JPS6255958B2 - - Google Patents
Info
- Publication number
- JPS6255958B2 JPS6255958B2 JP3650281A JP3650281A JPS6255958B2 JP S6255958 B2 JPS6255958 B2 JP S6255958B2 JP 3650281 A JP3650281 A JP 3650281A JP 3650281 A JP3650281 A JP 3650281A JP S6255958 B2 JPS6255958 B2 JP S6255958B2
- Authority
- JP
- Japan
- Prior art keywords
- groove line
- electron beam
- welding
- tip
- welded
- 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
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
- B23K15/00—Electron-beam welding or cutting
- B23K15/02—Control circuits therefor
Landscapes
- Engineering & Computer Science (AREA)
- Mechanical Engineering (AREA)
- Welding Or Cutting Using Electron Beams (AREA)
- Length Measuring Devices Characterised By Use Of Acoustic Means (AREA)
Description
【発明の詳細な説明】
本発明は被溶接部の突合せ部に電子ビームを照
射して、被溶接部材を突合せ溶接する電子ビーム
溶接方法に係り、特に良好な接合状況を得ること
のできる電子ビーム溶接方法に関する。DETAILED DESCRIPTION OF THE INVENTION The present invention relates to an electron beam welding method for butt welding parts to be welded by irradiating an electron beam to the butt part of the parts to be welded. Regarding welding methods.
電子ビーム溶接法は、他の溶接法に比較して極
めて溶け込みが深くかつビード幅が狭いという大
きな特徴を有するため、厚板の大型構造物等への
利用も増々多くなつている。 Electron beam welding has the major characteristics of extremely deep penetration and narrow bead width compared to other welding methods, and is therefore increasingly being used for large structures made of thick plates.
しかし、該電子ビーム溶接法により、特に厚板
の突合せ溶接を行つた場合、該溶接部先端がいず
れか一方側の被溶接部材側に偏向されて、所望の
接合長さが得られなくなるという大きな欠点が生
ずる。 However, when butt welding of thick plates is performed using the electron beam welding method, the tip of the weld is deflected toward one of the welded parts, making it impossible to obtain the desired joint length. Defects arise.
即ち、第1図に示すように、電子ビーム1を被
溶接部材2及び3の開先線4に正確に入射しても
磁界または電界等の影響により、電子ビーム1が
一方の被溶接部材側に偏向され、該溶接部5の大
部分が開先線4から外れて、長さlの未溶着部を
生じ、所望の接合長さYが得られなくなる。 That is, as shown in FIG. 1, even if the electron beam 1 is accurately incident on the groove line 4 of the welded members 2 and 3, the electron beam 1 may be directed toward one of the welded members due to the influence of the magnetic field or electric field. As a result, most of the welded portion 5 deviates from the groove line 4, resulting in an unwelded portion of length l, making it impossible to obtain the desired joint length Y.
従来、このような未溶着部欠陥を防止する方法
として、反射電子検出装置または光学的検出装置
等の開先線検出装置を設けて、電子ビームを開先
線に正確に入射したり、また、溶接中に電子ビー
ムが開先線から外れないよう開先線倣い装置を溶
接装置に設けていた。しかし、これらの装置はい
ずれも溶接部材開先表面を基準としているもの
で、被溶接部材内部に未溶着部があつても溶接後
完全に冷却した被溶接材を非破壊検査するまで該
欠陥の検出は不可能であつた。一方、出願人は特
願昭54−29897で、超音波探傷検出器を用いて溶
接部先端の偏向を修正する方法を出願している
が、本法では溶接部先端が該検出器を設定してな
い被溶接部材側に偏向した場合に欠点がある。更
に、出願人は特願昭55−57856で溶接部先端がが
超音波検出器を設定している被溶接部材側に常時
基定値以下に偏向するよう電子ビームの照射位置
を制御する方法を出願しているが、本法では突合
せ面に対し、常に電子ビームを一定角度範囲だけ
傾けて照射しなければならないという制約があ
る。 Conventionally, as a method for preventing such defects in the unwelded area, a groove line detection device such as a backscattered electron detection device or an optical detection device is provided, and an electron beam is accurately incident on the groove line. The welding equipment was equipped with a groove line tracing device to prevent the electron beam from deviating from the groove line during welding. However, all of these devices are based on the groove surface of the welding part, so even if there is an unwelded part inside the welded part, the defect cannot be detected until the welded part is completely cooled after welding and is subjected to a non-destructive inspection. Detection was impossible. On the other hand, the applicant has applied for a method of correcting the deflection of the tip of the weld using an ultrasonic flaw detection detector in Japanese Patent Application No. 54-29897, but in this method, the tip of the weld does not set the detector. There is a drawback when the beam is deflected to the side of the workpiece that is not in contact with the weld. Furthermore, the applicant applied in Japanese Patent Application No. 55-57856 for a method of controlling the irradiation position of the electron beam so that the tip of the weld is always deflected below a reference value toward the workpiece to be welded where an ultrasonic detector is set. However, this method has a limitation in that the abutting surfaces must always be irradiated with the electron beam at an angle within a certain range.
本発明の目的は上述した欠点に鑑みなされたも
ので、所望の接合長さを安定確保できる電子ビー
ム溶接方法を提供するにある。 The object of the present invention was made in view of the above-mentioned drawbacks, and it is an object of the present invention to provide an electron beam welding method that can stably secure a desired joining length.
このような目的を達成するために、本発明は、
第1の開先線に沿つて電子ビームを照射し、それ
によつて被溶接材中に生じる溶接部と第1の開先
線との関係を超音波信号により監視しながら溶接
する方法において、溶融部または溶融凝固直後の
溶接部先端領域の反射信号が常時受信できるよう
に、溶接部先端近傍に、前記第1の開先線に対し
て所定間隔離間した位置に2の開先線を設けたこ
とを特徴とするものである。そして特に好ましく
は上記において該第2の開先線と、前記溶接部先
端との距離が、第1の開先線と第2の開先線間の
距離に常時等しくなるよう電子ビームの照射位置
あるいは角度の一方を制御するようにしたもので
ある。 In order to achieve such an objective, the present invention
A method of welding by irradiating an electron beam along the first groove line and monitoring the relationship between the welded part and the first groove line generated in the welded material using ultrasonic signals. A second groove line is provided near the tip of the weld at a predetermined distance from the first groove line so that reflected signals from the weld or the weld tip immediately after melting and solidification can be received at all times. It is characterized by this. Particularly preferably, in the above, the electron beam irradiation position is such that the distance between the second groove line and the tip of the welded part is always equal to the distance between the first groove line and the second groove line. Alternatively, one of the angles is controlled.
また、本発明は被溶接部材の側面から突合せ溶
接部に超音波信号を発振した場合、溶融部または
溶融凝固直後の特に該溶接部先端から、第2の開
先線のエコーレベルより比較的レベルの低い反射
信号が検出されることに着目し、該反射信号と前
記第2の開先線からの反射信号との超音波の時間
的偏差が溶接中常に一定値に維持されるよう電子
ビームの照射位置あるいは角度の一方を調整する
ようにしたものである。 Furthermore, when an ultrasonic signal is emitted from the side surface of the workpiece to the butt weld, the echo level from the molten part or especially from the tip of the weld immediately after melting and solidification is relatively lower than the echo level of the second groove line. Focusing on the fact that a low reflected signal of Either the irradiation position or the angle is adjusted.
以下、本発明を詳細に説明する。第2図a〜第
4図bは溶接部先端近傍に設けた第2の開先線と
溶接部先端の偏向状態並びに被溶接部材の側面に
配設した超音波発振―受信装置(トランスジユー
サ)からの反射信号との関係を示す。 The present invention will be explained in detail below. Figures 2a to 4b show the second groove line provided near the tip of the weld, the deflection state of the tip of the weld, and the ultrasonic oscillation-receiving device (transducer) installed on the side of the workpiece. ) shows the relationship with the reflected signal from
第2図a、第3図a及び第4図aに示すよう
に、所望の接合長さを確保するための第1の開先
線4の他に、溶接部先端近傍に、該第1の開先線
4に対して平行な状態で所定間隔離間した位置に
第2の開先線6を設けることにより、溶接部5の
先端(以下、溶接部先端5aと称する。)が第1
の開先線4から左右に偏向した場合でも、常に該
溶接部先端5aからの反射信号が受信できること
になる。 As shown in Fig. 2a, Fig. 3a, and Fig. 4a, in addition to the first groove line 4 for ensuring the desired joint length, there is a groove line 4 near the tip of the weld. By providing the second groove line 6 at a position parallel to the groove line 4 and separated by a predetermined distance, the tip of the welded portion 5 (hereinafter referred to as the welded portion tip 5a) becomes the first groove line.
Even if the weld is deflected from the groove line 4 to the left or right, the reflected signal from the weld tip 5a can always be received.
今、第2図aは溶接部先端5aが第1の開先線
4と一致し、溶接部先端5aの偏向が無い場合
で、この場合の超音波反射信号は、第2図bに示
すように第2の開先線6からの反射信号6′と前
記溶接部先端5aからの反射信号5′である。こ
の場合、各反射信号の時間差Δtを計算すること
により、第2の開先線6と溶接部先端5aとの距
離差Δxが容易に判定できることになる。ここ
で、溶接中に前記の時間差Δtから判定した距離
差Δxと、あらかじめ設定してある第1の開先線
4と第2の開先線6との距離差Δlとが等しけれ
ば、即ち、Δx〓Δlであるならば、該溶接部5
は第1の開先線4と一致していることが判定され
る。従つて、該溶接部先端5aの偏向は無く、所
望の接合長さが得られていることが容易に判定で
き、電子ビームの照射位置を調整する必要がな
い。 Now, Fig. 2a shows a case where the welding part tip 5a coincides with the first groove line 4 and there is no deflection of the welding part tip 5a, and the ultrasonic reflection signal in this case is as shown in Fig. 2b. , a reflected signal 6' from the second groove line 6 and a reflected signal 5' from the welding portion tip 5a. In this case, by calculating the time difference Δt of each reflected signal, the distance difference Δx between the second groove line 6 and the welding portion tip 5a can be easily determined. Here, if the distance difference Δx determined from the time difference Δt during welding is equal to the preset distance difference Δl between the first groove line 4 and the second groove line 6, that is, If Δx=Δl, the welded portion 5
is determined to coincide with the first groove line 4. Therefore, there is no deflection of the welding part tip 5a, and it can be easily determined that the desired joining length has been obtained, and there is no need to adjust the irradiation position of the electron beam.
また、第3図aは溶接部先端5aが第1の開先
線4から外れて、該トランスジユーサ7を設置し
ている方向と反対方向に偏向した場合である。こ
の場合も、第3図bに示すように第2の開先線6
からの超音波反射信号6′と、該溶接部先端5a
からの超音波反射信号5′が受信できる。ただ
し、この第3図の場合の時間差Δtは第2図の偏
向が無い場合に比べて小さくなる。このことか
ら、該距離差ΔxはΔlに比べて小さいことが容
易に判定され、従つて溶接部先端5aの偏向方向
並びに偏向量が容易に判定できることになるた
め、電子ビームの照射位置を調整する有力な情報
源となる。 Further, FIG. 3a shows a case where the welding part tip 5a has deviated from the first groove line 4 and is deflected in the opposite direction to the direction in which the transducer 7 is installed. In this case as well, as shown in FIG. 3b, the second groove line 6
The ultrasonic reflected signal 6' from the welding part tip 5a
It is possible to receive an ultrasonic reflected signal 5' from. However, the time difference Δt in the case of FIG. 3 is smaller than that in the case of no deflection as shown in FIG. From this, it can be easily determined that the distance difference Δx is smaller than Δl, and therefore the direction and amount of deflection of the welding part tip 5a can be easily determined, so the irradiation position of the electron beam is adjusted. Become a powerful source of information.
更に、第4図aは溶接部先端5aが第1の開先
線4から外れて、トランスジユーサ7を設置して
いる方向に偏向した場合である。この場合も第2
図及び第3図と同様に、第2の開先線6からの超
音波反射信号6′と該溶接部先端5aからの反射
信号5′が受信できるが、偏向量が大きく、未溶
着長さlが大きい場合には、第1の開先線4から
の反射信号4′も受信できることがある。ここ
で、第4図bの時間差Δtは第2図bの偏向がな
い場合に比べて大きくなり、このことから距離差
ΔxもΔlに比べて大きいことが容易に判定さ
れ、従つて、この場合も溶接部先端5aの偏向方
向並びに偏向量が容易に判定できることになる。 Furthermore, FIG. 4a shows a case where the welding part tip 5a deviates from the first groove line 4 and is deflected in the direction in which the transducer 7 is installed. In this case also the second
Similarly to FIG. 3, the ultrasonic reflection signal 6' from the second groove line 6 and the reflection signal 5' from the welding part tip 5a can be received, but the amount of deflection is large and the unwelded length is If l is large, the reflected signal 4' from the first groove line 4 may also be received. Here, the time difference Δt in FIG. 4b is larger than in the case without deflection in FIG. 2b, and from this it can be easily determined that the distance difference Δx is also larger than Δl. Also, the direction and amount of deflection of the welded portion tip 5a can be easily determined.
以上、前記した情報源をもとに第3図及び第4
図の場合には、溶接中常にΔxがΔlに等しくな
るよう電子ビームの照射位置あるいは角度の一方
を調節することにより、所望の接合長さを安定確
保できるものである。 Based on the above information sources, Figures 3 and 4
In the case shown in the figure, by adjusting either the irradiation position or the angle of the electron beam so that Δx always becomes equal to Δl during welding, the desired joining length can be stably ensured.
以下、本発明の実施例について説明する。 Examples of the present invention will be described below.
第5図aは本発明の実施例について示したもの
で、一方の被溶接部材にのみトランスジユーサ7
を配置した突合せ電子ビーム溶接において、該ト
ランスジユーサ7により検出した第2の開先線6
からの反射信号6′及び溶接部先端5aからの反
射信号5′は超音波探傷器8上で第5図bのごと
く表示される。 FIG. 5a shows an embodiment of the present invention, in which a transducer 7 is attached only to one of the members to be welded.
In butt electron beam welding in which the second groove line 6 detected by the transducer 7
The reflected signal 6' from the welding part tip 5a and the reflected signal 5' from the welding part tip 5a are displayed on the ultrasonic flaw detector 8 as shown in FIG. 5b.
第5図bのごとく表示された該2つの反射信号
は、時間差演算回路9により、5′と6′との時間
差Δtまたは距離差Δxを検出する。該回路によ
り検出された時間差または距離差は、電圧変換回
路10により、それらの時間差または距離差に比
例した電圧に変換される。更に、該電圧変換され
た出力は増幅器11を介して増幅される。該増幅
器11により増幅された出力は、該距離差Δlの
電圧信号、即ち、基準電圧12とほぼ同じ値にな
るよう電子ビーム1の照射位置を制御する比較器
13に入力され、該比較器13からの出力信号は
該基準電圧12より大きいかまたは小さい場合に
のみ出力し、電子ビーム1の照射位置を制御する
制御回路14を作動するスイツチング回路14′
に入力される。該制御回路14からの出力信号
は、電子ビーム1を第1の開先線4を中心に左右
に偏向する直流偏向コイル電源15を制御し、溶
接部先端5aが溶接中常に第1の開先線4と一致
するように電子ビーム1の照射位置を自動的に制
御するようにしたものである。ここで、16は偏
向コイルで、17は電子銃である。 The time difference calculating circuit 9 detects the time difference Δt or the distance difference Δx between the two reflected signals 5' and 6' as shown in FIG. 5b. The time difference or distance difference detected by the circuit is converted by the voltage conversion circuit 10 into a voltage proportional to the time difference or distance difference. Further, the voltage-converted output is amplified via an amplifier 11. The output amplified by the amplifier 11 is input to a comparator 13 that controls the irradiation position of the electron beam 1 so that it becomes a voltage signal of the distance difference Δl, that is, approximately the same value as the reference voltage 12. A switching circuit 14' outputs an output signal from the reference voltage 12 only when it is larger or smaller than the reference voltage 12, and operates a control circuit 14 that controls the irradiation position of the electron beam 1.
is input. The output signal from the control circuit 14 controls a DC deflection coil power supply 15 that deflects the electron beam 1 to the left and right around the first groove line 4, so that the welding part tip 5a always remains in the first groove line during welding. The irradiation position of the electron beam 1 is automatically controlled so as to match the line 4. Here, 16 is a deflection coil, and 17 is an electron gun.
尚、本実施例における所望の長さはYが50mmで
あつたので、溶込み先端部までの深さを55mmと
し、更に第1の開先線4と第2の開先線6との距
離差は3mmとした。 In this example, the desired length Y was 50 mm, so the depth to the penetration tip was 55 mm, and the distance between the first groove line 4 and the second groove line 6 was The difference was 3 mm.
前記本発明の実施例により、溶接長さ3mの全
長にわたり所望の接合長さ50mmを確保できた。ま
た、裏側も同様の方法により溶接を行なつた。 According to the embodiment of the present invention, a desired joint length of 50 mm could be secured over the entire weld length of 3 m. Further, the back side was also welded using the same method.
尚、本実施例では電子ビーム1の照射位置を自
動制御しているか、超音波探傷器8に表示された
該時間差Δtを目視により読みとり、手動によつ
て電子ビーム1の照射位置を制御してもよいこと
は勿論である。 In this embodiment, the irradiation position of the electron beam 1 is automatically controlled, or the time difference Δt displayed on the ultrasonic flaw detector 8 is visually read and the irradiation position of the electron beam 1 is manually controlled. Of course, this is a good thing.
また、本実施例では該トランスジユーサ7を被
溶接部材の側面に1個配設し、側面から超音波を
発振する垂直探傷法を採用したが、被溶接部材の
表面または裏面に該トランスジユーサを複数個配
設した斜角探傷法の採用によつても本目的を達成
できる。 In addition, in this embodiment, one transducer 7 is disposed on the side surface of the workpiece to be welded, and a vertical flaw detection method in which ultrasonic waves are emitted from the side surface is adopted. This objective can also be achieved by adopting the angle angle flaw detection method in which multiple users are arranged.
以上説明したように、本発明においては、溶接
部先端を溶接中常に追跡しながら溶接するので、
信頼性のある溶接部が得られるという大きな特徴
がある。 As explained above, in the present invention, the tip of the welded part is constantly tracked during welding, so
A major feature is that reliable welds can be obtained.
第1図は電子ビーム溶接部に発生する偏向例を
説明する断面図、第2図a,b、第3図a,b及
び第4図a,bはそれぞれ電子ビーム溶接部と超
音波エコーとを示す図、第5図aは本発明の実施
例を示す一部断面略図、第5図bは実施例におけ
る超音波エコーを示す図である。
1……電子ビーム、2,3……被溶接部材、4
……第1の開先線、5……溶接部、5a……溶接
部先端、6……第2の開先線。
Fig. 1 is a cross-sectional view illustrating an example of deflection occurring in an electron beam weld, Fig. 2 a, b, Fig. 3 a, b, and Fig. 4 a, b are the electron beam weld and an ultrasonic echo, respectively. FIG. 5a is a schematic partial cross-sectional view showing an embodiment of the present invention, and FIG. 5b is a diagram showing an ultrasonic echo in the embodiment. 1... Electron beam, 2, 3... Member to be welded, 4
...First groove line, 5... Welded part, 5a... Welded part tip, 6... Second groove line.
Claims (1)
それによつて被溶接材中に生じる溶接部と第1の
開先線との関係を超音波信号により監視しながら
溶接する方法において、溶融部または溶融凝固直
後の溶接部先端領域の反射信号が常時受信できる
ように、溶接部先端近傍に、前記第1の開先線に
対して所定間隔離間した位置に第2の開先線を設
けたことを特徴とする電子ビーム溶接方法。 2 溶融部または溶融凝固直後の溶接部先端から
の反射信号と、前記第2の開先線からの反射信号
を検出し、該2つの反射信号の時間的偏差が溶接
中常に一定値に維持されるように電子ビームの照
射位置あるいは角度の一方を調整しながら溶接す
ることを特徴とする特許請求の範囲第1項記載の
電子ビーム溶接方法。[Claims] 1. Irradiating an electron beam along the first groove line,
In the method of welding while monitoring the relationship between the weld zone and the first groove line generated in the welded material using ultrasonic signals, the reflected signal of the molten zone or the weld zone tip area immediately after melting and solidification is constantly reflected. An electron beam welding method characterized in that a second groove line is provided near the tip of the welding part at a predetermined distance from the first groove line so as to be able to receive the electron beam. 2. Detecting the reflected signal from the molten part or the tip of the welded part immediately after melting and solidification, and the reflected signal from the second groove line, and ensuring that the temporal deviation of the two reflected signals is always maintained at a constant value during welding. 2. The electron beam welding method according to claim 1, wherein the welding is performed while adjusting either the irradiation position or the angle of the electron beam so that the electron beam irradiation position or angle is adjusted.
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP3650281A JPS57152383A (en) | 1981-03-16 | 1981-03-16 | Electron beam welding method |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP3650281A JPS57152383A (en) | 1981-03-16 | 1981-03-16 | Electron beam welding method |
Publications (2)
| Publication Number | Publication Date |
|---|---|
| JPS57152383A JPS57152383A (en) | 1982-09-20 |
| JPS6255958B2 true JPS6255958B2 (en) | 1987-11-24 |
Family
ID=12471592
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP3650281A Granted JPS57152383A (en) | 1981-03-16 | 1981-03-16 | Electron beam welding method |
Country Status (1)
| Country | Link |
|---|---|
| JP (1) | JPS57152383A (en) |
Families Citing this family (1)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| JPH0690021B2 (en) * | 1985-10-31 | 1994-11-14 | 日本鋼管株式会社 | Electrode positioning method for potential difference measurement |
-
1981
- 1981-03-16 JP JP3650281A patent/JPS57152383A/en active Granted
Also Published As
| Publication number | Publication date |
|---|---|
| JPS57152383A (en) | 1982-09-20 |
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