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JPS6349883B2 - - Google Patents
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JPS6349883B2 - - Google Patents

Info

Publication number
JPS6349883B2
JPS6349883B2 JP15769681A JP15769681A JPS6349883B2 JP S6349883 B2 JPS6349883 B2 JP S6349883B2 JP 15769681 A JP15769681 A JP 15769681A JP 15769681 A JP15769681 A JP 15769681A JP S6349883 B2 JPS6349883 B2 JP S6349883B2
Authority
JP
Japan
Prior art keywords
copper
sintered
magnetic flux
flux density
coercive force
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
Application number
JP15769681A
Other languages
Japanese (ja)
Other versions
JPS5858708A (en
Inventor
Kazuo Asaka
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.)
Resonac Corp
Original Assignee
Hitachi Powdered Metals Co Ltd
Priority date (The priority date 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 date listed.)
Filing date
Publication date
Application filed by Hitachi Powdered Metals Co Ltd filed Critical Hitachi Powdered Metals Co Ltd
Priority to JP15769681A priority Critical patent/JPS5858708A/en
Publication of JPS5858708A publication Critical patent/JPS5858708A/en
Publication of JPS6349883B2 publication Critical patent/JPS6349883B2/ja
Granted legal-status Critical Current

Links

Classifications

    • 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

Landscapes

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

Description

【発明の詳細な説明】 この発明は、磁束密度と保磁力のともに優れた
焼結磁心材料に関するものである。
DETAILED DESCRIPTION OF THE INVENTION The present invention relates to a sintered magnetic core material having excellent magnetic flux density and coercive force.

永久磁石のヨークとして用いられる焼結磁心の
材料は通常純鉄であり、その特性は磁束密度B25
が11〜15KG程度、保磁力Hcが0.6〜2.5Oe程度の
レベルにある。
The material of the sintered magnetic core used as the yoke of a permanent magnet is usually pure iron, and its characteristics are magnetic flux density B25
is around 11-15KG, and the coercive force Hc is around 0.6-2.5Oe.

しかし、永久磁石のヨークの中には上記レベル
の磁束密度と、より大きな保磁力とを必要とする
用途があり、材質の改良が望まれていた。
However, some permanent magnet yokes have applications that require the above-mentioned level of magnetic flux density and larger coercive force, and it has been desired to improve the material.

純鉄焼結材の保磁力を大きくするには、これに
炭素または銅を加えるのが有効である。しかし、
Fe−C系材料はその磁束密度が純鉄よりも低い
ので、所期の目的に合わない。また、通常の鉄銅
系の焼結合金は、その焼結時に「銅膨張」現象を
生じて焼結密度が低下し、それに伴い磁束密度も
低下する。
In order to increase the coercive force of pure iron sintered material, it is effective to add carbon or copper to it. but,
Since the magnetic flux density of Fe-C based materials is lower than that of pure iron, they are not suitable for the intended purpose. Further, when a typical iron-copper-based sintered alloy is sintered, a "copper expansion" phenomenon occurs, resulting in a decrease in sintered density and a corresponding decrease in magnetic flux density.

さきに本件出願人は、鉄銅系焼結合金における
焼結時の銅膨張が重量比で0.03%以上のホウ素の
存在によつて抑制されることを見出し、これを鉄
銅系高密度焼結合金の製造、ならびに圧粉体の接
合による複合焼結機械部品の製造に応用した。こ
の先発明(特願昭54−96389号)の内容は、特開
昭56−20142号として公開されている。
Previously, the applicant found that copper expansion during sintering in iron-copper sintered alloys was suppressed by the presence of boron of 0.03% or more by weight, and this was found to be suppressed in iron-copper-based high-density sintered alloys. It was applied to the production of gold and the production of composite sintered machine parts by joining green compacts. The content of the earlier invention (Japanese Patent Application No. 54-96389) has been published as Japanese Patent Application Laid-open No. 56-20142.

そして今回、密度低下の抑制による磁束密度の
改善という着想に基づいて上記先発明を焼結磁心
に応用したのがこの発明である。
This invention is based on the idea of improving magnetic flux density by suppressing density reduction, and applies the above-mentioned previous invention to a sintered magnetic core.

即ちこの発明は、銅0.5%〜15%を含有する鉄
−銅系の圧粉体を焼結して磁心を得るに際し、
0.03〜0.3%のホウ素を予め圧粉体に添加してお
くことをその骨子とするものである。
That is, this invention provides a method for obtaining a magnetic core by sintering an iron-copper compact containing 0.5% to 15% copper.
The gist of this method is to add 0.03 to 0.3% of boron to the powder compact in advance.

以下この発明を、その実施例を含む実験結果に
基づいて詳細に説明する。
The present invention will be described in detail below based on experimental results including examples thereof.

第1図は横軸に鉄−銅焼結材中の銅含有率を、
縦軸に焼結密度、保磁力および磁束密度をとり、
鉄粉と銅粉の混合粉の圧粉体を焼結する際に生じ
る寸法変化に対して、ホウ素の有無が如何に影響
するかを示したグラフである。試料の作成は粒度
100メツシユ以下で純度99%以上のアトマイズ鉄
粉、粒度が200メツシユ以下で純度99.6%以上の
電解銅粉の所定量、潤滑剤のステアリン酸亜鉛
0.5%、それにホウ素を含有させる試料の場合の
み、粒度が250メツシユ以下でホウ素含有量が20
%のフエロボロン粉を所定量配合して十分に混合
し、5t/cm2の成形圧で所定の試験片に成形し、ア
ンモニア分解ガス雰囲気の焼結炉中温度1150℃で
40分間焼結した。
In Figure 1, the horizontal axis shows the copper content in the iron-copper sintered material.
The vertical axis represents sintering density, coercive force, and magnetic flux density.
It is a graph showing how the presence or absence of boron influences the dimensional change that occurs when a green compact of a mixed powder of iron powder and copper powder is sintered. Sample preparation is based on particle size
Atomized iron powder with a particle size of 100 mesh or less and a purity of 99% or more, a specified amount of electrolytic copper powder with a particle size of 200 mesh or less and a purity of 99.6% or more, and zinc stearate as a lubricant.
0.5%, and only for samples containing boron, the particle size is less than 250 mesh and the boron content is 20%.
% of ferroboron powder was thoroughly mixed, molded into a specified test piece at a molding pressure of 5t/ cm2 , and heated at a temperature of 1150℃ in a sintering furnace in an ammonia decomposition gas atmosphere.
Sintered for 40 minutes.

第1図に示すように、鉄−銅焼結材(点線)は
銅含有率を増すにつれて保磁力は大きくなるが、
その反面、焼結時の膨張の影響で焼結密度が低下
するに伴い磁束密度は小さくなる。しかるに、こ
れに0.2%のホウ素を添加したもの(実線)は保
磁力の上昇率は幾分小さいものの、「銅膨張」が
抑制され焼結密度が低下しないため磁束密度は純
鉄のレベルを保つている。
As shown in Figure 1, the coercive force of the iron-copper sintered material (dotted line) increases as the copper content increases;
On the other hand, as the sintered density decreases due to the effect of expansion during sintering, the magnetic flux density decreases. However, when 0.2% boron is added (solid line), although the rate of increase in coercive force is somewhat smaller, "copper expansion" is suppressed and the sintered density does not decrease, so the magnetic flux density remains at the level of pure iron. ing.

即ちこの結果は、この発明によれば磁束密度は
従来材(純鉄)と同等で、且つ保持力はより優れ
た焼結磁心が得られることを示している。これは
別の表現をすれば、磁気エネルギー(磁束密度と
保磁力の積)のより大きな磁性材が得られること
を意味する。銅の好ましい含有率は、磁心の用途
が磁束密度と保磁力のいずれをより重視するかに
より異なるが、10%を中心とする8〜12%の例が
多い。ただし15%以上になると磁束密度が純鉄の
レベル以下に劣化するので、15%に止めるべきで
ある。一方、0.5%以下では純鉄の場合との有意
差が認められないので、0.5%を下限とする。尤
も、この値は常用範囲からみれば極めて小さく、
単なる限界的意義を持つに過ぎない。
In other words, this result shows that, according to the present invention, a sintered magnetic core with magnetic flux density equivalent to that of conventional material (pure iron) and superior coercive force can be obtained. Expressed in another way, this means that a magnetic material with greater magnetic energy (product of magnetic flux density and coercive force) can be obtained. The preferred content of copper varies depending on whether the use of the magnetic core emphasizes more on magnetic flux density or coercive force, but is often 8 to 12%, with a center of 10%. However, if it exceeds 15%, the magnetic flux density will deteriorate to below the level of pure iron, so it should be kept at 15%. On the other hand, if it is less than 0.5%, no significant difference from that of pure iron is observed, so 0.5% is set as the lower limit. Of course, this value is extremely small considering the range of normal use.
It has only marginal significance.

次に、第2図は銅の含有量が10%(実線)と4
%(点線)の場合について、ホウ素の添加量と焼
結材の諸特性との関係を示すもので、全体として
保磁力は銅含有量の高い方が、また磁束密度は銅
含有量の低い方が優れる傾向を示している。
Next, Figure 2 shows that the copper content is 10% (solid line) and 4%.
% (dotted line), it shows the relationship between the amount of boron added and various properties of the sintered material. Overall, the coercive force is higher when the copper content is higher, and the magnetic flux density is higher when the copper content is lower. shows a tendency to be superior.

焼結密度はホウ素の添加につれて上昇して添加
量0.1〜0.2%でピークを形成し、以後グラフは最
適の結果を示す0.2%に留めたが、0.3%迄は殆ど
変わらず、その後は漸減する。
The sintered density increases with the addition of boron and forms a peak at an addition amount of 0.1 to 0.2%.After that, the graph shows the optimal result at 0.2%, but there is almost no change up to 0.3%, and after that it gradually decreases. .

磁束密度はホウ素の添加によつて急激に上昇し
て添加量0.05〜0.1%でピークを形成し、以後0.3
%迄ほぼ同一のレベルを保つ。
The magnetic flux density increases rapidly with the addition of boron, forming a peak at an addition amount of 0.05 to 0.1%, and after that it increases to 0.3%.
% remains at almost the same level.

保磁力もホウ素の添加により上昇するが、その
ピークは銅の含有率により異なつている。そして
ピーク以後は漸減し、ホウ素0.2%における4.6〜
5.6が、0.3%では約10%減の4.0〜5.0に低下する。
Coercive force also increases with the addition of boron, but its peak differs depending on the copper content. After the peak, it gradually decreases to 4.6 at 0.2% boron.
5.6, but at 0.3% it drops by about 10% to 4.0-5.0.

以上の結果から総合すると、ホウ素の添加量は
銅膨張の抑制効果を生じる臨界値である0.03%を
下限とし、焼結密度、保磁力および磁束密度が調
和を保つ0.1〜0.2%の範囲が最も好ましい。
Overall, from the above results, the lower limit for the amount of boron added should be 0.03%, which is the critical value that produces the effect of suppressing copper expansion, and the range of 0.1 to 0.2%, where the sintered density, coercive force, and magnetic flux density are in harmony, is the best. preferable.

なお上限については、下限と異なり明確な臨界
現象は認められない。しかし過剰の添加が保磁力
を低下させる傾向は明らかであり、また焼結密度
も漸減することを併せ、0.3%までに留めるべき
である。
Regarding the upper limit, unlike the lower limit, no clear critical phenomenon is observed. However, it is clear that excessive addition tends to lower the coercive force, and since the sintered density also gradually decreases, it should be kept at 0.3% or less.

以上詳述したように、この発明の手法によれば
鉄銅系焼結合金の欠点であつた銅膨張を起こさず
に相当量の銅を含有させることができ、その結果
磁束密度と保磁力のともに優れた焼結磁心材料を
提供することができた。
As detailed above, according to the method of the present invention, a considerable amount of copper can be contained without causing copper expansion, which was a drawback of iron-copper sintered alloys, and as a result, magnetic flux density and coercive force can be improved. In both cases, we were able to provide excellent sintered magnetic core materials.

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

第1図は鉄−銅系焼結材の密度および磁気特性
に対する銅の含有量およびホウ素の有無の影響を
示すグラフ、第2図は同じくホウ素添加量の影響
を示すグラフである。
FIG. 1 is a graph showing the effects of copper content and the presence or absence of boron on the density and magnetic properties of iron-copper sintered materials, and FIG. 2 is a graph showing the effects of the amount of boron added.

Claims (1)

【特許請求の範囲】[Claims] 1 鉄銅系の焼結合金であつて、重量比でホウ素
0.03%〜0.3%、銅0.5%〜15%および鉄残部より
なることを特徴とする磁束密度および保磁力の大
きい焼結磁心。
1 Iron-copper based sintered alloy with boron content in weight ratio
A sintered magnetic core with high magnetic flux density and coercive force, characterized by comprising 0.03% to 0.3% copper, 0.5% to 15% copper, and the balance iron.
JP15769681A 1981-10-03 1981-10-03 Sintered magnetic core having high coercive force Granted JPS5858708A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP15769681A JPS5858708A (en) 1981-10-03 1981-10-03 Sintered magnetic core having high coercive force

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP15769681A JPS5858708A (en) 1981-10-03 1981-10-03 Sintered magnetic core having high coercive force

Publications (2)

Publication Number Publication Date
JPS5858708A JPS5858708A (en) 1983-04-07
JPS6349883B2 true JPS6349883B2 (en) 1988-10-06

Family

ID=15655378

Family Applications (1)

Application Number Title Priority Date Filing Date
JP15769681A Granted JPS5858708A (en) 1981-10-03 1981-10-03 Sintered magnetic core having high coercive force

Country Status (1)

Country Link
JP (1) JPS5858708A (en)

Also Published As

Publication number Publication date
JPS5858708A (en) 1983-04-07

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