JPS5846711B2 - Dopra sonar - Google Patents
Dopra sonarInfo
- Publication number
- JPS5846711B2 JPS5846711B2 JP50099955A JP9995575A JPS5846711B2 JP S5846711 B2 JPS5846711 B2 JP S5846711B2 JP 50099955 A JP50099955 A JP 50099955A JP 9995575 A JP9995575 A JP 9995575A JP S5846711 B2 JPS5846711 B2 JP S5846711B2
- Authority
- JP
- Japan
- Prior art keywords
- vibrator
- transducer
- sound
- housing
- width
- 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
Links
Classifications
-
- G—PHYSICS
- G01—MEASURING; TESTING
- G01S—RADIO 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
- G01S7/00—Details of systems according to groups G01S13/00, G01S15/00, G01S17/00
- G01S7/52—Details of systems according to groups G01S13/00, G01S15/00, G01S17/00 of systems according to group G01S15/00
- G01S7/52004—Means for monitoring or calibrating
- G01S7/52006—Means for monitoring or calibrating with provision for compensating the effects of temperature
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】
本発明は水中超音波のドプラ効果を利用した対地対水、
または対物速度計の構成要素である電気から音響に、ま
た音響から電気に変換を行なう圧電素子等の振動子を有
する送受信装置に関するもので、船舶等に装備するため
の犠装を簡単にできるようにすると共に、海水温度、塩
分、流体変動等によって生ずる音速の影響を自動的に修
正し、且つ自動音速補正の原理に近付けることのできる
実際の装置を提供すべくなしたもので、送信音波と受信
音波との間に生ずるドプラ効果に基づいて速度を測定す
る送受波器において、接水側面が平面形状を有して且つ
反接水側面が同一方向に同一角度で傾斜する複数の傾斜
面を有する音波透過材を設け、該音波透過材の前記各傾
斜面に、背面材料を取付けてなり且つドプラスペクトル
の基となる海底に考えられる双曲線に沿って両翼方向に
広い範囲をカバーし得る指向性領域をもつ如くスウエプ
トウイフグ状の振動子を進行方向の長さが幅よりも長く
なるように複数個配置した振動子ユニットを備えたこと
を特徴とするドプラソナー等における送受信装置、に係
るものである。DETAILED DESCRIPTION OF THE INVENTION The present invention utilizes the Doppler effect of underwater ultrasound to provide ground-to-water,
It also relates to a transmitter/receiver that has a vibrator such as a piezoelectric element that converts electricity to sound and sound to electricity, which is a component of an objective speedometer. It was designed to provide an actual device that can automatically correct the effects of sound speed caused by seawater temperature, salinity, fluid fluctuations, etc., and approximate the principle of automatic sound speed correction. In a transducer that measures velocity based on the Doppler effect that occurs between received sound waves, a plurality of inclined surfaces are used, the surface in contact with water has a planar shape, and the surface opposite to water contact is inclined in the same direction at the same angle. A sound wave transmitting material is provided, and a backing material is attached to each of the inclined surfaces of the sound wave transmitting material, and the directionality is such that the sound wave transmitting material can cover a wide range in both wing directions along a hyperbola considered to be on the sea floor, which is the basis of the Doppler spectrum. This relates to a transmitting/receiving device for Doppler sonar, etc., characterized in that it is equipped with a transducer unit in which a plurality of swept-whiff-shaped transducers are arranged so that the length in the traveling direction is longer than the width. It is.
従来の送受信装置を第1図について説明すると、1は船
底、2は送受波振動子、3は水温計測用ピックアップ、
4は空気抜配管であって、この従来の送受信装置には凹
所aがあるため船底を伝わる気泡が凹所aにたまって超
音波の妨害となり、音速補正のために水温計測を必要と
し、塩分補正を必要とする欠点があった。To explain the conventional transmitting and receiving device with reference to FIG. 1, 1 is the bottom of the ship, 2 is a wave transmitting/receiving oscillator, 3 is a pickup for measuring water temperature,
4 is an air vent pipe, and since this conventional transmitting/receiving device has a recess a, air bubbles traveling along the bottom of the ship accumulate in the recess a and interfere with the ultrasonic waves, making it necessary to measure the water temperature in order to correct the speed of sound. It had the disadvantage of requiring salinity correction.
この装置の凹所aのために生ずる欠点を除去するため、
第2図に示すような音響透過材5を凹所aに装着して音
波の送受波面が船底1と同一平面となるようにし、空気
溜りができて超音波の妨害となることを防ぐことも行な
われているが、音速補正が自動的に行なわれないので依
然として水温計測用ピックアップを必要としていた。In order to eliminate the drawbacks caused by the recess a of this device,
It is also possible to install an acoustically transparent material 5 in the recess a as shown in Fig. 2 so that the plane for transmitting and receiving sound waves is flush with the bottom 1 of the ship, thereby preventing air pockets from forming and interfering with the ultrasonic waves. However, since sound speed correction is not automatically performed, a pickup for measuring water temperature is still required.
さらに空気溜りによる妨害、音速補正、塩分補正の問題
が生じないようにするため、振動子を外から見て平らな
ポケットの中に油浸して等温に保つようにしたものもあ
るが、加熱、等温保持機構を具えなければならない欠点
があった。Furthermore, in order to avoid problems such as interference caused by air pockets, sound velocity correction, and salinity correction, some types of transducers are kept at an equal temperature by immersing the transducer in oil in a pocket that is flat when viewed from the outside. There was a drawback that an isothermal maintenance mechanism had to be provided.
従来の振動子ユニットは一素子型で配列振動子を構成し
ないものであったため音速の自動補正ができず、空気溜
りが発生するため船底を伝わる気泡の影響が大きく、振
動子の貼り付は耐圧性能を十分に得ることが困難であり
、また圧電振動子は円板、正方形、長方形などであった
が、これらは受波スペクトルの形状を広帯域にするとい
う性質があり、そのために検出誤差が生じる問題があっ
た。Conventional transducer units were one-element type and did not constitute an array transducer, so they could not automatically correct the sound speed, and air pockets were generated, which had a large effect on air bubbles traveling through the bottom of the ship. It was difficult to obtain sufficient performance, and piezoelectric vibrators were shaped like disks, squares, or rectangles, but these have the property of widening the shape of the receiving spectrum, which causes detection errors. There was a problem.
本発明はこのような欠点を除去したもので、まず自動音
速補正の原理を第3図について説明すると、速度υで走
行中の船6が水面7に対して角度θで前と後に送波周波
数ftで海底8に向けて送波し、前と後の方向における
受波信号の周波数をそれぞれfrl、fr2とすると、
の関係がある。The present invention eliminates such drawbacks. First, the principle of automatic sound speed correction will be explained with reference to FIG. ft toward the seabed 8, and if the frequencies of the received signals in the front and rear directions are frl and fr2, respectively, there is the following relationship.
ここでCは水中の音速である。第4図は圧電振動子9の
断面図で厚さ方向である矢印方向に振動するもので従来
用いられていた1個のものと同じであるが、このような
振動子を複数個用い、第5図に示すように前方向に角度
θで送受波する振動子io、1i、後方向に角度θで送
受波する振動子12.13として配列することにより、
とすることができるものである。Here C is the speed of sound in water. FIG. 4 is a cross-sectional view of a piezoelectric vibrator 9 that vibrates in the direction of the arrow, which is the thickness direction, and is the same as the single piezoelectric vibrator used conventionally. As shown in FIG. 5, by arranging the transducers io and 1i which transmit and receive waves at an angle θ in the front direction and the transducers 12 and 13 which transmit and receive waves at an angle θ in the rear direction, the following can be achieved.
ここにαは定数である。Here α is a constant.
式(2)の特徴は、船の速度υがfrtfr2だけに依
存し、他のものには依存しないことである。A feature of equation (2) is that the speed υ of the ship depends only on frtfr2 and nothing else.
次にその原理を第6図によって説明する。Next, the principle will be explained with reference to FIG.
振動子の距離をDとすると、θ方向の水中超音波の波長
がD cosθの整数倍となるとき、θ方向の超音波は
強め合い、
の関係ができる。If the distance between the transducers is D, then when the wavelength of the underwater ultrasound in the θ direction is an integral multiple of D cos θ, the ultrasound in the θ direction strengthens each other, creating the following relationship.
ここにnは整数、λは水中超音波波長である。Here, n is an integer and λ is the underwater ultrasound wavelength.
である。It is.
ここでり、nは次のようにしてきまる。振動子の大きさ
が決まり、送受波方向からθがきまり、水中の波長(平
均的なもの)λが与えられる。Here, n can be calculated as follows. The size of the vibrator is determined, θ is determined from the wave transmission and reception direction, and the underwater wavelength (average) λ is given.
次に式(3)よりn(1,2,3,・・・・・・・・・
)に対応したDが表として求まる。Next, from equation (3), n(1, 2, 3,...
) can be found as a table.
先にきめた振動子の大きさから、実際の配置に合うnと
Dを選んできめる。From the size of the vibrator determined earlier, select n and D that match the actual arrangement.
さらに詳述すると、水中の音速Cが温度、塩分等によっ
て変化すると水中超音波波長が変り、それに応じて式(
3)の条件にあう角度θが変るが、式(4)の定数αは
水中の音速Cに依存していないため式(4)は変らず、
したがって定数αは不変である。To explain in more detail, when the sound speed C in water changes due to temperature, salinity, etc., the underwater ultrasonic wavelength changes, and the equation (
Although the angle θ that satisfies the condition of 3) changes, the constant α in equation (4) does not depend on the speed of sound C in water, so equation (4) does not change.
Therefore, the constant α remains unchanged.
角度θの方向を向けて設ける振動子10,11゜12.
13を式(3)を満足するような距離りをおいて配置す
ることにより得られる振動子群を並列接続することによ
って、これをドプラソナーの送波および受波に使用すれ
ば、水中音速変化に依存しない送受信装置を構成するこ
とができる。Vibrator 10, 11°12.
13 at a distance that satisfies Equation (3) and connects them in parallel. If this is used for Doppler sonar transmission and reception, changes in underwater sound speed can be avoided. It is possible to configure independent transmitting and receiving devices.
これが自動音速補正の原理である。This is the principle of automatic sound speed correction.
原理的には第5図のように一方向に対して2個の振動子
があればよいわけであるが、第7図Aのように3個の振
動子を1群としたり、第7図Bのように4個の振動子を
1群とするように複数個の振動子を配置(ルてもよい。In principle, it is sufficient to have two oscillators in one direction as shown in Fig. 5, but it is also possible to have three oscillators in one group as shown in Fig. 7A, or as shown in Fig. 7. A plurality of oscillators may be arranged in a group of four oscillators as shown in B.
このように水中音速に依存しないようなドプラソナーの
送受信装置は、式(3)を満足させるように配列し、そ
れら振動子を電気的に並列に接続して構成するもので、
振動子の配列としては第5図、第7図A1第7図Bのよ
うな例がある。The Doppler sonar transmitter/receiver, which does not depend on the underwater sound speed, is constructed by arranging the transducers to satisfy equation (3) and electrically connecting them in parallel.
Examples of the arrangement of the vibrators are shown in FIG. 5, FIG. 7A, and FIG. 7B.
なお上述の原理を利用することにより、気中超音波を用
いた乗物の速度計、または地面に設置して用いる鉄道車
両、自動車等の速度検出装置にも全く同様に適用するこ
とができる。By utilizing the above-mentioned principle, it can be applied in exactly the same way to a speedometer for a vehicle using aerial ultrasonic waves, or a speed detection device for a railway vehicle, an automobile, etc. that is installed on the ground.
この場合、Cは空気中の音の伝播速度となるのみで、そ
の他は船の場合と全く同じである。In this case, C is only the propagation speed of sound in the air, and the rest is exactly the same as in the case of a ship.
上記した原理は、発振源が点でありスペクトルも線であ
る場合における理論上の原理であるが、実際上発振源が
点のように指向性をもたない場合には原理的に戒り立た
ない。The above principle is a theoretical principle when the oscillation source is a point and the spectrum is a line, but in practice it is not valid in principle when the oscillation source has no directivity like a point. do not have.
このため、発振スペクトルに指向性をもたせるべく振動
子を面形状にすることが考えふれるが、単に面形状にし
てもスペクトル幅の広がりにより誤差を生じて前記原理
から遠ざかってしまう問題がある。For this reason, it is often considered to make the vibrator in a planar shape in order to give the oscillation spectrum directivity, but even if the vibrator is made in a planar shape, there is a problem that an error occurs due to the broadening of the spectrum width, which deviates from the above-mentioned principle.
本発明はこのような問題を解決する具体的な構成を提供
するものであり、以下にそれを詳述する。The present invention provides a specific configuration for solving such problems, which will be explained in detail below.
第8図は本発明における振動子ユニットを支持する送受
信装置ハウジングの構造を示すもので、15は鋳物また
は樹脂で一体に作ったハウジングであって、これを船底
1に取り付けるにあたっては船底1に予め船底補強リン
グ14を溶接によって取り付けておき、船底補強リング
14の上面に防水アスベスト16を介在させてハウジン
グ15を植込みボルト22とナツトで固定する。FIG. 8 shows the structure of the transmitter/receiver housing that supports the transducer unit according to the present invention. Reference numeral 15 denotes a housing integrally made of cast metal or resin. The bottom reinforcing ring 14 is attached by welding, and the housing 15 is fixed with stud bolts 22 and nuts with waterproof asbestos 16 interposed on the top surface of the bottom reinforcing ring 14.
ハウジング15の下面には後述する第9図、第10図に
示す振動子ユニットを取り付けるための振動子ユニット
取付孔25,25が形成されている。Vibrator unit mounting holes 25, 25 are formed in the lower surface of the housing 15 for mounting a vibrator unit shown in FIGS. 9 and 10, which will be described later.
23は振動子ユニットのケーブルを通す電線穴であって
、電線穴23を通したケーブルは電線貫通金物17を通
って端子台18へ接続され、端子台18からはさらに別
の電線が電線貫通金物19を通って外に出る。Reference numeral 23 denotes an electric wire hole through which the cable of the transducer unit is passed. The cable passed through the electric wire hole 23 is connected to the terminal block 18 through the electric wire penetration metal fitting 17, and from the terminal block 18, another electric wire is connected to the electric wire penetration metal fitting. Go outside through 19.
端子台18の取り付けられている空間は防水用アスベス
ト16をはさんで上ぶた20でふたをされ、通しボルト
、ナツト21で固く締められている。The space in which the terminal block 18 is installed is covered with a top cover 20 with waterproof asbestos 16 in between, and is tightly tightened with through bolts and nuts 21.
上ぶた20の上面には上ぶた20を手で持つための上ぶ
た吊金具24が取り付けである。An upper lid hanging fitting 24 for holding the upper lid 20 by hand is attached to the upper surface of the upper lid 20.
次に前記振動子ユニット取付孔25内に取り付ける本発
明の送受信装置における振動子ユニットを第9図、第1
0図について説明する。Next, the transducer unit in the transmitter/receiver of the present invention is installed in the transducer unit mounting hole 25 as shown in FIG.
Figure 0 will be explained.
接水側面(海水に接する面)が平面を成し11反接水側
面(船側の面)が同一方向に同一角度で傾斜する複数の
傾斜面を有する音波透過材28を設け、該音波透過材2
8の前記各傾斜面には面形状を有し且つドプラシフトス
ペクトル幅を小さくする如く形成した振動子26.27
を設ける。A sound wave transmitting material 28 is provided which has a plurality of inclined surfaces whose water contact side (surface in contact with seawater) is a flat surface and whose anti-water contact side (surface on the ship's side) is inclined in the same direction at the same angle. 2
The oscillators 26 and 27 each have a surface shape on each of the inclined surfaces of 8 and are formed so as to reduce the width of the Doppler shift spectrum.
will be established.
該振動子26.27の背面には、コルク、バルサ材等の
背面材料29.30を取り付け、これら背面材料29.
30をコート材料31.32と共に前記音波透過材28
に接着し、リード線62を導出するようにしている。A back material 29.30 such as cork or balsa wood is attached to the back surface of the vibrator 26.27.
30 together with the coating material 31 and 32 of the sound wave transmitting material 28
The lead wire 62 is led out.
前記振動子26.27の傾斜角度と距離は式(3)に従
って求めた値にする。The inclination angle and distance of the vibrators 26 and 27 are determined according to equation (3).
これらを鋳物または樹脂で作った小さいハウジング34
の中に入れ、フランジ面を互に接着しておく。A small housing 34 made of cast iron or resin for these
and glue the flange surfaces together.
ケーブル64は電線貫通金物35を通してハウジング3
4の外に出るが、リード線62とケーブル64との境は
油等非圧縮性流体による耐圧液33の漏れを防ぐため、
接着固め63を施しておく。The cable 64 passes through the wire through fitting 35 and passes through the housing 3.
4, the boundary between the lead wire 62 and the cable 64 is designed to prevent leakage of the pressure-resistant fluid 33 due to incompressible fluid such as oil.
Adhesive hardening 63 is applied.
耐圧液33はプラグ36の入口から充填して栓をする。The pressure-resistant liquid 33 is filled from the inlet of the plug 36 to seal it.
ハウジング34はケーブル64を通すため、第10図の
ように一個所に溝を設けておくと都合がよい。In order to pass the cable 64 through the housing 34, it is convenient to provide a groove at one location as shown in FIG.
こうして出来た振動子ユニットのハウジング34を第8
図に示すハウジング15の振動子ユニット取付孔25に
下から入れ、押えリング37(第9図参照)と共に周囲
の取付穴に押えボルト38を螺合して取り付ける。The housing 34 of the vibrator unit thus made is placed in the eighth
It is inserted from below into the vibrator unit mounting hole 25 of the housing 15 shown in the figure, and is attached by screwing the holding bolt 38 into the surrounding mounting hole together with the holding ring 37 (see FIG. 9).
振動子ユニットを正しくはめ込むため、フラット振動子
ユニット取付マーク50,51,52,53がハウジン
グ15に付けてあり、さらにハウジング15を船底1に
正しく取り付けるための送受信装置取付マーク54.5
5もハウジング15に付けられている。Flat transducer unit mounting marks 50, 51, 52, and 53 are attached to the housing 15 in order to properly fit the transducer unit, and transmitter/receiver mounting marks 54.5 are provided to ensure that the housing 15 is correctly mounted on the bottom 1.
5 is also attached to the housing 15.
第9図において49は水密を保つためにOリングをはめ
込む01Jング溝であって、ハウジング15内の水密は
、0リング溝49にはめ込んだOリング、電線貫通金物
17、19、防水アスベスト16によって保っている。In FIG. 9, reference numeral 49 indicates an 01J groove into which an O-ring is fitted in order to maintain watertightness, and watertightness within the housing 15 is achieved by the O-ring fitted into the 0-ring groove 49, the wire penetration fittings 17 and 19, and the waterproof asbestos 16. I keep it.
このようにして組み立てた送受信装置は従来のような空
気抜配管4(第1図参照)がなく、端子台18の収納ス
ペースがフラット振動子ユニット組込用の取付孔25と
共にハウジング15に一体になっていてシステム構成ユ
ニットを少なくすることができ、従来のような台管溶接
をせず船底補強リング14を溶接すれば後は組立だけで
よく、振動子交換作業が従来に比べて容易である等の特
長を有している。The transmitting/receiving device assembled in this way does not have the air vent pipe 4 (see Fig. 1) like the conventional one, and the storage space for the terminal block 18 is integrated into the housing 15 along with the mounting hole 25 for incorporating the flat transducer unit. This makes it possible to reduce the number of system configuration units, and by welding the bottom reinforcing ring 14 instead of welding the main pipe as in the past, all that is left to do is assembly, making the transducer replacement work easier than before. It has the following features.
また振動子ユニットは平らな表面から斜め方向に超音波
の送受波指向特性を有し、自動音速補正ができ、振動子
の接着はくりが防止でき、コンパクトで扱いやすく、高
い圧力に耐える特長がある。In addition, the transducer unit has directional characteristics for transmitting and receiving ultrasonic waves in diagonal directions from a flat surface, enables automatic sound velocity correction, prevents the transducer from peeling off the adhesive, is compact, easy to handle, and can withstand high pressure. be.
次に振動子の形状について説明する。Next, the shape of the vibrator will be explained.
第11図、第12図は受波ドプラシフトスペクトル巾を
小さく、即ちスペクトル幅に対してその振幅を大きくす
ることができるようにした振動子の形状を示すもので、
振動子は複数個の配列により、第14図においてドプラ
シフトスペクトルの基となる海底に考えられる双曲線4
4.45間に沿い両翼方向に広い指向性領域48をもつ
ようなスウエプトウイング(swept wing :
飛行機の翼)状に形成されている。Figures 11 and 12 show the shape of a transducer that allows the received Doppler shift spectrum width to be small, that is, the amplitude to be large relative to the spectrum width.
By arranging multiple oscillators, the hyperbola 4 considered on the sea floor, which is the basis of the Doppler shift spectrum in Figure 14, is arranged.
Swept wing that has a wide directional area 48 in the direction of both wings along the 4.45
It is shaped like an airplane wing.
第11図は振動子39を音波透過材40に貼り付けた斜
視図であり、これを配列した状態の平面図が第12図で
あって41.42は振動子の輪郭である。FIG. 11 is a perspective view of the vibrator 39 attached to the sound wave transmitting material 40, and FIG. 12 is a plan view of the arrangement of the vibrator 39, and 41 and 42 are outlines of the vibrator.
振動子を第11図、第12図に示すような形状にせずに
もし複数個に切断されて全体として円形状を有する振動
子を用いるとすれば、その円形振動子が海底に作ると考
えられる指向性楕円47(第13図)は、ドプラシフト
スペクトルの基となる海底に考えられる双曲線44.4
5の間を幅方向にカバーする面積が小さく、そのために
第13図における周波数と振幅の関係を示す曲線43か
ら明らかなようにスペクトルの幅に対してその高さが低
いものとなり、結果的にドプラシフトスペクトル幅が広
くなってドプラシフト周波数のデジタルカウント誤差を
生じ易い問題を有することになる。If the oscillator were not shaped like the one shown in Figures 11 and 12, but instead a oscillator was cut into multiple pieces and had a circular shape as a whole, it would be possible to create a circular oscillator on the ocean floor. The directional ellipse 47 (Fig. 13) is a hyperbola 44.4 considered to be on the sea floor, which is the basis of the Doppler shift spectrum.
5 in the width direction is small, and therefore, as is clear from the curve 43 showing the relationship between frequency and amplitude in FIG. 13, its height is low relative to the width of the spectrum, resulting in This results in a problem in that the Doppler shift spectrum width becomes wide and digital counting errors in the Doppler shift frequency are likely to occur.
これに対し、前記第11図に示すスウエ振動子を第7図
A、B及び第12図のように配列することにより、第1
4図に示す如く海底に考えられる双曲線44.45間を
両翼方向に広範囲にわたってカバーする指向性領域48
とすることができる。In contrast, by arranging the suede vibrators shown in FIG. 11 as shown in FIGS. 7A and B and FIG.
As shown in Figure 4, a directional area 48 that covers a wide area in both wing directions between hyperbolas 44 and 45 that can be considered on the ocean floor.
It can be done.
即ち、前記比較例として示した複数個に分割され全体と
して円形状の振動子とした場合に比較して、前記第11
図に示すようなスウエプトウイング形状の振動子39を
第7図A、B及び第12図の如く船の進行方向に複数個
配置することにより、全体として、進行方向には前記円
形の場合の直径よりも長く、幅方向にはその直径より短
かくなるように形成する。That is, compared to the case where the vibrator is divided into a plurality of pieces and has a circular shape as a whole as shown in the comparative example, the 11th
By arranging a plurality of swept wing-shaped vibrators 39 in the traveling direction of the ship as shown in FIGS. 7A and B and FIG. It is formed to be longer than the diameter and shorter than the diameter in the width direction.
すると、海底に想定される指向性領域は、第13図及び
第14図から明らかなように、円形状の振動子によって
海底に想定される指向性楕円47に対して、進行方向に
は短かく、幅方向には長い指向性領域48となる。Then, as is clear from FIGS. 13 and 14, the directional area assumed on the seabed is shorter in the direction of travel than the directional ellipse 47 expected on the seafloor due to the circular vibrator. , resulting in a long directional region 48 in the width direction.
従って曲線43′で示すようにスペクトル幅に対してそ
の高さを高くすることができるので、結果的にドプラシ
フトスペクトル幅が狭くなり、ドプラシフト周波数のデ
ジタルカウント誤差を少なくして前記自動音速補正の原
理に近付けることができる。Therefore, as shown by curve 43', the height can be increased relative to the spectral width, resulting in a narrower Doppler shift spectral width, which reduces the digital count error of the Doppler shift frequency and allows the automatic sound velocity correction to be performed. You can get closer to the principle.
上記から明らかなよう(f1同一幅(第13.14図に
おける中心線46方向の幅)の指向性領域、或いは同一
の面積の指向性領域であるならば、第13図に示す円形
振動子の場合より第11.12図に示すようなスウエプ
トウイング形状の振動子の方が著しくドプラシフトスペ
クトル幅を狭くできる。As is clear from the above, if the directional area has the same width as f1 (width in the direction of the center line 46 in Fig. 13.14) or the directional area has the same area, the circular oscillator shown in Fig. 13 In some cases, a swept wing-shaped vibrator as shown in FIG. 11.12 can significantly narrow the Doppler shift spectrum width.
尚、振動子の数は第12図のように2個で配列を組んだ
ものに限らず、2個以上なら何個でもよい。Note that the number of vibrators is not limited to two vibrators arranged in an array as shown in FIG. 12, but may be any number as long as it is two or more.
第15図、第16図は振動子だけに注目し、上から見た
配置、大きさが概念的にわかるように描いたもので、第
15図は2個の振動子56.57を配置したものであり
、第16図は4個の振動子58.59,60.61を配
置したものである。Figures 15 and 16 focus only on the vibrator, and are drawn to conceptually understand the arrangement and size seen from above. In Figure 15, two vibrators 56 and 57 are arranged. FIG. 16 shows an arrangement in which four vibrators 58, 59 and 60, 61 are arranged.
第9図に示す音波透過材28が高圧に耐え、圧力によっ
て中心がへこむことがないようにするため、ハウジング
34内下面および音波透過材28の中心上面にそれぞれ
第17図に示す音波の反射吸収材料65、ピラー66を
接着するとよい。In order for the sound wave transmitting material 28 shown in FIG. 9 to withstand high pressure and to prevent the center from being dented by the pressure, the inner lower surface of the housing 34 and the center upper surface of the sound wave transmitting material 28 are provided with reflection and absorption of sound waves as shown in FIG. 17. It is preferable to bond the material 65 and the pillar 66.
音波の反射吸収材料65はコルク、バルサ材等で作り、
ハウジング34からの音波の伝播を遮断してピラー66
に直接雑音が乗ることを防ぐものである。The sound wave reflection/absorption material 65 is made of cork, balsa wood, etc.
The pillar 66 blocks the propagation of sound waves from the housing 34.
This prevents noise from being directly transmitted to the
ピラー66は金属、樹脂等で成形するのがよい。The pillar 66 is preferably molded from metal, resin, or the like.
第18図は音波の反射吸収材料65をハウジング34の
内面に貼り付け、ハウジング34から耐圧液33を経て
振動子26.27(第9図参照)に雑音が伝播するのを
防ぐようにした状態を示す断面図である。FIG. 18 shows a state in which a sound wave reflection/absorption material 65 is attached to the inner surface of the housing 34 to prevent noise from propagating from the housing 34 to the vibrator 26, 27 (see FIG. 9) via the pressure-resistant liquid 33. FIG.
第19図は第9図における振動子27がその側面から雑
音をひろうことなく、音波透過材28との接着面におけ
るはくりが起きないように音波の反射吸収材料65を背
面材料30と共にコート材料32でおおった状態を示す
断面図であって、雑音に耐える振動子を作る場合には第
18図の防音壁と合わせて用いることは特に大事である
。FIG. 19 shows that the vibrator 27 in FIG. 9 is coated with a coating material together with the backing material 30 so that the vibrator 27 in FIG. 18 is a cross-sectional view showing a state covered with a noise barrier. When making a vibrator that can withstand noise, it is especially important to use it in conjunction with the soundproof wall shown in FIG. 18.
第20図は音波透過材28とハウジング34とが確実に
密着状態で接着され、内部から耐圧液33(第9図参照
)が;嫡出しないようにしたもので、溝67によって音
波透過材28とハウジング34とを確実に密着させて接
着し、取付穴38に通すボルトにより、押えリング37
と共に音波透過材28とハウジング34をタイトに一体
化する。In FIG. 20, the sound wave transmitting material 28 and the housing 34 are firmly adhered to each other so that the pressure-resistant liquid 33 (see FIG. 9) does not come out from inside. The housing 34 is firmly attached and bonded, and the retaining ring 37 is attached with a bolt passed through the mounting hole 38.
At the same time, the sound wave transmitting material 28 and the housing 34 are tightly integrated.
本発明は上述したように音波透過材における反振動子取
付面(接水側面)が平面形状を有していることにより空
気溜りが生ずることがなく、従って送受信装置取付に際
して空気抜配管が不要となるため従来よりも蟻装が簡単
になり、振動子の有効な配列により速度とドプラシフト
周波数との間に水温、塩分等音速に無関係な定数を作る
ことができるので、加熱、等温保持機を設けなくても自
動的に音速補正ができ、船底補強リングの溶接作業等据
付は作業が簡単であると共に、端子台が送受波器と一体
になっているためシステム構成ユニット数を少なくして
システムを簡単にすることが可能であり、水中の高圧力
に耐えると共に接着した振動子のはくりがおこりに<<
、更に受波ドプラシフトスペクトル巾を狭くできるよう
に振動子を形成していることにより、発振源を面形状と
して指向性をもたせた際の誤差を少なくして自動音速補
正の原理に近付けることができる優れた効果を有してい
る。As described above, in the present invention, the anti-oscillator mounting surface (water-contacting surface) of the sound-transmitting material has a planar shape, which prevents air pockets from forming, and therefore eliminates the need for air vent piping when installing the transmitter/receiver. This makes ant control easier than before, and by effectively arranging the transducers, it is possible to create constants between velocity and Doppler shift frequency that are independent of sound velocity, such as water temperature and salinity, so a heating and isothermal holding machine is installed. The sound speed can be automatically corrected even if the ship is not equipped, and the installation work such as welding the bottom reinforcement ring is easy, and since the terminal block is integrated with the transducer, the number of system configuration units can be reduced and the system can be improved. It can be easily made, withstands high pressure underwater, and prevents the bonded vibrator from peeling off.
Furthermore, by forming the transducer so that the width of the received Doppler shift spectrum can be narrowed, it is possible to reduce errors when the oscillation source is made into a planar shape to provide directivity, and to approach the principle of automatic sound velocity correction. It has excellent effects.
第1図は従来のドプラソナー用送受波器の縦断面図、第
2図は従来のドプラソナー用送受波器に装着した音響透
過材の断面図、第3図は自動音速補正の原理説明図、第
4図は圧電振動子の断面図、第5図は振動子の配置説明
図、第6図は配列振動子の原理説明図、第7図Aは3個
の振動子による配列振動子の説明図、第7図Bは4個の
振動子による配列振動子の説明図、第8図は本発明によ
る送受信装置ハウジングの一実施例の縦断面ワ、第9図
は本発明による振動子ユニットの一実施例の縦断面図、
第10図は第9図の平面図、第11図は振動子の形状を
示す斜視図、第12図は配列振動子の平面緊、第13図
は円形面をもつ振動子による受波スペクトルの説明図、
第14図は第12図の配列振動子による受波スペクトル
の説明図、第15図、第16図は振動子の配置図、第1
7図はピラーの断面図、第18図は防音壁の断面図、第
19図は雑音を防ぐようにした振動子ユニットの要部断
面図、第20図は振動子取付部分の要部断面図である。
10.11,12,13,26,27,39゜56.5
7,58,59,60,61・・・・・・振動子、D・
・・・・・振動子の距離、θ・・・・・・角度。Figure 1 is a longitudinal cross-sectional view of a conventional Doppler sonar transducer, Figure 2 is a cross-sectional view of the acoustically transparent material attached to the conventional Doppler sonar transducer, and Figure 3 is a diagram explaining the principle of automatic sound velocity correction. Figure 4 is a cross-sectional view of a piezoelectric vibrator, Figure 5 is an explanatory diagram of the arrangement of vibrators, Figure 6 is an explanatory diagram of the principle of an arrayed vibrator, and Figure 7A is an explanatory diagram of an arrayed vibrator with three vibrators. , FIG. 7B is an explanatory diagram of an arrayed transducer made up of four transducers, FIG. 8 is a vertical cross-sectional view of an embodiment of the transmitter/receiver housing according to the present invention, and FIG. 9 is an illustration of an array of transducers according to the present invention. A longitudinal cross-sectional view of the embodiment,
Fig. 10 is a plan view of Fig. 9, Fig. 11 is a perspective view showing the shape of the transducer, Fig. 12 is a plan view of the array transducer, and Fig. 13 is the received wave spectrum by the transducer with a circular surface. Explanatory diagram,
Fig. 14 is an explanatory diagram of the reception spectrum by the array transducer in Fig. 12, Fig. 15 and Fig. 16 are arrangement diagrams of the transducer,
Figure 7 is a sectional view of the pillar, Figure 18 is a sectional view of the soundproof wall, Figure 19 is a sectional view of the main part of a vibrator unit designed to prevent noise, and Figure 20 is a sectional view of the main part of the vibrator mounting part. It is. 10.11, 12, 13, 26, 27, 39°56.5
7, 58, 59, 60, 61... vibrator, D.
...Distance of the vibrator, θ...Angle.
Claims (1)
づいて速度を測定する送受波器において、接水側面が平
面形状を有しはつ反接水側面が同一方向に同一角度で傾
斜する複数の傾斜面を有する音波透過材を設け、該音波
透過材の前記各傾斜面に、背面材料を取付けてなり且つ
ドプラシフトスペクトルの基となる海底に考えられる双
曲線に沿って両翼方向に広い範囲をカバーし得る指向性
領域をもつ如くスウエプトウイフグ状の振動子を進行方
向の長さが幅よりも長くなるように複数個配置した振動
子ユニットを備えたことを特徴とするドプラソナー等に
おける送受信装置。1. In a transducer that measures velocity based on the Doppler effect that occurs between transmitted and received sound waves, there are multiple transducers whose water-contacting surfaces have a planar shape and whose anti-water-contacting surfaces are inclined at the same angle in the same direction. A sound wave transmitting material having an inclined surface of Transmission/reception in Doppler sonar, etc., characterized by having a transducer unit in which a plurality of swept-whiff-shaped transducers are arranged so that the length in the traveling direction is longer than the width so as to have a directional area that can be covered. Device.
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP50099955A JPS5846711B2 (en) | 1975-08-18 | 1975-08-18 | Dopra sonar |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP50099955A JPS5846711B2 (en) | 1975-08-18 | 1975-08-18 | Dopra sonar |
Publications (2)
| Publication Number | Publication Date |
|---|---|
| JPS5223375A JPS5223375A (en) | 1977-02-22 |
| JPS5846711B2 true JPS5846711B2 (en) | 1983-10-18 |
Family
ID=14261104
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP50099955A Expired JPS5846711B2 (en) | 1975-08-18 | 1975-08-18 | Dopra sonar |
Country Status (1)
| Country | Link |
|---|---|
| JP (1) | JPS5846711B2 (en) |
Families Citing this family (3)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| JPS5582116A (en) * | 1978-12-18 | 1980-06-20 | Hitachi Chem Co Ltd | Molding composition |
| JPH0623222B2 (en) * | 1986-11-20 | 1994-03-30 | 日立化成工業株式会社 | Air-drying unsaturated polyester resin composition |
| CN112268531A (en) * | 2020-09-04 | 2021-01-26 | 珠江水利委员会珠江水利科学研究院 | Local terrain change monitoring device, local terrain monitoring method and system |
Family Cites Families (1)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| JPS539105B2 (en) * | 1971-10-11 | 1978-04-03 |
-
1975
- 1975-08-18 JP JP50099955A patent/JPS5846711B2/en not_active Expired
Also Published As
| Publication number | Publication date |
|---|---|
| JPS5223375A (en) | 1977-02-22 |
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