JPH02201132A - Optical fiber system distribution type temperature sensor - Google Patents
Optical fiber system distribution type temperature sensorInfo
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- JPH02201132A JPH02201132A JP1019994A JP1999489A JPH02201132A JP H02201132 A JPH02201132 A JP H02201132A JP 1019994 A JP1019994 A JP 1019994A JP 1999489 A JP1999489 A JP 1999489A JP H02201132 A JPH02201132 A JP H02201132A
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Abstract
Description
【発明の詳細な説明】
[産業上の利用分野]
本発明は温度センサ、特に光ファイバ式分布形温度セン
サに関するものである。DETAILED DESCRIPTION OF THE INVENTION [Field of Industrial Application] The present invention relates to a temperature sensor, and particularly to an optical fiber type distributed temperature sensor.
[従来の技術]
光ファイバ式分布形温度センサは、光フアイバ中のラマ
ン散乱光やレーり散乱光等の散乱光強度が温度によって
変化することを利用し、この変化を公知の0TDR(O
ptical tine DoIla+nRefiec
toietry)の手法で検知することにより、光ファ
イバの長手方向に沿った温度分布を計測するものである
。[Prior Art] Optical fiber type distributed temperature sensors utilize the fact that the intensity of scattered light such as Raman scattered light and Ray scattered light in an optical fiber changes depending on the temperature, and this change is detected by the well-known 0TDR (O
ptical tine DoIla+nRefiec
temperature distribution along the longitudinal direction of the optical fiber.
ラマン散乱光を利用した光ファイバ式分布形温度センサ
(以下、単にラマン式温度センサと呼ぶ)の計測概念を
第7図を用い以下に説明する。The measurement concept of an optical fiber distributed temperature sensor (hereinafter simply referred to as a Raman temperature sensor) using Raman scattered light will be explained below using FIG.
光源からパルス光(パルス’kA T * 、パルス周
期Tp)をセンサ用光ファイバに導くと、該光フアイバ
内でアンチストークス光やストークス光等の後方散乱光
(反射光)が励起され、その一部は計測装置に戻る。こ
の反射光をパルス光入射時刻を1=0とし、サンプリン
グ時間間隔T sで計測すると、アンチストークス光や
ストークス光の強度の時間関数1 a (t)、 I
s (t)がサンプリング時間間隔Tsの関数として求
まる。このとき、これらの比1 a (t) / I
s (j)が純粋に温度の関数であること、及び光パル
ス入射後、光フアイバ内の距離Xの位置で発生した反射
光が光パルス入射端(反射光計測部)に戻ってくるまで
の時間が2XX/’Coであること(CO;光フアイバ
中の光速)を利用すると、光ファイバの沿った線状の温
度分布が測定できる。When pulsed light (pulse 'kA T *, pulse period Tp) is guided from a light source to a sensor optical fiber, backscattered light (reflected light) such as anti-Stokes light and Stokes light is excited within the optical fiber, and one of the The section returns to the measuring device. When this reflected light is measured at a sampling time interval T s with the pulsed light incident time being 1=0, the time function of the intensity of the anti-Stokes light and Stokes light is 1 a (t), I
s (t) is determined as a function of the sampling time interval Ts. At this time, these ratios 1 a (t) / I
s (j) is purely a function of temperature, and the time it takes for the reflected light generated at a distance X within the optical fiber to return to the optical pulse input end (reflected light measurement section) By utilizing the fact that the time is 2XX/'Co (CO: the speed of light in an optical fiber), the linear temperature distribution along the optical fiber can be measured.
なお、反射光が計11される時間幅′「rは2xL/C
oであり(L;光ファイバ長さ)、この時間はTr内の
計測値が有効な温度分布情報を与える。In addition, the time width 'r' during which the reflected light is reflected is 2xL/C.
o (L: optical fiber length), and during this time, the measured value within the Tr provides effective temperature distribution information.
次に、第8図を用いて、ラマン式温度センサの概要を説
明する。Next, the outline of the Raman type temperature sensor will be explained using FIG.
このラマン式温度センサは、計測装置10とセンサ用光
ファイバ20から構成される。光源2からパルス光をセ
ンサ用光ファイバ20に導くと、該光フアイバ内で後方
散乱光(反射光)が励起され、励起された反射光の一部
は計測装置10側に戻り、光分岐器31、光ファイバ2
2を介して、光分岐器32に導かれる。This Raman temperature sensor is composed of a measuring device 10 and a sensor optical fiber 20. When pulsed light is guided from the light source 2 to the sensor optical fiber 20, backscattered light (reflected light) is excited within the optical fiber, and a part of the excited reflected light returns to the measurement device 10 side and is sent to the optical splitter. 31, optical fiber 2
2 to the optical splitter 32.
光分岐器32で1分された反射光のうち、光ファイバ2
3aに導かれたものは、アンチストークス光用の光学フ
ィルタ4 a、受光器5a及び平均化処理回路6aで構
成されるアンチストークス光/nOT D R計測回路
3Qaに入り、この光強度がらアンチストークス光強度
の時間関数J a(t)が求められる。他方、光分岐器
32で1分された後方散乱光のうち、光ファイバ23s
に樺がれたしのは、ストークス充用の光学フィルタ4s
、受光器5s及び平均化処理回路6sで構成されるスト
ークス光m0TDR計測回路30sに入り、この光強度
からストークス光強度の時間関数! 5(t)が求めら
れる。パルス光源2と平均化処J’!!!回1i136
a6sの同m1合せは、トリガ回路Iの同期信号によ
って行い、反射光のサンプリングは平均化処理回路6a
、6s内で、第7図に示す一定の時間間隔T sで行わ
れる。Of the reflected light split by the optical splitter 32, the optical fiber 2
3a enters the anti-Stokes light/nOT D R measurement circuit 3Qa, which is composed of an optical filter 4a for anti-Stokes light, a light receiver 5a, and an averaging processing circuit 6a, and the light intensity is used to measure the anti-Stokes light. A time function J a(t) of light intensity is determined. On the other hand, of the backscattered light split into one part by the optical splitter 32, the optical fiber 23s
This is an optical filter for Stokes 4s.
, enters the Stokes light m0TDR measuring circuit 30s, which is composed of a light receiver 5s and an averaging processing circuit 6s, and from this light intensity, the time function of the Stokes light intensity! 5(t) is obtained. Pulse light source 2 and averaging process J'! ! ! times 1i136
The same m1 matching of a6s is performed by the synchronization signal of the trigger circuit I, and the sampling of the reflected light is performed by the averaging processing circuit 6a.
, 6s at constant time intervals Ts as shown in FIG.
得られた時間関数I a(t)及びl5(t)を温度分
布演算回路7に入力し、I a(t)/ I 5(t)
の演算を行うことにより、センサm光ファイバに沿った
線状温度分布測定を行っている。The obtained time functions Ia(t) and l5(t) are input to the temperature distribution calculation circuit 7, and Ia(t)/I5(t)
By performing the calculation, the linear temperature distribution along the optical fiber of sensor m is measured.
また、平均化処理口1i’36は、第9図に示すように
、A/D変#A回路61、加算器62、メモリ回Ii¥
f63、同期回路64から構成される。平均化処理は以
下のようにして行う。Further, the averaging processing port 1i'36 includes an A/D conversion #A circuit 61, an adder 62, a memory circuit Ii'36, as shown in FIG.
f63 and a synchronization circuit 64. The averaging process is performed as follows.
受光器5から入力されたアナログ量をA/D変換回路6
1でディジタル量に変換し、そのディジタル量とメモリ
回路63に記憶されたディジタル量との和を加算器62
で行い、その結果を再び、メモリ回路63に記憶する。The analog quantity input from the light receiver 5 is converted into an A/D conversion circuit 6.
1 into a digital quantity, and the adder 62 adds the sum of the digital quantity and the digital quantity stored in the memory circuit 63.
The results are stored in the memory circuit 63 again.
この操作をパルス周期T”Pごとに、繰返し行い、最終
的にメモリ回路63に記憶された値を繰返し回数で割る
と、入力情報の平均値が求まる。この平均化処理を行う
と、入力情報に含まれたノイズが除去されるため、温度
測定精度は向上する。This operation is repeated for each pulse period T''P, and the value finally stored in the memory circuit 63 is divided by the number of repetitions to find the average value of the input information.When this averaging process is performed, the input information Since the noise included in the temperature is removed, the accuracy of temperature measurement is improved.
また、A/D変換回路61、加算器62、メモリ回路6
3の同期合わせは同期回路64によって行われている。Also, an A/D conversion circuit 61, an adder 62, a memory circuit 6
3 is synchronized by a synchronization circuit 64.
このラマン式温度センサは、例えば電力ゲーブルに沿わ
せてセンサ用光ファイバを敷設することにより、電カケ
ープルの長手方向の温度分布を知ることができ、送電容
量の制御等に利用したり、ゲーブルの劣化等により生じ
る部分的に温度の高い箇所の検知等が行なえる。また、
ビルやトンネル等の火災検知用として使用すれば、火災
発生位置の標定を行うこともできる。This Raman temperature sensor can detect the temperature distribution in the longitudinal direction of the power cable by laying a sensor optical fiber along the power cable, for example, and can be used to control the power transmission capacity, etc. It is possible to detect areas where the temperature is partially high due to deterioration or the like. Also,
If used for fire detection in buildings, tunnels, etc., it can also be used to locate the location of a fire outbreak.
[発明が解決しよとする課ul
ラマン式温度センサあるいはレーリ式温度センサは上述
した方法で線状の温度分布が測定できる有望な方式であ
り、その高機能化を図るなめ温度精度や距離分解能を向
上させる検討が進められている。[Issues to be solved by the invention] The Raman temperature sensor or Rayleigh temperature sensor is a promising method that can measure linear temperature distribution using the method described above. Studies are underway to improve this.
温度精度を向上させる為には、微弱な信号からノイズの
影響を除去するため、平均化処理回路の処理回数を大巾
に大きくしてやる必要があり、これに対応して、平均化
処理回路の処理ビット数も大きくしてやらねばならない
。In order to improve temperature accuracy, it is necessary to significantly increase the number of processing times of the averaging processing circuit in order to remove the influence of noise from weak signals. The number of bits must also be increased.
また、距離分解能を向上するためには、サンプリング時
間を短くする必要がある。Furthermore, in order to improve the distance resolution, it is necessary to shorten the sampling time.
しかし、第6図に示すように、処理ビット数Nbを大き
くするほど、処理時間tが長くなるため、高速形の回路
素子を用いても、所要のサンプリング時間間隔Ts内に
平均化処理ができない場合が生じる。特に、サンプリン
グ時間間隔Tsが短くなるほど、この傾向が顕著となる
。However, as shown in FIG. 6, as the number of processing bits Nb increases, the processing time t becomes longer, so even if high-speed circuit elements are used, the averaging process cannot be performed within the required sampling time interval Ts. A situation may arise. In particular, this tendency becomes more pronounced as the sampling time interval Ts becomes shorter.
このような観点から、上記分布形温度センサでは、温度
精度や距離分解能の向上を図ることは困難とされていた
。From this point of view, it has been difficult to improve temperature accuracy and distance resolution in the distributed temperature sensor.
本発明の目的は、前記した従来技術の欠点を解消し、温
度精度や距離分解能が高く、かつ、安価な光ファイバ式
分布形温度センサを提供することにある。SUMMARY OF THE INVENTION An object of the present invention is to eliminate the drawbacks of the prior art described above, and to provide an optical fiber type distributed temperature sensor that has high temperature accuracy and distance resolution and is inexpensive.
[課題を解決するための手Pi]
本発明の光ファイバ式分布形温度センサは、計測系内の
光源からセンサ用光ファイバに光パルスを入射させ、該
ファイバで発生する後方散乱光で形成される反射光を計
測系に導き、これら反射光の光強度を平均化処理装置に
よりサンプリングして平均化し、そのデータから光ファ
イバの温度を求め、光パルスの入射光時刻と反射光が計
測系へ到達する時刻の差から後方散乱光の発生位置を求
めることにより、温度と位置を同時計測し、該光ファイ
バの温度分布を計測する光ファイバ式分布形温度センサ
において、前記平均化処理装置をA/D変換器、前段加
算回路及び後段加算回路を直列に接続して構成し、前段
加算回路の処理ビット数をA/D変換器の出力ビット数
より大きく、かつ、後段加算回路の処理ビット数より少
なくした構成のものである。[Measures Pi for Solving the Problems] The optical fiber type distributed temperature sensor of the present invention allows a light pulse to be incident on a sensor optical fiber from a light source in a measurement system, and is formed by backscattered light generated in the fiber. The reflected light is guided to the measurement system, the light intensity of these reflected lights is sampled and averaged by an averaging processing device, the temperature of the optical fiber is determined from the data, and the incident light time of the optical pulse and the reflected light are sent to the measurement system. In an optical fiber type distributed temperature sensor that simultaneously measures temperature and position by determining the generation position of backscattered light from the difference in arrival times and measures the temperature distribution of the optical fiber, the averaging processing device is /D converter, front-stage addition circuit, and rear-stage addition circuit are connected in series, and the number of processing bits of the front-stage addition circuit is larger than the number of output bits of the A/D converter, and the number of processing bits of the rear-stage addition circuit is This is a configuration with a smaller number.
前記平均化処理装置に代えて、A/D変換器とその出力
を並列処理する複数組の加算回路とで構成され、各組の
加算回路の処理時間をサンプリング時間間隔の前記組数
倍の時間内とした平均化処理装置を備えてもよい。Instead of the averaging processing device, it is composed of an A/D converter and a plurality of sets of adding circuits that process the output thereof in parallel, and the processing time of each set of adding circuits is a time equal to the sampling time interval times the number of sets. An averaging processing device may be provided.
また、前記平均化処理装置に代えて、A/D変換器と、
複数回路で並列処理する前段加算回路と及び後段加算回
路とで構成した平均化処理装置を備えてもよい。Further, in place of the averaging processing device, an A/D converter;
An averaging processing device may be provided that includes a front-stage addition circuit and a rear-stage addition circuit that perform parallel processing using a plurality of circuits.
し作用1
本発明の要点は、平均化処理装置内の加算回路を、前段
と後段の回路に分け、前段回路の処理ビット数をA/D
変換器の出力と−y ト数より大きく、かつ、後段回路
の処理ビット数より少なくしたことにある。Function 1 The main point of the present invention is that the adding circuit in the averaging processing device is divided into a front-stage circuit and a rear-stage circuit, and the number of processing bits of the front-stage circuit is reduced by A/D.
The reason is that the output of the converter and -y are larger than the number of bits and smaller than the number of bits processed by the subsequent circuit.
前段加算回路の処理ビット数を選定するに当って考慮す
べき点は、後段加算回路は前段加算回路の出力を受けて
動作するため、その処理許容時間が比較的長くなること
から、前段加算回路の処理ビット数Nbを少なくするこ
とが有利であること、更には、その使用する回路素子に
高速の素子を使用しないで済むような工夫をなすことで
ある。この要求は、前段加算回路の処理ビット数をA、
/ D変換器の出力ビット数より大きく、がっ、後段
加算回路の処理ビット数より少なくすることで満たされ
、従来と同様な機能の回路素子を用いても、処理ビット
数が高く、かつ、サンプリング時間が短い平均化処理装
置を実現できる。When selecting the number of processing bits for the pre-stage adder circuit, the following points should be considered: Since the post-adder circuit operates by receiving the output from the pre-stage adder circuit, the allowable processing time is relatively long. It is advantageous to reduce the number of bits Nb to be processed, and furthermore, it is advantageous to devise a method that eliminates the need to use high-speed circuit elements. This request requires that the number of bits processed by the pre-addition circuit be A,
/ It can be satisfied by making the number of output bits larger than the output bits of the D converter, but smaller than the number of processing bits of the post-addition circuit, and even if circuit elements with the same functions as conventional ones are used, the number of processing bits is high, and An averaging processing device with short sampling time can be realized.
このように処理ビット数を高くできると平均化処理回数
を多くでき、ノイズの影響を除去して温度精度を高める
ことができる。また、サンプリング時間を短くできるな
め、距離分解能の高い光ファイバ式分布形温度センサを
実現できる。If the number of processing bits can be increased in this way, the number of times of averaging processing can be increased, and the influence of noise can be removed to improve temperature accuracy. Furthermore, since the sampling time can be shortened, an optical fiber type distributed temperature sensor with high distance resolution can be realized.
また、加算回路全体又は前段加算回路を複数回路で並列
処理することにより、平均化処理回路の処理ビット数を
大きくしても、短いサンプリング時間間隔で、処理可能
となり、温度精度や距超分解能を顕著に向上できる。In addition, by processing the entire adder circuit or the pre-adder circuit in parallel using multiple circuits, even if the number of processing bits of the averaging processing circuit is increased, the processing can be performed with a short sampling time interval, improving temperature accuracy and distance resolution. It can be significantly improved.
[実施例]
以下、本発明によるラマン散乱光利用先ファイバ式分布
形温度センサの実施例を、第1図により説明する。[Example] Hereinafter, an example of a fiber type distributed temperature sensor using Raman scattered light according to the present invention will be described with reference to FIG.
本実施例による光ファイバ式分布形温度センサの基本概
念及び構成は、第7図〜第9図に示す従来例とほぼ同じ
であり、異なる点は平均化処理回路6の加算器l?86
00を前段加算器#1601と後段加算回路602に分
けたことである。The basic concept and configuration of the optical fiber type distributed temperature sensor according to this embodiment is almost the same as the conventional example shown in FIGS. 7 to 9, and the difference is that the adder l? 86
00 is divided into a pre-stage adder #1601 and a post-stage adder circuit 602.
このとき、前段加算回路601は加算器62aとメモリ
63a″′C″楕成され、後段加算回路602は加jl
!、器62bとメモリ63b″C′梢成される。At this time, the front-stage addition circuit 601 is configured with the adder 62a and the memory 63a''C'', and the rear-stage addition circuit 602 is configured with the adder 62a and the memory 63a''C''.
! , a storage device 62b and a memory 63b''C'.
次に、加算回路600の動作について述べる。Next, the operation of adder circuit 600 will be described.
加算器1?1600のR能は第9図で説明した従来のも
と同じであるが、異なる点は以下の通りである。The R performance of the adder 1-1600 is the same as that of the conventional adder explained in FIG. 9, but the differences are as follows.
即ち、A/D変換器61でディジタル量に変換された値
を前段加算回路601に入力し、ここで各計測入力情報
を加算し、加算回数がある回数NOに達すると、その加
算結果を後段加算回路602に入力し、メモリ63a内
の記憶をクリアする。後段加算回路602は、加算回数
NOごとに、前段加算回路601の加算結果が入力され
、前に記憶した値と加算して、メモリ63bに入力する
。この操作を繰返すと、その最終結果が加算回路600
の全体の出力となる。That is, the value converted into a digital quantity by the A/D converter 61 is input to the pre-stage addition circuit 601, where each piece of measurement input information is added, and when the number of additions reaches a certain number NO, the addition result is sent to the post-stage addition circuit 601. The signal is input to the addition circuit 602 and the storage in the memory 63a is cleared. The post-addition circuit 602 receives the addition result of the pre-stage addition circuit 601 for each addition number NO, adds it to the previously stored value, and inputs the result to the memory 63b. When this operation is repeated, the final result is added to the adder circuit 600.
This is the entire output of
尚、加算回数NOは一定の値と設定してもよく、あるい
は、前段加算回路601の加算結果が処理ピント以上に
達した段階としても良い。Note that the number of additions NO may be set to a constant value, or may be set to a stage when the addition result of the pre-stage addition circuit 601 reaches the processing focus or higher.
次に、前段加算回路601の処理ビット数Nbの選定方
法について説明する。ここでは、サンプリング時間間隔
TsをT′5=2On、S、A/D変換器61の処理ビ
ット数を8ピツト、そして後段加算0路602の処理ビ
ット数を32ビットとした場合について述べる。Next, a method for selecting the number of processing bits Nb of the pre-stage addition circuit 601 will be explained. Here, a case will be described in which the sampling time interval Ts is T'5=2On, the number of processing bits of the S, A/D converter 61 is 8 bits, and the number of processing bits of the post-addition zero path 602 is 32 bits.
前段加算回路601と後段加算回路602(以下必要に
応じ「前段」 「後段」という)の処理時間をta 、
tbとし、それぞれの処理許容時間を]a。The processing time of the front-stage addition circuit 601 and the rear-stage addition circuit 602 (hereinafter referred to as "first stage" and "second stage" as necessary) is ta,
Let tb be the allowable processing time for each] a.
Tbとする。Let it be Tb.
前段の処理時間taは、その処理ビット数Nbの数に応
じて直線的に増加するので、その比例定数(傾き)をb
と置き、Nb=Oのときの遅れを定数aとすると、前段
の処理時間taは次式で表わされる。Since the processing time ta of the previous stage increases linearly according to the number of processing bits Nb, its proportionality constant (slope) is expressed as b
, and if the delay when Nb=O is a constant a, the processing time ta of the previous stage is expressed by the following equation.
ta=a+b−Nb
また、後段の処理時間しbは、求めるNbとは無関係で
あるから、これを定数tboと置く。ta=a+b-Nb Furthermore, since the subsequent processing time b has nothing to do with the desired Nb, it is set as a constant tbo.
tb=tb。tb=tb.
次に、前段の処理はサンプリング時間間隔Ts(20n
S)内でのみ可能であるがら、その前段の処理許容時間
Taはサンプリング時間間隔Tsで定まる。Next, the first stage processing is performed at a sampling time interval Ts (20n
Although this is possible only within S), the processing allowable time Ta for the preceding stage is determined by the sampling time interval Ts.
Ta=Ts
また、後段の処理許容時間Tbは、前段のメモリ63a
が最大になるまで後段を動作させる必要がないことを考
慮すれば、サンプリング時間間隔Tsに対して次の関係
に立つ。Ta=Ts Also, the allowable processing time Tb of the subsequent stage is the memory 63a of the previous stage.
Considering that there is no need to operate the subsequent stage until Ts reaches its maximum, the following relationship holds true for the sampling time interval Ts.
T b =T s −2”’
このようにt&段の処理許容時間Tbが前段の処理許容
時間Taより長くなるのは、前段のメモリ63bが最大
になるまで後段を動作させる必要がないので、その最小
時間は、A/D変換器61への入力が毎回最大値(8ビ
ット)となったときに定まり、その比は2 N1′/
2 a = 2 N−8となるからである。T b =T s -2''' The reason why the allowable processing time Tb of the t& stage is longer than the allowable processing time Ta of the preceding stage is because there is no need to operate the succeeding stage until the memory 63b of the preceding stage reaches its maximum. The minimum time is determined when the input to the A/D converter 61 reaches the maximum value (8 bits) each time, and the ratio is 2 N1'/
This is because 2 a = 2 N-8.
考慮すべき点は、後段加算回路602の処理許容時間T
bは比較的長いので、前段加算回路601の処理ビット
数をNbを少なくすることが有利であること、更には、
そ・の使用する素子に高速の素子を使用しないで済むよ
うな工夫である。What should be considered is the allowable processing time T of the post-addition circuit 602.
Since b is relatively long, it is advantageous to reduce the number of bits processed by the pre-stage addition circuit 601 from Nb;
This is a device that eliminates the need to use high-speed devices.
ここで、前段と後段のそれぞれの処理時間La。Here, each processing time La of the first stage and the second stage.
tbと処理許容時間Ta、Tbとの比をとり、それぞれ
を前段処理適性指数ka、後段処理適性指数kbと置く
と、
となる。If we take the ratio of tb to the allowable processing times Ta and Tb and set them as the front-stage processing suitability index ka and the second-stage processing suitability index kb, the following is obtained.
第2図に、後段の処理時間tbをパラメータとしたとき
の、前段の処理ビット数Nbと上記(1)式の関係の−
の1を示す、前段の処理ビット数Nbを増加させると、
(11式からも推測できるように、前段処理適性指数k
aは直線的に上り、後段処理適性指数kbは逆に指数関
数的に低下している。この第2図において、前段処理適
性指数ka、kbは共に1以下で且つ1に近いことが好
ましい。FIG. 2 shows the relationship between the number of processing bits Nb in the first stage and the equation (1) above, when the processing time tb in the second stage is taken as a parameter.
When the number of processing bits Nb of the previous stage is increased, which indicates 1,
(As can be inferred from equation 11, the pre-processing suitability index k
a increases linearly, and the post-processing suitability index kb decreases exponentially. In FIG. 2, it is preferable that the pre-processing suitability indices ka and kb are both 1 or less and close to 1.
l憂段処理適性指数kbついては、前段の処理と・y
h数Nbを少なく、例えばA/D変換器61の処理ビッ
ト数に等しい8ビットにとった場合、処理時間がtb=
30ns程度の高速の回路素子を用いたときでも、後段
の処理適性指数kbが1以内に納まらなくなり、後段の
処理に余裕がなくなって来るので、より高速の回路素子
を用いる必要が出てくる。逆に、前段の処理ビット数N
bを32ビットと多くすると、使用する素子の速度に対
する要求は緩くなるが、前段の処理適性指数kaが1を
越えてしまい、前段の処理に余裕がなくなる。Regarding the processing aptitude index kb, the previous processing and y
If the h number Nb is set to a small number, for example 8 bits, which is equal to the number of processing bits of the A/D converter 61, the processing time is tb=
Even when a high-speed circuit element of about 30 ns is used, the processing suitability index kb of the subsequent stage is no longer within 1, and there is no margin for processing in the subsequent stage, so it becomes necessary to use a higher-speed circuit element. Conversely, the number of processing bits in the previous stage N
If b is increased to 32 bits, the requirements for the speed of the elements used will be relaxed, but the processing suitability index ka of the preceding stage will exceed 1, and there will be no margin for processing of the preceding stage.
要するに、この第2図から次のことが結論される。In short, the following can be concluded from this Figure 2.
(1)前段加算回路601の処理ビット数Nbを、A/
D変換器61の処理ビット数(8ビット)と後段の処理
ビット数(32ビット)の間にとれば、処理適性指数k
a、kbは共に、30n s処理素子を32ビット使用
した場合の処理時間に相当する値(図中本印ンより小さ
くなる。(1) The number of processing bits Nb of the pre-stage addition circuit 601 is set to A/
If it is taken between the number of processing bits of the D converter 61 (8 bits) and the number of processing bits of the subsequent stage (32 bits), the processing suitability index k
Both a and kb are values corresponding to the processing time when a 30 ns processing element is used with 32 bits (smaller than the actual mark in the figure).
(2)前段加算回路601の処理適性指数kaは、その
処理ビット数Nbを小さくする程小さくなり、逆に、後
段加算回路602の処理適性指数kbは、前段処理ビッ
ト数Nbを大きくする程小さくなる。(2) The processing suitability index ka of the front-stage addition circuit 601 becomes smaller as the number of processing bits Nb thereof becomes smaller, and conversely, the processing suitability index kb of the second-stage addition circuit 602 becomes smaller as the number of processing bits Nb becomes larger. Become.
しかし、後段処理適性指数kbは前段処理ビット数Nb
に対して指数関数的に減少するので、NbをA/D変換
器61の処理ビット数より若干大きくするだけで、その
効果は大きい。However, the post-processing suitability index kb is the number of pre-processing bits Nb
Since the number of bits decreases exponentially with respect to the number of bits processed by the A/D converter 61, the effect is large even if Nb is made slightly larger than the number of bits processed by the A/D converter 61.
例えば、前段加算回路601の処理ビット数Nbを16
ビットとすると、その処理適性指数ka=0.8となっ
て1以内に収まり、かつ、処理時間taは?6nsと目
標としたサンプリング時間間隔Ts=20nsより短く
できる。For example, the number of processing bits Nb of the pre-stage addition circuit 601 is set to 16
If it is a bit, then its processing suitability index ka=0.8, which is within 1, and what is the processing time ta? 6 ns, which can be shorter than the targeted sampling time interval Ts=20 ns.
また、後段処理適性指数kbを前段処理適性指数kaと
同一値に設定すると、後段処理時間はしb =4gs
(16nsX2’ )となり、後段加算回路の32ビッ
ト処理素子としては十分低速なもので対応できる。Furthermore, if the post-processing aptitude index kb is set to the same value as the pre-processing aptitude index ka, the post-processing time is b = 4gs.
(16nsX2'), which can be handled by a sufficiently slow 32-bit processing element of the post-addition circuit.
第3図は別の実施例であり、上記の加算回路600を、
ラッチ回F1465と、4組の加算器62とメモリ63
で楕成し、各組の処理時間をサンプリング時間Tsの4
倍で対応できるようにしたものである。FIG. 3 shows another embodiment, in which the above adder circuit 600 is
Latch circuit F1465, four sets of adders 62 and memory 63
The processing time for each set is set to 4 of the sampling time Ts.
It is designed so that it can be handled twice as much.
A/D変換器61は入力情報をサンプリング時間間隔T
sごとに出力し、その結果をラッチ回路65に入力し、
このラッチ回路65の出力を各加算器62が4 X ’
f’ sの時間内で加算するものである。逆にいえば、
同一機能の回路素子を用いると、サンプリング時間間隔
Tsを1/4に短くできる。The A/D converter 61 samples input information at a sampling time interval T.
output every s, input the result to the latch circuit 65,
Each adder 62 receives the output of this latch circuit 65 by 4
The addition is performed within the time f's. Conversely,
By using circuit elements with the same function, the sampling time interval Ts can be shortened to 1/4.
本実施例は加算器62を4組使用しているが、この組数
は任意に選定できるものである。Although this embodiment uses four sets of adders 62, the number of sets can be arbitrarily selected.
第4図は第1図の技術と第3図の技術を組合わせたらめ
であり、前段加算回路601を並列前X器形とすること
により、加算回路600の処理時間を大幅に短くできる
ものである。FIG. 4 is a combination of the technology in FIG. 1 and the technology in FIG. 3, and by making the front-stage adder circuit 601 a parallel front-X type, the processing time of the adder circuit 600 can be significantly shortened. be.
第5図は、同一機能の回路素子を用い、本発明の回路構
成で実測した実行可能な最小サンプリング時間間隔を示
したものであり、いずれも、従来例より、短いサンプリ
ング時間に対応できることが分る。Figure 5 shows the minimum practicable sampling time interval actually measured with the circuit configuration of the present invention using circuit elements with the same function, and it is clear that both can support shorter sampling times than the conventional example. Ru.
上記実施例はいづれも加!回路に対する配慮であったが
、A/D変換器についてもこれを°並列加算器形として
同様に構成することにより、同様な効果が得られること
は言うまでもない。All of the above examples are included! Although consideration was given to the circuit, it goes without saying that similar effects can be obtained by similarly configuring the A/D converter as a parallel adder type.
[発明の効果]
本発明によれば、以下の顕著な効果を奏することができ
る。[Effects of the Invention] According to the present invention, the following remarkable effects can be achieved.
(1)従来と同機な機能の回路構成素子を用いても、処
理ビット数が高く、かつ、サンプリング時間が短い平均
化処理装置を実現できる。(1) It is possible to realize an averaging processing device with a high number of processing bits and a short sampling time even if circuit components having the same functions as those of conventional devices are used.
(2)処理ビット数を高くできるため、平均化処理回数
を多くでき、ノイズの影響を除去できる。その結果、温
度精度の高い光ファイバ式分布形温度センサを実現でき
る。(2) Since the number of processing bits can be increased, the number of times of averaging processing can be increased, and the influence of noise can be removed. As a result, an optical fiber type distributed temperature sensor with high temperature accuracy can be realized.
(3)サンプリング時間を短くできるため、距離分解能
の高い光ファイバ式分布形温度センサを実現できる。(3) Since the sampling time can be shortened, an optical fiber type distributed temperature sensor with high distance resolution can be realized.
(4)回路構成素子として、新規なものを開発する必要
がないため、高性能な装置を安価に実現できる。(4) Since there is no need to develop new circuit components, a high-performance device can be realized at low cost.
第1図は本発明による光ファイバ式分布形温度センサの
平均化処理回路の実施例を示す構成図、第2図はその前
段加算回路の処理ビット数と処理適性指数との関係を示
す図、第3図、第4図はそれぞれ平均化処理回路の他の
実施例を示す構成図、第5図は本発明の性能を従来型と
比較した説明図、第6図は処理ビット数と処理時間との
関係を示す図、第7図は従来の光ファイバ式分布形温度
センサの計測概念を示す図、第8図は従来考えられてい
た光ファイバ式分布形温度センサの構成図、第9図はそ
の平均化処理回路の構成図である。
図中、1はトリガ同局、2はパルス光源、4s、4aは
光学フィルタ、5s、5aは受光器、6s、6aは平均
化処理回路、7は温度分布演算回路、10はfl測装置
、20はセンサ用光ファイバ、2t、22.23a、2
3sは光ファイバ、30sはストーク光用0TDR計測
回路、30aはアンチストークス光用0TDR計測回路
、31.32は光分岐器、61はA/D変換回路、62
.62a、62bは加算器、63.63a、63bはメ
モリ、64は同期回路、65はラッチ回路、600は加
x回路、601は前段加算回路、602は後段加算回路
を示す。
64:同期回路
600:加算回路
601:前段加算回路
第3図
第2図
601(16ビット)
第4図
第5図
処理ビット数Nb
□時間音
(a)入射パルス光
□時間音
(b)センサからの反射光FIG. 1 is a block diagram showing an embodiment of the averaging processing circuit of the optical fiber type distributed temperature sensor according to the present invention, and FIG. 2 is a diagram showing the relationship between the number of processing bits and the processing suitability index of the pre-stage addition circuit. Figures 3 and 4 are block diagrams showing other embodiments of the averaging processing circuit, Figure 5 is an explanatory diagram comparing the performance of the present invention with the conventional type, and Figure 6 is the number of processing bits and processing time. Figure 7 is a diagram showing the measurement concept of a conventional optical fiber type distributed temperature sensor, Figure 8 is a configuration diagram of a conventionally considered optical fiber type distributed temperature sensor, Figure 9 is a configuration diagram of the averaging processing circuit. In the figure, 1 is a trigger station, 2 is a pulse light source, 4s, 4a are optical filters, 5s, 5a are light receivers, 6s, 6a are averaging processing circuits, 7 is a temperature distribution calculation circuit, 10 is a fl measuring device, 20 Optical fiber for sensor, 2t, 22.23a, 2
3s is an optical fiber, 30s is an 0TDR measurement circuit for Stokes light, 30a is an 0TDR measurement circuit for anti-Stokes light, 31.32 is an optical splitter, 61 is an A/D conversion circuit, 62
.. 62a and 62b are adders, 63.63a and 63b are memories, 64 is a synchronization circuit, 65 is a latch circuit, 600 is an addition circuit, 601 is a front-stage addition circuit, and 602 is a rear-stage addition circuit. 64: Synchronous circuit 600: Addition circuit 601: Pre-stage addition circuit Fig. 3 Fig. 2 601 (16 bits) Fig. 4 Fig. 5 Processing bit number Nb □ Time sound (a) Incident pulse light □ Time sound (b) Sensor reflected light from
Claims (1)
を入射させ、該ファイバで発生する後方散乱光で形成さ
れる反射光を計測系に導き、これら反射光の光強度を平
均化処理装置によりサンプリングして平均化し、そのデ
ータから光ファイバの温度を求め、光パルスの入射光時
刻と反射光が計測系へ到達する時刻の差から後方散乱光
の発生位置を求めることにより、温度と位置を同時計測
し、該光ファイバの温度分布を計測する光ファイバ式分
布形温度センサにおいて、前記平均化処理装置をA/D
変換器、前段加算回路及び後段加算回路を直列に接続し
て構成し、前段加算回路の処理ビット数をA/D変換器
の出力ビット数より大きく、かつ、後段加算回路の処理
ビット数より少なくしたことを特徴とする光ファイバ式
分布形温度センサ。 2、前記平均化処理装置に代えて、A/D変換器とその
出力を並列処理する複数組の加算回路とで構成され、各
組の加算回路の処理時間をサンプリング時間間隔の前記
組数倍の時間内とした平均化処理装置を備えたことを特
徴とする請求項1記載の光ファイバ式分布形温度センサ
。 3、前記平均化処理装置に代えて、A/D変換器と、複
数回路で並列処理する前段加算回路と及び後段加算回路
とで構成した平均化処理装置を備えたことを特徴とする
請求項1記載の光ファイバ式分布形温度センサ。[Claims] 1. A light pulse is input from a light source in the measurement system to a sensor optical fiber, and reflected light formed by backscattered light generated in the fiber is guided to the measurement system, and the light of these reflected lights is The intensity is sampled and averaged by an averaging processing device, the temperature of the optical fiber is determined from this data, and the generation position of backscattered light is determined from the difference between the incident light time of the optical pulse and the time at which the reflected light reaches the measurement system. Accordingly, in an optical fiber type distributed temperature sensor that simultaneously measures temperature and position and measures the temperature distribution of the optical fiber, the averaging processing device can be used as an A/D.
A converter, a pre-addition circuit, and a post-addition circuit are connected in series, and the number of processing bits of the pre-addition circuit is larger than the number of output bits of the A/D converter and smaller than the number of processing bits of the post-addition circuit. This is an optical fiber type distributed temperature sensor. 2. Instead of the averaging processing device, it is composed of an A/D converter and a plurality of sets of addition circuits that process the output thereof in parallel, and the processing time of each set of addition circuits is multiplied by the number of sets of the sampling time interval. 2. The optical fiber type distributed temperature sensor according to claim 1, further comprising an averaging processing device for averaging within a time period of . 3. In place of the averaging processing device, an averaging processing device comprising an A/D converter, a pre-addition circuit and a post-addition circuit that perform parallel processing using a plurality of circuits is provided. 1. The optical fiber type distributed temperature sensor according to 1.
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP1019994A JPH0715413B2 (en) | 1989-01-30 | 1989-01-30 | Optical fiber distributed temperature sensor |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP1019994A JPH0715413B2 (en) | 1989-01-30 | 1989-01-30 | Optical fiber distributed temperature sensor |
Related Child Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP8019051A Division JP2939173B2 (en) | 1996-02-05 | 1996-02-05 | Optical fiber distributed temperature sensor |
Publications (2)
| Publication Number | Publication Date |
|---|---|
| JPH02201132A true JPH02201132A (en) | 1990-08-09 |
| JPH0715413B2 JPH0715413B2 (en) | 1995-02-22 |
Family
ID=12014716
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP1019994A Expired - Lifetime JPH0715413B2 (en) | 1989-01-30 | 1989-01-30 | Optical fiber distributed temperature sensor |
Country Status (1)
| Country | Link |
|---|---|
| JP (1) | JPH0715413B2 (en) |
Cited By (1)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| US7162598B2 (en) | 1998-08-20 | 2007-01-09 | Hitachi, Ltd. | Storage system |
Citations (2)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| JPS61270632A (en) * | 1985-05-25 | 1986-11-29 | Hitachi Cable Ltd | Optical fiber type measuring instrument for temperature distribution |
| JPS63157285A (en) * | 1986-12-22 | 1988-06-30 | Advantest Corp | Repeating data collector |
-
1989
- 1989-01-30 JP JP1019994A patent/JPH0715413B2/en not_active Expired - Lifetime
Patent Citations (2)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| JPS61270632A (en) * | 1985-05-25 | 1986-11-29 | Hitachi Cable Ltd | Optical fiber type measuring instrument for temperature distribution |
| JPS63157285A (en) * | 1986-12-22 | 1988-06-30 | Advantest Corp | Repeating data collector |
Cited By (1)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| US7162598B2 (en) | 1998-08-20 | 2007-01-09 | Hitachi, Ltd. | Storage system |
Also Published As
| Publication number | Publication date |
|---|---|
| JPH0715413B2 (en) | 1995-02-22 |
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