JPH0159724B2 - - Google Patents
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- Publication number
- JPH0159724B2 JPH0159724B2 JP54063997A JP6399779A JPH0159724B2 JP H0159724 B2 JPH0159724 B2 JP H0159724B2 JP 54063997 A JP54063997 A JP 54063997A JP 6399779 A JP6399779 A JP 6399779A JP H0159724 B2 JPH0159724 B2 JP H0159724B2
- Authority
- JP
- Japan
- Prior art keywords
- powder
- gas
- reducing gas
- iron
- reducing
- 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
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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
Landscapes
- Engineering & Computer Science (AREA)
- Metallurgy (AREA)
- Paints Or Removers (AREA)
- Manufacture And Refinement Of Metals (AREA)
- Manufacture Of Metal Powder And Suspensions Thereof (AREA)
- Magnetic Record Carriers (AREA)
- Hard Magnetic Materials (AREA)
Description
本発明は還元金属鉄を主成分とする磁気記録用
粉体の工業的製造方法に関するものである。
従来、磁気記録用粉体としては1次粒子(凝集
のない個々の粒子)の形状が微細な針状粒子であ
るα−Fe2O3、β−FeOOH、蟻酸鉄などの鉄化
合物粉体、さらにはこれらの化合物にコバルト、
ニツケル、硼素等の添加物の有効量を含有させて
得られる粉体が実用に供されている。
このような鉄化合物粉体(例えば市販のγ−
Fe2O3)とそれを水素で還元して得た金属鉄の粉
体(Fe)について、各々の磁気特性を第1図の
ヒステリシスループのHcとσr、σsを挙げて比較
すると、第1表に示すようにγ−Fe2O3のHcと
σr、σsに比べ還元金属鉄のHcとσr、σsの数値が
大であり、磁気記録性能が大巾に向上している。
このような事実から、最近記録密度の一層の向上
と高周波数領域での出力増加を可能とするために
各種の鉄化合物粉体を還元性ガスを用いて還元し
て得られる還元金属鉄を主成分とする針状粒子材
料(以後「還元金属鉄粉体」と略称する。)が実
用化されようとしている。実用上望ましい還元金
属鉄粉体としては、上記Hc、σr、σsの数値が大
きいことの他に、これら磁気特性の分散値(バラ
ツキ)が許容範囲内に入ることが要求され、さら
にロツト間のバラツキも許容範囲内に入ることが
要求される。
ところが、公知の技術を用いて原料の酸化鉄粉
体を還元性ガスで適当な還元条件下において還元
しても、第1表に示すような磁気特性が得られる
のは稀である。換言すれば、実験室内で行う数百
グラム以下の小規模でかつ注意深く還元が行われ
た場合にのみ所定の磁気特性を有する還元金属鉄
粉体が得られるのであつて、未だ1バツチ当りKg
単位以上の工業規模の量産化技術は完成されてい
ない。
本発明者等はその原因について検討し多数の実
験を重ねた結果、所定の磁気特性値を備えた還元
金属鉄粉体を得るには原料の1次粒子の形状を保
持したまゝかつ焼結させずに還元しなければなら
ないことを見出し、本発明を完成したものであ
る。
すなわち、本発明の目的は原料とする鉄化合物
粉体の微細な粒子を水素を還元成分とする還元性
ガスを用いて還元して高性能の磁気記録用粉体で
ある還元金属鉄粉体を工業的規模で量産する技術
を提供することにある。
本発明に用いる原料の鉄化合物粉体とは、α−
Fe2O3、α−FOOH、β−FeOOH、γ−Fe2O3、
γ−FeOOH、蓚酸鉄、蟻酸鉄など、鉄と非金属
元素との化合物の微細な粉体、さらには此等にコ
バルト、ニツケル、錫、銀、銅、チタン、硅素、
アルミニウム砒素、燐、硼素の少くとも一種の有
効量を添加した粉体を意味する。特に酸化鉄、水
酸化鉄の類が好ましい。
本発明に用いる還元性ガスとしては純水素ガス
または水素に不活性成分として窒素、炭酸ガス、
低級炭化水素ガス等を含有している混合ガスが使
用できるが、後者の場合は水素が50容量%以上必
要である。いずれの還元性ガスの場合も、ガス中
の水分(H2O)は常に10000ppm以下、とくに
6000ppm以下が好ましい。
本発明の方法では原料の酸化鉄等の粉体と還元
性ガスとを圧力0.05〜50Kg/cm2(ゲージ)、温度
150〜500℃好ましくは200〜450℃の還元条件下で
接触させて還元する。この際、還元性ガスを空塔
線速度1〜20cm/secで通気しつゝ原料を撹拌し
なければならない。還元性ガスが粉体中に分散保
有され、粉体単独に比べて粘性の大巾に低下した
均質な粉体と還元性ガスとの混合物が反応の全期
間に亘つて形成される。しかし還元性ガスの通気
速度が20cm/secを越えるようにすると粉体中を
通過するガスがはつきりとした気泡状態となり、
しかも気泡同志の合体が起り微細粒子の飛散が顕
著となる。また1cm/sec未満の通気速度にした
場合は、粉体中の還元性ガスの分散保有量が減少
し、粉体と還元性ガスの均質な混合物が形成され
ない。
本発明においてこのような還元条件を必須の構
成とするのは、還元中に原料の焼結または崩壊に
よつて原料粉体の粒子形状が損われることを防止
しつゝ還元反応を完結させるためである。すなわ
ち酸化鉄を例として説明すると、酸化鉄を還元し
て鉄とする反応は2つの段階から成るが、
3Fe2O3+H2→2Fe3O4+H2O (1)
Fe3O4+4H2→3Fe+4H2O (2)
還元が始まると、先ず(1)の反応が起る。(1)は発
熱反応で比較的反応速度が速く、短時間のうちに
進行する。
しかも、この段階で粉体には大きな体積変化
(膨張)が起る。
次いで(2)の反応が起る。(2)は吸熱反応で反応速
度も遅く、還元終了までに長時間を要し、(1)とは
逆に体積を収縮する。(1)の段階では焼結が起り易
いため比較的低い温度条件下あるいは、還元性ガ
ス流速を大きくして、反応熱を除去し易くする条
件下で実施しなければならない。しかし、原料酸
化鉄粉体の粒子が微細なため、還元ガスの流速を
大きくすると粒子が飛散し易い。ほとんどの場
合、原料の1次粒子の大きさは、長さ0.05〜5ミ
クロンで直径0.01〜0.2ミクロンである。実際は
1次粒子が凝集した2次粒子となつているが、概
ね99重量%が40ミクロン以下である。したがつ
て、還元中に粒子の焼結が生じないようにするた
めに、例えば従来法の流動層方式を用いて還元性
ガス流速を0.5cm/sec程度にすると粒径10ミクロ
ン以下の粒子は反応系外へ飛散する。或いは回転
炉のような還元性ガスの流れ方向と粉体の流れ方
向とが交叉するような場合も、ガスの流通によつ
て粉体が飛散し、還元反応の継続はむずかしい。
一方、粒子飛散を抑制するために従来法の固定層
方式で通気する場合は、膨張と収縮という体積変
化にも追従できる機能を反応装置に装備しなけれ
ばならない。このような反応装置は構造が複雑と
なり原料の充填、製品の取出しにも支障を来た
し、本発明の目的とする量産化技術には適しな
い。また(2)の段階でも焼結が生起し易いため特願
昭52−12874号では、水素含有ガス空間速度
(SV)は少くとも
SV=3000/θ−3.7+1200(ただしθは時間)
で与えられるガス量が必要であると記している。
ところが上記SVで実施し得る固定層の層厚みは
せいぜい80mmに過ぎない。これ以上の層厚みで還
元する時は粒子体積の膨張、収縮のために局所的
な粒子移動が発生し、一定のガス通路ができる。
そのため層内温度分布の不均等箇所、H2O分圧
が異常に上昇する箇所が発生し、焼結が起る。
なお焼結の状況は電子顕微鏡写真で形状、寸
法、凝集状況の変化を見れば容易に確認できる。
勿論磁気特性の測定によつてもわかる。本発明の
還元条件では、原料粉体が還元性ガスにより流動
を開始しない範囲内の通気状態においてこれを撹
拌することによつて、水素の供給、反応熱の除去
と供給、生成水の分圧低減などの要因から粒子の
焼結防止に必要とされる還元性ガス供給速度の確
保と粒子の飛散防止という技術的困難性の問題が
工業的規模において解決される。
本発明の方法において、還元性ガスの供給方法
は、原料粉体中へ焼結板、多孔板、金網等で構成
される分散板を通して吹き込む方法である。また
は粉体を撹拌するための撹拌翼の付近に取付けた
多数の孔を有するスパージヤーから吹き込んでも
よい、撹拌翼を取付ける軸、腕木を中空構造にし
てその内部に還元性ガスを貫流させ、これ等に設
けた多数の孔から還元性ガスを噴出させる方法も
採用できる。分散板を介してガスを吹き込まない
後者の場合は分散板である必要はなく無孔の底板
でよい。
本発明の方法に用いる撹拌には、粉体のかきま
ぜに通常用いられる方法が使用される。例えば、
カイ型、リボン型、イカリ型などのかきまぜ腕型
混合形式が好適である。この場合、撹拌翼はでき
るだけ上述の分散板あるいは底板に近く取付ける
方がよい。なお翼形状、翼枚数、回転数などは原
料粉体の性状によつて適切なもを選定できる。
本発明の方法に於いて、還元反応の圧力の下限
0.05Kg/cm2(ゲージ)は、還元性ガスが半流動層
反応器、サイクロンとかバツグフイルターとかの
粉塵捕集器、熱交換器、それらをつなぐ導管等の
一連の装置を通過した後、大気に放出される最低
必要圧力である。使用した還元性ガスの大部分を
処理して循環再使用する場合は、循環ブロワー出
口から反応器、熱交換器、集塵器、脱湿装置等の
一連の装置を通過して循環ブロワー入口までの一
巡に要する圧力損失を補うのに最少限必要な圧力
である。反応圧力が高いほど粉体粒子表面から内
部へ拡散する水素分子の移動速度を速め還元反応
を進める望ましい効果を与えるが、反面、粉体粒
子内部で酸素原子と反応して生成した水(H2O)
分子の粒子内部から表面を通つて気体本体中への
移動速度を遅らせるという望ましくない効果をも
たらす。50Kg/cm2(ゲージ)を越える圧力では水
分子の粒子内部から移動速度の低下が顕著にな
る。したがつて実用的な還元圧力は0.05〜50Kg/
cm2(ゲージ)とすることが必要で、とくに2〜25
Kg/cm2(ゲージ)が好ましい範囲である。
本発明の方法に用いる反応温度についても、温
度が低い程還元反応がゆつくりと進み逆に温度が
高い程還元反応が急速に進む。しかし急激に反応
を進めると容易に粒子の焼結が起り、磁性特性が
悪化する。したがつて、反応温度の実用範囲は
150〜500℃とすることが必要であつて、とくに
200〜380℃が好ましい範囲である。
本発明の方法を用いれば、従来は実験室的規模
でのみ可能であつた鉄化合物微粉からの還元金属
鉄粉体の製造が工業的規模において可能となり、
しかも得られる還元金属鉄の磁気特性が優れてお
り、かつその品質上のバラツキが少い。従つて本
発明の方法は磁気記録用粉体の製造法として工業
的価値の高いものである。
本発明を実施例によつて、さらに具体的に説明
する。
実施例 1
内径250mm、撹拌機の翼径190mm、焼結金属板を
ガス分散板とする反応器に、1次粒子の最大寸法
が平均0.5ミクロンである市販の針状晶のγ−
Fe2O33Kgを仕込んだ。これに温度350℃、圧力2
Kg/cm2(ゲージ)の条件下で、還元性ガスとして
純度99容量%の水素ガスを通気し、撹拌しながら
7.5時間還元した。
環元終了後の磁気特性値を第2表の実験番号1
に示す。
比較例 1
実施例1と同じ反応器で撹拌翼のついていない
ものに、実施例1と同じ原料酸化鉄粉体を同一量
仕込み、かつ同じ条件で同一時間還元したところ
磁気特性値として第2表の実験番号2に示す値を
得た。実施例1に比べ特性値が低下しただけでな
く、反応器内の場所によつてかなりのバラツキが
見られた。
比較例 2
直径250mm、ガス分散板として焼結金属板を用
いた固定層式反応器(無撹拌)に実施例1と同じ
原料酸化鉄粉体を5.2Kg(層厚み150mm)を充填
し、還元性ガス流速5cm/secで実施例1と同じ
還元条件で還元した。
この流速ではガスの流れ方向に水(H2O)分
圧が上昇し、10000ppm以上となる箇所が発生し
た模様で層厚み方向上、中、下(層厚みの方向で
3等分)の位置によつて、得られた磁気特性値が
異なり、水分圧の最も小さい下層が最も磁気特性
がよい。結果を第2表の実験番号3の上、中、下
に示す。
実施例 2
実施例1に用いた装置に3種類の原料酸化鉄粉
体(ロツト番号A、B、C)をそれぞれ仕込んだ
実験を行つた。還元条件は全く、実施例1と同じ
である。実験結果を第3表の実験番号1〜9に示
す。明らかに撹拌翼をもつ反応器を用いた場合が
最も良い磁気特性を示す。
比較例 3
比較例1、2に用いた各装置に上述のA、B、
Cの各原料を仕込み実施例1と同一条件で還元を
行つた。結果を第3表に示す。実験番号3に用い
た装置の場合はいずれも最上層部サンプルの測定
値である。
実施例 3
直径1000mm、全高4000mm、ガス分散板として多
孔板と金網を重ねた構造をもち、翼径800mmの撹
拌翼を備えた反応器に、実施例2で用いた原料酸
化鉄粉体Aを30Kg仕込み、還元性ガス流速10cm/
sec、温度280℃、圧力11Kg/cm2(ゲージ)で、
CH4を2容量%、CO2を0.1容量%含む水素を用
いて10時間還元した。
第4表の実験番号1は還元しない状態での磁気
特性を、同2、3、4は異なるバツチにおける還
元後の磁気特性を示す。
再現性のあるデータが得られた。
The present invention relates to an industrial method for producing magnetic recording powder containing reduced metallic iron as a main component. Conventionally, magnetic recording powders include iron compound powders such as α-Fe 2 O 3 , β-FeOOH, and iron formate, whose primary particles (individual particles without agglomeration) are fine needle-like particles; Furthermore, these compounds contain cobalt,
Powders containing effective amounts of additives such as nickel and boron are in practical use. Such iron compound powder (for example, commercially available γ-
Comparing the magnetic properties of Fe 2 O 3 ) and metallic iron powder (Fe) obtained by reducing it with hydrogen, listing Hc, σr, and σs of the hysteresis loop in Figure 1, As shown in the table, the values of Hc, σr, and σs of reduced metal iron are larger than those of γ-Fe 2 O 3 , and the magnetic recording performance is greatly improved.
Based on these facts, in order to further improve recording density and increase output in the high frequency range, recently reduced metallic iron obtained by reducing various iron compound powders using reducing gas has been mainly used. The acicular particle material (hereinafter abbreviated as "reduced metal iron powder") used as a component is about to be put into practical use. Practically desirable reduced metallic iron powder is required not only to have large values for Hc, σr, and σs, but also to have a dispersion value (variation) of these magnetic properties within an allowable range, and also to have a variation between lots. It is also required that the variations fall within an acceptable range. However, even if the raw material iron oxide powder is reduced with a reducing gas under appropriate reducing conditions using known techniques, it is rare to obtain the magnetic properties shown in Table 1. In other words, reduced metallic iron powder with the desired magnetic properties can be obtained only when reduction is carried out carefully on a small scale of several hundred grams or less in the laboratory, and it is still possible to obtain reduced metallic iron powder with the desired magnetic properties.
The technology for mass production on an industrial scale beyond units has not been perfected. The inventors investigated the cause of this problem and conducted numerous experiments. As a result, the inventors found that in order to obtain reduced metal iron powder with predetermined magnetic property values, it is necessary to maintain the shape of the primary particles of the raw material and sinter the powder. The present invention was completed by discovering that the reduction should be carried out without causing any oxidation. That is, the purpose of the present invention is to reduce fine particles of iron compound powder as a raw material using a reducing gas containing hydrogen as a reducing component to obtain reduced metal iron powder, which is a high-performance magnetic recording powder. The goal is to provide technology for mass production on an industrial scale. The raw material iron compound powder used in the present invention is α-
Fe 2 O 3 , α-FOOH, β-FeOOH, γ-Fe 2 O 3 ,
Fine powder of compounds of iron and nonmetallic elements such as γ-FeOOH, iron oxalate, iron formate, etc., as well as cobalt, nickel, tin, silver, copper, titanium, silicon, etc.
It means a powder to which an effective amount of at least one of aluminum arsenic, phosphorus, and boron is added. Particularly preferred are iron oxides and iron hydroxides. The reducing gas used in the present invention is pure hydrogen gas or hydrogen with nitrogen, carbon dioxide gas, etc. as an inert component.
A mixed gas containing lower hydrocarbon gas etc. can be used, but in the latter case, hydrogen needs to be at least 50% by volume. In the case of any reducing gas, the water content (H 2 O) in the gas is always below 10,000 ppm, especially
It is preferably 6000ppm or less. In the method of the present invention, raw material powder such as iron oxide and reducing gas are heated at a pressure of 0.05 to 50 kg/cm 2 (gauge) and a temperature of
Reduction is carried out by contacting under reducing conditions at 150 to 500°C, preferably 200 to 450°C. At this time, the raw material must be stirred while a reducing gas is aerated at a superficial linear velocity of 1 to 20 cm/sec. The reducing gas is held dispersed in the powder, and a homogeneous mixture of the powder and the reducing gas is formed throughout the reaction period, the viscosity of which is significantly lower than that of the powder alone. However, if the aeration speed of the reducing gas exceeds 20 cm/sec, the gas passing through the powder will form a state of bubbles.
Moreover, coalescence of bubbles occurs and the scattering of fine particles becomes noticeable. Furthermore, when the ventilation rate is less than 1 cm/sec, the amount of the reducing gas dispersed in the powder decreases, and a homogeneous mixture of the powder and the reducing gas is not formed. The reason why such reduction conditions are essential in the present invention is to complete the reduction reaction while preventing the particle shape of the raw material powder from being damaged due to sintering or disintegration of the raw material during reduction. It is. In other words, using iron oxide as an example, the reaction of reducing iron oxide to iron consists of two steps: 3Fe 2 O 3 +H 2 →2Fe 3 O 4 +H 2 O (1) Fe 3 O 4 +4H 2 →3Fe+4H 2 O (2) When reduction begins, reaction (1) occurs first. (1) is an exothermic reaction that has a relatively fast reaction rate and proceeds in a short period of time. Moreover, a large volume change (expansion) occurs in the powder at this stage. Next, reaction (2) occurs. (2) is an endothermic reaction, the reaction rate is slow, it takes a long time to complete the reduction, and the volume contracts, contrary to (1). Since sintering is likely to occur in step (1), it must be carried out under relatively low temperature conditions or under conditions where the reducing gas flow rate is increased to facilitate the removal of reaction heat. However, since the particles of the raw material iron oxide powder are fine, the particles tend to scatter when the flow rate of the reducing gas is increased. In most cases, the primary particle size of the raw material is 0.05 to 5 microns in length and 0.01 to 0.2 microns in diameter. In reality, secondary particles are aggregated primary particles, but approximately 99% by weight are 40 microns or less. Therefore, in order to prevent particle sintering during reduction, for example, if a conventional fluidized bed method is used and the reducing gas flow rate is set to about 0.5 cm/sec, particles with a particle size of 10 microns or less will be reduced. Scattered outside the reaction system. Alternatively, in a rotary furnace where the flow direction of the reducing gas and the flow direction of the powder intersect, the powder is scattered due to the gas flow, making it difficult to continue the reduction reaction.
On the other hand, when aerating using the conventional fixed bed method to suppress particle scattering, the reactor must be equipped with a function that can follow volumetric changes such as expansion and contraction. Such a reactor has a complicated structure, which causes problems in filling raw materials and taking out products, and is not suitable for mass production technology, which is the object of the present invention. Furthermore, since sintering is likely to occur even in step (2), in Japanese Patent Application No. 12874/1987, the hydrogen-containing gas space velocity (SV) is given as at least SV=3000/θ−3.7+1200 (where θ is time). It states that the amount of gas required is
However, the layer thickness of the fixed layer that can be implemented with the above SV is only 80 mm at most. When reducing with a layer thickness greater than this, local particle movement occurs due to expansion and contraction of the particle volume, creating a constant gas passage.
As a result, there are places where the temperature distribution within the layer is uneven and places where the H 2 O partial pressure increases abnormally, causing sintering. The state of sintering can be easily confirmed by looking at changes in shape, size, and agglomeration status in electron micrographs.
Of course, this can also be determined by measuring magnetic properties. In the reducing conditions of the present invention, by stirring the raw material powder in an aerated state within a range in which it does not start flowing due to reducing gas, hydrogen is supplied, reaction heat is removed and supplied, and the partial pressure of the produced water is The technically difficult problem of securing the reducing gas supply rate required to prevent particle sintering and preventing particle scattering due to factors such as reduction can be solved on an industrial scale. In the method of the present invention, the reducing gas is supplied by blowing it into the raw material powder through a dispersion plate composed of a sintered plate, a perforated plate, a wire mesh, or the like. Alternatively, the air may be blown from a sparger with a large number of holes installed near the stirring blades for stirring the powder, or by making the shaft and arm to which the stirring blades are attached hollow and allowing the reducing gas to flow through them. It is also possible to adopt a method in which the reducing gas is ejected from a large number of holes provided in the pores. In the latter case, where gas is not blown through a distribution plate, a non-porous bottom plate may be used instead of a distribution plate. For stirring used in the method of the present invention, a method commonly used for stirring powder is used. for example,
Mixed stirring arm types such as chi type, ribbon type, and squid type are suitable. In this case, it is better to install the stirring blade as close to the above-mentioned dispersion plate or bottom plate as possible. Note that the blade shape, number of blades, rotation speed, etc. can be appropriately selected depending on the properties of the raw material powder. In the method of the present invention, the lower limit of the pressure of the reduction reaction
0.05Kg/cm 2 (gauge) means that the reducing gas is released into the atmosphere after passing through a series of devices such as a semi-fluidized bed reactor, dust collectors such as cyclones and bag filters, a heat exchanger, and conduits that connect them. This is the minimum pressure required to be released. When most of the used reducing gas is processed and recycled for reuse, it passes through a series of devices such as a reactor, heat exchanger, dust collector, dehumidifier, etc. from the circulation blower outlet to the circulation blower inlet. This is the minimum pressure required to compensate for the pressure loss required for one cycle. The higher the reaction pressure, the faster the movement speed of hydrogen molecules diffusing from the surface of the powder particle to the inside, giving the desired effect of promoting the reduction reaction. However, on the other hand, water (H 2 O)
This has the undesirable effect of slowing the rate of movement of molecules from inside the particle through the surface and into the body of gas. At pressures exceeding 50Kg/cm 2 (gauge), the speed of movement of water molecules from inside the particles becomes noticeably lower. Therefore, the practical reduction pressure is 0.05~50Kg/
cm 2 (gauge), especially 2 to 25
Kg/cm 2 (gauge) is a preferred range. Regarding the reaction temperature used in the method of the present invention, the lower the temperature, the slower the reduction reaction progresses, and conversely, the higher the temperature, the faster the reduction reaction progresses. However, if the reaction proceeds rapidly, sintering of the particles easily occurs and the magnetic properties deteriorate. Therefore, the practical range of reaction temperature is
It is necessary to keep the temperature between 150 and 500℃, especially
The preferred range is 200-380°C. By using the method of the present invention, it becomes possible to produce reduced metallic iron powder from iron compound fine powder on an industrial scale, which was previously possible only on a laboratory scale.
Moreover, the magnetic properties of the obtained reduced metal iron are excellent, and there is little variation in quality. Therefore, the method of the present invention has high industrial value as a method for producing magnetic recording powder. The present invention will be explained in more detail with reference to Examples. Example 1 In a reactor with an inner diameter of 250 mm, a stirrer blade diameter of 190 mm, and a sintered metal plate as a gas dispersion plate, commercially available acicular γ-
3Kg of Fe 2 O 3 was charged. This has a temperature of 350℃ and a pressure of 2
Under conditions of Kg/cm 2 (gauge), hydrogen gas with a purity of 99% by volume was introduced as a reducing gas, and the mixture was stirred.
It was reduced for 7.5 hours. The magnetic property values after completion of the ring element are shown in Experiment No. 1 in Table 2.
Shown below. Comparative Example 1 The same amount of the same raw material iron oxide powder as in Example 1 was charged into the same reactor as in Example 1 but without a stirring blade, and reduction was performed under the same conditions for the same time. Table 2 shows the magnetic properties. The values shown in Experiment No. 2 were obtained. Not only were the characteristic values lower than in Example 1, but considerable variation was observed depending on the location within the reactor. Comparative Example 2 A fixed bed reactor (no stirring) with a diameter of 250 mm and using a sintered metal plate as a gas dispersion plate was filled with 5.2 kg (layer thickness 150 mm) of the same raw material iron oxide powder as in Example 1, and reduced. Reduction was carried out under the same reducing conditions as in Example 1 at a gas flow rate of 5 cm/sec. At this flow rate, the partial pressure of water (H 2 O) increased in the gas flow direction, and there appeared to be places where it reached 10,000 ppm or more, and the water (H 2 O) partial pressure increased in the direction of the gas flow. The obtained magnetic property values vary depending on the material, and the lower layer with the lowest water pressure has the best magnetic properties. The results are shown above, middle, and below of Experiment No. 3 in Table 2. Example 2 An experiment was conducted in which three types of raw material iron oxide powder (lot numbers A, B, and C) were charged into the apparatus used in Example 1. The reduction conditions are exactly the same as in Example 1. The experimental results are shown in experiment numbers 1 to 9 in Table 3. Clearly, the best magnetic properties are obtained when a reactor with stirring blades is used. Comparative Example 3 The above-mentioned A, B,
Each raw material of C was charged and reduced under the same conditions as in Example 1. The results are shown in Table 3. In the case of the apparatus used in Experiment No. 3, the measured values are for the top layer sample. Example 3 The raw material iron oxide powder A used in Example 2 was placed in a reactor having a diameter of 1,000 mm, a total height of 4,000 mm, a structure in which a perforated plate and a wire mesh were stacked as a gas distribution plate, and a stirring blade with a blade diameter of 800 mm. 30Kg charged, reducing gas flow rate 10cm/
sec, temperature 280℃, pressure 11Kg/cm 2 (gauge),
Reduction was performed for 10 hours using hydrogen containing 2% by volume of CH 4 and 0.1% by volume of CO 2 . Experiment No. 1 in Table 4 shows the magnetic properties without reduction, and Experiment No. 2, 3, and 4 show the magnetic properties after reduction in different batches. Reproducible data were obtained.
【表】【table】
【表】【table】
【表】【table】
【表】
比較例 4
実施例3と同一の反応器に、実施例2で用いた
原料酸化鉄粉体Aを30Kg仕込み、還元性ガスとし
て純度99%の水素ガスを流速0.5cm/secで、温度
280℃、圧力11Kg/cm2(ゲージ)の条件下で20時間
還元した。
本比較例の場合、水素ガス流速が規定値より小
さく、粉体中の還元性ガスの分散保有量が著しく
減少することに対応して、製品品質上好ましくな
い還元ムラが大きく生じて仕舞い、第5表に示す
ように、層厚み方向の上、中、下(層厚み方向で
3等分)の位置によつて得られた製品の磁気特性
が大きく異なつてしまうことがわかつた。[Table] Comparative Example 4 Into the same reactor as in Example 3, 30 kg of the raw material iron oxide powder A used in Example 2 was charged, and hydrogen gas with a purity of 99% was used as the reducing gas at a flow rate of 0.5 cm/sec. temperature
Reduction was carried out for 20 hours at 280° C. and a pressure of 11 Kg/cm 2 (gauge). In the case of this comparative example, the hydrogen gas flow rate was lower than the specified value, and the amount of dispersed reducing gas in the powder was significantly reduced, resulting in significant reduction unevenness that was unfavorable in terms of product quality. As shown in Table 5, it was found that the magnetic properties of the obtained products differed greatly depending on the top, middle, and bottom (equally divided into three in the layer thickness direction) positions in the layer thickness direction.
【表】
比較例 5
実施例3と同一の反応器に、実施例2で用いた
原料酸化鉄粉体Aを30Kg仕込み、還元性ガスとし
て純度99%の水素ガスを、流速10cm/secで、温
度280℃、圧力0.03Kg/cm2(ゲージ)の条件下で還
元反応を実施しようとしたが、反応器、サイクロ
ン粉塵補集器、熱交換器およびこれらの導管等に
由来する圧損が0.045Kg/cm2(ゲージ)であつた
為、満足にガスを流通せしめることが出来ず、実
際上、還元反応を実施することが出来なかつた。[Table] Comparative Example 5 30 kg of raw material iron oxide powder A used in Example 2 was charged into the same reactor as in Example 3, and hydrogen gas with a purity of 99% was used as the reducing gas at a flow rate of 10 cm/sec. I tried to carry out the reduction reaction under the conditions of temperature 280℃ and pressure 0.03Kg/cm 2 (gauge), but the pressure drop due to the reactor, cyclone dust collector, heat exchanger, these conduits, etc. was 0.045Kg. /cm 2 (gauge), gas could not be circulated satisfactorily, and the reduction reaction could not actually be carried out.
第1図は磁性粉体のもつ磁気特性を示すヒステ
リシスループであり、σrは残留磁化率、σsは飽和
磁化率、Hcは保磁力を表す。
第2図は本発明の実施態様として、分散板を使
用した場合の反応器の主要部を示した図である。
第3図は本発明の実施態様として中空構造の撹拌
軸、撹拌翼を使用した場合の反応器の主要部を示
した図、第4図は本発明の実施態様としてガス・
スパージヤーを使用した場合の反応器の主要部を
示した図である。
1……反応器本体、2……撹拌翼、3,3′…
…還元性ガス導管、4……ガス分散板、5……還
元性ガス噴出孔、6……ガス・スパージヤー、7
……底板、8……撹拌軸。
Figure 1 shows a hysteresis loop showing the magnetic properties of magnetic powder, where σr represents residual magnetic susceptibility, σs represents saturation magnetic susceptibility, and Hc represents coercive force. FIG. 2 is a diagram showing the main parts of a reactor in which a dispersion plate is used as an embodiment of the present invention.
Figure 3 is a diagram showing the main parts of a reactor when a hollow stirring shaft and stirring blades are used as an embodiment of the present invention, and Figure 4 is a diagram showing the main parts of a reactor when a hollow stirring shaft and stirring blade are used as an embodiment of the present invention.
It is a diagram showing the main parts of a reactor when a sparger is used. 1... Reactor main body, 2... Stirring blade, 3, 3'...
...Reducing gas conduit, 4...Gas distribution plate, 5...Reducing gas outlet, 6...Gas spargeer, 7
...Bottom plate, 8...Stirring shaft.
Claims (1)
て金属鉄を主成分とする磁気記録用粉体を製造す
る方法において、ゲージ圧0.05〜50Kg/cm2の加圧
反応圧力及び加熱下に、該鉄化合物粉体を撹拌翼
により撹拌しつつ、該還元性ガスを、ガスのみで
は粉体が流動を開始しない1〜20cm/secの空塔
線速度において、該粉体の下部から通気し、該粉
体と該通気還元性ガスとの均質な混合物を形成せ
しめつつ還元することを特徴とする粉体の焼結お
よび飛散の両者が実質的に防止された磁気記録用
粉体の製造方法。 2 還元反応圧力がゲージ圧2〜25Kg/cm2である
特許請求の範囲第1項記載の磁気記録用粉体の製
造方法。 3 還元反応温度が150〜500℃である特許請求の
範囲第1項又は第2項記載の磁気記録用粉体の製
造方法。[Scope of Claims] 1. In a method for producing magnetic recording powder containing metallic iron as a main component by reducing iron compound powder using a reducing gas, applying a gauge pressure of 0.05 to 50 kg/cm 2 While stirring the iron compound powder with a stirring blade under pressure reaction pressure and heating, the reducing gas is added at a superficial linear velocity of 1 to 20 cm/sec, at which the powder does not start flowing with gas alone. A magnetism that substantially prevents both sintering and scattering of the powder, characterized in that the powder is vented from the lower part of the powder, and the powder is reduced while forming a homogeneous mixture of the powder and the aerated reducing gas. Method for producing recording powder. 2. The method for producing magnetic recording powder according to claim 1, wherein the reduction reaction pressure is a gauge pressure of 2 to 25 Kg/cm 2 . 3. The method for producing magnetic recording powder according to claim 1 or 2, wherein the reduction reaction temperature is 150 to 500°C.
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP6399779A JPS55157214A (en) | 1979-05-25 | 1979-05-25 | Manufacture of magnetic recording powder |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP6399779A JPS55157214A (en) | 1979-05-25 | 1979-05-25 | Manufacture of magnetic recording powder |
Publications (2)
| Publication Number | Publication Date |
|---|---|
| JPS55157214A JPS55157214A (en) | 1980-12-06 |
| JPH0159724B2 true JPH0159724B2 (en) | 1989-12-19 |
Family
ID=13245406
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP6399779A Granted JPS55157214A (en) | 1979-05-25 | 1979-05-25 | Manufacture of magnetic recording powder |
Country Status (1)
| Country | Link |
|---|---|
| JP (1) | JPS55157214A (en) |
Families Citing this family (2)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| DE3021111A1 (en) * | 1980-06-04 | 1981-12-17 | Basf Ag, 6700 Ludwigshafen | METHOD FOR THE PRODUCTION OF NEEDLE-SHAPED, FERROMAGNETIC METAL PARTICLES, ESSENTIALLY made of IRON |
| DE69315935T2 (en) * | 1992-09-10 | 1998-08-27 | Kao Corp | Method and device for producing magnetic metallic particles |
Family Cites Families (2)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| JPS4854497A (en) * | 1971-11-10 | 1973-07-31 | ||
| JPS53103197A (en) * | 1977-02-18 | 1978-09-08 | Hitachi Maxell | Method of manufacturing magnetic material for magnetic recording medium |
-
1979
- 1979-05-25 JP JP6399779A patent/JPS55157214A/en active Granted
Also Published As
| Publication number | Publication date |
|---|---|
| JPS55157214A (en) | 1980-12-06 |
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