JPS6029204B2 - Manufacturing method of high-density Ni-Zn ferrite - Google Patents
Manufacturing method of high-density Ni-Zn ferriteInfo
- Publication number
- JPS6029204B2 JPS6029204B2 JP51146475A JP14647576A JPS6029204B2 JP S6029204 B2 JPS6029204 B2 JP S6029204B2 JP 51146475 A JP51146475 A JP 51146475A JP 14647576 A JP14647576 A JP 14647576A JP S6029204 B2 JPS6029204 B2 JP S6029204B2
- Authority
- JP
- Japan
- Prior art keywords
- ferrite
- magnetic permeability
- density
- initial magnetic
- initial
- 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
Links
- 229910000859 α-Fe Inorganic materials 0.000 title claims description 15
- 229910018605 Ni—Zn Inorganic materials 0.000 title claims description 8
- 238000004519 manufacturing process Methods 0.000 title claims description 4
- 239000000843 powder Substances 0.000 claims description 11
- 239000000463 material Substances 0.000 claims description 9
- 238000001513 hot isostatic pressing Methods 0.000 claims description 5
- 238000005245 sintering Methods 0.000 claims description 5
- 238000001354 calcination Methods 0.000 claims description 4
- 239000011148 porous material Substances 0.000 claims description 3
- 238000000137 annealing Methods 0.000 claims 1
- 239000002994 raw material Substances 0.000 claims 1
- 230000035699 permeability Effects 0.000 description 22
- 239000013078 crystal Substances 0.000 description 14
- 230000000694 effects Effects 0.000 description 8
- 238000000034 method Methods 0.000 description 7
- 230000005347 demagnetization Effects 0.000 description 5
- 230000005415 magnetization Effects 0.000 description 4
- 239000000203 mixture Substances 0.000 description 4
- 239000002245 particle Substances 0.000 description 3
- IJGRMHOSHXDMSA-UHFFFAOYSA-N Atomic nitrogen Chemical compound N#N IJGRMHOSHXDMSA-UHFFFAOYSA-N 0.000 description 2
- 238000007796 conventional method Methods 0.000 description 2
- 230000007423 decrease Effects 0.000 description 2
- 238000010586 diagram Methods 0.000 description 2
- 238000010438 heat treatment Methods 0.000 description 2
- 235000010469 Glycine max Nutrition 0.000 description 1
- 244000068988 Glycine max Species 0.000 description 1
- 238000005056 compaction Methods 0.000 description 1
- 230000002860 competitive effect Effects 0.000 description 1
- 238000009826 distribution Methods 0.000 description 1
- 230000002401 inhibitory effect Effects 0.000 description 1
- 238000003754 machining Methods 0.000 description 1
- 239000000696 magnetic material Substances 0.000 description 1
- 238000002156 mixing Methods 0.000 description 1
- 238000000465 moulding Methods 0.000 description 1
- 229910052757 nitrogen Inorganic materials 0.000 description 1
- 229910000889 permalloy Inorganic materials 0.000 description 1
- 238000003825 pressing Methods 0.000 description 1
- 238000010298 pulverizing process Methods 0.000 description 1
- 239000000376 reactant Substances 0.000 description 1
- 229910052596 spinel Inorganic materials 0.000 description 1
- 239000011029 spinel Substances 0.000 description 1
- 239000000126 substance Substances 0.000 description 1
Landscapes
- Magnetic Ceramics (AREA)
- Soft Magnetic Materials (AREA)
Description
【発明の詳細な説明】
近年、情報量の増大に伴い、記録密度を向上させること
が重要な課題となっているが、磁気記録の分野でもこの
要求にこたえるため、記録周波数はより高周波へ移行し
つつある。[Detailed Description of the Invention] In recent years, with the increase in the amount of information, improving recording density has become an important issue.In order to meet this demand in the field of magnetic recording, the recording frequency has shifted to higher frequencies. It is being done.
それにつれて、磁気へッド‘こ使われる材料もより高周
波特性の優れたものが要求されるようになってきた。こ
のように材料に対しては、いわば極限に近い特性を発揮
することが要求されるため、その安定性が一層重要とな
る。現在、磁気ヘッドに使われている材料は、パーマロ
イ、Mn−Znフェライト、Ni−Znフェライトなど
が主なものであるが安定性面で従来問題があった。例え
ば、Mn−Znフェライトにおいては、デイスアコモデ
ーョン(以下DAと記す)という現象がよく知られてお
り、初透磁率が経時変化をし、長時間経過した後では当
初の値より10%も減少することがある。As a result, materials used in magnetic heads are required to have even better high frequency characteristics. In this way, materials are required to exhibit properties that are close to their limits, so their stability becomes even more important. Currently, the main materials used for magnetic heads are permalloy, Mn--Zn ferrite, Ni--Zn ferrite, etc., but they have traditionally had problems in terms of stability. For example, in Mn-Zn ferrite, a phenomenon called disaccommodation (hereinafter referred to as DA) is well known, in which the initial magnetic permeability changes over time, and after a long period of time it decreases by 10% from the initial value. may also decrease.
しかし、この場合には窒素中で熱処理することによって
、DAを1%以下にすることが可能である。Ni−Zn
フェライトにおいても小さいながらもDAが認められる
が、この場合にはDAよりもむしろ熱消磁などによる初
透磁率の変化の方が、材料の安定性を阻害する大きな要
因となる。Ni一Znフェライトの場合、実際に磁気ヘ
ッドとして使用される周波数帯城における磁化機構はM
h−Znフェライトと同様に磁壁移動によるものが主で
あると考えられている。However, in this case, it is possible to reduce the DA to 1% or less by heat treatment in nitrogen. Ni-Zn
DA is also observed in ferrite, although it is small, but in this case, the change in initial magnetic permeability due to thermal demagnetization is a greater factor in inhibiting the stability of the material than DA. In the case of Ni-Zn ferrite, the magnetization mechanism in the frequency band actually used as a magnetic head is M
Similar to h-Zn ferrite, it is thought that the main cause is domain wall movement.
したがって、初透磁率の大きさは磁壁移動の難易によっ
て決まるが、この場合、磁壁移動を妨げる要因として、
物質固有の結晶異方性、空孔および結晶粒界などが挙げ
られる。この中で、結晶異方性は組成によって決まるも
のであり、また、熱間静水圧プレス(mP)を行なった
後には空孔も極端に減少し、ほぼ理論密度に近い密度を
持った焼結体が得られるため、空孔の影響も小さいと思
われる。したがって、このような高密度Ni−Znフェ
ライトにおいて組成が同一の場合には、初透磁率を左右
する主な要因は結晶粒界と考えることができる。初透磁
率(とくに磁壁移動が王であると考えられる周波数帯城
における初透磁率)は、結晶粒径、すなわち結晶粒界の
数に大きく影響され、Ni−Znフェライトにおいても
、一般に結晶粒径が小さければ初透磁率は低く、粒径が
大きくなるにつれて初透磁率も高くなるが、粒径が数ミ
クロン以上ではほぼ一定の値となることが知られている
。磁化機構が滋壁移動による場合には、外部磁界によっ
て磁壁が移動し全体として磁化が生ずるが、一般に多結
晶体では、多結晶粒の結晶軸方向、すなわち磁化容易軸
方向が等方的に配列するために、単結晶に比べ磁壁移動
が容易ではない。このような多結晶体の本質的な欠点を
改善するため、従来は反焼粉をスピネル型単相とはせず
、禾反応物を残すことによって粉の活性を高め、暁縞に
おいて各結晶粒の結晶軸向がある程度揃うように結晶粒
成長させ、それによって磁壁移動を容易にし、初透磁率
を高める方法が探られていた。しかし、この方法によっ
て得られたNi−Znフェライトにおいては、磁壁が安
定に存在し得る位置、すなわちポテンシャル極小の位置
が均一に分布していないため、磁気的に不安定である。
そのため、例えば磁気ヘッド製造におけるボンディング
加工の際等、キュリー湿度以上に熱した場合、あるいは
何らかの原因で磁化された場合などには初透磁率が変化
する可能性が強い。本発明の方法では、このような欠点
を改良するために通常の焼緒では困難とされていた活性
の低いスピネル型単相の仮焼粉を用いた場合の高密度化
が、熱間静水圧プレスによって達成され、更にこの仮焼
粉の特長を生かすことにより、磁気的にあるいは結晶組
織の点でも非常に均一な競結体が得られる。Therefore, the magnitude of the initial magnetic permeability is determined by the difficulty of domain wall movement, but in this case, the factors that hinder domain wall movement are:
Examples include crystal anisotropy inherent to the substance, vacancies, and grain boundaries. Among these, the crystal anisotropy is determined by the composition, and after hot isostatic pressing (mP), the pores are also extremely reduced, resulting in a sintered material with a density close to the theoretical density. The effect of vacancies is also thought to be small because a large body is obtained. Therefore, when the compositions of such high-density Ni-Zn ferrites are the same, it can be considered that the main factor that influences the initial magnetic permeability is the grain boundary. The initial magnetic permeability (particularly the initial magnetic permeability in the frequency band where domain wall motion is considered to be king) is greatly influenced by the crystal grain size, that is, the number of grain boundaries, and even in Ni-Zn ferrite, the crystal grain size generally It is known that the smaller the particle size, the lower the initial magnetic permeability, and the larger the particle size, the higher the initial magnetic permeability. However, it is known that when the particle size is several microns or more, the initial magnetic permeability remains almost constant. When the magnetization mechanism is based on wall movement, the external magnetic field moves the domain walls and magnetization occurs as a whole, but generally in polycrystalline materials, the crystal axes of the polycrystalline grains, that is, the easy axis of magnetization, are arranged isotropically. Therefore, domain wall movement is not easy compared to single crystals. In order to improve the inherent disadvantages of polycrystals, conventional anti-sintering powder was not made into a spinel-type single phase, but the activity of the powder was increased by leaving the heat reactants, and each crystal grain in the dawn stripe was Researchers have been searching for ways to grow crystal grains so that their crystal axes are aligned to some extent, thereby facilitating domain wall movement and increasing initial magnetic permeability. However, the Ni-Zn ferrite obtained by this method is magnetically unstable because the positions where domain walls can stably exist, that is, the positions of potential minimum are not uniformly distributed.
Therefore, there is a strong possibility that the initial magnetic permeability will change if the material is heated above the Curie humidity, such as during bonding processing in the manufacture of a magnetic head, or if it is magnetized for some reason. In the method of the present invention, in order to improve these drawbacks, high density can be achieved by using spinel-type single-phase calcined powder with low activity, which has been considered difficult with normal calcining powder, by applying hot isostatic pressure. This is achieved by pressing, and by taking advantage of the features of this calcined powder, a competitive compact can be obtained that is extremely uniform both magnetically and in terms of crystal structure.
この方法で得られるNi−Znフェライトにおいては、
各結晶粒の結晶軸方向が等方的に分布しているため、主
に結晶粒界で磁壁移動が止められ、それによって初透磁
率の大きさが決まるが、この場合、ポテンシャル極小の
位置が均一に分布しているため、磁気的に非常に安定で
あり、高周波特性も優れている。また、この方法によれ
ば結晶軸方向が等方的に分布した良好な多結晶体が得ら
れるため、強度の均一性においても優れ、精密な加工を
行なう際に有利である。本発明は上記の事実に基づいて
なされたもので、以下に実施例を挙げて詳細に説明する
。実施例 1
いずれも配合組成がNi018.0モル%、Zn032
.5モル%およびFe20349.5モル%から成る2
種の試料A,,B,を作成した。In the Ni-Zn ferrite obtained by this method,
Since the crystal axis direction of each crystal grain is isotropically distributed, domain wall movement is mainly stopped at the grain boundaries, which determines the initial magnetic permeability. In this case, the position of the potential minimum is Because it is uniformly distributed, it is magnetically very stable and has excellent high frequency characteristics. Furthermore, according to this method, a good polycrystalline body with an isotropic distribution of crystal axis directions can be obtained, so that it has excellent uniformity of strength and is advantageous when performing precision processing. The present invention has been made based on the above facts, and will be described in detail below with reference to Examples. Example 1 In both cases, the blending composition is Ni018.0 mol%, Zn032
.. 2 consisting of 5 mol% and Fe20349.5 mol%
Seed samples A, B, were prepared.
試料A,は仮焼を130000で行ない、スピネル型単
相とした仮暁粉を用いた本発明方法により作成した試料
であり、試料Bは仮隣を90000で行ない、スピネル
相以外の相を含む仮焼粉を用いた従来技術による試料で
ある。いずれの試料も粉砕、成形後1240ooで−次
焼結を行なった後、1200oo、100ぴ気圧の条件
で熱間静水圧プレスを行ない、得られた高密度暁結体を
100000で焼鈍したものであり、理論密度の99.
8%の暁結密度を有する。第1図はA,,Bの初透磁率
の周波数依存性を表わしており、低周波においてはBの
初透磁率がA,のそれよりもわずかに高いが、高周波特
性はA,の方がはるかに優れている。Sample A is a sample prepared by the method of the present invention using a false soybean powder that was calcined at 130,000 C and made into a spinel-type single phase, and sample B was calcined at 90,000 C and contains a phase other than the spinel phase. This is a sample made using a conventional technique using calcined powder. After pulverization and molding, all samples were subjected to secondary sintering at 1240 oo, followed by hot isostatic pressing at 1200 oo and 100 pia, and the resulting high-density compacts were annealed at 100,000. Yes, the theoretical density is 99.
It has a dawn compaction density of 8%. Figure 1 shows the frequency dependence of the initial permeability of A, B. At low frequencies, the initial permeability of B is slightly higher than that of A, but the high frequency characteristics of A are better. much better.
また、熱消磁による初透磁率の変化を第1表に示すが、
これは各温度で10分間保持後冷却し、20o0で0.
9MHzにおける初透磁率を測定した結果である。なお
、キュリー温度はA,,B,とも13500である。A
,では熱消磁による影響がほとんど見られず、本発明の
効果が大きいが、B.においてはキュリー温度以下でも
熱消磁の影響が現われ始め、キコ.リー温度以上ではそ
の変化が更に大きくなる。熱消磁よによってB,の初透
磁率は低周波で増大するが、その反対に高周波特性が悪
くなりA,との差は更に大きくなる。このようにB,に
おいては、初透磁率が熱の影響で大きく変化し、高周波
特性も劣化するが、それに対して、スピネル型単相の仮
焼粉を用いたA,は均一性が高いため、熱による初透磁
率の変化がほとんどなく安定で、しかも高周波特性が優
れており、本発明の効果が顕著に現われている。第1表
実施例 0
第2表は、配合組成がいずれもNi020モル%、Zn
030モル%およびFe20350モル%である焼結体
ん,&の熱による初透磁率変化を実施例1と同様の方法
で測定した結果である。Table 1 shows the change in initial permeability due to thermal demagnetization.
This was held at each temperature for 10 minutes and then cooled to 0.
These are the results of measuring the initial magnetic permeability at 9 MHz. Note that the Curie temperature of both A and B is 13500. A
, there is almost no effect of thermal demagnetization, and the effect of the present invention is large, but in B. The effects of thermal demagnetization begin to appear even below the Curie temperature, and Kiko. Above the Lee temperature, the change becomes even larger. Due to thermal demagnetization, the initial magnetic permeability of B increases at low frequencies, but on the contrary, the high frequency characteristics deteriorate and the difference with A becomes even larger. In this way, in B, the initial magnetic permeability changes greatly due to the influence of heat, and the high frequency characteristics also deteriorate, but in contrast, A, which uses spinel-type single-phase calcined powder, has high uniformity. , it is stable with almost no change in initial magnetic permeability due to heat, and has excellent high frequency characteristics, demonstrating the effects of the present invention. Table 1 Example 0 Table 2 shows that the compositions are Ni020 mol%, Zn
These are the results of measuring the initial magnetic permeability change due to heat in a sintered body containing 0.030 mol% and Fe20350 mol% using the same method as in Example 1.
A2,&はそれぞれ実施例1のA,,B,と同様の仮焼
および一次競結を行なった後、110000、100ぴ
気圧の条件で熱間静水圧プレスを行ない、1000oo
で熱処理して得られた焼結体であり、いずれも約99.
7%の相対焼結密度を有し、キュリー温度は約190o
oである。実施例1と同様に、スピネル型単相の仮焼粉
を用いたA2においては、熱による初透磁率の変化がほ
とんど見られず、高周波特性も優れており、本発明の効
果は明白である。実施例1,Dから明らかなように、本
発明の方法によって得られた焼結体は、熱による磁気特
性の変化がほとんどなく非常に安定であり、かつ高周波
特性も優れている。A2 and & are respectively subjected to calcination and primary binding in the same manner as A, B of Example 1, and then subjected to hot isostatic pressing under the conditions of 110,000 and 100 p atm to obtain 1,000 oo
These are sintered bodies obtained by heat treatment at a temperature of about 99.
It has a relative sintered density of 7% and a Curie temperature of about 190o
It is o. Similar to Example 1, in A2 using spinel-type single-phase calcined powder, almost no change in initial magnetic permeability due to heat was observed, and the high frequency characteristics were also excellent, so the effects of the present invention are obvious. . As is clear from Examples 1 and D, the sintered body obtained by the method of the present invention is very stable with almost no change in magnetic properties due to heat, and also has excellent high frequency properties.
また、結晶組織が均一であるため、精密加工が容易であ
るなど、工業的に見てもその果は非常に大なるものがあ
り、本発明の磁○材料を磁気ヘッドに応用すれば大幅な
性能改善が期待される。In addition, since the crystal structure is uniform, precision machining is easy, and from an industrial perspective, the results are very significant.If the magnetic material of the present invention is applied to magnetic heads, it will be greatly improved. Expected to improve performance.
【図面の簡単な説明】
第1図は本発明により作成した試料A,と従来方法によ
り作成したB,の初透磁率の周波数依存性を表わす特性
曲線図である。
第2表
オ′図BRIEF DESCRIPTION OF THE DRAWINGS FIG. 1 is a characteristic curve diagram showing the frequency dependence of the initial magnetic permeability of sample A prepared according to the present invention and sample B prepared according to the conventional method. Table 2 Diagram
Claims (1)
してオープンポアー(試料表面から中心部まで通じる空
孔)を消滅させる程度にまで一次焼結を行なう工程と、
前記一次焼結後のフエライト材を熱間静水圧プレスする
工程と、前記熱間静水圧プレス後のフエライト材を適当
な条件下で焼鈍する各工程とから成るNi−Znフエラ
イトの製造方法において、上記仮焼工程において、スピ
ネル型単相のの仮焼粉を生成せしめることを特徴とする
Ni−Znフエライトの製造方法。1. A step of calcining at least the raw material, and a step of sintering the calcined powder to perform primary sintering to the extent that open pores (pores communicating from the surface of the sample to the center) are eliminated;
A method for producing Ni-Zn ferrite, which comprises the steps of hot isostatic pressing the ferrite material after the primary sintering, and annealing the ferrite material after the hot isostatic pressing under appropriate conditions, A method for producing Ni--Zn ferrite, characterized in that in the calcination step, a spinel-type single-phase calcined powder is produced.
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP51146475A JPS6029204B2 (en) | 1976-12-08 | 1976-12-08 | Manufacturing method of high-density Ni-Zn ferrite |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP51146475A JPS6029204B2 (en) | 1976-12-08 | 1976-12-08 | Manufacturing method of high-density Ni-Zn ferrite |
Publications (2)
| Publication Number | Publication Date |
|---|---|
| JPS5371299A JPS5371299A (en) | 1978-06-24 |
| JPS6029204B2 true JPS6029204B2 (en) | 1985-07-09 |
Family
ID=15408471
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP51146475A Expired JPS6029204B2 (en) | 1976-12-08 | 1976-12-08 | Manufacturing method of high-density Ni-Zn ferrite |
Country Status (1)
| Country | Link |
|---|---|
| JP (1) | JPS6029204B2 (en) |
Families Citing this family (1)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| JPS61111512A (en) * | 1984-11-06 | 1986-05-29 | Sumitomo Special Metals Co Ltd | Ni-zn ferrite for thin film head substrate |
-
1976
- 1976-12-08 JP JP51146475A patent/JPS6029204B2/en not_active Expired
Also Published As
| Publication number | Publication date |
|---|---|
| JPS5371299A (en) | 1978-06-24 |
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