JPH06258352A - Photovoltaic sensor - Google Patents
Photovoltaic sensorInfo
- Publication number
- JPH06258352A JPH06258352A JP5071244A JP7124493A JPH06258352A JP H06258352 A JPH06258352 A JP H06258352A JP 5071244 A JP5071244 A JP 5071244A JP 7124493 A JP7124493 A JP 7124493A JP H06258352 A JPH06258352 A JP H06258352A
- Authority
- JP
- Japan
- Prior art keywords
- optical
- electro
- crystal element
- crystal
- sensor
- 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.)
- Granted
Links
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- Measuring Instrument Details And Bridges, And Automatic Balancing Devices (AREA)
Abstract
Description
【0001】[0001]
【産業上の利用分野】本発明は、配電線路などの被測定
体の電圧を検出する光電圧センサに関するものである。BACKGROUND OF THE INVENTION 1. Field of the Invention The present invention relates to an optical voltage sensor for detecting the voltage of an object to be measured such as a distribution line.
【0002】[0002]
【従来の技術】従来この種の光電圧センサは、図2に示
すように光源(図示せず)からの光を光ファイバ1aで
導いてコリメータレンズ2aで平行光とし、偏光子3で
光を反射又は透過させて直線偏光3aとし、この直線偏
光は1/4波長板4を透過する際に2つの直線偏光4
a、4bに分かれ、90°の位相差が生じて円偏光とな
り、電気光学結晶素子5を通過する時に、その結晶に設
けられた電極膜6に印加された電圧に応じて生じる復屈
折を利用して光位相変調を行ない、その光を検光子7へ
透過又は反射させ、コリメータレンズ2bで光ファイバ
1bへ集光して電圧を検出していた。このような光電圧
センサに用いられる電気光学結晶素子は、例えばBi12
GeO20(BGOと略す)やBi12Si O20(BSOと
略す)などのような立方晶系のものが用いられ、切出し
面は三つの結晶軸x<001>、y<010>、z<1
00>に垂直に切り出されている。2. Description of the Related Art Conventionally, in this type of optical voltage sensor, as shown in FIG. 2, light from a light source (not shown) is guided by an optical fiber 1a, collimated by a collimator lens 2a, and polarized by a polarizer 3. It is reflected or transmitted to form linearly polarized light 3a, and when this linearly polarized light is transmitted through the quarter-wave plate 4, two linearly polarized light 4a.
It is divided into a and 4b, and a phase difference of 90 ° is generated to become circularly polarized light, and when passing through the electro-optic crystal element 5, the birefringence that occurs according to the voltage applied to the electrode film 6 provided on the crystal is used. Then, optical phase modulation is performed, the light is transmitted or reflected by the analyzer 7, and the collimator lens 2b collects the light on the optical fiber 1b to detect the voltage. An electro-optical crystal element used for such an optical voltage sensor is, for example, Bi 12
A cubic system such as GeO 20 (abbreviated as BGO) or Bi 12 S i O 20 (abbreviated as BSO) is used, and the cut surface has three crystal axes x <001>, y <010>, and z. <1
00> is cut out vertically.
【0003】[0003]
【発明が解決しようとする課題】ところで、このような
電気光学結晶素子は自然旋光能を有し、結晶の厚みLで
決まる旋光角Φだけ直線偏光が回転する。BGOの場合
は受光側から見て反時計方向に回転して直線偏光3a’
となる。このためセンサ感度が変化する。そこで結晶軸
z<100>を中心に電気光学結晶素子を回転させたと
きの回転角θとセンサ感度との関係を測定すると、縦軸
に感度をとり横軸に結晶の回転角θをとると図3に示す
ようにセンサ感度曲線bがえられ、回転角θ=Φ/2の
時が感度が最大となる。図中、右は受光側から見て結晶
を時計回り方向に回転させ、左は反時計回り方向に回転
させたとき示している。通常は偏光子の偏向方向はy軸
またはx軸と一致させているので、結晶の回転角θは0
のところを使用しており、センサ感度の少し低い領域と
なっていた。このセンサ感度の低下した領域は感度の変
化が大きい領域であり、自然旋光能の温度変化が顕著に
表れ、センサ全体の温度特性を悪化させる原因となって
いた。また、電気光学結晶素子を切り出す面方位の精度
や、偏光子及び1/4波長板と電気光学結晶素子の結晶
軸との軸ずれなど、構造上のバラツキが回転角θをバラ
つかせるので、センサの感度のバラツキが大きくなって
いた。本発明は、センサの感度を向上させ、感度のバラ
ツキをなくし、温度特性を安定にすることを目的とす
る。By the way, such an electro-optical crystal element has a natural optical rotatory power, and linearly polarized light rotates by an optical rotation angle Φ determined by the thickness L of the crystal. In the case of BGO, linearly polarized light 3a 'rotates counterclockwise when viewed from the light receiving side.
Becomes Therefore, the sensor sensitivity changes. Therefore, when the relationship between the rotation angle θ when the electro-optic crystal element is rotated around the crystal axis z <100> and the sensor sensitivity is measured, the vertical axis represents the sensitivity and the horizontal axis represents the crystal rotation angle θ. As shown in FIG. 3, the sensor sensitivity curve b is obtained, and the sensitivity becomes maximum when the rotation angle θ = Φ / 2. In the figure, the right side shows the crystal rotated clockwise as viewed from the light receiving side, and the left side shows the counterclockwise rotation. Since the polarization direction of the polarizer is usually aligned with the y-axis or the x-axis, the rotation angle θ of the crystal is 0.
However, the sensor sensitivity was a little low. The region in which the sensor sensitivity is lowered is a region in which the change in sensitivity is large, and the temperature change of the spontaneous optical rotation is remarkably exhibited, which causes the temperature characteristics of the entire sensor to be deteriorated. In addition, because the structural variations such as the accuracy of the plane orientation of cutting out the electro-optical crystal element and the axis deviation between the polarizer and the quarter-wave plate and the crystal axis of the electro-optical crystal element cause the rotation angle θ to vary, The variations in sensor sensitivity were increasing. It is an object of the present invention to improve the sensitivity of a sensor, eliminate variations in sensitivity, and stabilize temperature characteristics.
【0004】[0004]
【課題を解決するための手段】以上の問題を解決するた
め本発明は、光の進行方向に配置した偏光子と、1/4
波長板と、自然旋光能を有する電気光学結晶素子と、検
光子とから成り、上記電気光学結晶素子の周面にあっ
て、光の進行方向に対して垂直もしくは平行に対向する
2面に設けられた電極膜に電界を印加して電圧を検出す
る光電圧センサにおいて、電気光学結晶素子の入射およ
び出射面を電気光学結晶素子の1本の結晶軸に垂直に配
置し、電気光学結晶素子の他の2本の結晶軸のいずれか
1本を偏光子から出射した直線偏光の偏光方向に対し電
気光学結晶素子の旋光方向と反対方向に、透過光路長で
決まる旋光角の半分の角度だけ傾けて配置した電気光学
結晶素子を設けるようにしている。In order to solve the above problems, the present invention provides a polarizer arranged in the traveling direction of light and a quarter
A wave plate, an electro-optical crystal element having a natural optical rotation, and an analyzer, which are provided on two surfaces on the peripheral surface of the electro-optical crystal element which are perpendicular to or parallel to the light traveling direction. In an optical voltage sensor for detecting a voltage by applying an electric field to the formed electrode film, the entrance and exit surfaces of the electro-optical crystal element are arranged perpendicular to one crystal axis of the electro-optical crystal element, Any one of the other two crystal axes is tilted in the direction opposite to the optical rotation direction of the electro-optic crystal element with respect to the polarization direction of the linearly polarized light emitted from the polarizer, by half the optical rotation angle determined by the transmitted optical path length. The electro-optic crystal element is arranged in the same manner.
【0005】[0005]
【作用】したがって、センサ感度の極大点を使って計測
するようにしている。Therefore, the maximum point of the sensor sensitivity is used for the measurement.
【0006】[0006]
【実施例】本発明を図1に示す実施例について説明す
る。図2と同一のものには同一の符号を付して詳細な説
明を省略する。8は結晶素子の厚みLのBGO、結晶軸
x<001>、y<010>、z<100>のうち、入
射面および出射面を結晶軸z<100>に対し垂直に切
出し配置し、結晶軸y<010>を偏光子から出射した
直線偏光の偏光方向に対し、電気光学結晶素子の旋光方
向と反対方向に、電気光学結晶素子を傾けて切り出して
いる。その傾き量は電気光学結晶素子の旋光能をΦ0 と
し、旋光角をΦとするとΦ=L×Φ0となり、旋光角Φ
の半分の量傾けて切り出している。いま、BGOの厚み
Lを2mmとし、BGOの旋光能Φ0 が10.2deg
/mmであるので、旋光角Φは20.4degとなり、
その半分の量10.2deg傾けて切り出している。こ
のように構成したBGOの電極膜6に100Vの電圧を
印加すると図3に示すセンサ感度曲線aのようになっ
た。したがって偏光子3から出射された直線偏光3aは
1/4波長板4を透過する際に2つの直線偏向4a、4
bに分かれ、90°の位相差が生じて円偏光となる。こ
の円偏光が光学結晶素子5を通過しおわるまでに旋光角
Φだけ受光側から見て反時計回りに回転を受ける。一
方、結晶軸のほうは、偏光子3の偏光方向3aに対し、
その旋光角の半分に等しい大きさで旋光方向と反対方向
へ傾けてあるので、図3のセンサ感度曲線aにおいて回
転角θが0°のときセンサ感度が最大値をとるようにな
る。なお、この実施例では結晶軸y、xを上面及び側面
の法線に対してΦ/2だけ傾くように結晶を切り出した
が、結晶軸に対し上面及び側面を垂直に切り出した結晶
をz軸を軸にしてΦ/2だけ傾けても同じ効果が得られ
る。EXAMPLE The present invention will be described with reference to the example shown in FIG. The same parts as those in FIG. 2 are designated by the same reference numerals and detailed description thereof will be omitted. Reference numeral 8 denotes a BGO having a thickness L of the crystal element, crystal axes x <001>, y <010>, and z <100>, and the incident surface and the emission surface are cut out and arranged perpendicular to the crystal axis z <100>. The electro-optic crystal element is tilted and cut out in the direction opposite to the optical rotation direction of the electro-optic crystal element with respect to the polarization direction of the linearly polarized light emitted from the polarizer on the axis y <010>. The tilt amount is Φ = L × Φ 0 , where Φ 0 is the optical rotatory power of the electro-optical crystal element and Φ is the optical rotation angle, and the optical rotation angle Φ
It is cut out by tilting half the amount. Now, assuming that the thickness L of the BGO is 2 mm, the optical rotation power Φ 0 of the BGO is 10.2 deg.
/ Mm, the optical rotation angle Φ is 20.4 deg,
Half of that amount is cut out with an inclination of 10.2 deg. When a voltage of 100 V was applied to the BGO electrode film 6 thus constructed, a sensor sensitivity curve a shown in FIG. 3 was obtained. Therefore, when the linearly polarized light 3a emitted from the polarizer 3 passes through the quarter-wave plate 4, the two linearly polarized light 4a, 4a
It is divided into b and a phase difference of 90 ° is generated to become circularly polarized light. By the time the circularly polarized light passes through the optical crystal element 5, it is rotated counterclockwise by the optical rotation angle Φ when viewed from the light receiving side. On the other hand, with respect to the crystal axis, with respect to the polarization direction 3a of the polarizer 3,
Since it is tilted in the direction opposite to the optical rotation direction with a size equal to half the optical rotation angle, the sensor sensitivity takes the maximum value when the rotation angle θ is 0 ° in the sensor sensitivity curve a of FIG. In this example, the crystal was cut out so that the crystal axes y and x were inclined by Φ / 2 with respect to the normals to the upper surface and the side surface. The same effect can be obtained by tilting Φ / 2 around the axis.
【0007】[0007]
【発明の効果】以上述べたように構成したので、センサ
の感度を最大値のところで計測するのでSN比が向上し
て高精度となる。また、旋光角が温度変化しても感度の
変化はほとんどないのでセンサとしての温度特性が安定
する。さらに、結晶の面方位のずれ、偏光子や波長板と
結晶軸との軸ずれ、結晶の厚みの精度による旋光角の変
化等構造上のバラツキが生じても感度はほぼ一定である
ので、出力特性のバラツキのないセンサとなる。Since the configuration as described above is adopted, the sensitivity of the sensor is measured at the maximum value, so that the SN ratio is improved and the accuracy becomes high. Further, even if the optical rotation angle changes with temperature, the sensitivity hardly changes, so that the temperature characteristics of the sensor are stable. In addition, the sensitivity is almost constant even if there are structural variations such as misalignment of the crystal plane orientation, misalignment of the crystal axis with the polarizer or wave plate, and variation of the optical rotation angle due to the accuracy of the crystal thickness. The sensor has no characteristic variations.
【図1】本発明の実施例を示す光電圧センサの構成図。FIG. 1 is a configuration diagram of an optical voltage sensor showing an embodiment of the present invention.
【図2】従来の光電圧センサの構成図。FIG. 2 is a configuration diagram of a conventional optical voltage sensor.
【図3】結晶の回転角とセンサ感度との関係図。FIG. 3 is a relationship diagram between a crystal rotation angle and sensor sensitivity.
1a、1b 光ファイバ 2a、2b コリメータレンズ 3 偏光子 4 1/4波長板 5 電気光学結晶素子 6 電極膜 7 検光子 8 電気光学結晶素子 1a, 1b Optical fiber 2a, 2b Collimator lens 3 Polarizer 4 1/4 wavelength plate 5 Electro-optical crystal element 6 Electrode film 7 Analyzer 8 Electro-optical crystal element
Claims (1)
4波長板と、自然旋光能を有する電気光学結晶素子と、
検光子とから成り、上記電気光学結晶素子の周面にあっ
て、光の進行方向に対して垂直もしくは平行に対向する
2面に設けられた電極膜に電界を印加して電圧を検出す
る光電圧センサにおいて、電気光学結晶素子の入射およ
び出射面を電気光学結晶素子の1本の結晶軸に垂直に配
置し、電気光学結晶素子の他の2本の結晶軸のいずれか
1本を偏光子から出射した直線偏光の偏光方向に対し電
気光学結晶素子の旋光方向と反対方向に、透過光路長で
決まる旋光角の半分の角度だけ傾けて配置した電気光学
結晶素子を具えたことを特徴とする光電圧センサ。1. A polarizer arranged in a light traveling direction, and 1 /
A four-wave plate and an electro-optic crystal element having a natural optical rotatory power,
Light for detecting a voltage by applying an electric field to electrode films provided on two surfaces of the electro-optical crystal element, which are arranged on the peripheral surface of the electro-optical crystal element and which face each other in the direction perpendicular to or parallel to the traveling direction of light. In the voltage sensor, the entrance and exit faces of the electro-optic crystal element are arranged perpendicular to one crystal axis of the electro-optic crystal element, and one of the other two crystal axes of the electro-optic crystal element is used as a polarizer. It is characterized by comprising an electro-optical crystal element which is arranged in a direction opposite to the optical rotation direction of the electro-optical crystal element with respect to the polarization direction of the linearly polarized light emitted from Optical voltage sensor.
Priority Applications (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP07124493A JP3206614B2 (en) | 1993-03-05 | 1993-03-05 | Optical voltage sensor |
Applications Claiming Priority (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP07124493A JP3206614B2 (en) | 1993-03-05 | 1993-03-05 | Optical voltage sensor |
Publications (2)
Publication Number | Publication Date |
---|---|
JPH06258352A true JPH06258352A (en) | 1994-09-16 |
JP3206614B2 JP3206614B2 (en) | 2001-09-10 |
Family
ID=13455096
Family Applications (1)
Application Number | Title | Priority Date | Filing Date |
---|---|---|---|
JP07124493A Expired - Fee Related JP3206614B2 (en) | 1993-03-05 | 1993-03-05 | Optical voltage sensor |
Country Status (1)
Country | Link |
---|---|
JP (1) | JP3206614B2 (en) |
Cited By (1)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
US6411077B1 (en) | 1999-03-09 | 2002-06-25 | Hitachi, Ltd. | Optical-voltage sensor |
-
1993
- 1993-03-05 JP JP07124493A patent/JP3206614B2/en not_active Expired - Fee Related
Cited By (1)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
US6411077B1 (en) | 1999-03-09 | 2002-06-25 | Hitachi, Ltd. | Optical-voltage sensor |
Also Published As
Publication number | Publication date |
---|---|
JP3206614B2 (en) | 2001-09-10 |
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LAPS | Cancellation because of no payment of annual fees |