JPH029520B2 - - Google Patents

Info

Publication number
JPH029520B2
JPH029520B2 JP5287783A JP5287783A JPH029520B2 JP H029520 B2 JPH029520 B2 JP H029520B2 JP 5287783 A JP5287783 A JP 5287783A JP 5287783 A JP5287783 A JP 5287783A JP H029520 B2 JPH029520 B2 JP H029520B2
Authority
JP
Japan
Prior art keywords
ultrasonic
acoustic radiation
ultrasonic probe
frequency characteristics
ultrasonic transducer
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
JP5287783A
Other languages
Japanese (ja)
Other versions
JPS59178096A (en
Inventor
Shuzo Wadaka
Koichiro Misu
Fumio Takeda
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 JP5287783A priority Critical patent/JPS59178096A/en
Publication of JPS59178096A publication Critical patent/JPS59178096A/en
Publication of JPH029520B2 publication Critical patent/JPH029520B2/ja
Granted legal-status Critical Current

Links

Classifications

    • BPERFORMING OPERATIONS; TRANSPORTING
    • B06GENERATING OR TRANSMITTING MECHANICAL VIBRATIONS IN GENERAL
    • B06BMETHODS OR APPARATUS FOR GENERATING OR TRANSMITTING MECHANICAL VIBRATIONS OF INFRASONIC, SONIC, OR ULTRASONIC FREQUENCY, e.g. FOR PERFORMING MECHANICAL WORK IN GENERAL
    • B06B1/00Methods or apparatus for generating mechanical vibrations of infrasonic, sonic, or ultrasonic frequency
    • B06B1/02Methods or apparatus for generating mechanical vibrations of infrasonic, sonic, or ultrasonic frequency making use of electrical energy
    • B06B1/06Methods or apparatus for generating mechanical vibrations of infrasonic, sonic, or ultrasonic frequency making use of electrical energy operating with piezoelectric effect or with electrostriction
    • B06B1/0607Methods or apparatus for generating mechanical vibrations of infrasonic, sonic, or ultrasonic frequency making use of electrical energy operating with piezoelectric effect or with electrostriction using multiple elements
    • B06B1/0611Methods or apparatus for generating mechanical vibrations of infrasonic, sonic, or ultrasonic frequency making use of electrical energy operating with piezoelectric effect or with electrostriction using multiple elements in a pile
    • B06B1/0614Methods or apparatus for generating mechanical vibrations of infrasonic, sonic, or ultrasonic frequency making use of electrical energy operating with piezoelectric effect or with electrostriction using multiple elements in a pile for generating several frequencies

Landscapes

  • Engineering & Computer Science (AREA)
  • Mechanical Engineering (AREA)
  • Investigating Or Analyzing Materials By The Use Of Ultrasonic Waves (AREA)
  • Ultra Sonic Daignosis Equipment (AREA)
  • Transducers For Ultrasonic Waves (AREA)

Description

【発明の詳細な説明】 この発明は、非破壊検査や医療診断に用いられ
る超音波探触子に関するものである。
DETAILED DESCRIPTION OF THE INVENTION The present invention relates to an ultrasonic probe used for nondestructive testing and medical diagnosis.

従来のこの種の超音波探触子は、例えば、第1
図に示すように、1個の超音波振動子1を用い、
超音波振動子1の一方の音響放射面2上にバツキ
ング材3を設け、他方の音響放射面2上に音響イ
ンピーダンス変成層4を設けて構成されていた。
5はリード線である。
Conventional ultrasonic probes of this type, for example,
As shown in the figure, using one ultrasonic transducer 1,
A backing material 3 was provided on one acoustic radiation surface 2 of the ultrasonic transducer 1, and an acoustic impedance modification layer 4 was provided on the other acoustic radiation surface 2.
5 is a lead wire.

非破壊検査や医療診断では、被検体の音響伝ぱ
ん特性が周波数依存性を有する場合がある。この
ような特性を有する被検体を検査する場合、送信
超音波パルスの周波数特性をあらかじめ測定して
おき、被検体内からの受信パルスの周波数特性を
解析し、両周波数特性の差異などを検出して、被
検体内部の情報を得る方法が適用されている。し
たがつて、送信超音波パルスの周波数特性を制御
できれば、より情報量が増える。
In nondestructive testing and medical diagnosis, the acoustic propagation characteristics of a subject may be frequency dependent. When inspecting a subject with such characteristics, the frequency characteristics of the transmitted ultrasonic pulses are measured in advance, the frequency characteristics of the received pulses from inside the subject are analyzed, and differences between the two frequency characteristics are detected. Therefore, methods for obtaining information inside the subject are being applied. Therefore, if the frequency characteristics of the transmitted ultrasonic pulse can be controlled, the amount of information can be further increased.

さて、上記送信超音波パルスの周波数特性は、
超音波探触子とこれを励振する電気回路との組合
せで決定される。しかし、通常、上記電気回路
は、出力インピーダンス50Ωのものが用いられ、
超音波探触子の励振波形はほとんどインパルスと
みなしてもよい、極めて幅の狭いパルスである。
したがつて、送信超音波パルスの周波数特性を変
えるには、超音波探触子の定数を変える必要があ
る。しかし、従来のこの種の超音波探触子は、上
述したように、1個の超音波振動子1、バツキン
グ材3および音響インピーダンス変成層4のみで
構成されていたため、制御できる上記定数の自由
度が小さく、このため、所要の周波数特性を実現
することが困難な場合があるなどの欠点があつ
た。
Now, the frequency characteristics of the above transmitted ultrasonic pulse are:
It is determined by the combination of the ultrasonic probe and the electric circuit that excites it. However, the above electric circuit usually has an output impedance of 50Ω,
The excitation waveform of an ultrasonic probe is an extremely narrow pulse that can almost be considered an impulse.
Therefore, in order to change the frequency characteristics of the transmitted ultrasound pulse, it is necessary to change the constants of the ultrasound probe. However, as mentioned above, the conventional ultrasonic probe of this type is composed of only one ultrasonic transducer 1, bucking material 3, and acoustic impedance transformation layer 4, so there is freedom in controlling the above-mentioned constants. The frequency is small, and this has the disadvantage that it is sometimes difficult to achieve the required frequency characteristics.

この発明は、音響放射面積の異なる複数個の超
音波振動子1を遅延材6をはさんで積層すること
により、上述したような欠点を解決したものであ
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 invention solves the above-mentioned drawbacks by stacking a plurality of ultrasonic transducers 1 with different acoustic radiation areas with a delay material 6 in between. This will be explained in detail using examples.

第2図は、この発明に係る超音波探触子の一実
施例を示したものであり、音響放射面積の異なる
複数個の超音波振動子1を、遅延材6をはさんで
積層して構成している。7は超音波伝ぱん媒体で
ある。5はリード線であり、第2図に示すよう
に、超音波振動子1が同時に励振されるように結
線している。
FIG. 2 shows an embodiment of the ultrasonic probe according to the present invention, in which a plurality of ultrasonic transducers 1 having different acoustic radiation areas are stacked with a delay material 6 in between. It consists of 7 is an ultrasonic propagation medium. 5 is a lead wire, and as shown in FIG. 2, it is connected so that the ultrasonic transducer 1 is excited at the same time.

さて、第2図に示す超音波探触子を、従来と同
様の電気回路でインパルス励振すると、音響放射
面積の大きい超音波振動子1では、振幅レベルの
大きい超音波パルスが励振され、音響放射面積の
小さい超音波振動子1では、振幅レベルの小さい
超音波パルスが励振される。これは超音波振動子
1の静電容量が音響放射面積に比例し、この種の
技術分野において一般的に知られているところで
あるが、音響放射抵抗は静電容量に反比例し、通
常、音響放射抵抗の値は数kΩ〜数十kΩ程度であ
る。従つて、音響放射面積が例えば2倍に大きく
なれば、音響放射抵抗は1/2に減少し、電気回路
の電源抵抗(通常数十〜数百Ω)とのマツチング
が完全と迄は行かないが、それ相応によくなるの
で、電源からの実効パワーの供給が増加し、つま
り、振幅レベルの大きい超音波パルスが励振され
る。さらに、各超音波振動子1により励振された
超音波が被検材表面へ到達する時間は、バツキン
グ材3に近い方に位置する超音波振動子1ほど遅
れる。したがつて、第2図に示す超音波探触子で
は、被検材へ送信される超音波パルスは、各超音
波振動子1により励振された超音波パルスを、上
述の振幅レベルおよび時間遅れを考慮して合成し
たものとなり、例えば第3図に示すような波形と
なる。図中第1番目のパルスは第2図中の下側の
超音波振動子で励振されたもの、第2番目のパル
スは第2図中の中央の超音波振動子で励振された
もの、第3番目のパルスは第2図中の上側の超音
波振動子で励振されたものに対応する。なお、こ
れらパルスの時間的関係は第2図中に示す遅延材
6による。また、第3図に示す波形のフーリエ変
換が周波数特性であり、第3図の波形は、各超音
波振動子1の音響放射面積を変えることにより制
御できる。したがつて、この発明に係る超音波探
触子では、周波数特性を制御できる定数の自由度
が従来に比べ大きくなり、従来に比べ所要周波数
特性をより容易に実現できる利点がある。以上
は、超音波を送信する場合について説明したが、
以上のことは超音波を受信する場合についても同
様である。
Now, when the ultrasonic probe shown in Fig. 2 is subjected to impulse excitation using an electric circuit similar to the conventional one, the ultrasonic transducer 1, which has a large acoustic radiation area, is excited with an ultrasonic pulse having a large amplitude level, and the acoustic radiation is emitted. In the ultrasonic transducer 1 having a small area, ultrasonic pulses having a small amplitude level are excited. This is because the capacitance of the ultrasonic transducer 1 is proportional to the acoustic radiation area, which is generally known in this type of technical field, but the acoustic radiation resistance is inversely proportional to the capacitance, and normally the acoustic The value of the radiation resistance is about several kΩ to several tens of kΩ. Therefore, if the acoustic radiation area doubles, for example, the acoustic radiation resistance will decrease by half, and the matching with the power supply resistance of the electric circuit (usually several tens to hundreds of ohms) will not be perfect. is correspondingly better, so that the effective power supply from the power source increases, ie, ultrasonic pulses with higher amplitude levels are excited. Furthermore, the time for the ultrasonic waves excited by each ultrasonic transducer 1 to reach the surface of the test material is delayed as the ultrasonic transducer 1 is located closer to the bucking material 3. Therefore, in the ultrasonic probe shown in FIG. 2, the ultrasonic pulses transmitted to the test material are the same as those excited by each ultrasonic transducer 1 at the above-mentioned amplitude level and time delay. The waveform is synthesized by taking into account the following, and the waveform is as shown in FIG. 3, for example. The first pulse in the figure is excited by the lower ultrasonic transducer in Fig. 2, the second pulse is excited by the central ultrasonic transducer in Fig. The third pulse corresponds to that excited by the upper ultrasonic transducer in FIG. Note that the temporal relationship between these pulses is determined by the delay material 6 shown in FIG. Further, the Fourier transform of the waveform shown in FIG. 3 is the frequency characteristic, and the waveform shown in FIG. 3 can be controlled by changing the acoustic radiation area of each ultrasonic transducer 1. Therefore, the ultrasonic probe according to the present invention has an advantage in that the degree of freedom of the constants that can control the frequency characteristics is greater than in the past, and required frequency characteristics can be achieved more easily than in the past. The above explained the case of transmitting ultrasonic waves, but
The above also applies to the case of receiving ultrasonic waves.

なお、以上は、第2図に示す一実施例の場合に
ついて説明したが、この発明はこれに限らず、各
超音波振動子1の音響放射面積のみでなく、各超
音波振動子1間の遅延材6の厚さをも合せて制御
すれば、より多様の要求に応じられる超音波探触
子を構成できることは明らかであろう。また、こ
の発明は、被検材表面に対して斜めに超音波を送
受信する斜角形超音波探触子や、被検材表面に沿
つて超音波を送受信する表面波形超音波探触子に
適用してもよい。また、アレイ形超音波探触子の
各素子に適用してもよい。
Although the above description has been made regarding the case of the embodiment shown in FIG. 2, the present invention is not limited to this. It is clear that if the thickness of the delay material 6 is also controlled, an ultrasonic probe that can meet more diverse requirements can be constructed. Furthermore, this invention is applicable to an oblique ultrasonic probe that transmits and receives ultrasonic waves obliquely to the surface of a test material, and a surface wave type ultrasonic probe that transmits and receives ultrasound along the surface of a test material. You may. Further, the present invention may be applied to each element of an array type ultrasonic probe.

以上のように、この発明に係る超音波探触子で
は、音響放射面積の異なる複数個の超音波振動子
1を、遅延材6をはさんで積層することにより、
従来に比べ、超音波探触子の周波数特性をより大
きな自由度で制御できる利点がある。
As described above, in the ultrasonic probe according to the present invention, by stacking a plurality of ultrasonic transducers 1 with different acoustic radiation areas with the delay material 6 in between,
This has the advantage that the frequency characteristics of the ultrasonic probe can be controlled with a greater degree of freedom than in the past.

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

第1図は、従来の超音波探触子を示す図、第2
図は、この発明に係る超音波探触子の一実施例を
示す図、第3図は、第2図に示した各超音波振動
子の出力を合成した波形を示す図である。図中、
1は超音波振動子、2は音響放射面、3はバツキ
ング材、4は音響インピーダンス変成層、5はリ
ード線、6は遅延材、7は超音波伝ぱん媒体であ
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。
Fig. 1 shows a conventional ultrasonic probe, Fig. 2 shows a conventional ultrasonic probe;
This figure shows an embodiment of the ultrasonic probe according to the present invention, and FIG. 3 is a diagram showing a waveform obtained by combining the outputs of the respective ultrasonic transducers shown in FIG. 2. In the figure,
1 is an ultrasonic transducer, 2 is an acoustic radiation surface, 3 is a backing material, 4 is an acoustic impedance modification layer, 5 is a lead wire, 6 is a delay material, and 7 is an ultrasonic propagation medium. In the drawings, the same or corresponding parts are denoted by the same reference numerals.

Claims (1)

【特許請求の範囲】[Claims] 1 音響放射面積が異なる複数個の超音波振動子
を、遅延材をはさんで積層し、送信および受信超
音波パルスの周波数特性を制御できるようにした
ことを特徴とする超音波探触子。
1. An ultrasonic probe characterized in that a plurality of ultrasonic transducers with different acoustic radiation areas are stacked with a delay material sandwiched between them so that the frequency characteristics of transmitted and received ultrasonic pulses can be controlled.
JP5287783A 1983-03-29 1983-03-29 ultrasonic probe Granted JPS59178096A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP5287783A JPS59178096A (en) 1983-03-29 1983-03-29 ultrasonic probe

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP5287783A JPS59178096A (en) 1983-03-29 1983-03-29 ultrasonic probe

Publications (2)

Publication Number Publication Date
JPS59178096A JPS59178096A (en) 1984-10-09
JPH029520B2 true JPH029520B2 (en) 1990-03-02

Family

ID=12927106

Family Applications (1)

Application Number Title Priority Date Filing Date
JP5287783A Granted JPS59178096A (en) 1983-03-29 1983-03-29 ultrasonic probe

Country Status (1)

Country Link
JP (1) JPS59178096A (en)

Also Published As

Publication number Publication date
JPS59178096A (en) 1984-10-09

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