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JPH0116393B2 - - Google Patents
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JPH0116393B2 - - Google Patents

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Publication number
JPH0116393B2
JPH0116393B2 JP15116682A JP15116682A JPH0116393B2 JP H0116393 B2 JPH0116393 B2 JP H0116393B2 JP 15116682 A JP15116682 A JP 15116682A JP 15116682 A JP15116682 A JP 15116682A JP H0116393 B2 JPH0116393 B2 JP H0116393B2
Authority
JP
Japan
Prior art keywords
delay
array
array transducer
delay line
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
JP15116682A
Other languages
Japanese (ja)
Other versions
JPS5940279A (en
Inventor
Yasuto Takeuchi
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.)
Yokogawa Electric Corp
Original Assignee
Yokogawa 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 Yokogawa Electric Corp filed Critical Yokogawa Electric Corp
Priority to JP15116682A priority Critical patent/JPS5940279A/en
Publication of JPS5940279A publication Critical patent/JPS5940279A/en
Publication of JPH0116393B2 publication Critical patent/JPH0116393B2/ja
Granted legal-status Critical Current

Links

Classifications

    • GPHYSICS
    • G01MEASURING; TESTING
    • G01SRADIO DIRECTION-FINDING; RADIO NAVIGATION; DETERMINING DISTANCE OR VELOCITY BY USE OF RADIO WAVES; LOCATING OR PRESENCE-DETECTING BY USE OF THE REFLECTION OR RERADIATION OF RADIO WAVES; ANALOGOUS ARRANGEMENTS USING OTHER WAVES
    • G01S7/00Details of systems according to groups G01S13/00, G01S15/00, G01S17/00
    • G01S7/52Details of systems according to groups G01S13/00, G01S15/00, G01S17/00 of systems according to group G01S15/00
    • G01S7/52017Details of systems according to groups G01S13/00, G01S15/00, G01S17/00 of systems according to group G01S15/00 particularly adapted to short-range imaging
    • G01S7/52053Display arrangements

Landscapes

  • Engineering & Computer Science (AREA)
  • Computer Networks & Wireless Communication (AREA)
  • Physics & Mathematics (AREA)
  • General Physics & Mathematics (AREA)
  • Radar, Positioning & Navigation (AREA)
  • Remote Sensing (AREA)
  • Measurement Of Velocity Or Position Using Acoustic Or Ultrasonic Waves (AREA)

Description

【発明の詳細な説明】 本発明は、直線状の振動子アレイと円弧状の振
動子アレイを共用するスイツチド・アレイ走査型
の超音波映像装置に関する。
DETAILED DESCRIPTION OF THE INVENTION The present invention relates to a switched array scanning type ultrasound imaging apparatus that uses both a linear transducer array and an arcuate transducer array.

従来より、複数個の圧電振動子を直線状に配列
してなるリニヤアレイ振動子と複数個の圧電振動
子を円弧状に配列してなる円弧アレイ振動子はよ
く知られている。第1図はそのリニヤアレイ振動
子10によるビーム走査の様子を示すもので、等
密度平行音線群となるように、N個の圧電振動子
TDに対しm個(図では7個)を1組として1個
ずつずらせながらリニヤ走査し、かつその際m個
の振動子に対して中央部のものほど外側のものよ
り遅く付勢(位相駆動)して射出される超音波ビ
ームを図示のように集束し、ある深度においては
細いビームBで走査している。
2. Description of the Related Art Conventionally, linear array vibrators in which a plurality of piezoelectric vibrators are arranged in a straight line and circular array vibrators in which a plurality of piezoelectric vibrators are arranged in a circular arc are well known. FIG. 1 shows the state of beam scanning by the linear array vibrator 10, in which N piezoelectric vibrators are
Linear scanning is performed on the TD while shifting one set of m transducers (7 in the figure), and at this time, the m transducers in the center are energized more slowly than the outer ones (phase drive). ), the emitted ultrasonic beam is focused as shown in the figure, and a narrow beam B is used to scan at a certain depth.

また、第2図は円弧アレイ振動子20による走
査の様子を示すもので、第1図と同様に複数個の
圧電振動子TDをリニヤ走査した場合を示す。等
角度密度の走査ビームは筐体21の下面いわゆる
被検体との当接面近傍22で互いに交差するよう
な関係で被検体23に向つて射出される。従つ
て、被検体内では超音波ビームはセクタ走査とな
る。この場合も超音波ビームをある深さにおいて
細いビームとすべく、振動子TDを位相駆動して
いる。
Further, FIG. 2 shows the state of scanning by the circular arc array vibrator 20, and shows the case where a plurality of piezoelectric vibrators TD are linearly scanned similarly to FIG. 1. The scanning beams with equal angular density are emitted toward the subject 23 in such a manner that they intersect with each other at the lower surface of the housing 21, ie, near the contact surface 22 with the subject. Therefore, the ultrasound beam performs sector scanning within the subject. In this case as well, the transducer TD is phase-driven to make the ultrasonic beam narrow at a certain depth.

このようなリニヤアレイ振動子10は腹部観察
用に適し、一方円弧アレイ振動子20は胸部観察
用に好適なもので、1つの超音波診断装置に共用
できることが望ましい。しかしながら、リニヤア
レイと円弧アレイとでは利用する圧電振動子の位
相駆動における所要遅延時間分布が同一でないた
め、2組の遅延回路を設備しなければならないと
いう不便があつた。すなわち、リニヤアレイの場
合には波面としてアレイの所で凹面になるように
正の焦点距離を設定すべく凹面的な、すなわち中
央ほどおくらせる如き位相差分布を持たせたのに
対し、円弧アレイの場合にはアレイ自身が既に過
度な凹面を有しているので体内のどこか適当な深
さで集束させるためにはこの凹面を減殺するよう
な凸面的なすなわち同時駆動のm個の振動子の内
で中央部のものほど外側のものより早い付勢をし
なければ同様な集束波面が得られない。従つて、
所要位相差の分布という見地からは両者は互いに
逆の関係にあり、1つの遅延回路を共用すること
には無理があつた。
Such a linear array transducer 10 is suitable for abdominal observation, while the arcuate array transducer 20 is suitable for chest observation, and it is desirable that it can be used commonly in one ultrasound diagnostic apparatus. However, since the linear array and the circular arc array do not have the same required delay time distribution in the phase drive of the piezoelectric vibrators used, there is an inconvenience that two sets of delay circuits must be installed. In other words, in the case of a linear array, a positive focal length is set so that the wavefront becomes a concave surface at the array, and a concave phase difference distribution is created, that is, the phase difference distribution is delayed toward the center. In some cases, the array itself already has an excessively concave surface, so in order to focus it at an appropriate depth somewhere in the body, it is necessary to use a convex surface, that is, m oscillators driven simultaneously, to reduce this concavity. A similar focused wavefront cannot be obtained unless the center part is energized faster than the outer part. Therefore,
From the viewpoint of the distribution of the required phase difference, the two are in an inverse relationship to each other, and it is unreasonable to share one delay circuit.

本発明は、このような点に鑑み、その目的とす
るところは遅延回路の極く僅かの切換変更でリニ
ヤアレイ探触子と円弧アレイ探触子を共用できる
ようにしたスイツチド・アレイ走査型の超音波映
像装置を提供しようとするものである。
In view of these points, the purpose of the present invention is to provide a switched array scanning type ultrasonic probe that can be used in both linear array probes and circular arc array probes with extremely small switching changes in the delay circuit. The present invention aims to provide a sound wave imaging device.

以下図面を用いて本発明を詳しく説明する。第
3図は本発明に係る超音波映像装置の要部の一実
施例を示す構成図である。第3図において、31
はマルチプレクサ、321〜327は双方向性のバ
ツフアアンプ、33はデイレーマツプ、34はデ
イレーライン、35はスイツチ、36はパルサ、
37は増幅器である。マルチプレクサ31はリニ
ヤ走査のために振動子をm個ずつ選択してバツフ
アアンプ321〜327に接続するものである。デ
イレーマツプ33は、デイレーライン34の出力
とバツフアアンプ321〜327の入力でなるマト
リクス回路でなり、任意の行と列とをそれぞれ接
続できるようになつている。図では丸印のクロス
ポイントが接続点である。デイレーライン34は
LC梯子型の如き双方向伝搬可能なデイレーライ
ンで、複数個の中間タツプはデイレーマツプ33
に導かれている。このデイレーライン34にはス
イツチ35を介してパルサ36からのパルスが与
えられるようになつている。一方、反射波が受信
した場合にはデイレーライン34より得られるエ
コー信号はスイツチ35を介して受信回路の増幅
器37に導かれる。
The present invention will be explained in detail below using the drawings. FIG. 3 is a configuration diagram showing an embodiment of the essential parts of the ultrasound imaging apparatus according to the present invention. In Figure 3, 31
is a multiplexer, 32 1 to 32 7 are bidirectional buffer amplifiers, 33 is a delay map, 34 is a delay line, 35 is a switch, 36 is a pulser,
37 is an amplifier. The multiplexer 31 selects m transducers for linear scanning and connects them to the buffer amplifiers 32 1 to 32 7 . The delay map 33 is a matrix circuit consisting of the output of the delay line 34 and the inputs of the buffer amplifiers 32 1 to 32 7 , and is designed to connect arbitrary rows and columns, respectively. In the figure, the cross points marked with circles are connection points. day line 34
It is a delay line that can be propagated in both directions, such as an LC ladder type, and multiple intermediate taps are connected to the delay map 33.
guided by. A pulse from a pulser 36 is applied to this delay line 34 via a switch 35. On the other hand, when a reflected wave is received, the echo signal obtained from the delay line 34 is guided to the amplifier 37 of the receiving circuit via the switch 35.

なお、バツフアアンプ321〜327は双方向性
のものに限つたことはなく、送信と受信とで別々
のバツフアアンプを設けこれを切換えて使用する
ようにしてもよい。
Note that the buffer amplifiers 32 1 to 32 7 are not limited to bidirectional ones, and separate buffer amplifiers may be provided for transmission and reception, and these may be used by switching.

このような構成において、アレイ振動子10及
び20の圧電振動子の配列ピツチは実質上同一で
あるものとし、円弧アレイの弧長とリニヤアレイ
の走査幅とが等しいとする。このような場合にお
いてこれら振動子より発生する波面に関しては次
式が成立する。
In such a configuration, it is assumed that the arrangement pitch of the piezoelectric vibrators of the array vibrators 10 and 20 is substantially the same, and the arc length of the circular arc array and the scanning width of the linear array are equal. In such a case, the following equation holds true regarding the wavefronts generated by these vibrators.

1/f=1/a+1/b (1) ここに、fは合成結果の焦点の距離すなわちア
レイから焦束点までの距離(波面の曲率半径) a、bは各々のデイレーマツプ及びアレイの曲
率によるそれら固有の負又は正の焦点距離(負の
場合は凸波面) ここで、例えば、振動子のピツチを1.5mm、振
動子総数を64個、その内で所定の送受波開口で移
動可能な範囲が56個分であるとする。円弧アレイ
において、半径r=50mmとし(90゜強のセクタ走
査が可能となる)、集束点すなわちfをクロスオ
ーバポイントPcから80mm先にすなわちf=50+
80=130mmとしたい場合には、(1)式にf=130、a
=50を代入して、b=−81.25mmを得る。これを
第3図に示すように1つのデイレーマツプ33で
その懸垂するデイレーラインの入口と出口を切り
替えることにより、円弧アレイ20でセクタ走査
するときは−81.25mm(クロスオーバポイントPc
から距離81.25mmの点)に、他方リニヤアレイ1
0でリニヤ走査するときには振動子面より81.25
mmの深さにビームを集束することができるように
各々相当する電気的焦点距離を実現することがで
きる。従つて、リニヤアレイ振動子に対しても円
弧アレイ振動子に対しても同一接続パターンのデ
イレーマツプ33を共用できることになり、ただ
使い分けが必要なのはデイレーライン34のみで
ある。すなわち、円弧アレイ接続時は凸面状位相
駆動となるようにスイツチ35をS側に接続し、
パルサ36からのパルスをデイレーライン34に
導き(点線方向)、中央部の振動子ほど外側のも
のより早く付勢する。一方、リニヤアレイ振動子
を使用する場合は凹面波面が形成されればよいか
ら、スイツチ35をL側に接続し、パルサ36か
らのパルスをデイレーライン34の上述の場合の
反対側の端子に導き(実線方向)、中央部に比べ
て外側の振動子ほど早く付勢してやればよい。
1/f=1/a+1/b (1) Here, f is the distance of the focal point of the synthesis result, that is, the distance from the array to the focal point (radius of curvature of the wavefront). a, b depend on the curvature of each day map and array. Their inherent negative or positive focal length (if negative, the convex wavefront) Here, for example, the pitch of the transducer is 1.5 mm, the total number of transducers is 64, and the range within which the transducer can be moved within the specified transmitting and receiving aperture. Assume that there are 56 pieces. In the circular arc array, the radius r = 50 mm (sector scanning of just over 90 degrees is possible), and the focusing point, f, is set 80 mm ahead of the crossover point Pc, i.e., f = 50+
If you want to set 80=130mm, use f=130 and a in equation (1).
By substituting =50, we get b=-81.25mm. As shown in FIG. 3, by switching the entrance and exit of the suspended delay line using one day map 33, when scanning sectors with the circular arc array 20, -81.25 mm (crossover point Pc
at a distance of 81.25 mm from the other linear array 1
81.25 from the transducer surface when performing linear scanning at 0
Each corresponding electrical focal length can be achieved such that the beam can be focused to a depth of mm. Therefore, the same delay map 33 having the same connection pattern can be used for both the linear array vibrator and the arc array vibrator, and only the delay line 34 needs to be used properly. That is, when connecting the arc array, the switch 35 is connected to the S side so that convex phase drive is performed.
Pulses from the pulser 36 are guided to the delay line 34 (in the direction of the dotted line), and the vibrators in the center are energized faster than those on the outside. On the other hand, when using a linear array vibrator, since it is sufficient to form a concave wavefront, the switch 35 is connected to the L side, and the pulses from the pulser 36 are guided to the terminal on the opposite side of the delay line 34 from the above case. (in the direction of the solid line), the outer vibrators should be energized more quickly than the center.

なお、リニヤアレイ振動子と円弧アレイ振動子
とで振動子配列ピツチは必ずしも同一である必要
はなく、相異なるピツチであつてもよい。例え
ば、上記の例において、リニヤアレイ振動子の方
のピツチを1.5mmから1.6mmに変更した場合には焦
点(集束点)が71.41mmの深さの所に位置し、1.7
mmとすれば深度63.26mmの所となるだけで、デイ
レーマツプを変更する必要は全くない。
Note that the transducer arrangement pitches of the linear array transducer and the arc array transducer do not necessarily have to be the same, and may be different pitches. For example, in the above example, if the pitch of the linear array transducer is changed from 1.5 mm to 1.6 mm, the focal point (convergence point) will be located at a depth of 71.41 mm, and 1.7 mm.
mm, the depth will be 63.26mm, and there is no need to change the day map.

以上は送波時における位相駆動について説明し
たが、受波時についても全く同様の接続であり、
信号の流れの方向が送信時と逆の関係となるだけ
である。
The above explained the phase drive when transmitting waves, but the connection is exactly the same when receiving waves.
The only difference is that the direction of signal flow is the opposite of that during transmission.

以上説明したように、本発明によれば、集束用
のデイレーマツプをリニヤ走査の場合とセクタ走
査の場合とで互いに裏返しの関係で用いることに
より、同一の遅延回路系を両走査に共用すること
ができる超音波映像装置を実現することができ
る。
As explained above, according to the present invention, the same delay circuit system can be shared for both types of scanning by using the focusing delay map in a reverse relationship for linear scanning and sector scanning. It is possible to realize an ultrasonic imaging device that can perform

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

第1図はリニヤアレイ振動子による走査の様子
を説明するための図、第2図は円弧アレイ振動子
による走査の様子を説明するための図、第3図は
本発明に係る超音波映像装置の要部の一実施例を
示す構成図である。 TD……圧電振動子、10……リニヤアレイ振
動子、20……円弧アレイ振動子、33……デイ
レーマツプ、34……デイレーライン、35……
スイツチ、36……パルサ。
FIG. 1 is a diagram for explaining the state of scanning by a linear array transducer, FIG. 2 is a diagram for explaining the state of scanning by an arcuate array transducer, and FIG. 3 is a diagram for explaining the state of scanning by an arcuate array transducer. FIG. 2 is a configuration diagram showing an example of a main part. TD...Piezoelectric vibrator, 10...Linear array vibrator, 20...Circular array vibrator, 33...Delay map, 34...Delay line, 35...
Switch, 36...Parsa.

Claims (1)

【特許請求の範囲】 1 リニヤアレイ振動子と円弧アレイ振動子を共
用し得る超音波映像装置において、 入出力端間で信号の双方向伝搬が可能であり、
入出力端間に設けられ入力された信号を互いに異
なる時間遅れで取り出し得る複数個の中間タツプ
を有してなるデイレーラインと、 このデイレーラインに対する信号入力を入力端
側とするか出力側とするかを切り換えるスイツチ
と、 前記デイレーラインの複数個の中間タツプにそ
れぞれ連結した複数個のラインと、前記使用され
るアレイ振動子の選択された複数個の振動子に通
ずる複数個のラインとをそれぞれ定められた位相
差の関係で接続してなるデイレーマツプ を具備し、前記デイレーマツプの接続状態は変え
ないで前記スイツチによる切り換えによりデイレ
ーラインの信号伝搬方向を変えるだけで、リニヤ
アレイ振動子用の時間遅れと円弧アレイ振動子用
の時間遅れが得られるようにしたことを特徴とす
る超音波映像装置。
[Claims] 1. In an ultrasound imaging device that can share a linear array transducer and an arc array transducer, bidirectional propagation of signals is possible between input and output terminals,
A delay line provided between input and output terminals and having a plurality of intermediate taps from which input signals can be taken out with different time delays; a plurality of lines respectively connected to the plurality of intermediate taps of the delay line, and a plurality of lines leading to the selected plurality of transducers of the array transducer to be used. and a delay map connected with each other with a predetermined phase difference relationship, and by simply changing the signal propagation direction of the delay line by switching with the switch without changing the connection state of the delay map, the signal propagation direction of the delay line can be changed. An ultrasonic imaging device characterized in that a time delay for an arc array transducer and a time delay for an arc array transducer can be obtained.
JP15116682A 1982-08-31 1982-08-31 Ultrasonic imaging apparatus Granted JPS5940279A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP15116682A JPS5940279A (en) 1982-08-31 1982-08-31 Ultrasonic imaging apparatus

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP15116682A JPS5940279A (en) 1982-08-31 1982-08-31 Ultrasonic imaging apparatus

Publications (2)

Publication Number Publication Date
JPS5940279A JPS5940279A (en) 1984-03-05
JPH0116393B2 true JPH0116393B2 (en) 1989-03-24

Family

ID=15512761

Family Applications (1)

Application Number Title Priority Date Filing Date
JP15116682A Granted JPS5940279A (en) 1982-08-31 1982-08-31 Ultrasonic imaging apparatus

Country Status (1)

Country Link
JP (1) JPS5940279A (en)

Also Published As

Publication number Publication date
JPS5940279A (en) 1984-03-05

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