JPH038015B2 - - Google Patents
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- Publication number
- JPH038015B2 JPH038015B2 JP56028487A JP2848781A JPH038015B2 JP H038015 B2 JPH038015 B2 JP H038015B2 JP 56028487 A JP56028487 A JP 56028487A JP 2848781 A JP2848781 A JP 2848781A JP H038015 B2 JPH038015 B2 JP H038015B2
- Authority
- JP
- Japan
- Prior art keywords
- magnetic powder
- magnetic
- tape
- surface roughness
- powder
- 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 - Lifetime
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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
- G11B5/706—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 characterised by the composition of the magnetic material
- G11B5/70605—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 characterised by the composition of the magnetic material metals or alloys
- G11B5/70615—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 characterised by the composition of the magnetic material metals or alloys containing Fe metal or alloys
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- Engineering & Computer Science (AREA)
- Metallurgy (AREA)
- Paints Or Removers (AREA)
- Magnetic Record Carriers (AREA)
Description
鉄を主成分とする針状合金磁性粉は、従来磁気
記録媒体用に使われている、CrO2、γ−Fe2O3、
Co被着型γ−Fe2O3等の酸化物磁性粉に比較し、
1.5倍以上の保磁力と飽和磁気モーメントを持ち、
再生出力を大巾に向上させることが可能であり、
高密度記録用磁性材料に適した優れた特性をもつ
ている。
この合金性粉を作製する製造法については、い
ままで多くの方法が特許、文献等で発表されてい
る。それらの方法には大別してつぎの4つの方法
がある。(1)α−FeOOH等の針状鉄酸化物を加熱
還元する方法。(2)ボロハイドライド化合物のよう
な還元剤を用いて金属塩水溶液から金属粉を還元
析出させる方法。(3)Ar等の不活性気体中で金属
を蒸発させ金属粉を得る方法。(4)Hg陰極に金属
粉を電解析出させる方法等がある。しかしいずれ
の方法においても得られた金属粉の表面は化学的
に活性が強く、テープあるいはデイスク製造工程
においてバインダと化学反応を起こす、あるいは
化学反応を起こさないまでも金属磁性粉の持つ大
きな磁気モーメントのための磁性粉同士の凝集が
起こりやすく、磁性粉の分散性や、塗布後の塗膜
表面性をそこなう原因となる。
このような理由により、合金磁性粉を塗布した
記録媒体は出力Cにおいて酸化物磁性粉を用いた
媒体に比較し4〜10dBの向上を見ているにもか
かわらず、信号記録時に発生する変調ノイズ
(Nn)もそれにほぼ比例して増大し信号対雑音比
(C/N)では大きな改善が見られていない。
高C/N化を目的として、(1)合金磁性粉の表面
に緻密な極薄酸化被膜を生成したり、表面活性剤
を用いて合金磁性粉表面の改質を行うことによつ
て、合金磁性粉の塗膜中における分散性と塗膜表
面性を改良する方法。(2)磁性粉の粒子サイズを微
粒子化する、などの手段がとられている。
しかしノイズの発生原因は記録媒体の面粗さ
と、使用している磁性粉の粒子サイズおよび磁気
特性が相互に密接に結びついているものであり、
どちらか一方の改良のみでは本質的にC/Nを改
善することができない。
たとえば、オーデイオの分野で行われているよ
うに、そのS/Nをある記録波長における出力と
AC消去ノイズ(NAC)の比として評価するよう
な場合には、S/Nの向上はAC消去ノイズを低
減することによつて達成されるが、これは後述す
るようにAC消去ノイズ量は媒体面粗さより粒子
サイズに影響されるため、主に粒子サイズを微細
化することによつて可能となる。これに反してビ
デオの領域では、キヤリア信号記録時にキヤリア
近傍にサイドバンドとして発生する変調ノイズ
(Nm)が画像品質に与える影響は大きく、ノイ
ズ評価には変調ノイズも合わせて行う必要があ
り、オーデイオに比較してより厳しいものとな
る。この変調ノイズの発生原因は、従来、塗膜中
の磁性粒子の凝集塊あるいは面粗さにあると考え
られており、主に変調ノイズの低減はテープ塗布
法を改善することによつて行われていた。
しかし、本発明者等の検討によれば、変調ノイ
ズは磁性粉の凝集塊、塗膜面粗さ以外に磁性粉の
粒子サイズが大きな影響を与えるものであり、面
粗さ等の改良だけでは、酸化物系磁性粉を用いた
磁気記録媒体のC/N特性を凌駕する合金磁性粉
を用いた磁気記録媒体を得るのは困難であり、面
粗さの改良と粒子サイズの微細化を同時に行う必
要のあることを見出した。
本発明の目的は、針状合金磁性粉を塗布した磁
気記録媒体のC/N特性を向上するための手段を
与えるものであり、Co被着型γ−Fe2O3磁性粉末
を塗布したテープよりC/N特性が3dBあるいは
5dB以上となるべき、針状合金磁性粉末の粒子サ
イズと磁気特性、ならびに記録媒体面粗さの関係
を規定したものである。上記Co被着型γ−Fe2O3
塗布のテープとして、VTR用のT−60E(日立マ
クセル株式会社の商品名)テープを標準とした。
以下本発明の原理的な説明を行う。
磁気記録媒体から発生する全媒体ノイズ(N)
は第1図に示したごとく2つの部分から成りたつ
ている。1つはAC消去を行つたときに発生する
AC消去ノイズ(NAC)21と、他は信号を記録
したときに発生する変調ノイズ(Nn)22の2
種類である。なお以下の文章において、ノイズ量
とは第1図に示したように、1MHzから7MHzの帯
域の斜線部分を積分した値をいう。また、これら
のノイズ量間には式(1)に示したような関係が成り
立つている。
N=√A 2 C+2 ……(1)
本発明者等はこれらのノイズの発生原因を以下
に記したごとく明らかとした。
AC消去ノイズは主に磁性粉末の飽和磁化量
(σs)とその粒子サイズ、体積(v)ならびに媒
体の飽和磁束密度(Bs)に関係する量であり、
また水素還元法で作製された合金磁性粉の場合は
焼結の有無にも関係してくるものである。第3図
にAC消去ノイズと面粗さの関係を示したがこの
AC消去ノイズは塗膜中の磁性粉の分散性や面粗
さとの相関性が小さく、主に磁性粉の粒子サイズ
に関係してくる量であることが分かる。
一方変調ノイズはキヤリア信号記録時に、信号
近傍のサイドバンドとして発生し、その大きさは
信号出力に比例する。そしてその比例係数は第2
図に示したように面粗さが悪いほど、また粒子サ
イズが大きいほど大きくなり、従つて変調ノイズ
も大きくなる。
このように全媒体ノイズを低減するには、なか
でも変調ノイズを低減するにはテープ面粗さをよ
くし、なおかつ粒子サイズを小さくする必要があ
り、標準テープ(日立マクセルK.K.製VTR用T
−60E)よりC/N特性が3dB以上となるべき、
テープ面粗さと粒子サイズの関係は第4図に示し
た曲線上の点であるか、あるいはそれより下の領
域にあることを見い出した。
しかし、適当なテープ面粗さ、粒子サイズには
以下に記すような下限が存在するとともに、本発
明の効果を有効に発揮すべき合金磁性粉の磁気特
性は下記のような条件を満足せねばならない。
まずテープ面粗さは平滑にするほどC/Nが向
上するのであるが、平滑にしすぎて、例えば実施
例3に示したように面粗さが0.02μmP-P以下にな
ると、磁気テープ特にVTR用の場合には、テー
プ・ヘツド相対速度が大きいため、テープ・ヘツ
ド間の摩擦が増大し、走向特性が悪くなつたり、
テープ塗膜がはく離しヘツドの目づまりを起こ
す。このような理由から、ヘツドと直接接触する
ような磁気テープの場合はその面粗さを
0.025μmP-P以上にすることが望ましい。ただしこ
の制限は塗布型デイスクのように媒体面上をヘツ
ドが接触せず浮上しているような場合には必要な
いものである。
さらに針状合金磁性粉の粒子サイズについて
は、面粗さに下限のあることから、その長軸長を
0.45μm以下にすることが望ましいが、粒子サイ
ズが小さすぎると例えば実施例4のように長軸長
が0.1μm未満の針状合金磁性粉では、大気中にお
いてその表面が酸化され、酸化膜が針状合金の芯
にまで達つし、もはや磁性体として存在し得ない
か、あるいは金属磁性粉としての磁気的な特徴を
失つてしまう。
この針状合金磁性粉の粒子サイズの下限につい
ては従来粒状Fe粉の場合に超常磁性が現われ始
める100Å付近にあるとされていた。しかし、Fe
を主成分とする合金粉の場合には、それを大気中
にとりだしても燃焼しないように安定化するため
には、最低50Åの酸化保護膜が必要であり、例え
ば短軸長100Åの針状合金磁性粉では空気中にお
ける安定性を付与するにはそのすべてが酸化され
てしまう。また実施例4でも述べるように、その
粒子サイズが小さ過ぎる場合には、大部分がFe
酸化物となるため磁気特性をそこなうことにな
る。したがつて粒子サイズの下限は安定性を付与
する酸化膜の厚さから決定される。
このような理由から本発明に使われるべき針状
合金磁性粉の短軸長は0.02μm以上、長軸長で約
0.1μm以上であることが望ましい。また長軸短軸
比は一軸異方性を保持するように、5〜15の範囲
であればよい。
また、本発明に適用されるべき針状合金磁性粉
の磁気特性は以下の条件を満足しなくてはならな
い。針状合金磁性粉は一般にその保磁力は粒子サ
イズによつて影響され、粒子サイズが小さいほど
保磁力が増大する傾向がある。本発明でいう針状
合金磁性粉の長軸長は0.45〜0.1μmの範囲である
が、このような領域では、当該磁性粉試料(無配
向、充填率約10%)を最大測定磁場10KOeで、
測定した磁気特性は、角型比が少なくとも0.49以
上、保磁力1100Oe以上の特性をもつべきもので
あり、それ以下の角型比あるいは保磁力を有する
針状合金磁性粉を電子顕微鏡で観察すると針状性
が悪かつたり、また水素還元法で作られた合金粉
の場合には焼結現象が見られる。このような合金
磁性粉末を塗布したテープでは実施例5にあるよ
うに、出力が低く、かつノイズが増大するため本
発明の効果を有効に発揮することができない。こ
のように本発明に言う針状合金磁性粉末はその保
磁力が1100Oe、角型比が0.49以上であることが
望ましい。
なお本発明で対照となる合金磁性粉とは鉄を主
成分とした針状合金磁性粉であり、その金属組成
中の鉄含量が100重量%の純鉄金属粉末ならびに
ニツケル、コバルト、クロム、スズ、アルミニウ
ム、チタン、ボロン、シリコン等の添加元素を含
んだ合金をさす。
以下本発明を実施例を参照して詳細に説明す
る。
実施例 1
長軸長0.33μm、長軸対短軸比10の合金磁性粉
を、所定温度のトルエン中に懸濁しこの懸濁液中
に空気を吹き込み、曝気処理を行つて合金磁性粉
末の表面に緻密な酸化膜層を形成した。その磁性
粉Aの磁気特性は、Hc1350Oe、σs126emu/g、
σr/σs=0.50であつた。
この磁性粉を用いて、ポリウレタン樹脂をバイ
ンダとする磁性塗料を調製し、これをポリエステ
ルフイルム上に乾燥塗布厚4μmとなるように塗着
した後、表面粗さの異なる磁気テープを得るた
め、カレンダロール処理回数の異なる2種類のテ
ープを得た。それらのテープを2,3とし、その
特性等を第1表に示した。
実施例 2
長軸長0.37μm、長軸対短軸比10の合金磁性粉
を実施例1と同様な方法でその表面に酸化膜層を
形成した磁性粉Bを得た。その磁気特性は、
Hc1280Oe、σs128emu/g、σr/σs=0.51であつ
た。
この磁性粉を実施例1と同じバインダを用い
て、ボールミル処理時間を実施例1より長くして
分散性のよい塗料を調製しテープに塗着した。そ
の後実施例1と同様な方法で面粗さの異なる3種
類のテープ4,5,6を得た。その特性等を第1
表に示す。
実施例 3
実施例1、2と異なる粒子サイズをもつ3種類
の合金磁性粉を用いて、実施例1と同様な酸化膜
被覆処理を施した。これらの合金磁性粉をC.D.E
とした時、その粒子サイズと磁気特性は以下のよ
うであつた。
粉末C;長軸長0.45μm、軸比12
Hc=1250Oe、σs=129emu/g、σr/σs=0.53
粉末D;長軸長0.30μm、軸比8
Hc=1270Oe、σs=127emu/g、σr/σs=0.52
粉末E;長軸長0.22μm、軸比9
Hc=1400Oe、σs=124emu/g、σr/σs=0.50。
これらの合金磁性粉末を実施例2と同じバイン
ダ、分散条件で磁性粉塗料を調製し、テープに塗
着した。その後実施例1と同様な方法で、粒子サ
イズの異なるテープについて、それぞれ2種類の
面粗さの異なるテープ7,8,9,10,11,
12を得た。その特性等を第1表に示す。
上記実施例で得られたこれらの11種類の磁気テ
ープを最大磁場10kOeの条件で測定した時の磁気
特性、ならびに触針式粗さ計(ペルト社製ペルト
メータWVR型)を用いて測定した面粗さ
(75μmのハイパスフイルタを使用した時のピーク
対ピーク値;Rz)を第1表に示した。
実施例1、2、3で作製されたテープの記録再
生特性を改造したVHS型家庭用VTRデツキの走
向系を使つて測定した。測定ではヘツド出力を
0.1〜10MHzの周波数帯域でフラツトな利得
(60dB)をもつアンプを通して、その出力、AC
消去ノイズ、変調ノイズを測定した。測定条件は
ヘツドテープ相対速度4.0m/s、記録周波数4M
Hzである。使用ヘツドの有効ギヤツプ長は0.4μm
である。その結果も第1表に示した。
なお標準テープとして、Co被着型γ−Fe2O3
Acicular alloy magnetic powders containing iron as a main component are CrO 2 , γ-Fe 2 O 3 , CrO 2 , γ-Fe 2 O 3 ,
Compared to oxide magnetic powder such as Co-coated γ-Fe 2 O 3 ,
It has a coercive force and saturation magnetic moment more than 1.5 times,
It is possible to greatly improve the playback output,
It has excellent properties suitable as a magnetic material for high-density recording. Many methods for manufacturing this alloy powder have been published in patents, literature, etc. so far. These methods can be broadly classified into the following four methods. (1) A method of thermally reducing acicular iron oxides such as α-FeOOH. (2) A method in which metal powder is reduced and precipitated from an aqueous metal salt solution using a reducing agent such as a borohydride compound. (3) A method to obtain metal powder by evaporating metal in an inert gas such as Ar. (4) There is a method of electrolytically depositing metal powder on the Hg cathode. However, in either method, the surface of the metal powder obtained is highly chemically active, causing a chemical reaction with the binder during the tape or disk manufacturing process, or even if no chemical reaction occurs, the metal magnetic powder has a large magnetic moment. Because of this, agglomeration of magnetic powders tends to occur, which causes damage to the dispersibility of the magnetic powders and the surface properties of the coated film after application. For these reasons, even though recording media coated with alloy magnetic powder show an improvement of 4 to 10 dB in output C compared to media using oxide magnetic powder, the modulation noise generated during signal recording is (N n ) also increases almost proportionally, and no significant improvement is seen in the signal-to-noise ratio (C/N). For the purpose of increasing C/N, (1) forming a dense ultra-thin oxide film on the surface of the alloy magnetic powder or modifying the surface of the alloy magnetic powder using a surfactant; A method for improving the dispersibility of magnetic powder in a coating film and the surface properties of the coating film. (2) Measures have been taken to reduce the particle size of magnetic powder. However, the cause of noise is that the surface roughness of the recording medium and the particle size and magnetic properties of the magnetic powder used are closely linked to each other.
C/N cannot essentially be improved by improving only one of them. For example, as is done in the audio field, the S/N is calculated as the output at a certain recording wavelength.
When evaluated as a ratio of AC cancellation noise (N AC ), S/N improvement is achieved by reducing AC cancellation noise, but as will be explained later, this means that the amount of AC cancellation noise is Since this is influenced more by the particle size than by the medium surface roughness, this can be achieved mainly by making the particle size finer. On the other hand, in the video domain, modulation noise (Nm) that occurs as a sideband near the carrier when recording a carrier signal has a large effect on image quality, and noise evaluation must also include modulation noise. It is more severe compared to . The cause of this modulation noise has traditionally been thought to be agglomerates of magnetic particles in the coating film or surface roughness, and modulation noise has been mainly reduced by improving the tape coating method. was. However, according to the studies conducted by the present inventors, modulation noise is greatly influenced by the particle size of the magnetic powder, in addition to the agglomerates of the magnetic powder and the coating surface roughness, and improvements in surface roughness, etc. alone cannot improve modulation noise. It is difficult to obtain a magnetic recording medium using alloy magnetic powder that has superior C/N characteristics to magnetic recording media using oxide-based magnetic powder, and it is difficult to obtain a magnetic recording medium using alloy magnetic powder that has superior C/N characteristics to magnetic recording media using oxide-based magnetic powder. I saw what needed to be done. An object of the present invention is to provide a means for improving the C/N characteristics of a magnetic recording medium coated with acicular alloy magnetic powder, and to provide a tape coated with Co-coated γ-Fe 2 O 3 magnetic powder. The C/N characteristic is 3dB or more.
This specifies the relationship between the particle size of the acicular alloy magnetic powder, the magnetic properties, and the surface roughness of the recording medium, which should be 5 dB or more. The above Co-coated type γ-Fe 2 O 3
The standard application tape was T-60E (trade name of Hitachi Maxell, Ltd.) tape for VTRs. The principle of the present invention will be explained below. Total media noise (N) generated from magnetic recording media
consists of two parts as shown in Figure 1. One occurs when performing AC erase.
AC cancellation noise (N AC ) 21 and modulation noise (N n ) 22 that occurs when the signal is recorded.
It is a kind. In the following text, the amount of noise refers to the value integrated over the shaded area of the band from 1MHz to 7MHz, as shown in Figure 1. Furthermore, the relationship shown in equation (1) holds between these noise amounts. N=√ A 2 C + 2 (1) The inventors have clarified the cause of these noises as described below. The AC cancellation noise is mainly related to the saturation magnetization amount (σ s ) of the magnetic powder, its particle size, volume (v), and the saturation magnetic flux density (B s ) of the medium.
In addition, in the case of alloy magnetic powder produced by the hydrogen reduction method, the presence or absence of sintering also matters. Figure 3 shows the relationship between AC cancellation noise and surface roughness.
It can be seen that the AC erase noise has little correlation with the dispersibility and surface roughness of the magnetic powder in the coating film, and is mainly related to the particle size of the magnetic powder. On the other hand, modulation noise occurs as a sideband near the signal when recording a carrier signal, and its magnitude is proportional to the signal output. And its proportional coefficient is the second
As shown in the figure, the worse the surface roughness and the larger the particle size, the larger the modulation noise becomes. In order to reduce total media noise in this way, especially to reduce modulation noise, it is necessary to improve the tape surface roughness and reduce the particle size.
-60E), the C/N characteristic should be 3 dB or more.
It has been found that the relationship between tape surface roughness and particle size is at a point on the curve shown in FIG. 4 or in a region below it. However, there are lower limits to the appropriate tape surface roughness and particle size as described below, and the magnetic properties of the alloy magnetic powder to effectively exhibit the effects of the present invention must satisfy the following conditions. No. First, the smoother the tape surface, the better the C/N. However, if it is made too smooth and the surface roughness becomes less than 0.02 μm PP , as shown in Example 3, then the C/N will be improved. In this case, the relative speed between the tape and the head is high, so the friction between the tape and the head increases, resulting in poor strike characteristics.
The tape coating peels off and causes clogging of the head. For this reason, in the case of magnetic tape that comes into direct contact with the head, the surface roughness should be
It is desirable to make it 0.025μm PP or more. However, this restriction is not necessary in the case of a coated disk in which the head floats above the medium surface without contacting it. Furthermore, regarding the particle size of the acicular alloy magnetic powder, since there is a lower limit to the surface roughness, the length of its major axis must be determined.
It is desirable that the particle size be 0.45 μm or less, but if the particle size is too small, for example, in the case of acicular alloy magnetic powder with a major axis length of less than 0.1 μm, as in Example 4, the surface will be oxidized in the atmosphere, resulting in an oxide film. It reaches the core of the needle-like alloy and can no longer exist as a magnetic substance, or it loses its magnetic characteristics as a metal magnetic powder. The lower limit of the particle size of this acicular alloy magnetic powder was conventionally thought to be around 100 Å, where superparamagnetism begins to appear in the case of granular Fe powder. However, Fe
In the case of alloy powders whose main components are All of the alloy magnetic powder must be oxidized to provide stability in air. Furthermore, as described in Example 4, if the particle size is too small, most of the Fe
Since it becomes an oxide, the magnetic properties will be impaired. Therefore, the lower limit of particle size is determined by the thickness of the oxide film that provides stability. For this reason, the short axis length of the acicular alloy magnetic powder to be used in the present invention is 0.02 μm or more, and the long axis length is approximately
It is desirable that the thickness is 0.1 μm or more. Further, the long axis short axis ratio may be in the range of 5 to 15 so as to maintain uniaxial anisotropy. Further, the magnetic properties of the acicular alloy magnetic powder to be applied to the present invention must satisfy the following conditions. Generally, the coercive force of the acicular alloy magnetic powder is affected by the particle size, and the smaller the particle size, the higher the coercive force tends to be. The long axis length of the acicular alloy magnetic powder in the present invention is in the range of 0.45 to 0.1 μm. ,
The measured magnetic properties should have a squareness ratio of at least 0.49 and a coercive force of 1100 Oe or more.If an acicular alloy magnetic powder with a lower squareness ratio or coercive force is observed under an electron microscope, it will show a needle. In the case of alloy powders with poor shape or produced by hydrogen reduction, a sintering phenomenon is observed. As shown in Example 5, a tape coated with such an alloy magnetic powder has a low output and increases noise, so that the effects of the present invention cannot be effectively exhibited. As described above, it is desirable that the acicular alloy magnetic powder according to the present invention has a coercive force of 1100 Oe and a squareness ratio of 0.49 or more. The alloy magnetic powder to be compared in the present invention is an acicular alloy magnetic powder mainly composed of iron, and includes pure iron metal powder with an iron content of 100% by weight as well as nickel, cobalt, chromium, and tin. , refers to alloys containing additional elements such as aluminum, titanium, boron, and silicon. The present invention will be described in detail below with reference to Examples. Example 1 An alloy magnetic powder with a major axis length of 0.33 μm and a major axis to minor axis ratio of 10 was suspended in toluene at a predetermined temperature, air was blown into this suspension, and aeration treatment was performed to improve the surface of the alloy magnetic powder. A dense oxide film layer was formed on the surface. The magnetic properties of the magnetic powder A are Hc1350Oe, σ s 126emu/g,
σ r /σ s =0.50. Using this magnetic powder, a magnetic paint with polyurethane resin as a binder was prepared, and after coating it on a polyester film to a dry coating thickness of 4 μm, it was calendered to obtain magnetic tapes with different surface roughness. Two types of tapes were obtained which were subjected to different number of roll treatments. These tapes were named 2 and 3, and their properties are shown in Table 1. Example 2 Magnetic powder B having an oxide film layer formed on the surface of alloy magnetic powder having a major axis length of 0.37 μm and a major axis to minor axis ratio of 10 was obtained in the same manner as in Example 1. Its magnetic properties are
Hc1280Oe, σ s 128emu/g, σ r /σ s =0.51. Using the same binder as in Example 1, the magnetic powder was treated with a ball mill for a longer time than in Example 1 to prepare a paint with good dispersibility, and the paint was applied to a tape. Thereafter, three types of tapes 4, 5, and 6 having different surface roughness were obtained in the same manner as in Example 1. First, its characteristics etc.
Shown in the table. Example 3 The same oxide film coating treatment as in Example 1 was performed using three types of alloy magnetic powders having different particle sizes from those in Examples 1 and 2. CDE these alloy magnetic powders
The particle size and magnetic properties were as follows. Powder C: Long axis length 0.45μm, axial ratio 12 Hc = 1250Oe, σ s = 129emu/g, σ r /σ s = 0.53 Powder D: Long axis length 0.30μm, axial ratio 8 Hc = 1270Oe, σ s = 127emu /g, σ r /σ s = 0.52 Powder E; major axis length 0.22 μm, axial ratio 9 Hc = 1400 Oe, σ s = 124 emu/g, σ r /σ s = 0.50. A magnetic powder coating was prepared from these alloy magnetic powders using the same binder and dispersion conditions as in Example 2, and was applied to a tape. Thereafter, in the same manner as in Example 1, two types of tapes 7, 8, 9, 10, 11, and
I got 12. Its characteristics are shown in Table 1. The magnetic properties of these 11 types of magnetic tapes obtained in the above examples were measured under the conditions of a maximum magnetic field of 10 kOe, and the surface roughness was measured using a stylus roughness meter (Peltmeter WVR model manufactured by Pelt). Table 1 shows the peak-to-peak values (Rz) when using a 75 μm high-pass filter. The recording and reproducing characteristics of the tapes prepared in Examples 1, 2, and 3 were measured using a modified VHS type household VTR deck strike system. In the measurement, the head output is
The output, AC
Erasing noise and modulation noise were measured. Measurement conditions were head tape relative speed 4.0m/s, recording frequency 4M.
It is Hz. The effective gap length of the head used is 0.4μm.
It is. The results are also shown in Table 1. As a standard tape, Co-coated γ-Fe 2 O 3
【表】【table】
【表】
を用いた日立マクセルK.K.製VTR用テープT−
60Eを選び、出力C/Nについては(**印)標
純テープの値を0dBとした時の値を、また変調ノ
イズ対出力比とAC消去ノイズは(*印)標準テ
ープの値を1とした時の相対比を第1表に示し
た。
第2図はテープ面粗さと変調ノイズ対出力比
(Nn/C)の関係を各粒子サイズについて示した
ものでありテープ表面が平滑になるほど、また粒
子サイズが小さくなるほど、Nn/Cは域少する。
すなわちC/Nnは向上することを示している。
またこの図は各曲線を面粗さ0に外そうした、延
長線がほぼ原点近くを通つていることから、変調
ノイズの発生原因は磁性粒子の分散性よりも面粗
さに主たる原因のあることをも示しており、C/
Nnの向上には面粗さを平滑にすることが非常に
重要であることを示している。しかし、テープ8
では表面粗さが、0.02μmP-Pと非常に平滑であつ
たが、ヘツドとの摩擦力増大のためテープ塗膜の
はく離が起こり測定不可能であつた。
第3図はAC消去ノイズ(NAC)と面粗さの関
係を示したものであるが、AC消去ノイズは面粗
さにほとんど影響されないこと、さらに、その大
きさの序列は粒子サイズに対応していることが分
かる。
第2図、第3図中の測定点に付せられた数字は
前記各実施例で得られたテープのテープナンバで
ある。
実施例 4
長軸長0.08μm軸比5の合金磁性粉を作製した
後、空気に触れないようにして、実施例1と同じ
ようにトルエン中に懸濁した後、ゆるやかな酸化
条件(温度50℃)で空気曝気して粉末表面に酸化
被膜を形成させ合金磁性粉Fを得た。この磁性粉
の磁気特性は、
Hc=850Oe、σs=95emu/g、σr/σs=0.43
であり、もはや合金磁性粉の磁気特性を失つてい
た。
実施例 5
長軸長0.27μm、軸比7の合金磁性粉を作製し
た後、実施例1と同じようにトルエン中に懸濁
し、空気曝気して粉末表面に酸化被膜を形成させ
合金磁性粉Fを得た。この磁性粉の磁気特性は、
Hc=1030Oe、σr=127emu/g、σr/σs=0.48
であつた。
この合金磁性粉末は、同程度の長軸長の合金磁
性粉末Eより保磁力、角型比とも低くなつてい
る。この合金磁性粉末を、電子顕微鏡で観察する
と針状性が悪く、枝分かれや粒子間の焼結が認め
られた。
この合金磁性粉末を実施例2と同じバインダ、
ならびに分散条件で磁性粉塗料を調製し磁気テー
プ13を得た。
このテープの記録再生特性を実施例1、2、3
と同一条件で測定した結果、第1表に示したよう
に同定度の粒子サイズと面粗さをもつテープ11
より出力、C/Nともに劣つている。
上記の実施例をまとめると、長軸長が0.1μmか
ら0.5μmの間にあり、軸比が5〜15、かつその磁
気特性が保磁力1100Oe、角型比0.49以上の特性
を有する針状合金磁性粉を用いて磁気テープを作
製し、そのテープのC/N特性が標準テープ(日
立マクセルK.K.製、VTR用T−60E;Co被着型
γ−Fe2O3磁性粉使用)より3dB(曲線31)又は
5dB(曲線32)優れた特性を示す場合の粒子サイ
ズとテープ面粗さの関係は第4図に示したように
なる。第4図中、テープ面粗さが0.02μmP-P以下
のものについては、テープ走行特性、塗膜はく離
の点から、前述したように本発明からは除外され
るべきである。またテープ面粗さに下限があるこ
とから、長軸長0.5μmを越える針状合金磁性粉
は、標準テープに対してC/N3dB以上を達成す
ることが困難であり、本発明から除外されるべき
である。同様に長軸長が0.1μm未満の針状合金磁
性粉は、前述したようにその大気中における安定
性より、本発明から除外されるべきである。ま
た、本発明において効果を確認したのは、テープ
面粗さが0.08μmP-P以下の場合である。[Table] Hitachi Maxell KK VTR tape T- using
60E, the output C/N (marked with **) is the value when the value of the standard tape is set to 0 dB, and the modulation noise to output ratio and AC cancellation noise (marked with *) are the values of the standard tape, which are set to 1. The relative ratios are shown in Table 1. Figure 2 shows the relationship between tape surface roughness and modulation noise to output ratio (N n /C) for each particle size. The smoother the tape surface and the smaller the particle size, the smaller the N n /C. area decreases.
That is, it shows that C/N n is improved.
In addition, in this figure, each curve is removed from the surface roughness of 0, and the extension line passes almost near the origin, indicating that the main cause of modulation noise is surface roughness rather than the dispersion of magnetic particles. It also shows that C/
This shows that smoothing the surface roughness is very important for improving N n . However, tape 8
Although the surface roughness was very smooth at 0.02 μm PP , the tape coating peeled off due to the increased frictional force with the head, making measurement impossible. Figure 3 shows the relationship between AC cancellation noise (N AC ) and surface roughness, and it is clear that AC cancellation noise is hardly affected by surface roughness, and furthermore, the order of its size corresponds to particle size. I know what you're doing. The numbers attached to the measurement points in FIGS. 2 and 3 are the tape numbers of the tapes obtained in each of the above Examples. Example 4 After producing alloy magnetic powder with a major axis length of 0.08 μm and an axial ratio of 5, it was suspended in toluene in the same manner as in Example 1 without being exposed to air, and then subjected to mild oxidation conditions (temperature 50 ℃) to form an oxide film on the powder surface to obtain alloy magnetic powder F. The magnetic properties of this magnetic powder were Hc = 850 Oe, σ s = 95 emu/g, σ r /σ s = 0.43, and it had already lost the magnetic properties of the alloy magnetic powder. Example 5 After producing alloy magnetic powder with a major axis length of 0.27 μm and an axial ratio of 7, it was suspended in toluene in the same manner as in Example 1, and aerated with air to form an oxide film on the powder surface to obtain alloy magnetic powder F. I got it. The magnetic properties of this magnetic powder were Hc = 1030 Oe, σ r = 127 emu/g, and σ r /σ s = 0.48. This alloy magnetic powder has lower coercive force and squareness ratio than alloy magnetic powder E having the same major axis length. When this alloy magnetic powder was observed under an electron microscope, it was found that it had poor acicularity, and branching and sintering between particles were observed. This alloy magnetic powder was mixed with the same binder as in Example 2,
A magnetic powder paint was prepared under the same dispersion conditions to obtain a magnetic tape 13. Examples 1, 2, and 3 show the recording and playback characteristics of this tape.
As a result of measurement under the same conditions as shown in Table 1, tape 11 has the same particle size and surface roughness as shown in Table 1.
Both output and C/N are inferior. To summarize the above examples, an acicular alloy having a major axis length between 0.1 μm and 0.5 μm, an axial ratio of 5 to 15, and a magnetic property with a coercive force of 1100 Oe and a squareness ratio of 0.49 or more. A magnetic tape was made using magnetic powder, and the C/N characteristic of the tape was 3 dB better than the standard tape (manufactured by Hitachi Maxell KK, T-60E for VTR; using Co-coated γ-Fe 2 O 3 magnetic powder). Curve 31) or
The relationship between particle size and tape surface roughness when exhibiting excellent characteristics of 5 dB (curve 32) is shown in Figure 4. In FIG. 4, tapes with surface roughness of 0.02 μm PP or less should be excluded from the present invention from the viewpoint of tape running characteristics and coating peeling, as described above. Additionally, since there is a lower limit to tape surface roughness, acicular alloy magnetic powder with a major axis length exceeding 0.5 μm is difficult to achieve a C/N of 3 dB or more compared to standard tape, and is therefore excluded from the present invention. Should. Similarly, acicular alloy magnetic powder with a major axis length of less than 0.1 μm should be excluded from the present invention due to its stability in the atmosphere as described above. Furthermore, the effect of the present invention was confirmed when the tape surface roughness was 0.08 μm PP or less.
第1図は磁気テープのAC消去ノイズと変調ノ
イズを示したグラフ、第2図はテープ面粗さと変
調ノイズ対出力比(Nn/C)の関係を、それぞ
れ粒子サイズの異なる針状合金磁性粉を塗布した
テープについて示したグラフ、第3図は、テープ
面粗さとAC消去ノイズ(NAC)の関係を、それ
ぞれ粒子サイズの異なる針状合金磁性粉を塗布し
たテープについて示したグラフ、第4図は、針状
合金磁性粉を塗布したテープがCo被着型γ−
Fe2O3を塗布した標準テープよりC/Nが3dB以
上あるいは5dB以上の特性をもつ場合の針状合金
磁性粉の粒子サイズとテープ面粗さの相互関係を
示したグラフである。
1乃至12はテープナンバ、21はAC消去ノイ
ズ、22は変調ノイズ、31はC/Nが標準テー
プより3dBすぐれている場合、32はC/Nが標
準テープより5dBすぐれている場合を示す。
Figure 1 is a graph showing AC erasure noise and modulation noise of magnetic tape, and Figure 2 is a graph showing the relationship between tape surface roughness and modulation noise to output ratio (N n /C) for acicular alloy magnetic particles with different particle sizes. Figure 3 is a graph showing the relationship between tape surface roughness and AC cancellation noise (N AC ) for tapes coated with acicular alloy magnetic powder of different particle sizes. Figure 4 shows that the tape coated with acicular alloy magnetic powder is Co-coated γ-
2 is a graph showing the correlation between the particle size of acicular alloy magnetic powder and tape surface roughness when the C/N ratio is 3 dB or more or 5 dB or more compared to a standard tape coated with Fe 2 O 3 . 1 to 12 are tape numbers, 21 is AC erasure noise, 22 is modulation noise, 31 is a case where the C/N is 3 dB better than the standard tape, and 32 is a case where the C/N is 5 dB better than the standard tape.
Claims (1)
性粉を塗布した磁気記録媒体において、当該針状
合金磁性粉の保磁力が少なくとも1100Oe以上、
角型比が0.49以上であり、さらにその針状合金磁
性粉を塗布した時、塗膜表面の面粗さ(Rz;ピ
ーク対ピーク値μm単位)が0.08μmP-P以下、
0.025μmP-P以上であり、さらに使用した針状合金
磁性粉の長軸長(l;単純加算平均値μm単位)
がl=0.070×Rz-05で表わされる曲線上の点、あ
るいはそれより小さく、その下限が0.1μmであ
り、長軸短軸比が5〜15の範囲にあり、かつビデ
オ周波数帯での記録が可能であることを特徴とし
た磁気記録媒体。 2 上記針状合金磁性粉の長軸長の上限は、l=
0.062×Rz-048で表わされる曲線上にある特許請
求の範囲第1項記載の磁気記録媒体。 3 上記磁気記録媒体はビデオ用である特許請求
の範囲第1項、又は第2項記載の磁気記録媒体。 4 上記非磁性基材はテープ状である特許請求の
範囲第3項記載の磁気記録媒体。[Claims] 1. A magnetic recording medium in which acicular alloy magnetic powder mainly composed of iron is coated on a non-magnetic base material, wherein the coercive force of the acicular alloy magnetic powder is at least 1100 Oe or more,
The squareness ratio is 0.49 or more, and when the acicular alloy magnetic powder is applied, the surface roughness (Rz; peak-to-peak value in μm) of the coating film is 0.08μm PP or less,
0.025μm PP or more, and the long axis length of the used acicular alloy magnetic powder (l; simple average value in μm)
is a point on the curve expressed by l = 0.070 x Rz -05 or smaller, the lower limit is 0.1 μm, the major axis minor axis ratio is in the range of 5 to 15, and recording in the video frequency band. A magnetic recording medium characterized by being capable of. 2 The upper limit of the long axis length of the acicular alloy magnetic powder is l=
The magnetic recording medium according to claim 1, which lies on a curve expressed by 0.062×Rz -048 . 3. The magnetic recording medium according to claim 1 or 2, wherein the magnetic recording medium is for video. 4. The magnetic recording medium according to claim 3, wherein the non-magnetic base material is tape-shaped.
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP56028487A JPS57143733A (en) | 1981-03-02 | 1981-03-02 | Magnetic recording medium |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP56028487A JPS57143733A (en) | 1981-03-02 | 1981-03-02 | Magnetic recording medium |
Publications (2)
| Publication Number | Publication Date |
|---|---|
| JPS57143733A JPS57143733A (en) | 1982-09-06 |
| JPH038015B2 true JPH038015B2 (en) | 1991-02-05 |
Family
ID=12250018
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP56028487A Granted JPS57143733A (en) | 1981-03-02 | 1981-03-02 | Magnetic recording medium |
Country Status (1)
| Country | Link |
|---|---|
| JP (1) | JPS57143733A (en) |
Families Citing this family (4)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| JPH0654536B2 (en) * | 1983-02-04 | 1994-07-20 | 富士写真フイルム株式会社 | Magnetic recording medium |
| JPS59203224A (en) * | 1983-05-02 | 1984-11-17 | Fuji Photo Film Co Ltd | Magnetic recording medium |
| JPH0644341B2 (en) * | 1983-09-22 | 1994-06-08 | ティーディーケイ株式会社 | Magnetic recording medium |
| JPH03116416A (en) * | 1990-04-27 | 1991-05-17 | Hitachi Ltd | magnetic disk media |
Family Cites Families (2)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| JPS54159203A (en) * | 1978-06-07 | 1979-12-15 | Fuji Photo Film Co Ltd | Audio magnetic recording tape |
| JPS5677931A (en) * | 1979-11-28 | 1981-06-26 | Tdk Corp | Magnetic recording medium and its producton |
-
1981
- 1981-03-02 JP JP56028487A patent/JPS57143733A/en active Granted
Also Published As
| Publication number | Publication date |
|---|---|
| JPS57143733A (en) | 1982-09-06 |
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