JPH0790384B2 - Resistance spot welding method - Google Patents
Resistance spot welding methodInfo
- Publication number
- JPH0790384B2 JPH0790384B2 JP2303726A JP30372690A JPH0790384B2 JP H0790384 B2 JPH0790384 B2 JP H0790384B2 JP 2303726 A JP2303726 A JP 2303726A JP 30372690 A JP30372690 A JP 30372690A JP H0790384 B2 JPH0790384 B2 JP H0790384B2
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- nugget
- diameter
- welding
- waveform
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Description
【発明の詳細な説明】 (産業上の利用分野) この発明は抵抗スポット溶接方法に関するものである。TECHNICAL FIELD The present invention relates to a resistance spot welding method.
(従来の技術及びその問題点) 抵抗スポット溶接部の品質保証を行うために、従来はナ
ゲット径の大きさの保証だけが行われてきた。裸鋼板な
どは散りが発生しても溶接品質の劣化(ナゲット径の減
少)がみられないので、現場的には、この散りを品質モ
ニタとし、品質保証の手段としてきた。しかし最近使用
が多くなってきためっき鋼板では、この散り発生によっ
てかえってナゲット径が小さくなる。この場合散りは品
質確保の手段とはならない。また溶接ロボットの導入に
伴い、この散り発生による作業環境の劣化も大きな問題
となってきている。このため最近では、散りの発生しな
い、しかも品質確保(ナゲット径の確保)のできる溶接
の実現が望まれるようになってきている。(Prior Art and Problems Thereof) In order to guarantee the quality of the resistance spot welded portion, conventionally, only the size of the nugget diameter has been guaranteed. Since the deterioration of the welding quality (reduction of the nugget diameter) is not observed even when the bare steel plate or the like is spattered, this spot has been used as a quality monitor and as a means of quality assurance on site. However, in the case of plated steel sheets which have been used more and more recently, the nugget diameter is rather reduced due to the occurrence of the scattering. In this case, dust is not a means of ensuring quality. In addition, with the introduction of welding robots, the deterioration of the work environment due to the occurrence of this scattering has become a major problem. For this reason, in recent years, it has been desired to realize welding in which scattering does not occur and quality can be secured (nugget diameter is secured).
この目的を実現するためには、フィードバック制御が一
つの解となる。しかし現在のところ適確なモニタ法が確
立していない。もう一つの考えは、電源特性を調節する
ことにより、散りが発生せず、しかもある寸法のナゲッ
ト径が得られる電流域、いわゆる溶接条件裕度を拡大す
ることである。この考えの一部としては、電流波形の影
響や電源特性の影響についてのものが既に行われてお
り、結果としての、溶接条件裕度拡大の効果が得られる
ことが明らかになっている。しかしこのうち最も効果が
あると判断される直流電源(三相整流電源)を用いた電
源特性の電力化では、その調整効果が短時間側では現れ
ないという問題点が残っている。これはナゲット成長の
遅れが原因であると想定される。To achieve this goal, feedback control is one solution. However, an accurate monitoring method has not been established at present. Another idea is to adjust the power supply characteristics to increase the current range in which no scattering occurs and a certain size of the nugget diameter can be obtained, that is, the so-called welding condition margin. As part of this idea, the influence of the current waveform and the influence of the power source characteristic have already been made, and it has been clarified that the effect of widening the welding condition margin can be obtained as a result. However, in the power conversion of the power supply characteristics using the DC power supply (three-phase rectification power supply), which is judged to be most effective, there remains a problem that the adjustment effect does not appear on the short time side. This is assumed to be due to the delay in nugget growth.
この発明は上記従来の欠点を解決するためになされたも
のであって、その目的は、短時間通電条件においても、
従来よりも溶接条件裕度を拡大することが可能な抵抗ス
ポット溶接方法を提供することにある。The present invention has been made to solve the above-mentioned conventional drawbacks, and its purpose is to provide a short-time energization condition.
An object of the present invention is to provide a resistance spot welding method capable of expanding the welding condition tolerance as compared with the conventional method.
(問題点を解決するための手段) そこでこの発明の抵抗スポット溶接方法は、ナゲット形
成開始前の初期に最大電流を供給し、ナゲット形成開始
時期に電流値を低下させ、その後、次第に電流値を増加
していくことを特徴としている。(Means for Solving Problems) Therefore, the resistance spot welding method of the present invention supplies the maximum current in the initial stage before the start of nugget formation, reduces the current value at the nugget formation start time, and then gradually increases the current value. It is characterized by increasing.
(作用) 上記抵抗スポット溶接方法によれば、第1図に破線で示
すように、従来(同図実線)よりもナゲット形成開始時
期を早めてナゲット成長の遅れを解消し、しかもナゲッ
ト径と接触径が接近し難くなり、これにより短時間通電
条件においても溶接条件裕度拡大の効果が得られる。(Operation) According to the resistance spot welding method described above, as shown by the broken line in FIG. 1, the nugget formation start time is earlier than in the conventional case (solid line in the figure) to eliminate the delay in nugget growth, and to make contact with the nugget diameter. It is difficult for the diameters to approach each other, and the effect of increasing the welding condition tolerance can be obtained even under a short-time energization condition.
(実施例) 次にこの発明の抵抗スポット溶接方法の具体的な実施例
について、図面を参照しつつ詳細に説明する。(Example) Next, a specific example of the resistance spot welding method of the present invention will be described in detail with reference to the drawings.
まず第2図にコンピュータ制御式のインバータ電源の構
成図を示す。同図において、1はコンピュータ、2はGT
O制御装置、3は電極、4は加圧シリンダ、5はシャン
トをそれぞれ示している。この場合、発振周波数は、60
0Hzと設定した。また検出した溶接電流とチップ間電圧
は、A/Dコンバータを介してパーソナルコンピュータに
取り込み、フロッピーディスクに記録している。First, FIG. 2 shows a configuration diagram of a computer-controlled inverter power supply. In the figure, 1 is a computer, 2 is a GT
O control device, 3 is an electrode, 4 is a pressurizing cylinder, and 5 is a shunt. In this case, the oscillation frequency is 60
I set it to 0Hz. The detected welding current and tip-to-tip voltage are taken into a personal computer via an A / D converter and recorded on a floppy disk.
溶接電流値は第3図(a)に示すように、溶接全期間中
での実効電流値とした。これは第3図(b)にみるよう
に溶接電流波形によらずにナゲット径と良好な関係が成
立したためである。The welding current value was the effective current value during the entire welding period, as shown in FIG. This is because as shown in FIG. 3 (b), a good relationship with the nugget diameter was established regardless of the welding current waveform.
電極には先端半径50mmのR形電極を採用した。これはCF
形のように電極形状に起因する最大接触径の制限を排除
するためである。An R-shaped electrode with a tip radius of 50 mm was adopted as the electrode. This is CF
This is to eliminate the limitation of the maximum contact diameter due to the shape of the electrode such as the shape.
溶接機の加圧部には直上加圧式のものを採用した。加圧
シリンダは空気式の低摩擦特性のものを採用し、上下の
電極の中心軸がずれないように、下部電極には芯合わせ
機構を組込んでいる。The pressurizing part of the welding machine is a direct pressurizing type. The pressure cylinder is a pneumatic one with low friction characteristics, and a centering mechanism is incorporated in the lower electrode so that the center axes of the upper and lower electrodes do not shift.
溶接条件は、以下のRWMAのAクラス推奨条件を基準と
し、また試験片には60×70mm大の軟鋼平板を採用した。Welding conditions were based on the following RWMA recommended Class A conditions, and a 60 × 70 mm large mild steel flat plate was used as the test piece.
板厚(mm) 溶接時間(ms) 加圧力(kN) 0.4 83 1.2 0.8 133 1.9 1.2 200 2.7 このインバータ電源で電流波形コンピュータ制御するた
めには、GTOの設定電圧を決定する入力信号波形を与え
る必要がある。そこでGTO制御回路を簡単な二次システ
ムであるLRC回路の入出力特性にモデル化し、第4図に
示す既知のLRC回路のステップ応答波形と比較して、GTO
制御回路の入出力特性を示す以下の式の微分方程式の係
数を決定した。Plate thickness (mm) Welding time (ms) Pressurizing force (kN) 0.4 83 1.2 0.8 133 1.9 1.2 200 2.7 In order to control the current waveform computer with this inverter power supply, it is necessary to give an input signal waveform that determines the set voltage of the GTO. There is. Therefore, the GTO control circuit was modeled as the input / output characteristics of the LRC circuit, which is a simple secondary system, and compared with the step response waveform of the known LRC circuit shown in Fig. 4, and the GTO
The coefficient of the differential equation of the following equation showing the input / output characteristics of the control circuit was determined.
但し、ωn:固有周波数 ξ:減衰係数 そしてその微分方程式を差分化して解いて、出力したい
電流波形から入力信号波形を決定する手法を用いた。 However, ω n : natural frequency ξ: damping coefficient and a method of determining the input signal waveform from the current waveform to be output by solving by differentializing the differential equation and using it.
なお電流波形は脈動成分の重畳した直流波形を、平均化
処理し、変化を見易くして観察している。The current waveform is observed by averaging the DC waveform on which the pulsating component is superimposed to make it easier to see the change.
各電流・電圧波形とナゲット形成過程の関係を第5図に
表す。ナゲット径とコロナボンド径はスポット溶接部を
ねじり破段させたのちルーペで測定した。同図(a)は
従来の定電流型、同図(b)は従来の定電力型、同図
(C)は今回導入した初期高電流型の例である。(a)
の定電流型においてはナゲット成長時期に入熱が高くな
っているため、ナゲット径が飽和する前にナゲット径と
コロナボンド径(接触径)との幅が狭くなる。また
(b)の定電力型では、後期の入熱が比較的高くなるた
め、ナゲットが主に中期以降行成長し、後期にナゲット
径とコロナボンド径の幅が狭くなってくる。一方、
(C)の初期高電流型では、後期までナゲットが成長し
ているものの、ナゲット径とコロナボンド径の接近程度
は小さく、しかもナゲット形成開始時期は早くなってい
る。ナゲット径とコロナバンド径が接近すると散りが発
生し易くなることから、(C)の初期高電流型において
はナゲット成長が遅れず、しかも散りが抑制されると予
想される。The relationship between each current / voltage waveform and the nugget formation process is shown in FIG. The nugget diameter and corona bond diameter were measured with a magnifying glass after twisting and breaking the spot weld. The figure (a) is a conventional constant current type, the figure (b) is a conventional constant power type, and the figure (C) is an example of the initial high current type introduced this time. (A)
In the constant current type, since the heat input is high during the nugget growth period, the width between the nugget diameter and the corona bond diameter (contact diameter) becomes narrow before the nugget diameter saturates. In the constant power type of (b), since the heat input in the latter period is relatively high, the nugget grows mainly in the middle period and thereafter, and the nugget diameter and the corona bond diameter become narrow in the latter period. on the other hand,
In the initial high-current type of (C), although the nugget grows until the latter half, the nugget diameter and the corona bond diameter are close to each other, and the nugget formation start time is early. When the diameter of the nugget and the diameter of the corona band are close to each other, scattering easily occurs. Therefore, in the initial high-current type (C), it is expected that the nugget growth will not be delayed and the scattering will be suppressed.
第6図に各電流波形における溶接条件裕度を表す。溶接
時間は電源特性の定電力化の効果が消える短時間通電条
件(RWMAのAクラス推奨通電時間条件)としている。各
電流波形の溶接条件裕度を比較すると明らかなように、
初期高電流型において散り発生電流値が最も高くなって
いる。これは先に述べたナゲット形成過程の違いによっ
て説明・理解できる。またこのことは短時通電条件にお
ける初期高電流波形の溶接条件裕度拡大の効果を示して
いる。なお溶接部の品質保証の目安とされる4√h(h:
板厚)のナゲット径が得られる電流値は、どの電流波形
においてもそれほど差が認められない。これは先の第3
図(b)で示したように、電流波形に関わらずナゲット
径が溶接全期間での実効電流値で整理できるからであ
る。FIG. 6 shows the welding condition tolerance in each current waveform. The welding time is the short-time energization condition (RWMA A-class recommended energization time condition) where the effect of constant power supply characteristics disappears. As is clear by comparing the welding condition tolerance of each current waveform,
In the initial high current type, the scattered current value is the highest. This can be explained and understood by the difference in the nugget formation process described above. This also shows the effect of expanding the welding condition margin of the initial high current waveform under the short-time energization condition. 4√h (h:
The current value at which the nugget diameter (plate thickness) is obtained does not differ so much in any current waveform. This is the third
This is because the nugget diameter can be arranged by the effective current value during the entire welding period regardless of the current waveform, as shown in FIG.
このような特性は他の板厚材に対しても同様に確認され
る。Such characteristics are similarly confirmed for other thick plates.
次に初期高電流型を中心に電流波形とナゲット形成特性
との関係を検討した。初期高電流波形における中期以降
の電流波形を変えた場合のナゲット形成過程の変化をみ
た結果を第7図に示す。同図(a)は中期以降一定電流
の場合、同図(b)は途中まで電流を上げ後一定とした
場合、同図(C)は中期以降の電流を溶接終了時まで徐
々に上げていった場合をそれぞれ表している。これらを
比較すると、同図(C)のように電流を徐々に上げてい
った場合、ナゲットが後期まで成長している。したがっ
て大寸法のナゲットを形成しようとした場合、中期以降
の電流を徐々に上げていくのが好ましいといえる。Next, the relationship between the current waveform and the nugget formation characteristics was examined centering on the initial high current type. FIG. 7 shows the results of observing changes in the nugget formation process when the current waveform after the middle period in the initial high current waveform was changed. The figure (a) shows the case where the current is constant after the middle period, the figure (b) shows the case where the current is raised to a certain point and then becomes constant, and the figure (C) shows that the current after the middle period is gradually increased until the end of welding. It shows each case. Comparing these, when the current is gradually increased as shown in FIG. 7C, the nugget grows to the latter stage. Therefore, when trying to form a large-sized nugget, it can be said that it is preferable to gradually increase the current after the middle period.
次に第8図に各初期高電流波形とナゲット形成過程の関
係を示す。先の第7図の結果から、中期以降の電流を徐
々に上げていく波形をそれぞれ採用している。Next, FIG. 8 shows the relationship between each initial high current waveform and the nugget formation process. From the results shown in FIG. 7, the waveforms that gradually increase the current after the middle period are adopted.
まず第8図(a)(b)(c)の電流波形とナゲット形
成過程を、電流を下げる時期に注目して比較する。同図
(a)の電流波形においては初期の高電流期間が長いた
め、ナゲット形成開始時期にも電流値が高くなってい
る。そのためナゲットが初期に急速に成長してナゲット
径とコロナボンド径(接触径)が接近する。同図(b)
の電流波形においては、ほぼナゲット形成開始時期まで
が初期の高電流期間となっており、ナゲット形成開始時
期付近では電流が緩やかに下がっている。この場合のナ
ゲット形成過程は、ナゲット径とコロナボンド径が接近
しておらず、いわゆる溶接条件裕度が拡大するうえで適
正なパターンとなっている。それに対し、同図(C)の
電流波形においては、ナゲット形成開始時期以前に、既
に電流値が最も低い状態となっているため、初期にはナ
ゲットがあまり成長せず、中期になって急速に成長し、
ナゲット径とコロナボンド径が接近している。このこと
から適正な初期の高電流期間はぼナゲット形成開始時期
までであり、それより長くとても短くナゲット径とコロ
ナボンド形が接近する時期が存在するといえる。First, the current waveforms of FIGS. 8A, 8B, and 8C and the nugget formation process will be compared, focusing on the time when the current is reduced. In the current waveform of FIG. 10A, the initial high current period is long, so the current value is high even at the nugget formation start time. Therefore, the nugget grows rapidly in the initial stage, and the nugget diameter and the corona bond diameter (contact diameter) approach each other. The same figure (b)
In the current waveform, the initial high current period is almost up to the nugget formation start time, and the current gradually decreases near the nugget formation start time. In the nugget forming process in this case, the nugget diameter and the corona bond diameter are not close to each other, and the pattern is appropriate for expanding the so-called welding condition tolerance. On the other hand, in the current waveform of FIG. 6C, the current value is already in the lowest state before the nugget formation start time, so that the nugget does not grow much in the initial stage and rapidly grows in the middle period. Grow up,
The nugget diameter is close to the corona bond diameter. From this, it can be said that the proper initial high current period is until the time when the nugget formation is started, and there is a time when the nugget diameter and the corona bond shape are longer and much shorter than that.
次に電流を上げる時期を変化させた場合をみる。第9図
(a)は先の第8図(c)を再び示したものである。第
9図(b)は同図(a)の電流波形のように初期の高電
流期間を短くし、その分電流を早く上げていったもので
ある。同図(b)の場合は同図(a)の場合よりもナゲ
ット径とコロナボンド径の接近程度は小さくなってはい
るものの、中期の接近は解消されておらず、適正なナゲ
ット形成過程定とはいい難い。このことから初期のナゲ
ット成長を早めるために、電流を徐々に上げる時期を早
くすることは、中期におけるナゲット径とコロナボンド
径の接近をまねきやすくなるため適正ではないといえ
る。Next, let us consider the case where the timing of raising the current is changed. FIG. 9 (a) shows the above-mentioned FIG. 8 (c) again. As shown in the current waveform of FIG. 9A, FIG. 9B shows that the initial high current period is shortened and the current is increased faster by that amount. Although the nugget diameter and the corona bond diameter are closer to each other in the case of FIG. 11B than in the case of FIG. 9A, the approach in the middle period has not been resolved, and an appropriate nugget formation process is determined. Is hard to say. From this, it can be said that it is not appropriate to increase the time of gradually increasing the current in order to accelerate the initial nugget growth because it tends to cause the nugget diameter and the corona bond diameter to approach each other in the middle period.
第10図に各電流波形と溶接条件裕度の関係を表す。まず
同図(a)に第7図で示した各電流波形における溶接条
件裕度を示す。それから明らかなように、第7図(c)
のように中期以降に徐々に電流を上げていく波形におい
て、散り限界電流値が最も高くなっている。このことは
中期以降の電流を徐々に上げていくこと、比較的散りを
発生させずに大寸法のナゲットを得られ易くなることを
示唆している。次に同図(b)に第8図(a)(b)及
び第9図(b)で示した電流波形における溶接条件裕度
を示す。第8図(a)は初期に、第9図(b)は中期以
降にナゲット径とコロナボンド径が接近する場合を代表
している。この図から明らかなように、初期高電流波形
により溶接条件裕度を拡大しようとした場合、初期の高
電流期間(電流を下げる時期)と中期以降の電流の上げ
方に特に注意して、ナゲット径とコロナボンド径が接近
しないナゲット形成過程となるようにしなければならな
いといえる。Figure 10 shows the relationship between each current waveform and the welding condition tolerance. First, FIG. 7A shows the welding condition tolerance in each current waveform shown in FIG. As is clear from that, FIG. 7 (c)
In the waveform in which the current is gradually increased from the middle period onward, the dispersion limit current value is the highest. This suggests that the electric current is gradually increased after the middle period, and that a large-sized nugget can be easily obtained without relatively causing scattering. Next, FIG. 8B shows welding condition tolerances in the current waveforms shown in FIGS. 8A and 8B and FIG. 9B. FIG. 8 (a) represents the initial case, and FIG. 9 (b) represents the case where the nugget diameter and the corona bond diameter are close to each other after the middle period. As is clear from this figure, when trying to expand the welding condition tolerance by the initial high current waveform, pay particular attention to the initial high current period (time to decrease the current) and the current increase after the middle period It can be said that the nugget formation process should be such that the diameter and the corona bond diameter do not approach each other.
(発明の効果) 以上のようにこの発明の抵抗スポット溶接方法では、ナ
ゲット形成開始前の初期に最大電流を供給し、ナゲット
形成開始時期の電流値を下げ、その後、中期以降に電流
値を上げていくようにしてあるが、このような制御を行
うことにより、比較的散りを発生させずに大寸法のナゲ
ットを得られ易くなる。(Effects of the Invention) As described above, in the resistance spot welding method of the present invention, the maximum current is supplied in the initial stage before the nugget formation is started, the current value at the nugget formation start time is decreased, and then the current value is increased after the middle period. However, by carrying out such control, it becomes easy to obtain a large-sized nugget without causing scattering relatively.
第1図は通電時間とナゲット径、接触径との関係を模式
的に示すグラフ、第2図は本発明方法を実施する溶接装
置の概略構成を示す模式図、第3図(a)は電流波形を
示す波形図、第3図(b)は実効電流とナゲット径との
関係を示すグラフ、第4図はLRC回路のステップ応答波
形を示すグラフ、第5図(a)(b)(c)は溶接時間
とナゲット径、コロナボンド径との関係を、溶接電流及
び溶接電圧波形と対応して示すグラフ、第6図は各電流
波形と溶接条件裕度との関係を対応して示すグラフ、第
7図(a)(b)(c)は溶接時間とナゲット径、コロ
ナボンド径との関係を、溶接電流及び溶接電圧波形と対
応して示すグラフ、第8図(a)(b)(c)及び第9
図(a)(b)は溶接時間とナゲット径、コロナボンド
径との関係を、溶接電流及び溶接電圧波形と対応して示
すグラフ、第10図(a)(b)は各電流波形と溶接条件
裕度との関係を対応して示すグラフである。FIG. 1 is a graph schematically showing the relationship between energization time, nugget diameter, and contact diameter, FIG. 2 is a schematic diagram showing a schematic configuration of a welding apparatus for carrying out the method of the present invention, and FIG. FIG. 3 (b) is a graph showing the waveform, FIG. 3 (b) is a graph showing the relationship between the effective current and the nugget diameter, FIG. 4 is a graph showing the step response waveform of the LRC circuit, and FIG. 5 (a) (b) (c). ) Is a graph showing the relationship between the welding time, the nugget diameter, and the corona bond diameter in correspondence with the welding current and the welding voltage waveform, and FIG. 6 is a graph showing the relationship between each current waveform and the welding condition margin. 7 (a), (b) and (c) are graphs showing the relationship between welding time and nugget diameter, corona bond diameter in correspondence with welding current and welding voltage waveforms, and FIGS. 8 (a) and (b). (C) and 9th
Figures (a) and (b) are graphs showing the relationship between welding time, nugget diameter, and corona bond diameter in correspondence with welding current and welding voltage waveforms, and Figs. 10 (a) and (b) are current waveforms and welding. It is a graph which shows a relationship with conditional margin correspondingly.
Claims (1)
給し、ナゲット形成開始時期に電流値を低下させ、その
後、次第に電流値を増加していくことを特徴とする抵抗
スポット溶接方法。1. A resistance spot welding method characterized in that a maximum current is supplied in the initial stage before the start of nugget formation, the current value is lowered at the start of nugget formation, and thereafter the current value is gradually increased.
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP2303726A JPH0790384B2 (en) | 1990-11-08 | 1990-11-08 | Resistance spot welding method |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP2303726A JPH0790384B2 (en) | 1990-11-08 | 1990-11-08 | Resistance spot welding method |
Publications (2)
| Publication Number | Publication Date |
|---|---|
| JPH04178274A JPH04178274A (en) | 1992-06-25 |
| JPH0790384B2 true JPH0790384B2 (en) | 1995-10-04 |
Family
ID=17924529
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP2303726A Expired - Lifetime JPH0790384B2 (en) | 1990-11-08 | 1990-11-08 | Resistance spot welding method |
Country Status (1)
| Country | Link |
|---|---|
| JP (1) | JPH0790384B2 (en) |
Cited By (1)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| JP2009039758A (en) * | 2007-08-09 | 2009-02-26 | Kanto Auto Works Ltd | Nugget diameter measuring instrument for resistance spot welding |
Families Citing this family (2)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| JP6963282B2 (en) * | 2018-04-20 | 2021-11-05 | 株式会社神戸製鋼所 | Aluminum material resistance spot welding joints and aluminum material resistance spot welding method |
| JP7240672B2 (en) | 2019-10-18 | 2023-03-16 | 株式会社神戸製鋼所 | Aluminum material resistance spot welding method, aluminum material resistance spot welding controller, and resistance spot welding machine |
Family Cites Families (2)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| JPS6254584A (en) * | 1985-08-31 | 1987-03-10 | Toyota Motor Corp | Control method for resistance spot welder |
| JPS63180384A (en) * | 1987-01-22 | 1988-07-25 | Dengensha Mfg Co Ltd | Chip-to-chip power control type resistance welding control system |
-
1990
- 1990-11-08 JP JP2303726A patent/JPH0790384B2/en not_active Expired - Lifetime
Cited By (1)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| JP2009039758A (en) * | 2007-08-09 | 2009-02-26 | Kanto Auto Works Ltd | Nugget diameter measuring instrument for resistance spot welding |
Also Published As
| Publication number | Publication date |
|---|---|
| JPH04178274A (en) | 1992-06-25 |
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