JPH02206737A - Distribution type optical fiber temperature sensor and temperature measuring method - Google Patents

Distribution type optical fiber temperature sensor and temperature measuring method

Info

Publication number
JPH02206737A
JPH02206737A JP1026604A JP2660489A JPH02206737A JP H02206737 A JPH02206737 A JP H02206737A JP 1026604 A JP1026604 A JP 1026604A JP 2660489 A JP2660489 A JP 2660489A JP H02206737 A JPH02206737 A JP H02206737A
Authority
JP
Japan
Prior art keywords
optical fiber
measured
temperature
calibration
temperature 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.)
Pending
Application number
JP1026604A
Other languages
Japanese (ja)
Inventor
Koji Igawa
耕司 井川
Shozo Yoshida
吉田 省三
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.)
AGC Inc
Original Assignee
Asahi Glass Co Ltd
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 Asahi Glass Co Ltd filed Critical Asahi Glass Co Ltd
Priority to JP1026604A priority Critical patent/JPH02206737A/en
Publication of JPH02206737A publication Critical patent/JPH02206737A/en
Pending legal-status Critical Current

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  • Measuring Temperature Or Quantity Of Heat (AREA)

Abstract

PURPOSE:To miniaturize an entire system and to perform continuous operation by providing a calibration part for measuring the absolute temperature distribution from the temperature of an optical fiber in a part of the optical fiber to be measured and arranging a temperature sensor in the calibration part. CONSTITUTION:Laser pulses oscillated from a laser pulse emitting part 7 are made incident on the optical fiber to be measured 1 through an acoustic optical switch 4. The optical fiber for calibration 2 which is a part of the fiber 1 is incorporated in a heat insulating material 20 which is difficult to accept the variation of external temperature and the temperature sensor 3 is provided to the optical fiber 2. The Raman scattered light generated in the fiber 1 is introduced to a measuring device by a switch 4. In the measuring device, anti-Stokes light in the Raman scattered light is detected by a photoelectric conversion part 5, amplified by an amplifier 6 and transmitted to an AD converter 9. The signal digitized by the converter 9 is averaging-processed in a signal processing part 10 after performing stored measurement about ten thousand times. In such a case, the temperature of the calibration part is measured by the sensor 3 and transmitted to the processing part 10 by switching a switch 8, thereby measuring the absolute temperature distribution.

Description

【発明の詳細な説明】 [産業上の利用分野] 本発明は分布型光フアイバー温度センサー及び温度測定
方法に係り、特に被測定光ファイバーのラマン散乱光の
うち反ストークス光の強度から絶対的温度分布を測定す
る分布型光フアイバー温度センサー及び温度測定方法に
関するものである。
[Detailed Description of the Invention] [Industrial Application Field] The present invention relates to a distributed optical fiber temperature sensor and a temperature measurement method, and particularly relates to an absolute temperature distribution based on the intensity of anti-Stokes light among Raman scattered light of an optical fiber to be measured. The present invention relates to a distributed optical fiber temperature sensor and a temperature measurement method for measuring temperature.

[従来の技術] 第2図は、従来の分布型光フアイバー温度センサーのブ
ロック図である。半導体レーザ及びその駆動回路等から
なるレーザパルス発光部16から発振したレーザパルス
は、未駆動の光方向性結合器の音響光学光スイッチ14
を通じて被測定用光ファイバー11へ入射される。被測
定用光ファイバー11で発生したラマン散乱光は、駆動
された音響光学光スイッチで測定装置へ導光される。測
定装置では以下のような処理が行なわれる。ラマン散乱
光中の反ストーク光をフォトマルチプライヤ−、フォト
ダイオード等の光電変換部15で検出し、増幅器17で
増幅してAD変換器18へ伝送する。AD変換器18で
ディジタル化された信号は、信号処理部19で記憶され
10000回程度の測定後平均化処理がなされる。
[Prior Art] FIG. 2 is a block diagram of a conventional distributed optical fiber temperature sensor. A laser pulse emitted from a laser pulse emitting unit 16 consisting of a semiconductor laser and its driving circuit, etc. is transmitted to an acousto-optic optical switch 14 of an undriven optical directional coupler.
The light is input to the optical fiber 11 to be measured. The Raman scattered light generated in the optical fiber 11 to be measured is guided to the measuring device by the driven acousto-optic switch. The following processing is performed in the measuring device. Anti-Stokes light in the Raman scattered light is detected by a photoelectric converter 15 such as a photomultiplier or a photodiode, amplified by an amplifier 17, and transmitted to an AD converter 18. The signal digitized by the AD converter 18 is stored in the signal processing section 19 and subjected to averaging processing after being measured approximately 10,000 times.

この場合、被測定用光ファイバー11の一部が校正用光
ファイバー13として用いられており、校正用光ファイ
バー13は恒温槽によって既知の温度Tに設定され恒温
化されている。従来、反ストーネ光のみの測定では相対
的温度分布しか測定できなかったため、この恒温化され
た部分を絶対的温度分布測定のための基準温度部とし、
該基準温度部の反ストーク光強度とその他の部分の反ス
トークス光強度を比較して絶対的温度分布の測定を行な
っていた。
In this case, a part of the optical fiber 11 to be measured is used as the optical fiber 13 for calibration, and the optical fiber 13 for calibration is kept at a known temperature T in a constant temperature oven. Conventionally, only relative temperature distribution could be measured by measuring only the anti-Stone light, so this constant temperature area was used as the reference temperature area for measuring absolute temperature distribution.
The absolute temperature distribution was measured by comparing the anti-Stokes light intensity in the reference temperature part and the anti-Stokes light intensity in other parts.

[発明が解決しようとする課題] 従来の分布型光フアイバー温度センサーは、半導体レー
ザ等の発光部や測定装置の駆動時の変動に起因するドリ
フト(測定値の真の値からの変動)が生じ、また、絶対
的温度分布測定のため恒温槽を設けていたため以下に示
すような問題点を有していた。
[Problem to be solved by the invention] Conventional distributed optical fiber temperature sensors suffer from drift (variations in measured values from true values) due to fluctuations in the driving of the light emitting part such as a semiconductor laser or the measuring device. In addition, since a constant temperature bath was provided to measure the absolute temperature distribution, there were problems as shown below.

■ドリフトが生じた場合、被測定用光ファイバーの温度
分布が真の値から変動していた。
■When drift occurs, the temperature distribution of the optical fiber being measured fluctuates from its true value.

■恒温槽を常に一定温度に保持するための温度コントロ
ーラが必要となっていた。
■A temperature controller was required to keep the constant temperature bath at a constant temperature.

■温度コントローラが設けられていても、常に一定温度
に保持することは容易でなく、微小な温度変動は避けら
れなかった。
■Even if a temperature controller was installed, it was not easy to maintain a constant temperature at all times, and small temperature fluctuations were unavoidable.

■温度コントローラを含め、恒温槽自体が体積が太き(
、システム全体の大型化を招いていた。
■The constant temperature chamber itself, including the temperature controller, has a large volume (
This led to an increase in the size of the entire system.

■恒温槽によっては内蔵した氷水等の冷媒な交換するな
どの調整の必要が生じ、連続運転が不可能な場合があっ
た。
■Depending on the temperature chamber, it may be necessary to make adjustments such as replacing the built-in refrigerant, such as ice water, and continuous operation may not be possible.

[課題を解決するための手段] 本発明は、前述の問題点を解決すべ(なされたものであ
り、被測定光ファイバーヘレーザパルスを入射する発光
部と、被測定光ファイバーからのラマン散乱光を測定装
置へ光路変換する光方向性結合器と、該ラマン散乱光の
距離に関する強度分布から被測定光ファイバーの温度分
布を測定する測定装置とからなる分布型光フアイバー温
度センサーにおいて、該被測定光ファイバーの一部にそ
の温度から絶対的温度分布を測定する校正部を設け、該
校正部に温度センサーを配置したことを特徴とする分布
型光フアイバー温度センサーおよびその一部に温度セン
サーを設けた被測定光ファイバーへ発光部より発振した
レーザパルスを入射し、該被測定光ファイバーからのラ
マン散乱光を光方向性結合器により測定装置へ導光し、
該温度センサーが設けられた部分を校正部とし、該校正
部の反ストークス光強度と他の部分の反ストークス光強
度を比較することにより被測定光ファイバーの絶対的温
度分布を測定することを特徴とする温度測定方法を提供
するものである。
[Means for Solving the Problems] The present invention has been made to solve the above-mentioned problems, and includes a light emitting section that injects a laser pulse into an optical fiber to be measured, and a light emitting section that measures Raman scattered light from the optical fiber to be measured. In a distributed optical fiber temperature sensor consisting of an optical directional coupler that converts the optical path to the device, and a measurement device that measures the temperature distribution of the optical fiber to be measured from the intensity distribution of the Raman scattered light with respect to the distance, one of the optical fibers to be measured is Distributed optical fiber temperature sensor, characterized in that a calibration part for measuring absolute temperature distribution from the temperature is provided in the part, and a temperature sensor is arranged in the calibration part, and an optical fiber to be measured in which a part thereof is provided with a temperature sensor. A laser pulse oscillated from a light emitting part is input to the optical fiber to be measured, and the Raman scattered light from the optical fiber to be measured is guided to a measuring device by an optical directional coupler.
The part where the temperature sensor is provided is used as a calibration part, and the absolute temperature distribution of the optical fiber to be measured is measured by comparing the anti-Stokes light intensity of the calibration part and the anti-Stokes light intensity of other parts. The present invention provides a method for measuring temperature.

[作用] 本発明は、以下に示すような基本原理によって絶対的温
度分布を測定する。
[Operation] The present invention measures absolute temperature distribution based on the basic principle as shown below.

今、この分布型光フアイバー温度センサーのドリフト(
測定値の真の値からの変動)について考える。ドリフト
の要因が、音響光学光スイッチ、光電変換9部、レーザ
パルス発光部、増幅器、AD変換器、信号処理部の被測
定用光フアイバー以外の部分で発生しているならば、そ
の影響は被測定用光ファイバー及び校正用光ファイバー
も同様に受ける。例えば、発光パワーが△P変動した影
響は、被測定用光ファイバー及び校正用光ファイバーも
同様にΔTとして及ぼされる。すなわち、測定結果R(
Q)はR(Q)=t、 (Q)+ΔT (Qは距離、t
 (Q)は真の値)となる。一方、校正部で温度Tと距
離りは既知であるから、以下の処理を行なうと△Tがキ
ャンセルできる。
Now, the drift of this distributed fiber optic temperature sensor (
(variation of the measured value from the true value). If the cause of the drift occurs in the acousto-optic switch, photoelectric conversion section 9, laser pulse emitting section, amplifier, AD converter, and signal processing section other than the optical fiber under test, the influence will not be affected. Measurement optical fibers and calibration optical fibers are also received in the same way. For example, the influence of a ΔP change in the light emission power is similarly exerted on the optical fiber to be measured and the optical fiber for calibration as ΔT. That is, the measurement result R(
Q) is R(Q)=t, (Q)+ΔT (Q is distance, t
(Q) is the true value). On the other hand, since the temperature T and distance are known in the calibration section, ΔT can be canceled by performing the following process.

K=R(L) −T (=ΔT) R(Q)−に=t(Q) 従って、任意の温度でも校正部の温度を測定することに
より、絶対的温度分布の測定が可能となる。
K=R(L) −T (=ΔT) R(Q)−=t(Q) Therefore, by measuring the temperature of the calibration section at any temperature, it becomes possible to measure the absolute temperature distribution.

[実施例] 第1図に本発明の1実施例のブロック図を示す。半導体
レーザ及びその駆動回路等からなるレーザパルス発光部
7から発振したレーザパルスは、未駆動の光方向性結合
器の音響光学光スイッチ4を通じて被測定用光ファイバ
ー1へ入射される。被測定用光ファイバー1の1部は校
正用光ファイバーとして使用され、校正用光ファイバー
2は外界の温度変動の影響を受は難いよう断熱材20中
に内蔵され、温度センサー3が設けられている。被測定
用光ファイバー1で発生したラマン散乱光は、駆動され
た音響光学光スイッチで測定装置へ導光される。測定装
置では以下のような処理が行なわれる。ラマン散乱光中
の反ストーク光をフォトマルチプライヤ−、フォトダイ
オード等の光電変換部5で検出し、増幅器6で増幅して
AD変換器9へ伝送する。AD変換器9でディジタル化
された信号は、信号処理部lOで記憶され10000回
程度の測定径平均化処理がなされる。その際、校正部の
温度を温度センサー3で測定し、その測定信号をスイッ
チ8で切り替えてAD変換器9、信号処理部10へ伝送
して絶対的温度分布の測定を行なう、この場合断熱材2
0によって覆っても、校正用光ファイバー2の温度は時
々刻々変わるので温度センサー3の信号をリアルタイム
に取込む必要がある、本実施例では、リレーや、アナロ
グマルチプレクサ−等のスイッチ8を用いてラマン敗乱
光信号と信号の隙間に時分割多重化している。
[Embodiment] FIG. 1 shows a block diagram of an embodiment of the present invention. A laser pulse emitted from a laser pulse emitting unit 7 consisting of a semiconductor laser, its driving circuit, etc. is incident on the optical fiber 1 to be measured through the acousto-optic optical switch 4 of the undriven optical directional coupler. A part of the optical fiber 1 to be measured is used as a calibration optical fiber, and the calibration optical fiber 2 is housed in a heat insulating material 20 so as to be hardly affected by temperature fluctuations in the outside world, and a temperature sensor 3 is provided. Raman scattered light generated in the optical fiber 1 to be measured is guided to a measuring device by a driven acousto-optic switch. The following processing is performed in the measuring device. Anti-Stokes light in the Raman scattered light is detected by a photoelectric converter 5 such as a photomultiplier or a photodiode, amplified by an amplifier 6, and transmitted to an AD converter 9. The signal digitized by the AD converter 9 is stored in the signal processing unit 10 and subjected to measurement diameter averaging processing approximately 10,000 times. At that time, the temperature of the calibration section is measured by the temperature sensor 3, and the measurement signal is switched by the switch 8 and transmitted to the AD converter 9 and the signal processing section 10 to measure the absolute temperature distribution. 2
0, the temperature of the calibration optical fiber 2 changes from moment to moment, so it is necessary to capture the signal from the temperature sensor 3 in real time. Time division multiplexing is performed in the gap between the scattered optical signal and the signal.

また、AD変換器9との間にインターフェースを追加し
て並列に信号処理部lOへ取込めば、スイッチ8は不要
である。しかし、一般にこの方がスイッチ8を用いるよ
り高価になるので、スイッチ8を使用したほうが好まし
い。断熱材20は、校正用光フアイバ−2全体が均一な
温度となれば不要であるが、一般的に使用した方が外界
の温度変化を受は難いので好ましい、温度センサー3に
は、白金測温体や高精度半導体温度センサー、又は十分
に冷接点補償がなされた熱電対等が用いられている。
Further, if an interface is added between the AD converter 9 and the signal is input to the signal processing unit IO in parallel, the switch 8 is not necessary. However, since this is generally more expensive than using switch 8, it is preferable to use switch 8. The heat insulating material 20 is not necessary if the entire optical fiber 2 for calibration has a uniform temperature, but it is preferable to use it generally because it is difficult to receive temperature changes in the outside world. A hot body, a high-precision semiconductor temperature sensor, or a thermocouple with sufficient cold junction compensation is used.

[発明の効果] 本発明は、任意の温度で校正部の温度を測定することに
より、被測定用光ファイバーの絶対的温度分布の測定が
可能になるという優れた効果を有する。また、従来のよ
うな恒温槽が不要となるのでシステム全体の小型化も達
成され、恒温槽の調整による測定の中断もなく連続運転
が可能となるという効果も有する。
[Effects of the Invention] The present invention has the excellent effect that by measuring the temperature of the calibration section at an arbitrary temperature, it is possible to measure the absolute temperature distribution of the optical fiber to be measured. Furthermore, since the conventional constant temperature bath is not required, the entire system can be downsized, and continuous operation is possible without interrupting measurement due to adjustment of the constant temperature bath.

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

第1図は本発明による分布型光フアイバー温度センサー
のブロック図であり、第2図は従来例のブロック図であ
る。 1:被測定用光ファイバー 2:校正用光ファイバー 3:温度センサー 8:スイッチ
FIG. 1 is a block diagram of a distributed optical fiber temperature sensor according to the present invention, and FIG. 2 is a block diagram of a conventional example. 1: Optical fiber for measurement 2: Optical fiber for calibration 3: Temperature sensor 8: Switch

Claims (2)

【特許請求の範囲】[Claims] (1)被測定光ファイバーへレーザパルスを入射する発
光部と、被測定光ファイバーからのラマン散乱光を測定
装置へ光路変換する光方向性結合器と、該ラマン散乱光
の距離に関する強度分布から被測定光ファイバーの温度
分布を測定する測定装置とからなる分布型光ファイバー
温度センサーにおいて、該被測定光ファイバーの一部に
その温度から絶対的温度分布を測定する校正部を設け、
該校正部に温度センサーを配置したことを特徴とする分
布型光ファイバー温度センサー。
(1) A light emitting unit that injects a laser pulse into the optical fiber to be measured, an optical directional coupler that converts the optical path of the Raman scattered light from the optical fiber to be measured, and an optical directional coupler that converts the optical path of the Raman scattered light from the optical fiber to be measured, and the measured target from the intensity distribution of the Raman scattered light with respect to distance. In a distributed optical fiber temperature sensor comprising a measuring device for measuring temperature distribution of an optical fiber, a part of the optical fiber to be measured is provided with a calibration section for measuring the absolute temperature distribution from the temperature thereof,
A distributed optical fiber temperature sensor characterized in that a temperature sensor is disposed in the calibration section.
(2)その一部に温度センサーを設けた被測定光フアイ
バーへ発光部より発振したレーザパルスを入射し、該被
測定光ファイバーからのラマン散乱光を光方向性結合器
により測定装置へ導光し、該温度センサーが設けられた
部分を校正部とし、該校正部の反ストークス光強度と他
の部分の反ストークス光強度を比較することにより被測
定光ファイバーの絶対的温度分布を測定することを特徴
とする温度測定方法。
(2) A laser pulse oscillated from a light emitting part is input into the optical fiber to be measured, which has a temperature sensor installed in a part thereof, and the Raman scattered light from the optical fiber to be measured is guided to the measuring device by an optical directional coupler. , the part where the temperature sensor is provided is used as a calibration part, and the absolute temperature distribution of the optical fiber to be measured is measured by comparing the anti-Stokes light intensity of the calibration part and the anti-Stokes light intensity of other parts. temperature measurement method.
JP1026604A 1989-02-07 1989-02-07 Distribution type optical fiber temperature sensor and temperature measuring method Pending JPH02206737A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP1026604A JPH02206737A (en) 1989-02-07 1989-02-07 Distribution type optical fiber temperature sensor and temperature measuring method

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP1026604A JPH02206737A (en) 1989-02-07 1989-02-07 Distribution type optical fiber temperature sensor and temperature measuring method

Publications (1)

Publication Number Publication Date
JPH02206737A true JPH02206737A (en) 1990-08-16

Family

ID=12198115

Family Applications (1)

Application Number Title Priority Date Filing Date
JP1026604A Pending JPH02206737A (en) 1989-02-07 1989-02-07 Distribution type optical fiber temperature sensor and temperature measuring method

Country Status (1)

Country Link
JP (1) JPH02206737A (en)

Cited By (4)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPH04118535A (en) * 1990-09-10 1992-04-20 Toshiba Corp Temperature distribution measuring type optical fiber sensor
US6480326B2 (en) 2000-07-10 2002-11-12 Mpb Technologies Inc. Cascaded pumping system and method for producing distributed Raman amplification in optical fiber telecommunication systems
JP2009117134A (en) * 2007-11-05 2009-05-28 Hamamatsu Photonics Kk Manufacturing method of electron beam source
JP2011242142A (en) * 2010-05-14 2011-12-01 Yokogawa Electric Corp Temperature distribution measuring instrument

Cited By (4)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPH04118535A (en) * 1990-09-10 1992-04-20 Toshiba Corp Temperature distribution measuring type optical fiber sensor
US6480326B2 (en) 2000-07-10 2002-11-12 Mpb Technologies Inc. Cascaded pumping system and method for producing distributed Raman amplification in optical fiber telecommunication systems
JP2009117134A (en) * 2007-11-05 2009-05-28 Hamamatsu Photonics Kk Manufacturing method of electron beam source
JP2011242142A (en) * 2010-05-14 2011-12-01 Yokogawa Electric Corp Temperature distribution measuring instrument

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