JPH02111198A - Ultrasonic transducer - Google Patents

Ultrasonic transducer

Info

Publication number
JPH02111198A
JPH02111198A JP26357688A JP26357688A JPH02111198A JP H02111198 A JPH02111198 A JP H02111198A JP 26357688 A JP26357688 A JP 26357688A JP 26357688 A JP26357688 A JP 26357688A JP H02111198 A JPH02111198 A JP H02111198A
Authority
JP
Japan
Prior art keywords
piezoelectric ceramic
electrodes
electrode
ceramic vibrator
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.)
Pending
Application number
JP26357688A
Other languages
Japanese (ja)
Inventor
Keizo Tabuchi
田渕 恵三
Yoshimasa Yamashita
山下 義正
Katsuyoshi Ohira
大平 克義
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.)
Murata Manufacturing Co Ltd
Original Assignee
Murata Manufacturing Co 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 Murata Manufacturing Co Ltd filed Critical Murata Manufacturing Co Ltd
Priority to JP26357688A priority Critical patent/JPH02111198A/en
Publication of JPH02111198A publication Critical patent/JPH02111198A/en
Pending legal-status Critical Current

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  • Transducers For Ultrasonic Waves (AREA)

Abstract

PURPOSE:To reduce a side lobe near a main lobe by splitting an electrode formed to one face of a piezoelectric substance into plural electrodes concentrically and decreasing the degree of polarization of the piezoelectric substance beneath the split electrodes stepwise toward the outside. CONSTITUTION:An electrode 14 having a diameter slightly smaller than a diameter of a piezoelectric ceramic vibrator 12 is formed to nearly the entire left side face and three split electrodes 16, 18 and 20 are formed to the right side face of the piezoelectric ceramic vibrator 12 concentrically. The degree of polarization beneath the split electrodes 16-20 of the piezoelectric ceramic vibrator 12 is decreased stepwise toward the outside (peripheral part) from the center for each of the split electrodes 16, 18 and 20. Thus, the side lobe at 10 deg. and 350 deg. giving a large effect on the resolution is reduced to nearly a half as nearly 14dB.

Description

【発明の詳細な説明】 〔産業上の利用分野〕 この発明は超音波トランスジューサに関し、特にたとえ
ば水中ソナーなどのような水中通信機器に用いられ得る
、超音波トランスジューサに関する。
DETAILED DESCRIPTION OF THE INVENTION [Field of Industrial Application] The present invention relates to ultrasonic transducers, and more particularly to ultrasonic transducers that can be used in underwater communication equipment, such as underwater sonar.

(従来技術) この種の超音波トランスジューサでは、−Cに、第4図
において矢印で示すように、圧電磁器振動子1には一様
に分極処理が施されている。そして、円板状の圧電磁器
振動子1の主面には、全面電極2および3がそれぞれ対
向して形成される。
(Prior Art) In this type of ultrasonic transducer, the piezoelectric ceramic vibrator 1 is uniformly polarized as indicated by the arrow -C in FIG. Further, on the main surface of the disc-shaped piezoelectric ceramic vibrator 1, full-surface electrodes 2 and 3 are formed facing each other.

全面電極2および3間に所定の周波数の交流電圧が印加
されると、圧電磁器振動子1が振動して超音波が放射さ
れる。
When an alternating current voltage of a predetermined frequency is applied between the entire surface electrodes 2 and 3, the piezoelectric ceramic vibrator 1 vibrates and emits ultrasonic waves.

このようにして放射される超音波の指向特性が第5図で
示される。第5図図示の中のメインローブによって示さ
れる指向特性は鋭く、一般に、圧電磁器振動子1の直径
をDとし、超音波の波長をλとすると、D/λに逆比例
する。
The directional characteristics of the ultrasonic waves emitted in this way are shown in FIG. The directivity characteristic shown by the main lobe shown in FIG. 5 is sharp and is generally inversely proportional to D/λ, where D is the diameter of the piezoelectric ceramic vibrator 1 and λ is the wavelength of the ultrasonic wave.

〔発明が解決しようとする課題〕[Problem to be solved by the invention]

ところが、このような超音波トランスジューサでは、指
向特性は、一般に、第5図に示すように、比較的大きな
サイドローブを有する。たとえば、メインローブ(0°
)の近傍の±10° (100および350’)では、
サイドローブが25dBもあり、メインローブとの差が
小さく、したがって、角度の分解能があまりよくなかっ
た。
However, in such an ultrasonic transducer, the directional characteristics generally have relatively large side lobes, as shown in FIG. For example, the main lobe (0°
) in the vicinity of ±10° (100 and 350'),
The side lobe was as high as 25 dB, and the difference from the main lobe was small, so the angular resolution was not very good.

それゆえに、この発明の主たる目的は、角度の分解能の
よい、超音波トランスジューサを提供することである。
Therefore, a primary object of the present invention is to provide an ultrasonic transducer with good angular resolution.

〔課題を解決するための手段〕[Means to solve the problem]

この発明は、圧電体の対向する2面のそれぞれに電極を
形成した超音波トランスジューサにおいて、圧電体の一
方の面に形成する電極を同心状に複数に分割するととも
に、その分割電極直下の圧電体の分極度を外方に向かう
につれて段階的に小さくしたことを特徴とする、超音波
トランスジューサである。
In an ultrasonic transducer in which electrodes are formed on each of two opposing surfaces of a piezoelectric material, the electrode formed on one surface of the piezoelectric material is concentrically divided into a plurality of parts, and the piezoelectric material directly below the divided electrodes is This ultrasonic transducer is characterized in that the degree of polarization of the ultrasonic transducer is gradually decreased toward the outside.

〔作用〕[Effect]

圧電体の一方の面に形成される電極は同心状に複数に分
割されるが、他方の面には全面電極が形成される0分極
処理に際して、分割電極と全面電極との間には、外方に
向かうにつれて段階的に小さくなる直流電圧が印加され
る。したがって、各分割電極直下の圧電体の分極度は、
外方に向かうにつれて段階的に小さくなる。
The electrode formed on one surface of the piezoelectric material is concentrically divided into a plurality of parts, but during the zero polarization process in which a full-surface electrode is formed on the other surface, an external electrode is formed between the divided electrode and the full-surface electrode. A DC voltage is applied that gradually decreases toward the opposite direction. Therefore, the degree of polarization of the piezoelectric material directly under each divided electrode is
It gradually becomes smaller as it goes outward.

このような構造により、圧電振動子の放射面において、
従来は全面が均一にピストン運動していたのに対し、中
央部が最大で周辺部に向かうにつれて段階的に小さくな
る振幅分布を持つ運動をする。したがって、サイドロー
ブ、特にメインローブ近傍のサイドローブが小さ(なる
With this structure, on the radiation surface of the piezoelectric vibrator,
In the past, the piston moved uniformly over the entire surface, but the piston moves with an amplitude distribution that is maximum at the center and gradually decreases toward the periphery. Therefore, the side lobes, especially the side lobes near the main lobe, become small.

〔発明の効果〕〔Effect of the invention〕

この発明によれば、メインローブ近傍のサイドローブが
小さくなるので、メインローブによる角度の分解能が向
上する。
According to this invention, the side lobes near the main lobe are reduced, so the angular resolution of the main lobe is improved.

この発明の上述の目的、その他の目的、特徴および利点
は、図面を参照して行う以下の実施例の詳細な説明°か
ら一層明らかとなろう。
The above objects, other objects, features and advantages of the present invention will become more apparent from the following detailed description of embodiments with reference to the drawings.

〔実施例〕〔Example〕

第1図はこの発明の一実施例を示す断面図解図であり、
第2A図は右側面図、第2B図は左側面図である。超音
波トランスジューサ10は圧電磁器振動子12を含み、
圧電磁器振動子I2ばたとえば直径50φ、厚さ12.
5111111のセラミック焼成ユニットによって構成
される。そして、左側面(他方面)には、はぼ全面に、
圧電磁器振動子12の直径より若干小さい直径の電極1
4が形成される。圧電磁器振動子12の右側面(一方面
)には、同心状に、3つの分割電極16.18および2
0が形成される。
FIG. 1 is an illustrative cross-sectional view showing one embodiment of the present invention.
FIG. 2A is a right side view, and FIG. 2B is a left side view. The ultrasonic transducer 10 includes a piezoelectric ceramic vibrator 12,
For example, the piezoelectric ceramic vibrator I2 has a diameter of 50φ and a thickness of 12.
It is composed of 5111111 ceramic firing units. And on the left side (other side), there is a
Electrode 1 with a diameter slightly smaller than the diameter of piezoelectric ceramic vibrator 12
4 is formed. On the right side (one side) of the piezoelectric ceramic vibrator 12, three divided electrodes 16, 18 and 2 are arranged concentrically.
0 is formed.

圧電磁器振動子12に圧電性を付与するための分極処理
は、電極16〜20のそれぞれと、電極。
The polarization treatment for imparting piezoelectricity to the piezoelectric ceramic vibrator 12 is performed on each of the electrodes 16 to 20 and the electrode.

14との間に直流電圧を印加することによって行う。こ
の実施例では、たとえば、分割電極16および全面電極
14間にPVの電圧を印加するとすれば、分割電極18
および全面電極14間に印加する電圧は0.7PV、分
割電極20および全面電極14間に印加する電圧は0,
2PVに設定される。このような比率で分極電圧を印加
すると、圧電磁器振動子12の各分割電極16〜20直
下の分極度は、第1図で矢印で示すように、中心から外
方(周辺部)に向かうにつれて各分割電極16.18そ
して20毎に段階的に小さくなる。
This is done by applying a DC voltage between the In this embodiment, for example, if a PV voltage is applied between the divided electrode 16 and the entire surface electrode 14, the divided electrode 18
The voltage applied between the entire surface electrode 14 is 0.7 PV, and the voltage applied between the divided electrode 20 and the entire surface electrode 14 is 0.
It is set to 2PV. When a polarization voltage is applied at such a ratio, the degree of polarization directly below each of the divided electrodes 16 to 20 of the piezoelectric ceramic vibrator 12 increases from the center toward the outside (periphery), as shown by the arrows in FIG. Each segmented electrode 16, 18 and 20 becomes progressively smaller.

このような超音波トランスジューサ10において、全面
電極I4と電極16〜20との間にたとえば200kH
zの交流電圧を印加すると超音波が放射され、その指向
特性が第3図で示される。
In such an ultrasonic transducer 10, for example, 200 kHz is applied between the entire surface electrode I4 and the electrodes 16 to 20.
When an alternating current voltage of z is applied, ultrasonic waves are emitted, and their directional characteristics are shown in FIG.

このとき、圧電磁器振動子12の分極度は一様でないの
で、中央部から周辺部に向かうにつれて振幅が小さくな
るような運動を生じる。したがって、メインローブ(0
”)は、第5図で示す従来のものに比べて若干小さくな
るものの、分解能に大きな影響を及ぼす10°および3
50°でのサイドローブは、従来は24dB近くあった
のが、約14dBと半減する。したがって、メインロー
ブどサイドローブとの差は結果的に大きくなり、分解能
が著しく向上する。
At this time, since the degree of polarization of the piezoelectric ceramic vibrator 12 is not uniform, a movement occurs in which the amplitude decreases from the center toward the periphery. Therefore, the main lobe (0
”) is slightly smaller than the conventional one shown in Figure 5, but the 10° and 3° angles have a large effect on resolution.
The side lobe at 50°, which used to be nearly 24 dB, has been halved to about 14 dB. Therefore, the difference between the main lobe and the side lobe becomes large as a result, and the resolution is significantly improved.

なお、上述の実施例では、圧電磁器振動子12の一方の
面には3つの分割電極16.18および20を形成した
が、この分割数は2以上の任意の複数であればよい。
In the above embodiment, three divided electrodes 16, 18 and 20 were formed on one surface of the piezoelectric ceramic vibrator 12, but the number of divided electrodes may be any number greater than or equal to two.

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

第1図はこの発明の一実施例を示す断面図解図である。 第2A図および第2B図は、それぞれ、第1図実施例の
右側面図および左側面図である。 第3図は第1図実施例の指向特性を示すグラフである。 第4図は従来の超音波トランスジューサの一例を示す断
面図解図である。 第5図は従来の超音波トランスジューサの指向特性を示
すグラフである。 図において、10は超音波トランスジューサ、12は圧
電磁器振動子、14は全面電極、16〜20は電極を示
す。 第2B図 特許出願人 株式会社 村田製作所 代理人 弁理士 山 1) 義 人 第4 図 第2A図
FIG. 1 is an illustrative cross-sectional view showing one embodiment of the present invention. 2A and 2B are a right side view and a left side view, respectively, of the FIG. 1 embodiment. FIG. 3 is a graph showing the directional characteristics of the embodiment shown in FIG. FIG. 4 is an illustrative cross-sectional view showing an example of a conventional ultrasonic transducer. FIG. 5 is a graph showing the directivity characteristics of a conventional ultrasonic transducer. In the figure, 10 is an ultrasonic transducer, 12 is a piezoelectric ceramic vibrator, 14 is a full surface electrode, and 16 to 20 are electrodes. Figure 2B Patent Applicant Murata Manufacturing Co., Ltd. Representative Patent Attorney Yama 1) Yoshihito 4 Figure 2A

Claims (1)

【特許請求の範囲】 圧電体の対向する2面のそれぞれに電極を形成した超音
波トランスジューサにおいて、 前記圧電体の一方の面に形成する電極を同心状に複数に
分割するとともに、その分割電極直下の前記圧電体の分
極度を外方に向かうにつれて段階的に小さくしたことを
特徴とする、超音波トランスジューサ。
[Scope of Claims] In an ultrasonic transducer in which electrodes are formed on each of two opposing surfaces of a piezoelectric body, the electrode formed on one surface of the piezoelectric body is concentrically divided into a plurality of parts, and a portion directly below the divided electrodes is provided. An ultrasonic transducer characterized in that the degree of polarization of the piezoelectric body is gradually decreased toward the outside.
JP26357688A 1988-10-19 1988-10-19 Ultrasonic transducer Pending JPH02111198A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP26357688A JPH02111198A (en) 1988-10-19 1988-10-19 Ultrasonic transducer

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP26357688A JPH02111198A (en) 1988-10-19 1988-10-19 Ultrasonic transducer

Publications (1)

Publication Number Publication Date
JPH02111198A true JPH02111198A (en) 1990-04-24

Family

ID=17391474

Family Applications (1)

Application Number Title Priority Date Filing Date
JP26357688A Pending JPH02111198A (en) 1988-10-19 1988-10-19 Ultrasonic transducer

Country Status (1)

Country Link
JP (1) JPH02111198A (en)

Cited By (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPH1127798A (en) * 1997-07-04 1999-01-29 S C:Kk Method for generating ultrasonic vibration
US11715448B2 (en) 2018-05-30 2023-08-01 Roland Corporation Electronic wind instrument and method for manufacturing electronic wind instrument

Cited By (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPH1127798A (en) * 1997-07-04 1999-01-29 S C:Kk Method for generating ultrasonic vibration
US11715448B2 (en) 2018-05-30 2023-08-01 Roland Corporation Electronic wind instrument and method for manufacturing electronic wind instrument

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