JPH06258022A - Measuring method of hole position - Google Patents

Measuring method of hole position

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Publication number
JPH06258022A
JPH06258022A JP4294993A JP4294993A JPH06258022A JP H06258022 A JPH06258022 A JP H06258022A JP 4294993 A JP4294993 A JP 4294993A JP 4294993 A JP4294993 A JP 4294993A JP H06258022 A JPH06258022 A JP H06258022A
Authority
JP
Japan
Prior art keywords
circular hole
slit light
end point
point
hole
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.)
Pending
Application number
JP4294993A
Other languages
Japanese (ja)
Inventor
Naoji Yamaoka
直次 山岡
Koji Oda
幸治 小田
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.)
Honda Motor Co Ltd
Original Assignee
Honda Motor 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 Honda Motor Co Ltd filed Critical Honda Motor Co Ltd
Priority to JP4294993A priority Critical patent/JPH06258022A/en
Publication of JPH06258022A publication Critical patent/JPH06258022A/en
Pending legal-status Critical Current

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  • Length Measuring Devices By Optical Means (AREA)

Abstract

PURPOSE:To allow highly accurate measurement of the central position of a circular hole made in a work. CONSTITUTION:The surface of a work W is irradiated with horizontal and vertical slit lights 101, 102 projected from light sources 11, 12 while traversing a circular hole Wa and the image thereof is picked up by means of cameras 21, 22. Optical axis of one slit light 101 is inclined significantly so that the slit light 10, does not impinge on the inner peripheral face of the hole on the side of point A thus preventing the point A from shifting from the edge of the circular hole Wa due to the slit light image of the inner peripheral face of the hole. Two circles having a predetermined diameter corresponding to that of the hole Wa are drawn, while passing through points A, C and point A, D, on a plane including the point A and two end points C, D of the irradiating image of the slit light 102 and the intermediate point between the centers of both circles is determined as the central position of the circular hole.

Description

【発明の詳細な説明】Detailed Description of the Invention

【0001】[0001]

【産業上の利用分野】本発明は、ワークに形成した円形
孔の中心位置を光学的に測定する孔位置の測定方法に関
する。
BACKGROUND OF THE INVENTION 1. Field of the Invention The present invention relates to a hole position measuring method for optically measuring the center position of a circular hole formed in a work.

【0002】[0002]

【従来の技術】従来、この種の測定方法として、特開平
3−160303号公報により、図5に示す如く、ワー
クWの表面に円形孔Waを横切る互いに交差する2つの
スリット光a、bを照射し、これらスリット光の照射像
を両スリット光の光面に斜交する光軸を持つ1台のカメ
ラcで撮像し、円形孔Waの孔縁に合致する、一方のス
リット光aの照射像の2つの端点a1、a2と、他方の
スリット光bの照射像の2つの端点b1、b2との位置
を検出し、a1とa2の結線の垂直2等分線とb1とb
2の結線の垂直2等分線との交点として円形孔Waの中
心位置を割出すようにしたものが知られている。ここ
で、各スリット光a、bは何れもカメラcの視線に斜交
するため、各スリット光の照射像は光切断像となり、カ
メラの画面上の各端点の位置から光切断の解析法に基づ
いて各端点の空間座標値を算定することができ、従って
円形孔Waの空間座標系における中心位置を求めること
ができる。
2. Description of the Related Art Conventionally, as a measuring method of this kind, according to Japanese Patent Laid-Open No. 3-160303, as shown in FIG. 5, two slit lights a and b intersecting each other across a circular hole Wa are formed on the surface of a work W. Irradiation, and the irradiation image of these slit lights is picked up by one camera c having an optical axis oblique to the optical surfaces of both slit lights, and irradiation of one slit light a that matches the edge of the circular hole Wa. The positions of the two end points a1 and a2 of the image and the two end points b1 and b2 of the irradiation image of the other slit light b are detected, and the perpendicular bisector of the connection line between a1 and a2 and b1 and b2.
It is known that the center position of the circular hole Wa is indexed as the intersection of the two connections with the perpendicular bisector. Here, since each of the slit lights a and b obliquely intersects the line of sight of the camera c, the irradiation image of each slit light becomes a light-section image, and the analysis method of light-section is performed from the position of each end point on the screen of the camera. Based on this, the spatial coordinate value of each end point can be calculated, and thus the center position of the circular hole Wa in the spatial coordinate system can be obtained.

【0003】[0003]

【発明が解決しようとする課題】ところで、円形孔Wa
がカメラcに正対する位置からずれると、ずれ方向の孔
内周面に照射されたスリット光の像も撮像され、例えば
端点a1がカメラcの視線から離れる方向にずれると、
カメラcの画面上で端点a1がワークの板厚分だけ内側
にずれ、その結果円形孔Waの中心位置の測定誤差を生
ずる。本発明は、以上の点に鑑み、円形孔の中心位置を
より正確に測定し得るようにした方法を提供することを
その目的としている。
By the way, the circular hole Wa
When is displaced from the position directly facing the camera c, an image of the slit light irradiated on the inner peripheral surface of the hole in the displacement direction is also captured. For example, when the end point a1 is displaced from the line of sight of the camera c,
On the screen of the camera c, the end point a1 shifts inward by the plate thickness of the work, resulting in a measurement error of the center position of the circular hole Wa. In view of the above points, an object of the present invention is to provide a method capable of more accurately measuring the center position of a circular hole.

【0004】[0004]

【課題を解決するための手段】上記目的を達成すべく、
本発明は、ワークに形成した円形孔の中心位置を光学的
に測定する方法であって、ワークの表面に円形孔を横切
る互いに交差する第1と第2の2つのスリット光を照射
し、これらスリット光の照射像を撮像手段で撮像して、
円形孔の孔縁に合致する各照射像の端点の位置を検出
し、これら端点の位置から円形孔の中心位置を割出すも
のにおいて、前記両スリット光の一方の第1スリット光
を、円形孔の予測される最大限のずれを生じても第1ス
リット光の照射像の2つの端点のうちの一方の第1端点
側の円形孔の内周面に第1スリット光が当たらないよう
に、ワークの表面に照射し、この第1端点と第2スリッ
ト光の照射像の2つの端点のうちの一方の第2端点と他
方の第3端点との空間座標値を撮像手段の画面上の該各
端点の位置から算定し、空間座標系におけるこれら3つ
の端点を含む平面上に描かれる、円形孔の孔径に対応す
る所定径の円であって、第1端点と第2端点とを通る円
の中心座標値と、第1端点と第3端点とを通る円の中心
座標値とを算出し、これら両円の中心の中点を円形孔の
中心位置として求めることを特徴とする。
[Means for Solving the Problems] In order to achieve the above object,
The present invention is a method for optically measuring the center position of a circular hole formed in a work, which comprises irradiating the surface of the work with two slit light beams, a first slit light beam and a second slit light beam that intersect each other across the circular hole. The irradiation image of the slit light is taken by the imaging means,
In the one in which the position of the end point of each irradiation image that matches the hole edge of the circular hole is detected and the center position of the circular hole is indexed from the position of these end points, one of the first slit light of the both slit light is a circular hole. Even if the predicted maximum deviation of the first slit light is generated, the first slit light does not hit the inner peripheral surface of the circular hole on the side of one of the two end points of the irradiation image of the first slit light, The surface of the work is irradiated, and the spatial coordinate values of the first end point and the second end point of one of the two end points of the irradiation image of the second slit light and the third end point of the other end point are displayed on the screen of the imaging means. A circle that is calculated from the position of each end point and that is drawn on a plane including these three end points in the spatial coordinate system and has a predetermined diameter corresponding to the hole diameter of the circular hole and that passes through the first end point and the second end point. And a center coordinate value of a circle passing through the first end point and the third end point, And obtaining the middle point of the center of these two circles centered position of the circular hole.

【0005】[0005]

【作用】第1スリット光の照射像の一方の端点たる第1
端点側の孔内周面には第1スリット光が当たらないた
め、第1端点の位置は正確に検出できるが、第1スリッ
ト光の照射像の他方の端点側の孔内周面には第1スリッ
ト光が当たるため、該他方の端点の位置は正確に検出で
きなくなり、そこで第1端点と第2スリット光の照射像
の第2と第3の2つの端点との計3つの端点の位置から
円形孔の中心位置を求めるようにしている。この場合、
これら3つの端点を含む空間座標系における平面上に描
かれる、これら3つの端点を通る円の方程式を求めて、
この円の中心座標を円形孔の中心位置とすることも考え
られるが、第2と第3の端点の位置には多少とも誤差が
含まれる可能性があり、この誤差により3つの端点を通
る円の径が円形孔の孔径に対し大きな差を生じて、円の
中心が実際の円形孔の中心から大きくずれてしまうこと
がある。これに対し、本発明で描かれる2つの円の径は
円形孔の孔径に対応する値に予め規定されており、且つ
両円が何れも正確度の高い第1端点を通るため、両円の
中心の中点は円形孔の中心から左程ずれることはなく、
円形孔の中心位置を精度良く測定できる。
[Function] The first slit which is one of the end points of the irradiation image of the first slit light
Since the first slit light does not impinge on the hole inner peripheral surface on the end point side, the position of the first end point can be accurately detected, but the hole inner peripheral surface on the other end point side of the irradiation image of the first slit light does not have the first slit light. Since one slit light hits, the position of the other end point cannot be accurately detected, and therefore the positions of the first end point and the second and third end points of the irradiation image of the second slit light, the total of three end points. The center position of the circular hole is obtained from. in this case,
Obtaining the equation of a circle drawn on a plane in a spatial coordinate system including these three end points and passing through these three end points,
Although it is conceivable to use the center coordinates of this circle as the center position of the circular hole, there may be some error in the positions of the second and third end points, and due to this error, the circle passing through the three end points The diameter of the circle may greatly differ from the diameter of the circular hole, and the center of the circle may deviate from the actual center of the circular hole. On the other hand, the diameters of the two circles drawn in the present invention are preliminarily set to values corresponding to the hole diameters of the circular holes, and both circles pass through the highly accurate first end point. The middle point of the center does not shift to the left from the center of the circular hole,
The center position of the circular hole can be accurately measured.

【0006】[0006]

【実施例】図1はワークWに形成した円形孔Waの位置
を測定する装置の概要を示しており、該装置は、第1と
第2の1対のスリット光源11、12と、第1と第2の1
対のカメラ21、22と、該両カメラ21、22からの画像
信号を入力するコンピュータ3とで構成されている。ス
リット光源11、12とカメラ21、22はロボット等の動
作端に取付けられる図示しない支持枠に所要の位置関係
で搭載され、ワークWに対向する所定の測定位置に移動
セットされる。
FIG. 1 shows an outline of an apparatus for measuring the position of a circular hole Wa formed in a work W. The apparatus comprises a pair of first and second slit light sources 1 1 , 1 2 . First and second one
It is composed of a pair of cameras 2 1 and 2 2 and a computer 3 which inputs image signals from the cameras 2 1 and 2 2 . The slit light sources 1 1 and 1 2 and the cameras 2 1 and 2 2 are mounted on a support frame (not shown) attached to the operating end of a robot or the like in a required positional relationship, and are moved and set to a predetermined measurement position facing the work W. .

【0007】第1スリット光源11は水平な第1スリッ
ト光101を照射するように構成され、また、第2スリ
ット光源12は垂直な第2スリット光102を照射するよ
うに構成されており、ワークWの表面に円形孔Waを横
切るように照射された各スリット光101、102の線状
の照射像を前記両カメラ21、22で撮像する。第1スリ
ット光101の照射像には円形孔Waの孔縁に合致する
左右2つの端点A、Bが現われ、また、第2スリット光
102の照射像にも円形孔Waの孔縁に合致する上下2
つの端点C、Dが現われる。
The first slit light source 1 1 is configured to emit the horizontal first slit light 10 1 , and the second slit light source 1 2 is configured to emit the vertical second slit light 10 2. Accordingly, the linear irradiation images of the slit lights 10 1 , 10 2 which are irradiated on the surface of the work W so as to traverse the circular hole Wa are captured by the both cameras 2 1 , 2 2 . Two left and right end points A and B that match the hole edge of the circular hole Wa appear in the irradiation image of the first slit light 10 1 , and also in the irradiation edge of the circular hole Wa in the irradiation image of the second slit light 10 2. Up and down 2
Two endpoints C and D appear.

【0008】両カメラ21、22は、夫々の光軸01、02
が第1スリット光101の光面に合致する水平面上で図
2に示す如く斜交するように配置されており、該水平面
上にとった第2スリット光102の光軸方向の水平座標
軸をX軸、これに直交する水平座標軸をZ軸、該水平面
に直交する垂直座標軸をY軸、光軸01、02の交点を原
点0とする空間座標系における前記各端点の座標値を両
カメラ21、22の画面上における該各端点の位置から三
角測量法の原理で算定するようにした。図2の状態にお
ける第1カメラ21と第2カメラ22の画面は夫々図3
(a)と同図(b)に示す通りになり、画面上に前記原
点0に対応する中心点を原点として水平のx軸と垂直の
y軸をとると、画面のx軸座標値とy軸座標値は空間座
標系における各カメラ21、22の投影面Q1、Q2上での
原点0からの水平距離と垂直距離を表わすことになる。
例えば前記A点を考えると、第1カメラ21の投影面Q1
へのA点の投影点A1の原点0からの水平距離は第1カ
メラ21の画面上のA点のx軸座標値x1となり、同様に
第2カメラ22の投影面Q2へのA点の投影点A2の原点
0からの水平距離は第2カメラ22の画面上のA点のx
軸座標値x2となる。そして、第1カメラ21からA1
引いた視線e1の方程式をx1から求めると共に、第2カ
メラ22からA2に引いた視線e2の方程式をx2から求
め、両視線の交点として空間座標系におけるA点のX軸
座標値とZ軸座標値とを算定することができる。尚、A
点はX−Z座標面に合致する第1スリット光101の照
射像の端点であるため、A点のY軸座標値は零になる
が、C点やD点のようにY軸座標値が零にならない端点
については、端点に対する各カメラ21、22の視線のX
−Z座標面への投影線の方程式を各カメラ21、22の画
面上における端点のx軸座標値から求め、両投影線の交
点として上記と同様に端点のX軸座標値とZ軸座標値と
を算定すると共に、両カメラの何れか一方例えば第1カ
メラ21を基準にしてその投影面Q1に平行な前記交点を
含む面と第1カメラ21の間の距離を求め、この距離
と、第1カメラ21とその投影面Q1の間の距離との比を
第1カメラ21の画面上における端点のy軸座標値に乗
算して、端点のY軸座標値を算定する。
Both cameras 2 1 , 2 2 have their optical axes 0 1 , 0 2 respectively.
Are arranged so as to cross obliquely as shown in FIG. 2 on a horizontal plane that coincides with the optical plane of the first slit light 10 1 , and the horizontal coordinate axis of the second slit light 10 2 on the horizontal plane in the optical axis direction. Is the X-axis, the horizontal coordinate axis orthogonal thereto is the Z-axis, the vertical coordinate axis orthogonal to the horizontal plane is the Y-axis, and the coordinate value of each end point in the spatial coordinate system with the origin 0 at the intersection of the optical axes 0 1 and 0 2 is It is calculated from the positions of the respective end points on the screen of both cameras 2 1 , 2 2 by the principle of triangulation method. The screens of the first camera 2 1 and the second camera 2 2 in the state of FIG.
As shown in (a) and (b) of the figure, when the horizontal x-axis and the vertical y-axis are taken on the screen with the center point corresponding to the origin 0 as the origin, the x-axis coordinate value of the screen and y The axial coordinate values represent the horizontal distance and the vertical distance from the origin 0 on the projection planes Q 1 and Q 2 of the cameras 2 1 and 2 2 in the spatial coordinate system.
For example, consider the point A, the first camera 2 1 projection plane Q 1
Horizontal distance x-axis coordinate value x 1 next to the point A on the first camera 2 1 screen from the origin 0 of the projection point A 1 of the point A to, likewise the second camera 2 2 to the projection plane Q 2 The horizontal distance from the origin 0 of the projected point A 2 of the point A is x of the point A on the screen of the second camera 2 2.
The axis coordinate value becomes x 2 . Then, the equation of the line of sight e 1 drawn from the first camera 2 1 to A 1 is obtained from x 1, and the equation of the line of sight e 2 drawn from the second camera 2 2 to A 2 is obtained from x 2 , The X-axis coordinate value and the Z-axis coordinate value of point A in the spatial coordinate system can be calculated as the intersections. Incidentally, A
Since the point is the end point of the first radiation image of the slit light 10 1 matching the X-Z coordinate plane, Y-axis coordinate value of the point A becomes zero, Y-axis coordinate value as point C or point D For the end points that do not become zero, X of the line of sight of each camera 2 1 , 2 2 with respect to the end points
-The equation of the projection line on the Z coordinate plane is obtained from the x-axis coordinate value of the end point on the screen of each camera 2 1 , 2 2 , and as the intersection of both projection lines, the X-axis coordinate value of the end point and the Z-axis are the same as above. The coordinate value is calculated, and the distance between the first camera 2 1 and a plane including the intersection point parallel to the projection plane Q 1 of one of the cameras, for example, the first camera 2 1 , is obtained. The ratio of this distance to the distance between the first camera 2 1 and its projection plane Q 1 is multiplied by the y-axis coordinate value of the end point on the screen of the first camera 2 1 to obtain the Y-axis coordinate value of the end point. Calculate.

【0009】尚、光軸が第1と第2の両スリット光10
1、102の光面に斜交するように配置した1台のカメラ
を用い、上記した従来技術と同様に光切断の解析法で各
端点の空間座標値を算定するようにしても良い。
It should be noted that the optical axes are both the first and second slit light beams 10
It is also possible to use one camera arranged so as to be oblique to the optical planes of 1 and 10 2 and calculate the spatial coordinate value of each end point by the light-cutting analysis method as in the above-described conventional technique.

【0010】ところで、第1スリット光源11は、円形
孔Waが予想される最大限のずれを生じても第1スリッ
ト光101の照射像の一方の端点例えば左方のA点側の
孔内周面に第1スリット光101が当たらないように、
左方に大きく傾けて配置されており、そのためA点は円
形孔Waの孔縁に正確に合致するが、第1スリット光1
1の照射像の他方の端点たるB点側の孔内周面には第
1スリット光101が当たり、図2の状態では第2カメ
ラ22の画面にB点側の孔内周面に照射された第1スリ
ット光101の像が写り、第1スリット孔101の照射像
の右方の端点たるB点は円形孔Waの孔縁からワークW
の板厚分だけ内側にずれてしまう。そこで、B点は孔位
置の測定に使用せず、A点と第2スリット光102の照
射像の2つの端点たるC点とD点との計3つの端点の位
置に基づいて以下の如く円形孔Waの中心位置を割出す
ようにした。
By the way, the first slit light source 1 1 has a hole on the side of one end point of the irradiation image of the first slit light 10 1 , for example, on the left side point A side even if the circular hole Wa has the maximum expected deviation. To prevent the first slit light 10 1 from hitting the inner peripheral surface,
It is arranged at a large inclination to the left, so that the point A exactly coincides with the hole edge of the circular hole Wa, but the first slit light 1
The first slit light 10 1 impinges on the hole inner peripheral surface on the B point side, which is the other end point of the irradiation image of 0 1 , and in the state of FIG. 2, the hole inner peripheral surface on the B point side on the screen of the second camera 2 2. The image of the first slit light 10 1 radiated on the image of the first slit hole 10 1 is reflected, and the right end point B of the irradiation image of the first slit hole 10 1 is at the work W from the hole edge of the circular hole Wa.
It will be displaced inward by the plate thickness of. Therefore, B point is not used for the measurement of the hole positions, as follows, based on the position of the total three end points of the two end points serving points C and D of the A point and the irradiation image of the second slit light 10 2 The center position of the circular hole Wa is indexed.

【0011】即ち、A、C、D各点の空間座標値を上記
の如く算定し、空間座標系においてこれら3つの点を含
む図4に示す如き平面Pの方程式を求め、該平面上に描
かれる円形孔Waの孔径に対応する所定径の円であっ
て、A点とC点とを通る第1の円S1と、A点とD点を
通る第2の円S2との方程式を求め、該両円S1、S2
の中心M1、M2の空間座標値から該両中心M1、M2
の中点Mの空間座標値を算出し、この中点Mの位置を円
形孔Waの中心位置とするようにした。ここで、C点と
D点は円形孔Waの孔縁に正確に合致しないことがある
が、両円S1、S2の径が予め規定され且つ両円S1、
S2が何れも正確度の高いA点を通るため、両円S1、
S2の中心M1、M2の中点Mは円形孔Waの中心から
左程ずれることはなく、A、C、Dの3点を通る円の方
程式を求めてその円の中心を円形孔の中心とする場合に
比し、円形孔Waの中心位置を精度良く測定できる。
That is, the spatial coordinate values of the points A, C and D are calculated as described above, the equation of the plane P including these three points as shown in FIG. 4 is obtained in the spatial coordinate system, and the equation is drawn on the plane. An equation of a first circle S1 passing through the points A and C and a second circle S2 passing through the points A and D, which is a circle having a predetermined diameter corresponding to the diameter of the circular hole Wa to be formed, Both circles S1 and S2
From the spatial coordinate values of the centers M1 and M2 of the
The spatial coordinate value of the midpoint M is calculated, and the position of the midpoint M is set as the center position of the circular hole Wa. Here, the points C and D may not exactly coincide with the hole edge of the circular hole Wa, but the diameters of both circles S1 and S2 are predetermined and both circles S1 and
Since both S2 pass through the point A with high accuracy, both circles S1,
The midpoint M of the centers M1 and M2 of S2 does not deviate to the left from the center of the circular hole Wa, and the equation of a circle passing through the three points A, C, and D is obtained, and the center of the circle is defined as the center of the circular hole. The center position of the circular hole Wa can be measured more accurately than in the case of performing.

【0012】[0012]

【発明の効果】以上の説明から明らかなように、本発明
によれば、ワークが或る程度位置ずれしても、第1スリ
ット光の照射像の2つの端点のうちの一方の第1端点は
円形孔の孔縁に正確に合致し、対2スリット光の照射像
の第2と第3の2つの端点の位置に多少の誤差が含まれ
ていても、第1と第2の端点を通る所定径の円の中心
と、第1と第3の端点を通る所定径の円の中心との中点
の位置は円形孔の中心から左程ずれることはなく、円形
孔の中心位置を精度良く測定できる。
As is apparent from the above description, according to the present invention, even if the work is displaced to some extent, one of the two end points of the irradiation image of the first slit light is the first end point. Accurately matches the edge of the circular hole, and even if the positions of the second and third end points of the irradiation image of the pair 2 slit light include some errors, the first and second end points are The position of the midpoint between the center of the circle of the predetermined diameter passing through and the center of the circle of the predetermined diameter passing through the first and third end points does not deviate to the left from the center of the circular hole, and the center position of the circular hole is accurate. It can be measured well.

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

【図1】 本発明方法の実施に用いる測定装置の一例の
概要を示す斜視図
FIG. 1 is a perspective view showing an outline of an example of a measuring apparatus used for carrying out the method of the present invention.

【図2】 その要部の平面図FIG. 2 is a plan view of the main part.

【図3】 (a)(b)各カメラの画面を示す図3A and 3B are diagrams showing screens of respective cameras.

【図4】 端点を通るように描かれる円を示す図FIG. 4 is a diagram showing a circle drawn so as to pass through end points.

【図5】 従来例の斜視図FIG. 5 is a perspective view of a conventional example.

【符号の説明】[Explanation of symbols]

W ワーク Wa 円形孔 11、12 スリット光源 101 第1スリ
ット光 102 第2スリット光 21、22 カメラ(撮像
手段) A 第1端点 C 第2端点 D 第3端点 S1、S2 円 M1、M2 円の中心 M 2つの円の中心の中点(円形孔の中心)
W workpiece Wa circular hole 1 1, 1 2 slit light source 10 1 first slit light 10 2 second slit light 2 1, 2 2 camera (imaging means) A first end point C second end point D third endpoint S1, S2 yen M1, M2 Circle center M Midpoint center of two circles (center of circular hole)

Claims (1)

【特許請求の範囲】[Claims] 【請求項1】 ワークに形成した円形孔の中心位置を光
学的に測定する方法であって、ワークの表面に円形孔を
横切る互いに交差する第1と第2の2つのスリット光を
照射し、これらスリット光の照射像を撮像手段で撮像し
て、円形孔の孔縁に合致する各照射像の端点の位置を検
出し、これら端点の位置から円形孔の中心位置を割出す
ものにおいて、前記両スリット光の一方の第1スリット
光を、円形孔の予測される最大限のずれを生じても第1
スリット光の照射像の2つの端点のうちの一方の第1端
点側の円形孔の内周面に第1スリット光が当たらないよ
うに、ワークの表面に照射し、この第1端点と第2スリ
ット光の照射像の2つの端点のうちの一方の第2端点と
他方の第3端点との空間座標値を撮像手段の画面上の該
各端点の位置から算定し、空間座標系におけるこれら3
つの端点を含む平面上に描かれる、円形孔の孔径に対応
する所定径の円であって、第1端点と第2端点とを通る
円の中心座標値と、第1端点と第3端点とを通る円の中
心座標値とを算出し、これら両円の中心の中点を円形孔
の中心位置として求めることを特徴とする孔位置の測定
方法。
1. A method for optically measuring the center position of a circular hole formed in a work, comprising irradiating the surface of the work with first and second slit light beams that intersect each other across the circular hole. An image of these slit light irradiation images is picked up by an image pickup means to detect the position of the end point of each irradiation image that matches the hole edge of the circular hole, and the center position of the circular hole is calculated from the position of these end points. The first slit light of one of the two slit lights is not changed to the first slit light even if the predicted maximum deviation of the circular hole occurs.
The surface of the work is irradiated so that the first slit light does not hit the inner peripheral surface of the circular hole on the side of the first end point of one of the two end points of the irradiation image of the slit light, and the first end point and the second end point are irradiated. The spatial coordinate values of one of the two end points and the other third end point of the two end points of the irradiation image of the slit light are calculated from the position of each end point on the screen of the image pickup means, and these 3 in the spatial coordinate system are calculated.
A circle having a predetermined diameter corresponding to the diameter of a circular hole drawn on a plane including two end points, the center coordinate value of a circle passing through the first end point and the second end point, and the first end point and the third end point. A method for measuring a hole position, characterized in that the center coordinate value of a circle passing through is calculated, and the midpoint between the centers of these circles is determined as the center position of the circular hole.
JP4294993A 1993-03-03 1993-03-03 Measuring method of hole position Pending JPH06258022A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP4294993A JPH06258022A (en) 1993-03-03 1993-03-03 Measuring method of hole position

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP4294993A JPH06258022A (en) 1993-03-03 1993-03-03 Measuring method of hole position

Publications (1)

Publication Number Publication Date
JPH06258022A true JPH06258022A (en) 1994-09-16

Family

ID=12650275

Family Applications (1)

Application Number Title Priority Date Filing Date
JP4294993A Pending JPH06258022A (en) 1993-03-03 1993-03-03 Measuring method of hole position

Country Status (1)

Country Link
JP (1) JPH06258022A (en)

Cited By (3)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
KR20040033929A (en) * 2002-10-16 2004-04-28 한국생산기술연구원 Scanner and method for measuring a hole using the same
CN106679564A (en) * 2016-12-15 2017-05-17 哈尔滨飞机工业集团有限责任公司 Measurement method of long circular hole
CN108662990A (en) * 2018-03-23 2018-10-16 舟山市宏基工业产品设计研究所 A kind of inclination measurement apparatus and method of cylinder cover slant hole

Cited By (4)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
KR20040033929A (en) * 2002-10-16 2004-04-28 한국생산기술연구원 Scanner and method for measuring a hole using the same
CN106679564A (en) * 2016-12-15 2017-05-17 哈尔滨飞机工业集团有限责任公司 Measurement method of long circular hole
CN108662990A (en) * 2018-03-23 2018-10-16 舟山市宏基工业产品设计研究所 A kind of inclination measurement apparatus and method of cylinder cover slant hole
CN108662990B (en) * 2018-03-23 2020-08-11 舟山市宏基工业产品设计研究所 Inclination measuring device and method for inclined hole of cylinder cover

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