JPH0381071A - Nonconsumable electrode arc welding method for aluminum alloy - Google Patents

Nonconsumable electrode arc welding method for aluminum alloy

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Publication number
JPH0381071A
JPH0381071A JP21953589A JP21953589A JPH0381071A JP H0381071 A JPH0381071 A JP H0381071A JP 21953589 A JP21953589 A JP 21953589A JP 21953589 A JP21953589 A JP 21953589A JP H0381071 A JPH0381071 A JP H0381071A
Authority
JP
Japan
Prior art keywords
current
welding
electrode
polarity
tip
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.)
Granted
Application number
JP21953589A
Other languages
Japanese (ja)
Other versions
JP2836112B2 (en
Inventor
Tomoyuki Kamiyama
智之 上山
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.)
Daihen Corp
Original Assignee
Daihen Corp
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Filing date
Publication date
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Priority to JP21953589A priority Critical patent/JP2836112B2/en
Publication of JPH0381071A publication Critical patent/JPH0381071A/en
Application granted granted Critical
Publication of JP2836112B2 publication Critical patent/JP2836112B2/en
Anticipated expiration legal-status Critical
Expired - Fee Related legal-status Critical Current

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Abstract

PURPOSE:To narrow a bead width and to deepen penetration by applying a reverse polarity current having a specified crest value of a welding current and the specified weld time when a nonconsumable electrode is in the positive polarity and applying a straight polarity current having a specified crest value of a welding current and the specified weld time when the nonconsumable electrode is in the negative polarity. CONSTITUTION:The nonconsumable electrode with the tip 1a having an inclined flat shape on both sides is arranges in the direction where the long side directions L1 and L2 of the electrode tip are coincident with the weld line directions. When the nonconsumable electrode is in the positive polarity, the reverse polarity current having 300-500A crest value of the welding current and 0.5-3mus weld time is applied. When the nonconsumble electrode is in the negative polarity, the straight polarity current having 150-500A crest value of the welding current and 9-15mus weld time is applied to perform welding.

Description

【発明の詳細な説明】 [産業上の利用分野] 本発明は、アルミニウム合金の中厚板を、1パスで深い
溶は込みを得る非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 [Industrial Application Field] The present invention relates to a non-consumable electrode arc welding method for obtaining deep penetration in a single pass of a medium-thick aluminum alloy plate.

[従来の技術] 従来から、アルミニウム合金の深い溶は込みの溶接結果
を得る非消耗電極アーク溶接方法として、第1の方法は
、アルミニウム合金の酸化膜を溶接前に機械的又は化学
的に除去しておいて、直流正極性TIG溶接する方法で
あり、この方法では、ある程度の深い溶は込みは得られ
るが、溶接前に酸化皮膜の除去作業の余分の工程が必要
であり、また、除去作業後に発生した酸化皮膜が溶融金
属中に巻き込まれ、溶接欠陥を発生することが多い。
[Prior Art] Conventionally, as a non-consumable electrode arc welding method for obtaining a deep penetration welding result of aluminum alloy, the first method is to mechanically or chemically remove the oxide film of the aluminum alloy before welding. This method uses direct current positive polarity TIG welding. Although this method can achieve a certain degree of deep penetration, it requires an extra step of removing the oxide film before welding, and The oxide film formed after the work gets caught up in the molten metal and often causes welding defects.

また、第2の方法は、矩形波の交流パルス電流を用いて
、交流電流の正負極性の通電時間比率又はa電比率又は
その両者を適宜に調整する方法であり、この方法では、
アルミニウム表面の酸化皮膜を除去し、ある程度の深い
溶は込みを得ることができるが、ビード幅が広がり、熱
影響範囲が広がり、また電極先端の消耗が大で、電極先
端形状整形のために、しばしば中断しなければならない
In addition, the second method is a method of appropriately adjusting the energization time ratio of positive and negative polarity of the alternating current, the a-current ratio, or both using a rectangular wave alternating current pulse current.
Although it is possible to remove the oxide film on the aluminum surface and achieve a certain degree of deep weld penetration, the bead width increases, the heat-affected area expands, and the electrode tip wears out considerably. Must be interrupted often.

さらに、第3の方法は、交流プラズマ溶接方法であるが
、この方法では、深い溶は込みは得られるが、大電流に
なるとシリーズアークが発生しやすくなるので、実用上
、板厚8 [mm]以下の生厚板程度までであって、そ
れ以上の厚板では採用が困難であった。
Furthermore, the third method is AC plasma welding, but although deep penetration can be achieved with this method, series arcs are likely to occur when the current is large, so in practice it is recommended that the plate thickness be 8 [mm]. ] or below, and it was difficult to use thicker plates.

さらに、非消耗電極の先端を平面状に裁断して、電極軸
を中心に回転又は揺動してアークの指向性を高めて、開
先壁の溶は込みを得たり、アーク磁気制御方法と組合せ
てアンダーカットの防止及び不良ビードの改善を行った
りしているが、ビード幅が広くなっている。
Furthermore, the tip of the non-consumable electrode is cut into a flat shape and rotated or oscillated around the electrode axis to increase the directivity of the arc and obtain melt penetration in the groove wall. Although this combination is used to prevent undercuts and improve defective beads, the bead width has become wider.

[発明が解決しようとする問題点] 従来のアルミニウム合金の中厚板の溶接方法においては
、いずれの方法も、アルミニウム合金表面の酸化皮膜を
充分に除去して欠陥のない溶接部が得られないか、又は
ビード幅が狭くて深い溶は込みを得ることができないか
、又は非消耗電極先端の消耗が大であるかのいずれかの
問題点があり、これらが同時に解決させていない。
[Problems to be Solved by the Invention] None of the conventional welding methods for medium-thick aluminum alloy plates can sufficiently remove the oxide film on the aluminum alloy surface to obtain a defect-free weld. However, there are problems in that the bead width is narrow and deep penetration cannot be obtained, or the tip of the non-consumable electrode is severely worn out, and these problems have not been solved at the same time.

[問題点を解決するための手段] 本発明のアルミニウム合金の非消耗電極アーク溶接方法
は、■適正なりリーニング幅を確保すること、■ビード
幅を狭くすること、■溶は込み深さを大にすること、■
電極の消耗を少なくすること、以上の4つの要求を同時
に満足させるために、 A、電極先端が両面傾斜偏平形状の非消耗電極を、その
電極先端の長辺方向と溶接線方向とが一致する方向に配
置して矩形波交流電流を通電すること、 B、ビード幅を狭くして溶は込み深さを深くし、電極消
耗を少なくするために、正極性溶接電流の波高値Isを
所定値以上にすること、C1上記Bと同じ作用効果を得
るために、正極性溶接電流の通電時間Tsを所定値以上
にすること、 D、適正なりリーニング幅を確保した上で、ビード幅を
狭くし、電極の消耗を極めて小さくするために、逆極性
溶接電流の通電時間Trをできるだけ小さい所定値にす
ること、 E、上記りと同じ作用効果で、逆極性溶接電流の波高値
Irを、適正なりリーニング幅を確保することができる
必要最小限度の所定値にすること、 F、前述した■乃至■を同時に満足するように、上記B
乃至E項のパラメータの相互関係を検討して、4つのパ
ラメータの適正範囲内で、アルミニウム合金の非消耗電
極アーク溶接する方法[作用及び実施例コ (第2図乃至第6図の説明) 本発明のアルミニウム合金の非消耗電極アーク溶接方法
において通電する溶接電流は、矩形波の交流電流であっ
て、この矩形波交流電流の4つのパラメータを、第2図
に示すように、非消耗電極がプラス極性のとき(以下、
逆極性という)の溶接電流の波高値をIr、通電時間を
Trとし、また電極がマイナス極性のとき(以下、正極
性という)の溶接電流の波高値をIs。
[Means for Solving the Problems] The method of non-consumable electrode arc welding of aluminum alloys of the present invention includes: (1) securing an appropriate leaning width, (2) narrowing the bead width, and (2) increasing the penetration depth. To do,■
In order to reduce electrode wear and satisfy the above four requirements at the same time, A. A non-consumable electrode whose tip has a flat shape with both sides inclined is made such that the long side direction of the electrode tip coincides with the direction of the welding line. B. In order to narrow the bead width, deepen the penetration depth, and reduce electrode wear, the peak value Is of the positive welding current is set to a predetermined value. C. In order to obtain the same effect as in B above, the conduction time Ts of the positive welding current should be set to a predetermined value or more. D. After ensuring an appropriate leaning width, narrow the bead width. , In order to minimize the consumption of the electrode, the conduction time Tr of the reverse polarity welding current is set to a predetermined value as small as possible; E. With the same effect as above, the peak value Ir of the reverse polarity welding current is set to an appropriate value. F. The above B should be set so that the above-mentioned ■ to ■ are satisfied at the same time.
A method for non-consumable electrode arc welding of aluminum alloys by examining the interrelationships of the parameters in sections E to E and within the appropriate range of the four parameters [Function and Examples (Explanation of Figures 2 to 6)] The welding current applied in the non-consumable electrode arc welding method for aluminum alloys of the invention is a rectangular wave alternating current, and the four parameters of this rectangular wave alternating current are determined by the non-consumable electrode as shown in FIG. When the polarity is positive (hereinafter,
The peak value of the welding current when the electrode is of negative polarity (hereinafter referred to as positive polarity) is Ir, the energization time is Tr, and the peak value of the welding current when the electrode is of negative polarity (hereinafter referred to as positive polarity) is Is.

通電時間をTsとする。Let the energization time be Ts.

これらの4つのパラメータを変化させたときに、本発明
の溶接方法において同特に満゛足させたい4つの項目す
なわち、■溶は込み深さ、■ビード幅、■クリーニング
幅、■電極消耗の程度について検討した結果は、第1表
のとおりでなお、以下の本発明の溶接方法に使用する非
消耗電極1の先端1aの形状は、第3図に示すように、
両面傾斜偏平形状であって、同図(A)は正面図であり
、同図(B)は側面図であり、同図(C)は電極先端方
向からみた平面図であって、同図(C)の矢印り、L2
方向に示す長辺方向が後述する第4図に示す溶接線り方
向と一致するように配置される。すなわち、電極先端1
aから被溶接物3及び4に発生するアーク4の広がりは
第4図(A)及び(B)に示すようになり、その結果、
上記4つのパラメータの適正値とも関係して、ビード幅
が第5図(A)に示す従来の方法の8!から同図(B)
に示す本発明の方法の82に変化して狭くなる。同様に
溶は込み深さは、同図(A)及び(B)に示すように、
PlからPlに増加している。なお、第5図のビード形
状は、板厚10[mmlのアルミニウム合金(A505
2)を、溶接電流350[A]で溶接速度50[cm/
min]で溶接した場合であって、同図(A)は、Ts
−10及びTr−6[ms]の正弦波による従来の溶接
方法であり、同図(B)は、l5−350   [A]
  、   Ts−10[ms  コ 、Ir−350
[A]及びTr〜1[ms]の矩形波による本発明の溶
接方法の場合を示す。また、第6図は、溶接開始前の電
極先端が、同図(A)に示すように、偏平形状である非
消耗電極(以下、偏平電極という)を使用して、l5=
350[Aコ。
When these four parameters are changed, the four items that are particularly desired to be satisfied in the welding method of the present invention are: ■ penetration depth, ■ bead width, ■ cleaning width, and ■ extent of electrode wear. The results of the study are shown in Table 1, and the shape of the tip 1a of the non-consumable electrode 1 used in the welding method of the present invention below is as shown in FIG.
The figure (A) is a front view, the figure (B) is a side view, and the figure (C) is a plan view seen from the direction of the tip of the electrode. C) arrow, L2
It is arranged so that the long side direction shown in the direction coincides with the welding line direction shown in FIG. 4, which will be described later. That is, the electrode tip 1
The spread of the arc 4 generated from a to the objects 3 and 4 to be welded is as shown in FIGS. 4(A) and 4(B), and as a result,
In relation to the appropriate values of the above four parameters, the bead width is 8! in the conventional method shown in FIG. 5(A). From the same figure (B)
82 of the method of the invention shown in FIG. Similarly, the penetration depth is as shown in (A) and (B) in the same figure.
It increases from Pl to Pl. Note that the bead shape in Fig. 5 is made of aluminum alloy (A505) with a plate thickness of 10 mm.
2) at a welding current of 350 [A] and a welding speed of 50 [cm/
(A) shows the case of welding at Ts
This is a conventional welding method using sine waves of -10 and Tr-6 [ms], and the figure (B) shows l5-350 [A]
, Ts-10[ms ko, Ir-350
[A] and the case of the welding method of the present invention using a rectangular wave of Tr~1 [ms] is shown. In addition, FIG. 6 shows that l5=
350 [A.

Ts−10[mSコ、  I r−350[A]及びT
r−1[ms]の矩形波電流を10分間繰り返した後に
、5分間休止し、再び通電し、これらのサイクルを合計
6回繰り返して、1時間溶接したとき、同図(B)に示
すように、電極先端形状が多少丸くなっている程度しか
消耗していない。これに対して、比較のために、溶接開
始前の電極先端形状が図示していない断面円形尖頭形状
の非消耗電極(以下、尖頭丸形電極という)を使用して
、正極性及び逆極性電流の実効値が350[A]で、正
極性及び逆極性電流の通電時間がそれぞれ10[ms]
及び6 [ms]の正弦波を使用して1時間溶接すると
、電極先端形状は、同図(C)に示すように、完全に溶
融消耗して先端は丸くなり、アークの再スタートが極め
て困難になっている。
Ts-10 [mS Co, I r-350 [A] and T
After repeating a rectangular wave current of r-1 [ms] for 10 minutes, pausing for 5 minutes, and turning on the current again, these cycles were repeated a total of 6 times and welded for 1 hour, as shown in the same figure (B). However, the electrode tip was only worn to the extent that it was slightly rounded. On the other hand, for comparison, we used a non-consumable electrode (hereinafter referred to as a round pointed electrode) whose electrode tip shape before welding started was a circular pointed cross section (not shown). The effective value of polarity current is 350 [A], and the conduction time of positive polarity and reverse polarity current is 10 [ms] each.
When welding for 1 hour using a sine wave of 6 [ms], the shape of the electrode tip was completely melted and consumed, and the tip became rounded, making it extremely difficult to restart the arc, as shown in Figure (C). It has become.

(第7図の説明) 次に、第7図は、上記4つのパラメータのうち、電極が
マイナス(正極性)のときの溶接電流15−400 [
Aコとその通電時間TsmlO[ms]と電極がプラス
(逆極性)のときの溶接電流Ir−400[A] とを
一定値にしておいて、逆極性電流の通電時間Trを0.
5[m s ]から6[ms]まで変化させたとき(横
軸)の溶は込み深さP [mml  (縦軸)を求めた
線図である。この実施例の溶接条件は、被溶接材が板厚
10[mm]のマグネシウム含有アルミニウム合金であ
り、溶接速度は50[cm/m1nlであって、実線で
示す本発明の溶接方法の偏平形電極を使用したときの溶
は込み深さPは、点線で示す従来方法の尖頭丸形電極を
使用して上記と同一条件で溶接したときよりも大になっ
ている。
(Explanation of Fig. 7) Next, Fig. 7 shows the welding current of 15-400 when the electrode is negative (positive polarity) among the above four parameters.
A, its energization time TsmlO [ms], and the welding current Ir-400 [A] when the electrode is positive (reverse polarity) are set to constant values, and the energization time Tr of the reverse polarity current is set to 0.
It is a diagram showing the melt penetration depth P [mml (vertical axis) when changing from 5 [ms] to 6 [ms] (horizontal axis). The welding conditions of this example are that the material to be welded is a magnesium-containing aluminum alloy with a plate thickness of 10 mm, the welding speed is 50 cm/ml, and the flat electrode of the welding method of the present invention is shown by the solid line. The penetration depth P when using the welding method is larger than that when welding is performed under the same conditions as above using the conventional method of pointed round electrode shown by the dotted line.

(第1図の説明) 第1図は、前述した4つのパラメータのうち、正極性溶
接電流の通電時間Tsが約10[ms]逆極性溶接電流
の通電時間Trが1[mslで溶接速度50[cm/m
in]としたときの正極性溶接電流Is及び正極性電流
に等しい逆極性電流Ir(横軸)を変化させたとき、溶
は込み深さPとビード幅Wとの比P/W(縦軸)を示す
線図である。同図において、正極性電流又は逆極性電流
が290[A1未満の斜線で示す領域においては、逆極
性電流が小さいために、クリーニング作用が充分に行わ
れないので、酸化皮膜が溶着金属内に巻き込まれて良好
tl溶接結果が得られないが、290[A3以上では良
好な溶着金属が得られる。また、同図の実線は、本発明
の溶接方法に使用する偏平電極を用いたときの溶は込み
深さとビード幅との比P/Wを示し、点線で示す従来の
尖頭丸形電極を使用したときよりも大きなP/W値を得
ることができる。
(Explanation of Figure 1) Figure 1 shows that among the four parameters mentioned above, the conduction time Ts of the positive polarity welding current is about 10 [ms], the conduction time Tr of the reverse polarity welding current is 1 [msl], and the welding speed is 50 [msl]. [cm/m
in], and when the positive welding current Is and the reverse polarity current Ir (horizontal axis), which is equal to the positive current, are changed, the ratio P/W of penetration depth P and bead width W (vertical axis ). In the figure, in the shaded area where the positive polarity current or the reverse polarity current is less than 290 [A1], the cleaning action is not performed sufficiently because the reverse polarity current is small, so the oxide film gets caught up in the weld metal. However, good weld metal can be obtained with 290[A3 or higher]. In addition, the solid line in the figure shows the ratio P/W of penetration depth to bead width when using the flat electrode used in the welding method of the present invention, and the dotted line shows the ratio P/W of the conventional pointed round electrode. A larger P/W value can be obtained than when using it.

(適正溶接条件範囲) 本発明の溶接方法において、適正溶接条件の範囲限定理
由について説明する。
(Appropriate Welding Condition Range) In the welding method of the present invention, the reason for limiting the range of appropriate welding conditions will be explained.

正極性電流Is 逆極性電流が通電時間T r = 3 [m s ] 
、溶接電流の波高値1 r−500[:A]になったと
きに、正極性電流の波高値Isが150[A1未満にな
ると、電子放出による電極先端部分の冷却作用が小さく
なって、電極が溶落する。したがって、正極性電流は、
150[A3以上とすることが必要である。
Positive polarity current Is Reverse polarity current conduction time T r = 3 [ms]
, when the peak value Is of the positive polarity current becomes less than 150[A1] when the peak value of the welding current reaches 1r-500[:A], the cooling effect of the electrode tip due to electron emission becomes small, and the electrode melts away. Therefore, the positive polarity current is
It is necessary to make it 150 [A3 or more.

正極性及び逆極性溶接電流の通電時間Ts。Current application time Ts of positive polarity and reverse polarity welding current.

T 「 本発明の溶接方法において、周波数を50〜100 [
Hzlにすると、溶接部の溶は込み、アークの安定性が
よく、この範囲内では溶は込みが浅くなったり、アーク
切れを生じることがない。この範囲外では、溶接部の溶
は込みが浅くなったり、アーク切れが生じやすくなる。
T "In the welding method of the present invention, the frequency is 50 to 100 [
Hzl provides good weld penetration and arc stability, and within this range, shallow penetration and arc breakage do not occur. Outside this range, the weld penetration becomes shallow and arc breakage tends to occur.

さらに、逆極性時間Trを0.5〜3 [ms]にする
と、逆極性電流の波高値Irを500[A]まで増加さ
せることができ、電極の消耗を小さくすることができる
。また、正極性電流a常時間を9乃至15[ms]にす
ることにより、逆極性電流よりも大きくして、通常の直
流電流による非消耗電極と同様の溶は込み形状を得るこ
とができる。
Further, when the reverse polarity time Tr is set to 0.5 to 3 [ms], the peak value Ir of the reverse polarity current can be increased to 500 [A], and the wear of the electrode can be reduced. Further, by setting the normal time of the positive polarity current a to 9 to 15 [ms], the current can be made larger than the reverse polarity current, and a melt-in shape similar to that of a non-consumable electrode using a normal direct current can be obtained.

逆極性電流Ir 逆極性電流通電時間を0.5乃至3[ms]にしている
ので、アルミニウム合金の溶接に必要なりリーニング幅
を確保するために、逆極性電流の波高値■「は300[
A3以上が必要となる。
Reverse polarity current Ir Since the reverse polarity current conduction time is set to 0.5 to 3 [ms], the peak value of the reverse polarity current is 300 [ms] in order to ensure the leaning width necessary for welding aluminum alloys.
A3 or higher is required.

[発明の効果コ 本発明の溶接方法は下記の効果がある。[Effects of invention The welding method of the present invention has the following effects.

A、[樋先端が偏平形状の非消耗電極を、その長辺方向
と溶接線方向とが一致するように配置することにより、
ビード幅の狭い深い溶は込み形状が得られる。
A. [By arranging a non-consumable electrode with a flat gutter tip so that its long side direction matches the welding line direction,
A deep melt-in shape with a narrow bead width can be obtained.

B、正極性溶接電流の波高値Isを150[A3以上と
することにより、電子放出による電極先端の冷却作用を
促進して電極の溶落消耗を防ぐ。
B. By setting the peak value Is of the positive welding current to 150 [A3 or more, the cooling effect of the electrode tip due to electron emission is promoted and the wear and tear of the electrode is prevented.

C6正極性溶接電流の通電時間Tsを9乃至15[ms
]にして、逆極性溶接電流の通電時間Trの0.5乃至
3[ms]よりも大きくすることにより、クリーニング
に必要な逆極性溶接電流の通電時間Trを最小限にして
、電極の消耗を少なくするとともに、直流正極性の場合
と同様の深い溶は込み形状を得ることができる。
The application time Ts of the C6 positive polarity welding current is 9 to 15 [ms].
], and by making the conduction time Tr of the reverse polarity welding current larger than 0.5 to 3 [ms], the conduction time Tr of the reverse polarity welding current necessary for cleaning can be minimized and the wear of the electrode can be reduced. At the same time, it is possible to obtain the same deep weld penetration shape as in the case of direct current positive polarity.

D、逆極性溶接電流の通電時間Trを0.5乃至3[m
s]の短時間にし、かつ逆極性溶接電流の波高値Irを
500[A]まで増大させることができ、逆極性電流の
通電時間Trが短時間であるにもかかわらず、充分なり
リーニング幅を確保することができる。
D. The conduction time Tr of the reverse polarity welding current is 0.5 to 3 [m
s], and the peak value Ir of the reverse polarity welding current can be increased to 500 [A], and even though the conduction time Tr of the reverse polarity current is short, the leaning width can be sufficiently maintained. can be secured.

E、前述したように、逆極性電流の通電時間Trを0.
5乃至3[ms]の短時間に設定しているので、逆極性
溶接電流の波高値!rを300[A]必要であり、それ
によってクリーニング作用を確保することができる。
E. As mentioned above, the conduction time Tr of the reverse polarity current is set to 0.
Since it is set to a short time of 5 to 3 [ms], the peak value of the reverse polarity welding current! r is required to be 300 [A], thereby ensuring the cleaning effect.

F、上記のように、正極性電流の通電時間9乃至15[
ms]と大きくし、また逆極性電流の通電時間を0.5
乃至3[ms]の短時間にして、交流電流の周波数を5
0乃至100 [Hz]にすることによって、溶接部の
溶は込みを大きくしアークの安定を向上させることがで
きる。
F. As mentioned above, the positive polarity current conduction time is 9 to 15[
ms] and the conduction time of the reverse polarity current to 0.5
The frequency of the alternating current is set to 5 for a short time of 3 [ms].
By setting the frequency to 0 to 100 [Hz], it is possible to increase the penetration of the welded part and improve the stability of the arc.

以上のように、本発明の溶接条件は、上記の各条件が互
いに関係して、一体となって、■適正なりリーニング幅
を確保した上で、■ビード幅が狭くて、■溶は込みが深
く、■電極の消耗を最小限にすることができる。
As described above, the welding conditions of the present invention are such that the above conditions are related to each other and work together to: 1) ensure an appropriate leaning width, 2) have a narrow bead width, and 2) prevent weld penetration. Deep ■Can minimize electrode wear.

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

第1図は、本発明の溶接方法により溶接したときの正極
性及び逆極性溶接電流の波高値Is。 I r (横軸)と、溶は込み深さPとビード幅Wとの
比P/W(縦軸)との関係を示す図である。 第2図は、本発明の溶接方法に使用する溶接電流の波高
値及び通電時間の4つのパラメタの定義を説明する図で
ある。 第3図は、本発明の溶接に使用する電極先端が両面傾斜
偏平形状の電極であって、同図(A)は正面図、同図(
B)は側面図であり、同図(C)は電極先端方向からみ
た平面図である。 第4図(A)及び(B)は、第2図に示す電極の先端か
ら発生するアークの広がりを示す図であって、それぞれ
正面図及び側面図を示す。 第5図(A)及び(B)は、それぞれ従来の方法及び本
発明の方法により溶接したときのビードの断面形状Bを
説明する図である。 第6図(A)は、溶接開始前の偏平電極の先端形状を示
す図、同図(B)は、通電休止をくり返し1時間通電後
の偏平電極の先端形状の変化状態を示す図、同図(C)
は、本発明の溶接方法と対比するための従来の尖頭丸形
電極の1時間aWS後の先端形状の変化状態を示す図で
ある。 第7図は、逆極性電流の通電時間Trをかえたときの溶
は込み深さPについて、本発明の溶接方法に使用する偏
平電極の場合(実線)及び対比のための尖頭丸形電極の
場合(点線)について示した線図である。 1・・・電極先端1aが両面傾斜偏平形状の非消耗電極
、Ll、L2・・・長辺方向、L・・・溶接線、Ir・
・・電極がプラス極性(逆極性)のときの溶接電流の波
高値 Tr・・・電極がプラス極性(逆極性)のときの溶接電
流の通電時間 Is・・・電極がマイナス極性(正極性)のときの溶接
電流の波高値 Ts・・・電極がマイナス極性(正極性)のときの溶接
電流の通電時間
FIG. 1 shows the peak values Is of positive polarity and reverse polarity welding currents when welding by the welding method of the present invention. It is a figure which shows the relationship between Ir (horizontal axis) and ratio P/W (vertical axis) of melt penetration depth P and bead width W (vertical axis). FIG. 2 is a diagram illustrating the definition of four parameters, the peak value of the welding current and the current application time, used in the welding method of the present invention. FIG. 3 shows an electrode whose tip used in welding according to the present invention has a flat shape with both sides inclined; FIG.
B) is a side view, and (C) is a plan view seen from the direction of the electrode tip. FIGS. 4A and 4B are diagrams showing the spread of an arc generated from the tip of the electrode shown in FIG. 2, and show a front view and a side view, respectively. FIGS. 5A and 5B are diagrams illustrating the cross-sectional shape B of the bead when welded by the conventional method and the method of the present invention, respectively. FIG. 6(A) is a diagram showing the shape of the tip of the flat electrode before welding starts, and FIG. Diagram (C)
FIG. 2 is a diagram showing a state of change in the tip shape of a conventional pointed round electrode after 1 hour of aWS for comparison with the welding method of the present invention. Figure 7 shows the penetration depth P when the current application time Tr of the reverse polarity current is changed in the case of a flat electrode used in the welding method of the present invention (solid line) and a pointed round electrode for comparison. It is a diagram shown about the case (dotted line). 1... Non-consumable electrode with electrode tip 1a having a flat shape with both sides inclined, Ll, L2... Long side direction, L... Welding line, Ir.
...The peak value Tr of the welding current when the electrode has positive polarity (reverse polarity)...The application time Is of the welding current when the electrode has positive polarity (reverse polarity)...The electrode has negative polarity (positive polarity) The peak value Ts of the welding current when the electrode is negative polarity (positive polarity) the welding current conduction time

Claims (1)

【特許請求の範囲】 1、アルミニウム合金の非消耗電極アーク溶接方法にお
いて、電極先端が両面傾斜偏平形状の非消耗電極を、そ
の電極先端の長辺方向と溶接線方向とが一致する方向に
配置して、前記非消耗電極とアルミニウム合金との間に
、略矩形波の交流電流を供給し、前記非消耗電極がプラ
ス極性のときに、溶接電流の波高値Irが300乃至5
00[A]で、かつ通電時間Trが0. 5〜3[ms]の逆極性電流を通電し、前記非消耗電極
がマイナス極性のときに溶接電流の波高値Isが150
乃至500[A]で、かつ通電時間Tsが9〜15[m
s]の正極性電流を通電して溶接するアルミニウム合金
の非消耗電極アーク溶接方法。
[Claims] 1. In a non-consumable electrode arc welding method for aluminum alloy, a non-consumable electrode whose tip has a flat shape with both sides inclined is arranged in a direction in which the long side direction of the electrode tip and the direction of the welding line coincide. Then, a substantially rectangular alternating current is supplied between the non-consumable electrode and the aluminum alloy, and when the non-consumable electrode has positive polarity, the peak value Ir of the welding current is 300 to 5.
00 [A] and the current application time Tr is 0. A reverse polarity current of 5 to 3 [ms] is applied, and when the non-consumable electrode has negative polarity, the peak value Is of the welding current is 150
to 500 [A] and the current application time Ts is 9 to 15 [m
A non-consumable electrode arc welding method for aluminum alloys, which involves welding by applying a positive current of [s].
JP21953589A 1989-08-25 1989-08-25 Non-consumable electrode arc welding method for aluminum alloy Expired - Fee Related JP2836112B2 (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP21953589A JP2836112B2 (en) 1989-08-25 1989-08-25 Non-consumable electrode arc welding method for aluminum alloy

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP21953589A JP2836112B2 (en) 1989-08-25 1989-08-25 Non-consumable electrode arc welding method for aluminum alloy

Publications (2)

Publication Number Publication Date
JPH0381071A true JPH0381071A (en) 1991-04-05
JP2836112B2 JP2836112B2 (en) 1998-12-14

Family

ID=16737008

Family Applications (1)

Application Number Title Priority Date Filing Date
JP21953589A Expired - Fee Related JP2836112B2 (en) 1989-08-25 1989-08-25 Non-consumable electrode arc welding method for aluminum alloy

Country Status (1)

Country Link
JP (1) JP2836112B2 (en)

Cited By (4)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JP2010005642A (en) * 2008-06-25 2010-01-14 Daihen Corp Ac plasma welding method
JP2010253533A (en) * 2009-04-28 2010-11-11 Bab-Hitachi Industrial Co Tig welding equipment
US8106327B2 (en) 2004-08-24 2012-01-31 Saipem S.P.A. ARC welding torch including a wire guide open on one side and arranged to receive a welding wire from a laterally spaced apart location and method of using same
JP2015202505A (en) * 2014-04-14 2015-11-16 株式会社アマダミヤチ Tig welding method and tig welding device

Cited By (4)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US8106327B2 (en) 2004-08-24 2012-01-31 Saipem S.P.A. ARC welding torch including a wire guide open on one side and arranged to receive a welding wire from a laterally spaced apart location and method of using same
JP2010005642A (en) * 2008-06-25 2010-01-14 Daihen Corp Ac plasma welding method
JP2010253533A (en) * 2009-04-28 2010-11-11 Bab-Hitachi Industrial Co Tig welding equipment
JP2015202505A (en) * 2014-04-14 2015-11-16 株式会社アマダミヤチ Tig welding method and tig welding device

Also Published As

Publication number Publication date
JP2836112B2 (en) 1998-12-14

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