JPH0217457Y2 - - Google Patents

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Publication number
JPH0217457Y2
JPH0217457Y2 JP12743984U JP12743984U JPH0217457Y2 JP H0217457 Y2 JPH0217457 Y2 JP H0217457Y2 JP 12743984 U JP12743984 U JP 12743984U JP 12743984 U JP12743984 U JP 12743984U JP H0217457 Y2 JPH0217457 Y2 JP H0217457Y2
Authority
JP
Japan
Prior art keywords
slot
ferrite magnetic
magnetic core
ferrite
screwdriver
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
JP12743984U
Other languages
Japanese (ja)
Other versions
JPS6142817U (en
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 filed Critical
Priority to JP12743984U priority Critical patent/JPS6142817U/en
Publication of JPS6142817U publication Critical patent/JPS6142817U/en
Application granted granted Critical
Publication of JPH0217457Y2 publication Critical patent/JPH0217457Y2/ja
Granted legal-status Critical Current

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Description

【考案の詳細な説明】 〔産業上の利用分野〕 この考案は、コイルのインダクタンスの調整に
使用されるフエライト磁心に関する。
[Detailed Description of the Invention] [Industrial Application Field] This invention relates to a ferrite magnetic core used for adjusting the inductance of a coil.

〔従来の技術〕[Conventional technology]

フエライト磁心は、第5図〜第7図で示すよう
に、円柱形の本体1の周面2にねじ溝を設け、端
面にドライバー等の回転工具の先端を挿入するた
めの溝穴3を設けたものである。従来におけるフ
エライト磁心は、この溝穴3の平面形状及び水平
断面形状が何れも矩形になるよう形成されてい
た。
As shown in FIGS. 5 to 7, the ferrite magnetic core has a cylindrical main body 1 with a threaded groove on its circumferential surface 2, and a slotted hole 3 on its end surface for inserting the tip of a rotating tool such as a screwdriver. It is something that In the conventional ferrite magnetic core, the slot 3 has a rectangular planar shape and a horizontal cross-sectional shape.

〔考案が解決しようとする問題点〕[Problem that the invention attempts to solve]

この従来のフエライト磁心では、上記溝穴3に
ドライバー等の先端を挿入して回転させたときの
トルク強度が弱く、同溝穴3の隅角部分から比較
的簡単に破壊されてしまうという問題が指摘され
ている。
This conventional ferrite magnetic core has a problem in that the torque strength is weak when the tip of a screwdriver or the like is inserted into the slot 3 and rotated, and it is relatively easily broken from the corner part of the slot 3. It has been pointed out.

この主な原因は、製造過程で次ぎのようにして
生じるものと考えられる。即ち、フエライト磁心
の大量生産工程では、フエライト粉末をロータリ
ープレスで加圧成形することが行われるが、この
際、第8図で示すように、フエライト粉末aは、
水平に回転するテーブル4に保持されながら、円
形の軌跡bに沿つて送られていく。他方、これを
成形するパンチ5は、上記ロータリーテーブル4
の上位(または下位)に配置され、水平な回転軸
を有する押圧ローラ6によつて押下せしめられ
る。従つて、パンチ5の頭部に押圧ローラ6が偏
つて接触する所で、上記軌跡bと押圧ローラ6の
回転方向とのずれやパンチ5に対する押圧ローラ
6の作用線のずれ等によつて、パンチ5に矢印方
向の回転力が働く。すると、フエライト粉末aに
は、成形中にパンチ5によつて捩り力が与えら
れ、これによつて成形体、特にその溝穴の隅角部
に微細なクラツクが発生する。
The main cause of this is thought to occur in the manufacturing process as follows. That is, in the mass production process of ferrite magnetic cores, ferrite powder is pressure-molded using a rotary press. At this time, as shown in FIG. 8, ferrite powder a is
It is fed along a circular trajectory b while being held by a horizontally rotating table 4. On the other hand, the punch 5 for forming this is attached to the rotary table 4.
The pressure roller 6 is placed above (or below) and is pressed down by a pressure roller 6 having a horizontal rotation axis. Therefore, at the place where the pressure roller 6 contacts the head of the punch 5 in an uneven manner, due to a deviation between the above-mentioned locus b and the rotational direction of the pressure roller 6, a deviation in the line of action of the pressure roller 6 with respect to the punch 5, etc. A rotational force acts on the punch 5 in the direction of the arrow. Then, a twisting force is applied to the ferrite powder a by the punch 5 during molding, and this causes minute cracks to occur in the molded product, particularly at the corners of its slots.

溝穴の隅角部は、元々応力が集中しやすいうえ
に、上記のような微細なクラツクが生じているこ
とから、コイルのインダクタンスを調整するた
め、上記フエライト磁心をコイルボビンのねじ穴
にねじ込み、ドライバーで回転する際等に、溝穴
3の隅角部を中心として破損されやすい。そして
このような破損は、ドライバー先端の角部が擦り
減り、回転時にドライバーの先端が溝穴3に対し
て滑りを生じるようになると一層頻繁に起こるよ
うになる。
Stress tends to concentrate at the corners of the slot holes, and the minute cracks mentioned above occur, so in order to adjust the inductance of the coil, the ferrite magnetic core was screwed into the screw hole of the coil bobbin. When rotating with a screwdriver, etc., the corners of the slot 3 are likely to be damaged. Such damage will occur more frequently if the corner of the driver tip becomes worn and the tip of the driver starts to slip against the slot 3 during rotation.

この考案は、従来のフエライト磁心における上
記のような問題を解消すべくなされたものであつ
て、ドライバー等の先端を差し込むことができる
従来の溝穴の基本形状をそのまゝ維持しながら、
同溝穴に特殊な形状を採用することにより、従来
のものに比べてトルク強度の高いフエライト磁心
を提供することを目的とするものである。
This idea was made to solve the above-mentioned problems with conventional ferrite magnetic cores, and while maintaining the basic shape of the conventional slot into which the tip of a screwdriver etc. can be inserted,
By adopting a special shape for the slot, the purpose is to provide a ferrite magnetic core with higher torque strength than conventional ones.

〔問題を解決するための手段〕[Means to solve the problem]

以下、この考案の構成を第1図〜第3図に基づ
き詳細に説明する。
Hereinafter, the configuration of this invention will be explained in detail based on FIGS. 1 to 3.

フエライト磁心11の溝穴13は、ドライバー
等の回転工具の先端を差し込む関係から、必然的
に平面形状及び水平断面形状が矩形に近い形状を
呈している。この考案では、この基本形状を維持
しながら、溝穴13の一方の対向面に当たる2面
を長辺よりなる平面14,14によつて形成し、
他方の対向面に当たる2面を平面14より短い円
弧面15,15によつて形成する。
The slot 13 of the ferrite magnetic core 11 necessarily has a planar shape and a horizontal cross-sectional shape close to a rectangle because the tip of a rotating tool such as a screwdriver is inserted into the slot 13 . In this invention, while maintaining this basic shape, two opposing surfaces of the slot 13 are formed by planes 14, 14 consisting of long sides,
The other two opposing surfaces are formed by arcuate surfaces 15, 15 shorter than the plane 14.

円弧面15,15は、周面12と同心円状のも
のが望ましく、円弧面15,15から平面14,
14に続く部分は、滑らかな曲面によつて連続さ
せ、角部を設けないのがよい。なお、この溝穴1
3は、ドライバー等の先端を差し込みやすいよう
に、開口部側が広く、奥へ行くに従つて挟くなる
よう形成するのが通例である。
The arcuate surfaces 15, 15 are preferably concentric with the circumferential surface 12, and from the arcuate surfaces 15, 15, the flat surface 14,
It is preferable that the portion following 14 be continuous with a smooth curved surface and have no corners. In addition, this slot 1
3 is usually formed so that the opening side is wide and the opening becomes narrower toward the back so that the tip of a screwdriver or the like can be easily inserted.

〔作 用〕[Effect]

この考案によるフエライト磁心では、溝穴13
の平面14,14と円弧面15,15との交叉角
が従来の矩形の溝穴の場合に比べて純くなる。従
つて、原料の成形密度のむらが小さくなり、円弧
面15,15と周面12間の成形密度が高くな
る。この点から、成形時にロータリープレスのパ
ンチ5が回転して、溝穴13の平面14,14に
過重が加わつても、成形体内部の歪を小さく抑え
ることができ、微細なクラツクの発生を防止する
ことができる。また溝穴の隅角部に応力の集中も
起こりにくゝなる。
In the ferrite magnetic core according to this invention, the slot 13
The intersecting angle between the planes 14, 14 and the arcuate surfaces 15, 15 is simpler than in the case of a conventional rectangular slot. Therefore, the unevenness in the molding density of the raw material is reduced, and the molding density between the arcuate surfaces 15, 15 and the circumferential surface 12 is increased. From this point of view, even if the punch 5 of the rotary press rotates during molding and excessive weight is applied to the flat surfaces 14, 14 of the slot 13, the distortion inside the molded product can be suppressed to a small level, and the occurrence of minute cracks can be prevented. can do. In addition, stress concentration at the corners of the slot becomes less likely.

〔実施例〕〔Example〕

次ぎに、上記の作用を確認するため、この考案
の実施例について説明する。
Next, an example of this invention will be described in order to confirm the above-mentioned effect.

Fe−Ni−Zn系のフエライト粉末をロータリー
プレスにてIton/cm2の圧力で加圧成形した。この
成形体は、直径3.2mm、長さ6mmの円柱形のもの
で、両端面に深さ1.4mmの溝穴が設けられている。
この溝穴は、平面形状及び水平断面形状が矩形に
近いもので、その長辺側が平面によつて形成さ
れ、短辺側が周面と同心円を含む円弧面によつて
形成されている。また、この溝穴の開口部は広
く、奥へ行くに従つて次第に狭くなつている。
Fe-Ni-Zn-based ferrite powder was pressure-molded using a rotary press at a pressure of Iton/cm 2 . This molded body has a cylindrical shape with a diameter of 3.2 mm and a length of 6 mm, and slots with a depth of 1.4 mm are provided on both end faces.
This slot has a planar shape and a horizontal cross-sectional shape that are close to rectangular, and its long side is formed by a flat surface, and its short side is formed by an arcuate surface including a concentric circle with the circumferential surface. Also, the opening of this slot is wide and gradually narrows as it goes deeper.

この成形体をトンネル炉にて焼成して焼結させ
た後、周面にねじ溝を切り込み、第1図〜第3図
で示すよようなフエライト磁心を作つた。
After this compact was sintered by firing in a tunnel furnace, thread grooves were cut into the circumferential surface to produce a ferrite magnetic core as shown in FIGS. 1 to 3.

このフエライト磁心250個について溝穴13に
ドライバーの先端を嵌め込み、捩りを与えてトル
ク強度を測定したところ、第4図の左側に示すよ
うな結果となつた。即ち、これらのサンプルで
は、トルク強度が500〜1000g・cmの範囲に分布
し、特に700〜800g・cmに集中した。
When the tip of a screwdriver was inserted into the slot 13 of these 250 ferrite magnetic cores and the torque strength was measured by applying twist, the results were as shown on the left side of FIG. 4. That is, in these samples, the torque strength was distributed in the range of 500 to 1000 g·cm, and was particularly concentrated in the range of 700 to 800 g·cm.

〔比較例〕[Comparative example]

上記実施例と比較のため、Fe−Ni−Zn系のフ
エライト粉末から同様の方法で第5図〜第7図に
示すようなフエライト磁心を製作した。このフエ
ライト磁心の溝穴3は、これを囲む4面が何れも
平面によつて形成され、その平面形状及び水平断
面形状が完全な矩形を呈している。
For comparison with the above examples, ferrite magnetic cores as shown in FIGS. 5 to 7 were manufactured from Fe--Ni--Zn based ferrite powder using the same method. The slot 3 of this ferrite magnetic core has four plane surfaces surrounding it, and its planar shape and horizontal cross-sectional shape are completely rectangular.

このフエライト磁心250個について上記実施例
と同様の方法でトルク強度を測定したところ、第
4図の左右側に示すような結果となつた。即ち、
これらのサンプルでは、トルク強度が200〜600
g・cmの範囲に分布し、特に300〜500g・cmに集
中した。
When the torque strength of 250 of these ferrite magnetic cores was measured in the same manner as in the above example, the results were as shown on the left and right sides of FIG. 4. That is,
In these samples, the torque strength is between 200 and 600
It was distributed in the g·cm range, and was particularly concentrated in the range of 300 to 500 g·cm.

〔考案の効果〕[Effect of idea]

以山説明した通り、この考案によれば矩形に近
い従来の溝穴の基本形状をそのまゝ維持しなが
ら、成形時に生じる微細なクラツク等によるフエ
ライト磁心のトルク強度の低下を防止することが
できる。従つてトルク強度の向上を図ることがで
きると同時に、従来使用されていたのと同じドラ
イバー等の工具を使用することができるので便利
である。
As explained above, with this invention, it is possible to maintain the basic shape of the conventional slotted hole, which is close to a rectangle, while preventing the reduction in torque strength of the ferrite magnetic core due to minute cracks that occur during molding. . Therefore, it is possible to improve the torque strength, and at the same time, it is convenient because the same tools such as a screwdriver that have been used in the past can be used.

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

第1図は、この考案の実施例を示すフエライト
磁心の平面図、第2図は、第1図のA−A線断面
図、第3図は、第1図のB−B線断面図、第4図
は、上記実施例とその比較例のトルク試験の結果
を示すグラフ、第5図は、フエライト磁心の従来
例を示す平面図、第6図は、第5図のA−A線断
面図、第7図は、第5図のB−B線断面図、第8
図は、フエライト磁心の加圧成形工程の概略を示
すプレス装置の説明図であり、同図イが側面図、
同図ロが平面配置図である。 11……本体、12……周面、13……溝穴、
14……平面、15……円弧面。
FIG. 1 is a plan view of a ferrite magnetic core showing an embodiment of this invention, FIG. 2 is a cross-sectional view taken along the line A-A in FIG. 1, and FIG. 3 is a cross-sectional view taken along the line B-B in FIG. FIG. 4 is a graph showing the results of the torque test of the above example and its comparative example, FIG. 5 is a plan view showing a conventional example of a ferrite magnetic core, and FIG. 6 is a cross section taken along the line A-A in FIG. Figure 7 is a sectional view taken along line B-B in Figure 5, and Figure 8 is
The figure is an explanatory diagram of a press device showing an outline of the pressure forming process of a ferrite magnetic core, and A is a side view;
Figure B is a plan layout. 11...Main body, 12...Surrounding surface, 13...Slot hole,
14...Flat surface, 15...Circular surface.

Claims (1)

【実用新案登録請求の範囲】[Scope of utility model registration request] フエライト製の円柱形をした本体11の外周面
12にねじ溝が設けられ、少なくとも一方の端面
の開口形状が四面からなる溝穴13が設けられて
なるフエライト磁心において、溝穴13の一方に
対向する面が平面14によつて形成され、他方に
対向する面が円弧面15によつて形成されたこと
を特徴とするフエライト磁心。
In a ferrite magnetic core, a threaded groove is provided on the outer circumferential surface 12 of a cylindrical main body 11 made of ferrite, and a slot 13 having a four-sided opening on at least one end face is provided, and one of the slots 13 is opposed to the other. A ferrite magnetic core characterized in that one surface facing the other is formed by a flat surface 14, and the other opposing surface is formed by an arcuate surface 15.
JP12743984U 1984-08-22 1984-08-22 ferrite magnetic core Granted JPS6142817U (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP12743984U JPS6142817U (en) 1984-08-22 1984-08-22 ferrite magnetic core

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP12743984U JPS6142817U (en) 1984-08-22 1984-08-22 ferrite magnetic core

Publications (2)

Publication Number Publication Date
JPS6142817U JPS6142817U (en) 1986-03-19
JPH0217457Y2 true JPH0217457Y2 (en) 1990-05-16

Family

ID=30686083

Family Applications (1)

Application Number Title Priority Date Filing Date
JP12743984U Granted JPS6142817U (en) 1984-08-22 1984-08-22 ferrite magnetic core

Country Status (1)

Country Link
JP (1) JPS6142817U (en)

Also Published As

Publication number Publication date
JPS6142817U (en) 1986-03-19

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