JPH01241392A - Composite welding method using tig and laser beam - Google Patents
Composite welding method using tig and laser beamInfo
- Publication number
- JPH01241392A JPH01241392A JP63067895A JP6789588A JPH01241392A JP H01241392 A JPH01241392 A JP H01241392A JP 63067895 A JP63067895 A JP 63067895A JP 6789588 A JP6789588 A JP 6789588A JP H01241392 A JPH01241392 A JP H01241392A
- Authority
- JP
- Japan
- Prior art keywords
- tig
- laser
- laser beam
- nozzle
- welding
- 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
Links
- 238000003466 welding Methods 0.000 title claims abstract description 30
- 239000002131 composite material Substances 0.000 title claims description 7
- 238000000034 method Methods 0.000 title claims description 7
- 229910000831 Steel Inorganic materials 0.000 claims abstract description 3
- 239000010959 steel Substances 0.000 claims abstract description 3
- 239000000463 material Substances 0.000 claims description 5
- 230000035515 penetration Effects 0.000 abstract description 13
- 239000007789 gas Substances 0.000 description 16
- 230000000694 effects Effects 0.000 description 5
- 230000007423 decrease Effects 0.000 description 4
- 238000010586 diagram Methods 0.000 description 4
- 238000010521 absorption reaction Methods 0.000 description 2
- 230000005540 biological transmission Effects 0.000 description 2
- 230000002301 combined effect Effects 0.000 description 2
- 230000003287 optical effect Effects 0.000 description 2
- 239000011324 bead Substances 0.000 description 1
- 238000007796 conventional method Methods 0.000 description 1
- 238000009826 distribution Methods 0.000 description 1
- 238000011156 evaluation Methods 0.000 description 1
- 238000002474 experimental method Methods 0.000 description 1
- 239000001307 helium Substances 0.000 description 1
- 229910052734 helium Inorganic materials 0.000 description 1
- SWQJXJOGLNCZEY-UHFFFAOYSA-N helium atom Chemical compound [He] SWQJXJOGLNCZEY-UHFFFAOYSA-N 0.000 description 1
- 239000011261 inert gas Substances 0.000 description 1
- 230000001678 irradiating effect Effects 0.000 description 1
- 238000004519 manufacturing process Methods 0.000 description 1
- 239000000155 melt Substances 0.000 description 1
- 238000002844 melting Methods 0.000 description 1
- 230000008018 melting Effects 0.000 description 1
- 238000003825 pressing Methods 0.000 description 1
- 238000012545 processing Methods 0.000 description 1
- WFKWXMTUELFFGS-UHFFFAOYSA-N tungsten Chemical compound [W] WFKWXMTUELFFGS-UHFFFAOYSA-N 0.000 description 1
- 229910052721 tungsten Inorganic materials 0.000 description 1
- 239000010937 tungsten Substances 0.000 description 1
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
- B23K26/00—Working by laser beam, e.g. welding, cutting or boring
- B23K26/346—Working by laser beam, e.g. welding, cutting or boring in combination with welding or cutting covered by groups B23K5/00 - B23K25/00, e.g. in combination with resistance welding
- B23K26/348—Working by laser beam, e.g. welding, cutting or boring in combination with welding or cutting covered by groups B23K5/00 - B23K25/00, e.g. in combination with resistance welding in combination with arc heating, e.g. TIG [tungsten inert gas], MIG [metal inert gas] or plasma welding
Landscapes
- Physics & Mathematics (AREA)
- Optics & Photonics (AREA)
- Engineering & Computer Science (AREA)
- Plasma & Fusion (AREA)
- Mechanical Engineering (AREA)
- Arc Welding In General (AREA)
- Laser Beam Processing (AREA)
Abstract
Description
【発明の詳細な説明】
（産業上の利用分野）
本発明は高エネルギービームとアークを併用した溶接方
法に関するものである。DETAILED DESCRIPTION OF THE INVENTION (Field of Industrial Application) The present invention relates to a welding method that uses a high-energy beam and an arc in combination.
（従来の技術）
ＴＩＧ （Ｔｕｎｇｓｔｅｎ ＩｎｅｒｔＧａｓ ＡＲ
Ｃ）とレーザの複合溶接法の従来技術として、例えば特
公昭５６−４９１９５号に記載の方法があげられる。こ
れにおいては、レーザ光を照射する部分をあらかじめＴ
ＩＧで溶融させておくことにより吸収率を上げ、溶は込
みを深めることがその主旨となるが、これは必しもレー
ザとＴＩＧノズルの位置関係等の諸条件を適切に定めた
ものではない。例えば複合溶接の際レーザノズルとＴＩ
Ｇ電極の間隔を大きくしすぎると複合効果は低下する。(Conventional technology) TIG (Tungsten InertGas AR
As a conventional technique of a combined welding method using C) and a laser, for example, there is a method described in Japanese Patent Publication No. 56-49195. In this case, the part to be irradiated with the laser beam is set in advance at T.
The main idea is to increase the absorption rate and deepen the penetration by melting with IG, but this does not necessarily mean that various conditions such as the positional relationship between the laser and the TIG nozzle are properly determined. . For example, when performing composite welding, the laser nozzle and TI
If the gap between the G electrodes is too large, the combined effect will be reduced.
またサイドから吹くガスの流量が大きすぎても同様に複
合効果が低下する等複合効果による深溶は込み溶接実現
の安定性・再現性に問題があった。Furthermore, if the flow rate of the gas blown from the side is too large, the composite effect similarly decreases, causing problems in the stability and reproducibility of deep penetration welding due to the composite effect.
（発明が解決しようとする課題）
このような問題は複合溶接時に発生するプラズマの位置
・大きさが安定しないことに帰因する。そこで、本発明
はレーザノズルとＴＩＧ電極の位置関係、ガスの流量な
どの具体的条件設定を行うことにより、最適なプラズマ
条件およびそのプラズマを安定して実現できるレーザと
ＴＩＧの複合溶接方法を提供することを目的とする。(Problems to be Solved by the Invention) Such problems are attributable to the fact that the position and size of plasma generated during composite welding are not stable. Therefore, the present invention provides a combined laser and TIG welding method that can stably achieve optimal plasma conditions and plasma by setting specific conditions such as the positional relationship between the laser nozzle and the TIG electrode and the flow rate of gas. The purpose is to
（課題を解決するための手段）
以上の問題点をふまえ、本発明は、レーザとＴＩＧを併
用した鋼材の溶接に於て、レーザノズルのレーザ放出穴
の内径Ｄ１を４ｍｍ以上８ｍｍ以下にし同外径を００を
１５ｍｍ以上にし、さらにレーザノズルの中心とＴＩＧ
電極電極間端間Ｉ１１ρを２＋＋＋ｎ以上５ｎ＋ｍ以下
にすること、またはこれらの条件の他にＴＩＧシールド
ガスの流量を５１／ｍｉｎ以上２０Ｊ：ｌ／ｍｉｎ以下
にすることにより、与えられたレーザパワー、ＴＩＧパ
ワー、溶接速度のもとで溶込みに寄与するレーザエネル
ギーを最大にして、最大溶造みを得ることを特徴とする
ものである。(Means for Solving the Problems) In view of the above-mentioned problems, the present invention aims to set the inner diameter D1 of the laser emission hole of the laser nozzle to 4 mm or more and 8 mm or less when welding steel materials using a combination of laser and TIG. Set the diameter of 00 to 15 mm or more, and also align the center of the laser nozzle with the TIG
The given laser power, TIG It is characterized by maximizing the laser energy contributing to penetration under the power and welding speed to obtain the maximum welding depth.
（作 用） 以下図面に基づいて本発明の詳細な説明する。(For writing) The present invention will be described in detail below based on the drawings.
第１図は本発明にもとすくノズル部分の概略図である。FIG. 1 is a schematic diagram of a nozzle portion according to the present invention.
図中、レーザノズルの内径をＤＩ。In the figure, the inner diameter of the laser nozzle is DI.
外径をり。、レーザノズル中心とＴｒＧ’ｔ＋ｆｆｌ先
端との水平距離をｌ、レーザガス（センターガス）流量
をｆｃ、ＴＩＧガス（サイドガス）流量をｆｓとする。Measure the outer diameter. , the horizontal distance between the center of the laser nozzle and the tip of TrG't+ffl is l, the laser gas (center gas) flow rate is fc, and the TIG gas (side gas) flow rate is fs.
さて、ここで最も重要なことは、溶は込みの大きさは溶
接時に発生するプラズマと密接な関係があるという事で
ある。即ち発生するプラズマがある程度大きければそれ
だけレーザ光の吸収も大きくなりその分だけ溶接に寄与
するエネルギーを奪うことになる。またプラズマがＴＩ
Ｇ電極からある程度前れたとこにできるとＴＩＧによる
溶融部がレーザエネルギーを吸収する前に凝固すること
になり、複合効果が低下する。そこでＤｒ 、 Ｄｏ
、 Ｉｌ、、 ｆｃ 。Now, the most important thing here is that the size of the penetration is closely related to the plasma generated during welding. That is, the larger the generated plasma is to a certain extent, the greater the absorption of laser light, and the more energy that contributes to welding is taken away. Also, plasma is TI
If it is formed at a certain distance from the G electrode, the melted part caused by TIG will solidify before absorbing the laser energy, reducing the composite effect. So Dr. Do
, Il,, fc.
ｆ、を変えることにより溶接部における種々のガス圧分
布を実現し、これによってプラズマの位置、大ぎさを制
御する事を考える。以上の考えに基づいて実験を行った
ところ以下の事が判明した。Consider realizing various gas pressure distributions in the welding zone by changing f, and thereby controlling the position and magnitude of the plasma. Based on the above idea, we conducted an experiment and found the following.
■ レーザノズルの内径ＤＩ とプラズマ、溶は込み深
さの関係を調べたところ、Ｄ、が増加するとともにプラ
ズマの大きさは単調に減少し、かつ熔は込みも深くなる
傾向にあり、レーザノズル内径４ｍｍ以上で両者とも安
定する。■ When we investigated the relationship between the inner diameter DI of the laser nozzle, the plasma, and the depth of penetration, we found that as D increases, the size of the plasma decreases monotonically, and the depth of the melt tends to become deeper. Both are stable when the inner diameter is 4 mm or more.
■ レーザノズルの外径り。とプラズマ、溶は込み深さ
の関係を調べたところＤｏが１５ｍｍ未満ではプラズマ
の大きさにばらつぎがあるが、１５１ｕＩ１１以上でそ
の大きさは単調に減少し、かつ溶は込みも深くなる傾向
にあり、Ｄｏ＝２０ｍｍ以上で両者とも安定する。■ Laser nozzle outer diameter. When we investigated the relationship between plasma and penetration depth, we found that when Do is less than 15 mm, the plasma size varies, but when it is 151 uI or more, the size decreases monotonically and the penetration depth tends to become deeper. Both are stable when Do=20 mm or more.
■ レーザノズル中心とＴＩＧ電極先端との水平距＠Ｉ
１．とプラズマ溶は込み深さの関係を調べたところ１＝
２〜５ｍｍでプラズマはＴＩＧ電極電極引き寄せられ、
塁が５ｍｍ超ではＴＩＧ電極から離れていく傾向にある
。一方溶は込み深さはプラズマが離れてゆくとともに小
さくなる。■ Horizontal distance between the center of the laser nozzle and the tip of the TIG electrode @I
1. When we investigated the relationship between and the depth of plasma melt penetration, we found that 1=
Plasma is attracted to the TIG electrode at 2 to 5 mm,
If the base exceeds 5 mm, it tends to move away from the TIG electrode. On the other hand, the penetration depth becomes smaller as the plasma moves away.
■ 丁ＩＧガス流量ｆＳが２０ Ｉｔ ／ ｍｉｎ超に
なるとＴＩＧ’を極からプラズマが離れる事によって溶
は込み深さの減少が起こる。■ When the TIG gas flow rate fS exceeds 20 It/min, the plasma separates from the TIG' pole, causing a decrease in the penetration depth.
なお、本結果はレーザパワー８ｋＷ（一定）、ＴＩＧ’
を流１００ Ａ （一定）、溶接速度８ｍ／ｍ１ｎ（一
定）ノズル先端からワークまでの距離１０ｍｍ等の条件
で行い、得られたものであるが他の条件においても同様
の結果が得られることが確かめられている。なお、溶込
みの評価は厚さ３ｍｍの５ＵＳ３０４の平板で行い、加
工ガスはレーザガス、ＴＩＧガスともにヘリウムガスを
使用した。Note that this result is based on a laser power of 8 kW (constant) and TIG'
The results were obtained under conditions such as a flow rate of 100 A (constant), a welding speed of 8 m/m1 n (constant), and a distance of 10 mm from the nozzle tip to the workpiece, but similar results can be obtained under other conditions. It has been confirmed. The evaluation of penetration was performed using a 5US304 flat plate with a thickness of 3 mm, and helium gas was used as the processing gas for both laser gas and TIG gas.
以上の知見に基づいてレーザノズルの内径を４ｍｍ以上
に設定した。またノズル内径を大きくしすぎることによ
るガスの損失を考えて上限を８ｍｌ１１以下とした。ま
た上記■の事実に基づいてレーザノズルの外径り。１５
ｍｍ以上に設定した。上限は他の装置との接触かない限
り、特に制限はない。上記■の事実に基づいてレーザノ
ズルの中心とＴＩＧ を極光端間の距ｆｆ１ｌｔ ｕを
２ｍｍ以上５ｍｍ以下に設定した。さらに上記■の事実
に基づいてＴＩＧシールドガス流量を２０ｊ２／ｍｉｎ
以下に設定した。またガス流量を小さくしすぎることに
よるＴｌＧｇ極の消耗を考えて下限を５ｌ／ｍｉｎにし
た。Based on the above knowledge, the inner diameter of the laser nozzle was set to 4 mm or more. Further, in consideration of gas loss caused by making the nozzle inner diameter too large, the upper limit was set to 8 ml or less. Also, the outer diameter of the laser nozzle is determined based on the above fact. 15
mm or more. There is no particular upper limit as long as there is no contact with other devices. Based on the fact (2) above, the distance ff1ltu between the center of the laser nozzle and the extreme light end of the TIG was set to 2 mm or more and 5 mm or less. Furthermore, based on the above fact, the TIG shielding gas flow rate is set to 20j2/min.
It was set as below. In addition, in consideration of consumption of the TlGg electrode due to a too small gas flow rate, the lower limit was set to 5 l/min.
（実 施 例） 以下に、本発明を用いて造管を行った例を示す。(Example) An example of pipe making using the present invention will be shown below.
第２図は造管ラインの概略図である。レーザ発振器３か
ら出たレーザビームは、ミラー８−、、ｌ１１４により
その方向を変えた後レンズ６によって集光されレーザノ
ズル１から溶接部へと照射される。FIG. 2 is a schematic diagram of the pipe production line. The laser beam emitted from the laser oscillator 3 changes its direction by mirrors 8-, 114, is focused by a lens 6, and is irradiated from the laser nozzle 1 to the welding area.
第３図はレーザノズル部分の拡大図である。FIG. 3 is an enlarged view of the laser nozzle portion.
レーザノズル部分はＴＩＧ トーチ２の先端部と一体化
されており、両者の位置関係およびレーザノズルの内径
、外径は本発明に基づいて設定しであるノズルから出た
レーザビーム１１はＴＩＧアーク１２により溶融された
部分に照射されるようになっている。一方、第２図にお
いて被溶接バイブ９は造管方向にスリット１０が入って
いる。The laser nozzle part is integrated with the tip of the TIG torch 2, and the positional relationship between the two and the inner and outer diameters of the laser nozzle are set based on the present invention. The molten part is irradiated by the irradiation. On the other hand, in FIG. 2, the to-be-welded vibrator 9 has a slit 10 in the pipe-making direction.
溶接時はスクイズロール５−１＋ ５−２により左右
から押しつける事によってスリットの両サイドを密着さ
せ、密着部に真上からレーザビームおよびＴＩＧアーク
を照射し溶接を行った。During welding, both sides of the slit were brought into close contact by pressing from the left and right sides with squeeze rolls 5-1 + 5-2, and welding was performed by irradiating the adhered portion with a laser beam and a TIG arc from directly above.
溶接条件は次の通りである、
厚さ３ｍｍ
■レーザ発振器：リングモード（Ｍ＝１．５）パワー８
ｋＷ
■レーザノズル：内径４ｍｍ、外径２０ｍｍ、レーザガ
ス）Ｉｅ ４０ Ｉｌ／ Ｔｎｉｎ■造管速度：８ｍ／
ｍｉｎ
■ノズル先端からバイブ表面までの距離１０＋ｎｍ
以上の条件により欠陥のない溶接ビードが高速かつ安定
に得られた。Welding conditions are as follows, thickness 3mm ■Laser oscillator: ring mode (M=1.5) power 8
kW ■Laser nozzle: inner diameter 4mm, outer diameter 20mm, laser gas) Ie 40 Il/Tnin ■Pipe-making speed: 8m/
min ■Distance from the nozzle tip to the vibrator surface is 10+nm or more A defect-free weld bead was obtained quickly and stably.
（発明の効果）
以上から、本発明を用いると、プラズマの位置、大きさ
を、レーザエネルギーが溶接部に対して最も大きく寄与
するように、かつ複合効果が最も大きくなるように設定
出来る。(Effects of the Invention) As described above, by using the present invention, the position and size of the plasma can be set so that the laser energy makes the largest contribution to the welded part and the combined effect becomes the largest.
そして、このような最適複合条件のもとで溶接を行うと
、溶込みが最大になり溶接部の品質が飛躍的に向上する
等の顕著な効果がある。When welding is performed under such optimal combined conditions, there are remarkable effects such as maximum penetration and a dramatic improvement in the quality of the welded part.
第１図はレーザノズル先端部およびＴＩＧＩ−−チ先瑞
部を示した側面図、
又、第２図は本発明の実施態様例を示した概略図、第３
図は同じく本発明を実施した際のノズル部分の概略図で
ある。
１・・・レーザノズル ２・・・ＴＩＧ トーチ３・
・・レーザ発振器 ４・・・ＴＩＧ溶接機５・・・ス
クイズロール ６・・・レンズ。
７・・・光路ダクト ８・・・伝送ミラー９・・・
溶接バイブ１０・・・スリット１１・・・レーザビーム
１２・・・ＴＩＧアーク１３・・・ワーク
１４・・・被溶接材の移動方向
第１図
１：レーザノズル
２：ＴＩＧｌ−−チ
１４：被溶接材の移動方向
第２図
５、スクイズロール
６ レンズ
７ 光路ダクト
８、伝送ミラー
９ ／８接パイプ
ＩＱ・スリット
１１ レーザビーム
１４ 肢ｆｄ接材の移動方向FIG. 1 is a side view showing the tip of the laser nozzle and the TIGI tip part, FIG. 2 is a schematic diagram showing an embodiment of the present invention, and FIG.
The figure is also a schematic diagram of the nozzle portion when the present invention is implemented. 1... Laser nozzle 2... TIG torch 3.
...Laser oscillator 4...TIG welding machine 5...Squeeze roll 6...Lens. 7... Optical path duct 8... Transmission mirror 9...
Welding vibrator 10...Slit 11...Laser beam 12...TIG arc 13...Workpiece 14...Movement direction of welded material Direction of movement of welding material Fig. 2 5, Squeeze roll 6 Lens 7 Optical path duct 8, Transmission mirror 9 /8 contact pipe IQ/slit 11 Laser beam 14 Direction of movement of limb FD welding material
Claims (1)
ザノズルのレーザ放出穴の内径Ｄ＿１を４ｍｍ以上８ｍ
ｍ以下にし同外径Ｄ＿０を１５ｍｍ以上にし、さらにレ
ーザノズルの中心とＴＩＧ電極先端間の距離ｌを２ｍｍ
以上５ｍｍ以下にして溶接することを特徴とするレーザ
とＴＩＧの複合溶接方法。 ２ ＴＩＧシールドガスの流量を５ｌ／ｍｉｎ以上２０
ｌ／ｍｉｎ以下にすることを特徴とする請求項１記載の
レーザとＴＩＧの複合溶接方法。[Claims] 1. In welding steel materials using a combination of laser and TIG, the inner diameter D_1 of the laser emission hole of the laser nozzle is 4 mm or more and 8 m.
m or less, and the outer diameter D_0 is 15 mm or more, and the distance l between the center of the laser nozzle and the tip of the TIG electrode is 2 mm.
A composite welding method using laser and TIG, characterized in that the welding is performed with a thickness of 5 mm or less. 2 Increase the flow rate of TIG shielding gas to 5l/min or more20
2. The combined laser and TIG welding method according to claim 1, wherein the welding rate is 1/min or less.
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP63067895A JPH01241392A (en) | 1988-03-22 | 1988-03-22 | Composite welding method using tig and laser beam |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP63067895A JPH01241392A (en) | 1988-03-22 | 1988-03-22 | Composite welding method using tig and laser beam |
Publications (2)
| Publication Number | Publication Date |
|---|---|
| JPH01241392A true JPH01241392A (en) | 1989-09-26 |
| JPH0451271B2 JPH0451271B2 (en) | 1992-08-18 |
Family
ID=13358088
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP63067895A Granted JPH01241392A (en) | 1988-03-22 | 1988-03-22 | Composite welding method using tig and laser beam |
Country Status (1)
| Country | Link |
|---|---|
| JP (1) | JPH01241392A (en) |
Cited By (6)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| WO1995010386A1 (en) * | 1993-10-11 | 1995-04-20 | Fraunhofer-Gesellschaft zur Förderung der angewandten Forschung e.V. | Process and device for the laser-beam machining of workpieces |
| WO2001076806A1 (en) * | 2000-04-10 | 2001-10-18 | Mitsubishi Heavy Industries, Ltd. | Welding system |
| WO2003024658A1 (en) * | 2001-09-17 | 2003-03-27 | Honda Giken Kogyo Kabushiki Kaisha | Work welding method |
| US6683268B2 (en) * | 2000-05-31 | 2004-01-27 | L'air Liquide-Societe Anonyme A Directoire Et Conseil De Surveillance Pour L'etude Et L'exploitation Des Procedes Georges Claude | Application of a hybrid arc/laser process to the welding of pipe |
| CN104191092A (en) * | 2014-08-06 | 2014-12-10 | 沈阳富创精密设备有限公司 | Laser-TIG composite wire filling seal welding method for L-shaped aluminum alloy structure |
| US9061374B2 (en) | 2010-03-08 | 2015-06-23 | Kobe Steel, Ltd. | Laser/arc hybrid welding method and method for producing welded member using same |
Citations (1)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| JPS60106688A (en) * | 1983-11-16 | 1985-06-12 | Hitachi Ltd | Laser working device |
-
1988
- 1988-03-22 JP JP63067895A patent/JPH01241392A/en active Granted
Patent Citations (1)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| JPS60106688A (en) * | 1983-11-16 | 1985-06-12 | Hitachi Ltd | Laser working device |
Cited By (10)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| WO1995010386A1 (en) * | 1993-10-11 | 1995-04-20 | Fraunhofer-Gesellschaft zur Förderung der angewandten Forschung e.V. | Process and device for the laser-beam machining of workpieces |
| WO2001076806A1 (en) * | 2000-04-10 | 2001-10-18 | Mitsubishi Heavy Industries, Ltd. | Welding system |
| US6600133B2 (en) | 2000-04-10 | 2003-07-29 | Mitsubishi Heavy Industries, Ltd. | Welding system |
| US6683268B2 (en) * | 2000-05-31 | 2004-01-27 | L'air Liquide-Societe Anonyme A Directoire Et Conseil De Surveillance Pour L'etude Et L'exploitation Des Procedes Georges Claude | Application of a hybrid arc/laser process to the welding of pipe |
| WO2003024658A1 (en) * | 2001-09-17 | 2003-03-27 | Honda Giken Kogyo Kabushiki Kaisha | Work welding method |
| GB2384455A (en) * | 2001-09-17 | 2003-07-30 | Honda Motor Co Ltd | Work welding method |
| GB2384455B (en) * | 2001-09-17 | 2005-08-24 | Honda Motor Co Ltd | Work welding process |
| US7015417B2 (en) | 2001-09-17 | 2006-03-21 | Honda Giken Kogyo Kabushiki Kaisha | Workpiece welding process |
| US9061374B2 (en) | 2010-03-08 | 2015-06-23 | Kobe Steel, Ltd. | Laser/arc hybrid welding method and method for producing welded member using same |
| CN104191092A (en) * | 2014-08-06 | 2014-12-10 | 沈阳富创精密设备有限公司 | Laser-TIG composite wire filling seal welding method for L-shaped aluminum alloy structure |
Also Published As
| Publication number | Publication date |
|---|---|
| JPH0451271B2 (en) | 1992-08-18 |
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