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JP3448779B2 - Fiber optic sensor - Google Patents
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JP3448779B2 - Fiber optic sensor - Google Patents

Fiber optic sensor

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Publication number
JP3448779B2
JP3448779B2 JP10835992A JP10835992A JP3448779B2 JP 3448779 B2 JP3448779 B2 JP 3448779B2 JP 10835992 A JP10835992 A JP 10835992A JP 10835992 A JP10835992 A JP 10835992A JP 3448779 B2 JP3448779 B2 JP 3448779B2
Authority
JP
Japan
Prior art keywords
light
measurement
reference light
wavelength
multiplexer
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 - Fee Related
Application number
JP10835992A
Other languages
Japanese (ja)
Other versions
JPH07260426A (en
Inventor
郁男 荒井
国太 伊東
寿 佐藤
浩久 工藤
善文 井上
Original Assignee
株式会社クリスタルテクノロジー
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 株式会社クリスタルテクノロジー filed Critical 株式会社クリスタルテクノロジー
Priority to JP10835992A priority Critical patent/JP3448779B2/en
Publication of JPH07260426A publication Critical patent/JPH07260426A/en
Application granted granted Critical
Publication of JP3448779B2 publication Critical patent/JP3448779B2/en
Anticipated expiration legal-status Critical
Expired - Fee Related legal-status Critical Current

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  • Instruments For Measurement Of Length By Optical Means (AREA)
  • Length Measuring Devices By Optical Means (AREA)
  • Optical Transform (AREA)
  • Light Guides In General And Applications Therefor (AREA)
  • Optical Integrated Circuits (AREA)

Description

【発明の詳細な説明】 【0001】 【産業上の利用分野】本発明は振動振幅,または距離変
化量の超精密測定の分野で利用する光ファイバーセンサ
ー及び光導波路センサーに関するものである。 【0002】 【従来の技術】従来から振動や距離変化量の精密測定に
は光の干渉測定法が用いられていた。その方法は測定対
象物に基準光を照射しその反射光または通過光(以後測
定光とする)と基準光を干渉させ,発生する干渉現象,
例えば干渉縞やビート出力により距離変化の測定を行っ
ていた。 即ち一つの状態の干渉縞を観測しその縞の
強弱が反転し,また同様に成るまで測定対象との相対距
離を移動すればその時の移動距離が光の波長に相当する
わけである。従って波長のわかっている光を用いれば基
準光と反射光の干渉現象を利用することにより相対距離
の移動量を知ることが出来る。また光を標的に照射する
ファイバーと反射光を受けるファイバ−はそれぞれ別々
に設けられていた。 【0003】 【発明が解決しようとする課題】従来の光干渉法も光の
位相比較であるから高精度測定が可能であるが,一つの
干渉現象のみを観測した場合相対距離の変化は検出でき
ても,変化の方向は判別出来ないため別に移動方向を決
定する手段を必要とした。従って相対距離の変化の方向
が明かな場合は良いとしても,前後に振動する振動面を
測定する場合のように振動面が接近しつつあるのか,離
れつつあるのかを検出することは不可能であった。また
光を標的に照射するファイバーと反射光を受けるファイ
バーが別々であるため,受光側のファイバーに反射光を
入射させるためには特定の反射角を必要とし光ファイバ
ーセンサーを標的に接近させるには限界があり,充分接
近出来ないため受光感度も低下した。 【0004】 【課題を解決するための手段】本発明は課題を解決する
ための手段としてファイバー型の合分波器を4個使用
し,第図1に示すように接続した。第図1に於ては基
準光の入力路,は測定光の入力路,はそれぞれ合
分波器で,この場合は分波器として動作する。従って基
準光はでに分岐され,合分波器に導かれ
る。同様に測定光はで分岐されて▲10▼の経路
を経て合波器に導かれる。,合波器に導かれた
基準光と測定光は,合成され▲11▼▲12▼に出力さ
れる。これらの合成された出力は基準光と測定光が干渉
し合い,それらの位相差に応じて出力光の強さが変化す
る。従って▲11▼▲12▼の出力を別々の 光検波器
▲19▼▲20▼に印加することによりこれらの出力光
の強弱の変化が検出出来る。本発明では光干渉法で一般
に用いられる基準光と測定光を干渉させる部分を2箇所
設け,双方に基準光と測定光を導き干渉させて2系統の
ビート出力を得られる様にしたことが特徴であり, 更
に4分の1波長位相の異なる比較部を設け,常に90度
位相の異なる1対の干渉出力が得られる様にし,それら
をXY座標上でリサージュを描いた場合の位相が進むか
遅れるかで変位の方向を検出することができる様にし
た。また標的に照射した光の反射光を容易に受光するた
め,送受間に光合分波器▲14▼を挿入した。 【0005】 【作 用】作用を第1図に沿って説明する。第1図
は, が光ファイバー合分波器▲1
0▼▲11▼▲12▼が光ファイパー線路であり,
は分波器として動作し,は合波器として動作する。
また▲10▼の線路長は,が全く等しく,
▲10▼のみは4分の1波長だけ長くしてある。いま線
路に光が伝搬した場合,合波器には系統入力
光が1/2づつ加わる。 次にの系統の入力は合波器
には振幅は1/2づつであるが,互いに90度位相
が異なって加わる。 合波器の出力はファイバー線
路▲11▼▲12▼に導かれ光検波器▲19▼▲20▼
に加わり電流に変換される。 光検波器に2種類の光が
入射した場合の動作は干渉し2波のビート出力となる。
このとき入力波の1/4波長遅れ即ち90度遅れ位相は
検波器出力にもビートの波長で90度位相遅れと成って
出力されるから,▲19▼▲20▼のビート出力は互い
に直交した信号になる。従って両者をCRTオッシロス
コープのX軸とY軸に各々印加すればこれらのビート出
力で円形リサージュ図形を描き,リサージュ図の回転方
向が位相の遅進即ち対象物との相対位置の変化の方向を
示すことになる。なお▲10▼の長さは必ずしも4分の
1波長だけ長い必要はなく,ちょうど半波長の整数倍を
避ければ任意の長さでよい。この場合のリサージュは一
般に楕円となるが回転方向の判別は可能であり,本発明
の作用を達成できる。本発明は光ファイバーで構成する
だけでなく,固体化した光導波路集積回路でも同様な作
用が達成出来る。また先端部に光合分波器▲14▼を挿
入し送受を一体化したことにより,照射光と反射光は同
一経路を通るため,標的の反射面と入射光の関係は常に
垂直でよくセンサー端面と反射面との距離は無条件とな
った。 【0006】 【実施例】本発明の実施例を第2図に示す。
▲10▼▲11▼▲12▼▲19▼▲20▼ま
では先に説明した通りである。▲13▼▲14▼▲15
▼▲16▼▲17▼▲18▼は実際に測定の為に追加し
た部分で,▲13▼▲14▼は光ファイバー分波器,▲
15▼は光源からセンサー先端に光を導くファイバ−線
路,▲16▼はレーザー光源で1.55ミクロンのDF
Bレーザーを使用した。▲17▼は標的で矢印の方向即
ち反射面が光線と直交し変位の方向が光線と平行する方
向に設定した。▲18▼はセンサー用ファイバーの先端
部で,合分波器▲14▼を経て導かれた光は▲18▼の
先端より発し標的▲17▼で反射して戻り再び▲18▼
を経てその一部が分波器▲14▼でに導かれる。一方
レーザー光源▲16▼からの光は分波器▲13▼で分岐
されてを経て基準光となる。光検出器▲19▼▲20
▼の出力はCRTオッシロスコープのX軸Y軸にそれぞ
れ接続し標的▲17▼を振動させたところ,CRT面に
円形リサージュ図形が現れ振動変位量がレーザー光源の
半波長毎にリサージュが1回転することが確認出来た振
動変位の方向によりリサージュ図の回転方向が反転し予
想通りの結果が得られた。この結果から,標的▲17▼
の振動変位量または距離変化量は上記のリサージュの回
転角度を計測することにより,また標的▲17▼の接近
と後退の判別はこのリサージュの右回りか左回りかの回
転方向の計測により知ることが出来る。なおこれらの計
測は従来の方法を用いることができる。また▲15▼の
線路に光方向性結合器を挿入して測定光が光源側に戻る
ことを阻止すれば更に良好になる。 使用した光ファイバー 外形 125ミクロン 石英を基本材質とした単一モード 適応波長1.3ミクロン〜1.6ミクロン用 測定条件 測定波長 1.55ミクロン 光 源 半導体レーザー 【0007】 【発明の効果】本発明実施の結果位相計とカウンターを
用い広範囲の超高精度測定が可能と成った。
Description: BACKGROUND OF THE INVENTION 1. Field of the Invention The present invention relates to an optical fiber sensor and an optical waveguide sensor used in the field of ultra-precise measurement of vibration amplitude or distance change. 2. Description of the Related Art Conventionally, a light interference measurement method has been used for precise measurement of vibration and distance change. The method is to irradiate a reference light to an object to be measured and cause the reflected light or transmitted light (hereinafter referred to as measurement light) to interfere with the reference light, thereby generating an interference phenomenon,
For example, distance change is measured by interference fringes or beat output. That is, if the interference fringes in one state are observed, the strength of the fringes is reversed, and the relative distance to the object to be measured is moved until the fringes become similar, the moving distance at that time corresponds to the wavelength of light. Therefore, if light having a known wavelength is used, the amount of movement of the relative distance can be known by utilizing the interference phenomenon between the reference light and the reflected light. In addition, a fiber for irradiating the target with light and a fiber for receiving reflected light are separately provided. [0003] The conventional optical interferometry is also capable of high-precision measurement because it is a phase comparison of light, but when only one interference phenomenon is observed, a change in relative distance cannot be detected. However, since the direction of change cannot be determined, a means for separately determining the moving direction was required. Therefore, even if the direction of the relative distance change is clear, it is not possible to detect whether the vibrating surface is approaching or moving away, as in the case of measuring a vibrating surface that vibrates back and forth. there were. In addition, since the fiber that irradiates light to the target and the fiber that receives reflected light are separate, a specific reflection angle is required to make the reflected light incident on the fiber on the light receiving side, and there is a limit to bringing the optical fiber sensor close to the target. However, the light receiving sensitivity was also reduced due to insufficient access. According to the present invention, four fiber type multiplexers / demultiplexers are used as means for solving the problems and connected as shown in FIG. In FIG. 1, the input path of the reference light and the input path of the measurement light are multiplexer / demultiplexers, respectively, and in this case, they operate as a demultiplexer. Therefore, the reference light is branched at the で and guided to the multiplexer / demultiplexer. Similarly, the measurement light is branched and guided to the multiplexer through the path (10). The reference light and the measurement light guided to the multiplexer are combined and output to (11) and (12). In these combined outputs, the reference light and the measurement light interfere with each other, and the intensity of the output light changes in accordance with the phase difference between them. Therefore, by applying the outputs of <11> and <12> to separate photodetectors <19> and <20>, changes in the intensity of these output lights can be detected. The present invention is characterized in that two portions for interfering the reference light and the measurement light, which are generally used in the optical interference method, are provided, and the reference light and the measurement light are guided and interfered with each other to obtain two types of beat outputs. Further, a comparison unit having a quarter-wave phase different from each other is provided so that a pair of interference outputs having a phase difference of 90 degrees can always be obtained, and whether the phase advances when a Lissajous is drawn on the XY coordinates. The direction of displacement can be detected by delaying. In addition, an optical multiplexer / demultiplexer (14) was inserted between the transmission and reception to easily receive the reflected light of the light irradiated on the target. The operation will be described with reference to FIG. Fig. 1 shows an optical fiber multiplexer / demultiplexer.
0 ▼ 11 線路 12 is an optical fiber line,
Operates as a demultiplexer, and operates as a multiplexer.
The line length of (10) is exactly the same,
Only (10) is extended by a quarter wavelength. Now, when light propagates on the line, system input light is added to the multiplexer in half at a time. The input of the next system is applied to the multiplexer at a phase difference of 90 degrees, although the amplitude is 1 /. The output of the multiplexer is guided to the fiber lines (11) and (12) and the optical detectors (19) and (20).
And is converted to a current. When two types of light are incident on the photodetector, the operations interfere with each other, resulting in two-wave beat output.
At this time, the 1/4 wavelength delay of the input wave, that is, the 90-degree delayed phase is also output to the detector output with a 90-degree phase delay at the beat wavelength, so that the beat outputs of (19) and (20) are orthogonal to each other. Signal. Therefore, if both are applied to the X-axis and the Y-axis of the CRT oscilloscope, respectively, a circular Lissajous figure is drawn with these beat outputs, and the rotation direction of the Lissajous figure indicates the direction of the phase delay, that is, the change of the relative position with respect to the object. Will be. The length of {10} need not necessarily be longer by a quarter wavelength, but may be any length as long as it is not exactly an integral multiple of half a wavelength. The Lissajous in this case is generally an ellipse, but the rotation direction can be determined, and the operation of the present invention can be achieved. The present invention can achieve the same effect not only by using an optical fiber but also by using a solidified optical waveguide integrated circuit. In addition, by inserting an optical multiplexer / demultiplexer (14) at the tip and integrating the transmission and reception, the irradiation light and the reflected light pass through the same path, so that the relationship between the target reflection surface and the incident light is always vertical and the sensor end surface The distance between the reflector and the reflecting surface was unconditional. FIG. 2 shows an embodiment of the present invention.
The operations up to (10), (11), (12), (19), and (20) are as described above. ▲ 13 ▼ ▲ 14 ▼ ▲ 15
▼ (16), (17) and (18) are the parts added for actual measurement, (13) and (14) are optical fiber duplexers, and
Reference numeral 15 denotes a fiber line for guiding light from the light source to the tip of the sensor, and reference numeral 16 denotes a 1.55 micron DF laser light source.
A B laser was used. (17) is a target, which is set in the direction of the arrow, that is, the direction in which the reflection surface is orthogonal to the light beam and the direction of displacement is parallel to the light beam. (18) is the tip of the sensor fiber, and the light guided through the multiplexer / demultiplexer (14) is emitted from the tip of (18), reflected by the target (17) and returned again to (18).
A part of the light is guided to the demultiplexer (14) by way of. On the other hand, the light from the laser light source (16) is branched by the splitter (13) and becomes reference light. Photodetector ▲ 19 ▼ ▲ 20
The output of ▼ is connected to the X-axis and Y-axis of the CRT oscilloscope, respectively, and when the target 17 is vibrated, a circular Lissajous figure appears on the CRT surface and the amount of vibration displacement is one rotation of the Lissajous every half wavelength of the laser light source. The rotation direction of the Lissajous figure was reversed depending on the direction of the vibration displacement that was confirmed, and the expected result was obtained. From these results, the target (17)
The amount of vibration displacement or change in distance of the Lissajous can be determined by measuring the rotation angle of the above Lissajous, and whether the target (17) approaches or retreats can be determined by measuring the direction of rotation of the Lissajous clockwise or counterclockwise. Can be done. Note that a conventional method can be used for these measurements. It is further improved if an optical directional coupler is inserted into the line (15) to prevent the measurement light from returning to the light source side. Optical fiber used External shape Single-mode adaptive wavelength of 1.3 micron to 1.6 micron using 125 micron quartz as basic material Measurement wavelength 1.55 micron Light source Semiconductor laser Effect of the present invention As a result, a wide range of ultra-high-precision measurements were possible using a phase meter and counter.

【図面の簡単な説明】 【図1】 本発明の接続図である。 【図2】 第2図は本発明の実施例である。 【符号の説明】 : 分波器 : 分波器 : 合波器 : 合波器 : 基準光伝送路 : 測定光伝送路 : 分岐した基準光伝送路 : 分岐した基準光伝送路 : 分岐した測定光伝送路 ▲10▼: 分岐した測定光伝送路で1/4波長長くし
てあるもの ▲11▼: 合波器と検出器間の伝送路 ▲12▼: 合波器と検出器間の伝送路 ▲13▼: 基準光の分波器 ▲14▼: 入出力結合分波器 ▲15▼: 基準光伝送線路 ▲16▼: レーザー光源 ▲17▼: 標的 ▲18▼: センサー用ファイバーの先端部 ▲19▼: 光検出器1 ▲20▼: 光検出器2
BRIEF DESCRIPTION OF THE DRAWINGS FIG. 1 is a connection diagram of the present invention. FIG. 2 is an embodiment of the present invention. [Description of Symbols]: Demultiplexer: Demultiplexer: Multiplexer: Multiplexer: Reference optical transmission line: Measurement optical transmission line: Branched reference optical transmission line: Branched reference optical transmission line: Branched measurement light Transmission line {circle around (10)}: A branched measurement light transmission line which is extended by 4 wavelength. {11}: Transmission line between the multiplexer and the detector. {12}: Transmission line between the multiplexer and the detector. {Circle around (13)}: Demultiplexer for reference light <14>: Input / output coupler / demultiplexer <15>: Reference light transmission line <16>: Laser light source <17>: Target <18>: Tip of sensor fiber <▲ 19 ▼: Photodetector 1 ▲ 20 ▼: Photodetector 2

───────────────────────────────────────────────────── フロントページの続き (72)発明者 井上 善文 千葉県大網白里町北飯塚199番地6 (56)参考文献 特開 昭63−47602(JP,A) (58)調査した分野(Int.Cl.7,DB名) G01B 9/00 - 11/30 G01D 5/26 ──────────────────────────────────────────────────続 き Continued on the front page (72) Inventor Yoshifumi Inoue 199-6 Kita-Iizuka, Oamishirasato-cho, Chiba Prefecture (56) References JP-A-63-47602 (JP, A) (58) Fields investigated (Int. Cl 7, DB name) G01B 9/00 -. 11/30 G01D 5/26

Claims (1)

(57)【特許請求の範囲】 【請求項1】基準光と、基準光と同一光源から取り出し
測定のための経路を経た測定光を干渉させてビートを得
る光干渉器において、基準光と測定光それぞれ分岐し、
その分岐出力を基準光と測定光で結合させた少なくとも
2組の結合出力端を持ち、その2組の結合出力間の位相
関係を検出する構造で、更に基準光と測定光それぞれの
分岐部分から結合部分に至る4系統の光線路長を3系統
はほぼ等しく、1系統のみ(波長/4)または、ちょう
ど半波長の整数倍を避けた任意の長さ相当分だけ長くす
るか、短くする事を特徴とした干渉型光ファイバー距離
センサー及び干渉型光導波路距離センサー。
(57) [Claim 1] In an optical interferometer for obtaining a beat by interfering a reference light and a measurement light taken out of the same light source as the reference light and passing through a path for measurement, a reference light and a measurement are obtained. Each of the light branches,
The structure has at least two sets of combined output ends obtained by combining the branched outputs with the reference light and the measuring light, and detects a phase relationship between the two sets of combined outputs. The lengths of the four optical lines leading to the coupling portion are almost the same for the three systems, and only one system (wavelength / 4) or a length longer or shorter by an arbitrary length corresponding to exactly an integer multiple of half a wavelength is avoided. An interference type optical fiber distance sensor and an interference type optical waveguide distance sensor.
JP10835992A 1992-03-17 1992-03-17 Fiber optic sensor Expired - Fee Related JP3448779B2 (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP10835992A JP3448779B2 (en) 1992-03-17 1992-03-17 Fiber optic sensor

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP10835992A JP3448779B2 (en) 1992-03-17 1992-03-17 Fiber optic sensor

Publications (2)

Publication Number Publication Date
JPH07260426A JPH07260426A (en) 1995-10-13
JP3448779B2 true JP3448779B2 (en) 2003-09-22

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JP10835992A Expired - Fee Related JP3448779B2 (en) 1992-03-17 1992-03-17 Fiber optic sensor

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JP (1) JP3448779B2 (en)

Families Citing this family (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
CN103238093A (en) * 2010-12-01 2013-08-07 日本电气株式会社 Optical branching element, optical waveguide device by using optical branching element, and method of manufacturing optical branching element, method of manufacturing optical waveguide device
JP6204272B2 (en) * 2014-06-05 2017-09-27 日本電信電話株式会社 Distance measuring device

Also Published As

Publication number Publication date
JPH07260426A (en) 1995-10-13

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