JP2020116630A - Indirect spot welding method - Google Patents

Indirect spot welding method Download PDF

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JP2020116630A
JP2020116630A JP2019012247A JP2019012247A JP2020116630A JP 2020116630 A JP2020116630 A JP 2020116630A JP 2019012247 A JP2019012247 A JP 2019012247A JP 2019012247 A JP2019012247 A JP 2019012247A JP 2020116630 A JP2020116630 A JP 2020116630A
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welding
metal plate
current
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resistance value
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JP6903386B2 (en
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圭一郎 木許
Keiichiro Kimoto
圭一郎 木許
知嗣 加藤
Tomotsugu Kato
知嗣 加藤
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Daihatsu Motor Co Ltd
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Abstract

To provide an indirect spot welding method, in which quality of each welding during actual welding is quantitatively evaluated.SOLUTION: An indirect spot welding method, in which an overlapped part P between a first metal plate 1 and a third metal plate 3 is pressurized by a welding electrode 10 and an earth electrode 20 is contacted with a site different from the overlapped part P so as to carry currents between both electrodes, includes a step of carrying currents between both electrodes without hardly pressurizing the overlapped part P by the welding electrode 10 at the early stage of welding.SELECTED DRAWING: Figure 2

Description

本発明は、インダイレクトスポット溶接方法に関する。 The present invention relates to an indirect spot welding method.

自動車の組立工程では、金属板からなる複数の部品をスポット溶接で接合することにより車体が組み立てられる。スポット溶接としては、複数の金属板を一対の電極で挟み込んで通電するダイレクトスポット溶接が多く用いられる。しかし、部品の形状によっては、複数の金属板を一対の電極で挟み込むことができず、ダイレクトスポット溶接を適用することができないことがある。この場合、複数の金属板の重合部を溶接電極で加圧すると共に、重合部と異なる部位にアース電極を当接させた状態で両電極間に通電することにより溶接するインダイレクトスポット溶接が適用される。 In a vehicle assembly process, a vehicle body is assembled by joining a plurality of metal plates by spot welding. As spot welding, direct spot welding in which a plurality of metal plates are sandwiched between a pair of electrodes and electricity is applied is often used. However, depending on the shape of the component, it may not be possible to sandwich a plurality of metal plates with a pair of electrodes, and direct spot welding may not be applicable. In this case, indirect spot welding is applied in which the overlapped portion of a plurality of metal plates is pressed by a welding electrode, and welding is performed by energizing between the electrodes in a state where the earth electrode is in contact with a portion different from the overlapped portion. It

しかし、インダイレクトスポット溶接では、溶接電極とアース電極とが離れて配置されることが多く、重合部以外の金属板同士の接触部(例えば、先に溶接された溶接点)を介して流れる電流(無効電流)が生じやすいため、良好なナゲットを形成することが困難であることが問題となっている。 However, in indirect spot welding, the welding electrode and the ground electrode are often arranged apart from each other, and a current flowing through a contact portion (for example, a welding point previously welded) between metal plates other than the overlapping portion. Since (reactive current) is likely to occur, it is a problem that it is difficult to form a good nugget.

例えば、下記の特許文献1には、金属板に予め座面を設け、この座面を溶接電極で押しつぶしながら加圧することにより、金属板同士の接触面積を小さくして電流密度を高めることで、ナゲットを形成しやすくする方法が示されている。 For example, in Patent Document 1 below, a seating surface is provided in advance on a metal plate, and the seating surface is pressed while being crushed by a welding electrode to reduce the contact area between the metal plates and increase the current density. A method for facilitating the formation of nuggets is shown.

また、下記の特許文献2には、加圧力及び電流値を制御することにより、ナゲットを安定して得ることができるインダイレクトスポット溶接方法が示されている。 Further, Patent Document 2 below discloses an indirect spot welding method capable of stably obtaining a nugget by controlling a pressing force and a current value.

特開2002−239742号公報JP, 2002-239742, A 特開2010−194609号公報JP, 2010-194609, A

しかしながら、溶接点におけるナゲットのできやすさを定量的に評価する手法がなかったため、上記のような手法を試しながら試行錯誤を繰り返し、適切なナゲットが形成される溶接条件を探し出すしかなかった。 However, since there was no method for quantitatively evaluating the ease of forming a nugget at the welding point, trial and error was repeated while trying the above-mentioned method to find out the welding conditions for forming an appropriate nugget.

そこで、本発明者らは、溶接に寄与する有効電流経路の抵抗値と、溶接に寄与しない無効電流経路の抵抗値とをそれぞれ個別に測定し、これらの抵抗値に基づいて設定される有効電流率に基づいて、溶接点におけるナゲットのできやすさを評価することを試みた。 Therefore, the present inventors individually measure the resistance value of the active current path that contributes to welding and the resistance value of the reactive current path that does not contribute to welding, and set the active current set based on these resistance values. An attempt was made to evaluate the easiness of the nugget at the welding point based on the rate.

具体的には、図4(A)に示すように、第1の金属板1と、断面ハット形状を成した第2の金属板2と、第1の金属板1と第2の金属板2とで構成される中空部に配された断面ハット形状を成した第3の金属板3とによって構成される部品100について、第1の金属板1と第3の金属板3の天板部3bとの重合部Pにインダイレクトスポット溶接を施す場合の評価方法について説明する。なお、各金属板の間には、既溶接点Q1,Q2が設けられている。 Specifically, as shown in FIG. 4(A), a first metal plate 1, a second metal plate 2 having a hat-shaped cross section, a first metal plate 1 and a second metal plate 2 are formed. For the component 100 constituted by the third metal plate 3 having a hat-shaped cross section and arranged in the hollow portion constituted by, the top plate portion 3b of the first metal plate 1 and the third metal plate 3 An evaluation method when indirect spot welding is performed on the overlapped portion P with will be described. In addition, already welded points Q1 and Q2 are provided between the respective metal plates.

まず、溶接に寄与しない無効電流経路の抵抗値RBを測定する。具体的には、抵抗測定器30の一方の端子31を、部品100のうち、溶接時に溶接電極を当接させる部位である重合部Pに上方から当接させる。また、抵抗測定器30の他方の端子32を、部品100のうち、溶接時にアース電極を当接させる部位である、一方の既溶接点Q2に下方から当接させる。この状態で、部品100の重合部Pを加圧することなく、両端子31、32間の電流経路の抵抗値を測定する。重合部Pを加圧していないことで、両金属板1,3の重合部Pは実質的に接触しておらず、絶縁しなくても重合部Pにほとんど電流が流れない。従って、一方の端子31→第1の金属板1→既溶接点Q1→第2の金属板2→他方の端子32という、重合部P(両金属板1,3の界面)を通らない電流経路C1が形成され、この電流経路C1を、溶接に寄与しない無効電流の電流経路とみなすことができる。 First, the resistance value R B of the reactive current path that does not contribute to welding is measured. Specifically, one terminal 31 of the resistance measuring device 30 is brought into contact with the overlapping portion P of the component 100, which is a portion with which the welding electrode is brought into contact during welding, from above. Further, the other terminal 32 of the resistance measuring device 30 is brought into contact with one already welded point Q2 of the component 100, which is a portion with which the ground electrode is brought into contact during welding, from below. In this state, the resistance value of the current path between the terminals 31 and 32 is measured without pressing the overlapping portion P of the component 100. Since the overlapped portion P is not pressed, the overlapped portions P of both metal plates 1 and 3 are not substantially in contact with each other, and almost no current flows through the overlapped portion P without insulation. Therefore, one terminal 31→first metal plate 1→welded point Q1→second metal plate 2→the other terminal 32 is a current path that does not pass through the overlapping portion P (interface between both metal plates 1 and 3). C1 is formed, and this current path C1 can be regarded as a current path of a reactive current that does not contribute to welding.

次に、溶接に寄与する有効電流経路の抵抗値RAを測定する。具体的には、図4(B)に示すように、抵抗測定器30の一方の端子31を、第1の金属板1に設けられたスリットSに挿入して、第3の金属板3の天板部3bの重合部P付近に上方から当接させる。また、抵抗測定器30の他方の端子32を、一方の既溶接点Q2に下方から当接させる。これにより、一方の端子31→第3の金属板3→既溶接点Q2→第2の金属板2→他方の端子32という電流経路C2が形成され、この電流経路C2の抵抗値を測定する。 Next, the resistance value RA of the effective current path that contributes to welding is measured. Specifically, as shown in FIG. 4(B), one terminal 31 of the resistance measuring device 30 is inserted into the slit S provided in the first metal plate 1 so that the third metal plate 3 has The top plate portion 3b is brought into contact with the vicinity of the overlapping portion P from above. Further, the other terminal 32 of the resistance measuring device 30 is brought into contact with one already welded point Q2 from below. As a result, a current path C2 of one terminal 31→the third metal plate 3→the already-welded point Q2→the second metal plate 2→the other terminal 32 is formed, and the resistance value of this current path C2 is measured.

以上のようにして測定された抵抗値RB、RAに基づいて、溶接点におけるナゲットのできやすさを評価することができる。例えば、有効電流経路の抵抗値RAと無効電流経路の抵抗値RBとの合成抵抗である全体抵抗RT{=RA・RB/(RA+RB)}として求め、有効電流率Kを、全体抵抗RTに対する無効電流経路の抵抗値RBの比率として求める(K=RB/RT)。有効電流率Kは、有効電流の流れやすさを表す指標であり、有効電流率Kの値に基づいて、重合部Pにおけるナゲットのできやすさを評価することができる。そして、この有効電流率Kを評価指標として溶接位置等の溶接条件を決定することで、良品の得られる理想的な溶接条件を設定することが可能になる。 Based on the resistance values R B and R A measured as described above, the ease with which the nugget can be formed at the welding point can be evaluated. For example, calculated as a resistance value of the active current path R A and the total resistance value is a combined resistance of the R B reactive current path resistance R T {= R A · R B / (R A + R B)}, the effective current ratio K is determined as the ratio of the resistance value R B of the reactive current path to the total resistance R T (K=R B /R T ). The effective current rate K is an index representing the ease with which an active current flows, and the ease with which a nugget can be formed in the overlapping portion P can be evaluated based on the value of the effective current rate K. Then, by determining the welding conditions such as the welding position by using the effective current rate K as an evaluation index, it becomes possible to set the ideal welding conditions for obtaining a good product.

しかし、実際の溶接時、例えば自動車の生産ライン等の大量生産の現場では、それぞれの溶接ごとに溶接位置や板同士の隙間等のばらつきが生じるため、有効電流率Kの値にも誤差が生じる。このため、試作段階で算出した有効電流率Kに基づいて理想的な溶接条件を設定したとしても、実際の溶接時には、個々の溶接ごとのばらつきにより、有効電流率Kが良品範囲を外れて溶接不良を生じるおそれがあった。従って、自動車の生産ライン等では、それぞれの溶接ごとに有効電流率Kを算出し、溶接の良否を判定して不良品の後工程への流出を防止することが必要であった。 However, at the time of actual welding, for example, in a mass production site such as an automobile production line, there are variations in the welding position, the gap between the plates, and the like for each welding, so that the value of the effective current ratio K also has an error. .. Therefore, even if the ideal welding conditions are set based on the effective current rate K calculated at the trial production stage, the actual current welding will cause the effective current rate K to deviate from the non-defective product range due to variations in individual welding. There was a risk of causing defects. Therefore, in an automobile production line or the like, it has been necessary to calculate the effective current rate K for each welding, judge the quality of the welding, and prevent the defective product from flowing to the subsequent process.

しかし、上記の測定方法では、図4(A)のように、無効電流経路C1にのみ電流が流れている条件での抵抗値RBの測定と、図4(B)のように、有効電流経路C2にのみ電流が流れている条件での抵抗値RAの測定、といったように、いずれか一方の経路にだけ電流が流れている条件で個々の抵抗値を測定する必要があった。しかし、実際の溶接時には、溶接電極が重合部Pを加圧し、第1の金属板1と天板部3bとが接触することで、無効電流経路C1と有効電流経路C2の両方に電流が流れている{図3(B)参照}ため、上記のような測定方法を採用することができず、一連の溶接プロセスの中で有効電流率Kを算出することが難しかった。このため、自動車の生産ラインの溶接工程のように、ライン上を絶えず流れる部品に順次溶接が行われるような環境では、その全数について有効電流率Kを算出することができず、溶接の良否の判定ができないという課題があった。 However, in the above measuring method, as shown in FIG. 4A, the resistance value R B is measured under the condition that the current flows only in the reactive current path C1 and the effective current is measured as shown in FIG. 4B. It is necessary to measure each resistance value under the condition that the current flows through only one of the paths, such as the measurement of the resistance value R A under the condition that the current flows through the path C2 only. However, at the time of actual welding, the welding electrode pressurizes the overlapping portion P and the first metal plate 1 and the top plate portion 3b come into contact with each other, so that a current flows in both the reactive current path C1 and the active current path C2. Therefore, the measuring method as described above cannot be adopted, and it has been difficult to calculate the effective current rate K in a series of welding processes. Therefore, in an environment where welding is continuously performed on parts that constantly flow on the line, such as in a welding process of an automobile production line, the effective current rate K cannot be calculated for all of them, and the quality of the welding cannot be determined. There was a problem that it could not be judged.

上記の課題を解決するため、本発明は、複数のワークの重合部を溶接電極で加圧すると共に、前記重合部と異なる部位にアース電極を当接させて両電極間に通電するインダイレクトスポット溶接方法であって、溶接の初期に、溶接に寄与しない無効電流経路にのみ電流が流れるように、前記溶接電極を前記重合部に当接させて両電極間に通電するステップを含むことを特徴とする。 In order to solve the above-mentioned problems, the present invention applies indirect spot welding in which a superposed portion of a plurality of workpieces is pressed by a welding electrode, and a ground electrode is brought into contact with a portion different from the superposed portion to energize between the electrodes. In the method, at the initial stage of welding, a step of bringing the welding electrode into contact with the overlapping portion and energizing the electrodes so that a current flows only in a reactive current path that does not contribute to welding, To do.

本発明は、溶接の初期に、無効電流経路にのみ電流が流れた状態で通電するステップ、つまり、溶接電極による加圧をほとんど行わないステップを設けることで、重合部においてワーク同士がほとんど当接しない状態での測定を実施することができる。従って、無効電流経路の抵抗値(前述の抵抗値RBに相当)を測定することができる。これに加えて、その後のステップでの抵抗値の測定、つまり、溶接電極により重合部が相当の加圧力で加圧され、ワーク同士が十分に当接した状態での測定を行うことで、経路全体の抵抗値(前述の全体抵抗RTに相当)を測定することができる。これらの結果により、有効電流率Kを算出することができる。つまり、本発明によれば、一連の溶接プロセスの流れの中で、有効電流率Kを算出して溶接の良否を定量的に評価することが可能になる。従って、実際の生産ラインを流れる部品全数について、個々の溶接ごとに算出した有効電流率Kに基づいて、溶接の良否が判定でき、後工程への不良品の流出を防止したり、算出した有効電流率Kに基づいて、溶接条件を見直したりすることが可能になる。 According to the present invention, in the initial stage of welding, by providing a step of energizing in a state in which a current flows only in the reactive current path, that is, a step of hardly performing pressurization by the welding electrode, the workpieces almost come into contact with each other in the overlapping portion. It is possible to carry out the measurement in the state where it is not. Therefore, the resistance value of the reactive current path (corresponding to the resistance value R B described above) can be measured. In addition to this, the measurement of the resistance value in the subsequent step, that is, the overlapped portion is pressed by the welding electrode with a considerable pressing force, and the measurement is performed while the workpieces are sufficiently abutted, The total resistance value (corresponding to the total resistance R T described above) can be measured. Based on these results, the effective current rate K can be calculated. That is, according to the present invention, it is possible to quantitatively evaluate the quality of welding by calculating the effective current rate K in the flow of a series of welding processes. Therefore, the quality of welding can be judged based on the effective current rate K calculated for each individual welding for all the parts that actually flow in the production line, and the outflow of defective products to the subsequent process can be prevented, or the calculated effective It is possible to review the welding conditions based on the current rate K.

本発明によれば、一連の溶接プロセスの中で、個々の溶接の良否を定量的に評価することができる。 According to the present invention, the quality of each welding can be quantitatively evaluated in a series of welding processes.

インダイレクトスポット溶接を施す様子を示す断面図である。It is sectional drawing which shows a mode that indirect spot welding is performed. 上記インダイレクトスポット溶接の溶接中の電流値、加圧力、抵抗値を示すグラフである。It is a graph which shows the current value, pressurizing force, and resistance value during welding of the said indirect spot welding. 上記インダイレクトスポット溶接の溶接中に流れる電流の経路を示す図で、(A)図が第1のステップにおける図、(B)図がそれ以降のステップにおける図である。It is a figure which shows the path|route of the electric current which flows during the said indirect spot welding, (A) figure is a figure in a 1st step, and (B) figure is a figure in a subsequent step. プローブを用いた各経路の抵抗値の測定方法を示す図である。It is a figure which shows the measuring method of the resistance value of each path|route using a probe.

以下、本発明の実施の形態を図面に基づいて説明する。 Embodiments of the present invention will be described below with reference to the drawings.

本実施形態では、自動車の車体の組立工程において行われるインダイレクトスポット溶接方法を示し、具体的には、図1に示すような車体の骨格部品100を溶接する場合を示す。骨格部品100は、紙面直交方向に延びるフレーム状の部品であり、略平板状を成した第1の金属板(ワーク)1と、断面ハット形状を成した第2の金属板2と、第1の金属板1と第2の金属板2とで構成される中空部に配された断面ハット形状を成した第3の金属板(ワーク)3とで構成される。金属板1〜3としては、例えば鋼板が使用され、具体的には軟鋼板、高張力鋼板(引張強度490MPa以上)、超高張力鋼板(引張強度980MPa以上)等が使用される。 In this embodiment, an indirect spot welding method performed in an assembling process of a vehicle body of an automobile is shown, and specifically, a case of welding a skeleton component 100 of the vehicle body as shown in FIG. 1 is shown. The skeleton component 100 is a frame-shaped component that extends in the direction orthogonal to the paper surface, and includes a first metal plate (work) 1 having a substantially flat plate shape, a second metal plate 2 having a hat-shaped cross section, and a first metal plate. And a third metal plate (work) 3 having a hat-shaped cross section, which is arranged in a hollow portion formed by the metal plate 1 and the second metal plate 2. As the metal plates 1 to 3, for example, steel plates are used, and specifically, mild steel plates, high-tensile steel plates (tensile strength of 490 MPa or more), ultra-high-tensile steel plates (tensile strength of 980 MPa or more) and the like are used.

第1の金属板1と第2の金属板2のフランジ部2aとは、ダイレクトスポット溶接により予め溶接された既接合点Q1を介して接合されている。第2の金属板2の底部2bと第3の金属板3のフランジ部3aとは、ダイレクトスポット溶接により予め溶接された既接合点Q2を介して接合されている。 The 1st metal plate 1 and the flange part 2a of the 2nd metal plate 2 are joined via the already joined point Q1 previously welded by direct spot welding. The bottom portion 2b of the second metal plate 2 and the flange portion 3a of the third metal plate 3 are joined via the already joined point Q2 that has been welded in advance by direct spot welding.

そして、第1の金属板1と第3の金属板3の天板部3bとの重合部Pを、インダイレクトスポット溶接により接合する。インダイレクトスポット溶接装置は、溶接電極10及びアース電極20と、溶接電極10を軸線方向に駆動して金属板を加圧する加圧手段(エアシリンダや電動シリンダ等)と、加圧手段による溶接電極10の加圧力及び両電極10,20間の電流値を制御する制御部(図示省略)とを備える。 Then, the overlapping portion P of the first metal plate 1 and the top plate portion 3b of the third metal plate 3 is joined by indirect spot welding. The indirect spot welding apparatus includes a welding electrode 10 and a ground electrode 20, a pressurizing unit (an air cylinder, an electric cylinder, or the like) that drives the welding electrode 10 in the axial direction to pressurize a metal plate, and a welding electrode using the pressing unit. A control unit (not shown) that controls the pressing force of 10 and the current value between both electrodes 10 and 20 is provided.

重合部Pに対するインダイレクトスポット溶接は、以下の手順で行われる。まず、骨格部品100のうち、重合部Pと異なる部位にアース電極20を当接させる。図示例では、第2の金属板2の底部2b、特に、第2の金属板2の底部2bと第3の金属板3のフランジ部3aとの既接合点Q2に、アース電極20を下方から当接させている。この状態で、第1の金属板1と第3の金属板3の天板部3bとの重合部Pを厚さ方向一方側(図中上側)から溶接電極10で加圧しながら、両電極10,20間に通電することにより、重合部Pを溶接する。 The indirect spot welding on the overlap portion P is performed by the following procedure. First, the ground electrode 20 is brought into contact with a portion of the skeleton component 100 different from the overlapping portion P. In the illustrated example, the ground electrode 20 is applied from below to the bottom portion 2b of the second metal plate 2, particularly the already-joined point Q2 between the bottom portion 2b of the second metal plate 2 and the flange portion 3a of the third metal plate 3. Abutting. In this state, while pressing the overlapping portion P of the first metal plate 1 and the top plate portion 3b of the third metal plate 3 from one side in the thickness direction (the upper side in the figure) with the welding electrode 10, both electrodes 10 , 20 to weld the overlapping portion P.

本実施形態では、溶接電極10による加圧力及び両電極10,20間の電流値の一方又は双方を変化させながら、溶接が行われる。具体的には、図2に示す加圧通電パターンに従って溶接が行われる。 In the present embodiment, welding is performed while changing one or both of the pressure applied by the welding electrode 10 and the current value between the electrodes 10 and 20. Specifically, welding is performed in accordance with the pressurizing and energizing pattern shown in FIG.

図2に示すように、まずステップS1では、溶接電極10で重合部Pを極めて小さい加圧力F1で加圧すると共に、電極10,20間に最も小さい電流値I1を通電する。このステップは、後述する有効電流率Kを算出するために設けられたステップであり、重合部Pの溶接には直接寄与しないステップである。 As shown in FIG. 2, first, in step S1, the overlapping portion P is pressed by the welding electrode 10 with an extremely small pressing force F1, and a minimum current value I1 is applied between the electrodes 10 and 20. This step is a step provided for calculating an effective current ratio K described later, and is a step which does not directly contribute to welding of the overlap portion P.

そして、溶接電極10により高加圧力F2で重合部Pを加圧しながら、低電流値I2で通電する(ステップS2)。その後、加圧力をF2からF3まで低下させながら、電流値I2よりも低い電流値I3で通電する(ステップS3)。そして、加圧力をF3で維持しながら、段階的に電流値を上げていく。具体的には、電流値I4(ステップS4)、電流値I5(ステップS5)、電流値I6(ステップS6)、そして、電流値I7(ステップS7)と段階的に上げていく。 Then, the welding electrode 10 is energized at a low current value I2 while pressurizing the overlapping portion P with a high pressing force F2 (step S2). Then, while the applied pressure is reduced from F2 to F3, energization is performed with a current value I3 lower than the current value I2 (step S3). Then, while maintaining the applied pressure at F3, the current value is gradually increased. Specifically, the current value I4 (step S4), the current value I5 (step S5), the current value I6 (step S6), and the current value I7 (step S7) are gradually increased.

これらのステップのうち、低加圧力F3で加圧しながら相対的に高い電流値I4〜I7で通電するステップS4〜S7が、ナゲットを成長させるナゲット成長期となる。 Of these steps, steps S4 to S7 of energizing with a relatively high current value I4 to I7 while pressurizing with a low pressurizing force F3 are the nugget growth period for growing the nugget.

以上のような通電パターンにより、重合部Pを高温で維持してナゲットの成長を促すことができ、金属板1と金属板3の天板部3bとの重合部Pに、所望の大きさ及び形状を有する接合点としてのナゲットを形成し、このナゲットを介して両金属板1,3を接合することができる。 With the energization pattern as described above, the overlapping portion P can be maintained at a high temperature to promote the growth of the nugget, and the overlapping portion P between the metal plate 1 and the top plate portion 3b of the metal plate 3 has a desired size and It is possible to form a nugget having a shape as a joining point and join the metal plates 1 and 3 through the nugget.

次に、上記の溶接時に、各経路の抵抗値を測定し、有効電流率Kを算出する方法について、図3(A)および図3(B)を用いて説明する。 Next, a method for measuring the resistance value of each path and calculating the active current rate K during the above welding will be described with reference to FIGS. 3(A) and 3(B).

図3(A)に示すように、溶接電極10およびアース電極20は、電流供給部としてのトランス4に接続され、この通電経路上に電流測定器5が設けられる。電流測定器5によって測定された電流値Iと、トランス4の二次コイルの電圧値Vにより、抵抗値を算出することができる。この電圧値Vは、トランス4と溶接電極10およびアース電極20とを接続するケーブル等の抵抗値(電圧降下)の影響も受けるが、これらのケーブル等の抵抗値は非常に小さいため、実質的に一対の電極10,20間の電圧値とみなすことができる。 As shown in FIG. 3(A), the welding electrode 10 and the ground electrode 20 are connected to a transformer 4 as a current supply unit, and a current measuring device 5 is provided on this energizing path. The resistance value can be calculated from the current value I measured by the current measuring device 5 and the voltage value V of the secondary coil of the transformer 4. This voltage value V is also affected by the resistance value (voltage drop) of the cable or the like connecting the transformer 4 to the welding electrode 10 and the ground electrode 20, but since the resistance value of these cables and the like is very small, it is substantially It can be regarded as a voltage value between the pair of electrodes 10 and 20.

まず、ステップS1で無効電流経路の抵抗値を測定する。ステップS1では、溶接電極10の加圧力が小さいため、重合部Pにおいて、第1の金属板1と第3の金属板3とは実質的に接触していない。従って、重合部Pの溶接に寄与しない無効電流経路C1にのみ電流が流れた状態である。このため、上記電流値Iおよび電圧値Vにより、無効電流経路C1の抵抗値RBを算出することができる。 First, in step S1, the resistance value of the reactive current path is measured. In step S1, since the welding electrode 10 has a small pressure, the first metal plate 1 and the third metal plate 3 are not substantially in contact with each other in the overlapping portion P. Therefore, the current flows only in the reactive current path C1 that does not contribute to the welding of the overlapping portion P. Therefore, the resistance value R B of the reactive current path C1 can be calculated from the current value I and the voltage value V.

そして、その後のステップ(例えばステップS2)で、溶接電極10が重合部Pを相対的に大きな加圧力で加圧することにより、前述のように第1の金属板1と第3の金属板3とが重合部Pにおいて接触する。これにより、図3(B)に示すように、無効電流経路C1に加えて、重合部Pを介した有効電流経路C2にも電流が流れる。この状態で測定される上記電流値Iおよび電圧値Vにより、無効電流経路C1と有効電流経路C2の合成抵抗である全体抵抗値RTを算出することができる。 Then, in a subsequent step (for example, step S2), the welding electrode 10 presses the overlapping portion P with a relatively large pressing force, so that the first metal plate 1 and the third metal plate 3 are connected to each other as described above. Contact at the superposition section P. As a result, as shown in FIG. 3B, in addition to the reactive current path C1, the current also flows through the effective current path C2 via the overlapping portion P. From the current value I and the voltage value V measured in this state, it is possible to calculate the total resistance value R T which is the combined resistance of the reactive current path C1 and the active current path C2.

以上のようにして測定された各抵抗値に基づいて、有効電流率K(K=RB/RT)を算出することができる。有効電流率Kは、回路全体を流れる電流のうち、重合部Pを流れる電流、つまり溶接に寄与する電流の割合を示す指標であり、この値が大きいほど、重合部Pに流れる電流の割合が大きくなる。 Based on the resistance value measured as described above, it is possible to calculate the active current ratio K (K = R B / R T). The effective current ratio K is an index showing the ratio of the current flowing through the overlapping portion P, that is, the ratio of the current contributing to welding, among the current flowing through the entire circuit. The larger this value is, the lower the ratio of the current flowing through the overlapping portion P is. growing.

本実施形態の溶接方法では、溶接の開始時に、重合部Pをほとんど加圧しないステップS1をあえて設けることで、無効電流経路C1にのみ電流が流れた状態を作り出し、無効電流経路C1の抵抗値RBの測定が可能になる。また上記のように、十分に重合部Pが加圧された段階で電流Iおよび電圧Vを測定することで、全体抵抗RTを算出することができる(図2の抵抗値参照)。また、これらの抵抗値RBと全体抵抗RTとから、有効電流経路C2の抵抗値RAを算出することができる。このように、異なるステップで上記のように測定を行うことで、抵抗値RT、RA、RBの全ての抵抗値の算出が可能になる。 In the welding method of the present embodiment, at the start of welding, by intentionally providing step S1 in which the overlapping portion P is hardly pressed, a state in which current flows only in the reactive current path C1 is created, and the resistance value of the reactive current path C1 is created. It becomes possible to measure R B. Further, as described above, the total resistance R T can be calculated by measuring the current I and the voltage V when the overlapping portion P is sufficiently pressurized (see the resistance value in FIG. 2). Further, from these resistance value R B and total resistance R T, can be calculated resistance value R A of the active current path C2. Thus, by performing the measurement as described above at different steps, the resistance value R T, R A, it is possible to calculate all of the resistance value of R B.

そしてこれらの抵抗値により、有効電流率Kを算出することができ、この有効電流率Kに基づいて、重合部Pの溶接の良否を判定することができる。つまり、有効電流率Kが小さすぎると、重合部Pに十分な電流が流れず、ナゲットが成長しないため溶接不良を生じてしまう。一方で、有効電流率Kが高すぎると、重合部Pに過剰な電流が流れて、重合部Pにおける第1の金属板1や第3の金属板3の溶け落ちや割れの原因となってしまう。従って、有効電流率Kが所定の範囲内にあるか否かにより、溶接の良否を定量的に評価することができる。 Then, the effective current rate K can be calculated from these resistance values, and the quality of welding of the overlapping portion P can be determined based on the effective current rate K. That is, if the effective current ratio K is too small, a sufficient current does not flow in the overlapping portion P and the nugget does not grow, resulting in poor welding. On the other hand, if the effective current ratio K is too high, an excessive current flows in the overlapping portion P, which may cause burn-through or cracking of the first metal plate 1 or the third metal plate 3 in the overlapping portion P. I will end up. Therefore, the quality of welding can be quantitatively evaluated depending on whether the effective current rate K is within a predetermined range.

また以上の方法によれば、溶接の一連のプロセスの中で有効電流率Kを算出することが可能になり、例えば自動車の生産ラインの溶接工程において、その全数の有効電流率Kを算出して、個々の溶接の良否を定量的に評価することが可能になる。これにより、後工程への不良品の流出を防止したり、算出される有効電流率Kに基づいて、溶接条件の見直しを実施するといったことが可能になる。 Further, according to the above method, it becomes possible to calculate the effective current rate K in a series of welding processes. For example, in the welding process of the automobile production line, the effective current rate K is calculated for all of them. Therefore, it becomes possible to quantitatively evaluate the quality of individual welding. As a result, it is possible to prevent defective products from flowing out to the subsequent process, and to review the welding conditions based on the calculated effective current rate K.

ステップS1における加圧力F1は、その他のステップの加圧力F2,F3と比較してその大きさが特に小さく、ステップS1は、重合部Pをほとんど加圧しない状態で通電するステップである。このステップS1における重合部Pを「ほとんど加圧しない」状態とは、溶接電極10を第3の金属板3に押し当てて、無効電流経路C1に電流を流せるだけの加圧力で加圧する状態であり、第1の金属板1が変形して第3の金属板3に接触するよりも低い加圧力で、重合部Pを加圧する状態でもある。一例として、本実施形態では、加圧力F1を5[kgf]に設定している。このような加圧力で通電するステップを溶接の初期、つまり、両金属板1,3が溶接電極10によって重合部Pを相当の加圧力で加圧する前の段階であって、両金属板1,3が重合部Pで実質的に接触していない段階で設けることで、無効電流経路C1の抵抗値の算出が可能になる。 The pressing force F1 in step S1 is particularly small as compared with the pressing forces F2 and F3 in the other steps, and step S1 is a step of energizing the overlapping portion P with almost no pressurization. The state in which the overlapped portion P in "step S1 is hardly pressed" is a state in which the welding electrode 10 is pressed against the third metal plate 3 and is pressed with a pressing force sufficient to allow a current to flow in the reactive current path C1. There is also a state in which the overlapping portion P is pressed with a lower pressure than when the first metal plate 1 is deformed and comes into contact with the third metal plate 3. As an example, in this embodiment, the pressing force F1 is set to 5 [kgf]. The step of energizing with such a pressing force is an initial stage of welding, that is, a stage before both metal plates 1 and 3 press the overlap portion P with a considerable pressing force by the welding electrode 10. The resistance value of the reactive current path C1 can be calculated by providing 3 at a stage where the overlapping portion P is not substantially in contact.

また、以上のようにして算出される溶接時の有効電流率Kを用いて、溶接時の発熱密度Dを算出してもよい。発熱密度Dは、溶接時の重合部Pに流れる電流をIP、電圧をV、重合部Pにおける第1の金属板1と第3の金属板3との接触面積をSとすると、D=V・IP/Sとして算出することができる。電圧Vは、前述したトランス4の二次コイルの電圧値を用いることができる。 Further, the heat generation density D during welding may be calculated using the effective current rate K during welding calculated as described above. The heat generation density D is D = , where I P is the current flowing in the overlapping portion P during welding, V is the voltage, and S is the contact area between the first metal plate 1 and the third metal plate 3 in the overlapping portion P. It can be calculated as V·I P /S. The voltage value of the secondary coil of the transformer 4 described above can be used as the voltage V.

重合部Pに流れる電流値IPは、全体抵抗RTから有効電流経路C2の抵抗値RAを算出することにより、IP=V/RAにより求めることができる。抵抗値RAは、RA=RT・RB/(RB―RT)により求めることができる。 The current value I P flowing in the overlapping portion P can be obtained from I P =V/ RA by calculating the resistance value RA of the effective current path C2 from the total resistance RT . The resistance value R A can be obtained by RA =R T ·R B /(R B −R T ).

接触面積Sは、溶接電極10の基準位置からの変位量xとの相関関係を用いて算出することができる。つまり、予め上記の板組みを溶接する際の、各時刻における金属板1,3同士の接触面積Sと、そのときの溶接電極10の基準位置からの変位量xとの相関関係を取得する。そして、実際の溶接時の溶接電極10の各時刻における変位量xから、上記の相関関係を用いて、各時刻における接触面積Sを取得することができる。 The contact area S can be calculated using the correlation with the displacement amount x of the welding electrode 10 from the reference position. That is, the correlation between the contact area S between the metal plates 1 and 3 at each time and the displacement amount x from the reference position of the welding electrode 10 at each time when the above plate assembly is welded in advance is acquired. Then, the contact area S at each time can be obtained from the displacement amount x of the welding electrode 10 at each time during actual welding by using the above correlation.

以上のようにして算出された各値により、実際の溶接時における発熱密度Dを算出することができる。つまり、実際の溶接の一連のプロセスの中で、発熱密度Dを算出することが可能になる。発熱密度Dは、抵抗溶接の原理原則を考慮して、金属板1,3同士の接触部の発熱状態に影響を及ぼす複数の動的な因子(具体的には、重合部Pを流れる電流値Ipと、温度に依存して変化する抵抗値と、金属板の硬さや電極の加圧力に依存して変化する接触面積S)を一本化したパラメータである。発熱密度Dにより、重合部Pの単位面積当たり発熱エネルギーの大小を定量的に評価することができる。 The heat generation density D during actual welding can be calculated from the respective values calculated as described above. That is, it becomes possible to calculate the heat generation density D in a series of actual welding processes. The heat generation density D is a plurality of dynamic factors that affect the heat generation state of the contact portion between the metal plates 1 and 3 in consideration of the principle of resistance welding (specifically, the current value flowing in the overlapping portion P). It is a parameter that integrates I p , the resistance value that changes depending on the temperature, and the contact area S) that changes depending on the hardness of the metal plate and the pressing force of the electrode. From the heat generation density D, the magnitude of heat generation energy per unit area of the overlapping portion P can be quantitatively evaluated.

以上、本発明の実施形態について説明したが、本発明は上述の実施形態に限定されるものではなく、本発明の要旨を逸脱しない範囲で種々の変更を加え得ることは勿論である。 Although the embodiments of the present invention have been described above, the present invention is not limited to the above-described embodiments, and it goes without saying that various modifications can be made without departing from the scope of the present invention.

以上の説明では、有効電流率を無効電流経路と有効電流経路との抵抗値に基づいて設定したが、電流値により設定してもよく、例えば、全体の抵抗値に対する有効電流経路を流れる電流値としてもよい。 In the above description, the active current rate is set based on the resistance values of the reactive current path and the active current path, but it may be set by the current value, for example, the current value flowing through the active current path with respect to the entire resistance value. May be

1 第1の金属板(ワーク)
2 第2の金属板
3 第3の金属板(ワーク)
10 溶接電極
20 アース電極
C1 無効電流経路
C2 有効電流経路
P 重合部
Q1,Q2 既接合点
1 First metal plate (work)
2 Second metal plate 3 Third metal plate (work)
10 Welding electrode 20 Earth electrode C1 Reactive current path C2 Active current path P Overlapping part Q1, Q2 Already joined point

Claims (1)

複数のワークの重合部を溶接電極で加圧すると共に、前記重合部と異なる部位にアース電極を当接させて両電極間に通電するインダイレクトスポット溶接方法であって、
溶接の初期に、溶接に寄与しない無効電流経路にのみ電流が流れるように、前記溶接電極を前記重合部に当接させて両電極間に通電するステップを含むことを特徴とするインダイレクトスポット溶接方法。
An indirect spot welding method in which a superposed portion of a plurality of works is pressed with a welding electrode, and a ground electrode is brought into contact with a portion different from the superposed portion to energize between both electrodes,
At the initial stage of welding, indirect spot welding including a step of bringing the welding electrode into contact with the overlapped portion and energizing the electrodes so that a current flows only in a reactive current path that does not contribute to welding. Method.
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Citations (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPH0999379A (en) * 1995-10-02 1997-04-15 Nas Toa Co Ltd Welding current controller of resistance welding machine
JP2012071333A (en) * 2010-09-29 2012-04-12 Honda Motor Co Ltd Spot welding method and spot welding apparatus

Patent Citations (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPH0999379A (en) * 1995-10-02 1997-04-15 Nas Toa Co Ltd Welding current controller of resistance welding machine
JP2012071333A (en) * 2010-09-29 2012-04-12 Honda Motor Co Ltd Spot welding method and spot welding apparatus

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