JPH0216471B2 - - Google Patents
Info
- Publication number
- JPH0216471B2 JPH0216471B2 JP56139026A JP13902681A JPH0216471B2 JP H0216471 B2 JPH0216471 B2 JP H0216471B2 JP 56139026 A JP56139026 A JP 56139026A JP 13902681 A JP13902681 A JP 13902681A JP H0216471 B2 JPH0216471 B2 JP H0216471B2
- Authority
- JP
- Japan
- Prior art keywords
- magneto
- current
- light
- measuring device
- optical element
- 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 - Lifetime
Links
Classifications
-
- G—PHYSICS
- G01—MEASURING; TESTING
- G01R—MEASURING ELECTRIC VARIABLES; MEASURING MAGNETIC VARIABLES
- G01R15/00—Details of measuring arrangements of the types provided for in groups G01R17/00 - G01R29/00, G01R33/00 - G01R33/26 or G01R35/00
- G01R15/14—Adaptations providing voltage or current isolation, e.g. for high-voltage or high-current networks
- G01R15/24—Adaptations providing voltage or current isolation, e.g. for high-voltage or high-current networks using light-modulating devices
- G01R15/245—Adaptations providing voltage or current isolation, e.g. for high-voltage or high-current networks using light-modulating devices using magneto-optical modulators, e.g. based on the Faraday or Cotton-Mouton effect
- G01R15/246—Adaptations providing voltage or current isolation, e.g. for high-voltage or high-current networks using light-modulating devices using magneto-optical modulators, e.g. based on the Faraday or Cotton-Mouton effect based on the Faraday, i.e. linear magneto-optic, effect
Landscapes
- Engineering & Computer Science (AREA)
- Power Engineering (AREA)
- Physics & Mathematics (AREA)
- General Physics & Mathematics (AREA)
- Measuring Instrument Details And Bridges, And Automatic Balancing Devices (AREA)
Description
【発明の詳細な説明】
本発明は磁気光学素子によるフアラデー回転を
観測して導体中を流れる電流を検出し、その電流
量を測定する電流測定装置に関するもので、その
目的とするところは磁気光学素子に光学特性の温
度変化が小さく、高感度な希土類鉄ガーネツト混
晶を用いることによつて、広い温度範囲にわたつ
て安定して動作し、信頼性が高く小型な電流測定
装置を得ることである。DETAILED DESCRIPTION OF THE INVENTION The present invention relates to a current measuring device that detects a current flowing in a conductor by observing Faraday rotation by a magneto-optical element, and measures the amount of current. By using a highly sensitive rare earth iron garnet mixed crystal with small temperature changes in optical properties for the element, we can obtain a highly reliable and compact current measuring device that operates stably over a wide temperature range. be.
最近、高電圧、電流を測定する従来から周知の
変流器CTに代わつて、フラデー効果を利用して、
光を媒体として非接触で電圧,電流測定する方法
が提案されている。第1図にフアラデー効果を用
いた電圧,電流の測定方法の原理図を示す。第1
図において導体中を流れる電流量に比例して発生
した磁界H中に磁気光学素子1が配置されてい
る。この磁気光学素子1に偏光子2で直線偏光
(矢印で示されている)にされた光を通過させる。 Recently, the Fraday effect has been used to replace the conventionally well-known current transformer CT that measures high voltage and current.
A method for non-contact voltage and current measurement using light as a medium has been proposed. Figure 1 shows the principle of the method for measuring voltage and current using the Faraday effect. 1st
In the figure, a magneto-optical element 1 is placed in a magnetic field H generated in proportion to the amount of current flowing through a conductor. Light that has been linearly polarized (indicated by an arrow) by a polarizer 2 is passed through the magneto-optical element 1 .
フアラデー効果により、偏光面は磁界強度Hに
比例して回転を受ける。その回転角はθで示され
ている。回転を受けた偏光は、偏光子2と透過偏
光方向を異らしめた検光子3を通過し、回転角θ
の大きさが光量変化に変換される。 Due to the Faraday effect, the plane of polarization is rotated in proportion to the magnetic field strength H. Its rotation angle is indicated by θ. The rotated polarized light passes through a polarizer 2 and an analyzer 3 whose transmission polarization direction is different, and the rotation angle θ
The magnitude of is converted into a change in light amount.
例えば、偏光子2と検光子3の透過偏光方向を
45゜異らしめた場合、検光子3を透過したのち
の光量変化は、次式で示される。 For example, when the transmitted polarization directions of the polarizer 2 and the analyzer 3 are different by 45 degrees, the change in the amount of light after passing through the analyzer 3 is expressed by the following equation.
ΔI=κsin2θ ……(1)
ここで、θ=VH,ΔIは光量変化量,κは比
例定数,θはフアラデー回転角〔度〕,Vはヴエ
ルデ定数〔度/cmOe〕,Hは磁界強度〔Oe〕,
は磁気光学素子の厚み〔cm〕である。また、Vは
ヴエルデ定数と呼ばれるもので、単位は〔゜/cm
Oe〕であり、磁気光学素子の感度を表わすもの
である。 ΔI=κsin2θ...(1) Here, θ=VH, ΔI is the amount of change in light intensity, κ is the proportionality constant, θ is the Faraday rotation angle [degrees], V is the Werde constant [degrees/cmOe], and H is the magnetic field strength [degrees]. Oe〕,
is the thickness [cm] of the magneto-optical element. Also, V is called the Werdet constant, and its unit is [°/cm
Oe], which represents the sensitivity of the magneto-optical element.
従来、磁気光学素子としては、鉛ガラス,常磁
性ガラス,又はY3Fe5O12結晶が用いられる場合
が多い。鉛ガラスのヴエルデ定数の温度変化は無
いが、V=0.15×10-2゜/cmOeと小さく、装置が
大型化する欠点がある常磁性ガラス,Y3Fe5O12
結晶のヴエルデ定数の温度変化は大きく、これら
の磁気光学素子を用いた電流測定装置は、周囲温
度変化に対して、測定感度が変化し、測定誤差が
大きいことが最大の欠点である。 Conventionally, lead glass, paramagnetic glass, or Y 3 Fe 5 O 12 crystal is often used as a magneto-optical element. Paramagnetic glass, Y 3 Fe 5 O 12 Although the Welde constant of lead glass does not change with temperature, it is small at V = 0.15 × 10 -2 ° / cmOe and has the disadvantage of increasing the size of the device.
The Welde constant of a crystal changes greatly with temperature, and the biggest drawback of current measuring devices using these magneto-optical elements is that the measurement sensitivity changes with respect to changes in ambient temperature, resulting in large measurement errors.
たとえば、Y3Fe5O12結晶は、ヴエルデ定数が
V=0.21゜/cmOe(室温)と、ガラスにくらべて、
2桁大きなものであるが、第2図に示すように、
その温度変化は大きい。−25℃〜+125℃の温度範
囲で±12%の変化を示している。したがつて、
Y3Fe5O12結晶を用いた電流測定装置の測定誤差
は大きく、たとえば高圧送電線の電流測定のよう
に、周囲温度変化が激しく、しかも装置の高信頼
性が要求される場合の使用には適さない。 For example, Y 3 Fe 5 O 12 crystal has a Werde constant of V=0.21°/cmOe (room temperature), which is higher than that of glass.
Although it is two orders of magnitude larger, as shown in Figure 2,
The temperature change is large. It shows a change of ±12% in the temperature range of -25℃ to +125℃. Therefore,
Current measuring devices using Y 3 Fe 5 O 12 crystals have large measurement errors, making them difficult to use in situations where ambient temperature changes are large and high reliability is required, such as when measuring current on high-voltage power transmission lines. is not suitable.
本発明は、前記従来の欠点を鑑みてなされたも
のであり、ヴエルデ定数の温度変化の極めて小さ
い希土類鉄ガーネツト混晶(TbXY1-X)3Fe5O12
(0.1≦X≦0.3)を用いて、温度変化に安定な信
頼性の高い、電流測定装置を実現したものであ
る。第3図は(TbXY1-X)3Fe5O12のヴエルデ定数
の温度変化を、テルビユウム濃度に対して示す。
温度範囲は−25℃〜+125℃であり、波長1.153μ
mである。第3図に示す通り、(0.1≦X≦0.3)
では、ヴエルデ定数の温度による変化は±6%以
下におさえられY3Fe5O12に比べ温度変化は半分
以下となり電流測定として実用上満足すべきもの
となり、特にX=0.19付でヴエルデ定数の変化
は±1.7%以下の値になつている。又、希土類ガ
ーネツト混晶のヴエルデ定数はV=0.29゜/cmOe
とY3Fe5O12結晶の場合より大きく電流測定装置
として用いた場合には高感度化が可能で装置のよ
り小型化が実現できる。 The present invention has been made in view of the above - mentioned conventional drawbacks, and is a rare earth iron garnet mixed crystal ( Tb
(0.1≦X≦0.3), we have realized a highly reliable current measuring device that is stable against temperature changes. FIG. 3 shows the temperature change of the Werde's constant of (Tb X Y 1-X ) 3 Fe 5 O 12 with respect to the terbium concentration.
Temperature range is -25℃ to +125℃, wavelength 1.153μ
It is m. As shown in Figure 3, (0.1≦X≦0.3)
In this case, the change in Weerde's constant due to temperature is suppressed to less than ±6%, and the temperature change is less than half that of Y 3 Fe 5 O 12 , which is practically satisfactory for current measurement. is less than ±1.7%. Also, the Werde constant of rare earth garnet mixed crystal is V=0.29°/cmOe
When used as a current measuring device, it is possible to increase the sensitivity and make the device more compact.
以下に本発明の実施例における電流測定装置を
説明する。 A current measuring device according to an embodiment of the present invention will be described below.
第4図に、本発明の実施例による電流測定装置
の構成を示す。同図において、1は(Tb0.19
Y00.81)3Fe5O12結晶よりなる磁気光学素子であり、
その厚さが1mmになるように両側面が平行に研磨
されている。2は磁気光学素子1の1端面に設け
られた偏光子であり、3は磁気光学素子1の他面
に設けられ、かつ偏光子2に対して透過偏光方向
が45゜傾くよう設置された検光子である。偏光子、
検光子としては温度変化に対して偏光特性が良好
なグラントムソンプリズムを用いた。磁気光学素
子1,偏光子2,検光子3より構成される磁気光
学変換部は、電流通過導体4より60cmの間隔をお
いて配置されている。5,6はそれぞれセルフオ
ツクレンズで磁気光学変換部に入射する光又は磁
気光学変換部を透過した光を平行光線にするため
のものである。7,8は光伝送路を形成するオプ
テイカルフアイバーである。9はフアイバー7に
光を入射する光源であり、光の波長としては
(Tb0.19Y0.81)3Fe5O12結晶に対して透過度がよい
波長1.0μm〜1.6μmの範囲のうち、波長1.153μm
のものを用いた。10は、磁気光学変換部を透過
した光出力を検知する光検知手段で、ここで検知
した光強度に応じて電気信号に変換される。 FIG. 4 shows the configuration of a current measuring device according to an embodiment of the present invention. In the same figure, 1 is (Tb 0.19
Y 00.81 ) 3 Fe 5 O 12 is a magneto-optical element made of crystal,
Both sides are polished parallel to each other so that the thickness is 1 mm. 2 is a polarizer provided on one end surface of the magneto-optical element 1, and 3 is a polarizer provided on the other surface of the magneto-optical element 1, and is installed so that the transmitted polarization direction is inclined by 45 degrees with respect to the polarizer 2. It is a photon. polarizer,
A Glan-Thompson prism, which has good polarization characteristics against temperature changes, was used as the analyzer. A magneto-optic converter composed of a magneto-optical element 1, a polarizer 2, and an analyzer 3 is arranged at a distance of 60 cm from the current passing conductor 4. Reference numerals 5 and 6 denote self-occurring lenses for converting the light incident on the magneto-optic conversion section or the light transmitted through the magneto-optic conversion section into parallel light beams. 7 and 8 are optical fibers forming an optical transmission path. 9 is a light source that inputs light into the fiber 7, and the wavelength of the light is (Tb 0.19 Y 0.81 ) 3 Fe 5 O 12 Among the wavelength range of 1.0 μm to 1.6 μm that has good transmittance to the crystal, the wavelength is 1.153 μm. μm
I used the one from Reference numeral 10 denotes a light detection means for detecting the light output transmitted through the magneto-optic converter, and converts it into an electric signal according to the light intensity detected here.
このような構成において、電流通過導体4と磁
気光学変換部との距離を変化させるか、磁気光学
素子1の厚みを変えることによつて、100KAオ
ーダまでの電流量の検知が可能であつた。この場
合、室温から100℃の温度変化に対して、測定誤
差は、わずか±2%以下であつた。 In such a configuration, by changing the distance between the current passing conductor 4 and the magneto-optic conversion section or by changing the thickness of the magneto-optic element 1, it was possible to detect a current amount of up to 100 KA order. In this case, the measurement error was only ±2% or less for a temperature change from room temperature to 100°C.
以上述べたことから明らかなように、本発明の
電流測定装置によれば、磁気光学素子の周囲の電
流検出手段として何ら特別のものを用いることな
く、通常の電流測定における手段を用いて電流導
体中の電流量を感度良く、かつ環境の温度変化に
影響されずに高精度で測定できるものであり、そ
の工業的価値は大なるものがある。 As is clear from the above description, according to the current measuring device of the present invention, a current conductor can be detected by using ordinary current measuring means without using any special current detecting means around the magneto-optical element. It is possible to measure the amount of current in the air with high sensitivity and high precision without being affected by environmental temperature changes, and has great industrial value.
第1図は、フアラデー効果を用いた電流測定装
置の基本原理を説明するための図、第2図は、
Y3Fe5O12のヴエルデ定数の温度変化を示す図、
第3図は、(TbXY1-X)3Fe5O12のヴエルデ定数の
温度変化分を、テルビユウム濃度Xに対してプロ
ツトした図、第4図は、本発明の一実施例におけ
る電流測定装置の構成を示す図である。
1……磁気光学素子、2……偏光子、3……検
光子、4……電流通過導体、7,8……オプテイ
カルフアイバ、9……光源、10……光検知手
段。
Figure 1 is a diagram for explaining the basic principle of a current measuring device using the Faraday effect, and Figure 2 is a diagram for explaining the basic principle of a current measuring device using the Faraday effect.
A diagram showing the temperature change of the Werde constant of Y 3 Fe 5 O 12 ,
FIG. 3 is a diagram plotting the temperature change of the Werde constant of (Tb X Y 1-X ) 3 Fe 5 O 12 against the terbium concentration X, and FIG. FIG. 2 is a diagram showing the configuration of a measuring device. DESCRIPTION OF SYMBOLS 1... Magneto-optical element, 2... Polarizer, 3... Analyzer, 4... Current passing conductor, 7, 8... Optical fiber, 9... Light source, 10... Light detection means.
Claims (1)
光子との間に一般式(TbXY1-X)3Fe5O12(0.1≦X
≦0.3)で示される希土類鉄ガーネツト混晶より
なる磁気光学素子を配置した磁気光学変換部と、
前記磁気光学変換部の両端に設けられた光伝送路
と、前記光伝送路に光を入射する光発生手段と、
前記入射光が前記磁気光学変換部を透過した後の
出力を検知する検知手段とを備え、前記磁気光学
変換部を電流導体近傍に配置することにより、前
記電流導体を流れる電流量を前記検知部で検出す
ることを特徴とする電流測定装置。1 The general formula (Tb X Y 1-X ) 3 Fe 5 O 12 (0.1≦X
≦0.3);
an optical transmission path provided at both ends of the magneto-optic converter; a light generating means for inputting light into the optical transmission path;
and a detection means for detecting an output after the incident light passes through the magneto-optic conversion section, and by arranging the magneto-optic conversion section near the current conductor, the amount of current flowing through the current conductor can be detected by the detection section. A current measuring device characterized by detecting.
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP56139026A JPS5839953A (en) | 1981-09-02 | 1981-09-02 | Measuring apparatus of electric current |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP56139026A JPS5839953A (en) | 1981-09-02 | 1981-09-02 | Measuring apparatus of electric current |
Publications (2)
| Publication Number | Publication Date |
|---|---|
| JPS5839953A JPS5839953A (en) | 1983-03-08 |
| JPH0216471B2 true JPH0216471B2 (en) | 1990-04-17 |
Family
ID=15235730
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP56139026A Granted JPS5839953A (en) | 1981-09-02 | 1981-09-02 | Measuring apparatus of electric current |
Country Status (1)
| Country | Link |
|---|---|
| JP (1) | JPS5839953A (en) |
Families Citing this family (2)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| GB9201896D0 (en) * | 1992-01-29 | 1992-03-18 | Instr Transformers Ltd | Electric current measurement |
| US12539898B2 (en) | 2021-06-11 | 2026-02-03 | Pellerin Milnor Corporation | Overhead rail and trolley system |
Family Cites Families (1)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| JPS5735760A (en) * | 1980-08-14 | 1982-02-26 | Matsushita Electric Ind Co Ltd | Current measuring device |
-
1981
- 1981-09-02 JP JP56139026A patent/JPS5839953A/en active Granted
Also Published As
| Publication number | Publication date |
|---|---|
| JPS5839953A (en) | 1983-03-08 |
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