JPH0236117Y2 - - Google Patents

Info

Publication number
JPH0236117Y2
JPH0236117Y2 JP11254081U JP11254081U JPH0236117Y2 JP H0236117 Y2 JPH0236117 Y2 JP H0236117Y2 JP 11254081 U JP11254081 U JP 11254081U JP 11254081 U JP11254081 U JP 11254081U JP H0236117 Y2 JPH0236117 Y2 JP H0236117Y2
Authority
JP
Japan
Prior art keywords
ultrasonic
acoustic impedance
ultrasonic transducer
array probe
quartz plate
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
JP11254081U
Other languages
Japanese (ja)
Other versions
JPS5817550U (en
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 filed Critical
Priority to JP11254081U priority Critical patent/JPS5817550U/en
Publication of JPS5817550U publication Critical patent/JPS5817550U/en
Application granted granted Critical
Publication of JPH0236117Y2 publication Critical patent/JPH0236117Y2/ja
Granted legal-status Critical Current

Links

Landscapes

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

Description

【考案の詳細な説明】 この考案は、複数個の超音波振動子を配列して
構成する超音波アレイ探触子に関するものであ
る。
[Detailed Description of the Invention] This invention relates to an ultrasonic array probe configured by arranging a plurality of ultrasonic transducers.

従来のこの種の超音波アレイ探触子は、例え
ば、第1図に示すように、いわゆるバツキング材
と呼ばれる部材2の上に、直方体形状の複数個の
超音波振動子1を直線上に沿つて配列して構成し
ていた。図中、3,3′は超音波振動子1の電極
である。
A conventional ultrasonic array probe of this type, for example, as shown in FIG. It was constructed by arranging them. In the figure, 3 and 3' are electrodes of the ultrasonic transducer 1.

バツキング材2は、超音波振動子1から被検材
内へ放射される超音波パルスのパルス幅を短く
し、超音波アレイ探触子の距離分解能を向上させ
るために設けられているものであり、高い距離分
解能を得るには、バツキング材2の材料には、密
度と音速との積で与えられる音響インピーダンス
の値が、振動子の音響インピーダンスに近い値を
有することが要求される。さらに、バツキング材
2の材料には、超音波振動子1からバツキング材
2内へ放射された超音波パルスが、バツキング材
2の裏面4で反射され再び超音波振動子1に雑音
として受信されないようにするため、超音波の減
衰率が大きいことが要求される。これらの要求を
ほぼ満足する材料としては、従来、一般に、エポ
キシ樹脂などの高分子有機材料に金属粉末を混合
して製作した材料が用いられている。
The backing material 2 is provided to shorten the pulse width of the ultrasonic pulse emitted from the ultrasonic transducer 1 into the test material and improve the distance resolution of the ultrasonic array probe. In order to obtain high distance resolution, the material of the backing material 2 is required to have an acoustic impedance value given by the product of density and sound speed close to the acoustic impedance of the vibrator. Furthermore, the material of the bucking material 2 is designed to prevent the ultrasonic pulses emitted from the ultrasonic transducer 1 into the bucking material 2 from being reflected by the back surface 4 of the bucking material 2 and being received by the ultrasonic transducer 1 as noise again. Therefore, a high attenuation rate of ultrasonic waves is required. As a material that substantially satisfies these requirements, a material produced by mixing metal powder with a polymeric organic material such as an epoxy resin has conventionally been used.

ところで、この種の超音波アレイ探触子は、各
超音波振動子1の励振信号および受信信号の位相
をそれぞれ独立に電子的に制御し、各超音波振動
子1により送受信される超音波ビームの波面を合
成し、合成超音波ビームの指向方向を電子的に走
査する場合などに用いられるものであり、このと
き超音波振動子1相互間に電気的相互結合があれ
ば、合成超音波ビームのサイドローブレベルが大
きくなるなどの性能劣化を招くことが知られてい
る。
By the way, this type of ultrasonic array probe electronically controls the phases of the excitation signal and reception signal of each ultrasonic transducer 1 independently, and the ultrasonic beam transmitted and received by each ultrasonic transducer 1. It is used in cases where the wavefronts of It is known that this can lead to performance deterioration, such as an increase in the sidelobe level.

さて、従来のこの種の超音波アレイ探触子を用
いて、例えば金属などのように導電性を有する被
検材を検査する場合には、容易にわかるように、
各超音波振動子1の被検材側の各電極3を共通接
地し、各超音波振動子1からのリード線は、各超
音波振動子1のバツキング材2側の各電極3′か
ら取出す必要があるが、従来のこの種の超音波ア
レイ探触子においては、隣接する超音波振動子1
間の間隔を狭くすると、超音波振動子1の電極
3′が、金属粉末を混入して製作したバツキング
材2に直接接触していたため、隣接する超音波振
動子1の電極3′間の電気的抵抗値が小さくなり、
このため隣接する超音波振動子1間に電気的相互
結合が生じ、上述したような性能劣化を招く欠点
があつた。
As can be easily seen, when testing a conductive material such as metal using a conventional ultrasonic array probe of this type,
The electrodes 3 on the test material side of each ultrasonic vibrator 1 are commonly grounded, and the lead wires from each ultrasonic vibrator 1 are taken out from each electrode 3' on the backing material 2 side of each ultrasonic vibrator 1. However, in conventional ultrasonic array probes of this type, adjacent ultrasonic transducers 1
When the distance between the electrodes 3' of the ultrasonic transducers 1 was narrowed, the electrodes 3' of the ultrasonic transducers 1 were in direct contact with the backing material 2 made by mixing metal powder, so the electricity between the electrodes 3' of the adjacent ultrasonic transducers 1 was reduced. The resistance value becomes smaller,
As a result, electrical mutual coupling occurs between adjacent ultrasonic transducers 1, resulting in the drawback of deterioration of performance as described above.

この考案は、厚さが4分の1波長の石英板5の
一方の面上に複数個の超音波振動子1を直線上に
沿つて配列し、石英板5の他方の面上に超音波の
減衰率の大きい部材6を設け、上記部材6の音響
インピーダンスを、石英板5の音響インピーダン
スの2乗と超音波振動子1の音響インピーダンス
の比となるようにして超音波アレイ探触子を構成
することにより、上述したような欠点を解決しよ
うとするものであり、以下第2図に示す一実施例
を用いて詳細に説明する。
This idea involves arranging a plurality of ultrasonic transducers 1 along a straight line on one side of a quartz plate 5 with a thickness of 1/4 wavelength, and transmitting ultrasonic waves onto the other side of the quartz plate 5. A member 6 having a large attenuation rate is provided, and the acoustic impedance of the member 6 is set to be the ratio of the square of the acoustic impedance of the quartz plate 5 to the acoustic impedance of the ultrasonic transducer 1 to form an ultrasonic array probe. This configuration is intended to solve the above-mentioned drawbacks, and will be described in detail below using an embodiment shown in FIG.

第2図において、1は厚さが4分の1波長の石
英板5の一方の面上に、従来と同様に直線上に沿
つて配列した超音波振動子であり、3,3′は超
音波振動子1の電極である。
In FIG. 2, 1 is an ultrasonic transducer arranged along a straight line on one side of a quartz plate 5 with a thickness of 1/4 wavelength, as in the conventional case, and 3 and 3' are ultrasonic transducers. These are the electrodes of the acoustic wave vibrator 1.

6はタングステン粉末とエポキシ樹脂との混合材
からなる部材である。混合比を変化させて、音響
インピーダンスの変化の測定や、流動性について
実験したところ、音響インピーダンスが約7×
106Kg/m2/secとなる混合比の場合が、流動性も
良好に保たれ注入整形ができる利点もあり、か
つ、超音波減衰率も十分大きくとれることがわか
つた。超音波振動子1の音響インピーダンスは、
圧電セラミツクを用いる場合、約30×106Kg/
m2/secである。そこで、超音波振動子1と部材
6間には音響インピーダンスが約13×106Kg/
m2/secの石英板5を選んで組合せた。
6 is a member made of a mixed material of tungsten powder and epoxy resin. When we measured changes in acoustic impedance and experimented with fluidity by changing the mixing ratio, we found that the acoustic impedance was approximately 7×
It was found that a mixing ratio of 10 6 Kg/m 2 /sec has the advantage of maintaining good fluidity and allowing injection shaping, and also provides a sufficiently high ultrasonic attenuation rate. The acoustic impedance of the ultrasonic transducer 1 is
When using piezoelectric ceramic, approximately 30×10 6 Kg/
m 2 /sec. Therefore, the acoustic impedance between the ultrasonic transducer 1 and the member 6 is approximately 13×10 6 Kg/
A quartz plate 5 of m 2 /sec was selected and combined.

すなわち、部材6の音響インピーダンスは、近
似的に石英板5の音響インピーダンスの2乗と超
音波振動子1の音響インピーダンスとの比となつ
ている。
That is, the acoustic impedance of the member 6 is approximately the ratio of the square of the acoustic impedance of the quartz plate 5 to the acoustic impedance of the ultrasonic transducer 1.

さて、第2図に示すこの考案に係る超音波アレ
イ探触子では、石英板5が、厚さが4分の1波長
で、かつ、音響インピーダンスの値が超音波振動
子1の音響インピーダンスの値と上記超音波の減
衰率の大きい部材6の音響インピーダンスの値と
の積の平方根で与えられるので、超音波振動子1
から上記超音波の減衰率の大きい部材6を見込ん
だ音響インピーダンスの値は、超音波振動子1の
音響インピーダンスの値と等しく、このため、従
来と同等の距離分解能を得ることができる。
Now, in the ultrasonic array probe according to this invention shown in FIG. Since it is given by the square root of the product of the value and the value of the acoustic impedance of the member 6 with a large attenuation rate of the ultrasonic waves, the ultrasonic transducer 1
The value of the acoustic impedance considering the member 6 having a large attenuation rate of ultrasonic waves is equal to the value of the acoustic impedance of the ultrasonic transducer 1, and therefore it is possible to obtain a distance resolution equivalent to that of the conventional method.

また、超音波振動子1から石英板5を通過して
上記部材6に放射された超音波パルスは、部材6
の材料として、超音波の減衰率が従来と同等に大
きいものを用いているため、部材6の裏面4で反
射され再び超音波振動子1に、少なくとも従来よ
り大きなレベルで雑音として受信されることはな
い。
Further, the ultrasonic pulses emitted from the ultrasonic transducer 1 to the member 6 through the quartz plate 5 are transmitted to the member 6.
Since a material with a high ultrasonic attenuation rate equivalent to that of conventional materials is used for the There isn't.

しかし、この考案に係る超音波アレイ探触子を
用いて、従来と同様に、各超音波振動子1の被検
材側の各電極3を共通接地し、他方の各電極3′
からリード線を取り出して、金属などの導電性を
有する被検材を検査する場合には、従来とは異な
り、隣接する超音波振動子1間の間隔を狭くして
も、電極3′が接触している面が電気的絶縁体で
ある石英板5であるため、隣接する超音波振動子
1間に電気的相互結合が生じることはない。した
がつて前記したような性能劣化を招かないという
利点がある。
However, using the ultrasonic array probe according to this invention, each electrode 3 on the specimen side of each ultrasonic transducer 1 is commonly grounded, and each electrode 3' of the other ultrasonic transducer 1 is
When inspecting a conductive material such as a metal by taking out a lead wire from the Since the quartz plate 5 is an electrical insulator, electrical mutual coupling does not occur between adjacent ultrasonic transducers 1. Therefore, there is an advantage that the above-mentioned performance deterioration does not occur.

なお、この考案はこれに限らず、被検材と超音
波振動子1との間に、厚さが4分の1波長の1層
あるいは多層の音響インピーダンス変成層を設け
た超音波アレイ探触子の場合についても同様に使
用してもよい。
Note that this invention is not limited to this, but is also applicable to ultrasonic array probes in which one or multiple layers of acoustic impedance modification layers with a thickness of 1/4 wavelength are provided between the test material and the ultrasonic transducer 1. It may be used in the same way for children.

以上のように、この考案に係る超音波アレイ探
触子では、厚さが4分の1波長の石英板5の一方
の面上に、複数個の超音波振動子1を直線上に沿
つて配列し、石英板5の他方の面上に超音波の減
衰率の大きい部材6を設け、部材6の音響インピ
ーダンスを、石英板5の音響インピーダンスの2
乗と超音波振動子1の音響インピーダンスの比と
なるように構成したことにより、隣接する超音波
振動子1間の間隔を狭くしても、隣接する超音波
振動子1間の電気的相互結合を生じず、このた
め、前記したような性能劣化を招かないという利
点がある。
As described above, in the ultrasonic array probe according to this invention, a plurality of ultrasonic transducers 1 are arranged in a straight line on one side of the quartz plate 5 having a thickness of 1/4 wavelength. A member 6 with a large attenuation rate of ultrasonic waves is provided on the other surface of the quartz plate 5, and the acoustic impedance of the member 6 is set to 2 of the acoustic impedance of the quartz plate 5.
By configuring the ratio of the acoustic impedance of the ultrasonic transducers 1 to Therefore, there is an advantage that the above-mentioned performance deterioration does not occur.

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

第1図は従来の超音波アレイ探触子の構成図、
第2図はこの考案に係る超音波アレイ探触子の構
成図である。図中、1は超音波振動子、2は従来
のバツキング材、3,3′は超音波振動子1の電
極、5は石英板、6はタングステン粉末とエポキ
シ樹脂との混合材からなる部材である。なお、図
中同一あるいは相当部分には同一符号を付して示
してある。
Figure 1 is a configuration diagram of a conventional ultrasonic array probe.
FIG. 2 is a configuration diagram of the ultrasonic array probe according to this invention. In the figure, 1 is an ultrasonic vibrator, 2 is a conventional backing material, 3 and 3' are electrodes of the ultrasonic vibrator 1, 5 is a quartz plate, and 6 is a member made of a mixed material of tungsten powder and epoxy resin. be. It should be noted that the same or corresponding parts in the figures are indicated by the same reference numerals.

Claims (1)

【実用新案登録請求の範囲】[Scope of utility model registration request] 厚さが4分の1波長の電気的絶縁板の一方の面
上に、複数個の超音波振動子を直線上に沿つて配
列し、上記電気的絶縁板の他方の面上には金属粉
末とエポキシ樹脂との混合材からなる部材を設
け、上記混合材からなる部材の音響インピーダン
スを、上記電気的絶縁板の音響インピーダンスの
2乗と上記超音波振動子の音響インピーダンスと
の比となるようにしたことを特徴とする超音波ア
レイ探触子。
A plurality of ultrasonic transducers are arranged in a straight line on one side of an electrically insulating plate with a thickness of 1/4 wavelength, and metal powder is arranged on the other side of the electrically insulating plate. and an epoxy resin, and the acoustic impedance of the member made of the mixed material is a ratio of the square of the acoustic impedance of the electrically insulating plate and the acoustic impedance of the ultrasonic transducer. An ultrasonic array probe characterized by:
JP11254081U 1981-07-29 1981-07-29 Ultrasonic array probe Granted JPS5817550U (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP11254081U JPS5817550U (en) 1981-07-29 1981-07-29 Ultrasonic array probe

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP11254081U JPS5817550U (en) 1981-07-29 1981-07-29 Ultrasonic array probe

Publications (2)

Publication Number Publication Date
JPS5817550U JPS5817550U (en) 1983-02-03
JPH0236117Y2 true JPH0236117Y2 (en) 1990-10-02

Family

ID=29906865

Family Applications (1)

Application Number Title Priority Date Filing Date
JP11254081U Granted JPS5817550U (en) 1981-07-29 1981-07-29 Ultrasonic array probe

Country Status (1)

Country Link
JP (1) JPS5817550U (en)

Also Published As

Publication number Publication date
JPS5817550U (en) 1983-02-03

Similar Documents

Publication Publication Date Title
US5099459A (en) Phased array ultrosonic transducer including different sized phezoelectric segments
US4550606A (en) Ultrasonic transducer array with controlled excitation pattern
US4398325A (en) Process for producing ultrasonic transducers having complex shapes
EP0294826B1 (en) Ultrasonic transducer structure
US4217516A (en) Probe for ultrasonic diagnostic apparatus
JPS5977799A (en) Apodictic supersonic transducer
JPS61110050A (en) Ultrasonic probe
JPS605133A (en) Ultrasonic converter improved in vibration mode
WO1993011528A1 (en) Acoustic non-destructive testing
US2946904A (en) Ultrasonic transducer arrangement for sending and receiving
US4467237A (en) Multielement ultrasonic probe and its production process
Powell et al. Flexible ultrasonic transducer arrays for nondestructive evaluation applications. II. Performance assessment of different array configurations
US4414482A (en) Non-resonant ultrasonic transducer array for a phased array imaging system using1/4 λ piezo elements
JPH0236117Y2 (en)
JPS5768999A (en) Ultrasonic wave probe
JPS5929816B2 (en) ultrasonic probe
JPH0349389B2 (en)
JPS63159750A (en) Array type ultrasonic probe
JPS5991797A (en) Ultrasonic wave probe
JPS59178378A (en) Ultrasonic probe
DeSilets et al. Highly efficient transducer arrays useful in nondestructive testing applications
JPS5944051B2 (en) ultrasonic probe
Erhard et al. Calculation and construction of phased array-UT probes
JPH0534880B2 (en)
JPH02271845A (en) Ultrasonic diagnostic device