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JPS5914189B2 - Ultrasonic inspection device for resistance spot welds - Google Patents
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JPS5914189B2 - Ultrasonic inspection device for resistance spot welds - Google Patents

Ultrasonic inspection device for resistance spot welds

Info

Publication number
JPS5914189B2
JPS5914189B2 JP53037558A JP3755878A JPS5914189B2 JP S5914189 B2 JPS5914189 B2 JP S5914189B2 JP 53037558 A JP53037558 A JP 53037558A JP 3755878 A JP3755878 A JP 3755878A JP S5914189 B2 JPS5914189 B2 JP S5914189B2
Authority
JP
Japan
Prior art keywords
ultrasonic
circuit
electrode
value
welded
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
JP53037558A
Other languages
Japanese (ja)
Other versions
JPS54130178A (en
Inventor
嘉郎 羽深
光 川和田
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.)
Mitsubishi Electric Corp
Original Assignee
Mitsubishi Electric Corp
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 Mitsubishi Electric Corp filed Critical Mitsubishi Electric Corp
Priority to JP53037558A priority Critical patent/JPS5914189B2/en
Publication of JPS54130178A publication Critical patent/JPS54130178A/en
Publication of JPS5914189B2 publication Critical patent/JPS5914189B2/en
Expired legal-status Critical Current

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  • Investigating Or Analyzing Materials By The Use Of Ultrasonic Waves (AREA)

Description

【発明の詳細な説明】 この発明は抵抗溶接部の超音波検査装置に関す10るも
のである。
DETAILED DESCRIPTION OF THE INVENTION The present invention relates to an ultrasonic inspection device for resistance welds.

一般にスポット溶接部の超音波による非破壊検査は溶接
工程と別の工程を設けて行ない、超音波探傷器を使用し
、探触子を溶接部に当てて、ブラウン管上に表われる多
重反射波形を観測して溶接15状態を判定していたため
、検査に多くの時間を消費するとともに、定量的な判定
方法でないため検査員による判定の差を生じる欠点があ
つた。
Generally, non-destructive ultrasonic testing of spot welds is performed in a separate process from the welding process, and an ultrasonic flaw detector is used to place a probe on the weld and detect multiple reflection waveforms that appear on a cathode ray tube. Since the state of the weld 15 was determined by observation, a large amount of time was consumed in the inspection, and since it was not a quantitative determination method, there was a drawback that the determination differed between inspectors.

また、溶接中にイン・プロセスで超音波により非破壊検
査を行なう従来の方法は、一対の電極の20−方に発信
用の振動子、他方に受信用の振動子を装着し、溶接部に
超音波を透過させ、超音波の透過量の変化をブラウン管
上で観測するものであつた(透過法)。この方法により
、検査時間の低減と、検査の信頼性は飛躍的に向上した
が、送信・25受信用2ケの振動子が必要なこと、また
シリーズ・スポット溶接のように、電極が片側だけにあ
るものに対して適用できないという欠点がある。また、
他の方法として電極の一方側に送・受信用の振動子を装
着し、反射法により非破壊検査を30行なう振動子反射
法もあるが、この方法では振動子を取付けた側の電極の
先端面、あるいは、被溶接材と電極との接触面における
反射波を利用しているため、溶接状態を判定する精度が
著しく低いものであつた。35そこで、このような問題
点を改善する方法として、一方の電極に送受信兼用の振
動子を装着してパルス状の超音波を送出させ、他方の電
極にもうけた超音波反射面で反射された超音波を検知し
、その波高値の変化を検出して、溶接状態を定量的に判
定するようにしたものが開発されている。
In addition, the conventional method of performing in-process non-destructive testing using ultrasonic waves during welding involves attaching a transmitting transducer to one end of a pair of electrodes and a receiving transducer to the other. Ultrasonic waves were transmitted through the device, and changes in the amount of ultrasound transmitted were observed on a cathode ray tube (transmission method). This method reduces inspection time and dramatically improves inspection reliability, but requires two transducers for transmitting and receiving, and unlike series spot welding, the electrode is only on one side. The drawback is that it cannot be applied to anything that exists. Also,
Another method is the transducer reflection method, in which a transducer for transmitting and receiving is attached to one side of the electrode, and a non-destructive inspection is performed using the reflection method. Since the reflected waves from the surface or the contact surface between the material to be welded and the electrode are used, the accuracy of determining the welding state is extremely low. 35 Therefore, as a method to improve these problems, one electrode was equipped with a transducer for both transmitting and receiving purposes to send out pulsed ultrasonic waves, which were then reflected by an ultrasonic reflecting surface provided on the other electrode. A device has been developed that detects ultrasonic waves and detects changes in the wave height value to quantitatively determine the welding state.

まず上記従来の超音波検査装置について説明する。第1
図は従来の超音波検査装置の溶接時における、電極、超
音波振動子および被溶接材の配置と超音波の進行状態を
示す図、第2図は振動子に検知されブラウン管上に示さ
れた、多重反射波形を示す図で、1は電極、2は送受信
兼用の超音波振動子で、電極1に穿設された孔3の内端
面31に装着される。
First, the conventional ultrasonic inspection apparatus described above will be explained. 1st
The figure shows the arrangement of electrodes, ultrasonic transducers, and materials to be welded, and the progress state of ultrasonic waves during welding with a conventional ultrasonic inspection device. Figure 2 shows the progress of ultrasonic waves detected by the transducer and displayed on the cathode ray tube. , a diagram showing multiple reflection waveforms, 1 is an electrode, 2 is an ultrasonic transducer for both transmitting and receiving purposes, and is attached to the inner end surface 31 of a hole 3 made in the electrode 1.

4は電極1に対向する他方の電極、5は電極4に穿設さ
れた孔、51は孔5の内端面で超音波反射面を形成する
Reference numeral 4 denotes the other electrode facing the electrode 1, 5 a hole formed in the electrode 4, and 51 an inner end surface of the hole 5 forming an ultrasonic reflecting surface.

6は電極1の先端面、7は電極4の先端面、8および9
はそれぞれ被溶接材、10は被溶接材8,9の接触面、
11は被溶接材8の電極1の先端面6との接触面、12
は被溶接材9の電極4の先端面7との接触面、13は超
音波振動子2を駆動し、また超音波振動子2に超音波反
射波が入力した際変換される電気信号を検出する送受信
装置である。
6 is the tip surface of electrode 1, 7 is the tip surface of electrode 4, 8 and 9
are the materials to be welded, 10 is the contact surface of the materials 8 and 9 to be welded,
11 is a contact surface of the material to be welded 8 with the tip surface 6 of the electrode 1; 12;
13 is the contact surface of the welding material 9 with the tip surface 7 of the electrode 4; 13 drives the ultrasonic vibrator 2; and detects an electric signal converted when an ultrasonic reflected wave is input to the ultrasonic vibrator 2. It is a transmitting and receiving device.

Tは送信波、B1は送信波Tが接触面10,11および
12においてそれぞれ反射した反射波が合成され、振動
子2に入力された第1の反射波、B2は第1の反射波B
,が電極1の孔3の内端面31で反射したのち再び電極
4の方向に進行し、接触面11および12でそれぞれ反
射され合成された第2の反射波、Cは進行波Tのうち接
触面10,11および12を透過した超音波が超音波反
射面51で反射された後再び接触面10,11および1
2を透過して振動子2に到達した反射波である。第1の
反射波B1の主成分は接触面11および電極1の先端面
6よりの反射波であり、通電時間の時間経過につれて接
触面11と電極1の接触状態がよくなること及び接触面
積が増加するため反射波B1は単調に減少する。
T is a transmitted wave, B1 is a first reflected wave that is a combination of the reflected waves of the transmitted wave T reflected at contact surfaces 10, 11, and 12 and input to the vibrator 2, and B2 is a first reflected wave B.
, is reflected by the inner end surface 31 of the hole 3 of the electrode 1, and then travels toward the electrode 4 again, and is reflected and synthesized from the contact surfaces 11 and 12, respectively, resulting in a second reflected wave.C is the contact wave of the traveling wave T. After the ultrasonic waves transmitted through the surfaces 10, 11 and 12 are reflected by the ultrasonic reflecting surface 51, the ultrasonic waves pass through the contact surfaces 10, 11 and 1 again.
This is a reflected wave that has passed through the oscillator 2 and reached the oscillator 2. The main component of the first reflected wave B1 is the reflected wave from the contact surface 11 and the tip surface 6 of the electrode 1, and as the energization time elapses, the contact state between the contact surface 11 and the electrode 1 improves and the contact area increases. Therefore, the reflected wave B1 decreases monotonically.

また反射波B2は反射波B1とほぼ相似的な変化をする
。一方、反射面51よりの反射波Cは、溶接部を、2度
通過するため、被爵接材8,9の温度上昇による物性変
化の影響を受けるので、反射波Bl,B2のように単調
な変化はしない。
Further, the reflected wave B2 changes almost similarly to the reflected wave B1. On the other hand, the reflected wave C from the reflecting surface 51 passes through the weld twice and is affected by changes in physical properties due to the temperature rise of the welding materials 8 and 9, so it becomes monotonous like the reflected waves Bl and B2. There will be no changes.

第3図は爵接時間と反射波Cの波高値との関係を示す図
で、溶接電流が流れ初める時間T。
FIG. 3 is a diagram showing the relationship between the contact time and the peak value of the reflected wave C, where T is the time at which the welding current begins to flow.

からある時点T,まで、溶接時間の時間経過と共に反射
波Cの波高値は単調に増加する。この理由は溶接時間の
経過とともに溶接面10,11および12の温度が上昇
し、接触状態が良くなるためである。さらに溶接時間が
経過すると時点t1から時点T2まで間に急激に減少す
る。溶接部の断面を検査すると、時点t1から時点T2
に至る過程において微少な溶融部(ナゲツト)が形成さ
れ始めている。すなわち、時点t1から時点T2への変
化は、接合面10附近の金属が固相から液相に転相する
場合の超音波の急激な減衰によるものと考えられる。従
つてこの時点T2を検出することにより、溶融部の形成
の有無を検知することができる。さらに通電時間が経過
すると反射波Cの尖頭値は再び増加し、時点T3で通電
が終了する。第3図は反射波Cの通電時間終了時点T3
における尖頭値H2と、時点T2における尖頭値H,と
の差H2−H1と溶融部径との関係を示す図で、両者の
間には良い相関関係が得られている。
From then until a certain point T, the peak value of the reflected wave C increases monotonically as the welding time elapses. The reason for this is that the temperature of the welding surfaces 10, 11, and 12 increases as the welding time passes, and the contact condition improves. Further, as the welding time elapses, it rapidly decreases from time t1 to time T2. When the cross section of the welded part is inspected, from time t1 to time T2
In the process leading to this, minute melted areas (nuggets) begin to form. That is, the change from time t1 to time T2 is considered to be due to rapid attenuation of the ultrasonic waves when the metal near the bonding surface 10 undergoes a phase change from a solid phase to a liquid phase. Therefore, by detecting this time point T2, it is possible to detect whether or not a melted portion is formed. As the energization time further elapses, the peak value of the reflected wave C increases again, and the energization ends at time T3. Figure 3 shows the end point T3 of the energization time of the reflected wave C.
This is a diagram showing the relationship between the difference H2-H1 between the peak value H2 at time T2 and the peak value H at time T2 and the diameter of the melted part, and a good correlation is obtained between the two.

したがつて反射波Cをゲート回路により選択的に検出し
、通電時間終了時T3の反射波の尖頭値H2と時点T2
における尖頭値H,とを検出し、その差H2一H1を求
めることにより形成される溶融部の径を知ることができ
るので、このことから溶接部分の良否について信頼性の
高い推定をすることができる。ところでスポツト溶接に
於いては電極は消耗品である為に何点が打てば別の電極
と交換する必要がある。
Therefore, the reflected wave C is selectively detected by the gate circuit, and the peak value H2 of the reflected wave at the end of the energization time T3 and the time T2 are detected.
By detecting the peak value H, of I can do it. By the way, in spot welding, the electrode is a consumable item, so it is necessary to replace it with another electrode after several points have been struck.

その場合静的状態(被溶接材を加圧していない状態)に
おいて第1底面波と第2底面波の相対値は電極の取付状
態等によつていろいろ違つた値となる。
In this case, in a static state (state where the material to be welded is not pressurized), the relative values of the first fundamental wave and the second fundamental wave will vary depending on the mounting state of the electrode, etc.

これは実験上明らかなことである。第2点としては長時
間溶接していると電極先端の変形や振動子等への超音波
の変換効率が悪くなるから超音波透過量とナゲツト面積
の関係がずれてくるのでこれを校正する必要があつた。
This is experimentally clear. The second point is that when welding for a long time, the electrode tip deforms and the conversion efficiency of ultrasonic waves to the vibrator etc. deteriorates, so the relationship between the amount of ultrasonic transmission and the nugget area deviates, so this needs to be calibrated. It was hot.

このようなバラツキをカバーして、超音波透過量とナゲ
ツト面積を常に1対1に対応させる方法が無かつた為に
従来の方法では、電極を交換するたびに超音波透過量と
溶融部の面積の関係を求める必要があつた。
Since there was no way to cover such variations and always make a one-to-one correspondence between the amount of ultrasonic transmission and the nugget area, the conventional method has been used to It was necessary to find the relationship between areas.

この発明はこのような問題点を改善するために、なされ
たものであり以下この発明による超音波検査装置のプロ
ツク図を示す。
The present invention has been made to solve these problems, and a block diagram of an ultrasonic inspection apparatus according to the present invention will be shown below.

第4図において14は溶融部、15は通電時間開始信号
を受けると同時に超音波振動子2に電圧を間欠的に印加
してパルス状の超音波を送信させるための送信回路、1
6は超音波振動子2が超音波反射波を受信し電気信号に
変換した信号を増幅して出力する受信回路、17はゲー
ト回路で、受信回路16の出力電圧として電極4の超音
波反射面51からの反射波の波高値を選択するための回
路、18は受信回路16の出力電圧の極小値を検出して
保持し、かつこの尖頭値H1を出力する検出 保持回路
、19は溶接時間中に検出・保持回路18から出力電圧
を表示する表示装置、20は検出・保持回路18から出
力電圧H1を受信したときのみ通電時間終了信号を受け
た時点の受信回路16の出力電圧を保持し、かつこの尖
頭値H2を出力する保持回路、21は検出・保持回路1
8の出力゛亀圧H1と保持回路20の出力電圧H2との
差H2−H1を出力する差動増幅回路、22は受信回路
16からの出力信号を導入してB2エコーのみゲートに
より選択してその尖頭値をホールド出力するゲート回路
、3は上記差動増幅回路21の出力[12−H]の値と
ゲート回路22から生ずるB2エコーに対する電気信号
の比H2−H,/B2を演算する演算回路、24は上記
演算回路23の演算結果を表示する表示装置である。
In FIG. 4, 14 is a melting part, 15 is a transmitting circuit for intermittently applying voltage to the ultrasonic transducer 2 to transmit pulsed ultrasonic waves at the same time as receiving the energization time start signal, 1
Reference numeral 6 denotes a receiving circuit that receives the ultrasonic reflected wave from the ultrasonic transducer 2, amplifies and outputs the signal converted into an electrical signal, and 17 is a gate circuit, which uses the ultrasonic reflecting surface of the electrode 4 as the output voltage of the receiving circuit 16. 18 is a detection/holding circuit for detecting and holding the minimum value of the output voltage of the receiving circuit 16 and outputting this peak value H1; 19 is a welding time A display device 20 that displays the output voltage from the detection/holding circuit 18 holds the output voltage of the receiving circuit 16 at the time of receiving the energization time end signal only when the output voltage H1 is received from the detection/holding circuit 18. , and a holding circuit that outputs this peak value H2, 21 is a detection/holding circuit 1
The output of 8 is a differential amplifier circuit which outputs the difference H2-H1 between the turtle pressure H1 and the output voltage H2 of the holding circuit 20. 22 is a differential amplifier circuit that outputs the difference H2-H1 between the turtle pressure H1 and the output voltage H2 of the holding circuit 20; A gate circuit 3 holds and outputs the peak value, and calculates the ratio H2-H, /B2 of the electrical signal to the B2 echo generated from the gate circuit 22 and the value of the output [12-H] of the differential amplifier circuit 21. The arithmetic circuit 24 is a display device that displays the arithmetic results of the arithmetic circuit 23.

以上のように差信号H2−H,とB2エコーに対応する
電気信号B2の比を演算回路において計算し、この比の
値をナゲツト面積に対応させることにはその面積を求め
ることができ又B2エコーを感度基準とし使用するので
超音波透過量とナゲツト面積の関係を一定に保つことが
できる。
As described above, by calculating the ratio of the difference signal H2-H and the electric signal B2 corresponding to the B2 echo in an arithmetic circuit, and making the value of this ratio correspond to the nugget area, the area can be obtained. Since the echo is used as the sensitivity standard, the relationship between the amount of ultrasound transmitted and the nugget area can be kept constant.

これは以下に説明する実1験例により明らかである。This is clear from the practical example described below.

第5図は従来の方法により超音波透過量△H(H2−H
,)とナゲツト面積の関係を第1底面波B,を一定にし
てとつた図である。
Figure 5 shows the ultrasonic transmission amount △H (H2-H) obtained by the conventional method.
, ) and the nugget area when the first bottom wave B is kept constant.

実験によれば使用した電極の形状、振動子はすべて同じ
ものであり、被溶接材は1.6m10spcc材で溶接
条件は加圧力が350k9、溶接電流8.8KA1?接
時間6〜18サイクルである。従つて第5図から明らか
なようにB,エコーを基準にした場合、超音波透過量と
ナゲツト面積は1対1に対応しない。非常にずれた関係
となつている。第6図は第5図と同様の条件のもとでB
2エコーを一定にした場合のこの発明による超音波透過
量とナゲツト面積の関係を示した図であり第6図より明
らかなように超音波透過量とナゲツト面積はほぼ一定の
関係になつている。
According to the experiment, the shapes of the electrodes and vibrators used were all the same, the material to be welded was 1.6m10spcc, and the welding conditions were a pressure of 350k9 and a welding current of 8.8KA1. The contact time is 6 to 18 cycles. Therefore, as is clear from FIG. 5, when B and echo are used as a reference, the amount of ultrasound transmission and the nugget area do not correspond one-to-one. They have a very skewed relationship. Figure 6 shows B under the same conditions as Figure 5.
2 is a diagram showing the relationship between the amount of ultrasound transmitted and the nugget area according to the present invention when the echoes are held constant.As is clear from FIG. 6, the relationship between the amount of ultrasound transmitted and the nugget area is almost constant. .

従つて電極の形状振動子等が同じならば、超音波透過量
とB2波の比はある定数の関係となる。このようにB2
エコーを各電極毎に一定にしておけば電極を交換しても
同じ板厚、材質の溶接では溶接部の大きさと超音波透過
量の関係を一本の直線上にのせることができる。
Therefore, if the electrodes have the same shape and vibrator, etc., the ratio of the amount of ultrasound transmitted and the B2 wave has a certain constant relationship. Like this B2
If the echo is kept constant for each electrode, even if the electrodes are replaced, the relationship between the size of the weld and the amount of ultrasonic transmission can be placed on a single straight line when welding the same plate thickness and material.

この方法により電極を交換した場合でも常にナゲツト面
積と超音波透過量を1対1に対応することができた為に
電極毎の超音波透過量の違いを校正でき、チツプ交換毎
に超音波透過量とナゲツト面積の関係を取る必要がなく
なつた。
With this method, even when the electrodes are replaced, the nugget area and the amount of ultrasound transmission always correspond one-to-one, so it is possible to calibrate the difference in the amount of ultrasound transmission for each electrode, and the amount of ultrasound transmission can be adjusted every time the chip is replaced. It is no longer necessary to calculate the relationship between quantity and nugget area.

この発明は以上の説明により明らかなように重ねられた
被溶接材を両面から電極で挟み加圧通電して溶接するも
のにおいて、一方の電極に配設せる超音波振動子を駆動
してパルス状に超音波を送出させ、他方の電極に形成せ
る反射面で、被溶接材を通つて伝搬してきた超音波を反
射させこの反射波が上記被溶接材を再び通つて上記超音
波振動子に戻つてきたのを超音波送出時の間に検出しこ
の検出せる反射波の尖頭値の変化から上記被溶接材に形
成される溶融部分の大きさを判別する場合に、静的状態
での電極の底面から反射される波の第2回目のものを用
いて上記判定をするようにしたものである。
As is clear from the above description, this invention is for welding stacked materials to be welded by sandwiching them between electrodes from both sides and applying pressure and current. The ultrasonic wave is transmitted through the welding material, and the reflecting surface formed on the other electrode reflects the ultrasonic wave that has propagated through the welding material, and the reflected wave passes through the welding material again and returns to the ultrasonic vibrator. When determining the size of the molten part formed in the welded material from the change in the peak value of the reflected wave detected during the ultrasonic transmission, the bottom surface of the electrode in a static state. The above determination is made using the second wave reflected from the wave.

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

第1図は溶接装置の要部の構成とその動作原理をするた
めの断面図、第2図は超音波振動子で検出された超音波
反射波の波形、第3図はこの検出方法の情報媒体である
超音波反射波Cの尖頭値の変化を示す特性図、第5図は
被溶接材を加圧しない状態での電極の第1底面波を一定
にした場合の超音波変化量H2−H1と溶融部の面積の
関係の特囲図、第6図は、被溶接材を加圧しない状態で
の電極の第2底面波を一定にした場合の超音波変化量H
2一山と溶融部の面積の関係の特性図、第4図はこの発
明の一完施例の構成を示ず。
Figure 1 is a sectional view showing the configuration of the main parts of the welding equipment and its operating principle, Figure 2 is the waveform of the ultrasonic reflected wave detected by the ultrasonic transducer, and Figure 3 is information about this detection method. A characteristic diagram showing the change in the peak value of the ultrasonic reflected wave C, which is a medium, and Fig. 5 shows the ultrasonic change amount H2 when the first bottom wave of the electrode is kept constant without applying pressure to the welded material. - Figure 6, a special diagram of the relationship between H1 and the area of the molten zone, shows the amount of change in ultrasonic waves H when the second bottom wave of the electrode is kept constant when the material to be welded is not pressurized.
FIG. 4, which is a characteristic diagram of the relationship between the peak and the area of the melted part, does not show the structure of a complete embodiment of the present invention.

Claims (1)

【特許請求の範囲】[Claims] 1 超音波振動子を取付けた電極と超音波反射面を形成
した電極とで被溶接材を挾み、上記両電極間に上記被溶
接材を通して溶接電流を通電するための装置と、上記振
動子を駆動してパルス状に超音波を送出させるための送
信回路と、上記超音波の送出休止時間内に上記超音波反
射面からの超音波反射波を上記振動子により検知して電
気信号として取り出す受信回路と、上記受信回路の出力
信号から上記反射波検出に対する通電時間中における波
高値の極小値を検出するとともに上記極小値に対応する
電気信号H_1を送出する第1の送出回路と、上記極小
値を通過した後の上記出力信号の波高値を検出するとと
もに上記波高値に対応する電気信号H_2を送出する第
2の送出回路と、上記受信回路の出力を導入し、上記超
音波振動子の付設した電極の上記被溶接材に接する電極
面の間を2回通過した反射波に相当する電気信号B_2
を送出するゲート回路と、上記電気信号H_1とH_2
の差信号H_2−H_1を出力する差動増幅回路と、上
記ゲート回路から生ずる電気信号B_2の値と上記差信
号H_2−H_1の値の比H_2−H_1/B_2を求
める演算回路とを備え、上記H_2−H_1/B_2の
値をもとにして被溶接材に形成される溶融部の大きさを
求めるとともに、この値から上記被溶接材の溶接状態の
良否を判断するようにした抵抗点溶接部の超音波検査装
置。
1. A device for sandwiching a material to be welded between an electrode to which an ultrasonic vibrator is attached and an electrode on which an ultrasonic reflecting surface is formed, and passing a welding current through the material to be welded between the two electrodes, and the vibrator. a transmitting circuit for driving the ultrasonic waves to send out ultrasonic waves in a pulsed manner; and detecting ultrasonic reflected waves from the ultrasonic reflecting surface with the vibrator during the ultrasonic sending pause time and extracting them as electrical signals. a receiving circuit; a first sending circuit that detects a minimum value of a peak value during the energization time for the reflected wave detection from the output signal of the receiving circuit and sends out an electrical signal H_1 corresponding to the minimum value; A second sending circuit that detects the peak value of the output signal after passing through the peak value and sends out an electrical signal H_2 corresponding to the peak value, and the output of the receiving circuit are introduced, and the output of the ultrasonic transducer is Electric signal B_2 corresponding to the reflected wave that passed twice between the electrode surfaces of the attached electrodes that are in contact with the welded material.
a gate circuit that sends out the electrical signals H_1 and H_2;
a differential amplifier circuit that outputs a difference signal H_2-H_1, and an arithmetic circuit that calculates a ratio H_2-H_1/B_2 between the value of the electrical signal B_2 generated from the gate circuit and the value of the difference signal H_2-H_1, A resistance spot weld where the size of the fusion zone formed in the welded material is determined based on the value of H_2-H_1/B_2, and the quality of the welding state of the welded material is determined from this value. ultrasonic inspection equipment.
JP53037558A 1978-03-31 1978-03-31 Ultrasonic inspection device for resistance spot welds Expired JPS5914189B2 (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP53037558A JPS5914189B2 (en) 1978-03-31 1978-03-31 Ultrasonic inspection device for resistance spot welds

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP53037558A JPS5914189B2 (en) 1978-03-31 1978-03-31 Ultrasonic inspection device for resistance spot welds

Publications (2)

Publication Number Publication Date
JPS54130178A JPS54130178A (en) 1979-10-09
JPS5914189B2 true JPS5914189B2 (en) 1984-04-03

Family

ID=12500838

Family Applications (1)

Application Number Title Priority Date Filing Date
JP53037558A Expired JPS5914189B2 (en) 1978-03-31 1978-03-31 Ultrasonic inspection device for resistance spot welds

Country Status (1)

Country Link
JP (1) JPS5914189B2 (en)

Cited By (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
DE102009061145B3 (en) * 2008-08-04 2018-07-19 Honda Motor Co., Ltd. Evaluation method using ultrasonic waves

Families Citing this family (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
CN107478721A (en) * 2016-06-08 2017-12-15 武汉理工大学 A kind of point quality real-time ultrasound the cannot-harm-detection device and method

Cited By (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
DE102009061145B3 (en) * 2008-08-04 2018-07-19 Honda Motor Co., Ltd. Evaluation method using ultrasonic waves

Also Published As

Publication number Publication date
JPS54130178A (en) 1979-10-09

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