JPH0228403Y2 - - Google Patents

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Publication number
JPH0228403Y2
JPH0228403Y2 JP1384580U JP1384580U JPH0228403Y2 JP H0228403 Y2 JPH0228403 Y2 JP H0228403Y2 JP 1384580 U JP1384580 U JP 1384580U JP 1384580 U JP1384580 U JP 1384580U JP H0228403 Y2 JPH0228403 Y2 JP H0228403Y2
Authority
JP
Japan
Prior art keywords
light
intermittent
intermittent light
output
transmission line
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.)
Expired
Application number
JP1384580U
Other languages
Japanese (ja)
Other versions
JPS56116610U (en
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 filed Critical
Priority to JP1384580U priority Critical patent/JPH0228403Y2/ja
Publication of JPS56116610U publication Critical patent/JPS56116610U/ja
Application granted granted Critical
Publication of JPH0228403Y2 publication Critical patent/JPH0228403Y2/ja
Expired legal-status Critical Current

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  • Arrangements For Transmission Of Measured Signals (AREA)
  • Optical Transform (AREA)
  • Length Measuring Devices By Optical Means (AREA)

Description

【考案の詳細な説明】 この考案は光フアイバを用いて機械的な変位量
を光量変化に変換して変位量を測定する装置に関
する。
[Detailed Description of the Invention] This invention relates to a device that measures the amount of displacement by converting the amount of mechanical displacement into a change in the amount of light using an optical fiber.

最近、電線ケーブルに代つて光フアイバが盛ん
に使用されるようになつてきた。光フアイバは電
線ケーブルのように電磁的な影響を受けないた
め、特に通信の分野で広く利用されつつある。し
かしながら、現在では未だ限られた分野でしか利
用されておらず、今後さらに広い分野で使用され
ることが望まれている。
Recently, optical fibers have been increasingly used in place of electric cables. Since optical fibers are not affected by electromagnetic influences like electric cables, they are becoming widely used, especially in the field of communications. However, it is currently only used in a limited number of fields, and it is hoped that it will be used in an even wider range of fields in the future.

この考案は上記の点に鑑みてなされたもので、
光フアイバの構造散乱(コア、クラツドの界面ゆ
らぎなどにより発生する)による伝送損失を利用
して機械的な変位量を測定するようにし、構造簡
単で精度良い変位量測定を可能とした変位量測定
装置を提供することを目的とする。
This idea was made in view of the above points,
Displacement measurement uses transmission loss due to optical fiber structural scattering (occurred due to interfacial fluctuations between the core and cladding) to measure mechanical displacement, making it possible to measure displacement with a simple structure and high accuracy. The purpose is to provide equipment.

以下この考案の一実施例を図面を参照して説明
する。第1図はこの考案による変化量測定装置の
構成を示すもので、この変化量測定装置は大きく
分けて、測定部10、検出部20、これら測定部
10と検出部20とを接続する2本の光フアイバ
31,32とから構成されている。
An embodiment of this invention will be described below with reference to the drawings. FIG. 1 shows the configuration of a change measuring device according to this invention. This change measuring device is roughly divided into a measuring section 10, a detecting section 20, and two wires connecting these measuring section 10 and detecting section 20. It is composed of optical fibers 31 and 32.

上記測定部10は、直流電源11、クロツク発
生器12、このクロツク発生器12からのクロツ
クに同期してパルスを発生するパルス発生器13
a,13b、このパルス発生器13a,13bか
らのパルス出力を受けて断続的に発光動作する投
光器14a,14b、上記光フアイバ31の一端
に取付けられ、上記投光器14aからの光を受け
る受光窓15、上記投光器14bからの光のレベ
ルを調整する調光器16、上記光フアイバ32の
一端に取付けられ、光フアイバ32からの光を出
す投光窓17、この投光窓17に対向配置された
光電変換機能を有する受光器18、この受光器1
8と投光窓17との間に介在され、上記調光器1
6を経て得られる投光器14bからの光を上記受
光器18に供給し得るような角度に配置された半
透鏡HM、上記受光器18からの光に対応した電
気信号を受けて検出部20の測定量として出力す
る測定回路19から構成されている。
The measurement unit 10 includes a DC power supply 11, a clock generator 12, and a pulse generator 13 that generates pulses in synchronization with the clock from the clock generator 12.
a, 13b, light emitters 14a, 14b that intermittently operate to emit light in response to pulse outputs from the pulse generators 13a, 13b, and a light receiving window 15 attached to one end of the optical fiber 31 to receive light from the light emitter 14a. , a dimmer 16 for adjusting the level of light from the light projector 14b, a light projection window 17 attached to one end of the optical fiber 32 to output light from the optical fiber 32, and a light projection window 17 disposed opposite to the light projection window 17. A light receiver 18 having a photoelectric conversion function, this light receiver 1
8 and the light projection window 17, the dimmer 1
A semi-transparent mirror HM is arranged at an angle such that the light from the projector 14b obtained through 6 can be supplied to the light receiver 18, and the detection unit 20 receives an electrical signal corresponding to the light from the light receiver 18 and measures It consists of a measuring circuit 19 that outputs a quantity.

また、検出部20は、被測定量(この実施例で
は流体流量とする)が検出される流体通路21
と、この流体通路21内を横切る如く配置された
検出用光フフアイバ22とで構成されている。上
記検出用光フアイバ22は、流体通路21に支持
部231,232で支持され、その両端がコネクタ
241,242によつて前記光フアイバ31,32
に接続されている。
The detection unit 20 also includes a fluid passage 21 in which a measured quantity (in this embodiment, fluid flow rate) is detected.
and a detection optical fiber 22 disposed so as to traverse the inside of this fluid passage 21. The detection optical fiber 22 is supported in the fluid passage 21 by support parts 23 1 , 23 2 , and both ends of the detection optical fiber 22 are connected to the optical fibers 31 , 32 by connectors 24 1 , 24 2 .
It is connected to the.

次に上記のように構成されたこの考案の動作を
第2図を参照して説明する。投孔器14aからは
第2図aのような断続的な光が発光している。一
方、投光器14bからは第2図cのような断続的
な光が発光している。この第2図a,cから明ら
かなように、発光器14aと14bは、それぞれ
交互に光を出すように制御されている。この制御
タイミングはクロツク発生器12により行なう。
Next, the operation of this device constructed as described above will be explained with reference to FIG. Intermittent light as shown in FIG. 2a is emitted from the hole thrower 14a. On the other hand, the light projector 14b emits intermittent light as shown in FIG. 2c. As is clear from FIGS. 2a and 2c, the light emitters 14a and 14b are controlled to alternately emit light. This control timing is performed by a clock generator 12.

しかして、上記投光器14aからの光は、受光
窓15に入つて光フアイバ31、検出用光フアイ
バ22、光フアイバ32を通つて投光窓17から
第2図bの如く多少減衰された光となつて出てく
る。この投光窓17から出た光は半透鏡HMを通
つて受光器18に入る。また、投光器14bから
の光は調光器16で第2図dの如く、上記投光窓
17から出てくる光(第2図b)と同レベルの光
に調節されたのち、半透鏡HMに照射される。し
たがつて、受光器18に入射される光は、第2図
bと光と第2図dの光が合成された第2図eのよ
うな同一レベルを持つた連続光となる。そして、
この連続光をその光レベルに応じた電気信号に変
換して測定回路19に入力させる。測定回路19
では、このような状態の信号が入力されたとき
を、測定量“0”としてその測定量“0”に対応
する信号を出力する。
Thus, the light from the light projector 14a enters the light receiving window 15, passes through the optical fiber 31, the detection optical fiber 22, and the optical fiber 32, and exits the light projecting window 17 as a somewhat attenuated light as shown in FIG. 2b. It grows old and comes out. The light emitted from the light projection window 17 passes through the semi-transparent mirror HM and enters the light receiver 18. Further, the light from the light projector 14b is adjusted by the dimmer 16 to the same level of light as the light coming out from the light projection window 17 (Fig. 2b), as shown in Fig. 2d, and then the semi-transparent mirror HM is irradiated. Therefore, the light incident on the light receiver 18 becomes continuous light having the same level as shown in FIG. 2e, in which the light in FIG. 2b and the light in FIG. 2d are combined. and,
This continuous light is converted into an electrical signal corresponding to the light level and input to the measuring circuit 19. Measuring circuit 19
Now, when a signal in such a state is input, the measured quantity is determined to be "0", and a signal corresponding to the measured quantity "0" is output.

上記のように、検出部20の流体通路21内に
流体を流す前に、予め投光窓17から発射される
光のレベルと調光器16を介して得られる投光器
14bからの光のレベルを等しくしておき、これ
らを合成した同一レベルの光を受光器18に入射
させ、そのときの受光器18からの信号を基準レ
ベルとして測定回路に設定しておく。
As described above, before flowing fluid into the fluid passage 21 of the detection unit 20, the level of light emitted from the light projection window 17 and the level of light from the light projector 14b obtained via the dimmer 16 are adjusted in advance. The light of the same level obtained by combining these lights is made to enter the light receiver 18, and the signal from the light receiver 18 at that time is set as a reference level in the measurement circuit.

このような状態に設定しておけば、流体通路2
1内を流れる流体の流速の大きさに応じた変化が
測定回路19から取出すことができる。すなわ
ち、流体の流れにより検出用光フアイバ22はそ
の流れの速度に応じた構造散乱が生じ、投光窓1
7からの光レベルが調光器16を介して得られる
投光器14bからの光レベルに対して差を生じ
る。したがつて、受光器18の入力光の波形は投
光窓17からの光レベルと調光器16からの光レ
ベルとの間に差が生じ、その変化分に応じた出力
を測定回路19から取出すことができるものであ
る。したがつて、流体通路21内を流れる流体の
流速の大きさに応じた出力を測定回路19から取
り出すことができる。
If this condition is set, the fluid passage 2
A change depending on the magnitude of the flow velocity of the fluid flowing through the measuring circuit 19 can be obtained from the measuring circuit 19. That is, due to the flow of the fluid, the detection optical fiber 22 undergoes structural scattering in accordance with the speed of the flow, and the light emitting window 1
7 makes a difference to the light level from the projector 14b obtained via the dimmer 16. Therefore, in the waveform of the input light to the light receiver 18, a difference occurs between the light level from the light projection window 17 and the light level from the dimmer 16, and an output corresponding to the difference is output from the measurement circuit 19. It is something that can be taken out. Therefore, it is possible to take out an output from the measurement circuit 19 that corresponds to the magnitude of the flow velocity of the fluid flowing within the fluid passage 21.

また、測定部10で発生する雑音成分は調光器
16から出力される光と投光窓17からの光にほ
ぼ同程度含まれているので、上記二つの光のレベ
ルを等しく調整し、この値を基準レベル(0レベ
ル)と設定することによつて、測定中に受光器1
8の入力光に現われる変化分を雑音成分の少い良
好な測定値とみなすことが可能である。したがつ
て、測定精度(S/N比)を向上できる。
Furthermore, since the noise component generated in the measurement unit 10 is included in the light output from the dimmer 16 and the light output from the light projection window 17 to approximately the same extent, the levels of the two lights are adjusted to be equal. By setting the value as the reference level (0 level), the receiver 1 can be
It is possible to regard the change appearing in the input light of No. 8 as a good measurement value with little noise component. Therefore, measurement accuracy (S/N ratio) can be improved.

なおこの考案による測定部10は第1図に示し
た実施例のような構成でなく、第3図のように構
成しても同様に実施することができる。第3図に
おいて第1図と同一部分には同一符号を付してい
る。この第3図の場合は、1台の投光器14から
の光を半透鏡HM1で分離し、これら分離された
光をクロツク発生器12で開閉制御される第1,
第2の電子シヤツタ40a,40bにより制御し
て、第2図a,cのような光を作り出している。
このような構成としても上記実施例と同じ目的を
達することができる。また、上記実施例では流体
の流速、流量を測定する場合を例にとつて説明し
たが、これに限られるものではなく、広い分野の
測定に適用できるものである。さらにまた、上記
実施例では、検出に用いられる光フアイバを検出
用光フアイバとして別個に設け、伝送の光フアイ
バにコネクタを用いて接続しているが、このよう
な構成でなく、一本の光フアイバの一部を検出用
光フアイバとして用いるようにしても良い。なお
検出用光フアイバ22は光フアイバ31,32よ
り、より構造散乱の大きいフアイバーを用いても
よい。その他この考案は上記実施例に限定される
ことなく要旨を逸脱しない範囲で種々変形して実
施することができるものである。
Note that the measuring section 10 according to this invention can be similarly implemented even if it is configured not like the embodiment shown in FIG. 1 but as shown in FIG. 3. In FIG. 3, the same parts as in FIG. 1 are given the same reference numerals. In the case of this FIG.
It is controlled by second electronic shutters 40a and 40b to produce light as shown in FIGS. 2a and 2c.
Even with such a configuration, the same purpose as the above embodiment can be achieved. Further, in the above embodiment, the case where the flow velocity and flow rate of a fluid is measured has been described as an example, but the present invention is not limited to this and can be applied to measurement in a wide range of fields. Furthermore, in the above embodiment, the optical fiber used for detection is separately provided as a detection optical fiber and connected to the transmission optical fiber using a connector, but instead of this configuration, a single optical fiber is used. A portion of the fiber may be used as a detection optical fiber. Note that the detection optical fiber 22 may be a fiber with larger structural scattering than the optical fibers 31 and 32. In addition, this invention is not limited to the above-mentioned embodiments, and can be implemented with various modifications without departing from the gist.

以上説明したようにこの考案によれば、光フア
イバの構造散乱による伝送損失を利用して機械的
な変化量を測定するようにしたので、構造簡単で
精度良い変化量の測定が可能となる変位量測定装
置を提供できる。また、光伝送路の出力光と断続
光発生手段からの断続光とを合成しているので、
光伝送路の減衰の影響を受けず安定して精度の高
い変位量測定が可能となる。
As explained above, according to this invention, the amount of mechanical change is measured using the transmission loss caused by the structural scattering of the optical fiber, so the displacement can be measured with a simple structure and with high accuracy. We can provide quantity measuring devices. In addition, since the output light of the optical transmission line and the intermittent light from the intermittent light generating means are combined,
Stable and highly accurate displacement measurement becomes possible without being affected by attenuation of the optical transmission line.

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

第1図はこの考案の一実施例を示す構成図、第
2図a〜eは同実施例の動作を示す図、第3図は
上記実施例の変形例を示すための要部構成図であ
る。 10……測定部、19……測定回路、20……
検出部、31,32……光フアイバ。
Fig. 1 is a block diagram showing an embodiment of this invention, Figs. 2 a to e are diagrams showing the operation of the same embodiment, and Fig. 3 is a block diagram of main parts showing a modification of the above embodiment. be. 10... Measuring section, 19... Measuring circuit, 20...
Detection unit, 31, 32...optical fiber.

Claims (1)

【実用新案登録請求の範囲】[Scope of utility model registration request] 所定間隔毎の断続光を交互に発生する断続光発
生手段と、この断続光発生手段から発せられた一
方の断続光を一端側から入力し、この入力光を他
端側から所定位置に設けられた受光器に対して出
力する如く配置され、かつその中途部が測定量検
出部に配置された光フアイバを用いた光伝送路
と、この光伝送路の上記他端側と上記受光器との
間に介在され、この光伝送路の出力光と上記断続
光発生手段から発生する他方の断続光とを合成す
る手段と、この合成する手段による合成光が所定
の基準状態において連続した同一レベルの光とな
るように上記他方の断続光を予め調整する手段
と、上記受光器からの出力を受けて、その変位を
測定量として出力する測定回路とを具備したこと
を特徴とする変位量測定装置。
An intermittent light generating means that alternately generates intermittent light at predetermined intervals, one intermittent light emitted from the intermittent light generating means is inputted from one end side, and this input light is provided at a predetermined position from the other end side. an optical transmission line using an optical fiber arranged so as to output to a light receiver, the middle part of which is arranged in a measured quantity detection section; and a link between the other end of the optical transmission line and the light receiver. A means for combining the output light of the optical transmission line with the other intermittent light generated from the intermittent light generating means, and a means for combining the output light of the optical transmission line with the other intermittent light generated from the intermittent light generating means, and a means for combining the output light of the optical transmission line with the other intermittent light generated from the intermittent light generating means, and a means for combining the output light of the optical transmission line with the other intermittent light generated from the intermittent light generating means, and a A displacement amount measuring device comprising means for adjusting the other intermittent light in advance so that the other intermittent light becomes light, and a measuring circuit that receives the output from the light receiver and outputs the displacement as a measured amount. .
JP1384580U 1980-02-06 1980-02-06 Expired JPH0228403Y2 (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP1384580U JPH0228403Y2 (en) 1980-02-06 1980-02-06

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP1384580U JPH0228403Y2 (en) 1980-02-06 1980-02-06

Publications (2)

Publication Number Publication Date
JPS56116610U JPS56116610U (en) 1981-09-07
JPH0228403Y2 true JPH0228403Y2 (en) 1990-07-31

Family

ID=29610352

Family Applications (1)

Application Number Title Priority Date Filing Date
JP1384580U Expired JPH0228403Y2 (en) 1980-02-06 1980-02-06

Country Status (1)

Country Link
JP (1) JPH0228403Y2 (en)

Also Published As

Publication number Publication date
JPS56116610U (en) 1981-09-07

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