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JPS6213115B2 - - Google Patents
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JPS6213115B2 - - Google Patents

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Publication number
JPS6213115B2
JPS6213115B2 JP18068080A JP18068080A JPS6213115B2 JP S6213115 B2 JPS6213115 B2 JP S6213115B2 JP 18068080 A JP18068080 A JP 18068080A JP 18068080 A JP18068080 A JP 18068080A JP S6213115 B2 JPS6213115 B2 JP S6213115B2
Authority
JP
Japan
Prior art keywords
welding
circuit
cycle
function
integral value
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
Application number
JP18068080A
Other languages
Japanese (ja)
Other versions
JPS57103788A (en
Inventor
Seiji Takagi
Masaru Tanaka
Current Assignee (The listed assignees may be inaccurate. Google has not performed a legal analysis and makes no representation or warranty as to the accuracy of the list.)
Panasonic Holdings Corp
Original Assignee
Matsushita Electric Industrial Co Ltd
Priority date (The priority date 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 date listed.)
Filing date
Publication date
Application filed by Matsushita Electric Industrial Co Ltd filed Critical Matsushita Electric Industrial Co Ltd
Priority to JP55180680A priority Critical patent/JPS57103788A/en
Publication of JPS57103788A publication Critical patent/JPS57103788A/en
Publication of JPS6213115B2 publication Critical patent/JPS6213115B2/ja
Granted legal-status Critical Current

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Description

【発明の詳細な説明】 本発明は、抵抗溶接機の出力制御方法ならびに
装置に関し、溶接中に溶接品質を把握し適正な品
質になるように制御せんとするものである。
DETAILED DESCRIPTION OF THE INVENTION The present invention relates to a method and apparatus for controlling the output of a resistance welding machine, and is intended to grasp the welding quality during welding and to control the welding quality so that the quality is appropriate.

従来、抵抗溶接時の溶接品質(引張剪断応力、
ナゲツト外観等)を溶接進行中に把握し、適正溶
接品質にすべく制御することは非常に困難であ
り、溶接後の溶接品質テストで把握されていたに
過ぎなかつた。
Conventionally, welding quality during resistance welding (tensile shear stress,
It is extremely difficult to grasp the appearance of nuggets, etc. during welding and to control the welding quality to achieve appropriate welding quality, and this has only been known through welding quality tests after welding.

すなわち、抵抗溶接(特にスポツト溶接)の溶
接品質の適正値は、予め予備実験を行い三大溶接
条件である溶接電流、全通電サイクル、加圧力の
適正値を決定することにより求められていた。
That is, the appropriate values for the welding quality of resistance welding (particularly spot welding) have been determined by conducting preliminary experiments in advance and determining the appropriate values for the three major welding conditions: welding current, total energization cycle, and pressurizing force.

また最近では、これら三大条件の内、溶接電流
の実効値、実際の通電サイクルを溶接中に測定す
ることにより、予め設定した値とのそれぞれの偏
差を求め間接的な溶接品質の判定を行つていた。
しかし、溶接品質と一義的関係にある成分因子を
検出し、溶接中に適正化制御を行わないためチツ
プの消耗等に対してはその都度三大条件の補正等
をしなければならなかつた。また突発的な前記条
件の変化があつた時は、再度溶接を行う必要があ
つた。
Recently, among these three major conditions, by measuring the effective value of welding current and the actual energization cycle during welding, the deviation from each value from the preset value is found and indirect judgment of welding quality has been made. It was on.
However, since component factors that have a primary relationship with welding quality are detected and optimization control is not performed during welding, it is necessary to correct the three major conditions each time for chip wear and the like. Furthermore, when there was a sudden change in the conditions, it was necessary to perform welding again.

本発明は、このような従来からの問題点を克服
すべく、溶接中に適正化制御し、溶接品質の均質
化を図ろうとするものである。
In order to overcome these conventional problems, the present invention attempts to perform appropriate control during welding and to homogenize welding quality.

まず、本発明の原理について説明する。 First, the principle of the present invention will be explained.

最初、模範溶接(標準溶接)を行い、この時の
溶接電流(実際に流れた電流)とチツプ間電圧
(チツプ間電圧の第1積分値、もしくはチツプ間
電圧の第2積分値)を記憶し、この時の各通電サ
イクル毎の入熱を計算し、この入熱になるように
2回目以降は、制御整流素子の点弧角を制御し、
溶接材への入熱制御を行う。すなわち、実験的に
入熱を模範溶接通りとすれば、強度一定(不変)
の溶接が可能との結論を得ている。
First, perform model welding (standard welding), and memorize the welding current (current that actually flowed) and chip-to-chip voltage (first integral value of chip-to-chip voltage or second integral value of chip-to-chip voltage). , calculate the heat input for each energization cycle at this time, and control the firing angle of the control rectifier from the second time onward to achieve this heat input,
Controls heat input to welding material. In other words, if the experimental heat input is as per the model welding, the strength will be constant (unchanged)
It has been concluded that welding is possible.

なお、本明細書中の第1関数は上記原理に基づ
き、以例定数K1を求める(第1関数K1=Ie×Vt
でIeとVtは模範溶接で既知であり、K1が求ま
る)。次に第2関数の比例定数K2を模範溶接によ
り求める。
Note that the first function in this specification is based on the above principle, and the following constant K 1 is calculated (first function K 1 =I e ×V t
( Ie and Vt are known from the model welding, and K1 can be found). Next, the proportionality constant K 2 of the second function is determined by model welding.

すなわち、第2関数 よりIeは既知、θは模範溶接時のθであり、K2
は求まる。
That is, the second function Therefore, Ie is known, θ is θ at the time of model welding, and K 2
is found.

以上により第1関数、第2関数は決定され、2
回目以降の溶接では、入熱一定の溶接を行う。
The first function and second function are determined by the above, and 2
For subsequent welding, welding with constant heat input is performed.

以下本発明の一実施例を第1図に示す。図にお
いて、1は双方向性三端子制御整流素子等の制御
整流素子、2は溶接トランス、3,3′は電極チ
ツプ、4,4′はチツプ間電圧検出線であり、チ
ツプ3,3′上のP1,P2点にそれぞれ一端が接続
されている。5は溶接施工材、6は第1積分回路
であり、入力側は検出線4,4′に接続されてお
り、この回路6により1サイクルから予め設定し
た任意設定通電サイクルまでのサイクル毎のチツ
プ間電圧を半サイクル間積分する。この1サイク
ル毎の積分値を第1積分値と呼ぶ。次にこの第1
積分値を次段の第2積分回路7に入力し、第1積
分値を1サイクルから任意設定通電サイクルまで
積分、すなわち第1積分値の全体を積分し、この
値を第2積分値と呼ぶ。次にこの第2積分値を次
段に設置した第1関数回路8に入力し、この回路
8は第2積分値(この値をVtと置く)と所望溶
接実効電流値(この値をIeと置く)との関係で
示された第1関数式を演算し、所望溶接実効電流
値を出力する回路構成になつており、この回路8
により前記所望溶接実効電流値Ieを求める。今
仮にIe=K1=Vtなる第1関数式を導入したとす
れば、その第1関数定数はK1である。また第1
積分回路6の次段に第1関数回路8を設置し、第
2積分回路7を削除してもかまわない。この時、
第1関数回路8は第1積分回路6の第1積分値群
の中でも特に任意設定通電サイクル時のみの第1
積分値(特にVoと呼ぶ)を受信し、第1関数式
により所望溶接実効電流値Ieを演算し、第1関
数回路8の出力端より溶接実効電流値Ieを出力
する。この時の第1関数式は、Ie=K1/Voであ
る。さらに第1関数回路8の次段に第2関数回路
9を設置し、その入力端に前記溶接実効電流値I
eを入力する。第2関数回路9は前記溶接実効電
流値Ieと前記制御整流素子1の点弧角信号との
関係式(第2関数式と呼ぶ)で表わされた演算回
路で構成されており、今もし、第2関数回路9に
溶接実効電流値Ieを入力すれば、第2関数回路
9の出力端より所望点弧角信号が発生する。今も
し、所望点弧角をθとし、溶接電流の瞬時値(i
と呼ぶ)を示せば、i=K2 sinθで示され、この
時の実効電流値Ieは次の第2関数式で表わされ
る。すなわち、 である。K2を第2関数定数と呼ぶ。すなわち、
第2関数回路9の出力端より所望点弧角θを表わ
す制御信号(この信号をV〓と呼ぶ)が発生す
る。さらに第2関数回路9の次段に点弧回路10
を設置し、点弧回路10は前記制御信号V〓なる
信号を受信し、制御整流素子1を駆動するに十分
なる信号に変換する。今、本溶接開始前に設定さ
れた制御整流素子1の点弧角をθとすれば、本
制御回路構成を駆動させることにより所望点弧角
θに変換される。そして残りの全通電サイクルは
θで持続される。ところで、前記任意設定通電サ
イクルを表示する信号は計数回路11による出力
で示される。すなわち、計数回路11は溶接電流
を電流検出装置(カーレント・トランスフオーマ
またはシヤント)12により検出し、この検出電
流により通電サイクル数を計数し、予め設定され
た前記任意通電サイクルになればそのサイクルを
示す信号を計数回路11より発生させる。その信
号出力を回路6,7,8,9に入力させ、その入
力により回路6,7,8,9は前記所望の働きを
する。なお、必ずしも回路11の出力を回路6,
7,8,9のすべてに入力する必要はなく、回路
7,8のみに入力してもかまわない。以上の回路
構成の各部波形を示せば、第2図,第3図のよう
になる。第2図イは時間tに対する溶接電流波形
iを示した図、同ロは検出端点P1,P2におけるチ
ツプ間電圧波形vを示した図、同ハは第1積分回
路6により積分した各通電サイクル毎の正の半サ
イクル間の積分値Vを示した図である。なお、負
の半サイクル間の積分でもかまわない。例えば
V1,V2,V3がその積分値である。今第1積分回
路6では正の半サイクル毎の積分値V1,V2,V3
……を第1積分値としている。また各サイクルの
最初の積分値は零にリセツトされている。ところ
で、t1,t2……t10は時間を示し、それぞれの波形
位置の対応をt1,t2,……t10で示す。チツプ間電
圧eは、溶接電流をi、直流抵抗分をR、インダ
クタンス分をLで示せば、e=iR+Ldi/dtで示さ れ、第1積分回路6で各サイクル毎のチツプ間電
圧を決まつた方向の半サイクル間積分すれば、V
=∫edt=∫i・Rdtとなり、これは溶接部の発
熱に比例した真の値となる。すなわち、第1積分
回路6の第1積分値はV1,V2……を示す。これ
らのV1,V2,……を抽出して、通電サイクルと
ともに表わし、その包絡線を示せば第3図とな
る。なお、第3図のα波形の全通電サイクルは10
サイクルであり、V1……V10まで示されている。
また同様にして求めたβ波形は5サイクル目で第
1積分値(これをV5′とする)が大きく低下して
いる。これは溶接中にチリが発生したためと思わ
れる。ところで今、5サイクル目を任意設定通電
サイクルとすれば、その時のα波形の値V5が前
記で示したVnとなる。β波形のV5′をVoとして
抽出すれば、これは真に発熱と比例した値となら
ず、後に示すように制御回路上考慮する必要があ
る。なお、第2積分値VtはVt=V1+V2+V3+V4
+V5である。
An embodiment of the present invention is shown in FIG. 1 below. In the figure, 1 is a control rectifier such as a bidirectional three-terminal control rectifier, 2 is a welding transformer, 3 and 3' are electrode chips, 4 and 4' are inter-chip voltage detection lines; One end is connected to the P 1 and P 2 points above. Reference numeral 5 indicates the welding work material, and 6 indicates a first integration circuit, the input side of which is connected to the detection lines 4 and 4'.This circuit 6 detects the chips for each cycle from the 1st cycle to the arbitrarily set energization cycle set in advance. Integrate the voltage across half a cycle. This integral value for each cycle is called a first integral value. Then this first
The integral value is input to the second integral circuit 7 in the next stage, and the first integral value is integrated from the first cycle to the arbitrarily set energization cycle, that is, the entire first integral value is integrated, and this value is called the second integral value. . Next, this second integral value is input to the first function circuit 8 installed at the next stage, and this circuit 8 inputs the second integral value (this value is set as V t ) and the desired welding effective current value (this value is set as I The circuit has a circuit configuration that calculates the first functional expression shown in the relationship between
The desired welding effective current value I e is determined by: If we now introduce a first functional expression I e = K 1 = V t , the first functional constant is K 1 . Also the first
The first function circuit 8 may be installed at the next stage of the integration circuit 6, and the second integration circuit 7 may be deleted. At this time,
The first function circuit 8 is the first integrated value group of the first integral value group of the first integral circuit 6.
The integrated value (particularly referred to as V o ) is received, a desired welding effective current value I e is calculated using the first functional equation, and the welding effective current value I e is outputted from the output end of the first functional circuit 8 . The first functional expression at this time is I e =K 1 /V o . Further, a second function circuit 9 is installed next to the first function circuit 8, and the welding effective current value I is connected to the input terminal of the second function circuit 9.
Enter e . The second function circuit 9 is composed of an arithmetic circuit expressed by a relational expression (referred to as a second function expression) between the welding effective current value I e and the firing angle signal of the control rectifying element 1. If the effective welding current value Ie is input to the second function circuit 9, a desired firing angle signal is generated from the output terminal of the second function circuit 9. Now, if the desired firing angle is θ, and the instantaneous value of welding current (i
), it is expressed as i=K 2 sin θ, and the effective current value I e at this time is expressed by the following second functional expression. That is, It is. K 2 is called the second function constant. That is,
A control signal representing the desired firing angle θ (this signal is referred to as V〓) is generated from the output terminal of the second function circuit 9. Further, an ignition circuit 10 is provided at the next stage of the second function circuit 9.
The ignition circuit 10 receives the control signal V and converts it into a signal sufficient to drive the control rectifier 1. Now, if the firing angle of the control rectifying element 1 set before the start of the main welding is θ 0 , it is converted to the desired firing angle θ by driving the main control circuit configuration. The entire remaining energization cycle is then sustained at θ. Incidentally, the signal indicating the arbitrarily set energization cycle is indicated by the output from the counting circuit 11. That is, the counting circuit 11 detects the welding current with a current detection device (current transformer or shunt) 12, counts the number of energization cycles based on the detected current, and when the preset arbitrary energization cycle is reached, the cycle is stopped. The counter circuit 11 generates a signal shown in FIG. The signal output is inputted to the circuits 6, 7, 8, and 9, and the circuits 6, 7, 8, and 9 perform the desired function based on the input. Note that the output of the circuit 11 is not necessarily the output of the circuit 6,
It is not necessary to input to all circuits 7, 8, and 9, and it is possible to input only to circuits 7 and 8. The waveforms of each part of the above circuit configuration are shown in FIGS. 2 and 3. Figure 2A shows the welding current waveform i with respect to time t, Figure 2B shows the inter-chip voltage waveform v at the detection end points P 1 and P 2 , and Figure 2C shows each voltage waveform integrated by the first integrating circuit 6. FIG. 3 is a diagram showing an integral value V during a positive half cycle for each energization cycle. Note that integration between negative half cycles may also be used. for example
V 1 , V 2 , and V 3 are the integral values. Now, in the first integration circuit 6, the integral values V 1 , V 2 , V 3 for each positive half cycle
... is taken as the first integral value. Also, the first integral value of each cycle is reset to zero. Incidentally, t 1 , t 2 . . . t 10 indicate time, and the correspondence between the respective waveform positions is indicated by t 1 , t 2 , . . . t 10 . The chip-to-chip voltage e is expressed as e=iR+Ldi/dt, where i is the welding current, R is the DC resistance, and L is the inductance.The first integrating circuit 6 determines the chip-to-chip voltage for each cycle. If we integrate for half a cycle in the direction, we get V
=∫edt=∫i・Rdt, which is a true value proportional to the heat generation of the welding part. That is, the first integral values of the first integrating circuit 6 indicate V 1 , V 2 . . . . If these V1 , V2 , . The total energization cycle of the α waveform in Figure 3 is 10.
The cycle is shown from V 1 to V 10 .
Further, in the β waveform obtained in the same manner, the first integral value (this is referred to as V 5 ') decreases significantly at the fifth cycle. This is probably due to dust generated during welding. Now, if the fifth cycle is the arbitrarily set energization cycle, the value V5 of the α waveform at that time becomes the Vn shown above. If V 5 ' of the β waveform is extracted as Vo , this value will not be truly proportional to the heat generation, and must be taken into consideration in the control circuit as will be shown later. Note that the second integral value V t is V t =V 1 +V 2 +V 3 +V 4
+ V5 .

次に本発明の制御方法について説明する。 Next, the control method of the present invention will be explained.

まず、第1行程として、標準溶接を行い、標準
溶接のチツプ間電圧を求める。例えば第3図のα
波形がこれに相当する。
First, as a first step, standard welding is performed and the inter-chip voltage of standard welding is determined. For example, α in Figure 3
The waveform corresponds to this.

ここで求めた値を第1積分値または第2積分値
とする。これらの値をVNとする。
The value obtained here is defined as the first integral value or the second integral value. Let these values be VN .

第2行程として、前記標準溶接時の実効電流I
eを求め、かつ、その時の点弧角をθとする。そ
して、Ieを一時記憶しておく。
As the second step, the effective current I during standard welding is
Find e and set the firing angle at that time to θ. Then, temporarily store I e .

第3行程として、前記VN,Ieより第1関数
K1,第2関数K2を求める。
As the third step, from the above V N and I e , the first function
Find K 1 and the second function K 2 .

第4行程として、任意溶接を行い、このチツプ
間電圧を求める。例えば、第3図のβ波形がこれ
に相当する。
In the fourth step, arbitrary welding is performed and the voltage between the chips is determined. For example, the β waveform in FIG. 3 corresponds to this.

かつ、上記任意溶接中にβ波形がα波形に漸近
するように、前記第1関数式,第2関数式を求
め、これらの関数よりθを求め、該点弧角θを各
サイクル毎に増減する。
In addition, the first and second functional expressions are determined so that the β waveform asymptotically approaches the α waveform during the arbitrary welding, θ is determined from these functions, and the firing angle θ is increased or decreased for each cycle. do.

ところで、予備実験で実効電流値Ieと第1関
数値Voを求める必要がある。そのため、Ieの検
出は、第1図の電流検出装置12で検出し、溶接
実効電流変換回路13で検出電流を実効電流に変
換し、その出力を回路8が受信することにより前
記目的を達成することが可能である。なお、回路
13により、電流波形の位相角θも演算され、出
力されるものとする。ただし、予備実験時に別の
装置によりIeが判明するときは、回路8にその
ことを予め別の方法で記憶させておけばよく特に
回路13が必ずしも必要であるということではな
い。
By the way, it is necessary to determine the effective current value I e and the first function value V o in a preliminary experiment. Therefore, Ie is detected by the current detection device 12 shown in FIG. 1, the detected current is converted into an effective current by the welding effective current conversion circuit 13, and the output is received by the circuit 8 to achieve the above purpose. It is possible to do so. It is assumed that the circuit 13 also calculates and outputs the phase angle θ of the current waveform. However, if Ie is determined by another device during a preliminary experiment, it may be sufficient to store this in advance in the circuit 8 using another method, and the circuit 13 is not necessarily required.

次に第4図、第5図は、第2関数回路9に内蔵
されている第2関数式の考え方の一例を示したも
のである。今、第4図のように電流波形をi=
K2sinθとし、通電角がθからπ、(π+θ)から
2πであると仮定する。
Next, FIGS. 4 and 5 show an example of the concept of the second function formula built in the second function circuit 9. Now, as shown in Figure 4, the current waveform is i=
Assume that K 2 sin θ and the conduction angle is π from θ and 2π from (π+θ).

その時の実効電流値は第7図のγ波形より求め
られる。すなわち、γ波形は、 である。
The effective current value at that time is determined from the γ waveform in FIG. In other words, the γ waveform is It is.

ところで、K2を求める方法は、実効電流値Ie
とθを検出して本溶接時に常にK2の補正をして
もよいが、予め予備実験でK2の値が判明してい
るなら回路13からの出力を受信する必要はな
い。また別の方法による、さらに別の第2関数を
求めてもかまわない。特にインダクタンス負荷の
時は考慮する必要がある。
By the way, the method for finding K 2 is to calculate the effective current value I e
Although it is possible to always correct K 2 during actual welding by detecting θ and θ, there is no need to receive the output from the circuit 13 if the value of K 2 is known in advance from a preliminary experiment. Furthermore, another second function may be obtained using another method. This must be taken into consideration especially when using an inductance load.

次に、もし第3図のβ波形のようにチリが発生
した時は、次のような操作を考えてもよい。その
回路例を第1図に付加して示す。14は異常検出
弁別回路、15はタイマー回路であり、回路6,
14,15,10の構成により次の操作が可能で
ある。まず回路6の出力を異常検出弁別回路14
で受信し、その回路14で第3図のα,β波形等
の包絡線を作成する。そして一時記憶する。さら
にβ波形のように任意設定通電サイクル内で
V5′のような異常電圧降下のある時は、異常電圧
降下有の弁別出力を発生させる(異常電圧降下な
しの時は弁別出力の発生はない)。そして、タイ
マー回路15を働かせ、点弧回路10を初期設定
電流に固定したままで、初期設定通電サイクルの
みの変更を行う。
Next, if dust occurs like the β waveform in FIG. 3, the following operation may be considered. An example of the circuit is shown in FIG. 14 is an abnormality detection discrimination circuit, 15 is a timer circuit, and circuits 6,
The configurations 14, 15, and 10 allow the following operations. First, the output of the circuit 6 is detected by the abnormality detection discrimination circuit 14.
The circuit 14 generates envelopes such as the α and β waveforms shown in FIG. and temporarily memorize it. Furthermore, as shown in the β waveform, within the arbitrarily set energization cycle,
When there is an abnormal voltage drop such as V 5 ', a discrimination output indicating that there is an abnormal voltage drop is generated (when there is no abnormal voltage drop, no discrimination output is generated). Then, the timer circuit 15 is activated to change only the initial setting energization cycle while keeping the ignition circuit 10 fixed at the initial setting current.

すなわち、タイマー回路15の出力が存在する
ときは、回路9の出力は遮断され、溶接電流を決
定する点弧角θは溶接前に決定されたθを回路1
5の出力で決まるタイマー時間持続する。
That is, when the output of the timer circuit 15 is present, the output of the circuit 9 is cut off, and the firing angle θ that determines the welding current is determined by changing θ determined before welding to the circuit 1.
It lasts for a timer period determined by the output of step 5.

このようにすれば、チリの発生に対しても誤動
作はしない。
In this way, malfunctions will not occur even when dust is generated.

なお、第1図において、実線で示したものが本
発明の基本回路であり、破線で示したものが補助
的な回路である。また任意設定通電サイクルは、
第3図からも分るように、予め、α,β波形の正
の微係数内、すなわち、3,4,5サイクル前後
に決定した方がよい。
In FIG. 1, what is shown by a solid line is the basic circuit of the present invention, and what is shown by a broken line is an auxiliary circuit. In addition, the optional setting energization cycle is
As can be seen from FIG. 3, it is better to decide in advance within the positive differential coefficients of the α and β waveforms, that is, around 3, 4, and 5 cycles.

以上のような本発明による出力制御方法ならび
に装置によれば、次のような効果がある。
According to the output control method and device according to the present invention as described above, the following effects can be achieved.

(1) 溶接中に溶接品質の一定化(均質化)制御が
できる。
(1) The welding quality can be controlled to be constant (homogenized) during welding.

(2) 第1関数式を採用しているため、所望溶接電
流の決定が簡易にできる。
(2) Since the first functional equation is adopted, the desired welding current can be easily determined.

(3) 従来方式のように、溶接後溶接品質のチエツ
クが不要であり、工場の省力、省人化に貢献で
きる。
(3) Unlike conventional methods, there is no need to check the welding quality after welding, contributing to labor and manpower savings in factories.

【図面の簡単な説明】[Brief explanation of the drawing]

第1図は本発明による抵抗溶接機の出力制御装
置の回路図、第2図イ,ロ,ハは抵抗溶接時の各
種波形を示した図、第3図は通電サイクルと第1
積分値との関係を示した図、第4図は溶接電流波
形を示した図、第5図は点弧角と溶接実効電流値
の関係を示した図である。 1…制御整流素子、2…溶接トランス、3,
3′…電極チツプ、4,4′…チツプ間電圧検出
線、5…溶接施工材(母材)、6…第1積分回
路、7…第2積分回路、8…第1関数回路、9…
第2関数回路、10…点弧回路、11…計数回
路、12…電流検出装置、13…溶接実効電流変
換回路、14…異常検出弁別回路、15…タイマ
ー回路。
Fig. 1 is a circuit diagram of the output control device of a resistance welding machine according to the present invention, Fig. 2 A, B, and C are diagrams showing various waveforms during resistance welding, and Fig. 3 shows the energization cycle and the first
FIG. 4 is a diagram showing the relationship with the integral value, FIG. 4 is a diagram showing the welding current waveform, and FIG. 5 is a diagram showing the relationship between the firing angle and the welding effective current value. 1... Control rectifying element, 2... Welding transformer, 3,
3'... Electrode chip, 4, 4'... Inter-chip voltage detection line, 5... Welding work material (base material), 6... First integral circuit, 7... Second integral circuit, 8... First function circuit, 9...
Second function circuit, 10... Ignition circuit, 11... Counting circuit, 12... Current detection device, 13... Welding effective current conversion circuit, 14... Abnormality detection discrimination circuit, 15... Timer circuit.

Claims (1)

【特許請求の範囲】 1 溶接出力を制御するための制御整流素子を内
蔵した抵抗溶接機の溶接時の電極チツプ間電圧を
検出し、全通電サイクル中の予め任意に設定した
任意設定通電サイクルまでの前記電極チツプ間電
圧の各サイクル毎の半サイクル間の積分値を求め
これらの値を第1積分値とし、もしくはさらにそ
の後前記各サイクル毎の第1積分値を第1のサイ
クルから前記任意設定通電サイクルまで累積した
値を第2積分値とし、かつ前記任意設定通電サイ
クルにおける前記各サイクル毎の第1積分値また
は全体的な第2積分値をその各積分値と所望溶接
実効電流値との関係で予め求められた第1関数式
に代入して所望溶接実効電流値を求め、かつ第1
関数式の第1関数定数は本溶接開始前の予備実験
により前記任意設定通電サイクル時の第1積分値
または第2積分値およびこれらに対応する溶接実
効電流値を測定し、第1関数式に代入することに
より予め求められており、さらに前記所望溶接実
効電流値を溶接実効電流値と前記制御整流素子の
所望点弧角との関係で予め求められた第2関数式
に代入して前記所望点弧角を求め、かつ第2関数
式の第2関数定数は予め前記予備実験で溶接実効
電流値とその導通角の関係を測定し、第2関数式
に代入して求めるかまたは本溶接中に前記操作を
行うことにより求められ、かつ本溶接開始前に設
定された前記点弧角を前記所望点弧角に変換する
ことにより抵抗溶接機の出力を制御することを特
徴とする抵抗溶接機の出力制御方法。 2 第1関数式が、任意設定通電サイクル時の第
1積分値をVo、電極チツプ間電圧の第2積分値
をVt、所望溶接実効電流値をIe、かつ第1関数
定数をK1とする時、Ie=K1/VoまたはIe
K1/Vtで表わされていることを特徴とする特許
請求の範囲第1項に記載の抵抗溶接機の出力制御
方法。 3 第2関数式が、溶接実効電流値をIe、制御
整流素子の点弧角をθ、第2関数定数をK2とす
る時、 で表わされていることを特徴とする特許請求の範
囲第1項に記載の抵抗溶接機の出力制御方法。 4 任意設定通電サイクルが、第1積分値の包絡
線上の正の微分係数内前後に予め設定されている
ことを特徴とする特許請求の範囲第1項に記載の
抵抗溶接機の出力制御方法。 5 溶接出力を制御するための制御整流素子を内
蔵した抵抗溶接機において、電極チツプ間電圧を
入力信号とし第1のサイクルから任意設定通電サ
イクルまでのサイクル毎の電極チツプ間電圧を半
サイクル間積分した第1積分値を出力する第1積
分回路と、その第1積分回路の出力側に直接また
は第1積分値を積分し第2積分値を出力する第2
積分回路を介して接続された前記任意設定通電サ
イクル時のみの第1積分値を選択的に受信するか
または第2積分値を受信し予め求められた第1関
数式に従つて演算し所望溶接実効電流値を出力す
る第1関数回路と、その第1関数回路の出力側に
接続された予め求められた第2関数式に従つて演
算し前記制御整流素子の所望点弧角信号を出力す
る第2関数回路と、その第2関数回路の出力側に
接続された前記制御整流素子の点弧角を前記所望
点弧角に変換する点弧回路とを備え、前記任意設
定通電サイクルを表示する信号は別に設置した計
数回路の出力側より次段に設置した前記第1積分
回路、第2積分回路、第1関数回路、第2関数回
路に入力され各々前記制御を行うことを特徴とす
る抵抗溶接機の出力制御装置。
[Claims] 1. Detects the voltage between electrode tips during welding of a resistance welding machine with a built-in control rectifying element for controlling welding output, and detects the voltage between the electrode tips during welding, up to an arbitrarily set energization cycle arbitrarily set in advance during the entire energization cycle. The integral value of the inter-electrode chip voltage during each half cycle for each cycle is determined and these values are used as the first integral value, or further, the first integral value for each cycle is determined from the first cycle to the arbitrary setting. The value accumulated up to the energization cycle is defined as the second integral value, and the first integral value for each cycle or the overall second integral value in the arbitrarily set energizing cycle is the sum of each integral value and the desired welding effective current value. The desired welding effective current value is determined by substituting it into the first functional formula determined in advance according to the relationship, and the first
The first function constant of the function formula is determined by measuring the first integral value or second integral value and the corresponding welding effective current value during the arbitrarily set energization cycle in a preliminary experiment before starting the actual welding, and then formulating the first function constant in the first function formula. The desired welding effective current value is further determined by substituting the desired welding effective current value into a second functional equation previously determined based on the relationship between the welding effective current value and the desired firing angle of the control rectifying element. The firing angle is determined, and the second function constant of the second function formula can be determined by measuring the relationship between the welding effective current value and its conduction angle in advance in the preliminary experiment and substituting it into the second function formula, or during actual welding. The resistance welding machine is characterized in that the output of the resistance welding machine is controlled by converting the firing angle, which is obtained by performing the above operation and is set before the start of main welding, into the desired firing angle. output control method. 2. The first functional expression represents the first integral value during the arbitrarily set energization cycle as Vo , the second integral value of the electrode tip voltage as Vt , the desired welding effective current value as Ie , and the first functional constant as K. 1 , I e = K 1 /V o or I e =
The output control method for a resistance welding machine according to claim 1, characterized in that the output is expressed as K 1 /V t . 3 When the second functional formula assumes that the welding effective current value is I e , the firing angle of the control rectifying element is θ, and the second function constant is K 2 , An output control method for a resistance welding machine according to claim 1, characterized in that: 4. The output control method for a resistance welding machine according to claim 1, wherein the arbitrarily set energization cycle is preset within a positive differential coefficient on the envelope of the first integral value. 5 In a resistance welding machine with a built-in control rectifying element for controlling welding output, the voltage between the electrode tips is used as an input signal, and the voltage between the electrode tips is integrated for half a cycle from the first cycle to the arbitrarily set energization cycle. a first integral circuit that outputs a first integral value, and a second integral circuit that integrates the first integral value directly or outputs a second integral value on the output side of the first integral circuit.
Selectively receives the first integral value only during the arbitrarily set energization cycle connected via the integral circuit, or receives the second integral value and calculates the desired welding value according to the first function equation determined in advance. a first function circuit that outputs an effective current value; and a second function equation determined in advance connected to the output side of the first function circuit that calculates and outputs a desired firing angle signal of the control rectifier. a second function circuit; and an ignition circuit connected to the output side of the second function circuit that converts the ignition angle of the control rectifier into the desired ignition angle, and displays the arbitrarily set energization cycle. A resistor characterized in that a signal is inputted from the output side of a separately installed counting circuit to the first integrating circuit, the second integrating circuit, the first function circuit, and the second function circuit installed at the next stage to perform the control respectively. Welding machine output control device.
JP55180680A 1980-12-19 1980-12-19 Method and device for controlling output of resistance welding machine Granted JPS57103788A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP55180680A JPS57103788A (en) 1980-12-19 1980-12-19 Method and device for controlling output of resistance welding machine

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP55180680A JPS57103788A (en) 1980-12-19 1980-12-19 Method and device for controlling output of resistance welding machine

Publications (2)

Publication Number Publication Date
JPS57103788A JPS57103788A (en) 1982-06-28
JPS6213115B2 true JPS6213115B2 (en) 1987-03-24

Family

ID=16087420

Family Applications (1)

Application Number Title Priority Date Filing Date
JP55180680A Granted JPS57103788A (en) 1980-12-19 1980-12-19 Method and device for controlling output of resistance welding machine

Country Status (1)

Country Link
JP (1) JPS57103788A (en)

Also Published As

Publication number Publication date
JPS57103788A (en) 1982-06-28

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