JPH0374956B2 - - Google Patents
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- Publication number
- JPH0374956B2 JPH0374956B2 JP59267027A JP26702784A JPH0374956B2 JP H0374956 B2 JPH0374956 B2 JP H0374956B2 JP 59267027 A JP59267027 A JP 59267027A JP 26702784 A JP26702784 A JP 26702784A JP H0374956 B2 JPH0374956 B2 JP H0374956B2
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- Japan
- Prior art keywords
- received
- directional
- received signal
- ultrasonic
- seabed
- 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 - Lifetime
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Description
【発明の詳細な説明】
(産業上の利用分野)
この発明は、水中の広範囲方向へ超音波パルス
を送波して、各方向から帰来する反射波を各々の
方向毎に別個に受波して、表示画面上の対応する
方位位置に表示する水中探知装置に関する。特
に、各方向から帰来する反射波を受波するときに
不要方向からの反射波を抑圧して受波することに
関する。[Detailed Description of the Invention] (Industrial Application Field) This invention transmits ultrasonic pulses in a wide range of directions underwater, and receives reflected waves returning from each direction separately. The present invention relates to an underwater detection device that displays images at corresponding azimuth positions on a display screen. In particular, it relates to suppressing reflected waves from unnecessary directions when receiving reflected waves returning from various directions.
(従来の技術)
水中の広範囲方向を瞬時に探知する場合、広範
囲方向に同時に超音波パルスを送波して、各方向
から帰来する反射波を各方向毎に指向性を有する
受波ビームで受波して、各方向の受波ビームを高
速度で時系列化して表示する装置が用いられる。(Conventional technology) When detecting a wide range of directions underwater instantly, ultrasonic pulses are simultaneously transmitted in a wide range of directions, and the reflected waves returning from each direction are received as reception beams with directivity in each direction. A device is used that displays the received beams in each direction in time series at high speed.
指向性受波ビームは、一般には、複数の超音波
受波器の受波信号を各受波信号の位相関係を制御
して合成することにより得られる。この場合、問
題は、指向性受波ビームが所望方向に最大の受波
感度を有すると同時に、不要方向にも若干の受波
感度を有することである。そのため、不要方向か
ら比較的強いレベルの反射波が帰来する場合、こ
の反射波があたかも所望方向から帰来する反射波
のごとく見られる欠点がある。この欠点が最も顕
著に生じるのは海底の広範囲方向を探知する場合
である。 A directional reception beam is generally obtained by combining reception signals of a plurality of ultrasonic receivers by controlling the phase relationship of each reception signal. In this case, the problem is that the directional reception beam has maximum reception sensitivity in the desired direction, and at the same time has some reception sensitivity in unnecessary directions. Therefore, when a relatively strong reflected wave returns from an unnecessary direction, there is a drawback that this reflected wave is seen as if it were a reflected wave returning from a desired direction. This drawback is most noticeable when detecting a wide range of directions on the ocean floor.
例えば、第2図において、海底Bの広範囲角θ
方向を探知する場合、θ0方向の受波ビーム3につ
いて見ると、θ0方向に最大の受波感度を有する主
ビームMと主ビームMに対してθSだけ異なる不要
方向θi方向に受波感度を有する副ビームS,S′と
が形成される。又、海底Bの広範囲角方向に超音
波を送波する場合、直下の海底方向からは極めて
強い反射波が帰来する。そのため、この反射波が
副ビームSによつて受波される結果、指向性受波
ビームの指向方向を広範囲θの範囲内を順次変化
させながら各方向の受波信号を表示画面上に表示
させると、第3図に示すように、海底Bの実像
B0が表示されると同時に、等距離D0の線上の位
置に虚像B0′が表示される。 For example, in Figure 2, the wide range angle θ of the seabed B
When detecting the direction, looking at the receiving beam 3 in the θ 0 direction, the main beam M has the maximum receiving sensitivity in the θ 0 direction, and the receiving beam 3 is received in the unnecessary direction θ i direction, which is different from the main beam M by θ S. Sub-beams S and S' having wave sensitivity are formed. Furthermore, when transmitting ultrasonic waves in a wide range of angular directions on the seabed B, extremely strong reflected waves return from the direction of the seabed immediately below. Therefore, as a result of this reflected wave being received by the sub-beam S, the receiving signals in each direction are displayed on the display screen while changing the directivity direction of the directional receiving beam sequentially within a wide range θ. And, as shown in Figure 3, the real image of seabed B
At the same time that B 0 is displayed, a virtual image B 0 ' is displayed at a position on the line equidistant D 0 .
この虚像B0は主ビームMによる反射波が増巾
器で増巾されるとき飽和する結果、主ビームMに
よる海底反射波と副ビームSによる海底反射波と
のレベル差あるいはレベル比率が小さくなり、表
示器上での輝度コントラストによる区別ができな
くなるために生じる。例えば、第5図において、
aは受波ビーム3による受波信号を示し、R0は
送信パルス、R1は主ビームMによる海底反射波
の受波信号、Rsは副ビームSによる海底反射波
の受波信号を示す。主ビーム海底反射波R1と副
ビーム海底反射とのレベル差Edは、受波ビーム
3(第2図)の指向特性によつて決まり、一般に
は、レベル差Edが十分大きくなるように決定さ
れている。従つて、第5図aの受波信号を表示器
で表示させる場合は、主ビーム海底反射波R1と
副ビーム海底反射波Rsとの表示輝度を十分異な
らせて表示することができる。すなわち、主ビー
ム海底反射波R1を最適輝度になるように輝度制
御を行なうことにより、副ビーム反射波を抑圧し
て表示することができる。 This virtual image B 0 becomes saturated when the wave reflected by the main beam M is amplified by the amplifier, and as a result, the level difference or level ratio between the wave reflected from the seafloor by the main beam M and the wave reflected by the sub-beam S becomes small. This occurs because it becomes impossible to distinguish based on brightness contrast on the display. For example, in Figure 5,
a indicates the received signal by the receiving beam 3, R 0 indicates the transmitted pulse, R 1 indicates the received signal of the seabed reflected wave by the main beam M, and R s indicates the received signal of the seabed reflected wave by the sub beam S. . The level difference E d between the main beam seabed reflection wave R 1 and the sub-beam seafloor reflection is determined by the directional characteristics of the receiving beam 3 (Fig. 2), and in general, the level difference E d is set to be sufficiently large. It has been decided. Therefore, when the received signal shown in FIG. 5a is displayed on a display, the display brightness of the main beam seabed reflected wave R 1 and the sub-beam seabed reflected wave R s can be displayed with sufficiently different display brightnesses. That is, by controlling the brightness of the main beam seabed reflected wave R 1 to the optimum brightness, it is possible to display the sub beam reflected wave while suppressing it.
ところが、受波信号aの波高値が増巾器の飽和
レベルEsを越えた場合、増巾器出力が飽和するか
ら、第5図a′のような増巾出力が形成される。 However, when the peak value of the received signal a exceeds the saturation level E s of the amplifier, the amplifier output is saturated and an amplified output as shown in FIG. 5a' is formed.
この増巾出力a′は、主ビーム海底反射波R′1と
副ビーム反射波Rsとのレベル差E′dが極めて小さ
い。そのため、この増巾信号a′を表示した場合、
主ビーム海底反射波R′1と副ビーム反射波Rsとの
輝度差が小さくなり、副ビーム海底反射波Rsの
輝度を抑圧すると、主ビーム海底反射波R′1の輝
度も同時に抑圧され、識別が困難になる。 In this amplified output a′, the level difference E′ d between the main beam seabed reflected wave R′ 1 and the sub-beam reflected wave R s is extremely small. Therefore, when displaying this amplified signal a′,
When the brightness difference between the main beam seabed reflected wave R′ 1 and the sub-beam reflected wave R s becomes small, and the brightness of the sub-beam seabed reflected wave R s is suppressed, the brightness of the main beam seabed reflected wave R′ 1 is also suppressed at the same time. , making identification difficult.
上記のように、海底反射波が飽和する場合、一
般には、海底反射波が飽和レベル以下になるよう
に、増巾器の利得制御が行われる。ところが、第
5図aの受波信号の場合、主ビーム海底反射波
R1はパルス巾が非常に短いため利得制御回路が
十分に応答することができない。又、主ビーム海
底反射波R1の出力前に生じる副ビーム海底反射
波に対しては利得制御回路が動作することができ
ない。そのため、従来は、第3図に示すような虚
像B′0を除去することが極めて困難である。 As mentioned above, when the seabed reflected waves are saturated, the gain control of the amplifier is generally performed so that the seabed reflected waves are below the saturation level. However, in the case of the received signal in Figure 5a, the main beam reflected from the ocean floor
Since R1 has a very short pulse width, the gain control circuit cannot respond sufficiently. Further, the gain control circuit cannot operate for the sub-beam sea-floor reflected wave that occurs before the output of the main beam sea-bottom reflected wave R1 . Therefore, conventionally, it is extremely difficult to remove the virtual image B'0 as shown in FIG.
(発明が解決しようとする問題点)
この発明は、上記欠点を解決するもので、すな
わち、複数の超音波受波器の受波信号を合成して
指向性受波ビームを形成し、この受波ビームの指
向方向を高速操作して広範囲方向を探知する水中
探知装置において、海底反射波が指向性受波ビー
ムの副極によつて受波される場合でもこれを検出
して除去することを目的とする。(Problems to be Solved by the Invention) The present invention solves the above-mentioned drawbacks. That is, the received signals of a plurality of ultrasonic receivers are combined to form a directional received beam, and the received In an underwater detection device that detects a wide range of directions by rapidly controlling the pointing direction of a wave beam, it is possible to detect and remove seabed reflected waves even if they are received by the sub-pole of the directional receiving beam. purpose.
(問題点を解決するための手段、作用)
問題点を解決するための手段として、指向性受
波ビームを形成する複数の超音波受波器のいずれ
かの受波信号の信号レベルを検出する信号レベル
検出器と、この信号レベルに応じて、指向性受波
ビームの増巾器の増巾度を制御する利得制御回路
とが用いられる。そして、超音波受波器のいずれ
かの受波信号の信号レベルに応じて、指向性受波
ビームの増巾器の増巾度を制御する利得制御回路
とが用いられる。そして、超音波受波器のいずれ
かの受波信号の信号レベルに応じて利得制御を行
なうことにより指向性受波ビームに含まれる海底
反射波が抑圧される。(Means and actions for solving the problem) As a means for solving the problem, detect the signal level of the reception signal of any one of the plurality of ultrasonic receivers that form a directional reception beam. A signal level detector and a gain control circuit that controls the degree of amplification of the directional received beam amplifier according to the signal level are used. A gain control circuit is used that controls the degree of amplification of the directional received beam amplifier in accordance with the signal level of any received signal of the ultrasonic receiver. Then, by controlling the gain according to the signal level of the received signal of any of the ultrasonic receivers, the seafloor reflected waves included in the directional received beam are suppressed.
(実施例)
第1図において、T1乃至Toは直線状に配列さ
れる超音波受波器を示し、ほぼ無指向性同一特性
の超音波受波器が複数個配列されて超音波受波装
置を構成している。T0は超音波送波器を示し送
信器1によつて励振されたとき水中探知を行なう
広範囲方向に超音波パルスを送波する。水中ある
いは海底で反射された反射波は超音波受波器T1
乃至Toの各々によつて受波された後指向性ビー
ム形成回路2へ導かれる。指向性ビーム形成回路
2は超音波受波器T1乃至Toの各受波信号を合成
して一方向に指向性を有する指向性受波ビーム3
を形成する。そして、指向性ビーム形成回路2は
指向性受波ビーム3の指向方向を探知範囲角θの
範囲内で高速走査する。この走査速度は、指向方
向がθ角変化する間に、ほぼ等距離線上の反射波
が出力し得る速度で行われる。(Example) In Fig. 1, T 1 to T o indicate ultrasonic receivers arranged in a straight line. constitutes a wave device. T 0 denotes an ultrasonic transmitter which, when excited by the transmitter 1, transmits ultrasonic pulses in a wide range of directions for underwater detection. The reflected waves reflected underwater or on the seabed are transmitted to the ultrasonic receiver T 1 .
After being received by each of T o to T o , it is guided to the directional beam forming circuit 2 . A directional beam forming circuit 2 synthesizes the received signals of the ultrasonic receivers T1 to T0 to form a directional received beam 3 having directivity in one direction.
form. Then, the directional beam forming circuit 2 scans the direction of the directional received beam 3 at high speed within the range of the detection range angle θ. The scanning speed is such that reflected waves on a substantially equidistant line can be output while the pointing direction changes by θ angle.
このような指向性ビーム形成回路2は出願人が
特願昭57−121439号で提供した受波ビームの指向
方向制御装置を用いることができる。 For such a directional beam forming circuit 2, a receiving beam directional control device provided by the applicant in Japanese Patent Application No. 121439/1988 can be used.
指向性ビーム形成回路2から出力される指向性
受波信号出力は可変利得増巾器4に導かれて増巾
された後表示器5へ導かれる。表示器5は走査回
路6によつて画素走査が行われる。画素走査は例
えば、第4図に示すように、扇形のラスタが形成
されるように行われ、かつ、受波ビーム3の探知
範囲角走査に同期して画素走査が行われる。従つ
て、水中から帰来する反射波が表示画面上の対応
方位位置に表示される。 The directional received signal output from the directional beam forming circuit 2 is guided to a variable gain amplifier 4, amplified, and then guided to a display 5. Pixel scanning of the display device 5 is performed by a scanning circuit 6. For example, as shown in FIG. 4, the pixel scanning is performed to form a fan-shaped raster, and the pixel scanning is performed in synchronization with the detection range angle scanning of the receiving beam 3. Therefore, reflected waves returning from the water are displayed at corresponding azimuth positions on the display screen.
他方、超音波受波器T1乃至Toのうち任意に定
めたいずれかの超音波受波器の受波信号、例え
ば、n番目の超音波受波器Toの受波がA/D変
換器7に導かれて受波信号レベルがデイジタルデ
ータに変換される。そして、デイジタルデータに
変換された受波信号レベルは読出し専用メモリ8
へ導かれる。読出し専用メモリ8には設定器9の
設定データも導かれており、読出し専用メモリ8
はA/D変換器7のデイジタルデータと設定器9
の設定データとによつて決まる記憶番地の記憶デ
ータが読出される。設定器9は可変利得増巾器4
の増巾度を所望の増巾度に設定しようとする設定
値が設定される。 On the other hand, the reception signal of any one of the ultrasonic receivers T 1 to T o , for example, the reception signal of the n-th ultrasonic receiver T o, is A/D. The received signal level is guided to a converter 7 and converted into digital data. The received signal level converted to digital data is stored in a read-only memory 8.
be led to. The setting data of the setting device 9 is also guided to the read-only memory 8.
is the digital data of the A/D converter 7 and the setting device 9
The stored data at the storage address determined by the setting data is read out. The setting device 9 is a variable gain amplifier 4
A setting value is set to set the degree of amplification to a desired degree of amplification.
読出し専用メモリ8から読出された記憶データ
は可変利得増巾器4へ導かれて、その増巾度を記
憶データの値に対応した増巾度に制御する。 The stored data read from the read-only memory 8 is guided to the variable gain amplifier 4, and its amplification degree is controlled to an amplification degree corresponding to the value of the stored data.
増巾度の制御は、例えば、増巾度の異なる増巾
器を複数個用意して、受波ビーム信号の増巾をい
ずれかの増巾器に切換えて使用するか、あるい
は、増巾器を適宜組合わせて増巾することにより
所望の増巾度を得る。又、可変利得増巾器4は減
衰器を用いて構成することもできる。すなわち、
各々の減衰度が異なる複数の減衰器を用いて、こ
れら減衰器を切換え、あるいは、組合わせを適宜
切換えて受波信号の減衰度を所定量になるように
してもよい。従つて、減衰器を用いる場合は受波
ビーム信号を増巾する増巾器は増巾度が一定のも
のを用いることができる。 The amplification degree can be controlled by, for example, preparing multiple amplifiers with different amplification degrees and switching the amplification of the received beam signal to one of the amplifiers. A desired degree of widening can be obtained by appropriately combining and widening. Further, the variable gain amplifier 4 can also be configured using an attenuator. That is,
A plurality of attenuators each having a different degree of attenuation may be used, and these attenuators may be switched, or the combination may be appropriately switched so that the degree of attenuation of the received signal becomes a predetermined amount. Therefore, when an attenuator is used, an amplifier that amplifies the received beam signal can have a constant amplification degree.
可変利得増巾器4の増巾度制御は、指向性ビー
ム形成回路2から出力される受波ビーム信号を増
巾したとき増巾出力が飽和しないように行われ
る。例えば、可変利得増巾器4の増巾出力の飽和
レベルをEs′設定器9の設定増巾度をGcont、受
波ビーム信号の入力レベルをVinとすると、可変
利得増巾度4が設定増巾度Gcontで増巾した場合
の出力レベルVoutは、
Vout=Vin×Gcont ……(1)
で与えられるから、この出力レベルVoutが飽和
しないためには、出力レベルVoutが
Vout≦Es ……(2)
になるように増巾度を制御すればよい。 The amplification degree control of the variable gain amplifier 4 is performed so that the amplification output does not become saturated when the received beam signal output from the directional beam forming circuit 2 is amplified. For example, if the saturation level of the amplification output of the variable gain amplifier 4 is the amplification degree set by the E s ' setter 9 is Gcont, and the input level of the received beam signal is Vin, then the variable gain amplification degree 4 is set. The output level Vout when amplified by the amplification degree Gcont is given by Vout=Vin×Gcont...(1) Therefore, in order for this output level Vout not to be saturated, the output level Vout must be Vout≦E s ... The degree of amplification can be controlled so that …(2) is achieved.
従つて、読出し専用メモリ8の記憶番地の入力
レベルVinと設定増巾度Gcoutとによつて指定さ
れる記憶番地に、出力レベルVoutが(2)式を満足
するような増巾度データを書込んでおけばよい。 Therefore, amplification degree data such that the output level Vout satisfies equation (2) is written to the memory address specified by the input level Vin and the set amplification degree Gcout of the memory address of the read-only memory 8. Just keep it in there.
(発明の結果)
以上説明したように、この発明は、指向性受波
ビームを形成する複数の超音波受波器のいずれか
の受波信号レベルを用いて受波ビームの増巾度あ
るいは減衰度を制御するようになされている。(Results of the Invention) As explained above, the present invention uses the received signal level of any one of a plurality of ultrasonic receivers that form a directional received beam to determine the degree of amplification or attenuation of the received beam. It is designed to control the degree of
第5図aは指向性ビーム形成回路2の出力信号
を示し、同図bは超音波受波器Toの受波信号を
示す。受波ビーム信号aにおいて、R0は送信パ
ルス、R1,R2,R3,R4は指向性受波ビーム3の
主ビームによつて受波される海底反射波、Rsは
副ビームによつて受波される海底反射波を示す。
海底反射波R1,R2,R3,R4は指向性受波ビーム
の指向方向が海底反射波の到来方向に一致したと
きに生じる。例えば、海底反射波R1は直下の海
底点P0(第2図)からの反射波を示し、指向性受
波ビーム3の主ビームMが直下の海底P0方向を
指向したときに生じる。 FIG. 5a shows the output signal of the directional beam forming circuit 2, and FIG. 5b shows the received signal of the ultrasonic receiver T o . In the reception beam signal a, R 0 is the transmission pulse, R 1 , R 2 , R 3 , R 4 are the seabed reflected waves received by the main beam of the directional reception beam 3, and R s is the sub beam. The figure shows the seafloor reflected waves received by the sea.
Seabed reflected waves R 1 , R 2 , R 3 , and R 4 are generated when the direction of the directional receiving beam matches the arrival direction of the seabed reflected waves. For example, the seabed reflected wave R 1 indicates a reflected wave from the seabed point P 0 (FIG. 2) just below, and is generated when the main beam M of the directional reception beam 3 is directed in the direction of the seabed P 0 just below.
今、時刻t1からt2の△t時間に指向性受波ビーム
3が探知範囲θを操作するものとすると、時刻t1
から△t/2時間後に海底反射波R1が生じる。そし
て、時刻t1から△t/2時間、並びに海底反射波R1
が生じてから時刻t2までの△2/2時間は副ビーム
SあるいはS′による海底反射波Rsが生じる。な
お、副ビームSによる海底反射波Rsが受波され
る時刻t1までの時間tSUBは、超音波パルスを送波
してから直下の海底点P0からの反射波が受波さ
れるまでの時間を求めることにより知ることがで
きる。従つて、直下の海底点P0までの距離をD0、
音波の伝播速度をCとすると、
tSUB=2D0/C
を計算することにより得られる。 Now, suppose that the directional reception beam 3 manipulates the detection range θ at time △ t from time t 1 to t 2 , then at time t 1
After △t/2 hours, a seafloor reflected wave R 1 is generated. Then, for Δt/2 hours from time t 1 and for Δ2/2 hours from the generation of the seabed reflected wave R 1 to time t 2 , a seabed reflected wave R s is generated by the sub-beam S or S′. Note that the time t SUB from when the seabed reflected wave R s by the sub beam S is received is the time t SUB from when the ultrasonic pulse is transmitted to when the reflected wave from the seabed point P 0 immediately below is received. You can find out by finding the time until. Therefore, the distance to the seabed point P 0 immediately below is D 0 ,
If the propagation speed of the sound wave is C, it can be obtained by calculating t SUB =2D 0 /C.
次に、時刻t2からt3の△t時間に指向性受波ビ
ーム3が探知範囲角θを走査するときは、探知パ
ルスの等位相波面が海底表面に到達するP1、P′1
点からの反射波R2、R′2が受波される。この反射
波R2、R′2が受波される時刻は指向性受波ビーム
3が直下の海底点P0方向を指向する時刻に対し
て△t〓1時間だけ変化する。この変化時間△t〓1は、
直下の海底点P0に対する海底反射波P1、P′1の変
移角△θ1を指向性受波ビーム3が走査する時間に
対応する。 Next, when the directional receiving beam 3 scans the detection range angle θ during time Δt from time t 2 to t 3 , the equiphase wavefront of the detection pulse reaches the seabed surface P 1 , P′ 1
Reflected waves R 2 and R′ 2 from the point are received. The time at which the reflected waves R 2 and R' 2 are received changes by △t〓 1 hour with respect to the time at which the directional reception beam 3 is directed toward the seabed point P 0 directly below. This change time △t〓 1 is
This corresponds to the time during which the directional reception beam 3 scans the displacement angle Δθ 1 of the seabed reflected waves P 1 and P′ 1 with respect to the seabed point P 0 immediately below.
同様にして、時刻t3からt4の△t時間には、探
知パルスの等位相波面が海底表面に到達するP2、
P′2からの反射波R3、R′3が受波される。 Similarly, at time △t from time t3 to time t4 , the equiphase wavefront of the detection pulse reaches the seafloor surface P2 ,
Reflected waves R 3 and R′ 3 from P′ 2 are received.
この発明においては、超音波受波器T1乃至To
のいずれかの受波信号(第5図b)を用いて増巾
度制御を行なうものである。 In this invention, the ultrasonic receivers T 1 to T o
Amplification degree control is performed using one of the received signals (FIG. 5b).
超音波受波器T1乃至Toの各々は、ほぼ無指向
性であるから、第5図bのように、直下の海底
P0からの反射波帰来時刻t1から所定時間tkは極め
て信号レベルの強い反射波が受波される。この信
号持続時間tkは、探知パルスの等位相波面が直下
の海底P0(第2図)に到達した後、海底Bの表面
をP1、P2、P3へ変移する時間にほぼ等しい。従
つて、この受波信号bの信号レベルを用いて増巾
度制御を行なうことにより、不要反射波Rsの出
現時に一致して増巾度制御を行なうことができ、
それによつて不要反射波Rsを十分抑圧して有効
な反射波のみを表示させることができる。 Each of the ultrasonic receivers T 1 to T o is almost omnidirectional, so as shown in Figure 5b, each of the ultrasonic receivers T 1 to T o
A reflected wave with an extremely strong signal level is received for a predetermined time t k from the return time t 1 of the reflected wave from P 0 . This signal duration t k is approximately equal to the time it takes for the equiphase wavefront of the detection pulse to travel on the surface of the seabed B to P 1 , P 2 , and P 3 after reaching the sea bottom P 0 (Figure 2) directly below. . Therefore, by performing the amplification degree control using the signal level of the received signal b, the amplification degree control can be performed at the same time as the unnecessary reflected wave R s appears.
Thereby, unnecessary reflected waves R s can be sufficiently suppressed and only effective reflected waves can be displayed.
第1図はこの発明の実施例を示し、第2図はそ
の探知状況を説明するための図、第3図は従来の
探知映像を説明するための図、第4図はこの発明
の表示ラスタを説明するための図、第5図はその
動作を説明するための波形図を示す。
1……送信器、2……指向性ビーム形成回路、
3……指向性受波ビーム、4……増巾器、5……
表示器、6……走査回路、7……A/D変換器、
8……読出専用メモリ、9……設定器。
FIG. 1 shows an embodiment of the present invention, FIG. 2 is a diagram for explaining the detection situation, FIG. 3 is a diagram for explaining a conventional detection image, and FIG. 4 is a display raster of the present invention. FIG. 5 shows a waveform diagram for explaining its operation. 1... Transmitter, 2... Directional beam forming circuit,
3... Directional receiving beam, 4... Amplifier, 5...
Display device, 6...scanning circuit, 7...A/D converter,
8... Read-only memory, 9... Setting device.
Claims (1)
向から帰来する反射波をそれぞれの対応位置に表
示する水中探知装置において、 ほぼ無指向性同一特性の複数の超音波受波器が
配列されて構成され、上記広範囲方向から帰来す
る反射波を受波して各超音波受波器がほぼ同一出
力を生じる超音波受波装置と、 上記超音波受波器の各受波信号の位相関係を適
宜設定して互いに合成することにより特定方向に
指向性を有する指向性受波ビームを形成し、か
つ、上記位相関係を変化させることにより該指向
性受波ビームの指向方向を順次変化させる指向性
受波ビーム形成回路と、 上記複数の超音波受波器のうち任意に定めたい
ずれかの超音波受波器の受波信号に基づいて、該
受波信号が受信されている間該受波信号の受信レ
ベルに対応して予め定めた特定の増幅度になるよ
うに、上記受波ビーム形成回路の出力する受波信
号を増幅する増幅器の制御を行なう信号レベル制
御回路とを具備してなる広範囲水中探知装置にお
ける不要反射波抑圧装置。[Claims] 1. In an underwater detection device that transmits and receives ultrasonic pulses in a wide range of directions and displays reflected waves returning from each direction at respective corresponding positions, a plurality of ultrasonic receivers having substantially omnidirectional and identical characteristics are provided. an ultrasonic receiver configured by arranging wave transducers, each ultrasonic receiver generating substantially the same output by receiving reflected waves returning from the wide range of directions, and each receiver of the ultrasonic receiver; By appropriately setting the phase relationship of the wave signals and combining them with each other, a directional received beam having directivity in a specific direction is formed, and by changing the phase relationship, the directional direction of the directional received beam can be changed. The received signal is received based on a directional receiving beam forming circuit that sequentially changes the received signal, and a received signal of any arbitrarily determined ultrasonic receiver among the plurality of ultrasonic receivers. a signal level control circuit that controls an amplifier that amplifies the received signal output from the received beam forming circuit so that the received signal is amplified to a predetermined specific amplification degree corresponding to the received level of the received signal; An unnecessary reflected wave suppression device in a wide range underwater detection device, comprising:
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP26702784A JPS61144583A (en) | 1984-12-18 | 1984-12-18 | Unnecessary reflected wave suppressing device in wide range underwater detecting device |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP26702784A JPS61144583A (en) | 1984-12-18 | 1984-12-18 | Unnecessary reflected wave suppressing device in wide range underwater detecting device |
Publications (2)
| Publication Number | Publication Date |
|---|---|
| JPS61144583A JPS61144583A (en) | 1986-07-02 |
| JPH0374956B2 true JPH0374956B2 (en) | 1991-11-28 |
Family
ID=17439034
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP26702784A Granted JPS61144583A (en) | 1984-12-18 | 1984-12-18 | Unnecessary reflected wave suppressing device in wide range underwater detecting device |
Country Status (1)
| Country | Link |
|---|---|
| JP (1) | JPS61144583A (en) |
Families Citing this family (1)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| JP5234611B2 (en) * | 2008-09-19 | 2013-07-10 | 古野電気株式会社 | Ultrasonic detector |
Family Cites Families (2)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| JPS58177883U (en) * | 1982-05-20 | 1983-11-28 | 海上電機株式会社 | Underwater signal receiving device |
| JPS5928681A (en) * | 1982-08-09 | 1984-02-15 | Furuno Electric Co Ltd | Measuring device of bearing in reception ultrasonic wave with high accuracy |
-
1984
- 1984-12-18 JP JP26702784A patent/JPS61144583A/en active Granted
Also Published As
| Publication number | Publication date |
|---|---|
| JPS61144583A (en) | 1986-07-02 |
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| Date | Code | Title | Description |
|---|---|---|---|
| LAPS | Cancellation because of no payment of annual fees |