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JPS6350885B2 - - Google Patents
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JPS6350885B2 - - Google Patents

Info

Publication number
JPS6350885B2
JPS6350885B2 JP10218184A JP10218184A JPS6350885B2 JP S6350885 B2 JPS6350885 B2 JP S6350885B2 JP 10218184 A JP10218184 A JP 10218184A JP 10218184 A JP10218184 A JP 10218184A JP S6350885 B2 JPS6350885 B2 JP S6350885B2
Authority
JP
Japan
Prior art keywords
sound wave
path
glass plate
curved surface
piezoelectric ceramic
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
JP10218184A
Other languages
Japanese (ja)
Other versions
JPS59229916A (en
Inventor
Katsumi Narita
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.)
Panasonic Holdings Corp
Original Assignee
Matsushita Electric Industrial 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 Matsushita Electric Industrial Co Ltd filed Critical Matsushita Electric Industrial Co Ltd
Priority to JP59102181A priority Critical patent/JPS59229916A/en
Publication of JPS59229916A publication Critical patent/JPS59229916A/en
Publication of JPS6350885B2 publication Critical patent/JPS6350885B2/ja
Granted legal-status Critical Current

Links

Classifications

    • HELECTRICITY
    • H03ELECTRONIC CIRCUITRY
    • H03HIMPEDANCE NETWORKS, e.g. RESONANT CIRCUITS; RESONATORS
    • H03H9/00Networks comprising electromechanical or electro-acoustic elements; Electromechanical resonators
    • H03H9/30Time-delay networks
    • H03H9/36Time-delay networks with non-adjustable delay time

Landscapes

  • Physics & Mathematics (AREA)
  • Acoustics & Sound (AREA)
  • Piezo-Electric Or Mechanical Vibrators, Or Delay Or Filter Circuits (AREA)

Description

【発明の詳細な説明】 本発明はガラス等の遅延媒体に入力および出力
の両機能を備えた一つの圧電変換素子を取付けて
なる超音波遅延線に関するものであり、特に上記
圧電変換素子より放射された音波が指向性を持つ
ことによつて生ずる伝搬路のずれを修正して変換
効率を向上させた超音波遅延線を提供するもので
ある。
DETAILED DESCRIPTION OF THE INVENTION The present invention relates to an ultrasonic delay line in which one piezoelectric transducer having both input and output functions is attached to a delay medium such as glass. The present invention provides an ultrasonic delay line that improves conversion efficiency by correcting deviations in propagation paths caused by the directivity of the transmitted sound waves.

一つの発射源から放射される波は発射源からあ
る一定の広がりをもつて伝搬するため、発射源の
方向によつて強さが異なり、一般に波のこのよう
な現象は指向性と呼ばれる。指向性は波の周波数
によつて異なり、周波数の低い波ほど発射源の主
軸からはずれて伝搬しやすい。遅延媒体中を伝搬
する音波を利用する超音波遅延線においては、音
波が上記指向性のため所定の伝搬路よりずれるた
め圧電変換素子における機械−電気変換効率が低
下するという欠点があつた。
Waves emitted from a single source propagate with a certain spread from the source, so the strength varies depending on the direction of the source, and this phenomenon of waves is generally called directional. Directivity varies depending on the wave frequency, and waves with lower frequencies tend to propagate further away from the main axis of the emission source. Ultrasonic delay lines that utilize sound waves propagating in a delay medium have the disadvantage that the sound waves deviate from a predetermined propagation path due to the above-mentioned directivity, resulting in a reduction in mechanical-electrical conversion efficiency in the piezoelectric transducer element.

この欠点を従来の遅延線を示す第1図をもとに
して具体的に説明する。同図において、1は遅延
媒体となるガラス板であり、このガラス板1の一
側面には電極2が形成されている。3は入力およ
び出力の両機能を備えた圧電磁器板であり、この
圧電磁器板3は前記電極2に半田付け等により取
付けられている。4は前記圧電磁器板3に取付け
られた電極であり、この電極4および前記電極2
にはそれぞれリード線5a,5bが接続されてい
る。
This drawback will be specifically explained with reference to FIG. 1, which shows a conventional delay line. In the figure, 1 is a glass plate serving as a delay medium, and an electrode 2 is formed on one side of this glass plate 1. 3 is a piezoelectric ceramic plate having both input and output functions, and this piezoelectric ceramic plate 3 is attached to the electrode 2 by soldering or the like. 4 is an electrode attached to the piezoelectric ceramic plate 3, and this electrode 4 and the electrode 2
Lead wires 5a and 5b are connected to these, respectively.

第1図において、リード線5aと5b間に信号
電圧を印加すると、信号電圧は圧電磁器板3によ
つて機械振動をする音波に変換され、ガラス板1
の反射平面1aに向かつて伝搬する。この時、音
波は指向性を有するため主軸方向に伝搬する音波
成分6aと、主軸方向よりずれた音波成分6b,
6c等が発生する。主軸方向に伝搬する音波成分
6aはガラス板1の反射平面1aに90゜の角度で
入射され、入射経路と同一の反射経路を通つて圧
電磁器板3にもどり、機械−電気変換が行なわれ
てリード線5b,5b間より2l/V(lはガラス板 1における図示の長さ、Vは音波の速度)だけ遅
延した信号電圧が得られる。一方、主軸方向より
ずれた音波成分6b,6c等はガラス板1の反射
平面1aに90゜以外の角度で入射するため、反射
波6′b,6′cは入射経路と異なつた反射経路を
通り、圧電磁器板3にはもどつてこない。
In FIG. 1, when a signal voltage is applied between lead wires 5a and 5b, the signal voltage is converted into a sound wave that vibrates mechanically by the piezoelectric ceramic plate 3, and the glass plate 1
The light propagates toward the reflection plane 1a of . At this time, since the sound waves have directivity, a sound wave component 6a propagates in the direction of the main axis, a sound wave component 6b that deviates from the direction of the main axis,
6c etc. occur. The sound wave component 6a propagating in the principal axis direction is incident on the reflection plane 1a of the glass plate 1 at an angle of 90°, returns to the piezoelectric ceramic plate 3 through the same reflection path as the incident path, and undergoes mechanical-electrical conversion. A signal voltage delayed by 2l/V (l is the illustrated length of the glass plate 1, V is the speed of the sound wave) from between the lead wires 5b and 5b is obtained. On the other hand, since the sound wave components 6b, 6c, etc. shifted from the principal axis direction are incident on the reflection plane 1a of the glass plate 1 at an angle other than 90°, the reflected waves 6'b, 6'c follow a reflection path different from the incident path. However, it does not return to the piezoelectric ceramic plate 3.

以上説明したように、従来の超音波遅延線では
音波の指向性のため圧電変換素子にもどつてこな
い音波成分が生じ、特に遅延媒体が長い場合また
は音波の周波数が低い場合に、上記音波成分の主
軸からのずれが大きく、変換効率が低下してい
た。
As explained above, in conventional ultrasonic delay lines, due to the directivity of the sound waves, sound wave components that do not reach the piezoelectric transducer are generated, and especially when the delay medium is long or the frequency of the sound waves is low, the sound wave components are The deviation from the main axis was large, resulting in a decrease in conversion efficiency.

上記欠点を補うために、信号の周波数を高くし
たり、また圧電変換素子の寸法を大きくする等の
試みがなされているが、信号の周波数や圧電変換
素子には、その超音波遅延線に適した値があるた
め、上記方法は適切ではなかつた。
In order to compensate for the above drawbacks, attempts have been made to increase the signal frequency and increase the dimensions of the piezoelectric transducer, but the signal frequency and piezoelectric transducer are not suitable for the ultrasonic delay line. The above method was not appropriate because of the

本発明は、上記従来の欠点を除去するものであ
り、圧電変換素子より放射した音波の指向性によ
る伝搬路からのずれを修正する反射曲面を形成し
た遅延媒体を備えた超音波遅延線を提供するもの
である。
The present invention eliminates the above-mentioned conventional drawbacks, and provides an ultrasonic delay line equipped with a delay medium formed with a reflection curved surface that corrects deviation from the propagation path due to the directivity of the sound wave emitted from a piezoelectric transducer. It is something to do.

以下図面をもとにして本発明の実施例を説明す
る。第2図は本発明の一実施例における超音波遅
延線の正面図であり、従来例を示す第1図と同一
箇所には同一番号を付している。本発明の特徴は
遅延媒体であるガラス板7における音波の反射面
7aが、圧電磁器板3の音波放射面の中点〇を中
心とした半径Rの球面の一部となつていることで
ある。
Embodiments of the present invention will be described below based on the drawings. FIG. 2 is a front view of an ultrasonic delay line in one embodiment of the present invention, and the same parts as in FIG. 1 showing the conventional example are given the same numbers. A feature of the present invention is that the sound wave reflecting surface 7a of the glass plate 7, which is a delay medium, is a part of a spherical surface with a radius R centered on the midpoint 0 of the sound wave emission surface of the piezoelectric ceramic plate 3. .

このような形状にガラス板7における音波の反
射面7aを形成すると、主軸方向に伝搬する音波
成分8aおよび主軸よりずれた方向に伝搬する音
波成分8b,8cは共に反射面7aで反射され、
入射経路と同一の反射経路を通つて反射面7aの
中心である。圧電磁器板3の中点0にもどること
になり、音波の損失が発生せず、従来の場合に比
較して変換効率が向上する。
When the sound wave reflecting surface 7a of the glass plate 7 is formed in such a shape, the sound wave component 8a propagating in the main axis direction and the sound wave components 8b and 8c propagating in a direction shifted from the main axis are both reflected by the reflection surface 7a,
It passes through the same reflection path as the incident path and reaches the center of the reflection surface 7a. Since the piezoelectric ceramic plate 3 returns to the midpoint 0, no loss of sound waves occurs, and the conversion efficiency is improved compared to the conventional case.

第3図は本発明の超音波遅延線のさらに他の実
施例を示している。この実施例の場合は遅延媒体
であるガラス板9は4個の平面9a〜9dと1個
の曲面9eを有しており、平面9aには、先の実
施例と同様に電極2,4、圧電変換素子である圧
電磁器板3およびリード線5a,5bが取り付け
られている。本実施例の特徴は反射面を多くと
り、曲面9eの形状を音波の入射経路と反射経路
が同一になるような曲面に加工していることであ
る。すなわち、圧電磁器板3より放射された音波
成分10a,10b,10cはそれぞれ平面9
d,9c,9bで各々異なる角度で入射および反
射して曲面9eに入射するが、曲面9eでは入射
経路と反射経路が同一となり、音波成分10a〜
10cは同じ経路を逆もどりして圧電磁器板3に
もどつてくる。このような曲面9eは実験的に容
易に規定できるものである。
FIG. 3 shows yet another embodiment of the ultrasonic delay line of the present invention. In this embodiment, the glass plate 9, which is a delay medium, has four flat surfaces 9a to 9d and one curved surface 9e, and the flat surface 9a has electrodes 2, 4, A piezoelectric ceramic plate 3, which is a piezoelectric transducer, and lead wires 5a and 5b are attached. The feature of this embodiment is that the number of reflective surfaces is large, and the shape of the curved surface 9e is processed into a curved surface such that the incident path of the sound wave and the reflection path are the same. That is, the sound wave components 10a, 10b, 10c radiated from the piezoelectric ceramic plate 3 are each on the plane 9.
d, 9c, and 9b are incident and reflected at different angles and incident on the curved surface 9e, but on the curved surface 9e, the incident path and the reflection path are the same, and the sound wave components 10a to 10b are incident on the curved surface 9e.
10c returns to the piezoelectric ceramic plate 3 along the same route. Such a curved surface 9e can be easily defined experimentally.

このようにガラス板9を形成すると、音波の経
路が長くなるため、大きい遅延時間を得られると
ともに変換効率を従来に比較して著しく大きくで
きる。
When the glass plate 9 is formed in this manner, the path of the sound wave becomes longer, so a longer delay time can be obtained, and the conversion efficiency can be significantly increased compared to the conventional method.

以上説明したように、本発明の超音波遅延線は
遅延媒体の反射面を所定の曲面に加工することに
より、従来のものより一段と変換効率を大きくで
きる効果があり、実用的価値が極めて大なるもの
である。
As explained above, the ultrasonic delay line of the present invention has the effect of increasing the conversion efficiency even more than conventional ones by processing the reflection surface of the delay medium into a predetermined curved surface, and has extremely high practical value. It is something.

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

第1図は従来の超音波遅延線の正面図、第2図
は 本発明の実施例における超音波遅延線の正面
図、第3図は本発明の他の実施例における超音波
遅延線の正面図である。 3……圧電変換素子(圧電磁器板)、7,9…
…遅延媒体(ガラス板)、7a,9e……曲面
(反射面)。
Fig. 1 is a front view of a conventional ultrasonic delay line, Fig. 2 is a front view of an ultrasonic delay line in an embodiment of the present invention, and Fig. 3 is a front view of an ultrasonic delay line in another embodiment of the present invention. It is a diagram. 3...Piezoelectric conversion element (piezoelectric ceramic plate), 7, 9...
...Delay medium (glass plate), 7a, 9e...curved surface (reflecting surface).

Claims (1)

【特許請求の範囲】[Claims] 1 ガラス板等の遅延媒体の一側面に入・出力兼
用の一個の圧電変換素子を取付け、上記遅延媒体
の音波の反射面を音波の入射経路と反射経路が同
一になる曲面に加工してなる超音波遅延線。
1 A piezoelectric transducer for both input and output is attached to one side of a delay medium such as a glass plate, and the sound wave reflecting surface of the delay medium is processed into a curved surface so that the sound wave's incident path and reflection path are the same. Ultrasonic delay line.
JP59102181A 1984-05-21 1984-05-21 ultrasonic delay line Granted JPS59229916A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP59102181A JPS59229916A (en) 1984-05-21 1984-05-21 ultrasonic delay line

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP59102181A JPS59229916A (en) 1984-05-21 1984-05-21 ultrasonic delay line

Publications (2)

Publication Number Publication Date
JPS59229916A JPS59229916A (en) 1984-12-24
JPS6350885B2 true JPS6350885B2 (en) 1988-10-12

Family

ID=14320503

Family Applications (1)

Application Number Title Priority Date Filing Date
JP59102181A Granted JPS59229916A (en) 1984-05-21 1984-05-21 ultrasonic delay line

Country Status (1)

Country Link
JP (1) JPS59229916A (en)

Families Citing this family (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS6016714A (en) * 1984-06-21 1985-01-28 Matsushita Electric Ind Co Ltd ultrasonic delay line

Also Published As

Publication number Publication date
JPS59229916A (en) 1984-12-24

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