JPS605044B2 - Ferrite manufacturing method - Google Patents
Ferrite manufacturing methodInfo
- Publication number
- JPS605044B2 JPS605044B2 JP50015308A JP1530875A JPS605044B2 JP S605044 B2 JPS605044 B2 JP S605044B2 JP 50015308 A JP50015308 A JP 50015308A JP 1530875 A JP1530875 A JP 1530875A JP S605044 B2 JPS605044 B2 JP S605044B2
- Authority
- JP
- Japan
- Prior art keywords
- ferrite
- particle size
- oxide
- raw materials
- 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.)
- Expired
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- Compounds Of Iron (AREA)
- Hard Magnetic Materials (AREA)
- Soft Magnetic Materials (AREA)
Description
【発明の詳細な説明】
本発明は、化学的活性の高い酸化鉄(Q−Fe203)
を素原料として用いることによって、気孔が極めて少な
く、高い透磁率、磁束密度および電気抵抗を有するNi
−Znフェライトの製造方法に係るものである。Detailed Description of the Invention The present invention provides iron oxide (Q-Fe203) with high chemical activity.
By using Ni as a raw material, it has extremely few pores and has high magnetic permeability, magnetic flux density, and electrical resistance.
- This relates to a method for manufacturing Zn ferrite.
一般にフェライトは酸化鉄を主成分として、酸化ニッケ
ル、酸化マンガン、酸化亜鉛およびその他の酸化物の一
つまたは二つ以上のものを混合し、焼成して得られる酸
化物強磁性材料で多結晶質の酸化物競結体として一般に
市場に供せられているものである。In general, ferrite is a polycrystalline oxide ferromagnetic material that is obtained by mixing iron oxide as a main component with one or more of nickel oxide, manganese oxide, zinc oxide, and other oxides and firing the mixture. It is generally available on the market as an oxide competitive complex of
この製造方法を通常乾式法と称する。しかしながら、酸
化物暁縞体の性質として競絹体内の1つの結晶粒子内お
よび結晶の粒界に数多〈の気孔が存在し、これがフェラ
イトの透磁率、磁束密度等の低下の著しい原因となる。
また乾式法では、素原料の混合が十分均一でない場合、
また素原料の粒度が大きい場合においても、暁結体のイ
オン分布が不均一となり、これも磁気特性を劣化させる
原因となる。空孔を除去する方法としては、フェライト
の粉末を適当な温度に加熱し、この状態で外部から加圧
するホットプレス法、または粉体を2〜1山on/の程
度の圧力で静水圧プレスする方法などがある。しかしこ
れらの方法はいずれも量産性‘こ欠ける欠点があり工業
的にも得策ではない。透常の乾式法によって空孔が少な
くイオン分布の均一な暁結体を得るには、仮競、造粒、
成形および焼成の各過程をいずれも最適条件に設定しな
ければならないことは勿論であるが、この他にも原料中
の不純物および原料の粒径によっても透磁率、残存空孔
率が著しく影響されることが報告されている。一般にフ
ェライトを暁結する過程では、フェライト粉末間におけ
る齢絹現象と、フェライト結晶粒中のある特定のもの夕
が他のフェライト結晶粒を春合しながら成長する過程と
が同時に起る。この暁結過程において、激しい粒境界の
移動を伴なう場合、結晶粒内に気孔がトラツプされ、大
きい粒子間での凝結では、結晶粒界に気孔が残存すると
いわれている。フェラ0ィト競給体を得る過程において
、鱗精密度を上げイオン分布を良くする方法として次の
ことが挙げられる。すなわち、仮焼終了時において仮晩
粉中にフェライト以外の異相を多く含有させ、仮焼粉粒
子間の各イオンの濃度勾配を大きくさせて・競タ給時に
、粒成長に伴なう粒界の移動と共に化学変化をおこさせ
る方法。この方法は、オルソフェラィト等の中間相の発
生を伴なうカーネット型フェライトの焼絹に用いて効果
がある。また、仮焼終了時に粒成長を起さない程度に、
できるだけイオン分布の均一なフェライト相を形成させ
たのち、この微粉末を焼結時に粒成長させる。Ni一Z
nフェライトでは特に中間相の形成を伴なわないため、
この方法によって繊密化を計る必要がある。これらの場
合、いずれも仮暁粉は微粒子であることが望ましいが、
特に物理的活性にのみ依存する仮焼粉から糠結をおこな
う。後者の場合においては仮焼粉は微粒子でなければ、
繊密化はきわめて困難となる。微粒子の仮焼粉を得るに
は、仮焼温度を低くすればよい。しかし低温でフェライ
ト化を促進させるには、表面活性の高い素原料微粒子を
用いる必要がある。Ni−Znフェライトの場合、素原
料のNio,Zno,Q−Fe203の酸素イオンの積
層状態は、Ni0はABCABC・・・・・・のfcc
類似の積層構造であり、Zn0はABAB・・・・・・
のhcp類似の構造である。これに対してQ−Fe20
3は菱面体構造で酸素イオンの配置も、fecもしくは
hCpとは異なる。素原料からフェライト化が進行する
場合、拡散の殆んどはイオン半径の小さい金属イオンに
よって進行すると考えるのは妥当であり、トポ化学的に
見て、酸素イオンの積層状態の類似した素原料間では、
金属イオンの拡散は容易である。したがって、フェライ
ト化が進行する場合の律遠段階は、Feイオンの拡散速
度で決まることになる。前記のことは、粒径の大きい素
原料を用いた場合、高温でなければフェライト化が進行
し難いこと、また生成したフェライトのイオン分布も不
均一であることと一致し、Q−Fe203の粒径がフェ
ライト生成にきわめて大きな影響を与えることがわかる
。Q−Fe203は、ブリテン・オブ・ザ。インステイ
テユート・フオ−・ケミカル・リサーチ・キヨート・ユ
ニバーシテイー(B側etinofthe Insti
tute for Chemical Researc
h KyotoUniversity)第4既登第4〜
5号406〜415頁発行年1965軒こ報告されてい
るように、通常の粒子(粒径5仏程度)では磁気モーメ
ントがC面からC軸方向へと額くことによって、弱強磁
性の現われるスピンフリッピング温度(以下Tsと記す
)は−15℃程度である。しかしながら結晶粒径が4・
となるにつれて、Tsは漸次低温側へと移行し、粒径約
lrでTsご−35℃となる。さらに0.1〆でrsご
−100qoと急激に低下し、250Aでは。−Tの変
化は。こ0.粋mu/夕で、ほぼ温度に依存しなくなる
。この理由として、粒子表面近くの腸イオンは、内部の
それとは結晶場および磁気的双極子場がことなること、
微粒子では格子欠陥や格子不整の影響が大きくきいてく
ることが挙げられる。これらの事実を、化学反応性とい
う観点から見れば、Tsが低温側へ移行することはとり
もなおさ’ず化学的活性が高いことを表わしていること
になる。発明者等は、前記事実に着目し、モル百分率に
て酸化ニッケル15〜25%、酸化亜鉛15〜35%、
酸化第二鉄45〜60%からなる函鉄酸塩母体の酸化第
「二鉄原料、すなわちQ一Fe203の粒度を種々変化
して、Ni−Znフェライトを作成し競結した結果、特
性において優れた結果を得た。This manufacturing method is usually called a dry method. However, as a property of the oxide stripe, there are numerous pores within each crystal grain and at the grain boundaries of the crystal, which causes a significant decrease in the magnetic permeability, magnetic flux density, etc. of ferrite. .
In addition, in the dry method, if the raw materials are not mixed uniformly,
Furthermore, even when the particle size of the raw material is large, the ion distribution of the crystals becomes non-uniform, which also causes deterioration of the magnetic properties. Pores can be removed by hot pressing, which heats ferrite powder to an appropriate temperature and presses it from the outside in this state, or by isostatic pressing the powder at a pressure of about 2 to 1 on/on. There are methods. However, all of these methods have the disadvantage of lacking mass production, and are not industrially advisable. In order to obtain Akatsuki crystals with few pores and uniform ion distribution using a transparent dry method, preparatory, granulation,
Of course, each process of forming and firing must be set to optimal conditions, but magnetic permeability and residual porosity are also significantly affected by impurities in the raw materials and the particle size of the raw materials. It has been reported that In general, in the process of crystallizing ferrite, the aging phenomenon between ferrite powders and the process in which certain ferrite crystal grains grow while spring coalescing with other ferrite crystal grains occur simultaneously. It is said that in this coagulation process, when accompanied by severe movement of grain boundaries, pores are trapped within the crystal grains, and when condensation occurs between large grains, pores remain at the grain boundaries. In the process of obtaining a ferrite competitive body, the following methods can be mentioned to increase scale precision and improve ion distribution. In other words, at the end of calcination, the calcination powder contains a large amount of different phases other than ferrite to increase the concentration gradient of each ion between the calcination powder particles. A method that causes a chemical change as the substance moves. This method is effective when used for burning Carnet-type ferrite, which involves the generation of intermediate phases such as orthoferrite. In addition, to the extent that grain growth does not occur at the end of calcination,
After forming a ferrite phase with as uniform an ion distribution as possible, this fine powder is subjected to grain growth during sintering. Ni-Z
Since n-ferrite does not involve the formation of an intermediate phase,
It is necessary to achieve densification using this method. In all of these cases, it is desirable that the false powder be fine particles;
In particular, brazing is performed from calcined powder that depends only on physical activity. In the latter case, unless the calcined powder is fine particles,
Refinement becomes extremely difficult. In order to obtain calcined powder of fine particles, the calcining temperature may be lowered. However, in order to promote ferrite formation at low temperatures, it is necessary to use raw material fine particles with high surface activity. In the case of Ni-Zn ferrite, the stacking state of oxygen ions of the raw materials Nio, Zno, and Q-Fe203 is as follows: Ni0 is ABCABC... fcc
It has a similar laminated structure, and Zn0 is ABAB...
It has a structure similar to hcp. On the other hand, Q-Fe20
3 has a rhombohedral structure and the arrangement of oxygen ions is also different from fec or hCp. When ferrite formation progresses from a raw material, it is reasonable to assume that most of the diffusion occurs by metal ions with a small ionic radius. So,
Diffusion of metal ions is easy. Therefore, the critical stage in which ferrite formation progresses is determined by the diffusion rate of Fe ions. The above is consistent with the fact that when a raw material with a large particle size is used, ferrite formation is difficult to proceed unless the temperature is high, and the ion distribution of the generated ferrite is also uneven. It can be seen that the diameter has a very large effect on ferrite formation. Q-Fe203 is Britain of the. Institute for Chemical Research Kiyoto University (B side etinofthe Insti
tute for Chemical Research
h Kyoto University) No. 4 Already Registered No. 4~
No. 5, pp. 406-415, published in 1965. As reported in this paper, in normal particles (particle size of about 5 Buddhas), weak ferromagnetism appears due to the magnetic moment moving from the C-plane toward the C-axis. The spin flipping temperature (hereinafter referred to as Ts) is about -15°C. However, the grain size is 4.
As the temperature increases, Ts gradually shifts to the lower temperature side, and at a particle size of about lr, Ts becomes -35°C. Furthermore, at 0.1〆, it suddenly decreased to -100qo per rs, and at 250A. -What is the change in T? This 0. At Ikimu/Yu, it becomes almost independent of temperature. The reason for this is that the intestinal ions near the particle surface have a different crystal field and magnetic dipole field than those inside the particle;
For fine particles, the effects of lattice defects and lattice misalignment are significant. If these facts are viewed from the viewpoint of chemical reactivity, the shift of Ts to the low temperature side clearly indicates that the chemical activity is high. The inventors paid attention to the above fact, and the mole percentage of nickel oxide was 15 to 25%, zinc oxide was 15 to 35%,
Ni-Zn ferrite was produced and bonded by variously changing the grain size of the ferric oxide raw material, that is, Q-Fe203, in a matrix of ferric oxide consisting of 45 to 60% ferric oxide, and as a result, it was found to have excellent properties. We obtained the following results.
ここで、ニッケル−亜鉛フェライトの配合比をモル%で
酸化ニッケル15〜25%、酸化亜鉛15〜35%およ
び酸化l第二鉄を45〜60%に限定した理由は、高透
磁率が得られる組成領域は、上記配合比の範囲内の場合
にのみ有効であり、かつその組成範囲でQ−Fe2Q原
料の粒度によって支配されるためである。したがって、
酸化亜鉛、酸化ニッケル、酸化・第二鉄は上記配合比以
下もしくはそれ以上ではたとえQ−Fe203の粒度を
変えても所望とする高透磁率は得られない。以下実施例
において本発明の態様および効果を示す。実施例
Ni017.8hol % , Zm032.9hol
% , Q −Fe2Q5仇hol%の割合に秤取し
た素原料をポールミルで混合、1000℃以下で焼成、
粉砕後れon/地で金型プレスで成型し、1350℃以
下で碗結した。Here, the reason why the blending ratio of nickel-zinc ferrite was limited to 15 to 25% of nickel oxide, 15 to 35% of zinc oxide, and 45 to 60% of ferric oxide in molar percentage is that high magnetic permeability can be obtained. This is because the composition range is effective only within the range of the above-mentioned compounding ratio, and is controlled by the particle size of the Q-Fe2Q raw material within that composition range. therefore,
If the mixing ratio of zinc oxide, nickel oxide, and ferric oxide is less than or greater than the above, the desired high magnetic permeability cannot be obtained even if the particle size of Q-Fe203 is changed. The embodiments and effects of the present invention will be shown below in Examples. Example Ni017.8hol%, Zm032.9hol
%, Q-Fe2Q5 hol%, the raw materials were mixed in a pole mill, fired at below 1000℃,
After pulverization, it was molded with a metal mold press and cassetted at 1350° C. or lower.
用いた素原料の平均粒径は、Ni○およびZn○がいず
れも3〆である。Q一Fe203は0.025r,0.
05仏,0.1仏,1〆および5山のものを用いた。前
記粒径を有する素原料からフェライトを得るための製造
条件は、すべて同一条件でおこなった。得られた試料に
ついて、0.9MHzにおける透磁率仏、電気抵抗p(
Q肌)、磁束密度Bo(G)および暁結密度d(夕/地
)を測定して第1表に示す結果を得た。第1表表から明
らかなように、Q−Fe203の粒径が1〆以上となり
、磁気的にもはや微粒子の性質を示さなくなるとともに
、暁結密度も著しく低下し、磁気特性も劣化することが
わかる。The average particle size of the raw materials used was 3.0 for both Ni○ and Zn○. Q-Fe203 is 0.025r, 0.
05 Buddha, 0.1 Buddha, 1〆 and 5 Mountain were used. All production conditions for obtaining ferrite from raw materials having the above particle size were the same. Regarding the obtained sample, magnetic permeability at 0.9 MHz and electrical resistance p(
The results shown in Table 1 were obtained by measuring the magnetic flux density Bo (G) and the dawn density d (evening/earth). As is clear from Table 1, when the particle size of Q-Fe203 becomes 1 or more, it no longer exhibits the properties of fine particles magnetically, and the crystal density also decreases significantly, and the magnetic properties also deteriorate. .
また、表に示した試料について、X線回折、組織観察お
よびX線マイクロアナライザーによる検討をおこなった
ところ、上記試料はいずれもNiZnフェライト単相で
あった。しかしながら、Q一Fe203の粒径が1.叫
以上になると、これから製造したフェライト孫絹体の空
孔はやや増加した。さらに5rの原料を用いた場合、空
孔は主として粒界に多くなり、X線マイクロアナライザ
ーによっても、Niイオンの分布が幾分不均一になって
いることが確認された。また、0.1仏以下のQ−Fe
2Q微粒子を用いることによって、仮競温度および競精
温度をそれぞれ100〜200℃程度低下することがで
きる。以上詳述した如く、Q一Fe203微粒子を素原
料とする本発明Ni−Znフェライト材料は、従釆の材
料に比して、低温でしかも初透磁率の高い高密度焼結体
として成し得るので、本材料を磁気ヘッドなどに適用す
れば、実用上益するところ大なるものがある。Moreover, when the samples shown in the table were examined by X-ray diffraction, structure observation, and an X-ray microanalyzer, all of the samples were found to have a single phase of NiZn ferrite. However, the particle size of Q-Fe203 is 1. When the temperature was exceeded, the number of pores in the ferrite silk body produced from this increased slightly. Furthermore, when a 5r raw material was used, the number of vacancies increased mainly at grain boundaries, and it was confirmed by an X-ray microanalyzer that the distribution of Ni ions was somewhat non-uniform. In addition, Q-Fe of 0.1 French or less
By using 2Q fine particles, the preliminary temperature and competitive temperature can be lowered by about 100 to 200°C, respectively. As detailed above, the Ni-Zn ferrite material of the present invention, which uses Q-Fe203 fine particles as the raw material, can be formed as a high-density sintered body at a lower temperature and with a higher initial magnetic permeability than the secondary materials. Therefore, if this material is applied to magnetic heads, etc., there will be great practical benefits.
Claims (1)
−亜鉛フエライトを製造するにあたり、該主成分のうち
Fe_2O_3のみに、他の主成分原料の粒径よりも小
さい、平均粒径0.5μ以下の素原料を用いることを特
徴とするNi−Znフエライトの製造方法。1 In producing nickel-zinc ferrite consisting of NiO, ZnO, and Fe_2O_3, raw materials with an average particle size of 0.5 μ or less, which is smaller than the particle size of the other main component raw materials, are used only for Fe_2O_3 among the main components. A method for producing Ni-Zn ferrite, characterized by the following.
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP50015308A JPS605044B2 (en) | 1975-02-07 | 1975-02-07 | Ferrite manufacturing method |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP50015308A JPS605044B2 (en) | 1975-02-07 | 1975-02-07 | Ferrite manufacturing method |
Publications (2)
| Publication Number | Publication Date |
|---|---|
| JPS5190310A JPS5190310A (en) | 1976-08-07 |
| JPS605044B2 true JPS605044B2 (en) | 1985-02-08 |
Family
ID=11885156
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP50015308A Expired JPS605044B2 (en) | 1975-02-07 | 1975-02-07 | Ferrite manufacturing method |
Country Status (1)
| Country | Link |
|---|---|
| JP (1) | JPS605044B2 (en) |
Families Citing this family (1)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| JP2729486B2 (en) * | 1988-07-09 | 1998-03-18 | 富士電気化学株式会社 | Nickel-zinc ferrite material for radio wave absorber |
Family Cites Families (1)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| NL281410A (en) * | 1962-07-25 | 1964-12-10 |
-
1975
- 1975-02-07 JP JP50015308A patent/JPS605044B2/en not_active Expired
Also Published As
| Publication number | Publication date |
|---|---|
| JPS5190310A (en) | 1976-08-07 |
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