JPS58105008A - Radiation thickness gauge - Google Patents

Radiation thickness gauge

Info

Publication number
JPS58105008A
JPS58105008A JP20424781A JP20424781A JPS58105008A JP S58105008 A JPS58105008 A JP S58105008A JP 20424781 A JP20424781 A JP 20424781A JP 20424781 A JP20424781 A JP 20424781A JP S58105008 A JPS58105008 A JP S58105008A
Authority
JP
Japan
Prior art keywords
signal
radiation
thickness
cart
output
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
JP20424781A
Other languages
Japanese (ja)
Inventor
Junichi Murakami
純一 村上
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.)
Toshiba Corp
Original Assignee
Toshiba Corp
Tokyo Shibaura Electric 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 Toshiba Corp, Tokyo Shibaura Electric Co Ltd filed Critical Toshiba Corp
Priority to JP20424781A priority Critical patent/JPS58105008A/en
Publication of JPS58105008A publication Critical patent/JPS58105008A/en
Pending 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
    • G01B15/00Measuring arrangements characterised by the use of electromagnetic waves or particle radiation, e.g. by the use of microwaves, X-rays, gamma rays or electrons
    • G01B15/02Measuring arrangements characterised by the use of electromagnetic waves or particle radiation, e.g. by the use of microwaves, X-rays, gamma rays or electrons for measuring thickness

Abstract

PURPOSE:To provide a titled thickness gauge which measures a thickness at a measuring point in the proximity of a plate end without any delay in answering and without being influenced by a lateral deflection, by a method wherein an output of a plate end detector is compared with outputs of a setter for each measuring point and a setter for returning point, and based on the comparing result, a measuring point and a returning point are determined. CONSTITUTION:A radiation thickness gauge is set so that is positioned at a center of an object 91 to be measured through movement of a C-frame 21, and based on a signal from a line central detecting switch 60, a profile computing part 50 finds a plate thickness of a central part. A C-frame truck 21 is then moved by means of a profile measuring command signal FS from the outside, a comparing circuit 73 outputs a coincidence signal when reaching a speed changing point (a), and the truck 21 is reduced in a moving speed. The output of the plate end detector 25 is normally supplied to a comparing circuit 42 which outputs a coincidence signal when the truck 21 reaches a measuring point (b), and the profile comparing part 50 finds a plate thickness of an edge part. Finally, if the truck 21 moves forward and a coincidence signal is outputted from a comparing circuit 92, the truck 21 is moved backward.

Description

【発明の詳細な説明】 発明の技術分野 本発明は例えば圧延鋼板等のプロフィルを測定する放射
線厚み計の改良に関する。
DETAILED DESCRIPTION OF THE INVENTION Technical Field of the Invention The present invention relates to an improvement in a radiation thickness meter for measuring the profile of, for example, rolled steel plates.

発明の技術的背景 一般に、圧延鋼板は第1図に示すようなりラウン形状の
ものが多い。このような緩慢な丸みのあるクラウン形状
の鋼板は冷却用コイルとして好適なものとされている。
TECHNICAL BACKGROUND OF THE INVENTION In general, rolled steel plates often have a round shape as shown in FIG. Such a gently rounded crown-shaped steel plate is suitable for use as a cooling coil.

このため、最近の圧延技術では、仕上げ圧延機にワーク
ロールベンディング法を採用し、圧下量、圧延ピッチ。
For this reason, recent rolling technology employs the work roll bending method in finishing rolling mills to improve rolling reduction and rolling pitch.

ロール冷却法等を適宜選択l〜で最適なりラウン量(板
厚分布)の圧延鋼板が作られている。
A rolled steel plate with an optimum round amount (plate thickness distribution) is produced by appropriately selecting a roll cooling method or the like.

一方、放射線厚み計は、圧延技術の進歩と歩調を合せて
単に銅板の中央部板厚の測定だけでなく、鋼板の板幅方
向のクラウン量(−b −7)、ウェッゾfit(−〇
−,)およびエッソドロップ蓋等を測定している。この
ような測定はプロフィル測定法と呼ばれている。図中、
aは左エッソ部板厚、bは中央部板厚、Cは右エツジ部
板厚である。
On the other hand, radiation thickness gauges have kept pace with the progress of rolling technology, and are capable of measuring not only the central thickness of copper plates, but also the crown amount (-b -7) in the width direction of steel plates, and the wezzo fit (-〇- ) and Esso Drop lids, etc. are being measured. Such a measurement is called a profile measurement method. In the figure,
a is the thickness of the left esso portion, b is the thickness of the center portion, and C is the thickness of the right edge portion.

以下、グロフィル測定手段を備えた従来の放射線厚み計
について第2図ないし第5図を参照して説明する。先ず
、第2図は機械的構成を示す図である。同図において1
はCフレーム台車であって、この台車1は台車駆動用モ
ータ2によって図示A矢印方向に移動する。このCフレ
ーム台車Iの下部枠1aおよび上部枠7bには放射線源
3および放射線検出器4(電離箱)が対向配置されてい
る。従って、Cフレーム台車Iは、第2図のように鋼板
6が台車I外側に存する場合には台車駆動用モータ2の
駆動によって図示右方向に移動する。このとき、放射線
源3から放射線が放射されている。この放射線は鋼板6
を透過するが、鋼板6の板厚が大きくなるとそれに比例
して減衰量が大きくなり、放射線量が減少する。
Hereinafter, a conventional radiation thickness meter equipped with a glofill measuring means will be described with reference to FIGS. 2 to 5. First, FIG. 2 is a diagram showing the mechanical configuration. In the same figure, 1
1 is a C-frame truck, and this truck 1 is moved in the direction of arrow A in the figure by a truck driving motor 2. A radiation source 3 and a radiation detector 4 (ionization chamber) are arranged opposite to each other on the lower frame 1a and the upper frame 7b of this C-frame truck I. Therefore, when the steel plate 6 is located outside the truck I as shown in FIG. 2, the C-frame truck I is moved to the right in the figure by the drive of the truck drive motor 2. At this time, radiation is being emitted from the radiation source 3. This radiation is the steel plate 6
However, as the thickness of the steel plate 6 increases, the amount of attenuation increases in proportion to the thickness, and the radiation dose decreases.

次に、第3図は信号処理系の構成図であって、放射線源
3から照射された放射線は直接又は鋼板6を介して放射
線検出器4によって検出される。この放射線検出器4は
放射線量に比例した電流信号に変換した後、前置増幅器
7によって増幅される。この前置増幅器7で増幅された
アナログ信号はA−D変換回路8と板厚検出回路9とに
供給される。このA−D変換回路8は入力アナログ信号
をディジタル化して後続の信号処理回路IOに供給する
。信号処理回路10はディジタル化号と予め設定された
鋼板6の中央5一 部板厚すとの偏差を求めてその偏差信号を後続のD−A
変換回路11に供給する。また、信号処理回路10は板
無し信号と予め設定した中央部板厚すとの平均値信号を
板厚検出回路9に送出している。この板厚検出回路9は
前置増幅器7からの信号が平均値信号を越えたとき、第
4図(b)のように立上って仮布信号を出力してカウン
タ12をリセットする。このカウンタ12は、仮布信号
によってリセットされた後、台車位置検出器5からの信
号を計数して台車の位置信号としこれを比較回路13へ
送出する。この比較回路13は位置信号が測定点一定器
I4で予め設定した測定点a又はC(エツジ部板厚の位
置)と比較し、一致したとき鋼板6のエツジ部板厚の測
定タイミング信号をプロフィル演算部15に与える。こ
こで、プロフィル演算部15は、D−A変換回路11で
変換されたアナログ信号と比較回路I3からの位置信号
とに基づいて鋼板6のクラウン量やウェツジ量を求めて
プロフィル測定を行なう。第4図(j)は鋼板形状を示
す。
Next, FIG. 3 is a block diagram of a signal processing system, and the radiation emitted from the radiation source 3 is detected by the radiation detector 4 either directly or via the steel plate 6. This radiation detector 4 converts the current signal into a current signal proportional to the radiation dose, which is then amplified by a preamplifier 7. The analog signal amplified by the preamplifier 7 is supplied to an A-D conversion circuit 8 and a plate thickness detection circuit 9. This A-D conversion circuit 8 digitizes the input analog signal and supplies it to the subsequent signal processing circuit IO. The signal processing circuit 10 calculates the deviation between the digitized code and the preset thickness of the center 5 part of the steel plate 6, and transmits the deviation signal to the subsequent D-A.
It is supplied to the conversion circuit 11. Further, the signal processing circuit 10 sends an average value signal of the no-plate signal and the preset central plate thickness to the plate thickness detection circuit 9. When the signal from the preamplifier 7 exceeds the average value signal, the board thickness detection circuit 9 rises as shown in FIG. 4(b), outputs a false cloth signal, and resets the counter 12. After being reset by the temporary fabric signal, the counter 12 counts the signal from the cart position detector 5 and sends it to the comparator circuit 13 as a cart position signal. This comparison circuit 13 compares the position signal with the measurement point a or C (edge thickness position) set in advance by the measurement point constant device I4, and when they match, profiles the edge thickness measurement timing signal of the steel plate 6. It is given to the arithmetic unit 15. Here, the profile calculation section 15 calculates the crown amount and wedge amount of the steel plate 6 based on the analog signal converted by the DA conversion circuit 11 and the position signal from the comparison circuit I3, and performs profile measurement. FIG. 4(j) shows the shape of the steel plate.

6− 背景技術の問題点 従来装置にあっては、根方信号により正確に板端を検出
し板幅に対応した信号を取り出すことができるが、その
ためには第5図に示すようにCフレーム台車Iを板無し
のB点位置に待機させその位置から銅板6に向って前進
させて根方信号を得る必要がある。Cは鋼板流れ方向を
示す。このため、第4図(c)に示すようにD−A変換
回路11から得られる偏差出力に遅れをもたらす。この
遅れは、検出器4および前置増幅器7吟に組込まれてい
る抵抗、コンデンサ等ニよる時定数のほか、測定系の1
次遅れ要素が原因である。このため、一般的に、板無し
の状態から鋼板6の厚みに相当するレベルに達するまで
台車lを移動させて本来の測定に入る必要がある。この
ため、例えば300 mseの時定数等を有する放射線
厚み針では、30 ta/ secの台車速度で2朝の
鋼板6を測定する場合、板端から約20鴫以内は測定不
可能となる。
6- Problems in the Background Art With conventional devices, it is possible to accurately detect the board edge using the root signal and extract a signal corresponding to the board width, but in order to do so, it is necessary to use the C frame as shown in Figure 5. It is necessary to make the trolley I wait at a point B without a plate and move it forward toward the copper plate 6 from that position to obtain a root signal. C indicates the flow direction of the steel plate. This causes a delay in the deviation output obtained from the DA conversion circuit 11, as shown in FIG. 4(c). This delay is caused by the time constant caused by the resistors and capacitors built into the detector 4 and preamplifier 7, as well as by the measurement system components.
This is caused by the next lag element. For this reason, it is generally necessary to move the cart 1 from a state without a plate until it reaches a level corresponding to the thickness of the steel plate 6 before starting the actual measurement. For this reason, for example, with a radiation thickness needle having a time constant of 300 msec, when measuring a two-day steel plate 6 at a cart speed of 30 ta/sec, it is impossible to measure within about 20 meters from the edge of the plate.

また、放射線厚み計が板端を検出した後設定器14の測
定点に達するまでの間に鋼板6に横振れとか板幅に変動
が生ずると、測定点は相対的に移動してしまう。このた
め正確に測定点を求める場合、台車1の往路で測定点a
、b等を求め、更に復路で測定点Cを求めるようにして
いるが、そのための位置補正が厄介である。通常、放射
線厚み計とこの厚み計下流に別設する板幅計との信号を
用いて中形電子計算機により距離のトラッキング計算を
行なって位置補正を行なっている。
Further, if lateral vibration or fluctuation in the plate width occurs in the steel plate 6 after the radiation thickness meter detects the plate end and before reaching the measurement point of the setter 14, the measurement point will move relatively. Therefore, when determining the measurement point accurately, measurement point a is
, b, etc., and then the measurement point C is determined on the return trip, but the position correction for this is troublesome. Normally, a medium-sized electronic computer performs distance tracking calculations using signals from a radiation thickness meter and a plate width meter separately installed downstream of the thickness meter to perform position correction.

発明の目的 本発明は上記実情にかんがみてなされたもので、被測定
物端部の測定点を応答遅れなく測定でき、また被測定物
の横振れ等の影替を受けることなくグロフィルを測定で
きる放射線厚み計を提供することを目的とする。
Purpose of the Invention The present invention has been made in view of the above-mentioned circumstances, and it is possible to measure the measurement point at the end of the object to be measured without response delay, and also to measure the glofil without being affected by shadow changes such as lateral vibration of the object to be measured. The purpose is to provide a radiation thickness gauge.

発明の概要 本発明は放射線検出系を備えた台車の所定個所に台車位
置検出器の外に板端検出器を設け、台車が被測定物のラ
イン中央に存するときに被測定物の中央部板厚を測定す
るとともに、ライさせ、また板端検出器の出力から被測
定物板端の測定点および台車折返し点を求めて被測定物
のエッソ部板厚を測定しかつ台車を折返し制御すること
により、上記目的を達成せんとするものである。
SUMMARY OF THE INVENTION The present invention provides a plate end detector outside the cart position detector at a predetermined location of a cart equipped with a radiation detection system, and when the cart is located at the center of the line of the object to be measured, the center plate of the object to be measured is detected. To measure the thickness of the object to be measured, to lie it, and to determine the measurement point at the end of the object to be measured and the turning point of the cart from the output of the edge detector, to measure the thickness of the esso part of the object to be measured, and to control the turning of the cart. This aims to achieve the above objectives.

発明の実施例 第6図および第7図は本発明の一実施例を示す図であっ
て、第6図は機械的構成を示し、第7図は信号処理系を
示す図である。先ず、放射線厚み計の機械的構成につい
て述べる。第6図において21は例えばCフレーム台車
であって、これは移動可能な構成となっている。このC
フレーム台車2Iの下部枠21aおよびその下部枠21
aの一側部には放射線源22および光源23がそれぞれ
配置されている。また、Cフレーム台車2Iの上部枠2
1bおよびその上部枠21bの一側部には放射線源22
からの放射線−〇 − 量を検出する例えば電離箱等の放射線検出器24および
光源23からの光の有無を検出する板端検出器25がそ
れぞれ配−されている。なお、上部枠2Ib側に放射線
源22.光源23を、下部枠21a側に放射線検出器2
4.板端検出器25をそれぞれ配置する構成でもよい。
Embodiment of the Invention FIGS. 6 and 7 are diagrams showing an embodiment of the present invention, in which FIG. 6 shows a mechanical configuration and FIG. 7 shows a signal processing system. First, the mechanical configuration of the radiation thickness meter will be described. In FIG. 6, 21 is, for example, a C-frame truck, which is movable. This C
Lower frame 21a of frame truck 2I and its lower frame 21
A radiation source 22 and a light source 23 are respectively arranged on one side of a. In addition, the upper frame 2 of the C frame trolley 2I
1b and one side of its upper frame 21b is a radiation source 22.
A radiation detector 24, such as an ionization chamber, for detecting the amount of radiation from the light source 23 and a plate end detector 25 for detecting the presence or absence of light from the light source 23 are respectively arranged. Note that a radiation source 22. is provided on the upper frame 2Ib side. The light source 23 is placed on the lower frame 21a side, and the radiation detector 2 is placed on the side of the lower frame 21a.
4. A configuration in which the plate edge detectors 25 are respectively arranged may also be used.

図中、26は台車駆動用モータ、27け台車位置検出器
である。板端検出器25は例えばIJ ニアアレイカメ
ラを使用する。
In the figure, 26 is a motor for driving a cart, and 27 is a cart position detector. The plate edge detector 25 uses, for example, an IJ near array camera.

次に、信号処理系は第7図のように構成される。この信
号処理系は、放射線測定系30と、測定点検出部40と
、プロフィル演算部50と、リミットスイッチ等によっ
て被測定物のライン中央を検出するライン中央検出スイ
ッチ60と、速度変更検出部70と、台車制御部80と
、台車折返し検出部90と、台車駆動用モータ26とで
構成されている。
Next, the signal processing system is configured as shown in FIG. This signal processing system includes a radiation measurement system 30, a measurement point detection section 40, a profile calculation section 50, a line center detection switch 60 that detects the line center of the object to be measured using a limit switch, etc., and a speed change detection section 70. , a truck control section 80, a truck return detection section 90, and a truck drive motor 26.

前記放射線測定系30は、放射線検出器24により検出
された信号と予め設定された被測定物の中央部板厚すの
信号とから偏差を求めて被10− 測定物の中央部板厚およびエツジ部板厚のための信号を
出力する。即ち、この放射線測定系30は、放射線源2
2からの放射線量を検出し電気的なアナログ信号に変換
する放射線検出器24が設けられ、この放射線検出器2
4の出力は前置増幅器31によって増幅される。前置増
幅器31の出力側にはA−D変換回路32が接続され、
ここで増幅出力をディジタル信号に変換して後続の信号
処理回路33に供給する。この信号処理回路33は、A
−D変換回路32からディジタル信号を受けると、その
ディジタル信号と予め設定された被測定物の中央部板厚
すの信号とから偏差を求めてその偏差信号を後続のD−
A変換回路34に供給しここでアナログ信号に変換して
プロフィル演算部50に入力する構成である。
The radiation measuring system 30 calculates the deviation from the signal detected by the radiation detector 24 and the preset signal of the center plate thickness of the object to be measured, and determines the center plate thickness and edge of the object to be measured. Outputs a signal for part thickness. That is, this radiation measurement system 30 includes a radiation source 2
A radiation detector 24 that detects the radiation dose from 2 and converts it into an electrical analog signal is provided, and this radiation detector 2
The output of 4 is amplified by preamplifier 31. An A-D conversion circuit 32 is connected to the output side of the preamplifier 31,
Here, the amplified output is converted into a digital signal and supplied to the subsequent signal processing circuit 33. This signal processing circuit 33 is
- When a digital signal is received from the D-conversion circuit 32, a deviation is calculated from the digital signal and a preset signal of the thickness of the center part of the object to be measured, and the deviation signal is used as a signal for the subsequent D-
The configuration is such that the signal is supplied to the A conversion circuit 34, where it is converted into an analog signal and input to the profile calculation section 50.

次に、測定点検出部60は、第8図に示す測定点口(第
1図のエツジ部板厚&、eに和尚する)を検出するもの
である。この検出部6oは、測定点口を中心に一定範囲
を連続的に測定する板端検出器25と、板端から測定点
1つまり第1図のaまたはa、cの両方の距離を設定す
る測定点設定器4Iと、板端検出器25の出力と測定点
設定器41の設定値とを比較し一致したとき一致信号を
出力する比較回路42とで構成されている。プロフィル
演算部50は一致へ号を受けて被測定板の厚み測定値、
すAわち第1図のエツジ部板厚a、cを求める。
Next, the measurement point detection section 60 detects the measurement point opening shown in FIG. 8 (corresponding to the edge part plate thickness &, e in FIG. 1). This detection unit 6o sets the distance from the plate edge to the plate edge detector 25, which continuously measures a certain range around the measurement point opening, that is, the measurement point 1, that is, a or both a and c in Fig. 1. It is comprised of a measurement point setter 4I and a comparison circuit 42 that compares the output of the board end detector 25 and the set value of the measurement point setter 41 and outputs a coincidence signal when they match. In response to the matching signal, the profile calculation unit 50 calculates the thickness measurement value of the plate to be measured;
In other words, find the edge plate thicknesses a and c in FIG.

次K、速度変更制御部70は、第8図に示す速度変更点
イを検出して台車制御部80へ減速指令信号を与える機
能を持っている。即ち、この速度変更制御部70は、例
えば位置検出用ラックにかみ合ったピニオンギヤの回転
数に対応した/4’ルスを出力するノ4ルス発信器を持
った台車位置検出器27と、ライン中央検出スイッチ6
0からの信号でリセットされた後、台車位置検出器27
のパルスを計ししてライン中央からの位置信号を州るア
ップ・ダウンカウンタ71と、速度変更点イを設定する
速度変更点設定器72と、ライン中央CL(第8図参照
)がらの台車位置信号と速度変更点設定値とを比較する
比較回路73とからなり、この比較回路73の一致信号
を減速指令信号として台車制御部80に供給する。この
台車制御部80は、ライン中央CL、速度変更点イ、折
返し点ハの情報に従って台車駆動用モータ26へ速度制
御のための信号を与える機能をもっている。
Next, the speed change control section 70 has a function of detecting the speed change point A shown in FIG. 8 and providing a deceleration command signal to the bogie control section 80. That is, this speed change control section 70 includes, for example, a bogie position detector 27 having a 4' las transmitter that outputs a 4' lus that corresponds to the rotational speed of a pinion gear engaged with a position detection rack, and a line center detector. switch 6
After being reset with the signal from 0, the bogie position detector 27
an up/down counter 71 that measures the pulses of and outputs a position signal from the center of the line, a speed change point setter 72 that sets the speed change point A, and a trolley including the line center CL (see Figure 8). It consists of a comparison circuit 73 that compares the position signal and the speed change point set value, and the coincidence signal of this comparison circuit 73 is supplied to the bogie control section 80 as a deceleration command signal. This bogie control section 80 has a function of giving a signal for speed control to the bogie drive motor 26 in accordance with information about the line center CL, speed change point A, and turning point C.

前記台車U1返し検出部90は、板端検出器25の出力
と第8図に示す折返し点ハを設定する折返し黒膜定器9
1の出力とを比較回路92で比較し一致したとき一致信
号を出力する構成である。台車制御部80は、比較回路
92から一致信号を受けると、台車駆動用モータ26へ
後退速度信号を出力する。
The bogie U1 return detection section 90 includes a return black film gauge 9 that sets the output of the board end detector 25 and the return point C shown in FIG.
This configuration is such that a comparison circuit 92 compares the output of the output signal 1 with the output of the output signal 1, and outputs a match signal when they match. When the trolley control unit 80 receives the match signal from the comparison circuit 92, it outputs a backward speed signal to the trolley drive motor 26.

次に、以上のように構成された放射線厚み計の作用を説
明する。通常、放射級厚与引は、Cフレーム21の移動
によって放射線源22と放射線検出器24との中心軸線
が被測定物91の中央部にUkするように設定される。
Next, the operation of the radiation thickness meter configured as above will be explained. Normally, the radiometric thickness is set so that the central axes of the radiation source 22 and the radiation detector 24 are aligned to the center of the object to be measured 91 due to the movement of the C frame 21.

従って、このとき、ライン中央検出スイッチ6oの信号
13− に基づいてプロフィル演算部50は放射線測定系30の
出力から中央部板厚を求めることになる。この場合の測
定動作は次のようになる。即ち、放射線源22から照射
された放射線は被測定板91を透過して放射線検出器2
4に入射される。放射線検出器24は入射された放射線
量に比例する電気的なアナログ信号に変換した後、前置
増幅器31に供給する。この前置増幅器31によって増
幅された信号はA−D変換回路32でディジタル信号に
変換され信号処理回路33に供給される。この信号処理
回路33はA−D変換回路32の出力と予め設定された
被測定板91の中央部板厚すとから被測定板中央部の厚
みの偏差信号を求めた後、D−A変換回路34に供給す
る。ここで、同回路34は再びアナログ信号に変換して
プロフィル演算部soK供給する。このプロフィル演算
部5θは既11C5イン中央検出スイッチ60から検出
信号が入っているので、この信号に基づいてD−A変換
回路34の出力から中央部板厚すを求めるもので14− ある。
Therefore, at this time, the profile calculation section 50 calculates the center plate thickness from the output of the radiation measurement system 30 based on the signal 13- of the line center detection switch 6o. The measurement operation in this case is as follows. That is, the radiation emitted from the radiation source 22 passes through the plate 91 to be measured and reaches the radiation detector 2.
4. The radiation detector 24 converts the incident radiation dose into an electrical analog signal proportional to the amount of radiation, and supplies the signal to the preamplifier 31 . The signal amplified by this preamplifier 31 is converted into a digital signal by an A/D conversion circuit 32 and supplied to a signal processing circuit 33. This signal processing circuit 33 calculates a deviation signal of the thickness of the center part of the board to be measured from the output of the A-D converter circuit 32 and the preset thickness of the center part of the board to be measured 91, and then performs D-A conversion. Supplied to circuit 34. Here, the same circuit 34 converts it into an analog signal again and supplies it to the profile calculation section soK. Since this profile calculation section 5.theta. receives a detection signal from the 11C5-in center detection switch 60, it calculates the center plate thickness from the output of the DA conversion circuit 34 based on this signal.

次に、外部からのプロフィル測定指令信号FSによって
Cフレーム台車21が移動するが、このとき既に次の設
定動作が行なわれている。
Next, the C frame truck 21 is moved by the profile measurement command signal FS from the outside, but at this time the next setting operation has already been performed.

つまり、速度変更点設定器72には速度変更点設定値イ
ー81測定点設定器41には測定点設定値ローS、折返
し恵投定器91には折返し恵投定値バーSがそれぞれ設
定されている。而して、これらの設定%72.41.9
1に設定値イーS、ローS、バーSが設定された後、上
述するようにプロフィル測定指令信号FSを入力すると
、台車制御部80は第9図(a)に示す速度Vlの前進
指令信号を台車駆動用モータ26に与える。この結果、
Cフレーム台車21は第8図に示すようにライン中央C
Lを開始点として速度V1で板端方向に向って前進する
。このとき、アップ・ダウンカウンタ71はライン中央
検出スイッチ60からの信号によって既にリセットされ
て計数可能状態にある。このため、カウンタ7ノは台車
位置検出器27の出力/4’ルスを計数し台車2Zがラ
イン中央CLからどの程度移動しているかの位置信号を
出力する。比較回路73は、そのカウンタ71からの位
置信号と速度変更点設定器72の速度変更点設定値イー
Sとを比較し、台車21が第8図に示す速度変更点イに
達したところで一致信号を出力する。
That is, the speed change point set value E 81 is set in the speed change point setter 72, the measurement point set value low S is set in the measurement point setter 41, and the return value bar S is set in the return value setting device 91, respectively. Therefore, these settings%72.41.9
1, the set values E S, LOW S, and S are set, and when the profile measurement command signal FS is input as described above, the trolley control unit 80 outputs the forward command signal at the speed Vl shown in FIG. 9(a). is applied to the trolley drive motor 26. As a result,
As shown in FIG. 8, the C frame truck 21
Starting from L, it moves forward toward the plate end at a speed of V1. At this time, the up/down counter 71 has already been reset by the signal from the line center detection switch 60 and is ready for counting. Therefore, the counter 7 counts the output/4' pulse of the truck position detector 27 and outputs a position signal indicating how far the truck 2Z has moved from the line center CL. The comparison circuit 73 compares the position signal from the counter 71 and the speed change point setting value E S of the speed change point setter 72, and outputs a match signal when the trolley 21 reaches the speed change point A shown in FIG. Output.

ここで、台車制御部80は一致信号を受けて第9図(a
)に示す速度V 2 (V2(Vl )を台車駆動用モ
ータ26に与え台車21の移動速度を下げる。
Here, the trolley control unit 80 receives the coincidence signal and FIG. 9(a)
) is applied to the cart drive motor 26 to reduce the moving speed of the cart 21.

一方、板端検出器25の視野は、第8図の二に示すよう
にし1jえば厚み測定点口を中心に速度変更点イの距離
をカバーする範囲となっている。
On the other hand, the field of view of the plate edge detector 25 is a range that covers the distance from the thickness measurement point 1j to the speed change point 1j as shown in FIG. 8-2.

例えば測定点口を板端から1511I+11、速度変更
点イを板端から50g1lとすれば、板端検出器25の
視野は被測定板91の走行方向Cと直交する方向に10
0謔となる。従って、板端検出器25の出力は、ライン
中央付近では光源23からの光は完全にさえぎられて零
となるが、板端検出器25は前述する検出視野を持って
いるので台車2Zが速度変更点イに達するまでには検出
出力が出始める。第9図(C)はその状態を示している
For example, if the measurement point opening is 1511I+11 from the plate edge and the speed change point A is 50g1l from the plate edge, the field of view of the plate edge detector 25 is 10 in the direction perpendicular to the running direction C of the plate 91 to be measured.
It will be 0 songs. Therefore, the output of the plate edge detector 25 becomes zero near the center of the line as the light from the light source 23 is completely blocked, but since the plate edge detector 25 has the aforementioned detection field of view, the output of the bogie 2Z is By the time change point A is reached, detection output begins to appear. FIG. 9(C) shows this state.

との板端検出器25の出力は常時比較回路42に供給さ
れている。そこで、比較回路42は板端検出器25の出
力と測定点設定器41の測定点設定値ローSとを比較し
ているが、台車21が測定点口に達したところで一致信
号が出力される。との一致信号を受けると、ゾロフィル
演算部50は放射線測定系30の出力から第1図に示す
エツジ部板厚aおよびCを求めて記憶出力する。但し、
後述するように台車2Zを折返して他端側の測定点口を
検出↑る場合には前記プロフィル演算部50はエツジ部
板厚aのみ求めて記憶する。更に、台車21が前進する
ことにより、板端検出器25の出力が折返し恵投定器9
Iの折返し恵投定値・・−8と一致すると、比較回路9
2から一致信号が出力される。
The output of the plate edge detector 25 is constantly supplied to the comparison circuit 42. Therefore, the comparison circuit 42 compares the output of the plate edge detector 25 and the measurement point set value low S of the measurement point setter 41, and a coincidence signal is output when the trolley 21 reaches the measurement point opening. . When receiving a coincidence signal, the Zorophil calculation unit 50 calculates the edge thicknesses a and C shown in FIG. 1 from the output of the radiation measurement system 30, and stores and outputs the calculated values. however,
As will be described later, when the cart 2Z is turned back and the measurement point at the other end is detected, the profile calculating section 50 calculates and stores only the edge plate thickness a. Furthermore, as the trolley 21 moves forward, the output of the plate end detector 25 is turned back to the projector 9.
If it matches the return estimate value of I...-8, the comparator circuit 9
A coincidence signal is output from 2.

これにより、台車制御部80は速度−vlの後退指令信
号を台車駆動用モータ26に与え台車21を後退させる
。そして、上記と同様な手段により、被測定物91の他
端側においてプロフィル演算部50は第1図に示すエツ
ジ部板厚Cを求めて記憶出力する。ここで、ライン中央
CLを中心に台車21が一往復して測定が終了すると、
台車制御部80は台車21をライン中央CLに停止させ
る。−万、ゾロフィル演算部50は、記憶値a、b、c
を用いてクラウン蓋。
As a result, the truck control unit 80 gives a backward command signal of speed -vl to the truck drive motor 26 to cause the truck 21 to move backward. Then, using the same means as described above, the profile calculating section 50 calculates the edge portion plate thickness C shown in FIG. 1 on the other end side of the object to be measured 91 and stores and outputs it. Here, when the cart 21 moves back and forth once around the line center CL and the measurement is completed,
The truck control unit 80 stops the truck 21 at the line center CL. -10,000, the Zorophil calculation unit 50 stores the stored values a, b, c.
Crown lid using.

ウェツゾ量等を計算して出力する。Calculates and outputs the wet amount, etc.

u上のように板端検出器25により被測定物91の板端
を検出し台車21を制御する方式では、被測定物91が
常に放射線ビーム内にあるので、板端から外れて検出す
ることもなく、応答遅れもない。また、測定点検出後、
放射線測定系の出力からエツジ部板厚を求めているので
、その板厚は正確であり、被測定板91の横振れ等の影
畳も受けない。なお、本実施例では省略されているが、
フ0ロフイル演算はライン中央CLに設置された固定用
厚み計の出力と、本実施911厚み計出力との差とをも
って行なう。従って、プロフィル演算部50の入力には
図示していないが、固定用厚み計の出力が必要であるこ
とは百うまでもない。
In the method shown above in which the plate edge of the object to be measured 91 is detected by the plate edge detector 25 and the trolley 21 is controlled, the object to be measured 91 is always within the radiation beam, so it is difficult to detect the object 91 off the edge of the plate. There is no delay in response. Also, after detecting the measurement point,
Since the thickness of the edge portion is determined from the output of the radiation measurement system, the thickness is accurate and is not affected by the effects of lateral vibration of the plate 91 to be measured. Although omitted in this example,
The flow calculation is performed using the difference between the output of the fixed thickness gauge installed at the center of the line CL and the output of the thickness gauge of this embodiment 911. Therefore, although not shown, it goes without saying that the output of the fixed thickness gauge is required as an input to the profile calculation section 50.

なお、本発明は上記実施例に限定されるものではない。Note that the present invention is not limited to the above embodiments.

例えば速度変更点イと折返し点−・との間に、第2およ
び第3の速度変更点を設け、折返し点ハでの台車速度を
充分減少させて台車21が板端を越え過ぎないようにす
ることができる。また、本装置は、ソフト的に処理でき
る部分はコンピュータを使用して実施できる。また、光
源23の光をミラー等で反射させて板端検出器25に導
くようにすれば、凹板端検出器25は放射線の影響を受
けない位置に設置できる。さらに、板端の距離が分って
いるので、被測定物91の板端付近の厚みを板端の変化
に追従させて測定することもできる。その他、本発明は
その要旨を逸脱しない範囲で種々変形して実施できる。
For example, a second and a third speed change point are provided between the speed change point A and the turning point -, and the speed of the cart at the turning point C is sufficiently reduced so that the cart 21 does not go over the edge of the plate. can do. Further, in this apparatus, the portions that can be processed by software can be implemented using a computer. Furthermore, if the light from the light source 23 is reflected by a mirror or the like and guided to the plate edge detector 25, the concave plate edge detector 25 can be installed at a position where it is not affected by radiation. Furthermore, since the distance between the plate edges is known, the thickness of the object 91 near the plate edge can be measured by following changes in the plate edge. In addition, the present invention can be implemented with various modifications without departing from the gist thereof.

発明の効果 以上詳記したように本発明によれは、ライン中央を検出
仮台車位置信号を測定しているため正確に台車の位置を
知ることができる。また、速度変更点設定値を設け、こ
の設定値と前記位置信号との比較により台車を減速制御
しているので、台車の測定点検出が容易であり、板端で
の台車の行き過ぎも防ぐことができる。また、板端検出
器の出力と各測定点設定器、折返し恵投定器出力との比
較結果圧基づいて測定点および折返し点を得ており、こ
のため板端に近い測定点の厚を応答遅れなく測定でき、
かつ被測定物の横振れの影響を受けずにプロフィルの測
定が可能である放射線厚み唱を提供できる0
Effects of the Invention As described in detail above, according to the present invention, the center of the line is detected and the temporary truck position signal is measured, so the position of the truck can be accurately known. In addition, since a speed change point set value is provided and the trolley is decelerated by comparing this set value with the position signal, it is easy to detect the measuring point of the trolley and prevent the trolley from overshooting at the edge of the plate. I can do it. In addition, the measurement points and turning points are obtained based on the pressure comparison results between the output of the sheet edge detector, each measuring point setter, and the output of the turning device. It can be measured without
Also, it can provide a radiation thickness measurement that allows profile measurement without being affected by the lateral vibration of the object to be measured.

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

第1図ないし第5図は従来の放射線厚み制を説明する図
であって、第1図は圧延鋤板の断面形状を表わす図、第
2図は機械系の構成図、第3図は信号処理系の構成図、
第4図(=)〜(C)および第5図は従来の放射線厚み
組の問題点を説明する図、第6図ないし第9図(a)〜
(c)は本発明に係る放射線厚み剖の一実施例を説明す
るための図であって、第6図は機械系の構成図、第7図
は信号処理系の構成図、第8図は被測定物の各検出点を
示す図、第9図(a)〜(C)は動作特性図である。 21・・・台車、22・・・放射線、23・・・光源、
24・・・放射線検出器、25・・・板端検出器、26
・・・台車駆動用モータ、27・・・台車位置検出器、
30・・・放射線測定系、33・・・信号処理回路、4
0・・・測定点検出部、4I・・・測定点設定器、42
・・・比較回路、50・・・プロフィル演算部、60・
・・ライン中央検出スイッチ、70・・・速度変更検出
部、71・・・カウンタ、72・・・速度変更点検出部
、80・・・台車制御部、90・・・折返し点検出部、
9I・・・折返し恵投定器。 出願人代理人  弁理士 鈴 江 武 彦第1図 第2図 ]a 第3図 ・□
Figures 1 to 5 are diagrams explaining the conventional radiation thickness system, in which Figure 1 is a diagram showing the cross-sectional shape of a rolling plow plate, Figure 2 is a configuration diagram of the mechanical system, and Figure 3 is a signal diagram. Processing system configuration diagram,
Figures 4 (=) to (C) and Figure 5 are diagrams explaining the problems of the conventional radiation thickness set, Figures 6 to 9 (a) to
(c) is a diagram for explaining one embodiment of radiation thickness analysis according to the present invention, in which FIG. 6 is a configuration diagram of a mechanical system, FIG. 7 is a configuration diagram of a signal processing system, and FIG. Figures 9(a) to 9(c) showing each detection point of the object to be measured are operational characteristic diagrams. 21... Trolley, 22... Radiation, 23... Light source,
24... Radiation detector, 25... Board edge detector, 26
... Bogie drive motor, 27... Bogie position detector,
30... Radiation measurement system, 33... Signal processing circuit, 4
0...Measuring point detector, 4I...Measuring point setter, 42
... Comparison circuit, 50 ... Profile calculation section, 60.
...Line center detection switch, 70... Speed change detection section, 71... Counter, 72... Speed change point detection section, 80... Bogie control section, 90... Turning point detection section,
9I...Folded Megumi projector. Applicant's agent Patent attorney Takehiko Suzue Figure 1 Figure 2]a Figure 3・□

Claims (2)

【特許請求の範囲】[Claims] (1)放射線検出系を備えた台車を移動させて被測定物
のプロフィルを測定する放射線厚み計において、前記被
測定物を透過して得られた放射&飯に比911する信号
と予め設定された被測定物の板厚信号との偏差を求める
放射線測定系と、ライン中央を検出するライン中央検出
手段と、前記台車に設置された台車位置検出器の出力を
、前記ライン中央検出手段によって検出した信号に基づ
いて測定して台車の位置信号とし、との位m侶号を用い
て前記被測定物の速度変更点を得る速度変更検出部と、
この速度変更検出部の出力に基づいて台車の速度を降下
させる手段と、前記台車に板端検出器を設け、この検出
器出力と予め設定した測定点設定値とから被測定物のエ
ッソ部&厚の測定タイミングを得る測定点検出部と、前
記ライン中央検出手段で得た検出信号および前記エツジ
部板厚の測定タイミングに基づいて、前記放射線測定系
から出力される偏差信号により被測定物のプロフィルを
測定するプロフィル演算部とを備えたことを特徴とする
放射線厚み制。
(1) In a radiation thickness meter that measures the profile of an object by moving a cart equipped with a radiation detection system, a signal that is preset to be 911 compared to the radiation obtained by passing through the object. a radiation measurement system for determining the deviation from a plate thickness signal of the object to be measured, a line center detection means for detecting the center of the line, and an output of a cart position detector installed on the cart, which is detected by the line center detection means. a speed change detection unit that measures the position signal of the trolley based on the signal and obtains a speed change point of the object to be measured using the second position;
A means for reducing the speed of the cart based on the output of the speed change detection section and a plate edge detector are provided on the cart, and the esso portion & Based on the measurement point detection section that obtains the thickness measurement timing, the detection signal obtained by the line center detection means, and the measurement timing of the edge portion plate thickness, the deviation signal output from the radiation measurement system is used to detect the object to be measured. A radiation thickness system characterized by comprising a profile calculation section that measures a profile.
(2)  放射線検出系を備えた台車を移動させて被測
定物のプロフィルを測定する放射線厚み計において、前
記被測定物を透過して得られた放射線量に比例する信号
と予め設定された被測定物の板厚信号との偏差を求める
放射線測定系と、ライン中央を検出するライン中央検出
手段と、前記台車に設置された台車位置検出器の出力を
、前記ライン中央検出手段によって検出した信号に基づ
いて測定して台車の位置信号としこの位置信号を用いて
前記被測定物の速度変更点を得る速度変更検出部と、こ
の速度変更検出部の出力に基づいて台車の速度を降下さ
せる手段と、前記台車に板端検出器を設けこの検出器出
力と予め設定した測定点設定値とから被測定物の一方の
エツジ部板厚の測定タイミングを得る測定点検山部と、
前記板端検出器の出力と予め設定した台車折返し黒膜定
値とから被測定物の折返し点を検出して台車を反対側の
板端へ進行させ唖台車折返し検出部と、台車の折返し後
、前記測定点検出器の出力を用いて被測定物の他方のエ
ツジ部板厚の測定タイミングを得る手段と、前記ライン
中央検出手段で得た検出信号および両エツジ部板厚の測
定タイミングに基づいて、前記放射線測定系から出力さ
れる偏差信号により被測定物のプロフィルを測定するプ
ロフィル演算部とを備えたことを特徴とする放射線厚み
計。
(2) In a radiation thickness meter that measures the profile of an object by moving a cart equipped with a radiation detection system, a signal proportional to the radiation dose obtained by passing through the object and a preset radiation a radiation measurement system for determining the deviation from a plate thickness signal of the object to be measured; a line center detection means for detecting the center of the line; and a signal detected by the line center detection means from the output of a cart position detector installed on the cart. a speed change detection section that measures the position of the cart based on the position signal and uses this position signal to obtain a speed change point of the object to be measured; and means for reducing the speed of the cart based on the output of the speed change detection section. and a measurement inspection peak part in which a plate edge detector is provided on the cart and the timing of measuring the plate thickness of one edge part of the object to be measured is obtained from the output of the detector and a preset measurement point setting value;
Detecting the turning point of the object to be measured from the output of the plate end detector and a preset cart turning black film constant value, moving the cart to the opposite plate end, and connecting the cart to the turning point detecting section; means for obtaining the measurement timing of the thickness of the other edge portion of the object to be measured using the output of the measurement point detector; and a means for obtaining the measurement timing of the thickness of the other edge portion of the object to be measured based on the detection signal obtained by the line center detection means and the measurement timing of the thickness of both edge portions. . A radiation thickness meter comprising: a profile calculation section that measures the profile of the object based on the deviation signal output from the radiation measurement system.
JP20424781A 1981-12-17 1981-12-17 Radiation thickness gauge Pending JPS58105008A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP20424781A JPS58105008A (en) 1981-12-17 1981-12-17 Radiation thickness gauge

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP20424781A JPS58105008A (en) 1981-12-17 1981-12-17 Radiation thickness gauge

Publications (1)

Publication Number Publication Date
JPS58105008A true JPS58105008A (en) 1983-06-22

Family

ID=16487286

Family Applications (1)

Application Number Title Priority Date Filing Date
JP20424781A Pending JPS58105008A (en) 1981-12-17 1981-12-17 Radiation thickness gauge

Country Status (1)

Country Link
JP (1) JPS58105008A (en)

Cited By (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS60177202A (en) * 1984-02-23 1985-09-11 Toshiba Mach Co Ltd Scanning type transmission thickness gage

Cited By (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS60177202A (en) * 1984-02-23 1985-09-11 Toshiba Mach Co Ltd Scanning type transmission thickness gage

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