Deprecated: The each() function is deprecated. This message will be suppressed on further calls in /home/zhenxiangba/zhenxiangba.com/public_html/phproxy-improved-master/index.php on line 456
JPH0424121B2 - - Google Patents
[go: Go Back, main page]

JPH0424121B2 - - Google Patents

Info

Publication number
JPH0424121B2
JPH0424121B2 JP57100419A JP10041982A JPH0424121B2 JP H0424121 B2 JPH0424121 B2 JP H0424121B2 JP 57100419 A JP57100419 A JP 57100419A JP 10041982 A JP10041982 A JP 10041982A JP H0424121 B2 JPH0424121 B2 JP H0424121B2
Authority
JP
Japan
Prior art keywords
width
rolling
change
rolling mill
diameter
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 - Lifetime
Application number
JP57100419A
Other languages
Japanese (ja)
Other versions
JPS58218314A (en
Inventor
Koji Inazaki
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
Nippon Steel Corp
Priority date (The priority date is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the date listed.)
Filing date
Publication date
Application filed by Nippon Steel Corp filed Critical Nippon Steel Corp
Priority to JP57100419A priority Critical patent/JPS58218314A/en
Priority to GB08315887A priority patent/GB2124364B/en
Priority to DE19833321104 priority patent/DE3321104A1/en
Priority to FR8309684A priority patent/FR2528333B1/en
Publication of JPS58218314A publication Critical patent/JPS58218314A/en
Publication of JPH0424121B2 publication Critical patent/JPH0424121B2/ja
Granted 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
    • BPERFORMING OPERATIONS; TRANSPORTING
    • B21MECHANICAL METAL-WORKING WITHOUT ESSENTIALLY REMOVING MATERIAL; PUNCHING METAL
    • B21BROLLING OF METAL
    • B21B1/00Metal-rolling methods or mills for making semi-finished products of solid or profiled cross-section; Sequence of operations in milling trains; Layout of rolling-mill plant, e.g. grouping of stands; Succession of passes or of sectional pass alternations
    • B21B1/16Metal-rolling methods or mills for making semi-finished products of solid or profiled cross-section; Sequence of operations in milling trains; Layout of rolling-mill plant, e.g. grouping of stands; Succession of passes or of sectional pass alternations for rolling wire rods, bars, merchant bars, rounds wire or material of like small cross-section
    • B21B1/18Metal-rolling methods or mills for making semi-finished products of solid or profiled cross-section; Sequence of operations in milling trains; Layout of rolling-mill plant, e.g. grouping of stands; Succession of passes or of sectional pass alternations for rolling wire rods, bars, merchant bars, rounds wire or material of like small cross-section in a continuous process

Landscapes

  • Engineering & Computer Science (AREA)
  • Mechanical Engineering (AREA)
  • Control Of Metal Rolling (AREA)

Description

【発明の詳細な説明】 本発明は丸棒、線材等の円形断面条材の寸法制
御に関するものである。
DETAILED DESCRIPTION OF THE INVENTION The present invention relates to dimensional control of circular cross-section strips such as round bars and wires.

丸棒線材の圧延に於ては孔型が用いられ複数の
圧延機により水平垂直交互に、圧下圧下が加えら
れて真円に近い仕上り寸法に加工される。ここで
圧延材の寸法(断面形状)は最終段の圧延機の圧
下でほぼ決定されるのでこの圧延機の孔型形状は
極めて精密加工され製品寸法毎に取り替えられ
る。しかしながら孔型圧延の場合第1図に示すよ
うにロールギヤツプ量によつて孔型の底に接する
点A,Aの寸法(以下天地寸法という)が変化す
るし、孔型に拘束されないフリー面の寸法B,B
(以下巾寸法という)も変化する。第1図aは適
正な圧下の場合、(b)はロールギヤツプが過大な場
合、(c)はロールギヤツプが過小な場合である。
In rolling round rods and wire rods, a groove die is used, and a plurality of rolling mills apply rolling reductions alternately horizontally and vertically to produce finished dimensions close to perfect circles. Here, the dimensions (cross-sectional shape) of the rolled material are almost determined by the rolling force of the final stage rolling mill, so the hole shape of this rolling mill is extremely precisely machined and replaced for each product size. However, in the case of groove rolling, as shown in Figure 1, the dimensions of points A and A that contact the bottom of the groove (hereinafter referred to as vertical dimensions) change depending on the amount of roll gap, and the dimensions of the free surface that is not constrained by the groove. B,B
(hereinafter referred to as width dimension) also changes. FIG. 1a shows the case when the rolling reduction is proper, FIG. 1b shows the case when the roll gap is too large, and FIG. 1c shows the case when the roll gap is too small.

更に圧延が進んでロールが摩耗すると製品の断
面形状は変化する。即ち第2図のロールの肩と称
する部分Xが圧延機の圧下による肉の流れにより
最も摩耗し、従つてこの肩の部位の寸法(以下肩
寸法)が最も大きな値となる。この肩寸法は正確
な位置を指定できないが通常は巾寸法から30゜近
辺に存在する。第3図は80゜の棒の断面形状で、
マイクロメータにより5゜毎に測定した直径をプロ
ツトしたものであるが明瞭に肩寸法が識別され
る。この2ケの突出した肩C,C又はC′,C′の間
の部位がフリー面D,D′であり、このフリー面
と直交する部位が天地E,Eである。一般に丸棒
の断面は第3図の如き形状をしており肩寸法が最
大値で、天地寸法、巾寸法のいずれかが最小寸法
となる場合と、第1図cのように巾寸法が最大と
なる場合のいずれかに整理される。
As rolling progresses further and the rolls wear out, the cross-sectional shape of the product changes. That is, the portion X called the shoulder of the roll in FIG. 2 is worn the most due to the flow of meat due to rolling by the rolling mill, and therefore the dimension of this shoulder portion (hereinafter referred to as shoulder dimension) has the largest value. Although the exact position of this shoulder dimension cannot be specified, it is usually located around 30° from the width dimension. Figure 3 shows the cross-sectional shape of an 80° bar.
This is a plot of the diameter measured every 5 degrees with a micrometer, and the shoulder dimension can be clearly identified. The areas between these two protruding shoulders C, C or C', C' are the free surfaces D, D', and the areas orthogonal to these free surfaces are the top and bottom E, E. Generally, the cross section of a round bar has a shape as shown in Figure 3, with the shoulder dimension being the maximum value and either the top, bottom or width dimension being the minimum dimension, or the width dimension being the maximum as shown in Figure 1 c. It will be sorted in one of the following cases.

しかしながら従来の圧延ラインではかかる圧延
条材の断面形状を知ることは不可能であり、切断
したサンプルを測定する抜き取り検査や冷却後剪
断された製品を限界ゲージやマイクロメータで検
査することしかできなかつた。
However, with conventional rolling lines, it is impossible to know the cross-sectional shape of such rolled strips, and the only methods available are sampling inspections that measure cut samples or inspections of products that have been sheared after cooling using limit gauges or micrometers. Ta.

近年エレクトロニクスの進歩により圧延機の後
面(下流)に光電式の寸法測定器を設けて丸棒の
寸法を測定し、これをもとに圧延機の圧下装置を
動かして寸法の制御を行なう試みがなされてい
る。例えば特公昭50−39066,55−39067のように
天地と巾の寸法を測定して上流側の2つの圧延機
の圧下もしくは張力を制御する方法があるが、圧
延条材は圧延後捻転するので圧延機のロールに対
応して直交2軸の光学式寸法測定器を設けたとし
ても必らずしも天地、巾寸法の測定はできない欠
点があつた。又たとえ天地、巾寸法の測定ができ
たとしても前述のように最大寸法は肩寸法の場合
が多いので天地、巾の寸法制御を行なうだけでは
製品の寸法精度に確実な寄与ができない問題があ
つた。
In recent years, with advances in electronics, attempts have been made to measure the dimensions of the round bar by installing a photoelectric dimension measuring device at the rear (downstream) of the rolling mill, and to control the dimensions by operating the rolling mill's rolling device based on this measurement. being done. For example, there is a method as shown in Japanese Patent Publication No. 50-39066 and 55-39067 in which the height and width dimensions are measured to control the rolling reduction or tension of the two upstream rolling mills, but since the rolled strip is twisted after rolling, Even if an optical dimension measuring device with two orthogonal axes was installed in correspondence with the rolls of a rolling mill, there was a drawback that it was not always possible to measure the vertical and width dimensions. Furthermore, even if the height and width dimensions can be measured, as mentioned above, the maximum dimension is often the shoulder dimension, so there is a problem that simply controlling the height and width dimensions cannot reliably contribute to the dimensional accuracy of the product. Ta.

本発明は従来法のかかる欠点に鑑みなされたも
ので高精度の連続回転式の寸法測定器を用いて断
面形状を測定して天地、巾、肩の各寸法を識別
し、しかる後に所定の関係式を用いて最終段の圧
延機圧下を修正するとともに寸法変動に大きく影
響する圧延温度を検出して予測修正することによ
つて条材の総合的寸法精度の向上を計るものであ
る。
The present invention was developed in view of the drawbacks of the conventional method, and uses a high-precision continuously rotating dimension measuring device to measure the cross-sectional shape, identify the top, bottom, width, and shoulder dimensions, and then determine the predetermined relationship. This method aims to improve the overall dimensional accuracy of the strip by correcting the rolling reduction of the final stage using the formula, and by detecting and predicting the rolling temperature, which has a large effect on dimensional fluctuations.

本発明の丸棒の寸法制御方法は、孔型による連
続式圧延機列の出側に圧延材の回りを回転する条
材寸法計測器を設け、該計測器の出力により条材
の断面形状を求め、この断面形状で最も急峻な変
化をする角度位置を巾位置とし、該角度と直交す
る角度位置を天地位置、もしくは最も変化が緩い
角度位置を天地位置それと直交する角度位置を巾
位置としそしてこの巾、天地位置を除いた断面形
状のうち最大径を肩径とし、夫々巾、天地、肩径
の目標値からの偏差ΔB0,ΔH0,ΔL0を求め、こ
れらに第9図に示す最下流圧延機の圧下変化と
巾、天地、肩径の変化との関係から(6)、(7)、(8)式
により圧下変化を加えた場合の巾、天地、肩径の
目標値からの予測偏差を計算することによりこれ
ら3つの偏差の最大値が最小となる圧下を制御す
ることを特徴とするが、以下本発明の構成を詳細
に説明する。
The method for controlling the size of a round bar according to the present invention includes installing a strip size measuring device that rotates around the rolled material on the exit side of a row of continuous rolling mills using grooves, and measuring the cross-sectional shape of the strip using the output of the measuring device. In this cross-sectional shape, the angular position where the steepest change occurs is defined as the width position, the angular position perpendicular to the angle is defined as the vertical position, or the angular position where the change is the gentlest is defined as the vertical position, and the angular position orthogonal to that is defined as the width position. The maximum diameter of the cross-sectional shape excluding the width and top and bottom positions is taken as the shoulder diameter, and the deviations ΔB 0 , ΔH 0 , and ΔL 0 from the target values of the width, top and bottom, and shoulder diameter are determined, and these are shown in Figure 9. From the relationship between the rolling reduction change of the most downstream rolling mill and the width, top/bottom, and shoulder diameter changes, use formulas (6), (7), and (8) to determine the target values for the width, top/bottom, and shoulder diameter when adding rolling reduction changes. The present invention is characterized in that the reduction in which the maximum value of these three deviations becomes the minimum is controlled by calculating the predicted deviation of these three deviations.The configuration of the present invention will be described in detail below.

第4図は本発明方法を実施する際に使用する回
転型の棒線材の寸法計測装置を示し、光源2から
発せられた光はレンズ3を通つて平行光線とな
り、棒線材の影が受光レンズ4を通つて光電変換
アレイ素子5の上に結像する。光電変換アレイ素
子5には電荷結合素子を用いている。この像は発
信器6から加えられるパルスによつてアレイ素子
5から明暗に対応したパルス列の形で出力され、
カウンタ7で計数される。パルスカウントに変換
された棒線材の直径は演算装置9に入力される。
ここでパルス列はスリツプリング8を通して伝達
される。棒線材の鉛直に対してどの角度の直径を
計つたかを認識する為に角度検出器13の出力も
演算装置9に入力されている。
FIG. 4 shows a rotating rod and wire rod dimension measuring device used when carrying out the method of the present invention, in which light emitted from a light source 2 passes through a lens 3 and becomes a parallel ray, and the shadow of the rod and wire rod is reflected by a light receiving lens. 4 and is imaged onto the photoelectric conversion array element 5. A charge coupled device is used for the photoelectric conversion array element 5. This image is outputted from the array element 5 in the form of a pulse train corresponding to brightness and darkness by pulses applied from the transmitter 6.
It is counted by counter 7. The diameter of the rod and wire rod converted into pulse counts is input to the calculation device 9.
Here, the pulse train is transmitted through the slip ring 8. The output of the angle detector 13 is also input to the arithmetic unit 9 in order to recognize at which angle the diameter is measured with respect to the vertical of the wire rod.

第5図は本寸法計測装置の立体図であるが、第
4図に於ける光源2、レンズ3,4、アレイ素子
5、スリツプリング8は回転体12に一体となつ
て装着されており、固定軸11を中心としてモー
タ10により一定方向に連続回転する。この回転
体12へのパルス信号の入力と同じく回転体12
からの明暗信号はスリツプリング8を介して行な
われており、回転体12は毎分45回転で回転して
いるので棒線材の一断面の測定には回転体が180゜
回る時間である0.66秒を要する。第4図の角度検
出器13は基準角度からの回転角度とこの180゜回
転の信号を発生する。棒線材1の直径の測定は回
転体が6゜回転する度に行なわれ半回転で計30カ所
の直径値が演算装置9に入力される。かかる回転
式の寸法計測装置としては本願発明者らが申請中
の実願昭53−20271号、実願昭53−23729号、特願
昭54−160952号等がある。
FIG. 5 is a three-dimensional view of this dimension measuring device, and the light source 2, lenses 3, 4, array element 5, and slip ring 8 in FIG. 4 are integrally attached to the rotating body 12. It is continuously rotated in a fixed direction by a motor 10 around a fixed shaft 11. Similarly to the input of the pulse signal to the rotating body 12, the rotating body 12
The light/dark signal is transmitted through the slip ring 8, and since the rotating body 12 rotates at 45 revolutions per minute, it takes 0.66 seconds, which is the time it takes for the rotating body to rotate 180°, to measure one cross section of the wire rod. It takes. An angle detector 13 in FIG. 4 generates a signal indicating the rotation angle from the reference angle and this 180° rotation. The diameter of the rod and wire rod 1 is measured every time the rotating body rotates by 6 degrees, and diameter values at a total of 30 points are input to the calculation device 9 in half a rotation. Examples of such rotary dimension measuring devices include Utility Application No. 53-20271, Utility Model Application No. 53-23729, and Japanese Patent Application No. 160952-1989, which are currently being filed by the inventors of the present application.

さて30ケの直径値による棒線材の断面形状は演
算装置9により第3図のようにグラフイツク表示
もされるが、同時に時間軸で表わした第6図のよ
うにも記録計(図示せず)に出力される。かかる
時間軸上の一断面の直径のパターンを数多く調査
した結果直径値が最も急峻な変化をする点がフリ
ー面に対応することがわかつた。従つて第6図で
は(a)点が巾寸法でありこれと直交する角度(b)の径
が天地径となる。更にこの巾、天地の近傍の径を
除いたうち巾寸法に近い角度で最大のもの(c)が肩
寸法に対応する。これら巾、天地、肩の角度は第
4図の角度検出器の信号と対応づけられるが、棒
線材の捻転がある場合はロールの天地、巾に相当
する角度との対応は完全でないこともある。又巾
寸法の識別にあたつては正弦波からの偏差が最大
となる直径をもつてすることも可能である。又ロ
ールの天地部の摩耗変化が少ないことからロール
の既知の孔形の曲率に一致する部位をさがしその
中心をもつて天地径とすることも有効である。即
ち30ケの直径の差分をとりその差分列のうち最も
変化が小さい点をもつて天地としても良い。この
ようにして天地径H0、巾径B0、肩径L0が求まる
と目標径D0との偏差が夫々ΔH0、ΔB0、ΔL0が求
まり天地径H0、巾径B0のいずれかが最小径とな
ることも知られているのでこれらの偏差ΔH0
ΔB0,ΔL0の絶対値を小さくすれば条材の寸法が
目標径D0に近くなつて精度を向上できる。次に
寸法制御方法について説明する。
Now, the cross-sectional shape of the rod and wire material according to the 30 diameter values is displayed graphically by the computing device 9 as shown in Fig. 3, but at the same time it is also displayed on the time axis as shown in Fig. 6 using a recorder (not shown). is output to. As a result of investigating many patterns of the diameter of one cross section on the time axis, it was found that the point where the diameter value changes most steeply corresponds to the free surface. Therefore, in Fig. 6, point (a) is the width dimension, and the diameter at the angle (b) perpendicular to this is the top and bottom diameter. Furthermore, among this width and the diameter near the top and bottom, the largest angle (c) that is close to the width dimension corresponds to the shoulder dimension. These width, top and bottom, and shoulder angles are correlated with the signals from the angle detector shown in Figure 4, but if the rod or wire material is twisted, the correspondence with the angles corresponding to the top, bottom, and width of the roll may not be perfect. . In addition, when identifying the width dimension, it is also possible to use the diameter that has the maximum deviation from the sine wave. Furthermore, since the top and bottom portions of the roll undergo little wear and tear, it is also effective to find a portion of the roll that matches the known curvature of the hole shape and use its center as the top and bottom diameter. In other words, the difference between the 30 diameters may be taken and the point with the smallest change in the difference sequence may be taken as the top and bottom. In this way, when the top and bottom diameters H 0 , width diameter B 0 , and shoulder diameter L 0 are determined, the deviations from the target diameter D 0 are found, ΔH 0 , ΔB 0 , and ΔL 0 , respectively. It is also known that one of them has the minimum diameter, so these deviations ΔH 0 ,
By reducing the absolute values of ΔB 0 and ΔL 0 , the dimensions of the strip become closer to the target diameter D 0 and accuracy can be improved. Next, the dimension control method will be explained.

第7図にロール孔型及び棒線材の断面の上半分
を示す。ロールの孔型は基準隙d0のときP0を中心
として基準半径R0となるよう研削されている。
このときロールギヤツプの圧延荷重によるスプリ
ングアツプを無視するならば棒線材の断面は第7
図の斜線ような形となり天地ではロール形状と一
致するがフリー面ではロールに拘束されない部分
は基準半径R0とは異なる。今第7図に於てロー
ルのギヤツプがd0からΔだけ大きくなつたときを
考えると片側ではd0+Δ/2のP′に断面の中心が移 動し天地径は2R0+ΔとなつてΔだけ大きくなる
が、他の径は天地径からの角度をθとすると、 となりR0>>Δ/2であるので(1)式は D(θ)=2R0+(1+D(Δ/2R)2+Δ/R0cosθ
)2/ 1 ≒2R0+(1+1/2Δ/R0cosθ) =2R0+Δcosθ ……(2)式 となつてΔcosθしか大きくならない。
FIG. 7 shows the upper half of the cross section of the roll hole mold and the rod and wire rod. The hole shape of the roll is ground so that it has a reference radius R 0 with P 0 as the center when the reference gap d 0 is set.
At this time, if the spring-up due to the rolling load of the roll gap is ignored, the cross section of the rod and wire rod is 7th.
It has a shape like the diagonal line in the figure, and matches the roll shape on the top and bottom, but on the free surface, the part that is not restrained by the roll differs from the reference radius R 0 . Now, in Fig. 7, if we consider that the gap of the roll increases by Δ from d 0 , the center of the cross section on one side moves to P′ of d 0 +Δ/2, and the top-to-bottom diameter becomes 2R 0 +Δ, and Δ However, for other diameters, if the angle from the top and bottom diameters is θ, Since R 0 >>Δ/2, equation (1) is D(θ)=2R 0 +(1+D(Δ/2R) 2 +Δ/R 0 cosθ
) 2/ 1 ≒2R 0 + (1+1/2Δ/R 0 cosθ) = 2R 0 +Δcosθ ……(2), and only Δcosθ becomes large.

従つて肩径が巾寸法径側にあつて天地径からは
60゜程度であるので圧下量がΔ変化させても0.5Δ
しか変化しない。この関係を第8図aに示す。第
8図は縦軸に肩径変化ΔL又は巾径変化ΔBをと
り、横軸に圧下修正量ΔSをとつて表わした。
Therefore, the shoulder diameter is on the width dimension side, and from the top and bottom diameter
Since it is about 60°, even if the reduction amount changes by Δ, it will only change by 0.5Δ.
only changes. This relationship is shown in Figure 8a. In FIG. 8, the vertical axis shows shoulder diameter change ΔL or width diameter change ΔB, and the horizontal axis shows reduction correction amount ΔS.

一方巾寸法は直径ロールに拘束されていないの
で一つ上流の圧延機の天地が当該圧延機のフリー
面に対応することから一つ上流の圧延機の圧下が
支配的である。しかしながら孔型に適正に肉が充
満している状態では最終圧延機のロールギヤツプ
を小さくすると巾方向に肉が逃げて巾寸法が大き
くなり逆にギヤツプを大きくすると肉が不足気味
になつて巾寸法が小さくなる。この関係を第8図
bに示すが圧下の変化量Δに比べ巾寸法の変化は
小さくかつ飽和する。これから巾寸法の修正は一
つ上流の圧延機の圧下で大まかに行ない微修正は
最終圧延機で行なうことが可能であることがわか
る。よつて前述の棒線材の寸法計測器の出力より
天地、巾、肩寸法の目標径との偏差ΔH0,ΔB0
ΔL0がわかると必要な圧下修正量を決定すること
ができる。第9図は縦軸に寸法偏差、横軸に圧下
修正量をとりΔH,ΔB,ΔLが種々変化した時の
関係を表わす。
On the other hand, since the width dimension is not restricted by the diameter roll, the top and bottom of the rolling mill one upstream corresponds to the free surface of the rolling mill, so the rolling reduction of the rolling mill one upstream is dominant. However, when the groove is properly filled with meat, if the roll gap of the final rolling mill is made smaller, the meat escapes in the width direction and the width becomes larger.On the other hand, if the gap is made larger, the meat becomes insufficient and the width becomes smaller. becomes smaller. This relationship is shown in FIG. 8b, and the change in the width dimension is small compared to the amount of change Δ in the rolling reduction and reaches saturation. From this it can be seen that the width dimension can be roughly corrected in the rolling mill one upstream, and fine corrections can be made in the final rolling mill. Therefore, from the output of the above-mentioned bar and wire dimension measuring device, the deviations of the height, width, and shoulder dimensions from the target diameter are ΔH 0 , ΔB 0 ,
If ΔL 0 is known, the necessary reduction correction amount can be determined. FIG. 9 shows the relationship when ΔH, ΔB, and ΔL are variously changed, with the vertical axis representing the dimensional deviation and the horizontal axis representing the reduction correction amount.

まず第9図aのように肩偏差が大きく次いで天
地、巾となつている場合は肩角度θを60゜、圧下
変化に対する肩径変化率を0.5、巾変化率を0.33
として圧下ΔSを負の方向にΔS0修正すると肩と
天地の偏差が等しくかつ巾偏差が零となつてこの
とき最も寸法偏差が小さくなる。第9図bは天地
偏差が大きく次いで肩、巾となつている場合であ
るが、この場合もΔSを負に動かして天地偏差と
巾偏差が等しいP点で偏差が最小となる。次に圧
下が過大で噛出して巾偏差が最も大きく、次いで
肩、天地の第9図cの場合は逆に圧下を正の方向
にΔS0動かしたP点で天地と巾の偏差が等しくか
つこのとき偏差が最小となる。ところが第9図d
のように巾寸法が極端に小さい場合は圧下をΔS0
修正してP点で偏差の最小化を計るよりは、1つ
上流側の圧延機の圧下のギヤツプを大きくするこ
とにより当該圧延機での巾寸法を大きくして巾偏
差をΔB0′とし、しかる後に当該圧延機圧下を
ΔS0′修正するとP′点で偏差最小となり、より偏差
が小さくなる。この場合のように巾寸法の偏差が
大きい場合は巾寸法変化直線は第8図bのように
圧下の過大変化時に飽和現象を起すので最適圧下
修正量が求まり難く、従つて圧下修正をなるべく
小さくする方が正確でかつ偏差を小さくできる。
First, as shown in Figure 9a, if the shoulder deviation is large, followed by the top, bottom, and width, the shoulder angle θ should be 60°, the shoulder diameter change rate with respect to the reduction change should be 0.5, and the width change rate should be 0.33.
If the reduction ΔS is corrected in the negative direction by ΔS 0 , the shoulder and top deviations will be equal and the width deviation will be zero, at which point the dimensional deviation will be the smallest. Figure 9b shows a case where the vertical deviation is large, followed by the shoulder and width, but in this case too, by moving ΔS negatively, the deviation becomes minimum at point P where the vertical deviation and the width deviation are equal. Next, the roll reduction is too large and the width deviation is the largest, and then the shoulders and the top and bottom. At this time, the deviation is minimum. However, Fig. 9d
If the width dimension is extremely small as in
Rather than correcting and minimizing the deviation at point P, by increasing the rolling gap of the rolling mill one upstream, the width dimension at that rolling mill is increased and the width deviation is set to ΔB 0 '. After that, when the rolling mill reduction is corrected by ΔS 0 ', the deviation becomes minimum at point P', and the deviation becomes smaller. If the width dimension deviation is large as in this case, the width dimension change straight line will become saturated when the rolling reduction changes excessively as shown in Figure 8b, making it difficult to determine the optimum rolling reduction correction amount.Therefore, the rolling reduction correction should be made as small as possible. It is more accurate and the deviation can be reduced.

以上説明したように最終圧延機の圧下修正量
ΔSが小さい場合これに対する天地変化ΔH、肩
変化ΔL、巾変化ΔBを夫々 ΔH=ΔS ……(3)式 ΔL=ΔScosθ θ=60゜〜70゜ ……(4)式 ΔB=A・ΔS ……(5)式 と線型で近似できるので目標径からの天地、肩、
巾の偏差ΔH0,ΔL0,ΔB0がわかれば夫々の偏差
(絶対値)の最大値を最小にするΔSが(3),(4),(5)
を利用した ΔH=ΔH0+ΔS ……(6)式 ΔL=ΔL0+ΔS・cosθ ……(7)式 ΔB=ΔB0+A・ΔS ………(8)式 の3つの式の左辺いずれか2つの絶対値が等しい
ΔSを求めてその時の残る一つの式の絶対値を含
めて最大値を決定し、これを3つの式の3つの組
合せについて行ない、最大値が最も小さいものを
選び出せばそのときの解ΔSが最適解となる。こ
の場合のcosθとAは棒線材のサイズ毎にあらかじ
め求めて記憶した定数であるが、制御の過程で圧
下をΔS動かした場合の天地、肩、巾の各寸法の
変化を前述の寸法計測器により求め、これよりこ
れら定数の修正を適宜行なつても良い。更に圧延
条材の温度が変化した場合は第10図に示すよう
に巾広がりの特性が変化する。この図は圧延機の
ロールギヤツプを固定したものであるが、実際に
は変形抵抗が変化するので圧延機の剛性が小さい
場合は圧延荷重の変化ΔFによりミル定数をMと
するとΔF/Mだけロールギヤツプは変化する。
従つて圧延温度の変化ΔTによる第10図のごと
き巾寸法の変化ΔB〓Tは ΔB〓T=C・ΔT(C<O) ……(9)式 のみではなく圧下変化ΔF/Mによる巾変化を加
えた ΔB=C・ΔT+A・ΔF/M ……(10)式 となるが実際に観測できるのは(10)式よる巾変化
ΔBと温度変化ΔT及び圧力変化ΔFの数多くのデ
ータより統計的に係数C,Aも決定できる。この
場合は圧延機の圧下は外部からは意図的は動かさ
ない方が望ましいし、圧延力変化ΔFはロードセ
ルにより実測しても良いが数式モデルによりΔT
より予測しても良い。従つてΔTだけ圧延温度が
変化した場合の天地、肩、巾の各寸法偏差は(6),
(7),(8)にミルスプリングアツプ変化ΔF/Mと(10)
式を考慮した(11),(12),(13)式となる。
As explained above, when the rolling reduction correction amount ΔS of the final rolling mill is small, the vertical change ΔH, shoulder change ΔL, and width change ΔB are calculated as follows: ΔH=ΔS ...Equation (3) ΔL=ΔScosθ θ=60° to 70° ...Equation (4) ΔB=A・ΔS ...It can be approximated linearly with Equation (5), so the height, shoulder,
If the width deviations ΔH 0 , ΔL 0 , and ΔB 0 are known, ΔS that minimizes the maximum value of each deviation (absolute value) can be found as (3), (4), (5)
Using ΔH=ΔH 0 +ΔS ...Equation (6) ΔL=ΔL 0 +ΔS・cosθ ...Equation (7) ΔB=ΔB 0 +A・ΔS ......Equation 2 of the left side of the three equations in Equation (8) Find ΔS where the two absolute values are equal, determine the maximum value by including the absolute value of the remaining one equation, do this for three combinations of the three equations, and select the one with the smallest maximum value. The solution ΔS at that time is the optimal solution. In this case, cos θ and A are constants determined and memorized in advance for each size of rod and wire rod, but the above-mentioned dimension measuring device measures the changes in the vertical, shoulder, and width dimensions when the rolling reduction is changed by ΔS during the control process. From this, these constants may be modified as appropriate. Further, when the temperature of the rolled strip material changes, the width spread characteristic changes as shown in FIG. 10. In this figure, the roll gap of the rolling mill is fixed, but in reality the deformation resistance changes, so if the rigidity of the rolling mill is small, the roll gap will change by ΔF/M due to the change in rolling load ΔF, assuming the mill constant is M. Change.
Therefore, the change in width dimension ΔB〓 T as shown in Fig. 10 due to the change in rolling temperature ΔT is ΔB〓 T = C・ΔT (C<O) ......The change in width due to not only the formula (9) but also the change in rolling reduction ΔF/M ΔB=C・ΔT+A・ΔF/M...Equation (10) is obtained, but what can actually be observed is statistically based on numerous data of width change ΔB, temperature change ΔT, and pressure change ΔF according to equation (10). The coefficients C and A can also be determined. In this case, it is preferable not to intentionally change the rolling force of the rolling mill from the outside, and the rolling force change ΔF may be actually measured using a load cell, but the mathematical model
It's better to predict. Therefore, when the rolling temperature changes by ΔT, the dimensional deviations of top, bottom, shoulder, and width are (6),
(7) and (8) are the mill spring up change ΔF/M and (10)
Equations (11), (12), and (13) are obtained by considering Eq.

ΔH=ΔH0+ΔF/M+ΔS ……(11)式 ΔL=ΔL0+(ΔF/M+ΔS)cosθ……(12)式 ΔB=ΔB0+A(ΔF/M+ΔS) ……(13)式 これらの式も第8図と同様に示される(6),(7),
(8)式より最適圧下修正量ΔSを決定したのと全く
同じ手続きで(11),(12),(13)のいずれか2式の絶
対値が等しいという連立方程式を解き、そのとき
の残る一つの式の絶対値と併せて最大値を求めこ
れらの中で最大値が最も小さい場合のΔSをもつ
て最適解とすれば良い。これらの最適解に基づく
圧下の修正は修正結果を寸法計測器で確認しなが
ら行なわれるので圧下電動機の応答と寸法計測器
までの輸送遅れ時間を考慮して1本の圧延条材で
10回乃至20回行なわれる。更に圧延条材の温度を
検出する温度計は圧延機の入側に設けられ、測定
された温度はやはり圧延機までの到達時間分遅れ
させられる。
ΔH=ΔH 0 +ΔF/M+ΔS...Equation (11) ΔL=ΔL 0 +(ΔF/M+ΔS) cosθ...Equation (12) ΔB=ΔB 0 +A(ΔF/M+ΔS)...Equation (13) These equations also (6), (7), shown similarly to Figure 8.
Using exactly the same procedure used to determine the optimal reduction correction amount ΔS from equation (8), solve the simultaneous equations in which the absolute values of any two equations (11), (12), and (13) are equal, and then The maximum value may be found together with the absolute value of one equation, and ΔS where the maximum value is the smallest among these may be used as the optimal solution. The reduction is corrected based on these optimal solutions while checking the correction results with a dimension measuring instrument, so the response of the rolling motor and the transport delay time to the dimension measuring instrument are taken into consideration to ensure that one rolled strip is corrected.
It is performed 10 to 20 times. Furthermore, a thermometer for detecting the temperature of the rolled strip is provided on the entry side of the rolling mill, and the measured temperature is also delayed by the time it takes to reach the rolling mill.

以上述べたごとく本願発明の方法によれば寸法
計測器が示す偏差出力は圧下修正ににより小さく
なつており寸法精度が向上していることが分り、
本方法によれば極めて精密な寸法精度の棒線材が
製造可能であり、需要家での引抜工程の不要化等
効果が大きい。
As described above, according to the method of the present invention, the deviation output indicated by the dimension measuring instrument is reduced by the reduction correction, and the dimensional accuracy is improved.
According to this method, it is possible to manufacture rods and wires with extremely precise dimensional accuracy, and has great effects such as eliminating the need for a drawing process at the customer.

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

第1図はロールギヤツプと圧延材の形状の関係
図、第2図はロール摩耗と肩の形状の説明図、第
3図は棒断面の形状を示す図、第4図は寸法計測
器の原理図、第5図は寸法計測器の立体図、第6
図は時間軸と断面の関係を示すグラフ、第7図は
ロール孔型と棒線材断面上半分の図、第8図は圧
下修正量と肩径の変化の割合も示す図、第9図は
圧下修正量と天地、巾、肩の各偏差との関係を示
す図、また第10図は温度と巾広がりの関係の説
明図である。 1……棒線材、2……光源、3……レンズ、4
……受光レンズ、5……光電変換アレイ素子、6
……発信器、7……カウンタ、8……スリツプリ
ング、9……演算装置、10……モータ、11…
…固定軸、12……回転体、13……角度検出
器。
Figure 1 is a diagram showing the relationship between the roll gap and the shape of the rolled material, Figure 2 is an explanatory diagram of roll wear and the shape of the shoulder, Figure 3 is a diagram showing the shape of the bar cross section, and Figure 4 is a diagram of the principle of the dimension measuring instrument. , Figure 5 is a three-dimensional view of the dimension measuring instrument, Figure 6
The figure is a graph showing the relationship between the time axis and the cross section, Figure 7 is a diagram of the roll hole type and the upper half of the rod and wire cross section, Figure 8 is a diagram showing the reduction correction amount and the rate of change in shoulder diameter, and Figure 9 is a graph showing the relationship between the time axis and the cross section. FIG. 10 is a diagram showing the relationship between the amount of reduction correction and each deviation of the top, bottom, width, and shoulder, and FIG. 10 is an explanatory diagram of the relationship between temperature and width spread. 1...Wire rod, 2...Light source, 3...Lens, 4
... Light receiving lens, 5 ... Photoelectric conversion array element, 6
...Transmitter, 7...Counter, 8...Slip ring, 9...Arithmetic device, 10...Motor, 11...
... Fixed axis, 12 ... Rotating body, 13 ... Angle detector.

Claims (1)

【特許請求の範囲】 1 孔型による連続式圧延機列の出側に圧延材の
回りを回転する条材寸法計測器を設け、該計測器
の出力により条材の断面形状を求め、この断面形
状で最も急峻な変化をする角度位置を幅位置と
し、該角度と直交する角度位置を天地位置、もし
くは最も変化が緩い角度位置を天地位置それと直
交する角度位置を幅位置としそしてこのの幅、天
地位置を除いた断面形状のうち最大径を肩径と
し、各々幅、天地、肩径の目標値からの偏差
ΔB0,ΔH0,ΔL0を求め、これらに最下流圧延機
の圧下修正量ΔSを加えた後の各々幅、天地、肩
径の目標値からの偏差ΔB,ΔH,ΔLを次の式に
より計算し、これら偏差ΔB,ΔH,ΔLの内の最
大値が最も小さくなるような圧下修正量ΔSを求
めて、ロールギヤツプを制御することを特徴とす
る丸棒の寸法制御方法。 ΔB=ΔB0+A・ΔS ΔH=ΔH0+ΔS ΔL=ΔL0+ΔS・cosθ ここでAは幅変化率であり、cosθは肩径変化率
を表す三角関数で棒線材のサイズ毎にあらかじめ
求めて記憶した定数である。 2 圧延機の入側に圧延材の表面温度計を設け、
測定された圧延温度変化ΔTにより圧延力変化
ΔFを求め、特許請求の範囲第1項の計算式の代
わりに次の式によることを特徴とする特許請求の
範囲第1項記載の丸棒の寸法制御方法。 ΔB=ΔB0+A(ΔF/M+ΔS) ΔH=ΔH0+ΔF/M+ΔS ΔL=ΔL0+(ΔF/M+ΔS)cosθ ここでMは、あらかじめ求めて記憶したミル定
数。 3 圧延機の圧下修正後の幅、天地、肩径の目標
値からの偏差を求める式を条材寸法計測器の出力
をもとに修正することを特徴とする特許請求の範
囲第1項または第2項記載の丸棒の寸法制御方
法。 4 幅寸法の粗修正を最下流圧延機より一つ上流
の圧延機の圧下にて行うことを特徴とする特許請
求の範囲第1項〜第3項のいずれかに記載の丸棒
制御方法。
[Claims] 1. A strip dimension measuring device that rotates around the rolled material is provided on the exit side of a row of continuous rolling mills using grooves, and the cross-sectional shape of the strip is determined by the output of the measuring device, and the cross-sectional shape of the strip is determined by the output of the measuring device. The angular position where the shape changes most steeply is the width position, the angular position perpendicular to this angle is the vertical position, or the angular position where the change is the gentlest is the vertical position, and the angular position perpendicular to the vertical position is the width position, and the width of this The maximum diameter of the cross-sectional shape excluding the top and bottom positions is taken as the shoulder diameter, and the deviations ΔB 0 , ΔH 0 , and ΔL 0 from the target values of the width, top and bottom, and shoulder diameter are determined respectively, and the rolling correction amount of the most downstream rolling mill is calculated from these. After adding ΔS, calculate the deviations ΔB, ΔH, and ΔL from the target values of the width, top and bottom, and shoulder diameter using the following formulas, and calculate the deviations such that the maximum value of these deviations ΔB, ΔH, and ΔL is the smallest. A dimensional control method for a round bar, characterized in that the roll gap is controlled by determining the reduction correction amount ΔS. ΔB=ΔB 0 +A・ΔS ΔH=ΔH 0 +ΔS ΔL=ΔL 0 +ΔS・cosθ Here, A is the rate of change in width, and cosθ is a trigonometric function representing the rate of change in shoulder diameter, which is determined in advance for each size of rod and wire and stored. is a constant. 2. Install a surface thermometer for the rolled material on the entrance side of the rolling mill,
The dimensions of the round bar according to claim 1, wherein the rolling force change ΔF is calculated from the measured rolling temperature change ΔT, and the following formula is used instead of the calculation formula set forth in claim 1. Control method. ΔB=ΔB 0 +A(ΔF/M+ΔS) ΔH=ΔH 0 +ΔF/M+ΔS ΔL=ΔL 0 +(ΔF/M+ΔS)cosθ Here, M is a Mill constant determined and memorized in advance. 3. Claim 1 or 3, characterized in that the formula for determining the deviation from target values of the width, top and bottom, and shoulder diameter after correction of rolling mill reduction is corrected based on the output of a strip size measuring device, or The method for controlling the dimensions of a round bar according to item 2. 4. A round bar control method according to any one of claims 1 to 3, characterized in that the rough correction of the width dimension is performed at a rolling mill one upstream from the most downstream rolling mill.
JP57100419A 1982-06-11 1982-06-11 Method for controlling dimension of round bar Granted JPS58218314A (en)

Priority Applications (4)

Application Number Priority Date Filing Date Title
JP57100419A JPS58218314A (en) 1982-06-11 1982-06-11 Method for controlling dimension of round bar
GB08315887A GB2124364B (en) 1982-06-11 1983-06-09 Methods of gauging and controlling profile of bar or like workpiece
DE19833321104 DE3321104A1 (en) 1982-06-11 1983-06-10 METHOD FOR MEASURING AND CONTROLLABLY INFLUENCING THE PROFILE OF A ROUND BAR MATERIAL OR SIMILAR WORKPIECE
FR8309684A FR2528333B1 (en) 1982-06-11 1983-06-10 METHOD FOR CALIBRATING AND CONTROLLING THE PROFILE OF A BAR-LIKE PART OR THE LIKE

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP57100419A JPS58218314A (en) 1982-06-11 1982-06-11 Method for controlling dimension of round bar

Publications (2)

Publication Number Publication Date
JPS58218314A JPS58218314A (en) 1983-12-19
JPH0424121B2 true JPH0424121B2 (en) 1992-04-24

Family

ID=14273453

Family Applications (1)

Application Number Title Priority Date Filing Date
JP57100419A Granted JPS58218314A (en) 1982-06-11 1982-06-11 Method for controlling dimension of round bar

Country Status (1)

Country Link
JP (1) JPS58218314A (en)

Families Citing this family (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
DE19853256A1 (en) * 1998-11-18 2000-05-31 Schloemann Siemag Ag Measuring method for the height and width of a rod-shaped rolling stock
CN116713314B (en) * 2023-07-12 2024-01-23 索罗曼(广州)新材料有限公司 Titanium flat bar rolling one-step forming device and method

Also Published As

Publication number Publication date
JPS58218314A (en) 1983-12-19

Similar Documents

Publication Publication Date Title
CA2682635C (en) Method for measuring the roundness of round profiles
CA1168437A (en) Process and device for the contact free measurement of a dimension
KR101198492B1 (en) method and system for measurement of roll diameter
WO1991019189A1 (en) An apparatus and method for nondestructively determining the dimensional changes of an object as a function of temperature
EP0510431B1 (en) Method and apparatus for evaluating gear motion characteristics, based on tooth profile deflection differentiated by rotation angle of the gear
US4159572A (en) Dynamic gage averaging and length determining device and method for continuous sheet material
JPH0424121B2 (en)
US5373545A (en) Method for the on-line nondestructive measurement of a characteristic of a continuously produced
CN113911806A (en) Online real-time detection method for strip tension
JPH1019546A (en) Measuring method of length of moving workpiece
WO1995004914A1 (en) Virtual two gauge profile system
JPH05123749A (en) Plate speed detection method in tandem rolling mill
JP2829065B2 (en) Method of measuring thickness of rolled strip
JPH07270436A (en) Measuring device for moving objects
EP0735343B1 (en) Diameter monitoring system
US7747065B2 (en) Pixel positioning systems and methods
JPH0377013B2 (en)
JPH0778423B2 (en) Measuring method for plastic sheet width
JP3189721B2 (en) Estimation method of thickness of tapered steel plate
JP3010885B2 (en) H-section steel web height measuring method and measuring device
GB2124364A (en) Methods of gauging and controlling profile of a bar or like workpiece
JPS60253907A (en) Shape measuring instrument
JP2000155023A (en) Steel thickness measuring device
JP3443974B2 (en) Roll gap setting method
JPS6035609B2 (en) Surface roughness measuring device