JPS638404B2 - - Google Patents

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Publication number
JPS638404B2
JPS638404B2 JP7129178A JP7129178A JPS638404B2 JP S638404 B2 JPS638404 B2 JP S638404B2 JP 7129178 A JP7129178 A JP 7129178A JP 7129178 A JP7129178 A JP 7129178A JP S638404 B2 JPS638404 B2 JP S638404B2
Authority
JP
Japan
Prior art keywords
target object
point
image
monitor
lens
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
JP7129178A
Other languages
Japanese (ja)
Other versions
JPS54161962A (en
Inventor
Kazuo Takashima
Minoru Tanaka
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.)
Mitsubishi Electric Corp
Original Assignee
Mitsubishi Electric Corp
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 Mitsubishi Electric Corp filed Critical Mitsubishi Electric Corp
Priority to JP7129178A priority Critical patent/JPS54161962A/en
Publication of JPS54161962A publication Critical patent/JPS54161962A/en
Publication of JPS638404B2 publication Critical patent/JPS638404B2/ja
Granted legal-status Critical Current

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  • Length Measuring Devices By Optical Means (AREA)

Description

【発明の詳細な説明】 この発明は、光学的手段を用い非接触で物体の
寸法を測定する装置に関するものである。
DETAILED DESCRIPTION OF THE INVENTION The present invention relates to an apparatus for measuring the dimensions of an object in a non-contact manner using optical means.

従来この種の装置として、第1図に示すものが
あつた。図において、1は対象物体、2は対象物
体1を撮像するレンズおよび映像を電気信号に変
換する検出器を含むカメラ、3は対象物体1を撮
像するレンズ、4はレンズ3により撮像された映
像を電気信号に変換する1次元、または2次元検
出器(以下の説明では、2次元検出器で代表す
る。)5は2次元検出器4の出力を受けて、映像
表示するモニター、6は処理装置である。
A conventional device of this type is shown in FIG. In the figure, 1 is a target object, 2 is a camera including a lens that images the target object 1 and a detector that converts the image into an electrical signal, 3 is a lens that images the target object 1, and 4 is an image captured by the lens 3. A one-dimensional or two-dimensional detector (in the following explanation, a two-dimensional detector is used as a representative) that converts the signal into an electrical signal. 5 is a monitor that receives the output of the two-dimensional detector 4 and displays an image, and 6 is a processing device. It is a device.

次に動作について説明する。対象物体1をカメ
ラ2で撮像すると、2次元検出器4から第2図に
示すような画像1aがモニター5に得られる。こ
のとき画像の寸法bと、実際の対象物体1の寸法
wとは、次式(1)で示される関係にある。
Next, the operation will be explained. When the target object 1 is imaged by the camera 2, an image 1a as shown in FIG. 2 is obtained from the two-dimensional detector 4 on the monitor 5. At this time, the dimension b of the image and the actual dimension w of the target object 1 have a relationship expressed by the following equation (1).

w=m・α・b ……(1) ここで、mは光学系の倍率でレンズ3から対象
物体1までの距離Lと、レンズ3からカメラ2の
2次元検出器3までの距離lとにより m=l/L ……(2) で求められる。また、レンズ3の焦点距離fで示
せば m=f/L−f ……(3) となる。一般に焦点距離fは一定値に固定されて
いるので、Lを一定値に保てば光学系の倍率mは
変動しない値となる。また、αはカメラ2および
モニター5で決められる電気的な倍率であり、一
般には一定値である。したがつて、光学系の倍率
m、電気的倍率αを事前に計算または測定により
求めておき、モニター5に得られる画像の寸法b
を測定し、上述の(1)式による演算を処理装置6に
よりおこなえば対象物体1の寸法wが得られる。
画像の寸法bの測定については、通常おこなわれ
ている映像信号処理技術によりおこなわれ、適当
な照明装置を用いて、対象物体1の画像と背景の
分離が容易になるような工夫もされている。
w=m・α・b...(1) Here, m is the magnification of the optical system, and the distance L from the lens 3 to the target object 1, and the distance l from the lens 3 to the two-dimensional detector 3 of the camera 2. It is determined by m=l/L...(2). Moreover, if the focal length f of the lens 3 is expressed, m=f/L−f (3). Generally, the focal length f is fixed at a constant value, so if L is kept at a constant value, the magnification m of the optical system will be a value that does not change. Further, α is an electrical magnification determined by the camera 2 and the monitor 5, and is generally a constant value. Therefore, the magnification m of the optical system and the electrical magnification α are calculated or measured in advance, and the size b of the image obtained on the monitor 5 is determined.
The dimension w of the target object 1 can be obtained by measuring and calculating the above equation (1) using the processing device 6.
The measurement of the image dimension b is carried out using a commonly used video signal processing technique, and an appropriate lighting device is also used to facilitate the separation of the image of the target object 1 from the background. .

従来の寸法測定装置は以上のように構成されて
いるので事前に光学系の倍率mを計算又は測定で
求めておく必要があり、また光学系の倍率mは、
対象物体からレンズまでの距離Lを一定に保つこ
とが必要であり、しかも対象物体の厚みが変動し
たり、対象物が振動したり、さらに、対象物体が
傾いていてもそれらを検出することができず、正
確な寸法測定ができないなどの欠点があつた。
Since the conventional dimension measuring device is configured as described above, it is necessary to calculate or measure the magnification m of the optical system in advance, and the magnification m of the optical system is
It is necessary to keep the distance L from the target object to the lens constant, and even if the thickness of the target object fluctuates, the target object vibrates, or even if the target object is tilted, it cannot be detected. There were drawbacks such as the inability to measure dimensions accurately.

この発明は、上記のような従来のものの欠点を
除去するためになされたもので、適当な投光手段
により対象物体の両側に明暗部を形成しこの明暗
部と上記対象物体とを撮像して対象物体の寸法測
定方向両端の座標が演算できるようにしたので対
象物体の振動、厚さ変化、傾きに影響されずに寸
法測定がおこなえ、必要に応じては変動要素の変
動値まで測定できる寸法測定装置を提供すること
を目的とする。
This invention was made in order to eliminate the drawbacks of the conventional ones as described above, and involves forming bright and dark areas on both sides of a target object using a suitable light projecting means, and imaging the bright and dark areas and the target object. Since the coordinates of both ends of the target object in the dimension measurement direction can be calculated, dimensions can be measured without being affected by vibrations, thickness changes, and inclinations of the target object, and if necessary, it is possible to measure the variable values of variable elements. The purpose is to provide a measuring device.

以下、この発明の一実施例を第3図ないし第5
図について説明する。第3図において、7は第4
図に示すようにカメラ2の光軸であるy軸上に発
散点Pが位置するように設けた投光装置、8は対
象物体1を乗せるテーブルである。第4図はこの
発明の動作および光学系の配置をしめす概略図
で、イは2次元検出器4の受光面である。第5図
は、この発明の動作を説明するための2次元検出
器4のモニター5に出来る対象物体1およびテー
ブル8の像をしめし、ロはビデオ信号波形を説明
するための抽出線ハ,トはテーブル8の投光装置
7で照明される明るい部分の像、ニ,ヘはテーブ
ル8のうちで対象物体1の影になり暗くなる部分
の像ホは対象物体1の投光装置7で照明された明
るい部分の像を示す。
An embodiment of the present invention will be described below in Figures 3 to 5.
The diagram will be explained. In Figure 3, 7 is the fourth
As shown in the figure, a light projecting device is provided such that a divergence point P is located on the y-axis, which is the optical axis of the camera 2, and 8 is a table on which the target object 1 is placed. FIG. 4 is a schematic diagram showing the operation of the present invention and the arrangement of the optical system, where A is the light receiving surface of the two-dimensional detector 4. Fig. 5 shows the images of the target object 1 and the table 8 formed on the monitor 5 of the two-dimensional detector 4 to explain the operation of the present invention; is an image of the bright part of the table 8 illuminated by the projector 7, d and f is an image of the dark part of the table 8 that is in the shadow of the target object 1. The image shows the bright part of the image.

次に、この発明による装置の動作を説明する。
第3図において、対象物体1がカメラ2により撮
像されてモニター5に対象物体1の映像が得られ
るまで従来の装置の説明の所で述べたとおりであ
る。しかしながら、この発明においては第4図に
示すように投光装置7はその発散点Pが、カメラ
2の幅方向軸上に位置し、高さ方向についてレン
ズ3の第2主点位置0より投光装置7の発散点P
が対象物体1側に設けられているので、テーブル
8上に出来る投光装置1の照明による対象物体1
の影の部分もカメラ2で撮像されモニター5に得
られる。第4図及び第5図でさらに詳しく説明す
ると、対象物体1に対してレンズ3の第2主点位
置0と投光装置7の照明光発散点位置Pは幅方向
光軸が等しくテーブル8に直交するように配置さ
れておりこの交点をO′とし、O点とO′点との距
離YOO′と、O点とP点との距離YOPは適当に決め
ておく。P点から発散する照明光は対象物体1お
よびテーブル8を照明するがテーブル8の表面上
で見て対象物体1のQ点からR点までの間に対応
する影のため、T点からN点までの間が暗くな
る。一方カメラ2はテーブル8の表面上での視野
がS点からZ点までとして、対象物体1のQ点か
らR点を撮像している。すなわちテーブル8の表
面上でU点からV点に相当する部分は明るく見
え、第5図のホに対応し、これ以外の視野部分で
はテーブル8のS点からU点、V点からZ点を撮
像している。この撮像部分中で前述した対象物体
1の影の部分に含まれるT点からU点、V点から
N点は暗く見え第5図のニ,ヘにそれぞれ対応す
る。また、残りのテーブル8の表面上を撮像して
いる部分S点からT点およびN点からZ点は明る
く見え第5図でハ,トの各部に対応する。以上の
ようにして第5図のようにモニター5に得られる
映像は全てテーブル8の表面上での対象物として
考えられる。したがつて、テーブル8表面上での
画像の寸法例えばO′からU点までの距離XOUは従
来の装置の説明の所で述べた(1)式から XOU=m・α・bOU ……(4) として求められ、mは(2)式または(3)式のLを
YOO′とおいて一定値となり、電気的倍率αは事前
に設定する一定値であり、bOUはモニター5での
映像O′U間の距離であるから、bOUの測定により
XOUが求められる。ここでbOUの測定は処理装置
6で通常用いられている映像処理技術によりおこ
なわれる。
Next, the operation of the device according to the present invention will be explained.
In FIG. 3, the process until the target object 1 is imaged by the camera 2 and the image of the target object 1 is obtained on the monitor 5 is as described in the description of the conventional apparatus. However, in this invention, as shown in FIG. 4, the light projecting device 7 has its divergence point P located on the axis in the width direction of the camera 2, and projects from the second principal point position 0 of the lens 3 in the height direction. Divergence point P of optical device 7
is provided on the target object 1 side, so that the target object 1 created by the illumination of the projector 1 on the table 8
The shadow part is also imaged by the camera 2 and displayed on the monitor 5. To explain in more detail with reference to FIGS. 4 and 5, the second principal point position 0 of the lens 3 and the illumination light divergence point position P of the light projector 7 with respect to the target object 1 have the same optical axis in the width direction on the table 8. They are arranged so as to intersect at right angles, and the intersection point is O', and the distance Y OO ' between points O and O' and the distance Y OP between points O and P are determined appropriately. The illumination light diverging from point P illuminates target object 1 and table 8, but due to the corresponding shadow between point Q and point R of target object 1 when viewed on the surface of table 8, the illumination light diverges from point T to point N. It gets dark until then. On the other hand, the camera 2 has a field of view on the surface of the table 8 from the point S to the point Z, and images the target object 1 from the point Q to the point R. In other words, the area corresponding to point U to V on the surface of table 8 appears bright, corresponding to E in Fig. 5, and in the other visual field areas, points S to U and point V to Z on table 8 appear bright. Imaging. In this imaged portion, points T to U and points V to N included in the shadow portion of the target object 1 described above appear dark and correspond to d and f in FIG. 5, respectively. Further, the portions from point S to point T and point from point N to point Z, which are imaged on the surface of the remaining table 8, appear bright and correspond to the portions C and G in FIG. As described above, all images obtained on the monitor 5 as shown in FIG. 5 can be considered as objects on the surface of the table 8. Therefore, the dimensions of the image on the surface of the table 8, for example the distance from O' to point U, X O ' U , can be calculated from equation (1) mentioned in the explanation of the conventional device: X O ' U = m・α・b OU ......(4) is obtained, and m is obtained by subtracting L in equation (2) or (3).
Since Y OO ′ becomes a constant value, the electrical magnification α is a constant value set in advance, and b OU is the distance between the images O′U on the monitor 5, by measuring b OU
X OU is required. Here, b OU is measured using an image processing technique commonly used in the processing device 6.

同様にしてテーブル8の表面上の各点間の距離
はモニター5の映像寸法から計算により求められ
る。対象物体1のQ点は、O点とU点を結ぶ直線
yUとP点、T点を結ぶ直線yTの交点でありOを原
点とした各直線の方程式は、第4図に示すような
矢印方向をそれぞれx軸、y軸の方向とすれば、 yUi=YOO′/XOUXi ……(5) yTi=YOO′−YOP/XOTXi−YOP ……(6) で与えられる。これらの各式(5)(6)からiをQとお
けば XQ=YOP/K2−K1 ……(7) YQ=YOP/K2−K1K1 ……(8) としてQ(XQ、YQ)座標が求められる。ここで K1=XOO′/XOU ……(9) K2=YOO′−YOP/XOT ……(10) である。
Similarly, the distance between each point on the surface of the table 8 is calculated from the image size of the monitor 5. Point Q of target object 1 is the straight line connecting point O and point U
The equation of each straight line, which is the intersection of the straight line y T connecting y U and points P and T, with O as the origin, is as shown in Figure 4, if the directions of the arrows are the x-axis and y-axis directions, respectively. It is given by y Ui =Y OO ′/X OU X i ……(5) y Ti =Y OO ′−Y OP /X OT X i −Y OP ……(6). From these equations ( 5 ) and ( 6 ) , if i is set as Q, then ), the Q(X Q , Y Q ) coordinates are obtained. Here, K 1 =X OO ′/X OU ……(9) K 2 =Y OO ′−Y OP /X OT ……(10).

XQ、YQを求めるためのYOO′、YOPは装置の構成
で決まる定数で、XOU、XOTはモニター5の映像
寸法で例えば第5図イ線上での寸法bOU、bOT
ら前述(4)式の説明のようにして計算で求まる。同
様にして対象物体1のR(XR、YR)座標は直線yV
とyNの交点であるから yVi=−YOO′/XOVXi ……(11) yNi=−YOO′−YOP/XONxi−YOP ……(12) により XR=YOP/K2−K1 ……(7) YR=YOP/K2−K1K1 ……(8) ただし K1=−XOO′/XOU ……(13) K2=YOO′−YOP/XON ……(14) として求められ、XOU、XONは、モニター5の映
像寸法bOV、bONを測定することにより計算でき
る。
Y OO ′ and Y OP for determining X Q and Y Q are constants determined by the configuration of the device, and X O ′ U and X OT are the image dimensions of the monitor 5, for example, the dimension b on line A in Figure 5. It can be calculated from OU and b OT as explained in equation (4) above. Similarly, the R (X R , Y R ) coordinates of target object 1 are the straight line y V
Since it is the intersection of and y N , y Vi = −Y OO /X O V 12 ) Accordingly , _ _ _ _ _ _ _ _ _ ...(13) K 2 = Y OO ′−Y OP /X ON ...(14) where X OU , X ON are the image dimensions of monitor 5 b OV , b It can be calculated by measuring ON.

以上のようにしてQ(XQ、YQ)およびR(XR
YR)の各点の座標が求められる。
As described above, Q (X Q , Y Q ) and R (X R ,
The coordinates of each point in Y R ) are determined.

対象物体1の幅方向の寸法Wは対象物体の傾き
を考えて W=√(|Q|+|R|)2+(|Q|−|R
|)2……(15) として計算できる。
The dimension W in the width direction of the target object 1 is determined by considering the inclination of the target object: W=√(| Q |+| R |) 2 +(| Q |-| R
|) 2 ...(15) It can be calculated as follows.

また、対象物体1とレンズ3のO点までの距離
Lは L=|YQ|+|YR|/2 ……(16) として求められ、対象物体1の傾き△は △=|YQ|−|YR| ……(17) で得られる。
Also, the distance L between the target object 1 and the point O of the lens 3 is obtained as L=|Y Q |+|Y R |/2 ...(16), and the inclination △ of the target object 1 is △=|Y Q |−|Y R | ...(17) is obtained as follows.

これらの演算は、処理装置6によりおこなわれ
る。
These calculations are performed by the processing device 6.

尚、ここで処理装置6の構成について補足的に
説明すると、処理装置6は上述の(15)式の演算
結果を表示又は出力する寸法表示部又は寸法出力
部、(17)式の演算結果を表示して対象物体1の
傾き△の定量値を示す傾き量表示部を備えてい
る。
Here, to provide a supplementary explanation of the configuration of the processing device 6, the processing device 6 includes a dimension display section or a dimension output section that displays or outputs the calculation result of the above-mentioned equation (15), and a dimension output section that displays the calculation result of the equation (17). A tilt amount display unit is provided to display a quantitative value of the tilt Δ of the target object 1.

従つて、傾き△の値に応じて別途制御手段によ
り対象物体1の傾きを是正するようにすることも
できる。
Therefore, the inclination of the target object 1 can be corrected by a separate control means depending on the value of the inclination Δ.

なお、上記実施例ではレンズ3の第2王点〇を
原点として計算式を展開したが、これは任意に選
ぶことができる。
In the above embodiment, the calculation formula was developed using the second king point 0 of the lens 3 as the origin, but this can be arbitrarily selected.

実施例のように、投光装置7の発散点Pをレン
ズ3の主軸上に位置するように設ければ、演算が
容易となり、演算時間が短かく、又処理装置6の
構成が簡略となる。
As in the embodiment, if the divergence point P of the light projecting device 7 is located on the main axis of the lens 3, the calculation becomes easy, the calculation time is shortened, and the configuration of the processing device 6 is simplified. .

実施例では2次元検出器4からの電気的映像信
号を一旦モニタ5を経由して、処理装置6に入力
しているが、2次元検出器4と処理装置6とを直
結してもよい。
In the embodiment, the electrical video signal from the two-dimensional detector 4 is inputted to the processing device 6 via the monitor 5, but the two-dimensional detector 4 and the processing device 6 may be directly connected.

以上のようにして、この発明によれば、対象物
体の両側に明暗部を形成する投光手段と、対象物
体及び明暗部を撮像する撮像手段とを、適当な配
置することにより、対象物体と、この影の映像寸
法から、対象物体の寸法を座標によつて求めるこ
とができ、対象物体の傾き、振動、厚さ変化に関
係なく寸法が測定でる効果がある。
As described above, according to the present invention, by appropriately arranging the light projection means that forms bright and dark areas on both sides of the target object and the imaging means that images the target object and the bright and dark areas, From the image dimensions of this shadow, the dimensions of the target object can be found in terms of coordinates, and the effect is that the dimensions can be measured regardless of the tilt, vibration, or thickness change of the target object.

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

第1図は従来の装置の構造を示す図、第2図は
従来装置の動作を説明するためのモニターの図、
第3図は、この発明による寸法測定装置の一実施
例を示す図、第4,5図はこの発明による装置の
実施例の動作を説明するための光学系配置とモニ
ターの映像を示す図である。 図において、1は対象物体、2はカメラ、3は
レンズ、4は2次元検出器、5はモニター、6は
処理装置、7は投光装置。なお、図中、同一符号
は同一、または相当部を示す。
FIG. 1 is a diagram showing the structure of a conventional device, FIG. 2 is a diagram of a monitor for explaining the operation of the conventional device,
FIG. 3 is a diagram showing an embodiment of the dimension measuring device according to the present invention, and FIGS. 4 and 5 are diagrams showing the optical system arrangement and monitor images for explaining the operation of the embodiment of the device according to the present invention. be. In the figure, 1 is a target object, 2 is a camera, 3 is a lens, 4 is a two-dimensional detector, 5 is a monitor, 6 is a processing device, and 7 is a light projector. In addition, in the figures, the same reference numerals indicate the same or equivalent parts.

Claims (1)

【特許請求の範囲】[Claims] 1 対象物体に投光し、該対象物体の背景両側に
対象物体の影を生ぜしめる投光手段、上記対象物
体および背景を結像する光学レンズとこの光学レ
ンズによる光学像に対応した電気信号を出力する
光電検出器を有する撮像手段、この撮像手段によ
り撮像された上記対象物体の影の端縁信号と上記
対象物体の端縁信号とにより、上記対象物体の幅
方向端縁の座標を求め、この座標に基いて上記対
象物体の寸法を算出する処理装置を備えたことを
特徴とする寸法測定装置。
1. A light projecting means that projects light onto a target object and creates a shadow of the target object on both sides of the background of the target object, an optical lens that forms an image of the target object and the background, and an electrical signal corresponding to the optical image formed by this optical lens. an imaging means having a photoelectric detector for outputting, determining the coordinates of the edge in the width direction of the target object based on the edge signal of the shadow of the target object imaged by the imaging means and the edge signal of the target object; A dimension measuring device comprising a processing device that calculates the dimensions of the target object based on the coordinates.
JP7129178A 1978-06-12 1978-06-12 Size measuring apparatus Granted JPS54161962A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP7129178A JPS54161962A (en) 1978-06-12 1978-06-12 Size measuring apparatus

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP7129178A JPS54161962A (en) 1978-06-12 1978-06-12 Size measuring apparatus

Publications (2)

Publication Number Publication Date
JPS54161962A JPS54161962A (en) 1979-12-22
JPS638404B2 true JPS638404B2 (en) 1988-02-23

Family

ID=13456431

Family Applications (1)

Application Number Title Priority Date Filing Date
JP7129178A Granted JPS54161962A (en) 1978-06-12 1978-06-12 Size measuring apparatus

Country Status (1)

Country Link
JP (1) JPS54161962A (en)

Families Citing this family (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS59136606A (en) * 1983-01-26 1984-08-06 Kawasaki Heavy Ind Ltd Detector for weld line
JPS6022606A (en) * 1983-07-18 1985-02-05 Saburo Tsuji Method for measuring three-dimensional position of object

Also Published As

Publication number Publication date
JPS54161962A (en) 1979-12-22

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