JPH04293399A - Array type piezoelectric transducer - Google Patents

Array type piezoelectric transducer

Info

Publication number
JPH04293399A
JPH04293399A JP9158567A JP5856791A JPH04293399A JP H04293399 A JPH04293399 A JP H04293399A JP 9158567 A JP9158567 A JP 9158567A JP 5856791 A JP5856791 A JP 5856791A JP H04293399 A JPH04293399 A JP H04293399A
Authority
JP
Japan
Prior art keywords
axis direction
short axis
electrode
short
weighting
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.)
Pending
Application number
JP9158567A
Other languages
Japanese (ja)
Inventor
Shinichiro Umemura
晋一郎 梅村
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.)
Hitachi Ltd
Original Assignee
Hitachi 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 Hitachi Ltd filed Critical Hitachi Ltd
Priority to JP9158567A priority Critical patent/JPH04293399A/en
Publication of JPH04293399A publication Critical patent/JPH04293399A/en
Pending legal-status Critical Current

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

Abstract

PURPOSE:To realize excellent resolution in the direction of a short axis while maintaining an enough focal depth by controlling the effective area of the electrode of a piezoelectric element. CONSTITUTION:The effective area of the electrode of piezoelectric elements 1-1 to 1-N is weighted by making the area projected in the direction of a long axis per the unit length in the short axis direction large at the center part of an opening and making it smaller toward the end part. By such weighting in the short axis direction, the transmission sound pressure and receiving sensitivity of an ultrasonic wave in the short axis direction can be made large at the center part of the opening and made smaller toward the end part. At this time, a repetitive pitch in the long axis direction of the shape of the electrode is set below a half wave length. Thus, the formation of grating lobe caused by the weighting in the short axis direction can be prevented.

Description

【発明の詳細な説明】[Detailed description of the invention]

【0001】0001

【産業上の利用分野】本発明は、医療診断用をはじめと
し、探傷用,水中探索用などの電子走査型超音波撮像装
置に用いられるアレイ型圧電変換器に関する。
BACKGROUND OF THE INVENTION 1. Field of the Invention The present invention relates to an array type piezoelectric transducer used in electronic scanning ultrasonic imaging devices for medical diagnosis, flaw detection, underwater exploration, and the like.

【0002】0002

【従来の技術】電子走査型超音波撮像装置は、手動ある
いは自動の機械走査型装置と比較してはるかに優れた走
査の自由度ならびに高速性を有するため、医療診断をは
じめとし、水中探索、探傷などの各分野において広く用
いられている。このような電子走査型超音波撮像装置に
おいて超音波信号・電気信号の変換を行なうためには、
通常、平面または曲面の上に電気的に独立な多数の圧電
素子を配列したアレイ型圧電変換器が用いられている。 すなわち、アレイ型圧電変換器の各素子による超音波の
送信・受信のタイミングやゲインを電気的に制御するこ
とにより、撮像に必要な超音波音場を形成する。
BACKGROUND OF THE INVENTION Electronic scanning ultrasonic imaging devices have far superior scanning freedom and high speed compared to manual or automatic mechanical scanning devices, and are therefore useful for medical diagnosis, underwater exploration, and other applications. It is widely used in various fields such as flaw detection. In order to convert ultrasound signals and electrical signals in such an electronic scanning ultrasound imaging device,
Generally, an array type piezoelectric transducer is used in which a large number of electrically independent piezoelectric elements are arranged on a flat or curved surface. That is, by electrically controlling the timing and gain of ultrasonic transmission/reception by each element of the array type piezoelectric transducer, an ultrasonic sound field necessary for imaging is formed.

【0003】撮像にとって理想的な送信ならびに受信の
超音波音場の形成をフレキシブルに行なうためには、圧
電素子の電気的独立性に関し、平面または曲面の上の特
定の1次元方向に限ることなく、本来、2次元方向に独
立性を与えるべきである。しかしながら、そのためには
、電気的独立性を1次元方向に限ったときに100素子
程度ですんでいた1つのアレイ型圧電変換器あたりの素
子数が、1000〜10000素子必要となり、それに
必要な引き出し線数ならびに電子回路規模は膨大なもの
となる。従って、2次元アレイ型圧電変換器による超音
波撮像は、圧電変換器用に使うことのできる高耐圧電子
回路の一層の小型化が進まないかぎり、現時点において
は必ずしも実用的でない。
[0003] In order to flexibly form the ultrasonic sound field for transmission and reception that is ideal for imaging, the electrical independence of the piezoelectric element must not be limited to a specific one-dimensional direction on a flat or curved surface. , originally, independence should be given in two-dimensional directions. However, in order to achieve this, the number of elements per array-type piezoelectric transducer, which used to be about 100 when electrical independence is limited to one dimension, will now need 1000 to 10000 elements, and the number of lead wires required for this will increase. The number and scale of electronic circuits will be enormous. Therefore, ultrasonic imaging using two-dimensional array type piezoelectric transducers is not necessarily practical at present unless high voltage electronic circuits that can be used for piezoelectric transducers become further miniaturized.

【0004】電気的独立性を1次元方向に限った1次元
アレイ型圧電変換器による超音波撮像の問題点は、アレ
イ配列の平面あるいは曲面に含まれ、アレイの配列方向
(長軸と呼ばれる)に垂直な軸(短軸と呼ばれる)の方
向の超音波音場の形成である。短軸方向にも、長軸方向
と同じように分解能を得るため、音響的円柱レンズを取
り付けるか圧電素子そのものに曲率を与えることにより
集束をおこなうことは可能であり、現に、現在実用に供
している多くの超音波診断装置のアレイ型圧電変換器の
多くがそのような構成となっている。この短軸集束によ
り、短軸方向の分解能は、その短軸集束の焦点距離程度
の距離において格段に向上する反面、その焦点距離から
大幅に離れた距離においては充分な短軸方向分解能が得
られず、短軸集束がないときに比べても劣化してしまう
ことすらある。この問題を解決するためには、充分な大
きさの焦点深度を維持しながら、良好な短軸方向分解能
を実現する短軸集束方法が必要である。
[0004] The problem with ultrasonic imaging using a one-dimensional array type piezoelectric transducer whose electrical independence is limited to one-dimensional direction is that it is included in the plane or curved surface of the array arrangement, and the direction of the array arrangement (called the long axis) is the formation of an ultrasonic sound field in the direction of the axis perpendicular to (called the minor axis). In order to obtain the same resolution in the short-axis direction as in the long-axis direction, it is possible to perform focusing by attaching an acoustic cylindrical lens or by adding curvature to the piezoelectric element itself. Many of the array-type piezoelectric transducers used in many ultrasonic diagnostic apparatuses have such a configuration. Due to this short-axis focusing, the resolution in the short-axis direction is significantly improved at a distance that is about the focal length of the short-axis focusing, but sufficient short-axis resolution cannot be obtained at distances significantly away from the focal length. In fact, it may even deteriorate compared to when there is no short-axis focusing. To solve this problem, a short-axis focusing method is needed that achieves good short-axis resolution while maintaining a sufficiently large depth of focus.

【0005】上記問題を解決する一般的方法として、超
音波の送信音圧および受信感度を、短軸方向に関して開
口の中央部で高く、端部に行くにしたがって低くする重
み付けを行なう方法が知られている。
[0005] As a general method for solving the above problem, a method is known in which the transmitting sound pressure and receiving sensitivity of ultrasonic waves are weighted such that they are higher in the center of the aperture in the short axis direction and lower toward the ends. ing.

【0006】このような重み付けを実現できる可能性の
ある一案として、アレイ型圧電変換器を構成する圧電素
子の分極強度について短軸方向に分布を与える方法が提
案されている。すなわち、分極強度について、開口の中
央部では100%分極し、端部に行くにしたがって分極
の程度を減らしていくことにより、必要な重み付けを行
なおうとするものであり、分極時の印加電圧を制御する
ことにより望ましい分極の程度を得る手法が提案されて
いる。この提案は、比較的簡便に重み付けを可能とする
ように見えるが、実際には、高温下で高電圧をかけて行
なわれる分極工程において、隣接する電極間で印加電圧
に差をつけて分極を行なうのは容易なことではない。ま
た、中途半端に分極された圧電材料の特性は、100%
分極されたものと比較して質的に異なる場合もあるので
、この点も実用上注意を要する。なお、本発明に関連す
る従来技術として、日本超音波医学会講演論文集57−
285「短軸方向の高分解能化の基礎検討」を挙げるこ
とができる。
As a possible method for realizing such weighting, a method has been proposed in which the polarization strength of piezoelectric elements constituting an array type piezoelectric transducer is distributed in the minor axis direction. In other words, the polarization intensity is 100% polarized at the center of the aperture, and the degree of polarization is reduced toward the edges to achieve the necessary weighting, and the applied voltage at the time of polarization is A method for obtaining a desired degree of polarization through control has been proposed. This proposal seems to enable weighting relatively easily, but in reality, in the polarization process, which is performed under high temperature and high voltage, polarization is achieved by applying a difference in voltage between adjacent electrodes. It's not an easy thing to do. In addition, the characteristics of a piezoelectric material that is half-polarized are 100%
Since there may be qualitative differences compared to polarized ones, this point also requires attention in practical terms. In addition, as a prior art related to the present invention, Japanese Society of Ultrasonics in Medicine Proceedings 57-
285 ``Basic study of high resolution in short axis direction''.

【0007】[0007]

【発明が解決しようとする課題】本発明は、以上の点を
鑑みてなされたもので、より実用性の高い短軸重み付け
方法により、充分な大きさの焦点深度を維持しながら、
良好な短軸方向分解能を実現しようとするものである。
SUMMARY OF THE INVENTION The present invention has been made in view of the above points, and uses a more practical short-axis weighting method to maintain a sufficiently large depth of focus.
The objective is to achieve good resolution in the short axis direction.

【0008】[0008]

【課題を解決するための手段】分極の程度を制御するこ
とにより重み付けを実現することは、先に述べたように
必ずしも容易ではないので、本発明では、分極の程度の
代わりに圧電素子の電極の実効面積を制御することによ
り実現する。すなわち、電極実効面積について、短軸方
向単位長さあたりの長軸方向に投影した面積を、開口の
中央部で大きく、端部に行くにしたがって小さくするこ
とにより重み付けを行なう。ただし、重み付けのための
電極形状によっては、不要応答の一種であるグレイティ
ング・ロ−ブを形成してしまう恐れがあるので、この点
に配慮し、電極形状の繰り返しピッチは、半波長以下と
する。
[Means for Solving the Problems] As mentioned above, it is not necessarily easy to realize weighting by controlling the degree of polarization, so in the present invention, instead of controlling the degree of polarization, the This is achieved by controlling the effective area of That is, the effective area of the electrode is weighted by making the area projected in the long axis direction per unit length in the short axis direction larger at the center of the opening and smaller toward the ends. However, depending on the shape of the electrodes used for weighting, there is a risk of forming a grating lobe, which is a type of unnecessary response. do.

【0009】[0009]

【作用】電極実効面積に分布を与えることによる短軸方
向重み付けにより、分極の制御に依存することなく、超
音波の送信音圧および受信感度を、短軸方向に関して開
口の中央部で高く、端部に行くにしたがって低くするこ
とができ、充分な大きさの焦点深度を維持しながら、良
好な短軸方向分解能を実現することができた。
[Operation] Weighting in the short axis direction by giving a distribution to the effective area of the electrodes allows the transmission sound pressure and reception sensitivity of ultrasound to be high in the center of the aperture in the short axis direction, and high at the edges, without depending on polarization control. The depth of focus can be lowered as the depth of focus increases, and good short-axis resolution can be achieved while maintaining a sufficiently large depth of focus.

【0010】0010

【実施例】以下、本発明の実施例を図1〜図2を用いて
詳細に説明する。
Embodiments Hereinafter, embodiments of the present invention will be explained in detail with reference to FIGS. 1 and 2.

【0011】本発明の一実施例のアレイ型圧電変換器の
電極形状を図1に示す。電気・機械変換は、圧電セラミ
クスまたは圧電高分子など圧電材料に対し、厚み方向に
電界をかけたときに生ずる厚み変位ならびに厚み方向に
応力がかかったときに厚み方向に生ずる分極により行な
い、音響整合層などを介して接触する生体または水中へ
超音波を送信したり、逆に、それらからの超音波を受信
する。超音波周波数3MHz(生体または水中における
波長0.5mm)、短軸長10mm、電極形状の長軸方
向繰り返しピッチ0.25mm(半波長に相当する)、
素子ピッチ0.5mmのアレイ型圧電変換器の接地電極
に対向する電極の形状を、その短軸に関する対称軸の片
側について図示した。アレイ型圧電変換器全体は、実際
には100個程度の多数の素子からなるが、図では、そ
の一部について示した。
FIG. 1 shows the electrode shape of an array type piezoelectric transducer according to an embodiment of the present invention. Electrical-mechanical conversion is performed by the thickness displacement that occurs when an electric field is applied in the thickness direction of piezoelectric materials such as piezoelectric ceramics or piezoelectric polymers, and the polarization that occurs in the thickness direction when stress is applied in the thickness direction. It transmits ultrasonic waves to the living body or water it comes into contact with through layers, and conversely receives ultrasonic waves from them. Ultrasonic frequency 3 MHz (wavelength 0.5 mm in living body or water), short axis length 10 mm, long axis direction repetition pitch of electrode shape 0.25 mm (equivalent to half wavelength),
The shape of the electrode facing the ground electrode of an array type piezoelectric transducer with an element pitch of 0.5 mm is illustrated on one side of the axis of symmetry with respect to its short axis. The entire array type piezoelectric transducer actually consists of a large number of elements, about 100, but only a portion of them are shown in the figure.

【0012】素子ピッチが生体または水中における半波
長より大きいので、それを2分割した幅に電極形状の長
軸方向繰り返しピッチを設定し、隣接する繰り返しピッ
チ2個分を電気的に共通接続して、電気的に独立したア
レイ素子として扱っている。これによって、電極形状の
長軸方向繰り返しピッチを半波長以下に抑えることがで
き、短軸方向重み付けに起因するグレイティング・ロ−
ブの形成を防ぐことができた。図1の右側には、電極実
効面積について、短軸方向単位長さあたりの長軸方向に
投影した面積を、短軸方向座標についてプロットした。 単位長さあたり投影面積を、開口の中央部で大きく、端
部に行くにしたがって小さくすることにより、目的とす
る重み付けが行なわれるよう構成されている。
Since the element pitch is larger than half a wavelength in a living body or underwater, the repeating pitch in the long axis direction of the electrode shape is set to the width divided into two, and two adjacent repeating pitches are electrically connected in common. , treated as electrically independent array elements. As a result, the repetition pitch in the long axis direction of the electrode shape can be suppressed to less than half a wavelength, and the grating rotation caused by weighting in the short axis direction can be suppressed.
It was possible to prevent the formation of blisters. On the right side of FIG. 1, regarding the effective area of the electrode, the area projected in the major axis direction per unit length in the minor axis direction is plotted with respect to the coordinate in the minor axis direction. The projected area per unit length is large at the center of the aperture and becomes smaller toward the ends, thereby achieving the desired weighting.

【0013】本発明の他の一実施例のアレイ型圧電変換
器の電極形状を図2に示す。電気・機械変換の原理,超
音波周波数,短軸長,電極形状の長軸方向繰り返しピッ
チ,素子ピッチなどは、図1の実施例と同様であり、接
地電極に対向する電極の形状を、アレイの一部について
、その短軸に関する対称軸の片側を図示した。本実施例
では、接地電極に対向する電極を短軸方向にも半波長以
下に細分し、細分した電極間のギャップを、開口の中央
部で小さく、端部に行くにしたがって大きくすることに
より、目的とする重み付けが行なわれるよう構成されて
いる。隣接する長軸方向繰り返しピッチ2個分について
、短軸方向・長軸方向に細分された電極を電気的に共通
接続して、電気的に独立したアレイ素子として扱ってい
る。図2の右側には、短軸方向単位長さあたりの長軸方
向に投影した電極実効面積を、短軸方向座標についてプ
ロットした。単位長さあたり投影面積が、開口の中央部
で大きく、端部に行くにしたがって小さくなっている。
FIG. 2 shows the electrode shape of an array type piezoelectric transducer according to another embodiment of the present invention. The principles of electrical/mechanical conversion, ultrasonic frequency, short axis length, electrode shape repetition pitch in the long axis direction, element pitch, etc. are the same as in the embodiment shown in Fig. 1, and the shape of the electrode facing the ground electrode is One side of the axis of symmetry with respect to its short axis is illustrated for a portion of the figure. In this example, the electrode facing the ground electrode is subdivided into half wavelengths or less in the short axis direction, and the gap between the subdivided electrodes is made smaller at the center of the opening and becomes larger toward the ends. The configuration is such that the desired weighting is performed. For two adjacent repeating pitches in the long axis direction, the electrodes subdivided in the short axis direction and the long axis direction are electrically connected in common and treated as electrically independent array elements. On the right side of FIG. 2, the effective area of the electrode projected in the long axis direction per unit length in the short axis direction is plotted with respect to the short axis direction coordinate. The projected area per unit length is large at the center of the opening and becomes smaller toward the ends.

【0014】本実施例においては、PZT系セラミクス
などを圧電材料として用い、図2における細分した電極
間のギャップの部分をセラミクスを圧電活性のない高分
子材料に置き換えた、いわゆる複合圧電体構造をとるこ
ともできる。この構造をとる場合には、電気的に独立し
たアレイ素子として扱っている範囲の電極は連続電極と
してもよい。その場合でも、圧電活性のない高分子材料
の上に置かれた電極は電極実効面積にかぞえられないの
で、図2の右側にプロットした単位長さあたり投影面積
は、同様のものとなる。
In this example, a so-called composite piezoelectric structure is created in which PZT-based ceramics or the like is used as the piezoelectric material, and the gap between the subdivided electrodes in FIG. 2 is replaced with a polymeric material that has no piezoelectric activity. You can also take it. When this structure is adopted, the electrodes in the range treated as electrically independent array elements may be continuous electrodes. Even in that case, since an electrode placed on a polymer material with no piezoelectric activity is not counted as the effective area of the electrode, the projected area per unit length plotted on the right side of FIG. 2 will be the same.

【0015】[0015]

【発明の効果】以上述べたごとく、本発明によれば、ア
レイ素子の送信および受信感度を、短軸方向に関して開
口の中央部で高く、端部に行くにしたがって低くするこ
とができ、その結果として、良好な短軸方向分解能を確
保しながら、実用に充分な大きさの焦点深度を実現する
ことができる。
[Effects of the Invention] As described above, according to the present invention, the transmission and reception sensitivities of the array element can be made high at the center of the aperture in the short axis direction and decreased toward the ends. As a result, it is possible to achieve a depth of focus large enough for practical use while ensuring good resolution in the short axis direction.

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

【図1】本発明の一実施例の電極形状を示す図。FIG. 1 is a diagram showing the shape of an electrode according to an embodiment of the present invention.

【図2】本発明の他の一実施例の電極形状を示す図。FIG. 2 is a diagram showing the shape of an electrode according to another embodiment of the present invention.

【符号の説明】[Explanation of symbols]

1―1〜1―N…アレイ型圧電変換器を構成する電気的
に独立な圧電素子。
1-1 to 1-N...Electrically independent piezoelectric elements constituting an array type piezoelectric transducer.

Claims (1)

【特許請求の範囲】[Claims] 【請求項1】同一形状の圧電素子多数を一次元方向に配
列してなる電子走査型超音波変換器において、圧電素子
の電極有効面積を配列方向に投影してできる分布に関し
、開口中央部の単位長さあたり分布密度を端部よりも大
きくしたことを特徴とするアレイ型圧電変換器。
Claim 1: In an electronic scanning ultrasonic transducer in which a large number of piezoelectric elements of the same shape are arranged in a one-dimensional direction, a distribution obtained by projecting the electrode effective area of the piezoelectric elements in the arrangement direction is determined. An array type piezoelectric transducer characterized in that the distribution density per unit length is greater than that at the ends.
JP9158567A 1991-03-22 1991-03-22 Array type piezoelectric transducer Pending JPH04293399A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP9158567A JPH04293399A (en) 1991-03-22 1991-03-22 Array type piezoelectric transducer

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP9158567A JPH04293399A (en) 1991-03-22 1991-03-22 Array type piezoelectric transducer

Publications (1)

Publication Number Publication Date
JPH04293399A true JPH04293399A (en) 1992-10-16

Family

ID=13088023

Family Applications (1)

Application Number Title Priority Date Filing Date
JP9158567A Pending JPH04293399A (en) 1991-03-22 1991-03-22 Array type piezoelectric transducer

Country Status (1)

Country Link
JP (1) JPH04293399A (en)

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