JP2540135Y2 - Split cylindrical ferrite core - Google Patents

Split cylindrical ferrite core

Info

Publication number
JP2540135Y2
JP2540135Y2 JP6260291U JP6260291U JP2540135Y2 JP 2540135 Y2 JP2540135 Y2 JP 2540135Y2 JP 6260291 U JP6260291 U JP 6260291U JP 6260291 U JP6260291 U JP 6260291U JP 2540135 Y2 JP2540135 Y2 JP 2540135Y2
Authority
JP
Japan
Prior art keywords
core
split
cylindrical
ferrite core
ferrite
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
JP6260291U
Other languages
Japanese (ja)
Other versions
JPH058917U (en
Inventor
秀一 立谷
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.)
Tokin Corp
Original Assignee
Tokin Corp
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 Tokin Corp filed Critical Tokin Corp
Priority to JP6260291U priority Critical patent/JP2540135Y2/en
Publication of JPH058917U publication Critical patent/JPH058917U/en
Application granted granted Critical
Publication of JP2540135Y2 publication Critical patent/JP2540135Y2/en
Anticipated expiration legal-status Critical
Expired - Lifetime legal-status Critical Current

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Description

【考案の詳細な説明】[Detailed description of the invention]

【0001】[0001]

【産業上の利用分野】本考案は、電子機器と電子機器と
を結ぶ、信号線における高周波電磁ノイズを防止するた
めに用いる分割型筒状フェライトコアの構造に関するも
のである。
BACKGROUND OF THE INVENTION 1. Field of the Invention The present invention relates to the structure of a split-type cylindrical ferrite core used for preventing high-frequency electromagnetic noise in a signal line connecting electronic equipment with electronic equipment.

【0002】[0002]

【従来の技術】従来、機器間の信号線を接続する信号線
間の電磁ノイズを抑制するためには、図3に示すよう
に、信号線2がアンテナとして作用している信号線のイ
ンピーダンスを大きくするため、信号線2に筒状フェラ
イトコア1を貫通させて高周波電磁ノイズの放射を防止
してデータラインフィルタとしている。配設ずみの信号
線に対しては、半円筒形のフェライトコアのコア分割片
の2個からなる分割型筒状フェライトコア(以下コアと
称す)が用いられ、樹脂製の結束帯でコア分割片の外周
を緊縛するか、ヒンジで連結した分割型ケースを被せる
かして、信号線を両側から挟んで筒状に保持していた。
2. Description of the Related Art Conventionally, in order to suppress electromagnetic noise between signal lines connecting signal lines between devices, as shown in FIG. 3, the impedance of a signal line in which a signal line 2 acts as an antenna is reduced. In order to increase the size, a cylindrical ferrite core 1 is passed through the signal line 2 to prevent radiation of high-frequency electromagnetic noise, thereby forming a data line filter. For the installed signal lines, a split cylindrical ferrite core (hereinafter referred to as a core) consisting of two core split pieces of a semi-cylindrical ferrite core is used, and the core is split by a resin band. The signal line is held in a tubular shape by sandwiching the signal line from both sides by binding the outer periphery of the piece or covering the split type case connected by a hinge.

【0003】[0003]

【考案が解決しようとする課題】従来の半円筒形のコア
分割片の場合、結束帯やケースが必要である上、結束帯
は扱いが厄介である欠点と、正確に筒状に突き合わせて
緊縛することが難しい欠点があり、ケースはコア分割片
をケースに収納できるように寸法精度よく作る必要があ
った。また、コア分割片を結束帯やケースを損傷せずに
信号線から取り外すことが容易でなく、分割型筒状フェ
ライトコアを交換することが困難であるという問題もあ
った。
In the case of the conventional semi-cylindrical core segment, a binding band and a case are required, and the binding band has a drawback that it is cumbersome to handle. There is a drawback that it is difficult to perform the operation, and the case has to be made with high dimensional accuracy so that the core divided pieces can be stored in the case. Further, there is a problem that it is not easy to remove the core split piece from the signal line without damaging the binding band and the case, and it is difficult to replace the split cylindrical ferrite core.

【0004】[0004]

【課題を解決するための手段】前記課題を解決するため
に、本考案はコア分割片を、筒状体軸線に沿いかつ中間
に垂直段部を設けて二分割した樋形状とし、この段部に
着磁したフェライト磁石をその磁極を段部に当接して配
接し、コア分割片を筒状に組合わせる。
In order to solve the above-mentioned problems, according to the present invention, a core divided piece is formed into a gutter shape which is divided into two along a cylindrical body axis and provided with a vertical step in the middle. The ferrite magnet magnetized is arranged in contact with its magnetic pole in contact with the step, and the core divided pieces are combined in a cylindrical shape.

【0005】[0005]

【作用】段部に配接した着磁されたフェライト磁石は、
磁気的吸着力でコア分割片を筒状に保つよう働き、また
筒状体の軸線方向に、コア分割体にその末飽和領域の直
流磁界を印加し、磁壁の移動を抑制し比透磁率特性の高
周波における損失成分を減少させる。この損失減少は、
高周波成分に対するインピーダンスの減少を抑制し、イ
ンピーダンスの高周波数特性の絶対値を高める。
[Function] The magnetized ferrite magnet connected to the step is
The magnetic attraction force keeps the core split piece cylindrical, and applies a DC magnetic field in the last saturation region to the core split body in the axial direction of the cylindrical body to suppress the movement of the domain wall and to achieve relative permeability characteristics. Loss component at high frequencies. This loss reduction is
A decrease in impedance with respect to a high frequency component is suppressed, and the absolute value of the high frequency characteristic of the impedance is increased.

【0006】即ち本考案は、筒状体の軸線に沿い、かつ
中間に垂直段部を設けて二分割したコア分割体を、段部
に磁極を当接して配設したフェライト磁石を介してコア
分割体を筒状に組み合わせたことを特徴とする分割型筒
状フェライトコアである。
That is, according to the present invention, a core split body divided into two along a cylinder axis and provided with a vertical step in the middle is provided through a ferrite magnet provided with a magnetic pole in contact with the step. A divided cylindrical ferrite core, wherein divided bodies are combined in a cylindrical shape.

【0007】[0007]

【実施例】図1(a)は、本考案による分割型筒状フェ
ライトコアの一実施例の外観斜視図である。図1に示す
本考案による分割型筒状フェライトコアは、2個のコア
分割体3と、2個(1個を図示)のフェライト磁石(以
下磁石と称す)4からなる。コア分割体3(以下分割体
と称す)は、断面八角形の筒状体の軸線に沿い、かつ図
1の(b)に示すように中央に同じ向きの垂直段部5
(以下段部と称す)があるように二等分割し、段部5を
若干後退させている樋形状である。磁石4は直方体のも
ので、磁極面が段部5に対応する矩形である。磁極面の
間隔は、段部5の中央からの後退長さの約2倍である。
フェライト磁石4は、高い材料固有抵抗を有し、信号線
に流れる信号電流が作る磁界により渦電流を生ずること
のない、即ち損失の発生しない材質である。1個目のコ
ア分割体3の段部5に、磁極面を当接し磁極の向きを同
じか、逆向きにして2個の磁石4をそれぞれ配設する。
この一方の分割体3を信号線(図示しない)の下にして
中央溝に信号線を通して配置し、2個目の分割体3を磁
石4の磁極面に段部5に対向して組み合わせる。図1の
(a)に示すように、分割体3の端面がほぼ面一になっ
た分割型筒状フェライトコアが、磁石4の磁気的吸着力
により出来上がる。原理的には分割体3の段部5が1箇
所であっても筒状に保持できるが、強固に保持出来ない
ので実用的ではなく、コア分割体の両側にフェライト磁
石を配置する。また直流磁界の印加が局部的である点か
らも好ましくない。分割体3の材質が飽和磁束密度30
00ガウスのニッケル系フェライト材である場合、磁石
4の磁化の強さが約500ガウスのもので、高周波輻射
ノイズ防止能力が最良である。
FIG. 1A is an external perspective view of one embodiment of a split-type tubular ferrite core according to the present invention. The split cylindrical ferrite core according to the present invention shown in FIG. 1 includes two core split bodies 3 and two (one is shown) ferrite magnets (hereinafter, referred to as magnets) 4. The core divided body 3 (hereinafter referred to as a divided body) has a vertical stepped portion 5 having the same direction along the axis of the cylindrical body having an octagonal cross section and having the same direction as shown in FIG.
(Hereinafter referred to as “step”), and has a gutter shape in which the step 5 is slightly retreated. The magnet 4 is a rectangular parallelepiped, and has a rectangular magnetic pole surface corresponding to the step 5. The interval between the pole faces is about twice the retreat length from the center of the step 5.
The ferrite magnet 4 has a high material specific resistance, and does not generate an eddy current due to a magnetic field generated by a signal current flowing through a signal line, that is, a material that does not generate a loss. The two magnets 4 are disposed on the stepped portion 5 of the first core segment 3 with the magnetic pole surfaces in contact with the magnetic poles in the same or opposite directions.
One of the divided bodies 3 is arranged under the signal line (not shown) through the signal line in the central groove, and the second divided body 3 is combined with the magnetic pole surface of the magnet 4 so as to face the step 5. As shown in FIG. 1A, a divided cylindrical ferrite core in which the end faces of the divided body 3 are substantially flush is formed by the magnetic attraction force of the magnet 4. In principle, even if there is only one step 5 in the split body 3, it can be held in a cylindrical shape, but it is not practical because it cannot be firmly held, and ferrite magnets are arranged on both sides of the core split body. Further, it is not preferable in that the application of the DC magnetic field is local. The material of the divided body 3 has a saturation magnetic flux density of 30.
In the case of a nickel-based ferrite material of 00 gauss, the magnet 4 has a magnetization strength of about 500 gauss and has the best high-frequency radiation noise prevention ability.

【0008】図2は、本考案の他の実施例の分解斜視図
である。この実施例のコア分割体6は、2箇所の段部5
を逆向きに形成している。先に説明したと同様に、段部
5に磁石4(鎖線で示す)を磁極の向きと同じに、かつ
軸線と平行に配設して分割型筒状フェライトコアに組み
立てる。コア分割体6は、端面が面一である筒状にする
ための磁石4の大きさが容易にわかる利点がある。ま
た、本考案はコア分割体を2個の磁石で組つける例で示
したが、コア分割体の両端に各々1個ずつ計4個の磁石
を用いることにより、より強固にコア分割体を固定する
ことが出来る。
FIG. 2 is an exploded perspective view of another embodiment of the present invention. The core split body 6 of this embodiment has two step portions 5.
Are formed in the opposite direction. As described above, the magnet 4 (indicated by a chain line) is disposed on the step portion 5 in the same direction as the magnetic pole and parallel to the axis, and assembled into a split-type cylindrical ferrite core. The core divided body 6 has an advantage that the size of the magnet 4 for making the end face flush with the cylindrical shape can be easily recognized. Although the present invention has been described with an example in which the core divided body is assembled with two magnets, the core divided body is more firmly fixed by using a total of four magnets, one at each end of the core divided body. You can do it.

【0009】[0009]

【考案の効果】本考案は、上述のとおり構成されている
ので、次に記載する効果を奏する。磁石の磁気的吸着力
で筒状に保持するので、信号線に装着することが容易で
ある。また、信号線から簡単に取り外すことが出来る。
筒状に保持するための部材が必要でないので、資材費を
節減出来、取り外しや交換を無駄なく実施できる。磁石
による筒状体の軸線方向への直流磁界の印加により、デ
ータラインとしての高周波電磁ノイズに対する減衰効果
が高まる。
The present invention is configured as described above, and has the following effects. Since it is held in a cylindrical shape by the magnetic attraction of the magnet, it is easy to mount it on the signal line. Also, it can be easily removed from the signal line.
Since a member for holding the tube is not required, material costs can be reduced, and removal and replacement can be performed without waste. By applying a DC magnetic field in the axial direction of the cylindrical body by the magnet, the effect of attenuating high-frequency electromagnetic noise as a data line is enhanced.

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

【図1】本考案による分割型筒状フェライトコアの一実
施例を示す外観斜視図であり、図1の(a)は完成斜視
図、図1の(b)は分解斜視図。
1 is an external perspective view showing an embodiment of a split type cylindrical ferrite core according to the present invention, wherein FIG. 1 (a) is a completed perspective view, and FIG. 1 (b) is an exploded perspective view.

【図2】本考案の他の実施例を示す分解斜視図。FIG. 2 is an exploded perspective view showing another embodiment of the present invention.

【図3】従来の非分割型の筒状フェライトコアを信号線
への装着した斜視図。
FIG. 3 is a perspective view showing a conventional non-split type ferrite core attached to a signal line.

【符号の説明】[Explanation of symbols]

1 筒状フェライトコア 2 信号線 3 コア分割体 4 フェライト磁石 5 垂直段部 6 コア分割体 DESCRIPTION OF SYMBOLS 1 Cylindrical ferrite core 2 Signal line 3 Core division body 4 Ferrite magnet 5 Vertical step part 6 Core division body

Claims (1)

(57)【実用新案登録請求の範囲】(57) [Scope of request for utility model registration] 【請求項1】 筒状体の軸線に沿い、かつ中間に垂直段
部を設けて二分割したコア分割体を、段部に磁極を当接
して配設したフェライト磁石を介してコア分割体を筒状
に組み合わせたことを特徴とする分割型筒状フェライト
コア。
1. A core split body which is divided into two along a cylindrical body axis and provided with a vertical step in the middle, and a core split through a ferrite magnet which is disposed with a magnetic pole in contact with the step. A split type cylindrical ferrite core characterized by being combined in a cylindrical shape.
JP6260291U 1991-07-12 1991-07-12 Split cylindrical ferrite core Expired - Lifetime JP2540135Y2 (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP6260291U JP2540135Y2 (en) 1991-07-12 1991-07-12 Split cylindrical ferrite core

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP6260291U JP2540135Y2 (en) 1991-07-12 1991-07-12 Split cylindrical ferrite core

Publications (2)

Publication Number Publication Date
JPH058917U JPH058917U (en) 1993-02-05
JP2540135Y2 true JP2540135Y2 (en) 1997-07-02

Family

ID=13205044

Family Applications (1)

Application Number Title Priority Date Filing Date
JP6260291U Expired - Lifetime JP2540135Y2 (en) 1991-07-12 1991-07-12 Split cylindrical ferrite core

Country Status (1)

Country Link
JP (1) JP2540135Y2 (en)

Families Citing this family (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JP6421424B2 (en) * 2014-03-07 2018-11-14 北川工業株式会社 Bus bar assembly and method of manufacturing bus bar assembly
DE102015110142A1 (en) * 2015-06-24 2016-12-29 Epcos Ag Inductive component for a busbar

Also Published As

Publication number Publication date
JPH058917U (en) 1993-02-05

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A01 Written decision to grant a patent or to grant a registration (utility model)

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Effective date: 19970107