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JP7245589B2 - How to set welding conditions for spot welding - Google Patents
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JP7245589B2 - How to set welding conditions for spot welding - Google Patents

How to set welding conditions for spot welding Download PDF

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JP7245589B2
JP7245589B2 JP2018241067A JP2018241067A JP7245589B2 JP 7245589 B2 JP7245589 B2 JP 7245589B2 JP 2018241067 A JP2018241067 A JP 2018241067A JP 2018241067 A JP2018241067 A JP 2018241067A JP 7245589 B2 JP7245589 B2 JP 7245589B2
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welding
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圭一郎 木許
知嗣 加藤
麻人 岡村
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Daihatsu Motor Co Ltd
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Description

本発明は、スポット溶接の溶接条件(電流値及び加圧力)の設定方法に関する。 The present invention relates to a method for setting welding conditions (current value and applied pressure) for spot welding.

例えば自動車の車体の組立工程では、複数の鋼板に一対の電極を当接させて通電することにより、鋼板同士の接触部を抵抗発熱により溶融させてナゲットを形成するスポット溶接が行われている。 For example, in the assembly process of an automobile body, spot welding is performed in which a pair of electrodes are brought into contact with a plurality of steel plates and an electric current is passed through them, so that the contact portions of the steel plates are melted by resistance heat generation to form a nugget.

スポット溶接では、複数の金属板の間に適切なナゲットを形成するための様々な手法が提案されている。例えば、下記の特許文献1には、図4に示す通電パターンが示されている。この通電パターンでは、ナゲットを成長させる程度の高い電流値を維持する時間帯と、スパッタを発生させずに鋼板を軟化させる程度の低い電流値を維持する時間帯を交互に繰り返しながら、電流値を徐々に高くしている。これにより、ナゲットが急成長するのを抑え、スパッタの発生を抑えることができるので、溶接部位の品質を確保し、効率良くスポット抵抗溶接を行うことができる、と記載されている。 For spot welding, various techniques have been proposed for forming a suitable nugget between multiple metal plates. For example, Japanese Unexamined Patent Application Publication No. 2002-200003 discloses an energization pattern shown in FIG. 4 . In this energization pattern, the current value is increased while alternately repeating a time period in which a high current value is maintained to grow nuggets and a time period in which a low current value is maintained to soften the steel sheet without generating spatter. gradually increasing. It is described that, as a result, the rapid growth of the nugget can be suppressed and the generation of spatter can be suppressed, so that the quality of the welded portion can be ensured and the spot resistance welding can be performed efficiently.

また、下記の特許文献2には、電流値及び加圧力を制御しながら行うインダイレクトスポット溶接方法が示されている。具体的には、図5に示すように、通電時間を2つの時間帯t1、t2に区分し、最初の時間帯t1では高加圧力f1で加圧しながら低電流値c1で通電する。これにより、電極と金属板との間の接触面積を確保して電流密度を抑え、金属板表面の溶融飛散を防止する。次の時間帯t2では、低加圧力f2で加圧しながら高電流値c2で通電する。これにより、電極先端の金属板への沈み込みを抑え、電流密度を十分に高めることができるため、ナゲットを成長させるに十分な発熱が得られ、ナゲットを安定して得ることができる、と記載されている。 Further, Patent Document 2 below discloses an indirect spot welding method that is performed while controlling the current value and the applied pressure. Specifically, as shown in FIG. 5, the energization time is divided into two time periods t1 and t2, and in the first time period t1, high pressure f1 is applied while low current value c1 is applied. Thereby, the contact area between the electrode and the metal plate is secured, the current density is suppressed, and the melt scattering on the metal plate surface is prevented. In the next time period t2, the high current value c2 is applied while applying the low pressure f2. As a result, it is possible to suppress the sinking of the tip of the electrode into the metal plate and sufficiently increase the current density, so that sufficient heat can be obtained to grow the nugget and the nugget can be stably obtained. It is

また、本発明者らは、特願2018-102540において、図6に示すようなインダイレクトスポット溶接の加圧通電パターンを提案している。具体的には、第1のステップS1で、溶接電極により金属板の重合部を高加圧力F1で加圧しながら、溶接電極とアース電極との間に低電流値C1を通電する。続く第2のステップS2では、溶接電極による加圧力を高加圧力F1から低加圧力F2まで低下させながら、両電極間に、第1のステップS1の電流値C1よりも低い電流値C2を通電する。その後、低加圧力F2を維持しながら、第3、第4のステップS3、S4で電流値をC4、C5と段階的に上げ、第5のステップS5では低電流値C5を通電する。 In addition, the present inventors have proposed a pressurization current pattern for indirect spot welding as shown in FIG. 6 in Japanese Patent Application No. 2018-102540. Specifically, in a first step S1, a low current value C1 is applied between the welding electrode and the ground electrode while applying a high pressing force F1 to the overlapped portion of the metal plate with the welding electrode. In the subsequent second step S2, while decreasing the pressure applied by the welding electrode from the high pressure F1 to the low pressure F2, a current value C2 lower than the current value C1 in the first step S1 is applied between both electrodes. do. Thereafter, while maintaining the low pressing force F2, the current value is increased stepwise to C4 and C5 in the third and fourth steps S3 and S4, and the low current value C5 is applied in the fifth step S5.

特開2006-181621号公報JP 2006-181621 A 特開2010-194609号公報JP 2010-194609 A

しかし、上記のような方法を採用した場合でも、金属板間に適切なナゲットが形成されないことがある。例えば、軟鋼板同士をスポット溶接で接合する場合、軟鋼板自体の固有抵抗値が低いため、軟鋼板同士の接触部が発熱しにくく、上記のような方法によっても軟鋼板同士の接触部を溶融させることは難しい。このような溶接しづらい板組みをスポット溶接で接合する際には、経験等に基づいてトライアンドエラーを繰り返すことにより電流値や加圧力を調整するしかないため、最適な溶接条件(例えば通電パターン)の設定に非常に手間がかかる。 However, even when the above method is adopted, there are cases where an appropriate nugget is not formed between the metal plates. For example, when joining mild steel plates by spot welding, the contact portion between the mild steel plates is less likely to generate heat because the specific resistance value of the mild steel plate itself is low. It is difficult to let When joining such difficult-to-weld plate assemblies by spot welding, there is no choice but to adjust the current value and pressure by repeating trial and error based on experience, etc., so the optimum welding conditions (such as the current pattern ) is very time-consuming to set up.

そこで、本発明が解決すべき課題は、溶接しづらい板組みであっても、最適な溶接条件を容易に設定できるようにすることにある。 Therefore, the problem to be solved by the present invention is to enable the optimum welding conditions to be easily set even for a plate combination that is difficult to weld.

スポット溶接(抵抗溶接)とは、金属板同士の接触部における電流密度(電流値I/接触面積S)と抵抗値Rとの関係によって接触部を抵抗発熱させることで、接触部を溶融させてナゲットを形成する工法である。本発明者らは、金属板同士の接触部の発熱状態に影響を及ぼす複数の因子(具体的には、接触部を流れる電流値Iと、温度に依存して変化する接触部の抵抗値R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)を一本化することを検討した。その結果、金属板同士の接触部に投入される発熱エネルギーJ(=I・V=I・R)を、金属板同士の接触面積Sで割った値である発熱密度Dにより、接触部における発熱状態をモニタリングできることを見出した。 Spot welding (resistance welding) is a method of melting the contact portion by causing the contact portion to generate resistance heat according to the relationship between the current density (current value I/contact area S) and the resistance value R at the contact portion between metal plates. This is a method of forming a nugget. The present inventors have investigated several factors that affect the heat generation state of the contact portion between metal plates (specifically, the current value I flowing through the contact portion and the resistance value R of the contact portion that changes depending on the temperature In addition, the inventors considered unifying the contact area S), which varies depending on the hardness of the metal plate and the pressing force of the electrode. As a result, the heat generation density D, which is the value obtained by dividing the heat energy J (=I V = I 2 R) input to the contact area between the metal plates by the contact area S between the metal plates, It was found that the exothermic state can be monitored.

上記の知見によってなされた本発明は、重ね合わせた複数の金属板に一対の電極を当接させた状態で、前記一対の電極間に通電することにより、前記複数の金属板を接合する際の溶接条件を設定するための方法であって、前記一対の電極間を流れる電流値をI、前記一対の電極間の電圧をV、前記複数の金属板同士の接触面積をSとしたとき、D=I・V/Sで表される発熱密度Dに基づいて通電パターンを設定することを特徴とする。 The present invention, which has been made based on the above findings, is a method for joining a plurality of metal plates by applying an electric current between the pair of electrodes in a state in which the pair of electrodes are in contact with the plurality of superimposed metal plates. A method for setting welding conditions, wherein D is the current value flowing between the pair of electrodes, V is the voltage between the pair of electrodes, and S is the contact area between the plurality of metal plates. The energization pattern is set based on the heat generation density D expressed by =I·V/S.

具体的には、例えば、仮設定した通電パターンに従って溶接を行ったときの発熱密度Dを取得する工程と、前記発熱密度Dに基づいて前記仮設定した通電パターンを調整する工程とを経て、最適な通電パターンを設定することができる。 Specifically, for example, through a step of acquiring a heat generation density D when welding is performed according to a temporarily set energization pattern, and a step of adjusting the temporarily set energization pattern based on the heat generation density D, the optimum energization pattern can be set.

上記のように、発熱密度Dに基づいて通電パターンを設定することで、溶接しづらい板組みであっても、金属板同士の接触部を十分に発熱させる最適な溶接条件を容易に設定することができる。 As described above, by setting the energization pattern based on the heat generation density D, it is possible to easily set the optimum welding conditions that sufficiently generate heat at the contact portions of the metal plates even in a plate combination that is difficult to weld. can be done.

ダイレクトスポット溶接装置の模式図である。1 is a schematic diagram of a direct spot welding device; FIG. 仮設定した加圧通電パターン及び発熱密度を示すグラフである。7 is a graph showing a temporarily set pressurizing energization pattern and heat generation density; 調整後の加圧通電パターン及び発熱密度を示すグラフである。It is a graph which shows the pressurization energization pattern and heat generation density after adjustment. 特許文献1に記載された通電パターンである。This is the energization pattern described in Patent Literature 1. FIG. 特許文献2に記載された加圧通電パターンである。This is a pressurizing energization pattern described in Patent Document 2. FIG. 特願2018-102540に記載された加圧通電パターンである。This is a pressurization energization pattern described in Japanese Patent Application No. 2018-102540.

以下、本発明の実施の形態を図面に基づいて説明する。 BEST MODE FOR CARRYING OUT THE INVENTION Hereinafter, embodiments of the present invention will be described with reference to the drawings.

図1は、2枚の金属板1,2からなる板組みを一対の電極3,4で挟持した状態で通電するダイレクトスポット溶接装置を模式的に示す図である。本実施形態の金属板1,2は鋼板であり、例えば引張強度300MPa以下、板厚1.2mm以下の軟鋼板である。電極3,4は電流供給部としてのトランス5に接続され、この通電経路上に電流測定器6が設けられる。電極3は加圧手段7(例えばシリンダ)に取り付けられる。加圧手段7で電極3を駆動して金属板1に押し付けることにより、金属板1,2に所定の加圧力が付与される。 FIG. 1 is a diagram schematically showing a direct spot welding apparatus in which a pair of electrodes 3 and 4 are held between a pair of electrodes 3 and 4 and current is passed through a combination of two metal plates 1 and 2. As shown in FIG. The metal plates 1 and 2 of this embodiment are steel plates, for example, mild steel plates having a tensile strength of 300 MPa or less and a plate thickness of 1.2 mm or less. The electrodes 3 and 4 are connected to a transformer 5 as a current supply section, and a current measuring device 6 is provided on this current path. The electrode 3 is attached to a pressure means 7 (eg a cylinder). A predetermined pressure is applied to the metal plates 1 and 2 by driving the electrode 3 with the pressure means 7 and pressing it against the metal plate 1 .

本実施形態の溶接条件の設定方法は、以下の手順で行われる。
(1)仮設定した溶接条件で金属板1,2に溶接を施してサンプルを作成する。
(2)サンプルの断面から金属板1,2同士の接触面積を測定する。
(3)サンプルの発熱密度を算出する。
(4)サンプルの発熱密度に基づいて、溶接条件を調整する。
以下、各手順を詳しく説明する。
A method for setting welding conditions according to the present embodiment is performed in the following procedure.
(1) A sample is prepared by welding the metal plates 1 and 2 under temporarily set welding conditions.
(2) Measure the contact area between the metal plates 1 and 2 from the cross section of the sample.
(3) Calculate the heat generation density of the sample.
(4) Adjust the welding conditions based on the heat generation density of the sample.
Each procedure will be described in detail below.

(1)サンプルの作成
図2に、仮設定した溶接条件(加圧通電パターン)を示す。この加圧通電パターンは、図6に示すものと概ね同様である。具体的には、まず、高加圧力F1で加圧しながら低電流値C1で通電する(ステップS1)。その後、加圧力をF1からF2まで低下させながら、電流値C1よりも低い電流値C2で通電する(ステップS2)。そして、加圧力をF2で維持しながら、電流値C1よりも高い電流値C3(ステップS3)、電流値C3よりも高い電流値C4(ステップS4)、電流値C4よりも低い電流値C5(ステップS5)で通電する。これらのステップのうち、低加圧力F2で加圧しながら相対的に高い電流値C3~C5で通電するステップS3~S5が、ナゲットを成長させるナゲット成長期となる。
(1) Preparation of sample Fig. 2 shows temporarily set welding conditions (pressurization current pattern). This pressurizing energization pattern is generally the same as that shown in FIG. Specifically, first, a low current value C1 is applied while a high pressure force F1 is applied (step S1). After that, while decreasing the pressing force from F1 to F2, current is applied at a current value C2 lower than the current value C1 (step S2). Then, while maintaining the applied force at F2, a current value C3 higher than the current value C1 (step S3), a current value C4 higher than the current value C3 (step S4), and a current value C5 lower than the current value C4 (step S5) turns on electricity. Among these steps, steps S3 to S5 in which relatively high current values C3 to C5 are applied while applying a low pressure force F2 constitute a nugget growth period for growing nuggets.

この通電パターンで金属板1,2に溶接を施し、通電開始から複数の時刻で通電を止めた複数のサンプルを作成する。例えば、通電開始から1サイクル(=1/60秒)までで通電を止めた第1のサンプル、通電開始から2サイクルまでで通電を止めた第2のサンプル、・・・のように、通電時間を1サイクルごと長くした複数のサンプルを作成する。各サンプルの溶接を行っている間の電流値I及び電圧Vの時間変化を記録する。具体的に、電極3,4間に通電する電流値I、すなわち、金属板1,2の接触部を通る通電経路の電流値Iを電流測定器6で測定し、その時間変化を記録する。電圧Vは、トランス5の二次コイルの電圧である。この電圧Vは、トランス5と電極3,4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3,4間の電圧とみなすことができる。 The metal plates 1 and 2 are welded in this energization pattern, and a plurality of samples are produced by stopping the energization at a plurality of times from the start of the energization. For example, the first sample where the energization is stopped within 1 cycle (= 1/60 second) from the start of energization, the second sample where the energization is stopped within 2 cycles after the start of energization, and so on. is lengthened for each cycle to create a plurality of samples. The changes in current value I and voltage V over time during welding of each sample are recorded. Specifically, the current value I flowing between the electrodes 3 and 4, that is, the current value I of the current path passing through the contact portion of the metal plates 1 and 2 is measured by the current measuring device 6, and the change over time is recorded. A voltage V is the voltage of the secondary coil of the transformer 5 . This voltage V is also affected by the resistance value (voltage drop) of the cable connecting the transformer 5 and the electrodes 3 and 4, but since the resistance value of these cables is very small, the voltage V is substantially equal to that of the pair of electrodes. It can be regarded as a voltage between 3 and 4.

(2)接触面積の測定
上記の各サンプルを切断し、各サンプルにおいて、金属板1,2同士の接触面積を測定する。具体的には、各サンプルの断面から、金属板1,2同士の接触部の直径を測定し、この直径から当該接触部の面積を算出する。尚、このときの接触部とは、各サンプルの断面において金属板1,2同士が実際に接触している領域(例えばナゲット形成部)だけでなく、両電極3,4で加圧することで圧接していた痕跡のある領域を含む。この各サンプルにおける金属板1,2同士の接触面積が、図2に示す加圧通電パターンの複数の時刻における金属板1,2同士の接触面積となる。
(2) Measurement of contact area Each sample is cut, and the contact area between the metal plates 1 and 2 is measured in each sample. Specifically, the diameter of the contact portion between the metal plates 1 and 2 is measured from the cross section of each sample, and the area of the contact portion is calculated from this diameter. The contact portion at this time means not only the region where the metal plates 1 and 2 are actually in contact with each other (for example, the nugget forming portion) in the cross section of each sample, but also Including areas with traces of The contact area between the metal plates 1 and 2 in each sample is the contact area between the metal plates 1 and 2 at a plurality of times in the pressurizing current pattern shown in FIG.

(3)発熱密度Dの算出
上記(2)で測定した複数の時刻における金属板1,2同士の接触面積Sと、そのときの電流値I及び電圧Vとから、各時刻における接触部の発熱密度D(=I・V/S=I・R/S)を算出する。発熱密度Dは、抵抗溶接の原理原則を考慮して、金属板1,2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、接触部を流れる電流値Iと、温度に依存して変化する接触部の抵抗値R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。
(3) Calculation of heat generation density D Based on the contact area S between the metal plates 1 and 2 at a plurality of times measured in (2) above, and the current value I and voltage V at that time, heat generation at the contact portion at each time Calculate the density D (=I·V/S=I 2 ·R/S). Considering the principle of resistance welding, the heat generation density D is determined by a plurality of dynamic factors (specifically, the current value I , the resistance value R of the contact portion, which varies depending on the temperature, and the contact area S, which varies depending on the hardness of the metal plate and the pressing force of the electrode.

上記で算出した発熱密度Dの時間変化を、図2のグラフに点線で示す。このグラフから分かるように、ステップS3の初期は発熱密度Dが上昇しているが、時刻t1以降は発熱密度Dが低下している。同様に、ステップS4の初期は発熱密度Dが上昇しているが、時刻t2以降は発熱密度Dが低下している。さらに、ステップS5では、全期間において発熱密度Dが低下している。 The change over time of the heat generation density D calculated above is indicated by a dotted line in the graph of FIG. As can be seen from this graph, the heat generation density D increases at the beginning of step S3, but decreases after time t1. Similarly, the heat generation density D increases at the beginning of step S4, but decreases after time t2. Furthermore, in step S5, the heat generation density D decreases throughout the period.

(4)通電パターンの調整
上記(3)で取得した発熱密度Dに基づいて、図2に示す仮設定した通電パターン、特にナゲット成長期(ステップS3~S5)における通電パターンを調整する。具体的には、ナゲット成長期において発熱密度Dがなるべく低下しないように、電流値及び通電時間を調整する。具体的には、ナゲットを成長させるのに必要となる発熱密度Dの基準値D1を設定し、発熱密度Dが早期に基準値D1を超え、その後基準値D1以下とならないように、通電パターンを調整する。
(4) Adjustment of energization pattern Based on the heat generation density D obtained in (3) above, the temporarily set energization pattern shown in FIG. 2, especially the energization pattern during the nugget growth period (steps S3 to S5), is adjusted. Specifically, the current value and the energization time are adjusted so that the heat generation density D does not decrease as much as possible during the nugget growth period. Specifically, a reference value D1 of the heat generation density D required to grow the nugget is set, and the energization pattern is adjusted so that the heat generation density D does not exceed the reference value D1 at an early stage and then fall below the reference value D1. adjust.

例えば、図2のステップS3では、発熱密度Dが基準値D1に達する前に低下している。また、ステップS4では、発熱密度Dが一旦基準値D1を超えているが、その後低下して基準値D1を下回っている。これらの結果から、本実施形態の板組みでは、ナゲット成長期において、各ステップ(一定の電流値で通電する時間)を短くして、発熱密度Dが低下し始める前に電流値を上昇させることが好ましいと考えられる。また、ステップS5では、発熱密度Dが基準値D1を下回ったまま低下し続けているため、このステップS5はナゲットの成長にほとんど寄与しておらず、省略可能と考えられる。 For example, at step S3 in FIG. 2, the heat density D decreases before reaching the reference value D1. Further, in step S4, the heat generation density D once exceeds the reference value D1, but then decreases to fall below the reference value D1. From these results, in the board structure of the present embodiment, each step (the time of energizing at a constant current value) is shortened in the nugget growth period, and the current value is increased before the heat generation density D starts to decrease. is considered preferable. Further, in step S5, since the heat density D continues to decrease while remaining below the reference value D1, this step S5 hardly contributes to the growth of the nugget and can be omitted.

上記のような発熱密度Dに基づく検討に従って、図2に示す仮設定した通電パターンを調整し、図3に示す通電パターンを設定する。この通電パターンでは、ナゲット成長期(ステップS3’~S6’)において、電流値をC3’からC6’まで短時間で段階的に上昇させている。これにより、発熱密度Dが、基準値D1以上まで上昇した後、基準値D1を下回ることなく高い値で維持される。このように、金属板1,2の接触部における発熱密度Dを高い値で維持することで、接触部が高温で維持されるため、ナゲットの成長を促進することができる。また、上記のように、発熱密度Dを低下させないために短時間に高電流値で通電することで、ナゲット成長期の通電時間が短縮され、スポット溶接のサイクルタイムが短縮される。 According to the examination based on the heat generation density D as described above, the temporarily set energization pattern shown in FIG. 2 is adjusted, and the energization pattern shown in FIG. 3 is set. In this energization pattern, the current value is increased stepwise from C3' to C6' in a short period of time during the nugget growth period (steps S3' to S6'). As a result, the heat generation density D is maintained at a high value without falling below the reference value D1 after increasing to the reference value D1 or higher. By maintaining the heat generation density D at the contact portion of the metal plates 1 and 2 at a high value in this manner, the contact portion is maintained at a high temperature, so that the growth of the nugget can be promoted. In addition, as described above, in order to prevent the heat generation density D from decreasing, a high current value is applied for a short period of time, thereby shortening the energization time during the nugget growth period and shortening the spot welding cycle time.

従来は、所定の溶接条件(通電パターン)で溶接してナゲットを形成し、このナゲットが所望の大きさ及び形状でない場合は、通電パターンの各ステップの電流値や通電時間(サイクル)を経験等に基づいて手探りで調整するのが通例であった。このような手法で、図2に示す通電パターンから図3に示す通電パターンに到達するには、膨大なトライアンドエラーが必要となる。そこで、上記のように、仮設定した通電パターンの複数の時刻における発熱密度Dを取得し、この発熱密度Dに基づいて電流値及び通電時間を調整することで、最適な通電パターンを得るための工数が大幅に少なくなる。 Conventionally, a nugget is formed by welding under predetermined welding conditions (energization pattern), and if the nugget is not of the desired size and shape, the current value and energization time (cycle) of each step of the energization pattern are determined by experience. It was customary to make blind adjustments based on In order to reach the energization pattern shown in FIG. 3 from the energization pattern shown in FIG. 2 with such a method, a huge amount of trial and error is required. Therefore, as described above, the heat generation density D at a plurality of times of the temporarily set energization pattern is obtained, and the current value and the energization time are adjusted based on the heat generation density D, thereby obtaining the optimum energization pattern. Man-hours are greatly reduced.

上記の実施形態では、サンプルの断面から金属板1,2同士の接触面積Sを求めた場合を示したが、これに限られない。例えば、予め、所定の板組みを溶接する際の、各時刻における金属板1,2同士の接触面積Sと、そのときの溶接電極3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、上記と同じ板組みに溶接を施す際の通電パターンを設定する際に、上記の相関関係を用いて、溶接中の溶接電極3の変位量xから各時刻における接触面積Sを取得することができる。この場合、サンプルを切断して接触面積Sを測定する必要がないため、接触面積S、ひいては発熱密度Dを容易に取得することができる。 In the above-described embodiment, the case where the contact area S between the metal plates 1 and 2 is obtained from the cross section of the sample has been shown, but the present invention is not limited to this. For example, the correlation between the contact area S between the metal plates 1 and 2 at each time and the displacement amount x of the welding electrode 3 from the reference position at that time is acquired in advance when welding a predetermined combination of plates. . Then, when setting the energization pattern for welding the same plate assembly as described above, the above correlation is used to obtain the contact area S at each time from the displacement amount x of the welding electrode 3 during welding. can be done. In this case, since it is not necessary to cut the sample and measure the contact area S, the contact area S and the heat generation density D can be easily obtained.

また、上記の実施形態では、発熱密度Dそのものの値に基づいて通電パターンを設定する場合を示したが、これに限らず、例えば、発熱密度Dに有効電流率Kを乗じた指標(実質発熱密度D’=K・D)に基づいて通電パターンを設定してもよい。有効電流率Kは、電極3,4間を流れる全電流のうち、金属板1,2同士の接触部を通って溶接に寄与する有効電流の割合を表す指標である。具体的に、有効電流の通電経路の抵抗値をR、無効電流の通電経路の抵抗値をRとしたとき、有効電流率Kは、例えばK=R/(R+R)で定義することができる。あるいは、有効電流率Kを、K=R/Rと定義してもよい。あるいは、有効電流の通電経路の抵抗値Rと無効電流の通電経路の抵抗値Rの合成抵抗値をRTOTALとしたとき、有効電流率Kを、K=R/RTOTALと定義してもよい。 Further, in the above-described embodiment, the case where the energization pattern is set based on the value of the heat generation density D itself is shown, but this is not restrictive. For example, an index (actual heat generation The energization pattern may be set based on the density D'=K·D). The active current rate K is an index representing the ratio of the active current that passes through the contact portion between the metal plates 1 and 2 and contributes to the welding in the total current flowing between the electrodes 3 and 4 . Specifically, when the resistance value of the conducting path of the active current is RA and the resistance value of the conducting path of the reactive current is RB , the active current rate K is, for example, K= RB /( RA + RB ). can be defined. Alternatively, the active current rate K may be defined as K= RB / RA . Alternatively, when the combined resistance value of the resistance value RA of the active current conduction path and the resistance value RB of the reactive current conduction path is R TOTAL , the active current rate K is defined as K = RB /R TOTAL . may

また、上記の実施形態では、サンプルに溶接を施す際の発熱密度Dに基づいて、通電パターン(電流値及び通電時間)を調整した場合を示したが、これに限らず、発熱密度Dに基づいて、加圧パターン(加圧力及び加圧時間)、あるいは、通電パターン及び加圧パターンの双方を調整してもよい。 In addition, in the above embodiment, the case where the energization pattern (current value and energization time) is adjusted based on the heat generation density D when welding the sample is shown, but not limited to this, based on the heat generation density D The pressurization pattern (pressurization force and pressurization time), or both the energization pattern and the pressurization pattern may be adjusted.

また、上記の実施形態では、実際に溶接を行ったときの電流値I、電圧V、及び接触面積Sから発熱密度Dを取得する場合を示したが、これに限らず、例えばシミュレーションにより、仮設定した所定の通電パターンで溶接を行ったときの発熱密度Dを取得してもよい。 Further, in the above-described embodiment, the case where the heat generation density D is obtained from the current value I, the voltage V, and the contact area S when welding is actually performed has been shown. A heat generation density D may be obtained when welding is performed with a predetermined energization pattern that has been set.

また、本発明に係る溶接条件の設定方法は、上記のようなダイレクトスポット溶接に限らず、インダイレクトスポット溶接やシリーズスポット溶接など、他のスポット溶接に適用することができる。また、溶接を施す板組みも上記に限らず、3枚以上の金属板からなる板組みや、高張力鋼板や超高張力鋼板を含む板組みのスポット溶接にも、本発明に係る溶接条件の設定方法を適用することができる。 Moreover, the method for setting welding conditions according to the present invention is not limited to direct spot welding as described above, but can be applied to other spot welding such as indirect spot welding and series spot welding. In addition, the plate assembly to be welded is not limited to the above, and the welding conditions according to the present invention can also be applied to spot welding of plate assembly consisting of three or more metal plates and plate assembly including high-tensile steel plate and ultra-high-tensile steel plate. A setting method can be applied.

1,2 金属板
3,4 電極
5 トランス
6 電流測定器
7 加圧手段
1, 2 metal plates 3, 4 electrode 5 transformer 6 current measuring device 7 pressure means

Claims (2)

重ね合わせた複数の金属板に一対の電極を当接させた状態で、前記一対の電極間に通電することにより、前記複数の金属板を接合する際の溶接条件を設定するための方法であって、
前記一対の電極間を流れる電流値をI、前記一対の電極間の電圧をV、前記複数の金属板同士の接触面積をSとしたとき、D=I・V/Sで表される発熱密度Dが、一旦基準値D1を超えたら、通電終了まで基準値D1を下回らないように通電パターンを設定するスポット溶接の溶接条件の設定方法。
A method for setting welding conditions for joining a plurality of metal plates by energizing between the pair of electrodes in a state in which the pair of electrodes are in contact with the plurality of superimposed metal plates. hand,
When the current value flowing between the pair of electrodes is I, the voltage between the pair of electrodes is V, and the contact area between the plurality of metal plates is S, the heat generation density is expressed by D=IV/S. A method for setting welding conditions for spot welding in which, once D exceeds a reference value D1, an energization pattern is set so that it does not fall below the reference value D1 until the end of energization .
仮設定した通電パターンに従って溶接を行ったときの発熱密度Dを取得する工程と、前記発熱密度Dに基づいて前記仮設定した通電パターンを調整する工程とを有する請求項1に記載のスポット溶接の溶接条件の設定方法。 The step of acquiring the heat generation density D when welding is performed according to the temporarily set energization pattern, and the step of adjusting the temporarily set energization pattern based on the heat generation density D. Spot welding according to claim 1. How to set welding conditions.
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