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JPH0156387B2 - - Google Patents
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JPH0156387B2 - - Google Patents

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Publication number
JPH0156387B2
JPH0156387B2 JP57217156A JP21715682A JPH0156387B2 JP H0156387 B2 JPH0156387 B2 JP H0156387B2 JP 57217156 A JP57217156 A JP 57217156A JP 21715682 A JP21715682 A JP 21715682A JP H0156387 B2 JPH0156387 B2 JP H0156387B2
Authority
JP
Japan
Prior art keywords
optical
optical fiber
polarizer
light
beam splitter
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
Application number
JP57217156A
Other languages
Japanese (ja)
Other versions
JPS59107271A (en
Inventor
Shuichi Tai
Kazuo Hisama
Toshio Aranishi
Koji Takioka
Toshishige Nagao
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.)
Mitsubishi Electric Corp
Original Assignee
Mitsubishi Electric Corp
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 Mitsubishi Electric Corp filed Critical Mitsubishi Electric Corp
Priority to JP57217156A priority Critical patent/JPS59107271A/en
Publication of JPS59107271A publication Critical patent/JPS59107271A/en
Publication of JPH0156387B2 publication Critical patent/JPH0156387B2/ja
Granted legal-status Critical Current

Links

Landscapes

  • Measuring Magnetic Variables (AREA)
  • Measuring Instrument Details And Bridges, And Automatic Balancing Devices (AREA)
  • Light Guides In General And Applications Therefor (AREA)

Description

【発明の詳細な説明】 この発明は、各種物理量たとえば電圧、電流な
どを測定するための光フアイバ応用センサに関す
るものである。
DETAILED DESCRIPTION OF THE INVENTION The present invention relates to an optical fiber applied sensor for measuring various physical quantities such as voltage and current.

第1図は、光フアイバ応用センサの一例として
電流(磁界)センサを示したもので、1は光送信
機、2は光受信機、3a,3bは光フアイバ、4
a,4bは屈折率分布型レンズ、5は偏光子、6
は光フアラデー素子、7は検光子である。
FIG. 1 shows a current (magnetic field) sensor as an example of an optical fiber applied sensor, where 1 is an optical transmitter, 2 is an optical receiver, 3a and 3b are optical fibers, and 4 is an optical fiber sensor.
a, 4b are gradient index lenses, 5 is a polarizer, 6
is an optical faraday element, and 7 is an analyzer.

光送信機1からの光は、光フアイバ3aにより
光センサ部に導かれる。光センサ部では、光フア
イバ3aからの光を屈折率分布型レンズ4aでコ
リメートしたのち、偏光子5で直線偏光に変換し
光フアラデー素子6(これは鉛ガラス、YIG結
晶、磁性薄膜等からなる)に導く。いま、光フア
ラデー素子6に平行に磁界が印加されたとする
と、光フアラデー素子6を通過する直線偏光の偏
光面が磁界の強度に比例して回転する。この回転
の程度を、偏光子5と光軸が45゜だけ傾いた検光
子7によつて光強度に変換し、その光を屈折率分
布型レンズ4bで絞り、光フアイバ3bを経て光
受信機2に導く。光受信機2では、光信号を電気
信号に変換し、光センサ部に印加された磁界の強
さを求める動作が行われる。磁界強度がわかれ
ば、直ちに電流の大きさがわかる。偏光子5、検
光子7としては、グラントムソンプリズムや偏光
ビームスプリツタを用いている。
Light from the optical transmitter 1 is guided to the optical sensor section by an optical fiber 3a. In the optical sensor section, the light from the optical fiber 3a is collimated by a refractive index gradient lens 4a, and then converted into linearly polarized light by a polarizer 5. ). Now, if a magnetic field is applied in parallel to the optical Faraday element 6, the plane of polarization of the linearly polarized light passing through the optical Faraday element 6 rotates in proportion to the strength of the magnetic field. The degree of this rotation is converted into light intensity by a polarizer 5 and an analyzer 7 whose optical axis is tilted by 45 degrees, and the light is focused by a gradient index lens 4b and sent to an optical receiver via an optical fiber 3b. Lead to 2. The optical receiver 2 performs an operation of converting an optical signal into an electrical signal and determining the strength of the magnetic field applied to the optical sensor section. If you know the strength of the magnetic field, you can immediately determine the magnitude of the current. As the polarizer 5 and analyzer 7, a Glan-Thompson prism or a polarizing beam splitter is used.

従来の光フアイバ応用センサは以上のように構
成されているので、光源に使用する発光ダイオー
ドや半導体レーザの温度依存性が誤差の原因とな
る。すなわち発光ダイオードや半導体レーザの発
光スペクトルは一般に温度上昇とともに長波長側
へシフトし、また偏光子5や検光子7として使用
しているグラントムソンプリズムや偏光子スプリ
ツタの消光比は波長変動によりわずかではあるが
変化する。この変化は数パーセント程度のもので
あるが、これが光センサ出力の誤差となるもの
で、きわめて高い精度が要求される電圧・電流セ
ンサとして用いる場合には問題となる。
Since the conventional optical fiber applied sensor is configured as described above, the temperature dependence of the light emitting diode or semiconductor laser used as the light source causes errors. In other words, the emission spectra of light-emitting diodes and semiconductor lasers generally shift toward longer wavelengths as the temperature rises, and the extinction ratio of the Glan-Thompson prism and polarizer splitter used as the polarizer 5 and analyzer 7 changes slightly due to wavelength fluctuations. Yes, but it changes. Although this change is on the order of several percent, it causes an error in the optical sensor output, which is a problem when used as a voltage/current sensor that requires extremely high accuracy.

この発明は、上記のような従来のものの欠点を
除去するためになされたもので、偏光子および検
光子としてそれぞれ偏光ビームスプリツタを使用
し、その一方の偏光ビームスプリツタは透過光
(P偏光分離)を、他方の偏光ビームスプリツタ
は反射光(S偏光分離)を使用することにより、
光源の波長変化による光センサ出力の変動を除去
できるようにした光フアイバ応用センサを提供す
ることを目的としている。
This invention was made in order to eliminate the drawbacks of the conventional ones as described above, and uses a polarizing beam splitter as a polarizer and an analyzer, respectively, and one polarizing beam splitter uses transmitted light (P-polarized light). separation), and the other polarization beam splitter uses reflected light (S polarization separation).
It is an object of the present invention to provide an optical fiber applied sensor that can eliminate fluctuations in optical sensor output due to changes in the wavelength of a light source.

以下、この発明の一実施例を図について説明す
る。第2図において、1は光送信機、2は光受信
機、3a,3bは光フアイバ、4a,4bは屈折
率分布型レンズ、6はフアラデー素子、8aおよ
び8bは偏光ビームスプリツタからなる偏光子お
よび検光子、9はプリズムである。偏光子8aお
よび検光子8bの偏光ビームスプリツタは、一方
が透過(P偏光分離)として、また他方が反射
(S偏光分離)として使用される。
An embodiment of the present invention will be described below with reference to the drawings. In FIG. 2, 1 is an optical transmitter, 2 is an optical receiver, 3a and 3b are optical fibers, 4a and 4b are gradient index lenses, 6 is a Faraday element, and 8a and 8b are polarized beam splitters. 9 is a prism. One of the polarizing beam splitters of the polarizer 8a and the analyzer 8b is used for transmission (P polarization separation) and the other for reflection (S polarization separation).

実験の結果によれば、グラントムソンプリズム
や偏光ビームスプリツタの消光比(偏光分離度)
は、光源のスペクトルの変化によりわずかではあ
るが変化することが確かめられた。すなわち偏光
子および検光として透過(P偏光分離)のみを使
用した場合には、光源(たとえば発光タイオー
ド)の温度が0℃から70℃まで上昇したとき、セ
ンサ出力は数パーセント増加し、反射(S偏光分
離)のみを使用した場合には数パーセント減少す
る。
According to experimental results, the extinction ratio (degree of polarization separation) of the Glan-Thompson prism and polarization beam splitter
was confirmed to change slightly due to changes in the spectrum of the light source. That is, if only transmission (P-polarized light separation) is used as a polarizer and analyzer, when the temperature of the light source (e.g., a light emitting diode) increases from 0°C to 70°C, the sensor output will increase by several percent, and the reflection ( If only S-polarization splitting is used, it decreases by several percent.

ところがこの発明においては、偏光子8aおよ
び検光子8bの偏光ビームスプリツタは、一方の
偏光ビームスプリツタとして透過光のみを、他方
の偏光ビームスプリツタとして反射光のみを使用
するので、反射で分離されるS偏光は光源の温度
上昇とともに減少し、逆に透過で分離されるP偏
光は増加することになり、全体としてはその変化
が打消され、センサ出力には光源の温度変化によ
る影響は現われない。実験によれば、P偏光もし
くはS偏光のみを利用した従来のセンサの温度に
よる出力変動が数パーセントであつたのに対し
て、この発明のセンサでは1%以内に収まつてい
ることが判つた。
However, in this invention, the polarizing beam splitters of the polarizer 8a and the analyzer 8b use only the transmitted light as one polarizing beam splitter and only the reflected light as the other polarizing beam splitter, so they are separated by reflection. The S-polarized light that is transmitted decreases as the temperature of the light source increases, and conversely, the P-polarized light that is separated by transmission increases.As a whole, this change is canceled out, and the sensor output is not affected by the temperature change of the light source. do not have. According to experiments, it was found that while the output fluctuation due to temperature of conventional sensors using only P-polarized light or S-polarized light was several percent, the sensor of the present invention had fluctuations within 1%. .

なお上記の実施例では、電流センサについて説
明したが、偏光子および検光子を使用するセンサ
であれば、どのようなセンサにも適用できる。
Note that in the above embodiment, a current sensor has been described, but the present invention can be applied to any sensor as long as it uses a polarizer and an analyzer.

以上のようにこの発明によれば、偏光子および
検光子として、一方は偏光ビームスプリツタは透
過光(P偏光分離)を、他方は偏光ビームスプリ
ツタの反射光(S偏光分離)を使用し、光源の温
度変化による発光スペクトルの変動の影響を相殺
するようにしたので、測定の精度が大幅に向上
し、信頼性の高いものが得られる効果がある。
As described above, according to the present invention, as a polarizer and an analyzer, one uses the transmitted light (P polarization separation) from the polarization beam splitter, and the other uses the reflected light (S polarization separation) from the polarization beam splitter. Since the influence of fluctuations in the emission spectrum due to changes in the temperature of the light source is offset, the measurement accuracy is greatly improved and highly reliable results can be obtained.

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

第1図は従来の光フアイバ応用センサの構成を
示すブロツク図、第2図はこの発明の一実施例に
よる光フアイバ応用センサの構成を示すブロツク
図である。 1……光送信機、2……光受信機、3a,3b
……光フアイバ、4a,4b……屈折率分布型レ
ンズ、6……光フアラデー素子、8a……偏光
子、8b……検光子、9……プリズム。なお、図
中同一符号は同一又は相当部分を示す。
FIG. 1 is a block diagram showing the configuration of a conventional optical fiber applied sensor, and FIG. 2 is a block diagram showing the configuration of an optical fiber applied sensor according to an embodiment of the present invention. 1... Optical transmitter, 2... Optical receiver, 3a, 3b
...Optical fiber, 4a, 4b... Gradient index lens, 6... Optical Faraday element, 8a... Polarizer, 8b... Analyzer, 9... Prism. Note that the same reference numerals in the figures indicate the same or equivalent parts.

Claims (1)

【特許請求の範囲】[Claims] 1 光送信機からの光を光フアイバ、偏光子、光
フアラデー素子、検光子および光フアイバを介し
て光受信機に導いて各種物理量を測定するように
した光フアイバ応用センサにおいて、上記偏光子
および上記検光子としてそれぞれ偏光ビームスプ
リツタを使用し、一方の偏光ビームスプリツタは
透過光を用い、他方の偏光ビームスプリツタは反
射光を用いたことを特徴とする光フアイバ応用セ
ンサ。
1. In an optical fiber applied sensor that measures various physical quantities by guiding light from an optical transmitter to an optical receiver via an optical fiber, a polarizer, an optical faraday element, an analyzer, and an optical fiber, the above polarizer and An optical fiber applied sensor characterized in that each of the analyzers uses a polarizing beam splitter, one polarizing beam splitter uses transmitted light, and the other polarizing beam splitter uses reflected light.
JP57217156A 1982-12-10 1982-12-10 Optical fiber applied sensor Granted JPS59107271A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP57217156A JPS59107271A (en) 1982-12-10 1982-12-10 Optical fiber applied sensor

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP57217156A JPS59107271A (en) 1982-12-10 1982-12-10 Optical fiber applied sensor

Publications (2)

Publication Number Publication Date
JPS59107271A JPS59107271A (en) 1984-06-21
JPH0156387B2 true JPH0156387B2 (en) 1989-11-29

Family

ID=16699725

Family Applications (1)

Application Number Title Priority Date Filing Date
JP57217156A Granted JPS59107271A (en) 1982-12-10 1982-12-10 Optical fiber applied sensor

Country Status (1)

Country Link
JP (1) JPS59107271A (en)

Families Citing this family (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPH0619384B2 (en) * 1986-12-17 1994-03-16 三菱電機株式会社 Optical fiber type voltage and electric field measuring device
JPH01162680U (en) * 1988-04-28 1989-11-13

Family Cites Families (4)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
CA1003500A (en) * 1974-02-18 1977-01-11 Safwat G. Zaky Optical modulator having compensation for thermal and space charge effects
JPS5667764A (en) * 1979-11-08 1981-06-08 Sumitomo Electric Ind Ltd Voltage/current measurement device by light beam
JPS57114119A (en) * 1981-01-07 1982-07-15 Ricoh Co Ltd Electrooptical element in optical switch device
JPS57135329A (en) * 1981-02-16 1982-08-20 Masaki Yamamoto Polarization analyzing device

Also Published As

Publication number Publication date
JPS59107271A (en) 1984-06-21

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