JPS6249146B2 - - Google Patents
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- Publication number
- JPS6249146B2 JPS6249146B2 JP53065528A JP6552878A JPS6249146B2 JP S6249146 B2 JPS6249146 B2 JP S6249146B2 JP 53065528 A JP53065528 A JP 53065528A JP 6552878 A JP6552878 A JP 6552878A JP S6249146 B2 JPS6249146 B2 JP S6249146B2
- Authority
- JP
- Japan
- Prior art keywords
- molten pool
- welding
- magnetic field
- aluminum
- dcsp
- 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
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- Arc Welding Control (AREA)
Description
【発明の詳細な説明】
この発明は、アルミニウムのDCSP―TIG溶接
における欠陥防止法に関する。DETAILED DESCRIPTION OF THE INVENTION The present invention relates to a method for preventing defects in DCSP-TIG welding of aluminum.
この明細書において、アルミニウムとは純アル
ミニウムとアルミニウム合金の両者を含むものと
する。また左回転および右回転というのは、トー
チ側からみた方向をいう。 In this specification, aluminum includes both pure aluminum and aluminum alloys. Further, left rotation and right rotation refer to directions seen from the torch side.
アルミニウムのDCSP―TIG溶接は、MIG溶接
や交流TIG溶接に比べてビード幅が狭くかつ深い
溶け込みが得られる高能率溶接法として注目され
ているが、アルミニウム独特の表面の酸化皮膜の
存在により他の溶接法ではみられない変形ブロ
ー・ホールおよび羽毛状晶が発生し、継手性能に
悪影響を及ぼすばかりか、羽毛状晶はX線透過写
真上に解析像を発生させるため、非破壊検査上の
障害にもなるという欠点がある。 DCSP-TIG welding of aluminum is attracting attention as a highly efficient welding method that can achieve a narrower bead width and deeper penetration than MIG welding or AC TIG welding, but due to the presence of an oxide film on the surface unique to aluminum, other methods Deformation blow holes and feather-like crystals that are not seen with welding methods occur, which not only adversely affects joint performance, but also poses an obstacle to non-destructive testing because feather-like crystals generate analytical images on X-ray photographs. It also has the disadvantage of becoming
変形ブロー・ホールは、溶接条件や開先部の前
処理を検討することにより解消可能であるが、そ
の溶接条件範囲は非常に狭く実用上問題が多い
し、羽毛状晶は溶接条件を変化させても解消する
ことは困難である。 Deformed blow holes can be eliminated by considering welding conditions and groove pretreatment, but the range of welding conditions is very narrow and there are many practical problems, and feathery crystals can be eliminated by changing welding conditions. However, it is difficult to eliminate it.
この発明の目的は、アルミニウムのDCSP―
TIG溶接に生ずる上記特有の欠陥防止する方法を
提供することにある。 The purpose of this invention is to
The object of the present invention is to provide a method for preventing the above-mentioned defects that occur in TIG welding.
上記の目的を達成するために、この発明による
アルミニウムのDCSP―TIG溶接における欠陥防
止法は、アルミニウムのDCSP―TIG溶接にあた
り、溶融池に、この溶融池を流れる溶接電流に直
交する成分をもち周波数が2〜15Hzの交番磁界を
与え、ローレンツ力により溶融池を左右交互に回
転させて撹拌することを特徴とするものである。 In order to achieve the above object, the method for preventing defects in DCSP-TIG welding of aluminum according to the present invention is to provide a method for preventing defects in DCSP-TIG welding of aluminum. applies an alternating magnetic field of 2 to 15 Hz, and the molten pool is stirred by rotating left and right alternately by Lorentz force.
この発明につき、以下図面を参照して説明す
る。 This invention will be explained below with reference to the drawings.
第1図において、1はTIGトーチ、2はその電
極、3は溶接アーク、4はアルミニウム被溶接
材、5は被溶接材4を介してTIGトーチ1に対向
せしめられたコイル鉄芯で、これに磁界発生コイ
ル6が巻かれている。7はコイル6に交番電流を
供給する電源である。 In Fig. 1, 1 is a TIG torch, 2 is its electrode, 3 is a welding arc, 4 is an aluminum material to be welded, and 5 is a coil iron core that is opposed to the TIG torch 1 through the material to be welded 4. A magnetic field generating coil 6 is wound around. 7 is a power source that supplies an alternating current to the coil 6.
上記において、被溶接材4をDCSP―TIG溶接
により第3図および第4図に示すように矢印18
方向に突合わせ溶接する。8はその溶接金属、9
は溶融池で、コイル6に交番電流が供給せられる
ことにより鉄芯5から発生した磁力線10が被溶
接材4を貫通し、溶融池9に交番磁界を与える。
このさい溶接電流11は、第3図に矢印で示され
ているように、アーク3の直下に集中するが、磁
力線10を横切ることになるため、ローレンツ力
により溶融池9は第4図に矢印19で示されてい
るように回転し、撹拌される。溶融池9に与える
のは、交番磁界であるため、第4図の回転方向は
つぎに反転せられ、以後回転方向が左回転と右回
転と交互に変化して回転を繰返すことになる。 In the above, the material to be welded 4 is welded by DCSP-TIG welding as shown by the arrow 18 in FIGS. 3 and 4.
Butt weld in the direction. 8 is the weld metal, 9
is a molten pool, and when an alternating current is supplied to the coil 6, magnetic lines of force 10 generated from the iron core 5 penetrate the material to be welded 4 and apply an alternating magnetic field to the molten pool 9.
At this time, the welding current 11 is concentrated directly below the arc 3, as shown by the arrow in FIG. Rotate and stir as shown at 19. Since an alternating magnetic field is applied to the molten pool 9, the direction of rotation shown in FIG. 4 is then reversed, and thereafter the direction of rotation alternates between left rotation and right rotation, and the rotation is repeated.
上記コイル6は鉄芯5に巻付けられ、トーチ1
に対向せしめられているが、コイル6をトーチ1
に巻付けても交番磁界を溶融池9に与えることが
できる。 The coil 6 is wound around the iron core 5, and the torch 1
The coil 6 is placed opposite the torch 1.
An alternating magnetic field can be applied to the molten pool 9 even if the wire is wound around the molten pool 9.
交番磁界の周波数を2〜15Hzに限定したのは、
つぎの理由による。すなわち、周波数が2Hz未満
では、左右交互の回転速度が遅いために溶融池が
充分に撹拌せられず、また15Hzを超えると、逆に
左右交互の回転速度が速すぎて充分に溶融池が撹
拌せられないからである。第8図a〜gは、アル
ミニウム被溶接材として、JIS、5083P―0を使
用し、溶接速度300mm/min、溶接電流220Aで
DCSP―TIG溶接を行なうにあたり、溶融池に、
この溶融池を流れる溶接電流に直交する成分をも
ち周波数が0.2Hz、5Hz、10Hz、15Hz、20Hzおよ
び30Hzの交番磁界をそれぞれ与え、ローレンツ力
により、溶融池を左右に交互に回転させた場合の
各溶接金属の表面マクロ組織を示す。 The reason why the frequency of the alternating magnetic field is limited to 2 to 15 Hz is because
This is due to the following reasons. In other words, if the frequency is less than 2Hz, the molten pool will not be stirred sufficiently because the rotation speed of the left and right alternations is slow, and if it exceeds 15Hz, the molten pool will not be sufficiently stirred because the rotation speed of the left and right alternations is too fast. This is because they cannot be forced to do so. In Figure 8 a to g, JIS, 5083P-0 was used as the aluminum material to be welded, welding speed was 300 mm/min, and welding current was 220 A.
When performing DCSP-TIG welding, in the molten pool,
An alternating magnetic field with a component perpendicular to the welding current flowing through this molten pool and frequencies of 0.2Hz, 5Hz, 10Hz, 15Hz, 20Hz, and 30Hz is applied, respectively, and the molten pool is rotated alternately left and right by Lorentz force. The surface macrostructure of each weld metal is shown.
第8図aは周波数0、すなわち溶融池に交番電
流を与えず、したがつて溶融池を全く撹拌しない
従来例を示すものであつて、溶接金属の表面には
羽毛状晶が明瞭に認められる。同図c〜eの周波
数が5Hz、10Hzおよび15Hzの場合は、溶融池が撹
拌されて結晶が微細化し、その結果羽毛状晶が発
生していない。同図fおよびgの周波数が20Hzお
よび30Hzの場合は、溶融池が充分撹拌されないた
め、羽毛状晶の存在が認められる。同図bの周波
数2Hzの場合は、羽毛状晶の存在は認められな
い。しかしながら、溶接金属の表面デイツプル状
態からみて周波数2Hz未満では溶融池が充分に撹
拌されないことを同図は物語つている。 Figure 8a shows a conventional example where the frequency is 0, that is, no alternating current is applied to the molten pool, and therefore the molten pool is not stirred at all, and feather-like crystals are clearly observed on the surface of the weld metal. . When the frequencies c to e in the same figure are 5 Hz, 10 Hz, and 15 Hz, the molten pool is stirred and the crystals become finer, and as a result, no feathery crystals are generated. When the frequencies f and g in the figure are 20 Hz and 30 Hz, the molten pool is not sufficiently stirred, and the presence of feather-like crystals is observed. In the case of a frequency of 2 Hz as shown in Figure b, the presence of feathered crystals is not recognized. However, from the surface dimple state of the weld metal, the figure shows that the molten pool is not sufficiently stirred at a frequency of less than 2 Hz.
以上のように、第8図から周波数が2〜15Hzの
範囲内において溶融池の撹拌効果があり、なかで
も5〜10Hzが優れていることが分かる。 As described above, it can be seen from FIG. 8 that there is an effect of stirring the molten pool within the frequency range of 2 to 15 Hz, and that 5 to 10 Hz is particularly excellent.
つぎに、シールドガスとしてのHeに、とくに
ブロー・ホールを発生させ易くするため、0.5%
H2ガスを含有させ、上記と同条件でDCSP―TIG
溶接を行なつた。このさい溶融池に交番磁界を与
えなかつた場合の溶接金属の表面状態を第9図
イ、同横断面を同図ロとしてそれぞれ写真で示
す。また溶融池に周波数5Hzの交番磁界を与えた
場合の溶接金属の表面状態を第10図イに、同横
断面を同図ロにそれぞれ写真で示す。第9図イ,
ロでは、ブロー・ホールの存在が明瞭に認めら
れ、第10図イ,ロでは、溶融池の撹拌効果によ
りブロー・ホールの溶接金属からの放出が促進さ
れたためブロー・ホールの発生はほとんど認めら
れない。 Next, we added 0.5% to He as a shielding gas to make it easier to generate blow holes.
DCSP-TIG containing H2 gas and under the same conditions as above.
Performed welding. The surface condition of the weld metal when no alternating magnetic field was applied to the molten pool at this time is shown in photographs in FIG. 9A, and the cross section thereof is shown in FIG. 9B. Furthermore, the surface condition of the weld metal when an alternating magnetic field with a frequency of 5 Hz is applied to the molten pool is shown in Fig. 10A, and the cross section thereof is shown in Fig. 10B, respectively. Figure 9 A,
In Figure 10 (B), the existence of blow holes is clearly recognized, and in Figure 10 (A) and (B), the generation of blow holes is hardly recognized because the release of blow holes from the weld metal is promoted by the stirring effect of the molten pool. do not have.
なお、通常のDCSP―TIG溶接では、上記のよ
うに多量のH2ガスが含まれることはなく、ブロ
ー・ホールの発生の多くの原因は、溶接開先の汚
れや酸化皮膜の巻込みによるものであるため、ブ
ロー・ホールは変形状に現われる。 Note that normal DCSP-TIG welding does not contain large amounts of H 2 gas as mentioned above, and blow holes are often caused by dirt in the welding groove or entrainment of oxide film. Therefore, the blow hole appears in a deformed shape.
この発明によれば、アルミニウムのDCSP―
TIG溶接にあたり、上述のように溶融池に交番磁
界を与え、ローレンツ力により溶融池を左右交互
に回転させて撹拌するものであるから、アルミニ
ウム独特の酸化皮膜の存在に起因する変形ブロ
ー・ホールは溶接金属以外に放出されるか、少な
くとも許容範囲内の丸い形状のブロー・ホールと
なされる。また羽毛状晶は、一方向の回転による
溶融池の撹拌ではその発生を防止することはでき
ないが、左右交互の回転の繰返しによる撹拌で結
晶粒が微細化し、その発生が抑制される。 According to this invention, DCSP of aluminum
During TIG welding, as mentioned above, an alternating magnetic field is applied to the molten pool, and the molten pool is rotated alternately left and right by Lorentz force to stir it, so deformation blow holes due to the presence of an oxide film unique to aluminum are avoided. It is ejected outside the weld metal, or at least forms a blow hole with an acceptable round shape. Furthermore, although the generation of feather-like crystals cannot be prevented by stirring the molten pool by rotation in one direction, the crystal grains become finer by stirring by repeating rotations alternating left and right, thereby suppressing their generation.
ところで、アルミニウムのDCSP―TIG溶接で
は、その溶接電流が増大すると、その理由は明確
ではないが、溶接電流が磁界を生じ、溶融池が右
回転する現象が生じる。その結果、第5図に示さ
れているように、ビード12に変形が生じ、溶接
進行方向に向つて右側にアンダー・カツト13が
生じる。 By the way, in DCSP-TIG welding of aluminum, when the welding current increases, the welding current generates a magnetic field, which causes the molten pool to rotate clockwise, although the reason is not clear. As a result, as shown in FIG. 5, the bead 12 is deformed and an undercut 13 is created on the right side in the direction of welding progress.
しかしながら、この発明の実施例では、溶融池
に与える交番磁界が、とくに溶接電流の増大にと
もなつて発生する溶融池に対する右回転力を左回
転力によつて相殺する非平衡交番磁界となすこと
により、第5図に鎖線20で示されているような
適正なビード形状を得る。 However, in the embodiment of the present invention, the alternating magnetic field applied to the molten pool is a non-balanced alternating magnetic field in which the clockwise rotational force on the molten pool, which occurs as the welding current increases, is canceled out by the counterclockwise rotational force. As a result, a proper bead shape as shown by the chain line 20 in FIG. 5 is obtained.
非平衡な交番電流を発生させるには、第6図お
よび第7図に示されているように、交番電流にお
いてたとえば正の時間t1を負の時間t2より長くす
るか、正の電流値A1を負の電流値A2より大きく
すればよい。もちろんこれらの逆の場合もあり得
るわけで、要するに左回転を行なう磁界を発生す
る極性の時間を長くするか、電流値を大きくすれ
ばよい。電源電流波形は図示のように矩形波が一
般的であるが、これに限らない。 To generate an unbalanced alternating current, for example, in the alternating current the positive time t 1 is made longer than the negative time t 2 or the positive current value It is sufficient to make A 1 larger than the negative current value A 2 . Of course, the opposite case is also possible, and in short, the polarity time for generating the magnetic field for counterclockwise rotation may be lengthened or the current value may be increased. Although the power supply current waveform is generally a rectangular wave as shown in the figure, it is not limited to this.
第1図はこの発明の方法を示す全体側面図、第
2図は同要部の拡大縦断面図、第3図および第4
図は同要部の平面図で、第3図は溶接電流の状態
を示し、第4図は溶融池の撹拌状態を示す。第5
図はビードの状態を示す横断面図、第6図および
第7図はそれぞれ非平衡交番電流の波形を示す
図、第8図a〜gは溶融池に与える交番磁界の周
波数を種々変化させた場合における羽毛状晶発生
の有無を示す溶接金属の平面図、第9図イおよび
ロは溶融池に交番磁界を与えなかつた場合にブロ
ーホールが発生している状態を示す溶接金属の平
面図および横断面図、第10図イおよびロは溶融
池に周波数5Hzの交番磁界を与えた場合に、ブロ
ー・ホールが発生しない状態を示す溶接金属の平
面図および横断面図である。
1…TIGトーチ、4…アルミニウム被溶接材、
6…磁界発生コイル、9…溶融池。
Fig. 1 is an overall side view showing the method of the present invention, Fig. 2 is an enlarged vertical cross-sectional view of the main parts, Figs.
The figure is a plan view of the main part, FIG. 3 shows the state of welding current, and FIG. 4 shows the state of stirring of the molten pool. Fifth
The figure is a cross-sectional view showing the state of the bead, Figures 6 and 7 are diagrams each showing the waveform of a nonequilibrium alternating current, and Figures 8 a to g show the results of various changes in the frequency of the alternating magnetic field applied to the molten pool. Figures 9A and 9B are plan views of weld metal showing the presence or absence of feather-like crystals in the case where blowholes are generated when no alternating magnetic field is applied to the molten pool; 10A and 10B are a plan view and a cross-sectional view of the weld metal showing a state in which no blow holes are generated when an alternating magnetic field with a frequency of 5 Hz is applied to the molten pool. 1... TIG torch, 4... Aluminum material to be welded,
6... Magnetic field generating coil, 9... Molten pool.
Claims (1)
溶融池に、この溶融池を流れる溶接電流に直交す
る成分をもち周波数が2〜15Hzの交番磁界を与
え、ローレンツ力により溶融池を左右交互に回転
させて撹拌することを特徴とするアルミニウムの
DCSP―TIG溶接における欠陥防止法。1 For DCSP-TIG welding of aluminum,
An aluminum alloy that is characterized by applying an alternating magnetic field to the molten pool with a component perpendicular to the welding current flowing through the molten pool and having a frequency of 2 to 15 Hz, and stirring the molten pool by rotating the molten pool alternately left and right by Lorentz force.
DCSP - Defect prevention method in TIG welding.
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP6552878A JPS54155954A (en) | 1978-05-30 | 1978-05-30 | Deffective prevention in aluminum dcspp tig welding |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP6552878A JPS54155954A (en) | 1978-05-30 | 1978-05-30 | Deffective prevention in aluminum dcspp tig welding |
Publications (2)
| Publication Number | Publication Date |
|---|---|
| JPS54155954A JPS54155954A (en) | 1979-12-08 |
| JPS6249146B2 true JPS6249146B2 (en) | 1987-10-17 |
Family
ID=13289594
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP6552878A Granted JPS54155954A (en) | 1978-05-30 | 1978-05-30 | Deffective prevention in aluminum dcspp tig welding |
Country Status (1)
| Country | Link |
|---|---|
| JP (1) | JPS54155954A (en) |
Families Citing this family (2)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| JPS5739077A (en) * | 1980-08-15 | 1982-03-04 | Mitsubishi Heavy Ind Ltd | Arc welding method |
| JPS6117372A (en) * | 1984-07-03 | 1986-01-25 | Mitsubishi Heavy Ind Ltd | Magnetic agitation horizontal position welding |
-
1978
- 1978-05-30 JP JP6552878A patent/JPS54155954A/en active Granted
Also Published As
| Publication number | Publication date |
|---|---|
| JPS54155954A (en) | 1979-12-08 |
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