JPH02201233A - Distribution type optical fiber temperature sensor and its method of temperature measurement - Google Patents

Distribution type optical fiber temperature sensor and its method of temperature measurement

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Publication number
JPH02201233A
JPH02201233A JP1019820A JP1982089A JPH02201233A JP H02201233 A JPH02201233 A JP H02201233A JP 1019820 A JP1019820 A JP 1019820A JP 1982089 A JP1982089 A JP 1982089A JP H02201233 A JPH02201233 A JP H02201233A
Authority
JP
Japan
Prior art keywords
temperature
fiber
measured
optical fiber
light
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
JP1019820A
Other languages
Japanese (ja)
Inventor
Toshihiro Imai
今井 俊宏
Yuzuru Tanabe
譲 田辺
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 JP1019820A priority Critical patent/JPH02201233A/en
Publication of JPH02201233A publication Critical patent/JPH02201233A/en
Pending legal-status Critical Current

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  • Measuring Temperature Or Quantity Of Heat (AREA)

Abstract

PURPOSE:To enable measurement of an absolute temperature distribution of a fiber to be measured by providing a thermostatic device to keep a part of the fiber to be measured at a fixed temperature. CONSTITUTION:A thermostatic device such as Peltier element 8 provided in a fiber 4 to be measured keeps a part of the fiber 4 to be measured provided with the device at a known fixed temperature and serves as a reference temperature part 10 with respect to a change in temperature in a range other than the part. Then, a variation of intensity of an anti-Stokes light pertaining to a variation of temperature for a reference temperature is stored into a computer 7 at a desired point. The reference temperature is preferably a room temperature level of about 20-30 deg.. Thus, the intensity of the anti-Stokes light is compared with the reference temperature part 10 thereby enabling measuring of an absolute temperature distribution of the fiber 4 to be measured.

Description

【発明の詳細な説明】[Detailed description of the invention]

[産業上の利用分野] 本発明は、分布型光ファイバ温度センサ及び温度測定方
法に係り、特に被測定ファイバ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
型光ファイバ温度センサ及び温度測定方法に関するもの
である。 [従来の技術] 光ファイバに高ビークパワーのパルスレーザ光を入射し
た時に生じるラマン散乱光を0TDR法により検出し、
光ファイバに沿った任意の位置の温度を連続的に測定す
る分布型光ファイバ温度センサは知られている。また、
ラマン散乱光を用いる分布型光ファイバ温度センサは、
大別すると次の2方式に分けられる。 (1)反ストークス光のみを検出し、その強度から温度
分布を測定する方法。 (2)反ストークス光とストークス光の強度比を検出し
、温度分布を測定する方法。 本発明は上記(1)の測定方法の以下に示すような問題
点を解消しようとするものである。 [発明の解決しようとする課題] 従来の分布型光ファイバ温度センサの基本的構成を第3
図に示す、光源の半導体レーザ12からのパルスレーザ
光は音響光学素子等の光方向性結合器13を通過し、被
測定ファイバ14に導かれる。被測定ファイバ14から
は、入射光量に応じたラマン散乱光が発生する0発生す
るラマン散乱光中のストークス光1反ストークス光のう
ち、反ストークス光のみをCCD等の検出器15にて検
出後、信号処理装置16において、tooo。 同程度の平均化処理を行なう、処理された信号はコンピ
ューター17によりデータとして表示される。この例で
は、検出器15.信号処理装置16、コンピューター1
7を合わせて測定装置としている。パルス発振器11は
、半導体レーザ12の駆動及び信号処理装置16のトリ
ガ信号の発振を行う。この系において問題となるのは検
出光として反ストークス光のみを用いるので、被測定フ
ァイバ14の温度変化を、相対的にしか知ることができ
ないことであった。即ち、周辺の温度が変化すると測定
値が変化してしまい、絶対的な温度測定ができないとい
う問題を有していた。
[Industrial Application Field] The present invention relates to a distributed optical fiber temperature sensor and a temperature measurement method, and in particular to a distributed optical fiber temperature sensor that measures the absolute temperature distribution from the intensity of anti-Stokes light among the Raman scattered light of a fiber to be measured. The present invention relates to a fiber temperature sensor and a temperature measurement method. [Prior art] Raman scattered light generated when a high peak power pulsed laser beam is input into an optical fiber is detected by the 0TDR method,
Distributed optical fiber temperature sensors that continuously measure temperature at arbitrary positions along an optical fiber are known. Also,
A distributed optical fiber temperature sensor using Raman scattered light is
Broadly speaking, it can be divided into the following two methods. (1) A method of detecting only anti-Stokes light and measuring temperature distribution from its intensity. (2) A method of detecting the intensity ratio of anti-Stokes light and Stokes light and measuring temperature distribution. The present invention aims to solve the following problems of the measurement method (1) above. [Problem to be solved by the invention] The basic configuration of the conventional distributed optical fiber temperature sensor is
Pulsed laser light from a semiconductor laser 12 as a light source shown in the figure passes through an optical directional coupler 13 such as an acousto-optic device, and is guided to a fiber 14 to be measured. From the fiber to be measured 14, Raman scattered light is generated according to the amount of incident light. , in the signal processing device 16, tooo. The processed signal, which is subjected to the same level of averaging processing, is displayed as data by the computer 17. In this example, detector 15. Signal processing device 16, computer 1
7 together constitute a measuring device. The pulse oscillator 11 drives the semiconductor laser 12 and oscillates a trigger signal for the signal processing device 16 . A problem with this system is that only the anti-Stokes light is used as the detection light, so the temperature change in the fiber 14 to be measured can only be known relatively. That is, when the surrounding temperature changes, the measured value changes, and there is a problem that absolute temperature measurement cannot be performed.

【課題を解決するための手段】[Means to solve the problem]

本発明は、前述の問題点を解決すべ(なされたものであ
り、被測定ファイバへパルスレーザ光を入射する光源と
、被測定ファイバ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ファイバ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温度センサにおい
て1、該被測定ファイバの一部を一定温度に保持する恒
温装置を設けたことを特徴とする分布型光ファイバ温度
センサ及びその一部に温度を一定に保持する恒温装置を
設けた被測定ファイバへ光源より発振したパルスレーザ
光を入射し、該被測定ファイバ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、該恒温装置が設
けられた部分を基準温度部とし、該基準温度部の反スト
ークス光強度と他の部分の反ストークス強度を比較する
ことにより被測定ファイバ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。 【作用] 本発明において、被測定ファイバ中に設けられたベルチ
ェ素子等の恒温装置は、恒温装置の設けられた被測定フ
ァイバの部分を既知の一定温度に保ち、それ以外の範囲
における温度変化に対して、基準温度部となる。よって
、基準温度に対する温度変化量に関する反ストークス光
強度の変化量を任意の点でコンピューターに記憶してお
けば、被測定ファイバの任意の点の絶対温度を計測する
ことができる。 [実施例] 本発明の実施例を第1図と第2図に示す。 光源の半導体レーザ2からのパルスレーザ光は音響光学
素子等の光方向性結合器3を通過し、被測定ファイバ4
に導かれる。被測定ファイバ4からは、入射光量に応じ
たラマン散乱光が発生する0発生するラマン散乱光中の
ストークス光1反ストークス光のうち、反ストークス光
のみをCCD等の検出器5にて検出後、信号処理装置6
において、10000回程度の平均化処理を行なう、処
理された信号はコンピューター7によりデータとして表
示される。この例では、検出器5、信号処理装置6、コ
ンピューター7を合わせて測定装置としている。パルス
発振器1は、半導体レーザ2の駆動及び信号処理装置6
のトリガ信号の発振を行なう、基準温度部lOとなる部
分は、素線もしくは心線で直径30mm程度のベルチェ
素子8を内蔵したドラムに巻かれる0巻かれる被測定フ
ァイバ4の長さは、システムにおける分解能により異な
るが、分解能程度以上、即ち分解能が±10 m程度の
場合20 ra程度以上巻きつければ十分である。実際
には短いほどよいのでこの例では20 mとされればよ
い。又、この部分の温度が常に一定になるように、コン
ピューター7により温度コントローラー9を通じて制御
される。 測定データの処理例を第2図に示す。通常、被測定ファ
イバからのラマン散乱光強度の距離に関する信号波形は
、eの指数関数で表わされる減衰曲線となる。しかし、
本発明においては、基準温度に対する温度変化量に関す
る反ストークス光強度の変化量を任意の点でコンビエー
タ−に記憶しておき、絶対的な温度変化のみを取り出し
表示するよう処理している。従って、第2図に示すよう
温度変化のない部分は、距離に関して減衰曲線とならず
平坦な直線状となり、温度変化のあった部分のみを表示
できる。 また、基準温度部を作り出す恒温装置は、室温よりも高
温に保ってもよいし、低温に保ってもよく、ペルチェ素
子の他に電熱線を内蔵した恒温槽等が使用でき、基準温
度としては約20℃〜30℃の室温レベルが好ましい。 [発明の効果] 本発明は、反ストークス光強度を基準温度部と比較して
被測定ファイバの絶対的温度分布を測定できるという優
れた効果を有する。
The present invention has been made to solve the above-mentioned problems, and includes a light source that injects a pulsed laser beam into a fiber to be measured, and an optical directional coupling that converts the optical path of Raman scattered light from the fiber to be measured to a measuring device. In a distributed optical fiber temperature sensor consisting of a measuring device that measures the temperature distribution of the fiber to be measured from the intensity distribution of the Raman scattered light with respect to the distance, 1. A constant temperature sensor that maintains a part of the fiber to be measured at a constant temperature; A distributed optical fiber temperature sensor is characterized in that it is equipped with a device, and a part of the fiber to be measured is provided with a constant temperature device that keeps the temperature constant. The Raman scattered light from the is guided to the measurement device by an optical directional coupler, and the part where the constant temperature device is installed is set as a reference temperature part, and the anti-Stokes light intensity in the reference temperature part and the anti-Stokes intensity in other parts are calculated. The present invention provides a temperature measurement method characterized by measuring the absolute temperature distribution of the fiber under test by comparing the The constant temperature device maintains the part of the fiber under test where the constant temperature device is installed at a known constant temperature, and serves as a reference temperature section for temperature changes in other ranges.Therefore, the reaction regarding the amount of temperature change with respect to the reference temperature is By storing the amount of change in the Stokes light intensity in a computer at an arbitrary point, the absolute temperature at an arbitrary point on the fiber to be measured can be measured. [Example] An example of the present invention is shown in Fig. 1. It is shown in Fig. 2. Pulsed laser light from a semiconductor laser 2 as a light source passes through an optical directional coupler 3 such as an acousto-optic device, and is connected to a fiber under test 4.
guided by. From the fiber to be measured 4, Raman scattered light is generated according to the amount of incident light. , signal processing device 6
In this step, the processed signal, which is averaged approximately 10,000 times, is displayed as data by the computer 7. In this example, the detector 5, signal processing device 6, and computer 7 are collectively used as a measuring device. The pulse oscillator 1 is a driver for the semiconductor laser 2 and a signal processing device 6
The reference temperature section 1O, which oscillates the trigger signal of Although it varies depending on the resolution, if the resolution is higher than the resolution, that is, the resolution is about ±10 m, it is sufficient to wrap the wire around 20 ra or more. Actually, the shorter the distance, the better, so in this example, it may be 20 m. Further, the computer 7 controls the temperature through the temperature controller 9 so that the temperature of this part is always constant. FIG. 2 shows an example of processing the measurement data. Usually, the signal waveform of the Raman scattered light intensity relative to the distance from the fiber under test is an attenuation curve expressed by an exponential function of e. but,
In the present invention, the amount of change in the anti-Stokes light intensity with respect to the amount of temperature change with respect to the reference temperature is stored in the combinator at an arbitrary point, and only the absolute temperature change is extracted and displayed. Therefore, as shown in FIG. 2, the portions where there is no temperature change do not form an attenuation curve with respect to distance, but form a flat straight line, and only the portions where the temperature has changed can be displayed. In addition, the constant temperature device that creates the reference temperature section may be kept at a higher or lower temperature than room temperature, and in addition to the Peltier element, a constant temperature chamber with a built-in heating wire can be used, and the reference temperature can be Room temperature levels of about 20°C to 30°C are preferred. [Effects of the Invention] The present invention has an excellent effect in that the absolute temperature distribution of the fiber to be measured can be measured by comparing the anti-Stokes light intensity with a reference temperature section.

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

第1図と第2図は本発明の実施例を示し、第1図は分布
型光ファイバ温度センサのブロック図であり、第2図は
コンピューターによって処理されたデータの表示例を示
すグラフであり、第3図は従来の分布型光ファイバ温度
センサのブロック図である。 4・・・被測定ファイバ  7・・・コンピューター8
・・・ペルチェ素子 第1図 第2図
1 and 2 show embodiments of the present invention, FIG. 1 is a block diagram of a distributed optical fiber temperature sensor, and FIG. 2 is a graph showing an example of displaying data processed by a computer. , FIG. 3 is a block diagram of a conventional distributed optical fiber temperature sensor. 4...Fiber under test 7...Computer 8
...Peltier element Figure 1 Figure 2

Claims (2)

【特許請求の範囲】[Claims] (1)被測定ファイバへパルスレーザ光を入射する光源
と、被測定ファイバ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ファイバ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温度センサにお
いて、該被測定ファイバの一部を一定温度に保持する恒
温装置を設けたことを特徴とする分布型光ファイバ温度
センサ。
(1) A light source that injects a pulsed laser beam into the fiber under test, an optical directional coupler that converts the optical path of the Raman scattered light from the fiber under test to the measuring device, and a measured object based on the intensity distribution of the Raman scattered light with respect to distance. 1. A distributed optical fiber temperature sensor comprising a measuring device for measuring the temperature distribution of a fiber, the distributed optical fiber temperature sensor comprising a constant temperature device that maintains a part of the fiber to be measured at a constant temperature.
(2)その一部に温度を一定に保持する恒温装置を設け
た被測定ファイバへ光源より発振したパルスレーザ光を
入射し、該被測定ファイバ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、該恒温装置が設けら
れた部分を基準温度部とし、該基準温度部の反ストーク
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
とにより被測定ファイバ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 pulsed laser beam oscillated from a light source is input into the fiber to be measured, which is equipped with a constant temperature device that keeps the temperature constant, and the Raman scattered light from the fiber to be measured is measured by an optical directional coupler. The absolute temperature of the fiber to be measured is determined by guiding the light to the device, setting the part where the constant temperature device is installed as a reference temperature part, and comparing the anti-Stokes light intensity in the reference temperature part with the anti-Stokes light intensity in other parts. A temperature measurement method characterized by measuring distribution.
JP1019820A 1989-01-31 1989-01-31 Distribution type optical fiber temperature sensor and its method of temperature measurement Pending JPH02201233A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP1019820A JPH02201233A (en) 1989-01-31 1989-01-31 Distribution type optical fiber temperature sensor and its method of temperature measurement

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP1019820A JPH02201233A (en) 1989-01-31 1989-01-31 Distribution type optical fiber temperature sensor and its method of temperature measurement

Publications (1)

Publication Number Publication Date
JPH02201233A true JPH02201233A (en) 1990-08-09

Family

ID=12009954

Family Applications (1)

Application Number Title Priority Date Filing Date
JP1019820A Pending JPH02201233A (en) 1989-01-31 1989-01-31 Distribution type optical fiber temperature sensor and its method of temperature measurement

Country Status (1)

Country Link
JP (1) JPH02201233A (en)

Cited By (5)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPH05157635A (en) * 1991-12-03 1993-06-25 Tokyo Electric Power Co Inc:The Optical fiber type temperature distribution measuring device
US6817759B2 (en) * 2001-11-30 2004-11-16 National Chiao Tung University Method of enhancing spatial resolution for distributed temperature measurement
WO2008023695A1 (en) * 2006-08-24 2008-02-28 Sumitomo Electric Industries, Ltd. Optical fiber temperature sensor
JP2013092388A (en) * 2011-10-24 2013-05-16 Yokogawa Electric Corp Fiber temperature distribution measurement device
CN104389588B (en) * 2014-11-14 2017-02-22 大连理工大学 Single-light-source optical fiber distribution temperature and fixed-point pressure measurement system and method

Cited By (7)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPH05157635A (en) * 1991-12-03 1993-06-25 Tokyo Electric Power Co Inc:The Optical fiber type temperature distribution measuring device
US6817759B2 (en) * 2001-11-30 2004-11-16 National Chiao Tung University Method of enhancing spatial resolution for distributed temperature measurement
WO2008023695A1 (en) * 2006-08-24 2008-02-28 Sumitomo Electric Industries, Ltd. Optical fiber temperature sensor
US7997792B2 (en) 2006-08-24 2011-08-16 Sumitomo Electric Industries, Ltd. Optical fiber temperature sensor
JP2013092388A (en) * 2011-10-24 2013-05-16 Yokogawa Electric Corp Fiber temperature distribution measurement device
US9046425B2 (en) 2011-10-24 2015-06-02 Yokogawa Electric Corporation Opticalfiber temperature distribution measurement apparatus
CN104389588B (en) * 2014-11-14 2017-02-22 大连理工大学 Single-light-source optical fiber distribution temperature and fixed-point pressure measurement system and method

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