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JPH0348241B2 - - Google Patents
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JPH0348241B2 - - Google Patents

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Publication number
JPH0348241B2
JPH0348241B2 JP61062172A JP6217286A JPH0348241B2 JP H0348241 B2 JPH0348241 B2 JP H0348241B2 JP 61062172 A JP61062172 A JP 61062172A JP 6217286 A JP6217286 A JP 6217286A JP H0348241 B2 JPH0348241 B2 JP H0348241B2
Authority
JP
Japan
Prior art keywords
powder
particle size
alloy
average particle
apparent density
Prior art date
Legal status (The legal status is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the status listed.)
Expired - Lifetime
Application number
JP61062172A
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Japanese (ja)
Other versions
JPS62222002A (en
Inventor
Taku Meguro
Kazu Sasaki
Hideki Nakamura
Current Assignee (The listed assignees may be inaccurate. Google has not performed a legal analysis and makes no representation or warranty as to the accuracy of the list.)
Proterial Ltd
Original Assignee
Hitachi Metals Ltd
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Filing date
Publication date
Application filed by Hitachi Metals Ltd filed Critical Hitachi Metals Ltd
Priority to JP61062172A priority Critical patent/JPS62222002A/en
Publication of JPS62222002A publication Critical patent/JPS62222002A/en
Publication of JPH0348241B2 publication Critical patent/JPH0348241B2/ja
Granted legal-status Critical Current

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  • Manufacture Of Metal Powder And Suspensions Thereof (AREA)
  • Powder Metallurgy (AREA)
  • Soft Magnetic Materials (AREA)

Description

【発明の詳細な説明】[Detailed description of the invention]

〔産業上の利用分野〕 本発明は、Fe−Si−Al系合金圧粉磁心の製造
方法に関する。 〔従来の技術〕 従来よりFe−Si−Al系合金圧粉磁心は、鉄圧
粉磁心及びFe−Ni合金圧粉磁心とともに高周波
数帯域において、安定して高い透磁率を示すこと
から電子機器内の電源より発生する高周波ノイ
ズ、すなわちノーマルモードと称せられる電源ラ
イン間を往復するノイズを、大インピーダンスと
して減衰させるチヨークコイルとして用いられて
きた。Fe−Si−Al系合金圧粉磁心は鉄圧粉磁心
より高周波特性に優れているほか、特に直流重畳
特性に優れていること、及びNi、Mo等効果な原
料を含まず、Fe−Ni合金圧粉磁心よりは低廉で
あることから、近年徐々に需要が増加しつつあ
る。 従来、Fe−Si−Al系合金圧粉磁心はインゴツ
トを溶製し、これを拡散焼鈍してAl、Siの偏析
を低減した上で粗粉砕し、さらに、数段階の粉砕
工程を経て原料粉末とした後、粉末表面を無機絶
縁物質で被覆し圧粉成形して加熱することにより
製造されてきた。 〔発明が解決しようとする問題点〕 しかしながら、上述のようなインゴツトの粉砕
による工程では、インゴツトの製造、焼鈍、粉砕
の全工程が長く、勢い圧粉用原料粉末の原価が高
くなり、結果としてFe−Si−Al系合金圧粉磁心
自体の高価格をもたらし、チヨークコイルとして
の普及が制約されている現状である。 本発明は、以上の事情に鑑みてなされたもので
粉末粒子の性状と圧粉磁心の磁気的性質との関係
についての新たな知見に基づいて、良好な磁性を
安定して有しかつ、より廉価なFe−Si−Al系合
金圧粉磁心を提供することを目的とする。 〔問題点を解決するための手段〕 本発明は、後述する粉末の形態及び粒度と圧粉
磁心の磁気的性質との関係についての新たな知見
に基づき、高性能で廉価なFe−Si−Al系合金圧
粉磁心を得るためには、Fe−Si−Al系合金の溶
湯を直接液体中に流入させて平均粒径が20mm以下
のシヨツト状ないし扁平状の粗粉末を製造し、然
る後該粗粉末をさらに粉砕して得られた平均粒度
が40〜110μmの範囲内にあり、かつ見掛密度が
2.6〜3.8g/cm3である粉末を原料粉末として用い
ることが有効であることを見出したものである。 なお、ここでFe−Si−Al系合金とは、いわゆ
るセンダスト合金として知られる合金系のことで
あつて、Si4〜13%、Al4〜7%、残部Feを主成
分とし、その他不可避の不純物と、必要に応じて
5%以下の添加元素を含む高透磁率合金を指す。 〔作用〕 まず、本発明者らが新たに見出した知見の一つ
について説明する。 圧粉磁心においては、実効透磁率が高周波帯域
まで安定して高くほぼ一定の値を保つことが最も
重要である。この目的のためにFe−Si−Al系合
金圧粉磁心においては、粉末粒子の表面に水ガラ
ス等の無機絶縁物質を被覆したものを加圧成形す
ることで粒子間が一定程度絶縁された状態で磁心
となし、これを熱処理して上記の特性を得てい
る。粉末粒子の表面絶縁に有機物でなく、耐熱性
のある無機物を用いるのは、最終の熱処理を可能
とするためである。 実効透磁率の値とその周波数特性に影響する因
子として最も大きなものは、本発明者らによれば
(A)粒子の形態と(B)粒度である。 (A)については粒子が絶縁皮膜で覆われていて
も、成形の際に粒子相互が圧着すると、皮膜が破
壊されて絶縁が劣化し易く、交番磁界の周波数が
高くなるほど渦電流が流れ易くなり、実効透磁率
が減少する。従つて、周波数特性の面から、粒子
の形状として、局部的な圧着による絶縁破壊を起
こしにくいことが求められる。すなわち、粒子表
面が乱れた不規則形状であると、成形時に絶縁破
壊し易く、表面の滑らかな球状粒子が最も好まし
い。よつて、不規則形状となるほど粉末の見掛密
度は低くなるので形状パラメータとしての見掛密
度は高いことが望ましい。 しかしながら透磁率は、一方圧粉磁心の密度の
パラメータでもあり、見掛密度の最も高い完全球
状粒子の場合には点接触で圧密化されるので、成
形体の密度はかえつて低く、また反磁場係数が高
くなることもあつて、高い透磁率を達成すること
がやや困難となる。従つて良好な絶縁状態を保つ
ことによつて実効透磁率が減少し始める周波数を
より高くすることと、成形体の密度を高めること
によつて初期直流の実効透磁率を高めることの間
には、均衡を図る必要がある。この目的のために
は、粉末の見掛密度として適正な範囲がある。 一方、(B)の視点からは、粉末粒子があまりに粗
大であると、交番磁界による渦電流が生じ易く、
実効透磁率の周波数特性が劣化し易く、また成形
体の強度が低下するので粒子の粒度には上限があ
る。逆にあまりに細粒であると、粉末粒子の圧縮
性が低下して初期(直流)の透磁率が低下するの
で下限の粒度が存在する。 本発明者らは、以上の知見を基にFe−Si−Al
系合金圧粉磁心について最適の粉末粒子の見掛密
度と粒度を規定し、この規定された範囲内の粉末
を廉価に製造するための条件をさらに検討した。 すなわち、Fe−Si−Al系合金の溶湯を直接液
体中に流入させて、平均粒径が20mm以下のシヨツ
ト状ないし扁平状の粗粉末を製造し、然る後該粗
粉末をさらに粉砕して得られた平均粒度が40〜
110μm、見掛密度2.6〜3.8g/cm3の粉末を用いた
圧粉磁心が優れた特性を有し、かつ従来より廉価
に製造し得ることを見出し、本発明をなすに至つ
た。 以下本発明をさらに詳細に説明する。 まず、平均粒度の上限を110μmとした理由に
ついて述べる。 第1図は、見掛密度が3.4±0.1g/cm3とほぼ等
しく、平均粒度の異なる5.5%Al−9.5%Si−残Fe
の合金粉末より成る圧粉磁心の透磁率の高周波数
特性の平均粒度依存性を示したものである。粉末
は粒度調整の後、水素気流中900℃にて焼鈍し、
水ガラスを固形分として0.8重量%を粉末表面に
被覆し、20ton/cm3の圧力で外径28mm、内径15mm、
高さ8mmのリング状に成形後、大気中700℃にて
焼鈍を行なつた。この成形体の透磁率をインピー
ダンスメーターによつて測定した。第1図縦軸の
μe13M/μe10Kは、13MHzにおける実効透磁率
μe13Mと10KHzにおける実効透磁率μe10Kの比で
あり、透磁率の高周波数特性の目安とした。第1
図から平均粒度が大きくなるほど、μe13M/
μe10Kが小さくなつて周波数特性が劣化していく
様子が認められる。特に平均粒度が110μmを越
えるとμe13M/μe10Kが0.4を下まわり劣化が著
しい。従つて、平均粒度の上限は110μmとした。
なお、平均粒度130μmを越えると成形体の強度
が低く、ハンドリングが不可能であつた。 次に平均粒度の下限を40μmとした理由を述べ
る。 第2図は、第1図において用いたとの同一の方
法で製造した成形体の10KHzにおける実効透磁率
μe10Kの平均粒度依存性を示したものである。粒
度が大きくなるほどμe10Kは大きくなるが、Fe
−Si−Al系合金圧粉磁心に要求されるμe10Kの最
低値70を得るには、平均粒度を40μm以上としな
ければならないことがわかる。 次いで、見掛密度の下限を2.6g/cm3とした理
由について述べる。第3図は、平均粒度が70±
5μmとほぼ等しく、見掛密度の異なる5.5%Al−
9.5%Si−残Feの合金粉末より成る圧粉磁心の周
波数特性の見掛密度依存性を示す。 磁心の製造方法は、第1図、第2図の場合と同
様である。見掛密度が低い不規則形状粉末ほど、
μe13M/μe10Kが低く周波数特性に劣る。
μe13M/μe10Kの必要値を第1図において触れた
ように0.4として見掛密度の下限を2.6とした。 さらに、見掛密度の上限を3.8g/cm3とした理
由につき述べる。 第4図は第3図と同様の粉末を用い、長さ40
mm、幅10mm、高さ7mmの成形体を作成して、その
抗折力を測定した結果である。見掛密度の高い粉
末、すなわち粒子間の接触面積が小さく、絡み合
いの少ない粉末の成形体ほど抗折力が低くなつて
いる。Fe−Si−Al系合金は、塑性変形能が低く、
従つてその圧粉成形体は、鉄やFe−Ni合金の成
形体に比して強度が小さくなるが、少なくとも自
動プレス成形ラインにおいて取扱いできる強度と
して、最低でも0.2Kg/mm2は必要である。この点
から、粉末の見掛密度の上限を3.8g/cm3とする。 以上、第1図〜第4図に示したように、安定し
た透磁率と周波数特性を有する圧粉磁心を得る上
で、40〜110μmの平均粒度、2.6〜3.8g/cm3の見
掛密度の粉末が実用的なものであることが明らか
である。 なお、当然のことながら粉末を加圧成形する際
の圧力によつても透磁率とその周波数特性は変化
するが、Fe−Si−Al系合金の場合には、15ton/
cm2以上の成形圧力でないと70以上の透磁率を得る
ことは難しい。 また成形圧は、金型寿命の制約から現状では最
大上げても25ton/cm2程度が上限である。15から
25ton/cm2程度まで成形圧が変化しても、上述の
ような粉末粒子の粒度及び見掛密度の特性に及ぼ
す影響は総体として変わらない。 以上のように特定された粒度と見掛密度を有す
る粉末を廉価に得るために、本発明者らは溶湯か
ら直接粉末を製造する手法に着眼し、種々検討を
行なつた。その結果、Fe−Si−Al系合金の溶湯
をノズルを通して溶湯流となし、これを直接静止
もしくは撹拌された液体中に流入させて平均粒径
が20mm以下のシヨツト状ないし扁平状の粗粉末を
製造し、然る後該粗粉末をさらに微粉砕すること
で廉価に目的の粉末が得られることを見出した。
この粗粉末製造法において、用いられる冷却液体
は、後処理の容易さを考慮すると水が好ましい
が、特に限定されない。微粉砕後の最終目的の粒
度が40〜110μmと、粗粉末の20mm以下数mmのオ
ーダーに比べると小さいので、粗粉末の形態上の
制約はないが、得られる形状は静止浴では、球に
近いシヨツト状であり、撹拌を加えると扁平状と
なり易い傾向が認められた。また、溶解原料に水
分が残存している場合やH2含有量の多い溶湯で
はシヨツト状となり易いし、グリセリンなどの高
粘性物質の水溶液でもシヨツト状となり易い傾向
にあつた。 粗粉末の平均粒径を20mm以下とした理由を述べ
る。 第5図は、本発明の製造方法による粗粉末及び
従来技術のインゴツトの粒径(サイズ)によつ
て、Fe−Si−Al系合金圧粉磁心のμe10Kがどう
変化するかを示したものである。すなわち、種々
の初期粒径(サイズ)の粗粉末及びインゴツトを
粉砕して、平均粒度100±5μm及び45±5μmの粉
末を製造した。見掛密度は3.3±0.2g/cm3とおよ
そ等しい。インゴツトも含めてすべてAl、Siの
偏折防止のための拡散焼鈍は行なわずに、上記諸
元に粉砕した後、水素気流中の焼鈍、水ガラス
0.8重量%の絶縁処理、20ton/cm2の加圧成形によ
つて圧粉磁心とした。 第5図中、の曲線は平均粒度100±5μm、
は同45±5μmの粉砕粉による磁心のμe10Kであ
る。これによると、初期の粗粉及びインゴツト状
態で、拡散焼鈍を行なわない場合には、初期粒径
は小さいほどμe10Kが高くなることがわかる。
1000℃前後の拡散焼鈍の省略を前提として、第5
図においてほとんどμe10Kの劣化のない初期粗粉
の粒径は20mm以下である。従つて、粗粉末の平均
粒径を20mm以下と規定した。 本発明の粗粉末製造法において、溶湯流が安定
して通過させるためのノズル径は、Fe−Si−Al
系合金の場合、溶湯温度が1600℃程度でも3mmφ
以上は必要である。従つて、冷却条件によつても
異なるが、得られる粗粉末の粒径を20mm以下とす
ることは容易である。粉砕効率の面からもより粒
径を小さくすることは有利であり、溶湯流に対し
て数Kg/cm2〜数10Kg/cm2の不活性ガス流を横ない
し斜め横から当てて、溶湯の飛散を促進させるこ
とが有効である。 このように本発明の粗粉は、従来のインゴツト
に比べて凝固冷却速度が高いために、AlやSiの
偏析がなく、従つて高温の焼鈍が全く不要であ
る。 インゴツトの焼鈍が不要になつたばかりでな
く、粉砕もより容易である。粗粉末の粉砕方法は
特に限定されず、広範な方法を適用できる。たと
えばローラーミル、ハンマーミル等によつて粗粉
砕して数100μmの粉末とした後、振動ミル、ア
トライター、ボールミル、ジエツトミル等によつ
て目的の粒度と見掛密度とすることができる。振
動ミル、アトライターなど粉砕機として投入エネ
ルギーの高い装置では、粉砕条件によつては一回
の粉砕によつて目的の粉末を得ることが可能であ
る。 以上本発明のFe−Si−Al系合金粉末の製造方
法を説明してきたが、冷却液体槽中へ合金溶湯流
を流入せしめる方法は、インゴツトを製造した
後、これを拡散焼鈍し、数段階の工程で粉砕する
従来工程に比べて大幅な工程の短縮、エネルギー
節減となり、原料粉末の原価を低減させることが
できる画期的なものである。 以下具体的な本発明の内容について実施例を挙
げてさらに説明する。 〔実施例〕 実施例 1 Ar雰囲気にて溶解した5.5%Al−9.5%Si−残
Feの1600℃の溶湯を5mmφのノズルを通じて静
止水槽中に流下せしめ、平均粒度10mmのシヨツト
状粉末とした。これをスタンプミルによつて−50
メツシユまで粉砕した後、振動ミルによつて乾式
微粉砕した。振動数、振幅、粉砕媒体及び粉末の
充填率を制御して平均粒度80μm、見掛密度3.30
g/cm3の粉末を得た。 この粉末を水素気流中で900℃×1時間の歪取
り処理を施し、0.5、1.0、1.5wt%の水ガラスによ
つて表面を絶縁被覆した後、20ton/cm2の圧力で
加圧成形し、その後700℃×0.5時間の熱処理によ
つて圧粉磁心とした。このようにして得られた圧
粉磁心のμe10Kとμe13M/μe10Kは第1表の通り
であり、高い透磁率が高周波帯域まで安定してい
る。
[Industrial Application Field] The present invention relates to a method for manufacturing a Fe-Si-Al alloy dust core. [Prior art] Fe-Si-Al alloy powder magnetic cores have been used in electronic devices because they exhibit stable high magnetic permeability in high frequency bands, along with iron powder magnetic cores and Fe-Ni alloy powder magnetic cores. These coils have been used as high-impedance coils to attenuate high-frequency noise generated from power supplies, that is, noise that travels back and forth between power supply lines and is called normal mode. The Fe-Si-Al alloy powder magnetic core has superior high-frequency characteristics than the iron powder magnetic core, and is particularly excellent in DC superposition characteristics, and does not contain effective raw materials such as Ni and Mo. Since it is cheaper than powder magnetic core, demand has been gradually increasing in recent years. Conventionally, Fe-Si-Al alloy powder magnetic cores are made by melting an ingot, diffusion annealing it to reduce the segregation of Al and Si, and then coarsely pulverizing it. It has been manufactured by coating the powder surface with an inorganic insulating material, compacting it, and heating it. [Problems to be solved by the invention] However, in the process of pulverizing the ingot as described above, the entire process of manufacturing, annealing, and pulverizing the ingot is long, and the cost of raw material powder for force compaction is high. The current situation is that the Fe-Si-Al alloy powder magnetic core itself is expensive, and its widespread use as a chiyoke coil is restricted. The present invention was made in view of the above circumstances, and is based on new findings regarding the relationship between the properties of powder particles and the magnetic properties of a powder magnetic core. The purpose is to provide an inexpensive Fe-Si-Al alloy powder magnetic core. [Means for Solving the Problems] The present invention is based on new knowledge regarding the relationship between the powder morphology and particle size and the magnetic properties of the dust core, which will be described later. In order to obtain a Fe-Si-Al alloy powder magnetic core, a molten Fe-Si-Al alloy is directly poured into a liquid to produce shot- or flat-shaped coarse powder with an average particle size of 20 mm or less, and then The average particle size obtained by further pulverizing the coarse powder is within the range of 40 to 110 μm, and the apparent density is
It has been found that it is effective to use a powder having a weight of 2.6 to 3.8 g/cm 3 as a raw material powder. Note that the Fe-Si-Al alloy here refers to an alloy known as a so-called sendust alloy, which is mainly composed of 4 to 13% Si, 4 to 7% Al, and the balance is Fe, with other unavoidable impurities. , refers to a high magnetic permeability alloy that optionally contains 5% or less of additional elements. [Operation] First, one of the findings newly discovered by the present inventors will be explained. In powder magnetic cores, it is most important that the effective magnetic permeability remains stably high and approximately constant up to a high frequency band. For this purpose, in Fe-Si-Al alloy powder magnetic cores, the surfaces of powder particles are coated with an inorganic insulating material such as water glass and then pressure-formed to create a state in which the particles are insulated to a certain degree. This is used as a magnetic core, which is then heat treated to obtain the above characteristics. The reason why a heat-resistant inorganic material is used instead of an organic material for the surface insulation of the powder particles is to enable the final heat treatment. According to the inventors, the biggest factor influencing the value of effective magnetic permeability and its frequency characteristics is
(A) Particle morphology and (B) particle size. Regarding (A), even if the particles are covered with an insulating film, if the particles are pressed against each other during molding, the film is likely to be destroyed and the insulation will deteriorate, and the higher the frequency of the alternating magnetic field, the more likely eddy currents will flow. , the effective permeability decreases. Therefore, from the viewpoint of frequency characteristics, the particle shape is required to be difficult to cause dielectric breakdown due to local pressure bonding. That is, if the particle surface is disordered and has an irregular shape, dielectric breakdown will easily occur during molding, and spherical particles with a smooth surface are most preferable. Therefore, the apparent density of the powder decreases as the shape becomes more irregular, so it is desirable that the apparent density as a shape parameter be high. However, magnetic permeability is also a parameter for the density of the powder magnetic core, and in the case of perfectly spherical particles with the highest apparent density, they are consolidated by point contact, so the density of the compact is rather low, and the demagnetizing field The coefficient becomes high, making it somewhat difficult to achieve high magnetic permeability. Therefore, there is a trade-off between increasing the frequency at which the effective permeability begins to decrease by maintaining good insulation and increasing the initial DC effective permeability by increasing the density of the compact. , there is a need to strike a balance. For this purpose, there is a suitable range for the apparent density of the powder. On the other hand, from the viewpoint of (B), if the powder particles are too coarse, eddy currents are likely to occur due to the alternating magnetic field.
There is an upper limit to the particle size because the frequency characteristics of effective magnetic permeability are likely to deteriorate and the strength of the compact is reduced. On the other hand, if the particles are too fine, the compressibility of the powder particles decreases and the initial (DC) magnetic permeability decreases, so there is a lower limit to the particle size. Based on the above findings, the present inventors have developed Fe-Si-Al
The optimum apparent density and particle size of the powder particles for the alloy powder magnetic core were defined, and the conditions for producing powder within the defined range at a low cost were further investigated. That is, a molten Fe-Si-Al alloy is directly poured into a liquid to produce shot-like or flat-shaped coarse powder with an average particle size of 20 mm or less, and then the coarse powder is further crushed. The average particle size obtained is 40~
It was discovered that a powder magnetic core using powder having a diameter of 110 μm and an apparent density of 2.6 to 3.8 g/cm 3 has excellent properties and can be manufactured at a lower cost than before, and the present invention has been completed. The present invention will be explained in more detail below. First, the reason why the upper limit of the average particle size was set to 110 μm will be described. Figure 1 shows 5.5%Al-9.5%Si-residue Fe with approximately the same apparent density as 3.4±0.1g/ cm3 and different average particle sizes.
This figure shows the dependence of the high-frequency characteristics of magnetic permeability on the average particle size of a dust core made of alloy powder. After adjusting the particle size, the powder was annealed at 900℃ in a hydrogen stream.
The powder surface was coated with 0.8% by weight of water glass as a solid content, and the outer diameter was 28mm and the inner diameter was 15mm under a pressure of 20ton/ cm3 .
After forming into a ring shape with a height of 8 mm, it was annealed at 700°C in the air. The magnetic permeability of this molded body was measured using an impedance meter. μe13M/μe10K on the vertical axis in FIG. 1 is the ratio of the effective magnetic permeability μe13M at 13 MHz to the effective magnetic permeability μe10K at 10 KHz, and was used as a measure of the high frequency characteristics of magnetic permeability. 1st
From the figure, the larger the average particle size, the more μe13M/
It can be seen that as μe10K decreases, the frequency characteristics deteriorate. In particular, when the average particle size exceeds 110 μm, μe13M/μe10K falls below 0.4, resulting in significant deterioration. Therefore, the upper limit of the average particle size was set to 110 μm.
In addition, when the average particle size exceeded 130 μm, the strength of the molded product was low and it was impossible to handle it. Next, the reason for setting the lower limit of the average particle size to 40 μm will be explained. FIG. 2 shows the dependence of the effective magnetic permeability μe10K at 10 KHz on the average particle size of a molded body manufactured by the same method as used in FIG. 1. μe10K increases as the particle size increases, but Fe
It can be seen that in order to obtain the minimum μe10K of 70 required for a -Si-Al alloy dust core, the average particle size must be 40 μm or more. Next, the reason for setting the lower limit of the apparent density to 2.6 g/cm 3 will be described. Figure 3 shows that the average particle size is 70±
5.5% Al−, which is approximately equal to 5μm and has a different apparent density.
This figure shows the apparent density dependence of the frequency characteristics of a dust core made of 9.5% Si-remaining Fe alloy powder. The method of manufacturing the magnetic core is the same as in the case of FIGS. 1 and 2. Irregularly shaped powders with lower apparent density
μe13M/μe10K is low and frequency characteristics are poor.
As mentioned in Fig. 1, the required value of μe13M/μe10K was set to 0.4, and the lower limit of the apparent density was set to 2.6. Furthermore, the reason for setting the upper limit of the apparent density to 3.8 g/cm 3 will be described. Figure 4 uses the same powder as in Figure 3, with a length of 40 mm.
This is the result of measuring the transverse rupture strength of a molded body having a width of 10 mm and a height of 7 mm. The transverse rupture strength of a molded body of powder with a higher apparent density, that is, a powder having a smaller contact area between particles and less entanglement, has a lower transverse rupture strength. Fe-Si-Al alloys have low plastic deformability;
Therefore, the strength of the compacted compact is lower than that of iron or Fe-Ni alloy compacts, but it must have a strength of at least 0.2 kg/mm 2 so that it can be handled at least on an automatic press forming line. . From this point of view, the upper limit of the apparent density of the powder is set at 3.8 g/cm 3 . As shown in Figures 1 to 4, in order to obtain a dust core with stable magnetic permeability and frequency characteristics, the average particle size is 40 to 110 μm, and the apparent density is 2.6 to 3.8 g/ cm3. It is clear that the powder is of practical use. Naturally, the magnetic permeability and its frequency characteristics change depending on the pressure when the powder is compacted, but in the case of Fe-Si-Al alloy, the permeability is 15 tons/
It is difficult to obtain a magnetic permeability of 70 or higher without a molding pressure of cm 2 or higher. Furthermore, the molding pressure is currently limited to about 25 ton/cm 2 even if it is increased to the maximum due to limitations on mold life. from 15
Even if the molding pressure changes up to about 25 ton/cm 2 , the effects on the characteristics of the particle size and apparent density of the powder particles as described above do not change as a whole. In order to obtain powder having the particle size and apparent density specified above at a low cost, the present inventors focused on a method of producing powder directly from molten metal and conducted various studies. As a result, the molten metal of the Fe-Si-Al alloy is passed through a nozzle to form a molten metal flow, which is then directly flowed into a stationary or stirred liquid to produce shot- or flat-shaped coarse powder with an average particle size of 20 mm or less. It has been found that the desired powder can be obtained at a low cost by manufacturing and then further finely pulverizing the coarse powder.
In this coarse powder production method, the cooling liquid used is preferably water in view of ease of post-treatment, but is not particularly limited. The final target particle size after pulverization is 40 to 110 μm, which is smaller than that of coarse powder, which is on the order of 20 mm or less, so there are no restrictions on the shape of coarse powder, but the shape obtained is similar to that of a sphere in a static bath. It was found that it had a nearly shot shape, and that it tended to become flat when agitation was applied. In addition, when water remained in the dissolved raw material or when the molten metal had a high H 2 content, it was likely to become shot-like, and an aqueous solution of a highly viscous substance such as glycerin also tended to become shot-like. The reason why the average particle size of the coarse powder was set to 20 mm or less will be explained. Figure 5 shows how the μe10K of the Fe-Si-Al alloy powder magnetic core changes depending on the particle size of the coarse powder produced by the production method of the present invention and the ingot produced by the prior art. be. That is, coarse powders and ingots of various initial particle sizes were ground to produce powders with average particle sizes of 100±5 μm and 45±5 μm. The apparent density is approximately equal to 3.3±0.2 g/cm 3 . All ingots, including ingots, were crushed to the above specifications without being subjected to diffusion annealing to prevent Al and Si polarization, and then annealed in a hydrogen stream and water glass.
A powder magnetic core was obtained by insulation treatment at 0.8% by weight and pressure molding at 20 tons/cm 2 . In Figure 5, the curve shows an average particle size of 100±5μm,
is the μe10K of the magnetic core made of pulverized powder of 45±5 μm. According to this, it can be seen that when diffusion annealing is not performed in the initial coarse powder and ingot state, the smaller the initial particle size, the higher the μe10K.
On the premise of omitting diffusion annealing at around 1000℃, the fifth
In the figure, the particle size of the initial coarse powder with almost no μe10K deterioration is 20 mm or less. Therefore, the average particle size of the coarse powder was defined as 20 mm or less. In the coarse powder production method of the present invention, the nozzle diameter for stably passing the molten metal is determined by Fe-Si-Al
In the case of alloys, the diameter is 3mm even if the molten metal temperature is around 1600℃.
The above is necessary. Therefore, although it varies depending on the cooling conditions, it is easy to make the particle size of the obtained coarse powder 20 mm or less. It is advantageous to make the particle size even smaller from the perspective of crushing efficiency, and by applying an inert gas flow of several kg/cm 2 to several tens of kg/cm 2 to the molten metal from the side or diagonally, the molten metal can be crushed. It is effective to promote scattering. As described above, since the coarse powder of the present invention has a higher solidification and cooling rate than conventional ingots, there is no segregation of Al or Si, and therefore high-temperature annealing is not required at all. Not only does ingot annealing become unnecessary, but it is also easier to crush. The method of pulverizing the coarse powder is not particularly limited, and a wide variety of methods can be applied. For example, after coarsely pulverizing the powder using a roller mill, hammer mill, etc. to obtain a powder of several 100 μm, the desired particle size and apparent density can be obtained using a vibration mill, attritor, ball mill, jet mill, etc. In devices such as vibrating mills and attritors that require high energy input, it is possible to obtain the desired powder in one pulverization process, depending on the pulverization conditions. The method for manufacturing the Fe-Si-Al alloy powder of the present invention has been described above, but the method of flowing the molten alloy into a cooling liquid bath involves manufacturing an ingot, then diffusion annealing it, and performing several steps. This is an epoch-making method that significantly shortens the process and saves energy compared to the conventional process of grinding in the process, reducing the cost of raw material powder. Hereinafter, specific contents of the present invention will be further explained with reference to Examples. [Example] Example 1 5.5% Al-9.5% Si-residue dissolved in Ar atmosphere
Molten Fe at 1600°C was poured into a still water tank through a nozzle with a diameter of 5 mm to form shot-like powder with an average particle size of 10 mm. -50 by stamp mill
After pulverizing to mesh, it was dry-pulverized using a vibrating mill. By controlling the vibration frequency, amplitude, grinding media and powder filling rate, the average particle size is 80 μm and the apparent density is 3.30.
A powder of g/cm 3 was obtained. This powder was strain-removed in a hydrogen stream at 900℃ for 1 hour, the surface was insulated with 0.5, 1.0, and 1.5wt% water glass, and then pressure molded at a pressure of 20ton/ cm2. Then, a powder magnetic core was obtained by heat treatment at 700°C for 0.5 hours. μe10K and μe13M/μe10K of the powder magnetic core thus obtained are shown in Table 1, and the high magnetic permeability is stable up to the high frequency band.

【表】 実施例 2 Ar雰囲気にて溶解した5.5%Al−9.5%Si−残
Feの1600℃の溶湯を5mmφのノズルを通じて流
下させるとともに、この溶湯流に対し、斜め上
45゜方向から10Kg/cm2の圧力、15/minの流量
のArガス流を当てることによつて溶湯を飛散さ
せ、撹拌された水槽内で飛散溶湯を冷却した。得
られた粗粉末の平均粒度は2.5mmであつた。 この粗粉末をハンマーミルによつて、平均粒度
600μmまで粉砕の後、振動ミルによつて平均粒
度76μmに乾式微粉砕した。振動数、振幅、粉砕
媒体及び粉末の充填率を制御して、平均粒度51μ
m、見掛密度3.62g/cm3の粉末を得た。 この粉末を水素気流中で900℃×1時間の歪取
り処理を施し、0.5、1.0、1.5wt%の水ガラスによ
つて表面を絶縁被覆した後、20ton/cm2の圧力で
加圧成形し、その後700℃×0.5時間の熱処理によ
つて圧粉磁心とした。このようにして得られた圧
粉磁心のμe10Kとμe13M/μe10Kは第1表の通り
であり、高い透磁率が高周波帯域まで安定してい
る。
[Table] Example 2 5.5% Al-9.5% Si-residue dissolved in Ar atmosphere
Fe molten metal at 1600℃ is flowed down through a 5mmφ nozzle, and the molten metal is flowed diagonally upward.
The molten metal was scattered by applying an Ar gas flow at a pressure of 10 Kg/cm 2 and a flow rate of 15 min from a 45° direction, and the scattered molten metal was cooled in a stirred water tank. The average particle size of the obtained coarse powder was 2.5 mm. This coarse powder is processed by a hammer mill to obtain an average particle size of
After pulverizing to 600 μm, dry pulverization was performed using a vibrating mill to an average particle size of 76 μm. By controlling the vibration frequency, amplitude, grinding media and powder filling rate, the average particle size is 51μ
A powder with an apparent density of 3.62 g/cm 3 was obtained. This powder was strain-removed in a hydrogen stream at 900℃ for 1 hour, the surface was insulated with 0.5, 1.0, and 1.5wt% water glass, and then pressure molded at a pressure of 20ton/ cm2. Then, a powder magnetic core was obtained by heat treatment at 700°C for 0.5 hours. μe10K and μe13M/μe10K of the powder magnetic core thus obtained are shown in Table 1, and the high magnetic permeability is stable up to the high frequency band.

【表】 〔発明の効果〕 以上から明らかなように本発明のFe−Si−Al
系合金圧粉磁心の製造方法は、高い周波数帯域に
わたつて安定して高い透磁率を示す圧粉磁心の製
造方法として最適で、かつ従来からある溶製イン
ゴツトを製造、焼鈍を経た後これを粉砕して得ら
れる粉末を用いた圧粉磁心の製造方法より廉価な
圧粉磁心を提供するもので、その工業的価値が大
である。
[Table] [Effects of the invention] As is clear from the above, the Fe-Si-Al of the present invention
The method for producing powder magnetic cores made from alloy alloys is the most suitable method for producing powder magnetic cores that exhibit stable high magnetic permeability over a high frequency range, and is a conventional method for producing powder magnetic cores that produce molten ingots, undergo annealing, and then This method provides a powder magnetic core that is cheaper than the method of manufacturing a powder magnetic core using powder obtained by pulverization, and has great industrial value.

【図面の簡単な説明】[Brief explanation of drawings]

第1図は粉末の平均粒度と透磁率の周波数特性
との相関図、第2図は粉末の平均粒度と透磁率と
の相関図、第3図は粉末の見掛密度と透磁率の周
波数特性との相関図、第4図は粉末の見掛密度と
抗折力との相関図、第5図は初期粗粉粒径と透磁
率の相関図である。
Figure 1 is a correlation diagram between the average particle size of powder and the frequency characteristics of magnetic permeability, Figure 2 is a diagram of the correlation between the average particle size of powder and magnetic permeability, and Figure 3 is the frequency characteristic of apparent density and magnetic permeability of powder. FIG. 4 is a correlation diagram between the apparent density of powder and transverse rupture strength, and FIG. 5 is a correlation diagram between initial coarse powder particle size and magnetic permeability.

Claims (1)

【特許請求の範囲】[Claims] 1 Fe−Si−Al系合金の粉末の表面を無機絶縁
物質で被覆し、加圧成形後熱処理してなるFe−
Si−Al系合金圧粉磁心の製造方法において、Fe
−Si−Al系合金の溶湯を直接液体中に流入させ
て、平均粒径が20mm以下のシヨツト状ないし扁平
状の粗粉末を製造し、然る後該粗粉末をさらに粉
砕して得られた平均粒度が40〜110μm、見掛密
度2.6〜3.8g/cm3の粉末を用いたことを特徴とす
るFe−Si−Al系合金圧粉磁心の製造方法。
1 Fe-Si-Al alloy powder is coated with an inorganic insulating material and then heat-treated after pressure molding.
In the manufacturing method of Si-Al alloy dust core, Fe
- A shot-like or flat-shaped coarse powder with an average particle size of 20 mm or less is produced by directly flowing a molten Si-Al alloy into a liquid, and then the coarse powder is further pulverized. A method for producing an Fe-Si-Al alloy powder magnetic core, characterized in that powder having an average particle size of 40 to 110 μm and an apparent density of 2.6 to 3.8 g/cm 3 is used.
JP61062172A 1986-03-20 1986-03-20 Production of dust core of fe-si-al alloy Granted JPS62222002A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP61062172A JPS62222002A (en) 1986-03-20 1986-03-20 Production of dust core of fe-si-al alloy

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP61062172A JPS62222002A (en) 1986-03-20 1986-03-20 Production of dust core of fe-si-al alloy

Publications (2)

Publication Number Publication Date
JPS62222002A JPS62222002A (en) 1987-09-30
JPH0348241B2 true JPH0348241B2 (en) 1991-07-23

Family

ID=13192437

Family Applications (1)

Application Number Title Priority Date Filing Date
JP61062172A Granted JPS62222002A (en) 1986-03-20 1986-03-20 Production of dust core of fe-si-al alloy

Country Status (1)

Country Link
JP (1) JPS62222002A (en)

Family Cites Families (4)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS5442644A (en) * 1977-09-09 1979-04-04 Nippon Electric Co Method of positioning electrodes of laminated condenser
JPS58221204A (en) * 1982-06-18 1983-12-22 Tohoku Metal Ind Ltd Production of iron-silicon-aluminum magnetic alloy compact core
JPS6021301A (en) * 1983-07-11 1985-02-02 Kawasaki Steel Corp Iron powder for compacted magnetic core
JPS6148502A (en) * 1984-08-14 1986-03-10 Nippon Soda Co Ltd Manufacture of cu-sb-pb alloy powder for filler

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Publication number Publication date
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