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JPS6348319B2 - - Google Patents
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JPS6348319B2 - - Google Patents

Info

Publication number
JPS6348319B2
JPS6348319B2 JP56139065A JP13906581A JPS6348319B2 JP S6348319 B2 JPS6348319 B2 JP S6348319B2 JP 56139065 A JP56139065 A JP 56139065A JP 13906581 A JP13906581 A JP 13906581A JP S6348319 B2 JPS6348319 B2 JP S6348319B2
Authority
JP
Japan
Prior art keywords
phase
transducer
directions
signal
signals
Prior art date
Legal status (The legal status is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the status listed.)
Expired
Application number
JP56139065A
Other languages
Japanese (ja)
Other versions
JPS5839970A (en
Inventor
Kyonori Okuno
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.)
Japan Radio Co Ltd
Original Assignee
Japan Radio 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 Japan Radio Co Ltd filed Critical Japan Radio Co Ltd
Priority to JP13906581A priority Critical patent/JPS5839970A/en
Publication of JPS5839970A publication Critical patent/JPS5839970A/en
Publication of JPS6348319B2 publication Critical patent/JPS6348319B2/ja
Granted legal-status Critical Current

Links

Classifications

    • GPHYSICS
    • G01MEASURING; TESTING
    • G01SRADIO 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
    • G01S15/00Systems using the reflection or reradiation of acoustic waves, e.g. sonar systems
    • G01S15/02Systems using the reflection or reradiation of acoustic waves, e.g. sonar systems using reflection of acoustic waves
    • G01S15/50Systems of measurement, based on relative movement of the target
    • G01S15/58Velocity or trajectory determination systems; Sense-of-movement determination systems
    • G01S15/60Velocity or trajectory determination systems; Sense-of-movement determination systems wherein the transmitter and receiver are mounted on the moving object, e.g. for determining ground speed, drift angle, ground track

Landscapes

  • Physics & Mathematics (AREA)
  • Engineering & Computer Science (AREA)
  • Radar, Positioning & Navigation (AREA)
  • Remote Sensing (AREA)
  • Acoustics & Sound (AREA)
  • Computer Networks & Wireless Communication (AREA)
  • General Physics & Mathematics (AREA)
  • Measurement Of Velocity Or Position Using Acoustic Or Ultrasonic Waves (AREA)

Description

【発明の詳細な説明】 本発明はドプラ効果を利用した速度測定装置に
係り、特に超音波信号の送波及び受波を行う送受
波器に関するものである。
DETAILED DESCRIPTION OF THE INVENTION The present invention relates to a velocity measuring device that utilizes the Doppler effect, and particularly to a transducer that transmits and receives ultrasonic signals.

従来から知られているドプラ効果を利用した船
舶用速度測定装置は、ドプラ・ソナーあるいはド
プラ・ログなどの名称で知られているように、船
舶より発射された超音波周波数と水底面あるいは
水中の微少物体によつて散乱反射された後、再び
受信された超音波信号の周波数との間に船速に対
応したドプラ偏位が生じることによつて船速を測
定するものである。
Conventionally known speed measurement devices for ships that utilize the Doppler effect, known as Doppler sonar or Doppler log, measure the ultrasonic frequency emitted from a ship and the surface of the water on the bottom or underwater surface. The ship's speed is measured by the occurrence of a Doppler deviation corresponding to the ship's speed between the frequency of the ultrasonic signal that is received again after being scattered and reflected by a minute object.

このような従来装置においては、船舶の動揺に
伴つて超音波信号の発射角度に変化をきたし、そ
れに基づいて測定誤差を生じるものであつたが、
その誤差を軽減する目的で、例えば船舶の前後進
速度を測定する場合には前方向と後方向に等しい
俯角で超音波信号を発射し、それぞれの受信信号
のドプラ偏位の差を求めて前記測定誤差を軽減す
る“JANUS方式”と呼ばれる方法が用いられて
いる。しかしながらこのような方法では送受波器
を前方向用と後方向用とにそれぞれ別個に用いる
ため送受波器装置が大型となり、またそれぞれの
方向の超音波ビームの俯角を正確に一致させるこ
とが困難なため前記の誤差軽減も充分に達成し得
ない欠点があつた。
In such conventional devices, the emission angle of the ultrasonic signal changes as the ship oscillates, resulting in measurement errors.
In order to reduce this error, for example, when measuring the forward and backward speed of a ship, ultrasonic signals are emitted at equal depression angles in the forward and aft directions, and the difference in Doppler deviation of each received signal is determined. A method called the "JANUS method" is used to reduce measurement errors. However, in this method, the transducer device is large because the transducer is used separately for the forward direction and the backward direction, and it is difficult to accurately match the depression angle of the ultrasonic beam in each direction. Therefore, there was a drawback that the above-mentioned error reduction could not be sufficiently achieved.

本発明は、かかる欠点を解消せんとするもので
あつて、単一の送受波器によつて相対する方向例
えば前方向と後方向の超音波信号の発射及び受信
を行ない、もつて装置の小型化を図り、併せてそ
れぞれの放射方向も正確に一致させることを目的
とするものである。
The present invention aims to eliminate such drawbacks, and uses a single transducer to emit and receive ultrasonic signals in opposite directions, such as forward and backward directions, thereby making it possible to reduce the size of the device. The purpose of this is to ensure that the respective radiation directions are exactly the same.

以下図面に示す本発明の一実施例につき詳説す
る。
An embodiment of the present invention shown in the drawings will be explained in detail below.

第1図はフエーズアレー型送受波器の原理図で
あつて、21……2oは素子、θはビーム合成方向
である。第1図に示すように、直線上に間隔dで
n個の素子を配置するフエーズアレー型送受波器
において素子の励振振幅を等しくまた素子間の励
振位相差をδとした場合、この送受波器の指向特
性R(θ)は次の(1)で表わされるが、このことは
広く知られている。
FIG. 1 is a diagram showing the principle of a phase array type transducer, where 2 1 . . . 2 o are elements, and θ is the beam combining direction. As shown in Figure 1, in a phase array type transducer in which n elements are arranged on a straight line with an interval d, if the excitation amplitudes of the elements are equal and the excitation phase difference between the elements is δ, then this transducer The directional characteristic R(θ) is expressed by the following (1), which is widely known.

R(θ)=|1/n・Sin(nφ/2)/Sin(φ/2
)|……(1) 但しφ=2π/λd・sinθ−δ λ:波長 d:素子の間隔 δ:位相差 上記(1)式はφ=2πm(但しm=0、±1、……)
で極大値をとるため、|θ|<π/2の範囲で唯一の メインローブが生じるためには次の(2)式の条件が
満足されねばならない。
R(θ)=|1/n・Sin(nφ/2)/Sin(φ/2
)|……(1) However, φ=2π/λd・sinθ−δ λ: Wavelength d: Element spacing δ: Phase difference Equation (1) above is φ=2πm (however, m=0, ±1,...)
Therefore, in order for a unique main lobe to occur in the range |θ|<π/2, the following condition of equation (2) must be satisfied.

d≦λ(1−δ/2π) ……(2) 素子間隔dが(2)式を満足しない場合は法線方向
に対して対称な2つのメインローブが生じること
になる。一方、(2)式を満足する場合は唯一のメイ
ンローブが生じ、その方向は素子間の位相差δの
等号の向きにより法線方向に対して対称に変化す
ることになる。本発明はこのような原理にもとず
き単一の送受波器で送波時には等価的に(2)式の条
件を満足しないように工夫し、法線方向に対して
対称な2つのメインローブを作り、また逆に受波
時には等価的に(2)式の条件を満足するように工夫
し、かつ素子間の位相差δの等号を変えることに
より前方向と後方向よりの信号を別々に受信でき
るように構成したものである。
d≦λ(1−δ/2π) (2) If the element spacing d does not satisfy equation (2), two main lobes symmetrical with respect to the normal direction will be generated. On the other hand, when formula (2) is satisfied, only one main lobe is generated, and its direction changes symmetrically with respect to the normal direction depending on the direction of the equal sign of the phase difference δ between the elements. Based on this principle, the present invention is devised so that the condition of equation (2) is not equivalently satisfied when transmitting waves using a single transducer, and two main transducers symmetrical with respect to the normal direction are used. By creating a lobe and conversely satisfying the condition of equation (2) equivalently during reception, and by changing the equal sign of the phase difference δ between the elements, the signals from the front and rear directions can be It is configured so that it can be received separately.

第2図に示す本発明の一実施例によれば、1は
送受波器、21……2oは素子、3および4は位相
反転器、5および6は送受切換器、7は送信器、
8は進相器、9は遅相器、そして10および11
は加算器である。
According to an embodiment of the present invention shown in FIG. 2, 1 is a transducer, 2 1 ...2 o is an element, 3 and 4 are phase inverters, 5 and 6 are transducers, and 7 is a transmitter. ,
8 is a phase advancer, 9 is a phase lag, and 10 and 11
is an adder.

送受波器1の素子21〜2oは第2図に示すよう
に4個目ごとに互いに接続されていて、1相から
4相までの4種類にまとめられている。
The elements 2 1 to 2 o of the transducer 1 are connected to each other every fourth as shown in FIG. 2, and are grouped into four types from 1 phase to 4 phases.

送波時における動作は、送信器7で発生された
信号が送受切換器5および6を通り送受波器1を
駆動する。この時位相反転器3および4により3
相と4相の信号は、それぞれ1相と2相の信号と
比べると位相が反転していることになる。このた
め素子21〜2oの駆動位相は第3図に示すごとき
ものとなり、今素子間間隔dをλ/2に選んだ場
合は等価的な素子間隔はλとなり、また位相差δ
はπのため前記(1)式および(2)式よりメインローブ
の方向は法線に対して30度となりまた左右対称に
2個発生する。
During wave transmission, a signal generated by the transmitter 7 passes through the transmitter/receiver switchers 5 and 6 and drives the transmitter/receiver 1. At this time, the phase inverters 3 and 4
The phases of the phase and four-phase signals are inverted compared to the one-phase and two-phase signals, respectively. Therefore, the drive phase of elements 2 1 to 2 o becomes as shown in Fig. 3. If the inter-element spacing d is selected to be λ/2, the equivalent element spacing will be λ, and the phase difference δ
is π, so from equations (1) and (2) above, the direction of the main lobe is 30 degrees with respect to the normal line, and two main lobes are generated symmetrically.

次に受波時の動作については、まず送受波器1
からの信号のうち1相と、位相反転器3を通つた
2相の信号とが加え合わされた上送受切換器5へ
導かれる。同様に、3相と位相反転器4を通つて
4相の信号とが加えられた上送受切換器6へ導か
れる。送受切換器6を通つた信号のうち一方は進
相器8で位相をπ/2だけ進めた後、送受切換器
5を通つた信号と加算器10によつて加算され前
方向の受信信号EFを得ることができる。
Next, regarding the operation during wave reception, first the transducer 1
One phase of the signals from the two-phase signal and the two-phase signals passed through the phase inverter 3 are added to the upper transmission/reception switch 5. Similarly, the three-phase signal and the four-phase signal are introduced through the phase inverter 4 to the upper transmission/reception switch 6. One of the signals passing through the transmitter/receiver switch 6 is advanced in phase by π/2 by a phase advancer 8, and then added to the signal that has passed through the transmitter/receiver switch 5 by an adder 10, resulting in a forward reception signal E. You can get F.

送受切換器6を通る信号のうちの他方は、遅相
器9で位相をπ/2だけ遅らせた後、送受切換器
5を通つた信号と加算器11によつて加算され後
方向の受信信号EAを得ることができる。このた
め素子21〜2oの位相関係は、前方向の受信信号
EFに対しては第4図に示すごとく、また後方向
の受信信号EAに対しては第5図に示すようにな
る。このため(1)式および(2)式よりメインローブの
方向は法線方向に対して+30度と−30度となりそ
れぞれ目的方向の信号を受信することが可能とな
る。
The other of the signals passing through the transmitter/receiver switch 6 is delayed in phase by π/2 in a phase delayer 9, and then added to the signal that has passed through the transmitter/receiver switch 5 by an adder 11 to produce a backward reception signal. EA can be obtained. Therefore, the phase relationship between elements 2 1 to 2 o is
As shown in FIG. 4 for E F , and as shown in FIG. 5 for backward received signal E A. Therefore, from equations (1) and (2), the directions of the main lobe are +30 degrees and -30 degrees with respect to the normal direction, making it possible to receive signals in the respective target directions.

以上の実施例説明においては、素子間間隔dを
λ/2に、また位相差δをπ/2に選択したが、
それらは前記(1)式および(2)式を満足する範囲で任
意に選択可能である。また、位相反転器3および
4を送受波器1に内蔵したり、あるいは素子2の
分極方向を工夫することにより省略することも可
能である。
In the above embodiment description, the inter-element spacing d was selected to be λ/2 and the phase difference δ was selected to be π/2.
They can be arbitrarily selected within a range that satisfies the above formulas (1) and (2). Furthermore, it is also possible to omit the phase inverters 3 and 4 by incorporating them into the transducer 1 or by modifying the polarization direction of the element 2.

同様に、素子2の励振振幅を変えサイドローブ
レベルを抑圧するシエーデイングの技法を適用す
ることもまた可能である。また、前述実施例では
発射方向を前後方向のみとした速度測定について
述べたが、同様に左右方向にも超音波信号を発射
し、前後のみならず左右方向の速度成分をも同時
に測定することが可能である。
Similarly, it is also possible to apply a shading technique that changes the excitation amplitude of the element 2 and suppresses the sidelobe level. In addition, although the above embodiment described speed measurement in which the emission direction was only in the front-rear direction, it is also possible to emit ultrasonic signals in the left-right direction as well, and simultaneously measure velocity components not only in the front-rear direction but also in the left-right direction. It is possible.

以上述べたとおり、単一の送受波器によつて、
送波時には相対する方向例えば前後方向にほゞ等
しい俯角をもつた2個の超音波ビームを合成し、
前後方向に同時に超音波信号を発射し、一方受波
時には前方向、後方向それぞれ単独にビーム合成
を行なうため、ドプラ効果を利用した速度測定装
置における送受波器装置の小型化が可能となり、
さらに前後方向で超音波ビームの俯角が正確に一
致するためJANUS方式による前述の動揺誤差を
軽減せしめることが可能となつた効果は実用上顕
著なものである。
As mentioned above, with a single transducer,
When transmitting waves, two ultrasonic beams with approximately equal depression angles are combined in opposite directions, for example, in the front-back direction,
Ultrasonic signals are simultaneously emitted in the front and rear directions, while beams are combined separately in the front and rear directions when receiving waves, making it possible to downsize the transducer device in speed measurement devices that utilize the Doppler effect.
Furthermore, since the depression angles of the ultrasonic beams accurately match in the front-rear direction, the effect of reducing the above-mentioned oscillation error due to the JANUS method is significant in practical terms.

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

第1図は、フエーズアレー型送受波器の動作原
理を説明するための図、第2図は本発明実施例装
置を示すブロツク回路図、第3図は該実施例にお
ける送波時のビーム合成を説明する図、第4図お
よび第5図は、該実施例における前方向受波時と
後方向受波時のビーム合成をそれぞれ説明する図
面である。 符号の説明 1……送受波器、21〜2o……素
子、3,4……位相反転器、5,6……送受切換
器、7……送信器、8……進相器、9……遅相
器、10,11……加算器。
Fig. 1 is a diagram for explaining the operating principle of a phase array type transducer, Fig. 2 is a block circuit diagram showing a device according to an embodiment of the present invention, and Fig. 3 is a diagram showing beam combination during wave transmission in the embodiment. The explanatory diagrams, FIG. 4 and FIG. 5, are diagrams for explaining beam synthesis during forward reception and backward reception in this embodiment, respectively. Explanation of symbols 1... Transducer/receiver, 2 1 - 2 o ... Element, 3, 4... Phase inverter, 5, 6... Transmitter/receiver switch, 7... Transmitter, 8... Phase advancer, 9... Phase delay device, 10, 11... Adder.

Claims (1)

【特許請求の範囲】[Claims] 1 単一のフエーズアレー型送受波器によつて、
送波時には少くとも前後の相対する方向に実質的
に等しい俯角を有する2つの超音波ビームを合成
して、該合成ビームを前記相対する方向に同時に
発射する装置と、一方受波時には前記相対する方
向のそれぞれにつきビーム合成を行い、もつて前
記相対する方向のうちのどちらか所望の方向につ
いての信号を受信する装置とを具備したことを特
徴とするドプラ効果を利用した速度測定装置にお
ける送受波装置。
1 By a single phase array type transducer,
a device that combines two ultrasonic beams having substantially equal depression angles in at least front and rear opposite directions when transmitting waves, and simultaneously emits the combined beams in the opposite directions; A wave transmitting/receiving device in a speed measuring device using the Doppler effect, comprising a device that performs beam synthesis in each direction and receives a signal in one of the desired directions among the opposing directions. Device.
JP13906581A 1981-09-03 1981-09-03 Transmitting and receiving device of speed measuring instrument Granted JPS5839970A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP13906581A JPS5839970A (en) 1981-09-03 1981-09-03 Transmitting and receiving device of speed measuring instrument

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP13906581A JPS5839970A (en) 1981-09-03 1981-09-03 Transmitting and receiving device of speed measuring instrument

Publications (2)

Publication Number Publication Date
JPS5839970A JPS5839970A (en) 1983-03-08
JPS6348319B2 true JPS6348319B2 (en) 1988-09-28

Family

ID=15236671

Family Applications (1)

Application Number Title Priority Date Filing Date
JP13906581A Granted JPS5839970A (en) 1981-09-03 1981-09-03 Transmitting and receiving device of speed measuring instrument

Country Status (1)

Country Link
JP (1) JPS5839970A (en)

Cited By (4)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPH01321804A (en) * 1988-06-21 1989-12-27 Fujikura Ltd How to pass the column of an overhead cable inspection device and the section where the column passes
JPH0236708A (en) * 1988-07-26 1990-02-06 Furukawa Electric Co Ltd:The Steel tower clearing rail for transmission line self-traveling machine
JPH0236706A (en) * 1988-07-26 1990-02-06 Furukawa Electric Co Ltd:The Steel tower clearing method and device for transmission line self-traveling machine
JPH02250609A (en) * 1989-03-23 1990-10-08 Furukawa Electric Co Ltd:The Method of overriding iron tower for transmission line self-traveling vehicle and device therefor

Families Citing this family (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS61246687A (en) * 1985-04-24 1986-11-01 Japan Radio Co Ltd Speed measuring apparatus

Family Cites Families (5)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US3441904A (en) * 1967-12-15 1969-04-29 Us Navy Electro-mechanical directional transducer
JPS50156817A (en) * 1974-06-07 1975-12-18
US3985063A (en) * 1974-08-30 1976-10-12 Borg-Warner Corporation Hydraulic control system
JPS5823595B2 (en) * 1975-07-04 1983-05-16 沖電気工業株式会社 Ultrasonic image display device
JPS5229625A (en) * 1975-09-01 1977-03-05 Kubota Ltd Construction for pipe joint

Cited By (4)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPH01321804A (en) * 1988-06-21 1989-12-27 Fujikura Ltd How to pass the column of an overhead cable inspection device and the section where the column passes
JPH0236708A (en) * 1988-07-26 1990-02-06 Furukawa Electric Co Ltd:The Steel tower clearing rail for transmission line self-traveling machine
JPH0236706A (en) * 1988-07-26 1990-02-06 Furukawa Electric Co Ltd:The Steel tower clearing method and device for transmission line self-traveling machine
JPH02250609A (en) * 1989-03-23 1990-10-08 Furukawa Electric Co Ltd:The Method of overriding iron tower for transmission line self-traveling vehicle and device therefor

Also Published As

Publication number Publication date
JPS5839970A (en) 1983-03-08

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