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JP2010247215A - Resistance welding method of high tensile steel sheet - Google Patents

Resistance welding method of high tensile steel sheet Download PDF

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JP2010247215A
JP2010247215A JP2009102077A JP2009102077A JP2010247215A JP 2010247215 A JP2010247215 A JP 2010247215A JP 2009102077 A JP2009102077 A JP 2009102077A JP 2009102077 A JP2009102077 A JP 2009102077A JP 2010247215 A JP2010247215 A JP 2010247215A
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energization
nugget
current
dust
welding
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JP5332857B2 (en
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Toru Okada
徹 岡田
Masato Uchihara
正人 内原
Manabu Fukumoto
学 福本
Kiyoyuki Fukui
清之 福井
Kanji Suzuki
幹治 鈴木
Koji Nomura
浩二 野村
Hiroshi Chikagawa
博 近川
Tetsuhiro Toyoda
哲弘 豊田
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Nippon Steel Corp
Toyota Motor Corp
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Sumitomo Metal Industries Ltd
Toyota Motor Corp
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Abstract

<P>PROBLEM TO BE SOLVED: To provide a resistance welding method that suppresses generation of expulsion together with initial expulsion and expands a nugget diameter, in lap resistance welding of a high tensile steel sheet. <P>SOLUTION: A resistance welding method of a high tensile steel sheet is provided in which at least two steel sheets including at least one high tensile steel sheet are superimposed and resistance-welded. The method includes: a first step in which a nugget 3 is formed having a nugget diameter of 3√t to 5√t (t is the thickness (mm) of one steel sheet having a smaller thickness of the two steel sheets) by energization to at least the two steel sheets; a second step in which a welding current is reduced after the first step; and a third step in which a welding current greater than that of the first step is energized after the second step and the nugget 3 is expanded by imparting a pressurizing force of 110-150% of the pressurizing force in the first step. <P>COPYRIGHT: (C)2011,JPO&INPIT

Description

本発明は、高張力鋼板の抵抗溶接方法に関し、具体的には、主に自動車車体の組立てで使用される抵抗溶接において、チリ(またはスパッタ:母材の溶融飛散現象)の発生を抑制し、ナゲット径を拡大することができる高張力鋼板の抵抗溶接方法に関する。   The present invention relates to a resistance welding method for a high-strength steel sheet, specifically, in resistance welding mainly used in the assembly of an automobile body, suppressing the occurrence of dust (or spatter: melting and scattering phenomenon of a base material), The present invention relates to a resistance welding method for a high-strength steel sheet capable of expanding the nugget diameter.

近年、自動車産業分野では、車体の軽量化および衝突安全性の向上を図るため、公称引張強さが例えば440MPa以上である高張力鋼板(ハイテン)の使用が拡大している。   In recent years, in the automotive industry field, in order to reduce the weight of a vehicle body and improve the collision safety, the use of high-tensile steel plates (high tensile) having a nominal tensile strength of, for example, 440 MPa or more is expanding.

車体の組立てで主に使用されるスポット溶接では、板厚t(mm)に応じたナゲット径の確保が求められる。一般的に、ナゲット径4√t(mm)が得られる電流値から、チリが発生する電流値までの範囲として規定される適正電流範囲が重要な指標とされる。   In spot welding mainly used in assembling the vehicle body, it is required to secure a nugget diameter corresponding to the plate thickness t (mm). In general, an appropriate current range defined as a range from a current value at which a nugget diameter of 4√t (mm) is obtained to a current value at which dust is generated is an important index.

図1は、通電を1回だけ行う1段通電方式による抵抗溶接における通電時間と、電流または加圧力との関係の一例を示すグラフである。高張力鋼板の抵抗溶接において図1にグラフで示す1段通電方式ではチリが発生し易く、適正電流範囲の確保が困難となる。   FIG. 1 is a graph showing an example of the relationship between the energization time and the current or the applied pressure in resistance welding by the one-stage energization method in which energization is performed only once. In resistance welding of high-tensile steel plates, the one-stage energization method shown in the graph of FIG. 1 is likely to generate dust, and it is difficult to ensure an appropriate current range.

一般的に、適正電流範囲を確保するためには加圧力の向上が有効である。しかし、例えば公称引張強さ980MPa級以上の超ハイテン材では、スポット溶接ガンの剛性の制約を超える加圧力が必要となる場合がある。   In general, it is effective to improve the pressing force in order to secure an appropriate current range. However, for example, in the case of an ultra-high tensile material having a nominal tensile strength of 980 MPa or more, a pressing force exceeding the restriction of the rigidity of the spot welding gun may be required.

また、スポット溶接においては、通常、種々の形状にプレス成形された鋼板が用いられる。しかし、鋼板の強度が高くなるとプレス成形の際にスプリングバックが大きくなるため、スポット溶接の際における板と板との隙間が大きくなる。一般的に、この隙間が大きくなるほどナゲットは形成され難くなり、適正電流範囲の確保はより困難になる。   In spot welding, steel plates press-formed into various shapes are usually used. However, when the strength of the steel plate is increased, the springback is increased during press forming, and the gap between the plates during spot welding is increased. In general, the larger the gap, the harder the nugget is formed, and it becomes more difficult to ensure an appropriate current range.

また、一般的に母材の引張強さが上昇するにつれて、母材に含まれる炭素や合金元素の量が増加する傾向にあるため、スポット溶接部の硬さは上昇し、界面破断を生じ易くなる。破断形態の観点から、高張力鋼板のナゲット径は軟鋼のナゲット径よりも大きいことが望まれる。   In general, as the tensile strength of the base material increases, the amount of carbon and alloy elements contained in the base material tends to increase, so that the hardness of the spot weld increases and is likely to cause interface fracture. Become. From the viewpoint of fracture mode, it is desirable that the nugget diameter of the high-tensile steel plate is larger than the nugget diameter of the mild steel.

図2は、予備通電によりワーク接触面同士のなじみをよくした後に本通電を行う2段通電方式による抵抗溶接における通電時間と、電流または加圧力との関係の一例を示すグラフである。
特許文献1、2には、高張力鋼板のスポット溶接におけるチリの発生を抑制するために、図2にグラフで例示する2段通電方式を用いる発明が開示されている。
FIG. 2 is a graph showing an example of the relationship between the energization time and the current or the applied pressure in resistance welding by the two-stage energization method in which the main energization is performed after the work contact surfaces are improved by preliminary energization.
Patent Documents 1 and 2 disclose an invention using a two-stage energization method illustrated by a graph in FIG. 2 in order to suppress generation of dust in spot welding of a high-tensile steel plate.

また、特許文献3には、通電中の加圧力を増大するとともに電流を降下させる2段通電方式を用いることにより、板厚比の大きな板組みにおいて薄板側へのナゲットを形成する発明が開示されている。   Patent Document 3 discloses an invention for forming a nugget on a thin plate side in a plate assembly having a large plate thickness ratio by using a two-stage energization method in which a pressurizing force during energization is increased and a current is lowered. ing.

特開平11−104849号公報Japanese Patent Laid-Open No. 11-104849 特開2003−236674号公報JP 2003-236684 A 特開2005−262259号公報JP 2005-262259 A

チリは、通電初期に発生する比較的軽微な初期チリと、通電中期から後期にかけて発生する比較的大きな中チリとの2種類に分類される。初期チリは、母材の引張強さが高く変形し難いことに起因して、重ね合わせ板の隙間や電極の当りの悪さ等により板接触面のなじみが悪くなって電流が局所的に集中するために、発生する。   Chile is classified into two types: a relatively light initial dust that occurs in the early stage of energization, and a relatively large medium dust that occurs in the middle and later stages of energization. In the initial dust, due to the high tensile strength of the base material and the difficulty of deformation, the contact of the plate contact surface becomes worse due to the gap between the stacked plates and the poor contact of the electrodes, and the current is concentrated locally. To occur.

初期チリは、特許文献1、2に開示される予備通電により板接触面のなじみを改善することで抑制することが確かに可能である。しかし、中チリは、圧接部の強度不足が原因であるため、これらの従来の技術では抑制することができない。また、特許文献3により開示された発明では、特に、強度が高い鋼板を抵抗溶接する場合や、板隙が存在する場合にはチリ発生を抑制しながら充分な大きさのナゲットを形成することが難しい。   The initial dust can surely be suppressed by improving the familiarity of the plate contact surface by the preliminary energization disclosed in Patent Documents 1 and 2. However, since medium dust is caused by insufficient strength of the pressure contact portion, it cannot be suppressed by these conventional techniques. In addition, in the invention disclosed in Patent Document 3, a sufficiently large nugget can be formed while suppressing generation of dust when a steel plate having high strength is resistance-welded or when a gap exists. difficult.

本発明は、これら従来の技術が有する課題に鑑みてなされたものであり、高張力鋼板の重ね合わせ抵抗溶接において、初期チリとともに中チリの発生を抑制し、ナゲット径を拡大することができる抵抗溶接方法を提供することを目的とする。   The present invention has been made in view of the problems of these conventional techniques, and in resistance to overlap welding of high-strength steel sheets, resistance that can suppress the generation of medium dust as well as initial dust and can increase the nugget diameter. An object is to provide a welding method.

本発明者らは、上記課題を解決するために種々の検討を行い、以下に列記する知見(a)〜(c)を得た。   The inventors of the present invention have made various studies in order to solve the above-described problems, and have obtained knowledge (a) to (c) listed below.

(a)図3は、スポット溶接における軟鋼からなる鋼板1、2の通電径およびナゲット3の成長の様子を模式的に示す説明図である。   (A) FIG. 3 is an explanatory view schematically showing the energized diameter of the steel plates 1 and 2 made of mild steel and the growth of the nugget 3 in spot welding.

スポット溶接では、コロナボンド4と呼ばれる、ナゲット3の周囲に電極5、6により加圧された領域が存在する。チリは、溶融金属の内圧がコロナボンド4に作用する外圧を超えると発生するため、コロナボンド4が溶融し狭くなるにつれチリ発生の危険性が高まる。なお、図3における符号7は通電経路を示す。   In spot welding, a region called corona bond 4 and pressurized by electrodes 5 and 6 exists around nugget 3. Since dust is generated when the internal pressure of the molten metal exceeds the external pressure acting on the corona bond 4, the risk of dust generation increases as the corona bond 4 melts and narrows. In addition, the code | symbol 7 in FIG. 3 shows an electricity supply path | route.

図3に示すように、軟鋼からなる鋼板1、2の溶接では、コロナボンド4の領域が広いため、チリが発生し難い。さらに通電後期においては、温度上昇による伝熱で鋼板1、2の軟化域が拡大してコロナボンド4の領域が広がるため、大きなナゲット径までチリの発生が抑制される。   As shown in FIG. 3, in the welding of the steel plates 1 and 2 made of mild steel, since the area of the corona bond 4 is wide, dust is hardly generated. Further, in the later stage of energization, the softened regions of the steel plates 1 and 2 are expanded by the heat transfer due to the temperature rise and the region of the corona bond 4 is expanded, so that generation of dust is suppressed to a large nugget diameter.

図4は、スポット溶接における高張力鋼からなる鋼板8、9の通電径およびナゲット3の成長の様子を模式的に示す説明図である。
図4に示すように、高張力鋼からなる鋼板8、9の溶接では、母材強度が高いため、スポット溶接時の加圧力で母材が変形し難く、軟鋼からなる鋼板1、2に比較してコロナボンド4の領域が小さくなる。このため、通電領域7での電流密度が高まり、ナゲット3が急激に成長するため、チリが発生し易い。
FIG. 4 is an explanatory view schematically showing the diameters of the steel plates 8 and 9 made of high-strength steel and the growth of the nugget 3 in spot welding.
As shown in FIG. 4, in the welding of steel plates 8 and 9 made of high-strength steel, the strength of the base material is high, so that the base material is not easily deformed by the applied pressure during spot welding. Thus, the area of the corona bond 4 is reduced. For this reason, the current density in the energization region 7 increases, and the nugget 3 grows rapidly, so that dust is easily generated.

(b)図5は、1段通電方式により高張力鋼板をスポット溶接する際のナゲット3とコロナボンド4との成長を模式的に示す説明図である。図5に示すように、高張力鋼板のスポット溶接においては、通電初期の通電径が狭いことに加え、伝熱によるコロナボンド4の拡大も小さいため、チリが発生し易くなると考えられる。   (B) FIG. 5 is an explanatory view schematically showing the growth of the nugget 3 and the corona bond 4 when spot-welding a high-tensile steel plate by the one-stage energization method. As shown in FIG. 5, in spot welding of a high-strength steel sheet, in addition to a narrow energization diameter at the initial stage of energization, the expansion of the corona bond 4 due to heat transfer is also small, so it is considered that dust is likely to occur.

(c)ナゲット3の成長速度には通電径が最も影響を及ぼすことが知られている。本発明者らは、高張力鋼板のスポット溶接においてチリの発生を抑制するためには、ナゲット3が緩やかに成長するように通電径を拡大することが重要であると考え、そのためには、本通電の前に予備通電を行い、予備通電工程で適切な大きさのナゲット3を形成した後に、本通電工程の前までにコロナボンド4を拡大することが重要であることを知見した。以下、予備通電工程を第1工程といい、本通電工程を第3工程というとともに、第1工程と第3工程との間に、コロナボンド4の領域すなわち加圧領域を拡大する工程を第2工程という。   (C) It is known that the energization diameter has the most influence on the growth rate of the nugget 3. In order to suppress generation of dust in spot welding of a high-strength steel sheet, the present inventors consider that it is important to expand the conduction diameter so that the nugget 3 grows gently. It was found that it is important to expand the corona bond 4 before the main energization process after performing the pre-energization before energization and forming the nugget 3 having an appropriate size in the pre-energization process. Hereinafter, the preliminary energization process is referred to as the first process, the main energization process is referred to as the third process, and the process of expanding the area of the corona bond 4, that is, the pressurization area, between the first process and the third process. This is called a process.

本発明者らは、第1工程、第2工程および第3工程から構成される多段通電溶接において、第1工程と第2工程における通電条件を検討するため、板厚1.4mmの高張力鋼板を2枚重ね合わせた板組みにて第1工程の通電電流を変化させることで、第1工程で得られるナゲット径を変更し、各ナゲット径に対して第2工程の通電電流を第1工程の通電電流の50%に降下し、その時間を0サイクル、5サイクルまたは9サイクルの3水準として、第3工程におけるチリ発生限界電流を調査した。溶接条件を表1に示すとともに結果を表2に示す。なお、加圧力は、第1工程、第2工程、第3工程において一定値(320kgf)とした。   In the multistage energization welding composed of the first step, the second step, and the third step, the present inventors have investigated the energization conditions in the first step and the second step, and thus a high-tensile steel plate having a thickness of 1.4 mm. The nugget diameter obtained in the first step is changed by changing the energization current in the first step with a plate assembly in which two sheets are stacked, and the energization current in the second step is changed for each nugget diameter in the first step. The current limit of dust generation in the third step was investigated by setting the time to 3 levels of 0 cycle, 5 cycles or 9 cycles. The welding conditions are shown in Table 1 and the results are shown in Table 2. The applied pressure was a constant value (320 kgf) in the first step, the second step, and the third step.

Figure 2010247215
Figure 2010247215

Figure 2010247215
Figure 2010247215

表2に示すように、第1工程で形成するナゲットが大きいほど第3工程におけるチリ発生限界電流が高くなることが分かる。ナゲット径が小さいか、またはナゲットが形成されない場合では、上述したような第1工程における通電による通電径の拡大効果が殆ど得られないため、チリ抑制効果が小さいと考えられる。   As shown in Table 2, it can be seen that the larger the nugget formed in the first step, the higher the limit current for generation of dust in the third step. In the case where the nugget diameter is small or no nugget is formed, the effect of enlarging the energization diameter by energization in the first step as described above is hardly obtained, so the effect of suppressing dust is considered to be small.

つまり、第1工程時に形成するナゲットは大きいほどよいが、大きなナゲット径を狙うと、第1工程時にチリが発生してしまう可能性が高くなる。逆に、高張力鋼板ではナゲットが急激に成長するため、小さなナゲット径は形成し難く、板隙や電極磨耗等の外乱があった場合、第1工程時にナゲットが形成されず、チリ抑制効果を得られなくなる可能性がある。   That is, the larger the nugget formed in the first step, the better. However, if a large nugget diameter is aimed at, the possibility that dust will be generated in the first step increases. On the other hand, since the nugget grows rapidly in the high-strength steel plate, it is difficult to form a small nugget diameter, and when there is a disturbance such as a gap or electrode wear, the nugget is not formed in the first step, and the dust suppression effect is achieved. It may not be obtained.

そのため、実用的には、第1工程時に形成するナゲット径は、高張力鋼板の板厚をt(mm)とした場合に3√t(mm)以上5√t(mm)以下の範囲とし、チリが発生しない程度に大きなナゲット径を形成するように条件を設定することが望ましい。この時、第1工程での溶接電流は、1段通電方式におけるチリ発生限界電流の70%以上95%以下に設定することが望ましい。70%未満では第1工程で上述したナゲット径を得るための通電時間が増加し、また95%超では外乱によりチリが発生する危険性が高くなるからである。   Therefore, practically, the nugget diameter formed in the first step is in the range of 3√t (mm) to 5√t (mm) when the thickness of the high-tensile steel plate is t (mm). It is desirable to set conditions so as to form a nugget diameter that is large enough not to generate dust. At this time, it is desirable to set the welding current in the first step to 70% or more and 95% or less of the dust generation limit current in the one-stage energization method. If it is less than 70%, the energization time for obtaining the above-described nugget diameter in the first step increases, and if it exceeds 95%, the risk of dust generation due to disturbance increases.

また、表2に示す結果から、第2工程の時間が長くなるほどチリ発生限界電流が高くなることが分かる。第2工程の時間を長くすることにより、第2工程において伝熱により材料軟化領域が拡大するため、チリ発生限界電流が高くなると推察される。第2工程の時間は長いほどよいが、過度な増大は溶接時間の増加を招くため好ましくない。実用的には、第2工程の時間は1サイクル以上15サイクル以下であることが望ましく、3サイクル以上10サイクル以下であることがさらに望ましい。   Further, from the results shown in Table 2, it can be seen that as the time of the second step becomes longer, the dust generation limit current becomes higher. By extending the time of the second step, the material softening region is expanded by heat transfer in the second step, so that it is assumed that the limit generation current of dust is increased. The longer the time for the second step, the better. However, excessive increase is undesirable because it causes an increase in welding time. Practically, the time of the second step is preferably 1 cycle or more and 15 cycles or less, and more preferably 3 cycles or more and 10 cycles or less.

次に、第2工程における溶接電流について検討するため、第2工程の電流値を第1工程の溶接電流の0〜90%に変化させて、チリ発生限界電流に及ぼす影響を調査した。溶接条件を表3に、結果を表4に示す。なお、加圧力は、第1工程、第2工程、第3工程において一定値(320kgf)とした。   Next, in order to examine the welding current in the second step, the current value in the second step was changed to 0 to 90% of the welding current in the first step, and the influence on the dust generation limit current was investigated. Table 3 shows the welding conditions and Table 4 shows the results. The applied pressure was a constant value (320 kgf) in the first step, the second step, and the third step.

Figure 2010247215
Figure 2010247215

Figure 2010247215
Figure 2010247215

なお、第1工程の通電により、4.8mm(4√t)のナゲット径を有するナゲットが得られた。表4に示すように、第2工程での電流値によらず、1段通電方式に比べチリ発生限界電流が高くなる。ただし、第2工程での電流値が過大となると外乱の影響でチリが発生するおそれがあるため、第2工程における溶接電流は第1工程の溶接電流の90%以下であることが望ましい。   Note that a nugget having a nugget diameter of 4.8 mm (4√t) was obtained by energization in the first step. As shown in Table 4, the generation limit current for dust generation is higher than that in the single-stage energization method regardless of the current value in the second step. However, if the current value in the second step is excessive, dust may be generated due to the influence of disturbance. Therefore, the welding current in the second step is desirably 90% or less of the welding current in the first step.

また、第2工程の電流値が過小となると、第3工程でのナゲット成長は緩やかになるが、それだけ第3工程の所要時間が長くなり溶接時間が増大する。また、投入エネルギーが増加するという問題もある。従って、第2工程での溶接電流は、第1工程の溶接電流の20%以上90%以下が望ましい。更に望ましくは、第2工程での溶接電流は、第1工程の溶接電流の50%以上90%以下である。   Further, if the current value in the second step becomes too small, the nugget growth in the third step becomes slow, but the time required for the third step becomes longer and the welding time increases. There is also a problem that the input energy increases. Therefore, the welding current in the second step is desirably 20% or more and 90% or less of the welding current in the first step. More desirably, the welding current in the second step is not less than 50% and not more than 90% of the welding current in the first step.

このように、第1工程および第2工程の効果によって、第3工程において従来の1段通電方式のチリ発生限界電流よりも高い電流を用いてもチリが発生することなくナゲット径を拡大できるようになる。ただし、この方法では、トータルの通電時間が長くなることが懸念される。   As described above, the effect of the first step and the second step allows the nugget diameter to be expanded without generating dust even when a current higher than the current limit for generation of dust in the third step is used in the third step. become. However, with this method, there is a concern that the total energization time becomes longer.

そこで、本発明者らは、通電中に加圧力を増加して通電することを検討し、少なくとも第3工程の加圧力を第1工程の加圧力よりも高くすることにより、第1工程から第3工程までのトータルの通電時間を短縮することができることを知見した。すなわち、第3工程の加圧力を高めることにより、加圧領域が拡大するため、第3工程でのチリ発生が抑制され、より高い電流での通電が可能となり、第3工程での通電時間が短縮される。   Therefore, the present inventors examined increasing the applied pressure during energization, and at least increasing the applied pressure in the third step from the applied pressure in the first step, thereby increasing the applied pressure from the first step. It has been found that the total energization time up to 3 steps can be shortened. That is, by increasing the pressurizing force in the third step, the pressurization region is expanded, so that the generation of dust in the third step is suppressed, energization with a higher current is possible, and the energization time in the third step is Shortened.

なお、加圧力の変更は、第2工程の開始から第3工程の開始までの間の任意のタイミングで、行うことができる。第2工程においても加圧力を高めることにより、第2工程において加圧領域が拡大するので、第2工程と第3工程の加圧力を高くすることが望ましい。なお、第1工程から高い加圧力を用いた場合、第1工程で所定のナゲット径を得るために高い電流値が必要となり、エネルギーコストが嵩むという問題がある。
本発明は、これらの知見に基づいてなされたものである。
The applied pressure can be changed at an arbitrary timing from the start of the second process to the start of the third process. Since the pressurizing region is expanded in the second step by increasing the pressure in the second step, it is desirable to increase the pressure in the second step and the third step. When a high pressure is used from the first step, a high current value is required to obtain a predetermined nugget diameter in the first step, which increases the energy cost.
The present invention has been made based on these findings.

本発明に係る高張力鋼板の抵抗溶接方法は、少なくとも1枚の高張力鋼板を含む、少なくとも2枚の鋼板を重ね合わせて抵抗溶接する高張力鋼板の抵抗溶接方法であって、この少なくとも2枚の鋼板への通電により所定のナゲット径を有するナゲットを形成する第1工程と、この第1工程の後に溶接電流を降下する第2工程と、この第2工程の後に第1工程の溶接電流より大きな溶接電流を通電するとともに第1工程の加圧力より大きい加圧力を付与してナゲットを拡大する第3工程とを有することを特徴とする。   A resistance welding method for a high strength steel sheet according to the present invention is a resistance welding method for a high strength steel sheet that includes at least one high strength steel sheet and that performs resistance welding by superposing at least two steel sheets. From the first step of forming a nugget having a predetermined nugget diameter by energizing the steel plate, the second step of lowering the welding current after the first step, and the welding current of the first step after the second step And a third step of enlarging the nugget by applying a large welding current and applying a pressing force larger than the pressing force of the first step.

この発明では、所定のナゲット径は、3√t(mm)以上5√t(mm)以下であることが望ましい。ただし、tは2枚の鋼板のうちの板厚が小さい鋼板の板厚(mm)である。
これらの発明では、第3工程における加圧力は、第1工程における加圧力の110%以上150%以下あることが望ましい。
In the present invention, the predetermined nugget diameter is desirably 3√t (mm) or more and 5√t (mm) or less. However, t is the plate thickness (mm) of a steel plate having a small plate thickness of the two steel plates.
In these inventions, the applied pressure in the third step is desirably 110% or more and 150% or less of the applied pressure in the first step.

これらの発明では、第2工程の処理時間は、1.0サイクル以上15サイクル以下であることが望ましい。ただし、1.0サイクルは、商用電源周波数が60Hzの場合には(1/60)秒であり、商用電源周波数が50Hzの場合には(1/50)秒である。   In these inventions, the processing time of the second step is desirably 1.0 cycle or more and 15 cycles or less. However, 1.0 cycle is (1/60) seconds when the commercial power supply frequency is 60 Hz, and (1/50) seconds when the commercial power supply frequency is 50 Hz.

これらの発明では、第2工程における溶接電流は、第1工程における溶接電流の20%以上90%以下であることが望ましい。
これらの発明では、第3工程における溶接電流は、第1工程における溶接電流の100%以上200%以下であることが望ましい。
In these inventions, the welding current in the second step is desirably 20% or more and 90% or less of the welding current in the first step.
In these inventions, the welding current in the third step is desirably 100% or more and 200% or less of the welding current in the first step.

これらの発明では、高張力鋼板は、引張強度が440MPa以上の鋼板であることが望ましい。
これらの本発明の第3工程の通電は、通電と通電停止との周期を複数回繰り返すパルセーション通電で行うことが望ましい。この場合に、複数回の周期における第2周期以降の通電時の溶接電流は、第1周期の通電時の溶接電流より大きいことがさらに望ましい。
In these inventions, the high-tensile steel plate is desirably a steel plate having a tensile strength of 440 MPa or more.
The energization in the third step of the present invention is preferably performed by pulsation energization in which the cycle of energization and energization stop is repeated a plurality of times. In this case, it is more desirable that the welding current during energization after the second period in a plurality of cycles is greater than the welding current during energization during the first period.

本発明によれば、高張力鋼板の抵抗溶接において、溶接時間の増加を抑制しながら、通電時のチリ(初期チリおよび中チリ)の発生を抑制し、充分な大きさのナゲット径を有するナゲットを確実に形成することができる。また、板−板間に隙間が存在する場合であってもこの効果が失われることはない。   According to the present invention, in resistance welding of a high-strength steel sheet, a nugget having a sufficiently large nugget diameter is suppressed by suppressing generation of dust (initial dust and medium dust) during energization while suppressing increase in welding time. Can be reliably formed. Even if there is a gap between the plates, this effect is not lost.

このため、本発明によれば、チリ発生を抑制して生産ラインにおける作業環境を改善することができる。さらに、抵抗溶接継手の強度特性はチリが発生すると劣化することが知られているが、チリの発生を防止し、ナゲット径を拡大することによって、強度特性に優れた抵抗溶接継手を作ることができる。また、チリ発生に伴うバリ取りなどの後工程を省略できるため、作業能率の向上にもつながる。   For this reason, according to this invention, generation | occurrence | production of dust can be suppressed and the working environment in a production line can be improved. Furthermore, the strength characteristics of resistance welded joints are known to deteriorate when dust occurs, but resistance welded joints with superior strength characteristics can be made by preventing the generation of dust and increasing the nugget diameter. it can. In addition, post-processing such as deburring associated with the generation of dust can be omitted, leading to improved work efficiency.

一般的に、4√t(mm)以上のナゲット径が生産管理上の基準とされることが多い。しかし、実際の生産においては、板隙、分流、電極磨耗の影響等を考慮し、安全を見込んで狙いナゲット径が得られる電流値よりも高めの電流値に設定される。そのため、従来の1段通電ではチリが発生し易かった。これに対し、本発明によれば、第1工程で所定寸法のナゲットが形成され、第2工程でナゲットの周囲に存在する軟化領域が拡大されるので、第3工程で、従来の技術ではチリが発生していた電流値であってもチリが発生することなくナゲット径を拡大でき、さらに、第3工程では高い加圧力が付与されるので、溶接時間の増大が抑制され、効率的な溶接を行うことができる。   In general, a nugget diameter of 4√t (mm) or more is often used as a production management standard. However, in actual production, the current value is set to be higher than the current value for obtaining the target nugget diameter in consideration of safety in consideration of the influence of plate gap, shunt flow, electrode wear, and the like. For this reason, dust is easily generated in the conventional one-stage energization. On the other hand, according to the present invention, a nugget having a predetermined size is formed in the first step, and the softened region existing around the nugget is enlarged in the second step. The nugget diameter can be expanded without generation of dust even if the current value has been generated. Furthermore, since a high pressurizing force is applied in the third step, an increase in welding time is suppressed and efficient welding is achieved. It can be performed.

図1は、通電を1回だけ行う1段通電方式による抵抗溶接における通電時間と、電流または加圧力との関係の一例を示すグラフである。FIG. 1 is a graph showing an example of the relationship between the energization time and the current or the applied pressure in resistance welding by the one-stage energization method in which energization is performed only once. 図2は、予備通電によりワーク接触面同士のなじみをよくした後に本通電を行う2段通電方式による抵抗溶接における通電時間と、電流または加圧力との関係の一例を示すグラフである。FIG. 2 is a graph showing an example of the relationship between the energization time and the current or the applied pressure in resistance welding by the two-stage energization method in which the main energization is performed after the familiarity between the workpiece contact surfaces is improved by preliminary energization. 図3は、スポット溶接における軟鋼からなる鋼板の通電径およびナゲットの成長の様子を模式的に示す説明図である。FIG. 3 is an explanatory view schematically showing a current-carrying diameter of a steel plate made of mild steel and the state of nugget growth in spot welding. 図4は、スポット溶接における高張力鋼からなる鋼板の通電径およびナゲットの成長の様子を模式的に示す説明図である。FIG. 4 is an explanatory view schematically showing a current-carrying diameter of a steel plate made of high-strength steel and spot nugget growth in spot welding. 図5は、1段通電方式により高張力鋼板をスポット溶接する際のナゲットとコロナボンドとの成長を模式的に示す説明図である。FIG. 5 is an explanatory view schematically showing the growth of nuggets and corona bonds when spot-welding a high-tensile steel plate by a one-stage energization method. 図6は、本発明に係る高張力鋼板の抵抗溶接方法における通電時間と、電流または加圧力との関係の一例を示すグラフである。FIG. 6 is a graph showing an example of the relationship between the energization time and the current or the applied pressure in the resistance welding method for high-tensile steel plates according to the present invention. 図7は、本発明に係る高張力鋼板の抵抗溶接方法におけるナゲットとコロナボンド(加圧領域)との成長を模式的に示す説明図である。FIG. 7 is an explanatory view schematically showing growth of a nugget and a corona bond (pressure region) in the resistance welding method for a high-strength steel sheet according to the present invention. 図8は、本発明に係る高張力鋼板の抵抗溶接方法における通電時間と、電流または加圧力との関係の一例を示すグラフであり、第3工程の通電方式がパルセーション通電方式であってその通電電流が一定の場合である。FIG. 8 is a graph showing an example of the relationship between the energization time and the current or the applied pressure in the resistance welding method for high-strength steel sheets according to the present invention. The energization method in the third step is a pulsation energization method. This is the case when the energization current is constant. 図9は、本発明に係る高張力鋼板の抵抗溶接方法における通電時間と、電流または加圧力との関係の一例を示すグラフであり、第3工程の通電方式がパルセーション通電方式であって第1周期の通電電流が第2周期以降に比べて小さい場合である。FIG. 9 is a graph showing an example of the relationship between energization time and current or applied pressure in the resistance welding method for high-tensile steel plates according to the present invention. The energization method in the third step is a pulsation energization method. This is a case where the energization current of one cycle is smaller than that after the second cycle.

以下、本発明を実施するための形態を説明する。なお、本発明は、スポット溶接、片側スポット溶接、シリーズスポット溶接、さらにはダイレクトスポット溶接等の抵抗溶接に対して広く適用可能である。以降の説明では、自動車の分野で広く用いられるスポット溶接を例にとる。   Hereinafter, modes for carrying out the present invention will be described. The present invention can be widely applied to resistance welding such as spot welding, one-side spot welding, series spot welding, and direct spot welding. In the following description, spot welding widely used in the field of automobiles is taken as an example.

本発明が対象とする板組みは、少なくとも1枚の公称引張強さ440MPa級以上の高張力鋼板を含む、複数枚の重ね合わせ鋼板である。   The plate assembly to which the present invention is directed is a plurality of laminated steel plates including at least one high tensile steel plate having a nominal tensile strength of 440 MPa or higher.

高張力鋼板の種類は、特に規定する必要はない。例えば、析出強化鋼やDP鋼、TRIP(加工誘起変態)鋼、さらには熱間プレス鋼板等の、公知の各種の公称引張強さが440MPa以上の高張力鋼板に適用可能である。また、板組みに含まれるいずれの鋼板は、冷延鋼板でもよく、または熱延鋼板でもよい。さらに裸鋼板でもめっき鋼板でもよく、めっきの種類にも限定されない。   The type of high-tensile steel plate need not be specified. For example, the present invention can be applied to various known high tensile strength steel sheets having a nominal tensile strength of 440 MPa or more, such as precipitation strengthened steel, DP steel, TRIP (work induced transformation) steel, and hot pressed steel sheets. Moreover, any steel plate included in the plate assembly may be a cold-rolled steel plate or a hot-rolled steel plate. Furthermore, it may be a bare steel plate or a plated steel plate, and is not limited to the type of plating.

高張力鋼板の板厚も特に規定する必要はない。一般に、自動車用部品や車体で使用される鋼板の板厚は0.4mm以上4.0mm以下であり、本発明はこの範囲において充分な効果を有する。   The thickness of the high-tensile steel plate need not be specified. In general, the thickness of a steel plate used in automobile parts and vehicle bodies is 0.4 mm or more and 4.0 mm or less, and the present invention has a sufficient effect in this range.

図6は、本発明に係る高張力鋼板の抵抗溶接方法における通電時間と、電流または加圧力との関係の一例を示すグラフである。また、図7は、本発明に係る高張力鋼板の抵抗溶接方法におけるナゲットとコロナボンド(加圧領域)との成長を模式的に示す説明図である。   FIG. 6 is a graph showing an example of the relationship between the energization time and the current or the applied pressure in the resistance welding method for high-tensile steel plates according to the present invention. Moreover, FIG. 7 is explanatory drawing which shows typically the growth of the nugget and the corona bond (pressurization area | region) in the resistance welding method of the high strength steel plate which concerns on this invention.

図6に示すように、本発明に係る抵抗溶接方法は、適正な大きさのナゲットを形成する第1工程である予備通電工程と、予備通電後に電流を降下させるとともに加圧力を上昇させ、ナゲットの周囲の加圧域の拡大を図る第2工程と、第2工程後に第2工程の加圧力を維持しながら予備通電電流よりも大きな電流を流しナゲット径を拡大する第3工程である本通電工程とにより構成される。以下、第1工程〜第3工程を詳細に説明する。   As shown in FIG. 6, the resistance welding method according to the present invention includes a preliminary energization process that is a first process for forming a nugget of an appropriate size, a current decrease and a pressurization force after the preliminary energization, A second step for expanding the pressurizing region around the main body and a third step for expanding the nugget diameter by flowing a current larger than the preliminary energization current while maintaining the applied pressure in the second step after the second step. Process. Hereinafter, the first to third steps will be described in detail.

第1工程では、図7のAに示すように、溶接する2枚の鋼板のうちの板厚が小さい鋼板の板厚をt(mm)としたときに3√t(mm)以上5√t(mm)以下のナゲット径を有するナゲット3を形成するように、第1工程における通電電流(以下「第1通電電流」という)と、通電時間(以下「第1通電時間」)とを調整する。 In the first step, as shown in A 2 in FIG. 7, when the 3√t (mm) more than the thickness of the plate thickness is small steel plate of the two steel plates to be welded was t (mm) 5√ The energizing current in the first step (hereinafter referred to as “first energizing current”) and the energizing time (hereinafter referred to as “first energizing time”) are adjusted so as to form a nugget 3 having a nugget diameter of t (mm) or less. To do.

第1工程で形成されるナゲット3のナゲット径が大きいほど、後述する第3工程でのチリ抑制効果が得られるが、第1工程における通電時のチリが発生するおそれが高くなる。第1工程で形成されるナゲット3のナゲット径が小さいか、または第1工程でナゲット3が形成されない場合には、第1工程における通電径の拡大効果が殆ど得られないため、第3工程におけるチリ抑制効果が小さくなる。   As the nugget diameter of the nugget 3 formed in the first step is larger, the effect of suppressing dust in the third step, which will be described later, is obtained, but there is a higher possibility that dust will be generated during energization in the first step. If the nugget diameter of the nugget 3 formed in the first step is small or if the nugget 3 is not formed in the first step, the effect of enlarging the energized diameter in the first step is hardly obtained. The effect of suppressing dust is reduced.

すなわち、高張力鋼板ではナゲット3が急激に成長し易いため、ナゲット径の狙い値が過小である場合には、板隙や電極磨耗等の外乱の影響を受け、第1工程における通電時にナゲット3が形成されず、第3工程における通電時にチリ抑制効果が充分に得られないおそれが高い。このため、実用的には、第1工程における通電時に形成するナゲット3のナゲット径は、3√t(mm)以上5√t(mm)以下の範囲でチリが発生しない程度に大きなナゲット径を狙うように溶接条件を設定する。   That is, since the nugget 3 is likely to grow rapidly in a high-strength steel plate, if the target value of the nugget diameter is too small, the nugget 3 is affected by disturbances such as a plate gap and electrode wear and is energized in the first step. Is not formed, and there is a high possibility that the effect of suppressing dust is not sufficiently obtained during energization in the third step. Therefore, practically, the nugget diameter of the nugget 3 formed at the time of energization in the first process has a large nugget diameter that does not generate dust in the range of 3√t (mm) to 5√t (mm). Set the welding conditions to aim.

この時、第1工程での溶接条件は、1段通電方式でのチリ発生電流の70%以上95%以下に設定することが望ましい。70%未満では上述したナゲット径を得るためのサイクルタイムが増加し、また95%超では外乱によりチリが発生する危険性があるからである。   At this time, it is desirable to set the welding conditions in the first step to 70% or more and 95% or less of the dust generation current in the one-stage energization method. If it is less than 70%, the cycle time for obtaining the above-described nugget diameter increases, and if it exceeds 95%, there is a risk of dust generation due to disturbance.

本発明の第2工程では、溶接電流は、第1工程の電流に比較して小さくする。第2工程における溶接電流はゼロとしてもよい。これにより、第2工程では、図7のBに示すように、ナゲット3の成長は抑制され、かつ伝熱によりコロナボンド4は拡大される。 In the second step of the present invention, the welding current is made smaller than the current in the first step. The welding current in the second step may be zero. Thus, in the second step, as shown in B 2 in FIG. 7, the growth of the nugget 3 is suppressed, and the corona bond 4 is enlarged by heat transfer.

すなわち、第3工程の直前では、第2工程の直前に比べて、ナゲット3の大きさに対してコロナボンド4の割合が大きくなり、さらにこれに伴い、第3工程において、通電径が拡大されるため第3工程におけるチリ発生が抑制される。   That is, immediately before the third step, the ratio of the corona bond 4 with respect to the size of the nugget 3 is larger than that immediately before the second step. Further, in accordance with this, the energization diameter is increased in the third step. Therefore, generation of dust in the third step is suppressed.

溶接電流が過大であると、外乱の影響により第2工程においてチリが発生し易くなり、一方、溶接電流が過小であると、ナゲットが冷却されて第3工程の処理時間が増加し易いといった問題を生じる。このため、第2工程における溶接電流は、第1工程における溶接電流の20%以上90%以下とすることが望ましい。さらに望ましくは、第2工程での溶接電流は、第1工程の溶接電流の50%以上90%以下である。   If the welding current is excessive, dust is likely to be generated in the second step due to the influence of disturbance, whereas if the welding current is excessive, the nugget is cooled and the processing time of the third step is likely to increase. Produce. For this reason, it is desirable that the welding current in the second step be 20% or more and 90% or less of the welding current in the first step. More desirably, the welding current in the second step is not less than 50% and not more than 90% of the welding current in the first step.

第2工程の処理時間が長くなるほど第3工程でのチリ抑制効果が得られるものの、過度な延長はタクトタイムの増大を招くため好ましくない。一方、第2工程の処理時間が過小であると第2工程におけるコロナボンド4の拡大効果が小さく、第3工程におけるチリ抑制効果が小さくなる。したがって、第2工程の処理時間は、1.0サイクル以上15サイクル以下とすることが望ましく、さらに望ましくは3.0サイクル以上10サイクル以下である。   Although the effect of suppressing dust in the third step is obtained as the treatment time of the second step becomes longer, excessive extension is not preferable because it causes an increase in tact time. On the other hand, if the treatment time of the second step is too short, the effect of expanding the corona bond 4 in the second step is small and the effect of suppressing dust in the third step is small. Accordingly, the processing time of the second step is desirably 1.0 cycle or more and 15 cycles or less, and more desirably 3.0 cycles or more and 10 cycles or less.

第2工程では、加圧力を第1工程の加圧力より大きくするのが望ましい。加圧力の上昇によりチリ抑制の効果が大きくなる。ただし、過大な加圧力では、溶接部の板厚減少が大きくなるため好ましくない。例えば、第1工程の加圧力の110%以上150%以下に設定する。   In the second step, it is desirable that the pressure is larger than the pressure in the first step. The effect of suppressing dust is increased by increasing the pressure. However, an excessive pressurizing force is not preferable because a reduction in the thickness of the welded portion increases. For example, it is set to 110% or more and 150% or less of the applied pressure in the first step.

第3工程では、第1工程の加圧力より大きい加圧力で加圧するとともに、第1工程の電流よりも高い溶接電流を流してナゲット3のナゲット径を拡大する。第3工程の開始時には、図7のBに示すように、ナゲット3のナゲット径に対して充分なコロナボンド4が形成されており、第3工程における通電によりナゲット3のナゲット径が拡大しても充分な通電径を備えているため、図7のDに示すように、チリの発生を抑制しながらナゲット3のナゲット径を拡大することができる。 In the third step, the nugget diameter of the nugget 3 is increased by applying a welding current higher than the pressure in the first step and applying a welding current higher than the current in the first step. At the start of the third step, as shown in B 2 in FIG. 7, and sufficient corona bond 4 are formed for the nugget diameter of the nugget 3, the nugget diameter of the nugget 3 is expanded by energizing the third step due to the provision of a sufficient current diameter also, as shown in D 2 of FIG. 7, it is possible to increase the nugget diameter of the nugget 3 while suppressing the generation of dust.

第3工程での溶接電流は、第1工程の通電電流の110%以上200%以下であることが望ましい。110%未満ではナゲット3のナゲット径を拡大するための処理時間が増加し、一方、200%超ではチリが発生し易くなる。なお、図6および図7により示す本実施の形態の第3工程は、連続して通電する連続通電方式であるが、連続通電方式に限定されるものでなく、図8に示すように通電と通電休止との周期を複数回繰り返す、所謂パルセーション通電方式としてもよい。パルセーション通電方式として、例えば、3サイクル通電後1サイクル休止とする周期を繰り返す通電方式が例示される。   The welding current in the third step is desirably 110% or more and 200% or less of the energization current in the first step. If it is less than 110%, the processing time for enlarging the nugget diameter of the nugget 3 increases, whereas if it exceeds 200%, dust tends to be generated. Note that the third step of the present embodiment shown in FIGS. 6 and 7 is a continuous energization method in which energization is continuously performed, but is not limited to the continuous energization method, and as shown in FIG. A so-called pulsation energization method may be used in which the cycle of energization is repeated a plurality of times. As the pulsation energization method, for example, an energization method that repeats a period of one cycle rest after three cycles energization is exemplified.

パルセーション通電方式では、通電休止により通電径拡大効果が大きくなり、連続通電方式に比べチリ発生を抑制できるので望ましい。また、パルセーション通電方式においては、第1周期の通電時にチリが発生しやすいので、複数回の周期のなかで、図9に示すように、第1周期における通電時の溶接電流を第2周期以降の通電時の溶接電流より小さくするのが望ましい。なお、第1周期の通電時の溶接電流は、第1工程の溶接電流よりも大きくするのが望ましい。   In the pulsation energization method, the effect of enlarging the energization diameter is increased by stopping energization, and dust generation can be suppressed as compared with the continuous energization method. Further, in the pulsation energization method, dust is likely to be generated during energization in the first cycle, and therefore, during a plurality of cycles, the welding current during energization in the first cycle is set to the second cycle as shown in FIG. It is desirable to make it smaller than the welding current during energization thereafter. In addition, it is desirable to make the welding current at the time of energization of the 1st period larger than the welding current of the 1st process.

第3工程の加圧力を第1工程の加圧力より大きくすることにより、コロナボンド4が拡大するため、第3工程の通電電流値を大きくすることが可能となり、ナゲット3のナゲット径を拡大しながら第3工程での通電時間を短縮することができる。第3工程における加圧力は、第1工程の加圧力の110%以上150%以下に設定するのが望ましい。110%未満では、加圧力の上昇によるチリ抑制の効果拡大が小さく、一方、150%超では溶接部の板厚減少が大きく、板がひずみ易いため好ましくない。   By making the pressure in the third step larger than the pressure in the first step, the corona bond 4 expands, so that the current value in the third step can be increased, and the nugget diameter of the nugget 3 is increased. However, the energization time in the third step can be shortened. The pressing force in the third step is preferably set to 110% to 150% of the pressing force in the first step. If it is less than 110%, the expansion of the effect of suppressing dust due to the increase in the applied pressure is small.

なお、以上の説明では、第2工程ならびに第3工程の加圧力を、第1工程の加圧力より高くする場合を例にとったが、必ずしもこの場合に限定されるものではなく、少なくとも第3工程の加圧力を第1工程の加圧力より高くすればよい。   In the above description, the case where the applied pressure in the second process and the third process is set higher than the applied pressure in the first process is taken as an example. However, the present invention is not necessarily limited to this case, and at least the third process. What is necessary is just to make the applied pressure of a process higher than the applied pressure of a 1st process.

以上説明したように、本発明によれば、高張力鋼板の抵抗溶接において、溶接時間の増加を抑制しながら、通電時のチリ(初期チリおよび中チリ)の発生を抑制し、充分な大きさのナゲット径を有するナゲット3を確実に形成することができる。また、板−板間に隙間が存在する場合であってもこの効果が失われることはない。   As described above, according to the present invention, in resistance welding of a high-strength steel plate, generation of dust (initial dust and medium dust) during energization is suppressed while suppressing an increase in welding time, and the size is sufficiently large. The nugget 3 having the nugget diameter can be surely formed. Even if there is a gap between the plates, this effect is not lost.

このため、本発明によれば、チリ発生を抑制して生産ラインにおける作業環境を改善することができる。さらに、本発明によれば、チリの発生を防止してナゲット3のナゲット径を拡大することができるので、強度特性に優れた抵抗溶接継手を作ることができる。また、チリ発生に伴うバリ取りなどの後工程を省略できるため、作業能率の向上にもつながる。   For this reason, according to this invention, generation | occurrence | production of dust can be suppressed and the working environment in a production line can be improved. Furthermore, according to the present invention, generation of dust can be prevented and the nugget diameter of the nugget 3 can be increased, so that a resistance weld joint having excellent strength characteristics can be made. In addition, post-processing such as deburring associated with the generation of dust can be omitted, leading to improved work efficiency.

さらに、本発明によれば、第1工程で所定寸法のナゲット3が形成され、第2工程でナゲット3の周囲に存在するコロナボンド4(軟化領域)が拡大されるので、第3工程で、従来の技術ではチリが発生していた電流値であってもチリが発生することなくナゲット3のナゲット径を拡大でき、さらに、第3工程では高い加圧力が付与されるので、溶接時間の増大が抑制され、効率的な溶接を行うことができる。   Furthermore, according to the present invention, the nugget 3 having a predetermined size is formed in the first step, and the corona bond 4 (softening region) existing around the nugget 3 is expanded in the second step. Therefore, in the third step, The nugget diameter of the nugget 3 can be increased without generation of dust even if the current value has generated dust in the conventional technology. Further, since a high pressing force is applied in the third step, the welding time is increased. Is suppressed, and efficient welding can be performed.

実施例を参照しながら、本発明をより具体的に説明する。
先端径6mmのドーム型電極を備えたエアー加圧方式の単相交流スポット溶接機を用い、板厚1.4mmの980MPa級亜鉛めっき鋼板を2枚重ね合わせて、本発明における第1工程、第2工程および第3工程からなる多段通電を行うとともに、第1工程後に加圧力を第1工程の加圧力(320kgf)の125%に上昇させ、第2工程と第3工程の加圧力を400kgfとした2段加圧の溶接を行い、チリの発生状況とナゲット径を調査した。
The present invention will be described more specifically with reference to examples.
Using a single-phase AC spot welder of an air pressure method with a dome-shaped electrode having a tip diameter of 6 mm, two 980 MPa grade galvanized steel sheets having a thickness of 1.4 mm are overlapped to form the first step, Multi-stage energization consisting of two steps and a third step is performed, and after the first step, the applied pressure is increased to 125% of the applied pressure (320 kgf) of the first step, and the applied pressure of the second step and the third step is set to 400 kgf. Two-stage pressurization welding was performed, and the occurrence of dust and the nugget diameter were investigated.

また、比較のため、1段通電の従来例ならびに第1工程から第3工程まで加圧力を一定(320kgf)とした多段通電の比較例も行った。それぞれの溶接条件を表5〜7に、結果を表8に示す。なお、第1工程における溶接電流は、1段通電方式でのチリ発生限界電流の90%の電流値である。また、各表のホールド時間は、第3工程における通電完了後、通電しない状態で電極により加圧している時間を意味する。   For comparison, a conventional example of one-stage energization and a comparative example of multi-stage energization with a constant pressure (320 kgf) from the first step to the third step were also performed. The respective welding conditions are shown in Tables 5 to 7, and the results are shown in Table 8. In addition, the welding current in the first step is a current value that is 90% of the dust generation limit current in the one-stage energization method. The hold time in each table means the time during which pressure is applied by the electrode without energization after completion of energization in the third step.

Figure 2010247215
Figure 2010247215

Figure 2010247215
Figure 2010247215

Figure 2010247215
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Figure 2010247215
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表8に示すように、本発明によりチリ発生を抑制しながら、従来例(1段通電方式)、比較例(加圧力一定多段通電方式)よりもナゲット径を拡大できることが分かる。なお、表8において、本発明例は、比較例に比べナゲット径の拡大効果が小さいように見られるが、第3工程の処理時間が18サイクルと十分に長いため、使用した電極により得られるナゲット径の最大値に飽和しつつあるためと考えられる。すなわち、本発明例によれば、比較例に較べて、短い通電時間で大きなナゲット径のナゲットを形成することが可能となる。   As shown in Table 8, it can be seen that the nugget diameter can be increased as compared with the conventional example (one-stage energization method) and the comparative example (constant pressure multi-stage energization method) while suppressing generation of dust by the present invention. In Table 8, the example of the present invention seems to have a smaller nugget diameter expansion effect than the comparative example, but the processing time of the third step is sufficiently long as 18 cycles, so the nugget obtained by the used electrode This is thought to be because the maximum value of the diameter is being saturated. That is, according to the example of the present invention, it is possible to form a nugget having a large nugget diameter in a short energization time as compared with the comparative example.

板厚1.4mmの980MPa級鋼板を2枚重ね合わせた板組にて、FEM解析によるスポット溶接のシミュレーションを行い、チリ発生限界電流と最大ナゲット径を調査した。なお、解析は、電場―温度場連成解析と温度場―応力場連成解析を(1/2)サイクルごとに交互に繰り返す増分連成解析手法にて行った、   A spot welding simulation by FEM analysis was performed on a plate assembly in which two 980 MPa class steel plates having a thickness of 1.4 mm were overlapped, and the limit current for generation of dust and the maximum nugget diameter were investigated. The analysis was performed by an incremental coupled analysis method in which an electric field-temperature field coupled analysis and a temperature field-stress field coupled analysis were alternately repeated every (1/2) cycle.

本発明例では、第1工程、第2工程および第3工程からなり、かつ第1工程の後に加圧力を増加させる多段通電で、第3工程の通電方法として、連続通電方式(本発明例1)とパルセーション通電方式(本発明例2)を実施し、1段通電の方式(従来例)と比較した。なお、本発明例2では、パルセーション通電における複数回の通電電流を一定としたタイプAと、パルセーション通電における第1周期の溶接電流を第2周期以降の溶接電流の80%としたタイプBを実施した。比較例、本発明例1、本発明例2のそれぞれの溶接条件を表9〜11に示す。なお、電極は先端径6mmのドーム型とした。   In the present invention example, a continuous energization method (invention example 1) is used as the energization method of the third step by multi-stage energization consisting of the first step, the second step and the third step and increasing the applied pressure after the first step. ) And the pulsation energization method (Example 2 of the present invention) were performed and compared with the one-stage energization method (conventional example). In addition, in Example 2 of the present invention, type A in which the energization current for a plurality of times in pulsation energization is constant, and type B in which the welding current in the first period in pulsation energization is 80% of the welding current after the second period. Carried out. Tables 9 to 11 show the welding conditions of Comparative Example, Invention Example 1 and Invention Example 2. The electrode was a dome shape with a tip diameter of 6 mm.

解析結果を従来例と比較して表12に示す。表12に示すように、1段通電では、チリが発生しない限界の電流(チリ発生電流)が6.6kAでそのときのナゲット径が5.4mmであるが、本発明例1では8.0kA、6.3mmとなり、多段通電によりチリ発生が抑制された。さらに、パルセーション通電方式は、連続通電方式に比べ、チリ発生電流が大きくなり、チリの発生が一層抑制されることが判った。また、パルセーション通電方式では、第1番目の通電電流を小さくしたタイプBは、電流を一定としたタイプAに比べ、チリ発生抑制効果が大きいことが判った。   The analysis results are shown in Table 12 in comparison with the conventional example. As shown in Table 12, in the one-stage energization, the limit current at which no dust is generated (dust generation current) is 6.6 kA and the nugget diameter at that time is 5.4 mm, but in Example 1 of the present invention, 8.0 kA. 6.3 mm, and generation of dust was suppressed by multi-stage energization. Further, it was found that the pulsation energization method has a larger dust generation current than the continuous energization method, and the generation of dust is further suppressed. In addition, in the pulsation energization method, it was found that Type B with the first energization current being smaller has a greater effect of suppressing the generation of dust than Type A with a constant current.

Figure 2010247215
Figure 2010247215

Figure 2010247215
Figure 2010247215

Figure 2010247215
Figure 2010247215

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Figure 2010247215

1、2 軟鋼からなる鋼板
3 ナゲット
4 コロナボンド
5、6 電極
7 通電経路
8、9 高張力鋼からなる鋼板
1, 2 Steel plate made of mild steel 3 Nugget 4 Coronabond 5, 6 Electrode 7 Current path 8, 9 Steel plate made of high-strength steel

Claims (9)

少なくとも1枚の高張力鋼板を含む、少なくとも2枚の鋼板を重ね合わせて抵抗溶接する高張力鋼板の抵抗溶接方法であって、前記少なくとも2枚の鋼板への通電により所定のナゲット径を有するナゲットを形成する第1工程と、前記第1工程の後に溶接電流を降下する第2工程と、前記第2工程の後に前記第1工程の溶接電流より大きな溶接電流を通電するとともに前記第1工程の加圧力より大きい加圧力を付与してナゲットを拡大する第3工程とを有することを特徴とする高張力鋼板の抵抗溶接方法。   A resistance welding method for a high strength steel plate including at least one high strength steel plate, wherein at least two steel plates are overlapped and resistance welded, wherein the nugget has a predetermined nugget diameter by energizing the at least two steel plates. A first step of forming a welding current, a second step of lowering the welding current after the first step, a current flowing larger than the welding current of the first step after the second step, and the first step And a third step of enlarging the nugget by applying a pressing force larger than the pressing force. 前記所定のナゲット径は、3√t以上5√t以下である請求項1に記載の高張力鋼板の抵抗溶接方法。
ただし、tは前記少なくとも2枚の鋼板のうちの板厚が小さい鋼板の板厚(mm)である。
The resistance welding method for high-tensile steel sheets according to claim 1, wherein the predetermined nugget diameter is 3√t or more and 5√t or less.
However, t is the plate thickness (mm) of the steel plate having a small plate thickness among the at least two steel plates.
前記第3工程における加圧力は、前記第1工程における加圧力の110%以上150%以下ある請求項1または請求項2に記載の高張力鋼板の抵抗溶接方法。   The resistance welding method for high-tensile steel sheets according to claim 1 or 2, wherein the pressing force in the third step is 110% to 150% of the pressing force in the first step. 前記第2工程の処理時間は、1.0サイクル以上15サイクル以下である請求項1から請求項3までのいずれか1項に記載の高張力鋼板の抵抗溶接方法。   The high-strength steel sheet resistance welding method according to any one of claims 1 to 3, wherein a processing time of the second step is 1.0 cycle or more and 15 cycles or less. 前記第2工程における溶接電流は、前記第1工程における溶接電流の20%以上90%以下である請求項1から請求項4までのいずれか1項に記載の高張力鋼板の抵抗溶接方法。   The high-strength steel sheet resistance welding method according to any one of claims 1 to 4, wherein a welding current in the second step is 20% or more and 90% or less of a welding current in the first step. 前記第3工程における溶接電流は、前記第1工程における溶接電流の110%以上200%以下である請求項1から請求項5までのいずれか1項に記載の高張力鋼板の抵抗溶接方法。   6. The high-strength steel sheet resistance welding method according to claim 1, wherein the welding current in the third step is not less than 110% and not more than 200% of the welding current in the first step. 前記高張力鋼板は、引張強度が440MPa以上の鋼板である請求項1から請求項6までのいずれか1項に記載の高張力鋼板の抵抗溶接方法。   The resistance welding method for a high strength steel sheet according to any one of claims 1 to 6, wherein the high strength steel sheet is a steel sheet having a tensile strength of 440 MPa or more. 前記第3工程の通電は、通電と通電停止との周期を複数回繰り返すパルセーション通電で行う請求項1から請求項7までのいずれか1項に記載の高張力鋼板の抵抗溶接方法。   The high-strength steel sheet resistance welding method according to any one of claims 1 to 7, wherein the energization in the third step is performed by pulsation energization in which a cycle of energization and energization stop is repeated a plurality of times. 前記複数回の周期における第2周期以降の通電時の溶接電流は、第1周期の通電時の溶接電流より大きい請求項8に記載の高張力鋼板の抵抗溶接方法。   The resistance welding method for high-tensile steel sheets according to claim 8, wherein a welding current during energization after the second cycle in the plurality of cycles is larger than a welding current during energization during the first cycle.
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