JPH034975Y2 - - Google Patents

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Publication number
JPH034975Y2
JPH034975Y2 JP5636783U JP5636783U JPH034975Y2 JP H034975 Y2 JPH034975 Y2 JP H034975Y2 JP 5636783 U JP5636783 U JP 5636783U JP 5636783 U JP5636783 U JP 5636783U JP H034975 Y2 JPH034975 Y2 JP H034975Y2
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Japan
Prior art keywords
magnetic
recording medium
magnetic recording
head
magnetic layer
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Expired
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JP5636783U
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JPS59164934U (en
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  • Manufacturing Of Magnetic Record Carriers (AREA)

Description

【考案の詳細な説明】[Detailed explanation of the idea]

産業上の利用分野 本考案は、磁気記録媒体に関するものであり、
特に、角度あるいは回転制御に用いられる型の磁
気記録媒体に関するものである。 従来技術 従来、角度あるいは回転制御に用いられている
磁気記録媒体として、プラスチツクあるいは金属
製等の円形基体の外周部、内周部または平面部に
磁性層を施したようなものが使用されてきてい
る。これらの磁気記録媒体に対して記録又は再生
を行なう場合、磁気ヘツドあるいは磁気センサを
磁性層表面からわずかに、例えば、数μmから数
百μm離して行なうか、磁性層に対して低い圧力
で接触させて行なつていた。しかしながら、非接
触で記録、再生する場合は、安定した出力を得る
ために磁気ヘツド又はセンサと磁気記録媒体の磁
性層との間のわずかな間隙を回転中一定に保つ必
要があり、磁気記録媒体の寸法精度は、振れを防
止するため高度なものが要求され、磁気記録媒体
自体が高価なものとなつてしまうという問題があ
り、また、温度伸縮を考慮すると磁気記録媒体の
磁性層と磁気ヘツド又はセンサとの間の距離をあ
まり近づけることができず、大きな出力を得るの
が困難であるという問題もあつた。一方、磁気ヘ
ツドを磁気記録媒体の磁性層に接触させる型式で
は、連続使用の場合、磁性層およびヘツドに摩耗
が発生するという問題があつた。 考案の目的 本考案の目的は、前述したような従来技術の問
題点を解消し、寸法精度をそれ程必要とせず大き
な再生出力を得ることができしかも摩耗の極めて
少ない安価な磁気記録媒体を提供することであ
る。 考案の構成 本考案による磁気記録媒体は、基体の表面にゴ
ム硬度が30゜から90゜の磁性層を有することを特徴
とし、従つて、その磁性層が適度なゴム弾性を有
し、極くわずかな圧力でヘツドを接触させるだけ
で十分なヘツドタツチを保ち、安定した大きな出
力を得ることができるようにしている。 実施例 次に、添付図面に基づいて本考案の実施例につ
いて本考案をより詳細に説明する。 第1図は、本考案による磁気記録媒体の一実施
例を示す斜視図である。この実施例の磁気記録媒
体は、円形基体1と、この円形基体1の外周表面
に対して磁性材料とゴム弾性を有する樹脂とを混
練した材料を一体成形してなるJISK6301−1971
によるゴム硬度30゜から90゜の範囲内のある硬度を
有する磁性層2とを備えてなつている。 第2図は、本考案による磁気記録媒体の別の実
施例を示す斜視図である。この実施例の磁気記録
媒体は、円板状基体3と、この円板状基体3の上
表面に対して磁性材料とゴム弾性を有する樹脂と
を混練した材料を一体成形してなるJISK6301−
1971によるゴム硬度30゜から90゜の範囲内のある硬
度を有する磁性層4とを備えてなつている。 第1図及び第2図の実施例では、磁性層は円形
基体の外周表面や円板状基体の上表面に設けられ
ているのであるが、円筒状基体等の場合には、円
筒内周面に磁性層を形成することもでき、本考案
はこのような場合も含むものである。 次に、本考案による磁気記録媒体の製造方法の
一例について第3図を参照して説明する。 第3図に概略断面図にて示すように、金型の下
型5内に所望形状の基体6を予め設置する。基体
6の形成材料としては、変形が少ないもの、軽い
ものがよく、プラスチツク、繊維強化プラスチツ
ク、無機材料添加強化プラスチツク、金属等、例
えば、ポリフエニレンサルフアイド、ナイロン、
ポリカーボネイト、鉄、アルミニウム、銅、しん
ちゆう等でよい。次に、磁性材料とゴム弾性を有
する樹脂とを混練した材料7を、下型5の内周面
と基体6の外周面との間の空隙に充填する。この
場合、下型5の内周面には、付着防止用のシリコ
ーン等の離型材9を塗付しておくとよい。また、
磁性材料としては、特に限定されないが、粒子サ
イズの小さいものが好ましく、例えば、r−
Fe2O3、Fe3O4、Co−rFe2O3、Co−Fe3O4
CrO2、Baフエライト、Srフエライト、希土類磁
石材料(SmCo5、Sm2Co17等)が使用される。混
練するゴム弾性を有する樹脂としては、各種のゴ
ムあるいは樹脂とゴムとの混合物でよく、シリコ
ンゴム、ウレタンゴム、SBR、NBR等を使用で
き、特に、シリコーンゴムは、復元性に優れ熱、
化学的安定性の良好なことと合わせて、高性能の
磁性層を形成しうる点で好ましい。また、磁性材
料と樹脂との混練は、例えば、ニーダーや三本ロ
ールミル等の通常の混合装置で適当時間混合すれ
ばよい。その後、下型5に対して上型8をかぶせ
て、これらをヒータ10を内蔵した平圧熱プレス
11A及び11Bの間に挿入して、加圧及び加熱
することにより、樹脂を固化成形すればよい。上
型8の下面の基体6の外周付近に相当する位置に
は、混練物7の逃げ用の凹み8Aを形成しておく
とよい。 このようにして形成された磁気記録媒体を第4
図A及びBにそれぞれ平面図及び正面図にて示し
ている。 本考案の磁気記録媒体における磁性層のゴム硬
度と磁気記録媒体の偏心と出力変動との関係を調
べるため、第5図に斜視図にて示すような磁気記
録媒体を種々形成して実験してみた。第5図の磁
気記録媒体は、直径50mm、厚さ5mmの基体12の
外周面に厚さ1.5mmの磁性層13を施し、中心部
に回転軸14を固定したものである。基体12の
中心に対して回転軸14を所定量ずらして固定し
回転させ偏心の大きさを種々調整し、また、磁性
層13のゴム硬度の種々異なるものについて、磁
性層13に対して磁気ヘツドを接触させてその再
生出力を測定した結果を第6図に示している。 第6図は、磁気ヘツド接触ヘツド圧5g、記録
密度100FRPI、回転数180rpmにて測定した結果
を示すもので、横軸に振れ(偏心)量μmをとり、
縦軸に出力変動%をとつて示したものである。第
6図において、曲線Aは、磁性層13のゴム硬度
が90゜以上の場合を示し、曲線Bはゴム硬度が60゜
の場合を示し、曲線Cはゴム硬度が40゜の場合を
示し、曲線Dはゴム硬度が30゜の場合を示してい
る。 実験によると、磁性層は、ゴム硬度の低い程ヘ
ツドを接触させた場合の追随性が優れ、低いヘツ
ド圧で大きな偏心のある媒体に対しても良好なヘ
ツドタツチを示した。第6図の曲線から明らかな
ように、磁性層のゴム硬度が低い程出力変動は少
なくなつた。尚、ヘッド圧は高い程出力変動が低
下する傾向が認められた。但し、ゴム硬度が90゜
以上となるとほとんど効果が認められなかつた。
ゴム硬度と、十分なヘツドタツチを得るための最
低必要なヘツド圧とは相関があり、硬度が低い程
ヘツド圧は小となる。摩耗に関しては、ヘツド圧
が低い方が少なく有利となる場合が多いが、磁性
層のゴム硬度を大きく下げると耐摩耗性が低下す
ることもある。ゴム硬度30゜未満では機械的強度
が大きく低下する。従つて、磁性層のゴム硬度
は、用途に応じて、例えば、磁気ヘツドの接触圧
等に応じて30゜から90゜の範囲内の適当な値に選定
されるべきである。 次に、本考案による磁気記録媒体の具体的試作
例について説明しておく。 第5図に示したような形状、寸法の磁気記録媒
体を、基体12をアルミニウム、回転軸(シヤフ
ト)14を鉄、磁性層13を次のようなものとし
て作製した。 磁性層の組成:磁性体rFe2O3(MRM400戸田工
業株式会社) 60部 シリコーンゴム(KE78VBS信越化学株式
会社) 40部 ゴム硬度: 50゜ そして、この本考案による磁気記録媒体は、回
転軸を基準とした外周部の振れを10μとした。 一方、比較サンプルとして、磁性層の組成中、
シリコーンゴムの代りに不飽和ポリエステルを用
いた以外は前述の磁気記録媒体と同様のものを作
製した。 これら本考案による磁気記録媒体及び比較サン
プルについて、磁気ヘツドにて記録密度
100FRPI、回転数180rpm、ヘツド圧5gにて磁
気記録を行ない、磁気ヘツドにてヘツド圧5gに
て再生を行なつたところ、次の表に示すような結
果が得られた。シリコーンゴムは圧縮後の復元性
が優れていることから、耐候性、耐薬品性、寸法
安定性、耐熱性等の物性が良好であることも合せ
て本考案には適切な材料である。
Industrial Application Field The present invention relates to magnetic recording media.
In particular, it relates to magnetic recording media of the type used for angular or rotational control. Prior Art Conventionally, as a magnetic recording medium used for angle or rotational control, a circular base made of plastic or metal with a magnetic layer applied to the outer periphery, inner periphery, or flat surface has been used. There is. When recording or reproducing data on these magnetic recording media, the magnetic head or magnetic sensor is placed slightly away from the surface of the magnetic layer, for example, from several μm to several hundred μm, or the magnetic head or sensor is placed in contact with the magnetic layer with low pressure. I let him do it. However, when recording and reproducing without contact, it is necessary to keep a small gap between the magnetic head or sensor and the magnetic layer of the magnetic recording medium constant during rotation in order to obtain stable output. The dimensional accuracy of the magnetic recording medium is required to be highly accurate in order to prevent vibration, which poses the problem of making the magnetic recording medium itself expensive.In addition, considering temperature expansion and contraction, the magnetic layer and magnetic head of the magnetic recording medium must be highly accurate. Another problem is that the distance between the sensor and the sensor cannot be made very close, making it difficult to obtain a large output. On the other hand, in the type in which the magnetic head is brought into contact with the magnetic layer of the magnetic recording medium, there is a problem in that the magnetic layer and the head wear out when used continuously. Purpose of the invention The purpose of the invention is to solve the problems of the prior art as described above, and to provide an inexpensive magnetic recording medium that does not require much dimensional accuracy, can obtain a large reproduction output, and has extremely low wear. That's true. Structure of the invention The magnetic recording medium according to the invention is characterized by having a magnetic layer on the surface of the base with a rubber hardness of 30° to 90°. Just by bringing the heads into contact with a slight pressure, sufficient head contact is maintained and a stable and large output can be obtained. Embodiments Next, the present invention will be described in more detail with regard to embodiments of the present invention based on the accompanying drawings. FIG. 1 is a perspective view showing an embodiment of a magnetic recording medium according to the present invention. The magnetic recording medium of this embodiment is made by integrally molding a circular base 1 and a material obtained by kneading a magnetic material and a resin having rubber elasticity on the outer peripheral surface of the circular base 1 according to JISK6301-1971.
The magnetic layer 2 has a rubber hardness in the range of 30° to 90°. FIG. 2 is a perspective view showing another embodiment of the magnetic recording medium according to the present invention. The magnetic recording medium of this embodiment is JISK6301-1, which is made by integrally molding a disk-shaped substrate 3 and a material obtained by kneading a magnetic material and a resin having rubber elasticity on the upper surface of the disk-shaped substrate 3.
1971, the magnetic layer 4 has a hardness within the range of 30° to 90°. In the embodiments shown in FIGS. 1 and 2, the magnetic layer is provided on the outer peripheral surface of the circular base or the upper surface of the disc-shaped base, but in the case of a cylindrical base, etc., the magnetic layer is provided on the inner peripheral surface of the cylinder. It is also possible to form a magnetic layer on the magnetic layer, and the present invention also includes such a case. Next, an example of a method for manufacturing a magnetic recording medium according to the present invention will be described with reference to FIG. As shown in a schematic cross-sectional view in FIG. 3, a base body 6 having a desired shape is placed in advance in the lower mold 5 of the mold. The material for forming the base body 6 is preferably one that is less deformable and light, such as plastic, fiber-reinforced plastic, inorganic material-added reinforced plastic, metal, etc., such as polyphenylene sulfide, nylon, etc.
Polycarbonate, iron, aluminum, copper, steel, etc. may be used. Next, the gap between the inner circumferential surface of the lower mold 5 and the outer circumferential surface of the base body 6 is filled with a material 7 obtained by kneading a magnetic material and a resin having rubber elasticity. In this case, it is preferable to apply a mold release material 9 such as silicone to prevent adhesion on the inner peripheral surface of the lower mold 5. Also,
The magnetic material is not particularly limited, but one with a small particle size is preferable, such as r-
Fe 2 O 3 , Fe 3 O 4 , Co−rFe 2 O 3 , Co−Fe 3 O 4 ,
CrO 2 , Ba ferrite, Sr ferrite, rare earth magnet materials (SmCo 5 , Sm 2 Co 17 , etc.) are used. The resin having rubber elasticity to be kneaded may be any of various rubbers or a mixture of resin and rubber, such as silicone rubber, urethane rubber, SBR, NBR, etc. In particular, silicone rubber has excellent recovery properties and is resistant to heat and heat.
It is preferable because it has good chemical stability and can form a high-performance magnetic layer. Further, the magnetic material and the resin may be kneaded by, for example, a conventional mixing device such as a kneader or a three-roll mill for an appropriate time. After that, the upper mold 8 is placed over the lower mold 5, and these are inserted between the flat pressure heat presses 11A and 11B with a built-in heater 10, and the resin is solidified and molded by applying pressure and heating. good. It is preferable to form a recess 8A on the lower surface of the upper die 8 at a position corresponding to the vicinity of the outer periphery of the base body 6 for escape of the kneaded material 7. The magnetic recording medium thus formed was
Figures A and B show a plan view and a front view, respectively. In order to investigate the relationship between the rubber hardness of the magnetic layer in the magnetic recording medium of the present invention, the eccentricity of the magnetic recording medium, and the output fluctuation, experiments were conducted by forming various magnetic recording media as shown in the perspective view in Fig. 5. saw. The magnetic recording medium shown in FIG. 5 has a base body 12 with a diameter of 50 mm and a thickness of 5 mm, a magnetic layer 13 with a thickness of 1.5 mm on the outer peripheral surface, and a rotating shaft 14 fixed in the center. The rotating shaft 14 is fixed and rotated by shifting it by a predetermined amount with respect to the center of the base 12, and the eccentricity is adjusted in various ways. FIG. 6 shows the results of measuring the playback output by contacting the device. Figure 6 shows the results of measurements at a magnetic head contact pressure of 5 g, a recording density of 100 FRPI, and a rotation speed of 180 rpm. The horizontal axis represents the amount of runout (eccentricity) μm.
The output fluctuation percentage is plotted on the vertical axis. In FIG. 6, curve A shows the case where the rubber hardness of the magnetic layer 13 is 90° or more, curve B shows the case where the rubber hardness is 60°, curve C shows the case where the rubber hardness is 40°, Curve D shows the case where the rubber hardness is 30°. Experiments have shown that the lower the rubber hardness of the magnetic layer, the better the followability when the head is brought into contact with the magnetic layer, and the magnetic layer exhibits good head contact even with a highly eccentric medium at low head pressure. As is clear from the curve in FIG. 6, the lower the rubber hardness of the magnetic layer, the smaller the output fluctuation. It was observed that the higher the head pressure, the lower the output fluctuation. However, when the rubber hardness exceeded 90°, almost no effect was observed.
There is a correlation between rubber hardness and the minimum required head pressure to obtain sufficient head touch; the lower the hardness, the lower the head pressure. As for wear, a lower head pressure is often more advantageous, but if the rubber hardness of the magnetic layer is significantly lowered, the wear resistance may be lowered. If the rubber hardness is less than 30°, the mechanical strength will decrease significantly. Therefore, the rubber hardness of the magnetic layer should be selected to an appropriate value within the range of 30° to 90° depending on the application, for example, the contact pressure of the magnetic head. Next, a specific example of a prototype of the magnetic recording medium according to the present invention will be explained. A magnetic recording medium having the shape and dimensions shown in FIG. 5 was fabricated using aluminum for the base 12, iron for the rotating shaft 14, and magnetic layer 13 as follows. Composition of magnetic layer: Magnetic material rFe 2 O 3 (MRM400 Toda Kogyo Co., Ltd.) 60 parts Silicone rubber (KE78VBS Shin-Etsu Chemical Co., Ltd.) 40 parts Rubber hardness: 50° The magnetic recording medium according to the present invention The runout at the outer periphery was set at 10μ as a reference. On the other hand, as a comparative sample, in the composition of the magnetic layer,
A magnetic recording medium similar to the above-mentioned magnetic recording medium was prepared except that unsaturated polyester was used instead of silicone rubber. Regarding these magnetic recording media according to the present invention and comparative samples, the recording density was determined by the magnetic head.
Magnetic recording was performed at 100 FRPI, rotation speed 180 rpm, and head pressure 5 g, and reproduction was performed using a magnetic head at 5 g head pressure, and the results shown in the following table were obtained. Silicone rubber is an appropriate material for the present invention because it has excellent recovery properties after compression and also has good physical properties such as weather resistance, chemical resistance, dimensional stability, and heat resistance.

【表】 不飽和ポリエステルを用いた比較サンプルとシ
リコーンゴムを用いた本考案の磁気記録媒体とを
比較すると、前者は最高かつ均一な出力を得るた
めのヘツド位置の調整が微妙であり長時間を要し
たが、後者はほとんど微調整することなしに十分
な出力を得ることができた。これは、第7図A及
びBに媒体と磁気ヘツドとの間の関係を平面的に
示すように、硬度の高い磁性層15を有する比較
サンプルは、磁性層15と磁気ヘツド17のヘツ
ド面とが線接触となるため(第7図A参照)、わ
ずかな狂いでも空隙が生じてしまい出力低下の原
因となるが、本考案の磁気記録媒体は、磁性層1
6に適度のゴム弾性があるため磁気ヘツド17が
磁性層16に食い込む形となり(第7図B参照)、
多少の狂いは吸収してしまうため微妙なヘツド位
置決めの調整が不要となるのである。これは、本
考案の磁気記録媒体が、従来品と比較して、実装
された場合に安定した出力を得るためのヘツド位
置の調整が容易で量産性に優れていることを示し
ている。 考案の効果 前述したことから明らかなように、本考案によ
る磁気記録媒体は、接触再生方式にて使用する場
合、磁性層に適度のゴム弾性があるため、極わず
かな圧力でヘツドを接触させるだけで十分なヘツ
ドタツチが得られ、安定した書込み、読み出しが
可能となり、また、媒体が偏心していてもヘツド
に対して柔軟に対応でき、従つて、媒体の寸法精
度をそれほど高くする必要がないので、安価なも
のとすることができる。また、本考案による磁気
記録媒体を非接触再生方式にて使用する場合に
は、書込時において前述したと同様の効果が得ら
れる。 即ち、若干の偏心がある磁気ドラムを使用した
場合、書込、再生共に磁気ヘツドを非接触とする
と(書込・再生共に偏心の影響を受けて、出力変
動は重畳されて大きくなる。)、まず書込で偏心の
影響が生じ記録磁化強度はヘツドが近付いた部分
では強く、遠のいた部分では弱くなるという不均
一なものとなる上、再生に於てもヘツド・媒体間
距離の変動によつて出力が変化する。 しかしながら、本考案の磁気ドラムを使用すれ
ば若干の偏心があつても書込時にはヘツドを接触
させることができるため、記録磁化強度は全周に
渡つて強く均一となる。再生時には非接触とすれ
ばヘツド・媒体間距離が変化するため出力は変動
するが、その大きさは再生時の影響のみに限定さ
れる。 このような偏心によるレベル変動の程度を本考
案の磁気ドラムと従来の磁気ドラムとについて比
較測定した結果の一例を次の表に示す。
[Table] Comparing a comparison sample using unsaturated polyester with the magnetic recording medium of the present invention using silicone rubber, it was found that in the former, the adjustment of the head position to obtain the highest and uniform output was delicate and took a long time. However, the latter was able to obtain sufficient output with almost no fine-tuning. This is because, as shown in FIGS. 7A and 7B, which planarly shows the relationship between the medium and the magnetic head, the comparison sample having the magnetic layer 15 with high hardness has a high relationship between the magnetic layer 15 and the magnetic head 17. Since this is a line contact (see Figure 7A), even a slight deviation will create a gap and cause a decrease in output. However, in the magnetic recording medium of the present invention, the magnetic layer 1
6 has appropriate rubber elasticity, so that the magnetic head 17 bites into the magnetic layer 16 (see FIG. 7B).
Since slight deviations are absorbed, there is no need for delicate head positioning adjustments. This indicates that the magnetic recording medium of the present invention is easier to adjust the head position to obtain a stable output when mounted, and is superior in mass production than conventional products. Effects of the invention As is clear from the above, when the magnetic recording medium according to the invention is used in the contact playback method, the magnetic layer has appropriate rubber elasticity, so the head can be brought into contact with only a slight pressure. A sufficient head touch can be obtained, stable writing and reading are possible, and even if the medium is eccentric, it can be flexibly adapted to the head, and therefore the dimensional accuracy of the medium does not need to be very high. It can be made inexpensive. Further, when the magnetic recording medium according to the present invention is used in a non-contact reproduction method, the same effects as described above can be obtained during writing. That is, when using a magnetic drum with some eccentricity, if the magnetic head is made non-contact for both writing and reproducing (both writing and reproducing are affected by the eccentricity, output fluctuations are superimposed and become large). First, the influence of eccentricity occurs during writing, and the recording magnetization strength becomes uneven, strong in areas where the head approaches and weak in areas farther away.Furthermore, during playback, changes in the distance between the head and the medium cause the recorded magnetization strength to become uneven. The output changes accordingly. However, if the magnetic drum of the present invention is used, the heads can be brought into contact during writing even if there is some eccentricity, so the recording magnetization strength will be strong and uniform over the entire circumference. If non-contact is used during playback, the output will fluctuate as the distance between the head and the medium changes, but the magnitude of this will be limited only to the effect during playback. The following table shows an example of the results of comparing and measuring the degree of level fluctuation due to such eccentricity between the magnetic drum of the present invention and a conventional magnetic drum.

【表】 サンプルA:本考案の磁気ドラム:ゴム硬度60゜ サンプルB:ゴム弾性のない不飽和PETをバイ
ンダーとした磁気ドラム 尚、寸法および形状は第5図と同様。 条件:記録密度 100FRPI 回転数 180rpm ヘツド・媒体間距離:20μ(最近距離)
[Table] Sample A: Magnetic drum of the present invention: Rubber hardness 60° Sample B: Magnetic drum with binder made of unsaturated PET with no rubber elasticity The dimensions and shape are the same as in Figure 5. Conditions: Recording density 100FRPI Rotation speed 180rpm Head-medium distance: 20μ (nearest distance)

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

第1図は本考案による磁気記録媒体の一実施例
を示す斜視図、第2図は本考案による磁気記録媒
体の別の実施例を示す斜視図、第3図は本考案の
磁気記録媒体の製造方法の一例を説明するための
概略断面図、第4図A及びBは第3図に関して説
明した製造方法によつて形成された磁気記録媒体
のそれぞれ平面図及び正面図、第5図は本考案の
磁気記録媒体の性能を調べるため種々試作した磁
気記録媒体の形状を示す斜視図、第6図は第5図
に示したような磁気記録媒体について種々測定し
た結果である振れ量と出力変動との関係を示す
図、第7図Aは比較サンプルと磁気ヘツドとの関
係を示す概略平面図、第7図Bは本考案による磁
気記録媒体と磁気ヘツドとの関係を示す概略平面
図である。 1,3,6,12……基体、2,4,7,13
……磁性層、14……回転軸、15,16……磁
性層、17……磁気ヘツド。
FIG. 1 is a perspective view showing one embodiment of the magnetic recording medium according to the present invention, FIG. 2 is a perspective view showing another embodiment of the magnetic recording medium according to the present invention, and FIG. 3 is a perspective view showing the magnetic recording medium according to the present invention. A schematic sectional view for explaining an example of the manufacturing method, FIGS. 4A and 4B are a plan view and a front view, respectively, of a magnetic recording medium formed by the manufacturing method explained in connection with FIG. 3, and FIG. A perspective view showing the shapes of various trial magnetic recording media manufactured to investigate the performance of the magnetic recording media of the invention. Figure 6 shows the amount of runout and output fluctuations that are the results of various measurements on the magnetic recording media shown in Figure 5. FIG. 7A is a schematic plan view showing the relationship between the comparative sample and the magnetic head, and FIG. 7B is a schematic plan view showing the relationship between the magnetic recording medium and the magnetic head according to the present invention. . 1, 3, 6, 12...Base, 2, 4, 7, 13
...Magnetic layer, 14...Rotating shaft, 15, 16...Magnetic layer, 17...Magnetic head.

Claims (1)

【実用新案登録請求の範囲】 (1) 基体の表面にゴム硬度が30゜から90゜の磁性層
を有することを特徴とする磁気記録媒体。 (2) 前記磁性層は、磁性材料とゴム弾性を有する
樹脂とを混練した材料を前記基体表面に対して
一体成形してなるものである実用新案登録請求
の範囲第1項記載の磁気記録媒体。 (3) 前記樹脂は、シリコンゴムである実用新案登
録請求の範囲第2項記載の磁気記録媒体。
[Claims for Utility Model Registration] (1) A magnetic recording medium characterized by having a magnetic layer on the surface of a substrate with a rubber hardness of 30° to 90°. (2) The magnetic recording medium according to claim 1, wherein the magnetic layer is formed by integrally molding a material obtained by kneading a magnetic material and a resin having rubber elasticity onto the surface of the substrate. . (3) The magnetic recording medium according to claim 2, wherein the resin is silicone rubber.
JP5636783U 1983-04-15 1983-04-15 magnetic recording medium Granted JPS59164934U (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP5636783U JPS59164934U (en) 1983-04-15 1983-04-15 magnetic recording medium

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP5636783U JPS59164934U (en) 1983-04-15 1983-04-15 magnetic recording medium

Publications (2)

Publication Number Publication Date
JPS59164934U JPS59164934U (en) 1984-11-05
JPH034975Y2 true JPH034975Y2 (en) 1991-02-08

Family

ID=30186690

Family Applications (1)

Application Number Title Priority Date Filing Date
JP5636783U Granted JPS59164934U (en) 1983-04-15 1983-04-15 magnetic recording medium

Country Status (1)

Country Link
JP (1) JPS59164934U (en)

Also Published As

Publication number Publication date
JPS59164934U (en) 1984-11-05

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