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JPS5812130A - High-density magnetic recording medium and its production - Google Patents

High-density magnetic recording medium and its production

Info

Publication number
JPS5812130A
JPS5812130A JP10821881A JP10821881A JPS5812130A JP S5812130 A JPS5812130 A JP S5812130A JP 10821881 A JP10821881 A JP 10821881A JP 10821881 A JP10821881 A JP 10821881A JP S5812130 A JPS5812130 A JP S5812130A
Authority
JP
Japan
Prior art keywords
magnetic
recording medium
medium
magnetic recording
density
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
JP10821881A
Other languages
Japanese (ja)
Other versions
JPS6250888B2 (en
Inventor
Koki Yokoyama
横山 弘毅
Masahiro Fukazawa
深沢 昌広
Akizo Hideyama
日出山 章蔵
Minoru Hashimoto
稔 橋本
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.)
Toshiba Corp
Original Assignee
Toshiba Corp
Tokyo Shibaura Electric 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 Toshiba Corp, Tokyo Shibaura Electric Co Ltd filed Critical Toshiba Corp
Priority to JP10821881A priority Critical patent/JPS5812130A/en
Publication of JPS5812130A publication Critical patent/JPS5812130A/en
Publication of JPS6250888B2 publication Critical patent/JPS6250888B2/ja
Granted 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
    • G11B5/84Processes or apparatus specially adapted for manufacturing record carriers
    • G11B5/842Coating a support with a liquid magnetic dispersion
    • G11B5/845Coating a support with a liquid magnetic dispersion in a magnetic field

Landscapes

  • Chemical & Material Sciences (AREA)
  • Dispersion Chemistry (AREA)
  • Paints Or Removers (AREA)
  • Magnetic Record Carriers (AREA)
  • Manufacturing Of Magnetic Record Carriers (AREA)

Abstract

PURPOSE:To increase the recording density, by distributing the magnetization facilitating axis of magnetic particles having the uniaxial anisotropy at the area between a direction vertical to the face of a magnetic recording medium and the traveling direction of a magnetic head. CONSTITUTION:A magnetic recording medium 1 is obtained by coating a magnetic coating material containing uniaxial anisotropic magnetic particles of hexagonal ferrite, metallic cobalt, etc. on a supporter of a polyethylene terephthalate film, etc. The magnetic fields of different directions of application are successively applied within a plane including the lengthwise direction of the medium 1 and the direction vertical to the medium 1 with use of an orienting magnet 2 wile traveling the medium 1 toward an arrow 3. In this case, the magnetic field is lessened with each change of the direction of the applied magnetic field or the coated film is heated. Thus the viscosity is successively increased for the coated liquid.

Description

【発明の詳細な説明】 不発flJa高密覆磁気記−に適する記載媒体に関する
ものである。
DETAILED DESCRIPTION OF THE INVENTION The present invention relates to a recording medium suitable for non-explosion flJa high-density magnetic recording.

周知の工うに、ビデオ記載、コンビ轟−一・データ記載
、オーディオ記載などに用いる磁気記載媒体においてに
、記載の大容量化、小形軽量化を達放するために、記鋒
密度の同上が強く要望されている自従来、磁気記載媒体
として、r−ν・、0.。
As is well known, in magnetic recording media used for video recording, combination data recording, audio recording, etc., in order to achieve larger recording capacity, smaller size, and lighter weight, the recording density is strongly increased. Conventionally, desired magnetic recording media include r-ν·, 0. .

Orb@など、針状′を育する磁性粉tIk布し、記載
方向に配向さぞたものが広く用いられてきた。この1う
な磁気記載媒体の高記載密度化を図るには、磁性粒子の
tイズを微細化する。磁性体の保磁力を高める、塗膜の
膜厚を薄くする、などの方法があり、それぞれ方策が講
じられてIIた。しかし、磁性粒子サイズ會限界値1り
小さくすると磁気特性の安定性が低下すること、保磁力
を大きくしすぎると磁気ヘッドに1本記録が困Jlにな
ること、膜厚を薄くすると再生信号出力が低下すること
などの問題があり、このLうな方法にする高密度化につ
いてにすでに1つの限界に達していると考えられる。他
方、高密直配fIkを達成する別の手段として垂直磁化
記録が研究されているが、筐だこれに用いる記載媒体が
、0o−Orl[に限られており、膜の均一性、耐久性
などに盲だ問題があるほか、垂直磁化記載方式に従来記
録方式と相反的であるため、互換性t%fないこと11
これ管実用化する上での問題点である。
Magnetic powders such as Orb@, which are made of magnetic powder tIk that grows needle-like shapes and are oriented in the indicated direction, have been widely used. In order to increase the recording density of this type of magnetic recording medium, the size of the magnetic particles is made finer. There are methods such as increasing the coercive force of the magnetic material and reducing the thickness of the coating film, and each method has been taken. However, if the magnetic particle size limit value is reduced by 1, the stability of the magnetic properties will decrease, if the coercive force is too large, it will be difficult to record one line on the magnetic head, and if the film thickness is made thinner, the reproduced signal will be output There are problems such as a decrease in the density, and it is thought that a limit has already been reached in increasing the density using this L method. On the other hand, perpendicular magnetization recording is being researched as another means of achieving high-density direct fIk, but the housing and recording medium used for this are limited to 0o-Orl, and film uniformity, durability, etc. In addition to the problem of blindness, the perpendicular magnetization writing method is contradictory to the conventional recording method, so there is no compatibility.11
This is a problem in putting the pipe into practical use.

本発明者らに上記の高密度記録媒体の問題点に着目し、
種々研究検討を重ねた結果、−軸異方性tVする磁性粒
子を用い、この磁性粒子の磁化容易軸tts体#1に画
直な方向と磁気ヘッド走行方向との間に分布さぜること
にエフ、記録密度の向上が可能であること見出し、本発
明をなすに至ったすなわち、本発明に媒体1liK垂直
な方向と、磁気ヘッドの走行方向(媒体、長平方向と名
づけることにする)とを含む平面と平行な平面内に磁性
粒子の磁化容易軸を分布させた磁気記載媒体である。ま
たこれに使用される磁性粒子として、六方晶の結晶構造
を有する磁性体、たとえば、六方晶フェライト、あるい
は金属コバルト等を用いる点で特徴づけられる。さらに
磁性特性にて本発明の磁気記録媒体t−特徴づけれ゛ば
、媒体IIに垂直な方向と磁気ヘッド走行方向の間の任
意の方向で測定した磁化曲線の保磁力が、媒体面内で、
ヘッド走行方向と直角な方向で測定した保磁力の1.2
倍以上であることで示される。ここで1,2倍以上[9
定した理由に、この値未満の場合に、磁性粒子の磁化容
易軸分布が十分でなく、本発明の特徴である記録密度向
上の効果が十分に@められなくなるからである。
The present inventors focused on the problems of the above-mentioned high-density recording media, and
As a result of various research studies, we found that using magnetic particles with -axis anisotropy tV, we distributed the magnetic particles between the direction perpendicular to the axis of easy magnetization tts body #1 and the running direction of the magnetic head. They discovered that it was possible to improve the recording density and developed the present invention.That is, in the present invention, a direction perpendicular to the medium 1liK and a direction in which the magnetic head runs (hereinafter referred to as the longitudinal direction of the medium) are used. This is a magnetic recording medium in which the easy axis of magnetization of magnetic particles is distributed in a plane parallel to a plane containing the magnetic particles. Further, it is characterized in that a magnetic material having a hexagonal crystal structure, such as hexagonal ferrite or metallic cobalt, is used as the magnetic particles. Furthermore, if the magnetic recording medium of the present invention is characterized by magnetic properties, the coercive force of the magnetization curve measured in any direction between the direction perpendicular to the medium II and the running direction of the magnetic head is ,
1.2 of coercive force measured in the direction perpendicular to the head running direction
This is indicated by more than double the amount. Here, more than 1 or 2 times [9
The reason for this is that if the value is less than this value, the easy axis distribution of the magnetic particles will not be sufficient, and the effect of improving the recording density, which is a feature of the present invention, will not be sufficiently achieved.

上記本発明に係る磁気記載媒体に次のようにして容易に
製造し得る。すなわち、−軸異方性磁性体微粒子たとえ
ば、バリウムフェライトの0へT1置換体微粒子100
重量部に対し、バインダとしての樹脂たとえば、塩化ビ
ニル、酢酸ビニル共重合体、ポリウレタン樹脂など10
〜40重量部、分散剤として、レシチンなど、0.5〜
20重量部機度、お工び溶剤例えば、メチルエチルケト
ン、メチルイソブチルケトン、シクロヘキサノン、トル
エンなど200重量部程度を1分散機例えばサンドグラ
インダ、ボールンル、三本ロールミルなどt用い1く混
合分散して塗料状の磁性組成物を調製する。この組成物
にイソシアネートなど硬化剤を適宜添加し、叉持基体例
えばポリエチレンテレフタレートフィルムにリバースコ
ータ、グラビヤコータ、スピンコータなどの塗布機を用
いて塗布し、電磁石または永久磁石を用いて媒体長手方
向と媒体と垂直な方向を含む面内で、印加方向の異なる
磁界を順次印加する。この際印加磁界方向tfえるごと
に磁界を弱めてゆくか、あるいは、塗膜を加熱すること
にLり、塗工された塗液の粘度1−*vc高めてゆく、
こうすることに19、所要の面内に磁性粒子の磁化容易
軸を分布させた磁気記鎌媒体を得る。
The above magnetic recording medium according to the present invention can be easily manufactured as follows. That is, minus-axis anisotropic magnetic material fine particles, for example, 0 to T1 substitution product fine particles of barium ferrite, 100
Resin as a binder, such as vinyl chloride, vinyl acetate copolymer, polyurethane resin, etc. 10 parts by weight
~40 parts by weight, as a dispersant, lecithin, etc., 0.5~
Mix and disperse about 200 parts by weight of a solvent such as methyl ethyl ketone, methyl isobutyl ketone, cyclohexanone, toluene, etc. using a dispersing machine such as a sand grinder, ball mill, or three-roll mill to form a paint. A magnetic composition is prepared. A curing agent such as an isocyanate is appropriately added to this composition, and the mixture is coated onto a holding substrate such as a polyethylene terephthalate film using a coating machine such as a reverse coater, gravure coater, or spin coater, and is coated in the longitudinal direction of the medium using an electromagnet or permanent magnet. Magnetic fields with different application directions are sequentially applied within a plane including a direction perpendicular to the . At this time, the magnetic field is weakened every time the applied magnetic field direction tf increases, or the viscosity of the applied coating liquid is increased by 1-*vc by heating the coating film.
In this way, 19, a magnetic recording medium is obtained in which the easy axis of magnetization of the magnetic particles is distributed within a required plane.

次に本発明の実施例を述べる。Next, examples of the present invention will be described.

実施例 平均径0.1 sya  のバリウムフェライトのO’
o e T i置換体微粒子粉80重量部あたり、バイ
ンダとして塩化ビニル、酢酸ビニル共重合体10重量部
、分散剤として、レシチン、4重量部溶剤として、メチ
ルイソブチルケトン80重量部、トルエン80重量部、
シクロへ中サノン80重量部を加え、サンドミルを用い
て、分散塗料化した。この塗料に硬化剤としてインシア
ネー)10重量m+t−加えポリエチレンテレフタレー
トフィルムff1K塗布しt後、フィルム面内配向磁界
2 KO,を印加し、次いでフィルムを加熱しつつさら
に、フィルムfiJK垂直方向に磁界2 KO・を印加
し、乾燥を行なって磁気記載媒体を作製した。この磁気
記載媒体の静磁気測定を行な−)たところ、膜1内配向
磁界印加方向テ、残留磁化Br=1100G−保磁力H
a = 10000・、筐た膜面に−直な方向で反磁界
補正を行なった結果、Br−1000G 、 Hc=9
60’Oeであった。
Example O' of barium ferrite with an average diameter of 0.1 sya
Per 80 parts by weight of o e Ti-substituted fine particle powder, 10 parts by weight of vinyl chloride and vinyl acetate copolymer as a binder, 4 parts by weight of lecithin as a dispersant, 80 parts by weight of methyl isobutyl ketone and 80 parts by weight of toluene as a solvent. ,
80 parts by weight of Nakasanon was added to the cyclo, and a dispersion paint was prepared using a sand mill. To this coating material, a hardening agent of 10 weight m+t was added to a polyethylene terephthalate film ff1K, and after that, an in-plane orientation magnetic field of 2 KO, was applied to the film, and then, while heating the film, a magnetic field of 2 KO was applied in the perpendicular direction to the film fiJK. * was applied and drying was performed to produce a magnetic recording medium. When the magnetostatic measurement of this magnetic recording medium was carried out, it was found that the direction of application of the orientation magnetic field in the film 1 was TE, residual magnetization Br = 1100G - coercive force H
a = 10000・, as a result of demagnetizing field correction in the direction perpendicular to the film surface of the casing, Br-1000G, Hc = 9
It was 60'Oe.

他方111面内で、配向磁界印加方向と直角な方向でB
r=600G、Haz7000sであった0以上の磁気
測足結果によれば、膜面内配向磁界印加方向と膜面と―
直な方向のBr、Haが大きくこれら二方向と垂直な方
向のBr、Heが小さい、この結果から磁性粒子が上記
二方向を含む面内に、磁化容易軸が分布しているという
ことがわかる。
On the other hand, in the 111 plane, B in the direction perpendicular to the direction of applying the alignment magnetic field.
According to the magnetic foot measurement results of 0 or more at r = 600G and Haz 7000s, the direction of application of the in-plane orientation magnetic field and the film surface are -
Br and Ha in the normal direction are large and Br and He in the direction perpendicular to these two directions are small.From this result, it can be seen that the axis of easy magnetization of the magnetic particles is distributed in a plane that includes the above two directions. .

次にこの磁気記録媒体に対し、フェライトコアを用い几
磁気ヘッドを用い、山内配向磁界方向にヘッドを走らせ
て高密度記帰を行ない、再生出力tgべた。@3図にそ
の結果を示す、なお比較例として上記にエフ作製した磁
性塗料を塗布後配同逃理を全く行なわず、乾燥させた磁
性膜(Br=8000・Ha−8000−について、同
様に記鋒栴生會行なった結果を同時に示し几1図VCL
り、本発明の実施例の記録媒体に高密度領域での再生出
力の同上が顕著であることがわかる。すなわち、記録c
tT11@な記録密度が大幅に同上していることがわか
る・ 布をさせた磁気記録媒体が何故し高密度記録に適するか
について框、今後十分に研究し、解明してゆかなければ
ならない課題であるが、現時点で考えられる理由として
は、■高密度記*t−行なゎぜるVcに膜面に垂直方向
に配向した粒子が有効であり■これと他の方向に配向し
た粒子との組み合わせKより、電流磁化パターンが可能
、さらに■磁気記録媒体に有効でない方位の粒子が減っ
ている。の3点を指摘することがで禽る。
Next, high-density recording was performed on this magnetic recording medium using a ferrite core and a magnetic head, by running the head in the direction of the Yamauchi alignment magnetic field, and the reproduction output tg was determined. The results are shown in Fig. 3. As a comparative example, the magnetic coating prepared above was coated with the magnetic paint (Br = 8000/Ha-8000-), which was dried without any release. Figure 1 VCL shows the results of the meeting at the same time.
It can be seen that the reproduction output of the recording medium according to the embodiment of the present invention is significantly different from the above in the high-density region. That is, record c
It can be seen that the recording density of tT11@ has significantly increased as above.The question of why cloth-covered magnetic recording media are suitable for high-density recording is an issue that must be fully researched and clarified in the future. However, the reasons that can be considered at the moment are: ■ Particles oriented perpendicular to the film surface are effective for high-density recording *t-processing Vc, and ■ Particles oriented in other directions are effective. With combination K, a current magnetization pattern is possible, and (1) particles with orientations that are not effective for magnetic recording media are reduced. I would like to point out three points.

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

厘1図および藁2図に本発明の磁気記録媒体を製造する
ための磁性粒子の磁化容昌軸分布Mllt行うための磁
石配置図、謳3図に本発明の紀鍮媒体冥施例お工び比較
例の記帰密度−再生出力特性曲線図である。 1・・・・・・磁気記録媒体、 2・・・−・・配向用
磁石、3・・・・・・媒体走行方向、 4・・・・・・
磁界方向。
Figures 1 and 2 are magnet arrangement diagrams for the magnetization axis distribution of magnetic particles for manufacturing the magnetic recording medium of the present invention, and Figure 3 is an example of the construction of the magnetic recording medium of the present invention. FIG. 4 is a recording density-reproduction output characteristic curve diagram of a comparative example. 1... Magnetic recording medium, 2... Orienting magnet, 3... Medium running direction, 4...
Magnetic field direction.

Claims (1)

【特許請求の範囲】 (1)媒体fl:jl直な方向と磁気ヘッドの走行方向
とを含む平[1iまたにこれと平行な平面内に磁性粒子
の磁化容鳥軸を分布さぜ7tQとt特徴とする高密度磁
気記載媒体。 (2、特許請求の範囲1に1項の記載において磁性粒子
が、六方晶の結晶構造會肩する磁性体であることt−特
徴とする、高密度磁気記載媒体。 (3)特許請求の範囲第1項の記載において、磁性粒子
が六方晶フェライトであることtII!#徴とする高密
度磁気記載媒体。 (4)特許請求の範11!1!!!111項の記載にお
いて磁性粒子が金綱コバルト1またはその合金であるこ
とtq#黴とする高密度磁気記載媒体。 (5)特許請求の範i!1111項の記載において、媒
体面に−直な方向と磁気ヘッド走行方向との間の任意の
方向で測定した磁化amの保磁力が、媒体面内でヘッド
走行方向と直角な方向で測定した磁化曲線の保磁力の1
,2倍以上であることt%黴とする高密度磁気記載媒体
・ (6)支持基体上に磁性塗料を塗布した後媒体長手方向
と媒体と喬直な方向管含む面内で印加方向の異なる磁界
t*次印加することt4I黴とする高密度磁気記#ll
I&体の製造方法。
[Claims] (1) The magnetization axis of the magnetic particles is distributed within a plane [1i and parallel to the plane including the direction perpendicular to the medium fl:jl and the running direction of the magnetic head. A high-density magnetic recording medium characterized by t. (2. High-density magnetic recording medium characterized in that the magnetic particles in claim 1 are magnetic materials having a hexagonal crystal structure. (3) Claims In the description of claim 1, the high-density magnetic recording medium is characterized in that the magnetic particles are hexagonal ferrite. (4) In the description of claim 11!1!!!111, the magnetic particles are metal wire. A high-density magnetic recording medium made of cobalt-1 or an alloy thereof. (5) In the description of claim i! The coercive force of the magnetization am measured in any direction is 1 of the coercive force of the magnetization curve measured in the direction perpendicular to the head running direction within the medium plane.
, a high-density magnetic recording medium with t% moldiness of at least twice as much (6) After coating the magnetic paint on the support substrate, the application direction is different in the longitudinal direction of the medium and in the plane including the direction perpendicular to the medium. High-density magnetic recording #ll with magnetic field t* applied as t4I mold
I&body manufacturing method.
JP10821881A 1981-07-13 1981-07-13 High-density magnetic recording medium and its production Granted JPS5812130A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP10821881A JPS5812130A (en) 1981-07-13 1981-07-13 High-density magnetic recording medium and its production

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP10821881A JPS5812130A (en) 1981-07-13 1981-07-13 High-density magnetic recording medium and its production

Publications (2)

Publication Number Publication Date
JPS5812130A true JPS5812130A (en) 1983-01-24
JPS6250888B2 JPS6250888B2 (en) 1987-10-27

Family

ID=14479021

Family Applications (1)

Application Number Title Priority Date Filing Date
JP10821881A Granted JPS5812130A (en) 1981-07-13 1981-07-13 High-density magnetic recording medium and its production

Country Status (1)

Country Link
JP (1) JPS5812130A (en)

Cited By (3)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS60164925A (en) * 1984-02-07 1985-08-28 Hitachi Maxell Ltd Magnetic recording medium
JPS61188702A (en) * 1985-02-18 1986-08-22 Matsushita Electric Ind Co Ltd Magnetic recording and reproducing device
JPS63237218A (en) * 1987-03-25 1988-10-03 Fuji Photo Film Co Ltd Production of magnetic recording medium

Cited By (4)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS60164925A (en) * 1984-02-07 1985-08-28 Hitachi Maxell Ltd Magnetic recording medium
JPS61188702A (en) * 1985-02-18 1986-08-22 Matsushita Electric Ind Co Ltd Magnetic recording and reproducing device
JPH0466042B2 (en) * 1985-02-18 1992-10-22 Matsushita Electric Ind Co Ltd
JPS63237218A (en) * 1987-03-25 1988-10-03 Fuji Photo Film Co Ltd Production of magnetic recording medium

Also Published As

Publication number Publication date
JPS6250888B2 (en) 1987-10-27

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