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JPS60203821A - Optical fiber vibrator - Google Patents

Optical fiber vibrator

Info

Publication number
JPS60203821A
JPS60203821A JP6201484A JP6201484A JPS60203821A JP S60203821 A JPS60203821 A JP S60203821A JP 6201484 A JP6201484 A JP 6201484A JP 6201484 A JP6201484 A JP 6201484A JP S60203821 A JPS60203821 A JP S60203821A
Authority
JP
Japan
Prior art keywords
optical fiber
light
amplitude
vibration
signal
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
JP6201484A
Other languages
Japanese (ja)
Inventor
Tomoji Sato
佐藤 東史
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
Original Assignee
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 Hitachi Cable Ltd filed Critical Hitachi Cable Ltd
Priority to JP6201484A priority Critical patent/JPS60203821A/en
Publication of JPS60203821A publication Critical patent/JPS60203821A/en
Pending legal-status Critical Current

Links

Classifications

    • GPHYSICS
    • G01MEASURING; TESTING
    • G01HMEASUREMENT OF MECHANICAL VIBRATIONS OR ULTRASONIC, SONIC OR INFRASONIC WAVES
    • G01H9/00Measuring mechanical vibrations or ultrasonic, sonic or infrasonic waves by using radiation-sensitive means, e.g. optical means
    • G01H9/004Measuring mechanical vibrations or ultrasonic, sonic or infrasonic waves by using radiation-sensitive means, e.g. optical means using fibre optic sensors

Landscapes

  • Physics & Mathematics (AREA)
  • General Physics & Mathematics (AREA)
  • Measurement Of Mechanical Vibrations Or Ultrasonic Waves (AREA)

Abstract

PURPOSE:To measure vibration only based upon a multimode optical fiber by making coherent light modulated at its amplitude incident upon the multimode optical fiber and detecting the projected light through a specific filtering means. CONSTITUTION:Light modulated in amplitude by a signal from a tracking generator 9 and emitted from a semiconductor light emitting diode 8 is made incident upon the multimode optical fiber 10 to be a vibration sensor, the projected light is received by a photodetector 12 through the mode filtering means 11 and the oscillation frequency is found out from the electric signal by a spectrum analyzer 1. The means 11 increases the variation of the amplitude of the photodetected signal at the vibration of the fiber 10 by increasing the its insersion loss to measure only the oscillation frequency synchronously with a modulation signal (a) of the generator 9. Thus, the constitution can be simplified.

Description

【発明の詳細な説明】 〔発明の背景と目的〕 本発明は光ファイバ蛋動計に係シ、特に微小な振動でも
篩感度で測定するのに好適な光フアイバ振動計に関する
ものである。
BACKGROUND AND OBJECTS OF THE INVENTION The present invention relates to an optical fiber vibrometer, and particularly to an optical fiber vibrometer suitable for measuring even minute vibrations with sieve sensitivity.

従来の電気を用いた振動計は、センサ部から出力される
信号をメタルケーブルを介して受信するようになってお
シ、センサ部には球が人っていて、その球がどの位移動
したかを検出する構成としである。しかし、上記したよ
うに、センサ部はメカニカルな機構を用いであるので、
振動数によって球の動く振幅が異なり、例えば、周波数
が大きくなると、球が応答できなくなり、球が動く距離
、つまり振幅が小さくなる。したがって、正確な振幅を
めるKは、使用前に周波数と振幅との関係を較正してお
く必要がある。しかしながら、被測定物の振動数が未知
の場合あるいは複数の振動数が1資してランダムな振動
数となっている場合は、正確な較正を行うことができな
い。また、センサ部は設置場所の振動数しか検知できな
いので、例えば、ケーブルの振動を調べるときのように
、被測定物のどの部分が振動するかわからない場合は、
センサ部を多数取りつけなければならないという不便が
ある。また、メタルケーブルを介して信号を受けている
ので、電磁誘導によるノイズが発生しやすく、高精度の
測定が困難であるという欠点もある。− ところで、これに対して第1図に示すような測定系で構
成された光を用いた振動計がある。これは、光源1から
の光を偏光板2を用いて直線偏光とし、その光を偏光ビ
ームスプリッタ6に入れ、P偏光とS偏光とに分岐し、
1方の偏光は振動センサとしての偏波面保存光ファイバ
4に入射し、他方の偏光は参照用偏波面保存光ファイバ
5に入射し、この2本の偏波面保存光ファイバ4,5か
らの出射光を干渉させ、その光をピンホール6を介して
受光器7に入射させて光の強弱を検出し、振動量を測定
するようにしである。
Conventional vibration meters that use electricity receive signals output from a sensor section via a metal cable. This is a configuration that detects whether However, as mentioned above, the sensor part uses a mechanical mechanism, so
The amplitude of the ball's movement varies depending on the frequency; for example, as the frequency increases, the ball becomes unable to respond, and the distance the ball moves, that is, the amplitude, decreases. Therefore, it is necessary to calibrate the relationship between frequency and amplitude before using K, which measures accurate amplitude. However, when the frequency of the object to be measured is unknown or when a plurality of frequencies contribute to a random frequency, accurate calibration cannot be performed. In addition, the sensor unit can only detect the vibration frequency at the installation location, so if you do not know which part of the object to be measured is vibrating, such as when investigating the vibration of a cable,
There is an inconvenience that a large number of sensor sections must be attached. Furthermore, since signals are received via metal cables, noise due to electromagnetic induction is likely to occur, making it difficult to perform highly accurate measurements. - By the way, on the other hand, there is a vibration meter that uses light and is configured with a measurement system as shown in FIG. This converts light from a light source 1 into linearly polarized light using a polarizing plate 2, enters the polarizing beam splitter 6, and splits the light into P-polarized light and S-polarized light.
One polarized light enters a polarization-maintaining optical fiber 4 as a vibration sensor, the other polarized light enters a reference polarization-maintaining optical fiber 5, and the output from these two polarization-maintaining optical fibers 4 and 5. The emitted light is interfered with, and the light is made to enter the light receiver 7 through the pinhole 6 to detect the intensity of the light and measure the amount of vibration.

しかし、第1図に示す従来の測定系では、2本ノ光ファ
イバ4.5を用いているので、光学系を数多く必要とし
、コスト而で問題がある。
However, since the conventional measurement system shown in FIG. 1 uses two optical fibers 4.5, it requires a large number of optical systems, which poses a problem in terms of cost.

本発明は上記に鑑みてなされたもので、その目的とする
ところは、振動センサとしてのマルチモード光ファイバ
のみを用いて振動を測定することができ、しかも、微小
な振動で)も、高感度で測定することができる光フアイ
バ振動計を提供することにある。
The present invention has been made in view of the above, and its purpose is to be able to measure vibrations using only a multimode optical fiber as a vibration sensor, and to be able to measure vibrations (with very small vibrations) with high sensitivity. The purpose of the present invention is to provide a fiber optic vibrometer that can measure

〔発明の概要〕[Summary of the invention]

本発明の特徴は、コヒーレントな光を振幅変調して出射
する光源と、この光源からの光を入射する振動センサと
してのマルチモード光ファイバと、この光ファイバから
出射した光を電気値に変換する受光器と、この受光器と
上記光ファイバの出射端との間に設けた上記光ファイバ
が振動したときに上記受光器に受信される光信号の振幅
の変動を大きくするモードフィルタリング機構と、上記
受光器の出力を人力して振動数をめるスペクトルアナラ
イザとよりなる構成とした点にある。
The features of the present invention include a light source that outputs amplitude-modulated coherent light, a multimode optical fiber as a vibration sensor that receives the light from this light source, and a system that converts the light emitted from this optical fiber into an electrical value. a mode filtering mechanism that increases fluctuations in the amplitude of an optical signal received by the light receiver when the optical fiber provided between the light receiver and the output end of the optical fiber vibrates; The structure consists of a spectrum analyzer that manually calculates the frequency of the output of the light receiver.

〔実施例〕〔Example〕

以下本発明を第2図に示した実施例および第6図、第4
図を用いて詳細に説明する。
The embodiment of the present invention shown in FIG. 2 and FIGS. 6 and 4 will be described below.
This will be explained in detail using figures.

第2図は本発明の光フアイバ振動計の一実施例を示す構
成説明図である。第2図において、8はコヒーレントな
光を送出する半導体発光ダイオードからなる光源で、光
源8からの光は、トラッキングジェネレータ9からの電
気信号によって振幅変調される。光源8からのコヒーレ
ントな振幅変調された光を振動センサとしてのマルチモ
ード光ファイバ10に入射し、マルチモード光ファイバ
10からの光信号は、モードフィルタリング機構11を
介して受光器12で受信し、電気信号に変換する。この
電気信号はスペクトルアナライザ13に人力し、ここで
振動数をめる。
FIG. 2 is a configuration explanatory diagram showing an embodiment of the optical fiber vibrometer of the present invention. In FIG. 2, reference numeral 8 denotes a light source composed of a semiconductor light emitting diode that emits coherent light, and the light from the light source 8 is amplitude-modulated by an electrical signal from a tracking generator 9. Coherent amplitude-modulated light from a light source 8 is incident on a multimode optical fiber 10 serving as a vibration sensor, and an optical signal from the multimode optical fiber 10 is received by a light receiver 12 via a mode filtering mechanism 11. Convert to electrical signal. This electrical signal is manually input to the spectrum analyzer 13, where the frequency is measured.

モードフィルタリング機構11は測定の感度を上げるた
めに設けたもので、第6図はモードフィルタリング機構
の効果を示す線図で、振動数、振幅一定の場合を示しで
ある。横軸はモードフィルタ挿入損失、縦軸はそのとき
の電気信号の振幅の大きさであり、これよシ、モードフ
ィルタ挿入損失を大きくすれば、光パワーの変化量が大
きくなり、電気信号の振幅も大きくなることがわかる。
The mode filtering mechanism 11 is provided to increase the sensitivity of measurement, and FIG. 6 is a diagram showing the effect of the mode filtering mechanism, and shows the case where the frequency and amplitude are constant. The horizontal axis is the insertion loss of the mode filter, and the vertical axis is the amplitude of the electrical signal at that time.Increasing the insertion loss of the mode filter increases the amount of change in optical power, which increases the amplitude of the electrical signal. You can see that it also gets bigger.

これより、モードフィルタリング機構11.を設けるこ
とにより測定感度を上げることができることが理解でき
る。
From this, the mode filtering mechanism 11. It can be understood that measurement sensitivity can be increased by providing .

なお、コヒーレントな光がマルチモード光ファイバ10
に入射すると、モード間の伝搬定数の違いによシ光が干
渉し、光ファイバ10の断面を見ると、第4図に示すよ
うに、スペックルと呼ばれる光の強弱が発生する。第4
図において、14はクラッド、15はコア、16はスペ
ックルであり、このスペックル15は、光ファイバ10
が振動すると光ファイバ10のコア15内で動く。した
がって、マルチモード光ファイバ10からの出射光が受
光器12に入る前にモードフィルタリング機構11を透
過させる。この場合、モードフィルタリング機構11は
、光ファイバ10に軸づれを与える。軸づれを与えれば
、マルチモード光ファイバ10が振動することによシ、
スペックル16の動きが生じ、軸づれ部の結合効率が変
化し、受光器12には変調光信号のほかに振動の周波数
と同一の光の強弱信号が受信される。そのため、受光器
12からの眠気信号をスペクトルアナライザ16に人力
して変調信号αと同期をとれば、振動数のみが測定でき
る。ここで、実際の測定例を第5図に示す。第5図Ca
)は本発明の振動計の場合で。
Note that coherent light is transmitted through a multimode optical fiber 10.
When the light enters the optical fiber, the light interferes due to the difference in the propagation constant between the modes, and when looking at the cross section of the optical fiber 10, as shown in FIG. 4, the intensity of light called speckle occurs. Fourth
In the figure, 14 is a cladding, 15 is a core, and 16 is a speckle, and this speckle 15 is a part of the optical fiber 10.
When it vibrates, it moves within the core 15 of the optical fiber 10. Therefore, the light emitted from the multimode optical fiber 10 is transmitted through the mode filtering mechanism 11 before entering the light receiver 12. In this case, the mode filtering mechanism 11 imparts an axial shift to the optical fiber 10. When the axis misalignment is applied, the multimode optical fiber 10 vibrates, causing
As the speckle 16 moves, the coupling efficiency of the off-axis portion changes, and the light receiver 12 receives a light intensity signal having the same frequency as the vibration, in addition to the modulated optical signal. Therefore, if the drowsiness signal from the light receiver 12 is manually input to the spectrum analyzer 16 and synchronized with the modulation signal α, only the frequency can be measured. Here, an actual measurement example is shown in FIG. Figure 5 Ca
) is for the vibration meter of the present invention.

同図(6)は比較のために示した従来の振動計の場合で
ある。第5図に示すように、振動が生じていれば、光パ
ワーが変化し、受光器12からの電気信号も振動数と同
じ周波数で同様に変化する。
Figure (6) shows the case of a conventional vibration meter shown for comparison. As shown in FIG. 5, if vibration occurs, the optical power changes, and the electrical signal from the light receiver 12 also changes at the same frequency as the vibration frequency.

上記した本発明の実施例によれば、被測定振動数が異な
っても同一の振幅の信号を得ることができ、また、振動
数が不明であっても振幅の較正が可能である。しかも、
振動センサとしてのマルチモード光ファイバ10しか用
いていないので、構成が比較的簡単になる。そして、微
小振動でもモードフィルタリング機構11の損失を上げ
ることによって感度よく測定することができる。
According to the embodiment of the present invention described above, a signal with the same amplitude can be obtained even if the measured vibration frequency is different, and even if the vibration frequency is unknown, the amplitude can be calibrated. Moreover,
Since only the multimode optical fiber 10 is used as the vibration sensor, the configuration is relatively simple. Even minute vibrations can be measured with high sensitivity by increasing the loss of the mode filtering mechanism 11.

なお、変調信号は直流でもよい。しかし、この場合は、
スペクトルアナライザの代りにオシロスコープを用いる
Note that the modulation signal may be a direct current. However, in this case,
Use an oscilloscope instead of a spectrum analyzer.

〔発明の効果〕〔Effect of the invention〕

以上説明したように、本発明によれば、振動セ/すとし
てのマルチモード光ファイバのみを用いて振動を測定す
ることができ、しかも、微小な振動でも高感度で測定す
ることができ、かつ、装置の構成が簡単になるという効
果がある。
As explained above, according to the present invention, vibrations can be measured using only a multimode optical fiber as a vibration sensor, and even minute vibrations can be measured with high sensitivity. This has the effect of simplifying the configuration of the device.

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

第1図は従来の光フアイバ振動計の構成説明図。 第2図は本発明の光フアイバ振動計の一実施例を示す構
成説明図、第3図は第1図のモードフィルタリング機構
の効果を説明するための線図、第4図は第2図のマルチ
モード光ファイバ端面のスペックルパターンを示す図、
第5図は本発明の光フアイバ振動計による測定例を示す
図である。 8;光源、9;トラッキングジェネレータ。 10;マルチモード光ファイバ、 11;モードフィルタリング機構、 12;受光器、16;スペクトルアナライザ。
FIG. 1 is an explanatory diagram of the configuration of a conventional optical fiber vibrometer. Fig. 2 is a configuration explanatory diagram showing one embodiment of the optical fiber vibrometer of the present invention, Fig. 3 is a diagram for explaining the effect of the mode filtering mechanism shown in Fig. 1, and Fig. 4 is a diagram showing the effect of the mode filtering mechanism of Fig. 2. A diagram showing a speckle pattern on the end face of a multimode optical fiber,
FIG. 5 is a diagram showing an example of measurement using the optical fiber vibrometer of the present invention. 8; light source; 9; tracking generator. 10; Multimode optical fiber; 11; Mode filtering mechanism; 12; Photoreceiver; 16; Spectrum analyzer.

Claims (1)

【特許請求の範囲】[Claims] (1) コヒーレントな光を振幅変調して出射する光源
と、該光源からの光を入射する振動セ/すとしてのマル
チモード光ファイバと、該光ファイバから出射した光を
電気1ぼに変換する受光器と、該受光器と前記光ファイ
バの出射端との間に設けた前記光ファイバが振動したと
きに前記受光器に受信される光信号の振幅の変動を大き
くするモードフィルタリング機構と、前記受光器の出力
を人力して振動数をめスペクトルアナライザとよりなる
ことを特徴とする光フアイバ振動計。
(1) A light source that outputs amplitude-modulated coherent light, a multimode optical fiber as a vibration cell into which the light from the light source enters, and converts the light emitted from the optical fiber into electricity. a mode filtering mechanism that increases fluctuations in the amplitude of an optical signal received by the light receiver when the optical fiber provided between the light receiver and the output end of the optical fiber vibrates; An optical fiber vibrometer characterized by comprising a spectrum analyzer and a spectrum analyzer that measures the frequency by manually inputting the output of a light receiver.
JP6201484A 1984-03-28 1984-03-28 Optical fiber vibrator Pending JPS60203821A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP6201484A JPS60203821A (en) 1984-03-28 1984-03-28 Optical fiber vibrator

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP6201484A JPS60203821A (en) 1984-03-28 1984-03-28 Optical fiber vibrator

Publications (1)

Publication Number Publication Date
JPS60203821A true JPS60203821A (en) 1985-10-15

Family

ID=13187876

Family Applications (1)

Application Number Title Priority Date Filing Date
JP6201484A Pending JPS60203821A (en) 1984-03-28 1984-03-28 Optical fiber vibrator

Country Status (1)

Country Link
JP (1) JPS60203821A (en)

Cited By (3)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
WO1993003400A1 (en) * 1991-08-02 1993-02-18 The Furukawa Electric Co., Ltd. Method of probing optical transmission line
JP2008309497A (en) * 2007-06-12 2008-12-25 Oputeikon:Kk Fiber optic sensor
CN111021732A (en) * 2019-12-18 2020-04-17 中交第三航务工程局有限公司南京分公司 Concrete vibrating rod positioning method based on optical fiber sensing

Cited By (4)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
WO1993003400A1 (en) * 1991-08-02 1993-02-18 The Furukawa Electric Co., Ltd. Method of probing optical transmission line
US5457998A (en) * 1991-08-02 1995-10-17 The Furukawa Electric Co., Ltd. Method of detecting an optical transmission line
JP2008309497A (en) * 2007-06-12 2008-12-25 Oputeikon:Kk Fiber optic sensor
CN111021732A (en) * 2019-12-18 2020-04-17 中交第三航务工程局有限公司南京分公司 Concrete vibrating rod positioning method based on optical fiber sensing

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