JPH01302174A - Current measuring apparatus - Google Patents
Current measuring apparatusInfo
- Publication number
- JPH01302174A JPH01302174A JP63133168A JP13316888A JPH01302174A JP H01302174 A JPH01302174 A JP H01302174A JP 63133168 A JP63133168 A JP 63133168A JP 13316888 A JP13316888 A JP 13316888A JP H01302174 A JPH01302174 A JP H01302174A
- Authority
- JP
- Japan
- Prior art keywords
- light
- optical
- magnetic field
- field sensor
- current
- 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
Links
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- Measuring Instrument Details And Bridges, And Automatic Balancing Devices (AREA)
Abstract
Description
【発明の詳細な説明】
〔産業上の利用分野〕
本発明は、屋内変電所等に設置された高圧電線を流れる
電流の大きさを、ファラデー効果を利用した光磁界セン
サを用いて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 measurement method that measures the magnitude of current flowing through a high-voltage electric wire installed in an indoor substation, etc. using an optical magnetic field sensor that utilizes the Faraday effect. This relates to a measuring device.
ファラデー効果を利用して、電線を流れる電流を測定す
ることは公知であり、第3図は、例えば昭和60年1月
、情報調査会発行の「光フアイバセンサ〈基礎と応用〉
」のP、111に示された従来の電流測定装置の構成を
示すブロック図である。It is well known that the Faraday effect can be used to measure the current flowing through an electric wire.
111 is a block diagram showing the configuration of the conventional current measuring device shown in P.
図において1は光送信器を示し、光送信器1には送光用
光ファイバ31の端面が接続されており、また該送光用
光ファイバ31の他端面ば、光磁界セフサ2内のマイク
ロレンズ32に当接している。光磁界センサ2は、この
マイクロレンズ32、偏光子3、ファラデー素子4.検
光子5及びマイクロレンズ33を光学的に結合して構成
されている。マイクロレンズ33には受光用光ファイバ
34の端面が当接しており、該受光用光ファイバ34の
他端面ば、受光した光の光量を電気量に変換して電気信
号を出力する光受信器6に接続されている。In the figure, reference numeral 1 denotes an optical transmitter, to which the end face of a light transmitting optical fiber 31 is connected, and the other end face of the light transmitting optical fiber 31 is connected to a microelectromagnetic field sensor 2. It is in contact with the lens 32. The optical magnetic field sensor 2 includes the microlens 32, the polarizer 3, the Faraday element 4. It is constructed by optically coupling an analyzer 5 and a microlens 33. An end face of a light-receiving optical fiber 34 is in contact with the microlens 33, and the other end face of the light-receiving optical fiber 34 is an optical receiver 6 that converts the amount of received light into an amount of electricity and outputs an electric signal. It is connected to the.
次に動作について説明する。Next, the operation will be explained.
光送信器1から出射された光は送光用光ファイバ31に
よって光磁界センサ2に導入される。光磁界センサ2に
導入された光はマイクロレンズ32により平行光線に変
換され、偏光子3によって直線偏光される。偏光子3か
ら出射される直線偏光波は、ファラデー素子4内を伝播
する間にその偏光面が、光の進行方向と平行な外部磁界
が存在する場合、その磁界の強さに応じてファラデー回
転される。この回転角は、検光子5にて強度変調に変換
され、マイクロレンズ33.受光用光ファイバ34を通
して光受信器6にて光/電気変換される。この電気出力
を測定することにより、光磁界センサ2の周囲の外部の
被測定磁界を測定できる。電線を流れる電流はその値に
比例した磁界を発生しているので、測定された磁界から
電線を流れる電流を知ることができる。Light emitted from the optical transmitter 1 is introduced into the optical magnetic field sensor 2 through a light transmitting optical fiber 31. The light introduced into the optical magnetic field sensor 2 is converted into parallel light by the microlens 32 and linearly polarized by the polarizer 3. When the linearly polarized light wave emitted from the polarizer 3 is propagated in the Faraday element 4, its plane of polarization undergoes Faraday rotation depending on the strength of the magnetic field when an external magnetic field is parallel to the traveling direction of the light. be done. This rotation angle is converted into intensity modulation by the analyzer 5, and the microlens 33. The light is passed through the light-receiving optical fiber 34 and subjected to optical/electrical conversion at the optical receiver 6. By measuring this electrical output, the external magnetic field to be measured around the optical magnetic field sensor 2 can be measured. Since the current flowing through the wire generates a magnetic field proportional to its value, the current flowing through the wire can be determined from the measured magnetic field.
上述したような従来の電流測定装置では、光送信器1と
光磁界センサ2との間、光磁界センサ2と光受信器6と
の間は、光ファイバにて接続されているので、光ファイ
バの外被の樹脂が紫外線等にて劣化する場合には、塩害
の影響を受は易くなって絶縁性能が低下する。この結果
、絶縁性能に対する要求が厳しい高圧電線においては使
用できないという問題点がある。In the conventional current measuring device as described above, the optical transmitter 1 and the optical magnetic field sensor 2 are connected by optical fibers, and the optical magnetic field sensor 2 and the optical receiver 6 are connected by optical fibers. If the resin of the outer covering deteriorates due to ultraviolet rays or the like, it becomes susceptible to salt damage and the insulation performance decreases. As a result, there is a problem that it cannot be used in high-voltage electric wires that have strict requirements for insulation performance.
また、光磁界センサを電線に取付けるために一次的に送
電を停止する必要があるという難点がある。Another drawback is that power transmission must be temporarily stopped in order to attach the optical magnetic field sensor to the electric wire.
本発明はかかる事情に鑑みてなされたものであり、光送
信器及び光受信器と光磁界センサとの間で光を空間伝送
することとし、また光磁界センサを対象物(電線)に着
脱可能に取付けるための取付機構を備えることにより、
光ファイバを使用しないので絶縁性能低下の心配がなく
なって、高圧電線においても使用でき、しかも光磁界セ
ンサを電線に取付ける際に一次的に送電を停止すること
が不要である電流測定装置を提供することを目的とする
。The present invention has been made in view of the above circumstances, and is capable of spatially transmitting light between an optical transmitter, an optical receiver, and an optical magnetic field sensor, and also allows the optical magnetic field sensor to be attached to and detached from an object (electrical wire). By providing a mounting mechanism for attaching to
To provide a current measuring device which does not use an optical fiber so there is no need to worry about deterioration of insulation performance, can be used even on high-voltage electric wires, and does not require temporarily stopping power transmission when attaching an optical magnetic field sensor to the electric wires. The purpose is to
また、光送信器から光磁界センサへの光と光磁界センサ
から光受信器への光とが同一の光路を有することにより
、光送信器、光受信器と光磁界センサとの光軸合わせが
簡便である電流測定装置を提供することを目的とする。In addition, since the light from the optical transmitter to the optical magnetic field sensor and the light from the optical magnetic field sensor to the optical receiver have the same optical path, the optical axes of the optical transmitter, optical receiver, and optical magnetic field sensor can be aligned. The object is to provide a simple current measuring device.
更に、光送信器からの光を用いて光磁界センサの像を得
ることにより、光送信器、光受信器と光磁界センサとの
光軸合わせが容易である電流測定装置を提供することを
目的とする。Furthermore, it is an object of the present invention to provide a current measuring device in which the optical axes of the optical transmitter, the optical receiver, and the optical magnetic field sensor can be easily aligned by obtaining an image of the optical magnetic field sensor using light from the optical transmitter. shall be.
本発明に係る電流測定装置は、送光部から光磁界センサ
への光、及び光磁界センサから受光部への光を空間伝送
する構成とし、また光磁界センサを対象物に着脱可能に
取付けるための取付機構を具備することを特徴とする。The current measuring device according to the present invention has a configuration that spatially transmits light from a light transmitting section to a magneto-optical field sensor and light from a magneto-optic field sensor to a light receiving section, and also has a structure in which the magneto-optic field sensor is detachably attached to an object. It is characterized by having a mounting mechanism.
本発明の電流測定装置にあっては、送光部から出射され
た光は空間を介して光磁界センサへ入射され、また光磁
界センサから出射された光は空間を介して受光部へ入射
される。従って光を伝送するための光ファイバは不要で
あり、光ファイバの劣化に伴う絶縁性能低下の虞がない
。また、取付機構を用いて光磁界センサを着脱可能に対
象物に取付けることができるので、送電を停止すること
なく光磁界センサを対象物に取付けれる。In the current measuring device of the present invention, the light emitted from the light transmitting section is incident on the optical magnetic field sensor through the space, and the light emitted from the optical magnetic field sensor is incident on the light receiving section through the space. Ru. Therefore, there is no need for an optical fiber for transmitting light, and there is no risk of deterioration in insulation performance due to deterioration of the optical fiber. Furthermore, since the optical magnetic field sensor can be detachably attached to the object using the attachment mechanism, the optical magnetic field sensor can be attached to the object without stopping power transmission.
また、送光部からの光の光路と受光部への光の光路とが
一致しており、光路の軸合わせは1本ですみ、光軸合わ
せは簡便である。In addition, the optical path of the light from the light transmitting section and the optical path of the light to the light receiving section coincide with each other, and alignment of the optical paths can be performed using only one optical path, making it easy to align the optical axes.
更に、光磁界センサの像を得ることができる。Furthermore, an image of the optical magnetic field sensor can be obtained.
従ってこの像の目視によって光軸合わせを行なえるので
、その光軸合わせの作業は容易である。Therefore, since the optical axis can be aligned by visually observing this image, the optical axis alignment operation is easy.
以下、本発明をその実施例を示す図面に基づいて具体的
に説明する。DESCRIPTION OF THE PREFERRED EMBODIMENTS The present invention will be specifically described below based on drawings showing embodiments thereof.
第1図は本発明に係る電流測定装置の構成を示す模式図
であり、図においてAは測定対象物たる高圧電線、2は
高圧電線Aに取付けられた光磁界センサ、11は地上に
配置された地上側装置を示す。FIG. 1 is a schematic diagram showing the configuration of a current measuring device according to the present invention. In the figure, A is a high-voltage electric wire as an object to be measured, 2 is an optical magnetic field sensor attached to high-voltage electric wire A, and 11 is a sensor placed on the ground. This figure shows the ground-side equipment.
高圧電線Aは空中に配されており、該高圧電線Aには、
バネを利用した取付機構lOにより光磁界センサ2が取
付けられている。光磁界センサ2は、その入射側から、
プリズム8a+偏光子3.ファラデー素子4.検光子5
.プリズム8bをこの順に光学的に結合して構成されて
いる。High-voltage electric wire A is placed in the air, and the high-voltage electric wire A has
The optical magnetic field sensor 2 is attached by an attachment mechanism lO using a spring. The optical magnetic field sensor 2 has, from its incident side,
Prism 8a + polarizer 3. Faraday element 4. Analyzer 5
.. The prisms 8b are optically coupled in this order.
地上側装置11は、光を光磁界センサ2へ送信する光送
信器l、光送信器lからの光を平行光として光磁界セン
サ2 (プリズム8a)に向けて出射するレンズ7a、
光磁界センサ2 (プリズム8b)からの光を集束させ
るレンズ7b、レンズ7bからの集束光を受光し、電気
信号に変換して出力する光受信器6、及び光受信器6の
出力信号に基づいて高圧電線Aの電流を測定する信号処
理回路9を具備する。The ground-side device 11 includes an optical transmitter l that transmits light to the optical magnetic field sensor 2, a lens 7a that emits the light from the optical transmitter l as parallel light toward the optical magnetic field sensor 2 (prism 8a),
Based on the lens 7b that focuses the light from the optical magnetic field sensor 2 (prism 8b), the optical receiver 6 that receives the focused light from the lens 7b, converts it into an electrical signal and outputs it, and the output signal of the optical receiver 6. A signal processing circuit 9 is provided for measuring the current of the high voltage electric wire A.
次に動作について説明する。Next, the operation will be explained.
まず、絶縁棒を使用して取付機構10を高圧電線Aに装
着させる操作を行って、光磁界センサ2を高圧電線Aに
取付ける。First, the optical magnetic field sensor 2 is attached to the high-voltage electric wire A by attaching the attachment mechanism 10 to the high-voltage electric wire A using an insulating rod.
光発信器1から出射された光はレンズ7aにて平行光と
なる。この平行光は空間を通過して(矢符B方向)、プ
リズム8aに入射し、その進路が90’曲げられた後、
偏光子3にて直線偏光される。直線偏光された光(直線
偏光波)は、ファラデー素子4を通過する間に、高圧電
線Aを流れる電流の大きさによって発生された磁界の強
さに比例してその偏光面が回転し、検光子5により強度
変調される。The light emitted from the optical transmitter 1 becomes parallel light at the lens 7a. This parallel light passes through space (in the direction of arrow B), enters the prism 8a, and after its path is bent by 90',
The light is linearly polarized by the polarizer 3. While the linearly polarized light (linearly polarized wave) passes through the Faraday element 4, its plane of polarization rotates in proportion to the strength of the magnetic field generated by the magnitude of the current flowing through the high-voltage wire A, and is detected. The intensity is modulated by photons 5.
強度変調された光は、プリズム8bにて進路が90”曲
げられた後、再び空間を通過して(矢符C方向)プリズ
ム7b (地上側装置11)に入射し、集束光となる。After the path of the intensity-modulated light is bent by 90'' at the prism 8b, it passes through space again (in the direction of arrow C) and enters the prism 7b (ground-side device 11), where it becomes a focused light.
集束光は光受信器6にて受光されて光電変換され、光量
に応じた電気信号が信号処理回路9へ出力される。信号
処理回路9は入力した電気信号により、高圧Tl線Aの
電流を測定する。The focused light is received by the optical receiver 6 and photoelectrically converted, and an electrical signal corresponding to the amount of light is output to the signal processing circuit 9. The signal processing circuit 9 measures the current of the high voltage Tl line A based on the input electric signal.
本実施例では、地上側装置11.光磁界センサ2間にお
いて光を空間伝送しているので、従来のように光伝送用
の光ファイバが不要であるので、絶縁信顛性が高く、高
圧電線の電流を測定することができる。また、光磁界セ
ンサの電線への着脱が自在であるので、光磁界センサの
取付時に送電を停止させなくてもよい。In this embodiment, the ground side device 11. Since light is spatially transmitted between the optical magnetic field sensors 2, there is no need for an optical fiber for light transmission unlike in the past, so insulation reliability is high and current in high voltage electric wires can be measured. Further, since the optical magnetic field sensor can be freely attached to and removed from the electric wire, there is no need to stop power transmission when the optical magnetic field sensor is attached.
第2図は本発明に係る電流測定装置の別の実施例の構成
を示す模式図であって、図中Aは高圧電線、2は光磁界
センサ、11は地上側装置であり、高圧電線Aには前述
の実施例と同様に、バネを利用した取付機構10により
光磁界センサ2が取付けられている。本実施例における
磁界センサ2は、ファラデー素子4と該ファラデー素子
4の一端面に被着された反射膜14とから構成されてお
り、偏光子3及び検光子5は地上側装置11内に収納さ
れている。FIG. 2 is a schematic diagram showing the configuration of another embodiment of the current measuring device according to the present invention, in which A is a high-voltage electric wire, 2 is an optical magnetic field sensor, 11 is a ground-side device, and the high-voltage electric wire A As in the previous embodiment, the optical magnetic field sensor 2 is mounted on the mounting mechanism 10 using a spring. The magnetic field sensor 2 in this embodiment is composed of a Faraday element 4 and a reflective film 14 attached to one end surface of the Faraday element 4, and the polarizer 3 and analyzer 5 are housed in the ground-side device 11. has been done.
地上側装置11は、上述の偏光子3.検光子5に加えて
、光を送信する光送信器1、光送信器1からの光を平行
光とするレンズ7a、偏光子3からの光と検光子5への
光とを1本の光路にする光合分配器12、光送信器1か
らの光と同波長域の光のみを透過させる光学フィルタ1
5、検光子5を通過した平行光を集束させるレンズ7b
、レンズ7bからの集束光を受光し、電気信号に変換し
て出力する光受信器6、光受信器6の出力信号に基づい
て高圧電&JIAの電流を測定する信号処理回路9、光
磁界センサ2からの戻り光の一部を分配する光分配器1
3、光分配器13からの分配光を集束させるレンズ7c
、及びレンズ7cからの集束光を受光して光磁界センサ
2の像を結ぶ半透明板16を具備する。The ground side device 11 includes the above-mentioned polarizer 3. In addition to the analyzer 5, there is an optical transmitter 1 that transmits light, a lens 7a that converts the light from the optical transmitter 1 into parallel light, and a single optical path that connects the light from the polarizer 3 and the light to the analyzer 5. an optical filter 1 that transmits only light in the same wavelength range as the light from the optical transmitter 1;
5. Lens 7b that focuses the parallel light that has passed through the analyzer 5
, an optical receiver 6 that receives the focused light from the lens 7b, converts it into an electrical signal and outputs it, a signal processing circuit 9 that measures the high voltage electric & JIA current based on the output signal of the optical receiver 6, and an optical magnetic field sensor. a light distributor 1 that distributes a portion of the return light from 2;
3. Lens 7c that focuses the distributed light from the optical splitter 13
, and a semi-transparent plate 16 that receives the focused light from the lens 7c and forms an image of the optical magnetic field sensor 2.
次に動作について説明する。Next, the operation will be explained.
前述の実施例と同様に、まず、絶縁棒を使用して取付機
構10を高圧電線Aに装着させる操作を行 □って、
光磁界センサ2を高圧電線Aに取付ける。As in the previous embodiment, first, attach the attachment mechanism 10 to the high-voltage wire A using an insulating rod.
Attach the optical magnetic field sensor 2 to the high voltage electric wire A.
光発信器lから出射された光はレンズ7aにて平行光と
なった後、偏光子3にて直線偏光されて直線偏光波とな
る。直線偏光波は光合分配器12にてその進路が90°
曲げられ、光分配器13を通過した後、地上側装置11
外へ出る。地上側装置11外へ出た直線偏光波は空間を
通過して(矢符り方向)、光磁界センサ2 (ファラデ
ー素子4)内に入射する。ファラデー素子4を通過する
間に、直線偏光波は、高圧電線Aを流れる電流によって
発生する磁界の強さに比例してその偏光面が回転し、そ
の後反射膜14にて反射して元の光路を戻る間に、前記
偏光面の回転角と同じ角度だけ偏光面が更に回転する。The light emitted from the optical transmitter l becomes parallel light by the lens 7a, and then linearly polarized by the polarizer 3 to become a linearly polarized light wave. The course of the linearly polarized light wave is 90° at the optical combiner/distributor 12.
After being bent and passing through the light distributor 13, the ground side device 11
Go outside. The linearly polarized light wave exiting the ground-side device 11 passes through space (in the direction of the arrow) and enters the optical magnetic field sensor 2 (Faraday element 4). While passing through the Faraday element 4, the plane of polarization of the linearly polarized light wave rotates in proportion to the strength of the magnetic field generated by the current flowing through the high-voltage wire A, and is then reflected by the reflective film 14 to return to the original optical path. During the return, the plane of polarization is further rotated by the same angle as the rotation angle of the plane of polarization.
磁界の強さに応じてその偏光面が回転した直線偏光波は
、光磁界センサ2外に出射し、前と同一の光路にて空間
を通過しく矢符E方向)、再び地上側装置ll内に入射
する。The linearly polarized light wave whose polarization plane has been rotated according to the strength of the magnetic field is emitted outside the optical magnetic field sensor 2, passes through the space along the same optical path as before (in the direction of arrow E), and returns to the inside of the ground-side device ll. incident on .
地上側装置11内に入射した直線偏光波は、光分配器1
3にてその一部が屈折され、残りの大部分は光分配器1
3及び光合分配器12内を直進し、光学フィルタ19を
透過して外乱光が除去される。外乱光が除去された直線
偏光波は、検光子5にて強度変調を受けた後、レンズ7
bにて集束され、その集束光は光受信器6に入射する。The linearly polarized light wave incident on the ground side device 11 is transmitted to the optical splitter 1
A part of the light is refracted by the light splitter 1, and most of the remaining light is refracted by the light splitter 1.
3 and the light combiner/distributor 12, and is transmitted through the optical filter 19 to remove the disturbance light. The linearly polarized light wave from which the disturbance light has been removed undergoes intensity modulation at the analyzer 5, and then passes through the lens 7.
b, and the focused light enters the optical receiver 6.
光受信器6はこの集束光を受光して光電変換し、光量に
応じた電気信号を信号処理回路9へ出力する。信号処理
回路9は入力した電気信号により、高圧電線Aの電流を
測定する。The optical receiver 6 receives this focused light, performs photoelectric conversion, and outputs an electric signal corresponding to the amount of light to the signal processing circuit 9. The signal processing circuit 9 measures the current of the high-voltage electric wire A based on the input electric signal.
光分配器13にて屈折された光は、レンズ7cにて集束
され、光磁界センサ2の像が半透明板16に結像される
。The light refracted by the optical distributor 13 is focused by the lens 7c, and the image of the optical magnetic field sensor 2 is formed on the semi-transparent plate 16.
本実施例では、前述の実施例と同様に、地上側装置11
.光磁界センサ2間において光を空間伝送しているので
、高圧電線の電流を測定するこ止ができ、また、光磁界
センサ2取付時に送電を停止することが不要である。In this embodiment, as in the previous embodiment, the ground side device 11
.. Since light is spatially transmitted between the optical magnetic field sensors 2, it is possible to stop measuring the current in the high voltage electric wire, and there is no need to stop power transmission when the optical magnetic field sensors 2 are attached.
ところで伝送媒体として光ファイバを使用せず、光の空
間伝送を利用して離隔した位置にある対象物(電線)の
電流を測定するように構成した本発明の電流測定装置に
あっては、地上側装置11.光磁界センサ2間の光軸を
正確に設定することが必要である。By the way, the current measuring device of the present invention, which is configured to measure the current of a distant object (electrical wire) by using spatial transmission of light without using an optical fiber as a transmission medium, can be used on the ground. Side device 11. It is necessary to accurately set the optical axis between the optical magnetic field sensors 2.
上述の実施例では、光の往路(地上側装置11から光磁
界センサ2へ向かう光路)と光の復路(光磁界センサ2
から地上側装置11へ向かう光路)とを一致させ、また
光磁界センサ2の像を得られるようになっているので、
両者間の光軸設定は比較的容易である。この光軸設定は
具体的には以下の如く行なえる。In the above embodiment, the outgoing path of light (the optical path from the ground side device 11 to the optical magnetic field sensor 2) and the returning path of light (the optical path from the optical magnetic field sensor 2)
This makes it possible to match the optical path (from
Setting the optical axis between the two is relatively easy. Specifically, this optical axis setting can be performed as follows.
即ち、光磁界センサ2を高圧電線Aに取付けた後、半透
明板16の中央に光磁界センサ2の像が位置するように
地上側装置11を位置決めし、更に光送信器1から出射
して光磁界センサ2から戻る光が光磁界センサ2の像と
重なるように地上側装置11を位置決めすると、この位
置が往路と復路の光路が一致する位置となる。なおより
正確には、光受信器6の電気出力が最大となるように地
上側装置11の位置を微調整する。That is, after attaching the optical magnetic field sensor 2 to the high-voltage electric wire A, the ground-side device 11 is positioned so that the image of the optical magnetic field sensor 2 is located at the center of the semi-transparent plate 16, and then the image is emitted from the optical transmitter 1. When the ground-side device 11 is positioned so that the light returning from the magneto-optical field sensor 2 overlaps the image of the magneto-optical field sensor 2, this position becomes a position where the optical paths of the outward and return paths coincide. More precisely, the position of the ground-side device 11 is finely adjusted so that the electrical output of the optical receiver 6 is maximized.
以上のような光軸設定のためのすべての操作は、高圧電
線Aから離隔した位置(地上側)にて行なえるので、そ
の操作は容易である。All the operations for setting the optical axis as described above can be performed at a position away from the high-voltage electric wire A (on the ground side), so the operations are easy.
なお上述した例では、信号光以外の外乱光の影響による
誤差を除くために光学フィルタ15を地上側装置ll内
に設ける構成としたが、予め光受信器6内に内蔵してお
いてもよく、また外乱光の影響による誤差が無視できる
場合には設けないこととしてもよい。In the above example, the optical filter 15 is provided in the ground-side device 11 in order to remove errors due to the influence of disturbance light other than the signal light, but it may be built in the optical receiver 6 in advance. , or may not be provided if the error due to the influence of ambient light can be ignored.
また、光磁界センサ2の像を得るための光学系(光分配
器13.レンズ7c及び半透明板16)を設けない場合
にあっても、往路と復路の光路を一致させたことによる
光路設定作業の容易さは保持される。Furthermore, even if an optical system (light distributor 13, lens 7c, and semitransparent plate 16) for obtaining an image of the magneto-optical field sensor 2 is not provided, the optical path can be set by making the optical paths of the outgoing and returning paths coincide. Ease of work is preserved.
以上詳述した如く本発明の電流測定装置では、光送信器
、光受信器と光磁界センサとの間の光を空間伝送するの
で、絶縁信顛性が高く、高圧電線においても電流を測定
することができる。As detailed above, the current measuring device of the present invention spatially transmits light between the optical transmitter, the optical receiver, and the optical magnetic field sensor, so it has high insulation reliability and can measure current even in high-voltage electric wires. be able to.
また、光磁界センサを対象物に取付けるための取付機構
を備えているので、光磁界センサの取付時に対象物への
送電を停止する必要がない。Further, since a mounting mechanism for attaching the optical magnetic field sensor to the object is provided, there is no need to stop power transmission to the object when attaching the optical magnetic field sensor.
また、光磁界センサへの光路と光磁界センサからの光路
とを同一としているので、光送信器、光受信器と光磁界
との間の光軸合わせが1回ですみ、その操作は簡便であ
る。In addition, since the optical path to the optical magnetic field sensor and the optical path from the optical magnetic field sensor are the same, the optical axis alignment between the optical transmitter, optical receiver, and optical magnetic field only needs to be done once, and the operation is simple. be.
更に、光磁界センサの像を目視にて観察しながら光路の
設定が行なえるので、上述の光軸合わせは容易である。Furthermore, since the optical path can be set while visually observing the image of the optical magnetic field sensor, the above-mentioned optical axis alignment is easy.
第1図は本発明に係る電流測定装置の構成を示す模式図
、第2図は本発明に係る電流測定装置の別の実施例の構
成を示す模式図、第3図は従来の電流測定装置の構成を
示す模式図である。
1・・・光送信器 2・・・光磁界センサ 3・・・偏
光子4・・・ファラデー素子 5・・・検光子 6・・
・光受信器10・・・取付機構 11・・・地上側装置
12・・・光合分配器13・・・光分配器 16・・
・半透明板 A・・・高圧電線なお、図中、同一符号は
同一、又は相当部分を示す。FIG. 1 is a schematic diagram showing the configuration of a current measuring device according to the present invention, FIG. 2 is a schematic diagram showing the configuration of another embodiment of the current measuring device according to the present invention, and FIG. 3 is a conventional current measuring device FIG. 1... Optical transmitter 2... Optical magnetic field sensor 3... Polarizer 4... Faraday element 5... Analyzer 6...
- Optical receiver 10... Mounting mechanism 11... Ground side device 12... Optical combiner/distributor 13... Optical distributor 16...
・Semi-transparent plate A...High-voltage electric wire In the figures, the same reference numerals indicate the same or equivalent parts.
Claims (1)
電流測定装置において、 前記対象物に取付けられ、磁界の変化に感応する光磁界
センサと、 空間を介して前記光磁界センサへ光を送光する送光部と
、 空間を介して前記光磁界センサからの光を受光する受光
部と、 該受光部の受光強度に基づき前記対象物の電流を検出す
る電流検出部と、 前記光磁界センサを前記対象物に着脱自在に取付ける取
付機構と を具備することを特徴とする電流測定装置。 2、前記送光部から前記光磁界センサへの光路と前記光
磁界センサから前記受光部への光路とが一致すべく、前
記送光部からの光及び/または前記受光部への光の光路
を変更する光路変更手段と、 前記送光部から送光され、前記光磁界センサを通過した
光にて得られる前記光磁界センサの像を結ぶ結像手段と を備えた請求項1記載の電流測定装置。[Claims] 1. A current measuring device that measures the current of an object using the Faraday effect, comprising: an optical magnetic field sensor that is attached to the object and is sensitive to changes in a magnetic field; a light transmitting section that transmits light to the magnetic field sensor; a light receiving section that receives light from the optical magnetic field sensor via space; and a current detecting section that detects the current of the object based on the received light intensity of the light receiving section. A current measuring device comprising: and an attachment mechanism for detachably attaching the optical magnetic field sensor to the object. 2. The optical path of the light from the light transmitting unit and/or the light to the light receiving unit is adjusted so that the optical path from the light transmitting unit to the optical magnetic field sensor and the optical path from the optical magnetic field sensor to the light receiving unit match. 2. The current according to claim 1, further comprising: an optical path changing means for changing the current; and an imaging means for forming an image of the magneto-optical field sensor obtained by light transmitted from the light transmitting section and passed through the magneto-optical field sensor. measuring device.
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP63133168A JPH01302174A (en) | 1988-05-31 | 1988-05-31 | Current measuring apparatus |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP63133168A JPH01302174A (en) | 1988-05-31 | 1988-05-31 | Current measuring apparatus |
Publications (1)
| Publication Number | Publication Date |
|---|---|
| JPH01302174A true JPH01302174A (en) | 1989-12-06 |
Family
ID=15098270
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP63133168A Pending JPH01302174A (en) | 1988-05-31 | 1988-05-31 | Current measuring apparatus |
Country Status (1)
| Country | Link |
|---|---|
| JP (1) | JPH01302174A (en) |
Cited By (1)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| CN104515886A (en) * | 2014-11-17 | 2015-04-15 | 龚恒 | Current transformer |
-
1988
- 1988-05-31 JP JP63133168A patent/JPH01302174A/en active Pending
Cited By (1)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| CN104515886A (en) * | 2014-11-17 | 2015-04-15 | 龚恒 | Current transformer |
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