JPH0333436B2 - - Google Patents
Info
- Publication number
- JPH0333436B2 JPH0333436B2 JP59095132A JP9513284A JPH0333436B2 JP H0333436 B2 JPH0333436 B2 JP H0333436B2 JP 59095132 A JP59095132 A JP 59095132A JP 9513284 A JP9513284 A JP 9513284A JP H0333436 B2 JPH0333436 B2 JP H0333436B2
- Authority
- JP
- Japan
- Prior art keywords
- electrode
- welding
- wire
- current
- arc
- 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 - Lifetime
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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
- B23K9/00—Arc welding or cutting
- B23K9/08—Arrangements or circuits for magnetic control of the arc
-
- 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
- B23K9/00—Arc welding or cutting
- B23K9/18—Submerged-arc welding
- B23K9/186—Submerged-arc welding making use of a consumable electrodes
- B23K9/188—Submerged-arc welding making use of a consumable electrodes making use of several electrodes
Landscapes
- Engineering & Computer Science (AREA)
- Physics & Mathematics (AREA)
- Plasma & Fusion (AREA)
- Mechanical Engineering (AREA)
- Arc Welding In General (AREA)
- Arc Welding Control (AREA)
Description
本発明は多電極ワイヤを用いてサブマージアー
ク溶接を高速で行なう方法に関し、特にアークを
電磁気的に振動させて溶融池にかかるアーク力の
分散軽減を図ることによりサブマージアーク溶接
を一層高速で行なえる様にしたものである。
薄板のサブマージアーク溶接を高速で行なう場
合には多電極溶接法によることが有効とされ、こ
れまでに例えば2電極法であれば最高約150cm/
min、3電極法であれば最高約250cm/minまで
高速化が可能とされている。しかしより一層の高
速化を図つて溶接作業性を高めようとする産業界
の要請は非常に強く、従来の高速サブマージアー
ク溶接法ではその技術内容からして上記要請に十
分対応することができない状況にある。即ち多電
極方式においては溶接が高速化するにつれて電極
後方へ向かうアーク力が増加して溶融池の要鋼が
必要以上に後方へ流され、アンダーカツトやハン
ピング等の溶接欠陥を生じ易くなる。そこでこの
ような不都合の発生を未然に防止するためには溶
融池に作用するアーク力を分散軽減することが有
効な手段と考えられ、このような観点から従来で
は溶接ワイヤを機械的に振動する方法が実施され
ている。しかしこの方法ではワイヤを約10〜30Hz
という周波数で振動させるので、ワイヤ先端の溶
滴が強制的にふり落とされ、それがビードエツジ
のばりとして残つたり、あるいはワイヤがフラツ
クをかき分けるために溶鋼に有害な窒素が入り込
むという問題があり、そのために高速化の要請に
十分対応できない状況にあるという点については
上述したところである。
本発明者等はかかる状況に鑑み、ワイヤを機械
的に振動させなくとも溶融池にかかるアーク力を
分散軽減できるような手段を開発すべく研究を行
なつてきたが、所定強さの磁気力を利用してアー
クを電磁気的に振動させる事によつてより一層の
高速化を実現できる方法を完成しここに提供しよ
うとするものである。
しかしてこの様な本発明の多電極式高速サブマ
ージアーク溶接方法とは、少なくとも第2位以後
の電極ワイヤ下方に交番磁界を付与して、隣接先
行する電極のアークを溶接線と直交する水平方向
に振動させながら溶接すると共に、該電極ワイヤ
下方で測定される磁束密度値(単位:ガウス)
が、隣接先行する電極ワイヤの溶接電流値(単
位:アンペア)の少なくとも1/4以上の値となる
ように前記磁界の強度を維持しつつサブマージア
ーク溶接を行なう点に要旨を有するものである。
以下図面を参照しつつ本発明の構成及び作用効
果を具体的に説明する。第1図及び第2図は本発
明方法の原理説明図であり、理解の便のため2電
極法により高速サブマージアーク溶接を行なう場
合を示している。P1、P2は夫々先行電極及び後
行電極であり、1a,1bは夫々電極ワイヤで、
その先端部から発生するアーク6a,6bは溶接
方向(矢印A方向)と反対の方向に放射されてい
る。その為に溶融池の溶鋼5は後方凝固面上に吹
き上げられ、前方に溶鋼不足を来たし、アンダー
カツトが起こり易くなる状況が形成される。そし
てこの状況はワイヤ先端間隔dが小さいときほど
両電極のアーク力が協調し易くなつて顕著な傾向
を示す。
ところが本発明では第2図に示す様に後行電極
ワイヤ1bの下方において先行電極P1のアーク
6aを垂直方向に横切るような磁力線が作用する
磁界8を与えるので、アーク6aはフレミングの
左手の法則に従つて紙面に直角方向(溶接線と直
角方向)に力を受け、溶接線を横切る方行へ偏向
させられる。この場合において磁力線の方向即ち
磁気ベクトルHを常に一定として電流の方向即ち
電流ベクトルIの向きを経時的に変化させれば、
アーク6aは溶接線を横切る方向に振動されるこ
とになる。この場合先行の電極ワイヤ1aは特に
強制的に振動させていないから、ワイヤ先端の溶
滴が強制的にふり落とされたり、フラツクスがワ
イヤによつてかき乱されるという心配はなくな
り、ビードエツジのばり発生や溶鋼へ窒素混入と
いつた外観及び構造上の溶接欠陥の発生は回避で
きる。
以上は先行電極のアークに対して後行電極の磁
界が作用する場合を説明したが、先行電極の下方
に磁界を直接作用させることにより、即ち自極下
で強く作用する磁界によつて自極のアークを直接
制御することも当然考えられる。しかし本発明は
高速溶接即ちアークが水平に近い状態で吹き流れ
ている場合の効果的な適用を意図しているので、
上述の様に後行電極下方に磁界を作用させるだけ
で目的は十分達せられ、しかもその方が先行電極
のアークを制御する上でより効果的である。
しかしながら後行電極P2の下方に磁界8を付
与するに当つては条件的に次の配慮が必要にな
る。即ち電極ワイヤ1b先端において測定される
磁束密度値(単位:ガウス)が隣接先行する電極
ワイヤ1aの溶接電流値(単位:アンペア)の少
なくとも1/4以上(両者を無名数化して比較、例
えば1000アンペアに対して250ガウス以上)とな
るようにしなければ電極ワイヤ1b下のアーク6
aを溶接線を横切る方向へ駆動する力を十分誘起
せしめ得ず、ひいてはアンダーカツト等の不都合
を排除する効果も期待できなくなる。
ただし、上記磁界強さを測定するにあたり「ワ
イヤ先端位置」を特定しなければならないが、そ
れは便宜上ワイヤが通常「ワイヤエクステンシヨ
ン」と呼ばれている長さ(ワイヤ方向に沿つた流
電チツプと鋼板面との距離)だけ突き出たときの
位置(たとえば第1図X1,X2点)とする。
又電極ワイヤ先端間隔lとの関係においても多
少の考慮を要する。即ちワイヤ先端間隔l1,2(第
1極目と第2極目の先端間隔)が短くなるほどア
ーク6a,6bの協調性が増し、溶鋼5がより後
方へ排斥駆動されるようになつて好ましくないの
で、ワイヤ先端間隔l1,2の減少程度に応じて磁界
8が強くなるという状態をつくることが好まし
い。本発明者等の実験ではワイヤ先端間隔値(単
位:mm)と磁束密度値(単位:ガウス)との積が
約3000以上(例えばその間隔が20mmの場合であれ
ば150ガウス以上)になるようにすれば、ワイヤ
先端間隔l1,2が短くなつてもアーク6a,6bの
協調性を増加させないことを確認している。
ところで電極ワイヤ1b下方に磁界8を付与す
るには電極ワイヤ1bの周囲に外部磁界を形成す
ることが有効であるが、その具体的手段としては
下記の諸法を挙げることができる。即ち
(1) 電極ワイヤ1bの周囲に電磁ソレノイドを設
ける方法。この場合、汎用のワイヤガイドノズ
ル(図示していない)周囲に電磁ソレノイドを
設けるようにすれば電極間隔の狭い多電極溶接
においても特別なスペースを必要としないので
装置設計上好ましい。
(2) (1)の構成において電極ワイヤガイドノズルを
鉄又は鉄合金等の強磁性体とし、その周囲に電
磁ソレノイドを設ける方法。このようにする
と、上記ノズルが鉄心として作用することによ
つて電極ワイヤ1b下方への磁束の集中がより
効果的に行われるため、該ノズルをたとえば弱
磁性体の銅で製作した場合に比べ電磁ソレノイ
ドに要求される励磁強さが小さくてすむ。従つ
て電磁ソレノイドの小型化が可能で、電極間隔
のより狭い多電極溶接にも容易に適用すること
ができる。
(3) 電極ワイヤガイドノズルを適当な磁力を有す
る永久磁石により構成する方法。
この方法によれば、溶接条件がほぼきまつて
いる場合、特に電磁コイルを用いることなく、
アークに対して必要な磁界を及ぼすことがで
き、励磁電源装置やスイツチ投入操作を省略す
ることができる。
(4) 電極ワイヤガイドノズルを永久磁石とし、そ
の周囲にさらに電磁ソレノイドを設ける方法。
この方法によれば同じ磁力を得るにも電磁ソ
レノイドの励磁能力を上記(1)或いは(2)の場合よ
り低めることもでき電磁ソレノイドをさらに小
型化できるという利点がある。
尚上記(1)〜(4)のいずれかの方法により励起され
た磁気を電極ワイヤ1b先端まで効率良く導くた
めには電磁ソレノイド、磁心たるワイヤガイドノ
ズル、永久磁石等をできるだけ電極ワイヤ1b先
端付近まで延設することが望ましいことは言うま
でもない。ところが電極ワイヤ1b先端からは、
超高温のアークが発生しており、又溶融池からは
高温の輻射熱、ガスが放出されているので電極ワ
イヤ1b先端に近づけるにしても限度がある。そ
こで実施に際してはワイヤガイドノズルの先端に
装着される通電チツプ2b(通常銅合金で造られ、
使い捨てにされる)として鉄又は鉄合金製のもの
を使用するのが便利である。この場合ワイヤへの
通電性及び鉄スパツタの溶着防止等を考慮して通
電チツプ2bに銅めつき、浸銅処理、耐熱合金溶
射処理等を施したり、また鉄もしくは鉄合金製の
通電チツプ2bの先端部外周を鋼もしくは鋼合金
製のもので覆つたような複合構造体とすることも
可能である。
尚本発明の原理からすれば電極ワイヤ1b先端
及びその近傍における磁界は必ずしも一方向であ
る必要はなく、交番磁界を利用する場合には交流
電磁石の直流アークを用いることにより所期の目
的を十分達成することができる。但しこの場合、
上述の(4)の磁界形成方法は採用できない。
又アーク電流として例えば50乃至60Hzという商
用周波数電流を使用する場合には、励磁電流とし
て直流の代わりに50Hzより周波数の低い交流を使
用することができる。
次に本発明の実施例を示す。
実施例 1
第3図に示す様に第1電極(先行極)及び第2
電極(後行極)を鉛直線に対して溶接方向と反対
方向に夫々4゜と20゜傾け4.0mmφの軟鋼ワイヤ及び
SiO2−MnO系フラツクスを使用して2電極式サ
ブマージアーク溶接法により第4図で示される開
先形状を有する軟鋼板4の両面ワンパス溶接を行
なつた。その際第2電極1bに電磁ソレノイド1
0を使用して下記条件のもとで溶接を行ない、ワ
イヤ先端における磁界強さとビードの状態との関
係を調べた。但し溶接電流には50Hzの交流を、又
励磁電流には直流を使用した。結果は第1表に示
す通りであるが、通電チツプ2a,2bとしては
銅合金製で長さ30mmのものを使用し、又鋼板面に
おける第1電極1aと第2電極1bとの間隔l1,2
は15mmとした。
〔溶接条件〕
第1電極:900×36V
第2電極:700×42V
溶接速度:170cm/min
The present invention relates to a method of performing submerged arc welding at high speed using a multi-electrode wire, and in particular, submerged arc welding can be performed at higher speed by electromagnetically vibrating the arc to reduce the dispersion of the arc force applied to the molten pool. It was made in a similar manner. Multi-electrode welding is considered effective when submerged arc welding of thin plates is performed at high speed.
It is said that the three-electrode method can increase the speed up to about 250 cm/min. However, there is a very strong demand from industry to further increase welding speed and improve welding workability, and the conventional high-speed submerged arc welding method is unable to adequately meet the above demands due to its technical content. It is in. That is, in the multi-electrode method, as welding speed increases, the arc force directed toward the rear of the electrodes increases, causing the essential steel in the molten pool to flow further rearward than necessary, making welding defects such as undercuts and humping more likely to occur. Therefore, in order to prevent such inconveniences from occurring, it is considered an effective means to disperse and reduce the arc force acting on the molten pool.From this perspective, conventional methods have been to mechanically vibrate the welding wire. method is implemented. But this method runs the wire at about 10-30Hz
Since the vibration is performed at a frequency of As mentioned above, for this reason, it is not possible to sufficiently meet the demand for higher speeds. In view of this situation, the present inventors have conducted research to develop a means to disperse and reduce the arc force applied to the molten pool without mechanically vibrating the wire. We have completed a method that can achieve even higher speeds by electromagnetically oscillating the arc using this method. However, in the multi-electrode high-speed submerged arc welding method of the present invention, an alternating magnetic field is applied below at least the second and subsequent electrode wires to direct the arcs of adjacent and preceding electrodes in a horizontal direction orthogonal to the welding line. Magnetic flux density value (unit: Gauss) measured below the electrode wire while welding while vibrating
However, the gist of this method is to perform submerged arc welding while maintaining the strength of the magnetic field so that the welding current value (unit: ampere) of the adjacent preceding electrode wire is at least 1/4 or more. The configuration and effects of the present invention will be specifically explained below with reference to the drawings. FIGS. 1 and 2 are explanatory diagrams of the principle of the method of the present invention, and for ease of understanding, show a case in which high-speed submerged arc welding is performed by a two-electrode method. P 1 and P 2 are leading electrodes and trailing electrodes, respectively; 1a and 1b are electrode wires, respectively;
Arcs 6a and 6b generated from their tips are radiated in a direction opposite to the welding direction (direction of arrow A). Therefore, the molten steel 5 in the molten pool is blown up onto the rear solidification surface, resulting in a shortage of molten steel in the front, creating a situation where undercuts are likely to occur. This situation shows a remarkable tendency, as the smaller the distance d between the wire tips, the easier it is for the arc forces of both electrodes to coordinate. However, in the present invention, as shown in FIG. 2, a magnetic field 8 is applied below the trailing electrode wire 1b in which lines of magnetic force act so as to perpendicularly cross the arc 6a of the leading electrode P1 , so that the arc 6a is located on Fleming's left hand. According to the law, a force is applied in a direction perpendicular to the plane of the paper (perpendicular to the weld line), and it is deflected in a direction that crosses the weld line. In this case, if the direction of the magnetic lines of force, that is, the magnetic vector H, is always kept constant, and the direction of the current, that is, the direction of the current vector I, is changed over time, then
The arc 6a will be vibrated in a direction across the weld line. In this case, since the leading electrode wire 1a is not particularly forcibly vibrated, there is no need to worry about the droplets at the tip of the wire being forcibly shaken off or the flux being disturbed by the wire, and the occurrence of burrs at the bead edge. It is possible to avoid appearance and structural welding defects caused by nitrogen intrusion into molten steel. Above, we have explained the case where the magnetic field of the trailing electrode acts on the arc of the leading electrode, but by applying a magnetic field directly below the leading electrode, that is, by a magnetic field that acts strongly under the leading electrode, the self-polar Of course, it is also conceivable to control the arc directly. However, since the present invention is intended to be effectively applied to high-speed welding, that is, when the arc is flowing in a nearly horizontal state,
As mentioned above, simply applying a magnetic field below the trailing electrode is sufficient to achieve the purpose, and is more effective in controlling the arc of the leading electrode. However, when applying the magnetic field 8 below the trailing electrode P2 , the following considerations must be made. That is, the magnetic flux density value (unit: Gauss) measured at the tip of the electrode wire 1b is at least 1/4 or more of the welding current value (unit: ampere) of the adjacent and preceding electrode wire 1a (both are anonymized and compared, for example, 1000 arc 6 under electrode wire 1b).
It is not possible to induce a sufficient force to drive a in the direction across the welding line, and furthermore, it cannot be expected to be effective in eliminating inconveniences such as undercuts. However, in order to measure the above magnetic field strength, it is necessary to specify the ``wire tip position,'' which is because the length of the wire is usually called the ``wire extension'' (the current tip along the wire direction). (distance from the steel plate surface) (for example, points X 1 and X 2 in Figure 1). Further, some consideration must be given to the relationship with the electrode wire tip distance l. In other words, the shorter the distance between the wire tips l 1 and 2 (the distance between the tips of the first and second poles), the more cooperative the arcs 6a and 6b become, and the more the molten steel 5 is driven backwards, which is undesirable. , it is preferable to create a state in which the magnetic field 8 becomes stronger as the distance between the wire tips l 1 and 2 decreases. In experiments conducted by the inventors, the product of the wire tip spacing value (unit: mm) and the magnetic flux density value (unit: Gauss) is approximately 3000 or more (for example, if the spacing is 20 mm, it is 150 Gauss or more). It has been confirmed that if the distance between the wire tips l 1 and 2 becomes shorter, the coordination of the arcs 6a and 6b will not increase. By the way, in order to apply the magnetic field 8 below the electrode wire 1b, it is effective to form an external magnetic field around the electrode wire 1b, and the following methods can be cited as specific means for this. (1) A method of providing an electromagnetic solenoid around the electrode wire 1b. In this case, it is preferable in terms of device design to provide an electromagnetic solenoid around a general-purpose wire guide nozzle (not shown) because no special space is required even in multi-electrode welding with narrow electrode spacing. (2) In the configuration of (1), the electrode wire guide nozzle is made of a ferromagnetic material such as iron or iron alloy, and an electromagnetic solenoid is provided around it. In this case, since the nozzle acts as an iron core, the magnetic flux is more effectively concentrated below the electrode wire 1b. The excitation strength required for the solenoid is small. Therefore, the electromagnetic solenoid can be made smaller and can be easily applied to multi-electrode welding with narrower electrode spacing. (3) A method in which the electrode wire guide nozzle is constructed of a permanent magnet having an appropriate magnetic force. According to this method, when the welding conditions are almost strict, it is possible to
A necessary magnetic field can be applied to the arc, and the need for an excitation power supply or switch-on operation can be omitted. (4) A method in which the electrode wire guide nozzle is a permanent magnet and an electromagnetic solenoid is further provided around it. This method has the advantage that the excitation capacity of the electromagnetic solenoid can be lowered than in the above cases (1) or (2) to obtain the same magnetic force, and the electromagnetic solenoid can be further miniaturized. In order to efficiently guide the magnetism excited by any of the methods (1) to (4) above to the tip of the electrode wire 1b, place the electromagnetic solenoid, wire guide nozzle serving as a magnetic core, permanent magnet, etc. as close to the tip of the electrode wire 1b as possible. It goes without saying that it is desirable to extend the However, from the tip of the electrode wire 1b,
Since an ultra-high temperature arc is generated and high-temperature radiant heat and gas are emitted from the molten pool, there is a limit to how close it can get to the tip of the electrode wire 1b. Therefore, when implementing it, a current-carrying chip 2b (usually made of copper alloy) attached to the tip of the wire guide nozzle,
It is convenient to use ones made of iron or iron alloys (disposable). In this case, in order to conduct electricity to the wire and prevent welding of iron spatters, the current-carrying chip 2b may be subjected to copper plating, copper dipping treatment, heat-resistant alloy spraying, etc., or the current-carrying chip 2b may be made of iron or iron alloy. It is also possible to form a composite structure in which the outer periphery of the tip is covered with something made of steel or a steel alloy. According to the principle of the present invention, the magnetic field at the tip of the electrode wire 1b and its vicinity does not necessarily have to be unidirectional; when using an alternating magnetic field, the DC arc of an AC electromagnet can be used to achieve the desired purpose. can be achieved. However, in this case,
The above magnetic field forming method (4) cannot be adopted. Further, when using a commercial frequency current of 50 to 60 Hz as the arc current, for example, an alternating current with a frequency lower than 50 Hz can be used as the exciting current instead of a direct current. Next, examples of the present invention will be shown. Example 1 As shown in Fig. 3, the first electrode (leading electrode) and the second
The electrode (trailing electrode) was tilted at 4° and 20° in the direction opposite to the welding direction with respect to the vertical line, respectively.
One-pass welding on both sides of a mild steel plate 4 having the groove shape shown in FIG. 4 was performed by two-electrode submerged arc welding using SiO 2 --MnO flux. At that time, the electromagnetic solenoid 1 is connected to the second electrode 1b.
Welding was performed under the following conditions using 0.0 to investigate the relationship between the magnetic field strength at the tip of the wire and the state of the bead. However, 50Hz alternating current was used for the welding current, and direct current was used for the excitation current. The results are shown in Table 1. The current-carrying chips 2a and 2b were made of copper alloy and had a length of 30 mm, and the distance between the first electrode 1a and the second electrode 1b on the surface of the steel plate was l 1 , 2
was set to 15mm. [Welding conditions] 1st electrode: 900×36V 2nd electrode: 700×42V Welding speed: 170cm/min
第1電極:1200A×34V 第2電極:900A×42V 第3電極:700A×44V 溶接速度:330cm/min 1st electrode: 1200A×34V 2nd electrode: 900A×42V 3rd electrode: 700A×44V Welding speed: 330cm/min
【表】
実施例 3
アンダーカツトの発生状態と電極ワイヤ間隔、
溶接電流、磁束密度の関係を調べるために第3電
極に電磁ソレノイドを付して3電極式サブマージ
アーク溶接を行なつた。この場合電磁ソレノイド
のコアを軟鋼製とし、ワイヤガイドノズルを兼用
させた。又第3電極の通電チツプとしては第5図
bで示されるような軟鋼部27とクロム銅部28
の複合体構造のものを使用すると共に、4.0mmφ
の軟鋼製ワイヤ及びSiO2−Al2O3−CaO−TiO2
−CaF2系フラツクスを使用した。そして溶接電
流には50Hzの交流を励磁電流には直流を使用し、
深さ3mmの90゜溝を両面に有する9mm厚の軟鋼板
を下記条件のもとで溶接してアンダーカツト発生
の有無を調べた。但し第1、第2、第3電極の傾
きは夫夫2゜、12゜、24゜傾き方向は実施例1と同じ
であり、通電チツプと鋼板面との間隔は第1、第
2電極が30mm、第3電極が25mmである。結果は第
3表に示す通りである。
〔溶接条件〕
A第1電極:900A×35V
第2電極:600A×40V
第3電極:500A×45V
溶接速度:300cm/min
B第1電極:1000A×35V
第2電極:800A×40V
第3電極:650A×45V
溶接速度:360cm/min[Table] Example 3 Condition of undercut occurrence and electrode wire spacing,
In order to investigate the relationship between welding current and magnetic flux density, three-electrode submerged arc welding was performed by attaching an electromagnetic solenoid to the third electrode. In this case, the core of the electromagnetic solenoid was made of mild steel and also served as a wire guide nozzle. Further, as the current-carrying chip of the third electrode, a mild steel part 27 and a chromium copper part 28 as shown in FIG. 5b are used.
In addition to using a composite structure of 4.0mmφ
mild steel wire and SiO 2 −Al 2 O 3 −CaO−TiO 2
−CaF 2 -based flux was used. The welding current uses 50Hz alternating current and the exciting current uses direct current.
A 9 mm thick mild steel plate with 3 mm deep 90° grooves on both sides was welded under the following conditions and the occurrence of undercuts was examined. However, the inclinations of the first, second, and third electrodes are 2°, 12°, and 24°; the inclination directions are the same as in Example 1, and the distance between the current-carrying chip and the steel plate surface is such that the first and second electrodes are 30mm, and the third electrode is 25mm. The results are shown in Table 3. [Welding conditions] A 1st electrode: 900A x 35V 2nd electrode: 600A x 40V 3rd electrode: 500A x 45V Welding speed: 300cm/min B 1st electrode: 1000A x 35V 2nd electrode: 800A x 40V 3rd electrode :650A×45V Welding speed: 360cm/min
【表】
ことを示す。
上記第1〜第3表から明らかな様に実施例1か
ら実施例3のいずれの実施例においても第2位以
後の電極下方での磁束密度(単位:ガウス)が隣
接先行電極の溶接電流値(単位:アンペア)の少
なくとも1/4以上あればアンダーカツトの発生は
全く見られない。
実施例 4
通電チツプとして鋼部を有する銅・鋼複合構造
体のものを使用し、ワイヤ励磁能力及び耐熱性を
調べた。但し通電チツプとしては第5図a〜cで
示されるものを用意した。図中21,25,29
はワイヤ通過孔、22,26,30は接続ねじ
部、23,27,31は鋼部、24,28は銅
部、32は銅めつき部である。まず励磁能力即ち
磁界強さの向上を確認するため実施例1の実験番
号1−3において通電チツプを上記a〜cのもの
と交換して実施した結果、ワイヤ先端において
夫々1300、1700、1500ガウスと著しく向上するこ
とが認められた。
次に実施例1の条件により、上記a〜cの通電
チツプをこれらチツプ先端が鋼板面から30mmとな
るように第2電極に取付けて100m連続溶接した
結果、通電特性、溶損度等はいずれも通常の銅合
金製のものに比べて見劣りすることはなかつた。
本発明は以上の様に構成されるが、要はワイヤ
を機械的に振動させずに所定強さの磁気力を利用
してアークを電磁気的に振動させて溶融池にかか
るアーク力の分散軽減を図るようにしたので、溶
接部の品質を何ら損うことなくサブマージアーク
溶接をより一層高速で行なえる様になつた。[Table] Shows that.
As is clear from Tables 1 to 3 above, in any of Examples 1 to 3, the magnetic flux density (unit: Gauss) below the second and subsequent electrodes is the welding current value of the adjacent preceding electrode. (Unit: ampere) If it is at least 1/4 or more, no undercut will occur at all. Example 4 A copper/steel composite structure having a steel part was used as an energizing chip, and its wire excitation ability and heat resistance were investigated. However, the current-carrying chips shown in FIGS. 5a to 5c were prepared. 21, 25, 29 in the figure
22, 26, 30 are connecting screw portions, 23, 27, 31 are steel portions, 24, 28 are copper portions, and 32 is a copper plated portion. First, in order to confirm the improvement in the excitation ability, that is, the magnetic field strength, in Experiment No. 1-3 of Example 1, the current-carrying chips were replaced with the ones a to c above. A significant improvement was observed. Next, under the conditions of Example 1, the current-carrying chips a to c above were attached to the second electrode so that the tips of these chips were 30 mm from the steel plate surface, and welded continuously for 100 m. However, it was not inferior to those made of ordinary copper alloy. The present invention is configured as described above, but the key point is to electromagnetically vibrate the arc using magnetic force of a predetermined strength without mechanically vibrating the wire, thereby reducing the dispersion of the arc force applied to the molten pool. As a result, submerged arc welding can now be performed at even higher speeds without any loss in quality of the welded part.
第1図及び第2図は本発明方法の原理説明図、
第3図〜第5図は実施例条件説明図である。
P1……先行電極、P2……後行電極、1a,1
b……電極ワイヤ、2a,2b……通電チツプ、
4……鋼板、5……溶鋼、6a,6b……アー
ク、7……溶接金属、8……磁界、H……磁気ベ
クトル、I……電流ベクトル。
1 and 2 are diagrams explaining the principle of the method of the present invention,
FIGS. 3 to 5 are explanatory diagrams of the conditions of the embodiment. P 1 ... Leading electrode, P 2 ... Trailing electrode, 1a, 1
b... Electrode wire, 2a, 2b... Current-carrying chip,
4... Steel plate, 5... Molten steel, 6a, 6b... Arc, 7... Welding metal, 8... Magnetic field, H... Magnetic vector, I... Current vector.
Claims (1)
位:ガウス)ならびに隣接先行する電極における
溶接電流値(単位:アンペア)をそれぞれ無名数
化したものが、下記条件を満たすように少なくと
も2極目以降の電極ワイヤ下方に交番磁界を付与
して、隣接先行する電極のアークを溶接線と直交
する水平方向に振動させながら溶接することを特
徴とする多電極式高速サブマージアーク溶接方
法。 溶接電流値/磁束密度値≦4[Claims] 1. The magnetic flux density value (unit: Gauss) measured below the electrode wire and the welding current value (unit: ampere) at the adjacent preceding electrode are anonymized so that the following conditions are satisfied. A multi-electrode high-speed submerged arc welding method, characterized in that an alternating magnetic field is applied below the electrode wires of at least the second and subsequent electrodes, and welding is performed while the arcs of adjacent and preceding electrodes are vibrated in a horizontal direction perpendicular to the welding line. . Welding current value/magnetic flux density value≦4
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP9513284A JPS60240382A (en) | 1984-05-12 | 1984-05-12 | Multiple-electrode high speed submerged arc welding |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP9513284A JPS60240382A (en) | 1984-05-12 | 1984-05-12 | Multiple-electrode high speed submerged arc welding |
Publications (2)
| Publication Number | Publication Date |
|---|---|
| JPS60240382A JPS60240382A (en) | 1985-11-29 |
| JPH0333436B2 true JPH0333436B2 (en) | 1991-05-17 |
Family
ID=14129291
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP9513284A Granted JPS60240382A (en) | 1984-05-12 | 1984-05-12 | Multiple-electrode high speed submerged arc welding |
Country Status (1)
| Country | Link |
|---|---|
| JP (1) | JPS60240382A (en) |
Family Cites Families (1)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| JPS5533833A (en) * | 1978-08-31 | 1980-03-10 | Nippon Steel Corp | High speed inclined position submerged arc welding method |
-
1984
- 1984-05-12 JP JP9513284A patent/JPS60240382A/en active Granted
Also Published As
| Publication number | Publication date |
|---|---|
| JPS60240382A (en) | 1985-11-29 |
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