JPH0311401B2 - - Google Patents
Info
- Publication number
- JPH0311401B2 JPH0311401B2 JP56155027A JP15502781A JPH0311401B2 JP H0311401 B2 JPH0311401 B2 JP H0311401B2 JP 56155027 A JP56155027 A JP 56155027A JP 15502781 A JP15502781 A JP 15502781A JP H0311401 B2 JPH0311401 B2 JP H0311401B2
- Authority
- JP
- Japan
- Prior art keywords
- scanning
- light
- measured
- mirror
- imaging
- 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
Links
Classifications
-
- G—PHYSICS
- G01—MEASURING; TESTING
- G01B—MEASURING LENGTH, THICKNESS OR SIMILAR LINEAR DIMENSIONS; MEASURING ANGLES; MEASURING AREAS; MEASURING IRREGULARITIES OF SURFACES OR CONTOURS
- G01B11/00—Measuring arrangements characterised by the use of optical techniques
- G01B11/24—Measuring arrangements characterised by the use of optical techniques for measuring contours or curvatures
-
- G—PHYSICS
- G01—MEASURING; TESTING
- G01B—MEASURING LENGTH, THICKNESS OR SIMILAR LINEAR DIMENSIONS; MEASURING ANGLES; MEASURING AREAS; MEASURING IRREGULARITIES OF SURFACES OR CONTOURS
- G01B11/00—Measuring arrangements characterised by the use of optical techniques
- G01B11/02—Measuring arrangements characterised by the use of optical techniques for measuring length, width or thickness
- G01B11/026—Measuring arrangements characterised by the use of optical techniques for measuring length, width or thickness by measuring distance between sensor and object
Landscapes
- Physics & Mathematics (AREA)
- General Physics & Mathematics (AREA)
- Measurement Of Optical Distance (AREA)
- Length Measuring Devices By Optical Means (AREA)
Description
【発明の詳細な説明】
本発明は物体検知装置に係り、特に物体と物体
検知装置間の距離を測定することによつて物体の
凹凸面を認識するようにした物体検知装置に関す
る。DETAILED DESCRIPTION OF THE INVENTION The present invention relates to an object detection device, and more particularly to an object detection device that recognizes the uneven surface of an object by measuring the distance between the object and the object detection device.
従来から物体の表面を検知する物体検知装置と
しては、種々のものが提案されているが、特に物
体の表面に凹凸を有するものの認識にはそれなり
の工夫が成されている。 Various types of object detection devices have been proposed for detecting the surface of an object, and certain efforts have been made especially for recognizing objects with uneven surfaces.
その最も一般的な物体表面の検知装置として
は、複数のテレビジヨンカメラを用いて物体を少
し異つた2方向より撮像して、これらを合成する
ことで両眼立体視の原理によつて物体表面の凹凸
を認識しようとする試みがなされている。 The most common object surface detection device uses multiple television cameras to capture images of an object from two slightly different directions, and then combines these images to detect the object surface using the principle of binocular stereoscopic vision. Attempts have been made to recognize the unevenness of the surface.
更に他の方法として第1図に示す様に、光投影
機2よりのスポツトを回転鏡1に与えて物体3の
表面でスポツト投影光を走査させ、該スポツト投
影光を光検出器4で検出するものである。 Still another method, as shown in FIG. 1, is to apply a spot from a light projector 2 to a rotating mirror 1, scan the surface of an object 3 with the spot projected light, and detect the spot projected light with a photodetector 4. It is something to do.
第2図は従来の他の方法を示すもので物体3に
光源5に設けたスリツト5bを通してランプ5a
よりのスリツト通過光6を投影することで物体上
にスリツト通過光6に相当する投影6aを行な
い、テレビジヨンカメラ7でスリツト通過光の投
影された物体3の撮像を行うようにして物体表面
上の凹凸をより明確に認識しようとするものであ
る。 FIG. 2 shows another conventional method in which a lamp 5a is passed through a slit 5b provided in a light source 5 to an object 3.
By projecting the slit-passing light 6, a projection 6a corresponding to the slit-passing light 6 is performed on the object, and the television camera 7 captures an image of the object 3 on which the slit-passing light is projected. The aim is to more clearly recognize the unevenness of the surface.
上述の如き従来の物体検知装置によると物体の
表面の凹凸を正確に検出できない欠点を持つてい
た。 Conventional object detection devices as described above have the drawback of not being able to accurately detect irregularities on the surface of an object.
本発明は上述の欠点を除去した物体検知装置を
提供するもので、その特徴とするところは、光ビ
ームによつて被測定物体の表面を走査し、観測点
と光ビーム走査装置とで三角形を形成し、被測定
物体迄の距離を測定することで、物体表面の位置
を検出するようにしたものである。 The present invention provides an object detection device that eliminates the above-mentioned drawbacks, and is characterized by scanning the surface of an object to be measured with a light beam, and forming a triangle between an observation point and a light beam scanning device. The position of the surface of the object is detected by forming the object and measuring the distance to the object.
以下、本発明について、第3図及び第4図に基
づき具体的に説明する。 Hereinafter, the present invention will be specifically explained based on FIGS. 3 and 4.
第3図は本発明の原理的構成を示すものであ
り、レーザ源8から発せられたレーザ光はスキヤ
ニングミラー9で偏向される。 FIG. 3 shows the basic configuration of the present invention, in which laser light emitted from a laser source 8 is deflected by a scanning mirror 9. As shown in FIG.
該スキヤニングミラー9は矢印方向に支点9a
を中心に揺動させることで被測定物体3AがA位
置にあるとすれば、偏向されたレーザ光はA位置
で該被測定物体表面上を走査する。 The scanning mirror 9 has a fulcrum 9a in the direction of the arrow.
If the object to be measured 3A is located at position A by swinging around , the deflected laser beam scans the surface of the object to be measured at position A.
上記被測定物体3Aの表面で反射された反射光
は90゜反射鏡10で反射されて結像レンズ11で
結像される。 The reflected light reflected from the surface of the object to be measured 3A is reflected by a 90° reflecting mirror 10 and formed into an image by an imaging lens 11.
上記結像レンズ11の結像面にプリズムミラー
12を配設する。 A prism mirror 12 is disposed on the imaging surface of the imaging lens 11.
該プリズムミラーの表面は鏡面となされている
ために、該プリズムミラーの丁度中央に結像され
た時には、その光像がプリズムミラーの頂部を境
に傾斜面12L,12Rで左右均等に分割されるの
で、左右に配設された光検知器13a,13bの
出力が互いに等しく、その差が零となる。一方、
結像面が右又は左にずれれば、プリズムミラー1
2の傾斜面12L,12Rで反射されて、反射光量
に応じた出力を光検知器13a,13bより送出
する。 Since the surface of the prism mirror is a mirror surface, when an image is formed exactly at the center of the prism mirror, the light image is divided equally on the left and right by the inclined surfaces 12 L and 12 R with the top of the prism mirror as the border. Therefore, the outputs of the left and right photodetectors 13a and 13b are equal to each other, and the difference therebetween is zero. on the other hand,
If the image plane shifts to the right or left, prism mirror 1
The light is reflected by the two inclined surfaces 12 L and 12 R , and outputs corresponding to the amount of reflected light are sent out from the photodetectors 13a and 13b.
この両光検知器よりの出力を比較回路14で比
較して端子15に出力させる。 The outputs from both photodetectors are compared by a comparison circuit 14 and outputted to a terminal 15.
更に、被測定物体に凹凸等があつて該被測定物
体の表面が3Bで示す位置Bに後退した場合にも
レーザ源8よりのレーザ光はスキヤニングミラー
9で反射され、点線で示すように被測定物体3B
の表面を走査し、反射光は反射鏡10を通つて結
像レンズ11の結像されてプリズムミラー12に
結像される。 Furthermore, even if the surface of the object to be measured has irregularities or the like and retreats to position B shown by 3B, the laser beam from the laser source 8 is reflected by the scanning mirror 9, as shown by the dotted line. Measured object 3B
The reflected light passes through a reflecting mirror 10 and is imaged by an imaging lens 11 and then onto a prism mirror 12.
すなわち、上記構成では、被測定物体の表面か
らその変位方向に延びる直線(なお直線の途中に
ミラーが介在した場合は、このミラーを介して反
射方向に延びる直線)である観測線16と、被測
定物体からの反射光とが位置的に一致した時に、
2つの光検出器13a,13bの出力が互いに等
しくなり、比較器14の出力が零となる。このこ
とから、本発明では、まず、比較器14の出力を
確認しながらスキヤニングミラー9を走査し、比
較器14の出力が零となつた時(すなわち、被測
定物体表面からの反射光が観測線16と一致した
時)のスキヤニングミラー9の走査角度θ(ここ
では、スキヤニングミラー9の中心を通るx軸方
向の水平線9bとスキヤニングミラー9の反射光
との成す角度をθとする)を求める。 That is, in the above configuration, the observation line 16, which is a straight line extending from the surface of the object to be measured in its displacement direction (if a mirror is interposed in the middle of the straight line, a straight line extending in the reflection direction via this mirror), and the object to be measured are connected to each other. When the reflected light from the measurement object matches the position,
The outputs of the two photodetectors 13a and 13b become equal to each other, and the output of the comparator 14 becomes zero. Therefore, in the present invention, first, the scanning mirror 9 is scanned while checking the output of the comparator 14, and when the output of the comparator 14 becomes zero (that is, the reflected light from the surface of the object to be measured is The scanning angle θ of the scanning mirror 9 (here, the angle formed by the horizontal line 9b in the x-axis direction passing through the center of the scanning mirror 9 and the reflected light of the scanning mirror 9 is defined as θ). ).
すると、上記構成において、スキヤニングミラ
ー9の中心位置と反射鏡10とのx軸及びy軸方
向の距離DX及びDYは予め知られているので、上
記スキヤニングミラー9の走査角度θを知ること
により、被測定物体3A,3Bから反射鏡10の
中心位置までの距離りAX、BXは三角関数を用い
て容易に算出することができる。以上のようにし
て、被測定物体表面の位置を正確に測定すること
が可能となる。 Then, in the above configuration, since the distances D By knowing this, the distances A X and B X from the objects to be measured 3A and 3B to the center position of the reflecting mirror 10 can be easily calculated using trigonometric functions. In the manner described above, it is possible to accurately measure the position of the surface of the object to be measured.
第4図は本発明の物体検知装置の具体的な構成
図であり、第3図と同一部分には同一符号を付し
て重複説明を省略する。レーザ源8よりのレーザ
光はx方向スキヤニングミラー9xとy方向スキ
ヤニングミラー9yを通して被測定物体3A又は
3Bに反射光が投影される。 FIG. 4 is a specific configuration diagram of the object detection device of the present invention, and the same parts as in FIG. 3 are given the same reference numerals and redundant explanation will be omitted. The laser beam from the laser source 8 passes through an x-direction scanning mirror 9x and a y-direction scanning mirror 9y, and reflected light is projected onto the object to be measured 3A or 3B.
尚、上記スキヤナーはx方向に1ライン行つた
後、y方向に移動し次のラインをx方向に行なう
ことを操り返すため、上記x方向スキヤニングミ
ラー9yの走査周期TYに比べてX方向スキヤニ
ングミラー9xの走査周期TXは、TX≪TYに選択
する必要がある。 In addition, since the scanner scans one line in the x direction, moves in the y direction, and performs the next line in the x direction, the scanning period T Y of the x direction scanning mirror 9y is The scanning period T X of the scanning mirror 9x needs to be selected such that T X <<T Y.
又、上記x及びy方向スキヤニングミラー9
x,9yはコンピユーター20よりの制御信号に
より走査用のコントローラ18,19を通して回
転制御される。 Moreover, the x and y direction scanning mirror 9
The rotations of x and 9y are controlled by control signals from the computer 20 through scanning controllers 18 and 19.
一方、被測定物体からの反射光は、y方向スキ
ヤニングミラー9yで反射され、更に第1及び第
2の反射鏡10b,10aで反射されて、結像レ
ンズ11を通じてプリズムミラー12に結像す
る。 On the other hand, the reflected light from the object to be measured is reflected by the y-direction scanning mirror 9y, further reflected by the first and second reflecting mirrors 10b and 10a, and is imaged on the prism mirror 12 through the imaging lens 11. .
光検出器13a,13bよりの検出々力は増憤
器17a,17bで増幅されて比較用の比較回路
14で比較した出力をコンピユータ20に入力し
て、その比較回路14の出力が零になる時のxお
よびy方向スキヤニングミラー9x,9yの各走
査角度θ(第3図参照)を知ることで、第3図に
おける距離Ax、Bxを求めたのと同様な原理によ
り、被測定物体表面の位置を測定することができ
る。 The detection power from the photodetectors 13a and 13b is amplified by intensifiers 17a and 17b, and the outputs compared by a comparison circuit 14 are inputted to the computer 20, and the output of the comparison circuit 14 becomes zero. By knowing the scanning angles θ of the scanning mirrors 9x and 9y in the x and y directions at The position of the object surface can be measured.
本発明は上述の如く構成されたので被測定物体
から物体検知装置の基準位置までの距離を極めて
正確に検出することが出来るので、物体に凹凸が
あつても、これを正確に認識することが出来る特
徴を有するものである。 Since the present invention is configured as described above, the distance from the object to be measured to the reference position of the object detection device can be detected extremely accurately, so even if the object has unevenness, it can be recognized accurately. It has the characteristics of being able to
第1図は従来の物体検知装置の検知方法を説明
する略線図、第2図は従来の他の物体検知装置の
検知方法を説明する斜視図、第3図は本発明の物
体検知装置の原理を説明するための光路図と光検
知器の系統図、第4図は本発明の具体的な構成を
示す光路系の斜視図と電気系の系統図である。
3,3A,3B……被測定物体、8……レーザ
源、9,9X,9Y……スキヤニングミラー、1
0,10a,10b……反射鏡、11……結像レ
ンズ、12……プリズムミラー、13a,13b
……光検出器、14……比較回路、20……コン
ピユータ。
FIG. 1 is a schematic diagram illustrating the detection method of a conventional object detection device, FIG. 2 is a perspective view illustrating the detection method of another conventional object detection device, and FIG. 3 is a diagram of the object detection device of the present invention. FIG. 4 is a perspective view of an optical path system and a system diagram of an electrical system showing a specific configuration of the present invention. 3, 3A, 3B...Object to be measured, 8...Laser source, 9, 9X, 9Y...Scanning mirror, 1
0, 10a, 10b... Reflecting mirror, 11... Imaging lens, 12... Prism mirror, 13a, 13b
...Photodetector, 14...Comparison circuit, 20...Computer.
Claims (1)
平面内で走査する第1の走査手段と、 該第1の走査手段で走査されたレーザ光ビーム
を前記平面とは直交する平面内で走査して、被測
定物体表面に照射する第2の走査手段と、 該被測定物体表面からその変位方向に延びた観
測線上に配置され、前記第2の走査手段を介して
導かれた前記被測定物体表面からの反射光を結像
させる結像手段と、 該結像手段による結像位置に配置され、該結像
位置にできた光像を2方向に分割する光分割手段
と、 該光分割手段で分割されたそれぞれの光を検出
する一対の光検出手段と、 該一対の光検出手段の検出結果に基づき、前記
被測定物体表面からの反射光が前記観測線上を通
るように前記第1および第2の走査手段の各走査
角度を制御する走査角度制御手段と、 該制御された各走査角度に基づき前記被測定物
体表面の位置を算出する位置算出手段とを備えた
ことを特徴とする物体検知装置。[Claims] 1. A light source that outputs a laser beam; a first scanning device that scans the laser beam output from the light source within one plane; and a device scanned by the first scanning device. a second scanning means for scanning a laser beam in a plane orthogonal to the plane and irradiating the surface of the object to be measured; an imaging means for forming an image of the reflected light from the surface of the object to be measured guided through a second scanning means; and an optical image formed at the imaging position, which is disposed at an imaging position by the imaging means. a light splitting means for splitting the light into two directions; a pair of light detection means for detecting the respective lights split by the light splitting means; and a light detection means for detecting the respective lights split by the light splitting means; scanning angle control means for controlling each scanning angle of the first and second scanning means so that the reflected light passes on the observation line; and controlling the position of the surface of the object to be measured based on the controlled scanning angles. An object detection device comprising: a position calculation means for calculating a position.
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP15502781A JPS5855804A (en) | 1981-09-30 | 1981-09-30 | Body detecting device |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP15502781A JPS5855804A (en) | 1981-09-30 | 1981-09-30 | Body detecting device |
Publications (2)
| Publication Number | Publication Date |
|---|---|
| JPS5855804A JPS5855804A (en) | 1983-04-02 |
| JPH0311401B2 true JPH0311401B2 (en) | 1991-02-15 |
Family
ID=15597059
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP15502781A Granted JPS5855804A (en) | 1981-09-30 | 1981-09-30 | Body detecting device |
Country Status (1)
| Country | Link |
|---|---|
| JP (1) | JPS5855804A (en) |
Families Citing this family (5)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| JPS60218008A (en) * | 1984-04-13 | 1985-10-31 | Toshiba Corp | Three-dimensional measuring instrument |
| DE3503086C1 (en) * | 1985-01-30 | 1986-06-19 | Dipl.-Ing. Bruno Richter GmbH & Co. Elektronische Betriebskontroll-Geräte KG, 8602 Stegaurach | Method and device for measuring the wall thickness of transparent objects |
| JPS61195307A (en) * | 1985-02-26 | 1986-08-29 | Nippon Steel Corp | Range finder |
| JPH0752104B2 (en) * | 1985-09-25 | 1995-06-05 | 松下電工株式会社 | Reflective photoelectric switch |
| JPH02276908A (en) * | 1989-04-18 | 1990-11-13 | Hamamatsu Photonics Kk | Three-dimensional position recognizing device |
Family Cites Families (2)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| JPS519623A (en) * | 1974-07-15 | 1976-01-26 | Matsushita Electric Industrial Co Ltd | Isobunrigatakaraasatsuzosochi |
| JPS5813890B2 (en) * | 1974-08-27 | 1983-03-16 | オリンパス光学工業株式会社 | Niji Genteki Hikari Henkousouchi |
-
1981
- 1981-09-30 JP JP15502781A patent/JPS5855804A/en active Granted
Also Published As
| Publication number | Publication date |
|---|---|
| JPS5855804A (en) | 1983-04-02 |
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