JPS59151065A - Optical current transformer - Google Patents

Optical current transformer

Info

Publication number
JPS59151065A
JPS59151065A JP58024615A JP2461583A JPS59151065A JP S59151065 A JPS59151065 A JP S59151065A JP 58024615 A JP58024615 A JP 58024615A JP 2461583 A JP2461583 A JP 2461583A JP S59151065 A JPS59151065 A JP S59151065A
Authority
JP
Japan
Prior art keywords
glass
faraday effect
current transformer
reflection surface
atm
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
JP58024615A
Other languages
Japanese (ja)
Inventor
Genji Takahashi
高橋 源治
Tadashi Sato
忠 佐藤
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.)
Hitachi Ltd
Original Assignee
Hitachi Ltd
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 Hitachi Ltd filed Critical Hitachi Ltd
Priority to JP58024615A priority Critical patent/JPS59151065A/en
Publication of JPS59151065A publication Critical patent/JPS59151065A/en
Pending legal-status Critical Current

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Abstract

PURPOSE:To enable stable measurement of electric current with high accuracy by coating the entire reflection surface of the Faraday effect glass of an optical current transformer with a reflection film or covering the surface thereof with a protective cover to avoid direct contact of said surface with the atm. CONSTITUTION:When the light linearly polarized by a polarizer 1 is made incident to Faraday effect glass 2, the linearly polarized light s totally reflected twice each by the respective angle parts of the glass 2 and is changed to elliptically polarized light. The rotating angle of the plane of polarization thereof is detected and the intensity of the magnetic field is measured, by which the electric current flowing in a primary conductor 6 is measured. A reflection film 7 such as multilayered film of silver, aluminum and dielectric material is formed by means such as vacuum deposition or the like on the reflection surface of the glass 2 to avoid direction contact of the glass 2 with the atm. The stable measurement is thus made possible without sticking of water drops and the contaminated material in the atm. on the reflection surface even if the current transformer is used in a climatic environment of adverse temp. and humidity.

Description

【発明の詳細な説明】 〔発明の利用分野〕 本発明は光変流器に係り、特に正常な元の偏光を伝達す
る光変流器に関する。
DETAILED DESCRIPTION OF THE INVENTION [Field of Application of the Invention] The present invention relates to optical current transformers, and more particularly to optical current transformers that transmit normal original polarized light.

〔従来技術〕[Prior art]

電流による磁界中におかれた、鉛ガラスなどのファラデ
ー効果を示すガラス(以Fファラデー効果ガラスという
)中を偏光が通過するとき、偏光面は次式に示す角度θ
だけ回転する。
When polarized light passes through a glass exhibiting the Faraday effect such as lead glass (hereinafter referred to as Faraday effect glass) placed in a magnetic field caused by an electric current, the plane of polarization is at an angle θ given by the following equation.
only rotates.

1=Ve−H−、L 但し、Ve:グエルデ定数 H:光路と平行にある磁界の強さ L ニガラス内の光路の長さ この回転角θを周知の方法で検出し磁界の強さHを測定
することによって、ガラス近傍に流れる電流を測定する
変流器が一般的である。第1図にファラデー効果ガラス
の応用例の構造を示し、偏光子1、ファラデー効果ガラ
ス2、検光子3、集光レンズ4、光フ゛アイパー5およ
び被測定電流が流れる1次導体6よりなっており、光は
この順次に進むよう(′こなっている。金偏光子1で直
線偏光した光をファラデー効果ガラス2に入射すると、
この直a偏光は該ガラス2のそれぞれの角部で2回ずつ
全反射されて、直線偏光が楕円偏光に変化し、そのため
ノアラブ−回転角の回転量が低下し同時に出力感度が低
下しないような構造になっている。この原理は東京大学
生産技術研究報告Vol。
1=Ve-H-,L However, Ve: Guerde constant H: Strength of the magnetic field parallel to the optical path L Length of the optical path inside the glass Detect this rotation angle θ using a well-known method and calculate the strength of the magnetic field H. Current transformers that measure the current flowing near the glass are common. Figure 1 shows the structure of an applied example of Faraday effect glass, which consists of a polarizer 1, a Faraday effect glass 2, an analyzer 3, a condenser lens 4, an optical eyeper 5, and a primary conductor 6 through which the current to be measured flows. , the light travels in this order ('). When light linearly polarized by the gold polarizer 1 is incident on the Faraday effect glass 2,
This directly a-polarized light is totally reflected twice at each corner of the glass 2, changing the linearly polarized light into elliptically polarized light, so that the amount of rotation of the Noah Arab rotation angle decreases, and at the same time, the output sensitivity does not decrease. It has a structure. This principle is described in the University of Tokyo Production Technology Research Report Vol.

28A5(1980年3月)に発表された斉藤氏他3名
による「レーザによる電力用電流電圧測定装置に関する
基礎的研究」によって公知で必る。直線偏光の偏光面の
ファラデー効果による回転は、光路と平行な磁界の強さ
と光路の長さに比例するので、aより入射した直線偏光
は1人感体6を一周しbよシ出射するため、ノア2デー
回転角θは次式に示すように光路と鎖交している1人感
体6の電流のみに比例している。
It was made public by ``Fundamental Research on Power Current and Voltage Measuring Devices Using Lasers'' by Mr. Saito and three others published in 28A5 (March 1980). The rotation of the polarization plane of linearly polarized light due to the Faraday effect is proportional to the strength of the magnetic field parallel to the optical path and the length of the optical path, so the linearly polarized light incident from a goes around the human sensitive body 6 and exits from b. , the Noah 2-day rotation angle θ is proportional only to the current of the single sensitive body 6 interlinked with the optical path, as shown in the following equation.

θ=Ve’/H−dt=Ve’I 但(−1y e / :ヴエルデ定数 I(:光路と平行な磁界の強さ t ニガラスの光路長 ■ :光路と鎖交する電流 したがって1人感体6の近傍にある他の導体に流れる電
流は、前記光路に沿っての積分で零となるため影響は無
視できる。このようにファラデー効果ガラスを用いた光
変流器は非常に優れた特慮を有しており、ガラス利質と
しては鉛ガラス、重フリントガラス、磁性ガラス、石英
ガラス等が用いられる。上記のごとく直線偏光を維持す
るためには7アラデー効果ガラスの各角部において、そ
れぞれ2回ずつ全反射させる必要があり、7アラデー効
果ガラス2を直線偏光が一周するのに6回の全反射が行
われる。通常の場合は第1図に示すファラデー効果ガラ
ス2の形状のま−でも測定ができるが、厳しい使用条件
の下で使用される場合、即ち温度、湿度など気象条件の
悪い環境で使用されるときは、反射面に水滴十人気中の
汚れた物質が付着して、全反射効率が低下するばかシで
なく光軸がずれる危険さえある。
θ=Ve'/H-dt=Ve'I However, (-1y e/: Weerde's constant I (: Strength of magnetic field parallel to the optical path t Nigarasu's optical path length ■: Current interlinking with the optical path Therefore, one person The influence of the current flowing in other conductors in the vicinity of 6 can be ignored because the integration along the optical path becomes zero.In this way, the optical current transformer using Faraday effect glass is a very good special consideration. Lead glass, heavy flint glass, magnetic glass, quartz glass, etc. are used as the glass material.In order to maintain linearly polarized light as described above, 7. It is necessary to carry out total reflection twice at a time, and total reflection takes place six times for linearly polarized light to go around the seven Alladay effect glass 2. In the normal case, the shape of the Faraday effect glass 2 shown in FIG. However, when used under harsh conditions, i.e., in environments with poor weather conditions such as temperature and humidity, dirty substances from water droplets may adhere to the reflective surface. There is a risk that the total internal reflection efficiency will not only decrease, but also that the optical axis will shift.

〔発明の目的〕[Purpose of the invention]

本発明は上述の点に鑑みてなされたもので、その目的と
するところは、安定した精度の高い電流測定ができる光
変流器を提供するにある。
The present invention has been made in view of the above points, and an object thereof is to provide an optical current transformer that can perform stable and highly accurate current measurement.

〔発明の概要〕[Summary of the invention]

本発明は光変流器のファラデー効果ガラスの全反射面を
反射膜でコーティングするか、あるいは保護カバーで被
覆するかして、大気に直接触れないようにすることによ
り、所期の目的を達成するようになしたものである。
The present invention achieves the intended purpose by coating the total reflection surface of the Faraday effect glass of the optical current transformer with a reflective film or covering it with a protective cover to prevent direct contact with the atmosphere. This is what I did.

〔発明の実施例〕[Embodiments of the invention]

以下本発明に係る光変流器の一実施例を図面を参照して
説明する。
An embodiment of the optical current transformer according to the present invention will be described below with reference to the drawings.

光変流器のファラデー効果ガラスの全体の構造は従来例
で説明した通pであるが、第2図に示すようにファラデ
ー効果ガラス20反射面に、銀、アルミおよび誘電体多
層膜などの反射膜7が真空蒸着などの手段によって形成
されており、前記ファラデー効果ガラス2の反射面が大
気に直接触れるのを遮断している。
The overall structure of the Faraday effect glass of the optical current transformer is the same as that described in the conventional example, but as shown in Figure 2, the Faraday effect glass 20 has a reflective surface made of silver, aluminum, dielectric multilayer, etc. A film 7 is formed by means such as vacuum deposition, and blocks the reflective surface of the Faraday effect glass 2 from coming into direct contact with the atmosphere.

第3図は本発明の他の実施例を示し、ファラデー効果ガ
ラス20反射面は全反射のま\で、反射面に触れないよ
うな間隙gを形成した保護カバー8を該反射面に固設し
、この間隙g以外の部分は反射面に接着されている。こ
の場合でも前記ファラデー効果ガラス2の反射面が大気
から遮断される。
FIG. 3 shows another embodiment of the present invention, in which the reflective surface of the Faraday effect glass 20 remains in total reflection, and a protective cover 8 with a gap g formed therein so as not to touch the reflective surface is fixed to the reflective surface. However, the portion other than this gap g is bonded to the reflective surface. Even in this case, the reflective surface of the Faraday effect glass 2 is shielded from the atmosphere.

このように本発明の実施例によれば、7アラデー効果ガ
ラスの反射面は大気と遮断され、結露や大気中の粉塵な
どの影響によって反射効率が低下したシ光軸がずれたシ
することを防ぐことができ、いかなる厳しい気象条件の
下でも正常な直線偏向と光路が保持され、正確な測定が
保証される。
As described above, according to the embodiment of the present invention, the reflective surface of the 7 Allade effect glass is shielded from the atmosphere, and it is possible to prevent the reflection efficiency from decreasing or the optical axis from shifting due to the influence of dew condensation or dust in the atmosphere. normal linear deflection and optical path are maintained under any harsh weather conditions, ensuring accurate measurements.

〔発明の効果〕〔Effect of the invention〕

上記のように本発明によれば、ファラデー効果ガラスの
反射面に反射膜または保護カバーを設けたので、どんな
気象条件の下でも安定したf*Ifの高い電流測定がで
きる光変流器を提供できるようになった効果は犬である
As described above, according to the present invention, a reflective film or a protective cover is provided on the reflective surface of the Faraday effect glass, thereby providing an optical current transformer that can stably measure current with a high f*If under any weather conditions. The effect that can now be done is a dog.

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

第1図はファラデー効果ガラスを用いた光変流器の構造
を示す斜視図、第2図は本発明の光変流器に用いるファ
ラデー効果ガラスの一実施例を示す説明図、第3図は同
じく772デー効果ガラスの他の実施例を示す説明図で
ある。 1・・・偏光子、2・・・ファラデー効果ガ2ス、3・
・・検光子、5・・・光ファイバー、6・・−一次導体
、7・・・反射膜、8・・・保護カバー、a・・・直線
偏光入射光、b・・・直線偏光出射光。 鮭10 3F
FIG. 1 is a perspective view showing the structure of an optical current transformer using Faraday effect glass, FIG. 2 is an explanatory view showing an example of Faraday effect glass used in the optical current transformer of the present invention, and FIG. It is an explanatory view showing another example of the same 772 day effect glass. 1... Polarizer, 2... Faraday effect gas, 3...
...Analyzer, 5...Optical fiber, 6...-Primary conductor, 7...Reflection film, 8...Protective cover, a...Linearly polarized incident light, b...Linearly polarized light emitted. Salmon 10 3F

Claims (1)

【特許請求の範囲】 1、 ファラデー効果ガラスを測定すべき電流が流れる
1次導体と鎖交させ、かつ光路が周回するファラデー効
果ガラ″スの全反射−面に反射膜を設けて、7アラデ一
回転ガラスと大気を遮断した構造となしたことを%徴と
する光変流器。 2、前記反射膜が前記ファラデー効果ガラスと同一もし
くは同等の膨張率をもつ保護カバーであり、この保護カ
バーで前記全反射面と大気を遮断し、しかも光路に当る
部分の全反射面と該保護カバーとが接触しないようにし
たことを特徴とする特許請求の範囲第1項記載の光変流
器。
[Claims] 1. A Faraday effect glass is interlinked with a primary conductor through which the current to be measured flows, and a reflective film is provided on the total reflection surface of the Faraday effect glass around which the optical path circulates. An optical current transformer characterized by having a structure that blocks the single rotation glass and the atmosphere. 2. The reflective film is a protective cover having the same or equivalent expansion coefficient as the Faraday effect glass, and the protective cover 2. The optical current transformer according to claim 1, wherein the total reflection surface and the atmosphere are shielded from each other, and the total reflection surface in a portion corresponding to the optical path does not come into contact with the protective cover.
JP58024615A 1983-02-18 1983-02-18 Optical current transformer Pending JPS59151065A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP58024615A JPS59151065A (en) 1983-02-18 1983-02-18 Optical current transformer

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP58024615A JPS59151065A (en) 1983-02-18 1983-02-18 Optical current transformer

Publications (1)

Publication Number Publication Date
JPS59151065A true JPS59151065A (en) 1984-08-29

Family

ID=12143050

Family Applications (1)

Application Number Title Priority Date Filing Date
JP58024615A Pending JPS59151065A (en) 1983-02-18 1983-02-18 Optical current transformer

Country Status (1)

Country Link
JP (1) JPS59151065A (en)

Cited By (3)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US6862126B2 (en) 2002-03-14 2005-03-01 Fujitsu Limited Transmission wavelength characteristics variable optical element, and wavelength characteristics variable apparatus, optical amplifier, optical transmission system, and control method of transmission wavelength characteristics, using same
US7016096B2 (en) 2002-05-21 2006-03-21 Fujitsu Limited Transmission wavelength characteristics variable optical element, and wavelength characteristics variable apparatus, optical amplifier, and optical transmission system, using same
JP2019090714A (en) * 2017-11-15 2019-06-13 株式会社東芝 Optical magnetic field and current measuring device

Cited By (3)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US6862126B2 (en) 2002-03-14 2005-03-01 Fujitsu Limited Transmission wavelength characteristics variable optical element, and wavelength characteristics variable apparatus, optical amplifier, optical transmission system, and control method of transmission wavelength characteristics, using same
US7016096B2 (en) 2002-05-21 2006-03-21 Fujitsu Limited Transmission wavelength characteristics variable optical element, and wavelength characteristics variable apparatus, optical amplifier, and optical transmission system, using same
JP2019090714A (en) * 2017-11-15 2019-06-13 株式会社東芝 Optical magnetic field and current measuring device

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