JPH05297086A - Optical magnetic field sensor - Google Patents
Optical magnetic field sensorInfo
- Publication number
- JPH05297086A JPH05297086A JP3162753A JP16275391A JPH05297086A JP H05297086 A JPH05297086 A JP H05297086A JP 3162753 A JP3162753 A JP 3162753A JP 16275391 A JP16275391 A JP 16275391A JP H05297086 A JPH05297086 A JP H05297086A
- Authority
- JP
- Japan
- Prior art keywords
- optical
- magnetic field
- field sensor
- optical fiber
- face
- 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
Landscapes
- Measuring Magnetic Variables (AREA)
Abstract
Description
【0001】[0001]
【産業上の利用分野】本発明は、高圧配電線等の電流状
態を検知するための光方式磁界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 magnetic field sensor for detecting a current state of a high voltage distribution line or the like.
【0002】[0002]
【従来の技術】以下に従来の光方式磁界センサについて
説明する。図2は、従来の光方式磁界センサの構成を示
す斜視図である。図2において、1はレンズ、2は偏光
ビームスプリッタ、3は磁気光学素子、4は偏光ビーム
スプリッタ、5はキューブミラーである。2. Description of the Related Art A conventional optical magnetic field sensor will be described below. FIG. 2 is a perspective view showing the configuration of a conventional optical magnetic field sensor. In FIG. 2, 1 is a lens, 2 is a polarization beam splitter, 3 is a magneto-optical element, 4 is a polarization beam splitter, and 5 is a cube mirror.
【0003】従来の光方式磁界センサの動作について図
面を参照にしながら説明する。図3は光方式磁界センサ
の原理図である。この図3では、前記レンズ1およびキ
ューブミラー5は省略している。そして、発光素子6か
ら出射された光は偏光ビームスプリッタ2で直線偏光成
分7のみが透過する。この直線偏光成分7が磁気光学素
子3を透過すると、印加磁界8の光の進行方向と平行を
なす成分によって回転を受ける。この回転を受けた光9
の偏光ビームスプリッタ4の透過方向成分10のみが受
光素子11によって検出される。ここで、印加磁界と検
出される光強度の関係を図4に示す。また、偏光ビーム
スプリッタ2,4は相互に45°の関係をなすように配
されている。これは図4の0点までバイアスをかけ、交
流磁界に対する直線対称性を持たせるためである。The operation of the conventional optical magnetic field sensor will be described with reference to the drawings. FIG. 3 is a principle diagram of an optical magnetic field sensor. In FIG. 3, the lens 1 and the cube mirror 5 are omitted. Then, with respect to the light emitted from the light emitting element 6, only the linearly polarized light component 7 is transmitted by the polarization beam splitter 2. When this linearly polarized light component 7 passes through the magneto-optical element 3, it is rotated by the component of the applied magnetic field 8 that is parallel to the light traveling direction. Light 9 that received this rotation
Only the transmission direction component 10 of the polarization beam splitter 4 is detected by the light receiving element 11. Here, the relationship between the applied magnetic field and the detected light intensity is shown in FIG. Further, the polarization beam splitters 2 and 4 are arranged so as to form a 45 ° relationship with each other. This is because bias is applied up to the point 0 in FIG. 4 so as to have linear symmetry with respect to the AC magnetic field.
【0004】図5に、高圧配電線への応用例を示す。1
2は配電線、13は磁界周回積分用コア、14は光方式
磁界センサである。そして、磁界周回積分用コア13の
ギャップ部15に発生する磁界を光方式磁界センサ14
に印加する。このときの配電線12に流れる電流値と前
記ギャップ部15に発生する磁界強度の関係は、式
(1)で表される。この式(1)の関係を用いれば、配
電線12に流れる電流値を換算することができる。FIG. 5 shows an application example to a high voltage distribution line. 1
Reference numeral 2 is a distribution line, 13 is a magnetic field loop integration core, and 14 is an optical magnetic field sensor. The magnetic field generated in the gap portion 15 of the magnetic field orbital integration core 13 is detected by the optical magnetic field sensor 14
Apply to. The relationship between the value of the current flowing through the distribution line 12 and the strength of the magnetic field generated in the gap portion 15 at this time is expressed by equation (1). The value of the current flowing through the distribution line 12 can be converted by using the relationship of the equation (1).
【0005】Hg=K・I/δ (1) ただし、Hgは磁界強度、Kは比例定数、Iは電流値、
δはギャップ長をそれぞれ表す。Hg = K · I / δ (1) where Hg is the magnetic field strength, K is the proportional constant, I is the current value,
δ represents the gap length.
【0006】[0006]
【発明が解決しようとする課題】しかしながら、上記の
ような従来の構成では、高価な光学部品を必要とするた
めコスト高となる。また、電流の検出感度を高めるには
磁界強度を上げる必要があり、式(1)の関係からギャ
ップ長を短かくする必要があるが、光学系の大きさに制
約があるため、小型化が困難でギャップ長を短かくする
ことができず、発生磁界強度を上げるにも限界があると
いう問題点を有していた。However, the conventional structure as described above requires expensive optical parts, resulting in high cost. Further, in order to increase the current detection sensitivity, it is necessary to increase the magnetic field strength, and it is necessary to shorten the gap length from the relationship of the equation (1), but there is a restriction on the size of the optical system, so miniaturization is not It is difficult to make the gap length short, and there is a limit in increasing the strength of the generated magnetic field.
【0007】本発明は前記従来の問題点を解決するもの
で、安価で小型な光方式磁界センサを提供することを目
的とする。The present invention solves the above-mentioned conventional problems, and an object of the present invention is to provide an inexpensive and compact optical magnetic field sensor.
【0008】[0008]
【課題を解決するための手段】この目的を達成するため
に本発明の光方式磁界センサは、その軸方向に対して4
5°に傾斜した端面を有する第1の光ファイバの前記端
面と相対する側面にその軸方向に対して垂直な端面を有
する第2の光ファイバの前記垂直な端面を接合した光フ
ァイバ対を2組と、その一方の光ファイバ対と他方の光
ファイバ対との間に磁気光学素子と、その両側に位置す
る一対の偏光子とを設けた構成とする。また、より小型
化するため、前記偏光子に分子共鳴吸収型の薄型偏光子
を用いた構成とする。In order to achieve this object, the optical magnetic field sensor of the present invention has an axial direction of 4 mm.
Two optical fiber pairs in which the vertical end face of the second optical fiber having the end face perpendicular to the axial direction is joined to the side face of the first optical fiber having the end face inclined at 5 ° facing the end face are provided. A set, a magneto-optical element between one optical fiber pair and the other optical fiber pair, and a pair of polarizers located on both sides of the magneto-optical element are provided. In addition, in order to further reduce the size, a thin film polarizer of molecular resonance absorption type is used as the polarizer.
【0009】[0009]
【作用】この構成によって、光を伝送するためのレンズ
及び光路を偏光するためのキューブミラーが不要とな
る。また、前記垂直な端面を有する第2の光ファイバの
長さを調節することにより、光学系の大きさを可変する
ことができる。以上により、安価で小型の光方式磁界セ
ンサが提供できる。With this structure, a lens for transmitting light and a cube mirror for polarizing the optical path are unnecessary. Also, the size of the optical system can be changed by adjusting the length of the second optical fiber having the vertical end face. As described above, an inexpensive and compact optical magnetic field sensor can be provided.
【0010】また、分子共鳴吸収型の薄型偏光子を用い
ることにより、より小型化も可能である。Further, by using a molecular resonance absorption type thin polarizer, further miniaturization is possible.
【0011】[0011]
【実施例】以下本発明の一実施例について図面を参照し
ながら説明する。図1は、本発明の一実施例における光
方式磁界センサの概略を示すものである。図1におい
て、21はその軸方向に対して45°に傾斜した端面を
有する光ファイバ、22はその軸方向に対して垂直な端
面を有する光ファイバ、23は分子共鳴吸収型の薄型偏
光子、24は磁気光学素子、25は薄型偏光子23と同
様の薄型偏光子、26は光ファイバ22と同様の垂直な
端面を有する光ファイバ、27は光ファイバ21と同様
の45°に傾斜した端面を有する光ファイバである。な
お、薄型偏光子23,25は分子共鳴吸収型のもので、
例えばガラス表面にハロゲン化金属を蒸着した後還元し
て作製したガラス主体の複合物である。DETAILED DESCRIPTION OF THE PREFERRED EMBODIMENTS An embodiment of the present invention will be described below with reference to the drawings. FIG. 1 is a schematic view of an optical magnetic field sensor according to an embodiment of the present invention. In FIG. 1, 21 is an optical fiber having an end face inclined at 45 ° with respect to its axial direction, 22 is an optical fiber having an end face perpendicular to its axial direction, 23 is a molecular resonance absorption type thin polarizer, Reference numeral 24 is a magneto-optical element, 25 is a thin polarizer similar to the thin polarizer 23, 26 is an optical fiber having a vertical end face similar to the optical fiber 22, and 27 is an end face inclined at 45 ° similar to the optical fiber 21. It is an optical fiber having. The thin polarizers 23 and 25 are of the molecular resonance absorption type,
For example, it is a glass-based composite material produced by depositing a metal halide on the glass surface and then reducing it.
【0012】以上のように構成された光方式磁界センサ
についてその動作を説明する。まず、45°に傾斜した
端面を有する光ファイバ21のコアに導入された光は、
前記45°に傾斜した端面の境界面との屈折率差によ
り、フレネル反射を受け、前記端面と45°の角度をな
す側面より出射される。この出射された光は、垂直な端
面を有する光ファイバ22のコア部に導入され、薄型偏
光子23により直線偏光成分のみが磁気光学素子24に
入射される。このとき、光路に対して平行な印加磁界成
分によって、偏光面の回転を受ける。この光は、薄型偏
光子25,垂直な端面を有する光ファイバ26,45°
に傾斜した端面を有する光ファイバ27を通して出射さ
れる。このとき、薄型偏光子23,25は透過方向が4
5°の角度を有して配されている。また、垂直な端面を
有する光ファイバ22,26の端面は、鏡面研磨されて
おり、この長さを調整することによって光路長を自由に
調整することができ、小型で安価な光方式磁界センサが
得られる。The operation of the optical magnetic field sensor configured as described above will be described. First, the light introduced into the core of the optical fiber 21 having the end face inclined at 45 ° is
Due to the difference in refractive index from the boundary surface of the end surface inclined at 45 °, Fresnel reflection is performed and the light is emitted from the side surface forming an angle of 45 ° with the end surface. The emitted light is introduced into the core portion of the optical fiber 22 having a vertical end face, and only the linearly polarized light component is incident on the magneto-optical element 24 by the thin polarizer 23. At this time, the polarization plane is rotated by the applied magnetic field component parallel to the optical path. This light is transmitted through a thin polarizer 25, an optical fiber 26 having a vertical end face, and 45 °.
The light is emitted through an optical fiber 27 having an end surface inclined to. At this time, the thin polarizers 23 and 25 have a transmission direction of 4
It is arranged with an angle of 5 °. In addition, the end faces of the optical fibers 22 and 26 having the vertical end faces are mirror-polished, and the optical path length can be freely adjusted by adjusting the length, so that a small and inexpensive optical magnetic field sensor can be provided. can get.
【0013】なお、本実施例ではより小型化を図るた
め、偏光子に分子共鳴吸収型の薄型偏光子を用いた例を
示したが、他の偏光子、例えば前記偏光ビームスプリッ
タやルチル結晶偏光子を用いても光ファイバの光路長の
調整により、従来よりも小型化できる。In this embodiment, an example using a molecular resonance absorption type thin polarizer as a polarizer is shown for the purpose of further miniaturization, but other polarizers such as the above-mentioned polarization beam splitter or rutile crystal polarization are used. Even if a child is used, the size can be made smaller than before by adjusting the optical path length of the optical fiber.
【0014】[0014]
【発明の効果】以上のように本発明は、45°に傾斜し
た端面を有する第1の光ファイバの前記端面と相対する
側面に垂直な端面を有する第2の光ファイバを接合させ
た光ファイバ対を2組用いることにより、安価で小型化
された優れた光方式磁界センサを実現できるものであ
る。As described above, according to the present invention, an optical fiber obtained by joining a second optical fiber having an end face perpendicular to the side face opposite to the end face of the first optical fiber having an end face inclined at 45 °. By using two pairs, it is possible to realize an inexpensive and miniaturized excellent optical magnetic field sensor.
【図1】本発明の一実施例における光方式磁界センサの
斜視図FIG. 1 is a perspective view of an optical magnetic field sensor according to an embodiment of the present invention.
【図2】従来の光方式磁界センサの斜視図FIG. 2 is a perspective view of a conventional optical magnetic field sensor.
【図3】光方式磁界センサの原理図[Fig. 3] Principle diagram of optical magnetic field sensor
【図4】光方式磁界センサの特性図FIG. 4 is a characteristic diagram of an optical magnetic field sensor.
【図5】光方式磁界センサの応用例を説明する図FIG. 5 is a diagram illustrating an application example of an optical magnetic field sensor.
21,27 45°傾斜した端面を有する光ファイバ 22,26 垂直な端面を有する光ファイバ 23,25 薄型偏光子 24 磁気光学素子 21, 27 Optical fiber having an end surface inclined by 45 ° 22, 26 Optical fiber having a vertical end surface 23, 25 Thin polarizer 24 Magneto-optical element
Claims (2)
面を有する第1の光ファイバの前記端面と相対する側面
にその軸方向に対して垂直な端面を有する第2の光ファ
イバの前記垂直な端面を接合した光ファイバ対を2組
と、その一方の光ファイバ対と他方の光ファイバ対との
間に磁気光学素子とその両側に位置する一対の偏光子を
設けた光方式磁界センサ。1. A second optical fiber having an end face perpendicular to the axial direction on a side surface facing the end face of the first optical fiber having an end face inclined at 45 ° with respect to the axial direction. An optical magnetic field sensor in which two pairs of optical fibers having vertical end faces are joined, and a magneto-optical element and a pair of polarizers located on both sides thereof are provided between one pair of the optical fibers and the other pair of the optical fibers. .
光子を用いた請求項1記載の光方式磁界センサ。2. The optical magnetic field sensor according to claim 1, wherein a molecular resonance absorption type thin polarizer is used as the polarizer.
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP3162753A JPH05297086A (en) | 1991-07-03 | 1991-07-03 | Optical magnetic field sensor |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP3162753A JPH05297086A (en) | 1991-07-03 | 1991-07-03 | Optical magnetic field sensor |
Publications (1)
| Publication Number | Publication Date |
|---|---|
| JPH05297086A true JPH05297086A (en) | 1993-11-12 |
Family
ID=15760603
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP3162753A Pending JPH05297086A (en) | 1991-07-03 | 1991-07-03 | Optical magnetic field sensor |
Country Status (1)
| Country | Link |
|---|---|
| JP (1) | JPH05297086A (en) |
Cited By (1)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| US6008927A (en) * | 1997-03-27 | 1999-12-28 | Matsushita Electric Industrial Co., Ltd. | Optical fiber modulator having an optical fiber having a poled portion serving as an electrooptic element and method for making same |
-
1991
- 1991-07-03 JP JP3162753A patent/JPH05297086A/en active Pending
Cited By (1)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| US6008927A (en) * | 1997-03-27 | 1999-12-28 | Matsushita Electric Industrial Co., Ltd. | Optical fiber modulator having an optical fiber having a poled portion serving as an electrooptic element and method for making same |
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