JPS63152B2 - - Google Patents
Info
- Publication number
- JPS63152B2 JPS63152B2 JP12508779A JP12508779A JPS63152B2 JP S63152 B2 JPS63152 B2 JP S63152B2 JP 12508779 A JP12508779 A JP 12508779A JP 12508779 A JP12508779 A JP 12508779A JP S63152 B2 JPS63152 B2 JP S63152B2
- Authority
- JP
- Japan
- Prior art keywords
- welding
- arc
- short
- short circuits
- burn
- 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
Links
- 238000003466 welding Methods 0.000 claims description 82
- CURLTUGMZLYLDI-UHFFFAOYSA-N Carbon dioxide Chemical compound O=C=O CURLTUGMZLYLDI-UHFFFAOYSA-N 0.000 claims description 22
- 229910002092 carbon dioxide Inorganic materials 0.000 claims description 11
- 239000001569 carbon dioxide Substances 0.000 claims description 11
- 238000000034 method Methods 0.000 claims description 7
- 230000007704 transition Effects 0.000 description 12
- 239000002184 metal Substances 0.000 description 11
- 239000000155 melt Substances 0.000 description 4
- 229910001209 Low-carbon steel Inorganic materials 0.000 description 2
- 230000008859 change Effects 0.000 description 2
- 230000007423 decrease Effects 0.000 description 2
- 230000007547 defect Effects 0.000 description 2
- 238000010586 diagram Methods 0.000 description 2
- 230000001788 irregular Effects 0.000 description 2
- 239000000463 material Substances 0.000 description 2
- 230000008439 repair process Effects 0.000 description 2
- 230000008901 benefit Effects 0.000 description 1
- 230000002950 deficient Effects 0.000 description 1
- 230000003111 delayed effect Effects 0.000 description 1
- 238000001514 detection method Methods 0.000 description 1
- 230000000694 effects Effects 0.000 description 1
- 238000002844 melting Methods 0.000 description 1
- 230000008018 melting Effects 0.000 description 1
- 230000035515 penetration Effects 0.000 description 1
- 230000008569 process Effects 0.000 description 1
- 239000007787 solid Substances 0.000 description 1
- 238000011179 visual inspection Methods 0.000 description 1
Landscapes
- Arc Welding In General (AREA)
Description
【発明の詳細な説明】
本発明は高速度炭酸ガスアーク溶接の不良検出
方法に関するものである。DETAILED DESCRIPTION OF THE INVENTION The present invention relates to a method for detecting defects in high-speed carbon dioxide arc welding.
通常、炭酸ガスアーク溶接方法のうち、比較的
大電流を使用した溶接では電極先端で溶融した溶
融金属が大塊の溶滴となり、電磁反発力によつ
て、電極先端から不規則に溶滴が離脱する粒滴移
行形態(以下、粒滴移行という)となり、逆に比
較的小電流を使用した溶接では溶滴が溶融池面に
接触することによつて移行する接触移行形態(以
下、短絡移行という)となることが知られてい
る。後者の短絡移行溶接においては、アークの発
生と短絡とがくり返して行われ、短絡のたびに溶
滴が溶融池に移行するので、アーク発生状態が良
好なときにはアーク発生と短絡とが規則正しく反
復して行われ良好な溶接結果が得られる。このア
ーク発生と短絡との一定時間内のくり返し回数
(以下1秒間にくり返される回数を「短絡回数」
といい、Hzで表わす。)は、アークの発生状態が
良好なときは、溶接電極の直径、その材質、溶接
電流、溶接電圧、ワイヤ突き出し長さなどの溶接
条件の相違によつて異なるが、30乃至120Hzぐら
いである。この短絡回数は、溶接条件が一定であ
れば、アーク発生状態が良好なときは、30乃至
120Hzの範囲内で略一定の短絡回数を示している
が、アークの発生状態が不良になつて溶接結果が
不良になるようなときには、短絡回数に変化が現
われる。したがつて、短絡移行溶接においては、
短絡回数が設定範囲よりもはずれ例えば10乃至30
Hzに低下したときに溶接不良であると判断するこ
とが通常行われている。しかし、前者の粒滴移行
溶接においては、短絡移行溶接のように溶滴が必
ずしも短絡によつて移行しないために、短絡移行
溶接のような規則正しい短絡が行われない。した
がつて、粒滴移行溶接においては、短絡移行溶接
のように短絡回数の増減によつて溶接不良を判断
するようなことは行われていなかつた。 Normally, in carbon dioxide arc welding, in welding that uses a relatively large current, the molten metal melted at the tip of the electrode becomes large droplets, and the droplets irregularly separate from the tip of the electrode due to electromagnetic repulsion. On the other hand, in welding using a relatively small current, a contact transfer mode occurs in which droplets transfer when they come into contact with the molten pool surface (hereinafter referred to as short-circuit transfer). ) is known to be. In the latter type of short-circuit transfer welding, arc generation and short circuiting occur repeatedly, and each time a short circuit occurs, the droplets transfer to the molten pool, so when arc generation conditions are good, arc generation and short circuits repeat regularly. Good welding results can be obtained. The number of times this arc generation and short circuit occur within a certain period of time (hereinafter the number of times repeated per second is the "number of short circuits")
It is expressed in Hz. ) is approximately 30 to 120 Hz when the arc is in good condition, although it varies depending on the welding conditions such as the diameter of the welding electrode, its material, welding current, welding voltage, and wire protrusion length. If the welding conditions are constant, the number of short circuits will be 30 to 30 when the arc generation condition is good.
Although the number of short circuits is approximately constant within the range of 120 Hz, when the arc generation condition becomes poor and the welding result becomes poor, the number of short circuits changes. Therefore, in short-circuit transition welding,
The number of short circuits is outside the setting range, for example 10 to 30.
It is common practice to judge that welding is defective when the value drops to Hz. However, in the former type of droplet transfer welding, the droplets do not necessarily transfer due to a short circuit as in short-circuit transfer welding, so regular short circuits as in short-circuit transfer welding are not performed. Therefore, in droplet transfer welding, welding defects have not been determined based on an increase or decrease in the number of short circuits, unlike short circuit transfer welding.
この粒滴移行溶接のうちでも、大電流域では第
1図または第2図に示すように電極1と被溶接物
2との間にアーク3を発生させることによつて生
じる溶融池2aが大きく、かつ、くぼみ2bも大
きくなるので、電極先端を溶融池内まで埋もれさ
せ、電極先端の溶融部分1aが大きくくぼんだ溶
融池内で移行が行われるようにして溶接(以下
「埋れアーク」という)が行われている。溶接電
流が大電流の埋もれアークであつても、溶接速度
が低速度例えば50cm/minであるときは、第1図
に示すように溶融池のくぼみが大きく電極先端の
溶融部分1aが大塊に成長して電磁反発力によつ
て離脱し前述したような不規則な短絡が行われ
る。しかし、同じく大電流の埋もれアーク溶接で
あつても、溶接速度が高速度例えば1m/min以
上の場合には、アーク電圧を低くすると第2図に
示すように溶融池2aのくぼみが狭くなり、電極
の先端が溶融池前方2cにそつて溶けてとがり、
これにそつて電極先端の溶融部分1aは流れ落ち
るので、スパツタが少ない利点がある。しかも、
この高溶接速度埋れアーク溶接では、強力なアー
ク力によつて、アーク直下の被溶接物の溶融金属
が後方に押し流されて固体露出面が現われるの
で、深い溶け込みを得ることができる反面、アー
ク直下に溶融金属がなく、被溶接物の未溶融部分
に直接にアークがあたるために被溶接物が溶け落
ちやすいという欠点もある。このような溶け落ち
が生じても、炭酸ガスアーク溶接では定電圧特性
の電源を使用しているために溶接電圧はほとんど
変化しないので、この溶け落ちを溶接電圧の変化
によつて検出することはできない。 In droplet transfer welding, as shown in Fig. 1 or 2, in the large current range, the molten pool 2a generated by generating the arc 3 between the electrode 1 and the workpiece 2 becomes large. , and since the depression 2b also becomes larger, welding (hereinafter referred to as "buried arc") is carried out by burying the electrode tip into the molten pool so that the molten part 1a of the electrode tip transfers within the large depression of the molten pool. It is being said. Even if the welding current is a buried arc with a large current, when the welding speed is low, for example 50 cm/min, the molten pool will have a large depression as shown in Figure 1, and the molten part 1a at the tip of the electrode will become a large lump. They grow and separate due to electromagnetic repulsion, resulting in irregular short circuits as described above. However, even in buried arc welding with a large current, when the welding speed is high, for example, 1 m/min or more, when the arc voltage is lowered, the depression in the molten pool 2a becomes narrower, as shown in Fig. 2. The tip of the electrode melts along the front 2c of the molten pool and becomes sharp.
Along with this, the molten portion 1a at the tip of the electrode flows down, so there is an advantage that there is less spatter. Moreover,
In this high welding speed buried arc welding, the molten metal of the workpiece directly under the arc is swept backwards by the strong arc force, exposing the solid exposed surface, making it possible to obtain deep penetration. Another drawback is that there is no molten metal in the welding process, and the arc directly hits the unmolten parts of the welded object, making it easy for the welded object to melt through. Even if such burn-through occurs, carbon dioxide arc welding uses a power source with constant voltage characteristics, so the welding voltage hardly changes, so this burn-through cannot be detected by changes in the welding voltage. .
それに対して、短絡移行溶接においては、たと
え溶け落ちが生じたとしても、被溶接物の溶融池
の表面状態が変化するために、溶け落ち前の規則
正しいアークの発生と短絡との反復状態に変化を
生じ、短絡回数に明確な変化が生じる。さらに
は、短絡移行溶接においては、薄板が使用される
ために、溶け落ちを生じることによつてアークが
発生していた溶融金属が流出すると、アークの発
生位置が変動し、ときにはアーク長が長くなり、
そのために溶接電流が減少し短絡回数も減少す
る。このように短絡移行溶接では、埋れアーク溶
接にくらべて溶け落ちが生じにくく、たとえ生じ
たとしても、アークが不安定になることから溶接
電流、短絡回数等に顕著な変化等が現われるため
に溶け落ちの検出を容易かつ迅速に行うことがで
きるので、自動的に溶接の中止を行うことが容易
であつた。 On the other hand, in short-circuit transition welding, even if burn-through occurs, the surface condition of the molten pool of the workpiece changes, resulting in a repeating state of regular arc generation and short circuit before burn-through. This causes a clear change in the number of short circuits. Furthermore, because thin plates are used in short-circuit transition welding, when the molten metal that generated the arc flows out due to burn-through, the position of the arc changes, and sometimes the arc length becomes longer. Become,
Therefore, the welding current is reduced and the number of short circuits is also reduced. In this way, in short-circuit transition welding, burn-through is less likely to occur than in buried arc welding, and even if burn-through occurs, the arc becomes unstable, resulting in noticeable changes in the welding current, number of short circuits, etc. Since the drop could be detected easily and quickly, it was easy to automatically stop welding.
しかし、高速度埋もれアーク溶接では第2図に
示すように電極先端と溶融池前方2cすなわち被
溶接物の未溶融部分との間にアーク3が発生して
いるので、アークが発生している後方の溶融池2
a内で溶融金属が被溶接物よりも溶け落ちて流出
してもアークの安定性にはほとんど影響しない。
したがつて、溶け落ちが生じても溶接電圧および
溶接電流にはほとんど影響が現われない。そのた
めに埋れアーク溶接において溶け落ちが生じて
も、アーク電圧、溶接電流の変化を検出しただけ
では確実な判断をすることができず、目視によつ
て発見しているために、その発見が遅れて溶け落
ちが大になり、その補修に過大な労力を要してい
た。 However, in high-speed buried arc welding, as shown in Figure 2, an arc 3 is generated between the electrode tip and the front 2c of the molten pool, that is, the unmelted part of the workpiece. molten pool 2
Even if the molten metal melts down and flows out from the object to be welded within a, the stability of the arc is hardly affected.
Therefore, even if burn-through occurs, the welding voltage and welding current are hardly affected. Therefore, even if burn-through occurs during buried arc welding, it is not possible to make a reliable judgment just by detecting changes in arc voltage and welding current, and detection is delayed because it is detected by visual inspection. This resulted in a large amount of burn-through, and excessive effort was required to repair it.
そこで、本発明者は、高速度炭酸ガスアーク溶
接において、被溶接物の溶融金属が溶け落ちやす
く、しかも溶融金属が溶け落ちて流出してもアー
クの発生位置が変化せず、アークが略安定に発生
し、溶接電圧も溶接電流も略一定しているような
埋れアーク溶接においても、早期にかつ確実に溶
け落ちを検出して溶接を中止させる高速度炭酸ガ
スアーク溶接方法を提案するものである。 Therefore, the present inventor discovered that in high-speed carbon dioxide arc welding, the molten metal of the object to be welded easily melts down, and even if the molten metal melts down and flows out, the position of the arc does not change, and the arc is almost stable. The present invention proposes a high-speed carbon dioxide arc welding method that can detect burn-through early and reliably and stop welding even in buried arc welding where the welding voltage and welding current are approximately constant.
高速度埋れアーク溶接では、短絡移行溶接より
も大電流であつてかつアーク発生が継続している
ので、短絡移行溶接のように短絡回数の多い短絡
は生じないし、また第1図に示すような低速度埋
もれアーク溶接のような不規則な短絡も生じてい
ない。しかし、高速度埋れアーク溶接において溶
け落ちが生じない正常な状態においても、短絡移
行現象とは全く異なる現象で短絡が生じている。
すなわち電極先端の溶滴と後方に押し流された被
溶接物の溶融金属とが低い周期で比較的規則的に
短絡が発生し、その短絡回数は10乃至50Hzであ
る。これに対して短絡移行溶接の各種溶接条件に
適合した安定なアーク状態が継続しているときの
短絡回数は30Hz乃至120Hzであるが、アーク状態
が不安定になると短絡回数は10Hz乃至30Hzに低下
する。したがつて、埋れアーク溶接においては、
正常なアーク発生状態においても、その短絡回数
は、短絡移行溶接のアーク不安定状態における短
絡回数の範囲を含んでしまう。しかし、ここで埋
れアーク溶接において、溶け落ちを生じたときの
アーク状態を検討すると、前述したようにアーク
は安定に継続しているが、溶融池の後方に押し流
された被溶接物の溶融金属は溶け落ちによつて流
出するために電極先端の溶滴と後方に押し流され
た溶融金属との短絡の機会が減少して短絡回数が
減少し、その短絡回数は0乃至5Hzとなる。この
ように、埋れアーク溶接においては、短絡移行溶
接と全く異なる現象に基ずいて短絡が発生してい
るために、短絡移行溶接においてアークが不安定
状態となる範囲内にある短絡回数であつても、さ
らに分析して溶け落ちが生じていない範囲と溶け
落ちが生じている範囲とを明確に区別することが
できる。すなわち埋れアーク溶接においては、溶
け落ちが生じていないときの短絡回数は10乃至50
Hzであり、溶け落ちが生じたときの短絡回数は0
乃至5Hzである。 In high-speed buried arc welding, the current is larger than in short-circuit transition welding, and the arc continues to be generated, so short circuits do not occur as often as in short-circuit transition welding, and short circuits as shown in Figure 1 do not occur. There are no irregular short circuits that occur with low-speed buried arc welding. However, even under normal conditions in which burn-through does not occur during high-speed buried arc welding, short circuits occur due to a phenomenon completely different from the short circuit transfer phenomenon.
That is, short circuits occur relatively regularly between the droplet at the tip of the electrode and the molten metal of the object to be welded that has been swept backward, and the number of short circuits is 10 to 50 Hz. On the other hand, when a stable arc condition that meets various welding conditions in short-circuit transition welding continues, the number of short circuits is 30Hz to 120Hz, but when the arc condition becomes unstable, the number of short circuits decreases to 10Hz to 30Hz. do. Therefore, in buried arc welding,
Even in a normal arc generation state, the number of short circuits includes the range of the number of short circuits in an unstable arc state of short-circuit transition welding. However, if we consider the arc condition when burn-through occurs in buried arc welding, the arc continues stably as mentioned above, but the molten metal of the workpiece is swept away behind the molten pool. Since the molten metal flows out by melting through, the chance of short circuit between the droplet at the tip of the electrode and the molten metal swept backward is reduced, and the number of short circuits is reduced, and the number of short circuits is 0 to 5 Hz. In this way, in buried arc welding, short circuits occur based on a phenomenon completely different from that in short-circuit transition welding, so even if the number of short circuits is within the range where the arc becomes unstable in short-circuit transition welding By further analysis, it is possible to clearly distinguish between a range where burn-through has not occurred and a range where burn-through has occurred. In other words, in buried arc welding, the number of short circuits when no burn through occurs is 10 to 50.
Hz, and the number of short circuits when burn-through occurs is 0.
The frequency ranges from 5Hz to 5Hz.
つぎに、本発明の高速度炭酸ガスアーク溶接方
法の実施例を示す。 Next, an example of the high-speed carbon dioxide gas arc welding method of the present invention will be shown.
シールドガス CO2 25/min
電 極 軟鋼 直径1.6mm
被 溶 接材 軟鋼 板厚2.3mm
横 向 姿勢 重ね合せ隅肉溶接
実施例1 実施例2
溶 接 電流 390A 360A
溶 接 電圧 32V 28V
溶 接 速度 2m/sec 1.5m/sec
溶け落ちを生じる前の短絡回数 20Hz 15Hz
溶け落ちを生じた後の短絡回数 2Hz 0Hz
以上のように本発明の高速度炭酸ガスアーク溶
接方法によると、埋れアーク溶接の短絡現象と短
絡移行溶接の短絡現象との相違から、短絡移行溶
接ではアーク不安定とされる短絡回数10乃至30Hz
の範囲が、埋れアーク溶接においては被溶接物の
溶け落ちを生じることのない正常な範囲になり、
かつ短絡回数が0乃至5Hzになると、被溶接物が
溶け落ちを生じる範囲であるとして、被溶接物に
溶け落ちが発生したとき確実にかつ迅速に溶接を
中止することができるので、溶け落ち部分の補修
に過大な労力を要することがないので効果は大で
ある。Shielding gas CO 2 25/min Electrode Mild steel Diameter 1.6mm Material to be welded Mild steel Plate thickness 2.3mm Lateral position Lap fillet welding Example 1 Example 2 Welding current 390A 360A Welding voltage 32V 28V Welding speed 2m /sec 1.5m/sec Number of short circuits before burn-through occurs 20Hz 15Hz Number of short circuits after burn-through occurs 2Hz 0Hz As described above, according to the high-speed carbon dioxide arc welding method of the present invention, the short circuit phenomenon of buried arc welding and Due to the difference from the short circuit phenomenon in short-circuit transition welding, the arc is unstable in short-circuit transition welding when the number of short circuits is 10 to 30 Hz.
This range is the normal range in which burn-through of the welded object does not occur in buried arc welding, and
In addition, when the number of short circuits becomes 0 to 5 Hz, it is assumed that the welded object is in the range where burn-through occurs, and when burn-through occurs in the welded object, welding can be reliably and quickly stopped. The effect is great because it does not require excessive effort to repair.
第1図は低速度炭酸ガスアーク溶接の粒滴移行
形態を説明する図、第2図は高速度炭酸ガスアー
ク溶接の埋れアークにおける粒滴移行形態を説明
する図である。
FIG. 1 is a diagram illustrating the droplet transfer form in low-speed carbon dioxide arc welding, and FIG. 2 is a diagram explaining the droplet transfer form in a buried arc in high-speed carbon dioxide arc welding.
Claims (1)
が1m/minをこえる高速度であつて、かつ埋れ
アーク状態で溶接しているときに短絡回数が5サ
イクル以下になつたことを検出して溶接を中止す
る炭酸ガスアーク溶接方法。1. In the carbon dioxide arc welding method, when the welding speed is high, exceeding 1 m/min, and welding is performed in a buried arc state, it is detected that the number of short circuits has become 5 cycles or less, and welding is stopped. Carbon dioxide arc welding method.
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP12508779A JPS5647279A (en) | 1979-09-27 | 1979-09-27 | Co2 gas shielded arc welding |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP12508779A JPS5647279A (en) | 1979-09-27 | 1979-09-27 | Co2 gas shielded arc welding |
Publications (2)
| Publication Number | Publication Date |
|---|---|
| JPS5647279A JPS5647279A (en) | 1981-04-28 |
| JPS63152B2 true JPS63152B2 (en) | 1988-01-05 |
Family
ID=14901506
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP12508779A Granted JPS5647279A (en) | 1979-09-27 | 1979-09-27 | Co2 gas shielded arc welding |
Country Status (1)
| Country | Link |
|---|---|
| JP (1) | JPS5647279A (en) |
Families Citing this family (3)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| JP6812363B2 (en) | 2015-05-18 | 2021-01-13 | スミス アンド ネフュー ピーエルシーSmith & Nephew Public Limited Company | Negative pressure wound therapy equipment and methods |
| AU2016305091B2 (en) | 2015-08-13 | 2021-06-10 | Smith & Nephew, Inc. | Systems and methods for applying reduced pressure therapy |
| US11389582B2 (en) | 2017-09-29 | 2022-07-19 | T.J. Smith And Nephew, Limited | Negative pressure wound therapy apparatus with removable panels |
-
1979
- 1979-09-27 JP JP12508779A patent/JPS5647279A/en active Granted
Also Published As
| Publication number | Publication date |
|---|---|
| JPS5647279A (en) | 1981-04-28 |
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