JPS6227600B2 - - Google Patents

Info

Publication number
JPS6227600B2
JPS6227600B2 JP3989080A JP3989080A JPS6227600B2 JP S6227600 B2 JPS6227600 B2 JP S6227600B2 JP 3989080 A JP3989080 A JP 3989080A JP 3989080 A JP3989080 A JP 3989080A JP S6227600 B2 JPS6227600 B2 JP S6227600B2
Authority
JP
Japan
Prior art keywords
electrode
elements
divided
ultrasonic
electrodes
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
JP3989080A
Other languages
Japanese (ja)
Other versions
JPS56137798A (en
Inventor
Nobushi Iwashita
Atsuo Iida
Kenji Kawabe
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.)
Fujitsu Ltd
Original Assignee
Fujitsu Ltd
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 Fujitsu Ltd filed Critical Fujitsu Ltd
Priority to JP3989080A priority Critical patent/JPS56137798A/en
Publication of JPS56137798A publication Critical patent/JPS56137798A/en
Publication of JPS6227600B2 publication Critical patent/JPS6227600B2/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
    • B06B1/0622Methods 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 on one surface

Description

【発明の詳細な説明】 本発明は、超音波診断装置などに使用される超
音波振動子に関する。
DETAILED DESCRIPTION OF THE INVENTION The present invention relates to an ultrasonic transducer used in an ultrasonic diagnostic apparatus or the like.

従来の超音波診断装置に用いられているフエー
ズドアレー型の超音波振動子は、第1図に示すよ
うに多数個の矩形の振動素子A1,A2……をその
長さ方向と直交する方向で平行に配列し、その個
個の振動素子に順次所定の遅延時間をもたせて駆
動電圧を与える事により、個々の振動素子からの
音波の合成波を所望の方向に発信させる。振動素
子A1,A2,……は例えば幅0.4mm、長さ16mmの角
柱状圧電材料からなり、同材料のベースBを共通
にして例えば0.1mm間隔で配列される。振動素子
A1,A2,……の表面には一対の電極の一方C1
C2,……が設けられ、それぞれにリード線D1
D2,……が接続される。ベースBの裏面には該
一対の電極の他方が共通電極Eとして設けられ、
これにはリード線Fが接続される。なお図示しな
いが電極Eの下面には、下面からの超音波放射を
防止するバツキング材などが設けられる。この種
のフエーズドアレー型の超音波振動子では、個々
の振動素子を同時ではなく所定の遅延時間をもつ
て逐次駆動して超音波送出方向を所望方向にする
セクタ駆動方法をとると隣接の振動素子間で相互
干渉が発生する。例えば振動素子A2を駆動する
と全方向に放射される超音波のうちの該素子側面
から放射される分X2が、第2図に示すように隣
接する振動素子A1,A3の側面に入つてこれを振
動させ、その振動Y1,Y3が振動素子A1,A3本来
の振動に重畳される。従つて、今駆動順はA1
A2,A3の順とすると、素子A1では振動終了が遅
延されまた素子A3では本来の動作タイミングの
前に振動開始することになり、この結果超音波振
動子から発信される超音波波形は遅延時間の与え
方、言い換えれば合成波の発信方向により変動す
るという問題が生じる。超音波診断を反射パルス
の振幅およびタイミングで行なう場合はこれでも
格別支障が出ることはないが、反射波形それ自身
を利用する場合は問題である。この反射波形を分
析対象とする方式には次の利点がある。即ち単な
る反射波の振幅およびタイミングでは目標物以外
のものからの反射波(超音波は光ほど集束性がよ
くないのでかゝる反射波はかなり大きい)を目標
〓〓〓〓〓
物からの反射波と全く区別なく扱つてしまい目標
物の解析に支障を生じることがあるが、この点反
射波の波形を利用する方式では、該反射波は送信
波の反射波である事が容易に同定でき、送信波は
前記の遅延時間調整により目標物へ向けて発射す
るから、目標物からの反射波と目標物以外のもの
からの反射波とを分別することが可能となり、
CCDフイルタなどにより所望波形の反射波のみ
を抽出して、例えば超音波断層像の輪郭を鮮明に
する等の利点を得ることができる。
The phased array type ultrasonic transducer used in conventional ultrasonic diagnostic equipment has a large number of rectangular transducer elements A 1 , A 2 . By arranging them in parallel with each other and sequentially applying a driving voltage to each vibrating element with a predetermined delay time, a composite wave of sound waves from the individual vibrating elements is emitted in a desired direction. The vibrating elements A 1 , A 2 , . . . are made of a prismatic piezoelectric material having a width of 0.4 mm and a length of 16 mm, for example, and are arranged at intervals of, for example, 0.1 mm with a common base B made of the same material. Vibration element
On the surfaces of A 1 , A 2 , ..., one of the pair of electrodes C 1 ,
C 2 , ... are provided, and lead wires D 1 , ... are provided respectively.
D 2 , ... are connected. The other of the pair of electrodes is provided on the back surface of the base B as a common electrode E,
A lead wire F is connected to this. Although not shown, a backing material or the like is provided on the lower surface of the electrode E to prevent ultrasonic radiation from being emitted from the lower surface. In this type of phased array type ultrasonic transducer, if a sector drive method is used in which the individual transducer elements are sequentially driven with a predetermined delay time rather than simultaneously, and the ultrasound transmission direction is set in the desired direction, adjacent transducer elements Mutual interference occurs between the two. For example, when a transducer element A 2 is driven, a portion of the ultrasonic waves emitted in all directions, X 2 emitted from the side surface of the element, is transmitted to the side surfaces of the adjacent transducer elements A 1 and A 3 as shown in Fig. 2. The vibrations Y 1 and Y 3 are superimposed on the original vibrations of the vibration elements A 1 and A 3 . Therefore, the driving order now is A 1 ,
If A 2 and A 3 are in this order, the end of vibration will be delayed in element A 1 , and the vibration will start in element A 3 before the original operation timing, and as a result, the ultrasonic wave emitted from the ultrasonic transducer will A problem arises in that the waveform varies depending on how the delay time is given, in other words, the direction in which the composite wave is transmitted. Although this poses no particular problem when ultrasonic diagnosis is performed using the amplitude and timing of the reflected pulse, it is a problem when the reflected waveform itself is used. The method of analyzing this reflected waveform has the following advantages. In other words, by simply looking at the amplitude and timing of the reflected waves, you cannot target the reflected waves from things other than the target (ultrasonic waves are not as focused as light, so such reflected waves are quite large).
This may cause trouble in analyzing the target because it is treated completely indistinguishably from the reflected wave from an object. However, in the method that uses the waveform of the reflected wave, it is possible that the reflected wave is a reflected wave of the transmitted wave. It can be easily identified, and since the transmitted wave is emitted toward the target by adjusting the delay time described above, it is possible to separate the reflected waves from the target and those from things other than the target.
By extracting only the reflected waves of a desired waveform using a CCD filter or the like, it is possible to obtain advantages such as making the outline of an ultrasound tomographic image clearer, for example.

本発明は、フエーズドアレー型の超音波振動子
の個々の振動素子の相互の干渉を低減させ、合成
波の発信方向に拘らず常に同一の発信波形を得よ
うとするもので、その特徴とするところは圧電材
料の対向する2面に電極を設けてなる振動素子を
その長さ方向とは交叉する方向に所定間隙を隔て
て複数個配列した超音波振動子において、各振動
素子の電極の少なくとも一方を長さ方向で複数個
に分割し、超音波発射に際しては、隣接する振動
素子の対向し合わない分割電極部分を駆動する点
にある。以下図示の実施例を参照しながら本発明
を詳細に説明する。
The present invention aims to reduce the mutual interference of the individual vibrating elements of a phased array type ultrasonic transducer and always obtain the same transmitted waveform regardless of the direction in which the composite wave is transmitted. In an ultrasonic vibrator in which a plurality of vibrating elements each having electrodes provided on two opposing sides of a piezoelectric material are arranged at a predetermined interval in a direction intersecting the longitudinal direction of the vibrating elements, at least one of the electrodes of each vibrating element is arranged. is divided into a plurality of parts in the length direction, and when emitting ultrasonic waves, divided electrode parts of adjacent vibrating elements that do not face each other are driven. The present invention will be explained in detail below with reference to the illustrated embodiments.

第3図は本発明の一実施例で、第1図と同一部
分には同一符号が付してある。本例が第1図と異
なる点は、各振動素子A1,A2……の個別電極、
本例ではプラス側電極をそれぞれ2分割し、それ
ぞれにリード線を接続した点にある。C11,C12
振動素子A1の電極C1を分割した各分割電極部分
であり、それぞれにリード線D11,D12が接続され
る。他も同様であり、振動素子A2,A3……の一
方の分割電極部分C21,C31……はリード線D21
D31……に接続され、他方の分割電極部分C22
C32……はリード線D22,D32……に接続される。
かゝるフエーズドアレー型の超音波振動子はリニ
アスキヤンおよびセクタスキヤン各方式での使用
が可能であるが、これらの発信時には隣接する振
動素子相互間で対向しない側の分割電極部分を選
択使用する。例えば振動素子A1で電極部分C12
駆動した(電圧を印加した)場合には振動素子
A2では電極部分C21を駆動し、電極部分C11,C22
は休止状態とし、以下同様にして全体として電極
部分C12,C21,C32,C41,C52,……のみを駆動
して所要とするスキヤンを行なう。このようにす
れば、例えば振動素子A2において駆動信号によ
り振動が生ずる部分は電極部分C21の下部圧電材
料に限られ、他方の電極部分C22の下部圧電材料
には振動が生じない。従つて振動素子A2の振動
が、電極C21の下部圧電材料から素子間々隙、お
よび素子A1,A3の電極C11,C31の下部圧電材料
を通つて、及び電極C22の下部圧電材料を通りか
つ素子間々隙を通つて隣接振動素子A1,A3の電
圧部分C12,C32側へ伝達される度合は極めて少な
い。各素子の分割電極C11とC12,C21とC22……間
の圧電材料に溝を作つておけば、なお更である。
こうして振動素子A1,A2,A3……の電極部分
C12,C21,C32,……に駆動電圧を印加して発生
させる超音波の波形は第1図のものよりはるかに
素子間干渉のないものになる。
FIG. 3 shows an embodiment of the present invention, in which the same parts as in FIG. 1 are given the same reference numerals. This example differs from Fig. 1 in that the individual electrodes of each vibrating element A 1 , A 2 .
In this example, each positive side electrode is divided into two parts, and a lead wire is connected to each part. C 11 and C 12 are divided electrode portions obtained by dividing the electrode C 1 of the vibration element A 1 , and lead wires D 11 and D 12 are connected to them, respectively. The same applies to the other parts, and one of the divided electrode parts C 21 , C 31 ... of the vibration elements A 2 , A 3 ... is connected to the lead wire D 21 ,
D 31 ... is connected to the other divided electrode portion C 22 ,
C 32 ... is connected to lead wires D 22 , D 32 ....
Such a phased array type ultrasonic transducer can be used in linear scan and sector scan methods, but when transmitting these signals, the divided electrode portions on the side that do not face each other between adjacent transducer elements are selectively used. For example, if the electrode part C 12 is driven (voltage is applied) with the vibration element A 1 , the vibration element
In A 2 , the electrode part C 21 is driven, and the electrode parts C 11 , C 22
is in a rest state, and in the same manner, only the electrode portions C 12 , C 21 , C 32 , C 41 , C 52 , . . . are driven to perform the required scan. In this way, for example, in the vibrating element A2 , the portion where vibration occurs due to the drive signal is limited to the lower piezoelectric material of the electrode portion C21 , and no vibration occurs in the lower piezoelectric material of the other electrode portion C22 . Therefore, the vibration of the vibration element A 2 is transmitted from the lower piezoelectric material of the electrode C 21 to the element gap, through the lower piezoelectric material of the electrodes C 11 and C 31 of the elements A 1 and A 3 , and from the lower piezoelectric material of the electrode C 22 . The degree of transmission to the voltage portions C 12 and C 32 of the adjacent vibrating elements A 1 and A 3 through the piezoelectric material and the gap between the elements is extremely small. It would be even better if grooves were made in the piezoelectric material between the divided electrodes C 11 and C 12 , C 21 and C 22 . . . of each element.
In this way, the electrode parts of the vibrating elements A 1 , A 2 , A 3 ...
The waveform of the ultrasonic wave generated by applying a driving voltage to C 12 , C 21 , C 32 , . . . is much freer from inter-element interference than that shown in FIG.

この超音波振動子は上述した様に送信時には相
互干渉を避けるために千鳥状に選んだ電極部分
C12,C21,C32……またはC11,C22,C31……しか
用いないが、受信時には相互干渉の問題は無視で
きるので受信面積を拡げるために全ての電極部分
C11,C21,C31,……,C12,C22,C32……を用い
る。第4図はこれら電極部分の切替回路を示す図
で、32個の振動素子A1〜A32を有する超音波振動
子を例としたものである。SWは32個の受信専用
スイツチSRと同数の送受切替用スイツチSTR
有するスイツチ群で、各受信専用スイツチSR
送信時には使用されない電極部分C11,C22,……
C311,C322に接続され、また各送受切替用スイツ
チSTRは送受両用に使用される電極部分C12
C21,……C312,C321に接続される。超音波振動
子の共通電極Eは接地されるが、これは全ての振
動素子A1〜A32に共通な1枚の導電板である代り
に、個々の振動素子毎に分かれているものでもよ
い。そして個々の振動素子の共通電極が独立して
設けられる場合には、それを対向する電極C1
C2……と同様に分割してもよい。スイツチ群SW
は制御回路CONTからの切替スイツチ制御信号
SCにより連動して制御される。そして図示の如
く送信側Tに切替つている時は駆動信号DVが遅
延回路TD1,TD2,……TD31,TD32、スイツチ
TRを通して電極部分C12,C21,……C312,C321
に印加される。セクタスキヤンの場合には遅延回
路TD1〜TD32の遅延量に振動素子の配列順に所
望程度(これは走査角に応じて変更される)ずつ
異ならされる。受信時にはスイツチ群SWのスイ
〓〓〓〓〓
ツチSR,STRを全て受信側Rに切替え、電極部
分C11〜C321,C12〜C322の出力を合成する。セク
タスキヤンの場合振動素子A1〜A32の各出力はそ
れぞれ遅延回路RD1〜RD32を通して合成され、最
終出力OUTを生じる。この遅延回路RD1〜RD32
の遅延量は遅延回路TD1〜TD32のそれに見合う
ものである。
As mentioned above, this ultrasonic transducer has electrode parts selected in a staggered manner to avoid mutual interference during transmission.
Although only C 12 , C 21 , C 32 ... or C 11 , C 22 , C 31 ... are used, the problem of mutual interference can be ignored during reception, so all electrode parts are used to expand the reception area.
C 11 , C 21 , C 31 , ..., C 12 , C 22 , C 32 ... are used. FIG. 4 is a diagram showing a switching circuit for these electrode portions, taking as an example an ultrasonic vibrator having 32 vibrating elements A 1 to A 32 . SW is a switch group having 32 reception-only switches SR and the same number of transmission/reception switching switches STR , and each reception-only switch SR has electrode portions C 11 , C 22 , . . . that are not used during transmission.
C 311 , C 322 , and each transmission/reception switching switch S TR has an electrode portion C 12 , which is used for both transmission and reception.
Connected to C 21 , ...C 312 , C 321 . The common electrode E of the ultrasonic vibrator is grounded, but instead of being a single conductive plate common to all the vibrating elements A1 to A32 , it may be separated for each individual vibrating element. . When the common electrode of each vibrating element is provided independently, it is connected to the opposing electrode C 1 ,
C 2 ...may be divided in the same way. switch group SW
is the changeover switch control signal from the control circuit CONT
Controlled by SC. As shown in the figure, when switching to the transmitting side T, the drive signal DV passes through the delay circuits TD 1 , TD 2 , ... TD 31 , TD 32 and the switch S TR to the electrode portions C 12 , C 21 , ... C 312 , C321
is applied to In the case of sector scan, the delay amounts of the delay circuits TD 1 to TD 32 are varied by a desired degree (this is changed depending on the scan angle) in the order in which the vibrating elements are arranged. At the time of reception, the switch group SW is switched.
Both S R and S TR are switched to the receiving side R, and the outputs of the electrode portions C 11 to C 321 and C 12 to C 322 are combined. In the case of sector scan, the outputs of the vibrating elements A 1 to A 32 are combined through delay circuits RD 1 to RD 32 , respectively, to produce the final output OUT. This delay circuit RD 1 ~ RD 32
The amount of delay is commensurate with that of the delay circuits TD 1 to TD 32 .

第5図は本発明の他の実施例である。本例では
各振動素子(A1で代表する)の駆動電極を4分
割し、1つおきの分割電極部分C11,C13をリード
線D11に、また残りの電極部分C12,C14をリード
線D12に接続する。そして隣接する振動素子相互
間で非対向の電極部分に接続されたリード線
D11,D22,……またはD12,D21,……を選択して
駆動する。受信時に全ての電極部分を用いる点は
第3図と同様である。本例では更に電極部分C11
とC12,C12とC13,C13とC14の各間の圧電素子
(他の素子についても同様)を切削して溝部Gを
設けてある。この溝部Gは同一振動素子内で振動
が電極部分C11,C12,……の配列方向に伝達され
る度合を低減するので、前記の如くこれにより隣
接振動素子間の相互干渉は更に抑制される。尚、
第5図の様に各素子の電極を多数の電極部分に分
割して各素子の分割電極をX,Y方にマトリスク
状に配列した場合には、各振動素子A1,A2……
の駆動時点を異ならせる通常のセクタ走査に加
え、各振動素子の各分割電極部分に印加する電圧
にも同様な遅延を持たせることによりX―Z面に
おける該セクタスキヤンの効果をY―Z面におい
ても持たせることができ、通常のセクタ走査にお
けるより超音波ビームをY―Z面において絞るこ
とができる。
FIG. 5 shows another embodiment of the invention. In this example, the drive electrode of each vibration element (represented by A 1 ) is divided into four parts, and every other divided electrode part C 11 and C 13 is used as the lead wire D 11 , and the remaining electrode parts C 12 and C 14 are used as the lead wire D 11. Connect to lead wire D 12 . And lead wires connected to non-opposing electrode parts between adjacent vibrating elements
D 11 , D 22 , . . . or D 12 , D 21 , . . . are selected and driven. This is similar to FIG. 3 in that all electrode portions are used during reception. In this example, the electrode part C 11
Grooves G are provided by cutting the piezoelectric element between C 12 and C 12 , C 12 and C 13 , and C 13 and C 14 (the same applies to other elements). This groove G reduces the degree to which vibration is transmitted in the arrangement direction of the electrode portions C 11 , C 12 , . . . within the same vibrating element, so as mentioned above, mutual interference between adjacent vibrating elements is further suppressed Ru. still,
When the electrodes of each element are divided into many electrode parts and the divided electrodes of each element are arranged in a matrix shape in the X and Y directions as shown in Fig. 5, each vibrating element A 1 , A 2 . . .
In addition to normal sector scanning in which the driving time points of This allows the ultrasonic beam to be focused in the YZ plane more than in normal sector scanning.

以上述べたように本発明によれば、フエーズド
アレイ型の超音波振動子を構成する各振動素子相
互間の干渉を低減できるので、合成波の発信方向
によらず同一の発信波形が得られる利点がある。
As described above, according to the present invention, it is possible to reduce the interference between the vibrating elements constituting the phased array type ultrasonic transducer, so there is an advantage that the same transmitted waveform can be obtained regardless of the direction in which the composite wave is transmitted. be.

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

第1図は従来のフエーズドアレイ型超音波振動
子の一例を示す斜視図、第2図は振動素子間の相
互干渉の説明図、第3図は本発明の一実施例を示
す斜視図、第4図はその電極切替回路を示す構成
図、第5図は本発明の他の実施例を示す斜視図で
ある。 図中、A1,A2……は振動素子、C11,C12……
は一対の電極の一方の分割電極部分、Eは他方の
電極、SWは送受切替用スイツチ群である。
FIG. 1 is a perspective view showing an example of a conventional phased array type ultrasonic transducer, FIG. 2 is an illustration of mutual interference between transducer elements, FIG. 3 is a perspective view showing an embodiment of the present invention, and FIG. The figure is a configuration diagram showing the electrode switching circuit, and FIG. 5 is a perspective view showing another embodiment of the present invention. In the figure, A 1 , A 2 ... are vibration elements, C 11 , C 12 ...
is a divided electrode portion of one of the pair of electrodes, E is the other electrode, and SW is a group of switches for switching between transmission and reception.

Claims (1)

【特許請求の範囲】 1 圧電材料の対向する2面に電極を設けてなる
振動素子をその長さ方向とは交叉する方向に所定
間隔を隔てて複数個配列した超音波振動子におい
て、各振動素子の電極の少なくとも一方を長さ方
向で複数個に分割し、超音波発射に際しては、隣
接する振動素子の対向し合わない分割電極部分を
駆動することを特徴とする超音波振動子。 2 分割電極間の圧電材料に溝が設けられたこと
を特徴とする特許請求の範囲第1項記載の超音波
振動子。
[Claims] 1. In an ultrasonic vibrator in which a plurality of vibrating elements each having electrodes provided on two opposing surfaces of a piezoelectric material are arranged at a predetermined interval in a direction intersecting the length direction of the vibrating elements, each vibration An ultrasonic transducer characterized in that at least one of the electrodes of the element is divided into a plurality of parts in the length direction, and when emitting ultrasonic waves, the divided electrode parts of adjacent transducer elements that do not face each other are driven. 2. The ultrasonic transducer according to claim 1, wherein a groove is provided in the piezoelectric material between the divided electrodes.
JP3989080A 1980-03-28 1980-03-28 Ultrasonic vibrator Granted JPS56137798A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP3989080A JPS56137798A (en) 1980-03-28 1980-03-28 Ultrasonic vibrator

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP3989080A JPS56137798A (en) 1980-03-28 1980-03-28 Ultrasonic vibrator

Publications (2)

Publication Number Publication Date
JPS56137798A JPS56137798A (en) 1981-10-27
JPS6227600B2 true JPS6227600B2 (en) 1987-06-16

Family

ID=12565558

Family Applications (1)

Application Number Title Priority Date Filing Date
JP3989080A Granted JPS56137798A (en) 1980-03-28 1980-03-28 Ultrasonic vibrator

Country Status (1)

Country Link
JP (1) JPS56137798A (en)

Cited By (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPH0339198Y2 (en) * 1988-06-01 1991-08-19

Families Citing this family (3)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPH0832109B2 (en) * 1986-12-24 1996-03-27 株式会社東芝 Ultrasonic probe
JP2633549B2 (en) * 1987-02-26 1997-07-23 株式会社東芝 Ultrasonic probe
CN113840668B (en) * 2020-04-14 2022-04-29 本多电子株式会社 Ultrasonic vibrator for measuring equipment

Cited By (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPH0339198Y2 (en) * 1988-06-01 1991-08-19

Also Published As

Publication number Publication date
JPS56137798A (en) 1981-10-27

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