JPS6338220A - Common mode choke coil for pulse transmission line - Google Patents

Common mode choke coil for pulse transmission line

Info

Publication number
JPS6338220A
JPS6338220A JP18225486A JP18225486A JPS6338220A JP S6338220 A JPS6338220 A JP S6338220A JP 18225486 A JP18225486 A JP 18225486A JP 18225486 A JP18225486 A JP 18225486A JP S6338220 A JPS6338220 A JP S6338220A
Authority
JP
Japan
Prior art keywords
core
common mode
windings
wound
magnetic
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.)
Granted
Application number
JP18225486A
Other languages
Japanese (ja)
Other versions
JPH0666199B2 (en
Inventor
Kusuo Takagi
高木 国主男
Hideo Tanaka
秀夫 田中
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.)
Nippon Telegraph and Telephone Corp
Original Assignee
Nippon Telegraph and Telephone 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 Nippon Telegraph and Telephone Corp filed Critical Nippon Telegraph and Telephone Corp
Priority to JP18225486A priority Critical patent/JPH0666199B2/en
Publication of JPS6338220A publication Critical patent/JPS6338220A/en
Publication of JPH0666199B2 publication Critical patent/JPH0666199B2/en
Anticipated expiration legal-status Critical
Expired - Fee Related legal-status Critical Current

Links

Classifications

    • HELECTRICITY
    • H01ELECTRIC ELEMENTS
    • H01FMAGNETS; INDUCTANCES; TRANSFORMERS; SELECTION OF MATERIALS FOR THEIR MAGNETIC PROPERTIES
    • H01F38/00Adaptations of transformers or inductances for specific applications or functions
    • H01F38/20Instruments transformers
    • H01F38/22Instruments transformers for single phase ac
    • H01F38/28Current transformers
    • H01F38/30Constructions
    • H01F2038/305Constructions with toroidal magnetic core

Landscapes

  • Coils Or Transformers For Communication (AREA)

Abstract

PURPOSE:To provide good particle characteristics over a wide band to a common mode noise current which conducts through a transmission line thereby to be able to apply it to a high speed pulse transmission line by forming a densely concentrated winding on the short axis magnetic path of symmetrical magnetic paths, and forming a rough winding on a part except the part on which the concentrated winding is wound. CONSTITUTION:A closed magnetic path core 12 has a long axis X-X and a short axis Y-Y, and is so formed symmetrically with respect to the axis Y-Y that a distance between opposed magnetic paths becomes maximum near the axis Y-Y. Windings 13, 13 are formed in a multilayer or concentrically wound at that part of the length l0 of the core 12 where the distance between the opposing magnetic paths is maximum. Windings 15, 15' are roughly wound uniformly oppositely to the parts of lengths l1, l2 longer than l0 of the core 12, and the winding directions of the windings wound between input/output terminals 10-11 and 10'-11' are so formed so that magnetic fluxes generated in the core 12 are in the same direction of a common mode current flowing in phase from one terminal and strengthen each other.

Description

【発明の詳細な説明】 〔産業上の利用分野〕 本発明は、パルス平衡伝送路を同方向に伝導する高周波
のコモンモードノイズを広帯域にわたり阻止するコモン
モードチョークコイルに関するものである。
DETAILED DESCRIPTION OF THE INVENTION [Field of Industrial Application] The present invention relates to a common mode choke coil that blocks high frequency common mode noise transmitted in the same direction in a pulse balanced transmission line over a wide band.

〔従来技術〕[Prior art]

第9図は、平衡伝送路を伝導するパルス信号および外来
電磁雑音の誘導によるコモンモード雑t″f電流の伝導
状況を説明するための図であり、1゜1′は平衡伝送路
、2は伝送路1,1′に接続さtyだパルス信号伝送装
置−8nは伝送路1,1′を伝導するパルス列からなる
ディジタル信号、3は装置2が収容された電話局等の建
物、4は放送波。
FIG. 9 is a diagram for explaining the conduction status of common mode noise t″f current due to the induction of pulse signals and external electromagnetic noise conducted in a balanced transmission line, where 1°1′ is a balanced transmission line, 2 is a A pulse signal transmission device 8n connected to the transmission lines 1 and 1' is a digital signal consisting of a pulse train transmitted through the transmission lines 1 and 1', 3 is a building such as a telephone office in which the device 2 is housed, and 4 is a broadcasting device. wave.

無線波や、高周波機器等からの外来雑音、Ncは外来雑
音4の伝送路1,1′への誘導によるコモンモード雑音
電流、5は伝送路1,1′に接続された通信端末機器、
6は通信端末機器5の対地インピーダンス、7は伝送路
を流れるコモンモー1〜雑音電流Ncの侵入を防11二
するため通4n端末機)li+5の信号入力部に挿入さ
れたコモンモードチョークコイルである。
External noise from radio waves, high frequency equipment, etc., Nc is a common mode noise current due to induction of external noise 4 into transmission lines 1, 1', 5 is communication terminal equipment connected to transmission lines 1, 1',
6 is the ground impedance of the communication terminal equipment 5, and 7 is a common mode choke coil inserted into the signal input section of the terminal (4n terminal) li+5 to prevent the intrusion of the common mode 1 to noise current Nc flowing through the transmission path. .

また、第10図は、第9図のコモンモードチョークコイ
ルとして従来から広く用いられている円形状トロイダル
コアを用いたものの説明図であり、8は円形状トロイダ
ルコア、9,9′はコア8へ捲回された巻線、10.1
0’および11.11’は、それぞれ巻線9,9′の入
力端子および出力端子である。巻線9,9′のコア8に
対する巻方向は、入力端子10.10’または出力端子
11.11’から同相で流入するコモンモード電流に対
してコア8内に生じる磁束が同方向となって互いに強め
合うように捲回される。第10図の(A)は、コア8に
対して巻線9,9′を対向させて捲回し、(B)では巻
線9,9′をそろえて捲回しである。第10図において
、Cは入出力巻線間に存在する容量である。
Further, FIG. 10 is an explanatory diagram of the common mode choke coil shown in FIG. 9 using a circular toroidal core that has been widely used in the past. Winding wound into 10.1
0' and 11.11' are the input and output terminals of windings 9 and 9', respectively. The winding direction of the windings 9 and 9' with respect to the core 8 is such that the magnetic flux generated in the core 8 is in the same direction as the common mode current flowing in the same phase from the input terminal 10.10' or the output terminal 11.11'. They are wound so that they strengthen each other. In FIG. 10(A), the windings 9 and 9' are wound to face the core 8, and in FIG. 10(B), the windings 9 and 9' are wound together. In FIG. 10, C is the capacitance existing between the input and output windings.

〔発明が解決しようとする問題点〕[Problem that the invention seeks to solve]

このようなコモンモードチョークコイルにおけるコモン
モード雑音電流Ncに対する阻止効果は、インダクタン
スLおよび上記容量Cによってきまり、インダクタンス
Lが大きく容量Cが小さいほど広帯域にわたり良好な阻
止特性を持つ。特に。
The blocking effect against common mode noise current Nc in such a common mode choke coil is determined by the inductance L and the capacitance C, and the larger the inductance L and the smaller the capacitance C, the better the blocking characteristics over a wide band. especially.

高域特性は容量Cによって影響され、容量Cが小さいほ
ど高周波雑音が阻止できる。一方インダクタンスLは、
コアの透磁率をμ、断面積をS9巻数をN、コアの平均
磁路長をdとすると、L=μSN2/dで表わされるこ
とが知られている。従って、コアの材質や形状を一定と
すると、大きなインダクタンスLを得るためには1巻数
Nを大きくする必要があるが、しかし巻数Nを大きくす
ると円形状のコアの内径からきまる円内に巻線が密集し
、多巻線による人出カ端子間容量Cが増加して高域特性
が低下する結果となる。
The high frequency characteristics are influenced by the capacitance C, and the smaller the capacitance C is, the more high frequency noise can be blocked. On the other hand, the inductance L is
It is known that when the magnetic permeability of the core is μ, the cross-sectional area is S9, the number of turns is N, and the average magnetic path length of the core is d, it is expressed as L=μSN2/d. Therefore, assuming that the material and shape of the core are constant, it is necessary to increase the number of turns N in order to obtain a large inductance L. However, when the number of turns N is increased, the windings are wound within a circle determined from the inner diameter of the circular core. are crowded together, the capacitance C between the output terminals due to multiple windings increases, and the high frequency characteristics deteriorate.

すなわち、第11図は、第10図に示すようなコモンモ
ードチョークコイルの電気的等価回路図であり、上記容
量Cが大きいと巻線久方端子から流入したコモンモード
雑音電流Ncが巻線9,9′を通過せず容量Cを通って
反対側にぬけるために。
That is, FIG. 11 is an electrical equivalent circuit diagram of the common mode choke coil as shown in FIG. , 9' to pass through capacitance C to the other side.

インダクタンスLとして作用せず、雑音阻止効果が低減
する。また、特に、第10図の(B)に示す、一定形状
コアに隣線巻線同志が密集したり、多層に重ね巻きする
等によって巻数Nを大きくすると、第11図にCsで示
すような巻線9,9′間の容量が増加し、全体として第
9図に示す伝送路−3= 1.1′の線間に挿入される容量Cが増加する。
It does not act as an inductance L, and the noise blocking effect is reduced. In particular, if the number of turns N is increased by crowding adjacent wire windings around a core of a certain shape as shown in FIG. The capacitance between the windings 9 and 9' increases, and the capacitance C inserted between the lines of the transmission line -3=1.1' shown in FIG. 9 increases as a whole.

このようなコモンモードチョークコイルをディジタル信
号伝送路に用いた場合、パルス伝送への影響が表われる
。すなわち、第12図の(A)は、伝送路1,1′間を
流れるパルス列からなるディジタル信号Sn(ノーマル
モード)の−例であり、(B)はこのような伝送路に上
記のような線間容kk Csの大きいコモンモードチョ
ークコイルを挿入したときの伝送信号の波形例を示す。
When such a common mode choke coil is used in a digital signal transmission line, it has an effect on pulse transmission. That is, (A) in FIG. 12 is an example of a digital signal Sn (normal mode) consisting of a pulse train flowing between transmission lines 1 and 1', and (B) is an example of a digital signal Sn (normal mode) consisting of a pulse train flowing between transmission lines 1 and 1'. An example of the waveform of a transmission signal when a common mode choke coil with a large line capacitance kk Cs is inserted is shown.

すなわち、容量Csの集積による影響が現われ、波形が
歪んだものとなる。この結果、第9図で伝送路1,1′
にコモンモード雑音電流Ncを阻止するために挿入した
コモンモードチョークコイルによって本来の情報伝送に
用いるディジタル信号(パルス伝送信号)Snが変形す
る。この容量Csの影響は、パルス伝送信号Snのパル
ス立上り時間や、パルス幅が小さく高速度伝送となるほ
ど大きく、極端な場合は容量Csの集積によって回線短
絡状態となる等により、通信端末機器の正常動作を妨げ
たり、使用不能となる欠点がある。一方、これをさける
ためにコモンモードチョークコイルの巻数Nを小さくす
るとインダクタンスLを大きくできないために、十分な
雑音電流Ncの阻止がはがれず、外来雑音4によって通
信端末機器が誤動作等の障害をおこすという問題があっ
た。
In other words, the influence of the accumulation of capacitors Cs appears and the waveform becomes distorted. As a result, in Fig. 9, transmission lines 1, 1'
The digital signal (pulse transmission signal) Sn used for original information transmission is deformed by the common mode choke coil inserted to block the common mode noise current Nc. The influence of this capacitance Cs becomes larger as the pulse rise time and pulse width of the pulse transmission signal Sn become smaller and the faster the transmission becomes, and in extreme cases, the accumulation of capacitance Cs may cause a line short-circuit, which may affect the normal operation of communication terminal equipment. There are drawbacks that may hinder operation or make it unusable. On the other hand, if the number of turns N of the common mode choke coil is reduced in order to avoid this, the inductance L cannot be increased, so the noise current Nc cannot be sufficiently blocked, and the external noise 4 may cause trouble such as malfunction of the communication terminal equipment. There was a problem with causing it.

このように、従来用いられているコモンモードチョーク
コイルをパルス伝送路に適用したときパルス信号への影
響のないものは外来雑音に対する阻止特性の広帯域化が
はかれず、雑音阻止特性の良好なものはパルス伝送路へ
適用できないという問題があった。
In this way, when conventionally used common mode choke coils are applied to pulse transmission lines, those that do not affect the pulse signal cannot achieve a broadband blocking characteristic against external noise, and those with good noise blocking characteristics cannot be achieved. The problem was that it could not be applied to pulse transmission lines.

本発明の目的は、伝送路を伝導するコモンモード雑音電
流に対し、広帯域にわたり良好な阻止特性を有し、高速
パルス伝送路への適用が可能なコモンモードチョークコ
イルを提供することにある。
An object of the present invention is to provide a common mode choke coil that has good blocking characteristics over a wide band against common mode noise current conducted through a transmission line and can be applied to a high-speed pulse transmission line.

本発明の前記ならびにその他の目的と新規な特徴は、本
明細書の以下の記述及び添付図面によって説明する。
The above and other objects and novel features of the present invention are explained by the following description of the specification and the accompanying drawings.

〔問題点を解決するための手段〕[Means for solving problems]

本願において開示される発明のうち、代表的なものの概
要を簡単に説明すれば、下記のとおりである。
A brief overview of typical inventions disclosed in this application is as follows.

所定の高周波領域まで一定値以上の実効透磁率を有する
閉磁路コアに同相電流に対して互いに同方向磁束が生じ
るように2つの巻線を捲回したコモンモードチョークコ
イルにおいて、前記閉磁路コアを互いに直交する短軸と
長軸のうち、長軸に対して対称で、かつ該対称磁路間距
離を短軸部で最大に形成し、該短軸磁路部分に密なる集
中巻線を、該集中巻線部分を除く前記対称磁路部分に疎
なる均等巻線を、それぞれ対向して捲回したことを主な
特徴とするものである。
In a common mode choke coil in which two windings are wound so that magnetic fluxes in the same direction are generated in a closed magnetic circuit core having an effective magnetic permeability of a certain value or more up to a predetermined high frequency region, the closed magnetic circuit core is Among the short and long axes that are orthogonal to each other, the short axis and the long axis are symmetrical about the long axis, and the distance between the symmetrical magnetic paths is maximized at the short axis, and the concentrated winding is concentrated in the short axis magnetic path. The main feature is that sparse uniform windings are wound oppositely in the symmetrical magnetic path portion except for the concentrated winding portion.

〔作用〕[Effect]

前記手段によれば、閉磁路コアが互いに直交する長軸と
短軸とを有し、長軸に対して対称でこの対称磁路の対向
距離を短軸部分で最大になるように形成し、この対称磁
路の短軸磁路部分に密なる集中巻線を施し、前記対称磁
路の密なる集中巻線を施した部分以外には疎なる巻線を
施すことにより、多巻数による入出力端子間容量Cの増
加および対向者線間容量の増加が抑制され、かつインダ
クタンスLが増加するので、パルス伝送には何ら悪影響
を与えず、かつコモンモードの伝導雑音を広帯域にわた
って阻止することができる。
According to the above means, the closed magnetic path core has a long axis and a short axis that are orthogonal to each other, and is formed symmetrically with respect to the long axis so that the opposing distance of the symmetrical magnetic path is maximized at the short axis portion, By applying densely concentrated windings to the short-axis magnetic path portion of this symmetrical magnetic path, and sparsely concentrated windings to areas other than the portions of the symmetrical magnetic path where densely concentrated windings have been applied, input/output with a large number of turns is possible. Since increases in capacitance C between terminals and capacitance between opposing lines are suppressed, and inductance L increases, pulse transmission is not adversely affected at all, and common mode conduction noise can be blocked over a wide band. .

したがって、高速度ディジタル伝送路などの立上がりが
速く、パルス幅小で繰り返しの速い伝送路に適用したと
き、伝送信号には影響を与えず、伝送路を伝導する広い
周波数成分を有するコモンモード雑音を阻止することが
できる。
Therefore, when applied to a transmission line such as a high-speed digital transmission line where the rise is fast, the pulse width is small, and the repetition is quick, the common mode noise having a wide frequency component that is transmitted through the transmission line does not affect the transmitted signal. can be prevented.

〔発明の実施例〕[Embodiments of the invention]

以下、本発明の実施例について図面を用いて具体的に説
明する。
Embodiments of the present invention will be specifically described below with reference to the drawings.

なお、実施例を説明するための全図において。In addition, in all the figures for explaining an example.

同一機能を有するものは同一符号を付け、その繰り返し
の説明は省略する。
Components having the same function are given the same reference numerals, and repeated explanations thereof will be omitted.

〔実施例■〕[Example ■]

本発明の実施例■のパルス伝送路用コモンモードチョー
クコイルの概略構成を第1図(説明図)に示す。
FIG. 1 (explanatory diagram) shows a schematic configuration of a common mode choke coil for a pulse transmission line according to Embodiment 2 of the present invention.

第1図において、12は第10図に示す従来の円形状ト
ロイダルコア8と同程度の透磁率μおよび平均磁路長d
、断面積Sを有する閉磁路コアであり、長軸X−Xおよ
び短軸Y−Yを有し、長軸X−Xに対して対称で、短軸
Y−Y部分付近における対向磁路間距離が最大となるよ
う形成されている。また、13.13’は対向磁路間距
離が最大の閉磁路コア12の長さQ。の部分に多層にま
たは集中的に捲回した巻線である。14.14’および
巻線15゜15′は閉磁路コア12の上記のa。以上の
それぞれ長さQ、、 Q、部分に対向して疎に均等に捲
回した巻線であり、入出力端子10−11および入出力
端子10’−11’間に捲回したこれらの巻線の巻方向
は一方の端子から同相で流入するコモンモード電流に対
して閉磁路コア12内に生じる磁束が同方向となって互
いに強め合う方向に捲回しである。Co、 C1゜C2
は巻線13.14.15および巻線13’、 14’、
 15’の両端間に生じるそれぞれの巻線間容量である
にの内5巻線13.13’の両端間容量C6は集中巻線
が施されているため大きな値を持ち、疎なる巻線14゜
15および14’、15’の両端間容量C□、C2は、
それぞれ小さな値を持つ。一方、集中巻11A13,1
3′は。
In FIG. 1, 12 indicates a magnetic permeability μ and an average magnetic path length d, which are comparable to those of the conventional circular toroidal core 8 shown in FIG.
, is a closed magnetic circuit core having a cross-sectional area S, has a long axis XX and a short axis Y-Y, is symmetrical about the long axis XX, and has a gap between opposing magnetic paths near the short axis Y-Y portion. It is formed to maximize the distance. Moreover, 13.13' is the length Q of the closed magnetic circuit core 12 with the maximum distance between opposing magnetic paths. It is a winding that is wound in multiple layers or in a concentrated manner. 14.14' and winding 15.15' are the above a of the closed magnetic circuit core 12. These windings are wound sparsely and evenly opposite the lengths Q and Q above, and these windings are wound between input/output terminals 10-11 and input/output terminals 10'-11'. The winding direction of the wire is such that the magnetic flux generated in the closed magnetic circuit core 12 in response to the common mode current flowing in the same phase from one terminal is in the same direction and strengthens each other. Co, C1゜C2
are windings 13, 14, 15 and windings 13', 14',
The capacitance between the windings 13' and 13' is the capacitance between the windings 15' and 15', and the capacitance C6 between the windings 13' and 13' has a large value because of the concentrated winding. The capacitance C□, C2 between both ends of ゜15 and 14', 15' is
Each has a small value. On the other hand, concentrated winding 11A13,1
3' is.

閉磁路コア12の対向距離が最も大きい短軸Y−Y部分
付近に捲回されているので、自身の巻数が多くても両巻
線間対向ギャップgを一定以上とっておけば、巻線13
.13’間対向容量Csoは小さく構成できる。また巻
線14 、14 ’間および巻線15 、15 ’間対
向容量Cs1.Cs2は、それぞれこれらの巻線がいず
れも疎に捲回しであるため小さい。
Since the closed magnetic circuit core 12 is wound near the short axis Y-Y portion where the facing distance is the largest, even if the number of windings is large, if the facing gap g between both windings is kept above a certain level, the winding 13
.. 13' opposing capacitance Cso can be configured to be small. Also, the opposing capacitance Cs1 between the windings 14 and 14' and between the windings 15 and 15'. Cs2 is small because each of these windings is loosely wound.

第2図は、第1図のコモンモードチョークコイルの電気
的等価回路図であり、インダクタンスLを増加させるた
め、上記のような巻き方で巻線Nを大きくしたとき増加
する容量は、巻線間対向容量C0部分のみであり、容量
c11 C2+ Csa Hcsl、Cs2は、いずれ
もその増加をおさえることができる。したがって、入出
力端子10−11問および入出力端子10 ’−11’
間にそれぞれ直列挿入される容量C6,C,、C2のう
ち容tc。の値が大きくても全体としての入出力端子間
容量Cは大きくならない。また、容量Cs、、 Cs、
、 Cs2の集積からなる対向者線間容量もこれらがい
ずれも小さいため。
Fig. 2 is an electrical equivalent circuit diagram of the common mode choke coil shown in Fig. 1. In order to increase the inductance L, when the winding N is increased using the winding method described above, the increased capacitance is It is possible to suppress the increase in both the capacitances c11 C2+ Csa Hcsl and Cs2. Therefore, input/output terminal 10-11 and input/output terminal 10'-11'
Of the capacitors C6, C, and C2 inserted in series between them, the capacitor tc. Even if the value of is large, the overall capacitance C between the input and output terminals does not become large. Also, the capacitance Cs,, Cs,
, Cs2 are both small.

増加を抑えることができる。increase can be suppressed.

以上の説明かられかるように、第1図のコモンモードチ
ョークコイルを、第9図のコモンモートチョークコイル
7のかわりに適用すれば、ノーマルモードのパルス伝送
信号Snに対しては何ら影響がなくかつ外来雑音4によ
るコモンモード雑音電流Ncに対しては、インダクタン
スLが大きく入出力端子間容量Cが小さいため、広帯域
にわたり雑音電流Ncを阻止することができる。
As can be seen from the above explanation, if the common mode choke coil of FIG. 1 is applied in place of the common mode choke coil 7 of FIG. 9, there will be no effect on the normal mode pulse transmission signal Sn. In addition, with respect to the common mode noise current Nc due to the external noise 4, the inductance L is large and the capacitance C between the input and output terminals is small, so that the noise current Nc can be blocked over a wide band.

〔実施例II ) 本発明の実施例Hのパルス伝送路用コモンモードチョー
クコイルの概略構成を第3図(説明図)に示す。
[Example II] A schematic configuration of a common mode choke coil for a pulse transmission line according to Example H of the present invention is shown in FIG. 3 (explanatory diagram).

第:3図におイテ、16は長軸x−x、短軸Y−Yを有
する楕円形状閉磁路コア、17.17’は対向磁路間距
離が最大となる短軸Y−Y付近の磁路部分に集中的に対
向して捲回した巻線、巻線18.18’および19.1
9’は巻線17.17’の捲回された以外の磁路部分に
疎に対向して捲回した巻線である。本実施例■では、閉
磁路コア16の形状がなめらかになっているため、巻線
を流れる雑音電流によってコア16内に生じる磁束の漏
洩が少なく、第1図のものと比べ同一巻数の場合、イン
ダクタンス1.を大きくできる利点がある。
16 is an elliptical closed magnetic circuit core with a long axis x-x and a short axis Y-Y, and 17.17' is a core near the short axis Y-Y where the distance between opposing magnetic paths is maximum. Windings 18.18' and 19.1 wound intensively opposite to the magnetic path section.
Reference numeral 9' denotes a winding that is wound loosely opposite to the magnetic path portion other than the winding of the winding 17 and 17'. In this embodiment (2), since the shape of the closed magnetic circuit core 16 is smooth, there is less leakage of magnetic flux generated in the core 16 due to noise current flowing through the winding, and compared to the one in FIG. 1, when the number of turns is the same, Inductance1. It has the advantage of being able to increase the size of

〔実施例■〕[Example ■]

本発明の実施例■のパルス伝送路用コモンモードチョー
クコイルの概略構成を第4図(説明図)に示す。第4図
の(A)は、閉磁路ループに沿った断面磁路(斜線部)
に巻線を施した図であり、(B)はコアのみの外観図で
ある。
FIG. 4 (explanatory diagram) shows a schematic configuration of a common mode choke coil for a pulse transmission line according to Example 2 of the present invention. (A) in Figure 4 shows the cross-sectional magnetic path (shaded area) along the closed magnetic path loop.
FIG. 3B is a diagram showing windings applied to the core, and (B) is an external view of only the core.

第4図において、20は閉磁路コア、21.21’l:
1コア20の短軸部分に集中的に対向して捲回した巻線
、22.22’および23.23’はそれぞれコア20
の−1;記巻線21.21’以外のコア部分に対向して
捲回した巻線である。
In Fig. 4, 20 is a closed magnetic circuit core, 21.21'l:
The windings 22, 22' and 23, 23', which are wound intensively opposite to each other on the short axis portion of the core 20, are the core 20.
-1: This is a winding wound opposite to the core portion other than the winding 21 and 21'.

本実施例■のパルス伝送路用コンモードチョークコイル
は、第1図の実施例■をもとにコア外径の縦、横寸法(
hxp)がそれぞれ一定に制約された場合の例であり、
第4図に示すように、短軸部分のコア外径が一定に抑え
られるため、この部=11= 分での巻線を多く捲回できるように、前記コアの厚さを
薄くシ、その分高さく幅)方向に拡大して全体として閉
磁路に垂直なコア断面積を等しくすることにより、第1
図と同等の効果を得ている。
The commode choke coil for pulse transmission line of this embodiment (■) is based on the example (2) of Fig. 1, and the vertical and horizontal dimensions of the core outer diameter (
hxp) are each constrained to be constant,
As shown in Fig. 4, since the outer diameter of the core at the short axis portion is kept constant, the thickness of the core is made thinner so that more windings can be wound in this portion = 11 = min. By expanding the core cross-sectional area perpendicular to the closed magnetic path as a whole by expanding it in the height and width directions, the first
The same effect as shown in the figure is obtained.

このように構成することにより、外径寸法を小形化した
ときにも、巻数Nを多くできるためインダクタンスLが
減少しない効果がある。
With this configuration, even when the outer diameter size is reduced, the number of turns N can be increased, so that the inductance L does not decrease.

第5図乃至第8図は1本発明のコアについて、組立時の
巻線方法を容易にするための実施例の説明図であり、第
5図は、第1図のコア12を長軸にK)って2等分した
コア12A、12Bをコの字形板ばね24を用いて組立
てた構成図である。
5 to 8 are explanatory diagrams of an embodiment of the core of the present invention for facilitating the winding method during assembly, and FIG. 5 shows the core 12 of FIG. K) is a configuration diagram in which cores 12A and 12B, which are divided into two, are assembled using a U-shaped leaf spring 24.

第6図は、第5図の分解斜視図であり、ばね24のコア
12A、12 Bとの押さえ而a、a’、b、b’、は
、ばねの嵌合によってずれないよう平面としである。
FIG. 6 is an exploded perspective view of FIG. 5, and the retainers a, a', b, and b' of the spring 24 and the cores 12A and 12B are made flat so that they do not shift due to the fitting of the springs. be.

第7図は、第3図の楕円形状コアについて同様に長軸に
沿って2等分し、ばね押さえのためにコアの長軸外側部
分に平面a、a’、b、b’を設けたものである。
Figure 7 shows that the elliptical core in Figure 3 is similarly divided into two equal parts along the long axis, and planes a, a', b, and b' are provided on the outside of the core's long axis to hold the spring. It is something.

第8図は、同様にコアの短軸部分を外側にふくらませ、
両側に向って直線状にのびたコア25Δ、25Bを用い
たものである。これらはいずれも閉磁路を2分割した開
磁路状態でコイル巻線を施こした後、板ばねを用いて閉
磁路を組立てることができるため、巻線が容易に行える
Figure 8 shows the short axis of the core bulging outward in the same way.
This uses cores 25Δ and 25B that extend linearly toward both sides. In all of these, the coil winding can be performed in an open magnetic path state in which the closed magnetic path is divided into two, and then the closed magnetic path can be assembled using leaf springs, so that winding can be easily performed.

以上、本発明を実施例にもとづき具体的に説明したが、
本発明は、前記実施例に限定されるものではなく、その
要旨を逸脱しない範囲において種々変更可能であること
は言うまでもない。
The present invention has been specifically explained above based on examples, but
It goes without saying that the present invention is not limited to the embodiments described above, and can be modified in various ways without departing from the spirit thereof.

〔発明の効果〕〔Effect of the invention〕

以上、説明したように、本発明によれば、閉磁路コアが
互いに直交する長軸と短軸とを有し、長軸に対して対称
でこの対称磁路の対向距離を短軸部分で最大になるよう
に形成し、この対称磁路の短軸磁路部分に密なる集中巻
線を施し、前記対称磁路の密なる集中巻線を施した部分
以外には疎なる巻線を施すことにより、多巻数による入
出力端子間容量Cの増加および対向巻線間容址の増加が
抑制され、かつインダクタンスLが増加するので、パル
ス伝送には何ら悪影響を与えず、かつコモンモードの伝
導雑音電流を広帯域にわたって阻止することができる。
As explained above, according to the present invention, the closed magnetic circuit core has a long axis and a short axis that are orthogonal to each other, and is symmetrical about the long axis, and the opposing distance of this symmetrical magnetic path is maximized at the short axis portion. A densely concentrated winding is applied to the short-axis magnetic path portion of this symmetrical magnetic path, and a sparsely concentrated winding is applied to the portion of the symmetrical magnetic path other than the portion where the densely concentrated winding is applied. This suppresses the increase in the capacitance C between the input and output terminals and the increase in the capacitance between the opposing windings due to the large number of turns, and increases the inductance L, so there is no adverse effect on pulse transmission and common mode conduction noise is suppressed. Current can be blocked over a wide band.

したがって、高速度ディジタル伝送路などの立上がりが
速く、パルス幅小で繰り返しの速い伝送路に適用したと
き、伝送信号には影響を与えず、伝送路を伝導する広い
周波数成分を有するコモンモード雑音電流を阻止するこ
とができる。
Therefore, when applied to a transmission line such as a high-speed digital transmission line where the rise is fast, the pulse width is small, and the repetition is quick, common mode noise current with a wide frequency component that does not affect the transmitted signal and is conducted through the transmission line. can be prevented.

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

第1図は、本発明の実施例Iのパルス伝送路用コンモー
ドチョークコイルの概略構成を示す説明図、 第2図は、第1図の電気的等価回路図、第3図は、本発
明の実施例■のパルス伝送路用コンモードチョークコイ
ルの概略構成を示す説明図、 第4図は、本発明の実施例■のパルス伝送路用コンモー
ドチョークコイルの概略構成を示す説明図、 第5図は、第1図のコアを長軸に沿って2等分したコア
をコの字形板ばねを用いて組立てた構成図。 第6図は、第5図の分解斜視図。 第7図は、第3図の楕円形状コアについて同様に長軸に
沿って2等分し、ばね押さえのためにコアの長軸外側部
分に平面a、a’、b、b’を設けた図、 第8図は、同様にコアの短軸部分を外側にふくらませ、
両側に向って直線状にのびたコアを用いた図、 第9図は、平衡伝送路のパルス信号および外来雑音電流
の伝導状況説明図、 第10図は、従来の円形状トロイダルコアを用いたコモ
ンモードチョークコイルの説明図、第11図は、第10
図のコイルの電気的等価回路図、 第12図は、従来のコモンモートチゴークコイルを用い
たときのパルス伝送波形図である。 図中、12.16.20・・閉磁路コア、13.13’
、 17゜17’、 21.21’・・・猪中的に施し
た密なる集中巻線、14、 14’、  15. 15
’、  18. 18’、  19. 19’、  2
2. 22’。 23.23’・・・疎に捲回された巻線、24・・・ば
ね、25A。 25B・・・コアである。
FIG. 1 is an explanatory diagram showing a schematic configuration of a commode choke coil for a pulse transmission line according to Embodiment I of the present invention, FIG. 2 is an electrical equivalent circuit diagram of FIG. 1, and FIG. 3 is an illustration of the present invention. FIG. 4 is an explanatory diagram showing a schematic configuration of a commode choke coil for a pulse transmission line according to Example (■) of the present invention; FIG. FIG. 5 is a configuration diagram in which the core of FIG. 1 is divided into two equal parts along the long axis and assembled using a U-shaped leaf spring. FIG. 6 is an exploded perspective view of FIG. 5. Figure 7 shows that the elliptical core in Figure 3 is similarly divided into two equal parts along the long axis, and planes a, a', b, and b' are provided on the outside of the core's long axis to hold the spring. Figure 8 shows the short axis of the core bulging outward in the same way.
Figure 9 is an explanatory diagram of the conduction situation of pulse signals and external noise current in a balanced transmission line. Figure 10 is a common diagram using a conventional circular toroidal core. An explanatory diagram of the mode choke coil, FIG.
FIG. 12 is a pulse transmission waveform diagram when a conventional common mode coil is used. In the figure, 12.16.20...Closed magnetic circuit core, 13.13'
, 17°17', 21.21'...Dense concentrated winding, 14, 14', 15. 15
', 18. 18', 19. 19', 2
2. 22'. 23.23'... Loosely wound winding, 24... Spring, 25A. 25B...Core.

Claims (1)

【特許請求の範囲】[Claims] (1)所定の高周波領域まで一定値以上の実効透磁率を
有する閉磁路コアに同相電流に対して互いに同方向磁束
が生じるように2つの巻線を捲回したコモンモードチョ
ークコイルにおいて、前記閉磁路コアを互いに直交する
短軸と長軸のうち、長軸に対して対称で、かつ該対称磁
路間距離を短軸部で最大に形成し、該短軸磁路部分に密
なる集中巻線を、該集中巻線部分を除く前記対称磁路部
分に疎なる均等巻線を、それぞれ対向して捲回したこと
を特徴とするパルス伝送路用コモンモードチョークコイ
ル。
(1) In a common mode choke coil in which two windings are wound in a closed magnetic circuit core having an effective magnetic permeability of a certain value or more up to a predetermined high frequency region so that magnetic flux is generated in the same direction for an in-phase current, the closed magnetic Among the short axis and long axis that are perpendicular to each other, the path core is symmetrical with respect to the long axis, and the distance between the symmetrical magnetic paths is maximized at the short axis part, and the concentrated winding is dense in the short axis magnetic path part. 1. A common mode choke coil for a pulse transmission path, characterized in that a wire is wound with equal windings sparse in the symmetrical magnetic path portions excluding the concentrated winding portions, each facing the other.
JP18225486A 1986-08-01 1986-08-01 Common mode choke coil for pulse transmission path Expired - Fee Related JPH0666199B2 (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP18225486A JPH0666199B2 (en) 1986-08-01 1986-08-01 Common mode choke coil for pulse transmission path

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP18225486A JPH0666199B2 (en) 1986-08-01 1986-08-01 Common mode choke coil for pulse transmission path

Publications (2)

Publication Number Publication Date
JPS6338220A true JPS6338220A (en) 1988-02-18
JPH0666199B2 JPH0666199B2 (en) 1994-08-24

Family

ID=16115040

Family Applications (1)

Application Number Title Priority Date Filing Date
JP18225486A Expired - Fee Related JPH0666199B2 (en) 1986-08-01 1986-08-01 Common mode choke coil for pulse transmission path

Country Status (1)

Country Link
JP (1) JPH0666199B2 (en)

Cited By (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US5726611A (en) * 1993-05-26 1998-03-10 Nippon Telegraph And Telephone Corporation EMC filter for a balanced multi-wired telecommunication line with bifilar windings

Families Citing this family (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
GB0503502D0 (en) * 2005-02-19 2005-03-30 Tyco Electronics Ltd Uk An energy storage coil

Cited By (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US5726611A (en) * 1993-05-26 1998-03-10 Nippon Telegraph And Telephone Corporation EMC filter for a balanced multi-wired telecommunication line with bifilar windings

Also Published As

Publication number Publication date
JPH0666199B2 (en) 1994-08-24

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