JPS63148417A - Production of magnetic recording medium - Google Patents

Production of magnetic recording medium

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Publication number
JPS63148417A
JPS63148417A JP29349386A JP29349386A JPS63148417A JP S63148417 A JPS63148417 A JP S63148417A JP 29349386 A JP29349386 A JP 29349386A JP 29349386 A JP29349386 A JP 29349386A JP S63148417 A JPS63148417 A JP S63148417A
Authority
JP
Japan
Prior art keywords
magnetic
magnetic field
recording medium
magnetic recording
frequency
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
JP29349386A
Other languages
Japanese (ja)
Other versions
JPH0640388B2 (en
Inventor
Kazunori Komatsu
和則 小松
Tsunehiko Sato
佐藤 恒彦
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.)
Fujifilm Holdings Corp
Original Assignee
Fuji Photo Film 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 Fuji Photo Film Co Ltd filed Critical Fuji Photo Film Co Ltd
Priority to JP29349386A priority Critical patent/JPH0640388B2/en
Publication of JPS63148417A publication Critical patent/JPS63148417A/en
Publication of JPH0640388B2 publication Critical patent/JPH0640388B2/en
Anticipated expiration legal-status Critical
Expired - Lifetime legal-status Critical Current

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  • Manufacturing Of Magnetic Record Carriers (AREA)

Abstract

PURPOSE:To ensure the stable production of a magnetic recording medium of high quality by setting a range of magnetic field intensity and at the same time setting variably the relationship between the frequency (Hz) and the applying speed within a specific range to easily set a satisfactory random orientation treatment. CONSTITUTION:The magnetic grains are orientated at random in their undried states by a frequency variable AC magnetic field generating device 4 for a magnetic liquid applied on a nonmagnetic supporter 2. In this case, the frequency (Hz) produced by the device 4 is set so that the absolute numeric value is variable within a 0.1-1 range against the traveling speed, i.e., the passing speed (m/min) in the device of the supporter 2. At the same time, the intensity of an AC magnetic field to be applied is set within a 0.1-1 range of the reluctance force of a magnetic material. Under such conditions, an orientation process is carried out. Then, an undried magnetic application layer is dried and hardened through a drying device 5. Thus, a sheet type magnetic recording medium is obtained. In such a way, the random orientation process is easily set even in a production mode of various magnetic recording media. Then, it is possible to obtain a magnetic recording medium of the stable quality.

Description

【発明の詳細な説明】 (産業上の利用分野) 本発明は磁気記録媒体の製法に関するものであり、特に
フロッピーディスク等の塗布型ディスク媒体を製造する
場合に適用して好適な磁気記録媒体の製造方法に関する
ものである。
Detailed Description of the Invention (Field of Industrial Application) The present invention relates to a method for manufacturing a magnetic recording medium, and in particular to a method for manufacturing a magnetic recording medium suitable for manufacturing a coated disk medium such as a floppy disk. This relates to a manufacturing method.

(従来の技術) 磁気ディスクや磁気テープ等の磁気記録媒体は、一般に
、帯状の非磁性支持体をその長手方向に連続移送しなが
ら該支持体上に、溶剤により溶解された結合剤中に強磁
性微粒子を分散させてなる磁性液を塗着し1次いで上記
磁性液を乾燥固化させたのち支持体を打抜きあるいは裁
断して製造されている。
(Prior Art) Magnetic recording media such as magnetic disks and magnetic tapes generally have a strip-shaped non-magnetic support that is continuously transported in the longitudinal direction of the support while being strongly immersed in a binder dissolved in a solvent. It is manufactured by applying a magnetic liquid containing magnetic fine particles dispersed therein, then drying and solidifying the magnetic liquid, and then punching or cutting the support.

ところが、磁気ディスクの製造においては、製造中に強
磁性微粒子が特定方向に配列され磁気記録媒体に異方性
が生ずると、種々の方向に対する磁気特性および電気特
性にも異方性が生ずる。例えば、磁性粒子が磁性液塗布
方向(すなわち非磁性支持体の移送方向)K沿って配列
されると、特に、磁気ディスクの場合のように磁気ヘッ
ト9が直線的に走査するのではなく1円周方向に同心円
状に走査する場合には、この塗布方向の再生出力信号レ
ベルが他方向のそれに比して高くなり、その結果、該磁
気ディスクから読み取られる再生出力信号レベルはディ
スクの回転に従って変化する(この現象は一般にモジュ
レーションと称されている)。特に、磁性層の塗布厚を
薄くしたり、塗布スピードを速くしたりした場合には磁
性粒子が機械的影響を受は易く、特定方向に配向処理さ
れたような状態が高い割合で発生する。したがって従来
より磁気ディスク等を製造する場合には、磁性液塗布時
の流動配向により磁性粒子に直線的方向性が生じるとい
う前記のような問題を解決するため、磁性液が未乾燥中
に磁界を作用させて、磁性粒子の配向を無秩序化(ラン
ダマイズ化b>させる方法がとられている。上述の様に
、磁性液が未乾燥中に磁界を作用させる方法として、特
開昭57−198545号公報に開示されているような
交流磁場を印加する方法が知られている。
However, in the manufacture of magnetic disks, if ferromagnetic particles are arranged in a particular direction during manufacture and anisotropy occurs in the magnetic recording medium, anisotropy also occurs in the magnetic and electrical properties in various directions. For example, if the magnetic particles are arranged along the direction K of applying the magnetic liquid (i.e. the direction of transport of the non-magnetic support), the magnetic head 9 does not scan linearly as in the case of a magnetic disk, but in a circular direction. When scanning concentrically in the circumferential direction, the reproduction output signal level in this coating direction is higher than that in the other direction, and as a result, the reproduction output signal level read from the magnetic disk changes as the disk rotates. (This phenomenon is generally called modulation.) In particular, when the coating thickness of the magnetic layer is reduced or the coating speed is increased, the magnetic particles are susceptible to mechanical effects, and a state in which they appear to be oriented in a specific direction occurs at a high rate. Therefore, in the conventional manufacturing of magnetic disks, etc., in order to solve the above-mentioned problem of linear orientation of magnetic particles caused by the flow orientation during magnetic liquid application, a magnetic field is applied while the magnetic liquid is not dry. As mentioned above, a method of applying a magnetic field to a magnetic liquid while it is not dry is disclosed in Japanese Patent Application Laid-open No. 198545/1983. A method of applying an alternating magnetic field as disclosed in the publication is known.

(発明が解決しようとする問題点) ところが上述の交流磁場によるランダム配向処理を磁気
記録媒体の製造方法に適用した場合、液組成および塗布
スピードの影響を受け、これらが変わるとランダム配向
処理がうまく行かない事が判明した。また、同一組成の
液でも1分散状態・磁性粉末の磁気的特性等の微妙な変
化によって完全に?ンダマイズ化するための磁場条件が
変化してしまい、安定したランダム配向処理が出来ない
事が判明した。
(Problem to be Solved by the Invention) However, when the above-mentioned random orientation treatment using an alternating magnetic field is applied to a method for manufacturing a magnetic recording medium, it is affected by the liquid composition and coating speed, and if these changes, the random orientation treatment may not work properly. It turned out that I wasn't going. Also, even if the liquid has the same composition, it may be completely different due to subtle changes in the dispersion state or magnetic properties of the magnetic powder. It was found that the magnetic field conditions for randomization changed, making stable random orientation processing impossible.

そこで、これらの原因をつきとめてみると、まず第一の
問題においては、液組成および塗布スビ−y<支持体走
行速度)に対し【最適周波数が存在する事が判明した。
When these causes were ascertained, it was found that for the first problem, there is an optimum frequency for the liquid composition and coating speed, y<support running speed.

すなわち1周波数が高過ぎると磁場の変化に磁性体の動
ぎが追従°できなくなり、印加磁場の方向と垂直な向き
(長手方向への磁場印加に対して、横方向)へ磁性体が
揃ってしまい、また逆に周波数が低過ぎると磁場印加方
向に磁性体が揃ってしまうためである事が判明した。
In other words, if one frequency is too high, the movement of the magnetic body will not be able to follow changes in the magnetic field, and the magnetic body will align in a direction perpendicular to the direction of the applied magnetic field (in the lateral direction relative to the longitudinal direction of the magnetic field applied). It turned out that this is because, conversely, if the frequency is too low, the magnetic material aligns in the direction of the magnetic field application.

また、第二の問題においては、液組成と磁場強度とのバ
ランス点でランダマイズ化するため分散状態・磁性粉末
の磁気的特性等の液物性の微妙な変化の影響を受けやす
いためである事が判明した。
In addition, regarding the second problem, because it is randomized based on the balance between liquid composition and magnetic field strength, it is likely to be affected by subtle changes in liquid physical properties such as the dispersion state and magnetic properties of magnetic powder. found.

(問題点を解決するための手段) 本発明者らは上記の如き欠点を解消すべ(種々検討の結
果、ある特定の液組成および塗布スピードに対し最適周
波数を決定する事により、広い磁場強度領域(磁材抗磁
力の1/1o〜1/l)で高いランダム配向処理が可能
となる事を見出した。すなわち、周波数が磁性層の磁場
中通過速度に対して、周波数(HM)/塗布スピーhe
 (rIL/分)L/10〜1/1まで可変となる交流
磁場発生装置を使用してランダム配向処理を行う事によ
り高特性の磁気記録媒体を製造し得ることを見出し1本
発明を達成した。
(Means for Solving the Problems) The present inventors have solved the above-mentioned drawbacks (as a result of various studies, by determining the optimum frequency for a certain specific liquid composition and coating speed, (1/1o to 1/l of the coercive force of the magnetic material) enables high random orientation treatment.In other words, the frequency (HM)/coating speed is he
(rIL/min) It was discovered that a magnetic recording medium with high characteristics could be manufactured by performing a random orientation process using an alternating current magnetic field generator that can be varied from L/10 to 1/1. 1. The present invention was achieved. .

以下、本発明の方法を実施した装置を図面を参照しつつ
詳細に説明する。
Hereinafter, an apparatus implementing the method of the present invention will be described in detail with reference to the drawings.

第1図は本発明の方法を適用した磁気記録媒体の製造装
置の一実施態様の概略図を示すものである。送り出しロ
ールlに巻回された長尺、帯状の非磁性支持体2は、矢
印A方向に連続移送され、巻取りロール6に巻取られる
ようになっている。
FIG. 1 shows a schematic diagram of an embodiment of a magnetic recording medium manufacturing apparatus to which the method of the present invention is applied. The long, strip-shaped non-magnetic support 2 wound around the delivery roll 1 is continuously transported in the direction of arrow A, and is wound around the take-up roll 6.

移送される非磁性支持体20表面に近接する位置には、
塗布装置3が配設されており磁性液を塗布する。
At a position close to the surface of the nonmagnetic support 20 to be transferred,
A coating device 3 is provided to apply magnetic liquid.

上記塗布装置3から支持体移送方向Aの下流側には、磁
界を作用させてランダム配向処理を行うための周波数可
変交流磁場発生装置4が配設され。
A frequency-variable AC magnetic field generator 4 is disposed downstream from the coating device 3 in the support transport direction A to apply a magnetic field to perform a random orientation process.

そしてさらに下流側に乾燥装置5が配設されている。Further, a drying device 5 is provided on the downstream side.

上記製造装置において、非磁性支持体2上に層成された
磁性液は1周波数可変交流磁場発生装置4により未乾燥
状態で磁性粒子がランダム配向される。この時、周波数
可変交流磁場発生装置4が発生する周波数(Hz)は、
非磁性支持体2の走行速度(磁場発生装置4内の通過速
度(m/分))に対し、絶対数値が0.1〜lの範囲で
可変となるように設定されており、又、印加する交流磁
場の磁場強度は磁材抗磁力の0.1〜1の範囲に設定さ
れている。
In the above manufacturing apparatus, the magnetic particles of the magnetic liquid layered on the non-magnetic support 2 are randomly oriented in an undried state by the single frequency variable alternating current magnetic field generator 4. At this time, the frequency (Hz) generated by the variable frequency alternating current magnetic field generator 4 is
The absolute value is set to be variable in the range of 0.1 to 1 with respect to the traveling speed of the non-magnetic support 2 (the speed of passage through the magnetic field generator 4 (m/min)), and the applied The magnetic field strength of the alternating current magnetic field is set within the range of 0.1 to 1 of the coercive force of the magnetic material.

上記のよ5にして配向処理された後5次いで乾燥装置5
を通過すると、該未乾燥磁性塗布層が乾燥・固化し、シ
ート状の磁気記録媒体が得られる。
After the orientation treatment as described in 5 above, 5 then a drying device 5.
When passing through, the undried magnetic coating layer dries and solidifies, yielding a sheet-like magnetic recording medium.

この磁気記録媒体をその後打ち抜くことにより磁気ディ
スク等を形成することができる。
By subsequently punching out this magnetic recording medium, a magnetic disk or the like can be formed.

上記磁場発生装置4のように印加する磁場強度を磁性液
中の磁性粒子(磁材)の抗磁力に対して一定範囲内とし
、かつ交番磁界を発生する電流の周波数を塗布スピード
に対して一定範囲内に可変とすることにより、塗布液の
例えば分散状態・磁性粒子の磁気的特性等の緒特性によ
る影響が多少生じても、該磁性粒子のランダム配向を所
望の範囲に容易に行うことができる。これは、磁性粒子
の抗磁力とほぼ同等かそれよりも小さくかつ1/10以
上の強さの交流磁場を印加させることによって、磁性粒
子のランダム化が効果的に進行することに加え、交流磁
場が磁性粒子に与える力学的影響はその周波数と磁場内
通過速度(塗布スピード0)との関係にも左右され、本
発明者らが設定した次式。
The intensity of the magnetic field applied like the magnetic field generator 4 is kept within a certain range relative to the coercive force of the magnetic particles (magnetic material) in the magnetic liquid, and the frequency of the current that generates the alternating magnetic field is kept constant relative to the coating speed. By making it variable within a range, it is possible to easily achieve random orientation of the magnetic particles within a desired range even if there is some influence due to the characteristics of the coating liquid, such as the dispersion state or the magnetic properties of the magnetic particles. can. This is because the randomization of magnetic particles progresses effectively by applying an alternating magnetic field that is approximately equal to or smaller than the coercive force of the magnetic particles and has a strength of 1/10 or more, and in addition, the alternating magnetic field The mechanical influence of .

周波数(EI! )/塗布スピード”(m/分)の値が
0.1〜lの範囲においては、配向比C3Q比)が極端
に悪化する領域が存在することがなく、ランダム配向処
理が効果的に行われ配向比をほぼ1に近づけることが出
来ることによる。
When the value of frequency (EI!)/application speed (m/min) is in the range of 0.1 to 1, there is no region where the orientation ratio (C3Q ratio) deteriorates extremely, and random orientation treatment is effective. This is because the orientation ratio can be brought close to approximately 1.

なお、磁場印加時間は特に限定されるものではなく、例
えば磁場強度や支持体走行速度等により適宜変更するこ
とができる。又1本明細書において配向比C3Q比)と
は、磁性層の長手方向の角型比SQ、とそれに直交する
角型比S Q 土との比C8Q上/SQ/)で示したも
のである。
Note that the magnetic field application time is not particularly limited, and can be changed as appropriate depending on, for example, the magnetic field strength and the support traveling speed. In this specification, the orientation ratio (C3Q ratio) is expressed as the squareness ratio SQ in the longitudinal direction of the magnetic layer and the squareness ratio SQ perpendicular to it (C8Q upper/SQ/). .

従って1本発明の方法を実施した周波数可変交流磁場発
生装置4を用いるととくより、種々の磁気記録媒体を製
造する場合でも、ランダム配向処理の設定が容易になり
、安定した品質の磁気記録媒体を提供することができる
Therefore, by using the variable frequency alternating current magnetic field generator 4 that implements the method of the present invention, the random orientation process can be easily set even when manufacturing various magnetic recording media, and magnetic recording media of stable quality can be produced. can be provided.

〔実施例〕〔Example〕

以下、本発明を実施例にて詳細に説明する。 Hereinafter, the present invention will be explained in detail with reference to Examples.

厚さ75μmのポリエチレンテレフタレート(PF:T
 )から成る非磁性支持体上K、乾燥厚み2μmに相当
する磁性液を塗布し、その移送方向下流側に配設された
周波数可変交流磁場発生装置4にて磁性粒子の配向のラ
ンダマイズ化を行い、乾燥、打ち抜きをし、磁気ディス
クを製造する工程において。
Polyethylene terephthalate (PF:T) with a thickness of 75 μm
) A magnetic liquid equivalent to a dry thickness of 2 μm is applied onto a non-magnetic support (K), and the orientation of the magnetic particles is randomized using a variable frequency alternating current magnetic field generator 4 installed downstream in the transfer direction. , drying, punching, and in the process of manufacturing magnetic disks.

塗布スピードが50m/分、loom/分のそれぞれに
おいて周波数を5 Hz、 50Hz、 100Hzの
3通りに変化させランダム配向処理を行った場合の磁性
粒子のランダマイズ化の違いを、製造したそれぞれの磁
性層の配向比C3Q比)を測定することにより調べた。
The differences in the randomization of the magnetic particles when random orientation treatment was performed by changing the frequency to three different frequencies of 5 Hz, 50 Hz, and 100 Hz at coating speeds of 50 m/min and room/min, respectively, were compared to the results of each manufactured magnetic layer. It was investigated by measuring the orientation ratio (C3Q ratio).

なお配向比(SQ比)は、その値が1の時、磁性粒子が
完全にランダマイズ化された事を示すものである。
Note that when the orientation ratio (SQ ratio) is 1, it indicates that the magnetic particles are completely randomized.

本実施例では、液組成の異なる2種類の液A。In this example, two types of liquids A having different liquid compositions are used.

Bを塗布液として使用した。A、B2種類の液の組成は
下記の表11表2に示す通りである。
B was used as a coating liquid. The compositions of the two types of liquids A and B are as shown in Table 11 and Table 2 below.

表  1CA液) γ−B’e203 (磁材抗磁力240Daン    
 400重tmポリウレタンにツボラン3022)  
    60重1部塩化ビニル酢酸ビニル共重合体(V
MCH)   40重量部レシチン         
          6重量部ステアリン酸     
           5重量部カーボン      
           30重量部メチルエチルケトン
            soo重量部メチルイソブチ
ルケトン          200重量部シクロヘキ
サノン             200重量部表  
2CB液) Co−含有r −Fe20B (磁材抗磁力600宜鴎
 100重量部ニトロセルロース          
   IO!鎗部ポリウレタンにツボラン2304) 
      8重量部ポリイソシアネート      
                8重量部0r203
                  2重量部カーボ
ン                  2重量部ステ
アリン酸                1重量部ス
テアリン酸ブチル             1重量部
メチルエチルケトン           300重量
部上述のようVC1周波数可変交流磁場発生装置により
ランダム配向処理した磁気ディスクの配向比C3Q比)
を磁場強度に対してプロットした結果を第2図、第3図
および第4図、第5図に示す。第2因、第3図は塗布ス
ピード9がson/分の場合、第4因、第5図は塗布ス
ピードが100m/分の結果を示したものである。この
結果より1例えば第2図のA液の結果を見れば1周波数
100および50Hzでも確かに配向比IKなる(完全
にランダマイズ化される)磁場強度が磁材抗磁力(24
0・oe>をはさんで両側に2点存在し、この磁場強度
にてランダム配向処理を行えば配向比中1なる磁気ディ
スクが製造可能である。しかしながら、同一組成であっ
ても、液の分散状態・磁性粉末の磁気的特性等の微妙な
変化の影響を受け、この最適磁場強度点は変化してしま
い、安定に製造出来ない。したがってこの第2図A液の
結果より明らかなように、最適周波数である5Hz と
する事により、配向比中1となる磁場強度領域が広くな
り、この磁場強度領域の中心付近の磁場強度に設定し配
向処理を行うことKより、安定に高品質の磁気ディスク
を製造し得る。さらに、第4図に示すようK。
Table 1CA liquid) γ-B'e203 (Magnetic material coercive force 240Da)
400 weight tm polyurethane and Tuboran 3022)
60 weight 1 part vinyl chloride vinyl acetate copolymer (V
MCH) 40 parts by weight lecithin
6 parts by weight stearic acid
5 parts by weight carbon
30 parts by weight Methyl ethyl ketone soo parts by weight Methyl isobutyl ketone 200 parts by weight Cyclohexanone 200 parts by weight Table
2CB liquid) Co-containing r -Fe20B (Magnetic material coercive force 600 Yio 100 parts by weight Nitrocellulose
IO! Tsuboran 2304 for Yaribe polyurethane)
8 parts by weight polyisocyanate
8 parts by weight 0r203
2 parts by weight Carbon 2 parts by weight Stearic acid 1 part by weight Butyl stearate 1 part by weight Methyl ethyl ketone 300 parts by weight Orientation ratio (C3Q ratio) of a magnetic disk subjected to random orientation treatment using the VC1 frequency variable AC magnetic field generator as described above
The results of plotting the value against the magnetic field strength are shown in FIGS. 2, 3, 4, and 5. The second factor, FIG. 3, shows the results when the coating speed 9 is son/min, and the fourth factor, FIG. 5, shows the results when the coating speed is 100 m/min. From this result, for example, looking at the results for liquid A in Figure 2, it is clear that even at frequencies of 100 and 50 Hz, the magnetic field strength that provides the orientation ratio IK (completely randomized) is equal to the coercive force of the magnetic material (24
There are two points on both sides with 0·oe> in between, and if random orientation processing is performed at this magnetic field strength, a magnetic disk with an orientation ratio of 1 can be manufactured. However, even if the composition is the same, the optimal magnetic field strength point changes due to the influence of subtle changes in the dispersion state of the liquid, the magnetic properties of the magnetic powder, etc., and stable production is therefore not possible. Therefore, as is clear from the results for liquid A in Figure 2, by setting the optimum frequency to 5Hz, the magnetic field strength region where the orientation ratio is 1 becomes wider, and the magnetic field strength is set near the center of this magnetic field strength region. By performing the orientation treatment, high-quality magnetic disks can be stably manufactured. Furthermore, K as shown in FIG.

塗布スピーrを上げるにつれ同じ塗布液でも最適周波数
も高くなる事が明らかである。
It is clear that as the coating speed r increases, the optimum frequency also increases for the same coating liquid.

また、B液を塗布した場合(第3図、第5図)最適周波
数はA液とは異なるが、上述のようなA液の場合の結果
と同様の傾向を示した。このように、液の組成および塗
布スピードにより最適周波数は変化するが、通常周波数
(Hり/塗布スピーfcm/分)の値がl/10〜1/
lまで可能となるような周波数可変領域を有する交流磁
場発生装置を使用しランダム配向処理を行えば、安定に
高品質の磁気記録媒体を製造し得ることが判る。
Further, when liquid B was applied (FIGS. 3 and 5), although the optimum frequency was different from that of liquid A, it showed the same tendency as the result in the case of liquid A as described above. In this way, the optimum frequency changes depending on the composition of the liquid and the coating speed, but the value of the frequency (Hri/coating speed fcm/min) is usually 1/10 to 1/1/2.
It can be seen that if a random orientation process is performed using an alternating current magnetic field generator having a frequency variable range that allows up to 1, a high quality magnetic recording medium can be stably manufactured.

(発明の効果) 以上述べたように本発明の方法は磁場強度の範囲設定と
共畝周波数(Hz)と塗布スピードとの関係を特定範囲
内に可変設定することにより、該範囲内では配向比中1
なる状態を連続して保つことができるので、安定したラ
ンダム配向処理を行うことができる。したがって1本発
明の方法を用いた装置によれば、良好なランダム配向処
理の設定が容易であり、高品質な磁気記録媒体の安定製
造を保証することができる。
(Effects of the Invention) As described above, the method of the present invention variably sets the relationship between the magnetic field strength range, the common ridge frequency (Hz), and the coating speed within a specific range, so that the orientation ratio can be adjusted within the range. 1st year of junior high school
Since this state can be maintained continuously, stable random alignment processing can be performed. Therefore, according to the apparatus using the method of the present invention, it is easy to set up a good random orientation treatment, and it is possible to guarantee stable production of high-quality magnetic recording media.

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

第1図は本預明の方法を用いた磁気記録媒体の製造装置
の一実施態様を示す概略図、第2図〜第5図は本発明を
説明するための実施例のグラフである。 1・・・送り出しロール 2・・・非磁性支持体3・・
・塗布装置
FIG. 1 is a schematic diagram showing an embodiment of a magnetic recording medium manufacturing apparatus using the method of the present invention, and FIGS. 2 to 5 are graphs of examples for explaining the present invention. 1... Delivery roll 2... Non-magnetic support 3...
・Coating device

Claims (1)

【特許請求の範囲】[Claims] 連続的に走行する支持体上に磁性液を塗布して磁性層を
設け、該磁性層に未乾燥中に交流磁場を印加してランダ
ム配向処理を行う磁気記録媒体の製造方法において、印
加する交流磁場の磁場強度が磁材抗磁力の1/10〜1
/1まで、かつ周波数が磁性層の磁場中通過速度に対し
て、周波数(Hz)/塗布スピード(m/分)が1/1
0〜1/1まで可変である範囲で配向処理をする事を特
徴とする磁気記録媒体の製造方法。
In a method for producing a magnetic recording medium, a magnetic layer is provided by coating a magnetic liquid on a continuously running support, and an alternating current magnetic field is applied to the magnetic layer while it is not dry to perform a random orientation treatment. The magnetic field strength is 1/10 to 1 of the coercive force of the magnetic material.
/1, and the frequency (Hz)/coating speed (m/min) is 1/1 of the magnetic layer passing speed in the magnetic field.
A method for manufacturing a magnetic recording medium, characterized in that orientation treatment is performed in a variable range from 0 to 1/1.
JP29349386A 1986-12-11 1986-12-11 Method of manufacturing magnetic recording medium Expired - Lifetime JPH0640388B2 (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP29349386A JPH0640388B2 (en) 1986-12-11 1986-12-11 Method of manufacturing magnetic recording medium

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP29349386A JPH0640388B2 (en) 1986-12-11 1986-12-11 Method of manufacturing magnetic recording medium

Publications (2)

Publication Number Publication Date
JPS63148417A true JPS63148417A (en) 1988-06-21
JPH0640388B2 JPH0640388B2 (en) 1994-05-25

Family

ID=17795449

Family Applications (1)

Application Number Title Priority Date Filing Date
JP29349386A Expired - Lifetime JPH0640388B2 (en) 1986-12-11 1986-12-11 Method of manufacturing magnetic recording medium

Country Status (1)

Country Link
JP (1) JPH0640388B2 (en)

Also Published As

Publication number Publication date
JPH0640388B2 (en) 1994-05-25

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