JPS5910021A - Ultrasonic wave delay line - Google Patents

Ultrasonic wave delay line

Info

Publication number
JPS5910021A
JPS5910021A JP11941482A JP11941482A JPS5910021A JP S5910021 A JPS5910021 A JP S5910021A JP 11941482 A JP11941482 A JP 11941482A JP 11941482 A JP11941482 A JP 11941482A JP S5910021 A JPS5910021 A JP S5910021A
Authority
JP
Japan
Prior art keywords
delay
medium
ultrasonic wave
line
piezoelectric element
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
JP11941482A
Other languages
Japanese (ja)
Inventor
Hiroshi Kuroda
廣 黒田
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 JP11941482A priority Critical patent/JPS5910021A/en
Publication of JPS5910021A publication Critical patent/JPS5910021A/en
Pending legal-status Critical Current

Links

Classifications

    • HELECTRICITY
    • H03ELECTRONIC CIRCUITRY
    • H03HIMPEDANCE NETWORKS, e.g. RESONANT CIRCUITS; RESONATORS
    • H03H9/00Networks comprising electromechanical or electro-acoustic devices; 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)

Abstract

PURPOSE:To obtain a transmission line of a double length with a delay means of the same size, by forming an ultrasonic wave delay line in such a way that the ultrasonic wave radiated from an input piezoelectric element is made incident to an output piezoelectric element after going and coming back the transmission line within a delay means. CONSTITUTION:Both input and output piezoelectric elements 11 and 12 are attached in parallel to the side surface 16 of a pair of side surfaces 16 and 17 which are formed by cutting obliquely with a 45 angle the corner parts at both sides of a side of a delay means 13 of glass, etc. The surface 16 is vertical to the main transmission surface of the medium 13. A transmission line 14 is provided within said main transmission surface, and a sound absorbing member 15 is provided. The ultrasonic wave radiated from the element 11 to the medium 13 is transmitted while reflected repetitively along the line 14 within the medium 13 and furthermore reflected by the other surface 17 to go back to the element 12 through the same line 14. In such a way, a double delay time is obtained with the same size of the delay medium.

Description

【発明の詳細な説明】 産業上の利用分野 本発明は超1波遅延線に関する。[Detailed description of the invention] Industrial applications The present invention relates to ultra-single wave delay lines.

超1波遅延線は、カラーテレビジョン受像機。Super 1-wave delay line is a color television receiver.

yTR等で1水平操作期間(約64μ5ec)の遅れを
作るためなどに利用されている、 従来例の構成とその問題点 従来の超音波遅延線の構成を第1図によシ親明すると、
(1)ハ入力圧%素子、<2) Vi出力圧電素子であ
り、ガラス等の遅延媒体(3)の一対の角部を450に
切り取った側面にそれぞれ取付けられている。(4)は
超音波伝播経路、(5)は@上相である。ところで、こ
の杓な構成の板台、入力用電素’−7−0,)から放射
さil、たIイ3M波は伝播り1路(4)を−回たり通
って出力圧電素子(2)に入射するので、所定の遅延時
間を得るのに、比較的大きな遅延媒体(3)を必要とす
る。そこで、小形化するだめに反射回数を増大し、よう
とすると、吸召材(5)を塗布し得るi¥Il積が減少
し、スプリアス化を号のレベノLが増大してし7甘うと
いうI’d:+R1・(がη−しる。
The configuration of a conventional example and its problems, which are used to create a delay of one horizontal operation period (approximately 64 μ5 ec) in yTR, etc. The configuration of a conventional ultrasonic delay line is explained in Fig. 1.
(1) C input pressure % element, <2) Vi output piezoelectric element, each of which is attached to a side surface of a pair of corners of a delay medium (3) such as glass cut out at 450 mm. (4) is the ultrasonic propagation path, and (5) is the @upper phase. By the way, the 3M waves radiated from the input electric element (7-0,), which has a simple configuration, propagate through one path (4) and go around the output piezoelectric element (2). ), a relatively large delay medium (3) is required to obtain a predetermined delay time. Therefore, if we try to increase the number of reflections to avoid miniaturization, the I\Il product that can be applied with the absorbing material (5) will decrease, and the level L of spurious will increase. I'd:+R1・( is η-sign.

イ(−明の目的 本発明は、/l・か、?、 [[+;顯点に鑑み、小形
化す為ことかできかつスプリアスレベルがi’ii大す
ることのない超音波遅延線の提供を目的とする。
In view of the problems, the present invention provides an ultrasonic delay line that can be miniaturized and that does not increase the spurious level. With the goal.

発明の構成 本発明は、このため遅延/+!体の伝播主m」に垂1白
な1つの0Ii17′lilに入力圧電素子と出力圧電
素子とを増刊り、入力圧算1.隼子〃ら方!i船さi′
また超音波が遅延媒体内の伝播経路を征伐して出力圧電
素子に入射する様にした超音波遅延線を提供する。
Structure of the Invention The present invention therefore has a delay/+! The input piezoelectric element and the output piezoelectric element are added to one 0Ii17'lil perpendicular to the body propagation main m, and the input pressure calculation 1. Hayako! i ship i'
The present invention also provides an ultrasonic delay line in which ultrasonic waves travel through a propagation path within a delay medium and are incident on an output piezoelectric element.

実施例の説明 次の本発明の一実施例を第2図及び第6図により説明す
ると、α])は入力圧%素子、02は出力圧電集子で、
ガラス等の遅延媒体0罎の一辺の両側に0ffJする角
部を450の角片で斜め切り取って形成した一対の側面
頭Qηの内の一方の側面(ト)に並列して取+Iけらt
lている。この側面伽jは遅延媒体θ1の伝播主面1に
垂直である。0→F!、創記伝播主面内の超音波の伝播
経路、0■1音劇である。
DESCRIPTION OF EMBODIMENTS The following embodiment of the present invention will be described with reference to FIGS. 2 and 6. α]) is an input pressure % element, 02 is an output piezoelectric collector,
Cut off the corners of the delay medium such as glass diagonally on both sides with a corner piece of 450.
I'm there. This side surface j is perpendicular to the main propagation surface 1 of the delay medium θ1. 0→F! , the propagation path of the ultrasonic wave in the principal plane of creation propagation, is 0■1 musical drama.

この様な構成により、入力E−’RL素子01)から遅
延媒体03に放射された超音波は、遅延媒体09内で伝
播経路04)K沿って反射を繰り返して伝播し、さらに
他方の側面α力で反射して会、播主面内の同一の伝播経
路(14)を通り出力圧電素子(2)に戻ろ○従って、
2倍の長さの伝播経路長を同一の大きさの遅延媒体で得
ることができ、かつ吸音材(1Gの塗布面積も減少しな
い。
With such a configuration, the ultrasonic wave emitted from the input E-'RL element 01) to the delay medium 03 is repeatedly reflected and propagated along the propagation path 04) K within the delay medium 09, and further propagates along the other side surface α. It is reflected by the force and returns to the output piezoelectric element (2) through the same propagation path (14) in the propagating plane. Therefore,
A propagation path length twice as long can be obtained with the same size delay medium, and the application area of the sound absorbing material (1G) does not decrease.

発明の効呆 本発明の超音波遅延線によれは、以上の島明から明らか
な様に、同一の大きさで2倍の遅延時間を得ることがで
き、従来の大きさの半分の大きさで所望の遅延時間を廟
する超音波遅延線を構成することかでき、かつ吸音拐塗
布面積を減少しないので、スフリアル個刊のレベルも増
大しない。
Effects of the invention As is clear from Akira Shima above, the ultrasonic delay line of the present invention can obtain twice the delay time with the same size, and is half the size of the conventional one. It is possible to construct an ultrasonic delay line with a desired delay time, and since the area of the sound absorbing layer is not reduced, the level of individual distribution of Sufurial is not increased.

4.1スliM+の簡単な目(明 第1図は従来の超音波遅延線の1百1図、第2図及び第
3N1は不発、明の一実施例を示し、第2図は正面図、
第6図ii側面図である。
4.1 A simple view of sliM+ (bright Figure 1 is a 101 diagram of a conventional ultrasonic delay line, Figures 2 and 3N1 are an undeveloped example, and Figure 2 is a front view) ,
FIG. 6 ii is a side view.

0ηは入力圧%、素子、(2)は出力圧電素子、α葎は
遅延媒体、04)は超音波の伝播経路、OQは吸音拐、
恥は入力圧%素子及び出力圧霜1素子を取付は九fil
1面
0η is the input pressure %, element, (2) is the output piezoelectric element, α is the delay medium, 04) is the propagation path of the ultrasonic wave, OQ is the sound absorption wave,
The shame is that it takes 9 fil to install the input pressure % element and the output pressure frost 1 element.
Page 1

Claims (1)

【特許請求の範囲】[Claims] (1)、遅延媒体の伝播主面に垂面な1つの側面に入力
圧電素子と出力圧電素子とを増刊けた超音波遅延線。
(1) An ultrasonic delay line in which an input piezoelectric element and an output piezoelectric element are added to one side surface perpendicular to the main propagation plane of a delay medium.
JP11941482A 1982-07-08 1982-07-08 Ultrasonic wave delay line Pending JPS5910021A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP11941482A JPS5910021A (en) 1982-07-08 1982-07-08 Ultrasonic wave delay line

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP11941482A JPS5910021A (en) 1982-07-08 1982-07-08 Ultrasonic wave delay line

Publications (1)

Publication Number Publication Date
JPS5910021A true JPS5910021A (en) 1984-01-19

Family

ID=14760870

Family Applications (1)

Application Number Title Priority Date Filing Date
JP11941482A Pending JPS5910021A (en) 1982-07-08 1982-07-08 Ultrasonic wave delay line

Country Status (1)

Country Link
JP (1) JPS5910021A (en)

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