JPS6133766A - Method and device for monitoring welding in gas shielded arc welding - Google Patents

Method and device for monitoring welding in gas shielded arc welding

Info

Publication number
JPS6133766A
JPS6133766A JP4926384A JP4926384A JPS6133766A JP S6133766 A JPS6133766 A JP S6133766A JP 4926384 A JP4926384 A JP 4926384A JP 4926384 A JP4926384 A JP 4926384A JP S6133766 A JPS6133766 A JP S6133766A
Authority
JP
Japan
Prior art keywords
welding
voltage
spike
output
circuit
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
JP4926384A
Other languages
Japanese (ja)
Inventor
Noboru Sugiyama
暢 杉山
Minoru Kobayashi
実 小林
Yutaka Nishikawa
裕 西川
Tetsuo Suga
哲男 菅
Masayoshi Iwasaki
岩崎 全良
Toshiro Nakatsuka
中塚 敏郎
Yasuhide Nakai
康秀 中井
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.)
Kobe Steel Ltd
Original Assignee
Kobe Steel 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 Kobe Steel Ltd filed Critical Kobe Steel Ltd
Priority to JP4926384A priority Critical patent/JPS6133766A/en
Publication of JPS6133766A publication Critical patent/JPS6133766A/en
Pending legal-status Critical Current

Links

Classifications

    • BPERFORMING OPERATIONS; TRANSPORTING
    • B23MACHINE TOOLS; METAL-WORKING NOT OTHERWISE PROVIDED FOR
    • B23KSOLDERING OR UNSOLDERING; WELDING; CLADDING OR PLATING BY SOLDERING OR WELDING; CUTTING BY APPLYING HEAT LOCALLY, e.g. FLAME CUTTING; WORKING BY LASER BEAM
    • B23K9/00Arc welding or cutting
    • B23K9/06Arrangements or circuits for starting the arc, e.g. by generating ignition voltage, or for stabilising the arc

Abstract

PURPOSE:To make detection at a high speed with a simple device and with high sensitivity and accuracy by subjecting the dynamical spiky voltage generated by the intrusion of air to a frequency sepn. and detecting the intrusion of the air. CONSTITUTION:An arithmetic circuit 7, to which the output S from a frequency band filter 6-1 and the output N from a low-frequency filter 6-2 are derived, operates an S/N ratio (detected intensity value) and outputs a detection signal M. A decision circuit 8 compares the detected intensity value S/N with the 1st criterion value K1 for the purpose of deciding the presence or absence of the generation of the spiky voltage S and outputs the signal C of the fixed waveform corresponding to the generation frequency of the pulse signal in a multivibrator circuit 9 when S/N>K1. An integration circuit 10 generates the voltage P corresponding to the generation frequency of the pulse signal. An air intrusion detector 11 delivers an air intrusion detection signal L as a command signal for driving alarm to an alarm device 12 when the output P from the circuit 10 attains the 2nd criterion value K2 for the purpose of discriminating the generation frequency of the voltage S.

Description

【発明の詳細な説明】 本発明は、ガスシールドアーク溶接における溶接監視方
法並びに装置間する。
DETAILED DESCRIPTION OF THE INVENTION The present invention relates to a welding monitoring method and apparatus for gas shielded arc welding.

一般に、ガスシールドアーク溶接においては、アルゴン
等のシールドガスによって完全に遮蔽して、溶接部の空
気による窒化や酸化を防止して良好な溶接結果を得るよ
うに設定されているが、実際の溶接作業においては、シ
ールド作用がアーク長の変化などの何らかの原因によっ
て低下すること及びアーク部に大気の風が直接あたるこ
となどに起因して、アーク中に空気が混入する場合があ
り、これにより溶接部のih撃値等の機械的性質の劣化
のみならず、気泡等の溶接欠陥の発生を来すようになる
Generally, in gas-shielded arc welding, settings are made to completely shield the welding area with a shielding gas such as argon to prevent nitridation and oxidation caused by air in the welding area and to obtain good welding results. During work, air may get mixed into the arc due to the shielding effect being reduced due to some reason such as a change in the arc length, or due to atmospheric wind hitting the arc directly, which may cause the welding to fail. This results in not only deterioration of mechanical properties such as the IH shock value of the part, but also the occurrence of welding defects such as bubbles.

例えば9%Ni鋼の共金TIG溶接においては、溶接の
ままのフェライト系溶接金属に高い低温靭性を確保する
為には、酸素、窒素等のガス成分、リン、硫黄などの不
純物元素を極力低減する必要があり、溶接部への空気(
酸素、窒素)の侵入は大問題である。
For example, in co-metal TIG welding of 9% Ni steel, in order to ensure high low-temperature toughness of the as-welded ferritic weld metal, gas components such as oxygen and nitrogen, and impurity elements such as phosphorus and sulfur are reduced as much as possible. Air to the welding area (
Intrusion of oxygen, nitrogen) is a major problem.

このような溶接部への空気の侵入状態を監視ず方法とし
て、従来、(a)溶接アーク電圧、電流を通常の計器で
監視する方法、(bl空気混入により発生する窒素酸化
物を捕集ノズルで採集し、その窒素酸化物を測定して検
出する方法(特開昭51−78553号)、(C)混入
した空気成分を発光スペクトルを測定して検出する方法
(特開昭56−43536号)等が提案されている。
Conventionally, methods for monitoring the state of air intrusion into the welding zone include (a) monitoring the welding arc voltage and current with ordinary instruments, and (bl) using a nozzle to collect nitrogen oxides generated due to air intrusion. (C) A method of detecting the mixed air component by measuring the emission spectrum (Japanese Patent Application Laid-open No. 56-43536). ) etc. have been proposed.

しかし、上記(a)の方法は、空気混入によって生ずる
電圧・電流の変動が微小である為に測定が難しく実用的
でない。また、(blの方法は、シールドガスの外乱及
び迅速性に問題があり、fc)の方法ではアークの光を
採光する器具を要する為、装置が複雑になると云う問題
がある。
However, the above method (a) is difficult to measure and is not practical because the fluctuations in voltage and current caused by air inclusion are minute. In addition, the method (bl) has problems with shielding gas disturbance and speed, and the method (fc) requires a device for collecting the arc light, resulting in a complicated apparatus.

本発明者等は上記従来の欠点・問題点を除去する為に種
々な検討と実験を重ねた結果、アーク雰囲気中に空気が
侵入した場合に、溶接アーク電圧波形は定常時電圧波形
にスパイク状電圧波形が多数重畳した波形となることを
見出し、このスパイク状電圧を取出して信号処理するこ
とにより、本発明を完成するに至った。。
The inventors of the present invention have conducted various studies and experiments in order to eliminate the above-mentioned conventional drawbacks and problems, and have found that when air enters the arc atmosphere, the welding arc voltage waveform becomes spike-like in the steady state voltage waveform. The present invention was completed by discovering that the voltage waveform is a waveform in which many voltage waveforms are superimposed, and by extracting this spike-like voltage and subjecting it to signal processing. .

本発明は、溶接アーク電圧を監視して特定周期範囲のス
パイク状電圧が重畳された場合にこれを検出して該検出
値を予め設定された判定基準と比較し、」二記検出値が
上記判定基準を越えた場合に空気侵入検出信号を発生せ
しめる構成とすることによって、純電気的ではあるが空
気の侵入を実用的に確実に検出することができ、従って
、検出の迅速性に優れ、簡単な装置で精度の高い監視を
行うことができるガスシールドアーク溶接における溶接
監視方法及び装置を提供することを目的とする。
The present invention monitors the welding arc voltage, detects when a spike-like voltage in a specific cycle range is superimposed, and compares the detected value with a preset criterion, By configuring the system to generate an air intrusion detection signal when the determination standard is exceeded, air intrusion can be detected practically and reliably, albeit purely electrically.Therefore, the detection speed is excellent. An object of the present invention is to provide a welding monitoring method and device for gas-shielded arc welding that can perform highly accurate monitoring with a simple device.

以下、本発明の一実施例を図面を参照して説明する。Hereinafter, one embodiment of the present invention will be described with reference to the drawings.

第1図は本発明を実施した装置のプロンク図、第2図は
溶接アーク電圧波形図を示している。第1図におい、1
は溶接電源、2はアーク電極、3はシールドガス雰囲気
、4はアーク電圧が導かれる絶縁増幅器、5はレベル変
換器(増幅器)であって、入力を信号処理に適したレベ
ルの信号に変換する。6−1は周波数帯域フィルタであ
って、第2図に示すスパイク状電圧(動的変動部分)S
の特定周波数範囲Sを通過帯域とし、レベル変換器5に
よりレベル変換された第2図の溶接アーク電圧からこの
スパイク状電圧分Sを分離して出力する。6−2は低周
波フィルタであって、レベル変換器5の出力を受け、第
2図に示す溶接アーク電圧のうちの定常時電圧分Nを通
過させる。7は演算回路であって、周波数帯域フィルタ
6−1の出力Sと低周波フィルタ6−2の出力Nが導か
れ、S/N比(検出強度値)を演算して該S/N比の大
きさを持つ検出信号Mを出力する。8は判定回路(比較
回路)であって、検出強度値S/Nを、スパイク状電圧
Sの発生の有無を判定する為の第1の判定基準値に1と
比較し、S/N>Klである場合に次のマルチバイブレ
ーク回路9でパルス信号の発生頻度に応じた定形波の信
号Cを出力する。10は周波数/電圧変換回路(積分回
路)であって、パルス信号の発生頻度に応じた電圧Pを
発生ずる。11は空気侵入検出器であって、周波数/電
圧変換回路10の出力Pが、スパイク状電圧Sの発生頻
度を判別する為の第2の判別基準値に2に達すると空気
侵入検出信号りを、例えば、警報器12に警報器駆動指
令信号Yとして送出する他、必要に応じて、溶接中断指
令やシールドガス流量の増大指令等の制御信号として用
いる。
FIG. 1 shows a diagram of a device embodying the present invention, and FIG. 2 shows a welding arc voltage waveform diagram. In Figure 1, 1
is a welding power source, 2 is an arc electrode, 3 is a shielding gas atmosphere, 4 is an isolation amplifier to which the arc voltage is guided, and 5 is a level converter (amplifier) that converts the input into a signal at a level suitable for signal processing. . 6-1 is a frequency band filter, and the spike-like voltage (dynamically fluctuating part) S shown in FIG.
The specific frequency range S of is set as a pass band, and this spike-like voltage S is separated from the welding arc voltage shown in FIG. 2 whose level has been converted by a level converter 5 and is output. 6-2 is a low frequency filter which receives the output of the level converter 5 and passes the steady state voltage N of the welding arc voltage shown in FIG. 7 is an arithmetic circuit which receives the output S of the frequency band filter 6-1 and the output N of the low frequency filter 6-2, calculates the S/N ratio (detection intensity value), and calculates the S/N ratio. A detection signal M having a certain magnitude is output. Reference numeral 8 denotes a determination circuit (comparison circuit) which compares the detected strength value S/N with 1 to a first determination reference value for determining the presence or absence of the spike-like voltage S, and determines that S/N>Kl In this case, the next multi-by-break circuit 9 outputs a signal C of a regular wave according to the frequency of occurrence of the pulse signal. Reference numeral 10 denotes a frequency/voltage conversion circuit (integration circuit), which generates a voltage P depending on the frequency of pulse signal generation. Reference numeral 11 denotes an air intrusion detector, which generates an air intrusion detection signal when the output P of the frequency/voltage conversion circuit 10 reaches a second determination reference value 2 for determining the frequency of occurrence of the spike voltage S. For example, in addition to being sent to the alarm device 12 as an alarm drive command signal Y, it is also used as a control signal such as a welding interruption command or a command to increase the shielding gas flow rate as necessary.

第2図に示す溶接アーク電圧のスパイク状電圧Sは、ア
ーク中の発光スペクトルのスペクトル線の変動に起因す
るものと考えられる。即ち、本発明者等の実験結果によ
れば、TIG熔接溶接合、空気侵入時にはスパイク状電
圧Sが発生することが確認されたが、この時、アーク中
には、無風状態の空気非侵入時には見られない多数の鉄
スペクトル線が検出された。これは、溶融プール中の溶
融鉄が侵入空気の酸素に触れて比較的蒸気圧高い酸化鉄
が生成しこれがアーク柱に混入して電気抵抗の変化をも
たらす為であると考えられる。上記スパイク状電圧の大
きさは上記鉄スペクトルの強度に対応し、その発生周期
はかなり広範囲にわたるが、10〜20m−5eeのも
のが高い頻度で発生するので、監視もしくは検出精度の
面からはこの周期範囲のものが適していることが実験に
より確められた。
The spike-like voltage S of the welding arc voltage shown in FIG. 2 is considered to be caused by fluctuations in the spectral lines of the emission spectrum in the arc. That is, according to the experimental results of the present inventors, it was confirmed that a spike-like voltage S is generated during TIG welding when air enters, but at this time, when there is no wind in the arc and no air enters, a spike voltage S is generated. A large number of missing iron spectral lines were detected. This is thought to be because molten iron in the molten pool comes in contact with oxygen from the invading air, producing iron oxide with a relatively high vapor pressure, which mixes into the arc column and causes a change in electrical resistance. The magnitude of the above-mentioned spike-like voltage corresponds to the intensity of the above-mentioned iron spectrum, and the period of occurrence is quite wide, but since 10 to 20 m-5ee occurs frequently, this is difficult from the viewpoint of monitoring or detection accuracy. Experiments have confirmed that a periodic range is suitable.

実施例の周波数帯域フィルタ6−1はこの10〜20 
m−s e cの周期に対応する特定周波数帯域S (
約50〜100Hz)を通過帯域とする。
The frequency band filter 6-1 of the embodiment has these 10 to 20
A specific frequency band S (
The pass band is approximately 50 to 100 Hz).

従って、周波数帯域フィルタ6−1は定常時電圧Nにス
パイク状電圧Sが重畳されていない場合は出力しないが
、空気の侵入によりスパイク状電圧Sが発生するとこれ
を分離して出力する。周波数帯域フィルタ6−1で分離
されたスパイク状電圧分Sは演算回路7において、定常
時電圧分Nで割算され、検出強度値S/Nが演算される
が、これは、溶接条件の変動に伴う影響を除去する為で
ある。
Therefore, the frequency band filter 6-1 does not output when the spike-like voltage S is not superimposed on the steady-state voltage N, but when the spike-like voltage S is generated due to the intrusion of air, it separates it and outputs it. The spike-like voltage component S separated by the frequency band filter 6-1 is divided by the steady state voltage component N in the calculation circuit 7 to calculate the detected strength value S/N. This is to eliminate the effects associated with this.

判定回路8の第1の判定基準値に1は、シールド雰囲気
内への侵入空気量を変えて、窒素含有率と溶接金属の靭
性(吸収エネルギー)との相関関係を測定し、上記靭性
の許容値に基いて予め設定した限界窒素濃度を与えた時
の侵入空気量時の検出信号Mの値(検出強度値S/N)
(但し、通常の溶接アーク電圧の雑音をVsとした場合
、M〉Vsとなるように、K1を設定する。)が用いら
れる。勿論、この第1の判定基準値に1を定める為の特
性値としては上記窒素含有量の他、溶接金属中の発生気
孔数等の他の溶接欠陥状況を利用することもできる。判
定回路8は演算回路8が出力した場合に検出信号Mの大
きさ即ちパルス波高値が第1の判定基準値に1を越えて
いるパルスを検出してその都度定レベルの判定信号Cを
出力する。この出力Cはスパイク状電圧Sの周期と対応
関係にある周波数を持つ信号であって、マルチバイブレ
ーク回路9で周波数に比例した太さを持つ所定幅の矩形
波の電圧信号■に変換される。
The first judgment reference value 1 of the judgment circuit 8 measures the correlation between the nitrogen content and the toughness (absorbed energy) of the weld metal by changing the amount of air entering the shield atmosphere, and determines the tolerance of the above toughness. Value of detection signal M (detection intensity value S/N) at the time of intruding air amount when a preset limit nitrogen concentration is given based on the value
(However, when the noise of the normal welding arc voltage is Vs, K1 is set so that M>Vs.) is used. Of course, other welding defect conditions such as the number of pores generated in the weld metal can be used in addition to the nitrogen content as the characteristic value for setting the first criterion value to 1. The judgment circuit 8 detects a pulse whose magnitude of the detection signal M, that is, the pulse height value exceeds the first judgment reference value by 1 when the arithmetic circuit 8 outputs it, and outputs a judgment signal C at a constant level each time. do. This output C is a signal having a frequency corresponding to the period of the spike voltage S, and is converted by the multi-by-break circuit 9 into a rectangular wave voltage signal (2) having a predetermined width and a thickness proportional to the frequency.

かくして、周期が10〜20m−5ecの範囲内にあり
、所定の大きさを越える波高のスパイク状電圧Sの発生
が検出されるが、本実施例ではスパイク状電圧Sの発生
頻度をも判定条件に加味して検出精度を上げる為に、周
波数/電圧変換回路10に導いて発生頻度に応じたアナ
ログ信号Pに変換し、この信号大きさが判定基準値に2
に達した時に空気侵入検出器11が出力動作して空気侵
入検出信号りを送出するようにしである。この判定基準
値に2は、風速とシャルピー値或いは風速と単位長さ当
りの気孔数との関係を実験的に求め、その風速で信号を
発するように定めらられる。
In this way, the occurrence of a spike-like voltage S whose period is within the range of 10 to 20 m-5 ec and whose wave height exceeds a predetermined magnitude is detected, but in this embodiment, the frequency of occurrence of the spike-like voltage S is also used as a determination condition. In order to increase the detection accuracy by taking into consideration
The air intrusion detector 11 operates to output an air intrusion detection signal when the air intrusion detection signal reaches this point. This criterion value of 2 is determined by experimentally determining the relationship between wind speed and Charpy value or between wind speed and the number of pores per unit length, and is determined to emit a signal at that wind speed.

従って、溶接アーク電圧にスパイク状電圧Sが重畳され
、該スパイク状電圧Sが上記周期範囲にあって所定以上
の大きさを有し、且つ発生頻度が高い場合にのみ上記空
気侵入検出信号I2が発生して警報器12が作動し、空
気の侵入があったことが報知されるので、いたずらに警
報器12が鳴動したりする誤検出は防止され、その検出
精度は極めて高い。
Therefore, only when the spike-like voltage S is superimposed on the welding arc voltage, the spike-like voltage S is within the periodic range, has a magnitude greater than a predetermined value, and occurs frequently, the air intrusion detection signal I2 is activated. When this occurs, the alarm 12 is activated and the presence of air intrusion is notified. This prevents erroneous detection such as the alarm 12 going off unnecessarily, and the detection accuracy is extremely high.

なお、上記実施例は、シールドガスがArガスである場
合について説明したが、Arガス中にHeガスを添加す
ると、アーク温度が上昇することにより、鉄スペクトル
線強度が増加し、対応してスパイク状電圧の波高が高く
なるので、検出感度をより高めることができる。
Note that the above embodiment has been described with reference to the case where the shielding gas is Ar gas, but when He gas is added to Ar gas, the iron spectral line intensity increases due to the increase in arc temperature, and a corresponding spike occurs. Since the wave height of the voltage becomes higher, detection sensitivity can be further increased.

以下に、上記第1図の装置を用いて実験を行ったときの
実験結果について説明する。
Below, the results of an experiment conducted using the apparatus shown in FIG. 1 will be explained.

〔第1の実験結果〕 〈溶接条件〉 電極:2%Th入りW(inφ) ワイヤ:9%Ni鋼(1,2mφ) C: 0.02%、Mn:0.45%、Sl:0.05
%、P:0.002%、Ni:11.15%: O: 
0.005%N : O,OO2%。
[First experimental results] <Welding conditions> Electrode: 2% Th-containing W (inφ) Wire: 9% Ni steel (1.2mφ) C: 0.02%, Mn: 0.45%, Sl: 0. 05
%, P: 0.002%, Ni: 11.15%: O:
0.005%N: O, OO2%.

母材:JTS  G3127 5L9N60、極性:D
C− 姿勢:立向(ウィービング) 溶接電流72 B OA、溶接電圧:11V、溶接速度
:5cm/min、 シールドガス流量:Ar、254!/min。
Base material: JTS G3127 5L9N60, polarity: D
C- Posture: Vertical (weaving) Welding current 72 B OA, Welding voltage: 11V, Welding speed: 5cm/min, Shielding gas flow rate: Ar, 254! /min.

(2重シールド) ワイヤ供給速度:20g/min、 電極の突出し長さ:15mm、 電源:市販500AのTIG溶接電源。(double shield) Wire feeding speed: 20g/min, Electrode protrusion length: 15mm, Power source: Commercially available 500A TIG welding power source.

上記条件下において、風速を制御して空気侵入量を調整
し、各風速における検出強度値S/N及び溶着金属中の
総窒素量を測定した。一方許容窒素限界量は、靭性面(
−196℃で10Kg以上)から見て約1100ppで
あると考えられるので、これを考慮して限界S/N比、
即ち、判定基準値Kを定めた。第3図はその監視状況を
図示したもので、許容窒素量に対する空気侵入の状況を
精度良く検出していることが分かる。
Under the above conditions, the amount of air intrusion was adjusted by controlling the wind speed, and the detected intensity value S/N and the total amount of nitrogen in the weld metal at each wind speed were measured. On the other hand, the allowable limit amount of nitrogen is determined from the toughness aspect (
Considering this, the limit S/N ratio is
That is, a criterion value K was determined. FIG. 3 shows the monitoring situation, and it can be seen that the air intrusion situation with respect to the allowable nitrogen amount is detected with high accuracy.

次に、上記判別基準値に2を、発生気孔数に基づいて設
定した場合の例を示す。
Next, an example will be shown in which the discrimination reference value is set to 2 based on the number of generated pores.

〔第2の実験結果〕 〈溶接条件〉 ワイヤ:MOS 0 (1,6mmφ)C: 0.09
%、Mn:1.09%、Si1.46%、P:0.01
3%、 S:0.012%、 母材:JISG3106.5M50A。
[Second experimental results] <Welding conditions> Wire: MOS 0 (1.6 mmφ) C: 0.09
%, Mn: 1.09%, Si 1.46%, P: 0.01
3%, S: 0.012%, Base material: JISG3106.5M50A.

極性:DC(+) 姿勢二下向(ストレート)、 溶接電流:375A、溶接電圧:30V、溶接速度: 
89 cm/m i n。
Polarity: DC (+) Posture 2 downward (straight), Welding current: 375A, Welding voltage: 30V, Welding speed:
89 cm/min.

シールドガス流量:C0125j!/min。Shield gas flow rate: C0125j! /min.

ワイヤ供給速度:940cm/min、電極の突出し長
さ:19mm、 電源二市販500A容量のCO溶接電源。
Wire feeding speed: 940cm/min, electrode protrusion length: 19mm, power supply 2 Commercially available CO welding power source with 500A capacity.

上記条件下において、シールドガス中の窒素%を変化さ
せ、各濃度における検出信号Mを測定し、その濃度表作
変化を求める一方、各濃度における気孔発生数を求めた
。CO溶接における気孔発生数の許容値を約200個/
6インチ(15,24cm)  (はぼJTS級に相当
)とすると、これに対応する検出信号Mの値となった時
点で空気侵入検出信号りを発生せしめた。第4図はこの
時の監視状況を示したもので上記許容値に対応する窒素
量で警報が発生しており、空気侵入の状況を確実に検出
していることが分かる。
Under the above conditions, the percentage of nitrogen in the shielding gas was varied, the detection signal M at each concentration was measured, and the change in the concentration table was determined, while the number of pores generated at each concentration was determined. The allowable number of pores in CO welding has been set to approximately 200/
Assuming 6 inches (15.24 cm) (equivalent to JTS class), an air intrusion detection signal was generated when the corresponding value of the detection signal M was reached. FIG. 4 shows the monitoring situation at this time, and it can be seen that an alarm is generated when the amount of nitrogen corresponds to the above-mentioned allowable value, and that the situation of air intrusion is reliably detected.

なお、上記は9%Ni鋼の共金TIG溶接の場合につい
て説明したが、一般の消耗電極式ガスシールドアーク溶
接に本発明を実施して同様の効果が得られることは明ら
かである。
Although the above description has been made regarding the case of alloy TIG welding of 9% Ni steel, it is clear that similar effects can be obtained by applying the present invention to general consumable electrode type gas shield arc welding.

また、本発明は、スパイク状電圧の周期を適正に選択す
れば、アーク溶接におけるアーク安定性の評価方法とし
ても効果的な方法であることが理解される。
Furthermore, it is understood that the present invention is an effective method for evaluating arc stability in arc welding if the period of the spike voltage is appropriately selected.

以上の如く、本発明によれば、空気侵入により発生する
動的なスパイク状電圧を周波数分離して該スパイク状電
圧の存在の有無に基づいて検出するものであるから、従
来の溶接アーク電圧の変化から検出しようとする場合と
異なって、確実に空気侵入を検出することができ、純電
気的に検出するものであるから、迅速性に優れ、装置も
簡単で、感度・精度の高い検出を行うことができる。
As described above, according to the present invention, the dynamic spike-like voltage generated due to air intrusion is frequency-separated and detected based on the presence or absence of the spike-like voltage. Unlike detection based on changes, air intrusion can be reliably detected, and since it is purely electrically detected, it is quick, the equipment is simple, and the detection is highly sensitive and accurate. It can be carried out.

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

第1図は本発明によるガスシールドアーク溶接における
溶接監視方法を実施したブロック図、第2図は溶接アー
ク電圧の波形図、第3図及び第4図は実験における警報
発生状態を示すグラフ線図である。 5− レベル変換器、6−1 =−周波数帯域フィルタ
、6−2−低周波フィルタ、7−演算回路、8=−判定
回路、9−マルチバイブレーク回路、1゜−周波数/電
圧変換回路、11−空気侵入検出器。
Fig. 1 is a block diagram implementing the welding monitoring method in gas-shielded arc welding according to the present invention, Fig. 2 is a waveform diagram of welding arc voltage, and Figs. 3 and 4 are graph diagrams showing alarm generation states in experiments. It is. 5- Level converter, 6-1 =- Frequency band filter, 6-2- Low frequency filter, 7- Arithmetic circuit, 8 =- Judgment circuit, 9- Multi-by-break circuit, 1°- Frequency/voltage conversion circuit, 11 - Air intrusion detector.

Claims (7)

【特許請求の範囲】[Claims] (1)溶接アーク電圧を監視して特定周期範囲のスパイ
ク状電圧が重畳された場合にこれを検出して該検出値を
あらかじめ設定された判定基準と比較し、検出値が上記
判定基準を越えた場合に空気侵入検出信号を発生せしめ
ることを特徴とするガスシールド溶接における溶接監視
方法。
(1) Monitor the welding arc voltage, detect when a spike-like voltage in a specific periodic range is superimposed, and compare the detected value with a preset judgment standard, and if the detected value exceeds the above judgment standard. A welding monitoring method for gas shield welding, characterized in that an air intrusion detection signal is generated when an air intrusion is detected.
(2)スパイク状電圧の特定周期範囲が10〜20m・
secであることを特徴とする特許請求の範囲第1項記
載のガスシールド溶接における溶接監視方法。
(2) The specific periodic range of spike voltage is 10 to 20 m.
2. The welding monitoring method in gas shield welding according to claim 1, wherein the welding monitoring method is sec.
(3)判定基準の一つがスパイク状電圧の大きさであり
、他の一つが該スパイク状電圧の発生頻度であることを
特徴とする特許請求の範囲第1項又は第2項記載のガス
シールド溶接における溶接監視方法。
(3) The gas shield according to claim 1 or 2, wherein one of the criteria is the magnitude of the spike voltage, and another one is the frequency of occurrence of the spike voltage. Welding monitoring method in welding.
(4)スパイク状電圧と溶接アーク電圧の定常時電圧と
の比を判定基準と比較することを特徴とする特許請求の
範囲第1項又は第2項又は第3項記載のガスシールド溶
接における溶接監視方法。
(4) Welding in gas shield welding according to claim 1, 2, or 3, characterized in that the ratio of the spike voltage to the steady state voltage of the welding arc voltage is compared with a criterion. Monitoring method.
(5)ガスシールド溶接が、9%Ni鋼の共金TIG溶
接である特許請求の範囲第1項又は第2項又は第3項又
は第4項記載のガスシールド溶接における溶接監視方法
(5) The welding monitoring method in gas shield welding according to claim 1 or 2 or 3 or 4, wherein the gas shield welding is cometal TIG welding of 9% Ni steel.
(6)溶接アーク電圧をレベル変換する増幅器、該増幅
器の出力から特定周波数域のスパイク状電圧分と定常時
電圧分を分離するフィルタ回路、上記スパイク状電圧分
と上記定常時電圧分とを比較する演算回路、該演算回路
の出力が第1の判定基準値を越えた場合に出力する判定
回路、該判定回路の出力の時間積分値が第2の判定基準
値を越えた場合に空気侵入検出信号を発生する回路を具
えるとこを特徴とするガスシールド溶接における溶接監
視装置。
(6) An amplifier that converts the level of the welding arc voltage, a filter circuit that separates the spike voltage component in a specific frequency range from the steady state voltage component from the output of the amplifier, and a comparison between the spike voltage component and the steady state voltage component. an arithmetic circuit that outputs an output when the output of the arithmetic circuit exceeds a first judgment reference value, and an air intrusion detection circuit that outputs an output when the output of the arithmetic circuit exceeds a second judgment reference value. A welding monitoring device for gas shield welding, characterized by comprising a circuit that generates a signal.
(7)演算回路が、スパイク状電圧分と定常時電圧分と
の比を演算することを特徴とする特許請求の範囲第6項
記載のガスシールド溶接における溶接監視装置。
(7) A welding monitoring device for gas shield welding according to claim 6, wherein the arithmetic circuit calculates a ratio between a spike voltage component and a steady state voltage component.
JP4926384A 1984-03-16 1984-03-16 Method and device for monitoring welding in gas shielded arc welding Pending JPS6133766A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP4926384A JPS6133766A (en) 1984-03-16 1984-03-16 Method and device for monitoring welding in gas shielded arc welding

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP4926384A JPS6133766A (en) 1984-03-16 1984-03-16 Method and device for monitoring welding in gas shielded arc welding

Publications (1)

Publication Number Publication Date
JPS6133766A true JPS6133766A (en) 1986-02-17

Family

ID=12825938

Family Applications (1)

Application Number Title Priority Date Filing Date
JP4926384A Pending JPS6133766A (en) 1984-03-16 1984-03-16 Method and device for monitoring welding in gas shielded arc welding

Country Status (1)

Country Link
JP (1) JPS6133766A (en)

Cited By (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
WO2008101264A1 (en) * 2007-02-22 2008-08-28 Fronius International Gmbh Device and method for shielding gas measurement

Cited By (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
WO2008101264A1 (en) * 2007-02-22 2008-08-28 Fronius International Gmbh Device and method for shielding gas measurement
US8210025B2 (en) 2007-02-22 2012-07-03 Fronius International Gmbh Arrangement and method for protective-gas measurement

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