JPS587393B2 - Resistance welding method for steel plates - Google Patents
Resistance welding method for steel platesInfo
- Publication number
- JPS587393B2 JPS587393B2 JP54114833A JP11483379A JPS587393B2 JP S587393 B2 JPS587393 B2 JP S587393B2 JP 54114833 A JP54114833 A JP 54114833A JP 11483379 A JP11483379 A JP 11483379A JP S587393 B2 JPS587393 B2 JP S587393B2
- Authority
- JP
- Japan
- Prior art keywords
- welding
- nugget
- current
- thickness
- steel plates
- Prior art date
- Legal status (The legal status is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the status listed.)
- Expired
Links
- 238000003466 welding Methods 0.000 title claims description 104
- 229910000831 Steel Inorganic materials 0.000 title claims description 35
- 239000010959 steel Substances 0.000 title claims description 35
- 238000000034 method Methods 0.000 title claims description 27
- 230000004927 fusion Effects 0.000 claims description 19
- 238000003825 pressing Methods 0.000 claims description 7
- 238000010586 diagram Methods 0.000 description 8
- 230000020169 heat generation Effects 0.000 description 6
- 238000010438 heat treatment Methods 0.000 description 6
- 230000010349 pulsation Effects 0.000 description 5
- 239000000463 material Substances 0.000 description 3
- 230000033458 reproduction Effects 0.000 description 3
- 230000015572 biosynthetic process Effects 0.000 description 2
- 238000002844 melting Methods 0.000 description 2
- 230000008018 melting Effects 0.000 description 2
- 206010067482 No adverse event Diseases 0.000 description 1
- 230000002411 adverse Effects 0.000 description 1
- 238000013459 approach Methods 0.000 description 1
- 230000000052 comparative effect Effects 0.000 description 1
- 238000007796 conventional method Methods 0.000 description 1
- 238000005520 cutting process Methods 0.000 description 1
- 230000000694 effects Effects 0.000 description 1
- 238000007373 indentation Methods 0.000 description 1
- 230000002250 progressing effect Effects 0.000 description 1
- 238000007711 solidification Methods 0.000 description 1
- 230000008023 solidification Effects 0.000 description 1
- 230000003068 static effect Effects 0.000 description 1
- 230000001629 suppression Effects 0.000 description 1
- 239000002699 waste material Substances 0.000 description 1
Landscapes
- Resistance Welding (AREA)
Description
【発明の詳細な説明】
本発明は、鋼板の重ね合わせ部を電極により加圧挾持し
つつ電流を流し、ジュール熱によるナゲット(融接部)
を形成して鋼板を溶接する抵抗点溶接に8いて、ナゲッ
トか板厚力向に必袈以上に成長することを抑制し、必要
な強度をもつ溶接部を比較的少ない入熱で形成されるこ
とを目的とする鋼板の抵抗溶接力法であって、ナゲット
の径に対する厚さの比が0.25を超えやすい板厚1,
2ミリメートル以上の鋼板の抵抗溶接に好適な方法であ
る。Detailed Description of the Invention The present invention produces a nugget (fusion weld) by applying Joule heat to the overlapping portion of steel plates while applying pressure and clamping them with electrodes.
In resistance spot welding, which forms and welds steel plates, it is possible to suppress the nugget from growing more than necessary in the direction of the plate thickness, and to form a welded part with the necessary strength with relatively little heat input. This is a resistance welding force method for steel plates with the purpose of
This method is suitable for resistance welding of steel plates of 2 mm or more.
抵抗点溶接の接着メカニズムは、いうまでもなく抵抗発
熱(ジュール熱)による融接である。Needless to say, the bonding mechanism of resistance spot welding is fusion welding using resistance heat generation (Joule heat).
この発熱は電極の先端形状、加圧力、溶接電流、通電時
間等の溶接条件に大きく左右される。This heat generation is greatly influenced by welding conditions such as the shape of the electrode tip, pressing force, welding current, and energization time.
このため合理的な溶接条件として日本工業規格(JIS
)、米国抵抗溶接機製造者協会(RWMA)あるいは米
国溶接協会(AWS)などの推奨条件が示されている。Therefore, as a rational welding condition, the Japanese Industrial Standards (JIS)
), the Resistance Welding Machine Manufacturers Association (RWMA), or the American Welding Society (AWS).
これらの推奨条件で溶接する場合、生成するナゲットは
一般にいわゆる基石状の形態となる。When welding under these recommended conditions, the resulting nugget generally has a so-called foundation stone-like form.
ナゲットは直径方向に成長するとともに板厚方向にも十
分成長する。The nugget grows in the diameter direction and also grows sufficiently in the thickness direction.
第1図にはこれらの推奨条件で作られるナゲットの厚さ
のナゲット径に対する比と板厚との関係を示した。Figure 1 shows the relationship between the ratio of the thickness of the nugget to the nugget diameter and the plate thickness produced under these recommended conditions.
点溶接すべき板厚が薄い(1ミリメートル前後)場合に
は上記の比は比較的小さいが、板厚の増加とともにこの
比は大きな値を示すようになる。When the plate thickness to be spot welded is thin (about 1 mm), the above ratio is relatively small, but as the plate thickness increases, this ratio becomes large.
一力、点溶接部の強度は、その一例を第2図に示すよう
に、ナゲットの直径の大小と非常によい相関がある。The strength of a spot weld has a very good correlation with the diameter of the nugget, as shown in FIG.
このときのナゲット厚さはいずれも1.6ミリメートル
前後であり、ナゲット厚さは静的強度とは直接結びつか
ない。The nugget thickness at this time was approximately 1.6 mm in each case, and the nugget thickness was not directly related to static strength.
むしろナゲット厚さが必要以上に大きくなることは融接
部周辺の熱影響部を過大に拡げることとなり、疲労強度
上好ましいことではない。On the contrary, if the nugget thickness becomes larger than necessary, the heat-affected zone around the fusion weld will expand excessively, which is not preferable in terms of fatigue strength.
そこでナゲット厚さのナゲット径に対する比に注目する
ことが必要となってくる。Therefore, it is necessary to pay attention to the ratio of the nugget thickness to the nugget diameter.
本発明者らの研究によると、板厚が比較的薄い厚さ1ミ
リメートル以下の鋼板の点溶接に8いては、溶接開始直
後に必要ナゲット径に見合う通電通路が形成され、その
後ナゲットは主に板厚力向に成長するのに対し、鋼板の
厚さが1ミリメートルを超えさらに大きくなると、溶接
開始直後には所要ナゲット径に比し面積の挾い融接域即
ち通電通路が形成されるのみであり、以後の通電により
ナゲットは厚さを増しながら直径力向にも成長するので
、所要のナゲット径に達する際にはナゲット厚さもかな
りの厚さに成長する。According to the research conducted by the present inventors, when spot welding steel plates with a relatively thin thickness of 1 mm or less, a current-carrying path corresponding to the required nugget diameter is formed immediately after welding starts, and after that, the nugget mainly In contrast, when the thickness of a steel plate exceeds 1 mm and increases further, a fusion weld region, that is, a current-carrying path, whose area is smaller than the required nugget diameter is formed immediately after welding starts. As a result of subsequent energization, the nugget increases in thickness and also grows in the diametrical direction, so that when the required nugget diameter is reached, the nugget thickness also grows to a considerable thickness.
本発明者らはこれらの実験研究から、薄板と厚板とでナ
ゲット生成過程に大きな違いが生ずる理由として、薄板
の点溶接に8いては板厚が薄いことによって電極により
重ねた鋼板を加圧挾着した際に電極面積に対する鋼板ど
うしの接触面積の比が大きく、従って溶接開始直後から
所要ナゲット径に近い通電通路が得られ、ナゲット厚さ
は通電時間によって調整をすることが可能であるが、溶
接すべき板が厚くなると、電極による加圧挾持に際して
薄板に比して剛性が高く可撓性に欠けるため電極面積に
対する鋼板どうしの接触面積の比が小さく、従って溶接
開始時に鋼板どうしの接触部を通じて通電して融接域を
拡大してゆくので、溶接開始直後は所要ナゲット径に比
して小さい面積の通電通路しか得られず、しかも熱の放
散の良好な薄板に比して厚さが厚くなるに従って融接部
の熱の外気への放散が悪くなるので、溶接開始直後の通
電通路となる融接域から厚さ力向と電極の直径力向とに
融接域を拡げる結果、所要のナゲット径を得ようとすれ
は?のすと板厚力向にも十分に成長したナゲットとなっ
てしまうという知見を得た。From these experimental studies, the present inventors found that the reason why there is a large difference in the nugget formation process between thin plates and thick plates is that in spot welding of thin plates8, due to the thinness of the plates, pressure is applied to the stacked steel plates using an electrode. When clamped, the ratio of the contact area between the steel plates to the electrode area is large, so a current-carrying path close to the required nugget diameter can be obtained immediately after welding starts, and the nugget thickness can be adjusted by adjusting the current-carrying time. When the plates to be welded become thicker, they are more rigid and less flexible than thin plates when clamped under pressure by electrodes, so the ratio of the contact area between the steel plates to the electrode area is small, and therefore the steel plates do not come into contact with each other at the start of welding. Since the fusion welding area is expanded by passing current through the nugget, immediately after welding starts, only a current-carrying path with a small area compared to the required nugget diameter is obtained. As the fusion weld becomes thicker, the dissipation of heat from the fusion weld to the outside air becomes worse.As a result, the fusion weld area is expanded from the fusion weld area, which becomes the current-carrying path immediately after welding starts, to the thickness force direction and the diameter force direction of the electrode. How to get the required nugget diameter? We obtained the knowledge that if the plate is stretched, it will become a nugget that has grown sufficiently in the direction of the plate thickness and force.
そして前記実験研究の成果からナゲット厚さのナゲット
径に対する比が0.25を超えないように溶接条件を制
御すれば、点溶接部の融着部周辺の熱影響が強度に悪影
響を及ぼさないことを見出すとともに、前記した点溶接
の推奨条件等によるときは、第1図に示すように、鋼板
の板厚が1.1ミリメートル以下に8いてはナゲット厚
さのナゲット径に対する比が0.25を超えないが、板
厚が1. 2ミリメートルを超えると当該比が0,25
を超えてしまうことを見出した。The results of the above experimental research indicate that if the welding conditions are controlled so that the ratio of the nugget thickness to the nugget diameter does not exceed 0.25, the thermal effect around the fused part of the spot weld will not adversely affect the strength. In addition, when following the recommended spot welding conditions mentioned above, as shown in Figure 1, when the thickness of the steel plate is 1.1 mm or less, the ratio of the nugget thickness to the nugget diameter is 0.25. However, the plate thickness does not exceed 1. If it exceeds 2 mm, the ratio is 0.25
I found that it exceeds the
そこで本発明者らは、板厚が1.2ミリメートルを超え
る鋼板を点溶接で溶接するにあたり、溶接開始当初には
、鋼板の材質で定まるジュール熱による融接を生ずる電
流の大きさ、通常の点抵抗溶接に郭ける主溶接電流の大
きさの40%ないし70%の大きさの電流を、通電によ
る発熱量と逸散される発熱量とが平衡状態に達するまで
通電することにより、電極加圧力のもとて所要ナゲット
径に見合う面積の通電通路即ち前記電流値に見合った融
接部を確保する通電を行い、しかるのち主溶接電流を通
じて主として前記融接部の厚さ方向への拡大を行わせる
技術を開発した。Therefore, when welding steel plates with a thickness exceeding 1.2 mm by spot welding, the present inventors determined that at the beginning of welding, the magnitude of the current that causes fusion welding due to Joule heat, which is determined by the material of the steel plates, and the normal Electrode heating is achieved by applying a current that is 40% to 70% of the main welding current used in spot resistance welding until the amount of heat generated by energization and the amount of heat dissipated reach an equilibrium state. Under pressure, current is applied to ensure a current-carrying path with an area corresponding to the required nugget diameter, that is, a fusion weld corresponding to the current value, and then the main welding current mainly causes the fusion weld to expand in the thickness direction. We have developed the technology to do this.
即ち、本発明によるときは、溶接初期に主溶接電流の4
0%ないし70%の大きさの電流を通電するときは、電
極によ仝挾着面積の範囲内で鋼板の接触部から融接が開
始されるが、通電電流の大きさが小さいため、接触面の
軟化が優先し、次第に通電通路を拡大して融接域の面積
を拡大し、溶融域の厚みを増す前に所要のナゲット径に
見合う通電通路を形成することを見出したのである。That is, according to the present invention, the main welding current is 4
When applying a current with a magnitude of 0% to 70%, fusion welding starts from the contact area of the steel plate within the area clamped by the electrodes, but since the magnitude of the applied current is small, the contact They found that the softening of the surface takes priority, and the area of the fusion weld zone is expanded by gradually enlarging the current conduction path to form a current conduction path that matches the required nugget diameter before increasing the thickness of the fusion zone.
そしてこの通電が開始されてから時間が経過するにつれ
、通電電流の大きさに見合って通電通路の拡がりが止ま
り平衡に達する状態がみらわるが、通電通路確保のため
の上記初期通電の時間はこの最小値が好ましい。As time passes after this energization is started, the energization path stops expanding in proportion to the magnitude of the energizing current and reaches a state of equilibrium, but the initial energization time described above to secure the energization path is This minimum value is preferred.
勿論上記平衡に達してから前記初期通電を継続しても悪
い影響は発生しないが、エネルギーと時間の無駄となる
。Of course, if the initial energization is continued after the equilibrium is reached, no adverse effects will occur, but it will be a waste of energy and time.
上記した平衡状態に達したとき、鋼板の融接域は未だそ
の面積の拡張が行われ厚さ力向にその大きさを増す傾向
は極めて僅かであるから、融着域は厚さ方向の断面で極
めて偏平であることが観察される。When the above-mentioned equilibrium state is reached, the area of the fusion welded area of the steel plate is still expanding, and the tendency to increase in size in the thickness direction is extremely small. It is observed that it is extremely flat.
そこで次に前記の主溶接電流を電極に加えると、以後は
融着域の厚さの拡大と集中抵抗による径の拡大が行われ
るので、適切な厚さに成長したとき溶接を終了せしめる
。Then, when the main welding current is applied to the electrode, the thickness of the fused area and the diameter are expanded by the concentrated resistance, so welding is terminated when the welding area has grown to an appropriate thickness.
本発明により得られるナゲットの厚さ力向断面形状はほ
ぼ一様の厚さを示し、通電時間によってナゲット厚さを
制御することが可能であることを示している。The cross-sectional shape of the nugget obtained according to the present invention in the force direction shows a substantially uniform thickness, indicating that the nugget thickness can be controlled by changing the current application time.
以下、各種の溶接条件と対比して本発明を説明する。The present invention will be explained below in comparison with various welding conditions.
先ず、通常用いられる点溶接電極を用い、各種推奨条件
等のなかから次の溶接条件を選び厚さ3ミリメートル前
後の鋼板試片を二枚重ねて同一の抑圧条件の下に溶接し
てそのナゲットの成長過程を試片を切断して観察した。First, using a commonly used spot welding electrode, select the following welding conditions from among various recommended conditions, stack two steel plate specimens approximately 3 mm thick, and weld them under the same suppression conditions to measure the growth of the nugget. The process was observed by cutting specimens.
第3図はその溶接条件の通電電流と通電時間との関係を
線図であらわしたもので、主溶接電流の大きさは各溶接
条件とも同じである。FIG. 3 is a diagram showing the relationship between the applied current and the applied time under the welding conditions, and the magnitude of the main welding current is the same for each welding condition.
第3図Iは推奨条件等にみられる最も一般的な溶接法で
、溶接電流の大きさは通電時間中一定である。FIG. 3 I shows the most common welding method found in the recommended conditions, and the magnitude of the welding current is constant during the energization time.
この溶接法で作られるナゲットは、第4図に示すごとく
、通電初期(第4図a)は鋼板間の電極加圧範囲の中心
部の接触点から発熱が進み、その後ナゲットは通電通路
の直径力向への拡張が進まずに通電中期(第4図b)か
ら通電終期(第4図c)にかけて板厚力向へ大きく成長
し、通電時間とともに直径が所要の寸法に近づくと厚さ
も極めて厚く成長する。As shown in Fig. 4, the nugget made by this welding method generates heat from the contact point at the center of the electrode pressurizing range between the steel plates at the initial stage of energization (Fig. 4a), and then the nugget is The plate thickness grows significantly in the force direction from the middle stage of energization (Fig. 4 b) to the final stage of energization (Fig. 4 c) without progressing in the force direction, and as the diameter approaches the required dimension as the energization time increases, the thickness becomes extremely large. Grow thick.
このため鋼板の発熱による軟化も厚さ力向全域に及び溶
接終了時(第4図d)には電極の押圧力の影響をも受け
て電極による圧痕も大きい。For this reason, the steel plate is softened due to heat generation throughout the thickness and force direction, and at the end of welding (Fig. 4 d), it is also affected by the pressing force of the electrode, and the indentation caused by the electrode is large.
即ち、この溶接法では数箇所の発熱起点を中心に板厚お
よび直径力向へ成長し、ほぼ板厚に近い厚さのナゲット
を形成する。That is, in this welding method, the welding grows in the direction of the plate thickness and diameter around several heat generation starting points, forming a nugget with a thickness approximately close to the plate thickness.
第3図■は、溶接初期Fこ直線的に通電電流の大きさを
溶接電流の大きさまで傾斜的に増大させ、しかる後一定
電流の通電を行う溶接法である。Fig. 3 (3) shows a welding method in which the magnitude of the applied current is linearly increased in a gradient manner to the magnitude of the welding current at the initial stage of welding F, and then a constant current is applied.
溶接初期の傾斜的増大の時間は全通電時間の10%前後
が普通である。The time for the gradual increase in the initial stage of welding is usually about 10% of the total current application time.
傾斜的増大の目的は散りの防止にあり、ナゲットの形成
過程は第4図と大差がない。The purpose of the gradual increase is to prevent scattering, and the nugget formation process is not much different from that shown in FIG.
第3図■は溶接電流の通電と休止を繰返して行ういわゆ
るパルセーション溶接法を示す。FIG. 3 (■) shows a so-called pulsation welding method in which welding current is repeatedly turned on and off.
この方式の場合は第5図に示すように、各パルス毎に溶
融凝固が繰返され、各パルス毎にナゲットの生成が認め
られる。In this method, as shown in FIG. 5, melting and solidification are repeated for each pulse, and nuggets are observed for each pulse.
即ち第5図aは第1パルス投入の初期に生成されたナゲ
ットであって、第3図Iの溶接力法の初期と同様に数箇
所の鋼板接触点から発熱が進む結果第4図aとほぼ同様
のナゲットを形成している。That is, Fig. 5a shows the nugget generated at the beginning of the first pulse application, and as in the initial stage of the welding force method shown in Fig. 3I, heat generation progresses from several steel plate contact points, resulting in the nugget shown in Fig. 4a. They form almost similar nuggets.
そして第1パルスの通電の終期には第5図bに示すナゲ
ットが形成される。At the end of the first pulse energization, a nugget shown in FIG. 5b is formed.
しかも第1のパルスでは最終的に必要なナゲット径に見
合う通電通路の確保が十分でなく厚さ方向により早く成
長した傾向が見られる。Moreover, in the first pulse, there was a tendency for the nugget to grow faster in the thickness direction because it was not sufficient to secure a current-carrying path that matched the ultimately required nugget diameter.
第2のパルス通電に2いては第1のパルス通電で形成さ
れたナゲットを通電通路として発熱が進む傾向がみられ
、そのため第5図Cに示すように、第1のパルス通電に
おけるような板厚方向への成長は少く、直径力向への成
長が多く見られる。During the second pulse energization, there is a tendency for heat generation to proceed as the nugget formed during the first pulse energization acts as a energization path, and as a result, as shown in Figure 5C, the plate There is little growth in the thickness direction, and more growth in the diameter direction.
このような繰返しで最終的には第5図dに示すようにパ
ルス数だけのナゲットの重なり合った溶融凝固ゾーンが
形成され、結果的には直径力向へも板厚力向へも十分に
成長したナゲットが形成される。By repeating this process, a melt-solidified zone with overlapping nuggets corresponding to the number of pulses is finally formed as shown in Figure 5d, and as a result, the nuggets grow sufficiently in both the diameter force direction and the plate thickness force direction. nuggets are formed.
以上の事実から、溶接すべき鋼板が1ミリメートル以下
のように比較的薄い場合には、第6図に示すように上下
の電極P,Qにより加圧通電を行うとき、溶接開始直後
に所要ナゲット径に見合う通電通路か形成され、その後
ナゲットは主に板厚力向へ成長するのに対し、溶接すべ
き鋼板が厚い場合には従来の推奨条件の何れの溶接法に
よっても、第7図に示すように溶接開始直後に形成され
る通電通路は所要ナゲット径に比して拡がりが少く、以
後はナゲットは厚さを増しながら直径力向にも成長する
ことがわかる。From the above facts, when the steel plate to be welded is relatively thin, such as 1 mm or less, when applying pressure and current using the upper and lower electrodes P and Q as shown in Fig. 6, the required nugget can be obtained immediately after welding starts. A current-carrying path corresponding to the diameter is formed, and then the nugget grows mainly in the direction of plate thickness force. However, if the steel plate to be welded is thick, no matter which welding method under the conventional recommended conditions is used, the nugget will grow as shown in Figure 7. As shown, it can be seen that the current-carrying path formed immediately after the start of welding expands less than the required nugget diameter, and thereafter the nugget grows in the diametrical direction while increasing its thickness.
従って板厚が1.2ミリメートルを超える鋼板の抵抗点
溶接において、溶接開始直後に先ず第6図に見られるよ
うな所要ナゲット径に見合う、板厚力向には薄い通電通
路を形成することに成功すれば、板厚の大きな鋼板の抵
抗点溶接に8いてナゲット厚さを通電時間によって調整
することも可能となり、ナゲット厚さのナゲット径に対
する比を0.25以下にすることもできる。Therefore, in resistance spot welding of steel plates with a thickness exceeding 1.2 mm, it is necessary to first form a thin current-carrying path in the force direction of the plate thickness, commensurate with the required nugget diameter as shown in Figure 6, immediately after welding starts. If successful, it will be possible to adjust the nugget thickness by adjusting the current application time during resistance spot welding of thick steel plates, and the ratio of the nugget thickness to the nugget diameter can be made 0.25 or less.
本発明は溶接開始直後の所要ナゲット径に見合う通電通
路の形成を、主溶接電流の40%ないし70%の大きさ
の電流を通電することによって成功したものであって、
前記推奨条件と対比するために第3図と同様の溶接電流
の大きさと通電時間との関係をあらわす線図を第8図に
示す。The present invention succeeds in forming a current-carrying path corresponding to the required nugget diameter immediately after the start of welding by applying a current of 40% to 70% of the main welding current,
For comparison with the recommended conditions, FIG. 8 shows a diagram showing the relationship between the magnitude of the welding current and the current application time, similar to that shown in FIG. 3.
本発明においては溶接電流を二段階に制御し、溶接初期
の第一段階においては所定の電極加圧力の下で所要のナ
ゲット径に見合う通電通路を確保するため、該鋼板がジ
ュール熱による融接を生ずる溶接電流(これを主溶接電
流という)の40%ないし70%の大きさの電流を、接
合部における発熱量と逸散する熱量とが平衡し、通電通
路の拡がりがほぼ完了するような熱的平衡状態に達する
まで流し、次いで第二段階として前記主溶接電流を投入
するものである。In the present invention, the welding current is controlled in two stages, and in the first stage at the initial stage of welding, the steel plate is fusion welded by Joule heat in order to secure a current-carrying path suitable for the required nugget diameter under a predetermined electrode pressure. A current that is 40% to 70% of the welding current that produces the The welding current is allowed to flow until a thermal equilibrium state is reached, and then the main welding current is applied as a second step.
前記第一段階における電流値は鋼板のナゲット生成部表
面の軟化による拡がりのある面積での密着を目的とする
から、溶接しようとする箇所の温度が融点を超える必要
はないので、主溶接電流の70%以上の大きさを必要と
せず、また所定の加圧力で鋼板間の十分な軟化接触状態
を得るには最小限主溶接電流の40係の大きさが必要で
ある。The current value in the first stage is aimed at achieving close contact over a spread area due to the softening of the surface of the nugget forming part of the steel plate, so there is no need for the temperature of the part to be welded to exceed the melting point, so the main welding current is It is not necessary to have a magnitude of 70% or more, and a minimum magnitude of 40 times the main welding current is required in order to obtain a sufficiently softened contact state between the steel plates with a predetermined pressing force.
本発明の溶接力法によるときは、ナゲットの成長は第9
図に示すごとく、第一段階の通電を終了し第二段階の主
溶接電流の通電初期には第9図aを示すように極めて拡
がりがあって厚さがほぼ均一の薄い融接域が出現し、主
溶接電流の通電中期(第9図b)から終期にかけて通電
通路の厚さ力向へ主に成長し、集中抵抗による直径力向
への成長も伴って、通電終了時(第9図d)には所要の
ナケット径で厚さのほぼ均一なナゲットを得るのである
。When using the welding force method of the present invention, the nugget growth is
As shown in the figure, at the end of the first stage of energization and at the beginning of the second stage of applying the main welding current, a thin fusion weld area with an extremely wide spread and almost uniform thickness appears as shown in Figure 9a. However, the main welding current mainly grows in the thickness force direction of the energizing path from the middle of the energization period (Fig. 9b) to the final energization period, and also grows in the diameter force direction due to concentrated resistance, and at the end of energization (Fig. 9 In d), a nugget with a required nucket diameter and approximately uniform thickness is obtained.
第9図から本発明によるときは、第二段階の主溶接電流
の通電後期に8ける通電時間の制御によりナゲットの厚
みを調整し得ることは明らかである。From FIG. 9, it is clear that according to the present invention, the thickness of the nugget can be adjusted by controlling the current application time in the latter half of the second stage main welding current application.
以下本発明の実施例を説明する。Examples of the present invention will be described below.
本発明を自動車用ディスクホイルのディスクおよびリム
の抵抗点溶接に応用した。The present invention was applied to resistance spot welding of discs and rims of automobile disc wheels.
ディスクは板厚3.2ミリメートルのSHP材、リムは
板厚3.5ミリメートルのSHP材の組合せである。The disc is made of SHP material with a thickness of 3.2 mm, and the rim is made of SHP material with a thickness of 3.5 mm.
溶接に使用した電極の寸法は上部電極が直径25ミリメ
ートル、加圧面の球面の曲率が半径180ミリメートル
、下部電極は直径25ミリメートル、球面曲率の半径が
100ミリメートルで、電極加圧力は1.7トンである
。The dimensions of the electrodes used for welding were: the upper electrode had a diameter of 25 mm, the spherical curvature of the pressurizing surface had a radius of 180 mm, the lower electrode had a diameter of 25 mm, and the radius of spherical curvature was 100 mm, and the electrode pressing force was 1.7 tons. It is.
通電時間は溶接装置に接続する商業電源のサイクル数に
よってこれを定めた。The energization time was determined by the number of cycles of the commercial power source connected to the welding equipment.
第10図は実施例に使用した単相交流溶接装置の回路図
であって、溶接回路■は、加熱用及び溶接用の電流を供
給する電源回路■と、これと溶接部■との間を適宜開閉
制御する開閉電流制御回路■とからなる。Figure 10 is a circuit diagram of the single-phase AC welding device used in the example, in which the welding circuit (■) connects the power supply circuit (■) that supplies current for heating and welding, and the welding part (■). It consists of an opening/closing current control circuit (2) that controls opening/closing as appropriate.
すなわち、この制御回路■は溶接部材■を軟化すべく加
熱用制御信号と溶接すべき溶接用制御信号とを順次発す
るものである。That is, this control circuit (2) sequentially issues a heating control signal to soften the welding member (2) and a welding control signal to weld it.
そして、この回路■は、ボリューム等で溶接電流値を設
定する電流設定器1と、適用周波数に合せて電流設定器
1の抵抗値に見合った進角を決める位相制御回路2と、
この回路2で決められた進角(時間)の時差でサイリス
タ6のゲートへ加熱用または溶接用の制御信号を送るた
めの信号発生を行うサイリスク点弧回路3と、上述のよ
うに制御された適用周波数の溶接電流を所定の時間流す
かを決める通電時間設定回路4とが2系列より成る回路
及びサイリスタ5とを備えている。This circuit (2) includes a current setter 1 that sets the welding current value using a volume or the like, a phase control circuit 2 that determines an advance angle commensurate with the resistance value of the current setter 1 in accordance with the applied frequency,
A thyrisk ignition circuit 3 generates a signal to send a control signal for heating or welding to the gate of the thyristor 6 at a time difference of advance angle (time) determined by this circuit 2, and The welding current setting circuit 4 includes a thyristor 5 and a circuit consisting of two series of an energization time setting circuit 4 that determines whether or not a welding current of an applicable frequency is applied for a predetermined period of time.
上記溶接装置を用い、第一段階の通電電流を25キロア
ンペア、通電時間を商業電源の50サイクル、第二段階
の通電電流を32キロアンペア、通電時間を商業電源の
30サイクルないし45サイクルに設定して本発明を実
施した。Using the above welding equipment, the first stage current is set to 25 kiloamperes, the energization time is set to 50 cycles of the commercial power supply, the second stage energization current is set to 32 kiloamperes, and the energization time is set to 30 to 45 cycles of the commercial power supply. The present invention was carried out in this manner.
この実施例に3いては第二段階の通電初期に所望ナゲッ
ト径の18ミリメートルにほぼ近い通電通路が得られて
おり、すべての溶接部分で偏平な所望のナゲットを得ら
れた。In this Example 3, an energization path approximately close to the desired nugget diameter of 18 mm was obtained at the beginning of the second stage of energization, and the desired flat nugget was obtained at all welded portions.
これらのナゲット中第二段階の通電時間を45サイクル
として実施したものの断面を第11図に模写した。The cross section of these nuggets in which the second stage of energization time was set to 45 cycles is reproduced in FIG.
なお参考として第一段階の通電時間を接合部における通
電通路が生成途上の状態の30サイクルの通電に止めた
場合には、第一段階で鋼板間の接触部分が十分に軟化せ
ず、目標とするナゲット径は得られないばかりか、ナゲ
ットの厚さが厚いものとなった。For reference, if the energization time in the first stage is stopped at 30 cycles during which the energization path in the joint is in the process of being formed, the contact area between the steel plates will not soften sufficiently in the first stage, and the target will not be met. Not only was it not possible to obtain the desired nugget diameter, but the nugget became thick.
その一例の断面を第12図に模写で示す。A cross-section of one example is shown as a reproduction in FIG.
また比較のため推奨条件等によるパルセーション溶接を
試みた。For comparison, we also attempted pulsation welding under recommended conditions.
この溶接法は溶接電流を32キロアンペア、通電時間を
商業電源の36サイクルを1パルスとし、商業電源の1
2サイクルの休止時間をはさんで3パルス投入した。In this welding method, the welding current is 32 kiloamperes, the energization time is 36 cycles of the commercial power source as one pulse, and the welding current is 32 kiloamperes.
Three pulses were applied with two cycles of rest time in between.
この結果は第13図に溶接部断面の模写の一例を示すよ
うに、ナゲットが3回にわたり形成されていること、お
よび1回目、2回目のパルスで板厚方向にはそのほぼ全
域まで成長していることがわかる。This result shows that the nugget was formed three times, as shown in Figure 13, which shows an example of a cross-sectional copy of the weld, and that the nugget grew to almost the entire area in the thickness direction during the first and second pulses. It can be seen that
第14図は本発明の実施例(黒丸で示す)および比較の
ために行った第一段階の通電時間を短縮した実施例(白
丸で示す)ならびにパルセーション溶接法(三角で示す
)による人熱量( KA xsec:と形成したナゲッ
ト径との関係を示す図である。Figure 14 shows an example of the present invention (indicated by a black circle), an example in which the energization time in the first stage was shortened for comparison (indicated by a white circle), and the amount of human heat produced by the pulsation welding method (indicated by a triangle). (KA xsec: is a diagram showing the relationship between the formed nugget diameter.
図からわかるように本発明方法によると、従来のパルセ
ーション溶接法に比して約2/3の人熱量で同等あるい
はそれ以上の直径をもつナゲットが得られ、しかもナゲ
ットの偏平度は従来法よりはるかに良好であった。As can be seen from the figure, according to the method of the present invention, a nugget with a diameter equal to or larger than that of the conventional pulsation welding method can be obtained with about 2/3 the amount of human heat, and the flatness of the nugget is lower than that of the conventional pulsation welding method. It was much better.
以上要するに本発明によれば、鋼板の接合個所を第一段
階の通電加熱により軟化させ、所要の電極加圧力の下で
所要のナゲット径に見合う通電通路を確保し、然る後に
主溶接電流を投入する第二段階の通電加熱を行うので、
従来法の如く通電通路が十分に確保されない状態で大電
流を継続して投入することにより起る板厚方向へのナゲ
ットの成長あるいは散りを防止でき、所要ナゲット径に
見合う通電通路を確保した後のナゲットの成長は主に板
厚力向に行われるので通電時間の調整でナゲットの厚さ
を調整することができ、消費電力が少く、あわせて電極
への熱負荷も軽くなるため、電極の寿命向上をも達成す
ることができる有用な方法である。In summary, according to the present invention, the joint parts of the steel plates are softened by the first stage of electrical heating, a current-carrying path corresponding to the required nugget diameter is secured under the required electrode pressure, and then the main welding current is applied. Since the second stage of energization heating is performed,
It is possible to prevent the growth or scattering of nuggets in the plate thickness direction, which occurs when a large current is continuously applied without a sufficient current-carrying path as in the conventional method, and after securing a current-carrying path that matches the required nugget diameter. Since nugget growth occurs mainly in the direction of plate thickness force, the thickness of the nugget can be adjusted by adjusting the current application time, which reduces power consumption and also reduces the heat load on the electrode. This is a useful method that can also improve lifespan.
第1図は点溶接部に2ける鋼板の板厚と生成したナゲッ
ト厚のナゲット径との比との関係を示す線図、第2図は
点溶接部に8けるナゲット径とナゲットのせん断強度の
関係を示す線図、第3図は各種の推奨条件等による溶接
力法の通電電流と通電時間の関係を示す線図、第4図お
よび第5図は第3図の溶接力法によって形成されるナゲ
ットを示す断面図、第6図郭よび第7図は鋼板の溶接部
に2けるナゲットの成長を示す模式図、第8図は本発明
による通電電流と通電時間との関係を示す線図、第9図
は本発明により形成されるナゲットを示す断面図、第1
0図は本発明の実施に使用した溶接装置の回路図、第1
1図は本発明の実施によって得られたナゲットの断面を
模写した図、第12図2よび第13図は比較例のナゲッ
トの断面を模写した図、第14図はナゲット径と人熱量
の関係を示す線図である。
なお図中、P,EよびQは電極、1は電流設定器、2は
位相制御向路、3はサイリスク点弧回路、4は通電時間
設定回路、5はサイリスクを夫々示すものである。Figure 1 is a diagram showing the relationship between the thickness of the steel plate at the spot weld and the ratio of the nugget thickness to the nugget diameter, and Figure 2 is the nugget diameter at the spot weld and the shear strength of the nugget. Figure 3 is a diagram showing the relationship between energizing current and energizing time using the welding force method based on various recommended conditions, etc. Figures 4 and 5 are created using the welding force method shown in Figure 3. 6 and 7 are schematic diagrams showing the growth of a nugget in a welded part of a steel plate, and FIG. 8 is a line showing the relationship between the applied current and the applied time according to the present invention. FIG. 9 is a sectional view showing a nugget formed according to the present invention, and FIG.
Figure 0 is a circuit diagram of the welding device used to carry out the present invention.
Figure 1 is a reproduction of the cross section of a nugget obtained by implementing the present invention, Figures 12 and 13 are reproductions of the cross section of a nugget of a comparative example, and Figure 14 is the relationship between nugget diameter and human heat amount. FIG. In the figure, P, E and Q are electrodes, 1 is a current setting device, 2 is a phase control direction, 3 is a cyrisk ignition circuit, 4 is an energization time setting circuit, and 5 is a cyrisk, respectively.
Claims (1)
、 板厚が1. 2 ミリメートルを超える鋼板の重ね合せ
部を電極で加圧挾着せしめつつ該鋼板がジュール熱によ
り融接を生ずる大きさの溶接電流の40%ないし70%
の大きさの電流を、該重ね合せ部の接合面に該電流値に
見合った融接部を形成させかつ当該融接部の拡がりがほ
ぼ飽和に達するまで通電し、 しかる後前記電極による加圧挾着を維持しつつ、前記溶
接電流を通電せしめて最終的な溶接状態を形成すること
を特徴とする鋼板の抵抗溶接力法。[Claims] 1. In the resistance welding force method for steel plates using Joule heat, when the plate thickness is 1. 40% to 70% of the welding current of a magnitude that causes fusion welding of the steel plates by Joule heat while pressing the overlapped portion of steel plates exceeding 2 mm with electrodes.
A current with a magnitude of A resistance welding force method for steel plates, characterized in that the welding current is applied while maintaining clamping to form a final welded state.
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP54114833A JPS587393B2 (en) | 1979-09-07 | 1979-09-07 | Resistance welding method for steel plates |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP54114833A JPS587393B2 (en) | 1979-09-07 | 1979-09-07 | Resistance welding method for steel plates |
Publications (2)
| Publication Number | Publication Date |
|---|---|
| JPS5639179A JPS5639179A (en) | 1981-04-14 |
| JPS587393B2 true JPS587393B2 (en) | 1983-02-09 |
Family
ID=14647827
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP54114833A Expired JPS587393B2 (en) | 1979-09-07 | 1979-09-07 | Resistance welding method for steel plates |
Country Status (1)
| Country | Link |
|---|---|
| JP (1) | JPS587393B2 (en) |
Families Citing this family (2)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| JP6852035B2 (en) | 2018-10-16 | 2021-03-31 | 株式会社豊田中央研究所 | Spot welding method |
| JP6852036B2 (en) | 2018-10-16 | 2021-03-31 | 株式会社豊田中央研究所 | Electrode insert for resistance spot welding |
-
1979
- 1979-09-07 JP JP54114833A patent/JPS587393B2/en not_active Expired
Also Published As
| Publication number | Publication date |
|---|---|
| JPS5639179A (en) | 1981-04-14 |
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