JPS6116004B2 - - Google Patents
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- Publication number
- JPS6116004B2 JPS6116004B2 JP54100953A JP10095379A JPS6116004B2 JP S6116004 B2 JPS6116004 B2 JP S6116004B2 JP 54100953 A JP54100953 A JP 54100953A JP 10095379 A JP10095379 A JP 10095379A JP S6116004 B2 JPS6116004 B2 JP S6116004B2
- Authority
- JP
- Japan
- Prior art keywords
- diameter
- cross
- sectional area
- bar
- error
- 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
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- Length Measuring Devices By Optical Means (AREA)
- Length Measuring Devices With Unspecified Measuring Means (AREA)
- Control Of Metal Rolling (AREA)
Description
【発明の詳細な説明】
本発明は、圧延ライン等での走行中の熱間棒材
の断面積を実時間にて求め、基準断面積と比較し
て差を求める棒材断面積判定装置に関するもので
ある。DETAILED DESCRIPTION OF THE INVENTION The present invention relates to a bar cross-sectional area determination device that determines the cross-sectional area of a hot bar running on a rolling line or the like in real time and compares it with a reference cross-sectional area to determine the difference. It is something.
一般に棒鋼等の圧延に際しては最大,最小径、
及び偏径差、成品長等が寸法に関する保証項目で
あるが、近年輸出向では成品の重量を保証するこ
とが普通になりつつある。即ち最大,最小径が公
差内に入つていても単位長当りの重量が基準値を
超えていなければならないのである。この場合の
基準値は公称径と公称密度の積より求められる。
しかしながら棒鋼の場合は成品1本1本を測定す
ることは不可能に近いので結束状態で束毎に実貫
保証を行なうこともある。そこで圧延工程ではか
かる要求に応える為にサンプルをとりこれの最大
径,最小径をマイクロメータで測定し、最小径が
公称径(基準径)以上になるよう寸法調整を行な
つているがサンプルが局部的なものである為に相
当の余裕をもたせている。又近年では光学式の太
さ計が普及してきており、垂直―水平の2方向か
ら棒材の寸法を監視することが行なわれている。
こうした太さ計を用いる場合でも測定できるのは
直交2方向の直径であるので、やはりこれらの直
径のうち小さい方が基準径となるよう寸法調整を
行なつている。 Generally, when rolling steel bars, etc., the maximum and minimum diameter,
Warranty items related to dimensions include diameter deviation, finished product length, etc., but in recent years, it has become common for exporters to guarantee the weight of finished products. In other words, even if the maximum and minimum diameters are within the tolerance, the weight per unit length must exceed the standard value. In this case, the reference value is obtained from the product of the nominal diameter and the nominal density.
However, in the case of steel bars, it is nearly impossible to measure each finished product one by one, so actual performance guarantees are sometimes performed for each bundle in a bundled state. Therefore, in the rolling process, in order to meet such requirements, samples are taken, their maximum and minimum diameters are measured using a micrometer, and the dimensions are adjusted so that the minimum diameter is greater than the nominal diameter (standard diameter). Since it is local, a considerable amount of leeway is allowed. In recent years, optical thickness gauges have become popular, and the dimensions of bars can be monitored from two directions, vertical and horizontal.
Even when such a thickness gauge is used, only the diameters in two orthogonal directions can be measured, so the dimensions are adjusted so that the smaller of these diameters becomes the reference diameter.
以上のように従来法では圧延工程で測定できる
最小径を基準径より大き目に調整し、次に精整工
程で成品をリミツトゲージにより基準径より大き
いかどうかのチエツクを行なうことで重量保証を
行ない、束毎の実貫は設備費がかさむので省略す
ることが多い。このように従来法では寸法を太く
圧延しなければならないため歩留ロスが大きい。
一例をあげると寸法公差±1.5%でかつ重量保証
材の場合寸法のバラツキを1%とすると最小径を
基準径以上とする為に平均径はバラツキ1%の半
分の+0.5%以上となり、従つて断面積はほぼ+
1%となる。すると丁度基準値に平均径を制御し
た棒材に比べ1%の歩留ロスとなつてしまう。 As described above, in the conventional method, the minimum diameter that can be measured in the rolling process is adjusted to be larger than the standard diameter, and then, in the finishing process, the finished product is checked with a limit gauge to see if it is larger than the standard diameter to ensure weight. Actual cutting of each bundle is often omitted because equipment costs increase. As described above, in the conventional method, it is necessary to roll the material to a large size, resulting in a large yield loss.
For example, if the dimensional tolerance is ±1.5% and the dimensional variation is 1% for weight guarantee material, the average diameter will be more than +0.5%, which is half of the 1% variation, in order to make the minimum diameter greater than the standard diameter. Therefore, the cross-sectional area is approximately +
It will be 1%. This results in a yield loss of 1% compared to a bar whose average diameter is controlled exactly to the standard value.
本願発明は従来法のかゝる欠点に鑑みてなされ
たもので、棒材の断面積をリアルタイムで算定
し、オペレータの寸法調整を正確に基準断面積に
近ずけるよう誘導するものである。即ち本願発明
の目的は圧延ライン等の搬送中の棒材の断面にお
ける種々の位置の径を回転式の太さ計によつてス
パイラル状に求め、かくして得られた直径測定値
をもとに棒材の断面積を算定しかつ基準断面積と
の差を求め、表示する装置を提供することにあ
る。 The present invention has been made in view of these drawbacks of the conventional method, and is intended to calculate the cross-sectional area of a bar in real time and guide the operator to accurately adjust the dimensions to approach the reference cross-sectional area. That is, the object of the present invention is to spirally measure the diameter at various positions on the cross section of a bar being transported on a rolling line or the like using a rotary thickness gauge, and then to measure the diameter of the bar based on the diameter measurements thus obtained. An object of the present invention is to provide a device that calculates the cross-sectional area of a material, determines the difference from the reference cross-sectional area, and displays the difference.
以下図面により本願発明の詳細を説明する。第
1図に直径測定装置の原理を示す。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、
棒材1の影が受光レンズ4を通つて光電変換素子
アレイ5上に結像する。光電変換アレイ素子は電
荷結合装置(CCD)、バケツトブリゲート装置
(BBD)を応用したものが知られているが、本発
明ではCCDを用いており、アレイは1728ビツト
のものを採用した。このときの測定誤差は測定ス
パンを100mmとすると約60μmとなり実用上十分
である。又測定対象が小さい場合(最大径が20
mm)では512ビツトのものでも十分な精度が得ら
れる。光電変換アレイ素子5に投影された棒材1
の直径像は発信器6から加えられるシフトパルス
に従つてアレイ素子5から明暗に対応してパルス
列の型で出力されカウンタ7でパルスカウントさ
れる。このカウント動作は所定の周期で繰返し行
なわれ平均化される。パルスカウント値に変換さ
れた直径は演算装置9に伝達される。8はスプリ
ングである。 The details of the present invention will be explained below with reference to the drawings. Figure 1 shows the principle of the diameter measuring device. The light emitted from the light source 2 passes through the lens 3 and becomes a parallel ray,
The shadow of the bar 1 passes through the light receiving lens 4 and forms an image on the photoelectric conversion element array 5. Photoelectric conversion array elements using a charge coupled device (CCD) or a bucket bridge gate device (BBD) are known, but in the present invention, a CCD is used, and a 1728-bit array is used. The measurement error at this time is approximately 60 μm when the measurement span is 100 mm, which is sufficient for practical use. Also, if the object to be measured is small (maximum diameter is 20
mm), sufficient accuracy can be obtained even with 512 bits. Bar material 1 projected onto photoelectric conversion array element 5
According to the shift pulse applied from the transmitter 6, the diameter image is outputted from the array element 5 in the form of a pulse train corresponding to brightness and darkness, and is counted by the counter 7. This counting operation is repeated at a predetermined period and averaged. The diameter converted into a pulse count value is transmitted to the arithmetic unit 9. 8 is a spring.
第2図に本発明装置の具体的な構成を示す。即
ち前述の光源2、レンズ3、レンズ4、光電変換
アレイ素子5、スリツプリング8、および第1図
に於ける発信器6、カウンタ7は、回転体12に
1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1方向に連続回転する。
この回転体への電源の供給及び信号の授受は回転
体側のスリツプリング8とブラシ(図示せず)を
通じて行なわれる。本例では計数は回転体内で行
ない、その結果をスリツプリング8とブラシとの
信号授受手段により固定地上側へ伝えるが、シフ
トパルス及び信号パルスを伝送して固定地上側で
計数を行なつてもよい。又信号の授受にはトラン
ス結合を用いても良い。次に直径の測定タイミン
グについて説明する。 FIG. 2 shows a specific configuration of the device of the present invention. That is, the aforementioned light source 2, lens 3, lens 4, photoelectric conversion array element 5, slip ring 8, and the transmitter 6 and counter 7 in FIG. , are continuously rotated in one direction by a motor 10 around a fixed shaft 11.
Power is supplied to the rotating body and signals are exchanged through a slip ring 8 and a brush (not shown) on the rotating body side. In this example, counting is performed inside the rotating body, and the results are transmitted to the stationary ground side by the signal exchange means between the slip ring 8 and the brush, but it is also possible to carry out counting on the stationary ground side by transmitting shift pulses and signal pulses good. Further, transformer coupling may be used for transmitting and receiving signals. Next, the timing of measuring the diameter will be explained.
駆動モータ10には測寸部材2〜5が基準方向
(例えば鉛直線)から所定の角度θ回転する度に
信号を発生する角度検出器13が設置されてい
る。ここで投影式測寸機の場合180゜回転する度
に同じ部位の直径を測ることになるのでθは180
゜をn等分した数に等しくとる。即ち
θ=180゜/n (deg) …………(1)
である。次に第3図により断面積の近似の仕方に
ついて説明する。第3図の1点鎖線aは鉛直方向
直径部位を示しており、これを基準方向とする。
いまこの基準方向の直径測定値をD1とし、次に
θだけ時計方向に回転した方位の測定値をD2、
以下同様にして(n−1)θだけ回転した方位の
測定値をDoとすると、Do+1はD1と等しい方位の
径となる。いま材料1が停止していると考えると
かくして得られた直径データD1〜Doを用いて棒
材1の断面積は扇形の和の形で以下のように表わ
すことができる。 The drive motor 10 is equipped with an angle detector 13 that generates a signal every time the measuring members 2 to 5 rotate by a predetermined angle θ from a reference direction (for example, a vertical line). Here, in the case of a projection type measuring machine, the diameter of the same part is measured every time it rotates 180 degrees, so θ is 180
Take ゜ equal to the number divided into n equal parts. That is, θ=180°/n (deg) …………(1). Next, the method of approximating the cross-sectional area will be explained with reference to FIG. The one-dot chain line a in FIG. 3 indicates the vertical diameter portion, and this is taken as the reference direction.
Now let the diameter measurement value in this reference direction be D 1 , then the measurement value in the direction rotated clockwise by θ is D 2 ,
Similarly, if the measured value of the azimuth rotated by (n-1) θ is D o , D o+1 becomes the diameter of the azimuth equal to D 1 . Considering that the material 1 is now at rest, the cross-sectional area of the bar 1 can be expressed in the form of the sum of sector shapes as follows using the diameter data D 1 to D o obtained in this way.
従つて基準径D0のときの基準断面積S0に対する
差ΔSは
と表わされさらにDiを基準径D0と偏差ΔDiとの
和の形で
Di=D0+ΔDi …………(4)
と表わすとΔDiがD0に対して小さいので
又は
と表わすことができる。従つて基準断面積に対す
る誤差割合ΔRは(3),(5),(6)式ともに
のいずれの形でも表わされる。即ち(3)′,(5)′,
(6)′は順に各直径値の2乗和,偏差和,和の形と
なつている。このいずれの形で断面積誤差を表わ
すかについては演算装置での処理時間プログラム
の容易さによつて決められるが、誤差が問題なけ
れば(6)′の測定された径を累和する方式が最も容
易である。この(6)′式の場合の演算処理装置の処
理フローを第4図に示す。 Therefore, the difference ΔS with respect to the standard cross-sectional area S 0 when the standard diameter D 0 is Further, Di can be expressed in the form of the sum of the reference diameter D 0 and the deviation ΔDi as Di=D 0 +ΔDi ……(4) Since ΔDi is smaller than D 0 , or It can be expressed as Therefore, the error ratio ΔR with respect to the standard cross-sectional area is expressed by equations (3), (5), and (6). It can be expressed in either form. That is, (3)′, (5)′,
(6)' is in the form of the sum of squares, the sum of deviations, and the sum of each diameter value, in order. Which form to use to express the cross-sectional area error is determined by the ease of processing time programming in the arithmetic unit, but if there is no problem with the error, the method of (6)' in which the measured diameters are summed is the method used. Easiest. FIG. 4 shows the processing flow of the arithmetic processing unit in the case of equation (6)'.
次に断面積を扇形に分割して求める際の誤差に
ついて第5図により説明する。第5図は80φの棒
鋼の断面を5゜毎に測定したデータであり、見易
いように基準円からの偏差を拡大して表示したも
のである。今このような断面をもつ丸棒を角θを
いろいろ変えて(5)′式により断面積偏差率ΔRを
求めると(一例として鉛直方向を固定して考え
る)、第6図に示すごとくn=36に対してn=9
(θ=20゜)程度であればほぼ両側ともサンプリ
ング誤差は小さいがn=6(θ=30゜)以下にな
ると0.1〜0.15%の誤差となり、従来の2方向
(天地,左右)固定式の太さ計に対応するn=2
(θ=90゜)では0.2〜0.7%の誤差となる。従つ
てこの図からはnとしては9以上をとるべきであ
ることがわかる。しかしながら第6図では第5図
で鉛直軸を基準として考えた偏差率であるが、チ
ヤンネル数nが小さくなるとどの軸を基準に選ぶ
かによつても大きな誤差を生じる。従つてこうし
た誤差を避ける為にもチヤンネル数(分割数)n
はできる限り大きくとるべきであり、本発明の例
ではn=30(θ=6゜)としている。 Next, the error when calculating the cross-sectional area by dividing it into sectors will be explained with reference to FIG. Figure 5 shows the data obtained by measuring the cross section of an 80φ steel bar at 5° intervals, and the deviation from the reference circle is enlarged and displayed for ease of viewing. Now, if we change the angle θ of a round bar with such a cross section and calculate the cross-sectional area deviation rate ΔR using equation (5)' (considering the vertical direction fixed as an example), n= as shown in Figure 6. n=9 for 36
(θ = 20°), the sampling error is small on almost both sides, but when n = 6 (θ = 30°) or less, the error becomes 0.1 to 0.15%. n=2 corresponding to the thickness gauge
(θ=90°), the error will be 0.2 to 0.7%. Therefore, it can be seen from this figure that n should be 9 or more. However, although FIG. 6 shows the deviation rate based on the vertical axis in FIG. 5, when the number of channels n becomes small, a large error occurs depending on which axis is selected as the reference. Therefore, in order to avoid such errors, the number of channels (number of divisions) n
should be as large as possible, and in the example of the present invention, n=30 (θ=6°).
条材の長手方向の寸法バラツキについて第7図
に25φと65φの寸法変動の例を示す。同図によれ
ば先後端の一部を除きほぼ25φで5.5m、65φで
10m毎のサンプリングで大きな変動はなく従つて
サンプル長さ内の寸法バラツキはほぼ無視して良
いことがわかる。一方最終段速度はこの25φでは
7.35m/s,65φでは2.04m/sであつたので回
転支持体12の回転数をm(r.p.m)とすると
∴m40r.p.m
となるが、余裕を考えて本願発明の装置では45r.
p.mとした。この回転数は大きくなると第2図に
おける回転支持体12に強大な遠心力が働くので
現段階では45r.p.mが限界に近い速度であるとい
える。かくして第2図に示す測寸部材2,3,
4,5,8が0.66秒づつ回転し螺旋状に30分割角
度の直径値が刻々と求まり演算処理装置9は第4
図のフローに示す如く各角度位置の直径を加算し
半回転完了が角度検出器により検知されると(6)′
式により断面積偏差率ΔRを計算する。このとき
対象が熱間条材であれば温度を実測又は予測して
寸法の補正が必要であることはいうまでもない。
かくして得られた断面積偏差率ΔRは例えばニク
シー管や0.1%刻みのランプの点灯数等によつて
オペレータに刻々知らされるのでオペレータはこ
の偏差率の値及び変化に応じてロールギヤツプ変
更等のアクシヨンをとる。又部分的に偏差率ΔR
が負の箇所があれば上位のプロセスコンピユータ
ー(図示せず)によつてその箇所が追跡され、剪
断工程でリジエクトすることも可能である。 Regarding the dimensional variation in the longitudinal direction of the strip, Fig. 7 shows an example of the dimensional variation of 25φ and 65φ. According to the same figure, it is approximately 25φ and 5.5m except for a part of the front and rear ends, and 65φ is approximately 5.5m.
It can be seen that there is no large variation in sampling every 10 m, and therefore, the dimensional variation within the sample length can be almost ignored. On the other hand, the final stage speed is this 25φ
7.35m/s, and 2.04m/s for 65φ, so if the rotation speed of the rotating support 12 is m (rpm), then ∴m40r.pm, but considering the margin, the device of the present invention uses 45r.pm.
It was set as pm. As this rotational speed increases, a strong centrifugal force acts on the rotating support 12 in FIG. 2, so at this stage it can be said that 45 rpm is close to the limit speed. Thus, the measuring members 2, 3, shown in FIG.
4, 5, and 8 rotate every 0.66 seconds, and the diameter value of the 30-division angle is determined every moment in a spiral manner.
As shown in the flowchart of the figure, when the diameter of each angular position is added up and the completion of half a rotation is detected by the angle detector, (6)′
Calculate the cross-sectional area deviation rate ΔR using the formula. At this time, if the object is a hot strip, it goes without saying that it is necessary to actually measure or predict the temperature and correct the dimensions.
The cross-sectional area deviation rate ΔR obtained in this way is informed to the operator from time to time by, for example, the number of Nixie tubes or lamps lit in 0.1% increments, so the operator can take actions such as changing the roll gap according to the value and change of this deviation rate. Take. Also, partially the deviation rate ΔR
If there is a negative point, that point can be tracked by a higher-level process computer (not shown) and rejected in the shearing process.
こゝで本願発明では測寸体を1つとしたが直交
する2チヤンネルとすれば1/4回転ごとに断面積
が求まることはいうまでもない。 Here, in the present invention, one measuring body is used, but if two orthogonal channels are used, it goes without saying that the cross-sectional area can be determined every 1/4 rotation.
以上述べたように本願発明によれば断面積もし
くは単位長さ重量の正確な条材を圧延することが
でき、商取引、資源の有効利用上も極めて有効で
ある。 As described above, according to the present invention, it is possible to roll a strip with an accurate cross-sectional area or unit length and weight, and it is extremely effective in terms of commercial transactions and effective use of resources.
第1図は本願発明の構成を示す原理図、第2図
は同じくその機構部分の説明図、第3図は直径サ
ンプリングの説明図、第4図は本願発明の演算装
置の処理要領を説明するフローチヤート、第5図
は棒材のプロフイールの一例を示す図、第6図は
分割数と断面積誤差率の関係を示すグラフ、第7
図a,bは棒材の長手方向寸法変動例を示すグラ
フである。
1:棒材、2:ランプ、3,4: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:地上固定軸、12:回転軸、1
3:角度検出器。
Fig. 1 is a principle diagram showing the configuration of the present invention, Fig. 2 is an explanatory diagram of the mechanism, Fig. 3 is an explanatory diagram of diameter sampling, and Fig. 4 is an explanation of the processing procedure of the arithmetic device of the present invention. Flow chart, Figure 5 is a diagram showing an example of the profile of a bar, Figure 6 is a graph showing the relationship between the number of divisions and the cross-sectional area error rate, and Figure 7 is a graph showing the relationship between the number of divisions and the cross-sectional area error rate.
Figures a and b are graphs showing examples of changes in longitudinal dimensions of bars. 1: Bar, 2: Lamp, 3, 4: Lens, 5:
Photoelectric conversion array element, 6: Transmitter, 7: Counter, 8: Slip ring, 9: Arithmetic unit, 10:
Motor, 11: Ground fixed axis, 12: Rotating axis, 1
3: Angle detector.
Claims (1)
して連続回転し、半周回転をn等分(n>9)し
た角度位置における各直径値を測定する投影式直
径測定装置と、n箇の直径測定値Di(i=1〜
n)と基準直径D0を基に基準断面積S0に対する
測定断面積Sの偏差ΔS=S−S0=π/4n(〓〓/
Di2 −nD2 0)及び断面積偏差率ΔR=ΔS/S0を直径
測定装置の半回転毎に演算し、表示する演算装置
とからなる棒材断面積判定装置。[Claims] 1. Projected diameter that continuously rotates around a running hot bar about a pass line and measures each diameter value at an angular position that divides the half rotation into n equal parts (n > 9 ). A measuring device and n diameter measurements Di (i=1~
n) and the reference diameter D 0 , the deviation of the measured cross-sectional area S from the reference cross-sectional area S 0 is ΔS=S−S 0 =π/4n(〓〓/
Di 2 −nD 2 0 ) and a cross-sectional area deviation rate ΔR=ΔS/S 0 every half rotation of a diameter measuring device, and an arithmetic device that displays the results.
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP10095379A JPS5626211A (en) | 1979-08-08 | 1979-08-08 | Deciding device for bar stock sectional area |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP10095379A JPS5626211A (en) | 1979-08-08 | 1979-08-08 | Deciding device for bar stock sectional area |
Publications (2)
| Publication Number | Publication Date |
|---|---|
| JPS5626211A JPS5626211A (en) | 1981-03-13 |
| JPS6116004B2 true JPS6116004B2 (en) | 1986-04-26 |
Family
ID=14287712
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP10095379A Granted JPS5626211A (en) | 1979-08-08 | 1979-08-08 | Deciding device for bar stock sectional area |
Country Status (1)
| Country | Link |
|---|---|
| JP (1) | JPS5626211A (en) |
Cited By (1)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| JPS6261811U (en) * | 1985-10-08 | 1987-04-17 |
Families Citing this family (1)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| JP2016191588A (en) * | 2015-03-31 | 2016-11-10 | 学校法人早稲田大学 | Equipment for measuring the cross-sectional area of tensile test objects |
-
1979
- 1979-08-08 JP JP10095379A patent/JPS5626211A/en active Granted
Cited By (1)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| JPS6261811U (en) * | 1985-10-08 | 1987-04-17 |
Also Published As
| Publication number | Publication date |
|---|---|
| JPS5626211A (en) | 1981-03-13 |
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