JPH0771757B2 - Method and apparatus for manufacturing ultra-thin metal pipe using modulated output YAG laser - Google Patents
Method and apparatus for manufacturing ultra-thin metal pipe using modulated output YAG laserInfo
- Publication number
- JPH0771757B2 JPH0771757B2 JP2103089A JP10308990A JPH0771757B2 JP H0771757 B2 JPH0771757 B2 JP H0771757B2 JP 2103089 A JP2103089 A JP 2103089A JP 10308990 A JP10308990 A JP 10308990A JP H0771757 B2 JPH0771757 B2 JP H0771757B2
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- Japan
- Prior art keywords
- laser
- output
- yag laser
- metal foil
- thin metal
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Description
【発明の詳細な説明】 [産業上の利用分野] 本発明は、厚さ30〜150μmの極薄金属箔のYAGレーザ溶
接によるパイプの製造方法とその装置に関するものであ
る。TECHNICAL FIELD The present invention relates to a method and an apparatus for manufacturing a pipe by YAG laser welding of an ultrathin metal foil having a thickness of 30 to 150 μm.
[従来の技術] 極薄金属箔を連続的に管状に成形して相対する突き合せ
端面を楔形状に収束させ、その集束点近傍をTIG等の電
気溶接で行うことは溶接点のパイプエッジ端面のエッジ
のかえり、粗さ等の条件の正確な調節、ギャップ及びオ
フセット条件の正確な調節、突き合せの正確な調節なら
びに厳しい入熱制限が要求されるために極薄金属箔の溶
接には適さない。また熱影響層も大きいため溶接性の点
で問題があり、特に管の曲げ加工には適さない。さらに
従来のレーザ溶接を行う方法に於いても上記のエッジ、
ギャップ、オフセット等の、突き合せ条件の正確な調
整、及び厳しい入熱制限のために、極薄金属箔の溶接に
おいてはレーザの照射位置ならびにビーム径、パワーを
正確に限定する必要があり、技術的に困難である。[Prior Art] It is necessary to form an ultra-thin metal foil in a continuous tube shape to converge opposing butt end faces into a wedge shape and to perform electrical welding such as TIG near the focusing point to the pipe edge end face of the welding point. It is suitable for welding ultra-thin metal foil because it requires precise adjustment of conditions such as edge burr and roughness, accurate adjustment of gap and offset conditions, accurate adjustment of butt and strict heat input. Absent. Further, since the heat-affected layer is large, there is a problem in terms of weldability, and it is not particularly suitable for bending a pipe. Even in the conventional method of performing laser welding, the above edge,
Due to precise adjustment of butt conditions such as gaps and offsets, and severe heat input restriction, it is necessary to precisely limit the laser irradiation position, beam diameter, and power when welding ultra-thin metal foil. Is difficult.
また、特開昭60−96382号公報に見られるように低密度
集光YAGレーザで照射する溶接法は、上記のような厳し
い突き合せ条件の緩和を図るとともに、極薄金属箔表面
での非接触、溶融時のレーザの吸収率の比を小さくし、
溶け落ち、ハンピング等の溶接欠陥を防止するものであ
る。しかし溶接欠陥の防止については、同公開公報に書
かれているように、YAGレーザの非溶融時の吸収率
αc、溶融時の吸収率αmの変化比RyはRy>2.5程度で
あり、CO2レーザの吸収率変化比Rc>11に比べ十分小さ
いとは言え、非溶融時、溶融時において、レーザの投入
エネルギーの吸収率が2倍以上変化している事に変わり
は無く、極薄金属箔のように、熱容量の小さなものの溶
接においては、わずかの溶接状態の変化が溶接結果に大
きく影響するので、溶接欠陥の防止には十分とは言いが
たい。In addition, the welding method of irradiating with a low-density YAG laser as disclosed in JP-A-60-96382 aims at alleviating the severe butt conditions as described above, and at the same time, it does not apply to the non-thin metal foil surface. Reduce the ratio of laser absorptance during contact and melting,
This prevents welding defects such as burn-through and humping. However, as to the prevention of welding defects, as described in the publication, the change ratio R y between the absorption rate α c of the YAG laser when it is not melted and the absorption rate α m when it is melted is about R y > 2.5. Although it is sufficiently smaller than the absorption rate change ratio R c > 11 of the CO 2 laser, there is no change in that the absorption rate of the input energy of the laser changes more than twice when it is not melted and when it is melted. In the case of welding a material having a small heat capacity such as an ultra-thin metal foil, even a slight change in the welding state has a great effect on the welding result, so it cannot be said that it is sufficient to prevent welding defects.
[発明が解決しようとする課題] 本発明は、極薄金属箔を連続的に管状に成形して溶接に
よりパイプ化する際の電気溶接及び従来のレーザ溶接法
では克服出来ない厳しいエッジ条件、オフセット条件、
突き合せ条件ならびに入熱条件の問題を克服し、溶融熱
影響層の少ない品質の良い極薄金属箔パイプが得られる
製造方法と装置を提供する事を目的としている。[Problems to be Solved by the Invention] The present invention is directed to severe edge conditions and offsets that cannot be overcome by electric welding and a conventional laser welding method when continuously forming an ultrathin metal foil into a tubular shape and forming a pipe by welding. conditions,
It is an object of the present invention to provide a manufacturing method and apparatus capable of overcoming the problems of the butt condition and the heat input condition and obtaining a high quality ultra-thin metal foil pipe having a small heat-affected zone of melting.
[課題を解決するための手段] 本発明は、上記の目的を達成するためになされたもので
あり、その要旨とするところは 極薄金属箔を連続的に成形して相対する突き合せ端面を
楔形状に収束させ溶接する極薄金属箔パイプ製造装置に
於いて、レーザの励起ランプに対してそれぞれ並列に接
続されたランプ点火用トリガー回路を含むシマー電源部
と、干渉を抑制するためにパルストランスを介してパル
ス電源部とを備え、連続レーザ出力にパルスレーザ出力
を重畳させた変調出力を発するレーザ発振機と、極薄金
属箔の収束部に形成する楔形状部を低密度集光ビームで
照射する光学系とを備えたことを特徴とするYAGレーザ
による極薄金属箔パイプの製造装置と、 極薄金属箔を連続的に成形して相対する突き合せ端面を
楔形状に収束させ、該楔形状部にレーザを照射して溶接
する極薄金属箔パイプの製造方法において、端部のオフ
セットを極薄金属箔の板厚の30%以下に保持し成形され
た該楔形状部のギャップが極薄金属箔の板厚の1倍以上
5倍以下になる点に、連続出力にパルス出力を重畳させ
た変調出力を発する低密度集光YAGレーザビームの中心
を一致させて照射し、端面から板厚の2〜10倍の領域を
溶融し、溶融端面を凝固直前に押し付けて溶接を完了さ
せる方法である。[Means for Solving the Problems] The present invention has been made in order to achieve the above-mentioned object, and the gist of the present invention is to continuously form an ultra-thin metal foil so as to form opposing butt end surfaces. In an ultra-thin metal foil pipe manufacturing device that converges and welds in a wedge shape, a simmer power supply part including a lamp ignition trigger circuit connected in parallel to each laser excitation lamp and a pulse to suppress interference A low-density focused beam with a laser power source equipped with a pulsed power supply through a transformer, which emits a modulated output by superimposing a pulsed laser output on a continuous laser output, and a wedge-shaped part formed in the focusing part of an ultrathin metal foil. The ultra-thin metal foil pipe manufacturing device using the YAG laser, which is equipped with an optical system for irradiating with, and the ultra-thin metal foil are continuously molded to converge the facing end faces into a wedge shape. The wedge shape In the method of manufacturing an ultra-thin metal foil pipe in which a portion is irradiated with a laser and welded, the gap of the wedge-shaped portion formed by holding the offset of the end to 30% or less of the plate thickness of the ultra-thin metal foil is extremely thin. The thickness of the low density focused YAG laser beam that emits the modulated output by superimposing the pulse output on the continuous output is made to coincide with the point of 1 to 5 times the plate thickness of the metal foil, and the plate thickness is applied from the end face. Is a method of melting a region 2 to 10 times as large as the above and pressing the melting end face immediately before solidification to complete welding.
[作用] (1)本発明のパイプ製造方法の成形加工は第1図に示
すように、極薄金属箔を連続的に成形して相対する突き
合せ端面を楔形状に収束させ、溶接箇所においてエッジ
端面のオフセットが板厚の30%以下に納まる成形方法で
あればどのような方法にも適用できる。[Operation] (1) As shown in FIG. 1, in the forming process of the pipe manufacturing method of the present invention, an ultrathin metal foil is continuously formed so that the opposing end faces are converged into a wedge shape, and at the welded portion. It can be applied to any method as long as the offset of the edge face is within 30% of the plate thickness.
(2)第2、3図は連続出力にパルス出力を重畳させた
変調出力を発するYAGレーザ発振機を用いた低密度エネ
ルギービーム域ソフト溶接法の概念図である。YAGレー
ザを極薄金属箔の開先のギャップが板厚の1倍以上5倍
以下に開いたところに照射し、照射ビーム径を極薄金属
箔の両端面を板厚の2〜10倍の巾にわたり溶融させるよ
うに集光し、溶け落ち、ハンピングのない溶接を行う。
この時、極薄金属箔の両端溶融部の幅+両端部のギャッ
プ長g=YAGレーザのビーム径Dとなっている。ビーム
径Dはレンズの焦点距離f又は、焦点位置を鋼板の上側
にセットするディフォーカス照射によって制御する。レ
ーザの照射位置を開先ギャップが板厚の値未満の位置に
すると、突き合せ点に照射するのと同様になり両端部の
溶融による寄り合いが少なくなり、端部のオフセットを
板厚の10%以下の精度にする必要がある。これは極薄金
属箔に対しては非常に高度な技術が要求され、実行する
事は困難である。また、板厚の5倍の値を越える位置で
は、両端部が離れすぎているために上手く突き合せる事
が出来ず良好な溶接が出来ない。また、端面からの溶接
領域が板厚の2倍未満では不十分な溶接となり、それが
10倍超では過剰な溶接となり溶け落ちが生じる。(2) FIGS. 2 and 3 are conceptual diagrams of a low density energy beam region soft welding method using a YAG laser oscillator that emits a modulated output by superimposing a pulse output on a continuous output. The YAG laser is radiated where the gap of the groove of the ultra-thin metal foil is 1 to 5 times the plate thickness, and the irradiation beam diameter is 2-10 times the plate thickness on both ends of the ultra-thin metal foil. Focuses so that it melts across the width, and it welds without melting or humping.
At this time, the width of the melted portion at both ends of the ultrathin metal foil + gap length at both ends g = the beam diameter D of the YAG laser. The beam diameter D is controlled by the focal length f of the lens or the defocus irradiation that sets the focal position to the upper side of the steel plate. When the laser irradiation position is set so that the groove gap is less than the plate thickness value, it is similar to irradiation at the abutting point, and the leaning due to melting of both ends is reduced, and the edge offset is 10% of the plate thickness. The following precision is required. This requires very advanced technology for ultra-thin metal foil and is difficult to implement. In addition, at a position where the value exceeds 5 times the plate thickness, both ends are too far apart from each other, so that they cannot be abutted well and good welding cannot be performed. Also, if the welding area from the end face is less than twice the plate thickness, insufficient welding will result.
If it exceeds 10 times, excessive welding will occur and burn through will occur.
(3)YAGレーザを連続出力にパルス出力を重畳させた
変調出力を発する事には以下の様な利点がある。金属表
面のレーザ光の吸収率は非溶融、溶融時において大きく
異なり、これにより入熱状態が変化し、極薄金属箔の溶
接においては溶接欠陥の原因となる。そのため特開昭60
−96382号公報に見られるようにYAGレーザをもちい、極
薄金属箔表面での非溶融、溶融時のレーザの吸収率の比
を小さくし、溶け落ち、ハンピング等の溶接欠陥を防止
する方法が開示されている。しかし溶接欠陥の防止につ
いては、同公開公報に書かれているように、YAGレーザ
の非溶融時の吸収率αc、溶融時の吸収率αmの変化比
RyはRy>2.5程度であり、CO2レーザの吸収率変化比Rc>
11に比べ十分小さいとは言え、非溶融時、溶融時におい
て、レーザの投入エネルギーの吸収率が2倍以上変化し
ている事に変わりは無く、極薄金属箔のように、熱容量
の小さなものの溶接においては、わずかの溶接状態の変
化が溶接結果に大きく影響するので、レーザの投入エネ
ルギーを最適条件に制御する事はその制御範囲が狭く非
常に困難であり、溶接欠陥の防止には十分とは言いがた
い。(3) Issuing a modulation output by superimposing a pulse output on a continuous output of a YAG laser has the following advantages. The absorptance of laser light on the metal surface is greatly different between non-melting and melting, which changes the heat input state, which causes welding defects in the welding of ultra-thin metal foil. Therefore, JP-A-60
-96382 using a YAG laser, non-melting on the surface of the ultra-thin metal foil, to reduce the ratio of the laser absorption rate at the time of melting, there is a method of preventing welding defects such as burn-through, humping It is disclosed. However, as to the prevention of welding defects, as described in the publication, the change ratio of the absorption rate α c of the YAG laser when it is not melted and the absorption rate α m when it is melted.
R y is approximately R y > 2.5, and the absorption rate change ratio R c > of the CO 2 laser
Although it is sufficiently smaller than that of 11, the absorption rate of the input energy of the laser changes twice or more during non-melting and melting, and it has a small heat capacity like ultra-thin metal foil. In welding, a slight change in the welding state has a large effect on the welding result, so controlling the laser input energy to the optimum conditions is very difficult because the control range is narrow and it is sufficient to prevent welding defects. Is hard to say.
これに対し、本発明の連続出力にパルス出力を重畳させ
たリップル出力のYAGレーザを使用する事で上記の様な
レーザの投入エネルギーの最適制御の条件を緩和する事
が出来る。第4図に本発明の変調YAGレーザの概略を示
す。PPは変調出力のパルス部分のピーク出力値を、PCは
変調出力の連続発振部の出力値を、Pavは変調出力の時
間平均値を示す。その作用は以下のとおりである。金属
箔表面の非溶融状態時に、リップル出力のパルス部分の
高いエネルギーを照射し、金属箔表面を瞬時に溶融状態
に至らしめる。しかる後、溶融状態になりレーザビーム
の吸収率が0.9以上の効率になったところで吸収率の変
化に従ってリップル発振のレーザ出力をリップル出力の
パルス部ピーク値PPから連続出力部のPCへと変化低下さ
せることにより極薄金属箔の過溶融を防ぎ溶融状態を維
持する。さらに極薄金属箔の表面が凝固しはじめレーザ
ビームの吸収率が低下したところで再びリップル出力の
パルス部分の高いエネルギーを投入し、極薄金属箔表面
を溶融状態に保つ。パルス部分のエネルギー密度は高
く、表面の溶融の核を常に形成するが、それによる入熱
量は少なく、加入熱になる事はない。On the other hand, by using the ripple output YAG laser in which the pulse output is superimposed on the continuous output according to the present invention, the conditions for the optimum control of the laser input energy as described above can be relaxed. FIG. 4 shows an outline of the modulated YAG laser of the present invention. P P is the peak output value of the pulse portion of the modulation output, P C is the output value of the continuous oscillation part of the modulation output, and P av is the time average value of the modulation output. The operation is as follows. When the surface of the metal foil is in a non-melted state, the pulsed portion of the ripple output is irradiated with high energy to instantly bring the surface of the metal foil into a molten state. Then, when the laser beam absorpted into the molten state and the absorptance of the laser beam became 0.9 or more, the laser output of ripple oscillation was changed from the peak value P P of the ripple output to P C of the continuous output according to the change of the absorptivity. By reducing the change, the ultra-thin metal foil is prevented from over-melting and the molten state is maintained. Further, when the surface of the ultra-thin metal foil begins to solidify and the absorptance of the laser beam decreases, high energy of the pulse portion of the ripple output is input again to keep the ultra-thin metal foil surface in a molten state. The pulse part has a high energy density and always forms the nuclei of melting on the surface, but the heat input by it is small, and it does not become added heat.
上記の様な溶融凝固を高速で繰り返す事により、極薄金
属箔対して溶け落ち、ハンピング等の溶接欠陥の無い溶
接を安定して行う事を可能とする。こうしてレーザの投
入エネルギーの制御範囲も広くなり容易に極薄金属箔に
対して溶接を行う事を可能とする。By repeating the melting and solidification as described above at high speed, it is possible to stably perform welding without welding defects such as burn-through and humping for ultra-thin metal foil. In this way, the control range of the energy input of the laser is widened, and it is possible to easily weld the ultra-thin metal foil.
(4)低密度エネルギービームによる面熱源的溶接法に
よる成形条件の緩和は以下のような理由による。(4) The relaxation of the forming conditions by the surface heat source welding method using the low density energy beam is as follows.
第2図のギャップgが板厚の2倍程度あるところにレ
ーザを照射することで、突き合せ点で極薄金属箔を溶融
させる場合に比べつき合う範囲が広くなるので(第5
図)、オフセットの条件(板厚の10%以下)が緩和され
る。By irradiating the laser with the gap g in FIG. 2 at about twice the plate thickness, the contact range becomes wider than in the case where the ultrathin metal foil is melted at the butt point (the fifth point).
Figure), the condition of offset (10% or less of the plate thickness) is relaxed.
突き合せ点の状態(極薄金属箔の両端部の重なり具
合)が微妙に変化しても、そのために起こる熱容量の微
妙な変化には左右されず熱の投入が行えるため、ハンピ
ング・溶け落ちのない溶接を行える。この方法によりギ
ャップ及びオフセットの許容値(板厚の10%以下)が大
幅(2〜3倍)に拡大出来る。Even if the state of the butt point (the degree of overlap of both ends of the ultra-thin metal foil) changes subtly, heat can be input without being affected by the subtle changes in heat capacity that occur, so humping and burn-through can be prevented. Can do no welding. By this method, the allowable value of the gap and offset (10% or less of the plate thickness) can be greatly expanded (2 to 3 times).
(5)第10図に本発明によるレーザ発振機の励起用ラン
プ電源回路のブロックダイアグラムを示す。ランプに
は、ランプ点火用トリガー回路を含むシマー電源部と、
パルス電源部が互いの干渉を抑制するためにパルストラ
ンスを介して並列に接続されている。以下に各部ロック
の機能を示す。(5) FIG. 10 shows a block diagram of the excitation lamp power supply circuit of the laser oscillator according to the present invention. The lamp has a simmer power supply including a trigger circuit for lamp ignition,
The pulse power supply units are connected in parallel via a pulse transformer to suppress mutual interference. The function of each part lock is shown below.
・SCR制御回路定電流制御部18 ランプにシマー電流を供給する。これによりランプの導
通状態を維持し、かつYAGロッドをレーザ発振閾値付近
以上に励起する。・ SCR control circuit Constant current controller 18 Supplies simmer current to the lamp. This maintains the lamp in a conducting state and excites the YAG rod above the laser oscillation threshold.
・トリガー発生回路19 ランプ点灯開始時に、ランプに放電経路を形成させるた
めの高圧トリガーを発生する。-Trigger generation circuit 19 Generates a high-voltage trigger for forming a discharge path in the lamp when the lamp starts to light.
・ブースト電圧発生回路20 トリガーにより形成したランプ内の放電経路を、シマー
電源が立ち上がるまでの間維持するブースト電圧を供給
する。-Boost voltage generation circuit 20 Supplies a boost voltage that maintains the discharge path in the lamp formed by the trigger until the simmer power supply starts up.
・パルス発振部21、FET22及びパルストランス23(PT) ランプに供給するパルス電流を制御する。パルス電流は
FET22により制御し、パルストランス23(PT)を経てラ
ンプに供給される。-Pulse oscillator 21, FET22 and pulse transformer 23 (PT) Controls the pulse current supplied to the lamp. The pulse current is
It is controlled by FET22 and supplied to the lamp through pulse transformer 23 (PT).
・逆電流防止用ダイオード(D1、D2) シマー電流の放電によるランプインピーダンス変動に対
し、シマー電流を安定化する。-Reverse current prevention diodes (D1, D2) Stabilize the simmer current against fluctuations in the lamp impedance due to discharge of the simmer current.
・真空リレー(RY1) ランプ点灯時にトリガーパルス及びブースト電圧に対
し、パルス電源部をシマー電源部から遮断、保護する。・ Vacuum relay (RY1) Shields the pulse power supply from the simmer power supply against the trigger pulse and boost voltage when the lamp is lit.
次に本発明によるレーザのパルス発振原理について説明
する。パルス発振の基本原理そのものはノーマルパルス
方式と類似であるが、本発明においてはYAGロッドは予
めシマー電流によってレーザ発振閾値付近以上にまで励
起されている。このため本発明では、従来のノーマルパ
ルス方式に比べ低いパルス電流値を重畳する事により、
パルス発振を達成出来る。更にランプ内には常に放電経
路が形成されており、低インピーダンス状態で発光可能
のため、ランプ印加電圧も同時に低くする事が出来る。
即ち、パルス出力と周波数を一定と考えた場合、ランプ
に入力されるエネルギーの平均値は減少する。従って本
発明によれば、ランプの入力制限内において、パルス電
流の繰り返し周波数を上げる事が可能となる。Next, the principle of pulse oscillation of the laser according to the present invention will be described. Although the basic principle of pulse oscillation is similar to that of the normal pulse method, in the present invention, the YAG rod is excited in advance by the simmer current to a level above the laser oscillation threshold. Therefore, in the present invention, by superimposing a pulse current value lower than that of the conventional normal pulse system,
Pulse oscillation can be achieved. Furthermore, since a discharge path is always formed in the lamp and light can be emitted in a low impedance state, the voltage applied to the lamp can be lowered at the same time.
That is, when the pulse output and the frequency are considered to be constant, the average value of the energy input to the lamp decreases. Therefore, according to the present invention, it is possible to increase the repetition frequency of the pulse current within the input limit of the lamp.
また第10図では、1本のランプにシマー電流とパルス電
流を重畳して供給する場合を示したが、更に第11図に示
すように、これらのシマー電流とパルス電流を重畳して
供給される2本のランプによってYAGロッドを励起した
場合には、ランプ1本の場合よりも励起入力が増加し、
その結果高いレーザ出力が得られる。Further, in FIG. 10, the case where the simmer current and the pulse current are superimposed and supplied to one lamp is shown, but as shown in FIG. 11, the simmer current and the pulse current are superimposed and supplied. When the YAG rod is excited by two lamps, the excitation input increases more than the case of one lamp,
As a result, a high laser output can be obtained.
[実施例] (1)第6図に示すような装置を用いて厚さ30〜150μ
mの金属箔を端部のオフセットを極薄金属箔の板厚の30
%以下,端部の突き合せ角度0.3゜〜5゜となるように
パイプ状に成形し、連続レーザ出力にパルスレーザ出力
を重畳させた変調出力を発するYAGレーザを使って溶接
を行った。[Example] (1) Using an apparatus as shown in FIG.
The edge of the metal foil of m is 30
%, The pipe was shaped so that the abutting angles of the ends were 0.3 ° to 5 °, and welding was performed using a YAG laser that emits a modulated output by superimposing a pulse laser output on a continuous laser output.
上記実施例における疲労試験の手順は以下のとおりであ
る。第7図に示す様に溶接した極薄金属箔パイプをその
溶接ビードを含む様にW:10mm×:40mmの短冊状に切りと
り、第8図に示す様に角の曲率Rが0.5mmである二枚の
鋼板の角に溶接ビードが倣う様に挟み込み、前後に90度
ずつの繰り返し曲げを行う。リファレンスとして、極薄
金属箔の母材に対しても同じ実験を行う。The procedure of the fatigue test in the above example is as follows. An ultra-thin metal foil pipe welded as shown in Fig. 7 was cut into a strip of W: 10mm ×: 40mm to include the weld bead, and the corner curvature R was 0.5mm as shown in Fig. 8. It is sandwiched so that the welding bead follows the corners of two steel plates, and is repeatedly bent back and forth by 90 degrees. As a reference, the same experiment is performed on the base material of ultra-thin metal foil.
i)ステンレス鋼板SUS304(板厚0.10mm)を連続レーザ
出力にパルスレーザ出力を重畳させた変調出力を発する
YAGレーザを板の表面でのビーム径1mmφ、パルス部ピー
ク出力200W、連続出力部出力80W、平均出力100Wで、パ
イプの突き合せギャップが0.2mmのところに照射し溶接
を実施したところ、溶け落ち欠陥の無い溶接が溶接速度
3.0m/minで得られた。また、ビードの厚みは母材厚の12
0%以下であり、パイプ溶接部をサンプルとして切り出
し繰り返し曲げによる疲労破壊テストを行ったところ50
回以上と良好な結果が得られた。i) A stainless steel SUS304 (sheet thickness 0.10 mm) emits a modulated output by superimposing a pulsed laser output on a continuous laser output.
When the welding was carried out by irradiating the YAG laser on the surface of the plate with a beam diameter of 1 mmφ, a pulse peak output of 200 W, a continuous output of 80 W, and an average output of 100 W, where the pipe butt gap was 0.2 mm and welding was carried out, it melted down. Welding speed without defects
Obtained at 3.0 m / min. Also, the bead thickness is 12
It was 0% or less, and when a pipe welded portion was cut out and a fatigue fracture test by repeated bending was performed, it was 50.
Good results were obtained more than once.
ii)上記と同様ステンレス鋼板SUS304(板厚0.05mm)を
連続レーザ出力にパルスレーザ出力を重畳させた変調出
力を発するYAGレーザを板の表面でのビーム径1mmφ、パ
ルス部ピーク出力150W、連続出力部出力40W、平均出力5
0Wで、パイプの突き合せギャップが0.2mmのところに照
射し溶接を実施したところ、溶け落ち欠陥の無い溶接が
溶接速度2.5m/minで得られた。また、ビードの厚みは母
材厚の120%以下であり、パイプ溶接部をサンプルとし
て切り出し繰り返し曲げによる疲労破壊テストを行った
ところ50回以上と良好な結果が得られた。ii) Similar to the above, a YAG laser that emits a modulated output by superimposing a pulsed laser output on a stainless steel plate SUS304 (plate thickness of 0.05 mm) is a beam diameter of 1 mmφ on the plate surface, a peak output of 150 W, and a continuous output. Part output 40W, average output 5
Welding was performed at 0 W at a butt gap of the pipe of 0.2 mm, and welding with no burn-through defect was obtained at a welding speed of 2.5 m / min. The bead thickness was 120% or less of the base metal thickness, and when the pipe welded portion was cut out and subjected to a fatigue fracture test by repeated bending, a favorable result of 50 times or more was obtained.
iii)従来法との溶接性比較のため、板厚100μmのSUS3
04平板材をTIG溶接により突き合せ溶接し(TIG溶接では
板厚100μm、50μmの極薄金属箔パイプの溶接は不可
能であった為)、同様の繰り返し曲げ疲労試験を行った
ところ、母材部は破壊回数70回、TIG溶接部破断回数35
回でありTIG溶接法に比べ、レーザ溶接法が溶接性にお
いて優れている事がわかった。iii) For comparison of weldability with conventional method, SUS3 with 100 μm thickness
04 Flat plate materials were butt welded by TIG welding (because it was impossible to weld ultra-thin metal foil pipes with a plate thickness of 100 μm and 50 μm with TIG welding), and a similar repeated bending fatigue test was performed. The number of fractures is 70, and the number of fractures in TIG welds is 35
It was found that the laser welding method was superior in weldability compared to the TIG welding method.
iv)上記実施例において溶接のビード幅を測定したとこ
ろ、板厚100μmのSUS304平板材をTIG溶接により突き合
せ溶接したビード幅は約400μmであったが、本発明に
よるYAGレーザを用いた方法によるとビード幅は約100μ
mと4分の1になった。iv) When the bead width of the welding was measured in the above example, the bead width obtained by butt-welding a SUS304 flat plate material having a plate thickness of 100 μm by TIG welding was about 400 μm. However, according to the method using the YAG laser according to the present invention, And the bead width is about 100μ
It became m and 1/4.
(2)板厚50μmのSUS304箔に対し、レーザビーム径1.
0mmφ、YAGレーザ出力30Wの条件で、本発明の変調出力Y
AGレーザと連続出力YAGレーザによりビードオンテスト
を行った。変調出力YAGレーザでは良好なビードを得ら
れる範囲が2.5m/min〜3.1m/minであったのに対し、連続
出力YAGレーザでは同範囲が2.9m/min〜3.1m/minとな
り、本発明の変調出力YAGレーザによるビードオンテス
トが連続出力YAGレーザによるビードオンテストに対し
て2倍以上の広範囲にわたり良好なビードを得ることが
出来た(第9図)。この事は、連続出力YAGレーザでは
溶け落ち、ハンピングが起きてしまう溶接条件下におい
ても変調出力YAGレーザを用いる事によりそれを防ぐ事
が出来る事を意味している。(2) Laser beam diameter of 1.
Under the conditions of 0 mmφ and YAG laser output of 30 W, the modulation output Y of the present invention
A bead-on test was performed with an AG laser and a continuous output YAG laser. In the modulated output YAG laser, the range in which a good bead was obtained was 2.5 m / min to 3.1 m / min, while in the continuous output YAG laser, the same range was 2.9 m / min to 3.1 m / min. The bead-on test using the modulated output YAG laser was more than twice as good as the bead-on test using the continuous output YAG laser, and good beads could be obtained over a wide range (Fig. 9). This means that even under welding conditions where continuous output YAG laser melts down and humping occurs, it can be prevented by using a modulated output YAG laser.
[発明の効果] 本発明の方法及び装置により以下のような効果を得る事
が出来る。[Effect of the Invention] The following effects can be obtained by the method and apparatus of the present invention.
変調出力YAGレーザを極薄金属箔の両端部の開先が開
いたところに低密度集光ビームで照射することで、従来
のTIG溶接法、レーザ溶接法では出来なかった板厚150μ
m以下の極薄金属箔の突き合せ溶接を溶け落ち、ハンピ
ング等の溶接欠陥なく行うことが出来る。By irradiating a modulated output YAG laser with a low-density focused beam to the places where the grooves on both ends of the ultra-thin metal foil are open, a plate thickness of 150μ, which was not possible with the conventional TIG welding method or laser welding method.
Butt welding of ultra-thin metal foils of m or less can be performed without melting defects such as humping and welding defects.
変調出力YAGレーザを極薄金属箔の両端部の開先が開
いたところに低密度集光ビームで照射することで、突き
合せ点で極薄金属箔を溶融させる場合に比べつき合う範
囲が広くなるのでオフセットの条件(従来は板厚の10%
以下)を緩和することが出来る。By irradiating the modulated output YAG laser with a low-density focused beam where the grooves on both ends of the ultra-thin metal foil are opened, the contact area becomes wider than when melting the ultra-thin metal foil at the butt point. So offset condition (previously 10% of plate thickness
The following) can be relaxed.
変調出力YAGレーザにより従来のレーザ溶接法では溶
け落ち、ハンピング等が起きる溶接条件の下でも、それ
らを起こす事無く溶接を行う事が出来る。With the modulated output YAG laser, welding can be performed under the welding conditions such as burn-through and humping that occur in the conventional laser welding method without causing them.
以上、本発明によって従来は得られなかった様な極薄の
金属箔のパイプの溶接が溶け落ち、溶接欠陥を発生させ
ることなく安定して得られた。As described above, according to the present invention, the welding of the pipe of the ultra-thin metal foil which has not been obtained in the past can be stably obtained without melting and welding defects.
第1図は極薄金属箔の鋼管への成形の概念図である。第
2図はYAGレーザビームの集光状態、照射法の概念を示
した斜視図である。第3図は第2図の平面図である。第
4図は本発明の変調出力YAGレーザの出力特性の概念図
である。第5図は本発明による極薄金属箔のパイプへの
成形・溶接時の成形条件の緩和を示す模式図である。第
6図は本発明の実施に用いた装置例の概略図である。第
7図(a)(b)は実施例で用いた試験編の側面図と正
面図である。第8図は本発明実施例の実験の態様の正面
図である。第9図は本発明実施例のビードオンテストの
結果を示すグラフである。第10図は本発明による変調出
力YAGレーザ発振機の励起用ランプ電源回路のブロック
ダイアグラムである。第11図は本発明実施例に用いた2
本のランプを用いたレーザ構造を示す模式図である。 1……極薄金属箔、2……端部、3……端面、4……変
調出力YAGレーザ照射位置、5……変調出力YAGレーザビ
ーム、6……レンズ、7……低密度集光変調出力YAGレ
ーザビーム、8……変更出力YAGレーザビームスポッ
ト、9……溶接位置、10……溶融状態部、11……溶接ビ
ード、18……SCR制御回路定電流制御部、19……トリガ
ー発生回路、20……ブースト電圧発生回路、21……パル
ス発振部、22……FET、23……パルストランス、24……Y
AGロッド、25……アークランプ、26……楕円集光器、27
……共振器リアミラー、28……共振器出力ミラー、29…
…定電流ランプ電源、D……照射スポット径、d……溶
融幅、g……開先ギャップ、PC……変調出力連続発振部
出力値、PP……変調出力パルス部ピーク出力値、Pav…
…変調出力平均出力値。FIG. 1 is a conceptual diagram of forming an ultrathin metal foil into a steel pipe. FIG. 2 is a perspective view showing the concept of the irradiation method and the condensed state of the YAG laser beam. FIG. 3 is a plan view of FIG. FIG. 4 is a conceptual diagram of the output characteristics of the modulated output YAG laser of the present invention. FIG. 5 is a schematic diagram showing relaxation of forming conditions during forming / welding of an ultrathin metal foil to a pipe according to the present invention. FIG. 6 is a schematic diagram of an example of an apparatus used for implementing the present invention. 7 (a) and 7 (b) are a side view and a front view of the test piece used in the examples. FIG. 8 is a front view of the experimental mode of the embodiment of the present invention. FIG. 9 is a graph showing the results of the bead-on test of the example of the present invention. FIG. 10 is a block diagram of an exciting lamp power supply circuit of a modulation output YAG laser oscillator according to the present invention. FIG. 11 shows 2 used in the embodiment of the present invention.
It is a schematic diagram which shows the laser structure using the lamp of a book. 1 ... Ultra-thin metal foil, 2 ... Edge, 3 ... Edge, 4 ... Modulation output YAG laser irradiation position, 5 ... Modulation output YAG laser beam, 6 ... Lens, 7 ... Low density condensing Modulation output YAG laser beam, 8 …… Change output YAG laser beam spot, 9 …… Welding position, 10 …… Melting state part, 11 …… Welding bead, 18 …… SCR control circuit Constant current control part, 19 …… Trigger Generator circuit, 20 ... Boost voltage generator circuit, 21 ... Pulse oscillator, 22 ... FET, 23 ... Pulse transformer, 24 ... Y
AG rod, 25 ... Arc lamp, 26 ... Elliptical concentrator, 27
…… Resonator rear mirror, 28 …… Resonator output mirror, 29…
... constant current lamp power supply, D ... irradiation spot diameter, d ... melting width, g ... groove gap, P C ... modulation output continuous oscillation part output value, P P ... modulation output pulse part peak output value, P av ...
... Modulation output average output value.
Claims (3)
き合わせ端面を楔形状に収束させ、収束部近傍にレーザ
ビームを照射して突き合わせ部を溶接するYAGレーザに
よる極薄金属箔パイプの製造方法において、連続レーザ
出力にパルスレーザ出力を重畳させた変調出力を発する
YAGレーザにて溶接する事を特徴とする変調出力YAGレー
ザによる極薄金属パイプ製造方法。1. An ultra-thin metal foil pipe using a YAG laser for continuously forming an ultra-thin metal foil, converging opposing butting end faces into a wedge shape, and irradiating a laser beam in the vicinity of the converging portion to weld the abutting portion. In the manufacturing method of, a modulated output is generated by superimposing a pulsed laser output on a continuous laser output.
A method for manufacturing an ultra-thin metal pipe using a modulated output YAG laser, which is characterized by welding with a YAG laser.
1倍以上5倍以下になる点に低密度集光YAGレーザビー
ムの中心を一致させて照射し、端部から板厚の2〜10倍
の領域を溶融し、溶融端面を凝固直前に押し付けて溶接
する請求項1に記載の変調出力YAGレーザによる極薄金
属パイプの製造方法。2. The low-density focused YAG laser beam is irradiated with its center aligned with a point where the gap of the wedge-shaped portion becomes 1 to 5 times the sheet thickness of the ultrathin metal foil, and the sheet thickness starts from the edge. 2. A method for producing an ultra-thin metal pipe by a modulation output YAG laser according to claim 1, wherein a region 2 to 10 times larger than that of FIG.
き合わせ端面を楔形状に収束させる成形装置と、該楔形
状部にレーザを照射する溶接装置からなる極薄金属箔パ
イプの製造装置において、ランプに対してそれぞれ並列
に接続されたランプ点火用トリガー回路を含むシマー電
源部と、干渉を抑制するためにパルストランスを介した
パルス電源部とを備え、連続レーザ出力にパルスレーザ
出力を重畳させた変調出力を発するレーザ発振機と、極
薄金属箔の収束部に形成する楔形状部を低密度集光YAG
レーザビームで照射する光学系とを備えたことを特徴と
するYAGレーザによる極薄金属パイプの製造装置。3. An ultrathin metal foil pipe comprising a forming device for continuously forming an ultrathin metal foil and converging opposing end faces into a wedge shape, and a welding device for irradiating the wedge-shaped portion with a laser. In the device, a simmer power supply unit including a lamp ignition trigger circuit connected in parallel to each lamp and a pulse power supply unit via a pulse transformer for suppressing interference are provided, and a pulse laser output is provided as a continuous laser output. A low-density YAG laser oscillator that emits a modulated output that superimposes
An apparatus for manufacturing an ultra-thin metal pipe using a YAG laser, which is provided with an optical system for irradiating with a laser beam.
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP2103089A JPH0771757B2 (en) | 1990-04-20 | 1990-04-20 | Method and apparatus for manufacturing ultra-thin metal pipe using modulated output YAG laser |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP2103089A JPH0771757B2 (en) | 1990-04-20 | 1990-04-20 | Method and apparatus for manufacturing ultra-thin metal pipe using modulated output YAG laser |
Publications (2)
| Publication Number | Publication Date |
|---|---|
| JPH044987A JPH044987A (en) | 1992-01-09 |
| JPH0771757B2 true JPH0771757B2 (en) | 1995-08-02 |
Family
ID=14344912
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP2103089A Expired - Lifetime JPH0771757B2 (en) | 1990-04-20 | 1990-04-20 | Method and apparatus for manufacturing ultra-thin metal pipe using modulated output YAG laser |
Country Status (1)
| Country | Link |
|---|---|
| JP (1) | JPH0771757B2 (en) |
-
1990
- 1990-04-20 JP JP2103089A patent/JPH0771757B2/en not_active Expired - Lifetime
Also Published As
| Publication number | Publication date |
|---|---|
| JPH044987A (en) | 1992-01-09 |
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