JPS5924585A - Method and device for measuring electric power in high- frequency butt seam weld zone - Google Patents
Method and device for measuring electric power in high- frequency butt seam weld zoneInfo
- Publication number
- JPS5924585A JPS5924585A JP13302982A JP13302982A JPS5924585A JP S5924585 A JPS5924585 A JP S5924585A JP 13302982 A JP13302982 A JP 13302982A JP 13302982 A JP13302982 A JP 13302982A JP S5924585 A JPS5924585 A JP S5924585A
- Authority
- JP
- Japan
- Prior art keywords
- voltage
- frequency
- oscillation circuit
- current
- welding
- 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
Links
Classifications
-
- B—PERFORMING OPERATIONS; TRANSPORTING
- B23—MACHINE TOOLS; METAL-WORKING NOT OTHERWISE PROVIDED FOR
- B23K—SOLDERING OR UNSOLDERING; WELDING; CLADDING OR PLATING BY SOLDERING OR WELDING; CUTTING BY APPLYING HEAT LOCALLY, e.g. FLAME CUTTING; WORKING BY LASER BEAM
- B23K13/00—Welding by high-frequency current heating
- B23K13/01—Welding by high-frequency current heating by induction heating
- B23K13/02—Seam welding
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- Engineering & Computer Science (AREA)
- Mechanical Engineering (AREA)
- Investigating Or Analyzing Materials By The Use Of Electric Means (AREA)
- Investigating Or Analyzing Materials By The Use Of Magnetic Means (AREA)
Abstract
Description
【発明の詳細な説明】
本発明は高周波電縫抵抗溶接における溶接部に与えられ
る電力の瞬時値を測定する方法および装置に関する。DETAILED DESCRIPTION OF THE INVENTION The present invention relates to a method and apparatus for measuring the instantaneous value of electric power applied to a welding part in high frequency electric resistance welding.
高周波電縫溶接法は高速溶接がn」能であるなどの利点
から電縫管のシーム溶接などに利用さiLでいる。この
場合、溶接部に与えら11−る電力を一定にする必要が
あるがこれまでは、おもにオペレーターが溶接部の溶鋼
の目視観察やスクイズロール後でのVシェープエツジの
排出ビードの測温などによシ手動で人力をW1■整して
いた。この方法では、操作する人によって溶鋼の色の見
方や、板厚あるいは造管速度などの変化による溶鋼の表
面温度や色の変動に対する応答性に個人差や限界があシ
、しばしば冷接もしくはベネトレーターと称する溶接欠
陥の発生ずることがあった。また、発振器のプレート7
1を圧、電流、グリッド電流を制御信号として自動制御
する方法が提案さilているが、発振器伝送回路1.パ
イプ内の熱損失があり、精度が悪く、実用的ではない。High-frequency electric resistance welding is widely used for seam welding of electric resistance welding pipes because of its ability to perform high-speed welding. In this case, it is necessary to keep the power applied to the welding part constant, but until now, operators have mainly been responsible for visually observing the molten steel in the welding part and measuring the temperature of the discharge bead of the V-shaped edge after squeeze roll. I was manually adjusting the human power to W1■. With this method, there are individual differences and limitations in how the operator perceives the color of the molten steel, and in the responsiveness to changes in the surface temperature and color of the molten steel due to changes in plate thickness or pipe forming speed, and often involves cold welding or Venet welding. Welding defects called welding defects sometimes occur. Also, plate 7 of the oscillator
A method of automatically controlling oscillator transmission circuit 1 using voltage, current, and grid current as control signals has been proposed. There is heat loss in the pipe, the accuracy is poor, and it is not practical.
このような背titから0発明者らは高周波電流・電圧
などを測定することによって自動制御する方法を先に提
出(−た。この方法において、電力は高周波発振回路の
変流器(以下CTと称する)の−次側電流と二次側電圧
から口1算しているが、この際に必要な力率に相当する
比例定数は各リーイズの被溶接鋼管に対してあらかじめ
シンクロスコープなどから測定して求めておいた平均値
を用いていた。しかし、造′U中に管の板厚、■シェー
プ形状の変化等により、比例定数が変動するためVこ泪
7’−4して求めた電力は実際溶接部に力えらfl−で
いるiH力の瞬時値と異なることが判明した。The inventors previously proposed a method for automatic control by measuring high-frequency current and voltage. The proportional constant corresponding to the required power factor is calculated using a synchroscope etc. for each Lee's steel pipe to be welded. However, because the proportionality constant fluctuates due to changes in the thickness of the pipe, the shape of the pipe, etc. during construction, the power calculated by was found to be different from the instantaneous value of the iH force at the actual welding part.
高周波抵抗溶接法における高周波発振、負荷回路を第1
図に示す。第1図の(a) ij Vシュー1部お上び
管周技部を含む発振、負イWi回路、同図(blはVシ
ュー1部および管周技部を合成した発振、負荷回路、同
図(clは■シェーブ部、管周長部およびCTを合成し
た発振、負荷回路である。High frequency oscillation and load circuit in high frequency resistance welding method
As shown in the figure. Figure 1 (a) ij is an oscillation, negative I Wi circuit that includes the first part of the V-shoe and the circumference of the tube; In the same figure (cl is the oscillation and load circuit that combines the shave section, tube circumference section, and CT).
ここで、 Lo+ro ;伝送回路自己インダクタンス、抵抗。here, Lo+ro; Transmission circuit self-inductance, resistance.
L+、r+ ; CT−次側自己インダクタンス、抵抗
。L+, r+; CT-next side self-inductance, resistance.
Lz、rz : CT二次側自己インダクタンス、抵抗
、LSH’rN ; バイブ部総合自己インダクタンス
、抵抗、
L4.r4 ;” Vシェーブ部自己インダクタンス、
抵抗、
Ls+rs : バイブ周長部自己インダクタンス、抵
抗、
I+;CT−次側電流、
I2;CT二次側電流、
荀+ ; C’I’−次側電圧、
Ey;CT二次側電圧、
M;相互インダクタンス、
L;総合自己インダクタンス(=Lt+Lo −L’s
)、■ζ:総合抵抗(=r+ + ro + r+s
)。Lz, rz: CT secondary side self-inductance, resistance, LSH'rN; Vibrator overall self-inductance, resistance, L4. r4 ;” V-shave section self-inductance,
Resistance, Ls+rs: Self-inductance of the vibrator circumference, resistance, I+: CT-secondary side current, I2: CT secondary-side current, X+: C'I'-secondary-side voltage, Ey: CT secondary-side voltage, M: Mutual Inductance, L; total self-inductance (=Lt+Lo −L's
), ■ζ: Total resistance (=r+ + ro + r+s
).
測定器(LCRメータ)で第1図の回路定数を測定する
と、rs)rz 、ωLs )) rs であること
が認められる。この関係を用いると、■シェープ部に流
れる電流I4とCT−次側電流11の間には式(1)が
成立つ、
また、■シュー1部の電圧、電流IE2’ H14間の
位相差をθとすると、力率cosθは式(2)で表わさ
れる。When the circuit constants shown in FIG. 1 are measured with a measuring device (LCR meter), it is recognized that they are rs)rz, ωLs))rs. Using this relationship, ■Equation (1) holds true between the current I4 flowing in the shape part and the CT-next-side current 11. Also, ■The phase difference between the voltage and current IE2'H14 of the shoe 1 part is When θ is assumed, the power factor cos θ is expressed by equation (2).
したがって、■シ二−ブ(cl−に供給さ)]、る電力
Pは式(3)で表わさtする。Therefore, the power P generated by (supplied to cl-) is expressed by equation (3).
・・・・・・・・・(3)
これまでは%Vシェープ部に供給される電力は、CT−
次側の電流I+と、CT二次側の電圧E2の測定値と前
もって求めておいた比例定数αの平均値とからnInし
ていた。しかし、とのαは造管中一定ではなく、電カ一
定にするための自動制御が必ずしもう寸く行わi%ない
ことがわかった。・・・・・・・・・(3) Until now, the power supplied to the %V shape section was CT-
nIn was determined from the next-side current I+, the measured value of the voltage E2 on the CT secondary side, and the average value of the proportionality constant α determined in advance. However, it has been found that α is not constant during pipe making, and that automatic control to keep the electric power constant is not necessarily carried out precisely.
本発明は、上述した背景に鑑みてなさiまたものテアっ
て、シンクロスコープ、イメージ七ンーν一カメラおよ
び高周波電流計、電圧n1を組み合せて用い、造管中即
ち高周波電縫溶接中に卦ける比例定数を算出し、こね、
によって溶接部にJジえらiする電力の瞬時値を溶液中
連続的に求める方法および装置眞を提供することを目的
とする。In view of the above-mentioned background, the present invention has been devised by using a synchroscope, an image camera, a high frequency ammeter, and a voltage n1 in combination, during pipe making, that is, high frequency electric resistance welding. Calculate the proportionality constant, knead,
It is an object of the present invention to provide a method and apparatus for continuously determining the instantaneous value of electric power applied to a welding part in a solution.
本発明の要旨は、高周波発振恒i路のCT−次側の電圧
s ′t11流をシンノロスコープに人力し、このシン
クロスコープに描かれたり−リ”−シュ波形がY軸によ
って切らJLる電圧値2V+をイメージセフ サカメラ
と演算回路とによって求めるとともに電圧言1によって
一次側電圧の波高値E、を求め、とitらの電圧V+
、 E+を演り回路に入力してψ= 5in−’(VE
+)から−次(II+電圧、電流間の位相差ψを釣出し
、さらに、−次側電流II、二次側電圧& 、角周波数
ωを測定して演η−回路に入力し、後述する弐〇(塾ま
たは式(1υにしたがって溶接部1シ1時電力Pを求め
るものである。The gist of the present invention is to manually apply the voltage s't11 flow on the CT side of the high-frequency oscillation constant i path to a synchronoscope, and to cut the current waveform drawn on this synchroscope by the Y axis. The voltage value 2V+ is determined by the image safety camera and the arithmetic circuit, and the peak value E of the primary side voltage is determined by the voltage signal 1.
, E+ is input to the performance circuit and ψ=5in-'(VE
Find out the phase difference ψ between the -order (II+ voltage and current) from the -order (+), and further measure the -order current II, secondary side voltage & , and angular frequency ω and input them to the operation η- circuit, which will be described later. 2〇 (Cram school or formula (1υ) is used to find the power P for 1 welding part 1 hour.
以下、本発明を、図面を参照して具体的に説、明する。Hereinafter, the present invention will be specifically explained and explained with reference to the drawings.
式(3)の比例定数αを構成[2ているM 、Ls 、
rs 。The proportionality constant α in equation (3) consists of [2 M, Ls,
rs.
L2は造管中はとんど変化しないことがわかっている。It is known that L2 hardly changes during pipe making.
したがって、ω、 L3 、 I’sを造管中に測定す
ればよいことがわかる。Therefore, it can be seen that it is sufficient to measure ω, L3, and I's during pipe making.
第1図ニオイて、r、)’) r2.ωLs >> r
3とすると、L12は式(4)で表わされる。Figure 1: smell, r, )') r2. ωLs >> r
3, L12 is expressed by equation (4).
したがって、発振周波数fは式(5)で表わさ7’する
。Therefore, the oscillation frequency f is expressed by equation (5) as 7'.
式(5)から発振周波数fを測定することに正って角周
波数ωは2πfから、またLsは式(5)からn目りし
て求められる。なお、Lxは第1図の丘1と1+の間に
式(6)が成立つことから国司と(11(を測定するこ
とによっても求めら71.る。In addition to measuring the oscillation frequency f from Equation (5), the angular frequency ω can be obtained from 2πf, and Ls can be obtained from Equation (5) by nth division. Note that Lx can also be determined by measuring Kokushi and (11) since equation (6) holds true between hills 1 and 1+ in FIG.
一方、島とi、の間の位相差をψとすると力率cosψ
は式(7) 、 (8)で表わされる。On the other hand, if the phase difference between the island and i is ψ, then the power factor cosψ
is expressed by equations (7) and (8).
2rg
1〜たがってr3は、式(8)からe03 ψ、II
HI!+1を測定することによって求められる。ところ
で高周波高電流・11ε圧間の位相差を測定する技術が
これまで皆無であり、瞬時1シ1時のr、を求めること
が不可能であった。本発明ではシンクロスコープ、イメ
ージセンサカメラ、高周波高電流1の出力を用イ”’C
E+と11間の位相差ψを求めることができる。すなわ
ち1位相差ψの測定方法は、第2図、第3図に示すよう
に、シンクロスコープ1の縦軸に仏を、横軸にI+を人
力してリザージュ波形6を描かせる一方、イメージセン
サカメラ2の走査線がシンクロスコープのY’−Y軸に
一致するように配置する。2rg 1 ~ Therefore r3 is e03 ψ, II from equation (8)
HI! It is determined by measuring +1. By the way, until now there has been no technology for measuring the phase difference between high frequency high current and 11ε pressure, and it has been impossible to obtain the instantaneous r at 1 o'clock. In the present invention, a synchroscope, an image sensor camera, and a high frequency high current output are used.
The phase difference ψ between E+ and 11 can be determined. In other words, the method for measuring 1 phase difference ψ is as shown in Figs. 2 and 3, by manually drawing the Lissajous waveform 6 by manually drawing the Buddha on the vertical axis of the synchroscope 1 and I+ on the horizontal axis, while using the image sensor The camera 2 is arranged so that its scanning line coincides with the Y'-Y axis of the synchroscope.
イメージセンサカメラによって2つの11−1のある波
形5がイlらノするが、この波形を演′3つ、’ li
」回路7に入ノJしてここでリザージュ波形がY 1l
Ql+によって切らt上る部分ABの電圧2V+を演算
して求める。丑た、高周波電圧i13によって電圧E+
を求める。こitらの電圧Vl y lb+を演算回路
4に入力[7て式(9)にしたがって位相差ψを求める
。The image sensor camera captures a waveform 5 with two 11-1s.
” Enter the circuit 7 and here the Lissage waveform is Y 1l
Calculate and find the voltage 2V+ of the portion AB which is cut by Ql+ and increases by t. The voltage E+ is increased by the high frequency voltage i13.
seek. These voltages Vly lb+ are input to the arithmetic circuit 4 [7] and the phase difference ψ is determined according to equation (9).
一1■1
ψ−8in(−) ・・・・・・・・・(9)1
■シェープ部に供給さil、る電力は、式(3)、 (
(i) 。-1■1 ψ-8in(-) ・・・・・・・・・(9)1 ■The electric power supplied to the shape part is calculated by formula (3), (
(i).
(8)から式θ・0またけ(1■)で表わさノ1.る。From (8), it can be expressed by the formula θ・0 spanning (1■). Ru.
・・・・・−・・・・・・(M)
・・・・・・・・・Ot)
上式でω! J、I HII ) 008ψ、止2以外
の変数は造管中はとんど一定であり、造管前に適正な値
を演394装置に入力しておけばよい。・・・・・・−・・・・・・(M) ・・・・・・・・・Ot) In the above formula, ω! J, IHII) The variables other than 008ψ and stop 2 are almost constant during pipe making, and appropriate values can be input into the 394 machine before pipe making.
次に第4図を参照して溶接部に力えられる電力の瞬時値
を測定する装置およびその動作を説明する。Next, an apparatus for measuring the instantaneous value of electric power applied to a welding part and its operation will be described with reference to FIG.
高周波発振器14とCT9を結合する高周波伝送水冷パ
イプ17の片方に挿入した電流検出器8の出力i菅とC
’1” 9の一次側電圧E+とをシンクロスコープlに
入力する。シンクロスコープエのブラウン管面」二に描
かれたりサージュ波形がY軸によって切られる部分のT
lj圧2V+をイメージセンサカメラ2とリサージュ波
形電圧波$1[回路7でもとめる。一方、CT9の一次
側電正モを電圧N13で測定する。これら演算回路7、
電圧計3の出力全位相差・1υ、力演獅回路4に入力し
て式い+) 、 (11)のψを求める。電流検出器8
の出力α■、を電流演算器11に入力して電流I+を求
める。−まだ、C’l”、9の二次側電圧計を電圧側1
0で測定する。さらに、溶接部近傍に配置したサーチコ
イル15の出力を周波数演算回路16に入力して角周波
数ωを測定する。Output i and C of current detector 8 inserted into one side of high frequency transmission water cooling pipe 17 connecting high frequency oscillator 14 and CT9
Input the primary side voltage E+ of '1'9 into the synchroscope l.
The lj pressure 2V+ is also stopped by the image sensor camera 2 and the Lissajous waveform voltage wave $1 [circuit 7]. On the other hand, the primary side voltage of CT9 is measured at voltage N13. These arithmetic circuits 7,
Input the output total phase difference of the voltmeter 3, 1υ, to the force calculation circuit 4, and find the ψ of (11). Current detector 8
The output α■, is input to the current calculator 11 to obtain the current I+. - Still, the secondary side voltmeter of C'l'', 9 is connected to the voltage side 1.
Measure at 0. Further, the output of a search coil 15 placed near the welding portion is input to a frequency calculation circuit 16 to measure the angular frequency ω.
以上によって求めたl1il HII H止2 Hωを
位相差・電力演算回路4に入力して式(M) 、(11
)に従って■シュー1部に供給さJl、る電力Pを泪算
して求める。このようにして求めた電力Pは自動溶接制
御回路13へ入力し、この電力Pが一定になるように高
周波入力電流を制御する。The l1il HII H2 Hω obtained above is input to the phase difference/power calculation circuit 4, and formula (M), (11
), calculate and find the electric power P supplied to the first part of the shoe. The power P thus obtained is input to the automatic welding control circuit 13, and the high frequency input current is controlled so that the power P is constant.
本発明によれば、溶接部に乃えらノ1.る電力をオンラ
インで測定できるので、lδ接接電電力より正確に把握
でき、これによって自動電力制御も適切に行うことがで
き、溶接欠陥の発生がほとんどなくなった。なお、本発
明は電縫鋼管の製造分野だけでなく、銅板、形鋼などに
おける高周波抵抗溶接にも適用が可能である。According to the present invention, the welded portion has the following features: 1. Since the electric power generated by the welding process can be measured online, it can be grasped more accurately than the lδ contact electric power, and as a result, automatic power control can be performed appropriately, and the occurrence of welding defects has almost been eliminated. Note that the present invention is applicable not only to the field of manufacturing electric resistance welded steel pipes, but also to high frequency resistance welding of copper plates, shaped steel, and the like.
第1図は高周波抵抗溶接における発振、負荷回路を示し
た図、第2図はCT−次側電圧、電流間の位相差測定回
路を示した図、第3図は本発明に係るシンクロスコープ
に描かれるリサージュ波形を示した図、第4図は本発明
に係る溶接部電力測定装置の回路図である。
1・・・シンクロスコープ、2・・・イメージセンサカ
メラ、 3・・・−次側1[1,圧側
、4・・・位相差・’i[を力演算回路、5・・・イメ
ージセンサカメラの出力波形信号、6・・・リサージュ
波形、
7・・・リサージュ波形電圧演算回路、8・・・電流検
出器、
9・・・高周波発振回路の変流器CT。
10・・・二次側電圧計、 11・・・電流演算器、
13・・・自動溶接制御回路、
14・・・高周波発振器、 15・・・サーチコイル
。
16・・・周波数演算回路(周波数MN)。
代理人 弁理士 染 川 利 吉
第2図
第4図Fig. 1 is a diagram showing the oscillation and load circuit in high frequency resistance welding, Fig. 2 is a diagram showing the phase difference measurement circuit between the CT and secondary voltage and current, and Fig. 3 is a diagram showing the synchroscope according to the present invention. FIG. 4, which shows the drawn Lissajous waveform, is a circuit diagram of the welding part power measuring device according to the present invention. 1... Synchroscope, 2... Image sensor camera, 3...-Next side 1 [1, pressure side, 4... Phase difference/'i[ force calculation circuit, 5... Image sensor camera output waveform signal, 6... Lissajous waveform, 7... Lissajous waveform voltage calculation circuit, 8... current detector, 9... current transformer CT of the high frequency oscillation circuit. 10...Secondary side voltmeter, 11...Current calculator,
13... Automatic welding control circuit, 14... High frequency oscillator, 15... Search coil. 16...Frequency calculation circuit (frequency MN). Agent Patent Attorney Toshikichi SomekawaFigure 2Figure 4
Claims (2)
弓1.電流L ヲシンクロスコープに入力し、そのリサ
ージュ波形がY N111によって切らす)、る部分の
電圧2Vlをどして求め、さらに前記発振回路の二次側
電圧上〕2および角周波数ωを測定して溶接部に−Iう
えられる電力Pを。 から求めることを11“¥徴とする高周波電縫溶接部の
電力測定方法。 ただし、 Lolro ;伝送回路自己インダクタンス、抵抗。 L+、r+ : 高周波発振回路の変bIL器−次側自
己インダクタンス、抵抗、 Lt;r2: 高周波発振回路の変流器二次側自己イン
ダクタンス、抵抗、 LsHrs :被溶接管総合自己インダクタンス、抵抗
、 L4.r4: Vシュー1部自己インダクタンス、抵抗
、 Ls、rs ;管局長部自己インダクタンス、抵抗、M
;相互インダクタンス、 C;発振回路キャパシタンス。(1) Voltage E+ on the current transformer-next side of the high-frequency oscillation circuit. While measuring the current I + f, the voltage 1 of the -th +1111
Bow 1. Input the current L to the synchroscope, and find the voltage 2Vl at the part where the Lissajous waveform is cut off by YN111), and further measure the secondary side voltage 2 and the angular frequency ω of the oscillation circuit. The electric power P that can be applied to the welding part is -I. A method for measuring the power of a high-frequency electric resistance welding part, which is determined from Lt;r2: Current transformer secondary side self-inductance of high-frequency oscillation circuit, resistance, LsHrs: Total self-inductance of welded tube, resistance, L4.r4: V-shoe 1 part self-inductance, resistance, Ls, rs: Control section Self-inductance, resistance, M
; mutual inductance, C; oscillation circuit capacitance.
一次側電流計および一次側電流計と、前記発振回路の一
次側電流計、および一次(ill電圧E+を人力してリ
サージュ波形を描くシンクロスコープト、前記シンクロ
スコープのりザージュ波形を走査するイメージセンサカ
メラと、前i己イメージーヒンザカメシから出力さil
、た波形信号を人力して前記リーリ。 −シュ波形がY軸によって切ら1するf<jl、分の電
圧2V+を算出するりサージュ波形1シi I上演γ1
回路と、前記発振回路の二次側電圧E2を測定する電圧
計と、角周波数ωを測定する周波数目と、溶接中に前記
V+、E+ 、 I+ 、E2 、 Cat入力り、テ
溶JI部に与エラnる電力を算出する電力演算回路とを
有することを特徴とする高周波電縫溶接部の電力測定装
置。(2), the current transformer of the high frequency oscillation circuit - connected to the next side! a primary side ammeter and a primary side ammeter of the oscillation circuit, a synchroscope that manually draws a Lissajous waveform by applying the primary (ill voltage E+), and an image sensor that scans the Lissajous waveform of the synchroscope. The camera and the previous image - output from Hinza Kamishi
, manually input the waveform signal and perform the above-mentioned Reili. - Calculate the voltage 2V+ for f<jl, where the surge waveform is cut by the Y-axis.
circuit, a voltmeter that measures the secondary voltage E2 of the oscillation circuit, a frequency meter that measures the angular frequency ω, and the V+, E+, I+, E2, and Cat inputs during welding, and the welding JI section. A power measuring device for a high-frequency electric resistance welding part, comprising a power calculation circuit for calculating power given to an error.
Priority Applications (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP13302982A JPS5924585A (en) | 1982-07-30 | 1982-07-30 | Method and device for measuring electric power in high- frequency butt seam weld zone |
Applications Claiming Priority (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP13302982A JPS5924585A (en) | 1982-07-30 | 1982-07-30 | Method and device for measuring electric power in high- frequency butt seam weld zone |
Publications (1)
Publication Number | Publication Date |
---|---|
JPS5924585A true JPS5924585A (en) | 1984-02-08 |
Family
ID=15095133
Family Applications (1)
Application Number | Title | Priority Date | Filing Date |
---|---|---|---|
JP13302982A Pending JPS5924585A (en) | 1982-07-30 | 1982-07-30 | Method and device for measuring electric power in high- frequency butt seam weld zone |
Country Status (1)
Country | Link |
---|---|
JP (1) | JPS5924585A (en) |
Cited By (3)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
JPS62289383A (en) * | 1986-06-06 | 1987-12-16 | Sumitomo Metal Ind Ltd | Welding electric power measuring method for high-frequency welding equipment |
JP2008309295A (en) * | 2007-06-18 | 2008-12-25 | Higashio Mech Co Ltd | Flare joint |
US8911355B2 (en) | 2011-11-25 | 2014-12-16 | Olympus Medical Systems Corp. | Endoscope |
-
1982
- 1982-07-30 JP JP13302982A patent/JPS5924585A/en active Pending
Cited By (4)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
JPS62289383A (en) * | 1986-06-06 | 1987-12-16 | Sumitomo Metal Ind Ltd | Welding electric power measuring method for high-frequency welding equipment |
JPH0571357B2 (en) * | 1986-06-06 | 1993-10-07 | Sumitomo Metal Ind | |
JP2008309295A (en) * | 2007-06-18 | 2008-12-25 | Higashio Mech Co Ltd | Flare joint |
US8911355B2 (en) | 2011-11-25 | 2014-12-16 | Olympus Medical Systems Corp. | Endoscope |
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