JPS60226110A - Noise protection transformer - Google Patents

Noise protection transformer

Info

Publication number
JPS60226110A
JPS60226110A JP59082038A JP8203884A JPS60226110A JP S60226110 A JPS60226110 A JP S60226110A JP 59082038 A JP59082038 A JP 59082038A JP 8203884 A JP8203884 A JP 8203884A JP S60226110 A JPS60226110 A JP S60226110A
Authority
JP
Japan
Prior art keywords
core
closed magnetic
magnetic path
winding
windings
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
JP59082038A
Other languages
Japanese (ja)
Inventor
Kusuo Takagi
高木 国主男
Katsuaki Kubota
久保田 勝昭
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 JP59082038A priority Critical patent/JPS60226110A/en
Publication of JPS60226110A publication Critical patent/JPS60226110A/en
Pending legal-status Critical Current

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Classifications

    • HELECTRICITY
    • H01ELECTRIC ELEMENTS
    • H01FMAGNETS; INDUCTANCES; TRANSFORMERS; SELECTION OF MATERIALS FOR THEIR MAGNETIC PROPERTIES
    • H01F19/00Fixed transformers or mutual inductances of the signal type
    • H01F19/04Transformers or mutual inductances suitable for handling frequencies considerably beyond the audio range
    • H01F19/06Broad-band transformers, e.g. suitable for handling frequencies well down into the audio range

Landscapes

  • Engineering & Computer Science (AREA)
  • Multimedia (AREA)
  • Power Engineering (AREA)
  • Coils Or Transformers For Communication (AREA)
  • Inverter Devices (AREA)

Abstract

PURPOSE:To obtain stable and sufficient noise rejection characteristic without requiring any parts other than winding and core by simultaneously rejecting both high frequency normal and common mode noises through additional use of core which shows less drop of effective permeability at a high frequency or magnetic material such as magnetic sheet. CONSTITUTION:When a high frequency common mode noise Nc is input from the input end side, magnetic fluxes phic3 generate within a closed magnetic loop of core 7 by the winding 8-a and the winding 8-b are enhanced because these are generated in the same direction and it works as a large inductance to the Nc of primary side. When a high frequency normal mode noise Nn is input from the input side, the magnetic fluxes phin3 generated within a closed magnetic loop of core 7 by the widing 8-1 and the winding 8-b are cancelled each other because these are generated respectively in the opposite directions and the windings 8-a, 8-b and core 7 do not give any influence on the primary current of Nn. When a low frequency current (normal mode) Sn is input from the input side, the windings 8-a, 8-b and core 7 do not give any influence on Sn.

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同時に阻止することのでき
る雑音防護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 aims to simultaneously block 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 protection transformer that can provide noise protection.

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

従来、この種の雑音防護トランスとしては、第8図に示
すような構成のものが用いられている。
Conventionally, as this type of noise protection transformer, one having a configuration as shown in FIG. 8 has been used.

すなわち第8図fa+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
c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、(bl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Nc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Ncに対し大きなインダクタンスが
作用するようにしてコモンモードノイズの阻止をはかっ
ていた。
In other words, as shown in Fig. 8 fa+, common mode noise N due to the common mode current input in the same phase from the input terminal 1.1' side
For the common mode noise Nc, an electrostatic shield plate 4 is inserted between the primary winding 3 and the secondary winding 3', and this is grounded to reduce the inter-winding capacitance Co. To suppress the passage to the secondary side (as shown in bl),
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 Nc. Common mode noise was prevented by causing a large inductance to act on common mode noise Nc.

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Nnに対しては、第8図fc)に示すように
巻線3の画線間にキャパシタンスC。
In addition, with respect to normal mode noise Nn inputted from the input terminal 1.1' side with an opposite phase, a capacitance C is generated between the lines of the winding 3 as shown in FIG. 8fc).

を挿入してノーマルモトノイズの阻止をはかっていた。was inserted to block normal moto noise.

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に流れる低周波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 frequency signal current that originally flows in the primary winding 3 is efficiently transferred to the secondary winding 3. Since the common mode noise blocking windings 6 and 6' are wound around the core 5, which is designed to be interlinked with the core 5, 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fcl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CI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。
Furthermore, the fcl has the disadvantage that components other than the windings and core are required, such as the need for a large capacitance CI 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は、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防護トラン
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 an 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. An object of the present invention is to provide a noise protection transformer that can obtain blocking 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
ードノイズを同時にかつ双方とも阻止できるようにした
点にある。
The key point of the present invention is to make it possible to simultaneously block both high-frequency normal and common mode noise by additionally using a magnetic material such as a core or magnetic sheet that has a small drop in effective magnetic permeability at high frequencies in a transformer. That's the point.

〔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(a)は本発明の一実施例を、fblは(a)に
銅。
FIG. 1(a) shows an example of the present invention, and fbl is copper in FIG. 1(a).

アルミニウムなどの導電体からなる静電シールド板を装
着した実施例を、それぞれ示す。(alで7は高周波領
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ら磁性粉を塗着した磁性テープな
どの磁性材からなる第2のコア、(8−a>、(8−b
)、および(8′−a)、(8’−b)は、コア7の環
状閉磁路部分に入力端からの同相電流に対して互いに同
方向磁束が生じるようそれぞれ捲回した巻線である。
Examples are shown in which an electrostatic shield plate made of a conductive material such as aluminum is attached. (In al, 7 is a second core made of a magnetic material such as a plate-like material such as a magnetic dust core that has a small decrease in effective permeability up to a high frequency region, or a magnetic tape coated with these magnetic powders, (8-a >, (8-b
), (8'-a), and (8'-b) are windings respectively wound in the annular closed magnetic circuit portion of the core 7 so that magnetic fluxes in the same direction are generated in response to in-phase currents from the input end. .

1次巻線3および2次巻線3′は、コア5の磁路の中で
1次側磁路部分5Pと2次側磁路部分5Sに、それぞれ
同心的に配置された第2のコア7゜7′の該同心部分に
図示の如く捲回され、巻線3゜3′の外周部は、コア7
.7′の閉磁路構成部分によっておおわれている。
The primary winding 3 and the secondary winding 3' are arranged concentrically in a primary magnetic path section 5P and a secondary magnetic path section 5S in the magnetic path of the core 5, respectively. The outer periphery of the winding 3° 3' is wound around the core 7° 7' as shown in the figure.
.. It is covered by the closed magnetic circuit component 7'.

また(blにおいて、9および9′は2つの第2のコア
7.7′の相対向面部分またはそれぞれの全周をおおっ
た静電シールド板、10および10′は巻線3と巻vA
(8a)、(8−b)との間、および巻線3′と巻線(
8’−a>、(8’ −b)との間にそれぞれ配置した
静電シールド板である。
In addition, (in bl, 9 and 9' are electrostatic shield plates that cover the facing portions of the two second cores 7 and 7' or their respective entire circumferences, and 10 and 10' are the winding 3 and the winding vA.
(8a) and (8-b), and between winding 3' and winding (
8′-a> and (8′-b), respectively.

第2図は第1図(alの実施例の動作原理の説明図であ
り、第2図(alは高周波のコモンモードノイズ。
FIG. 2 is an explanatory diagram of the operating principle of the embodiment of FIG. 1 (al), and FIG. 2 (al is high-frequency common mode noise).

(blは高周波のノーマルモードノイズ5(C)は低周
波電流(ノーマルモード)が一方の端子側から入力した
ときの第1のコア5および第2のコア7に生じる磁束の
方向を示したものである。
(bl is high frequency normal mode noise 5 (C) is the direction of magnetic flux generated in the first core 5 and second core 7 when low frequency current (normal mode) is input from one terminal side It is.

以下に各図をもとにそれぞれの動作を説明する。Each operation will be explained below based on each figure.

まず第2図fa+で入力端側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(lha)および巻線
(8−b)によってコア7の閉磁路内に生じる磁束φc
3は互いに同方向であるため強めあい、1次側の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Ncによってコア5およびコア7内
に生じる磁束それぞれφ。およびφC2は、同相電流の
ため互いに反対方向に生じ打消し合うため1次側のNc
には何ら影響しない。なおコア5は高周波ではその実効
透磁率が小さいため、φc+はきわめて小さい値である
First, in Fig. 2 fa+, when high frequency common mode noise Nc is input from the input end side, magnetic flux φc is generated in the closed magnetic path of the core 7 by the winding (lha) and the winding (8-b).
3 are in the same direction, so they strengthen each other and act as a large inductance with respect to Nc on the primary side. On the other hand, the magnetic fluxes generated in core 5 and core 7 by Nc flowing through winding 3 are φ. and φC2 occur in opposite directions and cancel each other due to the common mode current, so Nc on the primary side
has no effect on Note that since the effective magnetic permeability of the core 5 is small at high frequencies, φc+ is an extremely small value.

次に第2図(blで入力端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)および巻線
(8−b)によってコア7の閉磁路内に生じる磁束φ、
は(alの場合とは逆に互いに反対方向となって打消し
合うため、Nnに対しS&i!(8−a)、(8−b)
およびコア7は1次側電流に何ら影響を与えない。
Next, when high-frequency normal mode noise Nn is input from the input terminal in FIG. 2 (bl), the magnetic flux φ generated in the closed magnetic path of the core 7 by the winding (8-a) and the winding (8-b),
(Contrary to the case of al, they cancel each other in opposite directions, so S&i! (8-a), (8-b) for Nn
And the core 7 has no effect on the primary current.

一方、巻線3によってコア5およびコア7内に生じる磁
束それぞれφ、およびφゎ2のうち、前者は(alの場
合と同様にコア5の高周波実効透磁率が小さいためにほ
とんど生じず、2次巻線3′側への影響はほとんどない
。しかし後者はコア5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。
On the other hand, among the magnetic fluxes φ and φゎ2 generated in the core 5 and core 7 by the winding 3, the former is hardly generated due to the small high-frequency effective magnetic permeability of the core 5 (as in the case of Al, and 2 There is almost no effect on the next winding 3'.However, the latter becomes a short-circuit magnetic flux flowing within the closed magnetic path of the core 5, and acts as a large inductance.

これらに対して第2図(C1で入力側から低周波電流(
ノーマルモード)Snが入力したとき、巻線(8−a)
、(8−b)によるコア7の閉磁路中の磁束は(blの
場合と同様に互いに反対方向となって打消し合うため、
Snに対し巻線(8−a)。
In contrast to these, in Figure 2 (C1, low frequency current from the input side (
Normal mode) When Sn is input, winding (8-a)
, (8-b), the magnetic fluxes in the closed magnetic path of the core 7 are in opposite directions and cancel each other out, as in the case of (bl), so
Winding (8-a) for Sn.

(8−b)およびコア7は何らの影響も与えない。(8-b) and core 7 have no effect.

巻m3によってコア5およびコア7内に生じる磁束それ
ぞれφsIおよびφ、2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にくらべはるかに大きいた
めSnによる磁束の大部分はφ。
Of the magnetic fluxes φsI and φ,2 generated in core 5 and core 7 by winding m3, the former has a much larger effective permeability at low frequencies than core 7, so most of the magnetic flux due to Sn is φ.

となってコア5内を流れ、これによって2次巻線3′の
出力端側に低周波の誘起電圧が発生ずる。
flows through the core 5, thereby generating a low-frequency induced voltage at the output end of the secondary winding 3'.

このように本発明では高周波における実効透磁率の低下
が少ない磁性材を用い、これに1次および2次巻線とは
異なる2つの巻線を施し、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であるため
、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次巻線とコアを共用して設けた巻線
を用いることによる高周波ノイズ阻止特性の悪化、およ
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。
In this way, the present invention uses a magnetic material whose effective magnetic permeability decreases little at high frequencies, provides two windings different from the primary and secondary windings, and devises the winding direction to achieve high frequency normal and Since the common mode acts as a large inductance for both mode noises, the noise blocking effect may be reduced depending on the grounding condition of the electrostatic shield plate between the primary and secondary windings, and the low frequency core This eliminates the deterioration of high frequency noise blocking characteristics due to the use of a winding that shares the core with the primary and secondary windings wound around the core, and eliminates the need to connect separate components such as inserting large line capacitance. There is an advantage.

第3図は本発明の実施例に用いているコア7およびこれ
を形成する磁性材7Aの構成の具体例を示すものであり
、1次巻線3または2次巻線3′の外側から巻きつける
部分をta+乃至(flに示し、コア5に接する内側部
分は(glに示しである。
FIG. 3 shows a specific example of the structure of the core 7 and the magnetic material 7A forming the core used in the embodiment of the present invention. The attached parts are shown as ta+ to (fl), and the inner part that contacts the core 5 is shown as (gl).

すなわち、くりぬき部9を設けた板状またはテープ状の
磁性材7Aを(a)や(C1のように形成し、これらを
巻線3または3′の外周に沿って(blまたは1dlの
ように囲んでコア7を形成し、その閉磁路部分に巻線(
8−a)、(8−b)を施す。なお接合部10は組立後
図示しない同一の磁性片などを用いて磁気的に短絡する
That is, a plate-shaped or tape-shaped magnetic material 7A provided with a hollowed out part 9 is formed as shown in (a) or (C1), and is placed along the outer periphery of the winding 3 or 3' (as shown in bl or 1dl). The core 7 is formed by surrounding the core 7, and the winding (
8-a) and (8-b) are performed. Note that after assembly, the joint portion 10 is magnetically short-circuited using the same magnetic piece (not shown) or the like.

(elおよび(f)ば巻線(8−a)、(8−b)を施
す部分に折曲げ部11を設けてこれに巻付けたり、同種
の磁性棒12を中心としてこれに巻付けるなどし5て巻
線中心部が飽和しないようにした例である。
(el and (f)) A bent part 11 is provided at the part where windings (8-a) and (8-b) are applied, and the winding is wound around this, or the same type of magnetic bar 12 is wound around this, etc. This is an example in which the central part of the winding is prevented from becoming saturated.

(glはコア5に接する内側部分を示しており、これに
tag、 (C1の如き磁性材7Aを巻き付けるもので
ある。
(gl indicates the inner part in contact with the core 5, and a magnetic material 7A such as tag, (C1) is wound around this.

第4図は各巻線間に挿入する静電シールド板9および1
0を一枚の板で一体的に形成した具体例であり、(al
は斜視図、(b)は第3図のコア7と組合せた断面図で
あり、巻線の全周を囲うための−F側と下側部分は図示
を省略しである。
Figure 4 shows electrostatic shield plates 9 and 1 inserted between each winding.
This is a specific example in which 0 is integrally formed with one plate, and (al
is a perspective view, and (b) is a sectional view combined with the core 7 of FIG. 3, and the -F side and lower portion for surrounding the entire circumference of the winding are omitted from illustration.

第5図は本発明の他の実施例を示す説明図であり、本実
施例は、2個の凹字形コア部20a、20bの中心磁路
部分に別々に巻線3または3′およびこれらの内、外周
にコア7を形成したものを挿入し中央で結合するなどに
より形成される。
FIG. 5 is an explanatory diagram showing another embodiment of the present invention. In this embodiment, the windings 3 or 3' and their It is formed by inserting a core 7 formed on the inner and outer peripheries and joining them at the center.

第6図+a)は第5図の巻線3または3′の外周に巻き
つけてコア7を形成するための磁性板7Aの形状を示す
ものであり、9はくり抜き部、11は底板部、12は凹
字形コア部の中央脚部の貫通穴である。(blはこれを
第6図中の巻&’j13の外周に巻付けて形成した組立
図の概略図であり、組立後底板11はおこして隣接巻線
3′側および巻線(8−a)、(8−b)側へ磁束がも
れないよう7と固着する。
Figure 6+a) shows the shape of the magnetic plate 7A for forming the core 7 by winding it around the outer periphery of the winding 3 or 3' in Figure 5, where 9 is a hollowed out part, 11 is a bottom plate part, 12 is a through hole in the central leg of the concave core. (bl is a schematic diagram of an assembly diagram formed by winding this around the outer periphery of the winding &'j13 in FIG. ) and (8-b) to prevent magnetic flux from leaking to the side.

(C)は(a)と異なる形状の磁性材を巻付けた例であ
る。
(C) is an example in which a magnetic material having a different shape from (a) is wound.

第7図は本発明の実施例について巻線侵入ノイズによる
電磁波の輻射防止効果を説明する展開図であり、(a)
は第1図(a)の磁性材(コア)7による磁気輻射に、
fblば第1図(b)から磁性材部分を除いた静電輻射
に対する防止効果をそれぞれ示したものである! すなわち入力端からの高周波ノイズ特にコモンモードノ
イズは、入力巻線のインピーダンスが大きい場合、ここ
から隣接巻線へ電磁波の輻射という形でも伝達する。こ
れらは例えば第7図で、巻線(8−a)、(8−b)か
ら巻線3.3’、(8”b)などへ、および巻線3から
巻線3′。
FIG. 7 is a developed diagram illustrating the effect of preventing electromagnetic wave radiation due to winding intrusion noise in an embodiment of the present invention, (a)
is due to the magnetic radiation due to the magnetic material (core) 7 in Fig. 1(a),
fbl shows the effect of preventing electrostatic radiation from FIG. 1(b) excluding the magnetic material part! That is, when the impedance of the input winding is large, high frequency noise, particularly common mode noise, from the input end is transmitted from there to the adjacent winding in the form of electromagnetic wave radiation. These are for example in FIG. 7 from windings (8-a), (8-b) to windings 3.3', (8''b), etc., and from winding 3 to winding 3'.

(8’−a)などへそれぞれ輻射する電磁波の(Ill
)に示す磁界成分それぞれm、 、 m4 、 m3 
、 m、 。
(Ill
) are the magnetic field components m, , m4, m3, respectively.
, m, .

m5および(b)に示す電界成分それぞれeI+”2+
e3 + ”4 + 05等であるが、一般には巻線イ
ンピーダンスの大きい巻線3からの輻射波m、。
The electric field components shown in m5 and (b) are eI+”2+, respectively.
e3 + "4 + 05, etc., but generally the radiation wave m from the winding 3 has a large winding impedance.

ms、C4,esなどが他より大きい。ms, C4, es, etc. are larger than others.

しかし本発明では第7図から明らかなように、1次巻′
#lAa側と2次巻線3′側とを分離した上で、これら
の巻線の全周もしくは少なくとも対向面近傍を(alで
は磁性材(コア)7で、またfblでは静電シールド板
9,9′、10.10’でそれぞれおおっているため、
反対側への輻射電磁界成分はこれらにほとんど吸収され
る。
However, in the present invention, as is clear from FIG.
After separating the #lAa side and the secondary winding 3' side, the entire circumference of these windings or at least the vicinity of the opposing surface is covered with a magnetic material (core) 7 for Al, and an electrostatic shield plate 9 for FBL. , 9', and 10.10', so
Most of the radiated electromagnetic field components to the opposite side are absorbed by these.

〔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次巻線貫通の閉磁路コアに、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第
2のコアを組合せ、後者に形成した2つの閉磁路とこれ
に施した巻線とによって入出力端のいずれの側から侵入
するノイズにも十分な阻止効果をもつようにしたもので
、第2のコアの存在によりノーマル、コモンいずれのモ
ードのノイズに対しても接地をとるなどの必要がなく有
効に防護できる利点がある。
As explained above, the present invention combines a closed magnetic circuit core passing through the primary and secondary windings, which has a large effective magnetic permeability at low frequencies, with a second core made of a magnetic material whose effective magnetic permeability decreases little at high frequencies. , the two closed magnetic circuits formed in the latter and the windings attached to these circuits have a sufficient blocking effect on noise entering from either side of the input/output end, and the presence of the second core It has the advantage of being able to effectively protect against both normal and common mode noise without the need for grounding.

また上記第2のコア、またはこれと静電シールド板とを
、1次、2次巻線間の少なくとも相対向面側外周をおお
うように配置し”ζあるため、巻線−から放射される輻
射雑音電磁界の影響を防止できるという利点もある。
In addition, since the second core or the electrostatic shield plate is arranged so as to cover at least the outer periphery of the opposing surface between the primary and secondary windings, radiation from the windings is Another advantage is that the effects of radiated noise electromagnetic fields can be prevented.

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

第1図1alは本発明の一実施例を示す説明図、第1図
(b)は同じく他の実施例を示す説明図、第2図(a)
〜(C)は、第1図(a)に示した実施例の動作原理説
明図、第1図1al〜fglは第1図1alの実施例に
おいて用いる第2のコアとその形成用磁性材の具体例を
示す説明図、第1図1alは各巻線間に挿入する静電シ
ールド板の具体例を示す斜視図、第4図(blは同断面
図、第5図は本発明の更に別の実施例を示す説明図、第
6図(al〜telは第5図に示す実施例において用い
る第2のコアとその形成用磁性材の具体例を示す説明図
、第7図(at、 (blは本発明の実施例について巻
線侵入ノイズによる電磁波の輻射防止効果を示す展開図
、第8図は従来の雑音防護トランスの回路構成を示す回
路図である。 符号説明 3・・・1次巻線、3′・・・2次巻線、5・・・低周
波における実効透磁率の大きい磁性体からなる第1のコ
ア、7A・・・高周波における実効透磁率の低下が少な
い磁性体、7・・・7Aで構成した第2のコア、8−a
、8−b・・・第2のコア5の閉磁路部分に巻線を施し
た部分、9.9′・・・第2のコア7の外周に沿って巻
付けた静電シールド板、10・・・巻線間に挿入した静
電シールド板、20a、20b・・・ヨ字形コア部。 代理人 弁理士 並 木 昭 夫 代理人 弁理士 松 崎 清 MI図 ((L) □□□□−−−( ) 第3図 (υ)(b) (C)(d) 第3図 (子) (1ン 第4図 (艮)Cシ) 拵5図 第6図 (α) (b) ((:) rn7図 (α)
FIG. 1 1al is an explanatory diagram showing one embodiment of the present invention, FIG. 1(b) is an explanatory diagram similarly showing another embodiment, and FIG. 2(a)
~(C) is an explanatory diagram of the operating principle of the embodiment shown in FIG. 1(a), and FIG. An explanatory diagram showing a specific example, FIG. 1 al is a perspective view showing a specific example of an electrostatic shield plate inserted between each winding, FIG. 4 is a sectional view of the same, and FIG. Explanatory drawings showing examples, FIG. 6 (al to tel are explanatory drawings showing specific examples of the second core and the magnetic material for forming it used in the example shown in FIG. 5, FIG. 7 (at, (bl) 8 is a developed diagram showing the radiation prevention effect of electromagnetic waves due to winding infiltration noise in the embodiment of the present invention, and FIG. 8 is a circuit diagram showing the circuit configuration of a conventional noise protection transformer. Wire, 3'...Secondary winding, 5...First core made of a magnetic material with large effective magnetic permeability at low frequencies, 7A...Magnetic material with little reduction in effective magnetic permeability at high frequencies, 7 ...Second core composed of 7A, 8-a
, 8-b... A portion where the closed magnetic circuit portion of the second core 5 is wound, 9.9'... An electrostatic shield plate wound along the outer periphery of the second core 7, 10 . . . Electrostatic shield plate inserted between the windings, 20a, 20b . . . Y-shaped core portion. Agent Patent attorney Akio Namiki Agent Patent attorney Kiyoshi Matsuzaki MI diagram ((L) □□□□---( ) Figure 3 (υ) (b) (C) (d) Figure 3 (child) ) (1n Figure 4 (艮) Cshi) Koshirae 5 Figure 6 (α) (b) ((:) rn7 Figure (α)

Claims (1)

【特許請求の範囲】 1)低周波高実効透磁率磁性材料により閉磁路を形成し
て成る第1のコアと、該コアの1次側に同心的に係合す
る第1の係合部を備えた第1の閉磁路および該第1の閉
磁路と一部を共用する第2の閉磁路を高周波高実効透磁
率磁性材料で形成して成る第2のコアと、前記第1のコ
アの2次側に同心的に係合する第2の保合部を備えた第
3の閉磁路および該第3の閉磁路と一部を共用する第4
の閉磁路を高周波高実効透磁率磁性材料で形成して成る
第3のコアと、を有し、ノーマルモードの電流に対して
互いに逆極性の磁束を発生するように前記第2の閉磁路
にそれぞれ捲回された第1および第2の各巻線の各一端
を、前記第1の閉磁路における第1の保合部に捲回した
1次巻線の各一端にそれぞれ接続し、同様に前記第4の
閉磁路にそれぞれ捲回された第3および第4の各巻線の
各一端を、前記第3の閉磁路における第2の保合部に捲
回した2次巻線の各一端にそれぞれ接続して成ることを
特徴とする雑音防護トランス。 2)低周波高実効透磁率磁性材料により閉磁路を形成し
て成る第1のコアと、該コアの1次側に同心的に係合す
る第1の係合部を備えた第1の閉磁路および該第1の閉
磁路と一部を共用する第2の閉磁路を高周波高実効透磁
率磁性材料で形成して成る第2のコアと、前記第1のコ
アの2次側に同心的に係合する第2の係合部を備えた第
3の閉磁路および該第3の閉磁路と一部を共用する第4
の閉磁路を高周波高実効透磁率磁性材料で形成して成る
第3のコアと、を有し、ノーマルモードの電流に対して
互いに逆極性の磁束を発生するように前記第2の閉磁路
にそれぞれ捲回された第1および第2の各巻線の各一端
を、前記第1の閉磁路における第1の係合部に捲回した
1次巻線の各一端にそれぞれ接続し、同様に前記第4の
閉磁路にそれぞれ捲回された第3および第4の各巻線の
各一端を、前記第3の閉磁路における第2の保合部に捲
回した2次巻線の各一端にそれぞれ接続して成る雑音防
護トランスにおいて、前記第2のコアにおける第1の閉
磁路と、前記第3のコアにおける第3の閉磁路と、の何
れか一方または双方の外周に沿って静電シールドを施し
たことを特徴とする雑音防護トランス。
[Claims] 1) A first core formed of a low frequency, high effective permeability magnetic material forming a closed magnetic path, and a first engaging portion that concentrically engages with the primary side of the core. a second core comprising a first closed magnetic path and a second closed magnetic path that shares a part with the first closed magnetic path, made of a high frequency, high effective permeability magnetic material; a third closed magnetic path including a second retaining portion that concentrically engages with the secondary side; and a fourth closed magnetic path that shares a portion with the third closed magnetic path.
a third core formed of a high-frequency, high-effective magnetic permeability magnetic material, and a third core formed of a magnetic material with a high frequency and high effective permeability, and the second closed magnetic path is configured to generate magnetic fluxes of opposite polarity with respect to the normal mode current. One end of each of the wound first and second windings is connected to one end of the primary winding wound to the first retaining part in the first closed magnetic circuit, and similarly One end of each of the third and fourth windings wound around the fourth closed magnetic path is connected to one end of each of the secondary windings wound around the second retaining part of the third closed magnetic path. A noise protection transformer characterized by being connected to each other. 2) A first closed magnetic core comprising a first core formed of a closed magnetic path made of a low frequency, high effective permeability magnetic material, and a first engaging portion concentrically engaged with the primary side of the core. a second core formed of a high frequency, high effective permeability magnetic material, and a second closed magnetic path that shares a portion with the first closed magnetic path; and a second core that is concentric with the secondary side of the first core. a third closed magnetic path including a second engaging portion that engages with the third closed magnetic path; and a fourth closed magnetic path that shares a portion with the third closed magnetic path.
a third core formed of a high-frequency, high-effective magnetic permeability magnetic material, and a third core formed of a magnetic material with a high frequency and high effective permeability, and the second closed magnetic path is configured to generate magnetic fluxes of opposite polarity with respect to the normal mode current. One end of each of the wound first and second windings is connected to one end of the primary winding wound around the first engaging part in the first closed magnetic circuit, and similarly One end of each of the third and fourth windings wound around the fourth closed magnetic path is connected to one end of each of the secondary windings wound around the second retaining part of the third closed magnetic path. In the noise protection transformer, an electrostatic shield is provided along the outer periphery of one or both of the first closed magnetic path in the second core and the third closed magnetic path in the third core. A noise protection transformer characterized by the following features:
JP59082038A 1984-04-25 1984-04-25 Noise protection transformer Pending JPS60226110A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP59082038A JPS60226110A (en) 1984-04-25 1984-04-25 Noise protection transformer

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP59082038A JPS60226110A (en) 1984-04-25 1984-04-25 Noise protection transformer

Publications (1)

Publication Number Publication Date
JPS60226110A true JPS60226110A (en) 1985-11-11

Family

ID=13763347

Family Applications (1)

Application Number Title Priority Date Filing Date
JP59082038A Pending JPS60226110A (en) 1984-04-25 1984-04-25 Noise protection transformer

Country Status (1)

Country Link
JP (1) JPS60226110A (en)

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