JPH0135409B2 - - Google Patents
Info
- Publication number
- JPH0135409B2 JPH0135409B2 JP55007811A JP781180A JPH0135409B2 JP H0135409 B2 JPH0135409 B2 JP H0135409B2 JP 55007811 A JP55007811 A JP 55007811A JP 781180 A JP781180 A JP 781180A JP H0135409 B2 JPH0135409 B2 JP H0135409B2
- Authority
- JP
- Japan
- Prior art keywords
- magnetic
- magnetic field
- paint
- particles
- support
- 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
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
- G11B5/84—Processes or apparatus specially adapted for manufacturing record carriers
- G11B5/842—Coating a support with a liquid magnetic dispersion
- G11B5/845—Coating a support with a liquid magnetic dispersion in a magnetic field
Landscapes
- Chemical & Material Sciences (AREA)
- Dispersion Chemistry (AREA)
- Manufacturing Of Magnetic Record Carriers (AREA)
Description
本発明は磁気記録媒体の磁場配向方法に関す
る。
一般に磁気記録媒体は磁性粒子とバインダーの
混合物である磁性塗料をポリエステルベース等の
支持体に塗布したものが普通である。そしてこの
塗布工程において、磁性粒子の磁化容易軸を記録
トラツクの方向と一致させる、即ち磁場配向させ
る必要がある。これは磁気記録媒体の感度、出
力、S/N、その他の特性を高めるために必要な
手段であることは良く知られている。この磁場配
向方法として、磁気記録媒体の記録トラツクの方
向に磁界を発生するよう直流電磁石又は永久磁石
を配置する方法が現在一般的に用いられている。
しかるに最近のように磁性塗料中の磁性粒子の
バインダーに対する密度を上げたものや、残留磁
束密度の高い磁性粒子を使用した高性能磁気記録
媒体が要求されるようになると、磁性塗料の粘度
が上り、磁性塗料中の磁性粒子が外部磁界の方向
に動きにくくなるという欠点が出て来た。このた
め無理に外部磁界を強くすると磁性粒子が凝集を
起して塗膜の表面が荒れたり、高域感度が下ると
いう欠点が出て来る。特に残留磁束密度の大きい
磁性粒子では後者の欠点が出やすい。この問題を
解決する試みの一つに、上記の直流電磁石又は永
久磁石による主直流磁界の他に補助電磁石又は永
久磁石を製造中の磁気記録媒体に接近させて配置
し、これにより直流又は交流補助磁界を磁性塗料
中の磁性粒子に作用させて配向度を向上させる方
法が提案されている(特公昭48−13043号)。しか
し、この方法では補助磁界を発生させるのに強力
な電磁石又は永久磁石を使用しなければならない
こと、磁界分布を厳密に制御する必要があること
などの問題があり費用の上昇が避けられない。又
この方法では表面が粗化して高周波域の感度が低
下する欠点がある。
そこで本発明者等は、これらの欠点を改善する
ため鋭意研究を重ねた結果、支持体に磁性塗料を
塗布した直後に次に述べるような方法で配向させ
るとすぐれた効果を生み出すことを見出した。
即ち、配向磁場を作るために従来用いられてい
る2個の永久磁石を同極同志対向させて作つた装
置のギヤツプ内、或いはその近辺に軟磁性材料で
作つた細い棒を支持体の巾方向と平行に設置し、
その上部に支持体が軽るく接するようにして走行
させる。
つまり従来提案された補助磁石の代わりに、単
純な軟磁性棒を使用することにより表面の粗化を
防止しながら同様な配向効果を得るものである。
すなわち本発明では同極対向永久磁石の間のギヤ
ツプの中央付近に磁性塗料を塗布したばかりの磁
気記録媒体に近接させて軟磁性棒を配置し、それ
により主配向磁場の磁界を集中増強させて磁性塗
料中の磁性粒子に作用させる。このように本発明
によると複雑高価な補助磁界発生装置が不要とな
り、装置費用が大幅に低減出来、しかも配向作用
は従来の方法に比して何らの遜色もないばかりか
磁性粒子の反転回数を制限することで磁性層表面
の粗化が抑制され高周波領域の特性劣化が防げ
る。
このようにするだけで得られる記録媒体の配向
度は20〜30%向上し、オーデイオ用のカセツトテ
ープの電磁変換特性を例にとれば感度が1dB以上
改善されることがわかつた。以下実施例にて具体
的に説明する。
第1〜7図は本発明の磁場配向方法の種々の態
様を示すものであるが、第1〜2図を参照して先
ず本発明の原理を説明する。これらの図におい
て、1,2は従来磁場配向に用いられている同極
対向の永久磁石または直流電磁石であり、プラス
チツクフイルム等の支持体3とその面に塗布され
たばかりの未乾燥の磁性塗膜4とから成る磁気記
録媒体がこれら両磁石1,2の間に通される。磁
石1,2は支持体3の幅方向に延びており、磁性
塗膜4のどの部分にも同じような配向磁場が加え
られるように配置されている。本発明に従つて、
これら両磁石の間には軟質磁性材料(一般に軟磁
性材料)の棒状体5が支持体3の幅方向に、しか
も支持体3に平行に近接して配置されている。好
ましくはこの棒状体は支持体面側に配置される。
未乾燥の磁性塗膜4を担持した支持体3が矢印の
方向に移動すると、磁性塗膜4は同極対向磁石か
ら配向磁場を受ける。棒状体は対向磁石による配
向磁場の磁界によりそれと同一の方向に磁化され
てそれ自体の磁場を生じ、それにより対向磁石に
よる配向磁場の磁界をほぼ同じ方向に増強され
る。このため磁性塗膜4が棒状体5の近くを通る
ときに磁性塗料中に分散された磁性粒子は増強さ
れた磁界の作用を受ける。これによりかなり粘度
の高いバインダー中に分散された磁性粒子でもバ
インダーの粘性に打ち克つて支持体の移動方向へ
配向するものと思われる。
このようにして、本発明によると従来の磁場配
向装置では可能でなかつた大きな配向効果を達成
できる。
実施例
第1図、第2図に示すように従来から磁性粒子
の配向に用いられている同極対向型の永久磁石
1,2のギヤツプの中に1本の軟質磁性体の円柱
状の棒5(材質S45C、直径8mm、長さ200mm)を
同極対向永久磁石の磁極面に棒5の長手方向を平
行にして磁性膜4を塗布済のベース3の下側か
ら、ベース面に平行に接するように固定する。こ
の状態に固定された同極対向型永久磁石1,2の
間を、磁性膜4を塗布した未乾燥状態のベース3
を軟質磁性材料の円い棒5に接しながら通過させ
た。このようにして製作した磁気テープと、同極
対向型永久磁石1,2のみで構成された磁界の中
を磁性膜4を塗布したベース3を通過させて製作
した磁気テープ(従来法)との配向度とオーデイ
オカセツトテープの電磁変換特性とを比較した。
結果は表1に示すように軟質磁性材の円柱棒5を
置いた方が単に同極対向型永久磁石で配向したも
のより優れていた。
尚、第3図から第7図までは軟質磁性体棒5を
置く位置を変えた時の図である。この場合は、配
向度、電特共少しずつ変るが少くとも同極対向型
永久磁石のみの時よりは良い結果が得られた。
第1の結果から次ぎのことが分かる。先ず、第
3〜4図の位置に軟磁性棒がある場合、磁性塗料
中の磁性粒子は同極対向磁石の上流側(図で右
側)から次第に配向磁界の作用を受けて磁化しそ
の方向に配向する。次ぎに同極対向磁石の中央部
を通り過ぎ、反転した配向磁場の中に入ると磁化
された磁性粒子は磁界の方向に反転する。このと
き軟磁性棒5の近くを通ると主磁石による配向磁
場の磁界は軟磁性棒5により増強されているから
磁性粒子は増強された磁界に強く引かれて配向性
が向上する。次ぎに第6〜7図の位置に軟磁性棒
がある場合、磁性塗料中の磁性粒子は同極対向磁
石の上流側(図で右側)から次第に配向磁界の作
用を受けて磁化しその方向に配向し始める。この
とき軟磁性棒5の近くを通ると主磁石による配向
磁場の磁界は軟磁性棒5により増強されているか
ら磁性粒子は増強された磁界に強く引かれて強く
磁化される。次ぎに同極対向磁石の中央部を通り
過ぎ、反転した配向磁場の中に入ると磁化された
磁性粒子は磁界の方向に反転する。磁性粒子は強
く磁化されているから配向磁場の作用を強く受け
て配向性が向上する。第5図の位置(図は対向磁
石の中央に描かれているが実際は下流側寄り)で
は第3〜4図の場合と同様な作用が働いていると
考えられる。なお、上流側寄りの位置でも第6〜
7図と同様な作用が生じているものと考えられ
る。先に引用した従来(特公昭48−13043号)の
交流補助磁石では磁気記録媒体が配向磁場中を通
り過ぎる間にも磁性粒子の多数回の反転を生じ、
又直流補助磁石の場合でも反転は3回となりこれ
が磁気記録媒体の表面粗さを増大し、高周波域で
の記録再生感度を低下させる問題があるが、本発
明では反転数は1回だけであり、表面平滑性の劣
化が防止出来る。
The present invention relates to a method for magnetic field orientation of a magnetic recording medium. Generally, a magnetic recording medium is one in which a support such as a polyester base is coated with a magnetic paint, which is a mixture of magnetic particles and a binder. In this coating step, it is necessary to align the axis of easy magnetization of the magnetic particles with the direction of the recording track, that is, to align them with a magnetic field. It is well known that this is a necessary means for improving the sensitivity, output, S/N, and other characteristics of magnetic recording media. As a magnetic field orientation method, a method in which DC electromagnets or permanent magnets are arranged so as to generate a magnetic field in the direction of the recording track of a magnetic recording medium is currently commonly used. However, as there has recently been a demand for high-performance magnetic recording media that use magnetic particles with higher density relative to the binder in magnetic paints and magnetic particles with high residual magnetic flux density, the viscosity of magnetic paints has increased. However, a drawback has emerged in that the magnetic particles in the magnetic paint become difficult to move in the direction of the external magnetic field. For this reason, if the external magnetic field is forcibly strengthened, the magnetic particles will agglomerate, causing the surface of the coating to become rough and resulting in a reduction in high-frequency sensitivity. The latter drawback is particularly likely to occur in magnetic particles with a large residual magnetic flux density. One attempt to solve this problem is to place auxiliary electromagnets or permanent magnets close to the magnetic recording medium being manufactured, in addition to the main DC magnetic field generated by the above-mentioned DC electromagnets or permanent magnets. A method has been proposed in which the degree of orientation is improved by applying a magnetic field to magnetic particles in a magnetic paint (Japanese Patent Publication No. 13043/1982). However, this method has problems such as the need to use a strong electromagnet or permanent magnet to generate the auxiliary magnetic field and the need to strictly control the magnetic field distribution, which inevitably increases costs. Furthermore, this method has the disadvantage that the surface becomes rough and the sensitivity in the high frequency range decreases. The inventors of the present invention have conducted intensive research to improve these drawbacks, and have discovered that an excellent effect can be produced by orienting the magnetic paint in the following manner immediately after applying the magnetic paint to the support. . In other words, a thin rod made of a soft magnetic material is placed in or near the gap of a device conventionally used to create an orienting magnetic field, which is made by placing two permanent magnets with the same polarity facing each other in the width direction of the support. installed parallel to
The support is made to lightly touch the top of the support. In other words, by using a simple soft magnetic bar instead of the auxiliary magnet that has been proposed in the past, the same orientation effect can be obtained while preventing surface roughening.
That is, in the present invention, a soft magnetic bar is placed near the center of the gap between the same-polar facing permanent magnets, close to the magnetic recording medium that has just been coated with magnetic paint, and thereby the magnetic field of the main orientation magnetic field is intensively enhanced. Act on magnetic particles in magnetic paint. As described above, according to the present invention, there is no need for a complicated and expensive auxiliary magnetic field generating device, and the cost of the device can be significantly reduced.Moreover, the alignment effect is comparable to that of conventional methods, and the number of times the magnetic particles are reversed can be reduced. By limiting the amount, roughening of the surface of the magnetic layer can be suppressed and deterioration of characteristics in the high frequency region can be prevented. It has been found that by simply doing this, the degree of orientation of the recording medium obtained can be improved by 20 to 30%, and, taking the electromagnetic conversion characteristics of an audio cassette tape as an example, the sensitivity can be improved by more than 1 dB. This will be explained in detail in Examples below. Although FIGS. 1 to 7 show various aspects of the magnetic field orientation method of the present invention, the principle of the present invention will first be explained with reference to FIGS. 1 to 2. In these figures, 1 and 2 are permanent magnets or DC electromagnets with the same poles facing each other, which are conventionally used for magnetic field alignment, and a support 3 such as a plastic film and an undried magnetic coating film just applied to its surface. A magnetic recording medium consisting of 4 is passed between these two magnets 1 and 2. The magnets 1 and 2 extend in the width direction of the support 3 and are arranged so that a similar orienting magnetic field is applied to any part of the magnetic coating 4. According to the invention,
Between these two magnets, a rod-shaped body 5 made of a soft magnetic material (generally a soft magnetic material) is arranged in the width direction of the support 3 and parallel to and close to the support 3 . Preferably, this rod-shaped body is arranged on the support surface side.
When the support 3 carrying the undried magnetic coating film 4 moves in the direction of the arrow, the magnetic coating film 4 receives an orienting magnetic field from the magnets facing the same polarity. The rod-shaped body is magnetized in the same direction by the magnetic field of the orienting magnetic field by the opposing magnets and generates its own magnetic field, thereby enhancing the magnetic field of the orienting magnetic field by the opposing magnets in substantially the same direction. Therefore, when the magnetic coating film 4 passes close to the rod-shaped body 5, the magnetic particles dispersed in the magnetic coating material are subjected to the action of an enhanced magnetic field. It is thought that this allows even magnetic particles dispersed in a binder with a fairly high viscosity to overcome the viscosity of the binder and become oriented in the direction of movement of the support. In this way, according to the present invention, great alignment effects not possible with conventional magnetic field alignment devices can be achieved. Embodiment As shown in FIGS. 1 and 2, a cylindrical rod of soft magnetic material is placed in the gap of permanent magnets 1 and 2 of the same pole facing type, which have been conventionally used to orient magnetic particles. 5 (material: S45C, diameter 8 mm, length 200 mm) with the longitudinal direction of the rod 5 parallel to the magnetic pole surface of the permanent magnet facing the same polarity, from the bottom of the base 3 coated with the magnetic film 4, parallel to the base surface. Fix it so that it touches. A base 3 in an undried state coated with a magnetic film 4 is inserted between the permanent magnets 1 and 2 of the same polarity facing type fixed in this state.
was passed in contact with a circular rod 5 made of a soft magnetic material. The magnetic tape manufactured in this way is different from the magnetic tape manufactured by passing the base 3 coated with the magnetic film 4 through a magnetic field composed of only the permanent magnets 1 and 2 of the same polarity facing type (conventional method). The degree of orientation and electromagnetic characteristics of audio cassette tapes were compared.
As shown in Table 1, the results showed that placing the cylindrical rod 5 made of soft magnetic material was superior to simply aligning with permanent magnets of the same polarity facing type. Note that FIGS. 3 to 7 are diagrams when the position where the soft magnetic rod 5 is placed is changed. In this case, although the degree of orientation and electric characteristics changed little by little, results were at least better than when only permanent magnets were used with the same poles facing each other. The following can be seen from the first result. First, when there is a soft magnetic bar in the position shown in Figures 3 and 4, the magnetic particles in the magnetic paint are gradually magnetized by the action of the orienting magnetic field from the upstream side (right side in the figure) of the magnet facing the same polarity, and are magnetized in that direction. Orient. Next, the magnetized magnetic particles pass through the center of the magnets with the same polarity and enter the reversed orientation magnetic field, and the magnetized magnetic particles reverse in the direction of the magnetic field. At this time, when passing near the soft magnetic bar 5, the magnetic field of the orientation magnetic field by the main magnet is enhanced by the soft magnetic bar 5, so the magnetic particles are strongly attracted by the enhanced magnetic field and their orientation improves. Next, when there is a soft magnetic bar in the position shown in Figures 6 and 7, the magnetic particles in the magnetic paint are gradually magnetized by the action of the orienting magnetic field from the upstream side (right side in the figure) of the magnet facing the same polarity, and move in that direction. Begins to orient. At this time, when passing near the soft magnetic bar 5, the magnetic field of the orientation magnetic field by the main magnet is enhanced by the soft magnetic bar 5, so the magnetic particles are strongly attracted by the enhanced magnetic field and are strongly magnetized. Next, the magnetized magnetic particles pass through the center of the magnets with the same polarity and enter the reversed orientation magnetic field, and the magnetized magnetic particles reverse in the direction of the magnetic field. Since magnetic particles are strongly magnetized, they are strongly influenced by an orienting magnetic field and their orientation improves. At the position shown in FIG. 5 (the figure is drawn at the center of the opposing magnets, but actually closer to the downstream side), it is thought that the same effect as in FIGS. 3 and 4 is working. In addition, even if the position is closer to the upstream side,
It is thought that the same effect as shown in Figure 7 is occurring. In the conventional AC auxiliary magnet (Japanese Patent Publication No. 48-13043) cited earlier, the magnetic particles reverse many times even while the magnetic recording medium passes through the alignment magnetic field.
Also, in the case of a DC auxiliary magnet, the reversal occurs three times, which increases the surface roughness of the magnetic recording medium and reduces the recording and reproducing sensitivity in a high frequency range, but in the present invention, the reversal is only one time. , deterioration of surface smoothness can be prevented.
【表】
* 従来法とは同極対向型永久磁石のみ
尚、実験テープの磁場配向工程以外の製造条件
は次の通りである。
即ち、磁性塗料をベースに塗布後、通常の熱風
乾燥ゾーンを通過させて乾燥し、その後表面加工
をほどこしてからカセツト巾に切断した。又塗布
スピードは毎分60mの早さで塗布した。ベースの
厚さは12μであり、磁性塗料の塗布厚は、乾燥後
で約6μであつた。又同極対向磁石の磁界は全て
約1800ガウスにセツトして実験を行つた。
尚、この実験に用いた磁性塗料は表2に示した
原料を、ボールミルで混練、分散させて作つた。[Table] *The conventional method uses only permanent magnets with the same poles facing each other.The manufacturing conditions other than the magnetic field orientation process for the experimental tape are as follows. That is, after applying the magnetic paint to the base, it was dried by passing through a conventional hot air drying zone, and then surface-treated and cut into cassette width pieces. The coating speed was 60 m/min. The thickness of the base was 12μ, and the coating thickness of the magnetic paint was approximately 6μ after drying. In addition, the experiments were conducted with the magnetic fields of the same-polarity opposing magnets all set at approximately 1800 Gauss. The magnetic paint used in this experiment was prepared by kneading and dispersing the raw materials shown in Table 2 in a ball mill.
【表】【table】
【表】
なお、上記の実施例では棒状体5として軟鉄丸
棒を用いたが、他の任意の断面形状を有する質磁
性材料を用いることができる。例えば三角平板
状、角棒を用いても同様な結果が確認され本発明
によると、配向度20〜30%、感度dB以上の向上
が可能になりまた特に粘性の高い性塗料に対する
効果が大きい。[Table] Note that although a soft iron round bar was used as the rod-shaped body 5 in the above embodiment, a magnetic material having any other arbitrary cross-sectional shape may be used. For example, similar results have been confirmed using a triangular flat plate shape or a square rod.According to the present invention, it is possible to improve the degree of orientation by 20 to 30% and the sensitivity by dB or more, and is particularly effective for highly viscous paints.
第1図は本発明の方法を実施する磁場配向装置
の平面図、第2図は同正面図、及び第3〜7図は
本発明の方法において、軟質磁性材料の軟鉄棒の
位置を種々に変えた場合の実施態様を示す正面図
である。
FIG. 1 is a plan view of a magnetic field orientation apparatus for carrying out the method of the present invention, FIG. 2 is a front view of the same, and FIGS. FIG. 7 is a front view showing a modified embodiment.
Claims (1)
散した磁性塗料を塗布し、前記磁性塗料が未だ流
動性を保持している間に前記磁性塗料を塗布した
前記非磁性支持体を一対の同極対向磁石により形
成される主配向磁場の中を給送させて前記磁性粒
子を前記配向磁場の磁界方向に配向させる磁気記
録媒体の製造方法において、前記支持体の一方の
面に沿つて前記主配向磁場の磁界方向にほぼ直交
する方向に軟磁性体材料から成る細長い板状また
は棒状物体を配置して前記主配向磁場の磁界を増
強する補助磁場を前記磁性塗料に作用させること
を特徴とする磁気記録媒体の製造方法。1. A magnetic paint in which magnetic particles are dispersed is applied to the surface of a sheet-like non-magnetic support, and while the magnetic paint still retains fluidity, the non-magnetic support coated with the magnetic paint is coated with a pair of identical supports. In a method for manufacturing a magnetic recording medium, the magnetic particles are fed in a main alignment magnetic field formed by pole-opposed magnets to align the magnetic particles in the direction of the alignment magnetic field, wherein the main magnetic particles are fed along one surface of the support. The method is characterized in that an elongated plate-like or rod-like object made of a soft magnetic material is arranged in a direction substantially perpendicular to the direction of the magnetic field of the orienting magnetic field, and an auxiliary magnetic field that enhances the magnetic field of the main orienting magnetic field is applied to the magnetic paint. A method for manufacturing a magnetic recording medium.
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP781180A JPS56105340A (en) | 1980-01-28 | 1980-01-28 | Production of magnetic recording medium |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP781180A JPS56105340A (en) | 1980-01-28 | 1980-01-28 | Production of magnetic recording medium |
Publications (2)
| Publication Number | Publication Date |
|---|---|
| JPS56105340A JPS56105340A (en) | 1981-08-21 |
| JPH0135409B2 true JPH0135409B2 (en) | 1989-07-25 |
Family
ID=11675980
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP781180A Granted JPS56105340A (en) | 1980-01-28 | 1980-01-28 | Production of magnetic recording medium |
Country Status (1)
| Country | Link |
|---|---|
| JP (1) | JPS56105340A (en) |
-
1980
- 1980-01-28 JP JP781180A patent/JPS56105340A/en active Granted
Also Published As
| Publication number | Publication date |
|---|---|
| JPS56105340A (en) | 1981-08-21 |
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