JPS5915748B2 - Inert gas consumable electrode arc welding method - Google Patents
Inert gas consumable electrode arc welding methodInfo
- Publication number
- JPS5915748B2 JPS5915748B2 JP6225373A JP6225373A JPS5915748B2 JP S5915748 B2 JPS5915748 B2 JP S5915748B2 JP 6225373 A JP6225373 A JP 6225373A JP 6225373 A JP6225373 A JP 6225373A JP S5915748 B2 JPS5915748 B2 JP S5915748B2
- Authority
- JP
- Japan
- Prior art keywords
- current
- welding
- consumable electrode
- welding method
- output
- 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 title claims description 69
- 238000000034 method Methods 0.000 title claims description 25
- 239000011261 inert gas Substances 0.000 title claims description 5
- 230000007423 decrease Effects 0.000 claims description 8
- 229910000838 Al alloy Inorganic materials 0.000 claims description 4
- 238000010586 diagram Methods 0.000 description 4
- 229910052751 metal Inorganic materials 0.000 description 2
- 239000002184 metal Substances 0.000 description 2
- 238000007796 conventional method Methods 0.000 description 1
- 238000002844 melting Methods 0.000 description 1
- 230000008018 melting Effects 0.000 description 1
- 150000004767 nitrides Chemical class 0.000 description 1
- 238000005493 welding type Methods 0.000 description 1
Landscapes
- Arc Welding In General (AREA)
Description
【発明の詳細な説明】
本発明は、直径2.4llLm以上の太径の消耗電極を
使用するアルミニウム合金の大電流不活性ガス消耗電極
アーク溶接方法に関するものである。DETAILED DESCRIPTION OF THE INVENTION The present invention relates to a high current inert gas consumable electrode arc welding method for aluminum alloys using a consumable electrode with a large diameter of 2.4 llLm or more.
アルミニウム合金の不活性ガス消耗電極アーク溶接(以
下MIG溶接といラ)において直径が1.211.6、
2.4關などの比較的細径の消耗電極を使用する通常の
MIG溶接の場合には、定電圧特性を有する直流溶接電
源を使用して、消耗電極を定速度で送給するようにして
いる。この場合。アーク長を一定に保持しようとする作
用は、主と5 して定電圧特性を有する溶接電源の自己
制御作用によるものである。これに対して、アルミニウ
ム合金の厚板を高能率に溶接するために直径が2.4、
3.2、4、O、4.8、5.6mwL等の太径線を消
耗電極として用いた溶接電流が400A以上の大電流、
0MIG溶接方法が開発され、実用化されている。第2
図は大電流MIG溶接方法における消耗電極1の先端と
被溶接物2に形成された溶融池3とを示すものである。
同図に示すように、大電流MIG溶接においては、必然
的に高電流を使用す15るために、溶接部のシールド不
良や溶接電流の変動などにより溶融池周辺にあつたアー
クの陰極点群が溶融池中に入つてアークカにより溶融金
属を吹き上げ、この溶融金属が酸化物および窒化物でお
おわれてしわ状に重ねられていくため、アーク20が荒
れて溶接不能の状態になる、いわゆるパツカリング現象
が生ずろ。したがつて大電流MIG溶接方法においては
、使用すべき溶接電流をパツカリング現象が発生する電
流以下に制限しなければならない。このようなパツカリ
ング限界電流を上25昇させるため、従来開発され実用
化されている大電流MIG溶接方法においては、溶接電
源の出力端子における出力電流値と出力電圧値との関係
を示す外部特性を出力電流値が50A増加すると出力電
圧値が10ないし30V低下する定電圧特性30に近い
垂下特性とした直流溶接電源を用いる方法が実用化され
ている。本明細書において「見掛けのアーク長」という
用語が用いられるが、これは第2図にLoで示すように
消耗電極の先端と被溶接物表面との間の最35短距離を
意味する。In inert gas consumable electrode arc welding (hereinafter referred to as MIG welding) of aluminum alloy, the diameter is 1.211.6,
In the case of normal MIG welding that uses a relatively small diameter consumable electrode such as a 2.4-meter, a DC welding power source with constant voltage characteristics is used to feed the consumable electrode at a constant speed. There is. in this case. The action of keeping the arc length constant is mainly due to the self-control action of the welding power source, which has constant voltage characteristics. On the other hand, in order to weld aluminum alloy thick plates with high efficiency, the diameter is 2.4,
3. A large welding current of 400 A or more using a large diameter wire such as 2, 4, O, 4.8, 5.6 mwL as a consumable electrode,
A 0MIG welding method has been developed and put into practical use. Second
The figure shows the tip of a consumable electrode 1 and a molten pool 3 formed on a workpiece 2 in a high-current MIG welding method.
As shown in the figure, in high-current MIG welding, a high current is inevitably used15. enters the molten pool and the arc force blows up the molten metal, and this molten metal is covered with oxides and nitrides and is layered in a wrinkled manner, causing the arc 20 to become rough and welding impossible, a so-called puckering phenomenon. It's coming. Therefore, in the high-current MIG welding method, the welding current to be used must be limited to a current that causes the puckering phenomenon or less. In order to increase this kind of puckering limit current by 25%, in the high current MIG welding method that has been developed and put into practical use, external characteristics that indicate the relationship between the output current value and the output voltage value at the output terminal of the welding power source are A method using a DC welding power source with drooping characteristics close to constant voltage characteristics 30, in which the output voltage value decreases by 10 to 30 V when the output current value increases by 50 A, has been put into practical use. The term "apparent arc length" is used herein to mean the shortest distance between the tip of the consumable electrode and the surface of the workpiece, as shown by Lo in FIG.
伺同図において実際のアーク長は破線で示したように電
極先端Pと実際のアーク発生点Q(陰極点)との間の距
離Laである。普通のMIG溶接方法においては,溶接
電流を一定に保持しておくと、見掛けのアーク長とアー
ク電圧とは第1図の曲線1に示すように略比例関係にあ
るので、適正なアーク長はアーク電圧を調整することに
よつて設定することができる。また第1図の曲線1上の
a及びb点におけるアークの発生状態はそれぞれ第3図
a及びbに示す通vである。これに対し、大電流MIG
溶接方法に於いては.第1図の曲線に示すように見掛け
のアーク長が変化してもアーク電圧が略30と一定にな
つている。この曲線の上の点c及びdにおけるアーク発
生状態は第3図c及びdに示す通9である。この場合見
掛けのアーク長の適正値は、経験上−27!17!L乃
至+2m7!Lであるとされているが.第3図cからd
に示すように見掛けのアーク長が大きくなつた場合でも
アーク電圧は略一定に保持されるため.見掛けのアーク
長の適正値に対応するアーク電圧を定めることはできな
い。したがつて大電流MIGアーク溶接方法においては
アーク電圧によつてアーク長を調整することができず、
電極送給速度を調整して見掛けのアーク長を調整するこ
とによりアーク長を調整しなければならない。ところで
、大電流MIG溶接方法17C訃いてはアーク長を短く
すると、単位電流当クの溶融速度が急に増加するアーク
自身の自己制御作用があるので、垂下特性または定電流
に近い特性の溶接電源を使用してもアークの安定点が存
在する。したがつて、溶接電源の出力端子における出力
電流値と出力電圧値との関係を示す外部特性を出力電流
値が50A増加すると出力電圧値が10ないし30V低
下する定電圧特性に近い垂下特性とした直流溶接電源を
利用して、さらにパツカリング限界電流を上昇させよう
とする試みがなされたが、適正な溶接条件の設定が困難
となるため実用化されるには至らなかつた。その理由は
、定電圧特性の溶接電源を使用する通常のMIG溶接方
法においては,溶接電圧は溶接電源の電圧調整器により
調整でき、また溶接電流は溶接電圧とは別個に消耗電極
の送給速度により調整できるため溶接電圧と溶接電流の
設定が容易である。これに対して従来の外部特性で出力
電流値が50A増加すると出力電圧値が10ないし30
V低下する垂下特性を使用するMIG溶接方法において
見掛けのアーク長および溶接電流を設定する場合には、
消耗電極の送給速度調整器と溶接電源の出力電流調整器
とを相互に関係させながら設定しなければならないので
、各々を独立して調整できない欠点があつた。本発明の
目的は、適正な溶接条件を容易に設定でき、しかもパツ
カリング限界電流を従来実用化されていたこの種の溶接
方法における限界値より上昇させることができるように
した大電流MIG溶接方法を提案することにある。本発
明の溶接方法は.溶接電流が400A以上の大電流MI
G溶接方法において、溶接電源の出力端子における出力
電流値と出力電圧値の関係を示す外部特性が、出力電流
値が50A増加すると出力電圧値が50V以上低下する
略定電流特性の直流溶接電源を使用することを特徴とし
たものである。In the figure, the actual arc length is the distance La between the electrode tip P and the actual arc generation point Q (cathode point), as shown by the broken line. In the normal MIG welding method, if the welding current is held constant, the apparent arc length and arc voltage are approximately proportional as shown in curve 1 in Figure 1, so the appropriate arc length is It can be set by adjusting the arc voltage. Further, the arc generation states at points a and b on curve 1 in FIG. 1 are as shown in FIGS. 3 a and b, respectively. On the other hand, large current MIG
Regarding the welding method. As shown by the curve in FIG. 1, the arc voltage remains constant at approximately 30° even if the apparent arc length changes. The arcing conditions at points c and d on this curve are as shown in Figure 3 c and d. In this case, the appropriate value for the apparent arc length is -27!17! from experience. L~+2m7! It is said that L. Figure 3 c to d
As shown in Figure 2, the arc voltage remains approximately constant even when the apparent arc length increases. It is not possible to determine the arc voltage that corresponds to the appropriate value of the apparent arc length. Therefore, in the high current MIG arc welding method, the arc length cannot be adjusted by the arc voltage.
The arc length must be adjusted by adjusting the electrode feed rate to adjust the apparent arc length. By the way, in high current MIG welding method 17C, when the arc length is shortened, the arc itself has a self-control action that rapidly increases the melting rate per unit current, so welding power sources with drooping characteristics or characteristics close to constant current There is a stable point of the arc even if . Therefore, the external characteristic showing the relationship between the output current value and the output voltage value at the output terminal of the welding power source was made into a drooping characteristic that is close to a constant voltage characteristic in which the output voltage value decreases by 10 to 30 V when the output current value increases by 50 A. Attempts have been made to further increase the puckering limit current using a DC welding power source, but this has not been put to practical use because it is difficult to set appropriate welding conditions. The reason for this is that in the normal MIG welding method that uses a welding power source with constant voltage characteristics, the welding voltage can be adjusted by the voltage regulator of the welding power source, and the welding current is determined separately from the welding voltage by the feed rate of the consumable electrode. It is easy to set the welding voltage and welding current because the welding voltage and welding current can be adjusted by On the other hand, when the output current value increases by 50A with conventional external characteristics, the output voltage value increases by 10 to 30A.
When setting the apparent arc length and welding current in the MIG welding method that uses the droop characteristic that V decreases,
Since the feed speed regulator of the consumable electrode and the output current regulator of the welding power source must be set in relation to each other, there is a drawback that each cannot be adjusted independently. An object of the present invention is to provide a high-current MIG welding method that allows for easy setting of appropriate welding conditions and that allows the limit current for puckering to be raised above the limit value of this type of welding method that has been put into practical use in the past. It's about making suggestions. The welding method of the present invention is. Large current MI with welding current of 400A or more
In the G welding method, a DC welding power source is used in which the external characteristic indicating the relationship between the output current value and the output voltage value at the output terminal of the welding power source is a nearly constant current characteristic in which the output voltage value decreases by 50 V or more when the output current value increases by 50 A. It is characterized by its use.
出力電流値の増加に対する出力電圧値の減少を50V/
50A以上にすると、溶接電流の設定は出力電圧とは無
関係に溶接電源の出力電流の調整器によつてのみ定める
ため、見掛けのアーク長は溶接電流とは無関係に消耗電
極の送給速度調整器によつてのみ調整できる。したがつ
て、溶接電流と見掛けのアーク長を独立して調整できる
ので、適正条件の設定が容易である。つぎにパツカリン
グ発生の限界電流についてみると、従来から実用化され
ている出力電流値が50A増加すると出力電圧値が10
ないし30低下する定電圧特性に近い垂下特性の溶接電
源においては、電極直径2.4,3.2,4.0,4.
8mmに対して.パツカリング発生の限界電流はそれぞ
れ550,620,680,700Aであるが.本発明
の溶接方法に係る出力電流値が50A増加すると出力電
圧値が50以上低下する略定電流特性の溶接電源に訃い
ては、電極直径2.4,3.2,4.0,4.81tm
に対して、パツカリング発生の限界電流はそれぞれ58
0,680,750,800Aとなl).従来より限界
電流を上昇させることができた。The decrease in output voltage value with respect to the increase in output current value is 50V/
When setting the welding current to 50A or more, the welding current setting is determined only by the output current regulator of the welding power source, regardless of the output voltage, so the apparent arc length is determined by the consumable electrode feed speed regulator, regardless of the welding current. It can only be adjusted by Therefore, since the welding current and the apparent arc length can be adjusted independently, it is easy to set appropriate conditions. Next, looking at the limiting current that causes puckering, when the output current value that has been put into practical use increases by 50A, the output voltage value increases by 10A.
In welding power sources with drooping characteristics close to constant voltage characteristics where the voltage drops by 30 to 30, electrode diameters of 2.4, 3.2, 4.0, 4.
For 8mm. The limiting currents for occurrence of puckering are 550, 620, 680, and 700 A, respectively. In the welding power source of the welding method of the present invention, which has a substantially constant current characteristic in which the output voltage value decreases by 50 or more when the output current value increases by 50 A, electrode diameters of 2.4, 3.2, 4.0, 4. 81tm
However, the limiting current for puckering occurrence is 58, respectively.
0,680,750,800A). It was possible to increase the limiting current compared to the conventional method.
また本発明の溶接方法に係る略定電流特性の溶接電源に
おいては、電源電圧変動による溶接電流の変化がほとん
どなく、比較的パツカリング発生限界電流の近くで使用
してもパツカリング現象を生じることはない。In addition, in the welding power source with substantially constant current characteristics according to the welding method of the present invention, there is almost no change in welding current due to fluctuations in the power supply voltage, and the puckering phenomenon does not occur even when used relatively close to the puckering generation limit current. .
出力電流400A以上で,このような出力電流値が50
A増加すると出力電圧値が50V以上低下する略定電流
特註を、サイリスタ式溶接電源によつて容易に得ること
ができる。本発明の溶接方法によると、適正な溶接条件
の設定が容易で、しかもパツカリング発生の限界電流が
高いので、高能率の大電流MIG溶接ができ.実益が大
である。When the output current is 400A or more, the output current value is 50A or more.
A substantially constant current characteristic in which the output voltage value decreases by 50 V or more as A increases can be easily obtained using a thyristor type welding power source. According to the welding method of the present invention, it is easy to set appropriate welding conditions, and the limiting current for occurrence of puckering is high, so high-efficiency, large-current MIG welding can be performed. The actual benefits are great.
第1図は溶接電流を一定にした場合の普通のMIG溶接
方法および大電流MIG溶接方法における見掛けのアー
ク長とアーク電圧との関係を示す線図、第2図は大電流
MlG溶接方法における消耗電極の先端と溶融池を示す
説明図.第3図a乃至dはそれぞれ第1図の曲線1及び
の上の点a乃至dにおける消耗電極の先端附近の状態を
示す説明図である。
1・・・消耗電極.2・・・被溶接物,3・・・溶融池
。Figure 1 is a diagram showing the relationship between the apparent arc length and arc voltage in the ordinary MIG welding method and the high current MIG welding method when the welding current is held constant, and Figure 2 is a diagram showing the relationship between the apparent arc length and the arc voltage in the high current MIG welding method. Explanatory diagram showing the tip of the electrode and the molten pool. 3A to 3D are explanatory diagrams showing the state near the tip of the consumable electrode at points a to d on curves 1 and 1 in FIG. 1, respectively. 1...Consumable electrode. 2... object to be welded, 3... molten pool.
Claims (1)
ルミニウム合金の大電流不活性ガス消耗電極アーク溶接
方法において、溶接電源の出力端子における出力電流値
と出力電圧値との関係を示す外部特性を出力電流値が5
0A増加すると出力電圧値が50V以上低下する略定電
流特性とした直流溶接電源を使用して、消耗電極を定速
度送給することを特徴とする不活性ガス消耗電極アーク
溶接方法。1 External characteristics showing the relationship between the output current value and output voltage value at the output terminal of the welding power source in the high current inert gas consumable electrode arc welding method for aluminum alloy using a large diameter consumable electrode with a diameter of 2.4 mm or more The output current value is 5
An inert gas consumable electrode arc welding method characterized in that a consumable electrode is fed at a constant speed using a DC welding power source with a substantially constant current characteristic in which the output voltage value decreases by 50 V or more when the output voltage increases by 0 A.
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP6225373A JPS5915748B2 (en) | 1973-06-02 | 1973-06-02 | Inert gas consumable electrode arc welding method |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP6225373A JPS5915748B2 (en) | 1973-06-02 | 1973-06-02 | Inert gas consumable electrode arc welding method |
Publications (2)
| Publication Number | Publication Date |
|---|---|
| JPS5010244A JPS5010244A (en) | 1975-02-01 |
| JPS5915748B2 true JPS5915748B2 (en) | 1984-04-11 |
Family
ID=13194778
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP6225373A Expired JPS5915748B2 (en) | 1973-06-02 | 1973-06-02 | Inert gas consumable electrode arc welding method |
Country Status (1)
| Country | Link |
|---|---|
| JP (1) | JPS5915748B2 (en) |
Cited By (2)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| WO2020130319A1 (en) * | 2018-12-21 | 2020-06-25 | 한국표준과학연구원 | Laser spatial modulation super resolution optical microscope |
| US11675175B2 (en) | 2018-01-16 | 2023-06-13 | Illumina, Inc. | Multi-arm structured illumination imaging |
-
1973
- 1973-06-02 JP JP6225373A patent/JPS5915748B2/en not_active Expired
Cited By (2)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| US11675175B2 (en) | 2018-01-16 | 2023-06-13 | Illumina, Inc. | Multi-arm structured illumination imaging |
| WO2020130319A1 (en) * | 2018-12-21 | 2020-06-25 | 한국표준과학연구원 | Laser spatial modulation super resolution optical microscope |
Also Published As
| Publication number | Publication date |
|---|---|
| JPS5010244A (en) | 1975-02-01 |
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