JPH03278501A - Soft magnetic core material and manufacture thereof - Google Patents
Soft magnetic core material and manufacture thereofInfo
- Publication number
- JPH03278501A JPH03278501A JP2079841A JP7984190A JPH03278501A JP H03278501 A JPH03278501 A JP H03278501A JP 2079841 A JP2079841 A JP 2079841A JP 7984190 A JP7984190 A JP 7984190A JP H03278501 A JPH03278501 A JP H03278501A
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- JP
- Japan
- Prior art keywords
- magnetic core
- deposited
- magnetic
- solidified
- core material
- Prior art date
- Legal status (The legal status is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the status listed.)
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Abstract
Description
【発明の詳細な説明】
(産業上の利用分野)
本発明は、トランス、インダクタ、電磁ソレノイド、モ
ータなどに用いられる高周波用の軟質磁心材料およびそ
の製造方法に関するものである。DETAILED DESCRIPTION OF THE INVENTION (Field of Industrial Application) The present invention relates to a high-frequency soft magnetic core material used in transformers, inductors, electromagnetic solenoids, motors, etc., and a method for manufacturing the same.
(従来の技術)
従来、交流もしくは直流パルスで動作するトランス、イ
ンダクタ、電磁ソレノイド、モータなどの磁心材料とし
ては、フェライト磁心、絶縁処理したFe−Si合金や
Fe−Ni合金等の金属薄板を使った積層磁心、金属系
磁性粉を絶縁処理だのち加圧成形した圧粉磁心などが主
に使用されている。(Prior art) Conventionally, ferrite magnetic cores and thin metal plates such as insulated Fe-Si alloys and Fe-Ni alloys have been used as magnetic core materials for transformers, inductors, electromagnetic solenoids, motors, etc. that operate with alternating current or direct current pulses. Mainly used are laminated magnetic cores and powder magnetic cores made of metal-based magnetic powder that is insulated and then pressure-formed.
しかし、フェライ+−m心は、透磁率が高く磁心損失も
小さいという長所はあるものの、磁束密度が低り0.5
テスラ程度しか得られない、又、金属薄板を使った積層
磁心は磁束密度および透磁率は高いが、高周波域では渦
電流の増大により磁心損失が大きくなるため、一般には
数KHz〜数十KH2が使用出来る周波数の限界である
。However, although the Ferrite+-m core has the advantage of high magnetic permeability and low core loss, it has a low magnetic flux density of 0.5
Although laminated magnetic cores made of thin metal plates have high magnetic flux density and magnetic permeability, magnetic core loss increases due to increased eddy current in the high frequency range, so generally several KHz to several tens of KH2 are obtained. This is the limit of frequencies that can be used.
一方、圧粉磁心は磁束密度が比較的高く磁心損失も小さ
いが、透磁率が低いという問題点がある。On the other hand, powder magnetic cores have a relatively high magnetic flux density and low core loss, but have a problem of low magnetic permeability.
圧粉磁心の透磁率がフェライトコアや金属薄板の積層コ
アに対して低い土な理由は、圧粉成形では相対密度が特
開昭63−137142号公報に開示されているように
90%前後と小さいため、高透磁率の磁性粉を使用して
も粒子間空隙の影響でバルクとしての透磁率が低下する
ためである。又、相対密度を増加するため、絶縁用バイ
ンダー量の減少や成形圧力の増加などを図っても90%
を大きく上回る相対密度を得ることは極めて難しく、却
って粒間の絶縁不良による粒子間渦電流の増加に伴う磁
心損失増加を招くという結果になっていた。The reason why the permeability of the powder magnetic core is lower than that of the ferrite core or the laminated core of thin metal sheets is because the relative density in powder compacting is around 90% as disclosed in JP-A-63-137142. This is because the bulk magnetic permeability decreases due to the influence of interparticle gaps even if magnetic powder with high magnetic permeability is used because of its small size. In addition, even if efforts are made to increase the relative density by reducing the amount of insulating binder or increasing the molding pressure, the
It is extremely difficult to obtain a relative density that greatly exceeds , and the result is that the core loss increases due to an increase in interparticle eddy current due to poor insulation between the particles.
以上の様に、従来の磁心材料には磁束密度が高く、透磁
率が高く磁心損失が小さいという特性を併せ持つものが
なかった。As described above, none of the conventional magnetic core materials has the characteristics of high magnetic flux density, high magnetic permeability, and low core loss.
(発明が解決しようとする課題)
ところが、近年、電子機器の小型化高密度化に伴い、こ
れらに使用されるトランス、インダクタ等の小型化、高
周波化要求が急速に高まってきている。このため、高磁
束密度で透磁率が高く磁心損失が小さいという特性を併
せもつ磁心材料が求められている。(Problems to be Solved by the Invention) However, in recent years, as electronic devices have become smaller and more densely packed, demands for smaller size and higher frequency of transformers, inductors, etc. used in these devices have rapidly increased. Therefore, there is a need for a magnetic core material that has the characteristics of high magnetic flux density, high magnetic permeability, and low core loss.
本発明は、上記の事情に鑑み、高磁束密度で透磁率が高
く磁心損失が小さいという特性を併せもつ軟質磁心材料
とその製造方法の提供を目的とするものである。In view of the above circumstances, the present invention aims to provide a soft magnetic core material having the characteristics of high magnetic flux density, high magnetic permeability, and low core loss, and a method for manufacturing the same.
(課題を解決するための手段および作用)本発明の軟質
磁心材料は以下の特徴を有する。(Means and effects for solving the problems) The soft magnetic core material of the present invention has the following characteristics.
Si、 Alを1種あるいは2種合計で0.2〜17御
t%含有し、残部が実質的にFeよりなる組成の材料を
堆積凝固させた形成物であって、粒界に酸化物絶縁層が
形成されており、相対密度が95%以上である。A product formed by depositing and solidifying a material containing one or two types of Si or Al in a total of 0.2 to 17 t%, with the remainder essentially consisting of Fe, with oxide insulation at the grain boundaries. A layer is formed and the relative density is 95% or more.
また、この様な軟質磁心材料は、以下のような方法によ
って製造できる。Moreover, such a soft magnetic core material can be manufactured by the following method.
(1)Si、 Alの少なくとも1種以上を含むPe基
合金を溶融後、酸素を含む雰囲気中で液滴状として堆積
凝固させる。(1) After melting a Pe-based alloy containing at least one of Si and Al, it is deposited and solidified in the form of droplets in an oxygen-containing atmosphere.
(2)S i 、 Alの少なくとも1種以上を含むF
e基合金を溶融後、酸素を含む雰囲気中で液滴状として
堆積凝固させた後、成形加工を行い、その後に熱処理を
行う。(2) F containing at least one of S i and Al
After the e-based alloy is melted, it is deposited and solidified in the form of droplets in an oxygen-containing atmosphere, then molded and then heat treated.
以下、本発明の限定理由およびその作用をまず軟質磁心
材料について述べる。Hereinafter, the reasons for the limitations of the present invention and its effects will first be described with respect to soft magnetic core materials.
本発明においては、素材として、FeをベースにSi、
Alを1種あるいは2種合計でO,:l’−17wt
%含有したものを使用する。In the present invention, the materials are Fe-based, Si,
One or two types of Al in total O,:l'-17wt
% content is used.
これは素材の磁束密度低下を少なくし、且つ素材の電気
抵抗率を高くするためである。This is to reduce the decrease in magnetic flux density of the material and to increase the electrical resistivity of the material.
即ち、St、 Atは0.2wt%より少ないと電気抵
抗率の増加という点で効果がなく、17−t%を超える
と磁束密度の低下が大きいことから前記範囲が選択され
る。又、Si、Ajの添加は、後で述べる製造法を採る
ことによって電気絶縁効果をもつ酸化物絶縁層を形成さ
せるためであり、0.2wt%未満では酸化物絶縁層の
形成効果が小さい。That is, the above range is selected because if St and At are less than 0.2 wt %, there will be no effect in terms of increasing the electrical resistivity, and if it exceeds 17-t %, the magnetic flux density will be greatly reduced. Further, the addition of Si and Aj is to form an oxide insulating layer having an electrically insulating effect by using the manufacturing method described later, and if it is less than 0.2 wt %, the effect of forming the oxide insulating layer is small.
また、粒界の酸化物絶縁層は高周波域における渦電流損
を低減させるためのものである。これにより従来の圧粉
磁心のような絶縁用バインダーを使用せずに粒間渦電流
を効果的に防止することが出来る。Further, the oxide insulating layer at the grain boundary is for reducing eddy current loss in a high frequency range. This makes it possible to effectively prevent intergranular eddy currents without using an insulating binder like in conventional dust cores.
相対密度については、圧粉磁心より大きな透磁率を得る
という目的から95%以上に限定される。The relative density is limited to 95% or more for the purpose of obtaining a magnetic permeability greater than that of a powder magnetic core.
即ち、従来技術の項で述べたように、圧粉磁心では、相
対密度が90%前後と低く、これが透磁率低下の主因と
なっている。本発明においては、これを95%以上とす
ることによって従来の圧粉磁心より大幅に透磁率を向上
させるとともに磁束密度も向上することができる。That is, as described in the section on the prior art, powder magnetic cores have a low relative density of around 90%, which is the main cause of the decrease in magnetic permeability. In the present invention, by setting this to 95% or more, it is possible to significantly improve magnetic permeability and improve magnetic flux density compared to conventional powder magnetic cores.
次に、製造方法について述べる。Next, the manufacturing method will be described.
まず、上記組成の材料を溶融して、ガスアトマイズ法ま
たは遠心法あるいは溶射法等により微細な液滴として分
散させ、これを基板上に堆積させる。このとき、液滴を
液相または固液共存状態で堆積させることによりポロシ
ティの非常に少ないバルクを得ることが出来る。ここで
、固液共存状態とは液滴が半凝固の状態で液相を残して
おり完全に固相になっていないことを指す。また、分散
粒子は出来るだけ細かくし、酸素を含む雰囲気中で分散
および堆積を行うことにより、液滴陳下中または堆積中
に液滴表面がStまたはAlを主体とした酸化物で覆わ
れるようにする。この酸化物被覆は粒界に絶縁層を形成
させるためのものであり、これによって高周波域におけ
る渦電流損を低減させることが出来る。First, a material having the above composition is melted and dispersed into fine droplets by gas atomization, centrifugation, thermal spraying, or the like, and these are deposited on a substrate. At this time, a bulk with very little porosity can be obtained by depositing droplets in a liquid phase or in a solid-liquid coexistence state. Here, the solid-liquid coexistence state refers to a state in which the droplets are in a semi-solidified state, leaving a liquid phase and not completely turning into a solid phase. In addition, by making the dispersed particles as fine as possible and dispersing and depositing them in an oxygen-containing atmosphere, we can ensure that the droplet surface is covered with oxides mainly composed of St or Al during droplet dispensation or deposition. Make it. This oxide coating is for forming an insulating layer at the grain boundaries, thereby reducing eddy current loss in the high frequency range.
一方、従来の圧粉磁心の製造においては、磁性粉を固相
状態で圧縮成形するため磁性粉の変形量が小さいことに
加え、成形体の強度確保と粒間絶縁のためのバインダー
添加を行うため、相対密度を95%以上にすることは困
難であった。On the other hand, in the production of conventional powder magnetic cores, magnetic powder is compression molded in a solid state, so the amount of deformation of the magnetic powder is small, and a binder is added to ensure the strength of the compact and to provide intergranular insulation. Therefore, it was difficult to increase the relative density to 95% or more.
以上の方法により、高磁束密度で透磁率が高く磁心損失
が小さいという特性を併せもつ磁性材料が得られるが、
堆積したままの状態では、寸法や表面状態が均一でなく
そのまま磁心として用いるには、適さない場合が多い。By the above method, a magnetic material with the characteristics of high magnetic flux density, high magnetic permeability, and low core loss can be obtained.
In the as-deposited state, the dimensions and surface condition are not uniform and it is often not suitable for use as a magnetic core.
その場合、堆積後の高温状態または再加熱後に圧延また
は鍛造等により所望の形状寸法に加工し、その後に熱処
理を行うことが有効となる。これにより、バルク中に僅
かに残ったポロシティの圧着効果で透磁率や磁束密度の
一層の向上が図れ、且つ、熱処理によって粒界部分の酸
素が粒内のSL又はAlと優先的に結合し、粒界の酸化
物層の強化を図ることが出来る。熱処理の温度範囲とし
ては、Si、 Alと粒界酸素との反応を図るため60
0〜1200℃の範囲で行うことが望ましい。In that case, it is effective to process the material into the desired shape and dimensions by rolling or forging after deposition or after reheating, and then perform heat treatment. As a result, magnetic permeability and magnetic flux density can be further improved by the compression effect of the porosity slightly remaining in the bulk, and oxygen in the grain boundary portion is preferentially combined with SL or Al in the grains by heat treatment, It is possible to strengthen the oxide layer at grain boundaries. The temperature range for the heat treatment is 60°C in order to promote the reaction between Si, Al and grain boundary oxygen.
It is desirable to carry out in the range of 0-1200 degreeC.
(実施例) 以下実施例により本発明の内容を詳細に説明する。(Example) The contents of the present invention will be explained in detail below using examples.
〔実施例1〕
Siを0.5evt%および8.0evt%含むFe−
Si合金を、溶融後、ガスアトマイズ法により分散し金
属板上に堆積させた。このとき、ガスは酸素を10vo
I1%含むArを使用した。又、平均粒子径は34mで
形成物の相対密度は約97%であった。この材料から、
機械加工により外径25腸、内径18■、高さが5閣の
リングを作製し、磁気特性を測定した結果が第1表のA
とBである。また、比較材として、Stを0.5wt%
含むFe−Si合金をガスアトマイズ法で分散し、粒子
を堆積させず冷却回収して2st%のエポキシ樹脂と混
合した後、成形圧8t/dにてプレス成形した同サイズ
のリングの測定結果を第1表のCに示す、この結果、本
発明にょる軟質磁心は透磁率、磁束密度ともに比較材の
圧粉磁心に対し大幅な向上が見られた。[Example 1] Fe- containing 0.5 evt% and 8.0 evt% of Si
After melting, the Si alloy was dispersed by gas atomization and deposited on a metal plate. At this time, the gas contains 10 vol of oxygen.
Ar containing 1% I was used. The average particle diameter was 34 m, and the relative density of the formed particles was about 97%. From this material,
A ring with an outer diameter of 25 cm, an inner diameter of 18 cm, and a height of 5 cm was manufactured by machining, and the magnetic properties were measured.The results are A in Table 1.
and B. In addition, as a comparative material, 0.5 wt% of St
The Fe-Si alloy containing Fe-Si alloy was dispersed by gas atomization, cooled and collected without depositing particles, mixed with 2st% epoxy resin, and then press-formed at a molding pressure of 8 t/d. As shown in C in Table 1, the soft magnetic core according to the present invention showed significant improvement in both magnetic permeability and magnetic flux density compared to the powder magnetic core of the comparative material.
尚、透磁率の測定についてはLCRメータ、磁束密度の
測定には直流B−H測定器、磁心損失の測定については
U関数針を使用し、以下同じ方法によった。Incidentally, an LCR meter was used to measure the magnetic permeability, a DC B-H measuring device was used to measure the magnetic flux density, and a U function needle was used to measure the magnetic core loss, and the same method was used hereinafter.
〔実施例2〕
Siを0.5wt%および8.0wt%含むFe −S
i合金を、実施例1と同じ条件で堆積させた後、約15
園の厚みから高温状態のまま厚み7腫に圧延加工し、不
活性ガス中で900℃×30分の熱処理を行った。得ら
れたFe−Si合合板から、放電加工により外径25■
、内径18m、高さが7■のリングを作製し、磁気特性
を測定した。その結果が第1表のDとEである。この結
果、本発明による軟質磁心は透磁率、磁束密度ともに比
較材Cの圧粉磁心より大幅に向上するとともに、堆積ま
まの材料A、Bよりも更に特性の向上が見られた。この
とき、本材料の相対密度は約98〜99%に向上してい
た。[Example 2] Fe-S containing 0.5 wt% and 8.0 wt% of Si
After depositing the i alloy under the same conditions as in Example 1, approximately 15
The material was rolled to a thickness of 7 mm at a high temperature, and heat treated at 900° C. for 30 minutes in an inert gas. From the obtained Fe-Si plywood, the outer diameter was 25cm by electrical discharge machining.
A ring with an inner diameter of 18 m and a height of 7 cm was prepared, and its magnetic properties were measured. The results are D and E in Table 1. As a result, the soft magnetic core according to the present invention had significantly improved magnetic permeability and magnetic flux density compared to the powder magnetic core of Comparative Material C, and also showed further improved properties than the as-deposited materials A and B. At this time, the relative density of the material had improved to about 98-99%.
また、粒界部分の酸化物絶縁層の確認のため材料Eの粒
界近傍の原子分布をオージェ電子分光分析によって調査
した結果を第1図に示す、この図から判るように粒界部
分には粒界表面から50〜150人の厚さで酸素とSi
のピークがみられ、その原子濃度の比は約2対1である
。このことは、粒界表面にSiO□を主体とするごく薄
い電気絶縁層が形成されていることを示している。In addition, in order to confirm the presence of oxide insulating layers in the grain boundary areas, the atomic distribution near the grain boundaries of material E was investigated using Auger electron spectroscopy. The results are shown in Figure 1.As can be seen from this figure, there are Oxygen and Si at a thickness of 50 to 150 μm from the grain boundary surface
A peak is observed, and the ratio of the atomic concentrations is approximately 2:1. This indicates that a very thin electrically insulating layer mainly composed of SiO□ is formed on the grain boundary surface.
〔実施例3〕
Si:9.5wt%と4224.5wt%を含むFe−
5i−A1合金を、溶融後ガスアトマイズ法により分散
し金属板上に堆積させた。このときの雰囲気は酸素を5
ν0!%含むArを使用した。また、平均粒子径は53
nであった0次にこの堆積物を再加熱し厚み約10閣か
ら5鵬に鍛造加工し、不活性ガス中で850℃×60分
の熱処理を行った。得られたFe−5i−A7合金板か
ら、放電加工により外径25■、内径18M、高さが5
−のリングを作製し、磁気特性を測定した結果が第1表
のFである。この材料の相対密度は98%であった。ま
た、比較材として該合金をガスアトマイズ法で分散し、
才子を堆積させず冷却回収して水ガラスを主体くする無
機バインダーと混合した後、成形圧工zt/dにてプレ
ス成形し、その後不活性ガス中1750℃×30分の熱
処理を施した同サイズの1゜ングの測定結果を第1表の
Gに示す。この結果、本発明による軟質磁心は透磁率、
磁束密度とも侃比較材の圧粉磁心に対し大幅な向上が見
られた。[Example 3] Fe- containing Si: 9.5 wt% and 4224.5 wt%
After melting, the 5i-A1 alloy was dispersed by gas atomization and deposited on a metal plate. At this time, the atmosphere contained 5 oxygen
ν0! % of Ar was used. In addition, the average particle diameter is 53
This deposit was reheated and forged to a thickness of about 10 mm to 5 mm, and heat treated at 850° C. for 60 minutes in an inert gas. The obtained Fe-5i-A7 alloy plate was processed by electric discharge machining to have an outer diameter of 25 mm, an inner diameter of 18 mm, and a height of 5 mm.
F in Table 1 is the result of manufacturing a ring with a value of - and measuring its magnetic properties. The relative density of this material was 98%. In addition, as a comparative material, the alloy was dispersed by gas atomization method,
After cooling and collecting without depositing saccharides and mixing with an inorganic binder mainly composed of water glass, the same was press-molded using a molding press ZT/D, and then heat-treated at 1750°C for 30 minutes in an inert gas. The measurement results for 1° of size are shown in G in Table 1. As a result, the soft magnetic core according to the present invention has magnetic permeability,
A significant improvement in magnetic flux density was seen compared to the comparison powder core.
〔実施例4〕
Alを3.0wt%含むPe−Al合金を、溶融後ガス
7トマイズ法により分散し金属板上に堆積させた。[Example 4] A Pe-Al alloy containing 3.0 wt% of Al was melted and then dispersed by a gas totomization method and deposited on a metal plate.
このとき、ガスは酸素を2voj2%含むArを使用し
た。又、平均粒子径は38nで形成物の相対密度は約9
6%であった。この材料から、機械加工により外径25
■、内径18醜、高さが5閣のリングを作製し、磁気特
性を測定した結果が第1表のHである。また、比較材と
して該合金をガスアトマイズ法で分散し、粒子を堆積さ
せず冷却回収して2wt%のエポキシ樹脂と混合した後
、成形圧8t/dにてプレス成形した同サイズのリング
の測定結果を第1表の■に示す、この結果、本発明によ
る軟質磁心は透磁率、磁束密度ともに比較材の圧粉磁心
に対し大幅な向上が見られた。At this time, Ar gas containing 2 voj 2% of oxygen was used. Also, the average particle diameter is 38n and the relative density of the formed particles is about 9
It was 6%. From this material, the outer diameter is 25 mm by machining.
(2) A ring with an inner diameter of 18 mm and a height of 5 mm was prepared, and the magnetic properties were measured. The results are H in Table 1. In addition, as a comparison material, the alloy was dispersed by gas atomization, cooled and collected without depositing particles, mixed with 2 wt% epoxy resin, and then press-formed at a molding pressure of 8 t/d. Measurement results of a ring of the same size. The results are shown in (■) in Table 1. As a result, the soft magnetic core according to the present invention showed a significant improvement in both magnetic permeability and magnetic flux density compared to the comparative powder magnetic core.
第1表
実施例の磁気特性
〔測定条件〕1.:
f=100K)lx、 8# : Ha−8000A
ノ層鉄損: Bm−100mr、 f−1(IOKI(
z(発明の効果)
前記の樺に、本発明の製造方法によれば、従来の圧粉磁
心に比較して相対密度が高く、且つ、酸化物絶縁層を粒
界に形成した高周波用軟質磁心材料を容易に製造できる
。Table 1 Magnetic properties of Examples [Measurement conditions] 1. : f=100K) lx, 8#: Ha-8000A
Layer iron loss: Bm-100mr, f-1 (IOKI (
z (Effect of the invention) According to the manufacturing method of the present invention, a soft magnetic core for high frequency is produced in the birch described above, which has a higher relative density than a conventional powder magnetic core and has an oxide insulating layer formed at the grain boundaries. The material can be easily manufactured.
また、この磁心材料が高磁束密度で透磁率が高く磁心損
失が小さいという特性を併せもつことから、この材料を
使用することにより、従来の圧粉磁心やフェライト磁心
等に比較してより小型のトランスやインダクタの製造が
可能となり、その1第1図は材料已について、オージェ
電子分光分析法で主要元素の原子濃度変化を粒界表面か
ら粒内深さ方向に測定した結果を示す図である。In addition, this magnetic core material has the characteristics of high magnetic flux density, high magnetic permeability, and low magnetic core loss, so by using this material, it can be made smaller than conventional powder magnetic cores or ferrite magnetic cores. It has become possible to manufacture transformers and inductors, part 1. Figure 1 shows the results of measuring changes in the atomic concentration of major elements from the grain boundary surface to the depth within the grain using Auger electron spectroscopy for the material. .
Claims (3)
7wt%含有し残部が実質的にFeよりなる組成の材料
を堆積凝固させた形成物であって、粒界に酸化物絶縁層
が形成されており、相対密度が95%以上であることを
特徴とする軟質磁心材料。(1) 0.2 to 1 total of one or two types of Si and Al
A material formed by depositing and solidifying a material containing 7 wt% with the remainder substantially consisting of Fe, characterized by having an oxide insulating layer formed at the grain boundaries and having a relative density of 95% or more. Soft magnetic core material.
金を溶融後、酸素を含む雰囲気中で液滴状として堆積凝
固させることを特徴とする請求項1記載の軟質磁心材料
の製造方法。(2) The method for producing a soft magnetic core material according to claim 1, wherein the Fe-based alloy containing at least one of Si and Al is melted and then deposited and solidified in the form of droplets in an oxygen-containing atmosphere.
金を溶融後、酸素を含む雰囲気中で液滴状として堆積凝
固させた後、成形加工を行い、その後に熱処理を行うこ
とを特徴とする請求項1記載の軟質磁心材料の製造方法
。(3) A Fe-based alloy containing at least one of Si and Al is melted, deposited and solidified in the form of droplets in an oxygen-containing atmosphere, and then formed and then heat treated. The method for manufacturing a soft magnetic core material according to claim 1.
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP2079841A JPH03278501A (en) | 1990-03-28 | 1990-03-28 | Soft magnetic core material and manufacture thereof |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP2079841A JPH03278501A (en) | 1990-03-28 | 1990-03-28 | Soft magnetic core material and manufacture thereof |
Publications (1)
| Publication Number | Publication Date |
|---|---|
| JPH03278501A true JPH03278501A (en) | 1991-12-10 |
Family
ID=13701430
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP2079841A Pending JPH03278501A (en) | 1990-03-28 | 1990-03-28 | Soft magnetic core material and manufacture thereof |
Country Status (1)
| Country | Link |
|---|---|
| JP (1) | JPH03278501A (en) |
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-
1990
- 1990-03-28 JP JP2079841A patent/JPH03278501A/en active Pending
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|---|---|---|---|---|
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| KR20140058528A (en) * | 2011-06-30 | 2014-05-14 | 퍼시몬 테크놀로지스 코포레이션 | System and method for making a structured material |
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| JP2016143700A (en) * | 2015-01-30 | 2016-08-08 | 東光株式会社 | Metal magnetic material and electronic component |
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