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JPS6248162B2 - - Google Patents
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JPS6248162B2 - - Google Patents

Info

Publication number
JPS6248162B2
JPS6248162B2 JP18766080A JP18766080A JPS6248162B2 JP S6248162 B2 JPS6248162 B2 JP S6248162B2 JP 18766080 A JP18766080 A JP 18766080A JP 18766080 A JP18766080 A JP 18766080A JP S6248162 B2 JPS6248162 B2 JP S6248162B2
Authority
JP
Japan
Prior art keywords
light
image
target object
photoelectric conversion
points
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
JP18766080A
Other languages
Japanese (ja)
Other versions
JPS57110908A (en
Inventor
Kazuo Tanie
Kyoshi Komorya
Tomoaki Nagasu
Akira Tate
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.)
National Institute of Advanced Industrial Science and Technology AIST
Original Assignee
Agency of Industrial Science and Technology
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 Agency of Industrial Science and Technology filed Critical Agency of Industrial Science and Technology
Priority to JP18766080A priority Critical patent/JPS57110908A/en
Publication of JPS57110908A publication Critical patent/JPS57110908A/en
Publication of JPS6248162B2 publication Critical patent/JPS6248162B2/ja
Granted legal-status Critical Current

Links

Classifications

    • GPHYSICS
    • G01MEASURING; TESTING
    • G01BMEASURING LENGTH, THICKNESS OR SIMILAR LINEAR DIMENSIONS; MEASURING ANGLES; MEASURING AREAS; MEASURING IRREGULARITIES OF SURFACES OR CONTOURS
    • G01B11/00Measuring arrangements characterised by the use of optical techniques
    • G01B11/24Measuring arrangements characterised by the use of optical techniques for measuring contours or curvatures

Landscapes

  • Physics & Mathematics (AREA)
  • General Physics & Mathematics (AREA)
  • Length Measuring Devices By Optical Means (AREA)
  • Measurement Of Optical Distance (AREA)

Description

【発明の詳細な説明】 本発明は、曲面形状を有する物体のある基準位
置からの等高位置を計測し、結果的にその物体の
形状を測定する方法に関するものである。
DETAILED DESCRIPTION OF THE INVENTION The present invention relates to a method of measuring the contour position of an object having a curved surface shape from a certain reference position and, as a result, measuring the shape of the object.

従来、モアレ縞を利用して立体形状を測定する
方法は知られているが、このモアレ方式では対象
物体の形状を等高線に相当する縞によつて表示で
きるとしても対象物体が凸または凹のいずれの方
向に変形しているのか不明であり、また縞が太く
なるとその中心位置が不明で精度のよい測定を行
うことができない。
Conventionally, a method for measuring three-dimensional shapes using moiré fringes is known, but in this moiré method, even if the shape of the target object can be displayed by stripes corresponding to contour lines, it is difficult to determine whether the target object is convex or concave. It is unclear whether the stripes are deforming in the direction of , and if the stripes become thick, the center position is unknown, making it impossible to perform accurate measurements.

本発明は、このような問題を解決した物体形状
の測定方法を提供しようとするものである。
The present invention aims to provide a method for measuring the shape of an object that solves these problems.

本発明の詳細な説明に先立ち、まず、第1図な
いし第3図を参照して本発明の基本的な測定原理
について説明する。
Prior to a detailed explanation of the present invention, first, the basic measurement principle of the present invention will be explained with reference to FIGS. 1 to 3.

第1図において、投影装置10はスリツト光
(スリツトは紙面に垂直)からなる投射光を対象
物体11に投影するもので、上記投射光が光軸と
交る回転中心、例えば投影レンズ等の中心点Pに
おいて回転し、そのときの回転量が点Pからl1
け離れた位置にある軸線L上において一定ピツチ
Δxの直線的移動で与えられるように構成する。
In FIG. 1, a projection device 10 projects a projection light consisting of a slit light (the slit is perpendicular to the plane of the drawing) onto a target object 11, and the projection light is a center of rotation where the projection light intersects with the optical axis, for example, the center of a projection lens, etc. It is configured so that it rotates at a point P, and the amount of rotation at that time is given by a linear movement of a constant pitch Δx on an axis L located at a distance l1 from the point P.

一方、ITVカメラ等からなる受光装置12は、
その光電変換面13を上記軸線L上に配置し、受
光レンズの中心点Qを上記投影レンズと同様に軸
線Lからl1だけ離れた位置に配置して、対象物体
11からの反射方向が光電変換素子で受光される
ように構成する。
On the other hand, the light receiving device 12 consisting of an ITV camera etc.
The photoelectric conversion surface 13 is arranged on the axis L, and the center point Q of the light receiving lens is arranged at a distance l1 from the axis L, like the projection lens, so that the direction of reflection from the target object 11 is The configuration is such that the light is received by the conversion element.

このような構成を有する装置において、軸線L
上の点P1を通る投射光を点Pを通して対象物体1
1に投影したとすると、対象物体上の点A1でそ
の投射光が反射し、点Qを通つて光電変換面上の
点Q1にその像が得られる。また、投射光を点P
において回転させ、点P2から点Pを通して対象物
体11に投射したとすると、その投射光は対象物
体11上の点A2で反射して光電変換面上の点Q2
に結像する。
In a device having such a configuration, the axis L
Projection light that passes through point P 1 above passes through point P to target object 1
1, the projected light is reflected at point A 1 on the target object, passes through point Q, and its image is obtained at point Q 1 on the photoelectric conversion surface. In addition, the projection light is
Suppose that the projected light is rotated at , and projected onto the target object 11 from point P 2 through point P, the projected light will be reflected at point A 2 on target object 11 and will be reflected at point Q 2 on the photoelectric conversion surface.
image is formed.

ここで、対象物体11上の点A1,A2が上記点
P,Qを結ぶ直線から距離l2だけ離れた等高面上
にあるとすると、 P1P2:A1A2=Q1Q2:A1A2=l1:l2 であるため、 P1P2=Q1Q2 となり、即ち点P1,P2から発した投射光がそれぞ
れ対象物体の等高位置(PQを通り、紙面に垂直
な平面から等距離にある点)で反射して光電変換
面上に像をつくるとき、その像間の間隔Q1Q2
必ずP1P2の長さに等しくなる。逆に、点P1,P2
ら発した投射光がP1P2と等しい間隔で結像しない
ときには、それらの点が等高面上に存在しないこ
とになる。
Here, if the points A 1 and A 2 on the target object 11 are on a contour plane that is a distance l 2 away from the straight line connecting the points P and Q, then P 1 P 2 :A 1 A 2 =Q 1 Q 2 : A 1 A 2 = l 1 : l 2 , so P 1 P 2 = Q 1 Q 2 , that is, the projected light emitted from points P 1 and P 2 is at the same height position of the target object ( When an image is created on the photoelectric conversion surface by passing through PQ and reflecting at a point equidistant from a plane perpendicular to the plane of the paper, the distance between the images Q 1 Q 2 is always equal to the length of P 1 P 2 Become. Conversely, when the projection lights emitted from points P 1 and P 2 do not form images at equal intervals to P 1 P 2 , those points do not exist on the contour plane.

従つて、上記軸線L上において投影装置を回転
させるためのある一定のピツチΔxの直線的移動
を与えて、点P1,P2,……からのスリツト光を順
次対象物体11上に投射し、その反射光を受光装
置12の光電変換面に結像させると、第2図に示
すように、光電変換面13上において対象物体の
表面の凹凸に応じて湾曲した像I1,I2,……が得
られ、これらの像I1,I2,……と、前記投影装置
を回転させるためのピツチΔxに相応する間隔を
もつた走査線L1,L2との交点a1,a2,……,b1
b2,……を求めれば、それらの点群がすべて同一
の等高面上にあり、その接続によつて等高線を得
ることができる。さらに具体的に説明すると、ま
ず、最初のスリツト光で光電変換面上に変形像I1
を得たとき、光電変換面を走査して走査線L1
スリツト光の像I1との交点a1,b1を求め、次にス
リツト光を一定ピツチΔxだけ移動させて変形像
I2を得たときに光電変換面を走査して上記走査線
L1と一定ピツチだけ離れた走査線L2との交点a2
b2を求め、以下同様にして順次交点a3,b3,a4
b4,……を求めることにより、等高面上の点群を
得ることができる。
Therefore, the slit light from points P 1 , P 2 , . When the reflected light is imaged on the photoelectric conversion surface of the light receiving device 12, as shown in FIG. 2, images I 1 , I 2 , ... are obtained, and the intersection points a 1 , a of these images I 1 , I 2 , ... and scanning lines L 1 , L 2 having an interval corresponding to the pitch Δx for rotating the projection device 2 ,..., b1 ,
If we find b 2 ,..., all of these points are on the same contour surface, and by connecting them we can obtain contour lines. To explain more specifically, first, the first slit light creates a deformed image I 1 on the photoelectric conversion surface.
When the photoelectric conversion surface is obtained, the intersection points a 1 and b 1 of the scanning line L 1 and the image I 1 of the slit light are obtained by scanning the photoelectric conversion surface, and then the slit light is moved by a fixed pitch Δx to obtain the deformed image.
When I2 is obtained, the photoelectric conversion surface is scanned and the above scanning line is
Intersection point a 2 between L 1 and scanning line L 2 separated by a certain pitch,
Find b 2 , and then in the same way, sequentially find the intersections a 3 , b 3 , a 4 ,
By finding b 4 ,..., we can obtain a group of points on the contour surface.

また、上記スリツト光の像I1,I2,……と走査
線L1,L2,……の対応関係を変化させれば、第
3図から明らかなように、異なる等高面上の点群
を求めることができる。即ち、第3図において、
等高面S1上の点群A1,A2,A3,……は、点P1
P2……を通るスリツト光の像と走査線L1,,L2
……とのそれぞれの交点として得ることができ、
また等高面S2上の点群B1,B2,B3,……は点
P1,P2,……を通るスリツト光の像と走査線
L2,L3,……とのそれぞれの交点として、さら
に等高面S3上の点群C1,C2,C3,……は点P1
P2,……を通るスリツト光の像と走査線L3
L4,……とのそれぞれの交点として得ることが
できる。従つて、これらの多数の等高面上の点群
を求めて重畳することにより対象物体の形状を評
価することが可能となる。
Furthermore, if the correspondence between the slit light images I 1 , I 2 , . . . and the scanning lines L 1 , L 2 , . . . is changed, as is clear from FIG. Point clouds can be found. That is, in FIG.
The point group A 1 , A 2 , A 3 , ... on the contour surface S 1 is the point P 1 ,
Image of slit light passing through P 2 ... and scanning lines L 1 , , L 2 ,
It can be obtained as the respective intersections with...
Also, the point group B 1 , B 2 , B 3 , ... on the contour surface S 2 is a point
Image and scanning line of slit light passing through P 1 , P 2 , ...
As the respective intersections with L 2 , L 3 , ..., the point group C 1 , C 2 , C 3 , ... on the contour surface S 3 is the point P 1 ,
Image of slit light passing through P 2 , ... and scanning line L 3 ,
It can be obtained as the respective intersections with L 4 ,... Therefore, by finding and superimposing a group of points on a large number of these contour planes, it is possible to evaluate the shape of the target object.

本発明は、このような原理を用いて対象物体上
における等高位置を求めようとするものであり、
前記モアレ方式に比して対象物体が凸または凹の
いずれの方向に変形しているのかを明確にした形
状測定を行うことができ、またスリツト光の像に
ついての細線化処理が容易であるため、高精度の
形状測定を行うことができるものである。
The present invention attempts to find a contour position on a target object using such a principle,
Compared to the moiré method, it is possible to perform shape measurement that clearly determines whether the object is deformed in a convex or concave direction, and it is easier to thin the image of the slit light. , it is possible to perform highly accurate shape measurement.

即ち、本発明の測定方法は、光軸と交る回転中
心において回転可能な投影装置から対象物体に対
して上記回転方向と直交するスリツト光またはそ
の方向に振れるレーザ光を投射し、その反射光を
受光装置の光電変換面に結像させ、上記投影装置
をその回転の中心点から離れた位置にある軸線上
において一定のピツチの直線的移動を与えるよう
に回転させ、各回転位置において上記光電変換面
に得られる反射光のスリツト像またはスポツト光
の像の軌跡と上記ピツチに相応する間隔をもつた
直線との交点として、対象物体における等高面上
の点群を検出し、これに基づいて物体形状を測定
することを特徴とするものである。
That is, in the measurement method of the present invention, a slit beam or a laser beam swinging in the direction perpendicular to the rotation direction is projected onto the target object from a projection device that is rotatable at a rotation center that intersects with the optical axis, and the reflected light is is imaged on the photoelectric conversion surface of the light receiving device, and the projecting device is rotated so as to give a linear movement of a constant pitch on an axis located away from the center of rotation, and the photoelectric conversion surface is focused at each rotational position. A group of points on the contour plane of the target object is detected as the intersection of the locus of the slit image of the reflected light or the image of the spot light obtained on the conversion surface and a straight line with an interval corresponding to the pitch, and based on this, This method is characterized by measuring the shape of an object.

さらに具体的に説明すると、第4図は投影装置
10によつてスリツト光を投射する場合を示し、
また第5図及び第6図は投影装置によつてレーザ
光を投射する場合を示している。
To explain more specifically, FIG. 4 shows a case where slit light is projected by the projection device 10,
Further, FIGS. 5 and 6 show the case where a laser beam is projected by a projection device.

第4図の測定装置における投影装置10は、基
台20上に図示しないモータによつて回転駆動さ
れる回転台21を備え、この回転台21上に、そ
の中心点Pにスリツト23を配置したスリツト光
の投光器22を固定し、光源24からの光を光学
系25及び上記スリツト23により上記回転方向
と直交する方向即ち紙面に垂直な方向に長い断面
をもつたスリツト光として投射できるように構成
している。この投影装置10の回転位置は、その
突杆部26の溝27にガイド28内を直線的に摺
動する摺動子29上のピン30を摺動自在に嵌入
し、上記摺動子29に位置サーボ系を構成する位
置検出器31を連結して計測するものである。
The projection device 10 in the measuring device shown in FIG. 4 includes a rotating table 21 on a base 20 which is rotationally driven by a motor (not shown), and a slit 23 is arranged on the rotating table 21 at its center point P. The slit light projector 22 is fixed, and the light from the light source 24 is projected by the optical system 25 and the slit 23 as a slit light having a long cross section in a direction perpendicular to the rotational direction, that is, a direction perpendicular to the plane of the paper. are doing. The rotational position of the projection device 10 is determined by slidably fitting the pin 30 on the slider 29 that linearly slides within the guide 28 into the groove 27 of the protrusion 26. Measurement is performed by connecting position detectors 31 that constitute a position servo system.

一方、上記基台20にはITVカメラからなる受
光装置12を、その光電変換面33が摺動子29
の中心軸上に位置するように配設し、そのビデイ
オ信号がインターフエースを介して電子計算機に
入力されるように構成している。なお、以上にお
いては受光装置の光電変換面33を摺動子29の
中心軸線上に位置させる旨の説明をしているが、
必要な係数を用いることにより上記光電変換面3
3の位置を任意に設定することができる。
On the other hand, the light receiving device 12 consisting of an ITV camera is mounted on the base 20, and its photoelectric conversion surface 33 is attached to the slider 29.
The video signal is input to the electronic computer via the interface. In addition, although the above explanation is that the photoelectric conversion surface 33 of the light receiving device is positioned on the central axis of the slider 29,
By using necessary coefficients, the photoelectric conversion surface 3
The position of 3 can be set arbitrarily.

上記構成を有する装置においては、回転台21
を所要の位置にセツトして投光器22によりスリ
ツト光を対象物体11に投射し、その反射光を受
光装置12によつて受光するが、この受光装置に
おいては、光電変換面33を256×256程度の画素
に分割し、また各画素の明暗信号を6ビツト程度
にAD変換し、スリツト光の像をデイジタル画像
として電子計算機のメモリに格納する。これらの
操作が終了した後、電子計算機による制御で回転
台21を位置検出器31がΔxだけ移動するまで
回転させる。この回転は、回転台のモータと位置
検出器31からなる位置サーボ系によつて制御さ
れる。その後、再びスリツト光の像を受光装置で
とらえ、それをデイジタル画像として電子計算機
のメモリに格納し、これを必要回数にわたつて繰
返した後に、各フレームのデイジタル画像を空間
微分することにより、得られたスリツト像の細線
化処理を行い、そのスリツト像を適当な関数式
f1,f2,……で近似する。以後は、上記スリツト
像の関数式で表わされた曲線群と、回転台21を
回転させる場合の摺動子29のピツチΔxと同一
間隔をもつ直線群との交点をそれぞれ求めること
により、等高面上に位置する点群を得ることがで
き、これによつて前述の如く対象物体の形状を測
定することができる。
In the apparatus having the above configuration, the rotary table 21
is set at a required position, the projector 22 projects the slit light onto the target object 11, and the reflected light is received by the light receiver 12. In this light receiver, the photoelectric conversion surface 33 is approximately 256 x 256 pixels. The light and dark signals of each pixel are AD converted into about 6 bits, and the image of the slit light is stored in the memory of an electronic computer as a digital image. After these operations are completed, the rotating table 21 is rotated under the control of an electronic computer until the position detector 31 moves by Δx. This rotation is controlled by a position servo system consisting of a rotary table motor and a position detector 31. After that, the image of the slit light is again captured by the light receiving device, stored as a digital image in the memory of the electronic computer, and after repeating this as many times as necessary, the digital image of each frame is spatially differentiated. The resulting slit image is thinned, and the slit image is converted into a suitable functional formula.
Approximate by f 1 , f 2 , ... From now on, by finding the intersections of the curve group expressed by the above-mentioned functional formula of the slit image and the straight line group having the same interval as the pitch Δx of the slider 29 when rotating the rotary table 21, the equation is calculated. A cloud of points located on a high surface can be obtained, by means of which the shape of the object can be measured as described above.

第5図に示す測定装置は、レーザ光を投射する
もので、基本的には第4図の装置と共に共通性を
有しているが、レーザ光がスポツト光として投射
されるので、それをスリツト光と等価なものに変
換するための手段を有している。即ち、第5図の
測定装置における投影装置10は、第6図に詳細
に示すように、機枠40上にミラー41を回転さ
せる回転軸42を水平に支持させ、この回転軸4
2を駆動用モータ43によつて回転させると共
に、その回転軸42に取付けた回転角度検出器4
4によつてミラー41の回転角度を検出できるよ
うにして、それらによりサーボ系を構成させ、ま
た機枠40上に上記ミラー41の中心に向つてレ
ーザ光を投射するレーザ光源45を固定し、その
軸線が投影装置の回転台21(第5図)の中心点
Pと一致するようにして上記機枠40を回転台2
1上に固定している。
The measuring device shown in Fig. 5 projects a laser beam, and is basically similar to the device shown in Fig. 4, but since the laser beam is projected as a spot beam, it can be used as a slit. It has a means to convert it into something equivalent to light. That is, as shown in detail in FIG. 6, the projection device 10 in the measuring device shown in FIG.
2 is rotated by a drive motor 43, and a rotation angle detector 4 is attached to the rotation shaft 42.
4 to be able to detect the rotation angle of the mirror 41 and constitute a servo system, and a laser light source 45 that projects a laser beam toward the center of the mirror 41 is fixed on the machine frame 40. The machine frame 40 is moved to the rotary base 21 so that its axis coincides with the center point P of the rotary base 21 (FIG. 5) of the projection device.
It is fixed at 1.

一方、基台20において対象物体11からの反
射光を検出する受光装置12としては、セルスポ
ツトの商品名で市販されている半導体位置検出器
を使用している。この検出器は、光電変換面46
において受光したスポツト光の図心の座標に相当
する信号を出力する半導体位置検出器で、x座標
検出用AD変換器及びy座標検出用AD変換器、並
びにインターフエースを介して電子計算機に接続
している。
On the other hand, as the light receiving device 12 for detecting the reflected light from the target object 11 on the base 20, a semiconductor position detector commercially available under the trade name Cell Spot is used. This detector has a photoelectric conversion surface 46
A semiconductor position detector that outputs a signal corresponding to the coordinates of the centroid of the spot light received by ing.

なお、その他の構成は第4図の場合と同様であ
る。
Note that the other configurations are the same as in the case of FIG. 4.

この測定装置による測定に際しては、まず、電
子計算機の制御により回転台21を適当な初期位
置にセツトし、この状態でミラー41を上から下
へ回転させる。電子計算機は、インタフエースを
介してミラー41のサーボ系へミラー回転信号を
出力すると同時に、ミラーの各回転位置における
受光装置12からのスポツトの像の座標を逐次メ
モリへ格納する。その後、回転台21を電子計算
機による制御で位置検出器31において一定ピツ
チΔxだけ移動させることにより回転させて、同
様の操作を行い、回転台の各回転位置に対してそ
れを繰返す。而して、各回転位置において光電変
換面46に得られる反射光の像の軌跡について、
第4図で説明した場合と同様の関数式による近似
を行い、上記軌跡と上記一定ピツチΔxに相応す
る間隔をもつた直線群との交点を求めることによ
り、対象物体の等高面上に位置する点群を得るこ
とができ、これに基づいて対象物体の形状を測定
することが可能となる。
When performing measurements using this measuring device, first, the rotary table 21 is set at an appropriate initial position under the control of an electronic computer, and the mirror 41 is rotated from top to bottom in this state. The electronic computer outputs a mirror rotation signal to the servo system of the mirror 41 via the interface, and at the same time sequentially stores the coordinates of the image of the spot from the light receiving device 12 at each rotational position of the mirror in the memory. Thereafter, the rotary table 21 is rotated by moving the rotary table 21 by a fixed pitch Δx using the position detector 31 under the control of an electronic computer, and the same operation is performed, which is repeated for each rotational position of the rotary table. Therefore, regarding the locus of the image of the reflected light obtained on the photoelectric conversion surface 46 at each rotational position,
By performing approximation using the same functional formula as explained in Fig. 4 and finding the intersection of the above trajectory and a group of straight lines with an interval corresponding to the above constant pitch Δx, the position on the contour plane of the target object is determined. It is possible to obtain a point group based on which the shape of the target object can be measured.

以上に詳述したところから明らかなように、本
発明の測定方法は、一般に利用されている三角測
量等の原理に基づくことなく、本発明に特有の原
理に基づいている。即ち、本発明は、スリツト光
をその回転の中心点から離れた位置にある軸線上
において一定のピツチの直線的移動を与えること
により回転させながら、対象物体を照射し、その
各位置において反射光の像を光電変換面に結像さ
せれば、その像は直線あるいは曲線となるが、そ
の像を構成する各点のうち、上記ピツチに対応し
た間隔の直線上に存する点は、上記物体における
等高点から反射した光であるという原理に基づい
て構成されたものであり、そのため、投射スリツ
ト光を回転させる場合の上記直線的移動のピツチ
のみを一定に保つだけでよく、スリツト光が投射
された後に物体で反射して戻つてくるまでの光の
経路の角度を測定したり、各機器や対象物体の反
射点間の距離等を測る必要はなく、それにより構
成を著しく簡単なものとして、対象物件の形状
を、それが凸または凹のいずれの方向に変形して
いるのかを含めて、正確かつ簡単に測定すること
ができる。
As is clear from the above detailed description, the measuring method of the present invention is not based on the generally used principle of triangulation, but is based on a principle unique to the present invention. That is, in the present invention, the target object is irradiated while rotating the slit light by giving a linear movement of a constant pitch on the axis located at a position away from the center of rotation, and the reflected light is reflected at each position. If an image of It is constructed based on the principle that the light is reflected from a contour point, and therefore, when rotating the projection slit light, it is only necessary to keep the pitch of the above linear movement constant, and the slit light is There is no need to measure the angle of the path of the light until it is reflected by an object and returns, or to measure the distance between the reflection points of each device or target object, which greatly simplifies the configuration. , it is possible to accurately and easily measure the shape of a target object, including whether it is deformed in a convex or concave direction.

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

第1図ないし第3図は本発明における測定原理
についての説明図、第4図及び第5図は本発明の
異なる装置例の構成図、第6図は第5図の投影装
置の構成を示す斜視図である。 10……投影装置、11……対象物体、12…
…受光装置、13,33,46……光電変換面。
FIGS. 1 to 3 are explanatory diagrams of the measurement principle in the present invention, FIGS. 4 and 5 are configuration diagrams of different apparatus examples of the present invention, and FIG. 6 is a configuration of the projection apparatus of FIG. 5. FIG. 10... Projection device, 11... Target object, 12...
...Light receiving device, 13, 33, 46...Photoelectric conversion surface.

Claims (1)

【特許請求の範囲】 1 光軸と交る回転中心において回転可能な投影
装置から対象物体に対して上記回転方向と直交す
るスリツト光からなる投射光を投射し、その反射
光を受光装置の光電変換面に結像させ、上記投影
装置をその回転の中心点から離れた位置にある軸
線上において一定のピツチの直線的移動を与える
ように回転させ、各回転位置において上記光電変
換面に得られる反射光の像と上記ピツチに相応す
る間隔をもつた直線との交点として、対象物体に
おける等高面上の点群を検出し、これに基づいて
物体形状を測定することを特徴とする物体形状の
測定方法。 2 光軸と交る回転中心において回転可能な投影
装置から対象物体に対して上記回転方向と直交す
る方向に振れるレーザ光を投射し、その反射光を
受光装置の光電変換面に結像させ、上記投影装置
をその回転の中心点から離れた位置にある軸線上
において一定のピツチの直線的移動を与えるよう
に回転させ、各回転位置において上記光電変換面
に得られる反射光の像の軌跡と上記ピツチに相応
する間隔をもつた直線との交点として、対象物体
における等高面上の点群を検出し、これに基づい
て物体形状を測定することを特徴とする物体形状
の測定方法。
[Scope of Claims] 1 Projection light consisting of slit light perpendicular to the rotational direction is projected onto a target object from a projection device that is rotatable at a rotation center that intersects with the optical axis, and the reflected light is transmitted to a photodetector of a light receiving device. An image is formed on the photoelectric conversion surface, and the projection device is rotated so as to give a linear movement of a constant pitch on an axis located away from the center of rotation, and an image is obtained on the photoelectric conversion surface at each rotational position. An object shape characterized in that a group of points on a contour plane of a target object is detected as the intersection of an image of reflected light and a straight line having an interval corresponding to the pitch, and the object shape is measured based on this. How to measure. 2. Projecting a laser beam that swings in a direction perpendicular to the rotational direction onto the target object from a rotatable projection device at a rotation center that intersects with the optical axis, and focusing the reflected light on a photoelectric conversion surface of a light receiving device, The projection device is rotated so as to give a linear movement of a constant pitch on an axis located away from the center of rotation, and the locus of the image of the reflected light obtained on the photoelectric conversion surface at each rotational position is A method for measuring the shape of an object, characterized in that a group of points on a contour plane of the target object are detected as points of intersection with a straight line having an interval corresponding to the pitch, and the shape of the object is measured based on the detected points.
JP18766080A 1980-12-27 1980-12-27 Measuring method for shape of object Granted JPS57110908A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP18766080A JPS57110908A (en) 1980-12-27 1980-12-27 Measuring method for shape of object

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP18766080A JPS57110908A (en) 1980-12-27 1980-12-27 Measuring method for shape of object

Publications (2)

Publication Number Publication Date
JPS57110908A JPS57110908A (en) 1982-07-10
JPS6248162B2 true JPS6248162B2 (en) 1987-10-13

Family

ID=16209950

Family Applications (1)

Application Number Title Priority Date Filing Date
JP18766080A Granted JPS57110908A (en) 1980-12-27 1980-12-27 Measuring method for shape of object

Country Status (1)

Country Link
JP (1) JPS57110908A (en)

Families Citing this family (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS60152909A (en) * 1984-01-21 1985-08-12 Sanwa Seiki Kk Non-contact type three-dimensional measuring instrument
DE10212364A1 (en) * 2002-03-20 2003-10-16 Steinbichler Optotechnik Gmbh Method and device for determining the absolute coordinates of an object

Also Published As

Publication number Publication date
JPS57110908A (en) 1982-07-10

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