Deprecated: The each() function is deprecated. This message will be suppressed on further calls in /home/zhenxiangba/zhenxiangba.com/public_html/phproxy-improved-master/index.php on line 456
JPH0123755B2 - - Google Patents
[go: Go Back, main page]

JPH0123755B2 - - Google Patents

Info

Publication number
JPH0123755B2
JPH0123755B2 JP2258583A JP2258583A JPH0123755B2 JP H0123755 B2 JPH0123755 B2 JP H0123755B2 JP 2258583 A JP2258583 A JP 2258583A JP 2258583 A JP2258583 A JP 2258583A JP H0123755 B2 JPH0123755 B2 JP H0123755B2
Authority
JP
Japan
Prior art keywords
frequency
signal
ultrasonic
transducer
sludge
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
JP2258583A
Other languages
Japanese (ja)
Other versions
JPS59147257A (en
Inventor
Hideyuki Takahashi
Yozo Matsuda
Hiroshi Kamata
Hisami Hayakawa
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.)
Oki Electric Industry Co Ltd
Original Assignee
Oki Electric Industry 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 Oki Electric Industry Co Ltd filed Critical Oki Electric Industry Co Ltd
Priority to JP2258583A priority Critical patent/JPS59147257A/en
Publication of JPS59147257A publication Critical patent/JPS59147257A/en
Publication of JPH0123755B2 publication Critical patent/JPH0123755B2/ja
Granted legal-status Critical Current

Links

Classifications

    • GPHYSICS
    • G01MEASURING; TESTING
    • G01NINVESTIGATING OR ANALYSING MATERIALS BY DETERMINING THEIR CHEMICAL OR PHYSICAL PROPERTIES
    • G01N29/00Investigating or analysing materials by the use of ultrasonic, sonic or infrasonic waves; Visualisation of the interior of objects by transmitting ultrasonic or sonic waves through the object
    • G01N29/02Analysing fluids
    • G01N29/024Analysing fluids by measuring propagation velocity or propagation time of acoustic waves

Landscapes

  • Physics & Mathematics (AREA)
  • Acoustics & Sound (AREA)
  • Health & Medical Sciences (AREA)
  • Life Sciences & Earth Sciences (AREA)
  • Chemical & Material Sciences (AREA)
  • Analytical Chemistry (AREA)
  • Biochemistry (AREA)
  • General Health & Medical Sciences (AREA)
  • General Physics & Mathematics (AREA)
  • Immunology (AREA)
  • Pathology (AREA)
  • Measurement Of Velocity Or Position Using Acoustic Or Ultrasonic Waves (AREA)

Description

【発明の詳細な説明】 (技術分野) 本発明はヘドロ層表面と水底面の深さやヘドロ
層の厚さを高精度に測定することのできるヘドロ
探査機に関するものである。
DETAILED DESCRIPTION OF THE INVENTION (Technical Field) The present invention relates to a sludge probe capable of measuring the depth of the sludge layer surface and water bottom surface and the thickness of the sludge layer with high precision.

(従来技術) 第1図は従来のヘドロ探査機を示すものであ
る。ここではまず、モータ1の駆動により記録ペ
ン2が記録紙3上の記録開始点に達し、同期パル
ス発生器4より同期パルスが送出されると、送信
タイミング回路5から送信器6及び7へ送信タイ
ミングパルスが出される。送信器6は該パルスを
受けて比較的低周波fLのパルス状信号を作成し、
また送信器7は比較的高周波fHのパルス状信号を
作成する。該低周波パルス状信号は送受切換器8
を介して送受波器10に送出され、ここで超音波
信号S1に変換され水中17に送出される。また
前記高周波パルス状信号は送受切換器9を介して
送受波器11に送出され、ここで超音波信号S2
に変換され水中17に送出される。
(Prior Art) Figure 1 shows a conventional sludge probe. First, when the recording pen 2 reaches the recording start point on the recording paper 3 by driving the motor 1 and a synchronization pulse is sent from the synchronization pulse generator 4, the transmission timing circuit 5 sends the synchronization pulse to the transmitters 6 and 7. A timing pulse is issued. The transmitter 6 receives the pulse and creates a pulse-like signal of relatively low frequency f L ,
The transmitter 7 also generates a pulsed signal of relatively high frequency fH . The low frequency pulsed signal is sent to the transmitter/receiver switch 8.
The ultrasonic signal is sent to the transducer 10 via the transducer 10, where it is converted into an ultrasonic signal S1 and sent into the water 17. Further, the high frequency pulsed signal is sent to the transducer 11 via the transmitter/receiver switch 9, where the ultrasonic signal S2
It is converted into water and sent into the water 17.

超音波信号S1は水中17を伝搬しヘドロ層1
8を通過し水底面19により反射され送受波器1
0にて再び受信され、また超音波信号S2はヘド
ロ層表面18aにより反射され送受波器11にて
再び受信されるが、伝搬距離の違いにより信号S
2の方がより早く受信される。受信された信号は
送受切換器8及び9を介して受信器12及び13
にそれぞれ送出され、ここで一定レベルまで増幅
され、更にフイルタ14及び15で超音波信号S
1及びS2の周波数成分のみが取出され記録増幅
器16に送出される。記録増幅器16はフイルタ
14及び15より送出される信号を所定レベルま
で増幅し放電破壊記録器の記録ペン2に印加し、
記録紙3上にヘドロ層表面18a、水底面19の
深さをそれぞれ記録する。
The ultrasonic signal S1 propagates through the water 17 and reaches the sludge layer 1.
8 and is reflected by the water bottom surface 19 to the transducer 1.
0, and the ultrasonic signal S2 is reflected by the sludge layer surface 18a and received again by the transducer 11, but due to the difference in propagation distance, the signal S2
2 is received faster. The received signals are sent to receivers 12 and 13 via transmitter/receiver switchers 8 and 9.
The ultrasonic signals S
Only the frequency components 1 and S2 are extracted and sent to the recording amplifier 16. The recording amplifier 16 amplifies the signals sent from the filters 14 and 15 to a predetermined level and applies it to the recording pen 2 of the discharge breakdown recorder.
The depths of the sludge layer surface 18a and the water bottom surface 19 are recorded on the recording paper 3, respectively.

上記装置においてヘドロ層表面18aと水底面
19の深さの差よりヘドロ層18の厚さを高精
度・高分解能に測定しようとする場合、低周波の
超音波信号S1の周波数fLを30KHz以下とし、か
つその指向特性を鋭いものとしなければならない
が、このような信号を得ようとすると送受波器1
0の形状が極めて大きくなり、従つて送受波器1
1との間に測定点のずれが生じることになり、結
局測定精度が悪くなつてしまう欠点があつた。
When using the above device to measure the thickness of the sludge layer 18 with high accuracy and high resolution from the difference in depth between the sludge layer surface 18a and the water bottom surface 19, the frequency f L of the low-frequency ultrasonic signal S1 must be set to 30 KHz or less. However, in order to obtain such a signal, the transducer 1
0 becomes extremely large, and therefore the transducer 1
This resulted in a deviation of the measurement point between the measurement point and the measurement point, which resulted in a disadvantage that the measurement accuracy deteriorated.

(発明の目的) 本発明は上記従来の欠点を除去し、ヘドロ層の
厚さを高精度・高分解能に測定することのできる
ヘドロ探査機を実現することを目的とするもので
ある。
(Object of the Invention) An object of the present invention is to eliminate the above-mentioned conventional drawbacks and to realize a sludge probe capable of measuring the thickness of a sludge layer with high precision and high resolution.

(発明の構成) 本発明は2周波の音波を同時に音場媒質に送波
した時、音場媒質の非線形特性によつて音波同士
が相互作用を起こし前記2周波の和と差の周波数
成分を発生し、この場合の差の周波数成分が極め
て鋭い指向性を有する音波となるというパラメト
リツク効果を利用して、前述した目的を達成しよ
うとするもので、その要旨とするところはヘドロ
層表面にて反射される比較的高い周波数fHの超音
波信号の伝搬時間よりヘドロ層表面の深さを測定
し、ヘドロ層を通過する比較的低い周波数fLの超
音波信号の伝搬時間より水底面の深さを測定する
ヘドロ探査機において、前記周波数fHの超音波の
発信信号を作成する第1の発振器と、前記周波数
fHに対して周波数fLだけ異なる周波数fhの超音波
の発信信号を作成する第2の発振器と、前記2つ
の発信信号を合成して一の送受波器に加える手段
と、該一の送受波器にて受信された信号中より周
波数fH又はfhあるいはfH及びfhの信号成分と周波
数fLの信号成分とをそれぞれ分離する手段とを備
え、前記周波数fH及びfhの2つの超音波信号を前
記送受波器より同時に発信するようにしたことを
特徴とするヘドロ探査機と、前記周波数fHの超音
波の発信信号を作成する発振器と、前記周波数fH
に対して周波数fLだけ異なる周波数fhを中心とし
た所定周波数範囲Δf内の任意の周波数fh′の超音
波の発信信号を作成する周波数可変発振器と、前
記2つの発信信号を合成して一の送受波器に加え
る手段と、該一の送受波器にて受信された信号中
より周波数fH又はfh′あるいはfH及びfh′の信号成
分と周波数(fH−fh′)の信号成分とをそれぞれ
分離する手段とを備え、前記周波数fH及びfh′の
2つの超音波信号を前記送受波器より同時に発信
するようにしたことを特徴とするヘドロ探査機に
ある。
(Structure of the Invention) According to the present invention, when sound waves of two frequencies are simultaneously transmitted to a sound field medium, the sound waves interact with each other due to the nonlinear characteristics of the sound field medium, and the frequency components of the sum and difference of the two frequencies are generated. The aim is to achieve the above-mentioned objective by utilizing the parametric effect in which the frequency component of the difference in this case becomes a sound wave with extremely sharp directivity. The depth of the sludge layer surface is measured from the propagation time of an ultrasonic signal with a relatively high frequency f In a sludge probe that measures depth, a first oscillator that creates an ultrasonic transmission signal of the frequency fH ;
a second oscillator for generating an ultrasonic transmission signal having a frequency f h that differs from f H by a frequency f L ; means for separating the signal components of the frequencies f H or f h or f H and f h from the signal components of the frequencies f L from the signals received by the transducer ; a sludge probe characterized in that two ultrasonic signals of the frequency f H are simultaneously emitted from the transducer; an oscillator that generates an ultrasonic signal of the frequency f H ;
a variable frequency oscillator that generates an ultrasonic transmission signal of an arbitrary frequency f h ' within a predetermined frequency range Δf centered on a frequency f h that differs from the frequency f L by a frequency f L ; a means for adding signals to one transducer, and signal components of frequency f H or f h ′ or f H and f h ′ and frequency (f H − f h ′) from the signal received by the one transducer; ), and two ultrasonic signals of the frequencies f H and f h ' are simultaneously emitted from the transducer. .

(実施例) 第2図は本発明の第1の実施例を示すもので、
図中第1図と同一構成部分は同一符号をもつて表
わす。即ち、1はモータ、2は記録ペン、3は記
録紙、4は同期パルス発生器、5は送信タイミン
グ回路、8は送受切換器、11は超音波の送受波
器、12は受信器、14,15はフイルタ、16
は記録増幅器、17は水中、18はヘドロ層、1
8aはヘドロ層表面、19は水底面、20,21
は発振器、22は合成回路、23は送信器、2
4,25は増幅器である。
(Example) FIG. 2 shows a first example of the present invention.
Components in the figure that are the same as those in FIG. 1 are denoted by the same reference numerals. That is, 1 is a motor, 2 is a recording pen, 3 is a recording paper, 4 is a synchronous pulse generator, 5 is a transmission timing circuit, 8 is a transmitter/receiver switch, 11 is an ultrasonic transducer, 12 is a receiver, and 14 , 15 is a filter, 16
is a recording amplifier, 17 is underwater, 18 is a sludge layer, 1
8a is the sludge layer surface, 19 is the water bottom surface, 20, 21
is an oscillator, 22 is a synthesis circuit, 23 is a transmitter, 2
4 and 25 are amplifiers.

発振器20はヘドロ層表面18aで反射される
比較的高い周波数fH(例えば100KHz)のパルス状
信号P1を発生し、また発振器21は周波数fH
対してヘドロ層18を通過し得る信号の周波数fL
(例えば10KHz)分だけ異なる周波数fh(例えば
90KHz)のパルス状信号P2を発生する如くなつ
ている。フイルタ14は周波数fHの信号成分を取
出し、またフイルタ15は周波数fHとfhとの差の
周波数fLの信号成分を取出す如くなつている。な
お、信号P2もヘドロ層表面18aで反射される
からフイルタ14の特性は周波数fhの信号成分を
取出す如くなしてもよく、更に周波数fHとfhの両
方の信号成分を取出す如くなしてもよい。また前
記合成回路22、送信器23及び送受切換器8は
信号P1とP2を合成して一の送受波器11に加
える手段を構成し、また、送受切換器8、受信器
12、フイルタ14及び15は一の送受波器11
にて受信された信号中より周波数fH又はfhあるい
はfH及びfhの信号成分と周波数fLの信号成分とを
それぞれ分離する手段を構成する。
The oscillator 20 generates a pulsed signal P1 of a relatively high frequency f H (for example, 100 KHz) that is reflected by the sludge layer surface 18a, and the oscillator 21 generates a pulsed signal P1 having a relatively high frequency f H (for example, 100 KHz), which is reflected at the sludge layer surface 18a, and the oscillator 21 generates a signal P1 that can pass through the sludge layer 18 with respect to the frequency f H. f L
(e.g. 10KHz) different frequency f h (e.g.
It is designed to generate a pulse-like signal P2 of 90KHz). Filter 14 extracts a signal component of frequency f H , and filter 15 extracts a signal component of frequency f L , which is the difference between frequencies f H and f h . Incidentally, since the signal P2 is also reflected by the sludge layer surface 18a, the characteristics of the filter 14 may be such that it extracts the signal component of the frequency f h , or further, that it extracts the signal component of both the frequencies f H and f h . Good too. Further, the combining circuit 22, the transmitter 23, and the transmitter/receiver 8 constitute means for combining the signals P1 and P2 and add them to one transmitter/receiver 11. 15 is one transducer 11
means for separating the signal component of the frequency f H or f h or f H and f h from the signal component of the frequency f L from the signal received at the.

次に動作について説明する。モータ1の駆動に
より記録ペン2が記録紙3上の記録開始点に達
し、同期パルス発生器4より同期パルスが送出さ
れると、送信タイミング回路5から発信器20及
び21へ送信タイミングパルスが送出される。該
パルスを受けて発振器20はパルス状信号(発信
信号)P1を、また発振器21はパルス状信号
(発信信号)P2を作成し、それぞれ合成回路2
2へ送出する。該信号P1及びP2は合成回路2
2で加算・合成され、送信器23で所定レベルま
で増幅され、送受切換器8を通して送受波器11
に送出される。送受波器11は該信号P1,P2
を受けて周波数fHのパルス状の超音波信号SO1
と周波数fhのパルス状の超音波信号SO2を同時
に発信する。
Next, the operation will be explained. When the recording pen 2 reaches the recording start point on the recording paper 3 by driving the motor 1 and a synchronization pulse is sent from the synchronization pulse generator 4, a transmission timing pulse is sent from the transmission timing circuit 5 to the transmitters 20 and 21. be done. In response to the pulse, the oscillator 20 generates a pulse-like signal (transmission signal) P1, and the oscillator 21 generates a pulse-form signal (transmission signal) P2, which are sent to the synthesis circuit 2.
Send to 2. The signals P1 and P2 are sent to the combining circuit 2.
2, and is amplified to a predetermined level by the transmitter 23.
will be sent to. The transducer 11 receives the signals P1 and P2.
A pulsed ultrasonic signal SO1 with a frequency f H
and a pulsed ultrasonic signal SO2 of frequency f h are simultaneously transmitted.

前記2つの周波数の異なる超音波信号SO1,
SO2が音場媒質中、即ち水中17を伝搬すると、
該音場媒質の非線形性によつて超音波信号同士が
相互作用して2つの信号の周波数の和と差の周波
数を有する超音波信号が発生する。この時の差の
周波数fL(=fH−fh)を有する超音波信号SO3は
鋭い指向性を有する。
the two ultrasonic signals SO1 having different frequencies;
When SO2 propagates in the sound field medium, that is, in water 17,
Due to the nonlinearity of the sound field medium, the ultrasonic signals interact with each other, and an ultrasonic signal having a frequency that is the sum and difference of the frequencies of the two signals is generated. At this time, the ultrasonic signal SO3 having the difference frequency f L (=f H - f h ) has sharp directivity.

超音波信号SO1,SO2は水中17を伝搬し、
ヘドロ層表面18aにより反射され送受波器11
にて受信されるが、超音波信号SO3はヘドロ層
18を通過し、水底面19により反射され同じく
送受波器11に受信される。これらの信号は送受
切換器8を介して受信器12に送られ、ここで一
定レベルまで増幅された後、フイルタ14及び1
5に送出される。フイルタ14では周波数fHの成
分、即ち超音波信号SO1の受信信号が抽出され、
またフイルタ15では周波数fLの成分、即ち超音
波信号SO3の受信信号が抽出され、これらはそ
れぞれ増幅器24及び25にて所定レベルまで増
幅される。ただし、超音波信号SO3が形成され
る能率は低能率であり、また送受波器11の周波
数特性を補正するために増幅器24と25は異な
つた増幅度に設定される。記録増幅器16は増幅
器24及び25でほぼ同じレベルまで増幅された
受信信号を更に記録に必要なレベルまで増幅し、
記録ペン2に印加し記録紙3上にヘドロ層表面1
8a、水底面19の深さを記録する。而して、こ
の記録結果よりヘドロ層表面18aの深さと水底
面19の深さとの差を読取ることによつてヘドロ
層18の厚さを測定することができる。
The ultrasonic signals SO1 and SO2 propagate through the water 17,
The transducer 11 is reflected by the sludge layer surface 18a.
However, the ultrasonic signal SO3 passes through the sludge layer 18, is reflected by the water bottom surface 19, and is also received by the transducer 11. These signals are sent to the receiver 12 via the transmitter/receiver switch 8, where they are amplified to a certain level and then passed through the filters 14 and 1.
Sent on 5th. The filter 14 extracts the frequency f H component, that is, the received signal of the ultrasonic signal SO1,
Further, the filter 15 extracts the frequency f L component, that is, the received signal of the ultrasonic signal SO3, and these are amplified to a predetermined level by amplifiers 24 and 25, respectively. However, the efficiency with which the ultrasonic signal SO3 is formed is low, and in order to correct the frequency characteristics of the transducer 11, the amplifiers 24 and 25 are set to different amplification degrees. The recording amplifier 16 further amplifies the received signal, which has been amplified to almost the same level by the amplifiers 24 and 25, to a level necessary for recording.
A voltage is applied to the recording pen 2 to form a sludge layer surface 1 on the recording paper 3.
8a, record the depth of the water bottom surface 19. The thickness of the sludge layer 18 can be measured by reading the difference between the depth of the sludge layer surface 18a and the depth of the water bottom surface 19 from this recorded result.

このように上記実施例によれば、比較的高い周
波数の2つの超音波信号を同時に発信し、パラメ
トリツク効果により前記2つの信号の周波数の差
に相当する比較的低い周波数で、かつ指向性の鋭
い超音波信号を発生させ、ヘドロ層表面と水底面
の深さを測定するようになしたため、低い周波数
の超音波信号を発生する送受波器を必要とせず、
高い周波数の信号と低い周波数の信号との測定点
のずれをなくすことができ、従つて同一地点のヘ
ドロ層表面の深さと水底面の深さを記録紙上の同
一軸上に記録することができ、高精度なヘドロ層
の厚さの測定ができる。
In this way, according to the above embodiment, two ultrasonic signals with relatively high frequencies are simultaneously transmitted, and due to the parametric effect, ultrasonic signals are transmitted at a relatively low frequency corresponding to the frequency difference between the two signals, and with directivity. Because it generates sharp ultrasonic signals and measures the depth of the sludge layer surface and water bottom, there is no need for a transducer that generates low frequency ultrasonic signals.
It is possible to eliminate the deviation in measurement points between high frequency signals and low frequency signals, and therefore the depth of the sludge layer surface and the depth of the water bottom at the same point can be recorded on the same axis on the recording paper. , it is possible to measure the thickness of the sludge layer with high precision.

なお、周波数fHとfhの和と差の周波数成分は水
中以外にも送信器23の非直線性によつて生ずる
ことがあるので、この点充分注意して予め抑圧し
ておく必要がある。
Note that the frequency components of the sum and difference between frequencies f H and f h may be generated not only underwater but also due to the nonlinearity of the transmitter 23, so it is necessary to pay sufficient attention to this point and suppress them in advance. .

第3図は本発明の第2の実施例を示すもので、
ここでは比較的高い周波数の超音波信号のうちの
一つの周波数を可変となしている。即ち、図中2
6は周波数可変発振器、27は周波数可変フイル
タであつて、周波数可変発振器26は前記周波数
fhを中心とした所定の周波数範囲Δf内で任意の周
波数fh′の発信信号を作成し得る如くなつており、
周波数可変フイルタ27は周波数可変発振器26
の発振周波数に合わせて周波数fL′(=fH−fh′)
の信号を取出し得る如く構成されている。このよ
うな構成によればヘドロ層の堆積状態や水底の土
質等によつて超音波信号SO3の周波数を選択す
ることができ、より広範囲なヘドロ層に対して高
精度な探査が可能となる。なお、前記合成回路2
2、送信器23及び送受切換器8は周波数fHの発
信信号と周波数fhを中心とした所定の周波数範囲
Δf内で任意の周波数fh′の発信信号を合成して一
の送受波器11に加える手段を構成し、また、送
受切換器8、受信器12、フイルタ14及び周波
数可変フイルタ27は一の送受波器11にて受信
された信号中より周波数fH又はfh′あるいはfH及び
fh′の信号成分と周波数(fH−fh′)の信号成分と
をそれぞれ分離する手段を構成する。また、その
他の構成、効果は第1の実施例と同様である。
FIG. 3 shows a second embodiment of the present invention,
Here, the frequency of one of the relatively high frequency ultrasonic signals is made variable. In other words, 2 in the figure
6 is a variable frequency oscillator, 27 is a variable frequency filter, and the variable frequency oscillator 26 is a variable frequency oscillator.
It is now possible to create a transmission signal of any frequency f h ' within a predetermined frequency range Δf centered on f h ,
The variable frequency filter 27 is the variable frequency oscillator 26
The frequency f L ′ (= f H − f h ′) according to the oscillation frequency of
It is constructed so that the signal can be extracted. According to such a configuration, the frequency of the ultrasonic signal SO3 can be selected depending on the deposition state of the sludge layer, the soil quality of the water bottom, etc., and it becomes possible to probe a wider range of the sludge layer with high precision. Note that the synthesis circuit 2
2. The transmitter 23 and the transmitter/receiver switch 8 combine the transmitting signal of the frequency f H and the transmitting signal of an arbitrary frequency f h ' within a predetermined frequency range Δf centered on the frequency f h to form one transmitter/receiver. The transmitter/receiver switch 8, the receiver 12, the filter 14, and the variable frequency filter 27 select the frequency f H or f h ′ or f from the signal received by the transducer 11. H and
A means is configured to separate the signal component of f h ′ and the signal component of frequency (f H −f h ′), respectively. Further, the other configurations and effects are similar to those of the first embodiment.

(発明の効果) 以上説明したように本発明によれば、ヘドロ層
表面にて反射される比較的高い周波数fHの超音波
信号の伝搬時間よりヘドロ層表面の深さを測定
し、ヘドロ層を通過する比較的低い周波数fLの超
音波信号の伝搬時間より水底面の深さを測定する
ヘドロ探査機において、前記周波数fHの超音波の
発信信号を作成する第1の発振器と、前記周波数
fHに対して周波数fLだけ異なる周波数fhの超音波
の発信信号を作成する第2の発振器と、前記2つ
の発信信号を合成して一の送受波器に加える手段
と、該一の送受波器にて受信された信号中より周
波数fH又はfhあるいはfH及びfhの信号成分と周波
数fLの信号成分とをそれぞれ分離する手段とを備
え、前記周波数fH及びfhの2つの超音波信号を前
記送受波器より同時に発信するようにしたので、
パラメトリツク効果により該2つの信号の周波数
の差に相当する比較的低い周波数で、かつ指向性
の鋭い超音波信号を発生させることができ、低い
周波数の超音波信号を発生するための大型の送受
波器を必要とせず装置の小型化がなし得るととも
に、高い周波数と低い周波数の超音波信号の発信
点のずれをなくすことができ、前記超音波信号の
指向性の鋭さと相俟つて同一地点のヘドロ層表面
の深さと水底面の深さを記録紙上の同一軸上に記
録することができ、高精度かつ高分解能なヘドロ
層の厚さの測定がなし得る。また周波数fHの超音
波の発信信号を作成する発振器と、前記周波数fH
に対して周波数fLだけ異なる周波数fhを中心とし
た所定周波数範囲Δf内の任意の周波数fh′の超音
波の発信信号を作成する周波数可変発振器と、前
記2つの発信信号を合成して一の送受波器に加え
る手段と、該一の送受波器にて受信された信号中
より周波数fH又はfh′あるいはfH及びfh′の信号成
分と周波数(fH−fh′)の信号成分とをそれぞれ
分離する手段とを備え、前記周波数fH及びfh′の
2つの超音波信号を前記送受波器より同時に発信
するようにしたものによれば前述の効果を有する
ことは勿論のこと、低い周波数の超音波信号の周
波数を任意に変えることができ、ヘドロ層や水底
の状態に応じた高精度な測定がなし得る等の利点
がある。
(Effects of the Invention) As explained above, according to the present invention, the depth of the sludge layer surface is measured from the propagation time of the ultrasonic signal of relatively high frequency f H reflected on the sludge layer surface, and the sludge layer surface depth is measured. In a sludge probe that measures the depth of the water bottom surface based on the propagation time of an ultrasonic signal with a relatively low frequency f L passing through the sludge probe, a first oscillator that generates an ultrasonic transmission signal with a frequency f H ; frequency
a second oscillator for generating an ultrasonic transmission signal having a frequency f h that differs from f H by a frequency f L ; means for separating the signal components of the frequencies f H or f h or f H and f h from the signal components of the frequencies f L from the signals received by the transducer ; Since the two ultrasonic signals are simultaneously transmitted from the transducer,
Due to the parametric effect, it is possible to generate ultrasonic signals with a relatively low frequency corresponding to the frequency difference between the two signals and with sharp directivity. The device can be miniaturized without the need for a transducer, and it is also possible to eliminate the shift in the transmission points of high and low frequency ultrasonic signals. The depth of the surface of the sludge layer and the depth of the bottom surface of the water can be recorded on the same axis on recording paper, making it possible to measure the thickness of the sludge layer with high precision and high resolution. Further, an oscillator for creating an ultrasonic transmission signal of frequency f H , and an oscillator for generating an ultrasonic transmission signal of frequency f H
a variable frequency oscillator that generates an ultrasonic transmission signal of an arbitrary frequency f h ' within a predetermined frequency range Δf centered on a frequency f h that differs from the frequency f L by a frequency f L ; a means for adding signals to one transducer, and signal components of frequency f H or f h ′ or f H and f h ′ and frequency (f H − f h ′) from the signal received by the one transducer; ), and the two ultrasonic signals of the frequencies f H and f h ' are simultaneously emitted from the transducer, the above-mentioned effects can be achieved. Of course, there are advantages in that the frequency of the low-frequency ultrasonic signal can be changed arbitrarily, and highly accurate measurements can be made depending on the state of the sludge layer and the bottom of the water.

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

図面は本発明の説明に供するもので、第1図は
従来のヘドロ探査機を示すブロツク図、第2図は
本発明のヘドロ探査機の第1の実施例を示すブロ
ツク図、第3図は本発明の第2の実施例を示すブ
ロツク図である。 1……モータ、2……記録ペン、3……記録
紙、4……同期パルス発生器、5……送信タイミ
ング回路、8……送受切換器、11……送受波
器、12……受信器、14,15……フイルタ、
16……記録増幅器、17……水中、18……ヘ
ドロ層、18a……ヘドロ層表面、19……水底
面、20,21……発振器、22……合成回路、
23……送信器、24,25……増幅器、26…
…周波数可変発振器、27……周波数可変フイル
タ。
The drawings serve to explain the present invention; FIG. 1 is a block diagram showing a conventional sludge probe, FIG. 2 is a block diagram showing a first embodiment of the sludge probe of the present invention, and FIG. FIG. 3 is a block diagram showing a second embodiment of the present invention. 1... Motor, 2... Recording pen, 3... Recording paper, 4... Synchronous pulse generator, 5... Transmission timing circuit, 8... Transmission/reception switch, 11... Transducer/receiver, 12... Reception vessel, 14, 15...filter,
16... Recording amplifier, 17... Underwater, 18... Sludge layer, 18a... Sludge layer surface, 19... Water bottom surface, 20, 21... Oscillator, 22... Synthesis circuit,
23... Transmitter, 24, 25... Amplifier, 26...
...Variable frequency oscillator, 27...Variable frequency filter.

Claims (1)

【特許請求の範囲】 1 ヘドロ層表面にて反射される比較的高い周波
数fHの超音波信号の伝搬時間よりヘドロ層表面の
深さを測定し、ヘドロ層を通過する比較的低い周
波数fLの超音波信号の伝搬時間より水底面の深さ
を測定するヘドロ探査機において、前記周波数fH
の超音波の発信信号を作成する第1の発振器と、
前記周波数fHに対して周波数fLだけ異なる周波数
fhの超音波の発信信号を作成する第2の発振器
と、前記2つの発信信号を合成して一の送受波器
に加える手段と、該一の送受波器にて受信された
信号中より周波数fH又はfhあるいはfH及びfhの信
号成分と周波数fLの信号成分とをそれぞれ分離す
る手段とを備え、前記周波数fH及びfhの2つの超
音波信号を前記送受波器より同時に発信するよう
にしたことを特徴とするヘドロ探査機。 2 ヘドロ層表面にて反射される比較的高い周波
数fHの超音波信号の伝搬時間よりヘドロ層表面の
深さを測定し、ヘドロ層を通過する比較的低い周
波数fLの超音波信号の伝搬時間より水底面の深さ
を測定するヘドロ探査機において、前記周波数fH
の超音波の発信信号を作成する発振器と、前記周
波数fHに対して周波数fLだけ異なる周波数fhを中
心とした所定周波数範囲Δf内の任意の周波数fh
の超音波の発信信号を作成する周波数可変発振器
と、前記2つの発信信号を合成して一の送受波器
に加える手段と、該一の送受波器にて受信された
信号中より周波数fH又はfh′あるいはfH及びfh′の
信号成分と周波数(fH−fh′)の信号成分とをそ
れぞれ分離する手段とを備え、記周波数fH及び
fh′の2つの超音波信号を前記送受波器より同時
に発信するようにしたことを特徴とするヘドロ探
査機。
[Claims] 1. The depth of the sludge layer surface is measured from the propagation time of an ultrasonic signal with a relatively high frequency f H reflected on the sludge layer surface, and the relatively low frequency f L passing through the sludge layer is measured. In a sludge probe that measures the depth of the water bottom based on the propagation time of an ultrasonic signal, the frequency f H
a first oscillator that generates an ultrasonic transmission signal;
A frequency that differs from the frequency f H by the frequency f L
a second oscillator for generating an ultrasonic transmission signal f h ; a means for combining the two transmission signals and applying the signal to one transducer; and means for separating signal components of frequencies f H or f h or f H and f h and signal components of frequencies f L , and transmits the two ultrasonic signals of frequencies f H and f h to the transducer. A sludge probe that is characterized by transmitting signals more simultaneously. 2. Measure the depth of the sludge layer surface from the propagation time of the ultrasonic signal with a relatively high frequency f H reflected on the sludge layer surface, and measure the propagation of the ultrasonic signal with a relatively low frequency f L passing through the sludge layer. In a sludge probe that measures the depth of the water bottom surface based on time, the frequency f H
an oscillator that generates an ultrasonic transmission signal, and an arbitrary frequency f h within a predetermined frequency range Δf centered on a frequency f h that differs from the frequency f H by a frequency f L.
a variable frequency oscillator for generating an ultrasonic transmission signal; a means for synthesizing the two transmission signals and applying it to one transducer ; or means for separating the signal component of f h ′ or f H and f h ′ from the signal component of frequency (f H −f h ′),
A sludge probe characterized in that two ultrasonic signals f h ' are transmitted simultaneously from the transducer.
JP2258583A 1983-02-14 1983-02-14 Sludge searching machine Granted JPS59147257A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP2258583A JPS59147257A (en) 1983-02-14 1983-02-14 Sludge searching machine

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP2258583A JPS59147257A (en) 1983-02-14 1983-02-14 Sludge searching machine

Publications (2)

Publication Number Publication Date
JPS59147257A JPS59147257A (en) 1984-08-23
JPH0123755B2 true JPH0123755B2 (en) 1989-05-08

Family

ID=12086925

Family Applications (1)

Application Number Title Priority Date Filing Date
JP2258583A Granted JPS59147257A (en) 1983-02-14 1983-02-14 Sludge searching machine

Country Status (1)

Country Link
JP (1) JPS59147257A (en)

Families Citing this family (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JP2012013522A (en) * 2010-06-30 2012-01-19 Korea Atomic Energy Research Inst Method and apparatus for low frequency vibration excitation using ultrasonic wave
JP7188717B1 (en) 2022-03-14 2022-12-13 株式会社人材開発支援機構 Sludge thickness measuring method and sludge thickness measuring device

Also Published As

Publication number Publication date
JPS59147257A (en) 1984-08-23

Similar Documents

Publication Publication Date Title
GB1357329A (en) Detection apparatus
JPS617408A (en) Circuit device for compensating acoustic travelling path error on measurement of wall thickness in ultrasonic pulse
GB2121174A (en) Measurement of distance using ultrasound
JPS60192281A (en) Sludge investigating machine
JPH0123755B2 (en)
US4492117A (en) Ultrasonic nondestructive test apparatus
RU2039368C1 (en) Method of distance measurement and device for its implementation
JPH0449668B2 (en)
RU2097785C1 (en) Phase parametric sonar
SU606127A1 (en) Meter of sound velocity in liquid
SU964542A1 (en) Flow rate meter
SU1388789A1 (en) Ultrasonic flaw detector
SU1352375A1 (en) Device for measuring thin structure of liquid flow speed
SU580498A1 (en) Ultrasound propagation rate meter
SU1620931A1 (en) Device for determining content of gas in gas-liquid medium
SU317322A1 (en) METHOD OF MEASURING TIME DIFFERENCE
SU1702290A1 (en) Acoustic device for determining gas content in gas-fluid media
RU1820233C (en) Method for determination of acoustic resistance in transient layer
JPS58191911A (en) Sludge probing machine
JPS6339843B2 (en)
SU1377622A1 (en) Method of determining temperature
JPS5926911B2 (en) Listening device in underwater detection equipment
SU1233033A1 (en) Method of measuring sound pressure
SU672494A1 (en) Single-channel compensation-type flowmeter
SU744317A1 (en) Ultrasonic method for determining acoustic parameters of fluid