JPS5961576A - Resistance welding of pipe - Google Patents
Resistance welding of pipeInfo
- Publication number
- JPS5961576A JPS5961576A JP16974582A JP16974582A JPS5961576A JP S5961576 A JPS5961576 A JP S5961576A JP 16974582 A JP16974582 A JP 16974582A JP 16974582 A JP16974582 A JP 16974582A JP S5961576 A JPS5961576 A JP S5961576A
- Authority
- JP
- Japan
- Prior art keywords
- pipe
- welding
- welded
- electrode
- 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.)
- Granted
Links
- 238000003466 welding Methods 0.000 title claims abstract description 84
- 238000000034 method Methods 0.000 claims description 5
- 239000000463 material Substances 0.000 description 15
- 238000012360 testing method Methods 0.000 description 11
- 230000000694 effects Effects 0.000 description 8
- 230000020169 heat generation Effects 0.000 description 4
- 230000005856 abnormality Effects 0.000 description 2
- 239000010953 base metal Substances 0.000 description 2
- 239000003795 chemical substances by application Substances 0.000 description 2
- 239000012141 concentrate Substances 0.000 description 2
- 238000002788 crimping Methods 0.000 description 2
- 239000012530 fluid Substances 0.000 description 2
- 238000010438 heat treatment Methods 0.000 description 2
- 238000009527 percussion Methods 0.000 description 2
- XLYOFNOQVPJJNP-UHFFFAOYSA-N water Substances O XLYOFNOQVPJJNP-UHFFFAOYSA-N 0.000 description 2
- 229910000831 Steel Inorganic materials 0.000 description 1
- 239000003990 capacitor Substances 0.000 description 1
- 238000007796 conventional method Methods 0.000 description 1
- 238000001816 cooling Methods 0.000 description 1
- 238000005336 cracking Methods 0.000 description 1
- 230000007423 decrease Effects 0.000 description 1
- 239000000428 dust Substances 0.000 description 1
- 238000005516 engineering process Methods 0.000 description 1
- 238000002474 experimental method Methods 0.000 description 1
- 230000004907 flux Effects 0.000 description 1
- 238000005286 illumination Methods 0.000 description 1
- 229910001234 light alloy Inorganic materials 0.000 description 1
- 230000013011 mating Effects 0.000 description 1
- 238000002844 melting Methods 0.000 description 1
- 230000008018 melting Effects 0.000 description 1
- 239000002184 metal Substances 0.000 description 1
- 238000012545 processing Methods 0.000 description 1
- 238000011160 research Methods 0.000 description 1
- 239000011343 solid material Substances 0.000 description 1
- 239000010959 steel Substances 0.000 description 1
- 238000003860 storage Methods 0.000 description 1
- 230000001052 transient effect Effects 0.000 description 1
- 230000037303 wrinkles Effects 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
- B23K11/00—Resistance welding; Severing by resistance heating
- B23K11/08—Seam welding not restricted to one of the preceding subgroups
- B23K11/082—Seam welding not restricted to one of the preceding subgroups of three-dimensional seams
Landscapes
- Engineering & Computer Science (AREA)
- Mechanical Engineering (AREA)
- Butt Welding And Welding Of Specific Article (AREA)
- Resistance Welding (AREA)
Abstract
Description
【発明の詳細な説明】
この発明はパイプの抵抗溶接法に関し、はソ直角に切っ
たパイプの切断端を相手側のパイプ胴又は板曲に確実に
溶接するものである。DETAILED DESCRIPTION OF THE INVENTION The present invention relates to a pipe resistance welding method, which reliably welds the cut end of a pipe cut at a right angle to a mating pipe body or bent plate.
抵抗溶接には点溶接、シーム溶接、プロジェクション溶
接、ハツト溶接、フラッシュ溶接・パーカッション溶接
がある。そのどの溶接法によっても、パイプ切断端のは
ソ全1酉を相手側のパイプ嗣又は板曲に確実に溶接でき
る方法はない。その必要がある場合、アーク溶接による
ほかなかった。Resistance welding includes spot welding, seam welding, projection welding, heart welding, flash welding, and percussion welding. No matter which welding method is used, there is no way to reliably weld the entire length of the cut end of the pipe to the pipe heir or bent plate on the other side. If that was necessary, arc welding was the only option.
点溶接、シーム溶接は重ね溶接であるから目的が違う。Spot welding and seam welding have different purposes because they are lap welds.
プロジェクション溶接は最初に接触した突起(プロジェ
クション)に溶接面、流が集中して、そこだけ溶着する
もので、パイプ全1Mの一部しか溶接できない。バット
溶接は棒端をFli伺け、表皮を外周へ押出して芯部の
高熱部をfl:、着させるのであるから、パイプ端同士
ならよいが、パイプ端とパイプ胴の溶接は考えられなか
った。In projection welding, the welding surface and flow concentrate on the first protrusion (projection) that comes into contact, and welding occurs only there, so only a portion of the 1M pipe can be welded. Butt welding involves attaching the ends of the rod, extruding the outer skin to the outer periphery, and attaching the high-temperature part of the core, so it would be fine to weld the ends of the pipe together, but welding the ends of the pipe and the pipe body was unthinkable. .
フラッシュ溶接もパイプ端同士の突合溶接には使えるが
、パイプ端と板面との溶接には使えない。Flash welding can also be used for butt welding pipe ends, but it cannot be used for welding pipe ends to plate surfaces.
パーカッション溶接は小さな突起を瞬間溶融し圧着する
もので、パイプ端の全周溶接には使えない。Percussion welding involves instantly melting and crimping small protrusions, and cannot be used to weld the entire circumference of pipe ends.
以上が溶接技術者の常識的見解である。The above is the common sense opinion of welding engineers.
本発明は上記の難問を解決すべく、約−年間の研究、実
験の結果、遂に目的を達成した。同時に直流抵抗溶接に
おける発熱現象は!極の(+)(−)によシ大きな差異
を生ずるという重大な事実をつかんだ。アーク溶接にお
けるアークの加熱カフ5(tIIN性に左右される現象
は昔から知られている。しかし、アークを生じない抵抗
溶接にも、これほどの極性効果があるとは驚くべき事で
あった。従来、抵抗溶接用電源は、一部、省エネルギー
、軽合金点溶接用として直流ill源が用いられている
だけで、はとんど交流1!源であったためこの現象が分
らなかったのである。The present invention has finally achieved its purpose after about several years of research and experimentation to solve the above-mentioned difficult problem. At the same time, what is the heat generation phenomenon in DC resistance welding? We discovered the important fact that there is a large difference between the polarities (+) and (-). The heating cuff of the arc in arc welding5 (tIIN) has been known for a long time.However, it was surprising that resistance welding, which does not generate an arc, had such a polarity effect. Conventionally, power sources for resistance welding have only used DC illumination sources for energy saving and spot welding of light alloys, and have mostly been AC 1! sources, so this phenomenon has not been understood. .
この発明の(1沈要をまず述べると、はy軸に直角に切
ったパイプ切断端を相手側パイプ胴又は板面に当て、直
流抵抗溶接機の(−)電極を上記パイプ切断端側、(+
)電極を上記パイプ胴又は板面側に接続し、溶接電流を
流しながら両者を圧着することを特徴とするパイプの抵
抗溶接法である。First, to explain the main points of this invention, place the cut end of the pipe cut perpendicularly to the y-axis against the pipe body or plate surface of the other party, and place the (-) electrode of the DC resistance welding machine on the cut end side of the pipe. (+
) This is a resistance welding method for pipes, which is characterized in that an electrode is connected to the pipe body or the plate side, and the two are crimped while flowing a welding current.
次に図面を参照して、この発明の実施態様を説明する。Next, embodiments of the present invention will be described with reference to the drawings.
第1.2図は整流式直流抵抗溶接機の下側電極により溶
接物である小径側パイプユを垂直姿勢でクランプし、そ
の上端に大径側パイプ/の胴を水平姿勢で載せ、そのパ
イプ胴を上部1!極3により圧下しつ\溶接通電する実
施例を示す。Figure 1.2 shows the welding object, the small-diameter pipe, being clamped in a vertical position by the lower electrode of a rectifying DC resistance welding machine, and the large-diameter pipe being placed on the upper end in a horizontal position. Top 1! An example is shown in which the welding current is applied while the electrode 3 is being pressed down.
そのグ、3はバイプコをつかむ固定t%と可aの電極、
7は可動電極用動用流体圧シリンダ、6は上部電極3を
駆動する流体圧シリンダ、Sは従来の交流電源変圧器に
替わる整流素子つき変圧器である。3 is a fixed t% and a flexible electrode that grips the vipco,
7 is a working fluid pressure cylinder for the movable electrode, 6 is a fluid pressure cylinder for driving the upper electrode 3, and S is a transformer with a rectifying element in place of a conventional AC power transformer.
第3〜6図は第1.2図の溶接物の両パイプl、コだけ
取出し、その溶接前後の状態を示す。Figures 3 to 6 show the welded pipes 1 and 1 of Figure 1.2 taken out and their states before and after welding.
第3,4図のようにパイプ/の胴にパイプコの切断端を
当て、溶接電流を流すと、最初から接触している二点に
電流が集中して流れ、小さな溶着部りを生ずる。バイブ
/胴倶1は熱容量が大で、パイグー先端側はこれに比し
熱容量が小である。このように熱容量に差があるものを
溶接するには従来コンデンサー蓄勢式市、源又は交流電
、源で大熱容量側も瞬間的に溶接温度に達する瞬間大電
流を流すと同時に圧着する方法が用いられている。As shown in Figures 3 and 4, when the cut end of the pipe is applied to the body of the pipe and welding current is applied, the current flows concentrated at the two points that are in contact from the beginning, creating a small weld. The vibrator/body 1 has a large heat capacity, and the tip of the pie goo has a small heat capacity in comparison. In order to weld materials with such differences in heat capacity, conventional methods have been used, such as a capacitor storage type, power source, or AC power source, in which a large current is applied instantaneously to reach the welding temperature on the high heat capacity side of the source, and crimping is performed at the same time. It is being
しかし、第3.4図のような直角切断したま\のパイプ
一端の溶接は瞬間大電流の通電で最初の接触部が飛散し
良好な溶着部が得られぬためこれを防止する目的でバイ
プコ端面を潰し九抄胴に適合する形に加工して抵抗溶接
が行なわれている例もあるが、それでも比較的肉厚が厚
く外径の小さいパイプ同士の組合せに限られて居る。However, when welding one end of a pipe that has been cut at right angles as shown in Figure 3.4, the initial contact part will scatter due to the application of a large instantaneous current, making it impossible to obtain a good weld. In some cases, resistance welding has been performed by crushing the end face and processing it into a shape that fits the nine-piece barrel, but even then, this is limited to the combination of pipes with relatively thick walls and small outer diameters.
この発明によれば、パイプlを(+)を極、パイブコを
(−)電、極につ力ぎ交流電源の場合より少い溶接電流
を流す。するとパイグーの接触端は飛散することなく軟
化して最初は第4図9,9のような小さな溶着部を生じ
、上部電極3の降下につれ円弧状溶着面積が左右へ広が
り、第6図のように、はソ全固を溶着し得るのである。According to this invention, the pipe 1 is connected to the (+) terminal, and the pipe is connected to the (-) terminal, so that a smaller welding current is passed than in the case of an AC power supply. Then, the contact end of the pie goo softens without scattering, and at first a small welded area as shown in Fig. 4, 9 is formed, and as the upper electrode 3 descends, the arc-shaped welded area expands to the left and right, and as shown in Fig. 6. Therefore, it is possible to weld completely solid materials.
なお、パイプ/がバイプコよυ充分に木ければ完全な全
周溶接となるが、直径の差が小さいほど第6図の不溶着
部IOかや\大きく残る(外見上は分らない)。とれは
溶接物の形状からやむを得ないが、強度的には全く間頌
でない。Note that if the pipe is sufficiently woody, it will be completely welded all around, but the smaller the difference in diameter, the larger the unwelded part IO in Figure 6 will remain (it cannot be seen from the outside). Although cracking is unavoidable due to the shape of the welded product, it is not an improvement at all in terms of strength.
強度試験のためパイプl側を固定し、パイプλ側を押倒
すと、溶接部でなく、これに隣接したパイプ母材か切れ
るのである。For a strength test, when the pipe L side is fixed and the pipe λ side is pushed down, not the welded part but the adjacent pipe base material breaks.
次にこの発明の実験データと同じ溶接物を在来の交流抵
抗溶接機によって溶接したW1合とを示す。Next, the experimental data of the present invention and the W1 case obtained by welding the same welded object using a conventional AC resistance welding machine are shown.
(I)〈溶接物ン 材 質 外径 肉厚パ
イプ/ S TKM 22,1m O,9關パ
イプ、Z 12,7 0.9く溶接条件
〉 加圧力 溶接電流 通電時間350ky
18000A 11 Hzく試験結果〉引張強度
破断筒所
1900kg 母材
なお交流電源では全く溶着しなかった。(I)〈Welded object Material Outer diameter Thick walled pipe/STKM 22.1m O.9 pipe, Z 12.7 0.9 Welding conditions〉 Pressure welding current Welding time 350ky
18000A 11 Hz test results〉Tensile strength
The broken tube weighed 1900 kg and the base material did not weld at all with AC power supply.
(■)<溶接物〉 材 質 外 径 肉厚
ノくイブ/ STKM 2 B、61nll
j、27111パイプコ # 22.2
1.2く溶接条件〉 加圧力 溶接電流 通電
時間本発明 450kg22000A 11 Hz交
流WL源 450 kl 26500 A 1
5 Hzく試験結果〉 引張強度 破断筒所
本発明 2500ky 母材
交流電源 700 溶接部
(■)<溶接物〉 材 質 外 径 肉厚
パイプ/ STKM 34mm 2.3mm
パイプ、2 21.7 1.9く溶接条
件〉 加圧力 溶接電流 通電時間本発明
1500kg27000A 15Hz交流電源
1500 54000 1M〈試験結果〉
引張強度 破断箇所本発明 3500kg
母材
交流雷1源 2500ky 溶接部パイプ端を
パイプ胴に溶接する上記実施例に比べると、パイプ端を
平板面に溶接するのは、この発明によればさらに容易に
なる。次の実験データは第7図のパイプと平板の溶接で
ある。(■) <Welded object> Material Outer diameter Thick walled tube/STKM 2 B, 61nll
j, 27111 Pipeco # 22.2
1.2 Welding conditions> Pressure force Welding current Current application time Invention 450 kg 22000 A 11 Hz AC WL source 450 kl 26500 A 1
5 Hz test results> Tensile strength Breaking tube location Invention 2500ky Base metal AC power supply 700 Welded part (■) <Welded product> Material Outer diameter Thick pipe/STKM 34mm 2.3mm
Pipe, 2 21.7 1.9 Welding conditions> Pressure welding current Current application time Invention
1500kg27000A 15Hz AC power supply
1500 54000 1M〈Test results〉
Tensile strength Break point: Invention 3500kg
Base metal AC lightning source 1 source 2500 ky Welding part Compared to the above embodiment in which the pipe end is welded to the pipe body, according to the present invention, it is easier to weld the pipe end to the flat plate surface. The next experimental data is the welding of the pipe and flat plate shown in Figure 7.
(■)く溶接物〉 材 質 外 径 肉厚平
板/a 5PCC1゜2mm
バイプコ STKM 25.4*am 1.2〈
溶接条件〉 加圧力 溶接電流 通電時間50
0 kg 500[]OA 13 Hz〈
試験結果〉 引張強度 破断筒所
2000kg 母材
なお交流電源では平板la側にプロジェクションを作ら
ないかぎり溶接不能。(■) Welded product> Material Outer diameter Thickness flat plate/a 5PCC1゜2mm Vipco STKM 25.4*am 1.2〈
Welding conditions〉 Pressure force Welding current Current application time 50
0 kg 500[]OA 13 Hz〈
Test results〉 Tensile strength: 2000 kg at fracture tube Base material: With AC power source, welding is not possible unless a projection is made on the flat plate la side.
次の実験データは第8図の角パイプ/hと丸バイプコと
の溶接である。なお以下の実験はすべて交流電源では溶
接不能。The next experimental data is the welding of the square pipe/h and the round pipe in Fig. 8. In addition, all of the following experiments cannot be welded using an AC power source.
(■)<溶接物ン 材 質 外 径 肉厚角
パイプ/b 5TKR21mm(角)16龍パイプコ
If 19 1.6〈溶接条件〉
加圧力 溶接部、流 通電時間5[[kg240[
]OA 6 Hz〈試験結果〉 引張強度 破断
筒所
2400ky 母材
次の実験データは第9図の角バイブ/bと蓋板10との
溶接である。(■) <Welded object Material Outer diameter Thick square pipe/b 5TKR21mm (square) 16 dragon pipe If 19 1.6 <Welding conditions>
Pressure force Welding part, flow Current application time 5 [[kg240[
] OA 6 Hz <Test results> Tensile strength Breaking tube 2400ky Base material The following experimental data is the welding of the square vibrator/b and the cover plate 10 in FIG.
(■)く溶接物〉 材質 寸 法 肉厚角
イ(イブ/ b 5TKR20X20+n+++
1.2mrA蓋板10 5PCC20X30
1.2く溶接条件〉 加圧力 溶接電流 通電時
間450ky21000A 6Hz
く試験結果〉 引張強度 水圧試験320ky
5ky/cr/lで異常なし次の実験データは第10
図のバイブ/Cと蓋板10の溶接でおる。(■) Welded item〉 Material Dimensions Thickness square A (Eve/b 5TKR20X20+n+++
1.2mrA cover plate 10 5PCC20X30
1.2 Welding conditions〉 Pressure force Welding current Current conduction time 450ky21000A 6Hz Test results〉 Tensile strength Water pressure test 320ky
No abnormality at 5ky/cr/l The next experimental data is the 10th
The vibrator/C shown in the figure and the cover plate 10 are welded together.
(■)く溶接物〉 材 質 外径 内厚バ
イブ/c STKM 2B、4龍 12關蓋
板/θ 5PCC2B 1.6〈溶接条件
〉 加圧力 溶接電流 通電時間400 kp
20000A 6 Hz〈試験結果ン 引張強
度 水圧試験450kg 5ky/dで異常な
し次の実験データは第11図の角パイプ/b相互のT形
溶接である。(■) Welded object> Material Outer diameter Inner thickness Vibe/c STKM 2B, 4 dragons 12 cap plate/θ 5PCC2B 1.6 <Welding conditions> Pressure force Welding current Current conduction time 400 kp
20000A 6 Hz (Test results) Tensile strength Water pressure test 450 kg 5 ky/d No abnormality The next experimental data is the T-shaped welding of square pipes/b in Fig. 11.
閏)く溶接物〉 材質 寸法 肉厚角パイ
プ/ d 5TKR21X21?IIII+ 1.
6mm角パイプ/g 5TKR19X19郵 1,6
1く溶接条件〉 加圧力 溶接電流 通電時間60
0kg 2500OA、 7 Hz〈試験結
果〉 引張強度 破断筒所
1500ky 母材
このように従来の交流電源溶接機では全く溶接不能の溶
接対象を、申分のない強度で抵抗溶接できる。仁の発明
が電源を直流とし、パイプ端側を(−)、その相手側を
(+) !極に接続しただけで、このように優れた効果
をあげ得た原因を考案すると、次のような点があげられ
る。Welded parts〉 Material Dimensions Thick walled square pipe/d 5TKR21X21? III+ 1.
6mm square pipe/g 5TKR19X19 1,6
1. Welding conditions> Pressure force Welding current Current application time 60
0kg 2500OA, 7Hz <Test results> Tensile strength Breaking tube 1500ky Base material In this way, welding objects that cannot be welded at all with conventional AC power welding machines can be resistance welded with perfect strength. Jin's invention uses DC as the power source, with the end of the pipe being (-) and the other end being (+)! If we consider the reasons why we were able to achieve such excellent results simply by connecting to the poles, we can think of the following points.
(α) 交流電源は周期的に電流値が零になり発熱し々
い冷却期間があるが、直流電源では電流値は零になるこ
とがないので溶接部は連続した発熱が得られる。(α) With an AC power source, the current value periodically drops to zero and there is a cooling period during which heat is generated, but with a DC power source, the current value never drops to zero, so the welded part generates continuous heat.
(h) 直流電流のピンチ効果($束性)により1t
1流が一点に集中しようとするので局部集中加熱がはか
れ、発熱効果が優れている。(h) 1t due to the pinch effect of DC current ($ flux)
Since the first stream tends to concentrate at one point, localized heating is achieved, and the heat generation effect is excellent.
<c> 通電時、交流t′fIでは過度電流(定常電
流の2〜3倍値)が流れるが、直流電源では過渥菫流が
発生しないのと、溶接突合せ部の接触抵抗が働き、電流
は自動的に最初は低く、順次大きくなって行くため初期
チリ(溶融金属の飛散)を防げると共に、必要溶接皺流
が自己制イ卸される。<c> When energizing, a transient current (2 to 3 times the steady current) flows with AC t'fI, but with a DC power supply, excessive current does not occur, and the contact resistance of the welded butt works, so that the current decreases. is automatically low at first and gradually increases, thereby preventing initial dust (scattering of molten metal) and self-controlling the necessary welding wrinkle flow.
(d) 直流電源の極性による発熱の差異の利用。(d) Use of differences in heat generation due to polarity of DC power supply.
以上が相乗的に働いて、パイプ端のT形溶接のような熱
容量が大きく異る溶接対象を、上記実施例のように広い
範囲ではソ完全な抵抗溶接が可能になったのであろう。The above may work synergistically to make perfect resistance welding possible over a wide range of welding targets with greatly different heat capacities, such as T-welds at the ends of pipes, as in the above example.
同じく直流′電源を用いても、この発明の電極接続法の
逆、つまりパイプ端側を(+)、相手側を(−)につ匁
ぐと、この発明の効果は全く得られない。Similarly, even if a direct current power source is used, if the electrode connection method of the present invention is reversed, that is, the pipe end side is connected to (+) and the other side is connected to (-), the effects of this invention cannot be obtained at all.
なお、との発明の実施態様は図示した例に限らず、丸パ
イプ、各種角パイプの切断端をT形溶接と力るようバイ
ブ胴、平板、曲げ板、湾曲板等に溶接する場合、すべて
に適用できる。溶接物は鋼に限らない。直流電源は通常
、整流式を用いる事にガるが、これに限るわけでない。Note that the embodiments of the invention are not limited to the illustrated example, but can be applied to any case where the cut ends of round pipes and various square pipes are welded to a vibrator body, flat plate, bent plate, curved plate, etc. such as T-shaped welding. Applicable to Welded objects are not limited to steel. A rectifier type DC power source is usually used, but it is not limited to this.
この発明は1關未満の肉厚の薄肉パイプ端でさえ、他の
パイプ胴、板面にはソ全周抵抗溶接できるという抵抗溶
接技術上、革命的成果をあげた。また抵抗溶接において
も、アーク溶接における極性効果同様、極性効果を活用
して熱容量界る両溶接物の発熱を均衡させ得ることを実
証し、直流電源を用いる事により抵抗溶接の用途を大き
く広げる道を開いた。This invention achieved a revolutionary result in resistance welding technology in that even the end of a thin pipe with a wall thickness of less than 1 inch can be resistance welded all around to other pipe bodies and plate surfaces. In addition, in resistance welding, we demonstrated that it is possible to use the polarity effect to balance the heat generation of both welding materials, which have different heat capacities, just like the polarity effect in arc welding, and we found a way to greatly expand the applications of resistance welding by using a DC power source. I opened it.
直流電源と極性効果により、直角切断しただけのパイプ
端を平らな面だけでなく、曲面、屈曲面にでも−そのま
\押し准んで、はソ全IWI溶接できる事は、生産性向
上効果大である。しかも安定した高品質の溶接部を得ら
れる。そして使用する電流値は交流1!源に比べ20%
減となるので、省エネルギ効果も大きい。Using the DC power supply and polarity effect, the end of a pipe cut at right angles can be welded not only on flat surfaces, but also on curved and bent surfaces. It is. Moreover, stable and high quality welds can be obtained. And the current value used is AC 1! 20% compared to the source
The energy saving effect is also significant.
第1.2図はこの発明の一実施態様を示す正面及び側面
図、第5.4図は第1.2図の溶接物である両パイプの
溶接開始時の関係位置を示す立面図と平面図、第5.6
図は同じく溶接完了時の立面図と平面図、第7〜11図
はこの発明を適用した各種形状の溶接物の斜視図である
。
l・・・胴側バイブ、コ・・・切断端側バイブ、3・・
・(→電極、ダ、3・・・(→電極。
特許出願人 日本溶接機株式会社
囮 代理人 弁理士 福 1)弐 通 ′−人ふ・
同 代理人 弁理士 福 1)賢 三 X4、
−7ノFigure 1.2 is a front and side view showing one embodiment of the present invention, and Figure 5.4 is an elevational view showing the relative positions of both pipes, which are the welded objects in Figure 1.2, at the start of welding. Plan view, Section 5.6
The figures are also an elevation view and a plan view when welding is completed, and Figures 7 to 11 are perspective views of welded products of various shapes to which the present invention is applied. L... Torso side vibe, K... Cut end side vibe, 3...
・(→electrode, da, 3...(→electrode. Patent applicant Nippon Welding Co., Ltd. Decoy Agent Patent attorney Fuku 1) Nitō ′-Hitofu・ Same agent Patent attorney Fuku 1) Kenzo X4,
-7ノ
Claims (1)
は板面に当て、直流抵抗溶接機の(−)電極を上記パイ
プ切断端側、(→電極を上記パイプ胴又は板曲側に接続
し、溶接電流を流しながら両者を正嫡することを特徴と
するパイプの抵抗溶接法。Place the cut end of the pipe cut perpendicular to the axis on the pipe body or plate surface of the other party, and place the (-) electrode of the DC resistance welding machine on the cut end side of the pipe, (→Place the electrode on the curved side of the pipe body or plate side) A resistance welding method for pipes, which is characterized by connecting them and making them legitimate while flowing welding current.
Priority Applications (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP16974582A JPS6055231B2 (en) | 1982-09-30 | 1982-09-30 | Pipe resistance welding method |
Applications Claiming Priority (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP16974582A JPS6055231B2 (en) | 1982-09-30 | 1982-09-30 | Pipe resistance welding method |
Publications (2)
Publication Number | Publication Date |
---|---|
JPS5961576A true JPS5961576A (en) | 1984-04-07 |
JPS6055231B2 JPS6055231B2 (en) | 1985-12-04 |
Family
ID=15892055
Family Applications (1)
Application Number | Title | Priority Date | Filing Date |
---|---|---|---|
JP16974582A Expired JPS6055231B2 (en) | 1982-09-30 | 1982-09-30 | Pipe resistance welding method |
Country Status (1)
Country | Link |
---|---|
JP (1) | JPS6055231B2 (en) |
-
1982
- 1982-09-30 JP JP16974582A patent/JPS6055231B2/en not_active Expired
Also Published As
Publication number | Publication date |
---|---|
JPS6055231B2 (en) | 1985-12-04 |
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