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JPS5914188B2 - Ultrasonic inspection device for resistance spot welds - Google Patents
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JPS5914188B2 - Ultrasonic inspection device for resistance spot welds - Google Patents

Ultrasonic inspection device for resistance spot welds

Info

Publication number
JPS5914188B2
JPS5914188B2 JP53037557A JP3755778A JPS5914188B2 JP S5914188 B2 JPS5914188 B2 JP S5914188B2 JP 53037557 A JP53037557 A JP 53037557A JP 3755778 A JP3755778 A JP 3755778A JP S5914188 B2 JPS5914188 B2 JP S5914188B2
Authority
JP
Japan
Prior art keywords
ultrasonic
circuit
welded
electrode
peak 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
JP53037557A
Other languages
Japanese (ja)
Other versions
JPS54130177A (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 JP53037557A priority Critical patent/JPS5914188B2/en
Publication of JPS54130177A publication Critical patent/JPS54130177A/en
Publication of JPS5914188B2 publication Critical patent/JPS5914188B2/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5 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状10態を判定していたため、
検査に多くの時間を費するとともに、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, nondestructive 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 observe the multiple reflection waveforms that appear on the cathode ray tube. Since the 10 welding states were determined by
In addition to requiring a lot of time to conduct the inspection, this method also had the disadvantage of causing differences in the judgments of different inspectors because it was not a quantitative judgment method.

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15−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)。
In addition, the conventional method of performing in-process nondestructive 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, and Ultrasonic waves were transmitted through the device, and changes in the amount of ultrasound transmitted were observed on a cathode ray tube (transmission method).

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、発信・ク0 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25行
なう振動子反射法もあるが、この方法では振動子を片付
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。90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35に判定するようにしたものが開発されて
いる。
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. Another method is the transducer reflection method, in which a transmitting/receiving transducer 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 tip end surface of the electrode or the contact surface between the welded material and the electrode are used, the accuracy of determining the welding state is extremely low. 90 So,
As a method to improve these problems, one electrode is equipped with a transducer for both transmitting and receiving purposes to send out pulsed ultrasonic waves, and the ultrasonic waves reflected by the ultrasonic reflecting surface attached to the other electrode are absorbed. A device has been developed that quantitatively determines the welding condition by detecting the change in the peak value.

まず上記従来の超音波検査装置について説明する。に0
− 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. to 0
- Figure 1 shows the arrangement of electrodes, ultrasonic transducers and materials to be welded, and the progress of ultrasonic waves during welding using a conventional ultrasonic inspection device. In the diagram showing a multiple reflection waveform, 1 is an electrode, and 2 is an ultrasonic transducer for both transmission and reception, which 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
は被爵接材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 contact member 9 with the tip surface 7 of the electrode 4, and 13 is the contact surface for driving the ultrasonic transducer 2, and the electrical signal that is converted when the ultrasonic reflected wave is input to the ultrasonic transducer 2. This is a transmitting/receiving device to be detected.

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
1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で反射された後に再び接触面10,11および
12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.
1 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. The ultrasonic wave transmitted through the surfaces 10, 11, and 12 is reflected by the ultrasonic reflecting surface 51, and then transmitted through the contact surfaces 10, 11, and 12 again to reach the vibrator 2. 1st
The main component of the reflected wave B1 is the reflected wave from the contact surface 11 and the tip surface 6 of the electrode 1, and the contact state between the contact surface 11 and the electrode 1 improves as the energization time elapses, and the contact area increases. The reflected wave B1 monotonically decreases.

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、洛接部を2度通
過するため、被溶接材8,9の温度上昇による物注変化
の影響を受けるので、反射波B,,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, since the reflected wave C from the reflecting surface 51 passes through the contact area twice, it is affected by the change in temperature due to the temperature rise of the welded materials 8 and 9, so the reflected waves B, , B2, etc. There are no monotonous changes.

第3図は溶接時間と反射波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 welding 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t1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
の経過とともに接触面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。さらに爵接時間
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T
2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T
3における尖頭値H2と、時点T2における尖頭値H1
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 t1, 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 contact surfaces 10, 11, and 12 increases as welding time progresses, and the contact condition improves. Furthermore, as the contact 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 T
In the process of reaching No. 2, 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 T of the energization time of the reflected wave C.
The peak value H2 at time 3 and the peak value H1 at time T2
This is a diagram showing the relationship between the difference H2-H1 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H1とを検出し、その差H2−H,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。ところで従来の抵抗溶接部
の超音波検査方法であると、同一材質、板厚の被溶接材
を同一の電極で溶接条件を変えて溶接すると超音波透過
量の変化分H2−H,と溶融部の大きさ(面積)の関係
図は溶接条件によつて変化の大きいものとなる。
Therefore, the reflected wave C is selectively detected by a gate circuit, the peak value H2 of the reflected wave at the end of the energization time T3 and the peak value H1 at time T2 are detected, and the difference H2-H is calculated. Since it is possible to know the diameter of the welded part formed by this, it is possible to make a highly reliable estimate of the quality of the welded part from this. By the way, in the conventional ultrasonic inspection method for resistance welds, when welding workpieces of the same material and thickness with the same electrode under different welding conditions, the change in the amount of ultrasonic transmission H2-H and the molten area The relationship diagram of the size (area) of will vary greatly depending on the welding conditions.

これは実験より明らかなことである。従つて従来の方法
であると后接条件が一定のもとで限つて超音波透過量の
変化分H2−H1と溶融部の大きさ(面積)の関係図は
有効であると言えよう。このように溶接条件等による超
音波透過量と溶融部の大きさ(面積)の関係図の変化を
少なくする必要があつた。
This is clear from experiments. Therefore, in the conventional method, it can be said that the diagram of the relationship between the change H2-H1 in the amount of ultrasonic transmission and the size (area) of the melted part is effective only under constant contact conditions. In this way, it was necessary to reduce changes in the relationship diagram between the amount of ultrasonic transmission and the size (area) of the fused portion due to welding conditions and the like.

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について
詳述する。
The present invention has been made to solve these problems, and the ultrasonic inspection apparatus according to the present invention will be described in detail 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出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
変換した信号を増巾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の出力電圧H,と保持回路20の出力゛亀圧H2との
差H2−H1を出力する差動増巾回路、28は溶融部の
大きさを計算するのに必要な定数A,B,C′を保持し
、出力する回路、27は差動増巾回路21からの出力H
2−H1と検出・保持回路18からの出力H1と保持出
力回路28からの出力A2B,C′を基にして溶融部の
大きさを計算する演算回路、22は上記演算回路27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 a voltage to the ultrasonic transducer 2 to send out pulsed ultrasonic waves at the same time as receiving the energization time start signal;
6 is a receiving circuit that receives the ultrasonic reflected wave from the ultrasonic transducer 2, amplifies and outputs the signal converted into an electric signal, and 17 is a gate circuit that uses the ultrasonic reflection of the electrode 4 as the output voltage of the receiving circuit 16. 18 is a circuit for selecting the peak value of the reflected wave from the surface 51; 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; A display device 20 displays the output voltage from the detection/holding circuit 18 during welding time, and displays 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. A holding circuit that holds and outputs this peak value H2, 21 is a detection/holding circuit 1
8 is a differential amplification circuit that outputs the difference H2-H1 between the output voltage H and the output voltage H2 of the holding circuit 20, and 28 is a constant A, B, which is necessary to calculate the size of the melted part. 27 is the output H from the differential amplification circuit 21.
2-A calculation circuit that calculates the size of the melted portion based on H1, the output H1 from the detection/holding circuit 18, and the outputs A2B and C' from the holding output circuit 28; 22 is the calculation result of the calculation circuit 27; It is a display device for displaying images.

以上のように差信号H2−H1と極小値の尖頭値H,と
後で述べる被溶接の板厚・材質等により決定される定数
A,B,C′により溶融部の大きさ(面積)を計算する
ことができる。
As described above, the size (area) of the molten part is determined by the difference signal H2-H1, the peak value H of the minimum value, and constants A, B, and C' determined by the thickness and material of the workpiece to be welded, etc., which will be described later. can be calculated.

また、この方法によると溶接条件に依存するバラツキを
無くす事ができる。これは以下に説明する実1験例によ
り明らかである。
Further, according to this method, variations depending on welding conditions can be eliminated. This is clear from the practical example described below.

この一実施例である第5図は、従来と同様の方法で板厚
1.6m77!のSpcc材を溶接条件イ,口,ハと変
えて溶接して得た超音波透過量の変化分H2−H,と爵
融部の大きさ(面積)の関係図である。第5図から明ら
かなように洛接条件(溶接竜流、加圧分)を変化させる
と超音波透過量H2Hlと溶融部の大きさの関係は平行
移動した関係となる。すなわち、溶接条件(溶接電流、
加圧分)を変化させると超音波透過量の変化分H2−H
1が零の時の溶融部の大きさ(面積)はいろいろの値を
取ることになる。第6図は第5図のデータのうち超音波
透過量の変化分が零の時のH1の大きさとその時の溶融
部の大きさ(面積)の関係図である。
One example of this, shown in Fig. 5, shows a plate thickness of 1.6 m77! FIG. 2 is a diagram showing the relationship between the change H2-H in the amount of ultrasonic transmission and the size (area) of the fusion zone obtained by welding the Spcc material of 1. As is clear from FIG. 5, when the contact conditions (welding torrent, pressurization) are changed, the relationship between the amount of ultrasonic transmission H2Hl and the size of the molten zone shifts in parallel. In other words, welding conditions (welding current,
When the amount of applied pressure is changed, the amount of change in ultrasound transmission amount H2-H
When 1 is zero, the size (area) of the molten part takes on various values. FIG. 6 is a diagram showing the relationship between the magnitude of H1 when the amount of change in the amount of ultrasonic transmission is zero among the data in FIG. 5, and the size (area) of the melted part at that time.

これより明らかなように極小点での超音波透過波の尖頭
値H,と癖融部の大きさは良い比例関係がある。第7図
は、上記第5図と第6図を1つの関係図としたものであ
る。
As is clear from this, there is a good proportional relationship between the peak value H of the ultrasonic transmitted wave at the minimum point and the size of the fused zone. FIG. 7 is a diagram showing the relationship between FIG. 5 and FIG. 6 described above.

横軸に超音波透過量(相対イ旬、縦軸に?融部の大きさ
(面積)をとつてある。図中の直線二は、H1と極小点
での?融部の面積の関係を示しており、直線イ,口,ハ
等はH2−H1と溶融部の面積の関係を示している。す
なわち、超音波透過量と溶融部の大きさの関係は、極小
点に於いて溶接条件に依らず一対一に対応しているが、
極小点を過ぎてからは、溶接条件により直線イ,口,ハ
と分離する。上記第7図の関係を式で表わすと次式とな
る。
The horizontal axis shows the amount of ultrasonic transmission (relative frequency), and the vertical axis shows the size (area) of the fusion zone. Straight line 2 in the figure shows the relationship between H1 and the area of the fusion zone at the minimum point. The lines A, C, C, etc. indicate the relationship between H2-H1 and the area of the molten zone.In other words, the relationship between the amount of ultrasonic transmission and the size of the fused zone is determined by the welding conditions at the minimum point. Although it corresponds one-on-one regardless of
After passing the minimum point, it separates into straight lines A, C, and C depending on the welding conditions. The relationship shown in FIG. 7 above can be expressed as the following equation.

S−A−H1+B・(H2−H1)+CI−(1)A:
直線二の傾きであり、H2−H1−0での超音波透過量
H1に対する溶融部の面積の割合。
S-A-H1+B・(H2-H1)+CI-(1)A:
It is the slope of straight line 2, and is the ratio of the area of the melted part to the amount of ultrasound transmission H1 at H2-H1-0.

B:直線イ,口,ハ等の傾きであり、超音波透過量(H
2−H1)に対する溶融部の面積の増加分。
B: The slope of straight lines A, C, etc., and the amount of ultrasound transmission (H
2-H1) Increase in the area of the melted part.

C:被溶接材に依存する定数。C: Constant depending on the material to be welded.

このように上式を用いることにより、板厚、材質毎に上
記各定数A,B,C′を予め求めておけば溶接条件等に
よるバラツキを少なくして溶融部の大きさを測定するこ
とができる。
By using the above equations, if the constants A, B, and C' are determined in advance for each plate thickness and material, it is possible to measure the size of the fused zone while reducing variations due to welding conditions, etc. can.

この発明は、以上の説明により明らかなように、重ねら
れた被洛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播して来た超音波
を反射させこの反射波が上記被爵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、この検出せる反射板の尖頭値の変化のうち、極小点
での反射波の尖頭値と、溶接電流終了時の反射波の尖頭
値と上記極小点での反射波の尖頭値との差の値等より、
上記被爵接材に形成される溶融部分の面積を算出できる
ようにしたものである。
As is clear from the above description, the present invention is applicable to welding by sandwiching stacked materials to be welded from both sides between electrodes and applying pressure and current, in which an ultrasonic vibrator disposed on one electrode is driven. The ultrasonic wave is transmitted in a pulsed manner, and the ultrasonic wave that has propagated through the welding material is reflected by the reflecting surface formed on the other electrode, and this reflected wave passes through the welding material again and then The return to the ultrasonic transducer is detected during the ultrasonic wave transmission, and among the changes in the peak value of the reflector that is detected, the peak value of the reflected wave at the minimum point and the reflection at the end of the welding current are detected. From the value of the difference between the peak value of the wave and the peak value of the reflected wave at the minimum point, etc.,
The area of the melted portion formed in the above-mentioned welding material can be calculated.

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

第1図は溶接装置の要部の構成と、その動作原理を説明
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図、第3図はこの検査方法の情報媒
体である反射波Cの尖頭値の変化を示す特性図、第4図
はこの発明の一実施例の構成を示すプロツタ図、第5図
は爵接条件を変えた場合の反射波Cの変化量(H2−H
,)と被爵接材の爵融部(SH2−H1)の大きさとの
関係を示す図、第6図は溶接条件を変えた場合の反射波
Cの変化量と被爵接材の溶融部の大きさとの関係を示す
図、第7図は第5図と第6図に示した特性を1つにまと
めた特性図である。 図において1,4は電極、2は超音波振動子、3,5は
孔、51は超音波反射面、8,9は被溶接材、10,1
1,12は超音波反射面を形成する各部材の接触面、1
3は送受信装置、14は溶融部分、15は送信回路、1
6は受信回路、17はゲート回路、18は検出保持回路
、19,22は表示装置、20は保持回路、21は差動
増巾回路、27は演算回路、28は保持・出力回路であ
る。
Figure 1 is a cross-sectional view to explain the configuration of the main parts of the welding equipment and its operating principle, Figure 2 is a waveform diagram of the ultrasonic reflected waves detected by the ultrasonic transducer, and Figure 3 is a diagram for this inspection. A characteristic diagram showing changes in the peak value of the reflected wave C, which is the information medium of the method, FIG. 4 is a plotter diagram showing the configuration of an embodiment of the present invention, and FIG. Amount of change in wave C (H2-H
, ) and the size of the molten part (SH2-H1) of the welding material. Figure 6 shows the amount of change in the reflected wave C and the molten part of the welding material when welding conditions are changed. FIG. 7 is a characteristic diagram that combines the characteristics shown in FIGS. 5 and 6 into one. In the figure, 1 and 4 are electrodes, 2 is an ultrasonic vibrator, 3 and 5 are holes, 51 is an ultrasonic reflecting surface, 8 and 9 are materials to be welded, 10 and 1
1 and 12 are contact surfaces of each member forming an ultrasonic reflecting surface, 1
3 is a transmitting/receiving device, 14 is a melting part, 15 is a transmitting circuit, 1
6 is a receiving circuit, 17 is a gate circuit, 18 is a detection and holding circuit, 19 and 22 are display devices, 20 is a holding circuit, 21 is a differential amplification circuit, 27 is an arithmetic circuit, and 28 is a holding/output circuit.

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検
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対応する電気信号H_1
を送出する第一の送出回路と、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
を出力する差動増巾回路とを備え上記第1の送出回路か
らの電気信号H_1と、上記差動増幅回路からの差信号
H_2−H_1をもとにして上記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その大きさの値から上
記被溶接材の溶融状態の良否を判定するようにした抵抗
点溶融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 between the two electrodes through the material to be inspected, 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, and detecting the minimum value of the peak value during the energization time for the reflected wave detection from the output signal of the receiving circuit and generating a corresponding electric signal H_1;
a first sending circuit that sends out the electrical signal; a second sending circuit that detects the peak value of the output signal after passing through the minimum value and sends out an electrical signal H_2 corresponding to the peak value; Difference signal between H_1 and H_2 H_2-H_1
and a differential amplification circuit that outputs a molten material formed on the welded material based on the electric signal H_1 from the first sending circuit and the difference signal H_2-H_1 from the differential amplification circuit. An ultrasonic inspection device for a resistance point welded part, which determines the size of the welded part and determines the quality of the melted state of the welded material based on the value of the size.
JP53037557A 1978-03-31 1978-03-31 Ultrasonic inspection device for resistance spot welds Expired JPS5914188B2 (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP53037557A JPS5914188B2 (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
JP53037557A JPS5914188B2 (en) 1978-03-31 1978-03-31 Ultrasonic inspection device for resistance spot welds

Publications (2)

Publication Number Publication Date
JPS54130177A JPS54130177A (en) 1979-10-09
JPS5914188B2 true JPS5914188B2 (en) 1984-04-03

Family

ID=12500808

Family Applications (1)

Application Number Title Priority Date Filing Date
JP53037557A Expired JPS5914188B2 (en) 1978-03-31 1978-03-31 Ultrasonic inspection device for resistance spot welds

Country Status (1)

Country Link
JP (1) JPS5914188B2 (en)

Families Citing this family (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS61155952A (en) * 1984-12-25 1986-07-15 ウエスチングハウス エレクトリック コ−ポレ−ション Ultrasonic inspection method of welding section

Also Published As

Publication number Publication date
JPS54130177A (en) 1979-10-09

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