JPS58199434A - Magnetic recording medium - Google Patents
Magnetic recording mediumInfo
- Publication number
- JPS58199434A JPS58199434A JP8205082A JP8205082A JPS58199434A JP S58199434 A JPS58199434 A JP S58199434A JP 8205082 A JP8205082 A JP 8205082A JP 8205082 A JP8205082 A JP 8205082A JP S58199434 A JPS58199434 A JP S58199434A
- Authority
- JP
- Japan
- Prior art keywords
- magnetic
- anisotropic
- coercive force
- recording medium
- temperature
- 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.)
- Pending
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
- G11B5/62—Record carriers characterised by the selection of the material
- G11B5/68—Record carriers characterised by the selection of the material comprising one or more layers of magnetisable material homogeneously mixed with a bonding agent
- G11B5/70—Record carriers characterised by the selection of the material comprising one or more layers of magnetisable material homogeneously mixed with a bonding agent on a base layer
Landscapes
- Paints Or Removers (AREA)
- Magnetic Record Carriers (AREA)
Abstract
Description
【発明の詳細な説明】
この発明は磁気記録媒体に関し、その目的とするところ
は高密度記録に適した磁気記録媒体を提供することにあ
る。DETAILED DESCRIPTION OF THE INVENTION The present invention relates to a magnetic recording medium, and an object thereof is to provide a magnetic recording medium suitable for high-density recording.
磁気記録媒体は、通常、磁性粉末を結合剤樹脂とともに
ポリエステルフィルムなどの基体上に塗着して磁性層を
形成することによりつくられ、磁性層中の針状磁性粉末
を磁気テープの長手方向に配向させるなどして磁気特性
を向上させている。Magnetic recording media are usually made by applying magnetic powder together with a binder resin onto a substrate such as a polyester film to form a magnetic layer. Magnetic properties are improved by orienting the material.
ところがこのように針状磁性粉末を長手方向に配向させ
たものでは長手方向の磁化を用いているため記録密度の
向上に限度があり、信号の記録密度を増加してゆくと磁
気記録媒体内の反磁界が増加して残留磁化が減衰してし
まい、記録信号め検出が困難となる。 −
一方(超高密度記録に於ては磁気テープの長手方向の磁
化のみならず、磁性層面に垂直な方向の磁化成分も有効
に作用することが報告されて−おりどの垂直磁化成分を
利用する磁気記録方式に適した磁気記録媒体どして、゛
・コバルト含有酸化鉄磁性粉末を長手方向に配向しない
で記録素子として用いるなどの試みがなされているが、
従来一般に使用き′れtいるコバルト含有酸化鉄磁性粉
末を”記録素す・々し石川いたも、やり早、未だ垂直磁
化力i零分”。However, since the acicular magnetic powder is oriented in the longitudinal direction, there is a limit to the improvement in recording density because it uses magnetization in the longitudinal direction, and as the signal recording density is increased, the As the demagnetizing field increases, residual magnetization attenuates, making it difficult to detect recorded signals. - On the other hand, it has been reported that in ultra-high-density recording, not only the magnetization in the longitudinal direction of the magnetic tape but also the magnetization component in the direction perpendicular to the magnetic layer surface acts effectively. Attempts have been made to use cobalt-containing iron oxide magnetic powder as a recording element without longitudinally oriented magnetic recording media suitable for magnetic recording systems.
The cobalt-containing iron oxide magnetic powder, which has not been commonly used in the past, was used as a recording material by Ishikawa, but it was easy to use, and the perpendicular magnetization force was still zero.
に良好でなく記録波長1μ以下の短波長記録が良へ 、
パ )・ ”
好屹行なえないなどの難点かあ6.高密度記録が良好に
行なえない。 □゛ 。However, short wavelength recording of 1μ or less is better.
6. High-density recording cannot be performed well. □゛.
この発明者らは込・かる−情に−−み種々検討を行な?
、た枦果、従来の磁気記録媒体では保磁力の温度依存性
が磁気記録媒体の磁気トルクを面内で測定し7−リエ展
開して得られる異方性′エネルギーの二[軸異方性成分
の温度・依存“性に一致するかあるいは同じ傾向を示し
、”保′−力の温度依存性と異方性−ネルギニの二軸異
方□性成分の温度−存“佳が□こI□ 5、′
のような関係にある件高、密度記、録に適シた、ものが
、得られないが、保磁力の温度−在住が磁気記録媒体の
磁気トルクを面内で測定しフーリエ展開して得られる異
方性エネルギーの三軸異方性成分の温度依存性にほぼ一
致すると、・、垂直磁化が充分に良好になって記録波長
が1μ以下の短波長記録が充分に行なえ、高密度記録に
適した磁気記録媒体が得られることを見いだし、この発
明をなすに至つ“た。The inventors were deeply moved and conducted various studies.
As a result, in conventional magnetic recording media, the temperature dependence of the coercive force is determined by measuring the magnetic torque of the magnetic recording medium in the plane and expanding the anisotropy' energy by two [axial anisotropy]. Temperature dependence of the component or exhibits the same tendency, and the temperature dependence and anisotropy of the coercive force - Nergini's biaxial anisotropic component temperature-preservation is good. □ 5. Although it is not possible to obtain a relationship suitable for height and density recording, it is possible to measure the magnetic torque of a magnetic recording medium in the plane of the temperature of coercive force and use Fourier If the anisotropic energy obtained by the expansion almost matches the temperature dependence of the triaxial anisotropic component, the perpendicular magnetization will be sufficiently good and short wavelength recording with a recording wavelength of 1 μm or less will be possible. It was discovered that a magnetic recording medium suitable for high-density recording could be obtained, leading to the present invention.
好にするため、保磁力の温度依存性が磁気記録媒体られ
る異方性エネルギーの三軸異方性成分の温度依存性にほ
ぼ一致し、温度θ℃で面内で磁気トルクを測定してフー
リエ展開することにより求め′ た異方性エネルギーの
玉軸異方性成分(Kco)と、温度θ℃での保磁力(H
co)およttjt”和磁化(llso)と、温度10
0℃で面内で磁気トルクを測定してフーリー展開するド
と蔽より求めた異方性−ネ′ブギーの三軸異方性成分(
Kcloo)、と、温度↓00℃での7 ”
′□ 。In order to make the temperature better, the temperature dependence of the coercive force almost matches the temperature dependence of the triaxial anisotropic component of the anisotropic energy of the magnetic recording medium, and the magnetic torque is measured in the plane at a temperature of θ°C and then Fourier The ball axis anisotropy component (Kco) of the anisotropic energy obtained by expansion and the coercive force (H
co) and ttjt” sum magnetization (llso) and temperature 10
The anisotropy obtained from the Fourie expansion by measuring the magnetic torque in the plane at 0°C - Ne'Bougie's triaxial anisotropy component (
Kcloo), and temperature ↓7 at 00℃
′□.
す保磁力(、Hc 1’o、o)およq飽和磁、化(I
sloo)とが、式%式%
で表わされる関係にあることが好ましく、この範囲外に
なって保磁力の温度依存性が前記玉軸異方性成分の温度
依存性に一致しなくなると、垂直磁化が充分に良好にな
らず、高密度記録が良好軽打なえない。The coercive force (, Hc 1'o, o) and q saturation magnetism, (I
slooo) is preferably in the relationship expressed by the formula % formula %. If the temperature dependence of the coercive force does not match the temperature dependence of the ball axis anisotropy component outside this range, the vertical Magnetization is not good enough, and high-density recording cannot be performed well.
このよう、に、この発明の磁気記録媒体は保磁力の温度
依存性が磁気記録媒体の磁気トルク、を面内で測定し7
−リエ展開して得られる異方性エネルギーの三軸異方性
成分の温度依存性にほぼで致する関係にあるこζが好ま
しく、従ってこの発明において使用する磁性粉末として
は、磁気記録媒体としたとき上記の式で表わされる関係
が保持できるものであるこ・とが好ましく、たとえ番シ
、・酸化鉄磁性粉末の粒子内部にコ、バ/I/)を均一
に固溶させた比較的三軸異方性成分の多い軸匙(長軸/
短軸)が3〜15の針状のコバルト含有酸化鉄磁性粉末
が好適なものとして使用され、保磁力600〜L−50
0エルステツドのものが好ましぐ使用される0 ・
1.・・ ・ ・ ゛・ 1 ・この
ような磁性粉末を使用してこの発明の磁気記録媒体を製
造するには常法に準じて行なえばよく、たとえば1.前
記のコバルト含有酸化鉄磁性粉末を、結合剤樹脂、有機
溶剤およびその他の添加剤等とともに混合分散して磁性
塗料を調製し、この磁性塗料をポリエステルフィルみな
どの基体上にロールコータ−など任意の塗布手段によっ
て塗布し、乾燥すればよい。 。As described above, the magnetic recording medium of the present invention has a temperature dependence of coercive force that can be measured by measuring the magnetic torque of the magnetic recording medium in-plane.
- It is preferable that the anisotropic energy obtained by the Rie expansion has a relationship that approximately corresponds to the temperature dependence of the triaxial anisotropic component. Therefore, as the magnetic powder used in this invention, it is preferable that It is preferable that the relationship expressed by the above formula can be maintained. Spoon with many anisotropic components (long axis/
Acicular cobalt-containing iron oxide magnetic powder with a short axis of 3 to 15 is preferably used, and has a coercive force of 600 to L-50.
0 Oersted is preferably used.
1.・・ ・ ・゛・1 ・The magnetic recording medium of the present invention can be manufactured using such magnetic powder according to a conventional method. For example, 1. A magnetic paint is prepared by mixing and dispersing the above-mentioned cobalt-containing iron oxide magnetic powder with a binder resin, an organic solvent, and other additives, and this magnetic paint is applied onto a substrate such as a polyester film using a roll coater or other suitable method. It can be applied using the following application means and dried. .
・ここに用いる結合剤樹脂としては、塩化ビ→ルー酢酸
ビニル系共重合体、ポリビニルブチラール、ポリウレタ
ン系樹脂、繊維素系樹脂、イソシアネート化合物など従
来汎用されている結合剤樹脂が広く用いられる6’
、 、=また、有機溶剤としては
、トルエン、メチルイソブチ/I/り・トン〈メチルエ
チルtトン、シクロヘキサノシ、テトラヒドロフラン、
酢酸エチルなどの従来から汎用されている有機溶剤が単
独あるいは二種以上混合して使用さ・れる。・As the binder resin used here, conventionally widely used binder resins such as vinyl chloride→vinyl acetate copolymer, polyvinyl butyral, polyurethane resin, cellulose resin, and isocyanate compound are widely used6'
, ,=Also, as an organic solvent, toluene, methylisobutylene/I/ton (methyl ethyl ton), cyclohexanoyl, tetrahydrofuran,
Conventionally widely used organic solvents such as ethyl acetate can be used alone or in combination of two or more.
なお、磁性塗料中に°は通常使用されている各種添加剤
、たとえば分散側、潤滑剤、研磨剤、帯電防止剤などを
任意ji’mmi’t、でもよい。Incidentally, various additives commonly used in magnetic paints, such as dispersants, lubricants, abrasives, antistatic agents, etc., may be optionally added.
実施例1
粒径(長軸)0.15μ、軸比(長軸/短軸)8・のr
−Fe、03粉末1ooofを水1.OIt中に分散さ
せた後、これに硫酸コバル)380Fと硫酸第一鉄11
30Fとを加えて混合溶解し、次いで苛性ソーダ130
0gを溶解した苛性ソーダ水溶液51を加えて45℃で
8時間反応させた。反応終了後、水洗1、ヤ過、乾燥し
、その後空気中で450℃の潟、度で≦時間加熱酸化し
てコバルト固溶酸化鉄磁性粉末を得た。得られたコバル
ト固溶酸化鉄磁性粉末は三軸異方性の針状の粉末で、粒
径(長軸)は0.2μ、軸比(長軸/短軸)はβ 、コ
バルト含有量は5.7重量幅で、保磁力(Hc)は11
00エルステツドであった。Example 1 Particle size (long axis) 0.15μ, axial ratio (long axis/short axis) 8.r
-100 of Fe, 03 powder and 1.0 of water. After dispersing in OIt, this was mixed with cobal sulfate) 380F and ferrous sulfate 11
30F and mix and dissolve, then add caustic soda 130F.
A caustic soda aqueous solution 51 in which 0 g of sodium hydroxide was dissolved was added and reacted at 45° C. for 8 hours. After the reaction was completed, it was washed with water, filtered and dried, and then heated and oxidized in the air at 450° C. for ≦ hours to obtain cobalt solid-dissolved iron oxide magnetic powder. The obtained cobalt solid solution iron oxide magnetic powder is a triaxially anisotropic acicular powder with a particle size (long axis) of 0.2μ, an axial ratio (long axis/short axis) of β, and a cobalt content of 5.7 weight range, coercive force (Hc) is 11
It was 00 Oersted.
このようにして得られたコバルト固溶酸化鉄磁性粉末を
使用し、
Co固溶r −Fe、O,粉末 750重量部
VAGH(米国U 、C、C社製、塩化 125 〃
ビニルー酢酸ビニルービニルアル
コール共重合体)
バンデツクスT−5250(大 100 〃日本イン
キ社製、ウレタンエラス
トマー)
コロネー)L(日本ポリウレタンエ 25重量部業社
製、三官能性低分子量イソシア
ネート化合物)
ステアリン酸−n−ブチル 15 〃メチルイソ
ブチルケトン 600 〃トルエン
、・ 600 1/の組成からなる組成物をボ
ーαミル中で平日間混合分散して磁性塗料を調製した。Using the thus obtained cobalt solid solution iron oxide magnetic powder, Co solid solution r -Fe, O, powder 750 parts by weight VAGH (manufactured by U.C., U.S.A., chloride 125
Vinyl-vinyl acetate-vinyl alcohol copolymer) Bandex T-5250 (Dai 100, manufactured by Nippon Ink Co., Ltd., urethane elastomer) Coronae) L (manufactured by Nippon Polyurethane 25 Weight Division Co., Ltd., trifunctional low molecular weight isocyanate compound) Stearic acid -n-butyl 15 〃Methyl isobutyl ketone 600 〃Toluene
A magnetic coating material was prepared by mixing and dispersing a composition having a composition of .
この磁性塗料を厚さ12μのポリエステルベースフィル
ム上に乾燥厚が3μとなるように塗布、乾燥し、表面処
理を行なった後、所定6巾に裁mlしで磁気テープをつ
くった。This magnetic paint was applied onto a 12 μm thick polyester base film to a dry thickness of 3 μm, dried, surface treated, and then cut into a predetermined width of 6 to form a magnetic tape.
実施例2
実施例1におい5て、硫酸コバルトの使用量を38of
から28.51に変更し、硫酸節で鉄の使用量を113
0 f、から85ofに変更し、さらに苛性ソーダの使
、用量を1.300fから975Iに変更し・た以外は
実施例1と同・様にして、粒径(8長軸)0.18μ、
軸比(長軸/短軸) 8 、コバルト含有量4.6重量
%、保磁力(Hc) 950エルステツドの針状で三軸
異方性のコバルト固溶酸化鉄磁性粉末を得、このように
して得られたコバルト固溶酸化鉄磁性粉末を実施例1に
おける磁性塗料のCo固溶r −Fe20B粉末に代え
て同量使用した以外は実施例1と同様にして磁気テープ
をつくった。Example 2 In Example 1, the amount of cobalt sulfate used was 38 of
to 28.51, and the amount of iron used in the sulfuric acid clause was changed to 113.
The procedure was the same as in Example 1, except that the amount of caustic soda was changed from 0f to 85of, and the amount of caustic soda was changed from 1.300f to 975I, and the particle size (8 major axis) was 0.18μ,
An acicular, triaxially anisotropic cobalt solid solution iron oxide magnetic powder with an axial ratio (major axis/minor axis) of 8, a cobalt content of 4.6% by weight, and a coercive force (Hc) of 950 oersted was obtained. A magnetic tape was produced in the same manner as in Example 1, except that the same amount of the cobalt solid-solubilized iron oxide magnetic powder obtained in Example 1 was used in place of the Co-solid-solubilized r-Fe20B powder in the magnetic paint.
実施例3
実施例1において、出発原料の粒径(長軸)0.15μ
、軸比(長軸/短軸) 8 のr Fe20B粉末に
代えて、粒径(長軸)0.4μm軸比(長軸/短軸)1
0のγ−Fe、03粉末を出発原料として同量使用した
以外は実施例1と同様にして、粒径(長軸)0.42μ
、軸比(長軸/短軸)10、コバルト含有量5.7重量
%、保磁力(Hc)ios□エルステッドの針状施例1
における磁性塗料のCO固固溶−Fe、03粉末に代え
て同量使用した以外は実施例1と同様にして磁気テープ
をつくった。Example 3 In Example 1, the particle size (long axis) of the starting material was 0.15μ.
, axial ratio (long axis/short axis) of r Fe20B powder of 8, particle size (long axis) of 0.4 μm axial ratio (long axis/short axis) of 1
The same procedure as in Example 1 was carried out except that the same amount of γ-Fe, 03 powder was used as the starting material, and the particle size (long axis) was 0.42μ.
, axial ratio (major axis/minor axis) 10, cobalt content 5.7% by weight, coercive force (Hc) ios Ørsted needle-like example 1
A magnetic tape was prepared in the same manner as in Example 1, except that the same amount of CO solid solution -Fe and 03 powder in the magnetic paint was used in place of the powder.
比較例1
実施例1において、r Fe、03粉末の分散水溶液
中に硫酸コバルトと硫酸第一鉄を加え、さらに苛性ソー
ダを加えて反応させた後の空気中での加熱処理を省いた
以外は実施例1と同様にして、表面層にコバルトを含有
する粒径(長軸)0.2μ、軸比(長軸/短軸)8、コ
バルト含有量5.7重量%、保磁力(He)1100エ
ルステツドの針状で一軸異方性のコバルト含有酸化鉄磁
性粉末を得、さらにこのようにして得られたコバルト含
有酸化鉄磁性粉末を実施例1における磁性塗料のCo固
固溶−Fe、03粉末に代えて同量使用した以外は実施
例1と同様にして磁気テープをつくった。Comparative Example 1 The same procedure as in Example 1 was carried out except that cobalt sulfate and ferrous sulfate were added to the dispersion aqueous solution of rFe, 03 powder, and the heat treatment in air after adding and reacting with caustic soda was omitted. In the same manner as in Example 1, the particle size (major axis) containing cobalt in the surface layer was 0.2μ, the axial ratio (major axis/minor axis) was 8, the cobalt content was 5.7% by weight, and the coercive force (He) was 1100. A cobalt-containing iron oxide magnetic powder having an acicular shape and uniaxial anisotropy was obtained, and the cobalt-containing iron oxide magnetic powder thus obtained was further added to the Co solid solution of the magnetic paint in Example 1 - Fe, 03 powder. A magnetic tape was produced in the same manner as in Example 1, except that the same amount was used instead of .
各実施例および比較例で得られた磁気テープについて、
温度θ℃で面内で磁気トルクを測定し、これをフーリエ
展開して異方性エネルギーの三軸異方性成分(Kco)
を求め、温度θ℃での保磁力(HCO)および飽和磁化
(Iso )を測定した。また、温度100℃で面内で
磁気トルクを測定し、これを7−リエ展開して異方性エ
ネルギーの三軸異方性成分(Kcloo)を求め、温度
100℃での保磁力(Hcloo)および飽和磁化(l
51oo)を測定した。次いでこれらの測定値を、式
%式%
に代入してその数値を求めた。また、記録波長0.75
μにおける最大出力レベルを測定した。Regarding the magnetic tapes obtained in each example and comparative example,
The magnetic torque is measured in the plane at a temperature of θ℃, and this is Fourier expanded to obtain the triaxial anisotropic component of the anisotropic energy (Kco).
was determined, and the coercive force (HCO) and saturation magnetization (Iso) at a temperature of θ°C were measured. In addition, the magnetic torque was measured in the plane at a temperature of 100°C, and this was expanded into 7-liers to obtain the triaxial anisotropic component (Kcloo) of the anisotropic energy, and the coercive force (Hcloo) at a temperature of 100°C was obtained. and saturation magnetization (l
51oo) was measured. Next, these measured values were substituted into the formula % formula % to obtain the numerical value. Also, the recording wavelength is 0.75
The maximum output level at μ was measured.
下表はその結果である。The table below shows the results.
表
上表から明らかなように、この発明で得られた磁気テー
プ(実施例1〜3)は、従来の磁気チーα1)
プ(比較例1)に比し、0.75μの短波長での最大出
力レベルが大きく、このことからこの発明によって得ら
れる磁気記録媒体)ま高密度記録に適していゐことがわ
かる。As is clear from the above table, the magnetic tapes obtained according to the present invention (Examples 1 to 3) have a short wavelength of 0.75μ compared to the conventional magnetic tape (Comparative Example 1). The maximum output level is high, which indicates that the magnetic recording medium obtained by the present invention is suitable for high-density recording.
特許出願人 日立マクセル株式会社 1゛41″ αのPatent applicant: Hitachi Maxell, Ltd. 1゛41″ α's
Claims (1)
録媒体において、温度θ℃で面内で磁気トルクを測定し
て7−リエ展開することにより求めた異方性エネルギー
の三輪異方性成分(Kco)と、温度0℃での保磁力(
Hco)、および飽和磁化(Iso)と、温度100℃
で面内で磁気トルクを測定して7−リエ展開することに
より求めた異方性エネルギーの三軸異方性成分(Kcl
oo)と、温度100℃での保磁力(Hctao)およ
び飽和磁化(Isloo)、とが、式1式% で表わされる関係にあることを特徴とする磁気記録媒体
□ ′[Claims] 1. Anisotropy determined by measuring magnetic torque in the plane at a temperature of θ°C and performing 7-lier expansion in a magnetic recording medium in which magnetic powder is coated on a substrate together with a binder. The three-ring anisotropic component of energy (Kco) and the coercive force at a temperature of 0°C (
Hco), saturation magnetization (Iso), and temperature 100°C
The triaxial anisotropic component of the anisotropic energy (Kcl
A magnetic recording medium characterized in that the coercive force (Hctao) and saturation magnetization (Isloo) at a temperature of 100° C. have a relationship expressed by Formula 1 % □ ′
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP8205082A JPS58199434A (en) | 1982-05-15 | 1982-05-15 | Magnetic recording medium |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP8205082A JPS58199434A (en) | 1982-05-15 | 1982-05-15 | Magnetic recording medium |
Publications (1)
| Publication Number | Publication Date |
|---|---|
| JPS58199434A true JPS58199434A (en) | 1983-11-19 |
Family
ID=13763680
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP8205082A Pending JPS58199434A (en) | 1982-05-15 | 1982-05-15 | Magnetic recording medium |
Country Status (1)
| Country | Link |
|---|---|
| JP (1) | JPS58199434A (en) |
Cited By (1)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| WO2022070963A1 (en) * | 2020-09-30 | 2022-04-07 | 富士フイルム株式会社 | Magnetic recording medium, magnetic tape cartridge, and magnetic recording playback device |
-
1982
- 1982-05-15 JP JP8205082A patent/JPS58199434A/en active Pending
Cited By (3)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| WO2022070963A1 (en) * | 2020-09-30 | 2022-04-07 | 富士フイルム株式会社 | Magnetic recording medium, magnetic tape cartridge, and magnetic recording playback device |
| JPWO2022070963A1 (en) * | 2020-09-30 | 2022-04-07 | ||
| US11842756B2 (en) | 2020-09-30 | 2023-12-12 | Fujifilm Corporation | Magnetic recording medium, magnetic tape cartridge, and magnetic recording and reproducing device |
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