JPS63244304A - Magnetic head - Google Patents

Magnetic head

Info

Publication number
JPS63244304A
JPS63244304A JP7719987A JP7719987A JPS63244304A JP S63244304 A JPS63244304 A JP S63244304A JP 7719987 A JP7719987 A JP 7719987A JP 7719987 A JP7719987 A JP 7719987A JP S63244304 A JPS63244304 A JP S63244304A
Authority
JP
Japan
Prior art keywords
coil
recording
head
reproducing
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.)
Granted
Application number
JP7719987A
Other languages
Japanese (ja)
Other versions
JP2696831B2 (en
Inventor
Satoru Goto
哲 後藤
Kazuhiro Fujimura
和弘 藤村
Makoto Sato
誠 佐藤
Toshio Kitamura
北村 敏雄
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.)
Sony Corp
Original Assignee
Sony Corp
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 Sony Corp filed Critical Sony Corp
Priority to JP62077199A priority Critical patent/JP2696831B2/en
Publication of JPS63244304A publication Critical patent/JPS63244304A/en
Application granted granted Critical
Publication of JP2696831B2 publication Critical patent/JP2696831B2/en
Anticipated expiration legal-status Critical
Expired - Lifetime legal-status Critical Current

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Abstract

PURPOSE:To suppress the noise from a inductive noise source or a crosstalk from the head of a reverse side or the like by arranging a first coil and a second coil, which generate alternately the recording magnetic fluxes of directions different from each other, independently of each other. CONSTITUTION:A reading/reproducing coil 15 is constituted of the first coil 17 which is wound around one half of a bobbin 16, and the second coil 19 which is wound around the other half of the bobbin 16 as being separated by the partition 18 at the nearly middle part of the bobbin 16 and it is packaged in a recording/reproducing core 4. Here, the first coil 17 and the second coil 19 are arranged as being divided by the partition 18, but the respective coils 17, 19 can be wound around the same two bobbins and can be packaged in the recording/reproducing core 4 as being superimposed in series. Thus, the combined capacity of the recording/reproducing oil of the magnetic head can be made small and even if it resonates by receiving the inductive noise from the head of the reverse side of the two sided FDD or from an outside, it does not record/reproduce for media, and the head which is strong against the inductive noise and does not generate the cross talk can be obtained.

Description

【発明の詳細な説明】 [産業上の利用分野] 本発明は、フロッピーディスクドライブ(以下FDDと
記す)等の磁気ヘッドに関し、特に高密度記録/再生用
に好適なものとして、記録/再生の際にエラー発生が少
くなるようにしたものである。
Detailed Description of the Invention [Field of Industrial Application] The present invention relates to a magnetic head such as a floppy disk drive (hereinafter referred to as FDD), and is particularly suitable for high-density recording/reproduction. This is to reduce the occurrence of errors.

[発明の概要] 本発明は、2つのコイルを備え、互いに異なる方向の記
録磁束を発生するなどして記録/再生を行うFDD等の
磁気ヘッドにおいて、 2つのコイルを互いに独立して配置し、それらコイルの
結合容mを減少させて、その結合容量とコイルのインダ
クタンスで決まる共振周波数を上昇させ、誘導性ノイズ
源からのノイズや逆サイドのヘッドなどからのクロスト
ークを抑えることにより、 誤記録や誤再生などのエラー発生を少くしたものである
[Summary of the Invention] The present invention provides a magnetic head such as an FDD that includes two coils and performs recording/reproduction by generating recording magnetic flux in different directions, in which the two coils are arranged independently from each other, By reducing the coupling capacitance m of these coils and increasing the resonance frequency determined by the coupling capacitance and coil inductance, suppressing noise from inductive noise sources and crosstalk from the head on the opposite side, etc., it is possible to prevent erroneous recording. This reduces the occurrence of errors such as erroneous playback.

[従来の技術] 第5図は、従来からFDDに使用されている磁気ヘッド
と記録系の等価回路図である。この磁気ヘッド1は記録
/再生ヘッド2と消去ヘッド3とによって構成されてい
る。記録/再生ヘッド2の記録/再生コア4には記録/
再生コイル5が巻回され、この記録/再生コイル5はセ
ンタータップ6によって第1のコイル7と第2のコイル
8とに分割されている。これら第1のコイル7の巻き数
と第2のコイル8の巻き数とは互いに等しく、例えば1
60ターンである。そして記録/再生コア4の後方(矢
印&で示すディスク移動方向における後方)には、スペ
ーサ9を介して消去コア10が隣接して配置され、その
消去コア10には消去コイル11が巻回されている。そ
して消去コア10に形成された一対の消去ギャップI2
が記録/再生コア4に形成された記録/再生ギャップ1
3の後方両側に位置するように構成されている。
[Prior Art] FIG. 5 is an equivalent circuit diagram of a magnetic head and a recording system conventionally used in an FDD. This magnetic head 1 is composed of a recording/reproducing head 2 and an erasing head 3. The recording/playback core 4 of the recording/playback head 2 records/
A reproducing coil 5 is wound around the recording/reproducing coil 5, and the recording/reproducing coil 5 is divided into a first coil 7 and a second coil 8 by a center tap 6. The number of turns of the first coil 7 and the number of turns of the second coil 8 are equal to each other, for example, 1
It is 60 turns. An erasing core 10 is arranged adjacently to the rear of the recording/reproducing core 4 (rearward in the disk movement direction indicated by the arrow &) with a spacer 9 interposed therebetween, and an erasing coil 11 is wound around the erasing core 10. ing. A pair of erase gaps I2 formed in the erase core 10
recording/reproducing gap 1 formed in the recording/reproducing core 4
It is configured to be located on both rear sides of 3.

この磁気ヘッド1では、記録時に、センタータップ6か
ら第1のコイル7と第2のコイル8とにスイッチ回路1
4のスイッチングによって記録電流を交互に流し、それ
ら両コイル7.8の起磁力によって記録/再生コア4に
互いに異なる方向の記録磁束A、Bを交互に発生させる
。そして記録/再生ギャップ13部分でディスクに記録
磁化した記録トラックを形成する。この記録と同時に、
消去コイル11に直流の消去電流を流し、その消去コイ
ル+1の起磁力によって消去コアIOに一定方向の消去
磁束Eを発生させ、消去ギャップ12部分で前記記録ト
ラックの両側を消去しガートバンドを確保するように構
成されている。
In this magnetic head 1, during recording, a switch circuit 1 is connected from the center tap 6 to the first coil 7 and the second coil 8.
4, a recording current is caused to flow alternately, and recording magnetic fluxes A and B in mutually different directions are alternately generated in the recording/reproducing core 4 by the magnetomotive force of both coils 7 and 8. Then, a recording magnetized recording track is formed on the disk at the recording/reproducing gap 13 portion. At the same time as this record,
A DC erasing current is passed through the erasing coil 11, and the magnetomotive force of the erasing coil +1 generates an erasing magnetic flux E in a certain direction in the erasing core IO, erasing both sides of the recording track in the erasing gap 12 portion and securing a guard band. is configured to do so.

上記におけるコイル7.8は、一般に第6図に示すバイ
ファイラ巻きで形成される。このバイファイラ巻きは、
2本の導線を対にして巻く巻き方で、第1のコイル7と
第2のコイル8とは極性が違う以外、全く等価とみなす
ことができる。従って、記録(ライト)時の記録/再生
ギャップ13部分での発生磁界が各極性で対称になり、
非対称な場合に生ずるピークシフト(記録位置のずれ)
が防止される。
The coil 7.8 mentioned above is generally formed with bifilar winding as shown in FIG. This bifilar winding is
It is a winding method in which two conductive wires are wound as a pair, and the first coil 7 and the second coil 8 can be considered to be completely equivalent except for the difference in polarity. Therefore, the magnetic field generated at the recording/reproducing gap 13 during recording (writing) becomes symmetrical for each polarity,
Peak shift (displacement of recording position) that occurs in asymmetric cases
is prevented.

[発明が解決しようとする問題点コ しかしながら、上記従来の記録ヘッドの記録系では、第
5図に示すようにコイル7.8の結合容量Cが存在する
ために、コイル7.8と結合容量Cで共振回路が形成さ
れることになり、誘導性ノイズ源があると共振周波数の
誘導を受けやすいという問題点がある。結合容量Cはコ
イル7.8がバイファイラ巻きのため比較的大きく、一
方、上記共振回路での共振周波数f。は、コイル7.8
のインダクタンスをLとすると、 f O=1 / 2π、rττ− であり、結合容ff1Cが大きいと低くなる。最近の高
密度用のメディアおよびヘッドでは、より高い周波数の
記録/再生が可能になって来ており、最大記録周波数の
3〜5倍程度の信号は記録/再生してしまう。上記の共
振周波数f0が最大記録周波数(f 、、、、)の3〜
5倍程度であると、共振した周波数f0の誘導性ノイズ
がメディアに記録されてしまい、既に記録されている記
録面のS/Nが悪化し、再生時にエラーを引き起す原因
となる。
[Problems to be Solved by the Invention] However, in the recording system of the conventional recording head described above, since the coupling capacitance C of the coil 7.8 exists as shown in FIG. Since a resonant circuit is formed by C, there is a problem that the resonant frequency is easily induced in the presence of an inductive noise source. The coupling capacitance C is relatively large because the coil 7.8 is bifilar wound, and on the other hand, the resonant frequency f in the above-mentioned resonant circuit. is coil 7.8
If the inductance of is L, then fO=1/2π, rττ−, which becomes lower when the coupling capacity ff1C is large. Recent high-density media and heads have become capable of recording/reproducing at higher frequencies, and record/reproduce signals that are about 3 to 5 times the maximum recording frequency. The above resonance frequency f0 is 3 to 3 of the maximum recording frequency (f,,,,)
If it is about 5 times, the inductive noise of the resonant frequency f0 will be recorded on the medium, which will deteriorate the S/N of the already recorded recording surface and cause errors during reproduction.

特に両面記録用FDDにおいては、フロッピーディスク
の両サイドの磁気ヘッドが対向して配置され、一方サイ
ドのライト時にも他方サイドの磁気ヘッドは一方サイド
の磁気ヘッドといっしょに対向して移動される。従って
、ライト側の磁気ヘッドが、休止側の磁気ヘッドに対し
て誘導性ノイズ源となる。前述のように記録電流は、交
互にスイッチングされ、その結果略矩形波となるため大
きい奇数次高調波成分を有している。このため磁気ヘッ
ドが最大記録周波数f +maえの3〜5倍の高調波成
分に共振すると、前述したと同様にエラーの原因となる
。なお上記はクロストークと呼ばれている。
Particularly in double-sided recording FDDs, the magnetic heads on both sides of the floppy disk are arranged to face each other, and even when writing on one side, the magnetic head on the other side is moved together with the magnetic head on one side to face each other. Therefore, the magnetic head on the write side becomes an inductive noise source for the magnetic head on the rest side. As described above, the recording current is alternately switched, resulting in a substantially rectangular wave, and therefore has large odd harmonic components. For this reason, if the magnetic head resonates with a harmonic component of 3 to 5 times the maximum recording frequency f + ma, it causes an error as described above. Note that the above is called crosstalk.

本発明は、上記問題点を解決するためになされたもので
、磁気ヘッドの記録/再生コイルの結合容量を小さくし
て、外部あるいは両面FDDの逆サイドのヘッドなどか
らの誘導性ノイズを受けて共振してもメディアに対し記
録/再生せず、誘導性ノイズに強く、クロストークの発
生しないヘッドを得ることを目的とする。
The present invention was made in order to solve the above problems, and reduces the coupling capacitance of the recording/reproducing coil of a magnetic head to reduce inductive noise from the outside or from the head on the opposite side of a double-sided FDD. The purpose of the present invention is to obtain a head that does not record/reproduce on/from media even if it resonates, is resistant to inductive noise, and does not cause crosstalk.

[問題点を解決するための手段] 」−足口的を達成するための本発明の磁気ヘッドの構成
は、 第1のコイルと第2のコイルを備え互いに異なる方向の
記録磁束を交互に発生する磁気ヘッドにおいて、 前記第1のコイルと第2のコイルとを互いに独立して配
置したことを特徴とする。
[Means for Solving the Problems] The configuration of the magnetic head of the present invention for achieving the objective is to include a first coil and a second coil and alternately generate recording magnetic flux in different directions. The magnetic head is characterized in that the first coil and the second coil are arranged independently of each other.

[作用] 一般に2つの導体間の容量はその導体間の距離に反比例
するので、本考案は、従来のバイファイラ巻きのように
密着するのではなく、2つのコイルを分離・独立して結
合容量を小さくする。本考案は、結合容量の減少によっ
て、結合容量とコイルのインダクタンスで形成される磁
気ヘッドの共振回路の共振周波数を磁気ヘッドが記録/
再生可能な領域外に上昇させる。従って、外部の誘導性
ノイズや両面FDDにおける逆サイドの磁気ヘッドなど
からのクロストークを記録可能な周波数領域で共振して
メディアに記録したり、再生することがない。
[Function] In general, the capacitance between two conductors is inversely proportional to the distance between the conductors, so the present invention separates the two coils and independently calculates the coupling capacitance, instead of closely contacting them as in the conventional bifilar winding. Make it smaller. This invention enables the magnetic head to record/record the resonance frequency of the magnetic head's resonant circuit formed by the coupling capacitance and the inductance of the coil by reducing the coupling capacitance.
Raise it outside the renewable area. Therefore, external inductive noise and crosstalk from the magnetic head on the opposite side of a double-sided FDD will not resonate in the recordable frequency range and be recorded on or reproduced from the media.

[実施例] 以下、本発明の実施例を図面に基づいて詳細に説明する
。以下の実施例は、従来例と同様に記録/再生ヘッドが
2つのコイルを備え、切り換えによって交互に異なる方
向の記録磁束を発生する場合を示す。従って、従来例の
磁気ヘッドと同一の部分にはこれと共通の符号を付して
その説明を省略する。
[Example] Hereinafter, an example of the present invention will be described in detail based on the drawings. The following embodiment shows a case where the recording/reproducing head is provided with two coils as in the conventional example, and recording magnetic fluxes in different directions are generated alternately by switching. Therefore, the same parts as in the conventional magnetic head will be given the same reference numerals and their explanation will be omitted.

第1図は本発明の第1の実施例を示す構成図である。本
実施例での記録/再生コイル15は、ボビン16の一方
半分に巻かれた第1のコイル17と、ボビン16の略中
央部の仕切り18を隔ててボビン16の他方半分に巻か
れた第2のコイルI9とで構成され記録/再生コア4に
貫装される。
FIG. 1 is a block diagram showing a first embodiment of the present invention. The recording/reproducing coil 15 in this embodiment includes a first coil 17 wound around one half of the bobbin 16, and a first coil 17 wound around the other half of the bobbin 16 with a partition 18 in the approximate center of the bobbin 16 in between. The recording/reproducing core 4 is constructed of two coils I9 and is inserted through the recording/reproducing core 4.

上記では仕切りI8によって第1のコイル17と第2の
コイル19を分割配置としているが、それぞれのコイル
17.19を同形の2つのボビンに巻いて、シリーズに
重ねて記録/再生コア4に貫装しても良い。なお、仕切
り18は省略しても良いし、その厚みを調整することで
2つのコイル17.19の結合容量をより小さく所望の
範囲の値とすることができる。また、2つのボビンに巻
く場合は、ボビン間の空隙の距離調整によって同様に結
合容量をより小さくし、所望の範囲に抑えることができ
る。製作例によると従来的5opi’;’の結合容量を
約10pPにすることができる。
In the above example, the first coil 17 and the second coil 19 are separated by the partition I8, but each coil 17 and 19 is wound around two bobbins of the same shape, stacked in series, and passed through the recording/reproducing core 4. You can also wear it. Note that the partition 18 may be omitted, and by adjusting its thickness, the coupling capacitance between the two coils 17 and 19 can be made smaller within a desired range. Furthermore, when winding on two bobbins, the coupling capacity can be similarly made smaller and kept within a desired range by adjusting the distance of the gap between the bobbins. According to a fabrication example, the coupling capacity of the conventional 5opi';' can be reduced to about 10 pP.

この実施例では、第1のコイル17と第2のコイル19
の巻き数を同じにすればほぼ等価とみなせるので、記録
/再生ギャップI3での記録時(ライト時)の発生磁界
の非対称性は最小限に抑えられる。
In this embodiment, the first coil 17 and the second coil 19
If the number of turns is the same, it can be considered that they are almost equivalent, so the asymmetry of the generated magnetic field during recording (writing) in the recording/reproducing gap I3 can be minimized.

この実施例での他の態様として第1のコイル17の巻き
数を第2のコイル19の巻き数より大に構成する。この
ようにする理由は、高密度FDDの磁気ヘッドでは、記
録/再生ヘッド2と消去ヘッド3とは近接しており、記
録/再生ヘッド2で記録を行いながら、記録トラック両
側をトリムイレーズして一定の間隙(ガートバンド)を
生成する場合に、消去ヘッド3による消去(一般に直流
消去)磁束の干渉を受けるので、それをキャンセルする
ためである。第2図(イ)、(ロ)、(ハ)は、消去磁
束の干渉の説明図で、(イ)において第1のコイルと第
2のコイルが等価ならば第1のコイルの発生磁束Aと第
2のコイルの発生磁束Bは等しくなる。しかし消去磁束
Eの漏れ磁束E′の干渉があると、(ロ)に示すように
メディア上の記録磁化は非対称となってしまい、(ハ)
に示すように再生時においてピークシフト(点線図示位
置が正規のピーク点)が発生してしまう。そこで、前述
のように第1のコイルの巻き数を大にしてA=B+E’
 となる様に補償する。従来のバイファイラ巻きでは、
このような補償巻きは困難であったが、本実施例では独
立巻きなので容易に実施可能である。
Another aspect of this embodiment is that the number of turns of the first coil 17 is larger than the number of turns of the second coil 19. The reason for doing this is that in the magnetic head of a high-density FDD, the recording/reproducing head 2 and the erasing head 3 are close to each other, and while the recording/reproducing head 2 is recording, trim-erase is performed on both sides of the recording track. This is to cancel the interference of the erasing (generally DC erasing) magnetic flux caused by the erasing head 3 when a certain gap (guard band) is generated. Figures 2 (a), (b), and (c) are explanatory diagrams of the interference of erased magnetic flux. In (a), if the first coil and the second coil are equivalent, the generated magnetic flux A of the first coil and the magnetic flux B generated by the second coil are equal. However, if there is interference from the leakage magnetic flux E' of the erasing magnetic flux E, the recording magnetization on the medium becomes asymmetrical as shown in (b), and (c)
As shown in the figure, a peak shift occurs during playback (the position indicated by the dotted line is the normal peak point). Therefore, as mentioned above, by increasing the number of turns of the first coil, A=B+E'
We will compensate you accordingly. With conventional bifilar winding,
Although such compensation winding was difficult, it can be easily implemented in this embodiment since it is an independent winding.

第3図は、本発明の第2の実施例の構成図である。本実
施例での記録再生コイル15′はボビン16’ に第1
のコイル17’を内側に巻き、この第1のコイル17′
を取り巻く様に即ち同心状に第2のコイル19’を配置
する。しかし、2つのコイルが独立9分離して結合容量
が小さくなるものの、このままであれば第1のコイル1
7′と第2のコイル19′とは等価とはみなすことがで
きず、記録/再生ギャップ13での発生磁界に非対称が
生ずる。即ち、第2のコイル19’ は記録/再生コア
4との空隙が大きいので漏洩磁束が大きく、記録/再生
ギャップ13に磁束を放出する効率が悪いこと。また、
第2のコイルは、磁路における断面積が大きいので、比
例してインダクタンスLが大きいこと。さらに、影響は
小さいが、第2のコイルは導線の全長が長くなり直流抵
抗が太くなり、記録電流が少くなることなどによって第
2のコイル19’ の方の発生磁束が小となる。2つの
コイルによる異なる方向の記録磁束の対称性が求められ
る磁気ヘッドでは、上記の非対称を生じさせないため、
第2のコイル+9’の巻き数を第1のコイル17′の巻
き数よりも大とし、その巻き数差を適切に調整して発生
磁界を対称にする。
FIG. 3 is a block diagram of a second embodiment of the present invention. In this embodiment, the recording/reproducing coil 15' is attached to the bobbin 16'.
This first coil 17' is wound inwardly.
The second coil 19' is disposed so as to surround it, that is, concentrically. However, although the two coils are separated by 9 and the coupling capacitance is reduced, if this continues, the first coil 1
7' and the second coil 19' cannot be considered equivalent, and an asymmetry occurs in the magnetic field generated in the recording/reproducing gap 13. That is, since the gap between the second coil 19' and the recording/reproducing core 4 is large, leakage magnetic flux is large, and the efficiency of emitting magnetic flux to the recording/reproducing gap 13 is poor. Also,
Since the second coil has a large cross-sectional area in the magnetic path, the inductance L should be proportionally large. Furthermore, although the influence is small, the total length of the conductor wire of the second coil becomes longer, the direct current resistance becomes thicker, and the recording current becomes smaller, so that the magnetic flux generated in the second coil 19' becomes smaller. In a magnetic head that requires symmetry of recording magnetic flux in different directions by two coils, in order to avoid the above asymmetry,
The number of turns of the second coil +9' is made larger than the number of turns of the first coil 17', and the difference in the number of turns is appropriately adjusted to make the generated magnetic field symmetrical.

なお、第1の実施例と同様に2つのコイル間に仕切り1
8’ や空隙を設けて、結合容量をより小さく調整する
ことができる。
Note that, similarly to the first embodiment, there is a partition 1 between the two coils.
8' or a gap can be provided to adjust the coupling capacitance to a smaller value.

この第2の実施例の他の態様として、2つのコイル17
’、19′の巻き数を同数とし、この2つのコイル17
’、+9’ と消去コイルIfの極性関係を指定して、
第2図で説明した高密度FDDの磁気ヘッドにおける消
去ヘッドの干渉を補償する。第2図において、内側の第
1のコイルが発生する磁束をAとし、その外側の第2の
コイルが発生する磁束をBとなるように極性を決めるこ
とにより、内外のコイルの非対称性が消去磁束の漏洩に
よる記録磁束の非対称を相殺し、メディア」〕の磁化を
対称にする。上記において、記録磁束の非対称を相殺し
きれない場合は、2つのコイル17’、19’の巻き数
を変えるこ□とによって調整すれば良い。
Another aspect of this second embodiment is that two coils 17
', 19' have the same number of turns, and these two coils 17
', +9' and the polarity relationship of the erasing coil If,
The interference of the erase head in the magnetic head of the high-density FDD explained in FIG. 2 is compensated for. In Figure 2, by determining the polarity so that the magnetic flux generated by the first inner coil is A and the magnetic flux generated by the second outer coil is B, the asymmetry between the inner and outer coils is eliminated. This cancels the asymmetry of recording magnetic flux caused by magnetic flux leakage and makes the magnetization of the media symmetrical. In the above, if the asymmetry of the recording magnetic flux cannot be canceled out, the adjustment can be made by changing the number of turns of the two coils 17' and 19'.

第4図はライト時の記録/再生コイルに流れる記録電流
波形を示している。通常、コイルが有するインダクタン
スのため、2つのコイル間に接続される抵抗をRw。と
すると(第5図)、矩形波の立上がりの時定数τはτ=
 L / Rw。で決まるが、これにコイルの有する結
合容量Cが大きいと、点線で示すようにオーバーシュー
トが発生し記録が不安定となり、再生時にリードデータ
のゆらぎとなって現れ、エラー発生の一要因となる虞れ
がある。本実施例によれば、結合容量が減少するので、
このオーバーシュートも少くすることができ、上記エラ
ーを防止できる。
FIG. 4 shows the recording current waveform flowing through the recording/reproducing coil during writing. Usually, due to the inductance of the coils, the resistance connected between the two coils is Rw. (Figure 5), the time constant τ of the rise of the square wave is τ=
L/Rw. However, if the coupling capacitance C of the coil is large, overshoot will occur as shown by the dotted line, making recording unstable, which will appear as fluctuations in read data during playback, and become a factor in error occurrence. There is a risk. According to this embodiment, since the coupling capacitance is reduced,
This overshoot can also be reduced, and the above-mentioned error can be prevented.

上記矩形波の記録電流は奇数次高調波成分を有しており
、しかも低次数の高調波はどエネルギーが大きく、クロ
ストークを受けてエラーを発生しやすいが、本実施例で
は、記録周波数の3〜5倍を越える点に共振点を移動さ
せることで、低次のクロストークなどを防止するととも
に、共振点を記録/再生ヘッドの記録/再生可能領域外
とじてクロストークやノイズを防止する。
The above-mentioned rectangular wave recording current has odd-order harmonic components, and low-order harmonics have large energy and are likely to receive crosstalk and cause errors. By moving the resonance point to a point that exceeds 3 to 5 times, it prevents low-order crosstalk, and also prevents crosstalk and noise by moving the resonance point outside the recording/playback area of the recording/playback head. .

なお、本発明はその主旨に沿って種々の記録装置に適用
可能であり、また消去コアのない単独の磁気ヘッドにも
適用されるなど種々の実施態様を取り得るものである。
It should be noted that the present invention can be applied to various recording devices in line with the gist thereof, and can take various embodiments, such as being applied to a single magnetic head without an erasing core.

[発明の効果] 以上の説明で明らかなように、本発明の磁気ヘッドによ
れば、結合容量が小さくなることによって、誘導性ノイ
ズに強くでき、両面FDDにおいては逆サイドの磁気ヘ
ッドからのクロストークを起さないようにすることがで
きる。一方、記録電流波形のオーバーシュートが少くな
り、記録磁化が安定し、リードデータのゆらぎが少くな
って、エラー要因を減らすことができる。また、従来の
ように導線を2本対にして巻く必要がないので巻線工程
が容易になり、2つの巻き数を違えることが容易なので
、従来のバイファイラ巻きよりさらに非対称とした高密
度FDD用の小さいヘッドを得ることができる。
[Effects of the Invention] As is clear from the above description, the magnetic head of the present invention can be made resistant to inductive noise by reducing the coupling capacitance, and in a double-sided FDD, crosstalk from the magnetic head on the opposite side can be reduced. You can prevent talk from occurring. On the other hand, overshoot of the recording current waveform is reduced, recording magnetization is stabilized, fluctuations in read data are reduced, and error factors can be reduced. In addition, since there is no need to wind the conductor wires in pairs as in the past, the winding process becomes easier, and the number of turns can be easily changed, making it more asymmetrical than conventional bifilar winding for high-density FDDs. You can get a smaller head.

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

第1図は本発明の第1の実施例を示す構成図、第2図(
イ)、(ロ)、(ハ)は消去磁束の干渉の説明図、第3
図は本発明の第2の実施例の構成図、第4図はライト時
の記録電流波形図、第5図は従来の磁気ヘッドと記録系
の等価回路図、第6図は従来のコイルのバイファイラ巻
きの説明図である。 l・・・磁気ヘッド、17.17’ ・・・第1のコイ
ル、19.19′・・・第2のコイル、A、B・・・記
録磁束。 第1力大旗例ぬ1和 第1図 (イ)消に磁宋の干渉 (ロ)×ゴンアの礁イ乙 第2図 篤2の大七例の7#八圃 第3図 請は官!L、70 第4図
FIG. 1 is a configuration diagram showing a first embodiment of the present invention, and FIG. 2 (
A), (B), and (C) are explanatory diagrams of interference of erasure magnetic flux, 3rd
Figure 4 is a diagram of the configuration of the second embodiment of the present invention, Figure 4 is a recording current waveform diagram during writing, Figure 5 is an equivalent circuit diagram of a conventional magnetic head and recording system, and Figure 6 is a diagram of a conventional coil. It is an explanatory view of bifilar winding. l...Magnetic head, 17.17'...First coil, 19.19'...Second coil, A, B...Recording magnetic flux. 1st Power Great Banner Unprecedented 1 Sum Figure 1 (a) Eliminate the interference of the Sung Dynasty (b) ! L, 70 Figure 4

Claims (4)

【特許請求の範囲】[Claims] (1)第1のコイルと第2のコイルを備え互いに異なる
方向の記録磁束を交互に発生する磁気ヘッドにおいて、 前記第1のコイルと第2のコイルとを互いに独立して配
置したことを特徴とする磁気ヘッド。
(1) A magnetic head that includes a first coil and a second coil and alternately generates recording magnetic flux in mutually different directions, characterized in that the first coil and the second coil are arranged independently of each other. magnetic head.
(2)前記配置が記録磁束方向に第1のコイルと第2の
コイルとを分割した配置であることを特徴とする前記特
許請求の範囲第1項に記載の磁気ヘッド。
(2) The magnetic head according to claim 1, wherein the arrangement is such that the first coil and the second coil are divided in the recording magnetic flux direction.
(3)前記配置が第1のコイルに第2のコイルを同心状
に重ねた配置であることを特徴とする前記特許請求の範
囲第1項に記載の磁気ヘッド。
(3) The magnetic head according to claim 1, wherein the arrangement is such that a first coil and a second coil are concentrically overlapped.
(4)前記配置は第1のコイルと第2のコイルの接する
境界に結合容量調整用の仕切りまたは空隙を設けたもの
であることを特徴とする前記特許請求の範囲第1項〜第
3項のいずれかに記載の磁気ヘッド。
(4) Claims 1 to 3 above, characterized in that the arrangement is such that a partition or a gap for adjusting coupling capacity is provided at the boundary where the first coil and the second coil touch. A magnetic head according to any of the above.
JP62077199A 1987-03-30 1987-03-30 Magnetic head Expired - Lifetime JP2696831B2 (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP62077199A JP2696831B2 (en) 1987-03-30 1987-03-30 Magnetic head

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP62077199A JP2696831B2 (en) 1987-03-30 1987-03-30 Magnetic head

Related Child Applications (1)

Application Number Title Priority Date Filing Date
JP32132796A Division JP2784917B2 (en) 1996-12-02 1996-12-02 Magnetic head

Publications (2)

Publication Number Publication Date
JPS63244304A true JPS63244304A (en) 1988-10-11
JP2696831B2 JP2696831B2 (en) 1998-01-14

Family

ID=13627153

Family Applications (1)

Application Number Title Priority Date Filing Date
JP62077199A Expired - Lifetime JP2696831B2 (en) 1987-03-30 1987-03-30 Magnetic head

Country Status (1)

Country Link
JP (1) JP2696831B2 (en)

Cited By (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPH0292805U (en) * 1988-12-28 1990-07-24

Citations (6)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS59139120A (en) * 1983-01-25 1984-08-09 Seiko Epson Corp Magnetic recording device
JPS6070913U (en) * 1983-10-22 1985-05-20 ティーディーケイ株式会社 Coil bobbin for magnetic head
JPS60217511A (en) * 1984-04-12 1985-10-31 Mitsubishi Electric Corp Magnetic head
JPS61187005U (en) * 1985-05-13 1986-11-21
JPS61269212A (en) * 1985-05-24 1986-11-28 Seiko Epson Corp Magnetic head
JPS62117708U (en) * 1986-01-16 1987-07-27

Patent Citations (6)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS59139120A (en) * 1983-01-25 1984-08-09 Seiko Epson Corp Magnetic recording device
JPS6070913U (en) * 1983-10-22 1985-05-20 ティーディーケイ株式会社 Coil bobbin for magnetic head
JPS60217511A (en) * 1984-04-12 1985-10-31 Mitsubishi Electric Corp Magnetic head
JPS61187005U (en) * 1985-05-13 1986-11-21
JPS61269212A (en) * 1985-05-24 1986-11-28 Seiko Epson Corp Magnetic head
JPS62117708U (en) * 1986-01-16 1987-07-27

Cited By (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPH0292805U (en) * 1988-12-28 1990-07-24

Also Published As

Publication number Publication date
JP2696831B2 (en) 1998-01-14

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