JPS60260119A - Noise interruption composite transformer - Google Patents

Noise interruption composite transformer

Info

Publication number
JPS60260119A
JPS60260119A JP59115507A JP11550784A JPS60260119A JP S60260119 A JPS60260119 A JP S60260119A JP 59115507 A JP59115507 A JP 59115507A JP 11550784 A JP11550784 A JP 11550784A JP S60260119 A JPS60260119 A JP S60260119A
Authority
JP
Japan
Prior art keywords
core
noise
magnetic
windings
high frequency
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.)
Pending
Application number
JP59115507A
Other languages
Japanese (ja)
Inventor
Katsuaki Kubota
久保田 勝昭
Kusuo Takagi
高木 国主男
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 JP59115507A priority Critical patent/JPS60260119A/en
Publication of JPS60260119A publication Critical patent/JPS60260119A/en
Pending legal-status Critical Current

Links

Classifications

    • HELECTRICITY
    • H01ELECTRIC ELEMENTS
    • H01FMAGNETS; INDUCTANCES; TRANSFORMERS; SELECTION OF MATERIALS FOR THEIR MAGNETIC PROPERTIES
    • H01F30/00Fixed transformers not covered by group H01F19/00
    • H01F30/06Fixed transformers not covered by group H01F19/00 characterised by the structure
    • H01F30/10Single-phase transformers

Abstract

PURPOSE:To interrupt noise in both high frequency normal and common modes for a wider frequency band and also interrupt the noise which enters from any of the input end or output end and passes to the other end in both directions by additionally utilizing the core which shows less reduction of effective permeability at a high frequency or magnetic material such as magnetic sheet. CONSTITUTION:Two kinds of cores (7, 7' and 8, 8') consisting of a magnetic material which shows less deterioration of effective permeability at a high frequency are combined a closed magnetic path core (first core 5) passing through the primary and secondary windings (3, 3') having large effective permeability at a low frequency in accordance with the object input noise frequency. This transformer sufficiently interrupts the noise which enters from any side of input and output devices. Moreover, since the magnetic paths of windings for interrupting common mode noise and interrupting high frequency normal mode noise are separated (like 8 and 7, 8' and 7'), magnetic interference between windings can be prevented and moreover influence of radiated electromagnetic field generated from the winding can be prevented by covering the external circumference of opposed surface of each core with the electrostatic shield plate.

Description

【発明の詳細な説明】 〔発明の属する技術分野〕 本発明は、入力端または出力端のいずれか一方から侵入
し他方へ通過する高周波のノーマルモードノイズおよび
コモンモードノイズの両者を阻止することのできる雑音
阻止複合トランスに関するものである。
[Detailed Description of the Invention] [Technical field to which the invention pertains] The present invention is directed to a method for blocking both high-frequency normal mode noise and common mode noise that enter from either an input end or an output end and pass to the other end. The present invention relates to a noise rejection composite transformer that can be used.

〔従来技術とその問題点〕[Prior art and its problems]

従来、この種の雑音阻止トランスとしては、第8図に示
すよ5な構成のものが用いられている。
Conventionally, as this type of noise blocking transformer, one having five configurations as shown in FIG. 8 has been used.

すなわち第8図(a)に示すように入力端1,1′側か
ら同相で入力する同相電流によるコモンモードノイズN
。に対しては1次巻線3と2次巻線3′との間に静電シ
ールド板4を挿入し、これを接地して巻線間容量Coを
減少させることによりコモンモードノイズNcの2次側
への通過をおさえたり、(b)に示すように1次巻線3
と2次巻線3′とを捲回したコア5に、1次巻線3と直
列にコモンモードノイズN0に対して互いに同方向磁束
が生じるような巻線6および6′を設け、これによって
コモンモードノイズN。に対し大き女インダクタンスが
作用するようにしてコモンモードノイズの阻止をはかつ
ていた。
In other words, as shown in Figure 8(a), common mode noise N due to common mode currents input in the same phase from the input terminals 1 and 1'
. For this purpose, by inserting an electrostatic shield plate 4 between the primary winding 3 and the secondary winding 3' and grounding it to reduce the inter-winding capacitance Co, the common mode noise Nc can be reduced by 2. To suppress the passage to the next side, or as shown in (b),
and a secondary winding 3' are wound around the core 5, and windings 6 and 6' are provided in series with the primary winding 3 so as to generate magnetic flux in the same direction with respect to the common mode noise N0. Common mode noise N. In the past, common mode noise was blocked by having a large inductance act against it.

また入力端1,1′側から逆位相で入力するノーマルモ
ードノイズN、に対しては、第8図(C)に示すように
巻線3の画線間にキャパシタンスC1を挿入してノーマ
ルモードノイズの阻止をはかつていた。
In addition, to deal with the normal mode noise N input from the input terminals 1 and 1' in opposite phase, a capacitance C1 is inserted between the lines of the winding 3 as shown in Fig. 8(C). There was a noise blocker.

しかしくa)では静電シールド板4の接地状態が悪いと
ノイズ阻止特性が低下したり、(b)では本来1次巻線
3に流れる低周旋信号電流による磁束を効率よく2次巻
線3′に鎖交させるよう設計されたコア5にコモンモー
ドノイズ阻止用巻線6゜6′が捲回されているため、高
周波のコモンモードノイズ入力時にこれらによるインダ
クタンスが大きくならず、十分なノイズ阻止特性が得ら
れないなどの欠点があった。
However, in a), if the grounding condition of the electrostatic shield plate 4 is poor, the noise blocking characteristics deteriorate, and in (b), the magnetic flux due to the low circular signal current that originally flows in the primary winding 3 is efficiently transferred to the secondary winding 3. Since the common mode noise blocking winding 6°6' is wound around the core 5, which is designed to be interlinked with the common mode noise, the inductance due to these does not increase when high frequency common mode noise is input, and sufficient noise blocking is achieved. There were drawbacks such as the inability to obtain certain characteristics.

また(C)では高周波のノーマルモードノイズNnを阻
止するには大容量のキャパシタンスC1が必要となるな
ど巻線やコア以外の部品を必要とするという欠点があっ
た。
In addition, (C) has the disadvantage that components other than the windings and core are required, such as the need for a large capacitance C1 to block the high frequency normal mode noise Nn.

〔発明の目的〕[Purpose of the invention]

本発明は、上述のような従来技術の欠点を除去するため
になされたものであり、従って本発明の目的状、巻線や
コア以外の部品を必要とせず、しかも常に安定して十分
なノイズ阻止特性が得られるようにした雑音阻止複合ト
ランスを提供することにある。
The present invention has been made in order to eliminate the drawbacks of the prior art as described above, and the object of the present invention is to eliminate the need for components other than windings and cores, and to always provide stable and sufficient noise. It is an object of the present invention to provide a noise rejection composite transformer capable of obtaining rejection characteristics.

〔発明の要点〕[Key points of the invention]

本発明の要点は、トランスにおいて、高周波における実
効透磁率の低下が少ないコアまたは磁性シートなどの磁
性材を追加的に用いて、高周波のノーマル、コモン両モ
ードノイズを広帯域にわたつて阻止し7、しかも入力端
または出力端のいずれか一方から侵入し他端へ通過する
ノイズを双方向とも阻止できるようにした点にある。
The main point of the present invention is to block high-frequency normal and common mode noise over a wide band by additionally using a magnetic material such as a core or magnetic sheet that has a small decrease in effective magnetic permeability at high frequencies in the transformer7. Moreover, noise that enters from either the input end or the output end and passes to the other end can be blocked in both directions.

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

次に図を参照して本発明の詳細な説明する。 The present invention will now be described in detail with reference to the drawings.

第1図は、本発明の一実施例を示す断面図である。同図
において、7,8及び7’、8’杜、高周波領域まで実
効透磁率の低下が少ない磁性圧粉鉄心などで形成した板
状またはこれを塗着した磁性テープ々どの磁性材からな
るコアである。
FIG. 1 is a sectional view showing one embodiment of the present invention. In the figure, 7, 8, 7', 8' cores are made of magnetic materials such as plate-shaped magnetic powder cores, etc., which have a small drop in effective permeability up to high frequency ranges, or magnetic tape coated with the same. It is.

1次巻iF!i13は、低周波で高い実効透磁率を有す
る第1のコア5の脚部と第2のコア7の一部分(中央脚
部)を一体にしてこの周囲に巻きつけたものである。2
次巻線3′も同様に、第1のコア5の他方の脚部と第3
のコア7′の一部分(中央脚部)を一体にしてこのまわ
りに巻きつけたものである。また巻線(8−a )、 
(8−b )は、第4のコア8の環状閉磁路に、入力端
からの高周波のコモンモード電流に対して互いに同方向
磁束が生ずるよう捲回した巻線である。巻線(8’−a
)、(8’−b)も全く同様に第5のコア8′に捲回さ
れたものである。9は、各巻線間を静電的にじゃへいす
るための静電シールド板である。
Volume 1 iF! i13 is formed by integrating the leg portion of the first core 5 and a portion (center leg portion) of the second core 7, which have a high effective magnetic permeability at low frequencies, and wrapping the leg portion around the leg portion. 2
Similarly, the next winding 3' is connected to the other leg of the first core 5 and the third
A part of the core 7' (center leg part) of the core 7' is integrated and wrapped around it. Also, the winding (8-a),
(8-b) is a winding wound around the annular closed magnetic path of the fourth core 8 so that magnetic fluxes are generated in the same direction with respect to the high-frequency common mode current from the input end. Winding wire (8'-a
) and (8'-b) are also wound around the fifth core 8' in exactly the same way. 9 is an electrostatic shield plate for electrostatically shielding between each winding.

第2図は、第1図に示した実施例の動作原理を説明する
ための説明図であり、(a)は、高周波のコモンモード
ノイズ、(b)は、高周波のノーマルモードノイズ、(
c)は、低周波の信号電流(ノーマルモード)が、それ
ぞれ一方の端子側から入力したときに第1のコア5.第
2のコア7、第4のコア8に生じる各磁束の方向を示し
たもので、第1図中で示した静電シールド板9は図示を
省略しである。以下に各図をもとにそれぞれの動作を説
明する。
FIG. 2 is an explanatory diagram for explaining the operating principle of the embodiment shown in FIG. 1, in which (a) shows high frequency common mode noise, (b) shows high frequency normal mode noise, (
c) When a low frequency signal current (normal mode) is input from one terminal side, the first core 5. This figure shows the direction of each magnetic flux generated in the second core 7 and fourth core 8, and the electrostatic shield plate 9 shown in FIG. 1 is not shown. Each operation will be explained below based on each figure.

まず(a)で、入力端1,1′から高周波のコモンモー
ドノイズNcが入力したとき巻線(8−a)及び(8−
b)によってコア8の閉磁路内に生じる磁束φC3は、
互いに同方向であるため強めあい、1次側のコモンモー
ドノイズNcに対して大きなインダクタンスとして作用
する。これに対して巻線3を流れるコモンモードノイズ
N。によってコア5及び7内に生じる磁束φ。1.φc
2は同一磁路の中で逆方向に発生するため、1次側のコ
モンモートノイズN。には何ら影響を及ばさない。なお
コア5は高周波では実効透磁率が小さいため、その中に
生じる磁束φcxld、きわめて小さい値のものである
First, in (a), when high frequency common mode noise Nc is input from input terminals 1 and 1', windings (8-a) and (8-
The magnetic flux φC3 generated in the closed magnetic path of the core 8 due to b) is
Since they are in the same direction, they strengthen each other and act as a large inductance against the common mode noise Nc on the primary side. On the other hand, common mode noise N flowing through winding 3. The magnetic flux φ generated in cores 5 and 7 by φ. 1. φc
2 occurs in the opposite direction within the same magnetic path, so it is common moat noise N on the primary side. has no effect on. Note that since the core 5 has a small effective magnetic permeability at high frequencies, the magnetic flux φcxld generated therein has an extremely small value.

次に(b)で、入力側から高周波のノーマルモードノイ
ズNnが入力したとき、巻線(8−a)及び(8−b)
によってコア8の閉磁路内に生じる磁束φn3は、(a
)とは逆に互いに反対方向となって打ち消し合5ため、
ノーマルモードノイズNnに対して何ら影響を及ぼさな
い。−万巻線3によってコア5及びコア7内に生ずる磁
束φn1.φn2のうち前者は、(a)の場合と同様に
コア5の高周波での実効透磁率が小さいためにほとんど
生じず、2次巻@ :37側への影響はほとんどない。
Next, in (b), when high frequency normal mode noise Nn is input from the input side, the windings (8-a) and (8-b)
The magnetic flux φn3 generated in the closed magnetic path of the core 8 by (a
), they are in opposite directions and cancel each other5, so
It has no effect on normal mode noise Nn. - Magnetic flux φn1. generated in the core 5 and core 7 by the ten thousand windings 3. The former of φn2 hardly occurs because the effective magnetic permeability of the core 5 at high frequencies is small, as in the case of (a), and has almost no effect on the secondary winding @:37 side.

しかし後者は、コア7の閉磁路内を流れる短絡磁束とな
り、大きなインダクタンスとして作用する。これに対し
くc)で入力側から低周波信号電流(ノーマルモード)
Snが入力したとき、巻線(8−a)及び(8−b)に
よるコア8の閉磁路中の磁束は、cb)の場合と同様に
互いに反対方向となって打ち消し合うため低周波信号電
流Snに対し何ら影響を及ぼさない。しかし、巻線3に
よってコア5及び7内に生ずる磁束φ81.φs2のう
ち前者はコア5の低周波における実効透磁率がコア7の
それにくらべはるかに大きいため、信号電流Sllによ
る磁束の大部分は、φ81となってコア5内を流れ、2
次巻線3′の出力端に低周波の誘導電圧が発生する。
However, the latter becomes a short-circuit magnetic flux flowing within the closed magnetic path of the core 7, and acts as a large inductance. On the other hand, in c), low frequency signal current is generated from the input side (normal mode).
When Sn is input, the magnetic fluxes in the closed magnetic path of the core 8 due to windings (8-a) and (8-b) are in opposite directions and cancel each other out, as in the case of cb), so the low frequency signal current It has no effect on Sn. However, the magnetic flux φ81. Since the effective magnetic permeability of the core 5 at low frequencies in the former of φs2 is much larger than that of the core 7, most of the magnetic flux due to the signal current Sll becomes φ81 and flows inside the core 5, and the 2
A low frequency induced voltage is generated at the output end of the secondary winding 3'.

このように本発明では、高周波姉おける実効透磁率の低
下が少ない2組の磁性材(7,7’と8゜8′)を用い
、この一方に1次または2次巻線(3,3’)を第1の
コア5と共通に捲回し、他方に1次及び2次とは異なる
2組の巻線(8−a)、(8−b)と(8’−a )、
 (8’−b )を施し、その巻方向を工夫して高周波
のノーマル、コモン両モードノイズに対してそれぞれ大
きなインダクタンスとして作用するようにしておる。
In this way, in the present invention, two sets of magnetic materials (7, 7' and 8°8') with a small decrease in effective magnetic permeability in the high frequency upper half are used, and one of the sets is equipped with the primary or secondary winding (3, 3). ') is wound in common with the first core 5, and on the other side, two sets of windings (8-a), (8-b) and (8'-a) different from the primary and secondary windings,
(8'-b), and the winding direction is devised so that it acts as a large inductance for both high-frequency normal and common mode noises.

また巻線間の電磁波の輻射を防ぐ九め巻1113と巻線
(8−a)及び(8−b)との間を静電シールド板でじ
ゃへいするとともに、それぞれの巻線電流による閉磁路
間の磁気干渉を防ぐためコア7゜8を分離して構成しで
ある(これにより磁気能率の低下を防ぐことができる)
In addition, an electrostatic shield plate is used between the ninth winding 1113 and the windings (8-a) and (8-b) to prevent radiation of electromagnetic waves between the windings, and a closed magnetic path is created by each winding current. In order to prevent magnetic interference between the cores, the cores 7 and 8 are separated (this prevents a decrease in magnetic efficiency).
.

したがって従来のように1次・2次巻線間静電シールド
板の接地状態によってノイズ阻止効果が低下したり、低
周波コアに捲回した1次、2次巻線とコアを共有して設
けた巻線を用いることによる高周波ノイズ阻止特性の悪
化及び大容量の線間キャパシタンス挿入など別部品の接
続などの必要がなくなるという利点がある。
Therefore, unlike conventional methods, the noise blocking effect may be reduced depending on the grounding condition of the electrostatic shield plate between the primary and secondary windings, or the core may be shared with the primary and secondary windings wound around the low frequency core. This has the advantage of eliminating the need for deterioration in high-frequency noise blocking characteristics due to the use of a winding wire having a large capacity, and the need for connecting separate components such as inserting a large line capacitance.

第3図(a)は本発明の実施例の組立断面図であり、コ
ア5の閉磁路の一部を中心にコア7.7′金それと同心
状に配置しこれに1次・2次巻線3゜3′を施し、コア
8及び巻線(8−a)ld、コア5の前記閉磁路部分に
静電シールド板9をはさんで同心状に配置し、コア7の
磁路の一部Mで外周を非接触に囲んだもので、さらにコ
ア7の外周は、静電シールド板9でおおっである。
FIG. 3(a) is an assembled sectional view of an embodiment of the present invention, in which a part of the closed magnetic path of the core 5 is arranged concentrically with the core 7, 7', and the primary and secondary windings are arranged around a part of the closed magnetic path of the core 5. The core 8, the winding (8-a) ld, and the electrostatic shield plate 9 are placed concentrically in the closed magnetic path portion of the core 5, and one of the magnetic paths of the core 7 is The outer periphery of the core 7 is surrounded by a portion M in a non-contact manner, and the outer periphery of the core 7 is further covered with an electrostatic shield plate 9.

(b)は、その平面図であり、1次側と2次側巻線3.
3’(図には現れていない)は静電シールド板9にて分
離されている。(c)は、概略斜視図であり、静電シー
ルド板及びコア7は図示を省略しである。
(b) is a plan view thereof, showing the primary and secondary windings 3.
3' (not shown) is separated by an electrostatic shield plate 9. (c) is a schematic perspective view, and the electrostatic shield plate and the core 7 are not shown.

第4図(a)は、本発明において用いるコア7゜7′の
具体例を示す分解斜視図、第4図(b)はその一部を形
成するための磁性材の原形を示す平面図である。コア5
に巻きつける中心部分(7a)。
Fig. 4(a) is an exploded perspective view showing a specific example of the core 7゜7' used in the present invention, and Fig. 4(b) is a plan view showing the original form of the magnetic material forming a part thereof. be. core 5
The center part (7a) to be wrapped around.

その上部両端にかぶせる部分(7−b)、中心部分(7
−a)に1次巻線3を巻きつけその外側をおおう部分(
7−c)を板状またはテープ状の磁性材から図示の如く
作成し、閉磁路を構成するようにしたものである なお、第4図(b)は、第4図(a)における中心部分
(7−a)を形成する原材料となる磁性材の平面図であ
ることは容易に判るであろう。
The part that covers both ends of the upper part (7-b), the center part (7-b)
-a) The part where the primary winding 3 is wound and the outside is covered (
7-c) is made from a plate-shaped or tape-shaped magnetic material as shown in the figure to constitute a closed magnetic circuit. Note that FIG. 4(b) shows the center part in FIG. 4(a). It will be easily understood that this is a plan view of the magnetic material that is the raw material for forming (7-a).

第5図(a)は、第4図(a)のコア7の側面部分とコ
ア8と静電シールド板9を一体化構造として図示したも
ので、(b)は(a)の構造の組立手順を示す説明図で
、点線の部分でコアの側面部分(7−c)を矢印方向に
内側に折り曲げて組立てる。
FIG. 5(a) shows the side part of the core 7 in FIG. 4(a), the core 8, and the electrostatic shield plate 9 as an integrated structure, and FIG. 5(b) shows the assembly of the structure in FIG. 4(a). In the explanatory diagram showing the procedure, the side portion (7-c) of the core is bent inward in the direction of the arrow at the dotted line portion to assemble.

第5図(a)はまたコア8とシールド板9のくりぬき部
Qの外周の一部に共通に巻線(8a ) z(8−b、
)を施した組立図でもあり、このような構造にすること
によってコア7.8及びその巻線部分が容易に形成でき
る。
FIG. 5(a) also shows windings (8a) z(8-b,
), and by adopting such a structure, the core 7.8 and its winding portion can be easily formed.

第6図は、本発明の他の実施例を示す斜視図でちり、低
周波で高い実効透磁率を有するコア5として、ヨの字形
の磁性材を2個突き合せその中央部(突き合せ部分)で
結合したものを用い、1次・2次巻線(3,3’)間容
量を減少させると共に1次側から2次側又はその逆への
電磁波の輻射を阻止するため両巻線を分離して構成した
もので、静電シールド板及びコア7は図示を省略しであ
る。
FIG. 6 is a perspective view showing another embodiment of the present invention, in which two pieces of Y-shaped magnetic material are butted together as a core 5 having high effective magnetic permeability at low frequencies, and the central part (butted part ) to reduce the capacitance between the primary and secondary windings (3, 3') and to prevent the radiation of electromagnetic waves from the primary side to the secondary side or vice versa. It is constructed separately, and the electrostatic shield plate and core 7 are not shown.

第7図は、第6図に示した実施例の組立図であり、(a
)はその側面図、(b)は平面図である。これらの図に
おいて、10は、トランス全周をおおう磁性材である。
FIG. 7 is an assembly diagram of the embodiment shown in FIG.
) is its side view, and (b) is its plan view. In these figures, 10 is a magnetic material that covers the entire circumference of the transformer.

これらの図については、改めて説明するまでもないであ
ろつ。
There is no need to explain these figures again.

〔発明の効果〕〔Effect of the invention〕

以上説明したように本願発明は、低周波における実効透
磁率の大きい1次、2次巻線(3,3’)貫通の閉磁路
コア(第1のコア5)に、高周波における実効透磁率の
低下が少ない磁性材からなる2種類のコア(7,7’と
8.8 ’)を、対象とする入力ノイズの周波数に応じ
て組み合せたもので、入出力端のいずれの側から侵入す
るノイズに対しても十分な阻止効果をもつという利点が
ある。またコモンモードノイズを阻止する巻線と高周波
のノーマルモードノイズを阻止する巻線の磁路が(8と
7,8′と7′の如く)分離されているので巻線間の磁
気干渉を防止できる(従って磁気能率の低下を阻止でき
る)という利点もある。さらに各コアの対向面外周を静
電シールド板でおおったものは巻線から放射される輻射
電磁界の影響を防止できるという利点もある。
As explained above, the present invention provides a closed magnetic circuit core (first core 5) passing through the primary and secondary windings (3, 3') that has a large effective magnetic permeability at low frequencies, and a closed magnetic circuit core (first core 5) that has a large effective magnetic permeability at high frequencies. Two types of cores (7, 7' and 8.8') made of magnetic material with low degradation are combined according to the frequency of the target input noise, and noise that enters from either side of the input/output end. It also has the advantage of having a sufficient blocking effect against. In addition, the magnetic paths of the winding that blocks common mode noise and the winding that blocks high frequency normal mode noise are separated (as in 8 and 7, 8' and 7'), preventing magnetic interference between the windings. (therefore, it is possible to prevent a decrease in magnetic efficiency). Furthermore, covering the outer periphery of the opposing surface of each core with an electrostatic shield plate has the advantage that it can prevent the influence of the radiated electromagnetic field radiated from the windings.

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

wl、1図は本発明の一実施例を示す断面図、第2図(
a)=(bL (c)はそれぞれ本発明の一実施例の動
作説明図、第3図(a)は本発明の一実施例の組立断面
図、第3図(b)は同平面図、第3図(C)は同斜視図
、第4図(a)は本発明において用いるコア7.7′の
具体例を示す分解斜視図、第4図(b)はその一部を形
成するための磁性材の原形を示す平面図、第5図(a)
a第4図(a)に示したコア7の側面部分とコア8と静
電シールド板9の一体化構造を示す斜視図、第5図(b
)はその組立手順の説明図、第6図は本発明の他の実施
例を示す斜視図、第7図(a)は第6図に示した実施例
の組立側面図、第7図(b)は同平面図、第8図(a)
。 (b)j(C)はそれぞれ従来の雑音阻止トランスの回
路構成例を示す回路図、である。 符号説明 3・・・・・・1次巻線、3′・・・・・・2次巻線、
5・・・・・・低周波高実効透磁率磁性体からなる第1
のコア、7゜7′・・・・・・高周波高実効透磁率磁性
体からなる第2゜第3のコア、8,8’・・・・・・同
第4.第5のコア、(8−a )、 (8−b )・・
・・・・コア8の閉磁路部分に施した巻線、(8’−a
)、(8乙b)・・・・・・同じくコア8′に施した巻
線、9・・・・・・シールド板、10・・・・・・ケー
ス 代理人 弁理士 並 木 昭 夫 代理人 弁理士 松 崎 清 第1図 第2図 (a) 第2の (bン (C) 第5図 第7図 (+1)
wl, Figure 1 is a sectional view showing one embodiment of the present invention, Figure 2 (
a) = (bL) (c) is an explanatory diagram of the operation of one embodiment of the present invention, FIG. 3(a) is an assembled sectional view of one embodiment of the present invention, FIG. 3(b) is a plan view thereof, FIG. 3(C) is a perspective view of the same, FIG. 4(a) is an exploded perspective view showing a specific example of the core 7.7' used in the present invention, and FIG. 4(b) is a part of the core 7.7'. A plan view showing the original shape of the magnetic material, FIG. 5(a)
a A perspective view showing the integrated structure of the side part of the core 7, the core 8, and the electrostatic shield plate 9 shown in FIG. 4(a); FIG. 5(b)
) is an explanatory diagram of the assembly procedure, FIG. 6 is a perspective view showing another embodiment of the present invention, FIG. 7(a) is an assembly side view of the embodiment shown in FIG. 6, and FIG. 7(b) ) is the same plan view, Fig. 8(a)
. (b) and (c) are circuit diagrams showing examples of circuit configurations of conventional noise blocking transformers, respectively. Symbol explanation 3...Primary winding, 3'...Secondary winding,
5...The first layer made of a low frequency, high effective permeability magnetic material
core, 7゜7'... 2nd゜3rd core made of high frequency, high effective permeability magnetic material, 8, 8'... same 4th core. Fifth core, (8-a), (8-b)...
...Winding applied to the closed magnetic circuit part of core 8, (8'-a
), (8 Ob)...Similar winding applied to core 8', 9...Shield plate, 10...Case agent Patent attorney Akio Namiki Person Patent Attorney Kiyoshi Matsuzaki Figure 1 Figure 2 (a) Second (b (C) Figure 5 Figure 7 (+1)

Claims (1)

【特許請求の範囲】 1)低周波高実効透磁率磁性材で少なくも第1の脚部と
第2の脚部を含む閉磁路を形成して成る第1のコアと、
中央脚部とその周囲に該脚部を共通磁路として閉磁路を
高周波高実効透磁率磁性材で形成してなる二つのコア(
第2および第3の各コア)と、高周波高実効透磁率磁性
材で閉磁路を形成してなる二つのコア(第4および第5
の各コア)と、をもち、 前記第1のコアの第1の脚部と前記第2のコアの中央脚
部とを一体にして1次巻線を捲回し、前記第1のコアの
第2の脚部と前記第3のコアの中央脚部とを一体にして
2次巻線を捲回し、さらK、前記第4のコアに、コモン
モードの電流に対して同方向磁束が生じるように捲回さ
れた二つの巻線の各一端を前記1次巻線の各端部に接続
し、前記第5のコアに、コモンモードの電流に対して同
方向磁束が生じるように捲回された二つの巻線の各 −
一端を前記2次巻線の各端部に接続し、前記第2のコア
と第3のコアの間、前記第2のコアと第4のコアの間、
前記第3のコアと第5のコアの間、の何れか一つまたは
複数に静電シールドをほどこし、またはほどこさないで
成ることを特徴とする雑音阻止複合トランス。
[Scope of Claims] 1) A first core formed of a low frequency, high effective permeability magnetic material forming a closed magnetic path including at least a first leg portion and a second leg portion;
Two cores are formed of a high frequency, high effective permeability magnetic material, and a closed magnetic path is formed around the center leg and its surroundings using the leg as a common magnetic path.
2nd and 3rd cores), and two cores (4th and 5th cores) that form a closed magnetic path with a high frequency, high effective permeability magnetic material.
each core), the first leg of the first core and the central leg of the second core are integrated to wind a primary winding, A secondary winding is wound by integrating the second leg and the central leg of the third core, and further, K, the fourth core is configured to generate a magnetic flux in the same direction with respect to the common mode current. One end of each of two windings wound on the primary winding is connected to each end of the primary winding, and the fifth core is wound so that a magnetic flux is generated in the same direction with respect to a common mode current. Each of the two windings −
one end connected to each end of the secondary winding, between the second core and the third core, between the second core and the fourth core,
A noise-blocking composite transformer characterized in that an electrostatic shield is provided or not provided between one or more of the third core and the fifth core.
JP59115507A 1984-06-07 1984-06-07 Noise interruption composite transformer Pending JPS60260119A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP59115507A JPS60260119A (en) 1984-06-07 1984-06-07 Noise interruption composite transformer

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP59115507A JPS60260119A (en) 1984-06-07 1984-06-07 Noise interruption composite transformer

Publications (1)

Publication Number Publication Date
JPS60260119A true JPS60260119A (en) 1985-12-23

Family

ID=14664228

Family Applications (1)

Application Number Title Priority Date Filing Date
JP59115507A Pending JPS60260119A (en) 1984-06-07 1984-06-07 Noise interruption composite transformer

Country Status (1)

Country Link
JP (1) JPS60260119A (en)

Cited By (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
WO2005048451A1 (en) * 2003-11-12 2005-05-26 Matsushita Electric Industrial Co., Ltd. Communication transformer
WO2020170499A1 (en) * 2019-02-19 2020-08-27 株式会社明電舎 Insulation transformer

Cited By (3)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
WO2005048451A1 (en) * 2003-11-12 2005-05-26 Matsushita Electric Industrial Co., Ltd. Communication transformer
US7573363B2 (en) 2003-11-12 2009-08-11 Panasonic Corporation Communication transformer for power line communication
WO2020170499A1 (en) * 2019-02-19 2020-08-27 株式会社明電舎 Insulation transformer

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