JPH02228580A - Sonar transmission circuit - Google Patents
Sonar transmission circuitInfo
- Publication number
- JPH02228580A JPH02228580A JP5115089A JP5115089A JPH02228580A JP H02228580 A JPH02228580 A JP H02228580A JP 5115089 A JP5115089 A JP 5115089A JP 5115089 A JP5115089 A JP 5115089A JP H02228580 A JPH02228580 A JP H02228580A
- Authority
- JP
- Japan
- Prior art keywords
- transmission
- circuit
- transducer
- beams
- split
- 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.)
- Granted
Links
- 230000005540 biological transmission Effects 0.000 title claims abstract description 84
- XLYOFNOQVPJJNP-UHFFFAOYSA-N water Substances O XLYOFNOQVPJJNP-UHFFFAOYSA-N 0.000 claims description 2
- 230000015572 biosynthetic process Effects 0.000 abstract description 4
- 238000005259 measurement Methods 0.000 abstract description 3
- 238000003786 synthesis reaction Methods 0.000 abstract 1
- 230000010363 phase shift Effects 0.000 description 12
- 238000010586 diagram Methods 0.000 description 9
- 238000002592 echocardiography Methods 0.000 description 4
- 239000002131 composite material Substances 0.000 description 2
- 238000000034 method Methods 0.000 description 2
- 230000003321 amplification Effects 0.000 description 1
- 239000003795 chemical substances by application Substances 0.000 description 1
- 239000012141 concentrate Substances 0.000 description 1
- 230000001934 delay Effects 0.000 description 1
- 238000001514 detection method Methods 0.000 description 1
- 230000006866 deterioration Effects 0.000 description 1
- 230000000694 effects Effects 0.000 description 1
- 230000002452 interceptive effect Effects 0.000 description 1
- 238000003199 nucleic acid amplification method Methods 0.000 description 1
- 230000005855 radiation Effects 0.000 description 1
Landscapes
- Measurement Of Velocity Or Position Using Acoustic Or Ultrasonic Waves (AREA)
Abstract
Description
【発明の詳細な説明】
〔産業上の利用分野〕
本発明はンーナー送信回路に関し、特に水中に音波を発
射して目標物体からの反響音を受信し、これを映像表示
して目標の捜索、探知を行うアクティブソーナー装置に
おいて、回転ビーム送信(Rotating Dire
ctional Transmission、以下RD
Tと略称する)を行うソーナー送信回路に関する。[Detailed Description of the Invention] [Industrial Application Field] The present invention relates to a sound transmitting circuit, and in particular, it emits sound waves into water, receives echoes from a target object, displays the echoes as images, and searches for a target. In active sonar devices that perform detection, rotating beam transmission (Rotating Dire
ctional Transmission, hereinafter referred to as RD
This invention relates to a sonar transmitter circuit that performs a sonar transmission circuit (abbreviated as T).
アクティプソーナー装置にンいて、高い目標捜索能力を
得るためには1%定方向にのみ送信エネルギーを集中的
に放射し、これを送信パルスごとに順次回転し全方位範
囲または特定角度範囲に送信を行うことが必要である。For active sonar devices, in order to obtain a high target search ability, it is necessary to concentrate 1% of the transmission energy in a fixed direction, rotate this sequentially for each transmission pulse, and transmit in an omnidirectional range or a specific angular range. It is necessary to do so.
第4図は凡DTを行なう従来のソーナー送信回路の構成
図である。FIG. 4 is a block diagram of a conventional sonar transmitter circuit that performs DT.
第4図に示すソーナー送信回路は、iステーブ。The sonar transmitting circuit shown in FIG. 4 is an i-stave.
jスタックの送受波器素子から成る円周配列型の送受波
器1と、送信パルスごとに利用するmステーブの送受波
器素子を切シ替える送信切替回路2a、RDTによる送
波ビーム形成に必要なmステープ、第4図の場合は10
ステープの送受波器素子に対して送信電力を印加する1
0チヤンネルの電力増幅器10−1〜10−10.電力
増幅器10−1〜10−10に供給する送信信号の整相
を行なう送信整相回路9−1〜9−5、送信信号として
のPCW波を形成するパルス変調回路6、送信周波数を
発振する発信回路7のほか、RDT送信のタイミングお
よびパルス幅制御を行なうRDT制御回路8aを備えて
成る。A circumferentially arrayed transducer 1 consisting of j-stack transducer elements and a transmission switching circuit 2a that switches the m-stave transducer elements used for each transmission pulse, necessary for transmitting beam formation by RDT. m staple, 10 in the case of Figure 4
Applying transmission power to the transducer element of the tape 1
0 channel power amplifiers 10-1 to 10-10. Transmission phasing circuits 9-1 to 9-5 perform phasing of transmission signals supplied to power amplifiers 10-1 to 10-10, a pulse modulation circuit 6 forms a PCW wave as a transmission signal, and oscillates a transmission frequency. In addition to the transmitting circuit 7, it is provided with an RDT control circuit 8a that controls the timing and pulse width of RDT transmission.
回転ビーム送信、すなわちRDT送信を行なうには、送
受波器1をビームの指向特性等を勘案して決定する連続
し九mステープずつ送信ごとに円周方同右もしくは左ご
とに通常拡1ステープずつシフトしながら切シ出し、各
ステーブに対応した電力増幅器の入力信号を円周方向に
対称なステーブごとに遅延し、送受波器素子の円周配列
位置による相互間の行程差を無くすことによって、音響
的には恰もmステープの等価矩形板配列による送波ビー
ムを得て、との送波ビームを円周方向にステーブごとの
ステップで次次に形成していくものである。To perform rotating beam transmission, that is, RDT transmission, the transducer 1 is normally expanded by 1 step on each side of the circumference on the same right or left side for each transmission in consecutive 9 m steps determined by taking into account the beam's directivity characteristics, etc. By cutting out while shifting, delaying the input signal of the power amplifier corresponding to each stave for each stave that is symmetrical in the circumferential direction, and eliminating the difference in path between the transducer elements due to the circumferential array position, Acoustically speaking, a transmitting beam is obtained by an equivalent rectangular plate arrangement of m-staves, and the transmitting beam is successively formed in the circumferential direction in steps for each stave.
第4図の場合は10ステープの送受波器素子を右回夛に
1ステーブずつシフトしながらビーム回転を行なう几D
Tの場合で、10ステープのうち両端の2ステープを基
準とし中央の2ステーブに到るまでの対称2ステ一プ分
ずつに次次に基準ステーブと同一位相となるように遅延
を与える整相を行なって等価矩形板配列を形成している
。In the case of Figure 4, beam rotation is performed by shifting the transducer elements of 10 staves clockwise one stave at a time.
In the case of T, phasing that uses the two end staves of the 10 staves as a reference and delays each two symmetrical steps until reaching the two central staves so that the phase is the same as that of the reference stave. is performed to form an equivalent rectangular plate array.
送信整相回路9−1〜9−5は、10ステープの両端ス
テーブに対応する電力増幅器10−1と10−10に基
準位相ψ□を付与し、中央の隣接2ステープに対応する
電力増幅器10−5.10−6に対する位相量ψ、まで
の各位相91〜95間には前述した目的の移相を施し、
従って10ステープは見掛上行程差のない状態で駆動さ
れる。The transmission phasing circuits 9-1 to 9-5 provide a reference phase ψ□ to the power amplifiers 10-1 and 10-10 corresponding to the staves at both ends of the 10 staves, and the power amplifiers 10 corresponding to the two adjacent staves in the center. -5.The phase amount ψ for 10-6 is applied to each phase between 91 and 95 as described above,
Therefore, the ten staples are driven with no apparent difference in stroke.
このような送波ビームによる1個の送信パルスが送出さ
れるごとに送信切替回路2aによって電力増幅器10−
1〜10−10と送受波器1のステーブ対応を右もしく
は左方向に1ステーブずクシフトし、ステーブ間の配列
角度差αだけシフトした方向に送波ビームを形成して次
の送信を行表い、これを所要の角度範囲にわたって順次
繰返す。Every time one transmission pulse is transmitted by such a transmission beam, the transmission switching circuit 2a switches the power amplifier 10-
1 to 10-10 and the stave correspondence of the transducer 1 are shifted by one stave to the right or left, and a transmission beam is formed in the direction shifted by the arrangement angle difference α between the staves to perform the next transmission. This is then repeated over the required angle range.
第5図は従来のRDT送信における送信ビーム方位の特
性図である。RDTにおける送信ビーム方位は、音響基
準方位を#□とした場合、1送信ごとにステーブ配列角
度差αのステップで変化し、PCW波による送信パルス
がθ□、θ□+α、θ。+2α・・・とαごとに送信間
隔δで送出される状態を示している。FIG. 5 is a characteristic diagram of the transmission beam direction in conventional RDT transmission. When the acoustic reference direction is #□, the transmission beam direction in RDT changes in steps of the stave arrangement angle difference α for each transmission, and the transmission pulses by the PCW wave are θ□, θ□+α, θ. +2α . . . shows a state in which data is transmitted at a transmission interval δ for each α.
こうして次次く形成される送信ビームの指向性は、通常
、隣接ビームとほぼ3a波減衰で交差するように調整さ
れる。The directivity of the subsequently formed transmit beam is usually adjusted so that it intersects the adjacent beam with approximately 3a-wave attenuation.
上述した従来のンーナー送信回路によるRDT送波ビー
ムは、隣接ビーム間で互いにほぼ3dB減衰点で交差す
るように設定されているため、放射エネルギーは送受波
器の全周にわたってほぼ均一となるものの、各送波ビー
ムの中間方位では正常な送信パルスのほかに送信パルス
幅分時間のずれた送信パルスも放射されることとなシ、
同一目標からの反響音が2つ発生し、距離測定に大きな
誤差を生ずるとともに、奥行のある目標の場合には2つ
の反響音が重畳し波形による目標類別を著しく阻害する
という欠点がある。The RDT transmission beams from the conventional transducer transmitter circuit described above are set so that adjacent beams intersect with each other at approximately 3 dB attenuation points, so the radiated energy is approximately uniform over the entire circumference of the transducer. In addition to the normal transmission pulse, in the intermediate direction of each transmission beam, a transmission pulse with a time difference of the transmission pulse width is also emitted.
Two echoes from the same target are generated, causing a large error in distance measurement, and in the case of a deep target, the two echoes are superimposed, significantly interfering with target classification based on waveforms.
本発明の目的は上述した欠点を除去し、送波ビームの中
間方位でも距離誤差と目標類別機能の低下を著しく抑圧
しうるソーナー送信回路を提供することKある。SUMMARY OF THE INVENTION An object of the present invention is to provide a sonar transmitting circuit which eliminates the above-mentioned drawbacks and can significantly suppress distance errors and deterioration of target classification function even in intermediate directions of a transmitted beam.
本発明の回路は1円筒状に配列した送受波器素子から成
る送受波器の一部分ずつを送信パルスで駆動しかつ送信
パルスごとに円周方向に所定のステップでシフトしつつ
切シ替えて水中に音波を放射する回転ビーム送信を行な
うソーナー送信回路において、送信パルスごとに駆動す
る送受波器素子群を重複を許容して円周方向に2分割し
た右および左の送受波器素子群でそれぞれ同一方位を指
向した左右一対のビームから成るスプリットビームを形
成するスプリットビー、ム形成手段と、前記スプリット
ビームの回転におけるステップ間シフトを連続的に実行
させるように前記スプリットビームを形成する左右ビー
ム間に連続的に位相差を付与する位相差付与手段とを備
えて構成される。The circuit of the present invention drives each part of a transducer consisting of transducer elements arranged in a cylindrical shape with a transmission pulse, and switches the transducer while shifting in a predetermined step in the circumferential direction for each transmission pulse. In a sonar transmission circuit that transmits a rotating beam that emits sound waves, the transducer element group that is driven for each transmission pulse is divided into two in the circumferential direction, allowing overlap, and the transducer element group is divided into right and left transducer element groups, respectively. A split beam forming means for forming a split beam consisting of a pair of left and right beams oriented in the same direction, and a left and right beam forming means for forming the split beam so as to continuously perform a shift between steps in the rotation of the split beam. and a phase difference applying means for continuously applying a phase difference to.
次に図面を参照して本発明を説明する。第1図は本発明
のンーナー送信回路の一実施例の構成図である。Next, the present invention will be explained with reference to the drawings. FIG. 1 is a block diagram of an embodiment of a receiver transmitting circuit according to the present invention.
第1図に示す実施例は、送受波器1、送信切替回路2、
スプリットビームを形成する右ビームに対する送信電力
を供給するに個の電力増幅器3−IB、3−2B、3−
3R・・・3−に几、左ビームに対する送信電力を供給
するに個の電力増幅器3−IL。The embodiment shown in FIG. 1 includes a transducer 1, a transmission switching circuit 2,
power amplifiers 3-IB, 3-2B, 3- for supplying transmission power for the right beam forming a split beam;
3R...1 power amplifier 3-IL for supplying transmission power for the left beam.
3−2L、3−3L・・・3−kL、電力増幅器3−I
R〜3−kRに対応し右ビーム形成に必要な整相のため
の位相量ψIRtψ5iteψ31L・−・ψkmを与
えるに個の送信整相回路4−IR〜4−kJ左ビーム形
成に必要な整相のための位相量ψ□1.ψ2Ltψ3L
・・・ψkLを与えるに個の送信整相回路4−IL〜4
−kL。3-2L, 3-3L...3-kL, power amplifier 3-I
Transmission phasing circuits 4-IR to 4-kJ to give the phase amount ψIRtψ5iteψ31L·-·ψkm for phasing required for right beam formation corresponding to R~3-kR 4-IR to 4-kJ phasing required for left beam formation The phase amount ψ□1. ψ2Ltψ3L
...Transmission phasing circuits 4-IL to 4 to give ψkL
-kL.
ステーブ間の送波ビーム回転を連続的に変化させるため
の連続的可変位相を付与するための右ビーム用の可変移
相回路5a、左ビーム用の可変移相回路5 b 、pc
wの送信パルスを発生するパルス変調回路61発信回転
7 、RDT制御回路8を備えて構成される。A variable phase shift circuit 5a for the right beam, a variable phase shift circuit 5b for the left beam, and a variable phase shift circuit 5b for the left beam to provide a continuously variable phase for continuously changing the transmission beam rotation between the staves.
The device is configured to include a pulse modulation circuit 61 that generates a transmission pulse of w, a transmission rotation 7, and an RDT control circuit 8.
次に、第1図の実施例の動作について説明する。Next, the operation of the embodiment shown in FIG. 1 will be explained.
各部動作に先立ち、スプリットビームについて説明する
。スプリットビームは、左右同数のステーブの送受波器
素子によって同一指向方向に形成した右、左ビームから
成る一対の送波ビームを言い、第1図の例で言えはステ
ーブ1〜5で右ビームを、ステープ1Ni−4で左ビー
ムを形成し、このスプリットビームは空間的に合成され
た合成ビームとして送受信され、2つのビームの空間的
交差領域で目標を高い識別性で探知する目的で運用され
る。Before explaining the operation of each part, the split beam will be explained. A split beam refers to a pair of transmitted beams consisting of right and left beams formed in the same directivity direction by transducer elements of the same number of left and right staves, and in the example in Figure 1, the right beam is , the left beam is formed by the staple 1Ni-4, and this split beam is transmitted and received as a spatially combined composite beam, and is operated for the purpose of detecting targets with high discrimination in the spatial intersection area of the two beams. .
第1図において、発信回路7で発生した連続SIN波の
送信信号は、パルス変調回路6に供給され、RDT制御
回路8で指定されたパルス幅のパルス変調波とされる。In FIG. 1, a continuous SIN wave transmission signal generated by a transmitting circuit 7 is supplied to a pulse modulating circuit 6, and converted into a pulse modulated wave having a pulse width specified by an RDT control circuit 8.
パルス変調回路6の出力信号は、左右のスプリットビー
ムに対応する可変移相回路5a、5bに与えられ、ψい
φRだけ移相される。The output signal of the pulse modulation circuit 6 is applied to variable phase shift circuits 5a and 5b corresponding to left and right split beams, and is phase-shifted by φR.
可変移相回路5a、5bによってスプリットビームの右
ビームに与える移相量ψR1左ビームに与える移相量ψ
8は、第2図(a)に示す如く、送信パルスの始端時に
は左右ビームの音響的中心方向θ。Phase shift amount ψR1 given to the right beam of the split beam by variable phase shift circuits 5a and 5b Phase shift amount ψ given to the left beam
8 is the acoustic center direction θ of the left and right beams at the beginning of the transmission pulse, as shown in FIG. 2(a).
がステープの配列角度差αの1/2だけ左にシフトした
方位に対して直角に交る音響的位置になってスプリット
ビームの合成ビームがθ□−α/2を指向するように互
いの移相差(ψ、−ψR)を制御され、送信ビームの中
央では第2図(b)の如く合成ビームが左右ビームの音
響的中心方向θmと一致し、さらに送信パルス終端時に
は、第2図(C)に示す如く始端時とは逆に、左右ビー
ムの音響的中心方向がステープの配列角度差αの1/2
だけ右にシフトした方位に対して直角に交わる音響的位
置になるように制御してスプリットビームの合成ビーム
がθ□+α/2を指向するように制御し、かつθ□−α
/2からθ。+α/2tで連続的に変化させる。are shifted to the left by 1/2 of the arrangement angle difference α of the staples, and the acoustic position is perpendicular to the azimuth, and the combined beam of the split beams is directed in the direction θ The phase difference (ψ, -ψR) is controlled, and at the center of the transmission beam, the combined beam coincides with the acoustic center direction θm of the left and right beams as shown in Figure 2 (b), and furthermore, at the end of the transmission pulse, the combined beam coincides with the acoustic center direction θm of the left and right beams as shown in Figure 2 (C). ), contrary to the starting point, the acoustic center direction of the left and right beams is 1/2 of the staple arrangement angle difference α.
The combined beam of the split beam is controlled to be directed at θ□+α/2 by controlling the acoustic position to intersect at right angles to the azimuth shifted to the right by θ□−α.
/2 to θ. Continuously change by +α/2t.
すなわち、送信パルスの送出から終了まで、スプリット
ビームによる合成ビームはθ□を中心とし−α/2から
+α/2までステーブの配列角度差αにわたって連続的
に方位変化させながら合成ビームを振ることとなシ、こ
の状態をステーブ歩進ごとに繰返す。In other words, from the sending of the transmission pulse to the end, the combined beam by the split beam is swung while continuously changing its direction from -α/2 to +α/2 over the stave arrangement angle difference α with the center at θ□. This state is repeated every time the stave advances.
送信整相回路4−IR〜4−kRのそれぞれに付与する
位相ψ1R〜ψkinおよび送信整相回路4−1L〜4
−kLのそれぞれに付与する位相ψ1L〜ψkLはスプ
リットビームの右および左ビーム形成に必要な整相のた
めの移相量を与えるように設定され、各移相量は、前述
した如く、1個の送信指向性ビームを形成するために必
要な連続したステイープ群の各ステイープの・配列位置
、すなわち配列角度と配列半径によって決まる固定量で
、音響的に等価な矩形平面板に置換するためのものであ
る。通常、ψIR・ψ2R・ψ3R”’ψkRとψIL
・ψ2L・ψ3L・・・ψれは、左右対応で同一量が設
定される。Phases ψ1R to ψkin given to each of the transmission phasing circuits 4-IR to 4-kR and transmission phasing circuits 4-1L to 4
The phases ψ1L to ψkL given to each of -kL are set to give the phase shift amount necessary for forming the right and left beams of the split beam, and each phase shift amount is one phase shift amount as described above. A fixed amount determined by the arrangement position, i.e., arrangement angle and arrangement radius, of each staple in a continuous group of staples necessary to form a transmitting directional beam of It is. Usually, ψIR, ψ2R, ψ3R"'ψkR and ψIL
- ψ2L, ψ3L... The same amount is set for ψ for left and right.
送信整相回路4−IR〜4−kn、 、 4−I L〜
4−kLの出力はそれぞれ電力増幅器3−IR〜3−k
R,3−IL〜3kLに供給されて電力増幅を行ない、
送信切替回路2を介して送受波器1に供給する。Transmission phasing circuit 4-IR~4-kn, , 4-IL~
The outputs of 4-kL are respectively connected to power amplifiers 3-IR to 3-k.
R, 3-IL ~ 3kL is supplied to perform power amplification,
The signal is supplied to the transducer 1 via the transmission switching circuit 2.
送受波器1は、提供された信号を電気青畳変換し、同一
方向を指向したスプリットビームを形成し、さらに、そ
の合成として合成ビームを形成する。The transducer 1 electrically converts the provided signal to form split beams oriented in the same direction, and further forms a composite beam as a combination of the split beams.
次に、1個の送信パルスが終了すると、RDT制御回路
8の制御で送信切替回路2が、電力増幅器3−IR〜3
−kR,3−IL〜3−kLと送受波器ステイープとの
対応を円周方向に1個ずつシフトし。Next, when one transmission pulse ends, the transmission switching circuit 2 switches the power amplifiers 3-IR to 3 under the control of the RDT control circuit 8.
-kR, 3-IL to 3-kL and the transducer staples are shifted one by one in the circumferential direction.
同様の動作が行われる。これを順次繰り返すことによっ
て、所要の送信角度だけ連続した回転ビーム送信が得ら
れる。A similar operation is performed. By sequentially repeating this process, continuous rotating beam transmission can be obtained for the required transmission angle.
第3図は第1図の実施例の送信ビーム方位の特性図であ
る。本実施例における送信ビーム方位は、青畳基準方位
θ□を中心として−a/2から+α/2まで連続的に変
化し、かつこの変化パターンが+α、+2α・・・+n
αと全放射角範囲にわたって連続的に回転していく状態
を示している。FIG. 3 is a characteristic diagram of the transmission beam direction of the embodiment shown in FIG. The transmission beam direction in this embodiment changes continuously from -a/2 to +α/2 centering on the blue tatami reference direction θ□, and this change pattern is +α, +2α...+n
It shows a state of continuous rotation over α and the entire radiation angle range.
こうして、ビーム回転におけるスタック間のステップシ
フトを連続的に実施することができる。In this way, step shifts between stacks in beam rotation can be performed continuously.
なお上述した実施例でのビームの回転速度は、目標に放
射されるエネルギーを確保するために、通常、送信パル
ス幅期間で3dB送信ビ一ム幅に相当する角度になるよ
うに設定している。Note that the rotational speed of the beam in the above-described embodiment is normally set to an angle corresponding to 3 dB transmission beam width in the transmission pulse width period, in order to ensure the energy radiated to the target. .
また、上述した実施例ではステーブを左右等分割したス
プリットビーム形成としているが、この代りに1部のス
テーブを重複利用する方法でも同様に実施しうることは
明らかである。Further, in the above-described embodiment, a split beam is formed in which the stave is divided into left and right equal parts, but it is clear that the same method can be implemented in which a portion of the stave is used redundantly instead of this.
以上説明したように本発明は、一対のスプリット送信ビ
ームを形成し左右ビームの位相差を連続的に制御すると
とくよって、全周または所要の角度範囲に連続回転のビ
ーム送信を行うことができ、ステップ制御のビーム送信
よシも著しく高い類別能力と大幅に誤差を抑圧した距離
測定ができるという効果がある。As explained above, the present invention forms a pair of split transmission beams and continuously controls the phase difference between the left and right beams, thereby making it possible to perform continuous rotational beam transmission over the entire circumference or within a required angular range. Step-controlled beam transmission also has the advantage of significantly higher classification ability and distance measurement with significantly suppressed errors.
第1図は本発明のソーナー送信回路の一実施例の構成図
、第2図は第1図の実施例のステープ間ビーム回転時に
おけるスプリットビーム移相内容を示す説明図、第3図
は第1図の実施例における送信ビーム方位の特性図、第
4図はRDTを行なう従来のソーナー送信回路の構成図
、第5図は従来のR,DT送信における送信ビームの特
性図である。
1・・・送受波器、2,2a・・・送信切替回路、3−
IR〜3−kR,3−IL〜3−kL、10−1〜10
−10・・・電力増幅器、4−IR〜4−kR,4−I
L〜4−kL。
9−1〜9−5・・・送信整相回路、sa、sb・・・
可変移相回路、6・・・パルス変調回路、7・・・発信
回路、8゜8a・・・RDT制御回路。
代理人 弁理士 内 原 晋
・41区3ベトヘ
第5図FIG. 1 is a block diagram of an embodiment of the sonar transmission circuit of the present invention, FIG. 2 is an explanatory diagram showing the content of split beam phase shift during beam rotation between staples in the embodiment of FIG. 1, and FIG. FIG. 1 is a characteristic diagram of the transmission beam direction in the embodiment, FIG. 4 is a block diagram of a conventional sonar transmission circuit that performs RDT, and FIG. 5 is a characteristic diagram of the transmission beam in the conventional R and DT transmission. 1... Transducer/receiver, 2, 2a... Transmission switching circuit, 3-
IR~3-kR, 3-IL~3-kL, 10-1~10
-10...Power amplifier, 4-IR to 4-kR, 4-I
L~4-kL. 9-1 to 9-5... Transmission phasing circuit, sa, sb...
Variable phase shift circuit, 6... Pulse modulation circuit, 7... Transmission circuit, 8°8a... RDT control circuit. Agent: Susumu Uchihara, Patent Attorney, 41 Ward 3 Betohe Figure 5
Claims (1)
分ずつを送信パルスで駆動しかつ送信パルスごとに円周
方向に所定のステップでシフトしつつ切り替えて水中に
音波を放射する回転ビーム送信を行なうソーナー送信回
路において、 送信パルスごとに駆動する送受波器素子群を重複を許容
して円周方向に2分割した右および左の送受波器素子群
でそれぞれ同一方位を指向した左右一対のビームから成
るスプリットビームを形成するスプリットビーム形成手
段と、 前記スプリットビームの回転におけるステップ間シフト
を連続的に実行させるように前記スプリッドビームを形
成する左右ビーム間に連続的に位相差を付与する位相差
付与手段と、 を備えて成ることを特徴とするソーナー送信回路。[Scope of Claims] A transmitter/receiver consisting of transducer elements arranged in a cylindrical shape is driven by a transmitting pulse, and is switched while being shifted in a predetermined step in the circumferential direction for each transmitting pulse, thereby transmitting sound waves into the water. In a sonar transmission circuit that transmits a rotating beam that emits a split beam forming means for forming a split beam consisting of a pair of left and right beams oriented in the direction of the left and right beams; A sonar transmission circuit comprising: a phase difference imparting means for imparting a phase difference to; and a sonar transmitting circuit.
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP1051150A JP2567084B2 (en) | 1989-03-02 | 1989-03-02 | Sonar transmitter circuit |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP1051150A JP2567084B2 (en) | 1989-03-02 | 1989-03-02 | Sonar transmitter circuit |
Publications (2)
| Publication Number | Publication Date |
|---|---|
| JPH02228580A true JPH02228580A (en) | 1990-09-11 |
| JP2567084B2 JP2567084B2 (en) | 1996-12-25 |
Family
ID=12878788
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP1051150A Expired - Lifetime JP2567084B2 (en) | 1989-03-02 | 1989-03-02 | Sonar transmitter circuit |
Country Status (1)
| Country | Link |
|---|---|
| JP (1) | JP2567084B2 (en) |
Families Citing this family (1)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| JP2734397B2 (en) | 1995-03-22 | 1998-03-30 | 日本電気株式会社 | Active sonar device |
-
1989
- 1989-03-02 JP JP1051150A patent/JP2567084B2/en not_active Expired - Lifetime
Also Published As
| Publication number | Publication date |
|---|---|
| JP2567084B2 (en) | 1996-12-25 |
Similar Documents
| Publication | Publication Date | Title |
|---|---|---|
| US4631710A (en) | Azimuth adaptive phased array sonar | |
| JPS58132677A (en) | Ultrasonic pickup device | |
| US4079352A (en) | Echo sounding technique | |
| EP0293803A2 (en) | Fan-shape scanning ultrasonic flaw detecting apparatus | |
| JPH02228580A (en) | Sonar transmission circuit | |
| JP2001190551A (en) | Ultrasonograph | |
| JP2783246B2 (en) | Active sonar device | |
| JP3772411B2 (en) | Method of controlling transmission from spherical array and spherical array transmitter | |
| JPH01185471A (en) | Sonar apparatus | |
| JPH01180483A (en) | Sonar equipment | |
| JP3111258B2 (en) | Underwater detector | |
| JP2648689B2 (en) | Underwater sound source direction detection device | |
| JP2005106705A (en) | Apparatus for transmitting and receiving ultrasonic wave and scanning sonar | |
| JPH0727850A (en) | Ultrasonic sensor | |
| JPS5930078A (en) | Sonar transmitting and receiving apparatus | |
| JPH02134142A (en) | Electronic radial type ultrasonic beam device | |
| JPH04208889A (en) | Active sonar device | |
| JPS60242365A (en) | Ultrasonic inspecting device | |
| JPS6360348B2 (en) | ||
| JPH0524229Y2 (en) | ||
| JPS59114479A (en) | Sonar transmitting and receiving apparatus | |
| US2665416A (en) | Apparatus for determining the direction of wave energy | |
| JPH0384488A (en) | Ultrasonic distance measuring instrument | |
| GB2058351A (en) | Improvements in or relating to sonar systems | |
| JPH0375172B2 (en) |
Legal Events
| Date | Code | Title | Description |
|---|---|---|---|
| S533 | Written request for registration of change of name |
Free format text: JAPANESE INTERMEDIATE CODE: R313533 |
|
| R350 | Written notification of registration of transfer |
Free format text: JAPANESE INTERMEDIATE CODE: R350 |
|
| FPAY | Renewal fee payment (event date is renewal date of database) |
Free format text: PAYMENT UNTIL: 20071003 Year of fee payment: 11 |
|
| FPAY | Renewal fee payment (event date is renewal date of database) |
Free format text: PAYMENT UNTIL: 20081003 Year of fee payment: 12 |
|
| FPAY | Renewal fee payment (event date is renewal date of database) |
Free format text: PAYMENT UNTIL: 20081003 Year of fee payment: 12 |
|
| S531 | Written request for registration of change of domicile |
Free format text: JAPANESE INTERMEDIATE CODE: R313531 |
|
| FPAY | Renewal fee payment (event date is renewal date of database) |
Free format text: PAYMENT UNTIL: 20081003 Year of fee payment: 12 |
|
| R350 | Written notification of registration of transfer |
Free format text: JAPANESE INTERMEDIATE CODE: R350 |
|
| FPAY | Renewal fee payment (event date is renewal date of database) |
Free format text: PAYMENT UNTIL: 20091003 Year of fee payment: 13 |
|
| EXPY | Cancellation because of completion of term | ||
| FPAY | Renewal fee payment (event date is renewal date of database) |
Free format text: PAYMENT UNTIL: 20091003 Year of fee payment: 13 |