JPH0160773B2 - - Google Patents

Info

Publication number
JPH0160773B2
JPH0160773B2 JP10008183A JP10008183A JPH0160773B2 JP H0160773 B2 JPH0160773 B2 JP H0160773B2 JP 10008183 A JP10008183 A JP 10008183A JP 10008183 A JP10008183 A JP 10008183A JP H0160773 B2 JPH0160773 B2 JP H0160773B2
Authority
JP
Japan
Prior art keywords
point
water temperature
ultrasonic
directivity angle
sharp
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
JP10008183A
Other languages
Japanese (ja)
Other versions
JPS59224532A (en
Inventor
Kyomi Minohara
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.)
Furuno Electric Co Ltd
Original Assignee
Furuno Electric 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 Furuno Electric Co Ltd filed Critical Furuno Electric Co Ltd
Priority to JP10008183A priority Critical patent/JPS59224532A/en
Publication of JPS59224532A publication Critical patent/JPS59224532A/en
Publication of JPH0160773B2 publication Critical patent/JPH0160773B2/ja
Granted legal-status Critical Current

Links

Classifications

    • GPHYSICS
    • G01MEASURING; TESTING
    • G01KMEASURING TEMPERATURE; MEASURING QUANTITY OF HEAT; THERMALLY-SENSITIVE ELEMENTS NOT OTHERWISE PROVIDED FOR
    • G01K11/00Measuring temperature based upon physical or chemical changes not covered by groups G01K3/00, G01K5/00, G01K7/00 or G01K9/00
    • G01K11/22Measuring temperature based upon physical or chemical changes not covered by groups G01K3/00, G01K5/00, G01K7/00 or G01K9/00 using measurement of acoustic effects

Landscapes

  • Physics & Mathematics (AREA)
  • Acoustics & Sound (AREA)
  • General Physics & Mathematics (AREA)
  • Measuring Temperature Or Quantity Of Heat (AREA)

Description

【発明の詳細な説明】 (発明の技術分野) この発明は水中に超音波を送波して水中で乱反
射される超音波を受波したとき、超音波の送波か
ら受波までの時間が水温に応じて変化することに
基づいて水温を測定する方法において、超音波の
送波、受波を円滑に行わせることに関する。
[Detailed Description of the Invention] (Technical Field of the Invention) This invention provides that when an ultrasonic wave is transmitted underwater and the ultrasonic wave that is diffusely reflected in the water is received, the time from the sending of the ultrasonic wave to the reception of the ultrasonic wave is The present invention relates to smooth transmission and reception of ultrasonic waves in a method of measuring water temperature based on changes in water temperature.

(発明の目的) 第1図において、P点からθ1方向に超音波を送
波し、Q点においてθ2方向に指向性を有する受波
器で受波を行うと、θ1とθ2の交点Rで乱反射され
る超音波を受波することができる。このとき、P
点から送波された超音波がR点で反射されQ点に
到達するまでの時間は、超音波の伝搬速度によつ
て決まり、伝搬速度は伝播路PRQの水温によつ
て影響される。従つて、P点から送波された音波
がR点で反射されてQ点に到達するまでの時間、
PQ間の距離と角θ1、θ2とによつて算出される伝
搬路PRQの伝搬距離に基づいて伝播路PRQにお
ける音波の伝搬速度が求められる。従つて、その
伝搬速度から伝搬路PRQに水温を知ることがで
きる。
(Object of the invention) In FIG. 1, when an ultrasonic wave is transmitted from point P in the θ 1 direction and received at point Q by a receiver having directivity in the θ 2 direction, θ 1 and θ 2 It is possible to receive the ultrasonic waves that are diffusely reflected at the intersection point R. At this time, P
The time it takes for the ultrasonic wave transmitted from a point to be reflected at point R and reach point Q is determined by the propagation speed of the ultrasonic wave, and the propagation speed is influenced by the water temperature in the propagation path PRQ. Therefore, the time it takes for a sound wave transmitted from point P to be reflected at point R and reach point Q,
The propagation speed of the sound wave in the propagation path PRQ is determined based on the propagation distance of the propagation path PRQ calculated from the distance between PQ and the angles θ 1 and θ 2 . Therefore, the water temperature in the propagation path PRQ can be determined from the propagation speed.

上記において、PRQの伝搬距離はPQ間距離と
角θ1、θ2とによつて算出されるから、P点の送波
ビームの指向方向及びQ点の受波ビームの指向方
向は正確にθ1、θ2に一致していなければならな
い。そして、送波ビーム及び受波ビームは各々の
指向角X1、X2を極力鋭くしなければR点からの
反射波を正確に受波することができない。そのた
め、送波ビーム並びに受波ビームはペンシル状の
鋭い指向角のビームがR点で交又するように配置
しなければならない。
In the above, since the propagation distance of PRQ is calculated by the distance between PQ and the angles θ 1 and θ 2 , the directivity direction of the transmitting beam at point P and the directivity direction of the receiving beam at point Q are exactly θ 1 and θ 2 . Unless the directivity angles X 1 and X 2 of the transmitted beam and the received beam are made as sharp as possible, the reflected wave from point R cannot be accurately received. Therefore, the transmitting beam and the receiving beam must be arranged so that the pencil-shaped beams with sharp directivity angles intersect at point R.

ところが、このようなビームを配置する場合、
水平面上の方位を非常に正確に一致させなければ
ならず、水平方位がわずかにずれても送波ビーム
と受波ビームをR点で交又させることができな
い。
However, when arranging such a beam,
The directions on the horizontal plane must be matched very precisely, and even if the horizontal directions are slightly shifted, the transmitting beam and the receiving beam cannot intersect at point R.

この発明は、送波ビームあるいは受波ビームの
ビーム形状を工夫することにより、超音波信号の
送受波を円滑に行わせることを目的とする。
An object of the present invention is to smoothly transmit and receive ultrasonic signals by devising the beam shape of a transmitting beam or a receiving beam.

(発明の実施例) 第2図において、超音波送波器Z1はP点からθ1
方向に超音波信号を送波する。この送波ビーム
B1はペンシル状の鋭い指向角に設定されている。
(Embodiment of the invention) In FIG. 2, the ultrasonic transmitter Z 1 is θ 1 from the point P.
The ultrasonic signal is transmitted in the direction. This transmitting beam
B 1 has a sharp, pencil-like beam angle.

一方、Q点には超音波受波器Z2が設置され、第
1図と同様にしてR点からの反射波を受波する。
この受波ビームB2はθ2方向に向けて設置される。
そして、その指向角は鉛直方向に鋭く水平方向に
若干広くなるように形成されている。
On the other hand, an ultrasonic receiver Z2 is installed at point Q, and receives the reflected wave from point R in the same manner as in FIG.
This received beam B 2 is installed toward the θ 2 direction.
The directivity angle is sharp in the vertical direction and slightly wide in the horizontal direction.

このように送波ビームB1、受波ビームB2を配
置すると、送波ビームB1はその水平方位が受波
ビームB2の水平方向の指向角β内に収まるよう
に設置するだけでR点からの反射波を容易に受波
することができる。
When transmitting beam B 1 and receiving beam B 2 are arranged in this way, transmitting beam B 1 only needs to be installed so that its horizontal direction falls within the horizontal directivity angle β of receiving beam B 2 . Reflected waves from a point can be easily received.

反射点Rは、受波ビームB2の鉛直方向の指向
角αが鋭角に設定されているから、送波ビーム
B1の水平方位を受波ビームB2の水平指向角β内
で変化させても、水平方向に若干変化するだけで
深度方向には変化しない。
Since the vertical directivity angle α of the receiving beam B 2 is set to an acute angle, the reflection point R is located at the transmitting beam.
Even if the horizontal azimuth of B 1 is changed within the horizontal directivity angle β of the received beam B 2 , it only changes slightly in the horizontal direction and does not change in the depth direction.

一般に、水温は深度方向に対して変化する傾向
が強いから、測定点が水平方向に若干変化しても
測定誤差はほとんど生じない。又、受波ビーム
B2の水平方向の広がりに比してPQ間距離は十分
に大きいから、反射点Rが水平方向に若干変化し
ても伝播距離PRQに与える距離変化はほとんど
無視し得る程度に小さい。従つて、PQ間距離と
ビームB1、B2の指向方向θ1、θ2とによつて超音
波の伝播路PRQを正確に算出することができる。
In general, water temperature has a strong tendency to change in the depth direction, so even if the measurement point changes slightly in the horizontal direction, almost no measurement error occurs. Also, the receiving beam
Since the distance between PQ is sufficiently large compared to the horizontal spread of B2 , even if the reflection point R changes slightly in the horizontal direction, the change in distance given to the propagation distance PRQ is so small that it can be almost ignored. Therefore, the ultrasonic propagation path PRQ can be accurately calculated based on the distance between PQ and the directivity directions θ 1 and θ 2 of the beams B 1 and B 2 .

(発明の効果) 受波ビームの水平方向の指向角を若干広くする
ことにより送波ビームと受波ビームの交又を容易
に行わせることができる。
(Effects of the Invention) By slightly widening the horizontal directivity angle of the receiving beam, it is possible to easily cause the transmitting beam and the receiving beam to intersect.

(発明の他の実施例) 第2図における送波ビームB1と受波ビームB2
は逆にしてもよい。すなわち、送波ビームの水平
方向の指向角を若干広くして、受波ビームをペン
シル状の鋭い指向特性にしてもよい。
(Other embodiments of the invention) Transmitting beam B 1 and receiving beam B 2 in FIG.
may be reversed. In other words, the horizontal directivity angle of the transmitted beam may be slightly widened to give the received beam a sharp, pencil-like directivity characteristic.

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

第1図は水温測定の原理を説明する図、第2図
はこの発明の実施例を示す。
FIG. 1 is a diagram explaining the principle of water temperature measurement, and FIG. 2 shows an embodiment of the present invention.

Claims (1)

【特許請求の範囲】 1 第1の地点から水中に送波した超音波が水中
で乱反射され、該乱反射された反射波を第2の地
点で受波したとき、上記超音波の送波から該受波
までの時間が水温によつて変化することに基づい
て水温を測定する方法において、 上記第1の地点から超音波を送波する送波ビー
ムあるいは第2の地点で超音波を受波する受波ビ
ームのいずれか一方をペンシル状の鋭い指向角を
有するビームを用い、他方を鉛直方向の指向角が
鋭く水平方向の指向角が若干広い指向特性のビー
ムを用いることを特徴とする水温測定に用いる超
音波ビームの送受波方法。
[Claims] 1. When an ultrasonic wave transmitted into the water from a first point is diffusely reflected in the water and the diffusely reflected reflected wave is received at a second point, the In a method of measuring water temperature based on the fact that the time until wave reception changes depending on the water temperature, a transmission beam that transmits ultrasonic waves from the first point or receives the ultrasonic waves at a second point is used. Water temperature measurement characterized by using one of the receiving beams as a beam with a pencil-like sharp directivity angle, and the other as a beam with a sharp vertical directivity angle and a slightly wide horizontal directivity angle. A method of transmitting and receiving ultrasonic beams used in
JP10008183A 1983-06-03 1983-06-03 Transmitting and receiving method of ultrasonic wave beam used for measurement of water temperature Granted JPS59224532A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP10008183A JPS59224532A (en) 1983-06-03 1983-06-03 Transmitting and receiving method of ultrasonic wave beam used for measurement of water temperature

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP10008183A JPS59224532A (en) 1983-06-03 1983-06-03 Transmitting and receiving method of ultrasonic wave beam used for measurement of water temperature

Publications (2)

Publication Number Publication Date
JPS59224532A JPS59224532A (en) 1984-12-17
JPH0160773B2 true JPH0160773B2 (en) 1989-12-25

Family

ID=14264488

Family Applications (1)

Application Number Title Priority Date Filing Date
JP10008183A Granted JPS59224532A (en) 1983-06-03 1983-06-03 Transmitting and receiving method of ultrasonic wave beam used for measurement of water temperature

Country Status (1)

Country Link
JP (1) JPS59224532A (en)

Also Published As

Publication number Publication date
JPS59224532A (en) 1984-12-17

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