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JPS6338740B2 - - Google Patents
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JPS6338740B2 - - Google Patents

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Publication number
JPS6338740B2
JPS6338740B2 JP56048982A JP4898281A JPS6338740B2 JP S6338740 B2 JPS6338740 B2 JP S6338740B2 JP 56048982 A JP56048982 A JP 56048982A JP 4898281 A JP4898281 A JP 4898281A JP S6338740 B2 JPS6338740 B2 JP S6338740B2
Authority
JP
Japan
Prior art keywords
edge
rays
light
shape
striation
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
JP56048982A
Other languages
Japanese (ja)
Other versions
JPS57164374A (en
Inventor
Kyotaka Inada
Kyohiko Kawaguchi
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.)
Nippon Steel Corp
Original Assignee
Sumitomo Metal Industries 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 Sumitomo Metal Industries Ltd filed Critical Sumitomo Metal Industries Ltd
Priority to JP56048982A priority Critical patent/JPS57164374A/en
Publication of JPS57164374A publication Critical patent/JPS57164374A/en
Publication of JPS6338740B2 publication Critical patent/JPS6338740B2/ja
Granted legal-status Critical Current

Links

Classifications

    • GPHYSICS
    • G06COMPUTING OR CALCULATING; COUNTING
    • G06VIMAGE OR VIDEO RECOGNITION OR UNDERSTANDING
    • G06V20/00Scenes; Scene-specific elements
    • G06V20/60Type of objects
    • G06V20/64Three-dimensional [3D] objects

Landscapes

  • Engineering & Computer Science (AREA)
  • Physics & Mathematics (AREA)
  • General Physics & Mathematics (AREA)
  • Multimedia (AREA)
  • Theoretical Computer Science (AREA)
  • Image Input (AREA)
  • Image Processing (AREA)
  • Image Analysis (AREA)

Description

【発明の詳細な説明】 本発明は物体の2次元形状を認識する方法に関
し、例えば厚板(6mm厚以上の鋼板)の形状認識
に有効な方法を提案するものである。
DETAILED DESCRIPTION OF THE INVENTION The present invention relates to a method for recognizing the two-dimensional shape of an object, and proposes a method effective for recognizing the shape of a thick plate (a steel plate with a thickness of 6 mm or more), for example.

圧延中の鋼板の平面形状(有効幅、長さ、コー
ナ部形状、直角度等)を短時間で、即ち可逆圧延
機を出た後圧延方向が逆転される際の余剰時間等
の間に計測する方法は従来存在せず、このために
圧延中の平面形状を圧延制御に反映させることが
できなかつた。
Measures the planar shape (effective width, length, corner shape, squareness, etc.) of a steel plate during rolling in a short period of time, such as during the extra time when the rolling direction is reversed after leaving the reversing mill. Conventionally, there has been no method to do this, and for this reason, it has been impossible to reflect the planar shape during rolling in rolling control.

従来厚板等の平面形状を測定する手段として、
次の3つが代表的なものとして知られている。そ
の一つは熱間鋼材の自家発光スペクトルを利用す
るものであつて、赤外域光電増倍管と鏡体とを組
合せてなる光学系を鋼材上方に配し、鏡体揺動に
よりその視野を鋼材上で走査し、光電増倍管出力
急変時点がその鋼材の端縁部であるとして、走査
系の信号と光電増倍管出力とを関連づけて鋼材の
幅及び/又は長さを求める構成としてあり、
KELK社製の幅、長さ計がこれに相当する。とこ
ろがこの装置は、長手方向を主走査方向とし、幅
方向を副走査方向とする走査及び幅方向を主走査
方向とし、長手方向を副走査方向とする走査を行
つて、幅方向各部における長さ及び長手方向各部
における幅寸法を求めるので、計測対象を2〜3
秒間も停止させる必要がある。また自家発光スペ
クトルを利用するために計測対象の表面状態、温
度の影響を受けやすく、特にエツジ部のスケー
ル、水のり等により誤差を生じがちであり、加え
て極めて高価である。
Conventionally, as a means of measuring the planar shape of thick plates, etc.
The following three are known as representative ones. One of these uses the self-emission spectrum of hot-worked steel, in which an optical system consisting of an infrared photomultiplier tube and a mirror is placed above the steel, and the field of view is changed by swinging the mirror. A configuration in which a steel material is scanned and the width and/or length of the steel material is determined by correlating the scanning system signal and the photomultiplier tube output, assuming that the point of sudden change in the photomultiplier tube output is at the edge of the steel material. can be,
The width and length meters manufactured by KELK are equivalent to this. However, this device performs scanning in which the longitudinal direction is the main scanning direction and the width direction is the sub-scanning direction, and scanning in which the width direction is the main scanning direction and the longitudinal direction is the sub-scanning direction. Since the width dimension at each part in the longitudinal direction is determined, the measurement target is 2 to 3.
It needs to be stopped for even seconds. Furthermore, since it uses a self-emission spectrum, it is easily affected by the surface condition and temperature of the object to be measured, and is particularly prone to errors due to scale on edges, water deposits, etc. In addition, it is extremely expensive.

次に近赤外、或は可視域のテレビジヨンにより
計測対象を撮影し、そのパターン認識により形状
を求める方法がある。ところがこの方法も圧延中
の厚板等熱間鋼材を計測対象とする場合は、温度
ムラによる影響が大きく、エツジが冷えていた
り、スケールに覆われている場合には誤差を生じ
る。
Next, there is a method in which the object to be measured is photographed using near-infrared or visible television, and the shape is determined by pattern recognition. However, when this method is used to measure hot steel materials such as thick plates being rolled, the influence of temperature unevenness is significant, and errors occur if the edges are cold or covered with scale.

三つ目は下部光源式の幅計を用いる方法であ
る。これはこの幅計によつて長手方向各部の幅寸
法を求め、これと長手方向への移送距離情報とか
ら形状を計測する方法であり、厚板精整ライン
等、環境のよい処では使用可能であるが、圧延ラ
インではスケール、水が下部の光源に落下して使
用できず、また移送速度に限界がある。
The third method is to use a width meter with a bottom light source. This is a method that uses this width meter to determine the width of each part in the longitudinal direction, and then measures the shape from this and the information about the transfer distance in the longitudinal direction. It can be used in places with good environments such as thick plate finishing lines. However, in a rolling line, scale and water fall into the light source at the bottom, making it unusable, and there is a limit to the transfer speed.

本発明は斯かる事情に鑑みてなされたものであ
つて、高速の形状認識が可能であり、また計測対
象の表面状態、温度にも殆んど影響されずに精度
が高く、厚板形状を圧延パス毎に認識して、次の
圧延パスの制御情報となし得る2次元形状認識方
法を提供することを目的とする。
The present invention was developed in view of the above circumstances, and is capable of high-speed shape recognition, and is highly accurate, being almost unaffected by the surface condition and temperature of the object to be measured, and is capable of recognizing the shape of a thick plate. It is an object of the present invention to provide a two-dimensional shape recognition method that recognizes each rolling pass and can be used as control information for the next rolling pass.

本発明の第1の方法は端縁形状を詳細に検知す
ることができる方法であり、形状認識対象とする
面に光の連続投射又は光の走査投射にて、相互に
非平行な2本の光条を描き、これらの光条を2次
元撮像装置にて撮像し、その撮像画像のデータ処
理により各光条の端縁の位置を求める第1の過程
と、この位置に基いて特定される前記面の端縁を
含む部分に光の連続投射又は光の走査投射にて光
条を描き、この光条を2次元撮像装置にて撮像
し、その撮像画像のデータ処理により前記端縁の
形状を求める第2の過程を含み、第2の過程を1
回又は複数回実行することを特徴とする。
The first method of the present invention is a method that can detect the edge shape in detail, and involves continuous projection of light or scanning projection of light onto the surface to be recognized. A first process of drawing striations, capturing images of these striations with a two-dimensional imaging device, and determining the position of the edge of each striation through data processing of the captured image, and specifying the position based on this position. A ray is drawn on a portion including the edge of the surface by continuous projection of light or scanning projection of light, the ray is imaged with a two-dimensional imaging device, and the shape of the edge is determined by data processing of the captured image. , and the second process is 1
It is characterized by being executed once or multiple times.

第1図はこの第1の方法の実施状態を示す模式
図である。形状認識対象とする厚板は図示しない
可逆圧延機を出て白抜矢符方向に送られ、略々一
定の位置に停止され、その後逆送されていく。4
1はHMD(Hot Metal Detector)であつて、厚
板10の先端部形状が、中央部の張り出した舌状
であれ、中央部が凹んだフイツシユテール状であ
れ、厚板が停止位置に到達したときにその先端部
を検知し得る上方位置に配されており、該HMD
41が厚板10を検知した出力信号に同期してレ
ーザビーム発生装置11,21のビーム投射口を
覆つているシヤツタ(図示せず)を開くと共に演
算装置1に対して演算開始を指令するようにして
いる。レーザビーム発生装置11,21は例えば
Arレーザ装置であり、3511〜5145Åの範囲の波
長の光を出力する。この波長は、熱間厚板の自然
発光が赤色、近赤、赤外域であるのに比して短
い。12,22はレーザビームを拡散すべく発生
装置11,21の前方に配した凸レンズであり、
更にこれらの凸レンズ12,22夫々の前方には
回転鏡13,23が配設されている。回転鏡1
3,23は6角柱状をなしその中心に回転中心と
なる軸130,230を備え、周囲の6面に矩形
状の平面鏡131,231を備えている。第2図
は回転鏡13(23も同様)の内部構造を略示し
ており、ガラス板にアルミニウム等を蒸着して鏡
面とした平面鏡131は六角柱の一方の底面を構
成する基板132にその一端部を枢支してあり、
また同じく他方の底面を構成する基板133側で
は平面鏡131を軸130側に向けて付勢するよ
うに基板133の周縁部に取付けた爪状の押え部
材134,134にして遠心方向への飛出しを防
止しており、更に平面鏡131の裏面(軸130
側)の押え部材134,134と対向する基板1
33側端部には圧電素子135,135の一端が
取付けられている。基板132,133は6角形
の角部に配した連結杆136及び軸130にて連
結されており、この連結杆136の外周側の面及
び基板周縁部には平面鏡131の裏面周縁部を当
接させるべき緩衝材が付されている。而して前記
圧電素子135,135はその他端を基板133
裏面に固設したホルダに取付けてあり、この圧電
素子に課電しない状態では平面鏡131は軸心と
平行になるように諸寸法を定めてある。各圧電素
子135には2つの電極136,136が固着さ
れており、夫々のリード線は、六角柱部より外部
に位置する軸130に設けた全圧電素子(合計12
個)に共通のスリツプリング137,137に連
なり、図示しないブラシを経て反射角度制御回路
14に接続されている。
FIG. 1 is a schematic diagram showing the state of implementation of this first method. A thick plate whose shape is to be recognized leaves a reversible rolling mill (not shown), is sent in the direction of the white arrow, is stopped at a substantially fixed position, and is then sent back. 4
Reference numeral 1 is an HMD (Hot Metal Detector) that detects when the thick plate 10 reaches the stop position, regardless of whether the tip shape of the thick plate 10 is a tongue-like shape with a protruding central part or a fishtail-like shape with a concave central part. The tip of the HMD is placed in an upper position where it can be detected.
41 opens the shutters (not shown) covering the beam projection ports of the laser beam generators 11 and 21 in synchronization with the output signal that detects the thick plate 10, and also instructs the arithmetic unit 1 to start calculation. I have to. For example, the laser beam generators 11 and 21 are
It is an Ar laser device that outputs light with a wavelength in the range of 3511 to 5145 Å. This wavelength is shorter than the natural luminescence of hot slabs, which is in the red, near-red, and infrared regions. 12 and 22 are convex lenses placed in front of the generators 11 and 21 to diffuse the laser beam;
Furthermore, rotating mirrors 13 and 23 are arranged in front of these convex lenses 12 and 22, respectively. rotating mirror 1
3 and 23 are in the shape of a hexagonal prism, and have a shaft 130, 230 at the center thereof, which is the center of rotation, and rectangular plane mirrors 131, 231 on six surrounding surfaces. FIG. 2 schematically shows the internal structure of the rotating mirror 13 (23 is the same). A plane mirror 131 whose mirror surface is made by vapor-depositing aluminum or the like on a glass plate is attached to one end of a substrate 132 constituting one bottom surface of a hexagonal prism. It is pivotally supported by the
Similarly, on the substrate 133 side that constitutes the other bottom surface, claw-shaped holding members 134, 134 are attached to the peripheral edge of the substrate 133 so as to urge the plane mirror 131 toward the shaft 130 side, and the plane mirror 131 is pushed out in the centrifugal direction. In addition, the back surface of the plane mirror 131 (shaft 130
the substrate 1 facing the holding members 134, 134 on the side)
One end of the piezoelectric elements 135, 135 is attached to the end portion on the 33 side. The substrates 132 and 133 are connected by a connecting rod 136 and a shaft 130 arranged at the corners of a hexagon, and the peripheral edge of the back surface of the plane mirror 131 is brought into contact with the outer peripheral surface of the connecting rod 136 and the peripheral edge of the substrate. Comes with cushioning material to protect it. The other ends of the piezoelectric elements 135, 135 are connected to the substrate 133.
The plane mirror 131 is attached to a holder fixed to the back surface, and dimensions are determined so that the plane mirror 131 is parallel to the axis when no voltage is applied to the piezoelectric element. Two electrodes 136, 136 are fixed to each piezoelectric element 135, and each lead wire connects all the piezoelectric elements (total 12
The reflection angle control circuit 14 is connected to a common slip ring 137, 137, and is connected to the reflection angle control circuit 14 via a brush (not shown).

回転鏡23も同様の構造として反射角度制御回
路24に接続されている。軸130,230はモ
ータ(図示せず)に連なつており、高速で回転し
ている。そして回転鏡13はレーザビーム発生装
置11から発せられ、レンズ12で拡散されたレ
ーザビームが厚板10の長手方向の中心を幅方向
に照射走査して適幅の光条l1を描くように、また
回転鏡23はレーザビーム発生装置21から発せ
られ、レンズ22で拡散されたレーザビームが厚
板10の幅方向の中心を長手方向に照射走査して
適幅の光条l2を描くように夫々の軸130,23
0の方向が定められている。
The rotating mirror 23 has a similar structure and is connected to the reflection angle control circuit 24. The shafts 130, 230 are connected to a motor (not shown) and rotate at high speed. The rotating mirror 13 is configured so that the laser beam emitted from the laser beam generator 11 and diffused by the lens 12 scans the longitudinal center of the thick plate 10 in the width direction to draw a light streak l 1 of an appropriate width. In addition, the rotating mirror 23 is configured so that the laser beam emitted from the laser beam generator 21 and diffused by the lens 22 scans the center of the width direction of the thick plate 10 in the longitudinal direction to draw a light streak of an appropriate width. the respective shafts 130, 23
The direction of 0 is determined.

反射角度制御回路14,24は演算装置1から
与えられる信号に応じて回転鏡13,23の圧電
素子135等に直流電圧を印加する。圧電素子1
35は印加電圧の極性に応じて収縮し、また伸長
して平面鏡131,231の基板133,233
側端部が軸130,230に対し接近し又離隔
し、また印加電圧の値に応じて接近、離隔量が定
まることになる。これに伴い光条の位置が変じる
ことになる。つまり演算装置出力によつて光条位
置を自在に変更調節し得る構成としてある。
The reflection angle control circuits 14 and 24 apply a DC voltage to the piezoelectric elements 135 and the like of the rotating mirrors 13 and 23 in accordance with signals given from the arithmetic unit 1. Piezoelectric element 1
35 contracts and expands depending on the polarity of the applied voltage to connect the substrates 133, 233 of the plane mirrors 131, 231.
The side end portions approach or separate from the shafts 130, 230, and the amount of approach or separation is determined depending on the value of the applied voltage. As a result, the position of the rays will change. In other words, the configuration is such that the position of the striations can be freely changed and adjusted based on the output of the arithmetic device.

2aはテレビジヨンカメラ2のカメラヘツド、
2bはコントロールユニツトである。カメラヘツ
ド2aのレンズ面には前述の波長のレーザ光を選
択的に透過させる干渉フイルタ3が取付けられて
いる。厚板の自家発光スペクトルはより長波長側
に在るからテレビジヨンカメラ2の撮像画像は厚
板上の光条だけが明瞭に捉えられた状態になる。
また厚板下のローラコンベヤのローラ上にレーザ
ビームが投じられた場合には画像としてはこの部
分の光条も現れ得るが、ビデオ信号を適宜のしき
い値を用いて2値化することにより厚板上の光条
のみを有効とすることが可能になる。コントロー
ルユニツト2bの出力、即ちビデオ信号はエツジ
リスト3へ入力され、ここでビデオ信号が2値化
され光条とそれ以外の部分とが弁別され、光条の
エツジの座標値がメモリされる。
2a is the camera head of television camera 2;
2b is a control unit. An interference filter 3 is attached to the lens surface of the camera head 2a to selectively transmit laser light of the aforementioned wavelength. Since the self-emission spectrum of the thick plate is on the longer wavelength side, the image taken by the television camera 2 clearly captures only the rays on the thick plate.
Furthermore, if a laser beam is projected onto the rollers of a roller conveyor below the plank, streaks in this area may also appear in the image, but by binarizing the video signal using an appropriate threshold, It becomes possible to make only the rays on the plank effective. The output of the control unit 2b, that is, the video signal, is input to the edge list 3, where the video signal is binarized, striations and other parts are distinguished, and the coordinate values of the edges of the striations are memorized.

この第1の方法の場合には光条の幅は厚板10
のトツプ及びボトムの形状に応じて定められる。
光条は後述するように端部を照明するために使用
されるが、端縁がその凹凸の大きさのために、ま
た制御の誤差のために光条内に入らない、即ち照
明されないことになることがないようにある程度
の幅をもたせることが望まれ、またデータ処理の
簡便さ等からは狭幅であることが望ましい。従つ
て厚板のトツプ、ボトムの最凸部と最凹部との離
隔寸法が最大100mm程度である場合には300mm程度
に選択するのがよい。
In the case of this first method, the width of the striation is 10 mm.
It is determined according to the shape of the top and bottom.
The rays are used to illuminate the edges as described below, but due to the size of the irregularities and control errors, the edges do not fall within the rays, that is, they are not illuminated. It is desirable to have a certain width to prevent this from occurring, and it is also desirable to have a narrow width from the viewpoint of ease of data processing. Therefore, if the distance between the most convex part and the most concave part of the top or bottom of the thick plate is about 100 mm at most, it is better to select about 300 mm.

第3図は撮像画像(但し、2値化して光条l1
l2のみが現れた状態)を略示している。エツジリ
スト3には例えば画像の左上隅を原点とするX−
Y座標系において、光条l1の垂直方向の両端縁
Yu、Yd及び光条l2の水平方向の両端縁Xl、Xrに
ついてのX、Y座標が得られる。これらは各端縁
の線を構成する画素のX、Y座標の集合である
が、演算装置1は端縁Yu及びYdについては夫々
のY座標群についての平均値(Yu)及び(Yd)
を求め、これをもつて端縁位置とする。一方端縁
Xl及びXrについては夫々のX座標群についての
平均値(Xl)及び(Xr)を求め、これをもつて
端縁位置とする。演算装置1は更にエツジリスト
3の内容から光条l1、l2の交点座標(Xc、Yc)
を求める。これには光条l1、l2の交叉部に形成さ
れる正方形部分の4隅の座標値の平均を用いる。
Figure 3 shows the captured image (however, it is binarized and shows the light streak l 1 ,
The state in which only l 2 appears) is shown schematically. For example, Edge List 3 has an X-
In the Y coordinate system, both vertical edges of ray l 1
The X and Y coordinates of Yu, Yd and both horizontal edges Xl and Xr of the ray l2 are obtained. These are a set of X and Y coordinates of pixels that constitute each edge line, but the calculation device 1 calculates the average values (Yu) and (Yd) for each Y coordinate group for edges Yu and Yd.
Find this and use this as the edge position. one edge
Regarding Xl and Xr, the average values (Xl) and (Xr) for each X coordinate group are determined, and these are taken as the edge position. The arithmetic unit 1 further calculates the intersection coordinates (Xc, Yc) of the rays l 1 and l 2 from the contents of the edge list 3.
seek. For this purpose, the average of the coordinate values of the four corners of the square portion formed at the intersection of the rays l 1 and l 2 is used.

演算装置1はこのようにして求めた(Xc、
Yc)、(Xl)、(Xr)、(Yu)、(Yd)から光条移動
量を L11=Xr−Xc L12=Xl−Xc L21=Yu−Yc L22=Yd−Yc として求める。
Arithmetic unit 1 was obtained in this way (Xc,
Find the amount of streak movement from Yc), (Xl), (Xr), (Yu), and (Yd) as L 11 = Xr−Xc L 12 = Xl−Xc L 21 = Yu−Yc L 22 = Yd−Yc .

そしてこの移動量L11、L12は順次所定時間ずつ
反射角度制御回路14へ、また移動量L21、L22
順次所定時間ずつ反射角度制御回路24へ入力さ
れる。反射角度制御回路14,24はこれらの入
力信号に基き回転鏡13の圧電素子135、回転
鏡24の圧電素子に対し上記移動量だけ光条l1
l2を振らせるべき極性の電圧を印加する。これに
より厚板のトツプ部、一側縁部及びボトム部、他
側縁部が順次照射されることになる。第4図は光
条l1、l2が振られてなる光条l11、l21にてトツプ
部、一側縁部が照射されている状態の撮像画像を
示している。また第5図は光条l1、l2が振られて
なる光条l12、l22にてボトム部、他側縁部が照射
されている状態の撮像画像を示している。また回
転鏡の各鏡面の倒れ角を各々異る角度に設定し、
第7図に示すように4辺に対応する部分を同時に
照射し、4辺に対応する撮像画像よりエツジを得
ることも可能である。
The moving amounts L 11 and L 12 are sequentially input to the reflection angle control circuit 14 at predetermined time intervals, and the moving amounts L 21 and L 22 are sequentially input to the reflection angle control circuit 24 at predetermined time intervals. Based on these input signals, the reflection angle control circuits 14 and 24 control the piezoelectric elements 135 of the rotating mirror 13 and the piezoelectric elements of the rotating mirror 24 by the above-mentioned movement amount .
Apply a voltage of the polarity that should cause l2 to swing. As a result, the top, one edge, bottom, and other edge of the plank are sequentially irradiated. FIG. 4 shows a captured image in which the top portion and one side edge are illuminated by the rays l 11 and l 21 formed by the rays l 1 and l 2 . Further, FIG. 5 shows a captured image in which the bottom part and the other side edge part are illuminated by the rays l 12 and l 22 formed by the rays l 1 and l 2 . In addition, the angle of inclination of each mirror surface of the rotating mirror is set to a different angle,
As shown in FIG. 7, it is also possible to simultaneously irradiate portions corresponding to four sides and obtain edges from captured images corresponding to the four sides.

エツジリスト3における2値化された信号にお
いては厚板外での光条l11等の輪郭はなく、これ
に替つて厚板の周縁が明暗の境界となる。これに
よりエツジリスト3には厚板周縁の座標が格納さ
れることになる。演算装置1はこの座標情報を所
要の形状情報に加工し、これをプリンタ等の出力
表示装置4へ出力し、また可逆圧延機制御用のプ
ロコン5へその圧延制御用信号として与える。
In the binarized signal in Edge List 3, there are no outlines such as rays l11 outside the thick plate, and instead, the periphery of the thick plate becomes the boundary between bright and dark. As a result, the coordinates of the peripheral edge of the thick plate are stored in the edge list 3. The arithmetic unit 1 processes this coordinate information into required shape information, outputs this to an output display device 4 such as a printer, and supplies it to a processing controller 5 for controlling the reversible rolling mill as a rolling control signal.

なお上述の実施例では光源としてレーザビーム
発生装置を使用したが他のものでもよく、熱間材
の自家発光色とは異る色の光源を用いて、これを
スリツトにとおして適当な幅のビームとしてもよ
い。また光条は走査によらず連続的照射によつて
描くこととしてもよい。そして走査手段は前述の
如き回転鏡に限らず従来知られている他の手段を
用いてもよい。また光条の位置変更手段としては
圧電素子に限らずソレノイド等他の手段を用いて
もよい。
In the above embodiment, a laser beam generator was used as the light source, but other types may be used.A light source with a color different from the self-luminous color of the hot material is used, and the light source is passed through a slit of an appropriate width. It can also be used as a beam. Furthermore, the striations may be drawn by continuous irradiation instead of scanning. The scanning means is not limited to the above-mentioned rotating mirror, but other conventionally known means may be used. Furthermore, the means for changing the position of the striations is not limited to the piezoelectric element, but other means such as a solenoid may also be used.

更に厚板サイズ、所望分解能等に応じて、複数
のテレビカメラを用い、夫々にて撮像部分を分担
させることとしてもよい。
Furthermore, depending on the plate size, desired resolution, etc., a plurality of television cameras may be used and the imaging portion may be shared by each television camera.

この場合にはエツジリストをテレビカメラ台数
分だけ用い、演算装置にて座標系の統一をすれば
よいが、光条l1、l2の交点はいずれのカメラの視
野内にも含まれるようにし、これを基準に座標系
を統一する。
In this case, it is sufficient to use as many edge lists as there are TV cameras and unify the coordinate systems using the arithmetic unit, but the intersection of the rays l 1 and l 2 should be included in the field of view of each camera, The coordinate system is unified based on this.

またHMDを用いることなく、撮像画像により
鋼板を自動検知することとしてもよい。
Alternatively, the steel plate may be automatically detected using a captured image without using an HMD.

次に本発明の第2の方法を説明する。この方法
はトツプ、ボトムの幅寸法、或は側縁部の長さ等
を求めてこれから形状認識をするものであり、形
状認識対象とする面に、光の連続投射又は光の走
査投射にて相互に非平行な2本の光条を描き、こ
れらの光条を2次元撮像装置にて撮像し、その撮
像画像のデータ処理により各光条の端縁の位置を
求める第1の過程と、これらの長さに基いて特定
される前記面上の他の部分に前記光条と平行的な
光条を同様に描き、該光条を2次元撮像装置にて
撮像し、その撮像画像のデータ処理により各光条
の端縁の位置を求める第2の過程とを含み、第2
の過程を1回又は複数回実行することを特徴とす
る。
Next, a second method of the present invention will be explained. This method involves determining the width of the top and bottom, the length of the side edges, etc., and then recognizing the shape.The method involves continuously projecting light or scanning light onto the surface to be recognized. a first step of drawing two mutually non-parallel rays, capturing images of these rays with a two-dimensional imaging device, and determining the position of the edge of each ray through data processing of the captured images; Similarly, rays parallel to the rays are drawn on other parts of the surface specified based on these lengths, and the rays are imaged with a two-dimensional imaging device, and the captured image data is a second step of determining the position of the edge of each striation by processing;
It is characterized by performing the process one or more times.

以下この方法について説明する。この方法の実
施に用いる装置は第1図に示したものと同様であ
り、光条l1、l2を描く第1の過程も同様である。
ただ第2の方法では光条の幅内に厚板端縁を含ま
せないので光条の幅は狭くてもよく、凸レンズ1
2,22の使用は省略できる。
This method will be explained below. The apparatus used to carry out this method is similar to that shown in FIG. 1, and the first step of drawing the striations l 1 and l 2 is also similar.
However, in the second method, the edge of the plate is not included within the width of the ray, so the width of the ray may be narrow, and the convex lens 1
The use of 2 and 22 can be omitted.

而して第6図に示すように第1の方法と同様に
して光条l1、l2を略中央部に描き、(Xr)、(Xl)、
(Yu)、(Yd)、及び(Xc、Yc)を求める。次に
この方法では光条l1をトツプ部、ボトム部の端縁
よりも少し中央部寄りの位置に順次移動し、また
光条l2を両側縁部の端縁よりも少し中央部寄りの
位置に順次移動する。即ち演算装置1はその移動
量を L111=Xr−Xc−α1 L121=Xl−Xc−α1 L211=Yu−Yc−α2 L221=Yd−Yc−α2 として求める。ここに、α1、α2は(Xr)、(Yu)
等、光条l1、l2にて端縁とされた位置から中央部
へ寄せるべき長手方向及び幅方向の距離であり、
凹凸の大きい長手方向についてはα1=150mm程度、
幅方向についてはこれより短いα2=100mm程度と
するのがよい。
Then, as shown in Fig. 6, in the same way as the first method, rays l 1 and l 2 are drawn approximately in the center, and (Xr), (Xl),
Find (Yu), (Yd), and (Xc, Yc). Next, in this method, the ray l 1 is sequentially moved to a position slightly closer to the center than the edges of the top and bottom parts, and the ray l 2 is moved to a position slightly closer to the center than the edges of both sides. Move to positions sequentially. That is, the arithmetic unit 1 calculates the amount of movement as L 111 =Xr-Xc-α 1 L 121 = Xl-Xc-α 1 L 211 = Yu-Yc-α 2 L 221 = Yd-Yc-α 2 . Here, α 1 and α 2 are (Xr), (Yu)
etc., is the distance in the longitudinal direction and width direction that should be moved from the edge position of the striations l 1 and l 2 to the center,
For longitudinal directions with large irregularities, α 1 = approximately 150 mm;
In the width direction, it is preferable to set α 2 to be shorter than this, approximately 100 mm.

演算装置1は斯かる演算の後この移動量を実現
すべく所定の信号を反射角度制御回路14,24
へ出力する。これにより圧電素子に電圧を印加し
て四周の端縁近傍に光条l111、l121、l211、l222を描
く。これらの光条は撮像され、光条の端縁の座標
はエツジリスト3に格納されるが、この方法では
演算装置1は光条l111、l121の長手方向端縁(厚板
の幅方向端縁)位置又は端縁間長さを求め、また
光条l211、l221の長手方向端縁の位置又は端縁間長
さを求める。
After the calculation, the calculation device 1 sends a predetermined signal to the reflection angle control circuits 14 and 24 in order to realize this movement amount.
Output to. As a result, a voltage is applied to the piezoelectric element to draw striations l 111 , l 121 , l 211 , and l 222 near the edges of the four peripheries. These rays are imaged and the coordinates of the edges of the rays are stored in the edge list 3. In this method, the computing device 1 is able to detect the longitudinal edges of the rays l 111 and l 121 (widthwise edges of the plate). (edge) position or the length between the edges, and also determine the position of the longitudinal edge of the rays l 211 and l 221 or the length between the edges.

そして次には各光条をβ(例えば10mm)ずつ中
央部へ寄せた位置に描いて同様に光条の端縁の位
置等を求める。
Next, each ray is drawn at a position moved closer to the center by β (for example, 10 mm), and the position of the edge of the ray is determined in the same way.

即ち L112=Xr−Xc−α1−β L122=Xl−Xc−α1−β L212=Yu−Yc−α2−β L222=Yd−Yc−α2−β として光条l1からL112、L122離れた光条l112、l122
を順次描き、また光条l2からL212、L222離れた光
条l212、l222を順次描く。以下このようにしてβ刻
みで同様の処理を反復し、これによつて形状を認
識する。
That is, L 112 = Xr−Xc−α 1 −β L 122 = Xl−Xc−α 1 −β L 212 = Yu−Yc−α 2 −β L 222 = Yd−Yc−α 2 −β as the light l 1 Rays away from L 112 , L 122 L 112 , L 122
, and also sequentially draw rays L 212 and L 222 , which are L 212 and L 222 away from ray L 2 . Thereafter, the same process is repeated in increments of β, thereby recognizing the shape.

以上のような本発明方法による場合は認識対象
の温度、表面状態等に全く影響されずに形状認識
できる。また1フレームの画像の撮像には一般に
1/30秒程度で足りるから本発明による場合は形
状認識は1秒以内に十分可能であり、著しく高速
化することができる。このため厚板圧延において
は形状認識のために特に厚板を停止させずとも搬
送方向逆転時等の利用によつて迅速に形状認識処
理ができ、その結果、圧延能率を何ら損うことな
く形状認識が行え、しかもその認識結果を次の圧
延パスの圧延制御に利用し得る等、本発明は優れ
た効果を奏する。
According to the method of the present invention as described above, shape recognition can be performed without being affected by the temperature, surface condition, etc. of the object to be recognized. Furthermore, since it generally takes about 1/30 second to capture one frame of image, shape recognition according to the present invention is sufficiently possible within one second, and the speed can be significantly increased. For this reason, in thick plate rolling, shape recognition can be performed quickly by reversing the conveying direction without having to stop the plate for shape recognition, and as a result, the shape can be recognized without any loss in rolling efficiency. The present invention has excellent effects, such as being able to perform recognition and use the recognition results for rolling control of the next rolling pass.

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

図面は本発明の実施例を示すものであつて、第
1図は第1の方法の実施状態を示す模式図、第2
図は回転鏡の内部構造略示図、第3図は撮像画像
の略示図、第4,5図は認識原理の説明図、第6
図は第2の方法によつて描かれた光条の説明図、
第7図は第1の方法の他の実施状態を示す撮像画
像図である。 1……演算装置、2……テレビジヨンカメラ、
3……エツジリスト、11,21……レーザビー
ム発生装置、13,23……回転鏡、14,24
……反射角度制御回路、135……圧電素子。
The drawings show embodiments of the present invention, and FIG. 1 is a schematic diagram showing the implementation state of the first method, and FIG.
The figure is a schematic diagram of the internal structure of the rotating mirror, Figure 3 is a schematic diagram of the captured image, Figures 4 and 5 are explanatory diagrams of the recognition principle, and Figure 6 is an illustration of the recognition principle.
The figure is an explanatory diagram of rays drawn by the second method,
FIG. 7 is a captured image diagram showing another implementation state of the first method. 1... Arithmetic device, 2... Television camera,
3... Edge list, 11, 21... Laser beam generator, 13, 23... Rotating mirror, 14, 24
...Reflection angle control circuit, 135...Piezoelectric element.

Claims (1)

【特許請求の範囲】 1 形状認識対象とする面に、光の連続投射又は
光の走査投射にて、相互に非平行な2本の光条を
描き、これらの光条を2次元撮像装置にて撮像
し、その撮像画像のデータ処理により各光条の端
縁の位置を求める第1の過程と、この位置に基い
て特定される前記面の端縁を含む部分に光の連続
投射又は光の走査投射にて光条を描き、この光条
を2次元撮像装置にて撮像し、その撮像画像のデ
ータ処理により前記端縁の形状を求める第2の過
程を含み、第2の過程を1回又は複数回実行する
ことを特徴とする2次元形状認識方法。 2 形状認識対象とする面に、光の連続投射又は
光の走査投射にて、相互に非平行な2本の光条を
描き、これらの光条を2次元撮像装置にて撮像
し、その撮像画像のデータ処理により各光条の端
縁の位置を求める第1の過程と、これらの長さに
基いて特定される前記面上の他の部分に前記光条
と平行的な光条を同様に描き、該光条を2次元撮
像装置にて撮像し、その撮像画像のデータ処理に
より各光条の端縁の位置を求める第2の過程とを
含み、第2の過程を1回又は複数回実行すること
を特徴とする2次元形状認識方法。
[Claims] 1. Two mutually non-parallel rays are drawn on a surface to be recognized by shape by continuous projection of light or scanning projection of light, and these rays are transmitted to a two-dimensional imaging device. The first step is to obtain the position of the edge of each striation by data processing the captured image, and to continuously project light or light onto the portion including the edge of the surface specified based on this position. A second step includes drawing a striation by scanning and projecting the striation, capturing an image of the striation using a two-dimensional imaging device, and determining the shape of the edge through data processing of the captured image. A two-dimensional shape recognition method characterized by being executed once or multiple times. 2 Draw two mutually non-parallel rays on the surface to be shape recognized by continuous projection of light or scanning projection of light, image these rays with a two-dimensional imaging device, and capture the image. A first process of determining the position of the edge of each striation by image data processing, and similarly placing striations parallel to the striation on other parts of the surface specified based on these lengths. a second step in which the rays are imaged with a two-dimensional imaging device, and the position of the edge of each ray is determined by data processing of the captured image, and the second step is performed one or more times. A two-dimensional shape recognition method characterized in that the two-dimensional shape recognition method is performed twice.
JP56048982A 1981-03-31 1981-03-31 Recognition method for two-dimensional shape Granted JPS57164374A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP56048982A JPS57164374A (en) 1981-03-31 1981-03-31 Recognition method for two-dimensional shape

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP56048982A JPS57164374A (en) 1981-03-31 1981-03-31 Recognition method for two-dimensional shape

Publications (2)

Publication Number Publication Date
JPS57164374A JPS57164374A (en) 1982-10-08
JPS6338740B2 true JPS6338740B2 (en) 1988-08-02

Family

ID=12818442

Family Applications (1)

Application Number Title Priority Date Filing Date
JP56048982A Granted JPS57164374A (en) 1981-03-31 1981-03-31 Recognition method for two-dimensional shape

Country Status (1)

Country Link
JP (1) JPS57164374A (en)

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* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
CN110187496B (en) * 2019-05-13 2021-10-29 大族激光科技产业集团股份有限公司 A laser scanning device and method

Also Published As

Publication number Publication date
JPS57164374A (en) 1982-10-08

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