JPS6051245B2 - Manufacturing method of NiZn ferrite - Google Patents
Manufacturing method of NiZn ferriteInfo
- Publication number
- JPS6051245B2 JPS6051245B2 JP52027012A JP2701277A JPS6051245B2 JP S6051245 B2 JPS6051245 B2 JP S6051245B2 JP 52027012 A JP52027012 A JP 52027012A JP 2701277 A JP2701277 A JP 2701277A JP S6051245 B2 JPS6051245 B2 JP S6051245B2
- Authority
- JP
- Japan
- Prior art keywords
- hip
- magnetic
- ferrite
- sintered body
- sintered
- 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.)
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- Magnetic Ceramics (AREA)
- Soft Magnetic Materials (AREA)
Description
【発明の詳細な説明】
本発明は極めて高い焼結密度を有し、結晶粒径が均一
で特に高周波帯域における透磁率の損失項が小さく、著
しく高周波特性に優れたNiZn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 relates to a method for producing NiZn ferrite which has an extremely high sintered density, a uniform crystal grain size, a small permeability loss term especially in a high frequency band, and excellent high frequency characteristics. It is something.
近年、磁気記録応用分野の拡大および進展に伴なつて
、磁気テープを主体とした磁気記録媒体も著しい進歩を
とげ、高密度の記録が可能となつてきた。BACKGROUND ART In recent years, with the expansion and progress of the field of magnetic recording applications, magnetic recording media, mainly magnetic tapes, have also made remarkable progress, making it possible to perform high-density recording.
記録媒体と共に、磁気記録に必要不可欠な磁気ヘッドに
ついても、高密度記録化に見合うだけの各種磁気特性、
高周波特性、耐摩耗性等の各種要求特性は厳しさの一途
を辿つている。こうした中で、フェライト磁気ヘッドは
、欠け、割れなどの脆さはあるが、周波数特性および耐
摩耗性に優れており、最近では特にMH2帯において優
れた周波数特性を有する磁気記録材料が要求される趨勢
にある。かかる要求特性を満足するためには、厳密な組
成的検討は勿論のこと、結晶粒径が均一で小さく、しか
も焼結密度がほぼ理論密度に等しいような極めて高密度
の焼結体でなければならない。NiZnフェライトは、
工業的には主として通常の乾式法によつて製造されてい
るが、この場合焼結密度は、99.2%程度が限度てあ
る。この方法による高密度焼結体は、焼結温度が高いた
め結晶粒子も大となり、しばしは高周波における透磁率
が著しく低下することになる。さらに高温で焼結した場
合には、還元相の一種である第2相の析出を伴なつて、
機械的強度に著しいバラツキが生じ、加工時に割れ、欠
けおよび結晶粒子の脱落等が生じることはよく知られて
おり、発明者達もかかる欠点を改善した。機械的強度大
なる酸化金属磁心材料をすでに特許として出願している
。 ところで高密度UiZnフェライトを製造する従来
法としては、共沈法もしくは空気酸化法等の湿式法によ
つて作成した粉末、または乾式法で得られた所定の組成
を有する仮焼粉をホットプレスによつて焼結し高密度化
する方法がある。この方法は通常の乾式法に比べて優れ
ており、平均結晶粒径5〜20μ程度、相対焼結密度9
9.0〜99.8%程度の焼結体を得ることができる。
しかしながら、ホットブレス法の難点は、加圧方法が静
水圧的ではないことから、複雑な形状の焼結体を得るこ
とができないこと、また装置的な制約から大型の焼結体
を得ることが困難であり、連続ホットブレスを用いても
工業的に得策ではない。この方法のさらに大きな欠点は
、フェライトをアルミナ等の粉末で被覆して熱間加圧を
おこなう必要があり、焼結時にフェライトと被覆材との
間で生じる固相反応を防止することが不可能な点である
。したがつて、焼結体の中心部と表面に近い部分とでは
、組織的にバラツキが生じ、特に表面近傍においては、
他の化合物が生成するため、焼結体表面からかなりの部
分を除去しなければならず収率も低下する。前記欠点を
除去する方法として、熱間静水圧ブレスを用いた製造法
が特開昭49−128296により公知となつている。Along with the recording medium, the magnetic head, which is essential for magnetic recording, has various magnetic properties and characteristics that are suitable for high-density recording.
Various required characteristics such as high frequency characteristics and wear resistance are becoming increasingly strict. Under these circumstances, ferrite magnetic heads have excellent frequency characteristics and wear resistance, although they are brittle such as chipping and cracking.Recently, magnetic recording materials with excellent frequency characteristics, especially in the MH2 band, are required. It's on trend. In order to satisfy these required properties, in addition to strict compositional considerations, the crystal grain size must be uniform and small, and the sintered body must be extremely dense, with a sintered density almost equal to the theoretical density. No. NiZn ferrite is
Industrially, it is mainly manufactured by a normal dry method, but in this case, the sintered density is limited to about 99.2%. A high-density sintered body produced by this method has large crystal grains due to the high sintering temperature, and often has a marked decrease in magnetic permeability at high frequencies. When sintered at an even higher temperature, a second phase, which is a type of reduced phase, is precipitated.
It is well known that significant variations in mechanical strength occur, resulting in cracking, chipping, and shedding of crystal grains during processing, and the inventors have also improved these drawbacks. We have already filed a patent application for a metal oxide magnetic core material with high mechanical strength. By the way, as a conventional method for manufacturing high-density UiZn ferrite, a powder prepared by a wet method such as a coprecipitation method or an air oxidation method, or a calcined powder having a predetermined composition obtained by a dry method is heated in a hot press. There is a method of sintering and increasing the density. This method is superior to the normal dry method, with an average grain size of about 5 to 20μ and a relative sintering density of 9.
A sintered body of about 9.0 to 99.8% can be obtained.
However, the drawbacks of the hot press method are that it is not possible to obtain sintered bodies with complex shapes because the pressurization method is not hydrostatic, and that it is difficult to obtain large sintered bodies due to equipment limitations. This is difficult, and it is not industrially advisable to use continuous hot breath. A further disadvantage of this method is that the ferrite must be coated with powder such as alumina and hot pressurized, making it impossible to prevent the solid phase reaction that occurs between the ferrite and the coating material during sintering. This is a point. Therefore, there are variations in structure between the center of the sintered body and the parts near the surface, especially near the surface.
Since other compounds are produced, a considerable portion must be removed from the surface of the sintered body, resulting in a decrease in yield. As a method for eliminating the above-mentioned drawbacks, a manufacturing method using hot isostatic pressing is known from JP-A-49-128296.
しかしながら、細部においてはまだ検討の必要がある。
熱間静水圧ブレス(以下HIPと略記する)法を用いた
場合、アルミナ等の被覆材も不要てほぼ理論密度に近い
焼結体を得ることができるが、加圧時に蓄積される歪応
力ならびにHIP時に還元雰囲気による還元相の生成ま
たはフェライトマトリックス自体が化学量論組成よりも
若干酸素不足の組成に還元されることなどによつてHI
P後の磁気特性は著しく劣化する。前記歪応力は、適当
な条件下で歪取り焼鈍をおこなうことによつて、磁気特
性の回復を図ることができる。どころで、NiZnフェ
ライトは、八面体位置占有傾向が極めて強いNi2+お
よび四面体位置占有傾向が著しいZn2+を含有してい
るため、還元雰囲気中で焼結した場合、しばしばこれら
のイオンはスピネル相から分離して、それぞれNi2+
過剰の場合にはNacl型、Zn2+過剰の場合には六
方晶Zincite型構造と考えられる第2相を形成す
る。However, the details still need to be considered.
When using the hot isostatic pressing (hereinafter abbreviated as HIP) method, a sintered body with almost theoretical density can be obtained without the need for a covering material such as alumina. HI occurs due to the formation of a reduced phase due to the reducing atmosphere during HIP, or because the ferrite matrix itself is reduced to a composition that is slightly oxygen deficient compared to the stoichiometric composition.
The magnetic properties after P are significantly deteriorated. The strain stress can be recovered by performing strain relief annealing under appropriate conditions to recover the magnetic properties. However, since NiZn ferrite contains Ni2+, which has a very strong tendency to occupy octahedral positions, and Zn2+, which has a strong tendency to occupy tetrahedral positions, when sintered in a reducing atmosphere, these ions are often separated from the spinel phase. and Ni2+, respectively.
In the case of excess Zn2+, a second phase is formed which is considered to be a NaCl type structure, and in the case of excess Zn2+, a second phase is formed which is considered to be a hexagonal Zincite type structure.
これら第2相の形成はフェライトマトリックスの組成的
な変動を引き起こし、しばしは独立した結晶粒子として
生成するため、所定の磁気特性が得難く、焼結体の硬度
等の機械的性質にバラツキが生じ、加工性を著しく劣化
せしめる。またHIPは通常装置土の制約からk雰囲気
中でおこなうため、第2相の生成を伴なわない場合にお
いてすら、特にHIP処理後のNiZnフェライトは、
化学量論組成よりも幾分酸素欠損の組成すなわち還元組
成となる。同様のことは、予備焼結を還元雰囲気下でお
こなつた場合には生ずるわけで、因みに空気中1250
℃以上で焼結したNiZnフェライトは還元組成を形成
することによつて電気抵抗率が低下し、同時に高周波帯
域での透磁率の低下ならびにその損失の増大を引き起こ
す。The formation of these second phases causes compositional fluctuations in the ferrite matrix and is often generated as independent crystal grains, making it difficult to obtain desired magnetic properties and causing variations in mechanical properties such as hardness of the sintered body. , which significantly deteriorates workability. Furthermore, because HIP is usually performed in a K atmosphere due to equipment soil limitations, even in cases where the formation of a second phase is not involved, the NiZn ferrite after HIP treatment is
The composition becomes a somewhat oxygen-deficient composition, that is, a reduced composition, rather than the stoichiometric composition. A similar thing occurs when preliminary sintering is carried out in a reducing atmosphere;
NiZn ferrite sintered at temperatures above .degree. C. forms a reduced composition, thereby decreasing its electrical resistivity, and at the same time causing a decrease in magnetic permeability and an increase in loss in the high frequency band.
さらにHIPによつて高密度化を図る場合には前記還元
組成を形成するN2を含む予備焼結時の雰囲気は緻密化
を著しく阻害する。すなわち、一次焼結温度よりも低温
側でHIPをおこなう場合には、緻密化が進行する機構
は明らかではないが、熱力学的に見て(1)式が大まか
な近似として成り立つや考えることができる。Furthermore, when densification is attempted by HIP, the atmosphere during preliminary sintering containing N2 forming the reducing composition significantly inhibits densification. In other words, when HIP is performed at a temperature lower than the primary sintering temperature, the mechanism by which densification progresses is not clear, but from a thermodynamic point of view, it can be considered that equation (1) holds true as a rough approximation. can.
ここでPextは外圧すなわちHIP圧力、PpOre
は焼結体内部の空孔圧、rは空孔径、γは空孔の界面張
力である。Here, Pext is external pressure, that is, HIP pressure, PpOre
is the pore pressure inside the sintered body, r is the pore diameter, and γ is the interfacial tension of the pores.
ところでHIPによるさ103atmの静水圧は、10
00℃程度においてもイオンが化学結合力(1CP〜1
σAtmの静水圧に相当)によつて配列している結晶粒
子内にそれ程大なる影響を及ぼさないと考えられる。し
たがつて、HIPの実効温度が一次焼結温度よりも低い
場合には加圧時において、結晶粒子は化学結合力よりも
はるかに弱い束縛力(つまり界面張力)て釣合つている
結晶粒界に沿つて辷ることにより、大部分の緻密化が進
行すると推定される。事実、予備焼結体がオープンボア
の生成を伴なわない限り結晶粒界が多い程、・すなわち
結晶粒径が小さい程、HIP時において緻密化は容易に
進行し、NiZnフェライトもこの方法により高密度焼
結体を得ることができる。NiZnフェライトを空気に
おいて一次焼結をおこなつた場合、焼結体内部の空孔は
数気圧程度の空気を含有すると推定される。一次焼結温
度よりも低温側でHIPをおこない、前記機構で緻密化
が進行する楊合には、(1)式におけるHIP後のPp
Oreは数百気圧程度にまで上昇し、空孔の体積は11
100程度にまで減少することになる。勿論酸化物内で
l拡散速度の大きい02は、その一部がHIP時に結晶
粒界から焼結体表面へと拡散離脱するてあろうが、拡散
速度の遅いN2は、その大部分が高圧状態で閉じ込めら
れ、HIP時のAr雰囲気と共に焼結体内部の粒界にお
いても還元雰囲気となり、これが第2還元相の析出およ
びフェライトマトリックスが還元側へと組成がシフトす
るひとつの原因となることが予想される。なお、一次焼
結温度よりもHIP温度が高い場合にも、ほぼ同様のこ
とが起り得ると考えられる。事実かかる試料を実施例に
おいて後述するように、所定の磁気特性を得る目的で長
時間焼鈍した場合には、圧縮された空孔の体積が再び膨
張することによつて、焼結密度を低下させる場合がしば
しば起る。また、かかる高圧ガスを内胞するNlZnフ
ェライトを用いて磁気ヘッド等の磁心を製造する場合、
研削およびラップ等の加工時において、材料表面の結晶
粒子が高圧ガスによつて脱落せしめられ、あるいは磁気
ヘッドを形成した後も磁気ディスクもしくは磁気テープ
との接触による脱粒を伴なつて摩耗、破損の問題が生じ
、磁気ヘッドの寿命は著しく短縮することになる。本発
明の方法は、前記欠点を除去するためになされたもので
ある。By the way, the hydrostatic pressure of 103 atm due to HIP is 10
Even at around 00°C, ions have a chemical bonding strength (1CP~1
It is considered that this does not have a large effect on the crystal grains arranged by the hydrostatic pressure of σAtm). Therefore, if the effective temperature of HIP is lower than the primary sintering temperature, the crystal grains will form grain boundaries that are balanced by a binding force (i.e., interfacial tension) that is much weaker than the chemical bond force during pressurization. It is estimated that most of the densification progresses by walking along the . In fact, as long as the preliminary sintered body does not involve the formation of open bores, the more grain boundaries there are, i.e., the smaller the grain size, the easier densification will progress during HIP, and NiZn ferrite can also be densified by this method. A dense sintered body can be obtained. When NiZn ferrite is primarily sintered in air, it is estimated that the pores inside the sintered body contain air at a pressure of about several atmospheres. In the case where HIP is performed at a lower temperature than the primary sintering temperature and densification progresses by the above mechanism, Pp after HIP in equation (1) is
Ore rises to several hundred atmospheres, and the volume of the pores is 11
The number will decrease to about 100. Of course, a portion of 02, which has a high diffusion rate in the oxide, will diffuse away from the grain boundaries to the surface of the sintered body during HIP, but most of the N2, which has a slow diffusion rate, will be released under high pressure. It is expected that this will become a reducing atmosphere at the grain boundaries inside the sintered body along with the Ar atmosphere during HIP, and this will be one of the reasons for the precipitation of the second reduced phase and the composition shift of the ferrite matrix toward the reducing side. be done. In addition, it is thought that almost the same thing can occur even when the HIP temperature is higher than the primary sintering temperature. In fact, as described later in Examples, when such a sample is annealed for a long time in order to obtain predetermined magnetic properties, the volume of the compressed pores expands again, reducing the sintered density. cases often occur. In addition, when manufacturing magnetic cores such as magnetic heads using NlZn ferrite containing such high-pressure gas,
During processing such as grinding and lapping, crystal grains on the material surface are removed by high-pressure gas, or even after the magnetic head is formed, they may come into contact with the magnetic disk or magnetic tape, causing wear and damage. Problems arise and the life of the magnetic head is significantly shortened. The method of the present invention has been made to eliminate the above-mentioned drawbacks.
すなわち、本発明の方法においては、一次焼結を酸素中
でおこなうことによつて、前記第2相の生成ならびに還
元組成の生成を防止し、一次焼結体の内部空孔内のガス
を拡散速度の大なる02とすることによつて、HIP時
に高密度化を促進させ、併せてHIP後の高圧ガスを含
む空孔の生成を極力防止するものてある。かくして得ら
れた焼結体は、所定の磁気特性を有し、機械的強度にバ
ラツキが無く、著しく加工性に優れた高密度焼結体とな
る。That is, in the method of the present invention, by performing the primary sintering in oxygen, the formation of the second phase and the reduction composition are prevented, and the gas in the internal pores of the primary sintered body is diffused. By setting the speed to 02, which is high, densification is promoted during HIP, and at the same time, the generation of pores containing high pressure gas after HIP is prevented as much as possible. The thus obtained sintered body is a high-density sintered body that has predetermined magnetic properties, has no variation in mechanical strength, and has excellent workability.
さらに高周波領域における透磁率の損失が小さいことも
大なる特徴である。以下実施例に基づき本発明の態様を
示す。実施例
本発明の方法を用いて製造をおこなつた磁心材料用のN
iZnフェライト、モル比でNjOlO〜25%、Zn
Ol5〜40%、Fe2O345〜60%から成る組成
物である。Another important feature is that the loss of magnetic permeability in the high frequency region is small. Embodiments of the present invention will be illustrated below based on Examples. Example N for magnetic core material manufactured using the method of the present invention
iZn ferrite, molar ratio NjOlO ~ 25%, Zn
The composition consists of 5 to 40% Ol and 45 to 60% Fe2O.
なお所定の電気抵抗値を得る目的をもつて、特に重量比
でMnO2O.OOl〜3.0%を配合しているが、M
nO2を配合しなく共同様に高密度焼結体を得ることが
てきる。かかる混合物を所望の形状に加圧成形後、二段
工程により焼結をおこない、さらに熱処理を施した工程
を含むものから構成される。すなわち、各素原料を上記
組成となるように配合したのち、ボールミルもしくは振
動ミルによつて十分に混合をおこない、空気中800〜
1300℃で3吟以上仮焼したのち、再度ボールミルも
しくは振動ミル等により十分に粉砕をおこなつた。In addition, for the purpose of obtaining a predetermined electrical resistance value, MnO2O. Although OOl ~ 3.0% is blended, M
Similarly, a high-density sintered body can be obtained without adding nO2. It is comprised of a process in which the mixture is pressure-molded into a desired shape, sintered in a two-step process, and then heat-treated. That is, after blending each raw material so that it has the above composition, it is thoroughly mixed using a ball mill or a vibration mill, and the
After calcining at 1300° C. for 3 or more minutes, the mixture was thoroughly pulverized again using a ball mill, vibration mill, or the like.
次いで粉砕粉を加圧により金型成形もしくはラバープレ
ス成形したのち、酸素中1300℃以下で30分以上一
次焼結をおこなつたのち、Ar雰囲気下で500〜17
0〔TmllOOO〜1250℃の条件でHIPをおこ
なつた。さらに最終工程として、著しい結晶粒成長を生
ずる温度ならびに/または第2相が析出する温度以下て
焼鈍を施すことによつて所定の磁気特性を有し、平均結
晶粒径20p以下てしかも焼結密度がほぼ100%のN
iZnフェライトを製造することができた。上記素原料
としては、一般に酸化物が用いられるが、本発明におい
ては必ずしもかかる酸化物に限定されるものではなく、
その他酸化物の代りに焼成時に容易に酸化物に変化し得
る例えばオキシ水酸化物、水酸化物、炭酸塩、硝酸塩、
硫酸塩および蓚酸塩の如き化合物を用いることもできる
。Next, the pulverized powder is molded into a mold or rubber press by pressure, and then primary sintered in oxygen at 1300°C or less for 30 minutes or more, and then sintered in an Ar atmosphere to form a 500-170°C
HIP was performed under conditions of 0[TmllOOOO~1250°C. Furthermore, as a final step, annealing is performed at a temperature below which significant crystal grain growth occurs and/or a temperature at which a second phase precipitates. is almost 100% N
iZn ferrite could be manufactured. Although oxides are generally used as the raw materials, the present invention is not necessarily limited to such oxides.
In place of other oxides, there are oxyhydroxides, hydroxides, carbonates, nitrates, etc. that can be easily converted into oxides during firing.
Compounds such as sulfates and oxalates can also be used.
第1表は、組成がモル比でそれぞれA(NlOl7.5
、ZnO32.5、Fe2O35O.O)およびB(N
jOl8.O、ZnO32.5.Fe2O349.5)
である各素原料にMnO2を0.18Wt%添加した混
合粉末を前記製造工程にしたがい、仮焼:空気中(1)
900℃および(■)1200℃、一次焼結:酸素中、
(1)1120℃および(■)1220′C1田P:1
1000C11000atmおよび1200℃、150
01tm1焼鈍:酸素中、(1)1000℃および(■
)1100℃の各条件で製造した焼結体の諸特性である
。Table 1 shows the composition of A(NlOl7.5
, ZnO32.5, Fe2O35O. O) and B(N
jOl8. O, ZnO32.5. Fe2O349.5)
A mixed powder in which 0.18 wt% of MnO2 was added to each raw material was calcined in air (1) according to the manufacturing process described above.
900℃ and (■) 1200℃, primary sintering: in oxygen,
(1) 1120℃ and (■) 1220'C1P: 1
1000C11000atm and 1200℃, 150
01tm1 annealing: in oxygen, (1) 1000°C and (■
) Characteristics of sintered bodies manufactured under various conditions of 1100°C.
表から明らかなごとく、本発明の方法で得た焼結体の密
度は相対値d/Dx(Dx:理論密度)で99.7〜9
9.9%を有し、極めて高密度である。As is clear from the table, the density of the sintered body obtained by the method of the present invention is 99.7 to 9 in relative value d/Dx (Dx: theoretical density).
It has an extremely high density of 9.9%.
因みに従来の焼結法およびホットブレス法を用いて最適
条件下で製造した組成Aの焼結体は、d/DXがそれぞ
れ98.9%および99.6%であつた。しかしながら
、■焼および一次焼結を空気中でおこなつた場合でも、
HIP法によつてd/DXに関しては99.8%程度の
焼結体を得ることができる。また磁気特性の内、磁束密
度BlOl抗磁力HClキュリー点Tcは、本発明の方
法と従来のHIP法およびホットブレス法との間に大き
い差異は見られないが、初透磁率P″およびその損失項
P″の周波数特性は著しく異なる。第1図は、第1表に
示す試料Aのμ″およびp″の周波数特性である。図か
ら明らかなように、本発明の方法(■)で得られた焼結
体イは、仮焼を空気中でおこなつた従来のHIP法によ
るそれ口およびホットブレス法で得た試料ハに比べて、
2MFIz上の高周波帯域でのp″が大であると共にμ
2は著しく減少している。すなわち本発明の方法で製造
したNiZnフェライトはM土帯で用いる磁気記録材料
として好適であり、焼結体イを用いて3M1Iz近傍で
使用する磁心を製造し、その出力特性を測定したところ
、従来材により作製した同じ形状構造の磁心の出力特性
に比べて、より大きな出力電圧を得ることが出来るとい
う優れた特性を示すことがわかつた。第2図および第3
図は、それぞれ本発明の方法および従来の仮焼ならびに
一次焼結を空気中でおこなつたHIP法によつて製造し
た焼結体を用いて作成した磁気ヘッド(磁心をエポキシ
系樹脂に埋設し、研磨(最終仕上バフ研磨)して得られ
たラップ面を、倍率500倍で撮影した光学顕微鏡組織
写真である。)図から明らかなように、本発明の方法に
より得られた材料から作成した磁心は、結晶粒子の脱落
を伴なわず、鮮明なラップ面が得られるのに対して、従
来法のそれは、加工時において粒子の脱落が生じている
。すなわち本発明の方法で製造したNiZnフェライト
は極めて高密度でしかも機械的性質にバラツキがなく、
著しく加工性に優れており、第2相も生成していないこ
とがわかる。以上述べたごとく、本発明による方法を用
いるならば、高周波帯域において著しく優れた磁気特性
を有し、極めて加工性に優れたNiZnフェライトが通
常のHIP装置を用いることによつて容易に製造するこ
とができる。Incidentally, the sintered bodies of composition A manufactured under optimal conditions using the conventional sintering method and hot pressing method had d/DX of 98.9% and 99.6%, respectively. However, even when sintering and primary sintering are performed in air,
By the HIP method, a sintered body with a d/DX of about 99.8% can be obtained. Among the magnetic properties, there is no major difference between the method of the present invention and the conventional HIP method and hot breath method in the magnetic flux density BlO coercive force HCl Curie point Tc, but the initial permeability P'' and its loss The frequency characteristics of term P'' are significantly different. FIG. 1 shows the μ″ and p″ frequency characteristics of Sample A shown in Table 1. As is clear from the figure, the sintered body A obtained by the method of the present invention (■) is different from the sample A obtained by the conventional HIP method in which calcination is performed in air, and the sample A obtained by the hot press method. Compared to,
In the high frequency band above 2MFIz, p″ is large and μ
2 has decreased significantly. That is, the NiZn ferrite produced by the method of the present invention is suitable as a magnetic recording material used in the M soil band, and when a magnetic core used in the vicinity of 3M1Iz was produced using the sintered body A and its output characteristics were measured, it was found that it was better than the conventional one. It was found that this material exhibits superior characteristics in that it is able to obtain a larger output voltage compared to the output characteristics of a magnetic core of the same shape and structure made from the same material. Figures 2 and 3
The figures show magnetic heads (magnetic core embedded in epoxy resin) manufactured using sintered bodies manufactured by the method of the present invention and the conventional HIP method in which calcination and primary sintering were performed in air. (This is an optical microscope structure photograph taken at a magnification of 500 times of the lapped surface obtained by polishing (final finishing buffing). With the magnetic core, a sharp lap surface can be obtained without crystal grains falling off, whereas with conventional methods, particles fall off during processing. In other words, the NiZn ferrite produced by the method of the present invention has extremely high density and has uniform mechanical properties.
It can be seen that the workability is extremely excellent and no second phase is formed. As described above, if the method according to the present invention is used, NiZn ferrite, which has extremely excellent magnetic properties in a high frequency band and is extremely easy to work with, can be easily produced using a normal HIP device. I can do it.
また安価な工業用原料を用いて、所定の磁気特性を有す
る材料を容易に量産できるため、工業的価値も大なるも
のがある。Furthermore, since materials having predetermined magnetic properties can be easily mass-produced using inexpensive industrial raw materials, they have great industrial value.
第1図は、本発明の方法で得られた組成Aイ、”従来の
HIP方法でられた同組成口およびホットブレス法で得
られた同組成ハの各焼結体について透磁率の周波数特性
図、第2図および第3図は、それぞれ本発明の方法およ
び従来のHIP方法によつて製造した組成Aの材料から
作成したNiZnフェライト磁気ヘッド磁心のラップ面
の顕微鏡写真である。Figure 1 shows the frequency characteristics of magnetic permeability for each sintered body of composition A obtained by the method of the present invention, composition A obtained by the conventional HIP method, and composition C obtained by the hot pressing method. 2 and 3 are micrographs of the lap surfaces of NiZn ferrite magnetic head cores made from materials of composition A produced by the method of the present invention and the conventional HIP method, respectively.
Claims (1)
ンボア(試料表面から中心部までに通じる空孔)を形成
させない程度にまで一次焼結をおこなう工程と、該一次
焼結後のフェライト材を熱間静圧プレスする工程と該熱
間静圧プレス後のフェライト材を焼鈍する各工程の内、
該一次焼結工程を酸素雰囲気中でおこなうことを特徴と
するNiZnフェライトの製造方法。1. A step of calcining the raw material, a step of sintering the calcined powder to perform primary sintering to the extent that no open bores (holes extending from the surface of the sample to the center) are formed, and the primary sintering. Of the subsequent steps of hot isostatic pressing the ferrite material and annealing the ferrite material after the hot isostatic pressing,
A method for producing NiZn ferrite, characterized in that the primary sintering step is performed in an oxygen atmosphere.
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP52027012A JPS6051245B2 (en) | 1977-03-14 | 1977-03-14 | Manufacturing method of NiZn ferrite |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP52027012A JPS6051245B2 (en) | 1977-03-14 | 1977-03-14 | Manufacturing method of NiZn ferrite |
Publications (2)
| Publication Number | Publication Date |
|---|---|
| JPS53112494A JPS53112494A (en) | 1978-09-30 |
| JPS6051245B2 true JPS6051245B2 (en) | 1985-11-13 |
Family
ID=12209178
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP52027012A Expired JPS6051245B2 (en) | 1977-03-14 | 1977-03-14 | Manufacturing method of NiZn ferrite |
Country Status (1)
| Country | Link |
|---|---|
| JP (1) | JPS6051245B2 (en) |
Family Cites Families (2)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| JPS5610770B2 (en) * | 1972-08-21 | 1981-03-10 | ||
| JPS5427558B2 (en) * | 1973-04-12 | 1979-09-11 |
-
1977
- 1977-03-14 JP JP52027012A patent/JPS6051245B2/en not_active Expired
Also Published As
| Publication number | Publication date |
|---|---|
| JPS53112494A (en) | 1978-09-30 |
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