JPH03210912A - Elongation percentage meter - Google Patents

Elongation percentage meter

Info

Publication number
JPH03210912A
JPH03210912A JP2005978A JP597890A JPH03210912A JP H03210912 A JPH03210912 A JP H03210912A JP 2005978 A JP2005978 A JP 2005978A JP 597890 A JP597890 A JP 597890A JP H03210912 A JPH03210912 A JP H03210912A
Authority
JP
Japan
Prior art keywords
laser beam
rolled material
light
difference
moving speed
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
JP2005978A
Other languages
Japanese (ja)
Inventor
Yuji Adachi
祐司 安達
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 JP2005978A priority Critical patent/JPH03210912A/en
Publication of JPH03210912A publication Critical patent/JPH03210912A/en
Pending legal-status Critical Current

Links

Classifications

    • BPERFORMING OPERATIONS; TRANSPORTING
    • B21MECHANICAL METAL-WORKING WITHOUT ESSENTIALLY REMOVING MATERIAL; PUNCHING METAL
    • B21BROLLING OF METAL
    • B21B37/00Control devices or methods specially adapted for metal-rolling mills or the work produced thereby
    • B21B37/56Elongation control

Landscapes

  • Engineering & Computer Science (AREA)
  • Mechanical Engineering (AREA)
  • Length Measuring Devices By Optical Means (AREA)
  • Control Of Metal Rolling (AREA)

Abstract

PURPOSE:To measure elongation percentage with high accurcy from the speed difference of an object by providing a projecting means with which light beams are projected on different two positions of the object on which tension is acted and a photodetecting means with which reflected lights which are obtained from projecting positions are received in an elongation percentage meter. CONSTITUTION:A laser beam LB that is emitted from a laser 33 is projected on the surface of a rolled stock 31 on the inlet and outlet sides of rolling mill through a half-mirror 34 and reflected irregularly from the surface. The laser beam laser beam that is irregularly reflecting is received with photodetectors 38b, 39b and made incident on a photodetecting part 40 through optical fibers 38a, 39a. And the difference of travel speed of the rolled stock 31 is determined from the difference of Doppler shift of reflected light DELTA fb - DELTA fa. Then, elongation percentage can be stably measured with high accuracy.

Description

【発明の詳細な説明】 〔産業上の利用分野〕 本発明は、例えば熱間あるいは冷間圧延時の圧延材の伸
び率を測定する伸び率計に関するものである。
DETAILED DESCRIPTION OF THE INVENTION [Field of Industrial Application] The present invention relates to an extensometer that measures the elongation rate of a rolled material during hot or cold rolling, for example.

〔従来の技術〕[Conventional technology]

圧延途中にある圧延材の伸び率は、圧延機の入口及び出
口の圧延材の夫々の移動速度を求めて測定する。
The elongation rate of the rolled material during rolling is measured by determining the respective moving speeds of the rolled material at the entrance and exit of the rolling mill.

第4図は例えば特開昭60−148612号、特開昭6
0180615号に示されている従来の圧延材の伸び率
測定方法の説明図である。
Figure 4 shows, for example, JP-A-60-148612, JP-A-6
0180615 is an explanatory diagram of a conventional method for measuring the elongation rate of a rolled material.

圧延材1は巻戻しロール2から圧延機3の圧延ロール3
a、3a間を通して巻取りロール4に巻取られるように
なっている。圧延機3の入側には圧延材1に接触してい
る入側デフロール5を設けており、圧延機3の出側には
圧延材1に接触している出側デフロール6を設けている
。そして各デフロール5,6の回転軸にはタコジェネレ
ータからなる回転計7.8が各別に取付けられている。
The rolled material 1 is transferred from the unwinding roll 2 to the rolling roll 3 of the rolling mill 3.
The film is wound onto a winding roll 4 through the space between a and 3a. An inlet defroll 5 that is in contact with the rolled material 1 is provided on the inlet side of the rolling mill 3, and an outlet defrole 6 that is in contact with the rolled material 1 is provided on the exit side of the rolling mill 3. A tachometer 7.8 consisting of a tachogenerator is attached to the rotating shaft of each of the differential rolls 5, 6.

回転計7.8は圧延材1の移動速度V、、V、を各別に
検出する。それにより圧延材1の伸び率ηは、■s により求めている。
The tachometers 7.8 individually detect the moving speeds V, , V, of the rolled material 1. Accordingly, the elongation rate η of the rolled material 1 is determined by ■s.

〔発明が解決しようとする課題〕[Problem to be solved by the invention]

前述した伸び率測定方法によれば、入側及び出側デフロ
ール5及び6が圧延材1に接触しているために圧延材1
に対して滑りが生じることがある。
According to the elongation rate measuring method described above, since the entry and exit side defrolls 5 and 6 are in contact with the rolled material 1, the rolled material 1
Slip may occur against the surface.

一方、それらのデフロール5.6は摩耗する。そのよう
なことから圧延材1の移動速度の測定誤差は±1%程度
になり、また安定して検出できず、圧延材1の伸び率を
常に高精度に測定できないという問題がある。
On the other hand, those deflation rolls 5.6 wear out. As a result, the measurement error of the moving speed of the rolled material 1 is approximately ±1%, and there is a problem that stable detection is not possible, and the elongation rate of the rolled material 1 cannot always be measured with high accuracy.

そのために圧延材に接触せずに圧延材の移動速度を検出
する方法が考えられる。第5図はその伸び率測定方法の
説明図である。圧延材1は巻戻しロール2から圧延機3
の圧延ロール3a、3a間を通して巻取りロール4に巻
取られるようになっている。圧延機3の入側及び出側に
は、レーザ光を出射して物体の速度を非接触で測定する
レーザドツプラ一方式速度計9.10を夫々設けている
。レーザドツプラ一方式速度計9.10が各別に検出し
た圧延材lの移動速度V、、Vゎの速度信号は、減算器
11に与えられ、その減算結果V、−V、の速度差信号
を除算器12に与える。除算器12には前記移動速度■
、の速度信号が与えられている。
For this purpose, a method of detecting the moving speed of the rolled material without contacting the rolled material may be considered. FIG. 5 is an explanatory diagram of the elongation rate measuring method. The rolled material 1 is transferred from the unwinding roll 2 to the rolling mill 3
The material is wound onto a winding roll 4 through the rolling rolls 3a, 3a. Laser Doppler one-way speedometers 9 and 10 are provided on the inlet and outlet sides of the rolling mill 3, respectively, for emitting laser light to measure the speed of an object in a non-contact manner. The speed signals of the moving speeds V, V, and V of the rolled material l detected individually by the laser Doppler one-way speedometers 9 and 10 are given to the subtracter 11, and the subtraction results are divided by the speed difference signal of V, -V. Give to container 12. The divider 12 has the moving speed ■
A velocity signal of , is given.

これにより除算器12は、それに与えられた速度差V、
−V、の速度差信号を移動速度V、の速度信号で除算し
、即ち前記(11式の算出内容により圧延材1の伸び率
を測定する。
As a result, the divider 12 calculates the velocity difference V given to it,
-V, the speed difference signal is divided by the speed signal of the moving speed V, that is, the elongation rate of the rolled material 1 is measured according to the calculation contents of equation (11).

しかし乍ら、この伸び率測定方法によれば、レーザドツ
プラ一方式速度計9.10が個々に有する速度検出誤差
及びパスラインにおける圧延状態の変動の影響をうけて
、速度測定誤差は±0.3%程度になる。
However, according to this elongation rate measurement method, the speed measurement error is ±0.3 due to the influence of the speed detection error of each laser Doppler speedometer 9.10 and the fluctuation of the rolling state in the pass line. It will be about %.

それにより、この測定条件で伸び率を測定する場合には
、圧延機3の入側及び出側で圧延材1の移動速度を測定
した測定誤差は、レーザドツプラ一方式速度計9,10
が個々に有している速度測定誤差により、求め得る移動
速度差V、−V、の誤となる。但しε、、ε、は移動速
度V、、V、の測定誤差(1%程度)である。
Therefore, when measuring the elongation rate under these measurement conditions, the measurement error when measuring the moving speed of the rolled material 1 at the entrance and exit sides of the rolling mill 3 is
Due to the speed measurement error that each has, the obtainable moving speed difference V, -V becomes incorrect. However, ε, ,ε are measurement errors (about 1%) of the moving speeds V, ,V.

ところで、Jε、+ε7 : V 1.  V @にな
るから、それにより伸び率を求めた場合には、その測定
誤差が大きくなり、この方法によっても伸び率が高精度
に測定できないという問題がある。
By the way, Jε, +ε7: V 1. V@, so if the elongation rate is determined using this method, the measurement error will be large, and there is a problem that the elongation rate cannot be measured with high precision even with this method.

本発明は斯かる問題に鑑み張力が作用している物体の伸
び率を常に高精度に測定できる伸び率計を提供すること
を目的とする。
In view of this problem, it is an object of the present invention to provide an extensometer that can constantly and accurately measure the elongation rate of an object on which tension is applied.

〔課題を解決するための手段〕[Means to solve the problem]

本発明に係る伸び率計は、張力が作用している物体の伸
び率を測定する伸び率計において、前記物体の異なる2
位置に光を投射する投光手段と、それらの投射位置から
得た反射光を受光する光検知手段とを備えることを特徴
とする。
The extensometer according to the present invention is an extensometer that measures the elongation rate of an object on which tension is applied.
It is characterized by comprising a light projection means for projecting light onto positions, and a light detection means for receiving reflected light obtained from those projection positions.

〔作用〕[Effect]

投光手段は伸び率を測定すべき物体の異なる2位置に光
を投射する。光検知手段は投射位置からの反射光の周波
数差を求める。
The light projecting means projects light onto two different positions of the object whose elongation rate is to be measured. The light detection means determines the frequency difference of reflected light from the projection position.

依って、周波数差から物体の移動速度差を直接に求め得
て、伸び率を高精度に測定する。
Therefore, the moving speed difference of the object can be directly determined from the frequency difference, and the elongation rate can be measured with high precision.

〔実施例〕〔Example〕

以下本発明をその実施例を示す図面により詳述する。 The present invention will be described in detail below with reference to drawings showing embodiments thereof.

第1図は本発明に係る伸び率計の模式図、第2図及び第
3図は本発明の詳細な説明する説明図である。
FIG. 1 is a schematic diagram of an extensometer according to the present invention, and FIGS. 2 and 3 are explanatory diagrams for explaining the present invention in detail.

先ず第2図及び第3図により発明の詳細な説明する。First, the invention will be explained in detail with reference to FIGS. 2 and 3.

第2図に示すように、矢符方向に移動している例えば鋼
板Aの表面に、所定角度で移動方向に向けたレーザビー
ムLBをレーザLから投射すると、そのレーザビームL
Bは投射位置の鋼板Aの表面で乱反射する。そしてレー
ザLと鋼板Aとの間に相対的な運動があるときには、乱
反射したレーザビームLBの周波数が変化するドツプラ
ー効果が得られ、それによってレーザビームLBの周波
数の変化量たるドツプラーシフトが得られる。
As shown in FIG. 2, when a laser beam LB directed in the moving direction at a predetermined angle is projected from a laser L onto the surface of, for example, a steel plate A that is moving in the direction of the arrow, the laser beam L
B is diffusely reflected on the surface of the steel plate A at the projection position. When there is a relative movement between the laser L and the steel plate A, a Doppler effect is obtained in which the frequency of the diffusely reflected laser beam LB changes, resulting in a Doppler shift, which is the amount of change in the frequency of the laser beam LB. It will be done.

ここでレーザLが出射するレーザビームLBの周波数を
fとすると乱反射したレーザビームの周波数Fは、 F=f+Δf  ・・・(3) となり、Δfがドツプラーシフトとして得られる。
Here, when the frequency of the laser beam LB emitted by the laser L is f, the frequency F of the diffusely reflected laser beam is F=f+Δf (3), where Δf is obtained as a Doppler shift.

ところで、鋼板Aの移動速度をVとすると、その移動速
度■のベクトルは第3図に示すようにレーザビームLB
に平行な移動速度ベクトル■、と、直角な移動速度ベク
トルV2とに分けて考えることができる。一方、ドツプ
ラーシフトΔfは、Δf=(V+/c)  ・F  ・
・・(4)(但し、Cは光速度) として求めることができ、それによりドツプラーシフト
Δrは、レーザビームLBと平行な移動速度ヘクトル■
1に比例し、そして周波数Fの変化量として得られる。
By the way, if the moving speed of the steel plate A is V, the vector of the moving speed ■ is the laser beam LB as shown in FIG.
It can be divided into a moving speed vector V2 that is parallel to V2, and a moving speed vector V2 that is perpendicular to V2. On the other hand, the Doppler shift Δf is Δf=(V+/c) ・F ・
...(4) (where C is the speed of light), and thereby the Doppler shift Δr is the moving speed parallel to the laser beam LB in hectors ■
1 and is obtained as the amount of change in frequency F.

したがって、ドツプラーシフトΔfを求めることにより
、鋼板Aの移動速度を求め得ることになる。
Therefore, by determining the Doppler shift Δf, the moving speed of the steel plate A can be determined.

さて、第1図において、図示しない巻戻しロールから矢
符方向に引出された圧延材31は圧延機32の圧延ロー
ル32a 、 32aの間を通して図示しない巻取りロ
ールに巻取られる。レーザ33が出射するレーザビーム
LBを、ハーフミラ−34を介して第1の光ファイバ3
4の基端部へ入射させており、/’%−フミラー34で
反射したレーザビームLBを、ミラー36で反射さセて
第2の光ファイバ370基端部へ入射させている。光フ
ァイバ35 (37)の先端部35a (37a)は圧
延機32の入側(出側)に位置させており、その先端部
35a (37a)を圧延材31の移動方向(移動方向
と反対方向)へ向けるとともに、光ファイバ35(37
)が出射するレーザビームLBの圧延材31への入射角
をθ、(θ、)として、光ファイバ35 (37)の先
端部35a (37a)を固定して夫々を配設している
Now, in FIG. 1, a rolled material 31 pulled out in the direction of the arrow from a rewinding roll (not shown) passes between rolling rolls 32a, 32a of a rolling mill 32 and is wound up by a winding roll (not shown). The laser beam LB emitted by the laser 33 is transmitted to the first optical fiber 3 via the half mirror 34.
The laser beam LB is reflected by the /'%-f mirror 34 and is reflected by the mirror 36 and is made to enter the base end of the second optical fiber 370. The tip 35a (37a) of the optical fiber 35 (37) is located on the entry side (output side) of the rolling mill 32, and the tip 35a (37a) is placed in the direction of movement of the rolled material 31 (in the opposite direction to the movement direction). ), and the optical fiber 35 (37
) The incident angles of the laser beam LB emitted by the laser beam LB into the rolled material 31 are set to θ, (θ, ), and the optical fibers 35 (37) are disposed with their tip portions 35a (37a) fixed.

なお、入射角θ、とθゎとは同一角度に選定しである。Incidentally, the incident angles θ and θゎ are selected to be the same angle.

光ファイバ35 (37)の先端部35a (37a)
寄りには、第1 (第2)の光ファイバ38a (39
a)の先端部に取付けた受光部38b (39b)を、
その受光面38c (39c)をレーザビームLBの投
射位置に向けて、圧延材31から適長離隔した位置に固
定して配設している。また受光部38b (39b)は
入射角θ1 (θ、)と路間−角度に選定している。そ
れにより受光部38b (39b)は、光ファイバ35
(37)から出射したレーザビームLBが圧延材31で
乱反射したその反射光を受光するようになっている。光
ファイバ38a、39aの基端部はともに光検知部40
に挿入されており、受光部38b。
Tip 35a (37a) of optical fiber 35 (37)
Nearby, the first (second) optical fiber 38a (39
The light receiving part 38b (39b) attached to the tip of a),
The light-receiving surface 38c (39c) is fixedly disposed at a position separated from the rolled material 31 by an appropriate distance with its light-receiving surface 38c (39c) facing the projection position of the laser beam LB. Further, the light receiving portion 38b (39b) is selected to have an incident angle θ1 (θ,) and a path-to-road angle. Thereby, the light receiving section 38b (39b) connects the optical fiber 35
The laser beam LB emitted from (37) is diffusely reflected by the rolled material 31, and the reflected light thereof is received. The base ends of the optical fibers 38a and 39a both have a light detection section 40.
The light receiving section 38b is inserted into the light receiving section 38b.

39bが受光した反射光は光検知部40に入射するよう
になっている。光検知部40は入射した2つの反射光が
互いに干渉して夫々の反射光の周波数の周波数差が得ら
れるようになっている。
The reflected light received by 39b is made to enter the photodetector 40. The light detection unit 40 is configured such that two incident reflected lights interfere with each other to obtain a frequency difference between the frequencies of the respective reflected lights.

次にこのように構成した伸び型針の動作を説明する。Next, the operation of the extendable needle configured as described above will be explained.

レーザ33がレーザビームLBを出射すると、そのレー
ザビームLBは光ファイバ35 (36)を介して圧延
機32の入側(出側)の圧延材31の表面に投射され、
その表面で乱反射する。乱反射したレーザ光は受光部3
8b (39b)が受光し、光ファイバ38a (39
a)を介して受光した夫々のレーザ光が光検知部40へ
入射する。それにより光検知部40において受光した2
つの反射光が干渉して、夫々の反射光の周波数差たるビ
ート周波数が得られる。
When the laser 33 emits the laser beam LB, the laser beam LB is projected onto the surface of the rolled material 31 on the entry side (output side) of the rolling mill 32 via the optical fiber 35 (36).
It reflects diffusely on its surface. The diffusely reflected laser beam is sent to the light receiving section 3.
8b (39b) receives the light, and the optical fiber 38a (39
The respective laser beams received through a) enter the photodetector section 40. As a result, the light detected by the light detection unit 40 is
The two reflected lights interfere, and a beat frequency, which is the frequency difference between the two reflected lights, is obtained.

即ち、レーザビームLBの周波数をFとし、圧延機32
の入側(出側)における圧延材31の移動速度を■、 
(Vb)とすると、前述したドツプラー効果により受光
部38b (39b)には、その移動速度■、。
That is, the frequency of the laser beam LB is F, and the rolling mill 32
The moving speed of the rolled material 31 on the entry side (output side) of
(Vb), the light receiving section 38b (39b) has a moving speed of 2 due to the above-mentioned Doppler effect.

■、に関連したドツプラーシフトΔf、(Δfb)が、 として得られる。これらのドツプラーシフトΔf3Δf
、は圧延機32の人、出側における圧延材31の移動速
度に関連しており、それにより移動速度差V、−V、は
、前記(51,(61式により、として得られる。そし
てθ1=θ5であるから、λ (但しλは光の波長) となり、λ、 cos θは一定であるから、ドツプラ
ーシフト差へf、−へf、を求めることにより移動速度
差Vb−V、が求まる。
(2) The Doppler shift Δf, (Δfb) associated with , is obtained as follows. These Doppler shifts Δf3Δf
, is related to the moving speed of the rolled material 31 on the exit side of the rolling mill 32, so that the moving speed difference V, -V, is obtained as (51, (61), and θ1 = θ5, so λ (where λ is the wavelength of light), and since λ and cos θ are constant, by finding the Doppler shift difference f and - to f, the moving speed difference Vb - V, Seek.

このようにして圧延機32の人、出側における圧延材3
1の移動速度がドツプラーシフトとして得られて、圧延
材31の移動速度差Vb−V、を直接に求め得ることに
なる。
In this way, the person of the rolling mill 32, the rolled material 3 on the exit side
The moving speed of 1 is obtained as a Doppler shift, and the moving speed difference Vb-V of the rolled material 31 can be directly determined.

そしてこのドツプラーシフトの差Δfb−Δf1、即ち
ビート周波数自体は路数%の誤差で測定できる。それに
より、このようにして求めた移動速度差V、−V、を用
いて伸び率ηを ■。
The Doppler shift difference Δfb−Δf1, that is, the beat frequency itself can be measured with an error of the number of paths. Thereby, the elongation rate η is calculated by using the moving speed difference V, -V, obtained in this way.

により算出できる。なお、圧延機32の入側の移動速度
V、は受光部38bで得たドツプラーシフトΔf。
It can be calculated by Note that the moving speed V on the entrance side of the rolling mill 32 is the Doppler shift Δf obtained by the light receiving section 38b.

を用いてもよく、あるいは従来のように回転計7で求め
た移動速度■、を用いてもよい。
Alternatively, the moving speed (2) determined by the tachometer 7 as in the conventional method may be used.

このようにして圧延機の入側と出側の圧延材の移動速度
差が直接に求められるから、圧延機の入側で求めた移動
速度に誤差が生じても、従来のように圧延機の入側及び
出側で夫々求めた移動速度を用いて伸び率を求める場合
に比べて、極めて高精度に伸び率を測定できることにな
る。
In this way, the difference in the moving speed of the rolled material on the inlet and outlet sides of the rolling mill can be directly determined, so even if an error occurs in the moving speed determined on the inlet side of the rolling mill, it is possible to This means that the elongation rate can be measured with extremely high accuracy compared to the case where the elongation rate is determined using the moving speeds determined respectively on the entry side and the exit side.

本実施例では、張力が作用している圧延材の伸び率を測
定する場合について説明したが、それは単なる例示であ
り、圧延材以外の張力が作用している物体の伸び率を測
定することもできる。また投射する光はレーザビームに
限定されるものではない。
In this example, a case was explained in which the elongation rate of a rolled material to which tension is applied is measured, but this is merely an example, and the elongation rate of an object other than a rolled material to which tension is applied may also be measured. can. Furthermore, the light to be projected is not limited to a laser beam.

〔発明の効果〕〔Effect of the invention〕

以上詳述したように、本発明は、伸び率を測定すべき物
体の異なる2位置に光を投射して、それらの反射光のド
ツプラーシフトを求め、そのドツプラーシフトの差、つ
まり投射光の周波数の周波数差から物体の移動速度差を
直接に求めるから、移動速度を求める測定器自体の測定
誤差をともなわない。また移動速度差を非接触で測定す
るから、その測定値を常に安定に得ることができる。し
たがって、伸び率を常に高精度にしかも安定して測定で
きる伸び型針を提供できる優れた効果がある。
As described in detail above, the present invention projects light onto two different positions of an object whose elongation rate is to be measured, determines the Doppler shift of the reflected light, and calculates the difference between the Doppler shifts, that is, the projected light Since the difference in moving speed of the object is directly determined from the frequency difference between the frequencies, there is no measurement error in the measuring device itself that determines the moving speed. Furthermore, since the difference in moving speed is measured without contact, the measured value can always be stably obtained. Therefore, there is an excellent effect of providing an elongated needle that can always measure the elongation rate with high precision and stability.

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

第1図は本発明に係る伸び重重の模式図、第2図及び第
3図は発明の詳細な説明する説明図、第4図は従来の伸
び率測定方法を説明する図、第5図は他の伸び率測定方
法を説明する図である。 31・・・圧延材 32・・・圧延機 33・・・レー
ザ35.37・・・光ファイバ 38b、 39b・・
・受光部38a 、 39a・・・光ファイバ 40・
・・光検知部第 図 第 図 第 図 △ a 第 図 η 第 図
FIG. 1 is a schematic diagram of the elongation weight according to the present invention, FIGS. 2 and 3 are explanatory diagrams explaining the invention in detail, FIG. 4 is a diagram explaining the conventional elongation rate measuring method, and FIG. It is a figure explaining other elongation rate measuring methods. 31...Rolled material 32...Rolling machine 33...Laser 35.37...Optical fiber 38b, 39b...
・Light receiving parts 38a, 39a...optical fiber 40・
・・Photodetector part Fig. Fig. Fig. △ a Fig. η Fig.

Claims (1)

【特許請求の範囲】 1、張力が作用している物体の伸び率を測定する伸び率
計において、 前記物体の異なる2位置に光を投射する投 光手段と、それらの投射位置から得た反射光を受光する
光検知手段とを備えることを特徴とする伸び率計。
[Claims] 1. An extensometer that measures the elongation rate of an object on which tension is applied, comprising: a light projection means for projecting light onto two different positions on the object; and reflections obtained from those projection positions. An extensometer characterized by comprising a light detection means for receiving light.
JP2005978A 1990-01-13 1990-01-13 Elongation percentage meter Pending JPH03210912A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP2005978A JPH03210912A (en) 1990-01-13 1990-01-13 Elongation percentage meter

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP2005978A JPH03210912A (en) 1990-01-13 1990-01-13 Elongation percentage meter

Publications (1)

Publication Number Publication Date
JPH03210912A true JPH03210912A (en) 1991-09-13

Family

ID=11625925

Family Applications (1)

Application Number Title Priority Date Filing Date
JP2005978A Pending JPH03210912A (en) 1990-01-13 1990-01-13 Elongation percentage meter

Country Status (1)

Country Link
JP (1) JPH03210912A (en)

Cited By (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
WO2008131931A1 (en) * 2007-04-25 2008-11-06 Kocks Technik Gmbh & Co. Kg Method and device for measuring the tensile force acting upon a moving pipe, or a moving rod
KR100939315B1 (en) * 2002-11-02 2010-01-28 주식회사 포스코 Crop shape and speed measuring device of hot bar using optical fiber

Cited By (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
KR100939315B1 (en) * 2002-11-02 2010-01-28 주식회사 포스코 Crop shape and speed measuring device of hot bar using optical fiber
WO2008131931A1 (en) * 2007-04-25 2008-11-06 Kocks Technik Gmbh & Co. Kg Method and device for measuring the tensile force acting upon a moving pipe, or a moving rod

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