above as an embodiment of the present invention.
第1図において符号lは磁気コア半体として高透磁率の
酸化物磁性体であるフェライトから成るフェライトコア
半体である。また、符号2は同じく磁気コアを体として
Fe−B系合金から成るFe−Bコア半体である。フェ
ライトコア半体1とFe−Bコア半体2を磁気ギャップ
4を介して突き合わせ接合して本実施例の磁気コアが構
成される。両コア半体1.2のそれぞれの突き合わせ而
において磁気ギャップ4の両側部分には磁気ギャップ4
のトラック幅を決めるトラック溝6゜6′が形成されて
おり、このトラック溝にガラス3を充填し、このガラス
3の溶着により両コア半体1.2が接合される。また、
この場合Fe−Bコア半体には巻線窓5が形成されてお
り、この巻線窓5を介して不図示のコイル巻線をこの磁
気コアに巻回して消去ヘッドが構成される。In FIG. 1, reference numeral 1 denotes a ferrite core half made of ferrite, which is an oxide magnetic material with high magnetic permeability, as a magnetic core half. Further, reference numeral 2 designates an Fe-B core half made of an Fe-B alloy, which also includes a magnetic core. The magnetic core of this embodiment is constructed by butting and joining a ferrite core half 1 and an Fe-B core half 2 with a magnetic gap 4 interposed therebetween. There is a magnetic gap 4 on both sides of the magnetic gap 4 at the point where both core halves 1.2 butt each other.
A track groove 6.degree. 6' is formed to determine the track width of the core, and this track groove is filled with glass 3, and by welding the glass 3, both core halves 1.2 are joined. Also,
In this case, a winding window 5 is formed in the Fe--B core half, and a coil winding (not shown) is wound around the magnetic core through the winding window 5 to form an erasing head.
ところでFe−B系合金の特徴として、まずフェライト
とほぼ同等の高い#摩耗性を有する。By the way, as a characteristic of Fe-B alloy, firstly, it has a high wear resistance almost equivalent to that of ferrite.
第2図はこれを示すものであり、磁気コアの摩耗試験と
してそれぞれセンダスト、Fe−B系合金、フェライト
から形成した磁気コアのそれぞれについて磁気テープを
摺動走行させ、磁気テープの走行時間とそれぞれの摩耗
量の関係を測定した結果を示すものである。この図から
明らかなように、Fe−B系合金の摩耗量はセンタスト
より大幅に小さくフェライトに近い。Figure 2 shows this.As a magnetic core wear test, a magnetic tape was slid on each magnetic core made of sendust, Fe-B alloy, and ferrite, and the running time of the magnetic tape and each This shows the results of measuring the relationship between the amount of wear. As is clear from this figure, the amount of wear of the Fe-B alloy is significantly smaller than that of Centast and is close to that of ferrite.
また、Fe−B系合金の特徴としてセンタストに近い高
飽和磁束密度を有する。すなわち、センダストの飽和磁
束密度は8000〜10000ヵウスであるのに対して
Fe−B系合金の飽和磁束密度は約7000ガウス程度
になる。Further, as a characteristic of the Fe-B alloy, it has a high saturation magnetic flux density close to centast. That is, the saturation magnetic flux density of Sendust is 8,000 to 10,000 Gauss, whereas the saturation magnetic flux density of Fe-B alloy is about 7,000 Gauss.
このような本実施例の磁気コアの構造によれば、第4図
の従来例の場合より飽和磁束密度を高めることができる
。また、第5図および第6図の従来例の場合よりも磁気
コアの耐摩耗性を向上できると共にフェライトとFe−
B系合金の面摩耗性の差が少ないことにより、磁気コア
の片減りを防l−することもできる。また、一方のコア
半体1に比抵抗の大きいフェライトを用いていることで
センダストコアに比べて比抵抗が太きく渦電流が少なく
、Qが高い効率的な磁気コアを構成できる。According to the structure of the magnetic core of this embodiment, the saturation magnetic flux density can be increased compared to the conventional example shown in FIG. Moreover, the wear resistance of the magnetic core can be improved compared to the conventional examples shown in FIGS. 5 and 6, and the ferrite and Fe-
Since there is little difference in the surface abrasion properties of the B-based alloys, uneven wear of the magnetic core can also be prevented. Further, by using ferrite having a high resistivity for one core half 1, it is possible to construct an efficient magnetic core with a higher resistivity, less eddy current, and a higher Q than a Sendust core.
なお、以北の本実施例の磁気コアの構造において、Fe
−Bコア半体2は第1図に矢印で示す磁気テープ摺動方
向の上流側に配置し、フェライトコア半体lは磁気テー
プ摺動方向の下流側に配置するものとする。このように
配置することにより、磁気ギャップ4の近傍に発生する
磁界は第3図に実線で示すように、磁気テープ摺動方向
に対して2瞬な立ち上りとゆるやかな立ち下りを持つも
のとなり、消去磁界として理想的なものとなる0両方の
コア享体(a)、(b)がフェライトから成る場合には
同図に破線で示すように発生磁界の立ち上りと立ち下り
が同様のカーブになるのに対して、本実施例の場合は上
に述べたような磁界で良好に消去を行なえる。In addition, in the structure of the magnetic core of this example north of this, Fe
-B The core half 2 is placed on the upstream side in the magnetic tape sliding direction shown by the arrow in FIG. 1, and the ferrite core half 1 is placed on the downstream side in the magnetic tape sliding direction. With this arrangement, the magnetic field generated near the magnetic gap 4 has two instantaneous rises and a gradual fall in the magnetic tape sliding direction, as shown by the solid line in FIG. If both core bodies (a) and (b) are made of ferrite, which is ideal as an erasing magnetic field, the rise and fall of the generated magnetic field will have similar curves, as shown by the broken line in the same figure. On the other hand, in the case of this embodiment, erasing can be performed satisfactorily using the magnetic field as described above.
[発明の効果]
以りの説明から明らかなように、本発明によれば、一対
の磁気コア半体を磁気ギャップを介し接合してなる磁気
コアを磁気記録媒体に相対的に摺動させて情報の記録、
再生または消去を行なう磁気ヘッドにおいて、前記媒体
の摺動方向の上流側の磁気コア半体はFe−B系合金か
ら形成し、下流側の磁気コア半体は酸化物磁性体から形
成した構造を採用したので、磁気コアの飽和磁束密度と
共に1耐摩耗性を向りでき、また効率を向」ニジて消費
電力を低減できるという優れた効果が得られる。[Effects of the Invention] As is clear from the description below, according to the present invention, a magnetic core formed by joining a pair of magnetic core halves through a magnetic gap is made to slide relative to a magnetic recording medium. recording information,
In a magnetic head for reading or erasing, the magnetic core half on the upstream side in the sliding direction of the medium is formed from an Fe-B alloy, and the magnetic core half on the downstream side is formed from an oxide magnetic material. By adopting this method, it is possible to improve wear resistance as well as the saturation magnetic flux density of the magnetic core, and to improve efficiency and reduce power consumption, which is an excellent effect.
第1図は本発明の実施例による磁気ヘッドの磁気コアの
構造を示す斜視図、第2図は磁気コアの摩耗試験におけ
る磁気テープの摺動走行時間と異なるコア材から成る磁
気コアのそれぞれの摩耗量の関係を示す線図、第3図は
磁気ギャップ近傍の発生磁界の違いを示す説明図、第4
図〜第6図はそれぞれ異なる従来の磁気ヘッドの磁気コ
アの構造を示す斜視図である。
l・・・フェライトコア半体
2・・・Fe−8コア半体
3・・・ガラス 4・・・磁気ギャップ5・・
・巻線窓 6.6′・・・トラック溝第4図FIG. 1 is a perspective view showing the structure of a magnetic core of a magnetic head according to an embodiment of the present invention, and FIG. 2 shows the sliding running time of a magnetic tape in a magnetic core wear test and the relationship between magnetic cores made of different core materials. Figure 3 is a diagram showing the relationship between the amount of wear, and Figure 4 is an explanatory diagram showing the difference in magnetic fields generated near the magnetic gap.
6 are perspective views showing the structures of magnetic cores of different conventional magnetic heads. l... Ferrite core half body 2... Fe-8 core half body 3... Glass 4... Magnetic gap 5...
・Winding window 6.6'...Track groove Fig. 4
Claims (1)
磁気コアを磁気記録媒体に相対的に摺動させて情報の記
録、再生または消去を行なう磁気ヘッドにおいて、前記
媒体の摺動方向の上流側の磁気コア半体はFe−B系合
金から形成し、下流側の磁気コア半体は酸化物磁性体か
ら形成したことを特徴とする磁気ヘッド。In a magnetic head that records, reproduces, or erases information by sliding a magnetic core formed by joining a pair of magnetic core halves through a magnetic gap relative to a magnetic recording medium, upstream in the sliding direction of the medium. A magnetic head characterized in that the magnetic core half on the side is formed from an Fe-B alloy, and the magnetic core half on the downstream side is formed from an oxide magnetic material.
Priority Applications (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP7754387A JPS63247902A (en) | 1987-04-01 | 1987-04-01 | Magnetic head |
Applications Claiming Priority (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP7754387A JPS63247902A (en) | 1987-04-01 | 1987-04-01 | Magnetic head |
Publications (1)
Publication Number | Publication Date |
---|---|
JPS63247902A true JPS63247902A (en) | 1988-10-14 |
Family
ID=13636914
Family Applications (1)
Application Number | Title | Priority Date | Filing Date |
---|---|---|---|
JP7754387A Pending JPS63247902A (en) | 1987-04-01 | 1987-04-01 | Magnetic head |
Country Status (1)
Country | Link |
---|---|
JP (1) | JPS63247902A (en) |
-
1987
- 1987-04-01 JP JP7754387A patent/JPS63247902A/en active Pending
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