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JPH0577241B2 - - Google Patents
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JPH0577241B2 - - Google Patents

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Publication number
JPH0577241B2
JPH0577241B2 JP25946486A JP25946486A JPH0577241B2 JP H0577241 B2 JPH0577241 B2 JP H0577241B2 JP 25946486 A JP25946486 A JP 25946486A JP 25946486 A JP25946486 A JP 25946486A JP H0577241 B2 JPH0577241 B2 JP H0577241B2
Authority
JP
Japan
Prior art keywords
light
optical fiber
measured
amount
distance
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 - Lifetime
Application number
JP25946486A
Other languages
Japanese (ja)
Other versions
JPS63113301A (en
Inventor
Tsutomu Fujita
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.)
Kanadevia Corp
Original Assignee
Hitachi Shipbuilding and Engineering Co 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 Shipbuilding and Engineering Co Ltd filed Critical Hitachi Shipbuilding and Engineering Co Ltd
Priority to JP25946486A priority Critical patent/JPS63113301A/en
Publication of JPS63113301A publication Critical patent/JPS63113301A/en
Publication of JPH0577241B2 publication Critical patent/JPH0577241B2/ja
Granted legal-status Critical Current

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  • Measurement Of Optical Distance (AREA)
  • Length Measuring Devices By Optical Means (AREA)

Description

【発明の詳細な説明】 〔産業上の利用分野〕 この発明は、被測定物との距離の測定を非接触
により行なう非接触変位測定方法に関する。
DETAILED DESCRIPTION OF THE INVENTION [Field of Industrial Application] The present invention relates to a non-contact displacement measuring method for measuring the distance to an object to be measured in a non-contact manner.

〔従来の技術〕[Conventional technology]

一般に、被測定物との距離の測定を非接触によ
り行なう場合、たとえば第4図に示すような光フ
アイバを利用した測定が行なわれており、投光用
光フアイバ1の先端と受光用光フアイバ2の先端
とが被測定物3の表面から同一距離になるよう、
両光フアイバ1,2を配設し、投光用光フアイバ
1により被測定物3の表面に光を投射し、被測定
物3の表面からの反射光を受光用光フアイバ2に
より受光し、受光用光フアイバ2の受光量にもと
づき、両光フアイバ1,2の先端と被測定物3の
表面との距離Dを導出している。
Generally, when measuring the distance to the object to be measured without contact, measurement is carried out using an optical fiber as shown in FIG. so that the tip of 2 is at the same distance from the surface of the object to be measured 3.
Both optical fibers 1 and 2 are arranged, the light emitting optical fiber 1 projects light onto the surface of the object to be measured 3, the light reflected from the surface of the object to be measured 3 is received by the light receiving optical fiber 2, Based on the amount of light received by the light-receiving optical fiber 2, the distance D between the tips of both optical fibers 1 and 2 and the surface of the object to be measured 3 is derived.

このとき、両光フアイバ1,2の先端と被測定
物3の表面との距離Dが小さい場合、第5図aに
示すように、投光用光フアイバ1による被測定物
3の表面における光の投射スポツトSと、受光用
光フアイバ2による被測定物3の表面における受
光視野Rとが重なることはなく、同図bさらには
cに示すように、距離Dが大きくなるに連れ、投
射スポツトSと受光視野Rとの重なりが次第に大
きくなるため、距離Dと受光用光フアイバ2の受
光量との関係は第6図中の実線に示すようにな
り、距離Dの増加に伴う投射スポツトSと受光視
野Rとの重なりの増加により、受光用光フアイバ
2の受光量は次第に増加するが、距離Dがある程
度以上になると、反射光の減衰が大きくなつて受
光用光フアイバ2の受光量は次第に減少する。
At this time, if the distance D between the tips of both optical fibers 1 and 2 and the surface of the object to be measured 3 is small, as shown in FIG. The projection spot S and the light receiving field R on the surface of the object to be measured 3 by the light receiving optical fiber 2 do not overlap, and as shown in FIGS. As the overlap between S and the light-receiving field of view R gradually increases, the relationship between the distance D and the amount of light received by the light-receiving optical fiber 2 becomes as shown by the solid line in FIG. The amount of light received by the light receiving optical fiber 2 gradually increases due to the increase in the overlap between It gradually decreases.

従つて、被測定物3と同一反射率のテストピー
スに対する前記したような距離と受光量との関係
を予め求めておけば、当該関係曲線上の実際の被
測定物3からの反射光の受光量に相当する点か
ら、両光フアイバ1,2の先端と被測定物3の表
面との距離Dを容易に導出できることになる。
Therefore, if the relationship between the distance and the amount of received light as described above is determined in advance for a test piece having the same reflectance as the object to be measured 3, the actual reception of reflected light from the object to be measured 3 on the relationship curve can be determined in advance. From the point corresponding to the amount, the distance D between the tips of both optical fibers 1 and 2 and the surface of the object to be measured 3 can be easily derived.

そして、このような光フアイバを利用した測定
方法の利点として、たとえば投射光用光源に可視
光レーザなどの単一波長のコヒーレント光源を用
いた場合に、分解能が波長程度(0.1μm)とな
つて距離検出精度は非常に高くなり、しかも装置
が小型でかつ軽量な構成となり、取り扱いが容易
になるなどの点が挙げられる。
An advantage of such a measurement method using an optical fiber is that, for example, when a coherent light source with a single wavelength such as a visible laser is used as the light source for projection light, the resolution is on the order of the wavelength (0.1 μm). Distance detection accuracy is extremely high, and the device is small and lightweight, making it easy to handle.

〔発明が解決しようとする問題点〕[Problem that the invention seeks to solve]

しかし、この場合、被測定物3の反射率が異な
れば、前記したような距離と受光量との関係も変
化し、たとえば反射率が第6図中の実線の場合よ
りも大きいと、距離と受光量との関係曲線は、同
図中の1点鎖線のように同図中の実線の場合より
も縦軸の受光量の正方向に全体的に変位し、反射
率が同図中の実線の場合よりも小さいと、距離と
受光量との関係曲線は、同図中の2点鎖線のよう
に縦軸の負方向に全体的に変位するため、たとえ
ば被測定物3の表面性状が変化して反射率が途中
で変化するような場合に、反射率の変化により受
光量が変化したときに、実際には距離は変わらず
に反射率が変化したために生じた受光量の変化で
あつても、距離の変化としてしか検出できず、表
面性状が一様でない被測定物3との距離の測定に
は適用できないことになり、応用性に欠けるとい
う問題点がある。
However, in this case, if the reflectance of the object to be measured 3 differs, the relationship between the distance and the amount of received light will change as described above. For example, if the reflectance is larger than the solid line in FIG. The relationship curve with the amount of received light is generally shifted in the positive direction of the amount of received light on the vertical axis compared to the solid line in the same figure, as shown by the dashed-dotted line in the same figure, and the reflectance is as shown by the solid line in the same figure. If the relationship between the distance and the amount of light received is smaller than the case of When the reflectance changes midway through the distance, when the amount of light received changes due to the change in reflectance, it is actually a change in the amount of light received due to the change in reflectance without changing the distance. However, this method can only be detected as a change in distance, and cannot be applied to measuring the distance to the object 3 whose surface texture is not uniform, resulting in a lack of applicability.

そこで、この発明では、表面性状が一様でない
被測定物との距離の測定にも適用できるようにす
ることを技術的課題とする。
Therefore, a technical problem of the present invention is to enable the method to be applied to measurement of distance to an object to be measured whose surface properties are not uniform.

〔問題点を解決するための手段〕[Means for solving problems]

この発明は、前記の点に留意してなされたもの
であり、投光用光フアイバの先端と受光用光フア
イバの先端とが被測定物表面から同一距離になる
よう、前記両光フアイバを配設し、前記投光用光
フアイバにより前記被測定物表面に光を照射し、
前記被測定物表面からの反射光を前記受光用光フ
アイバにより受光し、前記受光用光フアイバの受
光量にもとづき前記両光フアイバの先端と前記被
測定物表面との距離を測定する非接触変位測定方
法において、前記投光用光フアイバを一部分岐し
て受光用補助光フアイバを形成し、前記受光用光
フアイバの受光量と前記受光用補助光フアイバの
受光量との比にもとづき、前記投光用光フアイバ
および受光用光フアイバの先端と被測定物表面と
の距離を測定することを特徴とする非接触変位測
定方法である。
This invention has been made with the above points in mind, and the optical fibers are arranged so that the tip of the light-emitting optical fiber and the tip of the light-receiving optical fiber are at the same distance from the surface of the object to be measured. and irradiate the surface of the object to be measured with light using the light emitting optical fiber,
Non-contact displacement, in which the reflected light from the surface of the object to be measured is received by the optical fiber for light reception, and the distance between the tips of the optical fibers and the surface of the object to be measured is measured based on the amount of light received by the optical fiber for light reception. In the measuring method, a part of the light emitting optical fiber is branched to form a light receiving auxiliary optical fiber, and the light emitting and receiving auxiliary optical fibers are determined based on the ratio of the amount of light received by the light receiving optical fiber and the light receiving amount of the light receiving auxiliary optical fiber. This is a non-contact displacement measuring method characterized by measuring the distance between the tips of the optical fiber for light and the optical fiber for light reception and the surface of the object to be measured.

〔作用〕[Effect]

したがつて、この発明によると、たとえば被測
定物の表面性状が、ある位置を境に変化して反射
率が変化する場合、投光用、受光用光フアイバの
先端と被測定物表面との距離を一定とすると、受
光用光フアイバの受光量の変化の割合と受光用補
助光フアイバの受光量の変化の割合とは等しくな
り、受光用光フアイバの受光量と受光用補助光フ
アイバの受光量との比が、被測定物の表面性状の
変化による反射率の変化に依存せず、距離のみに
依存して変化することになり、表面性状が一様で
ない被測定物との距離の測定が可能となる。
Therefore, according to the present invention, for example, when the surface properties of the object to be measured change after a certain position and the reflectance changes, the relationship between the tips of the light emitting and receiving optical fibers and the surface of the object to be measured changes. If the distance is constant, the rate of change in the amount of light received by the light-receiving optical fiber and the rate of change in the amount of light received by the auxiliary light-receiving optical fiber are equal, and the amount of light received by the light-receiving optical fiber and the amount of light received by the auxiliary light-receiving optical fiber are equal. The ratio to the measured object changes depending only on the distance, not on changes in reflectance due to changes in the surface texture of the object to be measured, making it possible to measure distances to objects whose surface texture is not uniform. becomes possible.

〔実施例〕〔Example〕

つぎに、この発明を、その1実施例を示した第
1図ないし第3図とともに詳細に説明する。
Next, the present invention will be explained in detail with reference to FIGS. 1 to 3 showing one embodiment thereof.

第1図において、第4図と同一記号は同一のも
のもしくは相当するものを示し、第4図と異なる
点は、投光用光フアイバ1の一部を分岐し、受光
用補助光フアイバ4を形成し、受光用光フアイバ
2の受光量と受光用補助光フアイバ4の受光量と
の比にもとづき、両光フアイバ1,2の先端と被
測定物3の表面との距離Dを測定するようにした
点である。
In Fig. 1, the same symbols as in Fig. 4 indicate the same or equivalent parts, and the difference from Fig. 4 is that a part of the light emitting optical fiber 1 is branched and a light receiving auxiliary optical fiber 4 is and measure the distance D between the tips of both optical fibers 1 and 2 and the surface of the object to be measured 3 based on the ratio of the amount of light received by the light-receiving optical fiber 2 and the amount of light received by the auxiliary light-receiving optical fiber 4. This is the point I made.

ところで、表面性状が一様で反射率が一定のテ
スト用被測定物3を用い、距離Dと受光用光フア
イバ2の受光量φ1および受光用補助光フアイバ
4の受光量φ2それぞれとの関係を調べた結果、
受光用光フアイバ2の場合、第2図a中の1点鎖
線に示すように、前記した第6図中の各曲線と同
様のパターンとなり、受光用補助光フアイバ4の
場合、第2図a中の2点鎖線に示すように距離D
が増加するに連れて受光量が次第に減少するパタ
ーンとなり、受光用光フアイバ2の受光量φ1と
受光用補助光フアイバ4の受光量φ2との比φ1/
φ2は、第2図bに示すように距離Dが増加する
に連れて次第に大きくなる。
By the way, using a test object 3 with uniform surface properties and a constant reflectance, the relationship between the distance D and the amount of light received by the light receiving optical fiber 2 φ1 and the amount of light received by the auxiliary light receiving fiber 4 φ2 is calculated. As a result of my investigation,
In the case of the light-receiving optical fiber 2, the pattern is similar to each curve in FIG. 6 described above, as shown by the dashed-dotted line in FIG. Distance D as shown in the middle two-dot chain line
The pattern is such that the amount of light received gradually decreases as
φ2 gradually increases as the distance D increases, as shown in FIG. 2b.

このとき、被測定物3の表面性状が、ある位置
を境に変化して反射率が変化する場合、両光フア
イバ1,2の先端と被測定物3の表面との距離を
一定とすると、受光用光フアイバ2の受光量φ1
の変化の割合と受光用補助光フアイバ4の受光量
φ2の変化の割合とが等しくなるため、両フアイ
バ2,4の受光量の比φ1/φ2は変化せず、当該
受光量の比から求められる距離も何ら変化せず、
両フアイバ2,4の受光両の比φ1/φ2は被測定
物の表面性状の変化による反射率の変化に依存せ
ず、距離Dのみに依存して変化することになる。
At this time, if the surface texture of the object to be measured 3 changes after a certain position and the reflectance changes, then if the distance between the tips of both optical fibers 1 and 2 and the surface of the object to be measured 3 is constant, then Amount of light received by optical fiber 2 for light reception φ1
Since the rate of change in the amount of light received by the auxiliary light receiving fiber 4 is equal to the rate of change in the amount of light received by the auxiliary optical fiber 4, the ratio φ1/φ2 of the amount of light received by both fibers 2 and 4 does not change, and can be calculated from the ratio of the amount of received light. There is no change in the distance traveled,
The light receiving ratio φ1/φ2 of both fibers 2 and 4 does not depend on changes in reflectance due to changes in surface properties of the object to be measured, but changes depending only on distance D.

従つて、テスト用の被測定物を用い、第2図b
に示すような距離Dに対する受光用フアイバ2お
よび受光用補助光フアイバ4の受光両の比φ1/
φ2の関係を予め求めておけば、第3図に示すよ
うに、被測定物3がたとえば異なる材質A,Bか
らなり、表面性状が途中で変化する場合であつて
も、予め求めた距離Dと受光量の比φ1/φ2との
関係曲線、および両フアイバ1,2を第3図中の
矢印方向に移動させて得られる両フアイバ2,4
の受光量の比φ1/φ2にもとづき、両光フアイバ
1,2の先端と被測定物3の表面との距離Dを連
続的に導出、測定することができる。
Therefore, using a test object to be measured, FIG.
The ratio of the light receiving fiber 2 and the light receiving auxiliary optical fiber 4 to the distance D as shown in φ1/
If the relationship of φ2 is determined in advance, as shown in FIG. and the ratio of received light amount φ1/φ2, and both fibers 2 and 4 obtained by moving both fibers 1 and 2 in the direction of the arrow in FIG.
Based on the ratio φ1/φ2 of the amount of received light, the distance D between the tips of both optical fibers 1 and 2 and the surface of the object to be measured 3 can be continuously derived and measured.

〔発明の効果〕 以上のように、この発明の非接触変位測定方法
によると、表面性状が一様でない被測定物であつ
ても、投光用、受光用光フアイバの先端と被測定
物の表面との距離を、小型で軽量な測定装置によ
り連続的にしかも容易に測定することができ、従
来の欠点を解消することが可能となり、応用範囲
の拡張を図ることができ、その効果は極めて大き
い。
[Effects of the Invention] As described above, according to the non-contact displacement measurement method of the present invention, even if the surface of the object is uneven, the tips of the light emitting and light receiving optical fibers can be easily connected to the object. The distance to the surface can be measured continuously and easily using a small and lightweight measuring device, making it possible to eliminate the drawbacks of conventional methods and expanding the range of applications, with extremely effective results. big.

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

第1図ないし第3図はこの発明の非接触変位測
定方法の1実施例を示し、第1図は断面図、第2
図aおよびbはそれぞれ距離と受光量および受光
量比との関係図、第3図は測定時の断面図、第4
図は従来の非接触変位測定方法による測定時の斜
視図、第5図a,b,cはそれぞれ異なる状態で
の被測定物表面における投射スポツト、受光視野
を示す図、第6図は距離と受光量との関係図であ
る。 1……投光用光フアイバ、2……受光用光フア
イバ、3……被測定物、4……受光用補助光フア
イバ。
1 to 3 show one embodiment of the non-contact displacement measuring method of the present invention, FIG. 1 is a sectional view, and FIG.
Figures a and b are relationship diagrams between distance, received light amount, and received light amount ratio, respectively, Figure 3 is a cross-sectional view during measurement, and Figure 4
The figure is a perspective view during measurement using the conventional non-contact displacement measurement method, Figures 5a, b, and c are diagrams showing the projection spot and light receiving field of view on the surface of the object to be measured in different states, and Figure 6 is a diagram showing the distance and field of view. It is a relationship diagram with the amount of light received. DESCRIPTION OF SYMBOLS 1... Optical fiber for light emission, 2... Optical fiber for light reception, 3... Object to be measured, 4... Auxiliary optical fiber for light reception.

Claims (1)

【特許請求の範囲】 1 投光用光フアイバの先端と受光用光フアイバ
の先端とが被測定物表面から同一距離になるよ
う、前記両光フアイバを配設し、前記投光用光フ
アイバにより前記被測定物表面に光を照射し、前
記被測定物表面からの反射光を前記受光用光フア
イバにより受光し、前記受光用光フアイバの受光
量にもとづき前記両光フアイバの先端と前記被測
定物表面との距離を測定する非接触変位測定方法
において、 前記投光用光フアイバを一部分岐して受光用補
助光フアイバを形成し、前記受光用光フアイバの
受光量と前記受光用補助光フアイバの受光量との
比にもとづき、前記投光用光フアイバおよび受光
用光フアイバの先端と被測定物表面との距離を測
定することを特徴とする非接触変位測定方法。
[Scope of Claims] 1. Both the optical fibers are arranged so that the tip of the light-emitting optical fiber and the tip of the light-receiving optical fiber are the same distance from the surface of the object to be measured, and the light-emitting optical fiber The surface of the object to be measured is irradiated with light, the reflected light from the surface of the object to be measured is received by the optical fiber for light reception, and the tips of the optical fibers and the object to be measured are connected based on the amount of light received by the optical fiber for light reception. In a non-contact displacement measurement method for measuring a distance to an object surface, a portion of the light emitting optical fiber is branched to form a light receiving auxiliary optical fiber, and the amount of light received by the light receiving optical fiber and the light receiving auxiliary optical fiber are A non-contact displacement measuring method, characterized in that the distance between the tip of the light emitting optical fiber and the light receiving optical fiber and the surface of the object to be measured is measured based on the ratio of the amount of light received to the amount of light received.
JP25946486A 1986-10-30 1986-10-30 Non-contact displacement measurement method Granted JPS63113301A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP25946486A JPS63113301A (en) 1986-10-30 1986-10-30 Non-contact displacement measurement method

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP25946486A JPS63113301A (en) 1986-10-30 1986-10-30 Non-contact displacement measurement method

Publications (2)

Publication Number Publication Date
JPS63113301A JPS63113301A (en) 1988-05-18
JPH0577241B2 true JPH0577241B2 (en) 1993-10-26

Family

ID=17334433

Family Applications (1)

Application Number Title Priority Date Filing Date
JP25946486A Granted JPS63113301A (en) 1986-10-30 1986-10-30 Non-contact displacement measurement method

Country Status (1)

Country Link
JP (1) JPS63113301A (en)

Families Citing this family (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US8826188B2 (en) * 2011-08-26 2014-09-02 Qualcomm Incorporated Proximity sensor calibration
US11719818B2 (en) * 2017-03-16 2023-08-08 Trinamix Gmbh Detector for optically detecting at least one object

Also Published As

Publication number Publication date
JPS63113301A (en) 1988-05-18

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