JPH0473103B2 - - Google Patents
Info
- Publication number
- JPH0473103B2 JPH0473103B2 JP58217815A JP21781583A JPH0473103B2 JP H0473103 B2 JPH0473103 B2 JP H0473103B2 JP 58217815 A JP58217815 A JP 58217815A JP 21781583 A JP21781583 A JP 21781583A JP H0473103 B2 JPH0473103 B2 JP H0473103B2
- Authority
- JP
- Japan
- Prior art keywords
- measuring device
- storage box
- coil
- transmitting
- ultrasonic measuring
- 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 - Lifetime
Links
Classifications
-
- G—PHYSICS
- G01—MEASURING; TESTING
- G01N—INVESTIGATING OR ANALYSING MATERIALS BY DETERMINING THEIR CHEMICAL OR PHYSICAL PROPERTIES
- G01N29/00—Investigating or analysing materials by the use of ultrasonic, sonic or infrasonic waves; Visualisation of the interior of objects by transmitting ultrasonic or sonic waves through the object
- G01N29/22—Details, e.g. general constructional or apparatus details
- G01N29/24—Probes
- G01N29/2412—Probes using the magnetostrictive properties of the material to be examined, e.g. electromagnetic acoustic transducers [EMAT]
-
- G—PHYSICS
- G01—MEASURING; TESTING
- G01N—INVESTIGATING OR ANALYSING MATERIALS BY DETERMINING THEIR CHEMICAL OR PHYSICAL PROPERTIES
- G01N2291/00—Indexing codes associated with group G01N29/00
- G01N2291/02—Indexing codes associated with the analysed material
- G01N2291/028—Material parameters
- G01N2291/02854—Length, thickness
Landscapes
- Physics & Mathematics (AREA)
- Electromagnetism (AREA)
- Health & Medical Sciences (AREA)
- Life Sciences & Earth Sciences (AREA)
- Chemical & Material Sciences (AREA)
- Analytical Chemistry (AREA)
- Biochemistry (AREA)
- General Health & Medical Sciences (AREA)
- General Physics & Mathematics (AREA)
- Immunology (AREA)
- Pathology (AREA)
- Length Measuring Devices Characterised By Use Of Acoustic Means (AREA)
- Investigating Or Analyzing Materials By The Use Of Ultrasonic Waves (AREA)
Description
【発明の詳細な説明】
〔発明の利用分野〕
本発明は導電性被検材内に電磁的な作用で超音
波を発生させかつ逆の過程で該超音波を検出して
導電性被検材の厚み測定や探傷などを非接触で行
なう電磁超音波計測装置に関する。[Detailed Description of the Invention] [Field of Application of the Invention] The present invention generates ultrasonic waves in a conductive test material by electromagnetic action and detects the ultrasonic waves in the reverse process. This invention relates to an electromagnetic ultrasonic measuring device that performs non-contact thickness measurement and flaw detection.
従来この種の静磁界を発生する直流電磁石など
の磁石と送受信コイルとを有し、送受信コイルに
パルス電流などの高周波電流を流すことにより被
検材内表面に発生する渦電流と上記静磁界との相
互作用により被検材内に超音波を発生して、かつ
逆の過程で該超音波(変化歪)と磁界との相互作
用により発生する渦電流を上記送受信コイルで検
出する電磁超音波計測装置は、金属材などの導電
性被検材の厚み測定や探傷などの計測を被検材と
非接触で行なえる装置として注目されてきてい
る。なおこの装置で上記送受信コイルはそれ自身
では機械的強度が弱いなどのため非導電性の収納
箱内に樹脂などで固着したうえ該収納箱を介して
上記磁石の極間などの所定位置に装着しているの
が通常である。しかるにこの従来装置では送受信
コイルにパルス電流などの高周波電流を流すと、
該高周波電流と静磁界(直流磁界)との相互作用
により送受信コイル自身も振動して超音波を発生
し、該超音波が収納箱内の樹脂などを伝播しその
底面で反射して送受信コイルで検出され超音波雑
音信号となつて超音波計測の支障となるなどの欠
点があつた。
Conventionally, it has a magnet such as a DC electromagnet that generates this type of static magnetic field and a transmitter/receiver coil, and by passing a high frequency current such as a pulse current through the transmitter/receiver coil, the eddy current generated on the inner surface of the material to be examined and the static magnetic field are combined. Electromagnetic ultrasonic measurement in which ultrasonic waves are generated in the material under test due to the interaction of The device has been attracting attention as a device that can perform measurements such as thickness measurement and flaw detection of conductive materials such as metal materials without contacting the materials to be tested. In this device, the transmitter/receiver coil itself has weak mechanical strength, so it is fixed in a non-conductive storage box with resin, etc., and then attached to a predetermined position, such as between the poles of the magnet, through the storage box. It is normal to do so. However, with this conventional device, when a high frequency current such as a pulse current is passed through the transmitting and receiving coil,
Due to the interaction between the high-frequency current and the static magnetic field (DC magnetic field), the transmitting and receiving coil itself vibrates and generates ultrasonic waves.The ultrasonic waves propagate through the resin in the storage box and are reflected at the bottom of the box, causing the transmitting and receiving coil to vibrate and generate ultrasonic waves. There were drawbacks such as the detected ultrasonic noise signal becoming a hindrance to ultrasonic measurement.
本発明の目的は上記した従来技術の欠点である
送受信コイルの収納箱からの超音波雑音信号を除
去した電磁超音波計測装置を提供するにある。
SUMMARY OF THE INVENTION An object of the present invention is to provide an electromagnetic ultrasonic measuring device that eliminates the ultrasonic noise signal from the transmitting/receiving coil storage box, which is the drawback of the prior art described above.
本発明は送受信コイルを非導電性の収納箱内に
酸化タングステン粉などの金属微粉などの音波散
乱剤を混入した樹脂などの充てん材で固着し、送
受信コイル自射の振動により収納箱内で発生する
超音波雑音を上記音波散乱剤により散乱吸収し除
去するようにした電磁超音波計測装置である。
In the present invention, the transmitter/receiver coil is fixed in a non-conductive storage box with a filler such as resin mixed with a sound wave scattering agent such as fine metal powder such as tungsten oxide powder, and vibrations generated by the transmitter/receiver coil self-emission are generated inside the storage box. This is an electromagnetic ultrasonic measuring device in which the ultrasonic noise generated by the electromagnetic wave is scattered and absorbed by the above-mentioned sound scattering agent and removed.
以下に本発明の一実施例を第1図ないし第3図
により説明する。
An embodiment of the present invention will be described below with reference to FIGS. 1 to 3.
第1図は本発明による電磁超音波計測装置の一
実施例を示す部分斜視断面ほかブロツク図であ
る。第1図において、導電性の被検材1の表面と
対向して、逆U字形の鉄心2と直流励磁コイル3
とからなる直流電磁石が配置され、かつ鉄心2の
極間に送受信コイル4を収納した収納箱5が取り
付けられている。また直流励磁コイル3に励磁電
流を供給する励磁電源6、送受信コイル4にパル
ス電流などの高周波電流を供給するパルス発生器
7、送受信コイル4により検出された信号を増幅
する増幅器8、増幅器8の出力により被検材1の
厚みや探傷などの超音波計測結果を表示する表示
器9が設けられる。 FIG. 1 is a partial perspective cross section and block diagram showing an embodiment of an electromagnetic ultrasonic measuring device according to the present invention. In FIG. 1, an inverted U-shaped iron core 2 and a DC excitation coil 3 are placed facing the surface of a conductive test material 1.
A DC electromagnet consisting of the above is arranged, and a storage box 5 containing a transmitting/receiving coil 4 is attached between the poles of the iron core 2. Also, an excitation power supply 6 that supplies excitation current to the DC excitation coil 3, a pulse generator 7 that supplies high frequency current such as a pulse current to the transmission and reception coil 4, an amplifier 8 that amplifies the signal detected by the transmission and reception coil 4, and an amplifier 8 that amplifies the signal detected by the transmission and reception coil 4. A display 9 is provided which displays the ultrasonic measurement results such as the thickness of the material 1 to be inspected and flaw detection based on the output.
この構成で、まず励磁電源6より直流励磁コイ
ル3に励磁直流を流して直流電磁石を励磁し、対
向する被検材1内の上記鉄心2の極間に対応する
部分に直流電磁(図中に点線で示す)を発生させ
ておき、つぎにパルス発生器7より送受信コイル
4にパルス電流などの高周波電流を流すと対向す
る被検材1内の表面の部分に渦電流を誘起し発生
する。すると該渦電流と上記直流磁界との相互作
用により、被検材1内の表面の部分に変化歪を生
じて超音波を発生し、該超音波が被検材1内を伝
播する。かくて伝播した超音波が被検材1内の欠
陥および底面より反射して被検材1内の上記表面
の部分に戻り到達すると、上記と逆の過程で該超
音波による変化歪と上記直流磁界との相互作用に
より被検材1内の表面の部分に渦電流を発生し、
該渦電流は送受信コイル4で検出されて増幅器8
を介し増幅されたのち表示器9により被検材1の
厚みや探傷などの超音波計測結果が表示される。 In this configuration, first, an excitation DC is passed through the DC excitation coil 3 from the excitation power supply 6 to excite the DC electromagnet, and a DC electromagnet ( When a high frequency current such as a pulse current is caused to flow from the pulse generator 7 to the transmitting/receiving coil 4 (shown by a dotted line), an eddy current is induced and generated on the opposing surface of the test material 1. Then, due to the interaction between the eddy current and the DC magnetic field, varying strain is generated on the surface of the material 1 to be tested, generating ultrasonic waves, which propagate within the material 1 to be tested. When the ultrasonic waves propagated in this way reflect from defects and the bottom surface of the test material 1 and return to the above-mentioned surface part of the test material 1, the change distortion caused by the ultrasonic waves and the above-mentioned direct current are generated in the reverse process. An eddy current is generated on the surface of the test material 1 due to interaction with the magnetic field,
The eddy current is detected by the transmitting/receiving coil 4 and sent to the amplifier 8.
After being amplified via the display 9, the ultrasonic measurement results such as the thickness of the material 1 to be inspected and flaw detection are displayed.
つぎに第2図は第1図の送受信コイル4を収納
する収納箱5の部分の部分拡大斜視断面図であ
る。第2図において、送受信コイル4は一般には
外径(直経)0.1〜0.3mm程度の導線を数層にして
数10回渦巻き状に巻回したものが用いられるもの
で、それ自身では機械的な強度が弱いことなどの
ため従来から非導電性の収納箱内に樹脂などで固
着したうえ該収納箱を介して直流電磁石の鉄心の
極間などの所定位置に装着していたが、これに対
し本発明によれば次のようにして送受信コイル4
を非導電性の収納箱5内に酸化タングステン粉な
どの金属微粉などの音波散乱剤を混入した樹脂な
どの充てん材で固着するようにしている。すなわ
ち送受信コイル4は非導電性の収納箱5内の下部
(図において)に設置され、収納箱5の内部穴1
0から送受信コイルの両端の口出し線11と12
が引き出されている。この状態で上部穴10から
金属微粉などの音波散乱剤たとえば酸化タングス
テン粉を混入した樹脂などの充てん材たとえばエ
ポキシ系樹脂13が注入され乾燥されて硬化さ
れ、これにより送受信コイル4は収納箱5内の所
定位置に固着される。その後に収納箱5のフラン
ジ部に設けられた取付穴14を用いて第1図の鉄
心2の極間の所定位置に取り付けられる。 Next, FIG. 2 is a partially enlarged perspective sectional view of the storage box 5 that houses the transmitting/receiving coil 4 shown in FIG. In Fig. 2, the transmitting/receiving coil 4 is generally made of several layers of conductive wire with an outer diameter (diameter) of about 0.1 to 0.3 mm and wound several tens of times in a spiral shape. Due to its weak strength, it has traditionally been fixed in a non-conductive storage box with resin, etc., and then mounted in a predetermined position, such as between the poles of a DC electromagnet's iron core, through the storage box. On the other hand, according to the present invention, the transmitter/receiver coil 4
is fixed in a non-conductive storage box 5 with a filler such as resin mixed with a sound scattering agent such as fine metal powder such as tungsten oxide powder. That is, the transmitter/receiver coil 4 is installed at the lower part (in the figure) inside the non-conductive storage box 5, and is connected to the internal hole 1 of the storage box 5.
0 to lead wires 11 and 12 at both ends of the transmitting and receiving coil.
is being brought out. In this state, a filler such as an epoxy resin 13 mixed with a sound scattering agent such as a metal powder or a tungsten oxide powder is injected from the upper hole 10 and is dried and hardened. is fixed in place. Thereafter, it is attached to a predetermined position between the poles of the iron core 2 in FIG. 1 using the attachment hole 14 provided in the flange portion of the storage box 5.
この構成による第1図と第2図の送受信コイル
4の検出信号の波形が第3図に例示される。すな
わち第1図と第2図の送受信コイル4にパルス電
流などの高周波電流を流すと、該高周波電流と上
記直流磁界との相互作用により送受信コイル4自
身も振動して超音波を発生し該超音波が収納箱5
内の樹脂などの充てん材を伝播しその裏面より反
射して送受信コイル4で検出されるため、第3図
に示すように送受信コイル4からの送信波Tと送
受信コイルで検出される被検材1の第1および第
2底面エコーB1およびB2など(欠陥エコーは図
示していない)のほか、従来装置では送受信コイ
ル4の収納箱5の裏面からの第1および第2エコ
ーBP1およびBP2(図中に点線で示す)の波形が
超音波雑音信号として混在して表示器9に表示さ
れるので超音波計測に支障をきたすのに反して、
本発明によれば送受信コイル4自身の振動で発生
した超音波は収納箱5内の樹脂などの充てん材を
伝播するうちに混入する酸化タングステン粉など
の金属微粉などの音波散乱剤に衝突し散乱して吸
収され送受信コイル4で検出できない程に減衰さ
れるため、従来の収納箱5の裏面からの第1およ
び第2エコーBP1およびBP2の波形が超音波雑音
信号として表示器9に表示されることがないので
超音波計測の障害が除去され性能が大幅に向上す
る。 The waveform of the detection signal of the transmitting/receiving coil 4 of FIGS. 1 and 2 with this configuration is illustrated in FIG. 3. In other words, when a high frequency current such as a pulse current is passed through the transmitting/receiving coil 4 shown in FIGS. Sound wave storage box 5
The transmitting wave T from the transmitting/receiving coil 4 and the test material detected by the transmitting/receiving coil propagate through the filling material such as resin inside and are reflected from the back surface and detected by the transmitting/receiving coil 4, as shown in Fig. 3. In addition to the first and second bottom echoes B 1 and B 2 (defective echoes are not shown), the conventional device also detects first and second echoes BP 1 and BP 1 from the back side of the storage box 5 of the transmitting/receiving coil 4 The waveform of BP 2 (indicated by the dotted line in the figure) is mixed as an ultrasonic noise signal and displayed on the display 9, which interferes with ultrasonic measurement.
According to the present invention, the ultrasonic waves generated by the vibration of the transmitter/receiver coil 4 propagate through the filling material such as resin in the storage box 5, collide with the sound scattering agent such as fine metal powder such as tungsten oxide powder mixed in, and are scattered. The waveforms of the first and second echoes BP 1 and BP 2 from the back of the conventional storage box 5 are displayed on the display 9 as ultrasonic noise signals. This eliminates obstacles to ultrasonic measurement and greatly improves performance.
なお上記実施例では磁界を発生するのに直流電
磁石を用いているが永久磁石を用いてもよく、そ
の場合には励磁電源は不要である。また直流電磁
石を構成する鉄心と直流励磁コイルの形態も第1
図に例示するものに限りものではない。また送受
信コイルは一体で兼用のものを説明したが、送信
コイルと受信コイルの2個のコイルからなるもの
を用いてもよく、コイルの形状についても特定形
状に限るものではない。さらに送受信コイルの収
納箱内の充てん物は樹脂に限るものでなく、混入
する音波散乱剤も酸化タングステン粉などの金属
微粉などに限定されるものでなく音波散乱効果の
ある微粉状の音波散乱剤であればよい。 In the above embodiment, a DC electromagnet is used to generate the magnetic field, but a permanent magnet may also be used, and in that case, an excitation power source is not required. In addition, the configuration of the iron core and DC excitation coil that make up the DC electromagnet is also the first.
It is not limited to what is illustrated in the figure. Moreover, although the transmitting and receiving coil is described as being integrated and used for both purposes, a coil consisting of two coils, a transmitting coil and a receiving coil, may also be used, and the shape of the coil is not limited to a specific shape. Furthermore, the filling material in the storage box of the transmitter/receiver coil is not limited to resin, and the sound wave scattering agent mixed in is not limited to fine metal powder such as tungsten oxide powder, but also a fine powder sound scattering agent that has a sound scattering effect. That's fine.
以上のように本実施例によれば、送受信コイル
を酸化タングステン粉などの金属微粉などの微粉
状の音波散乱剤を混入したエポキシ系の樹脂など
の充てん材を用いて収納箱内に固着することによ
り、送受信コイル自身の振動により収納箱内で発
生する超音波雑音を散乱吸収し減衰させて除去す
ることができる。 As described above, according to this embodiment, the transmitter/receiver coil is fixed in the storage box using a filler such as epoxy resin mixed with a fine sound scattering agent such as a fine metal powder such as tungsten oxide powder. As a result, ultrasonic noise generated within the storage box due to the vibration of the transmitter/receiver coil itself can be scattered, absorbed, attenuated, and removed.
以上の説明のように本発明の電磁超音波計測装
置によれば、従来装置の欠点となつていた送受信
コイル自身の高周波振動による超音波雑音を容易
かつ十分に除去することができるため、超音波計
測性が大幅に向上できる。
As described above, according to the electromagnetic ultrasonic measuring device of the present invention, it is possible to easily and sufficiently remove ultrasonic noise caused by the high-frequency vibration of the transmitting and receiving coil itself, which was a drawback of conventional devices. Measurability can be greatly improved.
第1図は本発明による電磁超音波計測装置の一
実施例を示す部分斜視断面ほかブロツク図、第2
図は第1図の送受信コイルの収納箱部分の部分拡
大斜視断面図、第3図は動作波形図である。
1……被検材、2……直流電磁石の鉄心、3…
…同じく直流励磁コイル、4……送受信コイル、
5……収納箱、6……励磁電源、7……パルス発
生器、8……増幅器、9……表示器、10……上
部穴、11,12……口出し線、13……超音波
散乱剤を混入した充てん材。
FIG. 1 is a partial perspective cross section and block diagram showing an embodiment of the electromagnetic ultrasonic measuring device according to the present invention, and FIG.
The figure is a partially enlarged perspective sectional view of the storage box portion of the transmitting/receiving coil shown in FIG. 1, and FIG. 3 is an operational waveform diagram. 1... Test material, 2... Iron core of DC electromagnet, 3...
...Same DC excitation coil, 4...Transmission/reception coil,
5... Storage box, 6... Excitation power supply, 7... Pulse generator, 8... Amplifier, 9... Display, 10... Upper hole, 11, 12... Lead wire, 13... Ultrasonic scattering Filling material mixed with agent.
Claims (1)
し、該送受信コイルに高周波電流を流すことによ
り被検材内に発生する渦電流と被検材内の上記静
磁界との相互作用により被検材内に超音波を発生
し、かつ逆の過程で該超音波を上記送受信コイル
により検出する電磁超音波計測装置において、上
記送受信コイルを非導電性の収納箱内に音波散乱
剤を混入した充てん材で固着してなる電磁超音波
計測装置。 2 上記音波散乱剤は金属微粉からなることを特
徴とする特許請求の範囲第1項記載の電磁超音波
計測装置。 3 上記金属微粉は酸化タングステン粉からなる
ことを特徴とする特許請求の範囲第2項記載の電
磁超音波計測装置。 4 上記充てん材は樹脂からなることを特徴とす
る特許請求の範囲第1項記載の電磁超音波計測装
置。[Scope of Claims] 1. It has a magnet that generates a static magnetic field and a transmitter/receiver coil, and when a high-frequency current is passed through the transmitter/receiver coil, an eddy current generated in the specimen material and the static magnetic field in the specimen material are combined. In an electromagnetic ultrasonic measuring device that generates ultrasonic waves in the material being tested through the interaction of An electromagnetic ultrasonic measuring device that is fixed with a filler containing a scattering agent. 2. The electromagnetic ultrasonic measuring device according to claim 1, wherein the sound wave scattering agent is made of fine metal powder. 3. The electromagnetic ultrasonic measuring device according to claim 2, wherein the metal fine powder is made of tungsten oxide powder. 4. The electromagnetic ultrasonic measuring device according to claim 1, wherein the filler is made of resin.
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP58217815A JPS60111153A (en) | 1983-11-21 | 1983-11-21 | Electromagnetic ultrasonic measuring device |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP58217815A JPS60111153A (en) | 1983-11-21 | 1983-11-21 | Electromagnetic ultrasonic measuring device |
Publications (2)
| Publication Number | Publication Date |
|---|---|
| JPS60111153A JPS60111153A (en) | 1985-06-17 |
| JPH0473103B2 true JPH0473103B2 (en) | 1992-11-19 |
Family
ID=16710167
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP58217815A Granted JPS60111153A (en) | 1983-11-21 | 1983-11-21 | Electromagnetic ultrasonic measuring device |
Country Status (1)
| Country | Link |
|---|---|
| JP (1) | JPS60111153A (en) |
-
1983
- 1983-11-21 JP JP58217815A patent/JPS60111153A/en active Granted
Also Published As
| Publication number | Publication date |
|---|---|
| JPS60111153A (en) | 1985-06-17 |
Similar Documents
| Publication | Publication Date | Title |
|---|---|---|
| CN108802185B (en) | Metal material defect detection sensor based on pulsed eddy current and electromagnetic ultrasonic | |
| US12449320B2 (en) | Electromagnetic ultrasonic double-wave transducer | |
| CN109521083B (en) | An electromagnetic acoustic composite non-destructive testing device, system and method | |
| CN209745873U (en) | Electromagnetic-acoustic composite nondestructive testing device and system | |
| CN109060206A (en) | A kind of ferrimagnet stress measurement device and method | |
| CN117168573B (en) | Pipeline liquid level height detection device and method based on electromagnetic ultrasonic longitudinal wave | |
| CN104076094A (en) | Ultrasonic transduction probe for exciting and receiving ultrasonic horizontal shear guide wave | |
| Rieger et al. | Examination of the liquid volume inside metal tanks using noncontact EMATs from outside | |
| JPH01500460A (en) | Improved probe for hybrid analytical test equipment | |
| JPH0587780A (en) | Method and apparatus for nondestructive inspection of metal pipes | |
| JP4117366B2 (en) | Electromagnetic ultrasonic flaw detection / measurement method and apparatus | |
| US7395715B2 (en) | Electromagnetic ultrasound probe | |
| CN101231269B (en) | Electromagnetic ultrasonic transducer capable of charging or discharging magnetism for build-in permanent magnet as well as use method | |
| Legg et al. | Flaw detection in metals using electromagnetic sound generation | |
| JPS60111153A (en) | Electromagnetic ultrasonic measuring device | |
| Van den Berg et al. | Development of an electromagnetic acoustic transducer for inspecting the wall thickness of offshore risers from the inside | |
| JPS62277556A (en) | Electromagnetic ultrasonic probe | |
| JPS60188805A (en) | Electromagnetic ultrasonic measuring instrument | |
| US3624711A (en) | Material tester | |
| SU1437816A1 (en) | Method of measuring magnetostriction coefficient | |
| JPS636678Y2 (en) | ||
| JPS63259405A (en) | Magneto-ultrasonic measuring apparatus | |
| JPH0543062B2 (en) | ||
| JPS6333440Y2 (en) | ||
| Alers et al. | Electromagnetic acoustic transducer |