JPH03476A - Tig welding method - Google Patents

Tig welding method

Info

Publication number
JPH03476A
JPH03476A JP13455589A JP13455589A JPH03476A JP H03476 A JPH03476 A JP H03476A JP 13455589 A JP13455589 A JP 13455589A JP 13455589 A JP13455589 A JP 13455589A JP H03476 A JPH03476 A JP H03476A
Authority
JP
Japan
Prior art keywords
arc length
welding
region
arc
penetration depth
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
Application number
JP13455589A
Other languages
Japanese (ja)
Other versions
JP2744806B2 (en
Inventor
Tsuneo Mita
常夫 三田
Takayuki Kashima
孝之 鹿島
Yoshifumi Yamanaka
山中 善文
Current Assignee (The listed assignees may be inaccurate. Google has not performed a legal analysis and makes no representation or warranty as to the accuracy of the list.)
Via Mechanics Ltd
Original Assignee
Hitachi Seiko Ltd
Priority date (The priority date 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 date listed.)
Filing date
Publication date
Application filed by Hitachi Seiko Ltd filed Critical Hitachi Seiko Ltd
Priority to JP13455589A priority Critical patent/JP2744806B2/en
Publication of JPH03476A publication Critical patent/JPH03476A/en
Application granted granted Critical
Publication of JP2744806B2 publication Critical patent/JP2744806B2/en
Anticipated expiration legal-status Critical
Expired - Lifetime legal-status Critical Current

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  • Arc Welding In General (AREA)

Abstract

PURPOSE:To obtain an uniform weld bead by setting the arc length in the region where the arc length is longer than the region where the arc length is in proportion to the depth of penetration and the depth of penetration is not changed by the arc length. CONSTITUTION:Nonconsumable electrode arc welding is performed by using a welding power source having an almost constant-current characteristic. The arc length is then set in the second region where the arc length is longer than the first region where the arc length is approximately in inverse proportion to the depth of penetration and the depth of penetration is hardly changed by the arc length. In addition, the arc length is set in the third region where the arc length is longer than the second region and the depth of penetration is approximately in proportion to the arc length. By this method, a drop of a welding current due to resistance heat generation of an electrode is suppressed and fine welding is performed.

Description

【発明の詳細な説明】 〔産業上の利用分野〕 本発明はティグ溶接方法に係り、特にアルミニウムまた
はアルミニウム合金などの交流ティグ溶接に好適な方法
に関するものである。
DETAILED DESCRIPTION OF THE INVENTION [Industrial Application Field] The present invention relates to a TIG welding method, and particularly to a method suitable for AC TIG welding of aluminum or aluminum alloys.

〔従来の技術〕[Conventional technology]

アーク溶接における溶込み深さに及ぼす溶接条件の影響
を表わす式としては、安藷、長谷用;「溶接アーク現象
」増補版、産報出版(1967年)p、 368〜36
9に掲載されているJ acksonO式、溶込み深さ
=ki、l’iてπ=八へン一ここで k:溶接方法に
よって定まる定数■;溶接電流 V:溶接速度 Vmiアーク電圧 が広く知られており、電流■が小さいほど、溶接速度V
が速いほど、またアーク電圧V、(アーク長)が高い(
長い)はど、溶込み深さが減少することを示している。
The formula expressing the influence of welding conditions on the penetration depth in arc welding is given by Yasutoshi and Hase, "Welding Arc Phenomena" expanded edition, Sanpo Publishing (1967), p. 368-36.
According to the Jackson O formula published in 9, penetration depth = ki, l'i and π = 8, where k: constant determined by the welding method; welding current V: welding speed Vmi arc voltage is widely known. , and the smaller the current ■, the welding speed V
The faster the arc voltage V, (arc length) is, the higher the arc voltage V (arc length) is (
(long) indicates that the penetration depth decreases.

溶込み深さに及ぼすこのような溶接条件の影響について
は、例えば横尾、三田、渡辺;「ティグ溶接入門」産報
出版(1986年)p、 80〜83、(社)軽金属協
会編;「アルミニウムハンドブックJ Rt)軽金属協
会(昭和56年) p、 115〜116などにも記載
されている。
Regarding the influence of welding conditions on the penetration depth, see, for example, Yokoo, Mita, Watanabe, "Introduction to TIG Welding", Sanpo Publishing (1986), p. 80-83, edited by the Light Metals Association of Japan, "Aluminum It is also described in Handbook JRt) Light Metals Association (1981) p. 115-116.

すなわち、溶接電流、溶接速度を一定とした溶接では、
アーク長(アーク電圧)を長く (高く)するほど溶込
み深さは浅くなるとされている。
In other words, when welding with constant welding current and welding speed,
It is said that the longer (higher) the arc length (arc voltage), the shallower the penetration depth.

〔発明が解決しようとする課題〕[Problem to be solved by the invention]

従来、ティグ溶接においては、前記J acksonの
式が成立する範囲内に溶接条件を設定し、比較的短いア
ーク長(アルミニウムやアルミニウム合金の溶接では約
3ms程度)で溶接を行っていたため、低電流域では手
ぶれ等によるアーク長の変動の影響を大きく受けて溶込
み深さが変化し、均一な溶接ビードが得にくかった。ま
た、狭隘な場所や深い開先などで溶接線にトーチを近付
けにくい場合には、アーク長を短く保つために電極突出
し長を長くしており、その結果、電極の抵抗発熱により
電極の溶断電流が低くなり、溶接電流値が制限されてし
まう。また、従来の方法では、溶接電流を大きくしても
得られる溶込み深さに限界があった。
Conventionally, in TIG welding, welding conditions were set within the range where Jackson's equation holds true, and welding was performed with a relatively short arc length (approximately 3 ms for welding aluminum and aluminum alloys). In the area, the penetration depth changes due to changes in the arc length due to camera shake, making it difficult to obtain a uniform weld bead. In addition, when it is difficult to get the torch close to the welding line in a narrow space or deep groove, the electrode protrusion length is increased to keep the arc length short. becomes low, and the welding current value is limited. Further, in the conventional method, there is a limit to the penetration depth that can be obtained even if the welding current is increased.

本発明の目的は、従来知られていないアーク長と溶込み
深さの関係を利用して上記問題点を解決し、アルミニウ
ムやアルミニウム合金などのアーク溶接作業性、溶接品
質を改善する方法を提供することにある。
The purpose of the present invention is to provide a method for solving the above problems by utilizing the previously unknown relationship between arc length and penetration depth, and improving workability and welding quality for arc welding of aluminum, aluminum alloys, etc. It's about doing.

〔課題を解決するための手段〕[Means to solve the problem]

略定電流特性の溶接電流を用いて行う非消耗電極式アー
ク溶接において、溶接電流、溶接速度を一定としてアー
ク長を変化させると、アーク長とアーク電圧の間には第
2図のような関係が成立する。また、アークによる母材
への入熱は〔電流×電圧×効率〕であるから、溶接電流
を一定とした場合の母材への入熱は、アーク電圧と同様
にアーク長の変化とともに第3図のように変化する。
In non-consumable electrode arc welding using a welding current with approximately constant current characteristics, when the welding current and welding speed are kept constant and the arc length is varied, the relationship between the arc length and arc voltage is as shown in Figure 2. holds true. Also, since the heat input to the base metal by the arc is [current × voltage × efficiency], when the welding current is constant, the heat input to the base metal changes as the arc length changes. It changes as shown in the figure.

一方、母材に加えられるアーク圧力は、アーク長の増加
とともに第4図のように減少する。
On the other hand, the arc pressure applied to the base metal decreases as the arc length increases, as shown in FIG.

アーク溶接における母材の溶込み深さは、母材に加えら
れる入熱と母材を堀り下げる力すなわちアーク圧力によ
って決定されると考えられる。よって、溶込み深さPD
は上記入熱W、とアーク圧力P、を用いて、 P D = a W、+ b P、+ c(a、b、c
:溶接条件など決まる定数)と表わすことができ、第3
図および第4図からアーク長と溶込み深さの間には第1
図のような関係が成立することになる。すなわち、アー
ク長と溶込み深さが略反比例する公知の領域A(第1の
領域)のほかに、溶込み深さがアーク長によってほとん
ど変動しない領域B(第2の領域)および溶込み深さと
アーク長が略比例する領域C(第3の領域)が存在する
The penetration depth of the base metal in arc welding is considered to be determined by the heat input applied to the base metal and the force that excavates the base metal, that is, the arc pressure. Therefore, penetration depth PD
Using the above heat input W and arc pressure P, P D = a W, + b P, + c (a, b, c
: constant determined by welding conditions, etc.), and the third
From Fig. 4 and Fig. 4, there is a difference between arc length and penetration depth.
The relationship shown in the figure will be established. That is, in addition to the well-known region A (first region) where the arc length and penetration depth are approximately inversely proportional, there is also a region B (second region) where the penetration depth hardly changes depending on the arc length and the penetration depth. There is a region C (third region) where the arc length and the arc length are approximately proportional.

このような新知見に基づき、請求項1記載の発明は、上
記第1の領域Aよりアーク長が長く、溶込み深さがアー
ク長によってほとんど変動しない第2の領域Bに、アー
ク長を設定することを特徴とする。
Based on such new knowledge, the invention according to claim 1 sets the arc length in a second region B, which has a longer arc length than the first region A and whose penetration depth hardly changes depending on the arc length. It is characterized by

また、請求項2記載の発明は、上記第2の領域Bよりア
ーク長が長く、溶込み深さとアーク長が略比例する第3
の領域Cに、アーク長を設定することを特徴とする。
Further, the invention according to claim 2 provides a third region having a longer arc length than the second region B, and in which the penetration depth and the arc length are approximately proportional.
The arc length is set in region C of .

〔実施例〕〔Example〕

以下、本発明の実施例を第5図および第6図を用いて説
明する。
Embodiments of the present invention will be described below with reference to FIGS. 5 and 6.

第5図は、略定電流特性の溶接電源(無負荷電圧40V
)を用い、溶接電流100A、溶接速度300mu /
 m t n %シールドガスA r ・10 II 
/minで板厚3龍のアルミニウム合金A 5052の
交流ティグ溶接を行った場合のアーク長と溶込み深さの
関係を示したものである。本例において、アーク長が4
n以下の場合には、アーク長の増加とともに溶込み深さ
は減少するが、アーク長を4〜5鶴程度にすると、溶込
み深さはほとんど変化しなかった。また、アーク長を6
f1以上にすると、アーク長の増加とともに溶込み深さ
が増加し、アーク長と溶込み深さが略反比例する公知の
領域よりも深い溶込みを得ることができた。
Figure 5 shows a welding power source with approximately constant current characteristics (no-load voltage 40V).
), welding current 100A, welding speed 300mu/
m t n % shielding gas A r ・10 II
This figure shows the relationship between arc length and penetration depth when AC TIG welding is performed on aluminum alloy A 5052 with a plate thickness of 3. In this example, the arc length is 4
In the case of n or less, the penetration depth decreased as the arc length increased, but when the arc length was set to about 4 to 5 cranes, the penetration depth hardly changed. Also, the arc length is 6
When f1 or more, the penetration depth increases as the arc length increases, and it was possible to obtain deeper penetration than in the known region where arc length and penetration depth are approximately inversely proportional.

第6図は、上記と同一の溶接電源を用い、溶接電流20
OA、溶接速度250m5/min、シールドガスA 
r ・1!M/winで板厚5龍のアルミニウムAl1
00の交流ティグ溶接を行った場合のアーク長と溶込み
深さの関係を示す。本例でも、前記第5図の例と同様に
、アーク長が4〜6fl程度では溶込み深さはほとんど
変化せず、アーク長を6f1以上にすると、アーク長の
増加とともに溶込み深さが増加し、公知の領域(アーク
長41■以下)よりも深い溶込みを得ることができた。
Figure 6 shows a welding current of 20% using the same welding power source as above.
OA, welding speed 250m5/min, shielding gas A
r・1! Aluminum Al1 with M/win plate thickness of 5 dragons
2 shows the relationship between arc length and penetration depth when AC TIG welding is performed. In this example, as well as the example shown in Fig. 5, the penetration depth hardly changes when the arc length is about 4 to 6 fl, and when the arc length is 6 fl or more, the penetration depth increases as the arc length increases. It was possible to obtain deeper penetration than the known range (arc length of 41 cm or less).

上記実施例では、アーク長によって溶込み深さがほとん
ど変化しない領域は、いずれもアーク長が4〜61mの
領域となっているが、この値は、板厚や溶接条件によっ
て異なることは言うまでもない。
In the above examples, the area where the penetration depth hardly changes depending on the arc length is the area where the arc length is 4 to 61 m, but it goes without saying that this value varies depending on the plate thickness and welding conditions. .

また、上記実施例は溶接に用いる交流周波数を商用周波
数(50Hz)とした場合であるが、これに限定される
ことはなく、より高い、あるいは低い周波数を採用して
も、本発明の作用が損われることはない。
Furthermore, although the above embodiments are based on the case where the AC frequency used for welding is a commercial frequency (50 Hz), the present invention is not limited to this, and even if a higher or lower frequency is adopted, the effect of the present invention can still be achieved. It won't be damaged.

なお、第1図に示すアーク長と溶込み深さの関係は、交
流ティグ溶接だけでなく、直流ティグ溶接においても近
似的に成立する。所定の溶込み深さを得るために必要な
母材入熱、したがってアーク長は母材の材W(融点)に
よって異なるが、それに応じた無負荷電圧を持つ溶接電
源を使用すれば、アルミニウムやアルミニウム合金以外
の材料を対象とする直流ティグ溶接においても本発明の
適用が可能である。
Note that the relationship between arc length and penetration depth shown in FIG. 1 approximately holds true not only in AC TIG welding but also in DC TIG welding. The base metal heat input and therefore the arc length required to obtain a predetermined penetration depth vary depending on the base material W (melting point), but if a welding power source with a no-load voltage corresponding to the welding power source is used, aluminum or The present invention can also be applied to DC TIG welding for materials other than aluminum alloys.

〔発明の効果〕〔Effect of the invention〕

請求項1記載の発明によれば、アーク長が多少変化して
も溶込み深さがほとんど変動しない溶接ができるため、
手ぶれや母材位置の変動による影響を受けずに均一な溶
接ビードを得ることができる。
According to the invention set forth in claim 1, it is possible to perform welding in which the penetration depth hardly changes even if the arc length changes slightly.
A uniform weld bead can be obtained without being affected by camera shake or changes in the base metal position.

一方、請求項2記載の発明によれば、アーク長を長くす
るほど溶込み深さが増加する溶接ができるため、従来よ
りも深い溶込みを得ることができ、また溶接線にトーチ
を近付けにくい場合でも従来・のように電極突出し長さ
を長くする必要がなく、したがって電極の抵抗発熱によ
る溶断電流の低下を抑え、良好な溶接ができるという効
果がある。
On the other hand, according to the invention described in claim 2, it is possible to perform welding in which the penetration depth increases as the arc length becomes longer, so it is possible to obtain deeper penetration than conventionally, and it is difficult to bring the torch close to the weld line. Even in this case, there is no need to increase the protruding length of the electrode as in the conventional method, and therefore the reduction in fusing current due to resistance heating of the electrode can be suppressed, resulting in good welding.

【図面の簡単な説明】[Brief explanation of the drawing]

第1図は本発明のティグ溶接方法におけるアーク長と溶
込み深さの関係を示す線図、第2図〜第4図は本発明の
詳細な説明するための線図、第5図および第6図は本発
明の実施例を示す線図である。 l・・・アーク長、■1・・・アーク電圧、W3・・・
母材入熱、P、・・・アーク圧力、PD・・・溶込み深
さ、A、B、C・・・lとPDの関係の分類を示す領域
、a、b、c・・・PDを決定する定数。 第1図 第2図
Fig. 1 is a diagram showing the relationship between arc length and penetration depth in the TIG welding method of the present invention, Figs. 2 to 4 are diagrams for explaining the present invention in detail, and Figs. FIG. 6 is a diagram showing an embodiment of the present invention. l...Arc length, ■1...Arc voltage, W3...
Base metal heat input, P... arc pressure, PD... penetration depth, A, B, C... area indicating the classification of the relationship between l and PD, a, b, c... PD A constant that determines. Figure 1 Figure 2

Claims (1)

【特許請求の範囲】 1、略定電流特性の溶接電源を用いて行う非消耗電極式
アーク溶接において、アーク長と溶込み深さが略反比例
する第1の領域よりアーク長が長く、溶込み深さがアー
ク長によってほとんど変動しない第2の領域に、アーク
長を設定することを特徴とするティグ溶接方法。 2、略定電流特性の溶接電源を用いて行う非消耗電極式
アーク溶接において、上記第2の領域よりアーク長が長
く、溶込み深さとアーク長が略比例する第3の領域に、
アーク長を設定することを特徴とするティグ溶接方法。
[Claims] 1. In non-consumable electrode arc welding performed using a welding power source with substantially constant current characteristics, the arc length is longer than the first region where the arc length and penetration depth are substantially inversely proportional, and the penetration depth is A TIG welding method characterized in that the arc length is set in a second region where the depth hardly changes depending on the arc length. 2. In non-consumable electrode arc welding performed using a welding power source with approximately constant current characteristics, a third region where the arc length is longer than the second region and where the penetration depth and arc length are approximately proportional,
A TIG welding method characterized by setting the arc length.
JP13455589A 1989-05-30 1989-05-30 Tig welding method Expired - Lifetime JP2744806B2 (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP13455589A JP2744806B2 (en) 1989-05-30 1989-05-30 Tig welding method

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP13455589A JP2744806B2 (en) 1989-05-30 1989-05-30 Tig welding method

Publications (2)

Publication Number Publication Date
JPH03476A true JPH03476A (en) 1991-01-07
JP2744806B2 JP2744806B2 (en) 1998-04-28

Family

ID=15131062

Family Applications (1)

Application Number Title Priority Date Filing Date
JP13455589A Expired - Lifetime JP2744806B2 (en) 1989-05-30 1989-05-30 Tig welding method

Country Status (1)

Country Link
JP (1) JP2744806B2 (en)

Cited By (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JP2021079431A (en) * 2019-11-22 2021-05-27 株式会社Ihi Angle estimation method for heat-affected zone of metallic component
JP2021079430A (en) * 2019-11-22 2021-05-27 株式会社Ihi Arc penetration depth estimation method

Cited By (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JP2021079431A (en) * 2019-11-22 2021-05-27 株式会社Ihi Angle estimation method for heat-affected zone of metallic component
JP2021079430A (en) * 2019-11-22 2021-05-27 株式会社Ihi Arc penetration depth estimation method

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JP2744806B2 (en) 1998-04-28

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