JPS6253043B2 - - Google Patents
Info
- Publication number
- JPS6253043B2 JPS6253043B2 JP56099353A JP9935381A JPS6253043B2 JP S6253043 B2 JPS6253043 B2 JP S6253043B2 JP 56099353 A JP56099353 A JP 56099353A JP 9935381 A JP9935381 A JP 9935381A JP S6253043 B2 JPS6253043 B2 JP S6253043B2
- Authority
- JP
- Japan
- Prior art keywords
- radiation
- steel plate
- radiation detector
- radiation source
- width direction
- 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
Links
- 230000005855 radiation Effects 0.000 claims description 82
- 238000005259 measurement Methods 0.000 claims description 18
- 239000000463 material Substances 0.000 claims description 10
- 229910000831 Steel Inorganic materials 0.000 description 39
- 239000010959 steel Substances 0.000 description 39
- 238000005096 rolling process Methods 0.000 description 8
- 238000012935 Averaging Methods 0.000 description 3
- 230000007423 decrease Effects 0.000 description 3
- 238000001514 detection method Methods 0.000 description 3
- 230000005856 abnormality Effects 0.000 description 2
- 230000002238 attenuated effect Effects 0.000 description 2
- 239000002131 composite material Substances 0.000 description 2
- 238000010586 diagram Methods 0.000 description 2
- XAGFODPZIPBFFR-UHFFFAOYSA-N aluminium Chemical compound [Al] XAGFODPZIPBFFR-UHFFFAOYSA-N 0.000 description 1
- 229910052782 aluminium Inorganic materials 0.000 description 1
- 230000007547 defect Effects 0.000 description 1
- 230000002950 deficient Effects 0.000 description 1
- 230000003111 delayed effect Effects 0.000 description 1
- 230000000694 effects Effects 0.000 description 1
- 238000000034 method Methods 0.000 description 1
Classifications
-
- G—PHYSICS
- G01—MEASURING; TESTING
- G01B—MEASURING LENGTH, THICKNESS OR SIMILAR LINEAR DIMENSIONS; MEASURING ANGLES; MEASURING AREAS; MEASURING IRREGULARITIES OF SURFACES OR CONTOURS
- G01B15/00—Measuring arrangements characterised by the use of electromagnetic waves or particle radiation, e.g. by the use of microwaves, X-rays, gamma rays or electrons
- G01B15/02—Measuring 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
- G01B15/025—Measuring 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 by measuring absorption
Landscapes
- Physics & Mathematics (AREA)
- Electromagnetism (AREA)
- General Physics & Mathematics (AREA)
- Length-Measuring Devices Using Wave Or Particle Radiation (AREA)
- Analysing Materials By The Use Of Radiation (AREA)
Description
【発明の詳細な説明】
本発明は鋼板その他の板材の断面形状を測定す
る装置に関する。
一般に鋼板の圧延工程では圧延された鋼板の断
面形状を測定し、この断面形状から圧延等の状態
を求めて圧延の工程管理等をおこなつている。従
来このような鋼板等の断面形状を測定する装置は
第1図に示す如きものが用いられている。すなわ
ち、1はフレームであつて走査駆動機構2によつ
て測定すべき板材たとえば鋼板3の幅方向に所定
の走査速度で移動されるように構成されている。
このフレーム1には放射線源4が設けられ、この
放射線源4から上記鋼板3に向けて放射線ビーム
が照射される。また、このフレーム1には放射線
検出器5が設けられており、この放射線検出器5
は鋼板3を介して放射線源4に対向している。そ
して、上記放射線源4から放射された放射線ビー
ムは鋼板3を透過して放射線検出器5に入射する
ように構成されている。この放射線ビームが鋼板
3を透過する際には鋼板3の厚さに対応して減衰
するので、放射線検出器5で線量を検出して放射
線ビームの減衰を求めることにより鋼板3の厚さ
を検出できる。そしてこの放射線源4および放射
線検出器5は走査駆動機構2によつて鋼板3の幅
方向に移動されるので、鋼板停止時の測定では鋼
板長手方向と直交する鋼板幅方向の板厚が連続的
に求められ、また鋼板走行時の測定では鋼板長手
方向(走行方向)に対して斜め方向の板厚が幅方
向の擬似板厚として連続的に求められ、よつてこ
の鋼板3の断面板厚形状が求められる。ところ
で、このような断面板厚形状の分解能を上げるに
は放射線ビームをできるだけ鋭いものにしなけれ
ばならない。しかし、この放射線ビームを絞ると
放射線量が減少するため線源に起因する統計雑音
が増大し、測定精度を損なう。このため従来は放
射線ビームをあまり鋭くすることはできず、分解
能、精度の向上に限界があつた。また、たとえば
圧延ロールに傷が生じた場合には第2図に示す如
く鋼板3の表面上に小突起6が形成される。しか
し、このような小突起6の検出信号は外部から加
わる単発的な雑音と区別することができない。こ
のため従来は複数回の走査にわたつて一定してこ
のような小突起6に対応した信号があつた場合に
のみはじめて小突起6がある旨の判定をせざるを
得ず、このような小突起6の発生すなわち圧延ロ
ールの異常の発見が遅れ、多くの不良製品を発生
させてしまう不具合があつた。
本発明は以上の事情にもとづいてなされたもの
で、その目的とするところは板材の断面板厚形状
を正確かつ確実に測定することができる装置を得
ることにある。
以下本発明を第3図に示す一実施例にしたがつ
て説明する。図中101はフレームであつて、そ
の形状は略コ字状をなしている。そして、このフ
レーム101は走査駆動機構102によつて測定
すべき板材たとえば鋼板103の幅方向に所定の
走査速度で移動されるように構成されている。そ
して、このフレーム101の下部には放射線源1
04が設けられており、この放射線源104から
は上記鋼板103に向けて放射線ビーム105が
放射される。また、このフレーム101には複数
個の放射線検出器106……が設けられており、
これら放射線検出器106……は上記鋼板103
を介して放射線源104……に対向している。そ
して、これら放射線検出器106……は一直線上
に配列されており、その配列方向は上記フレーム
101の走査駆動方向と一致している。そして、
上記放射線源104から放射された放射線ビーム
105は鋼板103を透過して各放射線検出器1
06……に入射するように構成されている。そし
て、各放射線検出器106……にそれぞれ入射す
る単位放射線ビーム105a……は充分な分解能
が得られるように鋭いビームとなつている。そし
て、これら各放射線検出器106……は入射した
放射線量に対応した信号を出力し、これらの信号
はそれぞれ信号処理回路107に送られるように
構成されている。また、前記走査駆動機構102
からはフレーム101の走査位置に対応した位置
信号が上記信号処理回路107に送られるように
構成されている。また、この信号処理回路107
にはフレーム101上に設定された測定基準点か
ら各放射線検出器106……までの走査方向の距
離から各放射線検出器の測定距離(測定幅方向距
離)があらかじめ入力されている。そして、この
信号処理回路107では上記走査駆動回路102
から送られる位置信号からその時の走査速度を求
め、上記基準点から各放射線検出器106……ま
での測定距離をそれぞれこの走査速度で除し、各
放射線検出器106……毎に測定時間差を算出す
る。そして、上記各放射線検出器106……から
送られてくる信号をそれぞれ上記測定時間差を相
殺するようにずらすとともにこれらの信号レベル
を平均し、ひとつの信号に合成する。そして、こ
の合成された信号と位置信号とから鋼板103の
断面形状を求め、これを記録表示機構108に記
録表示させるように構成されている。
以上の如く構成された本発明の一実施例は、放
射線源104から放射された放射線ビーム105
は鋼板103を透過する際にこの鋼板103の板
厚に対応して減衰され、各放射線検出器106…
…に入射する。そして各放射線検出器106……
は入射した放射線量に対応した信号が出力され、
この信号が信号処理回路107に送られて合成さ
れ、この放射線ビーム105が透過した位置の鋼
板103の板厚が測定される。そして、これら放
射線源104および放射線検出器106……は走
査駆動機構102によつてフレーム101ととも
に走査され、鋼板103の幅方向の板厚が連続的
に測定され、この鋼板103の断面板厚形状が求
められる。そして、このものは各放射線検出器1
06……に入射する単位放射線ビーム105a…
…を充分に鋭くして分解能を上げることができ、
かつこのようにビームを鋭くしても精度を低下さ
せることがなく、また圧延ローラの傷等により発
生する小突起の如き欠陥も確実に検出できる。以
下その理由を説明する。すなわち放射線検出器に
入射する放射線ビームを鋭くすることにより分解
能を上げることができるが、その反面統計雑音が
増大して精度が低下することは前述した通りであ
る。ところで、この一実施例のものは複数の放射
線検出器106……が走査方向に配列されている
ので、各放射線検出器106……が鋼板103上
の任意の測定位置に対応した位置を通過する時刻
はそれぞれ異なる。そしてこれらの時間差は前述
した如き測定基準点から各放射線検出器106…
…までの距離を走査速度で除して得られた測定時
間差に等しい。よつて各放射線検出器106……
からの信号を測定時間差だけずらして平均化すれ
ばこれら時間的にずれた信号をひとつの信号に合
成できる。その結果、鋼板停止時の測定では、鋼
板長手方向とほぼ直交する鋼板幅方向の複数の同
一位置信号を例えば相加平均して合成された合成
板厚信号が得られ、また鋼板走行時の測定では鋼
板長手方向に対して斜め方向の鋼板幅方向の複数
の同一位置信号を例えば相加平均して合成された
擬似合成板厚信号が得られる。ところで、前記の
統計雑音は放射線源104側に起因するものであ
るから各放射線検出器106……に同時に入る。
しかるにこれら放射線検出器106……からの信
号はそれぞれ異なる測定時間差だけずらされて合
成されるので、この同時に入つた統計雑音は平均
化され、放射線検出器106……の数をNとすれ
ば1/√に減少する。よつて単位放射線ビーム
105a……を鋭くして分解能を上げてその反面
統計雑音が増大してもこの統計雑音の影響が減少
するので、精度を損なうことはない。また、外部
からの雑音も各放射線検出器106……に同時に
入るので上記と同様にその影響が減少し、前述し
た小突起に対応した信号との判別が容易となるの
でこのような小突起の発生すなわち圧延ロールの
異常を早期に発見できるものである。
なお、本発明は上記の一実施例には限定されな
い。
たとえば各放射線検出器からの信号は必らずし
も測定時間差だけずらしてから平均化するだけで
なく、各放射線検出器毎に走査が終了するまで記
憶しておいて各放射線検出器毎の断面板厚形状を
求め、これらを測定基準点から各放射線検出器ま
での距離に対応してそれぞれずらして合成しても
よい。但し、この場合は走査駆動機構102によ
る移動速度を記憶しているか、あるいは走査駆動
機構102による移動速度と各放射線検出器の測
定距離とが一定の関係を保持しているものとす
る。
また鋼板の幅方向中央部の板厚を測定する固定
形厚さ計と組み合せて圧延中の鋼板のクラウンを
測定できるようにしてもよい。
さらに本発明は鋼板に限らずアルミニウム板そ
の他の板材の断面板厚形状測定装置一般に適用で
きる。
上述の如く本発明は複数の放射線検出器を走査
方向に配列し、これら放射線検出器からの信号を
信号処理回路で時間的あるいは図形的にずらして
合成するものである。よつて放射線源側に起因す
る統計雑音や外部からの雑音等各放射線検出器に
同時に入る雑音は平均化され、その影響が減少す
る。したがつて放射線ビームを鋭くして分解能を
上げてもビームを鋭くしたことによる統計雑音の
増大等を減殺し、精度を損なうことなく分解能を
上げることができる。また外部からの雑音の影響
が小さくなるので、この外部からの雑音と紛らわ
しい小突起の検出も確実におこなうことができる
等その効果は大である。 DETAILED DESCRIPTION OF THE INVENTION The present invention relates to an apparatus for measuring the cross-sectional shape of steel plates and other plate materials. Generally, in the process of rolling a steel plate, the cross-sectional shape of the rolled steel plate is measured, and the rolling conditions are determined from this cross-sectional shape to control the rolling process. Conventionally, an apparatus as shown in FIG. 1 has been used to measure the cross-sectional shape of such steel plates. That is, reference numeral 1 denotes a frame, which is configured to be moved by a scanning drive mechanism 2 at a predetermined scanning speed in the width direction of a plate material to be measured, such as a steel plate 3.
This frame 1 is provided with a radiation source 4, and a radiation beam is irradiated from this radiation source 4 toward the steel plate 3. Further, this frame 1 is provided with a radiation detector 5, and this radiation detector 5
is opposed to the radiation source 4 via the steel plate 3. The radiation beam emitted from the radiation source 4 is configured to pass through the steel plate 3 and enter the radiation detector 5. When this radiation beam passes through the steel plate 3, it is attenuated in accordance with the thickness of the steel plate 3, so the thickness of the steel plate 3 is detected by detecting the dose with the radiation detector 5 and determining the attenuation of the radiation beam. can. Since the radiation source 4 and the radiation detector 5 are moved in the width direction of the steel plate 3 by the scanning drive mechanism 2, the thickness in the width direction of the steel plate perpendicular to the longitudinal direction of the steel plate is continuous during measurement when the steel plate is stopped. In addition, in the measurement when the steel plate is running, the plate thickness in the diagonal direction with respect to the longitudinal direction (travel direction) of the steel plate is continuously determined as the pseudo thickness in the width direction. is required. By the way, in order to increase the resolution of such a cross-sectional plate thickness shape, the radiation beam must be made as sharp as possible. However, when this radiation beam is narrowed down, the radiation dose decreases, and statistical noise caused by the radiation source increases, impairing measurement accuracy. For this reason, in the past, it was not possible to make the radiation beam very sharp, and there was a limit to the improvement of resolution and accuracy. Further, for example, when a scratch occurs on a rolling roll, small protrusions 6 are formed on the surface of the steel plate 3 as shown in FIG. However, such a detection signal of the small protrusion 6 cannot be distinguished from a single noise added from the outside. For this reason, conventionally, the presence of a small protrusion 6 had to be determined only when a signal corresponding to such a small protrusion 6 was consistently received over multiple scans; There was a problem in that the occurrence of the protrusions 6, that is, the detection of abnormalities in the rolling rolls was delayed, resulting in a large number of defective products. The present invention has been made based on the above-mentioned circumstances, and its object is to obtain an apparatus that can accurately and reliably measure the cross-sectional thickness shape of a plate material. The present invention will be explained below with reference to an embodiment shown in FIG. In the figure, reference numeral 101 denotes a frame, which has a substantially U-shape. The frame 101 is configured to be moved by a scanning drive mechanism 102 at a predetermined scanning speed in the width direction of a plate material, such as a steel plate 103, to be measured. A radiation source 1 is provided at the bottom of this frame 101.
04 is provided, and a radiation beam 105 is emitted from this radiation source 104 toward the steel plate 103. Further, this frame 101 is provided with a plurality of radiation detectors 106...
These radiation detectors 106... are the steel plates 103
The radiation source 104 faces the radiation source 104 through. These radiation detectors 106 . . . are arranged in a straight line, and the arrangement direction matches the scanning drive direction of the frame 101. and,
Radiation beam emitted from the radiation source 104
105 is transmitted through the steel plate 103 to each radiation detector 1
06... is configured to be incident. The unit radiation beams 105a that are incident on each of the radiation detectors 106 are sharp beams so as to obtain sufficient resolution. Each of these radiation detectors 106 outputs a signal corresponding to the amount of incident radiation, and these signals are each sent to a signal processing circuit 107. Further, the scanning drive mechanism 102
From there, a position signal corresponding to the scanning position of the frame 101 is sent to the signal processing circuit 107. Moreover, this signal processing circuit 107
The measurement distance (measurement width direction distance) of each radiation detector is input in advance from the distance in the scanning direction from the measurement reference point set on the frame 101 to each radiation detector 106 . In this signal processing circuit 107, the scanning drive circuit 102
Find the scanning speed at that time from the position signal sent from the reference point, divide the measured distance from the reference point to each radiation detector 106 by this scanning speed, and calculate the measurement time difference for each radiation detector 106... do. Then, the signals sent from each of the radiation detectors 106 are shifted so as to cancel out the measurement time difference, and the signal levels are averaged and combined into one signal. Then, the cross-sectional shape of the steel plate 103 is determined from the combined signal and the position signal, and the recording and display mechanism 108 records and displays this. One embodiment of the present invention configured as described above has a radiation beam 105 emitted from a radiation source 104.
When transmitted through the steel plate 103, it is attenuated in accordance with the thickness of the steel plate 103, and each radiation detector 106...
It is incident on... And each radiation detector 106...
outputs a signal corresponding to the incident radiation dose,
This signal is sent to a signal processing circuit 107 and synthesized, and the thickness of the steel plate 103 at the position through which this radiation beam 105 has passed is measured. These radiation sources 104 and radiation detectors 106 are scanned together with the frame 101 by the scanning drive mechanism 102, and the thickness of the steel plate 103 in the width direction is continuously measured, and the cross-sectional thickness shape of the steel plate 103 is is required. And this one is for each radiation detector 1
06... Unit radiation beam 105a... incident on...
... can be made sufficiently sharp to increase resolution,
Furthermore, even if the beam is sharpened in this way, the accuracy will not be reduced, and defects such as small protrusions caused by scratches on rolling rollers can be reliably detected. The reason will be explained below. That is, by sharpening the radiation beam incident on the radiation detector, the resolution can be increased, but as described above, on the other hand, statistical noise increases and accuracy decreases. By the way, in this embodiment, a plurality of radiation detectors 106... are arranged in the scanning direction, so each radiation detector 106... passes through a position corresponding to an arbitrary measurement position on the steel plate 103. Times vary. These time differences are calculated from the measurement reference point as described above to each radiation detector 106...
It is equal to the measurement time difference obtained by dividing the distance to ... by the scanning speed. Therefore, each radiation detector 106...
By shifting the signals from each other by the measurement time difference and averaging them, these time-shifted signals can be combined into a single signal. As a result, in measurements when the steel plate is stopped, a composite plate thickness signal can be obtained, for example, by arithmetic averaging of multiple signals at the same position in the width direction of the steel plate, which is approximately perpendicular to the longitudinal direction of the steel plate, and in measurements when the steel plate is running. In this case, a pseudo composite plate thickness signal is obtained by, for example, arithmetic averaging a plurality of signals at the same position in the width direction of the steel plate in a diagonal direction with respect to the longitudinal direction of the steel plate. By the way, since the above-mentioned statistical noise originates from the radiation source 104 side, it enters each radiation detector 106 at the same time.
However, since the signals from these radiation detectors 106 are synthesized after being shifted by different measurement time differences, the statistical noise that enters at the same time is averaged, and if the number of radiation detectors 106 is N, then it is 1. /√ decreases. Therefore, even if the unit radiation beams 105a are sharpened to increase the resolution and, on the other hand, increase the statistical noise, the influence of this statistical noise is reduced, so there is no loss of accuracy. In addition, since external noise also enters each radiation detector 106 at the same time, its influence is reduced in the same way as above, and it becomes easy to distinguish the signal from the signal corresponding to the small protrusion mentioned above. This allows early detection of abnormalities in the rolling rolls. Note that the present invention is not limited to the above embodiment. For example, the signals from each radiation detector are not necessarily averaged after being shifted by the measurement time difference, but they are also stored until the end of scanning for each radiation detector, and the signals from each radiation detector are The face plate thickness shapes may be obtained, and these may be synthesized by shifting them corresponding to the distances from the measurement reference point to each radiation detector. However, in this case, it is assumed that the moving speed of the scanning drive mechanism 102 is stored or that the moving speed of the scanning drive mechanism 102 and the measured distance of each radiation detector maintain a constant relationship. Further, it may be possible to measure the crown of the steel plate during rolling by combining it with a fixed thickness gage that measures the thickness of the central portion of the steel plate in the width direction. Further, the present invention is applicable not only to steel plates but also to general cross-sectional plate thickness shape measuring devices for aluminum plates and other plate materials. As described above, the present invention arranges a plurality of radiation detectors in the scanning direction, and synthesizes the signals from these radiation detectors by shifting them temporally or graphically using a signal processing circuit. Therefore, noises that simultaneously enter each radiation detector, such as statistical noise caused by the radiation source and noise from the outside, are averaged, and their influence is reduced. Therefore, even if the resolution is increased by sharpening the radiation beam, the increase in statistical noise due to the sharpening of the beam can be reduced, and the resolution can be increased without compromising accuracy. Furthermore, since the influence of external noise is reduced, small protrusions that may be confused with external noise can be detected reliably, which has great effects.
第1図は従来例の概略構成図、第2図は板材の
断面図である。第3図は本発明の一実施例の概略
構成図である。
101……フレーム、102……走査駆動機
構、103……鋼板(板材)、104……放射線
源、106……放射線検出器、107……信号処
理回路。
FIG. 1 is a schematic configuration diagram of a conventional example, and FIG. 2 is a sectional view of a plate material. FIG. 3 is a schematic diagram of an embodiment of the present invention. 101... Frame, 102... Scanning drive mechanism, 103... Steel plate (plate material), 104... Radiation source, 106... Radiation detector, 107... Signal processing circuit.
Claims (1)
に測定すべき板材を介して対向し直線上に配列さ
れた複数の放射線検出器と、上記放射線源および
放射線検出器をこの放射線検出器の配列方向に移
動させる走査機構と、この走査機構による移動速
度と上記放射線検出器の測定距離とに基づいて各
放射線検出器の出力をずらして上記板材幅方向の
同一位置のデータを得るとともに、この同一位置
のデータを合成して上記板材の断面形状を求める
信号処理回路とを具備したことを特徴とする板材
の断面板厚形状測定装置。1. A radiation source that emits radiation, a plurality of radiation detectors arranged in a straight line facing this radiation source through a plate to be measured, and the radiation source and the radiation detector arranged in the arrangement direction of the radiation detectors. A scanning mechanism is used to shift the output of each radiation detector based on the speed of movement by this scanning mechanism and the measurement distance of the radiation detector to obtain data at the same position in the width direction of the plate material, and data at the same position in the width direction of the board is obtained. 1. An apparatus for measuring the cross-sectional thickness shape of a plate material, comprising: a signal processing circuit that synthesizes the data of and obtains the cross-sectional shape of the plate material.
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP56099353A JPS58707A (en) | 1981-06-26 | 1981-06-26 | Measuring device for sectional plate thickness and shape of plate material |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP56099353A JPS58707A (en) | 1981-06-26 | 1981-06-26 | Measuring device for sectional plate thickness and shape of plate material |
Publications (2)
| Publication Number | Publication Date |
|---|---|
| JPS58707A JPS58707A (en) | 1983-01-05 |
| JPS6253043B2 true JPS6253043B2 (en) | 1987-11-09 |
Family
ID=14245236
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP56099353A Granted JPS58707A (en) | 1981-06-26 | 1981-06-26 | Measuring device for sectional plate thickness and shape of plate material |
Country Status (1)
| Country | Link |
|---|---|
| JP (1) | JPS58707A (en) |
Families Citing this family (3)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| JPS60230009A (en) * | 1984-04-28 | 1985-11-15 | Toshiba Corp | Radiation thickness gauge |
| KR100866888B1 (en) | 2006-10-04 | 2008-11-04 | 한국원자력연구원 | Radiation sensor and measuring method for measuring sheet thickness with improved sensitivity using wire collection electrode and mixed pressurized gas in ion chamber |
| KR100856276B1 (en) | 2007-05-15 | 2008-09-03 | 주식회사 포스코 | Rolled Material Thickness Measuring Device |
-
1981
- 1981-06-26 JP JP56099353A patent/JPS58707A/en active Granted
Also Published As
| Publication number | Publication date |
|---|---|
| JPS58707A (en) | 1983-01-05 |
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