JPH024052B2 - - Google Patents
Info
- Publication number
- JPH024052B2 JPH024052B2 JP4272383A JP4272383A JPH024052B2 JP H024052 B2 JPH024052 B2 JP H024052B2 JP 4272383 A JP4272383 A JP 4272383A JP 4272383 A JP4272383 A JP 4272383A JP H024052 B2 JPH024052 B2 JP H024052B2
- Authority
- JP
- Japan
- Prior art keywords
- magnetic
- head
- magnetic head
- recording
- gap
- 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
Links
- 230000005415 magnetization Effects 0.000 description 11
- 238000010586 diagram Methods 0.000 description 4
- 230000005347 demagnetization Effects 0.000 description 2
- 230000000694 effects Effects 0.000 description 2
- 238000000034 method Methods 0.000 description 2
Classifications
-
- G—PHYSICS
- G11—INFORMATION STORAGE
- G11B—INFORMATION STORAGE BASED ON RELATIVE MOVEMENT BETWEEN RECORD CARRIER AND TRANSDUCER
- G11B5/00—Recording by magnetisation or demagnetisation of a record carrier; Reproducing by magnetic means; Record carriers therefor
- G11B5/127—Structure or manufacture of heads, e.g. inductive
- G11B5/187—Structure or manufacture of the surface of the head in physical contact with, or immediately adjacent to the recording medium; Pole pieces; Gap features
Landscapes
- Engineering & Computer Science (AREA)
- Manufacturing & Machinery (AREA)
- Recording Or Reproducing By Magnetic Means (AREA)
- Magnetic Heads (AREA)
Description
【発明の詳細な説明】
産業上の利用分野
本発明は例えば短波長記録に適するビデオテー
プレコーダーなどの磁気記録再生装置に関するも
のである。DETAILED DESCRIPTION OF THE INVENTION Field of the Invention The present invention relates to a magnetic recording/reproducing apparatus such as a video tape recorder suitable for short wavelength recording.
従来例の構成とその問題点
従来、ビデオテープレコーダーなどの磁気記録
再生装置においては、長手方向磁化(面内磁化)
が一般的であつた。長手方向磁化は、短波長記録
においては記録減磁が発生することが知られてい
る。このため、ビデオテープレコーダーなどにお
いては、記録波長が1μm報度のところから記録
減磁が増加し、これ以上の短波長記録の実用化は
困難であつた。Conventional structure and its problems Traditionally, in magnetic recording and reproducing devices such as video tape recorders, longitudinal magnetization (in-plane magnetization)
was common. It is known that recording demagnetization occurs in longitudinal magnetization during short wavelength recording. For this reason, in video tape recorders and the like, recording demagnetization increases when the recording wavelength reaches 1 μm, making it difficult to put shorter wavelength recording into practical use.
一方、これ以上の短波長記録を目的とした垂直
磁化方式が検討され、実用化への提案が数多くさ
れている。しかし、現在提案されている垂直磁化
方式の多くは、記録再生に主磁極と補助磁極が必
要であり、また記録媒体としても、垂直磁化膜と
水平磁化膜の2層膜構造が必要であるなど構成が
複雑になるなどの欠点がある。 On the other hand, perpendicular magnetization systems aimed at recording at even shorter wavelengths have been studied, and many proposals for practical use have been made. However, most of the perpendicular magnetization methods currently proposed require a main magnetic pole and an auxiliary magnetic pole for recording and reproduction, and also require a two-layer film structure of a perpendicular magnetization film and a horizontal magnetization film for the recording medium. There are drawbacks such as a complicated configuration.
また、磁気ヘツドのギヤツプ幅方向と磁気テー
プの走行方向とをほぼ同一にするいわゆるトラン
スバース(TRANSVERSE)記録も提案されて
いるが、従来は長手方向磁化のギヤツプ長に相当
するギヤツプ幅より長い波長(実際には3倍程度
以上)しか記録再生できないと考えられており、
大幅な短波長記録の実現にはならなかつた。 Also, so-called TRANSVERSE recording has been proposed, in which the gap width direction of the magnetic head is almost the same as the running direction of the magnetic tape. (Actually, it is thought that only about 3 times more can be recorded and played back.
This did not lead to the realization of significantly shorter wavelength records.
発明の目的
本発明は、上述した従来の欠点を除去し、大幅
な短波長記録を可能にする磁気記録再生あるいは
再生装置を提供することを目的とするものであ
る。OBJECTS OF THE INVENTION It is an object of the present invention to provide a magnetic recording/reproducing device which eliminates the above-mentioned conventional drawbacks and enables recording at significantly shorter wavelengths.
発明の構成
上記目的を達成するために、本発明は、磁気記
録媒体とこの磁気記録媒体に対して所要の相対速
度で移動する磁気ヘツドを有し、かつ前記磁気ヘ
ツドのギヤツプ幅方向と前記相対位置を移動させ
る方向とを同一方向とするトランスバース記録を
用いた磁気記録再生あるいは再生装置であつて、
再生用の磁気ヘツドとしてヘツド・ギヤツプ部を
構成する対峙コアのコア幅の双方の長さを異なら
しめた磁気ヘツドを用いる構成にしたものであ
り、ギヤツプ幅による再生波長の制限を除去で
き、トランスバース記録による大幅な短波長記録
が実現できる。Composition of the Invention In order to achieve the above object, the present invention has a magnetic recording medium and a magnetic head that moves at a required relative speed with respect to the magnetic recording medium. A magnetic recording/reproducing device using transverse recording in which the direction of position movement is the same as the direction of movement,
This configuration uses a magnetic head with different core widths on both sides of the opposing cores constituting the head gap portion as the magnetic head for reproduction.This eliminates the restriction on the reproduction wavelength due to the gap width, and the transformer Significantly short wavelength recording can be realized by birth recording.
実施例の説明
以下本発明の一実施例を図面に基づいて説明す
る。第1図は本発明のテープヘツド系の要部構成
図を示す。1は磁気ヘツド、2は磁気テープ、3
は磁気ヘツド支持体、4は磁気ヘツド1に巻かれ
たコイルである。G1は上記磁気ヘツド1のギヤ
ツプ部である。矢印5は磁気ヘツド1の進行方向
を示しており、これはギヤツプ部G1のギヤツプ
幅方向と同一方向である。なお、相対的に失印5
と逆方向に磁気テープ2が走行してもさしつかえ
ない。これは、ギヤツプ部G1のギヤツプ長GA
をトラツク幅とするトランスバース記録を示して
いる。DESCRIPTION OF EMBODIMENTS An embodiment of the present invention will be described below based on the drawings. FIG. 1 shows a block diagram of essential parts of a tape head system according to the present invention. 1 is a magnetic head, 2 is a magnetic tape, 3
4 is a magnetic head support, and 4 is a coil wound around the magnetic head 1. G1 is a gap portion of the magnetic head 1. An arrow 5 indicates the direction of movement of the magnetic head 1, which is the same direction as the gap width direction of the gap portion G1. In addition, the relative loss of seals is 5.
There is no problem even if the magnetic tape 2 runs in the opposite direction. This is the gap length GA of the gap part G1.
The figure shows a transverse recording with a track width of .
第2図は上記磁気ヘツド1のギヤツプ部G1を
磁気テープ2の手前下方側から見た斜視図であ
る。第2図において、磁気ヘツド1のギヤツプ部
G1の前端部は対峙するコア端6およびコア端7
で構成され、直線8はコア端6とコア端7を結ん
だ直線である。同時に、後端部は対峙するコア端
9およびコア端10で構成され、直線11はコア
端9とコア端10を結んだ直線である。そして、
直線8と矢印5の延長線12とは直角でない角度
で交わり、直線11と延長線12とは直角で交わ
つている。これは、対峙するコアすなわちコア端
6とコア端9の間のコア幅の長さL1とコア端7
とコア端10の間のコア幅の長さL2の双方の長
さが異なることにより生じる。 FIG. 2 is a perspective view of the gap G1 of the magnetic head 1 viewed from the lower side in front of the magnetic tape 2. As shown in FIG. In FIG. 2, the front end of the gap G1 of the magnetic head 1 has opposing core ends 6 and 7.
The straight line 8 is a straight line connecting the core ends 6 and 7. At the same time, the rear end portion is composed of a core end 9 and a core end 10 facing each other, and a straight line 11 is a straight line connecting the core end 9 and the core end 10. and,
The straight line 8 and the extension line 12 of the arrow 5 intersect at an angle that is not a right angle, and the straight line 11 and the extension line 12 intersect at a right angle. This is the core width length L 1 between the opposing cores, that is, core end 6 and core end 9, and core end 7.
This is caused by the fact that the length L2 of the core width between the core end 10 and the core width L2 are different.
このような構成のテープ・ヘツド系において、
コイル4に第3図に示すような記録電流を流す
と、第4図に示すような磁化パターンが得られ
る。第4図において、13は記録トラツクを示
し、14は磁化ベクトルを示す。これは、いわゆ
るトランスバース記録と称するものである。 In a tape head system configured like this,
When a recording current as shown in FIG. 3 is passed through the coil 4, a magnetization pattern as shown in FIG. 4 is obtained. In FIG. 4, 13 indicates a recording track, and 14 indicates a magnetization vector. This is what is called transverse recording.
従来のトランスバース記録の再生においては、
第5図(第2図と同様な方向から見た斜視図)に
例示するように、コア端15とコア端17との間
のコア幅の長さL3とコア端16とコア端18と
の間のコア幅の長さL4とが等しい、すなわちギ
ヤツプ幅がL(L=L3=L4)である磁気ヘツド1
9を用いているため、第6図に示すような再生周
波数特性が得られる。第6図におけるA点は周波
数特性の谷であり、これは、磁気テープ2に記録
された信号の波長と上記ギヤツプ幅Lとが等しく
なつたところで生じる再生ギヤツプロスであり、
これより短かい波長の信号(高い周波数の信号)
では図の如く複数の再生ギヤツプ・ロスがあるこ
とから実際の使用(記録再生)には供し得ないも
のであつた。 When playing back conventional transverse recordings,
As illustrated in FIG. 5 (a perspective view seen from the same direction as FIG. 2), the length L 3 of the core width between the core end 15 and the core end 17, the core end 16 and the core end 18, The magnetic head 1 has a gap width L (L=L 3 =L 4 ), in which the length L 4 of the core width between
9 is used, reproduction frequency characteristics as shown in FIG. 6 can be obtained. Point A in FIG. 6 is the valley of the frequency characteristic, and this is the playback gap loss that occurs when the wavelength of the signal recorded on the magnetic tape 2 and the gap width L become equal.
Signals with shorter wavelengths (higher frequency signals)
However, as shown in the figure, there are multiple playback gaps and losses, so it cannot be used for actual use (recording and playback).
しかし、第2図に示すように、L1とL2の長さ
が異なるようなヘツド・ギヤツプ部G1を有する
磁気ヘツド1で第4図に示したような記録トラツ
ク13を再生すると、その再生周波数特性は第7
図に示すような、いわゆる谷の生じないものが得
られる。これにより、ギヤツプ幅による再生波長
の制限が取り除かれるため、トランスバース記録
により大幅な短波長記号を再生することが可能に
なる。この記録波長は、通常用いられている長手
方向磁化より十分に短かいものである。 However, as shown in FIG . 2 , when the recorded track 13 shown in FIG . The reproduction frequency characteristic is the 7th
As shown in the figure, a product without so-called valleys can be obtained. This removes the limitation on the reproduction wavelength due to the gap width, making it possible to reproduce significantly shorter wavelength symbols by transverse recording. This recording wavelength is sufficiently shorter than the commonly used longitudinal magnetization.
ここで、再生周波数特性における谷の生じない
理由としては、コア端6および7で形成されるギ
ヤツプ前端部の角度が記録された信号の磁壁の角
度とが異なることによるものと考える。なお、ギ
ヤツプ前端部の角度が記録された信号の磁壁の角
度と同一で、ギヤツプ後端部の角度が記録された
信号の磁壁の角度と異なるような構成の磁気ヘツ
ド(図示せず)でも同様な効果が得られる。これ
らの磁気ヘツドは、トランスバース記録におい
て、再生用の磁気ヘツドにおけるヘツド・ギヤツ
プ部を構成する対峙コアのコア幅の双方の長さを
異ならせしめることにより得られる。 Here, it is considered that the reason why no valley occurs in the reproduction frequency characteristic is that the angle of the front end of the gap formed by the core ends 6 and 7 is different from the angle of the domain wall of the recorded signal. Note that this also applies to a magnetic head (not shown) configured such that the angle at the front end of the gap is the same as the angle of the domain wall of the recorded signal, and the angle at the rear end of the gap is different from the angle of the domain wall of the recorded signal. You can get the following effect. These magnetic heads are obtained in transverse recording by making the core widths of opposing cores that constitute a head gap in a reproducing magnetic head different in length.
発明の効果
以上発明によれば、ギヤツプ幅による再生波長
の制限を除去でき、トランスバース記録による大
幅な短波長記録が実現できる。また、本発明によ
れば、垂直磁化方式のような特殊なヘツドと特殊
な媒体を必要とすることもないなどの特徴を有
し、その工業的価値は極めて大きい。Effects of the Invention According to the invention described above, it is possible to eliminate the restriction on reproduction wavelength due to the gap width, and to realize significantly short wavelength recording by transverse recording. Furthermore, the present invention has the feature that it does not require a special head or a special medium unlike the perpendicular magnetization method, and its industrial value is extremely large.
第1図は本発明におけるテープ・ヘツド系の一
構成例を示す要部概略斜視図、第2図は第1図に
おける磁気ヘツドの一構成例を示す概略斜視図、
第3図は記録信号の一例を示す信号波形図、第4
図は本発明で使用する磁気テープに記録された記
録パターンの一例を示す概略斜視図、第5図は従
来例の磁気ヘツドの構成例を示す要部概略斜視
図、第6図は従来例の磁気ヘツドを用いた場合の
再生周波数特性の一例を示す概略特性図、第7図
は本発明における磁気ヘツドを用いた場合の再生
周波数特性の一例を示す概略特性図である。
1…磁気ヘツド、2…磁気テープ、4…コイ
ル、5…相対移動方向、6,7,9,10…コア
端、G1…ヘツド・ギヤツプ部、L1,L2…コア幅
の長さ、GA…ギヤツプ長。
FIG. 1 is a schematic perspective view of essential parts showing an example of the structure of a tape head system according to the present invention, FIG. 2 is a schematic perspective view showing an example of the structure of the magnetic head in FIG. 1,
Figure 3 is a signal waveform diagram showing an example of a recording signal;
The figure is a schematic perspective view showing an example of the recording pattern recorded on the magnetic tape used in the present invention, FIG. 5 is a schematic perspective view of the main part showing an example of the configuration of a conventional magnetic head, and FIG. FIG. 7 is a schematic characteristic diagram showing an example of reproduction frequency characteristics when a magnetic head is used. FIG. 7 is a schematic characteristic diagram showing an example of reproduction frequency characteristics when a magnetic head is used in the present invention. 1... Magnetic head, 2... Magnetic tape, 4... Coil, 5... Relative movement direction, 6, 7, 9, 10... Core end, G 1 ... Head/gap portion, L 1 , L 2 ... Length of core width , GA...Gap length.
Claims (1)
要の相対速度で移動する磁気ヘツドを有し、か
つ、前記磁気ヘツドのギヤツプ幅方向と前記相対
移動させる方向とを同一方向とするトランスバー
ス記録を用いた磁気記録再生あるいは再生装置で
あつて、磁気ヘツドとしてヘツド・ギヤツプ部を
構成する対峙コアのコア幅の双方の長さを異なら
しめた磁気ヘツドを用いることを特徴とする磁気
記録再生あるいは再生装置。 2 磁気ヘツドのヘツド・ギヤツプ部の前端部の
対峙するコア端を結んだ直線を磁気記録媒体と磁
気ヘツドとの相対移動方向に対して直角になるよ
うに構成するとともに、磁気ヘツドのヘツド・ギ
ヤツプ部の後端部の対峙するコア端を結んだ直線
を上記相対移動方向に対して直角とは異なる角度
になるように構成したことを特徴とする特許請求
の範囲第1項記載の磁気記録再生あるいは再生装
置。 3 磁気ヘツドのヘツド・ギヤツプ部の前端部の
対峙するコア端を結んだ直線を磁気記録媒体と磁
気ヘツドとの相対移動方向に対して直角とは異な
る角度になるように構成するとともに、磁気ヘツ
ドのヘツド・ギヤツプ部の後端部の対峙するコア
端を結んだ直線を上記相対移動方向に対して直角
になるように構成したことを特徴とする特許請求
の範囲第1項記載の磁気記録再生あるいは再生装
置。[Scope of Claims] 1. A magnetic recording medium and a magnetic head that moves at a required relative speed with respect to the magnetic recording medium, and the gap width direction of the magnetic head and the direction of the relative movement are the same direction. A magnetic recording/reproducing device using transverse recording, characterized in that it uses a magnetic head in which the core widths of opposite cores constituting a head gap portion are different in length. magnetic recording/reproducing or reproducing device. 2. The straight line connecting the opposing core ends of the front end of the head gap of the magnetic head is configured to be perpendicular to the direction of relative movement between the magnetic recording medium and the magnetic head, and the head gap of the magnetic head is The magnetic recording and reproducing device according to claim 1, wherein a straight line connecting the opposing core ends of the rear end of the section is configured to form an angle different from a right angle with respect to the relative movement direction. Or a playback device. 3. Construct the straight line connecting the opposing core ends of the front end of the head gap portion of the magnetic head to be at an angle different from a right angle to the direction of relative movement between the magnetic recording medium and the magnetic head, and The magnetic recording/reproducing device according to claim 1, wherein a straight line connecting the opposing core ends of the rear end of the head gap portion of the head gap is arranged to be perpendicular to the direction of relative movement. Or a playback device.
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP58042723A JPS59167819A (en) | 1983-03-14 | 1983-03-14 | Magnetic recording and reproducing device |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP58042723A JPS59167819A (en) | 1983-03-14 | 1983-03-14 | Magnetic recording and reproducing device |
Publications (2)
| Publication Number | Publication Date |
|---|---|
| JPS59167819A JPS59167819A (en) | 1984-09-21 |
| JPH024052B2 true JPH024052B2 (en) | 1990-01-25 |
Family
ID=12643982
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP58042723A Granted JPS59167819A (en) | 1983-03-14 | 1983-03-14 | Magnetic recording and reproducing device |
Country Status (1)
| Country | Link |
|---|---|
| JP (1) | JPS59167819A (en) |
Families Citing this family (1)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| US5068959A (en) * | 1988-07-11 | 1991-12-03 | Digital Equipment Corporation | Method of manufacturing a thin film head |
-
1983
- 1983-03-14 JP JP58042723A patent/JPS59167819A/en active Granted
Also Published As
| Publication number | Publication date |
|---|---|
| JPS59167819A (en) | 1984-09-21 |
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