JPH03285129A - Processing method for receiving signal of optical fiber back-scattered light - Google Patents

Processing method for receiving signal of optical fiber back-scattered light

Info

Publication number
JPH03285129A
JPH03285129A JP2086411A JP8641190A JPH03285129A JP H03285129 A JPH03285129 A JP H03285129A JP 2086411 A JP2086411 A JP 2086411A JP 8641190 A JP8641190 A JP 8641190A JP H03285129 A JPH03285129 A JP H03285129A
Authority
JP
Japan
Prior art keywords
signal
width
pulse
differential
delay
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
JP2086411A
Other languages
Japanese (ja)
Inventor
Yasuo Ozawa
保夫 小沢
Shuichi Fujieda
藤枝 秀一
Akira Tokushima
徳島 彰
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.)
Hitachi Cable Ltd
Tokyo Electric Power Co Holdings Inc
Original Assignee
Tokyo Electric Power Co Inc
Hitachi Cable 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 Tokyo Electric Power Co Inc, Hitachi Cable Ltd filed Critical Tokyo Electric Power Co Inc
Priority to JP2086411A priority Critical patent/JPH03285129A/en
Publication of JPH03285129A publication Critical patent/JPH03285129A/en
Pending legal-status Critical Current

Links

Landscapes

  • Measuring Temperature Or Quantity Of Heat (AREA)
  • Optical Transform (AREA)

Abstract

PURPOSE:To improve the resolving power in a length direction to a large extent by adding the differential signal obtained by applying time differential processing to the temp. distribution signal calculated from the intensity of scattered light to the delay signal obtained by delaying the differential signal by the time equal to the pulse width of incident light. CONSTITUTION:A light receiving circuit is constituted of a differentiation circuit 8, an adder 9 and a delay circuit 10. Back scattering light is converted to an electric signal which is, in turn, subjected to averaging processing to obtain a noise removed input signal and this signal is differentiated timewise by the differentiation circuit to be deformed. Next, the differential signal is added to the signal delayed by the delay circuit 10 generating the delay corresponding to the width (t) of a sent-out light pulse. By adding the differential signal to the delay signal by the adder 9, the distortion of a waveform generated by the width of the sent-out light pulse is removed and the output signal 11 equal to temp. distribution to be calculated is obtained. Therefore, temp. distribution shorter than the width of the sent-out light pulse can be calculated and the resolving power in a length direction can be enhanced.

Description

【発明の詳細な説明】 [産業上の利用分野コ 本発明は、光ファイバ中にて発生するラマン散乱光を利
用した温度計測、特に光ファイバ後方散乱光の受信信号
処理方法に関するものである。
DETAILED DESCRIPTION OF THE INVENTION [Field of Industrial Application] The present invention relates to temperature measurement using Raman scattered light generated in an optical fiber, and particularly to a method for processing received signals of optical fiber backscattered light.

[従来の技術] 第3図は、光パルスの後方散乱光を利用して、温度計測
を行う場合のブロック図である。
[Prior Art] FIG. 3 is a block diagram when temperature measurement is performed using backscattered light of a light pulse.

パルス光源1から出力される光パルス5は、光分波器3
を経由して光ファイバ4へ導かれる。
The optical pulse 5 output from the pulse light source 1 is passed through the optical demultiplexer 3
is guided to the optical fiber 4 via.

方、光ファイバ4の中で発生した後方散乱光は、光分波
器3を経由して光受信口B2で受信・処理される。
On the other hand, the backscattered light generated in the optical fiber 4 is received and processed at the optical receiving port B2 via the optical demultiplexer 3.

第4図(a)は光ファイバの長さ方向の温度分布、第4
図(b)はパルス光源から出力される光パルス、第4図
fc)は得られる後方散乱光パルスを示すもので、パル
ス光源から出力される光パルスの幅tが、後方散乱光パ
ルスの分解能を決定することになり、従来は、得られた
後方散乱光をそのまま温度へ換算していた。
Figure 4(a) shows the temperature distribution in the length direction of the optical fiber.
Figure (b) shows the light pulse output from the pulsed light source, and Figure 4 (fc) shows the backscattered light pulse obtained.The width t of the light pulse output from the pulsed light source is the resolution of the backscattered light pulse. Conventionally, the obtained backscattered light was directly converted into temperature.

[発明が解決しようとする課題] しかし、長さ方向の分解能を上げようとすると、前記光
パルスの幅tをできる限り小さくする必要があるが、こ
の様な用途で必要となる光パルスは、数100mW〜数
Wと高出力であるためパルス幅を小さくするには限度が
ある。
[Problems to be Solved by the Invention] However, in order to increase the resolution in the longitudinal direction, it is necessary to reduce the width t of the optical pulse as much as possible. Since the output is as high as several 100 mW to several W, there is a limit to reducing the pulse width.

本発明の目的は、前記した従来技術の欠点を解消し、長
さ方向の分解能を大幅に改善できる光ファイバ後方散乱
光の受信信号処理方法を提供することにある。
SUMMARY OF THE INVENTION An object of the present invention is to provide a method for processing received signals of optical fiber backscattered light, which eliminates the drawbacks of the prior art described above and can significantly improve the resolution in the longitudinal direction.

[課題を解決するための手段] 本発明の信号処理方法は、光ファイバ中に入射した光パ
ルスによって発生するラマン散乱光を利用して温度計測
を行う装置において、散乱光強度から求めた温度分布信
号に時間微分処理をした微分信号と、該微分信号を入射
光V<ルス幅と等しい時間遅延した遅延信号とを加算す
るものである。
[Means for Solving the Problems] The signal processing method of the present invention is a device that measures temperature using Raman scattered light generated by a light pulse incident on an optical fiber. A differential signal obtained by subjecting the signal to time differential processing and a delayed signal obtained by delaying the differential signal by a time equal to the incident light V<the pulse width are added.

「作用] 電気信号に変換された後、平均化処理等によってノイズ
を除去された入力信号を時間で微分し、この微分信号を
入射光パルス幅と等しい時間遅延した遅延信号と加算す
ると、送出した光パルスの幅によって生じた波形の歪が
除去され、これによって長さ方向の分解能が向上する。
Effect: After being converted into an electrical signal, the input signal from which noise has been removed by averaging processing, etc. is differentiated with respect to time, and this differentiated signal is added to a delayed signal delayed by a time equal to the width of the incident light pulse. Waveform distortion caused by the width of the optical pulse is removed, thereby improving longitudinal resolution.

「実施例コ 以下、本発明を図示の実施例に基づいて説明する。"Example code" Hereinafter, the present invention will be explained based on illustrated embodiments.

従来の第3図と同様に、パルス光源1から出力される光
パルス5は、光分波器3を経由して光ファイバ4へ導か
れる。そして、光ファイバ4の中で発生した後方散乱光
は、光分波器3を経由して光受信回F!@2で受信・処
理される。
Similar to the conventional example shown in FIG. 3, the optical pulse 5 output from the pulsed light source 1 is guided to the optical fiber 4 via the optical demultiplexer 3. The backscattered light generated in the optical fiber 4 then passes through the optical demultiplexer 3 to the optical receiving circuit F! Received and processed by @2.

第1図は、この光受信回路2中における改良した信号処
理回路部分の具体例であり、微分回路8、加算器9、遅
延回路10で構成されている。7は、後方散乱光か電気
信号に変換された後、平均化処理等によってノイズを除
去された入力信号、11は長さ方向に分解能の向上した
出力信号を示す。
FIG. 1 shows a specific example of the improved signal processing circuit section in the optical receiving circuit 2, which is composed of a differentiating circuit 8, an adder 9, and a delay circuit 10. Reference numeral 7 indicates an input signal that has been converted into backscattered light or an electrical signal and has noise removed by averaging processing or the like, and 11 indicates an output signal with improved resolution in the length direction.

第2図の波形図において、(a)は長さ方向の温度分布
、(b)は送出した光パルス波形であり、(C)はこれ
らより得られる後方散乱光の強度をそのまま温度分布に
換算したもの、即ち第1図の入力信号7である。
In the waveform diagram in Figure 2, (a) is the temperature distribution in the length direction, (b) is the transmitted optical pulse waveform, and (C) is the intensity of the backscattered light obtained from these directly converted into temperature distribution. That is, the input signal 7 in FIG.

上記入力信号7(第2図(C))は、微分回路8によっ
て時間で微分され、第2図(d)のように変形される。
The input signal 7 (FIG. 2(C)) is differentiated with respect to time by a differentiating circuit 8 and transformed as shown in FIG. 2(d).

次に、送出した光パルスの幅tに相当する遅延を発生す
る遅延回路10によって遅延された信号(第2図(e)
)と加算される。このように、前記微分信号を加算器9
にて遅延信号〈第2図(e)〉と加算することにより、
送出した光パルスの幅によって生じた波形の歪が除去さ
れ、求める温度分布に等しい出力信号11〈第2図(f
))を得ることかできる。
Next, a signal delayed by a delay circuit 10 that generates a delay corresponding to the width t of the transmitted optical pulse (see FIG. 2(e)
) is added. In this way, the differential signal is sent to the adder 9
By adding the delayed signal <Figure 2 (e)> at
Waveform distortion caused by the width of the transmitted optical pulse is removed, and an output signal 11 equal to the desired temperature distribution (Fig. 2 (f)
)) can be obtained.

従って、送出する光パルスの幅よりも短い温度分布を求
めることができ、長さ方向の分解能を向上させることが
可能となる。
Therefore, it is possible to obtain a temperature distribution that is shorter than the width of the optical pulse to be sent out, and it is possible to improve the resolution in the longitudinal direction.

[発明の効果] 以上述べたように、本発明によれば、送出した光パルス
の幅によって生じた波形の歪か除去され、送出する光パ
ルスの幅よりも短い温度分布を求めることができ、長さ
方向の分解能を向上させることができる。
[Effects of the Invention] As described above, according to the present invention, waveform distortion caused by the width of the transmitted optical pulse can be removed, and a temperature distribution shorter than the width of the transmitted optical pulse can be obtained. The resolution in the length direction can be improved.

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

第1図は本発明の一実施例を示す信号処理回路図、第2
図は第1図の実施例における処理過程を示す波形例を示
す図、第3図は光ファイバ中にて発生するラマン散乱光
を利用した従来の温度計測のブロック図、第4図は従来
の温度計測における長さ方向の温度分布、送出パルス波
形及び後方散乱光強度から算出した温度分布を示す図で
ある。 図中、1はパルス光源、2は受信・処理回路、3は光分
波器、4は光ファイバ、5は送出された光パルス、6は
受信される後方散乱光、7は後方散乱光強度から算出さ
れた信号、8は微分回路、9は加算器、10は遅延回路
、11は長さ方向に分解能向上した信号を示す。
FIG. 1 is a signal processing circuit diagram showing one embodiment of the present invention, and FIG.
The figure shows a waveform example showing the processing process in the embodiment of Figure 1, Figure 3 is a block diagram of a conventional temperature measurement using Raman scattered light generated in an optical fiber, and Figure 4 is a diagram of a conventional temperature measurement. It is a figure which shows the temperature distribution in the length direction in temperature measurement, and the temperature distribution calculated from the sending pulse waveform and the backscattered light intensity. In the figure, 1 is a pulsed light source, 2 is a receiving/processing circuit, 3 is an optical demultiplexer, 4 is an optical fiber, 5 is a transmitted optical pulse, 6 is a received backscattered light, and 7 is a backscattered light intensity 8 is a differential circuit, 9 is an adder, 10 is a delay circuit, and 11 is a signal whose resolution has been improved in the length direction.

Claims (1)

【特許請求の範囲】[Claims] 1、光ファイバ中に入射した光パルスによって発生する
ラマン散乱光を利用して温度計測を行う装置において、
散乱光強度から求めた温度分布信号に時間微分処理をし
た微分信号と、該微分信号を入射光パルス幅と等しい時
間遅延した遅延信号とを加算することを特徴とする光フ
ァイバ後方散乱光の受信信号処理方法。
1. In a device that measures temperature using Raman scattered light generated by a light pulse incident on an optical fiber,
Receiving optical fiber backscattered light, characterized by adding a differential signal obtained by time differential processing to a temperature distribution signal obtained from scattered light intensity, and a delayed signal obtained by delaying the differential signal by a time equal to the incident light pulse width. Signal processing method.
JP2086411A 1990-03-30 1990-03-30 Processing method for receiving signal of optical fiber back-scattered light Pending JPH03285129A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP2086411A JPH03285129A (en) 1990-03-30 1990-03-30 Processing method for receiving signal of optical fiber back-scattered light

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP2086411A JPH03285129A (en) 1990-03-30 1990-03-30 Processing method for receiving signal of optical fiber back-scattered light

Publications (1)

Publication Number Publication Date
JPH03285129A true JPH03285129A (en) 1991-12-16

Family

ID=13886128

Family Applications (1)

Application Number Title Priority Date Filing Date
JP2086411A Pending JPH03285129A (en) 1990-03-30 1990-03-30 Processing method for receiving signal of optical fiber back-scattered light

Country Status (1)

Country Link
JP (1) JPH03285129A (en)

Cited By (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JP2009139265A (en) * 2007-12-07 2009-06-25 Toshiba Corp Detection method of twin pulse
EP2913646A4 (en) * 2012-10-26 2015-10-14 Fujitsu Ltd Temperature measuring system and abnormality detecting method

Cited By (4)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JP2009139265A (en) * 2007-12-07 2009-06-25 Toshiba Corp Detection method of twin pulse
EP2913646A4 (en) * 2012-10-26 2015-10-14 Fujitsu Ltd Temperature measuring system and abnormality detecting method
AU2012393096B2 (en) * 2012-10-26 2016-07-07 Fujitsu Limited Temperature measuring system and abnormality detecting method
US9816878B2 (en) 2012-10-26 2017-11-14 Fujitsu Limited Temperature measurement system and abnormality detection method

Similar Documents

Publication Publication Date Title
EP1209780A3 (en) Method and apparatus for generating a single-sideband optical frequency comb
DE69827662D1 (en) METHOD AND DEVICE FOR DETERMINING THE COMPOSITION OF EXHAUST GAS
CA2659457A1 (en) Raman amplification in distributed optical fiber sensing systems
JPH02118206U (en)
JPH03285129A (en) Processing method for receiving signal of optical fiber back-scattered light
FI982192A (en) Method for measuring vital signs and instrumentation
CA2183347A1 (en) Optical and gate
JP2748891B2 (en) Optical amplifier
CN215177558U (en) Measuring system
US8989576B2 (en) Device and method for processing an optical signal
EP0943925A3 (en) Electro-optic sampling oscilloscope
EP1130814A3 (en) System and method for heterodyne detection of an optical signal
JP2512520B2 (en) Optical repeater
JPH05303125A (en) Light intensity nonlinear filter, optical converter repeater, preamplifier for light signal, and light intensity variation measuring instrument
CN106291581A (en) Ultrafast imaging device based on Optical Time Division Multiplexing and method
JP2005345312A (en) Optical signal waveform measurement/evaluation apparatus by optoelectric sampling
JPH11271028A (en) Measuring apparatus for strain of optical fiber
CN113514149A (en) Optical pulse signal processing system
JP2623782B2 (en) Optical fiber temperature distribution measurement method
JP2752731B2 (en) Ultrashort light pulse generator
JPH09181380A (en) Optical triangular wave generator
JPS61134641A (en) Method for measuring extinction ratio of constant polarization fiber
JPH09211510A (en) Laser amplifier device and its use method as well as actual time photometric instrument and its using method
EP0403094A2 (en) Method of measuring backscattered light, and device for same measuring
JP3135407B2 (en) Optical fiber backscattered light measuring device