JPS611261A - Noise blocking transformer - Google Patents
Noise blocking transformerInfo
- Publication number
- JPS611261A JPS611261A JP12004184A JP12004184A JPS611261A JP S611261 A JPS611261 A JP S611261A JP 12004184 A JP12004184 A JP 12004184A JP 12004184 A JP12004184 A JP 12004184A JP S611261 A JPS611261 A JP S611261A
- Authority
- JP
- Japan
- Prior art keywords
- core
- magnetic
- mode noise
- input
- 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
Links
Classifications
-
- H—ELECTRICITY
- H02—GENERATION; CONVERSION OR DISTRIBUTION OF ELECTRIC POWER
- H02M—APPARATUS FOR CONVERSION BETWEEN AC AND AC, BETWEEN AC AND DC, OR BETWEEN DC AND DC, AND FOR USE WITH MAINS OR SIMILAR POWER SUPPLY SYSTEMS; CONVERSION OF DC OR AC INPUT POWER INTO SURGE OUTPUT POWER; CONTROL OR REGULATION THEREOF
- H02M1/00—Details of apparatus for conversion
- H02M1/12—Arrangements for reducing harmonics from AC input or output
Landscapes
- Engineering & Computer Science (AREA)
- Power Engineering (AREA)
- Power Conversion In General (AREA)
Abstract
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及び
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 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 transformer capable of
従来この種の雑音阻止トランスとしては、第7図に示す
ような構成のものが用いられている。すなわち入力端1
,1から同相で入力するコモンモードノイズNcに対し
ては、1次巻tlJ3と2次巻線3とを捲回したコア7
に、1次巻Ia3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4,5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
ズの阻止をはかつていた。Conventionally, as this type of noise blocking transformer, one having a configuration as shown in FIG. 7 has been used. In other words, input end 1
, 1, the core 7 is wound with the primary winding tlJ3 and the secondary winding 3.
In addition, windings 4 and 5 are provided in series with the primary winding Ia3 so that magnetic fluxes in the same direction are generated in response to the common mode noise Nc. It used to be possible to block mode noise.
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、図中の6に示すように、巻線
30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Nnを短絡させ、ノーマルモードノイズの阻
止をはかつていた。In addition, for the normal mode noise Nn that is input from the input terminals 1 and 1 in opposite phase, as shown in 6 in the figure, a capacitor C1 is inserted between the 30 winding lines to short-circuit the normal mode noise Nn. It was previously used to prevent normal mode noise.
しかしこのような構成のものでは、1次巻線3に流れる
本来の低周波信号電流による磁束を効率よく2次側巻線
3に鎖交させるよう設計されたコア7にコモンモードノ
イズ阻止用巻線4,5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はこれ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と
いう欠点があった。However, in this configuration, a common mode noise blocking winding is installed in the core 7, which is designed to efficiently link the magnetic flux due to the original low-frequency signal current flowing through the primary winding 3 to the secondary winding 3. Since the wires 4 and 5 are wound, the inductance does not increase when high-frequency common mode noise is input, resulting in a disadvantage that sufficient noise blocking characteristics cannot be obtained.
また高周波のノーマルモードノイズNce[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などの欠点があった。In addition, in order to stop high-frequency normal mode noise Nce, a large capacitance C1 is required, and components other than the winding and core are required.
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、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トランスを提
供することにある。The present invention has been made to eliminate the drawbacks of the prior art as described above, and therefore, an object of the present invention is to provide stable and sufficient noise suppression without requiring any components other than windings and cores. It is an object of the present invention to provide a noise-blocking transformer that allows characteristics to be obtained.
本発明による雑音阻止トランスは、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次側の成る部分に同心的に係合する係合部を備
えた閉磁路を第1の高周波高実効透磁率磁性材料で形成
して成る巣2のコアと、前記第1のコアの1次側の他の
部分に係合する係合部を備えた閉磁路を第2の高周波高
実効透磁率磁性材料で形成して成る筒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3のコアと拍1のコアの係合部
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のコアと第2のコアの同心的係合部に捲回
された1次巻線の各一端に接続すると共に、前記1次巻
線は前記第2のコアを形成する第1の高周波高実効透磁
率磁性材料でおおわれるようにし、
前記第1のコアの2次側にも、上記と同様に各コアなら
びに巻線を2次側としてほどこして成ることを特徴とし
ている。The noise-blocking transformer according to the present invention includes a first core formed of a low-frequency, high-effective magnetic permeability magnetic material forming a closed magnetic path, and an engaging portion that concentrically engages with a portion of the primary side of the core. A closed magnetic core comprising a core of the nest 2 formed of a first high-frequency, high-effective magnetic permeability magnetic material, and an engaging portion that engages with another portion of the primary side of the first core. and a core of the cylinder 3 formed of a second high-frequency, high-effective permeability magnetic material, and the third core and the third core are configured to generate magnetic fluxes of opposite polarity with respect to normal mode current. One end of each of the first and second windings respectively wound around the engaging portion of the first core and the primary winding wound around the concentric engaging portion of the first core and the second core. connected to one end of each of the windings, the primary winding being covered with a first high frequency, high effective permeability magnetic material forming the second core; Similarly to the above, this is characterized in that each core and winding are applied as a secondary side.
次に図を参照して本発明の一実施例を説明する。 Next, an embodiment of the present invention will be described with reference to the drawings.
第1図は本発明の一実施例の回路構成を示す回路図であ
り、第2図はその組立断面の説明図である。これらの図
において、8及び9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
を塗着した磁性テープなどの磁性材キ嚇からなるそれぞ
れ第2及び第3のコアである。FIG. 1 is a circuit diagram showing the circuit configuration of an embodiment of the present invention, and FIG. 2 is an explanatory diagram of an assembled cross section thereof. In these figures, 8 and 9 are second and third plates, respectively, made of a plate-like material such as a magnetic dust core, which has a small drop in effective magnetic permeability up to a high frequency range, or a magnetic material such as a magnetic tape coated with the plate-shaped plate. This is the third core.
巻線4,5はコア9の環状閉磁路の一部分とコア7の一
部分とに共通に巻きつけてあり、その巻方向は入力端1
,1からのコモンモードノイズに対して互いに同方向磁
束が生じるような巻方向にしである。The windings 4 and 5 are commonly wound around a part of the annular closed magnetic path of the core 9 and a part of the core 7, and the winding direction is the same as that of the input end 1.
, 1 so that magnetic fluxes in the same direction occur in response to common mode noise from the windings.
巻線3および3は、コア7の巻線4,5の施された部分
とは異なる磁路部分を中心に同軸状に配置された中空円
筒状の第2のコア8の同軸中空部分に入力端1,1から
の高周波のノーマルモードノイズに対し同方向磁束が発
生するように捲回され、883.3の外周は、少なくと
もこれら両巻線の対向面近傍または巻線3,3の外周に
沿って、その全周が第2のコア8を構成する磁性材でお
おわれている。The windings 3 and 3 are input to a coaxial hollow portion of a hollow cylindrical second core 8 that is coaxially arranged around a magnetic path portion different from the portion of the core 7 where the windings 4 and 5 are applied. It is wound so that magnetic flux in the same direction is generated in response to high-frequency normal mode noise from the ends 1, 1, and the outer periphery of 883.3 is at least near the facing surfaces of these two windings or the outer periphery of the windings 3, 3. The entire circumference thereof is covered with a magnetic material constituting the second core 8.
第3図は、本発明に用いたコアの周波数−実効透磁率特
性を示す特fil−ffであり、@1のコア7がμm、
@2のコア8がμ2、第3のコア9がμ3として示すよ
うな特性を有している。FIG. 3 is a characteristic fil-ff showing the frequency-effective magnetic permeability characteristics of the core used in the present invention, where the core 7 of @1 is μm,
The core 8 of @2 has the characteristics shown as μ2, and the third core 9 has the characteristics shown as μ3.
すなわちコア7は、低周波でμlのような高い実効透磁
率を有するため、高周波電流に対しては、磁束が通り難
く、低周波電流に対しては、磁束が今通り易い。これに
対してコア8,9はμ2.μ3のように高周波領域まで
実効透磁率特性が延びており、高周波電流に対しても磁
束が通り易いようになっている。That is, since the core 7 has a high effective magnetic permeability such as μl at low frequencies, it is difficult for magnetic flux to pass through the core 7 for high frequency currents, but it is easy for magnetic flux to pass through for low frequency currents. On the other hand, cores 8 and 9 have μ2. Like μ3, the effective magnetic permeability characteristic extends to the high frequency region, and magnetic flux can easily pass through even high frequency current.
第4図は、第2図に示した本発明の実施例の動作説明図
であり、(a)は高周波のコモンモートノイス、(b)
a高周波のノーマルモードノイズ、(C)ij低周波の
ノーマルモード信号電流がそれぞれ入力端より侵入した
場合にコア7.8.9に生ずる磁束の方向を示したもの
であるc以下に各図をもとにそれぞれの動作を説明する
。FIG. 4 is an explanatory diagram of the operation of the embodiment of the present invention shown in FIG. 2, in which (a) is high frequency common mode noise, (b)
(a) High frequency normal mode noise and (C) ij low frequency normal mode signal current respectively enter the core 7.8.9 from the input terminal. The operation of each will be explained below.
まず(a)で入力端より高周波のコモンモードノイズN
cが入力したとき1巻線4,5によってコア9の閉磁路
内に生じる磁束φc1は、互いに同方向に発生するため
強め合い、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。First, in (a), there is a high frequency common mode noise N from the input terminal.
When c is input, the magnetic fluxes φc1 generated in the closed magnetic circuit of the core 9 by the first windings 4 and 5 are generated in the same direction and therefore strengthen each other, acting as a large inductance against the common mode noise Nc.
これに対し巻線3に流れるコモンモードノイズNcによ
ってコア7及び8に生じる磁束φc2およびφc3は、
同相電流のため互いに反対方向に生じて打ち消し合い、
2次側には何ら影響を及ぼさない。On the other hand, the magnetic fluxes φc2 and φc3 generated in the cores 7 and 8 due to the common mode noise Nc flowing in the winding 3 are
Because of the common mode currents, they occur in opposite directions and cancel each other out,
It has no effect on the secondary side.
なおコア7内に生じる磁束φc2け、実際には第3図か
らも明らかなようにコア7の実効透磁率が高周波域で小
さいためきわめて小さい値である。Note that the magnetic flux φc2 generated in the core 7 is actually a very small value because the effective magnetic permeability of the core 7 is small in the high frequency range, as is clear from FIG.
次に(b)で入力側より高周波のノーマルモードノイズ
Nnが入力したとき、巻線4,5によってコア9の閉磁
路内に生じる磁束φnlは、(a)とは逆に互いに反対
方向となって打ち消し合うため、巻線4.5及びコア9
部分は、/−マルモードノイズNnに対し何ら影響を与
えない。Next, in (b), when high-frequency normal mode noise Nn is input from the input side, the magnetic flux φnl generated in the closed magnetic path of the core 9 by the windings 4 and 5 is in opposite directions, contrary to (a). winding 4.5 and core 9
The portion has no effect on the /-malmode noise Nn.
これに対し1次巻線3によってコア7及び8に生じる磁
束をそれぞれφn2及びφn3とすると、これらのうち
前者は(a)の場合と同様にコア7の実効透磁率が小さ
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φn3はコア8の閉磁路内を流れる短
絡磁束となりノーマルモードノイズNnに対して大きな
インダクタンスとして作用する。On the other hand, if the magnetic fluxes generated in the cores 7 and 8 by the primary winding 3 are φn2 and φn3, respectively, the former is hardly generated because the effective magnetic permeability of the core 7 is small, as in the case (a). , there is almost no influence on the secondary winding 3 side. However, φn3 becomes a short-circuit magnetic flux flowing in the closed magnetic circuit of the core 8, and acts as a large inductance against the normal mode noise Nn.
これに対して(C)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4,5によるコア8
の閉磁路内の磁束は、(b)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巻線4.5及びコア8の
部分は低周波電流Snに対しては何らの影響も与えない
。−万巻1$3によってコア7及びコア8内に生じる磁
束をそれぞれφs2及びφs3とすると、これらのうち
前者は、コア7の低周波における実効透磁率がコア8の
それにくらべはるかに太きいため、低周波電流Snによ
る磁束の大部分はφS2となってコア7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導電圧が
発生する。On the other hand, when low frequency current (normal mode) Sn is input from the input side in (C), the core 8 due to windings 4 and 5
As in the case of (b), the magnetic fluxes in the closed magnetic circuit cancel each other in opposite directions, so the winding 4.5 and core 8 have no effect on the low frequency current Sn. . - Let φs2 and φs3 be the magnetic fluxes generated in core 7 and core 8 due to 10,000 turns of 1$3, respectively. Of these, the former is because the effective magnetic permeability at low frequencies of core 7 is much larger than that of core 8. Most of the magnetic flux due to the low frequency current Sn becomes φS2 and flows through the core 7, 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周波数により実効透磁率の異なる
3種類のコアとその巻線の巻き方の方向を工夫し、高周
波のコモン、ノーマル両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。特に前
者に対しては低周波高実効透磁率コアと高周波高実効透
磁率コアの両方によるインダクタンス2を利用してノイ
ズ阻止特性の広帯域化をはかつである。In this way, in the present invention, three types of cores with different effective magnetic permeabilities depending on the frequency and the winding direction of their windings are devised so that each acts as a large inductance against both high-frequency common and normal noise. . Particularly for the former, the inductance 2 of both the low frequency high effective magnetic permeability core and the high frequency high effective magnetic permeability core is utilized to widen the noise blocking characteristic.
また、1次側および2次側とも同一構造にしであるため
、入出力双方向から侵入するノイズを阻止できる。Further, since both the primary side and the secondary side have the same structure, it is possible to prevent noise from entering from both input and output directions.
第5図は本発明の他の実施例の組立断面の説明図である
。すなわち同図に示した実施列は、第2図に示した実施
例において、コア8.9(8゜9′)の外周を静電シー
ルド板10(10’)でおおったものである。FIG. 5 is an explanatory diagram of an assembled cross section of another embodiment of the present invention. That is, the embodiment row shown in the same figure is the embodiment shown in FIG. 2 in which the outer periphery of the core 8.9 (8°9') is covered with an electrostatic shield plate 10 (10').
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伝達する。このような輻射
電磁波の伝達を阻止するため、第5図の実施例では巻線
3.3の外周部にあるコアとその更に外周に巻いた静電
シールド板10とによってその吸収をはかつている。If the impedance of the input winding is large, high-frequency noise, especially common mode noise, from the input end is transmitted from there to the adjacent winding in the form of electromagnetic radiation. In order to prevent the transmission of such radiated electromagnetic waves, in the embodiment shown in FIG. 5, the core at the outer periphery of the winding 3.3 and the electrostatic shield plate 10 wound around the outer periphery of the core absorb the electromagnetic waves. .
第6図は本発明の更に他の実施例の組立断面の説明図で
ある。FIG. 6 is an explanatory diagram of an assembled cross section of still another embodiment of the present invention.
同図に示す実施例は、低周波で高い実効透磁率を有する
コア7として、ヨの字形の磁性材を2個互いに突き合せ
たもの(突き合せ面を8で示す)を用い、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、1
次側巻線、2次側巻線を完全に分離し、コア8,8の外
周を静電シールド板10でおおったものである。The embodiment shown in the figure uses two V-shaped magnetic materials butted against each other (the butted surfaces are shown as 8) as the core 7 having high effective magnetic permeability at low frequencies, and the primary side From 2
In order to prevent electromagnetic wave radiation to the next side or vice versa, 1
The next winding and the secondary winding are completely separated, and the outer periphery of the cores 8, 8 is covered with an electrostatic shield plate 10.
なお、以上述べた諸実施例において、入来する高周波o
コモンモードノイズおよびノーマルモードノイズの周波
数が同じ場合には、μ2=μ3として第2および第3の
コア8,9を同一の磁性材で構成するものとしてよいこ
とはいうまでもない。In addition, in the embodiments described above, the incoming high frequency o
It goes without saying that if the frequencies of common mode noise and normal mode noise are the same, μ2=μ3 and the second and third cores 8 and 9 may be made of the same magnetic material.
以上説明したように本発明れ、低周波で高実効透磁率を
有する第1のコアの異なる磁路部分に高周波で高実効透
磁率を有する第2および第3のコアの一部を配置し、こ
れらの共通磁路部分にノイズ阻止用e線を施したもので
、これらによって入83力端双方向から侵入する高周波
のコモンノーマルモードノイズを阻止できる。As explained above, according to the present invention, parts of the second and third cores having high effective magnetic permeability at high frequencies are arranged in different magnetic path portions of the first core having high effective magnetic permeability at low frequencies, These common magnetic path portions are provided with noise blocking e-wires, which can block high frequency common normal mode noise that enters from both sides of the input terminal.
特に、高周波のコモンモートノイスに対して社、鶴1お
よび第3のコアそれぞれの有する実効透磁率によるそれ
ぞれのインダクタンスを利用しており、ノイズ阻止特性
の広帯域化がはかれるという利点がある。Particularly, in response to high frequency common mode noise, the respective inductances due to the effective magnetic permeability of the first core, the third core, and the third core are utilized, which has the advantage of widening the noise blocking characteristic.
第1図祉本発明の一実施例の回路構成を示す回路図、I
II!2115はその組立断面の説明図、嬉3図は本発
明において用いるコアの周波数−実効透磁率特性を示す
特性図、第4図は本発明の一実施例の動作説明図、#!
5図状本状本発明の実ms’o組立断面の説明図、@6
図は本発明の別の実施例の組立断面の説明図、第7図は
従来の雑音阻止トランスの構成例を示す回路図、である
。
符号説明
1.1・・・・・・入力端、2,2・・・・・・出力端
、3・・・・・・1次巻線、3・・・・・・2凍巻線、
8,9・・・・・・高周波で高い実効透磁率を有する第
2、第3のコア、7・・・・・・低周波で高い実効透磁
率を有する第1のコア、4.5・・・・・・2次側の第
L @2のコアに共通に巻いた巻線、9・・・・・・#
!2のコア8、第3のコア9の外周に沿って巻きつけた
静電シールド板、10・・・・・・第2のコア8の外周
に沿って巻きつけた静電シールド板
代理人 弁理士 並 木 昭 夫
代理人 弁理士 松 崎 清
第1図
9′5
Il¥ 2 図
第 4 図
(α)
第 4 図
(A)
第!5図FIG. 1 is a circuit diagram showing the circuit configuration of an embodiment of the present invention, I
II! 2115 is an explanatory diagram of its assembled cross section, Figure 3 is a characteristic diagram showing the frequency-effective magnetic permeability characteristics of the core used in the present invention, and Figure 4 is an explanatory diagram of the operation of an embodiment of the present invention.
5 Figure-shaped book-shape An explanatory diagram of the actual ms'o assembled cross section of the present invention, @6
The figure is an explanatory diagram of an assembled cross section of another embodiment of the present invention, and FIG. 7 is a circuit diagram showing an example of the configuration of a conventional noise rejection transformer. Symbol explanation 1.1...Input end, 2,2...Output end, 3...Primary winding, 3...2 freezing winding,
8, 9... Second and third cores having high effective magnetic permeability at high frequencies, 7... First core having high effective magnetic permeability at low frequencies, 4.5. ...Winding commonly wound around the Lth @2 core on the secondary side, 9...#
! Electrostatic shielding plate wrapped along the outer periphery of the second core 8, third core 9, 10... Electrostatic shielding plate wrapped along the outer periphery of the second core 8. Patent attorney. Akio Namiki Agent Patent Attorney Kiyoshi Matsuzaki Figure 1 9'5 Il¥ 2 Figure 4 (α) Figure 4 (A) Figure 4! Figure 5
Claims (1)
て成る第1のコアと、該コアの1次側の或る部分に同心
的に係合する係合部を備えた閉磁路を第1の高周波高実
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1次側の他の部分に係合する係合部を備えた
閉磁路を第2の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3のコ
アと第1のコアの係合部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のコアと第2のコ
アの同心的係合部に捲回された1次巻線の各一端に接続
すると共に、前記1次巻線は前記第2のコアを形成する
第1の高周波高実効透磁率磁性材料でおおわれるように
し、前記第1のコアの2次側にも、上記と同様に各コア
ならびに巻線を2次側としてほどこして成ることを特徴
とする雑音阻止トランス。1) A first core formed of a low frequency, high effective permeability magnetic material forming a closed magnetic path, and a closed magnetic path comprising an engaging portion that concentrically engages a certain portion of the primary side of the core. A closed magnetic circuit comprising a second core made of a first high-frequency, high-effective permeability magnetic material and an engaging portion that engages with another portion of the primary side of the first core. a third core made of a high-frequency, high-effective magnetic permeability magnetic material; One end of each of the first and second windings wound around the engaging portion, respectively, and one end of each of the primary winding wound around the concentric engaging portion of the first core and the second core. and the primary winding is covered with a first high frequency, high effective permeability magnetic material forming the second core, and the secondary side of the first core is also covered with a first high frequency, high effective permeability magnetic material forming the second core. A noise-blocking transformer characterized in that each core and winding are applied as a secondary side to the transformer.
Priority Applications (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP12004184A JPS611261A (en) | 1984-06-13 | 1984-06-13 | Noise blocking transformer |
Applications Claiming Priority (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP12004184A JPS611261A (en) | 1984-06-13 | 1984-06-13 | Noise blocking transformer |
Publications (1)
Publication Number | Publication Date |
---|---|
JPS611261A true JPS611261A (en) | 1986-01-07 |
Family
ID=14776432
Family Applications (1)
Application Number | Title | Priority Date | Filing Date |
---|---|---|---|
JP12004184A Pending JPS611261A (en) | 1984-06-13 | 1984-06-13 | Noise blocking transformer |
Country Status (1)
Country | Link |
---|---|
JP (1) | JPS611261A (en) |
Cited By (1)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
US6203348B1 (en) | 1998-07-06 | 2001-03-20 | Yazaki Corporation | Waterproof connector and waterproof rubber member |
-
1984
- 1984-06-13 JP JP12004184A patent/JPS611261A/en active Pending
Cited By (1)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
US6203348B1 (en) | 1998-07-06 | 2001-03-20 | Yazaki Corporation | Waterproof connector and waterproof rubber member |
Similar Documents
Publication | Publication Date | Title |
---|---|---|
US2553324A (en) | Wide band audio and video transformer | |
US5783984A (en) | Method and means for combining a transformer and inductor on a single core structure | |
US10559415B2 (en) | Common mode filter capable of balancing induced inductance and distributed capacitance | |
US2406045A (en) | Inductance device | |
US5422619A (en) | Common mode choke coil | |
US20190272935A1 (en) | Common mode choke for eliminating electrostatic interference | |
US4689592A (en) | Combined transformer and inductor | |
US3458843A (en) | Broadband shielded transformers | |
US2463778A (en) | Magnetic shielding | |
JPH04317307A (en) | Transformer | |
JPS611261A (en) | Noise blocking transformer | |
US4074210A (en) | Distribution type delay line | |
US4453131A (en) | Transformer coupled amplifier circuit | |
US3231837A (en) | All-pass transformer coupling network utilizing high frequency and low frequency transformers in parallel connection | |
US4160962A (en) | Dual section distributed parameter delay-line | |
JPH0410659Y2 (en) | ||
JPS5941297B2 (en) | power transformer | |
JPS61263105A (en) | Composite type common mode choke coil | |
JPS5822579A (en) | Switching power source | |
JPS611260A (en) | Noise protecting composite transformer | |
JPH0291905A (en) | Inductor for noise filter | |
US5121088A (en) | Frequency response equalizer | |
JPH0233390Y2 (en) | ||
JPS6347909A (en) | Shell type common mode choke coil | |
US2096801A (en) | Power transformer |