JPH0450663A - Current measuring device - Google Patents

Current measuring device

Info

Publication number
JPH0450663A
JPH0450663A JP2154429A JP15442990A JPH0450663A JP H0450663 A JPH0450663 A JP H0450663A JP 2154429 A JP2154429 A JP 2154429A JP 15442990 A JP15442990 A JP 15442990A JP H0450663 A JPH0450663 A JP H0450663A
Authority
JP
Japan
Prior art keywords
phase
current
conductor
plane
gap
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
JP2154429A
Other languages
Japanese (ja)
Inventor
Motohiro Shimada
島田 基博
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.)
Mitsubishi Electric Corp
Original Assignee
Mitsubishi Electric 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 Mitsubishi Electric Corp filed Critical Mitsubishi Electric Corp
Priority to JP2154429A priority Critical patent/JPH0450663A/en
Publication of JPH0450663A publication Critical patent/JPH0450663A/en
Pending legal-status Critical Current

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Abstract

PURPOSE:To make it possible to measure the current in its own phase accurately by constituting a plane including a magnetooptic element in each phase and the central axis of a conductor so that the plane intersects approximately orthogonally with a plane wherein the central axes of three conductors in three phases are arranged. CONSTITUTION:When a current flows through a conductor 1, a magnetic field is correspondingly generated in an iron core 16. The plane of polarization of the incident light that is cast into a magnetooptic element 8 through an optical fiber 9A is rotated by the Faraday effect in correspondence with the magnetic field in a gap 17. The transmitted light is received, nd the signal is processed. As a result, the current flowing through the conductor 1 can be measured. When the effect of the amgnetic field generated by the current flowing through the conductor 1 in an other phase, the magnetic field generated by the current in the other phase is generated in the direction which is approximately orthogonal to the tangent line on the circle of the shape of the iron core 16 having the gap at the provided position of the magnetooptic element 8. Therefore the magnetic-field detecting sensitivity is low. On the other hand, the magnetic field by the current in its own phase is generated in the tangent-line direction of the circle. Therefore, the magnetic-field detecting sensitivity is high, and the current in its own phase can be accurately measured.

Description

【発明の詳細な説明】 〔産業上の利用分野〕 この発明は導体に流れる電流を測定する電流測定装置に
関するものである。
DETAILED DESCRIPTION OF THE INVENTION [Field of Industrial Application] The present invention relates to a current measuring device that measures a current flowing through a conductor.

〔従来の技術〕[Conventional technology]

第4図は例えば実願昭63−149979号に示された
従来の電流測定装置の斜視図であり、一部を破断して示
している。図において、(1)は通電するだめの円筒状
の導体、C)は導体(1)を囲繞して設けられた変流器
で、詳細は図示しないがリンク状の鉄心とこの鉄心に巻
回された巻線とから構成され、導体(1)とは電気的に
接続されてこれと同一電位になっている。(3)は導体
(1)の中空部(4)に設けられた電流−光変換器て、
第5図はその詳細を示す平面図、第6図は第5図のM−
M線に沿った断面図である。
FIG. 4 is a perspective view of a conventional current measuring device disclosed in, for example, Japanese Utility Model Application No. 149979/1985, with a part cut away. In the figure, (1) is a cylindrical conductor that conducts current, and C) is a current transformer installed surrounding conductor (1). Although the details are not shown, it is connected to a link-shaped iron core and wound around this iron core. The conductor (1) is electrically connected to the conductor (1) and has the same potential as the conductor (1). (3) is a current-light converter provided in the hollow part (4) of the conductor (1);
Fig. 5 is a plan view showing the details, and Fig. 6 is M- of Fig. 5.
It is a sectional view along the M line.

(5)は三脚鉄心で、中央脚には空隙(6)が形成され
ている。(7)は三脚鉄心(5)の中央脚の上下に巻回
された巻線、8は三脚鉄心(5)の中央脚の空隙(6)
に設けられた磁気光学素子で、釦ガラス等のファラデー
効果を有する素子や偏光子、検光子(共に図示せず)な
どで構成されている。<9A)、 (9B)はそれぞれ
の一端が磁気光学素子(8)に光学的に結合された光フ
ァイバで、それぞれの他端は三脚鉄心(5)の中央脚に
形成された貫通穴(10)を経て導出されている。
(5) is a tripod core, and a gap (6) is formed in the center leg. (7) is the winding wound above and below the center leg of the tripod core (5), and 8 is the gap (6) in the center leg of the tripod core (5).
It is a magneto-optical element installed in the optical system, and is composed of an element having a Faraday effect such as a button glass, a polarizer, an analyzer (both not shown), and the like. <9A) and (9B) are optical fibers whose one end is optically coupled to the magneto-optical element (8), and whose other end is connected to the through hole (10) formed in the center leg of the tripod core (5). ).

第4図に戻って、(11)は変流器(2)の巻線と電流
光変換器(3)の巻線(7)とを接続するリード線、(
12)は変流器(2)やリード線(11)を覆うように
設けられた電界緩和用のシールドで、変流器(2)と同
様に導体(1)と電気的に接続されて同一電位になって
いる。以上の(1)〜(12)が図示しない円筒状の金
属容器に収納されており、この金属容器には絶縁媒体と
して六フッ化イオウ(SF6)ガスが封入されている。
Returning to FIG. 4, (11) is a lead wire connecting the winding of the current transformer (2) and the winding (7) of the current-optical converter (3);
12) is a shield provided to cover the current transformer (2) and the lead wire (11) to alleviate the electric field, and like the current transformer (2), it is electrically connected to the conductor (1) and is the same as the current transformer (2). It is at electric potential. The above items (1) to (12) are housed in a cylindrical metal container (not shown), and this metal container is filled with sulfur hexafluoride (SF6) gas as an insulating medium.

また、光ファイバ<9A)、 (9B)は金属容器外へ
導出されている。
Furthermore, the optical fibers <9A) and (9B) are led out of the metal container.

次に動作について説明する。導体(1)に電流か流れる
と、この電流に比例した電流が変流器(2)の巻線に流
れ、従って、これとリード線(11)を介して接続され
た電流−光変換器(3)の巻線(刀にも同様に流れる。
Next, the operation will be explained. When a current flows in the conductor (1), a current proportional to this current flows in the winding of the current transformer (2) and therefore in the current-to-light converter ( 3) winding (similarly flows to the sword).

これによって、磁気光学素子(8)か配置されている空
隙(6)に磁界が生じる。一方、図示外の発光源から発
した光を光ファイバ(9A)を介して磁気光学素子ts
+へ入射する。偏光子で偏波面が一定になった光か鉛ガ
ラス等のファラデー効果で、上記磁界の強さに応じてそ
の偏波面が回転する。検出子によりその回転角度に応じ
た透過光が取り出され、ファイバ(9B)を介してこの
透過光を図示外の受光器で受光することにより、空隙(
6)中の磁界の強さを知ることができ、従って、導体(
1)を流れる電流の測定を行うことができる。
This generates a magnetic field in the air gap (6) in which the magneto-optical element (8) is placed. On the other hand, light emitted from a light emitting source (not shown) is transmitted to the magneto-optical element ts via an optical fiber (9A).
incident on +. Due to the Faraday effect of light whose plane of polarization is made constant by a polarizer, the plane of polarization rotates depending on the strength of the magnetic field. Transmitted light corresponding to the rotation angle is extracted by the detector, and this transmitted light is received by a light receiver (not shown) through the fiber (9B), thereby detecting the gap (
6) We can know the strength of the magnetic field in the conductor (
1) Measurement of the current flowing through can be performed.

〔発明か解決しようとする課題〕[Invention or problem to be solved]

従来の電流測定装置は以上のように構成されているので
、万一の故障時や保守・点検時には金属容器内の絶縁媒
体を別の容器に回収して、金属容器に収容された導体の
、更にその中空部に設置された電流測定装置を分解する
必要があり、保守・点検時および故障時の迅速な復旧が
困難である。
Since the conventional current measuring device is configured as described above, in the event of a failure or maintenance/inspection, the insulating medium in the metal container is collected into another container, and the conductor contained in the metal container is Furthermore, it is necessary to disassemble the current measuring device installed in the hollow part, making it difficult to perform maintenance/inspection or to quickly restore the device in the event of a failure.

三相相分離母線の場合は、古くからあるリング形鉄心と
巻線を用いた電磁誘導式の変流器を、金属容器の外側で
これを取り巻くように設置する方法があるが、この場合
は磁気光学式に比べて、高精度、高負担のときに鉄心が
大きくなり、また、設置場所の電磁界の影響を受は易い
などの問題点があった。
In the case of a three-phase phase-separated bus, there is a method of installing an electromagnetic induction current transformer using a traditional ring-shaped iron core and windings so as to surround it outside the metal container, but in this case, Compared to the magneto-optical type, there are problems such as the iron core is large when high precision and high loads are required, and it is easily affected by the electromagnetic field at the installation location.

この発明は上記のような問題点を解消するためになされ
たもので、磁気光学式であって、かつ、保守・点検時お
よび故障時の処置、復旧を迅速に行なうことができる電
流測定装置を得ることを目的とする。
This invention was made in order to solve the above-mentioned problems, and provides a current measuring device that is magneto-optical and can quickly perform maintenance/inspection, troubleshooting, and recovery. The purpose is to obtain.

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

この発明に係る電流測定装置は、三相相分離母線の導体
の電流を測定するものにおいて、金属容器を囲繞するギ
ャップ付鉄心と、ギャップに設けられた磁気光学素子と
から成り、各相の磁気光学素子と導体の中心軸とを含む
平面が、三相三本の導体の中心軸が配置された平面とは
)直交するように配置したものである。
The current measuring device according to the present invention measures the current in the conductor of a three-phase phase separation bus bar, and is composed of an iron core with a gap surrounding a metal container and a magneto-optical element provided in the gap. The optical element and the central axis of the conductor are arranged so that the plane containing them is orthogonal to the plane in which the central axes of the three three-phase conductors are arranged.

〔作用〕[Effect]

この発明における電流測定装置は、各相において導体に
流れる電流に応じた磁界がギャップに生じ、この磁界が
磁気光学素子で検出され、また、他相の導体の電流によ
る磁界の影響が小さい位置に磁気光学素子を配置してい
るので、各相の電流を精度よく測定できる。
In the current measuring device of the present invention, a magnetic field is generated in the gap in accordance with the current flowing through the conductor in each phase, and this magnetic field is detected by a magneto-optical element, and is located at a position where the influence of the magnetic field due to the current in the conductor of the other phase is small. Since magneto-optical elements are arranged, the current in each phase can be measured with high accuracy.

更に、電流測定装置が金属容器の外側に配置されている
ので、金属容器内の絶縁媒体をそのままにした状態で、
保守・点検や故障修理を行なうことができる。
Furthermore, since the current measuring device is placed outside the metal container, it is possible to
Able to perform maintenance/inspection and troubleshooting.

〔実施例〕〔Example〕

以下、この発明の一実施例を図について説明する。第1
図、第2図はこの発明の一実施例による電流測定装置を
示す斜視図、および導体(1)の中心軸と直交する平面
に沿った断面図であり、いずれも−相分のみを示す。(
1)は通電するための円筒状の導体、(15)は導体(
1)を収納する円筒状の金属容器で、内部には絶縁媒体
としてSF、ガスが封入されている。(16)は金属容
器(2)を囲繞して設けられたギャップ付鉄心、(17
)はそのギャップ、6はギャップ(17)に設けられた
磁気光学素子で、従来例と同様に、鉛ガラス等のファラ
デー効果を有する素子や偏光子、検光子なとで構成され
ている。
An embodiment of the present invention will be described below with reference to the drawings. 1st
FIG. 2 is a perspective view showing a current measuring device according to an embodiment of the present invention, and a sectional view taken along a plane perpendicular to the central axis of the conductor (1), both of which show only the -phase component. (
1) is a cylindrical conductor for conducting electricity, and (15) is a conductor (
It is a cylindrical metal container that stores 1), and SF and gas are sealed inside as an insulating medium. (16) is an iron core with a gap provided surrounding the metal container (2), (17
) is the gap, and 6 is a magneto-optical element provided in the gap (17), which, like the conventional example, is composed of an element having a Faraday effect such as lead glass, a polarizer, an analyzer, etc.

(9A)、 (9B>はそれぞれの一端が磁気光学素子
B)に光学的に結合された光ファイバである。ギャップ
付鉄心(16)形状の円の接線方向の磁界成分により、
光ファイバ(9A)から入射された光の偏波面が回転す
るようになっている。
(9A) and (9B> are optical fibers each having one end optically coupled to the magneto-optical element B). Due to the magnetic field component in the tangential direction of the circle of the gapped core (16),
The plane of polarization of the light incident from the optical fiber (9A) is rotated.

第3図は第1図、第2図に示された電流測定装置の三相
分の配置を示す断面図であり、第2図の場合と同様に、
導体(1)の中心軸と直交する平面に沿った断面を示す
。導体(1)−本が一相分であり、接地された三つの金
属容器(15)かそれぞれ導体(1)を−本ずつ収納す
ることにより三相相分離母線を構成している。三本の導
体(1)はそれらの中心軸が同一水平面上にあるように
配置されている。各相において、磁気光学素子8)と導
体(1]の中心軸を含む平面がそれぞれ上記水平面と直
交する配置になっている。つまり、磁気光学素子6は導
体(1]の鉛直上方に配置されている。なお、三相の金
属容器(15)同士が図示外のところで電気的につなが
って閉回路を構成することのないように、必要な箇所に
は相互間に絶縁材(図示せず)が取付けられている。も
し、仮に閉回路ができると導体(1)の電流と逆向きの
電流か金属容器(15)に流れるので、これを防止する
ためである。
FIG. 3 is a sectional view showing the arrangement of three phases of the current measuring device shown in FIGS. 1 and 2, and as in the case of FIG. 2,
A cross section taken along a plane perpendicular to the central axis of the conductor (1) is shown. The conductor (1) corresponds to one phase, and a three-phase phase-separated bus bar is constructed by housing each of the conductors (1) in three grounded metal containers (15). The three conductors (1) are arranged so that their central axes are on the same horizontal plane. In each phase, the planes containing the central axes of the magneto-optical element 8) and the conductor (1) are arranged perpendicular to the horizontal plane.In other words, the magneto-optical element 6 is arranged vertically above the conductor (1). In order to prevent the three-phase metal containers (15) from being electrically connected in places other than shown to form a closed circuit, insulating materials (not shown) should be placed between them where necessary. This is to prevent if a closed circuit were to be formed, a current in the opposite direction to the current in the conductor (1) would flow into the metal container (15).

次に動作について説明する。導体(1)に電流か流れる
と、それに応じてギャップ付鉄心(16)に磁界が生じ
、従来と同様にして、光ファイバ(9A)を介して磁気
光学素子8に入射した光がギャップ(17)中の磁界に
応じてファラデー効果により、偏波面が回転し、透過光
を受光して信号処理することにより、結局、導体(1)
を流れる電流を測定することができる。
Next, the operation will be explained. When a current flows through the conductor (1), a magnetic field is generated in the gapped iron core (16) in response, and in the same way as in the past, light incident on the magneto-optical element 8 via the optical fiber (9A) is caused to flow through the gap (17). ) The plane of polarization rotates due to the Faraday effect according to the magnetic field in the conductor (1), and by receiving the transmitted light and processing the signal, the conductor (1)
The current flowing through can be measured.

なお、他相の導体(1)に流れる電流による磁界の影響
を考えると、磁気光学素子8の設置位置においては、他
相電流による磁界はギャップ付鉄心(16)形状の円の
接線とほゞ直交する方向に生じるので磁界検出感度が低
い。これに対して自相電流による磁界は上記円の接線方
向に生じるので磁界検出感度が高く、そのため、他相電
流の影響を殆んど受けずに自相電流を精度良く測定する
ことができる。
Furthermore, considering the influence of the magnetic field due to the current flowing through the conductor (1) of the other phase, at the installation position of the magneto-optical element 8, the magnetic field due to the other phase current is approximately equal to the tangent of the circle of the gapped core (16). Magnetic field detection sensitivity is low because it occurs in orthogonal directions. On the other hand, since the magnetic field due to the own-phase current is generated in the tangential direction of the circle, the magnetic field detection sensitivity is high, and therefore the own-phase current can be accurately measured with almost no influence from other-phase currents.

なお、上記実施例では磁気光学素子8に鉛ガラスを使用
したものを例示したが、他のファラデー素子を用いても
よい。また、各相の磁気光学素子(8)を導体(1)の
上方に設置したが鉛直下方に設けてもよく、この場合は
屋外における日射を遮って、温度上昇による磁気光学素
子8)への影響を小さくする効果がある。更に、三相の
導体を水平配置したものを示したが鉛直配置などでもよ
い。
In the above embodiment, the magneto-optical element 8 is made of lead glass, but other Faraday elements may be used. In addition, although the magneto-optical elements (8) for each phase were installed above the conductor (1), they may also be installed vertically below. In this case, solar radiation outdoors is blocked and the magneto-optical elements (8) are prevented from being affected by temperature rise. This has the effect of reducing the impact. Further, although the three-phase conductors are shown arranged horizontally, they may also be arranged vertically.

また、SF6ガス人の相分離母線を示したが、絶縁媒体
として空気や絶縁油を用いたものでもよく、その他、管
路気中送電線、ブッシング、ケーブルヘッドあるいは断
路器や遮断器などの母線部分で三相相分離された箇所等
にも適用できる。
In addition, although a phase-separated busbar for SF6 gas is shown, it may also use air or insulating oil as the insulating medium, and other busbars such as conduit aerial transmission lines, bushings, cable heads, disconnectors, circuit breakers, etc. It can also be applied to locations where three phases are separated in some areas.

〔発明の効果〕〔Effect of the invention〕

以上のように、この発明によれば、金属容器を囲繞する
ギャップ付鉄心と、ギャップに設けられた磁気光学素子
とから成り、各相の磁気光学素子と導体の中心軸とを含
む平面が、三相三本の導体の中心軸が配置された平面と
はゾ直交するように構成したので、磁気光学式の電流測
定を行なうものであって、かつ、保守・点検時および故
障時の処置、復旧を迅速に行なうことができると共に、
他相の電流の影響を少なくして自相の電流を精度良く測
定できるものが得られる効果がある。
As described above, according to the present invention, the plane is composed of an iron core with a gap surrounding a metal container and a magneto-optical element provided in the gap, and includes the magneto-optical element of each phase and the central axis of the conductor. Since the central axes of the three conductors of the three phases are configured to be perpendicular to the plane in which they are arranged, magneto-optical current measurement is performed, and it is easy to handle during maintenance, inspection, and troubleshooting. In addition to being able to perform recovery quickly,
This has the effect of reducing the influence of currents in other phases and allowing accurate measurement of the current in the own phase.

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

第1図、第2図はこの発明の一実施例による電流測定装
置を示す斜視図と断面図、第3図は第1図、第2図の電
流測定装置の三相分の配置を示す断面図、第4図は従来
の電流測定装置を示す斜視図、第5区は第4図の電流測
定装置の電流−光変換器を示す平面図、第6区は第5図
の■−■線に沿った断面図である。 図において、(1)は導体、(8)は磁気光学素子、(
15)は金属容器、(16)はギャップ付鉄心、<17
)はギャップである。 なお、各図中同一符号は同一または相当部分を示す。 代 理 人    弁理士  大 岩 増 雄第1図 第2図 第3図 第4図
1 and 2 are a perspective view and a sectional view showing a current measuring device according to an embodiment of the present invention, and FIG. 3 is a sectional view showing the arrangement of three phases of the current measuring device shown in FIGS. 1 and 2. Figure 4 is a perspective view showing a conventional current measuring device, Section 5 is a plan view showing the current-light converter of the current measuring device shown in Fig. 4, Section 6 is a line ■-■ in Fig. 5. FIG. In the figure, (1) is a conductor, (8) is a magneto-optical element, (
15) is a metal container, (16) is an iron core with a gap, <17
) is a gap. Note that the same reference numerals in each figure indicate the same or corresponding parts. Agent Masuo Oiwa, Patent Attorney Figure 1 Figure 2 Figure 3 Figure 4

Claims (1)

【特許請求の範囲】[Claims] 同一平面上に中心軸が配置された三本の導体とこれらの
導体を一本ずつ収納する三つの金属容器とこの金属容器
に封入された絶縁媒体とから成る三相相分離母線の上記
導体を流れる電流を測定するものにおいて、各相の上記
金属容器を囲繞して設けられたギャップ付鉄心とこのギ
ャップ付鉄心のギャップに設けられた磁気光学素子とか
ら成り、各相の上記磁気光学素子と導体の中心軸とを含
む平面が、上記三本の導体の中心軸が配置された平面と
ほゞ直交するように配置したことを特徴とする電流測定
装置。
The above conductor of a three-phase phase-separated bus bar consists of three conductors whose central axes are arranged on the same plane, three metal containers that house each of these conductors, and an insulating medium sealed in these metal containers. A device for measuring flowing current consists of an iron core with a gap provided surrounding the metal container of each phase and a magneto-optical element provided in the gap of the iron core with a gap, and the magneto-optic element of each phase and 1. A current measuring device characterized in that a plane including the central axes of the conductors is arranged so as to be substantially orthogonal to a plane in which the central axes of the three conductors are arranged.
JP2154429A 1990-06-13 1990-06-13 Current measuring device Pending JPH0450663A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP2154429A JPH0450663A (en) 1990-06-13 1990-06-13 Current measuring device

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP2154429A JPH0450663A (en) 1990-06-13 1990-06-13 Current measuring device

Publications (1)

Publication Number Publication Date
JPH0450663A true JPH0450663A (en) 1992-02-19

Family

ID=15583988

Family Applications (1)

Application Number Title Priority Date Filing Date
JP2154429A Pending JPH0450663A (en) 1990-06-13 1990-06-13 Current measuring device

Country Status (1)

Country Link
JP (1) JPH0450663A (en)

Cited By (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JP2011128092A (en) * 2009-12-21 2011-06-30 Japan Ae Power Systems Corp Single-phase optical current transformer

Cited By (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JP2011128092A (en) * 2009-12-21 2011-06-30 Japan Ae Power Systems Corp Single-phase optical current transformer
WO2011078096A1 (en) * 2009-12-21 2011-06-30 株式会社日本Aeパワーシステムズ Single-phase optical current transformer

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