JPS61263105A - Composite type common mode choke coil - Google Patents

Composite type common mode choke coil

Info

Publication number
JPS61263105A
JPS61263105A JP10325585A JP10325585A JPS61263105A JP S61263105 A JPS61263105 A JP S61263105A JP 10325585 A JP10325585 A JP 10325585A JP 10325585 A JP10325585 A JP 10325585A JP S61263105 A JPS61263105 A JP S61263105A
Authority
JP
Japan
Prior art keywords
core
winding
common mode
windings
closed 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
JP10325585A
Other languages
Japanese (ja)
Other versions
JPH0320057B2 (en
Inventor
Kusuo Takagi
高木 国主男
Yuzaburo Inoue
井上 裕三郎
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.)
Sanritsu Denki KK
Nippon Telegraph and Telephone Corp
Sanritsu Electric
Original Assignee
Sanritsu Denki KK
Nippon Telegraph and Telephone Corp
Sanritsu Electric
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 Sanritsu Denki KK, Nippon Telegraph and Telephone Corp, Sanritsu Electric filed Critical Sanritsu Denki KK
Priority to JP10325585A priority Critical patent/JPS61263105A/en
Publication of JPS61263105A publication Critical patent/JPS61263105A/en
Publication of JPH0320057B2 publication Critical patent/JPH0320057B2/ja
Granted legal-status Critical Current

Links

Classifications

    • HELECTRICITY
    • H01ELECTRIC ELEMENTS
    • H01FMAGNETS; INDUCTANCES; TRANSFORMERS; SELECTION OF MATERIALS FOR THEIR MAGNETIC PROPERTIES
    • H01F17/00Fixed inductances of the signal type 
    • H01F17/04Fixed inductances of the signal type  with magnetic core

Landscapes

  • Engineering & Computer Science (AREA)
  • Power Engineering (AREA)
  • Microelectronics & Electronic Packaging (AREA)
  • Coils Or Transformers For Communication (AREA)

Abstract

PURPOSE:To obtain a noise-preventing element which has excellent preventive characteristics against common mode noise for a wide-band in a high frequency region by providing close windings in an opposite direction in common with part of the closed magnetic circuit of the second core at one end or the both ends of the longitudinal part of the closed magnetic circuit of the first core in an opposite direction. CONSTITUTION:The first core 7 which has the same degree effective permeability mu1 and consists of a rectangular closed magnetic circuit and the second core 8 consisting of a closed magnetic circuit which has greater effective permeability mu2 in a low frequency region than the first core 7 are used. Equal winding 9, 9' wound thinly and uniformly each in an opposite direction along the longitudinal length l0 of the first core 7 and concentrated windings 10, 10' wound closely and concentratedly adhered closely with the adjacent windings along the length l1 of the longitudinal side of the first core 7 in common with part of the closed magnetic circuit of the second core each in an opposite direction are provided. The equal windings 9, 9' and the concentrated windings 10, 10' are each wound so as to generate the same direction magnetic flux in the first and the second cores against a common mode noise current which flows from input terminals 1, 1' or output terminals 2, 2' respectively.

Description

【発明の詳細な説明】 〔技術分野〕 本発明は、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 [Technical Field] The present invention relates to a common mode choke coil that blocks high frequency common mode noise over a wide band.

〔背景技術〕[Background technology]

従来、この種のコモンモードチョークコイルとしては、
第6図に示すような、円形状コアに巻線を施したものが
用いられている。すなわち、第6図において、1,1′
および2,2′は、巻線のそれぞれ入力端子および出力
端子、3は低周波領域から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円形状閉磁路コア54および
4′は入力端子1,1′または出力端子2,2′から同
相で流入する高周波のコモンモード電流に対して。
Conventionally, this type of common mode choke coil is
A circular core wound with wires as shown in FIG. 6 is used. That is, in Fig. 6, 1, 1'
2 and 2' are the input and output terminals of the winding, respectively. 3 is the circular closed magnetic circuit core 54 and 4' is the input terminal 1, which has an effective magnetic permeability above a certain value from a low frequency region to a predetermined high frequency region. , 1' or high frequency common mode current flowing in the same phase from output terminals 2, 2'.

コア3の閉磁路内に互いに同方向磁束が生じるような向
きに滝口された巻線であり5巻線4,4′は、第6図の
ように、コアの閉磁路の対向する位置に、または該閉磁
路に沿って両者をそろえて(図示せず)捲回される。ま
た、第7図は第6図の電気的等価回路図、第8図は第6
図の入力端子間インピーダンス−周波数特性(Z−f特
性)である。
The windings 4 and 4' are windings oriented in such a way that magnetic fluxes in the same direction are generated in the closed magnetic path of the core 3, and the windings 4 and 4' are placed at opposing positions in the closed magnetic path of the core, as shown in FIG. Alternatively, both are aligned and wound along the closed magnetic path (not shown). Also, Fig. 7 is an electrical equivalent circuit diagram of Fig. 6, and Fig. 8 is an electrical equivalent circuit diagram of Fig. 6.
It is the impedance-frequency characteristic (Zf characteristic) between the input terminals shown in the figure.

このような素子のコモンモードノイズ阻止特性は、Z−
f特性によってきまるが、高周波領域を中心にその上限
域、下限域をさらに拡大し、広帯域化をはかるためには
、広い周波数範囲にわたってインピーダンスZが要求さ
れる一定値a以上であることが望ましい。しかし、第6
図のような円形状コアを用いた従来の高周波コモンモー
ドチョークコイルでは、巻線4,4′の隣接巻線間容量
CNをおさえるため巻数を少なくしているが。
The common mode noise rejection characteristic of such an element is Z-
Although it depends on the f characteristic, in order to further expand the upper and lower limit ranges mainly in the high frequency region and achieve a wide band, it is desirable that the impedance Z be equal to or greater than a required constant value a over a wide frequency range. However, the 6th
In a conventional high frequency common mode choke coil using a circular core as shown in the figure, the number of turns is reduced in order to suppress the capacitance CN between adjacent windings 4 and 4'.

それでもなお入出力巻線間距離が小さいことによる入出
力巻線間容量C6が存在し、これによって全体としての
入出力端子間容量Cが大きく高域側特性を悪化させてい
る。一方、低域側における特性は巻線4.4′のインダ
クタンスしによってきまるが、高周波用コア3の実効透
磁率μは一般に小さく、かつ巻数が制限されているため
にインダクタンスLを十分大きくできず、これらの結果
Even so, there is still a capacitance C6 between the input and output windings due to the small distance between the input and output windings, and as a result, the overall capacitance C between the input and output terminals is large and deteriorates the high-frequency characteristics. On the other hand, the characteristics on the low frequency side are determined by the inductance of the winding 4.4', but the effective magnetic permeability μ of the high frequency core 3 is generally small and the number of turns is limited, so the inductance L cannot be made sufficiently large. , these results.

このような素子のZ−f特性は第8図の曲線5のように
なり、要求されるインピーダンスZの一定値aに対して
、インダクタンスし、容量Cからきまる自己共振周波数
f、を中心に帯域Aを有するが、前記理由から、この帯
域Aは大きくすることができない、なお、第6図で巻線
4,4′のそ九ぞれの巻線を増加していくと、容量Cが
増加すると共に、インダクタンスしも増加するためZ−
f特性は、第8図の曲線6のように自己共振周波数f1
が低域側に移動した自己共振周波数f2の曲線となる。
The Z-f characteristic of such an element is as shown in curve 5 in Fig. 8, and for a constant value a of the required impedance Z, the inductance and the band around the self-resonant frequency f determined by the capacitance C. However, for the reason mentioned above, this band A cannot be increased.In addition, as the number of windings 4 and 4' is increased in Fig. 6, the capacitance C increases. At the same time, the inductance also increases, so Z-
The f characteristic has a self-resonant frequency f1 as shown in curve 6 in FIG.
becomes a curve with a self-resonant frequency f2 shifted to the lower frequency side.

したがって、このような素子を用いて高周波領域におけ
る広帯域化をはかる手段として、第6図の構造のもので
透磁率および巻数の異なる第8図の曲線5および6のよ
うな2個のコイルを直列接続する方法が考えら九る。第
9図および第10図は、このような直列接続のZ−f特
性であり、第9図は帯域Bを大きくとろうとして自己共
振周波数fz、fzの比較的離れたものを接続した場合
、第10図は自己共振周波数f+、f2の接近したもの
を接続した場合の特性である。第9図に示すように、帯
域Bを大きくしようとすると、この帯域内に領域Cのよ
うに特性が要求値a以下に落ちこむ個所が存在し、また
、第10図のように自己共振周波数fr、fiを接近さ
せると、上記の落ちこみはなくなるが、要求値a以上と
なる帯域が、帯域B′のように十分大きくとれず、いず
れにしても広帯域化をはかることができない。
Therefore, as a means of widening the band in the high frequency range using such an element, two coils having the structure shown in Fig. 6 and having different magnetic permeability and number of turns as shown in curves 5 and 6 in Fig. 8 are connected in series. I can't think of a way to connect it. Figures 9 and 10 show the Z-f characteristics of such a series connection, and Figure 9 shows the result when the self-resonant frequencies fz and fz are connected relatively far apart in order to increase the band B. FIG. 10 shows the characteristics when devices with close self-resonant frequencies f+ and f2 are connected. As shown in FIG. 9, when trying to increase band B, there are areas within this band, such as region C, where the characteristics drop below the required value a, and as shown in FIG. 10, the self-resonant frequency fr , fi are made close to each other, the above-mentioned drop disappears, but the band where the value is equal to or greater than the required value a cannot be made sufficiently large like the band B', and in any case, it is impossible to achieve a wide band.

次に、第6図の素子を用いて、高周波領域における広帯
域化をはかる別の手段として第11図のような構造のも
のが考えられる。すなわち、第11図は前記のコア2個
をあわせて巻線4,4′を共通巻きとしたものである。
Next, a structure as shown in FIG. 11 can be considered as another means for widening the band in the high frequency region using the element shown in FIG. 6. That is, in FIG. 11, the windings 4 and 4' of the two cores are wound in common.

第12図および第13図はこのような構造のもののZ−
f特性であり、第12図は巻線4,4′の共通巻数を多
くした場合、第13図は共通巻数を少なくした場合であ
る。
Figures 12 and 13 show the Z-
Fig. 12 shows the f characteristic when the number of common turns of the windings 4 and 4' is increased, and Fig. 13 shows the case when the number of common turns of the windings 4 and 4' is decreased.

すなわち、第11図の構造では、共通巻きにしたことに
より、前記第9図の領域Cのような特性の落ちこみ部分
はなくなるが、一定値3以上の、インピーダンスZとな
る帯域は、巻数の多い第12図では、低域側りのみとな
り、巻数の少ない第13図では、高域側D′のみのよう
になり、直列接続の場合と同様に広帯域化をはかること
ができない。
In other words, in the structure shown in FIG. 11, by using a common winding, there is no drop in the characteristics like the area C in FIG. In FIG. 12, only the low frequency side is shown, and in FIG. 13, where the number of turns is small, only the high frequency side D' is shown, and it is not possible to achieve a wide band as in the case of series connection.

このように、従来の円形状コアを用いたコモンモードチ
ョークコイルでは、高周波領域における入出力巻線間容
量が、また低周波領域における。インダクタンス不足が
それぞれインピーダンス特性を悪化させ、透磁率の異な
るコアやそれぞれの巻数を変えたものを組合せても、広
帯域にわたり良好なノイズ阻止特性を確保することがで
きないという問題点があった。
As described above, in the conventional common mode choke coil using a circular core, the capacitance between the input and output windings is large in the high frequency region, and the capacitance between the input and output windings is large in the low frequency region. Insufficient inductance deteriorates impedance characteristics, and even if cores with different magnetic permeabilities and the number of turns of each core are combined, good noise blocking characteristics cannot be ensured over a wide band.

〔発明の目的〕[Purpose of the invention]

本発明の目的は、このような従来の問題点を解消し、高
周波領域において広帯域わたりコモンモードノイズ阻止
特性のすぐれた雑音防護素子を提供することにある。
An object of the present invention is to eliminate such conventional problems and provide a noise protection element with excellent common mode noise blocking characteristics over a wide band in the high frequency region.

本発明の前記ならびにその他の目的と新規な特徴は、本
明細書の記述及び添付図面によって明らかになるであろ
う。
The above and other objects and novel features of the present invention will become apparent from the description of this specification and the accompanying drawings.

〔発明の概要〕[Summary of the invention]

本願で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.

すなわち、従来の高周波用円形状コアにかわり、これと
同程度の実効透磁率を有し、互いに直交する短軸と長軸
を有し、長軸に対して対称な閉磁路からなる第1のコア
およびこれより低周波領域で実効透磁率の大きい閉磁路
からなる第2のコアを用い、第1のコア閉磁路の対向す
る長辺状部分の中央磁路部分には疎なる巻線を、前記対
向する第1のコア閉磁路の長辺状部分の片端または、両
端部分には、第2のコア閉磁路の一部と共通に、密なる
巻線をそれぞれ対向して施したことを最も主要な特徴と
するものである。
In other words, in place of the conventional circular core for high frequency, the first core has the same effective magnetic permeability, has a short axis and a long axis that are perpendicular to each other, and is composed of a closed magnetic path that is symmetrical about the long axis. A core and a second core consisting of a closed magnetic path with a large effective magnetic permeability in a lower frequency region are used, and sparse windings are provided in the central magnetic path portion of the opposing long side portions of the first core closed magnetic path. Most preferably, dense windings are provided at one end or both end portions of the long side portions of the opposing first core closed magnetic path in common with a portion of the second core closed magnetic path. This is the main feature.

これによって、従来の技術で、問題となっていた高周波
領域における入出力端子間容量を低減してインピーダン
ス特性を高域側に拡大すると共に、低周波領域における
インダクタンス不足をなくすることによってインピーダ
ンス特性を低域側にも拡大し、全体としてインピーダン
ス特性、すなわちコモンモードノイズの阻止特性の広帯
域化をはかったものである。
This reduces the capacitance between the input and output terminals in the high frequency range, which was a problem with conventional technology, and expands the impedance characteristics to the high frequency side.It also improves the impedance characteristics by eliminating the lack of inductance in the low frequency range. This extends to the low frequency side, and the overall impedance characteristic, that is, the common mode noise blocking characteristic, is aimed at widening the band.

以下、本発明の構成について、実施例とともに説明する
Hereinafter, the configuration of the present invention will be explained along with examples.

なお、実施例を説明するための企図において。Incidentally, for the purpose of explaining the embodiments.

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! ]

第1図は1本発明の実施例Iの複合形コモンモードチョ
ークコイルの構成を示す図、第2図は第1図の電気的等
価回路図である。
FIG. 1 is a diagram showing the configuration of a composite common mode choke coil according to Embodiment I of the present invention, and FIG. 2 is an electrical equivalent circuit diagram of FIG. 1.

第1図において、7は従来の高周波コモンモードチョー
クコイル用円形状コアと同程度の実効透磁率μ」を有し
、長方形状閉磁路からなる第1のコア、8は第1のコア
7より低周波領域において大きな実効透磁率μ2を有す
る閉磁路からなる第2のコア、9および9′は第1のコ
アの長辺の長さQo部分にそれぞれ対向して均等に単相
巻きで隣接間距離をあけるなどの疎で一様に捲回した均
等巻線、lOおよび10’は第1のコアの長辺の長さ2
8部分に第2のコアの閉磁路の一部と共通にそ践ぞれ対
向して隣接巻線を密着させた単相巻きまたは多層巻きな
どの密で集中的に捲回した集中巻線であり、均等巻線9
,9′および集中巻線10.10’は、それぞれ入力端
子1,1′または出力端子2,2′から流入するコモン
モードノイズ電流に対して、第1および第2のコア内で
互いに同方向磁束が生じるように櫓回しである。
In FIG. 1, 7 is a first core consisting of a rectangular closed magnetic path and has an effective magnetic permeability μ'' comparable to that of a circular core for a conventional high-frequency common mode choke coil, and 8 is a first core 7. The second cores, 9 and 9', each consisting of a closed magnetic circuit having a large effective magnetic permeability μ2 in the low frequency region, are wound evenly in a single phase, facing the length Qo portion of the long side of the first core. Evenly spaced and evenly wound windings, lO and 10' are the lengths of the long sides of the first core, 2
Concentrated winding, such as single-phase winding or multi-layer winding, in which adjacent windings are closely wound in common with a part of the closed magnetic circuit of the second core in 8 parts. Yes, equal winding 9
, 9' and the concentrated windings 10 and 10' are arranged in the same direction within the first and second cores with respect to the common mode noise current flowing from the input terminals 1, 1' or the output terminals 2, 2', respectively. The tower is rotated to generate magnetic flux.

ここで、容量C8および(、+はそれぞれ均等巻線9,
9および集中巻線10.10’の両端間浮遊容量である
Here, capacitances C8 and (, + are equal windings 9,
9 and the stray capacitance between both ends of the lumped winding 10 and 10'.

このような構成では、Qottntにくらべ十分大きく
設定しておけば容量C8を容量C8とくらべ小さくする
ことができるため、これらの直列接続からなる入力端子
1と出力端子2間または久方端子1′出力端子2′間容
量はほとんど容量C6できまるため、たとえ集中巻線1
0.10’ による容量C1の増加があっても高周波領
域におけるインピーダンス特性の悪化がなく、高域側へ
特性を拡大できる。また、低周波領域においては、長方
形状コアのため漏洩磁束は増加するが、それ以上に集中
巻線10.10’による第1のコア7および第2のコア
8、特に後者によるインダクタンスを大きくできるため
インピーダンス特性の低域側への拡大も可能である。
In such a configuration, capacitance C8 can be made smaller than capacitance C8 by setting it sufficiently larger than Qottnt. Since the capacitance between output terminal 2' is almost determined by capacitance C6, even if concentrated winding 1
Even if the capacitance C1 increases by 0.10', the impedance characteristics in the high frequency region do not deteriorate, and the characteristics can be expanded toward the high frequency region. In addition, in the low frequency region, leakage magnetic flux increases due to the rectangular core, but the inductance due to the first core 7 and second core 8, especially the latter, can be further increased due to the concentrated winding 10.10'. Therefore, it is also possible to expand the impedance characteristics to the lower frequency side.

また、第1図の構成では、第1のコア7をペースにして
共通巻線と単独巻線とが共存しているため、前記第9図
の領域Cにみられるような特性の落ちこみはなくなり、
第1のコア7の平均磁路長が第6図の円形状コア3と同
程度の場合でも従来にくらベインピーダンス特性が高域
側および低域側へ拡大される。
Furthermore, in the configuration shown in FIG. 1, since the common winding and the individual winding coexist with the first core 7 as the pace, the drop in characteristics as seen in the region C of FIG. 9 is eliminated. ,
Even when the average magnetic path length of the first core 7 is comparable to that of the circular core 3 of FIG. 6, the vane impedance characteristic is expanded to the high frequency side and the low frequency side compared to the conventional case.

〔実施例■〕[Example ■]

本実施例■は、第3図に示すように、第1図に示す第2
のコア8と実効透磁率μ3が同じもしくは異なる第3の
コア8′を第1のコア7のもう一方の側に設けたもので
あり、必要に応じて、第1゜第2.第3のコアの実効透
磁率をそれぞれμ宜。
As shown in FIG. 3, this embodiment
A third core 8' having the same or different effective permeability μ3 as the core 8 is provided on the other side of the first core 7, and if necessary, the first core 8', the second core 8', and the third core 8' have the same or different effective magnetic permeability μ3. The effective magnetic permeability of the third core is μ.

μ2.μ3とコア寸法および各巻線数を変えることによ
って任意の広帯域特性とすることができる。
μ2. By changing μ3, the core size, and the number of windings, arbitrary broadband characteristics can be obtained.

なお、第1乃至第3のコアをすべて同じ材質で構成して
実効透磁率μ厳=μ2=μ3とした場合でも、従来のも
のにくらべ広帯域化できることは明らかである。
It is clear that even if the first to third cores are all made of the same material and the effective magnetic permeability μ = μ2 = μ3, it is possible to achieve a wider band than the conventional one.

〔実施例■〕[Example ■]

本実施例■は、第4図に示すように、第1のコア7の両
端側をそれぞれ反対側に90°曲げ、これらの面外側に
第2のコア8および第3のコア8′を対向させて巻線1
0.10’で共通巻きしたものであり、コア8,8′お
よびこれらに施した共通前線間容量の影響が小さくなる
ようにしたものである。
In this embodiment (2), as shown in FIG. 4, both ends of the first core 7 are bent 90 degrees to opposite sides, and a second core 8 and a third core 8' are placed facing each other on the outside of these surfaces. Winding 1
The cores 8 and 8' are wound in common with a diameter of 0.10', and the influence of the capacitance between the cores 8 and 8' and the common front line applied thereto is reduced.

〔実施例■〕[Example ■]

本実施例■は、第5図に示すように、第3図の集中巻線
10.10’ を第1のコアの短辺側に設けたものであ
る。このようにすることによって疎なる巻線部分の長さ
QOが大きくなるため、それだけ容量C8が減少する。
In this embodiment (2), as shown in FIG. 5, the concentrated windings 10 and 10' of FIG. 3 are provided on the short side of the first core. By doing so, the length QO of the sparse winding portion increases, and the capacitance C8 decreases accordingly.

したがって、第4図および第5図の実施例■及び実施例
■ともさらに高域側に特性を拡大できる利点がある。
Therefore, both embodiments (1) and (2) in FIGS. 4 and 5 have the advantage that the characteristics can be further expanded to the higher frequency side.

以上、本発明を実施例にもとすき具体的に説明したが1
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、種々変更し得ることは勿
論である。
The present invention has been specifically explained above using examples.
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.

例えば、第1図乃至第4図に示す実施例では。For example, in the embodiment shown in FIGS. 1-4.

第1のコア7を長方形状のもので説明したが、入出万巻
線間容量Cが円形コアにくらべて小さくなる長方形や楕
円など偏平状のものとしても、同様の効果が得られるこ
とはいうまでもない。
Although the first core 7 has been described as having a rectangular shape, the same effect can be obtained even if the first core 7 is a flat shape such as a rectangle or an ellipse, where the capacitance C between the input and output windings is smaller than that of a circular core. Not even.

また、前記実施例では、巻線9,9′を一様に疎に捲回
した巻線、巻線10.10’ を密に捲回した巻線とし
て説明したが、前記巻線9,9′の両端間距離Q。を従
来の円形状コアの入出万巻線間最短距離より大きくとっ
ておきさえすれば、巻線9,9′および10.10’と
も従来の高周波円形コアに施される巻線と同様の均等(
はぼ均等も含む)な単相巻きなどとするだけでも高域側
では容量C8の減少がはかれ、低域側ではコア8による
インダクタンスLの増加がはかれるため、従来のものに
くらべて広帯域化がはかれることは明らかである。
Furthermore, in the above embodiment, the windings 9 and 9' are uniformly wound sparsely, and the windings 10 and 10' are densely wound. The distance Q between both ends of '. As long as the distance is set larger than the shortest distance between the input and output windings of the conventional circular core, the windings 9, 9' and 10,10' can be equally distributed (similar to the windings applied to the conventional high frequency circular core).
Even by using a single-phase winding (including approximately uniform winding), the capacitance C8 can be reduced on the high frequency side, and the inductance L due to the core 8 can be increased on the low frequency side, resulting in a wider band than the conventional one. It is clear that this will be measured.

〔効果〕〔effect〕

以上説明したように、本発明によれば、従来の高周波コ
モンモードチョークコイル用円形状コアのかわりに、互
いに直交する短軸と長軸を有し。
As explained above, according to the present invention, instead of the conventional circular core for a high frequency common mode choke coil, the coil has a short axis and a long axis that are orthogonal to each other.

長軸に対して対称な閉磁路からなる第1のコアと、低周
波領域で実効透磁率の大きい閉磁路からなる第2のコア
とを用い、第1のコアの長辺状磁路の大部分に疎なる巻
線を施すことによって、入出力端子間容量をおさえてイ
ンピーダンス特性を高域側に拡大し、低周波領域では第
1のコアと第2のコアの1部とを共通にして集中巻線を
施すことにより、インピーダンスを大幅に増加させ、低
域側にもインピーダンス特性を拡大することができる。
By using a first core consisting of a closed magnetic path symmetrical about the long axis and a second core consisting of a closed magnetic path with high effective magnetic permeability in the low frequency region, the length of the long side magnetic path of the first core is By applying sparse winding to the parts, the capacitance between the input and output terminals is suppressed and the impedance characteristics are expanded to the high frequency side, and in the low frequency range, part of the first core and the second core are used in common. By applying concentrated windings, the impedance can be significantly increased and the impedance characteristics can be expanded to the low frequency side as well.

これらによって第1のコアが、従来の円形コアと同程度
の実施透磁率及び平均磁路長をもつ場合でも、インピー
ダンス特性、すなわちコモンモードノイズ阻止特性を広
帯域に拡大することができる。
As a result, even if the first core has an effective magnetic permeability and an average magnetic path length comparable to those of a conventional circular core, the impedance characteristic, that is, the common mode noise blocking characteristic can be expanded over a wide band.

例えば、高周波機器から高用電力線へ誘導し機器へ侵入
する高周波ノイズ(高周波ウエルダなどからのノイズ、
周波数40MHz程度)、およびスイッチング電源を有
する機器からAC線へ送出される低周波の放射ノイズ(
50〜200KHz程度)に対して、本発明による広帯
域コモンモートチゴークコイル1個を用いて電源ライン
ブイルタを構成し。
For example, high-frequency noise (noise from high-frequency welders,
frequency of approximately 40 MHz), and low-frequency radiated noise (approximately 40 MHz) transmitted from devices with switching power supplies to AC lines.
(approximately 50 to 200 KHz), a power line converter is configured using one broadband common mode coil according to the present invention.

これを適用すれば、このような広帯域(0,05〜40
MHz)にわたるノイズの阻止を容易に実現することが
できる。
If this is applied, such a wide band (0.05 to 40
MHz) can be easily achieved.

【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の複合形コモンモートチミ
ークコイルの構成を示す斜視図、第2図は第1図の電気
的等価回路図。 第3図、第4図および第5図は、本発明の実施例■、■
および■の複合形コモンモードチョークコイルの構成を
示す斜視図。 第6図乃至第8図は、従来の円形状コアを用いた高周波
用コモンモードチョークコイルの説明図であり、第6図
は、その構成図、第7図は、第6図の電気的等価回路図
、第8図は、Z−f特性図、第9図および第10図は、
第6図のコイルの高周波用と低周波用との直列接続時の
インピーダンス特性図、 第11図は、第6図のコアを重ねて共通巻線を施こした
従来の複合形コモンモードチョークコイルの構成図、 第12図および第13図は、第11図のインピーダンス
特性図である。 図中、7・・・第1のコア、8・・・第2のコア、8′
・・・第3のコア、9,9′・・・疎に捲回した均等巻
線、to、io’・・・密に捲回した集中巻線である。
FIG. 1 is a perspective view showing the configuration of a composite common moat chimique coil according to Embodiment I of the present invention, and FIG. 2 is an electrical equivalent circuit diagram of FIG. 1. FIGS. 3, 4 and 5 show embodiments of the present invention.
FIG. 3 is a perspective view showing the configuration of the composite common mode choke coil shown in FIG. 6 to 8 are explanatory diagrams of a conventional high frequency common mode choke coil using a circular core, FIG. 6 is a configuration diagram thereof, and FIG. 7 is an electrical equivalent of FIG. 6. The circuit diagram, FIG. 8 is a Z-f characteristic diagram, and FIGS. 9 and 10 are
Figure 6 is an impedance characteristic diagram when high-frequency and low-frequency coils are connected in series. Figure 11 is a conventional composite common mode choke coil in which the cores in Figure 6 are overlapped and a common winding is applied. 12 and 13 are impedance characteristic diagrams of FIG. 11. In the figure, 7...first core, 8...second core, 8'
. . . Third core, 9, 9' . . . sparsely wound uniform winding; to, io' . . . densely wound concentrated winding.

Claims (2)

【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
有し、互いに直交する短軸と長軸を有し、長軸に対して
対称な閉磁路からなる第1のコアと、低周波領域におい
て、前記第1のコアと同等以上の実効透磁率を有する閉
磁路からなる第2および第3のコアのうち少なくとも一
つのコアと、前記第1のコアの対向する長辺状磁路の中
央部の一定長さ部分にそれぞれに対向して設けられた第
1の均等巻線組と、前記第1のコアの対向する長辺状磁
路の端部または短辺状磁路のうち少なくとも一方の側に
、該磁路と、前記第2または第3のコアのうち少なくと
も一方のコアの磁路の一部とを共通にそれぞれ対向して
捲回した第2の巻線組または第2、第3の巻線組とから
なり、前記第1および第2の巻線組または第1ないし第
3の巻線組の巻き方向を巻線入力端子または出力端子か
ら流入するコモンモードノイズ電流に対してコア内磁束
が互いに同一方向に生じるような向きに捲回したことを
特徴とする複合形コモンモードチョークコイル。
(1) A first core that has an effective magnetic permeability of a certain value or more up to a predetermined high frequency region, has a short axis and a long axis that are orthogonal to each other, and is composed of a closed magnetic path that is symmetrical with respect to the long axis, and a low frequency In the region, at least one core of the second and third cores each consisting of a closed magnetic path having an effective magnetic permeability equal to or higher than that of the first core, and a long-side magnetic path facing the first core. At least one of first equal winding sets provided opposite each other in a certain length portion of the central portion, and the opposite ends of the long side magnetic path or the short side magnetic path of the first core. On one side, a second winding set or a second , a third winding set, and the winding direction of the first and second winding sets or the first to third winding sets is determined by the common mode noise current flowing from the winding input terminal or the output terminal. A composite common mode choke coil is characterized in that it is wound in such a direction that the magnetic flux within the core is generated in the same direction.
(2)第1の巻線組の各巻線を疎に、第2の巻線組また
は第2と第3の巻線組の各巻線を密に、それぞれ捲回し
たことを特徴とする特許請求の範囲第1項記載の複合形
コモンモードチョークコイル。
(2) A patent claim characterized in that each winding of the first winding set is wound sparsely, and each winding of the second winding set or the second and third winding sets is wound densely. The composite common mode choke coil according to item 1.
JP10325585A 1985-05-15 1985-05-15 Composite type common mode choke coil Granted JPS61263105A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP10325585A JPS61263105A (en) 1985-05-15 1985-05-15 Composite type common mode choke coil

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP10325585A JPS61263105A (en) 1985-05-15 1985-05-15 Composite type common mode choke coil

Publications (2)

Publication Number Publication Date
JPS61263105A true JPS61263105A (en) 1986-11-21
JPH0320057B2 JPH0320057B2 (en) 1991-03-18

Family

ID=14349334

Family Applications (1)

Application Number Title Priority Date Filing Date
JP10325585A Granted JPS61263105A (en) 1985-05-15 1985-05-15 Composite type common mode choke coil

Country Status (1)

Country Link
JP (1) JPS61263105A (en)

Cited By (6)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPH03272611A (en) * 1990-03-23 1991-12-04 Iseki & Co Ltd Chuter of tractor mower
JPH0432513U (en) * 1990-07-13 1992-03-17
JPH0626232U (en) * 1992-09-04 1994-04-08 東光株式会社 choke coil
EP0626767A2 (en) * 1993-05-26 1994-11-30 Nippon Telegraph And Telephone Corporation EMC filter for a balanced multi-wired telecommunication line
WO2008072352A1 (en) * 2006-12-15 2008-06-19 Nippon Telegraph And Telephone Corporation Common mode choke coil
JP2016219754A (en) * 2015-05-26 2016-12-22 株式会社村田製作所 Coil component

Cited By (8)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPH03272611A (en) * 1990-03-23 1991-12-04 Iseki & Co Ltd Chuter of tractor mower
JPH0432513U (en) * 1990-07-13 1992-03-17
JPH0626232U (en) * 1992-09-04 1994-04-08 東光株式会社 choke coil
EP0626767A2 (en) * 1993-05-26 1994-11-30 Nippon Telegraph And Telephone Corporation EMC filter for a balanced multi-wired telecommunication line
EP0626767A3 (en) * 1993-05-26 1997-09-17 Nippon Telegraph & Telephone EMC filter for a balanced multi-wired telecommunication line.
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
WO2008072352A1 (en) * 2006-12-15 2008-06-19 Nippon Telegraph And Telephone Corporation Common mode choke coil
JP2016219754A (en) * 2015-05-26 2016-12-22 株式会社村田製作所 Coil component

Also Published As

Publication number Publication date
JPH0320057B2 (en) 1991-03-18

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