JPS6170468A - Current detector - Google Patents

Current detector

Info

Publication number
JPS6170468A
JPS6170468A JP59192988A JP19298884A JPS6170468A JP S6170468 A JPS6170468 A JP S6170468A JP 59192988 A JP59192988 A JP 59192988A JP 19298884 A JP19298884 A JP 19298884A JP S6170468 A JPS6170468 A JP S6170468A
Authority
JP
Japan
Prior art keywords
iron core
gap
current
conductor
core
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
JP59192988A
Other languages
Japanese (ja)
Inventor
Shinzo Ogura
小倉 新三
Masayuki Ariki
有木 正幸
Toshishige Nagao
永尾 俊繁
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 JP59192988A priority Critical patent/JPS6170468A/en
Publication of JPS6170468A publication Critical patent/JPS6170468A/en
Pending legal-status Critical Current

Links

Abstract

PURPOSE:To insert a conductor to be measured into an iron core magnetic circuit simply and to reduce an error by forming a driving device for driving a movable iron core arranged close to a gap in which a magnetic optical part is set up. CONSTITUTION:The titled device is provided with an iron core 1, a fixed iron core 1a, a movable iron core 1b, a driving device 7, a gap 11, etc. When a compression spring 7a in the device 7 is compressed, the leading end of the movable iron core 1b is opened from the fixed iron core 1a and a conductor 6 is passed through the opened part and inserted into the iron core 1. When the compression of the spring 7 is released, the movable iron core 1b is rotated in the clockwise direction by the device 7 and joined with the fixed iron core 1a. At the measurement of current flowing into the conductor 6, the conductor 6 arranged adjacently to the gap 11 is separated from the gap 11 because of the existence of a case 8 and a magnetic field formed on the gap 11 by the conductor 6 is weakened, so that an error is reduced.

Description

【発明の詳細な説明】 〔産業上の利用分野〕 この発明は磁気光学素子で電流の作る磁界の大きさを検
出しそれを電流値に変換して電流を測定する電流検出装
置に関するものである。
[Detailed Description of the Invention] [Field of Industrial Application] This invention relates to a current detection device that detects the magnitude of a magnetic field created by a current using a magneto-optical element, converts it into a current value, and measures the current. .

〔従来の技術) 第1図に従来の貫通型光電流検出装置を示している。図
において(11は一部lこギャップQηを有し。
[Prior Art] FIG. 1 shows a conventional through-type photocurrent detection device. In the figure (11 has a partial gap Qη).

磁気閉回路を構成する鉄心、(2)はギャップIJjJ
に設けられた磁気光学部で46°プリズム、マイクロレ
ンズ、光を一方向の成分にする偏光子、磁界がか一つて
いると光の偏光面が回転するファラデー素子、磁界の強
度に応じて光の強度が変る検光子から構成されている。
The iron core that constitutes the magnetic closed circuit, (2) is the gap IJjJ
The magneto-optical section installed in It consists of an analyzer whose intensity changes.

(3)は鉄心(υと磁気光学部(2)を固定する固定剤
、(4)は磁気光学部(2)と変換装置(5ンヲ接続す
る光フアイバーケーブル(5)は光送受信器。
(3) is the fixing agent that fixes the iron core (υ) and the magneto-optical section (2), (4) is the optical fiber cable (5) that connects the magneto-optical section (2) and the converter (5) is the optical transceiver.

光強度−電気変換器および表示器からなる変換装置、(
6)は被測定電流が流れている導体(a) 、 (b)
 、 (cl。
A conversion device consisting of a light intensity-to-electrical converter and an indicator (
6) are the conductors (a) and (b) through which the current to be measured flows.
, (cl.

(d)は磁気閉回路の外部に近在する通電導体である。(d) is a current-carrying conductor located near the outside of the magnetic closed circuit.

従来の光電流計は上記のように構成され、導体(6]f
ζ流れる電流により鉄心(υのギャップOυに設けた磁
気光学部に@1図に示すy方向の磁界が発生する。−万
変換装置(5)からは光フアイバーケーブル(4)によ
り光を磁気光学部(2)に送って居り磁界の大きさに比
例し光強度が磁気光学部(2)で変化し。
A conventional photocurrent meter is constructed as described above, with a conductor (6]f
The flowing current generates a magnetic field in the y direction shown in Figure @1 in the magneto-optical section installed in the gap Oυ of the iron core (υ). The light intensity changes in the magneto-optical section (2) in proportion to the magnitude of the magnetic field.

光フアイバーケーブル(4jで返還さn、変換装置(5
)内で光強度−電気変換を行ない電流値を表示器で表示
する。
Fiber optic cable (returned by 4j), conversion device (5
) performs light intensity-to-electricity conversion and displays the current value on a display.

ところが従来のものでは鉄心(υの外部近傍に通電導体
(a) 、 (b) 、 (c) 、 (d)が容易に
近在することが出来る。このような通電導体(a) 、
 (b) 、 (c) 、 (d)が存在した時の鉄心
(1)のギャップaυに対する磁束(φ)の様子を@1
−1図、第1−2図、第1−i11図に示す。この磁束
(fl)が導体(6)の電流がつくるギャップσηにお
ける磁界の大きさの誤差となってあられれる。@2図に
通電導体(a) 、 (b) 、 (cン、(d)の位
置と誤差(ε)の特性を示している。通電導体が(a)
 、 (C)の場合ギャップC11J部では通電導体(
a) 、 (c)の作るy方向の磁界が弱く、誤差(ε
)も少ないが通電導体が(d)の場合ではギャップαυ
を通るもれ磁束(−)が多少あるためギャップση部で
y方向の磁界がや\強く誤差(ε)がわずか多くなって
いる。通電導体が(b)の場合は更にy方向の磁束が強
くなり最大の誤差〔ε〕を生じこの誤差(ε)が特に問
題になる。上記には4点について述べたが、その他の近
接通電導体は@2図に示さnるように誤差(ε)を現象
的にプロットしである。
However, in the conventional type, current-carrying conductors (a), (b), (c), and (d) can easily be located near the outside of the iron core (υ).Such current-carrying conductors (a),
The state of the magnetic flux (φ) with respect to the gap aυ of the iron core (1) when (b), (c), and (d) exist is @1
It is shown in Figure-1, Figure 1-2, and Figure 1-i11. This magnetic flux (fl) results in an error in the magnitude of the magnetic field in the gap ση created by the current in the conductor (6). Figure @2 shows the position and error (ε) characteristics of current-carrying conductors (a), (b), (c), and (d).When the current-carrying conductor is (a)
, In the case of (C), the current-carrying conductor (
The magnetic field in the y direction created by a) and (c) is weak, and the error (ε
) is also small, but when the current-carrying conductor is (d), the gap αυ
Since there is some leakage magnetic flux (-) passing through the gap ση, the magnetic field in the y direction is a little stronger at the gap ση, and the error (ε) is slightly larger. When the current-carrying conductor is (b), the magnetic flux in the y direction becomes even stronger, causing the maximum error [ε], and this error (ε) becomes a particular problem. The four points have been described above, but the error (ε) for other adjacent current-carrying conductors is plotted phenomenologically as shown in Figure 2.

〔発明が解決しようとする問題点〕[Problem that the invention seeks to solve]

上記のように従来の電流検出装置では、磁気閉回路の外
部でギャップ(ロ)の近傍(こ通電導体がある場合、被
測定電流が流nている導体(6)の電流測定値に誤差(
ε)が生じ測定に支障を来たすという問題があった。
As mentioned above, in the conventional current detection device, when there is a current-carrying conductor (6) near the gap (B) outside the magnetic closed circuit, there is an error (
There was a problem in that ε) occurred, which interfered with measurement.

コノ発明はか\る問題を解決するためになされたもので
、磁気閉回路の外部でギャップの近傍に通電導体がある
場合でも被測定電流が流れている導体の電流測定値の誤
差が問題にならない程度の大きさにおさえるような装置
を得ることを目的としている。
This invention was made to solve this problem, and even if there is a current-carrying conductor near the gap outside the magnetic closed circuit, the error in the current measurement value of the conductor through which the current to be measured flows is a problem. The aim is to obtain a device whose size can be kept to a level where it will not become large.

〔問題点を解決するための手段〕[Means for solving problems]

この発明に係る電流検出装置は磁気閉回路を形成する可
動鉄心と固定鉄心から構成されギャップを有する鉄心と
このギャップの近傍に配設され。
The current detection device according to the present invention is composed of a movable core and a fixed core that form a magnetic closed circuit, and is arranged near the core having a gap and the gap.

可動鉄心を駆動する駆動装置およびこの駆動装置をとり
つけるケースをギャップ近傍にかけて取りつけたもので
ある。
A drive device for driving the movable iron core and a case for mounting this drive device are installed near the gap.

(作用〕 この発明においてはギャップ近傍にケースがあるために
磁気閉回路の外部に近在する通電導体がギャップに接近
することが出来ず、この通電導体がギャップに発生する
磁界の強さが被測定導体の測定電流の誤差として問題と
なる大きさにならないように抑制する。
(Function) In this invention, since there is a case near the gap, a current-carrying conductor near the outside of the magnetic closed circuit cannot approach the gap, and this current-carrying conductor is affected by the strength of the magnetic field generated in the gap. The error in the measurement current of the measurement conductor is suppressed so that it does not become a problem.

〔実施例〕〔Example〕

第3図はこの発明の一実施例を示す正面図で(1)は磁
気閉回路を構成する鉄心で(la)は固定鉄心。
FIG. 3 is a front view showing one embodiment of the present invention, in which (1) is an iron core that constitutes a magnetic closed circuit, and (la) is a fixed iron core.

(1b)は可動鉄心である。σηは鉄心(1)の1部に
設けられたギャップで図では固定鉄心(1a)に設けら
れているが可動鉄心(1b)に配設されてもよい。(2
)はギャップ(ロ)に設けられた磁気光学部、(3)は
鉄心(υと磁気光学部12)を固定する固定剤1(4)
は磁気光学部(2)と変換装置(5)を接続する光フア
イバーケーブル、(6)は被測定直流が流れる導体、(
7)はギャップaυの近傍に配設され、可動鉄心(1b
)を駆動する駆動装置、 (7a)は駆動装置の一部を
構成する圧縮ばね、(8)は駆動装置(7)をとりつけ
磁気閉回路の外部に近在する通電導体(a) 、 (b
) 、 (c) 、 (d)がギャップaυに接近する
のを防ぐケースである。
(1b) is a movable iron core. ση is a gap provided in a part of the iron core (1), and although it is provided in the fixed iron core (1a) in the figure, it may be provided in the movable iron core (1b). (2
) is the magneto-optical section installed in the gap (b), (3) is the fixing agent 1 (4) that fixes the iron core (υ and the magneto-optical section 12)
is an optical fiber cable connecting the magneto-optical section (2) and the converter (5), (6) is a conductor through which the DC to be measured flows, (
7) is arranged near the gap aυ, and the movable iron core (1b
), (7a) is a compression spring constituting a part of the drive device, and (8) is a current-carrying conductor (a), (b) to which the drive device (7) is attached and which is close to the outside of the magnetic closed circuit.
), (c), and (d) are prevented from approaching the gap aυ.

動作は駆動装置(7)の圧縮ばね(7a)を圧縮すると
可動鉄心(1b)の先端が固定鉄心(1a)の先端から
開いて導体(6)が通過して鉄心(1)内に入ってくる
。そこで圧縮ばね(7a)の圧縮を解くと、駆動装置(
7)が働いて駆動装置(7)に結合した可動鉄心(1b
)が時計方向に回動して固定鉄心(1a)と接合する。
In operation, when the compression spring (7a) of the drive device (7) is compressed, the tip of the movable core (1b) opens from the tip of the fixed core (1a), and the conductor (6) passes through and enters the core (1). come. Then, when the compression spring (7a) is released, the drive device (
7) works to move the movable iron core (1b) connected to the drive device (7).
) rotates clockwise and joins with the fixed iron core (1a).

そこで導体(6)の電流が測定されるがケース(8)が
あるためにギャップαυに近接してあった通電導体(6
)はギャップの近傍から離され、ギヤツブ但に通電導体
(6)が作る磁界が弱くなるため誤差(ε)が問題にな
らない値まで小さくなる。第4図はこの様子を示した特
性図であり、通電導体(a) *忙)、((至)による
誤差(ε)は従来と変らないが、通電導体(b)による
誤差(ε)が著しく小さくなっていることがわかる。
There, the current in the conductor (6) is measured, but because of the case (8), the current-carrying conductor (6), which was close to the gap αυ, is measured.
) is moved away from the vicinity of the gap, and the magnetic field created by the current-carrying conductor (6) in the gear becomes weaker, so that the error (ε) is reduced to a value that does not pose a problem. Figure 4 is a characteristic diagram showing this situation. The error (ε) due to the current-carrying conductor (a) and ((to) is the same as before, but the error (ε) due to the current-carrying conductor (b) is It can be seen that it has become significantly smaller.

(発明の効果) この発明は以上説明しt二とおり磁気光学部を設置した
ギャップの近傍に配役さした可動鉄心を駆動する駆動装
置を設けることにより、被測定電流導体を簡単に鉄心磁
気閉回路内に入れることが出来るばかりでなく、この駆
動装置をとりつけ磁気閉回路の外部に近在する通電導体
がギャップに接近することを防ぐケースを備えることに
よって誤差を小さくすることが出来るという効果がある
(Effects of the Invention) As described above, the present invention provides a driving device for driving a movable core placed near the gap in which the magneto-optical section is installed, thereby easily moving the current conductor to be measured into the core magnetic closed circuit. Not only can this drive device be installed in a case that prevents current-carrying conductors near the outside of the magnetic closed circuit from approaching the gap, it has the effect of reducing errors. .

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

第1図は従来の電流検出装置の正面図、第1−1図乃至
第1−3図は何れも通電導体の位置と磁束分布を示す図
、第2図は通電導体の位置と測定電流の誤差の関係を示
す図、第3図はこの発明の一実施例を示す正面図、第4
図は通電導体の位置と測定電流の誤差の関係を示す図で
ある。 図において、(1)は鉄心、(1a)は固定鉄心、 (
lb)は可動鉄心1口はギャップ、(2]は田気光学部
、(5)は変換装置、(6Iは導体、(7)は駆動装置
、(8]はケース、’ (a) 、 (b) 、 Cc
) 、 (d)は通電導体である。 なお図中同一符号は同−又は相当部分を示す。
Figure 1 is a front view of a conventional current detection device, Figures 1-1 to 1-3 are diagrams showing the position of the current-carrying conductor and magnetic flux distribution, and Figure 2 is a diagram showing the position of the current-carrying conductor and the measurement current. 3 is a front view showing an embodiment of the present invention, and 4 is a diagram showing the relationship between errors.
The figure is a diagram showing the relationship between the position of the current-carrying conductor and the error in the measured current. In the figure, (1) is the iron core, (1a) is the fixed iron core, (
lb) is the movable core 1 port is the gap, (2] is the optical part, (5) is the conversion device, (6I is the conductor, (7) is the drive device, (8) is the case, '(a), ( b), Cc
) and (d) are current-carrying conductors. Note that the same reference numerals in the figures indicate the same or equivalent parts.

Claims (1)

【特許請求の範囲】[Claims] 磁気閉回路を形成する可動鉄心と固定鉄心から構成され
ギャップを有する鉄心、この鉄心を貫通する導体に流れ
る電流が上記ギャップに作る磁界の大きさを光の強さに
変換するように上記ギャップに設けられた磁気光学部、
この磁気光学部で変換された光の強さを電流の大きさに
変換する変換装置、上記ギャップの近傍に配設され上記
可動鉄心を駆動する駆動装置、およびこの駆動装置をと
りつけ上記磁器閉回路の外部に近在する通電導体が上記
ギャップに接近することを防ぐケースを備えた電流検出
装置。
The core is composed of a movable core and a fixed core that form a magnetic closed circuit, and has a gap, and the current flowing through the conductor passing through the core converts the magnitude of the magnetic field created in the gap into the intensity of light. Magneto-optical section provided,
A conversion device that converts the intensity of light converted by the magneto-optical section into the magnitude of current, a drive device that is disposed near the gap and drives the movable core, and a magnetic closed circuit to which this drive device is attached. A current detection device comprising a case that prevents a current-carrying conductor near the outside of the device from approaching the gap.
JP59192988A 1984-09-14 1984-09-14 Current detector Pending JPS6170468A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP59192988A JPS6170468A (en) 1984-09-14 1984-09-14 Current detector

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP59192988A JPS6170468A (en) 1984-09-14 1984-09-14 Current detector

Publications (1)

Publication Number Publication Date
JPS6170468A true JPS6170468A (en) 1986-04-11

Family

ID=16300360

Family Applications (1)

Application Number Title Priority Date Filing Date
JP59192988A Pending JPS6170468A (en) 1984-09-14 1984-09-14 Current detector

Country Status (1)

Country Link
JP (1) JPS6170468A (en)

Cited By (3)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JP2013509586A (en) * 2009-10-28 2013-03-14 オプティセンスネットワーク、インク Optical sensor assembly and current measurement method in power distribution system
US9146358B2 (en) 2013-07-16 2015-09-29 Gridview Optical Solutions, Llc Collimator holder for electro-optical sensor
US9535097B2 (en) 2012-07-19 2017-01-03 Gridview Optical Solutions, Llc. Electro-optic current sensor with high dynamic range and accuracy

Cited By (4)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JP2013509586A (en) * 2009-10-28 2013-03-14 オプティセンスネットワーク、インク Optical sensor assembly and current measurement method in power distribution system
US9535097B2 (en) 2012-07-19 2017-01-03 Gridview Optical Solutions, Llc. Electro-optic current sensor with high dynamic range and accuracy
US9817038B2 (en) 2012-07-19 2017-11-14 Gridview Optical Solutions, Llc. Electro-optic current sensor with high dynamic range and accuracy
US9146358B2 (en) 2013-07-16 2015-09-29 Gridview Optical Solutions, Llc Collimator holder for electro-optical sensor

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