JPH0675062B2 - Ultrasonic probe device - Google Patents

Ultrasonic probe device

Info

Publication number
JPH0675062B2
JPH0675062B2 JP19521688A JP19521688A JPH0675062B2 JP H0675062 B2 JPH0675062 B2 JP H0675062B2 JP 19521688 A JP19521688 A JP 19521688A JP 19521688 A JP19521688 A JP 19521688A JP H0675062 B2 JPH0675062 B2 JP H0675062B2
Authority
JP
Japan
Prior art keywords
ultrasonic probe
ultrasonic
test material
wave
convex
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 - Fee Related
Application number
JP19521688A
Other languages
Japanese (ja)
Other versions
JPH0244246A (en
Inventor
洋次 田中
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 JP19521688A priority Critical patent/JPH0675062B2/en
Publication of JPH0244246A publication Critical patent/JPH0244246A/en
Publication of JPH0675062B2 publication Critical patent/JPH0675062B2/en
Anticipated expiration legal-status Critical
Expired - Fee Related legal-status Critical Current

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Classifications

    • GPHYSICS
    • G01MEASURING; TESTING
    • G01NINVESTIGATING OR ANALYSING MATERIALS BY DETERMINING THEIR CHEMICAL OR PHYSICAL PROPERTIES
    • G01N2291/00Indexing codes associated with group G01N29/00
    • G01N2291/04Wave modes and trajectories
    • G01N2291/044Internal reflections (echoes), e.g. on walls or defects

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

Description

【発明の詳細な説明】 〔産業上の利用分野〕 この発明は例えばパルス反射法を利用し,水浸法により
被検材の垂直探傷を行う超音波探触子装置に関するもの
である。
Description: TECHNICAL FIELD The present invention relates to an ultrasonic probe device for performing vertical flaw detection on a material to be inspected by a water immersion method using, for example, a pulse reflection method.

〔従来の技術〕[Conventional technology]

第4図は例えば超音波探傷法(昭和49年日刊工業新聞社
発行)に示された従来の超音波探触子装置の図である。
図において,(1)は被検材,(2)は音響放射面及び
振動子とも平坦な超音波探触子,(3)は音響結合材
(例えば水),(4)は被検材(1)内部の欠陥,
(5)は超音波ビームであり、Sは被検材(1)の表面
反射波,Fは被検材(1)内部の欠陥反射波,Bは被検材
(1)の底面反射波である。又,第5図は従来の超音波
探触子装置による探傷図形である。図において(7)は
被険材(1)を探傷する探傷ゲート、T1は第1回目の送
信パルス,T2は第2回目の送信パルス,Tnは第n回目の
送信パルス,は送信パルスの繰り返し時間,S1は送信パ
ルスT1に対する被検材(1)の第1回目の表面反射波
で、以下S2,S3,S4,S5,……Snはそれぞれ第2回目,第3
回目,第4回目,第5回目,……第n回目の表面反射
波,B1‐S1は表面反射波S1に対する被検材(1)の第1
回目の底面反射波で,以下B2‐S1……Bn-S1は表面反射
波S1に対する被検材(1)の第2回目……第n回目の底
面反射波,B1‐S2,B2‐S2,……Bn-S2,B1‐S3……Bn-
S3,B1‐S4……Bn-S4,Bn-S5……Bn-Snはそれぞれ第n回
目の表面反射波Snに対する被検材(1)の第n回目の底
面反射波,Fは第1回目の表面反射波S1に対する被検材
(1)の内部の欠陥反射波,F′は第2回目の表面反射波
S2に対する被検材(1)の内部の欠陥反射波である。図
に示すように第1回目の送信パルスT1において被検材
(1)の表面反射波の多重エコー(S1,S2……Sn),及
び被検材(1)内部の欠陥反射波(F,F′)及びそれぞ
れの表面反射波(S1,S2,……Sn)に対する被検材
(1)の底面反射波の多重エコー(B1‐S1,B2‐S1,…
…Bn-Sn)など数多くの反射波が現われる。又,上記多
重エコー(S1……Sn,B1‐S1……Bn-Sn)が送信パルス
(T1,T2,……Tn)ごとに繰返し時間tの間隔で同じよ
うに現われる。
FIG. 4 is a diagram of a conventional ultrasonic probe apparatus shown in, for example, the ultrasonic flaw detection method (published by Nikkan Kogyo Shimbun, 1974).
In the figure, (1) is the material to be tested, (2) is an ultrasonic probe whose acoustic radiation surface and transducer are flat, (3) is an acoustic coupling material (for example, water), and (4) is the material to be tested ( 1) Internal defects,
(5) is an ultrasonic beam, S is a surface reflection wave of the test material (1), F is a defect reflection wave inside the test material (1), and B is a bottom reflection wave of the test material (1). is there. Further, FIG. 5 is a flaw detection figure by the conventional ultrasonic probe device. In the figure, (7) is a flaw detection gate for flaw detection on the material (1), T 1 is the first transmission pulse, T 2 is the second transmission pulse, Tn is the nth transmission pulse, and is the transmission pulse. , S 1 is the first surface reflection wave of the test material (1) with respect to the transmission pulse T 1 , and the following S 2 , S 3 , S 4 , S 5 , ... Sn are respectively the second time, Third
The 4th time, 4th time, 5th time, ... The nth surface reflected wave, B 1 -S 1 is the first of the test material (1) for the surface reflected wave S 1.
B 2 -S 1 …… Bn-S 1 is the second bottom reflected wave of the test material (1) against the surface reflected wave S 1 …… the nth bottom reflected wave, B 1 -S 2 , B 2 ‐S 2 …… Bn-S 2 , B 1 ‐S 3 …… Bn-
S 3 , B 1 -S 4 ...... Bn-S 4 , Bn-S 5 ...... Bn-Sn are the nth bottom reflected waves of the test material (1) with respect to the nth surface reflected wave Sn, respectively. F is the defect reflection wave inside the test material (1) with respect to the first surface reflection wave S 1 , and F ′ is the second surface reflection wave.
It is a defect reflected wave inside the test material (1) with respect to S 2 . As shown in the figure, in the first transmission pulse T 1 , multiple echoes (S 1 , S 2 ... Sn) of the surface reflection wave of the test material (1) and the defect reflection wave inside the test material (1) Multiple echoes (B 1 -S 1 , B 2 -S 1 , of the bottom reflected waves of the test material (1) for (F, F ′) and the respective surface reflected waves (S 1 , S 2 , ... Sn) …
… Bn-Sn) and many other reflected waves appear. The multiple echoes (S 1 ... Sn, B 1- S 1 ... Bn-Sn) appear in the same manner at intervals of the repetition time t for each transmission pulse (T 1 , T 2 , ... Tn).

従来の超音波探触子装置は上記のように構成され,自動
化する場合に送信パルスTを繰り返し送信し,被検材
(1)あるいは超音波探触子(2)を操作することによ
り被検材(1)の全面にわたり超音波探傷を行ってい
る。又,被検材(1)と,超音波探触子(2)との相対
的な移動速度に応じて,送信パルスTの繰り返し時間t
が決定されている。すなわち,被検材(1)の探傷処理
能力をくする場合には,送信パルスTの繰り返し時間
tを短かくしなければならないため,第1回目の送信パ
ルスT1で生じた表面反射波S1からSn,及び底面反射波B1
‐S1からBn-Snが完全に消滅しないうちに第2回目以降
の送信パルスT2からTnを送信する必要が生じその場合に
は,第1回目の送信パルスT1による表面反射波S1と底面
反射波B1‐S1との間に残響エコーとして,第2回目以降
の送信パルスT2からTnによる表面反射波Sn及び底面反射
波Sn-Bnが現われる。このため,上記表面反射波Sn及び
底面反射波Sn-Bnを欠陥反射波Fとして誤って検出する
ことになる。
The conventional ultrasonic probe device is configured as described above, and when it is automated, repeatedly transmits the transmission pulse T and operates the test material (1) or the ultrasonic probe (2) to perform the test. Ultrasonic flaw detection is performed on the entire surface of the material (1). In addition, the repetition time t of the transmission pulse T depends on the relative moving speed of the test material (1) and the ultrasonic probe (2).
Has been decided. That is, in order to reduce the flaw detection processing capability of the test material (1), it is necessary to shorten the repetition time t of the transmission pulse T, so that the surface reflected wave S 1 generated by the first transmission pulse T 1 is generated. To Sn, and the bottom reflected wave B 1
-S 1 to Bn-It is necessary to transmit the transmission pulses T 2 to Tn from the second time onward before Bn-Sn is completely extinguished. In that case, the surface reflection wave S 1 from the transmission pulse T 1 from the first time is transmitted. As the reverberation echo between the bottom surface reflected wave B 1 and the bottom reflected wave B 1 -S 1 , the surface reflected wave Sn and the bottom reflected wave Sn-Bn due to the transmission pulses T 2 to Tn after the second time appear. Therefore, the surface reflected wave Sn and the bottom surface reflected wave Sn-Bn are erroneously detected as the defect reflected wave F.

〔発明が解決しようとする課題〕[Problems to be Solved by the Invention]

上記のように被検材(1)と振動子及び音響放射面が平
坦な超音波探触子(2)との間に音響結合材(3)であ
る水しかない超音波探触子装置では被検材(1)表面で
の反射波Sは約95%反射し,超音波探触子(2)の表面
では約60%反射するため超音波探触子(2)と被検材
(1)との間を1往復する毎に約5〜6dB程度しか減衰
しない。このため通常要求される欠陥検出能(例えばφ
1横穴欠陥をS/N≧20dB)から第1回目の表面反射波S1
対する残響エコーSn,Bn-Snの低下量を求めると−60dB以
下とする必要がある。すなわち超音波探触子(2)と被
検材(1)との間の距離を10〜12回往復するまでの時間
が経過しないうちに第2回目の送信パルスT2を発生させ
ると残響エコーとしてSn,Bn-Snが疑似エコーFとして現
われる問題が生じる。特にこの問題は,探傷処理速度の
速い自動探傷装置においては致命的な欠点となる。
As described above, in the ultrasonic probe device having only the water which is the acoustic coupling material (3) between the test material (1) and the ultrasonic probe (2) having a flat transducer and acoustic emission surface, The reflected wave S on the surface of the test material (1) is reflected by about 95% and is reflected by about 60% on the surface of the ultrasonic probe (2), so the ultrasonic probe (2) and the test material (1 ) Attenuates only about 5 to 6 dB for each round trip. Therefore, the defect detectability normally required (for example, φ
When the reduction amount of the reverberation echo Sn, Bn-Sn with respect to the first surface reflected wave S 1 is calculated from 1 lateral hole defect S / N ≧ 20 dB), it is necessary to be -60 dB or less. That is, if the second transmission pulse T 2 is generated before the time elapsing 10 to 12 times the distance between the ultrasonic probe (2) and the test material (1) elapses, the reverberation echo is generated. As a result, there arises a problem that Sn and Bn-Sn appear as pseudo echo F. In particular, this problem is a fatal drawback in an automatic flaw detection device with a high flaw detection processing speed.

この発明は,かかる問題点を解決するためになされたも
ので,凸形状の振動子を有し,かつ音響放射面が凸形状
をした超音波探触子を備え,さらに被検材と超音波探触
子との間の音響結合材の部分に,厚みが均一なアクリル
樹脂製のしきり板を超音波ビームの進行方向に対して35
°〜55°の角度範囲内で具備させることにより,残響エ
コーを防止し送信パルスの繰り返し時間を短かくするこ
とを目的とする。
The present invention has been made to solve the above problems, and has an ultrasonic probe having a convex vibrator and a convex acoustic emission surface, and further includes a test material and an ultrasonic wave. An acrylic resin divider plate with a uniform thickness is placed in the acoustic coupling part between the probe and the ultrasonic beam direction.
The purpose is to prevent reverberation echo and shorten the repetition time of the transmission pulse by providing the angle within the range of ° to 55 °.

〔課題を解決するための手段〕[Means for Solving the Problems]

この発明による超音波探触子装置は,振動子と音響放射
面とが凸形状をした超音波探触子を備え,さらに被検材
と超音波探触子との間の音響結合材の部分に厚みが均一
なアクリル樹脂製のしきり板を超音波ビームの進行方向
に対して35°〜55°の角度範囲内で具備したものであ
る。
An ultrasonic probe device according to the present invention includes an ultrasonic probe in which a transducer and an acoustic radiation surface have a convex shape, and a portion of an acoustic coupling material between a test material and the ultrasonic probe. In addition, a threshold plate made of acrylic resin having a uniform thickness is provided within an angle range of 35 ° to 55 ° with respect to the traveling direction of the ultrasonic beam.

〔作用〕[Action]

この発明においては,被検材と超音波探触子との間の音
響結合材の部分に厚みが均一なアクリル樹脂製のしきり
板を超音波ビームの進行方向に対して35°〜55°の角度
範囲内で具備することと超音波探触子の音響放射面及び
振動子の形状を凸形にすることにより,超音波探触子と
被検材との間を1往復する超音波の総合減衰量を増加さ
せ,送信パルスの繰り返し時間を短かくすることを可能
とするものである。
In the present invention, an acrylic resin partition plate having a uniform thickness is provided at a portion of the acoustic coupling material between the test material and the ultrasonic probe at 35 ° to 55 ° with respect to the traveling direction of the ultrasonic beam. By providing the ultrasonic probe within the angular range and by making the acoustic emission surface of the ultrasonic probe and the shape of the transducer convex, the total number of ultrasonic waves reciprocating once between the ultrasonic probe and the test material It is possible to increase the amount of attenuation and shorten the transmission pulse repetition time.

〔実施例〕〔Example〕

第1図は,この発明の一実施例を示す図であり,(1)
と(3)〜(5)は第4図に示した従来の装置と全く同
一のものである。図において,(6)はこの発明である
アクリル樹脂製のしきり板,(8)は凸形振動子,
(9)は凸形振動子(8)を有し,かつ音響放射面が凸
形状した超音波探触子である。
FIG. 1 is a diagram showing an embodiment of the present invention. (1)
And (3) to (5) are exactly the same as the conventional device shown in FIG. In the figure, (6) is a separator plate made of acrylic resin according to the present invention, (8) is a convex vibrator,
Reference numeral (9) is an ultrasonic probe having a convex oscillator (8) and having a convex sound emitting surface.

第2図は,第1図におけるしきり板(6)付近の拡大図
である。図において,X1はしきり板(6)を透過する前
の超音波ビーム,X2はしきり板(6)を透過後の超音波
ビーム,X3は超音波ビームX1がしきり板(6)表面によ
り反射される超音波ビーム,y1はしきり板(6)内部を
通過する横波超音波ビーム,αは超音波ビームX1のしき
り板(6)への入射角,βはしきり板(6)内部での屈
折角,θはしきり板(6)と超音波ビーム(5)とのな
す角である。
FIG. 2 is an enlarged view of the vicinity of the plate (6) in FIG. In the figure, X 1 is the ultrasonic beam before passing through the plate (6), X 2 is the ultrasonic beam after passing through the plate (6), X 3 is the ultrasonic beam X 1 is the plate (6) The ultrasonic beam reflected by the surface, y 1 is a transverse ultrasonic wave passing through the inside of the plate (6), α is the incident angle of the ultrasonic beam X 1 to the plate (6), β is the plate (6) ) Internal refraction angle, θ is an angle formed by the plate (6) and the ultrasonic beam (5).

第3図は上記のように構成された超音波探触子装置にお
いて,パルス反射法を利用し水浸法により被検材(1)
の垂直探傷を行った場合の探傷図形である。図において
(7)及び図における記号(S1,S2,S1‐S2……)は第5
図に示したものと全く同一のものである。
FIG. 3 shows the ultrasonic probe apparatus configured as described above, which is used for the test material (1) by the water immersion method using the pulse reflection method.
It is a flaw detection figure when vertical flaw detection is performed. In the figure, (7) and the symbols (S 1 , S 2 , S 1 -S 2 ...) in the figure are the fifth
It is exactly the same as that shown in the figure.

上記のように構成された超音波探触子装置において,被
検材(1)と超音波探触子(9)との間の音響結合材
(3)の部分に厚みが均一なアクリル樹脂製のしきり板
(6)を超音波ビーム(5)の進行方向に対してθ=35
°〜55°角度範囲内で具備した場合,超音波探触子
(9)より発生された超音波ビーム(5)はx1,x2,x3,y
1とに区別することができる。ここで水の音速C,アクリ
ル樹脂の横波音速Csとすると,α,β,θとの間に
(1),(2)式が成り立つ。
In the ultrasonic probe device configured as described above, the portion of the acoustic coupling material (3) between the test material (1) and the ultrasonic probe (9) is made of acrylic resin having a uniform thickness. Θ = 35 with respect to the traveling direction of ultrasonic beam (5)
If it is installed within the angle range of 55 ° to 55 °, the ultrasonic beam (5) generated from the ultrasonic probe (9) is x 1 , x 2 , x 3 , y
It can be distinguished as 1 . Here, assuming that the sound velocity of water is C and the transverse wave acoustic velocity of acrylic resin is Cs, equations (1) and (2) hold between α, β, and θ.

ここで,水の音速:C≒1480m/s(20℃) アクリル樹脂の横波音速 ≒1420m/s とすると(1)式は3式となる。 Here, if the sound velocity of water: C ≈ 1480 m / s (20 ° C) and the shear wave velocity of acrylic resin ≈ 1420 m / s, equation (1) becomes three equations.

sinα≒sinβ …………(3) (3)式より超音波ビームはx1→y1とほぼ直線的に進む
ことになる。
sin α ≒ sin β ………… (3) From the equation (3), the ultrasonic beam travels almost linearly as x 1 → y 1 .

次に,しきり板(6)における反射特であるx3のレベル
については,水の音響インピーダンスをz1,アクリル樹
脂の横波の音響インピーダンスをz2とすると(4)式に
より反射率γが求められる。
Next, regarding the level of x 3 which is the reflection characteristic in the plate (6), the reflectance γ is calculated by Eq. (4), where z 1 is the acoustic impedance of water and z 2 is the transverse impedance of acrylic resin. To be

ただし, ここで、CDはアクリル樹脂(6)中の縦波音速,ρ1
音響結合材(3)の密度,ρ2はアクリル樹脂(6)の
密度,γはアクリル樹脂(6)中の縦波屈折角である。
However, Here, C D is the longitudinal wave sound velocity in the acrylic resin (6), ρ 1 is the density of the acoustic coupling material (3), ρ 2 is the density of the acrylic resin (6), and γ is the longitudinal direction in the acrylic resin (6). Wave refraction angle.

(2)式と(4)式によりx3の反射率γはθ=35°〜55
°の角度範囲内とすると約10%以下となる。つまり超音
波ビームx1の90%以上が超音波ビームy1となって進行し
ていく。又,しきり板(6)は厚みが均一なことによ
り,超音波ビームy1とx2との関係も上記と同一となる。
From the expressions (2) and (4), the reflectance γ of x 3 is θ = 35 ° to 55
Within the angle range of °, it is about 10% or less. That is, 90% or more of the ultrasonic beam x 1 travels as the ultrasonic beam y 1 . Further, since the thickness of the dividing plate (6) is uniform, the relationship between the ultrasonic beams y 1 and x 2 is the same as above.

次に超音波ビームの減衰について記載する。しきり板
(6)内部の超音波ビームy1はアクリル材内の横波によ
り超音波が伝播している。このため水中を伝播する超音
波の減衰とアクリル材内の横波により伝播する超音波の
減衰とを比較すると約15倍,アクリル材内を伝播する場
合の方が減衰が大きくなる。
Next, the attenuation of the ultrasonic beam will be described. The ultrasonic beam y 1 inside the divider plate (6) is propagated by the transverse wave in the acrylic material. Therefore, comparing the attenuation of ultrasonic waves propagating in water with the attenuation of ultrasonic waves propagating by transverse waves in acrylic material is about 15 times, and the attenuation is greater when propagating in acrylic material.

上記の説明により被検材(1)と超音波探触子(9)と
の間の音響結合材(3)の部分に厚み均一なアクリル板
を超音波ビーム(5)の進行方向に対して,θ=35°〜
55°の角度範囲内で具備したしきり板(6)により以下
のことが可能になる。
According to the above description, an acrylic plate having a uniform thickness is provided in the acoustic coupling material (3) between the test material (1) and the ultrasonic probe (9) in the traveling direction of the ultrasonic beam (5). , Θ = 35 ° ~
The siding plate (6) provided within an angle range of 55 ° makes it possible to:

(I)超音波ビーム(5)の進行方向は変化しない。(I) The traveling direction of the ultrasonic beam (5) does not change.

(II)しきり板(6)を一回通過するたびに音圧レベル
を約5〜10dB程度低下させることが可能となる。
(II) It is possible to reduce the sound pressure level by about 5 to 10 dB each time the plate (6) is passed.

また,振動子(8)の形状を凸形とし,さらに音響放射
面を凸形にすることにより超音波探触子(9)と被検材
(1)との間を1往復するたびに約10dB音圧レベルを低
下させることが可能となる。
In addition, by making the shape of the transducer (8) convex and further making the acoustic radiation surface convex, about one reciprocation between the ultrasonic probe (9) and the test material (1) It is possible to reduce the sound pressure level by 10 dB.

上記よりこの発明は第3図に示すように第1回目の送信
パルスT1による被検材(1)の反射波の多重エコーの数
を減少させ,送信パルスTの繰り返し時間tを短かくす
ることを可能とした。
From the above, according to the present invention, as shown in FIG. 3, the number of multiple echoes of the reflected wave of the material (1) to be inspected by the first transmission pulse T 1 is reduced and the repetition time t of the transmission pulse T is shortened. Made it possible.

尚,本実施例はアクリル樹脂製のしきり板の例で示した
が、音響結合材の音速とほぼ同じ横波音速をもつプラス
チック,ゴム材料等でも角度の条件は若干異なるが同様
の効果が得られるので本発明の適用はまぬがれない。
Although the present embodiment has been described by using the example of the acrylic resin plate, the same effect can be obtained even if the angle condition is slightly different even if the acoustic wave velocity of the acoustic coupling material is the same as that of a plastic or rubber material. Therefore, the application of the present invention is unavoidable.

〔発明の効果〕〔The invention's effect〕

この発明は以上説明したとおり,被検材と超音波探触子
との間の音響結合材の部分に厚みが均一でかつ横波音速
が音響結合材の音速とほぼ同じしきり板を超音波ビーム
の進行方向に対して35°〜55°の角度範囲内で具備する
ことと超音波探触子の音響放射面及び振動子の形状を凸
形にすることにより送信パルスの繰り返し時間を短かく
することを可能とし,超音波探傷装置の自動化におい
て,被検材に対する処理時間の短縮,及び探傷密度を増
加させ,速度探傷及び密度探傷を可能とする効果が
ある。
As described above, according to the present invention, a portion of the acoustic coupling material between the test material and the ultrasonic probe has a uniform thickness and a transverse wave sound velocity is approximately the same as the sound velocity of the acoustic coupling material. To reduce the repetition time of the transmission pulse by providing it within the angle range of 35 ° to 55 ° with respect to the traveling direction and by making the acoustic emission surface of the ultrasonic probe and the shape of the transducer convex. In the automation of the ultrasonic flaw detector, there is an effect that the treatment time for the material to be inspected is shortened and the flaw detection density is increased to enable the velocity flaw detection and the density flaw detection.

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

第1図はこの発明の一実施例を示す図,第2図は第1図
の部分的拡大図,第3図はこの発明における探傷図形,
第4図は従来の超音波探触子装置を示す図,第5図は従
来の超音波探触子装置における探傷図形である。 図において,(1)は被検材,(2)は超音波探触子,
(3)は音響結合材,(4)は被検材内部の欠陥,
(5)は超音波ビーム,(6)はしきり板,(7)は探
傷ゲート,(8)は凸形振動子,(9)は音響放射面を
凸形にした超音波探触子である。 なお,各図中同一符号は同一または相当部分を示す。
FIG. 1 is a view showing an embodiment of the present invention, FIG. 2 is a partially enlarged view of FIG. 1, and FIG. 3 is a flaw detection figure in the present invention.
FIG. 4 is a diagram showing a conventional ultrasonic probe device, and FIG. 5 is a flaw detection figure in the conventional ultrasonic probe device. In the figure, (1) is the test material, (2) is the ultrasonic probe,
(3) is an acoustic coupling material, (4) is a defect inside the test material,
(5) is an ultrasonic beam, (6) is a plate, (7) is a flaw detection gate, (8) is a convex transducer, and (9) is an ultrasonic probe with a convex acoustic emission surface. . The same reference numerals in each figure indicate the same or corresponding parts.

Claims (1)

【特許請求の範囲】[Claims] 【請求項1】超音波探触子と被検材との間に距離空間を
設け、上記空間部分に水、油等の音響結合材を満たした
水浸法の超音波探触子装置において、超音波が拡散する
凸形状の振動子を有し、かつ音響放射面が凸形状をした
超音波探触子と、上記超音波探触子と被検材間の超音波
伝播経路上に厚みが均一で、かつ横波音速が上記音響結
合部材の音速とほぼ同じしきり板を超音速ビームの進行
方向に対して35°〜55°の角度範囲内で具備させたこと
を特徴とする超音波探触子装置。
1. An ultrasonic probe apparatus of a water immersion method in which a distance space is provided between an ultrasonic probe and a test material, and the space portion is filled with an acoustic coupling material such as water or oil, An ultrasonic probe having a convex vibrator in which ultrasonic waves are diffused and having a convex acoustic emission surface, and a thickness on the ultrasonic propagation path between the ultrasonic probe and the test material is An ultrasonic probe characterized in that a threshold plate, which is uniform and has a transverse sound velocity substantially equal to that of the acoustic coupling member, is provided within an angle range of 35 ° to 55 ° with respect to the traveling direction of the supersonic beam. Child device.
JP19521688A 1988-08-04 1988-08-04 Ultrasonic probe device Expired - Fee Related JPH0675062B2 (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP19521688A JPH0675062B2 (en) 1988-08-04 1988-08-04 Ultrasonic probe device

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP19521688A JPH0675062B2 (en) 1988-08-04 1988-08-04 Ultrasonic probe device

Publications (2)

Publication Number Publication Date
JPH0244246A JPH0244246A (en) 1990-02-14
JPH0675062B2 true JPH0675062B2 (en) 1994-09-21

Family

ID=16337396

Family Applications (1)

Application Number Title Priority Date Filing Date
JP19521688A Expired - Fee Related JPH0675062B2 (en) 1988-08-04 1988-08-04 Ultrasonic probe device

Country Status (1)

Country Link
JP (1) JPH0675062B2 (en)

Families Citing this family (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
CN104502463B (en) * 2014-12-10 2018-05-25 北京工业大学 A kind of colloid couplant based on ultrasound detection
JP6177290B2 (en) * 2015-09-04 2017-08-09 菱電湘南エレクトロニクス株式会社 Ultrasonic flaw detection apparatus and ultrasonic flaw detection method

Also Published As

Publication number Publication date
JPH0244246A (en) 1990-02-14

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