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JP2012230948A - Powder for magnetic core, dust core, and method of manufacturing the same - Google Patents

Powder for magnetic core, dust core, and method of manufacturing the same Download PDF

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Publication number
JP2012230948A
JP2012230948A JP2011096860A JP2011096860A JP2012230948A JP 2012230948 A JP2012230948 A JP 2012230948A JP 2011096860 A JP2011096860 A JP 2011096860A JP 2011096860 A JP2011096860 A JP 2011096860A JP 2012230948 A JP2012230948 A JP 2012230948A
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low
temperature
particles
soft magnetic
softening material
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Inventor
Masashi Otsubo
将士 大坪
Masaaki Tani
昌明 谷
Takeshi Hattori
毅 服部
Yusuke Oishi
雄介 大石
Daisuke Okamoto
大祐 岡本
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Toyota Motor Corp
Toyota Central R&D Labs Inc
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Toyota Motor Corp
Toyota Central R&D Labs Inc
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Priority to JP2011096860A priority Critical patent/JP2012230948A/en
Priority to PCT/IB2012/000792 priority patent/WO2012146967A1/en
Publication of JP2012230948A publication Critical patent/JP2012230948A/en
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    • HELECTRICITY
    • H01ELECTRIC ELEMENTS
    • H01FMAGNETS; INDUCTANCES; TRANSFORMERS; SELECTION OF MATERIALS FOR THEIR MAGNETIC PROPERTIES
    • H01F1/00Magnets or magnetic bodies characterised by the magnetic materials therefor; Selection of materials for their magnetic properties
    • H01F1/01Magnets or magnetic bodies characterised by the magnetic materials therefor; Selection of materials for their magnetic properties of inorganic materials
    • H01F1/03Magnets or magnetic bodies characterised by the magnetic materials therefor; Selection of materials for their magnetic properties of inorganic materials characterised by their coercivity
    • H01F1/12Magnets or magnetic bodies characterised by the magnetic materials therefor; Selection of materials for their magnetic properties of inorganic materials characterised by their coercivity of soft-magnetic materials
    • H01F1/33Magnets or magnetic bodies characterised by the magnetic materials therefor; Selection of materials for their magnetic properties of inorganic materials characterised by their coercivity of soft-magnetic materials mixtures of metallic and non-metallic particles; metallic particles having oxide skin
    • BPERFORMING OPERATIONS; TRANSPORTING
    • B22CASTING; POWDER METALLURGY
    • B22FWORKING METALLIC POWDER; MANUFACTURE OF ARTICLES FROM METALLIC POWDER; MAKING METALLIC POWDER; APPARATUS OR DEVICES SPECIALLY ADAPTED FOR METALLIC POWDER
    • B22F1/00Metallic powder; Treatment of metallic powder, e.g. to facilitate working or to improve properties
    • B22F1/16Metallic particles coated with a non-metal
    • HELECTRICITY
    • H01ELECTRIC ELEMENTS
    • H01FMAGNETS; INDUCTANCES; TRANSFORMERS; SELECTION OF MATERIALS FOR THEIR MAGNETIC PROPERTIES
    • H01F1/00Magnets or magnetic bodies characterised by the magnetic materials therefor; Selection of materials for their magnetic properties
    • H01F1/01Magnets or magnetic bodies characterised by the magnetic materials therefor; Selection of materials for their magnetic properties of inorganic materials
    • H01F1/03Magnets or magnetic bodies characterised by the magnetic materials therefor; Selection of materials for their magnetic properties of inorganic materials characterised by their coercivity
    • H01F1/12Magnets or magnetic bodies characterised by the magnetic materials therefor; Selection of materials for their magnetic properties of inorganic materials characterised by their coercivity of soft-magnetic materials
    • H01F1/14Magnets or magnetic bodies characterised by the magnetic materials therefor; Selection of materials for their magnetic properties of inorganic materials characterised by their coercivity of soft-magnetic materials metals or alloys
    • H01F1/20Magnets or magnetic bodies characterised by the magnetic materials therefor; Selection of materials for their magnetic properties of inorganic materials characterised by their coercivity of soft-magnetic materials metals or alloys in the form of particles, e.g. powder
    • H01F1/22Magnets or magnetic bodies characterised by the magnetic materials therefor; Selection of materials for their magnetic properties of inorganic materials characterised by their coercivity of soft-magnetic materials metals or alloys in the form of particles, e.g. powder pressed, sintered, or bound together
    • H01F1/24Magnets or magnetic bodies characterised by the magnetic materials therefor; Selection of materials for their magnetic properties of inorganic materials characterised by their coercivity of soft-magnetic materials metals or alloys in the form of particles, e.g. powder pressed, sintered, or bound together the particles being insulated
    • HELECTRICITY
    • H01ELECTRIC ELEMENTS
    • H01FMAGNETS; INDUCTANCES; TRANSFORMERS; SELECTION OF MATERIALS FOR THEIR MAGNETIC PROPERTIES
    • H01F41/00Apparatus or processes specially adapted for manufacturing or assembling magnets, inductances or transformers; Apparatus or processes specially adapted for manufacturing materials characterised by their magnetic properties
    • H01F41/02Apparatus or processes specially adapted for manufacturing or assembling magnets, inductances or transformers; Apparatus or processes specially adapted for manufacturing materials characterised by their magnetic properties for manufacturing cores, coils, or magnets
    • H01F41/0206Manufacturing of magnetic cores by mechanical means
    • H01F41/0246Manufacturing of magnetic circuits by moulding or by pressing powder
    • BPERFORMING OPERATIONS; TRANSPORTING
    • B22CASTING; POWDER METALLURGY
    • B22FWORKING METALLIC POWDER; MANUFACTURE OF ARTICLES FROM METALLIC POWDER; MAKING METALLIC POWDER; APPARATUS OR DEVICES SPECIALLY ADAPTED FOR METALLIC POWDER
    • B22F2998/00Supplementary information concerning processes or compositions relating to powder metallurgy
    • CCHEMISTRY; METALLURGY
    • C22METALLURGY; FERROUS OR NON-FERROUS ALLOYS; TREATMENT OF ALLOYS OR NON-FERROUS METALS
    • C22CALLOYS
    • C22C2202/00Physical properties
    • C22C2202/02Magnetic

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  • Engineering & Computer Science (AREA)
  • Power Engineering (AREA)
  • Chemical & Material Sciences (AREA)
  • Dispersion Chemistry (AREA)
  • Manufacturing & Machinery (AREA)
  • Powder Metallurgy (AREA)
  • Soft Magnetic Materials (AREA)

Abstract

【課題】比抵抗および強度に優れる圧粉磁心を提供する。
【解決手段】本発明は、軟磁性粒子と、この軟磁性粒子間に形成される粒界相と、からなる圧粉磁心であって、粒界相は、軟磁性粒子の焼鈍温度よりも低い軟化点を有する第一無機酸化物からなる低温軟化材(低融点ガラス粒子)からなるマトリックス中に、焼鈍温度よりも高い軟化点を有する第二無機酸化物からなる高温軟化材(シリカやアルミナのナノ粒子)からなる微粒子が分散した複合分散組織であることを特徴とする。粒界相がこのような複合分散組織からなることにより、各軟磁性粒子は、低温軟化材により強固に結合されると共に高温軟化材により所定間隔が保持され絶縁性が確保される。こうして高比抵抗と高強度が高次元で両立した本発明の圧粉磁心が得られた。
【選択図】図1A
A dust core having excellent specific resistance and strength is provided.
The present invention provides a dust core comprising soft magnetic particles and a grain boundary phase formed between the soft magnetic particles, the grain boundary phase being lower than the annealing temperature of the soft magnetic particles. In a matrix made of a low temperature softening material (low melting glass particles) made of a first inorganic oxide having a softening point, a high temperature softening material made of a second inorganic oxide having a softening point higher than the annealing temperature (of silica or alumina). It is a composite dispersed structure in which fine particles of nanoparticles are dispersed. When the grain boundary phase is composed of such a composite dispersed structure, each soft magnetic particle is firmly bonded by the low-temperature softening material, and a predetermined interval is maintained by the high-temperature softening material to ensure insulation. In this way, the dust core of the present invention in which high resistivity and high strength are compatible in a high dimension was obtained.
[Selection] Figure 1A

Description

本発明は、体積比抵抗値(以下単に「比抵抗」という。)および強度に優れる圧粉磁心、その製造に用いられる磁心用粉末および製造方法に関するものである。   The present invention relates to a dust core excellent in volume resistivity (hereinafter simply referred to as “resistivity”) and strength, a magnetic core powder used in the production thereof, and a production method.

変圧器(トランス)、電動機(モータ)、発電機、スピーカ、誘導加熱器、各種アクチュエータ等、我々の周囲には電磁気を利用した製品が多々ある。これらの製品は交番磁界を利用したものが多く、局所的に大きな交番磁界を効率的に得るために、通常、磁心(軟磁石)をその交番磁界中に設けている。   There are many products that use electromagnetism around us, such as transformers, motors, generators, speakers, induction heaters, and various actuators. Many of these products use an alternating magnetic field. In order to efficiently obtain a large alternating magnetic field locally, a magnetic core (soft magnet) is usually provided in the alternating magnetic field.

この磁心は、交番磁界中において高磁気特性であるのみならず、交番磁界中で使用する際に高周波損失(以下、磁心の材質に拘らず単に「鉄損」という。)が少ないことが求められる。鉄損には、渦電流損失、ヒステリシス損失および残留損失があるが、特に交番磁界の周波数と共に高くなる渦電流損失の低減を図ることが重要である。   This magnetic core is required not only to have high magnetic characteristics in an alternating magnetic field, but also to have low high-frequency loss (hereinafter simply referred to as “iron loss” regardless of the material of the magnetic core) when used in an alternating magnetic field. . Iron loss includes eddy current loss, hysteresis loss, and residual loss. It is particularly important to reduce eddy current loss that increases with the frequency of the alternating magnetic field.

そこで、絶縁被覆された軟磁性粒子(磁心用粉末の各粒子)を加圧成形した圧粉磁心の開発、研究が盛んに行われてきた。このような圧粉磁心は、絶縁被膜の存在により高比抵抗で低鉄損であると共に、形状自由度が高く種々の電磁機器に対応し易い。もっとも最近では、圧粉磁心の用途拡大を図るため、比抵抗のみならず、強度や耐熱性の向上も重視されている。このような圧粉磁心に関する提案が、例えば下記のような特許文献にある。   Therefore, development and research of a powder magnetic core obtained by press-molding soft magnetic particles (magnetic particles for magnetic core) that have been coated with insulation have been actively conducted. Such a powder magnetic core has a high specific resistance and a low iron loss due to the presence of the insulating coating, and has a high degree of freedom in shape and is easily compatible with various electromagnetic devices. Most recently, in order to expand applications of dust cores, not only specific resistance but also strength and heat resistance are emphasized. The proposal regarding such a powder magnetic core exists in the following patent documents, for example.

特開2004−143554号公報JP 2004-143554 A

特許文献1は、シリコーン樹脂、ガラスおよびアルミナからなる被膜を表面に形成した軟磁性粒子を加圧成形してなる圧粉磁心を提案している。この圧粉磁心は、シリコーン樹脂をバインダーとしているため、高温で焼鈍等したりすると、比抵抗が急減し得る。ちなみに、この特許文献1には、そのアルミナの形態(粒径等)について一切記載されていない。   Patent Document 1 proposes a powder magnetic core formed by press-molding soft magnetic particles having a coating made of silicone resin, glass and alumina formed on the surface thereof. Since this powder magnetic core uses a silicone resin as a binder, the specific resistance can be drastically reduced when annealed at a high temperature. Incidentally, this Patent Document 1 does not describe the form (particle size or the like) of the alumina at all.

本発明はこのような事情に鑑みてなされたものであり、従来の圧粉磁心とは異なり、高比抵抗および高強度を高温域まで安定して発揮し得る圧粉磁心を提供することを目的とする。またその圧粉磁心の製造に適した磁心用粉末およびそれらの製造方法を併せて提供する。   The present invention has been made in view of such circumstances, and an object thereof is to provide a dust core that can stably exhibit high specific resistance and high strength up to a high temperature range, unlike a conventional dust core. And Moreover, the powder for magnetic cores suitable for manufacture of the powder magnetic core, and those manufacturing methods are also provided.

本発明者はこの課題を解決すべく鋭意研究し、試行錯誤を重ねた結果、低融点ガラス等の低温軟化材と微細なシリカ粒子等の高温軟化材からなる粒界相を、軟磁性粒子からなる主相間に形成することにより、非常に高い比抵抗および圧環強度を発現する圧粉磁心が得られることを新たに見出した。この成果を発展させることにより、以降に述べる本発明を完成するに至った。   As a result of extensive research and trial and error, the present inventor has obtained a grain boundary phase composed of a low-temperature softening material such as low-melting glass and a high-temperature softening material such as fine silica particles from soft magnetic particles. It was newly found out that a dust core exhibiting a very high specific resistance and ring crushing strength can be obtained by forming between the main phases. By developing this result, the present invention described below has been completed.

《圧粉磁心および磁心用粉末》
(1)本発明の圧粉磁心は、軟磁性粒子からなる主相と、該軟磁性粒子間に形成される粒界相と、からなる圧粉磁心であって、前記粒界相は、該軟磁性粒子の焼鈍温度よりも低い軟化点を有する第一無機酸化物からなる低温軟化材と該焼鈍温度よりも高い軟化点を有する第二無機酸化物からなる高温軟化材とが複合してなることを特徴とする。
<Dust core and magnetic core powder>
(1) The powder magnetic core of the present invention is a powder magnetic core comprising a main phase composed of soft magnetic particles and a grain boundary phase formed between the soft magnetic particles. A composite of a low temperature softening material composed of a first inorganic oxide having a softening point lower than the annealing temperature of the soft magnetic particles and a high temperature softening material composed of a second inorganic oxide having a softening point higher than the annealing temperature. It is characterized by that.

(2)本発明の圧粉磁心は、高比抵抗および高強度であって、この特性を高温域でも安定して発揮し得る。本発明がこのような優れた効果を発現する理由は必ずしも定かではないが、現状、次のように考えられる。 (2) The dust core of the present invention has high specific resistance and high strength, and can stably exhibit these characteristics even in a high temperature range. The reason why the present invention exhibits such an excellent effect is not necessarily clear, but at present, it is considered as follows.

本発明の圧粉磁心は、無機酸化物からなる粒界相によって、主相である軟磁性粒子が保持または結合されると共に軟磁性粒子間の絶縁性が確保される。逆にいえば本発明の圧粉磁心では、耐熱性に劣るバインダー樹脂等を用いる必要がない。このため本発明によれば、高温域でも、高比抵抗および高強度を発揮する圧粉磁心が得られる。   In the dust core of the present invention, the soft magnetic particles as the main phase are held or bonded by the grain boundary phase made of an inorganic oxide, and insulation between the soft magnetic particles is secured. Conversely, in the dust core of the present invention, it is not necessary to use a binder resin or the like that is inferior in heat resistance. Therefore, according to the present invention, a dust core that exhibits high specific resistance and high strength can be obtained even in a high temperature range.

この点を詳述すると次の通りである。先ず、圧粉磁心は、磁心用粉末を所望形状に加圧成形して得られる。この際、軟磁性粒子内へ導入させる残留歪み等は、圧粉磁心の保磁力ひいてはヒステリシス損失を増加させるため、加圧成形後の熱処理(焼鈍)により除去されるのが通常である。   This point is described in detail as follows. First, a dust core is obtained by pressure-molding a magnetic core powder into a desired shape. At this time, residual strain or the like introduced into the soft magnetic particles is usually removed by heat treatment (annealing) after pressure molding in order to increase the coercive force of the dust core and thus the hysteresis loss.

この焼鈍時、焼鈍温度よりも軟化点の低い低温軟化材が軟化(さらには溶融)して、軟磁性粒子を被包するようになる。この低温軟化材は、軟磁性粒子間の絶縁性に寄与すると共に、バインダーの役割も果たして軟磁性粒子同士の結合を強固にする。さらに軟化等した低温軟化材は、各軟磁性粒子間の隙間(例えば三重点)へ流入等して、各軟磁性粒子のより安定的な保持に寄与する。こうして先ず、低温軟化材により各軟磁性粒子の絶縁性と結合が確保される。   During this annealing, the low-temperature softening material having a softening point lower than the annealing temperature softens (and melts) and encapsulates the soft magnetic particles. This low-temperature softening material contributes to the insulation between the soft magnetic particles and also serves as a binder to strengthen the bond between the soft magnetic particles. Further, the softened low-temperature softening material flows into gaps (for example, triple points) between the soft magnetic particles and contributes to more stable holding of the soft magnetic particles. Thus, first, the insulation and bonding of each soft magnetic particle is ensured by the low-temperature softening material.

もっとも、軟磁性粒子間における低温軟化材の介在量が不十分になると、軟磁性粒子が部分的に直接接触するようになり(図1B参照)、軟磁性粒子間の絶縁性が低下し、ひいては圧粉磁心の比抵抗が低下し得る。このような状態は、焼鈍時に軟化した低温軟化材が軟磁性粒子間から流出することによっても生じ得ると考えられる。   However, if the amount of the low-temperature softening material interposed between the soft magnetic particles becomes insufficient, the soft magnetic particles partially come into direct contact (refer to FIG. 1B), and the insulation between the soft magnetic particles is lowered, and consequently The specific resistance of the dust core can be reduced. It is considered that such a state can also occur when the low-temperature softening material softened during annealing flows out between the soft magnetic particles.

ところが本発明の場合、軟磁性粒子間(粒界)には、低温軟化材のみならず、焼鈍温度よりも軟化点の高い高温軟化材が存在している(図1A参照)。この高温軟化材は、焼鈍時にもあまり軟化等せず、少なからず元の形態を保持し、軟磁性粒子間の距離(粒子間距離)を一定以上に保つ。この結果、軟磁性粒子同士が直接接触する事態は大幅に低減され、軟磁性粒子間の絶縁性がより確実に確保されるようになる。   However, in the present invention, not only the low-temperature softening material but also the high-temperature softening material having a higher softening point than the annealing temperature exists between the soft magnetic particles (grain boundaries) (see FIG. 1A). This high-temperature softening material does not soften much during annealing, retains the original form as much as possible, and keeps the distance between the soft magnetic particles (inter-particle distance) above a certain level. As a result, the situation where the soft magnetic particles are in direct contact with each other is greatly reduced, and the insulation between the soft magnetic particles is more reliably ensured.

ここで低温軟化材に接触している高温軟化材は、高温焼鈍時に、その表面部分が低温軟化材と共に軟化または溶融することもわかっている。この場合、高温軟化材と低温軟化材が、少なくとも界面部分で融合した粒界相が形成される。具体的にいうと、低温軟化材が低融点ガラスであり、高温軟化材がシリカである場合なら、その粒界相は低融点ガラスからなるマトリックス中にシリカからなるシリカ濃化相が分散した複合分散組織が形成され得る。このような場合、高温軟化材が低温軟化材中に単に埋設しているに留まらず、両者が少なくとも界面部分で融合(溶融後に凝固)して一体的に結合した状態となるため、本発明の圧粉磁心は特に高い強度を発現すると考えられる。   Here, it is also known that the surface portion of the high-temperature softened material in contact with the low-temperature softened material is softened or melted together with the low-temperature softened material during high-temperature annealing. In this case, a grain boundary phase in which the high-temperature softening material and the low-temperature softening material are fused at least at the interface portion is formed. Specifically, if the low-temperature softening material is a low-melting glass and the high-temperature softening material is silica, the grain boundary phase is a composite in which a silica-concentrated phase made of silica is dispersed in a matrix made of low-melting glass. A dispersed tissue can be formed. In such a case, the high-temperature softening material is not simply embedded in the low-temperature softening material, but both are fused (solidified after melting) at least at the interface portion, and are integrally bonded. The dust core is considered to exhibit particularly high strength.

このように無機酸化物からなる低温軟化材および高温軟化材が、相乗的に作用することにより、高温域まで安定した高比抵抗および高強度を発現する圧粉磁心が得られるようになったと考えられる。   In this way, the low-temperature softening material and high-temperature softening material composed of inorganic oxides act synergistically, and it is considered that a powder magnetic core that exhibits stable high specific resistance and high strength can be obtained up to high temperature range. It is done.

《磁心用粉末》
本発明は、上述した圧粉磁心としてのみならず、その製造に適した磁心用粉末としても把握し得る。つまり本発明は、軟磁性粒子と、該軟磁性粒子の焼鈍温度よりも低い軟化点を有する第一無機酸化物からなる低温軟化材と該焼鈍温度よりも高い軟化点を有する第二無機酸化物からなる高温軟化材とが該軟磁性粒子の表面に付着してなる付着層と、からなることを特徴とする圧粉磁心に用いられる磁心用粉末でもよい。
<Magnetic core powder>
The present invention can be understood not only as the above-described powder magnetic core but also as a magnetic core powder suitable for its production. That is, the present invention provides a low-temperature softening material comprising soft magnetic particles, a first inorganic oxide having a softening point lower than the annealing temperature of the soft magnetic particles, and a second inorganic oxide having a softening point higher than the annealing temperature. It may be a powder for a magnetic core used for a powder magnetic core, characterized in that the high-temperature softening material comprising: an adhesion layer formed by adhering to the surface of the soft magnetic particles.

《圧粉磁心の製造方法》
本発明は、さらに上述した圧粉磁心の製造に適した圧粉磁心の製造方法としても把握し得る。つまり本発明は、上述した磁心用粉末を金型に充填する充填工程と、該金型内の磁心用粉末を加圧成形する成形工程と、該成形工程後に得られた成形体を、前記低温軟化材の軟化点以上かつ前記高温軟化材の軟化点未満の温度で焼鈍する焼鈍工程と、を備えることを特徴とする圧粉磁心の製造方法であってもよい。
<Production method of dust core>
The present invention can also be grasped as a method for manufacturing a dust core suitable for manufacturing the above-described dust core. That is, the present invention provides a filling step of filling the above-described magnetic core powder into a mold, a molding step of press-molding the magnetic core powder in the mold, and a molded body obtained after the molding step, the low temperature And a annealing step of annealing at a temperature equal to or higher than the softening point of the softening material and lower than the softening point of the high-temperature softening material.

《その他》
(1)本発明でいう「軟化点」は、加熱された無機酸化物の粘度が、温度上昇の過程で107.5dPa・sとなる温度である。このため、本発明でいう軟化点は一般的にいわれるガラス転移点(Tg)とは必ずしも一致しない。ちなみにこの軟化点はJIS R3103−1 ガラスの粘性および粘性定点−第1部:軟化点の測定方法−により特定される。
<Others>
(1) The “softening point” as used in the present invention is a temperature at which the viscosity of the heated inorganic oxide becomes 10 7.5 dPa · s in the course of temperature increase. For this reason, the softening point referred to in the present invention does not necessarily coincide with the generally referred glass transition point (Tg). Incidentally, the softening point is specified by the viscosity of JIS R3103-1 glass and the fixed point of viscosity-Part 1: Method for measuring softening point.

(2)本発明でいう「焼鈍温度」は、加圧成形後の残留歪みや残留応力の除去等を目的として、軟磁性粒子の成形体に対してなされる焼鈍工程における加熱温度である。 (2) The “annealing temperature” in the present invention is a heating temperature in an annealing process performed on a molded body of soft magnetic particles for the purpose of removing residual strain and residual stress after pressure molding.

(3)本発明に係る高温軟化材は、焼鈍時にその一部が軟化または溶融して低温軟化材と一体化した粒界相を形成していると好ましい。但し、高温軟化材が軟化または溶融していない圧粉磁心も、高比抵抗および高強度を発現し得る限り、本発明に含まれる。 (3) It is preferable that the high-temperature softening material according to the present invention partially softens or melts during annealing to form a grain boundary phase integrated with the low-temperature softening material. However, a dust core in which the high-temperature softening material is not softened or melted is also included in the present invention as long as it can exhibit high specific resistance and high strength.

(4)特に断らない限り本明細書でいう「x〜y」は下限値xおよび上限値yを含む。また本明細書に記載した種々の数値や数値範囲内に含まれる数値を任意に組み合わせて「a〜b」のような新たな数値範囲を構成し得る。 (4) Unless otherwise specified, “x to y” in this specification includes a lower limit value x and an upper limit value y. Moreover, a new numerical value range such as “ab” can be configured by arbitrarily combining various numerical values and numerical values included in the numerical value range described in this specification.

本発明の圧粉磁心に係る主相と粒界相とを模式的に示した説明図である。It is explanatory drawing which showed typically the main phase and grain boundary phase which concern on the powder magnetic core of this invention. 従来の圧粉磁心に係る主相と粒界相とを模式的に示した説明図である。It is explanatory drawing which showed typically the main phase and grain boundary phase which concern on the conventional dust core. 一実施例である圧粉磁心を構成する軟磁性粒子の表面近傍を観察した電子顕微鏡写真である。It is the electron micrograph which observed the surface vicinity of the soft-magnetic particle which comprises the powder magnetic core which is one Example. 種々の圧粉磁心の比抵抗と圧環強度の関係を示す分散図である。It is a dispersion | distribution figure which shows the relationship between the specific resistance of various powder magnetic cores, and crumbling strength. 本発明に係る低温軟化材を熱分析して得られたDTA曲線を示すグラフである。It is a graph which shows the DTA curve obtained by thermally analyzing the low temperature softening material which concerns on this invention.

発明の実施形態を挙げて本発明をより詳しく説明する。上述した本発明の構成に本明細書中から任意に選択した一つまたは二つ以上の構成を付加し得る。本明細書で説明する内容は、本発明に係る圧粉磁心のみならず、その製造に用いる磁心用粉末や製造方法にも適用され得る。製造方法に関する構成は、プロダクトバイプロセスとして理解すれば物に関する構成ともなり得る。なお、いずれの実施形態が最良であるか否かは、対象、要求性能等によって異なる。   The present invention will be described in more detail with reference to embodiments of the invention. One or two or more configurations arbitrarily selected from the present specification may be added to the configuration of the present invention described above. The contents described in the present specification can be applied not only to the powder magnetic core according to the present invention but also to the magnetic core powder and the manufacturing method used for the production thereof. A configuration related to a manufacturing method can be a configuration related to an object if understood as a product-by-process. Note that which embodiment is the best depends on the target, required performance, and the like.

《軟磁性粒子(軟磁性粉末)》
軟磁性粒子は、8属遷移元素(Fe、Co、Ni等)などの強磁性元素を主成分とすれば足るが、取扱性、入手性、コスト等から純鉄または鉄合金からなると好ましい。鉄合金は、Si含有鉄合金(Fe−Si合金)が好ましい。Siは軟磁性粒子の電気抵抗率を高め、圧粉磁心の比抵抗を向上させ、渦電流損失を低減させるからである。
《Soft magnetic particles (soft magnetic powder)》
The soft magnetic particles may be composed mainly of a ferromagnetic element such as a group 8 transition element (Fe, Co, Ni, etc.), but are preferably made of pure iron or an iron alloy from the viewpoint of handling, availability, and cost. The iron alloy is preferably a Si-containing iron alloy (Fe—Si alloy). This is because Si increases the electrical resistivity of the soft magnetic particles, improves the specific resistance of the dust core, and reduces eddy current loss.

軟磁性粒子は、全体を100質量%としたときにSiを0.2〜4質量%さらには0.8〜3.5質量%含むと好ましい。Siが過少では効果がなく、Siが過多になると、圧粉磁心の磁気的特性や成形性を低下させ得る。鉄合金は、その他にCoやAlを含んでもよい。   The soft magnetic particles preferably contain 0.2 to 4% by mass and further 0.8 to 3.5% by mass of Si when the total is 100% by mass. If there is too little Si, there is no effect, and if there is too much Si, the magnetic properties and moldability of the dust core can be reduced. The iron alloy may further contain Co or Al.

さらに軟磁性粉末は、複数の粉末を混合した混合粉末でもよい。例えば、純鉄粉とFe−49Co−2V(パーメンジュール)粉、純鉄粉とFe−3Si粉、センダスト(Fe−9Si−6Al)粉と純鉄粉等の混合粉末であってもよい。   Further, the soft magnetic powder may be a mixed powder obtained by mixing a plurality of powders. For example, a mixed powder such as pure iron powder and Fe-49Co-2V (permendur) powder, pure iron powder and Fe-3Si powder, Sendust (Fe-9Si-6Al) powder and pure iron powder may be used.

軟磁性粒子の最適な粒径は、対象とされる圧粉磁心の種類により異なる。通常、軟磁性粒子の粒径は5〜500μm、20〜300μmさらには40〜200μmであると好ましい。粒径が過大では高密度化や渦電流損失の低減化が図り難く、粒径が過小ではヒステリシス損失の低減が図り難い。なお、軟磁性粒子の分級は、篩い分法等により容易に行える。本明細書でいう軟磁性粒子の粒径は、所定のメッシュサイズの篩いによって分級したときに定まる粒径である。   The optimum particle size of the soft magnetic particles varies depending on the type of the dust core to be used. Usually, the particle diameter of the soft magnetic particles is preferably 5 to 500 μm, 20 to 300 μm, and more preferably 40 to 200 μm. If the particle size is too large, it is difficult to increase the density and reduce the eddy current loss. If the particle size is too small, it is difficult to reduce the hysteresis loss. The classification of soft magnetic particles can be easily performed by a sieving method or the like. The particle diameter of the soft magnetic particles referred to in this specification is a particle diameter determined when classified by a sieve having a predetermined mesh size.

軟磁性粒子の製造方法は問わず、軟磁性粒子は粉砕粉でもアトマイズ粉でもよい。アトマイズ粉は、水アトマイズ粉、ガスアトマイズ粉、ガス水アトマイズ粉のいずれでもよい。ガス(水)アトマイズ粉を用いると、絶縁被膜の破壊等が抑制されて比抵抗の高い圧粉磁心が安定して得られ易い。ガス(水)アトマイズ粉の各構成粒子は擬球状をしており、粒子相互間の攻撃性が低くいからである。   Regardless of the method of producing the soft magnetic particles, the soft magnetic particles may be pulverized powder or atomized powder. The atomized powder may be any of water atomized powder, gas atomized powder, and gas water atomized powder. When gas (water) atomized powder is used, destruction of the insulating coating or the like is suppressed, and a dust core having a high specific resistance is easily obtained stably. This is because each constituent particle of the gas (water) atomized powder has a pseudo-spherical shape, and the aggressiveness between the particles is low.

《低温軟化材》
低温軟化材は、磁心用粉末を加圧成形した成形体の焼鈍温度(軟磁性粒子の焼鈍温度)より低い軟化点を有する(第一)無機酸化物からなる。この無機酸化物は、焼鈍温度以上で、粘度が107.5dPa・s以下となるものであれば、その種類を問わない。
<Low temperature softener>
The low-temperature softening material is made of a (first) inorganic oxide having a softening point lower than the annealing temperature (annealing temperature of soft magnetic particles) of a molded body obtained by pressure-molding the magnetic core powder. The inorganic oxide may be of any type as long as it has an annealing temperature or higher and a viscosity of 10 7.5 dPa · s or lower.

このような低温軟化材として、食器やタイル等に使用される、いわゆる低融点ガラスがある。低温軟化材は、硼珪酸鉛系ガラスでもよいが、環境負荷の小さい組成系からなる低融点ガラス、例えば、低温軟化材は、硼珪酸塩系ガラス、珪酸塩系ガラス、リン酸塩系ガラス、硼酸塩系ガラス、酸化バナジウム系ガラス等の一種以上であるとより好適である。   As such a low-temperature softening material, there is a so-called low melting point glass used for tableware, tiles and the like. The low-temperature softening material may be lead borosilicate glass, but low-melting glass having a composition system with a small environmental load, for example, low-temperature softening material is borosilicate glass, silicate glass, phosphate glass, It is more preferable to use one or more of borate glass and vanadium oxide glass.

硼珪酸塩系ガラスの主成分として、例えば、SiO−B−LiO、SiO−B−NaO、SiO−B−CaOなどがある。珪酸塩系ガラスの主成分として、例えば、SiO−LiO、SiO−NaO、SiO−CaO、SiO−MgO、SiO−Al などがある。リン酸塩系ガラスの主成分として、例えば、P−LiO、P−NaO、P−CaO、P−MgO、P−Al などがある。硼酸塩系ガラスの主成分として、例えば、B−LiO、B−NaO、B−CaO、B−MgO、B−Alなどがある。酸化バナジウム系ガラスの主成分として、例えば、V−B、V−B−SiO、V−P、V−B−Pなどがある。 As a main component of the borosilicate glass, for example, SiO 2 -B 2 O 3 -Li 2 O, SiO 2 -B 2 O 3 -Na 2 O, and SiO 2 -B 2 O 3 -CaO. As a main component of the silicate-based glass, for example, SiO 2 -Li 2 O, SiO 2 -Na 2 O, SiO 2 -CaO, SiO 2 -MgO, and the like SiO 2 -Al 2 O 3. As the main component of the phosphate type glass, for example, P 2 O 5 -Li 2 O , P 2 O 5 -Na 2 O, P 2 O 5 -CaO, P 2 O 5 -MgO, P 2 O 5 -Al 2 O 3 and the like. As a main component of the borate-based glass, for example, B 2 O 3 -Li 2 O , B 2 O 3 -Na 2 O, B 2 O 3 -CaO, B 2 O 3 -MgO, B 2 O 3 -Al 2 O 3 etc. Examples of the main component of the vanadium oxide glass include V 2 O 5 —B 2 O 3 , V 2 O 5 —B 2 O 3 —SiO 2 , V 2 O 5 —P 2 O 5 , V 2 O 5 —B. 2 O 3 —P 2 O 5 and the like.

これら低融点ガラスは、SiO、NaO、ZnO、B、LiO、SnO、BaO、CaO、Al等の組成を調整することにより、軟化点を焼鈍温度に適した温度に調整可能である。 These low-melting glass, SiO 2, Na 2 O, ZnO, B 2 O 3, Li 2 O, SnO, BaO, CaO, by adjusting the composition such as Al 2 O 3, suitable for softening in the annealing temperature The temperature can be adjusted.

低温軟化材(特に低融点ガラス)は、磁心用粉末全体または圧粉磁心全体を100質量%としたときに、0.3〜4質量%、0.5〜3.5質量%さらには0.7〜3質量%であると好ましい。低温軟化材が過少では圧粉磁心の強度の向上が不十分となり、それが過多では圧粉磁心の磁気特性が低下し得る。   The low-temperature softening material (particularly low-melting glass) is 0.3 to 4% by mass, 0.5 to 3.5% by mass, and further preferably 0.00% when the entire magnetic core powder or the entire powder magnetic core is 100% by mass. It is preferable in it being 7-3 mass%. If the low-temperature softening material is too small, the strength of the dust core will not be sufficiently improved, and if it is excessive, the magnetic properties of the dust core may be reduced.

なお、低温軟化材は、圧粉磁心の焼鈍後に粒界相を形成すれば足りる。つまり、磁心用粉末の段階または圧粉磁心の焼鈍前の段階では、軟磁性粒子の表面に付着した粒子状で足りる。この低温軟化材の粒子(特に低融点ガラス粒子)は、軟磁性粒子より粒径が小さいと好ましく、例えば、0.5〜90μmさらには1〜50μm程度であるとよい。その粒径が過小では製造や取扱性が困難となり、粒径が過大になると緻密で密着性に優れた粒界相の形成が困難となる。   Note that the low-temperature softening material only needs to form a grain boundary phase after annealing of the powder magnetic core. That is, in the stage of the magnetic core powder or the stage before the annealing of the powder core, the particles attached to the surface of the soft magnetic particles are sufficient. The particles of the low-temperature softening material (particularly low-melting glass particles) preferably have a particle size smaller than that of the soft magnetic particles, for example, about 0.5 to 90 μm and further about 1 to 50 μm. If the particle size is too small, it becomes difficult to produce and handle, and if the particle size is too large, it is difficult to form a grain boundary phase that is dense and has excellent adhesion.

ちなみに低融点ガラス粒子の粒径は、種々の方法により特定できるが、本明細書でいう粒径は、走査型電子顕微鏡(SEM)による画像解析またはレーザ回折法により特定した。   Incidentally, the particle size of the low melting point glass particles can be specified by various methods, but the particle size referred to in the present specification was specified by image analysis by a scanning electron microscope (SEM) or laser diffraction method.

《高温軟化材》
高温軟化材は、焼鈍温度よりも高い軟化点を有する(第二)無機酸化物からなる。この無機酸化物は、焼鈍温度時に粘度が107.5dPa・s超であれば、その種類を問わない。
《High temperature softening material》
The high-temperature softening material is made of a (second) inorganic oxide having a softening point higher than the annealing temperature. The inorganic oxide may be of any type as long as the viscosity is higher than 10 7.5 dPa · s at the annealing temperature.

このような高温軟化材として、高融点のセラミックス粒子がある。具体的には、シリカ粒子、アルミナ粒子、チタニア粒子、ジルコニア粒子等である。このような粒子は、軟磁性粒子同士の直接接触の回避に適した微粒子、例えば、平均粒径が5〜500nmさらには10〜400nmのナノ粒子であると好ましい。この粒径が過大では圧粉磁心が低密度となり、粒径が過小では加圧成形により変形した軟磁性粒子同士の直接接触を十分に回避できない。   As such a high-temperature softening material, there are high melting point ceramic particles. Specifically, silica particles, alumina particles, titania particles, zirconia particles, and the like. Such particles are preferably fine particles suitable for avoiding direct contact between soft magnetic particles, for example, nanoparticles having an average particle size of 5 to 500 nm, more preferably 10 to 400 nm. If this particle size is too large, the dust core will have a low density, and if the particle size is too small, direct contact between soft magnetic particles deformed by pressure molding cannot be sufficiently avoided.

高温軟化材は、磁心用粉末全体または圧粉磁心全体を100質量%としたときに、0.1〜2.7質量%、0.2〜2.5質量%さらには0.4〜2.3質量%であると好ましい。高温軟化材が過少では圧粉磁心の比抵抗の向上が不十分となり、それが過多では圧粉磁心の強度の低下を招く。   The high-temperature softening material is 0.1 to 2.7% by mass, 0.2 to 2.5% by mass, or further 0.4 to 2.10% with respect to 100% by mass of the entire magnetic core powder or the entire powder magnetic core. It is preferable that it is 3 mass%. If the high-temperature softening material is too small, the specific resistance of the dust core is not sufficiently improved, and if it is too large, the strength of the dust core is reduced.

高温軟化材が微粒子(さらにはナノ粒子)からなる場合、本発明に係る粒界相は、低温軟化材からなるマトリックス中に、軟磁性粒子よりも粒径の小さい高温軟化材の粒子(微粒子またはナノ粒子)が分散した複合分散組織となる。この場合、本発明の圧粉磁心は、主相である軟磁性粒子の表面が、二種以上の無機酸化物が一体的または不連続的な状態で分布した粒界相(または被膜)により包囲(または被覆)された状態となる(図1A参照)。この点、軟磁性粒子の表面が単一の連続した絶縁層等で被膜されていた従来の圧粉磁心と異なる(図1B参照)。   When the high-temperature softening material is composed of fine particles (or nanoparticles), the grain boundary phase according to the present invention is the particles of the high-temperature softening material (fine particles or particles) having a smaller particle size than the soft magnetic particles in the matrix composed of the low-temperature softening material. It becomes a composite dispersed structure in which (nanoparticles) are dispersed. In this case, the dust core of the present invention is surrounded by the grain boundary phase (or film) in which the surface of the soft magnetic particles as the main phase is distributed in an integrated or discontinuous state of two or more inorganic oxides. (Or covered) (see FIG. 1A). This is different from the conventional dust core in which the surface of the soft magnetic particles is coated with a single continuous insulating layer or the like (see FIG. 1B).

《磁心用粉末の製造》
磁心用粉末は、軟磁性粒子の表面に低温軟化材および高温軟化材を付着させることにより得られる(付着工程)。低温軟化材と高温軟化材を軟磁性粒子の表面に付着させる順序は問わない。つまり、軟磁性粒子の表面に、軟磁性粒子を先に付着させた後に高温軟化材を付着させてもよいし、その逆でもよし、さらには、それらを同時に付着させてもよい。
<Manufacture of magnetic core powder>
The magnetic core powder is obtained by attaching a low-temperature softening material and a high-temperature softening material to the surface of the soft magnetic particles (attachment step). The order of attaching the low-temperature softening material and the high-temperature softening material to the surface of the soft magnetic particles is not limited. That is, the high temperature softening material may be attached to the surface of the soft magnetic particles after the soft magnetic particles are attached first, or vice versa, or they may be attached simultaneously.

この付着工程は湿式で行っても乾式で行ってもよい。例えば、低温軟化材(特に低融点ガラス粉末)を分散媒に分散させた分散液(スラリー)に、高温軟化材を付着させた軟磁性粒子の粉末を入れて攪拌混合し、その後、その分散媒を蒸発させ乾燥させてもよい(湿式付着工程)。また分散媒を介さずに、高温軟化材を付着させた軟磁性粒子の粉末と低温軟化材とを混合してもよい(乾式付着工程)。さらには、分散媒を介さずに、軟磁性粒子、低温軟化材および高温軟化材を同時に混合してもよい(同時乾式付着工程)。湿式であれば、より均一的な付着が可能になり、乾式であれば乾燥工程を省略できて効率的である。   This adhesion step may be performed wet or dry. For example, in a dispersion (slurry) in which a low-temperature softening material (particularly a low-melting glass powder) is dispersed in a dispersion medium, the powder of soft magnetic particles to which the high-temperature softening material is attached is stirred and mixed. May be evaporated and dried (wet deposition process). Moreover, you may mix the powder of the soft magnetic particle to which the high temperature softening material was made to adhere, and a low temperature softening material without using a dispersion medium (dry adhesion process). Furthermore, the soft magnetic particles, the low-temperature softening material, and the high-temperature softening material may be mixed at the same time without using a dispersion medium (simultaneous dry adhesion step). If wet, more uniform adhesion is possible, and if dry, the drying step can be omitted, which is efficient.

《圧粉磁心の製造》
本発明の圧粉磁心は、所望形状のキャビティを有する金型へ磁心用粉末を充填する充填工程と、その磁心用粉末を加圧成形して成形体とする成形工程と、その成形体を焼鈍する焼鈍工程とを経て得られる。ここでは成形工程と焼鈍工程について説明する。
<Manufacture of dust core>
The dust core of the present invention includes a filling step of filling a mold having a cavity of a desired shape with a magnetic core powder, a molding step of pressing the magnetic core powder into a molded body, and annealing the molded body. Obtained through an annealing step. Here, the forming process and the annealing process will be described.

(1)成形工程
成形工程で軟磁性粒子に印加される成形圧力は問わないが、高圧成形するほど高密度で高磁束密度の圧粉磁心が得られる。このような高圧成形方法として、金型潤滑温間高圧成形法がある。金型潤滑温間高圧成形法は、高級脂肪酸系潤滑剤を内面に塗布した金型へ前記磁心用粉末を充填する充填工程と、磁心用粉末と金型の内面との間に高級脂肪酸系潤滑剤とは別の金属石鹸被膜が生成される成形温度と成形圧力で加圧成形する温間高圧成形工程とからなる。
(1) Molding process The molding pressure applied to the soft magnetic particles in the molding process is not limited, but the higher the density, the higher the density and the higher magnetic flux density of the dust core. As such a high pressure molding method, there is a mold lubrication warm high pressure molding method. The mold lubrication warm high pressure molding method consists of a filling process in which a high-fatty acid lubricant is applied to the inner surface and the magnetic core powder is filled into the mold, and a higher fatty acid-based lubrication between the magnetic core powder and the inner surface of the mold. It comprises a molding temperature at which a metal soap film different from the agent is formed and a warm high-pressure molding process in which molding is performed at a molding pressure.

ここで「温間」とは、表面被膜(または絶縁被膜)への影響や高級脂肪酸系潤滑剤の変質などを考慮して、例えば、成形温度を70℃〜200℃さらには100〜180℃とすることをいう。この金型潤滑温間高圧成形法の詳細については、日本特許公報特許3309970号公報、日本特許4024705号公報など多くの公報に詳細が記載されている。この金型潤滑温間高圧成形法によれば、金型寿命を延しつつも超高圧成形が可能となり、高密度な圧粉磁心を容易に得ることが可能となる。   Here, “warm” means, for example, a molding temperature of 70 ° C. to 200 ° C., further 100 to 180 ° C., taking into consideration the influence on the surface coating (or insulating coating) and alteration of the higher fatty acid lubricant. To do. Details of the mold lubrication warm high pressure molding method are described in many publications such as Japanese Patent Publication No. 3309970 and Japanese Patent No. 4024705. According to this mold lubrication warm high-pressure molding method, ultra-high pressure molding is possible while prolonging the mold life, and a high-density powder magnetic core can be easily obtained.

(2)焼鈍工程
焼鈍工程は、成形体中の残留歪みや残留応力の除去を目的としてなされ、これにより圧粉磁心の保磁力やヒステリシス損失の低減が図られる。この際、低温軟化材は軟化し、軟磁性粒子間の間隙等に流動して、軟磁性粒子をより安定的に保持する。
(2) Annealing step The annealing step is performed for the purpose of removing residual strain and residual stress in the molded body, thereby reducing the coercive force and hysteresis loss of the dust core. At this time, the low-temperature softening material softens and flows into the gaps between the soft magnetic particles to hold the soft magnetic particles more stably.

焼鈍温度は、軟磁性粒子、低温軟化材および高温軟化材の種類に応じて適宜選択し得る。焼鈍温度は、通常、400〜900℃さらには600〜780℃程度である。加熱時間は0.1〜5時間さらには0.5〜2時間程度が好ましく、加熱雰囲気は不活性雰囲気が好ましい。   The annealing temperature can be appropriately selected according to the types of the soft magnetic particles, the low-temperature softening material, and the high-temperature softening material. The annealing temperature is usually about 400 to 900 ° C, further about 600 to 780 ° C. The heating time is preferably about 0.1 to 5 hours, more preferably about 0.5 to 2 hours, and the heating atmosphere is preferably an inert atmosphere.

なお、本発明では、粒界相が無機酸化物から構成され、シリコーン樹脂等を含まないため、高温軟化材の軟化点を超えない範囲内であれば、従来よりも高温の焼鈍ができる。この高温焼鈍によりヒステリシス損失のさらなる低減等を図れる。しかもその際、粒界相の劣化や比抵抗の低減もない。   In the present invention, since the grain boundary phase is composed of an inorganic oxide and does not contain a silicone resin or the like, annealing can be performed at a higher temperature than in the past as long as it does not exceed the softening point of the high-temperature softening material. This high-temperature annealing can further reduce hysteresis loss. In addition, there is no deterioration of the grain boundary phase or reduction of the specific resistance.

《圧粉磁心》
(1)特性
圧粉磁心の密度は、例えば、軟磁性粒子の真密度(ρ)に対する、圧粉磁心の嵩密度(ρ)の比である密度比(ρ/ρ)が83%以上、84%以上、85%以上さらに86%以上であると、高磁気特性が得られるので好ましい。
<Dust core>
(1) Characteristics As for the density of the dust core, for example, the density ratio (ρ / ρ 0 ), which is the ratio of the bulk density (ρ) of the dust core to the true density (ρ 0 ) of the soft magnetic particles, is 83% or more. 84% or more, 85% or more and 86% or more is preferable because high magnetic properties can be obtained.

圧粉磁心の比抵抗は、形状に依存しない圧粉磁心ごとの固有値であり、比抵抗が大きいほど、渦電流損失の低減を図れる。この比抵抗は、例えば、10μΩ・m以上、10μΩ・m以上さらには10μΩ・m以上であると好ましい。 The specific resistance of the dust core is an eigenvalue for each dust core that does not depend on the shape. The larger the specific resistance, the more the eddy current loss can be reduced. For example, the specific resistance is preferably 10 μΩ · m or more, 10 2 μΩ · m or more, and more preferably 10 3 μΩ · m or more.

圧粉磁心の強度は、高いほどその用途が拡大して好ましい。例えば、強度の代表的な指標である圧環強度が、20MPa以上、40MPa以上、60MPa以上さらには80MPa以上であるとよい。本発明の圧粉磁心では、従来の圧粉磁心と異なり、軟磁性粒子同士が単に塑性変形によって機械的に結合しているのみならず、低温軟化材により強固に結合している。このため本発明の圧粉磁心は、従来の圧粉磁心よりも高強度である。   The higher the strength of the powder magnetic core, the more preferable the use is. For example, the crushing strength, which is a representative index of strength, may be 20 MPa or more, 40 MPa or more, 60 MPa or more, or 80 MPa or more. In the dust core of the present invention, unlike the conventional dust core, the soft magnetic particles are not only mechanically bonded by plastic deformation but also firmly bonded by a low-temperature softening material. For this reason, the dust core of the present invention has higher strength than the conventional dust core.

(2)用途
本発明の圧粉磁心は、その形態を問わず、各種の電磁機器、例えば、モータ、アクチュエータ、トランス、誘導加熱器(IH)、スピーカ、リアクトル等に利用され得る。具体的には、電動機または発電機の界磁または電機子を構成する鉄心に用いられると好ましい。中でも、低損失で高出力(高磁束密度)が要求される駆動用モータ用の鉄心に本発明の圧粉磁心は好適である。ちなみに駆動用モータは自動車等に用いられる。
(2) Applications The dust core of the present invention can be used for various electromagnetic devices such as motors, actuators, transformers, induction heaters (IH), speakers, reactors, etc., regardless of the form. Specifically, it is preferably used for an iron core constituting a field or armature of an electric motor or generator. Among these, the dust core of the present invention is suitable for an iron core for a drive motor that requires low loss and high output (high magnetic flux density). Incidentally, the drive motor is used in automobiles and the like.

実施例を挙げて本発明をより具体的に説明する。
《試料の製造》
(原料)
(1)軟磁性粒子
軟磁性粒子(原料粉末)としてSiを含有する鉄合金からなるガス水アトマイズ粉を用意した。用意した軟磁性粒子の組成、粒度は表1Aおよび表2B(両者を併せて単に「表1」という。)に示した。表1に記載の粒度は、所定のメッシュサイズの篩いにより分級して求めたものである。なお、表1中の粒度欄に「〜以下」と記載した軟磁性粒子の場合でも、5μm未満の軟磁性粒子が含まれていなかったことはSEMにより確認している。
The present invention will be described more specifically with reference to examples.
<Production of sample>
(material)
(1) Soft magnetic particles Gas water atomized powder made of an iron alloy containing Si was prepared as soft magnetic particles (raw material powder). The compositions and particle sizes of the prepared soft magnetic particles are shown in Table 1A and Table 2B (both are simply referred to as “Table 1”). The particle sizes listed in Table 1 are obtained by classification using a sieve having a predetermined mesh size. In addition, even in the case of soft magnetic particles described as “˜” in the particle size column in Table 1, it was confirmed by SEM that no soft magnetic particles of less than 5 μm were contained.

(2)低融点ガラス粒子(低温軟化材)
軟磁性粒子の表面に付着させる低融点ガラス粒子を次の湿式粉砕により得た。原料として、表2に示す各種の組成(第一無機酸化物)からなるガラスビーズを用意した。なお、表2に示した低融点ガラス粒子A、B、DおよびEは日本琺瑯釉薬株式会社製、低融点ガラス粒子CおよびFは東罐マテリアル・テクノロジー株式会社製である。
(2) Low melting point glass particles (low temperature softening material)
Low melting point glass particles adhered to the surface of the soft magnetic particles were obtained by the following wet pulverization. Glass beads made of various compositions (first inorganic oxide) shown in Table 2 were prepared as raw materials. In addition, the low melting glass particles A, B, D, and E shown in Table 2 are manufactured by Nippon Glaze Co., Ltd., and the low melting glass particles C and F are manufactured by Toago Material Technology Co., Ltd.

粗粉砕したガラスビーズを湿式粉砕機(ダイノーミル:シンマルエンタープライズ社製)のチャンバーへ投入し、攪拌用プロペラを作動させて微粉砕した。この微粉砕したものを回収して乾燥させた。こうして各種の低融点ガラス粒子からなる粉末を得た。得られた低融点ガラス粒子の各粒径は表2に併せて示した。なお、この粒径は走査型電子顕微鏡(SEM)による画像解析により測定した。   The roughly pulverized glass beads were put into a chamber of a wet pulverizer (Dynomill: manufactured by Shinmaru Enterprise Co., Ltd.) and finely pulverized by operating a propeller for stirring. This finely pulverized product was collected and dried. Thus, powders composed of various low-melting glass particles were obtained. Each particle size of the obtained low melting point glass particles is shown together in Table 2. The particle size was measured by image analysis using a scanning electron microscope (SEM).

(3)ナノ粒子(高温軟化材)
軟磁性粒子の表面に付着させるセラミックスのナノ粒子(高温軟化材)を用意した。用意したナノ粒子の種類および平均粒径は表1に示した。なお、表1に示したシリカ製ナノ粒子は、いずれも組成がSiOであり、平均粒径15nmのものは株式会社トクヤマ製(品番:QS−10)である。平均粒径300nmのものは株式会社アドマテックス製(品番:SO−E1)である。またアルミナ製ナノ粒子は、組成がAlであり、ビューラー社製(マイクロポリッシュII)である。
(3) Nano particles (high temperature softening material)
Ceramic nanoparticles (high-temperature softening material) to be attached to the surface of the soft magnetic particles were prepared. The types and average particle diameters of the prepared nanoparticles are shown in Table 1. Incidentally, silica nanoparticles, shown in Table 1 are both SiO 2 in composition, the average particle diameter 15nm those manufactured by Tokuyama Corp. (Part: QS-10) is. Those having an average particle diameter of 300 nm are manufactured by Admatechs Co., Ltd. (product number: SO-E1). The alumina nanoparticles have a composition of Al 2 O 3 and are manufactured by Buehler (Micro Polish II).

ナノ粒子の平均粒径の特定方法には、レーザ回折散乱法、沈降法、画像解析法等があるが、本発明ではレーザ回折散乱法によってナノ粒子の平均粒径を特定した。   Examples of the method for specifying the average particle size of the nanoparticles include a laser diffraction scattering method, a sedimentation method, and an image analysis method. In the present invention, the average particle size of the nanoparticles was specified by the laser diffraction scattering method.

(磁心用粉末の製造)
軟磁性粒子の表面に低融点ガラス粒子およびナノ粒子を、次に示す各方式により付着させた(付着層形成工程)。
(Manufacture of magnetic core powder)
Low melting glass particles and nanoparticles were adhered to the surface of the soft magnetic particles by the following methods (adhesion layer forming step).

(1)湿式付着工程
先ず、上述した軟磁性粒子およびナノ粒子の各粉末を入れたチャンバーを容器回転揺動型粉体混合機(愛知電機株式会社製ロッキングミキサー)に取り付けて、各粉末を攪拌混合した。この混合は80rpmの条件で30分間行った。こうしてナノ粒子が表面に付着した軟磁性粒子(これを「一次複合粒子」という。)を得た。
(1) Wet adhesion process First, the chamber containing the above-mentioned soft magnetic particle and nano particle powders is attached to a container rotating and shaking type powder mixer (a rocking mixer manufactured by Aichi Electric Co., Ltd.), and each powder is stirred. Mixed. This mixing was performed for 30 minutes at 80 rpm. In this way, soft magnetic particles (hereinafter referred to as “primary composite particles”) having nanoparticles adhered to the surface were obtained.

次に、上記の低融点ガラス粒子を、その5〜20倍の分散媒(エタノール)に分散させた低融点ガラス分散液を調製した。このときの分散には、超音波撹拌装置を用いた。   Next, a low-melting-point glass dispersion in which the above-described low-melting-point glass particles were dispersed in a dispersion medium (ethanol) 5 to 20 times as large as the above-mentioned low-melting glass particles was prepared. An ultrasonic stirrer was used for dispersion at this time.

この低融点ガラス分散液中へ、上述した一次複合粒子の粉末を入れ、分散媒が揮発するまで超音波撹拌装置で攪拌した。この際、低融点ガラス分散液の温度は60〜70℃とした。さらに、この処理後の粉末を130℃の恒温槽に入れて大気雰囲気中で30分間乾燥させた。乾燥後に固化していた粉末は乳鉢で解砕した。こうして軟磁性粒子の表面にナノ粒子および低融点ガラス粒子が付着した複合粒子からなる粉末(磁心用粉末)を得た。   The powder of the primary composite particles described above was put into this low-melting glass dispersion and stirred with an ultrasonic stirrer until the dispersion medium volatilized. At this time, the temperature of the low-melting glass dispersion was 60 to 70 ° C. Further, the powder after the treatment was placed in a constant temperature bath at 130 ° C. and dried in the air atmosphere for 30 minutes. The powder that had solidified after drying was crushed in a mortar. Thus, a powder (magnetic core powder) composed of composite particles in which nanoparticles and low-melting glass particles were adhered to the surface of soft magnetic particles was obtained.

(2)乾式付着工程
前述した一次複合粒子と低融点ガラス粒子の各粉末を入れたポリ容器を回転ボールミル(筒井理化学器械株式会社製)に取り付けて攪拌混合した。この混合は60rpmの条件で30分間行った。混合後に固化していた粉末は乳鉢で解砕した。こうして軟磁性粒子の表面にナノ粒子および低融点ガラス粒子が付着した複合粒子からなる磁心用粉末を得た。
(2) Dry adhesion process A polycontainer containing the primary composite particles and low melting point glass particles described above was attached to a rotating ball mill (manufactured by Tsutsui Rika Kikai Co., Ltd.) and mixed with stirring. This mixing was performed for 30 minutes at 60 rpm. The powder that had solidified after mixing was crushed in a mortar. Thus, a magnetic core powder comprising composite particles in which nanoparticles and low-melting glass particles were adhered to the surface of soft magnetic particles was obtained.

(3)同時乾式付着工程
軟磁性粒子、ナノ粒子および低融点ガラス粒子の各粉末を同時に入れたポリ容器を、上記の容器回転揺動型粉体混合機に取り付けて攪拌混合した。この混合は80rpmの条件で30分間行った。混合後に固化していた粉末は乳鉢で解砕した。こうして軟磁性粒子の表面にナノ粒子および低融点ガラス粒子が付着した複合粒子からなる磁心用粉末を得た。
(3) Simultaneous dry adhesion process A polycontainer in which each powder of soft magnetic particles, nanoparticles, and low-melting-point glass particles was simultaneously placed was attached to the container rotating and oscillating powder mixer and mixed with stirring. This mixing was performed for 30 minutes at 80 rpm. The powder that had solidified after mixing was crushed in a mortar. Thus, a magnetic core powder comprising composite particles in which nanoparticles and low-melting glass particles were adhered to the surface of soft magnetic particles was obtained.

いずれの場合も磁心用粉末全体を100質量%として、低融点ガラス粒子(低温軟化材)の添加量(m1)およびナノ粒子(高温軟化材)の添加量(m2)を表1にそれぞれ示した。また表1中に示した「付着粒子全体に対する割合」は、両添加量の和(m1+m2)に対するナノ粒子の添加量の割合(m2/(m1+m2))の百分率である。また、表1A中では、湿式付着工程を「湿式」、乾式付着工程を「乾式」、同時乾式付着工程を「同時乾式」と表記した。   In either case, the total amount of the magnetic core powder was 100% by mass, and the addition amount (m1) of the low melting point glass particles (low temperature softening material) and the addition amount (m2) of the nanoparticles (high temperature softening material) are shown in Table 1, respectively. . In addition, the “ratio to the total amount of adhered particles” shown in Table 1 is a percentage of the ratio of the added amount of nanoparticles (m2 / (m1 + m2)) to the sum of both added amounts (m1 + m2). In Table 1A, the wet deposition process is represented as “wet”, the dry deposition process as “dry”, and the simultaneous dry deposition process as “simultaneous dry”.

(4)比較試料の製造
軟磁性粒子の表面に、低融点ガラス粒子またはナノ粒子のいずれか一方のみを付着させた複合粒子からなる磁心用粉末も製造した。低融点ガラス粒子のみの試料は、上述の乾式付着工程と同様に製造した。ナノ粒子のみの試料は、上述の一次複合粒子と同様に製造した。これらの試料をまとめて表1Bの試料No.C1〜C7に示した。
(4) Manufacture of Comparative Sample Magnetic core powder made of composite particles in which only one of low melting point glass particles or nanoparticles was attached to the surface of soft magnetic particles was also manufactured. A sample having only low melting point glass particles was produced in the same manner as in the above-described dry adhesion process. A sample containing only nanoparticles was produced in the same manner as the primary composite particles described above. These samples are collectively shown as sample No. 1 in Table 1B. Shown in C1-C7.

また、軟磁性粒子の表面にナノ粒子およびシリコーン樹脂を付着させた複合粒子からなる磁心用粉末も製造した(表3に示す試料No.D1およびD2)。この際の付着は次のようにしておこなった。先ず、シリコーン樹脂を、その50〜80倍の分散媒(エタノール)に溶解し、この溶液とナノ粒子を混合したコーティング液を調製した。次に、このコーティング液に軟磁性粒子を混合し、分散媒が揮発するまで超音波攪拌装置で攪拌した。この際のコーティング液の温度は60〜70℃とした。さらに、この処理後の粉末を恒温槽に入れて大気雰囲気中で30分間乾燥させた。このときの恒温槽の温度は、試料No.D1の場合が130℃、試料No.D2の場合が100℃とした。乾燥後に固化していた粉末は乳鉢で解砕した。なお、シリコーン樹脂には熱硬化型シリコーン樹脂(信越化学工業株式会社製KR−242A)を用いた。ナノ粒子には、平均粒径50nmのシリカ製ナノ粒子とシリカゾル(日産化学工業株式会社製IPA−ST、ナノ粒子濃度30%)を用いた。   In addition, magnetic core powders composed of composite particles in which nanoparticles and silicone resin were adhered to the surface of soft magnetic particles were also produced (sample Nos. D1 and D2 shown in Table 3). The adhesion at this time was performed as follows. First, a silicone resin was dissolved in 50 to 80 times its dispersion medium (ethanol) to prepare a coating liquid in which this solution and nanoparticles were mixed. Next, soft magnetic particles were mixed into this coating solution, and stirred with an ultrasonic stirring device until the dispersion medium volatilized. The temperature of the coating liquid at this time was 60 to 70 ° C. Further, the powder after the treatment was put in a thermostatic bath and dried for 30 minutes in an air atmosphere. The temperature of the thermostatic chamber at this time is the sample No. In the case of D1, the sample No. The case of D2 was 100 ° C. The powder that had solidified after drying was crushed in a mortar. In addition, the thermosetting silicone resin (Shin-Etsu Chemical Co., Ltd. KR-242A) was used for the silicone resin. As nanoparticles, silica nanoparticles having an average particle diameter of 50 nm and silica sol (IPA-ST, Nissan Chemical Industries, Ltd., nanoparticle concentration: 30%) were used.

(圧粉磁心の製造)
(1)充填工程および成形工程
各試料(磁心用粉末)を用いて金型潤滑温間高圧成形法により、リング状(外径:φ39mm×内径φ30mm×厚さ5mm)の成形体を製作した。この成形に際して、内部潤滑剤や樹脂バインダー等は一切使用しなかった。金型潤滑温間高圧成形法は、具体的には次のようにして行った。
(Manufacture of dust core)
(1) Filling Step and Molding Step A ring-shaped (outside diameter: φ39 mm × inside diameter φ30 mm × thickness 5 mm) shaped body was manufactured by using a mold lubrication warm high pressure molding method using each sample (magnetic core powder). No internal lubricant or resin binder was used at the time of molding. Specifically, the die lubrication warm high pressure molding method was performed as follows.

所望形状に応じたキャビティを有する超硬製の金型を用意した。この金型をバンドヒータで予め130℃に加熱しておいた。また、この金型の内周面には、予めTiNコート処理を施し、その表面粗さを0.4Zとした。   A cemented carbide mold having a cavity corresponding to a desired shape was prepared. This mold was previously heated to 130 ° C. with a band heater. Further, the inner peripheral surface of this mold was previously subjected to TiN coating treatment, and the surface roughness was set to 0.4Z.

加熱した金型の内周面に、水溶液に分散させたステアリン酸リチウム(1%)をスプレーガンにて10cm/分程度の割合で均一に塗布した。ここで用いた水溶液は、水に界面活性剤と消泡剤とを添加したものである。界面活性剤には、ポリオキシエチレンノニルフェニルエーテル(EO)6、(EO)10及びホウ酸エステルエマルボンT−80を用い、それぞれを水溶液全体(100体積%)に対して1体積%ずつ添加した。また、消泡剤には、FSアンチフォーム80を用い、水溶液全体(100体積%)に対して0.2体積%添加した。 Lithium stearate (1%) dispersed in an aqueous solution was uniformly applied to the inner peripheral surface of the heated mold at a rate of about 10 cm 3 / min with a spray gun. The aqueous solution used here is obtained by adding a surfactant and an antifoaming agent to water. As the surfactant, polyoxyethylene nonylphenyl ether (EO) 6, (EO) 10 and borate ester Emulbon T-80 were used, and each was added by 1% by volume with respect to the entire aqueous solution (100% by volume). did. As the antifoaming agent, FS Antifoam 80 was used and 0.2% by volume was added to the entire aqueous solution (100% by volume).

ステアリン酸リチウムには、融点が約225℃で、粒径が20μmのものを用いた。その分散量は、上記水溶液100cmに対して25gとした。これをさらにボールミル式粉砕装置で微細化処理(テフロン(登録商標)コート鋼球:100時間)し、得られた原液を20倍に希釈して最終濃度1%の水溶液として、上記塗布工程に供した。 A lithium stearate having a melting point of about 225 ° C. and a particle size of 20 μm was used. The dispersion amount was 25 g with respect to 100 cm 3 of the aqueous solution. This was further refined with a ball mill type pulverizer (Teflon (registered trademark) coated steel balls: 100 hours), and the obtained stock solution was diluted 20 times to obtain an aqueous solution having a final concentration of 1%, which was used in the coating step. did.

ステアリン酸リチウムが内面に塗布された金型へ、各磁心用粉末を充填した(充填工程)。金型を130℃に保持したまま、基本的に1568MPaの成形圧力で、充填された磁心用粉末を温間加圧成形した(成形工程)。なお、この温間高圧成形に際して、いずれの磁心用粉末も金型とかじり等を生じることがなく低い抜圧で成形体をその金型から取り出すことができた。   Each metal core powder was filled in a mold having lithium stearate coated on the inner surface (filling step). With the mold held at 130 ° C., the filled magnetic core powder was warm-pressed under a molding pressure of 1568 MPa (molding process). In this warm high-pressure molding, none of the magnetic core powders was galling with the mold, and the molded body could be taken out from the mold with a low pressure.

なお、上述した金型温度(130℃)は、試料No.D1の場合は150℃に、試料No.D2の場合は70℃に変更して行った。   The mold temperature (130 ° C.) described above is the same as the sample No. In the case of D1, the sample No. In the case of D2, the temperature was changed to 70 ° C.

(2)焼鈍工程
得られた各成形体に、流量8リットル/分の窒素雰囲気中で、炉内温度を750℃として、1時間保持する焼鈍を施した。但し、試料No.17は900℃で焼鈍した。こうして表1に示す複数の圧粉磁心を得た。
(2) Annealing process Each obtained compact was annealed at a furnace temperature of 750 ° C. for 1 hour in a nitrogen atmosphere with a flow rate of 8 liters / minute. However, sample No. No. 17 was annealed at 900 ° C. Thus, a plurality of dust cores shown in Table 1 were obtained.

《測定》
(1)比抵抗と圧環強度
上記のリング状の圧粉磁心を用いて圧環強度および比抵抗を測定した。圧環強度は、JIS Z 2507に準ずる方法により測定した。比抵抗は、デジタルマルチメータ(メーカ:(株)エーディーシー、型番:R6581)を用いて4端子法により測定した。各測定結果を表1に併せて示した。また各圧粉磁心の比抵抗と圧環強度との相関を図3にプロットした。
<Measurement>
(1) Specific resistance and crumbling strength The crumbling strength and specific resistance were measured using the above ring-shaped dust core. The crushing strength was measured by a method according to JIS Z 2507. The specific resistance was measured by a 4-terminal method using a digital multimeter (manufacturer: ADC, Inc., model number: R6581). Each measurement result was combined with Table 1 and shown. Further, the correlation between the specific resistance of each dust core and the crushing strength is plotted in FIG.

(2)密度
圧粉磁心の密度は、各試料(試験片)の質量と採寸から求まる体積に基づいて求めた。
(2) Density The density of the dust core was determined based on the volume determined from the mass and measurement of each sample (test piece).

《観察》
(1)表1Aに示した試料No.2の圧粉磁心の粒界相を、走査型電子顕微鏡(SEM)で観察した反射電子組織像を図2に示した。図2中、白色部位は軟磁性粒子であり、灰色部位は低融点ガラス相(低温軟化材相)であり、黒色部位はシリカ(SiO)相(高温軟化材相)である。この図2から、本発明に係る圧粉磁心では、軟磁性粒子の表面に密着してそれを被包する粒界相が、低温軟化材からなるマトリックス中に、高温軟化材からなるナノ粒子が一体化しつつ分散した複合分散組織となっていることが明らかとなった。
<< Observation >>
(1) Sample No. shown in Table 1A A reflection electron structure image obtained by observing the grain boundary phase of No. 2 dust core with a scanning electron microscope (SEM) is shown in FIG. In FIG. 2, the white part is soft magnetic particles, the gray part is a low-melting glass phase (low temperature softening material phase), and the black part is a silica (SiO 2 ) phase (high temperature softening material phase). From FIG. 2, in the powder magnetic core according to the present invention, the grain boundary phase that is in close contact with the surface of the soft magnetic particles and encapsulates the nanoparticles is composed of nanoparticles made of the high-temperature softening material in the matrix made of the low-temperature softening material. It became clear that it became a composite dispersed structure that was integrated and dispersed.

(2)このような粒界相が形成されることは、低融点ガラス粒子(低温軟化材)のみからなる試料と、この低融点ガラス粒子にナノ粒子(高温軟化材)を加えた試料とについて行った示差熱分析(DTA:Differential Thermal Analysis)の結果からも裏付けられる。これら両試料のDTA曲線を図4に示す。図4に示したグラフの縦軸は、各試料と基準物質との温度差ΔTに相当する電圧差とした。 (2) The formation of such a grain boundary phase is about a sample made of only low melting point glass particles (low temperature softening material) and a sample obtained by adding nanoparticles (high temperature softening material) to the low melting point glass particles. This is also supported by the results of the differential thermal analysis (DTA) performed. The DTA curves for both these samples are shown in FIG. The vertical axis of the graph shown in FIG. 4 is a voltage difference corresponding to the temperature difference ΔT between each sample and the reference material.

ここで用いた低融点ガラス粒子は、表2に示す硼珪酸塩系ガラス(A)である。低融点ガラス粒子に加えたナノ粒子は、平均粒径15nmのシリカ粒子であり、その混合割合は30質量%とした(試料No.2相当)。なお、混合試料は、低融点ガラス粒子とナノ粒子をメノウ乳鉢で混合して得た。またDTAは、理学電機株式会社製の熱分析装置(TG8120)を用いて、昇温速度10℃/min、大気雰囲気で行った。   The low melting point glass particles used here are borosilicate glass (A) shown in Table 2. The nanoparticles added to the low-melting glass particles were silica particles having an average particle diameter of 15 nm, and the mixing ratio was 30% by mass (corresponding to sample No. 2). The mixed sample was obtained by mixing low melting point glass particles and nanoparticles in an agate mortar. Moreover, DTA was performed in the air | atmosphere atmosphere with the temperature increase rate of 10 degree-C / min using the thermal analyzer (TG8120) by Rigaku Corporation.

図4から明らかなように、低融点ガラス粒子のみからなる試料のDTA曲線には軟化点(590℃)付近に安定域が存在するが、混合試料(低融点ガラス粒子+ナノ粒子)のDTA曲線にはそのような安定域が観られなかった。この安定域は、低融点ガラス粒子の軟化もしくは溶融に伴う吸熱反応により生じると考えられる。しかし、混合試料の場合、ナノ粒子(シリカ粒子)が昇温と共に低融点ガラス粒子と反応して徐々に溶解し、上述した吸熱反応が不明確となって安定域が出現しなくなったと考えられる。   As is clear from FIG. 4, the DTA curve of the sample consisting only of the low melting point glass particles has a stable region near the softening point (590 ° C.), but the DTA curve of the mixed sample (low melting point glass particles + nanoparticles). Did not see such a stable range. This stable region is considered to be caused by an endothermic reaction accompanying softening or melting of the low-melting glass particles. However, in the case of the mixed sample, it is considered that the nanoparticles (silica particles) react with the low-melting glass particles as the temperature rises and gradually dissolve, the endothermic reaction described above becomes unclear, and the stable region does not appear.

なお、このような傾向は、硼珪酸塩系ガラス粒子とシリカ粒子とを組み合わせた場合に限らず、他種の低融点ガラス粒子とナノ粒子とを組み合わせた場合も同様と考えられる。何故なら、低融点ガラス粒子の溶融によるナノ粒子の反応は低融点ガラス粒子が先に溶融することで起こる。従って、低融点ガラス粒子の種類によらず、低温軟化材である低融点ガラス粒子の方が、高温軟化材であるナノ粒子より先に軟化あるいは溶融するため、吸熱反応が不明確となって安定域が出現しなくなると考えられるからである。   Such a tendency is not limited to the case where the borosilicate glass particles and the silica particles are combined, but is also considered to be the same when the other types of low melting point glass particles and the nanoparticles are combined. This is because the reaction of the nanoparticles due to the melting of the low-melting glass particles occurs when the low-melting glass particles are melted first. Therefore, regardless of the type of low-melting glass particles, low-melting glass particles that are low-temperature softening materials soften or melt before nanoparticles that are high-temperature softening materials, so the endothermic reaction is unclear and stable. This is because it is considered that the area will not appear.

《評価》
(1)表1および図3から試料No.1〜18の圧粉磁心はいずれも、高密度(6.9g/cm 以上)であり磁気特性に優れると共に、圧環強度および比抵抗の両方に優れることがわかった。具体的には、比抵抗が10μΩ・m以上、10μΩ・m以上さらには、10μΩ・m以上のものがあり、圧環強度も20〜89MPaと高強度であった。
<Evaluation>
(1) From Table 1 and FIG. It was found that all of the dust cores 1 to 18 had high density (6.9 g / cm 3 or more), excellent magnetic properties, and excellent crushing strength and specific resistance. Specifically, the specific resistance is 10 μΩ · m or more, 10 2 μΩ · m or more, further 10 3 μΩ · m or more, and the crushing strength is as high as 20 to 89 MPa.

これらのことは、図3上にプロットした試料No.1〜18のマークが、試料No.C1、C2、C4〜C7、D1およびD2のマークよりも、全体的に右上方向へシフトしていることからもわかる。   These are the same as the sample No. plotted on FIG. The marks 1 to 18 indicate the sample numbers. It can also be seen from the fact that the marks are shifted to the upper right as a whole rather than the marks C1, C2, C4 to C7, D1 and D2.

ちなみに、低融点ガラス粒子の添加量が多いほど圧環強度が増加し、ナノ粒子の添加量が多いほど比抵抗が増加した。この傾向は、軟磁性粒子の粒度、低融点ガラス粒子の種類、ナノ粒子の粒度や種類、付着工程の方式等が異なっても同様であった。   Incidentally, the crushing strength increased as the amount of low melting point glass particles added increased, and the specific resistance increased as the amount of nanoparticles added increased. This tendency was the same even when the particle size of the soft magnetic particles, the type of the low-melting glass particles, the particle size and type of the nanoparticles, the method of the adhesion process, and the like were different.

(2)試料No.C1および試料No.C4〜C7からわかるように、粒界相が低温軟化材のみからなる場合、圧環強度は高いが比抵抗が極端に低くなった。この傾向は低融点ガラス粒子の種類や添加量が変化しても同様であった。 (2) Sample No. C1 and Sample No. As can be seen from C4 to C7, when the grain boundary phase is composed only of the low-temperature softening material, the crushing strength is high, but the specific resistance is extremely low. This tendency was the same even when the type and amount of the low melting point glass particles were changed.

また試料No.C2からわかるように、粒界相が高温軟化材のみからなる場合、比抵抗は高くなるが圧環強度は非常に低くなった。そして試料No.C3からわかるように、高温軟化材が増加すると、超高圧成形しているにもかかわらず、正常な成形体が得られなかった。   Sample No. As can be seen from C2, when the grain boundary phase is composed only of the high-temperature softening material, the specific resistance is increased, but the crushing strength is very low. And sample no. As can be seen from C3, when the high-temperature softening material increased, a normal molded body could not be obtained despite the ultra-high pressure molding.

(3)試料No.D1およびD2からわかるように、粒界相がシリコーン樹脂とシリカ粒子からなる圧粉磁心は、圧環強度が極端に低下することがわかる。これは、焼鈍時に高温軟化材の一部が軟化または溶融しても、シリコーン樹脂と一体化しないためである。また、粒界相にシリコーン樹脂が含まれる圧粉磁心に比べ、本実施例に係る各試料は、高温で焼鈍しても、高い比抵抗と共に十分に大きな圧環強度も保持している。特に試料No.17の圧粉磁心は、従来にない非常に高い温度(900℃)で焼鈍しているにも拘わらず、高い比抵抗と共に大きな圧環強度を発揮している。 (3) Sample No. As can be seen from D 1 and D 2, it can be seen that the dust core having a grain boundary phase composed of silicone resin and silica particles has an extremely reduced crushing strength. This is because even if a part of the high-temperature softening material is softened or melted during annealing, it is not integrated with the silicone resin. In addition, each sample according to this example retains a sufficiently high crushing strength as well as a high specific resistance even when annealed at a high temperature, compared to a powder magnetic core containing a silicone resin in the grain boundary phase. In particular, sample no. Although the powder magnetic core of 17 is annealed at a very high temperature (900 ° C.), which is not conventional, it exhibits a large crushing strength with a high specific resistance.

以上から本発明の圧粉磁心は、軟磁性粒子間の粒界相が低温軟化材および高温軟化材で構成され、それらが相乗的に作用することにより、高比抵抗と高強度を両立し得ることがわかった。さらに本発明の圧粉磁心は、その優れた特性を高温環境下でも安定して発現し得ることもわかった。   From the above, in the dust core of the present invention, the grain boundary phase between the soft magnetic particles is composed of the low-temperature softening material and the high-temperature softening material, and they can act synergistically to achieve both high specific resistance and high strength. I understood it. Furthermore, it has also been found that the powder magnetic core of the present invention can stably exhibit its excellent characteristics even in a high temperature environment.

Claims (12)

軟磁性粒子からなる主相と、
該軟磁性粒子間に形成される粒界相と、
からなる圧粉磁心であって、
前記粒界相は、
該軟磁性粒子の焼鈍温度よりも低い軟化点を有する第一無機酸化物からなる低温軟化材と該焼鈍温度よりも高い軟化点を有する第二無機酸化物からなる高温軟化材とが複合してなることを特徴とする圧粉磁心。
A main phase composed of soft magnetic particles;
A grain boundary phase formed between the soft magnetic particles;
A dust core consisting of
The grain boundary phase is
A low-temperature softening material composed of a first inorganic oxide having a softening point lower than the annealing temperature of the soft magnetic particles is combined with a high-temperature softening material composed of a second inorganic oxide having a softening point higher than the annealing temperature. A dust core characterized in that
前記粒界相は、前記低温軟化材からなるマトリックス中に、前記高温軟化材からなり前記軟磁性粒子よりも粒径が小さい微粒子が分散した複合分散組織を有する請求項1に記載の圧粉磁心。   2. The dust core according to claim 1, wherein the grain boundary phase has a composite dispersed structure in which fine particles made of the high-temperature softening material and having a smaller particle diameter than the soft magnetic particles are dispersed in a matrix made of the low-temperature softening material. . 前記微粒子は、平均粒径が5〜500nmのナノ粒子である請求項2に記載の圧粉磁心。   The dust core according to claim 2, wherein the fine particles are nanoparticles having an average particle diameter of 5 to 500 nm. 前記微粒子は、シリカ粒子またはアルミナ粒子である請求項2または3に記載の圧粉磁心。   The dust core according to claim 2 or 3, wherein the fine particles are silica particles or alumina particles. 前記低温軟化材は、低融点ガラスである請求項1〜4のいずれかに記載の圧粉磁心。   The dust core according to any one of claims 1 to 4, wherein the low-temperature softening material is low-melting glass. 前記低融点ガラスは、硼珪酸塩系ガラス、珪酸塩系ガラスまたはリン酸塩系ガラスの一種以上である請求項5に記載の圧粉磁心。   The dust core according to claim 5, wherein the low melting glass is one or more of borosilicate glass, silicate glass, or phosphate glass. 前記軟磁性粒子は、純鉄またはケイ素(Si)を含有する鉄合金からなる請求項1〜6のいずれかに記載の圧粉磁心。   The dust core according to claim 1, wherein the soft magnetic particles are made of an iron alloy containing pure iron or silicon (Si). 前記軟磁性粒子は、粒径が5〜500μmである請求項1または7に記載の圧粉磁心。   The powder magnetic core according to claim 1, wherein the soft magnetic particles have a particle size of 5 to 500 μm. 前記高温軟化材と前記低温軟化材は、少なくとも界面部分で融合している請求項1〜8に記載の圧粉磁心。   The dust core according to claim 1, wherein the high-temperature softening material and the low-temperature softening material are fused at least at an interface portion. 前記低温軟化材は、低融点ガラスであり、
前記高温軟化材は、シリカであり、
前記粒界相は、該低融点ガラスからなるマトリックス中に該シリカからなるシリカ濃化相が分散した複合分散組織を有する請求項9に記載の圧粉磁心。
The low-temperature softening material is a low-melting glass,
The high temperature softening material is silica,
The powder magnetic core according to claim 9, wherein the grain boundary phase has a composite dispersed structure in which a silica concentrated phase made of silica is dispersed in a matrix made of the low melting point glass.
軟磁性粒子と、
該軟磁性粒子の焼鈍温度よりも低い軟化点を有する第一無機酸化物からなる低温軟化材と該焼鈍温度よりも高い軟化点を有する第二無機酸化物からなる高温軟化材とが該軟磁性粒子の表面に付着してなる付着層と、
からなることを特徴とする圧粉磁心に用いられる磁心用粉末。
Soft magnetic particles,
A low temperature softening material comprising a first inorganic oxide having a softening point lower than the annealing temperature of the soft magnetic particles and a high temperature softening material comprising a second inorganic oxide having a softening point higher than the annealing temperature An adhesion layer formed on the surface of the particles;
A powder for a magnetic core used for a dust core characterized by comprising:
請求項11に記載の磁心用粉末を金型に充填する充填工程と、
該金型内の磁心用粉末を加圧成形する成形工程と、
該成形工程後に得られた成形体を、前記低温軟化材の軟化点以上かつ前記高温軟化材の軟化点未満の温度で焼鈍する焼鈍工程と、
を備えることを特徴とする圧粉磁心の製造方法。
A filling step of filling a mold with the magnetic core powder according to claim 11;
A molding step of pressure-molding the magnetic core powder in the mold;
An annealing step of annealing the molded body obtained after the molding step at a temperature equal to or higher than the softening point of the low-temperature softening material and lower than the softening point of the high-temperature softening material;
A method for producing a powder magnetic core comprising the steps of:
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