JPS6030005B2 - magnetic erase head - Google Patents

magnetic erase head

Info

Publication number
JPS6030005B2
JPS6030005B2 JP20271281A JP20271281A JPS6030005B2 JP S6030005 B2 JPS6030005 B2 JP S6030005B2 JP 20271281 A JP20271281 A JP 20271281A JP 20271281 A JP20271281 A JP 20271281A JP S6030005 B2 JPS6030005 B2 JP S6030005B2
Authority
JP
Japan
Prior art keywords
magnetic
pole
tape
magnetic pole
erasing
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
Application number
JP20271281A
Other languages
Japanese (ja)
Other versions
JPS58102306A (en
Inventor
範夫 宮武
光明 上西
信男 樫村
桂造 石渡
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 JP20271281A priority Critical patent/JPS6030005B2/en
Priority to US06/449,225 priority patent/US4613919A/en
Priority to CA000417684A priority patent/CA1195773A/en
Priority to EP82111647A priority patent/EP0081855B1/en
Priority to DE8282111647T priority patent/DE3279872D1/en
Publication of JPS58102306A publication Critical patent/JPS58102306A/en
Publication of JPS6030005B2 publication Critical patent/JPS6030005B2/en
Expired legal-status Critical Current

Links

Classifications

    • GPHYSICS
    • G11INFORMATION STORAGE
    • G11BINFORMATION STORAGE BASED ON RELATIVE MOVEMENT BETWEEN RECORD CARRIER AND TRANSDUCER
    • G11B5/00Recording by magnetisation or demagnetisation of a record carrier; Reproducing by magnetic means; Record carriers therefor
    • G11B5/127Structure or manufacture of heads, e.g. inductive
    • G11B5/325Erasing heads using permanent magnets

Description

【発明の詳細な説明】 本発明は磁気記録再生装置に用いる磁気消去ヘッドに関
するものであり、その目的とするところは偶数次歪の低
減を図ることができると共にノイズの低減を図ることが
できる磁気消去ヘッドを提供することにある。
DETAILED DESCRIPTION OF THE INVENTION The present invention relates to a magnetic erase head used in a magnetic recording/reproducing device, and its purpose is to reduce even-order distortion and reduce noise. The purpose of the present invention is to provide an erasing head.

一般に、磁気テープ等の記録媒体の信号を消去する方法
として、交流消去法、直流電磁石を用いるもの、永久磁
石を用いるもの、及びそれらを複合して用いるものが知
られている。
Generally, as methods for erasing signals from recording media such as magnetic tapes, there are known AC erasing methods, methods using direct current electromagnets, methods using permanent magnets, and methods using a combination of these methods.

また、直流電磁石を用いるもの、永久磁石を用いるもの
の中には、記録媒体に飽和磁界を与える飽和消去型のも
のと、ヘッド面を走行する記録媒体に反転且つ漸減する
磁界を与える漸減交番磁界型のものとがある。従来、飽
和消去型の消去ヘッドとしては、第1図及び第2図のも
のが考えられており、第1図、第2図ではオーディオコ
ンパクトテープもしくはマイクロカセットテープ1を消
去するための永久磁石を利用したものを示している。
Among those that use DC electromagnets and those that use permanent magnets, there are saturation erasing types that apply a saturated magnetic field to the recording medium, and gradually decreasing alternating magnetic field types that apply an inverted and gradually decreasing magnetic field to the recording medium running on the head surface. There is one. Conventionally, saturation erasing type erasing heads have been considered as those shown in Figs. 1 and 2. In Figs. It shows what was used.

第1図に示す消去ヘッドは、磁石材2、非磁性材3及び
高透磁率材4とから構成されており、磁石材2のテープ
沼動面はN極もしくはS極となるように摺動面に垂直に
着磁されている。
The erasing head shown in FIG. 1 is composed of a magnetic material 2, a non-magnetic material 3, and a high permeability material 4, and the magnetic tape surface of the magnetic material 2 slides so that it becomes the north pole or the south pole. Magnetized perpendicular to the surface.

テープーが消去ヘッドと摺動することによって、その約
半幅分が一方向に着磁され、R,L両トラックの信号が
消去される。高透磁率材4は磁石材2からの磁束の広が
りを押え、磁気テープーの上半幅分のクロス消去を防止
するためのものである。このような構成の単極飽和消去
型のヘッドで消去した後のテープは、テープのB−日カ
ーブで見れば、第3図の点30もしくは点32に着磁さ
れてものである。従って、このように飽和着磁消去され
たテープを用いて記録再生を行うと、磁気テープが磁気
中性点31に消磁されない為、偶数次歪の発生と、ノイ
ズレベルが高いという問題があった。第2図に示す消去
ヘッドは、主に上記した単極飽和消去ヘッドの偶数次歪
の問題を解決する構造のもので、磁石材5,6,7,8
,9と非磁性材3、及び高透磁率村4が積層された構成
となっている。上記磁石材5〜9のうち磁石材5,7,
9の組と、磁石材6,8の組はそのテープ摺動面の極性
が図示しているように互いに逆極性N,S,Nとなるよ
うに構成されている。このように構成することによって
、例えばテープ1のRトラックの中心部分は磁石材6の
S極で着磁され、第3図のB−日カーブで言えば、点3
2に着磁される。一方Rトラックの両端の部分は磁石材
5,7のN極で着滋されるため、同じく第3図のB−日
カーブで言えば点301こ着磁される。磁石材6の幅が
Rトラック幅の約1′2であれば、テープ1が上下に少
々うねって摺動走行しても、Rトラックの約半分は、点
301こ着磁され、残りの約半分は点32に着磁される
。同様にテープ1のLトラックは磁石材7,8,9にて
看磁される。上記のように着磁されたテープを用いて記
録再生した場合、各点30及び32に着磁されたテープ
部から発生する偶数次歪は互いに逆相となる為に打消さ
れ、標準レベルで記録再生した時の歪率は3%以下に抑
えることが可能である。しかし、上記の従来の消去ヘッ
ドは、ノイズ成分が多いという次点を有している。すな
わち、このノイズを一般にDC消去ノイズを言い、テー
プの粒子寸法にバラッキが多い場合、あるいは粒子の分
散性が悪い場合に顕著となる。そして、上記の飽和消去
型では一定磁界強度でテープ中の粒子を飽和磁化させる
ため、磁気中性点を消去する交流消去法に比べ、粒子寸
法及び分散性の影響を大きく受け、ノイズが多いという
大きな欠点であった。つまり、上述した第1図の消去ヘ
ッドではコスト面では安価であるが、偶数次歪が多く、
またノイズも多いという欠点を有し、一方、上述した第
2図の消去ヘッドは、偶数次歪の点では良好であるが、
ノイズの点では改善されていないという欠点を有してい
る。
When the tape slides against the erasing head, about half its width is magnetized in one direction, and the signals on both the R and L tracks are erased. The high magnetic permeability material 4 suppresses the spread of magnetic flux from the magnet material 2 and prevents cross erasure over the upper half width of the magnetic tape. After erasing with a single-pole saturation erasing head having such a configuration, the tape is magnetized at point 30 or point 32 in FIG. 3 when viewed from the B-day curve of the tape. Therefore, when recording and reproducing are performed using a tape that has been saturated and magnetized and erased in this way, the magnetic tape is not demagnetized to the magnetic neutral point 31, so there are problems in that even-order distortion occurs and the noise level is high. . The erase head shown in FIG. 2 has a structure that mainly solves the problem of even order distortion of the unipolar saturation erase head described above, and has magnet materials 5, 6, 7, 8
, 9, a non-magnetic material 3, and a high magnetic permeability layer 4 are laminated. Among the above magnet materials 5 to 9, magnet materials 5, 7,
The set 9 and the set of magnets 6 and 8 are constructed so that the polarities of their tape sliding surfaces are mutually opposite polarities N, S, and N, as shown. With this configuration, for example, the center part of the R track of the tape 1 is magnetized by the S pole of the magnet material 6, and in terms of the B-day curve in FIG.
It is magnetized to 2. On the other hand, since both ends of the R track are magnetized by the N poles of the magnets 5 and 7, points 301 on the B-day curve in FIG. 3 are also magnetized. If the width of the magnet material 6 is about 1'2 of the R track width, even if the tape 1 slides slightly up and down, about half of the R track will be magnetized at 301 points, and the remaining about 301 points will be magnetized. Half is magnetized to point 32. Similarly, the L track of the tape 1 is magnetized by magnets 7, 8, and 9. When recording and reproducing using a tape magnetized as described above, even-order distortion generated from the tape portion magnetized at each point 30 and 32 is canceled out because they are in opposite phases to each other, and recording is performed at the standard level. The distortion rate during reproduction can be suppressed to 3% or less. However, the conventional erasing head described above has the runner-up point of having a large number of noise components. That is, this noise is generally referred to as DC erase noise, and becomes noticeable when there is a large variation in particle size of the tape or when the dispersibility of the particles is poor. In the above-mentioned saturation erasing method, the particles in the tape are saturated and magnetized with a constant magnetic field strength, so compared to the AC erasing method that erases the magnetic neutral point, it is greatly affected by particle size and dispersion, resulting in more noise. This was a major drawback. In other words, although the erasing head shown in FIG.
It also has the disadvantage of a lot of noise.On the other hand, the erasing head shown in FIG. 2 described above is good in terms of even-order distortion, but
It has the disadvantage of not being improved in terms of noise.

本発明はこのような従来の欠点を解消するものであり、
磁気記録媒体に対して先行および後行する3個以上の磁
極を設け、第1の磁極は磁気記録媒体を飽和させるに十
分な磁界強度を有し、この第1の磁極に続行する最終磁
極以外の第2以降の磁極はそれに先行する磁極と逆檀性
で弱い磁界強度を有し、最終磁極は磁気記録媒体のトラ
ック幅方向に磁極分割したものである。
The present invention solves these conventional drawbacks,
Three or more magnetic poles are provided leading and trailing to the magnetic recording medium, the first magnetic pole has a magnetic field strength sufficient to saturate the magnetic recording medium, and any magnetic pole other than the final magnetic pole following the first magnetic pole is provided. The second and subsequent magnetic poles have a weak magnetic field strength that is opposite to the preceding magnetic pole, and the final magnetic pole is divided into magnetic poles in the track width direction of the magnetic recording medium.

かかる構成によれば、偶数次歪は勿論少くすることがで
き、ノィズの点でも改良された消去ヘッドを提供するこ
とができるものである。以下、本発明の磁気消去ヘッド
の実施例について説明する。
According to such a configuration, even-order distortion can of course be reduced, and an erasing head improved in terms of noise can also be provided. Embodiments of the magnetic erasing head of the present invention will be described below.

第4図は本発明の磁気消去ヘッドの一実施例を示してお
り、第4図において、1はコンパクトカセット用もしく
はマイクロカセット用の磁気テープで、その走行方向を
矢印40で示し、消去すべきR,Lトラックを各々記号
R,Lで示している。41は非磁性材で、テープーの消
去しない側の約半幅相当部が接する。
FIG. 4 shows an embodiment of the magnetic erasing head of the present invention. In FIG. 4, reference numeral 1 denotes a magnetic tape for compact cassettes or micro cassettes, the running direction of which is indicated by arrow 40, and the tape to be erased. The R and L tracks are indicated by symbols R and L, respectively. 41 is a non-magnetic material, which is in contact with a portion corresponding to about half the width of the non-erasing side of the tape.

42はクロス消去を防止するためのシールド板で、パー
マロィ等の高透磁率材を用いている。
42 is a shield plate for preventing cross erasing, and is made of a high magnetic permeability material such as permalloy.

43,44,45は各々第1磁極、第2磁極、最終磁極
で、第1磁極43は磁気テープ1の消去すべき幅以上の
高さを有し、その磁界強度は磁気テープを十分に飽和さ
せる値を有するものである。
43, 44, and 45 are a first magnetic pole, a second magnetic pole, and a final magnetic pole, respectively, and the first magnetic pole 43 has a height greater than the width of the magnetic tape 1 to be erased, and its magnetic field strength saturates the magnetic tape sufficiently. It has the value of

第2磁極44は第1磁極と同じく磁気テープーの消去す
べき幅以上の高さを有し、その磁極は第1磁極と逆極性
を有し、磁極強さは第1磁極より小さく且つ消去すべき
テープの抗磁力よりも大なる値を有している。テープー
が最終に当接する最終磁極45はテープ幅方向に複数の
磁極から構成されたもので、ここではシールド板42を
除いて下からN,S,N,S,NあるいはS,N,S,
N,Sとなる5極の磁極46,47,48,49,50
から構成されており、その各磁極46〜50の強さは第
2磁極44の強さと略等しいか、又はそれよりも弱い値
を有するものである。上記最終磁極45はあらかじめ着
磁した磁石材を重ね合せてテープ摺動面でN,S,N,
・…・・の磁極が現われるようにしたもの、あるいは磁
石材と高透磁率材を交互に配して着磁し、磁石材を例え
ばN極、高透磁率材のテープ摺動面に誘起される磁極が
S極となるようにしたものである。ここでは高透磁率材
47,49、磁石材46,48,50の組み合せで構成
した場合の例を示してある。また高透磁率材47,49
の厚みはテープ1のR,L各トラックの約半幅で、その
位置は各トラックの中心部にあり、テープが上下に蛇行
してもトラックの約言相当部がN極で、また残り享がS
極で着磁されるよう構成している。したがって、消去後
のテープはR,L各トラツク内の残留磁化は互いに打消
す向きに向いており、その比は1:1のため、偶数次歪
が発生しないという効果を有する。
Like the first magnetic pole, the second magnetic pole 44 has a height greater than the width of the magnetic tape to be erased, has opposite polarity to the first magnetic pole, and has a magnetic pole strength smaller than that of the first magnetic pole and erased. It has a larger value than the coercive force of the magnetic tape. The final magnetic pole 45, which the tape finally comes into contact with, is composed of a plurality of magnetic poles in the width direction of the tape.
5 magnetic poles N, S 46, 47, 48, 49, 50
The strength of each of the magnetic poles 46 to 50 is approximately equal to or weaker than the strength of the second magnetic pole 44. The final magnetic pole 45 is made by stacking magnet materials that have been magnetized in advance, and forming N, S, N,
The magnetic pole of ...... is made to appear, or the magnetic material and the high magnetic permeability material are arranged alternately and magnetized, and the magnetic material is induced to the N pole, for example, to the tape sliding surface of the high magnetic permeability material. The magnetic pole is the south pole. Here, an example is shown in which a combination of high magnetic permeability materials 47, 49 and magnet materials 46, 48, 50 is used. Also, high magnetic permeability materials 47, 49
The thickness of the tape is approximately half the width of the R and L tracks of tape 1, and its position is at the center of each track, so even if the tape meanders up and down, the part corresponding to the front part of the track is the north pole, and the remaining part of the track is the north pole. S
It is configured to be magnetized at the poles. Therefore, the residual magnetization in the R and L tracks of the tape after erasing is oriented in a direction that cancels each other out, and the ratio is 1:1, which has the effect that even-order distortion does not occur.

また、上述のように磁極配列して構成した消去ヘッドは
、従来の飽和消去型の消去へ.ッド‘こ比して、DC消
去ノイズが少いという長所を有する。その理由を第5図
、第6図を用いて説明する。第5図は消去しようちする
磁気テープのB−日カーブを、第6図は本例の消去ヘッ
ドの各磁極の磁界強度を図示したものである。第5図に
おいて、51は第1磁極43の磁界強度、52は第2磁
極44の磁界強度である。53,54は各々最終磁極4
5の磁界強度で、53は磁石材46,48,50のテー
プ摺動部の磁界強度、54は高透磁率材のテープ摺動部
での磁界強度を示している。
In addition, the erase head configured with magnetic poles arranged as described above can be used for conventional saturation erase type erasing. It has the advantage of less DC erasure noise compared to the standard. The reason for this will be explained using FIGS. 5 and 6. FIG. 5 shows the B-day curve of the magnetic tape being erased, and FIG. 6 shows the magnetic field strength of each magnetic pole of the erasing head of this example. In FIG. 5, 51 is the magnetic field strength of the first magnetic pole 43, and 52 is the magnetic field strength of the second magnetic pole 44. 53 and 54 are respectively the final magnetic poles 4
5, 53 indicates the magnetic field strength at the tape sliding portion of the magnet materials 46, 48, and 50, and 54 indicates the magnetic field strength at the tape sliding portion of the high magnetic permeability material.

逆に53は高透磁率材の、また54は磁石材の摺動部で
の磁界強度となるように着滋を逆にしてもよく、いずれ
にしてもテープ1のR,L各トラックの約事相当分は磁
界51,52,53を受け、残り約事相当分が磁界5・
,52,54を受ける。磁気テープが各磁界強度51,
52,53を受けると、磁気テープの初期状態でどのよ
うな残留磁化があろうとも磁界51で磁気テープは飽和
し、B−日カーブ上で点55になり、次に各磁界52,
53で各点56,57,58,59,60を通り、最終
的に点61で示した残留磁化となる。一方、各磁界51
,52,54を受けた場合には点55,56,57,5
8を通り、その後、また第3象限57近傍にもどり、最
終的に点59近傍に終ちつく。したがって、本例の消去
ヘッドで消去した場合、残留磁化は点61と59に存在
し、従来の消去ヘッドで消去した場合の残留磁化30,
32(第3図参照)に比して小さい値とすることができ
る。DCノイズはテープの粒子分布に粗密があったり、
粒子サイズに大小が著しい場合に大きくなり、飽和着磁
状態に近づくほどそのレベルが高くなる。本例の消去ヘ
ッドでは残留磁化を上述のように4・さくするため、従
釆の飽和消去型の磁気ヘッドよりもDCノイズが4・さ
いという利点を有している。また第2磁極44、最終磁
極45の磁界強度52,53,54を適当な値に設定す
れば、残留磁化61,59は更に小さい値とすることが
可能である。更に本例の消去ヘッドは残留磁化61,5
9が各々零近くにならなくとも、残留磁化61と59の
値が各々十と−であるから相互打消し‘こより偶数次歪
の発生がきわめて少いという従来のトラック分割方式の
着磁消去ヘッド(第2図参照)と同様の利点をも合せ持
っている。尚、以上の説明では第1、第2、最終の計3
つの磁極を有する消去ヘッドの例を示したが、これは3
極に限るものではなく、最終磁極以外は漸減の磁界分布
となる磁極構成、つまり4極以上を有する消去ヘッドも
実現可能である。
On the other hand, the magnetic field intensity may be reversed so that the magnetic field strength at the sliding part 53 is made of a high magnetic permeability material and the sliding part 54 is made of a magnet material. The portion corresponding to the matter receives magnetic fields 51, 52, and 53, and the remaining portion corresponding to the matter receives the magnetic field 5.
, 52, 54. The magnetic tape has a magnetic field strength of 51,
52, 53, the magnetic tape is saturated by the magnetic field 51, no matter what residual magnetization there is in the initial state of the magnetic tape, resulting in a point 55 on the B-day curve, and then each magnetic field 52,
53, it passes through points 56, 57, 58, 59, and 60, and finally becomes the residual magnetization shown at point 61. On the other hand, each magnetic field 51
, 52, 54, points 55, 56, 57, 5
8, then returns to the vicinity of the third quadrant 57, and finally ends in the vicinity of the point 59. Therefore, when erasing with the erase head of this example, residual magnetization exists at points 61 and 59, and when erasing with the conventional erase head, residual magnetization exists at points 61 and 59.
32 (see FIG. 3). DC noise can be caused by uneven distribution of particles on the tape,
It becomes large when the particle size is significantly different in size, and the level becomes higher as the saturation magnetization state is approached. In the erase head of this example, the residual magnetization is reduced by 4.degree. as described above, so it has the advantage that the DC noise is 4.degree. smaller than the conventional saturation erase type magnetic head. Further, by setting the magnetic field strengths 52, 53, 54 of the second magnetic pole 44 and the final magnetic pole 45 to appropriate values, the residual magnetizations 61, 59 can be made even smaller. Furthermore, the erase head of this example has a residual magnetization of 61,5
Even if 9 does not approach zero, the values of residual magnetization 61 and 59 are 0 and -, respectively, so they cancel each other out, so even-order distortion is extremely unlikely to occur. It also has the same advantages as (see Figure 2). In addition, in the above explanation, the first, second, and final three
An example of an erase head with one magnetic pole was shown;
The present invention is not limited to magnetic poles, and it is also possible to realize an erase head having a magnetic pole configuration in which the magnetic field distribution is gradually decreasing except for the final magnetic pole, that is, an erase head having four or more poles.

以上のように本発明によれば、磁気記録媒体に対して先
行および後行する3個以上の磁極を設け、第1の磁極は
磁気記録媒体を飽和させるに十分な磁界強度を有せしめ
ると共にこの第1の磁極に続行する最終磁極以外の第2
以降の磁極はそれに先行する磁極と逆磁性で弱い磁界強
度を有せしめ、最終磁極は磁気記録媒体のトラック中方
向に磁極分割したので、偶数次歪を低減すると共に著し
くノイズの低減を図ることができる利点を有するもので
ある。
As described above, according to the present invention, three or more magnetic poles are provided leading and trailing to a magnetic recording medium, and the first magnetic pole has a magnetic field strength sufficient to saturate the magnetic recording medium, and the first magnetic pole has a magnetic field strength sufficient to saturate the magnetic recording medium. A second pole other than the last pole following the first pole
The subsequent magnetic poles have a weak magnetic field strength due to their opposite magnetism to the preceding magnetic poles, and the final magnetic pole is divided into magnetic poles in the direction of the track of the magnetic recording medium, which reduces even-order distortion and significantly reduces noise. It has the advantage of being able to

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

第1図、第2図は従来の永久磁石消去ヘッドの構成斜視
図、第3図は飽和消去後の残留磁化を示す磁気テープの
B一日カーブ図、第4図は本発明の永久磁石消去ヘッド
の一実施例を示す構成斜視図、第5図は同ヘッドでの磁
界強度を受けた時のテープの状態を示すB一日カーブ図
、第6図は同ヘッドでの磁界強度の分布図である。 1・・…・磁気テープ、42・・・・・・高透磁率材、
43,44,45・・・・・・各々第1、第2、および
最終磁極、46,48,50・・・・・・最終磁極の磁
石材、47,49……最終磁極の高透磁率材。 第1図 第2図 第3図 第4図 第5図 第6図
Figures 1 and 2 are perspective views of the configuration of a conventional permanent magnet erasing head, Figure 3 is a B-day curve diagram of a magnetic tape showing residual magnetization after saturation erasing, and Figure 4 is a permanent magnet erasing head according to the present invention. A perspective view of the configuration of an embodiment of the head, FIG. 5 is a B-day curve diagram showing the state of the tape when subjected to magnetic field strength in the same head, and FIG. 6 is a distribution diagram of the magnetic field strength in the same head. It is. 1...magnetic tape, 42...high magnetic permeability material,
43, 44, 45... First, second, and final magnetic poles respectively, 46, 48, 50... Magnet material of the final magnetic pole, 47, 49... High magnetic permeability of the final magnetic pole. Material. Figure 1 Figure 2 Figure 3 Figure 4 Figure 5 Figure 6

Claims (1)

【特許請求の範囲】 1 磁気記録媒体に対して先行及び後行する3個以上の
磁極を設け、第1の磁極は上記磁気記録媒体を飽和させ
るに十分な磁界強度を有せしめると共にこの第1磁極に
続行する最終磁極以外の第2以降の磁極はそれに先行す
る磁極と逆極性で弱い磁界強度を有せしめ、最終磁極は
トラツク幅方向に分割磁極としてなる磁気消去ヘツド。 2 最終磁極は、永久磁石材料と高透磁率材の磁気記録
媒体の幅方向への積層構造体からなることを特徴とする
特許請求の範囲第1項記載の磁気消去ヘツド。
[Claims] 1. Three or more magnetic poles are provided leading and trailing to the magnetic recording medium, and the first magnetic pole has a magnetic field strength sufficient to saturate the magnetic recording medium, and the first magnetic pole has a magnetic field strength sufficient to saturate the magnetic recording medium. A magnetic erasing head in which the second and subsequent magnetic poles other than the final magnetic pole that follow the magnetic pole have opposite polarity to the preceding magnetic pole and have a weak magnetic field strength, and the final magnetic pole is a divided magnetic pole in the track width direction. 2. The magnetic erasing head according to claim 1, wherein the final magnetic pole is made of a laminated structure in the width direction of the magnetic recording medium of a permanent magnet material and a high magnetic permeability material.
JP20271281A 1981-12-15 1981-12-15 magnetic erase head Expired JPS6030005B2 (en)

Priority Applications (5)

Application Number Priority Date Filing Date Title
JP20271281A JPS6030005B2 (en) 1981-12-15 1981-12-15 magnetic erase head
US06/449,225 US4613919A (en) 1981-12-15 1982-12-13 Magnetic erasing head
CA000417684A CA1195773A (en) 1981-12-15 1982-12-14 Magnetic erasing head
EP82111647A EP0081855B1 (en) 1981-12-15 1982-12-15 Magnetic erasing head
DE8282111647T DE3279872D1 (en) 1981-12-15 1982-12-15 Magnetic erasing head

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP20271281A JPS6030005B2 (en) 1981-12-15 1981-12-15 magnetic erase head

Publications (2)

Publication Number Publication Date
JPS58102306A JPS58102306A (en) 1983-06-17
JPS6030005B2 true JPS6030005B2 (en) 1985-07-13

Family

ID=16461898

Family Applications (1)

Application Number Title Priority Date Filing Date
JP20271281A Expired JPS6030005B2 (en) 1981-12-15 1981-12-15 magnetic erase head

Country Status (1)

Country Link
JP (1) JPS6030005B2 (en)

Also Published As

Publication number Publication date
JPS58102306A (en) 1983-06-17

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