JPS639913B2 - - Google Patents
Info
- Publication number
- JPS639913B2 JPS639913B2 JP53071995A JP7199578A JPS639913B2 JP S639913 B2 JPS639913 B2 JP S639913B2 JP 53071995 A JP53071995 A JP 53071995A JP 7199578 A JP7199578 A JP 7199578A JP S639913 B2 JPS639913 B2 JP S639913B2
- Authority
- JP
- Japan
- Prior art keywords
- period
- current
- ratio
- during
- output current
- 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
Landscapes
- Arc Welding In General (AREA)
- Arc Welding Control (AREA)
Description
【発明の詳細な説明】
本発明は、交流アーク溶接方法の改良に関する
ものである。DETAILED DESCRIPTION OF THE INVENTION The present invention relates to improvements in alternating current arc welding methods.
一般にアルミニウムやマグネシウムなどの活性
金属の非消耗性アーク溶接では、交流アーク溶接
機が用いられている。 Generally, AC arc welding machines are used for non-consumable arc welding of active metals such as aluminum and magnesium.
この場合、可動鉄心形の交流アーク溶接機を用
いると、電極と被溶接物との電子放出能の差によ
つて、電極が被溶接物に対してマイナスとなる正
極性の期間中と電極がプラスとなる逆極性の期間
中とでは、アーク電圧波形および溶接電流波形が
異なる。すなわち、第1図aはアーク電圧波形を
示し、電極がマイナスとなる正極性の期間中Ts
のアーク電圧の平均値または波高値は、逆極性の
期間中Trのそれよりも小となり、さらに第1図
bは溶接電流波形を示し、正極性の期間中Tsの
平均値または波高値は、逆極性の期間中Trのそ
れよりも大となり、いわゆる整流作用を生じる。 In this case, if a movable core type AC arc welding machine is used, due to the difference in electron emission ability between the electrode and the workpiece, during the positive polarity period when the electrode is negative with respect to the workpiece, and when the electrode is The arc voltage waveform and welding current waveform are different during the period of positive reverse polarity. That is, Figure 1a shows the arc voltage waveform, and during the period of positive polarity when the electrode becomes negative, Ts
The average value or peak value of the arc voltage of Tr is smaller than that of Tr during the period of reverse polarity, and FIG. 1b shows the welding current waveform, and the average value or peak value of Ts during the period of positive polarity is During the period of reverse polarity, it becomes larger than that of the Tr, producing a so-called rectifying effect.
今、この正極性の期間中における溶接電流の平
均値をIsm、逆極性のそれをIrmとして、第2図
に示すような正極性の期間中の通電電流および逆
極性の期間中の通電電流の各平均値または各波高
値を制御可能な例えばサイリスタ式交流アーク溶
接機によつて、Ism+Irmを略一定に保持しなが
ら、正極性の期間中の通電電流の比率(以下SP
比という)すなわち
SP比=Ism/(Ism+Irm)
を変化させたときのビード形状を第3図aおよび
同図bに示す。第2図において、1,1は溶接機
の入力端子、2は溶接用変圧器、3は電極、4は
被溶接物、5はアーク、6a,6bはリアクト
ル、7a,7bはサイリスタ、8a,8bは点弧
回路、9a,9bは出力電流の検出および制御回
路である。また第3図aにおいて、Pは溶融金属
4aの溶け込み深さ、Wbはその溶融幅またはビ
ート幅、Wcはクリーニング幅を示す。同図bは、
前述したSP比を変化させたときの、同図aの溶
け込み深さP、ビード幅Wbおよびクリーニング
幅Wcの変化を示している。同図bに示すように、
クリーニング幅WcはSP比の増加とともに減少
し、ビード幅Wbはゆるやかに減少し、さらに溶
け込み深さPは、SP比の50%付近で最小になる。
一方、非消耗性電極は、SP比の増加とともに、
電極が被溶接物に対してプラスとなり発熱する逆
極性電流の減少によつて、電極の消耗は少なくな
る。すなわち、溶け込み深さPを大きくするため
には、SP比を大きくする必要があり、逆にクリ
ーニング幅Wcを大きくするためには、SP比を小
さくする必要があり、さらに電極への許容通電電
流を大きくするためにはSP比を大きくする必要
がある。さらにSP比が大なる期間とSP比が小な
る期間との各継続時間およびそのくり返し周期が
溶融池の形状に影響する。また、上述したSP比
を、正極性の期間中の通電電流の平均値Ismと逆
極性の期間中の通電電流の平均値Irmとによつて
表わしたが、このSP比をそれぞれの期間中の波
高値で表わしても第3図bと略同様の変化とな
る。 Now, assuming that the average value of the welding current during the period of positive polarity is Ism, and that of the reverse polarity as Irm, the applied current during the period of positive polarity and the applied current during the period of reverse polarity are as shown in Figure 2. For example, by using a thyristor-type AC arc welding machine that can control each average value or each peak value, while keeping Ism+Irm approximately constant, the ratio of current flowing during the period of positive polarity (hereinafter referred to as SP
Figures 3a and 3b show the bead shapes when the SP ratio = Ism/(Ism + Irm) is changed. In Fig. 2, 1 and 1 are input terminals of a welding machine, 2 is a welding transformer, 3 is an electrode, 4 is a workpiece to be welded, 5 is an arc, 6a and 6b are reactors, 7a and 7b are thyristors, 8a, 8b is an ignition circuit, and 9a and 9b are output current detection and control circuits. Further, in FIG. 3a, P indicates the penetration depth of the molten metal 4a, Wb indicates the melting width or beat width, and Wc indicates the cleaning width. Figure b is
This figure shows changes in the penetration depth P, bead width Wb, and cleaning width Wc shown in FIG. As shown in Figure b,
The cleaning width Wc decreases as the SP ratio increases, the bead width Wb gradually decreases, and the penetration depth P reaches a minimum near 50% of the SP ratio.
On the other hand, non-consumable electrodes, with increasing SP ratio,
By reducing the reverse polarity current that generates heat when the electrode becomes positive with respect to the object to be welded, wear of the electrode is reduced. In other words, in order to increase the penetration depth P, it is necessary to increase the SP ratio, and conversely, in order to increase the cleaning width Wc, it is necessary to decrease the SP ratio, and in addition, the allowable current flowing to the electrode In order to increase , it is necessary to increase the SP ratio. Furthermore, the duration of the period in which the SP ratio is large and the period in which the SP ratio is small and the repetition period thereof affect the shape of the molten pool. In addition, the above-mentioned SP ratio is expressed by the average value Ism of the current flowing during the period of positive polarity and the average value Irm of the current flowing during the period of reverse polarity. Even when expressed in terms of peak value, the change is approximately the same as that shown in FIG. 3b.
本発明のアーク溶接方法は、以上の検討にもと
ずいて、正極性の期間中の効果と逆極性の期間中
の効果とを有する交流電流を用いて、正極性の期
間中の電流値と逆極性の期間中の電流値との比が
第1の比率である電流を通電し、つぎに正極性の
期間中の電流値と逆極性の期間中の電流値との比
が第2の比率である電流を通電し、以後第1の比
率の電流と第2の比率の電流とを繰返し通電して
溶接する交流アーク溶接方法を提案したものであ
る。 Based on the above studies, the arc welding method of the present invention uses an alternating current that has an effect during the period of positive polarity and an effect during the period of reverse polarity, and the current value during the period of positive polarity is changed. A current is passed in which the ratio of the current value during the period of reverse polarity is a first ratio, and then the ratio of the current value during the period of positive polarity to the current value during the period of reverse polarity is a second ratio. The present invention proposes an AC arc welding method in which a current of a first ratio and a second ratio of current are applied repeatedly to perform welding.
以下、本発明のアーク溶接方法を第4図aない
しcを参照して説明する。 Hereinafter, the arc welding method of the present invention will be explained with reference to FIGS. 4a to 4c.
同図aは、第2図に示すサイリスタ式交流アー
ク溶接機から供給する正極性の期間中の出力電流
の波高値と逆極性の期間中の出力電流の波高値と
の和Is1+Ir1またはIs2+Ir2すなわち正の波高値か
ら負の波高値までの値(ピークピーク値)を一定
に保持するか、または正極性の期間中の出力電流
の平均値と逆極性の期間中の出力電流の平均値と
の和を一定に保持しておいて、正極性の期間中の
出力電流値が逆極性の期間中の出力電流値よりも
大になる第1の状態と、正極性の期間中の出力電
流値と逆極性の期間中の出力電流値とが略等しく
なる第2の状態とが、交流出力電流の1サイクル
tよりも長い周期Tでくり返して変化させた場合
の変化電流の波形を示している。上記の第1の状
態の継続時間も第2の継続時間もともに略等しい
周期Tの場合を示している。このような変化電流
を不活性ガスを主成分とするシールドガスで被包
された非消耗性電極およびアルミニウム、マグネ
シウム等の酸化皮膜を有する軽合金の被溶接物に
通電すると、SP比の大きい第1の状態において
は溶け込み深さPが大となり、さらにSP比の小
さい第2の状態においてはクリーニング幅が広く
なるのでビード止端部のぬれが良好となり止端部
のわれを生じることがなく、かつ、非消耗電極の
プラスの期間中の発熱の減少により、非消耗電極
の許容通電容量の増大または非消耗電極の消耗の
軽減をはかることができる。また交流出力電流の
周波数としては通常、商用周波が用いられるが、
溶融池の振動による粒子の微細化等を目的として
高周波のパルス状電流を使用してもよい。 Figure a shows the sum of the peak value of the output current during the period of positive polarity and the peak value of the output current during the period of reverse polarity supplied from the thyristor-type AC arc welding machine shown in Figure 2, Is 1 + Ir 1 or Is 2 + Ir 2 , that is, the value from the positive peak value to the negative peak value (peak-to-peak value) is held constant, or the average value of the output current during the period of positive polarity and the output current during the period of opposite polarity. A first state in which the output current value during the period of positive polarity is larger than the output current value during the period of reverse polarity while holding the sum with the average value of The waveform of the changing current when the second state in which the output current value and the output current value during the period of opposite polarity are approximately equal is repeatedly changed at a period T longer than one cycle t of the AC output current. It shows. A case is shown in which both the duration time of the first state and the second duration time described above have substantially the same period T. When such a changing current is applied to a non-consumable electrode covered with a shielding gas mainly composed of an inert gas and a workpiece made of a light alloy such as aluminum or magnesium with an oxide film, the In state 1, the penetration depth P is large, and in state 2, where the SP ratio is small, the cleaning width is wide, so the wetting of the bead toe is good and there is no cracking of the toe. In addition, by reducing heat generation during the positive period of the non-consumable electrode, it is possible to increase the allowable current carrying capacity of the non-consumable electrode or reduce wear and tear of the non-consumable electrode. Also, the commercial frequency is usually used as the frequency of the AC output current, but
A high-frequency pulsed current may be used for the purpose of making particles finer by vibrating the molten pool.
同図bは、SP比が大となる第1の状態の周期
T1を、第2の状態の周期T2よりも大にした場合
の交流出力電流の波形を示す。同図に示す変化電
流の周期は、不活性ガスを主成分とするガスシー
ルドされた非消耗電極を使用してアルミニウムを
溶接する場合はもちろん、被覆消耗電極またはガ
スシールドされた消耗電極を使用してアルミニウ
ム、その他の材質の被溶接物を溶接する場合にお
いて、特に厚板等の溶け込み深さPを大にする必
要がある場合に適している。逆に、不活性ガスを
主成分とするガスシールドされた非消耗性電極で
アルミニウムを溶接する場合において、被溶接物
が薄板であつて突合せ開先面の精度が高くなく、
フイラワイヤを使用するようなときには、SP比
の大なる第1の状態の周期をSP比の小なる第2
の状態の周期よりも短くして、溶け込み深さPを
あまり大にしないでクリーニング幅Wcを大にす
る必要がある。また、この場合、フイラワイヤを
SP比の変化例えばSP比の大なる第1の状態に同
期させて、溶融池に挿入すればフイラワイヤの溶
滴と溶融池とのぬれが良好になる。さらに、被覆
溶接棒の供給および退避、またはガスシールドさ
れた消耗電極の送給、停止、退避もしくは速度の
制御を、SP比の変化に略同期させて行うことに
よつて、例えば溶融池が拡大される期間に被覆溶
接棒もしくは消耗電極の溶滴を溶融池に投入させ
てぬれを良好とし、ビード形状を制御することが
できる。 Figure b shows the period of the first state where the SP ratio is large.
The waveform of the AC output current is shown when T 1 is made larger than the period T 2 of the second state. The period of the changing current shown in the figure applies not only when welding aluminum using a gas-shielded non-consumable electrode containing an inert gas as its main component, but also when using a covered consumable electrode or a gas-shielded consumable electrode. When welding workpieces made of aluminum or other materials, this method is particularly suitable when it is necessary to increase the penetration depth P of thick plates and the like. Conversely, when welding aluminum with a gas-shielded non-consumable electrode containing inert gas as its main component, the workpiece is a thin plate and the precision of the butt groove surface is not high;
When using filler wire, the period of the first state with a large SP ratio is changed to the second state with a small SP ratio.
It is necessary to make the cleaning width Wc larger without making the penetration depth P too large by making it shorter than the cycle of the state. Also, in this case, filler wire
If the filler wire is inserted into the molten pool in synchronization with a change in the SP ratio, for example, the first state where the SP ratio is large, wetting of the droplets of the filler wire and the molten pool will be good. Furthermore, by controlling the supply and withdrawal of a coated welding rod, or the supply, stop, withdrawal, or speed of a gas-shielded consumable electrode in approximately synchronization with changes in the SP ratio, for example, the molten pool can be expanded. During this period, droplets from a covered welding rod or consumable electrode are introduced into the molten pool to improve wetting and control the bead shape.
同図cは、交流出力電流の正極性の期間中にお
ける出力電流値が大小すなわちIs1とIs2とに変化
する第1の状態と第2の状態とに変化するが、こ
の第1の状態における逆極性の期間中の出力電流
値Ir1と第2の状態における逆極性の期間中の出
力電流値Ir2とが略同一である場合の出力電流の
波形を示し、このような変化電流を通電すること
によつて、クリーニング幅Wcを一定にすること
ができるので、大電流を使用する溶接においてク
リーニング幅Wcを確保するとともに、非消耗電
極の過熱を防ぎ、電極の消耗を軽減することがで
きる。 Figure c shows that the output current value during the period of positive polarity of the AC output current changes between a first state and a second state in which the value changes from small to large, that is, Is 1 and Is 2 , but this first state The waveform of the output current is shown when the output current value Ir 1 during the period of reverse polarity in the second state is approximately the same as the output current value Ir 2 during the period of reverse polarity in the second state, and such a changing current is By energizing, the cleaning width Wc can be kept constant, so it is possible to secure the cleaning width Wc in welding using a large current, prevent overheating of the non-consumable electrode, and reduce electrode wear. can.
さらに第5図は、前述した第4図cに示すよう
な逆極性の期間中における出力電流値Ir1および
Ir2を略一定に保つてクリーニング幅Wcを略一定
にしながら、SP比をくり返して変化させて、溶
融池の加熱による拡大および冷却による縮小をく
り返して形成されたビード外観を示す図である。
このようにSP比をくり返して変化させることに
より、溶融池の溶け込み深さや溶融池幅を制御し
て溶接すると、特に難姿勢溶接におけるたれ落ち
防止、片面溶接における良好な裏波の形成等に効
果を有する。 Furthermore, FIG. 5 shows the output current values Ir 1 and 1 during the period of reverse polarity as shown in FIG.
FIG. 7 is a diagram showing the appearance of a bead formed by repeatedly changing the SP ratio while keeping Ir 2 substantially constant and cleaning width Wc substantially constant, thereby repeatedly expanding the molten pool by heating and contracting it by cooling.
By repeatedly changing the SP ratio in this way, welding while controlling the penetration depth and width of the molten pool is particularly effective in preventing dripping in difficult position welding, and in forming good back waves in single-sided welding. has.
以上のように本発明の交流アーク溶接方法によ
れば、正極性の期間中の出力電流値、および逆極
性の期間の出力電流値の少なくとも一方を、交流
出力電流の1サイクルよりも長い周期でくり返し
て変化させ、しかもそれらの各くり返し周期を
個々に選定して、溶融池の溶け込み深さ、ビード
幅等の溶融池の形状を時々刻々と制御し、特に難
姿勢溶接、裏波溶接、開先精度の良好でない突合
せ溶接等において、良好な溶接結果を得ることが
できる利点がある。また、ガスシールド非消耗電
極を使用した場合には、非消耗電極の通電容量の
増大、電極の消耗の軽減の効果があり、フイラワ
イヤを使用する場合は、フイラワイヤの溶滴と被
溶接物の溶融池とのぬれをも良好とし、さらに、
被溶接物がアルミニウム等の酸化性皮膜を有する
ものである場合には、クリーニング幅を制御する
ことができ、特に大電流においてクリーニング幅
を広くしてビード止端部のぬれを良好としてビー
ド止端部のわれを皆無にすることができるなど多
くの利点を有する。 As described above, according to the AC arc welding method of the present invention, at least one of the output current value during the positive polarity period and the output current value during the reverse polarity period is set at a cycle longer than one cycle of the AC output current. The shape of the molten pool, such as the penetration depth and bead width, can be controlled moment by moment by repeatedly changing the molten pool, and by individually selecting each repetition period. There is an advantage that good welding results can be obtained in butt welding where the tip accuracy is not good. In addition, when a gas-shielded non-consumable electrode is used, it has the effect of increasing the current carrying capacity of the non-consumable electrode and reducing electrode wear. It also has good wettability with the pond, and
When the object to be welded has an oxidizing film such as aluminum, the cleaning width can be controlled, and the cleaning width can be widened to improve wetting of the bead toe, especially at high currents. It has many advantages, such as being able to completely eliminate departmental divisions.
第1図aおよびbは、通常の可動鉄心形交流ア
ーク溶接機の出力電流を不活性ガスシールド消耗
電極およびアルミニウム被溶接物に通電してアー
ク溶接をした場合のアーク電圧の波形および溶接
電流の波形を示す図、第2図は本発明の溶接方法
の実施に用いるサイリスタ式交流アーク溶接機、
第3図aは、溶融池の溶け込み深さP、ビード幅
Wbおよびクリーニング幅Wcを定義する図、同
図bはSP比(正極性の期間中の出力電流値に対
する正極性期間中の出力電流値と逆極性の期間中
の出力電流値との和)を変化させた場合の溶け込
み深さP、ビード幅Wbおよびクリーニング幅
Wcの変化を示す図、第4図aないしcは、本発
明の溶接方法に用いる交流アーク溶接機の出力電
流波形を示す図、第5図は、本発明の溶接方法の
一実施例を示す溶接ビードの外観図である。
Figures 1a and 1b show the arc voltage waveform and welding current when arc welding is performed by applying the output current of a normal movable core type AC arc welding machine to an inert gas shielded consumable electrode and an aluminum workpiece. A diagram showing waveforms, FIG. 2 is a thyristor-type AC arc welding machine used for carrying out the welding method of the present invention,
Figure 3a shows the penetration depth P of the molten pool and the bead width.
Figure b defines the Wb and cleaning width Wc. Figure b shows the SP ratio (the sum of the output current value during the positive polarity period and the output current value during the reverse polarity period relative to the output current value during the positive polarity period). Penetration depth P, bead width Wb and cleaning width when changed
Figures 4a to 4c show the output current waveforms of the AC arc welding machine used in the welding method of the present invention, and Figure 5 shows an embodiment of the welding method of the present invention. FIG. 3 is an external view of a weld bead.
Claims (1)
流を通電して溶接する交流アーク溶接方法におい
て、正極性の期間中の電流値と逆極性の期間中の
電流値との比が第1の比率である電流を通電し、
つぎに正極性の期間中の電流値と逆極性の期間中
の電流値との比が第2の比率である電流を通電
し、以後前記第1の比率の電流と第2の比率の電
流とを繰返し通電して溶接する交流アーク溶接方
法。1. In an AC arc welding method in which an AC output current is applied to an electrode and a workpiece from a welding power source to weld, the ratio of the current value during the period of positive polarity to the current value during the period of reverse polarity is the first Apply a current that is the ratio,
Next, a current is passed in which the ratio of the current value during the period of positive polarity to the current value during the period of reverse polarity is a second ratio, and thereafter the current of the first ratio and the current of the second ratio are An alternating current arc welding method that involves repeatedly applying current to welding.
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP7199578A JPS54162650A (en) | 1978-06-13 | 1978-06-13 | Ac arc welding |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP7199578A JPS54162650A (en) | 1978-06-13 | 1978-06-13 | Ac arc welding |
Publications (2)
| Publication Number | Publication Date |
|---|---|
| JPS54162650A JPS54162650A (en) | 1979-12-24 |
| JPS639913B2 true JPS639913B2 (en) | 1988-03-02 |
Family
ID=13476560
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP7199578A Granted JPS54162650A (en) | 1978-06-13 | 1978-06-13 | Ac arc welding |
Country Status (1)
| Country | Link |
|---|---|
| JP (1) | JPS54162650A (en) |
Families Citing this family (4)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| JPH01133678A (en) * | 1987-11-18 | 1989-05-25 | Kobe Steel Ltd | Method for controlling output of power source for consumable electrode ac arc welding |
| JP4498263B2 (en) * | 2005-11-08 | 2010-07-07 | 株式会社神戸製鋼所 | Pulse arc welding method |
| US9676051B2 (en) * | 2012-10-18 | 2017-06-13 | Lincoln Global, Inc. | System and methods providing modulation schemes for achieving a weld bead appearance |
| JP7821045B2 (en) * | 2022-06-09 | 2026-02-26 | 株式会社ダイヘン | AC pulse arc welding control method |
Family Cites Families (1)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| JPS5362755A (en) * | 1976-11-17 | 1978-06-05 | Hitachi Ltd | Pulse arc welding method |
-
1978
- 1978-06-13 JP JP7199578A patent/JPS54162650A/en active Granted
Also Published As
| Publication number | Publication date |
|---|---|
| JPS54162650A (en) | 1979-12-24 |
Similar Documents
| Publication | Publication Date | Title |
|---|---|---|
| US10040142B2 (en) | Variable polarity pulse with constant droplet size | |
| US3068352A (en) | Method for obtaining an improved weld in inert arc welding | |
| JP7407398B2 (en) | Arc welding control method | |
| Street | Pulsed arc welding: an introduction | |
| JP5461399B2 (en) | Short-time stud joining method in which an arc is generated by advancing the first workpiece in a plurality of stages in the direction of the second workpiece. | |
| US6156998A (en) | Control of welding arc length | |
| JPS639913B2 (en) | ||
| JP2001246470A (en) | High-speed carbon dioxide welding method | |
| JP2016159316A (en) | Arc welding method, arc welding device and control device for arc welding | |
| JP2005313179A (en) | Welding method interchanging dc arc welding and pulse arc welding and controlling heat input | |
| JP2011110600A (en) | Plasma mig welding method | |
| JPS6219947B2 (en) | ||
| JP3162137B2 (en) | Consumable electrode type gas shielded arc welding method and apparatus | |
| JP4676094B2 (en) | Method for controlling output voltage of welding power source | |
| JP2000254779A (en) | AC pulse arc welding method and welding equipment | |
| JPS62114772A (en) | Mig welding method | |
| JPS62279087A (en) | Welding method | |
| JPS62179872A (en) | Arc welding method for light metal | |
| JP2001121267A (en) | Method for arc welding of titanium and titanium alloy | |
| JP2703804B2 (en) | Control method and apparatus for AC tag welding | |
| JP2023180286A (en) | AC pulsed arc welding control method | |
| JP2024179185A (en) | Dissimilar material welding method | |
| JP2017213578A (en) | Non-consumable electrode type arc welding control method | |
| JP2023158362A (en) | Plasma arc hybrid welding device | |
| JP2003340574A (en) | Control method for output voltage of welding power source device |