JPH088186B2 - Current transformer - Google Patents

Current transformer

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Publication number
JPH088186B2
JPH088186B2 JP63328443A JP32844388A JPH088186B2 JP H088186 B2 JPH088186 B2 JP H088186B2 JP 63328443 A JP63328443 A JP 63328443A JP 32844388 A JP32844388 A JP 32844388A JP H088186 B2 JPH088186 B2 JP H088186B2
Authority
JP
Japan
Prior art keywords
winding
primary winding
secondary winding
current transformer
primary
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.)
Expired - Fee Related
Application number
JP63328443A
Other languages
Japanese (ja)
Other versions
JPH02174104A (en
Inventor
英雄 北川
Original Assignee
日本電気計器検定所
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Filing date
Publication date
Application filed by 日本電気計器検定所 filed Critical 日本電気計器検定所
Priority to JP63328443A priority Critical patent/JPH088186B2/en
Publication of JPH02174104A publication Critical patent/JPH02174104A/en
Publication of JPH088186B2 publication Critical patent/JPH088186B2/en
Anticipated expiration legal-status Critical
Expired - Fee Related legal-status Critical Current

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Description

【発明の詳細な説明】 〔産業上の利用分野〕 本発明は変流器に関するものである。DETAILED DESCRIPTION OF THE INVENTION [Field of Industrial Application] The present invention relates to a current transformer.

〔従来の技術〕[Conventional technology]

近時では電力計においても変流器(CT)の出力を電子
回路で処理する方式のものが開発されている。この電子
回路において通常使用する電流は数mA程度である。その
ため、変流器においてこのような数mA程度に電流を変成
して電子回路に供給する必要があり、その分、二次巻数
が増加する傾向にある。
Recently, a method of processing the output of a current transformer (CT) with an electronic circuit has also been developed for a power meter. The current normally used in this electronic circuit is about several mA. Therefore, in the current transformer, it is necessary to transform the current to about several mA and supply it to the electronic circuit, and the number of secondary turns tends to increase accordingly.

例えば、測定電流が数Aオーダーであれば、二次巻線
の巻数が1000回程度で良いが、数mAオーダーともなる
と、20000回以上も二次巻線を巻く必要があり、少ない
巻数で変成比を大きくする方法の出現が要望されてい
る。
For example, if the measured current is on the order of several A, the number of turns of the secondary winding may be about 1000, but if it is on the order of several mA, it is necessary to wind the secondary winding more than 20000 times, and the number of turns is small. The advent of methods to increase the ratio is desired.

従来、このような技術として次のようなものがあっ
た。
Conventionally, there are the following as such techniques.

まず、第11図において、1は棒形導体からなる一次巻
線、2は二次巻線であり、一次巻線1を構成する導体に
は、この導体よりも小さな抵抗の導体からなる分流回路
3が並列に接続されている。
First, in FIG. 11, 1 is a primary winding made of a rod-shaped conductor, 2 is a secondary winding, and a conductor forming the primary winding 1 has a shunt circuit having a resistance smaller than that of the conductor. 3 are connected in parallel.

これにより、このものは、一次巻線1に供給する電流
の一部を分流回路3に流し、その分、一次巻線1に流す
電流を小さくし、変成比を稼ごうというものである。
As a result, in this device, a part of the current supplied to the primary winding 1 is made to flow in the shunt circuit 3, and the current made to flow in the primary winding 1 is reduced by that amount, and the transformation ratio is increased.

しかしながら、このものは、一次巻線1を構成する導
体のインダクタンス成分が大きいことが原因で位相角が
大きく、また抵抗温度係数の影響が大きいという欠点が
ある。
However, this one has the drawback that the phase angle is large due to the large inductance component of the conductor forming the primary winding 1, and that the temperature coefficient of resistance has a large influence.

また、第12図において、4は一次鉄心、5はこの一次
鉄心4に装着されている一次巻線、6は二次鉄心、7は
この二次鉄心6に装着されている二次巻線である。一次
鉄心4は円筒状のもので、その中空部内に一次鉄心によ
る磁界が発生している。二次鉄心6は、棒状のもので、
この一次鉄心4の中空部内に挿入され、これにより二次
巻線7が一次巻線5による磁界内に配置される。
Further, in FIG. 12, 4 is a primary core, 5 is a primary winding mounted on the primary core 4, 6 is a secondary core, and 7 is a secondary winding mounted on the secondary core 6. is there. The primary iron core 4 has a cylindrical shape, and a magnetic field is generated in the hollow portion by the primary iron core. The secondary iron core 6 has a rod shape,
It is inserted into the hollow portion of the primary core 4 so that the secondary winding 7 is arranged in the magnetic field of the primary winding 5.

二次鉄心6は二次巻線7の軸心が一次巻線5の軸心に
対して角度αをなすように一次鉄心4に保持されてい
る。
The secondary core 6 is held by the primary core 4 so that the axis of the secondary winding 7 forms an angle α with the axis of the primary winding 5.

これにより、このものは、一次巻線5と二次巻線7と
を同軸に配置する場合に比べて(1/cosα)だけ変成比
を大きくしようというものである。
As a result, this is intended to increase the transformation ratio by (1 / cos α) as compared with the case where the primary winding 5 and the secondary winding 7 are coaxially arranged.

しかしながら、このものは、正確な測定のためには、
その傾斜角度を正確にして二次巻線7を固定しなければ
ならず、そのため二次鉄心6やボビンを固定する構造が
複雑になると言う問題がある。
However, this is
There is a problem that the secondary winding 7 must be fixed with the inclination angle being correct, which complicates the structure for fixing the secondary iron core 6 and the bobbin.

なお、図示はしないが変流器をカスケードに接続し
て、小さな二次電流を得る方法もあるが、この場合、一
断目の二次電流は大きく、電子回路で補償することがで
きないため、誤差が大きくなるという問題があり、一つ
の変流器で大きな変成比を得る方が望ましい。
Although not shown, there is also a method of connecting a current transformer in a cascade to obtain a small secondary current, but in this case, the secondary current at the first break is large and cannot be compensated by an electronic circuit. There is a problem that the error becomes large, and it is desirable to obtain a large transformation ratio with one current transformer.

〔発明が解決しようとする課題〕[Problems to be Solved by the Invention]

上述したように、従来の変流器にあっては、巻数比よ
り大きな変成比を得るにあたり、位相角、温度係数、巻
線の固定構造等が原因で安定した変成比が得られないと
いう問題がある。
As described above, in the conventional current transformer, when obtaining a transformation ratio larger than the turns ratio, a stable transformation ratio cannot be obtained due to the phase angle, temperature coefficient, winding fixing structure, etc. There is.

本発明は、このような従来技術の有する問題点に鑑み
てなされたもので、その目的とするところは、巻数比よ
り大きな変成比を安定して得ることができる変流器を提
供することにある。
The present invention has been made in view of the above problems of the prior art, and an object thereof is to provide a current transformer that can stably obtain a transformation ratio larger than the turns ratio. is there.

〔課題を解決するための手段〕[Means for solving the problem]

本発明の変流器は鉄心の前記一次巻線装着部に空隙を
設け、この一次巻線を、二次巻線にその磁束を鎖交させ
る有効面積が二次巻線の面積よりも小さくなるようにそ
の空隙に挿入したものである。
In the current transformer of the present invention, an air gap is provided in the primary winding mounting portion of the iron core, and the effective area for interlinking the magnetic flux with the primary winding is smaller than the area of the secondary winding. It was inserted in the space like this.

〔作用〕[Action]

二次巻線に鎖交する磁束の量は、一次巻線の起磁力、
及び一次巻線と二次巻線との面積比に依存する。
The amount of magnetic flux linked to the secondary winding is the magnetomotive force of the primary winding,
And the area ratio between the primary winding and the secondary winding.

本発明によれば、鉄心の一次巻線装着部に空隙を設
け、一次巻線をこの空隙に挿入するようにして、その磁
束を二次巻線に鎖交させる有効面積を二次巻線の面積よ
りも小さくなるように鉄心に装着したので、巻数比より
も大きな変成比を得ることができる。
According to the present invention, an air gap is provided in the primary winding mounting portion of the iron core, and the primary winding is inserted into this air gap so that the effective area for interlinking the magnetic flux with the secondary winding is Since it was mounted on the iron core so as to be smaller than the area, it is possible to obtain a transformation ratio larger than the turns ratio.

このように本発明は一次巻線と二次巻線との面積比を
調整することにより変成比を調節できる構造となってい
るので、インダクタンス成分の影響が小さく、また抵抗
温度係数の問題がなく、しかも空隙にスペーサ等を設け
ることで一次巻線は容易に鉄心へ固定することができ、
安定した状態で巻線比よりも大きな変成比が得られるこ
ととなる。
As described above, the present invention has a structure in which the transformation ratio can be adjusted by adjusting the area ratio between the primary winding and the secondary winding, so that the influence of the inductance component is small and there is no problem of the temperature coefficient of resistance. Moreover, the primary winding can be easily fixed to the iron core by providing a spacer or the like in the gap,
In a stable state, a transformation ratio larger than the winding ratio can be obtained.

〔実施例〕〔Example〕

以下に本発明の実施例について図面を参照しつつ説明
する。
Embodiments of the present invention will be described below with reference to the drawings.

第1図は本発明の第1実施例に係る変流器の正面図、
第2図はそのII−II線に沿う断面図、第3図はIII−III
線に沿う断面図である。なお、第3図中、Uは上向きの
磁束の方向を表わす記号である。
FIG. 1 is a front view of a current transformer according to a first embodiment of the present invention,
2 is a sectional view taken along line II-II, and FIG. 3 is III-III.
It is sectional drawing which follows the line. In FIG. 3, U is a symbol indicating the direction of upward magnetic flux.

これらの図において、8はMTコアからなる鉄心、11は
この鉄心8に装着されている一次巻線12は同じく二次巻
線である。
In these figures, 8 is an iron core made of an MT core, 11 is a primary winding 12 mounted on the iron core 8 and is a secondary winding.

鉄心8はM形部9とT形部10とからなり、これらM形
部9及びT形部10はその中心部において凸出し互いに対
向する部分が二次巻線装着部13,14とされている。二次
巻線12はこれら二次巻線装着部13,14に全巻数の半部ず
つに分けられて図示を省略するボビンを介して巻き付け
られている。
The iron core 8 is composed of an M-shaped portion 9 and a T-shaped portion 10, and the M-shaped portion 9 and the T-shaped portion 10 project at their central portions and are opposed to each other as secondary winding mounting portions 13 and 14. There is. The secondary winding 12 is divided into half parts of the total number of turns around the secondary winding mounting parts 13 and 14 and wound around bobbins (not shown).

二次巻線装着部13と二次巻線装着部14との間は一次巻
線11の装着部とされ、この装着部は空隙15により構成さ
れている。この空隙15にはスペーサ16が挿着固定されて
おり、このスペーサ16にはその前後方向中心部において
一方の側部から他方の側部に貫通するワイヤ挿通孔17が
設けられている。
A space between the secondary winding mounting portion 13 and the secondary winding mounting portion 14 is a mounting portion for the primary winding 11, and this mounting portion is constituted by a gap 15. A spacer 16 is inserted and fixed in the void 15, and a wire insertion hole 17 penetrating from one side portion to the other side portion is provided in the spacer 16 at the center portion in the front-rear direction.

一次巻線11は、一本のワイヤからなっておりこれがス
ペーサ16のワイヤ挿通孔17を通されて、その各端よりス
ペーサ16の前部に導かれるようにして該スペーサ16の半
分の部分に巻き付けられることにより構成される。
The primary winding 11 is composed of a single wire, which is passed through the wire insertion hole 17 of the spacer 16 and guided to the front portion of the spacer 16 from each end thereof so that the half portion of the spacer 16 is covered. It is composed by being wrapped.

これにより、空隙15における一次巻線11が通る箇所を
境にして一方の側と他方の側とで発生する磁束が反対向
きになり、空隙15の各側の面積の差分(有効面積)が二
次巻線12の鎖交磁束となって、巻数比より大きな変成比
が得られることとなる。
As a result, the magnetic fluxes generated on one side and the other side of the gap 15 where the primary winding 11 passes are the opposite directions, and the difference (effective area) between the areas on each side of the gap 15 is two. The interlinkage magnetic flux of the next winding 12 is obtained, and a transformation ratio larger than the turn ratio is obtained.

なお、スペーサ16は二次巻線12用のボビンと一体にし
ても良い。
The spacer 16 may be integrated with the bobbin for the secondary winding 12.

第4図は本発明の第2実施例の係る変流器の正面図、
第5図は第4図のV−V線に沿う断面図、第6図は第4
図のVI−VI線に沿う断面図である。なお、第6図中、U
は上向きの、Dは下向きの、それぞれ磁束の方向を表わ
す記号である。
FIG. 4 is a front view of a current transformer according to a second embodiment of the present invention,
FIG. 5 is a sectional view taken along the line VV of FIG. 4, and FIG.
It is sectional drawing which follows the VI-VI line of a figure. In FIG. 6, U
Is a symbol indicating upward and D is a symbol indicating downward, respectively.

これらの図において、この第2実施例の特徴はその一
次巻線11の構成と、これに伴うスペーサ16の構成にあ
る。
In these drawings, the feature of the second embodiment lies in the structure of the primary winding 11 and the structure of the spacer 16 associated therewith.

すなわち、一次巻線11は2つの巻線部11A11Bからな
り、これらの巻線部11A,11Bは第6図に示すように互い
に反対方向の磁束を発生するようにスペーサ16に巻き付
けられているしたがって、この巻線部11A,11Bは相互に
磁束を打ち消し合うため、有効面積はその巻線部11A,11
Bの面積の差に相当する。
That is, the primary winding 11 is composed of two winding portions 11A and 11B, and these winding portions 11A and 11B are wound around the spacer 16 so as to generate magnetic flux in opposite directions as shown in FIG. , The winding parts 11A and 11B cancel out the magnetic flux, so the effective area is
Equivalent to the area difference of B.

これにより、この一次巻線11から二次巻線12に鎖交す
る磁束は、巻線部11A,11Bが発生する磁束の差分とな
り、一次巻線11と二次巻線12との巻線比よりも大きな変
成比を得ることができることとなる。
As a result, the magnetic flux that links the primary winding 11 to the secondary winding 12 becomes the difference between the magnetic fluxes generated by the winding portions 11A and 11B, and the winding ratio between the primary winding 11 and the secondary winding 12 is increased. It is possible to obtain a larger metamorphic ratio.

スペーサ16には各巻線部11A,11Bの一部を挿通するた
めに2本のワイヤ挿通孔17A,17Bが前後方向に位置をず
らして設けてある。
Two wire insertion holes 17A and 17B are provided in the spacer 16 so as to insert a part of each winding portion 11A and 11B, and the positions are shifted in the front-rear direction.

尚、このような構造とする場合、第7図に示すよう
に、スペーサ16を厚肉のものとし、ワイヤ挿通孔17A,17
Bを前後方向にずらすと同時に、その厚さ方向にずらす
ことで、巻線部11A11Bとの高い電気的絶縁性が確保され
る。
In the case of such a structure, as shown in FIG. 7, the spacer 16 is thick and the wire insertion holes 17A, 17
By shifting B in the front-back direction and at the same time shifting it in the thickness direction, high electrical insulation with the winding portions 11A11B is secured.

第8図は本発明の第3実施例に係る変流器の側面図、
第9図はそのIX−IX線に沿う断面図である。
FIG. 8 is a side view of a current transformer according to a third embodiment of the present invention,
FIG. 9 is a sectional view taken along the line IX-IX.

これらの図に示すように、本発明はカットコアからな
る鉄心18を用いても良い。19,20は二次巻線12の装着部
であり、二次巻線12はこの装着部に全巻数の半分ずつに
分けられて巻き付けられている。
As shown in these figures, the present invention may use an iron core 18 made of a cut core. Numerals 19 and 20 are mounting parts for the secondary winding 12, and the secondary winding 12 is wound around the mounting part divided into half of the total number of turns.

一次巻線装着部となる空隙15は、この二次巻線装着部
19と二次巻線装着部20との間に設けられ、ここにはスペ
ーサ16が挿着されている。
The void 15 that serves as the primary winding mounting part is
It is provided between 19 and the secondary winding mounting portion 20, and the spacer 16 is inserted therein.

このスペーサ16は第1実施例のものと同じ構成であ
り、一次巻線11はこのスペーサ16にこの第1実施例のも
のと同じ構造で装着されているものである。
The spacer 16 has the same structure as that of the first embodiment, and the primary winding 11 is mounted on the spacer 16 with the same structure as that of the first embodiment.

第10図は本発明の変流器の出力誤差を補償する電子回
路であり、本発明の発明者により開発され、本願の出願
人により特許出願されているものである(特願昭63−27
6950号)。
FIG. 10 shows an electronic circuit for compensating the output error of the current transformer of the present invention, which was developed by the inventor of the present invention and applied for a patent by the applicant of the present application (Japanese Patent Application No. 63-27).
No. 6950).

この図において、21は本発明の変流器、22はその鉄
心、23は一次巻線、24は二次巻線である。
In this figure, 21 is the current transformer of the present invention, 22 is its core, 23 is a primary winding, and 24 is a secondary winding.

この二次巻線24の一端にはオペアンプ25の反転入力端
子が接続され、同他端にはオペアンプ25の非反転入力端
子が接続されている。
The inverting input terminal of the operational amplifier 25 is connected to one end of the secondary winding 24, and the non-inverting input terminal of the operational amplifier 25 is connected to the other end thereof.

オペアンプ25の反転入力端子と出力端子との間には第
1の帰還インピーダンス26が接続され、同アンプ25の非
反転入力端子と出力端子との間には第2の帰還インピー
ダンス27が接続されている。
The first feedback impedance 26 is connected between the inverting input terminal and the output terminal of the operational amplifier 25, and the second feedback impedance 27 is connected between the non-inverting input terminal and the output terminal of the same amplifier 25. There is.

二次巻線24の上記他端とオペアンプ25の非反転入力端
子との間には補償用インピーダンス28が接続され、これ
らの接続点とアースとの間に負担29が接続されている。
A compensating impedance 28 is connected between the other end of the secondary winding 24 and the non-inverting input terminal of the operational amplifier 25, and a load 29 is connected between these connection points and the ground.

ここで、第1の帰還インピーダンス26のインピーダン
スをZf、第2の帰還インピーダンス12のインピーダンス
をZm、補償用インピーダンス13のインピーダンスをZn、
二次漏れインピーダンスをZ21とすると、変流器21の二
次誘起電圧Eが零になる条件は、 Zn/Zm=Z21/Zf である。
Here, the impedance of the first feedback impedance 26 is Zf, the impedance of the second feedback impedance 12 is Zm, the impedance of the compensation impedance 13 is Zn,
When the secondary leakage impedance is Z21, the condition that the secondary induced voltage E of the current transformer 21 becomes zero is Zn / Zm = Z21 / Zf.

この条件を満足するように各インピーダンスZn,Zm,Zf
を設定することにより、二次誘起電圧Eを零にすること
ができ、励磁電流が零になって、誤差の補償が可能とな
る。
In order to satisfy this condition, each impedance Zn, Zm, Zf
By setting, the secondary induced voltage E can be made zero, the exciting current becomes zero, and the error can be compensated.

二次電流は二次巻線24の上記一端から、第1のインピ
ーダンス26、オペアンプ25の出力端子、同アンプ25の電
源端子、その接地点を通じ、負担29を介して二次巻線24
の上記他端へと還流する。よって、負担29はその二次電
流から測定量を得る。
The secondary current passes from the above-mentioned one end of the secondary winding 24, the first impedance 26, the output terminal of the operational amplifier 25, the power supply terminal of the amplifier 25, the ground point thereof, and the load 29 to the secondary winding 24.
Reflux to the other end of. Thus, the burden 29 derives the measured quantity from its secondary current.

このため、本補償回路は、負担29が測定量を電流とし
て取出しているもので有るから、使用温度条件により二
次漏れインピーダンスZ21が変化することで補償電圧の
過不足が生じたとしても、測定精度がこれに影響される
ことがない、というものである。
For this reason, in this compensation circuit, since the load 29 takes out the measured amount as a current, even if the secondary leakage impedance Z21 changes due to operating temperature conditions, even if the compensation voltage becomes excessive or insufficient, measurement is performed. The accuracy is not affected by this.

〔発明の効果〕〔The invention's effect〕

以上説明したように本発明によれば、鉄心の一次巻線
装着部に空隙を設け、一次巻線をこの空隙に挿入するよ
うにして、その磁束を二次巻線に鎖交させる有効面積を
二次巻線の面積よりも小さくなるように鉄心を装着した
ので、巻数比よりも大きな変成比を得るようにし、一次
巻線と二次巻線との面積比を調整することにより変成比
を調節できる構造としたので、インダクタンス成分の影
響が小さく、また抵抗温度係数の問題がなく、しかも空
隙にスペーサ等を設けることで一次巻線は容易に鉄心へ
固定することができ、安定した状態で巻線比よりも大き
な変成比が得られるという効果を奏する。
As described above, according to the present invention, a void is provided in the primary winding mounting portion of the iron core, and the primary winding is inserted into this void, so that the effective area for linking the magnetic flux with the secondary winding is increased. Since the iron core was installed so that it was smaller than the area of the secondary winding, a transformation ratio larger than the turns ratio was obtained, and the transformation ratio was adjusted by adjusting the area ratio between the primary winding and the secondary winding. Since the structure is adjustable, the influence of the inductance component is small, there is no problem of the temperature coefficient of resistance, and the primary winding can be easily fixed to the iron core by providing a spacer etc. in the air gap, and in a stable state. This has an effect that a transformation ratio larger than the winding ratio can be obtained.

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

第1図は本発明の第1実施例に係る変流器の正面図、第
2図は第1図のII−II線に沿う断面図、第3図は第1図
のIII−III線に沿う断面図、第4図は本発明の第2実施
例に係る変流器の正面図、第5図は第4図のV−V線に
沿う断面図、第6図は第4図のVI−VI線に沿う断面図、
第7図は第4図〜第6図の一次巻線を用いる場合のスペ
ーサの変形例の正面図、第8図は本発明の第3実施例に
係る変流器の側面図、第9図はそのIX−IX線に沿う断面
図、第10図は本発明の変流器に用いる好適な誤差補償回
路の回路図、第11図は分流回路を用いた従来例の説明
図、第12図は二次巻線を一次巻線に対して傾斜させて保
持する構造を用いた従来例の説明図である。 8…鉄心(MTコア)、11…一次巻線、11A,11B…相互に
逆方向の磁束を発生する巻線部、12…二次巻線、15…空
隙、16…スペーサ、17,17A,17B…ワイヤ挿通孔、18…鉄
心(カットコア)。
1 is a front view of a current transformer according to a first embodiment of the present invention, FIG. 2 is a sectional view taken along line II-II of FIG. 1, and FIG. 3 is taken along line III-III of FIG. 4 is a front view of a current transformer according to a second embodiment of the present invention, FIG. 5 is a cross-sectional view taken along the line VV of FIG. 4, and FIG. 6 is VI of FIG. -A cross-sectional view along line VI,
FIG. 7 is a front view of a modification of the spacer when the primary winding of FIGS. 4 to 6 is used, FIG. 8 is a side view of the current transformer according to the third embodiment of the present invention, and FIG. Is a sectional view taken along the line IX-IX, FIG. 10 is a circuit diagram of a suitable error compensation circuit used in the current transformer of the present invention, FIG. 11 is an explanatory view of a conventional example using a shunt circuit, and FIG. FIG. 6 is an explanatory diagram of a conventional example using a structure in which a secondary winding is inclined and held with respect to a primary winding. 8 ... Iron core (MT core), 11 ... Primary winding, 11A, 11B ... Winding parts that generate mutually opposite magnetic flux, 12 ... Secondary winding, 15 ... Air gap, 16 ... Spacer, 17, 17A, 17B ... Wire insertion hole, 18 ... Iron core (cut core).

Claims (1)

【特許請求の範囲】[Claims] 【請求項1】一次巻線と二次巻線とが装着される鉄心の
前記一次巻線装着部として空隙が設けられ、前記一次巻
線は、前記二次巻線にその磁束を鎖交させる有効面積が
該二次巻線の面積よりも小さくなるように前記空隙に挿
入されていることを特徴とする変流器。
1. An air gap is provided as the primary winding mounting portion of an iron core in which a primary winding and a secondary winding are mounted, and the primary winding links the magnetic flux to the secondary winding. A current transformer, characterized in that the current transformer is inserted into the air gap so that the effective area is smaller than the area of the secondary winding.
JP63328443A 1988-12-26 1988-12-26 Current transformer Expired - Fee Related JPH088186B2 (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP63328443A JPH088186B2 (en) 1988-12-26 1988-12-26 Current transformer

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP63328443A JPH088186B2 (en) 1988-12-26 1988-12-26 Current transformer

Publications (2)

Publication Number Publication Date
JPH02174104A JPH02174104A (en) 1990-07-05
JPH088186B2 true JPH088186B2 (en) 1996-01-29

Family

ID=18210331

Family Applications (1)

Application Number Title Priority Date Filing Date
JP63328443A Expired - Fee Related JPH088186B2 (en) 1988-12-26 1988-12-26 Current transformer

Country Status (1)

Country Link
JP (1) JPH088186B2 (en)

Families Citing this family (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
FR2701591B1 (en) * 1994-01-11 1995-11-24 Schlumberger Ind Inc Unshielded current transformer with air coupling.
JP2007285964A (en) * 2006-04-19 2007-11-01 Nec Tokin Corp Current detector

Family Cites Families (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS60183416U (en) * 1984-05-17 1985-12-05 株式会社東芝 Current transformer

Also Published As

Publication number Publication date
JPH02174104A (en) 1990-07-05

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