JPH0438513B2 - - Google Patents
Info
- Publication number
- JPH0438513B2 JPH0438513B2 JP12900885A JP12900885A JPH0438513B2 JP H0438513 B2 JPH0438513 B2 JP H0438513B2 JP 12900885 A JP12900885 A JP 12900885A JP 12900885 A JP12900885 A JP 12900885A JP H0438513 B2 JPH0438513 B2 JP H0438513B2
- Authority
- JP
- Japan
- Prior art keywords
- welding
- electrode
- electrodes
- bead
- pipe
- 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
Links
- 238000003466 welding Methods 0.000 claims description 64
- 238000004519 manufacturing process Methods 0.000 claims description 21
- 238000000034 method Methods 0.000 claims description 17
- 229910052719 titanium Inorganic materials 0.000 claims description 8
- 229910001069 Ti alloy Inorganic materials 0.000 claims description 4
- 238000005452 bending Methods 0.000 claims 1
- 239000011324 bead Substances 0.000 description 27
- 239000010936 titanium Substances 0.000 description 21
- 239000002184 metal Substances 0.000 description 17
- 229910052751 metal Inorganic materials 0.000 description 17
- 230000007547 defect Effects 0.000 description 7
- 238000009826 distribution Methods 0.000 description 5
- 230000000630 rising effect Effects 0.000 description 4
- 239000010935 stainless steel Substances 0.000 description 4
- 229910001220 stainless steel Inorganic materials 0.000 description 4
- 239000000463 material Substances 0.000 description 3
- 230000035515 penetration Effects 0.000 description 3
- 229910000831 Steel Inorganic materials 0.000 description 2
- RTAQQCXQSZGOHL-UHFFFAOYSA-N Titanium Chemical compound [Ti] RTAQQCXQSZGOHL-UHFFFAOYSA-N 0.000 description 2
- 238000010586 diagram Methods 0.000 description 2
- 239000007789 gas Substances 0.000 description 2
- 239000000047 product Substances 0.000 description 2
- 239000010959 steel Substances 0.000 description 2
- 229910045601 alloy Inorganic materials 0.000 description 1
- 239000000956 alloy Substances 0.000 description 1
- QVGXLLKOCUKJST-UHFFFAOYSA-N atomic oxygen Chemical compound [O] QVGXLLKOCUKJST-UHFFFAOYSA-N 0.000 description 1
- 230000015556 catabolic process Effects 0.000 description 1
- 239000012141 concentrate Substances 0.000 description 1
- 230000000694 effects Effects 0.000 description 1
- 239000012467 final product Substances 0.000 description 1
- 238000010438 heat treatment Methods 0.000 description 1
- 239000001301 oxygen Substances 0.000 description 1
- 229910052760 oxygen Inorganic materials 0.000 description 1
- 238000012805 post-processing Methods 0.000 description 1
- 238000004513 sizing Methods 0.000 description 1
- 238000007711 solidification Methods 0.000 description 1
- 230000008023 solidification Effects 0.000 description 1
- 230000008961 swelling Effects 0.000 description 1
Landscapes
- Arc Welding In General (AREA)
Description
[産業上の利用分野]
本発明は、TIG溶接により高速でTiまたはTi
合金管を製造する方法に関し、詳細には溶湯の盛
上りによる溶接の中断やハンピングビードの発生
等の問題を起こすことなく高速でTiまたはTi合
金管を製造する方法に関するものである。
[従来の技術]
Ti又はTi合金(以下Tiという)管を製造する
に当たつては、例えば第3図に示す様にアンコイ
ラー1に巻かれたTi製帯板Fを駆動ローラ2の
間に供給して矢印方向に送給し、基台K上で水平
方向に回転するブレークダウンローラ3、フイン
パスローラ4およびスクイズローラ5によつて
Ti製帯板Fを湾曲させ、端面同士を突合せて該
突合せ端部を溶接機7により溶接する。そして
Ti管はさらにサイジングローラ6へ供給して所
定の外径に仕上げられる。尚上記Ti管製造工程
における溶接機として単電極がTIG溶接機が使用
されている。
ところで上記製造方法において生産性を高めよ
うとすると、造管速度を高める必要があり、また
高速で走行するTi製帯板に対する溶接が十分な
溶込み得るものでなければならないので溶接点に
大きな溶接電流を供給しなければならない。しか
るにこの様な大電流を一気に溶接点へ供給する場
合には走行速度と電流値を正確に調和させること
が難しくて電流値が過大となり易く、その結果ビ
ードのアンダーカツトやアークの貫通といつた欠
陥が発生する。そして溶接チタン管は殆んど溶接
状態のまま、即ちビード部の後加工や補修溶接を
しないで使用されることから、ビード形状やビー
ド部の機械的特性に対する要求は特に厳しく、上
記欠陥は致命的なものと考えている。即ち従来の
単電極TIG溶接方法ではTi管を高速溶接するこ
とができないのが実状であつたと言わなければな
らない。
ところで鋼管あるいはステンレス鋼管の製造に
際し複数本の電極を使用してTIG溶接を行なう方
法が知られており、その具体的手法についても
種々の提案があつて(特公昭56−28629、特公昭
53−34771、特公昭52−91139等)、かなりの高速
生産も実現されている。即ち上記提案の溶接方法
は2本または3本の電極を使用すると共に電極先
端間距離を10〜20mmとし、且つ電極を被溶接材
(鋼管あるいはステンレス管)に対して垂直ある
いは複数電極が中心点に集中する様に指向させて
溶接を行なうものであり、溶融プールを一体化さ
せることにより入熱効率をあげて高速生産を達成
している。
[発明が解決しようとする問題点]
本発明者等はかねてよりTi管の高速生産を達
成することを目的として研究を行なつていたの
で、ステンレス鋼管に関する上記提案方法即ち複
数電極によるTIG溶接法に着目し、これをTi管
の製造に応用しようと考えた。即ち汎用されてい
る単電極TIG溶接では前述の如く溶接電流が1箇
所に集中し過ぎる為アンダーカツトビードやアー
クの貫通といつた欠陥が発生していたけれども複
数電極TIG溶接を採用した場合は溶接電流が分割
供給されることになつて1電極当りの溶接電流が
小さくて済み、上記単電極法における欠陥の発生
がより高速度レベルになるまで回避されると期待
されたからである。
たしかに複数電極によるTIG溶接法をTi管の
製造に適用してみると、前記欠陥は解消された
が、これは別に溶湯の盛上りやハンピングビード
等の問題が新たに発生することが明らかになつ
た。
即ち先行電極の後方に溶湯の盛上りが発生する
と、後行電極がこれと短絡して溶接の継続が不可
能となり、たとえ溶接できたとしても製品のビー
ド形状が悪化した。また先行電極による溶湯が長
手方向につながらずに途中で収縮してハンピング
ビードが形成されると、後行電極によつて形成さ
れるビードの形状が崩れ最終の製品ビード形状が
乱れたものとなつた。
[問題点を解決するための手段]
本発明はこうした問題点を解決しようと種々検
討を重ねた結果完成されたものであつて、その要
旨は、TIG溶接用非消耗電極を溶接進行方法に2
本以上配置し、このうち最終2本の電極先端間距
離L(mm)を下記()、()式を満足する様に
設定し、且つ使用する全電極の形成管体進行方向
に対する傾き角θを夫々同一又は異なつて下記
()式を満足する様に設定する点に存在する。
10≦L≦70 ……()
0.035VT1.5≦L≦0.007VT1.5+20 ……()
ただしV:造管速度(mm/min)
T:管肉厚(mm)
0゜≦θ≦45゜ ……()
[作用]
本発明者等は前記問題点を解決するに当たり溶
接条件殊に電極先端間距離、電極の傾き角、溶接
電流、造管速度等に着目し研究を行なつた。
以下研究の経緯に沿つて本発明を説明する。
尚試験溶接方法は単電極に代えて2本の電極を
配置する他は第3図に示す製造方法と概略同様で
ある。但しスクイズローラ5については従来の単
一ローラから比較的小径の5個のローラに代え
た。その理由は管状にまで湾曲されたTi帯板に
はスプリングバツク力が残留しており、突合わせ
部を溶接した後もビード部分にはこれを分離させ
ようとするスプリングバツク力が働き、これによ
つてビード中にミクロ欠陥が発生するという問題
があるからである。即ち複数個の小径スクイズロ
ーラ溶接点前後の突合わせ部を挟圧するという構
成を採用することにより、スプリングバツク力は
十分に抑えられ、ミクロ欠陥の発生を防止してい
る。また試験溶接では管内外面のビードに対して
酸素が混入するのを防止する目的で、溶接点近傍
をArガスでシールドしている。
上記溶接条件に基づき、まず2電極溶接により
電極間距離等を種々変更して試験溶接を行ない溶
湯盛上りの有無を調べたところ第1、2表に示す
結果が得られた。
[Industrial Application Field] The present invention is a method of welding Ti or Ti at high speed by TIG welding.
The present invention relates to a method of manufacturing an alloy tube, and more specifically, to a method of manufacturing a Ti or Ti alloy tube at high speed without causing problems such as interruption of welding due to bulging of molten metal or generation of humping beads. [Prior Art] When manufacturing Ti or Ti alloy (hereinafter referred to as Ti) pipes, for example, as shown in FIG. A breakdown roller 3, a fin pass roller 4, and a squeeze roller 5 rotate horizontally on a base K.
A Ti strip F is curved, its end faces are abutted against each other, and the abutted ends are welded by a welding machine 7. and
The Ti tube is further fed to a sizing roller 6 and finished to a predetermined outer diameter. Note that a single-electrode TIG welding machine is used as a welding machine in the above Ti pipe manufacturing process. By the way, in order to increase the productivity in the above manufacturing method, it is necessary to increase the pipe manufacturing speed, and the welding must be able to penetrate sufficiently into the Ti strip running at high speed, so large welds are required at the welding point. Current must be supplied. However, when such a large current is supplied to the welding point all at once, it is difficult to accurately match the running speed and the current value, and the current value tends to be excessive, resulting in bead undercuts and arc penetration. Defects occur. Since welded titanium tubes are used almost in the welded state, that is, without any post-processing or repair welding of the bead, the requirements for the bead shape and mechanical properties of the bead are particularly strict, and the above defects are fatal. I think it's something like that. In other words, it must be said that the reality is that Ti pipes cannot be welded at high speed using the conventional single electrode TIG welding method. By the way, a method of TIG welding using multiple electrodes is known when manufacturing steel pipes or stainless steel pipes, and various proposals have been made regarding the specific method (Japanese Patent Publication No. 56-28629, Japanese Patent Publication No. 28629).
53-34771, Special Publication No. 52-91139, etc.), and considerably high-speed production was also achieved. In other words, the welding method proposed above uses two or three electrodes, the distance between the electrode tips is 10 to 20 mm, and the electrodes are perpendicular to the material to be welded (steel pipe or stainless steel pipe), or the multiple electrodes are placed at the center point. Welding is performed by directing the molten pool to concentrate, and by integrating the molten pool, heat input efficiency is increased and high-speed production is achieved. [Problems to be Solved by the Invention] The present inventors have been conducting research for some time with the aim of achieving high-speed production of Ti pipes, and therefore, the above-mentioned proposed method for stainless steel pipes, that is, the TIG welding method using multiple electrodes. We focused on this and thought of applying this to the production of Ti tubes. In other words, as mentioned above, with the commonly used single-electrode TIG welding, the welding current is too concentrated in one location, resulting in defects such as undercut beads and arc penetration, but when multiple-electrode TIG welding is adopted, welding This is because it was expected that the welding current per electrode would be small because the current would be supplied in parts, and that the occurrence of defects in the single electrode method would be avoided until higher speed levels were reached. It is true that when the TIG welding method using multiple electrodes was applied to the manufacture of Ti pipes, the above-mentioned defects were resolved, but it became clear that new problems such as molten metal build-up and humping beads would occur. Summer. That is, when a bulge of molten metal occurs behind the leading electrode, the trailing electrode short-circuits with this, making it impossible to continue welding, and even if welding is possible, the bead shape of the product deteriorates. In addition, if the molten metal formed by the leading electrode does not connect in the longitudinal direction and shrinks midway to form a humping bead, the shape of the bead formed by the trailing electrode will collapse and the final product bead shape will be disordered. Summer. [Means for Solving the Problems] The present invention was completed as a result of various studies aimed at solving these problems.
The distance L (mm) between the tips of the final two electrodes is set to satisfy the following formulas () and (), and the inclination angle θ of all the electrodes with respect to the direction of movement of the forming tube is set. are set to be the same or different so as to satisfy the following equation (). 10≦L≦70 …() 0.035VT 1.5 ≦L≦0.007VT 1.5 +20 …() Where, V: Pipe manufacturing speed (mm/min) T: Pipe wall thickness (mm) 0゜≦θ≦45゜ … ...() [Function] In order to solve the above-mentioned problems, the present inventors conducted research focusing on welding conditions, particularly the distance between electrode tips, electrode inclination angle, welding current, pipe forming speed, etc. The present invention will be explained below along with the background of the research. The test welding method is roughly the same as the manufacturing method shown in FIG. 3, except that two electrodes are used instead of a single electrode. However, regarding the squeeze roller 5, the conventional single roller was replaced with five rollers having a relatively small diameter. The reason for this is that springback force remains in the Ti strip that has been curved into a tubular shape, and even after welding the butt part, springback force acts on the bead part to separate it. This is because there is a problem in that micro defects occur in the bead. That is, by adopting a structure in which a plurality of small-diameter squeeze rollers press the abutting portions before and after the welding point, the springback force is sufficiently suppressed and the generation of micro defects is prevented. In addition, during test welding, the area near the welding point was shielded with Ar gas to prevent oxygen from entering the bead on the inner and outer surfaces of the tube. Based on the above welding conditions, test welding was first carried out by two-electrode welding with various changes in the distance between the electrodes, etc., and the presence or absence of molten metal build-up was investigated, and the results shown in Tables 1 and 2 were obtained.
【表】【table】
【表】
次に溶接部に3本の電極を配置する他は前記と
同様の条件をとり、第2番目の電極先端と第3番
目の電極先端の距離L23等を種々変更して試験溶
接を行ない溶湯盛上りの有無を調べたところ、第
3、4表に示す結果が得られた。[Table] Next, test welding was performed under the same conditions as above except that three electrodes were placed in the welding area, and the distance L 23 between the second electrode tip and the third electrode tip was variously changed. When the presence or absence of molten metal buildup was investigated, the results shown in Tables 3 and 4 were obtained.
【表】【table】
【表】【table】
【表】
上記試験溶接の過程を観察したところ、溶湯の
盛上り現象は2つの電極を使用した場合には先行
電極と後行電極の間で、又3つの電極を使用した
場合には第2電極と第3電極の間で夫々発生する
ことが確認された。また溶湯盛上り現象は上記2
電極間の溶湯が熔融状態のままつながつた時に後
方側の溶湯が逆流して発生することが分かつた。
そして第1〜4表の結果からこの様な溶湯盛上
り現象は造管速度が速い程又Ti管の肉厚が大き
い程、又更に電極先端間距離が短かい程発生し易
いことが分かつた。
そこで第1〜4表の結果を電極先端間距離、
Ti管肉厚および造管速度の関数として整理した
ところ第1図に示す結果を得た。
即ち第1図に示す様に溶湯盛上り現象はL<
0.0035VT1.5の領域(A領域)で発生しており、
従つて溶湯盛上りを防止する為にはL≧
0.0035VT1.5とする必要があることが分かる。た
だしL>70(B領域)になると入熱効率が悪化す
るだけでなくシールド性に問題が出てくる。また
L>0.007VT1.5+20(C領域)になると入熱効率
が悪化し複数電極を用いることのメリツトが無く
なる。さらにL<10(D領域)になるとアークの
干渉が激しくなり溶接が不安定となる。従つて溶
湯の盛上りを防止し且つ満足し得る溶接性を得る
為には最終2本の電極先端間距離を、下記()、
()式を満足する様に設定する必要があるとの
結論に至つた。
10≦L≦70 ……()
0.0035VT1.5≦L≦0.007VT1.5+20 ……()
前述のように、従来のステンレス鋼管用の複数
電極溶接法では全体で単一の溶融プールを形成さ
せて入熱効率を上げようとの狙いから、電極先端
間距離は比較的短く設定されてきた。しかしチタ
ン管の溶接では溶湯盛上りという特異な現象が発
生するためにむしろ溶融プールの一体化を避け、
従来とは全く異なる設定条件を採用することが必
要とわかつた。
次にハンピングビードについては第1電極によ
つて形成されるビードの形状が重要であり、ここ
でビード幅が狭くなつたりあるいは途切れる現象
があると、2番目以降の電極によつて形成される
ビード形状も悪化する。
そこで第2図に示す様に、2電極配置の試験溶
接条件において電極先端間距離を20mm若しくは30
mmに固定し、第1電極の傾き角θ1を種々変更して
溶接を行ない、ハンピングビードの発生状況を調
査したところ第5表に示す結果が得られた。尚他
の試験条件は、T=0.7mm、Ti管径=25.4mm、I1=
300A若しくは200A、V=10m/minの夫々一定
とした。[Table] When we observed the above test welding process, we found that the molten metal build-up phenomenon occurs between the leading electrode and the trailing electrode when two electrodes are used, and between the leading electrode and the trailing electrode when three electrodes are used. It was confirmed that this phenomenon occurred between the electrode and the third electrode. In addition, the phenomenon of molten metal rising is explained in the above 2.
It was found that when the molten metal between the electrodes was connected in a molten state, the molten metal on the rear side flowed backwards. From the results in Tables 1 to 4, it was found that such molten metal swelling phenomenon occurs more easily as the pipe forming speed is faster, the wall thickness of the Ti pipe is larger, and the distance between the electrode tips is shorter. . Therefore, the results in Tables 1 to 4 are used as the distance between the electrode tips,
The results shown in Figure 1 were obtained by organizing the results as a function of Ti pipe wall thickness and pipe forming speed. That is, as shown in Fig. 1, the phenomenon of molten metal rising is L<
It occurs in the area of 0.0035VT 1.5 (area A),
Therefore, in order to prevent molten metal from rising, L≧
It turns out that it is necessary to set it to 0.0035VT 1.5 . However, when L>70 (region B), not only the heat input efficiency deteriorates but also problems arise in shielding performance. Furthermore, when L>0.007VT 1.5 +20 (region C), the heat input efficiency deteriorates and the advantage of using multiple electrodes disappears. Furthermore, when L<10 (D region), arc interference becomes severe and welding becomes unstable. Therefore, in order to prevent the molten metal from rising and to obtain satisfactory weldability, the distance between the final two electrode tips should be set as follows (),
We came to the conclusion that it is necessary to set it so that the formula () is satisfied. 10≦L≦70 …() 0.0035VT 1.5 ≦L≦0.007VT 1.5 +20 …() As mentioned above, in the conventional multi-electrode welding method for stainless steel pipes, a single molten pool is formed overall. With the aim of increasing heat input efficiency, the distance between the electrode tips has been set relatively short. However, when welding titanium pipes, a unique phenomenon of molten metal buildup occurs, so it is better to avoid integrating the molten pool.
It became clear that it was necessary to adopt setting conditions that were completely different from those used in the past. Next, regarding the humping bead, the shape of the bead formed by the first electrode is important, and if the bead width narrows or breaks, it will be formed by the second and subsequent electrodes. The bead shape also deteriorates. Therefore, as shown in Figure 2, the distance between the electrode tips was set to 20 mm or 30 mm under test welding conditions with a two-electrode arrangement.
Welding was carried out with the angle of inclination θ 1 of the first electrode fixed at mm and variously changed, and the occurrence of humping beads was investigated, and the results shown in Table 5 were obtained. Other test conditions are T = 0.7mm, Ti tube diameter = 25.4mm, I 1 =
300A or 200A, V=10m/min, respectively, were constant.
【表】【table】
【表】
第5表に示す様にθ1が−15゜以下の場合、即ち
電極が形成管体進行方向に対して逆方向に傾斜し
ている場合にはハンピングビードが発生し易く、
これが原因となつて2番目以降の電極による溶接
が不安定となり最終ビード形状が悪化した。ハン
ピングビードの発生状況は3つの電極を使用した
場合も同様の傾向が見られ、この問題を回避する
為にはθ1を0゜以上にする必要があることが分かつ
た。尚2極目以降の電極傾き角θ2あるいはθ3はハ
ンピングビードの発生に影響しなかつたが、電極
配置の構成上θ1≦θ2≦θ3とする必要があり、従つ
全電極の傾き角は0゜以上とする必要がある。しか
し45゜を越える様な電極傾き角は実用上アークの
安定性や作業性に問題が生じ、従つて電極の傾き
角は下記()式を満足する様に設定する必要が
あることを知つた。
0゜≦θ≦45゜ ……()
尚高速溶接での溶込みやシールド性の面からみ
ると15゜≦θ≦30゜が最適範囲である。また、電極
先端近傍のガスの流れを安定させシールド性を向
上させるためには、すべての電極を、あるいは少
なくとも2本の電極を平行に配置することが望ま
しい。
本発明の基本構成は上記の通りである。
ところで複数電極TIG溶接では各電極における
溶接電流の配分が製品ビードや溶接時のアークの
安定性に影響を及ぼす傾向がある。
そこで3電極溶接において溶接電流配分を種々
変更して溶接試験を行ない、次の結果が得られ
た。
管肉厚が薄い場合(若しくは造管速度が遅い場
合)には溶接電流の合計量(It)は比較的少なく
て済む。特に(It)≦600Aの場合には電極の溶接
電流配分をほぼ均一にすることが望ましく、具体
的にはI1:I2:I3=1:(0.9〜1.1):(0.9〜1.1)と
することが推奨される。尚いずれか1つの電極の
溶接電流を低くし過ぎた場合にはアークが不安定
になり、アークが他の電極やスクイズロールの方
へ偏る傾向がある。またいずれか1つの溶接電流
を100A未満とした場合に特にこの傾向が著しい。
一方管肉厚が大きい場合(若しくは造管速度が
速い場合)には溶接電流合計量(It)を多くしな
ければならず、It>600Aの場合には3電極の配
分を均一とするよりも最終の第3電極の電流を低
くする方が高品質のビードが得られて望ましい。
特に第3電極の電流値が250Aを超えるような高
電流溶接では溶湯量が多くなるため、凝固後のマ
クロ組織が大きくなつたりリビード表面が粗くな
る傾向がある。これを改善する方法としては最終
電極の電流を先行電極の溶接電流よりも最大30%
程度低くすることが有利である。こうしたことか
ら溶接電流の分配比は、I1:I2:I3=1:(0.9〜
1.1):(0.7〜1.1)とすることが推奨される。
その他本発明の実施に当たつては、溶接ビード
部のミクロ欠陥の発生を防止するために、小径多
段型スクイズローラを使用したが、例えばスクイ
ズローラに入る前のブレークダウンローラやフイ
ンパスローラの段階でロールフラワー(各成形ロ
ーラの孔型形状)を好適に定めて素材のスプリン
グバツグをゼロとする方法あるいは200〜400℃程
度に素材を加熱してスプリングバツクを抑える方
法を併用すれば、どのようなスクイズ方式を採用
しても製造は可能である。
[発明の効果]
本発明は以上の様に構成されており、溶湯の盛
上りあるいはハンピングビードを発生させること
がなく高速でTi管をTIG溶接することができ、
良好な品質のTi管を生産性良く得ることができ
る。[Table] As shown in Table 5, when θ 1 is -15° or less, that is, when the electrode is tilted in the opposite direction to the direction of movement of the forming tube, humping beads are likely to occur.
As a result, welding using the second and subsequent electrodes became unstable and the final bead shape deteriorated. A similar tendency was observed in the occurrence of humping beads when three electrodes were used, and it was found that in order to avoid this problem, it was necessary to set θ 1 to 0° or more. Although the electrode inclination angle θ 2 or θ 3 after the second pole did not affect the generation of humping bead, it is necessary to satisfy θ 1 ≦ θ 2 ≦ θ 3 due to the structure of the electrode arrangement, and therefore the angle of inclination of all electrodes is The angle of inclination must be 0° or more. However, if the electrode tilt angle exceeds 45°, there will be problems with arc stability and workability in practice, so we learned that the electrode tilt angle must be set to satisfy the following formula (). . 0゜≦θ≦45゜ ... () From the viewpoint of penetration and shielding properties during high-speed welding, 15゜≦θ≦30゜ is the optimal range. Further, in order to stabilize the flow of gas near the tip of the electrode and improve shielding properties, it is desirable to arrange all the electrodes or at least two electrodes in parallel. The basic configuration of the present invention is as described above. However, in multi-electrode TIG welding, the distribution of welding current in each electrode tends to affect the product bead and the stability of the arc during welding. Therefore, welding tests were conducted with various changes in welding current distribution in three-electrode welding, and the following results were obtained. When the pipe wall thickness is thin (or when the pipe manufacturing speed is slow), the total amount of welding current (It) can be relatively small. In particular, when (It)≦600A, it is desirable to make the welding current distribution of the electrode almost uniform, specifically, I 1 : I 2 : I 3 = 1: (0.9 to 1.1): (0.9 to 1.1) It is recommended that Note that if the welding current of any one electrode is made too low, the arc becomes unstable and tends to be biased toward other electrodes or the squeeze roll. Moreover, this tendency is particularly remarkable when any one of the welding currents is less than 100A. On the other hand, if the pipe wall thickness is large (or if the pipe manufacturing speed is fast), the total amount of welding current (It) must be increased, and if It>600A, the distribution of the three electrodes should be made uniform. It is preferable to lower the current of the final third electrode because a higher quality bead can be obtained.
In particular, in high-current welding where the current value of the third electrode exceeds 250 A, the amount of molten metal increases, so the macrostructure after solidification tends to become larger and the rebead surface tends to become rougher. A way to improve this is to increase the final electrode's welding current by up to 30% compared to the preceding electrode's welding current.
It is advantageous to reduce the amount. Therefore, the welding current distribution ratio is I 1 :I 2 :I 3 =1:(0.9~
1.1): (0.7 to 1.1) is recommended. In addition, in carrying out the present invention, a small diameter multi-stage squeeze roller was used in order to prevent the occurrence of micro-defects in the weld bead. If you use a method to eliminate the spring bag of the material by appropriately determining the roll flower (the hole shape of each forming roller) at the stage, or a method to suppress the spring bag by heating the material to about 200 to 400 degrees Celsius, it is possible to Manufacturing is possible even if a squeeze method such as this is adopted. [Effects of the Invention] The present invention is configured as described above, and can perform TIG welding of Ti pipes at high speed without generating molten metal buildup or humping beads.
Good quality Ti tubes can be obtained with high productivity.
第1図はLとVT1.5の関係を示すグラフ、第2
図は試験溶接方法を示す模式図、第3図はTi管
の製造方法を示す模式図である。
F……帯板、2……駆動ローラ、5……スクイ
ズローラ、7……溶接機。
Figure 1 is a graph showing the relationship between L and VT 1.5 , Figure 2 is a graph showing the relationship between L and VT 1.5.
The figure is a schematic diagram showing a test welding method, and FIG. 3 is a schematic diagram showing a Ti pipe manufacturing method. F... Band plate, 2... Drive roller, 5... Squeeze roller, 7... Welding machine.
Claims (1)
合わせ部をTIG溶接して管を製造する方法であつ
て、TIG溶接用非消耗電極を溶接進行方向に2本
以上配置し、このうち最終2本の電極先端間距離
L(mm)を下記()、()式を満足する様に設
定し、且つ使用する全電極の形成管体進行方向に
対する傾き角θを夫々同一又は異なつて下記
()式を満足する様に設定することを特徴とす
るTiまたはTi合金管の製造方法。 10≦L≦70 ……() 0.0035VT1.5≦L≦0.007VT1.5+20 ……() ただしV:造管速度(mm/min) T:管肉厚(mm) 0゜≦θ≦45゜ ……()[Claims] 1. A method of manufacturing a pipe by bending a Ti or Ti alloy strip plate and TIG welding the abutting portions of the end faces, comprising two or more non-consumable electrodes for TIG welding in the direction of welding progress. Set the distance L (mm) between the tips of the final two electrodes to satisfy the following formulas () and (), and set the inclination angle θ of all electrodes to the direction of movement of the forming tube, respectively. A method for manufacturing a Ti or Ti alloy tube, characterized by setting the same or different conditions to satisfy the following formula (). 10≦L≦70 …() 0.0035VT 1.5 ≦L≦0.007VT 1.5 +20 …() Where, V: Pipe manufacturing speed (mm/min) T: Pipe wall thickness (mm) 0゜≦θ≦45゜ … …()
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP12900885A JPS61286074A (en) | 1985-06-13 | 1985-06-13 | Production of ti or ti alloy pipe |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP12900885A JPS61286074A (en) | 1985-06-13 | 1985-06-13 | Production of ti or ti alloy pipe |
Publications (2)
| Publication Number | Publication Date |
|---|---|
| JPS61286074A JPS61286074A (en) | 1986-12-16 |
| JPH0438513B2 true JPH0438513B2 (en) | 1992-06-24 |
Family
ID=14998879
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP12900885A Granted JPS61286074A (en) | 1985-06-13 | 1985-06-13 | Production of ti or ti alloy pipe |
Country Status (1)
| Country | Link |
|---|---|
| JP (1) | JPS61286074A (en) |
-
1985
- 1985-06-13 JP JP12900885A patent/JPS61286074A/en active Granted
Also Published As
| Publication number | Publication date |
|---|---|
| JPS61286074A (en) | 1986-12-16 |
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| EXPY | Cancellation because of completion of term |