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JP2008162847A - Magnetic oxide material - Google Patents

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JP2008162847A
JP2008162847A JP2006354241A JP2006354241A JP2008162847A JP 2008162847 A JP2008162847 A JP 2008162847A JP 2006354241 A JP2006354241 A JP 2006354241A JP 2006354241 A JP2006354241 A JP 2006354241A JP 2008162847 A JP2008162847 A JP 2008162847A
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core loss
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Rei Hanamura
玲 花村
Yoshio Matsuo
良夫 松尾
Kiyoto Ono
清人 小野
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FDK Corp
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Abstract

【課題】 高温域に達して初透磁率の変動を小さくでき、コア損失を低値にできて100℃以上の高温でも十分な磁気特性を確保でき、表面抵抗を高く得ることができ、高電圧が加わる用途のコア材料等へ好ましく適用できる酸化物磁性材料を提供すること
【解決手段】 主成分はFeが47.2〜49.2モル%,ZnOが25〜30モル%,CuOが3〜10モル%,MnOが0.2〜2.8モル%であり残部をNiOとし、(Fe+MnO)の換算で49.4〜50.0モル%含有する組成にする。これによる焼結体は、混合した各材料の特質を相互に作用させたものとなり、材質特性は、周波数60kHz,飽和磁束密度100mT,温度60℃でのコア損失が200kW/m以下となり、コア損失が最小値を示す温度が100℃以上となる。Fe成分量が49.2モル%以下なので、表面抵抗は10〔GΩ〕以上と高く得ることができる。
【選択図】なし
PROBLEM TO BE SOLVED: To achieve a high temperature range, to reduce the fluctuation of the initial magnetic permeability, to reduce the core loss to a low value, to ensure sufficient magnetic properties even at a high temperature of 100 ° C. or higher, to obtain a high surface resistance, and to achieve a high voltage It is added the a main component to provide an oxide magnetic material core can preferably be applied to materials such applications Fe 2 O 3 47.2~49.2 mol%, ZnO is 25 to 30 mol%, CuO Is 3 to 10 mol%, MnO is 0.2 to 2.8 mol%, the balance is NiO, and the composition is 49.4 to 50.0 mol% in terms of (Fe 2 O 3 + MnO). The sintered body thus obtained has the characteristics of the mixed materials interacting with each other. The material characteristics are such that the core loss at a frequency of 60 kHz, a saturation magnetic flux density of 100 mT, and a temperature of 60 ° C. is 200 kW / m 3 or less. The temperature at which the loss reaches a minimum value is 100 ° C. or higher. Since the Fe component amount is 49.2 mol% or less, the surface resistance can be as high as 10 [GΩ] or more.
[Selection figure] None

Description

本発明は、MnNiCuZn系の酸化物磁性材料に関するもので、より具体的には、液晶バックライトのインバータトランス等のコア材料に適用するためコア損失を低減するようにしたものにおける温度依存性の改良に関する。   The present invention relates to an MnNiCuZn-based oxide magnetic material, and more specifically, an improvement in temperature dependency in a core loss material that is applied to a core material such as an inverter transformer of a liquid crystal backlight. About.

トランスやコイル等のコア材料に用いられる酸化物磁性材料としては、Mn−Zn系フェライトやNi−Zn系フェライトがよく知られている。   As oxide magnetic materials used for core materials such as transformers and coils, Mn—Zn ferrite and Ni—Zn ferrite are well known.

Mn−Zn系フェライトは、コア損失が小さく飽和磁束密度が高いことから、スイッチング電源などのコア材料に好んで使われている。しかし、Mn−Zn系フェライトは、固有抵抗が低いため直接に巻き線を施すことができず、絶縁のためボビン等を介在させる構成になり小型化が困難であるという欠点がある。   Mn—Zn-based ferrite is favorably used as a core material for switching power supplies and the like because of its low core loss and high saturation magnetic flux density. However, Mn—Zn ferrite cannot be directly wound because of its low specific resistance, and has a drawback that it is difficult to reduce the size because it has a configuration in which a bobbin or the like is interposed for insulation.

Ni−Zn系フェライトは、固有抵抗が格段に高いという特徴からコアを対して直接巻き線することが可能であり、小型化に有利であるため注目がある。しかし、Ni−Zn系フェライトはコア損失が大きいという欠点があるため改善策が求められている。対策技術としては、例えば特許文献1〜6などに見られるように多くの提案があり、組成としてFe,Ni,Znの他にMn,Cuなどを適宜に含ませて調整することにより、コア損失を改善するようにしている。
特開平ll−219812号公報 特開2002−198212号公報 特開2002−289421号公報 特開2004−107158号公報 特許2551009号公報 特許3487552号公報
Ni-Zn based ferrite can be directly wound around the core because of its remarkably high specific resistance, and is therefore attractive for downsizing. However, since Ni-Zn ferrite has a drawback of large core loss, an improvement measure is required. As countermeasure techniques, there are many proposals as seen in, for example, Patent Documents 1 to 6, and the core loss is adjusted by appropriately including Mn, Cu, etc. in addition to Fe, Ni, Zn as a composition. To improve.
Japanese Laid-Open Patent Publication No. 11-211981 JP 2002-198212 A JP 2002-289421 A JP 2004-107158 A Japanese Patent No. 2551009 Japanese Patent No. 3487552

ところで、液晶バックライトのインバータトランス等の用途では、小型化,高効率化の要求から高周波数,高電圧の駆動を採り、コア材料に対して例えば1000V以上の高電圧が加わる仕様になってきている。このため、コア材料は高い絶縁特性が求められるとともに、発熱が大きくなるため温度特性が重要となり、高温でもコア損失が小さく、高温域に達して初透磁率の変動が小さい特性が求められる。   By the way, in applications such as inverter transformers for liquid crystal backlights, high-frequency and high-voltage driving has been adopted due to demands for miniaturization and high efficiency, and a high voltage of, for example, 1000 V or more is applied to the core material. Yes. For this reason, the core material is required to have high insulation characteristics, temperature characteristics are important because heat generation is large, core loss is required to be small even at high temperatures, and characteristics in which fluctuations in initial permeability are small after reaching a high temperature range are required.

また、高電圧が加わる用途では、コア材料の表面で短絡による放電を起こす問題がある。つまり、Ni−Zn系フェライトは固有抵抗が高いという特質を有するが、焼成において表面はZnやCuなどの元素が蒸発等により飛散し、表面領域での組成がわずかに変化を起こし、相対的にFe量が増すことになる。そしてFe量(Fe)が50モル%を越える状況では、2価から3価に変わる際の電子移動のために抵抗値が著しく低減する現象を起こし、電気抵抗が極端に低下する。電気抵抗が低下する表面膜層は数10から数100μmの厚みとなり、コア材料の全体からはわずかな領域であるが、1000V以上の高電圧が加わる場合は短絡を起こしてしまう。 Further, in applications where high voltage is applied, there is a problem of causing discharge due to a short circuit on the surface of the core material. In other words, Ni-Zn ferrite has a characteristic of high specific resistance, but in the firing, elements such as Zn and Cu are scattered by evaporation or the like, and the composition in the surface region slightly changes, and relatively The amount of Fe will increase. In a situation where the amount of Fe (Fe 2 O 3 ) exceeds 50 mol%, a phenomenon in which the resistance value is remarkably reduced due to the electron transfer when changing from divalent to trivalent occurs, and the electric resistance is extremely reduced. The surface film layer in which the electric resistance is reduced has a thickness of several tens to several hundreds of μm, and is a small region from the whole core material. However, when a high voltage of 1000 V or more is applied, a short circuit occurs.

この発明は上述した課題を解決するもので、その目的は、高温域に達して初透磁率の変動を小さくすることができ、コア損失を低値にできて100℃以上の高温でも十分な磁気特性を確保することができ、表面抵抗を高く得ることができ、高電圧が加わる用途のコア材料等へ好ましく適用できる酸化物磁性材料を提供することにある。   The object of the present invention is to solve the above-mentioned problems. The object of the present invention is to reach a high temperature range to reduce the fluctuation of the initial magnetic permeability, to reduce the core loss to a low value, and to achieve sufficient magnetism even at a high temperature of 100 ° C. or higher. An object of the present invention is to provide an oxide magnetic material that can secure characteristics, obtain a high surface resistance, and can be preferably applied to a core material or the like for applications where high voltage is applied.

上述した目的を達成するために、本発明に係る酸化物磁性材料は、MnNiCuZn系の酸化物磁性材料であって、主成分は
酸化第二鉄(Fe)が47.2〜49.2モル%,
酸化亜鉛(ZnO)が25〜30モル%,
酸化銅(CuO)が3〜10モル%,
酸化マンガン(MnO)が0.2〜2.8モル%であり
残部を酸化ニッケル(NiO)とし、
酸化第二鉄と酸化マンガンとをFe+MnOの換算で
49.4モル% ≦ (Fe+MnO)≦ 50.0モル%
含有する組成とする。
In order to achieve the above-described object, the oxide magnetic material according to the present invention is an MnNiCuZn-based oxide magnetic material, the main component of which is 47.2 to 49.ferric oxide (Fe 2 O 3 ). 2 mol%,
Zinc oxide (ZnO) is 25-30 mol%,
3-10 mol% copper oxide (CuO),
Manganese oxide (MnO) is 0.2 to 2.8 mol% and the balance is nickel oxide (NiO),
Ferric oxide and manganese oxide in terms of Fe 2 O 3 + MnO 49.4 mol% ≦ (Fe 2 O 3 + MnO) ≦ 50.0 mol%
It is set as the composition to contain.

また、上記組成による焼結体は平均結晶粒子径を8〜20μmとし、周波数60kHz,飽和磁束密度100mT,温度600℃でのコア損失が200kW/m以下であり、コア損失が最小値を示す温度が100℃以上であり、初透磁率の相対温度係数(αμir )は温度範囲25℃から130℃において20×10−6 以下であるものとする。 The sintered body having the above composition has an average crystal particle diameter of 8 to 20 μm, a core loss of 200 kW / m 3 or less at a frequency of 60 kHz, a saturation magnetic flux density of 100 mT, and a temperature of 600 ° C. The temperature is 100 ° C. or higher, and the relative temperature coefficient (αμir) of the initial permeability is 20 × 10 −6 or lower in the temperature range of 25 ° C. to 130 ° C.

このように、最小値が100℃以上となる温度−コア損失特性は、下に凸の負の温度特性を持つことになり、室温(或いはそれ以下)から温度が上昇する(最小値の温度まで)につれて損失が低下するという特性を持ち、使用に伴う発熱を生じた場合にコア損失が低下することになる。   As described above, the temperature-core loss characteristic at which the minimum value is 100 ° C. or more has a negative convex temperature characteristic, and the temperature rises from room temperature (or lower) (up to the minimum temperature). ) Has a characteristic that the loss is reduced, and the core loss is reduced when heat is generated due to use.

本発明では、Fe,ZnO,CuO,MnO,NiOおよび(Fe+MnO)を上述した所定の配合比とすることにより、得られた焼結体は、高温でのコア損失が小さくなり、広い温度範囲において初透磁率の変動が小さくなる。上述した本発明に係る組成は実験から見いだした結果であり、焼結体の材質特性は、周波数60kHz,飽和磁束密度100mT,温度600℃でのコア損失が200kW/m以下であり、コア損失が最小値を示す温度が100℃以上であり、初透磁率の相対温度係数(αμir )は温度範囲25℃から130℃において20×10−6 以下であることを確認した。 In the present invention, by setting Fe 2 O 3 , ZnO, CuO, MnO, NiO and (Fe 2 O 3 + MnO) to the above-described predetermined mixing ratio, the obtained sintered body has a core loss at a high temperature. It becomes smaller, and the fluctuation of the initial permeability becomes smaller in a wide temperature range. The composition according to the present invention described above is the result of an experiment, and the material characteristics of the sintered body are as follows: the core loss at a frequency of 60 kHz, a saturation magnetic flux density of 100 mT, and a temperature of 600 ° C. is 200 kW / m 3 or less. Was 100 ° C. or higher, and the relative temperature coefficient (αμir) of the initial permeability was 20 × 10 −6 or lower in the temperature range of 25 ° C. to 130 ° C.

この場合、コア損失が最小値を示す温度が100℃以上になるので、発熱に伴って悪化するコア損失について余裕があり、高周波数,高電圧の駆動を行うスイッチング電源のコア材料として好ましいと言える。   In this case, since the temperature at which the core loss reaches a minimum value is 100 ° C. or more, there is a margin for the core loss that deteriorates with heat generation, and it can be said that it is preferable as a core material for a switching power supply that drives at high frequency and high voltage. .

また、Feの配合が49.2モル%以下となるので、焼成時に表面でCuやZnの蒸発,移動が起きて表面領域において組成が変化したとしても、当該表面領域についてFeが相対的に50モル%を越える事態は起こし難くなり、表面抵抗を高く得ることができる。 In addition, since the Fe 2 O 3 content is 49.2 mol% or less, even if Cu or Zn evaporates or moves on the surface during firing and the composition changes in the surface region, the Fe 2 O content in the surface region is reduced. The situation in which 3 exceeds 50 mol% is less likely to occur, and a high surface resistance can be obtained.

Fe+MnOの換算で49.4モル% ≦ (Fe+MnO)≦ 50.0モル%、つまり、50モル%近くが損失が小さく、最小値が100℃以上にすることができる。 In terms of Fe 2 O 3 + MnO, 49.4 mol% ≦ (Fe 2 O 3 + MnO) ≦ 50.0 mol%, that is, near 50 mol%, the loss is small, and the minimum value can be 100 ° C. or more. .

本発明に係る酸化物磁性材料では、主成分はFeが47.2〜49.2モル%,ZnOが25〜30モル%,CuOが3〜10モル%,MnOが0.2〜2.8モル%であり残部をNiOとし、(Fe+MnO)の換算で49.4〜50.0モル%含有する組成とするので、これによる焼結体(酸化物磁性材料)は、混合した各材料の特質を相互に作用させたものとなる。 The oxide magnetic material according to the present invention, the main component is Fe 2 O 3 is from 47.2 to 49.2 mol%, ZnO is 25 to 30 mol%, CuO is from 3 to 10 mol%, 0.2 is MnO Since the composition is 2.8 mol%, the balance is NiO, and 49.4 to 50.0 mol% in terms of (Fe 2 O 3 + MnO), the sintered body (oxide magnetic material) is The characteristics of the mixed materials interact with each other.

焼結体の材質特性は、周波数60kHz,飽和磁束密度100mT,温度60℃でのコア損失が200kW/m以下となり、コア損失が最小値を示す温度が100℃以上となる。すなわち本発明に係る焼結体にあっては、高温域に達して初透磁率の変動を小さくすることができ、コア損失を低値にできて100℃以上の高温でも十分な磁気特性を確保することができる。 As for the material properties of the sintered body, the core loss at a frequency of 60 kHz, a saturation magnetic flux density of 100 mT, and a temperature of 60 ° C. is 200 kW / m 3 or less, and the temperature at which the core loss shows a minimum value is 100 ° C. or more. That is, in the sintered body according to the present invention, the fluctuation of the initial permeability can be reduced by reaching the high temperature range, the core loss can be lowered, and sufficient magnetic properties are ensured even at a high temperature of 100 ° C. or higher. can do.

また、Feの配合が49.2モル%以下となるので、表面領域についてFeが相対的に50モル%を越える事態は起こし難くなり、表面抵抗を高く得ることができる。表面抵抗は実施例に示すように、10〔GΩ〕以上には十分に高く得ることができ、したがって、1000V以上の高電圧が加わる場合でも短絡,放電を防止でき、高電圧が加わる用途のコア材料等へ好ましく適用できる。 Also, since the blending of Fe 2 O 3 is less than 49.2 mol%, a situation in which the surface area is Fe 2 O 3 exceeds a relatively 50 mol% hardly caused, can be obtained a high surface resistance. As shown in the examples, the surface resistance can be sufficiently high above 10 [GΩ], and therefore, even when a high voltage of 1000 V or higher is applied, a short circuit and discharge can be prevented, and a core for applications where a high voltage is applied. It can be preferably applied to materials and the like.

以下、本発明の好適な実施の形態について説明する。   Hereinafter, preferred embodiments of the present invention will be described.

本発明に係る酸化物磁性材料は、酸化第二鉄(Fe2O3),酸化亜鉛(ZnO),酸化銅(CuO),酸化ニッケル(NiO)等を主成分とし、いわゆるMnNiCuZn系フェライトの組成になっている。具体的には、主成分は
酸化第二鉄(Fe)が47.2〜49.2モル%,
酸化亜鉛(ZnO)が25〜30モル%,
酸化銅(CuO)が3〜10モル%,
酸化マンガン(MnO)が0.2〜2.8モル%であり
残部を酸化ニッケル(NiO)とし、
酸化第二鉄と酸化マンガンとをFe+MnOの換算で
49.4モル% ≦ (Fe+MnO)≦ 50.0モル%
含有する組成とする。
The oxide magnetic material according to the present invention is composed mainly of ferric oxide (Fe2O3), zinc oxide (ZnO), copper oxide (CuO), nickel oxide (NiO), etc., and has a composition of so-called MnNiCuZn ferrite. Yes. Specifically, the main component is 47.2 to 49.2 mol% of ferric oxide (Fe 2 O 3 ),
Zinc oxide (ZnO) is 25-30 mol%,
3-10 mol% copper oxide (CuO),
Manganese oxide (MnO) is 0.2 to 2.8 mol% and the balance is nickel oxide (NiO),
Ferric oxide and manganese oxide in terms of Fe 2 O 3 + MnO 49.4 mol% ≦ (Fe 2 O 3 + MnO) ≦ 50.0 mol%
It is set as the composition to contain.

製造には、まず上述した各原料成分を所定量秤量して湿式混合する。例えばボールミルで粉砕しつつ混ぜて混合紛体を製造し、これを乾燥させて解砕し、次に仮焼きする。仮焼きは、例えば電気炉を使用して大気中で温度を850℃程度とする。   For production, first, a predetermined amount of each of the above-mentioned raw material components is weighed and wet mixed. For example, a mixed powder is manufactured by pulverizing with a ball mill, dried, crushed, and then calcined. In the calcining, for example, an electric furnace is used and the temperature is set to about 850 ° C. in the atmosphere.

仮焼きすることでは粒成長するので、次にアトマイザ等によりそれを再び湿式粉砕する。これを乾燥させて解砕し、この粉体にボリビニルアルコール(PVA)を加えてスラリを形成し、スプレードライにより造粒して所定粒径の粉体を得る。   Since the grains grow when calcined, it is wet-pulverized again by an atomizer or the like. This is dried and crushed. Polyvinyl alcohol (PVA) is added to the powder to form a slurry, which is granulated by spray drying to obtain a powder having a predetermined particle diameter.

次に、造粒した紛体に成形のための圧力を加えて、例えばリング形状に成形し、この後、ガス炉等で焼成を行う。焼成は、例えば大気中で温度を1000〜1200℃とし、所定時間(例えば2時間)の焼成により焼結体を製造する。得られた焼結体にバレル研磨等の仕上げ加工を施し、形状,寸法を所定に加工した酸化物磁性材料を得る。   Next, pressure for molding is applied to the granulated powder to form, for example, a ring shape, and then firing is performed in a gas furnace or the like. Firing is performed at a temperature of 1000 to 1200 ° C. in the atmosphere, for example, and a sintered body is produced by firing for a predetermined time (for example, 2 hours). The obtained sintered body is subjected to finish processing such as barrel polishing to obtain an oxide magnetic material having a predetermined shape and size.

この焼結体は、平均結晶粒子径が8〜20μmとなるように製造しており、これは、焼成条件の最適化などにより実現している。   This sintered body is manufactured to have an average crystal particle diameter of 8 to 20 μm, which is realized by optimizing the firing conditions.

ZnOの配合は、25モル%以下ではコア損失が大きくなり、30モルを超えるとキュリー温度(Tc)が低下してしまい、発熱時に十分な安全性を確保できなくなる。そこで、ZnOの配合は25〜30モル%としてあり、この範囲であればコア損失を小さくでき、キュリー温度を高く得ることができる。   When ZnO is blended in an amount of 25 mol% or less, the core loss increases, and when it exceeds 30 mol, the Curie temperature (Tc) decreases, and sufficient safety cannot be secured during heat generation. Therefore, the ZnO content is 25 to 30 mol%, and in this range, the core loss can be reduced and the Curie temperature can be increased.

CuOの配合は、3モル%以下では焼結が進まなくなり、焼成を高温で行う必要がでてきて現実的ではなく、10モル%以上ではコア損失が悪化してしまう。そこで、CuOの配合は3〜10モル%としてあり、比較的に低温度で焼成を適正に行うことができ、所定の焼結密度が得られてコア損失を小さくできる。   When the CuO content is 3 mol% or less, sintering does not proceed, and it is necessary to perform firing at a high temperature, which is not practical. If it is 10 mol% or more, the core loss is deteriorated. Therefore, the CuO content is 3 to 10 mol%, and firing can be appropriately performed at a relatively low temperature, a predetermined sintered density can be obtained, and the core loss can be reduced.

Feの配合は、増加に伴って初透磁率の相対温度係数が大きくなる傾向を示す。また、Feあるいは(Fe+MnO)について、配合量が低減するとコア損失が大きくなる傾向を示し、コア損失が最小値を示す温度が100℃以下になってしまう。そこで、Feの配合は49.2モル%以下とし、酸化マンガンとの関係はFe+MnOの換算で50.0モル%以下に設定している。 The composition of Fe 2 O 3 tends to increase the relative temperature coefficient of the initial magnetic permeability as it increases. Further, the Fe 2 O 3 or (Fe 2 O 3 + MnO) , the amount is reduced tended to core loss increases, the temperature indicating the minimum core loss becomes 100 ° C. or less. Therefore, the Fe 2 O 3 content is 49.2 mol% or less, and the relationship with manganese oxide is set to 50.0 mol% or less in terms of Fe 2 O 3 + MnO.

Feの配合を49.2モル%以下とすることでは、焼成時に表面でCuやZnの蒸発,移動が起きて表面領域において組成が変化したとしても、当該表面領域についてFeが相対的に50モル%を越える事態は起こし難くなり、表面抵抗を高く得ることができる。したがって、高電圧が加わる用途において短絡を防止できる。 By setting the blending of Fe 2 O 3 to 49.2 mol% or less, even if Cu or Zn evaporates or moves on the surface during firing and the composition changes in the surface region, the Fe 2 O 3 is in the surface region. Is relatively difficult to occur, and a high surface resistance can be obtained. Therefore, a short circuit can be prevented in applications where high voltage is applied.

そして、後述する試料について磁気特性を測定した結果から、最適には、Feの配合は47.2〜49.2モル%の範囲が好ましく、(Fe+MnO)は49.4〜50.0モル%の範囲とし、MnOの配合は0.2〜2.8モル%としてある。 Then, from the result of measurement of the magnetic characteristics of the sample which will be described later, and optimally, the formulation of Fe 2 O 3 is preferably in the range of 47.2 to 49.2 mol%, (Fe 2 O 3 + MnO) is 49.4 It is made into the range of -50.0 mol%, and the compounding of MnO is 0.2-2.8 mol%.

コア損失が最小値を示す温度は、主成分の組成によりある程度決定してしまうが、コア損失は微細結晶構造に大きく依存することから、結晶構造(結晶粒子とその粒界)については製造工程における精密な制御が重要となる。つまり、焼結体は多結晶体であり、結晶粒子それぞれで組成にバラツキがあることがコア損失を悪化させる要因のひとつと言え、本発明では焼結体の平均結晶粒子径は8〜20μmとなるので、粒子径の分布が狭い範囲に集中し、その結果、コア全体が示す材質特性を所定分布に集中させて均一化でき、コア損失の改善が行える。   The temperature at which the core loss shows the minimum value is determined to some extent by the composition of the main component, but since the core loss largely depends on the fine crystal structure, the crystal structure (crystal grains and their grain boundaries) is in the manufacturing process. Precise control is important. That is, the sintered body is a polycrystalline body, and it can be said that the variation in the composition of each crystal particle is one of the factors that deteriorate the core loss. In the present invention, the average crystal particle diameter of the sintered body is 8 to 20 μm. Therefore, the particle size distribution is concentrated in a narrow range, and as a result, the material characteristics of the entire core can be concentrated and uniformed in a predetermined distribution, and the core loss can be improved.

上述した組成からなる焼結体は、材質特性が、周波数60kHz,飽和磁束密度100mT,温度60℃でのコア損失が200kW/m以下となり、コア損失が最小値を示す温度は100℃以上となり、そして初透磁率の相対温度係数(αμir )は温度範囲25℃から130℃において20×10−6 以下となるようになっている。この材質特性は、高電圧が加わる用途のコア材料として最適であり、液晶バックライトのインバータトランス等のコア材料への適用が好ましいと言える。 The sintered body having the composition described above has material properties of a core loss of 200 kW / m 3 or less at a frequency of 60 kHz, a saturation magnetic flux density of 100 mT, and a temperature of 60 ° C., and a temperature at which the core loss shows a minimum value is 100 ° C. or more. The relative temperature coefficient (αμir) of the initial magnetic permeability is 20 × 10 −6 or less in the temperature range of 25 ° C. to 130 ° C. This material property is optimal as a core material for applications where a high voltage is applied, and it can be said that application to a core material such as an inverter transformer of a liquid crystal backlight is preferable.

上述した製造手順により試料を製造した。つまり、本発明の効果を実証するため、組成を変更して複数の試料を製造し、それら各試料についてコア損失,初透磁率の相対温度係数,表面抵抗を測定した。   Samples were manufactured according to the manufacturing procedure described above. That is, in order to demonstrate the effect of the present invention, a plurality of samples were manufactured with different compositions, and the core loss, the relative temperature coefficient of initial permeability, and the surface resistance were measured for each sample.

試料は表1に示すように、組成を変更した32の試料とし、外形をリング形状のものとした。主成分の配合は、酸化第二鉄(Fe)は43.22〜49.70モル%の範囲で変更し、酸化亜鉛(ZnO)は27.50〜29.90モル%の範囲で変更し、酸化銅(CuO)は4.92〜6.10モル%の範囲で変更し、酸化マンガン(MnO)は0.00〜8.04モル%の範囲で変更し、残部となる酸化ニッケル(NiO)は15.63〜17.00モル%の範囲で変更し、そして、酸化第二鉄,酸化マンガンはFe+MnOの換算について47.0〜51.26モル%の範囲で変更し、これらの組み合わせから32個の試料を用意した。 As shown in Table 1, the samples were 32 samples with different compositions, and the outer shape was a ring shape. The composition of the main component is changed in the range of 43.22 to 49.70 mol% for ferric oxide (Fe 2 O 3 ), and in the range of 27.50 to 29.90 mol% for zinc oxide. The copper oxide (CuO) is changed in the range of 4.92 to 6.10 mol%, the manganese oxide (MnO) is changed in the range of 0.00 to 8.04 mol%, and the remaining nickel oxide (NiO) is changed in the range of 15.63 to 17.00 mol%, and ferric oxide and manganese oxide are changed in the range of 47.0 to 51.26 mol% in terms of Fe 2 O 3 + MnO. And 32 samples were prepared from these combinations.

また、これら各組成による焼結体は、平均結晶粒子径が8〜20μmとなるように製造しており、これは焼成条件の最適化などにより実現した。   Moreover, the sintered compact by these each composition was manufactured so that an average crystal particle diameter might be set to 8-20 micrometers, and this was implement | achieved by optimization of baking conditions.

表に示した各試料は、いずれも本発明(請求項1に係る発明)に含まれるものである。そして、表における実施例は請求項3に係る発明に対応するものであり、比較例は本発明に対応するものの請求項3に係る発明の要件を満たさないものである。

Figure 2008162847
Figure 2008162847
Each sample shown in the table is included in the present invention (the invention according to claim 1). And the Example in a table | surface respond | corresponds to the invention which concerns on Claim 3, and a comparative example does not satisfy the requirements of the invention which concerns on Claim 3 although it respond | corresponds to this invention.
Figure 2008162847
Figure 2008162847

コア損失の測定にはB−Hアナライザを使用し、周波数60kHz,飽和磁束密度100mTにおいて常温25℃から高温140℃の範囲について測定を行った。初透磁率の相対温度係数の測定にはインピーダンスアナライザを使用し、周波数100kHz,電流0.01Aにおいて初透磁率の温度特性を測定した。表面抵抗の測定にはオームメータを使用し、電極間の距離20mm,電圧500Vの条件により測定を行った。   The BH analyzer was used to measure the core loss, and the measurement was performed in the range from room temperature 25 ° C. to high temperature 140 ° C. at a frequency of 60 kHz and a saturation magnetic flux density of 100 mT. An impedance analyzer was used to measure the relative temperature coefficient of the initial permeability, and the temperature characteristics of the initial permeability were measured at a frequency of 100 kHz and a current of 0.01 A. The surface resistance was measured using an ohmmeter under the conditions of a distance between electrodes of 20 mm and a voltage of 500V.

各試料についてコア損失,初透磁率の相対温度係数,表面抵抗を測定したところ、表1に示す測定結果から明らかなように、各原料成分の特質を相互に作用させて好適な磁気特性を発現させるには、各成分の組成を本発明に係る所定範囲とすることが好ましい。すなわち、主成分が
酸化第二鉄(Fe)が47.2〜49.2モル%,
酸化亜鉛(ZnO)が25〜30モル%,
酸化銅(CuO)が3〜10モル%,
酸化マンガン(MnO)が0.2〜2.8モル%であり
残部を酸化ニッケル(NiO)とし、
酸化第二鉄と酸化マンガンとをFe+MnOの換算で
49.4モル% ≦ (Fe+MnO)≦ 50.0モル%
含有する組成のものでは、表面抵抗を10〔GΩ〕以上に十分に高く得ることができることを確認した。したがって、1000V以上の高電圧が加わる場合でも短絡,放電を防止でき、高電圧が加わる用途のコア材料等へ好ましく適用できる。
The core loss, relative temperature coefficient of initial permeability, and surface resistance of each sample were measured. As is apparent from the measurement results shown in Table 1, the characteristics of each raw material component interacted with each other to produce suitable magnetic properties. In order to achieve this, it is preferable that the composition of each component is within a predetermined range according to the present invention. That is, the main component is 47.2 to 49.2 mol% of ferric oxide (Fe 2 O 3 ),
Zinc oxide (ZnO) is 25 to 30 mol%,
3-10 mol% copper oxide (CuO),
Manganese oxide (MnO) is 0.2 to 2.8 mol% and the balance is nickel oxide (NiO),
Ferric oxide and manganese oxide in terms of Fe 2 O 3 + MnO 49.4 mol% ≦ (Fe 2 O 3 + MnO) ≦ 50.0 mol%
It was confirmed that the composition having the composition can obtain a surface resistance sufficiently high to 10 [GΩ] or more. Therefore, even when a high voltage of 1000 V or more is applied, short circuit and discharge can be prevented, and it can be preferably applied to a core material or the like for applications where a high voltage is applied.

更に、表1に示す実施例1〜6では、周波数60kHz,飽和磁束密度100mT,温度60℃でのコア損失が200kW/m以下となり、コア損失が最小値を示す温度が100℃以上となり、初透磁率の相対温度係数(αμir )は温度範囲25℃から130℃において20×10−6 以下となる材質特性が得られることを確認した。 Furthermore, in Examples 1 to 6 shown in Table 1, the core loss at a frequency of 60 kHz, a saturation magnetic flux density of 100 mT, and a temperature of 60 ° C. is 200 kW / m 3 or less, and the temperature at which the core loss shows a minimum value is 100 ° C. or more. It was confirmed that a material characteristic having a relative temperature coefficient (αμir) of initial permeability of 20 × 10 −6 or less was obtained in a temperature range of 25 ° C. to 130 ° C.

Claims (3)

MnNiCuZn系の酸化物磁性材料であって、
主成分は
酸化第二鉄(Fe)が47.2〜49.2モル%,
酸化亜鉛(ZnO)が25〜30モル%,
酸化銅(CuO)が3〜10モル%,
酸化マンガン(MnO)が0.2〜2.8モル%であり、
残部を酸化ニッケル(NiO)とし、
前記酸化第二鉄と前記酸化マンガンとをFe+MnOの換算で
49.4モル% ≦ (Fe+MnO)≦ 50.0モル%
含有する組成であることを特徴とする酸化物磁性材料。
MnNiCuZn-based oxide magnetic material,
The main component is 47.2 to 49.2 mol% of ferric oxide (Fe 2 O 3 ),
Zinc oxide (ZnO) is 25-30 mol%,
3-10 mol% copper oxide (CuO),
Manganese oxide (MnO) is 0.2 to 2.8 mol%,
The balance is nickel oxide (NiO),
The ferric oxide and the manganese oxide in terms of Fe 2 O 3 + MnO are 49.4 mol% ≦ (Fe 2 O 3 + MnO) ≦ 50.0 mol%.
An oxide magnetic material having a composition containing the oxide magnetic material.
前記組成による焼結体は、平均結晶粒子径が8〜20μmであることを特徴とする請求項1に記載の酸化物磁性材料。   2. The oxide magnetic material according to claim 1, wherein the sintered body having the composition has an average crystal particle diameter of 8 to 20 μm. 前記組成による焼結体は、周波数60kHz,飽和磁束密度100mT,温度60℃でのコア損失が200kW/m以下であり、コア損失が最小値を示す温度が100℃以上であり、初透磁率の相対温度係数(αμir )は温度範囲25℃から130℃において20×10−6以下であることを特徴とする請求項1あるいは2の何れかに記載の酸化物磁性材料。 The sintered body having the above composition has a core loss at a frequency of 60 kHz, a saturation magnetic flux density of 100 mT, a temperature of 60 ° C. of 200 kW / m 3 or less, a temperature at which the core loss shows a minimum value is 100 ° C. or more, and an initial permeability. 3. The oxide magnetic material according to claim 1, wherein a relative temperature coefficient (α μir) is 20 × 10 −6 or less in a temperature range of 25 ° C. to 130 ° C. 3.
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Publication number Priority date Publication date Assignee Title
CN118125817A (en) * 2024-03-06 2024-06-04 中山市东晨磁性电子制品有限公司 A low-temperature sintered high-permeability high-Curie temperature NiCuZn material and preparation method thereof

Cited By (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
CN118125817A (en) * 2024-03-06 2024-06-04 中山市东晨磁性电子制品有限公司 A low-temperature sintered high-permeability high-Curie temperature NiCuZn material and preparation method thereof

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