JPS6085381A - Sludge surveyor - Google Patents

Sludge surveyor

Info

Publication number
JPS6085381A
JPS6085381A JP58192464A JP19246483A JPS6085381A JP S6085381 A JPS6085381 A JP S6085381A JP 58192464 A JP58192464 A JP 58192464A JP 19246483 A JP19246483 A JP 19246483A JP S6085381 A JPS6085381 A JP S6085381A
Authority
JP
Japan
Prior art keywords
delay
sludge
frequency
depth
recording
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
Application number
JP58192464A
Other languages
Japanese (ja)
Other versions
JPH0449668B2 (en
Inventor
Hideyuki Takahashi
秀幸 高橋
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 JP58192464A priority Critical patent/JPS6085381A/en
Publication of JPS6085381A publication Critical patent/JPS6085381A/en
Publication of JPH0449668B2 publication Critical patent/JPH0449668B2/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
    • G01S15/88Sonar systems specially adapted for specific applications

Landscapes

  • Engineering & Computer Science (AREA)
  • Radar, Positioning & Navigation (AREA)
  • Remote Sensing (AREA)
  • Physics & Mathematics (AREA)
  • Acoustics & Sound (AREA)
  • Computer Networks & Wireless Communication (AREA)
  • General Physics & Mathematics (AREA)
  • Investigating Or Analyzing Materials By The Use Of Ultrasonic Waves (AREA)
  • Geophysics And Detection Of Objects (AREA)
  • Measurement Of Velocity Or Position Using Acoustic Or Ultrasonic Waves (AREA)

Abstract

PURPOSE:To minimize errors in depth to the surface of sludge and the bottom of water by attaching a delay circuit to a system of receiving sound wave. CONSTITUTION:Variable delay circuits 21 and 22 added are connected to amplifiers 15 and 16 and then, to a record amplifier 17 through a variable switch. Two different frequencies fH and fL pass through the delay circuits 21 and 22 to delay the received wave signal for the correction of the time delay in the receiving system, which enables a recording with limited depth errors. The delay circuit 21 or 22 are given a preset delay value, which is adjusted with a rigid body placed under water and as a signal reflected from the rigid body will not vary with the frequency, it indicates the same depth. Thus, errors in the electric system can be minimized by adjusting and calibrating the delay circuits 21 and 22 so that depth values may appear at the respective fixed position on the record.

Description

【発明の詳細な説明】 〔技術分野〕 本発明は、水底における堆私ヘドロの層厚を測定するヘ
ドロ探査機に関する。
DETAILED DESCRIPTION OF THE INVENTION [Technical Field] The present invention relates to a sludge probe that measures the layer thickness of private sludge on the bottom of an ocean.

〔従来技術〕[Prior art]

以下に1.従来のヘドロ探査機について図面を基に説明
すると共に、その欠点について述べる。
Below are 1. A conventional sludge probe will be explained based on drawings, and its drawbacks will be discussed.

第1図は、従来のヘドロ探査1少のブロック構成図であ
シ、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、6,7は発振
器、8は合成回路、9は送信器2,10は送受切換器、
11は送受波器、12は受信器、13,14はフィルタ
ー、15.16は増幅器、17は記録増幅器、18は水
中、19はヘドロ表面、20は水底面である。尚、Hは
ヘドロ表面19捷での深さ、Lはヘドロ下の水底面20
までの深さ、送受波器11からの点線は周波数の異なる
2つの音波を示す。
FIG. 1 is a block diagram of a conventional sludge probe 1. 1 is a motor, 2 is a recording pen, 3 is a recording paper, 4 is a synchronization pulse generator, 5 is a transmission timing circuit, 6 and 7 are oscillator, 8 is a synthesis circuit, 9 is a transmitter 2, 10 is a transmitter/receiver switch,
11 is a transducer, 12 is a receiver, 13 and 14 are filters, 15 and 16 are amplifiers, 17 is a recording amplifier, 18 is underwater, 19 is the sludge surface, and 20 is the bottom surface of the water. In addition, H is the depth at 19 degrees on the sludge surface, and L is the water bottom surface 20 below the sludge.
The dotted lines from the transducer 11 indicate two sound waves with different frequencies.

従来のヘドロ探査機は、上記のように朽成されている。Conventional sludge probes have fallen into disrepair as described above.

次に、その作用について述べるがその前に本ヘドロ探査
機における基本原理について述べておく。
Next, I will explain its function, but before that, I will explain the basic principle of this sludge probe.

それは、2周波の音波を同時に音場媒質に送波した時、
音場妹質の非線形特性によって音波相互作用を起し、前
記2周波の和と差の周波数分を発生し、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
うパラメトリック効果を利用したところにある。すなわ
ち、比較的高い周波数りの超音波信号を1、前記図面で
いうならばヘドロ表面19に反射させて超音波信号の伝
搬時間よシヘドロ表面19までの深さを測定し、ヘドロ
層を通過する比較的低い周波数りの超音波信号で前記図
面における水底面20に反射させてその伝搬時間より水
底までの深さを測定して、両筒波数類+ fLの測定結
果によシヘドロ層の厚さを測定するのである。
That is, when two-frequency sound waves are simultaneously sent to a sound field medium,
A parametric effect is created in which a sound wave interaction is caused by the nonlinear characteristics of the sound field, and a frequency component of the sum and difference of the two frequencies is generated, and in this case, the frequency component of the difference becomes a sound wave with extremely sharp directivity. It's where I used it. That is, an ultrasonic signal with a relatively high frequency is reflected from the sludge surface 19 in the drawing, the propagation time of the ultrasonic signal and the depth to the sludge surface 19 are measured, and the signal passes through the sludge layer. An ultrasonic signal with a relatively low frequency is reflected on the water bottom surface 20 in the above drawing, and the depth to the water bottom is measured from the propagation time, and the thickness of the Shihedro layer is determined based on the measurement results of both cylinder wave numbers + fL. is measured.

以下、前記図面に基き説明する。The following will explain based on the drawings.

モーフ1によってベルト2が記録紙3の上を移動し記録
ペン2が記録開始点に達すると、同期パルス発生器4よ
シパルスが発生する。該パルスは送信タイミング回路5
で送信タイミングが作成される0 送信タイミングにより、発振器6では比較的高い周波数
k(例えば100 KH25を、発振器7ではhよシ低
い周波数h(例えば90 KH2)のパルス信号を発信
することとなる。
When the belt 2 moves over the recording paper 3 by the morph 1 and the recording pen 2 reaches the recording start point, the synchronization pulse generator 4 generates a pulse. The pulse is sent to the transmission timing circuit 5
The transmission timing is created at 0. According to the transmission timing, the oscillator 6 transmits a pulse signal with a relatively high frequency k (for example, 100 KH25), and the oscillator 7 transmits a pulse signal with a frequency h that is lower than h (for example, 90 KH2).

該周波数りとfLは、合成回路8にて合成し送信器9で
一定しベル迄増幅後、送受切換器io′f:通り送受波
器11に加えられる。
The frequencies RI and fL are combined in a combining circuit 8, amplified to a constant level in a transmitter 9, and then applied to a transmitter/receiver 11.

送受波器11で電気信号は超音波信号に変換され水中1
8に発射される。
The electrical signal is converted into an ultrasonic signal by the transducer 11 and sent to the underwater 1
It will be launched on 8.

水中18に発射された音波はヘドロ表面19で反射され
ると共に、前記パラメトリック効果による差の周波数り
の超音波信号が発生し水底面2゜にて反射される。該両
反射音波は送受sg:+1iにて受信される。
The sound waves emitted into the water 18 are reflected by the sludge surface 19, and an ultrasonic signal having a frequency difference due to the parametric effect is generated and reflected at the bottom surface 2 degrees of the water. Both reflected sound waves are received at transmission/reception sg:+1i.

該受信信号は送受切換器10を通シ受信器12で一定し
ベル迄増幅され、フィルタ13にて周誠数五(の信号の
みを通し、フィルタ14は、/Lの信号のみを通す。
The received signal is passed through a transmitter/receiver switch 10, amplified to a constant level by a receiver 12, and a filter 13 passes only a signal of 5(5), and a filter 14 passes only a signal of /L.

該両信号は増幅器15.16で夫れそれ一定レベルに増
幅後、記録増幅器17で加算後増幅して記録ペン2に加
え、記録紙3に記録する。
Both signals are amplified to a constant level by amplifiers 15 and 16, and then added and amplified by a recording amplifier 17, and then added to the recording pen 2 and recorded on the recording paper 3.

次に、第2図に示す従来のヘドロ探査機による記録例を
基に記録;LTh3への記録状態について述べる。
Next, the state of recording to LTh3 will be described based on an example of recording by the conventional sludge probe shown in FIG.

水中18の超音波が伝搬中に記録ペン2は移動しておシ
、送信時点と受信時点の記録ペン2の位置の差が深度と
なって記録紙3に記録される。
The recording pen 2 moves while the ultrasonic waves in the water 18 are propagating, and the difference in the position of the recording pen 2 between the time of transmission and the time of reception is recorded on the recording paper 3 as the depth.

そこで、受信系で扱う周波数fHとfr、とは10倍程
度の差があるだめ次のような欠点が生じてくる。
Therefore, since there is a difference of about 10 times between the frequencies fH and fr handled by the receiving system, the following drawback occurs.

それは、フィルタ13,14と増幅器15.16及び送
受波器11内での周波数jH,l!:fLの周波数特性
の差から遅延時間の差が生じるので、結果的に深度誤差
を生ずるという欠点である。
That is, the frequencies jH, l! in the filters 13, 14, amplifiers 15, 16, and transducer 11. : A difference in delay time arises from a difference in frequency characteristics of fL, resulting in a depth error.

〔発明の目的〕[Purpose of the invention]

そこで、本発明は同波数にとfLの遅延時間の差を補正
することにより、従来の欠点を解決することを目的とし
て成すものである。
SUMMARY OF THE INVENTION Therefore, the present invention aims to solve the conventional drawbacks by correcting the difference in delay time between fL and the same wave number.

〔発明の構成〕[Structure of the invention]

その、本発明の構成は次の通りである。 The structure of the present invention is as follows.

前記従来例における構成部品の両増幅器に夫れそれ可変
の遅延回路を設けて記録増幅器に接続する構成とするこ
とである。
Both amplifiers of the components in the conventional example are each provided with a variable delay circuit and connected to the recording amplifier.

〔実施例〕〔Example〕

以下に、前記すようガ目的と構成を特徴とした本発明の
2つの実施例を図面に基づいて説明すると共に、その効
果を述べる。尚、従来例と同一構成部品については従来
例とロー符号を使用する。
Hereinafter, two embodiments of the present invention characterized by the above-mentioned purpose and configuration will be explained based on the drawings, and the effects thereof will be described. Incidentally, for components that are the same as those in the conventional example, the same reference numerals as those in the conventional example are used.

第3図は、本発明の第J実施例によるヘドロ探査機のブ
ロック構成図であシ、1はモーフ12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、6,7は発振器、8は合成回路、9は送信器、10
は送受切換器、11は送受波器、12は受信器、13.
14はフィルタ、is、ieは増幅器、17は記録増幅
器、18は水中、19はヘドロ表面、20は水底面であ
り、Hはヘドロ表面19までの深さ、Lは水底面20ま
での深さ、点線は周波数の異なる2つの音波を示す。
FIG. 3 is a block configuration diagram of a sludge probe according to the J embodiment of the present invention, in which 1 is a morph 12, a recording pen, 3 is a recording paper, 4 is a synchronization pulse generator, 5 is a transmission timing circuit, 6 and 7 are oscillators, 8 is a synthesis circuit, 9 is a transmitter, 10
11 is a transmitter/receiver, 12 is a receiver, 13.
14 is a filter, is and ie are amplifiers, 17 is a recording amplifier, 18 is underwater, 19 is the sludge surface, 20 is the water bottom surface, H is the depth to the sludge surface 19, and L is the depth to the water bottom surface 20. , the dotted lines indicate two sound waves with different frequencies.

以上は従来例同様であり、以下に本発明により付加した
可変の遅延回路の構成について述べる。
The above is the same as the conventional example, and the configuration of the variable delay circuit added according to the present invention will be described below.

21.22は本発明によシ付加した可変の遅延回路であ
わ、増幅器15.16に接続して可変のスイッチを介し
て記録増幅器17に接続している。
Reference numerals 21 and 22 denote variable delay circuits added according to the present invention, which are connected to amplifiers 15 and 16 and then connected to the recording amplifier 17 via a variable switch.

本発明の第1実施例は、このように構成され、その動作
も従来同様であるが5.2つの異なる周波数fiI+、
h−は遅延回路21.22を通シ、受波信号を遅延さす
ことにより受信系の時間遅れを補正し、深度誤差の少々
い記録が行々えることとなる。
The first embodiment of the present invention is configured as described above, and its operation is similar to the conventional one, but 5. two different frequencies fiI+,
h- is passed through delay circuits 21 and 22, and by delaying the received signal, the time delay of the receiving system is corrected, and recording with a slight depth error can be performed.

尚6.遅延回路21、あるいは22は予じめ設定した遅
延量を有しており、この遅延量の調整は水中に剛体を置
きこれより反射する信号は周波数によシ異なることはな
いので同一の深度を示すこととなる。これによって記録
上同一場所に表われるように遅延回路21.22を調整
し較正することによシミ気系の誤差を最少にするのであ
る。
Note 6. The delay circuit 21 or 22 has a preset delay amount, and this delay amount can be adjusted by placing a rigid body in the water, and since the signals reflected from this body do not differ depending on the frequency, It will be shown. This minimizes stain system errors by adjusting and calibrating the delay circuits 21, 22 so that they appear at the same location on the record.

次に、第4図に示す受信信号を基に遅延量について述べ
る。尚、第4図において、遅延回路21への入力信号を
A1遅延回路22−への入力信号をBとしである。
Next, the amount of delay will be described based on the received signal shown in FIG. In FIG. 4, the input signal to the delay circuit 21 is A, and the input signal to the delay circuit 22- is B.

図に示すように、一定、レベルで記鉤するように設定し
た記録増幅器では高い周波数が早めに唄”かれる。同じ
立ち上がりの波数であっても波長が異なるためにfLは
遅れて咽かれてしまう。
As shown in the figure, in a recording amplifier that is set to record at a constant level, high frequencies are sung early. Even if the rising wave number is the same, the wavelengths are different, so fL is delayed and dies out. .

そこで、送信時点から記録される迄のI21vk n 
fiIの波をTH% fLO波をTLとすると、THT
したけ誤差を生ずることが分かる。この誤差時■1jだ
け、周波数kを入力する遅延回路22にて周波数fx、
を遅らすのである。また、周波数九による深度が異なる
」場合はfI(を入力する遅延回路21によって調整す
ればよい。
Therefore, I21vk n from the time of transmission to the time of recording
If the fiI wave is TH% and the fLO wave is TL, then THT
It can be seen that a certain amount of error occurs. When this error occurs, the frequency fx,
It delays the In addition, if the depth differs depending on the frequency 9, it may be adjusted by the delay circuit 21 that inputs fI().

尚1この場合、記録は遅らすのみしかできないため絶対
値H,Lは、この遅延時間だけの固定誤差を生ずること
になるので零点の位置をすらすl要があり、記録紙3の
目盛をずらず方法や、スケールを読む時ずらして読む方
法で行なう。
Note 1: In this case, since recording can only be delayed, the absolute values H and L will have a fixed error equal to this delay time. This can be done by reading the scale or by shifting the scale when reading.

続いて、前記第1実施例による遅延回路21゜22に代
えて次のような遅延回路を代願する方法も可能々ので、
第2実施例として説明する。71)、 5図に基づく。
Next, it is also possible to apply the following delay circuit instead of the delay circuits 21 and 22 according to the first embodiment.
This will be explained as a second embodiment. 71), based on Figure 5.

第5図は第2実姉例を示す遅延回路構成し4でちり、2
3はアナログ−デジタル変換器、24,25゜26.2
7はシフトレジスタ、28,29,30゜31は連動し
て動くスイッチ、32はデジタル−アナログ変換器であ
る。
Fig. 5 shows the delay circuit configuration showing the second example.
3 is an analog-digital converter, 24, 25° 26.2
7 is a shift register; 28, 29, 30; 31 are switches that operate in conjunction with each other; and 32 is a digital-to-analog converter.

本回路を前記第1実施例の遅延回路21.22と代える
と、捷ずアナログ−デジタル変換器23にて、本図の場
合4ビツトに変換しシフトレジスタ24〜27に入力す
る。
If this circuit is replaced with the delay circuits 21 and 22 of the first embodiment, the analog-to-digital converter 23 converts the signal into 4 bits in the case of this figure and inputs it to the shift registers 24-27.

この、シフトレジスタ24〜27の各ビットハ出力され
スイッチ28〜31につながっておシ、]個当シのシフ
ト長はnoビットとする。シフトパルスの間隙をT秒と
すると当然任意の点nビット目の遅延時間はルT秒とな
る。
Each bit of the shift registers 24 to 27 is outputted and connected to the switches 28 to 31, and the shift length of each bit is set to no bits. If the gap between shift pulses is T seconds, the delay time at any n-th bit is naturally T seconds.

このように、シフトレジスタ24〜27の初段からnビ
ット目の出力を取ればnTT秒延することができる。
In this way, by taking the n-th bit output from the first stage of the shift registers 24 to 27, it is possible to delay the processing by nTT seconds.

遅延した信号はデジタル−アナログ変換器32にて再び
アナログ信号に変換する。
The delayed signal is again converted into an analog signal by the digital-to-analog converter 32.

このように、第2実施例においても第1実が0例同様に
受信信号の遅延揺正を行なうことができる、〔発明の効
果〕 以上、詳細に説明したように本発明では周波数の異々る
2つの音波を水底に発信してヘドロ面と水底面からの反
射音波を受信することによシヘドロ層厚を測定するヘド
ロ探査機において@誠の受信系に遅延回路を付加したの
で次のような効果を発揮することができる。
In this way, in the second embodiment, the delay correction of the received signal can be performed in the same manner as in the case where the first fruit is 0. A delay circuit was added to @Makoto's receiving system in the sludge probe, which measures the thickness of the sludge layer by transmitting two sound waves to the bottom of the water and receiving the reflected sound waves from the sludge surface and the bottom surface. It can be effective.

それは、ヘドロ面までの深さと水底n1での深さを測定
して、その両者の差によって−\1・oQ厚を測定する
ので、従来の探査機では受信系内で2種の音波の周波数
特性の差から遅延時間の差を生じ前記深度に誤差を生ず
るという欠点を本発明では解決し、受信系に付加した遅
延回路によって遅延時間の差を調整できるのでヘドロ表
面及び水底面までの深度誤差を少なくできる効果である
It measures the depth to the sludge surface and the depth at the bottom n1, and determines the -\1・oQ thickness by the difference between the two, so in conventional probes, the two types of sound waves are The present invention solves the drawback that a difference in delay time occurs due to a difference in characteristics and causes an error in the depth, and since the difference in delay time can be adjusted by a delay circuit added to the receiving system, the depth error between the sludge surface and the water bottom can be reduced. This has the effect of reducing

これによって、ヘドロ層の正確な探査を行なうことがで
きる。
This allows accurate exploration of the sludge layer.

このように、本発明はヘドロ探査佛において有益に利用
するととができる。
Thus, the present invention can be advantageously utilized in sludge exploration.

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

第1図は従来のヘドロ探査機のブロック構成図、第2図
は従来の記録例を示す記録紙、第3図は本発明の第1実
施例によるヘドロ探査機のブロック構成図、第4図は受
信信号図、第5図は第2実施例を示す他の遅延回路図で
ある。 1・・・モータ 2・・・記録ペン 3・・・記録紙 
4・・・同期パルス発生器 11・・送受波器 18・
・・水中19・・ヘドロ表面 20・・・水底面特許出
願人 沖電気工業株式会社 代理人弁理士 金 倉 喬 二
FIG. 1 is a block diagram of a conventional sludge probe, FIG. 2 is a recording paper showing a conventional recording example, FIG. 3 is a block diagram of a sludge probe according to the first embodiment of the present invention, and FIG. 4 is a received signal diagram, and FIG. 5 is another delay circuit diagram showing the second embodiment. 1...Motor 2...Recording pen 3...Recording paper
4... Synchronous pulse generator 11... Transducer/receiver 18.
...Underwater 19...Sludge surface 20...Underwater surface Patent applicant Takashi Kanakura, Patent attorney representing Oki Electric Industry Co., Ltd.

Claims (1)

【特許請求の範囲】[Claims] 1 周波数Inの超音波を作成する発振器と周波数f+
yよシ低い周波数fLの超音波を作成する発振器を備え
、該周波数fHと九を合成して送受波器に加え、該送受
波器よシ水底に合成した間鼓数りとJLの超音波を同時
に発信しヘドロ表面と水底面から反射した両超音波を前
記送受波器で受信し、周波数りとり、の受信信号を2つ
のフィルタにて分離して夫れそれ増幅器で増幅し、周波
数fi■とfLの超音波の発信時点と受信時点を記録し
、該記録によシヘドロ表面と水底面までの深さを測定し
これを基にヘドロ層厚を測定するヘドロ探査機において
、前記周波数fH,!:JLの受信超音波を増幅する増
幅器の一方あるいは両方に遅延回路を設は周波数力(と
fLの周波数特性の差がら牛じる遅延量を遅延回路で予
じめ補正することを特徴としたヘドロ探査機。
1 Oscillator that creates ultrasonic waves with frequency In and frequency f+
Equipped with an oscillator that creates ultrasonic waves with a frequency fL lower than y, the frequencies fH and 9 are combined and added to the transducer, and the transducer generates ultrasonic waves of the combined frequency fL and JL on the bottom of the water. The two ultrasonic waves reflected from the sludge surface and the water bottom are received by the transducer, and the received signals are separated by two filters and amplified by respective amplifiers. In a sludge probe that records the transmission and reception times of ultrasonic waves of ,! : A delay circuit is installed in one or both of the amplifiers that amplify the received ultrasonic waves of JL, and the amount of delay due to the difference in the frequency characteristics of frequency power (and fL) is compensated in advance by the delay circuit. Sludge probe.
JP58192464A 1983-10-17 1983-10-17 Sludge surveyor Granted JPS6085381A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP58192464A JPS6085381A (en) 1983-10-17 1983-10-17 Sludge surveyor

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP58192464A JPS6085381A (en) 1983-10-17 1983-10-17 Sludge surveyor

Publications (2)

Publication Number Publication Date
JPS6085381A true JPS6085381A (en) 1985-05-14
JPH0449668B2 JPH0449668B2 (en) 1992-08-12

Family

ID=16291727

Family Applications (1)

Application Number Title Priority Date Filing Date
JP58192464A Granted JPS6085381A (en) 1983-10-17 1983-10-17 Sludge surveyor

Country Status (1)

Country Link
JP (1) JPS6085381A (en)

Cited By (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS6375554A (en) * 1986-09-17 1988-04-05 Nobuo Nakayama Method and device for measurement utilizing acoustic wave
WO2023176072A1 (en) 2022-03-14 2023-09-21 株式会社人材開発支援機構 Sludge thickness measurement method and sludge thickness measurement device

Citations (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS5672372A (en) * 1979-11-16 1981-06-16 Oki Electric Ind Co Ltd Sound depth meter
JPS5796255A (en) * 1980-12-05 1982-06-15 Oki Electric Ind Co Ltd Sludge detector

Patent Citations (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS5672372A (en) * 1979-11-16 1981-06-16 Oki Electric Ind Co Ltd Sound depth meter
JPS5796255A (en) * 1980-12-05 1982-06-15 Oki Electric Ind Co Ltd Sludge detector

Cited By (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS6375554A (en) * 1986-09-17 1988-04-05 Nobuo Nakayama Method and device for measurement utilizing acoustic wave
WO2023176072A1 (en) 2022-03-14 2023-09-21 株式会社人材開発支援機構 Sludge thickness measurement method and sludge thickness measurement device

Also Published As

Publication number Publication date
JPH0449668B2 (en) 1992-08-12

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